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1,941,325,218,288 | arxiv | \section{Introduction}
Eigenstate Thermalization Hypothesis(ETH)\cite{PhysRevE.50.888, PhysRevA.43.2046, rigol2008thermalization,doi:10.1126/science.aaf6725} is a key concept explaining the thermalization of the quantum many-body system. Recently, beyond the quantum thermalization, the system which strongly violates th... |
1,941,325,218,289 | arxiv | \section{Introduction}
\def\theequation{\thesection.\arabic{equation}}
\setcounter{equation}{0}
For a finite dimensional Hopf algebra $H$, there is a Yetter-Drinfel'd $\mathcal{D}(H)$-module algebra structure
on the Heisenberg double $\mathcal{H}(H^{*})$ endowed with a heterotic action of the Drinfel'd double $... |
1,941,325,218,290 | arxiv | \section{Introduction}
\label{sec:intro}
Open-domain conversational systems have made significant progress in generating good quality responses
driven by strong pre-trained language models \cite{radford2019language, devlin-etal-2019-bert} and large-scale corpora available for training such models.
However, instead o... |
1,941,325,218,291 | arxiv | \section{Introduction}
Dynamic nuclear polarization (DNP) is an important technique for achieving
highly polarized nuclear spin states. It has a wide range
of applications in electron spin resonance (ESR), nuclear magnetic
resonance, quantum optics and quantum information processing. Doped silicon is widely considered... |
1,941,325,218,292 | arxiv | \section{Introduction}
Identifying causality is a key step yet challenging task in many data-intensive scenarios. In recent years, many influential methods to infer causal network have been proposed. To identify the structure of Bayesian network (BN), \citet{ContinuousOptNIPS2018} proposed a NOTEARS algorithm to learn... |
1,941,325,218,293 | arxiv | \section{Introduction}
All the biochemistry that is essential to life as we know it, takes place in aqueous solutions \cite{harvey2004}. The physical properties of aqueous solutions are strongly dependent on the intermolecular interactions, and typically deviate substantially from ideality \cite{fawcett2004}. In this... |
1,941,325,218,294 | arxiv | \section{Subject}
\section{Introduction} \label{sec:intro}
One of the long-standing problems in the strong interaction theory is to understand the origin of spin effects in hadronic physics
within Quantum Chromodynamics (QCD). To achieve this goal, a promising route is to investigate the mechanisms that are resp... |
1,941,325,218,295 | arxiv | \section*{Introduction}
The financial crisis of 2007-2008 highlighted the enormous effect of contagion
over world bank networks (see e.g. \cite{gai10,elliott14,fink16}). Similar contagion effects appear also in the world trade
which is especially vulnerable to energy crisis mainly related to the trade of petroleum an... |
1,941,325,218,296 | arxiv | \section{Introduction}
In this brief note we study non-hyperelliptic curves of genus 3. The main idea is to determine an equation for the
generic genus 3 curve starting from a covering of full moduli dimension.
Determining the monodromy group of a generic genus $g$ curve covering $\mathbb P^1$ is a problem with ... |
1,941,325,218,297 | arxiv | \section{\label{introduction}Introduction}
Two-dimensional (2D) structures that are inspired by graphene such as hexagonal boron nitride (BN) and transition metal dichalcognides (TMDs) have attracted considerable attentions owing to their remarkable electronic properties \cite{Novoselov2004,Geim2007,Neto2009,Splendiani... |
1,941,325,218,298 | arxiv | \section{Introduction}\label{sec:intro}
In recent years, deep learning models have been particularly effective in dealing with data that have complex internal structures. For example, convolutional neural networks (CNN) are very effective in handling image data in which 2D spatial relationships are critical among the ... |
1,941,325,218,299 | arxiv | \section{\@startsection{section}{1}{\z@}{3.5ex plus 1ex minus
.2ex}{2.3ex plus .2ex}{\large\bf}}
\defAppendix \Alph{section}:{\arabic{section}.}
\def\arabic{section}.\arabic{subsection}.{\arabic{section}.\arabic{subsection}.}
\def\arabic{subsubsection}.{\arabic{subsubsection}.}
\def |
1,941,325,218,300 | arxiv |
\section{Introduction}
\label{sec:introduction}
The current state-of-the-art in all-sky CMB observations is provided
by the \textit{Planck}\ satellite \citep{planck2016-l01}, which observed the
microwave sky in nine frequency bands (30--857\,GHz) between 2009 and
2013. This experiment followed in the footsteps of CO... |
1,941,325,218,301 | arxiv | \section{\label{Sec:Introduction} Introduction}
\section{Introduction}
\begin{figure}[t]
\centering
\includegraphics[width=6cm]{1.eps}
\caption{Schematic representation of atomic levels and available inter level transitions for
generalized JC model.}\label{fig:1}
\end{figure}
Cavity quantum elect... |
1,941,325,218,302 | arxiv | \section{Introduction}
\label{sec:intro}
In the latest years, field theories, and especially conformal field theories, in
3d have become a favorite ground of research. The motivations for this are
related both to gravity and to condensed
matter, see for instance \cite{Maldacena,Huh} and references therein, based on
A... |
1,941,325,218,303 | arxiv | \section{\label{sec:intro}Introduction}
Since many years, beams of spin--polarized particles, ions, and atoms have attracted considerable interest both in fundamental and applied science \cite{Kes95, Blu99, Dap18, Mane.2005b}. In atomic, nuclear and particle physics, for example, many experiments have been performed e... |
1,941,325,218,304 | arxiv |
\section*{References}
\bibliographystyle{unsrtnat}
\section{Introduction}
Recent progress in artificial intelligence has resulted in the development of intelligent agents that can direct their activities towards achieving a goal. Moreover, rapidly advancing infrastructure around conversational technologies ha... |
1,941,325,218,305 | arxiv | \section{Introduction}
\label{intro}
Neural autoregressive models have become the \textit{de facto} standard in a wide range of sequence generation tasks, such as machine translation \cite{bahdanau2014neural}, summarization \cite{rush2015neural} and dialogue systems \cite{vinyals2015neural}. In these studies, a sequen... |
1,941,325,218,306 | arxiv | \section*{0. Introduction}
The study of CR-manifolds and the local analytic structure of real submanifolds of complex space has been a subject of extensive study over last half-century, originated and inspired by E. Bishop's pioneering paper in the 1960's (see [1]). Of particular interest for many mathematicians was th... |
1,941,325,218,307 | arxiv | \section{Introduction}
The demonstration of magnetism in the two-dimensional (2D) limit has long been the focus of fundamental questions in condensed matter physics ~\cite{onsager1944crystal}. In the 1960s, quasi-2D magnetic order has been identified in bulk magnets in which the weak interlayer interactions prevent ma... |
1,941,325,218,308 | arxiv | \section{Introduction}
It was noticed in \cite{LupercioUribeXicotencatl2} that the ring
structure defined in the homology of the loop space of the
symmetric product orbifold (see \cite{LupercioUribeXicotencatl})
induces a ring structure on the cohomology of the inertia
orbifold, by restricting the structure to the con... |
1,941,325,218,309 | arxiv | \section{Introduction}
In the ongoing effort to construct an ultraviolet complete theory of quantum gravity, higher curvature
theories of gravity emerge as corrections to the usual Einstein- Hilbert term. Such theories have now
come to play an important role in cosmology, black hole physics, supergravity, strin... |
1,941,325,218,310 | arxiv | \section*{Acknowledgments}
I am thankful to the Tomsk State University Competitiveness Improvement Program and to RFBR (research project No.~15-02-00293) for a partial support.
|
1,941,325,218,311 | arxiv | \section{Introduction}\label{sec:intro}
In lattice Quantum Chromodynamics (QCD) the Wilson-Dirac operator describes the interaction between quarks and gluons in the framework of quantum field theory. Results of lattice QCD simulations represent essential input to several of the current and planned experiments in elemen... |
1,941,325,218,312 | arxiv | \section{Introduction}
The number of known organic molecules (what is referred to as the {\it known chemical space}) is on the order of $10^6-10^7$ reported structures [1]. This is considerably smaller than the potential structural space of pharmaceutical chemicals (of the order $10^{60}$ [2]), and which itself only r... |
1,941,325,218,313 | arxiv | \section{Introduction}
Scientists and engineers are exploring a vast materials space for cheaper, higher energy-density, and reliable battery materials, in response to the growing demand of portable electronics and electric vehicles.\cite{Hautier2011} Understanding the suitability of the cathode and anode materials, bo... |
1,941,325,218,314 | arxiv | \section{Introduction}
For many years, there has been much interest in characterizing and
understanding complex networks in nature \cite%
{Strogatz01,AlbertBarabasi02,DorogovtsevMendes02,Newman03,EstradaFoxHighamOppo10}%
. While much of the venerable network literature is devoted to static
aspects (e.g., graph theory)... |
1,941,325,218,315 | arxiv | \section{Introduction}
Clusters of galaxies, the most extended gravitationally bound systems in the Universe, are expected to contain a significant population of non-thermal particles.
The mechanisms for producing cosmic rays (CR) in galaxy clusters can be divided into external processes and internal processes.
In e... |
1,941,325,218,316 | arxiv | \section{\label{sec.1}Introduction}
Photon blockade (PB) is a nonclassical anti-bunching effect and satisfies sub-Poissonian light statistics, which is the crucial role to generate and manipulate the single-photon source in most quantum information and computation sciences, such as quantum simulation~\cite{PhysRevLett.... |
1,941,325,218,317 | arxiv | \section{Introduction}
Transient stability assessment is one of the most critical tools for ensuring the reliability of power systems against any potential disturbances and contingencies \cite{kundur94,machowski11}. Due to the nonlinearity of system dynamics, the interconnected generators may not be able to resynchron... |
1,941,325,218,318 | arxiv | \section{Introduction}
The novelty of this contribution is the characterization for which implicit Runge-Kutta schemes for distributed parabolic optimal control problems discretization and optimization commute and the convergence order is preserved. This characterization is done in terms of simplifying assumptions fo... |
1,941,325,218,319 | arxiv | \section{Introduction}
\label{sec:intro}
In the era of precision cosmology, surveys are starting to rely on star-forming galaxies to go further into early cosmic times, when dark energy is just starting to dominate the energy-matter budget of the Universe. Star-forming galaxies with strong nebular emission lines (ELGs)... |
1,941,325,218,320 | arxiv | \section{Introduction}
\label{introduction}
The classical analysis of Krylov subspace solvers for matrix problems with {Hermitian} matrices relies on their spectral properties; see, e.g., \cite{BAxe94,BHac94}. Typically one seeks a preconditioner which {yields parameter} independent bounds for the extreme eigenvalues... |
1,941,325,218,321 | arxiv | \section{Introduction}
\subsection{Proof styles of interactive theorem proving}\label{problem}
\noindent
Interactive theorem provers, also known as proof assistants,
are computer programs for the development and verification
of mathematical texts in a formal language.
These systems make
it \emph{certain}%
\footnote{
... |
1,941,325,218,322 | arxiv | \section{Introduction}
\subsection{Maximal toral subalgebras and restriction}\label{maxtoral}
Let $\fg$ be a Lie superalgebra, not necessarily finite-dimensional. Assume that
$\fg$ contains a subalgebra $\fh$ such that
\begin{itemize}
\item $\ft:=\fh_{\ol{0}}$ has diagonalizable adjoint action on $\fg$ with... |
1,941,325,218,323 | arxiv | \subsection{Continual Learning in healthcare}
\label{sec:related-medical}
Healthcare has been frequently identified as a field prone to distribution shift from training data to deployment \citep{thiagarajan2018understanding, farquhar2018towards, lee2020clinical}. Domain adaptation has been extensively studied in this ... |
1,941,325,218,324 | arxiv |
\section{Manipulability Domain Transfer}
\input{content/problemFormulation}
\subsection{Riemannian-ICP Algorithm}
In the following, we give a detailed description of the novel ICP algorithm for manipulability domain adaptation on the $\spdmanifold{}$ manifold. Our work builds on the EEG classification method b... |
1,941,325,218,325 | arxiv | \section{}
Recently there is an increasing interest in using the spin of
particles, instead of their charge, as a basis for the operation of
a new type of electronic devices. In this work we show via
theoretical calculations that spin degrees of freedom can be
utilized for achieving spatial localization of both charge... |
1,941,325,218,326 | arxiv | \section{Introduction}
Let $G$ be a finite group expressible as a product $G = BC$ of subgroups $B$ and $C$ such that $B \cap C = \{1\}$, sometimes called a \emph{complementary factorisation} of $G$. If $C$ is cyclic, generated by $y$, say, then for every $b \in B$ there exists a unique $b' \in B$ and a unique $j \in... |
1,941,325,218,327 | arxiv | \section{Introduction}
~~~~~In the collision of an energetic particle $p$=$(p_0,{\bb p})$
with $n$ medium particles, how dense must the medium be for the
multiple collisions to become a single coherent (1+$n$)-body
collision, instead of a sequence of $n$ incoherent 2-body collisions?
It is instructive to find out the ... |
1,941,325,218,328 | arxiv | \section{Introduction}
\vspace{-0.8em}
During the last years, significant achievements have been made regarding the rendering capacity and quality of Head Mounted Display (HMD) systems~\cite{Oculusundatedmv}. Modern HMDs can render 360$\degree$ video at a sufficiently high frame-rate and resolution, allowing the viewe... |
1,941,325,218,329 | arxiv | \section*{References}}
\usepackage{geometry}
\usepackage{graphicx}
\usepackage{booktabs}
\usepackage{array}
\usepackage{paralist}
\usepackage{verbatim}
\usepackage{subfig}
\usepackage{natbib}
\usepackage{hyperref}
\usepackage{fancyhdr}
\pagestyle{fancy}
\renewcommand{\headrulewidth}{0pt}
\lhead{}\chead{}\rhead{}
... |
1,941,325,218,330 | arxiv | \chapter{Introduction}
\label{c:intro}
\section{Coxeter Groups}
\label{s:Coxeter}
We start by recalling the definition and some key properties of Coxeter groups.
\begin{defn}
A \textbf{Coxeter system} is a pair $(W, S)$ consisting of a group $W$ and a set of generators $S\subset W$, subject only to relat... |
1,941,325,218,331 | arxiv | \section{Conclusion}
\textbf{This section will be deleted}
\begin{enumerate}
\item Number of Super-PARK data \SW{54}
\item Total data, how many PD, how many Non-pd, no of male, female, etc \SW {Total: 726, PD: 262, NonPD: 464, Male: 325, Female: 401 }
\item a age-distribution plot: say the buckets will be ... |
1,941,325,218,332 | arxiv | \section{Introduction and Definitions}
\noindent Let $\mathcal{A}$ be the class of all analytic functions $f\left(
z\right) $ defined in the open unit disc $\mathbb{D}=\left \{ z\in \mathbb{C}:\left
\vert z\right \vert <1\right \} $ with the power series representation as
\begin{equation}
f(z)=z+\sum \limits_{n=2}^{\i... |
1,941,325,218,333 | arxiv | \section{Introduction} \label{sec:intro}
Strong winds or eruptive events are typical phenomena that lead massive stars to lose large amounts of material during the ark of their lives \citep[e.g.,][]{deJager1988,Vink2001,Mauron2011,Smith2014}. This phenomenon can lead to regions of high-density circumstellar material (C... |
1,941,325,218,334 | arxiv | \section{Introduction}
\gdef\@thefnmark{}\@footnotetext{$^1$Google Brain $^2$DeepMind $^3$Mila, Universit\'e de Montr\'eal $^4$University of Alberta $^5$University of Oxford}
A good representation of state is key to practical success in reinforcement learning.
While early applications used hand-engineered features \ci... |
1,941,325,218,335 | arxiv |
\section{INTRODUCTION}
\label{section1}
Large driving datasets form a basis for the development and safeguarding of highly automated driving functions. Only through a huge amount of recorded real traffic data the human driving behavior can be sufficiently represented and used in simulation for further develo... |
1,941,325,218,336 | arxiv | \chapter{ Introduction}
Light-cone quantization has proven to be a very fruitful approach
to study quantum field theories in 1+1-dimensions
\REF\bp{Hans-Christian Pauli and Stanley Brodsky, Phys. Rev. \us{D32}
1993, (1985); Phys. Rev. \us{D32}, 2001, (1985); Thomas Eller,
Hans-Christian Pauli and Stanley Brodsky, Ph... |
1,941,325,218,337 | arxiv | \section{Introduction}
\label{sec:introduction}
During the last years, several concepts related to the reduction of organizational boundaries, collaboration of several agents (internal and external to the organization) to build products around a common platform have been emerged and contributed to the establishment of... |
1,941,325,218,338 | arxiv | \subsection*{1. Introduction}
The aesthetic appeal of symmetry has been a guide for physicists. In the context of Conformal Field Theory (CFT), the Virasoro symmetry provides a powerful constraint that leads to a partial classification of two-dimensional CFTs \cite{BELAVIN1984333}. The notion of symmetry continues to ... |
1,941,325,218,339 | arxiv |
\section{Conclusion}
In this paper, we proposed a task-oriented network design for sparse feature segmentation. The sparsity prior on target objects can be clearly characterized by mathematical regularizer, while the complicated background needs trainable architectures. So we started from a variational image decom... |
1,941,325,218,340 | arxiv | \section{}
\section{Observations and analyses}
The system was observed during 5 nights from October 2008 to
January 2009 at the Athens University Observatory, using a 40-cm
Cassegrain telescope equipped with the CCD camera ST-8XMEI and B,
V, R, I Bessell filters.
The light curves (hereafter LCs) were analysed with... |
1,941,325,218,341 | arxiv | \section{INTRODUCTION}
The subject of Markov decision process (MDP) has been broadly explored in the area of robotics, wireless communication, and economics. In MDPs, the decision-maker is assumed to have complete state information. Notwithstanding, in many real world application, the direct observation of the state is... |
1,941,325,218,342 | arxiv |
\section{Introduction}
\label{sec:introduction}
We investigate the controlled Schl\"{o}gl system, for time~$t\ge0$,
\begin{subequations}\label{sys-y-u-Cu}
\begin{align}
& \tfrac{\partial}{\partial t} y -\nu\Delta y +(y-\zeta_1)(y-\zeta_2)(y-\zeta_3)=h+U_M^\diamond u,\label{sys-y-u}\\
&y(0)=y_0\in W^{1,2}(\Omega),\qqu... |
1,941,325,218,343 | arxiv | \section{Introduction}
\input{sections/introduction}
\section{Fundamentals}
\label{sec:fund_comp}
\input{sections/fundamental}
\section{Fundamental Algorithms}
\label{sec:fund_alg}
\input{sections/fund_algo}
\section{Deep Reinforcement Learning Versus Evolution Strategies}
This section compares different aspects of DR... |
1,941,325,218,344 | arxiv |
\section{Introduction}
\label{sec:introduction}
Deep Learning (DL) has received considerable attention in recent years due to its
success in areas such as computer vision tasks (e.g., object
recognition~\cite{krizhevsky2012imagenet} and image
generation~\cite{radford2015unsupervised}) using convolution neural networ... |
1,941,325,218,345 | arxiv | \section{Introduction}
\label{section_in}
It is now well known that modern convolutional neural networks \citep[e.g.][]{krizhevsky2012imagenet, simonyan2015very, he2016deep, szegedy2016rethinking} can achieve remarkable performance on large-scale image databases, e.g. ImageNet \citep{deng2009imagenet} and Places 365 \... |
1,941,325,218,346 | arxiv | \section{Introduction}
Nowadays, neural networks have become increasingly popular. They have started penetrating safety critical domains and embedded systems, in which they are often taking important decisions such as autonomous driving cars, rockets, robots, etc.
These neural networks become larger and larger while e... |
1,941,325,218,347 | arxiv |
\section{Introduction}
In the last many years, deep neural networks (DNNs) have achieved impressive results on various computer vision tasks, e.g., image classification~\cite{alex12imagenet}, face/object recognition~\cite{DBLP:journals/corr/HeZR015,DBLP:journals/corr/abs-1801-07698}, and semantic segmentation~\cite{... |
1,941,325,218,348 | arxiv | \section{Investigating transport inside re-healed flux surfaces}\label{sec:Istvan}
This section explores further the ten-order-of-magnitude difference in the predicted RE\xspace current when transport is/not accounted for within NIMROD\xspace's islands and re-healed flux surfaces. Radial profiles of the diffusion ... |
1,941,325,218,349 | arxiv | \section*{Acknowledgments}
We thank Prof.\ Schamel for providing this opportunity to further substantiate the validity of our results.
The numerical simulations were performed on the FERMI supercomputer at CINECA (Bologna, Italy), within the European project PRACE Pra04-771. P.J.M.\ was supported by Department of E... |
1,941,325,218,350 | arxiv | \section{Introduction}
Traditionally, the complex structure of a complex manifold $X$ is encoded in the sheaf of holomorphic functions $\mc{O}_X$. For applications to noncommutative geometry, such local constructions are not available and we are forced to use global differential geometric constructions. When the man... |
1,941,325,218,351 | arxiv | \section{Introduction}
Suppose that $M$ is a tracial von Neumann algebra and $N$ is a subalgebra of $M$. In this paper, we consider the following question: How ``hard'' is it to compute the conditional expectation function $E_N:M\to N$? In other words, given $x\in M$, how ``hard'' is it to compute the distance from... |
1,941,325,218,352 | arxiv | \section{Introduction}
\subsection{Compact ellipticals (cEs) and ultra compact dwarfs (UCDs)}
In the magnitude-surface brightness plane of stellar systems, early-type
galaxies populate a well defined sequence of increasing central surface
brightness with increasing total luminosity (Jerjen \& Binggeli
\cite{Jerjen97a},... |
1,941,325,218,353 | arxiv | \section{Introduction}
At present, merging black holes are the only directly detected source of gravitational waves~\cite{PhysRevLett.116.061102, PhysRevLett.116.241102, PhysRevLett.116.241103, PhysRevD.93.122003, PhysRevX.6.041014, PhysRevX.6.041015, GW150914_systematics, GW150914_applications, PhysRevLett.116.13110... |
1,941,325,218,354 | arxiv | \section{Introduction}
In this paper, we shall consider a homogenization limit as $\varepsilon \to 0_+$ of nonnegative weak solutions $u_\varepsilon = u_\varepsilon(x,t)$ for the following Cauchy-Dirichlet problem:
\begin{alignat}{4}
\partial_t u_\varepsilon &= \mathrm{div} \Big( a(\tfrac x \varepsilon, \tfrac t {\var... |
1,941,325,218,355 | arxiv | \section{Introduction}
\vspace{-2mm}
Unmanned aerial vehicles (UAVs) have found numerous interesting applications, due to its highly controllable mobility and swift deployment \cite{Access}. To support the various missions of UAVs, it is of paramount importance to realize high-quality UAV-to-ground communications. A pr... |
1,941,325,218,356 | arxiv | \section{Models and methods}
\label{sec:model}
The SIS model is defined as follows. Individuals lie in the vertices
of a quenched network of size $N$ and can be in two states: infected
or susceptible. An infected individual $i$ becomes spontaneously
susceptible with rate $1$, while a susceptible one turns to the
in... |
1,941,325,218,357 | arxiv | \section{Introduction}
For a Morse function $f$ on a compact manifold $M$, and choosing a Riemannian metric $g$ on $M$. In [1], Witten introduces a chain complex and the homology groups of $M$ by studing the negative gradient vector field associated to $(f,g)$, and he claimes that these groups are the ordinary homolog... |
1,941,325,218,358 | arxiv | \section{Introduction}
\label{sec:intro}
Smart Cities pervasively deploy video cameras for information collection \cite{xu2018real} and Situation Awareness (SAW). While cameras enable 24-7 continuous collection of city footprints, the huge amount of video data brings new challenges, among which the top two are the sca... |
1,941,325,218,359 | arxiv | \section{Introduction}
Fix a finite set $I$ and let $\mathbb{C}\{I\}$ be the algebra of functions on $I$. It is a commutative semisimple algebra. For each $i \in I$ there is an idempotent $e_i$, which satisfies $e_i(j) = \delta_{ij}$ for all $j \in I$. Any right $\mathbb{C}\{I\}$ module $M$ is an $I$ graded vector s... |
1,941,325,218,360 | arxiv | \section*{Author Summary}
It is well known that HIV can evolve to become drug resistant if it acquires specific drug-resistance mutations, but the underlying population genetic processes are not well understood. We found that the evolution of drug resistance in HIV populations within infected patients occurs by one mu... |
1,941,325,218,361 | arxiv | \section{Introduction}
{\it Cosmicflows} \citep{2012ApJ...749...78T,2012ApJ...749..174C,2012AN....333..436C,2013AJ....146...86T} is a project to map radial peculiar velocities of galaxies within 200 Mpc with the ultimate goal of reconstructing and simulating the motions of the large-scale structures and explaining the... |
1,941,325,218,362 | arxiv | \section{Introduction}
(Super)cocycles play an important role in the study of the geometric and topological
structures associated with physical theories (see \cite{dAI} for an earlier survey). In \cite{Bouq}
we discussed cocycles of super $L_\infty$-algebras (super Lie $n$-algebras for arbitrary $n$)
forming the \e... |
1,941,325,218,363 | arxiv | \section{Introduction}
\label{sec:intro}
The \textit{Fermi} bubbles are a prominent feature in the $\gamma$-ray sky, and are arguably one of the most remarkable findings of the \textit{Fermi} $\gamma$-ray space telescope to date~\citep{Su2010ApJ, Dobler2010ApJ, Ackermann2014ApJ}.
These giant $\gamma$-ray lobe struc... |
1,941,325,218,364 | arxiv | \section{Introduction}
The standard Pearson's correlation coefficient only provides information about the strength of a linear relationship between two variables. It cannot be used to establish the direction of the relation. However, in many economic and medical applications, the analysis and further inference should ... |
1,941,325,218,365 | arxiv |
\subsection{Out-of-sample performance}%
\label{sec:exps-oos}
We compare the reliability of (\text{DRC}{}) with the sample average approximation formulation:
\begin{align*}
\min ~~
& c^{\top}x, \\
\st{} ~~
& \frac{1}{N} \sum_{j = 1}^N z_j \geq 1 - \epsilon, \tag{\text{SAA}{}}\\
& x^{\top} \hat{\xi}^j_i - v_i... |
1,941,325,218,366 | arxiv | \section{Introduction}
A Hermitian metric $g$ on a complex manifold is locally conformal K\"ahler (LCK) if there exists a closed $1$-form $\theta$ (called the Lee from) such that $d\omega=\theta\wedge \omega$ where $\omega$ is the fundamental form of $g$.
A LCK metric $g$ is Vaisman if the Lee form $\theta$ is paral... |
1,941,325,218,367 | arxiv | \section{acknowledgments}
We thank T.~Forrest, D.~Voneshen, A.P.~Petrovi\'{c}, Y.~Ohtsubo, and C.~Berthod for useful discussions. We thank T.~K.~Kim and D.~Daisenberger for technical assistance. We thank Diamond Light Source for access to Beamline I05 (Proposals No. SI13797 and NT14572) that contributed to the results... |
1,941,325,218,368 | arxiv | \section{Introduction}\label{sec1}
Let $(\Omega,{\mathcal F}, ({\mathcal F}_t)_{t \geq0},{\mathbb P})$ be
a filtered probability space endowed with an $({\mathcal F}_t)_{t \geq
0}$-adapted Brownian motion $(W_t)_{t \geq0}$. On $(\Omega,{\mathcal
F},\break ({\mathcal F}_t)_{t \geq0},{\mathbb P})$ we consider ... |
1,941,325,218,369 | arxiv | \section{Introduction}\label{Intro}
Cross-domain text classification considers the setting that data distributions in source domain and target domain are different but related.
In such a scenario, the performance of traditional classification algorithms, which are built on the assumption that the source and target dat... |
1,941,325,218,370 | arxiv | \section{Introduction}
Accretion of magnetized hot plasma onto compact objects (such as neutron stars and black holes) is one of the most efficient mechanisms in the Universe in producing high-energy radiation. The astrophysical sources powered up by such a process include active galactic nuclei (AGNs, \cite{Marconi:20... |
1,941,325,218,371 | arxiv | \section{Introduction}
The use of chiral Lagrangians in combination with unitary techniques in coupled
channels of mesons and baryons has been a very fruitful scheme to study the
nature of many hadron resonances. The analysis of meson
baryon scattering amplitudes shows poles in the second Riemann sheet which are
iden... |
1,941,325,218,372 | arxiv | \section{Preliminary Results}\label{appendix:preliminary_results}
In this appendix we derive several results that we will use to prove the main results of the paper given by Proposition~\ref{prop:nash}~to~\ref{prop:filtering_expert}. For this, we consider communities given by $C=(C_d,C_s)$ which have the property that
... |
1,941,325,218,373 | arxiv | \section{Introduction}
A subset $Y$ of a metric space $(X,d)$ is a {\it separated net} (or Delone set) if for some $0<c<C$, any two $c$-balls centered at distinct elements of $Y$ are disjoint (i.e. $Y$ is uniformly discrete), and the $C$-neighborhood of $Y$ is all of $X$ (i.e. $Y$ is coarsely dense). Separated nets are... |
1,941,325,218,374 | arxiv | \section{Introduction}
In this paper we consider the following quasilinear elliptic problem in
$\mathbb{R}^{N}$
\begin{equation}
-\operatorname{div}(\phi(|\nabla u|)\nabla u)+V(x)\phi(\left\vert u\right\vert
)u=f(u)\text{,\qquad}u\in W^{1,\Phi}(\mathbb{R}^{N})\text{.}\label{e1
\end{equation}
where $\phi:[0,\inft... |
1,941,325,218,375 | arxiv | \section{Introduction}
The study of the properties of nuclei far from stability is one of the main frontiers of modern nuclear physics.
Among many possible observables for nuclear structure, the $\beta$-decay strengths provide important testing grounds for nuclear structure theories far from stability. The mechanism ... |
1,941,325,218,376 | arxiv | \section{Introduction}\label{intro}
Geological CO\ensuremath{_\textrm{2}}\xspace storage can be successfully implemented in deep saline aquifers that possess favorable characteristics \citep{IPCC2005}, e.g., the storage formation has sufficient capacity, injectivity, and containment properties to store the desired qua... |
1,941,325,218,377 | arxiv | \section{Introduction}
Standard cosmology is based on the Friedmann-Robertson-Walker (FRW) metric for a spatially
homogeneous and isotropic three-dimensional space. In terms of the proper time $t$ measured
by a comoving observer, and the corresponding radial ($r$) and angular ($\theta$ and $\phi$)
coordinates in th... |
1,941,325,218,378 | arxiv | \section{Introduction}
In an earlier paper \cite{ramsey:1997b} we studied the effect of parametric
particle creation on the inflaton dynamics in the post-inflation,
``preheating'' stage. It was shown that analysis of the dominant physical
processes during the early stages of reheating necessitates consideration
of se... |
1,941,325,218,379 | arxiv | \section{Introduction: viable wormhole models at last}
It is well known that traversable wormholes require exotic matter to
prevent self-collapse \cite{MT88}. Such matter is confined to a small
region around the throat, a region in which the weak energy condition
is violated. While it is desirable to keep this reg... |
1,941,325,218,380 | arxiv | \section*{Main}
\textbf{
\noindent
The Large Magellanic Cloud is the most massive satellite galaxy of the Milky Way, with an estimated mass exceeding a tenth of the mass of the Milky Way\cite{besla10,boylankolchin11,penarrubia16,shao18,erkal19}. Just past its closest approach of about 50 kpc, and flying by the Milky W... |
1,941,325,218,381 | arxiv | \section{Introduction}\label{sec:intro}
\noindent
There are various ways how self-adaptation following the MAPE-K feedback loop~\cite{Kephart&Chess2003} and in particular the analyzing and planning phases of the feedback loop can be realized.
On the one hand, \emph{rule-based} approaches~\cite{1537890,4061119} combin... |
1,941,325,218,382 | arxiv | \section{Introduction}
Gravitational-wave (GW) astronomy is rapidly entering a data-driven regime where astrophysical modeling uncertainties are becoming the key limiting factor.
The most popular astrophysical formation channels for the merging black-hole (BH) binaries detected by LIGO and Virgo include isolated bina... |
1,941,325,218,383 | arxiv | \section{Introduction}\label{sec:Introduction}
Over the past two decades, Bose-Einstein condensates (BECs) of ultracold atomic gases have become an ideal system to study both quantum and nonlinear dynamics, due to the high controllability over the two-body interactions~\cite{Smith2013}, trapping potentials~\cite{Pethic... |
1,941,325,218,384 | arxiv | \section{Introduction}
The Einstein-Gauss-Bonnet (EGB) gravity is one of the most promising
candidates for modified gravity \cite{Clifton2011}. This theory is a special case of the Lovelock gravity which
is the natural generalization of general relativity in higher dimensions
\cite{Lovelock1971}. It has
second... |
1,941,325,218,385 | arxiv |
\section{Introduction}
By {\em non-normal logics} we understand in this paper those propositional logics algebraically captured by varieties of {\em Boolean algebra expansions}, i.e.~algebras $\mathbb{A} = (\mathbb{B}, \mathcal{F}^\mathbb{A},$ $\mathcal{G}^\mathbb{A})$ such that $\mathbb{B}$ is a Boolean algebra, and ... |
1,941,325,218,386 | arxiv |
\section{Introduction}
Advances in computation and machine learning have enabled Deep Neural Networks (DNNs) to become the algorithm of choice for large-scale image classification \cite{krizhevsky2012imagenet, simonyan2014very, he2016deep}. To further understand the types of features that computer vision DNNs learn, \... |
1,941,325,218,387 | arxiv | \section{#1\label{sec-#1}}}
\newcommand{\ssecs}[1]{\subsection{#1\label{ssec-#1}}}
\newcommand{\sssecs}[1]{\subsubsection{#1\label{sssec-#1}}}
\newcommand{\fig}[4]{\begin{figure}[#4]\centering\includegraphics[width=#3\textwidth]{Graph-#1.pdf}\caption{#2}\label{fig-#1}\end{figure}}
\newcommand{\figa}[3]{\begin{figure}[#... |
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