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1,108,101,564,815 | arxiv | \section*{Combining ozone and UV-light for energy efficient removal of \ch{SO_x} in low-temperature flue gas}
\addcontentsline{toc}{section}{Combining ozone and UV-light for energy efficient removal of \ch{SO_x} in low-temperature flue gas}
\noindent
Reference number: 19-422 \\ \\
Marc Rovira, Klas Engvall, and Christ... |
1,108,101,564,816 | arxiv | \section{Introduction}
It is a well-known problem that perturbative approximations to low-dimensional condensed-matter systems of interacting fermions lead to expressions that diverge logarithmically at low energies.
The focus of this paper lies on a class of mostly zero- and one-dimensional systems characterized by t... |
1,108,101,564,817 | arxiv | \section{Introduction}
\setcounter{equation}{0}
Currently, the focus of high energy physics is the LHC experiment.
To understand the experiment data, we need to evaluate scattering
amplitudes to high accuracy level required by data. Thus for most
processes, the one-loop evaluation becomes necessary. In last ten
... |
1,108,101,564,818 | arxiv | \section{Preamble}
The second generation interferometric detectors of gravitational waves were
the result of major upgrades in the design and implementation of the LIGO
detectors in the USA\ and the Virgo detector in Europe, during 2009-2015. The
enthusiastic surge of interest in\ the anticipated detection of gravitat... |
1,108,101,564,819 | arxiv | \section{Introduction}
The Crab Pulsar is a recognized standard for astronomical timing measurements (\cite{lyn97}). As we prepared to demonstrate the performance of the STIS after installation in HST in 1997 February (\cite{kim98}), we found the Crab Pulsar to be uniquely suited for testing the time-tagging capabilit... |
1,108,101,564,820 | arxiv | \section{INTRODUCTION}
\label{sec:introduction}
ULTRASAT is a space mission instrumented with a scientific telescope which is designed for time domain astronomy.
Under the mission leadership of Weizmann Institute of Science (WIS)\footnote{\href{https://www.weizmann.ac.il/particle/}{Weizmann Institute of S... |
1,108,101,564,821 | arxiv |
\section{The CMS Collaboration \label{app:collab}}\begin{sloppypar}\hyphenpenalty=5000\widowpenalty=500\clubpenalty=5000\input{HIG-12-041-authorlist.tex}\end{sloppypar}
\end{document}
|
1,108,101,564,822 | arxiv | \section{Introduction}
In our earlier study \cite{Our1} we derived the following total Hamiltonian $H_T$ of the free gravitational
field
\begin{equation}
H_{T} = H_{c} + g_{00,0} \phi^{00} + 2 g_{0k,0} \phi^{0k} \; \; \; , \; \; \label{eq0}
\end{equation}
where $H_c$ is the `canonical', or `dynamical' part o... |
1,108,101,564,823 | arxiv | \section{Introduction}
Optical interferometry is a well-known experimental technique for making
precision displacement measurements, with examples ranging from Michelson
and Morley's famous aether-drift experiment to the extraordinary sensitivity
of modern gravitational-wave detectors. With careful attention to v... |
1,108,101,564,824 | arxiv | \section{Introduction}
Recovering a structured signal from a relatively small number of linear measurements has received a great deal of attention during the past few decades \cite{chandrasekaran2012convex, vershynin2015estimation, tropp2015convex, thrampoulidis2015recovering, vaiter2015low}. Typical examples of struc... |
1,108,101,564,825 | arxiv |
\section{Introduction} \label{sec:intro}
The Lennard-Jones (LJ) potential is one of the centerpieces in Molecular Dynamics (MD) simulations, the key computational method for studying atomistic phenomena across Chemistry, Physics, Biology and Mechanics. Despite the widespread use of MD simulations, a usually overlook... |
1,108,101,564,826 | arxiv | \section{Introduction}
Berry, Chen, Zame, Heath and Shepp (1997) initiated the infinite arms bandit problem on Bernoulli rewards.
They showed in the case of uniform prior on the mean of an arm,
a $\sqrt{2n}$ regret lower bound for $n$ rewards,
and provided algorithms based on success runs that achieve no more th... |
1,108,101,564,827 | arxiv | \section{Introduction}
Coronavirus, also known as COVID-19 was discovered in Wuhan, China, in December of 2019~\cite{who}. COVID-19 has many strains and can infect animals and humans. COVID-19 is hard to detect because it has common symptoms such as cold and flu. The symptoms also range in seriousness depending on the ... |
1,108,101,564,828 | arxiv | \section{Introduction}
This letter is devoted to the aim of understanding what happens
inside the finite Frenkel-Kontorova (FK)
chain~\cite{kont38I,kont38II,QuBo18MolPhys},
if the two characteristic ratios $a/b$ and $V_o/k$ change.
We select ref.~\onlinecite{mun20} to discuss some general problems of
the underst... |
1,108,101,564,829 | arxiv | \section{Introduction}
Acceleration strategies in the context of optimization have proved to be powerful. One example, termed \emph{heavy ball acceleration}, was introduced by Polyak~\cite{Polyak:1964}, while perhaps the most influential form of acceleration was introduction by Nesterov~\cite{Nesterov:1983} and is oft... |
1,108,101,564,830 | arxiv | \section{Introduction}
In~\cite{Gromov2014Dirac}, Gromov proposed a geometric comparison theory for metrics with scalar curvature lower bounds. He speculated that Riemannian polyhedrons should play the role of~triangles in Alexandrov's comparison theory for sectional curvature~\cite{AleksandrovRerestovskiiNikolaev86}. ... |
1,108,101,564,831 | arxiv | \section{Introduction}
The
discrete cosine transform (DCT)~\cite{britanak2007discrete,rao1990discrete}
is a fundamental building-block
for several image and video processing applications.
In fact,
the DCT closely approximates
the Karhunen-Lo\`eve transform (KLT)~\cite{britanak2007discrete},
which is capable of optima... |
1,108,101,564,832 | arxiv | \section*{PRELIMINARIES AND RESULTS}
The idea of category base is a generalization of both measure and topology and its main objective is to present measure and Baire category(topology) and also some other aspects of point set classification within a common framework. It was introduced by J.C.Morgan II in the mid seve... |
1,108,101,564,833 | arxiv | \section{Introduction}
The AdS/CFT correspondence is the most precise non-perturbative definition of quantum gravity. A central problem is how local bulk physics emerges from CFT data. This question has been studied extensively and is reasonably well-understood at large $N$, for small perturbations around vacuum AdS \... |
1,108,101,564,834 | arxiv | \section{Conclusion}
\label{sec:con}
We introduce a simple but effective loss function, PIoU, to exploit both the angle and IoU for accurate OBB regression. The PIoU loss is derived from IoU metric with a pixel-wise form, which is simple and suitable for both horizontal and oriented bounding box. To demonstrate its eff... |
1,108,101,564,835 | arxiv | \section{Introduction}
The purpose of this paper is to study the structure of the bounded derived
category $\Dbcoh(\boldsymbol{E})$ of coherent sheaves on a singular irreducible
projective curve $\boldsymbol{E}$ of arithmetic genus one.
In the smooth case, such structure results are easily obtained from Atiyah's
des... |
1,108,101,564,836 | arxiv | \section{Introduction}
\medskip
It is widely known that critical point theory and variational techniques play a major role in a host of problems arising in life sciences. Over the last decades, a strong development of these methods and their applications has been witnessed in connection with the qualitative study of d... |
1,108,101,564,837 | arxiv | \section*{Introduction}
\label{cint}
The goal of this paper is to try to understand the information contained in the
successive terms of spectral sequences, from the point of view of
\wwb{\infty,1}categories. Although many of the spectral sequences in common use are
stable, and may be described completely in terms of ... |
1,108,101,564,838 | arxiv | \section{Introduction}
In the \emph{standard model} (SM) of elementary particle physics, the total number of leptons of each flavour is conserved. The discovery of neutrino oscillations \cite{Fukuda:1998mi, Ahmad:2001an, Eguchi:2002dm} revealed that this is a broken symmetry and leptons can change their flavour. \em... |
1,108,101,564,839 | arxiv | \section{Introduction and results \label{sec-intro}}
The goal of this paper is to study scaling limits of random matrix products
$${\mathcal T}_{\lambda,n} {\mathcal T}_{\lambda,n-1}\cdots {\mathcal T}_{\lambda,1}$$
with $\lambda\to 0$ where the ${\mathcal T}_{\lambda,n}$ are perturbations of a fixed $d\times d$ matri... |
1,108,101,564,840 | arxiv | \section{Introduction}
Time-evolution of a quantum mechanical system characterized by a discrete energy spectrum allows energy level crossings in certain situations. When two levels cross under a modulation of some external parameter (e.g. magnetic and electric fields etc.) varying in time, the level crossings may or... |
1,108,101,564,841 | arxiv | \section{Introduction}
Modern machine learning models can yield highly accurate predictions in many applications. As these predictions are often used in critical decision making, it is increasingly important to accompany them with an uncertainty quantification of how much the true label may deviate from the predictio... |
1,108,101,564,842 | arxiv | \section{Introduction}
Gait can be regarded as an unique feature of a person, and it is usually determined by an individual's physical characters, \textit{e.g.}, height, weight, limb length, and walking habit, \textit{e.g.}, walking speed, posture combined with characteristic motions.
The study of human gait recognit... |
1,108,101,564,843 | arxiv | \section{Introduction}
Let $\D$ stand for the disk $\{z\in\C:|z|<1\}$, $\T$ for its boundary, and $m$ for the normalized Lebesgue measure on $\T$. For $0<p\le\infty$, we denote by $H^p$ the classical Hardy $p$-space of holomorphic functions on $\D$ (see \cite[Chapter II]{G}), viewed also as a subspace of $L^p(\T,m)$... |
1,108,101,564,844 | arxiv | \section*{Introduction}
Fix a congruence subgroup $G$ which is either of the form $\Gamma_0(N)$ or $\Gamma_1(N)$ for some $N$, and $A$ a subring of $\mathbb{C}$. A modular form on $G$ has a $q$-expansion:
\[ f(z) = \sum_{i \geq 0} a_i q^i \]
where $q = e^{2i\pi z}$ and $a_i \in \mathbb{C}$ for all $i\geq 0$. If $A$ is ... |
1,108,101,564,845 | arxiv | \section{Introduction}
In recent years there has been an increased demand from citizens, corporations, and governments to access e-government services. This requires the need for trustworthy e-governance solutions that provide citizens and businesses with safe and transparent public services, and without compromising t... |
1,108,101,564,846 | arxiv | \section{Introduction}
\label{introduction}
Early \emph{graph mode} or \emph{define-and-run}~\cite{DBLP:journals/corr/abs-1908-00213} deep learning frameworks like Caffe~\cite{DBLP:journals/corr/JiaSDKLGGD14}, Theano~\cite{DBLP:journals/corr/Al-RfouAAa16}, and TensorFlow~\cite{45381} defined APIs in which th... |
1,108,101,564,847 | arxiv | \section{Introduction}
A commonly encountered class of signals consists of one or more pure sinusoidal tones plus noise. For such signals, the Fourier transform (FT) is often the analysis method of first choice because it concentrates the power of each tone into a delta function located at the tone frequency, and ... |
1,108,101,564,848 | arxiv | \section{Evolving the Equations of General Relativistic
Magnetohydrodynamics on Adaptively-Refined Grids}
We have recently extended our adaptive mesh refinement (AMR) numerical
relativity code to solve the ideal magnetohydrodynamics (MHD)
equations, enabling us to simulate MHD effects in dynamical spacetimes
with AM... |
1,108,101,564,849 | arxiv | \section{Introduction}
The idea that quantum mechanics can be well defined even if the notion of time is absent has been proposed \cite{Rovelli:1989jn,Rovelli:1988qp} and developed in a number of different strategies \cite{Rovelli:1990jm,Rovelli:1991ni,Reisenberger:2001pk,Marolf:2002ve,Hartle:1992as}. The motivation f... |
1,108,101,564,850 | arxiv | \section{Introduction}
The 22.2\,GHz radio emission from luminous extragalactic H$_2$O masers originates in dense ($10^7$\,$<$\,$n({\rm H_2})$\,$<$\,$10^{11}$\,cm$^{-3}$) and warm ($T$\,$>$\,300\,K) gas clouds within a few parsecs from the nuclear engines of their parent galaxies. These masers trace circumnuclear accr... |
1,108,101,564,851 | arxiv | \section{Introduction}\label{sec:intro}
The morphology of star forming galaxies at $1\leq z \leq3$ is often dominated by giant ($\sim$1 kpc) and massive ($\gtrsim$10$^{8-9}\ \ensuremath{{\rm M}_\odot}$) clumps which contribute a significant fraction ($\sim$20-30\%) of the total system's star formation. These clumpy str... |
1,108,101,564,852 | arxiv | \section{Introduction}
Planet formation and evolution are heavily dependent on the circumstellar environment. The circumstellar material can dictate formation, composition, orbital parameters, and migration of planets. While much has been learned in recent years about circumstellar disks, especially with ALMA \citep{... |
1,108,101,564,853 | arxiv | \section{Introduction}
\label{sec:intro}
Motion Estimation/Compensation and video coding have wide range of applications in various areas of image/video processing, including restoration \cite{Foroosh_2000,Foroosh_Chellappa_1999,Foroosh_etal_1996,Cao_etal_2015,berthod1994reconstruction,shekarforoush19953d,lorette1997s... |
1,108,101,564,854 | arxiv | \section{Introduction}
Cataclysmic variables (CVs) are compact binaries comprised of a Roche-lobe filling sun-like star transferring gas to a white dwarf (WD) via an accretion disk (if the WD is non-magnetic) or via a magnetically channeled accretion column if the WD is magnetic. When a critical mass of hydrogen-ric... |
1,108,101,564,855 | arxiv | \section*{Acknowledgements}The author is indebted to Hans Gerd Evertz
for helpful discussions. Part of this work was performed at the
Institut f\"ur Theoretische Physik at TU-Graz under FWF grant number
P21240-N16.
|
1,108,101,564,856 | arxiv | \section{Introduction}
Radiation transfer is, by essence, a difficult problem (e.g., Rutily
\& Chevallier 2006), as well as a question of very large relevance in
astrophysics. It relies indeed on \emph{complex} non-linear
light--matter interactions (see e.g., Hubeny \& Mihalas 2014, Rutten
2003).
At the very heart of... |
1,108,101,564,857 | arxiv | \section{Introduction}
According to conventional wisdom, explicit regularization should be added to the least-squares objective when the Hilbert space $\cH$ is high- or infinite-dimensional \citep{Golub_1979,wahba1990spline,smola1998learning,shawe2004kernel,evgeniou2000regularization, de2005model, alvarez2012kernels}... |
1,108,101,564,858 | arxiv | \section{Introduction and main results}
\setcounter{equation}{0}
In this paper, we are concerned with the following elliptic equations
\begin{equation}\label{1.1}
\begin{cases}
-\Delta u= Q(x)u^{2^*-1 }+\varepsilon
u^{s},~ &{\text{in}~\Omega},\\[1mm]
u>0,~ &{\text{in}~\Omega},\\[1mm]
u=0, &{\text{on}~\partial \Omega... |
1,108,101,564,859 | arxiv | \section{Introduction}
During the last decade, outstanding results have been obtained on the
redshift distribution of faint galaxies up to
$I=22.5$ (see O. Le F\`evre, this conference) or $I=23$ (Cowie et al. 1996).
With the coming of 10 meter
class telescopes equipped with wide field multi-object
spectrographs ... |
1,108,101,564,860 | arxiv | \section{}
\section* {Introduction}
The first edition of Newton' s
{\it Mathematical Principles of Natural Philosophy},
commonly known as the {\it Principia}, appeared in 1687, transforming
our understanding of celestial mechanics and gravitational theory. In his magisterial book,
Newton gave a physical des... |
1,108,101,564,861 | arxiv | \section{Introduction}
One of the most important current questions in the field of star formation concerns the effect that environment and, especially, feedback may have on the star-formation process, in particular the stellar initial mass function (IMF) and the star-formation rate (SFR) or efficiency (SFE). Stars ap... |
1,108,101,564,862 | arxiv | \section{Introduction}
The behavior of nuclear matter at extreme temperatures is now being studied with the
highest collision energies ever achieved using the Large Hadron Collider (LHC) at CERN.
The ultrarelativistic heavy ion collisions being studied there will eventually
have a center of mass energy of 5.5 TeV pe... |
1,108,101,564,863 | arxiv | \section{Introduction}
In this paper let $(X,\omega)$ be a pair of a rational surface $X$ and an ample line bundle $\omega$.
We consider the moduli spaces
$M^X_\omega(c_1,d)$ of $\omega$-semistable torsion-free coherent sheaves of rank $2$ on $X$ with Chern classes $c_1\in H^2(X,{\mathbb Z})$ and $c_2$ such that $d=4c... |
1,108,101,564,864 | arxiv | \section{Introduction}\label{sec_intro}
Let $\Omega \subset \mathbb{R}^3$ be a bounded smooth domain occupied by a fluid and a rigid body. Let the rigid body $\mathcal{S}(t)$ be a regular, bounded domain and moving inside $\Omega$. The motion of the rigid body is governed by the balance equations for linear and angul... |
1,108,101,564,865 | arxiv | \section{Why is classical physics (in)deterministic?}
It is generally accepted that classical physics (i.e., Newton's mechanics and Maxwell's electrodynamics) is \emph{deterministic}. Restating a famous argument due to Laplace (known as Laplace's demon), determinism is usually assumed to be the ``view that a sufficien... |
1,108,101,564,866 | arxiv | \section{Introduction}
As a rule, group-theoretical methods alleviate description of the
complicated physical systems. In this respect Lie
algebras are of a special interest. Very elegant examples of their
applications were found in quantum mechanics within
the concept of the spectrum generating,
or, dynamical (super)... |
1,108,101,564,867 | arxiv | \section{Introduction}\label{sec:intro}
\subsection{Significance of Binary Supermassive Black Holes}
It is now well established that most, if not all, large galaxies in the local universe have supermassive black holes (SMBHs; $> 10^8\,\ensuremath{M_{\sun}}$) in their nuclei \citep[e.g.,][]{kormendy95,ff05}. Further, ... |
1,108,101,564,868 | arxiv | \section{Introduction}\label{sec:intro}
In vector similarity search one preprocesses $n$ vectors $x \in \mathbb{R}^d$ such that, given a query $q\in R^d$ computing the top (or bottom) $k$ values of $f(x,q)$ is most efficient.
The function $f$ can encode similarity between $x$ and $q$ like dot product $\langle x, q \ra... |
1,108,101,564,869 | arxiv | \section{Introduction}
Efficient computation of persistent homology has been a central quest in Topological Data Analysis (TDA) since the early days of the field about 20 years ago. Given a filtration (a nested sequence of simplicial complexes), computation of persistent homology involves reduction of a boundary matri... |
1,108,101,564,870 | arxiv | \section{Introduction}
One of the main tasks tackled with deep learning methods is the one of categorization: classification of images as representing specific objects, identification of words for speech recognition, etc. \citep[see][for reviews]{lecun2015deep, schmidhuber2015deep}. The identification of categories is... |
1,108,101,564,871 | arxiv | \chapter*{Preface}--not included
\title{Parameterized complexity of fair deletion problems.\thanks{Research was supported by the project GAUK 338216 and by the project SVV-2016-260332.
}}
\titlerunning{Fair deletion problems}
\author{Tomáš Masařík\inst{1}\thanks{Author was supported by the project CE-ITI P202/12/G061.... |
1,108,101,564,872 | arxiv |
\section{Conclusions}
\label{sec:conclusions}
In this paper, we have studied the problem of
mining frequent episodes over changing data streams. In particular our contribution in this work is three fold. We unearth an interesting aspect of temporal data mining where the data owner may desire results over a span ... |
1,108,101,564,873 | arxiv | \section{Introduction}
\label{sec:introducion}
Tag-aware recommendation systems (TRS), to better depict user preferences and item features, have been widely deployed to bridge the information gap between users and items \cite{hutchison_information_2006, bischoff_can_2008}. The fundamental factor of TRS is to provide a ... |
1,108,101,564,874 | arxiv | \section{Introduction}
Quantum phenomenon has been observed by numerous experiments on microscopic scales. However, on macroscopic scales, it is difficult to find quantum effects, such as quantum superpositions. A lot of physicists have been looking up the root of quantum-to-classical transition for decades. The reaso... |
1,108,101,564,875 | arxiv | \section{Introduction and summary of results}
In \cite{PabloPablo} we showed that, up to cubic order in curvature, the most general dimension-independent gravity theory constructed from arbitrary contractions of the metric and the Riemann tensor whose linearized spectrum coincides with the one of Einstein gravity can... |
1,108,101,564,876 | arxiv | \section{Introduction}
Bulk transition metal dichalcogenides (TMD) are layered van der Waals
solids displaying remarkable properties promising both for fondamental research
as well as for technological applications.
Metallic bulk transition
metal dichalchogenides (TMD) like NbSe$_2$,
present coexistence of charge den... |
1,108,101,564,877 | arxiv | \section{Introduction}
\label{intro}
Blazars are extremely bright and fast varying extragalactic sources observed throughout the
electromagnetic spectrum. Depending on the presence or absence of observed optical emission
lines they are classified as Flat Spectrum Radio Quasars (FSRQs) or BL Lac objects,
respectively... |
1,108,101,564,878 | arxiv | \section*{Introduction}
In this work we are interested in the convergence in distribution of
\begin{equation}\label{purpose}
\sqrt{N}\left(U\left(\frac{1}{N}\sum_{i=1}^{N}\delta_{X_i} \right)-U\left(\mu\right)\right)
\end{equation}
where $U$ is a general function defined on some Wasserstein space of ... |
1,108,101,564,879 | arxiv | \section{Introduction}
Generalized topological spaces have been introduced by Cs\'{a}sz\'{a}r in the last years of twentieth century (see \cite{csaszar} and \cite{genopen}). They are investigated by many authors from all over the world. They have invented generalized analogues of separation axioms (see \cite{sep}, \... |
1,108,101,564,880 | arxiv |
\section{Introduction}
Mechanical thrombectomy \cite{powers20152015,berkhemer2015randomized} is guided by an interventional C-arm system capable of 3-D imaging. Although its soft tissue contrast is comparable to helical CT scans, the prolonged acquisition time pose C-arm CBCT more susceptible to rigid head motion ... |
1,108,101,564,881 | arxiv | \section{Introduction}
Consider a fractional Brownian motion (fBm), a self-similar Gaussian
process with stationary increments. It was introduced by Kolmogorov
\cite{kol} and studied by Mandelbrot and Van Ness \cite{MN}. The fBm
with Hurst parameter $H\in(0,1)$ is a centered Gaussian process with
covariance func... |
1,108,101,564,882 | arxiv | \section{Introduction}
\label{Sec:1}
Over the last two decades, TWDP model has been extensively used to characterize small-scale fluctuations of a signal envelope, in cases where mmWave band and directional antennas are employed~\cite{Zoc19, Zoc19-1, Mav15}, as well as in wireless sensor networks within the cavity env... |
1,108,101,564,883 | arxiv |
\section{#1}\inputtex{#2}}
\providecommand{\isubsection}[2] {\subsection{#1}\inputtex{#2}}
\providecommand{\etal} {\emph{et al\@.}\xspace}
\providecommand{\ie} {\emph{i.e\@.}\xspace}
\providecommand{\eg} {\emph{e.g\@.}\xspace}
\providecommand{\cf} {\emph{cf\@.}\xspace}
\providecommand{\defacto} {\emph{de facto}\x... |
1,108,101,564,884 | arxiv |
\subsection{Data Analytic Pipelines}
The data analytic pipeline refers to a framework consisting of a sequence of computational transformations on the data to produce the final predictions (or outputs) \cite{kumar2015model}. Pipelines help users better understand and organize the analysis task, as well as increase t... |
1,108,101,564,885 | arxiv | \section{INTRODUCTION}
In a recent series of papers we have considered the evolution of
low--mass X--ray binaries (LMXBs), and in particular
the question of which LMXBs should be transient
according to the disk instability model.
To have low enough mass transfer rates for transient behavior,
short--period ($P \math... |
1,108,101,564,886 | arxiv | \section{The Einstein-Maxwell equations in a static space-time}
In 2+1 dimensions, the metric for an arbitrary static circularly symmetric
space-time can be written in the form
\begin{eqnarray} \label{metrica}
ds^{2}= e^{2 \, \alpha(r)}\, dt^{2}- e^{2 \, \beta(r)} \, dr^{2}- e^{2 \,
\gamma(r)} \, d\theta^{2}.
\end{... |
1,108,101,564,887 | arxiv | \section{Introduction}
Synthetic biology is concerned with building useful biological circuits with predictable dynamics. Most genetic circuits depend on the local machinery of a host chassis. Since the host must expend energy in expressing exogenous genes, resources are taken from endogenous processes which can imp... |
1,108,101,564,888 | arxiv |
\chapter*{Introduction}
\addcontentsline{toc}{chapter}{Introduction}
\begin{quote}
\emph{Siamo liberi di sceglierci ogni volta \\invece che lasciare troppe cose gi\`a decise \\ a scegliere per noi. (Tiromancino)}
\end{quote}
\
\noindent
\noindent This Ph.D. thesis \emph{The geometry of spherical random field... |
1,108,101,564,889 | arxiv | \section{\label{sec:intro}Introduction}
Introduced in order to resolve problems within the Big-Bang cosmological model (such as the horizon, flatness, and magnetic-monopole problems), inflation also naturally provides the seeds for generating primordial matter fluctuations from quantum fluctuations (see for instance Re... |
1,108,101,564,890 | arxiv | \section{Introduction}
\label{sec:introduction}
Gibbs processes are very popular point process models which are extensively used both in spatial statistics and in statistical physics, see e.g.\ \citep{moellerwaage04,ruelle69}. Especially the pairwise interaction processes allow a simple yet flexible modelling of point... |
1,108,101,564,891 | arxiv | \section{Introduction}
Wireless communications has come a long way, from mobile telephony in the 70s to nowadays massive, dynamic multimedia information access anywhere anytime in the era of Internet of everything (IoE). We have also witnessed a shift in research focus from outdoors to indoors since most data demand no... |
1,108,101,564,892 | arxiv | \section{Introduction}
In online music streaming services such as {\it Spotify}\footnote{https://www.spotify.com/}, a huge number of active users are interacting with a library of over 40 million audio tracks. Here, an important challenge is to recommend the right music item to each user. To this end, there has been a... |
1,108,101,564,893 | arxiv | \section{Conclusion}
In this paper we presented a novel approach for communicating information about a robot's internal state during physical interaction. Specifically, we introduced a class of soft, wrapped haptic displays that are mounted on the robot arm at the point of contact between the human and robot to commun... |
1,108,101,564,894 | arxiv | \section{Introduction}
\IEEEPARstart{T}{his} demo file is intended to serve as a ``starter file''
for IEEE journal papers produced under \LaTeX\ using
IEEEtran.cls version 1.8b and later.
I wish you the best of success.
\hfill mds
\hfill August 26, 2015
\subsection{Subsection Heading Here}
Subsection text here.
\... |
1,108,101,564,895 | arxiv | \section{Introduction} \label{intro}
Let $R$ be a commutative ring, and fix two scalars $[2]_s,[2]_t \in R$.
The \defnemph{two-colored Temperley--Lieb algebra} $2\mathrm{TL}_R(\prescript{}{s}{n}):=2\mathrm{TL}_R(\prescript{}{s}{n};[2]_s,[2]_t)$ is the $R$-algebra with generators
$e_i$ for $1 \leq i \leq n-1$,
subject... |
1,108,101,564,896 | arxiv |
\chapter{Introduction}
Two world-wide networks are currently searching for
extra-solar planetary systems by making densely sampled observations of
ongoing microlensing events toward the Galactic bulge (PLANET,
Albrow et al.\ 1996; GMAN, Pratt et al.\ 1996).
Several other groups will join the search shortly and
the... |
1,108,101,564,897 | arxiv | \section{Introduction}
The East process is a one-dimensional spin system that was introduced in the physics literature by J\"{a}ckle and Eisinger~\cite{JE91} in 1991
to model the behavior of cooled liquids near the glass transition point, specializing a class of models that goes back to~\cite{FH}.
Each site in ${\ens... |
1,108,101,564,898 | arxiv | \chapter{ILC Accelerator Parameters and Detector Concepts \label{sid:chapter_accelerator_detector}}
\input{Chapter_Accelerator_Detector/Section_ILCAcceleratorParameters.tex}
\input{Chapter_Accelerator_Detector/Section_DetectorConcepts.tex}
\input{Chapter_Accelerator_Detector/Section_SystematicErrors.tex}
\section{Det... |
1,108,101,564,899 | arxiv |
\section*{Acknowledgments}
This research work has been funded by the German Federal Ministry of Education and Research and the Hessian Ministry of Higher Education, Research, Science and the Arts within their joint support of the National Research Center for Applied Cybersecurity ATHENE.
\section*{Appendix}
\subse... |
1,108,101,564,900 | arxiv | \section{Introduction}
The description of complex systems in terms of the so-called "collective" variables has a long history in condensed matter physics. An important example of such a variable is the "order parameter field" usually employed for theoretical analysis of phase transitions. A convenience of this approac... |
1,108,101,564,901 | arxiv | \section{Introduction}
Zero-range processes (ZRP) are minimal models~\cite{spitz},
often used as simplified realisations of more complex processes
(for reviews, see \cite{kip,evans,lux}).
For instance they are instrumental for the understanding
of condensation transitions in driven diffusive systems~\cite{wis1,glm}.
T... |
1,108,101,564,902 | arxiv | \section{Introduction: Shape variations in the loop space and renormalization-group evolution}
Generalized loop space, associated to some base manifold, consists of the distributional version\footnote{In the sense that one needs to integrate over the integration contour or path ($\{\Gamma_i\}$) in the base manifold.}... |
1,108,101,564,903 | arxiv | \section{Introduction}
Since the early work of Euler \cite{Euler1844}, one-dimensional (1D) models have been successfully used to describe the flow of blood in the large arteries of the systemic network \cite{PedleyBook1980,Alastruey2011,Wang2015,Muller2014,Boileau2015}. They have proved to be valuable and efficient t... |
1,108,101,564,904 | arxiv | \section{Introduction and Notations}
A {\em body} is a compact set with nonempty interior. For a body $K$ which is star-shaped with respect to the origin its {\em radial function} is defined by
$$
\rho_K(u) = \max \{\lambda \ge 0 : \lambda u \in K\} \quad\mbox{for every } u\in S^{n-1}.
$$
A body $K$ is called a {... |
1,108,101,564,905 | arxiv | \section{Introduction}
Recently, a number of important progress have been made in the
physics of $J/\psi$ suppression as a signature of quark gluon plasma
that inevitably leads us to augment the original work by Matsui and
Satz\cite{Matsui86} with a more detailed study of heavy quark system
at finite temperatures, bef... |
1,108,101,564,906 | arxiv | \section{Introduction}
Nearly $\%40$ words in the English language have estimated to have ambiguous meanings, i.e., their meanings depend on their contexts. There are two documented reasons for such an ambiguity; Homonymy which means that an ambiguous word can have the same spelling or pronunciation with a word that... |
1,108,101,564,907 | arxiv | \section{Introduction}
The state of a quantum system in thermodynamic equilibrium with a heat reservoir
at temperature $T$ is given by the (un-normalized) Gibbs canonical density matrix
\begin{align}\label{GibsRhoDeffEq}
\hat{\rho} = e^{-\beta\hat{H}}, \qquad \beta = 1/(kT),
\end{align}
where $\hat{H}$ is the quantu... |
1,108,101,564,908 | arxiv | \section*{Introduction}
\begin{figure*}
\includegraphics[width=1\linewidth]{skin_setup.PNG}
\caption{Schematic (left) and picture (right) of the experimental set-up. Porcine skin is teared in front of an optical and an infrared camera, while both the applied force and displacement are measured. In the real set-up ... |
1,108,101,564,909 | arxiv | \section{Introduction}
\label{sec:introduction}
Recent results of heavy ion collision experiments at RHIC \cite{Adams:2005dq} and LHC \cite{Aamodt:2008zz}
shed some light on properties of the quark
gluon plasma and the position of the transition line in the temperature – baryon density plane.
New experiments w... |
1,108,101,564,910 | arxiv | \section{Introduction}
The focusing nonlinear Schr\"{o}dinger (NLS) equation in the space of
one dimension is a fundamentally important model which brings together nonlinearity and dispersion of modulated waves in many physical systems \cite{NLS2,NLS1}. It has been used as the main testbed for rogue
waves in fl... |
1,108,101,564,911 | arxiv | \section{Introduction}
This work is part of a large cycle 7 HST project (PID 7307) to study
the formation and evolution of rich star clusters in the LMC. Details
and first results can be found in Beaulieu (1998),
Elson (1998c) and Johnson (1998).
We have obtained observations (with WFPC2, NICMOS and
STIS) of 8 rich LM... |
1,108,101,564,912 | arxiv | \section{Introduction}
\label{sec:int}
Modeling the dynamic behavior of large systems of interacting agents remains a challenging problem in complex systems analysis.
Due to the large state space dimension of such systems, it has historically been an ongoing research goal to construct useful reduced-order models with ... |
1,108,101,564,913 | arxiv | \section{Introduction}
Let $M$ be a compact 3-manifold, and let $K$ be a knot inside $M$. Since the work of Dehn in 1910 \cite{dehn1910topologie}, deciding whether $K$ can be unknotted has been a major question in low-dimensional topology. Dehn formulated the word and the isomorphism problems for groups in an attempt... |
1,108,101,564,914 | arxiv | \chapter{Synergy between neuroscience and machine learning}
\label{ch:ml-ns-synergy}
Both, neuroscience and artificial intelligence, share, as one of their goals, the purpose of uncovering and understanding the mechanisms of intelligence\footnote{Here and throughout this work we adhere to using this loosely defined te... |
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