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400 | 1606.05267 | Martina Donnari | M. Donnari, M. Arca-Sedda, M. Merafina | Can dark energy explain the observed outflow in galaxy clusters? | 2 pages, 3 figures, 2 tables. To be published in the proceedings of
51th Rencontres de Moriond | null | null | null | astro-ph.CO astro-ph.GA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recent observations of the Virgo cluster and the Local Group suggested that
some galaxies are flowing out from their parent cluster. This may be the
signature that dark energy (DE) acts significantly also on small cosmological
scales. By means of direct N-body simulations we performed several simulations,
in which the effect of DE and gravity are taken into account, aiming to
determine whether DE can produce an outflow of galaxies compatible with
observations. Comparing the different simulations, our results suggest that the
observed outflow of galaxies is likely due to the local effect of DE.
| [{'version': 'v1', 'created': 'Wed, 15 Jun 2016 08:20:18 GMT'}] | 2016-06-17 | [array(['Donnari', 'M.', ''], dtype=object)
array(['Arca-Sedda', 'M.', ''], dtype=object)
array(['Merafina', 'M.', ''], dtype=object)] |
401 | 2105.03173 | Luigi Riso | Luigi Riso | Use of High Dimensional Modeling for automatic variables selection: the
best path algorithm | null | null | null | null | stat.ML cs.LG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This paper presents a new algorithm for automatic variables selection. In
particular, using the Graphical Models properties it is possible to develop a
method that can be used in the contest of large dataset. The advantage of this
algorithm is that can be combined with different forecasting models. In this
research we have used the OLS method and we have compared the result with the
LASSO method.
| [{'version': 'v1', 'created': 'Fri, 7 May 2021 11:33:06 GMT'}
{'version': 'v2', 'created': 'Fri, 14 Jan 2022 10:59:20 GMT'}] | 2022-01-17 | [array(['Riso', 'Luigi', ''], dtype=object)] |
402 | 1707.07972 | Giancarlo Strinati Calvanese | S. Simonucci and G. Calvanese Strinati | Non-local equation for the superconducting gap parameter | null | null | 10.1103/PhysRevB.96.054502 | null | cond-mat.supr-con | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The properties are considered in detail of a non-local (integral) equation
for the superconducting gap parameter, which is obtained by a coarse-graining
procedure applied to the Bogoliubov-deGennes (BdG) equations over the whole
coupling-vs-temperature phase diagram associated with the superfluid phase. It
is found that the limiting size of the coarse-graining procedure, which is
dictated by the range of the kernel of this integral equation, corresponds to
the size of the Cooper pairs over the whole coupling-vs-temperature phase
diagram up to the critical temperature, even when Cooper pairs turn into
composite bosons on the BEC side of the BCS-BEC crossover. A practical method
is further implemented to solve numerically this integral equation in an
efficient way, which is based on a novel algorithm for calculating the Fourier
transforms. Application of this method to the case of an isolated vortex,
throughout the BCS-BEC crossover and for all temperatures in the superfluid
phase, helps clarifying the nature of the length scales associated with a
single vortex and the kinds of details that are in practice disposed off by the
coarse-graining procedure on the BdG equations.
| [{'version': 'v1', 'created': 'Tue, 25 Jul 2017 13:05:38 GMT'}] | 2017-09-13 | [array(['Simonucci', 'S.', ''], dtype=object)
array(['Strinati', 'G. Calvanese', ''], dtype=object)] |
403 | 1401.0344 | Xin-Fa Deng | Xin-Fa Deng | Environmental dependence of different colors in the CMASS sample of the
SDSS DR9 | 12 pages, 6 figures, accepted by RAA | null | 10.1088/1674-4527/14/5/005 | null | astro-ph.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this study, I investigate the environmental dependence of galaxy colors in
the CMASS sample of the Sloan Digital Sky Survey Data Release 9 (SDSS DR9). To
decrease the radial selection effect, I divide the CMASS sample into subsamples
with a redshift binning size of 0.01 and analyze the environmental dependence
of the u-r, u-g, g-r, r-i and i-z colors for these subsamples in each redshift
bin. Statistical analysis shows that all the five colors weakly correlate with
the local environment, which may mean that the environmental processes
responsible for a galaxy's properties proceed slowly over cosmic time.
| [{'version': 'v1', 'created': 'Wed, 1 Jan 2014 22:47:06 GMT'}] | 2015-06-18 | [array(['Deng', 'Xin-Fa', ''], dtype=object)] |
404 | cond-mat/0308413 | C. A. Busser | C.A. B\"usser, Adriana Moreo and Elbio Dagotto | Unexpected Conductance Dip in the Kondo Regime of Linear Arrays of
Quantum Dots | null | null | 10.1103/PhysRevB.70.035402 | null | cond-mat.mes-hall cond-mat.str-el | null | Using exact-diagonalization of small clusters and Dyson equation embedding
techniques, the conductance $G$ of linear arrays of quantum dots is
investigated. The Hubbard interaction induces Kondo peaks at low temperatures
for an odd number of dots. Remarkably, the Kondo peak is split in half by a
deep minimum, and the conductance vanishes at one value of the gate voltage.
Tentative explanations for this unusual effect are proposed, including an
interference process between two channels contributing to $G$, with one more
and one less particle than the exactly-solved cluster ground-state. The Hubbard
interaction and fermionic statistics of electrons also appear to be important
to understand this phenomenon. Although most of the calculations used a
particle-hole symmetric Hamiltonian and formalism, results also presented here
show that the conductance dip exists even when this symmetry is broken. The
conductance cancellation effect obtained using numerical techniques is
potentially interesting, and other many-body techniques should be used to
confirm its existence.
| [{'version': 'v1', 'created': 'Wed, 20 Aug 2003 19:32:06 GMT'}] | 2009-11-10 | [array(['Büsser', 'C. A.', ''], dtype=object)
array(['Moreo', 'Adriana', ''], dtype=object)
array(['Dagotto', 'Elbio', ''], dtype=object)] |
405 | 1801.05486 | Ignacio Mart\'in-Navarro | Ignacio Martin-Navarro, Alexandre Vazdekis, Jesus Falcon-Barroso,
Francesco La Barbera, Akin Yildirim, and Glenn van de Ven | Timing the formation and assembly of early-type galaxies via spatially
resolved stellar populations analysis | Accepted for publication in MNRAS | null | 10.1093/mnras/stx3346 | null | astro-ph.GA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | To investigate star formation and assembly processes of massive galaxies, we
present here a spatially-resolved stellar populations analysis of a sample of
45 elliptical galaxies (Es) selected from the CALIFA survey. We find rather
flat age and [Mg/Fe] radial gradients, weakly dependent on the effective
velocity dispersion of the galaxy within half-light radius. However, our
analysis shows that metallicity gradients become steeper with increasing galaxy
velocity dispersion. In addition, we have homogeneously compared the stellar
populations gradients of our sample of Es to a sample of nearby relic galaxies,
i.e., local remnants of the high-z population of red nuggets. This comparison
indicates that, first, the cores of present-day massive galaxies were likely
formed in gas-rich, rapid star formation events at high redshift (z>2). This
led to radial metallicity variations steeper than observed in the local
Universe, and positive [Mg/Fe] gradients. Second, our analysis also suggests
that a later sequence of minor dry mergers, populating the outskirts of
early-type galaxies (ETGs), flattened the pristine [Mg/Fe] and metallicity
gradients. Finally, we find a tight age-[Mg/Fe] relation, supporting that the
duration of the star formation is the main driver of the [Mg/Fe] enhancement in
massive ETGs. However, the star formation time-scale alone is not able to fully
explain our [Mg/Fe] measurements. Interestingly, our results match the expected
effect that a variable stellar initial mass function would have on the [Mg/Fe]
ratio.
| [{'version': 'v1', 'created': 'Tue, 16 Jan 2018 21:26:45 GMT'}] | 2018-01-18 | [array(['Martin-Navarro', 'Ignacio', ''], dtype=object)
array(['Vazdekis', 'Alexandre', ''], dtype=object)
array(['Falcon-Barroso', 'Jesus', ''], dtype=object)
array(['La Barbera', 'Francesco', ''], dtype=object)
array(['Yildirim', 'Akin', ''], dtype=object)
array(['van de Ven', 'Glenn', ''], dtype=object)] |
406 | 1112.1733 | Petter Holme | Sungmin Lee, Petter Holme, Zhi-Xi Wu | Cooperation, structure and hierarchy in multiadaptive games | null | Phys. Rev. E. 84, 061148 (2011) | 10.1103/PhysRevE.84.061148 | null | q-bio.PE | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Game-theoretical models where the rules of the game and the interaction
structure both coevolves with the game dynamics -- multiadaptive games --
capture very flexible situations where cooperation among selfish agents can
emerge. In this work, we will discuss a multiadaptive model presented in a
recent Letter [Phys. Rev. Lett. 106, 028702 (2011)], and generalizations of it.
The model captures a non-equilibrium situation where social unrest increases
the incentive to cooperate and, simultaneously, agents are partly free to
influence with whom they interact. First, we investigate the details of how the
feedback from the behavior of agents determines the emergence of cooperation
and hierarchical contact structures. We also study the stability of the system
to different types of noise, and find that different regions of parameter space
show very different response. Some types of noise can destroy an all-cooperator
state. If, on the other hand, hubs are stable, then so is the all-C state.
Finally, we investigate the dependence of the ratio between the timescales of
strategy updates and the evolution of the interaction structure. We find that a
comparatively fast strategy dynamics is a prerequisite for the emergence of
cooperation.
| [{'version': 'v1', 'created': 'Wed, 7 Dec 2011 23:30:13 GMT'}] | 2012-10-10 | [array(['Lee', 'Sungmin', ''], dtype=object)
array(['Holme', 'Petter', ''], dtype=object)
array(['Wu', 'Zhi-Xi', ''], dtype=object)] |
407 | 0912.3507 | Sergio Iguri | Sergio Iguri, Toufik Mansour | Some recursive formulas for Selberg-type integrals | 11 pages. To appear in Jour. Phys. A | J. Phys. A: Math. Theor. 43 065201 (2010) | 10.1088/1751-8113/43/6/065201 | null | math-ph hep-th math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A set of recursive relations satisfied by Selberg-type integrals involving
monomial symmetric polynomials are derived, generalizing previously known
results. These formulas provide a well-defined algorithm for computing
Selberg-Schur integrals whenever the Kostka numbers relating Schur functions
and the corresponding monomial polynomials are explicitly known. We illustrate
the usefulness of our results discussing some interesting examples.
| [{'version': 'v1', 'created': 'Thu, 17 Dec 2009 20:17:57 GMT'}] | 2010-04-06 | [array(['Iguri', 'Sergio', ''], dtype=object)
array(['Mansour', 'Toufik', ''], dtype=object)] |
408 | 1705.07121 | Mansaf Alam Dr | Kashish A. Shakil, Farhana J. Zareen, Mansaf Alam and Suraiya Jabin | BAMHealthCloud: A Biometric Authentication and Data Management System
for Healthcare Data in Cloud | null | null | null | null | cs.CR cs.CY cs.DC | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Advancements in healthcare industry with new technology and population growth
has given rise to security threat to our most personal data. The healthcare
data management system consists of records in different formats such as text,
numeric, pictures and videos leading to data which is big and unstructured.
Also, hospitals have several branches at different locations throughout a
country and overseas. In view of these requirements a cloud based healthcare
management system can be an effective solution for efficient health care data
management. One of the major concerns of a cloud based healthcare system is the
security aspect. It includes theft to identity, tax fraudulence, insurance
frauds, medical frauds and defamation of high profile patients. Hence, a secure
data access and retrieval is needed in order to provide security of critical
medical records in health care management system. Biometric authentication
mechanism is suitable in this scenario since it overcomes the limitations of
token theft and forgetting passwords in conventional token id-password
mechanism used for providing security. It also has high accuracy rate for
secure data access and retrieval. In this paper we propose BAMHealthCloud which
is a cloud based system for management of healthcare data, it ensures security
of data through biometric authentication. It has been developed after
performing a detailed case study on healthcare sector in a developing country.
Training of the signature samples for authentication purpose has been performed
in parallel on hadoop MapReduce framework using Resilient Backpropagation
neural network. From rigorous experiments it can be concluded that it achieves
a speedup of 9x, Equal error rate (EER) of 0.12, sensitivity of 0.98 and
specificity of 0.95 as compared to other approaches existing in literature.
| [{'version': 'v1', 'created': 'Fri, 19 May 2017 11:00:40 GMT'}] | 2017-05-23 | [array(['Shakil', 'Kashish A.', ''], dtype=object)
array(['Zareen', 'Farhana J.', ''], dtype=object)
array(['Alam', 'Mansaf', ''], dtype=object)
array(['Jabin', 'Suraiya', ''], dtype=object)] |
409 | 0910.1522 | Marc Dietrich | M. Dietrich, G. Thummes | Two-stage high frequency pulse tube cooler for refrigeration at 25 K | null | Cryogenics50:281-286, 2010 | 10.1016/j.cryogenics.2010.01.010 | null | physics.ins-det | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A two-stage Stirling-type U-shape pulse tube cryocooler driven by a 10
kW-class linear compressor was designed, built and tested. A special feature of
the cold head is the absence of a heat exchanger at the cold end of the first
stage, since the intended application requires no cooling power at this
intermediate temperature. Simulations where done using Sage-software to find
optimum operating conditions and cold head geometry. Flow-impedance matching
was required to connect the compressor designed for 60 Hz operation to the 40
Hz cold head. A cooling power of 12.9 W at 25 K with an electrical input power
of 4.6 kW has been achieved up to now. The lowest temperature reached is 13.7
K.
| [{'version': 'v1', 'created': 'Thu, 8 Oct 2009 14:56:28 GMT'}
{'version': 'v2', 'created': 'Thu, 17 Dec 2009 15:41:25 GMT'}] | 2014-11-20 | [array(['Dietrich', 'M.', ''], dtype=object)
array(['Thummes', 'G.', ''], dtype=object)] |
410 | 2304.05966 | Vasileios Theodorou | Ioannis Kalogeropoulos, Maria Eleftheria Vlontzou, Nikos
Psaromanolakis, Eleni Zarogianni, Vasileios Theodorou | EdgeDS: Data Spaces enabled Multi-access Edge Computing | null | null | null | null | cs.NI | http://creativecommons.org/licenses/by/4.0/ | The potential of Edge Computing technologies is yet to be exploited for
multi-domain, multi-party data-driven systems. One aspect that needs to be
tackled for the realization of envisioned open edge Ecosystems, is the secure
and trusted exchange of data services among diverse stakeholders. In this work,
we present a novel approach for integrating mechanisms for trustworthy and
sovereign data exchange, into Multi-access Edge Computing (MEC) environments.
To this end, we introduce an architecture that extends the ETSI MEC
Architectural Framework with artifacts from the International Data Spaces
Reference Architecture Model, accompanied by processes that automatically
enrich Edge Computing applications with data space capabilities in an
as-a-service paradigm. To validate our approach, we implement an open-source
prototype solution and we conduct experiments that showcase its functionality
and scalability. To our knowledge, this is one of the first concrete
architectural specifications for enabling data space features in MEC systems.
| [{'version': 'v1', 'created': 'Wed, 12 Apr 2023 16:41:21 GMT'}] | 2023-04-13 | [array(['Kalogeropoulos', 'Ioannis', ''], dtype=object)
array(['Vlontzou', 'Maria Eleftheria', ''], dtype=object)
array(['Psaromanolakis', 'Nikos', ''], dtype=object)
array(['Zarogianni', 'Eleni', ''], dtype=object)
array(['Theodorou', 'Vasileios', ''], dtype=object)] |
411 | cond-mat/0510152 | Michael Pustilnik | M. Pustilnik, L. Borda | Phase transition, spin-charge separation, and spin filtering in a
quantum dot | null | Phys. Rev. B 73, 201301(R) (2006) | 10.1103/PhysRevB.73.201301 | null | cond-mat.mes-hall | null | We consider low temperature transport through a lateral quantum dot
asymmetrically coupled to two conducting leads, and tuned to the mixed-valence
region separating two adjacent Coulomb blockade valleys with spin S=1/2 and S=1
on the dot. We demonstrate that this system exhibits a quantum phase transition
driven by the gate voltage. In the vicinity of the transition the spin on the
dot is quantized, even though the fluctuations of charge are strong. The
spin-charge separation leads to an unusual Fano-like dependence of the
conductance on the gate voltage and to an almost perfect spin polarization of
the current through the dot in the presence of a magnetic field.
| [{'version': 'v1', 'created': 'Thu, 6 Oct 2005 16:59:07 GMT'}
{'version': 'v2', 'created': 'Sat, 1 Apr 2006 20:04:58 GMT'}] | 2007-05-23 | [array(['Pustilnik', 'M.', ''], dtype=object)
array(['Borda', 'L.', ''], dtype=object)] |
412 | 2108.08560 | Florian Merkle | Florian Merkle, Maximilian Samsinger, Pascal Sch\"ottle | Pruning in the Face of Adversaries | null | null | null | null | cs.LG cs.CR | http://creativecommons.org/licenses/by/4.0/ | The vulnerability of deep neural networks against adversarial examples -
inputs with small imperceptible perturbations - has gained a lot of attention
in the research community recently. Simultaneously, the number of parameters of
state-of-the-art deep learning models has been growing massively, with
implications on the memory and computational resources required to train and
deploy such models. One approach to control the size of neural networks is
retrospectively reducing the number of parameters, so-called neural network
pruning. Available research on the impact of neural network pruning on the
adversarial robustness is fragmentary and often does not adhere to established
principles of robustness evaluation. We close this gap by evaluating the
robustness of pruned models against L-0, L-2 and L-infinity attacks for a wide
range of attack strengths, several architectures, data sets, pruning methods,
and compression rates. Our results confirm that neural network pruning and
adversarial robustness are not mutually exclusive. Instead, sweet spots can be
found that are favorable in terms of model size and adversarial robustness.
Furthermore, we extend our analysis to situations that incorporate additional
assumptions on the adversarial scenario and show that depending on the
situation, different strategies are optimal.
| [{'version': 'v1', 'created': 'Thu, 19 Aug 2021 09:06:16 GMT'}] | 2021-08-20 | [array(['Merkle', 'Florian', ''], dtype=object)
array(['Samsinger', 'Maximilian', ''], dtype=object)
array(['Schöttle', 'Pascal', ''], dtype=object)] |
413 | 2012.13522 | Jianwen Xie | Jianwen Xie, Zilong Zheng, Ruiqi Gao, Wenguan Wang, Song-Chun Zhu,
Ying Nian Wu | Generative VoxelNet: Learning Energy-Based Models for 3D Shape Synthesis
and Analysis | 16 pages. IEEE Transactions on Pattern Analysis and Machine
Intelligence (TPAMI) 2020. arXiv admin note: substantial text overlap with
arXiv:1804.00586 | null | null | null | cs.CV | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | 3D data that contains rich geometry information of objects and scenes is
valuable for understanding 3D physical world. With the recent emergence of
large-scale 3D datasets, it becomes increasingly crucial to have a powerful 3D
generative model for 3D shape synthesis and analysis. This paper proposes a
deep 3D energy-based model to represent volumetric shapes. The maximum
likelihood training of the model follows an "analysis by synthesis" scheme. The
benefits of the proposed model are six-fold: first, unlike GANs and VAEs, the
model training does not rely on any auxiliary models; second, the model can
synthesize realistic 3D shapes by Markov chain Monte Carlo (MCMC); third, the
conditional model can be applied to 3D object recovery and super resolution;
fourth, the model can serve as a building block in a multi-grid modeling and
sampling framework for high resolution 3D shape synthesis; fifth, the model can
be used to train a 3D generator via MCMC teaching; sixth, the unsupervisedly
trained model provides a powerful feature extractor for 3D data, which is
useful for 3D object classification. Experiments demonstrate that the proposed
model can generate high-quality 3D shape patterns and can be useful for a wide
variety of 3D shape analysis.
| [{'version': 'v1', 'created': 'Fri, 25 Dec 2020 06:09:36 GMT'}] | 2020-12-29 | [array(['Xie', 'Jianwen', ''], dtype=object)
array(['Zheng', 'Zilong', ''], dtype=object)
array(['Gao', 'Ruiqi', ''], dtype=object)
array(['Wang', 'Wenguan', ''], dtype=object)
array(['Zhu', 'Song-Chun', ''], dtype=object)
array(['Wu', 'Ying Nian', ''], dtype=object)] |
414 | 1601.01573 | Mikko Laine | C. Christensen and M. Laine | Perturbative renormalization of the electric field correlator | 15 pages. v2: published version | null | 10.1016/j.physletb.2016.02.020 | null | hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The momentum diffusion coefficient of a heavy quark in a hot QCD plasma can
be extracted as a transport coefficient related to the correlator of two
colour-electric fields dressing a Polyakov loop. We determine the perturbative
renormalization factor for a particular lattice discretization of this
correlator within Wilson's SU(3) gauge theory, finding a ~12% NLO correction
for values of the bare coupling used in the current generation of simulations.
The impact of this result on existing lattice determinations is commented upon,
and a possibility for non-perturbative renormalization through the gradient
flow is pointed out.
| [{'version': 'v1', 'created': 'Thu, 7 Jan 2016 15:48:11 GMT'}
{'version': 'v2', 'created': 'Fri, 18 Mar 2016 16:14:33 GMT'}] | 2016-03-23 | [array(['Christensen', 'C.', ''], dtype=object)
array(['Laine', 'M.', ''], dtype=object)] |
415 | 1110.3948 | Claudio Codella | C. Codella, C. Ceccarelli, S. Bottinelli, M. Salez, S. Viti, B.
Lefloch, S. Cabrit, E. Caux, A. Faure, M. Vasta, L. Wiesenfeld | First detection of Hydrogen Chloride towards protostellar shocks | ApJ, in press | null | 10.1088/0004-637X/744/2/164 | null | astro-ph.GA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present the first detection of hydrogen chlorine in a protostellar shock,
by observing the fundamental transition at 626 GHz with the Herschel HIFI
spectrometer. We detected two of the three hyperfine lines, from which we
derived a line opacity < 1. Using a non-LTE LVG code, we constrained the HCl
column density, temperature and density of the emitting gas. The hypothesis
that the emission originates in the molecular cloud is ruled out, as it would
imply a too dense gas. Conversely, assuming that the emission originates in the
10"-15" size shocked gas previously observed at the IRAM PdB interferometer, we
obtain: N(HCl)=0.7-2 x 10(13) cm-2, temperature > 15 K and density > 3 x 10(5)
cm-3}. Combining with the Herschel HIFI CO(5-4) observations allows to further
constrain the gas density and temperature, 10(5)-10(6) cm-3 and 120-250 K, as
well as the HCl column density, 2 x 10(13) cm-2, and, finally, abundance: 3-6 x
10(-9). The estimated HCl abundance is consistent with that previously observed
in low- and high- mass protostars. This puzzling result in the L1157-B1 shock,
where species from volatile and refractory grains components are enhanced,
suggests either that HCl is not the main reservoir of chlorine in the gas
phase, against previous chemical models predictions, or that the elemental
chlorine abundance is low in L1157-B1. Astrochemical modelling suggests that
HCl is in fact formed in the gas phase, at low temperatures, prior to the
occurance of the shock, and that the latter does not enhance its abundance.
| [{'version': 'v1', 'created': 'Tue, 18 Oct 2011 12:06:32 GMT'}] | 2015-05-30 | [array(['Codella', 'C.', ''], dtype=object)
array(['Ceccarelli', 'C.', ''], dtype=object)
array(['Bottinelli', 'S.', ''], dtype=object)
array(['Salez', 'M.', ''], dtype=object)
array(['Viti', 'S.', ''], dtype=object)
array(['Lefloch', 'B.', ''], dtype=object)
array(['Cabrit', 'S.', ''], dtype=object)
array(['Caux', 'E.', ''], dtype=object)
array(['Faure', 'A.', ''], dtype=object)
array(['Vasta', 'M.', ''], dtype=object)
array(['Wiesenfeld', 'L.', ''], dtype=object)] |
416 | 1212.0408 | Serena Dipierro | Serena Dipierro, Andrea Pinamonti | Symmetry results for stable and monotone solutions to fibered systems of
PDEs | null | null | null | null | math.AP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the symmetry properties for solutions of elliptic systems of the
type {ll}-\dive(a_1(x,|\nabla u^1|(X))\nabla u^1(X))=F_{1}(x, u^1(X),...,
u^n(X)), ... -\dive(a_n(x,|\nabla u^n|(X))\nabla u^n(X))=F_{n}(x, u^1(X),...,
u^n(X)), where $x\in \R^m$ with $1\leq m< N$, $X=(x,y)\in \R^m\times \R^{N-m}$,
and $F_{1},..., F_{n}$ are the derivatives with respect to $\xi^1,..., \xi^n$
of some $F=F(x,\xi^1,..., \xi^n)$ such that for any $i=1,..., n$ and any fixed
$(x,\xi^1,..., \xi^{i-1},\xi^{i+1},..., \xi^n)\in \R^m\times \R^{n-1}$ the map
$\xi^i\to F(x,\xi^1,...,\xi^i,..., \xi^n)$ belongs to $C^2(\R)$. We obtain a
Poincar\'e-type formula for the solutions of the system and we use it to prove
a symmetry result both for stable and for monotone solutions.
| [{'version': 'v1', 'created': 'Mon, 3 Dec 2012 15:01:50 GMT'}] | 2012-12-04 | [array(['Dipierro', 'Serena', ''], dtype=object)
array(['Pinamonti', 'Andrea', ''], dtype=object)] |
417 | 2007.09308 | Kazuhiro Morimoto | Kazuhiro Morimoto, Ming-Lo Wu, Andrei Ardelean, Edoardo Charbon | Superluminal Motion-Assisted 4-Dimensional Light-in-Flight Imaging | 7 pages, 4 figures | Phys. Rev. X 11, 011005 (2021) | 10.1103/PhysRevX.11.011005 | null | physics.optics eess.IV | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Advances in high speed imaging techniques have opened new possibilities for
capturing ultrafast phenomena such as light propagation in air or through
media. Capturing light-in-flight in 3-dimensional xyt-space has been reported
based on various types of imaging systems, whereas reconstruction of
light-in-flight information in the fourth dimension z has been a challenge. We
demonstrate the first 4-dimensional light-in-flight imaging based on the
observation of a superluminal motion captured by a new time-gated megapixel
single-photon avalanche diode camera. A high resolution light-in-flight video
is generated with no laser scanning, camera translation, interpolation, nor
dark noise subtraction. A machine learning technique is applied to analyze the
measured spatio-temporal data set. A theoretical formula is introduced to
perform least-square regression, and extra-dimensional information is recovered
without prior knowledge. The algorithm relies on the mathematical formulation
equivalent to the superluminal motion in astrophysics, which is scaled by a
factor of a quadrillionth. The reconstructed light-in-flight trajectory shows a
good agreement with the actual geometry of the light path. Our approach could
potentially provide novel functionalities to high speed imaging applications
such as non-line-of-sight imaging and time-resolved optical tomography.
| [{'version': 'v1', 'created': 'Sat, 18 Jul 2020 01:56:45 GMT'}] | 2021-01-13 | [array(['Morimoto', 'Kazuhiro', ''], dtype=object)
array(['Wu', 'Ming-Lo', ''], dtype=object)
array(['Ardelean', 'Andrei', ''], dtype=object)
array(['Charbon', 'Edoardo', ''], dtype=object)] |
418 | 1908.10904 | Chuhong Mai | Chuhong Mai, Michael R. Line | Exploring Exoplanet Cloud Assumptions in \textit{JWST} Transmission
Spectra | 26 pages, 23 figures, 4 tables; Accepted for publication in ApJ | null | 10.3847/1538-4357/ab3e6d | null | astro-ph.EP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Clouds are ubiquitous in extrasolar planet atmospheres and are critical to
our understanding of planetary climate and chemistry. They also represent one
of the greater challenges to overcome when trying to interpret transit
transmission spectra of exoplanet atmospheres as their presence can inhibit
precise constraints on atmospheric composition and thermal properties. In this
work we take a phenomenological approach towards understanding 1) our ability
to constrain bulk cloud properties, and 2) the impact of clouds on constraining
various atmospheric properties as obtained through transmission spectroscopy
with the \textit{James Webb Space Telescope (JWST)}. We do this by exploring
retrievals of atmospheric and cloud properties for a generic "hot-Jupiter" as a
function of signal-to-noise ratio (SNR), \textit{JWST} observing modes and four
different cloud parameterizations. We find that most key atmospheric and cloud
inferences can be well constrained in the wavelength range ($\lambda = $ 0.6 -
11 $\mu$m), with NIRCam ($\lambda =$ 2.5 - 5 $\mu$m) being critical in
inferring atmospheric properties and NIRISS + MIRI ($\lambda =$ 0.6 - 2.5, 5 -
11 $\mu$m) being necessary for good constraints on cloud parameters. However,
constraining the cloud abundance and therefore the total cloud mass requires an
observable cloud base in the transit geometry. While higher SNR observations
can place tighter constraints on major parameters such as temperature,
metallicity and cloud sedimentation, they are unable to eliminate strong
degeneracies among cloud parameters. Our investigation of a generic
"warm-Neptune" with photochemical haze parameterization also shows promising
results in constraining atmospheric and haze properties in the cooler
temperature regime.
| [{'version': 'v1', 'created': 'Wed, 28 Aug 2019 18:52:34 GMT'}] | 2019-10-09 | [array(['Mai', 'Chuhong', ''], dtype=object)
array(['Line', 'Michael R.', ''], dtype=object)] |
419 | 1902.01133 | Daniel Sablowski | Daniel P. Sablowski, Silva J\"arvinen, Ilya Ilyin, Klaus G.
Strassmeier | Carbon 12C/13C isotope ratio of alpha Aurigae revised | accepted to A&A Letters to the Editor | A&A 622, L11 (2019) | 10.1051/0004-6361/201834663 | null | astro-ph.SR | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Context. Capella ({\alpha} Aur) is one of the few binaries in the sky with
two cool giant stars. With spectral types of G8III and G0III, the two
components appear at different but distinct stages in their evolution. The G0
secondary star is a Hertzsprung-gap giant, and the G8 primary star is thought
to be a clump giant. Aims. We present a new measure of the carbon 12 C/ 13 C
isotope ratio of the primary component of Capella using high-resolution R
$\approx$250 000 spectra obtained with the Potsdam Echelle Polarimetric and
Spectroscopic Instrument (PEPSI) with both the Vatican Advanced Technology
Telescope (VATT) and the Large Binocular Telescope (LBT). Methods.
Signal-to-noise ratios of up to 2 700 were obtained by averaging nightly
spectra. These average spectra were used to disentangle the two binary
components. The isotope ratio was derived with the use of spectrum synthesis
from the CN lines at 8004 {\AA}. Results. We found that the 12 C/ 13 C ratio of
the primary component of Capella is 17.8$\pm$1.9. Our measurement precision is
now primarily limited by the spectral-line data and by the grid-step size of
the model atmospheres rather than the data. The separated spectrum of the
secondary component does not show distinguishable 12 CN and 13 CN lines because
of its v sin i and higher temperature. Conclusions. Our new 12 C/ 13 C value is
significantly lower than the previous value of 27$\pm$4 but now agrees better
with the recent model prediction of 18.8 - 20.7.
| [{'version': 'v1', 'created': 'Mon, 4 Feb 2019 11:46:47 GMT'}] | 2019-02-13 | [array(['Sablowski', 'Daniel P.', ''], dtype=object)
array(['Järvinen', 'Silva', ''], dtype=object)
array(['Ilyin', 'Ilya', ''], dtype=object)
array(['Strassmeier', 'Klaus G.', ''], dtype=object)] |
420 | 2306.10245 | Chi Cheuk Tsang | Chi Cheuk Tsang | On the set of normalized dilatations of fully-punctured pseudo-Anosov
maps | 80 pages, 31 figures | null | null | null | math.GT math.DS | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We improve the bound on the number of tetrahedra in the veering triangulation
of a fully-punctured pseudo-Anosov mapping torus in terms of the normalized
dilatation. When the mapping torus has only one boundary component, we employ
various techniques to improve the bound further. Together with the author's
work with Hironaka in the case when the mapping torus has at least two boundary
components, this allows us to understand small elements of the set
$\mathcal{D}$ of normalized dilatations of fully-punctured pseudo-Anosov maps
using computational means. In particular, we certify that the minimum element
of $\mathcal{D}$ is $\mu^2$ and the minimum accumulation point of $\mathcal{D}$
is $\mu^4$, where $\mu = \frac{1 + \sqrt{5}}{2} \approx 1.618$ is the golden
ratio.
| [{'version': 'v1', 'created': 'Sat, 17 Jun 2023 03:11:51 GMT'}] | 2023-06-21 | [array(['Tsang', 'Chi Cheuk', ''], dtype=object)] |
421 | 1806.02709 | Reda Bellafqira | Reda Bellafqira, Gouenou Coatrieux, Emmanuelle Genin, Michel Cozic | Secure Multilayer Perceptron Based On Homomorphic Encryption | null | null | null | null | cs.CR | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work, we propose an outsourced Secure Multilayer Perceptron (SMLP)
scheme where privacy and confidentiality of both the data and the model are
ensured during the training and the classification phases. More clearly, this
SMLP : i) can be trained by a cloud server based on data previously outsourced
by a user in an homomorphically encrypted form; ii) its parameters are
homomorphically encrypted giving thus no clues to the cloud; and iii) it can
also be used for classifying new encrypted data sent by the user returning him
the encrypted classification result encrypted. The originality of this scheme
is threefold. To the best of our knowledge, it is the first multilayer
perceptron (MLP) secured in its training phase over homomorphically encrypted
data with no problem of convergence. And It does not require
extra-communications between the server and the user. It is based on the
Rectified Linear Unit (ReLU) activation function that we secure with no
approximation contrarily to actual SMLP solutions. To do so, we take advantage
of two semi-honest non-colluding servers. Experimental results carried out on a
binary database encrypted with the Paillier cryptosystem demonstrate the
overall performance of our scheme and its convergence.
| [{'version': 'v1', 'created': 'Thu, 7 Jun 2018 14:39:21 GMT'}] | 2018-06-08 | [array(['Bellafqira', 'Reda', ''], dtype=object)
array(['Coatrieux', 'Gouenou', ''], dtype=object)
array(['Genin', 'Emmanuelle', ''], dtype=object)
array(['Cozic', 'Michel', ''], dtype=object)] |
422 | 2005.12215 | Marco Chiani Dr. | Marco Chiani, Andrea Conti, Moe Z. Win | Piggybacking on Quantum Streams | null | Physical Review A (2020) | 10.1103/PhysRevA.102.012410 | null | quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This paper shows that it is possible to piggyback classical information on a
stream of qubits protected by quantum error correcting codes. The piggyback
channel can be created by introducing intentional errors corresponding to a
controlled sequence of syndromes. These syndromes are further protected, when
quantum noise is present, by classical error correcting codes according to a
performance-delay trade-off. Classical information can thus be added and
extracted at arbitrary epochs without consuming additional quantum resources
and without disturbing the quantum stream.
| [{'version': 'v1', 'created': 'Mon, 25 May 2020 16:33:01 GMT'}] | 2020-07-21 | [array(['Chiani', 'Marco', ''], dtype=object)
array(['Conti', 'Andrea', ''], dtype=object)
array(['Win', 'Moe Z.', ''], dtype=object)] |
423 | astro-ph/0412095 | Jamie Portsmouth | Jamie Portsmouth (Oxford), Edmund Bertschinger (MIT) | Kinetic theory of polarization in the Sunyaev-Zeldovich effect | 12 pages, 4 figures | null | null | null | astro-ph | null | We apply the coherency tensor formalism to the calculation of the spectral
distortions imprinted in the intensity and polarization of the cosmic microwave
background radiation due to the kinematic and thermal Sunyaev-Zeldovich effects
(SZE). We obtain the first relativistic corrections to the intensity produced
by the kinematic and thermal SZE, and the first correction to the polarization
magnitude due to electron thermal motion.
| [{'version': 'v1', 'created': 'Fri, 3 Dec 2004 21:21:31 GMT'}] | 2007-05-23 | [array(['Portsmouth', 'Jamie', '', 'Oxford'], dtype=object)
array(['Bertschinger', 'Edmund', '', 'MIT'], dtype=object)] |
424 | 2203.08918 | Valeriya Kotelnikova | Alexander Iksanov and Valeriya Kotelnikova | Small counts in nested Karlin's occupancy scheme generated by discrete
Weibull-like distributions | null | null | null | null | math.PR | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A nested Karlin's occupancy scheme is a symbiosis of classical Karlin's
balls-in-boxes scheme and a weighted branching process. To define it, imagine a
deterministic weighted branching process in which weights of the first
generation individuals are given by the elements of a discrete probability
distribution. For each positive integer $j$, identify the $j$th generation
individuals with the $j$th generation boxes. The collection of balls is one and
the same for all generations, and each ball starts at the root of the weighted
branching process tree and moves along the tree according to the following
rule: transition from a mother box to a daughter box occurs with probability
given by the ratio of the daughter and mother weights.
Assume that there are $n$ balls and that the discrete probability
distribution responsible for the first generation is Weibull-like. Denote by
$\mathcal{K}_n^{(j)}(l)$ and $\mathcal{K}_n^{*(j)}(l)$ the number of the $j$th
generation boxes which contain at least $l$ balls and exactly $l$ balls,
respectively. We prove functional limit theorems (FLTs) for the matrix-valued
processes $\big(\mathcal{K}_{[{\rm
e}^{T+\cdot}]}^{(j)}(l)\big)_{j,l\in\mathbb{N}}$ and $\big(\mathcal{ K}_{[{\rm
e}^{T+\cdot}]}^{*(j)}(l)\big)_{j,l\in\mathbb{N}}$, properly normalized and
centered, as $T\to \infty$. The present FLTs are an extension of a FLT proved
by Iksanov, Kabluchko and Kotelnikova (2022) for the vector-valued process
$\big(\mathcal{K}_{[{\rm e}^{T+\cdot}]}^{(j)}(1)\big)_{j\in\mathbb{N}}$. While
the rows of each of the limit matrix-valued processes are independent and
identically distributed, the entries within each row are stationary Gaussian
processes with explicitly given covariances and cross-covariances. We provide
an integral representation for each row. The results obtained are new even for
Karlin's occupancy scheme.
| [{'version': 'v1', 'created': 'Wed, 16 Mar 2022 20:04:38 GMT'}] | 2022-03-18 | [array(['Iksanov', 'Alexander', ''], dtype=object)
array(['Kotelnikova', 'Valeriya', ''], dtype=object)] |
425 | 2305.11112 | Yunpeng Wang | Yunpeng Wang, Zelong Yuan, Jianchun Wang | Ensemble data assimilation-based mixed subgrid-scale model for
large-eddy simulations | null | null | null | null | physics.flu-dyn | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | An ensemble Kalman filter (EnKF)-based mixed model (EnKF-MM) is proposed for
the subgrid-scale (SGS) closure in the large-eddy simulation (LES) of
turbulence. The model coefficients are determined through the EnKF-based data
assimilation technique. The direct numerical simulation (DNS) results are
filtered to obtain the benchmark data for LES. Reconstructing the correct
kinetic energy spectrum of the filtered DNS (fDNS) data has been adopted as the
target for the EnKF to optimize the coefficient of the functional part in the
mixed model. The proposed EnKF-MM framework is subsequently tested in the LES
of both the incompressible homogeneous isotropic turbulence (HIT) and turbulent
mixing layer (TML). The performance of LES is comprehensively examined through
the predictions of the flow statistics including the velocity spectrum, the
probability density functions (PDFs) of the SGS stress, the PDF of the strain
rate and the PDF of the SGS energy flux. The structure functions, the evolution
of turbulent kinetic energy, the mean flow and the Reynolds stress profile, and
the iso-surface of the Q-criterion are also examined to evaluate the
spatial-temporal predictions by different SGS models. The results of the
EnKF-MM framework are consistently more satisfying compared to the traditional
SGS models, including the dynamic Smagorinsky model (DSM), the dynamic mixed
model (DMM) and the velocity gradient model (VGM), demonstrating its great
potential in the optimization of SGS models for LES of turbulence.
| [{'version': 'v1', 'created': 'Thu, 18 May 2023 16:53:52 GMT'}
{'version': 'v2', 'created': 'Thu, 1 Jun 2023 12:25:09 GMT'}
{'version': 'v3', 'created': 'Thu, 6 Jul 2023 07:47:19 GMT'}] | 2023-07-07 | [array(['Wang', 'Yunpeng', ''], dtype=object)
array(['Yuan', 'Zelong', ''], dtype=object)
array(['Wang', 'Jianchun', ''], dtype=object)] |
426 | 0710.0271 | Christian Klingenberg F | Gui-Qiang Chen (1), Nadine Even (2), Christian Klingenberg (2) ((1)
Northwestern Univ., (2) W\"urzburg Univ.) | Hyperbolic Conservation Laws and Hydrodynamic Limit for Particle Systems | null | null | null | null | math.AP math-ph math.MP | null | We study the following class of scalar hyperbolic conservation laws with
discontinuous fluxes: \partial_t\rho+\partial_xF(x,\rho)=0. The main feature of
such a conservation law is the discontinuity of the flux function in the space
variable x. Kruzkov's approach for the L1-contraction does not apply since it
requires the Lipschitz continuity of the flux function; and entropy solutions
even for the Riemann problem are not unique under the classical entropy
conditions. On the other hand, it is known that, in statistical mechanics, some
microscopic interacting particle systems with discontinuous speed parameter
lambda(x), in the hydrodynamic limit, formally lead to scalar hyperbolic
conservation laws with discontinuous fluxes of the form:
\partial_t\rho+\partial_x(\lambda(x)h(\rho))=0. The natural question arises
which entropy solutions the hydrodynamic limit selects, thereby leading to a
suitable, physical relevant notion of entropy solutions of this class of
conservation laws. This paper is a first step and provides an answer to this
question for a family of discontinuous flux functions. In particular, we
identify the entropy condition for our PDE and proceed to show the
well-posedness by combining our existence result with a uniqueness result of
Audusse-Perthame (2005) for the family of flux functions; we establish a
compactness framework for the hydrodynamic limit of large particle systems and
the convergence of other approximate solutions to our PDE, which is based on
the notion and reduction of measure-valued entropy solutions; and we finally
establish the hydrodynamic limit for a ZRP with discontinuous speed-parameter
governed by an entropy solution to our PDE.
| [{'version': 'v1', 'created': 'Mon, 1 Oct 2007 11:54:25 GMT'}] | 2007-10-02 | [array(['Chen', 'Gui-Qiang', ''], dtype=object)
array(['Even', 'Nadine', ''], dtype=object)
array(['Klingenberg', 'Christian', ''], dtype=object)] |
427 | 1401.3567 | Youssef Khmou | Y.Khmou, S.Safi | 2D Direction Of Arrival Estimation with Modified Propagator | 4 pages, one latex file, 3 figures | null | null | null | cs.IT math.IT stat.AP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, a fast algorithm for the Direction Of Arrival (DOA) estimation
of radiating sources, based on partial covariance matrix and without eigende-
composition of incoming signals is extended to two dimensional problem of joint
azimuth and elevation estimation angles using Uniform Circular Array (UCA) in
case of non coherent narrowband signals. Simulation results are presented with
both Additive White Gaussian Noise (AWGN) and real symmetric Toeplitz noise.
| [{'version': 'v1', 'created': 'Wed, 15 Jan 2014 13:07:52 GMT'}] | 2015-03-18 | [array(['Khmou', 'Y.', ''], dtype=object)
array(['Safi', 'S.', ''], dtype=object)] |
428 | 2005.12566 | Xingchen Li | Xingchen Li, Xiang Wang, Xiangnan He, Long Chen, Jun Xiao, Tat-Seng
Chua | Hierarchical Fashion Graph Network for Personalized Outfit
Recommendation | null | null | null | null | cs.IR | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Fashion outfit recommendation has attracted increasing attentions from online
shopping services and fashion communities.Distinct from other scenarios (e.g.,
social networking or content sharing) which recommend a single item (e.g., a
friend or picture) to a user, outfit recommendation predicts user preference on
a set of well-matched fashion items.Hence, performing high-quality personalized
outfit recommendation should satisfy two requirements -- 1) the nice
compatibility of fashion items and 2) the consistence with user preference.
However, present works focus mainly on one of the requirements and only
consider either user-outfit or outfit-item relationships, thereby easily
leading to suboptimal representations and limiting the performance. In this
work, we unify two tasks, fashion compatibility modeling and personalized
outfit recommendation. Towards this end, we develop a new framework,
Hierarchical Fashion Graph Network(HFGN), to model relationships among users,
items, and outfits simultaneously. In particular, we construct a hierarchical
structure upon user-outfit interactions and outfit-item mappings. We then get
inspirations from recent graph neural networks, and employ the embedding
propagation on such hierarchical graph, so as to aggregate item information
into an outfit representation, and then refine a user's representation via
his/her historical outfits. Furthermore, we jointly train these two tasks to
optimize these representations. To demonstrate the effectiveness of HFGN, we
conduct extensive experiments on a benchmark dataset, and HFGN achieves
significant improvements over the state-of-the-art compatibility matching
models like NGNN and outfit recommenders like FHN.
| [{'version': 'v1', 'created': 'Tue, 26 May 2020 08:23:35 GMT'}] | 2020-05-27 | [array(['Li', 'Xingchen', ''], dtype=object)
array(['Wang', 'Xiang', ''], dtype=object)
array(['He', 'Xiangnan', ''], dtype=object)
array(['Chen', 'Long', ''], dtype=object)
array(['Xiao', 'Jun', ''], dtype=object)
array(['Chua', 'Tat-Seng', ''], dtype=object)] |
429 | 1609.09229 | Eskil Rydhe | Eskil Rydhe | On the characterization of Triebel--Lizorkin type spaces of analytic
functions | null | Journal of Fourier Analysis and Applications, 24(6) (2018),
1491-1517 | 10.1007/s00041-017-9584-0 | null | math.FA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider different characterizations of Triebel--Lizorkin type spaces of
analytic functions on the unit disc. Even though our results appear in the
folklore, detailed descriptions are hard to find, and in fact we are unable to
discuss the full range of parameters. Without additional effort we work with
vector-valued analytic functions, and also consider a generalized scale of
function spaces, including for example so-called $Q$-spaces. The primary aim of
this note is to generalize, and clarify, a remarkable result by Cohn and
Verbitsky, on factorization of Triebel--Lizorkin spaces. Their result remains
valid for functions taking values in an arbitrary Banach space, provided that
the vector-valuedness "sits in the right factor". On the other hand, if we
impose vector-valuedness on the "wrong" factor, then the factorization fails
even for separable Hilbert spaces.
| [{'version': 'v1', 'created': 'Thu, 29 Sep 2016 07:17:19 GMT'}] | 2018-12-03 | [array(['Rydhe', 'Eskil', ''], dtype=object)] |
430 | 1211.3934 | Mikko Alava | Shao-Meng Qin, Hannu Verkasalo, Mikael Mohtaschemi, Tuomo Hartonen,
Mikko Alava | Patterns, entropy, and predictability of human mobility and life | 5 figures, for data see smartphonedata.aalto.fi, accepted to PLoS One | null | 10.1371/journal.pone.0051353 | null | physics.soc-ph cs.SI | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Cellular phones are now offering an ubiquitous means for scientists to
observe life: how people act, move and respond to external influences. They can
be utilized as measurement devices of individual persons and for groups of
people of the social context and the related interactions. The picture of human
life that emerges shows complexity, which is manifested in such data in
properties of the spatiotemporal tracks of individuals. We extract from
smartphone-based data for a set of persons important locations such as "home",
"work" and so forth over fixed length time-slots covering the days in the
data-set. This set of typical places is heavy-tailed, a power-law distribution
with an exponent close to -1.7. To analyze the regularities and stochastic
features present, the days are classified for each person into regular,
personal patterns. To this are superimposed fluctuations for each day. This
randomness is measured by "life" entropy, computed both before and after
finding the clustering so as to subtract the contribution of a number of
patterns. The main issue, that we then address, is how predictable individuals
are in their mobility. The patterns and entropy are reflected in the
predictability of the mobility of the life both individually and on average. We
explore the simple approaches to guess the location from the typical behavior,
and of exploiting the transition probabilities with time from location or
activity A to B. The patterns allow an enhanced predictability, at least up to
a few hours into the future from the current location. Such fixed habits are
most clearly visible in the working-day length.
| [{'version': 'v1', 'created': 'Fri, 16 Nov 2012 16:02:36 GMT'}] | 2015-06-12 | [array(['Qin', 'Shao-Meng', ''], dtype=object)
array(['Verkasalo', 'Hannu', ''], dtype=object)
array(['Mohtaschemi', 'Mikael', ''], dtype=object)
array(['Hartonen', 'Tuomo', ''], dtype=object)
array(['Alava', 'Mikko', ''], dtype=object)] |
431 | 0805.1517 | Haim Suchowski | Haim Suchowski, Dan Oron, Ady Arie and Yaron Silberberg | Geometrical Representation of Sum Frequency Generation and Adiabatic
Frequency Conversion | 4 pages, 4 figures | null | 10.1103/PhysRevA.78.063821 | null | physics.optics | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a geometrical representation of sum frequency generation process
in the undepleted pump approximation. The analogy of such dynamics with the
known optical Bloch equations is discussed. We use this analogy to present a
novel technique for the achievement of both high efficiency and large bandwidth
in a sum frequency conversion processes using adiabatic inversion scheme,
adapted from NMR and light-matter interaction. The adiabatic constraints are
derived in this context. Last, this adiabatic frequency conversion scheme is
realized experimentally by a proper design of adiabatic aperiodically poled KTP
device, using quasi phased matched method. In the experiments we achieved high
efficiency signal to idler conversion over a bandwidth of 140nm.
| [{'version': 'v1', 'created': 'Sun, 11 May 2008 08:59:02 GMT'}] | 2009-11-13 | [array(['Suchowski', 'Haim', ''], dtype=object)
array(['Oron', 'Dan', ''], dtype=object)
array(['Arie', 'Ady', ''], dtype=object)
array(['Silberberg', 'Yaron', ''], dtype=object)] |
432 | 1912.03010 | Yu Wu | Chengyi Wang, Yu Wu, Yujiao Du, Jinyu Li, Shujie Liu, Liang Lu, Shuo
Ren, Guoli Ye, Sheng Zhao, Ming Zhou | Semantic Mask for Transformer based End-to-End Speech Recognition | null | null | null | null | cs.CL cs.SD eess.AS | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Attention-based encoder-decoder model has achieved impressive results for
both automatic speech recognition (ASR) and text-to-speech (TTS) tasks. This
approach takes advantage of the memorization capacity of neural networks to
learn the mapping from the input sequence to the output sequence from scratch,
without the assumption of prior knowledge such as the alignments. However, this
model is prone to overfitting, especially when the amount of training data is
limited. Inspired by SpecAugment and BERT, in this paper, we propose a semantic
mask based regularization for training such kind of end-to-end (E2E) model. The
idea is to mask the input features corresponding to a particular output token,
e.g., a word or a word-piece, in order to encourage the model to fill the token
based on the contextual information. While this approach is applicable to the
encoder-decoder framework with any type of neural network architecture, we
study the transformer-based model for ASR in this work. We perform experiments
on Librispeech 960h and TedLium2 data sets, and achieve the state-of-the-art
performance on the test set in the scope of E2E models.
| [{'version': 'v1', 'created': 'Fri, 6 Dec 2019 07:55:04 GMT'}
{'version': 'v2', 'created': 'Mon, 16 Mar 2020 02:41:44 GMT'}] | 2020-03-17 | [array(['Wang', 'Chengyi', ''], dtype=object)
array(['Wu', 'Yu', ''], dtype=object)
array(['Du', 'Yujiao', ''], dtype=object)
array(['Li', 'Jinyu', ''], dtype=object)
array(['Liu', 'Shujie', ''], dtype=object)
array(['Lu', 'Liang', ''], dtype=object)
array(['Ren', 'Shuo', ''], dtype=object)
array(['Ye', 'Guoli', ''], dtype=object)
array(['Zhao', 'Sheng', ''], dtype=object)
array(['Zhou', 'Ming', ''], dtype=object)] |
433 | 2011.06336 | Neha Singh | Neha Singh and Tomasz Bulik | Constraining parameters of coalescing stellar mass binary black hole
systems with the Einstein Telescope alone | 13 pages, 7 figures. Published in Physical Review D | Phys. Rev. D 104, 043014 (2021) | 10.1103/PhysRevD.104.043014 | Virgo document number VIR-0876B-20 | astro-ph.HE gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Einstein Telescope (ET) is the future third generation gravitational wave
detector consisting of three independent interferometers arranged in a
triangular configuration, with the sensitivity large enough to be able to
detect stellar mass black holes even beyond the redshift of 10. In this paper,
we analyze the capabilities of ET as a standalone instrument and not part of a
network. We show that the analysis of detection of binary coalescences in the
three individual interferometers of the ET allow us to weakly constrain the sky
location of the source. We present the analysis that leads to the constraints
on the redshift and source frame chirp mass of detected binaries. We show that
these values can be estimated with the accuracy comparable to the one expected
from networks of gravitational wave interferometers. Thus, we show that the ET
as a single instrument is able to break the redshift - chirp mass degeneracy
and is therefore a valuable tool to explore properties of populations of
merging compact object binaries.
| [{'version': 'v1', 'created': 'Thu, 12 Nov 2020 12:10:15 GMT'}
{'version': 'v2', 'created': 'Mon, 16 Aug 2021 17:55:12 GMT'}] | 2021-08-25 | [array(['Singh', 'Neha', ''], dtype=object)
array(['Bulik', 'Tomasz', ''], dtype=object)] |
434 | 1802.02625 | Lilia Anguelova | Lilia Anguelova, Peter Suranyi and L.C. Rohana Wijewardhana | On Non-slow Roll Inflationary Regimes | 10 pages, contribution to the proceedings of the 10th International
Symposium "Quantum Theory and Symmetries", 2017 | Springer Proc. Math. Stat. 255 (2018) 161-171 | null | null | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We summarize our work on constant roll inflationary models. It was understood
recently that constant roll inflation, in a regime beyond the slow roll
approximation, can give models that are in agreement with the observational
constraints. We describe a new class of constant roll inflationary models and
investigate the behavior of scalar perturbations in them. We also comment on
other non-slow roll regimes of inflation.
| [{'version': 'v1', 'created': 'Wed, 7 Feb 2018 20:43:41 GMT'}] | 2018-11-14 | [array(['Anguelova', 'Lilia', ''], dtype=object)
array(['Suranyi', 'Peter', ''], dtype=object)
array(['Wijewardhana', 'L. C. Rohana', ''], dtype=object)] |
435 | quant-ph/9504018 | Haret Rosu | H.C. Rosu, M. Reyes, K.B. Wolf, O. Obreg\'on | Supersymmetric features of the Maxwell fish-eye lens | 5 pages in Latex, one figure not included has been published as Fig.
2 in Phys. Lett. A 208 (1995) 33-39 | SPIE Vol. 2730 (1996) 436-439 | 10.1117/12.231113 | IFUG-95/05 r | quant-ph | null | We provide a supersymmetric analysis of the Maxwell fisheye (MF) wave problem
at zero energy. Working in the so-called $R_{0}=0$ sector, we obtain the
corresponding superpartner (fermionic) MF effective potential within Witten's
one-dimensional (radial) supersymmetric procedure.
| [{'version': 'v1', 'created': 'Wed, 26 Apr 1995 03:36:00 GMT'}
{'version': 'v2', 'created': 'Mon, 5 Jun 1995 03:30:00 GMT'}
{'version': 'v3', 'created': 'Wed, 24 Apr 1996 17:03:00 GMT'}] | 2015-06-26 | [array(['Rosu', 'H. C.', ''], dtype=object)
array(['Reyes', 'M.', ''], dtype=object)
array(['Wolf', 'K. B.', ''], dtype=object)
array(['Obregón', 'O.', ''], dtype=object)] |
436 | 1811.06723 | Sandra Carillo | Sandra Carillo, Michel Chipot, Vanda Valente and Giorgio Vergara
Caffarelli | On weak regularity requirements of the relaxation modulus in
viscoelasticity | null | Communications Applied Industrial Mathematics, Volume 10 Issue 1,
2019, 78-87 | 10.2478/caim-2019-0014 | null | math-ph math.AP math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The existence and uniqueness of solution to a one-dimensional hyperbolic
integro-differential problem arising in viscoelasticity is here considered. The
kernel, in the linear viscoelasticity equation, represents the relaxation
function which is characteristic of the considered material. Specifically, the
case of a kernel, which does not satisfy the classical regularity requirements
is analysed. This choice is suggested by applications according to the
literature to model a wider variety of materials. A notable example of kernel,
not satisfying the classical regularity requirements, is represented by a wedge
continuous function. Indeed, the linear integro-differential viscoelasticity
equation, characterised by a suitable wedge continuous relaxation function, is
shown to give the classical linear wave equation via a limit procedure.
| [{'version': 'v1', 'created': 'Fri, 16 Nov 2018 09:37:28 GMT'}] | 2019-06-03 | [array(['Carillo', 'Sandra', ''], dtype=object)
array(['Chipot', 'Michel', ''], dtype=object)
array(['Valente', 'Vanda', ''], dtype=object)
array(['Caffarelli', 'Giorgio Vergara', ''], dtype=object)] |
437 | 1710.08118 | Yunzhong Chen | Y. Z. Chen, M. D\"obeli, E. Pomjakushina, Y. L. Gan, N. Pryds, and T.
Lippert | Scavenging of oxygen vacancies at modulation-doped oxide interfaces:
Evidence from oxygen isotope tracing | to be apprear in PRMater, 2017 | null | null | null | cond-mat.mtrl-sci | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The introduction of manganite buffer layers, La7/8Sr1/8MnO3 (LSMO) in
particular, at the metallic interface between SrTiO3 (STO) and another band
insulator suppresses the carrier density of the interfacial two-dimensional
electron gas (2DEG) and improves significantly the electron mobility. However,
the mechanisms underlying the extreme mobility enhancement remain elusive.
Herein, we used 18O isotope exchanged SrTi18O3 as substrates to create 2DEG at
room temperature with and without the LSMO buffer layer. By mapping the oxygen
profile across the interface between STO18 and disordered LaAlO3 or
yttria-stabilized zirconia (YSZ), we provide unambiguous evidence that redox
reactions occur at oxide interfaces even grown at room temperature. Moreover,
the manganite buffer layer not only suppresses the carrier density but also
strongly suppresses the oxygen exchange dynamics of the STO substrate, which
likely prevents the reduction of STO during the formation of the 2DEG. The
underlying mechanism on the enhanced electron mobility at buffered oxide
interfaces is also discussed.
| [{'version': 'v1', 'created': 'Mon, 23 Oct 2017 07:26:37 GMT'}] | 2017-10-24 | [array(['Chen', 'Y. Z.', ''], dtype=object)
array(['Döbeli', 'M.', ''], dtype=object)
array(['Pomjakushina', 'E.', ''], dtype=object)
array(['Gan', 'Y. L.', ''], dtype=object)
array(['Pryds', 'N.', ''], dtype=object)
array(['Lippert', 'T.', ''], dtype=object)] |
438 | astro-ph/0406557 | Marijke Haverkorn | M. Haverkorn, P. Katgert, A. G. de Bruyn | Properties of the warm magnetized ISM, as inferred from WSRT
polarimetric imaging | 12 pages, 6 figures, accepted by A&A | Astron.Astrophys. 427 (2004) 169-177 | 10.1051/0004-6361:200400042 | null | astro-ph | null | We describe a first attempt to derive properties of the regular and turbulent
Galactic magnetic field from multi-frequency polarimetric observations of the
diffuse Galactic synchrotron background. A single-cell-size model of the thin
Galactic disk is constructed which includes random and regular magnetic fields
and thermal and relativistic electrons. The disk is irradiated from behind with
a uniform partially polarized background. Radiation from the background and
from the thin disk is Faraday rotated and depolarized while propagating through
the medium. The model parameters are estimated from a comparison with 350 MHz
observations in two regions at intermediate latitudes done with the Westerbork
Synthesis Radio Telescope. We obtain good consistency between the estimates for
the random and regular magnetic field strengths and typical scales of structure
in the two regions. The regular magnetic field strength found is a few
microGauss, and the ratio of random to regular magnetic field strength is 0.7
+/- 0.5, for a typical scale of the random component of 15 +/- 10 pc.
Furthermore, the regular magnetic field is directed almost perpendicular to the
line of sight. This modeling is a potentially powerful method to estimate the
structure of the Galactic magnetic field, especially when more polarimetric
observations of the diffuse synchrotron background at intermediate latitudes
become available.
| [{'version': 'v1', 'created': 'Thu, 24 Jun 2004 19:12:24 GMT'}] | 2009-11-10 | [array(['Haverkorn', 'M.', ''], dtype=object)
array(['Katgert', 'P.', ''], dtype=object)
array(['de Bruyn', 'A. G.', ''], dtype=object)] |
439 | 1310.6867 | Peter Vancso | P\'eter Vancs\'o, G\'eza I. M\'ark, Philippe Lambin, Alexandre Mayer,
Chanyong Hwang and L\'aszl\'o P. Bir\'o | Effect of the disorder in graphene grain boundaries: A wave packet
dynamics study | Applied Surface Science (2013) | null | 10.1016/j.apsusc.2013.09.127 | null | cond-mat.mes-hall | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Chemical vapor deposition (CVD) on Cu foil is one of the most promising
methods to produce graphene samples despite of introducing numerous grain
boundaries into the perfect graphene lattice. A rich variety of GB structures
can be realized experimentally by controlling the parameters in the CVD method.
Grain boundaries contain non-hexagonal carbon rings (4,5,7,8 membered rings)
and vacancies in various ratios and arrangements. Using wave packet dynamic
(WPD) simulations and tight-binding electronic structure calculations, we have
studied the effect of the structure of GBs on the transport properties. Three
model GBs with increasing disorder were created in the computer: a periodic 5-7
GB, a "serpentine" GB, and a disordered GB containing 4,8 membered rings and
vacancies. It was found that for small energies (E=EF+-1eV) the transmission
decreases with increasing disorder. Four membered rings and vacancies are
identified as the principal scattering centres. Revealing the connection
between the properties of GBs and the CVD growth method may open new
opportunities in the graphene based nanoelectronics.
| [{'version': 'v1', 'created': 'Fri, 25 Oct 2013 10:10:38 GMT'}] | 2013-10-28 | [array(['Vancsó', 'Péter', ''], dtype=object)
array(['Márk', 'Géza I.', ''], dtype=object)
array(['Lambin', 'Philippe', ''], dtype=object)
array(['Mayer', 'Alexandre', ''], dtype=object)
array(['Hwang', 'Chanyong', ''], dtype=object)
array(['Biró', 'László P.', ''], dtype=object)] |
440 | 1301.5938 | Chiara Orsini | Chiara Orsini, Enrico Gregori, Luciano Lenzini, Dmitri Krioukov | Evolution of the Internet k-dense structure | 13 pages | IEEE/ACM Transactions on Networking (TON), Volume 22 Issue 6,
December 2014, Pages 1769-1780 | 10.1109/TNET.2013.2282756 | null | cs.SI cs.NI physics.soc-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | As the Internet AS-level topology grows over time, some of its structural
properties remain unchanged. Such time- invariant properties are generally
interesting, because they tend to reflect some fundamental processes or
constraints behind Internet growth. As has been shown before, the
time-invariant structural properties of the Internet include some most basic
ones, such as the degree distribution or clustering. Here we add to this
time-invariant list a non-trivial property - k-dense decomposition. This
property is derived from a recursive form of edge multiplicity, defined as the
number of triangles that share a given edge. We show that after proper
normalization, the k- dense decomposition of the Internet has remained stable
over the last decade, even though the Internet size has approximately doubled,
and so has the k-density of its k-densest core. This core consists mostly of
content providers peering at Internet eXchange Points, and it only loosely
overlaps with the high-degree or high-rank AS core, consisting mostly of tier-1
transit providers. We thus show that high degrees and high k-densities reflect
two different Internet-specific properties of ASes (transit versus content
providers). As a consequence, even though degrees and k-densities of nodes are
correlated, the relative fluctuations are strong, and related to that, random
graphs with the same degree distribution or even degree correlations as in the
Internet, do not reproduce its k-dense decomposition. Therefore an interesting
open question is what Internet topology models or generators can fully explain
or at least reproduce the k-dense properties of the Internet.
| [{'version': 'v1', 'created': 'Fri, 25 Jan 2013 01:10:42 GMT'}
{'version': 'v2', 'created': 'Fri, 1 Feb 2013 01:16:01 GMT'}
{'version': 'v3', 'created': 'Wed, 7 Aug 2013 20:09:29 GMT'}
{'version': 'v4', 'created': 'Mon, 28 Oct 2013 16:48:47 GMT'}
{'version': 'v5', 'created': 'Thu, 13 Aug 2015 18:42:45 GMT'}] | 2015-08-14 | [array(['Orsini', 'Chiara', ''], dtype=object)
array(['Gregori', 'Enrico', ''], dtype=object)
array(['Lenzini', 'Luciano', ''], dtype=object)
array(['Krioukov', 'Dmitri', ''], dtype=object)] |
441 | 1709.08352 | Vincent Cros | J.-Y. Chauleau, W. Legrand, N. Reyren, D. Maccariello, S. Collin, H.
Popescu, K. Bouzehouane, V. Cros, N. Jaouen, and A. Fert | Chirality in magnetic multilayers probed by the symmetry and the
amplitude of dichroism in X-ray resonant magnetic scattering | 8 pages, 3 figures | Phys. Rev. Lett. 120, 037202 (2018) | 10.1103/PhysRevLett.120.037202 | null | cond-mat.mtrl-sci cond-mat.other | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Chirality in condensed matter is now a topic of the utmost importance because
of its significant role in the understanding and mastering of a large variety
of new fundamental physicals mechanisms. Versatile experimental approaches,
capable to reveal easily the exact winding of order parameters are therefore
essential. Here we report X-ray resonant magnetic scattering (XRMS) as a
straightforward tool to identify directly the properties of chiral magnetic
systems. We show that it can straight-forwardly and unambiguously determine the
main characteristics of chiral magnetic distributions: i.e. its chiral nature,
the quantitative winding sense (clockwise or counter-clockwise) and its type
(N\'eel/cycloidal or Bloch/helical). This method is model-independent, does not
require a-priori knowledge of magnetic parameters and can be applied to any
system with magnetic domains ranging from few nanometers (wavelength limited)
to several microns. By using prototypical multilayers with tailored magnetic
chiralities based on the Co|Pt interface we illustrate the strength of this
method.
| [{'version': 'v1', 'created': 'Mon, 25 Sep 2017 07:16:49 GMT'}] | 2018-01-24 | [array(['Chauleau', 'J. -Y.', ''], dtype=object)
array(['Legrand', 'W.', ''], dtype=object)
array(['Reyren', 'N.', ''], dtype=object)
array(['Maccariello', 'D.', ''], dtype=object)
array(['Collin', 'S.', ''], dtype=object)
array(['Popescu', 'H.', ''], dtype=object)
array(['Bouzehouane', 'K.', ''], dtype=object)
array(['Cros', 'V.', ''], dtype=object)
array(['Jaouen', 'N.', ''], dtype=object)
array(['Fert', 'A.', ''], dtype=object)] |
442 | math-ph/9904030 | Oswaldo Monteiro Del Cima | O.M. Del Cima, D.H.T. Franco, J.A. Helayel-Neto and O. Piguet | An algebraic proof on the finiteness of Yang-Mills-Chern-Simons theory
in D=3 | 5 pages, revtex | Lett.Math.Phys.47:265,1999 | 10.1023/A:1007595121742 | TUW-98-12 | math-ph math.MP | null | A rigorous algebraic proof of the full finiteness in all orders of
perturbation theory is given for the Yang-Mills-Chern-Simons theory in a
general three-dimensional Riemannian manifold. We show the validity of a trace
identity, playing the role of a local form of the Callan-Symanzik equation, in
all loop orders, which yields the vanishing of the beta-functions associated to
the topological mass and gauge coupling constant as well as the anomalous
dimensions of the fields.
| [{'version': 'v1', 'created': 'Tue, 27 Apr 1999 14:15:56 GMT'}] | 2010-02-05 | [array(['Del Cima', 'O. M.', ''], dtype=object)
array(['Franco', 'D. H. T.', ''], dtype=object)
array(['Helayel-Neto', 'J. A.', ''], dtype=object)
array(['Piguet', 'O.', ''], dtype=object)] |
443 | 1704.06690 | Hung-Hsi Lin Hung-Hsi Lin | Hung-Hsi Lin, Felipe Vallini, Mu-Han Yang, Rajat Sharma, Matthew W.
Puckett, Sergio Montoya, Christian D. Wurm, Eric E. Fullerton, and Yeshaiahu
Fainman | Electronic Metamaterials with Tunable Second-order Optical
Nonlinearities | 12 pages, 4 figures, 1 table | null | null | null | physics.optics | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The ability to engineer metamaterials with tunable nonlinear optical
properties is crucial for nonlinear optics. Traditionally, metals have been
employed to enhance nonlinear optical interactions through field localization.
Here, inspired by the electronic properties of materials, we introduce and
demonstrate experimentally an asymmetric metal-semiconductor-metal (MSM)
metamaterial that exhibits a large and electronically tunable effective
second-order optical susceptibility (\c{hi}(2)). The induced \c{hi}(2)
originates from the interaction between the third-order optical susceptibility
of the semiconductor (\c{hi}(3)) with the engineered internal electric field
resulting from the two metals with dissimilar work function at its interfaces.
We demonstrate a five times larger second-harmonic intensity from the MSM
metamaterial, compared to contributions from its constituents with electrically
tunable nonlinear coefficient ranging from 2.8 to 15.6 pm/V.
| [{'version': 'v1', 'created': 'Fri, 21 Apr 2017 19:45:52 GMT'}] | 2017-04-25 | [array(['Lin', 'Hung-Hsi', ''], dtype=object)
array(['Vallini', 'Felipe', ''], dtype=object)
array(['Yang', 'Mu-Han', ''], dtype=object)
array(['Sharma', 'Rajat', ''], dtype=object)
array(['Puckett', 'Matthew W.', ''], dtype=object)
array(['Montoya', 'Sergio', ''], dtype=object)
array(['Wurm', 'Christian D.', ''], dtype=object)
array(['Fullerton', 'Eric E.', ''], dtype=object)
array(['Fainman', 'Yeshaiahu', ''], dtype=object)] |
444 | 2109.10358 | Kevin Kelly | Andr\'e de Gouv\^ea, Patrick J. Fox, Boris J. Kayser, and Kevin J.
Kelly | Characterizing Heavy Neutral Fermions via their Decays | 28 pages plus references, 19 figures. Comments welcome | null | 10.1103/PhysRevD.105.015019 | FERMILAB-PUB-21-453-T, NUHEP-TH/21-11 | hep-ph hep-ex | http://creativecommons.org/licenses/by/4.0/ | Many extensions of the Standard Model of particle physics contain new
electrically-neutral fermions. Should one of these particles be discovered,
questions will naturally arise regarding its nature. For instance: is it a
self-conjugate particle (i.e., is it a Dirac or a Majorana fermion)?, does it
interact via the Standard Model force carriers or something else? One set of
well-motivated particles in this class are Heavy Neutral Leptons (HNLs),
Standard Model gauge-singlet fermions that mix with the neutrinos and may be
produced in meson decays. We demonstrate that measuring the three body decays
of the HNL (or phenomenologically similar heavy fermions) can help determine
whether they are Majorana or Dirac fermions. We also investigate the ability to
distinguish among different models for the physics responsible for the HNL
decay. We compare the reach assuming full and partial event reconstruction, and
propose experimental analyses. Should a new fermion be discovered, studying its
three body decays provides a powerful diagnostic tool of its nature.
| [{'version': 'v1', 'created': 'Tue, 21 Sep 2021 18:00:01 GMT'}] | 2022-02-02 | [array(['de Gouvêa', 'André', ''], dtype=object)
array(['Fox', 'Patrick J.', ''], dtype=object)
array(['Kayser', 'Boris J.', ''], dtype=object)
array(['Kelly', 'Kevin J.', ''], dtype=object)] |
445 | 1312.6387 | Graham Kells | G. Kells, D. Sen, J.K. Slingerland and S. Vishveshwara | Topological Blocking in Quantum Quench Dynamics | 18 pages, 11 figures | Phys. Rev. B 89, 235130 (2014) | 10.1103/PhysRevB.89.235130 | null | cond-mat.str-el cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the non-equilibrium dynamics of quenching through a quantum critical
point in topological systems, focusing on one of their defining features:
ground state degeneracies and associated topological sectors. We present the
notion of 'topological blocking', experienced by the dynamics due to a mismatch
in degeneracies between two phases and we argue that the dynamic evolution of
the quench depends strongly on the topological sector being probed. We
demonstrate this interplay between quench and topology in models stemming from
two extensively studied systems, the transverse Ising chain and the Kitaev
honeycomb model. Through non-local maps of each of these systems, we
effectively study spinless fermionic $p$-wave paired superconductors. Confining
the systems to ring and toroidal geometries, respectively, enables us to
cleanly address degeneracies, subtle issues of fermion occupation and parity,
and mismatches between topological sectors. We show that various features of
the quench, which are related to Kibble-Zurek physics, are sensitive to the
topological sector being probed, in particular, the overlap between the
time-evolved initial ground state and an appropriate low-energy state of the
final Hamiltonian. While most of our study is confined to translationally
invariant systems, where momentum is a convenient quantum number, we briefly
consider the effect of disorder and illustrate how this can influence the
quench in a qualitatively different way depending on the topological sector
considered.
| [{'version': 'v1', 'created': 'Sun, 22 Dec 2013 14:34:31 GMT'}
{'version': 'v2', 'created': 'Fri, 17 Jan 2014 10:08:27 GMT'}] | 2014-07-02 | [array(['Kells', 'G.', ''], dtype=object)
array(['Sen', 'D.', ''], dtype=object)
array(['Slingerland', 'J. K.', ''], dtype=object)
array(['Vishveshwara', 'S.', ''], dtype=object)] |
446 | hep-ph/9704298 | Bryan Webber | Yu.L. Dokshitzer and B.R. Webber | Power Corrections to Event Shape Distributions | 11 pages, LaTeX, 2 figures; further reference to related work by
Korchemsky and Sterman added 30/4/97 | Phys.Lett. B404 (1997) 321-327 | 10.1016/S0370-2693(97)00573-X | Cavendish-HEP-97/2 | hep-ph | null | We estimate the effects of non-perturbative physics on the differential
distributions of infrared- and collinear-safe $e^+e^-$ event shape variables,
by extending the notion of an infrared-regular effective strong coupling, which
accounts for the non-perturbative corrections to the mean values of several
shape variables, to their distributions. This leads to $1/Q$ power corrections
over a range of values of the shape variables considered, where $Q$ is the
centre-of-mass energy. In the case of the thrust variable, the leading
correction is simply a shift of the distribution, by an amount proportional to
$1/Q$. We show that this gives an excellent description of the data throughout
a wide range of $T$ and $Q$.
| [{'version': 'v1', 'created': 'Fri, 11 Apr 1997 17:34:27 GMT'}
{'version': 'v2', 'created': 'Wed, 30 Apr 1997 09:45:28 GMT'}] | 2009-10-30 | [array(['Dokshitzer', 'Yu. L.', ''], dtype=object)
array(['Webber', 'B. R.', ''], dtype=object)] |
447 | quant-ph/9511034 | Andrei Kirilyuk | Andrei P. Kirilyuk | Causal Wave Mechanics and the Advent of Complexity. I. Dynamic
multivaluedness | 21 pages, PostScript 3.0 from an MS Word file; material is included
into the author's book "Universal Concept of Complexity by the Dynamic
Redundance Paradigm: Causal Randomness, Complete Wave Mechanics, and the
Ultimate Unification of Knowledge" (Naukova Dumka, Kiev, 1997), 550 p., in
English, see also physics/9806002; new format of presentation and linguistic
changes in the revised version, no changes in the essential contents | Ann. Fond. Louis de Broglie 21 (1996) 455-480 | null | Preprint IMP-95-1 | quant-ph chao-dyn nlin.CD | null | Two major deviations from causality in the existing formulations of quantum
mechanics, related respectively to quantum chaos and indeterminate wave
reduction, are eliminated within the new, universal concept of dynamic
complexity. The analysis involves a new paradigm for description of a system
with interaction, the principle of dynamic multivaluedness (redundance), and
the ensuing concept of the fundamental dynamic uncertainty. It is shown that
both the wave reduction and truly unpredictable (chaotic) behaviour in quantum
systems can be completely and causally understood as a higher sublevel of the
same dynamic complexity that provides the causally complete picture of the
unified wave-particle duality and relativity at its lowest level
(quant-ph/9902015,16). The presentation is divided into five parts. The first
three parts deal with intrinsic randomness in Hamiltonian (isolated) quantum
systems as the basic case of dynamical chaos. In the last two parts a causal
solution to the problem of quantum indeterminacy and wave reduction is
proposed. Part I introduces the method of effective dynamical functions as a
generalisation of the optical potential formalism. The method provides a legal
transformation of the Schroedinger equation revealing the hidden
multivaluedness of interaction process, i. e. its self-consistent, dynamical
splitting into many equally real, but mutually incompatible branches, called
'realisations'. Each realisation incorporates the usual "complete" set of
eigenfunctions and eigenvalues for the entire problem. The method is presented
in detail for the Hamiltonian system with periodic (not small) perturbation,
both in its time-independent and time-dependent versions.
| [{'version': 'v1', 'created': 'Thu, 23 Nov 1995 21:05:35 GMT'}
{'version': 'v2', 'created': 'Thu, 25 Mar 1999 08:50:12 GMT'}] | 2008-02-03 | [array(['Kirilyuk', 'Andrei P.', ''], dtype=object)] |
448 | 2010.07653 | Kristina Kvashnina | Firoz Alam, K. David Wegner, Stephanie Pouget, Lucia Amidani, Kristina
Kvashnina, Dmitry Aldakov, Peter Reiss | Eu$^{2+}$: a suitable substituent for Pb$^{2+}$ in CsPbX$_3$ perovskite
nanocrystals? | The Journal of Chemical Physics (2019) | null | 10.1063/1.5126473 | null | physics.chem-ph | http://creativecommons.org/licenses/by/4.0/ | Eu$^{2+}$ is used to replace toxic Pb$^{2+}$ in metal halide perovskite
nanocrystals (NCs). The synthesis implies injection of cesium oleate into a
solution of europium (II) bromide at an experimentally determined optimum
temperature of 130C and a reaction time of 60s. Structural analysis indicates
the formation of spherical CsEuBr$_3$ nanoparticles with a mean size of 43nm.
Using EuI$_2$ instead of EuBr$_2$ leads to the formation of 18nm CsI
nanoparticles, while EuCl$_2$ does not show any reaction with cesium oleate
forming 80nm EuCl2 nanoparticles. The obtained CsEuBr3 NCs exhibit bright blue
emission at 413nm (FWHM 30 nm) with a room temperature photoluminescence
quantum yield of 39%. The emission originates from the Laporte-allowed
4f7-4f65d1 transition of Eu$^{2+}$ and shows a PL decay time of 263ns. The
long-term stability of the optical properties is observed, making inorganic
lead-free CsEuBr$_3$ NCs promising deep blue emitters for optoelectronics.
| [{'version': 'v1', 'created': 'Thu, 15 Oct 2020 10:39:25 GMT'}] | 2020-10-16 | [array(['Alam', 'Firoz', ''], dtype=object)
array(['Wegner', 'K. David', ''], dtype=object)
array(['Pouget', 'Stephanie', ''], dtype=object)
array(['Amidani', 'Lucia', ''], dtype=object)
array(['Kvashnina', 'Kristina', ''], dtype=object)
array(['Aldakov', 'Dmitry', ''], dtype=object)
array(['Reiss', 'Peter', ''], dtype=object)] |
449 | 1507.07623 | Hyeong-Kwan Ju | Daeseok Lee and Hyeong-Kwan Ju | Different Volume Computation Methods of Graph Polytopes | 14 pages, no figure | null | null | null | math.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The aim of this work is to introduce several different volume computation
methods of the graph polytope associated with various type of finite simple
graphs. Among them, we obtained the recursive volume formula (RVF) that is
fundamental and most useful to compute the volume of the graph polytope for an
arbitrary finite simple graph.
| [{'version': 'v1', 'created': 'Tue, 28 Jul 2015 02:23:55 GMT'}] | 2015-07-29 | [array(['Lee', 'Daeseok', ''], dtype=object)
array(['Ju', 'Hyeong-Kwan', ''], dtype=object)] |
450 | 1605.06217 | Xiao Liu | Xiao Liu, Jiang Wang, Shilei Wen, Errui Ding, Yuanqing Lin | Localizing by Describing: Attribute-Guided Attention Localization for
Fine-Grained Recognition | null | null | null | null | cs.CV | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A key challenge in fine-grained recognition is how to find and represent
discriminative local regions. Recent attention models are capable of learning
discriminative region localizers only from category labels with reinforcement
learning. However, not utilizing any explicit part information, they are not
able to accurately find multiple distinctive regions. In this work, we
introduce an attribute-guided attention localization scheme where the local
region localizers are learned under the guidance of part attribute
descriptions. By designing a novel reward strategy, we are able to learn to
locate regions that are spatially and semantically distinctive with
reinforcement learning algorithm. The attribute labeling requirement of the
scheme is more amenable than the accurate part location annotation required by
traditional part-based fine-grained recognition methods. Experimental results
on the CUB-200-2011 dataset demonstrate the superiority of the proposed scheme
on both fine-grained recognition and attribute recognition.
| [{'version': 'v1', 'created': 'Fri, 20 May 2016 05:54:54 GMT'}
{'version': 'v2', 'created': 'Mon, 23 May 2016 03:37:54 GMT'}] | 2016-05-24 | [array(['Liu', 'Xiao', ''], dtype=object)
array(['Wang', 'Jiang', ''], dtype=object)
array(['Wen', 'Shilei', ''], dtype=object)
array(['Ding', 'Errui', ''], dtype=object)
array(['Lin', 'Yuanqing', ''], dtype=object)] |
451 | 2011.09666 | Wenhua Wang | Wenhua Wang, Xiong Liu, Aiting Wang and Baode Li | Molecular Decomposition of Anisotropic Hardy Spaces with Variable
Exponents | 23 Pages. arXiv admin note: text overlap with arXiv:1705.05188 by
other authors | null | null | null | math.CA | http://creativecommons.org/licenses/by-sa/4.0/ | Let $A$ be an expansive dilation on $\mathbb{R}^n$, and
$p(\cdot):\mathbb{R}^n\rightarrow(0,\,\infty)$ be a variable exponent function
satisfying the globally log-H\"{o}lder continuous condition. Let
$H^{p(\cdot)}_A({\mathbb {R}}^n)$ be the variable anisotropic Hardy space
defined via the non-tangential grand maximal function. In this paper, the
authors establish its molecular decomposition, which is still new even in the
classical isotropic setting (in the case $A:=2\mathrm I_{n\times n}$). As
applications, the authors obtain the boundedness of anisotropic
Calder\'on-Zygmund operators from $H^{p(\cdot)}_{A}(\mathbb{R}^n)$ to
$L^{p(\cdot)}(\mathbb{R}^n)$ or from $H^{p(\cdot)}_{A}(\mathbb{R}^n)$ to
itself.
| [{'version': 'v1', 'created': 'Wed, 18 Nov 2020 08:39:12 GMT'}] | 2020-11-20 | [array(['Wang', 'Wenhua', ''], dtype=object)
array(['Liu', 'Xiong', ''], dtype=object)
array(['Wang', 'Aiting', ''], dtype=object)
array(['Li', 'Baode', ''], dtype=object)] |
452 | 2106.11257 | Alexander Borzunov | Eduard Gorbunov, Alexander Borzunov, Michael Diskin, Max Ryabinin | Secure Distributed Training at Scale | Accepted to International Conference on Machine Learning (ICML 2022).
61 pages, 10 figures. The version 4 fixes inaccuracies in the proofs of
Lemmas E.2 and E.4. Code: https://github.com/yandex-research/btard | null | null | null | cs.LG cs.DC math.OC | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Many areas of deep learning benefit from using increasingly larger neural
networks trained on public data, as is the case for pre-trained models for NLP
and computer vision. Training such models requires a lot of computational
resources (e.g., HPC clusters) that are not available to small research groups
and independent researchers. One way to address it is for several smaller
groups to pool their computational resources together and train a model that
benefits all participants. Unfortunately, in this case, any participant can
jeopardize the entire training run by sending incorrect updates, deliberately
or by mistake. Training in presence of such peers requires specialized
distributed training algorithms with Byzantine tolerance. These algorithms
often sacrifice efficiency by introducing redundant communication or passing
all updates through a trusted server, making it infeasible to apply them to
large-scale deep learning, where models can have billions of parameters. In
this work, we propose a novel protocol for secure (Byzantine-tolerant)
decentralized training that emphasizes communication efficiency.
| [{'version': 'v1', 'created': 'Mon, 21 Jun 2021 17:00:42 GMT'}
{'version': 'v2', 'created': 'Thu, 7 Oct 2021 15:31:02 GMT'}
{'version': 'v3', 'created': 'Tue, 28 Jun 2022 15:58:24 GMT'}
{'version': 'v4', 'created': 'Mon, 2 Jan 2023 03:24:04 GMT'}] | 2023-01-03 | [array(['Gorbunov', 'Eduard', ''], dtype=object)
array(['Borzunov', 'Alexander', ''], dtype=object)
array(['Diskin', 'Michael', ''], dtype=object)
array(['Ryabinin', 'Max', ''], dtype=object)] |
453 | 1210.7639 | Benjamin Jourdain | Benjamin Jourdain, Tony Leli\`evre, B{\l}a\.zej Miasojedow | Optimal scaling for the transient phase of the random walk Metropolis
algorithm: The mean-field limit | Published at http://dx.doi.org/10.1214/14-AAP1048 in the Annals of
Applied Probability (http://www.imstat.org/aap/) by the Institute of
Mathematical Statistics (http://www.imstat.org) | Annals of Applied Probability 2015, Vol. 25, No. 4, 2263-2300 | 10.1214/14-AAP1048 | IMS-AAP-AAP1048 | math.PR | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the random walk Metropolis algorithm on $\mathbb{R}^n$ with
Gaussian proposals, and when the target probability measure is the $n$-fold
product of a one-dimensional law. In the limit $n\to\infty$, it is well known
(see [Ann. Appl. Probab. 7 (1997) 110-120]) that, when the variance of the
proposal scales inversely proportional to the dimension $n$ whereas time is
accelerated by the factor $n$, a diffusive limit is obtained for each component
of the Markov chain if this chain starts at equilibrium. This paper extends
this result when the initial distribution is not the target probability
measure. Remarking that the interaction between the components of the chain due
to the common acceptance/rejection of the proposed moves is of mean-field type,
we obtain a propagation of chaos result under the same scaling as in the
stationary case. This proves that, in terms of the dimension $n$, the same
scaling holds for the transient phase of the Metropolis-Hastings algorithm as
near stationarity. The diffusive and mean-field limit of each component is a
diffusion process nonlinear in the sense of McKean. This opens the route to new
investigations of the optimal choice for the variance of the proposal
distribution in order to accelerate convergence to equilibrium (see [Optimal
scaling for the transient phase of Metropolis-Hastings algorithms: The longtime
behavior Bernoulli (2014) To appear]).
| [{'version': 'v1', 'created': 'Mon, 29 Oct 2012 12:30:46 GMT'}
{'version': 'v2', 'created': 'Wed, 18 Dec 2013 08:51:15 GMT'}
{'version': 'v3', 'created': 'Fri, 19 Jun 2015 07:49:36 GMT'}] | 2016-08-14 | [array(['Jourdain', 'Benjamin', ''], dtype=object)
array(['Lelièvre', 'Tony', ''], dtype=object)
array(['Miasojedow', 'Błażej', ''], dtype=object)] |
454 | 1609.03109 | Amr Abdelaziz | Amr Abdelaziz, Ron Burton and C. Emre Koksal | Message Authentication and Secret Key Agreement in VANETs via Angle of
Arrival | null | null | null | null | cs.CR | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the scope of VANETs, nature of exchanged safety/warning messages renders
itself highly location dependent as it is usually for incident reporting. Thus,
vehicles are required to periodically exchange beacon messages that include
speed, time and GPS location information. In this paper paper, we present a
physical layer assisted message authentication scheme that uses Angle of
Arrival (AoA) estimation to verify the message originator location based on the
claimed location information. Within the considered vehicular communication
settings, fundamental limits of AoA estimation are developed in terms of its
Cramer Rao Bound (CRB) and existence of efficient estimator. The problem of
deciding whether the received signal is originated from the claimed GPS
location is formulated as a two sided hypotheses testing problem whose solution
is given by Wald test statics. Moreover, we use correct decision, $P_D$, and
false alarm, $P_F$, probabilities as a quantitative performance measure. The
observation posterior likelihood function is shown to satisfy regularity
conditions necessary for asymptotic normality of the ML-AoA estimator. Thus, we
give $P_D$ and $P_F$ in a closed form.
We extend the potential of physical layer contribution in security to provide
physical layer assisted secret key agreement (SKA) protocol. A public key (PK)
based SKA in which communicating vehicles are required to validate their
respective physical location. We show that the risk of the Man in the Middle
attack, which is common in PK-SKA protocols without a trusted third party, is
waived up to the literal meaning of the word "middle".
| [{'version': 'v1', 'created': 'Sun, 11 Sep 2016 02:23:47 GMT'}] | 2016-09-13 | [array(['Abdelaziz', 'Amr', ''], dtype=object)
array(['Burton', 'Ron', ''], dtype=object)
array(['Koksal', 'C. Emre', ''], dtype=object)] |
455 | 2009.00302 | Nikolay Gulitskiy Dr. | N. V. Antonov, N. M. Gulitskiy, P. I. Kakin, G. E. Kochnev | Effects of turbulent environment on self-organized critical behavior:
Isotropy vs Anisotropy | null | Universe 6, 145 (2020) | 10.3390/universe6090145 | null | cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study a self-organized critical system under influence of turbulent motion
of the environment. The system is described by the anisotropic continuous
stochastic equation proposed by Hwa and Kardar [{\it Phys. Rev. Lett.} {\bf
62}: 1813 (1989)]. The motion of the environment is modelled by the isotropic
Kazantsev--Kraichnan "rapid-change" ensemble for an incompressible fluid: it is
Gaussian with vanishing correlation time and the pair correlation function of
the form $\propto\delta(t-t') / k^{d+\xi}$, where $k$ is the wave number and
$\xi$ is an arbitrary exponent with the most realistic values $\xi = 4/3$
(Kolmogorov turbulence) and $\xi \to 2$ (Batchelor's limit). Using the
field-theoretic renormalization group, we find infrared attractive fixed points
of the renormalization group equation associated with universality classes,
i.e., with regimes of critical behavior. The most realistic values of the
spatial dimension $d=2$ and the exponent $\xi=4/3$ correspond to the
universality class of pure turbulent advection where the nonlinearity of the
Hwa--Kardar (HK) equation is irrelevant. Nevertheless, the universality class
where both the (anisotropic) nonlinearity of the HK equation and the
(isotropic) advecting velocity field are relevant also exists for some values
of the parameters $\varepsilon=4-d$ and $\xi$. Depending on what terms
(anisotropic, isotropic, or both) are relevant in specific universality class,
different types of scaling behavior (ordinary one or generalized) are
established.
| [{'version': 'v1', 'created': 'Tue, 1 Sep 2020 09:12:22 GMT'}] | 2020-09-22 | [array(['Antonov', 'N. V.', ''], dtype=object)
array(['Gulitskiy', 'N. M.', ''], dtype=object)
array(['Kakin', 'P. I.', ''], dtype=object)
array(['Kochnev', 'G. E.', ''], dtype=object)] |
456 | 1710.04106 | Jorge Vel\'azquez-Castro PhD | Jorge Vel\'azquez-Castro, Andr\'es Anzo-Hern\'andez, Beatriz
Bonilla-Capilla, Mois\'es Soto-Bajo, Andr\'es Fraguela-Collar | Vector-borne disease risk indexes in spatially structured populations | 16 pages, 5 figures | null | null | null | q-bio.PE math.DS | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | There are economic and physical limitations when applying prevention and
control strategies for urban vector borne diseases. Consequently, there are
increasing concerns and interest in designing efficient strategies and
regulations that health agencies can follow in order to reduce the imminent
impact of viruses like Dengue, Zika and Chikungunya. That includes fumigation,
abatization, reducing the hatcheries, picking up trash, information campaigns.
A basic question that arise when designing control strategies is about which
and where these ones should focus. In other words, one would like to know
whether preventing the contagion or decrease vector population, and in which
area of the city, is more efficient. In this work, we propose risk indexes
based on the idea of secondary cases from patch to patch. Thus, they take into
account human mobility and indicate which patch has more chance to be a
corridor for the spread of the disease and which is more vulnerable. They can
also indicate the neighborhood where hatchery control will reduce more the
number of potential cases. In order to illustrate the usefulness of these
indexes, we run a set of numerical simulations in a mathematical model that
takes into account the urban mobility and the differences in population density
among the areas of a city. If i is a particular neighborhood, the transmission
risk index TR_i measures the potential secondary cases caused by a host in that
neighborhood. The vector transmission risk index VTR_i measures the potential
secondary cases caused by a vector. Finally, the vulnerability risk index VR_i
measures the potential secondary cases in the neighborhood. Transmission
indexes can be used to give geographical priority to some neighborhoods when
applying prevention and control measures. On the other hand, the vulnerability
index can be useful to implement monitoring campaigns or public health
investment.
| [{'version': 'v1', 'created': 'Wed, 11 Oct 2017 15:16:47 GMT'}] | 2017-10-12 | [array(['Velázquez-Castro', 'Jorge', ''], dtype=object)
array(['Anzo-Hernández', 'Andrés', ''], dtype=object)
array(['Bonilla-Capilla', 'Beatriz', ''], dtype=object)
array(['Soto-Bajo', 'Moisés', ''], dtype=object)
array(['Fraguela-Collar', 'Andrés', ''], dtype=object)] |
457 | 2111.04488 | Luca Giorgetti | Luca Giorgetti | A planar algebraic description of conditional expectations | 20 pages | Internat. J. Math. 33 (2022) 2250037 | 10.1142/S0129167X22500379 | null | math.OA math.CT math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Let $\mathcal{N}\subset\mathcal{M}$ be a unital inclusion of arbitrary von
Neumann algebras. We give a 2-{$C^*$}-categorical/planar algebraic description
of normal faithful conditional expectations
$E:\mathcal{M}\to\mathcal{N}\subset\mathcal{M}$ with finite index and their
duals $E':\mathcal{N}'\to\mathcal{M}'\subset\mathcal{N}'$ by means of the
solutions of the conjugate equations for the inclusion morphism
$\iota:\mathcal{N}\to\mathcal{M}$ and its conjugate morphism
$\overline{\iota}:\mathcal{M}\to\mathcal{N}$. In particular, the theory of
index for conditional expectations admits a 2-{$C^*$}-categorical formulation
in full generality. Moreover, we show that a pair
$(\mathcal{N}\subset\mathcal{M}, E)$ as above can be described by a Q-system,
and vice versa. These results are due to Longo in the subfactor/simple tensor
unit case [Lon90, Thm.\ 5.2], [Lon94, Thm.\ 5.1].
| [{'version': 'v1', 'created': 'Mon, 8 Nov 2021 13:24:48 GMT'}
{'version': 'v2', 'created': 'Mon, 31 Oct 2022 16:53:00 GMT'}] | 2022-11-01 | [array(['Giorgetti', 'Luca', ''], dtype=object)] |
458 | 0709.3371 | Zhiyong Wang | M. Ablikim, J. Z. Bai, et al | Search for the C-parity violating process J/psi->gamma gamma via
psi(2S)->pi+pi- J/psi | 4 pages 2 figures | Phys.Rev.D76:117101,2007 | 10.1103/PhysRevD.76.117101 | null | hep-ex | null | Using 14.0\times 10^6 \psi(2S) events collected with the BES-II detector, the
C-parity violating process J/psi->gamma gamma via psi(2S)->pi+pi- J/psi is
studied. We determine a new upper limit for the J/psi->gamma gamma branching
ratio of B(J/psi->gamma gamma)<2.2\times 10^{-5} at the 90% C.L., which is
about 20 times lower than the previous measurement.
| [{'version': 'v1', 'created': 'Fri, 21 Sep 2007 08:52:36 GMT'}] | 2008-11-26 | [array(['Ablikim', 'M.', ''], dtype=object)
array(['Bai', 'J. Z.', ''], dtype=object)] |
459 | 1910.13669 | Forrest Francis | Forrest J. Francis | An Investigation Into Several Explicit Versions of Burgess' Bound | 14 pages, version 2 | null | null | null | math.NT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Let $\chi$ be a Dirichlet character modulo $p$, a prime. In applications, one
often needs estimates for short sums involving $\chi$. One such estimate is the
family of bounds known as \emph{Burgess' bound}. In this paper, we explore
several minor adjustments one can make to the work of Enrique Trevi\~no on
explicit versions of Burgess' bound. For an application, we investigate the
problem of the existence of a $k$th power non-residue modulo $p$ which is less
than $p^\alpha$ for several fixed $\alpha$. We also provide a quick improvement
to the conductor bounds for norm-Euclidean cyclic fields.
| [{'version': 'v1', 'created': 'Wed, 30 Oct 2019 04:54:05 GMT'}
{'version': 'v2', 'created': 'Sun, 1 Dec 2019 23:00:15 GMT'}] | 2019-12-03 | [array(['Francis', 'Forrest J.', ''], dtype=object)] |
460 | math-ph/0211042 | Eric M. Rains | Peter J. Forrester, Eric M. Rains | Interpretations of some parameter dependent generalizations of classical
matrix ensembles | 49 pages, 3 figures, LaTeX | null | null | null | math-ph math.MP | null | Two types of parameter dependent generalizations of classical matrix
ensembles are defined by their probability density functions (PDFs). As the
parameter is varied, one interpolates between the eigenvalue PDF for the
superposition of two classical ensembles with orthogonal symmetry and the
eigenvalue PDF for a single classical ensemble with unitary symmetry, while the
other interpolates between a classical ensemble with orthogonal symmetry and a
classical ensemble with symplectic symmetry. We give interpretations of these
PDFs in terms of probabilities associated to the continuous
Robinson-Schensted-Knuth correspondence between matrices, with entries chosen
from certain exponential distributions, and non-intersecting lattice paths, and
in the course of this probability measures on partitions and pairs of
partitions are identified. The latter are generalized by using Macdonald
polynomial theory, and a particular continuum limit -- the Jacobi limit -- of
the resulting measures is shown to give PDFs related to those appearing in the
work of Anderson on the Selberg integral. By interpreting Anderson's work as
giving the PDF for the zeros of a certain rational function, it is then
possible to identify random matrices whose eigenvalue PDFs realize the original
parameter dependent PDFs. This line of theory allows sampling of the original
parameter dependent PDFs, their Anderson-type generalizations and associated
marginal distributions, from the zeros of certain polynomials defined in terms
of random three term recurrences.
| [{'version': 'v1', 'created': 'Tue, 19 Nov 2002 00:26:46 GMT'}] | 2007-05-23 | [array(['Forrester', 'Peter J.', ''], dtype=object)
array(['Rains', 'Eric M.', ''], dtype=object)] |
461 | 0904.0661 | Jungyeon Cho | Jungyeon Cho, A. Lazarian | Simulations of Electron Magnetohydrodynamic Turbulence | ApJ, accepted; 19 pages, 14 figures (corrections + new calculations
added) | Astrophys.J.701:236-252,2009 | 10.1088/0004-637X/701/1/236 | null | astro-ph.EP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present numerical simulations of electron magnetohydrodynamic (EMHD) and
electron reduced MHD (ERMHD) turbulence. Comparing scaling relations, we find
that both EMHD and ERMHD turbulence show similar spectra and anisotropy. We
develop new techniques to study anisotropy of EMHD turbulence. Our detailed
study of anisotropy of EMHD turbulence supports our earlier result of k_par ~
k_perp^(1/3) scaling. We find that the high-order statistics show a scaling
that is similar to the She-Leveque scaling. We observe that the bispectra,
which characterize the interaction of different scales within the turbulence
cascade, are very different for EMHD and MHD turbulence. We show that both
decaying and driven EMHD turbulence have the same statistical properties. We
calculate the probability distribution functions (PDFs) of MHD and EMHD
turbulence and compare them with those of interplanetary turbulence. We find
that, as in the case of the solar wind, the PDFs of the increments of magnetic
field strength in MHD and EMHD turbulence are well described by the Tsallis
distribution. We discuss implications of our results for astrophysical
situations, including the ADAFs and magnetic reconnection.
| [{'version': 'v1', 'created': 'Fri, 3 Apr 2009 22:16:00 GMT'}
{'version': 'v2', 'created': 'Tue, 16 Jun 2009 18:09:25 GMT'}] | 2009-07-24 | [array(['Cho', 'Jungyeon', ''], dtype=object)
array(['Lazarian', 'A.', ''], dtype=object)] |
462 | 0705.1905 | Koji Nagata | Koji Nagata | Multipartite omnidirectional generalized Bell inequality | 4 pages | J. Phys. A: Math. Theor. 40 (2007) 13101-13106. | 10.1088/1751-8113/40/43/017 | null | quant-ph | null | We derive a multipartite generalized Bell inequality which involves the
entire range of settings for each of the local observers. Especially, it is
applied to show non-local behavior of a six-qubit mixture of
Greenberger-Horne-Zeilinger correlations stronger than previous Bell
inequalities. For certain noise admixture to the correlations an explicit local
realistic model exists in the case of a standard Bell experiment. Bell
experiments with many local settings reveal the non-locality of the state. It
turns out that the new inequality is more stringent than many other Bell
inequalities in the specific quantum state.
| [{'version': 'v1', 'created': 'Mon, 14 May 2007 10:48:43 GMT'}
{'version': 'v2', 'created': 'Mon, 10 Sep 2007 06:02:15 GMT'}] | 2009-11-13 | [array(['Nagata', 'Koji', ''], dtype=object)] |
463 | 1805.11178 | Alexander Binder | Alexander Binder, Michael Bockmayr, Miriam H\"agele, Stephan Wienert,
Daniel Heim, Katharina Hellweg, Albrecht Stenzinger, Laura Parlow, Jan
Budczies, Benjamin Goeppert, Denise Treue, Manato Kotani, Masaru Ishii,
Manfred Dietel, Andreas Hocke, Carsten Denkert, Klaus-Robert M\"uller,
Frederick Klauschen | Towards computational fluorescence microscopy: Machine learning-based
integrated prediction of morphological and molecular tumor profiles | null | null | null | null | cs.CV | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recent advances in cancer research largely rely on new developments in
microscopic or molecular profiling techniques offering high level of detail
with respect to either spatial or molecular features, but usually not both.
Here, we present a novel machine learning-based computational approach that
allows for the identification of morphological tissue features and the
prediction of molecular properties from breast cancer imaging data. This
integration of microanatomic information of tumors with complex molecular
profiling data, including protein or gene expression, copy number variation,
gene methylation and somatic mutations, provides a novel means to
computationally score molecular markers with respect to their relevance to
cancer and their spatial associations within the tumor microenvironment.
| [{'version': 'v1', 'created': 'Mon, 28 May 2018 21:16:30 GMT'}] | 2018-05-30 | [array(['Binder', 'Alexander', ''], dtype=object)
array(['Bockmayr', 'Michael', ''], dtype=object)
array(['Hägele', 'Miriam', ''], dtype=object)
array(['Wienert', 'Stephan', ''], dtype=object)
array(['Heim', 'Daniel', ''], dtype=object)
array(['Hellweg', 'Katharina', ''], dtype=object)
array(['Stenzinger', 'Albrecht', ''], dtype=object)
array(['Parlow', 'Laura', ''], dtype=object)
array(['Budczies', 'Jan', ''], dtype=object)
array(['Goeppert', 'Benjamin', ''], dtype=object)
array(['Treue', 'Denise', ''], dtype=object)
array(['Kotani', 'Manato', ''], dtype=object)
array(['Ishii', 'Masaru', ''], dtype=object)
array(['Dietel', 'Manfred', ''], dtype=object)
array(['Hocke', 'Andreas', ''], dtype=object)
array(['Denkert', 'Carsten', ''], dtype=object)
array(['Müller', 'Klaus-Robert', ''], dtype=object)
array(['Klauschen', 'Frederick', ''], dtype=object)] |
464 | astro-ph/0510418 | Eric Aristidi | Abdelkrim Agabi (LUAN), Eric Aristidi (LUAN), Max Azouit (LUAN), Eric
Fossat (LUAN), Francois Martin (LUAN), Tatiana Sadibekova (LUAN), Jean Vernin
(LUAN), Aziz Ziad (LUAN) | First whole atmosphere night-time seeing measurements at Dome C,
Antarctica | accepted for publication in PASP (oct 2005) | Publ.Astron.Soc.Pac.118:344-348,2006 | 10.1086/498728 | null | astro-ph | null | We report site testing results obtained in night-time during the polar autumn
and winter at Dome C. These results were collected during the first Concordia
winterover by A. Agabi. They are based upon seeing and isoplanatic angle
monitoring, as well as in-situ balloon measurements 2 of the refractive index
structure constant profiles Cn (h). Atmosphere is divided into two regions: (i)
a 36 m high surface layer responsible of 87% of the turbulence and (ii) a very
stable free atmosphere above with a median seeing of 0.36+-0.19 arcsec at an
elevation of h = 30 m. The median seeing measured with a DIMM placed on top of
a 8.5 m high tower is 1.3+-0.8 arcsec.
| [{'version': 'v1', 'created': 'Fri, 14 Oct 2005 07:05:17 GMT'}] | 2009-11-13 | [array(['Agabi', 'Abdelkrim', '', 'LUAN'], dtype=object)
array(['Aristidi', 'Eric', '', 'LUAN'], dtype=object)
array(['Azouit', 'Max', '', 'LUAN'], dtype=object)
array(['Fossat', 'Eric', '', 'LUAN'], dtype=object)
array(['Martin', 'Francois', '', 'LUAN'], dtype=object)
array(['Sadibekova', 'Tatiana', '', 'LUAN'], dtype=object)
array(['Vernin', 'Jean', '', 'LUAN'], dtype=object)
array(['Ziad', 'Aziz', '', 'LUAN'], dtype=object)] |
465 | 1903.05311 | Shaoru Chen | Ximing Chen, Shaoru Chen, Victor M. Preciado | Safety Verification of Nonlinear Autonomous System via Occupation
Measures | Update proofs | null | null | null | math.OC | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we introduce a flexible notion of safety verification for
nonlinear autonomous systems by measuring how much time the system spends in
given unsafe regions. We consider this problem in the particular case of
nonlinear systems with a polynomial dynamics and unsafe regions described by a
collection of polynomial inequalities. In this context, we can quantify the
amount of time spent in the unsafe regions as the solution to an
infinite-dimensional linear program (LP). This LP measures the volume of the
unsafe region with respect to the occupation measure of the system
trajectories. Using Lasserre hierarchy, we approximate the solution to the
infinite-dimensional LP using a sequence of finite-dimensional semidefinite
programs (SDPs). The solutions to the SDPs in this hierarchy provide
monotonically converging upper bounds on the optimal solution to the
infinite-dimensional LP. Finally, we validate the performance of our framework
using numerical simulations.
| [{'version': 'v1', 'created': 'Wed, 13 Mar 2019 04:49:49 GMT'}
{'version': 'v2', 'created': 'Thu, 11 Apr 2019 17:11:39 GMT'}] | 2019-04-12 | [array(['Chen', 'Ximing', ''], dtype=object)
array(['Chen', 'Shaoru', ''], dtype=object)
array(['Preciado', 'Victor M.', ''], dtype=object)] |
466 | 0811.3770 | Denis Burgarella | Denis Burgarella, Veronique Buat, Tsutomu T. Takeuchi, Takehiko Wada
and Chris Pearson | Deep 15um AKARI observations in the CDFS: estimating dust luminosities
for a MIR-selected sample and for Lyman Break Galaxies and the evolution of
L(dust)/L(UV) with the redshift | Paper accepted for publication in PASJ | null | 10.1093/pasj/61.2.177 | null | astro-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Deep observations of the CDFS have been secured at 15um with AKARI/IRC
infrared space telescope (ESA open time). From these observations, we define a
sample of MIR-selected galaxies at 15um and we also obtain 15um flux densities
for a sample of LBGs at z=1 already observed at 24um with Spitzer/MIPS. Number
counts for the MIR-selected sample show a bump around a 15um flux density of
0.2mJy that can be attributed to galaxies at z>0.4 and at z>0.8 for the fainter
part of the bump. This bump seems to be shifted as compared to other works and
a possible origin can be the Cosmic variance. Thanks to this dataset, we have
tested, on the two above samples at z=1, the validity of the conversions from
monochromatic luminosities nu.f(nu) at a rest-frame wavelength of 8um by a
comparison with total dust luminosities estimated from Spitzer rest-frame 12um
data that we use as a reference. We find that the 8um dust luminosities are not
all consistent and that some of them are better when compared to L(dust)
evaluated from longer wavelength luminosities. We also find that the rest-frame
8um luminosities provide globally good estimates of L(dust). By comparing our
data for the two samples to several libraries of SEDs, we find that models can
explain the diversity of the observed f(24)/f(15) ratio quite reasonably for
the MIR-selected sample and better for the LBG sample which are less dispersed
than the MIR selection. However, when we analyse the luminosity dependence of
this ratio, we find important discrepancies. Finally, we revisit the evolution
of L(dust)/L(UV) ratio with the redshift z by re-calibrating previous L(dust)
at z=2 based on our results and added new data points at higher redshifts. The
decreasing trend is amplified as compared to the previous estimate.
| [{'version': 'v1', 'created': 'Sun, 23 Nov 2008 20:48:49 GMT'}] | 2015-05-13 | [array(['Burgarella', 'Denis', ''], dtype=object)
array(['Buat', 'Veronique', ''], dtype=object)
array(['Takeuchi', 'Tsutomu T.', ''], dtype=object)
array(['Wada', 'Takehiko', ''], dtype=object)
array(['Pearson', 'Chris', ''], dtype=object)] |
467 | 0905.4582 | Peter Grassl | Jan Novak, Chris J. Pearce, Peter Grassl, Liu Yang, James Thomason | Analysis of the microbond test using nonlinear fracture mechanics | Submitted to 17th international conference on composite materials
(ICCM-17) | null | null | null | cond-mat.mtrl-sci | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Microbond tests composed of single fibre and matrix droplet are often used to
determine the properties of fibre reinforced composites. Interfacial shear
strength is quantified by the maximum pull-out force assuming a uniform stress
distribution along the fibre. Here, nonlinear finite element analyses are
performed to investigate the validity of this assumption.
| [{'version': 'v1', 'created': 'Thu, 28 May 2009 09:08:28 GMT'}] | 2009-05-29 | [array(['Novak', 'Jan', ''], dtype=object)
array(['Pearce', 'Chris J.', ''], dtype=object)
array(['Grassl', 'Peter', ''], dtype=object)
array(['Yang', 'Liu', ''], dtype=object)
array(['Thomason', 'James', ''], dtype=object)] |
468 | 1611.06602 | Jovan Milosevic | P. Cirkovic and D. Devetak and M. Dordevic and J. Milosevic and M.
Stojanovic | Sub-leading flow modes in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
from HYDJET++ model | 10 pages, 7 figures | Chinese Physics C Vol. 41, No. 7 (2017) 074001 | 10.1088/1674-1137/41/7/074001 | null | nucl-ex | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recent LHC results on the appearance of sub-leading flow modes in PbPb
collisions at 2.76~TeV, related to initial-state fluctuations, are analyzed and
interpreted within the HYDJET++ model. Using the newly introduced Principal
Component Analysis (PCA) method applied to two-particle azimuthal correlations
extracted from the model calculations, the leading and the sub-leading flow
modes are studied as a function of the transverse momentum ($p_{T}$) over a
wide centrality range. The leading modes of the elliptic ($v^{(1)}_{2}$) and
triangular ($v^{(1)}_{3}$) flow calculated within the HYDJET++ model reproduce
rather well the $v_{2}\{2\}$ and $v_{3}\{2\}$ coefficients experimentally
measured using the two-particle correlations. Within the $p_{T} \le $~3~GeV/c
range where hydrodynamics dominates, the sub-leading flow effects are greatest
at the highest $p_{T}$ of around 3~GeV/c. The sub-leading elliptic flow mode
($v^{(2)}_{2}$), which corresponds to $n = 2$ harmonic, has a small non-zero
value and slowly increases from central to peripheral collisions, while the
sub-leading triangular flow mode ($v^{(2)}_{3}$), which corresponds to $n = 3$
harmonic, is even smaller and does not depend on centrality. For $n = $~2, the
relative magnitude of the effect measured with respect to the leading flow mode
shows a shallow minimum for semi-central collisions and increases for very
central and for peripheral collisions. For $n = $~3 case, there is no
centrality dependence. The sub-leading flow mode results obtained from the
HYDJET++ model are in a rather good agreement with the experimental
measurements of the CMS Collaboration.
| [{'version': 'v1', 'created': 'Sun, 20 Nov 2016 22:16:37 GMT'}
{'version': 'v2', 'created': 'Wed, 1 Feb 2017 13:22:21 GMT'}
{'version': 'v3', 'created': 'Fri, 31 Mar 2017 20:53:22 GMT'}] | 2017-04-24 | [array(['Cirkovic', 'P.', ''], dtype=object)
array(['Devetak', 'D.', ''], dtype=object)
array(['Dordevic', 'M.', ''], dtype=object)
array(['Milosevic', 'J.', ''], dtype=object)
array(['Stojanovic', 'M.', ''], dtype=object)] |
469 | cond-mat/0210526 | Nicolai Nygaard | N. Nygaard, G. M. Bruun, C. W. Clark and D. L. Feder | Microscopic Structure of a Vortex Line in a Superfluid Fermi Gas | 4 pages, 4 embedded figures. Added references. To be published in
Physical Review Letters | Phys. Rev. Lett. 90, 210402 (2003) | 10.1103/PhysRevLett.90.210402 | null | cond-mat.soft cond-mat.mes-hall cond-mat.supr-con | null | The microscopic properties of a single vortex in a dilute superfluid Fermi
gas at zero temperature are examined within the framework of self-consistent
Bogoliubov-de Gennes theory. Using only physical parameters as input, we study
the pair potential, the density, the energy, and the current distribution.
Comparison of the numerical results with analytical expressions clearly
indicates that the energy of the vortex is governed by the zero-temperature BCS
coherence length.
| [{'version': 'v1', 'created': 'Wed, 23 Oct 2002 17:49:18 GMT'}
{'version': 'v2', 'created': 'Wed, 16 Apr 2003 17:03:26 GMT'}] | 2007-05-23 | [array(['Nygaard', 'N.', ''], dtype=object)
array(['Bruun', 'G. M.', ''], dtype=object)
array(['Clark', 'C. W.', ''], dtype=object)
array(['Feder', 'D. L.', ''], dtype=object)] |
470 | 1906.09907 | Sibylle Hess | Sibylle Hess and Katharina Morik | C-SALT: Mining Class-Specific ALTerations in Boolean Matrix
Factorization | Joint European Conference on Machine Learning and Knowledge Discovery
in Databases. Springer, Cham, 2017 | null | null | null | cs.LG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Given labeled data represented by a binary matrix, we consider the task to
derive a Boolean matrix factorization which identifies commonalities and
specifications among the classes. While existing works focus on rank-one
factorizations which are either specific or common to the classes, we derive
class-specific alterations from common factorizations as well. Therewith, we
broaden the applicability of our new method to datasets whose
class-dependencies have a more complex structure. On the basis of synthetic and
real-world datasets, we show on the one hand that our method is able to filter
structure which corresponds to our model assumption, and on the other hand that
our model assumption is justified in real-world application. Our method is
parameter-free.
| [{'version': 'v1', 'created': 'Mon, 17 Jun 2019 22:38:00 GMT'}] | 2019-06-25 | [array(['Hess', 'Sibylle', ''], dtype=object)
array(['Morik', 'Katharina', ''], dtype=object)] |
471 | math/0209002 | Martino Prizzi | M. Prizzi and K.P. Rybakowski | Inertial manifolds on squeezed domains | 39 pages, 3 figures. To appear in "Jour. Dynam. Differerential
Equations" | null | null | null | math.AP math.DS | null | Let $\Omega$ be an arbitrary smooth bounded domain in $\R^2$ and $\epsilon>0$
be arbitrary. Squeeze $\Omega$ by the factor $\epsilon$ in the $y$-direction to
obtain the squeezed domain $\Omega_\epsilon=\{(x,\epsilon y)\mid (x,y)\in\Omega
\}$. In this paper we study the family of reaction-diffusion equations $$
\alignedat 2 u_t&=\Delta u+f(u),&\quad &t>0, (x,y)\in\Omega_\epsilon
\partial_{\nu_\epsilon} u&=0,& & t>0,
(x,y)\in\partial\Omega_\epsilon,\endalignedat\tag $E_\epsilon$ $$ where $f$ is
a dissipative nonlinearity of polynomial growth. In a previous paper we showed
that, as $\epsilon\to 0$, the equations $(E_\epsilon)$ have a limiting equation
which is an abstract semilinear parabolic equation defined on a closed linear
subspace of $H^1(\Omega)$. We also proved that the family ${\Cal A}_\epsilon$
of the corresponding attractors is upper semicontinuous at $\epsilon=0$. In
this paper we prove that, if $\Omega$ satisfies some natural assumptions, then
the limiting equation can be characterized as a reaction-diffusion equation on
a finite topological graph. Moreover, there is a family $\Cal M_\epsilon$ of
inertial $C^1$-manifolds for $(E_\epsilon)$, of some fixed finite dimension
$\nu$, and, as $\epsilon\to 0$, the flow on $\Cal M_\epsilon$ converges in the
$C^1$-sense to the limit flow on $\Cal M_0$.
| [{'version': 'v1', 'created': 'Sat, 31 Aug 2002 09:45:58 GMT'}] | 2007-05-23 | [array(['Prizzi', 'M.', ''], dtype=object)
array(['Rybakowski', 'K. P.', ''], dtype=object)] |
472 | 2008.12508 | Tony A. Wood | Mitchell Khoo, Tony A. Wood, Chris Manzie, Iman Shames | A Greedy and Distributable Approach to the Lexicographic Bottleneck
Assignment Problem with Conditions on Exactness | null | null | null | null | math.OC | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Solving the Lexicographic Bottleneck Assignment Problem (LexBAP) typically
relies on centralised computation with order quartic complexity. We consider
the Sequential Bottleneck Assignment Problem (SeqBAP), which yields a greedy
solution to the LexBAP and discuss the relationship between the SeqBAP, the
LexBAP, and the Bottleneck Assignment Problem (BAP). In particular, we
reexamine tools used to analyse the structure of the BAP, and apply them to
derive an algorithm that solves the SeqBAP with cubic complexity. We show that
the set of solutions of the LexBAP is a subset of the solutions of the SeqBAP
and analyse the conditions for which the solutions sets are identical.
Furthermore, we provide a method to verify the satisfaction of these
conditions. In cases where the conditions are satisfied, the proposed algorithm
for solving the SeqBAP solves the LexBAP with computation that has lower
complexity and can be distributed over a network of computing agents. The
applicability of the approach is demonstrated with a case study where mobile
robots are assigned to goal locations.
| [{'version': 'v1', 'created': 'Fri, 28 Aug 2020 07:05:55 GMT'}
{'version': 'v2', 'created': 'Fri, 7 Jan 2022 20:17:47 GMT'}] | 2022-01-11 | [array(['Khoo', 'Mitchell', ''], dtype=object)
array(['Wood', 'Tony A.', ''], dtype=object)
array(['Manzie', 'Chris', ''], dtype=object)
array(['Shames', 'Iman', ''], dtype=object)] |
473 | 2107.13910 | Jianfang Lin | Jianfang Lin, Yan Yu, Huiwen Xue and Xinghui Zhong | High order finite difference WENO methods with unequal-sized
sub-stencils for the Degasperis-Procesi type equations | null | null | 10.4208/cicp.OA-2021-0158 | null | math.NA cs.NA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we develop two finite difference weighted essentially
non-oscillatory (WENO) schemes with unequal-sized sub-stencils for solving the
Degasperis-Procesi (DP) and $\mu$-Degasperis-Procesi ($\mu$DP) equations, which
contain nonlinear high order derivatives, and possibly peakon solutions or
shock waves. By introducing auxiliary variable(s), we rewrite the DP equation
as a hyperbolic-elliptic system, and the \mdp equation as a first order system.
Then we choose a linear finite difference scheme with suitable order of
accuracy for the auxiliary variable(s), and two finite difference WENO schemes
with unequal-sized sub-stencils for the primal variable. One WENO scheme uses
one large stencil and several smaller stencils, and the other WENO scheme is
based on the multi-resolution framework which uses a series of unequal-sized
hierarchical central stencils. Comparing with the classical WENO scheme which
uses several small stencils of the same size to make up a big stencil, both
WENO schemes with unequal-sized sub-stencils are simple in the choice of the
stencil and enjoy the freedom of arbitrary positive linear weights. Another
advantage is that the final reconstructed polynomial on the target cell is a
polynomial of the same degree as the polynomial over the big stencil, while the
classical finite difference WENO reconstruction can only be obtained for
specific points inside the target interval. Numerical tests are provided to
demonstrate the high order accuracy and non-oscillatory properties of the
proposed schemes.
| [{'version': 'v1', 'created': 'Thu, 29 Jul 2021 11:40:37 GMT'}
{'version': 'v2', 'created': 'Wed, 22 Dec 2021 06:12:03 GMT'}] | 2022-03-14 | [array(['Lin', 'Jianfang', ''], dtype=object)
array(['Yu', 'Yan', ''], dtype=object)
array(['Xue', 'Huiwen', ''], dtype=object)
array(['Zhong', 'Xinghui', ''], dtype=object)] |
474 | 1801.08731 | \'Elie Goudout | \'Elie Goudout | Highest perfect power of a product of integers less than $x$ | 1 page, accepted for publication in the IJNT | Int. J. Number Theory, 14(7)(2018):2043-2044 | 10.1142/S1793042118501233 | null | math.NT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | For $x\geq 3$, we define $w(x)$ as the highest integer $w$ for which there
exist integers $m, y\geq 1$ and $1\leq n_1<\dots<n_m\leq x$ such that
$n_1\cdots n_m=y^w$. We show that \[w(x)=x\exp\big(-(\sqrt{2}+o(1))\sqrt{\log
x\log\log x}\big).\]
| [{'version': 'v1', 'created': 'Fri, 26 Jan 2018 09:40:24 GMT'}] | 2022-09-27 | [array(['Goudout', 'Élie', ''], dtype=object)] |
475 | 1812.08156 | Alex Zihao Zhu | Alex Zihao Zhu, Liangzhe Yuan, Kenneth Chaney, Kostas Daniilidis | Unsupervised Event-based Learning of Optical Flow, Depth, and Egomotion | 9 pages, 7 figures | null | null | null | cs.CV | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work, we propose a novel framework for unsupervised learning for
event cameras that learns motion information from only the event stream. In
particular, we propose an input representation of the events in the form of a
discretized volume that maintains the temporal distribution of the events,
which we pass through a neural network to predict the motion of the events.
This motion is used to attempt to remove any motion blur in the event image. We
then propose a loss function applied to the motion compensated event image that
measures the motion blur in this image. We train two networks with this
framework, one to predict optical flow, and one to predict egomotion and
depths, and evaluate these networks on the Multi Vehicle Stereo Event Camera
dataset, along with qualitative results from a variety of different scenes.
| [{'version': 'v1', 'created': 'Wed, 19 Dec 2018 18:50:54 GMT'}] | 2018-12-20 | [array(['Zhu', 'Alex Zihao', ''], dtype=object)
array(['Yuan', 'Liangzhe', ''], dtype=object)
array(['Chaney', 'Kenneth', ''], dtype=object)
array(['Daniilidis', 'Kostas', ''], dtype=object)] |
476 | 2103.00456 | Gaoqing Cao | Gaoqing Cao | Recent progresses on QCD phases in a strong magnetic field -- views from
Nambu--Jona-Lasinio model | null | null | 10.1140/epja/s10050-021-00570-0 | null | hep-ph nucl-th | http://creativecommons.org/licenses/by-nc-sa/4.0/ | In this review, we summarize recent progress on the possible phases of
quantum chromodynamics (QCD) in the presence of a strong magnetic field, mainly
from the views of the chiral effective Nambu--Jona-Lasinio model. Four kinds of
phase transitions are explored in detail: chiral symmetry breaking and
restoration, neutral pseudoscalar superfluidity, charged pion superfluidity and
charged rho superconductivity. In particular, we revisit the unsolved problems
of inverse magnetic catalysis effect and competition between the chiral density
wave and solitonic modulation phases. It is shown that useful results can be
obtained by adopting self-consistent schemes.
| [{'version': 'v1', 'created': 'Sun, 28 Feb 2021 11:11:04 GMT'}
{'version': 'v2', 'created': 'Sun, 11 Jul 2021 02:45:47 GMT'}
{'version': 'v3', 'created': 'Tue, 17 Aug 2021 02:16:23 GMT'}] | 2023-02-22 | [array(['Cao', 'Gaoqing', ''], dtype=object)] |
477 | 2209.01381 | Nasrin Shirali | Sayed Malek Javdannezhad, Mohammad Maschizadeh and Nasrin Shirali | On AB5* modules with Noetherian dimension | null | null | null | null | math.RA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we study the Noetherian dimension of sum of certain modules.
It is proved that for any module M which is an irredundant sum of submodules,
each of which has Noetherian dimension less than alpha, if M has finite
spanning dimension (fsd-module, for short) or it is a weakly atomic module,
then Noetherian dimension M less than alpha. Here, by a weakly atomic module we
mean a module M for which every proper non-small submodule N, has Noetherian
dimension strictly less than that of M. Also, it is proved that if M is an AB5*
module with Noetherian dimension and N_i is a family of submodules of M such
that Noetherian dimension M over N_i, less than alpha, for each i, then
Noetherian dimension M over intersection of N_is less than alpha. Using this,
we give a structure theorem for alpha-short modules in the category of AB5* and
finally, we classify alpha-short modules in this category.
| [{'version': 'v1', 'created': 'Sat, 3 Sep 2022 09:27:59 GMT'}
{'version': 'v2', 'created': 'Fri, 23 Jun 2023 17:11:13 GMT'}] | 2023-06-26 | [array(['Javdannezhad', 'Sayed Malek', ''], dtype=object)
array(['Maschizadeh', 'Mohammad', ''], dtype=object)
array(['Shirali', 'Nasrin', ''], dtype=object)] |
478 | 1809.00572 | Leigh Fletcher | L.N. Fletcher, G.S. Orton, J.A. Sinclair, S. Guerlet, P.L. Read, A.
Antunano, R.K. Achterberg, F.M. Flasar, P.G.J. Irwin, G.L. Bjoraker, J.
Hurley, B.E. Hesman, M. Segura, N. Gorius, A. Mamoutkine, S.B. Calcutt | A Hexagon in Saturn's Northern Stratosphere Surrounding the Emerging
Summertime Polar Vortex | 51 pages, 12 figures, published in Nature Communications | Nature Communications, Volume 9, Article number: 3564 (2018) | 10.1038/s41467-018-06017-3 | null | astro-ph.EP | http://creativecommons.org/licenses/by/4.0/ | Saturn's polar stratosphere exhibits the seasonal growth and dissipation of
broad, warm, vortices poleward of $\sim75^\circ$ latitude, which are strongest
in the summer and absent in winter. The longevity of the exploration of the
Saturn system by Cassini allows the use of infrared spectroscopy to trace the
formation of the North Polar Stratospheric Vortex (NPSV), a region of enhanced
temperatures and elevated hydrocarbon abundances at millibar pressures. We
constrain the timescales of stratospheric vortex formation and dissipation in
both hemispheres. Although the NPSV formed during late northern spring, by the
end of Cassini's reconnaissance (shortly after northern summer solstice), it
still did not display the contrasts in temperature and composition that were
evident at the south pole during southern summer. The newly-formed NPSV was
bounded by a strengthening stratospheric thermal gradient near $78^\circ$N. The
emergent boundary was hexagonal, suggesting that the Rossby wave responsible
for Saturn's long-lived polar hexagon - which was previously expected to be
trapped in the troposphere - can influence the stratospheric temperatures some
300 km above Saturn's clouds.
| [{'version': 'v1', 'created': 'Mon, 3 Sep 2018 12:13:36 GMT'}] | 2018-09-05 | [array(['Fletcher', 'L. N.', ''], dtype=object)
array(['Orton', 'G. S.', ''], dtype=object)
array(['Sinclair', 'J. A.', ''], dtype=object)
array(['Guerlet', 'S.', ''], dtype=object)
array(['Read', 'P. L.', ''], dtype=object)
array(['Antunano', 'A.', ''], dtype=object)
array(['Achterberg', 'R. K.', ''], dtype=object)
array(['Flasar', 'F. M.', ''], dtype=object)
array(['Irwin', 'P. G. J.', ''], dtype=object)
array(['Bjoraker', 'G. L.', ''], dtype=object)
array(['Hurley', 'J.', ''], dtype=object)
array(['Hesman', 'B. E.', ''], dtype=object)
array(['Segura', 'M.', ''], dtype=object)
array(['Gorius', 'N.', ''], dtype=object)
array(['Mamoutkine', 'A.', ''], dtype=object)
array(['Calcutt', 'S. B.', ''], dtype=object)] |
479 | nucl-th/0110056 | Arturo De Pace | A. De Pace and A. Molinari (INFN and Dipartimento di Fisica Teorica,
Torino, Italy) | Statistical theory of the many-body nuclear system | 27 pages, 3 figures; Dedicated to the memory of Herman Feshbach | Annals Phys. 296 (2002) 263-286 | 10.1006/aphy.2001.6205 | null | nucl-th | null | A recently proposed statistical theory of the mean fields associated with the
ground and excited collective states of a generic many-body system is extended
by increasing the dimensions of the P-space. In applying the new framework to
nuclear matter, in addition to the mean field energies we obtain their
fluctuations as well, together with the ones of the wavefunctions, in first
order of the expansion in the complexity of the Q-space states. The physics
described by the latter is assumed to be random. To extract numerical
predictions out of our scheme we develop a schematic version of the approach,
which, while much simplified, yields results of significance on the size of the
error affecting the mean fields, on the magnitude of the residual effective
interaction, on the ground state spectroscopic factor and on the mixing
occurring between the vectors spanning the P-space.
| [{'version': 'v1', 'created': 'Tue, 23 Oct 2001 14:07:40 GMT'}] | 2009-11-07 | [array(['De Pace', 'A.', '',
'INFN and Dipartimento di Fisica Teorica,\n Torino, Italy'],
dtype=object)
array(['Molinari', 'A.', '',
'INFN and Dipartimento di Fisica Teorica,\n Torino, Italy'],
dtype=object) ] |
480 | 1107.4584 | Guray Erkol | Guray Erkol and Altug Ozpineci | Tensor form factors of nucleon in QCD | 8 pages, 1 figure; minor changes, matches journal version | Phys. Lett. B 704 (2011) 551 | 10.1016/j.physletb.2011.09.089 | null | hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We extract the isovector tensor nucleon form factors, which play an important
role in understanding the transverse spin structure of the nucleon when related
to the quark helicity-flip generalized parton distributions via their first
moments. We employ the light-cone QCD sum rules to leading order in QCD and
include distribution amplitudes up to twist 6 in order to calculate the three
tensor form factors $H_T$, $E_T$ and $\tilde{H}_T$. Our results agree well with
those from other approaches in the low and high momentum-transfer regions.
| [{'version': 'v1', 'created': 'Fri, 22 Jul 2011 17:39:39 GMT'}
{'version': 'v2', 'created': 'Fri, 7 Oct 2011 12:07:29 GMT'}] | 2011-10-10 | [array(['Erkol', 'Guray', ''], dtype=object)
array(['Ozpineci', 'Altug', ''], dtype=object)] |
481 | 0903.2989 | Karsten Held | Y.-F. Yang and K. Held | Dynamical mean field theory for manganites | 11 pages, 18 figures In the 2nd version the only change is to correct
one (important) reference | null | 10.1103/PhysRevB.82.195109 | null | cond-mat.str-el cond-mat.mtrl-sci | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Doped and undoped manganites are modeled by the coupling between itinerant
$e_g$ electrons and static $t_{2g}$ spins, the Jahn-Teller and breathing phonon
modes, and the Coulomb interaction. We provide for a careful estimate of all
parameters and solve the corresponding Hamiltonian by dynamical mean field
theory. Our results for the one-electron spectrum, the optical conductivity,
the dynamic and static lattice distortion, as well as the Curie temperature
show the importance of all of the above ingredients for a realistic calculation
as well as for describing the unusual dynamical properties of manganites
including the insulating parent compound and the insulating-like paramagnetic
state of doped manganites.
| [{'version': 'v1', 'created': 'Tue, 17 Mar 2009 16:05:21 GMT'}
{'version': 'v2', 'created': 'Fri, 20 Mar 2009 07:52:20 GMT'}] | 2013-05-29 | [array(['Yang', 'Y. -F.', ''], dtype=object)
array(['Held', 'K.', ''], dtype=object)] |
482 | nucl-th/0507066 | Kazunari Kaneko | K. Kaneko and M. Hasegawa | Quenching of pairing gap at finite temperature in 184W | 5 pages, 4 figures, accepted for publication in PRC | Phys.Rev. C72 (2005) 024307 | 10.1103/PhysRevC.72.024307 | null | nucl-th | null | We extract pairing gap in $^{184}$W at finite temperature for the first time
from the experimental level densities of $^{183}$W, $^{184}$W, and $^{185}$W
using "thermal" odd-even mass difference. We found the quenching of pairing gap
near the critical temperature $T_c = 0.47$ MeV in the BCS calculations. It is
shown that the monopole pairing model with a deformed Woods-Saxon potential
explains the reduction of the pairing correlation using the partition function
with the number parity projection in the static path approximation plus
random-phase approximation.
| [{'version': 'v1', 'created': 'Wed, 27 Jul 2005 02:43:26 GMT'}] | 2009-11-11 | [array(['Kaneko', 'K.', ''], dtype=object)
array(['Hasegawa', 'M.', ''], dtype=object)] |
483 | cs/0610091 | Pedro Miramontes | R. Mansilla, E. K\"oppen, G. Cocho and P. Miramontes | On the Behavior of Journal Impact Factor Rank-Order Distribution | Submitted to the Journal of Informetrics, redundat text cropped,
bibliography corrected, new section added, typos corrected | null | null | null | cs.IR physics.soc-ph | null | An empirical law for the rank-order behavior of journal impact factors is
found. Using an extensive data base on impact factors including journals on
Education, Agrosciences, Geosciences, Biosciences and Environ- mental,
Chemical, Computer, Engineering, Material, Mathematical, Medical and Physical
Sciences we have found extremely good fits out- performing other rank-order
models. Some extensions to other areas of knowledge are discussed.
| [{'version': 'v1', 'created': 'Sat, 14 Oct 2006 17:03:46 GMT'}
{'version': 'v2', 'created': 'Tue, 17 Oct 2006 14:10:01 GMT'}
{'version': 'v3', 'created': 'Thu, 26 Oct 2006 17:54:29 GMT'}
{'version': 'v4', 'created': 'Sun, 24 Dec 2006 06:03:44 GMT'}] | 2007-05-23 | [array(['Mansilla', 'R.', ''], dtype=object)
array(['Köppen', 'E.', ''], dtype=object)
array(['Cocho', 'G.', ''], dtype=object)
array(['Miramontes', 'P.', ''], dtype=object)] |
484 | cs/0505051 | Jaime Gomez | Jaime Gomez, Ignacio Melgar, Juan Seijas, Diego Andina | Sub-Optimum Signal Linear Detector Using Wavelets and Support Vector
Machines | 6 pages | WSEAS Transactions on Communications, ISSN 1109-2742, issue 4, vol
2, p426-431, October-2003 | null | null | cs.IR cs.NE | null | The problem of known signal detection in Additive White Gaussian Noise is
considered. In previous work, a new detection scheme was introduced by the
authors, and it was demonstrated that optimum performance cannot be reached in
a real implementation. In this paper we analyse Support Vector Machines (SVM)
as an alternative, evaluating the results in terms of Probability of detection
curves for a fixed Probability of false alarm.
| [{'version': 'v1', 'created': 'Fri, 20 May 2005 14:54:40 GMT'}] | 2007-05-23 | [array(['Gomez', 'Jaime', ''], dtype=object)
array(['Melgar', 'Ignacio', ''], dtype=object)
array(['Seijas', 'Juan', ''], dtype=object)
array(['Andina', 'Diego', ''], dtype=object)] |
485 | 0910.1664 | Paul Joyce | Erkan Ozge Buzbas, Paul Joyce | Maximum likelihood estimates under $\mathbf{k}$-allele models with
selection can be numerically unstable | Published in at http://dx.doi.org/10.1214/09-AOAS237 the Annals of
Applied Statistics (http://www.imstat.org/aoas/) by the Institute of
Mathematical Statistics (http://www.imstat.org) | Annals of Applied Statistics 2009, Vol. 3, No. 3, 1147-1162 | 10.1214/09-AOAS237 | IMS-AOAS-AOAS237 | stat.AP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The stationary distribution of allele frequencies under a variety of
Wright--Fisher $k$-allele models with selection and parent independent mutation
is well studied. However, the statistical properties of maximum likelihood
estimates of parameters under these models are not well understood. Under each
of these models there is a point in data space which carries the strongest
possible signal for selection, yet, at this point, the likelihood is unbounded.
This result remains valid even if all of the mutation parameters are assumed to
be known. Therefore, standard simulation approaches used to approximate the
sampling distribution of the maximum likelihood estimate produce numerically
unstable results in the presence of substantial selection. We describe the
Bayesian alternative where the posterior distribution tends to produce more
accurate and reliable interval estimates for the selection intensity at a
locus.
| [{'version': 'v1', 'created': 'Fri, 9 Oct 2009 07:17:26 GMT'}] | 2009-10-12 | [array(['Buzbas', 'Erkan Ozge', ''], dtype=object)
array(['Joyce', 'Paul', ''], dtype=object)] |
486 | 0902.2662 | David Sanchez | Mircea Crisan, David Sanchez, Rosa Lopez, Llorens Serra, Ioan Grosu | Localized magnetic states in Rashba dots | 8 pages, 4 figures; to appear in Phys. Rev. B | Phys. Rev. B 79, 125319 (2009) | 10.1103/PhysRevB.79.125319 | null | cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the formation of local moments in quantum dots arising in quasi-one
dimensional electron wires due to localized spin-orbit (Rashba) interaction.
Using an Anderson-like model to describe the occurrence of the magnetic moments
in these Rashba dots, we calculate the local magnetization within the
mean-field approximation. We find that the magnetization becomes a nontrivial
function of the Rashba coupling strength. We discuss both the equilibrium and
nonequilibrium cases. Interestingly, we obtain a magnetic phase which is stable
at large bias due to the Rashba interaction.
| [{'version': 'v1', 'created': 'Mon, 16 Feb 2009 11:10:21 GMT'}] | 2009-11-13 | [array(['Crisan', 'Mircea', ''], dtype=object)
array(['Sanchez', 'David', ''], dtype=object)
array(['Lopez', 'Rosa', ''], dtype=object)
array(['Serra', 'Llorens', ''], dtype=object)
array(['Grosu', 'Ioan', ''], dtype=object)] |
487 | 1103.0666 | Xuekai Ma | Xuekai Ma, Zhenjun Yang, Daquan Lu, Wei Hu | Multiple-type solutions for multipole interface solitons in thermal
nonlinear media | 5 pages, 5 figures | Phys. Rev. A 84, 033802 (2011) | 10.1103/PhysRevA.84.033802 | null | physics.optics | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We address the existence of multipole interface solitons in one-dimensional
thermal nonlinear media with a step in the linear refractive index at the
sample center. It is found that there exist two types of solutions for tripole
and quadrupole interface solitons. The two types of interface solitons have
different profiles, beam widths, mass centers, and stability regions. For a
given propagation constant, only one type of interface soliton is proved to be
stable, while the other type can also survive over a long distance. In
addition, three types of solutions for fifth-order interface solitons are
found.
| [{'version': 'v1', 'created': 'Thu, 3 Mar 2011 12:26:50 GMT'}
{'version': 'v2', 'created': 'Mon, 5 Sep 2011 03:16:06 GMT'}] | 2011-09-06 | [array(['Ma', 'Xuekai', ''], dtype=object)
array(['Yang', 'Zhenjun', ''], dtype=object)
array(['Lu', 'Daquan', ''], dtype=object)
array(['Hu', 'Wei', ''], dtype=object)] |
488 | 0709.3873 | John Davis | J. Davis, A.J. Booth, M.J. Ireland, A.P. Jacob, J.R. North, S.M.
Owens, J.G. Robertson, W.J. Tango and P.G. Tuthill | The Emergent Flux and Effective Temperature of Delta Canis Majoris | 8 pages, 4 figures | null | 10.1071/AS07017 | null | astro-ph | null | New angular diameter determinations for the bright southern F8 supergiant
Delta CMa enable the bolometric emergent flux and effective temperature of the
star to be determined with improved accuracy. The spectral flux distribution
and bolometric flux have been determined from published photometry and
spectrophotometry and combined with the angular diameter to derive the
bolometric emergent flux F = (6.50 plus/minus 0.24) x 10^7 W/m^2 and the
effective temperature Teff = 5818 plus/minus 53 K. The new value for the
effective temperature is compared with previous interferometric and infrared
flux method determinations. The accuracy of the effective temperature is now
limited by the uncertainty in the bolometric flux rather than by the
uncertainty in the angular diameter.
| [{'version': 'v1', 'created': 'Tue, 25 Sep 2007 04:53:59 GMT'}] | 2009-11-13 | [array(['Davis', 'J.', ''], dtype=object)
array(['Booth', 'A. J.', ''], dtype=object)
array(['Ireland', 'M. J.', ''], dtype=object)
array(['Jacob', 'A. P.', ''], dtype=object)
array(['North', 'J. R.', ''], dtype=object)
array(['Owens', 'S. M.', ''], dtype=object)
array(['Robertson', 'J. G.', ''], dtype=object)
array(['Tango', 'W. J.', ''], dtype=object)
array(['Tuthill', 'P. G.', ''], dtype=object)] |
489 | 1508.02228 | Chandan Singh Dalawat | Chandan Singh Dalawat | The ramification filtration in certain $p$-extensions | 5 pages, reorganised, filled in the details, and wrote a summary | null | null | null | math.NT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that the recent result of Casta\~neda and Wu about the ramification
filtration in certain $p$-extensions of function fields of prime characteristic
$p$ is equally valid over local fields of mixed characteristic $(0,p)$. Apart
from being applicable to both equicharacteristic and mixed characteristic
cases, our method has the advantage of being purely local, purely conceptual,
more natural, and much shorter.
| [{'version': 'v1', 'created': 'Mon, 10 Aug 2015 13:01:10 GMT'}
{'version': 'v2', 'created': 'Sun, 16 Aug 2015 07:01:10 GMT'}] | 2015-08-18 | [array(['Dalawat', 'Chandan Singh', ''], dtype=object)] |
490 | hep-ph/9611385 | Jiri Chyla | J. Chyla, J. Cvach | Virtual Photon Structure from Jet Production at HERA | Contribution to the Workshop on "Future Physics at HERA", eds. G.
Ingelman, A. De Roeck, R. Klanner,4 pages, 3 figures, epsfig | null | null | null | hep-ph | null | The feasibility of measuring parton distribution functions of of virtual
photons via the jet production at HERA is investigated.
| [{'version': 'v1', 'created': 'Thu, 21 Nov 1996 09:48:29 GMT'}] | 2007-05-23 | [array(['Chyla', 'J.', ''], dtype=object)
array(['Cvach', 'J.', ''], dtype=object)] |
491 | hep-lat/9801013 | Don Weingarten | W. Lee and D. Weingarten | The Scalar Quarkonium Spectrum and Quarkonium-Glueball Mixing | 3 pages, 4 PostScript figures, talk given at Lattice 97 | Nucl.Phys.Proc.Suppl. 63 (1998) 194-196 | 10.1016/S0920-5632(97)00719-6 | IBM-HET-97-1 | hep-lat | null | We evaluate the valence approximation to the mass of scalar quarkonium and to
the mixing energy between scalar quarkonium and the lightest scalar glueball
for a range of different lattice sizes and quark masses. Our results support
the identification of $f_0(1710)$ as the lightest scalar glueball.
| [{'version': 'v1', 'created': 'Wed, 14 Jan 1998 20:01:53 GMT'}] | 2009-10-31 | [array(['Lee', 'W.', ''], dtype=object)
array(['Weingarten', 'D.', ''], dtype=object)] |
492 | cond-mat/9805249 | Antonio Garcia-Martin | A. Garcia-Martin, J.A. Torres, J.J. Saenz and M. Nieto-Vesperinas | Intensity Distribution of Modes in Surface Corrugated Waveguides | null | Phys. Rev. Lett. 80, 4165 (1998) | 10.1103/PhysRevLett.80.4165 | null | cond-mat.dis-nn physics.optics | null | Exact calculations of transmission and reflection coefficients in surface
randomly corrugated optical waveguides are presented. As the length of the
corrugated part of the waveguide increases, there is a strong preference to
forward coupling through the lowest mode. An oscillating behavior of the
enhanced backscattering as a function of the wavelength is predicted. Although
the transport is strongly non isotropic, the analysis of the probability
distributions of the transmitted waves confirms in this configuration
distributions predicted by Random Matrix Theory for volume disorder.
| [{'version': 'v1', 'created': 'Wed, 20 May 1998 12:58:19 GMT'}] | 2009-10-31 | [array(['Garcia-Martin', 'A.', ''], dtype=object)
array(['Torres', 'J. A.', ''], dtype=object)
array(['Saenz', 'J. J.', ''], dtype=object)
array(['Nieto-Vesperinas', 'M.', ''], dtype=object)] |
493 | 1802.09115 | Ram Seshadri | Joshua D. Bocarsly, Ryan F. Need, Ram Seshadri, and Stephen D. Wilson | Magnetoentropic signatures of skyrmionic phase behavior in FeGe | 6 pages and 4 figures | Phys. Rev. B 97, 100404 (2018) | 10.1103/PhysRevB.97.100404 | null | cond-mat.mtrl-sci | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We demonstrate that magnetocaloric measurements can rapidly reveal details of
the phase diagrams of high-temperature skyrmion hosts, concurrently yielding
quantitative latent heats of the field-driven magnetic phase transitions. Our
approach addresses an outstanding issue in the phase diagram of the skyrmion
host FeGe by showing that dc magnetic anomalies can be explained in terms of
entropic signatures consistent with a phase diagram containing a single pocket
of skyrmionic order and a Brazovskii transition.
| [{'version': 'v1', 'created': 'Mon, 26 Feb 2018 00:41:31 GMT'}
{'version': 'v2', 'created': 'Tue, 3 Apr 2018 20:11:52 GMT'}] | 2018-04-11 | [array(['Bocarsly', 'Joshua D.', ''], dtype=object)
array(['Need', 'Ryan F.', ''], dtype=object)
array(['Seshadri', 'Ram', ''], dtype=object)
array(['Wilson', 'Stephen D.', ''], dtype=object)] |
494 | 2110.00819 | Ali Fathi | Ali Fathi, Mohammad Rashid, Shayan Ranjbarzadeh, Mojtaba Tefagh | Multi-Feasibility Variable Selection | null | null | null | null | cs.DC math.OC q-bio.MN q-bio.QM | http://creativecommons.org/licenses/by-nc-sa/4.0/ | This paper is the report of the problem proposed for the !Optimizer 2021
competition, and the solutions of the gold medalist team, i.e., the Panda team.
The competition was held in two stages, the research and development stage and
a two-week contest stage, consisting of five rounds, and seven teams succeeded
in finishing both stages to the end. In this joint report of the winner team
Panda and the problem design committee coordinated by Mojtaba Tefagh, we first
explain each of the five rounds and then provide the solutions proposed by our
team (Panda) to fulfill the required tasks in the fastest and most accurate
way. Afterward, some preprocessing and data manipulating ideas used to enhance
the algorithms would be presented. All codes are written in the Julia language,
which showed a better performance than Python on optimization problems in our
comparisons during the R&D stage, and are publicly available in the Github
repository: https://github.com/Optimizer-Competition-Panda
| [{'version': 'v1', 'created': 'Sat, 2 Oct 2021 14:55:49 GMT'}] | 2021-10-05 | [array(['Fathi', 'Ali', ''], dtype=object)
array(['Rashid', 'Mohammad', ''], dtype=object)
array(['Ranjbarzadeh', 'Shayan', ''], dtype=object)
array(['Tefagh', 'Mojtaba', ''], dtype=object)] |
495 | 1304.7384 | Stefano Biagi Doc | Stefano Biagi | On M. M\'erigot's theorem on the convergence domain of the
Campbell-Baker-Hausdorff-Dynkin series | null | null | null | null | math.CA math.AP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The aim of this manuscript is to present the proof given by Michel M\'erigot
in 1974 for an enlarged convergence domain of the
Campbell-Baker-Hausdorff-Dynkin series in the Lie algebra of a Banach-Lie
group. This proof is based on a theorem, of independent interest, on the
lifetime of the solution of a Cauchy problem. We furnish all the details for
this ODE result in Appendix A.
| [{'version': 'v1', 'created': 'Sat, 27 Apr 2013 16:08:57 GMT'}] | 2013-04-30 | [array(['Biagi', 'Stefano', ''], dtype=object)] |
496 | 1208.3171 | Grey Ercole Ph. D. | Hamilton Bueno and Grey Ercole | A quasilinear problem with fast growing gradient | null | Applied Mathematics Letters 26 (2013) 520-523 | 10.1016/j.aml.2012.12.009 | null | math.AP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we consider the following Dirichlet problem for the
$p$-Laplacian in the positive parameters $\lambda$ and $\beta$: [{{array}
[c]{rcll}% -\Delta_{p}u & = & \lambda h(x,u)+\beta f(x,u,\nabla u) &
\text{in}\Omega u & = & 0 & \text{on}\partial\Omega, {array}. \hfill] where
$h,f$ are continuous nonlinearities satisfying $0\leq\omega_{1}(x)u^{q-1}\leq
h(x,u)\leq\omega_{2}(x)u^{q-1}$ with $1<q<p$ and $0\leq
f(x,u,v)\leq\omega_{3}(x)u^{a}|v|^{b}$, with $a,b>0$, and $\Omega$ is a bounded
domain of $\mathbb{R}^{N},$ $N\geq3.$ The functions $\omega_{i}$, $1\leq
i\leq3$, are nonnegative, continuous weights in $\bar{\Omega}$. We prove that
there exists a region $\mathcal{D}$ in the $\lambda\beta$-plane where the
Dirichlet problem has at least one positive solution. The novelty in this paper
is that our result is valid for nonlinearities with growth higher than $p$ in
the gradient variable.
| [{'version': 'v1', 'created': 'Wed, 15 Aug 2012 18:27:59 GMT'}
{'version': 'v2', 'created': 'Sun, 21 Oct 2012 02:17:56 GMT'}] | 2013-03-28 | [array(['Bueno', 'Hamilton', ''], dtype=object)
array(['Ercole', 'Grey', ''], dtype=object)] |
497 | 1805.01167 | Qiangpeng Yang | Qiangpeng Yang, Mengli Cheng, Wenmeng Zhou, Yan Chen, Minghui Qiu, Wei
Lin, Wei Chu | IncepText: A New Inception-Text Module with Deformable PSROI Pooling for
Multi-Oriented Scene Text Detection | Accepted by IJCAI 2018 | null | null | null | cs.CV | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Incidental scene text detection, especially for multi-oriented text regions,
is one of the most challenging tasks in many computer vision applications.
Different from the common object detection task, scene text often suffers from
a large variance of aspect ratio, scale, and orientation. To solve this
problem, we propose a novel end-to-end scene text detector IncepText from an
instance-aware segmentation perspective. We design a novel Inception-Text
module and introduce deformable PSROI pooling to deal with multi-oriented text
detection. Extensive experiments on ICDAR2015, RCTW-17, and MSRA-TD500 datasets
demonstrate our method's superiority in terms of both effectiveness and
efficiency. Our proposed method achieves 1st place result on ICDAR2015
challenge and the state-of-the-art performance on other datasets. Moreover, we
have released our implementation as an OCR product which is available for
public access.
| [{'version': 'v1', 'created': 'Thu, 3 May 2018 08:37:28 GMT'}
{'version': 'v2', 'created': 'Tue, 8 May 2018 03:01:23 GMT'}] | 2018-05-09 | [array(['Yang', 'Qiangpeng', ''], dtype=object)
array(['Cheng', 'Mengli', ''], dtype=object)
array(['Zhou', 'Wenmeng', ''], dtype=object)
array(['Chen', 'Yan', ''], dtype=object)
array(['Qiu', 'Minghui', ''], dtype=object)
array(['Lin', 'Wei', ''], dtype=object)
array(['Chu', 'Wei', ''], dtype=object)] |
498 | 1909.06390 | Rostom Mbarek | Rostom Mbarek, Damiano Caprioli | Espresso Acceleration of Ultra-High-Energy Cosmic Rays up to the Hillas
Limit in Relativistic MHD Jets | 36th International Cosmic Ray Conference (ICRC2019), held July
24th-August 1st, 2019 in Madison, WI, U.S.A. Online at
https://pos.sissa.it/cgi-bin/reader/conf.cgi?confid=358, id.348 | null | null | null | astro-ph.HE | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Espresso is a novel acceleration model for Ultra-High-Energy Cosmic Rays
(UHECRs), where lower-energy CRs produced in supernova remnants experience a
one-shot reacceleration in the relativistic jets of powerful Active Galactic
Nuclei (AGNs) to reach energies up to $10^{20}$ eV. To test the espresso
framework, we follow UHECR acceleration bottom-up from injection to the highest
energies by propagating 100,000 particles in realistic 3D magneto-hydrodynamic
(MHD) simulations of ultra-relativistic jets. We find that simulations agree
well with analytical expectations in terms of trajectories of individual
particles. We also quantify that $\sim 10\%$ of CR seeds gain a factor of
$\sim\Gamma^2$ in energy, where $\Gamma$ is the jet's effective Lorentz factor;
moreover, about $0.1\%$ of the particles undergo two or more shots to achieve
gains in excess of $\Gamma^2$. Particles are generally accelerated up to the
jet's Hillas limit, indicating that the espresso mechanism should boost
galactic CRs to UHECRs in typical AGN jets. Finally, we discuss how espresso
acceleration in AGN jets is consistent with UHECR spectra and chemical
composition, and also with the UHECR arrival directions measured by Auger and
Telescope Array.
| [{'version': 'v1', 'created': 'Fri, 13 Sep 2019 18:02:51 GMT'}] | 2019-09-17 | [array(['Mbarek', 'Rostom', ''], dtype=object)
array(['Caprioli', 'Damiano', ''], dtype=object)] |
499 | 1508.03685 | Masaaki Umehara | Naoya Ando, Toshifumi Fujiyama and Masaaki Umehara | C^1-umbilics with arbitrarily high indices | null | Pacific J. Math. 288 (2017) 1-26 | 10.2140/pjm.2017.288.1 | null | math.DG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, the existence of C^1-umbilics with arbitrarily high indices is
shown. This implies that more than C^1-regularity is required to prove
Loewner's conjecture.
| [{'version': 'v1', 'created': 'Sat, 15 Aug 2015 01:18:44 GMT'}] | 2017-04-19 | [array(['Ando', 'Naoya', ''], dtype=object)
array(['Fujiyama', 'Toshifumi', ''], dtype=object)
array(['Umehara', 'Masaaki', ''], dtype=object)] |