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1,941,325,219,188 | arxiv | \section{Introduction} \label{sec:Introduction}
The Dyson equation is at the heart of many important physical problems, taking its roots in many-body formalisms for the Green's function \cite{Kadanoff62, Economou06}.
The real-space version of the Dyson equation is of particular importance in the framework of inhomoge... |
1,941,325,219,189 | arxiv | \section{Introduction}
\IEEEPARstart{A}{} geometric sequence is a series of numbers in which the ratio between any two consecutive terms is fixed. Recall that a geometric sequence is expressed by
\begin{equation*}
\{a, ar, ar^2, ar^3, \cdots \}
\end{equation*}
where $a$ is the initial term and $r$ is the common ra... |
1,941,325,219,190 | arxiv | \section{Introduction}
The investigation of vector mesons is actual up to now due to their role
in forming the electromagnetic structure of particles and because, {\it e.g.},
in the $\rho$-family, only the $\rho(770)$ meson can be deemed to be well
understood \cite{PDG-06}. The other $\rho$-like mesons must be eith... |
1,941,325,219,191 | arxiv | \section{Introduction}
The theory of noncommutative martingales has enjoyed considerable progress in recent years due to its interaction with other field of mathematics such as operator spaces and free probability. Many classical martingale inequalities have been extended to the noncommutative setting. We refer ... |
1,941,325,219,192 | arxiv | \section{Introduction
The seminal paper by Birkhoff and von Neumann \cite{BiNe} showed
that the events of quantum mechanical measurements do not fulfill
the axioms of Boolean algebras and therefore also do not axioms of
the classical probability theory presented by Kolmogorov \cite{Kol}.
It initiated the research... |
1,941,325,219,193 | arxiv | \section{Introduction}\label{sec:intro}
Monitoring of regions of strong-field gravity is now possible with a wide array of observatories, including gravitational-wave detectors~\cite{Abbott:2016blz,Abbott:2020niy}
and very long baseline interferometry~\cite{Akiyama:2019cqa,Abuter:2020dou}. These observatories will be u... |
1,941,325,219,194 | arxiv | \section{Introduction}
\noindent
Black hole analogues are fluid dynamical analogue of the black hole space time
as perceived in the general theory of relativity
\cite{unr81,unr95,vis98,bil99,nov02,car05,bar05,us07},
and such analogue systems can be constructed for a small linear perturbation
propagating throug... |
1,941,325,219,195 | arxiv | \section{Introduction.}
Consider a smooth projective curve $C$ with a spin line bundle $L\to C$ such that $h^0(C,L) =~1$. Let $p\in C$ be a zero of the corresponding spinor (i.e. the holomorphic section of $L$). Let $f: C\to PH^0(C,L(p))^{\vee}$ be the map that maps a point on $C$ to the hyperplane in $H^0(C,L(p))$ ... |
1,941,325,219,196 | arxiv | \section*{Appendix \thesection\protect\indent \parbox[t]{11.15cm}{#1}}
\addcontentsline{toc}{section}{Appendix \thesection\ \ \ #1}}
\newcommand{\appwithlabel}[2]{\addtocounter{section}{1}\setcounter{equation}{0}
\renewcommand{\thesection}{\Alph{section}}
\section*{Appendix \thesection\protect\indent \parbox[t]{11.15cm... |
1,941,325,219,197 | arxiv |
\section{Introduction}
Sequence labeling is an important task that finds applications in many areas such as bio-informatics, natural language processing (NLP), speech recognition, image processing etc. Depending upon the underlying sequence labeling task, labels are assigned to the tokens present in the sequenc... |
1,941,325,219,198 | arxiv | \section{\label{sec:intro}Introduction}
The anomalous magnetic moment of the muon $a_\mu \equiv (g-2)_\mu/2$ presents an intriguing possible probe of new physics beyond the Standard Model (SM) \footnote{Recent lattice calculations of the hadronic vacuum polarization contribution to $g-2$ \cite{Borsanyi:2020mff,Lehner:... |
1,941,325,219,199 | arxiv | \section{Introduction}
The realization of the settings which emulate the spin-orbit (SO)\ coupling
in ultracold atomic gases \cite{SOC1,SOC2,SOC-2D,SOC-review} has opened up a
vast research area in studies of matter waves. In particular, the interplay
of the linear SO coupling with intrinsic nonlinearity of Bose-... |
1,941,325,219,200 | arxiv | \section{Introduction} \label{section:introduction}
How to learn complex temporal sequence patterns by means of neural network models has been a challenging problem.
Recurrent neural networks (RNNs) \cite{Jordan86,Elman90,Pollack91,Zipser89} have been one of the most popular models applied to temporal sequence learnin... |
1,941,325,219,201 | arxiv | \section{Introduction}
\label{sec:intro}
Non-equilibrium dynamics of strongly coupled system is one of the most challenging tasks in theoretical physics. It is not only interesting in cosmology and particle physics, but also interesting within condensed matter physics \cite{henkel,hohenberg,Polkovnikov:2010yn}. In re... |
1,941,325,219,202 | arxiv | \section{Introduction}
In the framework of the $\Lambda$CDM Universe hierarchical structure formation
feedback, either by star formation or processes connected to active galactic
nuclei (AGN), shape the observed galaxy population in today's Universe
\citep[e.g.,][]{croton_06a}. Powerful FR~I and FR~II radio galaxies ar... |
1,941,325,219,203 | arxiv | \section{Introduction}
In recent years a semiclassical first approximation to strongly coupled QCD, light-front~(LF) holographic AdS/QCD, has been developed~\cite{deTeramond:2005su,Brodsky:2006uqa,Brodsky:2007hb, Brodsky:2008pg,Brodsky:2008pf,deTeramond:2008ht,deTeramond:2010ge,Brodsky:2014yha} and successfully used ... |
1,941,325,219,204 | arxiv | \section{Introduction}
\fancyhead{}
\pagestyle{fancy}
\renewcommand{\headrulewidth}{0pt}
\fancyhead[LE,RO]{\thepage}
\fancyhead[CO]{L.-P. Arguin, P. Bourgade and M. Radziwi\l\l}
\fancyhead[CE]{The Fyodorov-Hiary-Keating Conjecture. I.}
\fancyfoot{}
Motivated by the problem of understanding the global maximum of the R... |
1,941,325,219,205 | arxiv | \section{Accuracy}\label{apx:accuracy}
\begin{figure*}[t!]
\subfigure[VGGNet ($B=64$)]{
\includegraphics[width=.48\hsize]{imgs/{VGG-10-64-0.01-accuracy}.pdf}
}
\subfigure[VGGNet ($B=4096$)]{
\includegraphics[width=.48\hsize]{imgs/{VGG-10-4096-0.1-accuracy}.pdf}
}
\subfigure[NIN ($B=64$)]{
\incl... |
1,941,325,219,206 | arxiv | \section{Introduction}
The Golden ratio is well known by everyone and this ratio possesses rich
application areas such as architecture, painting, design, music, nature,
optimization, and perceptual studies. However, in fact, it is probably fair
to say that the golden ratio has inspired thinkers of all disciplines... |
1,941,325,219,207 | arxiv | \section{Introduction}
When a primary cosmic ray particle interacts with a molecule in the atmosphere, a shower of energetic hadrons including pions $(\pi^\pm)$ and kaons $(K^\pm)$ are generated. These quickly decay and produce relativistic muons~\cite{muon1, pdg} that are highly boosted with the livetime long enough ... |
1,941,325,219,208 | arxiv | \section{Introduction}
\IEEEPARstart{T}{HE} early digital cryptocurrencies rely on central authorities to settle transactions. Digital cryptocurrencies did not flourish, until the advent of Bitcoin \cite{nakamoto2008bitcoin, antonopoulos2014mastering}. To avoid single points of failure, Bitcoin is designed as a decentr... |
1,941,325,219,209 | arxiv | \section{Introduction}
Of late, two-dimensional (2D) materials have piqued the curiosity of the scientific mind. From graphene\cite{NGgr04,ZTgr05} to transition metal dichalcogenides (TMDs),\cite{CPtmd14} this class of materials has received much acclaim for its role in next-generation nanoscale devices, with advanced ... |
1,941,325,219,210 | arxiv | \section{Introduction}
\label{intro}
Complex systems, consisting of several components that interact,
arise in a natural way in a wide range of applications.
The components may be complex themselves
(they may e.g.\ contain a database; may have
their specific internal logic and an appropriate inference mechanism;
... |
1,941,325,219,211 | arxiv | \section{Introduction}
The classical nearest-neighbor Heisenberg antiferromagnet on the pyrochlore lattice stands as an epitome of geometric frustration in three dimensions as shown by its failure to develop magnetic long-range order down to absolute zero temperature, realizing what has been dubbed a ``cooperative par... |
1,941,325,219,212 | arxiv | \section{Introduction}
A \textit{graph} on a set $X$ is a symmetric irreflexive relation $G \subseteq X^2$. A set $A \subseteq X$ is \textit{$G$-independent} iff $A^2 \cap G = \emptyset$. The \textit{chromatic number} of $G$, $\chi(G)$, is the least cardinality of a family of $G$-independent sets covering the underlyi... |
1,941,325,219,213 | arxiv | \section{Introduction}
A new tool is now available to probe the population of recently formed
massive stars, while still embedded in their parent clouds. Such stars
are surrounded by a compact H\,{\sc ii} region, with an ionization
front working outwards into the cloud. Regions undergoing massive star
formation contai... |
1,941,325,219,214 | arxiv | \section{Introduction}\label{sec:intro}
Multi-armed bandit (MAB) problems are well-known models of sequential decision-making under uncertainty~\citep{lairobbins} and have lately been used to model new and exciting decision problems in content recommendation systems, online advertising platforms, and
social networks, a... |
1,941,325,219,215 | arxiv | \section{Introduction\label{sec:Int}}
\textit{Introduction.--}Floquet topological phases, as created by time-periodic modulations, have been an experimental reality in both synthetic metamaterials \cite{Rechtsman2013,Szameit2017,Cheng2019,Aidelsburger2020} and actual condensed-matter systems \cite{Wang2013Exp,Mciver20... |
1,941,325,219,216 | arxiv | \section{Introduction}
Financial companies make decisions about how to control their risk exposure optimally through business activities aimed at maximizing or minimizing various objective functions. Such decisions have recently been the focus of numerous studies (e.g., \cite{Zhou2003}, \cite{He2015}, \cite{NS2020}). I... |
1,941,325,219,217 | arxiv | \section{Introduction and the model\label{sec:intro}}
A light, confining hidden sector coupled feebly to the Standard Model (SM) is in general an interesting possibility for new physics, often referred to as a hidden valley (HV)~\cite{Strassler:2006im}. More sharply, it can be part of the answers to outstanding questi... |
1,941,325,219,218 | arxiv | \section{Introduction}
\label{sec:intro}
Understanding the origin of polarization in the radiation from charged particles is of central importance in the study of many astrophysical objects like gamma-ray-bursts (GRBs)~\cite{wiersema2014,troja2017}, supernova remnants (SNRs)~\cite{milne1974,bandiera2016}, active gala... |
1,941,325,219,219 | arxiv | \section{Introduction}
The physics goal at RHIC is to study and identify the properties
of matter with partonic degrees of freedom~\cite{starwhitepaper}.
Hard probes such as identified particles at high $p_T$, heavy
flavor and jets are thought to be well calibrated probes since
they are calculable in the perturbative ... |
1,941,325,219,220 | arxiv | \section{introduction}
{\it Introduction.---}
In a bilayer system with a small interlayer twist angle $\theta$, moir\'e pattern forms and leads to novel two-dimensional (2D) phenomena. In twisted bilayer graphene (TBG), there are magic twist angles, at which Dirac Fermi velocity vanishes \cite{Bistritzer2011}. Low-ene... |
1,941,325,219,221 | arxiv | \section{introduction}
Let $A:=A_n$ be the free associative algebra with $n$ generators
over $\mathbb{C}$. Consider its lower central series as a Lie algebra,
i.e., the Lie ideals $L_m(A)\subset A$ defined recursively by
$L_1(A)=A, L_i(A)=[A,L_{i-1}(A)]$, and the corresponding
associated graded Lie algebra $B(A):=\o... |
1,941,325,219,222 | arxiv | \section{Introduction}
One main focus of heavy-ion collision experiments is to understand the properties of the liquid-gas phase transition in
nuclear matter \cite{Agostino05,Das05}. This phase transition is also important for various astrophysical reasons.
For example, it plays a significant role in the dynamics of su... |
1,941,325,219,223 | arxiv | \section{Introduction}
Over the last two years, Natural Language Processing has been shaken by the release of large pre-trained language models based on self-attention, like BERT \cite{bert}.
Ranking models based on BERT are currently state-of-the-art for adhoc IR, and rank first on leaderboards\footnote{\url{https://... |
1,941,325,219,224 | arxiv | \section{Introduction}
\label{Introduction}
The recent results of the Planck experiment
\cite{1303.5062,1303.5076}
generated lively discussions
\cite{1301.3119,1303.6267,1303.6270,1304.5243,1304.5981,1304.6217,1305.1971,1306.6766,1307.2904,1307.7715,1308.3255,1308.5870}
on the value of the effective number of relativi... |
1,941,325,219,225 | arxiv | \section{Introduction}\label{intro}
Studies of CP violation in the $B$-meson system and the determination
of the three angles $\alpha$, $\beta$ and $\gamma$ of the usual
non-squashed unitarity triangle \cite{ut} of the Cabibbo--Kobayashi--Maskawa
matrix (CKM matrix) \cite{ckm} are among the central targets of future... |
1,941,325,219,226 | arxiv | \section{Introduction}
Let $X$ be a smooth projective $n$-fold with ample canonical bundle defined
over $\mathbb{C}$.
Then by the celebrated solution of Calabi's conjecture (\cite{a,y}), there exists
a unique K\"{a}hler-Einstein form $\omega_{E}$ such that
\[
-\mbox{Ric}_{\omega_{E}} = \omega_{E},
\]
where $\mbox... |
1,941,325,219,227 | arxiv | \section{Introduction}
\label{s1}
The question of scale and nature of T-invariance violation in
fundamental interactions remains open. So far only the results,
obtained in K$^0$-meson decays \cite{1a}, evidence for such
violation. Many researches of T-noninvariant effects in nuclear
processes, in neutron $\beta$-decay... |
1,941,325,219,228 | arxiv | \section{Introduction}
We work over an algebraically closed field of characteristic 0. \\
Alexeev and Brion construct a moduli stack $AB(V)$ parametrizing finite torus equivariant maps from stable (also known as broken) toric varieties $X$ to a fixed projective variety $V$ \cite{ab}, generalizing Alexeev's construct... |
1,941,325,219,229 | arxiv | \section{Introduction} \label{sec:introduction}
In this paper, we consider a family of McKean-Vlasov stochastic differential equations (SDEs) on $\mathbb{R}^d$, parametrised by $\theta\in\mathbb{R}^p$, of the form
\begin{align}
\mathrm{d}x_t^{\theta}&= B(\theta,x_t^{\theta},\mu_t^{\theta})\mathrm{d}t + \sigma(x_t^{\the... |
1,941,325,219,230 | arxiv | \section{Introduction}
\vspace*{-.15cm}
The concept of parsimony is central in many scientific domains. In the context of statistics, signal processing or machine learning, it may take several forms. Classically, in a variable or feature selection problem, a sparse solution with many zeros is sought so that the mode... |
1,941,325,219,231 | arxiv | |
1,941,325,219,232 | arxiv |
\section{introduction}
Various extensions of the Standard Model include
additional quarks in vector representations of the standard model gauge
group. Examples include little Higgs theories \cite{lh,littlest,SU6Sp6}, topcolor models
\cite{tc}, and extra dimensional theories with bulk fermions. Vector-like matter... |
1,941,325,219,233 | arxiv | \section{Introduction}\label{sec:1}
Let $n$ and $t$ be positive integers with $t<n$, and let $q$ be a prime power.
Let ${\rm PG}(n-1,q)$ denote the $(n-1)$-dimensional
projective space over the finite field $\ensuremath{\mathbb{F}}_q$.
A {\em partial $(t-1)$-spread} $S$ of ${\rm PG}(n-1,q)$ is a collection
of $(t-1... |
1,941,325,219,234 | arxiv | \section{Reduced order model algorithms \label{sec:rom_algorithm}}
One natural extension to \cite{cagniart2017model,cagniart2019model,nonino2019overcoming} is \textcolor{black}{utilizing} neural networks to learn \textcolor{black}{a} coordinate transformation $T_{t,\mu}$. However, it is nontrivial to measure how a coor... |
1,941,325,219,235 | arxiv | \section{Introduction}
\subsection{Decay of correlations}
Let $(X,f,\mu)$ be a measure preserving dynamical system. Recall that the system is said to be \emph{mixing}
if for any functions $\phi$, $\psi$ in $L^2$ the covariance
\begin{equation}\label{eq:doc}
\cov(\phi\circ f^n,\psi) := \int \phi\circ f^n\psi d\mu - \... |
1,941,325,219,236 | arxiv | \section{Introduction}
Transformer based models achieved state-of-the-art results on a diverse set of tasks across different domains but most of the architectures have quadratic memory and computational complexity \citep{devlin2019bert}. Some recent studies introduced models with the reduction of original complexity \c... |
1,941,325,219,237 | arxiv | \section{Introduction} \label{s:preliminaries}
An important strategy to tackle the local-global conjectures in modular representation theory of finite groups is to try to reduce them to stronger statements about simple groups. Such reduction theorems are obtained by techniques of Clifford theory, and in particular, ... |
1,941,325,219,238 | arxiv | \section{Introduction}
In recent years, latent-state models --- particularly hidden Markov models (HMMs) --- have become increasingly popular tools for time series analyses. In many applications, the data at hand follow some pattern within some periods of time but reveal different stochastic properties during other pe... |
1,941,325,219,239 | arxiv | \section{INTRODUCTION}
The Eliashberg formalism \cite{Eliashberg1960A} allows for the analysis of classical phonon-mediated superconducting state at the quantitative level.
The input parameters to the Eliashberg equation are: the spectral function, otherwise called the Eliashberg function ($\alpha^{2}F\left(\omega\rig... |
1,941,325,219,240 | arxiv | \section{Introduction}
Systems whose constituents
posses an innate ability to convert energy available in their environment into directed
motion are commonly referred-to as active matter. In the context of biological systems, it encapsulates
a broad range of living phenomena, ranging from macroscopic multi-cellular
o... |
1,941,325,219,241 | arxiv | \section{Introduction}
\label{introd}
Spatially extended evolutionary game theory models have found widespread
applications in population dynamics, with the aim to explore the complex
spatio-temporal patterns that characterize ecological and biological systems in
which multiple species interact cooperatively or comp... |
1,941,325,219,242 | arxiv |
\section{Stochastic Continuous Greedy}\label{sec:scg}
In this section, we introduce our main algorithm, \alg (SCG), which is a stochastic variant of the continuous greedy method to to solve Problem~\eqref{eq:mainproblem}.
We only assume that the expected objective function $F$ is monotone and DR-submodular and the st... |
1,941,325,219,243 | arxiv | \section{Distributed Games and Strategies}\label{sec:diststrats}
\begin{abstract}
A summary of work on distributed games and strategies done within the first three years of the ERC project ECSYM is presented.
\end{abstract}
\section{Motivation}
\newcommand{{\it vs.}}{{\it vs.}}
My current interest is to develop a mat... |
1,941,325,219,244 | arxiv | \section{Introduction}
Some time ago, Cardy famously employed modular invariance to obtain
the high-temperature behavior of conformal field theory (CFT)
partition functions in two dimensions \cite{Cardy:1986ie}. This
result has since been exploited in a variety of contexts, including
the statistical physics of black h... |
1,941,325,219,245 | arxiv | \section{Introduction}
For us, an operator algebra is a norm closed algebra of operators on a Hilbert space, or equivalently a closed subalgebra $A$ of a $C^*$-algebra $B$.
In this paper we shall assume for simplicity that $A$ and $B$ share a common identity element.
In `noncommutative peak interpolation' as surveyed... |
1,941,325,219,246 | arxiv | \section{Introduction}
\label{intro}
The method of the radiative return, i.e. the study of events with
initial state radiation (ISR) at electron-positron colliders,
allows to measure the hadronic cross section over a wide
range of energies in a single experiment, without changing the beam energy.
Originally sugges... |
1,941,325,219,247 | arxiv | \section{Introduction}
In string theory an oft-used approach to studying black holes is to consider wrapped black strings in one dimension higher. The supergravity solution of the black string contains an AdS$_3$ factor in the near-horizon limit, and via the AdS/CFT corespondence there exists a dual two-dimensional CF... |
1,941,325,219,248 | arxiv | \section{Introduction \label{sec:Introduction}}
The smallest insects (body length $<$ 2 mm) such as thrips fly at a chord-based Reynolds number ($Re$) on the order of 10, representing what may be considered as the aerodynamic lower limit of flapping flight. Flight at such low $Re$~is challenged by significant viscous d... |
1,941,325,219,249 | arxiv | \section{Conclusions}
A strong magnetoelastic effect is reported in the CeCo$_{1-x}$Fe$_{x}$Si alloys. The forced magnetostriction $\Delta L(B) / L$ is shown to change by an order of magnitude in response to slight changes of the Fe content $x$ showing a maximum around the critical concentration $x_c$ where the N\'eel... |
1,941,325,219,250 | arxiv | \section{Introduction}
The domain of representation learning has undergone tremendous advances due to improved supervised learning techniques. However, unsupervised learning has the potential to leverage large pools of unlabeled data, and extend these advances to modalities that are otherwise impractical or impossible.... |
1,941,325,219,251 | arxiv | \section{Introduction}
Estimating statistics of frequency vectors implicitly defined by insertion-only update streams, as defined in the abstract, was first studied by Flajolet and Martin in \cite{FlajoletM85}. They studied the so-called {\em distinct elements problem}, in which $f(x)$ is the support size of $x$. In t... |
1,941,325,219,252 | arxiv | \section{Introduction}
The Fujita approximation theorem, \cite{fuj}, is an important result in
algebraic geometry. It states that whilst the section ring associated to a
big line bundle $L$ on an algebraic variety $X$
\[ R(L)\stackrel{\rm def}{=} \oplus_n H^0(nL, X)\]
is typically not a finitely generated algebra, i... |
1,941,325,219,253 | arxiv | \section*{Working plan}
\keywords{\emph{Fractional calculus, Caputo derivative, Fractional differential equation, Comparison principle, Lyapunov's first method, Lyapunov's second method, Asymptotic behavior, Stability, Asymptotic stability, Mittag-Leffler stability.}}
{\it 2010 Mathematics Subject Classification:} {\s... |
1,941,325,219,254 | arxiv | \section{Introduction}
\label{sec:intro}
The dynamical susceptibility $\chi({\bf q},\omega)$ of an interacting Fermi system, and, in particular, its imaginary part, is a fundamental quantity which contains the information about the strength of fluctuations of a particular order parameter. The charge ($c$) and spin ($s... |
1,941,325,219,255 | arxiv | \section{Introduction}
\label{secintroduction}
Recently Hucht \cite{Hucht09} (see also \cite{Kadauetal08}),
motivated by the phenomenon of magnetic friction,
formulated a nonequilibrium steady state (NESS) Ising model of a new type.
It consists of two parallel linear Ising chains having a relative
velocity $v$.
In ad... |
1,941,325,219,256 | arxiv | \section{Introduction}\label{sec:intro}
Along with the development of deep neural networks, text recognition methods have significantly improved.
Currently, most state-of-the-art methods can easily recognize simple horizontal texts.
Recently, the research trend has progressed to recognize more irregular texts: recogni... |
1,941,325,219,257 | arxiv | \section{Introduction}
\label{sec:introduction}
\setcounter{equation}{0}
The degeneracy of BPS states of certain wrapped brane/string
configurations defines a microscopic entropy which, in quite a number
of cases, has been successfully compared to the macroscopic entropy of
supersymmetric black hole solutions in the co... |
1,941,325,219,258 | arxiv | \section{Introduction}
On the 14th September 2015 the Advanced Laser Interferometer Gravitational-wave Observatory (LIGO) made the first direct detection of gravitational waves \cite{gw150914,gw151226}. To achieve the extraordinary sensitivity required for this discovery, Advanced LIGO uses a complex configuration of s... |
1,941,325,219,259 | arxiv | \section{Introduction}
The Ising model \cite{a3,onsager} has been used during long time as a "toy model" for diverses objectives, as to test and to improve new algorithms and methods of high precision for calculation of critical exponents in Equilibrium Statistical Mechanics using the Monte Carlo method
as Metropolis ... |
1,941,325,219,260 | arxiv |
\section{Introducing FLUTE}\label{sec:flute}
\begin{figure*}[t]%
\centering%
\includegraphics[width=0.48\linewidth]{figures/flute_diagram.pdf}%
\hfill%
\includegraphics[width=0.48\linewidth]{figures/flute_diagram_blender.pdf}%
\caption{\label{fig:flute_diagram}({\em Left}) FLUTE trains the sha... |
1,941,325,219,261 | arxiv | \section{Introduction}
Curriculum Learning (CL) attempts to optimize the order in which an agent accumulates experience, increasing performance while reducing training time for complex tasks~\cite{narvekar2020curriculum,foglino2019optimization,narvekar2017autonomous}. The core of CL is to generalize the experience and... |
1,941,325,219,262 | arxiv | \section{Introduction}\label{sec:introduction}}
\IEEEPARstart{M}{alware} remains a big threat to cyber security despite communities' tremendous countermeasure efforts. For example, Symantec \cite{symantec:Online} reports seeing 355,419,881 new malware variants in year 2015, 357,019,453 in year 2016, and 669,974,865 in... |
1,941,325,219,263 | arxiv | \section{GRB060124 observational properties}
On 2006-01-24 at 15:54:52 UT, Swift-BAT triggered on the precursor of GRB060124, that occurred $\sim 570$\,s before the main burst peak \cite{romano-060124}. This allowed Swift to immediately re-point the narrow field instruments (NFIs) and acquire a pointing towards the bur... |
1,941,325,219,264 | arxiv | \section{Introduction}
\label{secI}
First introduced in 1987, the reactive planning model of Georgeff and
Lansky's PRS system has subsequently proved to be one of the most
influential and long-lived approaches to programming multi-agent
systems \cite{GeorRRP}. The \as\ programming language, introduced by
Rao \citeyea... |
1,941,325,219,265 | arxiv |
\section{Introduction}
``You are preparing a paper for an upcoming deadline and try to fit the content
within the page limit. You identified a redundant sentence and remove it but to
your surprise, the page count of your paper increases!''
This is an example where a natural monotonicity property expected from the
ou... |
1,941,325,219,266 | arxiv | \section{Appendix}
\paragraph{Detailed derivation of equations}
We begin with a configuration model network, and consider two infectious
diseases which infect nodes of the network. We assume infection by
either disease confers immediate and complete protection from any future
infection by any disease. We index the d... |
1,941,325,219,267 | arxiv | \section{Introduction and statement of results}
A \emph{fibration of} $\mathbb R^3$ \emph{by oriented lines} is given by a unit vector field $V : \mathbb R^3 \to S^2$, for which all of the integral curves are oriented lines.
\begin{example} We offer three qualitatively distinct examples.
\label{ex:fibrations}
\begin{... |
1,941,325,219,268 | arxiv | \section{Introduction and main results}
Let $N$ be a natural number. The Jacobsthal function $j(N)$ is defined as the length of the largest gap between numbers which are coprime to $N$. In other words,
\[
j(N)=\max_{m}\{\text{For some } x\in \mathbb N \text{ the inequality } (x+i,N)>1 \text{ holds for all }i\leq m... |
1,941,325,219,269 | arxiv |
\subsection{The Recovery of Late Bloomers}
In this section we demonstrate how GD with softmax depresses initially weak operations as XNAS mitigates the effect.
We derive the corresponding update rules and explain the underlying functional structure.
\input{advantages_of_the_proposed_method/recovery_of_late_blommers.t... |
1,941,325,219,270 | arxiv | \section{Introduction}
Fine-grained visual categorization (FGVC) aims to distinguish objects in subordinate classes. For example, dog images are classified into different breeds of dogs, such as ``Chihuahua'', ``Pug'', ``Samoyed'' and so on~\cite{khosla2011novel,ParkhiVZJ12}. One challenge of FGVC is that it has to h... |
1,941,325,219,271 | arxiv | \section{Introduction}
In the current experimental program of nucleon structure studies, we find two broad areas
of experimentation. On the one hand, elastic scattering of electrons from nucleons
is used to measure the electromagnetic and axial form factors of the nucleon, over a
range of momentum transfer of $0.1 ... |
1,941,325,219,272 | arxiv | \section*{THG in graphene heterostructures}
Our samples are van der Waals heterostructures, consisting of a graphene sheet with a metallic nanoribbon array placed a few nanometers above it and separated by {either} an insulating $\mathrm{Al_2 O_3}$ ($3-20\,\mathrm{nm}$) or a monolayer h-BN spacer, as depicted in Fig. \... |
1,941,325,219,273 | arxiv |
\section{Localization from Relative Measurements}
\label{sec:localization}
Target tracking via the distributed estimator in Alg. \ref{alg:dist_lin_filt} requires knowledge of the true sensor locations. As mentioned earlier this is typically not the case, especially when large sensor networks are deployed. This section... |
1,941,325,219,274 | arxiv | \section{Introduction}
The goal of image captioning is to automatically describe the visual images with natural languages. This is a cross-modality task that transfers information from the image domain to the language domain \cite{wu2020fine}. With the release of captioning datasets \cite{vinyals2015show, vinyals... |
1,941,325,219,275 | arxiv | \section{Introduction}
During recent years positron annihilation spectroscopy (PAS) has become
a valuable method to study the microscopic structure of solids \cite{Tuomi13V85,Puska94V66}
and gives detailed information on the electron density and momentum distribution
\cite{Makko14V89,Kontr12V85,Tang05V94} in the regio... |
1,941,325,219,276 | arxiv | \section{Introduction}
The present paper is concerned with the so-called Combes-Thomas estimate of the following Schr\"{o}dinger operator with magnetic field
\begin{equation}\label{schrodinger-op}
H_{\La}(A,V)=\frac{1}{2}(-i\nabla-A(x))^{2}+V(x)\quad\text{on}\quad\La,
\end{equation}
where $i=\sqrt{-1}$ is the im... |
1,941,325,219,277 | arxiv | \section*{Introduction}
Imaging through dense, volumetric, scattering media has been a significant challenge for various applications, such as imaging through skin tissue and industrial remote sensing through the smoke. In conventional imaging, photons directly travel from the target to the sensor. However, in scatteri... |
1,941,325,219,278 | arxiv | |
1,941,325,219,279 | arxiv | \section{Introduction}
The simple, nonrelativistic quark model (QM) gives a qualitatively good
description of the baryon moments. Under the assumption that each baryon
is composed of three valence or constituent quarks in a state with all
internal orbital angular momenta equal to zero, the moments are given
by expecta... |
1,941,325,219,280 | arxiv | \section{Introduction}
A group $G$ is left-orderable if there exists a strict total ordering $<$ of its elements such that $g<h$ implies $fg<fh$ for all $f, g, h \in G$, and bi-orderable if $g<h$ implies $gf<hf$ also holds. Equivalently, a group $G$ is left-orderable if there is a subset $P \subset G$, called the \e... |
1,941,325,219,281 | arxiv | \section{Introduction}
With the rapid developments of deep learning, ConvNets have been the \textit{de facto} method for various computer vision tasks. It takes a long time and substantial effort to devise many useful models~\cite{DBLP:conf/cvpr/HeZRS16,DBLP:conf/cvpr/HuSS18,DBLP:conf/cvpr/HuangLMW17,DBLP:conf/eccv/MaZ... |
1,941,325,219,282 | arxiv | \section{Introduction}
The nontrivial vacuum structure of non-Abelian gauge theories
\cite{Belavin:1975fg,'tHooft:1976up,'tHooft:1976fv,Callan:1976je,Jackiw:1976pf}
plays an important role in particle theory. It underlies
baryon-number non-conservation in electroweak theory and the
existence of $\theta$-vacua in QCD. T... |
1,941,325,219,283 | arxiv | \section{Introduction}
Cool main-sequence stars have outer convection zones (spectral types F to
about M4) or are fully convective (spectral types later than M4). The turbulent
flows in the electrically conducting plasma along with the stellar
(differential) rotation support a hydromagnetic dynamo that constantly
... |
1,941,325,219,284 | arxiv | \partial{\partial}
\def{\boldsymbol\psi}{{\boldsymbol\psi}}
\def{\bar{\boldsymbol\psi}}{{\bar{\boldsymbol\psi}}}
\def{\boldsymbol\lambda}{{\boldsymbol\lambda}}
\def{\boldsymbol\sigma}{{\boldsymbol\sigma}}
\def{\bar \nu}{{\bar \nu}}
\def{\bar \psi}{{\bar \psi}}
\def{\bar X}{{\bar X}}
\def{\bar p}{{\bar p}}
\def{\bar q}{... |
1,941,325,219,285 | arxiv | \section*{Abstract}
Hyperspectral imaging (HSI) is an optical technique that processes the electromagnetic spectrum at a multitude of monochromatic, adjacent frequency bands. The wide-bandwidth spectral signature of a target object's reflectance allows fingerprinting its physical, biochemical, and physiological propert... |
1,941,325,219,286 | arxiv |
\section{Introduction}
Sequence segmentation is an important task for many speech and audio applications such as speaker diarization, laboratory phonology research, speech synthesis, and automatic speech recognition (ASR). Segmentation models can be used as a pre-process step to clean the data (e.g., removing non-spe... |
1,941,325,219,287 | arxiv | \section*{Acknowledgments}
We are grateful to R. Aloisio, P. Blasi and B. Hnatyk for joint
works on this and related subjects. We thank Alan Watson for
providing us with Auger energy spectrum as numerical files.
Our work is supported in part by \emph{ASI} through
grant \emph{WP 1300} (theoretical study).
|
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