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\section{Introduction}
Supersymmetric lattice models have been studied starting from the $\mathcal{N}=1$ supersymmetry in the tricritical Ising model \cite{FriadenQiuShenker, KastorMartinecShenker, Qiu} and the fully frustrated XY-model \cite{Foda}. In the introduction of \cite{SaleurWarner} the interested reader can ... | {'timestamp': '2016-02-16T02:08:47', 'yymm': '1510', 'arxiv_id': '1510.02520', 'language': 'en', 'url': 'https://arxiv.org/abs/1510.02520'} |
\section{Introduction}
In Part I, \cite{part1} we derived a quantum generalization of classical transition-state theory (TST), which corresponds to the $t \to 0_+$\ limit of a new form of quantum flux-side time-correlation function. This function uses a ring-polymer \cite{chandler} dividing surface, which is invarian... | {'timestamp': '2013-09-05T02:08:37', 'yymm': '1307', 'arxiv_id': '1307.3020', 'language': 'en', 'url': 'https://arxiv.org/abs/1307.3020'} |
\section{Asymptotic expansions}
\label{summary1x}
We have seen in Section~\ref{apriori_subsection} that existence of a smooth completion at null infinity requires $g_{AB}=\mathcal{O}(r^2)$ with $(\det \ol g_{AB})_{-4} > 0$, and thus $\varphi=\mathcal{O}(r)$ with $ \varphi_{-1}> 0$.
But then
\begin{equation*}
\frac... | {'timestamp': '2014-09-24T02:13:17', 'yymm': '1403', 'arxiv_id': '1403.3558', 'language': 'en', 'url': 'https://arxiv.org/abs/1403.3558'} |
\section{Introduction} \label{section:Introduction}
Hubel and Wiesel \cite{Hube59a} discovered that certain visual cells in cats' striate cortex have a directional preference.
It has turned out that there exists an intriguing and extremely precise spatial and directional organization into so-called cortical hypercolu... | {'timestamp': '2016-03-02T02:14:52', 'yymm': '1403', 'arxiv_id': '1403.3320', 'language': 'en', 'url': 'https://arxiv.org/abs/1403.3320'} |
\section{Introduction}
Rado asked in 1966 (see Problem P531 in \cite{rado1966abstract}) if it is possible to extend the concept of matroids to infinite
without loosing
duality and minors. Based on the works of Higgs (see \cite{higgs1969matroids}) and
Oxley (see \cite{oxley1978infinite} and \cite{oxley1992infinite... | {'timestamp': '2021-03-30T02:14:36', 'yymm': '2103', 'arxiv_id': '2103.14881', 'language': 'en', 'url': 'https://arxiv.org/abs/2103.14881'} |
\section{\bf{I.} Sample structure for the record-quality two-dimensional electron systems}
\begin{figure*}[h]
\centering
\includegraphics[width=.80\textwidth]{Supplement_R1_Page_2.png}
\caption{\label{figS1}Sample structure for the record-quality GaAs two-dimensional electron systems whose data are shown in the... | {'timestamp': '2020-10-07T02:02:27', 'yymm': '2010', 'arxiv_id': '2010.02283', 'language': 'en', 'url': 'https://arxiv.org/abs/2010.02283'} |
\section{Introduction}
The introduction of a conducting surface into a region disturbs the electromagnetic field. As a general
measure of the disturbance we can calculate the mode sum
\begin{equation}
\label{modesum}
S(\Omega) = \sum_{\alpha} \left (e^{-\omega_{\alpha}/\Omega} - e^{-\overline{\omega}_{\alpha}/\Omega... | {'timestamp': '2014-03-17T01:01:02', 'yymm': '1403', 'arxiv_id': '1403.3439', 'language': 'en', 'url': 'https://arxiv.org/abs/1403.3439'} |
\section{Introduction}
\label{sec:intro}
With the rapid growth of society and the modern logistics industry, road infrastructure has been greatly increased in today's world. There are a total of more than 64,000,000 kilometers of roads in the world~\cite{length}, which leads to massive operational requirements for pave... | {'timestamp': '2022-04-01T02:13:48', 'yymm': '2203', 'arxiv_id': '2203.16782', 'language': 'en', 'url': 'https://arxiv.org/abs/2203.16782'} |
\section{Introduction}
The study of supremum of Gaussian processes is a major area of study in probability and functional analysis as epitomized by the celebrated {\it majorizing measures} theorem of Fernique and Talagrand (see \cite{LedouxT}, \cite{Talagrand05} and references therein). There is by now a rich body o... | {'timestamp': '2012-02-23T02:03:17', 'yymm': '1202', 'arxiv_id': '1202.4970', 'language': 'en', 'url': 'https://arxiv.org/abs/1202.4970'} |
\section{Introduction}
\label{intro}
The development and refinement in recent years of new techniques in materials
growth has made it possible
to fabricate superconducting heterostructures with various materials and
high quality interfaces. These advances, coupled
with the continuing intense level of activity in the... | {'timestamp': '1999-02-07T03:52:15', 'yymm': '9902', 'arxiv_id': 'cond-mat/9902080', 'language': 'en', 'url': 'https://arxiv.org/abs/cond-mat/9902080'} |
\section{Introduction}
\begin{figure}[t]
\includegraphics[width=\columnwidth]{figures/intro_fig_2.png}
\caption{Overview of our experimental design. Two probes are evaluated using learning curves (including zero-shot). \robertal{}'s (red squares, upper text in black) accuracy is compared to a \textsc{No Language}... | {'timestamp': '2020-11-20T02:10:27', 'yymm': '1912', 'arxiv_id': '1912.13283', 'language': 'en', 'url': 'https://arxiv.org/abs/1912.13283'} |
\section{Introduction}
Spectral line surveys have revealed that high-mass star-forming
regions are rich reservoirs of molecules from simple diatomic species
to complex and larger molecules (e.g.,
\citealt{schilke1997b,hatchell1998b,comito2005,bisschop2007}).
However, there have been rarely studies undertaken to invest... | {'timestamp': '2008-01-29T14:32:19', 'yymm': '0801', 'arxiv_id': '0801.4493', 'language': 'en', 'url': 'https://arxiv.org/abs/0801.4493'} |
\section{Introduction} \label{sec:introduction}
We consider nonconvex quadratically constrained quadratic programs (QCQPs) of the form
\begin{align}
\label{eq:hqcqp} \tag{$\PC$}
\begin{array}{rl}
\min & \trans{\x}Q^0 \x \\
\subto & \trans{\x}Q^p \x \leq b_p, \quad p \in [m],
\end{array}
\end{... | {'timestamp': '2022-05-03T02:32:05', 'yymm': '2204', 'arxiv_id': '2204.09509', 'language': 'en', 'url': 'https://arxiv.org/abs/2204.09509'} |
\section{Introduction}
Conventional approaches to distributed network optimization are based on iterative descent in either the primal or dual domain. The reason for this is that for many types of network optimization problems there exist descent directions that can be computed in a distributed fashion. Subgradient de... | {'timestamp': '2012-03-14T01:03:42', 'yymm': '1203', 'arxiv_id': '1203.2808', 'language': 'en', 'url': 'https://arxiv.org/abs/1203.2808'} |
\section{introduction}
In the past few years, the synthesis of ferromagnetic semiconductors has become a major challenge for spintronics. Actually, growing a magnetic and semiconducting material could lead to promising advances like spin injection into non magnetic semiconductors, or electrical manipulation of carrier ... | {'timestamp': '2007-05-04T09:14:13', 'yymm': '0705', 'arxiv_id': '0705.0566', 'language': 'en', 'url': 'https://arxiv.org/abs/0705.0566'} |
\section{Introduction}
In 1914 Fekete constructed a formal power series $\sum_{n = 1}^{\infty} a_n x^n$ with the following \textit{universal} property: For any continuous function $f$ on $[-1,1]$ (with $f(0) = 0$) and given any $\varepsilon > 0$ there exists an integer $N > 0$ such that
$$
\sup_{-1 \leq x \leq 1} ... | {'timestamp': '2016-12-06T02:14:26', 'yymm': '1611', 'arxiv_id': '1611.10325', 'language': 'en', 'url': 'https://arxiv.org/abs/1611.10325'} |
\section{Introduction }
\label{intro}
Majorana zero modes (MZMs) in topological superconductors~\cite{m1,m2,m4,m5,m6} have generated significant interest because of their potential
utility in topological quantum computation~\cite{nayakrmp}. For this
purpose, proximity-induced topological superconductors based on
... | {'timestamp': '2021-05-17T02:06:22', 'yymm': '1907', 'arxiv_id': '1907.10626', 'language': 'en', 'url': 'https://arxiv.org/abs/1907.10626'} |
\section{Introduction}
\label{sec:intro}
Face hallucination
(FH) refers to the task of recovering high-resolution (HR) facial images from corresponding low-resolution (LR) inputs~\cite{baker_pami2002, chen2018fsrnet, grm2018face}. Solutions to this task have applications in face-oriented vision problems, such as face e... | {'timestamp': '2018-12-24T02:08:48', 'yymm': '1812', 'arxiv_id': '1812.09010', 'language': 'en', 'url': 'https://arxiv.org/abs/1812.09010'} |
\section{Introduction}
In this paper, a robust tracking control scheme is designed for a class of uncertain nonlinear systems. The design is composed of two steps. In the first step a linearized uncertainty model for the uncertain nonlinear system is developed using a robust feedback linearization approach.
The feed... | {'timestamp': '2012-03-01T02:01:34', 'yymm': '1202', 'arxiv_id': '1202.6436', 'language': 'en', 'url': 'https://arxiv.org/abs/1202.6436'} |
\section{Introduction}
One of the major goals of relativistic heavy-ion collisions is to explore the QCD phase diagram and phase boundary~\cite{StephanovPD,adams2005experimental,conservecharge0,conservecharge1}. Theoretical studies have shown the existence of a critical point (CP) at finite baryon chemical potential an... | {'timestamp': '2021-04-29T02:07:24', 'yymm': '2104', 'arxiv_id': '2104.11524', 'language': 'en', 'url': 'https://arxiv.org/abs/2104.11524'} |
\section{Introduction}
In general, a model of distributed computing is a set of \emph{runs}, i.e., all
allowed interleavings of \emph{steps} of concurrent processes.
There are multiple ways to define these sets of runs in a tractable way.
A natural one is based on \emph{failure models} that
describe the assumptions ... | {'timestamp': '2017-03-13T01:08:36', 'yymm': '1702', 'arxiv_id': '1702.00361', 'language': 'en', 'url': 'https://arxiv.org/abs/1702.00361'} |
\section{Introduction}
Recent observational and theoretical studies suggest that
gravitational microlensing can induce variability not only in
optical light, but also in the X-ray emission of lensed QSOs
\citep{Chart02a,Chart04,Dai03,Dai04,pj06,Pop01,Pop03a,Pop03b,Pop06a,Pop06b}.
Variability studies of QSOs indicate ... | {'timestamp': '2008-01-29T12:28:11', 'yymm': '0801', 'arxiv_id': '0801.4473', 'language': 'en', 'url': 'https://arxiv.org/abs/0801.4473'} |
\section{0pt}{6pt plus 4pt minus 2pt}{4pt plus 2pt minus 2pt}
\titlespacing\subsection{0pt}{6pt plus 4pt minus 2pt}{0pt plus 2pt minus 2pt}
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\titlespacing\paragraph{0pt}{6pt plus 4pt minus 2pt}{12pt plus 2pt minus 2pt}
\titleformat*{\secti... | {'timestamp': '2019-07-15T02:08:25', 'yymm': '1907', 'arxiv_id': '1907.01676', 'language': 'en', 'url': 'https://arxiv.org/abs/1907.01676'} |
\section{Introduction}
Recently, substantial progress has been achieved in the search of non-supersymmetric
Minkowski/dS vacua in the context of string/M-theory compactifications. This was mainly related
to the understanding of the superpotentials generated by background fluxes \cite{GVW} and by
non-perturbative eff... | {'timestamp': '2008-04-23T16:55:19', 'yymm': '0804', 'arxiv_id': '0804.3730', 'language': 'en', 'url': 'https://arxiv.org/abs/0804.3730'} |
\section{Related Work}
\label{sec:background}
There has been a growing interest in flaky tests in recent years, especially after the publication of Martin Fowler's article on the potential issues with non-deterministic tests \cite{fowler2011eradicating}, and Luo et al.'s \cite{luo2014empirical} seminal study.
To the ... | {'timestamp': '2022-12-05T02:03:21', 'yymm': '2212', 'arxiv_id': '2212.00908', 'language': 'en', 'url': 'https://arxiv.org/abs/2212.00908'} |
\section{Introduction}
Initial results from SuperKamiokande \cite{SuperK} appear
to confirm indications from IMB,~\cite{IMB} Kamiokande~\cite{Kam}
and Soudan~\cite{Soud} of an excess of $\nu_e$ relative to $\nu_\mu$
in the atmospheric neutrinos. One possible interpretation is
that neutrino flavor oscillations pla... | {'timestamp': '1997-08-15T18:23:02', 'yymm': '9708', 'arxiv_id': 'astro-ph/9708146', 'language': 'en', 'url': 'https://arxiv.org/abs/astro-ph/9708146'} |
\section{Introduction}
Please follow the steps outlined below when submitting your manuscript to
the IEEE Computer Society Press. This style guide now has several
important modifications (for example, you are no longer warned against the
use of sticky tape to attach your artwork to the paper), so all authors
should r... | {'timestamp': '2019-08-14T02:08:56', 'yymm': '1905', 'arxiv_id': '1905.01278', 'language': 'en', 'url': 'https://arxiv.org/abs/1905.01278'} |
\section{Introduction}\label{Intro}
Dimension reduction is a fundamental concept in science and engineering
for feature extraction and data visualization. Exploring the properties of low-dimensional structures in high-dimensional spaces attracts
broad attention. Popular dimension reduction methods include principal ... | {'timestamp': '2021-10-22T02:22:23', 'yymm': '2010', 'arxiv_id': '2010.10797', 'language': 'en', 'url': 'https://arxiv.org/abs/2010.10797'} |
\section{Introduction}
In this paper, we introduce a new non-displaceability criterion for Lagrangian
submanifolds of a given compact symplectic (four-)manifold. The criterion is
based on a Hamiltonian isotopy invariant of a Lagrangian
submanifold constructed using $J$-holomorphic disks \emph{of lowest area}
with boun... | {'timestamp': '2017-07-04T02:00:42', 'yymm': '1511', 'arxiv_id': '1511.00891', 'language': 'en', 'url': 'https://arxiv.org/abs/1511.00891'} |
\section{Introduction}
Pion-nucleon scattering in the $J^{P}=1/2^{+}$ channel captures the information on the
excitations of the nucleon ($N=p, n$). The $N\pi$ scattering in $p$-wave is elastic only
below the inelastic threshold $m_N+2m_\pi$ for $N\pi\pi$. The main feature in this
channel at low energies is th... | {'timestamp': '2017-02-01T02:04:58', 'yymm': '1610', 'arxiv_id': '1610.01422', 'language': 'en', 'url': 'https://arxiv.org/abs/1610.01422'} |
\section{Introduction}
Although global stabilization of dynamical systems is of importance in system theory and engineering \cite{Kh:02,An:02},
it is sometimes difficult or impossible to synthesize a global stabilizing controller for certain linear and nonlinear systems \cite{Va:02}.
The reasons could be the poor c... | {'timestamp': '2015-04-02T02:13:11', 'yymm': '1504', 'arxiv_id': '1504.00307', 'language': 'en', 'url': 'https://arxiv.org/abs/1504.00307'} |
\section{Introduction}
The discovery of the Higgs boson in 2012 at the LHC has attested the success
of the standard model (SM) in describing the observed fermions and their
interactions. However, there exist many theoretical issues or open questions
that have no satisfactory answer. In particular, the observed flavour... | {'timestamp': '2017-10-30T01:03:40', 'yymm': '1705', 'arxiv_id': '1705.09743', 'language': 'en', 'url': 'https://arxiv.org/abs/1705.09743'} |
\section{Introduction} \label{intro}
Black holes have proven to be an excellent testing ground for theories
of gravity. In particular, one of the recent exciting developments
in string theory has been the reproduction of many of the macroscopic
black hole properties from the microscopic D-brane picture---for reviews
a... | {'timestamp': '1997-08-25T22:44:30', 'yymm': '9708', 'arxiv_id': 'hep-th/9708091', 'language': 'en', 'url': 'https://arxiv.org/abs/hep-th/9708091'} |
\section*{Introduction}
Microbial Fuel Cells (MFCs) are devices that produce electricity from waste-water by utilizing microbial metabolic oxidation processes \cite{ieropoulos2013energy}. A MFC consists of a proton exchange membrane (PEM), an anode (negative half-cell) and a cathode (positive half-cell). Electricity is... | {'timestamp': '2017-03-07T02:07:14', 'yymm': '1703', 'arxiv_id': '1703.01580', 'language': 'en', 'url': 'https://arxiv.org/abs/1703.01580'} |
\section{Introduction}
The nature of the "central engine" of active galactic nuclei (AGN) is still an open question. However,
usually it is assumed that the nuclear activity is caused by the accretion of matter on a super-massive black hole
\cite[SMBH, see][]{re84,be85}.
The radiation from the accretion disc is i... | {'timestamp': '2019-03-01T02:06:26', 'yymm': '1902', 'arxiv_id': '1902.10845', 'language': 'en', 'url': 'https://arxiv.org/abs/1902.10845'} |
\section{Introduction}
Devising Convolutional Neural Networks (CNN) that can run efficiently on resource-constrained edge devices has become an important research area. There is a continued push to put increasingly more capabilities on-device for personal privacy, latency, and scale-ability of solutions. On these const... | {'timestamp': '2020-04-20T02:04:17', 'yymm': '1906', 'arxiv_id': '1906.02256', 'language': 'en', 'url': 'https://arxiv.org/abs/1906.02256'} |
\section{Introduction}
A common self-referenced technique to measure phase and amplitude of an ultrashort laser pulse is Frequency-resolved optical
gating (FROG)~\cite{Trebino:1993}. An investigated pulse is split in two replicas, imposing a relative
delay upon the two which are guided into a nonlinear medium where s... | {'timestamp': '2020-10-09T02:15:25', 'yymm': '2010', 'arxiv_id': '2010.03930', 'language': 'en', 'url': 'https://arxiv.org/abs/2010.03930'} |
\section{Introduction}
The accessory parameters appeared first in the Riemann-Hilbert problem
asking for an ordinary differential equation whose solutions transform
according to a given monodromy group \cite{bolibrukh}. They reappear
in Liouville theory in the quest for an auxiliary differential
equation in which ... | {'timestamp': '2021-04-09T02:11:42', 'yymm': '2103', 'arxiv_id': '2103.05943', 'language': 'en', 'url': 'https://arxiv.org/abs/2103.05943'} |
\section{Introduction}
Instrumental variable methods are powerful tools for causal inference with unmeasured treatment-outcome confounding.
\citet{angrist1996identification} use potential outcomes to clarify the role of a binary instrumental variable in identifying causal effects. They show that the classic two-stage ... | {'timestamp': '2019-06-06T02:16:11', 'yymm': '1906', 'arxiv_id': '1906.02030', 'language': 'en', 'url': 'https://arxiv.org/abs/1906.02030'} |
\section{Introduction}
In the Friedmann-Robertson-Walker solution for the structure of the
universe the geometry and future of the expansion uniquely depend on
the mean mass density, $\rho_0$, and a possible cosmological constant.
It is a statement of arithmetic\,\cite{oort} that at redshift zero
$\Omega_M \equiv\rho_... | {'timestamp': '1998-04-28T22:51:50', 'yymm': '9804', 'arxiv_id': 'astro-ph/9804312', 'language': 'en', 'url': 'https://arxiv.org/abs/astro-ph/9804312'} |
\section{#1}}
\renewcommand{\theequation}{\thesection.\arabic{equation}}
\newcommand{\begin{equation}}{\begin{equation}}
\newcommand{\end{equation}}{\end{equation}}
\newcommand{\begin{eqnarray}}{\begin{eqnarray}}
\newcommand{\end{eqnarray}}{\end{eqnarray}}
\newcommand{\nonumber}{\nonumber}
\newcommand{\underline{1}}{\u... | {'timestamp': '2007-07-16T06:29:49', 'yymm': '0601', 'arxiv_id': 'hep-th/0601177', 'language': 'en', 'url': 'https://arxiv.org/abs/hep-th/0601177'} |
\section{Introduction}\label{sec:intro}
In {the} past a few years, subspace clustering~\cite{vidal2010tutorial,soltanolkotabi2012geometric} has been extensively studied and has established solid applications, for example, in computer vision~\cite{elhamifar2009sparse} and network topology inference~\cite{eriksson2011hig... | {'timestamp': '2016-05-27T02:05:18', 'yymm': '1503', 'arxiv_id': '1503.08356', 'language': 'en', 'url': 'https://arxiv.org/abs/1503.08356'} |
\section{Introduction}
The Higgs boson mass in the Standard
Model (SM) is not stable against qunatum corrections
and has quadratic divergences. Because the reduced Planck
scale is about 16 order larger than the electroweak (EW) scale,
there exists huge fine-tuning to have the EW-scale
Higgs boson mass, which is calle... | {'timestamp': '2011-09-13T02:01:58', 'yymm': '1109', 'arxiv_id': '1109.2329', 'language': 'en', 'url': 'https://arxiv.org/abs/1109.2329'} |
\section{Introduction}
Since their origin in the early $20$th century, the study of Hardy inequalities has been a vigorous field of research.
On the one hand, this stems from the great variety of applications Hardy inequalities have in analysis and mathematical physics, for example as uncertainty principles in quantu... | {'timestamp': '2021-04-01T02:23:19', 'yymm': '2103', 'arxiv_id': '2103.17019', 'language': 'en', 'url': 'https://arxiv.org/abs/2103.17019'} |
\section{Introduction} \label{Introduction}
Social networks have become an integral part of our lives. These networks can be represented as graphs with nodes being entities (members) of the network and edges representing the association between entities (members).
As the size of these graphs increases, it becomes qui... | {'timestamp': '2019-02-01T02:11:23', 'yymm': '1901', 'arxiv_id': '1901.11308', 'language': 'en', 'url': 'https://arxiv.org/abs/1901.11308'} |
\section{Introduction}
\label{introduction}
Non-leptonic decays of hyperons (NLDH) can be understood by a
mechanism~\cite{LE-6129} due to non-perturbative flavor and parity mixings in
the physical hadrons and the intervention of the strong-interaction Yukawa
hamiltonian.
In Ref.~\cite{LE-6129} we have shown that this ... | {'timestamp': '1998-05-12T06:20:27', 'yymm': '9804', 'arxiv_id': 'hep-ph/9804340', 'language': 'en', 'url': 'https://arxiv.org/abs/hep-ph/9804340'} |
\section{Introduction\label{intro}}
Widespread deployment of mobile sensors is expected to revolutionize
our ability to monitor and control physical environments. However, for these networks
to reach their full range of applicability they must be capable of
operating in uncertain and unstructured environments. Real... | {'timestamp': '2013-12-30T02:13:59', 'yymm': '1209', 'arxiv_id': '1209.2194', 'language': 'en', 'url': 'https://arxiv.org/abs/1209.2194'} |
\section*{\abstractname}%
\else
\small
\begin{center}%
{\bfseries \ackname\vspace{-.5em}\vspace{\z@}}%
\end{center}%
\quotation
\fi}
{\if@twocolumn\else\endquotation\fi}
\fi
\makeatother
\theoremstyle{remark}
\newtheorem{rmk}[thm]{Remark}
\newcommand{{\mathbb{A}}}{{\mathbb{A}}}
\newcommand{{\mathbb{B}}}{{\ma... | {'timestamp': '2022-08-02T02:34:21', 'yymm': '2208', 'arxiv_id': '2208.00889', 'language': 'en', 'url': 'https://arxiv.org/abs/2208.00889'} |
\section{Introduction}
Solutions of general relativistic Liouville's equation ($grl$) in
a prescribed space-time
have been considered by some investigators.
Most authors have sought its solutions as functions of the
constants of motion, generated by Killing vectors of the space-time in
question. See for example Ehler... | {'timestamp': '1998-04-27T21:29:23', 'yymm': '9804', 'arxiv_id': 'astro-ph/9804120', 'language': 'en', 'url': 'https://arxiv.org/abs/astro-ph/9804120'} |
\section{Introduction}
\label{sec:introduction}
Reinforcement Learning (RL) is a powerful algorithmic paradigm used to solve sequential decision-making problems and has resulted in great success in various types of environments, e.g., mastering the game of GO \citep{silver2017mastering}, playing computer games ... | {'timestamp': '2022-07-06T02:15:54', 'yymm': '2207', 'arxiv_id': '2207.02016', 'language': 'en', 'url': 'https://arxiv.org/abs/2207.02016'} |
\section{Submission of papers to NeurIPS 2022}
Please read the instructions below carefully and follow them faithfully.
\subsection{Style}
Papers to be submitted to NeurIPS 2022 must be prepared according to the
instructions presented here. Papers may only be up to {\bf nine} pages long,
including figures. Additi... | {'timestamp': '2022-08-02T02:32:36', 'yymm': '2208', 'arxiv_id': '2208.00815', 'language': 'en', 'url': 'https://arxiv.org/abs/2208.00815'} |
\section{Introduction} The Coq Proof
Assistant~\cite{the_coq_development_team_2019} is an Interactive Theorem Prover
in which one proves lemmas using tactic scripts. Individual tactics in these
scripts represent actions that transform the proof state of the lemma currently
being proved. A wide range of tactics exist, w... | {'timestamp': '2020-08-04T02:04:44', 'yymm': '2008', 'arxiv_id': '2008.00120', 'language': 'en', 'url': 'https://arxiv.org/abs/2008.00120'} |
\section{Introduction}
\whizard\ is a multi-purpose event generator for collider
physics~\cite{Kilian:2007gr}. It is a very general framework for all
types of colliders, but with a special emphasis on the physics program
at lepton colliders, and has been used for many studies and design
reports for e.g. ILC, CLIC and
... | {'timestamp': '2020-02-17T02:17:10', 'yymm': '2002', 'arxiv_id': '2002.06122', 'language': 'en', 'url': 'https://arxiv.org/abs/2002.06122'} |
\section{Introduction}
Gas dynamical processes are believed to play an important role in
the evolution of astrophysical systems on all length scales.
Smoothed particle hydrodynamics~(SPH) is a powerful gridless
particle method to solve complex fluid-dynamical problems. SPH
has a number of attractive features such as i... | {'timestamp': '2006-01-20T21:27:10', 'yymm': '0601', 'arxiv_id': 'astro-ph/0601480', 'language': 'en', 'url': 'https://arxiv.org/abs/astro-ph/0601480'} |
\section{Introduction}\label{sec:intro}
Historically, humans have performed inconsistently in judgemental forecasting \cite{Makridakis2010,TetlockExp2017}, which incorporates subjective opinion and probability estimates to predictions \cite{Lawrence2006}. Yet, human judgement remains essential in cases where pure sta... | {'timestamp': '2022-05-25T02:01:58', 'yymm': '2205', 'arxiv_id': '2205.11590', 'language': 'en', 'url': 'https://arxiv.org/abs/2205.11590'} |
\section{Introduction}
\label{intro}
Continuous variable (CV) systems are ubiquitous in quantum
information and communication protocols. Most of the CV
quantum information protocols are based on Gaussian states
as they are easy to prepare, manipulate and
measure~\cite{weedbrook-rmp-2012, adesso-2014}. One of the centr... | {'timestamp': '2020-07-27T02:05:26', 'yymm': '2004', 'arxiv_id': '2004.06649', 'language': 'en', 'url': 'https://arxiv.org/abs/2004.06649'} |
\section{Introduction}
\label{sec:intro}
Monaural music source separation has been the focus of many research efforts for over a decade.
This task aims at separating a music recording into several tracks where each track corresponds to a single instrument.
A related goal is to design
algorithms that can separate vocal... | {'timestamp': '2017-06-16T02:07:36', 'yymm': '1611', 'arxiv_id': '1611.06265', 'language': 'en', 'url': 'https://arxiv.org/abs/1611.06265'} |
\section{Introduction}\label{sec:Intro}
We consider the problem of transmitting equiprobable messages over several uses of an additive white Gaussian noise (AWGN) channel. We consider different power restrictions at the transmitter: (i) equal power constraint (all the codewords in the transmission code have equal energ... | {'timestamp': '2020-08-19T02:22:23', 'yymm': '1907', 'arxiv_id': '1907.03163', 'language': 'en', 'url': 'https://arxiv.org/abs/1907.03163'} |
\section{Introduction}
In recent years, vehicular technology has attracted significant attention from the automotive and telecommunication industries, leading to the emergence of vehicle-to-everything (V2X) communications for improving road safety, traffic management services and driving comfort.
V2X supported by the s... | {'timestamp': '2023-02-02T02:17:21', 'yymm': '2302', 'arxiv_id': '2302.00576', 'language': 'en', 'url': 'https://arxiv.org/abs/2302.00576'} |
\section{Introduction}
Canonical correlation analysis (CCA) is a powerful tool to integrate two data matrices \cite{klami2013bayesian,sun2008least,yang2017canonical,cai2016kernel,wang2017novel}, which has been comprehensively used in many diverse fields. Given two matrices $\bm{X}\in \mathbb{R}^{n\times p}$ and $\bm{Y}... | {'timestamp': '2017-10-16T02:04:46', 'yymm': '1710', 'arxiv_id': '1710.04792', 'language': 'en', 'url': 'https://arxiv.org/abs/1710.04792'} |
\section{Introduction}
Several different methods to construct minimal polynomials of Salem numbers have been investigated in the literature (see e.g.\ \cite{BDGPS,boyd,grossmcmullen,smyth}). Various authors associate Salem numbers to Coxeter polynomials and use this relation in order to construct Salem numbers (cf.\ f... | {'timestamp': '2015-01-23T02:14:24', 'yymm': '1501', 'arxiv_id': '1501.05557', 'language': 'en', 'url': 'https://arxiv.org/abs/1501.05557'} |
\section{Introduction}
\label{intro}
The essential achievements in nanoscience and nanotechnology during the past
decade lead to great interest in studying nanoscale optical fields. The
phenomenon of surface plasmon amplification by stimulated emission of
radiation (spaser) was proposed in Ref.~\onlinecite{Ber... | {'timestamp': '2013-10-02T02:05:53', 'yymm': '1310', 'arxiv_id': '1310.0136', 'language': 'en', 'url': 'https://arxiv.org/abs/1310.0136'} |
\section*{Introduction}
Quantum particles were long thought to fall into one of two classes: fermions or bosons.
The two classes are distinguished by the effect on the many-particle wavefunction of
exchanging any pair of such particles: for fermions, the wavefunction acquires a minus
sign, whereas for bosons it does n... | {'timestamp': '2019-07-09T02:10:48', 'yymm': '1907', 'arxiv_id': '1907.03208', 'language': 'en', 'url': 'https://arxiv.org/abs/1907.03208'} |
\section{Introduction}
The equation of motion for a supernova remnant (SNR)
can be modeled by a single law of motion or multiple
laws of motion when the appropriate boundary
conditions are provided.
Examples of a single law of motion are:
the Sedov expansion
in
the presence of a circumstellar medium (CSM) wi... | {'timestamp': '2017-01-02T02:02:35', 'yymm': '1612', 'arxiv_id': '1612.09442', 'language': 'en', 'url': 'https://arxiv.org/abs/1612.09442'} |
\section{Introduction}
The Laplace-Beltrami operator is a fundamental and widely studied mathematical tool carrying a lot of intrinsic topological and geometric information about the Riemannian manifold on which it is defined.
Its various discretizations, through graph Laplacians, have inspired many applications in d... | {'timestamp': '2017-01-02T02:02:30', 'yymm': '1612', 'arxiv_id': '1612.09434', 'language': 'en', 'url': 'https://arxiv.org/abs/1612.09434'} |
\section{Introduction}
\label{sec1}
Modern scientific research is characterized by a collection of massive and diverse data sets. One of the most important goals is to integrate these different data sets for making better predictions and statistical inferences. Given a target problem to solve, transfer learning \ci... | {'timestamp': '2020-06-19T02:18:23', 'yymm': '2006', 'arxiv_id': '2006.10593', 'language': 'en', 'url': 'https://arxiv.org/abs/2006.10593'} |
\subsubsection{\large #1}}
\newcommand{\otimes}{\otimes}
\def \varkappa {\varkappa}
\def ~---\ {~---\ }
\def \nolinebreak {\nolinebreak}
\def\={\;=\;}
\def\begin{aligned}{\begin{aligned}}
\def\end{aligned}{\end{aligned}}
\newcommand{\longrightarrow}{\longrightarrow}
\newcommand{\longrightarrow}{\longrightarrow}... | {'timestamp': '2013-01-22T02:00:41', 'yymm': '1301', 'arxiv_id': '1301.4541', 'language': 'en', 'url': 'https://arxiv.org/abs/1301.4541'} |
\section{Introduction \label{Introduction}}
From the string worldsheet perspective, two-dimensional non-linear $\sigma$-models with boundaries provide a rich area to describe curved background geometries with D-brane configurations in string theory. These non-perturbative degrees of freedom are essential higher-dim... | {'timestamp': '2019-04-09T02:07:57', 'yymm': '1904', 'arxiv_id': '1904.03390', 'language': 'en', 'url': 'https://arxiv.org/abs/1904.03390'} |
\section{Introduction}
The growth of ultra-thin Ag films on Pt(111) has received much attention in the past few decades~\cite{Davies1982, Paffett1985, Roder1993a, Hartel1993, Grossmann1996, Schuster1996, Becker1993}, caused mainly by complex surface alloying~\cite{Roder1993, Struber1993, Bendounan2012} resulting in t... | {'timestamp': '2016-11-22T02:02:53', 'yymm': '1611', 'arxiv_id': '1611.06354', 'language': 'en', 'url': 'https://arxiv.org/abs/1611.06354'} |
\section{Introduction}
\label{sec:1}
A smooth flow $(\phi_t)$ generated by a smooth vector field $X$ on a
compact manifold~$M$ is called \emph{stable} if the range of the Lie
derivative $\mathcal L_X: C^\infty(M) \to C^\infty(M)$ is closed and
it is called \emph{cohomology-free} or \emph{rigid} if it is stable
and the ... | {'timestamp': '2013-03-29T01:01:31', 'yymm': '1303', 'arxiv_id': '1303.7074', 'language': 'en', 'url': 'https://arxiv.org/abs/1303.7074'} |
\section{Introduction}\label{sec:model.def}
A relatively simple formulation for the problem of directed polymer in random medium is the following \cite{Cook1989, Giacomin2007}. The lattice consists of $L$ planes in the transversal direction. In every plane there are $N$ points that are connected to all points of the... | {'timestamp': '2013-11-20T02:11:36', 'yymm': '1311', 'arxiv_id': '1311.4815', 'language': 'en', 'url': 'https://arxiv.org/abs/1311.4815'} |
\section{Introduction}
Polarization measurements from astrophysical objects are a key piece
of information to decipher the physics and geometry of regions that
emit the observed photons. The emission from $\gamma$-ray bursts
(GRBs) has been notoriously difficult to understand due to the
complexity of modeling their bro... | {'timestamp': '2019-08-13T02:20:41', 'yymm': '1901', 'arxiv_id': '1901.04719', 'language': 'en', 'url': 'https://arxiv.org/abs/1901.04719'} |
\section{Introduction}
Vertex decomposable simplicial complexes are recursively defined
simplicial complexes that have been extensively studied in both
combinatorial algebraic topology and combinatorial commutative
algebra. This family of complexes, first defined by
Provan and Billera \cite{PB} for pure simplic... | {'timestamp': '2022-07-14T02:22:44', 'yymm': '2207', 'arxiv_id': '2207.06391', 'language': 'en', 'url': 'https://arxiv.org/abs/2207.06391'} |
\section{Introduction}
The Higgs-like particle has been discovered recently in Large Hadron
Collider (LHC) \cite{Aad:2012tfa,Chatrchyan:2012ufa}.
The one of primary interests of particle physics is to understand the mechanism of
dynamical electroweak symmetry breaking.
The one of the promising mechanism to expla... | {'timestamp': '2013-11-21T02:02:00', 'yymm': '1311', 'arxiv_id': '1311.4918', 'language': 'en', 'url': 'https://arxiv.org/abs/1311.4918'} |
\section{Introduction}
Gravitational microlensing is arguably the most successful detection technique for finding extrasolar planets beyond the snowline. Moreover, microlensing planets are located several kiloparsecs away \citep{par06, ben96, wam97} and provide an independent measure of the planet abundance in our Gal... | {'timestamp': '2018-05-01T02:17:17', 'yymm': '1804', 'arxiv_id': '1804.10136', 'language': 'en', 'url': 'https://arxiv.org/abs/1804.10136'} |
\section{Introduction}
In the theory of motives, rigid tensor categories arise which have a faithful tensor functor
to a category of super vector spaces over a field of characteristic $0$, but which
are not known to be super Tannakian.
In view of the good properties of super Tannakian categories, this raises the que... | {'timestamp': '2021-01-01T02:38:02', 'yymm': '2012', 'arxiv_id': '2012.15703', 'language': 'en', 'url': 'https://arxiv.org/abs/2012.15703'} |
\section{Introduction}
In the seminal work on two-dimensional $N=(2,2)$ supersymmetric gauged linear sigma models \cite{Witten:1993yc}, Witten has introduced a powerful machinery to analyze both geometric and non-geometric phases of supersymmetric worldsheet theories. In particular the study of Abelian gauged linear si... | {'timestamp': '2017-01-05T02:04:51', 'yymm': '1505', 'arxiv_id': '1505.00099', 'language': 'en', 'url': 'https://arxiv.org/abs/1505.00099'} |
\section{Introduction}
Let $(U_t)$ be a one-dimensional time-homogeneous diffusion process satisfying the stochastic differential equation
\[ dU_t = \nu(U_t) dt + \sigma(U_t) dW_t, \qquad U_0 = u_0, \]
where $(W_t)$ denotes a Brownian motion. The aim of this note is to bound, from above and below, the transition p... | {'timestamp': '2008-07-29T09:15:37', 'yymm': '0807', 'arxiv_id': '0807.4586', 'language': 'en', 'url': 'https://arxiv.org/abs/0807.4586'} |
\section{Introduction}
An intriguing open question in condensed matter physics, one with potential practical significance, is whether there exists a lower bound for the density of a crystal. In other words, how large can the average distance between nearest neighbor atoms be, before crystalline long-range order is sup... | {'timestamp': '2021-05-12T02:02:43', 'yymm': '2103', 'arxiv_id': '2103.04245', 'language': 'en', 'url': 'https://arxiv.org/abs/2103.04245'} |
\section{Introduction}
A current exciting challenge in particle physics is the explanation of the smallness of the neutrino masses through new physics at TeV scale. In this regard, the inverse seesaw mechanism(ISS) \cite{ISS} became the paradigm of successful TeV scale seesaw mechanism. Its minimal implementation re... | {'timestamp': '2016-06-03T02:10:10', 'yymm': '1602', 'arxiv_id': '1602.08126', 'language': 'en', 'url': 'https://arxiv.org/abs/1602.08126'} |
\subsubsection{Auxiliary Multicut}
Given a graph $G$ and a function $f : V(G) \to [p]$, the \emph{cost} of $f$ in $G$, denoted $\mathfrak{c}_G(f)$ is defined as the number of edges $e = uv \in E(G)$ with $f(u) \neq f(v)$.
We use the following intermediate problem, which we call \textsc{Auxiliary Multicut}.
The inp... | {'timestamp': '2019-07-11T02:10:27', 'yymm': '1810', 'arxiv_id': '1810.06864', 'language': 'en', 'url': 'https://arxiv.org/abs/1810.06864'} |
\section{Introduction}
In psychology, social sciences, and many other fields, researchers are usually interested in ``latent'' variables that cannot be measured directly, e.g., depression, anxiety, or intelligence. To get a grip on these latent concepts, one commonly-used strategy is to construct a measurement model... | {'timestamp': '2018-06-13T02:12:57', 'yymm': '1806', 'arxiv_id': '1806.04610', 'language': 'en', 'url': 'https://arxiv.org/abs/1806.04610'} |
\section{Introduction}
\subsection{Motivation}
A central problem in K\"ahler geometry, proposed by Calabi \cite{EC2} in the 1980's, is to find a canonical K\"ahler metric in a given cohomology class of a compact K\"ahler manifold. Calabi suggested looking for \textit{extremal K\"ahler metrics}, characterized by the ... | {'timestamp': '2021-09-02T02:13:34', 'yymm': '2108', 'arxiv_id': '2108.12297', 'language': 'en', 'url': 'https://arxiv.org/abs/2108.12297'} |
\section{Introduction}
\label{1}
When analysing process behaviour, one of the early choices one has to make is between a linear and a branching view of time. In branching-time semantics, the choices a process has for proceeding from a particular state are taken into account when defining a notion of process equivalen... | {'timestamp': '2013-09-05T02:02:38', 'yymm': '1309', 'arxiv_id': '1309.0891', 'language': 'en', 'url': 'https://arxiv.org/abs/1309.0891'} |
\section{Introduction:}
We consider Einstein's equation of general theory of relativity for a fluid with heat flow having the following energy-momentum tensor
\be T^{\alpha\beta} = (\rho + p) v^\alpha v^\beta - pg^{\alpha\beta} + q^\alpha v^\beta + q^\beta v^\alpha,\ee
where, $p$ and $\rho$ are the isotropic pre... | {'timestamp': '2019-11-19T02:08:45', 'yymm': '1911', 'arxiv_id': '1911.07058', 'language': 'en', 'url': 'https://arxiv.org/abs/1911.07058'} |
\section{Introduction}
\IEEEPARstart{H}{idden} markov models are very popular for modeling and simulating processes, when you do not observe...
\section{System Model}
Let $(S_n, X_n)$ be a two-component process, where $(S_n)$ is unobservable component and $(X_n)$ is observable one, $n \in \{1,2,\ldots, N\}$... | {'timestamp': '2015-03-10T01:05:53', 'yymm': '1503', 'arxiv_id': '1503.00167', 'language': 'en', 'url': 'https://arxiv.org/abs/1503.00167'} |
\section{Introduction}
Let $\mathbb{B}_{N}$ be the unit ball in $\mathbb{C}_{N}$ and $S_N$ denote the unit sphere. Let $H(\mathbb{B}_{N})$ be
the space of all holomorphic functions on $\mathbb{B}_{N}$. Denote by $S(\mathbb{B}_{N})$ the set of all holomorphic self-maps of $\mathbb{B}_{N}$. The Dirichlet space $\mathca... | {'timestamp': '2018-12-27T02:32:46', 'yymm': '1812', 'arxiv_id': '1812.10248', 'language': 'en', 'url': 'https://arxiv.org/abs/1812.10248'} |
\section{Introduction}\label{Introduccion}
The braid group of $n$ strings ${\mathbb B}_n$, is defined by generators
and relations as follows
$$
{\mathbb B}_{n}=<\tau_{1}, \dots,\tau_{n-1}>_{/\sim}
$$
$$
\sim=\{ \tau_k\tau_j=\tau_j\tau_k, \textrm{ if }|k- j|>1; \ \
\tau_k\tau_{k+1}\tau_k=\tau_{k+1}\tau_{k}\t... | {'timestamp': '2009-04-07T19:14:41', 'yymm': '0809', 'arxiv_id': '0809.4173', 'language': 'en', 'url': 'https://arxiv.org/abs/0809.4173'} |
\section{\label{sec:level1}First-level heading}
In the 1980s, studying the effect of the volume cap-
ture of relativistic protons into the channeling regime,
Taratin and Vorobiev [4, 5] demonstrated the possibility
of volume reflection, i.e., the coherent small-angle scattering of particles at angle $\theta \; \til... | {'timestamp': '2014-10-14T02:11:20', 'yymm': '1410', 'arxiv_id': '1410.3138', 'language': 'en', 'url': 'https://arxiv.org/abs/1410.3138'} |
\section{Introduction}
Understanding the volatility of financial assets is a key problem in econometrics and finance. Over the last two decades, the literature that deals with the modelling of financial asset volatility has expanded significantly. Volatility, a latent variable as such, has been shown to be highly per... | {'timestamp': '2009-01-09T22:08:30', 'yymm': '0901', 'arxiv_id': '0901.1315', 'language': 'en', 'url': 'https://arxiv.org/abs/0901.1315'} |
\section{Introduction}
Cryptographic schemes are mainly classified into public key cryptography and symmetric key cryptography.
In symmetric key encryption schemes, both the sender and the receiver of a message use a common key, therefore they have to share the common key in advance.
Public key cryptographic schemes u... | {'timestamp': '2021-07-14T02:13:55', 'yymm': '2107', 'arxiv_id': '2107.05924', 'language': 'en', 'url': 'https://arxiv.org/abs/2107.05924'} |
\section{Introduction} \label{section_introduction}
It is well-known that Saturn, Jupiter, Uranus and Neptune have ring systems. For Mars, no rings have been detected yet, but it was suggested by \citet{soter1971dust} that Mars should possess a ring system, which consists of dust grains originating from Phobos and Deim... | {'timestamp': '2022-01-11T02:11:19', 'yymm': '2201', 'arxiv_id': '2201.02847', 'language': 'en', 'url': 'https://arxiv.org/abs/2201.02847'} |
\section{Introduction and main results}
We consider a lattice system of unbounded and continuous spins on the $d$-dimensional lattice $\mathds{Z}^d$. The formal Hamiltonian $H: \mathds{R}^{\mathds{Z}^d} \to \mathds{R}$ of the system is given by
\begin{equation}
\label{e_d_Hamiltonian}
H(x) = \sum_{i \in \mathds{... | {'timestamp': '2014-04-11T02:11:22', 'yymm': '1309', 'arxiv_id': '1309.0862', 'language': 'en', 'url': 'https://arxiv.org/abs/1309.0862'} |
\section{Introduction}
\label{sec:intro}
Nucleon polarizabilities are of fundamental importance for understanding the dynamics of the internal structure of nucleons. The static electric and magnetic dipole polarizabilities, $\alpha_{E1}$ and $\beta_{M1}$, characterize the response of the nucleon to external electromagn... | {'timestamp': '2020-04-28T02:04:06', 'yymm': '1912', 'arxiv_id': '1912.06915', 'language': 'en', 'url': 'https://arxiv.org/abs/1912.06915'} |
\section{Introduction}
The $q$-state Potts model \cite{Potts_52,Wu_82,Wu_84} is certainly one of
the simplest and most studied models in Statistical Mechanics.
However, despite many efforts over more than 50 years, its {\em exact}
solution (even in two dimensions) is still unknown. The ferromagnetic
regime is the ... | {'timestamp': '2009-05-22T12:37:21', 'yymm': '0901', 'arxiv_id': '0901.1010', 'language': 'en', 'url': 'https://arxiv.org/abs/0901.1010'} |
\section{Introduction}
\subsection{Innermost stable circular orbits in General Relativity}
Let us consider a classical test non-spinning particle moving at stable circular orbit around a central massive body. In Newtonian theory, this orbit can have arbitrary radius. This follows from the fact that the effective pote... | {'timestamp': '2016-05-16T02:10:06', 'yymm': '1605', 'arxiv_id': '1605.04189', 'language': 'en', 'url': 'https://arxiv.org/abs/1605.04189'} |
\section{Introduction}
Being the unique standard model (SM) fermion with a mass of the
electroweak symmetry breaking scale, the top quark may be closely
related to the TeV scale new physics. In particular, many of the new
physics candidates predict a $t\,\bar t$ ($t\,t$) resonance, i.e., a
heavy particle that decays ... | {'timestamp': '2009-04-13T00:35:42', 'yymm': '0809', 'arxiv_id': '0809.4487', 'language': 'en', 'url': 'https://arxiv.org/abs/0809.4487'} |
\section{Introduction}\label{Introduction}
The quantification of shapes has become an important research direction in both the applied and theoretical sciences. It has brought advances to many fields including network analysis \citep{lee2011discriminative}, geometric morphometrics \citep{boyer2011algorithms,gao2019gau... | {'timestamp': '2022-04-28T02:11:35', 'yymm': '2204', 'arxiv_id': '2204.12699', 'language': 'en', 'url': 'https://arxiv.org/abs/2204.12699'} |
\subsubsection{Training Neural Network Vehicle Dynamics}
Our fully-connected neural network approximates the nonlinear vehicle dynamics. Note that only the dynamic state variables are considered as input to the neural network. We denote $\left|{\bf x}_{d}\right|$ and $\left|{\bf u}\right|$ as the size of the ... | {'timestamp': '2022-07-15T02:19:04', 'yymm': '2201', 'arxiv_id': '2201.08321', 'language': 'en', 'url': 'https://arxiv.org/abs/2201.08321'} |
\section{Introduction} \label{sec:intro}
\subsection{A brief history of Mendelian
randomization} \label{sec:intro:historyofmr}
Mendelian randomization (MR) is a causal inference approach that uses the
random allocation of genes from parents to offspring as a foundation
for causal inference \parencite{Sanderson2022}... | {'timestamp': '2022-08-31T02:09:41', 'yymm': '2208', 'arxiv_id': '2208.14035', 'language': 'en', 'url': 'https://arxiv.org/abs/2208.14035'} |
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