text stringlengths 1 2.34M | meta dict |
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\section{Introduction} \label{sec:intro}
Blazars are the subclass of radio-loud active galactic nuclei (AGNs) with their relativistic jet pointing toward us \citep{urry}.
Multi-wavelength radiations covering from MHz, optical to TeV gamma-ray energies have been observed from blazars.
Blazar emission is dominated by ... | {
"timestamp": "2018-09-26T02:12:04",
"yymm": "1804",
"arxiv_id": "1804.05342",
"language": "en",
"url": "https://arxiv.org/abs/1804.05342"
} |
\section{Introduction\label{Introduction}}
The implied volatility index VIX was created in order to estimate, looking forward, the expected realized volatility. CBOE introduced the original VIX (now VXO) in 1986. It was based on an inverted Black-Scholes formula, where S\&P 100 near-term, at-the-money options were used... | {
"timestamp": "2018-04-17T02:08:48",
"yymm": "1804",
"arxiv_id": "1804.05279",
"language": "en",
"url": "https://arxiv.org/abs/1804.05279"
} |
\section{Introduction}
\label{introduction}
Computational models that distinguish between semantic similarity and
semantic relatedness \citep{Budanitsky/Hirst:06} are important for
many NLP applications, such as the automatic generation of
dictionaries, thesauri, and
ontologies~\cite{Biemann:05,Cimiano:05,Li:06}, and ... | {
"timestamp": "2018-04-20T02:07:22",
"yymm": "1804",
"arxiv_id": "1804.05388",
"language": "en",
"url": "https://arxiv.org/abs/1804.05388"
} |
\section{Introduction}
Video captioning, the task of automatically generating a natural-language description of a video, is a crucial challenge in both NLP and vision communities. In addition to visual features, audio features can also play a key role in video captioning. \autoref{fig:intro} shows an example where th... | {
"timestamp": "2018-04-17T02:12:20",
"yymm": "1804",
"arxiv_id": "1804.05448",
"language": "en",
"url": "https://arxiv.org/abs/1804.05448"
} |
\section{Introduction}
Link traversal is a usual practice for web page surfing. Extending such functionality for exploratory browsing of videos remains a new problem. Video hyperlinking, a new task initiated by \cite{Trecvid2016,14_MediaEval,over2015trecvid}, aims to enhance the accessibility of large video dataset by ... | {
"timestamp": "2018-04-17T02:08:58",
"yymm": "1804",
"arxiv_id": "1804.05286",
"language": "en",
"url": "https://arxiv.org/abs/1804.05286"
} |
\section{Introduction}\label{sec:intro}
The \emph{counting} of self-avoiding walks (SAWs) is extended here to the study of
\emph{weighted} SAWs. Each edge is assigned a weight, and the weight of a SAW
is defined as the product of the weights of its edges.
We study certain properties of the exponential growth r... | {
"timestamp": "2019-06-06T02:13:40",
"yymm": "1804",
"arxiv_id": "1804.05380",
"language": "en",
"url": "https://arxiv.org/abs/1804.05380"
} |
\section*{References}}
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\newcommand{{\mathrm{lcm}}}{{\mathrm{lcm}}}
\newcommand{{\mathrm{Tr}}}{{\mathrm{Tr}}}
\newcommand{{\mathrm{Tr}}}{{\mathrm{Tr}}}
\newcommand{{\mathrm{N}}}{{\mathrm{N}... | {
"timestamp": "2018-04-17T02:13:52",
"yymm": "1804",
"arxiv_id": "1804.05516",
"language": "en",
"url": "https://arxiv.org/abs/1804.05516"
} |
\section{Introduction}
\label{sect:intro}
We have catalogued the information about 57 double-lined spectroscopic binary T Tauri stars with known orbital elements (\citealt{Dudorov+Eretnova+2016, Dudorov+Eretnova+2017}). There are 14 systems among of them with well determined masses and radii. It is possible t... | {
"timestamp": "2018-04-17T02:09:46",
"yymm": "1804",
"arxiv_id": "1804.05315",
"language": "en",
"url": "https://arxiv.org/abs/1804.05315"
} |
\section{Introduction}\label{sec-intro}
Since the seminal work of Maldacena in 1997~\cite{Maldacena:1997re}, holography
has came to become one of the cornerstones of twenty-first century high energy
physics. The so called ``AdS/CFT duality'' has found a multitude of applications in
condensed matter physics, as it prov... | {
"timestamp": "2018-07-05T02:06:44",
"yymm": "1804",
"arxiv_id": "1804.05202",
"language": "en",
"url": "https://arxiv.org/abs/1804.05202"
} |
\subsubsection*{#1}}
\pagestyle{headings}
\markright{Reference sheet: \texttt{natbib}}
\usepackage{shortvrb}
\MakeShortVerb{\|}
\begin{document}
\thispagestyle{plain}
\newcommand{\textsc{Bib}\TeX}{\textsc{Bib}\TeX}
\newcommand{\texttt{#1}\def\filedate{#2}\def\fileversion{#3}}}{\texttt{#1}\def\filedate{#2}\def\filev... | {
"timestamp": "2018-04-17T02:14:31",
"yymm": "1804",
"arxiv_id": "1804.05551",
"language": "en",
"url": "https://arxiv.org/abs/1804.05551"
} |
\section{Introduction}
In recent years a lot of insight has been gained by trying to understand the landscape of supersymmetric quantum field theories and especially superconformal field theories (SCFTs). Even though much progress has been made towards understanding the properties of $\mathcal{N} = 1,2,4$ theories, i... | {
"timestamp": "2018-04-17T02:11:31",
"yymm": "1804",
"arxiv_id": "1804.05396",
"language": "en",
"url": "https://arxiv.org/abs/1804.05396"
} |
\section{Introduction}
\setcounter{equation}{0}
In this paper we consider realization results for operator-valued functions analytic in the neighborhood of the origin in two cases: the complex number setting and the quaternionic
setting. Recently, the authors proved realization theorems for functions associated to Pon... | {
"timestamp": "2018-04-17T02:07:52",
"yymm": "1804",
"arxiv_id": "1804.05255",
"language": "en",
"url": "https://arxiv.org/abs/1804.05255"
} |
\section{Introduction}\label{sec:introduction}
\renewcommand{\baselinestretch}{0.94}\normalsize
\emph{Mutually Uncorrelated} (\emph{MU}) codes satisfy the constraint in which the prefixes set and suffixes set of all codewords are disjoint. This class of codes was first studied by Levenshtein~\cite{L64} for the purpose ... | {
"timestamp": "2018-04-17T02:11:01",
"yymm": "1804",
"arxiv_id": "1804.05371",
"language": "en",
"url": "https://arxiv.org/abs/1804.05371"
} |
\section{#1}\setcounter{equation}{0}}
\renewcommand{\theequation}{\thesection.\arabic{equation}}
\newdimen\tableauside\tableauside=1.0ex
\newdimen\tableaurule\tableaurule=0.4pt
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\def\phantomhrule#1{\hbox{\vbox to0pt{\hrule height\tableaurule width#1\vss}}}
\def\phantomvrule#1{\vbox{\hbox to0pt{\vr... | {
"timestamp": "2018-11-29T02:14:55",
"yymm": "1804",
"arxiv_id": "1804.05574",
"language": "en",
"url": "https://arxiv.org/abs/1804.05574"
} |
\section{Introduction} \label{section1}
In this paper we study the phase separation of $n$-dimensional $\infty$ \!\!-\!\! Harmonic mappings $ u\!:\! \mathbb{R}^n \supseteq \Omega \longrightarrow \mathbb{R}^{N}$ by which we mean the classical solutions to the $\infty$-\!Laplace system
\begin{equation}}\newcommand{\... | {
"timestamp": "2018-04-17T02:12:41",
"yymm": "1804",
"arxiv_id": "1804.05466",
"language": "en",
"url": "https://arxiv.org/abs/1804.05466"
} |
\section{Introduction}
The Universe is expanding, driving galaxies further and further apart from each other. Locally, this effect is described by the Hubble Law, which linearly relates the distance and redshift of galaxies. However, on top of the `cosmological expansion' or `Hubble Flow', additional velocity compone... | {
"timestamp": "2018-05-22T02:15:34",
"yymm": "1804",
"arxiv_id": "1804.05520",
"language": "en",
"url": "https://arxiv.org/abs/1804.05520"
} |
\section{Introduction}\label{sec:intro}
Crowdsourcing is a popular method for collecting data but the collected data is often noisy and of low quality. The quality gets significantly degraded if solving the tasks require some costly effort. The problem can be addressed by rewarding the workers with a performance based ... | {
"timestamp": "2018-11-16T02:04:14",
"yymm": "1804",
"arxiv_id": "1804.05560",
"language": "en",
"url": "https://arxiv.org/abs/1804.05560"
} |
\section{Coefficients in the $p\mu$-model}\label{sec:coeff_pmu}
The coefficients in the $p\mu$-model are given by
\begin{gather*}
\mcl P_p^{p\mu} = \tfrac{\alpha\gas\alpha\liq \kappa_\mu}{\rho\gas c\gas^2 \rho\liq c\liq^2 \kappa_{p\mu}}, \quad
\mcl G_p^{p\mu} = \tfrac{1}{\kappa_{p\mu}} \left[ \tfrac{\alpha\gas}{\r... | {
"timestamp": "2018-04-17T02:07:15",
"yymm": "1804",
"arxiv_id": "1804.05241",
"language": "en",
"url": "https://arxiv.org/abs/1804.05241"
} |
\section{Introduction}
\label{sec:introduction}
Interstellar dust grains account for $\simeq$1\% of the mass of the interstellar medium (ISM). They are involved in different important processes such as photo-electric heating of the neutral interstellar gas, cooling in dense star-forming regions and the formation of ... | {
"timestamp": "2019-01-08T02:26:32",
"yymm": "1804",
"arxiv_id": "1804.05645",
"language": "en",
"url": "https://arxiv.org/abs/1804.05645"
} |
\section{Introduction}
The dynamics around the scission point is crucial to understand
many aspects of the fission final state, including for example
the kinetic energy distributions of the fragment and the
odd-even effects in mass distributions. At present \cite{sc16}, the
leading tool for microscopic fissio... | {
"timestamp": "2018-04-17T02:11:44",
"yymm": "1804",
"arxiv_id": "1804.05410",
"language": "en",
"url": "https://arxiv.org/abs/1804.05410"
} |
\section{Introduction}
Consider the following statement about the provenance of a piece of data $A$:
\begin{displayquote}
$A$ was generated using linear regression on $B$ and stored in file $C$ yesterday.
\end{displayquote}
Provenance capture as it pertains to information, in this case $A$, is the process of collec... | {
"timestamp": "2018-04-17T02:11:31",
"yymm": "1804",
"arxiv_id": "1804.05395",
"language": "en",
"url": "https://arxiv.org/abs/1804.05395"
} |
\section*{Acknowledgements}
We would like to acknowledge Jes\'us Mart\'inez-Mateo for providing the error correction code and Charles Ci Wen Lim for useful discussions.
We thank the Swiss NCCR QSIT and Davide Rusca thanks the EUs H2020 programme under the Marie Sk\l{}odowska-Curie project QCALL (GA 675662) for financi... | {
"timestamp": "2018-04-17T02:11:56",
"yymm": "1804",
"arxiv_id": "1804.05426",
"language": "en",
"url": "https://arxiv.org/abs/1804.05426"
} |
\section{Foreword} \label{sec-foreword}
\section{Introduction} \label{sec-intro}
\begin{figure*
\begin{center}
\includegraphics[width=0.85\textwidth,viewport=12 258 581 831]{figure1_structure.pdf}
\caption{(Color online) The crystal and magnetic structure of PdCrO$_2$. (a) the crystal structure showing ... | {
"timestamp": "2018-04-17T02:14:56",
"yymm": "1804",
"arxiv_id": "1804.05573",
"language": "en",
"url": "https://arxiv.org/abs/1804.05573"
} |
\subsection{Estimates of the constant of the best Diophantine approximations}
The results described above lead us to the following estimates $ C_{n,s} $
$$
\bgroup
\def1.5{1.5}
\begin{array}{lcl}
C_3 \geq & \cfrac { 2 } { 5 \sqrt{11} } & \approx 0.120605... \\
C_4 \geq & \cfrac { 16 } { 9 \... | {
"timestamp": "2019-04-10T02:19:29",
"yymm": "1804",
"arxiv_id": "1804.05385",
"language": "en",
"url": "https://arxiv.org/abs/1804.05385"
} |
\section*{Introduction}
Probability density estimation for high dimensional data is difficult. Kernel density estimation (KDE) for approximating probability density function (PDF) is a commonly used non-parametric technique which has been studied both empirically and theoretically. However, this technique usually has... | {
"timestamp": "2018-04-17T02:09:47",
"yymm": "1804",
"arxiv_id": "1804.05316",
"language": "en",
"url": "https://arxiv.org/abs/1804.05316"
} |
\section*{Abstract}
A transfunction is a function which maps between sets of finite measures on measurable spaces (see \cite{Mikusinski}).
Push-forward operators form one important class of examples of transfunctions and are identified with their respective measurable functions. In this regard, transfunctions are a g... | {
"timestamp": "2018-04-17T02:08:16",
"yymm": "1804",
"arxiv_id": "1804.05268",
"language": "en",
"url": "https://arxiv.org/abs/1804.05268"
} |
\section{Introduction} \label{sec:intro}
Many engineering problems and processes can be described by multi-dimensional surfaces that form the ``fitness" landscape of the solution \cite{Lee2011,Yang2010b,Moller2001,Do2011}.
A single point on the fitness landscape is obtained through evaluation of one n-dimensional sol... | {
"timestamp": "2018-04-17T02:12:03",
"yymm": "1804",
"arxiv_id": "1804.05429",
"language": "en",
"url": "https://arxiv.org/abs/1804.05429"
} |
\section{Introduction}
\label{intro}
The study of azimuthal anisotropy of final state hadrons is believed to be one of the important tools that can extract significant information regarding particle interactions in a hot and dense nuclear and/or partonic medium produced in high-energy heavy-ion collisions. Properties o... | {
"timestamp": "2018-04-17T02:14:53",
"yymm": "1804",
"arxiv_id": "1804.05570",
"language": "en",
"url": "https://arxiv.org/abs/1804.05570"
} |
\section{Introduction}
\label{sec-intro}
Birkhoff's Ergodic Theorem is one of the cornerstones of probability theory
and the theory of \dsy s. It states that if $T$ is a measure-preserving
transformation of
a \pr\ space $(\ps, \mu)$ and $f \in L^1(\ps, \mu)$, the
\emph{Birkhoff average}
\begin{equation} \label{ba-intr... | {
"timestamp": "2018-09-06T02:11:59",
"yymm": "1804",
"arxiv_id": "1804.05359",
"language": "en",
"url": "https://arxiv.org/abs/1804.05359"
} |
\section{Introduction}
Hybrid networks that integrate radio frequency (RF) and visible light communication (VLC) technologies have been proposed intensively in the recent years in order to achieve the end-user demands of both capacity and coverage, which are difficult to meet when either technology is operating solely.... | {
"timestamp": "2018-04-17T02:06:10",
"yymm": "1804",
"arxiv_id": "1804.05211",
"language": "en",
"url": "https://arxiv.org/abs/1804.05211"
} |
\section{Introduction}
The main results of the present paper are related to
the following inverse problem in noncommutative harmonic analysis:
To what extent a locally compact group is determined by its representation theory?
If $G$ is a locally compact group, then important information on its r... | {
"timestamp": "2019-09-05T02:13:57",
"yymm": "1804",
"arxiv_id": "1804.05562",
"language": "en",
"url": "https://arxiv.org/abs/1804.05562"
} |
\section{Proofs}
\begin{lemma}
Let $U \in \mathbb{R}^{2 \times 2}$ and let $C \in \mathbb{R}^{2 \times 2}$. Let additionally, U and C have similar rows (Row 1 == Row 2). Let $\beta_1 = 0$ and $\beta_2 = \beta_3 = 1$, for simplicity (though not obvious, these can be easily generalized). Then, $p_k^U$ is a direction for... | {
"timestamp": "2018-07-05T02:09:06",
"yymm": "1804",
"arxiv_id": "1804.05313",
"language": "en",
"url": "https://arxiv.org/abs/1804.05313"
} |
\section{Introduction}
Let $g,n\ge 0$ satisfy $2g-2+n > 0$. These notes will be concerned with certain classes in the Chow ring of the moduli space $\overline{\M}_{g,n}$ of stable curves of genus $g$ with $n$ marked points. All of our classes will be {\it tautological}; that is, they are contained in a certain subring ... | {
"timestamp": "2018-04-17T02:12:42",
"yymm": "1804",
"arxiv_id": "1804.05467",
"language": "en",
"url": "https://arxiv.org/abs/1804.05467"
} |
\section{Introduction}
Behavior of eigenvalues below the essential spectrum of standard
Schr\"odinger operators of the form $-\Delta +\varepsilon V$
defined on $L^2({\mathbb R}^n)$
is considerably studied so far. Here $V$ is a negative potential and $\varepsilon \geq 0$ is a parameter which is varied.
When $\va... | {
"timestamp": "2018-04-17T02:10:09",
"yymm": "1804",
"arxiv_id": "1804.05339",
"language": "en",
"url": "https://arxiv.org/abs/1804.05339"
} |
\section{\MakeUppercase{Introduction}}
In the parable of Simon's Ant \cite{simon1996sciences}, an ant follows a complex path along a beach on to reach its goal. The story shows how the interaction of simple rules and a complex environment result in complex behavior. But this relationship can be looked at in another wa... | {
"timestamp": "2018-04-17T02:11:42",
"yymm": "1804",
"arxiv_id": "1804.05409",
"language": "en",
"url": "https://arxiv.org/abs/1804.05409"
} |
\section{Introduction}
\label{sec:introduction}
Over several decades, the study of the critical behavior of many-body
systems has been mainly carried out through Monte Carlo simulations which
makes it one of the most important methods in statistical mechanics. At the
very beginning, to circumvent the critical slowing... | {
"timestamp": "2018-04-19T02:02:40",
"yymm": "1804",
"arxiv_id": "1804.05303",
"language": "en",
"url": "https://arxiv.org/abs/1804.05303"
} |
\section{Introduction and Basic Definitions}
There are numerous ways to represent real numbers. We may use, e.g., Cauchy sequences, Dedekind cuts, numerical base-10 expansions,
numerical base-2 expansions and continued fractions. If we work with full Turing computability, all these representations
yield the same clas... | {
"timestamp": "2020-03-30T02:12:35",
"yymm": "1804",
"arxiv_id": "1804.05330",
"language": "en",
"url": "https://arxiv.org/abs/1804.05330"
} |
\section{Introduction} \label{sec_intro}
This paper deals with the global Cauchy problem for systems of nonlinear
Schr\"odinger equations in two space dimensions. We consider systems of
the type
\begin{equation}\label{NLS}
\left\{
\begin{array}{l}
\op{L}_{m_{j}} u_{j} =F_j(u, \pa_x u), \quad t>0,\, x\in\R^2, ... | {
"timestamp": "2018-05-04T02:05:26",
"yymm": "1804",
"arxiv_id": "1804.05540",
"language": "en",
"url": "https://arxiv.org/abs/1804.05540"
} |
\section{Introduction}\label{intro}
A \textit{translating soliton} (\textit{translator} for short) is an oriented, connected smoothly immersed hypersurface $x:M^n \to \mathbb{R}^{n+1}$ on which its mean curvature vector $H$ satisfies
\begin{align*}
H=T^\perp,
\end{align*}
where $T \in \mathbb{R}^{n+1}$ is a fixed u... | {
"timestamp": "2018-10-09T02:05:09",
"yymm": "1804",
"arxiv_id": "1804.05463",
"language": "en",
"url": "https://arxiv.org/abs/1804.05463"
} |
\section{Introduction} \label{sec:sec1}
The Square Kilometre Array (SKA) will transform the field of pulsar astrophysics \citep{2015aska.confE..36K}, by allowing for the discovery of a large fraction of the radio pulsar population beaming towards Earth. One particular area of opportunity for advances in fundamental phy... | {
"timestamp": "2018-04-17T02:10:07",
"yymm": "1804",
"arxiv_id": "1804.05335",
"language": "en",
"url": "https://arxiv.org/abs/1804.05335"
} |
\section*{Introduction}
\indent
Perhaps that the main apparently embarrassing problem in differential geometry is the lack of an obvious notion of morphism. We argue that this is
not an well posed problem, that is, the definition of a `linear $G$-structure', for some Lie group $G$, as a faithful representation of ... | {
"timestamp": "2018-05-03T02:05:50",
"yymm": "1804",
"arxiv_id": "1804.05423",
"language": "en",
"url": "https://arxiv.org/abs/1804.05423"
} |
\section{Introduction}
The purpose of this paper is to solve an open problem about Depth of Boolean algebras, from \cite{MR3184760}. We refer to this monograph for a comprehensive account of Depth (and Length), and here we only spell out the pertinent definitions.
\begin{definition}
\label{lllplus}
$\Depth$ and... | {
"timestamp": "2018-04-17T02:09:29",
"yymm": "1804",
"arxiv_id": "1804.05304",
"language": "en",
"url": "https://arxiv.org/abs/1804.05304"
} |
\section{Introduction}
It is believed that
production of soft particles
in $AA$ collisions at RHIC and LHC energies occurs via formation
of the quark-gluon plasma (QGP) that
expands hydrodynamically as a near-ideal liquid \cite{Huov_hydro,Kodama_hydro}.
Hydrodynamic models have been successfully used for
descriptio... | {
"timestamp": "2018-04-17T02:11:36",
"yymm": "1804",
"arxiv_id": "1804.05405",
"language": "en",
"url": "https://arxiv.org/abs/1804.05405"
} |
\section*{Introduction}
\label{intro}
Ultrasound imaging is one of the most commonly used imaging modalities since it is inexpensive, safe and convenient. Ultrasound elastography estimates biomechanical properties of the tissue and can substantially improve the capabilities of ultrasound imaging in both diagnosis and ... | {
"timestamp": "2018-04-17T02:09:30",
"yymm": "1804",
"arxiv_id": "1804.05305",
"language": "en",
"url": "https://arxiv.org/abs/1804.05305"
} |
\section{Introduction}
\label{sec:introduction}
Given an input graph, the problem of finding a subgraph satisfying certain properties has diverse
applications. MAX CUT, MAX CLIQUE, TSP are a few canonical examples. Traditionally these problems have been studied in theoretical computer science from the worst-case perspe... | {
"timestamp": "2018-04-17T02:12:08",
"yymm": "1804",
"arxiv_id": "1804.05436",
"language": "en",
"url": "https://arxiv.org/abs/1804.05436"
} |
\chapter*{Remerciements}
Je remercie tout d'abord les rapporteurs, professeurs J. Keeling et W. Zwerger, d'avoir accept\'{e} de lire et de porter un oeil critique sur mon manuscrit. Je tiens aussi \`{a} remercier les autres membres du jury d'avoir accept\'{e} d'assister \`{a} ma soutenance.\\
La plus grande reconnai... | {
"timestamp": "2018-04-17T02:05:22",
"yymm": "1804",
"arxiv_id": "1804.05192",
"language": "en",
"url": "https://arxiv.org/abs/1804.05192"
} |
\section{\label{sec:level1}Introduction}
The Faraday effect is a well known dispersive phenomenon in which the plane of polarization of linearly polarized light is rotated while traversing a material placed in a magnetic field which is directed along the path of light propagation. Especially in recent years this circu... | {
"timestamp": "2019-02-25T02:02:05",
"yymm": "1804",
"arxiv_id": "1804.05642",
"language": "en",
"url": "https://arxiv.org/abs/1804.05642"
} |
\section{Introduction}
Recently, degenerate coupled Korteweg-de Vries equations for coupled multiplicity $l= 2, 3, 4$ have been considered for traveling wave solutions by G$\ddot{\rm u}$rses and Pekcan \cite{gurses2014traveling,asli}. The multi-system of Kaup-Boussinesq equations is
given by (see refs. \cite{antonowicz... | {
"timestamp": "2018-04-17T02:10:19",
"yymm": "1804",
"arxiv_id": "1804.05350",
"language": "en",
"url": "https://arxiv.org/abs/1804.05350"
} |
\section{Introduction}
\label{s:1}
The well-known explicit formula of Riemann--Von Mangoldt for the
number of primes up to $x$ ($\varrho = \beta + i \gamma$ denotes
non-trivial zeros of Riemann's zeta-function, $x > 2$, $T \leq
x$),
\begin{equation}
\psi(x) = \sum_{n \leq x} \Lambda(n) = x - \sum_{|\gamma| \leq
T} {x^\... | {
"timestamp": "2018-04-17T02:14:38",
"yymm": "1804",
"arxiv_id": "1804.05561",
"language": "en",
"url": "https://arxiv.org/abs/1804.05561"
} |
\section{Introduction}
For a given many body system,
it is not easy
to measure the quantum mechanical
correlations because of their infinitesimal sizes. In same cases for instance
like superconductivity, there exists strong correlations
and the pure
states persist even in the large number of the many body state. In ... | {
"timestamp": "2018-04-17T02:15:28",
"yymm": "1804",
"arxiv_id": "1804.05595",
"language": "en",
"url": "https://arxiv.org/abs/1804.05595"
} |
\section{Introduction}
Fractional Diffusion Equations (FDEs) are a generalization of the classical partial diffusion equations obtained by replacing a standard derivative with a fractional one.
In the last decade, FDEs have gained a lot of attention since they allow to model non-local behavior, e.g., enhanced diffu... | {
"timestamp": "2019-08-13T02:06:15",
"yymm": "1804",
"arxiv_id": "1804.05522",
"language": "en",
"url": "https://arxiv.org/abs/1804.05522"
} |
\section{Introduction}
Weyl's idea of gauge invariance \cite{x1} turned out to be a key
principle underlying the dynamical structure of all the fundamental physical
interactions. Following this idea and the subsequent works of Yang, Mills
and Utiyama \cite{x2}, Kibble and Sciama \cite{x3} formulated a new theory
of gr... | {
"timestamp": "2018-07-20T02:02:03",
"yymm": "1804",
"arxiv_id": "1804.05556",
"language": "en",
"url": "https://arxiv.org/abs/1804.05556"
} |
\section{Introduction}\label{sec:introduction}}
\else
\section{Introduction}
\label{sec:introduction}
\fi
\IEEEPARstart{T}{his} demo file is intended to serve as a ``starter file''
for IEEE Computer Society journal papers produced under \LaTeX\ using
IEEEtran.cls version 1.8b and later.
I wish you the best of succe... | {
"timestamp": "2019-02-20T02:03:09",
"yymm": "1804",
"arxiv_id": "1804.05515",
"language": "en",
"url": "https://arxiv.org/abs/1804.05515"
} |
\section{Introduction}
\emph{Rewriting Theory} \cite{Terese03} is a foundational theory of computing. Its
impact extends to both the theoretical side of computer science, and the development of programming languages. A clear example of both aspects is the paradigmatic term rewriting system, $\lambda$-calculus, wh... | {
"timestamp": "2020-03-04T02:04:55",
"yymm": "1804",
"arxiv_id": "1804.05578",
"language": "en",
"url": "https://arxiv.org/abs/1804.05578"
} |
\section{Introduction}
\label{intro}
During the last decades, there has been a large amount of research
on the electronic properties and electron transport in nanostructure
devices \cite{DevoretNature1992,TaruchaPRL1996,KouwenhovenScience1997,ReimannRMP2002}.
A tremendous progress has been made in this area and new exc... | {
"timestamp": "2018-12-17T02:10:08",
"yymm": "1804",
"arxiv_id": "1804.05528",
"language": "en",
"url": "https://arxiv.org/abs/1804.05528"
} |
\section{Introduction}
In a paper on spectral theory \cite{JSH}, J. Howland used the positive commutator of two bounded functions of the Heisenberg operators $P$ and $Q$, $ i[f(P), g(Q)]$, as a technical tool. Here $ P = -id/dx$ and $Q$ is multiplication by $x$ in $L^2({\mathbb{R}}} \newcommand{\Z}{{\mathbb{Z}})$. ... | {
"timestamp": "2018-04-17T02:06:52",
"yymm": "1804",
"arxiv_id": "1804.05227",
"language": "en",
"url": "https://arxiv.org/abs/1804.05227"
} |
\section{INTRODUCTION}
Planetary phase curves consist of four components: (1) reflection of starlight from the surface of the orbiting planet \citep{Jenkins03}; (2) the planet's thermal emission \citep{Charbonneau05}; (3) Doppler beaming caused by the orbital motion of the host star \citep{Loeb03}; and (4) ellipsoidal... | {
"timestamp": "2018-06-06T02:10:32",
"yymm": "1804",
"arxiv_id": "1804.05334",
"language": "en",
"url": "https://arxiv.org/abs/1804.05334"
} |
\section{Introduction}
\label{Sec1:Introduction}
Digital image is corrupted during acquisition, transmission and reception systems by different noises. The resultant noise due various sources in these situations can be modeled as additive Gaussian noise (AWGN). Thus the noisy image $y$ may be represented as follows:
\... | {
"timestamp": "2018-04-17T02:13:51",
"yymm": "1804",
"arxiv_id": "1804.05512",
"language": "en",
"url": "https://arxiv.org/abs/1804.05512"
} |
\section{Introduction}\label{introduction}
The research on exotic phases and the phase transitions has always been one of the central topics in statistical and condensed matter physics.\cite{Minnhagen} A typical example is the continuous $XY$ model on the square lattice, which has attracted much attention since Kos... | {
"timestamp": "2018-04-17T02:14:11",
"yymm": "1804",
"arxiv_id": "1804.05532",
"language": "en",
"url": "https://arxiv.org/abs/1804.05532"
} |
\section{Introduction}
Journey planning in schedule-based public transport is a most frequent problem nowadays and
journey planners (web or mobile applications) are abundant.
Given as input a timetable associated with a public transportation system, the \emph{journey planning}
problem asks for efficiently answering qu... | {
"timestamp": "2018-04-17T02:16:41",
"yymm": "1804",
"arxiv_id": "1804.05644",
"language": "en",
"url": "https://arxiv.org/abs/1804.05644"
} |
\section{Introduction}
The intense ongoing search for Majorana zero modes (MZMs) in solid states systems is motivated, in part, by the perspective of using them as a platform for fault-tolerant topological quantum computation \cite{Kitaev01,Kitaev03,Wilczek09,Stanescu2017}.
Several practical realizations of ``syntheti... | {
"timestamp": "2018-04-17T02:12:15",
"yymm": "1804",
"arxiv_id": "1804.05446",
"language": "en",
"url": "https://arxiv.org/abs/1804.05446"
} |
\section{The SDE $dX = I(X) \; dW.$}\label{app}
The aim in this appendix is to prove Theorem 1. Until further notice, we shall focus on the case $X_j(0) = 0$ for all $j$. To begin with, we present two results about any solution of the SDE \eqref{SDE0}
\begin{equation}
dX_j(t) = I_j(X(t))\, dW_t, \qquad X_j(0) = 0 \qua... | {
"timestamp": "2018-04-17T02:13:00",
"yymm": "1804",
"arxiv_id": "1804.05479",
"language": "en",
"url": "https://arxiv.org/abs/1804.05479"
} |
\subsection{Problem Statement}
We will first define the system model studied throughout this paper.
\begin{definition}[Control System]
$\ $ A state feedback control system $\Psi(X, U, f, \K)$ consists
of a plant, a controller over
$X \subseteq \reals^n$ and $U \subseteq \reals^m$.
\begin{compactenum}
\item $X \subsete... | {
"timestamp": "2019-06-06T02:06:00",
"yymm": "1804",
"arxiv_id": "1804.05285",
"language": "en",
"url": "https://arxiv.org/abs/1804.05285"
} |
\section{Introduction}
\bigskip The Bernoulli polynomials $B_n(z)$, are defined by the generating function \cite{comtet74}
\begin{equation}
\sum_{n=0}^{\infty} B_n(z)\,\frac{t^n}{n!}=\frac{t\, e^{zt}}{e^t-1}.
\end{equation}
When $z=0$, $B_n=B_n(0)$ are called the Bernoulli numbers. Graham et al. \cite[P. 560]{grah... | {
"timestamp": "2018-04-17T02:12:09",
"yymm": "1804",
"arxiv_id": "1804.05437",
"language": "en",
"url": "https://arxiv.org/abs/1804.05437"
} |
\section{Introduction}
The idea of algebraic deformation theory was introduced by M. Gerstenhaber \cite{G1, G2, G3, G4, G5}. He introduced deformation theory for associative algebras. His theory was extended to Lie algebras by A. Nijenhuis and R. Richardson \cite{NR1}, \cite{NR2}, \cite{NR3}. Let $k$ be a fixed field. ... | {
"timestamp": "2018-04-17T02:10:24",
"yymm": "1804",
"arxiv_id": "1804.05355",
"language": "en",
"url": "https://arxiv.org/abs/1804.05355"
} |
\section{Introduction}
Throughout this paper all groups are finite. Let $G$ be a group. The subgroups $X_{1},X_{2},...,X_{n}$, $n\geq 2$, form a \textit{covering} of $G$ if
\begin{equation*}
\bigcup_{i=1}^{n}X_{i}=G\,.
\end{equation*}%
A covering is said to be \textit{irredundant} if none of the subgroups can
be remo... | {
"timestamp": "2018-04-17T02:11:28",
"yymm": "1804",
"arxiv_id": "1804.05390",
"language": "en",
"url": "https://arxiv.org/abs/1804.05390"
} |
\section{Introduction}
Plasmonics aims to combine the advantages of nanometer scale electronics with the high operating frequency (terahertz and beyond) of photonics \cite{Ozbay2006pmp}.
A promising platform for plasmonics is graphene, which features high confinement, wide range of operating frequencies $\omega$, lon... | {
"timestamp": "2018-04-17T02:07:56",
"yymm": "1804",
"arxiv_id": "1804.05256",
"language": "en",
"url": "https://arxiv.org/abs/1804.05256"
} |
\section{A. 3-dimensional Langevin motion near a wall, with a potential \eq{V(x)}}
The 3-dimensional motion of a particle in a thermal bath, floating above a flat surface (blue curve). Here, \eq{x>0} is the distance between the particle and the surface.
The surface-single molecule potential
\eq{V(x)} is provi... | {
"timestamp": "2018-11-13T02:17:44",
"yymm": "1804",
"arxiv_id": "1804.05571",
"language": "en",
"url": "https://arxiv.org/abs/1804.05571"
} |
\section{Introduction}
\subsection{}\label{ss1.1}
Let $G$ be a complex connected semisimple group and $U$ a maximal unipotent subgroup
of $G$. The ring ${\mathscr{D}}(G/U)$ of algebraic differential
operators on $G/U$, has a rich structure which was analyzed in
\cite{BGG} and studied further more recently in
\cite{... | {
"timestamp": "2018-04-25T02:03:42",
"yymm": "1804",
"arxiv_id": "1804.05295",
"language": "en",
"url": "https://arxiv.org/abs/1804.05295"
} |
\section{Introduction}
In this paper we use entropy theory to study the spectral structure of probability-measure-preserving ({\pmp}) actions of general countable groups. We will use an extension of the classical Kolmogorov--{\sinai} entropy called Rokhlin entropy that was introduced by the author in 2014 \cite{S1} ... | {
"timestamp": "2018-04-17T02:08:23",
"yymm": "1804",
"arxiv_id": "1804.05270",
"language": "en",
"url": "https://arxiv.org/abs/1804.05270"
} |
\section{Introduction}
The well known Yamabe problem consists of finding a constant scalar curvature metric which is
pointwise conformal to a given metric $g$ on an $n$-dimensional ($n\ge3$) compact Riemannian
manifold $M$ without boundary. From a PDE\rq{}s point of view,
this is equivalent to finding a positive s... | {
"timestamp": "2018-04-17T02:14:38",
"yymm": "1804",
"arxiv_id": "1804.05559",
"language": "en",
"url": "https://arxiv.org/abs/1804.05559"
} |
\section{Introduction.}
\subsection{The Manifold Topology vs. Finer or Incomparable Topologies.}
In \cite{Heathcote}, the author supports that the manifold topology in a curved spacetime
is the best possible and most natural choice, against the class of topologies that was
suggested by Zeeman and G\"{o}bel (see... | {
"timestamp": "2018-11-19T02:01:17",
"yymm": "1804",
"arxiv_id": "1804.05419",
"language": "en",
"url": "https://arxiv.org/abs/1804.05419"
} |
\section{Numerical results}
\label{sec:numerics}
In this section we demonstrate that \eqref{eq:reg-mn} can be simulated
using an off-the-shelf, high-order method for hyperbolic
conservation laws.
Our simulations indicate that the results of \secref{acc} can be used to guide
the choice of the regularization paramete... | {
"timestamp": "2018-04-17T02:12:17",
"yymm": "1804",
"arxiv_id": "1804.05447",
"language": "en",
"url": "https://arxiv.org/abs/1804.05447"
} |
\section{Introduction}
Please follow the steps outlined below when submitting your manuscript to
the IEEE Computer Society Press. This style guide now has several
important modifications (for example, you are no longer warned against the
use of sticky tape to attach your artwork to the paper), so all authors
should r... | {
"timestamp": "2018-10-22T02:06:27",
"yymm": "1804",
"arxiv_id": "1804.05320",
"language": "en",
"url": "https://arxiv.org/abs/1804.05320"
} |
\section{Introduction} It is well known that the finite Laplace transform has been used as a tool for solving various problems
from different scientific area such as Engineering, Physics, Mathematics, to cite but a few, see for example
\cite{Dakto, Rutily, Debnath, Bertero, Ledermann}, some of these applications. To... | {
"timestamp": "2018-04-17T02:06:08",
"yymm": "1804",
"arxiv_id": "1804.05207",
"language": "en",
"url": "https://arxiv.org/abs/1804.05207"
} |
\section{Introduction}
It is well known that Rashba spin-orbit interaction in two-dimensional (2D)
electron systems appears due to asymmetry
in confining potentials on both sides of the corresponding
heterostructure.\cite{rashba60,bychkov84,nitta97,pfeffer99,koga02}
Such an interaction leads to various spin-orbit
rela... | {
"timestamp": "2018-04-17T02:10:22",
"yymm": "1804",
"arxiv_id": "1804.05353",
"language": "en",
"url": "https://arxiv.org/abs/1804.05353"
} |
\section{Introduction}
Over the last fifty years, topological defects behaving as solitary waves in non-linear scalar field theories, but never occurring in linear system, have been understood as the cornerstone in explaining the existence and the role of wall and/or brane structures in Condensed Matter \cite{Esch... | {
"timestamp": "2018-05-08T02:16:06",
"yymm": "1804",
"arxiv_id": "1804.05605",
"language": "en",
"url": "https://arxiv.org/abs/1804.05605"
} |
{
"timestamp": "2018-04-24T02:12:45",
"yymm": "1804",
"arxiv_id": "1804.05307",
"language": "en",
"url": "https://arxiv.org/abs/1804.05307"
} | |
\section{Introduction}
Three dimensional topologically nontrivial semimetals (nodal-point and nodal line semimetals) have attracted great attention recently \cite{Armitage18,Fang16,Kobayashi17}. Dirac and Weyl semimetals (DSM/WSM) contain isolated nodes with nontrivial topological properties in materials \cite{Armitag... | {
"timestamp": "2018-04-17T02:11:17",
"yymm": "1804",
"arxiv_id": "1804.05381",
"language": "en",
"url": "https://arxiv.org/abs/1804.05381"
} |
\section{Introduction}\label{sec:intro}
In recent years, IEEE 802.11-based WLANs, commonly known as Wi-Fi networks, have experienced a remarkable growth in terms of traffic consumption. According to \cite{index2015cisco}, in 2016 more traffic was offloaded from cellular networks onto Wi-Fi than remained on them. Moreo... | {
"timestamp": "2019-09-13T02:15:19",
"yymm": "1804",
"arxiv_id": "1804.05534",
"language": "en",
"url": "https://arxiv.org/abs/1804.05534"
} |
\section{Algorithm Description}
Quasiprobability strategies for classical simulation of quantum circuits represent density matrices as weighted sums of a fixed set of hermitian operators. Some examples include projectors onto stabilizer states \cite{bennink} and the phase-point operators of the qutrit discrete Wigner... | {
"timestamp": "2018-04-17T02:11:36",
"yymm": "1804",
"arxiv_id": "1804.05404",
"language": "en",
"url": "https://arxiv.org/abs/1804.05404"
} |
\section{Introduction}
After the discovery of the Higgs boson at the LHC
\cite{LHCHiggs}, the Higgs boson mass $M_h$ has
become a precision observable. Supersymmetric (SUSY) extensions of the
Standard Model are special because they allow to predict the Higgs
boson mass thanks to SUSY relations between the Higgs potent... | {
"timestamp": "2018-04-17T02:16:08",
"yymm": "1804",
"arxiv_id": "1804.05619",
"language": "en",
"url": "https://arxiv.org/abs/1804.05619"
} |
\section{\newpage\stdsection}
\usepgfplotslibrary{polar}
\usepgflibrary{shapes.geometric}
\usetikzlibrary{calc}
\pgfplotsset{compat=1.12}
\usepgfplotslibrary{fillbetween}
\usetikzlibrary{patterns}
\begin{document}
\maketitle
\newcommand{\an}[1]{\textcolor{blue}{#1}}
\newcommand{\ann}[1]{\textcolor{red}{#1}}
\begin... | {
"timestamp": "2018-04-17T02:12:55",
"yymm": "1804",
"arxiv_id": "1804.05474",
"language": "en",
"url": "https://arxiv.org/abs/1804.05474"
} |
\section{Introduction}\label{se1}
\setcounter{equation}{0}
Elastic scattering problems have received much attention from both the engineering and mathematical
communities due to their significant applications in diverse scientific areas such as
seismology, remote sensing, geophysics and nondestructive testing.
This p... | {
"timestamp": "2018-04-17T02:13:24",
"yymm": "1804",
"arxiv_id": "1804.05496",
"language": "en",
"url": "https://arxiv.org/abs/1804.05496"
} |
\section{Introduction}
Nonorthogonal multiple access (NOMA) is becoming one of the key enabling technologies for the fifth-generation (5G) wireless networks and the applications beyond, including the Internet of Things (IoT), and massive machine-type communications (MMTC) \cite{dai2015non,chen2018toward}. NOMA, through... | {
"timestamp": "2018-04-17T02:07:16",
"yymm": "1804",
"arxiv_id": "1804.05242",
"language": "en",
"url": "https://arxiv.org/abs/1804.05242"
} |
\section{Introduction}
The success of relativistic fluid dynamics in describing the evolution
of high-energy heavy-ion collisions~\cite{Heinz:2013th} and the existence
of very large magnetic fields in these collisions~\cite{Skokov:2009qp,Deng:2012pc,Tuchin:2013apa,Bzdak:2011yy} has
generated a lot of interest in obser... | {
"timestamp": "2018-10-16T02:13:51",
"yymm": "1804",
"arxiv_id": "1804.05210",
"language": "en",
"url": "https://arxiv.org/abs/1804.05210"
} |
\section{Introduction and objectives}
\label{sec:intro}
In a previous paper \citep{per15} we validated the Weather Research and Forecasting (WRF) Numerical Weather Prediction (NWP) model for the precipitable water vapour (PWV) at astronomical sites. We used high resolution radiosonde balloon data launched at Roque de... | {
"timestamp": "2018-04-17T02:05:42",
"yymm": "1804",
"arxiv_id": "1804.05200",
"language": "en",
"url": "https://arxiv.org/abs/1804.05200"
} |
\section{Introduction}
The heat kernel is one of the most widely used spectral functions in many areas of mathematics and physics \cite{vassilevich03}.
For instance, in the ambit of spectral geometry, the heat kernel provides an invaluable tool
for the analysis of the geometry of a Riemannian manifold \cite{gilkey95,... | {
"timestamp": "2018-04-17T02:11:39",
"yymm": "1804",
"arxiv_id": "1804.05407",
"language": "en",
"url": "https://arxiv.org/abs/1804.05407"
} |
\section{\label{sec:introduction} Introduction}
Capacitively coupled plasmas (CCPs) operated at radio frequencies (RFs) are powered by generators that are connected to the driven electrode via an external electrical circuit.\cite{lieberman_principles_2005,chabert_physics_2011} These circuits depend on the specific s... | {
"timestamp": "2018-04-17T02:16:28",
"yymm": "1804",
"arxiv_id": "1804.05638",
"language": "en",
"url": "https://arxiv.org/abs/1804.05638"
} |
\section{Introduction}
\label{ch:targeted}
Recently, there has been research interest in designing processes to detect and monitor animal species using unattended environmental recordings \cite{Ganchev_2017}. A key challenge in achieving this goal is interference from noise which can mask vocalisations of intere... | {
"timestamp": "2018-04-17T02:13:28",
"yymm": "1804",
"arxiv_id": "1804.05502",
"language": "en",
"url": "https://arxiv.org/abs/1804.05502"
} |
\section{Introduction}\label{section-introduction}
In this paper, we consider Schr\"odinger type-operator:
\[
H=H_0+V
\]
on $L^2(\mathbb{R}^d)$, $d\geq 1$.
The unperturbed operator $H_0$ has the form:
$H_0= p_0(D_x)$ on $\mathbb{R}^d$, where $D_x=-i\partial_x$
and $p_0$ is a real-valued smooth function. We suppose:... | {
"timestamp": "2020-03-20T01:06:17",
"yymm": "1804",
"arxiv_id": "1804.05488",
"language": "en",
"url": "https://arxiv.org/abs/1804.05488"
} |
\section{Introduction}\label{Sec:intro}
In \cite{L1} Lawson established two kinds of reflection principles for minimal surfaces in the three dimensional sphere $S^3$. Using one of them he constructed a family of embedded closed minimal surfaces in $S^3$. Moreover, the genus $g$ of such a surface can be any positive in... | {
"timestamp": "2018-07-06T02:05:42",
"yymm": "1804",
"arxiv_id": "1804.05421",
"language": "en",
"url": "https://arxiv.org/abs/1804.05421"
} |
\subsection{}}
\def{C_Q\sslash\Gm}{{C_Q\sslash{\mathbb{G}_m}}}
\newcommand{\mathbf{U}}{\mathbf{U}}
\newcommand{\mathbf{L}}{\mathbf{L}}
\newcommand{\mathbf{T}}{\mathbf{T}}
\def\mathbf{S}{\mathbf{S}}
\newcommand{\mathbf{k}}{\mathbf{k}}
\newcommand{{\mathbf m}}{\mathbf{m}}
\newcommand{\mathbf{n}}{\mathbf{n}}
\newcommand{... | {
"timestamp": "2018-04-17T02:09:42",
"yymm": "1804",
"arxiv_id": "1804.05310",
"language": "en",
"url": "https://arxiv.org/abs/1804.05310"
} |
\section{Introduction}
The term \textit{hybrid} refers to something that is a mixture of several other things and hence a \textit{hybrid fractal} is a fractal which is a mixture of other fractals; see Section~\ref{section:HF} for its precise definition. The present paper investigates several questions concerning the an... | {
"timestamp": "2018-04-17T02:12:05",
"yymm": "1804",
"arxiv_id": "1804.05434",
"language": "en",
"url": "https://arxiv.org/abs/1804.05434"
} |
\section{Introduction}
Let $k = \mathbb{F}_{q}$ be a finite field and let $F \in k[x_1, \ldots, x_n]$ denote a non-singular homogeneous polynomial of degree $3$. Moreover, let $X \subset \mathbb{P}_k^{n-1}$ be the smooth cubic hypersurface defined over $k$ by $F=0$. Let $C$ be a smooth projective curve over $k$. Then... | {
"timestamp": "2018-04-17T02:16:39",
"yymm": "1804",
"arxiv_id": "1804.05643",
"language": "en",
"url": "https://arxiv.org/abs/1804.05643"
} |
\section{Introduction}
\label{M}
The phase field approach has been widely used in models of multicomponent fluids to
avoid the mathematical difficulties related to the presence of sharp interfaces separating the fluid components. We consider a model of a binary
mixture of compressible viscous fluids proposed by A... | {
"timestamp": "2018-04-17T02:14:36",
"yymm": "1804",
"arxiv_id": "1804.05557",
"language": "en",
"url": "https://arxiv.org/abs/1804.05557"
} |
\section{Introduction}\label{sec:introduction}}
\section{Introduction}
Finding a suitable representation of high-dimensional and complex data for various tasks, such as clustering and topic modeling, is a fundamental challenge in many areas such as computer vision, machine learning, data mining, and medical image anal... | {
"timestamp": "2018-10-02T02:09:10",
"yymm": "1804",
"arxiv_id": "1804.05370",
"language": "en",
"url": "https://arxiv.org/abs/1804.05370"
} |
\section{Introduction
\vspace{-0.05in}
Intelligent transportation systems (ITSs) will be a major component of tomorrow's smart cities.
In essence, ITSs will provide a much safer and more coordinated traffic network
by using efficient traffic management approaches \cite{ferdowsi2017deep}.
One promising ITS service is t... | {
"timestamp": "2019-07-22T02:04:03",
"yymm": "1804",
"arxiv_id": "1804.05290",
"language": "en",
"url": "https://arxiv.org/abs/1804.05290"
} |
\section{Acknowledgement}
\label{sec.ack}
We wish to thank Professor Richard Stanley and an anonymous reviewer for helping us confirm the status of Theorem \ref{thm:generalization}.
\section{Algorithm for Finding a Bouquet}
\label{sec.alg}
In this section, we give an algorithm for finding a bouquet. Let $\Lc$
be a di... | {
"timestamp": "2019-09-16T02:07:00",
"yymm": "1804",
"arxiv_id": "1804.05537",
"language": "en",
"url": "https://arxiv.org/abs/1804.05537"
} |
\section{Introduction} \label{sec:intro}
Interstellar turbulence is supposed to be one of the most important factors to regulate star formation activities. Shocks induced by supersonic turbulence dramatically increase the density and temperature in the post-shock layer and promote the structure formation, such as dense... | {
"timestamp": "2018-07-25T02:06:46",
"yymm": "1804",
"arxiv_id": "1804.05603",
"language": "en",
"url": "https://arxiv.org/abs/1804.05603"
} |
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