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\section{Introduction}
An inverse atmospheric dispersion problem is stated as follows: given the
topography, the meteorological conditions and a set of detector readings
determine where and when the hazardous substance was released and in which
quantities. The problem is known as a source reconstruction problem, and i... | {'timestamp': '2016-07-19T02:05:37', 'yymm': '1607', 'arxiv_id': '1607.04804', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04804'} | arxiv | |
\section{Introduction}
Network operators continuously upgrade their networks due to increasing demands for ubiquitous communications. As popularities of cloud computing, Internet of Things (IoT), and 5G mobile communications increase, network traffic is becoming heavy and extremely bursty. Thus, just enlarging the netw... | {'timestamp': '2017-01-05T02:05:47', 'yymm': '1607', 'arxiv_id': '1607.04695', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04695'} | arxiv | |
\section{Introduction}
\subsection{The main theorem}
Let $F$ be a totally real field, $p$ be an odd prime, and ${\mathcal O}$ the ring of integers of a finite extension of $\Q_p$. In proving automorphy of geometric representations $\rho:G_F \rightarrow GL_2({\mathcal O})$ which are residually automorphic, there is a... | {'timestamp': '2016-07-19T02:04:41', 'yymm': '1607', 'arxiv_id': '1607.04750', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04750'} | arxiv | |
\section{Introduction}\label{sec1}
An important tool of modern harmonic analysis is the extrapolation theorem due to Rubio de Francia.
For a given operator $T$ we suppose that for some $p_0$, $1 \le p_0 < \infty$, and
for every weight belonging to the Muckenhoupt class $A_{p_0}$ the inequality
\begin{equation} \label{... | {'timestamp': '2017-10-23T02:06:44', 'yymm': '1607', 'arxiv_id': '1607.04565', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04565'} | arxiv | |
\section{Introduction}
The phenomenon of Brillouin scattering, whereby an acoustic field mediates
transitions between optical modes in an optical
waveguide~\cite{Brillouin1922,Boyd2003,Agrawal2012}, has been the focus of
intense research interest in recent years, driven by a suite of key
applications in nanophoto... | {'timestamp': '2016-08-26T02:02:51', 'yymm': '1607', 'arxiv_id': '1607.04740', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04740'} | arxiv | |
\section{Introduction \label{sec:intro}}
\IEEEPARstart{A}{utomatic} speech recognition, music classification, audio
indexing, and to a less visible extent biometric voice authentication, have now
achieved some degree of commercial success in mass markets. A vast proportion
of these applications are supported by PC plat... | {'timestamp': '2016-07-18T02:08:46', 'yymm': '1607', 'arxiv_id': '1607.04589', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04589'} | arxiv | |
\section{Introduction}
Let $\Omega$ be a domain of $\mathbb{R}^n$ and $W_0^{1,q}(\Omega)$ be the closure of $C_0^\infty(\Omega)$ with respect to the norm
$$\|u\|_{W_0^{1,q}(\Omega)}=\le(\int_\Omega\le(|\nabla u|^q+|u|^q\ri)dx\ri)^{1/q},$$
where $q\geq 1$. Then the Sobolev embedding theorem reads
$$W_0^{1,q}(\Omeg... | {'timestamp': '2016-07-18T02:07:27', 'yymm': '1607', 'arxiv_id': '1607.04521', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04521'} | arxiv | |
\section{Introduction}
Suppose that $F$ is a free group of finite rank, $\rr(F)$ denotes the rank of $F$, and $\brr(F) := \max
(\rr(F)-1,0)$ is the reduced rank of $F$. Let $H, K$ be finitely
generated subgroups of $F$ and let $\langle H, K \rangle$ denote the the subgroup generated by $H, K$, called th... | {'timestamp': '2016-07-19T02:07:49', 'yymm': '1607', 'arxiv_id': '1607.04890', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04890'} | arxiv | |
\section{Introduction}
The Downwards L\"{o}wenheim-Skolem-Tarski Theorem states that every model $M$ for a language $\mathcal{L}$, $|M| = \kappa \geq \aleph_0$, and cardinal $|\mathcal{L}| + \aleph_0 \leq \mu \leq \kappa$ there is an elementary submodel $M^\prime \prec M$, of cardinality $\mu$. Informally speaking, th... | {'timestamp': '2017-10-31T01:10:10', 'yymm': '1607', 'arxiv_id': '1607.04904', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04904'} | arxiv | |
\section{Introduction}
Recent years have witnessed a remarkable convergence of two broad trends. The first of these concerns information i.e.\ data -- rapid technological advances coupled with an increased presence of computing in nearly every aspect of daily life, have for the first time made it possible to acquire an... | {'timestamp': '2016-07-19T02:00:36', 'yymm': '1607', 'arxiv_id': '1607.04660', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04660'} | arxiv | |
\section{Introduction}\label{sec:intro}
Many central problems in geometry, topology, and mathematical physics lead to questions concerning the long-time dynamics of solutions to ordinary and parabolic partial differential equations. Three basic scenarios are possible. \\
First, under suitable dissipativity conditions... | {'timestamp': '2016-07-18T02:09:04', 'yymm': '1607', 'arxiv_id': '1607.04600', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04600'} | arxiv | |
\section{Introduction}
In the past decade, a new field dubbed topological insulator (TI)\cite{hasan2010colloquium,qi2011topological,kane2005z,bernevig2006quantum} has caused enormous attentions in the condensed matter physics. Different from the earliest topological states in quantum Hall effect\cite{klitzing1980new,t... | {'timestamp': '2016-07-19T02:04:37', 'yymm': '1607', 'arxiv_id': '1607.04743', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04743'} | arxiv | |
\section{Introduction}
Employing the AdS/CFT correspondence it was shown \cite{Hartnoll:2008vx} that a
holographic superconductor can be builded on a boundary of
a gravity theory consisting of a black hole which acquires scalar hair
at temperature below a critical temperature, while above the critical temperature ther... | {'timestamp': '2016-08-30T02:02:20', 'yymm': '1607', 'arxiv_id': '1607.04928', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04928'} | arxiv | |
\section{Introduction}
Heavy quarks (charm and beauty) are abundantly produced at the LHC \cite{LHC} in the early stages of hadronic collisions via hard scattering processes and experience the full evolution of the collision. The measurement of heavy flavours in \ensuremath{\mathrm {p\kern-0.05emp}}\ collisions can be... | {'timestamp': '2016-07-18T02:07:58', 'yymm': '1607', 'arxiv_id': '1607.04554', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04554'} | arxiv | |
\section{Introduction\label{sec:intro}}
In the United States, bladder cancer is the fourth and ninth most
widespread cancer among males and females, respectively, whereas in
Europe, approximately 50,000 people die from this disease each year
\cite{Alcaraz:2007}. Due to the high recurrence rate of $50\%$,
lifetime monit... | {'timestamp': '2016-07-19T02:04:58', 'yymm': '1607', 'arxiv_id': '1607.04773', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04773'} | arxiv | |
\section{Custodial symmetry in the SM and the THDM}
\label{Sec:CustSym}
The custodial symmetry is an approximate global \linebreak${SU(2)_L\times SU(2)_R}$ symmetry of the SM which is responsible for the tree-level value of the $\rho$ parameter \cite{Weinberg:1979bn,Susskind:1978ms,Sikivie:1980hm}. Since the Higgs pot... | {'timestamp': '2017-03-22T01:10:01', 'yymm': '1607', 'arxiv_id': '1607.04610', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04610'} | arxiv | |
\section{\label{sec:level1}Introduction\protect\\}
Contamination of a cylindrically or toroidally trapped electron plasma by a fractional population of ions can, under certain conditions, disrupt the equilibrium of the trapped electron cloud. The related instability, known as the ion resonance instability, manifests i... | {'timestamp': '2016-07-19T02:06:51', 'yymm': '1607', 'arxiv_id': '1607.04843', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04843'} | arxiv | |
\section{Introduction}
Radio galaxies and quasars have radio-emitting structure that can be conveniently divided into two
categories: extended structure, the dimensions of which range
from $10^{3}$ pc to even $10^{6}$ pc, and compact structure,
with dimensions typically ranging from 1 pc to 100 pc \citep{kel88}.... | {'timestamp': '2016-07-19T02:02:43', 'yymm': '1607', 'arxiv_id': '1607.04706', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04706'} | arxiv | |
\section{Introduction}
Let $X_{1},X_{2},....$ be a sequence of independent random variables with common distribution function $F$ and for each integer $n\geq 1$, let
X_{1,n}\leq ...\leq X_{n,n}$ denote the order statistics based on the first
n$ of these random variables. Cs\"{o}rg\H{o} and Mason (1985, 1986) have ... | {'timestamp': '2016-07-19T02:06:59', 'yymm': '1607', 'arxiv_id': '1607.04848', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04848'} | arxiv | |
\section*{abstract}
Light possesses both spin and orbital angular momentum (AM). While spin AM is determined by helicity of circular-polarization, orbital AM is characterized by topological charge of vortex beam. Interaction of AM with optical beam orbit leads to optical spin Hall or orbital Hall effect, exhibited as ... | {'timestamp': '2016-08-18T02:06:59', 'yymm': '1607', 'arxiv_id': '1607.04806', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04806'} | arxiv | |
\section{Introduction}
\label{sec:intro}
The precise measurement of the polarization of the Cosmic Microwave Background (CMB) is an active area of experimental physics, motivating a variety of current and upcoming polarimeter projects.
The CMB temperature anisotropy, measured to extreme precision over the last two de... | {'timestamp': '2016-07-19T02:00:45', 'yymm': '1607', 'arxiv_id': '1607.04668', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04668'} | arxiv | |
\section{Introduction}
Radio galaxies (RGs) are radio loud active galaxy nuclei (AGN) exhibiting clear structure of a compact central source, large-scale jets and lobes. These sources are also of interest due to the close proximity to the earth affording us an excellent opportunity for studying the physics of relat... | {'timestamp': '2016-07-18T02:09:51', 'yymm': '1607', 'arxiv_id': '1607.04633', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04633'} | arxiv | |
\section{Introduction}
Bulk acoustic wave (BAW) piezoelectric devices are widely used in research and industry to make temperature sensors, acoustic cavities or filters for several applications. Recently it has been demonstrated that quartz acoustic cavities can exhibit very high quality factors, up to a few billion... | {'timestamp': '2016-07-18T02:08:43', 'yymm': '1607', 'arxiv_id': '1607.04584', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04584'} | arxiv | |
\section{Introduction}
\label{intro}
Deep neural networks (DNNs) have been successful in modeling many aspects of
natural language including word meanings \cite{mikolov}\cite{le},
machine translation \cite{sutskever},
syntactic parsing \cite{vinyals_grammar}, language modeling \cite{jozefowicz} and
image captioning ... | {'timestamp': '2016-07-18T02:08:34', 'yymm': '1607', 'arxiv_id': '1607.04576', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04576'} | arxiv | |
\section{Introduction}
\label{section.introduction_chap_fb}
The Fermi bubbles are important Galactic structures that were recently discovered by the \textit{Fermi Gamma-ray Space Telescope} \citep{su_etal10}. The bubbles are two diffuse lobes of material extending $\sim$50$\arcdeg$ above and below the Galactic plane... | {'timestamp': '2016-07-19T02:08:34', 'yymm': '1607', 'arxiv_id': '1607.04906', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04906'} | arxiv | |
\section{Introduction}
It is well known that a degree $n$ Blaschke product is an $n$-to-$1$ (counting multiplicity) analytic self-map of the unit disk $\mathbb{D}$, and moreover that every such analytic $n$-to-$1$ self-map of the unit disk is a degree $n$ Blaschke product. We can restate this in a slightly more gener... | {'timestamp': '2016-07-18T02:09:10', 'yymm': '1607', 'arxiv_id': '1607.04607', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04607'} | arxiv | |
\section{Multi-threading}
We measure the performance of the obtained word vectors on the word similarity task, when the number of threads used for training change.
In Table~\ref{tab:threads} we report the correlation with human judgement for models trained on \texttt{small} for threads ranging from 1 to 32.
In Table~\... | {'timestamp': '2017-06-20T02:14:36', 'yymm': '1607', 'arxiv_id': '1607.04606', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04606'} | arxiv | |
\section{Introduction and Related Work}
Automatic analysis of urban traffic activities is an urgent need due to essential traffic management and increased vehicle violations. Among many traffic surveillance techniques, computer vision-based methods have attracted a great deal of attention and made great contributions t... | {'timestamp': '2016-08-02T02:11:40', 'yymm': '1607', 'arxiv_id': '1607.04564', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04564'} | arxiv | |
\section{Introduction}
Given a smooth manifold $M$, assume a family of smooth immersions in a semi-Rieman\-nian manifold $(\mathbf{M},\mathbf{g})$, $F_t:M\rightarrow \mathbf{M}$, $t\in [0,\delta)$, $\delta>0$, with mean curvature vector $\vec{H}_t$. The initial immersion $F_0$ is called a solution to the \textit{mean... | {'timestamp': '2018-03-23T01:10:14', 'yymm': '1607', 'arxiv_id': '1607.04571', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04571'} | arxiv | |
\section{Introduction}
Increasing the number of cellular base stations~(BSs) to serve a given area, also known as network densification, is foreseen to be a necessary solution
to address the large data rate
demands of the future fifth-generation~(5G) wireless communication networks~\cite{andrews-etal2014what,bhushan-et... | {'timestamp': '2017-06-06T02:07:57', 'yymm': '1607', 'arxiv_id': '1607.04931', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04931'} | arxiv | |
\section{Introduction}
When dealing with large data sets, it is often crucial to be able to extract a smaller well-diversified subset of the data. This is a classic problem in information retrieval, and appears in many natural settings.
For example, a news website often presents the reader with a small list of hi... | {'timestamp': '2016-07-18T02:07:59', 'yymm': '1607', 'arxiv_id': '1607.04557', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04557'} | arxiv | |
\section{Introduction}
Entanglement is a valuable resource in precision measurement, as measurements using entangled probe systems have fundamentally higher optimal sensitivity than those using unentangled states \cite{Bollinger1996}. A generic measurement using $N$ unentangled probes will have a standard deviation fr... | {'timestamp': '2018-03-26T02:09:50', 'yymm': '1607', 'arxiv_id': '1607.04646', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04646'} | arxiv | |
\section{Introduction}
\label{sec-1}
``The devil is in the tails" is the title of the paper by Donnelly and
Embrechts (2010) who refute the harsh criticism of mathematics (Salmon,
2012) in general, and of the Gaussian copula-based credit risk model
of Li (2000) in particular. As a member of the unholy trinity (Ko... | {'timestamp': '2016-07-19T02:03:59', 'yymm': '1607', 'arxiv_id': '1607.04736', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04736'} | arxiv | |
\section{Introduction} \label{intro}
The goal of this work is to further explore heterotic target space duality, with the hope of moving towards a more fully developed notion of dualities involving the $(0,2)$ heterotic string. At present, many heterotic string dualities -- including any complete notion of $(0,2)$ mir... | {'timestamp': '2016-07-18T02:09:48', 'yymm': '1607', 'arxiv_id': '1607.04628', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04628'} | arxiv | |
\section*{Introduction}
M. F. Atiyah \cite{MR0420729}
introduced the notion of the $\Gamma$-index $\mathrm{index}_{\Gamma}(\widetilde{D})$
for a lifted elliptic differential operator $\widetilde{D}$
on a Galois $\Gamma$-covering over a closed manifold
and proved that the $\Gamma$-index $\mathrm{index}_{\Gamma}(\wi... | {'timestamp': '2016-07-28T02:03:45', 'yymm': '1607', 'arxiv_id': '1607.04820', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04820'} | arxiv | |
\section*{Appendix}
\subsection{Proof of Lemma \ref{lem:sigmak}}
\begin{IEEEproof}
We first state the following result that will be used in the proof.
\begin{lemma}[Ger\v{s}hgorin circle theorem \cite{HJ12}]
Let A be a complex $n \times n$ matrix, with entries $a_{ij}$. Then, every eigenvalue of A lies within at least... | {'timestamp': '2016-07-19T02:05:07', 'yymm': '1607', 'arxiv_id': '1607.04776', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04776'} | arxiv | |
\section{Introduction} \label{Sec_Introduction}
Modification of hadron properties in extreme environments such as finite temperature and density is one of the important problems in hadron physics, which is useful to clarify the relation between hadrons and the vacuum.
Similarly, an external magnetic field comparable to... | {'timestamp': '2016-11-07T02:03:02', 'yymm': '1607', 'arxiv_id': '1607.04935', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04935'} | arxiv | |
\section{Introduction}\label{sec:introduction}
Quantitative investigations in logic, where properties and behaviour of typical objects are studied, form a rich and well-established branch of mathematics on the border of logic, combinatorics and theoretical computer science. From a combinatorial point of view, logical f... | {'timestamp': '2016-07-19T02:08:36', 'yymm': '1607', 'arxiv_id': '1607.04908', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04908'} | arxiv | |
\section*{1. Introduction}
The Riemann zeta function $\zeta(s)$ which basically was known already to Euler establishes the most important link between number theory and analysis. The proof of the Riemann hypothesis is a longstanding problem since it was formulated by Riemann \cite{rie} in 1859. The Riemann hypothesis ... | {'timestamp': '2016-07-18T02:07:55', 'yymm': '1607', 'arxiv_id': '1607.04551', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04551'} | arxiv | |
\section{Introduction}
In this paper we study a parameter estimation problem for the drift/viscosity coefficient of a linear parabolic stochastic partial differential equation (SPDE) driven by an additive space-time noise (possibly colored in space). We assume that the observable variable is one path of the solution,... | {'timestamp': '2016-11-15T02:07:03', 'yymm': '1607', 'arxiv_id': '1607.04912', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04912'} | arxiv | |
\section{Introduction}
Consider the standard stochastic approximation scheme given by,
\begin{equation}\label{recstd}
X_{n+1}=X_n+a(n)\left(h(X_n)+M_{n+1}\right)
\end{equation}
where $\left\{X_n\right\}_{n\geq0}$ is a sequence of $\mathbb{R}^d$-valued random variables, $h:\mathbb{R}^d\rightarrow\mathbb{R}^d$ is a Lip... | {'timestamp': '2016-07-19T02:03:49', 'yymm': '1607', 'arxiv_id': '1607.04735', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04735'} | arxiv | |
\section{Introduction}
Let $d\geq 3$ and let $G(n,d)$ denote the random $d$-regular graph on $n$ vertices (see e.g.\ the monograph \cite{bollobas}). Equivalently, we can think of $G(n,d)$ as a random model of symmetric $0-1$ matrices in which the row sums are conditioned to be $d$. It is expected that the spectral pr... | {'timestamp': '2016-07-19T02:05:12', 'yymm': '1607', 'arxiv_id': '1607.04785', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04785'} | arxiv | |
\section{Introduction}
\subsection{Introduction}
The Fisher--Rao metric on the space $\on{Prob}(M)$ of probability densities is invariant under the action of the diffeomorphism group $\on{Diff}(M)$.
Restricted to finite-dimensional submanifolds of $\on{Prob}(M)$,
so-called statistical manifolds, it is called Fisher's... | {'timestamp': '2018-05-10T02:05:43', 'yymm': '1607', 'arxiv_id': '1607.04550', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04550'} | arxiv | |
\section{Introduction}
Galaxy clusters are the largest virialized structures in the Universe and form
via aggregation of less massive systems \citep[e.g.][]{press74}. During merger
events, the intra-cluster medium (ICM) is heated by shocks and is believed to
become turbulent. Part of the energy involved in these pr... | {'timestamp': '2016-08-19T02:07:22', 'yymm': '1607', 'arxiv_id': '1607.04641', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04641'} | arxiv | |
\section{Introduction}
Adaptation is often viewed as a cumulative succession of fixations of beneficial mutations, and the waiting time between two successive beneficial mutations is viewed as one of the main factor limiting adaptation rate \citep{fisher1930, crowkimura1965}. This is however not true in general sinc... | {'timestamp': '2016-07-19T02:00:32', 'yymm': '1607', 'arxiv_id': '1607.04656', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04656'} | arxiv | |
\section{Introduction}
\subsection{Overview}
Distributing points on $\mathbb{S}^2:=\left\{x\in\mathbb{R}^3 : \ |x|=1\right\}$ is a classical problem arising in many settings in numerical analysis and approximation theory, in particular the study of radial basis functions, quadrature and polynomial interpolation, Quasi-... | {'timestamp': '2016-10-25T02:07:57', 'yymm': '1607', 'arxiv_id': '1607.04590', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04590'} | arxiv | |
\section{Introduction}
The problem of finding the best packings of lines, one-dimensional subspaces of a real or complex Euclidean space, is easy to state. Despite its simple geometric formulation, it has given rise to a surprisingly diverse literature over many years,
ranging from relatively elementary, low dimension... | {'timestamp': '2016-07-18T02:07:51', 'yymm': '1607', 'arxiv_id': '1607.04546', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04546'} | arxiv | |
\section{Error Probability Bound}\label{appendix:APPENDIX A}
In this section, we give a direct proof for \Cref{direct lemma1}. Specifically, we bound the error probability of the maximum likelihood decoder, and show that under the condition on $T$ in the lemma, the error probability is indeed approaching $0$ as $N \to... | {'timestamp': '2018-01-17T02:06:19', 'yymm': '1607', 'arxiv_id': '1607.04849', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04849'} | arxiv | |
\section{Introduction}
Distinct from conventional phase transitions driven by spontaneous symmetry breaking,
Lifshitz phase transition is driven by an abrupt change of the topology
of the Fermi surface~\cite{Lifshitz}. Recently, it has been predicted in three-dimensional (3D)
condensed matter materials that type-... | {'timestamp': '2016-11-23T02:02:10', 'yymm': '1607', 'arxiv_id': '1607.04924', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04924'} | arxiv | |
\section{Introduction \label{introd}}
Strong lensing
provides a useful tool to uncover the mass distribution in
galaxies \citep[e.g.,][]{0004-637X-575-1-87,2002MNRAS.337L...6T,2006ApJ...649..599K}
and galaxy clusters \citep[e.g.,][]{1989ApJ...337..621K,1998MNRAS.294..734A,2007MNRAS.376..180N,2010AdAst2010E...9Z,2... | {'timestamp': '2016-11-03T01:01:56', 'yymm': '1607', 'arxiv_id': '1607.04644', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04644'} | arxiv | |
\section*{\bf $\Psi_k$ Scientific Highlight Of The Month}
\newcommand{\ensuremath\mathrm{d}}{\ensuremath\mathrm{d}}
\begin{center}
{\large \bf Towards a Common Format for Computational Material Science Data}
{Luca M. Ghiringhelli$^{1,}$\footnote{ghiringhelli@fhi-berlin.mpg.de},
Christian Carbogno$^{1}$,
Sergey Levchen... | {'timestamp': '2016-07-19T02:04:00', 'yymm': '1607', 'arxiv_id': '1607.04738', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04738'} | arxiv | |
\section{Introduction}
Let $T$ be a bounded operator on a complex Hilbert space $\mathcal{H}$. Then $T$ is called complex symmetric if there exists a conjugation $C$ such that $T=CT^*C$. Here a conjugation is a conjugate-linear, isometric involution on $\mathcal{H}$. The operator $T$ may also be called $C$-symmetric... | {'timestamp': '2016-08-02T02:09:19', 'yymm': '1607', 'arxiv_id': '1607.04801', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04801'} | arxiv | |
\section{Introduction}
This paper explores Tur\'{a}n-type problems for a class of relational structures that can each be thought of as generalized directed hypergraphs. This class includes the standard undirected $r$-uniform hypergraphs that have been extensively studied in combinatorics as well as totally directed $r... | {'timestamp': '2016-07-19T02:09:36', 'yymm': '1607', 'arxiv_id': '1607.04927', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04927'} | arxiv | |
\section{Motivation}
Understanding of the analytic structure of the contribution of a graph to a Feynman amplitude, a time-honored problem \cite{Pham},
is related to an analysis of
its reduced graphs and the graphs in which internal edges are on the mass-shell. The former case relates to graphs in which internal edges... | {'timestamp': '2016-07-19T02:07:15', 'yymm': '1607', 'arxiv_id': '1607.04861', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04861'} | arxiv | |
\section{Introduction}
Let $\lambda_1,\ldots,\lambda_n$ be $n$ distinct values. The Lagrange interpolation formula says that a polynomial $P(x)$ of degree not greater than $n-1$ in one variable can be written in the following:
$$P(x) = \sum_{i=1}^nP(\lambda_i)L_i(x),$$
where
$$L_i(x) = \prod_{j\neq i}\frac{x-\lambda_... | {'timestamp': '2016-09-12T02:04:24', 'yymm': '1607', 'arxiv_id': '1607.04850', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04850'} | arxiv | |
\section*{Abstract}
We present a spectrally accurate method for the rapid evaluation of free-space Stokes
potentials, i.e. sums involving a large number of free space Green's
functions. We consider sums involving stokeslets, stresslets and
rotlets that appear in boundary integral methods and potential methods for solv... | {'timestamp': '2016-07-19T02:05:44', 'yymm': '1607', 'arxiv_id': '1607.04808', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04808'} | arxiv | |
\section{Introduction}
The Aubry-Andr\' e-Harper (AAH) model has been extensively used as a quasiperiodic model to theoretically study the phase transition between extended, critical and localized phases \cite{Harper, Aubry, Hiramoto1, Ostlund, Kohmoto1, Kohmoto2, Thouless, Hiramoto2, Geisel, Han, Chang, Takada, Liu, ... | {'timestamp': '2016-09-26T02:01:24', 'yymm': '1607', 'arxiv_id': '1607.04835', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04835'} | arxiv | |
\section*{Results}
\begin{figure}
\includegraphics[width=80mm]{figures/fig2_simulated_errors.eps}
\caption{\label{fig:simErr} Actual and estimated errors in simulated
data. (a) Root mean square (RMS) error
$\sqrt{\mean{(\mu_\text{est.}-\mu_\text{true})^2}}$ vs.~root mean
estimated error variance $\sqrt{\mean{... | {'timestamp': '2016-07-19T02:01:52', 'yymm': '1607', 'arxiv_id': '1607.04675', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04675'} | arxiv | |
\section{introduction}
At the outset, we fix the probability space $(\Omega,\Sigma,\mathbf{P})$ and
define the random vector (r.v.) $\mathcal{X}\ni\mathbf{X}=(X_1,\ldots,X_n)'$ as a map from
$(\Omega,\Sigma)$ to the $n(\in\mathbf{N})$-dimensional Borel space
$(\mathbf{R}_+^n,\mathcal{B}(\mathbf{R}_+^n))$. The cumul... | {'timestamp': '2016-07-19T02:03:59', 'yymm': '1607', 'arxiv_id': '1607.04737', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04737'} | arxiv | |
\section{Introduction}
Humanoid robots have been widely studied in the research of robotics.
With the recent development of motion capture devices such as RGB-D camera
(e.g., Kinect) and wearable sensor system (e.g., Xsens MVN), efforts have
been made to generate human-like motions for humanoid robots with high degree... | {'timestamp': '2016-07-26T02:11:48', 'yymm': '1607', 'arxiv_id': '1607.04907', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04907'} | arxiv | |
\section{Introduction}
Structure-from-Motion targets at recovering 3D structure and camera motion from monocular 2D feature tracks. Conventional SFM primarily concerns with the 3D reconstruction of a single rigidly moving object seen by a static camera, or a static and rigid scene observed by a moving camera --in both ... | {'timestamp': '2016-07-18T02:07:21', 'yymm': '1607', 'arxiv_id': '1607.04515', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04515'} | arxiv | |
\section{Numerical simulations of the quantum dynamics and the associated transient-absorption spectra}
\label{Equations of motion and transient-absorption spectra}
\setcounter{equation}{0}
We model Rb atoms as three- or five-level systems, as shown in Fig.~2(b) in the article. We consider a quantum system in the st... | {'timestamp': '2016-09-22T02:06:48', 'yymm': '1607', 'arxiv_id': '1607.04570', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04570'} | arxiv | |
\section{Proof-of-Concept Applications}
This paper demonstrates backscatter communication on commodity devices, and in this section we evaluate prototypes of three novel applications enabled by these techniques. We evaluate only the communication aspect of our prototypes and consider fully exploring their security an... | {'timestamp': '2016-07-19T02:00:40', 'yymm': '1607', 'arxiv_id': '1607.04663', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04663'} | arxiv | |
\section{Introduction}
The rapid growth of mobile wireless applications and consumers
continues to strain the limited cellular network capacity and has motivated the exploration of next generation 5G wireless networks.
The mobile industry predicts a $1000$x data
traffic growth by 2020. To meet this anticipated da... | {'timestamp': '2016-07-19T02:03:41', 'yymm': '1607', 'arxiv_id': '1607.04729', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04729'} | arxiv | |
\section{Introduction}\label{sec-intro}
In this paper we introduce a new higher categorical structure, called a weakly globular Tamsamani $n$-category and we prove its equivalence with a simpler higher categorical structure introduced by the author in \cite{Pa2}, called a weakly globular $n$-fold category.
Higher... | {'timestamp': '2016-09-15T02:01:06', 'yymm': '1607', 'arxiv_id': '1607.04870', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04870'} | arxiv | |
\section{INTRODUCTION}
\label{sec:intro}
A period of accelerated exponential expansion in the early Universe,
while a radical extrapolation from understood physics, naturally
solves the flatness, horizon, and monopole problems of standard
cosmology\cite{planck_p15xx_15}. This inflationary period also
explains the or... | {'timestamp': '2016-07-18T02:08:19', 'yymm': '1607', 'arxiv_id': '1607.04567', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04567'} | arxiv | |
\section{Introduction}\label{secIntr}
Understanding the nature and structure of the excited states of the
nucleon is a key contemporary problem in QCD. The Roper resonance,
$N^*(1440)$, was first deduced from the analysis of $\pi N$ phase shifts
in 1963 \cite{Roper1964}. However, its structure and nature have
aroused... | {'timestamp': '2017-02-16T02:04:50', 'yymm': '1607', 'arxiv_id': '1607.04536', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04536'} | arxiv | |
\section{Introduction and results} \label{sec:Intro}
Consider an $n$-variate polynomial of degree at most $d$:
\[ p=\sum_{|\alpha| \le d} c_{\alpha} x^{\alpha} \]
where $x:=(x_1,\ldots,x_n)$, $\alpha \in \ZZ_{\ge 0}^n$,
$|\alpha|:=\sum_i \alpha_i$, $x^{\alpha}:=\prod_i x_i^{\alpha_i}$,
and where each coefficient $... | {'timestamp': '2016-07-19T02:07:22', 'yymm': '1607', 'arxiv_id': '1607.04873', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04873'} | arxiv | |
\section{Introduction}
The dynamics of electrolytic solutions is essential in the description of most most processes in (bio)chemistry and soft matter physics.
This includes electrostatic screening via the formation of double layers, electro-osmotic flow\cite{anderson89a,paxton06a,ibele07a,reinmuller12a}, electrophore... | {'timestamp': '2016-11-23T02:05:55', 'yymm': '1607', 'arxiv_id': '1607.04572', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04572'} | arxiv | |
\section{Introduction}
Unless stated otherwise, the graphs considered in this paper are simple, loopless and finite. A \emph{homomorphism} $h$ of a graph $G$ to a graph $H$ is a mapping $h:V(G)\to V(H)$ such that adjacency is preserved by $h$, that is, the images of two adjacent vertices of $G$ must be adjacent in $H$.... | {'timestamp': '2018-01-31T02:06:13', 'yymm': '1607', 'arxiv_id': '1607.04777', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04777'} | arxiv | |
\section{Introduction}
A major goal of planetary exploration is to obtain a fundamental understanding
of planetary environments, both as they are currently and as they were in the past.
This knowledge
can be used to explore the questions of (a) how conditions for planetary habitability
arose and (b) the origins of li... | {'timestamp': '2016-09-09T02:00:35', 'yymm': '1607', 'arxiv_id': '1607.04687', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04687'} | arxiv | |
\section{Introduction}
The present paper concerns a time operator in quantum theory which is
defined, in a first stage of cognition, as a symmetric operator canonically conjugate to a Hamiltonian if it exists.
The uncertainty relation which is derived from the canonical commutation relation of a time operator and... | {'timestamp': '2017-03-29T02:05:32', 'yymm': '1607', 'arxiv_id': '1607.04702', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04702'} | arxiv | |
\section{Introduction}
Since 1981, inferring the main excitation sources of galaxies generally relies on diagrams involving emission line ratios \citep*{Baldwin1981,Veilleux1987}, the most widely used diagram being $\ifmmode [\text{O}\,\textsc{iii}] \else [O~{\scshape iii}]\fi\xspace/\ifmmode \text{H}\beta \else H$\be... | {'timestamp': '2016-07-18T02:09:05', 'yymm': '1607', 'arxiv_id': '1607.04601', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04601'} | arxiv | |
\section{Introduction}\label{se:intro}
In this paper, we consider mixed integer minimization problem as follows:
\begin{equation}\label{p:primal}
(\mathcal{P}_b):~~~~\min \{P(x,v)= Q(x)+W(x)-f^Tv~|~(x,v)\in \x_v\}
\end{equation}
where $Q(x)=\frac{1}{2}x^T A x-c^Tx$, $W(x)= \frac{1}{2}\lpa\frac{1}{2}x^T B x-\... | {'timestamp': '2016-07-19T02:04:39', 'yymm': '1607', 'arxiv_id': '1607.04748', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04748'} | arxiv | |
\subsection{LSTM Equations}
\input{lstm_equations}
\subsection{Parameter reduction}
\label{subsec:am_parameter_reduction}
In order to reduce memory consumption and computation, we compress the previously described acoustic model using projection layers that sit between the outputs of an LSTM layer and both the recurr... | {'timestamp': '2016-12-20T02:01:13', 'yymm': '1607', 'arxiv_id': '1607.04683', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04683'} | arxiv | |
\section{Introduction}
\IEEEPARstart
{T}{he} latest advantages in deep learning technologies has led to explosive growth in machine learning and computer vision for building systems that have shown significant improvements in a huge range of applications such as image classification \cite{krizhevsky2012imagenet}, \cite... | {'timestamp': '2016-07-20T02:11:16', 'yymm': '1607', 'arxiv_id': '1607.04889', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04889'} | arxiv | |
\section{Introduction}
Multifractal analysis is the study of the concentration of a measure on level sets. In particular, we use measures for a hyperbolic map to study the multifractal spectrum. Multifractal analysts historically modeled an expanding map with a finite state shift. Their main result is the expressio... | {'timestamp': '2016-07-19T02:05:17', 'yymm': '1607', 'arxiv_id': '1607.04786', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04786'} | arxiv | |
\section{Introduction}
Modified gravity theories may provide an attractive alternative to the standard explanations of the present day observations that have shaken the well-established foundations of the theoretical physics. Astronomical observations have confirmed that our Universe does not according to standard ... | {'timestamp': '2016-07-19T02:07:23', 'yymm': '1607', 'arxiv_id': '1607.04874', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04874'} | arxiv | |
\section{Stronger Hypotheses}\label{sec_StrongerHypotheses}
In this section we shall prove Theorems \ref{thm_MainTheorem_two},\ref{thm_MainTheorem_three} and \ref{thm_MainTheorem_four}. Let us start with Theorem \ref{thm_MainTheorem_two}. Let $l$,$m$,$\<S_n : n > m + 1\>$, $\<n_k: k < \omega\>$ be as in its statemen... | {'timestamp': '2016-07-19T02:05:21', 'yymm': '1607', 'arxiv_id': '1607.04790', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04790'} | arxiv | |
\section{Conclusion}
\label{sec:conclusion}
We have described \sys, a system for proving equivalence of SQL
rewrite rules. In support of \sys, we defined a formal language \sem,
following closely SQL's syntax. Our semantics extends that of SQL
from finite relations to infinite relations, and uses univalent types
fr... | {'timestamp': '2016-08-09T02:00:58', 'yymm': '1607', 'arxiv_id': '1607.04822', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04822'} | arxiv | |
\section{Introduction}
\paragraph{\bf Hard lattice problems.} Lattices are discrete subgroups of $\mathbb{R}^d$. More concretely, given a basis $B = \{\vc{b}_1, \dots, \vc{b}_d\} \subset \mathbb{R}^d$, the lattice $\mathcal{L} = \mathcal{L}(B)$ generated by $B$ is defined as $\mathcal{L}(B) = \left\{\sum_{i=1}^d \lamb... | {'timestamp': '2016-07-19T02:05:21', 'yymm': '1607', 'arxiv_id': '1607.04789', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04789'} | arxiv | |
\section{Introduction}
Exciton mediated many-body interactions give rise to a host of physical effects \cite{qiu2016screening,sahin2016computing,cudazzo2016exciton}
that determine the opto-electronic properties
of low dimensional transition metal dichalcogenides, MX$_2$
(M = Mo, W, Nb and X = S, Se) \cite{sc... | {'timestamp': '2016-09-22T02:02:41', 'yymm': '1607', 'arxiv_id': '1607.04856', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04856'} | arxiv | |
\section{A letter from Saratov} \label{story}
During his last trip to Moscow, the second author of this article came into possession of a remarkable mathematical letter. The custodian of the letter, a Russian businessman X who wished to remain anonymous,
presented the letter to Tabachnikov at the end of his lecture o... | {'timestamp': '2016-07-19T02:04:54', 'yymm': '1607', 'arxiv_id': '1607.04766', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04766'} | arxiv | |
\section{Introduction}
\label{sec:intro}
\begin{figure}
\begin{center}
\begin{tabular}{c}
\includegraphics[width=10cm]{img/AGN_spectra.pdf}
\end{tabular}
\end{center}
\caption{\label{fig:sy1_2} A spectrum of a Seyfert 1 galaxy (blue) and a Seyfert 2 galaxy (red) taken with the VLT/X-SHOOTER instrument as pa... | {'timestamp': '2016-07-18T02:07:39', 'yymm': '1607', 'arxiv_id': '1607.04533', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04533'} | arxiv | |
\section{Introduction}
The idea of optimally controlling the dynamical behavior of microsystems described by quantum mechanics has been an explicit dream for more than $50$ years \cite{Warren1993}. Among all the approaches to solving the resulting optimization problems, model-based optimal control relies on computer s... | {'timestamp': '2016-07-19T02:02:25', 'yymm': '1607', 'arxiv_id': '1607.04694', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04694'} | arxiv | |
\section{Introduction}\label{SEC:intro}
Let $p$ be a prime and let $G$ be a torsion-free abelian group.
The subject of this work is the group $Hom (G,\mathbb{Z}_p)$ of $p$-adic functionals on $G$.
This group is viewed as a $p$-adic dual of $G$, and is studied using the techniques of functional analysis.
This is... | {'timestamp': '2016-08-10T02:06:59', 'yymm': '1607', 'arxiv_id': '1607.04586', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04586'} | arxiv | |
\section{Introduction}\label{sec1}
Let $\mathbb{Z}$ be a finite dimensional vector space, and $\mathbb{R}^{m\times n}$ be
the vector space of all $m\!\times\!n$ real matrices equipped with the trace inner product
$\langle \cdot,\cdot\rangle$ and its induced norm $\|\cdot\|_F$. Denote by $\|X\|_*$
the nucl... | {'timestamp': '2017-01-23T02:03:03', 'yymm': '1607', 'arxiv_id': '1607.04826', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04826'} | arxiv | |
\section{Introduction}
Nowadays, millions of videos are being uploaded to the Internet every day. These videos capture all aspects of multimedia content about their uploader's daily life. These explosively growing user generated content videos online are becoming an crucial source of video data. Automatically categori... | {'timestamp': '2016-07-19T02:05:10', 'yymm': '1607', 'arxiv_id': '1607.04780', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04780'} | arxiv | |
\section*{Introduction}
The minimum energy required to reset one bit of information represents one of the fundamental limits of computation arising when one bit of information is erased or destroyed. Starting with a system encoding two possible states with the same probability and finishing the procedure with only one ... | {'timestamp': '2016-09-08T02:03:32', 'yymm': '1607', 'arxiv_id': '1607.04802', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04802'} | arxiv | |
\section{Introduction} \label{sec-intro}
In this paper we study sublanguages of Plotkin's functional programming language ${\mathrm{PCF}}$,
which we here take to be the simply typed $\lambda$-calculus over a single base type $\nat$,
with constants
\[ \begin{array}{rlcrl}
\num{n} & : \nat \mbox{~~for each $n \in \mat... | {'timestamp': '2018-06-20T02:09:57', 'yymm': '1607', 'arxiv_id': '1607.04611', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04611'} | arxiv | |
\section{Introduction}
In the conference, I talked about
the Hodge theoretic aspect of injectivity and
vanishing theorems (see \cite{fujino1}, \cite{fujino2},
and \cite{fujino3}).
Here, I will explain some analytic generalizations.
In \cite{fujino-matsumura}, Shin-ichi Matsumura and I
established the
following ... | {'timestamp': '2016-07-19T02:02:10', 'yymm': '1607', 'arxiv_id': '1607.04684', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04684'} | arxiv | |
\section{Introduction}
In this note, we study the area of a minimal submanifold in the unit ball in $\mathbb{R}^n$. For a minimal submanifold $\Sigma$ that passes through the center of the ball, it is well-known that the area of $\Sigma$ is bounded from below by the area of a flat $k$-dimensional disk:
\begin{theor... | {'timestamp': '2017-01-30T02:05:13', 'yymm': '1607', 'arxiv_id': '1607.04631', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04631'} | arxiv | |
\section{Introduction}
In this paper we study bounds for the density of a diffusion process at a small time under a local strong H\"ormander condition. To be more precise, let $X$ denote the process in ${\mathbb R}^n$ solution to
\be{equation-intro}
dX_{t}=\sum_{j=1}^{d}\sigma
_{j}(t,X_{t})\circ dW_{t}^{j}+b(t,X_{t})dt... | {'timestamp': '2016-07-19T02:12:54', 'yymm': '1607', 'arxiv_id': '1607.04542', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04542'} | arxiv | |
\section{Introduction}
Models of the nonlinear Schr{\"o}dinger (NLS)
type~\cite{sulem,ablowitz,siambook}
have proven to be rather universal in describing envelope
nonlinear wave structures in dispersive media. Such
structures emerge in fields ranging from water waves
and
nonlinear optics~\cite{kivshar} to plasmas~\ci... | {'timestamp': '2016-07-18T02:09:01', 'yymm': '1607', 'arxiv_id': '1607.04598', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04598'} | arxiv | |
\section{Introduction}
\subsection{Bloch functions} Let $\D$ be the unit disk in the complex plane and $\vp$ an analytic function defined in $\D$. We say that $\vp$ is a \emph{Bloch function} if
\be \label{Bloch}
\beta(\vp) = \sup_{z\in\D}(1-|z|^2)|\varphi'(z)|<\infty.
\ee
This defines a seminorm, and the Banach... | {'timestamp': '2016-12-26T02:05:25', 'yymm': '1607', 'arxiv_id': '1607.04626', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04626'} | arxiv | |
\section{Introduction}
\label{sec:intro}
As a key part of the human visual system, visual attention mechanisms filter irrelevant visual stimuli in order to focus more on the important parts. Computational models of attention try to mimic this process through the use of machines and algorithms. These models have gained... | {'timestamp': '2017-11-16T02:04:49', 'yymm': '1607', 'arxiv_id': '1607.04730', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04730'} | arxiv | |
\section{\label{sec:level1}First-level heading:\protect\\ The line
Tunnel field-effect transistor (TFET), a promising replacement of classical metal-oxide-semiconductor field-effect transistor (MOSFET) for future low-power integrated circuits, has been intensively studied over a decade. The advantages of TFET come fro... | {'timestamp': '2016-07-19T02:08:06', 'yymm': '1607', 'arxiv_id': '1607.04896', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04896'} | arxiv | |
\section{INTRODUCTION}
In recent years deep learning methods have demonstrated significant improvements in various tasks. These methods outperform human-level object detection in some tasks \cite{resnet}, and achieve state-of-the-art results in machine translation \cite{nmt} and speech processing \cite{graves2013speech... | {'timestamp': '2016-10-03T02:05:04', 'yymm': '1607', 'arxiv_id': '1607.04793', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04793'} | arxiv | |
\section{Introduction}\label{sec:intro}
Microquasars are X-ray binaries that exhibit spatially resolved, extended radio emission. The nomenclature is motivated by a structural similarity with the quasar family of active galactic nuclei (AGN). Both object classes are believed to comprise a compact central object embedd... | {'timestamp': '2016-07-19T02:10:20', 'yymm': '1607', 'arxiv_id': '1607.04613', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04613'} | arxiv | |
\section{Introduction}
Human Activity Recognition (HAR) is the understanding of human behaviour from data captured by pervasive sensors, such as cameras or wearable devices. It is a powerful tool in medical application areas, where consistent and continuous patient monitoring can be insightful. Wearable devices provide... | {'timestamp': '2016-07-20T02:06:21', 'yymm': '1607', 'arxiv_id': '1607.04867', 'language': 'en', 'url': 'https://arxiv.org/abs/1607.04867'} | arxiv |
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