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1,941,325,218,488 | arxiv | \section{Introduction}
A \emph{translation surface} is a pair $(X, \omega)$, where $X$ is a Riemann surface and $\omega$ is a nonzero Abelian differential on $X$. If $\omega(p) = 0$ for $p \in X$, we say that $p$ is a \emph{zero} or \emph{singularity}. The \emph{order} of $p$ is the order of $p$ viewed as a zero of ... |
1,941,325,218,489 | arxiv | \section{Introduction}
\label{secI}
The internal quark structure of the nucleon can explain the experimental results for its electromagnetic form factors.
For instance, in Ref. \cite{Nucleon,Gross08b}, we presented a successful description
of the most recent results from Jlab for
the proton elastic form factors \cite... |
1,941,325,218,490 | arxiv | \section{Introduction}
An automatic sequence can be defined intuitively as a sequence of multi-index with values in a finite set, such that for a given integer $d \geq 2$, each term of such sequence can be computed by using the base $d$ expansion of the its index. The phenomena of automates can be explained by using t... |
1,941,325,218,491 | arxiv | \section{Introduction}
Asteroids and comets are primordial bodies that formed in the earliest stage of the solar system. Their rotational states, shapes, and material reflect the collisions, disruptions, and chemical processes since then to the present. Some small solar system bodies exhibit behavior such as that shown... |
1,941,325,218,492 | arxiv | \section{Introduction}
\label{sec:intro}
The aim of statistical mechanics is extracting thermodynamic properties from microscopic Hamiltonian.
Some thermodynamic properties and macroscopic phenomena can be well described by taking the thermodynamic limit~\cite{Ruelle_text,Griffiths_review1972}.
For example, therm... |
1,941,325,218,493 | arxiv | \section{Algorithms for Computing Injective Resolutions}\label{sec:algo}
We describe two methods for constructing an injective resolution of a sheaf $F$ on a poset $\Pi$.
\subsection{Injective Resolutions via the order complex}\label{sec:algo_non-inductive}
We begin with a non-inductive construction of a (not nece... |
1,941,325,218,494 | arxiv |
\section{Background}
\label{sec:background}
\subsection{Distributed Hash Tables ?}
\textbf{Distributed key partitioning}
Explain general idea and give a few examples (Chord, Pastry) ? Also, structured vs unstructured ?
\textbf{Overlay network and routing}
Explain general idea and give a few examples (Chord, Pastry... |
1,941,325,218,495 | arxiv |
\section{Introduction}
\label{sec:introduction}
Understanding how information is stored, modified, and transmitted among the components of a complex system is fundamental to the sciences.
Application domains where this would be particularly enlightening include gene regulatory networks~\cite{gates2016control}, neura... |
1,941,325,218,496 | arxiv | \section{Introduction}
\IEEEPARstart{T}{}he data rate requirements of wireless communications
have increased rapidly with the explosive growth of mobile devices
and seamless multimedia applications. Hence, the bandwidth available
in the sub-6 \emph{Gigahertz} (GHz) and mmWave bands becomes tight,
but as a remedy, the ... |
1,941,325,218,497 | arxiv | \section{introduction}
Time reversal symmetry(TRS) is a general symmetry in various
physical systems. In quantum mechanics, it has exceptionally deep
consequences. In particular, the Kramer's degeneracy, i.e.,
double degeneracy of energy eigenvalues, for spin 1/2 particle
system with TRS is well-known since the e... |
1,941,325,218,498 | arxiv | \section{Introduction}
The time evolution of unstable states has been a perennial
research subject in various branches of theoretical physics.
The most recent problem which appears on the stage is the fate of unstable
D-branes in string theory. Since A. Sen brought up this problem \cite{sen1},
called rolling tachyon... |
1,941,325,218,499 | arxiv | \section{}
The Fermi Gamma-ray Observatory discovered about a thousand extragalactic sources emitting energy from 100 MeV to 100 GeV.
The majority of these sources belong to the class of blazars characterized by a quasi-featureless optical spectrum (BL Lac Objects).
This hampers the determination of their redshift and... |
1,941,325,218,500 | arxiv | \section{All models}
\label{appendix_all_models}
In the table below we present all models evaluated in the real world.
Their respective performance can be found in Figures \ref{fig:leaderboard_all} and \ref{fig:leaderboard_all_detailed}.
\pagebreak
\section{Offline models evaluation}
\label{appendix_offline}
On ... |
1,941,325,218,501 | arxiv | \section{Introduction}
\begin{pp}[Coarse base change for modular curves]
In the study of modular forms modulo a prime $p$, one often considers the $\mathbb{F}_p$-fiber $(X_H)_{\mathbb{F}_p}$ of the modular curve $X_H$ over $\mathbb{Z}$ for an open subgroup $H \subset \GL_2(\widehat{\mathbb{Z}})$. This $\mathbb{F}_p$-... |
1,941,325,218,502 | arxiv | \section{Introduction}
\paragraph{Description of the main result.}
This is the second part of the series, see \cite{KS-prob}, where we develop a new
type of ``quiver description'' of the categories of perverse sheaves on certain configuration
spaces. The ``quiver'' in our description is a block (direct summand) of th... |
1,941,325,218,503 | arxiv | \section{Introduction}
Let the circle act effectively on a compact symplectic manifold $(M,\omega)$ of dimension $2n$ with moment map
$\phi\colon M\to\R$. The fixed point set $M^{S^1}$, which is the same as the critical set of $\phi$,
contains at least two connected components --- the minimum and the maximum of $\ph... |
1,941,325,218,504 | arxiv | \section{#1}}
\renewcommand{\theequation}{\arabic{section}.\arabic{equation}}
\def\,\slash\!\!\!\! \cT{\,\slash\!\!\!\! \cT}
\def\slash\!\!\!\!D{\slash\!\!\!\!D}
\setlength{\topmargin}{0.0in} \setlength{\evensidemargin}{0.00in}
\setlength{\oddsidemargin}{0.0in} \setlength{\textwidth}{7.0in}
\setlength{\textheight}{8.... |
1,941,325,218,505 | arxiv | \section{Introduction}
Direct observations of sunspot numbers over 400 years, as well as proxy data for much
longer timescales \citep{beer2000}, show that both the amplitude and the duration of
the solar magnetic cycle vary from one cycle to the next. The importance of this
phenomenon lies in the contribution of varyi... |
1,941,325,218,506 | arxiv | \section*{Supplementary Material}
See the supplementary material for the memory window evolution during endurance cycling
with different amplitudes for the S1 samples with different top electrode size
and polarization-voltage characteristics for all samples.
\begin{acknowledgments}
This work was supported by the Russ... |
1,941,325,218,507 | arxiv | \section{Introduction}
\subsection{Motivation}
It is well known that convex functions defined on subdomains of
$\R^{n}$ are locally Lipschitz continuous and almost everywhere
twice differentiable. Moreover, the celebrated maximum principle due
to Aleksandrov provides a global regularity result for convex
function... |
1,941,325,218,508 | arxiv |
\section{Introduction and Definitions}
\input{Intro}
\section{Maximality}
\input{MainSection}
\bibliographystyle{spmpsci}
|
1,941,325,218,509 | arxiv | \section{Introduction}
\label{sec:introduction}
\IEEEPARstart{R}{etinal} images are widely used by ophthalmologists or automated image analyzing systems as a non-invasive way to detect and monitor various eye and body diseases~\cite{abramoff2010retinal}, such as glaucoma, diabetic retinopathy, and hypertension. Unfortu... |
1,941,325,218,510 | arxiv | \section{Introduction}
A simple random walker on a finite and connected graph starting from any vertex hits an arbitrary vertex in a finite time. This fact implies that if we consider a subset of the vertices of this graph as sinks, where the random walker is absorbed, then the survival probability of the random walk ... |
1,941,325,218,511 | arxiv | \section{Introduction}
We are interested in the amount of randomization that is needed in action selection mechanisms in order to maximize the expected value of a long term reward, depending on the uncertainty of the acting agent about the system state.
It is known that in a Markov Decision Process (MDP), the optima... |
1,941,325,218,512 | arxiv | \section{Introduction}
Several modifications of general relativity (GR) have been
considered in recent years that involve nonluminal gravitational
wave propagation. Depending on the theory, and on the choice of its
parameters, these nonluminal waves can propagate faster or slower
than light. Examples of such theories a... |
1,941,325,218,513 | arxiv | \section{INTRODUCTION}
Lane-changing models are a vital component in autonomous driving simulation tools, which are extensively used and playing an increasingly important role in behaviour studies. With the rise of autonomous driving research, the demand for establishing car behaviour model in simulators \cite{dosovits... |
1,941,325,218,514 | arxiv | \section{Introduction} \label{sec:intro}
Gravitational waves (GW) emitted by merging black holes are identified in the LIGO and Virgo data through the use of
search analysis pipelines, which use the known waveform morphology to identify weak signals in the
data \citep{O1:BBH, gw170104, GW170608, GW170814}. The obser... |
1,941,325,218,515 | arxiv |
\section{Supplementary Material}
\subsection{I. Details on the orthogonal block diagonalising states creation.}
A Young tableaux is a diagram composed of a collection of left-flushed boxes containing numbers which are strongly increasing down each column and across each row, and every consecutive row having a weakly ... |
1,941,325,218,516 | arxiv | \section{Introduction}
\noindent
Systems of coupled oscillations are largely studied on account of their wide
possibility of application in many significant branches (mechanics, medical and byological
sciences, ...).
The corresponding mathematical problem is in no way easy to handle when all the effects are overlapp... |
1,941,325,218,517 | arxiv | \section{Introduction}
A recent result of Totaro \cite{T} shows that for any prime $\ell$ the Chow group mod $\ell$ of a very general Abelian threefold is infinite, generalizing a result of Rosenschon and Srinivas in \cite{RS}. Our goal will be to prove the following analgous result, which extends work of Schoen in \ci... |
1,941,325,218,518 | arxiv | \section{Introduction}\label{s0}
In his celebrated 1988 paper \cite{Adams88}, Adams extends the Moser inequality in \cite{Mos} from the first order to the higher order gradients in the Euclidean space $\rr^{n\ge 2}$ - given the gradient $$\nabla=(\partial_{x_1},...,\partial_{x_n})$$ and the Laplacian
$$
\Delta=\su... |
1,941,325,218,519 | arxiv | \section{Introduction}
We address the task of pixel-level hand detection using first person wearable cameras. From the perspective of human activity understanding, pixel-level detection of hand and arm regions is an important sub-task for higher levels of human activity understanding using a wearable camera. The exact ... |
1,941,325,218,520 | arxiv | \section{Introduction}
Given a graph $H$, let $f(n,H)$ be the maximum number of edges not contained in any monochromatic
copy of $H$ in a 2-edge-coloring of the complete graph $K_n$, and let $ex(n,H)$ be the {\it Tur\'an number} of $H$,
i.e., the maximum number of edges in an $n$-vertex $H$-free graph.
The problem ... |
1,941,325,218,521 | arxiv | \section{Introduction}
Topological insulators (superconductors) have been attracting a lot of interest both theoretically
and experimentally.
Similar to trivial insulators, they have a band gap in the bulk.
The striking feature that distinguishes topological insulators (superconductors)
from trivial ones is that the... |
1,941,325,218,522 | arxiv | \section{Introduction} \label{intro}
Let $P$ be a poset. If it has the least element $0$, then a pseudocomplement of an element $a$ is, by definition, the greatest element $u$ disjoint with $x$, i.e., such that $0$ is the single lower bound of $u$ and $a$. If every element of $P$ has a pseudocomplement, the poset is... |
1,941,325,218,523 | arxiv | \section{Introduction}
In paper \cite{sh1} a new geometry called General Geometry is
formulated and it is shown that its the most simplest case is
geometry underlying electromagnetism. However, relation between
quantities defining geometry $F^\sigma\-_\lambda$ and the length
of a curve $A_\mu$ was assumed. Next, in pa... |
1,941,325,218,524 | arxiv | \section{Introduction}
The advent of graphene and other 2D materials has significantly increased the number of optically accessible, two-dimensional electron systems that exhibit the quantum Hall effect. \cite{Novoselov05,Zhang05,Fallahazad16,Li16} These materials can be engineered into devices with nearly atomic scal... |
1,941,325,218,525 | arxiv | \subsubsection*{\bibname}}
\begin{document}
\runningtitle{Nonstationary multi-output Gaussian processes via harmonizable spectral mixtures}
\twocolumn[
\aistatstitle{Nonstationary multi-output Gaussian processes\\ via harmonizable spectral mixtures}
\aistatsauthor{ Matías Altamirano \And Felipe Tobar}
\aistatsa... |
1,941,325,218,526 | arxiv | \section{Introduction}
In order to understand the formation, evolution, and quenching of galaxies, we must understand the gas that surrounds them: the circumgalactic medium (CGM).
This is because, first, accretion of gas from the CGM fuels star formation in star-forming galaxies. Without the additional gas supply, st... |
1,941,325,218,527 | arxiv | \section{Introduction}
\vspace{-0.2cm}
What distinguishes an extrasolar giant planet (EGP) from a brown dwarf (BD) is still a matter of debate. The current IAU definition of a planet is an object that is below the mass required for thermonuclear fusion of deuterium, which we currently believe occurs at 13 Jupiter mass... |
1,941,325,218,528 | arxiv | \section{Introduction}
It has recently become evident from high accuracy radial velocity (RV) measurements
that late-type (G and K) giant stars are RV variables
(see e.g. Hatzes \& Cochran 1993, 1994; Setiawan et al. 2003, 2004).
These variations occur on two greatly different timescales:
short term variability with p... |
1,941,325,218,529 | arxiv | \section{Introduction}
Our goal is to approximately solve an optimization problem of the form:
\begin{equation} \label{eqn:rankMin}
\min_{A : \mathrm{rank}(A) \le r} R(A) ~,
\end{equation}
where $R: \mathbb{R}^{m \times n} \to \mathbb{R}$ is a convex and smooth function. This problem arises in many machine learning ap... |
1,941,325,218,530 | arxiv | \section{Introduction}\label{sec:Introduction}
SIM will be the first instrument to use astrometry to detect and
characterize terrestrial planets. The ability to make these
detections depends on the performance of the instrument, the details
of the observing scenarios, and the analysis of the astrometric
data. This pape... |
1,941,325,218,531 | arxiv | \section{Introduction}
The nature of black hole (BH) event horizon is a focus of new frontiers of physics.
The stringy paradigm of BHs predicts a little exotic nature of
BH event horizon, which may appear as a modified boundary condition
for perturbations around a BH spacetime~\cite{Skenderis:2008qn,Almheiri:2012rt}... |
1,941,325,218,532 | arxiv | |
1,941,325,218,533 | arxiv | \section*{Abstract}\label{sec:abs}
We design dynamic routing policies for an overlay network which meet delay requirements of real-time traffic being served on top of an underlying legacy network, where the overlay nodes do not know the underlay characteristics. We pose the problem as a constrained MDP, and show that w... |
1,941,325,218,534 | arxiv | \section{INTRODUCTION \& RELATED WORK}
Lidar has been one of the most anticipated sensors in recent years. It emits light pulse with unique identity, and correlates the light bouncing off the surface with the original signal. The depth information to the object can be measured in three ways, the time of flight(ToF) mea... |
1,941,325,218,535 | arxiv | \section{Introduction}
Models with statistical interactions can be used to describe a variety of interesting systems. In particular, quasiparticles in the Fractional Quantum Hall effect, as well as other fractionalized phases of spins and bosons, have such interactions.\cite{Read1989,Kitaev2003,SenthilFisher_Z2,Stern2... |
1,941,325,218,536 | arxiv | \section{Introduction}
Single and multilayered boron nitride are $sp^2$ bonded boron and nitrogen atoms arranged in a hexagonal
honeycomb lattice arranged in ABAB stacking in multilayered and bulk materials. In spite of the fact that they are isomorphic to the multilayered graphene and graphite with similar lattice con... |
1,941,325,218,537 | arxiv | \section{Introduction}
A whole-sky map contains significant amount of foreground emission from astrophysical sources.
Hence, the ability to clean foreground contamination in CMB data is of the utmost importance for CMB observations.
In the WMAP observation, foreground were cleaned by two different methods \citep{WMAP:... |
1,941,325,218,538 | arxiv | \section*{Acknowledgements}
We are grateful to Nima Arkani-Hamed, Chris Kolda, and Hitoshi Murayama
for useful discussions. This work was
supported in part by the U.S. Department of Energy under Contract
DE-AC03-76SF00098 and in part by the National Science Foundation under
grant PHY-95-14797. C.C. is a research fello... |
1,941,325,218,539 | arxiv | \section{Introduction and model}
One interesting topic which arises in the study of biologically motivated neural systems is how dynamical processes affecting the synapses in different time scales can influence the collective behaviour of large neural assemblies. A well known example is the slow change in the synaptic ... |
1,941,325,218,540 | arxiv | \section{Introduction}
Specht modules are of fundamental importance in the study of reflection groups and their deformations.
We are particularly interested in the Iwahori--Hecke algebras of types $A$ and $B$.
In type $B$, these Hecke algebras have been studied from the point of view of their decomposition numbers~\c... |
1,941,325,218,541 | arxiv | \section{Introduction}
The minimum intensity of light for triggering visual experience has been a research topic for over a century. However, due to technological deficiencies, a reliable answer was not given until recent years. The earliest academic record investigating this question dates back to 1889 by Langley~\cit... |
1,941,325,218,542 | arxiv |
\section{Introduction}
The combined MAXIMA-1 \cite{MAXIMA1},\cite{MAXIMA2},\cite{MAXIMA3}, BOOMERANG \cite{BOOMERANG1},\cite{BOOMERANG2}
DASI \cite{DASI02} and COBE/DMR Cosmic Microwave Background (CMB)
observations \cite{COBE} imply that the Universe is flat
\cite{flat01}
and that most of the matter in
the Un... |
1,941,325,218,543 | arxiv | \section{Introduction}\label{Introduction}
In the past few years, 6d \Nequals{(2,0)} superconformal theories have been used effectively as a way to organize and understand various features of lower dimensional supersymmetric dynamics.
We might hope that similar development with 6d \Nequals{(1,0)} theories is not enti... |
1,941,325,218,544 | arxiv | \section{Introduction}
The aim of this paper is to give a new characterization of Sobolev-Slobodeckij spaces $W^{1+s,p}$ for $n/p<1+s$, where $n$ is the dimension of the domain. To achieve this we introduce a family of curvature energies inspired by the classical concept of integral Menger curvature. Their purpose is ... |
1,941,325,218,545 | arxiv | \section{Introduction}
The financial market, an ecosystem that involves over $90$ trillion\footnote{https://data.worldbank.org/indicator/CM.MKT.LCAP.CD/} market capitals globally in 2020, attracts the attention of hundreds of millions of investors to pursue desirable financial assets and achieve investment goals. Recen... |
1,941,325,218,546 | arxiv | \section{INTRODUCTION}
A geometrically thin, optically thick accretion disk is unstable to
self-induced warping when illuminated by a sufficiently strong central radiation
source (Pringle 1996; Maloney, Begelman \& Pringle 1996; see also
Petterson 1977). For a steady accretion disk, generating luminosity
with an effici... |
1,941,325,218,547 | arxiv | \section{Introduction}
Recently several string actions which
naturally describe curved space-times with singularities
have been obtained from WZWN models.
Following the coset construction \cite{witten,HH,bars},
in Ref.~\cite{ch} we analyzed a particular WZWN action
in the Poincar\'e $ISO(2,1)$ group.
\par
In a recent p... |
1,941,325,218,548 | arxiv | \section{Introduction}
Emerging highly distributed networked dynamical systems, such as critical infrastructure for power, water, and transportation, are high-dimensional and increasingly instrumented with new sensing, actuation, and communication technologies. A key problem is to design high performance control archit... |
1,941,325,218,549 | arxiv | \section{Introduction}
\label{intro}
The \emph{complexity} of a natural number $n$ is the least number of $1$'s
needed to write it using any combination of addition and multiplication, with
the order of the operations specified using parentheses grouped in any legal
nesting. For instance, $n=11$ has a complexity of ... |
1,941,325,218,550 | arxiv | \section*{\contentsname}
\@starttoc{toc}%
}
\makeatother
\begin{document}
\title[LogCFTs as limits of ordinary CFTs]{Logarithmic conformal field theories as limits of ordinary CFTs and some physical applications}
\author{John Cardy$^{1,2}$}
\address{$^1$Rudolf
Peierls Centre for Theoretical Physics, 1 Keble ... |
1,941,325,218,551 | arxiv | \section*{Introduction}
Understanding the evolution and maintenance of ecological diversity is a fundamental objective of ecological research. While the basic mechanisms of evolution have largely remained unchallenged since Darwin's foundational work, assessing the relative importance of different mechanisms known or... |
1,941,325,218,552 | arxiv | \section{Introduction}
\label{sec:introduction}
In late 90's two consecutive papers by G. Takeuti and Y. Yasumoto \cite{ty}, \cite{ty2}
were published. These papers aimed at applying Boolean valued model constructions
for bounded arithmetic and relating them to separation problems of complexity classes.
Prior to thei... |
1,941,325,218,553 | arxiv | \section{Introduction}
The recent experiments on the angular resolved
photoemission for one-dimensional (1D) correlated
electron systems\cite{ex1,ex2,ex3,ex4,ex5,ex6,ex7}
have revealed some striking properties inherent in
1D systems, such as the spin-charge separation.
In particular, the photoemission experiment... |
1,941,325,218,554 | arxiv | \section{Introduction}
Visualizing structural changes of molecules in reactions in real time has been a long-standing dream in chemical physics, physical chemistry, and biochemistry~\cite{
Zewail2014,
Miller2014}.
\hatada{In particular, seeing structural changes of photoexcited free molecules is of fundamental intere... |
1,941,325,218,555 | arxiv | \section{Introduction}
Despite decades of research, video understanding still challenges computer vision. The reasons for this are many, and include the hurdles of collecting, labeling and processing video data, which is typically much larger yet less abundant than images. Another reason is the inherent ambiguity of ac... |
1,941,325,218,556 | arxiv | \section*{}
In 1956 an article by Ernest Nagel and James R. Newman entitled ``G\"odel's proof''
was published in \emph{Scientific American,}
and in 1958 an expanded version of this article was published as a book with the same title.
This is a wonderful book, and it's still in print.
At the time of its original ... |
1,941,325,218,557 | arxiv | \section{Introduction}
Since the turn of the millennium, there has been a dramatic increase in the number and precision of new cosmological observations. Measurements of the cosmic microwave background (CMB) radiation have achieved extraordinary precision for the parameters of the standard cosmological model --- ... |
1,941,325,218,558 | arxiv | \section*{Acknowledgements}
We thank the anonymous reviewers for their valuable comments. This work is supported in part by NSF grants CRII-1755646, CRII-1755769, OAC-1835821, CNS-1813487 and CCF-1918757, a Google Faculty Research Award, and an AWS Machine Learning Research Award.
\section{Conclusion and Future... |
1,941,325,218,559 | arxiv | \section{Introduction}
Recent advances in energy harvesting devices allow wireless sensor networks to operate in a self-powered fashion for extended periods of time. However, due to size of sensors and low ambient energy sources, harvested energy from environment is low \cite{winston}. Hence, efficient utilization of ... |
1,941,325,218,560 | arxiv | \section{Introduction}
\subsection{The million- to billion-line radiative transfer challenge}
Measuring the spectra of exoplanetary atmospheres gives us a window into their thermal structure and chemical compositions \citep{brown01,burrows01,char09,sd10,madhu14,hs15}. A crucial bridge between observation and inferen... |
1,941,325,218,561 | arxiv | \section{Introduction}
\IEEEPARstart{T}{his} demo file is intended to serve as a ``starter file''
for IEEE Computer Society journal papers produced under \LaTeX\ using
IEEEtran.cls version 1.7 and later.
I wish you the best of success.
\hfill mds
\hfill January 11, 2007
\subsection{Subsection Headin... |
1,941,325,218,562 | arxiv | \section{Introduction}
Supervised learning is the most commonly applied form of machine learning. It works in two stages. During the training stage, the algorithm extracts patterns from the training dataset that contains pairs of samples and labels and converts these patterns into a mathematical representation called a... |
1,941,325,218,563 | arxiv | \chapter[X-Ray Polarimetry]{X-Ray Polarimetry}\label{ch_xraypolarimetry}
\author[P. Kaaret]{Philip Kaaret}
\address{Department of Physics and Astronomy, University of Iowa \\
Van Allen Hall, Iowa City, IA 52242, USA \\
philip-kaaret@uiowa.edu}
\begin{abstract}
We review the basic principles of X-ray polar... |
1,941,325,218,564 | arxiv | \section{Representations of Quantum Processes and Properties}
The finite time open dynamics of a quantum system is described by a quantum process (or operation) represented by a map, $\mathcal{E}: \rho \to \mathcal{E}(\rho)$. Since quantum operations take density matrices to density matrices, the map, in general, has ... |
1,941,325,218,565 | arxiv | \section*{Acknowledgements}
\noindent We express our gratitude to our colleagues in the CERN
accelerator departments for the excellent performance of the LHC. We
thank the technical and administrative staff at the LHCb
institutes.
We acknowledge support from CERN and from the national agencies:
CAPES, CNPq, FAPERJ and ... |
1,941,325,218,566 | arxiv |
\section{Introduction}
The discovery of graphene \cite{Geim2007} and more broadly of atomically thin materials has triggered a wealth of research in optoelectronics \cite{Koppens2014}, plasmonics \cite{Fei2012}, telecommunications \cite{Mueller2010}, solar energy harvesting \cite{Pospischil2014} and sensing \cite{Kim2... |
1,941,325,218,567 | arxiv | \section{Introduction}
\label{sec:intro}
\emph{Selfies} (photos of one self, typically captured with smartphone or webcams) have become very popular on social media platforms, particularly on Instagram\footnote{\url{https://www.instagram.com/}}, Snapchat\footnote{\url{https://www.snapchat.com/}} and TikTok.\footnote{\u... |
1,941,325,218,568 | arxiv | \section{Introduction}
WebAssembly\xspace is the fourth official language of the Web \cite{WebAssemblyCoreSpecification}.
The language provides low-level constructs enabling efficient execution times, much closer to native code than JavaScript.
It constitutes a fast and safe platform to execute programs in the browser ... |
1,941,325,218,569 | arxiv | \section{Introduction}
\label{sec:Introduction}
\IEEEPARstart{H}{uman} Presence-aware Systems (HPSs) are rapidly
growing as new services become available in various areas of modern
life \cite{Petrov-2019} such as assisted living, ambient intelligence,
smart spaces, home automation, human-robot collaboration, s... |
1,941,325,218,570 | arxiv | \section{Introduction}
The Lorentz and CPT symmetries, are certainly among the more important symmetries of nature (see f.e. \cite{Kostel}).
However, motivated by the fact that spontaneous breaking of Lorentz symmetry may arise in the context of string theory \cite{Kos01}, the possibility of Lorentz symmetry brea... |
1,941,325,218,571 | arxiv | \section{Introduction }
Very young, deeply embedded protostars with a stellar mass still smaller than the envelope mass are in the phase of heavy accretion, building up their final mass. The details of how these Class 0 protostars obtain their mass remain poorly understood, even though this phase is crucial for the su... |
1,941,325,218,572 | arxiv | \section{Introduction}
Let $G$ be a finite group scheme over a field $k$ of positive characteristic. There is a notion of $\pi$-cosupport~\cite{Benson/Iyengar/Krause/Pevtsova:2015a} for any $G$-module $M$, based on the notion of $\pi$-points of $G$ introduced by Friedlander and the fourth author~\cite{Friedlander/Pevt... |
1,941,325,218,573 | arxiv | \section{Introduction}
\label{sec:intro}
The {\em risk premium} or {\em market price of risk} is one of main concepts in mathematical
finance.
The risk premium is a measure of the trade-offs investors make between return and risk and is
defined by
the excess return relative to the risk-free interest rate earned from ... |
1,941,325,218,574 | arxiv | \section{Introduction}
Given two measure spaces $(X,\Sigma_{X}, \mu)$ and $(Y,\Sigma_{Y},
\nu)$ we consider a general set transformation ${\cal R}: \Sigma_{X}\rightarrow \Sigma_{Y}$.
We denote by $f_{\cal R}^*$ the rearrangement of a
$\mu-$measurable function $f$ with respect the transformation
$\cal R$ by means of... |
1,941,325,218,575 | arxiv | \subsection{Structural characterization upon heating and melting}
We first studied the evolution in structure of ZIF-4, which is composed of Zn(Im)$_4$ tetrahedra linked by Zn--N coordinative bonds (Figures~1a,b), and forms a three dimensional, crystalline network containing a maximum cavity diameter of 4.9\,{\AA} (Fi... |
1,941,325,218,576 | arxiv | \section{Introduction}
Graphene, a monolayer of carbon atoms arranged in a honeycomb lattice with $C_{3v}\otimes Z_2$ symmetry \cite{Wallace_47}, possesses an electronic spectrum that displays two non-equivalent points $K_{+},\,K_{-}$ where the conduction and valence bands touch, and in whose vicinity
the dispersion re... |
1,941,325,218,577 | arxiv | \section{Evaluation on Source Tasks}
\label{sec:eval_src_tasks}
In this section, we discuss the performance of the shared-private multi-task learning (MTL) frameworks on different combinations of QQP, SNLI and MNLI datasets as the {\em source tasks}.
We concatenate the representations generated by the shared and privat... |
1,941,325,218,578 | arxiv |
\section*{Acknowledgement}
The authors are pleased to acknowledge the support from TRIUMF to provide a stable beam during the experiment. Special thanks go to R. Henderson, R. Openshaw, G. Sheffer, and M. Goyette from the TRIUMF Detector Facility. We also thank D. Arseneau, G. Morris, B. Hitti, R. Abasalti, and D. Vya... |
1,941,325,218,579 | arxiv | \section*{Appendix}
\section*{Acknowledgments}
This work is funded by the European Research Council (ERC) through the ERC-2017-STG BigEarth Project under Grant 759764 and by the German Ministry for Education and Research as BIFOLD - Berlin Institute for the Foundations of Learning and Data (01IS18025A). The authors wo... |
1,941,325,218,580 | arxiv | \section{Introduction}
The {\it Chandra} and the {\it XMM-Newton}
satellites are currently providing a wealth of x-ray spectra on many
astronomical objects. There is a serious lack
of adequate atomic data, particularly in the K-shell energy range, needed for
the interpretation of these spectra.
Spectroscopy in the ... |
1,941,325,218,581 | arxiv | \section{Introduction}
Barnette's conjecture is a long standing unsolved problem in mathematics proposed by David W. Barnette in 1969. The conjecture states:
\begin{conjecture}\label{barcon}
Every $3$-regular, $3$-connected planar bipartite graph is Hamiltonian. We will henceforth use the term Barnette graphs to refer ... |
1,941,325,218,582 | arxiv | \section{Introduction}
Understanding the flow dynamics of atmospheres is crucial for
characterizing extrasolar planets. Dynamics strongly influence the
temperature distribution as well as the spectral behavior. An
essential tool for studying dynamics on the large-scale is a global
hydrodynamics model. Many studies h... |
1,941,325,218,583 | arxiv | \section{Introduction}
The purpose of this document is to prepare the reader for the tutorial sessions
on the forthcoming CERN Accelerator School (CAS), where basic methods for beam
optics calculations will be illustrated with the help of Octave\cite{OCTAVE},
MATLAB~\cite{MATLAB}, or Python~\cite{PYTHON}. At the scho... |
1,941,325,218,584 | arxiv | \section{Introduction}
The most important difference between mm and cm
interferometry is the effect of the troposphere at mm wavelengths.
The optical depth of the troposphere becomes significant below 1 cm,
leading to increased system temperatures due to atmospheric emission,
and increased demands on gain calibration ... |
1,941,325,218,585 | arxiv | \section{Introduction}
Active Galactic Nuclei (AGN) are sources of powerful collimated jets containing high-energy particles possibly including electrons and protons, and are believed to exist in environments typically hosting large densities of Dark Matter (DM), such as the center of massive elliptical galaxies. Ref.~... |
1,941,325,218,586 | arxiv |
\section{Introduction}
Autonomous driving has been the object of great research efforts in the last decades.
Human errors are a prominent cause of road accidents and fatalities.
Road congestion causes inefficiency in daily commutes and other aspects of road transportation.
A transportation system that is less relia... |
1,941,325,218,587 | arxiv | \section{Introduction}
Quasi-linear systems of conservation laws can be symmetrized, if they admit
an additional \emph{convex} conservation law (Godunov, 1961, Friedrichs and
Lax, 1971). The symmetric form implies hyperbolicity of governing equations.
For conservation laws with vanishing right-hand side, the hyperboli... |
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