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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1,803.05167 | A generalization of the steepest-edge rule and its number of simplex
iterations for a nondegenerate LP | In this paper, we propose a $p$-norm rule, which is a generalization of the
steepest-edge rule, as a pivoting rule for the simplex method. For a
nondegenerate linear programming problem, we show upper bounds for the number
of iterations of the simplex method with the steepest-edge and $p$-norm rules.
One of the upper... | math.OC | in this paper we propose a pnorm rule which is a generalization of the steepestedge rule as a pivoting rule for the simplex method for a nondegenerate linear programming problem we show upper bounds for the number of iterations of the simplex method with the steepestedge and pnorm rules one of the upper bounds is given... | [['in', 'this', 'paper', 'we', 'propose', 'a', 'pnorm', 'rule', 'which', 'is', 'a', 'generalization', 'of', 'the', 'steepestedge', 'rule', 'as', 'a', 'pivoting', 'rule', 'for', 'the', 'simplex', 'method', 'for', 'a', 'nondegenerate', 'linear', 'programming', 'problem', 'we', 'show', 'upper', 'bounds', 'for', 'the', 'nu... | [-0.12333795713720383, 0.05312366440118133, -0.07921799875844221, 0.044761521138504824, -0.08192168569869616, -0.13810354369003083, 0.18368750028221492, 0.2828062138816511, -0.297709073242429, -0.29870257232725234, 0.15536376794909018, -0.2629443990526261, -0.1687482658338237, 0.19086826042659194, -0.048098156119805655... |
1,803.05168 | A 1.6:1 Bandwidth Two-Layer Antireflection Structure for Silicon Matched
to the 190-310 GHz Atmospheric Window | Although high-resistivity, low-loss silicon is an excellent material for THz
transmission optics, its high refractive index necessitates antireflection
treatment. We fabricated a wide-bandwidth, two-layer antireflection treatment
by cutting subwavelength structures into the silicon surface using multi-depth
deep reac... | astro-ph.IM | although highresistivity lowloss silicon is an excellent material for thz transmission optics its high refractive index necessitates antireflection treatment we fabricated a widebandwidth twolayer antireflection treatment by cutting subwavelength structures into the silicon surface using multidepth deep reactive ion et... | [['although', 'highresistivity', 'lowloss', 'silicon', 'is', 'an', 'excellent', 'material', 'for', 'thz', 'transmission', 'optics', 'its', 'high', 'refractive', 'index', 'necessitates', 'antireflection', 'treatment', 'we', 'fabricated', 'a', 'widebandwidth', 'twolayer', 'antireflection', 'treatment', 'by', 'cutting', '... | [-0.06402064946884609, 0.11954503163658294, -0.03880883528700456, -0.12571051489147875, -0.044239911749356924, -0.2777967750038387, 0.03101613847162537, 0.5784311496248149, -0.172513889877897, -0.31239527127131667, 0.06576674678504016, -0.2766105578083432, -0.12211918287482489, 0.22565380223930315, -0.07261238082293232... |
1,803.05169 | Geometrical versus time-series representation of data in quantum control
learning | Recently machine learning techniques have become popular for analysing
physical systems and solving problems occurring in quantum computing. In this
paper we focus on using such techniques for finding the sequence of physical
operations implementing the given quantum logical operation. In this context we
analyse the ... | quant-ph cs.LG | recently machine learning techniques have become popular for analysing physical systems and solving problems occurring in quantum computing in this paper we focus on using such techniques for finding the sequence of physical operations implementing the given quantum logical operation in this context we analyse the flex... | [['recently', 'machine', 'learning', 'techniques', 'have', 'become', 'popular', 'for', 'analysing', 'physical', 'systems', 'and', 'solving', 'problems', 'occurring', 'in', 'quantum', 'computing', 'in', 'this', 'paper', 'we', 'focus', 'on', 'using', 'such', 'techniques', 'for', 'finding', 'the', 'sequence', 'of', 'physi... | [-0.10073762604147604, 0.03712554281767811, -0.08223415091361878, 0.05422686756908023, -0.06425145668840974, -0.15923387761207392, 0.019160270752099744, 0.4154561873538977, -0.2707322761144516, -0.314618145537148, 0.10193986973358168, -0.2127633103930874, -0.19451552817774734, 0.28562469485412983, -0.0873358092427145, ... |
1,803.0517 | xDeepFM: Combining Explicit and Implicit Feature Interactions for
Recommender Systems | Combinatorial features are essential for the success of many commercial
models. Manually crafting these features usually comes with high cost due to
the variety, volume and velocity of raw data in web-scale systems.
Factorization based models, which measure interactions in terms of vector
product, can learn patterns ... | cs.LG cs.IR | combinatorial features are essential for the success of many commercial models manually crafting these features usually comes with high cost due to the variety volume and velocity of raw data in webscale systems factorization based models which measure interactions in terms of vector product can learn patterns of combi... | [['combinatorial', 'features', 'are', 'essential', 'for', 'the', 'success', 'of', 'many', 'commercial', 'models', 'manually', 'crafting', 'these', 'features', 'usually', 'comes', 'with', 'high', 'cost', 'due', 'to', 'the', 'variety', 'volume', 'and', 'velocity', 'of', 'raw', 'data', 'in', 'webscale', 'systems', 'factor... | [-0.05062894443899654, 0.019743582632177174, -0.07519585977608681, 0.08734434445362065, -0.11681331859149954, -0.2067528785504564, -0.009463602129120804, 0.4414146968996839, -0.3114999365081945, -0.31988861754928766, 0.04783005894543685, -0.3024539123840728, -0.2251172781719728, 0.16746800433815734, -0.0716512934815367... |
1,803.05171 | High fidelity field stop collection for polarization-entangled photon
pair sources | We present an experimental demonstration of a bright and high fidelity
polarization entangled photon pair source. The source is constructed using two
critically phase matched $\beta$-Barium Borate crystals with parallel optical
axes and photon pairs are collected after filtering with a circular field-stop.
Near unity... | quant-ph | we present an experimental demonstration of a bright and high fidelity polarization entangled photon pair source the source is constructed using two critically phase matched betabarium borate crystals with parallel optical axes and photon pairs are collected after filtering with a circular fieldstop near unity fideliti... | [['we', 'present', 'an', 'experimental', 'demonstration', 'of', 'a', 'bright', 'and', 'high', 'fidelity', 'polarization', 'entangled', 'photon', 'pair', 'source', 'the', 'source', 'is', 'constructed', 'using', 'two', 'critically', 'phase', 'matched', 'betabarium', 'borate', 'crystals', 'with', 'parallel', 'optical', 'a... | [-0.13151368758568138, 0.17503212866793938, -0.03362010900095543, -0.004237679906723583, -0.02099566472073396, -0.17512778022358486, 0.043696405350084545, 0.5013483939509765, -0.18798755673125533, -0.31418208225958927, 0.06013046257088289, -0.3369920471153569, -0.003976308302406003, 0.2679335147909382, 0.01577997560996... |
1,803.05172 | Intermittent electron density and temperature fluctuations and
associated fluxes in the Alcator C-Mod scrape-off layer | The Alcator C-Mod mirror Langmuir probe system has been used to sample data
time series of fluctuating plasma parameters in the outboard mid-plane far
scrape-off layer. We present a statistical analysis of one second long time
series of electron density, temperature, radial electric drift velocity and the
correspondi... | physics.plasm-ph | the alcator cmod mirror langmuir probe system has been used to sample data time series of fluctuating plasma parameters in the outboard midplane far scrapeoff layer we present a statistical analysis of one second long time series of electron density temperature radial electric drift velocity and the corresponding parti... | [['the', 'alcator', 'cmod', 'mirror', 'langmuir', 'probe', 'system', 'has', 'been', 'used', 'to', 'sample', 'data', 'time', 'series', 'of', 'fluctuating', 'plasma', 'parameters', 'in', 'the', 'outboard', 'midplane', 'far', 'scrapeoff', 'layer', 'we', 'present', 'a', 'statistical', 'analysis', 'of', 'one', 'second', 'lo... | [-0.12022617300079155, 0.24852664781002234, -0.08094068568256073, 0.09284088185111238, 0.029167772207513515, -0.09703516489464854, -0.008566430893301129, 0.3736160748582012, -0.24337355400323227, -0.3048376005889591, 0.0607458500594005, -0.29584507464265886, 0.01257846906885569, 0.20881584566889394, 0.03690015691220118... |
1,803.05173 | Constrained BRST-BFV and BRST-BV Lagrangians for half-integer HS fields
on $R^{1,d-1}$ | Gauge invariant Lagrangian descriptions of irreducible and reducible
half-integer higher-spin mixed-symmetric massless and massive representations
of the Poincare group with off-shell algebraic constraints are constructed
within a metric-like formulation in a $d$-dimensional flat space-time on the
basis of a suggeste... | hep-th math-ph math.DS math.MP quant-ph | gauge invariant lagrangian descriptions of irreducible and reducible halfinteger higherspin mixedsymmetric massless and massive representations of the poincare group with offshell algebraic constraints are constructed within a metriclike formulation in a ddimensional flat spacetime on the basis of a suggested constrain... | [['gauge', 'invariant', 'lagrangian', 'descriptions', 'of', 'irreducible', 'and', 'reducible', 'halfinteger', 'higherspin', 'mixedsymmetric', 'massless', 'and', 'massive', 'representations', 'of', 'the', 'poincare', 'group', 'with', 'offshell', 'algebraic', 'constraints', 'are', 'constructed', 'within', 'a', 'metriclik... | [-0.15610478952349652, 0.1862950815065276, -0.08750656150458824, 0.10950645979139068, -0.12761360602896837, -0.1628871105478278, -0.056036489616547315, 0.31885203934230266, -0.1906788488051721, -0.29340530873741955, 0.034980184897514324, -0.17564088730585006, -0.14532170046032183, 0.06521057180749873, -0.06763941625665... |
1,803.05174 | Multi-objective Analysis of MAP-Elites Performance | In certain complex optimization tasks, it becomes necessary to use multiple
measures to characterize the performance of different algorithms. This paper
presents a method that combines ordinal effect sizes with Pareto dominance to
analyze such cases. Since the method is ordinal, it can also generalize across
differen... | cs.NE | in certain complex optimization tasks it becomes necessary to use multiple measures to characterize the performance of different algorithms this paper presents a method that combines ordinal effect sizes with pareto dominance to analyze such cases since the method is ordinal it can also generalize across different opti... | [['in', 'certain', 'complex', 'optimization', 'tasks', 'it', 'becomes', 'necessary', 'to', 'use', 'multiple', 'measures', 'to', 'characterize', 'the', 'performance', 'of', 'different', 'algorithms', 'this', 'paper', 'presents', 'a', 'method', 'that', 'combines', 'ordinal', 'effect', 'sizes', 'with', 'pareto', 'dominanc... | [-0.06871008178026512, 0.05724346209558305, -0.11592690788594813, 0.10389536243927633, -0.08488557950176041, -0.14505902149489727, 0.048037690260640246, 0.4298213555895049, -0.2769418837052995, -0.3384309083737176, 0.07638741965036325, -0.23041755795992655, -0.20507894194331663, 0.2242242149414559, -0.09813126926792079... |
1,803.05175 | The dynamics of thin gas layer moving between two fluids | The dynamics and stability of a thin gas layer moving between two fluid
layers moving in the same or opposite direction is studied. The linear
evolutionary equations describing the spatial-temporal dynamics of the
interface perturbations between gas and two fluid layers are derived for the
flat two-dimensional case. ... | physics.flu-dyn | the dynamics and stability of a thin gas layer moving between two fluid layers moving in the same or opposite direction is studied the linear evolutionary equations describing the spatialtemporal dynamics of the interface perturbations between gas and two fluid layers are derived for the flat twodimensional case integr... | [['the', 'dynamics', 'and', 'stability', 'of', 'a', 'thin', 'gas', 'layer', 'moving', 'between', 'two', 'fluid', 'layers', 'moving', 'in', 'the', 'same', 'or', 'opposite', 'direction', 'is', 'studied', 'the', 'linear', 'evolutionary', 'equations', 'describing', 'the', 'spatialtemporal', 'dynamics', 'of', 'the', 'interf... | [-0.18426119888358194, 0.11258735434643717, -0.04983942264354684, 0.027967193768644292, -0.010992264582051171, -0.1252565537223644, -0.05234504002025157, 0.33269060919216525, -0.29131516108302297, -0.2680030484423494, 0.1255196879169994, -0.293051952308613, -0.1200695566836253, 0.1876702271256363, 0.06574113304506884, ... |
1,803.05176 | Localization due to topological stochastic disorder in active networks | An active network is a prototype model in non-equilibrium statistical
mechanics. It can represent, for example, a system with particles that have a
self-propulsion mechanism. Each node of the network specifies a possible
location of a particle, and its orientation. The orientation (which is formally
like a spin degre... | cond-mat.stat-mech cond-mat.dis-nn cond-mat.soft quant-ph | an active network is a prototype model in nonequilibrium statistical mechanics it can represent for example a system with particles that have a selfpropulsion mechanism each node of the network specifies a possible location of a particle and its orientation the orientation which is formally like a spin degree of freedo... | [['an', 'active', 'network', 'is', 'a', 'prototype', 'model', 'in', 'nonequilibrium', 'statistical', 'mechanics', 'it', 'can', 'represent', 'for', 'example', 'a', 'system', 'with', 'particles', 'that', 'have', 'a', 'selfpropulsion', 'mechanism', 'each', 'node', 'of', 'the', 'network', 'specifies', 'a', 'possible', 'loc... | [-0.18768860840223608, 0.17193498357930798, -0.0823178406872396, 0.048655134759673105, -0.047607523339089526, -0.145566089962539, 0.021785931309975522, 0.3702130898562891, -0.287103925971815, -0.28580611565160335, 0.04057765950796805, -0.2497277186616444, -0.18657628408012292, 0.11940492966440155, -0.051242784902413366... |
1,803.05177 | Electrical conductivity of carbon nanofiber reinforced resins:
potentiality of Tunneling Atomic Force Microscopy (TUNA) technique | Epoxy nanocomposites able to meet pressing industrial requirements in the
field of structural material have been developed and characterized. Tunneling
Atomic Force Microscopy (TUNA), which is able to detect ultra-low currents
ranging from 80 fA to 120 pA, was used to correlate the local topography with
electrical pr... | physics.app-ph cond-mat.mtrl-sci | epoxy nanocomposites able to meet pressing industrial requirements in the field of structural material have been developed and characterized tunneling atomic force microscopy tuna which is able to detect ultralow currents ranging from 80 fa to 120 pa was used to correlate the local topography with electrical properties... | [['epoxy', 'nanocomposites', 'able', 'to', 'meet', 'pressing', 'industrial', 'requirements', 'in', 'the', 'field', 'of', 'structural', 'material', 'have', 'been', 'developed', 'and', 'characterized', 'tunneling', 'atomic', 'force', 'microscopy', 'tuna', 'which', 'is', 'able', 'to', 'detect', 'ultralow', 'currents', 'ra... | [-0.02263278226858994, 0.16236339465801403, -0.038287971615215244, -0.046440266383591, -0.0067554228583869246, -0.1921613197485657, 0.06354454061743736, 0.43618167388569756, -0.2690426217651321, -0.3773419468365994, 0.040924332827718485, -0.3161145734898362, -0.10040047602516781, 0.1825481187744239, -0.0330130569636821... |
1,803.05178 | Shape resonances of Be$^-$ and Mg$^-$ investigated with method of
analytic continuation | The regularized method of analytic continuation is used to study the
low-energy negative ion states of beryllium (configuration 2$s^2\varepsilon p\;
^2P$) and magnesium (configuration 3$s^2\varepsilon p\; ^2P$) atoms. The method
applies an additional perturbation potential and it requires only routine
bound-state mul... | physics.chem-ph | the regularized method of analytic continuation is used to study the lowenergy negative ion states of beryllium configuration 2s2varepsilon p 2p and magnesium configuration 3s2varepsilon p 2p atoms the method applies an additional perturbation potential and it requires only routine boundstate multielectron quantum calc... | [['the', 'regularized', 'method', 'of', 'analytic', 'continuation', 'is', 'used', 'to', 'study', 'the', 'lowenergy', 'negative', 'ion', 'states', 'of', 'beryllium', 'configuration', '2s2varepsilon', 'p', '2p', 'and', 'magnesium', 'configuration', '3s2varepsilon', 'p', '2p', 'atoms', 'the', 'method', 'applies', 'an', 'a... | [-0.04251020007016931, 0.11711024627980163, -0.011025685498573105, 0.0866264662327012, 0.02210089673719588, -0.174619544598767, 0.03972098714781597, 0.4037705607547918, -0.20962924966999494, -0.32897319374623135, 0.012738593733314808, -0.28789848985958516, -0.052106363859767205, 0.19270320197307123, 0.04901154800138423... |
1,803.05179 | Transmission Spectroscopy with the ACE-FTS Infrared Spectral Atlas of
Earth: A Model Validation and Feasibility Study | Infrared solar occultation measurements are well established for remote
sensing of Earth's atmosphere, and the corresponding primary transit
spectroscopy has turned out to be valuable for characterization of extrasolar
planets. Our objective is an assessment of the detectability of molecular
signatures in Earth's tra... | astro-ph.EP | infrared solar occultation measurements are well established for remote sensing of earths atmosphere and the corresponding primary transit spectroscopy has turned out to be valuable for characterization of extrasolar planets our objective is an assessment of the detectability of molecular signatures in earths transit s... | [['infrared', 'solar', 'occultation', 'measurements', 'are', 'well', 'established', 'for', 'remote', 'sensing', 'of', 'earths', 'atmosphere', 'and', 'the', 'corresponding', 'primary', 'transit', 'spectroscopy', 'has', 'turned', 'out', 'to', 'be', 'valuable', 'for', 'characterization', 'of', 'extrasolar', 'planets', 'ou... | [-0.07289431006403772, 0.09824732487817413, -0.05112691007275226, 0.06885773391672687, -0.027806403726917277, -0.0762779260681861, 0.06824529915725952, 0.3971004011661639, -0.21453258998530067, -0.3657823469003905, 0.10460143151974652, -0.31626987437121273, -0.10059572772970497, 0.17758705627206314, -0.0691185519688214... |
1,803.0518 | Bose-Einstein Condensation in a Dilute, Trapped Gas at Positive
Temperature | We consider an interacting, dilute Bose gas trapped in a harmonic potential
at a positive temperature. The system is analyzed in a combination of a
thermodynamic and a Gross-Pitaevskii (GP) limit where the trap frequency
$\omega$, the temperature $T$ and the particle number $N$ are related by $N
\sim (T / \omega)^{3}... | math-ph cond-mat.quant-gas math.MP | we consider an interacting dilute bose gas trapped in a harmonic potential at a positive temperature the system is analyzed in a combination of a thermodynamic and a grosspitaevskii gp limit where the trap frequency omega the temperature t and the particle number n are related by n sim t omega3 toinfty while the scatte... | [['we', 'consider', 'an', 'interacting', 'dilute', 'bose', 'gas', 'trapped', 'in', 'a', 'harmonic', 'potential', 'at', 'a', 'positive', 'temperature', 'the', 'system', 'is', 'analyzed', 'in', 'a', 'combination', 'of', 'a', 'thermodynamic', 'and', 'a', 'grosspitaevskii', 'gp', 'limit', 'where', 'the', 'trap', 'frequency... | [-0.13874686220660806, 0.18733904616537983, -0.059774279844714326, 0.04951971866830718, 0.05116602508642245, -0.10725223489280325, 0.0332035769810318, 0.305197477072943, -0.26132781388005244, -0.27497686300994245, 0.022326120591606012, -0.3099524729070254, -0.043927294775494376, 0.11686182232006104, 0.04025163792757667... |
1,803.05181 | Can Autism be Catered with Artificial Intelligence-Assisted Intervention
Technology? A Literature Review | This article presents an extensive literature review of technology based
intervention methodologies for individuals facing Autism Spectrum Disorder
(ASD). Reviewed methodologies include: contemporary Computer Aided Systems
(CAS), Computer Vision Assisted Technologies (CVAT) and Virtual Reality (VR) or
Artificial Inte... | cs.HC cs.AI cs.LG | this article presents an extensive literature review of technology based intervention methodologies for individuals facing autism spectrum disorder asd reviewed methodologies include contemporary computer aided systems cas computer vision assisted technologies cvat and virtual reality vr or artificial intelligence aias... | [['this', 'article', 'presents', 'an', 'extensive', 'literature', 'review', 'of', 'technology', 'based', 'intervention', 'methodologies', 'for', 'individuals', 'facing', 'autism', 'spectrum', 'disorder', 'asd', 'reviewed', 'methodologies', 'include', 'contemporary', 'computer', 'aided', 'systems', 'cas', 'computer', 'v... | [-0.05492649721680209, 0.0559839096620999, -0.08587873784592376, 0.04874105375551153, -0.13767107375955676, -0.20356220516841858, 0.042535899258218705, 0.414371363054961, -0.17732277291826903, -0.32486313092522323, 0.11627810451784171, -0.2597481382731348, -0.24435520194238053, 0.2626640706305625, -0.17386133410269394,... |
1,803.05182 | Approximative Theorem of Incomplete Riemann-Stieltjes Sum of Stochastic
Integral | The approximative theorems of incomplete Riemann-Stieltjes sums of Ito
stochastic integral, mean square integral and Stratonovich stochastic integral
with respect to Brownian motion are investigated. Some sufficient conditions of
incomplete Riemann-Stieltjes sums approaching stochastic integral are
developed, which e... | math.PR cs.NA | the approximative theorems of incomplete riemannstieltjes sums of ito stochastic integral mean square integral and stratonovich stochastic integral with respect to brownian motion are investigated some sufficient conditions of incomplete riemannstieltjes sums approaching stochastic integral are developed which establis... | [['the', 'approximative', 'theorems', 'of', 'incomplete', 'riemannstieltjes', 'sums', 'of', 'ito', 'stochastic', 'integral', 'mean', 'square', 'integral', 'and', 'stratonovich', 'stochastic', 'integral', 'with', 'respect', 'to', 'brownian', 'motion', 'are', 'investigated', 'some', 'sufficient', 'conditions', 'of', 'inc... | [-0.13664276765969893, -0.0025596355059833236, -0.10115564503057888, 0.15080390167845922, -0.17803539451084693, -0.09221288002851052, -0.020173426449411745, 0.38541646397700813, -0.3599004497412931, -0.2013897243860728, 0.1966685527145411, -0.284099830596736, -0.17302099460820583, 0.22632633143979491, -0.15647484010762... |
1,803.05183 | Cross Feshbach resonance | Feshbach resonance occurs when a pair of free particles is resonantly coupled
to a molecular bound state. In the field of ultracold quantum gases, atomic
Feshbach resonances became a usual tool for tailoring atomic interactions
opening up many new applications in this field. In a semiconductor microcavity,
the Feshba... | cond-mat.mes-hall | feshbach resonance occurs when a pair of free particles is resonantly coupled to a molecular bound state in the field of ultracold quantum gases atomic feshbach resonances became a usual tool for tailoring atomic interactions opening up many new applications in this field in a semiconductor microcavity the feshbach res... | [['feshbach', 'resonance', 'occurs', 'when', 'a', 'pair', 'of', 'free', 'particles', 'is', 'resonantly', 'coupled', 'to', 'a', 'molecular', 'bound', 'state', 'in', 'the', 'field', 'of', 'ultracold', 'quantum', 'gases', 'atomic', 'feshbach', 'resonances', 'became', 'a', 'usual', 'tool', 'for', 'tailoring', 'atomic', 'in... | [-0.17295363957768883, 0.27753872660085044, -0.055938397288916565, 0.06799126979092072, -0.020386062249348594, -0.1755929599483979, 0.07205150950346784, 0.38132001151298656, -0.22453764840832044, -0.27804070645622136, -0.08501980850665734, -0.2652311620302498, -0.035689431979674203, 0.23613013320056528, 0.1073774735126... |
1,803.05184 | A unified approach to fixed-wing aircraft path following guidance and
control | This paper addresses the path following control problem for scale-model
fixed-wing aircraft. Kinematic guidance and dynamic control laws are developed
within a single coherent framework that exploits a simple generic model of
aerodynamics forces acting on the aircraft and applies to almost all regular 3D
paths. The p... | cs.SY | this paper addresses the path following control problem for scalemodel fixedwing aircraft kinematic guidance and dynamic control laws are developed within a single coherent framework that exploits a simple generic model of aerodynamics forces acting on the aircraft and applies to almost all regular 3d paths the propose... | [['this', 'paper', 'addresses', 'the', 'path', 'following', 'control', 'problem', 'for', 'scalemodel', 'fixedwing', 'aircraft', 'kinematic', 'guidance', 'and', 'dynamic', 'control', 'laws', 'are', 'developed', 'within', 'a', 'single', 'coherent', 'framework', 'that', 'exploits', 'a', 'simple', 'generic', 'model', 'of',... | [-0.14655942432582378, 0.05215593228737513, -0.06430942133301869, 0.03159421002337088, -0.0882099524140358, -0.15433322956164677, 0.027721878477993112, 0.38239488468815885, -0.24795449810723463, -0.28744354570905367, 0.14505067420502504, -0.223441212537388, -0.15292801183337967, 0.2868213331171622, -0.09748349405514697... |
1,803.05185 | The influence of Coulomb correlations on nonequilibrium quantum
transport in quadruple quantum-dot structure | The description of quantum transport in a quadruple quantum-dot structure
(QQD) is proposed taking into account the Coulomb correlations and nonzero bias
voltages. To achieve this goal the combination of nonequilibrium Green's
functions and equation-of-motion technique is used. It is shown that the
anisotropy of kine... | cond-mat.mes-hall | the description of quantum transport in a quadruple quantumdot structure qqd is proposed taking into account the coulomb correlations and nonzero bias voltages to achieve this goal the combination of nonequilibrium greens functions and equationofmotion technique is used it is shown that the anisotropy of kinetic proces... | [['the', 'description', 'of', 'quantum', 'transport', 'in', 'a', 'quadruple', 'quantumdot', 'structure', 'qqd', 'is', 'proposed', 'taking', 'into', 'account', 'the', 'coulomb', 'correlations', 'and', 'nonzero', 'bias', 'voltages', 'to', 'achieve', 'this', 'goal', 'the', 'combination', 'of', 'nonequilibrium', 'greens', ... | [-0.1860825788068016, 0.1283306814692979, -0.08406362636014819, 0.1053495700445233, -0.027256596523026626, -0.14697398099944822, -0.008330782840494067, 0.3329928876625167, -0.2888803085157027, -0.29583761204654974, -0.07395823228224697, -0.298419188718415, -0.17523122656986945, 0.18670990398774545, 0.009242971500174866... |
1,803.05186 | Determinantal elliptic Selberg integrals | The classical Selberg integral contains a power of the Vandermonde
determinant. When that power is a square, it is easy to prove Selberg's
identity by interpreting it as a determinant of one-variable integrals. We give
similar proofs of summation and transformation formulas for continuous and
discrete elliptic Selber... | math.CA math.CO | the classical selberg integral contains a power of the vandermonde determinant when that power is a square it is easy to prove selbergs identity by interpreting it as a determinant of onevariable integrals we give similar proofs of summation and transformation formulas for continuous and discrete elliptic selberg integ... | [['the', 'classical', 'selberg', 'integral', 'contains', 'a', 'power', 'of', 'the', 'vandermonde', 'determinant', 'when', 'that', 'power', 'is', 'a', 'square', 'it', 'is', 'easy', 'to', 'prove', 'selbergs', 'identity', 'by', 'interpreting', 'it', 'as', 'a', 'determinant', 'of', 'onevariable', 'integrals', 'we', 'give',... | [-0.13783741716711953, 0.021469925444173088, -0.11334809824876801, 0.14233822217145542, -0.11998436324508258, -0.15293731252518547, 0.00516244030268994, 0.2986616611244603, -0.2772800587183258, -0.23365612278207087, 0.14090813467980848, -0.2669400952028399, -0.210679584682073, 0.26017194963408746, -0.10634693178626164,... |
1,803.05187 | Interlocked permutations | The zero-error capacity of channels with a countably infinite input alphabet
formally generalises Shannon's classical problem about the capacity of discrete
memoryless channels. We solve the problem for three particular channels. Our
results are purely combinatorial and in line with previous work of the third
author ... | math.CO | the zeroerror capacity of channels with a countably infinite input alphabet formally generalises shannons classical problem about the capacity of discrete memoryless channels we solve the problem for three particular channels our results are purely combinatorial and in line with previous work of the third author about ... | [['the', 'zeroerror', 'capacity', 'of', 'channels', 'with', 'a', 'countably', 'infinite', 'input', 'alphabet', 'formally', 'generalises', 'shannons', 'classical', 'problem', 'about', 'the', 'capacity', 'of', 'discrete', 'memoryless', 'channels', 'we', 'solve', 'the', 'problem', 'for', 'three', 'particular', 'channels',... | [-0.18177454722855163, 0.06528641630382258, -0.03157547253127001, 0.04653677359527471, -0.10578576517196334, -0.23279621869287626, 0.1700587246605024, 0.3206677639058658, -0.3447473191998291, -0.24512149347942702, 0.1118250329900362, -0.3008582152578296, -0.09679985197964219, 0.17934267564049486, -0.16631023443246984, ... |
1,803.05188 | Measurement of forward top pair production in the dilepton channel in
$pp$ collisions at $\sqrt{s}=13$ TeV | Forward top quark pair production is studied in $pp$ collisions in the $\mu
eb$ final state using a data sample corresponding to an integrated luminosity
of 1.93 fb$^{-1}$ collected with the LHCb experiment at a centre-of-mass energy
of 13 TeV. The cross-section is measured in a fiducial region where both
leptons hav... | hep-ex | forward top quark pair production is studied in pp collisions in the mu eb final state using a data sample corresponding to an integrated luminosity of 193 fb1 collected with the lhcb experiment at a centreofmass energy of 13 tev the crosssection is measured in a fiducial region where both leptons have a transverse mom... | [['forward', 'top', 'quark', 'pair', 'production', 'is', 'studied', 'in', 'pp', 'collisions', 'in', 'the', 'mu', 'eb', 'final', 'state', 'using', 'a', 'data', 'sample', 'corresponding', 'to', 'an', 'integrated', 'luminosity', 'of', '193', 'fb1', 'collected', 'with', 'the', 'lhcb', 'experiment', 'at', 'a', 'centreofmass... | [-0.06913465693425272, 0.20704544116375947, -0.06832160526649413, 0.10786381397997925, -0.01394785502318131, -0.09349734845906728, -0.009959918744746388, 0.3566656755905321, -0.19990349091265514, -0.3915814169746193, -0.009599611983108132, -0.37729170402477247, 0.14044830665825317, 0.16048042753187836, 0.04743259162219... |
1,803.05189 | Band Structure Dynamics in Indium Wires | One-dimensional Indium wires grown on Si(111) substrates, which are metallic
at high temperatures, become insulating below $\sim100$ K due to the formation
of a Charge Density Wave (CDW). The physics of this transition is not
conventional and involves a multiband Peierls instability with strong interband
coupling. Th... | cond-mat.mtrl-sci cond-mat.mes-hall | onedimensional indium wires grown on si111 substrates which are metallic at high temperatures become insulating below sim100 k due to the formation of a charge density wave cdw the physics of this transition is not conventional and involves a multiband peierls instability with strong interband coupling this cdw ground ... | [['onedimensional', 'indium', 'wires', 'grown', 'on', 'si111', 'substrates', 'which', 'are', 'metallic', 'at', 'high', 'temperatures', 'become', 'insulating', 'below', 'sim100', 'k', 'due', 'to', 'the', 'formation', 'of', 'a', 'charge', 'density', 'wave', 'cdw', 'the', 'physics', 'of', 'this', 'transition', 'is', 'not'... | [-0.17175018248458704, 0.26093956066295504, -0.07251210378638158, -0.0015632879198528827, -0.030948553622389834, -0.11774092437699438, 0.11955833001372715, 0.4342787390202284, -0.254490629574284, -0.26845633512052397, 0.04767810151369001, -0.30438311176064115, -0.09015112764512499, 0.1355177741808196, 0.047478974565553... |
1,803.0519 | Higher order concentration in presence of Poincar\'e-type inequalities | We show sharpened forms of the concentration of measure phenomenon typically
centered at stochastic expansions of order $d-1$ for any $d \in \mathbb{N}$.
Here we focus on differentiable functions on the Euclidean space in presence of
a Poincar\'e-type inequality. The bounds are based on $d$-th order derivatives.
| math.PR | we show sharpened forms of the concentration of measure phenomenon typically centered at stochastic expansions of order d1 for any d in mathbbn here we focus on differentiable functions on the euclidean space in presence of a poincaretype inequality the bounds are based on dth order derivatives | [['we', 'show', 'sharpened', 'forms', 'of', 'the', 'concentration', 'of', 'measure', 'phenomenon', 'typically', 'centered', 'at', 'stochastic', 'expansions', 'of', 'order', 'd1', 'for', 'any', 'd', 'in', 'mathbbn', 'here', 'we', 'focus', 'on', 'differentiable', 'functions', 'on', 'the', 'euclidean', 'space', 'in', 'pre... | [-0.15468615356912005, 0.06546482392289538, -0.05843924985643714, 0.07196574705712339, -0.053222691323211856, -0.07563138466843582, 0.02877250747715539, 0.34080836842668816, -0.23320044525601763, -0.19948798943152454, 0.15210964678826325, -0.3156235421576755, -0.16823383519782664, 0.19242153564428396, -0.06809335026117... |
1,803.05191 | Two-variable polynomial invariants of virtual knots arising from flat
virtual knot invariants | We introduce two sequences of two-variable polynomials $\{ L^n_K (t,
\ell)\}_{n=1}^{\infty}$ and $\{ F^n_K (t, \ell)\}_{n=1}^{\infty}$, expressed in
terms of index value of a crossing and $n$-dwrithe value of a virtual knot $K$,
where $t$ and $\ell$ are variables. Basing on the fact that $n$-dwrithe is a
flat virtual... | math.GT | we introduce two sequences of twovariable polynomials ln_k t ell_n1infty and fn_k t ell_n1infty expressed in terms of index value of a crossing and ndwrithe value of a virtual knot k where t and ell are variables basing on the fact that ndwrithe is a flat virtual knot invariant we prove that ln_k and fn_k are virtual k... | [['we', 'introduce', 'two', 'sequences', 'of', 'twovariable', 'polynomials', 'ln_k', 't', 'ell_n1infty', 'and', 'fn_k', 't', 'ell_n1infty', 'expressed', 'in', 'terms', 'of', 'index', 'value', 'of', 'a', 'crossing', 'and', 'ndwrithe', 'value', 'of', 'a', 'virtual', 'knot', 'k', 'where', 't', 'and', 'ell', 'are', 'variab... | [-0.27092918778380637, 0.16195355140002846, -0.11967537034585883, 0.07578170022638396, -0.11240056513726146, -0.2113105102347894, 0.03442158792580513, 0.34700064366989875, -0.28302023265086396, -0.2782685138311685, 0.060629127887549185, -0.18489231895419617, -0.1851506165547084, 0.15808783973791177, -0.1147107731409465... |
1,803.05192 | Real-time Cardiovascular MR with Spatio-temporal Artifact Suppression
using Deep Learning - Proof of Concept in Congenital Heart Disease | PURPOSE: Real-time assessment of ventricular volumes requires high
acceleration factors. Residual convolutional neural networks (CNN) have shown
potential for removing artifacts caused by data undersampling. In this study we
investigated the effect of different radial sampling patterns on the accuracy
of a CNN. We al... | cs.CV cs.NE | purpose realtime assessment of ventricular volumes requires high acceleration factors residual convolutional neural networks cnn have shown potential for removing artifacts caused by data undersampling in this study we investigated the effect of different radial sampling patterns on the accuracy of a cnn we also acquir... | [['purpose', 'realtime', 'assessment', 'of', 'ventricular', 'volumes', 'requires', 'high', 'acceleration', 'factors', 'residual', 'convolutional', 'neural', 'networks', 'cnn', 'have', 'shown', 'potential', 'for', 'removing', 'artifacts', 'caused', 'by', 'data', 'undersampling', 'in', 'this', 'study', 'we', 'investigate... | [-0.01056394628795548, -0.0021734338595854994, -0.04425889388895689, 0.08198427252414427, -0.058276948992314996, -0.18182861610904943, 0.005963044739518391, 0.46526188725719647, -0.21039089265146427, -0.34961046010982816, 0.11374903423474075, -0.26597789976821873, -0.14256737676202033, 0.23362158068018604, -0.148082079... |
1,803.05193 | Approximation of quantum control correction scheme using deep neural
networks | We study the functional relationship between quantum control pulses in the
idealized case and the pulses in the presence of an unwanted drift. We show
that a class of artificial neural networks called LSTM is able to model this
functional relationship with high efficiency, and hence the correction scheme
required to ... | quant-ph cs.LG | we study the functional relationship between quantum control pulses in the idealized case and the pulses in the presence of an unwanted drift we show that a class of artificial neural networks called lstm is able to model this functional relationship with high efficiency and hence the correction scheme required to coun... | [['we', 'study', 'the', 'functional', 'relationship', 'between', 'quantum', 'control', 'pulses', 'in', 'the', 'idealized', 'case', 'and', 'the', 'pulses', 'in', 'the', 'presence', 'of', 'an', 'unwanted', 'drift', 'we', 'show', 'that', 'a', 'class', 'of', 'artificial', 'neural', 'networks', 'called', 'lstm', 'is', 'able... | [-0.12849278407280937, 0.06318061127317111, -0.0872260114945033, 0.06572469962651238, -0.019897956225801917, -0.12985394362031538, 0.05469221282092964, 0.3867429709609817, -0.3176875072367051, -0.3211112484445467, 0.06562427749090335, -0.25752304145699945, -0.21188037656247616, 0.17748717076473813, -0.07951363509740023... |
1,803.05194 | Semisimple pointed isogeny graphs for abelian varieties | In this paper we show that if $\phi_{i}:A_{i}\rightarrow{A}$ is a semisimple
pointed $K$-rational $\ell$-isogeny graph of order $n$ for a prime $\ell$, then
the group of $\ell$-torsion points $A[\ell](\overline{K})$ contains a subspace
of dimension $n$ generated by $K$-rational points. We also show that the same
resu... | math.AG | in this paper we show that if phi_ia_irightarrowa is a semisimple pointed krational ellisogeny graph of order n for a prime ell then the group of elltorsion points aelloverlinek contains a subspace of dimension n generated by krational points we also show that the same result is true for elliptic curves without the sem... | [['in', 'this', 'paper', 'we', 'show', 'that', 'if', 'phi_ia_irightarrowa', 'is', 'a', 'semisimple', 'pointed', 'krational', 'ellisogeny', 'graph', 'of', 'order', 'n', 'for', 'a', 'prime', 'ell', 'then', 'the', 'group', 'of', 'elltorsion', 'points', 'aelloverlinek', 'contains', 'a', 'subspace', 'of', 'dimension', 'n', ... | [-0.22159065501261, 0.0785630633907056, -0.12480362941435463, 0.08217250674371482, -0.10902848811442586, -0.16600919772266737, 0.011435262306681456, 0.3246163136602656, -0.2707370048187472, -0.19532030044010262, 0.07362235303987069, -0.24045912719432366, -0.1808181736379157, 0.22223943319624742, -0.14586587006075158, -... |
1,803.05195 | Finite amplitude transverse oscillations of a magnetic rope | The effects of finite amplitudes on the transverse oscillations of a
quiescent prominence represented by a magnetic rope are investigated in terms
of the model proposed by Kolotkov et al. 2016. We consider a weakly nonlinear
case governed by a quadratic nonlinearity, and also analyse the fully nonlinear
equations of ... | astro-ph.SR | the effects of finite amplitudes on the transverse oscillations of a quiescent prominence represented by a magnetic rope are investigated in terms of the model proposed by kolotkov et al 2016 we consider a weakly nonlinear case governed by a quadratic nonlinearity and also analyse the fully nonlinear equations of motio... | [['the', 'effects', 'of', 'finite', 'amplitudes', 'on', 'the', 'transverse', 'oscillations', 'of', 'a', 'quiescent', 'prominence', 'represented', 'by', 'a', 'magnetic', 'rope', 'are', 'investigated', 'in', 'terms', 'of', 'the', 'model', 'proposed', 'by', 'kolotkov', 'et', 'al', '2016', 'we', 'consider', 'a', 'weakly', ... | [-0.1912079970329964, 0.2534163831410786, -0.001022405351082293, 0.06763297519825685, -0.057915668483250415, -0.08513857766609782, 0.028740326458444963, 0.35714989067771685, -0.2456726018876697, -0.2937832920919531, 0.07978661464160093, -0.2363659157472564, -0.10732379468748919, 0.21074784924186624, 0.02212533893717381... |
1,803.05196 | EdgeStereo: A Context Integrated Residual Pyramid Network for Stereo
Matching | Recent convolutional neural networks, especially end-to-end disparity
estimation models, achieve remarkable performance on stereo matching task.
However, existed methods, even with the complicated cascade structure, may fail
in the regions of non-textures, boundaries and tiny details. Focus on these
problems, we prop... | cs.CV | recent convolutional neural networks especially endtoend disparity estimation models achieve remarkable performance on stereo matching task however existed methods even with the complicated cascade structure may fail in the regions of nontextures boundaries and tiny details focus on these problems we propose a multitas... | [['recent', 'convolutional', 'neural', 'networks', 'especially', 'endtoend', 'disparity', 'estimation', 'models', 'achieve', 'remarkable', 'performance', 'on', 'stereo', 'matching', 'task', 'however', 'existed', 'methods', 'even', 'with', 'the', 'complicated', 'cascade', 'structure', 'may', 'fail', 'in', 'the', 'region... | [-0.08672642071829423, -0.03339124293176467, -0.07839308131185949, 0.03440199433297446, -0.09302910830899093, -0.17286635703318384, -0.0007923718305966375, 0.49053103601756065, -0.27917238243811116, -0.33614888594877956, 0.06911166871386261, -0.2649947936940742, -0.2529043858498163, 0.13790484922968685, -0.172398112536... |
1,803.05197 | The Value of Reactive Power for Voltage Control in Lossy Networks | Reactive power has been proposed as a method of voltage control for
distribution networks, providing a means of increasing the amount of energy
transferred from distributed generators to the bulk transmission network. The
value of reactive power can therefore be measured according to an increase in
transferred energy... | math.OC cs.SY | reactive power has been proposed as a method of voltage control for distribution networks providing a means of increasing the amount of energy transferred from distributed generators to the bulk transmission network the value of reactive power can therefore be measured according to an increase in transferred energy whe... | [['reactive', 'power', 'has', 'been', 'proposed', 'as', 'a', 'method', 'of', 'voltage', 'control', 'for', 'distribution', 'networks', 'providing', 'a', 'means', 'of', 'increasing', 'the', 'amount', 'of', 'energy', 'transferred', 'from', 'distributed', 'generators', 'to', 'the', 'bulk', 'transmission', 'network', 'the',... | [-0.1430111728865692, 0.05206973801726305, -0.041702160716223985, 0.03425032032716375, -0.031064702320294693, -0.12280620015763606, 0.046707013923412144, 0.3670652963233013, -0.2753087824437385, -0.3292479003146768, 0.06466072609421247, -0.2628232866947469, -0.059746127689066224, 0.24276603524758217, -0.090458483957590... |
1,803.05198 | Enhancing Favorable Propagation in Cell-Free Massive MIMO Through
Spatial User Grouping | Cell-Free (CF) Massive multiple-input multiple-output(MIMO) is a distributed
antenna system, wherein a large number of back-haul linked access points
randomly distributed over a coverage area serve simultaneously a smaller number
of users. CF Massive MIMO inherits favorable propagation of Massive MIMO
systems. Howeve... | cs.IT math.IT | cellfree cf massive multipleinput multipleoutputmimo is a distributed antenna system wherein a large number of backhaul linked access points randomly distributed over a coverage area serve simultaneously a smaller number of users cf massive mimo inherits favorable propagation of massive mimo systems however the level o... | [['cellfree', 'cf', 'massive', 'multipleinput', 'multipleoutputmimo', 'is', 'a', 'distributed', 'antenna', 'system', 'wherein', 'a', 'large', 'number', 'of', 'backhaul', 'linked', 'access', 'points', 'randomly', 'distributed', 'over', 'a', 'coverage', 'area', 'serve', 'simultaneously', 'a', 'smaller', 'number', 'of', '... | [-0.24656096925088145, 0.000608608244567529, -0.008165113779099344, 0.04733554232796025, -0.08600738497946847, -0.18966468523389526, 0.10317726764909609, 0.36867051021885366, -0.2638280763647628, -0.29181002221953173, 0.07066439980619842, -0.2008869718977964, -0.21405943788817855, 0.12569639940372693, -0.10064716514974... |
1,803.05199 | Maximal randomness expansion from steering inequality violations using
qudits | We consider the generation of randomness based upon the observed violation of
an Einstein-Podolsky-Rosen (EPR) steering inequality, known as one-sided
device-independent randomness expansion. We show that in the simplest scenario
-- involving only two parties applying two measurements with $d$ outcomes each
-- that t... | quant-ph | we consider the generation of randomness based upon the observed violation of an einsteinpodolskyrosen epr steering inequality known as onesided deviceindependent randomness expansion we show that in the simplest scenario involving only two parties applying two measurements with d outcomes each that there exist epr ste... | [['we', 'consider', 'the', 'generation', 'of', 'randomness', 'based', 'upon', 'the', 'observed', 'violation', 'of', 'an', 'einsteinpodolskyrosen', 'epr', 'steering', 'inequality', 'known', 'as', 'onesided', 'deviceindependent', 'randomness', 'expansion', 'we', 'show', 'that', 'in', 'the', 'simplest', 'scenario', 'invol... | [-0.14996829954422233, 0.17783110091804702, -0.03776205398219948, 0.08965221988764824, -0.02375954345334321, -0.26816902002707743, 0.08693068192903107, 0.2852012761635706, -0.27452235943637787, -0.25859106567222623, 0.08946919200728493, -0.28916504587590075, -0.07045439541107043, 0.19395538048508268, -0.087972770670118... |
1,803.052 | Combining Multi-level Contexts of Superpixel using Convolutional Neural
Networks to perform Natural Scene Labeling | Modern deep learning algorithms have triggered various image segmentation
approaches. However most of them deal with pixel based segmentation. However,
superpixels provide a certain degree of contextual information while reducing
computation cost. In our approach, we have performed superpixel level semantic
segmentat... | cs.CV | modern deep learning algorithms have triggered various image segmentation approaches however most of them deal with pixel based segmentation however superpixels provide a certain degree of contextual information while reducing computation cost in our approach we have performed superpixel level semantic segmentation con... | [['modern', 'deep', 'learning', 'algorithms', 'have', 'triggered', 'various', 'image', 'segmentation', 'approaches', 'however', 'most', 'of', 'them', 'deal', 'with', 'pixel', 'based', 'segmentation', 'however', 'superpixels', 'provide', 'a', 'certain', 'degree', 'of', 'contextual', 'information', 'while', 'reducing', '... | [-0.013438650066052209, -0.023592963353874757, -0.09263684446011315, 0.08978768522111871, -0.07305197548313239, -0.15454030066210123, 0.033354555749929675, 0.45392229417627006, -0.2250467338275222, -0.3920256539527567, 0.08444374875938424, -0.2766955692090632, -0.13729803970794088, 0.17972482847453086, -0.1321064142228... |
1,803.05201 | OSINT Analysis of the TOR Foundation | This research paper is a study on the TOR Foundation and the TOR Network. Due
to the blind confidence over this network and this foundation we have collect
data and gather information in open sources to understand how it is organized.
We discovered that the US government is very active through the financial
aspect an... | cs.CR | this research paper is a study on the tor foundation and the tor network due to the blind confidence over this network and this foundation we have collect data and gather information in open sources to understand how it is organized we discovered that the us government is very active through the financial aspect and de... | [['this', 'research', 'paper', 'is', 'a', 'study', 'on', 'the', 'tor', 'foundation', 'and', 'the', 'tor', 'network', 'due', 'to', 'the', 'blind', 'confidence', 'over', 'this', 'network', 'and', 'this', 'foundation', 'we', 'have', 'collect', 'data', 'and', 'gather', 'information', 'in', 'open', 'sources', 'to', 'underst... | [-0.12552975576060513, 0.03517020718261067, -0.09876476540341086, 0.07932643459034375, -0.14077370372113018, -0.16518412700610324, 0.13550525020192644, 0.37815103653286186, -0.2273837130494593, -0.33067747422804433, 0.17203870120630155, -0.306391754234764, -0.21524066154268526, 0.17917353867198385, -0.08884309655764983... |
1,803.05202 | Neutron-proton mass difference from gauge/gravity duality | Using gauge/gravity duality as a tool, we compute the strong sector, isospin
breaking induced contribution to the neutron-proton mass difference in the
Witten-Sakai-Sugimoto model of large $N$ QCD with two non-degenerate light
flavors. The mass difference, for which we provide an analytic expression,
turns out to be ... | hep-th hep-lat hep-ph | using gaugegravity duality as a tool we compute the strong sector isospin breaking induced contribution to the neutronproton mass difference in the wittensakaisugimoto model of large n qcd with two nondegenerate light flavors the mass difference for which we provide an analytic expression turns out to be positive and p... | [['using', 'gaugegravity', 'duality', 'as', 'a', 'tool', 'we', 'compute', 'the', 'strong', 'sector', 'isospin', 'breaking', 'induced', 'contribution', 'to', 'the', 'neutronproton', 'mass', 'difference', 'in', 'the', 'wittensakaisugimoto', 'model', 'of', 'large', 'n', 'qcd', 'with', 'two', 'nondegenerate', 'light', 'fla... | [-0.08658878906063881, 0.1783459335969787, -0.11929687925803116, 0.1651739900660841, -0.10084946491615543, -0.08334664604588551, 0.07215090700443469, 0.3254654536668966, -0.17649375702394476, -0.28888252641689155, -0.0038551963756189626, -0.3244560088603179, -0.050556475005958695, 0.08161989007954748, 0.052028900278683... |
1,803.05203 | The propagating speed of relic gravitational waves and their refractive
index during inflation | If the refractive index of the tensor modes increases during a conventional
inflationary stage of expansion the relic graviton spectrum is tilted towards
high frequencies. Two apparently diverse parametrizations of this effect are
shown to be related by a rescaling of the four-dimensional metric through a
conformal f... | gr-qc astro-ph.CO hep-ph hep-th | if the refractive index of the tensor modes increases during a conventional inflationary stage of expansion the relic graviton spectrum is tilted towards high frequencies two apparently diverse parametrizations of this effect are shown to be related by a rescaling of the fourdimensional metric through a conformal facto... | [['if', 'the', 'refractive', 'index', 'of', 'the', 'tensor', 'modes', 'increases', 'during', 'a', 'conventional', 'inflationary', 'stage', 'of', 'expansion', 'the', 'relic', 'graviton', 'spectrum', 'is', 'tilted', 'towards', 'high', 'frequencies', 'two', 'apparently', 'diverse', 'parametrizations', 'of', 'this', 'effec... | [-0.11273281278749732, 0.1790114896367076, -0.05860968266281631, 0.04325134442611174, -0.10147561442263268, -0.09973299921119025, 0.02688565186934767, 0.3670078255236149, -0.21409834710672707, -0.31843912734330954, 0.10168063977303413, -0.272231922953852, -0.13913100212201854, 0.2047576427775585, -0.004116703671246211,... |
1,803.05204 | Some remarks on Yamabe solitons | In this paper we have obtained evolution of some geometric quantities on a
compact Riemannian manifold $M^n$ when the metric is a Yamabe soliton. Using
these quantities we have obtained bound on the soliton constant. We have proved
that the commutator of two soliton vector fields with the same metric in a
given confo... | math.DG | in this paper we have obtained evolution of some geometric quantities on a compact riemannian manifold mn when the metric is a yamabe soliton using these quantities we have obtained bound on the soliton constant we have proved that the commutator of two soliton vector fields with the same metric in a given conformal cl... | [['in', 'this', 'paper', 'we', 'have', 'obtained', 'evolution', 'of', 'some', 'geometric', 'quantities', 'on', 'a', 'compact', 'riemannian', 'manifold', 'mn', 'when', 'the', 'metric', 'is', 'a', 'yamabe', 'soliton', 'using', 'these', 'quantities', 'we', 'have', 'obtained', 'bound', 'on', 'the', 'soliton', 'constant', '... | [-0.2115580026889109, 0.15425903993725246, -0.09925566079272401, 0.06141128804856202, -0.1395580496284224, -0.1396423053894458, -0.0676420995885218, 0.4231634360871145, -0.23245589807075226, -0.18141720244394882, 0.12032598788937321, -0.2682991407456852, -0.18341189064639843, 0.1824938454498936, -0.03673600060643539, 0... |
1,803.05205 | The complete enumeration of 4-polytopes and 3-spheres with nine vertices | We describe an algorithm to enumerate polytopes. This algorithm is then
implemented to give a complete classification of combinatorial spheres of
dimension 3 with 9 vertices and decide polytopality of those spheres. In
particular, we completely enumerate all combinatorial types of 4-dimensional
polytopes with 9 verti... | math.MG math.CO | we describe an algorithm to enumerate polytopes this algorithm is then implemented to give a complete classification of combinatorial spheres of dimension 3 with 9 vertices and decide polytopality of those spheres in particular we completely enumerate all combinatorial types of 4dimensional polytopes with 9 vertices it... | [['we', 'describe', 'an', 'algorithm', 'to', 'enumerate', 'polytopes', 'this', 'algorithm', 'is', 'then', 'implemented', 'to', 'give', 'a', 'complete', 'classification', 'of', 'combinatorial', 'spheres', 'of', 'dimension', '3', 'with', '9', 'vertices', 'and', 'decide', 'polytopality', 'of', 'those', 'spheres', 'in', 'p... | [-0.12369912356174854, 0.10406248534789565, -0.054560055225051605, 0.04784128680600251, -0.11370409391506502, -0.1722384017232931, -0.013557563446922584, 0.39739313960242806, -0.2934252492811405, -0.3167852819949556, 0.11499196752837827, -0.294560442982095, -0.19508265650548626, 0.1371040732777688, -0.1450914360917686,... |
1,803.05206 | Learning Latent Superstructures in Variational Autoencoders for Deep
Multidimensional Clustering | We investigate a variant of variational autoencoders where there is a
superstructure of discrete latent variables on top of the latent features. In
general, our superstructure is a tree structure of multiple super latent
variables and it is automatically learned from data. When there is only one
latent variable in th... | cs.LG | we investigate a variant of variational autoencoders where there is a superstructure of discrete latent variables on top of the latent features in general our superstructure is a tree structure of multiple super latent variables and it is automatically learned from data when there is only one latent variable in the sup... | [['we', 'investigate', 'a', 'variant', 'of', 'variational', 'autoencoders', 'where', 'there', 'is', 'a', 'superstructure', 'of', 'discrete', 'latent', 'variables', 'on', 'top', 'of', 'the', 'latent', 'features', 'in', 'general', 'our', 'superstructure', 'is', 'a', 'tree', 'structure', 'of', 'multiple', 'super', 'latent... | [-0.0364673998768604, 0.11593390977756667, -0.11287936320461865, 0.10072703316940793, -0.15719074494619337, -0.1732515277865801, 0.06182907691358456, 0.4105106867731564, -0.3618034493503353, -0.2932118955585692, 0.0771880728305347, -0.27800531405955553, -0.16634692372162901, 0.12013519358163374, -0.06942268910389097, 0... |
1,803.05207 | Sparse Fast DCT for Vectors with One-block Support | In this paper we present a new fast and deterministic algorithm for the
inverse discrete cosine transform of type II that reconstructs the input vector
$\mathbf{x}\in\mathbb{R}^{N}$, $N=2^{J-1}$, with short support of length $m$
from its discrete cosine transform
$\mathbf{x}^{\widehat{\mathrm{II}}}=\mathbf{C}_N^{\mat... | math.NA | in this paper we present a new fast and deterministic algorithm for the inverse discrete cosine transform of type ii that reconstructs the input vector mathbfxinmathbbrn n2j1 with short support of length m from its discrete cosine transform mathbfxwidehatmathrmiimathbfc_nmathrmiimathbfx the resulting algorithm has a ru... | [['in', 'this', 'paper', 'we', 'present', 'a', 'new', 'fast', 'and', 'deterministic', 'algorithm', 'for', 'the', 'inverse', 'discrete', 'cosine', 'transform', 'of', 'type', 'ii', 'that', 'reconstructs', 'the', 'input', 'vector', 'mathbfxinmathbbrn', 'n2j1', 'with', 'short', 'support', 'of', 'length', 'm', 'from', 'its'... | [-0.0757704574574271, 0.07524485887109261, -0.10445164350549811, 0.041203235992250724, -0.11566507945130781, -0.17071986990049481, 0.07512392438619155, 0.4198393149544363, -0.33258677757618466, -0.28571184311548004, 0.12347227148458605, -0.18194878907145365, -0.20022097033569994, 0.18442452576203758, -0.058196617573823... |
1,803.05208 | One-half of the Kibble-Zurek quench followed by free evolution | We drive the one-dimensional quantum Ising chain in the transverse field from
the paramagnetic phase to the critical point and study its free evolution
there. We analyze excitation of such a system at the critical point and
dynamics of its transverse magnetization and Loschmidt echo during free
evolution. We discuss ... | quant-ph cond-mat.quant-gas cond-mat.stat-mech | we drive the onedimensional quantum ising chain in the transverse field from the paramagnetic phase to the critical point and study its free evolution there we analyze excitation of such a system at the critical point and dynamics of its transverse magnetization and loschmidt echo during free evolution we discuss how t... | [['we', 'drive', 'the', 'onedimensional', 'quantum', 'ising', 'chain', 'in', 'the', 'transverse', 'field', 'from', 'the', 'paramagnetic', 'phase', 'to', 'the', 'critical', 'point', 'and', 'study', 'its', 'free', 'evolution', 'there', 'we', 'analyze', 'excitation', 'of', 'such', 'a', 'system', 'at', 'the', 'critical', '... | [-0.18723525655679876, 0.25321885777189385, -0.11020266758042234, 0.08072369029344637, 0.040054392187467106, -0.11029005673702193, 0.05236529750613896, 0.36476993420503184, -0.3024601230421398, -0.20817422257335502, 0.078614405665806, -0.28095672870219884, -0.13665680877298494, 0.16885476810503988, 0.07865325360900804,... |
1,803.05209 | Building Sparse Deep Feedforward Networks using Tree Receptive Fields | Sparse connectivity is an important factor behind the success of
convolutional neural networks and recurrent neural networks. In this paper, we
consider the problem of learning sparse connectivity for feedforward neural
networks (FNNs). The key idea is that a unit should be connected to a small
number of units at the... | cs.LG | sparse connectivity is an important factor behind the success of convolutional neural networks and recurrent neural networks in this paper we consider the problem of learning sparse connectivity for feedforward neural networks fnns the key idea is that a unit should be connected to a small number of units at the next l... | [['sparse', 'connectivity', 'is', 'an', 'important', 'factor', 'behind', 'the', 'success', 'of', 'convolutional', 'neural', 'networks', 'and', 'recurrent', 'neural', 'networks', 'in', 'this', 'paper', 'we', 'consider', 'the', 'problem', 'of', 'learning', 'sparse', 'connectivity', 'for', 'feedforward', 'neural', 'networ... | [-0.08199009707374177, 0.09630669110769743, 0.006373839684087655, 0.07180858928758393, -0.08563925391063094, -0.16184642632202856, 0.04071558080051608, 0.4648356455924182, -0.3227069798985432, -0.27557646742026354, 0.0676605263074603, -0.25889549951615004, -0.24900942667676457, 0.1913834565110376, -0.09889776172309087,... |
1,803.0521 | LivDet 2017 Fingerprint Liveness Detection Competition 2017 | Fingerprint Presentation Attack Detection (FPAD) deals with distinguishing
images coming from artificial replicas of the fingerprint characteristic, made
up of materials like silicone, gelatine or latex, and images coming from alive
fingerprints. Images are captured by modern scanners, typically relying on
solid-stat... | cs.CV | fingerprint presentation attack detection fpad deals with distinguishing images coming from artificial replicas of the fingerprint characteristic made up of materials like silicone gelatine or latex and images coming from alive fingerprints images are captured by modern scanners typically relying on solidstate or optic... | [['fingerprint', 'presentation', 'attack', 'detection', 'fpad', 'deals', 'with', 'distinguishing', 'images', 'coming', 'from', 'artificial', 'replicas', 'of', 'the', 'fingerprint', 'characteristic', 'made', 'up', 'of', 'materials', 'like', 'silicone', 'gelatine', 'or', 'latex', 'and', 'images', 'coming', 'from', 'alive... | [-0.08890583915144816, 0.0865276184733375, -0.0546942609391408, 0.013716728143481304, -0.06609444973582868, -0.15398349833412794, 0.056970180239295586, 0.3549644664861262, -0.22884608395397663, -0.3574390173656866, 0.13028603443381143, -0.33296524367760866, -0.12035503588267601, 0.21214639363879542, -0.0956330109678674... |
1,803.05211 | Renormalized solutions to a chemotaxis system with consumption of
chemoattractant | This paper investigates a high-dimensional chemotaxis system with consumption
of chemoattractant \begin{eqnarray*} \left\{\begin{array}{l} u_t=\Delta
u-\nabla\cdot(u\nabla v), v_t=\Delta v-uv, \end{array}\right. \end{eqnarray*}
under homogeneous boundary conditions of Neumann type, in a bounded convex
domain $\Omega\... | math.AP | this paper investigates a highdimensional chemotaxis system with consumption of chemoattractant begineqnarray leftbeginarrayl u_tdelta unablacdotunabla v v_tdelta vuv endarrayright endeqnarray under homogeneous boundary conditions of neumann type in a bounded convex domain omegasubsetmathbbrnngeq4 with smooth boundary ... | [['this', 'paper', 'investigates', 'a', 'highdimensional', 'chemotaxis', 'system', 'with', 'consumption', 'of', 'chemoattractant', 'begineqnarray', 'leftbeginarrayl', 'u_tdelta', 'unablacdotunabla', 'v', 'v_tdelta', 'vuv', 'endarrayright', 'endeqnarray', 'under', 'homogeneous', 'boundary', 'conditions', 'of', 'neumann'... | [-0.19792887587100266, 0.05627506747841835, -0.018187572395739458, -0.054494501231238245, -0.08017205744157158, -0.2901645580849921, -0.09426965831274477, 0.32331081681186336, -0.3208531470814099, -0.08398670832781742, 0.1958031895085393, -0.36637626379573096, -0.04370418066779772, 0.15284881232849631, -0.1517683271163... |
1,803.05212 | Maximum principle satisfying CWENO schemes for non-local conservation
laws | Central WENO schemes are a natural candidate for higher-order schemes for
non-local conservation laws, since the underlying reconstructions do not only
provide single point values of the solution but a complete (high-order)
reconstruction in every time step, which is beneficial to evaluate the integral
terms. Recentl... | math.NA | central weno schemes are a natural candidate for higherorder schemes for nonlocal conservation laws since the underlying reconstructions do not only provide single point values of the solution but a complete highorder reconstruction in every time step which is beneficial to evaluate the integral terms recently in c cha... | [['central', 'weno', 'schemes', 'are', 'a', 'natural', 'candidate', 'for', 'higherorder', 'schemes', 'for', 'nonlocal', 'conservation', 'laws', 'since', 'the', 'underlying', 'reconstructions', 'do', 'not', 'only', 'provide', 'single', 'point', 'values', 'of', 'the', 'solution', 'but', 'a', 'complete', 'highorder', 'rec... | [-0.09240023005501523, -0.003760701629794817, -0.09071271654748772, 0.016609182734100614, -0.10425403410853404, -0.18993089609042121, 0.0580123065770345, 0.3346370122680027, -0.22460793668869883, -0.3167164559320857, 0.07476721579749007, -0.17381050486841965, -0.07560536261674618, 0.1920101965507557, -0.144382720166403... |
1,803.05213 | Global generalized solutions to a nonlinear Keller-Segel equation with
singular sensitivity | We consider the chemotaxis system \begin{eqnarray*} \begin{cases}
\begin{array}{lll} \medskip u_t =\Delta u^m - \nabla(\frac{u}{v}\nabla v),&{}
x\in\Omega,\ t>0, \medskip v_t =\Delta v -uv,&{}x\in\Omega,\ t>0, \medskip
\frac{\partial u}{\partial \nu}=\frac{\partial
v}{\partial\nu}=0,&{}x\in\partial\Omega,\ t>0, \meds... | math.AP | we consider the chemotaxis system begineqnarray begincases beginarraylll medskip u_t delta um nablafracuvnabla v xinomega t0 medskip v_t delta v uvxinomega t0 medskip fracpartial upartial nufracpartial vpartialnu0xinpartialomega t0 medskip ux0u_0x vx0v_0x xinomega endarray endcases endeqnarray in a smooth bounded domai... | [['we', 'consider', 'the', 'chemotaxis', 'system', 'begineqnarray', 'begincases', 'beginarraylll', 'medskip', 'u_t', 'delta', 'um', 'nablafracuvnabla', 'v', 'xinomega', 't0', 'medskip', 'v_t', 'delta', 'v', 'uvxinomega', 't0', 'medskip', 'fracpartial', 'upartial', 'nufracpartial', 'vpartialnu0xinpartialomega', 't0', 'm... | [-0.23507740567067126, 0.002559043661070367, 0.06096009217688571, -0.06919124574683931, -0.08782096093383861, -0.3406892911247585, -0.1277144347820296, 0.3196530580702845, -0.35248221498171706, 0.02462987947291222, 0.20219139118705862, -0.5397607263960484, -0.016022165887989104, 0.09747388543210168, -0.1066854514883480... |
1,803.05214 | Exceptional Points in an Specialty Microcavity: Interplay between
State-Conversion and Cavity Control Parameters | Exploiting scattering-matrix in a gain-loss assisted optical-microcavity,
interplay between asymmetric-state-conversion and cavity-control parameters
around exceptional points is analyzed; where occupying a least area by coupled
states during switching, maximum conversion-efficiency with minimal asymmetry
is achieved... | physics.optics | exploiting scatteringmatrix in a gainloss assisted opticalmicrocavity interplay between asymmetricstateconversion and cavitycontrol parameters around exceptional points is analyzed where occupying a least area by coupled states during switching maximum conversionefficiency with minimal asymmetry is achieved | [['exploiting', 'scatteringmatrix', 'in', 'a', 'gainloss', 'assisted', 'opticalmicrocavity', 'interplay', 'between', 'asymmetricstateconversion', 'and', 'cavitycontrol', 'parameters', 'around', 'exceptional', 'points', 'is', 'analyzed', 'where', 'occupying', 'a', 'least', 'area', 'by', 'coupled', 'states', 'during', 's... | [-0.2352055958181154, 0.198015034198761, -0.03299680896452628, -0.01966566473856801, -0.013210902850914863, -0.22890067633125, 0.12675640842644498, 0.35374490030517336, -0.22566369420383126, -0.35135413508396596, 0.061924981429910986, -0.31502564216498286, -0.1380717804422602, 0.14841516234446317, -0.020873678411589935... |
1,803.05215 | Deep Image Demosaicking using a Cascade of Convolutional Residual
Denoising Networks | Demosaicking and denoising are among the most crucial steps of modern digital
camera pipelines and their joint treatment is a highly ill-posed inverse
problem where at-least two-thirds of the information are missing and the rest
are corrupted by noise. This poses a great challenge in obtaining meaningful
reconstructi... | cs.CV | demosaicking and denoising are among the most crucial steps of modern digital camera pipelines and their joint treatment is a highly illposed inverse problem where atleast twothirds of the information are missing and the rest are corrupted by noise this poses a great challenge in obtaining meaningful reconstructions an... | [['demosaicking', 'and', 'denoising', 'are', 'among', 'the', 'most', 'crucial', 'steps', 'of', 'modern', 'digital', 'camera', 'pipelines', 'and', 'their', 'joint', 'treatment', 'is', 'a', 'highly', 'illposed', 'inverse', 'problem', 'where', 'atleast', 'twothirds', 'of', 'the', 'information', 'are', 'missing', 'and', 't... | [-0.049514686792723035, -0.029774632100586076, -0.05450269855958011, 0.053935235997600174, -0.12308486653800711, -0.18378382825948375, 0.008621887455941463, 0.4485092716557639, -0.24258608750364036, -0.346258174404692, 0.10193110658307275, -0.2579546489153528, -0.22107673040531783, 0.21764717660357283, -0.1595314223906... |
1,803.05216 | Metric-space approach for distinguishing quantum phase transitions in
spin-imbalanced systems | Metric spaces are characterized by distances between pairs of elements.
Systems that are physically similar are expected to present smaller distances
(between their densities, wave functions and potentials) than systems that
present different physical behaviors. For this reason metric spaces are good
candidates for p... | quant-ph cond-mat.supr-con | metric spaces are characterized by distances between pairs of elements systems that are physically similar are expected to present smaller distances between their densities wave functions and potentials than systems that present different physical behaviors for this reason metric spaces are good candidates for probing ... | [['metric', 'spaces', 'are', 'characterized', 'by', 'distances', 'between', 'pairs', 'of', 'elements', 'systems', 'that', 'are', 'physically', 'similar', 'are', 'expected', 'to', 'present', 'smaller', 'distances', 'between', 'their', 'densities', 'wave', 'functions', 'and', 'potentials', 'than', 'systems', 'that', 'pre... | [-0.19447419887224027, 0.20204307735004295, -0.09958609954563079, 0.08912433267084395, -0.007321021641260601, -0.14385976929318262, 0.06042271685945961, 0.3915244586228787, -0.2285202646311813, -0.28125698070869326, 0.04548173560551158, -0.2915502241896549, -0.14985902583948127, 0.14459514320693775, 0.02629003394755633... |
1,803.05217 | Vapor-liquid equilibrium and equation of state of two-dimensional fluids
from a discrete perturbation theory | The interest in the description of the properties of fluids of restricted
dimensionality is growing for theoretical and practical reasons. In this work,
we have firstly developed an analytical expression for the Helmholtz free
energy of the two-dimensional square-well fluid in the Barker--Henderson
framework. This eq... | physics.chem-ph cond-mat.soft | the interest in the description of the properties of fluids of restricted dimensionality is growing for theoretical and practical reasons in this work we have firstly developed an analytical expression for the helmholtz free energy of the twodimensional squarewell fluid in the barkerhenderson framework this equation of... | [['the', 'interest', 'in', 'the', 'description', 'of', 'the', 'properties', 'of', 'fluids', 'of', 'restricted', 'dimensionality', 'is', 'growing', 'for', 'theoretical', 'and', 'practical', 'reasons', 'in', 'this', 'work', 'we', 'have', 'firstly', 'developed', 'an', 'analytical', 'expression', 'for', 'the', 'helmholtz',... | [-0.0804882962133043, 0.054788586302645985, -0.10038492559667561, 0.035025549518867535, -0.032825529422874734, -0.17001887911155952, -0.03216220522237596, 0.3307874945455449, -0.19910124280547672, -0.26861417349592775, 0.048177823048307505, -0.2815989335644496, -0.13044843074362888, 0.1956617598740211, -0.0104211994191... |
1,803.05218 | Crystallization of hard spheres revisited. I. Extracting kinetics and
free energy landscape from forward flux sampling | We investigate the kinetics and the free energy landscape of the
crystallization of hard spheres from a supersaturated metastable liquid though
direct simulations and forward flux sampling. In this first paper, we describe
and test two different ways to reconstruct the free energy barriers from the
sampled steady sta... | cond-mat.soft cond-mat.stat-mech | we investigate the kinetics and the free energy landscape of the crystallization of hard spheres from a supersaturated metastable liquid though direct simulations and forward flux sampling in this first paper we describe and test two different ways to reconstruct the free energy barriers from the sampled steady state p... | [['we', 'investigate', 'the', 'kinetics', 'and', 'the', 'free', 'energy', 'landscape', 'of', 'the', 'crystallization', 'of', 'hard', 'spheres', 'from', 'a', 'supersaturated', 'metastable', 'liquid', 'though', 'direct', 'simulations', 'and', 'forward', 'flux', 'sampling', 'in', 'this', 'first', 'paper', 'we', 'describe'... | [-0.03349221107489664, 0.15416828458860732, -0.13591065010551712, 0.09859355880791763, 0.004737330185209247, -0.10594008783240327, 0.0782032874787625, 0.37391645904201615, -0.2717799679208681, -0.3338422326960688, 0.05500691731229237, -0.23786455207913043, -0.06825330393161062, 0.16702751484749798, -0.00030886622065370... |
1,803.05219 | Global existence and boundedness of weak solutions to a
chemotaxis-stokes system with rotational flux term | In this paper, the three-dimensional chemotaxis-stokes system
\begin{eqnarray*} \left\{\begin{array}{lll} \medskip n_{t}+u\cdot\nabla
n=\Delta n^m-\nabla\cdot(n S(x,n,c)\cdot\nabla c),&x\in\Omega,\ \ t>0, \medskip
c_t+u\cdot\nabla c=\Delta c-nf(c),&x\in\Omega,\ \ t>0, \medskip u_t+\nabla
P=\Delta u +n\nabla\phi,&x\in... | math.AP | in this paper the threedimensional chemotaxisstokes system begineqnarray leftbeginarraylll medskip n_tucdotnabla ndelta nmnablacdotn sxnccdotnabla cxinomega t0 medskip c_tucdotnabla cdelta cnfcxinomega t0 medskip u_tnabla pdelta u nnablaphixinomega t0 nablacdot u0 xinomega t0 endarrayright endeqnarray posed in a bounde... | [['in', 'this', 'paper', 'the', 'threedimensional', 'chemotaxisstokes', 'system', 'begineqnarray', 'leftbeginarraylll', 'medskip', 'n_tucdotnabla', 'ndelta', 'nmnablacdotn', 'sxnccdotnabla', 'cxinomega', 't0', 'medskip', 'c_tucdotnabla', 'cdelta', 'cnfcxinomega', 't0', 'medskip', 'u_tnabla', 'pdelta', 'u', 'nnablaphixi... | [-0.231605215343948, 0.08067181765777516, 0.01673457786234269, -0.031768937031373234, -0.03414007578919386, -0.26623674056164043, -0.08303808745147441, 0.31921801671120975, -0.31152515715517687, -0.03696749289063554, 0.18010207836735337, -0.4009279567638741, -0.04764981384106053, 0.10219502042723345, -0.079036412094080... |
1,803.0522 | All-Lossy Quasi-Guided Dual-Mode Optical Waveguide Exhibiting
Exceptional Singularities | We explore exceptional points (EP) in a dual-mode symmetric planar optical
waveguide with transverse variation of inhomogeneous loss profile; where modal
evolution alongside an EP is reported in the context of selective optical mode
conversion.
| physics.optics | we explore exceptional points ep in a dualmode symmetric planar optical waveguide with transverse variation of inhomogeneous loss profile where modal evolution alongside an ep is reported in the context of selective optical mode conversion | [['we', 'explore', 'exceptional', 'points', 'ep', 'in', 'a', 'dualmode', 'symmetric', 'planar', 'optical', 'waveguide', 'with', 'transverse', 'variation', 'of', 'inhomogeneous', 'loss', 'profile', 'where', 'modal', 'evolution', 'alongside', 'an', 'ep', 'is', 'reported', 'in', 'the', 'context', 'of', 'selective', 'optic... | [-0.14874264651111194, 0.1199779737379036, -0.028921644176755634, -0.012135374236718885, -0.08293148283181447, -0.12112771255363311, 0.015923263199095216, 0.5072842980069774, -0.24409538049783025, -0.2055328176489898, 0.0412718232255429, -0.26365277765850936, -0.1323826179781463, 0.1362852339765855, 0.00756165324045079... |
1,803.05221 | Direct numerical computation and its application to the higher-order
radiative corrections | The direct computation method(DCM) is developed to calculate the multi-loop
amplitude for general masses and external momenta. The ultraviolet divergence
is under control in dimensional regularization. In this paper we report on the
progress of DCM to several scalar multi-loop integrals after the presentation
in ACAT... | hep-ph | the direct computation methoddcm is developed to calculate the multiloop amplitude for general masses and external momenta the ultraviolet divergence is under control in dimensional regularization in this paper we report on the progress of dcm to several scalar multiloop integrals after the presentation in acat2016 als... | [['the', 'direct', 'computation', 'methoddcm', 'is', 'developed', 'to', 'calculate', 'the', 'multiloop', 'amplitude', 'for', 'general', 'masses', 'and', 'external', 'momenta', 'the', 'ultraviolet', 'divergence', 'is', 'under', 'control', 'in', 'dimensional', 'regularization', 'in', 'this', 'paper', 'we', 'report', 'on'... | [-0.13921989390596015, 0.11299702512924789, -0.07268336911487286, 0.061222094405045516, -0.09461779428310081, -0.04865631097775014, 0.03814855230338566, 0.38371646814964344, -0.1977375352175021, -0.26070662190923927, 0.10763867208772324, -0.2258727924638718, -0.17170580975772415, 0.22787249011949437, -0.057584101707792... |
1,803.05222 | ALMA observations of the nearby AGB star L$_{\rm 2}$ Puppis. II. Gas
disk properties derived from $^{\rm 12}$CO and $^{\rm13}$CO $J=$3$-$2
emission | The circumstellar environment of the AGB star L$_{\rm 2}$ Puppis was observed
with ALMA in cycle 3, with a resolution of $15 \times 18 \rm\ mas$. The
molecular emission shows a differentially rotating disk, inclined to a nearly
edge-on position. In the first paper in this series (paper I) the molecular
emission was a... | astro-ph.SR | the circumstellar environment of the agb star l_rm 2 puppis was observed with alma in cycle 3 with a resolution of 15 times 18 rm mas the molecular emission shows a differentially rotating disk inclined to a nearly edgeon position in the first paper in this series paper i the molecular emission was analysed to accurate... | [['the', 'circumstellar', 'environment', 'of', 'the', 'agb', 'star', 'l_rm', '2', 'puppis', 'was', 'observed', 'with', 'alma', 'in', 'cycle', '3', 'with', 'a', 'resolution', 'of', '15', 'times', '18', 'rm', 'mas', 'the', 'molecular', 'emission', 'shows', 'a', 'differentially', 'rotating', 'disk', 'inclined', 'to', 'a',... | [-0.09466778266692667, 0.0639125344953278, -0.007641037997035753, 0.035616455172255104, -0.041739405990145834, -0.03728216281160712, -0.003385135968814471, 0.4213811387086198, -0.2118718255843435, -0.31435245243455506, 0.06753485084752486, -0.23691929514032034, -0.009113561993165474, 0.1363184278908496, -0.012581791117... |
1,803.05223 | MCScript: A Novel Dataset for Assessing Machine Comprehension Using
Script Knowledge | We introduce a large dataset of narrative texts and questions about these
texts, intended to be used in a machine comprehension task that requires
reasoning using commonsense knowledge. Our dataset complements similar datasets
in that we focus on stories about everyday activities, such as going to the
movies or worki... | cs.CL | we introduce a large dataset of narrative texts and questions about these texts intended to be used in a machine comprehension task that requires reasoning using commonsense knowledge our dataset complements similar datasets in that we focus on stories about everyday activities such as going to the movies or working in... | [['we', 'introduce', 'a', 'large', 'dataset', 'of', 'narrative', 'texts', 'and', 'questions', 'about', 'these', 'texts', 'intended', 'to', 'be', 'used', 'in', 'a', 'machine', 'comprehension', 'task', 'that', 'requires', 'reasoning', 'using', 'commonsense', 'knowledge', 'our', 'dataset', 'complements', 'similar', 'datas... | [-0.032153387385834425, 0.002441875549017364, -0.05739127601293895, 0.11922322385984226, -0.2070069103820138, -0.10147119156666036, 0.08604907216583817, 0.40208663813706136, -0.22966881275861564, -0.41264310584236413, 0.07907234763519631, -0.29013480317110246, -0.13427993540978458, 0.22971419582907587, -0.1481741316632... |
1,803.05224 | Excitonic Order and Superconductivity in the Two-Orbital Hubbard Model:
Variational Cluster Approach | Using the variational cluster approach based on the self-energy functional
theory, we study the possible occurrence of excitonic order and
superconductivity in the two-orbital Hubbard model with intra- and
inter-orbital Coulomb interactions. It is known that an antiferromagnetic Mott
insulator state appears in the re... | cond-mat.str-el cond-mat.supr-con | using the variational cluster approach based on the selfenergy functional theory we study the possible occurrence of excitonic order and superconductivity in the twoorbital hubbard model with intra and interorbital coulomb interactions it is known that an antiferromagnetic mott insulator state appears in the regime of ... | [['using', 'the', 'variational', 'cluster', 'approach', 'based', 'on', 'the', 'selfenergy', 'functional', 'theory', 'we', 'study', 'the', 'possible', 'occurrence', 'of', 'excitonic', 'order', 'and', 'superconductivity', 'in', 'the', 'twoorbital', 'hubbard', 'model', 'with', 'intra', 'and', 'interorbital', 'coulomb', 'i... | [-0.20401278141189397, 0.1833565872405349, -0.03902961762586033, 0.11116854523637945, -0.022098717423595066, -0.14935988073078235, 0.12501671514568502, 0.3811340544191075, -0.25132837871513597, -0.2523960479747171, -0.05197874192863975, -0.34714508488229134, -0.13722533186731056, 0.06594391830447244, 0.0939978279430813... |
1,803.05225 | Site-selective measurement of coupled spin pairs in an organic
semiconductor | From organic electronics to biological systems, understanding the role of
intermolecular interactions between spin pairs is a key challenge. Here we show
how such pairs can be selectively addressed with combined spin and optical
sensitivity. We demonstrate this for bound pairs of spin-triplet excitations
formed by si... | physics.chem-ph cond-mat.mtrl-sci | from organic electronics to biological systems understanding the role of intermolecular interactions between spin pairs is a key challenge here we show how such pairs can be selectively addressed with combined spin and optical sensitivity we demonstrate this for bound pairs of spintriplet excitations formed by singlet ... | [['from', 'organic', 'electronics', 'to', 'biological', 'systems', 'understanding', 'the', 'role', 'of', 'intermolecular', 'interactions', 'between', 'spin', 'pairs', 'is', 'a', 'key', 'challenge', 'here', 'we', 'show', 'how', 'such', 'pairs', 'can', 'be', 'selectively', 'addressed', 'with', 'combined', 'spin', 'and', ... | [-0.15083823432965623, 0.20056633165851612, 0.007613594977620749, 0.04996333221018675, -0.022968779254381757, -0.1534273632711941, 0.03099212944507599, 0.45048572858495095, -0.26438685298086173, -0.35092874420506337, -0.04494863301590686, -0.29265748758569377, -0.07038861487301126, 0.1957697092315122, 0.079117780124708... |
1,803.05226 | Uniform preconditioners for problems of negative order | Uniform preconditioners for operators of negative order discretized by
(dis)continuous piecewise polynomials of any order are constructed from a
boundedly invertible operator of opposite order discretized by continuous
piecewise linears. Besides the cost of the application of the latter
discretized operator, the othe... | math.NA | uniform preconditioners for operators of negative order discretized by discontinuous piecewise polynomials of any order are constructed from a boundedly invertible operator of opposite order discretized by continuous piecewise linears besides the cost of the application of the latter discretized operator the other cost... | [['uniform', 'preconditioners', 'for', 'operators', 'of', 'negative', 'order', 'discretized', 'by', 'discontinuous', 'piecewise', 'polynomials', 'of', 'any', 'order', 'are', 'constructed', 'from', 'a', 'boundedly', 'invertible', 'operator', 'of', 'opposite', 'order', 'discretized', 'by', 'continuous', 'piecewise', 'lin... | [-0.10223435567691923, 0.10453157363459468, -0.05787833978887647, -0.0037130455719307067, -0.10842254095477984, -0.1600266655255109, 0.011562552601099015, 0.3889833787549287, -0.31508053531870245, -0.23451247070683168, 0.14393668277654798, -0.23039064694661648, -0.1066968347877264, 0.13565210306085645, -0.0881851030886... |
1,803.05227 | Lecture notes on the co-representation theory of the compact quantum
group $SU_{q}(2).$ | This is an exposition of S.L Woronowicz co-representation theory of the
compact quantum group $SU_{q}(2)$ written for a seminar series.
| math.QA math-ph math.FA math.MP | this is an exposition of sl woronowicz corepresentation theory of the compact quantum group su_q2 written for a seminar series | [['this', 'is', 'an', 'exposition', 'of', 'sl', 'woronowicz', 'corepresentation', 'theory', 'of', 'the', 'compact', 'quantum', 'group', 'su_q2', 'written', 'for', 'a', 'seminar', 'series']] | [-0.20617261377628893, 0.07790499362236006, -0.2246338665485382, 0.044360329024493696, -0.1404475617222488, -0.07410366598051041, -0.058046483475482094, 0.2816623986698687, -0.30008254759013653, -0.18547014938667417, 0.12448092284612358, -0.2602404085919261, -0.1798853874206543, 0.24316369509324431, -0.1647181836422532... |
1,803.05228 | Ultra High Molecular Weight Polyethylene: optical features at millimeter
wavelengths | The next generation of experiments for the measurement of the Cosmic
Microwave Background (CMB) requires more and more the use of advanced
materials, with specific physical and structural properties. An example is the
material used for receiver's cryostat windows and internal lenses. The large
throughput of current C... | astro-ph.IM astro-ph.CO physics.ins-det | the next generation of experiments for the measurement of the cosmic microwave background cmb requires more and more the use of advanced materials with specific physical and structural properties an example is the material used for receivers cryostat windows and internal lenses the large throughput of current cmb exper... | [['the', 'next', 'generation', 'of', 'experiments', 'for', 'the', 'measurement', 'of', 'the', 'cosmic', 'microwave', 'background', 'cmb', 'requires', 'more', 'and', 'more', 'the', 'use', 'of', 'advanced', 'materials', 'with', 'specific', 'physical', 'and', 'structural', 'properties', 'an', 'example', 'is', 'the', 'mate... | [-0.10278785279682041, 0.12751640339368916, -0.03477736862470814, -0.007802022965220006, -0.06846099140365487, -0.09467871191546968, 0.021959224136283054, 0.41412024702066963, -0.23564674906378638, -0.3362302472072559, 0.10157400450291301, -0.2994436847326089, -0.09437536996573317, 0.24932673161147514, -0.0038705957931... |
1,803.05229 | Twinning to slip transition in ultrathin BCC Fe nanowires | We report twinning to slip transition with decreasing size and increasing
temperature in ultrathin $<$100$>$ BCC Fe nanowires. Molecular dynamics
simulations have been performed on different nanowire size in the range
0.404-3.634 nm at temperatures ranging from 10 to 900 K. The results indicate
that slip mode dominat... | cond-mat.mtrl-sci | we report twinning to slip transition with decreasing size and increasing temperature in ultrathin 100 bcc fe nanowires molecular dynamics simulations have been performed on different nanowire size in the range 04043634 nm at temperatures ranging from 10 to 900 k the results indicate that slip mode dominates at low siz... | [['we', 'report', 'twinning', 'to', 'slip', 'transition', 'with', 'decreasing', 'size', 'and', 'increasing', 'temperature', 'in', 'ultrathin', '100', 'bcc', 'fe', 'nanowires', 'molecular', 'dynamics', 'simulations', 'have', 'been', 'performed', 'on', 'different', 'nanowire', 'size', 'in', 'the', 'range', '04043634', 'n... | [-0.11265045482529483, 0.29735353266490466, -0.0026177840676003448, -0.08065106723976594, 0.007165837518793221, -0.14669087477765666, 0.03266727319957378, 0.4581921808858169, -0.2571400276501663, -0.3413546366306643, 0.06732689028164411, -0.30367665517648373, -0.014302240694329763, 0.1564144325190379, 0.048042446588321... |
1,803.0523 | Simplified models of circumstellar morphologies for interpreting
high-resolution data. Analytical approach to the equatorial density
enhancement | Equatorial density enhancements (EDEs) are a very common astronomical
phenomenon. Studies of the circumstellar environments (CSE) of young stellar
objects and of evolved stars have shown that these objects often possess these
features. These are believed to originate from different mechanisms, ranging
from binary int... | astro-ph.SR astro-ph.GA | equatorial density enhancements edes are a very common astronomical phenomenon studies of the circumstellar environments cse of young stellar objects and of evolved stars have shown that these objects often possess these features these are believed to originate from different mechanisms ranging from binary interactions... | [['equatorial', 'density', 'enhancements', 'edes', 'are', 'a', 'very', 'common', 'astronomical', 'phenomenon', 'studies', 'of', 'the', 'circumstellar', 'environments', 'cse', 'of', 'young', 'stellar', 'objects', 'and', 'of', 'evolved', 'stars', 'have', 'shown', 'that', 'these', 'objects', 'often', 'possess', 'these', '... | [-0.09567894784186501, 0.07181595597747946, -0.07339839934674092, 0.10340630340902135, -0.0966660858374089, -0.06870646737515926, -0.021520735966041683, 0.398961679989472, -0.24538471287302674, -0.32257193097425624, 0.07477007428510114, -0.23301414091931655, -0.09666658849641681, 0.1819523465940729, -0.0176065466208383... |
1,803.05231 | Deformation space of discrete groups of SU(2,1) in quaternionic
hyperbolic plane | In this note, we study deformations of discrete and Zariski dense subgroups
of SU(2, 1) in quaternionic hyperbolic space. Specifi- cally we consider two
examples coming from representations of 3-manifold groups (the figure eight
knot and Whitehead links complement) and show opposite behavior: one is not
deformable ou... | math.GT | in this note we study deformations of discrete and zariski dense subgroups of su2 1 in quaternionic hyperbolic space specifi cally we consider two examples coming from representations of 3manifold groups the figure eight knot and whitehead links complement and show opposite behavior one is not deformable outside u21 wh... | [['in', 'this', 'note', 'we', 'study', 'deformations', 'of', 'discrete', 'and', 'zariski', 'dense', 'subgroups', 'of', 'su2', '1', 'in', 'quaternionic', 'hyperbolic', 'space', 'specifi', 'cally', 'we', 'consider', 'two', 'examples', 'coming', 'from', 'representations', 'of', '3manifold', 'groups', 'the', 'figure', 'eig... | [-0.189305587419782, 0.10073437347824944, -0.07063600900353956, 0.050971125222009715, -0.0883444841248823, -0.13072654000124664, -0.033672059214383855, 0.38164640091298546, -0.2885796795980852, -0.23210420850359026, 0.12040451822657382, -0.31616678360666406, -0.18365295461882822, 0.15817881426697628, -0.170295377781034... |
1,803.05232 | Energy Reconstruction of Hadrons in highly granular combined ECAL and
HCAL systems | This paper discusses the hadronic energy reconstruction of two combined
electromagnetic and hadronic calorimeter systems using physics prototypes of
the CALICE collaboration: the silicon-tungsten electromagnetic calorimeter
(Si-W ECAL) and the scintillator-SiPM based analog hadron calorimeter (AHCAL);
and the scintil... | physics.ins-det | this paper discusses the hadronic energy reconstruction of two combined electromagnetic and hadronic calorimeter systems using physics prototypes of the calice collaboration the silicontungsten electromagnetic calorimeter siw ecal and the scintillatorsipm based analog hadron calorimeter ahcal and the scintillatortungst... | [['this', 'paper', 'discusses', 'the', 'hadronic', 'energy', 'reconstruction', 'of', 'two', 'combined', 'electromagnetic', 'and', 'hadronic', 'calorimeter', 'systems', 'using', 'physics', 'prototypes', 'of', 'the', 'calice', 'collaboration', 'the', 'silicontungsten', 'electromagnetic', 'calorimeter', 'siw', 'ecal', 'an... | [-0.06908460130948506, 0.1274492387533673, -0.07044731824195938, 0.056466231660075306, -0.0005571898616694226, -0.10060100228397433, -0.054561920535839914, 0.3631328437519176, -0.19166980571152564, -0.390049819204354, 0.07752495044619291, -0.3157397537899321, 0.008783252374408487, 0.21005232818424702, 0.019681877688041... |
1,803.05233 | CloudHealth: A Model-Driven Approach to Watch the Health of Cloud
Services | Cloud systems are complex and large systems where services provided by
different operators must coexist and eventually cooperate. In such a complex
environment, controlling the health of both the whole environment and the
individual services is extremely important to timely and effectively react to
misbehaviours, une... | cs.SE | cloud systems are complex and large systems where services provided by different operators must coexist and eventually cooperate in such a complex environment controlling the health of both the whole environment and the individual services is extremely important to timely and effectively react to misbehaviours unexpect... | [['cloud', 'systems', 'are', 'complex', 'and', 'large', 'systems', 'where', 'services', 'provided', 'by', 'different', 'operators', 'must', 'coexist', 'and', 'eventually', 'cooperate', 'in', 'such', 'a', 'complex', 'environment', 'controlling', 'the', 'health', 'of', 'both', 'the', 'whole', 'environment', 'and', 'the',... | [-0.12848546084898868, 0.09336617434838493, -0.07964957350938531, 0.07513105477770105, -0.06785689967954041, -0.14359562771983053, 0.0718772193410826, 0.38780287644384726, -0.2575049959846135, -0.35930272407989067, 0.16471080777578448, -0.3282423251823179, -0.12089282463451749, 0.1954984439880048, -0.11666702896013464,... |
1,803.05234 | Optical properties of dense lithium in electride phases by
first-principles calculations | The metal-semiconductor-metal transition in dense lithium is considered as an
archetype of interplay between interstitial electron localization and
delocalization induced by compression, which leads to exotic electride phases.
In this work, the dynamic dielectric response and optical properties of the
high-pressure e... | cond-mat.mtrl-sci physics.comp-ph physics.optics | the metalsemiconductormetal transition in dense lithium is considered as an archetype of interplay between interstitial electron localization and delocalization induced by compression which leads to exotic electride phases in this work the dynamic dielectric response and optical properties of the highpressure electride... | [['the', 'metalsemiconductormetal', 'transition', 'in', 'dense', 'lithium', 'is', 'considered', 'as', 'an', 'archetype', 'of', 'interplay', 'between', 'interstitial', 'electron', 'localization', 'and', 'delocalization', 'induced', 'by', 'compression', 'which', 'leads', 'to', 'exotic', 'electride', 'phases', 'in', 'this... | [-0.1066867838066537, 0.22210899808749673, -0.021166134143713863, 0.01893957623571623, -0.026154251811094584, -0.1384477888868423, 0.09587082624260802, 0.41944425836205484, -0.23841282899025829, -0.32331747172400355, 0.00932400401943596, -0.34704795413650574, -0.14401934608817102, 0.1556065651238896, 0.0499402375461068... |
1,803.05235 | Pseudo Dirac Nodal Sphere: Unusual Electronic Structure and Material
Realization | Topological semimetals (TSMs) in which conduction and valence bands cross at
zero-dimensional (0D) Dirac nodal points (DNPs) or 1D Dirac nodal lines (DNLs),
in 3D momentum space, have recently drawn much attention due to their exotic
electronic properties. Here we generalize the TSM state further to a
higher-symmetry... | cond-mat.mes-hall cond-mat.mtrl-sci | topological semimetals tsms in which conduction and valence bands cross at zerodimensional 0d dirac nodal points dnps or 1d dirac nodal lines dnls in 3d momentum space have recently drawn much attention due to their exotic electronic properties here we generalize the tsm state further to a highersymmetry and higherdime... | [['topological', 'semimetals', 'tsms', 'in', 'which', 'conduction', 'and', 'valence', 'bands', 'cross', 'at', 'zerodimensional', '0d', 'dirac', 'nodal', 'points', 'dnps', 'or', '1d', 'dirac', 'nodal', 'lines', 'dnls', 'in', '3d', 'momentum', 'space', 'have', 'recently', 'drawn', 'much', 'attention', 'due', 'to', 'their... | [-0.17731489990433735, 0.17950989356942457, -0.024420682034742357, 0.061819106650447056, -0.05445622190485655, -0.20647457573524255, 0.11434928198837208, 0.3738491711408199, -0.26142135745281153, -0.2665407283525972, 0.0075097952235292234, -0.35898614666603235, -0.13731622149916897, 0.11836889340576036, 0.0578787580655... |
1,803.05236 | Some negative results related to Poissonian pair correlation problems | We say that a sequence $(x_n)_{n \in \mathbb{N}}$ in $[0,1)$ has Poissonian
pair correlations if \begin{equation*} \lim_{N \to \infty} \frac{1}{N} \# \left
\lbrace 1 \leq l \neq m \leq N: \| x_l - x_m \| \leq \frac{s}{N} \right \rbrace
= 2s \end{equation*} for every $s \geq 0$. The aim of this article is twofold.
Fir... | math.NT | we say that a sequence x_n_n in mathbbn in 01 has poissonian pair correlations if beginequation lim_n to infty frac1n left lbrace 1 leq l neq m leq n x_l x_m leq fracsn right rbrace 2s endequation for every s geq 0 the aim of this article is twofold first we will establish a gap theorem which allows to deduce that a se... | [['we', 'say', 'that', 'a', 'sequence', 'x_n_n', 'in', 'mathbbn', 'in', '01', 'has', 'poissonian', 'pair', 'correlations', 'if', 'beginequation', 'lim_n', 'to', 'infty', 'frac1n', 'left', 'lbrace', '1', 'leq', 'l', 'neq', 'm', 'leq', 'n', 'x_l', 'x_m', 'leq', 'fracsn', 'right', 'rbrace', '2s', 'endequation', 'for', 'ev... | [-0.20472523398050216, 0.16975074589836153, -0.02557217111026384, 0.058905357045788816, -0.013451622151879696, -0.1684382578457053, -0.002546335884927237, 0.37437704854872167, -0.32270812009200894, -0.22218074115379585, 0.028912442404956475, -0.3545654751700152, -0.1284393628492702, 0.13570737715913203, -0.080920005444... |
1,803.05237 | Blue wing enhancement of the chromospheric Mg II h and k lines in a
solar flare | We performed coordinated observations of AR 12205, which produced a C-class
flare on 2014 November 11, with the Interface Region Imaging Spectrograph
(IRIS) and the Domeless Solar Telescope (DST) at Hida Observatory. Using
spectral data in the Si IV 1403 \AA, C II 1335 \AA, and Mg II h and k lines
from IRIS and the C... | astro-ph.SR | we performed coordinated observations of ar 12205 which produced a cclass flare on 2014 november 11 with the interface region imaging spectrograph iris and the domeless solar telescope dst at hida observatory using spectral data in the si iv 1403 aa c ii 1335 aa and mg ii h and k lines from iris and the ca ii k ca ii 8... | [['we', 'performed', 'coordinated', 'observations', 'of', 'ar', '12205', 'which', 'produced', 'a', 'cclass', 'flare', 'on', '2014', 'november', '11', 'with', 'the', 'interface', 'region', 'imaging', 'spectrograph', 'iris', 'and', 'the', 'domeless', 'solar', 'telescope', 'dst', 'at', 'hida', 'observatory', 'using', 'spe... | [-0.05499234424507314, 0.14862389309354412, 0.026395622436690178, 0.03372235539007104, -0.03206305986968801, -0.1593259396617887, 0.030271041323754213, 0.470514965640312, -0.17130327442902382, -0.3339368536344005, 0.06145761921717268, -0.28765146912041084, -0.034818000485689414, 0.16595823233947157, -0.0115531872053570... |
1,803.05238 | A Likely Detection of a Two-Planet System in a Low Magnification
Microlensing Event | We report on the analysis of a microlensing event OGLE-2014-BLG-1722 that
showed two distinct short term anomalies. The best fit model to the observed
light curves shows that the two anomalies are explained with two planetary mass
ratio companions to the primary lens. Although a binary source model is also
able to ex... | astro-ph.EP | we report on the analysis of a microlensing event ogle2014blg1722 that showed two distinct short term anomalies the best fit model to the observed light curves shows that the two anomalies are explained with two planetary mass ratio companions to the primary lens although a binary source model is also able to explain t... | [['we', 'report', 'on', 'the', 'analysis', 'of', 'a', 'microlensing', 'event', 'ogle2014blg1722', 'that', 'showed', 'two', 'distinct', 'short', 'term', 'anomalies', 'the', 'best', 'fit', 'model', 'to', 'the', 'observed', 'light', 'curves', 'shows', 'that', 'the', 'two', 'anomalies', 'are', 'explained', 'with', 'two', '... | [-0.15267236211587695, 0.08909265313000567, -0.0417213340492774, 0.05271624775596665, -0.0676730308771147, -0.11908653685553135, 0.07188084079087645, 0.3066604514471323, -0.16270262480922637, -0.40390254177180107, 0.08076916041191788, -0.3162049193313156, -0.08613796967277439, 0.18317298583544628, -0.048455527911900775... |
1,803.05239 | A complex network framework to model cognition: unveiling correlation
structures from connectivity | Several approaches to cognition and intelligence research rely on
statistics-based models testing, namely factor analysis. In the present work we
exploit the emerging dynamical systems perspective putting the focus on the
role of the network topology underlying the relationships between cognitive
processes. We go thr... | physics.soc-ph cond-mat.dis-nn q-bio.NC | several approaches to cognition and intelligence research rely on statisticsbased models testing namely factor analysis in the present work we exploit the emerging dynamical systems perspective putting the focus on the role of the network topology underlying the relationships between cognitive processes we go through a... | [['several', 'approaches', 'to', 'cognition', 'and', 'intelligence', 'research', 'rely', 'on', 'statisticsbased', 'models', 'testing', 'namely', 'factor', 'analysis', 'in', 'the', 'present', 'work', 'we', 'exploit', 'the', 'emerging', 'dynamical', 'systems', 'perspective', 'putting', 'the', 'focus', 'on', 'the', 'role'... | [-0.1362828565215301, 0.0683989655226469, -0.10431019497322447, 0.1239158691497761, -0.07675643298159825, -0.16116404101859066, 0.03311722514501279, 0.3833130389181782, -0.2933996547743632, -0.30820595728015, 0.06929812714080959, -0.23885102660674026, -0.2549015768389735, 0.16463156198553833, -0.011388564278245156, 0.0... |
1,803.0524 | Parametric model order reduction for large-scale and complex thermal
systems | In this paper, a parametric model order reduction (pMOR) technique is
proposed to find a simplified system representation of a large-scale and
complex thermal system. The main principle behind this technique is that any
change of the physical parameters in the high-fidelity model can be updated
directly in the simpli... | cs.SY | in this paper a parametric model order reduction pmor technique is proposed to find a simplified system representation of a largescale and complex thermal system the main principle behind this technique is that any change of the physical parameters in the highfidelity model can be updated directly in the simplified mod... | [['in', 'this', 'paper', 'a', 'parametric', 'model', 'order', 'reduction', 'pmor', 'technique', 'is', 'proposed', 'to', 'find', 'a', 'simplified', 'system', 'representation', 'of', 'a', 'largescale', 'and', 'complex', 'thermal', 'system', 'the', 'main', 'principle', 'behind', 'this', 'technique', 'is', 'that', 'any', '... | [-0.08423412446440622, 0.0545014986472035, -0.0993858115451241, 0.05719508693172512, -0.04629362636796114, -0.10108733635649762, 0.054186348025475374, 0.3070966515436091, -0.30015992334281855, -0.30594402108002794, 0.09834189584415237, -0.20562517892897383, -0.14303764957849952, 0.182994792225178, -0.030095730679617686... |
1,803.05241 | Plastic deformation of a permanently bonded network: stress relaxation
by pleats | We show that a flat two dimensional network of connected vertices, when
stretched, may deform plastically by producing `pleats'; system spanning linear
structures with width comparable to the lattice spacing, where the network
overlaps on itself. To understand the pleating process, we introduce an
external field that... | cond-mat.soft | we show that a flat two dimensional network of connected vertices when stretched may deform plastically by producing pleats system spanning linear structures with width comparable to the lattice spacing where the network overlaps on itself to understand the pleating process we introduce an external field that couples t... | [['we', 'show', 'that', 'a', 'flat', 'two', 'dimensional', 'network', 'of', 'connected', 'vertices', 'when', 'stretched', 'may', 'deform', 'plastically', 'by', 'producing', 'pleats', 'system', 'spanning', 'linear', 'structures', 'with', 'width', 'comparable', 'to', 'the', 'lattice', 'spacing', 'where', 'the', 'network'... | [-0.15446097341859166, 0.2400856173777035, -0.08526609332081588, 0.016626042106776474, -0.040333175785182154, -0.1060170628986431, 0.02196127693853615, 0.3940223930951427, -0.32164565987118027, -0.21811140450470917, 0.07970374462345396, -0.24047045019893523, -0.16034439998843214, 0.10748461658025489, -0.015812400512753... |
1,803.05242 | Ground-state properties of a dilute two-dimensional Bose gas | We revisit the problem of the calculation of low-temperature properties for
the dilute two-dimensional Bose gas. By using Popov's hydrodynamic approach and
perturbation theory on the one-loop level we recover not only the known
expansion for the ground-state energy but also calculate for the first time the
condensate... | cond-mat.quant-gas | we revisit the problem of the calculation of lowtemperature properties for the dilute twodimensional bose gas by using popovs hydrodynamic approach and perturbation theory on the oneloop level we recover not only the known expansion for the groundstate energy but also calculate for the first time the condensate density... | [['we', 'revisit', 'the', 'problem', 'of', 'the', 'calculation', 'of', 'lowtemperature', 'properties', 'for', 'the', 'dilute', 'twodimensional', 'bose', 'gas', 'by', 'using', 'popovs', 'hydrodynamic', 'approach', 'and', 'perturbation', 'theory', 'on', 'the', 'oneloop', 'level', 'we', 'recover', 'not', 'only', 'the', 'k... | [-0.09558803188422015, 0.11901694300244205, -0.09969934839934397, 0.08204869057338399, 0.041484923334792256, -0.07249960066893926, 0.06341860225522676, 0.2905826907282552, -0.21625919765434587, -0.24377763786021836, 0.051353206956544176, -0.27562525123357773, -0.10780066939276786, 0.14094857298410857, 0.091076796211732... |
1,803.05243 | Robust multipartite entanglement generation via a collision model | We examine a simple scheme to generate genuine multipartite entangled states
across disjoint qubit registers. We employ a shuttle qubit that is sequentially
coupled, in an energy preserving manner, to the constituents within each
register through rounds of interactions. We establish that stable $W$-type
entanglement ... | quant-ph | we examine a simple scheme to generate genuine multipartite entangled states across disjoint qubit registers we employ a shuttle qubit that is sequentially coupled in an energy preserving manner to the constituents within each register through rounds of interactions we establish that stable wtype entanglement can be ge... | [['we', 'examine', 'a', 'simple', 'scheme', 'to', 'generate', 'genuine', 'multipartite', 'entangled', 'states', 'across', 'disjoint', 'qubit', 'registers', 'we', 'employ', 'a', 'shuttle', 'qubit', 'that', 'is', 'sequentially', 'coupled', 'in', 'an', 'energy', 'preserving', 'manner', 'to', 'the', 'constituents', 'within... | [-0.1765022101324229, 0.2087869638988715, -0.051147442633130896, 0.038858901013043665, 0.042233505494715204, -0.22757085581709233, 0.08072611527916576, 0.4208772714028046, -0.2556638108477706, -0.27610088343776407, 0.03264312458424164, -0.2637395185684519, -0.11600966594137606, 0.20337270116876988, -0.0841634725065281,... |
1,803.05244 | Stochastic Dynamic Utilities and Inter-Temporal Preferences | We propose an axiomatic approach which economically underpins the
representation of dynamic preferences in terms of a stochastic utility
function, sensitive to the information available to the decision maker. Our
construction is iterative and based on inter-temporal preference relations,
whose characterization is inp... | math.PR q-fin.EC | we propose an axiomatic approach which economically underpins the representation of dynamic preferences in terms of a stochastic utility function sensitive to the information available to the decision maker our construction is iterative and based on intertemporal preference relations whose characterization is inpired b... | [['we', 'propose', 'an', 'axiomatic', 'approach', 'which', 'economically', 'underpins', 'the', 'representation', 'of', 'dynamic', 'preferences', 'in', 'terms', 'of', 'a', 'stochastic', 'utility', 'function', 'sensitive', 'to', 'the', 'information', 'available', 'to', 'the', 'decision', 'maker', 'our', 'construction', '... | [-0.056138481637287255, 0.04200137239020924, -0.13861532474402338, 0.08781093240820996, -0.18862140189223695, -0.11897070026728061, 0.11214896945836339, 0.37492960740653974, -0.3031518210498792, -0.3034481825526663, 0.10260639883323028, -0.2570158055860479, -0.19602967327776946, 0.13088793961225814, -0.1284045136516105... |
1,803.05245 | Device independent witness of arbitrary dimensional quantum systems
employing binary outcome measurements | Device independent dimension witnesses (DW) are a remarkable way to test the
dimension of a quantum system in a prepare-and-measure scenario imposing
minimal assumptions on the internal features of the devices. However, as the
dimension increases, the major obstacle in the realization of DW arises due to
the requirem... | quant-ph | device independent dimension witnesses dw are a remarkable way to test the dimension of a quantum system in a prepareandmeasure scenario imposing minimal assumptions on the internal features of the devices however as the dimension increases the major obstacle in the realization of dw arises due to the requirement of ma... | [['device', 'independent', 'dimension', 'witnesses', 'dw', 'are', 'a', 'remarkable', 'way', 'to', 'test', 'the', 'dimension', 'of', 'a', 'quantum', 'system', 'in', 'a', 'prepareandmeasure', 'scenario', 'imposing', 'minimal', 'assumptions', 'on', 'the', 'internal', 'features', 'of', 'the', 'devices', 'however', 'as', 't... | [-0.19473903427921957, 0.10109719709162751, -0.07063573079874678, 0.023148825606181016, -0.06837221968578555, -0.20201428794372145, 0.07912094660493876, 0.3293309415870857, -0.268053895603585, -0.2883618949281593, 0.0940524061843853, -0.2177637524787657, -0.12820732418287506, 0.2073272839789429, -0.09968629445923212, 0... |
1,803.05246 | On the connectivity threshold for colorings of random graphs and
hypergraphs | Let $\Omega_q=\Omega_q(H)$ denote the set of proper $[q]$-colorings of the
hypergraph $H$. Let $\Gamma_q$ be the graph with vertex set $\Omega_q$ and an
edge ${\sigma,\tau\}$ where $\sigma,\tau$ are colorings iff $h(\sigma,\tau)=1$.
Here $h(\sigma,\tau)$ is the Hamming distance $|\{v\in
V(H):\sigma(v)\neq\tau(v)\}|$.... | math.CO cs.DM math.PR | let omega_qomega_qh denote the set of proper qcolorings of the hypergraph h let gamma_q be the graph with vertex set omega_q and an edge sigmatau where sigmatau are colorings iff hsigmatau1 here hsigmatau is the hamming distance vin vhsigmavneqtauv we show that if hh_nmkkgeq 2 the random kuniform hypergraph with vn and... | [['let', 'omega_qomega_qh', 'denote', 'the', 'set', 'of', 'proper', 'qcolorings', 'of', 'the', 'hypergraph', 'h', 'let', 'gamma_q', 'be', 'the', 'graph', 'with', 'vertex', 'set', 'omega_q', 'and', 'an', 'edge', 'sigmatau', 'where', 'sigmatau', 'are', 'colorings', 'iff', 'hsigmatau1', 'here', 'hsigmatau', 'is', 'the', '... | [-0.19528214155385892, 0.22319452689092334, -0.030191647556299963, -0.07659843242145144, -0.08580819825486591, -0.2458056007201473, 0.014930784640212854, 0.3793543972695867, -0.32051707851933314, -0.23910371613067885, 0.037866163463331756, -0.39344731296102203, -0.07603684353331724, 0.031609254966800414, -0.10883194426... |
1,803.05247 | Identifiability of Undirected Dynamical Networks: a Graph-Theoretic
Approach | This paper deals with identifiability of undirected dynamical networks with
single-integrator node dynamics. We assume that the graph structure of such
networks is known, and aim to find graph-theoretic conditions under which the
state matrix of the network can be uniquely identified. As our main
contribution, we pre... | math.OC math.DS | this paper deals with identifiability of undirected dynamical networks with singleintegrator node dynamics we assume that the graph structure of such networks is known and aim to find graphtheoretic conditions under which the state matrix of the network can be uniquely identified as our main contribution we present a g... | [['this', 'paper', 'deals', 'with', 'identifiability', 'of', 'undirected', 'dynamical', 'networks', 'with', 'singleintegrator', 'node', 'dynamics', 'we', 'assume', 'that', 'the', 'graph', 'structure', 'of', 'such', 'networks', 'is', 'known', 'and', 'aim', 'to', 'find', 'graphtheoretic', 'conditions', 'under', 'which', ... | [-0.16252089377050682, 0.06321522598344757, -0.05024299361758818, 0.035022216961498105, -0.06940063295325548, -0.13799820256900927, 0.0314806593706342, 0.40250843810706827, -0.3032247802337347, -0.3054427092074085, 0.09541326425614435, -0.22655405467218262, -0.24388389021031937, 0.09576416876703753, -0.0697510591510809... |
1,803.05248 | Generalized Taylor operators and Hermite subdivision schemes | Hermite subdivision schemes act on vector valued data that is not only
considered as functions values in $\mathbb{R}^r$, but as consecutive
derivatives, which leads to a mild form of level dependence of the scheme.
Previously, we have proved that a property called spectral condition or sum
rule implies a factorizatio... | math.NA | hermite subdivision schemes act on vector valued data that is not only considered as functions values in mathbbrr but as consecutive derivatives which leads to a mild form of level dependence of the scheme previously we have proved that a property called spectral condition or sum rule implies a factorization in terms o... | [['hermite', 'subdivision', 'schemes', 'act', 'on', 'vector', 'valued', 'data', 'that', 'is', 'not', 'only', 'considered', 'as', 'functions', 'values', 'in', 'mathbbrr', 'but', 'as', 'consecutive', 'derivatives', 'which', 'leads', 'to', 'a', 'mild', 'form', 'of', 'level', 'dependence', 'of', 'the', 'scheme', 'previousl... | [-0.1291359000275061, 0.05478374828944785, -0.14694176690081936, 0.0837731870965366, -0.12163358547446067, -0.13197698729642987, 0.04108609317718617, 0.3831791401480454, -0.276936088029268, -0.2019804464449195, 0.10422856167271516, -0.21947927985775428, -0.17640872687325698, 0.21315574518788988, -0.1015415166514878, 0.... |
1,803.05249 | The skeleton of the UIPT, seen from infinity | We prove that geodesic rays in the Uniform Infinite Planar Triangulation
(UIPT) coalesce in a strong sense using the skeleton decomposition of random
triangulations discovered by Krikun. This implies the existence of a unique
horofunction measuring distances from infinity in the UIPT. We then use this
horofunction to... | math.PR math-ph math.CO math.MP | we prove that geodesic rays in the uniform infinite planar triangulation uipt coalesce in a strong sense using the skeleton decomposition of random triangulations discovered by krikun this implies the existence of a unique horofunction measuring distances from infinity in the uipt we then use this horofunction to defin... | [['we', 'prove', 'that', 'geodesic', 'rays', 'in', 'the', 'uniform', 'infinite', 'planar', 'triangulation', 'uipt', 'coalesce', 'in', 'a', 'strong', 'sense', 'using', 'the', 'skeleton', 'decomposition', 'of', 'random', 'triangulations', 'discovered', 'by', 'krikun', 'this', 'implies', 'the', 'existence', 'of', 'a', 'un... | [-0.09345821521811835, 0.13276453011304787, -0.14612567343789598, 0.09162498562819446, -0.08537391876072987, -0.07751792450232999, 0.07768245405800965, 0.3061594080665837, -0.3066229972016552, -0.21537003331898671, 0.11056880837903642, -0.25907068223813956, -0.1657069655742658, 0.17567517776852068, -0.10064081260327087... |
1,803.0525 | A mean-field game model for homogeneous flocking | Empirically derived continuum models of collective behavior among large
populations of dynamic agents are a subject of intense study in several fields,
including biology, engineering and finance. We formulate and study a mean-field
game model whose behavior mimics an empirically derived non-local homogeneous
flocking... | nlin.AO cs.SY math.DS math.OC | empirically derived continuum models of collective behavior among large populations of dynamic agents are a subject of intense study in several fields including biology engineering and finance we formulate and study a meanfield game model whose behavior mimics an empirically derived nonlocal homogeneous flocking model ... | [['empirically', 'derived', 'continuum', 'models', 'of', 'collective', 'behavior', 'among', 'large', 'populations', 'of', 'dynamic', 'agents', 'are', 'a', 'subject', 'of', 'intense', 'study', 'in', 'several', 'fields', 'including', 'biology', 'engineering', 'and', 'finance', 'we', 'formulate', 'and', 'study', 'a', 'mea... | [-0.1330474920533783, 0.058464413162567584, -0.14095900673419237, 0.06490524259015955, -0.04707450531793768, -0.15313427006844338, 0.09248858514828005, 0.35337526585665807, -0.30579376376155226, -0.2892963886220444, 0.057180963035566336, -0.2506478021977775, -0.19415425926108673, 0.12266850098967552, -0.057520972578400... |
1,803.05251 | The Local Bubble: a magnetic veil to our Galaxy | The magnetic field in the local interstellar medium does not follow the
large-scale Galactic magnetic field. The local magnetic field has probably been
distorted by the Local Bubble, a cavity of hot ionized gas extending all around
the Sun and surrounded by a shell of cold neutral gas and dust. However, so far
no con... | astro-ph.GA | the magnetic field in the local interstellar medium does not follow the largescale galactic magnetic field the local magnetic field has probably been distorted by the local bubble a cavity of hot ionized gas extending all around the sun and surrounded by a shell of cold neutral gas and dust however so far no conclusive... | [['the', 'magnetic', 'field', 'in', 'the', 'local', 'interstellar', 'medium', 'does', 'not', 'follow', 'the', 'largescale', 'galactic', 'magnetic', 'field', 'the', 'local', 'magnetic', 'field', 'has', 'probably', 'been', 'distorted', 'by', 'the', 'local', 'bubble', 'a', 'cavity', 'of', 'hot', 'ionized', 'gas', 'extendi... | [-0.09878309113589828, 0.11816331982109285, -0.0559548101382782, 0.06412880857653148, -0.08906359793481362, -0.026732637640088798, -0.006357282026917399, 0.40790329108781676, -0.22492788159083027, -0.3174234935863163, 0.041672882644599986, -0.23926816837081466, -0.04993406621848836, 0.14430323471041287, 0.0440903285042... |
1,803.05252 | Algebraic Machine Learning | Machine learning algorithms use error function minimization to fit a large
set of parameters in a preexisting model. However, error minimization
eventually leads to a memorization of the training dataset, losing the ability
to generalize to other datasets. To achieve generalization something else is
needed, for examp... | cs.LG cs.DM math.AC math.RA | machine learning algorithms use error function minimization to fit a large set of parameters in a preexisting model however error minimization eventually leads to a memorization of the training dataset losing the ability to generalize to other datasets to achieve generalization something else is needed for example a re... | [['machine', 'learning', 'algorithms', 'use', 'error', 'function', 'minimization', 'to', 'fit', 'a', 'large', 'set', 'of', 'parameters', 'in', 'a', 'preexisting', 'model', 'however', 'error', 'minimization', 'eventually', 'leads', 'to', 'a', 'memorization', 'of', 'the', 'training', 'dataset', 'losing', 'the', 'ability'... | [-0.03690334925139766, 0.010555731350697378, -0.11415221215713592, 0.09390925755225388, -0.16000827355088576, -0.1700287348701663, 0.05508413512725383, 0.3777048921611692, -0.3154478905888807, -0.33767131651208426, 0.10268207054718265, -0.25048409436602104, -0.15411364275496453, 0.1859028163887117, -0.14502447115567824... |
1,803.05253 | How to Implement Dependencies in Server Pages of JEE Web Applications | Java Enterprise Edition (JEE) applications are implemented in terms of a set
of components developed based on several JEE technologies includ- ing, but not
limited to, Servlet, JSP, JSF, EJB, JavaBeans. These JEE technologies rely on a
varied set of communication mechanisms to commu- nicate between each others.
Examp... | cs.SE | java enterprise edition jee applications are implemented in terms of a set of components developed based on several jee technologies includ ing but not limited to servlet jsp jsf ejb javabeans these jee technologies rely on a varied set of communication mechanisms to commu nicate between each others examples of these c... | [['java', 'enterprise', 'edition', 'jee', 'applications', 'are', 'implemented', 'in', 'terms', 'of', 'a', 'set', 'of', 'components', 'developed', 'based', 'on', 'several', 'jee', 'technologies', 'includ', 'ing', 'but', 'not', 'limited', 'to', 'servlet', 'jsp', 'jsf', 'ejb', 'javabeans', 'these', 'jee', 'technologies', ... | [-0.16541748463000294, 0.04615726165582229, -0.03694717277412432, 0.05186928249470699, -0.12119670597034214, -0.21242089746655882, 0.08210277609037657, 0.3996090245072859, -0.26609822060831273, -0.3505444036334427, 0.10549497723844528, -0.2618613804003944, -0.1488280630106256, 0.23801414368089532, -0.0908885286121636, ... |
1,803.05254 | Impacts of multi-Higgs on the $\rho$ parameter, decays of a neutral
Higgs to $WW$ and $ZZ$, and a charged Higgs to $WZ$ | In the standard model (SM), the $\rho$ parameter is equal to 1 and the ratio
$\lambda_{WZ}$ of Higgs $\to ZZ$ and Higgs $\to WW$ is also equal to 1 at the
tree level. When going beyond the SM with more than one types of Higgs
representations these quantities may be different from the SM predictions which
can provide ... | hep-ph hep-ex | in the standard model sm the rho parameter is equal to 1 and the ratio lambda_wz of higgs to zz and higgs to ww is also equal to 1 at the tree level when going beyond the sm with more than one types of higgs representations these quantities may be different from the sm predictions which can provide crucial information ... | [['in', 'the', 'standard', 'model', 'sm', 'the', 'rho', 'parameter', 'is', 'equal', 'to', '1', 'and', 'the', 'ratio', 'lambda_wz', 'of', 'higgs', 'to', 'zz', 'and', 'higgs', 'to', 'ww', 'is', 'also', 'equal', 'to', '1', 'at', 'the', 'tree', 'level', 'when', 'going', 'beyond', 'the', 'sm', 'with', 'more', 'than', 'one',... | [-0.04737951660865982, 0.2154596676343474, -0.07215262710855438, 0.1410644224058066, -0.11090553129284546, -0.2462659425872924, 0.0424856982887863, 0.32603990281450335, -0.25935365561524343, -0.31222605964104677, 0.04968734465314653, -0.2969814598881479, -0.04894609081334081, 0.1102962862764453, 0.0075419325188829985, ... |
1,803.05255 | Addressing the Challenges in Federating Edge Resources | This book chapter considers how Edge deployments can be brought to bear in a
global context by federating them across multiple geographic regions to create
a global Edge-based fabric that decentralizes data center computation. This is
currently impractical, not only because of technical challenges, but is also
shroud... | cs.DC | this book chapter considers how edge deployments can be brought to bear in a global context by federating them across multiple geographic regions to create a global edgebased fabric that decentralizes data center computation this is currently impractical not only because of technical challenges but is also shrouded by ... | [['this', 'book', 'chapter', 'considers', 'how', 'edge', 'deployments', 'can', 'be', 'brought', 'to', 'bear', 'in', 'a', 'global', 'context', 'by', 'federating', 'them', 'across', 'multiple', 'geographic', 'regions', 'to', 'create', 'a', 'global', 'edgebased', 'fabric', 'that', 'decentralizes', 'data', 'center', 'compu... | [-0.162502518429984, 0.05494549672043514, -0.015977499676261876, 0.06751532741513666, -0.11884377567574035, -0.16081314252927725, 0.07726992347256043, 0.40286351633691336, -0.306871083846619, -0.311809973184799, 0.18623921489695, -0.24818793696156422, -0.22204372039887793, 0.12789879345096822, -0.18961256105949573, 0.0... |
1,803.05256 | Newton-type Alternating Minimization Algorithm for Convex Optimization | We propose NAMA (Newton-type Alternating Minimization Algorithm) for solving
structured nonsmooth convex optimization problems where the sum of two
functions is to be minimized, one being strongly convex and the other composed
with a linear mapping. The proposed algorithm is a line-search method over a
continuous, re... | math.OC | we propose nama newtontype alternating minimization algorithm for solving structured nonsmooth convex optimization problems where the sum of two functions is to be minimized one being strongly convex and the other composed with a linear mapping the proposed algorithm is a linesearch method over a continuous realvalued ... | [['we', 'propose', 'nama', 'newtontype', 'alternating', 'minimization', 'algorithm', 'for', 'solving', 'structured', 'nonsmooth', 'convex', 'optimization', 'problems', 'where', 'the', 'sum', 'of', 'two', 'functions', 'is', 'to', 'be', 'minimized', 'one', 'being', 'strongly', 'convex', 'and', 'the', 'other', 'composed',... | [-0.07381263086687267, -0.005858223739419317, -0.08173479231787317, 0.06689346335141311, -0.09903736741075085, -0.18468476171363835, 0.025881249305611063, 0.4110220872802821, -0.3507040628967922, -0.27018280690219715, 0.15268536605642258, -0.21040461717833145, -0.1782236048652802, 0.21876073333888924, -0.06763112096266... |
1,803.05257 | Lov\'asz extension and graph cut | A set-pair Lov\'asz extension is established to construct equivalent
continuous optimization problems for graph $k$-cut problems.
| math.CO math.OC math.SP | a setpair lovasz extension is established to construct equivalent continuous optimization problems for graph kcut problems | [['a', 'setpair', 'lovasz', 'extension', 'is', 'established', 'to', 'construct', 'equivalent', 'continuous', 'optimization', 'problems', 'for', 'graph', 'kcut', 'problems']] | [-0.07269028201699257, -0.0714857650299867, -0.09539216915145517, 0.26622707201944046, -0.19783966802060604, -0.24827562182520826, -0.013700885822375615, 0.3605507045984268, -0.42867259234189986, -0.3073726140273114, 0.22755596563220024, -0.199139004945755, -0.16426295017202694, 0.16461842482288677, -0.194416196939225,... |
1,803.05258 | Face-MagNet: Magnifying Feature Maps to Detect Small Faces | In this paper, we introduce the Face Magnifier Network (Face-MageNet), a face
detector based on the Faster-RCNN framework which enables the flow of
discriminative information of small scale faces to the classifier without any
skip or residual connections. To achieve this, Face-MagNet deploys a set of
ConvTranspose, a... | cs.CV | in this paper we introduce the face magnifier network facemagenet a face detector based on the fasterrcnn framework which enables the flow of discriminative information of small scale faces to the classifier without any skip or residual connections to achieve this facemagnet deploys a set of convtranspose also known as... | [['in', 'this', 'paper', 'we', 'introduce', 'the', 'face', 'magnifier', 'network', 'facemagenet', 'a', 'face', 'detector', 'based', 'on', 'the', 'fasterrcnn', 'framework', 'which', 'enables', 'the', 'flow', 'of', 'discriminative', 'information', 'of', 'small', 'scale', 'faces', 'to', 'the', 'classifier', 'without', 'an... | [-0.043348837787142165, -0.04271876130503817, -0.044915608351286024, 0.01155014627893718, -0.07893644590885976, -0.1782111360837753, 0.03444055441949063, 0.44376820380775595, -0.23905941910253695, -0.31560223072003096, 0.09930414914896783, -0.28560153811047667, -0.20415714933710077, 0.19422357952480057, -0.122348062792... |
1,803.05259 | Products and Projective Limits of Continuous Valuations on $T_0$ Spaces | We show analogues of the Daniell-Kolmogorov and Prohorov theorems on the
existence of projective limits of measures, in the setting of continuous
valuations on $T_0$ topological spaces.
| math.PR math.FA | we show analogues of the daniellkolmogorov and prohorov theorems on the existence of projective limits of measures in the setting of continuous valuations on t_0 topological spaces | [['we', 'show', 'analogues', 'of', 'the', 'daniellkolmogorov', 'and', 'prohorov', 'theorems', 'on', 'the', 'existence', 'of', 'projective', 'limits', 'of', 'measures', 'in', 'the', 'setting', 'of', 'continuous', 'valuations', 'on', 't_0', 'topological', 'spaces']] | [-0.170564873121643, 0.07360097996962185, -0.11369021844047193, 0.107831481557626, 0.027985396150213022, -0.013286845471996527, 0.09630897021494232, 0.3430777116893576, -0.25948306696059614, -0.13893980532884598, 0.14684188852641875, -0.27723240082223827, -0.08872632051889713, 0.3006096272997988, -0.16763192572845861, ... |
1,803.0526 | A Static Program Slicing Approach for Output Stream Objects in JEE
Applications | In this paper, we propose a program slicing approach for the output stream
object in JEE applications. Our approach is based on extracting a dependency
call graph from KDM models of JEE applications. Then, it applies breath-first
search algorithm to identify the program slice as a graph reachability problem.
The prop... | cs.SE | in this paper we propose a program slicing approach for the output stream object in jee applications our approach is based on extracting a dependency call graph from kdm models of jee applications then it applies breathfirst search algorithm to identify the program slice as a graph reachability problem the proposed app... | [['in', 'this', 'paper', 'we', 'propose', 'a', 'program', 'slicing', 'approach', 'for', 'the', 'output', 'stream', 'object', 'in', 'jee', 'applications', 'our', 'approach', 'is', 'based', 'on', 'extracting', 'a', 'dependency', 'call', 'graph', 'from', 'kdm', 'models', 'of', 'jee', 'applications', 'then', 'it', 'applies... | [-0.059709252292911213, -0.06731800218088514, -0.16925979000516236, 0.08103303257764007, -0.13731154163057605, -0.13398927621698628, 0.044820476977232224, 0.3690414793168505, -0.2774542851373553, -0.35110455219013, 0.12421685954323039, -0.22163189423736185, -0.21940585951476047, 0.22779672170290724, -0.1005924249184317... |
1,803.05261 | Subnanosecond magnetization reversal of magnetic nanoparticle driven by
chirp microwave field pulse | We investigate the magnetization reversal of single-domain magnetic
nanoparticle driven by linear down-chirp microwave magnetic field pulse.
Numerical simulations based on the Landau-Lifshitz-Gilbert equation reveal that
solely down-chirp pulse is capable of inducing subnanosecond magnetization
reversal. With a certa... | cond-mat.mes-hall | we investigate the magnetization reversal of singledomain magnetic nanoparticle driven by linear downchirp microwave magnetic field pulse numerical simulations based on the landaulifshitzgilbert equation reveal that solely downchirp pulse is capable of inducing subnanosecond magnetization reversal with a certain range ... | [['we', 'investigate', 'the', 'magnetization', 'reversal', 'of', 'singledomain', 'magnetic', 'nanoparticle', 'driven', 'by', 'linear', 'downchirp', 'microwave', 'magnetic', 'field', 'pulse', 'numerical', 'simulations', 'based', 'on', 'the', 'landaulifshitzgilbert', 'equation', 'reveal', 'that', 'solely', 'downchirp', '... | [-0.21344126902682625, 0.22063332731827953, -0.023494507001874887, 0.0015999288004620567, -0.109430428845403, -0.1130952884119166, 0.0414687512361485, 0.4132670178361561, -0.2717857893880295, -0.33410228383929835, 0.0470320067965709, -0.1877627449353104, -0.06148188059704135, 0.31547582723585, 0.05460386158007643, 0.00... |
1,803.05262 | Learning to Play General Video-Games via an Object Embedding Network | Deep reinforcement learning (DRL) has proven to be an effective tool for
creating general video-game AI. However most current DRL video-game agents
learn end-to-end from the video-output of the game, which is superfluous for
many applications and creates a number of additional problems. More
importantly, directly wor... | cs.LG cs.AI | deep reinforcement learning drl has proven to be an effective tool for creating general videogame ai however most current drl videogame agents learn endtoend from the videooutput of the game which is superfluous for many applications and creates a number of additional problems more importantly directly working on pixel... | [['deep', 'reinforcement', 'learning', 'drl', 'has', 'proven', 'to', 'be', 'an', 'effective', 'tool', 'for', 'creating', 'general', 'videogame', 'ai', 'however', 'most', 'current', 'drl', 'videogame', 'agents', 'learn', 'endtoend', 'from', 'the', 'videooutput', 'of', 'the', 'game', 'which', 'is', 'superfluous', 'for', ... | [-0.022482970220720176, 0.0094843826503508, -0.1274130273120502, 0.039741567249467306, -0.14024103425939072, -0.18853010354274824, 0.041582480137986315, 0.44130858863619243, -0.279462852183421, -0.3087280787612227, 0.028589976451045218, -0.2610600008674619, -0.18925398666798682, 0.19696659761686602, -0.1266756361447178... |
1,803.05263 | Feature Selective Small Object Detection via Knowledge-based Recurrent
Attentive Neural Network | At present, the performance of deep neural network in general object
detection is comparable to or even surpasses that of human beings. However, due
to the limitations of deep learning itself, the small proportion of feature
pixels, and the occurence of blur and occlusion, the detection of small objects
in complex sc... | cs.CV cs.AI | at present the performance of deep neural network in general object detection is comparable to or even surpasses that of human beings however due to the limitations of deep learning itself the small proportion of feature pixels and the occurence of blur and occlusion the detection of small objects in complex scenes is ... | [['at', 'present', 'the', 'performance', 'of', 'deep', 'neural', 'network', 'in', 'general', 'object', 'detection', 'is', 'comparable', 'to', 'or', 'even', 'surpasses', 'that', 'of', 'human', 'beings', 'however', 'due', 'to', 'the', 'limitations', 'of', 'deep', 'learning', 'itself', 'the', 'small', 'proportion', 'of', ... | [-0.07042323169796504, 0.02004151434812229, -0.07530679872488594, 0.029483774677852796, -0.125538184819245, -0.13873012925069877, 0.04150549680826299, 0.44310193182153496, -0.23061105688127445, -0.35866876830033123, 0.09311712646475909, -0.25443021137327115, -0.21919949841436576, 0.2209258586850595, -0.1797160873871874... |
1,803.05264 | Towards Almost Global Synchronization on the Stiefel Manifold | A graph $\mathcal{G}$ is referred to as $\mathsf{S}^1$-synchronizing if,
roughly speaking, the Kuramoto-like model whose interaction topology is given
by $\mathcal{G}$ synchronizes almost globally. The Kuramoto model evolves on
the unit circle, \ie the $1$-sphere $\mathsf{S}^1$. This paper concerns
generalizations of... | math.OC | a graph mathcalg is referred to as mathsfs1synchronizing if roughly speaking the kuramotolike model whose interaction topology is given by mathcalg synchronizes almost globally the kuramoto model evolves on the unit circle ie the 1sphere mathsfs1 this paper concerns generalizations of the kuramotolike model and the con... | [['a', 'graph', 'mathcalg', 'is', 'referred', 'to', 'as', 'mathsfs1synchronizing', 'if', 'roughly', 'speaking', 'the', 'kuramotolike', 'model', 'whose', 'interaction', 'topology', 'is', 'given', 'by', 'mathcalg', 'synchronizes', 'almost', 'globally', 'the', 'kuramoto', 'model', 'evolves', 'on', 'the', 'unit', 'circle',... | [-0.152853437698546, 0.08940321410274399, -0.05234404721164278, 0.03891745760338381, -0.09313901474400024, -0.1409688106871077, -0.026289676662833827, 0.38723264213352065, -0.2621700887002849, -0.26746338084340093, 0.13826697251227285, -0.28245775987161326, -0.1992933249283981, 0.19695819207201046, -0.1296812711774172,... |
1,803.05265 | Rotation-Sensitive Regression for Oriented Scene Text Detection | Text in natural images is of arbitrary orientations, requiring detection in
terms of oriented bounding boxes. Normally, a multi-oriented text detector
often involves two key tasks: 1) text presence detection, which is a
classification problem disregarding text orientation; 2) oriented bounding box
regression, which c... | cs.CV | text in natural images is of arbitrary orientations requiring detection in terms of oriented bounding boxes normally a multioriented text detector often involves two key tasks 1 text presence detection which is a classification problem disregarding text orientation 2 oriented bounding box regression which concerns abou... | [['text', 'in', 'natural', 'images', 'is', 'of', 'arbitrary', 'orientations', 'requiring', 'detection', 'in', 'terms', 'of', 'oriented', 'bounding', 'boxes', 'normally', 'a', 'multioriented', 'text', 'detector', 'often', 'involves', 'two', 'key', 'tasks', '1', 'text', 'presence', 'detection', 'which', 'is', 'a', 'class... | [-0.09365004266728646, -0.04566171473707072, -0.02506755264621461, 0.022898612778953976, -0.10729408669576515, -0.1965840168093564, -0.010086420294828712, 0.4294807720463723, -0.22821321053270366, -0.3529617074877024, 0.08749645999487257, -0.32998212928068826, -0.13736909271465264, 0.19414715868188068, -0.1678510476252... |
1,803.05266 | On the Applicability of Registration Uncertainty | Estimating the uncertainty in (probabilistic) image registration enables,
e.g., surgeons to assess the operative risk based on the trustworthiness of the
registered image data. If surgeons receive inaccurately calculated registration
uncertainty and misplace unwarranted confidence in the alignment solutions,
severe c... | cs.CV | estimating the uncertainty in probabilistic image registration enables eg surgeons to assess the operative risk based on the trustworthiness of the registered image data if surgeons receive inaccurately calculated registration uncertainty and misplace unwarranted confidence in the alignment solutions severe consequence... | [['estimating', 'the', 'uncertainty', 'in', 'probabilistic', 'image', 'registration', 'enables', 'eg', 'surgeons', 'to', 'assess', 'the', 'operative', 'risk', 'based', 'on', 'the', 'trustworthiness', 'of', 'the', 'registered', 'image', 'data', 'if', 'surgeons', 'receive', 'inaccurately', 'calculated', 'registration', '... | [-0.06951717629090126, 0.017329910916321915, -0.09939102753097276, 0.1324415401216935, -0.10619279686149886, -0.13491148740021427, 0.06660808607557556, 0.4118276718231341, -0.27105717697850196, -0.35839121658566664, 0.12985778398962627, -0.2858540312233593, -0.12235102953854948, 0.17323748148456533, -0.1560533000367947... |
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