text stringlengths 1 1.41M | meta dict |
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\section{Introduction}
The fading channel is a widely adopted time-varying model for real-world wireless communications. In this model, the channel gain changes over time satisfying a certain distribution, called the channel distribution information (CDI). In a block fading channel model, the channel gain is assumed t... | {
"timestamp": "2017-01-24T02:04:39",
"yymm": "1701",
"arxiv_id": "1701.06111",
"language": "en",
"url": "https://arxiv.org/abs/1701.06111"
} |
\section{Introduction}
The study of the mathematical properties of multiloop Feynman integrals
has received increasing attention in the last years both by
the physics and the mathematics communities.
The high precision reached by the experimental measurements
carried out at the LHC, in fact, requires on the theory si... | {
"timestamp": "2017-01-24T02:00:17",
"yymm": "1701",
"arxiv_id": "1701.05905",
"language": "en",
"url": "https://arxiv.org/abs/1701.05905"
} |
\section{Introduction} \label{sec1}
NGC 4051 is an archetypical narrow-line Seyfert 1 (NLS1) at $z=0.0023$ with a mass of $(1.7\pm0.5)\times10^6\,M_\odot$ \citep{den09}.
High-resolution X-ray spectroscopic observations have detected a lot of blueshifted absorption lines
in the X-ray energy spectra (see, e.g.~\citealt... | {
"timestamp": "2017-01-24T02:08:04",
"yymm": "1701",
"arxiv_id": "1701.06298",
"language": "en",
"url": "https://arxiv.org/abs/1701.06298"
} |
\section*{Introduction}
Quantum channels are the most general input-output transformations allowed by quantum mechanics. Physically, they play a central role in quantum information theory, where they represent the communication from a sender to a receiver (\cite{Watrous-book}), in quantum information processing (\cite{... | {
"timestamp": "2017-07-04T02:07:03",
"yymm": "1701",
"arxiv_id": "1701.06205",
"language": "en",
"url": "https://arxiv.org/abs/1701.06205"
} |
\section{Introduction}{\label{Introduction}}
It has been known that the nucleon is a bound state of three valence quarks since 1970s. Many nucleon resonances, referred as $N^*$, have been observed~\cite{Olive:2016xmw}, the properties of nucleon resonances are the important issues in hadron physics, and attract lots of ... | {
"timestamp": "2017-05-17T02:05:21",
"yymm": "1701",
"arxiv_id": "1701.06007",
"language": "en",
"url": "https://arxiv.org/abs/1701.06007"
} |
\section{Introduction}
Active galactic nuclei (AGN) are one of the most extreme astrophysical sources in the Universe. These are compact, extremely luminous and often most variable shortest observed frequencies. Perpendicular to the plane of the accretion material, magnetically driven and collimated relativistic pla... | {
"timestamp": "2017-01-24T02:05:41",
"yymm": "1701",
"arxiv_id": "1701.06173",
"language": "en",
"url": "https://arxiv.org/abs/1701.06173"
} |
\section{Introduction}
To a smooth function $\phi:\mathbb{R}^{n-1}\rightarrow\mathbb{R}$ we associate the \emph{Fourier extension operator}
$$
Eg(x)=\int_{\mathbb{R}^{n-1}}e^{i(x'\cdot\xi+x_n\phi(\xi))}g(\xi)d\xi;$$
here $x=(x',x_n)\in\mathbb{R}^{n-1}\times\mathbb{R}$, and a-priori $g\in L^1(\mathbb{R}^{n-1})$.
Th... | {
"timestamp": "2017-06-21T02:02:31",
"yymm": "1701",
"arxiv_id": "1701.06099",
"language": "en",
"url": "https://arxiv.org/abs/1701.06099"
} |
\section{Introduction}
When an electron current flows perpendicular to a magnetic field through a conducting medium, the charges are forced to deviate to one side creating an imbalance which results in a measurable electric potential conveying important information about the material. A device based on this, so-called ... | {
"timestamp": "2017-01-25T02:05:22",
"yymm": "1701",
"arxiv_id": "1701.06310",
"language": "en",
"url": "https://arxiv.org/abs/1701.06310"
} |
\section*{Introduction}
In \cite{Ha} B. Hassett introduced new compactifications $\overline{\mathcal{M}}_{g,A[n]}$ of the moduli stack $\mathcal{M}_{g,n}$ parametrizing smooth genus $g$ curves with $n$ marked points, where the notion of stability is defined in terms of a fixed vector of rational weights $A[n] = (a_{1}... | {
"timestamp": "2017-01-23T02:07:52",
"yymm": "1701",
"arxiv_id": "1701.05861",
"language": "en",
"url": "https://arxiv.org/abs/1701.05861"
} |
\section{Introduction}
The High Altitude Water Cherenkov (HAWC) Observatory is a gamma-ray and
cosmic-ray air shower detector located 4100~meters above sea level at
$19^\circ$N latitude in Sierra Negra, Mexico. The detector is operating
continuously with $>90\%$ uptime, including scheduled maintenance periods, and
pro... | {
"timestamp": "2017-01-24T02:05:24",
"yymm": "1701",
"arxiv_id": "1701.06160",
"language": "en",
"url": "https://arxiv.org/abs/1701.06160"
} |
\section{Introduction}
Up to now, scanning gate microscopy ({SGM}) has been successfully used to
image local electron transport in various mesoscopic systems. In early
applications, SGM probed the interference effects produced by microscopic
disorder in graphene,~\cite{berezovsky_sgm_1, berezovsky_sgm_2} and it was
la... | {
"timestamp": "2017-01-24T02:06:49",
"yymm": "1701",
"arxiv_id": "1701.06230",
"language": "en",
"url": "https://arxiv.org/abs/1701.06230"
} |
\section{Introduction}
The recent statistics published by LinkedIn revealed that increasing a number of US employers relies on personality assessments as a way to screen their prospective employees (26\% in 2001 to 57\% in 2013\footnote{https://www.linkedin.com/pulse}). It appears that certain jobs are more likely to ... | {
"timestamp": "2017-01-24T02:06:51",
"yymm": "1701",
"arxiv_id": "1701.06233",
"language": "en",
"url": "https://arxiv.org/abs/1701.06233"
} |
\section{Introduction}
The index coding (IC) problem \cite{BiK} consists of a source generating messages connected to a set of receivers via a broadcast channel, each of which have some demands and possess some prior side-information. An optimal index code for a given configuration of demands and side-information is an... | {
"timestamp": "2017-01-24T02:07:38",
"yymm": "1701",
"arxiv_id": "1701.06273",
"language": "en",
"url": "https://arxiv.org/abs/1701.06273"
} |
\section{Introduction}
Mobile data traffic is predicted to increase significantly in the coming years \cite{Ericsson2017}, which imposes a severe strain on existing wireless networks. One of the most promising methods to offload traffic is storing content closer to the end users, a technique known as \emph{caching} \ci... | {
"timestamp": "2018-11-01T01:02:02",
"yymm": "1701",
"arxiv_id": "1701.06289",
"language": "en",
"url": "https://arxiv.org/abs/1701.06289"
} |
\section{Introduction}
Luttinger liquid theory is a powerful tool for the theoretical study of interacting systems in one dimension, allowing for detailed analysis of their low energy properties\cite{haldane81jpc,haldane81prl}. Many attempts have been made to extend the theory for the study of systems of higher dimens... | {
"timestamp": "2017-01-24T02:06:16",
"yymm": "1701",
"arxiv_id": "1701.06200",
"language": "en",
"url": "https://arxiv.org/abs/1701.06200"
} |
\section{Introduction}
Quantum Inverse Scattering Method (QISM) is a powerful tool for solving quantum integrable models \cite{TakF79,SklTF79,KorBI93L,FadLH96}. This method
allows one to find spectra of quantum Hamiltonians via the algebraic Bethe ansatz. The main advantage of the
algebraic Bethe ansatz is that it gi... | {
"timestamp": "2017-01-23T02:07:53",
"yymm": "1701",
"arxiv_id": "1701.05866",
"language": "en",
"url": "https://arxiv.org/abs/1701.05866"
} |
\section{Introduction}
\label{intro}
Deuterium fractionation $R_{\rm D}$ or D/H\,=\,[XD]/[XH] represents the enhancement of D content in molecules (the notation [X] stands for the relative abundance of chemical species X). $R_{\rm D}$ for molecules in Solar-system bodies and star-forming regions is often found to b... | {
"timestamp": "2017-01-23T02:07:46",
"yymm": "1701",
"arxiv_id": "1701.05856",
"language": "en",
"url": "https://arxiv.org/abs/1701.05856"
} |
\section{Introduction}
Variants of domination play an important role in graph theory. They give rise to theoretically interesting (and often difficult) problems and are widely applicable to model various real-life scenarios, see, e.g.~\cite{MR1605685,MR1605684}. The main subject of the present work is the study of dom... | {
"timestamp": "2017-08-21T02:03:55",
"yymm": "1701",
"arxiv_id": "1701.05886",
"language": "en",
"url": "https://arxiv.org/abs/1701.05886"
} |
\section{Introduction}
\label{sec:intro}
Throughout the paper $\F$ denotes an algebraically closed field.
Fix a nonzero $q \in \F$ that is not a root of unity.
An $\F$-algebra is meant to be associative and have a $1$.
We begin by recalling the notion of a Leonard pair.
We use the following terms.
A square m... | {
"timestamp": "2017-01-24T02:04:14",
"yymm": "1701",
"arxiv_id": "1701.06089",
"language": "en",
"url": "https://arxiv.org/abs/1701.06089"
} |
\section*{\refname}\small\renewcommand\bibnumfmt[1]{##1.}}
\usepackage{amssymb} \setcounter{tocdepth}{3} \usepackage{graphicx}
\makeatletter%
\@ifundefined{basedir}{%
\newcommand\basedir{}%
}{}%
\makeatother%
\usepackage{amsfonts}
\usepackage{amssymb}
\usepackage{stmaryrd}
\usepackage{multirow}
\usepackage{... | {
"timestamp": "2017-01-23T02:08:17",
"yymm": "1701",
"arxiv_id": "1701.05888",
"language": "en",
"url": "https://arxiv.org/abs/1701.05888"
} |
\section{Introduction}
\label{sec:Intro}
\IEEEPARstart{I}{n} the last decade, there has been considerable interest in digital music services that display the lyrics of songs that are synchronized with their audio. As a recent example, {\it Sound Hound}\footnote{https://www.soundhound.com/} provided a live-lyrics featur... | {
"timestamp": "2017-01-25T02:07:59",
"yymm": "1701",
"arxiv_id": "1701.06078",
"language": "en",
"url": "https://arxiv.org/abs/1701.06078"
} |
\section{Introduction}
A $d$-dimensional parametric family
\[ \condset{p_\theta}{\theta=
(\theta^1, \ldots , \theta^d)\in\Theta}, \quad \Theta\subset\bR^d
\]
of probability density functions on
a measure space $(\cX, {\cal B}, \nu) $ is called an exponential family with a
natural parameter $\theta=(\theta^i)$
(e.g... | {
"timestamp": "2017-01-24T02:04:43",
"yymm": "1701",
"arxiv_id": "1701.06119",
"language": "en",
"url": "https://arxiv.org/abs/1701.06119"
} |
\section{Introduction}\label{Introduction}
Nanoscopic effects associated with fluid interfaces play an important role in a wide range of natural phenomena and technological applications. These include the design of water-repellent surfaces, inkjet printing, oil recovery, as well as a growing number of applications in ... | {
"timestamp": "2017-01-24T02:05:55",
"yymm": "1701",
"arxiv_id": "1701.06182",
"language": "en",
"url": "https://arxiv.org/abs/1701.06182"
} |
\section{Introduction}
For a set $V$ and a positive integer $r$ we denote by $V^{(r)}$ the family of all $r$-subsets of $V$. An {\em $r$-uniform graph} or {\em $r$-graph $G$} consists of a set $V(G)$ of vertices and a set $E(G) \subseteq V(G) ^{(r)}$ of edges. An edge $e=\{a_1, a_2, \ldots, a_r\}$ will be simply denot... | {
"timestamp": "2017-01-24T02:05:03",
"yymm": "1701",
"arxiv_id": "1701.06139",
"language": "en",
"url": "https://arxiv.org/abs/1701.06139"
} |
\section{Introduction}
There is dynamical evidence for the existence of super massive BHs in
the center of many nearby galaxies \citep{Ferrarese&Ford2005} with
masses in the range $M_{\rm BH}\sim 10^6-10^9$ M$_\odot$ suggesting
that BHs, formed at the first evolutionary stages of our Universe,
now are living in th... | {
"timestamp": "2017-01-24T02:05:39",
"yymm": "1701",
"arxiv_id": "1701.06172",
"language": "en",
"url": "https://arxiv.org/abs/1701.06172"
} |
\section*{1 Introduction}
Quantum correlations other than entanglement \cite{ref1} have increasingly been discussed in quantum information. Among them, quantum discord has attracted attention and is calculated in terms of von Neumann entropies of density matrices \cite{ref2}. Thereby, its definition and calculation is... | {
"timestamp": "2018-07-26T02:05:46",
"yymm": "1701",
"arxiv_id": "1701.05922",
"language": "en",
"url": "https://arxiv.org/abs/1701.05922"
} |
\section{Introduction}
\label{sec:intro}
Coloring the vertices of a graph is one of the fundamental problems in graph theory, both scientifically and historically.
Proving that four colors always suffice to color a planar graph \cite{AH1,AH2,RSST} was a tantalizing open problem for
more than 100 years; the quest for so... | {
"timestamp": "2018-09-13T02:12:04",
"yymm": "1701",
"arxiv_id": "1701.05999",
"language": "en",
"url": "https://arxiv.org/abs/1701.05999"
} |
\section{Introduction}
The high energy scale during inflation, presumably well beyond the reach
of the current and future particle accelerator experiments, calls for an
effective theory description of inflation
\cite{Cheung:2007st,Weinberg:2008hq}. This is because by construction
the effective field theory approac... | {
"timestamp": "2017-04-04T02:07:50",
"yymm": "1701",
"arxiv_id": "1701.05875",
"language": "en",
"url": "https://arxiv.org/abs/1701.05875"
} |
\section{Introduction}
\label{sec:intro}
Dialog state tracking is one of key sub-tasks of dialog management, whose goal is to transfer human utterances into a slot-value representation (dialog state) that is easy for computer to process and track the information that appeared in the dialog. To provide a common testbed... | {
"timestamp": "2017-01-24T02:07:13",
"yymm": "1701",
"arxiv_id": "1701.06247",
"language": "en",
"url": "https://arxiv.org/abs/1701.06247"
} |
\section{Introduction}
The 20th century witnessed a crucial paradigm shift in social and behavioral sciences, which
can be described as ``moving from the description of social bodies to dynamic problems of changing group life''~\citep{Lewin:1947}. Unlike individualistic approaches, focused on
individual choices an... | {
"timestamp": "2017-03-08T02:01:04",
"yymm": "1701",
"arxiv_id": "1701.06307",
"language": "en",
"url": "https://arxiv.org/abs/1701.06307"
} |
\section*{Acknowledgments}
M.C. and K.P. are grateful for the warm
hospitality at JINR. This work was supported in
part by Bogoliubov-Infeld program of BLTP and
Russian Foundation for Basic Research.
| {
"timestamp": "2017-01-24T02:05:52",
"yymm": "1701",
"arxiv_id": "1701.06179",
"language": "en",
"url": "https://arxiv.org/abs/1701.06179"
} |
\section{Introduction}
The relativistic study of the radial oscillations and of the related instability of a star have begun with the works of Chandrasekhar \cite{1,2}.
The radial oscillations of a star are not related to the emission of gravitational waves, that are intrinsically quadrupolars. The emission of gravi... | {
"timestamp": "2017-02-03T02:04:03",
"yymm": "1701",
"arxiv_id": "1701.06193",
"language": "en",
"url": "https://arxiv.org/abs/1701.06193"
} |
\section{introduction}
The problem of communication for omniscience (CO) was originally formulated in \cite{Csiszar2004}. It is assumed that there are a finite number of users in a system. Each of them observes a distinct component of a discrete multiple correlated source in private. The users are allowed to exchang... | {
"timestamp": "2017-01-24T02:08:00",
"yymm": "1701",
"arxiv_id": "1701.06290",
"language": "en",
"url": "https://arxiv.org/abs/1701.06290"
} |
\section{Introduction}
\label{intro}
Light-front quantization offers a natural framework for formulating the
spatial structure of relativistic systems and exploring its connection
to the underlying dynamics; see \cite{Brodsky:1997de} for a review.
In this framework, hadronic current matrix
elements (vector, axial) ar... | {
"timestamp": "2017-01-23T02:08:02",
"yymm": "1701",
"arxiv_id": "1701.05871",
"language": "en",
"url": "https://arxiv.org/abs/1701.05871"
} |
\section{Introduction}
\subsection{Background}
The $q$-deformed class one $\mathfrak{gl}_{n}$ Whittaker functions, or {\it
$q$--Whittaker functions} for short, were defined in \cite{GLO1} as a special
class of joint eigenfuctions of the $q$-deformed Toda chain Hamiltonians
\cite{Etingof,Ruijsenaars} with the suppo... | {
"timestamp": "2017-01-24T02:08:00",
"yymm": "1701",
"arxiv_id": "1701.06292",
"language": "en",
"url": "https://arxiv.org/abs/1701.06292"
} |
\section{Introduction}
In general spacetimes the notion of particles loses its invariant meaning. One consequence of this observation is the detection of thermal particles in the Minkowski vacuum by a uniformly accelerated observer. This phenomenon is known as the Unruh effect \cite{Unruh:1976db}. It has immediate con... | {
"timestamp": "2017-05-12T02:04:43",
"yymm": "1701",
"arxiv_id": "1701.05906",
"language": "en",
"url": "https://arxiv.org/abs/1701.05906"
} |
\section{Introduction}
Traditionally, wireless services have been offered by Service Providers (SPs) that own the infrastructure they are operating on. Nowadays SPs are divided into (i) Mobile Network Operators (MNOs) that own the infrastructure, and (ii)
Mobile Virtual Network Operators (MVNOs) that do not own the... | {
"timestamp": "2017-01-24T02:03:29",
"yymm": "1701",
"arxiv_id": "1701.06051",
"language": "en",
"url": "https://arxiv.org/abs/1701.06051"
} |
\section{Introduction}\label{intro}
\hspace{0.4cm} Throughout this paper, let $R = \bigoplus_{n \in \Nn}
R_n$ be a Noetherian homogeneous ring with local base ring $(R_0,
\mathfrak{m}_0)$. So $R_0$ is a Noetherian ring and there are
finitely many elements $l_1, \dots, l_r \in R_1$ such that $R =
R_0[l_1, \dots, ... | {
"timestamp": "2017-01-24T02:03:56",
"yymm": "1701",
"arxiv_id": "1701.06072",
"language": "en",
"url": "https://arxiv.org/abs/1701.06072"
} |
\section{introduction
Binomial coefficients constitute an important class of numbers that arise naturally in mathematics, namely as coefficients in the expansion of the polynomial $(x+y)^n$. Accordingly, they appear in various mathematical areas. An elementary property of binomial coefficients is that $\binom{n}{m}$ i... | {
"timestamp": "2017-01-24T02:06:33",
"yymm": "1701",
"arxiv_id": "1701.06217",
"language": "en",
"url": "https://arxiv.org/abs/1701.06217"
} |
\section{Introduction}
\label{sec:intro}
The task of learning a generative model of a data distribution has long been a very difficult, yet rewarding research direction in the statistics and machine learning communities. Often positioned as a complement to discriminative models, generative models face a more difficult ... | {
"timestamp": "2017-06-14T02:08:26",
"yymm": "1701",
"arxiv_id": "1701.05927",
"language": "en",
"url": "https://arxiv.org/abs/1701.05927"
} |
\section{Introduction}
The knowledge of a person's spatial whereabouts is an important component of a ubiquitous system. In the past years, several researchers have proposed various methods for automatic collection of a user's spatial trajectories using smartphone applications~\cite{Chon14,Kjaergaard11,Stylianou15} run... | {
"timestamp": "2017-01-24T02:07:42",
"yymm": "1701",
"arxiv_id": "1701.06276",
"language": "en",
"url": "https://arxiv.org/abs/1701.06276"
} |
\section{Introduction}
Quantum systems are generally never completely isolated but interact with an environment with which they may exchange energy and other physical observable quantities. Their properties are naturally affected by their coupling to the external world. The understanding and control of the influence o... | {
"timestamp": "2017-01-24T02:03:10",
"yymm": "1701",
"arxiv_id": "1701.06027",
"language": "en",
"url": "https://arxiv.org/abs/1701.06027"
} |
\section{Introduction and main results}
For $n \geq 3$ Hardy inequality states, that for any $u \in
C^{\infty}_{c}({\mathbb{R}}^n)$ there holds
\[
\int_{{\mathbb{R}}^n} |\nabla u|^2 dx
\geq \Big( \frac{n-2}{2}\Big)^2 \int_{{\mathbb{R}}^n} \frac{u^2}{|x|^2} dx \ ,
\]
where $\frac{(n-2)^2}{4}$ is the best const... | {
"timestamp": "2018-04-06T02:02:19",
"yymm": "1701",
"arxiv_id": "1701.06336",
"language": "en",
"url": "https://arxiv.org/abs/1701.06336"
} |
\section{Introduction}
\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 1.7 and later.
I wish you the best of success.
\hfill mds
\hfill January 11, 2007
\subsection{Subsection Headin... | {
"timestamp": "2017-06-12T02:02:06",
"yymm": "1701",
"arxiv_id": "1701.06241",
"language": "en",
"url": "https://arxiv.org/abs/1701.06241"
} |
\section{Introduction} \label{sec:1}
\setcounter{equation}{0}
Consider a manager, who allocates some fixed some fixed total payment amount $M$ between $N$ producers (agents) in order to maximize the aggregate production. The profit of each agent equals to the difference between the reward obtained from the manager an... | {
"timestamp": "2017-01-24T02:03:17",
"yymm": "1701",
"arxiv_id": "1701.06038",
"language": "en",
"url": "https://arxiv.org/abs/1701.06038"
} |
\section{Introduction} \label{sec:intro}
The subject of this paper is a conjecture inspired by the following celebrated result by L.E. Dickson \cite{LED}:
\begin{theorem} [Dickson]
When $G=Gl_n(\mathbb{F}_q)$ acts via invertible linear substitution of variables on the polynomial ring $S = \mathbb{F}_q[x_1,x_2,\cdots,... | {
"timestamp": "2017-01-24T02:08:44",
"yymm": "1701",
"arxiv_id": "1701.06329",
"language": "en",
"url": "https://arxiv.org/abs/1701.06329"
} |
\section{Introduction}
\label{sec:intro}
There are many observational evidences in black hole (BH) X-ray binaries (BHBs) and active galactic nuclei (AGNs) for the coupling between the collimated relativistic jet and the accretion flow. One such evidence comes from \citet{Corbel2003} and \citet{Gallo2003}, who discover... | {
"timestamp": "2017-01-24T02:05:07",
"yymm": "1701",
"arxiv_id": "1701.06143",
"language": "en",
"url": "https://arxiv.org/abs/1701.06143"
} |
\section*{Appendix}
\subsection{Proof of Lemma~\ref{lemma:MAY}}\label{proof:2}
We first consider the general solution to Eq.~(\ref{eq:obj}) without the regularization function. With the observed graph structure, the objective in Eq.~(\ref{eq:obj}) without regularization term can be rewritten as the following dual for... | {
"timestamp": "2017-01-24T02:04:01",
"yymm": "1701",
"arxiv_id": "1701.06075",
"language": "en",
"url": "https://arxiv.org/abs/1701.06075"
} |
\section{Introduction}
In the recent study of string theory, one of the most important issues is to understand
a holographic principle \cite{Hooft, Susskind} at the full quantum level
(For a review see \cite{Bousso}).
The AdS/CFT correspondence \cite{M, GKP, Witten} is a realization of the holography.
This is, how... | {
"timestamp": "2017-02-01T02:03:14",
"yymm": "1701",
"arxiv_id": "1701.06340",
"language": "en",
"url": "https://arxiv.org/abs/1701.06340"
} |
\section{Introduction}\label{sec:intro}
In recent decades, functional data analysis (FDA) has received substantial attention and become increasingly important especially as the advent of ``Big Data'' era.
Representative monographs on FDA
include
\cite{Ramsay-Silverman05}, \cite{FerrV06}, \cite{HorvK12}, and \cite{Hsin... | {
"timestamp": "2017-01-24T02:07:24",
"yymm": "1701",
"arxiv_id": "1701.06263",
"language": "en",
"url": "https://arxiv.org/abs/1701.06263"
} |
\section{Introduction}
There are two well-motivated possibilities for generating the baryon asymmetry at high temperatures: right-handed neutrino leptogenesis and the Affleck-Dine baryogenesis \cite{Affleck:1984fy,Dine:1995kz,Dine:2003ax}. The Affleck-Dine mechanism utilises the fact that scalar potentials in supersym... | {
"timestamp": "2017-01-23T02:07:48",
"yymm": "1701",
"arxiv_id": "1701.05859",
"language": "en",
"url": "https://arxiv.org/abs/1701.05859"
} |
\section{Introduction}
\label{sec:intro}
\noindent
In Quantum Field Theory (QFT), there exist different representations for the Hilbert space of quantum states.
The one used most frequently is the Fock representation (using Dirac's bra-ket notation), in which a general state is a linear combination of $n$-particle sta... | {
"timestamp": "2017-01-24T02:03:30",
"yymm": "1701",
"arxiv_id": "1701.06053",
"language": "en",
"url": "https://arxiv.org/abs/1701.06053"
} |
\section{Introduction}
\noindent
The inflation model \citep{Starobinsky:1979ty,Starobinsky:1980te,Guth:1980zm,Linde:1981mu,Albrecht:1982wi,Sato:1980yn} has been the leading paradigm of the very early Universe in past three decades. Not only does it resolve the flatness, horizon and monopole problems in the hot big-bang... | {
"timestamp": "2018-11-29T02:10:55",
"yymm": "1701",
"arxiv_id": "1701.06115",
"language": "en",
"url": "https://arxiv.org/abs/1701.06115"
} |
\section{Introduction}
Strachey~\cite{str00} distinguished between {\em ad hoc} and
parametric polymorphic functions in programming languages, defining a
polymorphic program to be {\em parametric} if it applies the same
type-uniform algorithm at each of its type instantiations.
Reynolds~\cite{param_reynolds} introduce... | {
"timestamp": "2017-01-24T02:07:12",
"yymm": "1701",
"arxiv_id": "1701.06244",
"language": "en",
"url": "https://arxiv.org/abs/1701.06244"
} |
\section{Introduction}
Snyder spacetime \cite{Snyder} was introduced in 1947 as an attempt to avoid UV divergences in QFT.
By assuming a noncommutative structure of spacetime, and hence a deformation of the Heisenberg algebra,
it was possible to define a discrete
spacetime without breaking the Lorentz invariance, openi... | {
"timestamp": "2017-01-23T02:07:52",
"yymm": "1701",
"arxiv_id": "1701.05862",
"language": "en",
"url": "https://arxiv.org/abs/1701.05862"
} |
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