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300 | 1906.06568 | Hong Tao Liu | H. T. Liu, Hai Cheng Feng, Y. X. Xin, J. M. Bai, S. K. Li, and Fang
Wang | Search for Intra-day Optical Variability in $\gamma$-ray--loud Blazars
S5 0716+714 and 3C 273 | 23 pages, 8 Figures, 2 Tables, accepted for publication in The
Astrophysical Journal, typos | 2019, ApJ, 880, 155 | 10.3847/1538-4357/ab29fc | null | astro-ph.GA astro-ph.HE | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present the photometric observations of blazars S5 0716+714 and 3C 273
with high temporal resolution (30--60s) in the $I$ or $R$ bands. The
observations were performed with a 1.02 m optical telescope from 2007 March 07
to 2012 May 16. The $F$-test, one-way analysis of variance (ANOVA) test, and
$z$-transformed discrete correlation function (ZDCF) cross-correlation zero lag
test are used to search for intra-day variability (IDV). Four and five reliable
IDVs survive three tests for S5 0716+714 and 3C 273, respectively. IDVs are
found for S5 0716+714 and 3C 273. A flare on 2008 May 08 has $\Delta I \approx$
0.06$\pm$0.01 mag in a duration of 0.54 hr for S5 0716+714. A flare on 2011 May
10 shows $\Delta R \approx$ 0.05$\pm$0.01 mag in a duration of 0.40 hr for 3C
273. Sharp dips appear on 2011 May 9 for 3C 273, and show $\Delta R \approx$
0.05$\pm$0.01 mag. Under the assumptions that the IDV is tightly connected to
black hole mass, $M_{\bullet}$, and that the flare durations are representative
of the minimum characteristic timescales, we can estimate upper bounds to
$M_{\bullet}$. In the case of the Kerr black holes, $M_{\bullet} \la 10^{8.91}
M_{\odot}$ and $M_{\bullet} \la 10^{9.02} M_{\odot}$ are given for S5 0716+714
and 3C 273, respectively. These mass measurements are consistent with those
measurements reported in the literatures. Also, we discuss the origins of
optical variations found in this work.
| [{'version': 'v1', 'created': 'Sat, 15 Jun 2019 14:20:14 GMT'}
{'version': 'v2', 'created': 'Wed, 7 Aug 2019 01:08:51 GMT'}] | 2019-08-09 | [array(['Liu', 'H. T.', ''], dtype=object)
array(['Feng', 'Hai Cheng', ''], dtype=object)
array(['Xin', 'Y. X.', ''], dtype=object)
array(['Bai', 'J. M.', ''], dtype=object)
array(['Li', 'S. K.', ''], dtype=object)
array(['Wang', 'Fang', ''], dtype=object)] |
301 | quant-ph/0403146 | Anocha Yimsiriwattana | Anocha Yimsiriwattana and Samuel J. Lomonaco Jr | Distributed quantum computing: A distributed Shor algorithm | 13 pages, 12 figures, extra figures are removed | null | 10.1117/12.546504 | null | quant-ph | null | We present a distributed implementation of Shor's quantum factoring algorithm
on a distributed quantum network model. This model provides a means for small
capacity quantum computers to work together in such a way as to simulate a
large capacity quantum computer. In this paper, entanglement is used as a
resource for implementing non-local operations between two or more quantum
computers. These non-local operations are used to implement a distributed
factoring circuit with polynomially many gates. This distributed version of
Shor's algorithm requires an additional overhead of O((log N)^2) communication
complexity, where N denotes the integer to be factored.
| [{'version': 'v1', 'created': 'Fri, 19 Mar 2004 23:27:15 GMT'}
{'version': 'v2', 'created': 'Tue, 23 Mar 2004 09:50:57 GMT'}] | 2009-11-10 | [array(['Yimsiriwattana', 'Anocha', ''], dtype=object)
array(['Lomonaco', 'Samuel J.', 'Jr'], dtype=object)] |
302 | 1706.02372 | Xin Wang | Xin Wang, Howard A. Stone and Ramin Golestanian | Shape of the Growing Front of Biofilms | 13 pages, 4 figures | New Journal of Physics 19.12 (2017): 125007 | 10.1088/1367-2630/aa983f | null | physics.bio-ph cond-mat.soft q-bio.CB | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The spatial organization of bacteria in dense biofilms is key to their
collective behaviour, and understanding it will be important for medical and
technological applications. Here we study the morphology of a compact biofilm
that undergoes unidirectional growth, and determine the condition for the
stability of the growing interface as a function of the nutrient concentration
and mechanical tension. Our study suggests that transient behaviour may play an
important role in shaping the structure of a biofilm.
| [{'version': 'v1', 'created': 'Wed, 7 Jun 2017 20:28:58 GMT'}] | 2019-03-05 | [array(['Wang', 'Xin', ''], dtype=object)
array(['Stone', 'Howard A.', ''], dtype=object)
array(['Golestanian', 'Ramin', ''], dtype=object)] |
303 | 1607.02145 | Federico Lelli | Federico Lelli (1), Stacy S. McGaugh (1), James M. Schombert (2), and
Marcel S. Pawlowski (1) ((1) Case Western Reserve University, (2) University
of Oregon) | The Relation between Stellar and Dynamical Surface Densities in the
Central Regions of Disk Galaxies | Accepted for publication in ApJL (6 pages, 3 figures) | null | 10.3847/2041-8205/827/1/L19 | null | astro-ph.GA astro-ph.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use the SPARC (Spitzer Photometry & Accurate Rotation Curves) database to
study the relation between the central surface density of stars Sstar and
dynamical mass Sdyn in 135 disk galaxies (S0 to dIrr). We find that Sdyn
correlates tightly with Sstar over 4 dex. This central density relation can be
described by a double power law. High surface brightness galaxies are
consistent with a 1:1 relation, suggesting that they are self-gravitating and
baryon dominated in the inner parts. Low surface brightness galaxies
systematically deviate from the 1:1 line, indicating that the dark matter
contribution progressively increases but remains tightly coupled to the stellar
one. The observed scatter is small (~0.2 dex) and largely driven by
observational uncertainties. The residuals show no correlations with other
galaxy properties like stellar mass, size, or gas fraction.
| [{'version': 'v1', 'created': 'Thu, 7 Jul 2016 20:00:03 GMT'}] | 2016-08-17 | [array(['Lelli', 'Federico', ''], dtype=object)
array(['McGaugh', 'Stacy S.', ''], dtype=object)
array(['Schombert', 'James M.', ''], dtype=object)
array(['Pawlowski', 'Marcel S.', ''], dtype=object)] |
304 | 1902.07187 | Anastasios Giovanidis | Anastasios Giovanidis, Bruno Baynat, Antoine Vendeville | Performance Analysis of Online Social Platforms | Preliminary version of accepted paper at INFOCOM 2019 (Paris, France) | INFOCOM 2019, Paris, France | 10.1109/INFOCOM.2019.8737539 | null | cs.NI cs.PF | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We introduce an original mathematical model to analyze the diffusion of posts
within a generic online social platform. Each user of such a platform has his
own Wall and Newsfeed, as well as his own self-posting and re-posting activity.
As a main result, using our developed model, we derive in closed form the
probabilities that posts originating from a given user are found on the Wall
and Newsfeed of any other. These probabilities are the solution of a linear
system of equations. Conditions of existence of the solution are provided, and
two ways of solving the system are proposed, one using matrix inversion and
another using fixed-point iteration. Comparisons with simulations show the
accuracy of our model and its robustness with respect to the modeling
assumptions. Hence, this article introduces a novel measure which allows to
rank users by their influence on the social platform, by taking into account
not only the social graph structure, but also the platform design, user
activity (self- and re-posting), as well as competition among posts.
| [{'version': 'v1', 'created': 'Tue, 19 Feb 2019 18:38:29 GMT'}] | 2019-06-25 | [array(['Giovanidis', 'Anastasios', ''], dtype=object)
array(['Baynat', 'Bruno', ''], dtype=object)
array(['Vendeville', 'Antoine', ''], dtype=object)] |
305 | 0804.0520 | Vittorio Giovannetti | Vittorio Giovannetti, Simone Montangero, and Rosario Fazio | Quantum MERA Channels | 4 pages, 2 figures | Phys. Rev. Lett. 101, 180503 (2008) | 10.1103/PhysRevLett.101.180503 | null | quant-ph cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Tensor networks representations of many-body quantum systems can be described
in terms of quantum channels. We focus on channels associated with the
Multi-scale Entanglement Renormalization Ansatz (MERA) tensor network that has
been recently introduced to efficiently describe critical systems. Our approach
allows us to compute the MERA correspondent to the thermodynamic limit of a
critical system introducing a transfer matrix formalism, and to relate the
system critical exponents to the convergence rates of the associated channels.
| [{'version': 'v1', 'created': 'Thu, 3 Apr 2008 10:44:09 GMT'}
{'version': 'v2', 'created': 'Mon, 6 Oct 2008 13:18:40 GMT'}
{'version': 'v3', 'created': 'Fri, 14 Nov 2008 18:14:31 GMT'}] | 2009-11-13 | [array(['Giovannetti', 'Vittorio', ''], dtype=object)
array(['Montangero', 'Simone', ''], dtype=object)
array(['Fazio', 'Rosario', ''], dtype=object)] |
306 | astro-ph/0208168 | Martin White | C.S. Kochanek, Martin White, J. Huchra, L. Macri, T.H. Jarrett, S.E.
Schneider, J. Mader | Clusters of galaxies in the local universe | 22 pages, 15 figures | Astrophys.J.585:161-181,2003 | 10.1086/345896 | null | astro-ph | null | We use a matched filter algorithm to find and study clusters in both N-body
simulations artificially populated with galaxies and the 2MASS survey. In
addition to numerous checks of the matched filter algorithm, we present results
on the halo multiplicity function and the cluster number function. For a subset
of our identified clusters we have information on X-ray temperatures and
luminosities which we cross-correlate with optical richness and galaxy velocity
dispersions. With all quantities normalized by the spherical radius
corresponding to a mass overdensity of Delta_M=200 or the equivalent galaxy
number overdensity of Delta_N=200Omega^{-1}~666, we find that the number of
L>L_* galaxies in a cluster of mass M_{200} is log N_{*666} = (1.44 +/-
0.17)+(1.10 +/- 0.09)log(M_{200}h/10^{15}Msun) where the uncertainties are
dominated by the scatter created by three choices for relating the observed
quantities to the cluster mass. The region inside the virial radius has a
K-band cluster mass-to-light ratio of (M/L)_K=(116 +/- 46)h which is
essentially independent of cluster mass. Integrating over all clusters more
massive than M_{200}=10^{14}Msun/h, the virialized regions of clusters contain
~7% of the local stellar luminosity, quite comparable to the mass fraction in
such objects in currently popular LambdaCDM models.
| [{'version': 'v1', 'created': 'Wed, 7 Aug 2002 22:05:29 GMT'}] | 2008-11-07 | [array(['Kochanek', 'C. S.', ''], dtype=object)
array(['White', 'Martin', ''], dtype=object)
array(['Huchra', 'J.', ''], dtype=object)
array(['Macri', 'L.', ''], dtype=object)
array(['Jarrett', 'T. H.', ''], dtype=object)
array(['Schneider', 'S. E.', ''], dtype=object)
array(['Mader', 'J.', ''], dtype=object)] |
307 | cs/0502001 | Shengtian Yang | Shengtian Yang, Peiliang Qiu | Some Extensions of Gallager's Method to General Sources and Channels | submitted to 2005 IEEE International Symposium on Information Theory | null | null | null | cs.IT math.IT | null | The Gallager bound is well known in the area of channel coding. However, most
discussions about it mainly focus on its applications to memoryless channels.
We show in this paper that the bounds obtained by Gallager's method are very
tight even for general sources and channels that are defined in the
information-spectrum theory. Our method is mainly based on the estimations of
error exponents in those bounds, and by these estimations we proved the direct
part of the Slepian-Wolf theorem and channel coding theorem for general sources
and channels.
| [{'version': 'v1', 'created': 'Tue, 1 Feb 2005 02:19:01 GMT'}] | 2007-07-13 | [array(['Yang', 'Shengtian', ''], dtype=object)
array(['Qiu', 'Peiliang', ''], dtype=object)] |
308 | 0903.1291 | Andrew M. Childs | Andris Ambainis, Andrew M. Childs, Fran\c{c}ois Le Gall, Seiichiro
Tani | The quantum query complexity of certification | 8 pages; Updated to reflect changes in final journal version and to
point out that the main result only applies for k>1 | Quantum Information and Computation 10, 181-188 (2010) | 10.26421/QIC10.3-4 | null | quant-ph cs.CC | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the quantum query complexity of finding a certificate for a
d-regular, k-level balanced NAND formula. Up to logarithmic factors, we show
that the query complexity is Theta(d^{(k+1)/2}) for 0-certificates, and
Theta(d^{k/2}) for 1-certificates. In particular, this shows that the
zero-error quantum query complexity of evaluating such formulas is
O(d^{(k+1)/2}) (again neglecting a logarithmic factor). Our lower bound relies
on the fact that the quantum adversary method obeys a direct sum theorem.
| [{'version': 'v1', 'created': 'Fri, 6 Mar 2009 21:22:18 GMT'}
{'version': 'v2', 'created': 'Mon, 6 Oct 2014 18:40:56 GMT'}] | 2018-12-20 | [array(['Ambainis', 'Andris', ''], dtype=object)
array(['Childs', 'Andrew M.', ''], dtype=object)
array(['Gall', 'François Le', ''], dtype=object)
array(['Tani', 'Seiichiro', ''], dtype=object)] |
309 | 1311.4050 | Shunichiro Kittaka | Shunichiro Kittaka, Toshiro Sakakibara, Masato Hedo, Yoshichika Onuki,
and Kazushige Machida | Verification of Anisotropic s-Wave Superconducting Gap Structure in
CeRu2 from Low-Temperature Field-Angle-Resolved Specific Heat Measurements | 5 pages, 5 figures | J. Phys. Soc. Jpn. 82, 123706 (2013) | 10.7566/JPSJ.82.123706 | null | cond-mat.supr-con cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The field-angle-resolved specific heat C(T,H,phi) of the f-electron
superconductor CeRu2 (Tc=6.3 K) has been measured at low temperatures down to
90 mK on two single crystals of slightly different qualities. We reveal that
the C(phi) oscillation in a rotating magnetic field, originating from the gap
anisotropy, diminishes at low temperatures below the characteristic field H*,
as expected for an anisotropic gap without nodes. We also observe the
suppression of H* by decreasing the gap anisotropy ratio $\Delta_{\rm
min}/\Delta_{\rm max}$, a behavior that has been predicted from a microscopic
theory for anisotropic s-wave superconductors. The present technique is
established as a powerful tool for investigating minimum-gap structures as well
as nodal structures.
| [{'version': 'v1', 'created': 'Sat, 16 Nov 2013 12:27:49 GMT'}] | 2013-11-19 | [array(['Kittaka', 'Shunichiro', ''], dtype=object)
array(['Sakakibara', 'Toshiro', ''], dtype=object)
array(['Hedo', 'Masato', ''], dtype=object)
array(['Onuki', 'Yoshichika', ''], dtype=object)
array(['Machida', 'Kazushige', ''], dtype=object)] |
310 | 2206.00393 | Shunqi Mao | Shunqi Mao, Chaoyi Zhang, Heng Wang, Weidong Cai | Towards Generalisable Audio Representations for Audio-Visual Navigation | CVPR 2022 Embodied AI Workshop | null | null | null | cs.SD cs.CV cs.LG cs.RO eess.AS | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In audio-visual navigation (AVN), an intelligent agent needs to navigate to a
constantly sound-making object in complex 3D environments based on its audio
and visual perceptions. While existing methods attempt to improve the
navigation performance with preciously designed path planning or intricate task
settings, none has improved the model generalisation on unheard sounds with
task settings unchanged. We thus propose a contrastive learning-based method to
tackle this challenge by regularising the audio encoder, where the
sound-agnostic goal-driven latent representations can be learnt from various
audio signals of different classes. In addition, we consider two data
augmentation strategies to enrich the training sounds. We demonstrate that our
designs can be easily equipped to existing AVN frameworks to obtain an
immediate performance gain (13.4%$\uparrow$ in SPL on Replica and
12.2%$\uparrow$ in SPL on MP3D). Our project is available at
https://AV-GeN.github.io/.
| [{'version': 'v1', 'created': 'Wed, 1 Jun 2022 11:00:07 GMT'}] | 2022-06-02 | [array(['Mao', 'Shunqi', ''], dtype=object)
array(['Zhang', 'Chaoyi', ''], dtype=object)
array(['Wang', 'Heng', ''], dtype=object)
array(['Cai', 'Weidong', ''], dtype=object)] |
311 | 0809.0828 | Kenji Hamano | The BABAR Collaboration: B. Aubert, et al | Measurements of the Semileptonic Decays $\Bb\to D\ell\nub$ and $\Bb\to
D^*\ell\nub$ Using a Global Fit to $D X\ell\nub$ Final States | 18 pages, 5 figures, submitted to Physical Review D | Phys.Rev.D79:012002,2009 | 10.1103/PhysRevD.79.012002 | BABAR-PUB-08/027, SLAC-PUB-13371 | hep-ex | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Semileptonic $\bar{B}$ decays to $DX\ell\bar{\nu}$ ($\ell=e$ or $mu$) are
selected by reconstructing $D0\ell$ and $D^+\ell$ combinations from a sample of
230 million $\Upsilon(4S) \to B\bar{B}$ decays recorded with the BaBar detector
at the PEPII $e^+e^-$ collider at SLAC. A global fit to these samples in a
3-dimensional space of kinematic variables is used to determine the branching
fractions $\mathcal{B}(B^- \to D0\ell\bar{\nu}) = (2.34 \pm 0.03 \pm 0.13) %$
and $\mathcal{B}(B^- \to D^{*0}\ell\bar{\nu}) = (5.40 \pm 0.02 \pm 0.21)
%$,where the errors are statistical and systematic, respectively. The fit also
determines form factor parameters in a HQET-based parameterization, resulting
in $\rho_D2 = 1.20 \pm 0.04 \pm 0.07$ for $\bar{B} \to D\ell\bar{\nu}$ and
$\rho_{D^*}2 = 1.22 \pm 0.02 \pm 0.07$ for $\bar{B} \to D^*\ell\bar{\nu}$ These
values are used to obtain the product of the CKM matrix element $|V_{cb}|$
times the form factor at the zero recoil point for both $\bar{B} \to
D\ell\bar{\nu}$ decays, $\mathcal{G}(1)|V_{cb}| = (43.1 \pm 0.8 \pm 2.3)\times
10^{-3}$, and for $\bar{B} \to D^*\ell\bar{\nu}$ decays,
$\mathcal{F}(1)|V_{cb}| = (35.9 \pm 0.2 \pm 1.2)\times 10^{-3}$.
| [{'version': 'v1', 'created': 'Thu, 4 Sep 2008 14:57:16 GMT'}
{'version': 'v2', 'created': 'Wed, 17 Dec 2008 02:05:38 GMT'}] | 2010-04-12 | [array(['The BABAR Collaboration', '', ''], dtype=object)
array(['Aubert', 'B.', ''], dtype=object)] |
312 | 1809.06578 | Carsten Schneider | Peter Paule and Carsten Schneider | Towards a symbolic summation theory for unspecified sequences | null | null | null | null | cs.SC math.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The article addresses the problem whether indefinite double sums involving a
generic sequence can be simplified in terms of indefinite single sums.
Depending on the structure of the double sum, the proposed summation machinery
may provide such a simplification without exceptions. If it fails, it may
suggest a more advanced simplification introducing in addition a single nested
sum where the summand has to satisfy a particular constraint. More precisely,
an explicitly given parameterized telescoping equation must hold. Restricting
to the case that the arising unspecified sequences are specialized to the class
of indefinite nested sums defined over hypergeometric, multi-basic or mixed
hypergeometric products, it can be shown that this constraint is not only
sufficient but also necessary.
| [{'version': 'v1', 'created': 'Tue, 18 Sep 2018 08:16:23 GMT'}] | 2018-09-19 | [array(['Paule', 'Peter', ''], dtype=object)
array(['Schneider', 'Carsten', ''], dtype=object)] |
313 | 1703.04368 | Benjamin Goertzel | Ruiting Lian and Ben Goertzel and Linas Vepstas and David Hanson and
Changle Zhou | Symbol Grounding via Chaining of Morphisms | null | null | null | null | cs.AI | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A new model of symbol grounding is presented, in which the structures of
natural language, logical semantics, perception and action are represented
categorically, and symbol grounding is modeled via the composition of morphisms
between the relevant categories. This model gives conceptual insight into the
fundamentally systematic nature of symbol grounding, and also connects
naturally to practical real-world AI systems in current research and commercial
use. Specifically, it is argued that the structure of linguistic syntax can be
modeled as a certain asymmetric monoidal category, as e.g. implicit in the link
grammar formalism; the structure of spatiotemporal relationships and action
plans can be modeled similarly using "image grammars" and "action grammars";
and common-sense logical semantic structure can be modeled using
dependently-typed lambda calculus with uncertain truth values. Given these
formalisms, the grounding of linguistic descriptions in spatiotemporal
perceptions and coordinated actions consists of following morphisms from
language to logic through to spacetime and body (for comprehension), and vice
versa (for generation). The mapping is indicated between the spatial
relationships in the Region Connection Calculus and Allen Interval Algebra and
corresponding entries in the link grammar syntax parsing dictionary. Further,
the abstractions introduced here are shown to naturally model the structures
and systems currently being deployed in the context of using the OpenCog
cognitive architecture to control Hanson Robotics humanoid robots.
| [{'version': 'v1', 'created': 'Mon, 13 Mar 2017 13:06:49 GMT'}] | 2017-03-14 | [array(['Lian', 'Ruiting', ''], dtype=object)
array(['Goertzel', 'Ben', ''], dtype=object)
array(['Vepstas', 'Linas', ''], dtype=object)
array(['Hanson', 'David', ''], dtype=object)
array(['Zhou', 'Changle', ''], dtype=object)] |
314 | 1202.3651 | Arvind Ayyer | Arvind Ayyer and Dan Romik | New enumeration formulas for alternating sign matrices and square ice
partition functions | 35 pages | Advances in Mathematics, Volume 235 (2013), Pages 161-186 | 10.1016/j.aim.2012.11.006 | null | math.CO cond-mat.stat-mech math-ph math.MP math.PR | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The refined enumeration of alternating sign matrices (ASMs) of given order
having prescribed behavior near one or more of their boundary edges has been
the subject of extensive study, starting with the Refined Alternating Sign
Matrix Conjecture of Mills-Robbins-Rumsey, its proof by Zeilberger, and more
recent work on doubly-refined and triply-refined enumeration by several
authors. In this paper we extend the previously known results on this problem
by deriving explicit enumeration formulas for the "top-left-bottom"
(triply-refined) and "top-left-bottom-right" (quadruply-refined) enumerations.
The latter case solves the problem of computing the full boundary correlation
function for ASMs. The enumeration formulas are proved by deriving new
representations, which are of independent interest, for the partition function
of the square ice model with domain wall boundary conditions at the
"combinatorial point" 2{\pi}/3.
| [{'version': 'v1', 'created': 'Thu, 16 Feb 2012 17:50:04 GMT'}
{'version': 'v2', 'created': 'Mon, 8 Oct 2012 23:19:36 GMT'}] | 2020-06-16 | [array(['Ayyer', 'Arvind', ''], dtype=object)
array(['Romik', 'Dan', ''], dtype=object)] |
315 | 0911.3248 | Antal Jakovac | A. Jakovac | Non-universal lower bound for the shear viscosity to entropy density
ratio | 14 pages, 2 figures, revtex4; references added, minor corrections in
the text | Phys.Rev.D81:045020,2010 | 10.1103/PhysRevD.81.045020 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The lower bound of the shear viscosity to entropy density ratio is examined
using an exact representation of the ratio through the density of states. It is
shown that the lower bound in a generic physical system is not universal, its
value is determined by the entropy density. Some examples of physical systems
are discussed in the paper where one can expect violation of the conformal
1/4pi value.
| [{'version': 'v1', 'created': 'Tue, 17 Nov 2009 10:15:55 GMT'}
{'version': 'v2', 'created': 'Mon, 23 Nov 2009 10:14:13 GMT'}] | 2014-11-20 | [array(['Jakovac', 'A.', ''], dtype=object)] |
316 | 1504.06704 | Timur Mufakharov | T. Mufakharov, M. Mingaliev, Yu. Sotnikova, Ya. Naiden and A. Erkenov | The observed radio/gamma-ray emission correlation for blazars with the
Fermi-LAT and the RATAN-600 data | 14 pages, 5 tables, 8 figures, accepted to MNRAS | null | 10.1093/mnras/stv772 | null | astro-ph.HE astro-ph.GA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the correlation between gamma-ray and radio band radiation for 123
blazars, using the Fermi-LAT first source catalog (1FGL) and the RATAN-600 data
obtained at the same period of time (within a few months). We found an apparent
positive correlation for BL Lac and flat-spectrum radio quasar (FSRQ) sources
from our sample through testing the value of the Pearson product-moment
correlation coefficient. The BL Lac objects show higher values of the
correlation coefficient than FSRQs at all frequencies, except 21.7 GHz, and at
all bands, except $10-100$ GeV, typically at high confidence level (> 99%). At
higher gamma-ray energies the correlation weakens and even becomes negative for
BL Lacs and FSRQs. For BL Lac blazars, the correlation of the fluxes appeared
to be more sensitive to the considered gamma-ray energy band, than to the
frequency, while for FSRQ sources the correlation changed notably both with the
considered radio frequency and gamma-ray energy band. We used a data
randomization method to quantify the significance of the computed correlation
coefficients. We find that the statistical significance of the correlations we
obtained between the flux densities at all frequencies and the photon flux in
all gamma-ray bands below 3 GeV is high for BL Lacs (chance probability $\sim
10^{-3} - 10^{-7}$). The correlation coefficient is high and significant for
the $0.1-0.3$ GeV band and low and insignificant for the $10-100$ GeV band for
both types of blazars for all considered frequencies.
| [{'version': 'v1', 'created': 'Sat, 25 Apr 2015 09:26:13 GMT'}] | 2015-05-20 | [array(['Mufakharov', 'T.', ''], dtype=object)
array(['Mingaliev', 'M.', ''], dtype=object)
array(['Sotnikova', 'Yu.', ''], dtype=object)
array(['Naiden', 'Ya.', ''], dtype=object)
array(['Erkenov', 'A.', ''], dtype=object)] |
317 | 2208.00101 | Vladimir Ivanov | Yu. A. Nagovitsyn and V. G. Ivanov | Addition to the Gnevyshev-Ohl rule and prediction of solar cycle 25 | 12 pages, 6 figures; submitted to Solar Physics | null | null | null | astro-ph.SR | http://creativecommons.org/licenses/by/4.0/ | In addition to the Gnevyshev-Ohl rule (GOR), the relation of the odd cycle
with the subsequent even one in the 22-year Hale solar cycle was found. It is
shown that 3 years before the 11-year minimum $m$, the value of the relative
sunspot number SN in an odd cycle is closely related to the value of the
maximum in the next even cycle (correlation coefficient $\rho=0.94$), and the
same relation of an odd cycle with the previous even one is weaker. Like GOR,
cycles are linked in pairs, but opposite to the Rule.
Based on this result, we propose to use SN$_{m-3}$ on the descending phase of
the previous odd cycle as a precursor of the subsequent EVEN cycle (Figure 3a)
-- a precursor called MI3E. For the prediction of an odd cycle or a prediction
without consideration of parity (as in the article by Braj\v{s}a et al., 2022),
this method gives less reliable results.
To predict the amplitude of an ODD cycle, we propose to use the precursor of
the seventh year to its maximum $M$ MA7O -- SN$_{M-7}$ on the descending phase
of the previous even cycle (Figure 3b). It turned out that in this case, we can
also predict the years near the maximum with a high correlation coefficient
($\rho=0.90{-}0.94$).
Thus, the proposed approaches allow us to predict cycles of different parity.
According to our prediction, the current solar Cycle 25 in 2023 will reach a
maximum of 154 units with a prediction error of $\pm25$ (68% confidence) and
$\pm53$ (95% confidence). In 2024, SN will be almost as high as in 2023 -- 147
units, so with smaller time averaging scales, the maximum will fall at the end
of 2023.
| [{'version': 'v1', 'created': 'Fri, 29 Jul 2022 23:18:40 GMT'}] | 2022-08-02 | [array(['Nagovitsyn', 'Yu. A.', ''], dtype=object)
array(['Ivanov', 'V. G.', ''], dtype=object)] |
318 | 2001.09161 | Tony Metger | Tony Metger, Thomas Vidick | Self-testing of a single quantum device under computational assumptions | 58 pages, published in Quantum | Quantum 5, 544 (2021) | 10.22331/q-2021-09-16-544 | null | quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Self-testing is a method to characterise an arbitrary quantum system based
only on its classical input-output correlations, and plays an important role in
device-independent quantum information processing as well as quantum complexity
theory. Prior works on self-testing require the assumption that the system's
state is shared among multiple parties that only perform local measurements and
cannot communicate. Here, we replace the setting of multiple non-communicating
parties, which is difficult to enforce in practice, by a single computationally
bounded party. Specifically, we construct a protocol that allows a classical
verifier to robustly certify that a single computationally bounded quantum
device must have prepared a Bell pair and performed single-qubit measurements
on it, up to a change of basis applied to both the device's state and
measurements. This means that under computational assumptions, the verifier is
able to certify the presence of entanglement, a property usually closely
associated with two separated subsystems, inside a single quantum device. To
achieve this, we build on techniques first introduced by Brakerski et al.
(2018) and Mahadev (2018) which allow a classical verifier to constrain the
actions of a quantum device assuming the device does not break post-quantum
cryptography.
| [{'version': 'v1', 'created': 'Fri, 24 Jan 2020 19:00:15 GMT'}
{'version': 'v2', 'created': 'Tue, 1 Dec 2020 14:46:34 GMT'}
{'version': 'v3', 'created': 'Thu, 2 Sep 2021 16:31:34 GMT'}
{'version': 'v4', 'created': 'Tue, 17 May 2022 15:07:50 GMT'}] | 2022-05-18 | [array(['Metger', 'Tony', ''], dtype=object)
array(['Vidick', 'Thomas', ''], dtype=object)] |
319 | 0912.2652 | Saugata Basu | Saugata Basu | A complex analogue of Toda's Theorem | 31 pages. Final version to appear in Foundations of Computational
Mathematics | null | null | null | math.AG cs.CC math.AT math.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Toda \cite{Toda} proved in 1989 that the (discrete) polynomial time
hierarchy, $\mathbf{PH}$, is contained in the class $\mathbf{P}^{#\mathbf{P}}$,
namely the class of languages that can be decided by a Turing machine in
polynomial time given access to an oracle with the power to compute a function
in the counting complexity class $#\mathbf{P}$. This result, which illustrates
the power of counting is considered to be a seminal result in computational
complexity theory. An analogous result (with a compactness hypothesis) in the
complexity theory over the reals (in the sense of Blum-Shub-Smale real machines
\cite{BSS89}) was proved in \cite{BZ09}. Unlike Toda's proof in the discrete
case, which relied on sophisticated combinatorial arguments, the proof in
\cite{BZ09} is topological in nature in which the properties of the topological
join is used in a fundamental way. However, the constructions used in
\cite{BZ09} were semi-algebraic -- they used real inequalities in an essential
way and as such do not extend to the complex case. In this paper, we extend the
techniques developed in \cite{BZ09} to the complex projective case. A key role
is played by the complex join of quasi-projective complex varieties. As a
consequence we obtain a complex analogue of Toda's theorem. The results
contained in this paper, taken together with those contained in \cite{BZ09},
illustrate the central role of the Poincar\'e polynomial in algorithmic
algebraic geometry, as well as, in computational complexity theory over the
complex and real numbers -- namely, the ability to compute it efficiently
enables one to decide in polynomial time all languages in the (compact)
polynomial hierarchy over the appropriate field.
| [{'version': 'v1', 'created': 'Mon, 14 Dec 2009 14:50:38 GMT'}
{'version': 'v2', 'created': 'Tue, 15 Dec 2009 14:31:03 GMT'}
{'version': 'v3', 'created': 'Tue, 15 Dec 2009 21:43:13 GMT'}
{'version': 'v4', 'created': 'Thu, 17 Dec 2009 22:08:56 GMT'}
{'version': 'v5', 'created': 'Sun, 3 Jan 2010 16:46:48 GMT'}
{'version': 'v6', 'created': 'Mon, 1 Mar 2010 18:49:53 GMT'}
{'version': 'v7', 'created': 'Fri, 14 Oct 2011 10:06:57 GMT'}] | 2011-10-17 | [array(['Basu', 'Saugata', ''], dtype=object)] |
320 | 1707.09014 | Ritika Dusad | Azar B. Eyvazov, Ritika Dusad, Timothy J. S. Munsie, Hanna A.
Dabkowska, Graeme M. Luke, Ethan R. Kassner, J.C. S\'eamus Davis and Anna
Eyal | Common Glass-Forming Spin-Liquid State in the Pyrochlore Magnets
Dy$_2$Ti$_2$O$_7$ and Ho$_2$Ti$_2$O$_7$ | 9 pages, 4 figures | Phys. Rev. B 98, 214430 (2018) | 10.1103/PhysRevB.98.214430 | null | cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Despite a well-ordered pyrochlore crystal structure and strong magnetic
interactions between the Dy$^{3+}$ or Ho$^{3+}$ ions, no long range magnetic
order has been detected in the pyrochlore titanates Ho$_2$Ti$_2$O$_7$ and
Dy$_2$Ti$_2$O$_7$. To explore the actual magnetic phase formed by cooling these
materials, we measure their magnetization dynamics using toroidal,
boundary-free magnetization transport techniques. We find that the dynamical
magnetic susceptibility of both compounds has the same distinctive
phenomenology, that is indistinguishable in form from that of the dielectric
permittivity of dipolar glass-forming liquids. Moreover, Ho$_2$Ti$_2$O$_7$ and
Dy$_2$Ti$_2$O$_7$ both exhibit microscopic magnetic relaxation times that
increase along the super-Arrhenius trajectories analogous to those observed in
glass-forming dipolar liquids. Thus, upon cooling below about 2K,
Dy$_2$Ti$_2$O$_7$ and Ho$_2$Ti$_2$O$_7$ both appear to enter the same magnetic
state exhibiting the characteristics of a glass-forming spin-liquid.
| [{'version': 'v1', 'created': 'Thu, 27 Jul 2017 19:37:20 GMT'}
{'version': 'v2', 'created': 'Fri, 5 Jan 2018 20:47:35 GMT'}
{'version': 'v3', 'created': 'Tue, 27 Nov 2018 09:47:14 GMT'}] | 2018-12-26 | [array(['Eyvazov', 'Azar B.', ''], dtype=object)
array(['Dusad', 'Ritika', ''], dtype=object)
array(['Munsie', 'Timothy J. S.', ''], dtype=object)
array(['Dabkowska', 'Hanna A.', ''], dtype=object)
array(['Luke', 'Graeme M.', ''], dtype=object)
array(['Kassner', 'Ethan R.', ''], dtype=object)
array(['Davis', 'J. C. Séamus', ''], dtype=object)
array(['Eyal', 'Anna', ''], dtype=object)] |
321 | 1305.2024 | Guo-Qing Zheng | S. Maeda, K. Matano, H. Sawaoka, Y. Inada, Guo-qing Zheng | Superconductivity in Tetragonal LaPt_{2-x}Ge_{2+x} | 6 pages, 4 figures | J. Phys. Soc. Jpn. 82, 065002 (2013) | 10.7566/JPSJ.82.065002 | null | cond-mat.supr-con | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We find that a tetragonal CaBe_2Ge_2-type structure can be stabilized in
non-stoichiometric LaPt_{2-x}Ge_{2+x}. We further discovered that tetragonal
LaPt_{2-x}Ge_{2+x} with x=0.15 and 0.2 respectively superconduct at Tc=1.85 K
and 1.95 K, which is about four time higher than that in monoclinic LaPt_2Ge_2.
| [{'version': 'v1', 'created': 'Thu, 9 May 2013 07:54:51 GMT'}] | 2013-05-10 | [array(['Maeda', 'S.', ''], dtype=object)
array(['Matano', 'K.', ''], dtype=object)
array(['Sawaoka', 'H.', ''], dtype=object)
array(['Inada', 'Y.', ''], dtype=object)
array(['Zheng', 'Guo-qing', ''], dtype=object)] |
322 | 2306.14414 | Daniel Katz | Daniel J. Katz and Allison E. Wong | Rationality of Four-Valued Families of Weil Sums of Binomials | 32 pages | null | null | null | math.NT cs.CR cs.IT math.CO math.IT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the rationality of Weil sums of binomials of the form
$W^{K,s}_u=\sum_{x \in K} \psi(x^s - u x)$, where $K$ is a finite field whose
canonical additive character is $\psi$, and where $u$ is an element of
$K^{\times}$ and $s$ is a positive integer relatively prime to $|K^\times|$, so
that $x \mapsto x^s$ is a permutation of $K$. The Weil spectrum for $K$ and
$s$, which is the family of values $W^{K,s}_u$ as $u$ runs through $K^\times$,
is of interest in arithmetic geometry and in several information-theoretic
applications. The Weil spectrum always contains at least three distinct values
if $s$ is nondegenerate (i.e., if $s$ is not a power of $p$ modulo
$|K^\times|$, where $p$ is the characteristic of $K$). It is already known that
if the Weil spectrum contains precisely three distinct values, then they must
all be rational integers. We show that if the Weil spectrum contains precisely
four distinct values, then they must all be rational integers, with the sole
exception of the case where $|K|=5$ and $s \equiv 3 \pmod{4}$.
| [{'version': 'v1', 'created': 'Mon, 26 Jun 2023 04:32:48 GMT'}] | 2023-06-27 | [array(['Katz', 'Daniel J.', ''], dtype=object)
array(['Wong', 'Allison E.', ''], dtype=object)] |
323 | 2007.12058 | Rogelio Tomas | Jose L. Abelleira, Robert B. Appleby, Sergey Arsenyev, Javier
Barranco, Michael Benedikt, Maria Ilaria Besana, Oscar Blanco Garcia, Manuela
Boscolo, David Boutin, Xavier Buffat, Helmut Burkhardt, Francesco Cerutti,
Antoine Chance, Francesco Collamati, Emilia Cruz-Alaniz, Barbara Dalena,
Michael Hofer, Barbara L. Humann, Angelo Infantino, Jacqueline Keintzel, Andy
Langner, Marian Luckhof, Roman Martin, Tatiana Pieloni, Haroon Rafique,
Werner Riegler, Leon Van Riesen-Haupt, Daniel Schulte, Andrei Seryi, Claudia
Tambasco, Rogelio Tomas, Frank Zimmermann | FCC-hh Experimental Insertion Region Design | 74 pages | null | null | null | physics.acc-ph hep-ex | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Future Circular Collider study is exploring possible designs of circular
colliders for the post-LHC era, as recommended by the European Strategy Group
for High Energy Physics. One such option is FCC-hh, a proton-proton collider
with a centre-of-mass energy of 100 TeV. The experimental insertion regions are
key areas defining the performance of the collider. This paper presents the
first insertion region designs with a complete assessment of the main
challenges, as collision debris with two orders of magnitude larger power than
current colliders, beam-beam interactions in long insertions, dynamic aperture
for optics with peak $\beta$ functions one order of magnitude above current
colliders, photon background from synchrotron radiation and cross talk between
the insertion regions. An alternative design avoiding the use of crab cavities
with a small impact on performance is also presented.
| [{'version': 'v1', 'created': 'Thu, 23 Jul 2020 15:16:04 GMT'}] | 2020-07-24 | [array(['Abelleira', 'Jose L.', ''], dtype=object)
array(['Appleby', 'Robert B.', ''], dtype=object)
array(['Arsenyev', 'Sergey', ''], dtype=object)
array(['Barranco', 'Javier', ''], dtype=object)
array(['Benedikt', 'Michael', ''], dtype=object)
array(['Besana', 'Maria Ilaria', ''], dtype=object)
array(['Garcia', 'Oscar Blanco', ''], dtype=object)
array(['Boscolo', 'Manuela', ''], dtype=object)
array(['Boutin', 'David', ''], dtype=object)
array(['Buffat', 'Xavier', ''], dtype=object)
array(['Burkhardt', 'Helmut', ''], dtype=object)
array(['Cerutti', 'Francesco', ''], dtype=object)
array(['Chance', 'Antoine', ''], dtype=object)
array(['Collamati', 'Francesco', ''], dtype=object)
array(['Cruz-Alaniz', 'Emilia', ''], dtype=object)
array(['Dalena', 'Barbara', ''], dtype=object)
array(['Hofer', 'Michael', ''], dtype=object)
array(['Humann', 'Barbara L.', ''], dtype=object)
array(['Infantino', 'Angelo', ''], dtype=object)
array(['Keintzel', 'Jacqueline', ''], dtype=object)
array(['Langner', 'Andy', ''], dtype=object)
array(['Luckhof', 'Marian', ''], dtype=object)
array(['Martin', 'Roman', ''], dtype=object)
array(['Pieloni', 'Tatiana', ''], dtype=object)
array(['Rafique', 'Haroon', ''], dtype=object)
array(['Riegler', 'Werner', ''], dtype=object)
array(['Van Riesen-Haupt', 'Leon', ''], dtype=object)
array(['Schulte', 'Daniel', ''], dtype=object)
array(['Seryi', 'Andrei', ''], dtype=object)
array(['Tambasco', 'Claudia', ''], dtype=object)
array(['Tomas', 'Rogelio', ''], dtype=object)
array(['Zimmermann', 'Frank', ''], dtype=object)] |
324 | 1309.1937 | Takayuki Kihara | Kojiro Higuchi and Takayuki Kihara | Inside the Muchnik Degrees II: The Degree Structures induced by the
Arithmetical Hierarchy of Countably Continuous Functions | null | null | null | null | math.LO cs.LO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is known that infinitely many Medvedev degrees exist inside the Muchnik
degree of any nontrivial $\Pi^0_1$ subset of Cantor space. We shed light on the
fine structures inside these Muchnik degrees related to learnability and
piecewise computability. As for nonempty $\Pi^0_1$ subsets of Cantor space, we
show the existence of a finite-$\Delta^0_2$-piecewise degree containing
infinitely many finite-$(\Pi^0_1)_2$-piecewise degrees, and a
finite-$(\Pi^0_2)_2$-piecewise degree containing infinitely many
finite-$\Delta^0_2$-piecewise degrees (where $(\Pi^0_n)_2$ denotes the
difference of two $\Pi^0_n$ sets), whereas the greatest degrees in these three
"finite-$\Gamma$-piecewise" degree structures coincide. Moreover, as for
nonempty $\Pi^0_1$ subsets of Cantor space, we also show that every nonzero
finite-$(\Pi^0_1)_2$-piecewise degree includes infinitely many Medvedev (i.e.,
one-piecewise) degrees, every nonzero countable-$\Delta^0_2$-piecewise degree
includes infinitely many finite-piecewise degrees, every nonzero
finite-$(\Pi^0_2)_2$-countable-$\Delta^0_2$-piecewise degree includes
infinitely many countable-$\Delta^0_2$-piecewise degrees, and every nonzero
Muchnik (i.e., countable-$\Pi^0_2$-piecewise) degree includes infinitely many
finite-$(\Pi^0_2)_2$-countable-$\Delta^0_2$-piecewise degrees. Indeed, we show
that any nonzero Medvedev degree and nonzero countable-$\Delta^0_2$-piecewise
degree of a nonempty $\Pi^0_1$ subset of Cantor space have the strong
anticupping properties. Finally, we obtain an elementary difference between the
Medvedev (Muchnik) degree structure and the finite-$\Gamma$-piecewise degree
structure of all subsets of Baire space by showing that none of the
finite-$\Gamma$-piecewise structures are Brouwerian, where $\Gamma$ is any of
the Wadge classes mentioned above.
| [{'version': 'v1', 'created': 'Sun, 8 Sep 2013 08:01:40 GMT'}] | 2013-09-10 | [array(['Higuchi', 'Kojiro', ''], dtype=object)
array(['Kihara', 'Takayuki', ''], dtype=object)] |
325 | 1502.00305 | Vitor de Souza | C. J. Todero Peixoto and Vitor de Souza and Peter L. Biermann | Cosmic rays: the spectrum and chemical composition from $10^{10}$ to
$10^{20}$ eV | null | null | 10.1088/1475-7516/2015/07/042 | null | astro-ph.HE | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The production of energetic particles in the universe remains one of the
great mysteries of modern science. The mechanisms of acceleration in
astrophysical sources and the details about the propagation through the
galactic and extragalactic media are still to be defined. In recent years, the
cosmic ray flux has been measured with high precision in the energy range from
\energy{10} to \energyEV{20.5} by several experiments using different
techniques. In some energy ranges, it has been possible to determine the flux
of individual elements (hydrogen to iron nuclei). This paper explores an
astrophysical scenario in which only our Galaxy and the radio galaxy Cen A
produce all particles measured on Earth in the energy range from \energy{10} to
\energyEV{20.5}. Data from AMS-02, CREAM, KASCADE, KASCADE-Grande and the
Pierre Auger Observatories are considered. The model developed here is able to
describe the total and individual particle flux of all experiments considered.
It is shown that the theory used here is able to describe the smooth transition
from space-based to ground-based measurements. The flux of each element as
determined by KASCADE and KASCADE-Grande and the mass sensitivity parameter
\xmax measured by the Pierre Auger Observatory above \energyEV{18} are also
explored within the framework of the model. The transition from \energy{16} to
\energyEV{18} is carefully analyzed. It is shown that the data measured in this
energy range suggest the existence of an extra component of cosmic rays yet to
be understood.
| [{'version': 'v1', 'created': 'Sun, 1 Feb 2015 20:31:53 GMT'}] | 2015-08-06 | [array(['Peixoto', 'C. J. Todero', ''], dtype=object)
array(['de Souza', 'Vitor', ''], dtype=object)
array(['Biermann', 'Peter L.', ''], dtype=object)] |
326 | 1702.06706 | Jonas Fransson | J. Fransson and R. Somphonsane and H. Ramamoorthy and G. He and J. P.
Bird | Voltage-induced suppression of weak localization in graphene | Content contained in the theory section of arXiv:1802.09922 | null | null | null | cond-mat.mes-hall cond-mat.dis-nn cond-mat.mtrl-sci | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this theoretical study, we explore the manner in which the quantum
correction due to weak localization is suppressed in weakly-disordered
graphene, when it is subjected to the application of a non-zero voltage. Using
a nonequilibrium Green function approach, we address the scattering generated
by the disorder up to the level of the maximally crossed diagrams, hereby
capturing the interference among different, impurity-defined, Feynman paths.
Our calculations of the charge current, and of the resulting differential
conductance, reveal the logarithmic divergence typical of weak localization in
linear transport. The main finding of our work is that the applied voltage
suppresses the weak localization contribution in graphene, by introducing a
dephasing time that decreases inversely with increasing voltage.
| [{'version': 'v1', 'created': 'Wed, 22 Feb 2017 08:49:18 GMT'}
{'version': 'v2', 'created': 'Wed, 28 Feb 2018 07:04:30 GMT'}] | 2018-03-01 | [array(['Fransson', 'J.', ''], dtype=object)
array(['Somphonsane', 'R.', ''], dtype=object)
array(['Ramamoorthy', 'H.', ''], dtype=object)
array(['He', 'G.', ''], dtype=object)
array(['Bird', 'J. P.', ''], dtype=object)] |
327 | 1005.0557 | Sven Bjarke Gudnason | Sven Bjarke Gudnason | Fractional and semi-local non-Abelian Chern-Simons vortices | LaTeX, 38 pages, 16 figures. | Nucl.Phys.B840:160-185,2010 | 10.1016/j.nuclphysb.2010.07.004 | IFUP-TH/2010-15 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we study fractional as well as semi-local Chern-Simons vortices
in G = U(1) x SO(2M) and G = U(1) x USp(2M) theories. The master equations are
solved numerically using appropriate Ansatze for the moduli matrix field. In
the fractional case the vortices are solved in the transverse plane due to the
broken axial symmetry of the configurations (i.e. they are non-rotational
invariant). It is shown that unless the fractional vortex-centers are all
coincident (i.e. local case) the ring-like flux structure, characteristic of
Chern-Simons vortices, will become bell-like fluxes - just as those of the
standard Yang-Mills vortices. The asymptotic profile functions are calculated
in all cases and the effective size is identified.
| [{'version': 'v1', 'created': 'Tue, 4 May 2010 15:29:49 GMT'}] | 2010-08-17 | [array(['Gudnason', 'Sven Bjarke', ''], dtype=object)] |
328 | 1401.8191 | Yury F. Pirogov | Yu. F. Pirogov | Scalar graviton as dark matter | 6 pages. Report presented at the Intern. Session-Conference of SNP
DFS RAS "Physics of Fundamental Interactions", Protvino, 5-8 November 2013 | Phys. Atom. Nucl. 78, 528 (2015) | null | null | gr-qc astro-ph.CO hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the report, the theory of unimodular bimode gravity built on principles of
unimodular gauge invariance/relativity and general covariance is exposed.
Besides the massless tensor graviton of General Relativity, the theory includes
an (almost) massless scalar graviton treated as the gravitational dark matter.
A spherically symmetric vacuum solution, describing the coherent
scalar-graviton field for the soft-core dark halos with the asymptotically flat
rotation curves, is demonstrated.
| [{'version': 'v1', 'created': 'Fri, 31 Jan 2014 15:14:41 GMT'}] | 2020-01-01 | [array(['Pirogov', 'Yu. F.', ''], dtype=object)] |
329 | 1905.02760 | Christian Weiss | Christian Wei{\ss}, Thomas Skill | Sequences with almost Poissonian Pair Correlations | null | null | null | null | math.NT math.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Although a generic uniformly distributed sequence has Poissonian pair
correlations, only one explicit example has been found up to now. Additionally,
it is even known that many classes of uniformly distributed sequences, like van
der Corput sequences, Kronecker sequences and LS sequences, do not have
Poissonian pair correlations. In this paper, we show that van der Corput
sequences and the Kronecker sequence for the golden mean are as close to having
Poissonian pair correlations as possible: they both have $\alpha$-pair
correlations for all $0 < \alpha < 1$ but not for $\alpha = 1$ which
corresponds to Poissonian pair correlations.
| [{'version': 'v1', 'created': 'Tue, 7 May 2019 18:30:50 GMT'}
{'version': 'v2', 'created': 'Mon, 8 Feb 2021 12:02:13 GMT'}] | 2021-02-09 | [array(['Weiß', 'Christian', ''], dtype=object)
array(['Skill', 'Thomas', ''], dtype=object)] |
330 | 2110.15223 | Heiner Olbermann | Heiner Olbermann | Godunov variables and convex entropy for relativistic fluid dynamics
with bulk viscosity | 10 pages, v2: introduction modified, references added | null | 10.1063/5.0077711 | null | math.AP nucl-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Based on the conservation-dissipation formalism proposed by Zhu and
collaborators we formulate a general version of the Israel-Stewart theory for
relativistic fluid dynamics with bulk viscosity. Our generalization consists in
allowing for a wide range of dependence of the entropy density on the bulk
viscosity. We show the existence of Godunov-Boillat variables for this model.
By known properties of systems possessing such variables, this provides an
alternative proof of the recently established existence of solutions for the
Israel-Stewart theory locally in time, and a proof that entropy production is
positive across weak Lax shocks.
| [{'version': 'v1', 'created': 'Thu, 28 Oct 2021 15:35:41 GMT'}
{'version': 'v2', 'created': 'Tue, 8 Feb 2022 11:51:25 GMT'}] | 2022-03-14 | [array(['Olbermann', 'Heiner', ''], dtype=object)] |
331 | 1712.00958 | Shilei Li | Shilei Li, Rongzhen Jiao, and Li Yu | Femtosecond pulse with THz repetition frequency based on strong coupling
between quantum emitters and a plasmonic resonator | null | Phys. Rev. A 97, 033811 (2018) | 10.1103/PhysRevA.97.033811 | null | physics.optics | http://creativecommons.org/licenses/by-nc-sa/4.0/ | Nanoscale pulsed light is highly desirable in nano-integrated optics. In this
letter, we obtained femtosecond pulses with THz repetition frequency via the
strong coupling between quantum emitters (QEs) and plasmonic resonators. Our
structure consists of a V-groove (VG) plasmonic resonator and a nanowire
embedded with two-level QEs. The influences of the incident light intensity and
QE number density on the transmission response for this hybrid system are
investigated through semi-classical theory and simulation. It is found that the
transmission response can be modulated to the pulse form. The reason is the
strong coupling causes the output power of nanowire to behave as an oscillating
form, the oscillating output power in turn causes the field amplitude in the
resonator to oscillate over time. A feedback system is formed between the
plasmonic resonator and the QEs in nanowire. This provides a new method for
generating narrow pulsed lasers with ultrahigh repetition frequency in
plasmonic systems using a continous wave input, which has potential
applications in generating optical clock signals at the nanoscale.
| [{'version': 'v1', 'created': 'Mon, 4 Dec 2017 08:57:44 GMT'}
{'version': 'v2', 'created': 'Tue, 5 Dec 2017 01:28:13 GMT'}
{'version': 'v3', 'created': 'Mon, 11 Dec 2017 13:50:03 GMT'}] | 2018-03-14 | [array(['Li', 'Shilei', ''], dtype=object)
array(['Jiao', 'Rongzhen', ''], dtype=object)
array(['Yu', 'Li', ''], dtype=object)] |
332 | math/0701452 | Lars Andersson | Lars Andersson (UM and AEI), Thierry Barbot (UMPA-ENSL), Francois
Beguin (LM-Orsay), Abdelghani Zeghib (UMPA-ENSL) | Cosmological time versus CMC time II: the de Sitter and anti-de Sitter
cases | 45 pages | null | null | AEI-2007-001 | math.DG | null | This paper continues the investigation of constant mean curvature (CMC) time
functions in maximal globally hyperbolic spatially compact spacetimes of
constant sectional curvature, which was started in math.DG/0604486. In that
paper, the case of flat spacetimes was considered, and in the present paper,
the remaining cases of negative curvature (i.e. anti-de Sitter) spacetimes and
postitive curvature (i.e. de Sitter) spacetimes is dealt with. As in the flat
case, the existence of CMC time functions is obtained by using the level sets
of the cosmological time function as barriers. A major part of the work
consists of proving the required curvature estimates for these level sets.
The nonzero curvature case presents significant new difficulties, in part due
to the fact that the topological structure of nonzero constant curvature
spacetimes is much richer than that of the flat spacetimes. Further, the
timelike convergence condition fails for de Sitter spacetimes, and hence
uniqueness for CMC hypersurfaces fails in general. We characterize those de
Sitter spacetimes which admit CMC time functions (which are automatically
unique), as well as those which admit CMC foliations but no CMC time function.
| [{'version': 'v1', 'created': 'Tue, 16 Jan 2007 16:29:16 GMT'}] | 2007-05-23 | [array(['Andersson', 'Lars', '', 'UM and AEI'], dtype=object)
array(['Barbot', 'Thierry', '', 'UMPA-ENSL'], dtype=object)
array(['Beguin', 'Francois', '', 'LM-Orsay'], dtype=object)
array(['Zeghib', 'Abdelghani', '', 'UMPA-ENSL'], dtype=object)] |
333 | 1507.04006 | Huanian Zhang | Tao Han (Pittsburgh U. and Tsinghua U.), Shufang Su (Arizona U. and
Tsinghua U.), Yongcheng Wu (Tsinghua U.), Bin Zhang (Tsinghua U.), Huanian
Zhang (Arizona U.) | Sbottom discovery via mixed decays at the LHC | 26 pages and 7 figures | Phys. Rev. D 92, 115009 (2015) | 10.1103/PhysRevD.92.115009 | null | hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the search for bottom squark (sbottom) in SUSY at the LHC, the common
practice has been to assume a $100\%$ decay branching fraction for a given
search channel. In realistic MSSM scenarios, there are often more than one
significant decay modes to be present, which significantly weaken the current
sbottom search limits at the LHC. On the other hand, the combination of the
multiple decay modes offers alternative discovery channels for sbottom
searches. In this paper, we present the sbottom decays in a few representative
mass parameter scenarios. We then analyze the sbottom signal for the pair
production in QCD with one sbottom decaying via $\tilde{b}\rightarrow b
\chi_1^0,\ b \chi_2^0$, and the other one decaying via $\tilde{b} \rightarrow t
\chi_1^\pm$. With the gaugino subsequent decaying to gauge bosons or a Higgs
boson $\chi_2^0 \rightarrow Z \chi_1^0,\ h \chi_1^0$ and $\chi_1^\pm
\rightarrow W^\pm \chi_1^0$, we study the reach of those signals at the 14 TeV
LHC with 300 ${\rm fb^{-1}}$ integrated luminosity. For a left-handed bottom
squark, we find that a mass up to 920 GeV can be discovered at 5$\sigma$
significance for 250 GeV $< m_{\chi_1^0} <$ 350 GeV, or excluded up to 1050 GeV
at the 95\% confidence level for the $h$ channel ($\mu>0$); similarly, it can
be discovered up to 840 GeV, or excluded up to 900 GeV at the 95\% confidence
level for the $Z$ channel ($\mu<0$). The sbottom and stop signals in the same
SUSY parameter scenario are combined to obtain the optimal sensitivity, which
is about 150 GeV better than the individual reach of the sbottom or stop. For a
right-handed bottom squark with $\tilde{b} \tilde{b}^* \rightarrow b \chi_1^0,\
t \chi_1^\pm$ channel, we find that the sbottom mass up to 880 GeV can be
discovered at 5$\sigma$ significance, or excluded up to 1060 GeV at the 95\%
confidence level.
| [{'version': 'v1', 'created': 'Tue, 14 Jul 2015 20:05:51 GMT'}
{'version': 'v2', 'created': 'Wed, 2 Nov 2016 17:21:45 GMT'}
{'version': 'v3', 'created': 'Thu, 3 Nov 2016 00:56:49 GMT'}] | 2016-11-04 | [array(['Han', 'Tao', '', 'Pittsburgh U. and Tsinghua U.'], dtype=object)
array(['Su', 'Shufang', '', 'Arizona U. and\n Tsinghua U.'], dtype=object)
array(['Wu', 'Yongcheng', '', 'Tsinghua U.'], dtype=object)
array(['Zhang', 'Bin', '', 'Tsinghua U.'], dtype=object)
array(['Zhang', 'Huanian', '', 'Arizona U.'], dtype=object)] |
334 | 1206.3606 | Daniel A. Lidar | G.A. Paz-Silva and D. A. Lidar | Optimally combining dynamical decoupling and quantum error correction | 6 pages, 1 figure | Scientific Reports 3, 1530 (2013) | 10.1038/srep01530 | null | quant-ph cond-mat.other | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show how dynamical decoupling (DD) and quantum error correction (QEC) can
be optimally combined in the setting of fault tolerant quantum computing. To
this end we identify the optimal generator set of DD sequences designed to
protect quantum information encoded into stabilizer subspace or subsystem
codes. This generator set, comprising the stabilizers and logical operators of
the code, minimizes a natural cost function associated with the length of DD
sequences. We prove that with the optimal generator set the restrictive
local-bath assumption used in earlier work on hybrid DD-QEC schemes, can be
significantly relaxed, thus bringing hybrid DD-QEC schemes, and their
potentially considerable advantages, closer to realization.
| [{'version': 'v1', 'created': 'Fri, 15 Jun 2012 23:12:57 GMT'}] | 2014-02-25 | [array(['Paz-Silva', 'G. A.', ''], dtype=object)
array(['Lidar', 'D. A.', ''], dtype=object)] |
335 | 2012.01214 | Emidio Gabrielli | Marco Fabbrichesi and Emidio Gabrielli | Searching for the dark sector in two-body anti-muon decay with the
polarization of monochromatic positrons | 7 pages, 4 figures. Same as published version, new results included,
a few typos corrected | Phys. Rev. D 104, 015039 (2021) | 10.1103/PhysRevD.104.015039 | null | hep-ph hep-ex | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The $\mu^+ \to e^+ X$ decay, where $X$ is a dark sector boson, provides one
of the strongest available bounds on the scale of dark sector interactions. The
$X$ boson can be an axion or a dark photon. We show that the concurrent
determination of the anti-muon and positron polarizations makes possible to
distinguish with a confidence level of 99% between the two dark sector portals
with as few as 6 observed events in the case of the massless dark photon.
Instead, the massive spin-1, dimension 4 dark portal cannot be distinguished
from the axion-like case. We also discuss the possibility that the $X$ boson be
a massive spin-2 particle.
| [{'version': 'v1', 'created': 'Wed, 2 Dec 2020 13:55:34 GMT'}
{'version': 'v2', 'created': 'Wed, 22 Sep 2021 18:26:27 GMT'}] | 2021-09-24 | [array(['Fabbrichesi', 'Marco', ''], dtype=object)
array(['Gabrielli', 'Emidio', ''], dtype=object)] |
336 | math/9509222 | null | Paul G. A. Floris, Erik Koelink | A commuting q-analogue of the addition formula for disk polynomials | null | null | null | OP-SF 19 Sep 1995 | math.QA math.CA | null | Starting from the addition formula for $q$-disk polynomials, which is an
identity in non-commuting variables, we establish a basic analogue in commuting
variables of the addition and product formula for disk polynomials. These
contain as limiting cases the addition and product formula for little
$q$-Legendre polynomials. As $q$ tends to $1$ the addition and product formula
for disk polynomials are recovered.
| [{'version': 'v1', 'created': 'Tue, 19 Sep 1995 00:00:00 GMT'}] | 2016-09-06 | [array(['Floris', 'Paul G. A.', ''], dtype=object)
array(['Koelink', 'Erik', ''], dtype=object)] |
337 | 1206.6196 | Pierre-Francois Marteau | Pierre-Fran\c{c}ois Marteau (IRISA), Nicolas Bonnel (IRISA), Gilbas
M\'enier (IRISA) | Discrete Elastic Inner Vector Spaces with Application in Time Series and
Sequence Mining | arXiv admin note: substantial text overlap with arXiv:1101.4318 | IEEE Transactions on Knowledge and Data Engineering (2012) pp 1-14 | 10.1109/TKDE.2012.131 | null | cs.LG cs.DB | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This paper proposes a framework dedicated to the construction of what we call
discrete elastic inner product allowing one to embed sets of non-uniformly
sampled multivariate time series or sequences of varying lengths into inner
product space structures. This framework is based on a recursive definition
that covers the case of multiple embedded time elastic dimensions. We prove
that such inner products exist in our general framework and show how a simple
instance of this inner product class operates on some prospective applications,
while generalizing the Euclidean inner product. Classification experimentations
on time series and symbolic sequences datasets demonstrate the benefits that we
can expect by embedding time series or sequences into elastic inner spaces
rather than into classical Euclidean spaces. These experiments show good
accuracy when compared to the euclidean distance or even dynamic programming
algorithms while maintaining a linear algorithmic complexity at exploitation
stage, although a quadratic indexing phase beforehand is required.
| [{'version': 'v1', 'created': 'Wed, 27 Jun 2012 07:44:15 GMT'}] | 2012-06-28 | [array(['Marteau', 'Pierre-François', '', 'IRISA'], dtype=object)
array(['Bonnel', 'Nicolas', '', 'IRISA'], dtype=object)
array(['Ménier', 'Gilbas', '', 'IRISA'], dtype=object)] |
338 | 1805.01173 | Sandra Korte-Kerzel | Sebastian Schr\"oders, Stefanie Sandl\"obes, Carola Birke, Matthias
Loeck, Lars Peters, Christophe Tromas, Sandra Korte-Kerzel | Room temperature deformation in the Fe$_7$Mo$_6$ $\mu$-Phase | Accepted manuscript in International Journal of Plasticity | International Journal of Plasticity, Volume 108, September 2018,
Pages 125-143 | 10.1016/j.ijplas.2018.05.002 | null | cond-mat.mtrl-sci | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The role of TCP phases in deformation of superalloys and steels is still not
fully resolved. In particular, the intrinsic deformation mechanisms of these
phases are largely unknown including the active slip systems in most of these
complex crystal structures. Here, we present a first detailed investigation of
the mechanical properties of the Fe7Mo6 {\mu}-phase at room temperature using
microcompression and nanoindentation with statistical EBSD-assisted slip trace
analysis and TEM imaging. Slip occurs predominantly on the basal and prismatic
planes, resulting also in decohesion on prismatic planes with high defect
density. The correlation of the deformation structures and measured hardness
reveals pronounced hardening where interaction of slip planes occurs and
prevalent deformation at pre-existing defects.
| [{'version': 'v1', 'created': 'Thu, 3 May 2018 08:57:16 GMT'}
{'version': 'v2', 'created': 'Thu, 9 Aug 2018 14:23:48 GMT'}
{'version': 'v3', 'created': 'Fri, 10 Aug 2018 07:56:36 GMT'}] | 2018-08-13 | [array(['Schröders', 'Sebastian', ''], dtype=object)
array(['Sandlöbes', 'Stefanie', ''], dtype=object)
array(['Birke', 'Carola', ''], dtype=object)
array(['Loeck', 'Matthias', ''], dtype=object)
array(['Peters', 'Lars', ''], dtype=object)
array(['Tromas', 'Christophe', ''], dtype=object)
array(['Korte-Kerzel', 'Sandra', ''], dtype=object)] |
339 | 1703.06507 | Liang-Wen Pi | Andrew Vikartofsky, Liang-Wen Pi, Anthony F. Starace | Discontinuities in the Electromagnetic Fields of Vortex Beams in the
Complex Source/Sink Model | 10 pages, 4 figures | Phys. Rev. A 95, 053826 (2017) | 10.1103/PhysRevA.95.053826 | null | physics.optics physics.plasm-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | An analytical discontinuity is reported in what was thought to be the
discontinuity-free exact nonparaxial vortex beam phasor obtained within the
complex source/sink model. This discontinuity appears for all odd values of the
orbital angular momentum mode. Such discontinuities in the phasor lead to
nonphysical discontinuities in the real electromagnetic field components. We
identify the source of the discontinuities, and provide graphical evidence of
the discontinuous real electric fields for the first and third orbital angular
momentum modes. A simple means of avoiding these discontinuities is presented.
| [{'version': 'v1', 'created': 'Sun, 19 Mar 2017 20:25:12 GMT'}] | 2017-05-17 | [array(['Vikartofsky', 'Andrew', ''], dtype=object)
array(['Pi', 'Liang-Wen', ''], dtype=object)
array(['Starace', 'Anthony F.', ''], dtype=object)] |
340 | 1806.00101 | Akash Srivastava | Akash Srivastava, Kai Xu, Michael U. Gutmann and Charles Sutton | Generative Ratio Matching Networks | ICLR 2020; Code: https://github.com/GRAM-nets | null | null | null | stat.ML cs.LG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Deep generative models can learn to generate realistic-looking images, but
many of the most effective methods are adversarial and involve a saddlepoint
optimization, which requires a careful balancing of training between a
generator network and a critic network. Maximum mean discrepancy networks
(MMD-nets) avoid this issue by using kernel as a fixed adversary, but
unfortunately, they have not on their own been able to match the generative
quality of adversarial training. In this work, we take their insight of using
kernels as fixed adversaries further and present a novel method for training
deep generative models that does not involve saddlepoint optimization. We call
our method generative ratio matching or GRAM for short. In GRAM, the generator
and the critic networks do not play a zero-sum game against each other,
instead, they do so against a fixed kernel. Thus GRAM networks are not only
stable to train like MMD-nets but they also match and beat the generative
quality of adversarially trained generative networks.
| [{'version': 'v1', 'created': 'Thu, 31 May 2018 21:06:03 GMT'}
{'version': 'v2', 'created': 'Sat, 1 Jun 2019 23:48:13 GMT'}
{'version': 'v3', 'created': 'Sat, 15 Feb 2020 02:06:36 GMT'}] | 2020-02-18 | [array(['Srivastava', 'Akash', ''], dtype=object)
array(['Xu', 'Kai', ''], dtype=object)
array(['Gutmann', 'Michael U.', ''], dtype=object)
array(['Sutton', 'Charles', ''], dtype=object)] |
341 | 2001.05122 | Tao Xin | Tao Xin, Yishan Li, Yu-ang Fan, Xuanran Zhu, Yingjie Zhang, Xinfang
Nie, Jun Li, Qihang Liu, and Dawei Lu | Experimental Detection of the Quantum Phases of a Three-Dimensional
Topological Insulator on a Spin Quantum Simulator | 6 pages for main text+ 5 pages for supplementary information | Phys. Rev. Lett. 125, 090502 (2020) | 10.1103/PhysRevLett.125.090502 | null | quant-ph cond-mat.mes-hall | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The detection of topological phases of matter becomes a central issue in
recent years. Conventionally, the realization of a specific topological phase
in condensed matter physics relies on probing the underlying surface band
dispersion or quantum transport signature of a real material, which may be
imperfect or even absent. On the other hand, quantum simulation offers an
alternative approach to directly measure the topological invariant on a
universal quantum computer. However, experimentally demonstrating
high-dimensional topological phases remains a challenge due to the technical
limitations of current experimental platforms. Here, we investigate the
three-dimensional topological insulators in the AIII (chiral unitary) symmetry
class which yet lack experimental realization. Using the nuclear magnetic
resonance system, we experimentally demonstrate their topological properties,
where a dynamical quenching approach is adopted and the dynamical bulk-boundary
correspondence in the momentum space is observed. As a result, the topological
invariants are measured with high precision on the band-inversion surface,
exhibiting robustness to the decoherence effect. Our work paves the way towards
the quantum simulation of topological phases of matter in higher dimensions and
more complex systems through controllable quantum phases transitions.
| [{'version': 'v1', 'created': 'Wed, 15 Jan 2020 03:51:48 GMT'}] | 2020-09-02 | [array(['Xin', 'Tao', ''], dtype=object)
array(['Li', 'Yishan', ''], dtype=object)
array(['Fan', 'Yu-ang', ''], dtype=object)
array(['Zhu', 'Xuanran', ''], dtype=object)
array(['Zhang', 'Yingjie', ''], dtype=object)
array(['Nie', 'Xinfang', ''], dtype=object)
array(['Li', 'Jun', ''], dtype=object)
array(['Liu', 'Qihang', ''], dtype=object)
array(['Lu', 'Dawei', ''], dtype=object)] |
342 | 1302.3216 | Anthony Clark | Anthony J. Clark, Jay McCarty, Ivan Y. Lyubimov, and Marina G. Guenza | Thermodynamic consistency in variable-level coarse-graining of polymeric
liquids | null | A. J. Clark, J. McCarty, I. Y. Lyubimov, and M. G. Guenza, Phys.
Rev. Lett. 109, 168301 (2012) | 10.1103/PhysRevLett.109.168301 | null | cond-mat.soft | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Numerically optimized reduced descriptions of macromolecular liquids often
present thermodynamic inconsistency with atomistic level descriptions even if
the total correlation function, i.e. the structure, appears to be in agreement.
An analytical expression for the effective potential between a pair of
coarse-grained units is derived starting from the first-principles
Ornstein-Zernike equation, for a polymer liquid where each chain is represented
as a collection of interpenetrating blobs, with a variable number of blobs,
$n_b$, of size $N_b$. The potential is characterized by a long tail, slowly
decaying with characteristic scaling exponent of $N_b^{1/4}$. This general
result applies to any coarse-grained model of polymer melts with units larger
than the persistence length, highlighting the importance of the long,
repulsive, potential tail for the model to correctly predict both structural
and thermodynamic properties of the macromolecular liquid.
| [{'version': 'v1', 'created': 'Wed, 13 Feb 2013 20:55:26 GMT'}] | 2013-02-14 | [array(['Clark', 'Anthony J.', ''], dtype=object)
array(['McCarty', 'Jay', ''], dtype=object)
array(['Lyubimov', 'Ivan Y.', ''], dtype=object)
array(['Guenza', 'Marina G.', ''], dtype=object)] |
343 | 1705.04801 | Erik Slivken | Samuel Miner and Douglas Rizzolo and Erik Slivken | Asymptotic distribution of fixed points of pattern-avoiding involutions | 16 pages | Discrete Mathematics & Theoretical Computer Science, Vol. 19 no.
2, Permutation Patterns 2016, Permutation Patterns (December 11, 2017)
dmtcs:3658 | 10.23638/DMTCS-19-2-5 | null | math.CO math.PR | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | For a variety of pattern-avoiding classes, we describe the limiting
distribution for the number of fixed points for involutions chosen uniformly at
random from that class. In particular we consider monotone patterns of
arbitrary length as well as all patterns of length 3. For monotone patterns we
utilize the connection with standard Young tableaux with at most $k$ rows and
involutions avoiding a monotone pattern of length $k$. For every pattern of
length 3 we give the bivariate generating function with respect to fixed points
for the involutions that avoid that pattern, and where applicable apply tools
from analytic combinatorics to extract information about the limiting
distribution from the generating function. Many well-known distributions
appear.
| [{'version': 'v1', 'created': 'Sat, 13 May 2017 08:53:56 GMT'}
{'version': 'v2', 'created': 'Sun, 26 Nov 2017 11:54:37 GMT'}
{'version': 'v3', 'created': 'Fri, 8 Dec 2017 15:52:18 GMT'}] | 2023-06-22 | [array(['Miner', 'Samuel', ''], dtype=object)
array(['Rizzolo', 'Douglas', ''], dtype=object)
array(['Slivken', 'Erik', ''], dtype=object)] |
344 | 1502.05636 | Maxence Lepers | R. Vexiau (LAC), M. Lepers (LAC), M. Aymar (LAC), N. Bouloufa-Maafa
(LAC), O. Dulieu (LAC) | Long-range interactions between polar bialkali ground-state molecules in
arbitrary vibrational levels | null | null | null | null | physics.atom-ph quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We have calculated the isotropic $C\_6$ coefficients characterizing the
long-range van der Waals interaction between two identical heteronuclear
alkali-metal diatomic molecules in the same arbitrary vibrational level of
their ground electronic state $X^1\Sigma^+$. We consider the ten species made
up of $^7$Li, $^{23}$Na, $^{39}$K, $^{87}$Rb and $^{133}$Cs. Following our
previous work [M.~Lepers \textit{et.~al.}, Phys.~Rev.~A \textbf{88}, 032709
(2013)] we use the sum-over-state formula inherent to the second-order
perturbation theory, composed of the contributions from the transitions within
the ground state levels, from the transition between ground-state and excited
state levels, and from a crossed term. These calculations involve a combination
of experimental and quantum-chemical data for potential energy curves and
transition dipole moments. We also investigate the case where the two molecules
are in different vibrational levels and we show that the Moelwyn-Hughes
approximation is valid provided that it is applied for each of the three
contributions to the sum-over-state formula. Our results are particularly
relevant in the context of inelastic and reactive collisions between ultracold
bialkali molecules, in deeply bound or in Feshbach levels.
| [{'version': 'v1', 'created': 'Thu, 19 Feb 2015 17:23:28 GMT'}] | 2015-02-20 | [array(['Vexiau', 'R.', '', 'LAC'], dtype=object)
array(['Lepers', 'M.', '', 'LAC'], dtype=object)
array(['Aymar', 'M.', '', 'LAC'], dtype=object)
array(['Bouloufa-Maafa', 'N.', '', 'LAC'], dtype=object)
array(['Dulieu', 'O.', '', 'LAC'], dtype=object)] |
345 | 1006.2596 | Kenji Fukushima | Kenji Fukushima | Phase diagram of hot and dense QCD constrained by the Statistical Model | 5 pages, 3 figures; all figures updated, results and conclusions not
modified | Phys.Lett.B695:387-391,2011 | 10.1016/j.physletb.2010.11.040 | YITP-10-46 | hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a prescription to constrain the chiral effective model approach to
the QCD phase diagram using the thermal Statistical Model, which is a
description consistent with the experimental data at the freeze-out. In the
transition region where thermal quantities of hadrons blow up, deconfined
quarks and gluons should smoothly take over the degrees of freedom from hadrons
in the Statistical Model. We use the Polyakov-loop coupled Nambu--Jona-Lasinio
(PNJL) model as an effective description in the quark side. We require that the
validity regions of these descriptions should have an overlap on the phase
diagram, which constrains model uncertainty. Our results favor a phase diagram
with the chiral phase transition located at slightly higher temperature than
deconfinement.
| [{'version': 'v1', 'created': 'Mon, 14 Jun 2010 04:27:17 GMT'}
{'version': 'v2', 'created': 'Wed, 30 Jun 2010 10:24:55 GMT'}] | 2011-06-27 | [array(['Fukushima', 'Kenji', ''], dtype=object)] |
346 | hep-ph/9711305 | Tord Riemann | Tord Riemann | The Z Boson Resonance and Radiative Corrections | 15 pages, Latex, Lecture given at XXI School of Theoretical Physics
of the University of Silesia, Katowice, 19-24 September 1997, Ustron, Poland | Acta Phys.Polon. B28 (1997) 2317-2332 | null | DESY 97-218 | hep-ph | null | The Z line shape is measured at LEP with an accuracy at the per mille level.
Usually it is described in the Standard Model of electroweak interactions with
account of quantum corrections. Alternatively, one may attempt different
model-independent approaches in order to extract quantities like mass and width
of the Z boson. If a fit deviates from that in the standard approach, this may
give hints for New Physics contributions. I describe two model-independent
approaches and compare their applications to LEP data with the Standard Model
approach.
| [{'version': 'v1', 'created': 'Wed, 12 Nov 1997 12:37:29 GMT'}] | 2007-05-23 | [array(['Riemann', 'Tord', ''], dtype=object)] |
347 | 1701.03467 | Dane Kleiner | Dane Kleiner, Kevin A. Pimbblet, D. Heath Jones, B\"arbel S.
Koribalski and Paolo Serra | Evidence for HI replenishment in massive galaxies through gas accretion
from the cosmic web | 20 pages, 13 figures. Accepted in MNRAS | null | 10.1093/mnras/stw3328 | null | astro-ph.GA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We examine the HI-to-stellar mass ratio (HI fraction) for galaxies near
filament backbones within the nearby Universe ($d <$ 181 Mpc). This work uses
the 6 degree Field Galaxy Survey and the Discrete Persistent Structures
Extractor to define the filamentary structure of the local cosmic web. HI
spectral stacking of HI Parkes all sky survey observations yields the HI
fraction for filament galaxies and a field control sample. The HI fraction is
measured for different stellar masses and fifth nearest neighbour projected
densities ($\Sigma_{5}$) to disentangle what influences cold gas in galaxies.
For galaxies with stellar masses log($M_{\star}$) $<$ 11 M$_{\odot}$ in
projected densities 0 $\leq$ $\Sigma_{5}$ $<$ 3 galaxies Mpc$^{-2}$, all HI
fractions of galaxies near filaments are statistically indistinguishable from
the control sample. Galaxies with stellar masses log($M_{\star}$) $\geq$ 11
M$_{\odot}$ have a systematically higher HI fraction near filaments than the
control sample. The greatest difference is 0.75 dex, which is 5.5$\sigma$
difference at mean projected densities of 1.45 galaxies Mpc$^{-2}$. We suggest
that this is evidence for massive galaxies accreting cold gas from the
intrafilament medium that can replenish some HI gas. This supports cold mode
accretion where filament galaxies with a large gravitational potential can draw
gas from the large-scale structure.
| [{'version': 'v1', 'created': 'Thu, 12 Jan 2017 19:00:13 GMT'}
{'version': 'v2', 'created': 'Wed, 25 Jan 2017 05:26:27 GMT'}] | 2017-01-26 | [array(['Kleiner', 'Dane', ''], dtype=object)
array(['Pimbblet', 'Kevin A.', ''], dtype=object)
array(['Jones', 'D. Heath', ''], dtype=object)
array(['Koribalski', 'Bärbel S.', ''], dtype=object)
array(['Serra', 'Paolo', ''], dtype=object)] |
348 | 2203.10648 | Zijia Cheng | Zi-Jia Cheng, Ilya Belopolski, Tyler A. Cochran, Hung-Ju Tien, Xian P.
Yang, Wenlong Ma, Jia-Xin Yin, Junyi Zhang, Chris Jozwiak, Aaron Bostwick,
Eli Rotenberg, Guangming Cheng, Md. Shafayat Hossain, Qi Zhang, Nana Shumiya,
Daniel Multer, Maksim Litskevich, Yuxiao Jiang, Nan Yao, Biao Lian, Guoqing
Chang, Shuang Jia, Tay-Rong Chang, M. Zahid Hasan | Magnetization-direction-tunable kagome Weyl line | 12 pages, 4 figures. Comments are welcome! | null | null | null | cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Kagome magnets provide a fascinating platform for a plethora of topological
quantum phenomena. Here, utilizing angle-resolved photoemission spectroscopy,
we demonstrate Weyl lines with strong out-of-plane dispersion in an A-A stacked
kagome magnet TbxGd1-xMn6Sn6. On the Gd rich side, the Weyl line remains nearly
spin-orbit-gapless due to a remarkable cooperative interplay between Kane-Mele
spin-orbit-coupling, low site symmetry and in-plane magnetic order. Under Tb
substitution, the kagome Weyl line gaps due to a magnetic reorientation to
out-of-plane order. Our results illustrate the magnetic moment direction as an
efficient tuning knob for realizing distinct three-dimensional topological
phases.
| [{'version': 'v1', 'created': 'Sun, 20 Mar 2022 21:07:22 GMT'}] | 2022-03-22 | [array(['Cheng', 'Zi-Jia', ''], dtype=object)
array(['Belopolski', 'Ilya', ''], dtype=object)
array(['Cochran', 'Tyler A.', ''], dtype=object)
array(['Tien', 'Hung-Ju', ''], dtype=object)
array(['Yang', 'Xian P.', ''], dtype=object)
array(['Ma', 'Wenlong', ''], dtype=object)
array(['Yin', 'Jia-Xin', ''], dtype=object)
array(['Zhang', 'Junyi', ''], dtype=object)
array(['Jozwiak', 'Chris', ''], dtype=object)
array(['Bostwick', 'Aaron', ''], dtype=object)
array(['Rotenberg', 'Eli', ''], dtype=object)
array(['Cheng', 'Guangming', ''], dtype=object)
array(['Hossain', 'Md. Shafayat', ''], dtype=object)
array(['Zhang', 'Qi', ''], dtype=object)
array(['Shumiya', 'Nana', ''], dtype=object)
array(['Multer', 'Daniel', ''], dtype=object)
array(['Litskevich', 'Maksim', ''], dtype=object)
array(['Jiang', 'Yuxiao', ''], dtype=object)
array(['Yao', 'Nan', ''], dtype=object)
array(['Lian', 'Biao', ''], dtype=object)
array(['Chang', 'Guoqing', ''], dtype=object)
array(['Jia', 'Shuang', ''], dtype=object)
array(['Chang', 'Tay-Rong', ''], dtype=object)
array(['Hasan', 'M. Zahid', ''], dtype=object)] |
349 | 2101.03432 | Thomas Kecker | Thomas Kecker and Galina Filipuk | Regularising Transformations for Complex Differential Equations with
Movable Algebraic Singularities | 27 pages | Math Phys Anal Geom 25, 9 (2022) | 10.1007/s11040-022-09417-6 | null | math.CA | http://creativecommons.org/licenses/by/4.0/ | In a 1979 paper, K. Okamoto introduced the space of initial values for the
six Painlev\'e equations and their associated Hamiltonian systems, showing that
these define regular initial value problems at every point of an augmented
phase space, a rational surface with certain exceptional divisors removed. We
show that the construction of the space of initial values remains meaningful
for certain classes of second-order complex differential equations, and more
generally, Hamiltonian systems, where all movable singularities of all their
solutions are algebraic poles (by some authors denoted the quasi-Painlev\'e
property), which is a generalisation of the Painlev\'e property. The difference
here is that the initial value problems obtained in the extended phase space
become regular only after an additional change of dependent and independent
variables. Constructing the analogue of space of initial values for these
equations in this way also serves as an algorithm to single out, from a given
class of equations or system of equations, those equations which are free from
movable logarithmic branch points.
| [{'version': 'v1', 'created': 'Sat, 9 Jan 2021 21:51:59 GMT'}
{'version': 'v2', 'created': 'Mon, 7 Feb 2022 14:54:26 GMT'}
{'version': 'v3', 'created': 'Mon, 28 Mar 2022 13:51:43 GMT'}
{'version': 'v4', 'created': 'Tue, 29 Mar 2022 09:02:48 GMT'}] | 2022-03-30 | [array(['Kecker', 'Thomas', ''], dtype=object)
array(['Filipuk', 'Galina', ''], dtype=object)] |
350 | astro-ph/0004143 | Dmitri Khokhlov | D.L. Khokhlov | Neutrino-antineutrino transition under CP-transformation and solar
neutrino puzzle | This paper has been withdrawn | null | null | null | astro-ph | null | This paper has been withdrawn by the author due to the presented idea is
wrong.
| [{'version': 'v1', 'created': 'Tue, 11 Apr 2000 14:52:38 GMT'}
{'version': 'v2', 'created': 'Fri, 5 Dec 2003 16:57:00 GMT'}] | 2007-05-23 | [array(['Khokhlov', 'D. L.', ''], dtype=object)] |
351 | 1808.06983 | Andr\'es E. Piatti | A.E. Piatti, N. Hwang, A.A. Cole, M.S. Angelo and B. Emptage | Accurate radial velocity and metallicity of the Large Magellanic Cloud
old globular clusters NGC 1928 and NGC 1939 | 10 pages, 9 figures. Accepted for publication in Monthly Notices of
the Royal Astronomical Society | null | 10.1093/mnras/sty2324 | null | astro-ph.GA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present results obtained from spectroscopic observations of red giants
located in the fields of the Large Magellanic Cloud (LMC) globular clusters
(GCs) NGC 1928 and NGC 1939. We used the GMOS and AAOmega+2dF spectrographs to
obtain spectra centred on the CaII triplet, from which we derived individual
radial velocities (RVs) and metallicities. From cluster members we derived mean
RVs of RV_NGC1928=249.58+-4.65 km/s and RV_NGC939=258.85+-2.08 km/s, and mean
metallicities of [Fe/H]_NGC1928=-1.30+-0.15 dex and [Fe/H]_NGC1939=-2.00+-0.15
dex. We found that both GCs have RVs and positions consistent with being part
of the LMC disc, so that we rule out any possible origin but that in the same
galaxy. By computing the best solution of a disc that fully contains each GC,
we obtained circular velocities for the 15 known LMC GCs. We found that 11/15
of the GCs share the LMC rotation derived from $HST$ and $Gaia$ DR2 proper
motions. This outcome reveals that the LMC disc existed since the very early
epoch of the galaxy formation and experienced the steep relatively fast
chemical enrichment shown by its GC metallicities. The four remaining GCs
turned out to have circular velocities not compatible with an in situ cluster
formation, but rather with being stripped from the SMC.
| [{'version': 'v1', 'created': 'Tue, 21 Aug 2018 16:02:51 GMT'}] | 2018-08-29 | [array(['Piatti', 'A. E.', ''], dtype=object)
array(['Hwang', 'N.', ''], dtype=object)
array(['Cole', 'A. A.', ''], dtype=object)
array(['Angelo', 'M. S.', ''], dtype=object)
array(['Emptage', 'B.', ''], dtype=object)] |
352 | 1306.6894 | Egger Daniel | D. J. Egger and F. K. Wilhelm | Optimized controlled Z gates for two superconducting qubits coupled
through a resonator | null | null | 10.1088/0953-2048/27/1/014001 | null | quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Superconducting qubits are a promising candidate for building a quantum
computer. A continued challenge for fast yet accurate gates to minimize the
effects of decoherence. Here we apply numerical methods to design fast
entangling gates, specifically the controlled Z, in an architecture where two
qubits are coupled via a resonator. We find that the gates can be sped up by a
factor of two and reach any target fidelity. We also discuss how systematic
errors arising from experimental conditions affect the pulses and how to remedy
them, providing a strategy for the experimental implementation of our results.
We discuss the shape of the pulses, their spectrum and symmetry.
| [{'version': 'v1', 'created': 'Fri, 28 Jun 2013 17:07:48 GMT'}] | 2015-06-16 | [array(['Egger', 'D. J.', ''], dtype=object)
array(['Wilhelm', 'F. K.', ''], dtype=object)] |
353 | 0903.2105 | Frederic Klopp | Fr\'ed\'eric Klopp (LAGA), Shu Nakamura | Lifshitz Tails for Generalized Alloy Type Random Schr\"odinger Operators | null | null | null | null | math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study Lifshitz tails for random Schr\"odinger operators where the random
potential is alloy type in the sense that the single site potentials are
independent, identically distributed, but they may have various function forms.
We suppose the single site potentials are distributed in a finite set of
functions, and we show that under suitable symmetry conditions, they have
Lifshitz tail at the bottom of the spectrum except for special cases. When the
single site potential is symmetric with respect to all the axes, we give a
necessary and sufficient condition for the existence of Lifshitz tails. As an
application, we show that certain random displacement models have Lifshitz
singularity at the bottom of the spectrum, and also complete the study of
continuous Anderson type models undertaken in arXiv : 0804.4079
| [{'version': 'v1', 'created': 'Thu, 12 Mar 2009 07:28:08 GMT'}
{'version': 'v2', 'created': 'Mon, 16 Mar 2009 05:33:27 GMT'}] | 2009-03-16 | [array(['Klopp', 'Frédéric', '', 'LAGA'], dtype=object)
array(['Nakamura', 'Shu', ''], dtype=object)] |
354 | astro-ph/0110292 | Angela Iovino | M. Massarotti (Oss. Astron. Capodimonte), A. Iovino (Oss. Astron.
Brera), A. Buzzoni (TNG, Oss. Astron. Brera), D. Valls--Gabaud (Obs.
Midi-Pyrenees) | New insights on the accuracy of photometric redshift measurements | 18 pages, 9 encapsulated postscript figures, LateX, accepted for
publication in A&A | null | 10.1051/0004-6361:20011409 | null | astro-ph | null | We use the deepest and most complete redshift catalog currently available
(the Hubble Deep Field (HDF) North supplemented by new HDF South redshift data)
to minimize residuals between photometric and spectroscopic redshift estimates.
The good agreement at z_spec < 1.5 shows that model libraries provide a good
description of the galaxy population. At z_spec > 2.0, the systematic shift
between photometric and spectroscopic redshifts decreases when the modeling of
the absorption by the interstellar and intergalactic media is refined. As a
result, in the entire redshift range 0 < z < 6, residuals between photometric
and spectroscopic redshifts are roughly halved. For objects fainter than the
spectroscopic limit, the main source of uncertainty in photometric redshifts is
related to photometric errors, and can be assessed with
Monte Carlo simulations.
| [{'version': 'v1', 'created': 'Fri, 12 Oct 2001 09:24:33 GMT'}] | 2016-08-30 | [array(['Massarotti', 'M.', '', 'Oss. Astron. Capodimonte'], dtype=object)
array(['Iovino', 'A.', '', 'Oss. Astron.\n Brera'], dtype=object)
array(['Buzzoni', 'A.', '', 'TNG, Oss. Astron. Brera'], dtype=object)
array(['Valls--Gabaud', 'D.', '', 'Obs.\n Midi-Pyrenees'], dtype=object)] |
355 | 1909.11528 | Jordi Borras | Jordi Borras and Gregori Vazquez | Context-Aware Decentralized Invariant Signaling for Opportunistic
Communications | This paper was rejected. The authors decided to keep working and
improving this work. Currently, a more sophisticated work based on the
rejected paper is being written, which can be of major interest to anyone
interested in this research topic. The authors will upload this new work as
soon as possible | null | null | null | cs.IT math.IT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A novel scenario-adapted distributed signaling technique in the context of
opportunistic communications is presented in this work. Each opportunistic user
acquires locally sampled observations from the wireless environment to
determine the occupied and available degrees-of-freedom (DoF). Due to sensing
errors and locality of observations, a performance loss and inter-system
interference arise from subspace uncertainties. Yet, we show that addressing
the problem as a total least-squares (TLS) optimization, signaling patterns
robust to subspace uncertainties can be designed. Furthermore, given the
equivalence of minimum norm and TLS, the latter exhibits the interesting
properties of linear predictors. Specifically, the rotationally invariance
property is of paramount importance to guarantee the detectability by
neighboring nodes. Albeit these advantages, end-to-end subspace uncertainties
yield a performance loss that compromises both detectability and wireless
environment's performance. To combat the latter, we tackle the distributed
identification of the active subspace with and without side information about
neighboring nodes' subspaces. An extensive simulation analysis highlights the
performance of distributed concurrency schemes to achieve subspace agreement.
| [{'version': 'v1', 'created': 'Wed, 25 Sep 2019 14:37:36 GMT'}
{'version': 'v2', 'created': 'Fri, 29 Oct 2021 09:44:47 GMT'}] | 2021-11-01 | [array(['Borras', 'Jordi', ''], dtype=object)
array(['Vazquez', 'Gregori', ''], dtype=object)] |
356 | hep-th/0003182 | Alexander Kapustnikov | A. A. Kapustnikov | Superextension n=(2,2) of the complex Liouville equation and its
solution | 11 pages, LaTeX, talk given at the XIV-th Max Born Symposium,
Karpacz, Poland, September 21-25, 1999 | null | 10.1142/9789812793263_0019 | null | hep-th | null | It is shown that the method of the nonlinear realization of local
supersymmetry previously developed in framework of supergravity being applied
to the n=(2,2) superconformal symmetry allows one to get the new form of the
exactly solvable n=(2,2) super-Liouville equation. The general advantage of
this version as compared with the conventional one is that its bosonic part
includes the complex Liouville equation. We obtain the suitable supercovariant
constraints imposed on the corresponding superfields which provide the set of
the resulting system of component equations be the same as that in model of
N=2, D=4 Green-Schwarz superstring. The general solution of this system is
derived from the corresponding solution of the bosonic string equation.
| [{'version': 'v1', 'created': 'Tue, 21 Mar 2000 07:28:05 GMT'}] | 2016-11-23 | [array(['Kapustnikov', 'A. A.', ''], dtype=object)] |
357 | 1812.09279 | Sherry Chu | Sherry Chu, Mehran Kardar, David R. Nelson, and Daniel A. Beller | Evolution in range expansions with competition at rough boundaries | null | null | null | null | physics.bio-ph cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | When a biological population expands into new territory, genetic drift
develops an enormous influence on evolution at the propagating front. In such
range expansion processes, fluctuations in allele frequencies occur through
stochastic \textit{spatial} wandering of both genetic lineages and the
boundaries between genetically segregated sectors. Laboratory experiments on
microbial range expansions have shown that this stochastic wandering,
transverse to the front, is superdiffusive due to the front's growing
roughness, implying much faster loss of genetic diversity than predicted by
simple flat front diffusive models. We study the evolutionary consequences of
this superdiffusive wandering using two complementary numerical models of range
expansions: the stepping stone model, and a new interpretation of the model of
directed paths in random media, in the context of a roughening population
front. Through these approaches we compute statistics for the times since
common ancestry for pairs of individuals with a given spatial separation at the
front, and we explore how environmental heterogeneities can locally suppress
these superdiffusive fluctuations.
| [{'version': 'v1', 'created': 'Fri, 21 Dec 2018 17:42:44 GMT'}] | 2018-12-24 | [array(['Chu', 'Sherry', ''], dtype=object)
array(['Kardar', 'Mehran', ''], dtype=object)
array(['Nelson', 'David R.', ''], dtype=object)
array(['Beller', 'Daniel A.', ''], dtype=object)] |
358 | hep-ph/0602219 | Sergey Afonin | S.S. Afonin and D. Espriu | Qualitative solution of QCD sum rules | Version published in JHEP | JHEP 0609 (2006) 047 | 10.1088/1126-6708/2006/09/047 | UB-ECM-PF-06/08 | hep-ph | null | We show how such important features of QCD as chiral symmetry breaking or the
formation of a mass-gap can be directly traced from QCD sum rules for two point
functions assuming, in the large number of colors limit, exact duality between
the operator product expansion and the spectrum described by linearly (or
nearly linear) rising Regge trajectories as predicted by string theory. We see
how the presence of chiral symmetry breaking is intimately related to
confinement in this scenario, as expected from general arguments, and how Regge
trajectories change when chiral symmetry is broken. As a result the whole meson
mass spectrum can be parametrized with a good accuracy by the constant
$f_{\pi}$ only, thus realizing the program proposed by Migdal some time ago.
| [{'version': 'v1', 'created': 'Thu, 23 Feb 2006 20:55:02 GMT'}
{'version': 'v2', 'created': 'Tue, 7 Mar 2006 16:59:04 GMT'}
{'version': 'v3', 'created': 'Mon, 2 Oct 2006 13:55:07 GMT'}] | 2009-11-11 | [array(['Afonin', 'S. S.', ''], dtype=object)
array(['Espriu', 'D.', ''], dtype=object)] |
359 | 0804.1764 | Friedwardt Winterberg | Friedwardt Winterberg | Attainment of Gigavolt Potentials by Fluid Dynamic Suppression of the
Stepped Leader its Significance for Thermonuclear Ignition | 9 pages, 1 figure | null | null | null | physics.acc-ph physics.plasm-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is proposed to levitate a conducting sphere in a high pressure Taylor flow
and to charge it up to gigavolt potentials, either mechanically as in a Van de
Graaff electrostatic generator, or inductively by a rising magnetic field. If
the Taylor flow is sufficiently fast, it should overcome the electric pressure
and breakdown by stepped leader formation, leading to the maximum attainable
voltage by the Paschen law. Discharging the electrostatically stored energy can
be done by controlled breakdown. With gigajoule energies stored and released in
about 10^-8 sec, this implies and electric pulse power of the order 10^17 Watt,
opening the prospect of large driver energies for thermonuclear ignition.
| [{'version': 'v1', 'created': 'Thu, 10 Apr 2008 17:14:24 GMT'}
{'version': 'v2', 'created': 'Tue, 13 May 2008 17:53:14 GMT'}] | 2008-05-13 | [array(['Winterberg', 'Friedwardt', ''], dtype=object)] |
360 | 0706.4380 | Thorsten Renk | Thorsten Renk, Kari J. Eskola | Prospects of Jet Tomography Using Hard Processes inside a Soft Medium | 10 pages, 7 figures, talk given at the workshop 'High p_T physics at
the LHC', University of Jyvaskyla, Jyvaskyla, Finland, 23-27 March, 2007 | PoSLHC07:032,2007 | null | null | hep-ph | null | The term 'tomography' is commonly applied to the idea of studying properties
of a medium by the modifications this medium induces to a known probe
propagating through it. In the context of ultrarelativistic heavy-ion
collisions, rare high transverse momentum (p_T) processes taking place
alongside soft bulk-matter production can be viewed as a tomographic probe as
long as the energy scales are such that the modification of high p_T processes
can be dominantly ascribed to interactions with the medium during the
propagation of partons. Various high p_T observables have been suggested for
tomography, among them hard single hadron suppression, dihadron correlations
and gamma-hadron correlations. In this paper, we present a model study of a
number of different observables within the same calculational framework to
assess the sensitivity of the observables to different properties of the medium
and discuss the prospects of obtaining tomographic information.
| [{'version': 'v1', 'created': 'Fri, 29 Jun 2007 10:13:46 GMT'}] | 2008-11-26 | [array(['Renk', 'Thorsten', ''], dtype=object)
array(['Eskola', 'Kari J.', ''], dtype=object)] |
361 | 1505.06705 | Paola Arias | Paola Arias, Edwin Ireson, Fidel A. Schaposnik and Gianni Tallarita | Chern-Simons-Higgs Theory with Visible and Hidden Sectors and its ${\cal
N}=2$ SUSY Extension | 10 pages, 12 figures. Several typos fixed and the Gauss law is
explicitly written, figures correctly shown. Accepted in PLB | null | 10.1016/j.physletb.2015.08.005 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study vortex solutions in Abelian Chern-Simons-Higgs theories with visible
and hidden sectors. We first consider the case in which the two sectors are
connected through a BF-like gauge mixing term with no explicit interaction
between the the two scalars. Since first order Bogomolny equations do not exist
in this case, we derive the second order field equations. We then proceed to an
${\cal N}=2$ supersymmetric extension including a Higgs portal mixing among the
visible and hidden charged scalars. As expected, Bogomolnyi equations do exist
in this case and we study their string-like solutions numerically.
| [{'version': 'v1', 'created': 'Mon, 25 May 2015 17:57:55 GMT'}
{'version': 'v2', 'created': 'Fri, 14 Aug 2015 04:23:46 GMT'}
{'version': 'v3', 'created': 'Mon, 17 Aug 2015 17:20:11 GMT'}] | 2015-08-18 | [array(['Arias', 'Paola', ''], dtype=object)
array(['Ireson', 'Edwin', ''], dtype=object)
array(['Schaposnik', 'Fidel A.', ''], dtype=object)
array(['Tallarita', 'Gianni', ''], dtype=object)] |
362 | 1804.03593 | Guangxu Zhu | Yuqing Du and Guangxu Zhu and Jiayao Zhang and Kaibin Huang | Automatic Recognition of Space-Time Constellations by Learning on the
Grassmann Manifold (Extended Version) | An extended version for an IEEE submission | null | 10.1109/TSP.2018.2873542 | null | cs.IT math.IT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recent breakthroughs in machine learning especially artificial intelligence
shift the paradigm of wireless communication towards intelligence radios. One
of their core operations is automatic modulation recognition (AMR). Existing
research focuses on coherent modulation schemes such as QAM, PSK and FSK. The
AMR of (non-coherent) space-time modulation remains an uncharted area despite
its wide deployment in modern multiple-input-multiple-output (MIMO) systems.
The scheme using a so called Grassmann constellation enables rate-enhancement
using multi-antennas and blind detection. In this work, we propose an AMR
approach for Grassmann constellation based on data clustering, which differs
from traditional AMR based on classification using a modulation database. The
approach allows algorithms for clustering on the Grassmann manifold, such as
Grassmann K-means and depth-first search, originally developed for computer
vision to be applied to AMR. We further develop an analytical framework for
studying and designing these algorithms in the context of AMR. First, the
maximum-likelihood Grassmann constellation detection is proved to be equivalent
to clustering on the Grassmannian. Thereby, a well-known machine-learning
result that was originally established only for the Euclidean space is
rediscovered for the Grassmannian. Next, despite a rich literature on
algorithmic design, theoretical analysis of data clustering is largely
overlooked due to the lack of tractable techniques. We tackle the challenge by
introducing probabilistic metrics for measuring the inter-cluster separability
and intra-cluster connectivity of received space-time symbols and deriving them
using tools from differential geometry and Grassmannian packing. The results
provide useful insights into the effects of various parameters ranging from the
signal-to-noise ratio to constellation size, facilitating algorithmic design.
| [{'version': 'v1', 'created': 'Tue, 10 Apr 2018 15:40:29 GMT'}
{'version': 'v2', 'created': 'Wed, 11 Apr 2018 15:51:55 GMT'}] | 2018-11-14 | [array(['Du', 'Yuqing', ''], dtype=object)
array(['Zhu', 'Guangxu', ''], dtype=object)
array(['Zhang', 'Jiayao', ''], dtype=object)
array(['Huang', 'Kaibin', ''], dtype=object)] |
363 | 0706.2412 | Christian Corda cordac | Christian Corda | Generalized gauge-invariance for gravitational waves | This paper has been withdrawn by the author because an improved and
updated version has been put in the archive | null | null | null | gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The aim of this paper is to show the gauge-invariance on the response of
interferometers to gravitational waves (GWs). In this process, after a review
of results on the Tranverse-Traceless (TT) gauge, where, in general, the
theoretical computations on GWs are performed, which is due for completness, we
analyse the gauge of the local observer, which represents the gauge of a
laboratory environment on Earth. The gauge-invariance between the two gauges is
shown in its full angular and frequency dependences. In previous works in the
literature this gauge-invariance was shown only in the low frequencies
approximation or in the simplest geometry of the interferometer in respect to
the propagating GW (i.e. both of the arms of the interferometer are
perpendicular to the propagating GW). As far as the computation of the response
functions in the gauge of the local observer is concerned, a common
misconception about interferometers is also clarifed.
| [{'version': 'v1', 'created': 'Sat, 16 Jun 2007 10:43:36 GMT'}
{'version': 'v2', 'created': 'Fri, 30 May 2008 13:24:47 GMT'}
{'version': 'v3', 'created': 'Mon, 15 Sep 2008 05:14:55 GMT'}
{'version': 'v4', 'created': 'Thu, 18 Sep 2008 09:42:54 GMT'}
{'version': 'v5', 'created': 'Thu, 16 Oct 2008 13:30:16 GMT'}
{'version': 'v6', 'created': 'Thu, 24 Mar 2011 15:26:44 GMT'}] | 2011-03-25 | [array(['Corda', 'Christian', ''], dtype=object)] |
364 | 0802.3180 | Daniel Gomez Vergel | Daniel G\'omez Vergel | Schrodinger quantization of linearly polarized Gowdy $S^1\times S^2$ and
$S^3$ models coupled to massless scalar fields | 18 pages. Final version to appear in Classical and Quantum Gravity | Class.Quant.Grav.25:175016,2008 | 10.1088/0264-9381/25/17/175016 | null | gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we will construct the Schrodinger representation for the
linearly polarized Gowdy $S^1\times S^2$ and $S^3$ models coupled to massless
scalar fields. Here the quantum states belong to a $L^2$-space for a suitable
quantum configuration space endowed with a Gaussian measure, whose support is
analyzed. This study completes the quantization of these systems previously
performed in the Fock scheme, and provides a specially useful framework to
address physically relevant questions.
| [{'version': 'v1', 'created': 'Thu, 21 Feb 2008 18:01:02 GMT'}
{'version': 'v2', 'created': 'Tue, 27 May 2008 14:27:46 GMT'}
{'version': 'v3', 'created': 'Wed, 23 Jul 2008 12:53:35 GMT'}] | 2008-11-26 | [array(['Vergel', 'Daniel Gómez', ''], dtype=object)] |
365 | 2301.02567 | Boris N. Narozhny | Narozhny B.N | Hydrodynamic approach to many-body systems: exact conservation laws | 23 pages | Annals of Physics 454, 169341 (2023) | 10.1016/j.aop.2023.169341 | null | cond-mat.str-el cond-mat.mes-hall | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper I present a pedagogical derivation of continuity equations
manifesting exact conservation laws in an interacting electronic system based
on the nonequilibrium Keldysh technique. The purpose of this exercise is to lay
the groundwork for extending the hydrodynamic approach to electronic transport
to strongly correlated systems where the quasiparticle approximation and
Boltzmann kinetic theory fail.
| [{'version': 'v1', 'created': 'Fri, 6 Jan 2023 15:37:08 GMT'}
{'version': 'v2', 'created': 'Sun, 28 May 2023 15:45:59 GMT'}] | 2023-05-30 | [array(['N', 'Narozhny B.', ''], dtype=object)] |
366 | 2301.05166 | Salvatore Ferrone | Salvatore Ferrone, Paola Di Matteo, Alessandra Mastrobuono-Battisti,
Misha Haywood, Owain N. Snaith, Marco Montouri, Sergey Khoperskov, David
Valls-Gabaud | The e-TidalGCs Project: Modeling the extra-tidal features generated by
Galactic globular clusters | 51 pages, 34 figures, Accepted for publication on A&A | A&A 673, A44 (2023) | 10.1051/0004-6361/202244141 | null | astro-ph.GA | http://creativecommons.org/licenses/by/4.0/ | We present the e-TidalGCs Project which aims at modeling and predicting the
extra-tidal features surrounding all Galactic globular clusters for which 6D
phase space information, masses and sizes are available (currently 159 globular
clusters). We focus the analysis and presentation of the results on the
distribution of extra-tidal material on the sky, and on the different
structures found at different heliocentric distances. We emphasize the wide
variety of morphologies found: beyond the canonical tidal tails, our models
reveal that the extra-tidal features generated by globular clusters take a wide
variety of shapes, from thin and elongated shapes, to thick, and complex
halo-like structures. We also compare some of the most well studied stellar
streams found around Galactic globular clusters to our model predictions,
namely those associated to the clusters NGC 3201, NGC 4590, NGC 5466 and Pal 5.
Additionally, we investigate how the distribution and extension in the sky of
the simulated streams vary with the Galactic potential by making use of three
different models, containing or not a central spheroid, or a stellar bar.
Overall, our models predict that the mass lost by the current globular cluster
population in the field from the last 5 Gyrs is between
$0.3-2.1\times10^{7}M_{\odot}$, an amount comparable between 7-55 % of current
mass. Most of this lost mass is found in the inner Galaxy, with the half-mass
radius of this population being between 4-6 kpc. The outputs of the simulations
will be publicly available, at a time when the ESA Gaia mission and
complementary spectroscopic surveys are delivering exquisite data to which
these models can be compared.
| [{'version': 'v1', 'created': 'Thu, 12 Jan 2023 17:37:29 GMT'}] | 2023-05-03 | [array(['Ferrone', 'Salvatore', ''], dtype=object)
array(['Di Matteo', 'Paola', ''], dtype=object)
array(['Mastrobuono-Battisti', 'Alessandra', ''], dtype=object)
array(['Haywood', 'Misha', ''], dtype=object)
array(['Snaith', 'Owain N.', ''], dtype=object)
array(['Montouri', 'Marco', ''], dtype=object)
array(['Khoperskov', 'Sergey', ''], dtype=object)
array(['Valls-Gabaud', 'David', ''], dtype=object)] |
367 | 1510.01205 | Vinodh Kumar Bandaru | Vinodh Bandaru, Thomas Boeck, Dmitry Krasnov, J\"org Schumacher | A hybrid finite-difference/boundary element procedure for the simulation
of turbulent MHD duct flow at finite magnetic Reynolds numbers | null | Journal of Computational Physics, Volume 304, pp.320-339, 2016 | 10.1016/j.jcp.2015.10.007 | null | physics.flu-dyn | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A conservative coupled finite difference-boundary element computational
procedure for the simulation of turbulent magnetohydrodynamic flow in a
straight rectangular duct at finite magnetic Reynolds number is presented. The
flow is assumed to be periodic in the streamwise direction and is driven by a
mean pressure gradient. The duct walls are considered to be electrically
insulating. The co-evolution of the velocity and magnetic fields as described
respectively by the Navier-Stokes and the magnetic induction equations,
together with the coupling of the magnetic field between the conducting domain
and the non-conducting exterior is solved using the magnetic field formulation.
The aim is to simulate localized magnetic fields interacting with turbulent
duct flow. Detailed verification of the implementation of the numerical scheme
is conducted in the limiting case of low magnetic Reynolds number by comparing
with the results obtained using a quasistatic approach that has no coupling
with the exterior. The rigorous procedure with non-local magnetic boundary
conditions is compared versus simplified pseudo-vacuum boundary conditions and
the differences are quantified. Our first direct numerical simulations of
turbulent Hartmann duct flow at moderate magnetic Reynolds numbers and a low
flow Reynolds number show significant differences in the duct flow turbulence,
even at low interaction level between the flow and magnetic field
| [{'version': 'v1', 'created': 'Mon, 5 Oct 2015 16:14:38 GMT'}] | 2015-11-05 | [array(['Bandaru', 'Vinodh', ''], dtype=object)
array(['Boeck', 'Thomas', ''], dtype=object)
array(['Krasnov', 'Dmitry', ''], dtype=object)
array(['Schumacher', 'Jörg', ''], dtype=object)] |
368 | 2111.00789 | Russell Buchanan | Russell Buchanan, Marco Camurri, Frank Dellaert, Maurice Fallon | Learning Inertial Odometry for Dynamic Legged Robot State Estimation | To be presented at 5th Annual Conference on Robot Learning (CoRL),
2021 | null | null | null | cs.RO | http://creativecommons.org/licenses/by/4.0/ | This paper introduces a novel proprioceptive state estimator for legged
robots based on a learned displacement measurement from IMU data. Recent
research in pedestrian tracking has shown that motion can be inferred from
inertial data using convolutional neural networks. A learned inertial
displacement measurement can improve state estimation in challenging scenarios
where leg odometry is unreliable, such as slipping and compressible terrains.
Our work learns to estimate a displacement measurement from IMU data which is
then fused with traditional leg odometry. Our approach greatly reduces the
drift of proprioceptive state estimation, which is critical for legged robots
deployed in vision and lidar denied environments such as foggy sewers or dusty
mines. We compared results from an EKF and an incremental fixed-lag factor
graph estimator using data from several real robot experiments crossing
challenging terrains. Our results show a reduction of relative pose error by
37% in challenging scenarios when compared to a traditional kinematic-inertial
estimator without learned measurement. We also demonstrate a 22% reduction in
error when used with vision systems in visually degraded environments such as
an underground mine.
| [{'version': 'v1', 'created': 'Mon, 1 Nov 2021 09:37:34 GMT'}] | 2021-11-02 | [array(['Buchanan', 'Russell', ''], dtype=object)
array(['Camurri', 'Marco', ''], dtype=object)
array(['Dellaert', 'Frank', ''], dtype=object)
array(['Fallon', 'Maurice', ''], dtype=object)] |
369 | 1502.02922 | Amalia Coldea | M. D. Watson, T. Yamashita, S. Kasahara, W. Knafo, M. Nardone, J.
Beard, F. Hardy, A. McCollam, A. Narayanan, S. F. Blake, T. Wolf, A. A.
Haghighirad, C. Meingast, A. J. Schofield, H. von Lohneysen, Y. Matsuda, A.
I. Coldea, and T. Shibauchi | Dichotomy between the hole and electrons behavior in the multiband FeSe
probed by ultra high magnetic fields | Latex, 4 pages (2 figures, 1 table), and supplemental material | Phys. Rev. Lett. 115, 027006 (2015) | 10.1103/PhysRevLett.115.027006 | null | cond-mat.supr-con cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Magnetoresistivity \r{ho}xx and Hall resistivity \r{ho}xy in ultra high
magnetic fields up to 88T are measured down to 0.15K to clarify the multiband
electronic structure in high-quality single crystals of superconducting FeSe.
At low temperatures and high fields we observe quantum oscillations in both
resistivity and Hall effect, confirming the multiband Fermi surface with small
volumes. We propose a novel and independent approach to identify the sign of
corresponding cyclotron orbit in a compensated metal from magnetotransport
measurements. The observed significant differences in the relative amplitudes
of the quantum oscillations between the \r{ho}xx and \r{ho}xy components,
together with the positive sign of the high-field \r{ho}xy , reveal that the
largest pocket should correspond to the hole band. The low-field
magnetotransport data in the normal state suggest that, in addition to one hole
and one almost compensated electron bands, the orthorhombic phase of FeSe
exhibits an additional tiny electron pocket with a high mobility.
| [{'version': 'v1', 'created': 'Tue, 10 Feb 2015 14:35:46 GMT'}] | 2015-08-21 | [array(['Watson', 'M. D.', ''], dtype=object)
array(['Yamashita', 'T.', ''], dtype=object)
array(['Kasahara', 'S.', ''], dtype=object)
array(['Knafo', 'W.', ''], dtype=object)
array(['Nardone', 'M.', ''], dtype=object)
array(['Beard', 'J.', ''], dtype=object)
array(['Hardy', 'F.', ''], dtype=object)
array(['McCollam', 'A.', ''], dtype=object)
array(['Narayanan', 'A.', ''], dtype=object)
array(['Blake', 'S. F.', ''], dtype=object)
array(['Wolf', 'T.', ''], dtype=object)
array(['Haghighirad', 'A. A.', ''], dtype=object)
array(['Meingast', 'C.', ''], dtype=object)
array(['Schofield', 'A. J.', ''], dtype=object)
array(['von Lohneysen', 'H.', ''], dtype=object)
array(['Matsuda', 'Y.', ''], dtype=object)
array(['Coldea', 'A. I.', ''], dtype=object)
array(['Shibauchi', 'T.', ''], dtype=object)] |
370 | 1404.4634 | Camille Avestruz | Camille Avestruz, Erwin T. Lau, Daisuke Nagai, Alexey Vikhlinin | Testing X-ray Measurements of Galaxy Cluster Outskirts with Cosmological
Simulations | 13 pages, 11 figures, Accepted to ApJ | null | 10.1088/0004-637X/791/2/117 | null | astro-ph.CO astro-ph.GA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The study of galaxy cluster outskirts has emerged as one of the new frontiers
in extragalactic astrophysics and cosmology with the advent of new observations
in X-ray and microwave. However, the thermodynamic properties and chemical
enrichment of this diffuse and azimuthally asymmetric component of the
intracluster medium (ICM) are still not well understood. This work, for the
first time, systematically explores potential observational biases in these
regions. To assess X-ray measurements of galaxy cluster properties at large
radii ($>{R}_{500c}$), we use mock Chandra analyses of cosmological galaxy
cluster simulations. The pipeline is identical to that used for Chandra
observations, but the biases discussed in this paper are relevant for all X-ray
observations outside of ${R}_{500c}$. We find the following from our analysis:
(1) filament regions can contribute as much as $50\%$ at $R_{200c}$ to the
emission measure; (2) X-ray temperatures and metal abundances from model fitted
mock X-ray spectra in a multi-temperature ICM respectively vary to the level of
$10\%$ and $50\%$; (3) resulting density profiles vary to within $10\%$ out to
$R_{200c}$, and gas mass, total mass, and baryon fractions all vary to within a
few percent; (4) the bias from a metal abundance extrapolated a factor of five
higher than the true metal abundance results in total mass measurements biased
high by $20\%$ and total gas measurements biased low by $10\%$; and (5)
differences in projection and dynamical state of a cluster can lead to gas
density slope measurements that differ by a factor of $15\%$ and $30\%$,
respectively. The presented results can partially account for some of the
recent gas profile measurements in cluster outskirts by, e.g., Suzaku. Our
findings are pertinent to future X-ray cosmological constraints from cluster
outskirts.
| [{'version': 'v1', 'created': 'Thu, 17 Apr 2014 20:00:10 GMT'}
{'version': 'v2', 'created': 'Tue, 21 Oct 2014 21:58:12 GMT'}
{'version': 'v3', 'created': 'Thu, 23 Oct 2014 16:21:01 GMT'}] | 2014-10-24 | [array(['Avestruz', 'Camille', ''], dtype=object)
array(['Lau', 'Erwin T.', ''], dtype=object)
array(['Nagai', 'Daisuke', ''], dtype=object)
array(['Vikhlinin', 'Alexey', ''], dtype=object)] |
371 | 2010.03374 | Peter Yatsyshin Dr | Peter Yatsyshin, Serafim Kalliadasis and Andrew B. Duncan | Physics-constrained Bayesian inference of state functions in classical
density-functional theory | null | J. Chem. Phys. (2022) | 10.1063/5.0071629 | null | cond-mat.stat-mech physics.data-an stat.ML | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop a novel data-driven approach to the inverse problem of classical
statistical mechanics: given experimental data on the collective motion of a
classical many-body system, how does one characterise the free energy landscape
of that system? By combining non-parametric Bayesian inference with
physically-motivated constraints, we develop an efficient learning algorithm
which automates the construction of approximate free energy functionals. In
contrast to optimisation-based machine learning approaches, which seek to
minimise a cost function, the central idea of the proposed Bayesian inference
is to propagate a set of prior assumptions through the model, derived from
physical principles. The experimental data is used to probabilistically weigh
the possible model predictions. This naturally leads to humanly interpretable
algorithms with full uncertainty quantification of predictions. In our case,
the output of the learning algorithm is a probability distribution over a
family of free energy functionals, consistent with the observed particle data.
We find that surprisingly small data samples contain sufficient information for
inferring highly accurate analytic expressions of the underlying free energy
functionals, making our algorithm highly data efficient. We consider excluded
volume particle interactions, which are ubiquitous in nature, whilst being
highly challenging for modelling in terms of free energy. To validate our
approach we consider the paradigmatic case of one-dimensional fluid and develop
inference algorithms for the canonical and grand-canonical
statistical-mechanical ensembles. Extensions to higher-dimensional systems are
conceptually straightforward, whilst standard coarse-graining techniques allow
one to easily incorporate attractive interactions.
| [{'version': 'v1', 'created': 'Wed, 7 Oct 2020 12:43:42 GMT'}
{'version': 'v2', 'created': 'Mon, 23 Nov 2020 17:50:19 GMT'}
{'version': 'v3', 'created': 'Fri, 18 Jun 2021 17:20:40 GMT'}
{'version': 'v4', 'created': 'Wed, 23 Jun 2021 10:28:00 GMT'}] | 2022-03-01 | [array(['Yatsyshin', 'Peter', ''], dtype=object)
array(['Kalliadasis', 'Serafim', ''], dtype=object)
array(['Duncan', 'Andrew B.', ''], dtype=object)] |
372 | astro-ph/0511231 | Daniela Kirilova | Daniela P. Kirilova | More General BBN Constraints on Neutrino Oscillations Parameters -
Relaxed or Strengthened | 13 pages, 4 figures | Int.J.Mod.Phys.D16:1197-1210,2007 | 10.1142/S0218271807010791 | ULB-TH/04-01 | astro-ph hep-ph | null | I discuss BBN with nonequilibrium nu_e<->nu_s oscillations in the more
general case of non-zero population of nu_s before oscillations delta N_s>0. I
calculate He-4 primordial production Y_p(delta N_s) in the presence of
nu_e<->nu_s oscillations for different initial populations of nu_s state
0<=delta N_s<=1 and the full range of oscillation parameters.
Non-zero delta N_s has two-fold effect on He-4: (i) it enhances the energy
density and hence increases the cosmic expansion rate, leading to Y_p
overproduction and (ii) it suppresses the kinetic effects of oscillations on
BBN, namely the effects on pre-BBN nucleon kinetics caused by the nu_e energy
spectrum distortion and the neutrino-antineutrino asymmetry generation by
oscillations, leading to decreased Y_p overproduction. Depending on oscillation
parameters one or the other effect may dominate, causing, correspondingly,
either a relaxation of the cosmological constraints or their strengthening with
the increase of delta N_s .
I calculate more general BBN constraints on nu_e<->nu_s oscillation
parameters,corresponding to 3% Y_p overproduction, for different initial
populations of nu_s.Previous BBN constraints were derived assuming empty
sterile state before oscillations. The cosmological constraints for that case
strengthen with the increase of delta N_s value.
| [{'version': 'v1', 'created': 'Tue, 8 Nov 2005 18:08:49 GMT'}] | 2008-11-26 | [array(['Kirilova', 'Daniela P.', ''], dtype=object)] |
373 | 0705.0540 | Jon M. Miller | J. M. Miller (University of Michigan) | Relativistic X-ray Lines from the Inner Accretion Disks Around Black
Holes | 40 pages, includes color figures, to appear in ARAA, vol 45, in press | Ann.Rev.Astron.Astrophys.45:441-479,2007 | 10.1146/annurev.astro.45.051806.110555 | null | astro-ph | null | Relativistic X-ray emission lines from the inner accretion disk around black
holes are reviewed. Recent observations with the Chandra X-ray Observatory,
X-ray Multi-Mirror Mission-Newton, and Suzaku are revealing these lines to be
good probes of strong gravitational effects. A number of important
observational and theoretical developments are highlighted, including evidence
of black hole spin and effects such as gravitational light bending, the
detection of relativistic lines in stellar-mass black holes, and evidence of
orbital-timescale line flux variability. In addition, the robustness of the
relativistic disk lines against absorption, scattering, and continuum effects
is discussed. Finally, prospects for improved measures of black hole spin and
understanding the spin history of supermassive black holes in the context of
black hole-galaxy co-evolution are presented. The best data and most rigorous
results strongly suggest that relativistic X-ray disk lines can drive future
explorations of General Relativity and disk physics.
| [{'version': 'v1', 'created': 'Thu, 3 May 2007 21:00:46 GMT'}
{'version': 'v2', 'created': 'Tue, 29 May 2007 18:35:32 GMT'}
{'version': 'v3', 'created': 'Wed, 6 Jun 2007 15:33:00 GMT'}] | 2009-06-23 | [array(['Miller', 'J. M.', '', 'University of Michigan'], dtype=object)] |
374 | 2104.10419 | Xin Huang | Xin Huang, Xinxin Wang, Wenyu Lv, Xiaying Bai, Xiang Long, Kaipeng
Deng, Qingqing Dang, Shumin Han, Qiwen Liu, Xiaoguang Hu, Dianhai Yu, Yanjun
Ma, Osamu Yoshie | PP-YOLOv2: A Practical Object Detector | null | null | null | null | cs.CV | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Being effective and efficient is essential to an object detector for
practical use. To meet these two concerns, we comprehensively evaluate a
collection of existing refinements to improve the performance of PP-YOLO while
almost keep the infer time unchanged. This paper will analyze a collection of
refinements and empirically evaluate their impact on the final model
performance through incremental ablation study. Things we tried that didn't
work will also be discussed. By combining multiple effective refinements, we
boost PP-YOLO's performance from 45.9% mAP to 49.5% mAP on COCO2017 test-dev.
Since a significant margin of performance has been made, we present PP-YOLOv2.
In terms of speed, PP-YOLOv2 runs in 68.9FPS at 640x640 input size. Paddle
inference engine with TensorRT, FP16-precision, and batch size = 1 further
improves PP-YOLOv2's infer speed, which achieves 106.5 FPS. Such a performance
surpasses existing object detectors with roughly the same amount of parameters
(i.e., YOLOv4-CSP, YOLOv5l). Besides, PP-YOLOv2 with ResNet101 achieves 50.3%
mAP on COCO2017 test-dev. Source code is at
https://github.com/PaddlePaddle/PaddleDetection.
| [{'version': 'v1', 'created': 'Wed, 21 Apr 2021 08:55:37 GMT'}] | 2021-04-22 | [array(['Huang', 'Xin', ''], dtype=object)
array(['Wang', 'Xinxin', ''], dtype=object)
array(['Lv', 'Wenyu', ''], dtype=object)
array(['Bai', 'Xiaying', ''], dtype=object)
array(['Long', 'Xiang', ''], dtype=object)
array(['Deng', 'Kaipeng', ''], dtype=object)
array(['Dang', 'Qingqing', ''], dtype=object)
array(['Han', 'Shumin', ''], dtype=object)
array(['Liu', 'Qiwen', ''], dtype=object)
array(['Hu', 'Xiaoguang', ''], dtype=object)
array(['Yu', 'Dianhai', ''], dtype=object)
array(['Ma', 'Yanjun', ''], dtype=object)
array(['Yoshie', 'Osamu', ''], dtype=object)] |
375 | 1602.03310 | Sibashisa Dash Dr | Le Wang, Sibashisa Dash, Lei Chang, Lu You, Yaqing Feng, Xu He,
Kui-juan Jin, Yang Zhou, Hock Guan Ong, Peng Ren, Shiwei Wang, Lang Chen, and
Junling Wang | Oxygen vacancy induced room temperature metal-insulator transition in
nickelates films and its potential application in photovoltaics | null | null | null | null | cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Oxygen vacancy is intrinsically coupled with magnetic, electronic and
transport properties of transition-metal oxide materials and directly
determines their multifunctionality. Here, we demonstrate reversible control of
oxygen content by post-annealing at temperature lower than 300 degree
centigrade and realize the reversible metal-insulator transition in epitaxial
NdNiO3 films. Importantly, over six orders of magnitude in the resistance
modulation and a large change in optical band gap are demonstrated at room
temperature without destroying the parent framework and changing the p-type
conductive mechanism. Further study revealed that oxygen vacancies stabilized
the insulating phase at room temperature is universal for perovskite nickelates
films. Acting as electron donors, oxygen vacancies not only stabilize the
insulating phase at room temperature, but also induce a large magnetization of
~50 emu/cm3 due to the formation of strongly correlated Ni2+ t2g6eg2 states.
The band gap opening is an order of magnitude larger than that of the thermally
driven metal-insulator transition and continuously tunable. Potential
application of the newly found insulating phase in photovoltaics has been
demonstrated in the nickelates-based heterojunctions. Our discovery opens up
new possibilities for strongly correlated perovskite nickelates.
| [{'version': 'v1', 'created': 'Wed, 10 Feb 2016 09:49:55 GMT'}] | 2016-02-11 | [array(['Wang', 'Le', ''], dtype=object)
array(['Dash', 'Sibashisa', ''], dtype=object)
array(['Chang', 'Lei', ''], dtype=object)
array(['You', 'Lu', ''], dtype=object)
array(['Feng', 'Yaqing', ''], dtype=object)
array(['He', 'Xu', ''], dtype=object)
array(['Jin', 'Kui-juan', ''], dtype=object)
array(['Zhou', 'Yang', ''], dtype=object)
array(['Ong', 'Hock Guan', ''], dtype=object)
array(['Ren', 'Peng', ''], dtype=object)
array(['Wang', 'Shiwei', ''], dtype=object)
array(['Chen', 'Lang', ''], dtype=object)
array(['Wang', 'Junling', ''], dtype=object)] |
376 | 1004.2263 | Nathan Smith | Nathan Smith, Matthew S. Povich, Barbara A. Whitney, Ed Churchwell,
Brian L. Babler, Marilyn R. Meade, John Bally, Robert D. Gehrz, Thomas P.
Robitaille, and Keivan G. Stassun | Spitzer Space Telescope observations of the Carina Nebula: The steady
march of feedback-driven star formation | 25 pages, 15 figures, MNRAS accepted | null | 10.1111/j.1365-2966.2010.16792.x | null | astro-ph.SR astro-ph.GA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We report the first results of imaging the Carina Nebula with Spitzer/IRAC,
providing a catalog of point sources and YSOs based on SED fits. We discuss
several aspects of the extended emission, including dust pillars that result
when a clumpy molecular cloud is shredded by massive star feedback. There are
few "extended green objects" (EGOs) normally taken as signposts of outflow
activity, and none of the HH jets detected optically are seen as EGOs. A
population of "extended red objects" tends to be found around OB stars, some
with clear bow-shocks. These are dusty shocks where stellar winds collide with
flows off nearby clouds. Finally, the relative distributions of O stars and
subclusters of YSOs as compared to dust pillars shows that while some YSOs are
located within pillars, many more stars and YSOs reside just outside pillar
heads. We suggest that pillars are transient phenomena, part of a continuous
outwardly propagating wave of star formation driven by massive star feedback.
As pillars are destroyed, they leave newly formed stars in their wake, which
are then subsumed into the young OB association. Altogether, the current
generation of YSOs shows no strong deviation from a normal IMF. The number of
YSOs suggests a roughly constant star-formation rate over the past 3Myr,
implying that star formation in pillars constitutes an important mechanism to
construct unbound OB associations. Accelerated pillars may give birth to O-type
stars that, after several Myr, could appear to have formed in isolation.
| [{'version': 'v1', 'created': 'Tue, 13 Apr 2010 20:05:52 GMT'}] | 2015-05-18 | [array(['Smith', 'Nathan', ''], dtype=object)
array(['Povich', 'Matthew S.', ''], dtype=object)
array(['Whitney', 'Barbara A.', ''], dtype=object)
array(['Churchwell', 'Ed', ''], dtype=object)
array(['Babler', 'Brian L.', ''], dtype=object)
array(['Meade', 'Marilyn R.', ''], dtype=object)
array(['Bally', 'John', ''], dtype=object)
array(['Gehrz', 'Robert D.', ''], dtype=object)
array(['Robitaille', 'Thomas P.', ''], dtype=object)
array(['Stassun', 'Keivan G.', ''], dtype=object)] |
377 | 2204.10624 | Yinhong Liu | Yinhong Liu, Guy Emerson | Learning Functional Distributional Semantics with Visual Data | Accepted by ACL 2022 main conference | null | null | null | cs.CL cs.AI | http://creativecommons.org/publicdomain/zero/1.0/ | Functional Distributional Semantics is a recently proposed framework for
learning distributional semantics that provides linguistic interpretability. It
models the meaning of a word as a binary classifier rather than a numerical
vector. In this work, we propose a method to train a Functional Distributional
Semantics model with grounded visual data. We train it on the Visual Genome
dataset, which is closer to the kind of data encountered in human language
acquisition than a large text corpus. On four external evaluation datasets, our
model outperforms previous work on learning semantics from Visual Genome.
| [{'version': 'v1', 'created': 'Fri, 22 Apr 2022 10:41:39 GMT'}] | 2022-04-25 | [array(['Liu', 'Yinhong', ''], dtype=object)
array(['Emerson', 'Guy', ''], dtype=object)] |
378 | 1002.3760 | Parinya Karndumri | Edi Gava, Parinya Karndumri and K.S. Narain | AdS$_3$ vacua and RG flows in three dimensional gauged supergravities | 35 pages in JHEP form, 3 figures, typos corrected, references added | JHEP 04 (2010) 117 | 10.1007/JHEP04(2010)117 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study $AdS_3$ supersymmetric vacua in N=4 and N=8, three dimensional
gauged supergravities, with scalar manifolds $(\frac{SO(4,4)}{SO(4)\times
SO(4)})^2$ and $\frac{SO(8,8)}{SO(8)\times SO(8)}$, non-semisimple Chern-Simons
gaugings $SO(4)\ltimes {\bf R}^6$ and $(SO(4)\ltimes {\bf R}^6)^2$,
respectively. These are in turn equivalent to SO(4) and $SO(4)\times SO(4)$
Yang-Mills theories coupled to supergravity. For the N=4 case, we study
renormalization group flows between UV and IR $AdS_3$ vacua with the same
amount of supersymmetry: in one case, with (3,1) supersymmetry, we can find an
analytic solution whereas in another, with (2,0) supersymmetry, we give a
numerical solution. In both cases, the flows turn out to be v.e.v. flows, i.e.
they are driven by the expectation value of a relevant operator in the dual
$SCFT_2$. These provide examples of v.e.v. flows between two $AdS_3$ vacua
within a gauged supergravity framework.
| [{'version': 'v1', 'created': 'Fri, 19 Feb 2010 15:36:29 GMT'}
{'version': 'v2', 'created': 'Mon, 1 Mar 2010 15:20:00 GMT'}
{'version': 'v3', 'created': 'Tue, 2 Mar 2010 11:15:24 GMT'}
{'version': 'v4', 'created': 'Fri, 5 Mar 2010 16:14:38 GMT'}
{'version': 'v5', 'created': 'Wed, 28 Apr 2010 17:36:37 GMT'}
{'version': 'v6', 'created': 'Sun, 8 May 2011 15:38:15 GMT'}] | 2012-07-30 | [array(['Gava', 'Edi', ''], dtype=object)
array(['Karndumri', 'Parinya', ''], dtype=object)
array(['Narain', 'K. S.', ''], dtype=object)] |
379 | hep-th/9807183 | Katsushi Ito | Katsushi Ito, Chuan-Sheng Xiong and Sung-Kil Yang | Seiberg-Witten Theory as d<1 Topological Strings | 12 pages, latex | Phys.Lett. B441 (1998) 155-162 | 10.1016/S0370-2693(98)01124-1 | YITP-98-44 | hep-th | null | In view of two-dimensional topological gravity coupled to matter, we study
the Seiberg-Witten theory for the low-energy behavior of N=2 supersymmetric
Yang-Mills theory with ADE gauge groups. We construct a new solution of the
Picard-Fuchs equations obeyed by the Seiberg-Witten periods. Our solution is
expressed as the linear sum over the infinite set of one-point functions of
gravitational descendants in $d<1$ topological strings. It turns out that our
solution provides the power series expansion around the origin of the quantum
moduli space of the Coulomb branch. For SU(N) gauge group we show how the
Seiberg-Witten periods are reconstructed from the present solution.
| [{'version': 'v1', 'created': 'Fri, 24 Jul 1998 03:10:30 GMT'}] | 2009-10-31 | [array(['Ito', 'Katsushi', ''], dtype=object)
array(['Xiong', 'Chuan-Sheng', ''], dtype=object)
array(['Yang', 'Sung-Kil', ''], dtype=object)] |
380 | 0809.2205 | Christophe Martayan | Christophe Martayan (GEPI), Jean Zorec, Yves Fremat | ZAMS rotational velocities of Be/Oe stars and LGRBs progenitors in the
Magellanic Clouds | poster IAUS256 | null | null | null | astro-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Large and Small Magellanic Clouds are priviledged environments to perform
tests of theoretical predictions at low metallicity on rotational velocities
and stellar evolution. According to theoretical predictions, the rotational
velocities of B-type stars are expected to be higher in low metallicity
(LMC/SMC) than in high metallicity (MW) environments. To verify the models, we
observed with the VLT-FLAMES 523 B and Be stars, which form, at the moment, the
largest observed sample of these kind of objects in the MCs. We first
determined the stellar fundamental parameters and we found that B and Be stars
rotate faster in the MCs than in the MW. We also determined the first
distribution of the average ZAMS rotational velocities versus the mass of Be
stars. These results indicate that the appearance of Be stars is mass-,
metallicity-, stellar evolution-, and star-formation regions-dependant.
Moreover, the recent models of Long Gamma Ray Bursts progenitors foresee
possible LGRBs progenitors at the SMC's metallicity. We confront these models
with the observed (ZAMS rotational velocities, masses) distributions of the
fastest rotators (Be and Oe stars) in our sample. Furthermore, we compare the
corresponding predicted rates from our study with observed rates of LGRBs.
| [{'version': 'v1', 'created': 'Fri, 12 Sep 2008 12:48:11 GMT'}] | 2008-09-15 | [array(['Martayan', 'Christophe', '', 'GEPI'], dtype=object)
array(['Zorec', 'Jean', ''], dtype=object)
array(['Fremat', 'Yves', ''], dtype=object)] |
381 | 1308.3536 | Henry Adams | Henry Adams and Gunnar Carlsson | Evasion Paths in Mobile Sensor Networks | null | International Journal of Robotics Research 34 (2015), 90-104 | 10.1177/0278364914548051 | null | math.AT cs.RO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Suppose that ball-shaped sensors wander in a bounded domain. A sensor doesn't
know its location but does know when it overlaps a nearby sensor. We say that
an evasion path exists in this sensor network if a moving intruder can avoid
detection. In "Coordinate-free coverage in sensor networks with controlled
boundaries via homology", Vin deSilva and Robert Ghrist give a necessary
condition, depending only on the time-varying connectivity data of the sensors,
for an evasion path to exist. Using zigzag persistent homology, we provide an
equivalent condition that moreover can be computed in a streaming fashion.
However, no method with time-varying connectivity data as input can give
necessary and sufficient conditions for the existence of an evasion path.
Indeed, we show that the existence of an evasion path depends not only on the
fibrewise homotopy type of the region covered by sensors but also on its
embedding in spacetime. For planar sensors that also measure weak rotation and
distance information, we provide necessary and sufficient conditions for the
existence of an evasion path.
| [{'version': 'v1', 'created': 'Fri, 16 Aug 2013 02:16:09 GMT'}
{'version': 'v2', 'created': 'Sun, 15 Sep 2013 22:47:13 GMT'}
{'version': 'v3', 'created': 'Fri, 24 Jan 2014 17:19:28 GMT'}] | 2016-01-26 | [array(['Adams', 'Henry', ''], dtype=object)
array(['Carlsson', 'Gunnar', ''], dtype=object)] |
382 | 1111.3641 | Hao Zhang | Edmond L. Berger, Qing-Hong Cao, Chuan-Ren Chen, Jiang-Hao Yu, Hao
Zhang | Dynamical Origin of the Correlation between the Asymmetries $A_{FB}^t$
and $A_{FB}^{\ell}$ | null | null | null | ANL-HEP-PR-11-74; MSUHEP-111024 | hep-ph hep-ex | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A larger than expected forward-backward asymmetry in rapidity is observed in
top quark pairs produced in proton-antiproton collisions at the Tevatron. The
asymmetry is seen in both the top quark distribution $A_{FB}^t$ and in the
distribution of charged leptons $A_{FB}^\ell$ from top quark decay. In this
paper, we study the kinematic and dynamic aspects of the tight relationship of
the two observables arising from the spin correlation between the charged
lepton and the top quark with different polarization states. We also consider
two benchmark new physics models, an axigluon model and a flavor-changing
$W^\prime$ model. These models could explain the values of both $A_{FB}^t$ and
$A_{FB}^\ell$. We emphasize the value of both measurements, and we conclude
that a model which produces more right-handed than left-handed top quarks is
favored by the present data.
| [{'version': 'v1', 'created': 'Tue, 15 Nov 2011 21:00:16 GMT'}] | 2011-11-18 | [array(['Berger', 'Edmond L.', ''], dtype=object)
array(['Cao', 'Qing-Hong', ''], dtype=object)
array(['Chen', 'Chuan-Ren', ''], dtype=object)
array(['Yu', 'Jiang-Hao', ''], dtype=object)
array(['Zhang', 'Hao', ''], dtype=object)] |
383 | 1907.06164 | Menassie Ephrem | Menassie Ephrem | Primitive Ideals of Labelled Graph $C^*$-algebras | Houston Journal of Math. to appear | null | null | null | math.OA math.FA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Given a directed graph $E$ and a labeling $\mathcal{L}$, one forms the
labelled graph $C^*$-algebra by taking a weakly left--resolving labelled space
$(E, \mathcal{L}, \mathcal{B})$ and considering a universal generating family
of partial isometries and projections. In this paper we provide
characterization for primitive ideals of labelled graph $C^*$-algebras.
| [{'version': 'v1', 'created': 'Sun, 14 Jul 2019 04:00:38 GMT'}] | 2019-07-16 | [array(['Ephrem', 'Menassie', ''], dtype=object)] |
384 | 1805.02241 | Juliao Braga | Juliao Braga and Nizam Omar and Luciana F. Thome | Acquisition and use of knowledge over a restricted domain by intelligent
agents | 5 pages | null | 10.1145/3077286.3077293 | null | cs.AI cs.MA cs.NI | http://creativecommons.org/licenses/by/4.0/ | This short paper provides a description of an architecture to acquisition and
use of knowledge by intelligent agents over a restricted domain of the Internet
Infrastructure. The proposed architecture is added to an intelligent agent
deployment model over a very useful server for Internet Autonomous System
administrators. Such servers, which are heavily dependent on arbitrary and
eventual updates of human beings, become unreliable. This is a position paper
that proposes three research questions that are still in progress.
| [{'version': 'v1', 'created': 'Sun, 6 May 2018 16:32:19 GMT'}] | 2018-05-08 | [array(['Braga', 'Juliao', ''], dtype=object)
array(['Omar', 'Nizam', ''], dtype=object)
array(['Thome', 'Luciana F.', ''], dtype=object)] |
385 | 1106.2601 | Vikram Dhillon | Vikram Dhillon | Knowledge Dispersion Index for Measuring Intellectual Capital | Submitted to Innocentive | null | null | null | cs.SI q-fin.GN | http://creativecommons.org/licenses/by/3.0/ | In this paper we propose a novel index to quantify and measure the flow of
information on macro and micro scales. We discuss the implications of this
index for knowledge management fields and also as intellectual capital that can
thus be utilized by entrepreneurs. We explore different function and human
oriented metrics that can be used at micro-scales to process the flow of
information. We present a table of about 23 metrics, such as change in IT
inventory and percentage of employees with advanced degrees, that can be used
at micro scales to wholly quantify knowledge dispersion as intellectual
capital. At macro scales we split the economy in an industrial and consumer
sector where the flow of information in each determines how fast an economy is
going to grow and how overall an economy will perform given the aggregate
demand. Lastly, we propose a model for knowledge dispersion based on graph
theory and show how corrections in the flow become self-evident. Through the
principals of flow conservation and capacity constrains we also speculate how
this flow might seeks some equilibrium and exhibit self-correction codes. This
proposed model allows us to account for perturbations in form of local noise,
evolution of networks, provide robustness against local damage from lower
nodes, and help determine the underlying classification into network
super-families.
| [{'version': 'v1', 'created': 'Tue, 14 Jun 2011 03:02:58 GMT'}] | 2011-06-15 | [array(['Dhillon', 'Vikram', ''], dtype=object)] |
386 | 2110.15363 | Najme Ebrahimi Dr | Payman Pahlavan and Najme Ebrahimi | Dual-band Harmonic and Subharmonic Frequency Generation Circuitry for
Joint Communication and Localization Applications Under Severe Multipath
Environment | null | null | null | null | eess.SP cs.SY eess.SY | http://creativecommons.org/licenses/by/4.0/ | The next generation of ultra-dense connected and automated wireless sensor
networks (WSN) requires proximity intelligence for many of its applications,
especially for identification and localization. This work presents the first
bidirectional circuitry for Internet of Things (IoT) transponder that
reciprocally generates harmonics and subharmonics, dual-band frequencies. A
multi-band or wideband localization system is essential for future intelligent
WSN to mitigate the influence of multipath signals for indoor dense
environment. The proposed frequency generation circuitry is based on the novel
nonlinear ring resonator (NRR) operating based on standing wave resonation. The
proposed NRR generates two sustainable oscillation frequencies based on the
periodicity of the nonlinear circuit in the ring configuration. Due to the
symmetry and reciprocity of the ring layout, the two bidirectional ports can
excite the circuit at the two opposite nodes while maintaining the required
boundary conditions for oscillation. The sustainable resonance conditions occur
by creating zero, short impedance, or pole, infinite impedance, at subharmonic
and harmonic excitation ports. The NRR circuit consumes zero DC power and
covers two communication frequency plans interchangeably, which makes it a
premier technique compared to the conventional ultra-wideband (UWB)
localization system and conventional single-band nonlinear passive circuitry.
The latter is narrowband due to the tunning limitation of the nonlinear
varactor while the former is power-hungry approach with complex hardware
requirements.
| [{'version': 'v1', 'created': 'Fri, 29 Oct 2021 06:44:20 GMT'}] | 2021-11-01 | [array(['Pahlavan', 'Payman', ''], dtype=object)
array(['Ebrahimi', 'Najme', ''], dtype=object)] |
387 | 1312.4114 | Egor Ianovski | Egor Ianovski, Luke Ong | EGuaranteeNash for Boolean Games is NEXP-Hard | null | null | null | null | cs.GT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Boolean games are an expressive and natural formalism through which to
investigate problems of strategic interaction in multiagent systems. Although
they have been widely studied, almost all previous work on Nash equilibria in
Boolean games has focused on the restricted setting of pure strategies. This is
a shortcoming as finite games are guaranteed to have at least one equilibrium
in mixed strategies, but many simple games fail to have pure strategy
equilibria at all. We address this by showing that a natural decision problem
about mixed equilibria: determining whether a Boolean game has a mixed strategy
equilibrium that guarantees every player a given payoff, is NEXP-hard.
Accordingly, the $\epsilon$ variety of the problem is NEXP-complete. The proof
can be adapted to show coNEXP-hardness of a similar question: whether all Nash
equilibria of a Boolean game guarantee every player at least the given payoff.
| [{'version': 'v1', 'created': 'Sun, 15 Dec 2013 06:36:40 GMT'}] | 2013-12-17 | [array(['Ianovski', 'Egor', ''], dtype=object)
array(['Ong', 'Luke', ''], dtype=object)] |
388 | astro-ph/0208449 | Groenewegen | M.A.T. Groenewegen | Carbon stars in the Local Group | Unofficial proceedings of an invited talk at the Ringberg conference
on "The Chemical Evolution of Dwarf Galaxies". Slides are available at
http://www.ster.kuleuven.ac.be/~groen/presentation.html | null | null | null | astro-ph | null | The current status of carbon stars in the Local Group and beyond, is
discussed. Although many carbon stars and late M-stars have been identified in
Local Group galaxies, a coherent understanding in terms of the chemical
evolution- and star formation history of a galaxy is still largely lacking.
Although a few major new surveys have been carried out over the last three
years, the observational data is still incomplete in many respects: 1) for some
of the larger galaxies only a small fraction in area has been surveyed so far,
2) surveys have been conducted using different techniques, and some of the
older surveys are incomplete in bolometric magnitude, 3) only for some galaxies
is there information about the late M-star population, or it is sometimes
unpublished even when the data is available, 4) not all galaxies in the Local
Group have been surveyed, 5) especially for some of the older work insufficient
data is available to determine bolometric magnitudes. I have correlated carbon
star positions with the 2MASS 2nd incremental data release to obtain $JHK$, and
bolometric magnitudes, to remedy this situation in some cases.
From the existing observations one can derive the following: the formation of
carbon stars is both a function of metallicity and star-formation history. In
galaxies with a similar star formation history, there will be relatively more
carbon stars formed in the system with the lower metallicity. On the other
hand, the scarcity of AGB type carbon stars in some galaxies with the lowest
metallicity indicates that these systems have had a low, if any, star-formation
over the last few Gyrs.
| [{'version': 'v1', 'created': 'Sat, 24 Aug 2002 11:50:39 GMT'}] | 2007-05-23 | [array(['Groenewegen', 'M. A. T.', ''], dtype=object)] |
389 | hep-ex/9811021 | Brunner | ALEPH collaboration | Study of D0-Dbar0 mixing and D0 doubly cabibbo-suppressed decays | 14 pages, 5 figures | Phys.Lett.B436:211-221,1998 | 10.1016/S0370-2693(98)00946-0 | CERN-EP/98-118 | hep-ex | null | Using a sample of four million hadronic Z events collected in ALEPH from 1991
to 1995, the decays D*+ -> D0pi^+_s, with D0 decaying to K-pi+ or to K+pi-, are
studied. The relative branching ratio B(D0 -> K+pi-)/B(D0 -> K-pi+) is measured
to be (1.84+-0.59(stat.)+-0.34(syst.))%. The two possible contributions to the
D0 -> K+pi- decay, doubly cabibbo-suppressed decays and D0-Dbar0 mixing, are
disentangled by measuring the proper-time ditribution of the reconstructed
D0's. Assuming no interference between the two processes, the upper limit
obtained on the mixing rate is 0.92% at 95% CL. The possible effect of
interference between the two amplitudes is also assessed.
| [{'version': 'v1', 'created': 'Wed, 11 Nov 1998 13:14:37 GMT'}] | 2012-08-27 | [array(['ALEPH collaboration', '', ''], dtype=object)] |
390 | 1703.09139 | Tomoaki Matsumoto | Tomoaki Matsumoto, Masahiro N. Machida, and Shu-ichiro Inutsuka | Circumstellar disks and outflows in turbulent molecular cloud cores:
possible formation mechanism for misaligned systems | 14 pages, 15 figures, Accepted by ApJ | null | 10.3847/1538-4357/aa6a1c | null | astro-ph.SR astro-ph.GA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the formation of circumstellar disks and outflows subsequent
to the collapse of molecular cloud cores with the magnetic field and
turbulence. Numerical simulations are performed by using an adaptive mesh
refinement to follow the evolution up to $\sim 1000$~yr after the formation of
a protostar. In the simulations, circumstellar disks are formed around the
protostars; those in magnetized models are considerably smaller than those in
nonmagnetized models, but their size increases with time. The models with
stronger magnetic field tends to produce smaller disks. During evolution in the
magnetized models, the mass ratios of a disk to a protostar is approximately
constant at $\sim 1-10$\%. The circumstellar disks are aligned according to
their angular momentum, and the outflows accelerate along the magnetic field on
the $10-100$~au scale; this produces a disk that is misaligned with the
outflow. The outflows are classified into two types: a magneto-centrifugal wind
and a spiral flow. In the latter, because of the geometry, the axis of rotation
is misaligned with the magnetic field. The magnetic field has an internal
structure in the cloud cores, which also causes misalignment between the
outflows and the magnetic field on the scale of the cloud core. The
distribution of the angular momentum vectors in a core also has a non-monotonic
internal structure. This should create a time-dependent accretion of angular
momenta onto the circumstellar disk. Therefore, the circumstellar disks are
expected to change their orientation as well as their sizes in the long-term
evolutions.
| [{'version': 'v1', 'created': 'Mon, 27 Mar 2017 15:15:29 GMT'}
{'version': 'v2', 'created': 'Fri, 7 Apr 2017 18:18:35 GMT'}] | 2017-04-26 | [array(['Matsumoto', 'Tomoaki', ''], dtype=object)
array(['Machida', 'Masahiro N.', ''], dtype=object)
array(['Inutsuka', 'Shu-ichiro', ''], dtype=object)] |
391 | hep-th/0211227 | Dmitri Ryzhikh | L. V. Laperashvili (ITEP, Moscow, Russia) | Generalized Duality Symmetry of Non-Abelian Theories | 11 pages | null | null | null | hep-th | null | The quantum Yang-Mills theory describing dual ($\tilde g$) and non-dual ($g$)
charges and revealing the generalized duality symmetry was developed by analogy
with the Zwanziger formalism in QED.
| [{'version': 'v1', 'created': 'Sat, 23 Nov 2002 17:36:38 GMT'}
{'version': 'v2', 'created': 'Thu, 26 Dec 2002 17:28:14 GMT'}
{'version': 'v3', 'created': 'Fri, 27 Dec 2002 15:40:21 GMT'}] | 2007-05-23 | [array(['Laperashvili', 'L. V.', '', 'ITEP, Moscow, Russia'], dtype=object)] |
392 | 2006.04666 | Nayeon Lee | Nayeon Lee, Yejin Bang, Andrea Madotto, Pascale Fung | Misinformation Has High Perplexity | null | null | null | null | cs.CL cs.AI cs.LG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Debunking misinformation is an important and time-critical task as there
could be adverse consequences when misinformation is not quashed promptly.
However, the usual supervised approach to debunking via misinformation
classification requires human-annotated data and is not suited to the fast
time-frame of newly emerging events such as the COVID-19 outbreak. In this
paper, we postulate that misinformation itself has higher perplexity compared
to truthful statements, and propose to leverage the perplexity to debunk false
claims in an unsupervised manner. First, we extract reliable evidence from
scientific and news sources according to sentence similarity to the claims.
Second, we prime a language model with the extracted evidence and finally
evaluate the correctness of given claims based on the perplexity scores at
debunking time. We construct two new COVID-19-related test sets, one is
scientific, and another is political in content, and empirically verify that
our system performs favorably compared to existing systems. We are releasing
these datasets publicly to encourage more research in debunking misinformation
on COVID-19 and other topics.
| [{'version': 'v1', 'created': 'Mon, 8 Jun 2020 15:13:44 GMT'}
{'version': 'v2', 'created': 'Wed, 10 Jun 2020 08:49:30 GMT'}] | 2020-06-11 | [array(['Lee', 'Nayeon', ''], dtype=object)
array(['Bang', 'Yejin', ''], dtype=object)
array(['Madotto', 'Andrea', ''], dtype=object)
array(['Fung', 'Pascale', ''], dtype=object)] |
393 | 1702.08399 | Alex Samoletov | A. Samoletov and B. Vasiev | Dynamic principle for ensemble control tools | null | null | 10.1063/1.4993976 | null | physics.data-an | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Dynamical equations describing physical systems at statistical equilibrium
are commonly extended by mathematical tools called "thermostats". These tools
are designed for sampling ensembles of statistical mechanics. We propose a
dynamic principle for derivation of stochastic and deterministic thermostats.
It is based on fundamental physical assumptions such that the canonical measure
is invariant for the thermostat dynamics. This is a clear advantage over a
range of recently proposed and widely discussed in the literature mathematical
thermostat schemes. Following justification of the proposed principle we show
its generality and usefulness for modeling a wide range of natural systems.
| [{'version': 'v1', 'created': 'Mon, 27 Feb 2017 17:47:40 GMT'}
{'version': 'v2', 'created': 'Wed, 5 Jul 2017 06:15:14 GMT'}
{'version': 'v3', 'created': 'Sun, 15 Oct 2017 14:04:19 GMT'}] | 2018-01-17 | [array(['Samoletov', 'A.', ''], dtype=object)
array(['Vasiev', 'B.', ''], dtype=object)] |
394 | 2206.03769 | Adam Rancon | I. Balog, A. Ran\c{c}on, B. Delamotte | Critical probability distributions of the order parameter from the
functional renormalization group | 5+5 pages, 3+5 figures. Changed title compared to v1. Corresponds to
published version, some typos corrected | Phys. Rev. Lett. 129, 210602 (2022) | 10.1103/PhysRevLett.129.210602 | null | cond-mat.stat-mech hep-th | http://creativecommons.org/licenses/by/4.0/ | We show that the functional renormalization group (FRG) allows for the
calculation of the probability distribution function of the sum of strongly
correlated random variables. On the example of the three-dimensional Ising
model at criticality and using the simplest implementation of the FRG, we
compute the probability distribution functions of the order parameter or
equivalently its logarithm, called the rate functions in large deviations
theory. We compute the entire family of universal scaling functions, obtained
in the limit where the system size $L$ and the correlation length of the
infinite system $\xi_{\infty}$ diverge, with the ratio $\zeta=L/\xi_{\infty}$
held fixed. It compares very accurately with numerical simulations.
| [{'version': 'v1', 'created': 'Wed, 8 Jun 2022 09:31:39 GMT'}
{'version': 'v2', 'created': 'Tue, 10 Jan 2023 09:02:19 GMT'}] | 2023-01-11 | [array(['Balog', 'I.', ''], dtype=object)
array(['Rançon', 'A.', ''], dtype=object)
array(['Delamotte', 'B.', ''], dtype=object)] |
395 | 2306.08305 | Yongchun Xu | Yongchun Xu, Jie Yang, Zengtao Kuang, Qun Huang, Wei Huang, Heng Hu | Quantum Computing Enhanced Distance-Minimizing Data-Driven Computational
Mechanics | 22 pages, 14 figures | null | null | null | cs.CE | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The distance-minimizing data-driven computational mechanics has great
potential in engineering applications by eliminating material modeling error
and uncertainty. In this computational framework, the solution-seeking
procedure relies on minimizing the distance between the constitutive database
and the conservation law. However, the distance calculation is time-consuming
and often takes up most of the computational time in the case of a huge
database. In this paper, we show how to use quantum computing to enhance
data-driven computational mechanics by exponentially reducing the computational
complexity of distance calculation. The proposed method is not only validated
on the quantum computer simulator Qiskit, but also on the real quantum computer
from OriginQ. We believe that this work represents a promising step towards
integrating quantum computing into data-driven computational mechanics.
| [{'version': 'v1', 'created': 'Wed, 14 Jun 2023 07:22:52 GMT'}] | 2023-06-21 | [array(['Xu', 'Yongchun', ''], dtype=object)
array(['Yang', 'Jie', ''], dtype=object)
array(['Kuang', 'Zengtao', ''], dtype=object)
array(['Huang', 'Qun', ''], dtype=object)
array(['Huang', 'Wei', ''], dtype=object)
array(['Hu', 'Heng', ''], dtype=object)] |
396 | hep-ph/0001269 | Giuseppe Degrassi | G D'Agostini and G. Degrassi | Constraining the Higgs boson mass through the combination of direct
search and precision measurement results | Contributed paper to the workshop on Confidence Limit, CERN, Geneva
Jan. 17-18, 2000. 12 pages, 2 figures | null | null | null | hep-ph | null | We show that the likelihood ratio of Higgs search experiments is a form to
report the experimental results suitable to be combined with the information
from precision measurements to obtain a joint constraint on the Higgs mass. We
update our previous combined analysis using the new results on direct searches
and recent precision measurements, including also the Z0 leptonic partial width
result. The method is also improved to take into account small non linearity
effects in the theoretical formulae. We find an expected value for the Higgs
mass around 160-170 GeV with an expectation uncertainty, quantified by the
standard deviation of the distribution, of about 50-60 GeV. The 95% probability
upper limit comes out to be around 260-290 GeV.
| [{'version': 'v1', 'created': 'Wed, 26 Jan 2000 13:43:05 GMT'}] | 2007-05-23 | [array(["D'Agostini", 'G', ''], dtype=object)
array(['Degrassi', 'G.', ''], dtype=object)] |
397 | 2201.00495 | Oleg Kiselyov | Oleg Kiselyov (Tohoku University, Japan) and Jeremy Yallop (University
of Cambridge, UK) | let (rec) insertion without Effects, Lights or Magic | Peer-reviewed and accepted for presentation as a short paper at PEPM
2022 | null | null | null | cs.PL cs.SC | http://creativecommons.org/licenses/by/4.0/ | Let insertion in program generation is producing code with definitions
(let-statements). Although definitions precede uses in generated code, during
code generation `uses' come first: we might not even know a definition is
needed until we encounter a reoccurring expression. Definitions are thus
generated `in hindsight', which explains why this process is difficult to
understand and implement -- even more so for parameterized, recursive and
mutually recursive definitions.
We have earlier presented an interface for let(rec) insertion -- i.e. for
generating (mutually recursive) definitions. We demonstrated its expressiveness
and applications, but not its implementation, which relied on effects and
compiler magic.
We now show how one can understand let insertion, and hence implement it in
plain OCaml. We give the first denotational semantics of let(rec)-insertion,
which does not rely on any effects at all. The formalization has guided the
implementation of let(rec) insertion in the current version of MetaOCaml.
| [{'version': 'v1', 'created': 'Mon, 3 Jan 2022 06:32:39 GMT'}] | 2022-01-04 | [array(['Kiselyov', 'Oleg', '', 'Tohoku University, Japan'], dtype=object)
array(['Yallop', 'Jeremy', '', 'University\n of Cambridge, UK'],
dtype=object) ] |
398 | 2007.12027 | M H Mortad Ph.D. | Mohammed Hichem Mortad | Unbounded operators: (square) roots, nilpotence, closability and some
related invertibility results | 34 pages | null | null | null | math.FA math.OA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we are mainly concerned with studying arbitrary unbounded
square roots of linear operators as well as some of their basic properties. The
paper contains many examples and counterexamples. As an illustration, we give
explicit everywhere defined unbounded non-closable $nth$ roots of the identity
operator as well as the zero operator. We also show a non-closable unbounded
operator without any non-closable square root. Among other consequences, we
have a way of finding everywhere defined bijective operators, everywhere
defined operators which are surjective without being injective and everywhere
defined operators which are injective without being surjective. Some related
results on nilpotence are also given.
| [{'version': 'v1', 'created': 'Thu, 23 Jul 2020 14:11:55 GMT'}
{'version': 'v2', 'created': 'Mon, 27 Jul 2020 08:13:21 GMT'}] | 2020-07-28 | [array(['Mortad', 'Mohammed Hichem', ''], dtype=object)] |
399 | 1206.4907 | Francesco Knechtli | Nikos Irges, Francesco Knechtli and Kyoko Yoneyama | Mean-Field Gauge Interactions in Five Dimensions II. The Orbifold | 33 pages, 8 figures; text improved; references corrected; version
accepted for publication in Nucl. Phys. B | null | 10.1016/j.nuclphysb.2012.08.011 | WUB/12-14 | hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study Gauge-Higgs Unification in five dimensions on the lattice by means
of the mean-field expansion. We formulate it for the case of an SU(2) pure
gauge theory and orbifold boundary conditions along the extra dimension, which
explicitly break the gauge symmetry to U(1) on the boundaries. Our main result
is that the gauge boson mass computed from the static potential along
four-dimensional hyperplanes is nonzero implying spontaneous symmetry breaking.
This observation supports earlier data from Monte Carlo simulations [12].
| [{'version': 'v1', 'created': 'Thu, 21 Jun 2012 15:06:28 GMT'}
{'version': 'v2', 'created': 'Wed, 15 Aug 2012 11:20:51 GMT'}
{'version': 'v3', 'created': 'Mon, 20 Aug 2012 10:08:13 GMT'}] | 2015-06-05 | [array(['Irges', 'Nikos', ''], dtype=object)
array(['Knechtli', 'Francesco', ''], dtype=object)
array(['Yoneyama', 'Kyoko', ''], dtype=object)] |