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19,700 | 2111.07542 | Marius Hofert | Erik Hintz, Marius Hofert, Christiane Lemieux, Yoshihiro Taniguchi | Single-Index Importance Sampling with Stratification | null | null | null | null | stat.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In many stochastic problems, the output of interest depends on an input
random vector mainly through a single random variable (or index) via an
appropriate univariate transformation of the input. We exploit this feature by
proposing an importance sampling method that makes rare events more likely by
changing the distribution of the chosen index. Further variance reduction is
guaranteed by combining this single-index importance sampling approach with
stratified sampling. The dimension-reduction effect of single-index importance
sampling also enhances the effectiveness of quasi-Monte Carlo methods. The
proposed method applies to a wide range of financial or risk management
problems. We demonstrate its efficiency for estimating large loss probabilities
of a credit portfolio under a normal and t-copula model and show that our
method outperforms the current standard for these problems.
| [{'version': 'v1', 'created': 'Mon, 15 Nov 2021 05:28:34 GMT'}] | 2021-11-16 | [array(['Hintz', 'Erik', ''], dtype=object)
array(['Hofert', 'Marius', ''], dtype=object)
array(['Lemieux', 'Christiane', ''], dtype=object)
array(['Taniguchi', 'Yoshihiro', ''], dtype=object)] |
19,701 | 1704.04670 | Vladimir V. Sergeichuk | Andrii Dmytryshyn, Vyacheslav Futorny, Tetiana Klymchuk, Vladimir V.
Sergeichuk | Generalization of Roth's solvability criteria to systems of matrix
equations | 11 pages | Linear Algebra Appl. 527 (2017) 294-302 | 10.1016/j.laa.2017.04.011 | null | math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | W.E. Roth (1952) proved that the matrix equation $AX-XB=C$ has a solution if
and only if the matrices $\left[\begin{matrix}A&C\\0&B\end{matrix}\right]$ and
$\left[\begin{matrix}A&0\\0&B\end{matrix}\right]$ are similar. A. Dmytryshyn
and B. K{\aa}gstr\"om (2015) extended Roth's criterion to systems of matrix
equations $A_iX_{i'}M_i-N_iX_{i''}^{\sigma_i} B_i=C_i$ $(i=1,\dots,s)$ with
unknown matrices $X_1,\dots,X_t$, in which every $X^{\sigma}$ is $X$, $X^T$, or
$X^*$. We extend their criterion to systems of complex matrix equations that
include the complex conjugation of unknown matrices. We also prove an analogous
criterion for systems of quaternion matrix equations.
| [{'version': 'v1', 'created': 'Sat, 15 Apr 2017 18:02:20 GMT'}] | 2017-04-18 | [array(['Dmytryshyn', 'Andrii', ''], dtype=object)
array(['Futorny', 'Vyacheslav', ''], dtype=object)
array(['Klymchuk', 'Tetiana', ''], dtype=object)
array(['Sergeichuk', 'Vladimir V.', ''], dtype=object)] |
19,702 | 2105.02745 | Ingve Simonsen | Ver\'onica P. Simonsen, Dick Bedeaux, and Ingve Simonsen | Non-parametric reconstruction of the statistical properties of
penetrable, isotropic randomly rough surfaces from in-plane, co-polarized
light scattering data: Application to computer generated and experimental
scattering data | 23 pages, 9 figures | Phys. Rev. A 104, 043502 (2021) | 10.1103/PhysRevA.104.043502 | null | physics.optics physics.app-ph physics.class-ph | http://creativecommons.org/licenses/by/4.0/ | An approach is introduced for the non-parametric reconstruction of the
statistical properties of penetrable, isotropic randomly rough surfaces from
in-plane, co-polarized light scattering data. Starting from expressions within
the Kirchhoff approximation for the light scattered diffusely by a
two-dimensional randomly rough surface, an analytic expression for the
normalized surface height correlation function is obtained as an integral over
the in-plane and co-polarized scattering data with the introduction of only a
couple of additional approximations. The inversion approach consists of two
main steps. In the first step the surface roughness is estimated. Next, this
value is used to obtain the functional form of the surface height correlation
function without initially assuming any particular form for this function
(non-parametric inversion). The input data used in validating this inversion
approach consist of in-plane and co-polarized scattering data obtained for
different forms of the correlation function by either computer simulations or
by experiments for two-dimensional randomly rough dielectric or metallic
surfaces. Good agreement was obtained between the correlation function and
surface roughness obtained during the reconstruction and the corresponding
quantities assumed when generating the input scattering data; this was the case
for both dielectric and metallic surfaces, for both p- and s-polarized light,
and for different polar angles of incidence. The proposed inversion approach
provides an accurate, efficient, robust and contact-less method based on
in-plane and co-polarized scattering data for the non-parametric
characterization of the statistical properties of isotropic two-dimensional
randomly rough dielectric and metallic surface.
| [{'version': 'v1', 'created': 'Thu, 6 May 2021 15:14:22 GMT'}] | 2021-10-13 | [array(['Simonsen', 'Verónica P.', ''], dtype=object)
array(['Bedeaux', 'Dick', ''], dtype=object)
array(['Simonsen', 'Ingve', ''], dtype=object)] |
19,703 | 1401.4531 | Esa Vasili Vesalainen | Esa V. Vesalainen | Rellich Type Theorems for Unbounded Domains | null | Inverse Problems and Imaging, 8 (2014), 865--883 | 10.3934/ipi.2014.8.865 | null | math.AP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We give several generalizations of Rellich's classical uniqueness theorem to
unbounded domains. We give a natural half-space generalization for
super-exponentially decaying inhomogeneities using real variable techniques. We
also prove under super-exponential decay a discrete generalization where the
inhomogeneity only needs to vanish in a suitable cone.
The more traditional complex variable techniques are used to prove the
half-space result again, but with less exponential decay, and a variant with
polynomial decay, but with supports exponentially thin at infinity. As an
application, we prove the discreteness of non-scattering energies for
non-compactly supported potentials with suitable asymptotic behaviours and
supports.
| [{'version': 'v1', 'created': 'Sat, 18 Jan 2014 11:25:17 GMT'}] | 2014-09-02 | [array(['Vesalainen', 'Esa V.', ''], dtype=object)] |
19,704 | 1708.02371 | Alper Atamturk | Alper Atamturk, Carlos Deck and Hyemin Jeon | Successive Quadratic Upper-Bounding for Discrete Mean-Risk Minimization
and Network Interdiction | null | null | null | BCOL Research Report 17.05, IEOR, UC Berkeley | math.OC | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The advances in conic optimization have led to its increased utilization for
modeling data uncertainty. In particular, conic mean-risk optimization gained
prominence in probabilistic and robust optimization. Whereas the corresponding
conic models are solved efficiently over convex sets, their discrete
counterparts are intractable. In this paper, we give a highly effective
successive quadratic upper-bounding procedure for discrete mean-risk
minimization problems. The procedure is based on a reformulation of the
mean-risk problem through the perspective of its convex quadratic term.
Computational experiments conducted on the network interdiction problem with
stochastic capacities show that the proposed approach yields solutions within
1-2% of optimality in a small fraction of the time required by exact search
algorithms. We demonstrate the value of the proposed approach for constructing
efficient frontiers of flow-at-risk vs. interdiction cost for varying
confidence levels.
| [{'version': 'v1', 'created': 'Tue, 8 Aug 2017 04:54:37 GMT'}
{'version': 'v2', 'created': 'Sat, 25 Aug 2018 18:37:15 GMT'}] | 2018-08-28 | [array(['Atamturk', 'Alper', ''], dtype=object)
array(['Deck', 'Carlos', ''], dtype=object)
array(['Jeon', 'Hyemin', ''], dtype=object)] |
19,705 | 2211.04869 | Andrew Bragg | Yan Zhang, Guiquan Wang, Andrew D Bragg | Asymptotic closure model for inertial particle transport in turbulent
boundary layers | null | null | null | null | physics.flu-dyn | http://creativecommons.org/licenses/by/4.0/ | Transport equations for heavy inertial particles in turbulent boundary layers
may be derived from an underlying phase-space probability density function
(PDF) equation. These equations, however, are unclosed, and the standard
closure approach is to use a quasi-Normal approximation (QNA) in which the
fourth moments are approximated as behaving as if the velocities were Normally
distributed. Except for particles with weak inertia, the QNA leads to large
quantitative errors, and is not consistent with the known asymptotic
predictions of Sikovsky (Flow Turbulence Combust, vol. 92, 2014, pp. 41-64) for
the moments of the PDF in the viscous sublayer. We derive a new closure
approximation based on an asymptotic solution to the transport equations in
regions where the effect of particle inertia is significant. The new closure is
consistent with the asymptotic predictions of Sikovsky, but applies even
outside the viscous sublayer. Comparisons with direct numerical simulations
(DNS) show that the new closure gives similar results to the QNA (with the QNA
results in slightly better agreement with the DNS) when the viscous Stokes
number is $St<10$, but for $St>10$ the new model is in far better agreement
with the DNS than the QNA. While the predictions from the new model leave room
for improvement, the results suggest that this new closure strategy is a very
effective alternative to the traditional QNA approach, and the closure could be
refined in future work.
| [{'version': 'v1', 'created': 'Wed, 9 Nov 2022 13:24:47 GMT'}] | 2022-11-10 | [array(['Zhang', 'Yan', ''], dtype=object)
array(['Wang', 'Guiquan', ''], dtype=object)
array(['Bragg', 'Andrew D', ''], dtype=object)] |
19,706 | 2209.10043 | Michael Yao | Michael S. Yao, Allison Chae, Matthew T. MacLean, Anurag Verma,
Jeffrey Duda, James Gee, Drew A. Torigian, Daniel Rader, Charles Kahn, Walter
R. Witschey, Hersh Sagreiya | Learning-Based Radiomic Prediction of Type 2 Diabetes Mellitus Using
Image-Derived Phenotypes | 9 pages | null | null | null | cs.LG cs.AI eess.IV q-bio.QM | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Early diagnosis of Type 2 Diabetes Mellitus (T2DM) is crucial to enable
timely therapeutic interventions and lifestyle modifications. As medical
imaging data become more widely available for many patient populations, we
sought to investigate whether image-derived phenotypic data could be leveraged
in tabular learning classifier models to predict T2DM incidence without the use
of invasive blood lab measurements. We show that both neural network and
decision tree models that use image-derived phenotypes can predict patient T2DM
status with recall scores as high as 87.6%. We also propose the novel use of
these same architectures as 'SynthA1c encoders' that are able to output
interpretable values mimicking blood hemoglobin A1C empirical lab measurements.
Finally, we demonstrate that T2DM risk prediction model sensitivity to small
perturbations in input vector components can be used to predict performance on
covariates sampled from previously unseen patient populations.
| [{'version': 'v1', 'created': 'Tue, 20 Sep 2022 23:39:52 GMT'}] | 2022-09-22 | [array(['Yao', 'Michael S.', ''], dtype=object)
array(['Chae', 'Allison', ''], dtype=object)
array(['MacLean', 'Matthew T.', ''], dtype=object)
array(['Verma', 'Anurag', ''], dtype=object)
array(['Duda', 'Jeffrey', ''], dtype=object)
array(['Gee', 'James', ''], dtype=object)
array(['Torigian', 'Drew A.', ''], dtype=object)
array(['Rader', 'Daniel', ''], dtype=object)
array(['Kahn', 'Charles', ''], dtype=object)
array(['Witschey', 'Walter R.', ''], dtype=object)
array(['Sagreiya', 'Hersh', ''], dtype=object)] |
19,707 | 1202.2001 | Marcoen Cabbolet | Marcoen J.T.F. Cabbolet, Harrie C.M. de Swart | Set Matrix Theory as a Physically Motivated Generalization of
Zermelo-Fraenkel Set Theory | 16 pages; based on the third chapter (pp. 23-52) of the first
author's dissertation, entitled "Elementary Process Theory: axiomatic
introduction and applications" (Vrije Universiteit Brussel, 2011) | Logique et Analyse 225, 59-82 (2014) | null | null | math.LO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recently, the Elementary Process Theory (EPT) has been developed as a set of
fundamental principles that might underlie a gravitational repulsion of matter
and antimatter. This paper presents set matrix theory (SMT) as the foundation
of the mathematical-logical framework in which the EPT has been formalized:
Zermelo-Fraenkel set theory (ZF), namely, cannot be used as such. SMT is a
generalization of ZF: whereas ZF uses only sets as primitive objects, in the
framework of SMT finite matrices with set-valued entries are objects sui
generis, with a one-by-one set matrix [x] being identical to the set x. It is
proved that every set that can be constructed in ZF can also be constructed in
SMT: as a mathematical foundation, SMT is thus not weaker than ZF. In addition,
it is shown that SMT is more suitable han ZF for the intended application to
physics. The conclusion is that SMT, contrary to ZF, is acceptable as the
mathematical-logical foundation of the framework for physics that is determined
by the EPT.
| [{'version': 'v1', 'created': 'Thu, 9 Feb 2012 14:41:31 GMT'}
{'version': 'v2', 'created': 'Wed, 30 Jan 2013 21:57:15 GMT'}] | 2014-01-16 | [array(['Cabbolet', 'Marcoen J. T. F.', ''], dtype=object)
array(['de Swart', 'Harrie C. M.', ''], dtype=object)] |
19,708 | 1309.3680 | Robert Penna | Robert F. Penna, Akshay Kulkarni, Ramesh Narayan | A new equilibrium torus solution and GRMHD initial conditions | 8 pages, 4 figures, A&A accepted | null | 10.1051/0004-6361/201219666 | null | astro-ph.HE | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | General relativistic magnetohydrodynamic (GRMHD) simulations are providing
influential models for black hole spin measurements, gamma ray bursts, and
supermassive black hole feedback. Many of these simulations use the same
initial condition: a rotating torus of fluid in hydrostatic equilibrium. A
persistent concern is that simulation results sometimes depend on arbitrary
features of the initial torus. For example, the Bernoulli parameter (which is
related to outflows), appears to be controlled by the Bernoulli parameter of
the initial torus. In this paper, we give a new equilibrium torus solution and
describe two applications for the future. First, it can be used as a more
physical initial condition for GRMHD simulations than earlier torus solutions.
Second, it can be used in conjunction with earlier torus solutions to isolate
the simulation results that depend on initial conditions. We assume
axisymmetry, an ideal gas equation of state, constant entropy, and ignore
self-gravity. We fix an angular momentum distribution and solve the
relativistic Euler equations in the Kerr metric. The Bernoulli parameter,
rotation rate, and geometrical thickness of the torus can be adjusted
independently. Our torus tends to be more bound and have a larger radial extent
than earlier torus solutions. While this paper was in preparation, several
GRMHD simulations appeared based on our equilibrium torus. We believe it will
continue to provide a more realistic starting point for future simulations.
| [{'version': 'v1', 'created': 'Sat, 14 Sep 2013 15:29:55 GMT'}] | 2015-06-17 | [array(['Penna', 'Robert F.', ''], dtype=object)
array(['Kulkarni', 'Akshay', ''], dtype=object)
array(['Narayan', 'Ramesh', ''], dtype=object)] |
19,709 | 1304.1941 | Manabu Machida | Manabu Machida | Singular eigenfunctions for the three-dimensional radiative transport
equation | null | null | 10.1364/JOSAA.31.000067 | null | math-ph math.MP physics.optics | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Case's method obtains solutions to the radiative transport equation as
superpositions of elementary solutions when the specific intensity depends on
one spatial variable. In this paper, we find elementary solutions when the
specific intensity depends on three spatial variables in three-dimensional
space. By using the reference frame whose z-axis lies in the direction of the
wave vector, the angular part of each elementary solution becomes the singular
eigenfunction for the one-dimensional radiative transport equation. Thus Case's
method is generalized.
| [{'version': 'v1', 'created': 'Sat, 6 Apr 2013 22:18:04 GMT'}
{'version': 'v2', 'created': 'Sat, 7 Sep 2013 15:06:52 GMT'}] | 2015-06-15 | [array(['Machida', 'Manabu', ''], dtype=object)] |
19,710 | 2001.01713 | Chaim Even-Zohar | Chaim Even-Zohar, Michael Farber | Random Surfaces with Boundary | null | Discrete & Computational Geometry, online, 2021 | 10.1007/s00454-021-00301-8 | null | math.CO math.GT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A surface with boundary is randomly generated by gluing polygons along some
of their sides. We show that its genus and number of boundary components
asymptotically follow a bivariate normal distribution.
| [{'version': 'v1', 'created': 'Mon, 6 Jan 2020 18:56:06 GMT'}
{'version': 'v2', 'created': 'Fri, 5 Mar 2021 14:26:25 GMT'}] | 2021-04-21 | [array(['Even-Zohar', 'Chaim', ''], dtype=object)
array(['Farber', 'Michael', ''], dtype=object)] |
19,711 | 2112.12075 | Mahouton Norbert Hounkonnou | Jian Cao, Sama Arjika and Mahouton Norbert Hounkonnou | Generalized q-difference equations for general q-polynomials with double
q-binomial coefficients | null | null | null | null | math.CO | http://creativecommons.org/licenses/by/4.0/ | In this paper, we use the generalized q-polynomials with double q-binomial
coefficients and homogeneous q-operators [J. Difference Equ. Appl. 20 (2014),
837--851.] to construct q-difference equations with seven variables, which
generalize recent works of Jia et al [Symmetry 2021, 13, 1222.]. In addition,
we derive Rogers formulas, extended Rogers formulas and Srivastava--Agarwal
type bilinear generating functions for generalized q-polynomials, which
generalize generating functions for Cigler's polynomials [J. Difference Equ.
Appl. 24 (2018), 479--502.]. Finally, we also derive mixed generating functions
using q-difference equations.
| [{'version': 'v1', 'created': 'Fri, 17 Dec 2021 19:52:28 GMT'}] | 2021-12-23 | [array(['Cao', 'Jian', ''], dtype=object)
array(['Arjika', 'Sama', ''], dtype=object)
array(['Hounkonnou', 'Mahouton Norbert', ''], dtype=object)] |
19,712 | 1707.02787 | Myoung-Sun Heo | Geol Moon, Myoung-Sun Heo, Yonghee Kim, Heung-Ryoul Noh, Wonho Jhe | Nonlinear, Nonequilibrium and Collective Dynamics in a Periodically
Modulated Cold Atom System | 57 pages, 25 figures | null | 10.1016/j.physrep.2017.07.002 | null | physics.atom-ph cond-mat.quant-gas cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The physics of critical phenomena in a many-body system far from thermal
equilibrium is an interesting and important issue to be addressed both
experimentally and theoretically. The trapped cold atoms have been actively
used as a clean and versatile simulator for classical and quantum-mechanical
systems, deepening understanding of the many-body physics behind. Here we
review the nonlinear and collective dynamics in a periodically modulated
magneto-optically trapped cold atoms. By temporally modulating the intensity of
the trapping lasers with the controlled phases, one can realize two kinds of
nonlinear oscillators, the parametrically driven oscillator and the resonantly
driven Duffing oscillator, which exhibit the dynamical bistable states. Cold
atoms behave not only as the single-particle nonlinear oscillators, but also as
the coupled oscillators by the light-induced inter-atomic interaction, which
leads to the phase transitions far from equilibrium in a way similar to the
phase transition in equilibrium. The parametrically driven cold atoms show the
ideal mean-field symmetry-breaking transition, and the symmetry is broken with
respect to time translation by the modulation period. Such a phase transition
results from the cooperation and competition between the inter-particle
interaction and the fluctuations, which lead to the nonlinear switching of
atoms between the vibrational states, and the experimentally measured critical
characteristics prove it as the ideal mean-field transition class. On the other
hand, the resonantly driven cold atoms that possess the coexisting periodic
attractors exhibit the kinetic phase transition analogous to the discontinuous
gas-liquid phase transition in equilibrium, and interestingly the global
interaction between atoms causes the shift of the phase-transition boundary.
| [{'version': 'v1', 'created': 'Mon, 10 Jul 2017 10:22:57 GMT'}] | 2017-09-13 | [array(['Moon', 'Geol', ''], dtype=object)
array(['Heo', 'Myoung-Sun', ''], dtype=object)
array(['Kim', 'Yonghee', ''], dtype=object)
array(['Noh', 'Heung-Ryoul', ''], dtype=object)
array(['Jhe', 'Wonho', ''], dtype=object)] |
19,713 | 2101.02504 | Stephen DiAdamo | Stephen DiAdamo, Marco Ghibaudi, James Cruise | Distributed Quantum Computing and Network Control for Accelerated VQE | This work has been submitted to the IEEE for possible publication.
Copyright may be transferred without notice, after which this version may no
longer be accessible | IEEE Transactions on Quantum Engineering 2021 | 10.1109/TQE.2021.3057908 | null | quant-ph cs.SY eess.SY | http://creativecommons.org/licenses/by/4.0/ | Interconnecting small quantum computers will be essential in the future for
creating large scale, robust quantum computers. Methods for distributing
monolithic quantum algorithms efficiently are thus needed. In this work we
consider an approach for distributing the accelerated variational quantum
eigensolver (AVQE) algorithm over arbitrary sized - in terms of number of
qubits - distributed quantum computers. We consider approaches for distributing
qubit assignments of the Ansatz states required to estimate the expectation
value of Hamiltonian operators in quantum chemistry in a parallelized
computation and provide a systematic approach to generate distributed quantum
circuits for distributed quantum computing. Moreover, we propose an
architecture for a distributed quantum control system in the settings of
centralized and decentralized network control.
| [{'version': 'v1', 'created': 'Thu, 7 Jan 2021 11:50:24 GMT'}] | 2021-03-22 | [array(['DiAdamo', 'Stephen', ''], dtype=object)
array(['Ghibaudi', 'Marco', ''], dtype=object)
array(['Cruise', 'James', ''], dtype=object)] |
19,714 | 2007.11849 | Chen-Yu Wei | Chen-Yu Wei, Mehdi Jafarnia-Jahromi, Haipeng Luo, Rahul Jain | Learning Infinite-horizon Average-reward MDPs with Linear Function
Approximation | null | null | null | null | cs.LG stat.ML | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop several new algorithms for learning Markov Decision Processes in
an infinite-horizon average-reward setting with linear function approximation.
Using the optimism principle and assuming that the MDP has a linear structure,
we first propose a computationally inefficient algorithm with optimal
$\widetilde{O}(\sqrt{T})$ regret and another computationally efficient variant
with $\widetilde{O}(T^{3/4})$ regret, where $T$ is the number of interactions.
Next, taking inspiration from adversarial linear bandits, we develop yet
another efficient algorithm with $\widetilde{O}(\sqrt{T})$ regret under a
different set of assumptions, improving the best existing result by Hao et al.
(2020) with $\widetilde{O}(T^{2/3})$ regret. Moreover, we draw a connection
between this algorithm and the Natural Policy Gradient algorithm proposed by
Kakade (2002), and show that our analysis improves the sample complexity bound
recently given by Agarwal et al. (2020).
| [{'version': 'v1', 'created': 'Thu, 23 Jul 2020 08:23:44 GMT'}
{'version': 'v2', 'created': 'Mon, 26 Apr 2021 09:12:03 GMT'}] | 2021-04-27 | [array(['Wei', 'Chen-Yu', ''], dtype=object)
array(['Jafarnia-Jahromi', 'Mehdi', ''], dtype=object)
array(['Luo', 'Haipeng', ''], dtype=object)
array(['Jain', 'Rahul', ''], dtype=object)] |
19,715 | 1511.02861 | Megan Shabram | Megan Shabram, Brice-Olivier Demory, Jessi Cisewski, Eric B. Ford,
Leslie Rogers | The Eccentricity Distribution of Short-Period Planet Candidates Detected
by Kepler in Occultation | Accepted for publication in ApJ | null | 10.3847/0004-637X/820/2/93 | null | astro-ph.EP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We characterize the eccentricity distribution of a sample of ~50 short-period
planet candidates using transit and occultation measurements from NASA's Kepler
Mission. First, we evaluate the sensitivity of our hierarchical Bayesian
modeling and test its robustness to model misspecification using simulated
data. When analyzing actual data assuming a Rayleigh distribution for
eccentricity, we find that the posterior mode for the dispersion parameter is
$\sigma=0.081 \pm^{0.014}_{0.003}$. We find that a two-component Gaussian
mixture model for $e \cos \omega$ and $e \sin \omega$ provides a better model
than either a Rayleigh or Beta distribution. Based on our favored model, we
find that $\sim90\%$ of planet candidates in our sample come from a population
with an eccentricity distribution characterized by a small dispersion
($\sim0.01$), and $\sim10\%$ come from a population with a larger dispersion
($\sim0.22$). Finally, we investigate how the eccentricity distribution
correlates with selected planet and host star parameters. We find evidence that
suggests systems around higher metallicity stars and planet candidates with
smaller radii come from a more complex eccentricity distribution.
| [{'version': 'v1', 'created': 'Mon, 9 Nov 2015 21:00:02 GMT'}] | 2016-04-06 | [array(['Shabram', 'Megan', ''], dtype=object)
array(['Demory', 'Brice-Olivier', ''], dtype=object)
array(['Cisewski', 'Jessi', ''], dtype=object)
array(['Ford', 'Eric B.', ''], dtype=object)
array(['Rogers', 'Leslie', ''], dtype=object)] |
19,716 | 2105.10314 | Jean-Philip Piquemal | Christophe Gourlaouen and Jean-Philip Piquemal | On the Quantum Chemical Nature of Lead(II) "Lone Pair" | null | Molecules, 2022, 27(1), 27 | 10.3390/molecules27010027 | null | physics.chem-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss the quantum chemical nature of the Lead(II) valence basins,
sometime called the Lead "lone pair". Using various chemical interpretation
tools such as the molecular orbital analysis, Natural Bond Orbitals (NBO),
Natural Population Analysis (NPA) and Electron Localization Function (ELF)
topological analysis, we study a variety of Lead(II) complexes. A careful
analysis of the results show that the optimal structures of the lead complexes
are only govern by the 6s and 6p subshells whereas no involvement of the 5d
orbitals is found. Similarly, we do not find any significant contribution of
the 6d. Therefore, the Pb(II) complexation with its ligand can be explained
through the interaction of the 6s2 electrons and the accepting 6p orbitals. We
detail the potential structural and dynamical consequences of such electronic
structure organization of the Pb (II) valence domain.
| [{'version': 'v1', 'created': 'Fri, 21 May 2021 12:39:31 GMT'}
{'version': 'v2', 'created': 'Thu, 2 Dec 2021 10:47:33 GMT'}
{'version': 'v3', 'created': 'Thu, 16 Dec 2021 11:02:21 GMT'}] | 2021-12-23 | [array(['Gourlaouen', 'Christophe', ''], dtype=object)
array(['Piquemal', 'Jean-Philip', ''], dtype=object)] |
19,717 | 2107.06736 | Simone Dovetta | Simone Dovetta, Elio Marconi, Laura V. Spinolo | New regularity results for scalar conservation laws, and applications to
a source-destination model for traffic flows on networks | 28 pages, 2 figures | null | null | null | math.AP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We focus on entropy admissible solutions of scalar conservation laws in one
space dimension and establish new regularity results with respect to time.
First, we assume that the flux function $f$ is strictly convex and show that,
for every $ x \in \mathbb{R}$, the total variation of the composite function $f
\circ u(\cdot, x)$ is controlled by the total variation of the initial datum.
Next, we assume that $f$ is monotone and, under no convexity assumption, we
show that, for every $x$, the total variation of the left and right trace
$u(\cdot, x^\pm)$ is controlled by the total variation of the initial datum. We
also exhibit a counter-example showing that in the first result the total
variation bound does not extend to the function $u$, or equivalently that in
the second result we cannot drop the monotonicity assumption. We then discuss
applications to a source-destination model for traffic flows on road networks.
We introduce a new approach, based on the analysis of transport equations with
irregular coefficients, and, under the assumption that the network only
contains so-called T-junctions, we establish existence and uniqueness results
for merely bounded data in the class of solutions where the traffic is not
congested. Our assumptions on the network and the traffic congestion are
basically necessary to obtain well-posedness in view of a counter-example due
to Bressan and Yu. We also establish stability and propagation of $BV$
regularity, and this is again interesting in view of recent counter-examples.
| [{'version': 'v1', 'created': 'Wed, 14 Jul 2021 14:28:56 GMT'}] | 2021-07-15 | [array(['Dovetta', 'Simone', ''], dtype=object)
array(['Marconi', 'Elio', ''], dtype=object)
array(['Spinolo', 'Laura V.', ''], dtype=object)] |
19,718 | hep-ph/0408327 | Wei Zhu | Wei Zhu, Zhenqi Shen, Jifeng Yang and Jianhong Ruan | A unity of QCD evolution dynamics at small $x$ region | 43 pages, 21 figures, profoundly revised | null | null | null | hep-ph | null | The DGLAP, BFKL, modified DGLAP and modified BFKL equations are constructed
in a unified partonic framework. The antishadowing effect in the recombination
process is emphasized, which leads to two different small $x$ behaviors of
gluon distribution. In the meantime, the BFKL equation and modified DGLAP
equation are viewed as the corrections of the initial gluon correlations to the
evolution dynamics at twist-2 and twist-4, respectively. A partonic explanation
of Regge theory for the BFKL dynamics and the relation of the BFKL dynamics
with the helicity configuration of the initial gluons are presented.
| [{'version': 'v1', 'created': 'Mon, 30 Aug 2004 01:54:09 GMT'}
{'version': 'v2', 'created': 'Sun, 1 Jan 2006 07:13:14 GMT'}] | 2007-05-23 | [array(['Zhu', 'Wei', ''], dtype=object)
array(['Shen', 'Zhenqi', ''], dtype=object)
array(['Yang', 'Jifeng', ''], dtype=object)
array(['Ruan', 'Jianhong', ''], dtype=object)] |
19,719 | astro-ph/0010174 | Sandy Leggett | S. K. Leggett, F. Allard, T. R. Geballe, P. H. Hauschildt, A.
Schweitzer | Infrared Spectra and Spectral Energy Distributions of Late-M- and
L-Dwarfs | 31 pages incl. 5 Tables and 12 Figures, accepted by ApJ for Feb 2001
issue | null | 10.1086/319020 | null | astro-ph | null | We have obtained 1.0-2.5um spectra at R~600 of 14 disk dwarfs with spectral
types M6 to L7. For four of the dwarfs we have also obtained infrared spectra
at R~3000 in narrow intervals. In addition, we present new L' photometry for
four of the dwarfs in the sample, which allows improved determinations of their
bolometric luminosities. We resolve the L-dwarf Denis-P J 0205-1159 into an
identical pair of objects separated by 0.35". The spectra, with the published
energy distribution for one other dwarf, are compared to synthetic spectra
generated by upgraded model atmospheres. Good matches are found for 2200> Teff
K>1900 (spectral types around M9 to L3), but discrepancies exist at Teff> 2300
K (M8) and for Teff<1800 K (L4-L7). At the higher temperatures the mismatches
are due to incompleteness in the water vapor linelist. At the lower
temperatures the disagreement is probably due to our treatment of dust: we
assume a photospheric distribution in equilibrium with the gas phase. We derive
effective temperatures for the sample from the comparison with synthetic
spectra and also by comparing our observed total intrinsic luminosities to
structural model calculations (which are mostly independent of the atmosphere
but are dependent on the unknown masses and ages of the targets). The two
derivations agree to ~200 K except for the faintest object in the sample where
the discrepancy is larger. Agreement with other temperature determinations is
also ~200 K, except for the L7 dwarf.
| [{'version': 'v1', 'created': 'Tue, 10 Oct 2000 01:25:16 GMT'}] | 2009-10-31 | [array(['Leggett', 'S. K.', ''], dtype=object)
array(['Allard', 'F.', ''], dtype=object)
array(['Geballe', 'T. R.', ''], dtype=object)
array(['Hauschildt', 'P. H.', ''], dtype=object)
array(['Schweitzer', 'A.', ''], dtype=object)] |
19,720 | 1712.08820 | Tomohiro Nakama | Tomohiro Nakama, Teruaki Suyama, Kazunori Kohri and Nagisa Hiroshima | Constraints on small-scale primordial power by annihilation signals from
extragalactic dark matter minihalos | 11 pages, 7 figures | Phys. Rev. D 97, 023539 (2018) | 10.1103/PhysRevD.97.023539 | KEK-Cosmo-219, KEK-TH-2026 | astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We revisit constraints on small-scale primordial power from annihilation
signals from dark matter minihalos. Using gamma rays and neutrinos from
extragalactic minihalos and assuming the delta-function primordial spectrum, we
show the dependence of the constraints on annihilation modes, the mass of dark
matter, and the annihilation cross section. We report both conservative
constraints by assuming minihalos are fully destructed when becoming part of
halos originating from the standard almost-scale invariant primordial spectrum,
and optimistic constraints by neglecting destruction.
| [{'version': 'v1', 'created': 'Sat, 23 Dec 2017 18:47:35 GMT'}] | 2018-02-07 | [array(['Nakama', 'Tomohiro', ''], dtype=object)
array(['Suyama', 'Teruaki', ''], dtype=object)
array(['Kohri', 'Kazunori', ''], dtype=object)
array(['Hiroshima', 'Nagisa', ''], dtype=object)] |
19,721 | 2012.09812 | Dhruv Shah | Dhruv Shah, Benjamin Eysenbach, Gregory Kahn, Nicholas Rhinehart,
Sergey Levine | ViNG: Learning Open-World Navigation with Visual Goals | Presented at International Conference on Robotics and Automation
(ICRA) 2021 | null | 10.1109/ICRA48506.2021.9561936 | null | cs.RO cs.AI cs.LG | http://creativecommons.org/licenses/by/4.0/ | We propose a learning-based navigation system for reaching visually indicated
goals and demonstrate this system on a real mobile robot platform. Learning
provides an appealing alternative to conventional methods for robotic
navigation: instead of reasoning about environments in terms of geometry and
maps, learning can enable a robot to learn about navigational affordances,
understand what types of obstacles are traversable (e.g., tall grass) or not
(e.g., walls), and generalize over patterns in the environment. However, unlike
conventional planning algorithms, it is harder to change the goal for a learned
policy during deployment. We propose a method for learning to navigate towards
a goal image of the desired destination. By combining a learned policy with a
topological graph constructed out of previously observed data, our system can
determine how to reach this visually indicated goal even in the presence of
variable appearance and lighting. Three key insights, waypoint proposal, graph
pruning and negative mining, enable our method to learn to navigate in
real-world environments using only offline data, a setting where prior methods
struggle. We instantiate our method on a real outdoor ground robot and show
that our system, which we call ViNG, outperforms previously-proposed methods
for goal-conditioned reinforcement learning, including other methods that
incorporate reinforcement learning and search. We also study how \sysName
generalizes to unseen environments and evaluate its ability to adapt to such an
environment with growing experience. Finally, we demonstrate ViNG on a number
of real-world applications, such as last-mile delivery and warehouse
inspection. We encourage the reader to visit the project website for videos of
our experiments and demonstrations sites.google.com/view/ving-robot.
| [{'version': 'v1', 'created': 'Thu, 17 Dec 2020 18:22:32 GMT'}
{'version': 'v2', 'created': 'Fri, 26 Mar 2021 11:12:28 GMT'}] | 2022-10-11 | [array(['Shah', 'Dhruv', ''], dtype=object)
array(['Eysenbach', 'Benjamin', ''], dtype=object)
array(['Kahn', 'Gregory', ''], dtype=object)
array(['Rhinehart', 'Nicholas', ''], dtype=object)
array(['Levine', 'Sergey', ''], dtype=object)] |
19,722 | 2304.07130 | S{\l}awomir Dadas | S{\l}awomir Dadas | OPI at SemEval 2023 Task 9: A Simple But Effective Approach to
Multilingual Tweet Intimacy Analysis | null | null | null | null | cs.CL | http://creativecommons.org/licenses/by/4.0/ | This paper describes our submission to the SemEval 2023 multilingual tweet
intimacy analysis shared task. The goal of the task was to assess the level of
intimacy of Twitter posts in ten languages. The proposed approach consists of
several steps. First, we perform in-domain pre-training to create a language
model adapted to Twitter data. In the next step, we train an ensemble of
regression models to expand the training set with pseudo-labeled examples. The
extended dataset is used to train the final solution. Our method was ranked
first in five out of ten language subtasks, obtaining the highest average score
across all languages.
| [{'version': 'v1', 'created': 'Fri, 14 Apr 2023 13:49:28 GMT'}] | 2023-04-17 | [array(['Dadas', 'Sławomir', ''], dtype=object)] |
19,723 | 0711.3688 | Jean-Andre Marti | Jean-Andr\'e Marti (GTSI) | Regularity, Local and Microlocal Analysis in Theories of Generalized
Functions | null | null | null | null | math.FA | null | We introduce a general context involving a presheaf A and a subpresheaf B of
A. We show that all previously considered cases of local analysis of
generalized functions (defined from duality or algebraic techniques) can be
interpretated as the B-local analysis of sections of A. But the microlocal
analysis of the sections of sheaves or presheaves under consideration is
dissociated into a "frequential microlocal analysis " and into a "microlocal
asymptotic analysis". The frequential microlocal analysis based on the Fourier
transform leads to the study of propagation of singularities under only linear
(including pseudodifferential) operators in the theories described here, but
has been extended to some non linear cases in classical theories involving
Sobolev techniques. The microlocal asymptotic analysis can inherit from the
algebraic structure of B some good properties with respect to nonlinear
operations.
| [{'version': 'v1', 'created': 'Fri, 23 Nov 2007 09:39:18 GMT'}] | 2007-11-26 | [array(['Marti', 'Jean-André', '', 'GTSI'], dtype=object)] |
19,724 | 2107.00529 | Tommaso Benciolini | Tommaso Benciolini, Tim Br\"udigam, Marion Leibold | Multistage Stochastic Model Predictive Control for Urban Automated
Driving | This work has been accepted to the IEEE 2021 International Conference
on Intelligent Transportation Systems. The published version may be found at
https://doi.org/10.1109/ITSC48978.2021.9564572 | null | 10.1109/ITSC48978.2021.9564572 | null | eess.SY cs.SY | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Trajectory planning in urban automated driving is challenging because of the
high uncertainty resulting from the unknown future motion of other traffic
participants. Robust approaches guarantee safety, but tend to result in overly
conservative motion planning. Hence, we propose to use Stochastic Model
Predictive Control for vehicle control in urban driving, allowing to
efficiently plan the vehicle trajectory, while maintaining the risk probability
sufficiently low. For motion optimization, we propose to use a two-stage
hierarchical structure that plans the trajectory and the maneuver separately. A
high-level layer takes advantage of a long prediction horizon and of an
abstract model to plan the optimal maneuver, and a lower level is in charge of
executing the selected maneuver by properly planning the vehicle's trajectory.
Numerical simulations are included, showing the potential of our proposal.
| [{'version': 'v1', 'created': 'Thu, 1 Jul 2021 15:16:42 GMT'}
{'version': 'v2', 'created': 'Sat, 27 Nov 2021 09:13:07 GMT'}] | 2021-11-30 | [array(['Benciolini', 'Tommaso', ''], dtype=object)
array(['Brüdigam', 'Tim', ''], dtype=object)
array(['Leibold', 'Marion', ''], dtype=object)] |
19,725 | 1202.0792 | Andreas Menzel | Andreas M. Menzel | Collective motion of binary self-propelled particle mixtures | 16 pages, 10 figures | Phys. Rev. E 85, 021912 (2012) | 10.1103/PhysRevE.85.021912 | null | cond-mat.soft cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this study, we investigate the phenomenon of collective motion in binary
mixtures of self-propelled particles. We consider two particle species, each of
which consisting of pointlike objects that propel with a velocity of constant
magnitude. Within each species, the particles try to achieve polar alignment of
their velocity vectors, whereas we analyze the cases of preferred polar,
antiparallel, as well as perpendicular alignment between particles of different
species. Our focus is on the effect that the interplay between the two species
has on the threshold densities for the onset of collective motion and on the
nature of the solutions above onset. For this purpose, we start from suitable
Langevin equations in the particle picture, from which we derive mean field
equations of the Fokker-Planck type and finally macroscopic continuum field
equations. We perform particle simulations of the Langevin equations, linear
stability analyses of the Fokker-Planck and macroscopic continuum equations,
and we numerically solve the Fokker-Planck equations. Both, spatially
homogeneous and inhomogeneous solutions are investigated, where the latter
correspond to stripe-like flocks of collectively moving particles. In general,
the interaction between the two species reduces the threshold density for the
onset of collective motion of each species. However, this interaction also
reduces the spatial organization in the stripe-like flocks. The most
interesting behavior is found for the case of preferred perpendicular alignment
between different species. There, a competition between polar and truly nematic
orientational ordering of the velocity vectors takes place within each particle
species. Finally, depending on the alignment rule for particles of different
species and within certain ranges of particle densities, identical and inverted
spatial density profiles can be found for the two particle species.
| [{'version': 'v1', 'created': 'Fri, 3 Feb 2012 18:17:56 GMT'}] | 2013-11-20 | [array(['Menzel', 'Andreas M.', ''], dtype=object)] |
19,726 | 1610.08472 | Vladimir Kirilin | S. Giombi, V. Gurucharan, V. Kirilin, S. Prakash, E. Skvortsov | On the Higher-Spin Spectrum in Large N Chern-Simons Vector Models | 52 pages, 7 figures. v3: Minor corrections | null | 10.1007/JHEP01(2017)058 | PUPT-2512, LMU-ASC 52/16 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Chern-Simons gauge theories coupled to massless fundamental scalars or
fermions define interesting non-supersymmetric 3d CFTs that possess approximate
higher-spin symmetries at large N. In this paper, we compute the scaling
dimensions of the higher-spin operators in these models, to leading order in
the 1/N expansion and exactly in the 't Hooft coupling. We obtain these results
in two independent ways: by using conformal symmetry and the classical
equations of motion to fix the structure of the current non-conservation, and
by a direct Feynman diagram calculation. The full dependence on the 't Hooft
coupling can be restored by using results that follow from the weakly broken
higher-spin symmetry. This analysis also allows us to obtain some explicit
results for the non-conserved, parity-breaking structures that appear in planar
three-point functions of the higher-spin operators. At large spin, we find that
the anomalous dimensions grow logarithmically with the spin, in agreement with
general expectations. This logarithmic behavior disappears in the strong
coupling limit, where the anomalous dimensions turn into those of the critical
O(N) or Gross-Neveu models, in agreement with the conjectured 3d bosonization
duality.
| [{'version': 'v1', 'created': 'Wed, 26 Oct 2016 19:23:25 GMT'}
{'version': 'v2', 'created': 'Fri, 18 Nov 2016 13:54:36 GMT'}
{'version': 'v3', 'created': 'Tue, 19 Sep 2017 19:02:40 GMT'}] | 2017-09-21 | [array(['Giombi', 'S.', ''], dtype=object)
array(['Gurucharan', 'V.', ''], dtype=object)
array(['Kirilin', 'V.', ''], dtype=object)
array(['Prakash', 'S.', ''], dtype=object)
array(['Skvortsov', 'E.', ''], dtype=object)] |
19,727 | 1512.05676 | Dinko Atanasov Da | D. Atanasov, P. Ascher, K. Blaum, R. B. Cakirli, T. E. Cocolios, S.
George, F. Herfurth, D. Kisler, M. Kowalska, S. Kreim, Yu. A. Litvinov, D.
Lunney, V. Manea, D. Neidherr, M. Rosenbusch, L. Schweikhard, A. Welker, F.
Wienholtz, R. N. Wolf, K. Zuber | Precision Mass Measurements of 129-131Cd and Their Impact on Stellar
Nucleosynthesis via the Rapid Neutron Capture Process | null | Phys. Rev. Lett. 115, 232501 (2015) | 10.1103/PhysRevLett.115.232501 | null | nucl-ex | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Masses adjacent to the classical waiting-point nuclide 130Cd have been
measured by using the Penning- trap spectrometer ISOLTRAP at ISOLDE/CERN. We
find a significant deviation of over 400 keV from earlier values evaluated by
using nuclear beta-decay data. The new measurements show the reduction of the N
= 82 shell gap below the doubly magic 132Sn. The nucleosynthesis associated
with the ejected wind from type-II supernovae as well as from compact object
binary mergers is studied, by using state-of-the-art hydrodynamic simulations.
We find a consistent and direct impact of the newly measured masses on the
calculated abundances in the A = 128 - 132 region and a reduction of the
uncertainties from the precision mass input data.
| [{'version': 'v1', 'created': 'Thu, 17 Dec 2015 17:20:59 GMT'}] | 2015-12-18 | [array(['Atanasov', 'D.', ''], dtype=object)
array(['Ascher', 'P.', ''], dtype=object)
array(['Blaum', 'K.', ''], dtype=object)
array(['Cakirli', 'R. B.', ''], dtype=object)
array(['Cocolios', 'T. E.', ''], dtype=object)
array(['George', 'S.', ''], dtype=object)
array(['Herfurth', 'F.', ''], dtype=object)
array(['Kisler', 'D.', ''], dtype=object)
array(['Kowalska', 'M.', ''], dtype=object)
array(['Kreim', 'S.', ''], dtype=object)
array(['Litvinov', 'Yu. A.', ''], dtype=object)
array(['Lunney', 'D.', ''], dtype=object)
array(['Manea', 'V.', ''], dtype=object)
array(['Neidherr', 'D.', ''], dtype=object)
array(['Rosenbusch', 'M.', ''], dtype=object)
array(['Schweikhard', 'L.', ''], dtype=object)
array(['Welker', 'A.', ''], dtype=object)
array(['Wienholtz', 'F.', ''], dtype=object)
array(['Wolf', 'R. N.', ''], dtype=object)
array(['Zuber', 'K.', ''], dtype=object)] |
19,728 | math/0502464 | Ser-Peow Tan | Ser Peow Tan, Yan Loi Wong, Ying Zhang | Generalized Markoff Maps and McShane's Identity | 49 pages, 9 figures | Advances in Mathematics 217:2 (2008) 761-813 | 10.1016/j.aim.2007.09.004 | null | math.GT math.DG | null | We study general representations of the free group on two generators into
$SL(2,C)$, and the connection with generalized Markoff maps, following
Bowditch. We show that Bowditch's Q-conditions for generalized Markoff maps are
sufficient for the generalized McShane identity to hold for the corresponding
representations and that the subset of representations satisfying these
conditions is the largest open subset in the relative character variety on
which the mapping class group acts properly discontinuously. Moreover we
generalize Bowditch's results on variations of McShane's identity for complete,
finite volume hyperbolic 3-manifolds which fiber over the circle, with the
fiber a punctured-torus, to identities for incomplete hyperbolic structures on
such manifolds, hence obtaining identities for closed hyperbolic 3-manifolds
which are obtained by doing hyperbolic Dehn surgery on such manifolds.
| [{'version': 'v1', 'created': 'Tue, 22 Feb 2005 19:07:22 GMT'}] | 2007-11-21 | [array(['Tan', 'Ser Peow', ''], dtype=object)
array(['Wong', 'Yan Loi', ''], dtype=object)
array(['Zhang', 'Ying', ''], dtype=object)] |
19,729 | 1203.0141 | Xiaosong Chen | Maoxin Liu, Jingfang Fan, Liangsheng Li, and Xiaosong Chen | Continuous Percolation Phase Transitions of Two-dimensional Lattice
Networks under a Generalized Achlioptas Process | 7 pages, 14 figures, accepted for publication in Eur. Phys. J. B | null | 10.1140/epjb/e2012-20872-1 | null | cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The percolation phase transitions of two-dimensional lattice networks under a
generalized Achlioptas process (GAP) are investigated. During the GAP, two
edges are chosen randomly from the lattice and the edge with minimum product of
the two connecting cluster sizes is taken as the next occupied bond with a
probability $p$. At $p=0.5$, the GAP becomes the random growth model and leads
to the minority product rule at $p=1$. Using the finite-size scaling analysis,
we find that the percolation phase transitions of these systems with $0.5 \le p
\le 1$ are always continuous and their critical exponents depend on $p$.
Therefore, the universality class of the critical phenomena in two-dimensional
lattice networks under the GAP is related to the probability parameter $p$ in
addition.
| [{'version': 'v1', 'created': 'Thu, 1 Mar 2012 10:50:20 GMT'}] | 2012-03-02 | [array(['Liu', 'Maoxin', ''], dtype=object)
array(['Fan', 'Jingfang', ''], dtype=object)
array(['Li', 'Liangsheng', ''], dtype=object)
array(['Chen', 'Xiaosong', ''], dtype=object)] |
19,730 | cond-mat/0510722 | Ilya Finkler | Ilya Finkler, Bertrand I. Halperin (Harvard), Assa Auerbach
(Technion), Amir Yacoby (Weizmann) | Domain Patterns in the Microwave-Induced Zero-Resistance State | 19 pages, 5 figures; submitted to a special issue of Journal of
Statistical Physics, in honor of P. C. Hohenberg and J. S. Langer | null | 10.1007/s10955-006-9037-7 | null | cond-mat.mes-hall | null | It has been proposed that the microwave-induced ``zero-resistance''
phenomenon, observed in a GaAs two-dimensional electron system at low
temperatures in moderate magnetic fields, results from a state with multiple
domains, in which a large local electric field $\bE(\br)$ is oriented in
different directions. We explore here the questions of what may determine the
domain arrangement in a given sample, what do the domains look like in
representative cases, and what may be the consequences of domain-wall
localization on the macroscopic dc conductance. We consider both effects of
sample boundaries and effects of disorder, in a simple model, which has a
constant Hall conductivity, and is characterized by a Lyapunov functional.
| [{'version': 'v1', 'created': 'Thu, 27 Oct 2005 05:19:39 GMT'}] | 2015-06-25 | [array(['Finkler', 'Ilya', '', 'Harvard'], dtype=object)
array(['Halperin', 'Bertrand I.', '', 'Harvard'], dtype=object)
array(['Auerbach', 'Assa', '', 'Technion'], dtype=object)
array(['Yacoby', 'Amir', '', 'Weizmann'], dtype=object)] |
19,731 | 1805.00556 | Stefano Markidis Prof. | Sai Narasimhamurthy, Nikita Danilov, Sining Wu, Ganesan Umanesan,
Stefano Markidis, Sergio Rivas-Gomez, Ivy Bo Peng, Erwin Laure, Dirk Pleiter,
Shaun de Witt | SAGE: Percipient Storage for Exascale Data Centric Computing | null | Parallel Computing, 23 March 2018 | 10.1016/j.parco.2018.03.002 | null | cs.DC | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We aim to implement a Big Data/Extreme Computing (BDEC) capable system
infrastructure as we head towards the era of Exascale computing - termed SAGE
(Percipient StorAGe for Exascale Data Centric Computing). The SAGE system will
be capable of storing and processing immense volumes of data at the Exascale
regime, and provide the capability for Exascale class applications to use such
a storage infrastructure. SAGE addresses the increasing overlaps between Big
Data Analysis and HPC in an era of next-generation data centric computing that
has developed due to the proliferation of massive data sources, such as large,
dispersed scientific instruments and sensors, whose data needs to be processed,
analyzed and integrated into simulations to derive scientific and innovative
insights. Indeed, Exascale I/O, as a problem that has not been sufficiently
dealt with for simulation codes, is appropriately addressed by the SAGE
platform. The objective of this paper is to discuss the software architecture
of the SAGE system and look at early results we have obtained employing some of
its key methodologies, as the system continues to evolve.
| [{'version': 'v1', 'created': 'Tue, 1 May 2018 21:20:31 GMT'}] | 2018-05-03 | [array(['Narasimhamurthy', 'Sai', ''], dtype=object)
array(['Danilov', 'Nikita', ''], dtype=object)
array(['Wu', 'Sining', ''], dtype=object)
array(['Umanesan', 'Ganesan', ''], dtype=object)
array(['Markidis', 'Stefano', ''], dtype=object)
array(['Rivas-Gomez', 'Sergio', ''], dtype=object)
array(['Peng', 'Ivy Bo', ''], dtype=object)
array(['Laure', 'Erwin', ''], dtype=object)
array(['Pleiter', 'Dirk', ''], dtype=object)
array(['de Witt', 'Shaun', ''], dtype=object)] |
19,732 | 2204.03689 | Erin Beckman | Louigi Addario-Berry, Erin Beckman, Jessica Lin | Symmetric cooperative motion in one dimension | 33 pages, 0 figures | null | null | null | math.PR cs.NA math.AP math.NA | http://creativecommons.org/licenses/by/4.0/ | We explore the relationship between recursive distributional equations and
convergence results for finite difference schemes of parabolic partial
differential equations (PDEs). We focus on a family of random processes called
symmetric cooperative motions, which generalize the symmetric simple random
walk and the symmetric hipster random walk introduced in [Addario-Berry,
Cairns, Devroye, Kerriou and Mitchell, arXiv:1909.07367]. We obtain a
distributional convergence result for symmetric cooperative motions and, along
the way, obtain a novel proof of the Bernoulli central limit theorem. In
addition, we prove a PDE result relating distributional solutions and viscosity
solutions of the porous medium equation and the parabolic $p$-Laplace equation,
respectively, in one dimension.
| [{'version': 'v1', 'created': 'Thu, 7 Apr 2022 18:41:33 GMT'}] | 2022-04-11 | [array(['Addario-Berry', 'Louigi', ''], dtype=object)
array(['Beckman', 'Erin', ''], dtype=object)
array(['Lin', 'Jessica', ''], dtype=object)] |
19,733 | hep-lat/9709125 | Martin Luescher | S. Capitani, M. Guagnelli, M. Luescher, S. Sint, R. Sommer, P. Weisz
and H. Wittig | Non-perturbative quark mass renormalization | Talk given at LATTICE '97, 6 pages, Latex source, 7 eps figures,
needs epsfig | Nucl.Phys.Proc.Suppl. 63 (1998) 153-158 | 10.1016/S0920-5632(97)00707-X | DESY 97-188 | hep-lat | null | We show that the renormalization factor relating the renormalization group
invariant quark masses to the bare quark masses computed in lattice QCD can be
determined non-perturbatively. The calculation is based on an extension of a
finite-size technique previously employed to compute the running coupling in
quenched QCD. As a by-product we obtain the $\Lambda$--parameter in this theory
with completely controlled errors.
| [{'version': 'v1', 'created': 'Fri, 26 Sep 1997 14:54:35 GMT'}] | 2009-10-30 | [array(['Capitani', 'S.', ''], dtype=object)
array(['Guagnelli', 'M.', ''], dtype=object)
array(['Luescher', 'M.', ''], dtype=object)
array(['Sint', 'S.', ''], dtype=object)
array(['Sommer', 'R.', ''], dtype=object)
array(['Weisz', 'P.', ''], dtype=object)
array(['Wittig', 'H.', ''], dtype=object)] |
19,734 | 1701.07100 | Sebastian Streichan | Sebastian J Streichan and Matthew F Lefebvre and Nicholas Noll and
Eric F Wieschaus and Boris I Shraiman | Quantification of myosin distribution predicts global morphogenetic flow
in the fly embryo | 15 total pages, with 9 total figures (7 pages main text with 4
figures and 8 pages SI text with 5 SI figures) | null | null | null | q-bio.TO q-bio.CB q-bio.QM | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | During embryogenesis tissue layers continuously rearrange and fold into
specific shapes. Developmental biology identified patterns of gene expression
and cytoskeletal regulation underlying local tissue dynamics, but how actions
of multiple domains of distinct cell types coordinate to remodel tissues at the
organ scale remains unclear. We use in toto light-sheet microscopy, automated
image analysis, and physical modeling to quantitatively investigate the link
between kinetics of global tissue transformations and force generation patterns
during Drosophila gastrulation. We find embryo-scale shape changes are
represented by a temporal sequence of three simple flow field configurations.
Each phase is accompanied by a characteristic spatial myosin distribution,
quantified in terms of a coarse-grained 'myosin tensor' that captures both
concentration and anisotropy. Our model assumes tissue flow is driven by stress
proportional to the myosin tensor, and is effectively visco-elastic with two
parameters that control 'irrotational' and 'divergence-less' components of the
flow. With just three global parameters, this model achieves up to 90%
agreement between predicted and measured flow. The analysis uncovers importance
of a) spatial modulation of myosin distribution and b) long-range spreading of
its effect due to mechanical interaction of cells. In particular, we find
germband extension phase is associated with the onset of effective areal
incompressibility of the epithelium, which makes the relation of flow and
myosin forcing strongly non-local. Our analysis also revealed a new function
for basal myosin in generating a dorsally directed flow and, combined with
mutant analysis, identified an unconventional control mechanism through twist
dependent reduction of basal myosin levels on the ventral side. We conclude
that understanding morphogenetic flow requires a fundamentally global
perspective.
| [{'version': 'v1', 'created': 'Tue, 24 Jan 2017 22:56:37 GMT'}] | 2017-01-26 | [array(['Streichan', 'Sebastian J', ''], dtype=object)
array(['Lefebvre', 'Matthew F', ''], dtype=object)
array(['Noll', 'Nicholas', ''], dtype=object)
array(['Wieschaus', 'Eric F', ''], dtype=object)
array(['Shraiman', 'Boris I', ''], dtype=object)] |
19,735 | 1704.07607 | Denys Dutykh | Suelen Gasparin (LAMA, PUCPR), Julien Berger (LOCIE), Denys Dutykh
(LAMA), Nathan Mendes (PUCPR) | Solving nonlinear diffusive problems in buildings by means of a Spectral
Reduced-Order Model | 42 pages, 22 figures, 2 tables, 51 references. Other author's papers
can be downloaded at http://www.denys-dutykh.com/ | Journal of Building Performance Simulation (2019), Vol. 12, Issue
1, pp. 17-36 | 10.1080/19401493.2018.1458905 | null | physics.comp-ph cs.NA math.AP math.NA physics.class-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This paper proposes the use of a Spectral method to simulate diffusive
moisture transfer through porous materials as a Reduced-Order Model (ROM). The
Spectral approach is an a priori method assuming a separated representation of
the solution. The method is compared with both classical Euler implicit and
Crank-Nicolson schemes, considered as large original models. Their performance
- in terms of accuracy, complexity reduction and CPU time reduction - are
discussed for linear and nonlinear cases of moisture diffusive transfer through
single and multi-layered one-dimensional domains, considering highly
moisture-dependent properties. Results show that the Spectral reduced-order
model approach enables to simulate accurately the field of interest.
Furthermore, numerical gains become particularly interesting for nonlinear
cases since the proposed method can drastically reduce the computer run time,
by a factor of 100, when compared to the traditional Crank-Nicolson scheme for
one-dimensional applications.
| [{'version': 'v1', 'created': 'Tue, 25 Apr 2017 09:36:59 GMT'}
{'version': 'v2', 'created': 'Tue, 17 Apr 2018 14:25:56 GMT'}] | 2020-02-20 | [array(['Gasparin', 'Suelen', '', 'LAMA, PUCPR'], dtype=object)
array(['Berger', 'Julien', '', 'LOCIE'], dtype=object)
array(['Dutykh', 'Denys', '', 'LAMA'], dtype=object)
array(['Mendes', 'Nathan', '', 'PUCPR'], dtype=object)] |
19,736 | gr-qc/0612121 | Michael Seifert | Michael D. Seifert and Robert M. Wald | A general variational principle for spherically symmetric perturbations
in diffeomorphism covariant theories | 13 pages; submitted to Phys. Rev. D. v2: changed formatting, added
conclusion, corrected sign conventions | Phys.Rev.D75:084029,2007 | 10.1103/PhysRevD.75.084029 | null | gr-qc | null | We present a general method for the analysis of the stability of static,
spherically symmetric solutions to spherically symmetric perturbations in an
arbitrary diffeomorphism covariant Lagrangian field theory. Our method involves
fixing the gauge and solving the linearized gravitational field equations to
eliminate the metric perturbation variable in terms of the matter variables. In
a wide class of cases--which include f(R) gravity, the Einstein-aether theory
of Jacobson and Mattingly, and Bekenstein's TeVeS theory--the remaining
perturbation equations for the matter fields are second order in time. We show
how the symplectic current arising from the original Lagrangian gives rise to a
symmetric bilinear form on the variables of the reduced theory. If this
bilinear form is positive definite, it provides an inner product that puts the
equations of motion of the reduced theory into a self-adjoint form. A
variational principle can then be written down immediately, from which
stability can be tested readily. We illustrate our method in the case of
Einstein's equation with perfect fluid matter, thereby re-deriving, in a
systematic manner, Chandrasekhar's variational principle for radial
oscillations of spherically symmetric stars. In a subsequent paper, we will
apply our analysis to f(R) gravity, the Einstein-aether theory, and
Bekenstein's TeVeS theory.
| [{'version': 'v1', 'created': 'Tue, 19 Dec 2006 20:57:57 GMT'}
{'version': 'v2', 'created': 'Fri, 9 Mar 2007 22:51:58 GMT'}] | 2008-11-26 | [array(['Seifert', 'Michael D.', ''], dtype=object)
array(['Wald', 'Robert M.', ''], dtype=object)] |
19,737 | 2208.05444 | Heather Kulik | Chenru Duan, Aditya Nandy, Gianmarco Terrones, David W. Kastner, and
Heather J. Kulik | Active Learning Exploration of Transition Metal Complexes to Discover
Method-Insensitive and Synthetically Accessible Chromophores | null | null | null | null | physics.chem-ph cond-mat.mtrl-sci cs.LG q-bio.BM | http://creativecommons.org/licenses/by/4.0/ | Transition metal chromophores with earth-abundant transition metals are an
important design target for their applications in lighting and non-toxic
bioimaging, but their design is challenged by the scarcity of complexes that
simultaneously have optimal target absorption energies in the visible region as
well as well-defined ground states. Machine learning (ML) accelerated discovery
could overcome such challenges by enabling screening of a larger space, but is
limited by the fidelity of the data used in ML model training, which is
typically from a single approximate density functional. To address this
limitation, we search for consensus in predictions among 23 density functional
approximations across multiple rungs of Jacobs ladder. To accelerate the
discovery of complexes with absorption energies in the visible region while
minimizing MR character, we use 2D efficient global optimization to sample
candidate low-spin chromophores from multi-million complex spaces. Despite the
scarcity (i.e., approx. 0.01\%) of potential chromophores in this large
chemical space, we identify candidates with high likelihood (i.e., > 10\%) of
computational validation as the ML models improve during active learning,
representing a 1,000-fold acceleration in discovery. Absorption spectra of
promising chromophores from time-dependent density functional theory verify
that 2/3 of candidates have the desired excited state properties. The
observation that constituent ligands from our leads have demonstrated
interesting optical properties in the literature exemplifies the effectiveness
of our construction of a realistic design space and active learning approach.
| [{'version': 'v1', 'created': 'Wed, 10 Aug 2022 16:55:33 GMT'}
{'version': 'v2', 'created': 'Thu, 15 Sep 2022 16:15:21 GMT'}] | 2022-09-16 | [array(['Duan', 'Chenru', ''], dtype=object)
array(['Nandy', 'Aditya', ''], dtype=object)
array(['Terrones', 'Gianmarco', ''], dtype=object)
array(['Kastner', 'David W.', ''], dtype=object)
array(['Kulik', 'Heather J.', ''], dtype=object)] |
19,738 | 1705.02198 | Geoff Boeing | Geoff Boeing | A Multi-Scale Analysis of 27,000 Urban Street Networks: Every US City,
Town, Urbanized Area, and Zillow Neighborhood | null | Environment and Planning B: Urban Analytics and City Science, 2018 | 10.1177/2399808318784595 | null | cs.SI physics.soc-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | OpenStreetMap offers a valuable source of worldwide geospatial data useful to
urban researchers. This study uses the OSMnx software to automatically download
and analyze 27,000 US street networks from OpenStreetMap at metropolitan,
municipal, and neighborhood scales - namely, every US city and town, census
urbanized area, and Zillow-defined neighborhood. It presents empirical findings
on US urban form and street network characteristics, emphasizing measures
relevant to graph theory, transportation, urban design, and morphology such as
structure, connectedness, density, centrality, and resilience. In the past,
street network data acquisition and processing have been challenging and ad
hoc. This study illustrates the use of OSMnx and OpenStreetMap to consistently
conduct street network analysis with extremely large sample sizes, with clearly
defined network definitions and extents for reproducibility, and using
nonplanar, directed graphs. These street networks and measures data have been
shared in a public repository for other researchers to use.
| [{'version': 'v1', 'created': 'Wed, 29 Mar 2017 21:06:13 GMT'}
{'version': 'v2', 'created': 'Wed, 14 Feb 2018 18:56:53 GMT'}
{'version': 'v3', 'created': 'Tue, 5 Jun 2018 15:52:30 GMT'}
{'version': 'v4', 'created': 'Thu, 2 Aug 2018 18:37:12 GMT'}] | 2018-08-06 | [array(['Boeing', 'Geoff', ''], dtype=object)] |
19,739 | 1503.04606 | Michal Kowal | E. Ruchowska, H. Mach, M. Kowal, J. Skalski, W. A. Plociennik, B.
Fogelberg | Search for octupole correlations in $^{147}$Nd | Submitted to PRC | null | 10.1103/PhysRevC.92.034328 | null | nucl-th nucl-ex | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Properties of excited states in $^{147}$Nd have been studied with
multispectra and $\gamma \gamma$ coincidence measurements. Twenty-four new
$\gamma$-lines and three new levels have been introduced into the level scheme
of $^{147}$Nd. Lifetimes of eight excited levels in $^{147}$Nd, populated in
the $\beta$ decay of $^{147}$Pr, have been measured using the advanced
time-delayed $\beta\gamma\gamma$(t) method. Reduced transition probabilities
have been determined for 30 $\gamma$-transitions in $^{147}$Nd. Potential
energy surfaces on the ($\beta_{2}$,$\beta_{3}$) plane calculated for
$^{147}$Nd using the Strutinsky method predict two single quasiparticle
configurations with nonzero octupole deformation, with K=1/2 and K=5/2. We do
not observe parity doublet bands with K=5/2. For pair of opposite parity bands
that could form the K=1/2 parity doublet we were able only to determine lower
limit of the dipole moment, $|D_0|\geq$0.02 e$\cdot fm$.
| [{'version': 'v1', 'created': 'Mon, 16 Mar 2015 11:14:05 GMT'}] | 2015-10-28 | [array(['Ruchowska', 'E.', ''], dtype=object)
array(['Mach', 'H.', ''], dtype=object)
array(['Kowal', 'M.', ''], dtype=object)
array(['Skalski', 'J.', ''], dtype=object)
array(['Plociennik', 'W. A.', ''], dtype=object)
array(['Fogelberg', 'B.', ''], dtype=object)] |
19,740 | hep-ph/0411026 | Edmond Berger | Edmond L. Berger, Jianwei Qiu, and Yili Wang | Upsilon Transverse Momentum at Hadron Colliders | 4 pages, 5 figures. Presented at the 2004 Meeting of the APS Division
of Particles and Fields, University of California, Riverside, CA, Aug 26-31,
2004 | Int.J.Mod.Phys.A20:3753-3755,2005 | 10.1142/S0217751X05027515 | ANL-HEP-CP-04-110 | hep-ph | null | We predict the shape of the transverse momentum p_T spectrum of Upsilon
production. The distribution at low p_T is dominated by the region of small
impact parameter b and may be computed reliably in perturbation theory. We
resum to all orders in the strong coupling alpha_s the process-independent
large logarithmic contributions that arise from initial-state gluon showers in
the small p_T (< M_Upsilon) region. The cross section at large p_T is
represented by the alpha_s^3 lowest-order non-vanishing perturbative
contribution.
| [{'version': 'v1', 'created': 'Mon, 1 Nov 2004 21:39:01 GMT'}] | 2014-11-18 | [array(['Berger', 'Edmond L.', ''], dtype=object)
array(['Qiu', 'Jianwei', ''], dtype=object)
array(['Wang', 'Yili', ''], dtype=object)] |
19,741 | astro-ph/0110660 | Konishchev K. V. | E. V. Bugaev, M. G. Elbakidze and K. V. Konishchev | Baryon asymmetry of the Universe from evaporation of primordial black
holes | 5 pages (including 6 .eps files) | Phys.Atom.Nucl. 66 (2003) 476-480; Yad.Fiz. 66 (2003) 504-508 | 10.1134/1.1563709 | null | astro-ph | null | The process of baryogenesis through the evaporation of black holes formed at
the end of inflation phase is considered. The increase of black hole mass due
to accretion from the surrounding radiation after the reheating is taken into
account. It is shown that the influence of the accretion on the baryogenesis is
important only in the case when the initial values of black hole mass are
larger than $\sim 10^{4}{g}$. The behavior of calculated baryon asymmetry, as a
function of model parameters, is studied.
| [{'version': 'v1', 'created': 'Tue, 30 Oct 2001 16:59:37 GMT'}
{'version': 'v2', 'created': 'Wed, 31 Oct 2001 14:26:09 GMT'}
{'version': 'v3', 'created': 'Fri, 2 Nov 2001 13:00:00 GMT'}] | 2015-06-24 | [array(['Bugaev', 'E. V.', ''], dtype=object)
array(['Elbakidze', 'M. G.', ''], dtype=object)
array(['Konishchev', 'K. V.', ''], dtype=object)] |
19,742 | 2109.10732 | Gabriele Grillo | Elvise Berchio, Matteo Bonforte, Gabriele Grillo, Matteo Muratori | The Fractional Porous Medium Equation on noncompact Riemannian manifolds | null | null | null | null | math.AP math.DG math.FA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study nonnegative solutions to the Fractional Porous Medium Equation on a
suitable class of connected, noncompact Riemannian manifolds. We provide
existence and smoothing estimates for solutions, in an appropriate weak (dual)
sense, for data belonging either to the usual $L^1$ space or to a considerably
larger weighted space determined in terms of the fractional Green function. The
class of manifolds for which the results hold include both the Euclidean and
the hyperbolic spaces and even in the Euclidean situation involve a class of
data which is larger than previously known one.
| [{'version': 'v1', 'created': 'Wed, 22 Sep 2021 13:38:40 GMT'}] | 2021-09-23 | [array(['Berchio', 'Elvise', ''], dtype=object)
array(['Bonforte', 'Matteo', ''], dtype=object)
array(['Grillo', 'Gabriele', ''], dtype=object)
array(['Muratori', 'Matteo', ''], dtype=object)] |
19,743 | hep-th/9805190 | Harald Skarke | M. Kreuzer and H. Skarke | Classification of Reflexive Polyhedra in Three Dimensions | 19 pages, LaTeX2e | Adv.Theor.Math.Phys.2:847-864,1998 | null | TUW-98-13, UTTG-07-98 | hep-th math.AG | null | We present the last missing details of our algorithm for the classification
of reflexive polyhedra in arbitrary dimensions. We also present the results of
an application of this algorithm to the case of three dimensional reflexive
polyhedra. We get 4319 such polyhedra that give rise to K3 surfaces embedded in
toric varieties. 16 of these contain all others as subpolyhedra. The 4319
polyhedra form a single connected web if we define two polyhedra to be
connected if one of them contains the other.
| [{'version': 'v1', 'created': 'Wed, 27 May 1998 21:15:44 GMT'}] | 2008-11-26 | [array(['Kreuzer', 'M.', ''], dtype=object)
array(['Skarke', 'H.', ''], dtype=object)] |
19,744 | 1312.3465 | James Osborn | H. W. Shepherd, J. Osborn, R. W. Wilson, T. Butterley, R. Avila, V. S.
Dhillon and T. J. Morris | Stereo-SCIDAR: Optical turbulence profiling with high sensitivity using
a modified SCIDAR instrument | 11 pages, 11 figures, accepted by MNRAS 27/11/13 | MNRAS, 437(4), 3568-3577, 2013 | 10.1093/mnras/stt2150 | null | astro-ph.IM | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The next generation of adaptive optics (AO) systems will require tomographic
reconstruction techniques to map the optical refractive index fluctuations,
generated by the atmospheric turbulence, along the line of sight to the
astronomical target. These systems can be enhanced with data from an external
atmospheric profiler. This is important for Extremely Large Telescope scale
tomography. Here we propose a new instrument which utilises the generalised
SCIntillation Detection And Ranging (SCIDAR) technique to allow high
sensitivity vertical profiles of the atmospheric optical turbulence and wind
velocity profile above astronomical observatories. The new approach, which we
refer to as 'Stereo-SCIDAR', uses a stereoscopic system with the scintillation
pattern from each star of a double-star target incident on a separate detector.
Separating the pupil images for each star has several advantages including:
increased magnitude difference tolerance for the target stars; negating the
need for re-calibration due to the normalisation errors usually associated with
SCIDAR; an increase of at least a factor of two in the signal-to-noise ratio of
the cross-covariance function and hence the profile for equal magnitude target
stars and up to a factor of 16 improvement for targets of 3 magnitudes
difference; and easier real-time reconstruction of the wind-velocity profile.
Theoretical response functions are calculated for the instrument, and the
performance is investigated using a Monte-Carlo simulation. The technique is
demonstrated using data recorded at the 2.5 m Nordic Optical Telescope and the
1.0 m Jacobus Kapteyn Telescope, both on La Palma.
| [{'version': 'v1', 'created': 'Thu, 12 Dec 2013 12:38:02 GMT'}] | 2014-01-07 | [array(['Shepherd', 'H. W.', ''], dtype=object)
array(['Osborn', 'J.', ''], dtype=object)
array(['Wilson', 'R. W.', ''], dtype=object)
array(['Butterley', 'T.', ''], dtype=object)
array(['Avila', 'R.', ''], dtype=object)
array(['Dhillon', 'V. S.', ''], dtype=object)
array(['Morris', 'T. J.', ''], dtype=object)] |
19,745 | 2204.08792 | Yandong Ma | Kaiying Dou, Wenhui Du, Zhonglin He, Ying Dai, Baibiao Huang, and
Yandong Ma | Antiferromagnetic skyrmion crystal in Janus monolayer CrSi2N2As2 | null | null | null | null | cond-mat.mtrl-sci | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Antiferromagnetic skyrmion crystal (AF-SkX), a regular array of
antiferromagnetic skyrmions, is a fundamental phenomenon in the field of
condensed-matter physics. So far, only very few proposals have been made to
realize the AF-SkX, and most based on three-dimensional (3D) materials. Herein,
using first-principles calculations and Monte-Carlo simulations, we report the
identification of AF-SkX in two-dimensional lattice of Janus monolayer
CrSi2N2As2. Arising from the broken inversion symmetry and strong spin-orbit
coupling, large Dzyaloshinskii-Moriya interaction is obtained in Janus
monolayer CrSi2N2As2. This, combined with the geometric frustration of its
triangular lattice, gives rise to the skyrmion physics and long-sought AF-SkX
in the presence of external magnetic field. More intriguingly, this system
presents two different antiferromagnetic skyrmion phases, and such phenomenon
is distinct from those reported in 3D systems. Furthermore, by contacting with
Sc2CO2, the creation and annihilation of AF-SkX in Janus monolayer CrSi2N2As2
can be achieved through ferroelectricity. These findings greatly enrich the
research on antiferromagnetic skyrmions.
| [{'version': 'v1', 'created': 'Tue, 19 Apr 2022 10:29:05 GMT'}] | 2022-04-20 | [array(['Dou', 'Kaiying', ''], dtype=object)
array(['Du', 'Wenhui', ''], dtype=object)
array(['He', 'Zhonglin', ''], dtype=object)
array(['Dai', 'Ying', ''], dtype=object)
array(['Huang', 'Baibiao', ''], dtype=object)
array(['Ma', 'Yandong', ''], dtype=object)] |
19,746 | 0811.3314 | Kenji Kamide | Kenji Kamide, Takashi Kimura, and Susumu Kurihara | Tomonaga-Luttinger Liquid Renormalized by a Single Impurity | 4pages, 2 figures | null | 10.1088/1742-6596/150/2/022031 | null | cond-mat.mes-hall cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Effects of a single impurity potential on bulk properties of a spinful
Tomonaga-Luttinger (TL) liquid is studied. A boundary bosonization technique is
developed to include the impurity potential of {\it arbitrary} strength $V$.
Our new bosonization formula for fermion field $\psi$ smoothly connects the two
existing expressions in the strong ($V = \infty$) and the weak ($V = 0$)
impurity limits. With use of the formula, we found the TL parameters determined
from the long-distance correlation functions are renormalized due to the
partial transmission through the impurity potential.
| [{'version': 'v1', 'created': 'Thu, 20 Nov 2008 11:29:43 GMT'}] | 2009-11-13 | [array(['Kamide', 'Kenji', ''], dtype=object)
array(['Kimura', 'Takashi', ''], dtype=object)
array(['Kurihara', 'Susumu', ''], dtype=object)] |
19,747 | 1007.4878 | Francois Louchet | Paul Duval, Francois Louchet, Jerome Weiss and Maurine Montagnat | On the role of long range internal stresses on grain nucleation during
discontinuous recrystallization | 7 pages, 3 figures | null | null | null | cond-mat.mtrl-sci | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The essential role of long range elastic interactions in recrystallization is
demonstrated using a simple analytical model: pileup rearrangements following
absorption of leading dislocations by a dislocation-free embryo provides an
additional driving force that results in a drastic decrease of both the
nucleation critical radius and the saddle point energy. A very sharp transition
is evidenced, at which the saddle point totally disappears and nucleation
becomes spontaneous. This transition occurs for a well defined critical stress
corresponding to both a critical density of geometrically necessary
dislocations and a critical strain, without invoking any critical nucleus size
that may be reached with the help of some dislocation microstructure
instability. The present model is illustrated here by the case of
polycrystalline ice, but may apply to other crystalline material with
significant plastic anisotropy, as Zircaloy for instance.
| [{'version': 'v1', 'created': 'Wed, 28 Jul 2010 07:09:47 GMT'}] | 2010-07-29 | [array(['Duval', 'Paul', ''], dtype=object)
array(['Louchet', 'Francois', ''], dtype=object)
array(['Weiss', 'Jerome', ''], dtype=object)
array(['Montagnat', 'Maurine', ''], dtype=object)] |
19,748 | math/0608170 | Tomasz Brzezinski | Tomasz Brzezinski | Flat connections and (co)modules | 18 pages, LaTeX; significantly expanded with two new sections on
connections in (bi)comodules | null | null | null | math.QA math.RA | null | The relationship between comodules of a coring and flat connections is
reviewed. In particular we specialise to corings which are built on a tensor
product of algebra and a coalgebra. Such corings are in one-to-one
correspondence with entwining structures, and their comodules are entwined
modules. These include Yetter-Drinfeld and anti-Yetter-Drinfeld modules and
their generalisations, hence all the modules of interest to Hopf-cyclic
cohomology. In this way the interpretation of the latter as modules with flat
connections [A Kaygun and M Khalkhali, Hopf modules and noncommutative
differential geometry, Lett. Math. Phys. 76 (2006), 77--91] is obtained as a
corollary of a more general theory. We also introduce the notions of a
connection in a comodule and of a bicomodule connection, and show how comodules
with flat connections can be interpreted as modules of a C-ring. In this way
all the above mentioned Hopf modules can be interpreted as comodules with flat
connections.
| [{'version': 'v1', 'created': 'Mon, 7 Aug 2006 17:40:10 GMT'}
{'version': 'v2', 'created': 'Fri, 19 Jan 2007 13:18:38 GMT'}] | 2007-05-23 | [array(['Brzezinski', 'Tomasz', ''], dtype=object)] |
19,749 | 1506.08201 | Robin Mostardi | Robin E. Mostardi, Alice E. Shapley, Charles C. Steidel, Ryan F.
Trainor, Naveen A. Reddy, Brian Siana | A High-Resolution Hubble Space Telescope Study of Apparent Lyman
Continuum Leakers at $z\sim3$ | 31 pages, 5 tables, 19 figures. Accepted to ApJ. Version with
full-resolution figures is available at:
http://www.astro.ucla.edu/~aes/Mostardi_HST_LyC.pdf | null | 10.1088/0004-637X/810/2/107 | null | astro-ph.GA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present $U_{336}V_{606}J_{125}H_{160}$ follow-up $HST$ observations of 16
$z\sim3$ candidate LyC emitters in the HS1549+1919 field. With these data, we
obtain high spatial-resolution photometric redshifts of all sub-arcsecond
components of the LyC candidates in order to eliminate foreground contamination
and identify robust candidates for leaking LyC emission. Of the 16 candidates,
we find one object with a robust LyC detection that is not due to foreground
contamination. This object (MD5) resolves into two components; we refer to the
LyC-emitting component as MD5b. MD5b has an observed 1500\AA\ to 900\AA\
flux-density ratio of $(F_{UV}/F_{LyC})_{obs}=4.0\pm2.0$, compatible with
predictions from stellar population synthesis models. Assuming minimal IGM
absorption, this ratio corresponds to a relative (absolute) escape fraction of
$f_{esc,rel}^{MD5b}=75-100$% ($f_{esc,abs}^{MD5b}=14-19$%). The stellar
population fit to MD5b indicates an age of $\lesssim50$Myr, which is in the
youngest 10% of the $HST$ sample and the youngest third of typical $z\sim3$
Lyman break galaxies, and may be a contributing factor to its LyC detection. We
obtain a revised, contamination-free estimate for the comoving specific
ionizing emissivity at $z=2.85$, indicating (with large uncertainties) that
star-forming galaxies provide roughly the same contribution as QSOs to the
ionizing background at this redshift. Our results show that foreground
contamination prevents ground-based LyC studies from obtaining a full
understanding of LyC emission from $z\sim3$ star-forming galaxies. Future
progress in direct LyC searches is contingent upon the elimination of
foreground contaminants through high spatial-resolution observations, and upon
acquisition of sufficiently deep LyC imaging to probe ionizing radiation in
high-redshift galaxies.
| [{'version': 'v1', 'created': 'Fri, 26 Jun 2015 20:00:30 GMT'}
{'version': 'v2', 'created': 'Sat, 1 Aug 2015 18:15:35 GMT'}] | 2015-09-16 | [array(['Mostardi', 'Robin E.', ''], dtype=object)
array(['Shapley', 'Alice E.', ''], dtype=object)
array(['Steidel', 'Charles C.', ''], dtype=object)
array(['Trainor', 'Ryan F.', ''], dtype=object)
array(['Reddy', 'Naveen A.', ''], dtype=object)
array(['Siana', 'Brian', ''], dtype=object)] |
19,750 | 1111.6105 | Bing Shen | Bing Shen, Huan Yang, Bin Zeng, Cong Ren, Xibin Xu and Hai-Hu Wen | Multiple Magnetization Peaks and New Type of Vortex Phase Transitions in
Ba0.6K0.4Fe2As2 | 5 page, 5 figures | null | null | null | cond-mat.supr-con | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Magnetization and its relaxation have been measured on Ba0.6K0.4Fe2As2 single
crystals with Tc = 39 K. The magnetization hysteresis loops (MHLs) exhibit flux
jumps in the low temperature region, and a second peak-effect in the
intermediate temperature region, especially when the field sweeping rate is
low. Interestingly a third magnetization peak can be easily observed on the
MHLs in the high temperature region. Further analysis find that the first
magnetization peak is very sharp, which is associated with the strong vortex
pinning. However the first dip of the MHL corresponds to a moderate relaxation
rate, then a second peak appears accompanied by a vanishing vortex motion.
Finally a third magnetization peak emerges and the vortex motion becomes
drastic beyond this threshold. The novel features accompanying the second
magnetization peak suggest a new type of vortex phase transition.
| [{'version': 'v1', 'created': 'Fri, 25 Nov 2011 12:40:15 GMT'}
{'version': 'v2', 'created': 'Wed, 30 Nov 2011 12:08:12 GMT'}] | 2011-12-01 | [array(['Shen', 'Bing', ''], dtype=object)
array(['Yang', 'Huan', ''], dtype=object)
array(['Zeng', 'Bin', ''], dtype=object)
array(['Ren', 'Cong', ''], dtype=object)
array(['Xu', 'Xibin', ''], dtype=object)
array(['Wen', 'Hai-Hu', ''], dtype=object)] |
19,751 | 1107.2127 | Jesse Johnson | Jesse Johnson | An upper bound on common stabilizations of Heegaard splittings | 34 pages, 8 figures | null | null | null | math.GT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that for any two Heegaard splittings of genus $p$ and $q$ for the
same closed 3-manifold, there is a common stabilization of genus at most 3/2 p
+ 2q - 1. One may compare this to recent examples of Heegaard splittings whose
smallest common stabilizations have genus at least $p+q$ or $p + 1/2 q$
depending on the notion of equivalence.
| [{'version': 'v1', 'created': 'Mon, 11 Jul 2011 20:04:49 GMT'}] | 2011-07-13 | [array(['Johnson', 'Jesse', ''], dtype=object)] |
19,752 | 2004.08325 | Frantisek Marko | Frantisek Marko | Symmetrizers for Schur superalgebras | null | null | null | null | math.RA math.CO math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | For the Schur superalgebra $S=S(m|n,r)$ over a ground field $K$ of
characteristic zero, we define symmetrizers $T^{\lambda}[i:j]$ of the ordered
pairs of tableaux $T_i, T_j$ of the shape $\lambda$ and show that the $K$-span
$A_{\lambda,K}$ of all symmetrizers $T^{\lambda}[i:j]$ has a basis consisting
of $T^{\lambda}[i:j]$ for $T_i,T_j$ semistandard. The $S$-superbimodule
$A_{\lambda,K}$ is identified as %$\Delta(\lambda)^*\otimes_K \nabla(\lambda)$,
where $\Delta(\lambda)^*$ is the dual of the standard supermodule %and
$\nabla(\lambda)$ is the costandard supermodule of the highest weight
$\lambda$. $D_{\lambda}\otimes_K D^o_{\lambda}$, where $D_\lambda$ and
$D^o_\lambda$ are left and right irreducible $S$-supermodules of the highest
weight $\lambda$.
We define modified symmetrizers $T^{\lambda}\{i:j\}$ and show that their
$\mathbb{Z}$-span form a $\mathbb{Z}$-form $A_{\lambda,\mathbb{Z}}$ of
$A_{\lambda, \mathbb{Q}}$. We show that every modified symmetrizer
$T^\lambda\{i:j\}$ is a $\mathbb{Z}$-linear combination of symmetrizers
$T^\lambda\{i:j\}$ for $T_i, T_j$ semistandard. Using modular reduction to a
field $K$ of characteristic $p>2$, we obtain that $A_{\lambda,K}$ has a basis
consisting of modified symmetrizers $T^\lambda\{i:j\}$ for $T_i, T_j$
semistandard.
| [{'version': 'v1', 'created': 'Fri, 17 Apr 2020 16:12:45 GMT'}] | 2020-04-20 | [array(['Marko', 'Frantisek', ''], dtype=object)] |
19,753 | 1408.0476 | Meera Parish | Andrea M. Fischer and Meera M. Parish | Quasi-two-dimensional Fermi gases at finite temperature | 8 pages, 4 figures | Phys. Rev. B 90, 214503 (2014) | 10.1103/PhysRevB.90.214503 | null | cond-mat.quant-gas cond-mat.supr-con | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider a Fermi gas with short-range attractive interactions that is
confined along one direction by a tight harmonic potential. For this
quasi-two-dimensional (quasi-2D) Fermi gas, we compute the pressure equation of
state, radio frequency spectrum, and the superfluid critical temperature $T_c$
using a mean-field theory that accounts for all the energy levels of the
harmonic confinement. Our calculation for $T_c$ provides a natural
generalization of the Thouless criterion to the quasi-2D geometry, and it
correctly reduces to the 3D expression derived from the local density
approximation in the limit where the confinement frequency $\omega_z \to 0$.
Furthermore, our results suggest that $T_c$ can be enhanced by relaxing the
confinement and perturbing away from the 2D limit.
| [{'version': 'v1', 'created': 'Sun, 3 Aug 2014 09:35:56 GMT'}] | 2014-12-08 | [array(['Fischer', 'Andrea M.', ''], dtype=object)
array(['Parish', 'Meera M.', ''], dtype=object)] |
19,754 | cond-mat/9907002 | Daphne O. Klemme | Steven M. Girvin (Indiana University) | The Quantum Hall Effect: Novel Excitations and Broken Symmetries | 124 pages. Lectures delivered at Ecole d'Ete Les Houches, July 1998 | Topological Aspects of Low Dimensional Systems, ed. A. Comtet, T.
Jolicoeur, S. Ouvry, F. David (Springer-Verlag, Berlin and Les Editions de
Physique, Les Ulis, 2000) | null | IUCM98-010 | cond-mat.mes-hall | null | These pedagogical lecture notes present a general introduction to most
aspects of the integer and fractional quantum Hall effects. This is followed by
an extensive discussion of quantum Hall ferromagnetism, both for spins in
single-layer systems and `pseudospins' in double-layer systems. The effective
field theories describing various broken symmetry states and `skyrmion' and
`meron' spin textures are derived and discussed in some detail. Pedagogical
presentations on Berry phases and lowest Landau level projection are included
in appendices.
| [{'version': 'v1', 'created': 'Thu, 1 Jul 1999 21:14:59 GMT'}] | 2007-05-23 | [array(['Girvin', 'Steven M.', '', 'Indiana University'], dtype=object)] |
19,755 | 0806.4452 | Yong-Wan Kim | Yun Soo Myung, Yong-Wan Kim, Young-Jai Park | Thermodynamics of Gauss-Bonnet black holes revisited | 22 pages, 8 figures, version to appear in EPJC | Eur.Phys.J.C58:337-346,2008 | 10.1140/epjc/s10052-008-0745-9 | null | gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the Gauss-Bonnet black hole in five dimensional anti-de Sitter
spacetimes (GBAdS). We analyze all thermodynamic quantities of the GBAdS, which
is characterized by the Gauss-Bonnet coupling $c$ and mass $M$, comparing with
those of the Born-Infeld-AdS (BIAdS), Reissner-Norstr\"om-AdS black holes
(RNAdS), Schwarzschild-AdS (SAdS), and BTZ black holes. For $c<0$ we cannot
obtain the black hole with positively definite thermodynamic quantities of
mass, temperature, and entropy because the entropy does not satisfy the
area-law. On the other hand, for $c>0$, we find the BIAdS-like black hole,
showing that the coupling $c$ plays the role of pseudo-charge. Importantly, we
could not obtain the SAdS in the limits of $c\to 0$, which means that the GBAdS
is basically different from the SAdS. In addition, we clarify the connections
between thermodynamic and dynamical stability. Finally, we also conjecture that
if a black hole is big and thus globally stable, its quasinormal modes may take
analytic expressions.
| [{'version': 'v1', 'created': 'Fri, 27 Jun 2008 08:30:55 GMT'}
{'version': 'v2', 'created': 'Wed, 2 Jul 2008 07:23:11 GMT'}
{'version': 'v3', 'created': 'Sat, 27 Sep 2008 15:24:49 GMT'}] | 2008-12-18 | [array(['Myung', 'Yun Soo', ''], dtype=object)
array(['Kim', 'Yong-Wan', ''], dtype=object)
array(['Park', 'Young-Jai', ''], dtype=object)] |
19,756 | 1910.03711 | Bryan Brzycki | Bryan Brzycki, Andrew P. V. Siemion, Steve Croft, Daniel Czech, David
DeBoer, Julia DeMarines, Jamie Drew, J. Emilio Enriquez, Vishal Gajjar,
Nectaria Gizani, Howard Isaacson, Brian C. Lacki, Matt Lebofsky, David H. E.
MacMahon, Imke de Pater, Daniel C. Price, Sofia Z. Sheikh, Claire Webb, S.
Pete Worden | Breakthrough Listen Follow-up of the Random Transiter (EPIC 249706694/HD
139139) with the Green Bank Telescope | 3 pages, 1 table. Accepted for publication in RNAAS | null | null | null | astro-ph.EP astro-ph.IM | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The star EPIC 249706694 (HD 139139) was found to exhibit 28 transit-like
events over an 87 day period during the Kepler mission's K2 Campaign 15
(Rappaport et al. 2019). These events did not fall into an identifiable pattern
and could not be explained by a multitude of transit scenarios explored by the
authors. We conduct follow-up observations at C-band frequencies with the Green
Bank Telescope as part of the ongoing Breakthrough Listen search for
technosignatures. We search for narrow band signals above a signal-to-noise
threshold of 10 and with Doppler drift rates within +-5 Hz/s. We detect no
evidence of technosignatures from EPIC 249706694 and derive an upper limit for
the EIRP (Equivalent Isotropic Radiated Power) of putative transmissions to be
10 TW.
| [{'version': 'v1', 'created': 'Tue, 8 Oct 2019 22:57:00 GMT'}] | 2019-10-10 | [array(['Brzycki', 'Bryan', ''], dtype=object)
array(['Siemion', 'Andrew P. V.', ''], dtype=object)
array(['Croft', 'Steve', ''], dtype=object)
array(['Czech', 'Daniel', ''], dtype=object)
array(['DeBoer', 'David', ''], dtype=object)
array(['DeMarines', 'Julia', ''], dtype=object)
array(['Drew', 'Jamie', ''], dtype=object)
array(['Enriquez', 'J. Emilio', ''], dtype=object)
array(['Gajjar', 'Vishal', ''], dtype=object)
array(['Gizani', 'Nectaria', ''], dtype=object)
array(['Isaacson', 'Howard', ''], dtype=object)
array(['Lacki', 'Brian C.', ''], dtype=object)
array(['Lebofsky', 'Matt', ''], dtype=object)
array(['MacMahon', 'David H. E.', ''], dtype=object)
array(['de Pater', 'Imke', ''], dtype=object)
array(['Price', 'Daniel C.', ''], dtype=object)
array(['Sheikh', 'Sofia Z.', ''], dtype=object)
array(['Webb', 'Claire', ''], dtype=object)
array(['Worden', 'S. Pete', ''], dtype=object)] |
19,757 | nlin/0702013 | Vasyl Gafiychuk | V.Gafiychuk, B.Datsko, V.Meleshko | Nonlinear oscillations and stability domains in fractional
reaction-diffusion systems | 15 pages, 5 figures | null | null | null | nlin.PS nlin.AO | null | We study a fractional reaction-diffusion system with two types of variables:
activator and inhibitor. The interactions between components are modeled by
cubical nonlinearity. Linearization of the system around the homogeneous state
provides information about the stability of the solutions which is quite
different from linear stability analysis of the regular system with integer
derivatives. It is shown that by combining the fractional derivatives index
with the ratio of characteristic times, it is possible to find the marginal
value of the index where the oscillatory instability arises. The increase of
the value of fractional derivative index leads to the time periodic solutions.
The domains of existing of periodic solutions for different parameters of the
problem are obtained. A computer simulation of the corresponding nonlinear
fractional ordinary differential equations is presented. It is established by
computer simulation that there exists a set of stable spatio-temporal tructures
of the one-dimensional system under the Neumann and periodic boundary
condition. The features of these solutions consist in the transformation of the
steady state dissipative structures to homogeneous oscillations or space
temporary structures at a certain value of fractional index and the ratio of
characteristic times of system.
| [{'version': 'v1', 'created': 'Wed, 7 Feb 2007 14:38:33 GMT'}] | 2007-05-23 | [array(['Gafiychuk', 'V.', ''], dtype=object)
array(['Datsko', 'B.', ''], dtype=object)
array(['Meleshko', 'V.', ''], dtype=object)] |
19,758 | 1801.00562 | Masaaki Kimura | Y. Chiba and M. Kimura | Hoyle-analogue state in 13C studied with Antisymmetrized Molecular
Dynamics | null | Phys. Rev. C 101, 024317 (2020) | 10.1103/PhysRevC.101.024317 | null | nucl-th nucl-ex | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The cluster states in $^{13}{\rm C}$ are investigated by antisymmetrized
molecular dynamics. By investigating the spectroscopic factors, the cluster
configurations of the excited states are discussed. It is found that the
$1/2^+_2$ state is dominantly composed of the $^{12}{\rm C}(0^+_2)\otimes
s_{1/2}$ configuration and can be regarded as a Hoyle analogue state. On the
other hand, the p-wave states ($3/2^-$ and $1/2^-$) do not have such structure,
because of the coupling with other configurations. The isoscalar monopole and
dipole transition strengths from the ground to the excited states are also
studied. It is shown that the excited $1/2^-$ states have strong isoscalar
monopole transition strengths consistent with the observation. On the other
hand, the excited $1/2^+$ states unexpectedly have weak isoscalar dipole
transitions except for the $1/2^+_1$ state. It is discussed that the
suppression of the dipole transition is attributed to the property of the
dipole operator.
| [{'version': 'v1', 'created': 'Tue, 2 Jan 2018 07:11:19 GMT'}] | 2020-03-04 | [array(['Chiba', 'Y.', ''], dtype=object)
array(['Kimura', 'M.', ''], dtype=object)] |
19,759 | 1805.07586 | Giuseppe Greco | Sabine Frittella, Giuseppe Greco, Alexander Kurz, Alessandra
Palmigiano, Vlasta Sikimi\'c | Multi-type Display Calculus for Dynamic Epistemic Logic | null | Journal of Logic and Computation, Volume 26, Issue 6, 1 December
2016, Pages 2017--2065 | 10.1093/logcom/exu068 | null | math.LO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the present paper, we introduce a multi-type display calculus for dynamic
epistemic logic, which we refer to as Dynamic Calculus. The display-approach is
suitable to modularly chart the space of dynamic epistemic logics on
weaker-than-classical propositional base. The presence of types endows the
language of the Dynamic Calculus with additional expressivity, allows for a
smooth proof-theoretic treatment, and paves the way towards a general
methodology for the design of proof systems for the generality of dynamic
logics, and certainly beyond dynamic epistemic logic. We prove that the Dynamic
Calculus adequately captures Baltag-Moss-Solecki's dynamic epistemic logic, and
enjoys Belnap-style cut elimination.
| [{'version': 'v1', 'created': 'Sat, 19 May 2018 12:59:37 GMT'}] | 2018-05-22 | [array(['Frittella', 'Sabine', ''], dtype=object)
array(['Greco', 'Giuseppe', ''], dtype=object)
array(['Kurz', 'Alexander', ''], dtype=object)
array(['Palmigiano', 'Alessandra', ''], dtype=object)
array(['Sikimić', 'Vlasta', ''], dtype=object)] |
19,760 | 0708.2271 | Vladislav V. Kravchenko | Vladislav V. Kravchenko | Solution of the equation d/dx(pdu/dx)+qu=cu by a solution of the
equation d/dx(pdu/dx)+qu=0 | null | Published under the title: A representation for solutions of the
Sturm-Liouville equation. Complex Variables and Elliptic Problems, 2008, v.
53, No. 8, 775-789 | null | null | math-ph math.MP | null | We give a simple solution of the equation d/dx(pdu/dx)+qu=cu whenever a
nontrivial solution of d/dx(pdu/dx)+qu=0 is known. The method developed for
obtaining this result is based on the theory of pseudoanalytic functions and
their relationship with solutions of the stationary two-dimensional Schrodinger
equation. The final result, that is the formula for the general solution of the
equation d/dx(pdu/dx)+qu=cu has a simple and easily verifiable form.
| [{'version': 'v1', 'created': 'Thu, 16 Aug 2007 19:44:00 GMT'}
{'version': 'v2', 'created': 'Mon, 7 Jan 2008 17:57:42 GMT'}] | 2010-07-09 | [array(['Kravchenko', 'Vladislav V.', ''], dtype=object)] |
19,761 | 1501.01237 | Jan Verhoeven | Jan Verhoeven, Thomas Wieseh\"ofer, Stephan Stellmach | Anelastic Versus Fully Compressible Turbulent Rayleigh-B\'enard
Convection | 24 pages, 9 figures | null | 10.1088/0004-637X/805/1/62 | null | astro-ph.SR | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Numerical simulations of turbulent Rayleigh-B\'enard convection in an ideal
gas, using either the anelastic approximation or the fully compressible
equations, are compared. Theoretically, the anelastic approximation is expected
to hold in weakly superadiabatic systems with $\epsilon = \Delta T / T_r \ll
1$, where $\Delta T$ denotes the superadiabatic temperature drop over the
convective layer and $T_r$ the bottom temperature. Using direct numerical
simulations, a systematic comparison of anelastic and fully compressible
convection is carried out. With decreasing superadiabaticity $\epsilon$, the
fully compressible results are found to converge linearly to the anelastic
solution with larger density contrasts generally improving the match. We
conclude that in many solar and planetary applications, where the
superadiabaticity is expected to be vanishingly small, results obtained with
the anelastic approximation are in fact more accurate than fully compressible
computations, which typically fail to reach small $\epsilon$ for numerical
reasons. On the other hand, if the astrophysical system studied contains
$\epsilon\sim O(1)$ regions, such as the solar photosphere, fully compressible
simulations have the advantage of capturing the full physics. Interestingly,
even in weakly superadiabatic regions, like the bulk of the solar convection
zone, the errors introduced by using artificially large values for $\epsilon$
for efficiency reasons remain moderate. If quantitative errors of the order of
$10\%$ are acceptable in such low $\epsilon$ regions, our work suggests that
fully compressible simulations can indeed be computationally more efficient
than their anelastic counterparts.
| [{'version': 'v1', 'created': 'Tue, 6 Jan 2015 17:02:24 GMT'}
{'version': 'v2', 'created': 'Fri, 13 Mar 2015 15:10:42 GMT'}] | 2015-05-27 | [array(['Verhoeven', 'Jan', ''], dtype=object)
array(['Wiesehöfer', 'Thomas', ''], dtype=object)
array(['Stellmach', 'Stephan', ''], dtype=object)] |
19,762 | hep-ph/0602148 | Giacomo Morpurgo | G.Dillon and G.Morpurgo | The contribution of strange quarks to the proton magnetic moment | 11 pages, 1 eps figure | null | null | GEF-TH-02/2006 | hep-ph | null | This paper deals with how to extract the s-s(bar) contribution to the proton
magnetic moment from the experiments
| [{'version': 'v1', 'created': 'Thu, 16 Feb 2006 11:46:22 GMT'}
{'version': 'v2', 'created': 'Mon, 20 Feb 2006 11:15:08 GMT'}] | 2007-05-23 | [array(['Dillon', 'G.', ''], dtype=object)
array(['Morpurgo', 'G.', ''], dtype=object)] |
19,763 | 1812.08251 | Jimmy Mc Laughlin | Doug Bowman and James Mc Laughlin | Polynomial Continued Fractions | 13 pages | Acta Arith. 103 (2002), no. 4, 329--342 | 10.4064/aa103-4-3 | null | math.NT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Continued fractions whose elements are polynomial sequences have been
carefully studied mostly in the cases where the degree of the numerator
polynomial is less than or equal to two and the degree of the denominator
polynomial is less than or equal to one. Here we study cases of higher degree
for both numerator and denominator polynomials, with particular attention given
to cases in which the degrees are equal. We extend work of Ramanujan on
continued fractions with rational limits and also consider cases where the
limits are irrational.
| [{'version': 'v1', 'created': 'Wed, 19 Dec 2018 21:28:02 GMT'}] | 2018-12-26 | [array(['Bowman', 'Doug', ''], dtype=object)
array(['Laughlin', 'James Mc', ''], dtype=object)] |
19,764 | 1410.1219 | Jonathan Rollin | Maria Axenovich, Jonathan Rollin | Brooks Type Results for Conflict-Free Colorings and {a, b}-factors in
graphs | Fixed typos in statement of Theorem 7; 9 pages, 1 figure | Discrete Mathematics 338(12):2295--2301, 2015 | null | null | math.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A vertex-coloring of a hypergraph is conflict-free, if each edge contains a
vertex whose color is not repeated on any other vertex of that edge. Let $f(r,
\Delta)$ be the smallest integer $k$ such that each $r$-uniform hypergraph of
maximum vertex degree $\Delta$ has a conflict-free coloring with at most $k$
colors. As shown by Tardos and Pach, similarly to a classical Brooks' type
theorem for hypergraphs, $f(r, \Delta)\leq \Delta+1$. Compared to Brooks'
theorem, according to which there is only a couple of graphs/hypergraphs that
attain the $\Delta+1$ bound, we show that there are several infinite classes of
uniform hypergraphs for which the upper bound is attained. We provide bounds on
$f(r, \Delta)$ in terms of~$\Delta$ for large~$\Delta$ and establish the
connection between conflict-free colorings and so-called $\{t, r-t\}$-factors
in $r$-regular graphs. Here, a $\{t, r-t\}$-factor is a factor in which each
degree is either $t$ or $r-t$. Among others, we disprove a conjecture of Akbari
and Kano~[Graphs and Combinatorics 30(4):821--826, 2014] stating that there is
a $\{t,r-t\}$-factor in every $r$-regular graph for odd $r$ and any odd
$t<\frac{r}{3}$.
| [{'version': 'v1', 'created': 'Sun, 5 Oct 2014 22:47:53 GMT'}
{'version': 'v2', 'created': 'Mon, 5 Dec 2016 10:35:21 GMT'}] | 2016-12-06 | [array(['Axenovich', 'Maria', ''], dtype=object)
array(['Rollin', 'Jonathan', ''], dtype=object)] |
19,765 | 1307.0330 | Mohammad Hassan Vahidinia | M. H. Dehghani, M. H. Vahidinia | Quartic Quasi-topological Gravity, Black Holes and Holography | 27 pages, 14 figures, minor typos corrected, a comment on bulk
causality is added, updated to published version | JHEP, 10(2013)210 | 10.1007/JHEP10(2013)210 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we derive the field equations of quartic quasi-topological
gravity by varying the action with respect to the metric. Also, we obtain the
linearized graviton equations in the AdS background and find that it is
governed by a second-order field equation as in the cases of Einstein, Lovelock
or cubic quasi-topological gravities. But in contrast to the cubic
quasi-topological gravity, the linearized field equation around a black hole
has fourth-order radial derivative of the perturbation. Moreover, we analyze
the conditions of having ghost free AdS solutions and AdS planar black holes.
In addition, we compute the central charges of the dual conformal field theory
of this gravity theory by studying holographic Weyl anomaly. Finally, we
consider the effect of quartic term on the causality of dual theory in the
tensor channel and show that, in the contrast to the trivial result of cubic
quasi-topological gravity, the existence of both cubic and quartic terms leads
to a non-trivial constraint. However, this constraint does not imply any lower
positive bound on the viscosity/entropy ratio.
| [{'version': 'v1', 'created': 'Mon, 1 Jul 2013 10:56:07 GMT'}
{'version': 'v2', 'created': 'Mon, 11 Nov 2013 09:10:14 GMT'}] | 2013-11-12 | [array(['Dehghani', 'M. H.', ''], dtype=object)
array(['Vahidinia', 'M. H.', ''], dtype=object)] |
19,766 | 1802.08918 | Linyuan Lu | Linyuan Lu and Zhiyu Wang | Anti-Ramsey number of edge-disjoint rainbow spanning trees | 17 pages, fixed an error in the proof of Theorem 3 using Matroid
methods | null | null | null | math.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | An edge-colored graph $G$ is called rainbow if every edge of $G$ receives a
different color. The anti-Ramsey number of $t$ edge-disjoint rainbow spanning
trees, denoted by $r(n,t)$, is defined as the maximum number of colors in an
edge-coloring of $K_n$ containing no $t$ edge-disjoint rainbow spanning trees.
Jahanbekam and West [J. Graph Theory, 2014] conjectured that for any fixed $t$,
$r(n,t)=\binom{n-2}{2}+t$ whenever $n\geq 2t+2 \geq 6$. In this paper, we prove
this conjecture. We also determine $r(n,t)$ when $n = 2t+1$. Together with
previous results, this gives the anti-Ramsey number of $t$ edge-disjoint
rainbow spanning trees for all values of $n$ and $t$.
| [{'version': 'v1', 'created': 'Sat, 24 Feb 2018 21:37:07 GMT'}
{'version': 'v2', 'created': 'Thu, 14 Nov 2019 15:45:16 GMT'}
{'version': 'v3', 'created': 'Sat, 16 Nov 2019 20:46:32 GMT'}] | 2019-11-19 | [array(['Lu', 'Linyuan', ''], dtype=object)
array(['Wang', 'Zhiyu', ''], dtype=object)] |
19,767 | 2204.02750 | Yuzhi Shi Prof. | Yuzhi Shi, Qinghua Song, Ivan Toftul, Tongtong Zhu, Yefeng Yu, Weiming
Zhu, Din Ping Tsai, Yuri Kivshar and Ai Qun Liu | Optical manipulation with metamaterial structures | 49 pages, 5 figures | null | null | null | physics.optics physics.app-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Optical tweezers employing forces produced by light underpin important
manipulation tools in many areas of applied and biological physics.
Conventional optical tweezers are based on refractive optics, and they require
excessive auxiliary optical elements to reshape both amplitude and phase, as
well as wavevector and angular momentum of light, and thus impose limitations
to the overall cost and integration of optical systems. Metamaterials provide
both electric and optically induced magnetic response in subwavelength optical
structures, and they are highly beneficial to achieve unprecedented control of
light required for many applications, also opening new opportunities for
optical manipulation. Here, we review the recent advances in the field of
optical tweezers employing the physics and concepts of metamaterials (the
so-called meta-tweezers) and demonstrate that metamaterial structures could not
only advance classical operations with particles, such as trapping,
transporting, and sorting, but they uncover exotic optical forces such as
pulling and lateral forces. Remarkably, apart from manipulation of particles,
metastructures can be powered dynamically by light to realize ingenious
meta-robots. We provide an outlook for future opportunities in this area
ranging from enhanced particle manipulation to meta-robot actuation.
| [{'version': 'v1', 'created': 'Wed, 6 Apr 2022 11:49:03 GMT'}] | 2022-04-07 | [array(['Shi', 'Yuzhi', ''], dtype=object)
array(['Song', 'Qinghua', ''], dtype=object)
array(['Toftul', 'Ivan', ''], dtype=object)
array(['Zhu', 'Tongtong', ''], dtype=object)
array(['Yu', 'Yefeng', ''], dtype=object)
array(['Zhu', 'Weiming', ''], dtype=object)
array(['Tsai', 'Din Ping', ''], dtype=object)
array(['Kivshar', 'Yuri', ''], dtype=object)
array(['Liu', 'Ai Qun', ''], dtype=object)] |
19,768 | 2010.00859 | Kim Myung-Whun | Purevdorj Munkhbaatar and Kim Myung-Whun | Origin of the mid-infrared peaks in the optical conductivity of
LaMnO$_{3}$ | 10 pages, 3 figures | null | 10.1016/j.ssc.2021.114381 | null | cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We calculated the infrared conductivity spectrum of orbitally ordered
LaMnO$_3$ in phonon frequency and overtone frequency ranges. We considered
orbital exchange, Jahn-Teller electron-phonon coupling, and phonon--phonon
coupling. The fundamental excitation of the phonon-coupled orbiton was only
Raman active, not infrared active, while its overtone modes were both Raman and
infrared active. Our calculations reproduced the small peaks near 1300
cm$^{-1}$ observed both in Raman scattering and infrared conductivity spectra,
as consistent with previous experimental results.
| [{'version': 'v1', 'created': 'Fri, 2 Oct 2020 08:41:21 GMT'}
{'version': 'v2', 'created': 'Sat, 15 May 2021 03:07:47 GMT'}] | 2021-06-30 | [array(['Munkhbaatar', 'Purevdorj', ''], dtype=object)
array(['Myung-Whun', 'Kim', ''], dtype=object)] |
19,769 | 1609.06804 | Zhouyuan Huo | Zhouyuan Huo, Bin Gu, Heng Huang | Decoupled Asynchronous Proximal Stochastic Gradient Descent with
Variance Reduction | null | null | null | null | cs.LG math.OC | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the era of big data, optimizing large scale machine learning problems
becomes a challenging task and draws significant attention. Asynchronous
optimization algorithms come out as a promising solution. Recently, decoupled
asynchronous proximal stochastic gradient descent (DAP-SGD) is proposed to
minimize a composite function. It is claimed to be able to off-loads the
computation bottleneck from server to workers by allowing workers to evaluate
the proximal operators, therefore, server just need to do element-wise
operations. However, it still suffers from slow convergence rate because of the
variance of stochastic gradient is nonzero. In this paper, we propose a faster
method, decoupled asynchronous proximal stochastic variance reduced gradient
descent method (DAP-SVRG). We prove that our method has linear convergence for
strongly convex problem. Large-scale experiments are also conducted in this
paper, and results demonstrate our theoretical analysis.
| [{'version': 'v1', 'created': 'Thu, 22 Sep 2016 02:50:09 GMT'}
{'version': 'v2', 'created': 'Thu, 29 Sep 2016 01:54:25 GMT'}] | 2016-09-30 | [array(['Huo', 'Zhouyuan', ''], dtype=object)
array(['Gu', 'Bin', ''], dtype=object)
array(['Huang', 'Heng', ''], dtype=object)] |
19,770 | 1812.08117 | Daniel Ruprecht | Krasymyr Tretiak and Daniel Ruprecht | An arbitrary order time-stepping algorithm for tracking particles in
inhomogeneous magnetic fields | null | Journal of Computational Physics: X 4, pp. 100036, 2019 | 10.1016/j.jcpx.2019.100036 | null | math.NA cs.CE cs.NA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Lorentz equations describe the motion of electrically charged particles
in electric and magnetic fields and are used widely in plasma physics. The most
popular numerical algorithm for solving them is the Boris method, a variant of
the St\"ormer-Verlet algorithm. Boris' method is phase space volume conserving
and simulated particles typically remain near the correct trajectory. However,
it is only second order accurate. Therefore, in scenarios where it is not
enough to know that a particle stays on the right trajectory but one needs to
know where on the trajectory the particle is at a given time, Boris method
requires very small time steps to deliver accurate phase information, making it
computationally expensive. We derive an improved version of the high-order
Boris spectral deferred correction algorithm (Boris-SDC) by adopting a
convergence acceleration strategy for second order problems based on the
Generalised Minimum Residual (GMRES) method. Our new algorithm is easy to
implement as it still relies on the standard Boris method. Like Boris-SDC it
can deliver arbitrary order of accuracy through simple changes of runtime
parameter but possesses better long-term energy stability. We demonstrate for
two examples, a magnetic mirror trap and the Solev'ev equilibrium, that the new
method can deliver better accuracy at lower computational cost compared to the
standard Boris method. While our examples are motivated by tracking ions in the
magnetic field of a nuclear fusion reactor, the introduced algorithm can
potentially deliver similar improvements in efficiency for other applications.
| [{'version': 'v1', 'created': 'Wed, 19 Dec 2018 17:51:23 GMT'}
{'version': 'v2', 'created': 'Fri, 2 Aug 2019 08:29:03 GMT'}] | 2019-09-17 | [array(['Tretiak', 'Krasymyr', ''], dtype=object)
array(['Ruprecht', 'Daniel', ''], dtype=object)] |
19,771 | 1111.5822 | Ivan Katkov | Ivan Yu. Katkov and Igor V. Chilingarian | Multi-component parametric inversion of galaxy kinematics and stellar
populations using full spectral fitting | 3 pages, 2 figures; to appear in the proceedings of "The Spectral
Energy Distribution of Galaxies", Preston, UK, 5-9 September 2011 | null | 10.1017/S1743921312008770 | null | astro-ph.IM | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The stellar line-of-sight velocity distribution (LOSVD) can be strongly
asymmetric in regions where the light contributions of both disc and bulge in
spiral and lenticular galaxies are comparable. Existing techniques for the
stellar kinematics analysis do not take into account the difference of disc and
bulge stellar populations. Here we present a novel approach to the analysis of
stellar kinematics and stellar populations. We use a two-component model of
spectra where different stellar population components are convolved with pure
Gaussian LOSVDs. For this model we present Monte-Carlo simulations
demonstrating degeneracies between the parameters.
| [{'version': 'v1', 'created': 'Thu, 24 Nov 2011 17:35:29 GMT'}] | 2015-06-03 | [array(['Katkov', 'Ivan Yu.', ''], dtype=object)
array(['Chilingarian', 'Igor V.', ''], dtype=object)] |
19,772 | 2001.04403 | Craig Lent | Craig S. Lent | Blind witnesses quench quantum interference without transfer of
which-path information | 6 Figures | Entropy 22, 776 (2020) | 10.3390/e22070776 | null | quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We model the fundamental behavior of a two-branch quantum interference
device. Quantum interference oscillations are visible in the output as the
magnetic flux through the paths is varied. Multiple witness systems are
field-coupled to each branch. Each witness state entangles with the device
state, but for our {\em blind} witnesses which-path information is not
transferred to the quantum state of witnesses--they cannot "see" or make a
record of which path is traversed. Yet the presence of these minimal witnesses
rapidly quenches quantum interference. Thus, it is not the imprinting of
which-path information in the witness states that is essential for decoherence,
but simply the entanglement that embeds the device degrees of freedom in the
larger Hilbert space that includes the witnesses. The loss of interference
visibility can be understood as the result of phase cancellations from
different paths through the larger state space.
| [{'version': 'v1', 'created': 'Mon, 13 Jan 2020 17:09:36 GMT'}] | 2022-03-31 | [array(['Lent', 'Craig S.', ''], dtype=object)] |
19,773 | 1112.3958 | Jay Strader | Jay Strader, Anil C. Seth, Nelson Caldwell | Old Massive Globular Clusters and the Stellar Halo of the Dwarf
Starburst Galaxy NGC 4449 | 15 pages, AJ in press | null | 10.1088/0004-6256/143/2/52 | null | astro-ph.CO astro-ph.GA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use Hubble Space Telescope imaging to show that the nearby dwarf starburst
galaxy NGC 4449 has an unusual abundance of luminous red star clusters. Joint
constraints from integrated photometry, low-resolution spectroscopy, dynamical
mass-to-light ratios, and resolved color-magnitude diagrams provide evidence
that some of these clusters are old globular clusters. Spectroscopic data for
two massive clusters suggest intermediate metallicities ([Fe/H] ~ -1) and
subsolar Mg enhancement ([Mg/Fe] ~ -0.1 to -0.2). One of these clusters may be
the nucleus of a tidally disrupting dwarf galaxy; the other is very massive (~
3 x 10^6 M_sun). We have also identified a population of remote halo globular
clusters. NGC 4449 is consistent with an emerging picture of the ubiquity of
stellar halos among dwarf galaxies, and study of its globular clusters may help
distinguish between accretion and in situ scenarios for such halos.
| [{'version': 'v1', 'created': 'Fri, 16 Dec 2011 21:00:00 GMT'}] | 2015-06-03 | [array(['Strader', 'Jay', ''], dtype=object)
array(['Seth', 'Anil C.', ''], dtype=object)
array(['Caldwell', 'Nelson', ''], dtype=object)] |
19,774 | quant-ph/9704035 | Larry Ford | L.H. Ford | Electromagnetic Vacuum Fluctuations and Electron Coherence II: Effects
of Wavepacket Size | 16 pages, Latex, 3 figures, uses epsf | Phys.Rev. A56 (1997) 1812-1818 | 10.1103/PhysRevA.56.1812 | TUTP-97-5 | quant-ph hep-th | null | If one analyzes the effects of electromagnetic vacuum fluctuations upon an
electron interference pattern in an approximation in which the electrons follow
classical trajectories, an ultraviolet divergence results. It is shown that
this divergence is an artifact of the classical trajectory approximation, and
is absent when the finite sizes of electron wavepackets are accounted for. It
is shown that the vacuum fluctuation effect has a logarithmic dependence upon
the wavepacket size. However, at least in one model geometry, this dependence
cancels when one includes both vacuum fluctuation and photon emission effects.
| [{'version': 'v1', 'created': 'Thu, 17 Apr 1997 17:05:23 GMT'}] | 2009-10-30 | [array(['Ford', 'L. H.', ''], dtype=object)] |
19,775 | 1711.08244 | Ambrish Rawat | Ambrish Rawat, Martin Wistuba, Maria-Irina Nicolae | Adversarial Phenomenon in the Eyes of Bayesian Deep Learning | 13 pages, 7 figures | null | null | null | stat.ML cs.LG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Deep Learning models are vulnerable to adversarial examples, i.e.\ images
obtained via deliberate imperceptible perturbations, such that the model
misclassifies them with high confidence. However, class confidence by itself is
an incomplete picture of uncertainty. We therefore use principled Bayesian
methods to capture model uncertainty in prediction for observing adversarial
misclassification. We provide an extensive study with different Bayesian neural
networks attacked in both white-box and black-box setups. The behaviour of the
networks for noise, attacks and clean test data is compared. We observe that
Bayesian neural networks are uncertain in their predictions for adversarial
perturbations, a behaviour similar to the one observed for random Gaussian
perturbations. Thus, we conclude that Bayesian neural networks can be
considered for detecting adversarial examples.
| [{'version': 'v1', 'created': 'Wed, 22 Nov 2017 12:02:53 GMT'}] | 2017-11-23 | [array(['Rawat', 'Ambrish', ''], dtype=object)
array(['Wistuba', 'Martin', ''], dtype=object)
array(['Nicolae', 'Maria-Irina', ''], dtype=object)] |
19,776 | 0704.2982 | Michele Pestalozzi PhD | Michele Pestalozzi | Methanol masers as tools to study high-mass star formation | 8 pages, invited talk at the IAU Symposium 242, "Astrophysical masers
and their environment" | null | 10.1017/S1743921307012628 | null | astro-ph | null | In this contribution I will attempt to show that the study of galactic 6.7
and 12.2GHz methanol masers themselves, as opposed to the use of methanol
masers as signposts, can yield important conclusions contributing to the
understanding of high-mass star formation. Due to their exclusive association
with star formation, methanol masers are the best tools to do this, and their
large number allows to probe the entire Galaxy. In particular I will focus on
the determination of the luminosity function of methanol masers and on the
determination of an unambiguous signature for a circumstellar masing disc seen
edge-on. Finally I will try to point out some future fields of research in the
study of methanol masers.
| [{'version': 'v1', 'created': 'Mon, 23 Apr 2007 11:56:57 GMT'}] | 2009-11-13 | [array(['Pestalozzi', 'Michele', ''], dtype=object)] |
19,777 | 1207.3120 | Seddik Djouadi Dr. | Seddik M. Djouadi | Optimal Disturbance Rejection and Robustness for Infinite Dimensional
LTV Systems | 30 pages, 1 figure | null | null | null | math.OC | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we consider the optimal disturbance rejection problem for
possibly infinite dimensional linear time-varying (LTV) systems using a
framework based on operator algebras of classes of bounded linear operators.
This approach does not assume any state space representation and views LTV
systems as causal operators. After reducing the problem to a shortest distance
minimization in a space of bounded linear operators, duality theory is applied
to show existence of optimal solutions, which satisfy a "time-varying" allpass
or flatness condition. Under mild assumptions the optimal TV controller is
shown to be essentially unique. Next, the concept of M-ideals of operators is
used to show that the computation of time-varying (TV) controllers reduces to a
search over compact TV Youla parameters. This involves the norm of a TV compact
Hankel operator defined on the space of causal trace-class 2 operators and its
maximal vectors. Moreover, an operator identity to compute the optimal TV Youla
parameter is provided. These results are generalized to the mixed sensitivity
problem for TV systems as well, where it is shown that the optimum is equal to
the operator induced of a TV mixed Hankel-Toeplitz. The final outcome of the
approach developed here is that it leads to two tractable finite dimensional
convex optimizations producing estimates to the optimum within desired
tolerances, and a method to compute optimal time-varying controllers.
| [{'version': 'v1', 'created': 'Thu, 12 Jul 2012 23:26:57 GMT'}] | 2012-07-16 | [array(['Djouadi', 'Seddik M.', ''], dtype=object)] |
19,778 | cond-mat/9911140 | Bruno Bassetti | B.Bassetti, M.Cosentino Lagomarsino, P.Jona | A Model for the Self-Organization of Microtubules Driven by Molecular
Motors | 23 pages, 10 figures, LaTeX, eps | null | 10.1007/s100510051150 | null | cond-mat.stat-mech | null | We propose a two-dimensional model for the organization of stabilized
microtubules driven by molecular motors in an unconfined geometry. In this
model two kinds of dynamics are competing. The first one is purely diffusive,
with an interaction between the rotational degrees of freedom, the second one
is a local drive, dependent on microtubule polarity. As a result, there is a
configuration dependent driving field. Applying a molecular field
approximation, we are able to derive continuum equations. A study on the
solutions shows nonequilibrium steady states. The presence and stability of
such self-organized states are investigated in terms of entropy production.
Numerical simulations confirm analytical results.
| [{'version': 'v1', 'created': 'Wed, 10 Nov 1999 14:26:44 GMT'}] | 2019-08-17 | [array(['Bassetti', 'B.', ''], dtype=object)
array(['Lagomarsino', 'M. Cosentino', ''], dtype=object)
array(['Jona', 'P.', ''], dtype=object)] |
19,779 | math/0202136 | James Allen Fill | Keith Crank (National Science Foundation), James Allen Fill (Johns
Hopkins Univ.) | Interruptible exact sampling in the passive case | 17 pages. See also http://www.mts.jhu.edu/~fill/ . To be submitted
for publication in spring, 2002 | null | null | 632, Department of Mathematical Sciences, The Johns Hopkins
University | math.PR math.ST stat.TH | null | We establish, for various scenarios, whether or not interruptible exact
stationary sampling is possible when a finite-state Markov chain can only be
viewed passively. In particular, we prove that such sampling is not possible
using a single copy of the chain. Such sampling is possible when enough copies
of the chain are available, and we provide an algorithm that terminates with
probability one.
| [{'version': 'v1', 'created': 'Thu, 14 Feb 2002 20:51:17 GMT'}] | 2007-06-13 | [array(['Crank', 'Keith', '', 'National Science Foundation'], dtype=object)
array(['Fill', 'James Allen', '', 'Johns\n Hopkins Univ.'], dtype=object)] |
19,780 | 2203.12437 | Oliver Keszocze | Jan Sommer, M. Akif \"Ozkan, Oliver Keszocze, J\"urgen Teich | Efficient Hardware Acceleration of Sparsely Active Convolutional Spiking
Neural Networks | 12 pages, 12 figures, 5 tables, submitted to CODES 2022 | null | 10.1109/TCAD.2022.3197512 | null | cs.AR cs.NE | http://creativecommons.org/licenses/by/4.0/ | Spiking Neural Networks (SNNs) compute in an event-based matter to achieve a
more efficient computation than standard Neural Networks. In SNNs, neuronal
outputs (i.e. activations) are not encoded with real-valued activations but
with sequences of binary spikes. The motivation of using SNNs over conventional
neural networks is rooted in the special computational aspects of SNNs,
especially the very high degree of sparsity of neural output activations. Well
established architectures for conventional Convolutional Neural Networks (CNNs)
feature large spatial arrays of Processing Elements (PEs) that remain highly
underutilized in the face of activation sparsity. We propose a novel
architecture that is optimized for the processing of Convolutional SNNs (CSNNs)
that feature a high degree of activation sparsity. In our architecture, the
main strategy is to use less but highly utilized PEs. The PE array used to
perform the convolution is only as large as the kernel size, allowing all PEs
to be active as long as there are spikes to process. This constant flow of
spikes is ensured by compressing the feature maps (i.e. the activations) into
queues that can then be processed spike by spike. This compression is performed
in run-time using dedicated circuitry, leading to a self-timed scheduling. This
allows the processing time to scale directly with the number of spikes. A novel
memory organization scheme called memory interlacing is used to efficiently
store and retrieve the membrane potentials of the individual neurons using
multiple small parallel on-chip RAMs. Each RAM is hardwired to its PE, reducing
switching circuitry and allowing RAMs to be located in close proximity to the
respective PE. We implemented the proposed architecture on an FPGA and achieved
a significant speedup compared to other implementations while needing less
hardware resources and maintaining a lower energy consumption.
| [{'version': 'v1', 'created': 'Wed, 23 Mar 2022 14:18:58 GMT'}] | 2023-06-23 | [array(['Sommer', 'Jan', ''], dtype=object)
array(['Özkan', 'M. Akif', ''], dtype=object)
array(['Keszocze', 'Oliver', ''], dtype=object)
array(['Teich', 'Jürgen', ''], dtype=object)] |
19,781 | quant-ph/0603076 | Pawel Maslanka | Bartosz Zielinski, Magdalena Zych | A generalization of Margolus-Levitin bound | 6 pages, no figures; some comments added; final version accepted for
publication in Phys. Rev. A | null | 10.1103/PhysRevA.74.034301 | null | quant-ph | null | The Margolus-Levitin lower bound on minimal time required for a state to be
transformed into an orthogonal state is generalized. It is shown that for some
initial states new bound is stronger than the Margolus-Levitin one.
| [{'version': 'v1', 'created': 'Thu, 9 Mar 2006 12:49:11 GMT'}
{'version': 'v2', 'created': 'Fri, 10 Mar 2006 10:05:47 GMT'}
{'version': 'v3', 'created': 'Wed, 17 May 2006 13:10:13 GMT'}
{'version': 'v4', 'created': 'Fri, 18 Aug 2006 12:45:53 GMT'}] | 2009-11-13 | [array(['Zielinski', 'Bartosz', ''], dtype=object)
array(['Zych', 'Magdalena', ''], dtype=object)] |
19,782 | 2112.14293 | Babak Seradjeh | Alan Kostelecky, Ralf Lehnert, Navin McGinnis, Marco Schreck, Babak
Seradjeh | Lorentz violation in Dirac and Weyl semimetals | 18 pages, 7 figures. We welcome all feedback! | Physical Review Research 4, 023106 (2022) | 10.1103/PhysRevResearch.4.023106 | null | cond-mat.mes-hall cond-mat.mtrl-sci cond-mat.str-el hep-ph hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose a correspondence between the description of emergent Lorentz
symmetry in condensed-matter systems and the established general effective
field theory for Lorentz violation in fundamental theories of spacetime and
matter. This correspondence has potential implications in both directions. We
illustrate the proposal by investigating its consequences for the spectral and
transport properties of Dirac and Weyl semimetals. Particular realizations of
this framework give rise to Dirac nodal spectra with nodal lines and rings. We
demonstrate a bulk-boundary correspondence between bulk topological invariants
and drumhead surface states of these Dirac nodal semimetals. We calculate their
transport coefficients in leading-order perturbation theory, thereby
characterizing the unconventional electromagnetic response due to small
deviations from emergent Lorentz invariance. Some prospective future
applications of the correspondence are outlined.
| [{'version': 'v1', 'created': 'Tue, 28 Dec 2021 20:52:43 GMT'}] | 2022-07-08 | [array(['Kostelecky', 'Alan', ''], dtype=object)
array(['Lehnert', 'Ralf', ''], dtype=object)
array(['McGinnis', 'Navin', ''], dtype=object)
array(['Schreck', 'Marco', ''], dtype=object)
array(['Seradjeh', 'Babak', ''], dtype=object)] |
19,783 | 1807.00715 | Avinash Surendran Mr. | Avinash Surendran, Mahesh P. Burse, A. N. Ramaprakash, Padmakar S.
Parihar | Scalable Platform for Adaptive optics Real-time Control (SPARC) Part 2:
Field Programmable Gate Array (FPGA) implementation and performance | 19 pages, 6 figures, accepted in JATIS (SPIE) | null | 10.1117/1.JATIS.4.3.039002 | null | astro-ph.IM | http://creativecommons.org/licenses/by/4.0/ | The next generation of Adaptive Optics (AO) systems on large telescopes will
require immense computation performance and memory bandwidth, both of which are
challenging with the technology available today. The objective of this work is
to create a future-proof adaptive optics platform on an FPGA architecture,
which scales with the number of subapertures, pixels per subaperture and
external memory. We have created a scalable adaptive optics platform with an
off-the-shelf FPGA development board, which provides an AO reconstruction time
only limited by the external memory bandwidth. SPARC uses the same logic
resources irrespective of the number of subapertures in the AO system. This
paper is aimed at embedded developers who are interested in the FPGA design and
the accompanying hardware interfaces. The central theme of this paper is to
show how scalability is incorporated at different levels of the FPGA
implementation. This work is a continuation of Part 1 of the paper which
explains the concept, objectives, control scheme and method of validation used
for testing the platform.
| [{'version': 'v1', 'created': 'Mon, 2 Jul 2018 14:44:31 GMT'}] | 2018-08-03 | [array(['Surendran', 'Avinash', ''], dtype=object)
array(['Burse', 'Mahesh P.', ''], dtype=object)
array(['Ramaprakash', 'A. N.', ''], dtype=object)
array(['Parihar', 'Padmakar S.', ''], dtype=object)] |
19,784 | 2303.15794 | Kana Moriwaki | Kana Moriwaki, Takahiro Nishimichi, Naoki Yoshida | Machine Learning for Observational Cosmology | 55 pages, 8 figures, accepted for publication in Reports on Progress
in Physics | null | 10.1088/1361-6633/acd2ea | YITP-23-40 | astro-ph.IM astro-ph.CO astro-ph.GA astro-ph.HE | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | An array of large observational programs using ground-based and space-borne
telescopes is planned in the next decade. The forthcoming wide-field sky
surveys are expected to deliver a sheer volume of data exceeding an exabyte.
Processing the large amount of multiplex astronomical data is technically
challenging, and fully automated technologies based on machine learning and
artificial intelligence are urgently needed. Maximizing scientific returns from
the big data requires community-wide efforts. We summarize recent progress in
machine learning applications in observational cosmology. We also address
crucial issues in high-performance computing that are needed for the data
processing and statistical analysis.
| [{'version': 'v1', 'created': 'Tue, 28 Mar 2023 07:59:04 GMT'}
{'version': 'v2', 'created': 'Thu, 25 May 2023 06:44:05 GMT'}] | 2023-05-26 | [array(['Moriwaki', 'Kana', ''], dtype=object)
array(['Nishimichi', 'Takahiro', ''], dtype=object)
array(['Yoshida', 'Naoki', ''], dtype=object)] |
19,785 | 2210.13809 | Yuuki Shida | Yuuki Shida and Masami Sugawara and Ryosuke Tsumura and Haruaki Chiba
and Tokuhisa Uejima and Hiroyasu Iwata | Diagnostic Posture Control System for Seated-Style Echocardiography
Robot | null | null | null | null | cs.RO | http://creativecommons.org/licenses/by/4.0/ | Purpose: Conventional robotic ultrasound systems were utilized with patients
in supine positions. Meanwhile, the limitation of the systems is that it is
difficult to evacuate the patients in case of emergency (e.g., patient
discomfort and system failure) because the patients are restricted between the
robot system and bed. Then, it is ideal that the patient undergoes the
examination in the sitting position in terms of safety. Therefore, we validated
a feasibility study of seated-style echocardiography using a robot. Method:
Preliminary experiments were conducted to verify the following two points: (1)
the possibility of obtaining cardiac disease features in the sitting posture as
well as in the conventional examination, and (2) the relationship between
posture angle and physical burden. For reducing the physical burden, two unique
mechanisms were incorporated into the system: (1) a leg pendulum base mechanism
to reduce the load on the legs when the lateral bending angle increases, and
(2) a roll angle division by a lumbar lateral bending and thoracic rotation
mechanisms. Results: Preliminary results demonstrated that adjusting the
diagnostic posture angle enabled us to obtain the views, including cardiac
disease features, as in the conventional examination. The results showed that
the body burden increased as the posture's lateral bending angle increased. The
results also demonstrated that the body load reduction mechanism incorporated
in the results could reduce the physical load in the seated echocardiography.
Conclusion: These results showed the potential of the seated-style
echocardiography robot.
| [{'version': 'v1', 'created': 'Tue, 25 Oct 2022 07:35:42 GMT'}] | 2022-10-26 | [array(['Shida', 'Yuuki', ''], dtype=object)
array(['Sugawara', 'Masami', ''], dtype=object)
array(['Tsumura', 'Ryosuke', ''], dtype=object)
array(['Chiba', 'Haruaki', ''], dtype=object)
array(['Uejima', 'Tokuhisa', ''], dtype=object)
array(['Iwata', 'Hiroyasu', ''], dtype=object)] |
19,786 | 1906.09037 | Xintao Huan | Xintao Huan, Kyeong Soo Kim, Sanghyuk Lee, Eng Gee Lim, Alan Marshall | A Beaconless Asymmetric Energy-Efficient Time Synchronization Scheme for
Resource-Constrained Multi-Hop Wireless Sensor Networks | 12 pages, 16 figures | null | null | null | cs.NI cs.PF | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The ever-increasing number of WSN deployments based on a large number of
battery-powered, low-cost sensor nodes, which are limited in their computing
and power resources, puts the focus of WSN time synchronization research on
three major aspects, i.e., accuracy, energy consumption and computational
complexity. In the literature, the latter two aspects have not received much
attention compared to the accuracy of WSN time synchronization. Especially in
multi-hop WSNs, intermediate gateway nodes are overloaded with tasks for not
only relaying messages but also a variety of computations for their offspring
nodes as well as themselves. Therefore, not only minimizing the energy
consumption but also lowering the computational complexity while maintaining
the synchronization accuracy is crucial to the design of time synchronization
schemes for resource-constrained sensor nodes. In this paper, focusing on the
three aspects of WSN time synchronization, we introduce a framework of reverse
asymmetric time synchronization for resource-constrained multi-hop WSNs and
propose a beaconless energy-efficient time synchronization scheme based on
reverse one-way message dissemination. Experimental results with a WSN testbed
based on TelosB motes running TinyOS demonstrate that the proposed scheme
conserves up to 95% energy consumption compared to the flooding time
synchronization protocol while achieving microsecond-level synchronization
accuracy.
| [{'version': 'v1', 'created': 'Fri, 21 Jun 2019 10:01:11 GMT'}] | 2019-06-24 | [array(['Huan', 'Xintao', ''], dtype=object)
array(['Kim', 'Kyeong Soo', ''], dtype=object)
array(['Lee', 'Sanghyuk', ''], dtype=object)
array(['Lim', 'Eng Gee', ''], dtype=object)
array(['Marshall', 'Alan', ''], dtype=object)] |
19,787 | 2006.00162 | John Clemens | John D. Clemens | Relative primeness and Borel partition properties for equivalence
relations | Revised version to appear in Transactions of the American
Mathematical Society | null | null | null | math.LO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We introduce a notion of relative primeness for equivalence relations,
strengthening the notion of non-reducibility, and show for many standard
benchmark equivalence relations that non-reducibility may be strengthened to
relative primeness. We introduce several analogues of cardinal properties for
Borel equivalence relations, including the notion of a prime equivalence
relation and Borel partition properties on quotient spaces. In particular, we
introduce a notion of Borel weak compactness, and characterize partition
properties for the equivalence relations ${\mathbb F}_2$ and ${\mathbb E}_1$.
We also discuss dichotomies related to primeness, and see that many natural
questions related to Borel reducibility of equivalence relations may be viewed
in the framework of relative primeness and Borel partition properties.
| [{'version': 'v1', 'created': 'Sat, 30 May 2020 03:50:32 GMT'}
{'version': 'v2', 'created': 'Fri, 16 Apr 2021 22:47:13 GMT'}] | 2021-04-20 | [array(['Clemens', 'John D.', ''], dtype=object)] |
19,788 | 1412.2053 | Erhan Bayraktar | Erhan Bayraktar and Song Yao | Doubly Reflected BSDEs with Integrable Parameters and Related Dynkin
Games | Final version. To appear in Stochastic Processes and Their
Applications | null | null | null | math.PR math.OC q-fin.MF | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study a doubly reflected backward stochastic differential equation (BSDE)
with integrable parameters and the related Dynkin game. When the lower obstacle
$L$ and the upper obstacle $U$ of the equation are completely separated, we
construct a unique solution of the doubly reflected BSDE by pasting local
solutions and show that the $Y-$component of the unique solution represents the
value process of the corresponding Dynkin game under $g-$evaluation, a
nonlinear expectation induced by BSDEs with the same generator $g$ as the
doubly reflected BSDE concerned. In particular, the first time when process $Y
$ meets $L$ and the first time when process $Y $ meets $U$ form a saddle point
of the Dynkin game.
| [{'version': 'v1', 'created': 'Fri, 5 Dec 2014 16:42:50 GMT'}
{'version': 'v2', 'created': 'Sun, 5 Jul 2015 19:26:27 GMT'}] | 2015-07-07 | [array(['Bayraktar', 'Erhan', ''], dtype=object)
array(['Yao', 'Song', ''], dtype=object)] |
19,789 | 0709.3927 | R\'obert Juh\'asz | F. Igl\'oi and R. Juh\'asz | Exact relationship between the entanglement entropies of XY and quantum
Ising chains | 6 pages | Europhys. Lett. 81, 57003 (2008) | 10.1209/0295-5075/81/57003 | null | cond-mat.stat-mech quant-ph | null | We consider two prototypical quantum models, the spin-1/2 XY chain and the
quantum Ising chain and study their entanglement entropy, S(l,L), of blocks of
l spins in homogeneous or inhomogeneous systems of length L. By using two
different approaches, free-fermion techniques and perturbational expansion, an
exact relationship between the entropies is revealed. Using this relation we
translate known results between the two models and obtain, among others, the
additive constant of the entropy of the critical homogeneous quantum Ising
chain and the effective central charge of the random XY chain.
| [{'version': 'v1', 'created': 'Tue, 25 Sep 2007 11:53:50 GMT'}
{'version': 'v2', 'created': 'Tue, 5 Feb 2008 17:20:59 GMT'}] | 2009-11-13 | [array(['Iglói', 'F.', ''], dtype=object)
array(['Juhász', 'R.', ''], dtype=object)] |
19,790 | 1706.08846 | Riaz Ahmed | G. Abbas, Riaz Ahmed | Models of Collapsing and Expanding Anisotropic Gravitating Source in
$f(R,T)$ Theory of Gravity | 18 Pages, 8 Figures, Accepted for Publication in European Physical
Journal C | null | 10.1140/epjc/s10052-017-5025-0 | null | gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we have formulated the exact solutions of the non-static
anisotropic gravitating source in $f(R,T)$ gravity which may lead to expansion
and collapse. By assuming the no thermal conduction in gravitating source, we
have determine parametric solutions in $f(R,T)$ gravity with non-static
spherical geometry filled with anisotropic fluid. We have examined the range of
parameter for which expansion scalar become negative and positive leading to
collapse and expansion, respectively. Further, using the definition of mass
function the condition for the trapped surface have been explored and it has
been investigated there exists a single horizon in this case. The impact of
coupling parameter $\lambda$ has been discussed in detail in both cases. For
the various values of coupling parameter $\lambda$, we have plotted energy
density, anisotropic pressure and anisotropic parameter in case of collapse and
expansion. The physical significance of the graphs has been explained in
detail.
| [{'version': 'v1', 'created': 'Sat, 24 Jun 2017 08:15:28 GMT'}] | 2017-08-02 | [array(['Abbas', 'G.', ''], dtype=object)
array(['Ahmed', 'Riaz', ''], dtype=object)] |
19,791 | 2105.12931 | Weijun Tan | Delong Qi, Weijun Tan, Qi Yao, Jingfeng Liu | YOLO5Face: Why Reinventing a Face Detector | null | null | null | null | cs.CV | http://creativecommons.org/licenses/by/4.0/ | Tremendous progress has been made on face detection in recent years using
convolutional neural networks. While many face detectors use designs designated
for detecting faces, we treat face detection as a generic object detection
task. We implement a face detector based on the YOLOv5 object detector and call
it YOLO5Face. We make a few key modifications to the YOLOv5 and optimize it for
face detection. These modifications include adding a five-point landmark
regression head, using a stem block at the input of the backbone, using
smaller-size kernels in the SPP, and adding a P6 output in the PAN block. We
design detectors of different model sizes, from an extra-large model to achieve
the best performance to a super small model for real-time detection on an
embedded or mobile device. Experiment results on the WiderFace dataset show
that on VGA images, our face detectors can achieve state-of-the-art performance
in almost all the Easy, Medium, and Hard subsets, exceeding the more complex
designated face detectors. The code is available at
\url{https://github.com/deepcam-cn/yolov5-face}
| [{'version': 'v1', 'created': 'Thu, 27 May 2021 03:54:38 GMT'}
{'version': 'v2', 'created': 'Thu, 2 Dec 2021 04:40:13 GMT'}
{'version': 'v3', 'created': 'Thu, 27 Jan 2022 16:26:17 GMT'}] | 2022-01-28 | [array(['Qi', 'Delong', ''], dtype=object)
array(['Tan', 'Weijun', ''], dtype=object)
array(['Yao', 'Qi', ''], dtype=object)
array(['Liu', 'Jingfeng', ''], dtype=object)] |
19,792 | 2007.08894 | Henry Ki{\ss}ler | Henry Ki{\ss}ler | Off-shell Diagrammatics for Quantum Gravity | null | Phys. Lett. B 816 (2021) 136219 | 10.1016/j.physletb.2021.136219 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This article reports on how diagrammatic identities of Yang--Mills theory
translate to diagrammatics for pure gravity. For this, we consider the
Einstein--Hilbert action and follow the approach of Capper, Leibbrandt, and
Medrano and expand the inverse metric density around the Minkowski metric. By
analogy to Yang--Mills theory, cancellation identities are constructed for the
graviton as well as the ghost vertices up to the valency of six.
| [{'version': 'v1', 'created': 'Fri, 17 Jul 2020 10:51:30 GMT'}
{'version': 'v2', 'created': 'Wed, 24 Mar 2021 15:38:19 GMT'}] | 2021-03-25 | [array(['Kißler', 'Henry', ''], dtype=object)] |
19,793 | 1704.04449 | Jennifer Wilson | Jeremy Miller, Peter Patzt, and Jennifer C. H. Wilson | Central stability for the homology of congruence subgroups and the
second homology of Torelli groups | Corrections and substantial revisions. 36 pages, 1 figure. To appear
in Advances in Mathematics | Adv. Math. 354 (2019), 106740, 45 pp | 10.1016/j.aim.2019.106740 | null | math.AT math.GR math.GT math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We prove a representation stability result for the second homology groups of
Torelli subgroups of mapping class groups and automorphism groups of free
groups. This strengthens the results of Boldsen-Hauge Dollerup and Day-Putman.
We also prove a new representation stability result for the homology of certain
congruence subgroups, partially improving upon the work of Putman-Sam. These
results follow from a general theorem on syzygies of certain modules with
finite polynomial degree.
| [{'version': 'v1', 'created': 'Fri, 14 Apr 2017 15:14:27 GMT'}
{'version': 'v2', 'created': 'Mon, 22 Jul 2019 16:58:13 GMT'}] | 2020-09-28 | [array(['Miller', 'Jeremy', ''], dtype=object)
array(['Patzt', 'Peter', ''], dtype=object)
array(['Wilson', 'Jennifer C. H.', ''], dtype=object)] |
19,794 | 2206.12989 | David Eppstein | David Eppstein | Locked and unlocked smooth embeddings of surfaces | 8 pages, 8 figures. To appear in 34th Canadian Conference on
Computational Geometry | null | null | null | cs.CG math.MG | http://creativecommons.org/licenses/by/4.0/ | We study the continuous motion of smooth isometric embeddings of a planar
surface in three-dimensional Euclidean space, and two related discrete
analogues of these embeddings, polygonal embeddings and flat foldings without
interior vertices, under continuous changes of the embedding or folding. We
show that every star-shaped or spiral-shaped domain is unlocked: a continuous
motion unfolds it to a flat embedding. However, disks with two holes can have
locked embeddings that are topologically equivalent to a flat embedding but
cannot reach a flat embedding by continuous motion.
| [{'version': 'v1', 'created': 'Sun, 26 Jun 2022 22:57:15 GMT'}] | 2022-06-28 | [array(['Eppstein', 'David', ''], dtype=object)] |
19,795 | 1903.09344 | Weihuang Xu | Weihuang Xu, Guohao Yu, Alina Zare, Brendan Zurweller, Diane Rowland,
Joel Reyes-Cabrera, Felix B Fritschi, Roser Matamala, Thomas E. Juenger | Overcoming Small Minirhizotron Datasets Using Transfer Learning | null | Computers and Electronics in Agriculture, 175 (2020) | 10.1016/j.compag.2020.105466 | null | cs.CV | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Minirhizotron technology is widely used for studying the development of
roots. Such systems collect visible-wavelength color imagery of plant roots
in-situ by scanning an imaging system within a clear tube driven into the soil.
Automated analysis of root systems could facilitate new scientific discoveries
that would be critical to address the world's pressing food, resource, and
climate issues. A key component of automated analysis of plant roots from
imagery is the automated pixel-level segmentation of roots from their
surrounding soil. Supervised learning techniques appear to be an appropriate
tool for the challenge due to varying local soil and root conditions, however,
lack of enough annotated training data is a major limitation due to the
error-prone and time-consuming manually labeling process. In this paper, we
investigate the use of deep neural networks based on the U-net architecture for
automated, precise pixel-wise root segmentation in minirhizotron imagery. We
compiled two minirhizotron image datasets to accomplish this study: one with
17,550 peanut root images and another with 28 switchgrass root images. Both
datasets were paired with manually labeled ground truth masks. We trained three
neural networks with different architectures on the larger peanut root dataset
to explore the effect of the neural network depth on segmentation performance.
To tackle the more limited switchgrass root dataset, we showed that models
initialized with features pre-trained on the peanut dataset and then fine-tuned
on the switchgrass dataset can improve segmentation performance significantly.
We obtained 99\% segmentation accuracy in switchgrass imagery using only 21
training images. We also observed that features pre-trained on a closely
related but relatively moderate size dataset like our peanut dataset are more
effective than features pre-trained on the large but unrelated ImageNet
dataset.
| [{'version': 'v1', 'created': 'Fri, 22 Mar 2019 03:40:25 GMT'}
{'version': 'v2', 'created': 'Mon, 26 Aug 2019 17:53:20 GMT'}
{'version': 'v3', 'created': 'Fri, 24 Apr 2020 15:13:48 GMT'}] | 2020-07-02 | [array(['Xu', 'Weihuang', ''], dtype=object)
array(['Yu', 'Guohao', ''], dtype=object)
array(['Zare', 'Alina', ''], dtype=object)
array(['Zurweller', 'Brendan', ''], dtype=object)
array(['Rowland', 'Diane', ''], dtype=object)
array(['Reyes-Cabrera', 'Joel', ''], dtype=object)
array(['Fritschi', 'Felix B', ''], dtype=object)
array(['Matamala', 'Roser', ''], dtype=object)
array(['Juenger', 'Thomas E.', ''], dtype=object)] |
19,796 | astro-ph/9904257 | Stephan Wellstein | N. Langer (1), A. Heger (2), S. Wellstein (1) and F. Herwig (1) ((1)
Institut fuer Physik, Universitaet Potsdam, Germany (2) Astronomy and
Astrophysics Department, University of California, Santa Cruz) | Mixing and nucleosynthesis in rotating TP-AGB stars | 4 pages, 7 figures, final accepted version, only minor changes to
previous version | null | null | null | astro-ph | null | We present the first evolutionary models of intermediate mass stars up to
their thermal pulses which include effects of rotation on the stellar structure
as well as rotationally induced mixing of chemical species and angular
momentum. We find a significant angular momentum transport from the core to the
hydrogen-rich envelope and obtain a white dwarf rotation rate comparable to
current observational upper limits of 50 km/s.
Large angular momentum gradients at the bottom of the convective envelope and
the tip of the pulse driven convective shell are shown to produce marked
chemical mixing between the proton-rich and the 12C-rich layers during the so
called third dredge-up. This leads to a subsequent production of 13C which is
followed by neutron production through 13C(alpha,n) in radiative layers in
between thermal pulses. Although uncertainties in the efficiency of rotational
mixing processes persist, we conclude that rotation is capable of producing a
13C-rich layer as required for the occurrence of the s-process in TP-AGB stars.
| [{'version': 'v1', 'created': 'Tue, 20 Apr 1999 08:53:45 GMT'}
{'version': 'v2', 'created': 'Tue, 11 May 1999 14:55:51 GMT'}] | 2007-05-23 | [array(['Langer', 'N.', ''], dtype=object)
array(['Heger', 'A.', ''], dtype=object)
array(['Wellstein', 'S.', ''], dtype=object)
array(['Herwig', 'F.', ''], dtype=object)] |
19,797 | 1507.00719 | Jason Miller | Jason Miller and Scott Sheffield | Liouville quantum gravity and the Brownian map I: The QLE(8/3,0) metric | 73 pages, 14 figures | null | null | null | math.PR math-ph math.CV math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Liouville quantum gravity (LQG) and the Brownian map (TBM) are two distinct
models of measure-endowed random surfaces. LQG is defined in terms of a real
parameter $\gamma$, and it has long been believed that when $\gamma =
\sqrt{8/3}$, the LQG sphere should be equivalent (in some sense) to TBM.
However, the LQG sphere comes equipped with a conformal structure, and TBM
comes equipped with a metric space structure, and endowing either one with the
other's structure has been an open problem for some time.
This paper is the first in a three-part series that unifies LQG and TBM by
endowing each object with the other's structure and showing that the resulting
laws agree. The present work uses a form of the quantum Loewner evolution (QLE)
to construct a metric on a dense subset of a $\sqrt{8/3}$-LQG sphere and to
establish certain facts about the law of this metric, which are in agreement
with similar facts known for TBM. The subsequent papers will show that this
metric extends uniquely and continuously to the entire $\sqrt{8/3}$-LQG surface
and that the resulting measure-endowed metric space is TBM.
| [{'version': 'v1', 'created': 'Thu, 2 Jul 2015 19:54:32 GMT'}
{'version': 'v2', 'created': 'Sat, 27 Feb 2016 11:23:24 GMT'}
{'version': 'v3', 'created': 'Mon, 29 Jul 2019 12:58:43 GMT'}] | 2019-07-30 | [array(['Miller', 'Jason', ''], dtype=object)
array(['Sheffield', 'Scott', ''], dtype=object)] |
19,798 | 2010.00457 | Kartick Chandra Sarkar | Kartick Chandra Sarkar, Amiel Sternberg and Orly Gnat | A new ionisation network and radiation transport module in PLUTO | 19 pages, accepted by MNRAS. Added error estimates for radiative
transfer, and runtime plots for different components of the code. Added late
time (>1Myr) dynamics of the HII region | null | 10.1093/mnras/stab578 | null | astro-ph.GA astro-ph.IM | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We introduce a new general-purpose time-dependent ionisation network (IN) and
a radiation transport (RT) module in the magneto-hydrodynamic (MHD) code PLUTO.
Our ionisation network is reliable for temperatures ranging from 5e3 to 3e8 K,
and includes all ionisation states of H, He, C, N, O, Ne, Mg, Si, S and Fe
making it suitable for studying a variety of astrophysical scenarios. Radiation
loss for each ion-electron pair is calculated using CLOUDY-17 data on-the-fly.
Photo-ionisation and charge exchange are the chemical heating mechanisms. The
IN is fully coupled to the radiation transport module over a very large range
of opacities at different frequencies. The RT module employs a method of short
characteristics assuming spherical symmetry. The radiation module requires the
assumption of spherical symmetry, while the IN is compatible with full 3D. We
also include a simple prescription for dust opacity, grain destruction, and the
dust contribution to radiation pressure. We present numerical tests to show the
reliability and limitations of the new modules. We also present a
post-processing tool to calculate projected column densities and emission
spectra.
| [{'version': 'v1', 'created': 'Thu, 1 Oct 2020 14:51:35 GMT'}
{'version': 'v2', 'created': 'Mon, 1 Mar 2021 19:01:07 GMT'}] | 2021-03-17 | [array(['Sarkar', 'Kartick Chandra', ''], dtype=object)
array(['Sternberg', 'Amiel', ''], dtype=object)
array(['Gnat', 'Orly', ''], dtype=object)] |
19,799 | 1609.03383 | Andreas Michels | Andreas Michels, Raoul Weber, Ivan Titov, Denis Mettus, \'Elio Alberto
P\'erigo, Inma Peral, Oriol Vallcorba, Joachim Kohlbrecher, Kiyonori Suzuki,
Masaaki Ito, Akira Kato, and Masao Yano | Spin structures of textured and isotropic Nd-Fe-B-based nanocomposites:
Evidence for correlated crystallographic and spin texture | null | Phys. Rev. Applied 7, 024009 (2017) | 10.1103/PhysRevApplied.7.024009 | null | cond-mat.mes-hall | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We report the results of a comparative study of the magnetic microstructure
of textured and isotropic
$\mathrm{Nd}_2\mathrm{Fe}_{14}\mathrm{B}/\alpha$-$\mathrm{Fe}$ nanocomposites
using magnetometry, transmission electron microscopy, synchrotron x-ray
diffraction, and, in particular, magnetic small-angle neutron scattering
(SANS). Analysis of the magnetic neutron data of the textured specimen and
computation of the correlation function of the spin misalignment SANS cross
section suggests the existence of inhomogeneously magnetized regions on an
intraparticle nanometer length scale, about $40-50 \, \mathrm{nm}$ in the
remanent state. Possible origins for this spin disorder are discussed: it may
originate in thin grain-boundary layers (where the materials parameters are
different than in the $\mathrm{Nd}_2\mathrm{Fe}_{14}\mathrm{B}$ grains), or it
may reflect the presence of crystal defects (introduced via hot pressing), or
the dispersion in the orientation distribution of the magnetocrystalline
anisotropy axes of the $\mathrm{Nd}_2\mathrm{Fe}_{14}\mathrm{B}$ grains. X-ray
powder diffraction data reveal a crystallographic texture in the direction
perpendicular to the pressing direction -- a finding which might be related to
the presence of a texture in the magnetization distribution, as inferred from
the magnetic SANS data.
| [{'version': 'v1', 'created': 'Mon, 12 Sep 2016 13:16:05 GMT'}] | 2017-02-15 | [array(['Michels', 'Andreas', ''], dtype=object)
array(['Weber', 'Raoul', ''], dtype=object)
array(['Titov', 'Ivan', ''], dtype=object)
array(['Mettus', 'Denis', ''], dtype=object)
array(['Périgo', 'Élio Alberto', ''], dtype=object)
array(['Peral', 'Inma', ''], dtype=object)
array(['Vallcorba', 'Oriol', ''], dtype=object)
array(['Kohlbrecher', 'Joachim', ''], dtype=object)
array(['Suzuki', 'Kiyonori', ''], dtype=object)
array(['Ito', 'Masaaki', ''], dtype=object)
array(['Kato', 'Akira', ''], dtype=object)
array(['Yano', 'Masao', ''], dtype=object)] |