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1,116,691,497,415 | arxiv | \section{Introduction}
\label{sec:intro}
Rocks and rock-like materials ({\it e.g.}~concrete and stiff soils) commonly fail in a quasi-brittle manner, characterized by progressive softening during the post-peak stage.
During the softening process, numerous microcracks develop, grow, and coalesce to form localized macros... |
1,116,691,497,416 | arxiv | \section{Introduction}\label{intro}
Quantum computers consist of a finite number, $M$, of two state
systems. The resulting Hilbert space for this quantum system is
finite dimensional. Elementary gates are used to build an irreducible
algebra of operators on this space that can be used to model complex
systems. The ... |
1,116,691,497,417 | arxiv | \section{Introduction}
For fixed $n$, we seek a unit-volume $n$-hedral tile of space that minimizes surface area. Our Conjecture \ref{best3Dtiles} provides candidates from $n=4$, a certain irregular tetrahedron, to $n\geq 14$, Kelvin's truncated octahedron (see Figs. 1-7). The conjecture is known for $n=6$ and $n=5$. ... |
1,116,691,497,418 | arxiv | \subsection{Characterization of the optimal damping rule}
\label{damping_section}
This section aims to motivate and propose a heuristic rule for the optimal choice of the damping parameters $\mathbf{R}$ that can accelerate the convergence of the numerical quadrature in the Fourier space when approximating \eqref{i... |
1,116,691,497,419 | arxiv | \section{TO DO}
\section{Introduction}
This work deals with the complexity of smooth functions of many variables. The questions addressed in this paper can be phrased as: What does a random Morse function look like on a high-dimensional manifold? How many critical values of given index, or below a given level? What c... |
1,116,691,497,420 | arxiv | \section{Introduction}
Decentralized cryptocurrencies have witnessed explosive growth since
the first decentralized distributed currency Bitcoin was launched
in 2009~\cite{Nakamoto2008}. In contrast to traditional currencies,
decentralized cryptocurrencies are traded among participants over
a peer-to-peer (P2P) networ... |
1,116,691,497,421 | arxiv | \section{Introduction}
\label{intro}
Type Ia supernovae (SNe Ia) have become a major tool to determine
cosmological parameters. As a consequence of their uniformity of
properties and their enormous brightness they are suitable to be
applied in cosmological distance measurements.
However, they cannot be
claimed to be... |
1,116,691,497,422 | arxiv | \section{Introduction}
Channel quantization in a network with multiple receivers is fundamentally different from that in a point-to-point system. In a point-to-point system, the receiver can acquire the entire channel state information (CSI) and send the corresponding quantized feedback information to the transmitter ... |
1,116,691,497,423 | arxiv | \section{Introduction}
\label{secIntroduction}
A {\em Fano variety} is a smooth projective variety whose anti-canonical bundle is ample. It is proved by Koll\'{a}r-Miyaoka-Mori \cite{KMM} that there are finitely many deformation classes
of Fano varieties in each dimension. The complete classification has been kno... |
1,116,691,497,424 | arxiv |
\section{Introduction}
Multi-agent Path Finding (MAPF) is a problem that makes multiple agents move to their destinations without collisions.
MAPF is now receiving a lot of attention due to its high practicality, e.g., traffic control~\cite{dresner2008multiagent}, automated warehouse~\cite{wurman2008coordinating}, o... |
1,116,691,497,425 | arxiv | \section{Introduction}
\label{sec:Intro}
The quantification of entanglement in composite quantum systems remains a central question of foundational importance, as well as in terms of practical understanding and implementation of protocols in quantum information and quantum computation. We refer to \cite{HorodeckiEtAl:2... |
1,116,691,497,426 | arxiv | \section{Introduction}
The starting point of this note is the flow
\begin{equation}
\label{H1}
\dot z = f(z),
\end{equation}
in which $f $ or its conjugate
$\bar f$ is an entire function. A trajectory for (\ref{H1})
is a path $z(t)$ in the plane with $z'(t) = f(z(t)) \in \mathbb C$ for $t$ in some maximal inte... |
1,116,691,497,427 | arxiv | \section{ Introduction} Quantum entanglement plays an important role
in the study of fundamental principles of quantum
mechanics\cite{sakurai}. It is also the most important resource in
quantum information processing\cite{nielsen,decoy}. Among all types
of quantum entanglement, polarization entangled photon-pairs are
p... |
1,116,691,497,428 | arxiv | \section{Introduction}
Lascoux-Leclerc-Thibon (\cite{LLT}) conjectured that
the irreducible representations of Hecke algebras of type $A$ are
controlled by the upper global basis (\cite{Kash91,Kash93})
(or dual canonical basis (\cite{Lus93})) of
the basic representation of the affine quantum group $U_q(A^{(1)}_\... |
1,116,691,497,429 | arxiv | \section{Introduction}
The potential to determine the Hubble constant, $H_{0}$, using the double
image lens B0218+357 was established shortly after its discovery (Patnaik et
al. 1993) to be very high. This is because of the accurately measured value
for the time delay between the images, \mbox{(10.5 $\pm$ 0.4) d} (Big... |
1,116,691,497,430 | arxiv | \section{Introduction.}
{\bf \emph{Introduction.}} The discovery of a doubly charm meson~\cite{LHCb:2021vvq,LHCb:2021auc}, as well as the theoretical consensus on the existence of a doubly bottom counterpart~\cite{Bicudo:2012qt,Karliner:2013dqa,Francis:2016hui,Eichten:2017ffp,Leskovec:2019ioa}, is moving the spotlig... |
1,116,691,497,431 | arxiv | \section{Introduction}
A well-known property of shared object implementations is \emph{linearizability}~\cite{linearizability}.
Intuitively, with a linearizable object (implementation) each operation must appear as if it takes effect instantaneously
at some point during the time interval that it actually spans.
As poi... |
1,116,691,497,432 | arxiv | \section{Introduction}
The quantization of the gravitational interaction has crystallized as a considerably more challenging endeavor than the quantization of matter fields. Paired with the success of classical general relativity when it comes to the accuracy of predictions, the question has been raised whether we are... |
1,116,691,497,433 | arxiv | \section{Introduction}\label{sec:introduction}}
\IEEEPARstart{S}{ince} the invention of writing over 5000 years ago, people have been recording a great variety of things in written form. Up until the 20\textsuperscript{th} century, writing has been the primary way of storing information across generations. Consequent... |
1,116,691,497,434 | arxiv | \section{Introduction}
Interactions between a gaseous disk and embedded proto-planetary cores could be decisive to understand the distribution of semi-major axis, eccentricities and masses of extra-solar giant planets (Perryman 2000, Schneider 2004). Exchanges of angular momentum can efficiently operate through the exc... |
1,116,691,497,435 | arxiv | \section{Introduction}
\vspace{-1mm}
\label{introduction}
Video deblurring is a fundamental yet challenging task in low-level computer vision and graphics communities. It aims to restore the latent frames from a blurry video sequence. Serving as a preprocessing technique, video deblurring has wide applications suc... |
1,116,691,497,436 | arxiv | \section*{Introduction}
The enormous amount of data produced by the Next-Generation Sequencing (NGS) technologies opens the way for a more comprehensive characterization of mechanisms at the molecular level, which are at the basis of cellular life and may have a role in the occurrence and progress of disorders and dise... |
1,116,691,497,437 | arxiv | \section{Introduction}
\label{Intro}
Ferromagnetic two-dimensional (2D) structures are of uttermost importance in spintronics applications~\cite{Cinchetti2017_NatMat}. Such 2D magnetic systems can either be 2D Van der Waals (vdW) ferromagnets~\cite{gong2017_Nat, huang2017_Nat}, or ultrathin magnetic overlayers~\cite{Ga... |
1,116,691,497,438 | arxiv | \section{Introduction}
Weakly bound nuclei near the drip-line have properties which are not seen in strongly bound stable nuclei. The neutron halo is an typical example~\cite{Tanihata1985,Tanihata2013}. Apart from quantal penetration caused by the small separation energy, the neutron pairing correlation plays crucial ... |
1,116,691,497,439 | arxiv | \section{Introduction}\label{Introduction}
In homological algebra the projective and injective modules play a central role. The analogue in Gorenstein homological algebra are the Gorenstein projective and Gorenstein injective modules. These were defined by Auslander and Bridger in \cite{AB69} for a two sided Noetherian... |
1,116,691,497,440 | arxiv | \section{Introduction}
\label{sec1}
\newabbreviation{lbm}{LBM}{lattice Boltzmann method}
\newabbreviation{lb}{LB}{lattice Boltzmann}
\newabbreviation{ns}{NS}{Navier-Stokes}
\newabbreviation{pde}{PDE}{partial differential equation}
Mandelic acid is an aromatic alpha-hydroxy acid, with formula ${\rm C}_8{\rm H}_8{\rm O}_... |
1,116,691,497,441 | arxiv | \section{Introduction}
The field theory approach to gravity, see e.g. \cite{Feynman:1996kb}, tells us that gravity is not a gauge theory. Indeed, the carriers of force in a gauge theory (such as e.g. Maxwell electrodynamics) are spin one particles. For this reason there are two types of charged objects interacting by... |
1,116,691,497,442 | arxiv | \section{Introduction}\label{s:intro}
The stellar spectra even at modest resolution contain wealth of information
on stellar parameters. In fact, most of the classification work has been
done using medium/low resolution spectra. Hydrogen lines are good indicators
of temperature and luminosity for a good range in ... |
1,116,691,497,443 | arxiv | \section{Introduction}
This paper is devoted to show the existence and uniqueness of logarithmic models for any holomorphic foliation on $({\mathbb C}^n,0)$ of generalized hypersurface type. In the case of $n=2$, this result has been obtained by N. Corral in \cite{Cor}. The main result is Theorem \ref{teo:main} in th... |
1,116,691,497,444 | arxiv | \section{Introduction}
In recent years, computer vision has made tremendous progress across many complex recognition
tasks, including image classification \cite{krizhevsky2012nips,zheng2017learning}, image captioning \cite{chen2017sca,johnson2016cvpr,xu2015show,you2016image}, image generation \cite{tang2014nips,zhang2... |
1,116,691,497,445 | arxiv | \section{Introduction}
\label{sec:intro}
\ \ It has long been suggested that antikaon ($K^-$) condensation should be realized in high density hadronic matter\cite{kn86,mtt93,t95,lbm95,fmmt96,l96,pbpelk97}.\footnote{We consider antikaon ($K^-$) condensation, while we conventionally call it ``kaon condensation''.} It is... |
1,116,691,497,446 | arxiv | \section{Introduction}
In the last decades, the theory of optimal transport has made impressive inroads into other disciplines of mathematics, probably most notably with the Lott--Sturm--Villani theory \cite{LV09,Stu06a,Stu06b} of synthetic Ricci curvature bounds for metric measure spaces. More recently, optimal trans... |
1,116,691,497,447 | arxiv | \section{Introduction and Definitions}
\begin{theorem}[Waring's Problem/Hilbert-Waring Theorem]
For every integer $k \geq 2$ there exists a positive integer $g(k)$ such that every positive integer is the sum of at most $g(k)$ $k$-th powers of integers.
\end{theorem}
The idea behind Waring's Problem -- examining sums ... |
1,116,691,497,448 | arxiv | \subsection*{}%
\hbox{\hspace{.05\hsize}\defbox{\medskip#1\bigskip}}%
\subsection*{}}
\def{}
\def{\hbox{\it\tiny T}}{{\hbox{\it\tiny T}}}
\def\phantom{-}{\phantom{-}}
\def\buildrel{\rm w}\over\longrightarrow{\buildrel{\rm w}\over\longrightarrow}
\def\buildrel{\rm v}\over\longrightarrow{\buildrel{\rm v}\over\lon... |
1,116,691,497,449 | arxiv | \section{Introduction}
\label{sec:intro}
The $^{13}$C ($\alpha$,n) $^{16}$O\ reaction plays an important role in nuclear physics and
astrophysics. Many conventional nuclear physics experiments suffer from
background which is produced by the $^{13}$C ($\alpha$,n) $^{16}$O\ reaction in carbon
buildup on the target althou... |
1,116,691,497,450 | arxiv | \chapter{Speculative Analysis to Predict Impact of Architectural Decay on the Implementation of Software Systems}
\label{sec:prediction}
\section{Foundation}
\label{sec:emp3_found}
This chapter discusses the dissertation's third large study, which aims to solve a prediction problem by using
supervised machine learnin... |
1,116,691,497,451 | arxiv | \section{Introduction} \label{sec:intro}
The successful launch of the James Webb Space Telescope (JWST, \citealt{2006SSRv..123..485G}) and current progress in building of the ground-based extremely large telescopes (ELTs) are opening a new era of in-depth studies of extrasolar planets \citep{2014PASP..126.1134B,2015P... |
1,116,691,497,452 | arxiv | \section{Introduction}
Because of the difficulty to calculate the
physical accretion rate to the BH in an AGN, a dimensionless accretion
rate can be defined and estimated based on the bolometric luminosity and
BH mass, $\dot{m} = \frac{L_{bol}}{L_{Edd}}$. This parameter
can be used as the substitute for the actu... |
1,116,691,497,453 | arxiv | \section{Introduction}
The transformer \citep{vaswani2017attention} is a deep learning architecture commonly used to process sequences of data, such as text. Thanks to multi-head self-attention, the transformer builds contextual embeddings by capturing the relationships between the sequence elements. While being most ... |
1,116,691,497,454 | arxiv | \section*{Introduction}
Let $X$ be a complex algebraic variety. We call a regular map $p\colon X
\to X^{\rm qp}$ from $X$ to a quasi--projective variety $X^{\rm qp}$ a {\it
quasi--projective reduction} of $X$ if every regular map $f \colon X \to
Z$ to a quasi--projective variety $Z$ factors uniquely through $p$,
i.e... |
1,116,691,497,455 | arxiv | \section{Introduction\label{s1}}
Let $\sR^-$ and $\sR^+$ be, respectively, the subsets of all
negative and all positive real numbers, and let $\chi_E$ refer to
the characteristic function of the subset $E$ of the set of real
numbers $\sR$, i.e.
$$
\chi_E(t):=\left \{
\begin{array}{ll}
1 & \text{ if } t\in ... |
1,116,691,497,456 | arxiv | \section{Conclusion and Future Work}
This study demonstrates that SE-MoE, MoE training and inference system, can satisfy requirements well from NLP and CV tasks. It not only addresses the issue of large model about training and inference, but also achieves competitive performance. In the future, we will explore a unif... |
1,116,691,497,457 | arxiv | \section{Introduction}
The complexity and diversity of today's media landscape provides many challenges for researchers studying news. In this paper, we introduce
a broad news benchmark data set, called the NEws LAndscape (NELA2017) data set, to facilitate
the study of many problems in this domain. The data set
incl... |
1,116,691,497,458 | arxiv | \section{Introduction}
In \cite{ParSht2}, two of the authors of this paper have obtained
the complete power asymptotic expansion of the integrated density of
states of Schr\"odinger operators
\begin{equation*}
H= -\Delta +V
\end{equation*}
acting in $ \mathbb R^d$ assuming that the real-valued potential $V$ is either ... |
1,116,691,497,459 | arxiv | \section{Introduction and description of the results}\label{s1}
Non-semisimple Lie algebras play an important role in physics where they are frequently used to study various
physical systems and explain diverse physical phenomena. For example one could mention Schr\"odinger algebras
and groups, see \cite{DDM}, con... |
1,116,691,497,460 | arxiv | \section{Introduction}
In outsourcing the data storage to cloud servers, a mechanism, known as access control, is required to guarantee users' access to the appropriate data. For individual use, access control can be simply designed using asymmetric cryptography.
Data, encrypted by a public key, can be decrypted by ... |
1,116,691,497,461 | arxiv | \section{Introduction}
Computation of classical effective lagrangians that represent motions of wave packets in
theories involving field-theoretic dispersion relations with Lorentz-violating corrections has been of
considerable interest in the recent literature.
Specifically, the Standard Model Extension (SME) provide... |
1,116,691,497,462 | arxiv | \section{Introduction}
This paper reports on some recent progress that has been made in
the analytical modeling of defect formation, far from threshold,
in pattern forming physical systems. We will take a moment here to
very briefly sketch the physical and mathematical background that
motivates what is done in this pa... |
1,116,691,497,463 | arxiv | \section{Introduction}
\subsection{Background and motivation}
Inspiralling and coalescing binary neutron stars are key sources for
ground-based gravitational wave (GW) detectors \cite{CutlerThorne}.
An important science goal in the detection of such sources is to
obtain robust information on the highly uncertain equa... |
1,116,691,497,464 | arxiv | \section{Introduction}
Over the past few decades, inflation has been established as the leading paradigm for describing the early universe. It proposes a period of rapidly accelerated expansion during the first fraction of a second after the universe came to be \cite{Guth:1980zm,Linde:1981mu,Albrecht:1982wi}. At the cl... |
1,116,691,497,465 | arxiv | \section{Introduction}
In this paper, we study semi-classical quasimodes of WKB-type, formally associated with the low lying spectrum of a
Schr\"odinger operator $H_\hbar$ on a vector bundle $\mathcal{E}$ over a smooth Riemannian manifold $M$. More precisely, given an operator of the form
\begin{equation*}
H_\hbar ... |
1,116,691,497,466 | arxiv |
\section{Summary} \label{SEC:Conclusion}
In this paper we presented a database of real ham radio recordings with parallel clean and distorted speech data, offering a novel challenge for speech activity detection, enhancement, and reconstruction.
The database consists of diverse noise conditions wi... |
1,116,691,497,467 | arxiv | \section{Introduction and statement of a main result}\label{2sec1}
Let us denote the family of all meromorphic functions $f$ with no poles in the unit disk $\mathbb{D}:=\{z \in \mathbb{C}:|z|<1\}$ of the form
\begin{equation}\label{deq1}
f(z)=z+a_2z^2+a_3z^3+\cdots
\end{equation}
by $\mathcal{A}$. Clearly, functions in... |
1,116,691,497,468 | arxiv |
\section{Calculating $\fisherInfMark_{\chParMark}$}\label{app:chFIM}
To calculate elements of $\fisherInfMark_{\chParMark}$ based, we derive the derivatives $\partial [\bm{M}]_{n,t}/\partial \parameterMark_{\chParMark}$. For delays we obtain
\begin{align}
\frac{\partial \bm{M}}{\partial \tau_{\mathrm{b}}... |
1,116,691,497,469 | arxiv | \section{#1}\setcounter{equation}{0}}
\renewcommand{\baselinestretch}{1.2}
\begin{document}
\bibliographystyle{physics}
\begin{titlepage}
\begin{flushright}
{\sf\large TUM-T31-21/92}\\
{\sf\large July 1992}
\end{flushright}
\vspace{10mm}
\begin{center}
{\huge Current correlators to all orders in\\
\vspace*{4mm}
the... |
1,116,691,497,470 | arxiv | \section{Introduction}
Adding to the landscape of embedded systems, cloud computing, networking, and telecommunications -- \textit{edge computing} is proposed to provide solutions for various cyber-physical systems (CPS) and applications, such as augmented reality, predictive functions e.g. for anomaly detection, ... |
1,116,691,497,471 | arxiv | \section*{Introduction}
Let $A$ be a unital associative algebra over a field $k$. M.E.
Sweedler's result \cite[Theorem 7.0.4]{Sw} which states that the
functor ${\rm Hom} (- , \, A) : {\rm CoAlg}_k \to {\rm Alg}_k
^{\rm op}$ from the category of coalgebras over $k$ to the
opposite of the category of $k$-algebras has a ... |
1,116,691,497,472 | arxiv | \section{INTRODUCTION \label{sec:intro}}
The desire to manipulate visible light has existed for well over 2000 years \cite{Smith2015}.
Research on this topic has borne several technologies key to modern life, from spectacles to fibre optical cables.
For at least the last two decades, technology trends have pushed for ... |
1,116,691,497,473 | arxiv | \section{Appendix A: Details on the Templates}
\begin{table*}[!th]
\centering
\caption{This table presents details on the templates utilized in our paper. Here, we analyze 37 relations in ConceptNet \cite{speer2017conceptnet}. }
\label{tab:template}
\begin{tabular}{c|m{8.5cm}|c}
\hline
\textbf{Re... |
1,116,691,497,474 | arxiv | \section*{Acknowledgements}
\noindent We express our gratitude to our colleagues in the CERN
accelerator departments for the excellent performance of the LHC. We
thank the technical and administrative staff at the LHCb
institutes.
We acknowledge support from CERN and from the national agencies:
CAPES, CNPq, FAPERJ and... |
1,116,691,497,475 | arxiv | \section{Introduction}\vspace{-0mm}
\label{sec:intro}
The fundamental challenge of integrated planning and learning is to design an autonomous agent that can plan its actions to maximize its expected total rewards while interacting with an unknown task environment.
Recent research efforts tackling this challenge have ... |
1,116,691,497,476 | arxiv | \section{Introduction}
\label{sec:introduction}
Failure management is one of the fundamental instruments that allows network operators to provide communication services that are much more reliable than the individual network components (nodes and links). It allows reacting to failures of network components by reconfig... |
1,116,691,497,477 | arxiv | \section{Introduction}
Throughout this paper, we denote the \textit{complex plane} by $\mathbb{C}$ and set of integers greater than zero by $\mathbb{N}$.
We assume the function $f:\mathbb{C}\rightarrow\mathbb{C}$ is \textit{transcendental entire function} (TEF) unless otherwise stated.
For any $n\in\mathbb{N}, \;\; f... |
1,116,691,497,478 | arxiv | \section{Introduction}
Let $\Gamma$ be a totally ordered abelian group, and $\Gamma^{+}:=\{x\in\Gamma : x \ge 0\}$ the positive cone of $\Gamma$.
A dynamical system $(A,\Gamma^{+},\alpha)$ is a system consisting of a $C^*$-algebra $A$, an action
$\alpha:\Gamma^{+}\rightarrow \operatorname{End}{A}$ of $\Gamma^{+}$ by ... |
1,116,691,497,479 | arxiv | \section{Introduction}
Let $G$ be quasi-split reductive group defined over a $p$-adic field. The Plancherel measure is an analytic invariant associated with a parabolic induction on $G$. It was conjectured by Langlands, \cite{Lang}, that this invariant is a ratio of certain $L$-functions and hence of arithmetic sig... |
1,116,691,497,480 | arxiv | \section{Introduction}
Probabilistic databases (PDBs) provide a framework for representing uncertain data in databases. In database theory, they have been intensely studied since the late 1990s \cite{Suciu+2011,VandenBroeckSuciu2017}. Most efforts have been directed towards tuple-independent relational databases \emph{... |
1,116,691,497,481 | arxiv | \section{Introduction}
\subsection{Background and Motivations}
{\color{blue} Wireless communication and sensing are both indispensable for critical machine-type applications, e.g., the 5th generation (5G) and the future 6th generation (6G) networks~\cite{Saad2020,You2020,ITUITShandbook}. Nevertheless, the proliferation... |
1,116,691,497,482 | arxiv | \section{Models of gas expulsion}
\subsection{ICs for embedded clusters in MOND}\label{ics}
MOND has been tested for decades. On large scales, MOND encounters several unsolved challenges. The strong and weak lensing data from clusters of galaxies showed that MOND also requires dark matter such as neutrinos \citep{Natar... |
1,116,691,497,483 | arxiv |
\section{Introduction}
Conditional density estimation (CDE) refers to the problem of estimating a conditional density $p(y\vert x)$ for the input $x$ and target $y$. In contrast to classification where the target $y$ is simply a discrete class label, $y$ is typically continuous or high-dimensional in CDE. Furth... |
1,116,691,497,484 | arxiv | \section{\label{sec:introductionl}Introduction}
\subsection{\label{subsec:description}Problem Description}
With the advancement of experimental probes on the quantum spin system in both one-dimension (1D)\cite{Jompol2009} and two-dimension (2D)\cite{Gross2017}, rich ground state (GS) phases such as the disordered T... |
1,116,691,497,485 | arxiv | \section{Introduction}
\label{sec:intro}
Speaker verification solves the task whether two utterances are spoken by the same person. A recent shift towards neural network based speaker verification systems resulted in significantly better performance compared to the more traditional i-vector based systems \cite{x_vec... |
1,116,691,497,486 | arxiv | \section{Introduction}
A multiplet of the Standard Model gauge group $SU(2)_L\times
U(1)_Y$ \cite{hisano03} would be the simplest candidate of dark
matter as it requires no additional `ad hoc' interaction or
couplings. Its electroweak interaction leads to a right thermal
relic density if its mass is in the multi TeV ra... |
1,116,691,497,487 | arxiv | \section{Introduction and main results}
One of the most striking properties of holomorphic functions in several variables is the fact that the property of being holomorphic can be checked separately on each variable while the others are kept as constants. This fact is known as Hartogs Theorem. Another remarkable proper... |
1,116,691,497,488 | arxiv | \section{Idea Management}
Idea Management (IM) is the process by which organizations approach their communities of clients, employees, suppliers, and interested stakeholders to (1) request ideas, (2) collect and (3) evaluate them, and (4) select the most promising ones to source their innovation needs or to address a ... |
1,116,691,497,489 | arxiv | \section{Introduction}
Since the discovery of halo nuclei \cite{THH85}, the physics of exotic nuclei attracted much interest in the nuclear
physics community \cite{TSK13,SLY03}. Halo nuclei are characterized by a low separation energy of the last nucleon(s),
and therefore by an unusually large radius. More gener... |
1,116,691,497,490 | arxiv | \section{Introduction}
We consider the problem
\begin{equation}
\label{eq:LowRankOpti}
\min_{X \in \mathbb{R}_{\le r}^{m \times n}} f(X)
\end{equation}
of minimizing a differentiable function $f : \mathbb{R}^{m \times n} \to \mathbb{R}$ with locally Lipschitz continuous gradient on the \emph{determinantal variety} \cit... |
1,116,691,497,491 | arxiv | \section{Introduction}
The bilateral and nonlocal means filters \cite{tomasi1998bilateral,buades2005non} are widely used for edge-preserving smoothing and denoising of images \cite{paris2009bilateral,milanfar2013tour}. These are instances of kernel filters, where the similarity (affinity) between pixels is measured us... |
1,116,691,497,492 | arxiv | \section{Introduction}
The transport of radiation through dust plays a central role in many astrophysical objects as dust is efficient in absorbing and scattering ultraviolet (UV) through near-infrared photons and re-radiating the absorbed energy in the infrared and submillimeter (submm).
The interpretation of obser... |
1,116,691,497,493 | arxiv | \section{Introduction}
In recent times, our knowledge of non-perturbative string theory has greatly
progressed. A key element in this progress has been our ability to
identify certain quantum mechanical (or field-theoretical) systems which
describe non perturbative states in string theory. More precisely, BPS states
in... |
1,116,691,497,494 | arxiv | \section{\bf Introduction}
Jacobi structure on a manifold $M$ (Jacobi manifold) has been introduced by A. Lichnerowicz \cite{Lich2} and, as a local Lie algebra structure on $C^{\infty}(M,R)$,
by A. Kirillov \cite{Ki}. Jacobi structures have all properties of the Poisson structures, except that they are not necessarily... |
1,116,691,497,495 | arxiv | \section{Introduction}
\label{sec:introduction}
\begin{figure}[tb]
\centering
\includegraphics[width=0.85\linewidth]{Teaser}
\caption{Results of face swapping and additional visual attribute editing with the proposed system. The face regions of images in the first column are embedded to the images in the s... |
1,116,691,497,496 | arxiv |
\section{Introduction}\label{sec:introduction}
Smart contracts are programs stored on blockchains to execute transactions.
In recent years, smart contracts have been widely used for various purposes such as
to offer financial services~\cite{smartcontractusecase}.
Ethereum~\cite{ethereum_yellow_paper} is the largest d... |
1,116,691,497,497 | arxiv | \section{Introduction}\label{sec:intro}
\input{content/introduction.tex}
\section{Preliminaries and Problem Formulation}\label{sec:prelim}
\input{content/prelim.tex}
\section{Convergence Analysis}\label{sec:analysis}
\input{content/convergence.tex}
\section{Algorithm Design}\label{sec:alg}
\input{content/algorithm.... |
1,116,691,497,498 | arxiv | \section{Introduction}\label{sec:intro}
In its simplest realization inflationary cosmology can be effectively described as a quasi-deSitter space time. Early studies\cite{polyakov1,IR1,IR2,allen,folaci,dolgov} revealed that de Sitter space time features infrared instabilities and profuse particle production in inte... |
1,116,691,497,499 | arxiv |
\section{Introduction}
\label{section:intro}
LIS has been identified as one of the key technologies for beyond 5G \cite{husha_data,husha_data2,husha_asign,husha_pos}. In Fig. \ref{fig:LIS_concept} we show the concept of a LIS serving multiple users simultaneously. The LIS is a continuous radiating surface located ... |
1,116,691,497,500 | arxiv | \section{\label{sec:Introduction}Introduction}
Sawtooth oscillations\cite{Goeler1974} are internal relaxation events in a tokamak that lead to a rapid drop of core electron temperature. A significant question for sawtooth oscillations is what is the cause of the short crash time. In the traditional Kadomtsev model\ci... |
1,116,691,497,501 | arxiv | \section{Introduction}
The first generation of gravitational waves (GWs) detectors was based
on mechanical resonance in large aluminium cylinders that is triggered by gravitational wave flying through the detector \cite{Weber0}.
This type of GWs detectors, so-called Weber bars, are still operating connected in the w... |
1,116,691,497,502 | arxiv | \section*{Methods}
\label{sec:model}
Our model is meant for ferromagnetic insulators and it assumes that electrons and phonons are in local equilibrium at every moment in time. Consequently, they are considered as a single system referred to as ``the lattice''. The magnetization dynamics is given by the standard Landau... |
1,116,691,497,503 | arxiv | \section{Introduction}
\label{introduction}
Much attention has been paid to artificial lipid bilayer membranes as model systems
of biological cell membranes~\cite{AlbertsBook}.
They exhibit a wide variety of complex phenomena in both statics and dynamics, since
lipid densities, membrane deformation and surrounding... |
1,116,691,497,504 | arxiv | \section{Introduction}\label{sec:intro}
The impulsive phase of solar flares is characterised by intense emission of microwaves and hard X-rays (HXR), showing the presence of non-thermal electrons in the corona and chromosphere, respectively. These electrons are believed to be accelerated by the magnetic energy release... |
1,116,691,497,505 | arxiv | \section{The Advantages and Limitations of the Deconfounder Method}
We first discuss several advantages offered by the deconfounder
method. We then examine the assumptions required by the method and
discuss its limitations.
\subsection{The Deconfounder Method}
Suppose that we have a simple random sample of $n$ unit... |
1,116,691,497,506 | arxiv | \section{Introduction}\label{sec:intr}
Observations of high-redshift supernovae indicate that the universe
is accelerating at the present stage~\cite{SN} and this accelerating
expansion also has been confirmed by many other cosmological
experiments, such as observations of large scale structure (LSS)
\cite{LSS}, and m... |
1,116,691,497,507 | arxiv | \section{INTRODUCTION}
\IEEEPARstart{T}{he} accurate wireless channel characterization is, currently, of paramount importance for the understanding, evaluation and design of future wireless communication systems, which will operate under stringent requirements of capacity, reliability, latency, and scalability, to ena... |
1,116,691,497,508 | arxiv | \section{Introduction}
Double-lined eclipsing binaries provide a unique opportunity to test various theoretical aspects of modern astrophysics. Their absolute parameters of masses and radii can be determined with outstanding accuracy, often with errors of 1\% \citep{Torres2010}. Because of the precise estimates of s... |
1,116,691,497,509 | arxiv | \section{Introduction and summary}
\noindent
Noncommutative deformations of gauge field theory provide
a controlled theoretical framework beyond locality~\cite{SWDNS}.
Of particular importance are noncommutative instantons
(see e.g.~\cite{NSNCH, LPTWI} and references therein),
which are BPS~configurations in four dim... |
1,116,691,497,510 | arxiv | \section{Introduction}
Recently there has been a burst of activity dealing with quadratic
gravitation. For example, the curvature-squared terms added to the usual
Einstein action with cosmological constant have played a role in two recent
investigations of four-dimensional gravity: in critical gravity [1], and in... |
1,116,691,497,511 | arxiv | \section{Introduction}\label{sec:intro}
A \emph{flat waveguide} is a domain $\Omega$ in $\mathbb{R}^{n+m}$
which can be written as a product
of a bounded open subset $\omega$ with $\mathbb{R}^{n}$:
\begin{equation*}
\omega \subseteq \mathbb{R}^{m},\qquad
\Omega=\mathbb{R}^{n}\times \omega\subseteq \mathbb{R}^{n}_... |
1,116,691,497,512 | arxiv | \section{Introduction}
Accurate 3D human-pose estimation from a monocular RGB image finds applications to robotics, virtual/augmented reality, surveillance, and human computer interaction. The diverse variations in background, clothing, pose, occlusions, illumination, and camera parameters in real-world scenarios make... |
1,116,691,497,513 | arxiv | \section{Introduction}
\label{sec:introduction}
Deterministic thermostats are widely used to simulate equilibrium physical systems
described by ensembles other than microcanonical (constant energy and volume, $(E, V)$), such as constant
temperature-volume $(T, V)$ or temperature-pressure $(T, p)$
\cite{Nose91,Morriss... |
1,116,691,497,514 | arxiv | \section{Introduction and results}
In the following we will consider the standard even dimensional symplectic vector space $(\ensuremath{\mathdj{C}}^n,\omega_0:=dx_1\wedge dy_1+\hdots+dx_n \wedge dy_n)$, as well as the projective space $(\ensuremath{\ensuremath{\mathdj{C}}}P^n,\omega_{\operatorname{FS},r})$ endowed wit... |
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