text stringlengths 1 1.69M | meta dict |
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\section{Introduction}
\label{sec:Intro}
If one follows the by--now--standard procedures of perturbative quantum field theory,
then one finds that quantum gravity suffers from the problem that it is not perturbatively renormalizable. The natural coupling constant is $\kappa=2/M$, where $M$ is the reduced Planck mass. ... | {
"timestamp": "2018-07-31T02:20:11",
"yymm": "1802",
"arxiv_id": "1802.04281",
"language": "en",
"url": "https://arxiv.org/abs/1802.04281"
} |
\section{Introduction}
When performing a complex action, humans do not think or act in the level of granular primitive actions at the individual muscle or joint level. Instead, humans decompose complicated actions in a set of simpler actions. By combining simpler actions or motor primitives, humans can learn more comp... | {
"timestamp": "2018-02-13T02:20:25",
"yymm": "1802",
"arxiv_id": "1802.04132",
"language": "en",
"url": "https://arxiv.org/abs/1802.04132"
} |
\section{Introduction}
\label{sec:intro}
Most spoken language translation (SLT) systems integrate (loosely or closely) two main modules: source language speech recognition (ASR) and source-to-target
text translation (MT). In these approaches, a symbolic sequence of words (or characters) in the source language is use... | {
"timestamp": "2018-02-13T02:22:10",
"yymm": "1802",
"arxiv_id": "1802.04200",
"language": "en",
"url": "https://arxiv.org/abs/1802.04200"
} |
\section{Experimental setup}
\begin{figure}
\centering%
\includegraphics[width=\linewidth]{fig1}
\caption{(Color online) Schematic of the experimental setup and the definition of the coordinate
system. a) Sketch of the cross sections of the molecular beam and the laser beam
to illustrate the workin... | {
"timestamp": "2018-09-05T02:16:49",
"yymm": "1802",
"arxiv_id": "1802.04053",
"language": "en",
"url": "https://arxiv.org/abs/1802.04053"
} |
\section*{Acknowledgments}
The author is grateful to G. Duplan\v{c}i\'c, B. Klajn and B. Meli\'c for discussions.
This work was supported by the Ministry of Science of the Republic of Croatia
and by H2020 Twinning project No. 692194, ``RBI-T-WINNING''.
| {
"timestamp": "2018-02-13T02:17:49",
"yymm": "1802",
"arxiv_id": "1802.04025",
"language": "en",
"url": "https://arxiv.org/abs/1802.04025"
} |
\section{Introduction}
Differential privacy \cite{dwork2006calibrating} has emerged as a rigorous notion for privacy which allows accurate data analysis with a guaranteed bound on the increase in harm for each individual to contribute her data.
Methods to guarantee differential privacy have been widely studied, and r... | {
"timestamp": "2018-05-18T02:02:13",
"yymm": "1802",
"arxiv_id": "1802.04085",
"language": "en",
"url": "https://arxiv.org/abs/1802.04085"
} |
\section{Introduction}
In geotechnics, the large deformations of rock and soil masses commonly
occur in various geo-disasters such as landslides, debris flows, rock
collapses, and ground subsidence. Moreover, when analyzing the stability of
rock or soil slopes, the distribution and propagation of natural cracks is ... | {
"timestamp": "2018-02-14T02:00:13",
"yymm": "1802",
"arxiv_id": "1802.04256",
"language": "en",
"url": "https://arxiv.org/abs/1802.04256"
} |
\section{Introduction}
In this work we investigate the regularity of $p$-orthotropic functions in the plane for $1<p<2$.
Let $\Omega\subset\mathbb{R}^2$ be an open set. A weak solution of the orthotropic $p$-Laplace equation (also known as pseudo $p$-Laplace equation) is a function $u\in W^{1,p}(\Omega)$ such tha... | {
"timestamp": "2018-02-13T02:22:04",
"yymm": "1802",
"arxiv_id": "1802.04197",
"language": "en",
"url": "https://arxiv.org/abs/1802.04197"
} |
\part*{Auxiliary Material}
\end{document}
| {
"timestamp": "2018-06-22T02:08:39",
"yymm": "1802",
"arxiv_id": "1802.04329",
"language": "en",
"url": "https://arxiv.org/abs/1802.04329"
} |
\section{Introduction}
Due to their rapid deployment, flexibility, as well as collaborative sensing, self-organization, and intelligent-processing abilities, wireless sensor networks (WSNs) have found their way into a wide variety of industrial settings with varying requirements and characteristics: healthcare monito... | {
"timestamp": "2018-02-14T02:01:34",
"yymm": "1802",
"arxiv_id": "1802.04338",
"language": "en",
"url": "https://arxiv.org/abs/1802.04338"
} |
\section{Introduction}
\label{sec:1}
Consider the dynamical evolution, with non conserved order parameter, of a system undergoing a first order phase transition. A basic paradigm of statistical mechanics is that the corresponding macroscopic behavior is described by the motion by curvature of the interfaces separating... | {
"timestamp": "2018-02-13T02:22:02",
"yymm": "1802",
"arxiv_id": "1802.04194",
"language": "en",
"url": "https://arxiv.org/abs/1802.04194"
} |
\section{Introduction}
\label{sec-intro}
\setcounter{equation}{0}
\subsection{Statement of the problem}
Let $\Omega$ be an unbounded open set of ${\mathbb R}^3$ corresponding to a closed waveguide. Here by closed waveguide we mean that
there exists $\omega$ a $\mathcal C^2$ bounded open simply connected set of $... | {
"timestamp": "2019-01-29T02:22:53",
"yymm": "1802",
"arxiv_id": "1802.04185",
"language": "en",
"url": "https://arxiv.org/abs/1802.04185"
} |
\section{Introduction}
The irrationality of the value of the Riemann $\zeta$-function at odd integers is a long standing open problem. For even integer arguments, it was famously shown by Euler \cite{euler} that
\begin{equation*}
\zeta(2n) = (-1)^{n-1} \frac{2^{2n-1} \pi^{2n} B_{2n}}{(2n)!},
\end{equation*}
where $B_... | {
"timestamp": "2018-02-13T02:16:01",
"yymm": "1802",
"arxiv_id": "1802.03946",
"language": "en",
"url": "https://arxiv.org/abs/1802.03946"
} |
\subsection*{S1. Derivation of the spin-$\frac{1}{2}$ effective model from a single-band Hubbard model under a DC field}
This section is devoted to the derivation of the spin-$\frac{1}{2}$ effective model~(2).
We start from a half-filled, repulsive Hubbard model ($U>0$) with an arbitrary on-site potential term.
The ... | {
"timestamp": "2018-02-14T02:00:53",
"yymm": "1802",
"arxiv_id": "1802.04311",
"language": "en",
"url": "https://arxiv.org/abs/1802.04311"
} |
\section{Introduction}
Assume that we have a Boolean function $f:\{0, 1\}^n\to\{0, 1\}$ called \emph{outer function} and a Boolean function $g:A\times B\to\{0, 1\}$ called \emph{gadget}. Consider a composed function $f\circ g : A^n \times B^n\to \{0, 1\}$, defined as follows:
$$ (f\circ g)((a_1, \ldots, a_n), (b_1... | {
"timestamp": "2018-07-09T02:08:23",
"yymm": "1802",
"arxiv_id": "1802.04014",
"language": "en",
"url": "https://arxiv.org/abs/1802.04014"
} |
\section{Introduction}
It is a known fact that one of the conceptual problems of quantum theory is the so-called ''measurement problem'' - the standard Quantum Mechanics (QM) crucially depends on the concept of measurement, even though such notion is not defined rigurously within the theory \cite{OS, NG, GF}. Accordi... | {
"timestamp": "2018-02-13T02:20:17",
"yymm": "1802",
"arxiv_id": "1802.04125",
"language": "en",
"url": "https://arxiv.org/abs/1802.04125"
} |
\section{Introduction}
Consider the following one-dimensional stochastic differential equation with jumps:
\begin{equation}
dX_t=\left( \sum_{l=1}^{p_\alpha} \alpha^{(l)} a^{(l)}(X_t) \right)^{1/2}dw_t+\sum_{k=1}^{p_\beta} \beta^{(k)} b^{(k)}(X_t)dt+c(X_{t-})dJ_t,
\label{hm:sde}
\end{equation}
defined on a complete fi... | {
"timestamp": "2019-10-02T02:12:05",
"yymm": "1802",
"arxiv_id": "1802.03945",
"language": "en",
"url": "https://arxiv.org/abs/1802.03945"
} |
\section{Introduction}\label{sec:1}
Convolutional Neural Network (CNN) has become one of the most successful computational models
in machine learning and artificial intelligence.
Remarkable progress has been achieved in the design of successful CNN {\it network structures},
such as the VGG-Net \cite{simonyan2014ve... | {
"timestamp": "2018-07-31T02:04:08",
"yymm": "1802",
"arxiv_id": "1802.04145",
"language": "en",
"url": "https://arxiv.org/abs/1802.04145"
} |
\section{Introduction}
\begin{definition}
Given $f$ a complex valued function defined on the unit disc in $\mathbb{R}^2$, we define
$$Ef(x_1, x_2, x_3):= \int e^{i(\xi_1 x_1+\xi_2 x_2 +|\xi|^2 x_3)} f(\xi) d \xi .$$
\end{definition}
Stein conjectured \cite{Stein} in the 1960s the following restriction estim... | {
"timestamp": "2018-02-14T02:00:55",
"yymm": "1802",
"arxiv_id": "1802.04312",
"language": "en",
"url": "https://arxiv.org/abs/1802.04312"
} |
\subsubsection*{Example}}
\newcommand{\subsubsection*{Examples}}{\subsubsection*{Examples}}
\newcommand{\subsubsection*{Definition}}{\subsubsection*{Definition}}
\newcommand{\subsubsection*{Definitions}}{\subsubsection*{Definitions}}
\newcommand{\subsubsection*{Notation}}{\subsubsection*{Notation}}
\newcommand{\mathrm... | {
"timestamp": "2018-02-13T02:17:08",
"yymm": "1802",
"arxiv_id": "1802.03999",
"language": "en",
"url": "https://arxiv.org/abs/1802.03999"
} |
\section{Introduction}
This paper can be considered as a natural continuation of the investigations started in \cite{lamis} and \cite{lamisii} where we started to build the theory of means on infinite sets. An ordinary mean is for calculating the mean of two (or finitely many) numbers. This can be extended in many ways... | {
"timestamp": "2018-02-27T02:11:59",
"yymm": "1802",
"arxiv_id": "1802.04110",
"language": "en",
"url": "https://arxiv.org/abs/1802.04110"
} |
\section{Introduction}
The conventional description of black hole evaporation is based on quantum field theory on curved spacetime, with the back-reaction on the geometry taken into account via a mean-field approximation \cite{Hawking1974}. The approximation breaks down before evaporation brings the black hole mass d... | {
"timestamp": "2018-03-20T01:06:40",
"yymm": "1802",
"arxiv_id": "1802.04264",
"language": "en",
"url": "https://arxiv.org/abs/1802.04264"
} |
\section{Introduction}
One of the main tasks condensed matter physics deals with is the understanding of phases of matter. Traditionally, phase transitions were characterised following Landau's prescription, in terms of an order parameter. Then, the discovery of new phases of matter that did not break any symmetry, no... | {
"timestamp": "2018-10-05T02:11:30",
"yymm": "1802",
"arxiv_id": "1802.03973",
"language": "en",
"url": "https://arxiv.org/abs/1802.03973"
} |
\chapter{Bitcoin Point of Sale Terminals: Evaluation and Deployment}
\section{Introductory Remarks}
Bitcoin is a cryptographic currency publicly proposed in 2008~\cite{Nak08}. It has reached a level of adoption unrealized by decades of previously proposed digital currencies (from 1982~\cite{Cha82} onward). Unlike ... | {
"timestamp": "2018-02-13T02:23:18",
"yymm": "1802",
"arxiv_id": "1802.04236",
"language": "en",
"url": "https://arxiv.org/abs/1802.04236"
} |
\subsection*{Effective Hamiltonian of the system} \label{subsec:formalism}
\noindent Consider the circuit with four connected superconducting islands and the corresponding effective lumped circuit element model in Figure \ref{fig:circuit}.
The top-bottom symmetry between the capacitors and the Josephson junctions can... | {
"timestamp": "2019-10-28T01:11:06",
"yymm": "1802",
"arxiv_id": "1802.04299",
"language": "en",
"url": "https://arxiv.org/abs/1802.04299"
} |
\section{INTRODUCTION}
\label{intro}
Quantum correlations (QCs), existing between two or more parties \cite{horodecki2009quantum, modi2012classical}, are bestowed with properties unique to the quantum world and are of pivotal importance in quantum information science. The study of QCs not only unveils the fundamenta... | {
"timestamp": "2018-02-14T02:00:17",
"yymm": "1802",
"arxiv_id": "1802.04265",
"language": "en",
"url": "https://arxiv.org/abs/1802.04265"
} |
\section{Introduction}
This paper continues the study of the multipliers between two sub-Hardy Hilbert spaces. By the term ``multiplier'' between two Hilbert spaces $\mathscr{H}_{1}, \mathscr{H}_2$ of analytic functions on the open unit disk $\mathbb{D} = \{|z| < 1\}$ we mean the set
$\{\varphi \in \mathscr{O}(\math... | {
"timestamp": "2018-02-13T02:17:50",
"yymm": "1802",
"arxiv_id": "1802.04026",
"language": "en",
"url": "https://arxiv.org/abs/1802.04026"
} |
\section{Introduction}
Integrability is a unique tool allowing one to obtain exact non-perturbative results in fully interacting field theories even when the supersymmetry is of no use.
The range of theories where integrability is known to be applicable includes supersymmetric theories such as planar ${\cal N}=4$ ... | {
"timestamp": "2018-03-07T02:12:22",
"yymm": "1802",
"arxiv_id": "1802.04237",
"language": "en",
"url": "https://arxiv.org/abs/1802.04237"
} |
\section{ Introduction}
The problem of a rotating object in the presence of the gravitational field is essentially practical than viewing objects as a mere test particles, in order to ignore their intrinsic property due to the Orthodox General Theory of Relativity. Accordingly, several attempts were done in the last ... | {
"timestamp": "2018-02-13T02:18:47",
"yymm": "1802",
"arxiv_id": "1802.04058",
"language": "en",
"url": "https://arxiv.org/abs/1802.04058"
} |
\section{Introduction}
Planetary and preplanetary nebulae (PNe, pPNe) often show a remarkable
axial symmetry and fast bipolar outflows with velocities around 100
\mbox{km\,s$^{-1}$}. On the contrary, asymptotic giant branch (AGB) circumstellar
envelopes, their immediate precursors, are spherical, at least at
large-sca... | {
"timestamp": "2018-02-13T02:17:44",
"yymm": "1802",
"arxiv_id": "1802.04019",
"language": "en",
"url": "https://arxiv.org/abs/1802.04019"
} |
\section{Introduction}
The radii of tidally-locked, main-sequence K- and M-dwarfs in
eclipsing binary systems are consistently measured to be larger than
predicted by most evolutionary models. The radius discrepancies amount to
10--20 per cent at a fixed mass and thus for a fixed luminosity,
the effective temperat... | {
"timestamp": "2018-02-14T02:00:36",
"yymm": "1802",
"arxiv_id": "1802.04288",
"language": "en",
"url": "https://arxiv.org/abs/1802.04288"
} |
\section{Introduction}
Traditionally, image retrieval systems relied on keyword annotation to search for images relevant to a user's query. Although these systems were effective but they suffered from several problems such as the need to annotate huge image databases, deal with inconsistencies among the annotations pro... | {
"timestamp": "2018-02-13T02:22:28",
"yymm": "1802",
"arxiv_id": "1802.04204",
"language": "en",
"url": "https://arxiv.org/abs/1802.04204"
} |
\section{Introduction}
Gravitational waves (GWs) carry energy, linear momentum, and angular
momentum, and are therefore responsible for the final evolutionary
stages of compact binary systems. As energy and angular momentum are
dissipated away, the two objects inspiral and eventually merge. The
GW-driven orbital decay... | {
"timestamp": "2018-05-29T02:19:33",
"yymm": "1802",
"arxiv_id": "1802.04276",
"language": "en",
"url": "https://arxiv.org/abs/1802.04276"
} |
\section{Introduction}
In this paper, we systematize and analyze some results obtained in {\it Subset Combinatorics of Groups } after publications the surveys [1], [2], [3], [4]. The main topics: the descriptive and dynamical characterizations of subsets of a group with respect to their combinatorial size, Ramsey-prod... | {
"timestamp": "2018-02-13T02:19:56",
"yymm": "1802",
"arxiv_id": "1802.04106",
"language": "en",
"url": "https://arxiv.org/abs/1802.04106"
} |
\section{Introduction}
\label{intro}
Electronic mail or e-mail is a method of electronic communication between two or more users using the Internet. Nowadays emails are not just used for communication but also used for managing the task, solving customer queries. Email Classification or Categorization has been inspire... | {
"timestamp": "2018-02-13T02:16:41",
"yymm": "1802",
"arxiv_id": "1802.03971",
"language": "en",
"url": "https://arxiv.org/abs/1802.03971"
} |
\section{Introduction}
Lyman-$\alpha$ (\ifmmode{\mathrm{Ly}\alpha}\else Ly$\alpha$\xspace\fi) is the torch that lights up the distant Universe.
\cite{Partridge1967} recognized \ifmmode{\mathrm{Ly}\alpha}\else Ly$\alpha$\xspace\fi to be the strongest tracer of recombining ionized hydrogen ({\text{H\MakeUppercase{\romann... | {
"timestamp": "2018-03-29T02:08:48",
"yymm": "1802",
"arxiv_id": "1802.04280",
"language": "en",
"url": "https://arxiv.org/abs/1802.04280"
} |
\section{Introduction}
A function that assigns sets to all vertices of a graph is a \emph{set coloring} if the sets
assigned to adjacent vertices are disjoint.
For positive integers $a$ and $b\le a$, an {\em $(a:b)$-coloring} of a graph $G$ is a set coloring
with range $\binom {\{1,\ldots, a\}}{b}$, i.e., a set colori... | {
"timestamp": "2019-07-16T02:13:51",
"yymm": "1802",
"arxiv_id": "1802.04179",
"language": "en",
"url": "https://arxiv.org/abs/1802.04179"
} |
\section{Measure derivatives of Lions, associated It\^o formula and examples}
\label{sec measure derivatives and ito}
For the construction of the measure derivative in the sense of Lions
we follow the approach from~\cite[Section 6]{cardaliaguet2012}.
There are three main differences: The first difference is that we d... | {
"timestamp": "2018-05-08T02:16:41",
"yymm": "1802",
"arxiv_id": "1802.03974",
"language": "en",
"url": "https://arxiv.org/abs/1802.03974"
} |
\section{Introduction}
Reducible gauge field theories require ghosts, ghosts-for-ghosts, and higher-ghosts as much as necessary, whose gauge algebras may necessitate equations of motion to be closed algebras.
The Batalin-Vilkovisky (BV) formalism gives a convenient way to describe such gauge theories, in which the ac... | {
"timestamp": "2018-07-17T02:08:06",
"yymm": "1802",
"arxiv_id": "1802.04171",
"language": "en",
"url": "https://arxiv.org/abs/1802.04171"
} |
\section{Introduction}
The cataclysmic variable AR~Scorpii (AR~Sco) shows large-amplitude, highly periodic pulsations across the electromagnetic spectrum every 1.97 minutes, superimposed upon a strong waveform at the system's 3.56-h orbital period \citep{marsh16}. The system's low X-ray luminosity rules out the pre... | {
"timestamp": "2018-09-11T02:01:29",
"yymm": "1802",
"arxiv_id": "1802.04323",
"language": "en",
"url": "https://arxiv.org/abs/1802.04323"
} |
\section{#1} \vspace{-0.01in} }
\newcommand{\Subsection}[1]{ \vspace{-0.15in} \subsection{#1} \vspace{-0.015in} }
\newcommand{\Subsubsection}[1]{ \vspace{-0.15in} \subsubsection{#1} \vspace{-0.015in} }
\begin{document}
\pagenumbering{gobble}
\title{The Coupled TuFF-BFF Algorithm for Automatic 3D Segmentation of Micr... | {
"timestamp": "2018-02-13T02:20:54",
"yymm": "1802",
"arxiv_id": "1802.04156",
"language": "en",
"url": "https://arxiv.org/abs/1802.04156"
} |
\section{Introduction}
\label{sec:intro}
The need for improved energy resolution and sensitivity to smaller energy depositions led to the proposal to use cryogenic techniques as an instrument for detecting low energy particles.\\
In 1984 three different groups suggested low temperature detectors as an instrument t... | {
"timestamp": "2018-02-14T02:00:15",
"yymm": "1802",
"arxiv_id": "1802.04260",
"language": "en",
"url": "https://arxiv.org/abs/1802.04260"
} |
\section{Introduction}
The problem of index coding was introduced by Birk and Kol in \cite{BiK}.
The index coding problem consists of a single sender with a set of \textit{M} independent messages
\begin{displaymath}
\mathcal{X}=\lbrace x_1,x_2,\dots,x_M\rbrace,
\end{displaymath} and a set of $ N $ users
\be... | {
"timestamp": "2018-02-13T02:21:40",
"yymm": "1802",
"arxiv_id": "1802.04183",
"language": "en",
"url": "https://arxiv.org/abs/1802.04183"
} |
\section{Introduction}
The theory of center manifolds provides a powerful method of analysis of local
bifurcations in infinite-dimensional systems associated with a PDE. They allow to reduce, under certain conditions, the
infinite-dimensional dynamics near a bifurcation point to a finite-dimensional dynamics, describ... | {
"timestamp": "2018-02-13T02:20:17",
"yymm": "1802",
"arxiv_id": "1802.04123",
"language": "en",
"url": "https://arxiv.org/abs/1802.04123"
} |
\section{The Learning Algorithm}
\label{algorithm}
Having discussed the modelling of the control sequences and the RL problem, we will now introduce the actual learning algorithm we employ.
As we have seen above, we can not perform direct optimization of $R(c)$ as we cannot access $\nabla R(c)$.
However, it has long be... | {
"timestamp": "2018-04-16T02:07:59",
"yymm": "1802",
"arxiv_id": "1802.04063",
"language": "en",
"url": "https://arxiv.org/abs/1802.04063"
} |
\section{\label{sec:introduction}Introduction}
Topological semimetals (TSMs) are materials with non-trivial crossing of valence and conduction bands at points, lines, or loops within the Brillouin zone. They are topologically protected in the sense that the crossing cannot be lifted by a symmetry-preserving perturbatio... | {
"timestamp": "2018-05-09T02:00:25",
"yymm": "1802",
"arxiv_id": "1802.04300",
"language": "en",
"url": "https://arxiv.org/abs/1802.04300"
} |
\section{Introduction}
Revealing the morphological and chemical structure of the Milky Way
requires knowing the locations of objects on a Galaxy-wide scale. In
the Solar neighborhood, the distances to stars can be accurately
derived by measuring their parallax. Far from the Solar neighborhood,
distances to stars may b... | {
"timestamp": "2018-02-13T02:22:25",
"yymm": "1802",
"arxiv_id": "1802.04203",
"language": "en",
"url": "https://arxiv.org/abs/1802.04203"
} |
\section{Introduction}
Formal Concept Analysis~\cite{DBLP:books/daglib/0095956} is a mathematical framework that allows, from a binary relation, to extract interesting patterns called concepts.
Those patterns form a hierarchy called a concept lattice.
\medskip
The size of the lattice, potentially exponential in the s... | {
"timestamp": "2018-02-13T02:18:00",
"yymm": "1802",
"arxiv_id": "1802.04030",
"language": "en",
"url": "https://arxiv.org/abs/1802.04030"
} |
\section{Introduction}
Recently, Tsai and Wang \cite{TsaiWang17} considered $n$-dimensional minimal submanifolds $\Sigma\subset M$ where $(M,g)$ is an $(n+m)$-dimensional ambient Riemannian manifold. They
consider the partial Ricci operator on the normal bundle $N\Sigma$:
$$\mathcal{R}(V) = \text{tr}_{\Sigma}(R(\cdot,... | {
"timestamp": "2018-04-20T02:05:45",
"yymm": "1802",
"arxiv_id": "1802.03941",
"language": "en",
"url": "https://arxiv.org/abs/1802.03941"
} |
\section{Introduction}
Let $F_{q}$ be the Galois field of $q$ elements and let $\mathrm{PG}(v,q)$ be the $v$
-dimensional projective space over $F_{q}$. For an introduction to
geometrical objects in such spaces, see~\cite{Hirs, HirsSt}.
For an integer $\varrho $ with $0\leq \varrho \leq n$ we say that a set of
point... | {
"timestamp": "2018-02-13T02:22:44",
"yymm": "1802",
"arxiv_id": "1802.04214",
"language": "en",
"url": "https://arxiv.org/abs/1802.04214"
} |
\section{Introduction}
\label{sec:Intro}
The $\mathrm{^{22}Ne(p,\gamma)^{23}Na}$ reaction, which belongs to the NeNa cycle, is active in high temperature hydrogen burning \cite{Iliadis15-Book}. One astrophysical site of particular interest for this reaction is the Hot Bottom Burning (HBB) process in asymptotic giant b... | {
"timestamp": "2018-02-13T02:21:05",
"yymm": "1802",
"arxiv_id": "1802.04164",
"language": "en",
"url": "https://arxiv.org/abs/1802.04164"
} |
\section*{Introduction}
We assume throughout this article that algebras are finite dimensional algebras over a field $K$. A projective left module $Af$ with an idempotent $f$ is said to be \emph{minimal faithful projective-injective} in case $Af$ is a faithful projective-injective left module and every faithful project... | {
"timestamp": "2018-02-13T02:21:27",
"yymm": "1802",
"arxiv_id": "1802.04175",
"language": "en",
"url": "https://arxiv.org/abs/1802.04175"
} |
\section{Introduction}
Compared to other buildings, supermarkets consume proportionately more energy~\cite{TIMMA2016435,Mylona}.
This is mainly due to refrigeration needed to slow down the deterioration of food, by retaining them on a predetermined temperature~\cite{Mylona}.
Electricity costs associated with refrigerat... | {
"timestamp": "2018-02-13T02:20:20",
"yymm": "1802",
"arxiv_id": "1802.04128",
"language": "en",
"url": "https://arxiv.org/abs/1802.04128"
} |
\section{Introduction}
\label{Loss}
Standard classification tasks focus on building a classifier which predicts well on future examples. The overall goal is to minimize the number of mis-classifications. However, when the cost of mis-classification is very high, a generic classifier may still suffer from very high risk... | {
"timestamp": "2019-03-25T01:08:43",
"yymm": "1802",
"arxiv_id": "1802.04235",
"language": "en",
"url": "https://arxiv.org/abs/1802.04235"
} |
\section{Introduction}
Although studies of the transport of life-bearing rocks between planets have a long history \citep[e.g.][]{melosh1988},
claims of the discovery of traces of ancient life in the meteorite ALH84001 in the mid-1990s \citep{mcketal1996} accelerated
investigations into panspermia within the Solar s... | {
"timestamp": "2018-11-13T02:15:02",
"yymm": "1802",
"arxiv_id": "1802.04279",
"language": "en",
"url": "https://arxiv.org/abs/1802.04279"
} |
\section{Introduction}
The discovery of the Higgs boson~\cite{higgs,discovery} at the CERN
Large Hadron Collider (LHC) is of monumental significance. The
completion of the Standard Model (SM) provides us with a consistent
theory valid up to high scales. As a perturbative gauge theory, it
allows for precision predictio... | {
"timestamp": "2018-10-25T02:04:34",
"yymm": "1802",
"arxiv_id": "1802.04319",
"language": "en",
"url": "https://arxiv.org/abs/1802.04319"
} |
\section{\label{intr}Introduction}
Precise cosmological observations gathered in recent years have provided us with an increasingly detailed picture of the Universe and its constituents (see, e.g., \cite{Suzuki:2011hu,Anderson:2012sa,Ade:2015xua}). At the present time, the Universe appears to be dominated by two main ... | {
"timestamp": "2018-03-28T02:17:12",
"yymm": "1802",
"arxiv_id": "1802.03961",
"language": "en",
"url": "https://arxiv.org/abs/1802.03961"
} |
\section{Introduction}
Dark matter haloes are the fundamental building blocks of cosmic large-scale structure, and galaxies form by condensing in their cores. Understanding the structure, evolution and formation of dark matter haloes is an essential step towards understanding how galaxies form and ultimately, to test c... | {
"timestamp": "2018-07-02T02:07:21",
"yymm": "1802",
"arxiv_id": "1802.04271",
"language": "en",
"url": "https://arxiv.org/abs/1802.04271"
} |
\section{Introduction}
This paper considers estimation of the unknown sparse vector, of its $\ell_2$-norm and of the noise level in the sparse sequence model. The focus is on construction of estimators that are optimally adaptive in a minimax sense with respect to the noise level, to the form of the noise distribution... | {
"timestamp": "2019-04-18T02:11:20",
"yymm": "1802",
"arxiv_id": "1802.04230",
"language": "en",
"url": "https://arxiv.org/abs/1802.04230"
} |
\section{Introduction}
\fi
\iffalse
\keywords{zero-automata, probabilities, temporal logics}
\maketitle
\fi
The theory of automata on infinite trees is
rooted in Rabin's seminal theorem which establishes an
effective correspondence between the monadic second order logic (MSO)
theory of the infinite binary ... | {
"timestamp": "2018-02-13T02:18:58",
"yymm": "1802",
"arxiv_id": "1802.04067",
"language": "en",
"url": "https://arxiv.org/abs/1802.04067"
} |
\section*{Abstract}
We approach the problem of combining top-ranking association statistics or P\nobreakdash-values{} from a new perspective which leads to a remarkably simple and powerful method.
Statistical methods, such as the Rank Truncated Product (RTP), have been developed for combining top-ranking associations a... | {
"timestamp": "2019-06-12T02:03:12",
"yymm": "1802",
"arxiv_id": "1802.04321",
"language": "en",
"url": "https://arxiv.org/abs/1802.04321"
} |
\section{Introduction}
The Loewner equation
\begin{equation}\label{slit0}
\frac{\partial g_t(z)}{\partial t} = \frac{1}{g_t(z) - U(t)}, \quad g_0(z)=z\in\Ha:=\{z\in\mathbb{C}\,|\, \Im(z)>0\},
\end{equation} where $U:[0,\infty)\to \mathbb{R}$ is continuous,
is usually interpreted as describing a family $(g_t)_{t\ge... | {
"timestamp": "2019-08-01T02:12:51",
"yymm": "1802",
"arxiv_id": "1802.04318",
"language": "en",
"url": "https://arxiv.org/abs/1802.04318"
} |
\section{Introduction}\label{intro}
In this paper we consider a generalized pseudo-relativistic Hartree equation
\begin{equation}\label{original}
\sqrt{-\Delta+m^2}\, u+Vu=\left(W*F(u)\right)f(u)\ \ \text{in }\ \mathbb{R}^{N},\end{equation}
where $N\geq 2$, $F(t)=\int_0^t f(s)\mathrm{d} s$, assuming that the nonlinear... | {
"timestamp": "2018-02-13T02:16:34",
"yymm": "1802",
"arxiv_id": "1802.03963",
"language": "en",
"url": "https://arxiv.org/abs/1802.03963"
} |
\subsection{The double sum in the energy correction}
In this part we provide an integral representation for the double
sum
\begin{equation}
\sum_{k_{1}\in\mathbb{Z}}\sum_{k_{2}\neq n_{q}}D_{1}\left(k_{1},k_{2}\right)
\end{equation}
with
\begin{align}
D_{1}(k_{1},k_{2}) =&\; \frac{1}{\omega_{k_{1}} \omega_{k_{2}} \ome... | {
"timestamp": "2018-07-11T02:06:53",
"yymm": "1802",
"arxiv_id": "1802.04021",
"language": "en",
"url": "https://arxiv.org/abs/1802.04021"
} |
\section{Conclusion and Future Work}
\section{Introduction}
The inclusion of human-centered approaches in software engineering has received a lot of attention in recent years \cite{da2011user,salah2014systematic,brhel2015exploring,schon2017agile}.
Human-centered design (HCD) \cite{dis20099241}, design thinking (DT... | {
"timestamp": "2018-02-13T02:19:48",
"yymm": "1802",
"arxiv_id": "1802.04100",
"language": "en",
"url": "https://arxiv.org/abs/1802.04100"
} |
\section*{Acknowledgements}
This project has received funding from the European Research Council (ERC) under the European Union’s Horizon 2020 research and innovation programme (grant agreement n$^o$ 725594 - time-data), and was supported by the Swiss National Science Foundation (SNSF) under grant number 200021\_178865... | {
"timestamp": "2018-06-07T02:17:45",
"yymm": "1802",
"arxiv_id": "1802.04221",
"language": "en",
"url": "https://arxiv.org/abs/1802.04221"
} |
\section{Introduction} \label{introduction}
We study the maximum of a branching random walk in discrete time. The branching random walk can be described as follows.
Given are two ingredients, an offspring distribution on $\N_0$ with weights $(p(k))_{k \in \N_0}$ and a (centred) step size distribution on $\R$.
At time $... | {
"timestamp": "2019-06-27T02:15:32",
"yymm": "1802",
"arxiv_id": "1802.03960",
"language": "en",
"url": "https://arxiv.org/abs/1802.03960"
} |
\section{Introduction}\label{Sec:Int}
Quantum resource theories provide a rigorous structure to characterise the resources present in quantum systems~\cite{horodecki2013quantumness,coecke2016mathematical,brandao2015reversible,gour2017quantum,regula2017convex}. Such resources arise whenever there is a restriction impos... | {
"timestamp": "2018-10-23T02:15:11",
"yymm": "1802",
"arxiv_id": "1802.04066",
"language": "en",
"url": "https://arxiv.org/abs/1802.04066"
} |
\section{Introduction}
\noindent The first idea on syllogisms was produced in the field of proper thinking by the Greek philosopher Aristotle. His idea mainly said that in his Prior Analytics: \textquotedblleft syllogism is discourse in which, certain things being stated, something other than what is stated follows o... | {
"timestamp": "2018-03-08T02:04:44",
"yymm": "1802",
"arxiv_id": "1802.04127",
"language": "en",
"url": "https://arxiv.org/abs/1802.04127"
} |
\section{Introduction}
Estimating the mean of a random vector under weak tail assumptions
has attracted a lot of attention recently. A number of properties
have spurred the interest for these new results, where the empirical
mean is replaced by a more robust estimator. One aspect is
that it is possible to obtain an... | {
"timestamp": "2018-02-14T02:00:47",
"yymm": "1802",
"arxiv_id": "1802.04308",
"language": "en",
"url": "https://arxiv.org/abs/1802.04308"
} |
\section{Introduction}
Robotics control and artificial intelligence (AI) in a broader perspective heavily rely on the availability of compact and expressive representations of the sensor data. Designing such representations has long been performed manually by the designer, but deep learning now provides a genera... | {
"timestamp": "2018-06-06T02:10:18",
"yymm": "1802",
"arxiv_id": "1802.04181",
"language": "en",
"url": "https://arxiv.org/abs/1802.04181"
} |
\section{Introduction}
\label{sec:intro}
We are interested in the unconstrained \emph{stochastic} non-convex optimisation problem
\begin{subequations}
\label{eq:problem}
\begin{align}
\min_{x\in\mathbb{R}^d}{f(x)},
\end{align}
when the cost function~$f(x)$ is on the form
\begin{align}
f(x) = \frac{1}{n}\su... | {
"timestamp": "2018-02-14T02:00:48",
"yymm": "1802",
"arxiv_id": "1802.04310",
"language": "en",
"url": "https://arxiv.org/abs/1802.04310"
} |
\section{Introduction}
\label{sec:introduction}
The reliable reduction of image noise poses a constantly recurring problem in today’s imaging systems. In healthcare, noise may limit the reliability of medical image data for subsequent clinical workflows. For instance, in radiology using computed tomography (CT) or re... | {
"timestamp": "2019-06-18T02:23:43",
"yymm": "1802",
"arxiv_id": "1802.03943",
"language": "en",
"url": "https://arxiv.org/abs/1802.03943"
} |
\section{Introduction}
Competition between on-site spin-orbit coupling (SOC), Coulomb repulsion
and crystal field interactions in Iridates gives rise to a plethora of unusual features.
For one of the most studied iridium-based compounds, Sr$_2$IrO$_4$, localized transport~\cite{ChengSun2016,Kim2008,Kim2009}, absence of... | {
"timestamp": "2018-08-02T02:08:07",
"yymm": "1802",
"arxiv_id": "1802.04158",
"language": "en",
"url": "https://arxiv.org/abs/1802.04158"
} |
\section{Introduction}
Since Stanley's 1975 proof of the upper bound conjecture for simplicial spheres via the Stanley-Reisner ring, the study of graded rings associated to combinatorial objects has yielded many deep insights into combinatorics (and vice versa).
The \emph{Chow ring} of an atomic\xspace lattice, defined... | {
"timestamp": "2018-02-13T02:23:22",
"yymm": "1802",
"arxiv_id": "1802.04241",
"language": "en",
"url": "https://arxiv.org/abs/1802.04241"
} |
\section{Introduction}
\label{sec:introduction}
Anyons~\cite{Wilczek1982,Leinaas1977}, particles with an exchange statistics interpolating between bosons and fermions, play a crucial role in fascinating concepts of modern condensed matter physics, such as topological quantum phases, in particular fractional quantum Ha... | {
"timestamp": "2018-02-13T02:16:40",
"yymm": "1802",
"arxiv_id": "1802.03970",
"language": "en",
"url": "https://arxiv.org/abs/1802.03970"
} |
\subsection{Algorithm}
\label{sub:active_impl}
\begin{algorithm}[tb]
\caption{Active $\epsilon$-greedy}
\label{alg:egreedy_active}
$\pi_1$; $\epsilon$; $C_0 > 0$.
$\verb+explore+(x_t)$:
\begin{algorithmic}
\STATE $A_t = \{a : \verb+loss_diff+(\pi_t, x_t, a) \leq \Delta_{t,C_0}\}$;
\STATE $p_t(a) = \frac{\epsilon... | {
"timestamp": "2020-01-27T02:07:23",
"yymm": "1802",
"arxiv_id": "1802.04064",
"language": "en",
"url": "https://arxiv.org/abs/1802.04064"
} |
\section{Introduction}
Full-field electro-dynamical simulations are used in nano-optics to predict the optical response of small (often sub-wavelength) particles by solving the Maxwell's equations~\cite{maxwell_dynamical_1865}.
Examples are either the scattering or the confinement of an external electro-magnetic fie... | {
"timestamp": "2018-06-11T02:11:12",
"yymm": "1802",
"arxiv_id": "1802.04071",
"language": "en",
"url": "https://arxiv.org/abs/1802.04071"
} |
\section{Introduction}
\label{sec:intro}
A hydrodynamic viscous fingering (VF) instability can deform the interface between two different fluids when a high mobility fluid of lower viscosity displaces a more viscous and hence less mobile one in a porous medium \cite{ST1958,S1986,TH1986,Homsy1987,TH1988}. In numerou... | {
"timestamp": "2018-02-13T02:20:48",
"yymm": "1802",
"arxiv_id": "1802.04153",
"language": "en",
"url": "https://arxiv.org/abs/1802.04153"
} |
\section{\@startsection {section}{1}{\z@}%
{-3.5ex \@plus -1ex \@minus -.2ex
{2.3ex \@plus.2ex}%
{\normalfont\large\bfseries}}
\renewcommand\subsection{\@startsection{subsection}{2}{\z@}%
... | {
"timestamp": "2018-04-20T02:09:18",
"yymm": "1802",
"arxiv_id": "1802.04278",
"language": "en",
"url": "https://arxiv.org/abs/1802.04278"
} |
\section{Introduction}
\label{sec:1}
Though the study of topological properties of dendrites from the viewpoint of general topology proceed for more than three quarters of a century \cite{Char,Kur, Nad}, the attempts to study the geometrical properties of self-similar dendrites are rather fragmentary.
In 1985, M.~Ha... | {
"timestamp": "2018-02-13T02:20:41",
"yymm": "1802",
"arxiv_id": "1802.04148",
"language": "en",
"url": "https://arxiv.org/abs/1802.04148"
} |
\section{Introduction}
Semidefinite programming (SDP) has become a key tool in solving numerous problems across operations research, machine learning, and artificial intelligence. While there are too many applications of SDP to present even a representative sample, inference in graphical models \cite{ExpFamilies,erdo... | {
"timestamp": "2019-08-02T02:08:25",
"yymm": "1802",
"arxiv_id": "1802.04332",
"language": "en",
"url": "https://arxiv.org/abs/1802.04332"
} |
\section{Introduction}
\label{sec:Intro}
Although complex networks theory \cite{strogatz2001exploring, newman2003structure} was initially used to describe the structure underpinning individual complex systems, in recent years there has been an explosion in the number of situations in which (potentially large) sets of ... | {
"timestamp": "2018-02-13T02:16:36",
"yymm": "1802",
"arxiv_id": "1802.03966",
"language": "en",
"url": "https://arxiv.org/abs/1802.03966"
} |
\section{Introduction}
Accessing long timescales in molecular dynamics (MD) simulations remains a longstanding challenge.
Limited by the short time steps of a few femtoseconds, and despite recent progress in methods and hardware \cite{Lindorff-Larsen2011,Buch2011,Tiwary2015a,Paul2017},
it remains difficult to access t... | {
"timestamp": "2018-02-13T02:21:39",
"yymm": "1802",
"arxiv_id": "1802.04182",
"language": "en",
"url": "https://arxiv.org/abs/1802.04182"
} |
\section{Introduction}
Point-defects in crystalline solids,
being either intrinsic like vacancies, self-interstitial atoms,
and their small clusters,
or extrinsic like impurities and dopants,
play a major role in materials properties and their kinetic evolution.
Some properties of these point-defects, like their f... | {
"timestamp": "2018-02-13T02:18:49",
"yymm": "1802",
"arxiv_id": "1802.04062",
"language": "en",
"url": "https://arxiv.org/abs/1802.04062"
} |
\section{Introduction}
\label{sec:intro}
Polycyclic aromatic hydrocarbons (PAHs) are a highly abundant family of astronomical molecules that produce dominant infrared (IR) emission features in the 3-20 \textmu m~ spectral range, primarily at 3.3, 6.2, 7.7, 8.6, 11.2, 12.7 and 16.4 \textmu m~ (e.g., \citealt{leger1984,... | {
"timestamp": "2018-02-14T02:00:30",
"yymm": "1802",
"arxiv_id": "1802.04282",
"language": "en",
"url": "https://arxiv.org/abs/1802.04282"
} |
\section{Introduction}
Though machine learning advances greatly in many areas in recent years such as computer vision and natural language processing, limited interpretability hinders it from impacting areas that require clearer evidence for decision making such as health care and economy. In these domains, most widely... | {
"timestamp": "2018-05-24T02:05:17",
"yymm": "1802",
"arxiv_id": "1802.04253",
"language": "en",
"url": "https://arxiv.org/abs/1802.04253"
} |
\section{Introduction} \label{intro}
The hypothesis of cosmic inflation
\cite{Guth:1980zm,Linde:1981mu,Albrecht:1982wi,Linde:1983gd} provides a
plausible explanation of the large scale homogeneity of the universe and,
more importantly, of the primordial density perturbations that evolve into
cosmic structure. A simple... | {
"timestamp": "2018-05-18T02:07:34",
"yymm": "1802",
"arxiv_id": "1802.04160",
"language": "en",
"url": "https://arxiv.org/abs/1802.04160"
} |
\section{Introduction}
Spreading processes are ubiquitous in nature: from the contagion of diseases \citep{Anderson1991}, herd behaviour in animals \citep{Sumpter2008}, the diffusion of innovations \citep{Rogers2010}, rumour spreading \citep{Daley1965}, the evolution of social movements \citep{Gonzalez-Bailon2013}, th... | {
"timestamp": "2018-02-13T02:16:20",
"yymm": "1802",
"arxiv_id": "1802.03951",
"language": "en",
"url": "https://arxiv.org/abs/1802.03951"
} |
\section{Introduction}
The Born's interpretation of $|\psi|^2$ as position probability density is one of the most fundamental axioms of quantum mechanics as it provides a link between the mathematical formalism and empirical results \cite{M. Born}. This axiom has been incredibly successful in predicting position prob... | {
"timestamp": "2018-07-24T02:06:06",
"yymm": "1802",
"arxiv_id": "1802.04266",
"language": "en",
"url": "https://arxiv.org/abs/1802.04266"
} |
\section{#1}\setcounter{equation}{0}}
\renewcommand{\theequation}{\thesection.\arabic{equation}}
\newcommand{\TN}[1]{{\color{red} [{\bf TN:} #1]}}
\newcommand{\TNmod}[1]{{\color{red} #1}}
\newcommand{\SA}[1]{{\color{blue} [{\bf SA:} #1]}}
\newcommand{\DI}[1]{{\color[rgb]{0.1,0.5,0.1} #1}}
\allowdisplaybreaks
\allowd... | {
"timestamp": "2018-02-14T02:00:35",
"yymm": "1802",
"arxiv_id": "1802.04287",
"language": "en",
"url": "https://arxiv.org/abs/1802.04287"
} |
\subsection{Contributions of this work}
Over the course of single activity sessions, we measure
different quantities capturing user behaviour, e.g.,\
propensity to engage in social interactions, or amount of produced content,
and finally contrast results between bots and humans.
The present study advances our unde... | {
"timestamp": "2018-02-15T02:12:23",
"yymm": "1802",
"arxiv_id": "1802.04286",
"language": "en",
"url": "https://arxiv.org/abs/1802.04286"
} |
\section{Introduction}
\label{sec:Intro}
Dust is an essential component in understanding star formation
properties of galaxies
both observationally and theoretically.
Because dust absorbs stellar ultraviolet (UV)--optical light and reemits it in the infrared (IR)
\citep[e.g.][]{2000ApJ...533..682C,2002A&A...383... | {
"timestamp": "2018-07-24T02:10:54",
"yymm": "1802",
"arxiv_id": "1802.04027",
"language": "en",
"url": "https://arxiv.org/abs/1802.04027"
} |
\section{Introduction}
Let $C$ denote a smooth, irreducible, complex projective curve of genus $g \geq 3$. Let $U_C(2, d)$ be the moduli space of semistable, degree $d$, rank $2$ vector bundles on $C$ and let $U^s_C(2,d)$ be the open dense subset of stable bundles (when $d$ is odd, more precisely one has $U_C(2, d)=U... | {
"timestamp": "2018-09-07T02:07:14",
"yymm": "1802",
"arxiv_id": "1802.03956",
"language": "en",
"url": "https://arxiv.org/abs/1802.03956"
} |
\section{Introduction}
Engineering and contemporary science are based on the first-principle models of biological, social and physical systems.
A primary scientific model, such as Newton's laws or Maxwell's equations, begins in electromagnetism and then builds various applications in mechanical or electrical engineerin... | {
"timestamp": "2018-02-13T02:19:57",
"yymm": "1802",
"arxiv_id": "1802.04109",
"language": "en",
"url": "https://arxiv.org/abs/1802.04109"
} |
\section{Introduction\label{sec:intro}}
From the particle physics point of view, the simplest, most popular, and arguably most robust mechanism leading
to the correct amount of cold dark matter (DM) in the early Universe is thermal freeze-out (see, e.g.,\cite{Kolb:1990vq,Gondolo:1990dk,Jungman:1995df,Dodelson:2003ft})... | {
"timestamp": "2018-11-20T02:44:24",
"yymm": "1802",
"arxiv_id": "1802.04097",
"language": "en",
"url": "https://arxiv.org/abs/1802.04097"
} |
\section{Introduction}
\subsection{Empirical measures and quadrature}
Consider a discrete-time stochastic process $(X_k)_{k\ge 0}$ taking its values in some phase space $\Omega$, assumed to be a Polish space endowed with its Borel $\sigma$-algebra. We are concerned with the random atomic measure \[ \hat\mu_n = \frac1... | {
"timestamp": "2018-02-13T02:18:17",
"yymm": "1802",
"arxiv_id": "1802.04038",
"language": "en",
"url": "https://arxiv.org/abs/1802.04038"
} |
\section{Introduction}
The field of nuclear security addresses the danger of the nuclear weapons,
including proliferation of weapon technology, safeguards of
fissile materials, and the risk of nuclear terrorism. The latter topic encompasses cargo security, which specifically focuses
on preventing the smuggling of ... | {
"timestamp": "2018-03-21T01:04:08",
"yymm": "1802",
"arxiv_id": "1802.04225",
"language": "en",
"url": "https://arxiv.org/abs/1802.04225"
} |
\section{Entropy of a disordered star polymer}
The goal of this section is to calculate the total number of blobs $N_{\mathrm{blob}}$ in the star polymer, since the free energy $F$ is proportional to that number:
\begin{equation}
\beta F = N_{\mathrm{blob}}
\label{eq:blob_F}
\end{equation}
where $\beta=1/k_{\mathrm{B}... | {
"timestamp": "2018-02-13T02:16:19",
"yymm": "1802",
"arxiv_id": "1802.03949",
"language": "en",
"url": "https://arxiv.org/abs/1802.03949"
} |
\section{Introduction}
\label{intro}
In the Music Information Retrieval (MIR) field, many research problems of interest involve the automatic description of properties of musical signals, employing concepts that are understood by humans. For this, tasks are derived that can be solved by automated systems. In such case... | {
"timestamp": "2019-02-13T02:04:07",
"yymm": "1802",
"arxiv_id": "1802.04051",
"language": "en",
"url": "https://arxiv.org/abs/1802.04051"
} |
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