id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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1,801.05169 | A two-parameter eigenvalue problem for a class of block-operator
matrices | We consider a symmetric block operator spectral problem with two spectral
parameters. Under some reasonable restrictions, we state localisation theorems
for the pair-eigenvalues and discuss relations to a class of non-self-adjoint
spectral problems.
| math.SP | we consider a symmetric block operator spectral problem with two spectral parameters under some reasonable restrictions we state localisation theorems for the paireigenvalues and discuss relations to a class of nonselfadjoint spectral problems | [['we', 'consider', 'a', 'symmetric', 'block', 'operator', 'spectral', 'problem', 'with', 'two', 'spectral', 'parameters', 'under', 'some', 'reasonable', 'restrictions', 'we', 'state', 'localisation', 'theorems', 'for', 'the', 'paireigenvalues', 'and', 'discuss', 'relations', 'to', 'a', 'class', 'of', 'nonselfadjoint',... | [-0.12801422874326818, 0.053616286924807355, -0.06215956277446821, 0.13676523737376556, -0.10636642782628769, -0.16703296839841641, 0.011847883986774832, 0.4187281266786158, -0.2869563285494223, -0.2233832039637491, 0.19714027380541665, -0.23782381162163801, -0.12027378601487726, 0.18515087681589648, -0.102844494715100... |
1,801.0517 | Universal disorder-induced broadening of phonon bands: from disordered
lattices to glasses | The translational symmetry of solids gives rise to the existence of
low-frequency phonons. In ordered systems, some phonons characterized by
different wavevectors are degenerate, i.e. they share the same frequency
$\omega$; in finite-size systems, phonons form a discrete set of bands with
$n_q(\omega)$-fold degenerac... | cond-mat.stat-mech cond-mat.dis-nn cond-mat.mtrl-sci cond-mat.soft | the translational symmetry of solids gives rise to the existence of lowfrequency phonons in ordered systems some phonons characterized by different wavevectors are degenerate ie they share the same frequency omega in finitesize systems phonons form a discrete set of bands with n_qomegafold degeneracy here we focus on u... | [['the', 'translational', 'symmetry', 'of', 'solids', 'gives', 'rise', 'to', 'the', 'existence', 'of', 'lowfrequency', 'phonons', 'in', 'ordered', 'systems', 'some', 'phonons', 'characterized', 'by', 'different', 'wavevectors', 'are', 'degenerate', 'ie', 'they', 'share', 'the', 'same', 'frequency', 'omega', 'in', 'fini... | [-0.16044515339069862, 0.23670654408023006, -0.05171651100204517, 0.0467295416313048, -0.05386284290675501, -0.1366666332116259, 0.07042714229309702, 0.35214362361040885, -0.28779090192459034, -0.2495097451057041, 0.04203462491258521, -0.28497265105242614, -0.12303090568147142, 0.1629148888307219, 0.011976820516464927,... |
1,801.05171 | Deep Multi-Spectral Registration Using Invariant Descriptor Learning | In this paper, we introduce a novel deep-learning method to align
cross-spectral images. Our approach relies on a learned descriptor which is
invariant to different spectra. Multi-modal images of the same scene capture
different signals and therefore their registration is challenging and it is not
solved by classic a... | cs.CV | in this paper we introduce a novel deeplearning method to align crossspectral images our approach relies on a learned descriptor which is invariant to different spectra multimodal images of the same scene capture different signals and therefore their registration is challenging and it is not solved by classic approache... | [['in', 'this', 'paper', 'we', 'introduce', 'a', 'novel', 'deeplearning', 'method', 'to', 'align', 'crossspectral', 'images', 'our', 'approach', 'relies', 'on', 'a', 'learned', 'descriptor', 'which', 'is', 'invariant', 'to', 'different', 'spectra', 'multimodal', 'images', 'of', 'the', 'same', 'scene', 'capture', 'diffe... | [0.008359171689816695, -0.0579099922926173, -0.14169515681085215, 0.054420687621185446, -0.10810980193723901, -0.1797027238722922, -0.0032314518437243436, 0.5012872486743105, -0.24836361873112306, -0.34934984223854515, 0.05700300591058653, -0.2730367849502681, -0.1975321838467875, 0.19049409042824716, -0.18201447640616... |
1,801.05172 | Information-entropic measures in free and confined hydrogen atom | Shannon entropy ($S$), R{\'e}nyi entropy ($R$), Tsallis entropy ($T$), Fisher
information ($I$) and Onicescu energy ($E$) have been explored extensively in
both \emph{free} H atom (FHA) and \emph{confined} H atom (CHA). For a given
quantum state, accurate results are presented by employing respective
\emph{exact} ana... | quant-ph physics.atom-ph | shannon entropy s renyi entropy r tsallis entropy t fisher information i and onicescu energy e have been explored extensively in both emphfree h atom fha and emphconfined h atom cha for a given quantum state accurate results are presented by employing respective emphexact analytical wave functions in r space the pspace... | [['shannon', 'entropy', 's', 'renyi', 'entropy', 'r', 'tsallis', 'entropy', 't', 'fisher', 'information', 'i', 'and', 'onicescu', 'energy', 'e', 'have', 'been', 'explored', 'extensively', 'in', 'both', 'emphfree', 'h', 'atom', 'fha', 'and', 'emphconfined', 'h', 'atom', 'cha', 'for', 'a', 'given', 'quantum', 'state', 'a... | [-0.1217626539448527, 0.1616633194829634, -0.042319546337239444, 0.070755561885912, 0.012607608798694296, -0.19564752166983312, 0.02472520356241148, 0.36035419562316606, -0.2217364732624936, -0.27146807670634676, 0.026693232422985602, -0.3190588455668498, -0.0694452737863265, 0.1764704929023887, 0.015708075475441338, 0... |
1,801.05173 | Fully Convolutional Multi-scale Residual DenseNets for Cardiac
Segmentation and Automated Cardiac Diagnosis using Ensemble of Classifiers | Deep fully convolutional neural network (FCN) based architectures have shown
great potential in medical image segmentation. However, such architectures
usually have millions of parameters and inadequate number of training samples
leading to over-fitting and poor generalization. In this paper, we present a
novel highl... | cs.CV | deep fully convolutional neural network fcn based architectures have shown great potential in medical image segmentation however such architectures usually have millions of parameters and inadequate number of training samples leading to overfitting and poor generalization in this paper we present a novel highly paramet... | [['deep', 'fully', 'convolutional', 'neural', 'network', 'fcn', 'based', 'architectures', 'have', 'shown', 'great', 'potential', 'in', 'medical', 'image', 'segmentation', 'however', 'such', 'architectures', 'usually', 'have', 'millions', 'of', 'parameters', 'and', 'inadequate', 'number', 'of', 'training', 'samples', 'l... | [-0.012247469425332325, -0.03969625614377311, -0.049494890046603304, 0.05507440883787835, -0.11043776680591953, -0.19846502113077474, 0.013838321683053151, 0.45732325644991606, -0.25077975105987976, -0.3092649505739231, 0.09285614122711422, -0.23226680180033804, -0.2285754154670056, 0.19411058657537084, -0.169426325186... |
1,801.05174 | Searching for Exoplanets Using a Microresonator Astrocomb | Detection of weak radial velocity shifts of host stars induced by orbiting
planets is an important technique for discovering and characterizing planets
beyond our solar system. Optical frequency combs enable calibration of stellar
radial velocity shifts at levels required for detection of Earth analogs. A new
chip-ba... | physics.optics astro-ph.IM | detection of weak radial velocity shifts of host stars induced by orbiting planets is an important technique for discovering and characterizing planets beyond our solar system optical frequency combs enable calibration of stellar radial velocity shifts at levels required for detection of earth analogs a new chipbased d... | [['detection', 'of', 'weak', 'radial', 'velocity', 'shifts', 'of', 'host', 'stars', 'induced', 'by', 'orbiting', 'planets', 'is', 'an', 'important', 'technique', 'for', 'discovering', 'and', 'characterizing', 'planets', 'beyond', 'our', 'solar', 'system', 'optical', 'frequency', 'combs', 'enable', 'calibration', 'of', ... | [-0.10786994905326484, 0.15519784859113187, -0.037544379433643936, -0.0020027627835573613, -0.15159485608431672, -0.12893235003806588, 0.03652772394370688, 0.44815866168865487, -0.1575599136413075, -0.3223756624785952, 0.10316783376903974, -0.25553531675360913, -0.0814649066608784, 0.3366677812473802, -0.04590761730801... |
1,801.05175 | Maximization of the thermoelectric cooling of graded Peltier by
analytical heat equation resolution | Increasing the maximum cooling effect of a Peltier cooler can be achieved
through materials and device design. The use of inhomogeneous, FGM
(functionally graded materials) may be adopted in order to increase maximum
cooling without improvement of the zT (figure of merit), however these systems
are usually based on t... | physics.app-ph cond-mat.mtrl-sci | increasing the maximum cooling effect of a peltier cooler can be achieved through materials and device design the use of inhomogeneous fgm functionally graded materials may be adopted in order to increase maximum cooling without improvement of the zt figure of merit however these systems are usually based on the assump... | [['increasing', 'the', 'maximum', 'cooling', 'effect', 'of', 'a', 'peltier', 'cooler', 'can', 'be', 'achieved', 'through', 'materials', 'and', 'device', 'design', 'the', 'use', 'of', 'inhomogeneous', 'fgm', 'functionally', 'graded', 'materials', 'may', 'be', 'adopted', 'in', 'order', 'to', 'increase', 'maximum', 'cooli... | [-0.1291897008505728, 0.08077998923885073, -0.07226582908093884, 0.0056108626471497785, -0.08949204047439163, -0.12804430539435344, 0.04451211731153133, 0.36933608493672876, -0.31559818310518106, -0.3063989920140116, 0.08007818114216032, -0.2818061191767097, -0.10150922190197213, 0.2713431063035648, -0.0344834931718999... |
1,801.05176 | The hypergeometric function for the root system of type $A$ with a
certain degenerate parameter | We express explicitly the Heckman-Opdam hypergeometric function for the root
system of type A with a certain degenerate parameter in terms of the Lauricella
hypergeometric function.
| math.RT math.CA | we express explicitly the heckmanopdam hypergeometric function for the root system of type a with a certain degenerate parameter in terms of the lauricella hypergeometric function | [['we', 'express', 'explicitly', 'the', 'heckmanopdam', 'hypergeometric', 'function', 'for', 'the', 'root', 'system', 'of', 'type', 'a', 'with', 'a', 'certain', 'degenerate', 'parameter', 'in', 'terms', 'of', 'the', 'lauricella', 'hypergeometric', 'function']] | [-0.20108961127698421, 0.014788284360502776, -0.051010351413144514, 0.10512804676993535, -0.08963209619888893, -0.12347601866349578, 0.032111091539263725, 0.21645790668061146, -0.31636522681667256, -0.2121426176566344, 0.06713340649506651, -0.253691108754048, -0.22526714721551308, 0.23509839370560187, -0.02812618253609... |
1,801.05177 | A theorem on even pancyclic bipartite digraphs | We prove that a strongly connected balanced bipartite directed graph of order
$2a\geq 6$ with partite sets $X$ and $Y$ contains cycles of every length $2, 4,
\ldots , 2a$, provided $d(x)+d(y)\geq 3a$ for every pair of vertices $x$, $y$
either both in $X$ or both in $Y$.
| math.CO | we prove that a strongly connected balanced bipartite directed graph of order 2ageq 6 with partite sets x and y contains cycles of every length 2 4 ldots 2a provided dxdygeq 3a for every pair of vertices x y either both in x or both in y | [['we', 'prove', 'that', 'a', 'strongly', 'connected', 'balanced', 'bipartite', 'directed', 'graph', 'of', 'order', '2ageq', '6', 'with', 'partite', 'sets', 'x', 'and', 'y', 'contains', 'cycles', 'of', 'every', 'length', '2', '4', 'ldots', '2a', 'provided', 'dxdygeq', '3a', 'for', 'every', 'pair', 'of', 'vertices', 'x'... | [-0.2833068018105436, 0.1917256051117178, 0.03419464394608711, -0.015647663913191633, 0.05024520275579329, -0.24381656531601192, 0.045592489989197, 0.43677583653876123, -0.26784411249087847, -0.1967920554663114, 0.03861487593917929, -0.4211358542930573, -0.06175766533062337, 0.07892269797702418, -0.04401949059931522, -... |
1,801.05178 | Inter-thread Communication in Multithreaded, Reconfigurable Coarse-grain
Arrays | Traditional von Neumann GPGPUs only allow threads to communicate through
memory on a group-to-group basis. In this model, a group of producer threads
writes intermediate values to memory, which are read by a group of consumer
threads after a barrier synchronization. To alleviate the memory bandwidth
imposed by this m... | cs.AR | traditional von neumann gpgpus only allow threads to communicate through memory on a grouptogroup basis in this model a group of producer threads writes intermediate values to memory which are read by a group of consumer threads after a barrier synchronization to alleviate the memory bandwidth imposed by this method of... | [['traditional', 'von', 'neumann', 'gpgpus', 'only', 'allow', 'threads', 'to', 'communicate', 'through', 'memory', 'on', 'a', 'grouptogroup', 'basis', 'in', 'this', 'model', 'a', 'group', 'of', 'producer', 'threads', 'writes', 'intermediate', 'values', 'to', 'memory', 'which', 'are', 'read', 'by', 'a', 'group', 'of', '... | [-0.19845577413965573, 0.07111963632733337, -0.02810686449493528, 1.554847855506272e-05, -0.10362126296867841, -0.20221725970924156, 0.12968490780572053, 0.3726333302677202, -0.28950106365948747, -0.36350416665329416, 0.11141036619865817, -0.2047842963941224, -0.07565567049802677, 0.2290992850033652, -0.106074991927685... |
1,801.05179 | A criterion for the uniform eventual positivity of operator semigroups | Consider a $C_0$-semigroup $(e^{tA})_{t \ge 0}$ on a function space or, more
generally, on a Banach lattice $E$. We prove a sufficient criterion for the
operators $e^{tA}$ to be positive for all sufficiently large times $t$, while
the semigroup itself might not be positive. This complements recently
established crite... | math.FA math.AP | consider a c_0semigroup eta_t ge 0 on a function space or more generally on a banach lattice e we prove a sufficient criterion for the operators eta to be positive for all sufficiently large times t while the semigroup itself might not be positive this complements recently established criteria for the individual orbits... | [['consider', 'a', 'c_0semigroup', 'eta_t', 'ge', '0', 'on', 'a', 'function', 'space', 'or', 'more', 'generally', 'on', 'a', 'banach', 'lattice', 'e', 'we', 'prove', 'a', 'sufficient', 'criterion', 'for', 'the', 'operators', 'eta', 'to', 'be', 'positive', 'for', 'all', 'sufficiently', 'large', 'times', 't', 'while', 't... | [-0.13872452278155833, 0.1124840182398098, -0.07761235202729971, 0.11014875575916909, -0.0732737059609583, -0.14498128623039608, 0.027761117863771785, 0.3229870827621724, -0.28370349452527893, -0.18642936104555133, 0.14333829385542637, -0.28752116367490177, -0.10175735661367247, 0.2284796678780926, -0.04034356914281127... |
1,801.0518 | Stochastic grid bundling method for backward stochastic differential
equations | In this work, we apply the Stochastic Grid Bundling Method (SGBM) to
numerically solve backward stochastic differential equations (BSDEs). The SGBM
algorithm is based on conditional expectations approximation by means of
bundling of Monte Carlo sample paths and a local regress-later regression
within each bundle. The... | math.NA | in this work we apply the stochastic grid bundling method sgbm to numerically solve backward stochastic differential equations bsdes the sgbm algorithm is based on conditional expectations approximation by means of bundling of monte carlo sample paths and a local regresslater regression within each bundle the basic alg... | [['in', 'this', 'work', 'we', 'apply', 'the', 'stochastic', 'grid', 'bundling', 'method', 'sgbm', 'to', 'numerically', 'solve', 'backward', 'stochastic', 'differential', 'equations', 'bsdes', 'the', 'sgbm', 'algorithm', 'is', 'based', 'on', 'conditional', 'expectations', 'approximation', 'by', 'means', 'of', 'bundling'... | [-0.07843266709824093, -0.03391966964127571, -0.12398959904087968, 0.1161467264361319, -0.08655214625140352, -0.12135360317344787, 0.07083454845793626, 0.39053501833670884, -0.3076516968668789, -0.30838985761667614, 0.12831171260400606, -0.24910975453413783, -0.1713593735269481, 0.23913883864541627, -0.0427459940960210... |
1,801.05181 | Nonexistence of proper $p$-biharmonic maps and Liouville type theorems
I: case of $p\geq2$ | Let $u: (M, g)\to (N, h)$ be a map between Riemannian manifolds $(M, g)$ and
$(N, h)$. The $p$-bienergy of $u$ is defined by
$E_p(u)=\int_M|\tau(u)|^pd\nu_g$, where $\tau(u)$ is the tension field of $u$
and $p>1$. Critical points of $E_p(\cdot)$ are called $p$-biharmonic maps. In
this paper we will prove nonexistence... | math.DG | let u m gto n h be a map between riemannian manifolds m g and n h the pbienergy of u is defined by e_puint_mtauupdnu_g where tauu is the tension field of u and p1 critical points of e_pcdot are called pbiharmonic maps in this paper we will prove nonexistence result of proper pbiharmonic maps when pgeq2 in particular wh... | [['let', 'u', 'm', 'gto', 'n', 'h', 'be', 'a', 'map', 'between', 'riemannian', 'manifolds', 'm', 'g', 'and', 'n', 'h', 'the', 'pbienergy', 'of', 'u', 'is', 'defined', 'by', 'e_puint_mtauupdnu_g', 'where', 'tauu', 'is', 'the', 'tension', 'field', 'of', 'u', 'and', 'p1', 'critical', 'points', 'of', 'e_pcdot', 'are', 'cal... | [-0.1863847361256679, 0.11015811150272688, -0.04762700178970893, -0.001287660839346548, -0.050819361324732505, -0.16512672428662578, 0.006354163464469214, 0.3275786070028941, -0.28218621489902335, -0.228721089164416, 0.11235386746935547, -0.2940910592675209, -0.13058559178685147, 0.18190077445780237, -0.117725502215325... |
1,801.05182 | From Nodal Ring Topological Superfluids to Spiral Majorana Modes in Cold
Atomic Systems | In this work, we consider a 3D cubic optical lattice composed of coupled 1D
wires with 1D spin-orbit coupling. When the s-wave pairing is induced through
Feshbach resonance, the system becomes a topological superfluid with ring
nodes, which are the ring nodal degeneracies in the bulk, and supports a large
number of s... | cond-mat.quant-gas | in this work we consider a 3d cubic optical lattice composed of coupled 1d wires with 1d spinorbit coupling when the swave pairing is induced through feshbach resonance the system becomes a topological superfluid with ring nodes which are the ring nodal degeneracies in the bulk and supports a large number of surface ma... | [['in', 'this', 'work', 'we', 'consider', 'a', '3d', 'cubic', 'optical', 'lattice', 'composed', 'of', 'coupled', '1d', 'wires', 'with', '1d', 'spinorbit', 'coupling', 'when', 'the', 'swave', 'pairing', 'is', 'induced', 'through', 'feshbach', 'resonance', 'the', 'system', 'becomes', 'a', 'topological', 'superfluid', 'wi... | [-0.30794424432831113, 0.28125247202897025, -0.026200173026534605, -0.005920877814841971, -0.09555659293016391, -0.2233081983555275, 0.035372724329163115, 0.30554967803303706, -0.24373738121922447, -0.24375788512319993, -0.010473892616573721, -0.3113614244581158, -0.10484764162874989, 0.08999043132166322, 0.04686890933... |
1,801.05183 | Riemannian exponential and quantization | This article continues and completes our previous work [14] J. Phys. Commun.
2 (2018) 025007. First of all, we present two methods of quantization
associated with a linear connection given on a differentiable manifold, one of
them being the one presented in [14]. The two methods allow quantize functions
that come fro... | math-ph math.MP | this article continues and completes our previous work 14 j phys commun 2 2018 025007 first of all we present two methods of quantization associated with a linear connection given on a differentiable manifold one of them being the one presented in 14 the two methods allow quantize functions that come from covariant ten... | [['this', 'article', 'continues', 'and', 'completes', 'our', 'previous', 'work', '14', 'j', 'phys', 'commun', '2', '2018', '025007', 'first', 'of', 'all', 'we', 'present', 'two', 'methods', 'of', 'quantization', 'associated', 'with', 'a', 'linear', 'connection', 'given', 'on', 'a', 'differentiable', 'manifold', 'one', ... | [-0.0996990448684763, 0.06049932473165504, -0.08342619162344894, 0.02449711696816987, -0.0929335998489632, -0.11674821523996859, 0.022214328078947708, 0.3165583227666379, -0.2243135229929082, -0.29325608751278814, 0.10221494770395743, -0.25729324747670157, -0.1750701514025361, 0.21660241076201833, -0.06918363119041453,... |
1,801.05184 | Generalized K$\ddot{a}$hler Geometry and current algebras in classical
N=2 superconformal WZW model | I examine the Generalized K$\ddot{a}$hler geometry of classical $N=(2,2)$
superconformal WZW model on a compact group and relate the right-moving and
left-moving Kac-Moody superalgebra currents to the Generalized K$\ddot{a}$hler
geometry data using Hamiltonian formalism. It is shown that canonical Poisson
homogeneous... | hep-th | i examine the generalized kddotahler geometry of classical n22 superconformal wzw model on a compact group and relate the rightmoving and leftmoving kacmoody superalgebra currents to the generalized kddotahler geometry data using hamiltonian formalism it is shown that canonical poisson homogeneous space structure induc... | [['i', 'examine', 'the', 'generalized', 'kddotahler', 'geometry', 'of', 'classical', 'n22', 'superconformal', 'wzw', 'model', 'on', 'a', 'compact', 'group', 'and', 'relate', 'the', 'rightmoving', 'and', 'leftmoving', 'kacmoody', 'superalgebra', 'currents', 'to', 'the', 'generalized', 'kddotahler', 'geometry', 'data', '... | [-0.1623757740444374, 0.08731390410869182, -0.043810540326882766, 0.0982168437014157, -0.19280128412042993, -0.21753137046471238, -0.12895958392609713, 0.3539656251904708, -0.2751576058283637, -0.18319696223339701, 0.0867845684457924, -0.21075089275836945, -0.26262271753217603, 0.09780957131009974, -0.1465166205351677,... |
1,801.05185 | Tradeoff relations between accessible information, informational power,
and purity | The accessible information and the informational power quantify the maximum
amount of information that can be extracted from a quantum ensemble and by a
quantum measurement, respectively. Here, we investigate the tradeoff between
the accessible information (informational power, respectively) and the purity
of the sta... | quant-ph | the accessible information and the informational power quantify the maximum amount of information that can be extracted from a quantum ensemble and by a quantum measurement respectively here we investigate the tradeoff between the accessible information informational power respectively and the purity of the states of t... | [['the', 'accessible', 'information', 'and', 'the', 'informational', 'power', 'quantify', 'the', 'maximum', 'amount', 'of', 'information', 'that', 'can', 'be', 'extracted', 'from', 'a', 'quantum', 'ensemble', 'and', 'by', 'a', 'quantum', 'measurement', 'respectively', 'here', 'we', 'investigate', 'the', 'tradeoff', 'be... | [-0.11554882384148563, 0.16309373425462528, -0.09347417791059633, 0.07582937252624732, 0.002195036075831314, -0.1375756007619202, 0.11129740576829263, 0.30114194516917087, -0.2370974248739339, -0.33489524427753914, 0.11122865487886652, -0.29610571432502786, -0.09329172671078496, 0.20976794037706914, -0.0425848450636265... |
1,801.05186 | Functional ANOVA with Multiple Distributions: Implications for the
Sensitivity Analysis of Computer Experiments | The functional ANOVA expansion of a multivariate mapping plays a fundamental
role in statistics. The expansion is unique once a unique distribution is
assigned to the covariates. Recent investigations in the environmental and
climate sciences show that analysts may not be in a position to assign a unique
distribution... | stat.CO | the functional anova expansion of a multivariate mapping plays a fundamental role in statistics the expansion is unique once a unique distribution is assigned to the covariates recent investigations in the environmental and climate sciences show that analysts may not be in a position to assign a unique distribution in ... | [['the', 'functional', 'anova', 'expansion', 'of', 'a', 'multivariate', 'mapping', 'plays', 'a', 'fundamental', 'role', 'in', 'statistics', 'the', 'expansion', 'is', 'unique', 'once', 'a', 'unique', 'distribution', 'is', 'assigned', 'to', 'the', 'covariates', 'recent', 'investigations', 'in', 'the', 'environmental', 'a... | [-0.09676458815201408, 0.043855692806934556, -0.17806665647760153, 0.10969039800647085, -0.07590577242496822, -0.08540596947118285, 0.05485825626722848, 0.37107821333680363, -0.26586222814189064, -0.22513995786005306, 0.137937406788946, -0.26241089813115576, -0.1567859464871978, 0.1688102754867739, -0.06895658407833367... |
1,801.05187 | Future directions in locally compact groups | This text is the preprint version of the concluding chapter for the book New
Directions in Locally Compact Groups published by Cambridge University Press in
the series Lecture Notes of the LMS. The recent progress on locally compact
groups surveyed in that volume also reveals the considerable extent of the
unexplored... | math.GR | this text is the preprint version of the concluding chapter for the book new directions in locally compact groups published by cambridge university press in the series lecture notes of the lms the recent progress on locally compact groups surveyed in that volume also reveals the considerable extent of the unexplored te... | [['this', 'text', 'is', 'the', 'preprint', 'version', 'of', 'the', 'concluding', 'chapter', 'for', 'the', 'book', 'new', 'directions', 'in', 'locally', 'compact', 'groups', 'published', 'by', 'cambridge', 'university', 'press', 'in', 'the', 'series', 'lecture', 'notes', 'of', 'the', 'lms', 'the', 'recent', 'progress', ... | [-0.08688392689877963, 0.09396822220878676, -0.05969666974080435, 0.04268688434056085, -0.10260128723569663, -0.0639925967587764, 0.06280060491737831, 0.3560516415500497, -0.2519163972282984, -0.28331563487110367, 0.17554299193518572, -0.283750674182392, -0.14690006098496805, 0.21944400647946868, -0.15908385146723455, ... |
1,801.05188 | Geometrical bounds on irreversibility in open quantum systems | Clausius inequality has deep implications for reversibility and the arrow of
time. Quantum theory is able to extend this result for closed systems by
inspecting the trajectory of the density matrix on its manifold. Here we show
that this approach can provide an upper and lower bound to the irreversible
entropy produc... | quant-ph | clausius inequality has deep implications for reversibility and the arrow of time quantum theory is able to extend this result for closed systems by inspecting the trajectory of the density matrix on its manifold here we show that this approach can provide an upper and lower bound to the irreversible entropy production... | [['clausius', 'inequality', 'has', 'deep', 'implications', 'for', 'reversibility', 'and', 'the', 'arrow', 'of', 'time', 'quantum', 'theory', 'is', 'able', 'to', 'extend', 'this', 'result', 'for', 'closed', 'systems', 'by', 'inspecting', 'the', 'trajectory', 'of', 'the', 'density', 'matrix', 'on', 'its', 'manifold', 'he... | [-0.10873657308929112, 0.1138993379664455, -0.11717774409113363, 0.08114666196689498, -0.013990400735998438, -0.1470719408909125, 0.09394657995047358, 0.29841896894920084, -0.263272281259387, -0.2835911425007951, 0.11821616434220535, -0.2530488409212835, -0.15709656619444667, 0.2733509409729214, -0.0524395311395416, 0.... |
1,801.05189 | On the Kernel of $\mathbb{Z}_{2^s}$-Linear Hadamard Codes | The $\mathbb{Z}_{2^s}$-additive codes are subgroups of $\mathbb{Z}^n_{2^s}$,
and can be seen as a generalization of linear codes over $\mathbb{Z}_2$ and
$\mathbb{Z}_4$. A $\mathbb{Z}_{2^s}$-linear Hadamard code is a binary Hadamard
code which is the Gray map image of a $\mathbb{Z}_{2^s}$-additive code. It is
known th... | cs.IT math.IT | the mathbbz_2sadditive codes are subgroups of mathbbzn_2s and can be seen as a generalization of linear codes over mathbbz_2 and mathbbz_4 a mathbbz_2slinear hadamard code is a binary hadamard code which is the gray map image of a mathbbz_2sadditive code it is known that the dimension of the kernel can be used to give ... | [['the', 'mathbbz_2sadditive', 'codes', 'are', 'subgroups', 'of', 'mathbbzn_2s', 'and', 'can', 'be', 'seen', 'as', 'a', 'generalization', 'of', 'linear', 'codes', 'over', 'mathbbz_2', 'and', 'mathbbz_4', 'a', 'mathbbz_2slinear', 'hadamard', 'code', 'is', 'a', 'binary', 'hadamard', 'code', 'which', 'is', 'the', 'gray', ... | [-0.14575907262433477, 0.08600930627748496, -0.05207406266146347, 0.09384733936729833, 0.0010324086829581682, -0.18871022872391993, 0.010310843834426537, 0.37701343685513783, -0.2914773031732678, -0.24659094000000412, 0.1840193247786496, -0.25058500171333803, -0.1502771262361222, 0.23696118877308459, -0.082130453404540... |
1,801.0519 | Measurement of the inclusive $t\bar{t}$ cross-section in the lepton+jets
channel in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector | The inclusive $t\bar{t}$ production cross-section is measured in the
lepton+jets channel using 20.2 fb$^{-1}$ of proton--proton collision data at a
centre-of-mass energy of 8 TeV recorded with the ATLAS detector at the LHC.
Major systematic uncertainties due to the modelling of the jet energy scale and
$b$-tagging ef... | hep-ex | the inclusive tbart production crosssection is measured in the leptonjets channel using 202 fb1 of protonproton collision data at a centreofmass energy of 8 tev recorded with the atlas detector at the lhc major systematic uncertainties due to the modelling of the jet energy scale and btagging efficiency are constrained... | [['the', 'inclusive', 'tbart', 'production', 'crosssection', 'is', 'measured', 'in', 'the', 'leptonjets', 'channel', 'using', '202', 'fb1', 'of', 'protonproton', 'collision', 'data', 'at', 'a', 'centreofmass', 'energy', 'of', '8', 'tev', 'recorded', 'with', 'the', 'atlas', 'detector', 'at', 'the', 'lhc', 'major', 'syst... | [-0.03923651600279464, 0.14651947349813751, -0.057287311427615825, 0.11541256949276729, 0.022283308726132343, -0.09629537362307615, 8.367409654816643e-05, 0.3306705381904469, -0.16994135670810478, -0.42190554896827603, -0.0017006949638016522, -0.41592036654836817, 0.15645023081718837, 0.16589231325359252, 0.00971259997... |
1,801.05191 | New SUSY Fits for the ILC and CLIC | We review the MasterCode fits of several incarnations of the Minimal
Supersymmetric Standard Model (MSSM). These include the GUT models based on
mAMSB and SU(5), sub-GUT models as well as a model defined at low energies with
11 free parameters, the pMSSM11. The fit combines consistently measurements of
Higgs boson pr... | hep-ph | we review the mastercode fits of several incarnations of the minimal supersymmetric standard model mssm these include the gut models based on mamsb and su5 subgut models as well as a model defined at low energies with 11 free parameters the pmssm11 the fit combines consistently measurements of higgs boson properties se... | [['we', 'review', 'the', 'mastercode', 'fits', 'of', 'several', 'incarnations', 'of', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'mssm', 'these', 'include', 'the', 'gut', 'models', 'based', 'on', 'mamsb', 'and', 'su5', 'subgut', 'models', 'as', 'well', 'as', 'a', 'model', 'defined', 'at', 'low', 'energies... | [-0.01882753692067733, 0.19831614574165238, -0.024391028593527153, 0.21087534550072937, -0.07651500265395346, -0.2254849695940114, -0.004436954603685687, 0.3270256994922723, -0.16953802474745316, -0.35792049038476154, 0.07294244637281129, -0.28660468746966217, -0.023335048880956794, 0.1447932530863909, 0.06489946521469... |
1,801.05192 | Production of Electroweak SUSY Particles at ILC and CLIC | For the search for electroweak particles in the Minimal Supersymmetric
Standard Model (MSSM) as well as for future precision analyses of these
particles an accurate knowledge of their production and decay properties is
mandatory. We review the evaluation of the cross sections for the chargino,
neutralino and scalar l... | hep-ph | for the search for electroweak particles in the minimal supersymmetric standard model mssm as well as for future precision analyses of these particles an accurate knowledge of their production and decay properties is mandatory we review the evaluation of the cross sections for the chargino neutralino and scalar lepton ... | [['for', 'the', 'search', 'for', 'electroweak', 'particles', 'in', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'mssm', 'as', 'well', 'as', 'for', 'future', 'precision', 'analyses', 'of', 'these', 'particles', 'an', 'accurate', 'knowledge', 'of', 'their', 'production', 'and', 'decay', 'properties', 'is', 'm... | [-0.051722702626974724, 0.1842190630754302, -0.025087608078208107, 0.18471784243070616, -0.049925401663550965, -0.10841323828506762, 0.012030353966670541, 0.32296915206974613, -0.18495737462459752, -0.3017045675048557, 0.03615418626726844, -0.3533041928803402, -0.02346982059474939, 0.20880125055032878, 0.09909439333774... |
1,801.05193 | Some remark on the existence of infinitely many nonphysical solutions to
the incompressible Navier-Stokes equations | We prove that there exist infinitely many distributional solutions with
infinite kinetic energy to the incompressible Navier-Stokes equations in $
\mathbb{R}^2 $. We prove as well the existence of infinitely many
distributional solutions for Burgers equation in $ \mathbb{R} $.
| math.AP | we prove that there exist infinitely many distributional solutions with infinite kinetic energy to the incompressible navierstokes equations in mathbbr2 we prove as well the existence of infinitely many distributional solutions for burgers equation in mathbbr | [['we', 'prove', 'that', 'there', 'exist', 'infinitely', 'many', 'distributional', 'solutions', 'with', 'infinite', 'kinetic', 'energy', 'to', 'the', 'incompressible', 'navierstokes', 'equations', 'in', 'mathbbr2', 'we', 'prove', 'as', 'well', 'the', 'existence', 'of', 'infinitely', 'many', 'distributional', 'solutions... | [-0.22092637564573023, 0.06423126366765548, -0.06131533071553955, 0.11755186332286233, -0.05332566394160191, -0.14180491316235727, -0.11096784037848313, 0.27308418648317456, -0.3151036592510839, -0.20056117522633737, 0.13423257874092087, -0.3651744888888465, -0.10763905197381973, 0.17845473811030388, -0.013528575862033... |
1,801.05194 | Sparsity Preserving Optimal Control of Discretized PDE Systems | We focus on the problem of optimal control of large-scale systems whose
models are obtained by discretization of partial differential equations using
the Finite Element (FE) or Finite Difference (FD) methods. The motivation for
studying this pressing problem originates from the fact that the classical
numerical tools... | math.OC cs.SY physics.comp-ph physics.flu-dyn | we focus on the problem of optimal control of largescale systems whose models are obtained by discretization of partial differential equations using the finite element fe or finite difference fd methods the motivation for studying this pressing problem originates from the fact that the classical numerical tools used to... | [['we', 'focus', 'on', 'the', 'problem', 'of', 'optimal', 'control', 'of', 'largescale', 'systems', 'whose', 'models', 'are', 'obtained', 'by', 'discretization', 'of', 'partial', 'differential', 'equations', 'using', 'the', 'finite', 'element', 'fe', 'or', 'finite', 'difference', 'fd', 'methods', 'the', 'motivation', '... | [-0.11413762660183135, 0.02270102986478521, -0.0616238952510028, 0.0932446029563763, -0.09045860629636965, -0.16753030630385046, 0.03167121842478429, 0.383927479540906, -0.33566867696948316, -0.2514636663418588, 0.1680803343825645, -0.23431707434264432, -0.2239244334869226, 0.20823167454687053, -0.041242597929947854, 0... |
1,801.05195 | Multicolour containers, extremal entropy and counting | In breakthrough results, Saxton-Thomason and Balogh-Morris-Samotij developed
powerful theories of hypergraph containers. In this paper, we explore some
consequences of these theories. We use a simple container theorem of
Saxton-Thomason and an entropy-based framework to deduce container and counting
theorems for here... | math.CO | in breakthrough results saxtonthomason and baloghmorrissamotij developed powerful theories of hypergraph containers in this paper we explore some consequences of these theories we use a simple container theorem of saxtonthomason and an entropybased framework to deduce container and counting theorems for hereditary prop... | [['in', 'breakthrough', 'results', 'saxtonthomason', 'and', 'baloghmorrissamotij', 'developed', 'powerful', 'theories', 'of', 'hypergraph', 'containers', 'in', 'this', 'paper', 'we', 'explore', 'some', 'consequences', 'of', 'these', 'theories', 'we', 'use', 'a', 'simple', 'container', 'theorem', 'of', 'saxtonthomason',... | [-0.0756027611604989, 0.07608561630027609, -0.07499385415923907, 0.09702802503762989, -0.08778826065305899, -0.12717850530978791, 0.03737566275469987, 0.3576562392956285, -0.2297539412506175, -0.32099072651854205, 0.0952042952212922, -0.2465003555546751, -0.14007599077903346, 0.1966446023660281, -0.1635621225673344, 0.... |
1,801.05196 | Infinite charge mobility in muscovite at 300K | Evidence is presented for infinite charge mobility in natural crystals of
muscovite mica at room temperature. Muscovite has a basic layered structure
containing a flat monatomic sheet of potassium sandwiched between mirror
silicate layers. It is an excellent electrical insulator. Studies of defects in
muscovite cryst... | cond-mat.mtrl-sci nlin.PS | evidence is presented for infinite charge mobility in natural crystals of muscovite mica at room temperature muscovite has a basic layered structure containing a flat monatomic sheet of potassium sandwiched between mirror silicate layers it is an excellent electrical insulator studies of defects in muscovite crystals i... | [['evidence', 'is', 'presented', 'for', 'infinite', 'charge', 'mobility', 'in', 'natural', 'crystals', 'of', 'muscovite', 'mica', 'at', 'room', 'temperature', 'muscovite', 'has', 'a', 'basic', 'layered', 'structure', 'containing', 'a', 'flat', 'monatomic', 'sheet', 'of', 'potassium', 'sandwiched', 'between', 'mirror', ... | [-0.11996736755553983, 0.2748903934517641, 0.01147759233557638, -0.0323431406313891, 0.036785335384696825, -0.13623096475583946, 0.0730525294753204, 0.421578102888877, -0.23801970491560814, -0.30246483672163355, -0.00023592319245756472, -0.3740214606522014, 0.012240519159592239, 0.18612706228534398, 0.04587473713436583... |
1,801.05197 | A note on the cross-index of a complete graph based on a linear tree | In this paper it is shown that a complete graph with $n$ vertices has an
optimal diagram, i.e., a diagram whose crossing number equals the value of
Guy's formula, with a free maximal linear tree and without free hamiltonian
cycles for any odd integer $n \ge 7$.
| math.GT math.CO | in this paper it is shown that a complete graph with n vertices has an optimal diagram ie a diagram whose crossing number equals the value of guys formula with a free maximal linear tree and without free hamiltonian cycles for any odd integer n ge 7 | [['in', 'this', 'paper', 'it', 'is', 'shown', 'that', 'a', 'complete', 'graph', 'with', 'n', 'vertices', 'has', 'an', 'optimal', 'diagram', 'ie', 'a', 'diagram', 'whose', 'crossing', 'number', 'equals', 'the', 'value', 'of', 'guys', 'formula', 'with', 'a', 'free', 'maximal', 'linear', 'tree', 'and', 'without', 'free', ... | [-0.21722000757816862, 0.2122492895370592, -0.04736640952289738, 0.008732244748859964, -0.07827498751910443, -0.19362416804986113, 0.07971764218676439, 0.3047042387597104, -0.22842260022112665, -0.350127901128949, 0.07747661469732114, -0.3033477359827846, -0.1602139531218625, 0.13072213657358858, -0.03698332613443044, ... |
1,801.05198 | Why and How Java Developers Break APIs | Modern software development depends on APIs to reuse code and increase
productivity. As most software systems, these libraries and frameworks also
evolve, which may break existing clients. However, the main reasons to
introduce breaking changes in APIs are unclear. Therefore, in this paper, we
report the results of a... | cs.SE | modern software development depends on apis to reuse code and increase productivity as most software systems these libraries and frameworks also evolve which may break existing clients however the main reasons to introduce breaking changes in apis are unclear therefore in this paper we report the results of an almost 4... | [['modern', 'software', 'development', 'depends', 'on', 'apis', 'to', 'reuse', 'code', 'and', 'increase', 'productivity', 'as', 'most', 'software', 'systems', 'these', 'libraries', 'and', 'frameworks', 'also', 'evolve', 'which', 'may', 'break', 'existing', 'clients', 'however', 'the', 'main', 'reasons', 'to', 'introduc... | [-0.1029261123091911, 0.0641180933683618, -0.030816347672028004, 0.09451744687875377, -0.16235276178935962, -0.17823921366341713, 0.0743307533581079, 0.43929679172834907, -0.27422154056126347, -0.4045989245076723, 0.11948595880100105, -0.26902132910929316, -0.13929281356835985, 0.17555032165605317, -0.10629855230924366... |
1,801.05199 | The Fermi-Pasta-Ulam problem and its underlying integrable dynamics: an
approach through Lyapunov Exponents | FPU models, in dimension one, are perturbations either of the linear model or
of the Toda model; perturbations of the linear model include the usual
$\beta$-model, perturbations of Toda include the usual $\alpha+\beta$ model. In
this paper we explore and compare two families, or hierarchies, of FPU models,
closer and... | math.DS cond-mat.stat-mech | fpu models in dimension one are perturbations either of the linear model or of the toda model perturbations of the linear model include the usual betamodel perturbations of toda include the usual alphabeta model in this paper we explore and compare two families or hierarchies of fpu models closer and closer to either t... | [['fpu', 'models', 'in', 'dimension', 'one', 'are', 'perturbations', 'either', 'of', 'the', 'linear', 'model', 'or', 'of', 'the', 'toda', 'model', 'perturbations', 'of', 'the', 'linear', 'model', 'include', 'the', 'usual', 'betamodel', 'perturbations', 'of', 'toda', 'include', 'the', 'usual', 'alphabeta', 'model', 'in'... | [-0.08860217635519803, 0.09351361451218977, -0.04623258333145217, 0.1065965705713483, -0.05008083922739112, -0.19594978568228807, 0.024688742656938056, 0.2621907502187021, -0.2693592500167363, -0.2985707209135095, 0.1056580243879139, -0.2769812582794464, -0.1471484009317602, 0.18959798705340786, -0.005419165271186186, ... |
1,801.052 | Drop impact dynamics on slippery liquid-infused porous surfaces:
influence of oil thickness | Slippery liquid-infused porous surfaces (SLIPS) are porous nanostructures
impregnated with a low surface tension lubricant. They have recently shown
great promise in various applications that require non-wettable
superhydrophobic surfaces. In this paper, we investigate experimentally the
influence of the oil thicknes... | cond-mat.soft | slippery liquidinfused porous surfaces slips are porous nanostructures impregnated with a low surface tension lubricant they have recently shown great promise in various applications that require nonwettable superhydrophobic surfaces in this paper we investigate experimentally the influence of the oil thickness on the ... | [['slippery', 'liquidinfused', 'porous', 'surfaces', 'slips', 'are', 'porous', 'nanostructures', 'impregnated', 'with', 'a', 'low', 'surface', 'tension', 'lubricant', 'they', 'have', 'recently', 'shown', 'great', 'promise', 'in', 'various', 'applications', 'that', 'require', 'nonwettable', 'superhydrophobic', 'surfaces... | [-0.09451525597652452, 0.21771714827527516, -0.08220836419836972, -0.02280370182064683, -0.017974838082566214, -0.1296596851657498, 0.03244161101937262, 0.41719281284845083, -0.2508714562522826, -0.2950684389677541, 0.12159691124468046, -0.28553477478823786, -0.1716701686623153, 0.20226269495143587, -0.0859966553217763... |
1,801.05201 | Scaling Laws and Warning Signs for Bifurcations of SPDEs | Critical transitions (or tipping points) are drastic sudden changes observed
in many dynamical systems. Large classes of critical transitions are associated
to systems, which drift slowly towards a bifurcation point. In the context of
stochastic ordinary differential equations (SODEs), there are results on growth
of ... | math.DS math.PR nlin.PS | critical transitions or tipping points are drastic sudden changes observed in many dynamical systems large classes of critical transitions are associated to systems which drift slowly towards a bifurcation point in the context of stochastic ordinary differential equations sodes there are results on growth of variance a... | [['critical', 'transitions', 'or', 'tipping', 'points', 'are', 'drastic', 'sudden', 'changes', 'observed', 'in', 'many', 'dynamical', 'systems', 'large', 'classes', 'of', 'critical', 'transitions', 'are', 'associated', 'to', 'systems', 'which', 'drift', 'slowly', 'towards', 'a', 'bifurcation', 'point', 'in', 'the', 'co... | [-0.13550717746708674, 0.08642527680205819, -0.07758148068926864, 0.09284258586634601, -0.06756039302945918, -0.13551424747948385, 0.02055947560413213, 0.2975806161562645, -0.2788001598108078, -0.2455600384847502, 0.15021151936469743, -0.30160622147947447, -0.23280994856072315, 0.20745748579599796, -0.08928541559030205... |
1,801.05202 | Lower bounds for Combinatorial Algorithms for Boolean Matrix
Multiplication | In this paper we propose models of combinatorial algorithms for the Boolean
Matrix Multiplication (BMM), and prove lower bounds on computing BMM in these
models. First, we give a relatively relaxed combinatorial model which is an
extension of the model by Angluin (1976), and we prove that the time required
by any alg... | cs.CC | in this paper we propose models of combinatorial algorithms for the boolean matrix multiplication bmm and prove lower bounds on computing bmm in these models first we give a relatively relaxed combinatorial model which is an extension of the model by angluin 1976 and we prove that the time required by any algorithm for... | [['in', 'this', 'paper', 'we', 'propose', 'models', 'of', 'combinatorial', 'algorithms', 'for', 'the', 'boolean', 'matrix', 'multiplication', 'bmm', 'and', 'prove', 'lower', 'bounds', 'on', 'computing', 'bmm', 'in', 'these', 'models', 'first', 'we', 'give', 'a', 'relatively', 'relaxed', 'combinatorial', 'model', 'which... | [-0.10414277604677183, 0.08242286282338006, -0.08426152801233505, 0.10364945676208527, -0.027922054083078855, -0.19342034786924228, 0.07308757584253403, 0.3403255244147433, -0.24693765699062958, -0.3413062677718699, 0.11229733968334472, -0.21840389873358626, -0.18177844086000003, 0.19469463382655186, -0.090373295526720... |
1,801.05203 | Forward-Invariance and Wong-Zakai Approximation for Stochastic Moving
Boundary Problems | We discuss a class of stochastic second-order PDEs in one space-dimension
with an inner boundary moving according to a possibly non-linear, Stefan-type
condition. We show that proper separation of phases is attained, i.e., the
solution remains negative on one side and positive on the other side of the
moving interfac... | math.PR math.AP | we discuss a class of stochastic secondorder pdes in one spacedimension with an inner boundary moving according to a possibly nonlinear stefantype condition we show that proper separation of phases is attained ie the solution remains negative on one side and positive on the other side of the moving interface when start... | [['we', 'discuss', 'a', 'class', 'of', 'stochastic', 'secondorder', 'pdes', 'in', 'one', 'spacedimension', 'with', 'an', 'inner', 'boundary', 'moving', 'according', 'to', 'a', 'possibly', 'nonlinear', 'stefantype', 'condition', 'we', 'show', 'that', 'proper', 'separation', 'of', 'phases', 'is', 'attained', 'ie', 'the',... | [-0.14475372177308676, 0.06219862175510702, -0.06898263976285138, 0.03315073851323158, -0.0849715435358974, -0.15269820286517904, 0.008921829534132878, 0.33071199802624196, -0.3175553859009878, -0.2216315395150756, 0.1733313524836348, -0.2581723564659658, -0.1254649016545298, 0.18736210291648342, -0.07366065990021356, ... |
1,801.05204 | A Multi-Agent Neural Network for Dynamic Frequency Reuse in LTE Networks | Fractional Frequency Reuse techniques can be employed to address interference
in mobile networks, improving throughput for edge users. There is a tradeoff
between the coverage and overall throughput achievable, as interference
avoidance techniques lead to a loss in a cell's overall throughput, with
spectrum efficienc... | cs.NI cs.MA | fractional frequency reuse techniques can be employed to address interference in mobile networks improving throughput for edge users there is a tradeoff between the coverage and overall throughput achievable as interference avoidance techniques lead to a loss in a cells overall throughput with spectrum efficiency decre... | [['fractional', 'frequency', 'reuse', 'techniques', 'can', 'be', 'employed', 'to', 'address', 'interference', 'in', 'mobile', 'networks', 'improving', 'throughput', 'for', 'edge', 'users', 'there', 'is', 'a', 'tradeoff', 'between', 'the', 'coverage', 'and', 'overall', 'throughput', 'achievable', 'as', 'interference', '... | [-0.17754912471986914, 0.013582500717357586, -0.027355068082627106, 0.009235892625599118, -0.08297100750435339, -0.18068814602631486, 0.18384341511225916, 0.42034896232775953, -0.25023443930978445, -0.3187198455984655, 0.0467830227240675, -0.24922106060395507, -0.1719810137712078, 0.12398975109926572, -0.16025457253961... |
1,801.05205 | Lifetime measurement of the $^{229}$Th nuclear isomer | The first excited isomeric state of $^{229}$Th possesses the lowest energy
among all known excited nuclear states. The expected energy is accessible with
today's laser technology and in principle allows for a direct optical laser
excitation of the nucleus. The isomer decays via three channels to its
ground-state (int... | nucl-ex | the first excited isomeric state of 229th possesses the lowest energy among all known excited nuclear states the expected energy is accessible with todays laser technology and in principle allows for a direct optical laser excitation of the nucleus the isomer decays via three channels to its groundstate internal conver... | [['the', 'first', 'excited', 'isomeric', 'state', 'of', '229th', 'possesses', 'the', 'lowest', 'energy', 'among', 'all', 'known', 'excited', 'nuclear', 'states', 'the', 'expected', 'energy', 'is', 'accessible', 'with', 'todays', 'laser', 'technology', 'and', 'in', 'principle', 'allows', 'for', 'a', 'direct', 'optical',... | [-0.09810245047582496, 0.21041815316830184, -0.034825432534448635, 0.030737851373501178, 0.021164155180068842, -0.10888290143382728, 0.10542592151559665, 0.3546071264304613, -0.20802864664946719, -0.3144452025259572, 0.020128001857205834, -0.27241605514132233, 0.03501859152885644, 0.20527159771006695, 0.106049649424402... |
1,801.05206 | Sequences, yet Functions: The Dual Nature of Data-Stream Processing | Data-stream processing has continuously risen in importance as the amount of
available data has been steadily increas- ing over the last decade. Besides
traditional domains such as data-center monitoring and click analytics, there
is an increasing number of network-enabled production machines that generate
continuous... | cs.DB | datastream processing has continuously risen in importance as the amount of available data has been steadily increas ing over the last decade besides traditional domains such as datacenter monitoring and click analytics there is an increasing number of networkenabled production machines that generate continuous streams... | [['datastream', 'processing', 'has', 'continuously', 'risen', 'in', 'importance', 'as', 'the', 'amount', 'of', 'available', 'data', 'has', 'been', 'steadily', 'increas', 'ing', 'over', 'the', 'last', 'decade', 'besides', 'traditional', 'domains', 'such', 'as', 'datacenter', 'monitoring', 'and', 'click', 'analytics', 't... | [-0.06627282192628761, 0.039824394168843154, -0.09317599587289065, 0.08903777358150196, -0.14122721514474876, -0.15354694686134784, 0.06833234128565958, 0.4113867074009721, -0.2986307923668021, -0.33057851667938476, 0.10483292921789042, -0.2709212562164154, -0.1468134768629507, 0.25595301252475045, -0.14245018899614312... |
1,801.05207 | Dynamical resonance shift and unification of resonances in short-pulse
laser cluster interaction | Pronounced maximum absorption of laser light irradiating a rare-gas or metal
cluster is widely expected during the linear resonance (LR) when Mie-plasma
wavelength $\lambdaM$ of electrons equals the laser wavelength $\lambda$. On
the contrary, by performing molecular dynamics (MD) simulations of an argon
cluster irra... | physics.plasm-ph | pronounced maximum absorption of laser light irradiating a raregas or metal cluster is widely expected during the linear resonance lr when mieplasma wavelength lambdam of electrons equals the laser wavelength lambda on the contrary by performing molecular dynamics md simulations of an argon cluster irradiated by short ... | [['pronounced', 'maximum', 'absorption', 'of', 'laser', 'light', 'irradiating', 'a', 'raregas', 'or', 'metal', 'cluster', 'is', 'widely', 'expected', 'during', 'the', 'linear', 'resonance', 'lr', 'when', 'mieplasma', 'wavelength', 'lambdam', 'of', 'electrons', 'equals', 'the', 'laser', 'wavelength', 'lambda', 'on', 'th... | [-0.09170658399229943, 0.19776724036253612, -0.0737299890537915, 0.05820815358952597, 0.012553257006037188, -0.1538924019912984, 0.06400739001091862, 0.42793907673193476, -0.22688408554751632, -0.26994780187795714, 0.01675848756764656, -0.26887093461210304, -0.02859147495359153, 0.17643226644456914, 0.02241183396274825... |
1,801.05208 | The dynamically changing publication universe as a reference point in
national impact evaluation: A counterfactual case study on the Chinese
publication growth | National bibliometric performance is commonly measured via relative impact
indicators which appraise absolute national values through a global
environment. Consequenty the resulting impact values mirror changes in the
national performance as well as in its embedding. In order to assess the
importance of the environme... | cs.DL | national bibliometric performance is commonly measured via relative impact indicators which appraise absolute national values through a global environment consequenty the resulting impact values mirror changes in the national performance as well as in its embedding in order to assess the importance of the environment i... | [['national', 'bibliometric', 'performance', 'is', 'commonly', 'measured', 'via', 'relative', 'impact', 'indicators', 'which', 'appraise', 'absolute', 'national', 'values', 'through', 'a', 'global', 'environment', 'consequenty', 'the', 'resulting', 'impact', 'values', 'mirror', 'changes', 'in', 'the', 'national', 'perf... | [-0.03812382518365158, 0.05995306637395709, -0.08579402786173572, 0.13143205957021564, -0.07039023964027838, -0.0362992717327154, 0.11899284864079178, 0.38061875371834425, -0.2474637333538354, -0.35660120214181623, 0.07973030575653758, -0.2998073830848604, -0.10434058892694632, 0.1935368906156578, -0.10055467046753276,... |
1,801.05209 | Normal subgroups of the braid group and the metaconjecture of Ivanov | We show that many normal subgroups of the braid group modulo its centre, and
of the mapping class group of a sphere with marked points, have the property
that their automorphism and abstract commensurator groups are mapping class
groups of such spheres. As one application, we establish the automorphism
groups of each... | math.GT math.GR | we show that many normal subgroups of the braid group modulo its centre and of the mapping class group of a sphere with marked points have the property that their automorphism and abstract commensurator groups are mapping class groups of such spheres as one application we establish the automorphism groups of each term ... | [['we', 'show', 'that', 'many', 'normal', 'subgroups', 'of', 'the', 'braid', 'group', 'modulo', 'its', 'centre', 'and', 'of', 'the', 'mapping', 'class', 'group', 'of', 'a', 'sphere', 'with', 'marked', 'points', 'have', 'the', 'property', 'that', 'their', 'automorphism', 'and', 'abstract', 'commensurator', 'groups', 'ar... | [-0.1483711911840264, 0.05630930929056121, -0.13251212370253618, 0.034595578083544035, -0.09897751548736215, -0.08616946315687658, 0.05215286971455132, 0.36462030037165544, -0.3426559062024726, -0.2687563174102697, 0.14148104285382457, -0.28224838969277605, -0.14175256411879986, 0.21964668107332944, -0.1470035888931359... |
1,801.0521 | Enabling Quality-Driven Scalable Video Transmission over Multi-User NOMA
System | Recently, non-orthogonal multiple access (NOMA) has been proposed to achieve
higher spectral efficiency over conventional orthogonal multiple access.
Although it has the potential to meet increasing demands of video services, it
is still challenging to provide high performance video streaming. In this
research, we in... | cs.IT cs.MM cs.NI eess.SP math.IT | recently nonorthogonal multiple access noma has been proposed to achieve higher spectral efficiency over conventional orthogonal multiple access although it has the potential to meet increasing demands of video services it is still challenging to provide high performance video streaming in this research we investigate ... | [['recently', 'nonorthogonal', 'multiple', 'access', 'noma', 'has', 'been', 'proposed', 'to', 'achieve', 'higher', 'spectral', 'efficiency', 'over', 'conventional', 'orthogonal', 'multiple', 'access', 'although', 'it', 'has', 'the', 'potential', 'to', 'meet', 'increasing', 'demands', 'of', 'video', 'services', 'it', 'i... | [-0.23429449092771393, -0.062157152409199626, -0.053542111283168194, -0.011794343114597722, -0.08237697631702759, -0.2524946317076683, 0.07220604482339694, 0.4343583961762488, -0.24732981277629734, -0.2760452972142957, 0.07289640312083065, -0.21598039215663448, -0.19935913672641617, 0.16379008887568489, -0.145946747766... |
1,801.05211 | Radio haloes in nearby galaxies modelled with 1D cosmic-ray transport
using SPINNAKER | We present radio continuum maps of 12 nearby ($D\leq 27~\rm Mpc$), edge-on
($i\geq 76^{\circ}$), late-type spiral galaxies mostly at $1.4$ and 5 GHz,
observed with the Australia Telescope Compact Array, Very Large Array,
Westerbork Synthesis Radio Telescope, Effelsberg 100-m and Parkes 64-m
telescopes. All galaxies s... | astro-ph.GA | we present radio continuum maps of 12 nearby dleq 27rm mpc edgeon igeq 76circ latetype spiral galaxies mostly at 14 and 5 ghz observed with the australia telescope compact array very large array westerbork synthesis radio telescope effelsberg 100m and parkes 64m telescopes all galaxies show clear evidence of radio halo... | [['we', 'present', 'radio', 'continuum', 'maps', 'of', '12', 'nearby', 'dleq', '27rm', 'mpc', 'edgeon', 'igeq', '76circ', 'latetype', 'spiral', 'galaxies', 'mostly', 'at', '14', 'and', '5', 'ghz', 'observed', 'with', 'the', 'australia', 'telescope', 'compact', 'array', 'very', 'large', 'array', 'westerbork', 'synthesis... | [-0.07839313502453508, 0.11659840465906582, -0.012308906546041403, 0.10975550504630402, -0.0613800878580209, -0.08455060219632522, -0.008558018277155145, 0.4866731588187958, -0.16037440736275335, -0.3573631144263932, 0.05541151851370922, -0.28085496118329767, 0.012268162569530578, 0.23280863083932818, 0.017893897789573... |
1,801.05212 | Semi-Analytic Method for SINS Attitude and Parameters Online Estimation | In this note, the attitude and inertial sensors drift biases estimation for
Strapdown inertial navigation system is investigated. A semi-analytic method is
proposed, which contains two interlaced solution procedures. Specifically, the
attitude encoding the body frame changes and gyroscopes drift biases are
estimated ... | cs.RO | in this note the attitude and inertial sensors drift biases estimation for strapdown inertial navigation system is investigated a semianalytic method is proposed which contains two interlaced solution procedures specifically the attitude encoding the body frame changes and gyroscopes drift biases are estimated through ... | [['in', 'this', 'note', 'the', 'attitude', 'and', 'inertial', 'sensors', 'drift', 'biases', 'estimation', 'for', 'strapdown', 'inertial', 'navigation', 'system', 'is', 'investigated', 'a', 'semianalytic', 'method', 'is', 'proposed', 'which', 'contains', 'two', 'interlaced', 'solution', 'procedures', 'specifically', 'th... | [-0.1638603959176125, 0.10326089192389962, -0.06019091935895355, 0.0008724776262445657, -0.117401629439414, -0.19178140123205428, -0.04072464878713204, 0.4346974838073506, -0.27865580520169303, -0.32516502690586174, 0.15478578604807175, -0.24162920059241128, -0.1470513278336236, 0.1735099826120969, -0.17348947479022722... |
1,801.05213 | Frames of translates for model sets | We study spanning properties of a family of functions translated along simple
model sets. We characterize tight frame and dual frame generators for such
irregular translates and we apply the results to Gabor systems. We use the
connection between model sets and almost periodic functions and rely strongly
on a Poisson... | math.FA math.OA | we study spanning properties of a family of functions translated along simple model sets we characterize tight frame and dual frame generators for such irregular translates and we apply the results to gabor systems we use the connection between model sets and almost periodic functions and rely strongly on a poisson sum... | [['we', 'study', 'spanning', 'properties', 'of', 'a', 'family', 'of', 'functions', 'translated', 'along', 'simple', 'model', 'sets', 'we', 'characterize', 'tight', 'frame', 'and', 'dual', 'frame', 'generators', 'for', 'such', 'irregular', 'translates', 'and', 'we', 'apply', 'the', 'results', 'to', 'gabor', 'systems', '... | [-0.11385734969129165, 0.015940077192064417, -0.10039615711256134, 0.10310384753727536, -0.046134662621750915, -0.08292770244438073, 0.05428511701021129, 0.4153716637827884, -0.2799533435475381, -0.22827528802485303, 0.07622170679394327, -0.24086364664822474, -0.22323734452947974, 0.24508466581471436, -0.09807363120924... |
1,801.05214 | The nonlinear Brascamp-Lieb inequality for simple data | We establish a nonlinear generalisation of the classical Brascamp-Lieb
inequality in the case where the Lebesgue exponents lie in the interior of the
finiteness polytope. As a corollary we show that the best constant in Young's
convolution inequality in a small neighbourhood of the identity of a general
Lie group, ap... | math.CA | we establish a nonlinear generalisation of the classical brascamplieb inequality in the case where the lebesgue exponents lie in the interior of the finiteness polytope as a corollary we show that the best constant in youngs convolution inequality in a small neighbourhood of the identity of a general lie group approach... | [['we', 'establish', 'a', 'nonlinear', 'generalisation', 'of', 'the', 'classical', 'brascamplieb', 'inequality', 'in', 'the', 'case', 'where', 'the', 'lebesgue', 'exponents', 'lie', 'in', 'the', 'interior', 'of', 'the', 'finiteness', 'polytope', 'as', 'a', 'corollary', 'we', 'show', 'that', 'the', 'best', 'constant', '... | [-0.12066370763327225, 0.04099445031753552, -0.10080166087522734, 0.08584492979340698, -0.11118334782134631, -0.12598348504374965, 0.06795928145454515, 0.26369295916220375, -0.3256998137377276, -0.235728167163411, 0.0956504433277515, -0.23699256644980743, -0.15598721434546653, 0.21321417773741824, -0.11364518105983734,... |
1,801.05215 | Trends in Processor Architecture | This paper presents an overview of the main trends in processor architecture.
It starts with an analysis of the past evolution of processors and the main
driving forces behind it, and then it focuses on a description of the main
architectural features of current processors. Finally, it presents a discussion
on some p... | cs.AR | this paper presents an overview of the main trends in processor architecture it starts with an analysis of the past evolution of processors and the main driving forces behind it and then it focuses on a description of the main architectural features of current processors finally it presents a discussion on some promisi... | [['this', 'paper', 'presents', 'an', 'overview', 'of', 'the', 'main', 'trends', 'in', 'processor', 'architecture', 'it', 'starts', 'with', 'an', 'analysis', 'of', 'the', 'past', 'evolution', 'of', 'processors', 'and', 'the', 'main', 'driving', 'forces', 'behind', 'it', 'and', 'then', 'it', 'focuses', 'on', 'a', 'descri... | [-0.19191445543741187, 0.009318780484318268, -0.11835757906859119, -0.02639624543856674, -0.06367620516878864, -0.11980031145115694, -0.004208551981719211, 0.39364775146047276, -0.25861710323176035, -0.3016098425646002, 0.11536797239872006, -0.25341481507445374, -0.18933737644304832, 0.24773509794225296, -0.07413619286... |
1,801.05216 | Dual vibration configuration interaction (DVCI). An efficient
factorization of molecular Hamiltonian for high performance infrared spectrum
computation | Here is presented an original program based on molecular Schrodinger
equations. It is dedicated to target specific states of infrared vibrational
spectrum in a very precise way with a minimal usage of memory. An eigensolver
combined with a new probing technique accumulates information along the
iterations so that des... | physics.comp-ph cs.CC math.NA physics.chem-ph quant-ph | here is presented an original program based on molecular schrodinger equations it is dedicated to target specific states of infrared vibrational spectrum in a very precise way with a minimal usage of memory an eigensolver combined with a new probing technique accumulates information along the iterations so that desired... | [['here', 'is', 'presented', 'an', 'original', 'program', 'based', 'on', 'molecular', 'schrodinger', 'equations', 'it', 'is', 'dedicated', 'to', 'target', 'specific', 'states', 'of', 'infrared', 'vibrational', 'spectrum', 'in', 'a', 'very', 'precise', 'way', 'with', 'a', 'minimal', 'usage', 'of', 'memory', 'an', 'eigen... | [-0.1014498164698195, 0.10016984363867848, -0.13055056057727107, 0.030583892557143163, -0.10528696145047434, -0.1255161547770303, 0.05192228084398756, 0.3165316543622444, -0.30552871282158706, -0.24887687368139338, 0.09935786952197444, -0.2566825139578074, -0.14670373938637427, 0.16162189592320758, -0.0559288399559906,... |
1,801.05217 | Formation of trans-Neptunian satellite systems at the stage of
condensations | The formation of trans-Neptunian satellite systems at the stage of rarefied
preplanetesimals (i.e., condensations of dust and/or objects less than 1 m in
diameter) is discussed. It is assumed that trans-Neptunian objects (including
those with satellites) could form as a result of compression of parental
rarefied prep... | astro-ph.EP | the formation of transneptunian satellite systems at the stage of rarefied preplanetesimals ie condensations of dust andor objects less than 1 m in diameter is discussed it is assumed that transneptunian objects including those with satellites could form as a result of compression of parental rarefied preplanetesimals ... | [['the', 'formation', 'of', 'transneptunian', 'satellite', 'systems', 'at', 'the', 'stage', 'of', 'rarefied', 'preplanetesimals', 'ie', 'condensations', 'of', 'dust', 'andor', 'objects', 'less', 'than', '1', 'm', 'in', 'diameter', 'is', 'discussed', 'it', 'is', 'assumed', 'that', 'transneptunian', 'objects', 'including... | [-0.1483266793717235, 0.2000522872040433, -0.08631706522570191, 0.045937723054024784, -0.01684267948745884, -0.023402845645082833, -0.04939768117220172, 0.3272455017395125, -0.1802866720797226, -0.37797606185124155, 0.05250516473496079, -0.2573365763833272, 0.002847330416836243, 0.21692030330195447, -0.0592106006186514... |
1,801.05218 | Probing underlying event in Z-boson events using event shape observables | Experimental measurements of observables sensitive to the underlying event
(UE) in $Z$-boson events have been performed by both ATLAS and CMS experiments
at the LHC. However, in the busy LHC environment, these observables receive
substantial contribution from jets originating from initial state radiation
(ISR). We pr... | hep-ph | experimental measurements of observables sensitive to the underlying event ue in zboson events have been performed by both atlas and cms experiments at the lhc however in the busy lhc environment these observables receive substantial contribution from jets originating from initial state radiation isr we probe if using ... | [['experimental', 'measurements', 'of', 'observables', 'sensitive', 'to', 'the', 'underlying', 'event', 'ue', 'in', 'zboson', 'events', 'have', 'been', 'performed', 'by', 'both', 'atlas', 'and', 'cms', 'experiments', 'at', 'the', 'lhc', 'however', 'in', 'the', 'busy', 'lhc', 'environment', 'these', 'observables', 'rece... | [-0.021608811961616285, 0.16061984560736972, -0.15819164010463282, 0.15415067283093878, -0.08199127252575839, -0.12903682586167836, -0.002514546248777252, 0.3605732940033906, -0.22801685105595323, -0.3469501544152283, 0.028037338556411367, -0.37549645310112584, 0.057037387017367616, 0.15684604227620488, 0.0089713094704... |
1,801.05219 | Eligibility Traces and Plasticity on Behavioral Time Scales:
Experimental Support of neoHebbian Three-Factor Learning Rules | Most elementary behaviors such as moving the arm to grasp an object or
walking into the next room to explore a museum evolve on the time scale of
seconds; in contrast, neuronal action potentials occur on the time scale of a
few milliseconds. Learning rules of the brain must therefore bridge the gap
between these two ... | q-bio.NC | most elementary behaviors such as moving the arm to grasp an object or walking into the next room to explore a museum evolve on the time scale of seconds in contrast neuronal action potentials occur on the time scale of a few milliseconds learning rules of the brain must therefore bridge the gap between these two diffe... | [['most', 'elementary', 'behaviors', 'such', 'as', 'moving', 'the', 'arm', 'to', 'grasp', 'an', 'object', 'or', 'walking', 'into', 'the', 'next', 'room', 'to', 'explore', 'a', 'museum', 'evolve', 'on', 'the', 'time', 'scale', 'of', 'seconds', 'in', 'contrast', 'neuronal', 'action', 'potentials', 'occur', 'on', 'the', '... | [-0.11385278685903649, 0.11774456480464503, -0.05528528635924313, 0.03775807221769946, -0.0946367859821483, -0.14111675634190704, 0.07416028351635852, 0.41659342573227615, -0.25863793374424526, -0.28868588618697777, 0.10490754415838965, -0.21718944561062617, -0.19557117860023226, 0.16283433560295585, -0.063246584994964... |
1,801.0522 | Note on Bose-Einstein condensation of photons | This paper provides, firstly, a succinct mathematical derivation of
Bose-Einstein condensation (BEC) of photons elaborating on previous results
[M\"uller, E.E., Annals of Phys. 184, 219-230 (1988); M\"uller, E.E. Physica
139A, 165-174 (1986)] including new results on the condensate function, and,
secondly, applies th... | quant-ph cond-mat.quant-gas | this paper provides firstly a succinct mathematical derivation of boseeinstein condensation bec of photons elaborating on previous results muller ee annals of phys 184 219230 1988 muller ee physica 139a 165174 1986 including new results on the condensate function and secondly applies this framework to consistently expl... | [['this', 'paper', 'provides', 'firstly', 'a', 'succinct', 'mathematical', 'derivation', 'of', 'boseeinstein', 'condensation', 'bec', 'of', 'photons', 'elaborating', 'on', 'previous', 'results', 'muller', 'ee', 'annals', 'of', 'phys', '184', '219230', '1988', 'muller', 'ee', 'physica', '139a', '165174', '1986', 'includ... | [-0.06353251885792072, 0.12049449094444174, -0.07974878552803685, -0.018204233300242446, -0.06515348013702103, -0.14929852162657137, 0.10262888905576388, 0.30452802178280597, -0.12019032540477136, -0.32757543002001266, -0.07851477444372987, -0.28014564022570004, -0.1213768221840093, 0.21612204644903119, -0.067917851503... |
1,801.05221 | A fast subspace optimization method for nonlinear inverse problems in
Banach spaces with an application in parameter identification | We introduce and analyze a fast iterative method based on sequential Bregman
projections for nonlinear inverse problems in Banach spaces. The key idea, in
contrast to the standard Landweber method, is to use multiple search directions
per iteration in combination with a regulation of the step width in order to
reduce... | math.NA | we introduce and analyze a fast iterative method based on sequential bregman projections for nonlinear inverse problems in banach spaces the key idea in contrast to the standard landweber method is to use multiple search directions per iteration in combination with a regulation of the step width in order to reduce the ... | [['we', 'introduce', 'and', 'analyze', 'a', 'fast', 'iterative', 'method', 'based', 'on', 'sequential', 'bregman', 'projections', 'for', 'nonlinear', 'inverse', 'problems', 'in', 'banach', 'spaces', 'the', 'key', 'idea', 'in', 'contrast', 'to', 'the', 'standard', 'landweber', 'method', 'is', 'to', 'use', 'multiple', 's... | [-0.08941714392434126, -0.006238409286197566, -0.07315031246010524, 0.06802081947777576, -0.0797502076990592, -0.12768815723635876, 0.04631582928899055, 0.4051561220937098, -0.33288893158896826, -0.287583350262139, 0.1376548866998443, -0.23689325016069537, -0.13135416278237244, 0.22922602605103748, -0.08195044797321316... |
1,801.05222 | Calculating $p$-values and their significances with the Energy Test for
large datasets | The energy test method is a multi-dimensional test of whether two samples are
consistent with arising from the same underlying population, through the
calculation of a single test statistic (called the $T$-value). The method has
recently been used in particle physics to search for differences between
samples that ari... | physics.data-an hep-ex | the energy test method is a multidimensional test of whether two samples are consistent with arising from the same underlying population through the calculation of a single test statistic called the tvalue the method has recently been used in particle physics to search for differences between samples that arise from cp... | [['the', 'energy', 'test', 'method', 'is', 'a', 'multidimensional', 'test', 'of', 'whether', 'two', 'samples', 'are', 'consistent', 'with', 'arising', 'from', 'the', 'same', 'underlying', 'population', 'through', 'the', 'calculation', 'of', 'a', 'single', 'test', 'statistic', 'called', 'the', 'tvalue', 'the', 'method',... | [-0.012777748244820506, 0.09993879517516607, -0.14691713785420463, 0.11976422648951056, -0.030971046765542524, -0.11690857170066636, 0.04216814962524185, 0.3393446475409778, -0.2578996250963515, -0.34176620542053965, 0.09029888096384135, -0.2591088190704442, -0.0995031161127007, 0.21427407264220083, -0.0196707972153356... |
1,801.05223 | Detection and effects of meteoric smoke particles in the atmosphere | These are the lecture notes of a trial lecture on the given topic "The
detection and effects of meteoric debris in the atmosphere and why we should
care". I have shortened the title a little, while I have expanded on the
contents. First, I discuss some of the relevant nomenclature. Then, I go
through the composition,... | physics.ao-ph physics.space-ph | these are the lecture notes of a trial lecture on the given topic the detection and effects of meteoric debris in the atmosphere and why we should care i have shortened the title a little while i have expanded on the contents first i discuss some of the relevant nomenclature then i go through the composition size forma... | [['these', 'are', 'the', 'lecture', 'notes', 'of', 'a', 'trial', 'lecture', 'on', 'the', 'given', 'topic', 'the', 'detection', 'and', 'effects', 'of', 'meteoric', 'debris', 'in', 'the', 'atmosphere', 'and', 'why', 'we', 'should', 'care', 'i', 'have', 'shortened', 'the', 'title', 'a', 'little', 'while', 'i', 'have', 'ex... | [-0.050378876222838834, 0.20973119906221444, -0.06444035117657712, 0.0676671885049496, -0.06077816520079286, -0.06138342902617545, -0.004841931518485658, 0.3390134229746639, -0.17804876803699085, -0.32466018380613154, 0.18171253426171616, -0.3216155614687974, -0.13392144109870696, 0.16253289124434894, -0.11232306131233... |
1,801.05224 | Device-to-Device Aided Multicasting | We consider a device-to-device (D2D) aided multicast channel, where a
transmitter wishes to convey a common message to many receivers and these
receivers cooperate with each other. We propose a simple computationally
efficient scheme requiring only statistical channel knowledge at transmitter.
Our analysis in general... | cs.IT math.IT | we consider a devicetodevice d2d aided multicast channel where a transmitter wishes to convey a common message to many receivers and these receivers cooperate with each other we propose a simple computationally efficient scheme requiring only statistical channel knowledge at transmitter our analysis in general topologi... | [['we', 'consider', 'a', 'devicetodevice', 'd2d', 'aided', 'multicast', 'channel', 'where', 'a', 'transmitter', 'wishes', 'to', 'convey', 'a', 'common', 'message', 'to', 'many', 'receivers', 'and', 'these', 'receivers', 'cooperate', 'with', 'each', 'other', 'we', 'propose', 'a', 'simple', 'computationally', 'efficient'... | [-0.24923497499761785, 0.07017029817329674, -0.030932682551201282, -0.014436567047936463, -0.056768053260488, -0.31523917384665245, 0.1686452831997256, 0.4033949617145023, -0.2652802580619246, -0.22610200757569657, 0.045537598175564555, -0.27467095329448943, -0.14241254069876472, 0.0899661329378018, -0.0750201800487920... |
1,801.05225 | Homogenization of the fluid-saturated piezoelectric porous media | The paper is devoted to the homogenization of porous piezoelectric materials
saturated by electrically inert fluid. The solid part of a representative
volume element consists of the piezoelectric skeleton with embedded conductors.
The pore fluid in the periodic structure can constitute a single connected
domain, or a... | physics.comp-ph cs.CE | the paper is devoted to the homogenization of porous piezoelectric materials saturated by electrically inert fluid the solid part of a representative volume element consists of the piezoelectric skeleton with embedded conductors the pore fluid in the periodic structure can constitute a single connected domain or an arr... | [['the', 'paper', 'is', 'devoted', 'to', 'the', 'homogenization', 'of', 'porous', 'piezoelectric', 'materials', 'saturated', 'by', 'electrically', 'inert', 'fluid', 'the', 'solid', 'part', 'of', 'a', 'representative', 'volume', 'element', 'consists', 'of', 'the', 'piezoelectric', 'skeleton', 'with', 'embedded', 'conduc... | [-0.112446138558614, 0.14449423583594959, -0.030256464960700946, -0.025004533083723267, -0.02839704820113938, -0.1033421267073874, -0.024646586758402606, 0.38112714369213435, -0.2953590997335751, -0.2732713965608216, 0.09196275667253337, -0.2535745738392196, -0.13320846160896485, 0.19448001485136224, -0.000774398204166... |
1,801.05226 | Three-dimensional chimera patterns in networks of spiking neuron
oscillators | We study the stable spatiotemporal patterns that arise in a 3D network of
neuron oscillators, whose dynamics is described by the Leaky Integrate-and-Fire
(LIF) model. More specifically, we investigate the form of the chimera states
induced by a 3D coupling matrix with nonlocal topology. The observed patterns
are in m... | cond-mat.dis-nn nlin.CD nlin.PS | we study the stable spatiotemporal patterns that arise in a 3d network of neuron oscillators whose dynamics is described by the leaky integrateandfire lif model more specifically we investigate the form of the chimera states induced by a 3d coupling matrix with nonlocal topology the observed patterns are in many cases ... | [['we', 'study', 'the', 'stable', 'spatiotemporal', 'patterns', 'that', 'arise', 'in', 'a', '3d', 'network', 'of', 'neuron', 'oscillators', 'whose', 'dynamics', 'is', 'described', 'by', 'the', 'leaky', 'integrateandfire', 'lif', 'model', 'more', 'specifically', 'we', 'investigate', 'the', 'form', 'of', 'the', 'chimera'... | [-0.1523482667688087, 0.1726501393056369, -0.026915310820961585, 0.0608499803875517, 0.010537200429237606, -0.1263160835620769, 0.009593058324703956, 0.38623423729845086, -0.2585085539091277, -0.26763639074134454, 0.06340358507516666, -0.2922652279042074, -0.22020868427003099, 0.1807982063683035, -0.023675928240937123,... |
1,801.05227 | A Survey of Physical Layer Security Techniques for 5G Wireless Networks
and Challenges Ahead | Physical layer security which safeguards data confidentiality based on the
information-theoretic approaches has received significant research interest
recently. The key idea behind physical layer security is to utilize the
intrinsic randomness of the transmission channel to guarantee the security in
physical layer. T... | cs.IT math.IT | physical layer security which safeguards data confidentiality based on the informationtheoretic approaches has received significant research interest recently the key idea behind physical layer security is to utilize the intrinsic randomness of the transmission channel to guarantee the security in physical layer the ev... | [['physical', 'layer', 'security', 'which', 'safeguards', 'data', 'confidentiality', 'based', 'on', 'the', 'informationtheoretic', 'approaches', 'has', 'received', 'significant', 'research', 'interest', 'recently', 'the', 'key', 'idea', 'behind', 'physical', 'layer', 'security', 'is', 'to', 'utilize', 'the', 'intrinsic... | [-0.2670636252664468, -0.021361841309518247, 0.04790142116708165, -0.005199510101796354, -0.0957071445999714, -0.25935133398283555, 0.08070400152883704, 0.3450193722505404, -0.28374542380456164, -0.25867076930707367, 0.12176668341858547, -0.24328921671405027, -0.18162362063068802, 0.15751669138763882, -0.13387313631393... |
1,801.05228 | Accurate density measurement of a cold Rydberg gas via non collisional
two-body transitions | We experimentally demonstrate an original method to measure very accurately
the density of a frozen Rydberg gas. It is based on the use of adiabatic
transitions induced by the long-range dipole-dipole interaction in pairs of
nearest neighbor Rydberg atoms by sweeping an electric field with time. The
efficiency of thi... | quant-ph cond-mat.quant-gas physics.atom-ph | we experimentally demonstrate an original method to measure very accurately the density of a frozen rydberg gas it is based on the use of adiabatic transitions induced by the longrange dipoledipole interaction in pairs of nearest neighbor rydberg atoms by sweeping an electric field with time the efficiency of this twob... | [['we', 'experimentally', 'demonstrate', 'an', 'original', 'method', 'to', 'measure', 'very', 'accurately', 'the', 'density', 'of', 'a', 'frozen', 'rydberg', 'gas', 'it', 'is', 'based', 'on', 'the', 'use', 'of', 'adiabatic', 'transitions', 'induced', 'by', 'the', 'longrange', 'dipoledipole', 'interaction', 'in', 'pairs... | [-0.10366778523894027, 0.1530650668843511, -0.05188298029503945, 0.0013818011418215033, 0.016119893849024486, -0.08048569488917189, 0.0881005606648175, 0.37886072443155894, -0.2327901634451901, -0.3235311866095611, 0.0007650380992282439, -0.24941327888518572, -0.061787361130600085, 0.15326187750404893, 0.02725218020475... |
1,801.05229 | On the asymmetry of the forward and reverse martensitic transformations
in shape memory alloys | Differential Scanning Calorimetric, DSC, runs taken during martensitic phase
transformations in shape memory alloys, often look differently during cooling
and heating. Similar asymmetry is observed e.g. for the numbers of hits or the
critical exponents of energy and amplitude distributions (\epsilon and \alpha,
respe... | physics.app-ph | differential scanning calorimetric dsc runs taken during martensitic phase transformations in shape memory alloys often look differently during cooling and heating similar asymmetry is observed eg for the numbers of hits or the critical exponents of energy and amplitude distributions epsilon and alpha respectively in a... | [['differential', 'scanning', 'calorimetric', 'dsc', 'runs', 'taken', 'during', 'martensitic', 'phase', 'transformations', 'in', 'shape', 'memory', 'alloys', 'often', 'look', 'differently', 'during', 'cooling', 'and', 'heating', 'similar', 'asymmetry', 'is', 'observed', 'eg', 'for', 'the', 'numbers', 'of', 'hits', 'or'... | [-0.10636006862921424, 0.24372795454908683, -0.027325702158647568, 0.08294381314054738, -0.053829582083190594, -0.12887587264006914, 0.03825031054682683, 0.38469103821336703, -0.28598981951038505, -0.32833925465468405, 0.07073794205911284, -0.31676382755124294, -0.047196734763768525, 0.2173765483160698, 0.0279813922459... |
1,801.0523 | Real-time CPU-based large-scale 3D mesh reconstruction | In Robotics, especially in this era of autonomous driving, mapping is one key
ability of a robot to be able to navigate through an environment, localize on
it and analyze its traversability. To allow for real-time execution on
constrained hardware, the map usually estimated by feature-based or semi-dense
SLAM algorit... | cs.RO | in robotics especially in this era of autonomous driving mapping is one key ability of a robot to be able to navigate through an environment localize on it and analyze its traversability to allow for realtime execution on constrained hardware the map usually estimated by featurebased or semidense slam algorithms is a s... | [['in', 'robotics', 'especially', 'in', 'this', 'era', 'of', 'autonomous', 'driving', 'mapping', 'is', 'one', 'key', 'ability', 'of', 'a', 'robot', 'to', 'be', 'able', 'to', 'navigate', 'through', 'an', 'environment', 'localize', 'on', 'it', 'and', 'analyze', 'its', 'traversability', 'to', 'allow', 'for', 'realtime', '... | [-0.0672442161106564, -0.005702729814777527, -0.09758794401930843, 0.024704803876638252, -0.09785243093254084, -0.16077402752150405, 0.04804291011111692, 0.4663609499349556, -0.27646650297448355, -0.3509153918620754, 0.14189580389040898, -0.22202251047252658, -0.1589059390662674, 0.18533731954806346, -0.136102190134214... |
1,801.05231 | VLBA Determination of the Distance to Nearby Star-forming Regions. VIII.
The LkH$\alpha$ 101 cluster | The LkH$\alpha$ 101 cluster takes its name from its more massive member, the
LkH$\alpha$ 101star, which is an $\sim15$ M$_\odot$ star whose true nature is
still unknown. The distance to the LkH$\alpha$ 101 cluster has been
controversial for the last few decades, with estimated values ranging from 160
to 800 pc. We ha... | astro-ph.SR astro-ph.GA | the lkhalpha 101 cluster takes its name from its more massive member the lkhalpha 101star which is an sim15 m_odot star whose true nature is still unknown the distance to the lkhalpha 101 cluster has been controversial for the last few decades with estimated values ranging from 160 to 800 pc we have observed members an... | [['the', 'lkhalpha', '101', 'cluster', 'takes', 'its', 'name', 'from', 'its', 'more', 'massive', 'member', 'the', 'lkhalpha', '101star', 'which', 'is', 'an', 'sim15', 'm_odot', 'star', 'whose', 'true', 'nature', 'is', 'still', 'unknown', 'the', 'distance', 'to', 'the', 'lkhalpha', '101', 'cluster', 'has', 'been', 'cont... | [-0.0990372155232493, 0.07482599113578477, -0.07459151503388528, 0.014394104934331995, -0.11870778418249554, -0.07558982558979618, 0.10617776191362215, 0.43113886151393804, -0.21364584606209838, -0.38368114688330224, 0.10722828046849894, -0.28460188611514037, 0.010450854949239228, 0.1781647869437519, -0.010894943780645... |
1,801.05232 | Various complexity measures in confined hydrogen atom | Several well-known statistical measures similar to \emph{LMC} and
\emph{Fisher-Shannon} complexity have been computed for confined hydrogen atom
in both position ($r$) and momentum ($p$) spaces. Further, a more generalized
form of these quantities with R\'enyi entropy ($R$) is explored here. The role
of scaling param... | quant-ph | several wellknown statistical measures similar to emphlmc and emphfishershannon complexity have been computed for confined hydrogen atom in both position r and momentum p spaces further a more generalized form of these quantities with renyi entropy r is explored here the role of scaling parameter in the exponential par... | [['several', 'wellknown', 'statistical', 'measures', 'similar', 'to', 'emphlmc', 'and', 'emphfishershannon', 'complexity', 'have', 'been', 'computed', 'for', 'confined', 'hydrogen', 'atom', 'in', 'both', 'position', 'r', 'and', 'momentum', 'p', 'spaces', 'further', 'a', 'more', 'generalized', 'form', 'of', 'these', 'qu... | [-0.11975923708011049, 0.1458784036517296, -0.061322580272359636, 0.0910313194226682, 0.0068246899624424635, -0.15230507952327937, 0.02702734880010361, 0.35333069950974644, -0.25507037699789004, -0.27762018572478275, 0.07497315034756798, -0.2969265659374477, -0.10234873644389045, 0.18404768063658988, -0.026167104722681... |
1,801.05233 | Poor man's scaling: anisotropic Kondo and Coqblin--Schrieffer models | We discuss Kondo effect for a general model, describing a quantum impurity
with degenerate energy levels, interacting with a gas of itinerant electrons,
and derive scaling equation to the second order for such a model. We show how
the scaling equation for the spin-anisotropic Kondo model with the power law
density of... | cond-mat.mes-hall | we discuss kondo effect for a general model describing a quantum impurity with degenerate energy levels interacting with a gas of itinerant electrons and derive scaling equation to the second order for such a model we show how the scaling equation for the spinanisotropic kondo model with the power law density of states... | [['we', 'discuss', 'kondo', 'effect', 'for', 'a', 'general', 'model', 'describing', 'a', 'quantum', 'impurity', 'with', 'degenerate', 'energy', 'levels', 'interacting', 'with', 'a', 'gas', 'of', 'itinerant', 'electrons', 'and', 'derive', 'scaling', 'equation', 'to', 'the', 'second', 'order', 'for', 'such', 'a', 'model'... | [-0.09289303987483996, 0.12313014863488767, -0.10519653993945283, 0.12326809345324943, -0.018955396938618724, -0.22166470319523915, 0.05861429108439812, 0.240872344795287, -0.2660670082371395, -0.28875588535095803, -0.028395367530430413, -0.3378589639458089, -0.12651509377122908, 0.16181837062474216, 0.0583383176567872... |
1,801.05234 | Silicon dual pillar structure with a distributed Bragg reflector for
dielectric laser accelerators: Design and fabrication | Dielectric laser accelerators (DLAs) have proven to be good candidates for
miniaturized particle accelerators. They rely on micro-fabricated dielectrics
which are able to modulate the kinetic energy of the incoming electron beam
under a proper laser illumination. In this paper we demonstrate a dual pillar
structure w... | physics.acc-ph | dielectric laser accelerators dlas have proven to be good candidates for miniaturized particle accelerators they rely on microfabricated dielectrics which are able to modulate the kinetic energy of the incoming electron beam under a proper laser illumination in this paper we demonstrate a dual pillar structure with a d... | [['dielectric', 'laser', 'accelerators', 'dlas', 'have', 'proven', 'to', 'be', 'good', 'candidates', 'for', 'miniaturized', 'particle', 'accelerators', 'they', 'rely', 'on', 'microfabricated', 'dielectrics', 'which', 'are', 'able', 'to', 'modulate', 'the', 'kinetic', 'energy', 'of', 'the', 'incoming', 'electron', 'beam... | [-0.05987221294226835, 0.2209956342233844, -0.07558814190062028, -0.011993999494751776, -0.026090877968817948, -0.20823367114311883, 0.01257238196586037, 0.5018334114125796, -0.2714607379443589, -0.3356354593343678, 0.006154537190949278, -0.2640926771486799, -0.026689937231796128, 0.2529632156149351, -0.025621231318776... |
1,801.05235 | Primordial Black Holes - Perspectives in Gravitational Wave Astronomy - | This is a review article on the primordial black holes (PBHs), with
particular focus on the massive ones ($\gtrsim 10^{15}{\rm g}$) which have not
evaporated by the present epoch by the Hawking radiation. By the detections of
gravitational waves by LIGO, we have gained a completely novel tool to
observationally searc... | astro-ph.CO gr-qc | this is a review article on the primordial black holes pbhs with particular focus on the massive ones gtrsim 1015rm g which have not evaporated by the present epoch by the hawking radiation by the detections of gravitational waves by ligo we have gained a completely novel tool to observationally search for pbhs complem... | [['this', 'is', 'a', 'review', 'article', 'on', 'the', 'primordial', 'black', 'holes', 'pbhs', 'with', 'particular', 'focus', 'on', 'the', 'massive', 'ones', 'gtrsim', '1015rm', 'g', 'which', 'have', 'not', 'evaporated', 'by', 'the', 'present', 'epoch', 'by', 'the', 'hawking', 'radiation', 'by', 'the', 'detections', 'o... | [-0.11936598816090196, 0.17005396253037927, -0.059034902275121516, 0.14389401333460558, -0.15629615423782472, -0.019403634214962738, 0.01953812950776647, 0.30678997604527336, -0.12659371372960185, -0.3304536055159364, 0.10941603044267285, -0.29589927920977166, -0.11018750945821512, 0.27174289479844976, 0.00806357551271... |
1,801.05236 | MORF: A Framework for Predictive Modeling and Replication At Scale With
Privacy-Restricted MOOC Data | Big data repositories from online learning platforms such as Massive Open
Online Courses (MOOCs) represent an unprecedented opportunity to advance
research on education at scale and impact a global population of learners. To
date, such research has been hindered by poor reproducibility and a lack of
replication, larg... | cs.SE cs.CY cs.LG stat.ML | big data repositories from online learning platforms such as massive open online courses moocs represent an unprecedented opportunity to advance research on education at scale and impact a global population of learners to date such research has been hindered by poor reproducibility and a lack of replication largely due... | [['big', 'data', 'repositories', 'from', 'online', 'learning', 'platforms', 'such', 'as', 'massive', 'open', 'online', 'courses', 'moocs', 'represent', 'an', 'unprecedented', 'opportunity', 'to', 'advance', 'research', 'on', 'education', 'at', 'scale', 'and', 'impact', 'a', 'global', 'population', 'of', 'learners', 'to... | [-0.06999384874344614, 2.1648226340880022e-05, -0.06030622586038289, 0.02685878334738748, -0.14567119573487095, -0.18322311130519595, 0.057367769882616416, 0.4193053885964333, -0.24164713849087507, -0.3657110729028733, 0.13057971151085918, -0.2793743137812165, -0.0825638850524714, 0.2442062638826596, -0.075573932225770... |
1,801.05237 | Information is not a thermodynamic resource | The so-called information-thermodynamics link has been created in a series of
works starting from Maxwell demon and established by the idea of transforming
information into work in the though experiment of Szilard which then evolved
into the vast field of research. The aim of this note is firstly to present two
new m... | quant-ph cond-mat.stat-mech | the socalled informationthermodynamics link has been created in a series of works starting from maxwell demon and established by the idea of transforming information into work in the though experiment of szilard which then evolved into the vast field of research the aim of this note is firstly to present two new models... | [['the', 'socalled', 'informationthermodynamics', 'link', 'has', 'been', 'created', 'in', 'a', 'series', 'of', 'works', 'starting', 'from', 'maxwell', 'demon', 'and', 'established', 'by', 'the', 'idea', 'of', 'transforming', 'information', 'into', 'work', 'in', 'the', 'though', 'experiment', 'of', 'szilard', 'which', '... | [-0.12525585582153054, 0.10384498656678356, -0.10134740512033827, 0.04558573951005217, -0.04414009757487005, -0.13573299654301973, 0.05605804404088607, 0.29110580411118764, -0.25841326341686544, -0.31940742084560425, 0.12051588459463235, -0.27566056710814957, -0.13955284251112557, 0.1952270258120016, -0.053035136222381... |
1,801.05238 | Recent progress on the fabrication of silver nanowire-based transparent
electrodes | Transparent electrodes (TEs) made of metallic nanowires, such as Ag, Au, Cu,
and Ni, have attracted rising attention for several reasons: 1) they can act as
a substitute for tin oxide-based TEs such as indium-tin oxide (ITO) and
fluorine-doped tin oxide (FTO); 2) various methods exist for fabricating such
TEs such as... | physics.app-ph cond-mat.mtrl-sci | transparent electrodes tes made of metallic nanowires such as ag au cu and ni have attracted rising attention for several reasons 1 they can act as a substitute for tin oxidebased tes such as indiumtin oxide ito and fluorinedoped tin oxide fto 2 various methods exist for fabricating such tes such as filtration spraying... | [['transparent', 'electrodes', 'tes', 'made', 'of', 'metallic', 'nanowires', 'such', 'as', 'ag', 'au', 'cu', 'and', 'ni', 'have', 'attracted', 'rising', 'attention', 'for', 'several', 'reasons', '1', 'they', 'can', 'act', 'as', 'a', 'substitute', 'for', 'tin', 'oxidebased', 'tes', 'such', 'as', 'indiumtin', 'oxide', 'i... | [-0.05449264259191185, 0.15513518727356113, 0.027225212937947815, -0.06184406846934907, -0.03665381423112505, -0.17503716787089105, 0.010973089899890489, 0.4649096383150985, -0.22868544905923488, -0.3173643626533903, 0.12855134390666512, -0.3426795960403979, -0.15776245313605702, 0.26162967754410094, -0.082274000810618... |
1,801.05239 | The Radial Velocity Variability of the K-giant Gamma Draconis: Stellar
Variability Masquerading as a Planet | We present precise stellar radial velocity measurements of Gamma Dra taken
from 2003 to 2017. The data from 2003 to 2011 show coherent, long-lived
variations with a period of 702 d. These variations are consistent with the
presence of a planetary companion having m sin i = 10.7 M_Jup whose orbital
properties are typi... | astro-ph.SR | we present precise stellar radial velocity measurements of gamma dra taken from 2003 to 2017 the data from 2003 to 2011 show coherent longlived variations with a period of 702 d these variations are consistent with the presence of a planetary companion having m sin i 107 m_jup whose orbital properties are typical for g... | [['we', 'present', 'precise', 'stellar', 'radial', 'velocity', 'measurements', 'of', 'gamma', 'dra', 'taken', 'from', '2003', 'to', '2017', 'the', 'data', 'from', '2003', 'to', '2011', 'show', 'coherent', 'longlived', 'variations', 'with', 'a', 'period', 'of', '702', 'd', 'these', 'variations', 'are', 'consistent', 'wi... | [-0.13396216227472044, 0.1564606614638515, -0.10491816176263871, 0.041376336632273254, -0.11456894965168993, -0.09381134398677676, 0.0771258288904584, 0.3707047120602299, -0.18597880571561815, -0.3607517345248107, 0.07895618529373942, -0.2651565659843642, -0.09752432669559301, 0.20641168993530618, -0.11307510766451907,... |
1,801.0524 | de Finetti reductions for partially exchangeable probability
distributions | We introduce a general framework for de Finetti reduction results, applicable
to various notions of partially exchangeable probability distributions.
Explicit statements are derived for the cases of exchangeability, Markov
exchangeability, and some generalizations of these. Our techniques are
combinatorial and rely o... | math.PR cs.IT math.CO math.IT quant-ph | we introduce a general framework for de finetti reduction results applicable to various notions of partially exchangeable probability distributions explicit statements are derived for the cases of exchangeability markov exchangeability and some generalizations of these our techniques are combinatorial and rely on the b... | [['we', 'introduce', 'a', 'general', 'framework', 'for', 'de', 'finetti', 'reduction', 'results', 'applicable', 'to', 'various', 'notions', 'of', 'partially', 'exchangeable', 'probability', 'distributions', 'explicit', 'statements', 'are', 'derived', 'for', 'the', 'cases', 'of', 'exchangeability', 'markov', 'exchangeab... | [-0.0812895441463647, 0.06614588003139943, -0.10312927095219493, 0.1882643029675819, -0.10715010652963358, -0.12777046092714256, 0.04997712456119748, 0.339210008091938, -0.24019240868242028, -0.2752219391807627, 0.13136065925377458, -0.21392924866030136, -0.15407520790512746, 0.18354549036862758, -0.1719410979332259, 0... |
1,801.05241 | Laser wakefield acceleration with mid-IR laser pulses | We report on the first results of laser plasma wakefield acceleration driven
by ultrashort mid-infrared laser pulses (\lambda= 3.9 \mu m, 100 fs, 0.25 TW),
which enable near- and above-critical density interactions with
moderate-density gas jets. Relativistic electron acceleration up to ~12 MeV
occurs when the jet wi... | physics.plasm-ph physics.optics | we report on the first results of laser plasma wakefield acceleration driven by ultrashort midinfrared laser pulses lambda 39 mu m 100 fs 025 tw which enable near and abovecritical density interactions with moderatedensity gas jets relativistic electron acceleration up to 12 mev occurs when the jet width exceeds the th... | [['we', 'report', 'on', 'the', 'first', 'results', 'of', 'laser', 'plasma', 'wakefield', 'acceleration', 'driven', 'by', 'ultrashort', 'midinfrared', 'laser', 'pulses', 'lambda', '39', 'mu', 'm', '100', 'fs', '025', 'tw', 'which', 'enable', 'near', 'and', 'abovecritical', 'density', 'interactions', 'with', 'moderateden... | [-0.09991309279869923, 0.2501328903146916, -0.036667031629335586, 0.054175040774009746, 0.027616389451790697, -0.15351964076369473, -0.0009889383894400765, 0.5071673426968798, -0.2172488115840789, -0.3243641411142443, -0.049459895770526445, -0.31204180953779603, 0.05992458686420713, 0.2429817212590327, 0.05908321512091... |
1,801.05242 | A Bayesian Conjugate Gradient Method | A fundamental task in numerical computation is the solution of large linear
systems. The conjugate gradient method is an iterative method which offers
rapid convergence to the solution, particularly when an effective
preconditioner is employed. However, for more challenging systems a substantial
error can be present ... | stat.ME cs.NA math.NA math.ST stat.TH | a fundamental task in numerical computation is the solution of large linear systems the conjugate gradient method is an iterative method which offers rapid convergence to the solution particularly when an effective preconditioner is employed however for more challenging systems a substantial error can be present even a... | [['a', 'fundamental', 'task', 'in', 'numerical', 'computation', 'is', 'the', 'solution', 'of', 'large', 'linear', 'systems', 'the', 'conjugate', 'gradient', 'method', 'is', 'an', 'iterative', 'method', 'which', 'offers', 'rapid', 'convergence', 'to', 'the', 'solution', 'particularly', 'when', 'an', 'effective', 'precon... | [-0.06566704497990114, -0.007707960028072831, -0.11523518779061058, 0.07241973867821326, -0.051856489983605, -0.12941503881283298, 0.033555231479679946, 0.3933367699916874, -0.28703043880787765, -0.3034922672109074, 0.1719969228535963, -0.21139179672380642, -0.16648015678049877, 0.2475909612552783, -0.11274945800923651... |
1,801.05243 | Rank Selection of CP-decomposed Convolutional Layers with Variational
Bayesian Matrix Factorization | Convolutional Neural Networks (CNNs) is one of successful method in many
areas such as image classification tasks. However, the amount of memory and
computational cost needed for CNNs inference obstructs them to run efficiently
in mobile devices because of memory and computational ability limitation. One
of the metho... | cs.LG | convolutional neural networks cnns is one of successful method in many areas such as image classification tasks however the amount of memory and computational cost needed for cnns inference obstructs them to run efficiently in mobile devices because of memory and computational ability limitation one of the method to co... | [['convolutional', 'neural', 'networks', 'cnns', 'is', 'one', 'of', 'successful', 'method', 'in', 'many', 'areas', 'such', 'as', 'image', 'classification', 'tasks', 'however', 'the', 'amount', 'of', 'memory', 'and', 'computational', 'cost', 'needed', 'for', 'cnns', 'inference', 'obstructs', 'them', 'to', 'run', 'effici... | [-0.04454566076916914, 0.04725486318481368, -0.01870185685523514, -0.0010046305520650851, -0.06834557454567403, -0.2099203696246453, 0.06956285771411785, 0.4535034795408137, -0.32036965450000326, -0.3293140626240832, 0.10825924968169905, -0.21374407717667054, -0.15278846507377844, 0.1302939007388583, -0.096191280081560... |
1,801.05244 | Assessing Bayesian Nonparametric Log-Linear Models: an application to
Disclosure Risk estimation | We present a method for identification of models with good predictive
performances in the family of Bayesian log-linear mixed models with Dirichlet
process random effects. Such a problem arises in many different applications;
here we consider it in the context of disclosure risk estimation, an
increasingly relevant i... | stat.ME stat.AP | we present a method for identification of models with good predictive performances in the family of bayesian loglinear mixed models with dirichlet process random effects such a problem arises in many different applications here we consider it in the context of disclosure risk estimation an increasingly relevant issue r... | [['we', 'present', 'a', 'method', 'for', 'identification', 'of', 'models', 'with', 'good', 'predictive', 'performances', 'in', 'the', 'family', 'of', 'bayesian', 'loglinear', 'mixed', 'models', 'with', 'dirichlet', 'process', 'random', 'effects', 'such', 'a', 'problem', 'arises', 'in', 'many', 'different', 'application... | [-0.06113567076811879, 0.03563378357209794, -0.07796463640841586, 0.0690571718900782, -0.08495392226650296, -0.14144489754911815, 0.08607523200955561, 0.36836967217928007, -0.24740943329314546, -0.340232515729355, 0.13194278392521527, -0.2631543931109171, -0.15521460013547442, 0.22226075238298176, -0.11283713502896377,... |
1,801.05245 | Power-Law Statistics Of Driven Reconnection In The Magnetically Closed
Corona | Numerous observations have revealed that power-law distributions are
ubiquitous in energetic solar processes. Hard X-rays, soft X-rays, extreme
ultraviolet radiation, and radio waves all display power-law frequency
distributions. Since magnetic reconnection is the driving mechanism for many
energetic solar phenomena,... | astro-ph.SR | numerous observations have revealed that powerlaw distributions are ubiquitous in energetic solar processes hard xrays soft xrays extreme ultraviolet radiation and radio waves all display powerlaw frequency distributions since magnetic reconnection is the driving mechanism for many energetic solar phenomena it is likel... | [['numerous', 'observations', 'have', 'revealed', 'that', 'powerlaw', 'distributions', 'are', 'ubiquitous', 'in', 'energetic', 'solar', 'processes', 'hard', 'xrays', 'soft', 'xrays', 'extreme', 'ultraviolet', 'radiation', 'and', 'radio', 'waves', 'all', 'display', 'powerlaw', 'frequency', 'distributions', 'since', 'mag... | [-0.1015856865849486, 0.27273990718045626, -0.042843516159774664, 0.18778289655395047, -0.05275233873145137, -0.06840726748262917, 1.5837001208131923e-05, 0.4694418896101695, -0.21829791054526987, -0.3811347803339026, 0.00810822675571798, -0.28397119954172384, -0.11385643027050603, 0.24124338087946162, -0.0180566104130... |
1,801.05246 | Isospectral discrete and quantum graphs with the same flip counts and
nodal counts | The existence of non-isomorphic graphs which share the same Laplace spectrum
(to be referred to as isospectral graphs) leads naturally to the following
question: What additional information is required in order to resolve
isospectral graphs? It was suggested by Band, Shapira and Smilansky that this
might be achieved ... | math-ph math.MP | the existence of nonisomorphic graphs which share the same laplace spectrum to be referred to as isospectral graphs leads naturally to the following question what additional information is required in order to resolve isospectral graphs it was suggested by band shapira and smilansky that this might be achieved by eithe... | [['the', 'existence', 'of', 'nonisomorphic', 'graphs', 'which', 'share', 'the', 'same', 'laplace', 'spectrum', 'to', 'be', 'referred', 'to', 'as', 'isospectral', 'graphs', 'leads', 'naturally', 'to', 'the', 'following', 'question', 'what', 'additional', 'information', 'is', 'required', 'in', 'order', 'to', 'resolve', '... | [-0.12543221149135822, 0.14854217804100175, -0.0493023684287791, 0.10425325247096055, -0.13944895094323714, -0.16004689297070568, 0.050042696889111046, 0.3746501464422366, -0.2775518250162319, -0.3664809333010561, 0.11065807599787426, -0.26789076151168445, -0.13989325557140855, 0.15989446569573512, -0.11914805820511686... |
1,801.05247 | Using the Maximum Entropy Principle to Combine Simulations and Solution
Experiments | Molecular dynamics (MD) simulations allow investigating the structural
dynamics of biomolecular systems with unrivaled time and space resolution.
However, in order to compensate for the inaccuracies of the utilized empirical
force fields, it is becoming common to integrate MD simulations with
experimental data obtain... | physics.comp-ph cond-mat.stat-mech physics.bio-ph physics.chem-ph physics.data-an | molecular dynamics md simulations allow investigating the structural dynamics of biomolecular systems with unrivaled time and space resolution however in order to compensate for the inaccuracies of the utilized empirical force fields it is becoming common to integrate md simulations with experimental data obtained from... | [['molecular', 'dynamics', 'md', 'simulations', 'allow', 'investigating', 'the', 'structural', 'dynamics', 'of', 'biomolecular', 'systems', 'with', 'unrivaled', 'time', 'and', 'space', 'resolution', 'however', 'in', 'order', 'to', 'compensate', 'for', 'the', 'inaccuracies', 'of', 'the', 'utilized', 'empirical', 'force'... | [-0.05588164116876821, 0.05649035459512864, -0.10588532593101263, 0.07386360683109766, -0.050136751274112615, -0.11744759668751309, 0.03798337960615754, 0.4332205620904764, -0.28864919890960056, -0.3134067367995158, 0.14059873448956448, -0.2504519560219099, -0.1671344060334377, 0.2341677582085443, -0.028846181915529692... |
1,801.05248 | Relating unsaturated electrical and hydraulic conductivity of
cement-based materials | Unsaturated hydraulic ($K$) and electrical ($\sigma_b$) conductivity are
often considered durability indicators of cement-based materials. However, $K$
is difficult to measure experimentally. This is due to the large pressure
requirements at low degrees of saturation resulting from the fine pore-size
distribution of ... | cond-mat.soft cond-mat.mtrl-sci | unsaturated hydraulic k and electrical sigma_b conductivity are often considered durability indicators of cementbased materials however k is difficult to measure experimentally this is due to the large pressure requirements at low degrees of saturation resulting from the fine poresize distribution of cementbased materi... | [['unsaturated', 'hydraulic', 'k', 'and', 'electrical', 'sigma_b', 'conductivity', 'are', 'often', 'considered', 'durability', 'indicators', 'of', 'cementbased', 'materials', 'however', 'k', 'is', 'difficult', 'to', 'measure', 'experimentally', 'this', 'is', 'due', 'to', 'the', 'large', 'pressure', 'requirements', 'at'... | [-0.09651122337338407, 0.15135249757022695, -0.08162725886628443, 0.04025869557469342, -0.06615438392174877, -0.17733362331235195, 0.08071184783205339, 0.3674706053966399, -0.2540870040927844, -0.3354638823261742, 0.06589914348750833, -0.28025415333667103, -0.1282704314165517, 0.1759745516693374, -0.008486958444427225,... |
1,801.05249 | Regularity of weak solutions and supersolutions to the porous medium
equation | We study the relations between different regularity assumptions in the
definition of weak solutions and supersolutions to the porous medium equation.
In particular, we establish the equivalence of the conditions $u^m \in L^2_{\rm
loc}(0,T;H^1_{\rm loc}(\Omega))$ and $u^\frac{m+1}2 \in L^2_{\rm
loc}(0,T;H^1_{\rm loc}(... | math.AP | we study the relations between different regularity assumptions in the definition of weak solutions and supersolutions to the porous medium equation in particular we establish the equivalence of the conditions um in l2_rm loc0th1_rm locomega and ufracm12 in l2_rm loc0th1_rm locomega in the definition of weak solutions ... | [['we', 'study', 'the', 'relations', 'between', 'different', 'regularity', 'assumptions', 'in', 'the', 'definition', 'of', 'weak', 'solutions', 'and', 'supersolutions', 'to', 'the', 'porous', 'medium', 'equation', 'in', 'particular', 'we', 'establish', 'the', 'equivalence', 'of', 'the', 'conditions', 'um', 'in', 'l2_rm... | [-0.13501523902470416, 0.0025812056169591167, -0.09962913658131253, 0.06105781594841656, -0.06824268569577147, -0.07977525070309639, 0.027994643067094413, 0.3062791063704274, -0.28372435623949227, -0.2528047159991481, 0.13159116802694784, -0.27762826322154566, -0.10552653385834261, 0.15036361590027808, -0.0763950880955... |
1,801.0525 | Measurement of the production cross-section of a single top-quark in
association with a $Z$ boson at 13 TeV with the ATLAS detector | The production of a top quark in association with a $Z$ boson is studied in
the trilepton channel. The data collected by the ATLAS experiment at the LHC in
2015 and 2016 at a centre-of-mass energy of $\sqrt{s} = 13\,\text{TeV}$ are
used, corresponding to an integrated luminosity of $36.1\,\text{fb}^{-1}$.
Events cont... | hep-ex | the production of a top quark in association with a z boson is studied in the trilepton channel the data collected by the atlas experiment at the lhc in 2015 and 2016 at a centreofmass energy of sqrts 13texttev are used corresponding to an integrated luminosity of 361textfb1 events containing three identified leptons e... | [['the', 'production', 'of', 'a', 'top', 'quark', 'in', 'association', 'with', 'a', 'z', 'boson', 'is', 'studied', 'in', 'the', 'trilepton', 'channel', 'the', 'data', 'collected', 'by', 'the', 'atlas', 'experiment', 'at', 'the', 'lhc', 'in', '2015', 'and', '2016', 'at', 'a', 'centreofmass', 'energy', 'of', 'sqrts', '13... | [-0.06144254728609792, 0.15708007887098638, -0.07389522354311213, 0.1435729255237424, -0.028449222549860334, -0.10934637855047938, -0.006651740986853838, 0.327893412655926, -0.18260623647927723, -0.3500503520320716, 0.04040182159073522, -0.39698896184563637, 0.07617196917999536, 0.16536887677723605, 0.04357622873343142... |
1,801.05251 | Simplified Versions of the Conditional Gradient Method | We suggest simple modifications of the conditional gradient method for smooth
optimization problems, which maintain the basic convergence properties, but
reduce the implementation cost of each iteration essentially. Namely, we
propose the step-size procedure without any line-search, and inexact solution
of the direct... | math.OC | we suggest simple modifications of the conditional gradient method for smooth optimization problems which maintain the basic convergence properties but reduce the implementation cost of each iteration essentially namely we propose the stepsize procedure without any linesearch and inexact solution of the direction findi... | [['we', 'suggest', 'simple', 'modifications', 'of', 'the', 'conditional', 'gradient', 'method', 'for', 'smooth', 'optimization', 'problems', 'which', 'maintain', 'the', 'basic', 'convergence', 'properties', 'but', 'reduce', 'the', 'implementation', 'cost', 'of', 'each', 'iteration', 'essentially', 'namely', 'we', 'prop... | [-0.10203593644629498, -0.07037168248124155, -0.11632424182192024, 0.025333839036258205, -0.11965714122301765, -0.19921782207010047, 0.10450502277152347, 0.40692156919145156, -0.31067993332232746, -0.3208876108817224, 0.1229352381363112, -0.1738790244229936, -0.15145617593745037, 0.17623052073759027, -0.104346390081835... |
1,801.05252 | A probabilistic proof of Perron's theorem | We present an alternative proof of Perron's theorem, which is probabilistic
in nature. It rests on the representation of the Perron eigenvector as a
functional of the trajectory of an auxiliary Markov chain.
| math.PR | we present an alternative proof of perrons theorem which is probabilistic in nature it rests on the representation of the perron eigenvector as a functional of the trajectory of an auxiliary markov chain | [['we', 'present', 'an', 'alternative', 'proof', 'of', 'perrons', 'theorem', 'which', 'is', 'probabilistic', 'in', 'nature', 'it', 'rests', 'on', 'the', 'representation', 'of', 'the', 'perron', 'eigenvector', 'as', 'a', 'functional', 'of', 'the', 'trajectory', 'of', 'an', 'auxiliary', 'markov', 'chain']] | [-0.12414633690125564, 0.02679427967946553, -0.1916520514271476, 0.0674053050302477, -0.13118809839767037, -0.06817898875328177, 0.050679975407988284, 0.31431788646362047, -0.3261220685460351, -0.23096779154641836, 0.12495651293306076, -0.21880796664591992, -0.17347147586670789, 0.16570138383769628, -0.0796986688210657... |
1,801.05253 | A new characterization of endogeny | Aldous and Bandyopadhyay have shown that each solution to a recursive
distributional equation (RDE) gives rise to recursive tree process (RTP), which
is a sort of Markov chain in which time has a tree-like structure and in which
the state of each vertex is a random function of its descendants. If the state
at the roo... | math.PR | aldous and bandyopadhyay have shown that each solution to a recursive distributional equation rde gives rise to recursive tree process rtp which is a sort of markov chain in which time has a treelike structure and in which the state of each vertex is a random function of its descendants if the state at the root is meas... | [['aldous', 'and', 'bandyopadhyay', 'have', 'shown', 'that', 'each', 'solution', 'to', 'a', 'recursive', 'distributional', 'equation', 'rde', 'gives', 'rise', 'to', 'recursive', 'tree', 'process', 'rtp', 'which', 'is', 'a', 'sort', 'of', 'markov', 'chain', 'in', 'which', 'time', 'has', 'a', 'treelike', 'structure', 'an... | [-0.0887910419544342, 0.1392370635400499, -0.11983521373613792, 0.06430386933708873, -0.10831256398575052, -0.15687947452944867, 0.04734986439956736, 0.3635677128290648, -0.33297405157457377, -0.21923704885343528, 0.1055656786857392, -0.29745615262902847, -0.13837834508432184, 0.1193921565571252, -0.08961661498897763, ... |
1,801.05254 | Origin of orbits of secondaries in the discovered trans-Neptunian
binaries | The dependences of inclinations of orbits of secondaries in the discovered
trans-Neptunian binaries on the distance between the primary and the secondary,
on the eccentricity of orbits of the secondary around the primary, on the ratio
of diameters of the secondary and the primary, and on the elements of
heliocentric ... | astro-ph.EP | the dependences of inclinations of orbits of secondaries in the discovered transneptunian binaries on the distance between the primary and the secondary on the eccentricity of orbits of the secondary around the primary on the ratio of diameters of the secondary and the primary and on the elements of heliocentric orbits... | [['the', 'dependences', 'of', 'inclinations', 'of', 'orbits', 'of', 'secondaries', 'in', 'the', 'discovered', 'transneptunian', 'binaries', 'on', 'the', 'distance', 'between', 'the', 'primary', 'and', 'the', 'secondary', 'on', 'the', 'eccentricity', 'of', 'orbits', 'of', 'the', 'secondary', 'around', 'the', 'primary', ... | [-0.1856864828694248, 0.1462245108652243, -0.09082421464290445, 0.05056278604522067, 0.026445746734824697, -0.02226416493491547, 0.015755833798883765, 0.335239031777674, -0.1926726648053586, -0.3564175159072146, 0.042898691573106246, -0.2961826078618402, -0.04523858834144394, 0.21682245638961625, -0.0487067068415071, 0... |
1,801.05255 | Topological Magnons in a One-dimensional Itinerant Flatband Ferromagnet | Different from previous scenarios that topological magnons emerge in local
spin models, we propose an alternative that itinerant electron magnets can host
topological magnons. A one-dimensional Tasaki model with a flat band is
considered as the prototype. This model can be viewed as a quarter filled
periodic Anderson... | cond-mat.str-el | different from previous scenarios that topological magnons emerge in local spin models we propose an alternative that itinerant electron magnets can host topological magnons a onedimensional tasaki model with a flat band is considered as the prototype this model can be viewed as a quarter filled periodic anderson model... | [['different', 'from', 'previous', 'scenarios', 'that', 'topological', 'magnons', 'emerge', 'in', 'local', 'spin', 'models', 'we', 'propose', 'an', 'alternative', 'that', 'itinerant', 'electron', 'magnets', 'can', 'host', 'topological', 'magnons', 'a', 'onedimensional', 'tasaki', 'model', 'with', 'a', 'flat', 'band', '... | [-0.1868176826846915, 0.24981249161126232, -0.028400236030319964, 0.055947871926328996, -0.06225721060849019, -0.21466214557851318, 0.10316368207729755, 0.3823584093419957, -0.26800953751824197, -0.2610277190938742, -0.012997368291142756, -0.3597602694546872, -0.14387310600846354, 0.1134510807043798, 0.0464787775511262... |
1,801.05256 | Centralizers of normal subsystems revisited | In this paper we revisit two concepts which were originally introduced by
Aschbacher and are crucial in the theory of saturated fusion systems: Firstly,
we give a new approach to defining the centralizer of a normal subsystem.
Secondly, we revisit the construction of the product of two normal subsystems
which central... | math.GR | in this paper we revisit two concepts which were originally introduced by aschbacher and are crucial in the theory of saturated fusion systems firstly we give a new approach to defining the centralizer of a normal subsystem secondly we revisit the construction of the product of two normal subsystems which centralize ea... | [['in', 'this', 'paper', 'we', 'revisit', 'two', 'concepts', 'which', 'were', 'originally', 'introduced', 'by', 'aschbacher', 'and', 'are', 'crucial', 'in', 'the', 'theory', 'of', 'saturated', 'fusion', 'systems', 'firstly', 'we', 'give', 'a', 'new', 'approach', 'to', 'defining', 'the', 'centralizer', 'of', 'a', 'norma... | [-0.1241959715349916, 0.13368154681762154, -0.08059239601892121, 0.03289252343666652, -0.031967013235256636, -0.1394621752518809, 0.01350429285106794, 0.30006733932093066, -0.293060547795217, -0.23723602017282314, 0.11252689799557458, -0.2201478920771547, -0.19052068523640903, 0.15947943879291415, -0.11131450852800934,... |
1,801.05257 | Conics, Twistors, and anti-self-dual tri-K\"ahler metrics | We describe the range of the Radon transform on the space $M$ of irreducible
conics in $\CP^2$ in terms of natural differential operators associated to the
$SO(3)$-structure on $M=SL(3, \R)/SO(3)$ and its complexification. Following
\cite{moraru} we show that for any function $F$ in this range, the zero locus
of $F$ ... | math.DG hep-th math-ph math.MP | we describe the range of the radon transform on the space m of irreducible conics in cp2 in terms of natural differential operators associated to the so3structure on msl3 rso3 and its complexification following citemoraru we show that for any function f in this range the zero locus of f is a fourmanifold admitting an a... | [['we', 'describe', 'the', 'range', 'of', 'the', 'radon', 'transform', 'on', 'the', 'space', 'm', 'of', 'irreducible', 'conics', 'in', 'cp2', 'in', 'terms', 'of', 'natural', 'differential', 'operators', 'associated', 'to', 'the', 'so3structure', 'on', 'msl3', 'rso3', 'and', 'its', 'complexification', 'following', 'cite... | [-0.2127369165254554, 0.036851705063052596, -0.04168238715812712, 0.04649484719122105, -0.14409402456816914, -0.1046507711393187, -0.03916375360239555, 0.33678169607526004, -0.2634259145706892, -0.17372407609283333, 0.05660841459555939, -0.2833211221893567, -0.15880596705096875, 0.1609750535629579, -0.11604139281639664... |
1,801.05258 | Single-scale Renormalisation Group Improvement of Multi-scale Effective
Potentials | We present a new method for renormalisation group improvement of the
effective potential of a quantum field theory with an arbitrary number of
scalar fields. The method amounts to solving the renormalisation group equation
for the effective potential with the boundary conditions chosen on the
hypersurface where quant... | hep-ph hep-th | we present a new method for renormalisation group improvement of the effective potential of a quantum field theory with an arbitrary number of scalar fields the method amounts to solving the renormalisation group equation for the effective potential with the boundary conditions chosen on the hypersurface where quantum ... | [['we', 'present', 'a', 'new', 'method', 'for', 'renormalisation', 'group', 'improvement', 'of', 'the', 'effective', 'potential', 'of', 'a', 'quantum', 'field', 'theory', 'with', 'an', 'arbitrary', 'number', 'of', 'scalar', 'fields', 'the', 'method', 'amounts', 'to', 'solving', 'the', 'renormalisation', 'group', 'equat... | [-0.13144563798888828, 0.1253843932735554, -0.12364520265786584, 0.07919102714842428, -0.08285956807135929, -0.13357279564851246, 0.03226373101279023, 0.3121758136422495, -0.24789951257812587, -0.3174642548521819, 0.08335399702659545, -0.1989144712811337, -0.12853378799564266, 0.1969033252933751, -0.0010422929949329598... |
1,801.05259 | Hamiltonian partial differential equations and symplectic scale
manifolds | This paper defines symplectic scale manifolds based on
Hofer-Wysocki-Zehnder's scale calculus. We introduce Hamiltonian vector fields
and flows on these by narrowing down sc-smoothness to what we denote by strong
sc-smoothness, a concept which effectively formalizes the desired smoothness
properties for Hamiltonian f... | math.SG | this paper defines symplectic scale manifolds based on hoferwysockizehnders scale calculus we introduce hamiltonian vector fields and flows on these by narrowing down scsmoothness to what we denote by strong scsmoothness a concept which effectively formalizes the desired smoothness properties for hamiltonian functions ... | [['this', 'paper', 'defines', 'symplectic', 'scale', 'manifolds', 'based', 'on', 'hoferwysockizehnders', 'scale', 'calculus', 'we', 'introduce', 'hamiltonian', 'vector', 'fields', 'and', 'flows', 'on', 'these', 'by', 'narrowing', 'down', 'scsmoothness', 'to', 'what', 'we', 'denote', 'by', 'strong', 'scsmoothness', 'a',... | [-0.1299296203522115, 0.1396975584793836, -0.12158659189784278, 0.10113313866572247, -0.12885717266342706, -0.11188787497748207, -0.022225997326636895, 0.3581775398148845, -0.3250387129244498, -0.26796197570446467, 0.08832552368080036, -0.21746917793320286, -0.1915204686164442, 0.1485996689233515, -0.10469333027463613,... |
1,801.0526 | Curvature dependent surface energy for free standing monolayer graphene:
geometrical and material linearization with closed form solutions | Continuum modeling of a free-standing graphene monolayer, viewed as a two
dimensional 2-lattice, requires specifications of the components of the shift
vector that act as an auxiliary variable. The field equations are then the
equations ruling the shift vector, together with momentum and moment of
momentum equations.... | cond-mat.mtrl-sci | continuum modeling of a freestanding graphene monolayer viewed as a two dimensional 2lattice requires specifications of the components of the shift vector that act as an auxiliary variable the field equations are then the equations ruling the shift vector together with momentum and moment of momentum equations to intro... | [['continuum', 'modeling', 'of', 'a', 'freestanding', 'graphene', 'monolayer', 'viewed', 'as', 'a', 'two', 'dimensional', '2lattice', 'requires', 'specifications', 'of', 'the', 'components', 'of', 'the', 'shift', 'vector', 'that', 'act', 'as', 'an', 'auxiliary', 'variable', 'the', 'field', 'equations', 'are', 'then', '... | [-0.1489619408324264, 0.14426939124814453, -0.04371611238214731, -0.008986951655363859, -0.12253027860909545, -0.0916205590813964, 0.0016690096341941778, 0.38730878737260355, -0.3077449881335876, -0.284978639720066, 0.08597099614598847, -0.23830664001191812, -0.12846335851645563, 0.17194138600098086, 0.0075131325672070... |
1,801.05261 | Operators with Wentzell boundary conditions and the Dirichlet-to-Neumann
operator | In this paper we relate the generator property of an operator $A$ with
(abstract) generalized Wentzell boundary conditions on a Banach space $X$ and
its associated (abstract) Dirichlet-to-Neumann operator $N$ acting on a
"boundary" space $\partial X$. Our approach is based on similarity
transformations and perturbati... | math.FA | in this paper we relate the generator property of an operator a with abstract generalized wentzell boundary conditions on a banach space x and its associated abstract dirichlettoneumann operator n acting on a boundary space partial x our approach is based on similarity transformations and perturbation arguments and all... | [['in', 'this', 'paper', 'we', 'relate', 'the', 'generator', 'property', 'of', 'an', 'operator', 'a', 'with', 'abstract', 'generalized', 'wentzell', 'boundary', 'conditions', 'on', 'a', 'banach', 'space', 'x', 'and', 'its', 'associated', 'abstract', 'dirichlettoneumann', 'operator', 'n', 'acting', 'on', 'a', 'boundary'... | [-0.15342254849636686, 0.12077311172354224, -0.1071942119481231, 0.06341831026635929, -0.14619612765154275, -0.11647640928909507, 0.01879507034048573, 0.3846509098885176, -0.3119732503225838, -0.1303695012761307, 0.15959188481708447, -0.30021804547710496, -0.13616965849296717, 0.1707975359944006, -0.09015916192067275, ... |
1,801.05262 | Root number of the twists of an elliptic curve | We give an explicit description of the behaviour of the root number in the
family given by twists of an elliptic curve $E$ by the rational values of a
polynomial $f(T)$. In particular, we give a criterion (on $f$ depending on $E$)
for the family to have a constant root number over $\mathbb{Q}$. This completes
a work ... | math.NT | we give an explicit description of the behaviour of the root number in the family given by twists of an elliptic curve e by the rational values of a polynomial ft in particular we give a criterion on f depending on e for the family to have a constant root number over mathbbq this completes a work of rohrlich we detail ... | [['we', 'give', 'an', 'explicit', 'description', 'of', 'the', 'behaviour', 'of', 'the', 'root', 'number', 'in', 'the', 'family', 'given', 'by', 'twists', 'of', 'an', 'elliptic', 'curve', 'e', 'by', 'the', 'rational', 'values', 'of', 'a', 'polynomial', 'ft', 'in', 'particular', 'we', 'give', 'a', 'criterion', 'on', 'f',... | [-0.19307991734380464, 0.05484589748400129, -0.08988099615931151, -0.013275428513816771, -0.06618972680340689, -0.09836238874010293, 0.020826343155230385, 0.28770236926804105, -0.25040619295786126, -0.2925586068430489, 0.05967136868275702, -0.26378911408786493, -0.1357887276919581, 0.2631534477822056, -0.10195864900856... |
1,801.05263 | Maximum principles at infinity and the Ahlfors-Khas'minskii duality: an
overview | This note is meant to introduce the reader to a duality principle for
nonlinear equations that recently appeared in the literature. Motivations come
from the desire to give a unifying potential-theoretic framework for various
maximum principles at infinity appearing in the literature (Ekeland, Omori-Yau,
Pigola-Rigol... | math.DG math.AP | this note is meant to introduce the reader to a duality principle for nonlinear equations that recently appeared in the literature motivations come from the desire to give a unifying potentialtheoretic framework for various maximum principles at infinity appearing in the literature ekeland omoriyau pigolarigolisetti as... | [['this', 'note', 'is', 'meant', 'to', 'introduce', 'the', 'reader', 'to', 'a', 'duality', 'principle', 'for', 'nonlinear', 'equations', 'that', 'recently', 'appeared', 'in', 'the', 'literature', 'motivations', 'come', 'from', 'the', 'desire', 'to', 'give', 'a', 'unifying', 'potentialtheoretic', 'framework', 'for', 'va... | [-0.0939675368806663, 0.03980035220494324, -0.09811222272845167, 0.12697358299599235, -0.12046933524563151, -0.1117491676774018, 0.015570000958455316, 0.3034669163684219, -0.32511039838684186, -0.2539572196152314, 0.1403755791124225, -0.2554509396412236, -0.18965518146248186, 0.18568406755132286, -0.11745541354136194, ... |
1,801.05264 | Adaptive Reversible Watermarking Based on Linear Prediction for Medical
Videos | Reversible video watermarking can guarantee that the watermark logo and the
original frame can be recovered from the watermarked frame without any
distortion. Although reversible video watermarking has successfully been
applied in multimedia, its application has not been extensively explored in
medical videos. Revers... | cs.MM cs.GR | reversible video watermarking can guarantee that the watermark logo and the original frame can be recovered from the watermarked frame without any distortion although reversible video watermarking has successfully been applied in multimedia its application has not been extensively explored in medical videos reversible ... | [['reversible', 'video', 'watermarking', 'can', 'guarantee', 'that', 'the', 'watermark', 'logo', 'and', 'the', 'original', 'frame', 'can', 'be', 'recovered', 'from', 'the', 'watermarked', 'frame', 'without', 'any', 'distortion', 'although', 'reversible', 'video', 'watermarking', 'has', 'successfully', 'been', 'applied'... | [-0.06316294003562588, -0.021643498928541602, -0.07836208847131476, 0.07041125067238076, -0.08964749134352637, -0.16407058692259144, 0.017641726687240105, 0.4603679912061327, -0.26469445690098736, -0.2924696589406166, 0.14112550102096671, -0.2856805832176987, -0.14576103295484144, 0.18764738239244455, -0.25182918882864... |
1,801.05265 | Robust sustainable development assessment with composite indices
aggregating interacting dimensions: the hierarchical-SMAA-Choquet integral
approach | The evaluation of sustainable development - and, in particular, rural
development - through composite indices requires taking into account a
plurality of indicators, which are related to economic, social and
environmental aspects. The points of view evaluated by these indices are
naturally interacting: thus, a bonus ... | math.OC | the evaluation of sustainable development and in particular rural development through composite indices requires taking into account a plurality of indicators which are related to economic social and environmental aspects the points of view evaluated by these indices are naturally interacting thus a bonus has to be rec... | [['the', 'evaluation', 'of', 'sustainable', 'development', 'and', 'in', 'particular', 'rural', 'development', 'through', 'composite', 'indices', 'requires', 'taking', 'into', 'account', 'a', 'plurality', 'of', 'indicators', 'which', 'are', 'related', 'to', 'economic', 'social', 'and', 'environmental', 'aspects', 'the',... | [-0.06981417435209238, 0.06209342724575776, -0.10836222984299466, 0.1121341820771107, -0.07820440768030504, -0.12162130351023727, 0.10323917280125673, 0.3657969159252122, -0.24540772456469007, -0.3118168351520932, 0.12134803887627459, -0.2673017382370618, -0.15773749428542339, 0.17131997845549152, -0.11660410124980701,... |
1,801.05266 | Two components of the macroscopic general field | The general field, containing all the macroscopic fields in it, is divided
into the mass component, the source of which is the mass four-current, and the
charge component, the source of which is the charge four-current. The mass
component includes the gravitational field, acceleration field, pressure field,
dissipati... | physics.gen-ph | the general field containing all the macroscopic fields in it is divided into the mass component the source of which is the mass fourcurrent and the charge component the source of which is the charge fourcurrent the mass component includes the gravitational field acceleration field pressure field dissipation field stro... | [['the', 'general', 'field', 'containing', 'all', 'the', 'macroscopic', 'fields', 'in', 'it', 'is', 'divided', 'into', 'the', 'mass', 'component', 'the', 'source', 'of', 'which', 'is', 'the', 'mass', 'fourcurrent', 'and', 'the', 'charge', 'component', 'the', 'source', 'of', 'which', 'is', 'the', 'charge', 'fourcurrent'... | [-0.19867748828338724, 0.16785471467384402, -0.0680405132405992, 0.05315163587136859, -0.07370058247719759, -0.042005051356474206, -0.07745953375207526, 0.28873753702667143, -0.26606043929101103, -0.3041582888191832, 0.05943289367382282, -0.23361535468803984, -0.039688217427049366, 0.16651792674591498, 0.04823724603047... |
1,801.05267 | Doublon formation by ions impacting a strongly correlated finite lattice
system | Strongly correlated systems of fermions have a number of exciting collective
properties. Among them, the creation of a lattice that is occupied by doublons,
i.e. two quantum particles with opposite spins, offers interesting electronic
properties. In the past a variety of methods have been proposed to control
doublon ... | cond-mat.str-el | strongly correlated systems of fermions have a number of exciting collective properties among them the creation of a lattice that is occupied by doublons ie two quantum particles with opposite spins offers interesting electronic properties in the past a variety of methods have been proposed to control doublon formation... | [['strongly', 'correlated', 'systems', 'of', 'fermions', 'have', 'a', 'number', 'of', 'exciting', 'collective', 'properties', 'among', 'them', 'the', 'creation', 'of', 'a', 'lattice', 'that', 'is', 'occupied', 'by', 'doublons', 'ie', 'two', 'quantum', 'particles', 'with', 'opposite', 'spins', 'offers', 'interesting', '... | [-0.150866924089732, 0.26458130735769736, -0.07600245289168917, 0.0146797065935643, 0.006092342919342824, -0.14804221093151215, 0.06689550681668963, 0.41345451198316907, -0.22501103159644315, -0.25555581609542305, 0.009099508185770261, -0.28507759593645327, -0.12165264229432822, 0.15069180352797917, 0.06130520327473982... |
1,801.05268 | Effective theory analysis for vector-like quark model | We study a model with a down-type SU(2) singlet vector-like quark (VLQ) as a
minimal extension of the standard model (SM). In this model, flavor changing
neutral currents (FCNCs) arise at tree level and the unitarity of the $3\times
3$ Cabibbo-Kobayashi-Maskawa (CKM) matrix does not hold. In this paper, we
constrain ... | hep-ph hep-ex | we study a model with a downtype su2 singlet vectorlike quark vlq as a minimal extension of the standard model sm in this model flavor changing neutral currents fcncs arise at tree level and the unitarity of the 3times 3 cabibbokobayashimaskawa ckm matrix does not hold in this paper we constrain the fcnc coupling from ... | [['we', 'study', 'a', 'model', 'with', 'a', 'downtype', 'su2', 'singlet', 'vectorlike', 'quark', 'vlq', 'as', 'a', 'minimal', 'extension', 'of', 'the', 'standard', 'model', 'sm', 'in', 'this', 'model', 'flavor', 'changing', 'neutral', 'currents', 'fcncs', 'arise', 'at', 'tree', 'level', 'and', 'the', 'unitarity', 'of',... | [-0.10235660302793421, 0.23918227455188174, 0.00029505148844478966, 0.13243914309695556, -0.07480295183584577, -0.13897257992892942, 0.11291609309035155, 0.2710648638930059, -0.23196268859379865, -0.268237047264296, 0.04471075147021465, -0.2984037346758948, -0.06919591454587458, 0.09121863276181638, 0.05502259021008073... |
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