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\section{Introduction}
Suppose $E$ is a commutative $S$-algebra, in the sense of \cite{EKMM},
and $A$ is a commutative $E$-algebra. We want to capture the properties
and underlying structure of the homotopy groups $\pi_* A = A_*$ of $A$,
by studying operations associated to the cohomology theory that $E$
represen... | {
"timestamp": "2012-10-16T02:02:08",
"yymm": "1210",
"arxiv_id": "1210.3730",
"language": "en",
"url": "https://arxiv.org/abs/1210.3730"
} |
\subsection{Clustered Erd\"{o}s-R\'{e}nyi graphs} \label{sub:structure}
Recall that for an integer $n \ge 1$ and $0 \le p \le 1$, the Erd\"{o}s-R\'{e}nyi graph
$G(n, p)$ is the random graph obtained by starting with vertex set
$V = \{1,2,\ldots,n\}$ and connecting each pair of vertices $u, v \in V$,
independently wi... | {
"timestamp": "2012-10-16T02:02:14",
"yymm": "1210",
"arxiv_id": "1210.3735",
"language": "en",
"url": "https://arxiv.org/abs/1210.3735"
} |
\section{Introduction}
Young dense star clusters observed in the Milky Way and the Large
Magellanic Cloud (LMC), e.g.,
R136 \citep{1998ApJ...493..180M,2010MNRAS.408..731C},
NGC 3603 \citep{2006AJ....132..253S,2008ApJ...675.1319H},
Westerlund 1
\citep{2005A&A...434..949C,2008A&A...478..137B,2011MNRAS.412.2469G}
an... | {
"timestamp": "2012-10-16T02:02:10",
"yymm": "1210",
"arxiv_id": "1210.3732",
"language": "en",
"url": "https://arxiv.org/abs/1210.3732"
} |
\section*{}
\begin{Large}
\begin{center}
Abstract
\end{center}
\end{Large}
\begin{small}
\noindent\noindent
The current attempt is aimed to honor
the first centennial of Johannes
Diderik van der Waals (VDW) awarding
Nobel Prize in Physics. The VDW
theory of ordinary fluids is reviewed
in the firs... | {
"timestamp": "2012-10-16T02:01:28",
"yymm": "1210",
"arxiv_id": "1210.3688",
"language": "en",
"url": "https://arxiv.org/abs/1210.3688"
} |
\section{Introduction}
Suppose that one has $n$ copies of a quantum system each in the same state depending on an unknown parameter $\theta$, and one wishes to estimate $\theta$ by making some measurement on the $n$ systems together.
This yields data whose distribution depends on $\theta$ and on the choice of the... | {
"timestamp": "2013-08-30T02:06:24",
"yymm": "1210",
"arxiv_id": "1210.3749",
"language": "en",
"url": "https://arxiv.org/abs/1210.3749"
} |
\section{Introduction}
Ricci solitons are precisely those Riemannian metrics that are `nice' enough to be `upgraded' by the Ricci flow, in the sense that they just evolve by scaling and pull-back by diffeomorphisms. A good understanding of them is therefore crucial to study the singularity behavior of the Ricci flo... | {
"timestamp": "2012-10-16T02:00:56",
"yymm": "1210",
"arxiv_id": "1210.3656",
"language": "en",
"url": "https://arxiv.org/abs/1210.3656"
} |
\section{Introduction}
We consider spherically symmetric motions of atmosphere governed by the
compressible Euler equations:
\begin{eqnarray}
&&\frac{\partial\rho}{\partial t} +u\frac{\partial \rho}{\partial r}+\rho\frac{\partial u}{\partial r}
+\frac{2}{r}\rho u =0, \nonumber \\
&&\rho\Big(\frac{\partial u}{\... | {
"timestamp": "2013-07-16T02:07:20",
"yymm": "1210",
"arxiv_id": "1210.3670",
"language": "en",
"url": "https://arxiv.org/abs/1210.3670"
} |
\section{Introduction}
\label{intro}
Particle-based simulation methods have a long and successful history in plasma physics. The original proposal by Hockney~\cite{hockney:1826}, based on a method developed for fluid simulations
\cite{harlow:1964}, used computational macro-particles moving in a self-consistent, mean ... | {
"timestamp": "2012-12-14T02:02:49",
"yymm": "1210",
"arxiv_id": "1210.3743",
"language": "en",
"url": "https://arxiv.org/abs/1210.3743"
} |
\section*{References}
[1] Brennen, C. E., 1970, “Cavity Surface Wave Patterns and General Appearance,” J. Fluid Mech. 44 ptI, pp. 33-49
\noindent
[2] Andre, M.A. and Bardet, P.M., 2012, “Experimental investigation of boundary layer instabilities on the free surface of non-turbulent jet”, Proceedings of the Open Foru... | {
"timestamp": "2012-10-30T01:05:10",
"yymm": "1210",
"arxiv_id": "1210.3676",
"language": "en",
"url": "https://arxiv.org/abs/1210.3676"
} |
\section{Introduction}
\label{Intro}
The topic of vector meson interactions with nuclei has attracted, and continues to attract, much attention. After thorough experimental and theoretical studies of pion nuclear interaction and other pseudoscalar nucleus interactions, the turn came for exploring the properties of the... | {
"timestamp": "2012-10-16T02:02:16",
"yymm": "1210",
"arxiv_id": "1210.3738",
"language": "en",
"url": "https://arxiv.org/abs/1210.3738"
} |
\section{Introduction}
Gamma ray bursts (GRBs) are the most energetic explosions known in the Universe, second only to the Big Bang. Discovered in the 1960s, they were widely believed to originate in the Milky Way because of their relatively high flux of photons, which needs an unprecedented emission mechanism to accou... | {
"timestamp": "2013-01-23T02:02:56",
"yymm": "1210",
"arxiv_id": "1210.3699",
"language": "en",
"url": "https://arxiv.org/abs/1210.3699"
} |
\section{Introduction}
\label{introduction}
Microsphere composites are used in a multitude of industrial applications. Good examples are ultra-low density fillers in engineering materials such as composites, coatings, sealants, explosives, automotive components, paint and crack fillers and elastomers and as blowing age... | {
"timestamp": "2012-10-16T02:01:47",
"yymm": "1210",
"arxiv_id": "1210.3701",
"language": "en",
"url": "https://arxiv.org/abs/1210.3701"
} |
\section{Introduction} \label{sec:intro}
This paper considers a novel problem in experimental design: suppose an
experimenter is studying a physical or biological system that can be
modeled by a diffusion process of the general form
\begin{equation}
d\xbold_t = \fbold(\xbold_t,\theta,u_t) dt + \Sigma(\xbol... | {
"timestamp": "2013-06-10T02:00:46",
"yymm": "1210",
"arxiv_id": "1210.3739",
"language": "en",
"url": "https://arxiv.org/abs/1210.3739"
} |
\section{Introduction}
The development of solution methods and computational algorithms for solving multidimensional extremal problems is one of the important concerns in the linear tropical (idempotent) algebra \cite{Baccelli92Synchronization,Cuninghamegreen94Minimax,Kolokoltsov97Idempotent,Golan03Semirings,Heiderg... | {
"timestamp": "2012-10-16T02:00:59",
"yymm": "1210",
"arxiv_id": "1210.3658",
"language": "en",
"url": "https://arxiv.org/abs/1210.3658"
} |
\section{Introduction}
Recent years, the models based on the hypothesis that our universe
is a four-dimensional space-time hypersurface (3-brane) embedded in
a fundamental multi-dimensional space \ci{rushap},\ci{otherbr} have become quite popular,
see, for example, the reviews \ci{RuBar}-\ci{loc6} and the references
t... | {
"timestamp": "2013-06-04T02:05:04",
"yymm": "1210",
"arxiv_id": "1210.3698",
"language": "en",
"url": "https://arxiv.org/abs/1210.3698"
} |
\section{Introduction}
Scaling limits of discrete particle systems is a central question in Statistical Mechanics. In the case of interacting particle systems, where particles evolve according to some rule of interaction, it is of interest to characterize, in the continuum limit, the time trajectory of the spatial de... | {
"timestamp": "2013-03-26T01:02:43",
"yymm": "1210",
"arxiv_id": "1210.3662",
"language": "en",
"url": "https://arxiv.org/abs/1210.3662"
} |
\section*{Supplementary material for Bosonic Anderson insulators in a magnetic field}
\section*{I. HIERARCHICAL LOOP MODEL}
Here we analyze in more detail the hierarchical loop model defined in the main text. This model implements the ideas of the droplet picture in an analytically tractable and mathematically... | {
"timestamp": "2012-10-16T02:02:07",
"yymm": "1210",
"arxiv_id": "1210.3726",
"language": "en",
"url": "https://arxiv.org/abs/1210.3726"
} |
\section{Introduction}
Quantum computers take direct advantage of superposition and entanglement to perform computations.
Because quantum algorithms compute in ways which classical computers cannot,
for certain problems they provide exponential
speedups over their classical counterparts
\cite{Micheli2006,Ni2008a,Kotoc... | {
"timestamp": "2012-12-17T02:00:41",
"yymm": "1210",
"arxiv_id": "1210.3669",
"language": "en",
"url": "https://arxiv.org/abs/1210.3669"
} |
\section{Introduction}
The magnetic field’s configuration is essential for us to understand solar explosive phenomena such as flares
and coronal mass ejections. The corona has been the subject of extensive modeling for decades, but these efforts
have been hampered by our limited ability to determine the corona's thre... | {
"timestamp": "2012-10-16T02:01:07",
"yymm": "1210",
"arxiv_id": "1210.3668",
"language": "en",
"url": "https://arxiv.org/abs/1210.3668"
} |
\section{Introduction}
Magnetic materials that have high spin polarization at room
temperature or higher are highly desirable for spintronic
applications\cite{wolf,cro2-96}. Half-metallic materials are good
candidates because they can have high spin polarization at high
temperature\cite{hm}. In the case of CrO$_2$, 96... | {
"timestamp": "2012-10-30T01:00:48",
"yymm": "1210",
"arxiv_id": "1210.3706",
"language": "en",
"url": "https://arxiv.org/abs/1210.3706"
} |
\section*{Results and discussion}
\subsection*{Elastic energy of a thin shell}
The elastic energy of a deformed spherical shell of radius $R$ is calculated using \emph{shallow-shell theory}~\cite{koiter_stability}. This approach considers a shallow section of the shell, small enough so that slopes measured relative to ... | {
"timestamp": "2012-10-16T02:01:50",
"yymm": "1210",
"arxiv_id": "1210.3704",
"language": "en",
"url": "https://arxiv.org/abs/1210.3704"
} |
\section{#1}}
\def\left{\left}
\def\right{\right}
\def\mathbf{t}{\mathbf{t}}
\newcommand{\arctanh}[1]{\text{arctanh}}
\begin{document}
\begin{titlepage}
\begin{flushright}
{\tt hep-th/...}
\tt {FileName:....tex} \\
{\tt \today}
\end{flushright}
\vspace{0.5in}
\begin{center}
{\large \bf Diffractive and de... | {
"timestamp": "2012-10-16T02:02:05",
"yymm": "1210",
"arxiv_id": "1210.3724",
"language": "en",
"url": "https://arxiv.org/abs/1210.3724"
} |
\section{Introduction}\label{S:introduction}
Let $k$ be a field, and let ${k^{\operatorname{sep}}}$ be a separable closure.
Let $X$ be a smooth projective geometrically integral $k$-variety,
and let ${X^{\operatorname{sep}}} \colonequals X \times_k {k^{\operatorname{sep}}}$.
If $k=\mathbb{C}$, then the Lefschetz $(1,... | {
"timestamp": "2013-03-29T01:01:04",
"yymm": "1210",
"arxiv_id": "1210.3720",
"language": "en",
"url": "https://arxiv.org/abs/1210.3720"
} |
\section{Introduction}
There is recent interest in constructing theories of covering maps in various settings (Berestovskii-Plaut
\cite{BP3} and Brodskiy-Dydak-LaBuz-Mitra \cite{BDLM2}-\cite{BDLM3} for uniform spaces, Fischer-Zastrow \cite{FisZas} and Brodskiy-Dydak-LaBuz-Mitra \cite{BDLM} for locally path-connected... | {
"timestamp": "2012-10-18T02:03:20",
"yymm": "1210",
"arxiv_id": "1210.3733",
"language": "en",
"url": "https://arxiv.org/abs/1210.3733"
} |
\section{Introduction}
NGC\,6822 is an isolated barred dwarf irregular galaxy within the Local
Group. It is comparable in size to the SMC but has a slightly higher
metallicity (Muschielok et al. 1999; Venn et al. 2001). It contains
numerous supergiants and H{\sc ii} regions with obvious signs of star
formation and i... | {
"timestamp": "2012-10-16T02:01:43",
"yymm": "1210",
"arxiv_id": "1210.3695",
"language": "en",
"url": "https://arxiv.org/abs/1210.3695"
} |
\section{Introduction}
Spinor models play important role in contemporary theoretical physics.
The famous Nambu--Jona-Lasinio--Vaks--Larkin models \cite{NJL,VL} and
Gross--Neveu models \cite{GN,NePa} have been proposed initially as models for describing the
strong interactions. Later, with the development of the ... | {
"timestamp": "2012-10-16T02:02:04",
"yymm": "1210",
"arxiv_id": "1210.3722",
"language": "en",
"url": "https://arxiv.org/abs/1210.3722"
} |
\section{Introduction}
Granger causality \citep{granger69} provides a statistical framework for determining whether a time series $X$ is useful in forecasting another one $Y$, through a series of statistical tests.
It has found wide applicability in economics, including testing relationships between money and income \c... | {
"timestamp": "2012-11-05T02:01:07",
"yymm": "1210",
"arxiv_id": "1210.3711",
"language": "en",
"url": "https://arxiv.org/abs/1210.3711"
} |
\section{Introduction}
Consider the steady axisymmetric Euler equations for a fluid (incompressible and with
zero vorticity) with a free surface acted on only by gravity.
Using cylindrical coordinates and the Stokes stream function $\psi$
(see for example \cite[Exercise 4.18 (ii)]{fraenkel}),
we obtain the free bo... | {
"timestamp": "2012-10-16T02:01:21",
"yymm": "1210",
"arxiv_id": "1210.3682",
"language": "en",
"url": "https://arxiv.org/abs/1210.3682"
} |
\section{}
\begin{abstract}
For a $C^{1}$ degree two latitude preserving endomorphism $f$ of the $2$-sphere, we show that $f$ has $2^{n}$ periodic points.
\end{abstract}
\section{Introduction}
The relationship between the long term dynamics of an endomorphism of a manifold and its long term effect on the algebrai... | {
"timestamp": "2012-10-16T02:02:01",
"yymm": "1210",
"arxiv_id": "1210.3717",
"language": "en",
"url": "https://arxiv.org/abs/1210.3717"
} |
\subsection{Discrete Log based Equivocal Commitment Scheme \comdl}
\label{commitdl}
The committer and the receiver are given a group $\mathbb{G}$ of prime order $q$, its generator $g$ and an element $B \in \mathbb{G}$ such that $q$ is an $n-$bit prime. To commit to $x \in \mathbb{Z}_q$, choose $r \xleftarrow{\$} \mat... | {
"timestamp": "2012-10-16T02:02:03",
"yymm": "1210",
"arxiv_id": "1210.3719",
"language": "en",
"url": "https://arxiv.org/abs/1210.3719"
} |
\section*{The Pierre Auger Collaboration}
P.~Abreu$^{63}$, M.~Aglietta$^{51}$, M.~Ahlers$^{94}$, E.J.~Ahn$^{81}$, I.F.M.~Albuquerque$^{15}$, D.~Allard$^{29}$, I.~Allekotte$^{1}$, J.~Allen$^{85}$, P.~Allison$^{87}$, A.~Almela$^{11,\: 7}$, J.~Alvarez Castillo$^{56}$, J.~Alvarez-Mu\~{n}iz$^{73}$, R.~Alves Batista$^{16}$, ... | {
"timestamp": "2012-12-05T02:01:09",
"yymm": "1210",
"arxiv_id": "1210.3736",
"language": "en",
"url": "https://arxiv.org/abs/1210.3736"
} |
\section*{Abstract}
We demonstrate by mathematical analysis and systematic computer simulations that redistribution can lead to sustainable growth in a society. In accordance with economic models of risky human capital, we assume that dynamics of human capital is modeled as a multiplicative stochastic process which, i... | {
"timestamp": "2012-10-16T02:02:00",
"yymm": "1210",
"arxiv_id": "1210.3716",
"language": "en",
"url": "https://arxiv.org/abs/1210.3716"
} |
\section*{Acknowledgment}
We would like to thank F. Arroja, S. Dodelson, J-O. Gong,
L. Senatore, D. Wands and J. White for ueseful discussions and comments.
This work is supported in part by the JSPS Grant-in-Aid for Scientific Research
(A) No.~21244033, by the YITP Overseas Exchange Program for Young Researchers,
an... | {
"timestamp": "2013-03-19T02:15:19",
"yymm": "1210",
"arxiv_id": "1210.3692",
"language": "en",
"url": "https://arxiv.org/abs/1210.3692"
} |
\section{INTRODUCTION}
The study of the hadronic transitions between charmonium states has been an active field both for experimental and
theoretical research. The decays $\psip\to\eta\jp$ and $\pi^0\jp$ were first observed thirty years ago, and improved measurements of the corresponding branching fractions were perf... | {
"timestamp": "2012-10-16T02:02:20",
"yymm": "1210",
"arxiv_id": "1210.3746",
"language": "en",
"url": "https://arxiv.org/abs/1210.3746"
} |
\section{Introduction}
The spontaneous breaking of chiral symmetry (SBCS) in the QCD vacuum is believed
to be a consequence of the condensation of scalar quark-antiquark pairs.
It manifests itself in the generation of mass in strong interactions and, more
precisely, in lifting the degeneracies within chiral multip... | {
"timestamp": "2012-10-16T02:01:01",
"yymm": "1210",
"arxiv_id": "1210.3660",
"language": "en",
"url": "https://arxiv.org/abs/1210.3660"
} |
\section{Introduction: basic concepts and notation}
Let $S$ denote a closed marginally outer trapped surface (MOTS) in the spacetime $({\cal V},g)$.
This means that the outer null expansion vanishes $\theta_{\vec k}=0$, where here
the two future-pointing null vector fields orthogonal to $S$ are denoted by $\vec\ell$ a... | {
"timestamp": "2012-10-16T02:02:09",
"yymm": "1210",
"arxiv_id": "1210.3731",
"language": "en",
"url": "https://arxiv.org/abs/1210.3731"
} |
\section{Introduction}
The low-rank matrix completion is referred to recover an unknown low-rank matrix, exactly or approximately,
from the under-sampled observations with or without noises. This problem is of considerable interest in
many application areas, from machine learning to quantum state tomography.
A bas... | {
"timestamp": "2012-10-16T02:01:53",
"yymm": "1210",
"arxiv_id": "1210.3709",
"language": "en",
"url": "https://arxiv.org/abs/1210.3709"
} |
\section{The Double Chooz Experiment}
The primary goal of DC is measurement of the neutrino oscillation parameter $\theta_{13}$ through $\bar \nu_e$ disappearance.
The design of the Daya Bay and RENO detectors is similar to that of DC \cite{dc2012}.
All three experiments use the inverse beta decay (IBD) interacti... | {
"timestamp": "2012-10-23T02:01:23",
"yymm": "1210",
"arxiv_id": "1210.3748",
"language": "en",
"url": "https://arxiv.org/abs/1210.3748"
} |
\section{Introduction}
This work falls into a general framework which consists of observing the behavior of patterns and structures that can be formed after instability onset in an evaporating liquid layer. In previous work, we studied theoretical instability thresholds in pure fluids
[1,2] and in binary mixtures [3,... | {
"timestamp": "2012-10-16T02:02:08",
"yymm": "1210",
"arxiv_id": "1210.3728",
"language": "en",
"url": "https://arxiv.org/abs/1210.3728"
} |
\section{Introduction}
In recent years considerable progress has been made in understanding the evolutionary sequence of planetary nebulae (PNe). The evolution of the photoionised nebula needs to be understood with regard to the processes leading to its ejection, mass/density relation, chemical composition and the p... | {
"timestamp": "2012-10-17T02:11:20",
"yymm": "1210",
"arxiv_id": "1210.3750",
"language": "en",
"url": "https://arxiv.org/abs/1210.3750"
} |
\section{Introduction}
Trapped atomic ions are one of the most promising systems yet proposed for large-scale quantum information processing (QIP) and quantum simulation~\cite{Ladd2010}. Trapped ions benefit from long coherence times and have been used to perform high-fidelity single- and two-qubit gates~\cite{H.Haeff... | {
"timestamp": "2013-02-26T02:05:42",
"yymm": "1210",
"arxiv_id": "1210.3655",
"language": "en",
"url": "https://arxiv.org/abs/1210.3655"
} |
\section{Introduction}
Shape plays a key role in our cognitive system: in the perception of shape lies the beginning of concept formation.
Artists have implicitly acknowledged the importance of shapes since the dawn of times. Indeed, despite that lines do not divide objects from their background in the real world, li... | {
"timestamp": "2012-10-16T02:02:02",
"yymm": "1210",
"arxiv_id": "1210.3718",
"language": "en",
"url": "https://arxiv.org/abs/1210.3718"
} |
\section{Introduction}
When a liquid in a container is heated from below and cooled from the top a heat flux settles through the liquid. As the temperature of the bottom plate increases, the heat transport is successively dominated by different mechanisms: conduction, convection and boiling. To study this, experiments... | {
"timestamp": "2012-10-16T02:01:37",
"yymm": "1210",
"arxiv_id": "1210.3693",
"language": "en",
"url": "https://arxiv.org/abs/1210.3693"
} |
\section{Introduction}
The Large Hadron Collider (LHC) has clearly exhibited its ability to make discoveries with the observation of a new resonance~\cite{:2012gk,:2012gu} with even spin that decays to photons and Z bosons as expected of the Standard Model (SM) Higgs particle. Thus precise measurements of the decays... | {
"timestamp": "2012-10-22T02:02:32",
"yymm": "1210",
"arxiv_id": "1210.3657",
"language": "en",
"url": "https://arxiv.org/abs/1210.3657"
} |
\section{Introduction}
Considering the important role of the Higgs boson in particle physics,
hunting for it has been one of the major tasks of the running Large Hadron Collider (LHC).
Recently, both the ATLAS and CMS collaborations have reported some evidence for a light Higgs boson
near 125 GeV \cite{ATLAS,CMS} with ... | {
"timestamp": "2012-10-16T02:02:37",
"yymm": "1210",
"arxiv_id": "1210.3751",
"language": "en",
"url": "https://arxiv.org/abs/1210.3751"
} |
\section{Introduction}\label{secone}
The Szlenk index is an ordinal-valued isomorphic invariant of a Banach space that was introduced in \cite{Szlenk1968}. There it is used to show that the class of separable, reflexive Banach spaces contains no universal element, thereby solving a problem posed by Banach and Mazur in ... | {
"timestamp": "2012-10-16T02:01:43",
"yymm": "1210",
"arxiv_id": "1210.3696",
"language": "en",
"url": "https://arxiv.org/abs/1210.3696"
} |
\section{Introduction}
Throughout, let $\mathbb{N}$, $\mathbb{N}_0= \mathbb{N}\cup\{0\}$, $\mathbb{Z}$, and $\mathbb{C}$ be the sets of positive integers, nonnegative integers, integers, and complex numbers respectively.
The set of even positive integers and the set of odd positive integers
will be written $2 \... | {
"timestamp": "2012-10-29T01:01:37",
"yymm": "1210",
"arxiv_id": "1210.3708",
"language": "en",
"url": "https://arxiv.org/abs/1210.3708"
} |
\section{Introduction}
Distributed storage systems (DSS) are designed to store data over a distributed network of nodes. DSS have become increasingly important given the growing volumes of data being generated, analyzed and archived today.
OceanStore \cite{Rhea:Pond03}, Google File System (GFS) \cite{Ghemawat:Google... | {
"timestamp": "2012-10-16T02:01:05",
"yymm": "1210",
"arxiv_id": "1210.3664",
"language": "en",
"url": "https://arxiv.org/abs/1210.3664"
} |
\section{INTRODUCTION}
The A15 phase Nb$_3$Sn compound \cite{Matthias53} is currently being used in a variety of large-scale scientific projects employing high-field superconducting magnets (above 10 T) \cite{miyazaki03}, including ITER (the International Thermonuclear Experimental Reactor) \cite{vostner06, mitchell1... | {
"timestamp": "2012-10-16T02:01:52",
"yymm": "1210",
"arxiv_id": "1210.3705",
"language": "en",
"url": "https://arxiv.org/abs/1210.3705"
} |
\section{Introduction}
\label{sec:introduction}
Within the context of the currently favored hierarchical model for
structure formation, massive clusters of galaxies are, as a
population, the most recently formed gravitationally bound structures
in the cosmos. Consequently, characteristics such as the shape and
evolu... | {
"timestamp": "2013-04-09T02:03:27",
"yymm": "1210",
"arxiv_id": "1210.3689",
"language": "en",
"url": "https://arxiv.org/abs/1210.3689"
} |
\section{Introduction}
The recent surge of interest in bandstructure of unusual crystals spurred from various developments in studying condensed matter systems. To name two examples, relevant to the present work, are the successful isolation of single layer graphene \cite{Neto} and the fabrication of 3D topological ins... | {
"timestamp": "2012-11-30T02:01:52",
"yymm": "1210",
"arxiv_id": "1210.3703",
"language": "en",
"url": "https://arxiv.org/abs/1210.3703"
} |
\section{Introduction}
\indent Semiconductor nanowires grown by the vapour-liquid-solid (VLS) method \cite{dayeh2009,plante2009,schroer2010, joyce2010, dick2010} are the subject of active study, with many potential applications ranging from nanoscale circuits \cite{xiang2006} and gas sensors \cite{du2009} to high-effic... | {
"timestamp": "2013-05-27T02:00:23",
"yymm": "1210",
"arxiv_id": "1210.3665",
"language": "en",
"url": "https://arxiv.org/abs/1210.3665"
} |
\section{Introduction}
\label{sec:Introduction}
\def\D{\mathrm{d}}
\def\E{\mathrm{e}}
\def\I{\mathrm{i}}
While the LHC methodically examines the energy scale of the electroweak theory and above,
it is time to recall the two criteria for evaluating a physical theory,
mentioned by A. Einstein~\cite{Einstein... | {
"timestamp": "2012-10-16T02:01:43",
"yymm": "1210",
"arxiv_id": "1210.3697",
"language": "en",
"url": "https://arxiv.org/abs/1210.3697"
} |
\section{Introduction} \label{Section:Intro}
The classical approach to analyzing the cellular downlink is to model the network as a lattice or regular grid of base stations \cite{lee:1986}. By using the geometry of the grid, which typically assumes a honeycomb-like arrangement of hexagons, along with models for the un... | {
"timestamp": "2012-10-16T02:01:06",
"yymm": "1210",
"arxiv_id": "1210.3667",
"language": "en",
"url": "https://arxiv.org/abs/1210.3667"
} |
\section{Introduction}
The Whipple 10\,m $\gamma$-ray telescope is located at the Fred Lawrence Whipple Observatory in southern Arizona.
Until June 2011, it operated in the range $0.3 - 10$ TeV and pioneered the Imaging Atmospheric \v{C}erenkov
Telescope (IACT) technique for the detection of VHE $\gamma$-rays. The te... | {
"timestamp": "2012-10-16T02:02:04",
"yymm": "1210",
"arxiv_id": "1210.3723",
"language": "en",
"url": "https://arxiv.org/abs/1210.3723"
} |
\section*{Description}
A liquid drop of radius $R$ is suspended in another liquid. This drop is placed between two parallel plates separated by a distance $H$ and subjected to a simple shear flow. Both plates move with a speed $u_w$ in opposite directions, producing a shear rate of $\dot{\gamma}=\frac{2u_w}{H}$. The l... | {
"timestamp": "2012-10-16T02:01:15",
"yymm": "1210",
"arxiv_id": "1210.3674",
"language": "en",
"url": "https://arxiv.org/abs/1210.3674"
} |
\section{Conclusion}
We have introduced a model that describes the effect of a line
on which there is fast diffusion on the overall propagation of a species that diffuses with another constant and reproduces outside this line in a two dimensional framework.
We have found that this model conserves the population in ab... | {
"timestamp": "2012-10-17T02:09:50",
"yymm": "1210",
"arxiv_id": "1210.3721",
"language": "en",
"url": "https://arxiv.org/abs/1210.3721"
} |
\subsubsection*{\cref{#1}}}
\newcommand{\fullsoln}[2]{\medbreak\subsubsection*{\fullcref{#1}{#2}}}
\crefformat{chapter}{Lecture~#2#1#3}
\crefmultiformat{chapter}{Lectures~#2#1#3}{ and~#2#1#3}{, #2#1#3}{}
\crefname{exer}{exercise}{exercises}
\Crefname{exer}{Exercise}{Exercises}
\crefformat{exer}{Exercise~#2#1#3}
\cr... | {
"timestamp": "2012-10-16T02:01:14",
"yymm": "1210",
"arxiv_id": "1210.3671",
"language": "en",
"url": "https://arxiv.org/abs/1210.3671"
} |
\section{Introduction}
The purpose of these notes is to derive a bound on the volume of a tubular neighborhood of a real algebraic variety in terms of the degrees of the defining polynomials.
The problem is stated in probabilistic terms, namely, as the probability that a random point, uniformly distributed in a ball... | {
"timestamp": "2013-10-01T02:04:25",
"yymm": "1210",
"arxiv_id": "1210.3742",
"language": "en",
"url": "https://arxiv.org/abs/1210.3742"
} |
\section*{References}
| {
"timestamp": "2012-10-16T02:01:27",
"yymm": "1210",
"arxiv_id": "1210.3687",
"language": "es",
"url": "https://arxiv.org/abs/1210.3687"
} |
\section{Software Diversity based Adaptation (SDA)}
$\mathbf{Definitions}$:
Define the original network and the network after edges being cut as $G_0$ and $G_1$ respectively.
Define the network $G=(G,V,E)$ after edges $$\{(i,s)|s \in S\wedge (i,s)\notin E\}$$ being added as $G^{(i,S)}$, where $S \subseteq V$.
Define... | {
"timestamp": "2020-07-17T02:21:49",
"yymm": "2007",
"arxiv_id": "2007.08469",
"language": "en",
"url": "https://arxiv.org/abs/2007.08469"
} |
\section{Introduction}
\label{sec:1}
At the intraseasonal to interannual time scales, the variability of the large-scale atmospheric circulation in the mid-latitudes of both hemispheres is dominated by the ``annular modes'', which are usually defined based on empirical orthogonal function (EOF) analysis of zonal-mean ... | {
"timestamp": "2020-07-20T02:02:31",
"yymm": "2007",
"arxiv_id": "2007.08589",
"language": "en",
"url": "https://arxiv.org/abs/2007.08589"
} |
\section{Introduction}\label{sec:introduction}
As cosmological datasets increase in quantity and quality, so does our capacity to use them to pin down the properties of our universe~\cite{Scott:2018adl}. The error bars on the measurements of cosmological parameters have narrowed over recent years and discrepancies betw... | {
"timestamp": "2021-04-20T02:34:25",
"yymm": "2007",
"arxiv_id": "2007.08496",
"language": "en",
"url": "https://arxiv.org/abs/2007.08496"
} |
\section{Introduction}\label{sec:introduction}}
\begin{figure*}[hbt!]
\begin{centering}
\includegraphics[width=2\columnwidth]{fig/framework-01.pdf}
\par\end{centering}
\caption{\label{fig:framework}
The inference process of our proposed framework.
We extract features of each labeled and unlabeled instance,
train a li... | {
"timestamp": "2021-05-12T02:10:03",
"yymm": "2007",
"arxiv_id": "2007.08461",
"language": "en",
"url": "https://arxiv.org/abs/2007.08461"
} |
\section{Introduction}
Dualities play an important role in our understanding of string theory. One of the best-understood dualities is T-duality, which relates string theory on backgrounds with $U(1)^{d}$ isometries, with the backgrounds related by $\mathrm{O}(d,d)$ transformations. These T-dualities are already visib... | {
"timestamp": "2020-07-17T02:22:40",
"yymm": "2007",
"arxiv_id": "2007.08510",
"language": "en",
"url": "https://arxiv.org/abs/2007.08510"
} |
\section{Introduction}
The classical spin-1/2 Ising model with nearest neighbor interactions for a lattice with $N$ sites was
suggested by Lenz in 1920's is defined by the following Hamiltonian \cite{RefJ1}
\begin{eqnarray}\label{E:HalfHamil}
{\mathcal{H}_{\rm{spin}1/2}}
=-J\sum_{<ij>} s_{i}s_{j}-H\sum_{i=1}^{N}s_{... | {
"timestamp": "2020-07-20T02:02:33",
"yymm": "2007",
"arxiv_id": "2007.08593",
"language": "en",
"url": "https://arxiv.org/abs/2007.08593"
} |
\section{Introduction}\label{S1}
\setcounter{equation}{0}
\noindent
We continue the study of the sharp constants in multivariate inequalities
of approximation theory
that began in \cite{G2018, G2019, G2019b, G2020}. In this paper we prove
an asymptotic equality
between the sharp constants in the
multivariate
... | {
"timestamp": "2021-03-18T01:05:02",
"yymm": "2007",
"arxiv_id": "2007.08439",
"language": "en",
"url": "https://arxiv.org/abs/2007.08439"
} |
\section{Author's Response}
\label{sec:rebuttal}
We thank all the reviewers for their insightful and constructive comments.
\subsection{Reviewer 1}
\begin{itemize}
\item \textit{``My only suggestion is to reconsider looking at the lens distortion experiment. Typically distortion is much more visible at the edg... | {
"timestamp": "2020-07-20T02:01:58",
"yymm": "2007",
"arxiv_id": "2007.08574",
"language": "en",
"url": "https://arxiv.org/abs/2007.08574"
} |
\section{Convolutional Neural Network-based Principal Component Analysis (CNN-PCA)}
\label{sec-methodology}
In this section, we first give a brief overview of PCA and the 2D CNN-PCA method. The 3D procedure is then introduced and described in detail.
\subsection{PCA Representation}
\label{sec-pca}
We let the vector ... | {
"timestamp": "2020-07-17T02:22:01",
"yymm": "2007",
"arxiv_id": "2007.08478",
"language": "en",
"url": "https://arxiv.org/abs/2007.08478"
} |
\section{Introduction} \label{intro}
\textit{Functional data analysis} \citep{ramsay2013functional,horvath2012inference,ferraty2006nonparametric} considers statistical problems where the data and parameter spaces are comprised of \emph{functions} and \emph{operators}. The probabilistic models for such data/parameters... | {
"timestamp": "2020-07-17T02:21:28",
"yymm": "2007",
"arxiv_id": "2007.08458",
"language": "en",
"url": "https://arxiv.org/abs/2007.08458"
} |
\section{\uppercase{#1}}}
\newcommand{\cmbav}[1]{\left\langle #1 \right\rangle}
\newcommand{\pdmcomment}[1]{{\color{blue}{[pdm: #1]}}}
\newcommand{\pdm}[1]{{\color{blue}{#1}}}
\newcommand{\bscomment}[1]{{\color{red}{#1}}}
\newcommand{\blake}[1]{{\color{red}{[bds: #1]}}}
\newcommand{\tbcomment}[1]{{\color{purple}{[tb:... | {
"timestamp": "2020-07-17T02:21:50",
"yymm": "2007",
"arxiv_id": "2007.08472",
"language": "en",
"url": "https://arxiv.org/abs/2007.08472"
} |
\section{INTRODUCTION}
Stability and convergence analysis of adaptive controller schemes has traditionally been based on Lyapunov stability notions and techniques \cite{sun,fidan,narendrabook,goodwinbook,krsticbookadaptive} . Lyapunov-like functions are selected in the design of adaptive control to penalize the magnitu... | {
"timestamp": "2020-07-20T02:02:04",
"yymm": "2007",
"arxiv_id": "2007.08578",
"language": "en",
"url": "https://arxiv.org/abs/2007.08578"
} |
\section{Deep Learning -- Challenges presented by Hyperspectral Imagery}
\label{advanDL-why}
Since AlexNet~\cite{krizhevsky2012imagenet} won the ImageNet challenge in 2012, deep learning approaches have gradually replaced traditional methods becoming a predominant tool in a variety of computer vision applications. Rese... | {
"timestamp": "2020-07-20T02:02:32",
"yymm": "2007",
"arxiv_id": "2007.08592",
"language": "en",
"url": "https://arxiv.org/abs/2007.08592"
} |
\section{Introduction}
Accurate 6D object pose estimation plays an important role in a variety of tasks, such as augmented reality, robotic manipulation, scene understanding, etc.
In recent years, substantial progress has been made for instance-level 6D object pose estimation, where the exact 3D object models for pose... | {
"timestamp": "2020-07-17T02:21:24",
"yymm": "2007",
"arxiv_id": "2007.08454",
"language": "en",
"url": "https://arxiv.org/abs/2007.08454"
} |
\section{Introduction} \label{sec:intro}
High-sensitivity, unbiased surveys of the gamma-ray sky are important to finding new astrophysical objects -- both to understand their bulk properties, and to constrain new physics beyond the standard model. Discovering the sources of cosmic rays and determining the underly... | {
"timestamp": "2021-01-27T02:23:30",
"yymm": "2007",
"arxiv_id": "2007.08582",
"language": "en",
"url": "https://arxiv.org/abs/2007.08582"
} |
\section{Introduction}
\label{m_exampls}
There are many applications where it is necessary to predict the
number of future events from a population of units associated with
an on-going time-to-event process. Such applications also require
a prediction interval to quantify statistical prediction uncertainty
arising from... | {
"timestamp": "2020-08-10T02:09:04",
"yymm": "2007",
"arxiv_id": "2007.08648",
"language": "en",
"url": "https://arxiv.org/abs/2007.08648"
} |
\section{Introduction}
\textcolor{black}{Discrete-valued time series arise in a wide variety of fields ranging from finance to molecular biology and public health.
For instance, we can mention the number of transactions in stocks in the finance field, see \cite{brannas:quoreshi:2010}.
In the field of molecular biology... | {
"timestamp": "2020-07-20T02:03:28",
"yymm": "2007",
"arxiv_id": "2007.08623",
"language": "en",
"url": "https://arxiv.org/abs/2007.08623"
} |
\section{Linear stability analysis: $\M_1$ and $\M_2$}\label{Stability}
In this section, we present a linear stability analysis for the two paradigmatic models used in the main text namely the Stuart-Landau system $(\M_1)$ and the Lorenz system $(\M_2)$.
\subsection {Eigenvalue analysis of $\M_1$}
\label{Eigen_M_1}
\no... | {
"timestamp": "2020-07-20T02:03:57",
"yymm": "2007",
"arxiv_id": "2007.08642",
"language": "en",
"url": "https://arxiv.org/abs/2007.08642"
} |
\section{Introduction}
Debuting with the first detection of a stellar-mass black hole binary (SBHB) in 2015 \cite{Abbott:2016blz}, the LIGO/Virgo collaboration has issued the first catalog of the gravitational wave (GW) sources identified during the first and second observing runs (O1 and O2) \cite{LIGOScientific:201... | {
"timestamp": "2021-01-07T02:01:16",
"yymm": "2007",
"arxiv_id": "2007.08544",
"language": "en",
"url": "https://arxiv.org/abs/2007.08544"
} |
\section{Additional Results}
\label{appendix:results}
\noindent{\bf Short-term temporal video consistency.}
For each sequence, we first take two neighboring frames from the ground truth images to compute the optical flow between them using FlowNet2~\cite{ilg2017flownet}. We then use the optical flow to warp the corres... | {
"timestamp": "2020-07-17T02:22:39",
"yymm": "2007",
"arxiv_id": "2007.08509",
"language": "en",
"url": "https://arxiv.org/abs/2007.08509"
} |
\section{Conclusions}
We proposed a novel loss function which improves semantic coherence for cross-modal retrieval.
Our approach leverages a latent space learned on text alone, in order to enforce proximity within samples of the same modality, in the learned cross-modal space. We constrain text and image embeddings... | {
"timestamp": "2020-07-20T02:03:19",
"yymm": "2007",
"arxiv_id": "2007.08617",
"language": "en",
"url": "https://arxiv.org/abs/2007.08617"
} |
\section{Introduction}
\label{sec:Intro}
What do boiling water and ferromagnetics have in common? At first sight: not much. However, near the critical point in their phase diagrams, water and ferromagnets exhibit a similar behavior: various physical quantities scale in the same way, with exactly the same critical expo... | {
"timestamp": "2020-08-07T02:18:29",
"yymm": "2007",
"arxiv_id": "2007.08436",
"language": "en",
"url": "https://arxiv.org/abs/2007.08436"
} |
\section{Introduction}
A \emph{distance oracle} is a data structure that answers distance
queries (or approximate distance queries)
w.r.t.~some underlying graph or metric space.
On general graphs there
are many well known distance oracles that pit
space against multiplicative approximation~\cite{ThorupZ05},
space aga... | {
"timestamp": "2020-07-20T02:02:25",
"yymm": "2007",
"arxiv_id": "2007.08585",
"language": "en",
"url": "https://arxiv.org/abs/2007.08585"
} |
\section{Proof of Theorem~\ref{thm:main_result_rmax_pg}}
We need to understand the error $\ensuremath{\mathbb{E}}_{(s,a)\sim d} [\ensuremath{\mathds{1}}(s \in \Kcal)(A^\pi(s,a) - \theta^\star\cdot \bar \phi(s,a))]$, where $\pi$ is some policy and $d$ is some distribution. $\bar \phi$ refers to the centered features $... | {
"timestamp": "2020-08-14T02:19:06",
"yymm": "2007",
"arxiv_id": "2007.08459",
"language": "en",
"url": "https://arxiv.org/abs/2007.08459"
} |
\section{Introduction: IVOA provenance data model and provenance of CDS HiPS}
Datasets used in astronomy are generally the results of a flow of observation and processing steps. Information on this process is generally called "provenance" of the dataset and is stored in various formats and logical organizations. This m... | {
"timestamp": "2020-07-20T02:03:17",
"yymm": "2007",
"arxiv_id": "2007.08615",
"language": "en",
"url": "https://arxiv.org/abs/2007.08615"
} |
\section{Background}
\label{sec:background}
In this work, we demonstrate how the proposed explanation scheme can help obtain actionable insights in a material science application. Specifically, we are interested in understanding the behavior of a deep learning model that was trained on SEM images of feedstock materials... | {
"timestamp": "2020-07-20T02:03:41",
"yymm": "2007",
"arxiv_id": "2007.08631",
"language": "en",
"url": "https://arxiv.org/abs/2007.08631"
} |
\section{Introduction\label{sec:intro}}
Machine learning techniques are impacting science at an impressive
pace from robotics~\cite{argall2009survey} to genetics~\cite{libbrecht2015machine}, medicine~\cite{he2019practical}, and
physics~\cite{carleo2019machine}. In physics, reservoir
computing \cite{verstraeten2007exper... | {
"timestamp": "2020-10-21T02:28:13",
"yymm": "2007",
"arxiv_id": "2007.08634",
"language": "en",
"url": "https://arxiv.org/abs/2007.08634"
} |
\section{Introduction}
In length metrology by optical interferometry, the wavefront errors affect the period of the interference signal. The calibration of lasers against frequency standards achieves relative uncertainties smaller than $10^{-10}$, but it is not possible to trace back the wavelength to the frequency via... | {
"timestamp": "2020-07-20T02:00:12",
"yymm": "2007",
"arxiv_id": "2007.08524",
"language": "en",
"url": "https://arxiv.org/abs/2007.08524"
} |
\section{Outline of our Contributions}
In this section, we give a concise overview of the techniques involved in our algorithms.
The details of the proofs are deferred to the following sections.
\subsection{Intervals}
\label{sec:intervals_main}
We now give an overview of our dynamic algorithms for intervals achievi... | {
"timestamp": "2020-07-20T02:03:58",
"yymm": "2007",
"arxiv_id": "2007.08643",
"language": "en",
"url": "https://arxiv.org/abs/2007.08643"
} |
\section{Introduction}
Within the last decade, adversarial learning has become a core research area for studying robustness and machine learning. Adversarial attacks have expanded well beyond the original setting of imperceptible noise to more general notions of robustness, and can broadly be described as capturing se... | {
"timestamp": "2020-10-09T02:16:12",
"yymm": "2007",
"arxiv_id": "2007.08450",
"language": "en",
"url": "https://arxiv.org/abs/2007.08450"
} |
\section{Introduction}
Our work is motivated by the quest for high-level autonomy in service robots that can adapt to our everyday life. The key challenge comes from the fact that we cannot pre-program the robot since the working environment of a service robot is unpredictable \cite{paulius2019survey}, and the tasks f... | {
"timestamp": "2020-07-17T02:21:23",
"yymm": "2007",
"arxiv_id": "2007.08451",
"language": "en",
"url": "https://arxiv.org/abs/2007.08451"
} |
\section*{\large Appendices}
\section{Proofs} \label{sec:app:proofs}
Here we restate the Theorems and Propositions, as well as other mathematical claims appearing in the main text, and give their proof.
\subsection*{Theorem~\ref{prop:GAverageUnitaries}}
\GAverageUnitaries*
\begin{proof}
Let $S$ be the operator ov... | {
"timestamp": "2021-01-21T02:24:21",
"yymm": "2007",
"arxiv_id": "2007.08570",
"language": "en",
"url": "https://arxiv.org/abs/2007.08570"
} |
\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... | {
"timestamp": "2021-06-29T02:37:05",
"yymm": "2007",
"arxiv_id": "2007.08483",
"language": "en",
"url": "https://arxiv.org/abs/2007.08483"
} |
\section{Introduction}
With growing interests in autonomous vehicles, 3D object detection has received considerable attention. Due to the superior capability of modeling 3D objects, point cloud is the most popular type of data source. Most existing 3D detectors are point-based~\cite{qi2018frustum,wang2019frustum,Lan_20... | {
"timestamp": "2020-07-20T02:01:06",
"yymm": "2007",
"arxiv_id": "2007.08556",
"language": "en",
"url": "https://arxiv.org/abs/2007.08556"
} |
\section{Introduction}\label{sec:intro}
A general goal in geometric measure theory that has not yet been fully achieved is to understand in a systematic way how generic measures on a metric space interact with a prescribed family of sets in the space, e.g.~rectifiable curves, smooth submanifolds, etc. For instance, we... | {
"timestamp": "2020-12-17T02:24:06",
"yymm": "2007",
"arxiv_id": "2007.08503",
"language": "en",
"url": "https://arxiv.org/abs/2007.08503"
} |
\subsubsection*{\bibname}}
\usepackage{breqn}
\usepackage{stmaryrd}
\usepackage{mathtools}
\begin{document}
\twocolumn[
\aistatstitle{Active Learning under Label Shift}
\aistatsauthor{ Eric Zhao \And Anqi Liu \And Anima Anandkumar \And Yisong Yue }
\aistatsaddress{ California Institute of Technology } ]
\begin... | {
"timestamp": "2021-03-01T02:01:59",
"yymm": "2007",
"arxiv_id": "2007.08479",
"language": "en",
"url": "https://arxiv.org/abs/2007.08479"
} |
\section{Introduction}
\subsection{Motivation}
Given two nonempty subsets $A, B$ of a group $G$, the set $A$ is said to be a left (resp. right) complement to $B$ if $A \cdot B = G$ (resp. $B\cdot A = G$). If $A$ is a left (resp. right) complement to $B$ and no subset of $A$ other than $A$ is a left (resp. right) compl... | {
"timestamp": "2020-07-17T02:22:37",
"yymm": "2007",
"arxiv_id": "2007.08507",
"language": "en",
"url": "https://arxiv.org/abs/2007.08507"
} |
\section{Introduction} \label{sec:intro}
Stellar mass (M$_{*}$) is one of the fundamental physical properties of a galaxy
since it traces star formation and evolution process of the galaxy,
and is crucial to decompose the contributions from stars
and dark matter to the dynamics of a galaxy.
The stellar population synth... | {
"timestamp": "2020-07-20T02:02:57",
"yymm": "2007",
"arxiv_id": "2007.08610",
"language": "en",
"url": "https://arxiv.org/abs/2007.08610"
} |
\section{Introduction}
In gauge theories with fundamental representation matter fields, one
can often dial parameters in a manner which smoothly interpolates
between a Higgs regime and a confining regime without undergoing any
change in the realization of global
symmetries~\cite{tHooft:1979yoe,Osterwalder:1977pc,Fradk... | {
"timestamp": "2020-12-01T02:50:22",
"yymm": "2007",
"arxiv_id": "2007.08539",
"language": "en",
"url": "https://arxiv.org/abs/2007.08539"
} |
\section*{Introduction}
For a fixed metric space $X$, consider the family $\mathcal{S}$ of every metric quotient $S$ obtained from $X$.
The first result in this paper is a tool for proving that a given $S \in \mathcal{S}$ is the limit of a given sequence $S_n \in \mathcal{S}$.
It is based on comparing the data $\math... | {
"timestamp": "2020-07-17T02:20:32",
"yymm": "2007",
"arxiv_id": "2007.08420",
"language": "en",
"url": "https://arxiv.org/abs/2007.08420"
} |
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