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1,116,691,500,415 | arxiv | \section*{Introduction}
\addcontentsline{toc}{section}{Introduction}
General relativity (GR) and quantum mechanics are two of the best verif\/ied theories of modern physics. While general
relativity has been spectacularly successful in explaining the universe at astronomical and cosmological scales, quantum mechanics ... |
1,116,691,500,416 | arxiv | \section{Introduction}
Perhaps the most prominent application of optimization in ML is the empirical risk minimization problem. However, inspired by the success of GANs~\cite{NIPS2014_5ca3e9b1}, ML practictioners have developed more complicated min-max and adversarial optimization formulations
\cite{yu2021fast,kuhn20... |
1,116,691,500,417 | arxiv | \section{Introduction}
Real time processes at finite temperature play an essential role in
the physics of the early universe and of heavy ion collisions. A key
quantity in scenarios of baryogenesis~\cite{kuzmin,rs} is the rate for
electroweak baryon number violation (the sphaleron rate). In the broken
phase the sphale... |
1,116,691,500,418 | arxiv | \section{Introduction and Motivation}
Exact solutions of Einstein's Field Equations
\begin{equation}
G_{\mu\nu} = \kappa T_{\mu\nu} \label{ee}
\end{equation}
are, of course, of interest for various purposes. Since the equations are very complicated, to find solutions one often makes simplifying assumptio... |
1,116,691,500,419 | arxiv | \section{Introduction}
\label{sec:intro}
The production of bottom quarks has been extensively studied at hadron colliders. Early measurements were already carried out by the UA1 collaboration at the CERN S$p{\bar p}$S~\cite{Albajar:1986iu,Albajar:1988th}
and, subsequently,
by the CDF~\cite{Abe:1995dv,Acosta:2001rz,Acos... |
1,116,691,500,420 | arxiv | \section{Introduction}
Dark matter is a crucial ingredient in the cosmological history of the universe and accounts for about 27\% of the energy budget in the universe today.
As its existence is supported by galactic-scale to cosmological-scale gravity-based evidence, various experiments were performed, are operation... |
1,116,691,500,421 | arxiv | \section{Introduction}
The study of quantum mechanics in periodic structures is one of the central
topics in condensed matter physics since many decades \cite{Ashcroft}. The
behavior of electrons in a crystal or, more generally, interacting particles
in a periodic potential, even at the few-body level, puts forward a ... |
1,116,691,500,422 | arxiv | \section{Introduction}
A quadratic extension of a cyclotomic field, which is non-abelian Galois
over the rational number field $\Bbb Q$, is called a quasi-cyclotomic field.
All quasi-cyclotomic fields are described explicitly in [8] followed the works
in [1] and [3]. They are generated by a canonical $\mathbb Z/2\mathb... |
1,116,691,500,423 | arxiv | \section{Introduction}
The corrosion of a metal after the damage of its protective layer is a problem
of wide technological interest. The evolution of the
corrosion front is the result of a competition between localized dissolution
and passivation processes. The latter consists of the formation of a
passivation layer ... |
1,116,691,500,424 | arxiv | \section{Introduction}
The idea behind the Minkowski curvature flow treated in \cite{mink} is to consider the plane $\mathbb{R}^2$ with a different norm and study the motion of curves evolving by the minkowskian curvature in this new context. But, since we are working with (almost) arbitrary norms in $\mathbb{R}^2$ is... |
1,116,691,500,425 | arxiv | \section{Introduction}
In \cite{Manu:2020tty}, we studied aspects of entanglement and quantum
extremal surfaces (QES) in various families of holographic spacetimes
exhibiting cosmological singularities. This is inspired by the
exciting discoveries made recently on the black hole information
paradox
\cite{Penington:20... |
1,116,691,500,426 | arxiv | \section{Introduction}
The Standard Model (SM) accounts for almost all experimental high
energy physics data; however, the observation of neutrino oscillations
requires that the SM be extended to include nonzero neutrino masses.
While there are many ways to expand the SM to account for
neutrino oscillations, we attemp... |
1,116,691,500,427 | arxiv | \section{Introduction}
\IEEEPARstart{R}{ecent} years have witnessed the rapid evolution of communication technologies and fast proliferation of Internet of Things (IoT) devices with growing capabilities of data gathering, analyzing and knowledge utilization assisted by wireless networks~\cite{1,2,3,4}, which also enab... |
1,116,691,500,428 | arxiv | \section{Introduction}
\label{sec_intro}
In four-dimensional General Relativity, a fundamental connection between geometric optics and the algebraic structure of the Weyl tensor is provided by the Goldberg-Sachs (GS) theorem \cite{GolSac62,NP}, which states that an Einstein spacetime is algebraically special ... |
1,116,691,500,429 | arxiv |
\section{Introduction}\label{sec:intro}
Memristors are used for memory applications~\cite{Niu2010, Ho2011, Mohammad2013, Baghel2015, Radakovits2019}, where even storage of multiple bits per device is feasible~\cite{zangeneh_design_of_1t1r_reram,kim2010cnna,Taherinejad2015ems,Taherinejad2016cce}. In addition, memristo... |
1,116,691,500,430 | arxiv | \section{\bf Introduction and main results}
\smallskip
\noindent The long-standing famous Nagata conjecture for characteristic $0$ was proved
by Shestakov and Umirbaev \cite{SU1, SU2}, and a strong version
of the Nagata conjecture was proved by Umirbaev and Yu \cite{UY}.
That is, the Nagata automorphism
$(x-2y(y^2+x... |
1,116,691,500,431 | arxiv | \section{Introduction}
Recommender systems (RS) are a popular strategy to enable personalized users' experience \cite{ricci}.
Historical data (e.g., browsing activity and ratings) and product characteristics (e.g., title and description) are well-recognized data sources to train RSs.
Product information is often augme... |
1,116,691,500,432 | arxiv | \section{Introduction}
\label{Introduction}
Nowadays, the ubiquitous nature of mobile and wearable devices has allowed users to access a multitude of new applications, services and content. More and more personal related information is stored on (or accessed via) personal devices such as smart phones, which enhances u... |
1,116,691,500,433 | arxiv | \section{\label{sec1} Introduction}
Quantum walk(QW) is an extension of the classical random walk, in which the walker
is controlled by a quantum mechanical variable \cite{a2,PhysRevA.48.1687}.
The quantum interference from different walk paths brings about QW novel and
interesting features. An motivation for wor... |
1,116,691,500,434 | arxiv | \section{Gordon's integral: Introduction}
\noindent Among the important integrals in theoretical and mathematical physics is W. Gordon's integral \cite{gordon}, see also \cite{karule,landau,saad2003,tarasov2003},
\begin{align}\label{integral1}
\operatorname {J}_c^{j(\pm p)}(b,b';\lambda,w,z)&=\int_0^\infty x^{c+j-1}e^{... |
1,116,691,500,435 | arxiv | \section{INTRODUCTION}
\label{sec:intro}
Because Lyman $\alpha$ emission is easily quenched by dust,
the Lyman Alpha Emitting galaxies (LAEs)
are often characterized as protogalaxies experiencing their
first burst of star formation \citep{hum96}.
However, the differing behavior of Lyman $\alpha$ and
continuum ph... |
1,116,691,500,436 | arxiv | \section{Introduction}\label{sec:intro}
In this paper we propose a (1) general factorization framework (GFF) that (2) works also on implicit feedback data; (3) integrates recommendation context into the model; (4) and is flexible enough to employ the various underlying relationships of dimensions allowing us to adequa... |
1,116,691,500,437 | arxiv | \section{Introduction}
With the end of the {\em Spitzer} cold phase and the widespread availability of 8~$\mu$m and 24~$\mu$m bands observations in the archives, the availability of relations to determine the total infrared (TIR) emission from these wave bands by themselves is crucial to efficiently exploit the archiv... |
1,116,691,500,438 | arxiv | \section{Introduction}
We consider a unique continuation (or data assimilation) problem for the Helmholtz equation
\begin{align}\label{helholtz_intro}
\Delta u + k^2 u = -f,
\end{align}
and introduce a stabilized finite element method (FEM) to solve the problem computationally.
Such methods have been previousl... |
1,116,691,500,439 | arxiv | \section{Summary:}
While achieving a compression ratio of 2.0 bits$\slash$base ,the new
algorithm codes non-N bases\footnote{``non-N bases" refers to bases excpet N.Thus A,T,G or C. \ N stands for unknown base.} in fixed length.It dramatically reduces the time
of coding and decoding than previous DNA compression algori... |
1,116,691,500,440 | arxiv | \section{Introduction}
The Sloan Digital Sky Survey (SDSS)~\citep{Yo00} is an imaging and
spectroscopic survey that has now mapped over $ 1/4$ of the sky. It
has already proven to be a powerful tool for the identification of
Galactic substructure. For example, \citet{Ne02} and \citet{Ya03}
identified a ring at low Gal... |
1,116,691,500,441 | arxiv | \section{Introduction}
Let $V$ be a $2n$-dimensional vector space over the finite field $\F_q$. A {\it spread} $\cS$ of $V$ is a collection of $n$-dimensional subspaces that partitions the nonzero vectors in $V$. The members of $\cS$ are the {\it components}, and $V$ is the {\it ambient space}. The {\it kernel} is ... |
1,116,691,500,442 | arxiv | \section{Introduction}
In this paper we study existence and uniqueness of rational normal
curves in $\mathbb{P}^n$ passing through a given set of points and
intersecting some codimension two linear spaces in a very natural
way. More precisely, we require the curve to intersect each linear
space in $n-1$ distinct point... |
1,116,691,500,443 | arxiv | \section{Introduction}
Texts in scenes play an important role in communication between a machine and its surrounding environments. Automated machine understanding of texts in scenes has a vast range of applications such as navigation assistance for the visually impaired \cite{OrCam}, scene text translation for tourists... |
1,116,691,500,444 | arxiv | \section{Introduction}
In the last five decades
pseudo-differential operators
have become a standard tool in the study of partial differential equations.
It is natural to try
to define analogues of the Euclidean pseudo-differential calculus in other settings.
On one hand, while it is always possible to obtain a loc... |
1,116,691,500,445 | arxiv | \section{Introduction}
The long standing problem of finding an exact description of the CFT dual to
M-theory on $AdS_4\times S^7$ (and orbifolds thereof), or the low energy limit of the world volume theory
of $N$ coinciding M2-branes, was solved beautifully in a recent paper of
Aharony, Bergman, Jafferis and Maldacena... |
1,116,691,500,446 | arxiv | \section{KENN\ architecture}
\label{sec:architecture}
As seen in Section~\ref{sec:kenn}, the core of KENN\ method is in the TBF . In KENN\ the TBF is applied inside a \emph{Clause Enhancer} (CE), which is a module instantiated for each grounded clause $c$ that calculates function $\delta_c$ as defined in Equation~\ref... |
1,116,691,500,447 | arxiv | \section{Introduction}
The invention of the Loop algorithm\cite{Evertz} was a major breakthrough for Monte Carlo
simulations of quantum spin systems. This algorithm which is a quantum version of the
Swendsen-Wang cluster algorithm\cite{Kawashima} has many desirable features which makes it possible to study large
system... |
1,116,691,500,448 | arxiv | \section{Introduction and results}
\subsection{Context}
Consider a real separable Hilbert space $\mathcal{H}$ equipped with the Hilbertian inner product $\langle\cdot,\cdot\rangle$ and the associated norm $\|\cdot\|$. The set of bounded operators from $\mathcal{H}$ to $\mathcal{H}$ will be denoted by $\mathcal{L}(\ma... |
1,116,691,500,449 | arxiv | \section{Introduction}
It is well-known that physics beyond the Standard Model (SM) must exist in order to address a number of outstanding questions such as
the nature of dark matter, the generation of neutrino masses, the origin of the observed baryon asymmetry and
the solution to the hierarchy problem -- all of whi... |
1,116,691,500,450 | arxiv | \section{Introduction}
\para{}
A topological superconductor (SC) has a superconducting gap in the bulk but protected Majorana fermions on the boundaries or in the cores of vortices in an externally applied magnetic field \cite{qi-rmp-2011,sato-rpp-2017}.
There has been considerable excitement about the search for to... |
1,116,691,500,451 | arxiv | \section{Introduction}
Given a multigraph $G=(V,E)$, the {\em edge-coloring problem} (ECP) is to color the edges of $G$ with the minimum
number of colors so that no two adjacent edges have the same color. Its optimal value is called the {\em chromatic
index} of $G$, denoted by $\chi'(G)$. In addition to its great t... |
1,116,691,500,452 | arxiv | \section{Introduction}\label{section1}
Traditionally, magnetic reconnection and MHD wave theory have been viewed as separate areas of solar physics (see, e.g., Priest \& Forbes \cite{magneticreconnection2000}; Roberts \cite{Bernie}; De Moortel \cite{DeMoortel2005}; Nakariakov \& Verwichte \cite{NV2005}; De Moo... |
1,116,691,500,453 | arxiv | \section{Introduction}
The convolutional codes are widely used in digital communication systems to correct the transmission errors, which have been adopted by almost all advanced wireless communication standards. There are strong requirements to develop high performance decoding components with good scalability and r... |
1,116,691,500,454 | arxiv | \section{Introduction}
The study of metal poor, compact star forming galaxies was initiated
by \citet{sarsearl72}. Their importance was rapidly recognized because they were
considered to be ideal benchmarks in the study of the earliest stages of galaxy
evolution, and were studied in many works
(\citet{campbell88,pagel... |
1,116,691,500,455 | arxiv |
\section{Introduction} \vspace{-0.6em}
\noindent
The identification of dynamical systems from data is a powerful tool in Robotics \cite{aastrom1971system}.
Learnt analytic models may be used for control synthesis and can be utilized for gravitational and inertial compensation \cite{spong2020robot}.
Moreover, when use... |
1,116,691,500,456 | arxiv | \section{Two convex relaxations for sparse linear regression}
Given a collection of observed sample points $(x_i, y_i) \in \mathbb{R}^p \times \mathcal{Y}$, the goal
of a sparse learning task is to learn a linear function $x \mapsto \beta^T x$ that is then used
to predict an outcome of $y\in \mathcal{Y}$ for future/... |
1,116,691,500,457 | arxiv | \section{Introduction}
Dialog based interaction between a customer and a bot may become tedious and irrelevant if the system’s beliefs are not consistent with the set of beliefs of the customer. Beliefs are cognitive representational states that represent the presumed context of the conversation perceived by each agent... |
1,116,691,500,458 | arxiv | \section{Introduction}
\label{sec:1}
microRNAs (miRNAs) --short, endogenous, noncoding RNAs that operate post-transcriptionally via sequence-specific binding to target RNAs-- are increasingly recognized as key actors in the regulation of eukaryotic gene expression \cite{bartel,flynt,cech,gurt,metaz}. Following transcr... |
1,116,691,500,459 | arxiv | \section{Introduction}
Predicting pedestrian trajectory is an essential task for accomplishing mobility-based jobs in naturalistic environments, such as robotics navigation in crowded areas, safe autonomous driving and many other applications that require foreseeing motion in an interactive dynamical system. Existing l... |
1,116,691,500,460 | arxiv | \section{Introduction}
Let $G$ be a connected reductive algebraic group defined over a
field $k$ of characteristic not $2$, $\theta$ a $k$-involution of $G$, i.e. a
$k$-automorphism of $G$ of order two,
$H$ a $k$-open subgroup of the fixed point group
of $\theta$ and $G_k$ (resp. $H_k$) the set of $k$-rational points... |
1,116,691,500,461 | arxiv | \section{Introduction}
All topological spaces under consideration are assumed to be $T_1$ and Hausdorff.
A \emph{Dowker space} is a normal topological space whose product with the unit interval is not normal.
Dowker \cite{Dowker_C.H.} raised the question of their very existence, and
gave a useful characterizatio... |
1,116,691,500,462 | arxiv | \section{Introduction}
The \emph{maximum-entropy sampling problem}, a fundamental problem in optimal statistical design,
was formally introduced in \cite{SW} and then applied in many areas such as
the re-design of environmental-monitoring networks (see \cite{ZidekSunLe2000}, for example).
In the Gaussian case, the pr... |
1,116,691,500,463 | arxiv | \section{Introduction}
Advanced vehicle control algorithms are crucial for the development of safe and reliable \textcolor{black}{autonomous driving (AD)} applications to reduce road accidents and causalities~\cite{DO2021104856}. Conventional control designs such as PID and linear state feedback often serve in low-le... |
1,116,691,500,464 | arxiv | \section*{SUMMARY}
Artificial Intelligence (AI) applications can profoundly impact society. Recently, there has been extensive interest in studying how scientists design AI systems for general tasks. However, it remains an open question about whether the AI systems developed in this way can work as expected in differe... |
1,116,691,500,465 | arxiv | \section{Introduction}
After Hawking's famous work \cite{Hawking:1974rv} - the black holes radiate - known as {\it{Hawking effect}}, it is now well understood that it is related to the event horizon of a black hole. A closely related effect is the {\it{Unruh effect}} \cite{Unruh:1976db}, where a similar type o... |
1,116,691,500,466 | arxiv | \section{Introduction}
A complex behavior of the normal state transport properties in the copper high temperature superconductors (HTSC) have been studied for a long time. Nevertheless, up to now there is no consistent description for some basic transport properties of copper HTSC as, for example, for an unusual temper... |
1,116,691,500,467 | arxiv | \section{Introduction}
\label{sec:intro}
\begin{figure
\centering
\includegraphics[width=0.5\textwidth]{feature1.png}
\caption{\label{fig:feature} An illustration of the feature scattering mechanism. The classical inflationary trajectory is featureless. However, because of the quantum fluctuation of the isocurva... |
1,116,691,500,468 | arxiv | \section{Introduction}
Egocentric action anticipation \cite{damen2020epic} is receiving increasing attention recently, which aims to anticipate what the subject to do next based on the recordings from egocentric cameras. Different from the third-person action anticipation, it actually records what the subject observes ... |
1,116,691,500,469 | arxiv | \section{Introduction} \label{introduction}
After the remarkable discovery of Cachazo, He, and Yuan (CHY) \cite{Cachazo:2013hca, Cachazo:2013iea, Cachazo:2014xea} of general compact formulae for tree-level amplitudes as integrals over the space of punctured Riemann spheres localized over the so-called \textit{scatteri... |
1,116,691,500,470 | arxiv | \section{Introduction}
Given the advent of Graphics Processing Units (GPUs), deep convolutional neural networks (CNNs) with billions of floating number multiplications could receive speed-ups and make important strides in a large variety of computer vision tasks, \eg image classification~\cite{VGG,krizhevsky2012imagene... |
1,116,691,500,471 | arxiv | \section{Introduction}
\subsection*{Background}
This paper concerns dif\/ferential geometry in dimensions one to four, and (primarily) four kinds of geometric structure,
one in each dimension, governed by four nonlinear integrable dif\/ferential equations.
Associated to each manifold carrying one of these geometric s... |
1,116,691,500,472 | arxiv | \section{Introduction}
Supersymmetric models with extra dimensions
has attracted interest.
Since extra dimensions and supersymmetry have not been discovered,
these must be invisible
at low scales.
One of the simple ways to compactify extra dimensions and
break supersymmetry simultaneously
is the Scherk-Schwarz mech... |
1,116,691,500,473 | arxiv | \section{Classical Lagrange and Wolfe \\dual programs}
In this Section, we re-discuss the well-known programs with
holonomic constraints insisting on the following issues \cite{B}, \cite{H}, \cite{R}:
(i) the Lagrange-dual problem with weak respectively strong duality;
(ii) the Wolfe-dual problem; (iii) pertinent ex... |
1,116,691,500,474 | arxiv | \section{Introduction}
A long time has been passed since a straight double helical
structure had been proposed by Watson and Crick as relaxed
configuration of a DNA, but today, we know it
can almost never be found in this form in nature. The macromolecule
is able to play its important and essential role in the life,... |
1,116,691,500,475 | arxiv | \section{Introduction
The main purpose of this paper is to deepen the study of qualitative theory of differential equations induced by differentiable vector fields of the plane which are not necessarily of class $C^1$. For instance, problems addressed in \cite{MR2096702, MR2287882,MR2266382} include global injectivity... |
1,116,691,500,476 | arxiv | \section{Introduction}
In 1914, Ramanujan \cite{Ramanujan} gave a number of rapidly convergent series of $1/\pi$. Although the following series, due to Bauer \cite{Bauer},
is not listed in \cite{Ramanujan}, it gives an example of this kind:
\begin{align}
\sum^{\infty}_{k=0}(-1)^k(4k+1)\frac{(\frac{1}{2})_k^3}{k!^3... |
1,116,691,500,477 | arxiv | \section{Introduction}
Recently, deep neural networks is used to model implicit representations of 3D shapes has been widely applied for reconstruction \cite{duggal2021secrets}, generation \cite{chen2019learning}, compression \cite{tang2020deep} and rendering \cite{remelli2020meshsdf, takikawa2021neural}.
As one of th... |
1,116,691,500,478 | arxiv | \section*{Appendix}
\subsection*{A. Transference Formalism and Proofs}
\begin{example}[Freeze Quantification]
Suppose we want to express that whenever the event $Q$ occurs, it is followed
later by $R$, and then by $S$, such that the time difference between occurrences
of $Q$ and $R$ is at most $5$, and also the time ... |
1,116,691,500,479 | arxiv | \section{Introduction}
\hspace*{0.5 cm}Let $\Omega\subset {\bf R}^N$ be a bounded domain
with a $C^2$-smooth boundary $\partial\Omega$ and let
$\omega\subset\Omega$ be a subdomain. Write $Q=\Omega \times (0,T)$
with $T>0$ and write $\Sigma=\partial\Omega\times (0,T) $. Consider
the following parabolic equation:
$$
\l... |
1,116,691,500,480 | arxiv | \section{Introduction}\label{section Introduction}
Geometric group theorists traditionally restrict their attention to finitely
generated groups equipped with a word metric. A typical proof of \v Svarc-Milnor Lemma
(see \cite{Roe lectures} or \cite{Bridson-HaefligerBook}, p.140) involves such metrics. Recently, the st... |
1,116,691,500,481 | arxiv |
\section{Introduction}
\begin{figure}[h]
\centering
\includegraphics[width=0.85\hsize]{imgs/ResultsOfSiamFC}
\caption{Examples of NIR partial face images and detection results. First row shows input images. Left image was captured with iris on the move (IOTM) system, and right image is from public iris dat... |
1,116,691,500,482 | arxiv | \section{Introduction}
The resolution limit of conventional microscopes is determined by Rayleigh's criterion \cite{Rayleigh}. In the last few decades, various techniques have been invented to circumvent Rayleigh's limit by changing the imaging conditions. Such techniques utilize nonlinear optical properties of the ob... |
1,116,691,500,483 | arxiv |
\section{Future Applications}
We have analyzed the individual components of this dataset and presented experiments with baseline results for tasks such as attribute classification, relationship classification, description generation, and question answering. There are, however, more applications and experiments for wh... |
1,116,691,500,484 | arxiv | \section{Introduction}
The aim of generative models is to produce synthetic images, which are similar to samples in a dataset. Recently, remarkable approaches have been proposed and developed in this field \cite{goodfellow2014generative, kingma2018glow, kingma2016improved, oord2016pixel}. Each of these approaches has ... |
1,116,691,500,485 | arxiv | \section{Introduction and Preliminaries}
A loop is called an Osborn loop if it obeys any of the two
identities below.
\begin{equation}\label{eq:4.1}
\textrm{OS$_3$}~:~(x\cdot yz)x=xy\cdot [(x^\lambda \cdot xz)\cdot x]
\end{equation}
\begin{equation}\label{eq:6.1}
\textrm{OS$_5$}~:~(x\cdot yz)x=xy\cdot [(x\cdot x... |
1,116,691,500,486 | arxiv | \section{Introduction}
The standard two-sided and one-sided matching problems, and the closely related school choice problem, have been widely studied from an axiomatic viewpoint. A small number of algorithms dominate the literature. For two-sided matching, the Gale-Shapley algorithm; for one-sided matching, (random) ... |
1,116,691,500,487 | arxiv | \section{Introduction} \label{sec:introduction}
In typical microfluidic applications, the Reynolds number is very small and the flow is laminar. If chaotic mixing is not induced by the device geometry via fully three-dimensional flow fields, mixing is due to molecular diffusion only, resulting in long diffusion times, ... |
1,116,691,500,488 | arxiv | \section{Introduction}\label{sec:intro}
Wireless broadband systems are witnessing rapid growth in both the number of subscribers and the traffic volume per subscriber. More smartphone users are using web-based services such as video streaming, e.g. YouTube, and social networking, e.g. Facebook. These applications re... |
1,116,691,500,489 | arxiv | \section{Introduction}
\label{sec:intro}
Machine learning with distributed databases has been a hot research area~\cite{li2014communication}.
The amount of data at each client can be large, and hence the data uploading to a central server may be constrained by energy and bandwidth limitations.
Besides, local data may c... |
1,116,691,500,490 | arxiv | \section*{SUBMITTED TO "MECHANICS OF MATERIALS" ON 4th OCTOBER 2020}
\title{Rate-dependent adhesion of viscoelastic contacts. Part \textrm{I}:
contact area and contact line velocity within model multi-asperity contacts with rubber.}
\author{G. Violano}
\affiliation{Department of Mechanics, Mathematics and Management, ... |
1,116,691,500,491 | arxiv | \section{Introduction}
Star forming dwarf galaxies constitute one of the very common type of galaxies present in the local volume and increase in number and importance with redshift. They mostly have small intrinsic size and low absolute luminosity \citep{hodge1971}. Study of nearby dwarf galaxies are vital to throw li... |
1,116,691,500,492 | arxiv | \section{Introduction}
Cosmic rays (CRs, hereafter) are high-energy particles that
generate randomly distributed, large signals on charge-coupled
devices (CCDs), which could affect the measured fluxes of
astronomical objects if not detected or removed properly.
Generally, CRs are removed by combining three or more... |
1,116,691,500,493 | arxiv | \section*{ }
By expressing the time-independent Schr\"odinger equation in one
dimension as a system of two first-order differential equations, the
transfer matrix for a rectangular potential barrier is obtained
making use of the matrix exponential. It is shown that the transfer
matrix allows one to find the bound state... |
1,116,691,500,494 | arxiv | \section{Introduction}\label{Intro}
The research and development of quantum computers are currently an important and active field of quantum information science and technology \cite{QCFeynman,QCDeutsch,QCLloyd,DiVincenzoQC,QCQINandC,QSRMP2014,SCQRPP2017,
SCQNISQ20191,SCQARCMP2020,ZhugroupSQC2020,trappedionNISQ2019... |
1,116,691,500,495 | arxiv |
\section{Introduction}
The private retrieval of information from public databases has received
significant attention already for several decades from researchers in the
computer science community (see, e.g., \cite{Chor_etal1998,
Yekhanin2010}). While this line of work, commonly known as private information
retrieval... |
1,116,691,500,496 | arxiv | \section{Introduction}
Theoretical modeling of structure formation in a $\Lambda$-CDM
cosmology cannot match observed galaxy luminosity functions locally
unless some form of heating or ``feedback'' is included in the
simulations \citep[e.g.,][]{GranatoEtal2004}. This strong theoretical
requirement coupled with (1) the... |
1,116,691,500,497 | arxiv | \section{Introduction}
\label{sec:intro}
Over the past several decades, weakly interacting massive particles (WIMPs) have been the leading class of candidates for our universe's dark matter. This paradigm has been motivated primarily by
the fact that a stable particle species with a weak-scale mass and interaction st... |
1,116,691,500,498 | arxiv | \section{Introduction}
\label{sec:intro}
The latest set of gravitational--wave (GW) observations released by the LIGO Scientific \citep{LIGOScientific:2014pky}, Virgo \citep{VIRGO:2014yos} and KAGRA \citep{Aso:2013eba} Collaboration (LVK) as part of The third Gravitational-wave Transient Catalog (GWTC-3) catalog \citep... |
1,116,691,500,499 | arxiv | \section{Introduction}
Deep neural networks have achieved significant results for a variety of real-world tasks such as image processing~\cite{He2015a,Zhu2017}, natural language processing~\cite{Devlin2018}, and game playing~\cite{Silver2017}.
Their successes depend on hard-coded prior knowledge, such as translation in... |
1,116,691,500,500 | arxiv | \section{Introduction and Summary }
A double Wick rotation on the string world-sheet was proposed in
\cite{Arutyunov:2007tc} and now it is well known that it is a very
useful tool for the study of AdS/CFT correspondence, for review see
\cite{Arutyunov:2009ga}. It is crucial that double Wick rotation has
sense in case o... |
1,116,691,500,501 | arxiv | \section{Introduction}
The aim of this letter is to provide a coherent description of the impact of scalar ($J^{PC}=0^{++}$) and tensor ($J^{PC}=2^{++}$) mesons in tau decays with three pions in the final state.
The four targets of this theoretical analysis are
\begin{itemize}
\item{\bf Chiral invariance and (p... |
1,116,691,500,502 | arxiv | \section{Introduction}
The past decade has witnessed an explosive growth of data and the needs for high-speed data processing. A large-scale data often needs to be sorted to enable higher efficiency. Sorting is a key kernel in many applications such as data mining \cite{aggarwal2015data}, robotics \cite{bayindir2016re... |
1,116,691,500,503 | arxiv | \section{Introduction}
\label{intro}
Infrared (soft and collinear) singularities appear in the calculation
of multiparton QCD matrix elements.
Although the singularities cancel in the evaluation of inclusive cross
sections, their factorization properties are at the basis
of many important tools in perturbative QCD app... |
1,116,691,500,504 | arxiv | \section{Introduction}
\label{sec:intro}
The possibility of generation of short light pulses by locking the
longitudinal modes of a laser was discussed only a few years after the
development of the laser in 1960. Mode-locking techniques can be classified
into two major classes: (i) active mode-locking, based on an ... |
1,116,691,500,505 | arxiv | \section*{Code Availability}
Our codes are available at: https://github.com/weiT1993/CutQC.
\section*{Acknowledgements}
This work is partly funded by EPiQC, an NSF Expedition in Computing, under grants CCF-1730082/1730449.
This work is partly based upon work supported by the U.S. Department of Energy, Office of Scienc... |
1,116,691,500,506 | arxiv | \section{INTRODUCTION}
Understanding the structure and kinematics
of spiral galaxies, in particular explaining their rotation curves at
large galactic radii, remains one of the pressing open questions in astrophysics.
Optical observations of galactic rotation curves find that rather than falling off as one
would expec... |
1,116,691,500,507 | arxiv | \section{Introduction}
Exclusive electroproduction of vector mesons
was suggested in \cite{knnz} as an effective tool in
search for color transparency (CT) \cite{prp}.
The key idea is based upon
absence of strict correlation between the photon's
energy and virtuality, typical for reactions of
quasielastic scatterin... |
1,116,691,500,508 | arxiv | \section{Introduction}
As locally complicated spaces naturally appear in mathematics (examples:
boundaries of groups, limits under Gromov-Hausdorff convergence)
there is an effort to extend homotopy-theoretical concepts to such spaces.
This paper is devoted to a theory of coverings by locally path-connected
spaces. Ze... |
1,116,691,500,509 | arxiv | \section{\label{introdution}Introduction}
The study of the properties of networks led to the development of many mathematical, statistical and computational tools that can be used to analyze, model, and understand how systems behave in many areas of knowledge such as physics, biology, ecology, and social sciences, to ... |
1,116,691,500,510 | arxiv | \section{Introduction}
The present paper deals with analytic properties of the
{\em partial theta function}
\begin{equation}\label{eqtheta}
\theta (q,x):=\sum _{j=0}^{\infty}q^{j(j+1)/2}x^j~.
\end{equation}
It owes its name to the resemblance between the function
$\theta (q^2,x/q)=\sum _{j=0}^{\infty}q^{j^2}x^j$... |
1,116,691,500,511 | arxiv | \section{INTRODUCTION}
With recent developments in soft robotics~\cite{c1,c2,c3}, robot arms equipped with soft grippers are able to achieve more human-like tasks such as grasping fragile objects like vegetables and fruits. Soft grippers are made of compliant materials, which have high elasticity and compliance. On th... |
1,116,691,500,512 | arxiv | \section{Introduction}
\label{sec:intro}
Widely distributed radar systems are robust and fault-tolerant systems that provide high angular resolution and permit the exploitation of spatial diversity and occlusions avoidance \cite{haimovich2007mimo}. With applications in surveillance, assisted living, and health monitor... |
1,116,691,500,513 | arxiv | \section{Introduction}
Graph analysis has been receiving more and more attention on social networks, transportation, protein forecast, etc.
However, directly publishing graph statistics may leak sensitive information about an individual~\cite{RHMS_2}.
Recently, many research works have studied the problem of publishi... |
1,116,691,500,514 | arxiv | \section{Introduction}
Recently, technological advances in the experimental control of ultracold gases \cite{ug1,ug2}, trapped ions \cite{tri}, and nitrogen-vacancy centres in diamonds \cite{nv}, allowed to probe the time evolution of isolated quantum systems. Since, in such systems, the time evolution is unitary, no i... |
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