uuid int64 541B 3,299B | dataset stringclasses 1
value | text stringlengths 1 4.29M |
|---|---|---|
1,108,101,562,415 | arxiv | \section{Introduction}
Eigenvalues of various graph-theoretical matrices often reflect structure properties of graphs
meaningfully \cite{cvetkovic1}. In fact, studying eigenvalues of graphs and, then, characterizing those graphs based on certain properties
of their eigenvalues has a long standing history, see \cite{cve... |
1,108,101,562,416 | arxiv | \section{Introduction}
Free-boundary problems are known for their high mathematical complexity, both in terms of analysis and numerical modelling. The understanding and tracking of the free-boundary adds extra difficulties to the already challenging distributed parameter systems, and demands the use of a wide range of ... |
1,108,101,562,417 | arxiv | \section{INTRODUCTION}
Physical properties of anomalous X-ray pulsars (AXPs), soft gamma repeaters (SGRs), and dim isolated neutron stars (XDINs) indicated by the observations, significantly depend on the actual torque mechanism slowing down these sources. There are two basic torque models that try to explain the evol... |
1,108,101,562,418 | arxiv | \section*{Supplementary Material}
See supplementary online material for the structural and magnetic characterization of the bi- and trilayer samples, the carrier concentration of the Ga:ZnO layer, and a more elaborate discussion of the SMR trilayer simulation.
\begin{acknowledgments}
M.S.R. and J.M. would like to than... |
1,108,101,562,419 | arxiv | \chapter{Feynman rules}\label{app:feyn_rules}
In this Appendix we present the Feynman rules involving different types of anomalous couplings generated by effective Lagrangians defined various sections of chapters~\ref{chap:neutral_currents} and~\ref{chap:CC}.
\section{Neutral currents}\label{app:feyn_neutral}
In Tab.~\... |
1,108,101,562,420 | arxiv | \section{Introduction}
1E\,1048.1$-$5937{},
one of the original ``anomalous X-ray pulsars'' \citep[AXPs;][]{1995ApJ...442L..17M},
is now classified as part of a small class of pulsars known as magnetars -- neutron stars which display behavior thought to be powered by their immense magnetic fields.
For a recent revie... |
1,108,101,562,421 | arxiv | \section{Introduction}
In time-frequency analysis, one studies a signal $\psi \in L^2(\mathbb{R}^d)$ by considering various time-frequency representations of $\psi$. An important class of time-frequency representations is obtained by fixing $\varphi\in L^2(\mathbb{R}^d)$ and considering the \textit{short-time Fourier t... |
1,108,101,562,422 | arxiv | \section{Introduction \label{In}}
Within the standard model the calculation of the $K\rightarrow \pi\pi$
decay amplitudes is based on the effective low-energy hamiltonian for
$\Delta S=\nolinebreak 1$ transitions \cite{delS},
\begin{equation}
{\cal H}_{ef\hspace{-0.5mm}f}^{\scriptscriptstyle \Delta S=1}=\frac{G_F}{\sqr... |
1,108,101,562,423 | arxiv | \section{Introduction}
Models of dynamical electroweak symmetry breaking (DEWSB) like
Technicolor are possible extensions of the Standard Model, and many
proposals have been put forward for a strongly--interacting sector
beyond the Standard Model since the original proposals in
Refs.~\cite{Weinberg:1979bn,Susskind:1978... |
1,108,101,562,424 | arxiv | \section{Introduction}
Gamma-ray bursts (GRBs) are the most luminous explosive events in
the Universe. It is well known that the observed gamma-ray emission
are produced by relativistic outflows. The fireball of a GRB is required to have a
relativistic speed toward the earth in order to avoid the
``compactness p... |
1,108,101,562,425 | arxiv | \section{Introduction}
The geometry of a static and stationary spherically symmetric
wormhole consists of a two-mouthed tunnel (referred as a tube,
throat, or handle in the literature). This tube like structure is a
multiply connected spacetime which can join two asymptotically flat
regions of the same spacetime or ... |
1,108,101,562,426 | arxiv | \section{Introduction}
\par Modern statistical applications often encounter situations where it is critical to account for inherent heterogeneity and substructures in data \cite{luo2010, verbeke1996, Dietterich2000, Bouwmeester2013}. Under the presence of heterogeneity in the distribution of covariates, it is natural ... |
1,108,101,562,427 | arxiv | \section{Introduction}
The recent experimental data from Double Chooz [1], Daya Bay [2], RENO [3], T2K [4] and MINOS [5] collaborations, indicate not only a nonzero reactor angle ($\theta_{13}$) but also with its magnitude of the order of Cabibbo angle ($\theta_{c}$). Tri-Bimaximal (TBM) mixing [6] and Bimaximal (BM) m... |
1,108,101,562,428 | arxiv | \section{Introduction}
\input{intro.tex}
\label{intro}
\section{Problem Formulation and Theory}
\input{theory.tex}
\label{theory}
\section{Results and Discussion}
\input{results.tex}
\label{results}
\section{Summary}
\input{summary.tex}
\label{summary}
\begin{acknowledgments}
This work was sponsored by NSF grant CBET-0... |
1,108,101,562,429 | arxiv | \section{Introduction}
Ultracold atoms trapped in optical lattices are ideally suited for investigations of
the phase structure and phase transitions of strongly interacting quantum many-body systems.
A recently highlighted example is the superfluid to Mott insulator transition studied in Ref.~\cite{Greiner2002} u... |
1,108,101,562,430 | arxiv | \section{Introduction}
\label{sec-introduction}
The present world craves for optimization with respect to every possible aspects of the nature and its happenings due to the rapid depletion of easy energy sources and profit maximization. Hence a lot of focus has been made on optimization of different fields of engineeri... |
1,108,101,562,431 | arxiv | \section{Introduction}
The perovskite ($AB$O$_3$) family of materials has been paid considerable attention both in experimental and
theoretical studies due to their flexible and coupled compositional, structural, electrical and magnetic properties
~\cite{Bellaiche00p5427, Saito04p84, Bilc06p147602}.
Such flexibility... |
1,108,101,562,432 | arxiv | \section{Introduction}
\label{sec:intro}
\noindent
The processes that cause star formation activity in galaxies to diminish or ``quench'' are of great interest in understanding galaxy evolution. A number of observational and (semi-)numerical studies \citep{vdb+08,rb09,ww10,vdw+10,hopkins+10,more+11,prescott+11,wtc12,wt... |
1,108,101,562,433 | arxiv | \section{Introduction}
In a joint paper with Albert Schwarz \cite{ps2}, we gave definitions
of Hochschild cohomology and cyclic cohomology
of an \hbox{$A_\infty$}\ algebra, and showed that
these cohomology
theories classified the infinitesimal deformations of the
\hbox{$A_\infty$}\ structure and those deformations pres... |
1,108,101,562,434 | arxiv |
\section{Angular-averaged $A_{\rm PV}$}
\label{sec:angaver}
The parity-violating asymmetry $A_{\rm PV}$ is a function of the transferred
momentum $q$, or equivalently four momentum $Q$. These are functions
of the incoming electron beam energy $E_\mathrm{el}$ and the
scattering angle $\theta$. To be precise, one shoul... |
1,108,101,562,435 | arxiv | \section{Introduction}
The cuprate YBa$_{\text{2}}$Cu$_{\text{3}}$O$_{\text{7}-\delta}$ (YBCO) is one of the most prominent representatives of oxides exhibiting High-Temperature Superconductivity (HTS).\cite{PhysRevLett.58.908,1347-4065-26-4A-L314,bednorz}
The structure of YBCO is characterized by two different latti... |
1,108,101,562,436 | arxiv | \section{Introduction}\label{sec:intro}
The shape of the stellar body of a galaxy reflects its formation
process. Reconstructing the intrinsic, three-dimensional shapes of
spiral galaxies from their shapes projected on the sky has a long
tradition, and proved to be an exquisitely accurate and precise
approach, especia... |
1,108,101,562,437 | arxiv | \section{Introduction}
In \cite{Incurvati2016}, Luca Incurvati defines the scheme $\textsf{RP}_{m,n}$ as follows, for all integers $m, n$ such that $0<m\leq n$. The schema $\textsf{RP}_{m,n}$ is defined to be a schema of sentences in the $n$th-order language of set theory, where for each well-formed formula $\phi$ i... |
1,108,101,562,438 | arxiv | \section{Introduction}
\label{sect:intro}
The ability to fabricate ultra-clean graphene sheets by encapsulation in hexagonal boron nitride crystals~\cite{mayorov_nanolett_2011,wang_science_2013,taychatanapat_naturephys_2013,bandurin_science_2016} allows the investigation of ballistic transport in a large range of tem... |
1,108,101,562,439 | arxiv | \section*{Acknowledgments}
The authors acknowledge the support of \textit{Agence Nationale de la Recherche} through the \textit{Ethna}, \textit{ThermaEscape} and \textit{Monaco} projects. P.O.C. thanks B. Palpant for discussions.
{
\small
\linespread{1}
|
1,108,101,562,440 | arxiv |
\section{About this document}
\section{Executive Summary}
\subsection{Findings}
\begin{enumerate}
\item NASA, NSF, ESA, and CERN fund data archive centers dedicated to preserving and sharing data beyond the lifetime of individual projects. DOE does not have an equivalent data archive center for its Cosmic ... |
1,108,101,562,441 | arxiv | \section{Information Theory \& Emergence}
\subsubsection*{A Note on Notation}
The information theoretic formalisms around emergence unfortunately require notation to represent a number of overlapping, and potentially confusing, concepts. In general, one-dimensional random variables will be represented with italiciz... |
1,108,101,562,442 | arxiv | \section{Introduction}
The aim of this work is computing periods of words in the approximate pattern matching model (see e.g.\ \cite{Jewels,DBLP:books/cu/Gusfield1997}).
This task can be stated as the \emph{approximate period recovery (APR) problem} that was defined by Amir et al.~\cite{DBLP:journals/talg/AmirELPS12}.
... |
1,108,101,562,443 | arxiv | \section*{Introduction} \label{sec:intro}
In the normal heart, each heartbeat is associated with an action potential (AP).
The cardiac AP consists of a depolarized phase in which the voltage is elevated; this is associated with transient increased permeability of the cell membrane to Na$^+$ and Ca$^{2+}$.
The depolar... |
1,108,101,562,444 | arxiv | \section{Introduction}
Symmetries comprise the most fundamental laws of nature, allowing to
f\/ind conserved quantities and exact solutions of the equations of
motion. The existence of a suf\/f\/icient number of conserved quantities
facilitates the investigation of a given dynamical system. Complete
integrability of t... |
1,108,101,562,445 | arxiv | \section{Introduction}
Neural networks provide state-of-the-art results in a variety of machine learning tasks, however, several neural network's aspects complicate their usage in practice, including overconfidence~\cite{deepens}, vulnerability to adversarial attacks~\cite{adv_attacks}, and overfitting~\cite{overfittin... |
1,108,101,562,446 | arxiv | \section{Introduction}
Motivated by high accuracy at reduced computational cost with respect to uniform grid methods,
numerous adaptive discretization schemes of evolutionary partial differential equations (PDEs) have been developed since decades, see, e.g., \cite{Brandt77}.
Real world problems, for instance, fluid and... |
1,108,101,562,447 | arxiv | \section{Introduction}
Dark energy is a fundamental component of the nowadays standard
cosmological model.
It would be very difficult to explain the set of present days
cosmological observations without it.
Specifically, we refer to the luminosity-redshift
relationship from observations of supernovae of type Ia (... |
1,108,101,562,448 | arxiv | \section{%
\@startsection
{section}%
{1}%
{\z@}%
{0.8cm \@plus1ex \@minus .2ex}%
{0.5cm}%
{%
\normalfont\small\bfseries
\centering
}%
}%
\def\@hangfrom@section#1#2#3{\@hangfrom{#1#2}\MakeTextUppercase{#3}}%
\def\subsection{%
\@startsection
{subsection}%
{2}%
{\z@}... |
1,108,101,562,449 | arxiv | \section{Introduction}\label{sec:introduction}
Type Ic supernovae (SNe~Ic) are classified from their optical spectra as having no hydrogen or helium present \citep[for a review of supernova classification, see][]{F97}. They constitute $\sim 10$\% of the total number of SNe in the local universe \citep{Li:2011cl}. SNe~... |
1,108,101,562,450 | arxiv | \section{Introduction and Main Goal}
In \cite{Ram}, the authors give five continued fractions for certain
${\mathbb Z}$-linear combinations of zeta values, only obtained and checked numerically,
as well as other linear combinations involving powers of $\pi$, Catalan's
constant, etc... The purpose of the present paper ... |
1,108,101,562,451 | arxiv | \section*{Acknowledgments}
I am grateful to Antonio Pich for the illuminating discussion during this work and many important suggestions on the manuscript. Many thanks to Anjan S. Joshipura, Namit Mahajan, Saurabh D. Rindani and Utpal Sarkar for valuable and critical feedback on this work. I thank to Mehran Zahiri ... |
1,108,101,562,452 | arxiv | \section{Introduction}
During disruptions on the largest operating tokamak, JET, the current profile, $K\equiv\mu_0j_{||}/B$, flattens on a time scale $\lesssim 1$~ms, which is orders of magnitude shorter than the time scale for resistive diffusion. The evidence \cite{Wesson:1990,de Vries:2016} for the flattening is... |
1,108,101,562,453 | arxiv | \section{Introduction}
{\bf Introduction.} The Born-Oppenheimer (BO) problem \cite{bo} is
concerned with the analysis of Schr\"odinger type operators where
the small electron to nucleon mass ratio, plays the role of the
semiclassical parameter.
\cite{aventini-seiler,berry,lh,mead,mead2,mead_truhlar,jackiw,wilczek}.
Th... |
1,108,101,562,454 | arxiv | \section{Introduction}
\label{sec:Introduction}
Advances in the field of low-temperature scanning tunneling microscopy (STM) have enabled the detection and manipulation of the spin of individual magnetic atoms and molecules\cite{Stipe1998}.
With current STM techniques magnetic atoms can be arranged into artificial ass... |
1,108,101,562,455 | arxiv | \section{INTRODUCTION}
Dubins path planning problem is widely used for path planning and trajectory planning for unmanned aerial vehicles with finite yaw rate. For the vehicles with finite yaw rate, it is natural to use Dubins paths to generate flyable trajectories that satisfy the curvature constraints. Given an initi... |
1,108,101,562,456 | arxiv | \section{Introduction}
\label{intro}
Age- and cause-specific under-five mortality (ACSU5M) rates are a critical indicator of the health and well-being of children worldwide. Therefore, understanding patterns and trends in ACSU5M is crucial for informing and evaluating age and disease-targeted interventions and policie... |
1,108,101,562,457 | arxiv | \section{Introduction}
\label{Intro}
The ($K^-$,~$\pi^-$) reaction has been an essential tool for studying spectroscopy
in hypernuclear physics and strange particle physics \cite{Bruckner76,Bruckner78,Chrien79}.
This reaction has played an important role in understanding hypernuclear structures
related to the... |
1,108,101,562,458 | arxiv | \section{Continuum limit}
\label{app:cont_model}
The magnetic Hamiltonian $H_{\rm ph}$ for the photonic lattice is quadratic in the field operators and can be written in a diagonal form as
\begin{equation}
H_{\rm ph}= \sum_\lambda \omega_\lambda \Psi_\lambda^\dag \Psi_\lambda, \qquad {\rm where}\qquad [\Psi_\lambda,\Ps... |
1,108,101,562,459 | arxiv | \section{Introduction}
The smoothed boundary method \cite{Bueno-Orovio:2006a,Bueno-Orovio:2006b,Bueno-Orovio:2006c} and other similar approaches \cite{Gal:2006,Wu:2007,Gal:2008} have recently been demonstrated as powerful tools for solving various partial differential equations with boundary conditions imposed within ... |
1,108,101,562,460 | arxiv | \section{Introduction}
\label{Sec:Introduction}
Cool subdwarfs are the oldest members of the low-mass stellar population, with spectral types of K and M, masses between $\sim$0.6 and $\sim$0.08 M$_\sun$, and surface effective temperatures between ~4000 and ~2300 K \citep{kal09}. First coined by \citet{kui39}, subdwar... |
1,108,101,562,461 | arxiv | \section{Introduction}
The effect of electric fields on the behavior of dielectric block copolymer
melts in bulk and in thin films has found increasing interest in recent
years \cite{wirtz-ma92}-\cite{matsen06} (and references therein) due to the
possibility to create uniform alignment in macroscopic microphase separa... |
1,108,101,562,462 | arxiv | \section{Introduction}
Within the field of spintronics,\cite{book_awschalom_2002,zutic_2004,awschalom_2007} semiconductor devices with spin-orbit coupling have attracted great attention over the past years because they offer a setting where electronic spin polarizations can be generated and manipulated in the absenc... |
1,108,101,562,463 | arxiv | \section{Introduction}
The study of the size and shape of the density distributions of
protons and neutrons in nuclei is a classic, yet always contemporary
area of nuclear physics. The proton densities of a host of nuclei are
known quite well from the accurate nuclear charge densities measured
in experiments involvin... |
1,108,101,562,464 | arxiv | \section{Introduction}
One of the main challenges in molecular and systems biology is to infer mechanistic details of the processes that underlie available experimental data. A common strategy consists in applying controlled perturbations to the system of interest, and compare model predictions with gathered quantitati... |
1,108,101,562,465 | arxiv | \section*{INTRODUCTION}
The tumor suppressor p53 plays a central role in cellular responses to various stresses, such as oxidative stress, hypoxia, telomere erosion and DNA damage \cite{Levine2009,Junttila2009}. As a powerful transcription factor, p53 primarily functions by inducing the transcription of many different... |
1,108,101,562,466 | arxiv | \section{Introduction}
Higher-order topological superconductors (HOTSC) are novel forms of gapped quantum matter that host gappable surfaces but gapless corners or hinges in-between\cite{benalcazar2017quantized,schindler2018higher}. Since their initial discovery, HOTSC and their descendants have been discussed extensiv... |
1,108,101,562,467 | arxiv | \section{Conclusion}
\label{conclusion}
This paper presented an open-source labeled dataset and a benchmark for object detection for \gls{ssl}. The proposed dataset guarantees variety with images extracted from different sources under distinct lighting conditions and camera configurations. The labeled objects are Robo... |
1,108,101,562,468 | arxiv | \section{Introduction}
Data augmentation techniques are used to enhance models' performance by adding additional variations to the training data. These techniques are widely applied to improve automatic speech recognition (ASR) performance \cite{ko15_interspeech,kim17_interspeech,Hannun2014DeepSS,nguyen2020improving}. ... |
1,108,101,562,469 | arxiv | \section{Introduction}
On September 26, 2022, NASA's Double Asteroid Redirection Test (DART) mission will kinetically deflect Dimorphos, the smaller component of the binary asteroid 65803 Didymos, as a planetary defense demonstration test \citep{Rivkin2021}. Prior to the impact, DART will deploy the Light Italian CubeS... |
1,108,101,562,470 | arxiv | \section{Introduction}
\label{sec:intro}
The automated audio captioning task is a combination of audio and natural language processing to create meaningful natural language sentences \cite{DBLP:journals/corr/DrossosAV17}. The purpose of audio captioning is different than the previous audio processing tasks such as... |
1,108,101,562,471 | arxiv | \section{Introduction
In typical modern machine learning tasks, we often encounter large scale optimization problems, which require huge computational time to solve. Hence, saving computational time of optimization processes is practically quite important and is main interest in the optimization community. \par
To tac... |
1,108,101,562,472 | arxiv | \section{Optical and mechanical design}
\label{sec:appA}
The optomechanical crystal (OMC) studied in this work is numerically optimized for both optomechanical coupling and optical/acoustic quality factor, via finite-element method (FEM) simulation in COMSOL Multiphysics~\cite{COMSOL}, according to the procedure outli... |
1,108,101,562,473 | arxiv | \section{Introduction}
Particle-in-Cell (PIC) codes are among the most popular tools for the kinetic simulation of plasmas~\cite{birdsall}.
They consist in following the continuous trajectories of charged particles moving through a spatial domain under the action of external and self-induced electromagnetic (EM) field... |
1,108,101,562,474 | arxiv | \section{Introduction}
\label{intro}
There are many different types of bound-state problem that arise in atomic and
molecular physics. These range from the electronic structure problem, involving
antisymmetrised many-particle wavefunctions and Cou\-lomb interaction
potentials, to low-amplitude molecular vibrational pr... |
1,108,101,562,475 | arxiv | \section{Introduction}
In this note we investigate Adrian Raftery's
{\em mixture transition distribution model} (MTD)
from the perspective of algebraic statistics \cite{LAS, ascb}.
The MTD model, which was first proposed in \cite{Raf},
has a wide range of applications in engineering and the sciences \cite{RT}.
The art... |
1,108,101,562,476 | arxiv | \section{Introduction}
Despite more than fifty years since the seminal work of Anderson \cite{Ander58}, the localization of single particle wavefunctions in disordered quantum systems continues to attract a significant interest \cite{abr2010}. Exactly solvable models naturally have played a crucial role in the unders... |
1,108,101,562,477 | arxiv | \section{Introduction}
\label{sec_intro}
The aim of this work is to explore connections between the concepts given in the
title:
\begin{enum}
\item \emph{Noise-induced phase slips} are occasional losses of synchrony of
two coupled phase oscillators, due to stochastic perturbations~\cite{PRK}. The
problem of finding t... |
1,108,101,562,478 | arxiv | \section{Introduction}
Maritime history is the study of human activity at sea. It covers a broad thematic element of history, focusing on understanding humankind's various relationships to the oceans, seas, and major waterways of the globe \cite{hattendorf2012maritime}.
A large area of research in this field requires ... |
1,108,101,562,479 | arxiv |
\section{Introduction}
Coalgebra \cite{jacobs,r:universal-coalgebra} is a general framework in which several types of transition systems can be studied (deterministic and non-deterministic automata, weighted automata, transition systems with non deterministic and probabilistic branching, etc.). One of the strong poin... |
1,108,101,562,480 | arxiv | \section*{}
We have created an experimental procedure for determining the temperature coefficient of resistivity, $\alpha_R$, for introductory physics laboratories. As in the procedure from Henry [1], this method examines the relationship between temperature and resistivity to establish $\alpha_R$ within 10\% of the ac... |
1,108,101,562,481 | arxiv | \section{Introduction}
To process autonomous tasks, some blockchains execute digital programs called \emph{smart contracts} that become immutable once deployed \citep{zheng2020overview}.
Smart contracts are autonomous programs that can (1) customize contracting rules and functions between contractors and (2) facili... |
1,108,101,562,482 | arxiv | \section{Introduction: A Motivating Question}
Let ${\mathcal X}=\{x_1,x_2,...,x_n\}$ be a fixed set of real
numbers, and let $X_1,X_2,...,X_n$ be the successive values of a sample of size
$n$ that is drawn sequentially without replacement from the set $\mathcal X$.
We are concerned here with a systematic process... |
1,108,101,562,483 | arxiv | \section{Introduction}
Dispersal of infectious pathogens such as viruses through airborne sputum droplets can lead to the rapid transmission of diseases in the general population posing a great risk to public health. There are several minor and major infectious diseases that are transmitted through virus-carrying sput... |
1,108,101,562,484 | arxiv | \section{#1}%
\let\@seccntformat\@oldform%
}
\makeatother
\newtheorem{theorem}{Theorem}
\newtheorem{corollary}[theorem]{Corollary}
\newtheorem{definition}[theorem]{Definition}
\newtheorem{remark}[theorem]{Remark}
\newtheorem{lemma}[theorem]{Lemma}
\newtheorem{proposition}[theorem]{Proposition}
\tit... |
1,108,101,562,485 | arxiv | \section{0pt}{4pt plus 2pt minus 2pt}{4pt plus 2pt minus 2pt}
\def\BibTeX{{\rm B\kern-.05em{\sc i\kern-.025em b}\kern-.08em
T\kern-.1667em\lower.7ex\hbox{E}\kern-.125emX}}
\begin{document}
\input{writeup_10.tex}
\bibliographystyle{IEEEtran}
\section{Introduction}
For self-navigation, the most fundamental comput... |
1,108,101,562,486 | arxiv | \section{Introduction}
The goal of this paper is to present an alternative but equivalent approach to the classical construction of L-functions for automorphic representations of $\GL(1)$. Philosophically, we are trying to answer the question ``where does an L-function live?'' in the simplest case, Tate's classical co... |
1,108,101,562,487 | arxiv | \section{Introduction}
This package provides an essential feature to \LaTeX~that has been missing for too long. It adds a coffee stain to your documents. A lot of time can be saved by printing stains directly on the page rather than adding it manually. You can choose from four different stain types:
\begin{enumerate}
... |
1,108,101,562,488 | arxiv | \section{Introduction}
With many important applications in aerial or underwater missions, systems are underactuated either by design---in order to reduce actuator weight, expenses or energy consumption---or as a result of technical failures. In both cases, it is important to develop control policies that can exploit th... |
1,108,101,562,489 | arxiv | \section{Introduction}
\label{sec: introduction}
One of the most distinctive features of
quantum phases of matter is that they
are not completely
characterized by their pattern of symmetry breaking
(order parameters of some kind),
which is in a sharp contrast to classical statistical systems.
Instead, quantum ground s... |
1,108,101,562,490 | arxiv |
\section{Concluding Remarks}
\label{sec-discussion}
We analyze the impact of GDPR on storage systems. We find that
achieving strict compliance efficiently is hard; a naive attempt at
strict compliance results in significant slowdown. We modify
Redis to be GDPR-compliant and measure the performance overhead of
each mo... |
1,108,101,562,491 | arxiv | \section{Introduction}
Turbulent transport governs the spreading of contaminants in the
environment, mixing of chemical constituents in combustion engines or
in stellar interiors, accretion in proto-stellar molecular clouds,
acceleration of cosmic rays, and escape of hot particles from fusion
machines. Because of i... |
1,108,101,562,492 | arxiv | \section{Introduction}
Auto2, introduced by the author in \cite{auto2}, is a proof automation
tool for the proof assistant Isabelle. It is designed to be a
powerful, extensible prover that can consistently solve ``routine''
tasks encountered during a proof, thereby enabling a style of
formalization using succinct proo... |
1,108,101,562,493 | arxiv | \section{Introduction}
Learning to learn is essential in human intelligence but is still a wide area of research in machine learning.
\textit{Meta-learning} has emerged as a popular approach to enable models to perform well on new tasks using limited data.
It involves first a \textit{meta-training} process, when the mo... |
1,108,101,562,494 | arxiv | \section{Introduction}
When cosmic rays collide with nuclei in the air in Earth's atmosphere, hadrons are produced in inelastic collisions. These hadrons interact, lose energy, and finally decay, leading to a cascade of particles in the atmosphere that will finally hit the ground. Semileptonic decays of hadrons in the... |
1,108,101,562,495 | arxiv | \section{Introduction}
Let $A\in\mathbb{C}^{m\times n}$ be a matrix with singular value decomposition given by
$$A=U\Sigma V^*=\left[
\begin{array}{cc}
U_{k} & U_{m-k} \\
\end{array}
\right]\left[
\begin{array}{cc}
... |
1,108,101,562,496 | arxiv | \section{Introduction}
For a Banach space $X$, the continuous pairing between $X^*$, the topological dual of $X$, and $X$ is denoted by $\langle , \rangle$. A map $A : X \rightarrow X^{\ast}$ is called
$(S)_+$ if for every sequence $(u_n) \subset X$, $u_n \rightharpoonup u$, the
inequality
\begin{equation}
\limsup_{n... |
1,108,101,562,497 | arxiv | \section{The problem}
Consider a `triangle' of squares in a grid whose sides are $n$ squares long, as illustrated by the diagram in Figure \ref{7.fig}, for which $n=7$.
\begin{figure}
\caption{A triangle of size 7}
\label{7.fig}
\begin{equation*}
\setlength{\unitlength}{.5mm}
\begin{picture}(100,90)
\put(10,10)... |
1,108,101,562,498 | arxiv | \section{Introduction}
Dimensional regularization (DR) \cite{tHooft:1972tcz} is a widely used regularization scheme to regularize divergences in the loop Feynman integrals, where the spacetime dimension is continued to non-integer $d=4-2\epsilon$ dimensions. In general $d$ spacetime dimensions, there exists a special c... |
1,108,101,562,499 | arxiv | \section{Introduction}
The close proximity of the Magellanic Clouds offers an important opportunity to
study in detail the dynamics and composition of these galaxies. One of the
important issues that affects our interpretation of the observable parameters is
the three-dimensional structure of the Clouds. The Large Mag... |
1,108,101,562,500 | arxiv | \section{Introduction}
In recent 25 years, considerable progress has been made in loop quantum gravity (LQG)\cite{Ro04,Th07,As04,Ma07}, which is a non-perturbative and background independent quantization of general relativity. A particular feature of LQG is to to inherit the core concept of general relativity that... |
1,108,101,562,501 | arxiv |
\section{Introduction}\label{sec:Introduction}
Given a set $P$ of $n$ points, and a set \set{B} of $m$ boxes (i.e. axis-aligned closed hyper-rectangles) in $d$-dimensional space, the \textsc{Box Cover} problem consists in finding a set $\mathcal{C \subseteq B}$ of minimum size such that \set{C} covers $P$.
A... |
1,108,101,562,502 | arxiv | \section{Introduction}
The study of tangent bundles and their relationship to the base manifold often
rely on the Sasaki metric. However, we may gain valuable mathematical
and physical insights by choosing a more general metric. For mechanical systems,
tangent bundles arise naturally where the manifold is the configur... |
1,108,101,562,503 | arxiv | \section{Introduction}
In the present paper we consider overdetermined problems for the fractional Laplacian in unbounded exterior sets or bounded annular sets.
Different cases will be taken into account,
but the results obtained will lead in any case to
the classification of the solution and of
the domain, that wil... |
1,108,101,562,504 | arxiv | \section{Introduction\label{sec:intro}}
The presence and nature of dust in the universe can be explored by observing both the thermal radiation it emits, and its influence on stellar photons, which it absorbs and scatters to produce extinction.
Both of these methods sample different dust populations, with emission bein... |
1,108,101,562,505 | arxiv | \section{Introduction}
\label{sec:intro}
Optical interference coatings with as low as possible optical and mechanical losses are in demand for high-precision optical measurement applications such as atomic clocks and interferometric gravitational-wave detectors~\cite{Harry:2011book}.
In gravitational-wave observatorie... |
1,108,101,562,506 | arxiv | \section{Introduction}
Let $ K$ be a convex body in $ \mathbb{R}^n $ with $ C^2 $ boundary $ \partial K$ and everywhere positive Gaussian curvature $\kappa$. First, in \cite{gruber1993asymptotic} it was shown that
\begin{align*}
&\lim_{N\to\infty}\frac{\min\{\text{vol}_n\left(P \setminus K\right)\;|\textrm{$ K \subse... |
1,108,101,562,507 | arxiv |
\section*{\Large\centering Supplementary Material: \\Occupancy Planes for Single-view RGB-D Human Reconstruction}\vspace{0.2cm}
\input{./supp/tex/intro}
\input{./supp/tex/implementation}
\input{./supp/tex/quantitative}
\input{./supp/tex/qualitative}
\end{document}
\section{More Qualitative Results}\label{s... |
1,108,101,562,508 | arxiv |
\section{Conclusion}
Several basic but important concepts relevant to QIP are illustrated by experiments on a liquid-state ensemble NMR quantum information processor. While pure quantum mechanical states are not achievable here, the creation and application of pseudo-pure states is demonstrated. Tests of spinor beha... |
1,108,101,562,509 | arxiv | \section*{Abstract: } Let $X$ be a smooth projective toric surface,
and ${\mathbb H}^d(X)$ the Hilbert scheme parametrising the length $d$
zero-dimensional
subschemes of $X$. We compute the rational Chow ring $A^*({\mathbb H}^d(X))_{\mathbb Q}$. More
precisely, if $T\subset X$ is the two-dimensional torus contained... |
1,108,101,562,510 | arxiv |
\section{Background}
\label{sec::background}
\subsection{Reinforcement Learning}
We consider the standard RL setup where an agent interacts with an environment $\mathcal{E}$ over a number of discrete timesteps, where the interaction is modeled as a Markov Decision Process (MDP). At each timestep \(t\), the agent... |
1,108,101,562,511 | arxiv | \section{Introduction}
According to Einstein \cite{Einstein1917}, all interactions of light with matter are coherent in media large and homogeneous enough that statistical thermodynamics and Huygens construction are valid.
Most spectroscopists have long ignored Einstein's work. Thus they despised Townes' ideas before m... |
1,108,101,562,512 | arxiv | \section{Introduction}
Bound states of heavy quarks, in particular the charmonium state $J/\psi$ and its
excitations as well as the heavier bottomonium states, are sensitive probes for
deconfining features of the quark-gluon plasma (QGP) \cite{matsui}. Different
excitations of these states are expected to dissolve at ... |
1,108,101,562,513 | arxiv | \section{Introduction} \label{sec:intro}
The Standard Model with minimal
Higgs content is not expected to be the ultimate
theoretical structure responsible for electroweak symmetry breaking
\cite{hhg,habertasi}.
If the Standard Model is embedded in a more fundamental structure
characterized by a much larger energy sc... |
1,108,101,562,514 | arxiv | \section*{INTRODUCTION}
The adsorption of electronegative atoms on metal surfaces is of
paramount importance in surface science as well as
electrochemistry.\cite{Magnussen_CR102,Tripkovic_FD140,Andryushechkin_SSR73,Zhu_JESC163}
As an electronegative atom approaches a metal surface, charge is
transferred and it becomes... |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.