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 |
|---|---|---|---|---|---|---|
1,803.05867 | Capturing Structure Implicitly from Time-Series having Limited Data | Scientific fields such as insider-threat detection and highway-safety
planning often lack sufficient amounts of time-series data to estimate
statistical models for the purpose of scientific discovery. Moreover, the
available limited data are quite noisy. This presents a major challenge when
estimating time-series mod... | stat.ML cs.LG | scientific fields such as insiderthreat detection and highwaysafety planning often lack sufficient amounts of timeseries data to estimate statistical models for the purpose of scientific discovery moreover the available limited data are quite noisy this presents a major challenge when estimating timeseries models that ... | [['scientific', 'fields', 'such', 'as', 'insiderthreat', 'detection', 'and', 'highwaysafety', 'planning', 'often', 'lack', 'sufficient', 'amounts', 'of', 'timeseries', 'data', 'to', 'estimate', 'statistical', 'models', 'for', 'the', 'purpose', 'of', 'scientific', 'discovery', 'moreover', 'the', 'available', 'limited', ... | [-0.026219216090227877, 0.020430790946286703, -0.08779423452913761, 0.14746168983606497, -0.17318756717124156, -0.1650686762987503, 0.05226217698172799, 0.4293959238646286, -0.30013893212457854, -0.3542175153802548, 0.1449899777543864, -0.2585707410212074, -0.13433577632165647, 0.18385656260885297, -0.12415595302358269... |
1,803.05868 | Free subgroups of $3$-manifold groups | We show that any closed hyperbolic $3$-manifold $M$ has a co-final tower of
covers $M_i \to M$ of degrees $n_i$ such that any subgroup of $\pi_1(M_i)$
generated by $k_i$ elements is free, where $k_i \ge n_i^C$ and $C = C(M) > 0$.
Together with this result we show that $\log k_i \geq C_1 sys_1(M_i)$, where
$sys_1(M_i)... | math.GR math.GT | we show that any closed hyperbolic 3manifold m has a cofinal tower of covers m_i to m of degrees n_i such that any subgroup of pi_1m_i generated by k_i elements is free where k_i ge n_ic and c cm 0 together with this result we show that log k_i geq c_1 sys_1m_i where sys_1m_i denotes the systole of m_i thus providing a... | [['we', 'show', 'that', 'any', 'closed', 'hyperbolic', '3manifold', 'm', 'has', 'a', 'cofinal', 'tower', 'of', 'covers', 'm_i', 'to', 'm', 'of', 'degrees', 'n_i', 'such', 'that', 'any', 'subgroup', 'of', 'pi_1m_i', 'generated', 'by', 'k_i', 'elements', 'is', 'free', 'where', 'k_i', 'ge', 'n_ic', 'and', 'c', 'cm', '0', ... | [-0.24644323590252062, 0.20156446528641897, -0.005659046689169886, -0.008605916203637405, -0.051157091880905566, -0.18627953116336596, 0.028993679610404954, 0.3371784122883464, -0.2709916102618951, -0.2586448791781035, 0.07096772785070757, -0.32465114942296286, -0.09278232162013529, 0.20361225453266146, -0.132312688242... |
1,803.05869 | Magneto-elastic switching of magnetostrictive nanomagnets with in-plane
shape anisotropy | We theoretically study the effect of a material defect (material void) on
switching errors associated with magneto-elastic switching of magnetization in
elliptical magnetostrictive nanomagnets having in-plane magnetic anisotropy. We
find that the error probability increases significantly in the presence of the
defect... | cond-mat.mes-hall | we theoretically study the effect of a material defect material void on switching errors associated with magnetoelastic switching of magnetization in elliptical magnetostrictive nanomagnets having inplane magnetic anisotropy we find that the error probability increases significantly in the presence of the defect indica... | [['we', 'theoretically', 'study', 'the', 'effect', 'of', 'a', 'material', 'defect', 'material', 'void', 'on', 'switching', 'errors', 'associated', 'with', 'magnetoelastic', 'switching', 'of', 'magnetization', 'in', 'elliptical', 'magnetostrictive', 'nanomagnets', 'having', 'inplane', 'magnetic', 'anisotropy', 'we', 'fi... | [-0.20788383563726162, 0.18431743077854526, 0.004020143468725554, 0.04629504027469282, -0.08711177621578388, -0.1442962327001101, 0.04696893798028852, 0.4101832272313165, -0.25263131752028956, -0.2996695682485687, 0.06802978682813089, -0.25467051698079873, -0.1363771040874355, 0.20102833550925372, -0.04698685907712537,... |
1,803.0587 | pH Sensing by Lipids in Membranes: The Fundamentals of pH-driven
Migration, Polarization and Deformations of Lipid Bilayer Assemblies | Most biological molecules contain acido-basic groups that modulate their
structure and interactions. A consequence is that pH gradients, local
heterogeneities and dynamic variations are used by cells and organisms to drive
or regulate specific biological functions including energetic metabolism,
vesicular traffic, mi... | physics.bio-ph cond-mat.soft q-bio.SC | most biological molecules contain acidobasic groups that modulate their structure and interactions a consequence is that ph gradients local heterogeneities and dynamic variations are used by cells and organisms to drive or regulate specific biological functions including energetic metabolism vesicular traffic migration... | [['most', 'biological', 'molecules', 'contain', 'acidobasic', 'groups', 'that', 'modulate', 'their', 'structure', 'and', 'interactions', 'a', 'consequence', 'is', 'that', 'ph', 'gradients', 'local', 'heterogeneities', 'and', 'dynamic', 'variations', 'are', 'used', 'by', 'cells', 'and', 'organisms', 'to', 'drive', 'or',... | [-0.1163251416049212, 0.16453075335756376, -0.010013518937466312, 0.05026974875345666, -0.018963805042732894, -0.0877545596631758, 0.001282678654223132, 0.41134395715466304, -0.28047076029705875, -0.2716071690472723, 0.06113169909714852, -0.23078467490928578, -0.2525552947179877, 0.13905890198942972, -0.060258198398068... |
1,803.05871 | Distributed Data Vending on Blockchain | Recent advances in blockchain technologies have provided exciting
opportunities for decentralized applications. Specifically, blockchain-based
smart contracts enable credible transactions without authorized third parties.
The attractive properties of smart contracts facilitate distributed data
vending, allowing for p... | cs.CR cs.LG | recent advances in blockchain technologies have provided exciting opportunities for decentralized applications specifically blockchainbased smart contracts enable credible transactions without authorized third parties the attractive properties of smart contracts facilitate distributed data vending allowing for propriet... | [['recent', 'advances', 'in', 'blockchain', 'technologies', 'have', 'provided', 'exciting', 'opportunities', 'for', 'decentralized', 'applications', 'specifically', 'blockchainbased', 'smart', 'contracts', 'enable', 'credible', 'transactions', 'without', 'authorized', 'third', 'parties', 'the', 'attractive', 'propertie... | [-0.1232165503115937, -0.03461991189673108, -0.07182920270388687, 0.040849724900059024, -0.12302340264007258, -0.17441960809290083, 0.15026130814897237, 0.4019215093911999, -0.33219006713343796, -0.33714700660865454, 0.15394272632220501, -0.3507240050532651, -0.10996878734470283, 0.21799249435438484, -0.127988270874794... |
1,803.05872 | Virtual CNN Branching: Efficient Feature Ensemble for Person
Re-Identification | In this paper we introduce an ensemble method for convolutional neural
network (CNN), called "virtual branching," which can be implemented with nearly
no additional parameters and computation on top of standard CNNs. We propose
our method in the context of person re-identification (re-ID). Our CNN model
consists of s... | cs.CV | in this paper we introduce an ensemble method for convolutional neural network cnn called virtual branching which can be implemented with nearly no additional parameters and computation on top of standard cnns we propose our method in the context of person reidentification reid our cnn model consists of shared bottom l... | [['in', 'this', 'paper', 'we', 'introduce', 'an', 'ensemble', 'method', 'for', 'convolutional', 'neural', 'network', 'cnn', 'called', 'virtual', 'branching', 'which', 'can', 'be', 'implemented', 'with', 'nearly', 'no', 'additional', 'parameters', 'and', 'computation', 'on', 'top', 'of', 'standard', 'cnns', 'we', 'propo... | [-0.09213808623424388, 0.020121854615395125, -0.016766785234352925, 0.006995089886941128, -0.049250607009402904, -0.231921671522095, -0.002675205349214935, 0.4606168298400882, -0.24724205958795265, -0.33518548873848375, 0.029430307054899185, -0.26149082681010094, -0.19021528092724152, 0.19359017613946103, -0.1435693417... |
1,803.05873 | Deep Structure Inference Network for Facial Action Unit Recognition | Facial expressions are combinations of basic components called Action Units
(AU). Recognizing AUs is key for developing general facial expression analysis.
In recent years, most efforts in automatic AU recognition have been dedicated
to learning combinations of local features and to exploiting correlations
between Ac... | cs.CV | facial expressions are combinations of basic components called action units au recognizing aus is key for developing general facial expression analysis in recent years most efforts in automatic au recognition have been dedicated to learning combinations of local features and to exploiting correlations between action un... | [['facial', 'expressions', 'are', 'combinations', 'of', 'basic', 'components', 'called', 'action', 'units', 'au', 'recognizing', 'aus', 'is', 'key', 'for', 'developing', 'general', 'facial', 'expression', 'analysis', 'in', 'recent', 'years', 'most', 'efforts', 'in', 'automatic', 'au', 'recognition', 'have', 'been', 'de... | [-0.06964853481776946, -0.015853184398956003, -0.05234693344352783, 0.01510295151337256, -0.06887289727996804, -0.18151267683051064, 0.0025521625200105188, 0.44390306298711657, -0.24622733705260882, -0.35748657778696674, 0.06597266990209279, -0.2710801733872004, -0.23054828444512282, 0.17226723063555835, -0.13358937960... |
1,803.05874 | Synthesizing geocodes to facilitate access to detailed geographical
information in large scale administrative data | We investigate whether generating synthetic data can be a viable strategy for
providing access to detailed geocoding information for external researchers,
without compromising the confidentiality of the units included in the database.
Our work was motivated by a recent project at the Institute for Employment
Research... | stat.AP stat.ME | we investigate whether generating synthetic data can be a viable strategy for providing access to detailed geocoding information for external researchers without compromising the confidentiality of the units included in the database our work was motivated by a recent project at the institute for employment research iab... | [['we', 'investigate', 'whether', 'generating', 'synthetic', 'data', 'can', 'be', 'a', 'viable', 'strategy', 'for', 'providing', 'access', 'to', 'detailed', 'geocoding', 'information', 'for', 'external', 'researchers', 'without', 'compromising', 'the', 'confidentiality', 'of', 'the', 'units', 'included', 'in', 'the', '... | [-0.07066910256814245, -0.007346900220432663, -0.0642510383361171, 0.09350931585543705, -0.12618280622886602, -0.15765755977440576, 0.12634852179633824, 0.3860952006242677, -0.2274483540600539, -0.3303321683984496, 0.14776795175098834, -0.30265281736450206, -0.08981923518768031, 0.22486502775975753, -0.1208177133943344... |
1,803.05875 | Maxiset point of view for signal detection in inverse problems | This paper extends the successful maxiset paradigm from function estimation
to signal detection in inverse problems. In this context, the maxisets do not
have the same shape compared to the classical estimation framework.
Nevertheless, we introduce a robustified version of these maxisets, allowing to
exhibit tail con... | math.ST stat.TH | this paper extends the successful maxiset paradigm from function estimation to signal detection in inverse problems in this context the maxisets do not have the same shape compared to the classical estimation framework nevertheless we introduce a robustified version of these maxisets allowing to exhibit tail conditions... | [['this', 'paper', 'extends', 'the', 'successful', 'maxiset', 'paradigm', 'from', 'function', 'estimation', 'to', 'signal', 'detection', 'in', 'inverse', 'problems', 'in', 'this', 'context', 'the', 'maxisets', 'do', 'not', 'have', 'the', 'same', 'shape', 'compared', 'to', 'the', 'classical', 'estimation', 'framework', ... | [-0.04039365743202242, 0.007531463187964012, -0.11725651266787088, 0.0848940752118572, -0.10958962799684907, -0.1311964341650971, 0.03562005372386369, 0.39655300387830444, -0.27193778794907936, -0.2977520424562196, 0.1278335826778361, -0.19257274136003671, -0.1798781464864133, 0.20021707264205554, -0.1481888951296269, ... |
1,803.05876 | Predictions of Angular Observables for $\bar{B}_s\to K^{\ast}\ell\ell$
and $\bar{B}\to \rho\ell\ell$ in Standard Model | Exclusive semileptonic decays based on $b\to s$ transitions have been
attracting a lot of attention as some angular observables deviate significantly
from the Standard Model (SM) predictions in specific $q^2$ bins. B meson decays
induced by other Flavor Changing Neutral Current (FCNC), $b\to d$, can also
offer a prob... | hep-ph hep-ex | exclusive semileptonic decays based on bto s transitions have been attracting a lot of attention as some angular observables deviate significantly from the standard model sm predictions in specific q2 bins b meson decays induced by other flavor changing neutral current fcnc bto d can also offer a probe to new physics w... | [['exclusive', 'semileptonic', 'decays', 'based', 'on', 'bto', 's', 'transitions', 'have', 'been', 'attracting', 'a', 'lot', 'of', 'attention', 'as', 'some', 'angular', 'observables', 'deviate', 'significantly', 'from', 'the', 'standard', 'model', 'sm', 'predictions', 'in', 'specific', 'q2', 'bins', 'b', 'meson', 'deca... | [-0.03864642609384094, 0.27175497413781324, -0.029850508048214385, 0.1055874580929636, -0.11337563193204706, -0.21647033849196723, 0.1086507518413156, 0.31170859920685406, -0.23004901120210158, -0.18143277811497205, -0.031775780062221724, -0.3758503010832384, 0.0017897574742492593, 0.11891292511355743, 0.08382637111744... |
1,803.05877 | Orientational alignment in Cavity Quantum Electrodynamics | We consider the orientational alignment of dipoles due to strong matter light
coupling, for a non-vanishing density of excitations. We compare various
approaches to this problem in the limit of large numbers of emitters, and show
that direct Monte Carlo integration, mean-field theory, and large deviation
methods matc... | cond-mat.mes-hall cond-mat.soft | we consider the orientational alignment of dipoles due to strong matter light coupling for a nonvanishing density of excitations we compare various approaches to this problem in the limit of large numbers of emitters and show that direct monte carlo integration meanfield theory and large deviation methods match exactly... | [['we', 'consider', 'the', 'orientational', 'alignment', 'of', 'dipoles', 'due', 'to', 'strong', 'matter', 'light', 'coupling', 'for', 'a', 'nonvanishing', 'density', 'of', 'excitations', 'we', 'compare', 'various', 'approaches', 'to', 'this', 'problem', 'in', 'the', 'limit', 'of', 'large', 'numbers', 'of', 'emitters',... | [-0.17677448705098656, 0.18047158250606857, -0.06464125496486939, 0.08181389614257442, 0.02412300647052308, -0.07732869911029241, 0.04726761842530957, 0.35946417736366043, -0.2285216260961322, -0.31690468061931953, 0.014618133654991207, -0.2907201747225901, -0.11797873673115879, 0.10029723327119597, 0.0354418151329683,... |
1,803.05878 | The Laplace transform of the lognormal distribution | We study the analytical properties of the Laplace transform of the lognormal
distribution. Two integral expressions for the analytic continuation of the
Laplace transform of the lognormal distribution are provided, one of which
takes the form of a Mellin-Barnes integral. As a corollary, we obtain an
integral expressi... | math.PR | we study the analytical properties of the laplace transform of the lognormal distribution two integral expressions for the analytic continuation of the laplace transform of the lognormal distribution are provided one of which takes the form of a mellinbarnes integral as a corollary we obtain an integral expression for ... | [['we', 'study', 'the', 'analytical', 'properties', 'of', 'the', 'laplace', 'transform', 'of', 'the', 'lognormal', 'distribution', 'two', 'integral', 'expressions', 'for', 'the', 'analytic', 'continuation', 'of', 'the', 'laplace', 'transform', 'of', 'the', 'lognormal', 'distribution', 'are', 'provided', 'one', 'of', 'w... | [-0.11814469531572495, 0.010482740007668885, -0.18988573380137005, 0.13558831306447525, -0.06474327253929985, -0.023809425805946097, 0.01902286794099312, 0.3558178558014333, -0.260359148396394, -0.22680702755370966, 0.09612242778642283, -0.2501283520205806, -0.1916305882175668, 0.22524918275527084, -0.01290255062317905... |
1,803.05879 | Capillary stress and structural relaxation in moist granular materials | We propose a theoretical framework to calculate capillary stresses in complex
mesoporous materials, such as moist sand, nanoporous hydrates, and drying
colloidal films. Molecular simulations are mapped onto a phase-field model of
the liquid-vapor mixture, whose inhomogeneous stress tensor is integrated over
Voronoi p... | cond-mat.soft physics.flu-dyn | we propose a theoretical framework to calculate capillary stresses in complex mesoporous materials such as moist sand nanoporous hydrates and drying colloidal films molecular simulations are mapped onto a phasefield model of the liquidvapor mixture whose inhomogeneous stress tensor is integrated over voronoi polyhedra ... | [['we', 'propose', 'a', 'theoretical', 'framework', 'to', 'calculate', 'capillary', 'stresses', 'in', 'complex', 'mesoporous', 'materials', 'such', 'as', 'moist', 'sand', 'nanoporous', 'hydrates', 'and', 'drying', 'colloidal', 'films', 'molecular', 'simulations', 'are', 'mapped', 'onto', 'a', 'phasefield', 'model', 'of... | [-0.060477503971021654, 0.22117243340001283, -0.10533253964792966, -0.024534719136606594, 0.028721740415067712, -0.1085233779070913, 0.008916818629600164, 0.4026118356566456, -0.24854366582139095, -0.2641871278909476, -0.009920209118417163, -0.2918390487005612, -0.20158381802835187, 0.10790249851577796, -0.025815496527... |
1,803.0588 | GossipGraD: Scalable Deep Learning using Gossip Communication based
Asynchronous Gradient Descent | In this paper, we present GossipGraD - a gossip communication protocol based
Stochastic Gradient Descent (SGD) algorithm for scaling Deep Learning (DL)
algorithms on large-scale systems. The salient features of GossipGraD are: 1)
reduction in overall communication complexity from {\Theta}(log(p)) for p
compute nodes ... | cs.DC cs.LG | in this paper we present gossipgrad a gossip communication protocol based stochastic gradient descent sgd algorithm for scaling deep learning dl algorithms on largescale systems the salient features of gossipgrad are 1 reduction in overall communication complexity from thetalogp for p compute nodes in wellstudied sgd t... | [['in', 'this', 'paper', 'we', 'present', 'gossipgrad', 'a', 'gossip', 'communication', 'protocol', 'based', 'stochastic', 'gradient', 'descent', 'sgd', 'algorithm', 'for', 'scaling', 'deep', 'learning', 'dl', 'algorithms', 'on', 'largescale', 'systems', 'the', 'salient', 'features', 'of', 'gossipgrad', 'are', '1', 're... | [-0.15204109140096955, -0.010926228981358156, -0.0003960331607806055, 0.04198431447549371, -0.05256465325158749, -0.23727055058622973, 0.08769756998882393, 0.46886400284878377, -0.2566543069944392, -0.41734082114985255, 0.0835709887925473, -0.2622956823650636, -0.15764786812875634, 0.22026950919902638, -0.1003270849304... |
1,803.05881 | Soft-Photon Corrections to $\bar{B} \to D \tau^{-} \bar{\nu}_{\tau}$
Relative to $\bar{B} \to D \mu^{-} \bar{\nu}_{\mu}$ | We evaluate long-distance electromagnetic (QED) contributions to $\bar{B}{}^0
\to D^+ \tau^{-} \bar{\nu}_{\tau}$ and $B^- \to D^0 \tau^{-} \bar{\nu}_{\tau}$
relative to $\bar{B}{}^0 \to D^+ \mu^{-} \bar{\nu}_{\mu}$ and $B^- \to D^0
\mu^{-} \bar{\nu}_{\mu}$, respectively, in the standard model. We point out
that the Q... | hep-ph hep-ex | we evaluate longdistance electromagnetic qed contributions to barb0 to d tau barnu_tau and b to d0 tau barnu_tau relative to barb0 to d mu barnu_mu and b to d0 mu barnu_mu respectively in the standard model we point out that the qed corrections to the ratios rd and rd0 are not negligible contrary to the expectation tha... | [['we', 'evaluate', 'longdistance', 'electromagnetic', 'qed', 'contributions', 'to', 'barb0', 'to', 'd', 'tau', 'barnu_tau', 'and', 'b', 'to', 'd0', 'tau', 'barnu_tau', 'relative', 'to', 'barb0', 'to', 'd', 'mu', 'barnu_mu', 'and', 'b', 'to', 'd0', 'mu', 'barnu_mu', 'respectively', 'in', 'the', 'standard', 'model', 'we... | [-0.07856555015468904, 0.24795696245654758, -0.017389419389707325, 0.10505576839410923, 0.013126607090842589, -0.12793299554130144, 0.09317616098024677, 0.3550993942581447, -0.19708735023654042, -0.2538139704116249, -0.04058496882640386, -0.37261006034152433, 0.019675246992074284, 0.15235296882219218, 0.040613310551682... |
1,803.05882 | Index one minimal surfaces in spherical space forms | We prove that orientable index one minimal surfaces in spherical space forms
with large fundamental group have genus at most two. This confirms a conjecture
of R. Schoen for an infinite class of 3-manifolds.
| math.DG | we prove that orientable index one minimal surfaces in spherical space forms with large fundamental group have genus at most two this confirms a conjecture of r schoen for an infinite class of 3manifolds | [['we', 'prove', 'that', 'orientable', 'index', 'one', 'minimal', 'surfaces', 'in', 'spherical', 'space', 'forms', 'with', 'large', 'fundamental', 'group', 'have', 'genus', 'at', 'most', 'two', 'this', 'confirms', 'a', 'conjecture', 'of', 'r', 'schoen', 'for', 'an', 'infinite', 'class', 'of', '3manifolds']] | [-0.22070754149599986, 0.1260651344718473, -0.09448493739096996, 0.07251746682381696, -0.06069504431284526, -0.19093019601560252, -0.07193042129716452, 0.31608839909655645, -0.2211714197011829, -0.3006805956144543, 0.08542017747223486, -0.28274760863004145, -0.14040039405432148, 0.24721037048627348, -0.1654476924022139... |
1,803.05883 | Monodromy of elliptic curve convolution, seven-point sheaves of
$G_2$-type and motives of Beauville type | We study the Tannakian properties of the category of perverse sheaves on
elliptic curves endowed with the convolution product. We establish that for
certain sheaves with unipotent local monodromy over seven points the
corresponding Tannaka group is isomorphic to $G_2$. This monodromy approach
generalizes a result of ... | math.AG | we study the tannakian properties of the category of perverse sheaves on elliptic curves endowed with the convolution product we establish that for certain sheaves with unipotent local monodromy over seven points the corresponding tannaka group is isomorphic to g_2 this monodromy approach generalizes a result of katz o... | [['we', 'study', 'the', 'tannakian', 'properties', 'of', 'the', 'category', 'of', 'perverse', 'sheaves', 'on', 'elliptic', 'curves', 'endowed', 'with', 'the', 'convolution', 'product', 'we', 'establish', 'that', 'for', 'certain', 'sheaves', 'with', 'unipotent', 'local', 'monodromy', 'over', 'seven', 'points', 'the', 'c... | [-0.24508221574188743, -0.00033385111362535936, -0.16110684447845475, 0.04348977823592875, -0.10783148012658367, -0.10184936528475802, -0.040986393644191994, 0.31238752930257163, -0.37186299034653875, -0.15846750611958446, 0.08577685793060198, -0.23706937562979635, -0.17042684017634782, 0.21020200217264842, -0.25378236... |
1,803.05884 | Lineshape-asymmetry elimination in weak atomic transitions driven by an
intense standing wave field | Owing to the ac-Stark effect, the lineshape of a weak optical transition in
an atomic beam can become significantly distorted, when driven by an intense
standing wave field. We use an Yb atomic beam to study the lineshape of the 6s2
1S0 -> 5d6s 3D1 transition, which is excited with light circulating in a
Fabry-Perot ... | physics.atom-ph | owing to the acstark effect the lineshape of a weak optical transition in an atomic beam can become significantly distorted when driven by an intense standing wave field we use an yb atomic beam to study the lineshape of the 6s2 1s0 5d6s 3d1 transition which is excited with light circulating in a fabryperot resonator w... | [['owing', 'to', 'the', 'acstark', 'effect', 'the', 'lineshape', 'of', 'a', 'weak', 'optical', 'transition', 'in', 'an', 'atomic', 'beam', 'can', 'become', 'significantly', 'distorted', 'when', 'driven', 'by', 'an', 'intense', 'standing', 'wave', 'field', 'we', 'use', 'an', 'yb', 'atomic', 'beam', 'to', 'study', 'the',... | [-0.17024719679664652, 0.2107567906646595, -0.034874808487736365, -0.007927305820472115, -0.023868501958945257, -0.13467582791451027, 0.01719938823953271, 0.4334345131435178, -0.2543049498715184, -0.21916751926553182, 0.010097176191100682, -0.31363607581112196, -0.06723049461883916, 0.18778328419747678, 0.0422209603050... |
1,803.05885 | Identifiability of dynamical networks with partial node measurements | Much recent research has dealt with the identifiability of a dynamical
network in which the node signals are connected by causal linear transfer
functions and are excited by known external excitation signals and/or unknown
noise signals. A major research question concerns the identifiability of the
whole network - to... | math.OC cs.SY | much recent research has dealt with the identifiability of a dynamical network in which the node signals are connected by causal linear transfer functions and are excited by known external excitation signals andor unknown noise signals a major research question concerns the identifiability of the whole network topology... | [['much', 'recent', 'research', 'has', 'dealt', 'with', 'the', 'identifiability', 'of', 'a', 'dynamical', 'network', 'in', 'which', 'the', 'node', 'signals', 'are', 'connected', 'by', 'causal', 'linear', 'transfer', 'functions', 'and', 'are', 'excited', 'by', 'known', 'external', 'excitation', 'signals', 'andor', 'unkn... | [-0.1674533752922504, 0.11887630566739907, -0.035626836646694, 0.04522264571260928, -0.08493475324312548, -0.15253879339364496, 0.05686345426881585, 0.39382150648775216, -0.2886286959007472, -0.29149611909667444, 0.11852577650950229, -0.30177515500899915, -0.17260044278830713, 0.15450358785086585, -0.030411599117504087... |
1,803.05886 | Universal quantum computing with parafermions assisted by a half fluxon | Braiding of anyons such as Majoranas or parafermions provides only Clifford
gates which do not form a universal set of quantum gates. We propose a robust
and resource-efficient scheme to perform a non-Clifford gate on a logical qudit
encoded in parafermionic zero modes via the Aharonov-Casher effect. This gate
can be... | quant-ph cond-mat.mes-hall | braiding of anyons such as majoranas or parafermions provides only clifford gates which do not form a universal set of quantum gates we propose a robust and resourceefficient scheme to perform a nonclifford gate on a logical qudit encoded in parafermionic zero modes via the aharonovcasher effect this gate can be implem... | [['braiding', 'of', 'anyons', 'such', 'as', 'majoranas', 'or', 'parafermions', 'provides', 'only', 'clifford', 'gates', 'which', 'do', 'not', 'form', 'a', 'universal', 'set', 'of', 'quantum', 'gates', 'we', 'propose', 'a', 'robust', 'and', 'resourceefficient', 'scheme', 'to', 'perform', 'a', 'nonclifford', 'gate', 'on'... | [-0.2222267750939223, 0.2644718104497321, -0.03354259785002386, 0.025380797046367864, -0.058360476148459066, -0.2618817911371851, 0.11748879840888549, 0.352182536897525, -0.2050466782734795, -0.27214915256037886, 0.030630817294979965, -0.21782081821871083, -0.0788733929635065, 0.213473914728113, -0.03564532938688784, 0... |
1,803.05887 | Coulomb-gas electrostatics controls large fluctuations of the KPZ
equation | We establish a large deviation principle for the Kardar-Parisi-Zhang (KPZ)
equation, providing precise control over the left tail of the height
distribution for narrow wedge initial condition. Our analysis exploits an exact
connection between the KPZ one-point distribution and the Airy point process --
an infinite pa... | cond-mat.stat-mech math-ph math.MP math.PR | we establish a large deviation principle for the kardarparisizhang kpz equation providing precise control over the left tail of the height distribution for narrow wedge initial condition our analysis exploits an exact connection between the kpz onepoint distribution and the airy point process an infinite particle coulo... | [['we', 'establish', 'a', 'large', 'deviation', 'principle', 'for', 'the', 'kardarparisizhang', 'kpz', 'equation', 'providing', 'precise', 'control', 'over', 'the', 'left', 'tail', 'of', 'the', 'height', 'distribution', 'for', 'narrow', 'wedge', 'initial', 'condition', 'our', 'analysis', 'exploits', 'an', 'exact', 'con... | [-0.055715276560326814, 0.03462202086426189, -0.11735959790728408, 0.06813690291886973, -0.061685800722470166, -0.14866891156122522, 0.03532088280754905, 0.2998332650156565, -0.27141657250128615, -0.2504135903278456, 0.05774999488014004, -0.2833072989749568, -0.13329675222873616, 0.166919828901741, -0.05210667043060824... |
1,803.05888 | A solvable problem in statistical mechanics: the dipole-type Hamiltonian
mean field model | The present study regards the zeroth order mean field approximation of a
dipole-type interaction model, which is analytically solved in the canonical
and microcanonical ensembles. After writing the canonical partition function,
the free and internal energies, magnetization and the specific heat are derived
and graphi... | cond-mat.stat-mech | the present study regards the zeroth order mean field approximation of a dipoletype interaction model which is analytically solved in the canonical and microcanonical ensembles after writing the canonical partition function the free and internal energies magnetization and the specific heat are derived and graphically r... | [['the', 'present', 'study', 'regards', 'the', 'zeroth', 'order', 'mean', 'field', 'approximation', 'of', 'a', 'dipoletype', 'interaction', 'model', 'which', 'is', 'analytically', 'solved', 'in', 'the', 'canonical', 'and', 'microcanonical', 'ensembles', 'after', 'writing', 'the', 'canonical', 'partition', 'function', '... | [-0.10831416664260192, 0.14452686591539532, -0.09124812439597231, 0.12383020550430733, 0.015135841282578756, -0.11639647438590016, 0.014570715149379887, 0.35317190344996596, -0.25182637465614066, -0.2697868221439421, 0.031236420964052408, -0.2882011961417596, -0.11508898384992641, 0.13962852498468925, 0.037701873892766... |
1,803.05889 | Using Automatic Refactoring to Improve Energy Efficiency of Android Apps | The ever-growing popularity of mobile phones has brought additional
challenges to the software development lifecycle. Mobile applications (apps,
for short) ought to provide the same set of features as conventional software,
with limited resources: such as, limited processing capabilities, storage,
screen and, not les... | cs.SE | the evergrowing popularity of mobile phones has brought additional challenges to the software development lifecycle mobile applications apps for short ought to provide the same set of features as conventional software with limited resources such as limited processing capabilities storage screen and not less important p... | [['the', 'evergrowing', 'popularity', 'of', 'mobile', 'phones', 'has', 'brought', 'additional', 'challenges', 'to', 'the', 'software', 'development', 'lifecycle', 'mobile', 'applications', 'apps', 'for', 'short', 'ought', 'to', 'provide', 'the', 'same', 'set', 'of', 'features', 'as', 'conventional', 'software', 'with',... | [-0.08684170750049196, 0.004597270258435214, -0.042140218479804294, 0.11170256799159124, -0.16914252343573138, -0.2048856837597365, 0.08428861123830975, 0.4299815823829394, -0.2535253957513171, -0.40832611254250356, 0.13967455071379076, -0.31364071822559186, -0.0665365445712769, 0.21788510361726057, -0.1367412818155374... |
1,803.0589 | Blow-up results for space-time fractional stochastic partial
differential equations | Consider non-linear time-fractional stochastic reaction-diffusion equations
of the following type, $$\partial^\beta_tu_t(x)=-\nu(-\Delta)^{\alpha/2}
u_t(x)+I^{1-\beta}_t[b(u)+ \sigma(u)\stackrel{\cdot}{F}(t,x)]$$ in $(d+1)$
dimensions, where $\nu>0, \beta\in (0,1)$, $\alpha\in (0,2]$. The operator
$\partial^\beta_t$ ... | math.PR math-ph math.AP math.MP | consider nonlinear timefractional stochastic reactiondiffusion equations of the following type partialbeta_tu_txnudeltaalpha2 u_txi1beta_tbu sigmaustackrelcdotftx in d1 dimensions where nu0 betain 01 alphain 02 the operator partialbeta_t is the caputo fractional derivative while deltaalpha2 is the generator of an isotr... | [['consider', 'nonlinear', 'timefractional', 'stochastic', 'reactiondiffusion', 'equations', 'of', 'the', 'following', 'type', 'partialbeta_tu_txnudeltaalpha2', 'u_txi1beta_tbu', 'sigmaustackrelcdotftx', 'in', 'd1', 'dimensions', 'where', 'nu0', 'betain', '01', 'alphain', '02', 'the', 'operator', 'partialbeta_t', 'is',... | [-0.14540726879885027, 0.11386470600587226, -0.026172976482685212, 0.047885762152255755, -0.08783437065788707, -0.18084125220775604, -0.038665516857365405, 0.3051513727036638, -0.2761320571336092, -0.1955639509347464, 0.1436306530013766, -0.3072210025862543, -0.14751414023339748, 0.14849983588920548, -0.119988312953314... |
1,803.05891 | Restoring Heisenberg scaling in noisy quantum metrology by monitoring
the environment | We study quantum frequency estimation for $N$ qubits subjected to independent
Markovian noise, via strategies based on time-continuous monitoring of the
environment. Both physical intuition and an extended convexity property of the
quantum Fisher information (QFI) suggest that these strategies are more
effective than... | quant-ph | we study quantum frequency estimation for n qubits subjected to independent markovian noise via strategies based on timecontinuous monitoring of the environment both physical intuition and an extended convexity property of the quantum fisher information qfi suggest that these strategies are more effective than the stan... | [['we', 'study', 'quantum', 'frequency', 'estimation', 'for', 'n', 'qubits', 'subjected', 'to', 'independent', 'markovian', 'noise', 'via', 'strategies', 'based', 'on', 'timecontinuous', 'monitoring', 'of', 'the', 'environment', 'both', 'physical', 'intuition', 'and', 'an', 'extended', 'convexity', 'property', 'of', 't... | [-0.10263641984170645, 0.1309317619214957, -0.09151109561507878, 0.06363896795051514, -0.022810746715174395, -0.19812140359873195, 0.07118062835996929, 0.40274566500614745, -0.23255917501130513, -0.25515037340909713, 0.12644805220235555, -0.24404327086212935, -0.13056159118866975, 0.250546468011492, -0.0787470030077344... |
1,803.05892 | Afterglow Imaging and Polarization of Misaligned Structured GRB Jets and
Cocoons: Breaking the Degeneracy in GRB 170817A | The X-ray to radio afterglow emission of GRB 170817A/GW 170817 so far scales
as $F_\nu\propto\nu^{-0.6}t^{0.8}$ with observed frequency and time, consistent
with a single power-law segment of the synchrotron spectrum from the external
shock going into the ambient medium. This requires the effective isotropic
equivale... | astro-ph.HE | the xray to radio afterglow emission of grb 170817agw 170817 so far scales as f_nuproptonu06t08 with observed frequency and time consistent with a single powerlaw segment of the synchrotron spectrum from the external shock going into the ambient medium this requires the effective isotropic equivalent afterglow shock en... | [['the', 'xray', 'to', 'radio', 'afterglow', 'emission', 'of', 'grb', '170817agw', '170817', 'so', 'far', 'scales', 'as', 'f_nuproptonu06t08', 'with', 'observed', 'frequency', 'and', 'time', 'consistent', 'with', 'a', 'single', 'powerlaw', 'segment', 'of', 'the', 'synchrotron', 'spectrum', 'from', 'the', 'external', 's... | [-0.05620857294386636, 0.15588643199720903, -0.07327720805639502, 0.08719182170197091, -0.09285458265161001, -0.14773173797337694, 0.00690118240397205, 0.4846655003296124, -0.26725709865530384, -0.31448318450694857, 0.051652491745364175, -0.28339891177047355, 0.01048839599943118, 0.20111084517700067, 0.0364588815159927... |
1,803.05893 | Altitude Terrain Guarding and Guarding Uni-Monotone Polygons | We present an optimal, linear-time algorithm for the following version of
terrain guarding: given a 1.5D terrain and a horizontal line, place the minimum
number of guards on the line to see all of the terrain. We prove that the
cardinality of the minimum guard set coincides with the cardinality of a
maximum number of... | cs.CG | we present an optimal lineartime algorithm for the following version of terrain guarding given a 15d terrain and a horizontal line place the minimum number of guards on the line to see all of the terrain we prove that the cardinality of the minimum guard set coincides with the cardinality of a maximum number of witness... | [['we', 'present', 'an', 'optimal', 'lineartime', 'algorithm', 'for', 'the', 'following', 'version', 'of', 'terrain', 'guarding', 'given', 'a', '15d', 'terrain', 'and', 'a', 'horizontal', 'line', 'place', 'the', 'minimum', 'number', 'of', 'guards', 'on', 'the', 'line', 'to', 'see', 'all', 'of', 'the', 'terrain', 'we', ... | [-0.19025056007145424, 0.07415202614171744, -0.043603155643693985, 0.01671699105322154, -0.10289668918971623, -0.1407037862864811, 0.09570395890142887, 0.3438582561858412, -0.2734370871136586, -0.29047032375080833, 0.147289515869315, -0.2637816664544747, -0.12932536310316728, 0.18590372426819707, -0.13639863955950926, ... |
1,803.05894 | The diagrammatic coaction and the algebraic structure of cut Feynman
integrals | We present a new formula for the coaction of a large class of integrals. When
applied to one-loop (cut) Feynman integrals, it can be given a diagrammatic
representation purely in terms of pinches and cuts of the edges of the graph.
The coaction encodes the algebraic structure of these integrals, and offers
ways to ex... | hep-th hep-ph | we present a new formula for the coaction of a large class of integrals when applied to oneloop cut feynman integrals it can be given a diagrammatic representation purely in terms of pinches and cuts of the edges of the graph the coaction encodes the algebraic structure of these integrals and offers ways to extract imp... | [['we', 'present', 'a', 'new', 'formula', 'for', 'the', 'coaction', 'of', 'a', 'large', 'class', 'of', 'integrals', 'when', 'applied', 'to', 'oneloop', 'cut', 'feynman', 'integrals', 'it', 'can', 'be', 'given', 'a', 'diagrammatic', 'representation', 'purely', 'in', 'terms', 'of', 'pinches', 'and', 'cuts', 'of', 'the', ... | [-0.15980810427324885, 0.05095327424598818, -0.16167871205215442, 0.10016807979170947, -0.16909556031385634, -0.06960739002146936, 0.06505626396578242, 0.31144103473250534, -0.2992634690624285, -0.2534222163735552, 0.041689977821388696, -0.2622043805870604, -0.19716380481568582, 0.20491919642750253, -0.0493663232575388... |
1,803.05895 | Weak Modular Zilber-Pink with Derivatives | In unpublished notes Pila proposed a Modular Zilber-Pink with Derivatives
(MZPD) conjecture, which is a Zilber-Pink type statement for the modular
$j$-function and its derivatives. In this article we define D-special
varieties, then state and prove two functional (differential) analogues of the
MZPD conjecture for th... | math.NT math.AG math.LO | in unpublished notes pila proposed a modular zilberpink with derivatives mzpd conjecture which is a zilberpink type statement for the modular jfunction and its derivatives in this article we define dspecial varieties then state and prove two functional differential analogues of the mzpd conjecture for those varieties i... | [['in', 'unpublished', 'notes', 'pila', 'proposed', 'a', 'modular', 'zilberpink', 'with', 'derivatives', 'mzpd', 'conjecture', 'which', 'is', 'a', 'zilberpink', 'type', 'statement', 'for', 'the', 'modular', 'jfunction', 'and', 'its', 'derivatives', 'in', 'this', 'article', 'we', 'define', 'dspecial', 'varieties', 'then... | [-0.14508113229368932, -0.04479574951545871, -0.15315425677288017, 0.1344166715223258, -0.10663567595463946, -0.11751567904620354, 0.005327397272081808, 0.22859211983789401, -0.2838947076098363, -0.23517571423286782, 0.13281150462098867, -0.23901841044951147, -0.21831006764021135, 0.23350061423537372, -0.16335472150152... |
1,803.05896 | Length in the Cremona group | The Cremona group is the group of birational transformations of the plane. A
birational transformation for which there exists a pencil of lines which is
sent onto another pencil of lines is called a Jonqui\`eres transformation. By
the famous Noether-Castelnuovo theorem, every birational transformation $f$ is
a produc... | math.AG | the cremona group is the group of birational transformations of the plane a birational transformation for which there exists a pencil of lines which is sent onto another pencil of lines is called a jonquieres transformation by the famous noethercastelnuovo theorem every birational transformation f is a product of jonqu... | [['the', 'cremona', 'group', 'is', 'the', 'group', 'of', 'birational', 'transformations', 'of', 'the', 'plane', 'a', 'birational', 'transformation', 'for', 'which', 'there', 'exists', 'a', 'pencil', 'of', 'lines', 'which', 'is', 'sent', 'onto', 'another', 'pencil', 'of', 'lines', 'is', 'called', 'a', 'jonquieres', 'tra... | [-0.19179368978209732, 0.10589202448397732, -0.11097678028344482, 0.026899200085914468, -0.09170319924538001, -0.10150848359051513, 0.007041300545708754, 0.35971484021205424, -0.3676948891952634, -0.20558463688548498, 0.10641794232211366, -0.2637209526181002, -0.15964330349532307, 0.21761571262922028, -0.08675218258173... |
1,803.05897 | Contrasting information theoretic decompositions of modulatory and
arithmetic interactions in neural information processing systems | Biological and artificial neural systems are composed of many local
processors, and their capabilities depend upon the transfer function that
relates each local processor's outputs to its inputs. This paper uses a recent
advance in the foundations of information theory to study the properties of
local processors that... | cs.IT math.IT q-bio.NC q-bio.QM stat.ML | biological and artificial neural systems are composed of many local processors and their capabilities depend upon the transfer function that relates each local processors outputs to its inputs this paper uses a recent advance in the foundations of information theory to study the properties of local processors that use ... | [['biological', 'and', 'artificial', 'neural', 'systems', 'are', 'composed', 'of', 'many', 'local', 'processors', 'and', 'their', 'capabilities', 'depend', 'upon', 'the', 'transfer', 'function', 'that', 'relates', 'each', 'local', 'processors', 'outputs', 'to', 'its', 'inputs', 'this', 'paper', 'uses', 'a', 'recent', '... | [-0.10373942477111187, 0.0957563756696052, -0.10632751901323596, 0.050794415082782506, -0.11409759129371701, -0.1517071739687688, 0.026113196038123634, 0.4017305547495683, -0.3047303976325525, -0.31098804866300067, 0.09123733534607001, -0.2583109679331796, -0.2239209063878904, 0.22472604248155323, -0.07598560910102808,... |
1,803.05898 | Effects of a subadiabatic layer on convection and dynamos in spherical
wedge simulations | We consider the effect of a subadiabatic layer at the base of the convection
zone on convection itself and the associated large-scale dynamos in spherical
wedge geometry. We use a heat conduction prescription based on the Kramers
opacity law which allows the depth of the convection zone to dynamically adapt
to change... | astro-ph.SR | we consider the effect of a subadiabatic layer at the base of the convection zone on convection itself and the associated largescale dynamos in spherical wedge geometry we use a heat conduction prescription based on the kramers opacity law which allows the depth of the convection zone to dynamically adapt to changes in... | [['we', 'consider', 'the', 'effect', 'of', 'a', 'subadiabatic', 'layer', 'at', 'the', 'base', 'of', 'the', 'convection', 'zone', 'on', 'convection', 'itself', 'and', 'the', 'associated', 'largescale', 'dynamos', 'in', 'spherical', 'wedge', 'geometry', 'we', 'use', 'a', 'heat', 'conduction', 'prescription', 'based', 'on... | [-0.15735026195761748, 0.1905693728738697, -0.002307735610520467, 0.05071289769548457, -0.07918909173167776, -0.014943476984626614, 0.11094186759728472, 0.31518773704301567, -0.3213332516461378, -0.29086004275595767, 0.07602166650540312, -0.22503018615798281, -0.09678668991546147, 0.17910780835954937, -0.02870141937364... |
1,803.05899 | Moduli spaces of $G_{2}$ and $Spin(7)-$instantons on product manifolds | Let $X$ be a closed $6-$dimensional manifold with a half-closed
$SU(3)-$structure. On the product manifold $X\times S^{1}$, with respect to the
product $G_{2}-$structure and on a pullback vector bundle from $X$, we show
that any $G_{2}-$instanton is equivalent to a Hermitian Yang-Mills connection
on $X$ via a "broken... | math.DG math.AG | let x be a closed 6dimensional manifold with a halfclosed su3structure on the product manifold xtimes s1 with respect to the product g_2structure and on a pullback vector bundle from x we show that any g_2instanton is equivalent to a hermitian yangmills connection on x via a broken gauge this result reveals the topolog... | [['let', 'x', 'be', 'a', 'closed', '6dimensional', 'manifold', 'with', 'a', 'halfclosed', 'su3structure', 'on', 'the', 'product', 'manifold', 'xtimes', 's1', 'with', 'respect', 'to', 'the', 'product', 'g_2structure', 'and', 'on', 'a', 'pullback', 'vector', 'bundle', 'from', 'x', 'we', 'show', 'that', 'any', 'g_2instant... | [-0.21817914148559794, 0.09330725341733341, -0.06598087018937804, 0.033879079832695426, -0.10419389418675565, -0.14997318441746757, -0.0010424488340504468, 0.38925949335098264, -0.228910608147271, -0.1591463119177206, 0.10963454806333175, -0.25994947005528957, -0.15907480443711391, 0.19811857042368503, -0.1444466214044... |
1,803.059 | Toolflows for Mapping Convolutional Neural Networks on FPGAs: A Survey
and Future Directions | In the past decade, Convolutional Neural Networks (CNNs) have demonstrated
state-of-the-art performance in various Artificial Intelligence tasks. To
accelerate the experimentation and development of CNNs, several software
frameworks have been released, primarily targeting power-hungry CPUs and GPUs.
In this context, ... | cs.CV cs.AR cs.LG | in the past decade convolutional neural networks cnns have demonstrated stateoftheart performance in various artificial intelligence tasks to accelerate the experimentation and development of cnns several software frameworks have been released primarily targeting powerhungry cpus and gpus in this context reconfigurable... | [['in', 'the', 'past', 'decade', 'convolutional', 'neural', 'networks', 'cnns', 'have', 'demonstrated', 'stateoftheart', 'performance', 'in', 'various', 'artificial', 'intelligence', 'tasks', 'to', 'accelerate', 'the', 'experimentation', 'and', 'development', 'of', 'cnns', 'several', 'software', 'frameworks', 'have', '... | [-0.12830939983737702, -0.03294841090468227, -0.055808136981073106, 0.012108177514267914, -0.0957577524422701, -0.1544302212081004, -0.00044121121424613586, 0.4665109264459593, -0.21566316924645756, -0.3603158358844486, 0.08733678890098256, -0.2278606773499426, -0.20404328584855963, 0.2512071179226041, -0.0865617652323... |
1,803.05901 | Neutrino tomography of the Earth | Cosmic-ray interactions with the nuclei of the Earth's atmosphere produce a
flux of neutrinos in all directions with energies extending above the TeV
scale. However, the Earth is not a fully transparent medium for neutrinos with
energies above a few TeV. At these energies, the charged-current
neutrino-nucleon cross s... | hep-ph astro-ph.HE | cosmicray interactions with the nuclei of the earths atmosphere produce a flux of neutrinos in all directions with energies extending above the tev scale however the earth is not a fully transparent medium for neutrinos with energies above a few tev at these energies the chargedcurrent neutrinonucleon cross section is ... | [['cosmicray', 'interactions', 'with', 'the', 'nuclei', 'of', 'the', 'earths', 'atmosphere', 'produce', 'a', 'flux', 'of', 'neutrinos', 'in', 'all', 'directions', 'with', 'energies', 'extending', 'above', 'the', 'tev', 'scale', 'however', 'the', 'earth', 'is', 'not', 'a', 'fully', 'transparent', 'medium', 'for', 'neutr... | [-0.04525594642048008, 0.24705753978261924, -0.04757270980580692, 0.14817328697581794, -0.08440689454402994, -0.04473123356634888, 0.028370509904069717, 0.36390323509626527, -0.23292698234904047, -0.35447041442909955, 0.05795430817924367, -0.33806136507248763, -0.011015405962426289, 0.21504369582615646, 0.0392958510612... |
1,803.05902 | Velocity-dependent Lyapunov exponents in many-body quantum,
semi-classical, and classical chaos | The exponential growth or decay with time of the out-of-time-order commutator
(OTOC) is one widely used diagnostic of many-body chaos in spatially-extended
systems. In studies of many-body classical chaos, it has been noted that one
can define a velocity-dependent Lyapunov exponent, $\lambda({\bf v})$, which is
the g... | cond-mat.stat-mech cond-mat.str-el hep-th nlin.CD quant-ph | the exponential growth or decay with time of the outoftimeorder commutator otoc is one widely used diagnostic of manybody chaos in spatiallyextended systems in studies of manybody classical chaos it has been noted that one can define a velocitydependent lyapunov exponent lambdabf v which is the growth or decay rate alo... | [['the', 'exponential', 'growth', 'or', 'decay', 'with', 'time', 'of', 'the', 'outoftimeorder', 'commutator', 'otoc', 'is', 'one', 'widely', 'used', 'diagnostic', 'of', 'manybody', 'chaos', 'in', 'spatiallyextended', 'systems', 'in', 'studies', 'of', 'manybody', 'classical', 'chaos', 'it', 'has', 'been', 'noted', 'that... | [-0.17835063577254892, 0.18169304427068086, -0.10456751458816638, 0.07838307051043186, -0.00786106335619167, -0.19501583858740312, -0.013245179652671754, 0.3147544639561182, -0.2911893274723249, -0.16980706730626038, 0.08426534481788847, -0.30395884541849766, -0.15382376013422858, 0.231090263988459, 0.01622753551769891... |
1,803.05903 | Local $\beta$-deformations and Yang-Baxter sigma model | Homogeneous Yang-Baxter (YB) deformation of AdS$_5\times$S$^5$ superstring is
revisited. We calculate the YB sigma model action up to quadratic order in
fermions and show that homogeneous YB deformations are equivalent to
$\beta$-deformations of the AdS$_5\times$S$^5$ background when the classical
$r$-matrices consis... | hep-th | homogeneous yangbaxter yb deformation of ads_5timess5 superstring is revisited we calculate the yb sigma model action up to quadratic order in fermions and show that homogeneous yb deformations are equivalent to betadeformations of the ads_5timess5 background when the classical rmatrices consist of bosonic generators i... | [['homogeneous', 'yangbaxter', 'yb', 'deformation', 'of', 'ads_5timess5', 'superstring', 'is', 'revisited', 'we', 'calculate', 'the', 'yb', 'sigma', 'model', 'action', 'up', 'to', 'quadratic', 'order', 'in', 'fermions', 'and', 'show', 'that', 'homogeneous', 'yb', 'deformations', 'are', 'equivalent', 'to', 'betadeformat... | [-0.12376303619350351, 0.12894185320894597, 0.001968638738617301, 0.11067235254911735, -0.09817892653010195, -0.1887981960261684, -0.010405441063330583, 0.3234814266666829, -0.2060875314775677, -0.19417604377921965, 0.04307181114286539, -0.32085059691841405, -0.17747424740255588, 0.1266927066063213, -0.0890965402858065... |
1,803.05904 | A generalization of the CHSH inequality self-testing maximally entangled
states of any local dimension | For every $d \geq 2$, we present a generalization of the CHSH inequality with
the property that maximal violation self-tests the maximally entangled state of
local dimension $d$. This is the first example of a family of inequalities with
this property. Moreover, we provide a conjecture for a family of inequalities
ge... | quant-ph | for every d geq 2 we present a generalization of the chsh inequality with the property that maximal violation selftests the maximally entangled state of local dimension d this is the first example of a family of inequalities with this property moreover we provide a conjecture for a family of inequalities generalizing t... | [['for', 'every', 'd', 'geq', '2', 'we', 'present', 'a', 'generalization', 'of', 'the', 'chsh', 'inequality', 'with', 'the', 'property', 'that', 'maximal', 'violation', 'selftests', 'the', 'maximally', 'entangled', 'state', 'of', 'local', 'dimension', 'd', 'this', 'is', 'the', 'first', 'example', 'of', 'a', 'family', '... | [-0.14595484997126015, 0.15493651569286546, -0.05471983883886578, 0.017149031449584885, 0.011182396003897203, -0.24948893238770517, 0.022910659809527483, 0.25646464554394816, -0.2352248443330222, -0.2794123703930923, 0.08191661185837608, -0.32322509059226734, -0.1231584241415592, 0.17881571599579554, -0.062673903001036... |
1,803.05905 | Critical behavior of the van der Waals bonded ferromagnet
Fe$_{3-x}$GeTe$_2$ | The critical properties of the single-crystalline van der Waals bonded
ferromagnet Fe$_{3-x}$GeTe$_2$ were investigated by bulk dc magnetization
around the paramagnetic (PM) to ferromagnetic (FM) phase transition. The
Fe$_{3-x}$GeTe$_2$ single crystals grown by self-flux method with Fe deficiency
$x \approx 0.36$ exh... | cond-mat.str-el | the critical properties of the singlecrystalline van der waals bonded ferromagnet fe_3xgete_2 were investigated by bulk dc magnetization around the paramagnetic pm to ferromagnetic fm phase transition the fe_3xgete_2 single crystals grown by selfflux method with fe deficiency x approx 036 exhibit bulk fm ordering below... | [['the', 'critical', 'properties', 'of', 'the', 'singlecrystalline', 'van', 'der', 'waals', 'bonded', 'ferromagnet', 'fe_3xgete_2', 'were', 'investigated', 'by', 'bulk', 'dc', 'magnetization', 'around', 'the', 'paramagnetic', 'pm', 'to', 'ferromagnetic', 'fm', 'phase', 'transition', 'the', 'fe_3xgete_2', 'single', 'cry... | [-0.14541494419052248, 0.2403035519789543, -0.03104891860293348, -0.01960912625583326, 0.0015932770127582612, -0.2246938911884339, 0.13468374420023924, 0.34404678193481675, -0.21550094996987634, -0.3110089646105902, -0.01018253533521249, -0.396403645576282, -0.053401810880892964, 0.1925867695399389, 0.13152200542390347... |
1,803.05906 | A note on submanifolds of $\bar{M}^{2n+1}(f_1,f_2,f_3)$ with respect to
certain connections | The present paper deals with some results of almsot semi-invariant
submanifolds of generalized Sasakian-space-forms in \cite{ALEGRE3} with respect
to semisymmetric metric connection, semisymmetric non-metric connection,
Schouten-van Kampen connection and Tanaka-Webster connection.
| math.DG | the present paper deals with some results of almsot semiinvariant submanifolds of generalized sasakianspaceforms in citealegre3 with respect to semisymmetric metric connection semisymmetric nonmetric connection schoutenvan kampen connection and tanakawebster connection | [['the', 'present', 'paper', 'deals', 'with', 'some', 'results', 'of', 'almsot', 'semiinvariant', 'submanifolds', 'of', 'generalized', 'sasakianspaceforms', 'in', 'citealegre3', 'with', 'respect', 'to', 'semisymmetric', 'metric', 'connection', 'semisymmetric', 'nonmetric', 'connection', 'schoutenvan', 'kampen', 'connec... | [-0.3203353024698023, 0.040201434102872836, -0.031742232498423804, 0.14196303024374204, -0.2692305190039092, -0.19958492464803415, -0.0931006323843231, 0.4171470758216134, -0.22695879573965894, -0.2151721402428691, 0.048246115779279376, -0.3357426534760101, -0.3311306073747832, 0.046816015704374374, -0.2587078107071334... |
1,803.05907 | Water transport on infinite graphs | If the nodes of a graph are considered to be identical barrels - featuring
different water levels - and the edges to be (locked) water-filled pipes in
between the barrels, consider the optimization problem of how much the water
level in a fixed barrel can be raised with no pumps available, i.e. by opening
and closing... | math.PR | if the nodes of a graph are considered to be identical barrels featuring different water levels and the edges to be locked waterfilled pipes in between the barrels consider the optimization problem of how much the water level in a fixed barrel can be raised with no pumps available ie by opening and closing the locks in... | [['if', 'the', 'nodes', 'of', 'a', 'graph', 'are', 'considered', 'to', 'be', 'identical', 'barrels', 'featuring', 'different', 'water', 'levels', 'and', 'the', 'edges', 'to', 'be', 'locked', 'waterfilled', 'pipes', 'in', 'between', 'the', 'barrels', 'consider', 'the', 'optimization', 'problem', 'of', 'how', 'much', 'th... | [-0.14606043325767407, 0.17406103439932893, -0.02283068397650268, 0.026021405522183565, -0.043859105653742826, -0.18598700955707004, 0.08657874521322367, 0.3728537344775064, -0.2795364473741956, -0.2826273484643912, 0.11961391333176384, -0.30074016548072297, -0.08267591586734009, 0.11284862384124379, -0.057043027630590... |
1,803.05908 | Singular limit of BSDEs and Optimal control of two scale stochastic
systems in infinite dimensional spaces | In this paper we study by probabilistic techniques the convergence of the
value function for a two-scale, infinite-dimensional, stochastic controlled
system as the ratio between the two evolution speeds diverges. The value
function is represented as the solution of a \textit{backward stochastic
differential equation}... | math.OC | in this paper we study by probabilistic techniques the convergence of the value function for a twoscale infinitedimensional stochastic controlled system as the ratio between the two evolution speeds diverges the value function is represented as the solution of a textitbackward stochastic differential equation bsde that... | [['in', 'this', 'paper', 'we', 'study', 'by', 'probabilistic', 'techniques', 'the', 'convergence', 'of', 'the', 'value', 'function', 'for', 'a', 'twoscale', 'infinitedimensional', 'stochastic', 'controlled', 'system', 'as', 'the', 'ratio', 'between', 'the', 'two', 'evolution', 'speeds', 'diverges', 'the', 'value', 'fun... | [-0.14966404995868435, 0.05995783757713103, -0.09742008472859927, 0.0782612672553876, -0.07920352846954588, -0.09979960684840744, 0.02107486670085875, 0.2980411604113944, -0.3694638493428896, -0.23522785668437546, 0.1537640650079141, -0.26607005277581447, -0.13707924376006936, 0.18983694797734152, -0.089433802681326, 0... |
1,803.05909 | Efficient Hardware Realization of Convolutional Neural Networks using
Intra-Kernel Regular Pruning | The recent trend toward increasingly deep convolutional neural networks
(CNNs) leads to a higher demand of computational power and memory storage.
Consequently, the deployment of CNNs in hardware has become more challenging.
In this paper, we propose an Intra-Kernel Regular (IKR) pruning scheme to
reduce the size and... | cs.CV | the recent trend toward increasingly deep convolutional neural networks cnns leads to a higher demand of computational power and memory storage consequently the deployment of cnns in hardware has become more challenging in this paper we propose an intrakernel regular ikr pruning scheme to reduce the size and computatio... | [['the', 'recent', 'trend', 'toward', 'increasingly', 'deep', 'convolutional', 'neural', 'networks', 'cnns', 'leads', 'to', 'a', 'higher', 'demand', 'of', 'computational', 'power', 'and', 'memory', 'storage', 'consequently', 'the', 'deployment', 'of', 'cnns', 'in', 'hardware', 'has', 'become', 'more', 'challenging', 'i... | [-0.10222889307481628, 0.03583069037872902, -0.022557991813589758, 0.022203716916188807, -0.07034423166590038, -0.19875305692586942, 0.07659444812180422, 0.43214623790199513, -0.26187297078632865, -0.33990024324402074, 0.08072816886912997, -0.25764090456851874, -0.16770751978853873, 0.20469460612876672, -0.158412123355... |
1,803.0591 | Combining the color structures and intersection points of thick center
vortices and low-lying Dirac modes | We investigate several examples of Yang-Mills gauge configurations containing
center vortex structures, including intersection points between vortices and
nontrivial color structures residing on the vortex world-surfaces. Various
topological charge contributions of the color structures and intersection
points are stu... | hep-lat | we investigate several examples of yangmills gauge configurations containing center vortex structures including intersection points between vortices and nontrivial color structures residing on the vortex worldsurfaces various topological charge contributions of the color structures and intersection points are studied i... | [['we', 'investigate', 'several', 'examples', 'of', 'yangmills', 'gauge', 'configurations', 'containing', 'center', 'vortex', 'structures', 'including', 'intersection', 'points', 'between', 'vortices', 'and', 'nontrivial', 'color', 'structures', 'residing', 'on', 'the', 'vortex', 'worldsurfaces', 'various', 'topologica... | [-0.23714046238455921, 0.20523376660832368, -0.03150345420684008, 0.10651439872077283, -0.01624355121748522, -0.04298936193534995, -0.017038843717754763, 0.39617199149421034, -0.1861268968992483, -0.24824460621868424, 0.05188570362310309, -0.3126374549670693, -0.15203283539877327, 0.08333582176333841, 0.034325940534472... |
1,803.05911 | The solution of the Einstein equation in the interior of the black holes
by using arbitrary distribution functions | The aim of this paper is to obtain the solution of the Einstein equation in
the interior of the black holes by using arbitrary distribution functions;
corresponding to Gaussian, Rayleigh, Maxwell-Boltzmann and non-Gaussian
distributions. Also we calculate the Hawking temperature, the mass and heat
capacity for cosmol... | gr-qc hep-th | the aim of this paper is to obtain the solution of the einstein equation in the interior of the black holes by using arbitrary distribution functions corresponding to gaussian rayleigh maxwellboltzmann and nongaussian distributions also we calculate the hawking temperature the mass and heat capacity for cosmological ho... | [['the', 'aim', 'of', 'this', 'paper', 'is', 'to', 'obtain', 'the', 'solution', 'of', 'the', 'einstein', 'equation', 'in', 'the', 'interior', 'of', 'the', 'black', 'holes', 'by', 'using', 'arbitrary', 'distribution', 'functions', 'corresponding', 'to', 'gaussian', 'rayleigh', 'maxwellboltzmann', 'and', 'nongaussian', '... | [-0.09915032420518263, 0.08199280639890721, -0.12443834012550004, 0.1459707453636066, -0.06187147177088092, -0.09965141688666816, 0.02190615175476403, 0.26756024972166653, -0.2030931217771656, -0.2631777780798246, 0.11455192362213121, -0.33045710426456526, -0.04583805071559014, 0.17800125795996413, -0.04388716244050916... |
1,803.05912 | The redshift evolution of rest-UV spectroscopic properties in Lyman
Break Galaxies at z ~ 2-4 | We present the first comprehensive evolutionary analysis of the rest-frame UV
spectroscopic properties of star-forming galaxies at z ~ 2-4. We match samples
at different redshifts in UV luminosity and stellar mass, and perform
systematic measurements of spectral features and stellar population modeling.
By creating c... | astro-ph.GA | we present the first comprehensive evolutionary analysis of the restframe uv spectroscopic properties of starforming galaxies at z 24 we match samples at different redshifts in uv luminosity and stellar mass and perform systematic measurements of spectral features and stellar population modeling by creating composite s... | [['we', 'present', 'the', 'first', 'comprehensive', 'evolutionary', 'analysis', 'of', 'the', 'restframe', 'uv', 'spectroscopic', 'properties', 'of', 'starforming', 'galaxies', 'at', 'z', '24', 'we', 'match', 'samples', 'at', 'different', 'redshifts', 'in', 'uv', 'luminosity', 'and', 'stellar', 'mass', 'and', 'perform',... | [0.0090057255406864, 0.08310915234871209, 0.013000742541626096, 0.13873094889707863, -0.045573354247026146, -0.08180206734128297, 0.04456146734487265, 0.5299055221527815, -0.1309834906682372, -0.34940374916233125, -0.03996963651664555, -0.3160261807460338, 0.017939900916069746, 0.1479602375170216, 0.04131957107991911, ... |
1,803.05913 | Linear stability analysis of collective neutrino oscillations without
spurious modes | Collective neutrino oscillations are induced by the presence of neutrinos
themselves. As such they are intrinsically nonlinear phenomena and are much
more complex than linear counterparts such as the vacuum or MSW oscillations.
They obey integro-differential equations, numerical solutions of which are also
very chall... | hep-ph astro-ph.HE | collective neutrino oscillations are induced by the presence of neutrinos themselves as such they are intrinsically nonlinear phenomena and are much more complex than linear counterparts such as the vacuum or msw oscillations they obey integrodifferential equations numerical solutions of which are also very challenging... | [['collective', 'neutrino', 'oscillations', 'are', 'induced', 'by', 'the', 'presence', 'of', 'neutrinos', 'themselves', 'as', 'such', 'they', 'are', 'intrinsically', 'nonlinear', 'phenomena', 'and', 'are', 'much', 'more', 'complex', 'than', 'linear', 'counterparts', 'such', 'as', 'the', 'vacuum', 'or', 'msw', 'oscillat... | [-0.1072787270920856, 0.1257781712936302, -0.11226824145047286, 0.11730443069245666, -0.1060689074944063, -0.10883761875276618, -0.00014382377002748246, 0.32602199507845925, -0.27870285028015546, -0.2778556560784453, 0.12128464868116122, -0.285069123921552, -0.20068406712013384, 0.20370233108919553, -0.0365687078393275... |
1,803.05914 | Molecular Emission from a Galaxy Associated with a z~2.2 Damped
Lyman-alpha Absorber | Using the Atacama Large Millimeter/sub-millimeter Array, we have detected
CO(3-2) line and far-infrared continuum emission from a galaxy associated with
a high-metallicity ([M/H] = -0.27) damped Ly-alpha absorber (DLA) at z
=2.19289. The galaxy is located 3.5" away from the quasar sightline,
corresponding to a large ... | astro-ph.GA | using the atacama large millimetersubmillimeter array we have detected co32 line and farinfrared continuum emission from a galaxy associated with a highmetallicity mh 027 damped lyalpha absorber dla at z 219289 the galaxy is located 35 away from the quasar sightline corresponding to a large impact parameter of 30 kpc a... | [['using', 'the', 'atacama', 'large', 'millimetersubmillimeter', 'array', 'we', 'have', 'detected', 'co32', 'line', 'and', 'farinfrared', 'continuum', 'emission', 'from', 'a', 'galaxy', 'associated', 'with', 'a', 'highmetallicity', 'mh', '027', 'damped', 'lyalpha', 'absorber', 'dla', 'at', 'z', '219289', 'the', 'galaxy... | [-0.0633194461417868, 0.08885677558176903, 0.03278146874115794, 0.04124956163498135, -0.08111171381603767, -0.07980498354573551, 0.0566858906387431, 0.4619244875179397, -0.10319605327617282, -0.3174842023688695, 0.016355728597726483, -0.3507630435439448, 0.03984354988723579, 0.1532158172633658, 0.06264916052803016, -0.... |
1,803.05915 | Characterization of the Infrared/X-ray sub-second variability for the
black-hole transient GX 339-4 | We present a detailed analysis of the X-ray/IR fast variability of the
Black-Hole Transient GX 339-4 during its low/hard state in August 2008. Thanks
to simultaneous high time-resolution observations made with the VLT and RXTE,
we performed the first characterisation of the sub-second variability in the
near-infrared... | astro-ph.HE | we present a detailed analysis of the xrayir fast variability of the blackhole transient gx 3394 during its lowhard state in august 2008 thanks to simultaneous high timeresolution observations made with the vlt and rxte we performed the first characterisation of the subsecond variability in the nearinfrared band and of... | [['we', 'present', 'a', 'detailed', 'analysis', 'of', 'the', 'xrayir', 'fast', 'variability', 'of', 'the', 'blackhole', 'transient', 'gx', '3394', 'during', 'its', 'lowhard', 'state', 'in', 'august', '2008', 'thanks', 'to', 'simultaneous', 'high', 'timeresolution', 'observations', 'made', 'with', 'the', 'vlt', 'and', '... | [-0.06893926414757141, 0.11940847329284854, -0.0895766844277194, 0.09758000238119093, -0.07320022515559402, -0.09720132567155164, 0.07051473039434317, 0.47129050105563747, -0.2217652518429036, -0.3242822038743587, 0.11393227217744326, -0.2983255310614633, -0.025956377845460454, 0.22756376768940706, -0.0067239851112829,... |
1,803.05916 | Extended Gauge Theory Deformations From~Flux~Backgrounds | We consider supersymmetric deformations of gauge theories in various
dimensions obtained from a String Theory realisation of branes embedded in flux
backgrounds. In particular we obtain deformations which take the form of Wilson
line defects, where the R-symmetry is twisted into the gauge symmetry.
Furthermore we con... | hep-th | we consider supersymmetric deformations of gauge theories in various dimensions obtained from a string theory realisation of branes embedded in flux backgrounds in particular we obtain deformations which take the form of wilson line defects where the rsymmetry is twisted into the gauge symmetry furthermore we construct... | [['we', 'consider', 'supersymmetric', 'deformations', 'of', 'gauge', 'theories', 'in', 'various', 'dimensions', 'obtained', 'from', 'a', 'string', 'theory', 'realisation', 'of', 'branes', 'embedded', 'in', 'flux', 'backgrounds', 'in', 'particular', 'we', 'obtain', 'deformations', 'which', 'take', 'the', 'form', 'of', '... | [-0.18421205634843896, 0.18290031444507115, -0.026044506770135326, 0.10484038088223756, -0.04884506731689202, -0.1466679992577569, -0.06383632058030785, 0.36157270186496054, -0.15876990353519266, -0.2210138182466229, 0.09024715612141529, -0.24880867681085048, -0.1757308388072433, 0.0760028875277688, -0.0697314319849917... |
1,803.05917 | The Telltale Heartbeat: Detection and Characterization of Eccentric
Orbiting Planets via Tides on their Host Star | We present an analytic description of tides raised on a star by a small
orbiting body. In particular, we highlight the disproportionate effect of
eccentricity and thus the scope for using these tides to detect and
characterise the orbits of exoplanets and brown dwarfs. The tidal distortions
of the star produced by an... | astro-ph.EP astro-ph.IM astro-ph.SR | we present an analytic description of tides raised on a star by a small orbiting body in particular we highlight the disproportionate effect of eccentricity and thus the scope for using these tides to detect and characterise the orbits of exoplanets and brown dwarfs the tidal distortions of the star produced by an ecce... | [['we', 'present', 'an', 'analytic', 'description', 'of', 'tides', 'raised', 'on', 'a', 'star', 'by', 'a', 'small', 'orbiting', 'body', 'in', 'particular', 'we', 'highlight', 'the', 'disproportionate', 'effect', 'of', 'eccentricity', 'and', 'thus', 'the', 'scope', 'for', 'using', 'these', 'tides', 'to', 'detect', 'and'... | [-0.12532438272108648, 0.12971415847565176, -0.09370408216062442, 0.10073760731565447, -0.14863901145413125, -0.051910731474268494, 0.031056636915309355, 0.38876352034582706, -0.21000900743896828, -0.33095701176697684, 0.10748263292388353, -0.25918682418935196, -0.1030218200329201, 0.2849698763671576, -0.10187467276792... |
1,803.05918 | Spectroscopic Follow-Up of the Hercules Aquila Cloud | We designed a follow-up program to find the spectroscopic properties of the
Hercules-Aquila Cloud (HAC) and test scenarios for its formation. We measured
the radial velocities (RVs) of 45 RR Lyrae in the southern portion of the HAC
using the facilities at the MDM observatory, producing the first large sample
of veloc... | astro-ph.GA | we designed a followup program to find the spectroscopic properties of the herculesaquila cloud hac and test scenarios for its formation we measured the radial velocities rvs of 45 rr lyrae in the southern portion of the hac using the facilities at the mdm observatory producing the first large sample of velocities in t... | [['we', 'designed', 'a', 'followup', 'program', 'to', 'find', 'the', 'spectroscopic', 'properties', 'of', 'the', 'herculesaquila', 'cloud', 'hac', 'and', 'test', 'scenarios', 'for', 'its', 'formation', 'we', 'measured', 'the', 'radial', 'velocities', 'rvs', 'of', '45', 'rr', 'lyrae', 'in', 'the', 'southern', 'portion',... | [-0.10284222203224679, 0.09358902866207405, -0.12347499739707393, 0.06838551687199951, -0.097300773009877, -0.042498333453584246, 0.0394624045728158, 0.4204333254519631, -0.23178648517521866, -0.31108857969589093, 0.04110242629848311, -0.2783423012951115, -0.04143255396663924, 0.19330476289683515, -0.023418718258685925... |
1,803.05919 | Capturing near-equilibrium solutions: a comparison between high-order
discontinuous Galerkin methods and well-balanced schemes | Equilibrium or stationary solutions usually proceed through the exact balance
between hyperbolic transport terms and source terms. Such equilibrium solutions
are affected by truncation errors that prevent any classical numerical scheme
from capturing the evolution of small amplitude waves of physical significance.
In... | math.NA astro-ph.IM cs.NA | equilibrium or stationary solutions usually proceed through the exact balance between hyperbolic transport terms and source terms such equilibrium solutions are affected by truncation errors that prevent any classical numerical scheme from capturing the evolution of small amplitude waves of physical significance in ord... | [['equilibrium', 'or', 'stationary', 'solutions', 'usually', 'proceed', 'through', 'the', 'exact', 'balance', 'between', 'hyperbolic', 'transport', 'terms', 'and', 'source', 'terms', 'such', 'equilibrium', 'solutions', 'are', 'affected', 'by', 'truncation', 'errors', 'that', 'prevent', 'any', 'classical', 'numerical', ... | [-0.10724813094192713, 0.036554936839623936, -0.09458957752842154, 0.09444489952324689, -0.042372095129591086, -0.12382076509380273, 0.08036854795677387, 0.3467320604879107, -0.2730949548029064, -0.31091575731988996, 0.13850937809911557, -0.2447456154607337, -0.14332044270909014, 0.16569612134166212, -0.037570602701020... |
1,803.0592 | On the quantum entropy function in 4d gauged supergravity | We analyze BPS black hole attractors in the conformal 4d gauged supergravity
formalism and apply the technique known as supergravity localization in order
to evaluate Sen's quantum entropy function in the
$\mathrm{AdS}_2\!\times\!\mathrm{S}^2$ near-horizon geometry. Under certain
assumptions, we reduce the exact expr... | hep-th | we analyze bps black hole attractors in the conformal 4d gauged supergravity formalism and apply the technique known as supergravity localization in order to evaluate sens quantum entropy function in the mathrmads_2timesmathrms2 nearhorizon geometry under certain assumptions we reduce the exact expression of the functi... | [['we', 'analyze', 'bps', 'black', 'hole', 'attractors', 'in', 'the', 'conformal', '4d', 'gauged', 'supergravity', 'formalism', 'and', 'apply', 'the', 'technique', 'known', 'as', 'supergravity', 'localization', 'in', 'order', 'to', 'evaluate', 'sens', 'quantum', 'entropy', 'function', 'in', 'the', 'mathrmads_2timesmath... | [-0.10003000677047337, 0.05456082298005378, -0.03502583827675997, 0.18821009110471756, -0.07184422231889029, -0.16194978062559268, 0.0006410021128856557, 0.24764508633747054, -0.09852684248010997, -0.2567619050303541, 0.11737052257769078, -0.30929084538261026, -0.20013988736963315, 0.15118895223860046, -0.1066737232135... |
1,803.05921 | Thermodynamics of bosonic systems in adS spacetime | We analyze the thermodynamics of massless bosonic systems in D-dimensional
anti-de Sitter spacetime, considering scalar, electromagnetic, and
gravitational fields. Their dynamics are described by Poschl-Teller effective
potentials and quantized in a unified framework, with the determination of the
associated energy s... | hep-th cond-mat.stat-mech gr-qc | we analyze the thermodynamics of massless bosonic systems in ddimensional antide sitter spacetime considering scalar electromagnetic and gravitational fields their dynamics are described by poschlteller effective potentials and quantized in a unified framework with the determination of the associated energy spectra fro... | [['we', 'analyze', 'the', 'thermodynamics', 'of', 'massless', 'bosonic', 'systems', 'in', 'ddimensional', 'antide', 'sitter', 'spacetime', 'considering', 'scalar', 'electromagnetic', 'and', 'gravitational', 'fields', 'their', 'dynamics', 'are', 'described', 'by', 'poschlteller', 'effective', 'potentials', 'and', 'quant... | [-0.1432046430070222, 0.18981273039187108, -0.07388707228753831, 0.09167398855488594, -0.01728714601684016, -0.1305343625039707, -0.03295884005360536, 0.2745946808430107, -0.155043680225643, -0.24616921679644854, 0.03677642595181338, -0.2678737028204289, -0.1232540739493771, 0.1623293582503636, -0.007275800446298011, 0... |
1,803.05922 | Lithium abundance patterns of late-F stars: an in-depth analysis of the
lithium desert | We address the existence and origin of the lithium (Li) desert, a region in
the Li - T_eff plane sparsely populated by stars. Here we analyze some of the
explanations that have been suggested for this region, including mixing in the
late main sequence, a Li dip origin for stars with low Li abundances in the
region, a... | astro-ph.SR | we address the existence and origin of the lithium li desert a region in the li t_eff plane sparsely populated by stars here we analyze some of the explanations that have been suggested for this region including mixing in the late main sequence a li dip origin for stars with low li abundances in the region and a possib... | [['we', 'address', 'the', 'existence', 'and', 'origin', 'of', 'the', 'lithium', 'li', 'desert', 'a', 'region', 'in', 'the', 'li', 't_eff', 'plane', 'sparsely', 'populated', 'by', 'stars', 'here', 'we', 'analyze', 'some', 'of', 'the', 'explanations', 'that', 'have', 'been', 'suggested', 'for', 'this', 'region', 'includi... | [-0.044770085977974924, 0.2261034900955921, -0.00824269528074965, 0.09943883598601394, -0.10243755163766535, -0.06711932430304327, 0.13824483882220645, 0.37341648809794153, -0.15102456085435995, -0.4075479590418664, 0.025325941590680186, -0.3054815246170009, -0.03641484393510264, 0.15520208541644165, -0.130864678639055... |
1,803.05923 | ALMA Survey of Lupus Protoplanetary Disks II: Gas Disk Radii | We present ALMA Band 6 observations of a complete sample of protoplanetary
disks in the young (1-3 Myr) Lupus star-forming region, covering the 1.33 mm
continuum and the 12CO, 13CO, and C18O J=2-1 lines. The spatial resolution is
0.25 arcsec with a medium 3-sigma continuum sensitivity of 0.30 mJy,
corresponding to M_... | astro-ph.EP | we present alma band 6 observations of a complete sample of protoplanetary disks in the young 13 myr lupus starforming region covering the 133 mm continuum and the 12co 13co and c18o j21 lines the spatial resolution is 025 arcsec with a medium 3sigma continuum sensitivity of 030 mjy corresponding to m_dust 02 m_earth w... | [['we', 'present', 'alma', 'band', '6', 'observations', 'of', 'a', 'complete', 'sample', 'of', 'protoplanetary', 'disks', 'in', 'the', 'young', '13', 'myr', 'lupus', 'starforming', 'region', 'covering', 'the', '133', 'mm', 'continuum', 'and', 'the', '12co', '13co', 'and', 'c18o', 'j21', 'lines', 'the', 'spatial', 'reso... | [-0.031189038175350826, 0.10391391773740191, -0.012285849343995604, 0.04687549266964197, -0.04506218519779932, -0.06164479679072717, 0.03461055262678164, 0.45996234214763687, -0.16477314895766987, -0.34116898231904014, 0.08132128026267471, -0.24952469520078202, -0.00027588355340003726, 0.13545250628577418, -0.021825557... |
1,803.05924 | Investigating the Metallicity-Mixing Length Relation | Stellar models typically use the mixing length approximation as a way to
implement convection in a simplified manner. While conventionally the value of
the mixing length parameter, $\alpha$, used is the solar calibrated value, many
studies have shown that other values of $\alpha$ are needed to properly model
stars. T... | astro-ph.SR | stellar models typically use the mixing length approximation as a way to implement convection in a simplified manner while conventionally the value of the mixing length parameter alpha used is the solar calibrated value many studies have shown that other values of alpha are needed to properly model stars this uncertain... | [['stellar', 'models', 'typically', 'use', 'the', 'mixing', 'length', 'approximation', 'as', 'a', 'way', 'to', 'implement', 'convection', 'in', 'a', 'simplified', 'manner', 'while', 'conventionally', 'the', 'value', 'of', 'the', 'mixing', 'length', 'parameter', 'alpha', 'used', 'is', 'the', 'solar', 'calibrated', 'valu... | [-0.05243648374658626, 0.15046535078983972, -0.04649537818314617, 0.08146709140484532, -0.05936708410599214, -0.0863028751056203, 0.07920439846758895, 0.37365389088552226, -0.23210434310466926, -0.3908019272336627, 0.08228349768460783, -0.270520587555845, -0.0634026314405834, 0.23061139296521158, -0.0434196856639841, 0... |
1,803.05925 | Update on the X-ray variability plane for active galactic nuclei: The
role of the obscuration | Scaling relations are the most powerful astrophysical tools to set
constraints to the physical mechanisms of astro- nomical sources and to infer
properties that cannot be accessed directly. We re-investigate here one of
these scaling relations in active galactic nuclei (AGN); the so-called X-ray
variability plane (or... | astro-ph.GA astro-ph.HE | scaling relations are the most powerful astrophysical tools to set constraints to the physical mechanisms of astro nomical sources and to infer properties that cannot be accessed directly we reinvestigate here one of these scaling relations in active galactic nuclei agn the socalled xray variability plane or masslumino... | [['scaling', 'relations', 'are', 'the', 'most', 'powerful', 'astrophysical', 'tools', 'to', 'set', 'constraints', 'to', 'the', 'physical', 'mechanisms', 'of', 'astro', 'nomical', 'sources', 'and', 'to', 'infer', 'properties', 'that', 'can', 'not', 'be', 'accessed', 'directly', 'we', 'reinvestigate', 'here', 'one', 'of'... | [-0.09166070309031425, 0.0803988833719165, -0.0696141635940139, 0.11638330968090958, -0.12562922729996626, -0.06914727950963794, 0.08753140701790525, 0.3995384531575039, -0.19682996720075607, -0.35061384392469996, 0.07667383986706, -0.28989521150860614, -0.069751554171708, 0.22146285596924523, -0.04584307698159624, -0.... |
1,803.05926 | Learning meets Assessment: On the relation between Item Response Theory
and Bayesian Knowledge Tracing | Few models have been more ubiquitous in their respective fields than Bayesian
knowledge tracing and item response theory. Both of these models were developed
to analyze data on learners. However, the study designs that these models are
designed for differ; Bayesian knowledge tracing is designed to analyze
longitudina... | stat.ME | few models have been more ubiquitous in their respective fields than bayesian knowledge tracing and item response theory both of these models were developed to analyze data on learners however the study designs that these models are designed for differ bayesian knowledge tracing is designed to analyze longitudinal data... | [['few', 'models', 'have', 'been', 'more', 'ubiquitous', 'in', 'their', 'respective', 'fields', 'than', 'bayesian', 'knowledge', 'tracing', 'and', 'item', 'response', 'theory', 'both', 'of', 'these', 'models', 'were', 'developed', 'to', 'analyze', 'data', 'on', 'learners', 'however', 'the', 'study', 'designs', 'that', ... | [-0.03698862786163929, 0.06641652914946337, -0.08949503217791689, 0.10292889294696266, -0.13152536350495087, -0.1789659525556811, 0.025591105441081112, 0.4330639458036628, -0.28034332977800536, -0.3444873535812929, 0.09399834962294272, -0.28261649885439666, -0.19617140449037582, 0.1480092203019765, -0.06054872711156976... |
1,803.05927 | Galactic Rotation from Cepheids with Gaia DR2 and Effects of
Non-Axisymmetry | We apply a simple axisymmetric disc model to 218 Galactic Cepheids whose
accurate measurements of the distance and velocities are obtained by
cross-matching an existing Cepheids catalogue with the Gaia DR2 data. Our model
fit determines the "local centrifugal speed", $V_\mathrm{c}$ $-$ defined as the
rotation speed r... | astro-ph.GA | we apply a simple axisymmetric disc model to 218 galactic cepheids whose accurate measurements of the distance and velocities are obtained by crossmatching an existing cepheids catalogue with the gaia dr2 data our model fit determines the local centrifugal speed v_mathrmc defined as the rotation speed required to balan... | [['we', 'apply', 'a', 'simple', 'axisymmetric', 'disc', 'model', 'to', '218', 'galactic', 'cepheids', 'whose', 'accurate', 'measurements', 'of', 'the', 'distance', 'and', 'velocities', 'are', 'obtained', 'by', 'crossmatching', 'an', 'existing', 'cepheids', 'catalogue', 'with', 'the', 'gaia', 'dr2', 'data', 'our', 'mode... | [-0.07813740876288368, 0.07705941576301947, -0.06794183762170948, 0.06648290777832445, -0.12454763016272226, -0.05363277851510242, 0.005723981840464358, 0.40929837707848943, -0.2319661967687794, -0.36337097780779004, 0.044860404280989745, -0.26410770236057113, 0.022681149243536963, 0.25991689079281316, -0.0611934485602... |
1,803.05928 | RankME: Reliable Human Ratings for Natural Language Generation | Human evaluation for natural language generation (NLG) often suffers from
inconsistent user ratings. While previous research tends to attribute this
problem to individual user preferences, we show that the quality of human
judgements can also be improved by experimental design. We present a novel
rank-based magnitude... | cs.CL | human evaluation for natural language generation nlg often suffers from inconsistent user ratings while previous research tends to attribute this problem to individual user preferences we show that the quality of human judgements can also be improved by experimental design we present a novel rankbased magnitude estimat... | [['human', 'evaluation', 'for', 'natural', 'language', 'generation', 'nlg', 'often', 'suffers', 'from', 'inconsistent', 'user', 'ratings', 'while', 'previous', 'research', 'tends', 'to', 'attribute', 'this', 'problem', 'to', 'individual', 'user', 'preferences', 'we', 'show', 'that', 'the', 'quality', 'of', 'human', 'ju... | [-0.04925527635505652, -0.012153137120280842, -0.05873563210479915, 0.07412723518266785, -0.12925437576763454, -0.14992114933986278, 0.07714898081794076, 0.44863401377787354, -0.21102916043190684, -0.34677027788807135, 0.05285838706663153, -0.28004844245485594, -0.20005344076952364, 0.2184736061054969, -0.1690542507309... |
1,803.05929 | Remarks on Donaldson's symplectic submanifolds | This paper presents a few remarks about the topology of symplectic hyperplane
sections and the geometry of their complements. In particular, it contains a
detailed proof of the following result already stated with hints in [Gi]: for
sufficiently large degrees, the complements of Donaldson's symplectic
hyperplane sect... | math.SG | this paper presents a few remarks about the topology of symplectic hyperplane sections and the geometry of their complements in particular it contains a detailed proof of the following result already stated with hints in gi for sufficiently large degrees the complements of donaldsons symplectic hyperplane sections are ... | [['this', 'paper', 'presents', 'a', 'few', 'remarks', 'about', 'the', 'topology', 'of', 'symplectic', 'hyperplane', 'sections', 'and', 'the', 'geometry', 'of', 'their', 'complements', 'in', 'particular', 'it', 'contains', 'a', 'detailed', 'proof', 'of', 'the', 'following', 'result', 'already', 'stated', 'with', 'hints'... | [-0.19303196531466463, 0.021799799244300547, -0.10190654430877079, 0.0976807558379898, -0.12507726666940885, -0.10639032110233199, -0.003560722193850035, 0.2953762548636984, -0.24281322448091072, -0.2896636656739495, 0.07878995845517651, -0.24649259134788404, -0.1526222828606313, 0.20649918558245356, -0.208793338015675... |
1,803.0593 | Research and Development Workstation Environment: the new class of
Current Research Information Systems | Against the backdrop of the development of modern technologies in the field
of scientific research the new class of Current Research Information Systems
(CRIS) and related intelligent information technologies has arisen. It was
called - Research and Development Workstation Environment (RDWE) - the
comprehensive probl... | cs.CY | against the backdrop of the development of modern technologies in the field of scientific research the new class of current research information systems cris and related intelligent information technologies has arisen it was called research and development workstation environment rdwe the comprehensive problemoriented ... | [['against', 'the', 'backdrop', 'of', 'the', 'development', 'of', 'modern', 'technologies', 'in', 'the', 'field', 'of', 'scientific', 'research', 'the', 'new', 'class', 'of', 'current', 'research', 'information', 'systems', 'cris', 'and', 'related', 'intelligent', 'information', 'technologies', 'has', 'arisen', 'it', '... | [-0.11707821001118127, 0.04465955122873743, -0.04179779674677256, 0.020225343524173836, -0.12124780470243311, -0.10642960970201476, 0.01892965183258694, 0.35448128952797037, -0.23982092594203783, -0.34291678362795125, 0.12796434627477604, -0.2606571661547989, -0.15008320385402515, 0.24133549832576043, -0.08164991513903... |
1,803.05931 | The role of surface tension gradient in determining microscopic dynamic
contact angle | Following Gibb's interpretation of an interface as a dividing surface, we
derive a model for the microscopic dynamic contact angle by writing a force
balance for a control volume encompassing the interfaces and the contact line.
In doing so we identify that, in addition to the surface tension of respective
interfaces... | physics.flu-dyn | following gibbs interpretation of an interface as a dividing surface we derive a model for the microscopic dynamic contact angle by writing a force balance for a control volume encompassing the interfaces and the contact line in doing so we identify that in addition to the surface tension of respective interfaces the g... | [['following', 'gibbs', 'interpretation', 'of', 'an', 'interface', 'as', 'a', 'dividing', 'surface', 'we', 'derive', 'a', 'model', 'for', 'the', 'microscopic', 'dynamic', 'contact', 'angle', 'by', 'writing', 'a', 'force', 'balance', 'for', 'a', 'control', 'volume', 'encompassing', 'the', 'interfaces', 'and', 'the', 'co... | [-0.16098971019065092, 0.11727535301799269, -0.11452708608009164, 0.03546585988541748, -0.05320433174545707, -0.1296208371376534, 0.06019242229360151, 0.375248249207454, -0.27476923051157925, -0.3183057101930238, 0.06972874665569345, -0.2358550152976849, -0.15482387142732146, 0.18886388743042268, -0.025477140482890223,... |
1,803.05932 | Multilevel Monte Carlo Method for Ergodic SDEs without Contractivity | This paper proposes a new multilevel Monte Carlo (MLMC) method for the
ergodic SDEs which do not satisfy the contractivity condition. By introducing
the change of measure technique, we simulate the path with contractivity and
add the Radon-Nykodim derivative to the estimator. We can show the strong error
of the path ... | math.NA math.PR | this paper proposes a new multilevel monte carlo mlmc method for the ergodic sdes which do not satisfy the contractivity condition by introducing the change of measure technique we simulate the path with contractivity and add the radonnykodim derivative to the estimator we can show the strong error of the path is unifo... | [['this', 'paper', 'proposes', 'a', 'new', 'multilevel', 'monte', 'carlo', 'mlmc', 'method', 'for', 'the', 'ergodic', 'sdes', 'which', 'do', 'not', 'satisfy', 'the', 'contractivity', 'condition', 'by', 'introducing', 'the', 'change', 'of', 'measure', 'technique', 'we', 'simulate', 'the', 'path', 'with', 'contractivity'... | [-0.07020463698676654, 0.10478166901462135, -0.0879977524845994, 0.07306364227662838, -0.04970904437470294, -0.13227722872758196, 0.07760895455610894, 0.36195803862952053, -0.32556922519136045, -0.30719995946856216, 0.10612250603846318, -0.2914472242196401, -0.10957813405077017, 0.18486064279651535, -0.1143174820712634... |
1,803.05933 | Some Closure Results for Polynomial Factorization and Applications | In a sequence of seminal results in the 80's, Kaltofen showed that the
complexity class VP is closed under taking factors. A natural question in this
context is to understand if other natural classes of multivariate polynomials,
for instance, arithmetic formulas, algebraic branching programs, bounded depth
arithmetic... | cs.CC | in a sequence of seminal results in the 80s kaltofen showed that the complexity class vp is closed under taking factors a natural question in this context is to understand if other natural classes of multivariate polynomials for instance arithmetic formulas algebraic branching programs bounded depth arithmetic circuits... | [['in', 'a', 'sequence', 'of', 'seminal', 'results', 'in', 'the', '80s', 'kaltofen', 'showed', 'that', 'the', 'complexity', 'class', 'vp', 'is', 'closed', 'under', 'taking', 'factors', 'a', 'natural', 'question', 'in', 'this', 'context', 'is', 'to', 'understand', 'if', 'other', 'natural', 'classes', 'of', 'multivariate... | [-0.15273793489682752, 0.11826872071878824, -0.050349848283480644, 0.039336269486537075, -0.045959060957506556, -0.17832449220198518, 0.07025464801457322, 0.3179774846802401, -0.2988771945901034, -0.284430585699738, 0.05161122398931184, -0.21577728805601104, -0.14572231647374187, 0.25967739818669444, -0.113147698835695... |
1,803.05934 | Dual solutions for opposing mixed convection in porous media | The problem of steady mixed convection boundary-layer flow on a cooled
vertical permeable circular cylinder embedded in a fluid-saturated porous
medium is studied. Here, we evaluate the flow and heat transfer characteristics
numerically for various values of the governing parameters and demonstrate the
existence of d... | physics.flu-dyn | the problem of steady mixed convection boundarylayer flow on a cooled vertical permeable circular cylinder embedded in a fluidsaturated porous medium is studied here we evaluate the flow and heat transfer characteristics numerically for various values of the governing parameters and demonstrate the existence of dual so... | [['the', 'problem', 'of', 'steady', 'mixed', 'convection', 'boundarylayer', 'flow', 'on', 'a', 'cooled', 'vertical', 'permeable', 'circular', 'cylinder', 'embedded', 'in', 'a', 'fluidsaturated', 'porous', 'medium', 'is', 'studied', 'here', 'we', 'evaluate', 'the', 'flow', 'and', 'heat', 'transfer', 'characteristics', '... | [-0.13499855497103258, 0.1416802074961072, -0.0534016534722611, 0.011568975554980045, -0.027410889263538754, -0.09464077674327236, -0.00767856072999683, 0.3419452618953644, -0.3184393327317986, -0.21413409658798985, 0.16336498118927886, -0.2624436572340189, -0.08605550185722463, 0.20852613941236747, 0.00451213381636668... |
1,803.05935 | CIM/E Oriented Graph Database Model Architecture and Parallel Network
Topology Processing | CIM/E is an easy and efficient electric power model exchange standard between
different Energy Management System vendors. With the rapid growth of data size
and system complexity, the traditional relational database is not the best
option to store and process the data. In contrast, the graph database and graph
comput... | cs.DC | cime is an easy and efficient electric power model exchange standard between different energy management system vendors with the rapid growth of data size and system complexity the traditional relational database is not the best option to store and process the data in contrast the graph database and graph computation s... | [['cime', 'is', 'an', 'easy', 'and', 'efficient', 'electric', 'power', 'model', 'exchange', 'standard', 'between', 'different', 'energy', 'management', 'system', 'vendors', 'with', 'the', 'rapid', 'growth', 'of', 'data', 'size', 'and', 'system', 'complexity', 'the', 'traditional', 'relational', 'database', 'is', 'not',... | [-0.11831212432624857, -0.03179202772312153, -0.06009649564598843, 0.03306543987404755, -0.10689172289270607, -0.1497952199905463, 0.06278923459087862, 0.3916342313363801, -0.32402044793544627, -0.3795263454989062, 0.13502202645777175, -0.27930011221942325, -0.12877617411963319, 0.19771255546297173, -0.0863525989698246... |
1,803.05936 | Mapping Disorder in Entropically Ordered Crystals | Systems of hard shapes crystallize due to entropy. How is entropy distributed
among translational and rotational microscopic contributions? We answer this
question by decomposing thermal fluctuation of crystals of hard hexagons into
collective modes, a generalization and quantification of the Onsager picture of
hard ... | cond-mat.soft cond-mat.stat-mech | systems of hard shapes crystallize due to entropy how is entropy distributed among translational and rotational microscopic contributions we answer this question by decomposing thermal fluctuation of crystals of hard hexagons into collective modes a generalization and quantification of the onsager picture of hard rod l... | [['systems', 'of', 'hard', 'shapes', 'crystallize', 'due', 'to', 'entropy', 'how', 'is', 'entropy', 'distributed', 'among', 'translational', 'and', 'rotational', 'microscopic', 'contributions', 'we', 'answer', 'this', 'question', 'by', 'decomposing', 'thermal', 'fluctuation', 'of', 'crystals', 'of', 'hard', 'hexagons',... | [-0.11257069118248371, 0.24852451565977815, -0.09150884076106278, 0.02197850761517834, -0.02442592324374558, -0.14133492855403523, 0.07719186217185449, 0.3657927313795337, -0.2860293957032868, -0.24946762586326957, 0.03766596302021198, -0.3427873154037765, -0.1088009524528034, 0.07492696452740726, -0.022099283064243854... |
1,803.05937 | Definable decompositions for graphs of bounded linear cliquewidth | We prove that for every positive integer k, there exists an
MSO_1-transduction that given a graph of linear cliquewidth at most k outputs,
nondeterministically, some cliquewidth decomposition of the graph of width
bounded by a function of k. A direct corollary of this result is the
equivalence of the notions of CMSO_... | cs.LO | we prove that for every positive integer k there exists an mso_1transduction that given a graph of linear cliquewidth at most k outputs nondeterministically some cliquewidth decomposition of the graph of width bounded by a function of k a direct corollary of this result is the equivalence of the notions of cmso_1defina... | [['we', 'prove', 'that', 'for', 'every', 'positive', 'integer', 'k', 'there', 'exists', 'an', 'mso_1transduction', 'that', 'given', 'a', 'graph', 'of', 'linear', 'cliquewidth', 'at', 'most', 'k', 'outputs', 'nondeterministically', 'some', 'cliquewidth', 'decomposition', 'of', 'the', 'graph', 'of', 'width', 'bounded', '... | [-0.20339809144558063, 0.1200780793485043, -0.03226732049169469, 0.007720363984719433, -0.12318049236361323, -0.1436069058976939, 0.08417635870262466, 0.3558958586433838, -0.3703336748716036, -0.24708329972907386, 0.07487918154721887, -0.29245044342402754, -0.12277764722640658, 0.1663764878979017, -0.04601948778145015,... |
1,803.05938 | Low Rank plus Sparse Decomposition of ODFs for Improved Detection of
Group-level Differences and Variable Correlations in White Matter | A novel approach is presented for group statistical analysis of diffusion
weighted MRI datasets through voxelwise Orientation Distribution Functions
(ODF). Recent advances in MRI acquisition make it possible to use high quality
diffusion weighted protocols (multi-shell, large number of gradient directions)
for routin... | physics.med-ph physics.bio-ph q-bio.NC | a novel approach is presented for group statistical analysis of diffusion weighted mri datasets through voxelwise orientation distribution functions odf recent advances in mri acquisition make it possible to use high quality diffusion weighted protocols multishell large number of gradient directions for routine in vivo... | [['a', 'novel', 'approach', 'is', 'presented', 'for', 'group', 'statistical', 'analysis', 'of', 'diffusion', 'weighted', 'mri', 'datasets', 'through', 'voxelwise', 'orientation', 'distribution', 'functions', 'odf', 'recent', 'advances', 'in', 'mri', 'acquisition', 'make', 'it', 'possible', 'to', 'use', 'high', 'quality... | [-0.07926561255216932, 0.04933067451780423, -0.058386391713181614, 0.07533994304048641, -0.07885068643074004, -0.11867914813819713, 0.033019922291621186, 0.407329174031541, -0.2818827824999711, -0.31273419792071366, 0.10814712478799725, -0.2774313621175213, -0.17230716990409317, 0.15153251840321913, -0.0993238140371774... |
1,803.05939 | Noise-induced rectification in out-of-equilibrium structures | We consider the motion of overdamped particles on random potentials subjected
to a Gaussian white noise and a time-dependent periodic external forcing. The
random potential is modeled as the potential resulting from the interaction of
a point particle with a random polymer. The random polymer is made up, by means
of ... | cond-mat.dis-nn cond-mat.stat-mech | we consider the motion of overdamped particles on random potentials subjected to a gaussian white noise and a timedependent periodic external forcing the random potential is modeled as the potential resulting from the interaction of a point particle with a random polymer the random polymer is made up by means of some s... | [['we', 'consider', 'the', 'motion', 'of', 'overdamped', 'particles', 'on', 'random', 'potentials', 'subjected', 'to', 'a', 'gaussian', 'white', 'noise', 'and', 'a', 'timedependent', 'periodic', 'external', 'forcing', 'the', 'random', 'potential', 'is', 'modeled', 'as', 'the', 'potential', 'resulting', 'from', 'the', '... | [-0.1222701085562476, 0.1717268943805797, -0.10541207951963574, 0.02576182138248348, -0.013820577924200725, -0.10501002431107319, 0.05700280366217387, 0.3518001914337695, -0.2898014052945111, -0.23343063213331539, 0.07016583673914929, -0.2600785118884572, -0.16134595195327617, 0.1632919331210683, -0.01621792582951695, ... |
1,803.0594 | Smartphone picture organization: A hierarchical approach | We live in a society where the large majority of the population has a
camera-equipped smartphone. In addition, hard drives and cloud storage are
getting cheaper and cheaper, leading to a tremendous growth in stored personal
photos. Unlike photo collections captured by a digital camera, which typically
are pre-process... | cs.CV | we live in a society where the large majority of the population has a cameraequipped smartphone in addition hard drives and cloud storage are getting cheaper and cheaper leading to a tremendous growth in stored personal photos unlike photo collections captured by a digital camera which typically are preprocessed by the... | [['we', 'live', 'in', 'a', 'society', 'where', 'the', 'large', 'majority', 'of', 'the', 'population', 'has', 'a', 'cameraequipped', 'smartphone', 'in', 'addition', 'hard', 'drives', 'and', 'cloud', 'storage', 'are', 'getting', 'cheaper', 'and', 'cheaper', 'leading', 'to', 'a', 'tremendous', 'growth', 'in', 'stored', 'p... | [-0.04056100587203058, 0.06339382546310149, -0.07073579339981627, 0.08197531081946093, -0.1273200349567239, -0.15997247468890147, 0.06424586089925986, 0.4035341470415576, -0.2558959892211372, -0.3790607356809322, 0.08771528584503696, -0.3454395259420077, -0.13511715723685555, 0.20985914830931043, -0.14194922510068864, ... |
1,803.05941 | Excited States of Methylene, Polyenes, and Ozone from Heat-Bath
Configuration Interaction | The electronically excited states of methylene (CH$_2$), ethylene
(C$_2$H$_4$), butadiene (C$_4$H$_6$), hexatriene (C$_6$H$_8$), and ozone
(O$_3$) have long proven challenging due to their complex mixtures of static
and dynamic correlations. Semistochastic heat-bath configuration interaction
(SHCI), which efficiently... | physics.chem-ph physics.comp-ph | the electronically excited states of methylene ch_2 ethylene c_2h_4 butadiene c_4h_6 hexatriene c_6h_8 and ozone o_3 have long proven challenging due to their complex mixtures of static and dynamic correlations semistochastic heatbath configuration interaction shci which efficiently and systematically approaches the fu... | [['the', 'electronically', 'excited', 'states', 'of', 'methylene', 'ch_2', 'ethylene', 'c_2h_4', 'butadiene', 'c_4h_6', 'hexatriene', 'c_6h_8', 'and', 'ozone', 'o_3', 'have', 'long', 'proven', 'challenging', 'due', 'to', 'their', 'complex', 'mixtures', 'of', 'static', 'and', 'dynamic', 'correlations', 'semistochastic',... | [-0.08384452918081556, 0.15530673794852323, -0.017469530491753066, 0.07896757884447586, 0.042129352148790586, -0.12137512526620763, 0.06938507726853602, 0.40095681979752945, -0.18711620755072864, -0.3513191859125642, 0.0353097294363283, -0.3071951003666653, -0.04891636044611728, 0.1613469546932884, 0.04697413679145007,... |
1,803.05942 | Adaptive Tube-based Nonlinear MPC for Ecological Autonomous Cruise
Control of Plug-in Hybrid Electric Vehicles | This paper proposes an adaptive tube-based nonlinear model predictive control
(AT-NMPC) approach to the design of autonomous cruise control (ACC) systems.
The proposed method utilizes two separate models to define the constrained
receding horizon optimal control problem. A fixed nominal model is used to
handle the pr... | cs.SY | this paper proposes an adaptive tubebased nonlinear model predictive control atnmpc approach to the design of autonomous cruise control acc systems the proposed method utilizes two separate models to define the constrained receding horizon optimal control problem a fixed nominal model is used to handle the problem cons... | [['this', 'paper', 'proposes', 'an', 'adaptive', 'tubebased', 'nonlinear', 'model', 'predictive', 'control', 'atnmpc', 'approach', 'to', 'the', 'design', 'of', 'autonomous', 'cruise', 'control', 'acc', 'systems', 'the', 'proposed', 'method', 'utilizes', 'two', 'separate', 'models', 'to', 'define', 'the', 'constrained',... | [-0.10266127769136801, -0.02572311495343153, -0.10744118704254409, 0.04098020148391394, -0.10667500139970798, -0.2118612208723789, 0.05296708622154256, 0.3614391662898318, -0.27286385618693504, -0.3602812232178015, 0.12177876244133283, -0.20022738033003407, -0.13572560278892828, 0.2183903818925804, -0.13429299396375427... |
1,803.05943 | Closed form expressions for Appell polynomials | We show that any Appell sequence can be written in closed form as a forward
difference transformation of the identity. Such transformations are actually
multipliers in the abelian group of the Appell polynomials endowed with the
operation of binomial convolution. As a consequence, we obtain explicit
expressions for h... | math.NT | we show that any appell sequence can be written in closed form as a forward difference transformation of the identity such transformations are actually multipliers in the abelian group of the appell polynomials endowed with the operation of binomial convolution as a consequence we obtain explicit expressions for higher... | [['we', 'show', 'that', 'any', 'appell', 'sequence', 'can', 'be', 'written', 'in', 'closed', 'form', 'as', 'a', 'forward', 'difference', 'transformation', 'of', 'the', 'identity', 'such', 'transformations', 'are', 'actually', 'multipliers', 'in', 'the', 'abelian', 'group', 'of', 'the', 'appell', 'polynomials', 'endowed... | [-0.18326026454837208, 0.10383225767031672, -0.06036445617967521, 0.1075648725964129, -0.11540020290896835, -0.08028835732579591, -0.0198433186777542, 0.34727831757122496, -0.3090022102402276, -0.22928721716919218, 0.101941630406956, -0.2453651755475944, -0.20816611500277396, 0.233246873839792, -0.08748705312048635, 0.... |
1,803.05944 | $L^2$ concentration of blow-up solutions for the mass-critical NLS with
inverse-square potential | In this paper, we prove a refined version of a compactness lemma and we use
it to establish mass-concentration for the focusing nonlinear Schr\"{o}dinger
equation with an inverse-square potential.
| math.AP | in this paper we prove a refined version of a compactness lemma and we use it to establish massconcentration for the focusing nonlinear schrodinger equation with an inversesquare potential | [['in', 'this', 'paper', 'we', 'prove', 'a', 'refined', 'version', 'of', 'a', 'compactness', 'lemma', 'and', 'we', 'use', 'it', 'to', 'establish', 'massconcentration', 'for', 'the', 'focusing', 'nonlinear', 'schrodinger', 'equation', 'with', 'an', 'inversesquare', 'potential']] | [-0.09665045158231053, -0.037711223691264326, -0.15284249912305126, 0.13734370523437472, -0.13057549259272114, -0.13710896982329673, 0.013061183958378589, 0.3025876846292923, -0.2900712425852644, -0.24099757856336132, 0.09789390230535305, -0.28222178676615245, -0.18440826918030606, 0.2031983076755343, -0.09927676374028... |
1,803.05945 | Analog simulator of integro-differential equations with classical
memristors | An analog computer makes use of continuously changeable quantities of a
system, such as its electrical, mechanical, or hydraulic properties, to solve a
given problem. While these devices are usually computationally more powerful
than their digital counterparts, they suffer from analog noise which does not
allow for e... | cs.ET cs.NE quant-ph | an analog computer makes use of continuously changeable quantities of a system such as its electrical mechanical or hydraulic properties to solve a given problem while these devices are usually computationally more powerful than their digital counterparts they suffer from analog noise which does not allow for error con... | [['an', 'analog', 'computer', 'makes', 'use', 'of', 'continuously', 'changeable', 'quantities', 'of', 'a', 'system', 'such', 'as', 'its', 'electrical', 'mechanical', 'or', 'hydraulic', 'properties', 'to', 'solve', 'a', 'given', 'problem', 'while', 'these', 'devices', 'are', 'usually', 'computationally', 'more', 'powerf... | [-0.11994916280506837, 0.07438192547906239, -0.045668193270030674, 0.03447841308821011, -0.09872510333763278, -0.18359421376620805, 0.021964589827717165, 0.35542341897644064, -0.28302860814864883, -0.3229794210212222, 0.1465881885456811, -0.26118876451431816, -0.19779207508730706, 0.28486223483981743, -0.07760662990112... |
1,803.05946 | An Optimal Algorithm to Compute the Inverse Beacon Attraction Region | The beacon model is a recent paradigm for guiding the trajectory of messages
or small robotic agents in complex environments. A beacon is a fixed point with
an attraction pull that can move points within a given polygon. Points move
greedily towards a beacon: if unobstructed, they move along a straight line to
the be... | cs.CG | the beacon model is a recent paradigm for guiding the trajectory of messages or small robotic agents in complex environments a beacon is a fixed point with an attraction pull that can move points within a given polygon points move greedily towards a beacon if unobstructed they move along a straight line to the beacon a... | [['the', 'beacon', 'model', 'is', 'a', 'recent', 'paradigm', 'for', 'guiding', 'the', 'trajectory', 'of', 'messages', 'or', 'small', 'robotic', 'agents', 'in', 'complex', 'environments', 'a', 'beacon', 'is', 'a', 'fixed', 'point', 'with', 'an', 'attraction', 'pull', 'that', 'can', 'move', 'points', 'within', 'a', 'give... | [-0.17785832888297876, 0.08590828846032397, -0.10925303033958138, 0.006297548239631751, -0.08201677641021192, -0.16660588099378884, 0.1397684365665656, 0.36609490898863645, -0.2965046086796078, -0.26514004691993837, 0.07515820116107612, -0.32164755818472146, -0.1274337469830375, 0.13236880073320384, -0.0943050886263745... |
1,803.05947 | Control Inversion: A Clustering-Based Method for Distributed Wide-Area
Control of Power Systems | Wide-area control (WAC) has been shown to be an effective tool for damping
low-frequency oscillations in power systems. In the current state of art, WAC
is challenged by two main factors - namely, scalability of design and
complexity of implementation. In this paper we present a control design called
control inversio... | cs.SY | widearea control wac has been shown to be an effective tool for damping lowfrequency oscillations in power systems in the current state of art wac is challenged by two main factors namely scalability of design and complexity of implementation in this paper we present a control design called control inversion that bypas... | [['widearea', 'control', 'wac', 'has', 'been', 'shown', 'to', 'be', 'an', 'effective', 'tool', 'for', 'damping', 'lowfrequency', 'oscillations', 'in', 'power', 'systems', 'in', 'the', 'current', 'state', 'of', 'art', 'wac', 'is', 'challenged', 'by', 'two', 'main', 'factors', 'namely', 'scalability', 'of', 'design', 'an... | [-0.12042793775983755, -0.01105833557535774, -0.08013385736774052, -0.009257507179262898, -0.09110350848265714, -0.14933809598967915, 0.019621309048436102, 0.3384131336584687, -0.29078186462002414, -0.30514220255276847, 0.15364622125071623, -0.22110914889602892, -0.1962885751693149, 0.2317211620614774, -0.1040300341518... |
1,803.05948 | Average Cost of QuickXsort with Pivot Sampling | QuickXsort is a strategy to combine Quicksort with another sorting method X,
so that the result has essentially the same comparison cost as X in isolation,
but sorts in place even when X requires a linear-size buffer. We solve the
recurrence for QuickXsort precisely up to the linear term including the
optimization to... | cs.DS | quickxsort is a strategy to combine quicksort with another sorting method x so that the result has essentially the same comparison cost as x in isolation but sorts in place even when x requires a linearsize buffer we solve the recurrence for quickxsort precisely up to the linear term including the optimization to choos... | [['quickxsort', 'is', 'a', 'strategy', 'to', 'combine', 'quicksort', 'with', 'another', 'sorting', 'method', 'x', 'so', 'that', 'the', 'result', 'has', 'essentially', 'the', 'same', 'comparison', 'cost', 'as', 'x', 'in', 'isolation', 'but', 'sorts', 'in', 'place', 'even', 'when', 'x', 'requires', 'a', 'linearsize', 'bu... | [-0.07174992584827634, 0.05737925573709633, -0.09493499524889334, 0.028254232757414382, -0.07235270940388243, -0.17188532178682325, 0.15952077855993257, 0.37846086168939475, -0.28295932182421285, -0.34503940024756286, 0.11796451621513258, -0.23613622922079103, -0.09552725262555964, 0.18630568635355876, -0.0665706408479... |
1,803.05949 | Asymmetric regularization of the ground and excited state of the
helium-4 nucleus | We find the threshold structure of the two- and three-nucleon systems, with
the deuteron and 3H/3He as the only bound nuclei, sufficient to predict a pair
of four-nucleon states: a deeply bound state which is identified with the
helium-4 ground state, and a shallow, unstable state at an energy 0.38(25) MeV
above the ... | nucl-th physics.atom-ph | we find the threshold structure of the two and threenucleon systems with the deuteron and 3h3he as the only bound nuclei sufficient to predict a pair of fournucleon states a deeply bound state which is identified with the helium4 ground state and a shallow unstable state at an energy 03825 mev above the tritonproton th... | [['we', 'find', 'the', 'threshold', 'structure', 'of', 'the', 'two', 'and', 'threenucleon', 'systems', 'with', 'the', 'deuteron', 'and', '3h3he', 'as', 'the', 'only', 'bound', 'nuclei', 'sufficient', 'to', 'predict', 'a', 'pair', 'of', 'fournucleon', 'states', 'a', 'deeply', 'bound', 'state', 'which', 'is', 'identified... | [-0.12742595615303093, 0.21716527276759257, -0.10303946622377617, 0.08787826769616292, 0.017929953819902898, -0.11813146364747908, 0.03568187750916663, 0.3188245008175409, -0.21314474725535984, -0.2570869606074144, -0.024408233063193698, -0.3345134059282763, -0.06849953806272051, 0.07172606294196038, 0.1116117523993299... |
1,803.0595 | The fermion-boson map for large d | We show that the three-dimensional map between fermions and bosons at finite
temperature generalises for all odd dimensions $d>3$. We further argue that
such a map has a nontrivial large $d$ limit. Evidence comes from studying the
gap equations, the free energies and the partition functions of the $U(N)$
Gross-Neveu ... | hep-th | we show that the threedimensional map between fermions and bosons at finite temperature generalises for all odd dimensions d3 we further argue that such a map has a nontrivial large d limit evidence comes from studying the gap equations the free energies and the partition functions of the un grossneveu and cpn1 models ... | [['we', 'show', 'that', 'the', 'threedimensional', 'map', 'between', 'fermions', 'and', 'bosons', 'at', 'finite', 'temperature', 'generalises', 'for', 'all', 'odd', 'dimensions', 'd3', 'we', 'further', 'argue', 'that', 'such', 'a', 'map', 'has', 'a', 'nontrivial', 'large', 'd', 'limit', 'evidence', 'comes', 'from', 'st... | [-0.15124534752075783, 0.14647811712555786, -0.05444389316142492, 0.08888505920878656, -0.0038758961378508026, -0.12512400124909445, 0.006078423402089227, 0.3183971384728682, -0.2009617343234519, -0.2692805884649888, 0.06404237187581159, -0.3036183889018416, -0.18768943161869953, 0.16362542488301793, 0.0072228284275514... |
1,803.05951 | Cell structure formation in a two-dimensional density-based dislocation
dynamics model | Cellular patterns formed by self-organization of dislocations are a most
conspicuous feature of dislocation microstructure evolution during plastic
deformation. To elucidate the physical mechanisms underlying dislocation cell
structure formation, we use a minimal model for the evolution of dislocation
densities under... | cond-mat.mtrl-sci | cellular patterns formed by selforganization of dislocations are a most conspicuous feature of dislocation microstructure evolution during plastic deformation to elucidate the physical mechanisms underlying dislocation cell structure formation we use a minimal model for the evolution of dislocation densities under load... | [['cellular', 'patterns', 'formed', 'by', 'selforganization', 'of', 'dislocations', 'are', 'a', 'most', 'conspicuous', 'feature', 'of', 'dislocation', 'microstructure', 'evolution', 'during', 'plastic', 'deformation', 'to', 'elucidate', 'the', 'physical', 'mechanisms', 'underlying', 'dislocation', 'cell', 'structure', ... | [-0.15639029933529383, 0.09940132761976007, -0.09326721339549288, 0.05547705265420751, -0.062103710091071775, -0.10228608238860859, 0.06011910961135059, 0.4041351697288771, -0.32138322180563067, -0.2689504961067058, 0.07789274006801268, -0.18156248774438938, -0.22231704538278546, 0.1229490321443304, -0.0147526685036190... |
1,803.05952 | Probing sub-galactic mass structure with the power spectrum of
surface-brightness anomalies in high-resolution observations of galaxy-galaxy
strong gravitational lenses. II.Observational constraints on the sub-galactic
matter power spectrum | Stringent observational constraints on the sub-galactic matter power spectrum
would allow one to distinguish between the concordance $\Lambda$CDM and the
various alternative dark-matter models that predict significantly different
properties of mass structure in galactic haloes. Galaxy-galaxy strong
gravitational lens... | astro-ph.GA astro-ph.CO | stringent observational constraints on the subgalactic matter power spectrum would allow one to distinguish between the concordance lambdacdm and the various alternative darkmatter models that predict significantly different properties of mass structure in galactic haloes galaxygalaxy strong gravitational lensing provi... | [['stringent', 'observational', 'constraints', 'on', 'the', 'subgalactic', 'matter', 'power', 'spectrum', 'would', 'allow', 'one', 'to', 'distinguish', 'between', 'the', 'concordance', 'lambdacdm', 'and', 'the', 'various', 'alternative', 'darkmatter', 'models', 'that', 'predict', 'significantly', 'different', 'properti... | [-0.11766896878126198, 0.07688415343873203, -0.07887925286979779, 0.1478832971284409, -0.11559170033053859, -0.07177617024002678, 0.031143071630503984, 0.3208761791860604, -0.15477911512286444, -0.3922993228588577, 0.021409076193357697, -0.2792133121215359, -0.011186531914964966, 0.21586126156819418, 0.0124818065694695... |
1,803.05953 | Generalized Stirling Numbers I | We consider generalized Stirling numbers of the second kind $%
S_{a,b,r}^{\alpha_{s},\beta_{s},r_{s},p_{s}}\left( p,k\right) $, $%
k=0,1,\ldots .rp+\sum_{s=2}^{L}r_{s}p_{s}$, where $a,b,\alpha_{s},\beta_{s} $
are complex numbers, and $r,p,r_{s},p_{s}$ are non-negative integers given,
$s=2,\ldots ,L$. (The case $a=1,b... | math.CO math.NT | we consider generalized stirling numbers of the second kind s_abralpha_sbeta_sr_sp_sleft pkright k01ldots rpsum_s2lr_sp_s where abalpha_sbeta_s are complex numbers and rpr_sp_s are nonnegative integers given s2ldots l the case a1b0r1r_sp_s0 corresponds to the standard stirling numbers sleft pkright the numbers s_abralp... | [['we', 'consider', 'generalized', 'stirling', 'numbers', 'of', 'the', 'second', 'kind', 's_abralpha_sbeta_sr_sp_sleft', 'pkright', 'k01ldots', 'rpsum_s2lr_sp_s', 'where', 'abalpha_sbeta_s', 'are', 'complex', 'numbers', 'and', 'rpr_sp_s', 'are', 'nonnegative', 'integers', 'given', 's2ldots', 'l', 'the', 'case', 'a1b0r1... | [-0.22808936207841796, 0.13349058109675893, 0.003084184333252219, 0.10256702114286152, -0.13393865876311722, -0.08644993688302258, 0.010412366138412975, 0.23889995032312492, -0.2732211426572086, -0.2838812768056344, 0.06710229773363188, -0.2809957348084796, -0.17735679510336083, 0.2504873135386823, -0.08032984753998999... |
1,803.05954 | On some abelian varieties of type IV | We study a certain class of simple abelian varieties of type $\mathrm{IV}$
(in Albert's classification) over number fields with Mumford-Tate groups of
type $A$. In particular, we show that such abelian varieties have ordinary
reduction away from a set of places of Dirichlet density zero, thus confirming
a special cas... | math.NT | we study a certain class of simple abelian varieties of type mathrmiv in alberts classification over number fields with mumfordtate groups of type a in particular we show that such abelian varieties have ordinary reduction away from a set of places of dirichlet density zero thus confirming a special case of a broader c... | [['we', 'study', 'a', 'certain', 'class', 'of', 'simple', 'abelian', 'varieties', 'of', 'type', 'mathrmiv', 'in', 'alberts', 'classification', 'over', 'number', 'fields', 'with', 'mumfordtate', 'groups', 'of', 'type', 'a', 'in', 'particular', 'we', 'show', 'that', 'such', 'abelian', 'varieties', 'have', 'ordinary', 're... | [-0.1829270335774009, 0.05587646729336717, -0.07030461597232482, 0.05373317973825555, -0.09716706517009208, -0.12978057811060587, 0.041936633872608535, 0.2823715175096041, -0.26968135841143054, -0.2496869990315575, 0.11047921750025871, -0.20339550417012128, -0.1376754010024552, 0.2271214171241109, -0.1312671044232467, ... |
1,803.05955 | Logarithmic forms and singular projective foliations | In this article we study polynomial logarithmic $q$-forms on a projective
space and characterize those that define singular foliations of codimension
$q$. Our main result is the algebraic proof of their infinitesimal stability
when $q=2$ with some extra degree assumptions. We determine new irreducible
components of t... | math.AG math.DS | in this article we study polynomial logarithmic qforms on a projective space and characterize those that define singular foliations of codimension q our main result is the algebraic proof of their infinitesimal stability when q2 with some extra degree assumptions we determine new irreducible components of the moduli sp... | [['in', 'this', 'article', 'we', 'study', 'polynomial', 'logarithmic', 'qforms', 'on', 'a', 'projective', 'space', 'and', 'characterize', 'those', 'that', 'define', 'singular', 'foliations', 'of', 'codimension', 'q', 'our', 'main', 'result', 'is', 'the', 'algebraic', 'proof', 'of', 'their', 'infinitesimal', 'stability'... | [-0.18845239511158848, 0.05128359466496996, -0.11485049194016028, 0.06628366686241602, -0.08584906110523402, -0.09665964920817974, -0.020954247249652065, 0.319324403477367, -0.28625031077120056, -0.16717238040291704, 0.08846118646033574, -0.21544516444555484, -0.18969122099640248, 0.2184623922553978, -0.116290768240495... |
1,803.05956 | Electrometry by optical charge conversion of deep defects in 4H-SiC | Optically-active point defects in various host materials, such as diamond and
silicon carbide (SiC), have shown significant promise as local sensors of
magnetic fields, electric fields, strain and temperature. Current sensing
techniques take advantage of the relaxation and coherence times of the spin
state within the... | cond-mat.mes-hall physics.ins-det quant-ph | opticallyactive point defects in various host materials such as diamond and silicon carbide sic have shown significant promise as local sensors of magnetic fields electric fields strain and temperature current sensing techniques take advantage of the relaxation and coherence times of the spin state within these defects... | [['opticallyactive', 'point', 'defects', 'in', 'various', 'host', 'materials', 'such', 'as', 'diamond', 'and', 'silicon', 'carbide', 'sic', 'have', 'shown', 'significant', 'promise', 'as', 'local', 'sensors', 'of', 'magnetic', 'fields', 'electric', 'fields', 'strain', 'and', 'temperature', 'current', 'sensing', 'techni... | [-0.11866343504182733, 0.18237299542767693, -0.02663403615106348, -0.04395352524651843, 0.021123687997697645, -0.12125212610195017, 0.06197659053786355, 0.45140459530862276, -0.23712361347416688, -0.3053719688082339, 0.05358475765842161, -0.26887530251406133, -0.10176509829938032, 0.20648882668584015, -0.00072722269183... |
1,803.05957 | Interplay of Probabilistic Shaping and the Blind Phase Search Algorithm | Probabilistic shaping (PS) is a promising technique to approach the Shannon
limit using typical constellation geometries. However, the impact of PS on the
chain of signal processing algorithms of a coherent receiver still needs
further investigation. In this work we study the interplay of PS and phase
recovery using ... | eess.SP cs.IT math.IT | probabilistic shaping ps is a promising technique to approach the shannon limit using typical constellation geometries however the impact of ps on the chain of signal processing algorithms of a coherent receiver still needs further investigation in this work we study the interplay of ps and phase recovery using the bli... | [['probabilistic', 'shaping', 'ps', 'is', 'a', 'promising', 'technique', 'to', 'approach', 'the', 'shannon', 'limit', 'using', 'typical', 'constellation', 'geometries', 'however', 'the', 'impact', 'of', 'ps', 'on', 'the', 'chain', 'of', 'signal', 'processing', 'algorithms', 'of', 'a', 'coherent', 'receiver', 'still', '... | [-0.12806790713608887, 0.08518266334198416, -0.11640696953050793, 0.09675538957235404, -0.0342518729219834, -0.18727402441514035, 0.10725382157756637, 0.4170222809972862, -0.24353236421942712, -0.3239542251204451, 0.14100263985572384, -0.19456937031199534, -0.16532020681692908, 0.20114369007137914, -0.0736280800588429,... |
1,803.05958 | Description of gravity in the model with independent nonsymmetric
connection | A generalization of General Relativity is studied. The standard
Einstein-Hilbert action is considered in the Palatini formalism, where the
connection and the metric are independent variables, and the connection is not
symmetric. As a result of variation with respect to the metric Einstein
equations are obtained. A va... | gr-qc | a generalization of general relativity is studied the standard einsteinhilbert action is considered in the palatini formalism where the connection and the metric are independent variables and the connection is not symmetric as a result of variation with respect to the metric einstein equations are obtained a variation ... | [['a', 'generalization', 'of', 'general', 'relativity', 'is', 'studied', 'the', 'standard', 'einsteinhilbert', 'action', 'is', 'considered', 'in', 'the', 'palatini', 'formalism', 'where', 'the', 'connection', 'and', 'the', 'metric', 'are', 'independent', 'variables', 'and', 'the', 'connection', 'is', 'not', 'symmetric'... | [-0.16024954043127396, 0.10163306467310994, -0.10575002008998716, 0.05927830071320657, -0.12917668861966278, -0.10014914577776515, -0.031559085299581846, 0.2929182455818345, -0.250613875133363, -0.3019081275395709, 0.07386000243698347, -0.2777418232321538, -0.1637850627491905, 0.13285505035782005, -0.05236987284356351,... |
1,803.05959 | Mo2Cap2: Real-time Mobile 3D Motion Capture with a Cap-mounted Fisheye
Camera | We propose the first real-time approach for the egocentric estimation of 3D
human body pose in a wide range of unconstrained everyday activities. This
setting has a unique set of challenges, such as mobility of the hardware setup,
and robustness to long capture sessions with fast recovery from tracking
failures. We t... | cs.CV | we propose the first realtime approach for the egocentric estimation of 3d human body pose in a wide range of unconstrained everyday activities this setting has a unique set of challenges such as mobility of the hardware setup and robustness to long capture sessions with fast recovery from tracking failures we tackle t... | [['we', 'propose', 'the', 'first', 'realtime', 'approach', 'for', 'the', 'egocentric', 'estimation', 'of', '3d', 'human', 'body', 'pose', 'in', 'a', 'wide', 'range', 'of', 'unconstrained', 'everyday', 'activities', 'this', 'setting', 'has', 'a', 'unique', 'set', 'of', 'challenges', 'such', 'as', 'mobility', 'of', 'the'... | [-0.07681484095555119, -0.023534088694073398, -0.06240065674086107, 0.015943684863023735, -0.09566920325502845, -0.1925556310509657, 0.010877654276376852, 0.42071502230650076, -0.24200180072360244, -0.3780399361751014, 0.08854223289198465, -0.24025493832247938, -0.18164491176925188, 0.2194222343851315, -0.1940984551229... |
1,803.0596 | Topology and quantum phases of low dimensional fermionic systems | In this thesis, we study quantum phase transitions and topological phases in
low dimensional fermionic systems. In the first part, we study quantum phase
transitions and the nature of currents in one-dimensional systems, using field
theoretic techniques like bosonization and renormalization group. This involves
the s... | cond-mat.str-el | in this thesis we study quantum phase transitions and topological phases in low dimensional fermionic systems in the first part we study quantum phase transitions and the nature of currents in onedimensional systems using field theoretic techniques like bosonization and renormalization group this involves the study of ... | [['in', 'this', 'thesis', 'we', 'study', 'quantum', 'phase', 'transitions', 'and', 'topological', 'phases', 'in', 'low', 'dimensional', 'fermionic', 'systems', 'in', 'the', 'first', 'part', 'we', 'study', 'quantum', 'phase', 'transitions', 'and', 'the', 'nature', 'of', 'currents', 'in', 'onedimensional', 'systems', 'us... | [-0.22677797503187924, 0.18071436583508746, -0.07059124299117552, 0.019133611164210182, -0.02333512347447324, -0.12471488354138914, 0.08633013695256465, 0.32883849214530825, -0.2156783240422645, -0.23278250912966814, 0.0895315337265055, -0.28277411919878553, -0.18777165504490928, 0.1346208513147376, 0.01435204701488499... |
1,803.05961 | Chiron: Privacy-preserving Machine Learning as a Service | Major cloud operators offer machine learning (ML) as a service, enabling
customers who have the data but not ML expertise or infrastructure to train
predictive models on this data. Existing ML-as-a-service platforms require
users to reveal all training data to the service operator. We design,
implement, and evaluate ... | cs.CR | major cloud operators offer machine learning ml as a service enabling customers who have the data but not ml expertise or infrastructure to train predictive models on this data existing mlasaservice platforms require users to reveal all training data to the service operator we design implement and evaluate chiron a sys... | [['major', 'cloud', 'operators', 'offer', 'machine', 'learning', 'ml', 'as', 'a', 'service', 'enabling', 'customers', 'who', 'have', 'the', 'data', 'but', 'not', 'ml', 'expertise', 'or', 'infrastructure', 'to', 'train', 'predictive', 'models', 'on', 'this', 'data', 'existing', 'mlasaservice', 'platforms', 'require', 'u... | [-0.09514499113600222, -0.060432513643292725, -0.0748346729990129, 0.061462638355522424, -0.15640393905918362, -0.2792590566175998, 0.09559669913382295, 0.42039204735325975, -0.26605085192308037, -0.36322634218585326, 0.11709448123552864, -0.2883078575288074, -0.0856744322505002, 0.20949771872469558, -0.125437722624698... |
1,803.05962 | B Anomalies and Leptoquarks at the LHC: Beyond the Lepton-Quark Final
State | Leptoquarks provide some of the simplest explanations to the hints of lepton
flavor non-universality in $B$ decays. In particular, a new confining gauge
group can provide a natural and appealing origin for the leptoquarks. So far,
direct collider searches have been based on two body decays, namely to a quark
and a le... | hep-ph | leptoquarks provide some of the simplest explanations to the hints of lepton flavor nonuniversality in b decays in particular a new confining gauge group can provide a natural and appealing origin for the leptoquarks so far direct collider searches have been based on two body decays namely to a quark and a lepton we st... | [['leptoquarks', 'provide', 'some', 'of', 'the', 'simplest', 'explanations', 'to', 'the', 'hints', 'of', 'lepton', 'flavor', 'nonuniversality', 'in', 'b', 'decays', 'in', 'particular', 'a', 'new', 'confining', 'gauge', 'group', 'can', 'provide', 'a', 'natural', 'and', 'appealing', 'origin', 'for', 'the', 'leptoquarks',... | [-0.05771844628747673, 0.22812018073614568, -0.07198756677211232, 0.1778046927151961, -0.12265616696207754, -0.17294198655553403, 0.030566715995120185, 0.3061925694947281, -0.2267538920225155, -0.30530646721261645, 0.05112547140808836, -0.2767407752753746, -0.07078297242161728, 0.16460477428570872, 0.014472297446862344... |
1,803.05963 | Studying Invariances of Trained Convolutional Neural Networks | Convolutional Neural Networks (CNNs) define an exceptionally powerful class
of models for image classification, but the theoretical background and the
understanding of how invariances to certain transformations are learned is
limited. In a large scale screening with images modified by different affine
and nonaffine t... | cs.CV | convolutional neural networks cnns define an exceptionally powerful class of models for image classification but the theoretical background and the understanding of how invariances to certain transformations are learned is limited in a large scale screening with images modified by different affine and nonaffine transfo... | [['convolutional', 'neural', 'networks', 'cnns', 'define', 'an', 'exceptionally', 'powerful', 'class', 'of', 'models', 'for', 'image', 'classification', 'but', 'the', 'theoretical', 'background', 'and', 'the', 'understanding', 'of', 'how', 'invariances', 'to', 'certain', 'transformations', 'are', 'learned', 'is', 'limi... | [-0.06881047497569982, 0.08401996685879856, -0.06630695493160081, 0.08043018675276212, -0.13827207070287495, -0.1945322228961491, -0.00986687007216027, 0.423062374785779, -0.3332021513118571, -0.30987436918630484, 0.04466853111923214, -0.21043910808957805, -0.22486456695044163, 0.16506308549275947, -0.12349855074185938... |
1,803.05964 | Structure of X-ray emitting jets close to the launching site: from
embedded to disk-bearing sources | Several observations of stellar jets show evidence of X-ray emitting shocks
close to the launching site. In some cases, the shocked features appear to be
stationary, also for YSOs at different stages of evolution. We study the case
of HH 154, the jet originating from the embedded binary Class 0/I protostar IRS
5, and... | astro-ph.SR | several observations of stellar jets show evidence of xray emitting shocks close to the launching site in some cases the shocked features appear to be stationary also for ysos at different stages of evolution we study the case of hh 154 the jet originating from the embedded binary class 0i protostar irs 5 and the case ... | [['several', 'observations', 'of', 'stellar', 'jets', 'show', 'evidence', 'of', 'xray', 'emitting', 'shocks', 'close', 'to', 'the', 'launching', 'site', 'in', 'some', 'cases', 'the', 'shocked', 'features', 'appear', 'to', 'be', 'stationary', 'also', 'for', 'ysos', 'at', 'different', 'stages', 'of', 'evolution', 'we', '... | [-0.1028894132669827, 0.1505627582192494, -0.04600526873289277, 0.1163445305593421, -0.06313216034019614, -0.09061348115409502, -0.0026715528864583384, 0.4312071756873862, -0.23321507450055515, -0.2852378151158071, 0.049824960428557025, -0.255694021024902, 0.01849774698694506, 0.18163128611358664, 0.04673100579960396, ... |
1,803.05965 | On the Spectral Evolution of Helium-Atmosphere White Dwarfs Showing
Traces of Hydrogen | We present a detailed spectroscopic analysis of 115 helium-line (DB) and 28
cool, He-rich hydrogen-line (DA) white dwarfs based on atmosphere fits to
optical spectroscopy and photometry. We find that 63% of our DB population show
hydrogen lines, making them DBA stars. We also demonstrate the persistence of
pure DB wh... | astro-ph.SR | we present a detailed spectroscopic analysis of 115 heliumline db and 28 cool herich hydrogenline da white dwarfs based on atmosphere fits to optical spectroscopy and photometry we find that 63 of our db population show hydrogen lines making them dba stars we also demonstrate the persistence of pure db white dwarfs wit... | [['we', 'present', 'a', 'detailed', 'spectroscopic', 'analysis', 'of', '115', 'heliumline', 'db', 'and', '28', 'cool', 'herich', 'hydrogenline', 'da', 'white', 'dwarfs', 'based', 'on', 'atmosphere', 'fits', 'to', 'optical', 'spectroscopy', 'and', 'photometry', 'we', 'find', 'that', '63', 'of', 'our', 'db', 'population'... | [-0.054970816819899994, 0.18737861495608008, -0.03106011534232254, 0.09167190614409679, -0.07277392420872818, -0.08170901664957535, 0.13462532284105883, 0.4110751021326634, -0.1837224256131888, -0.3200888361683802, 0.07651807709133432, -0.2638106124001768, -0.07736524274846408, 0.19142787276538448, -0.08158203980399362... |
1,803.05966 | On entropy and intrinsic ergodicity of coded subshifts | Any coded subshift X defined by a set C of code words contains a subshift,
which we call L, consisting of limits of single code words. We show that when C
satisfies a unique decomposition property, the topological entropy h(X) of X is
determined completely by h(L) and the number of code words of each length. More
spe... | math.DS | any coded subshift x defined by a set c of code words contains a subshift which we call l consisting of limits of single code words we show that when c satisfies a unique decomposition property the topological entropy hx of x is determined completely by hl and the number of code words of each length more specifically w... | [['any', 'coded', 'subshift', 'x', 'defined', 'by', 'a', 'set', 'c', 'of', 'code', 'words', 'contains', 'a', 'subshift', 'which', 'we', 'call', 'l', 'consisting', 'of', 'limits', 'of', 'single', 'code', 'words', 'we', 'show', 'that', 'when', 'c', 'satisfies', 'a', 'unique', 'decomposition', 'property', 'the', 'topologi... | [-0.14877139516985544, 0.13255224132717558, -0.06870379368774593, 0.050181973563407416, -0.04167780354951641, -0.20274187735880592, 0.07075712406991183, 0.3443269808340119, -0.30536107955101344, -0.1943922300498733, 0.08350000664151074, -0.32051170479306684, -0.10678593067028228, 0.22088507525404566, -0.086025970946398... |
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