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 |
|---|---|---|---|---|---|---|
706.3314 | Structure of W3(OH) from Very High Spectral Resolution Observations of 5
Centimeter OH Masers | Recent studies of methanol and ground-state OH masers at very high spectral
resolution have shed new light on small-scale maser processes. The nearby
source W3(OH), which contains numerous bright masers in several different
transitions, provides an excellent laboratory for high spectral resolution
techniques. We pres... | astro-ph | recent studies of methanol and groundstate oh masers at very high spectral resolution have shed new light on smallscale maser processes the nearby source w3oh which contains numerous bright masers in several different transitions provides an excellent laboratory for high spectral resolution techniques we present a mode... | [['recent', 'studies', 'of', 'methanol', 'and', 'groundstate', 'oh', 'masers', 'at', 'very', 'high', 'spectral', 'resolution', 'have', 'shed', 'new', 'light', 'on', 'smallscale', 'maser', 'processes', 'the', 'nearby', 'source', 'w3oh', 'which', 'contains', 'numerous', 'bright', 'masers', 'in', 'several', 'different', '... | [-0.11643341726376813, 0.10204119225054815, -0.009420636296084976, 0.020838479082662575, -0.08133106571299457, -0.12452348624125566, -0.0016958095077978502, 0.47850376252306276, -0.16554172108374018, -0.3108851211514361, 0.07867917922235527, -0.24268228290279828, 0.020288007174524027, 0.18957077577539563, 0.02382524912... |
706.3315 | pi0 Fixed pT suppression and elliptic flow at LHC | Using a final state interaction model which describes the data on these two
observables, at RHIC, we make predictions at the LHC -- using the same
cross-section and pT-shift. The increase in the medium density between these
two energies (by a factor close to three) produces an increase of the fixed pT
pi0 suppression... | hep-ph | using a final state interaction model which describes the data on these two observables at rhic we make predictions at the lhc using the same crosssection and ptshift the increase in the medium density between these two energies by a factor close to three produces an increase of the fixed pt pi0 suppression by a factor... | [['using', 'a', 'final', 'state', 'interaction', 'model', 'which', 'describes', 'the', 'data', 'on', 'these', 'two', 'observables', 'at', 'rhic', 'we', 'make', 'predictions', 'at', 'the', 'lhc', 'using', 'the', 'same', 'crosssection', 'and', 'ptshift', 'the', 'increase', 'in', 'the', 'medium', 'density', 'between', 'th... | [-0.06824703233062544, 0.17724236039727906, -0.07707095817154781, 0.03166759371136626, 0.07169357750734145, -0.08757809364011115, 0.021235836387583702, 0.3416947614486245, -0.23054048693456658, -0.35658749232463766, 0.012665540091058409, -0.35469051653688605, 0.00805447094678653, 0.15582003284626725, 0.0906029900423053... |
706.3316 | Hadron beam test of a scintillating fibre tracker system for elastic
scattering and luminosity measurement in ATLAS | A scintillating fibre tracker is proposed to measure elastic proton
scattering at very small angles in the ATLAS experiment at CERN. The tracker
will be located in so-called Roman Pot units at a distance of 240 m on each
side of the ATLAS interaction point. An initial validation of the design
choices was achieved in ... | physics.ins-det | a scintillating fibre tracker is proposed to measure elastic proton scattering at very small angles in the atlas experiment at cern the tracker will be located in socalled roman pot units at a distance of 240 m on each side of the atlas interaction point an initial validation of the design choices was achieved in a bea... | [['a', 'scintillating', 'fibre', 'tracker', 'is', 'proposed', 'to', 'measure', 'elastic', 'proton', 'scattering', 'at', 'very', 'small', 'angles', 'in', 'the', 'atlas', 'experiment', 'at', 'cern', 'the', 'tracker', 'will', 'be', 'located', 'in', 'socalled', 'roman', 'pot', 'units', 'at', 'a', 'distance', 'of', '240', '... | [-0.06858231122238714, 0.1335162219979357, -0.1229341044441529, 0.03214127274807415, 0.00011070116984415545, -0.17081035734497152, -0.018082995238803225, 0.40099414772902653, -0.196552132996284, -0.344736554583356, 0.09114951043778852, -0.3120293101034293, -0.010816516544452983, 0.22363796815824732, -0.0153615245283007... |
706.3317 | Detecting phase synchronization by localized maps: Application to neural
networks | We present an approach which enables to state about the existence of phase
synchronization in coupled chaotic oscillators without having to measure the
phase. This is done by observing the oscillators at special times, and
analyzing whether this set of points is localized. In particular, we show that
this approach is... | cond-mat.stat-mech cond-mat.other | we present an approach which enables to state about the existence of phase synchronization in coupled chaotic oscillators without having to measure the phase this is done by observing the oscillators at special times and analyzing whether this set of points is localized in particular we show that this approach is fruit... | [['we', 'present', 'an', 'approach', 'which', 'enables', 'to', 'state', 'about', 'the', 'existence', 'of', 'phase', 'synchronization', 'in', 'coupled', 'chaotic', 'oscillators', 'without', 'having', 'to', 'measure', 'the', 'phase', 'this', 'is', 'done', 'by', 'observing', 'the', 'oscillators', 'at', 'special', 'times',... | [-0.20661282404843304, 0.18103774918841894, -0.04697319712880769, 0.001090631912243955, 0.011619720883943417, -0.15714368198848802, 0.09101899065807416, 0.3637581520863337, -0.24763565820952257, -0.26657333388280724, 0.09809004252109631, -0.23967513202022714, -0.24599895115803788, 0.1502130206697333, -0.064043540484559... |
706.3318 | Invariance of Gamma-dimension for projective families | This article is withdrawn because of a mistake in the main result of the
paper.
| math.AG math.CV | this article is withdrawn because of a mistake in the main result of the paper | [['this', 'article', 'is', 'withdrawn', 'because', 'of', 'a', 'mistake', 'in', 'the', 'main', 'result', 'of', 'the', 'paper']] | [-0.1344951432198286, -0.03212288456658522, -0.13723469669930638, -0.05327515477935473, -0.07392839429279169, 0.012353016467144092, 0.054972877237014474, 0.22857304612795512, -0.2815050592025121, -0.3224473816653093, 0.07905655667030563, -0.2462412018328905, -0.22825543880462645, 0.10643296279013156, -0.337539312181373... |
706.3319 | On the Photon Mass | We review the case for the photon having a tiny mass compatible with the
experimental limits. We go over some possible experimental tests for such a
photon mass including the violation of Lorentz symmetry. We point out that such
violations may already have been witnessed in tests involving high energy gamma
rays from... | physics.gen-ph | we review the case for the photon having a tiny mass compatible with the experimental limits we go over some possible experimental tests for such a photon mass including the violation of lorentz symmetry we point out that such violations may already have been witnessed in tests involving high energy gamma rays from out... | [['we', 'review', 'the', 'case', 'for', 'the', 'photon', 'having', 'a', 'tiny', 'mass', 'compatible', 'with', 'the', 'experimental', 'limits', 'we', 'go', 'over', 'some', 'possible', 'experimental', 'tests', 'for', 'such', 'a', 'photon', 'mass', 'including', 'the', 'violation', 'of', 'lorentz', 'symmetry', 'we', 'point... | [-0.10125058231454703, 0.20243755218783213, -0.04971458443680838, 0.10767859812345236, -0.06717653897020125, -0.06214027150323795, 0.07835188384858831, 0.38403163153317665, -0.193402579850367, -0.34104740319232785, 0.07496133117538487, -0.31535078187082566, -0.02095173073992614, 0.2739109261742523, 0.005079335668274472... |
706.332 | General Framework for phase synchronization through localized sets | We present an approach which enables to identify phase synchronization in
coupled chaotic oscillators without having to explicitly measure the phase. We
show that if one defines a typical event in one oscillator and then observes
another one whenever this event occurs, these observations give rise to a
localized set.... | cond-mat.stat-mech | we present an approach which enables to identify phase synchronization in coupled chaotic oscillators without having to explicitly measure the phase we show that if one defines a typical event in one oscillator and then observes another one whenever this event occurs these observations give rise to a localized set our ... | [['we', 'present', 'an', 'approach', 'which', 'enables', 'to', 'identify', 'phase', 'synchronization', 'in', 'coupled', 'chaotic', 'oscillators', 'without', 'having', 'to', 'explicitly', 'measure', 'the', 'phase', 'we', 'show', 'that', 'if', 'one', 'defines', 'a', 'typical', 'event', 'in', 'one', 'oscillator', 'and', '... | [-0.17578732981704748, 0.16341370041761996, -0.09387838576311389, 0.043178597903953723, -0.05274784935889049, -0.17755611806463165, 0.06639714600124325, 0.38927072661284073, -0.28354150084062263, -0.28323003779022166, 0.060842144482124313, -0.2564975285257858, -0.2226811759532071, 0.18334354907274247, -0.04245632694890... |
706.3321 | Elastoplastic model for the dynamics of solid-solid transformations :
role of non-affine deformation in microstructure selection | We study the nucleation dynamics of a model solid state transformation and
the criterion for microstructure selection using a molecular dynamics (MD)
simulation. Our simulations show a range of microstructures depending on the
depth of quench. We closely follow the dynamics of the solid and find that
transient {\em n... | cond-mat.mtrl-sci | we study the nucleation dynamics of a model solid state transformation and the criterion for microstructure selection using a molecular dynamics md simulation our simulations show a range of microstructures depending on the depth of quench we closely follow the dynamics of the solid and find that transient em nonaffine... | [['we', 'study', 'the', 'nucleation', 'dynamics', 'of', 'a', 'model', 'solid', 'state', 'transformation', 'and', 'the', 'criterion', 'for', 'microstructure', 'selection', 'using', 'a', 'molecular', 'dynamics', 'md', 'simulation', 'our', 'simulations', 'show', 'a', 'range', 'of', 'microstructures', 'depending', 'on', 't... | [-0.10124243761144452, 0.15241259801849205, -0.1493478775530278, 0.01583500384349155, -0.0324344358099151, -0.08793219030238845, 0.018972931209491898, 0.3856767442203679, -0.33062353603920697, -0.253997343120765, 0.07501733646495268, -0.23743781778109024, -0.20113649990378044, 0.13686880234321105, 0.029599563439645, 0.... |
706.3322 | Distance distribution in random graphs and application to networks
exploration | We consider the problem of determining the proportion of edges that are
discovered in an Erdos-Renyi graph when one constructs all shortest paths from
a given source node to all other nodes. This problem is equivalent to the one
of determining the proportion of edges connecting nodes that are at identical
distance fr... | cond-mat.stat-mech cond-mat.dis-nn | we consider the problem of determining the proportion of edges that are discovered in an erdosrenyi graph when one constructs all shortest paths from a given source node to all other nodes this problem is equivalent to the one of determining the proportion of edges connecting nodes that are at identical distance from t... | [['we', 'consider', 'the', 'problem', 'of', 'determining', 'the', 'proportion', 'of', 'edges', 'that', 'are', 'discovered', 'in', 'an', 'erdosrenyi', 'graph', 'when', 'one', 'constructs', 'all', 'shortest', 'paths', 'from', 'a', 'given', 'source', 'node', 'to', 'all', 'other', 'nodes', 'this', 'problem', 'is', 'equival... | [-0.172821308001573, 0.07843924801509422, -0.06600780376589031, 0.016113569334384084, -0.07488175714009904, -0.12825304253511433, 0.09665386955825446, 0.3646171954346866, -0.2807688119677388, -0.3279302007579283, 0.03240775153215036, -0.3550761485818018, -0.16690749453941012, 0.13843743378917375, -0.03333337941941449, ... |
706.3323 | Onset of Phase Synchronization in Neurons Conneted via Chemical Synapses | We study the onset of synchronous states in realistic chaotic neurons coupled
by mutually inhibitory chemical synapses. For the realistic parameters, namely
the synaptic strength and the intrinsic current, this synapse introduces
non-coherences in the neuronal dynamics, yet allowing for chaotic phase
synchronization ... | cond-mat.stat-mech | we study the onset of synchronous states in realistic chaotic neurons coupled by mutually inhibitory chemical synapses for the realistic parameters namely the synaptic strength and the intrinsic current this synapse introduces noncoherences in the neuronal dynamics yet allowing for chaotic phase synchronization in a la... | [['we', 'study', 'the', 'onset', 'of', 'synchronous', 'states', 'in', 'realistic', 'chaotic', 'neurons', 'coupled', 'by', 'mutually', 'inhibitory', 'chemical', 'synapses', 'for', 'the', 'realistic', 'parameters', 'namely', 'the', 'synaptic', 'strength', 'and', 'the', 'intrinsic', 'current', 'this', 'synapse', 'introduc... | [-0.23393605473478707, 0.23358207810944057, 0.060359806698911334, 0.04230527305865989, -0.018276162938598323, -0.18309486187610993, 0.1005501011694672, 0.3625650060883559, -0.23632404909414403, -0.24663649482981248, 0.019587955014739075, -0.19189321651013896, -0.3010526435203193, 0.14965680599219494, -0.043505982413668... |
706.3324 | Network Mutual Information and Synchronization under Time
Transformations | We investigate the effect of general time transformations on the phase
synchronization (PS) phenomenon and the mutual information rate (MIR) between
pairs of nodes in dynamical networks. We demonstrate two important results
concerning the invariance of both PS and the MIR. Under time transformations PS
can neither be... | cond-mat.stat-mech | we investigate the effect of general time transformations on the phase synchronization ps phenomenon and the mutual information rate mir between pairs of nodes in dynamical networks we demonstrate two important results concerning the invariance of both ps and the mir under time transformations ps can neither be introdu... | [['we', 'investigate', 'the', 'effect', 'of', 'general', 'time', 'transformations', 'on', 'the', 'phase', 'synchronization', 'ps', 'phenomenon', 'and', 'the', 'mutual', 'information', 'rate', 'mir', 'between', 'pairs', 'of', 'nodes', 'in', 'dynamical', 'networks', 'we', 'demonstrate', 'two', 'important', 'results', 'co... | [-0.16353026818127392, 0.14950771347193562, -0.08983441044952958, 0.05882037336878637, -0.013835634639922609, -0.11309339702773363, 0.08642765985643293, 0.4219210262093297, -0.2848247155705665, -0.27993975177486524, 0.12717515428580264, -0.22634055569490535, -0.17596734444947637, 0.19796754205797581, -0.070311767467733... |
706.3325 | Global Bifurcation Destroying The Experimental Torus T2 | We show experimentally the scenario of a two-frequency torus $T^2$ breakdown,
in which a global bifurcation occurs due to the collision of a torus with an
unstable periodic orbit, creating a heteroclinic saddle connection, followed by
an intermittent behavior.
| nlin.CD | we show experimentally the scenario of a twofrequency torus t2 breakdown in which a global bifurcation occurs due to the collision of a torus with an unstable periodic orbit creating a heteroclinic saddle connection followed by an intermittent behavior | [['we', 'show', 'experimentally', 'the', 'scenario', 'of', 'a', 'twofrequency', 'torus', 't2', 'breakdown', 'in', 'which', 'a', 'global', 'bifurcation', 'occurs', 'due', 'to', 'the', 'collision', 'of', 'a', 'torus', 'with', 'an', 'unstable', 'periodic', 'orbit', 'creating', 'a', 'heteroclinic', 'saddle', 'connection', ... | [-0.32969331860733336, 0.144882675744623, -0.13843139172651064, 0.06886466406285763, -0.017651685250875276, -0.1686101642270119, 0.08668949216819154, 0.30446174862579656, -0.2925826611045079, -0.1660321753901931, 0.11805318458041605, -0.19822834534809375, -0.22326249342698318, 0.19622491863675606, -0.06142540930364376,... |
706.3326 | Three-qubit pure-state canonical forms for Perfect Teleportation | Recently, Agrawal and Pati [Phys. Rev. A 74, 062320 (2006)] have given a
class of W-states that can be used for perfect teleportation. Here, two
canonical forms of perfect quantum channel are presented by transformation
operator and the GHZ state and the W state are special case of those two
canonical forms of perfec... | quant-ph | recently agrawal and pati phys rev a 74 062320 2006 have given a class of wstates that can be used for perfect teleportation here two canonical forms of perfect quantum channel are presented by transformation operator and the ghz state and the w state are special case of those two canonical forms of perfect quantum cha... | [['recently', 'agrawal', 'and', 'pati', 'phys', 'rev', 'a', '74', '062320', '2006', 'have', 'given', 'a', 'class', 'of', 'wstates', 'that', 'can', 'be', 'used', 'for', 'perfect', 'teleportation', 'here', 'two', 'canonical', 'forms', 'of', 'perfect', 'quantum', 'channel', 'are', 'presented', 'by', 'transformation', 'ope... | [-0.14085638073447626, 0.1559774438937893, -0.040108177898218855, -0.06191932025831193, -0.056725304952124134, -0.200601749602356, 0.038913932447030675, 0.3638069839653326, -0.18820663443511876, -0.2697998089133762, 0.03567617719818372, -0.24793885594044696, -0.13639401112959604, 0.2000274714664556, -0.0639423062311834... |
706.3327 | Analytical Bethe Ansatz for closed and open gl(M|N) super-spin chains in
arbitrary representations and for any Dynkin diagram | We present the analytical Bethe ansatz for spin chains based on the
superalgebras gl(M|N), $M\neq N$, with at each site an arbitrary representation
(and including inhomogeneities).
The calculation is done for closed and open spin chains. In this latter case,
the boundary matrices $K_{\pm}(u)$ are of general type, p... | hep-th | we present the analytical bethe ansatz for spin chains based on the superalgebras glmn mneq n with at each site an arbitrary representation and including inhomogeneities the calculation is done for closed and open spin chains in this latter case the boundary matrices k_pmu are of general type provided they commute we c... | [['we', 'present', 'the', 'analytical', 'bethe', 'ansatz', 'for', 'spin', 'chains', 'based', 'on', 'the', 'superalgebras', 'glmn', 'mneq', 'n', 'with', 'at', 'each', 'site', 'an', 'arbitrary', 'representation', 'and', 'including', 'inhomogeneities', 'the', 'calculation', 'is', 'done', 'for', 'closed', 'and', 'open', 's... | [-0.16076025351680615, 0.08398123256208508, -0.013438029422399562, 0.09545591320666308, -0.08940502909339361, -0.18904904082316804, 0.019701154282744472, 0.378902253770345, -0.21170869039220586, -0.20365452447377547, 0.1231592940135129, -0.2766758778409378, -0.10937906561004049, 0.17414835420109936, 0.01906700975676948... |
706.3328 | The spatial distribution of substellar objects in IC348 and the Orion
Trapezium Cluster | Aims: Some theoretical scenarios suggest the formation of brown dwarfs as
ejected stellar embryos in star-forming clusters. Such a formation mechanism
can result in different spatial distributions of stars and substellar objects.
We aim to investigate the spatial structure of stellar and substellar objects
in two wel... | astro-ph | aims some theoretical scenarios suggest the formation of brown dwarfs as ejected stellar embryos in starforming clusters such a formation mechanism can result in different spatial distributions of stars and substellar objects we aim to investigate the spatial structure of stellar and substellar objects in two well samp... | [['aims', 'some', 'theoretical', 'scenarios', 'suggest', 'the', 'formation', 'of', 'brown', 'dwarfs', 'as', 'ejected', 'stellar', 'embryos', 'in', 'starforming', 'clusters', 'such', 'a', 'formation', 'mechanism', 'can', 'result', 'in', 'different', 'spatial', 'distributions', 'of', 'stars', 'and', 'substellar', 'object... | [-0.06699149387164248, 0.15162563229635082, -0.09966844071017544, 0.1382877827492646, -0.10965351437701396, -0.05721154713106376, 0.09145865495558138, 0.42716072980159275, -0.20581814937866982, -0.35995327626286006, 0.05993451379041222, -0.22646675043980832, -0.044630731225738095, 0.1474265198811837, -0.074233114980301... |
706.3329 | Dirac Cat States in Relativistic Landau Levels | We show that a relativistic version of Schrodinger cat states, here called
Dirac cat states, can be built in relativistic Landau levels when an external
magnetic field couples to a relativistic spin 1/2 charged particle. Under
suitable initial conditions, the associated Dirac equation produces unitarily
Dirac cat sta... | quant-ph cond-mat.mes-hall hep-th | we show that a relativistic version of schrodinger cat states here called dirac cat states can be built in relativistic landau levels when an external magnetic field couples to a relativistic spin 12 charged particle under suitable initial conditions the associated dirac equation produces unitarily dirac cat states inv... | [['we', 'show', 'that', 'a', 'relativistic', 'version', 'of', 'schrodinger', 'cat', 'states', 'here', 'called', 'dirac', 'cat', 'states', 'can', 'be', 'built', 'in', 'relativistic', 'landau', 'levels', 'when', 'an', 'external', 'magnetic', 'field', 'couples', 'to', 'a', 'relativistic', 'spin', '12', 'charged', 'particl... | [-0.12890699662624255, 0.28012451704482516, -0.12716863043241056, 0.12414023322943489, -0.01715923027436742, -0.19071926244114543, -0.02806627317833915, 0.32780740994448754, -0.24204141928759568, -0.26257446771670206, -0.03808563622171242, -0.26899459150930244, -0.10976284747833714, 0.15819585605013167, -0.015035969830... |
706.333 | Coherent structures in localised and global pipe turbulence | The recent discovery of unstable travelling waves (TWs) in pipe flow has been
hailed as a significant breakthrough with the hope that they populate the
turbulent attractor. We confirm the existence of coherent states with internal
fast and slow streaks commensurate in both structure and energy with known TWs
using nu... | physics.flu-dyn | the recent discovery of unstable travelling waves tws in pipe flow has been hailed as a significant breakthrough with the hope that they populate the turbulent attractor we confirm the existence of coherent states with internal fast and slow streaks commensurate in both structure and energy with known tws using numeric... | [['the', 'recent', 'discovery', 'of', 'unstable', 'travelling', 'waves', 'tws', 'in', 'pipe', 'flow', 'has', 'been', 'hailed', 'as', 'a', 'significant', 'breakthrough', 'with', 'the', 'hope', 'that', 'they', 'populate', 'the', 'turbulent', 'attractor', 'we', 'confirm', 'the', 'existence', 'of', 'coherent', 'states', 'w... | [-0.17061144140097895, 0.27170372333341675, -0.07486026067635976, 0.06558069749280548, -0.0168948613008979, -0.09216660278798372, 0.012101561325835064, 0.3303247109138283, -0.2649183272078517, -0.2837573327778955, 0.08931232359191199, -0.21598924768477445, -0.09350560409075115, 0.20069820130811422, 0.007724146454847869... |
706.3331 | A Model for Counterparty Risk with Geometric Attenuation Effect and the
Valuation of CDS | In this paper, a geometric function is introduced to reflect the attenuation
speed of impact of one firm's default to its partner. If two firms are
competitions (copartners), the default intensity of one firm will decrease
(increase) abruptly when the other firm defaults. As time goes on, the impact
will decrease gra... | q-fin.RM math.PR | in this paper a geometric function is introduced to reflect the attenuation speed of impact of one firms default to its partner if two firms are competitions copartners the default intensity of one firm will decrease increase abruptly when the other firm defaults as time goes on the impact will decrease gradually until... | [['in', 'this', 'paper', 'a', 'geometric', 'function', 'is', 'introduced', 'to', 'reflect', 'the', 'attenuation', 'speed', 'of', 'impact', 'of', 'one', 'firms', 'default', 'to', 'its', 'partner', 'if', 'two', 'firms', 'are', 'competitions', 'copartners', 'the', 'default', 'intensity', 'of', 'one', 'firm', 'will', 'decr... | [-0.06211024442953723, 0.14841337473176064, -0.09893478587314132, 0.10836823650918502, -0.05946466801376681, -0.12592656547314532, 0.14560869315201194, 0.41423644764082773, -0.2914740490239291, -0.2871587371586689, 0.1322622161935128, -0.3147831977389398, -0.046495700659718184, 0.10484699517699136, -0.11343616288199666... |
706.3332 | X-ray flares on the UV Ceti-type star CC Eridani: a "peculiar"
time-evolution of spectral parameters | Context: Weak flares are supposed to be an important heating agent of the
outer layers of stellar atmospheres. However, due to instrumental limitations,
only large X-ray flares have been studied in detail until now.
Aims: We used an XMM-Newton observation of the very active BY-Dra type binary
star CC Eri in order t... | astro-ph | context weak flares are supposed to be an important heating agent of the outer layers of stellar atmospheres however due to instrumental limitations only large xray flares have been studied in detail until now aims we used an xmmnewton observation of the very active bydra type binary star cc eri in order to investigate... | [['context', 'weak', 'flares', 'are', 'supposed', 'to', 'be', 'an', 'important', 'heating', 'agent', 'of', 'the', 'outer', 'layers', 'of', 'stellar', 'atmospheres', 'however', 'due', 'to', 'instrumental', 'limitations', 'only', 'large', 'xray', 'flares', 'have', 'been', 'studied', 'in', 'detail', 'until', 'now', 'aims'... | [-0.08028368207340805, 0.1762575317833382, -0.04003331853966899, 0.14508600272384312, -0.05370554281398654, -0.11444928607563196, 0.04879355484831733, 0.42031129584493065, -0.17223719916412972, -0.3812114876090133, 0.08600953457889068, -0.2908651595557198, -0.05382646212261514, 0.24588929172227247, -0.05598202046707987... |
706.3333 | Computer-assisted access to the kidney | OBJECTIVES: The aim of this paper is to introduce the principles of
computer-assisted access to the kidney. The system provides the surgeon with a
pre-operative 3D planning on computed tomography (CT) images. After a rigid
registration with space-localized ultrasound (US) data, preoperative planning
can be transferre... | physics.med-ph | objectives the aim of this paper is to introduce the principles of computerassisted access to the kidney the system provides the surgeon with a preoperative 3d planning on computed tomography ct images after a rigid registration with spacelocalized ultrasound us data preoperative planning can be transferred to the intr... | [['objectives', 'the', 'aim', 'of', 'this', 'paper', 'is', 'to', 'introduce', 'the', 'principles', 'of', 'computerassisted', 'access', 'to', 'the', 'kidney', 'the', 'system', 'provides', 'the', 'surgeon', 'with', 'a', 'preoperative', '3d', 'planning', 'on', 'computed', 'tomography', 'ct', 'images', 'after', 'a', 'rigid... | [-0.029607007880541804, -0.005954559166650121, -0.11629238499964248, 0.03286512289196253, -0.09319977976610427, -0.1336055600731271, 0.07120595160316855, 0.43060738291078343, -0.17673399015524965, -0.3406210092125003, 0.12944152224585861, -0.2888128248596331, -0.10013340265785683, 0.2397862261950323, -0.133771566147107... |
706.3334 | Radius and profile of random planar maps with faces of arbitrary degrees | We prove some asymptotic results for the radius and the profile of large
random rooted planar maps with faces of arbitrary degrees. Using a bijection
due to Bouttier, Di Francesco and Guitter between rooted planar maps and
certain four-type trees with positive labels, we derive our results from a
conditional limit th... | math.PR | we prove some asymptotic results for the radius and the profile of large random rooted planar maps with faces of arbitrary degrees using a bijection due to bouttier di francesco and guitter between rooted planar maps and certain fourtype trees with positive labels we derive our results from a conditional limit theorem ... | [['we', 'prove', 'some', 'asymptotic', 'results', 'for', 'the', 'radius', 'and', 'the', 'profile', 'of', 'large', 'random', 'rooted', 'planar', 'maps', 'with', 'faces', 'of', 'arbitrary', 'degrees', 'using', 'a', 'bijection', 'due', 'to', 'bouttier', 'di', 'francesco', 'and', 'guitter', 'between', 'rooted', 'planar', '... | [-0.10276970527085819, 0.13183029781079345, -0.05399819192264164, 0.0628510828603778, -0.07408593751882252, -0.11945216759647194, 0.08560734454607755, 0.33169535011575935, -0.22406602951109802, -0.2750674568182021, 0.08635245727603896, -0.309706699103117, -0.18464226628604688, 0.15518914342841558, -0.13945819895812556,... |
706.3335 | Filtering and estimation in stochastic volatility models with rationally
distributed disturbances | This paper deals with the filtering problem for a class of discrete time
stochastic volatility models in which the disturbances have rational
probability density functions. This includes the Cauchy distributions and
Student t-distributions with odd number of degrees of freedom. Using state
space realizations to repre... | math.OC math.ST stat.TH | this paper deals with the filtering problem for a class of discrete time stochastic volatility models in which the disturbances have rational probability density functions this includes the cauchy distributions and student tdistributions with odd number of degrees of freedom using state space realizations to represent ... | [['this', 'paper', 'deals', 'with', 'the', 'filtering', 'problem', 'for', 'a', 'class', 'of', 'discrete', 'time', 'stochastic', 'volatility', 'models', 'in', 'which', 'the', 'disturbances', 'have', 'rational', 'probability', 'density', 'functions', 'this', 'includes', 'the', 'cauchy', 'distributions', 'and', 'student',... | [-0.10295243618454326, 0.08553302195740112, -0.08045355442159793, 0.07412814721669349, -0.048285911913569034, -0.09165328649983726, 0.031867398842638194, 0.3722555124968813, -0.2925431329528229, -0.27766150100924597, 0.08954790680926587, -0.2536640642537621, -0.16387795427152396, 0.12630562754266225, -0.057656324068247... |
706.3336 | Corps de nombres peu ramifies et formes automorphes autoduales | Let S be a finite set of primes, p in S, and Q_S a maximal algebraic
extension of Q unramified outside S and infinity. Assume that |S|>=2. We show
that the natural maps Gal(Q_p^bar/Q_p) --> Gal(Q_S/Q) are injective. Much of
the paper is devoted to the problem of constructing selfdual automorphic
cuspidal representati... | math.NT math.RT | let s be a finite set of primes p in s and q_s a maximal algebraic extension of q unramified outside s and infinity assume that s2 we show that the natural maps galq_pbarq_p galq_sq are injective much of the paper is devoted to the problem of constructing selfdual automorphic cuspidal representations of gl2na_q with pr... | [['let', 's', 'be', 'a', 'finite', 'set', 'of', 'primes', 'p', 'in', 's', 'and', 'q_s', 'a', 'maximal', 'algebraic', 'extension', 'of', 'q', 'unramified', 'outside', 's', 'and', 'infinity', 'assume', 'that', 's2', 'we', 'show', 'that', 'the', 'natural', 'maps', 'galq_pbarq_p', 'galq_sq', 'are', 'injective', 'much', 'of... | [-0.1969828342878108, 0.10726325565862448, -0.14636547355046278, 0.06699553956846209, -0.1102647861346689, -0.13858700925376005, 0.011651657750494345, 0.28991577308624983, -0.29113938715742077, -0.1901436966713951, 0.08837849748467073, -0.2690709822988517, -0.14198321253223734, 0.20430918494347744, -0.09070973559336867... |
706.3337 | Quasifinite representations of the Lie superalgebra of quantum pseudo
differential operators | In this paper we extend general results obtained by V. Kac and J. Liberati,
in "Unitary quasifinite representations of $W_\infty$", (Letters Math. Phys.,
53 (2000), 11-27), for quasifinite highest weight representations of
$\Z$-graded Lie algebras to ${1/2}\Z$-graded Lie superalgebras, and we apply
these to classify ... | math-ph math.MP | in this paper we extend general results obtained by v kac and j liberati in unitary quasifinite representations of w_infty letters math phys 53 2000 1127 for quasifinite highest weight representations of zgraded lie algebras to 12zgraded lie superalgebras and we apply these to classify the irreducible quasifinite highe... | [['in', 'this', 'paper', 'we', 'extend', 'general', 'results', 'obtained', 'by', 'v', 'kac', 'and', 'j', 'liberati', 'in', 'unitary', 'quasifinite', 'representations', 'of', 'w_infty', 'letters', 'math', 'phys', '53', '2000', '1127', 'for', 'quasifinite', 'highest', 'weight', 'representations', 'of', 'zgraded', 'lie', ... | [-0.14152430442707806, 0.07245774860172693, 0.01329544331107674, -0.03798954641438443, -0.17542787978891283, -0.15718992980164959, -0.0010176292110780447, 0.4043662688566436, -0.3176572111531578, -0.17875098373644568, 0.03727476531037547, -0.23763458246108274, -0.13986870734791818, 0.1574284961398948, -0.18612810953295... |
706.3338 | On the residual finiteness and other properties of (relative)
one-relator groups | A relative one-relator presentation has the form P = < X,H ; R > where X is a
set, H is a group, and R is a group word on X and H. We show that if the group
word on X obtained from R by deleting all the terms from H has what we call the
unique max-min property, then the group defined by P is residually finite if
and ... | math.GR | a relative onerelator presentation has the form p xh r where x is a set h is a group and r is a group word on x and h we show that if the group word on x obtained from r by deleting all the terms from h has what we call the unique maxmin property then the group defined by p is residually finite if and only if h is resi... | [['a', 'relative', 'onerelator', 'presentation', 'has', 'the', 'form', 'p', 'xh', 'r', 'where', 'x', 'is', 'a', 'set', 'h', 'is', 'a', 'group', 'and', 'r', 'is', 'a', 'group', 'word', 'on', 'x', 'and', 'h', 'we', 'show', 'that', 'if', 'the', 'group', 'word', 'on', 'x', 'obtained', 'from', 'r', 'by', 'deleting', 'all', ... | [-0.13560860175169817, 0.12042715385978837, -0.12846536300450312, 0.04279946080729866, -0.0698783042754571, -0.1422378497526926, 0.06486333458206985, 0.3630450309074226, -0.32674597304690034, -0.23368341467507622, 0.10622702836315344, -0.3121496552382322, -0.09080874114179936, 0.20798566720072775, -0.13285983944734356,... |
706.3339 | Redshifted formaldehyde from the gravitational lens B0218+357 | The gravitational lens toward B0218+357 offers the unique possibility to
study cool moderately dense gas with high sensitivity and angular resolution in
a cloud that existed half a Hubble time ago. Observations of the radio
continuum and six formaldehyde (H2CO) lines were carried out with the VLA, the
Plateau de Bure... | astro-ph | the gravitational lens toward b0218357 offers the unique possibility to study cool moderately dense gas with high sensitivity and angular resolution in a cloud that existed half a hubble time ago observations of the radio continuum and six formaldehyde h2co lines were carried out with the vla the plateau de bure interf... | [['the', 'gravitational', 'lens', 'toward', 'b0218357', 'offers', 'the', 'unique', 'possibility', 'to', 'study', 'cool', 'moderately', 'dense', 'gas', 'with', 'high', 'sensitivity', 'and', 'angular', 'resolution', 'in', 'a', 'cloud', 'that', 'existed', 'half', 'a', 'hubble', 'time', 'ago', 'observations', 'of', 'the', ... | [-0.08524336944632395, 0.10704828670841698, -0.0007336236781587726, 0.03192680187588721, -0.007633861912038634, -0.08590958901403244, 0.04069348632995235, 0.43898165628248664, -0.13358554455304616, -0.35300676710576867, 0.061910611825071994, -0.282108387481748, 0.011216302861111329, 0.1348977593770414, 0.05065961633400... |
706.334 | Visualization of ferromagnetic domains in TbNi$_2$B$_2$C and
ErNi$_2$B$_2$C single crystals: Weak ferromagnetism and its coexistence with
superconductivity | The magnetic flux structure in the basal plane, (001), of single crystals of
superconducting (R = Er) and non-superconducting (R = Tb) RNi$_2$B$_2$C was
studied by high resolution Bitter decoration at temperatures below $T_c$
(superconducting transition) and/or $T_N$ (antiferromagnetic transition). For
both materials... | cond-mat.supr-con | the magnetic flux structure in the basal plane 001 of single crystals of superconducting r er and nonsuperconducting r tb rni_2b_2c was studied by high resolution bitter decoration at temperatures below t_c superconducting transition andor t_n antiferromagnetic transition for both materials two sets of domain boundarie... | [['the', 'magnetic', 'flux', 'structure', 'in', 'the', 'basal', 'plane', '001', 'of', 'single', 'crystals', 'of', 'superconducting', 'r', 'er', 'and', 'nonsuperconducting', 'r', 'tb', 'rni_2b_2c', 'was', 'studied', 'by', 'high', 'resolution', 'bitter', 'decoration', 'at', 'temperatures', 'below', 't_c', 'superconductin... | [-0.18822887572960173, 0.29917670825057596, 0.061999000957204904, 0.01344078807795251, -0.052911548990725484, -0.1278265603194552, 0.11394238915325196, 0.44960423309571484, -0.242764867803713, -0.31339934331649716, 0.07082915156483188, -0.36475960545488134, -0.008214618450738797, 0.14139519652066954, 0.0829449523863775... |
706.3341 | A Sequent Calculus for Modelling Interferences | A logic calculus is presented that is a conservative extension of linear
logic. The motivation beneath this work concerns lazy evaluation, true
concurrency and interferences in proof search. The calculus includes two new
connectives to deal with multisequent structures and has the cut-elimination
property. Extensions... | cs.LO | a logic calculus is presented that is a conservative extension of linear logic the motivation beneath this work concerns lazy evaluation true concurrency and interferences in proof search the calculus includes two new connectives to deal with multisequent structures and has the cutelimination property extensions are pr... | [['a', 'logic', 'calculus', 'is', 'presented', 'that', 'is', 'a', 'conservative', 'extension', 'of', 'linear', 'logic', 'the', 'motivation', 'beneath', 'this', 'work', 'concerns', 'lazy', 'evaluation', 'true', 'concurrency', 'and', 'interferences', 'in', 'proof', 'search', 'the', 'calculus', 'includes', 'two', 'new', '... | [-0.1361886358134589, 0.007819833321813142, -0.10729915543266062, 0.1271703681087051, -0.20625616694396398, -0.1517447558811532, 0.034205114047201175, 0.32623998877012506, -0.2774178205005262, -0.2771805859575013, 0.08636902617773849, -0.2531372608862958, -0.16449573868226683, 0.18203190479972312, -0.1881727511195009, ... |
706.3342 | The Forgotten Night: The Number Devil Explores Spherical Geometry | This is a missing chapter from Hans Magnus Enzensberger's mathematical
adventure The Number Devil (Henry Holt and Company, New York, 1997). In the
book, a math-hating boy named Robert is visited in his dreams by the clever
Number Devil, who teaches him to love all things numerical. However, we all
forget our dreams f... | math.HO physics.ed-ph | this is a missing chapter from hans magnus enzensbergers mathematical adventure the number devil henry holt and company new york 1997 in the book a mathhating boy named robert is visited in his dreams by the clever number devil who teaches him to love all things numerical however we all forget our dreams from time to t... | [['this', 'is', 'a', 'missing', 'chapter', 'from', 'hans', 'magnus', 'enzensbergers', 'mathematical', 'adventure', 'the', 'number', 'devil', 'henry', 'holt', 'and', 'company', 'new', 'york', '1997', 'in', 'the', 'book', 'a', 'mathhating', 'boy', 'named', 'robert', 'is', 'visited', 'in', 'his', 'dreams', 'by', 'the', 'c... | [-0.11805023175732392, 0.10076490445516822, -0.1358004692748825, 0.05077904303666068, -0.23373088536488756, -0.15317607956097984, 0.05362019864501568, 0.2376503781415522, -0.2448232520553397, -0.37259942247736744, 0.09853176675629007, -0.31113346136549896, -0.21537602438432416, 0.18827337678521872, -0.23242912162663187... |
706.3343 | Flocking in noisy environments | We consider a perturbed version of the dynamics of a flock introduced by
Cucker and Smale ("Emergent behaviour in flocks") and prove, under similar
conditions, that nearly-alignment (a concept that is precised in the text) is
achieved with a certain probability, bounded from below.
| math.DS math.PR | we consider a perturbed version of the dynamics of a flock introduced by cucker and smale emergent behaviour in flocks and prove under similar conditions that nearlyalignment a concept that is precised in the text is achieved with a certain probability bounded from below | [['we', 'consider', 'a', 'perturbed', 'version', 'of', 'the', 'dynamics', 'of', 'a', 'flock', 'introduced', 'by', 'cucker', 'and', 'smale', 'emergent', 'behaviour', 'in', 'flocks', 'and', 'prove', 'under', 'similar', 'conditions', 'that', 'nearlyalignment', 'a', 'concept', 'that', 'is', 'precised', 'in', 'the', 'text',... | [-0.16370202592292496, 0.17646549109282883, -0.11818413834932238, 0.06463365818287224, -0.01233240857525447, -0.1199637396521, 0.023608434598806294, 0.29804648597573125, -0.271100101082824, -0.22973291881295832, 0.10420129695625673, -0.23357999807245336, -0.2459901628452678, 0.16495761076031729, -0.1495337361513182, 0.... |
706.3344 | SN 2001em: No Jet-Driven Gamma Ray Burst Event | We report on our second-epoch VLBI and VLA observations of the Type Ib/c
supernova 2001em, five years after the explosion. It was suggested that SN
2001em might be a jet-driven gamma ray burst (GRB), with the jet oriented near
the plane of the sky, which would entail relativistic expansion or motion. Our
VLBI image s... | astro-ph | we report on our secondepoch vlbi and vla observations of the type ibc supernova 2001em five years after the explosion it was suggested that sn 2001em might be a jetdriven gamma ray burst grb with the jet oriented near the plane of the sky which would entail relativistic expansion or motion our vlbi image shows that sn... | [['we', 'report', 'on', 'our', 'secondepoch', 'vlbi', 'and', 'vla', 'observations', 'of', 'the', 'type', 'ibc', 'supernova', '2001em', 'five', 'years', 'after', 'the', 'explosion', 'it', 'was', 'suggested', 'that', 'sn', '2001em', 'might', 'be', 'a', 'jetdriven', 'gamma', 'ray', 'burst', 'grb', 'with', 'the', 'jet', 'o... | [-0.07295374823310836, 0.12435404058284776, -0.051626022989777004, 0.0368765768954869, -0.15183828225161766, -0.0978729841299355, 0.026697236384180457, 0.47448069879954513, -0.16614725778274464, -0.29046266134263893, 0.08969364092106734, -0.2960762864712513, 0.03386469312915296, 0.2003789687896091, -0.01535206268489480... |
706.3345 | Orbital and Spin Excitations in Cobalt Oxide | By means of neutron scattering we have determined new branches of magnetic
excitations in orbitally active CoO (TN=290 K) up to 15 THz and for
temperatures from 6 K to 450 K. Data were taken in the (111) direction in six
single-crystal zones. From the dependence on temperature and Q we have
identified several branche... | cond-mat.str-el | by means of neutron scattering we have determined new branches of magnetic excitations in orbitally active coo tn290 k up to 15 thz and for temperatures from 6 k to 450 k data were taken in the 111 direction in six singlecrystal zones from the dependence on temperature and q we have identified several branches of magne... | [['by', 'means', 'of', 'neutron', 'scattering', 'we', 'have', 'determined', 'new', 'branches', 'of', 'magnetic', 'excitations', 'in', 'orbitally', 'active', 'coo', 'tn290', 'k', 'up', 'to', '15', 'thz', 'and', 'for', 'temperatures', 'from', '6', 'k', 'to', '450', 'k', 'data', 'were', 'taken', 'in', 'the', '111', 'direc... | [-0.14404557807593404, 0.23786023823926464, -0.022811803501099348, -0.02691694083981789, -0.029465131891461518, -0.0819948046372678, 0.12479577781871343, 0.427578141208356, -0.25176790258727777, -0.3498091760497445, 0.030100218839764308, -0.33906387561597884, -0.023627413066629417, 0.1973656683605021, 0.103274358926006... |
706.3346 | Asteroseismology of red giants: photometric observations of Arcturus by
SMEI | We present new results on oscillations of the K1.5 III giant Arcturus (alpha
Boo), from analysis of just over 2.5 yr of precise photometric observations
made by the Solar Mass Ejection Imager (SMEI) on board the Coriolis satellite.
A strong mode of oscillation is uncovered by the analysis, having frequency
3.51+/-0.0... | astro-ph | we present new results on oscillations of the k15 iii giant arcturus alpha boo from analysis of just over 25 yr of precise photometric observations made by the solar mass ejection imager smei on board the coriolis satellite a strong mode of oscillation is uncovered by the analysis having frequency 351003 microhertz by ... | [['we', 'present', 'new', 'results', 'on', 'oscillations', 'of', 'the', 'k15', 'iii', 'giant', 'arcturus', 'alpha', 'boo', 'from', 'analysis', 'of', 'just', 'over', '25', 'yr', 'of', 'precise', 'photometric', 'observations', 'made', 'by', 'the', 'solar', 'mass', 'ejection', 'imager', 'smei', 'on', 'board', 'the', 'cori... | [-0.1313206659029483, 0.15788874020258764, -0.0818911888759191, 0.07368711604871542, -0.12864749697282127, -0.0926966105491789, 0.0826232605225717, 0.35947811420549425, -0.19923306044534242, -0.3629474845437104, 0.13298534425720981, -0.27385771228817474, -0.08532419261009955, 0.27021543770260587, -0.018735847288840694,... |
706.3347 | Cyclic projectors and separation theorems in idempotent convex geometry | Semimodules over idempotent semirings like the max-plus or tropical semiring
have much in common with convex cones. This analogy is particularly apparent in
the case of subsemimodules of the n-fold cartesian product of the max-plus
semiring it is known that one can separate a vector from a closed subsemimodule
that d... | math.MG | semimodules over idempotent semirings like the maxplus or tropical semiring have much in common with convex cones this analogy is particularly apparent in the case of subsemimodules of the nfold cartesian product of the maxplus semiring it is known that one can separate a vector from a closed subsemimodule that does no... | [['semimodules', 'over', 'idempotent', 'semirings', 'like', 'the', 'maxplus', 'or', 'tropical', 'semiring', 'have', 'much', 'in', 'common', 'with', 'convex', 'cones', 'this', 'analogy', 'is', 'particularly', 'apparent', 'in', 'the', 'case', 'of', 'subsemimodules', 'of', 'the', 'nfold', 'cartesian', 'product', 'of', 'th... | [-0.15777781339368868, 0.06847346632358295, -0.0908595353549888, 0.11059178040009521, -0.08288035701781987, -0.1097686651578926, 0.0029690948080482848, 0.3278317796792967, -0.385478578864577, -0.14539536733034972, 0.13849258998075356, -0.25288199884684903, -0.16145338593975556, 0.196751026210461, -0.16267013720382031, ... |
706.3348 | Determining a regular language by glider-based structures called phases
fi_1 in Rule 110 | Rule 110 is a complex elementary cellular automaton able of supporting
universal computation and complicated collision-based reactions between
gliders. We propose a representation for coding initial conditions by means of
a finite subset of regular expressions. The sequences are extracted both from
de Bruijn diagrams... | nlin.CG | rule 110 is a complex elementary cellular automaton able of supporting universal computation and complicated collisionbased reactions between gliders we propose a representation for coding initial conditions by means of a finite subset of regular expressions the sequences are extracted both from de bruijn diagrams and ... | [['rule', '110', 'is', 'a', 'complex', 'elementary', 'cellular', 'automaton', 'able', 'of', 'supporting', 'universal', 'computation', 'and', 'complicated', 'collisionbased', 'reactions', 'between', 'gliders', 'we', 'propose', 'a', 'representation', 'for', 'coding', 'initial', 'conditions', 'by', 'means', 'of', 'a', 'fi... | [-0.1737144653669753, 0.15425661632985765, -0.08302148906931059, 0.11138968379931774, -0.05984472916739534, -0.16112485047735609, 0.12824436302171716, 0.36360464951218063, -0.25281106886356625, -0.24922538184519136, 0.07711500061133793, -0.1994064926837029, -0.1730018236140943, 0.1795280819425165, -0.05346995734552325,... |
706.3349 | High-resolution models of solar granulation: the 2D case | Using grid refinement, we have simulated solar granulation in 2D. The refined
region measures 1.97*2.58 Mm (vertical*horizontal). Grid spacing there is
1.82*2.84 km. The downflows exhibit strong Kelvin-Helmholtz instabilities.
Below the photosphere, acoustic pulses are generated. They proceed laterally
(in some cases... | astro-ph | using grid refinement we have simulated solar granulation in 2d the refined region measures 197258 mm verticalhorizontal grid spacing there is 182284 km the downflows exhibit strong kelvinhelmholtz instabilities below the photosphere acoustic pulses are generated they proceed laterally in some cases distances of at lea... | [['using', 'grid', 'refinement', 'we', 'have', 'simulated', 'solar', 'granulation', 'in', '2d', 'the', 'refined', 'region', 'measures', '197258', 'mm', 'verticalhorizontal', 'grid', 'spacing', 'there', 'is', '182284', 'km', 'the', 'downflows', 'exhibit', 'strong', 'kelvinhelmholtz', 'instabilities', 'below', 'the', 'ph... | [-0.09266623028088361, 0.22349959021469332, -0.0102168933119414, 0.11463514515660035, -0.060902201812187175, -0.07637856215379148, 0.013867052170922453, 0.4585793313596679, -0.2864849765407238, -0.309708621774642, 0.12111008776388052, -0.27175411385185316, -0.05745224768124556, 0.23446833761738403, -0.04671807751693227... |
706.335 | Optimal Replica Placement in Tree Networks with QoS and Bandwidth
Constraints and the Closest Allocation Policy | This paper deals with the replica placement problem on fully homogeneous tree
networks known as the Replica Placement optimization problem. The client
requests are known beforehand, while the number and location of the servers are
to be determined. We investigate the latter problem using the Closest access
policy whe... | cs.DC | this paper deals with the replica placement problem on fully homogeneous tree networks known as the replica placement optimization problem the client requests are known beforehand while the number and location of the servers are to be determined we investigate the latter problem using the closest access policy when add... | [['this', 'paper', 'deals', 'with', 'the', 'replica', 'placement', 'problem', 'on', 'fully', 'homogeneous', 'tree', 'networks', 'known', 'as', 'the', 'replica', 'placement', 'optimization', 'problem', 'the', 'client', 'requests', 'are', 'known', 'beforehand', 'while', 'the', 'number', 'and', 'location', 'of', 'the', 's... | [-0.19667816275300887, -0.0032574629032751544, 0.008935352121121608, 0.039408114285638125, -0.132720950876291, -0.20122637672779653, 0.16691930009087977, 0.4258069439003101, -0.34979490263817403, -0.35496920414555533, 0.1693107469061103, -0.25278352682407085, -0.1314743985923437, 0.09772449640127329, -0.114592216851619... |
706.3351 | Random Boolean Networks | This review explains in a self-contained way the properties of random Boolean
networks and their attractors, with a special focus on critical networks. Using
small example networks, analytical calculations, phenomenological arguments,
and problems to solve, the basic concepts are introduced and important results
conc... | cond-mat.stat-mech cond-mat.dis-nn | this review explains in a selfcontained way the properties of random boolean networks and their attractors with a special focus on critical networks using small example networks analytical calculations phenomenological arguments and problems to solve the basic concepts are introduced and important results concerning ph... | [['this', 'review', 'explains', 'in', 'a', 'selfcontained', 'way', 'the', 'properties', 'of', 'random', 'boolean', 'networks', 'and', 'their', 'attractors', 'with', 'a', 'special', 'focus', 'on', 'critical', 'networks', 'using', 'small', 'example', 'networks', 'analytical', 'calculations', 'phenomenological', 'argument... | [-0.16197970794005828, 0.08701782352714375, -0.047381135482679713, 0.14178486480589278, -0.08010995553975755, -0.1510722030800852, 0.08511252605610273, 0.33047219968654895, -0.22940208922055635, -0.27006320142271845, 0.11700764890040526, -0.2686411156615412, -0.2719275562261993, 0.20709203916432506, -0.0606615562415258... |
706.3352 | Probabilistic Representations of Solutions of the Forward Equations | In this paper we prove a stochastic representation for solutions of the
evolution equation $ \partial_t \psi_t = {1/2}L^*\psi_t $ where $ L^* $ is the
formal adjoint of an elliptic second order differential operator with smooth
coefficients corresponding to the infinitesimal generator of a finite
dimensional diffusio... | math.PR math.AP | in this paper we prove a stochastic representation for solutions of the evolution equation partial_t psi_t 12lpsi_t where l is the formal adjoint of an elliptic second order differential operator with smooth coefficients corresponding to the infinitesimal generator of a finite dimensional diffusion x_t given psi_0 psi ... | [['in', 'this', 'paper', 'we', 'prove', 'a', 'stochastic', 'representation', 'for', 'solutions', 'of', 'the', 'evolution', 'equation', 'partial_t', 'psi_t', '12lpsi_t', 'where', 'l', 'is', 'the', 'formal', 'adjoint', 'of', 'an', 'elliptic', 'second', 'order', 'differential', 'operator', 'with', 'smooth', 'coefficients'... | [-0.14194477710407227, 0.042035802442296696, -0.1185494975419715, 0.010288838653036692, -0.16364701763377526, -0.11859019444091246, -0.07615743356145685, 0.2566433866857551, -0.37109889890998604, -0.13670997843146324, 0.1190303314695484, -0.3176289300201461, -0.13406304884701967, 0.13997642974136398, -0.056340183480642... |
706.3353 | Microscopic origin of isotropic non-Heisenberg behavior in highly
correlated systems | We have reanalyzed the microscopic origin of the isotropic deviations that
are observed from the energy spacings predicted by the HDVV Hamiltonian.
Usually, a biquadratic spin operator is added to the HDVV Hamiltonian to
account for such deviations. It is shown here that this operator cannot
describe the effect of th... | cond-mat.str-el | we have reanalyzed the microscopic origin of the isotropic deviations that are observed from the energy spacings predicted by the hdvv hamiltonian usually a biquadratic spin operator is added to the hdvv hamiltonian to account for such deviations it is shown here that this operator cannot describe the effect of the exc... | [['we', 'have', 'reanalyzed', 'the', 'microscopic', 'origin', 'of', 'the', 'isotropic', 'deviations', 'that', 'are', 'observed', 'from', 'the', 'energy', 'spacings', 'predicted', 'by', 'the', 'hdvv', 'hamiltonian', 'usually', 'a', 'biquadratic', 'spin', 'operator', 'is', 'added', 'to', 'the', 'hdvv', 'hamiltonian', 'to... | [-0.1371959726139903, 0.18962525429204105, -0.07065247177903075, 0.12982850812957622, -0.02966720504919067, -0.09243814304005354, -0.0003202344197779894, 0.3320560903614387, -0.2650406955333892, -0.31086992650292816, 0.06085437562316656, -0.3368153593316674, -0.11129642985761165, 0.16981630714610219, 0.0565582303144037... |
706.3354 | Reliability of the Heitler-London approach for the exchange coupling
between electrons in semiconductor nanostructures | We calculate the exchange coupling J between electrons in a double-well
potential in a two-dimensional semiconductor environment within the
Heitler-London (HL) approach. Two functional forms are considered for the
double-well potential. We show that by choosing an appropriate and relatively
simple single-electron var... | cond-mat.other cond-mat.mes-hall quant-ph | we calculate the exchange coupling j between electrons in a doublewell potential in a twodimensional semiconductor environment within the heitlerlondon hl approach two functional forms are considered for the doublewell potential we show that by choosing an appropriate and relatively simple singleelectron variational wa... | [['we', 'calculate', 'the', 'exchange', 'coupling', 'j', 'between', 'electrons', 'in', 'a', 'doublewell', 'potential', 'in', 'a', 'twodimensional', 'semiconductor', 'environment', 'within', 'the', 'heitlerlondon', 'hl', 'approach', 'two', 'functional', 'forms', 'are', 'considered', 'for', 'the', 'doublewell', 'potentia... | [-0.10296968870929309, 0.07602896118519961, -0.05080180544672268, 0.09809330390056684, -0.0025105473984565053, -0.1874528297755335, 0.0696453344154482, 0.4003827626861277, -0.21807464569186172, -0.30331512696686247, -0.0058952731069266085, -0.2569113972995962, -0.13213321783003354, 0.18184182354515152, -0.0062073264226... |
706.3355 | Automorphisms of Generalized Down-Up Algebras | A generalization of down-up algebras was introduced by Cassidy and Shelton
(J. Algebra 279 (2004), no. 1), the so-called generalized down-up algebras. We
describe the automorphism group of conformal Noetherian generalized down-up
algebras L(f,r,s,\gamma) such that r is not a root of unity, listing explicitly
the elem... | math.RA math.RT | a generalization of downup algebras was introduced by cassidy and shelton j algebra 279 2004 no 1 the socalled generalized downup algebras we describe the automorphism group of conformal noetherian generalized downup algebras lfrsgamma such that r is not a root of unity listing explicitly the elements of the group in t... | [['a', 'generalization', 'of', 'downup', 'algebras', 'was', 'introduced', 'by', 'cassidy', 'and', 'shelton', 'j', 'algebra', '279', '2004', 'no', '1', 'the', 'socalled', 'generalized', 'downup', 'algebras', 'we', 'describe', 'the', 'automorphism', 'group', 'of', 'conformal', 'noetherian', 'generalized', 'downup', 'alge... | [-0.20968334926394644, 0.06741250075712023, -0.07217164941971282, 0.04188086992196206, -0.1436697178121124, -0.1599182295817677, -0.04326082633009979, 0.32821998851639883, -0.39473916723259855, -0.1639689439088925, 0.12178260605183563, -0.22933410070222485, -0.10106287913008051, 0.15979628714190408, -0.1371602128710147... |
706.3356 | The Physics of Ultraperipheral Collisions at the LHC | We discuss the physics of large impact parameter interactions at the LHC:
ultraperipheral collisions (UPCs). The dominant processes in UPCs are
photon-nucleon (nucleus) interactions. The current LHC detector configurations
can explore small $x$ hard phenomena with nuclei and nucleons at photon-nucleon
center-of-mass ... | nucl-ex hep-ex hep-ph nucl-th | we discuss the physics of large impact parameter interactions at the lhc ultraperipheral collisions upcs the dominant processes in upcs are photonnucleon nucleus interactions the current lhc detector configurations can explore small x hard phenomena with nuclei and nucleons at photonnucleon centerofmass energies above ... | [['we', 'discuss', 'the', 'physics', 'of', 'large', 'impact', 'parameter', 'interactions', 'at', 'the', 'lhc', 'ultraperipheral', 'collisions', 'upcs', 'the', 'dominant', 'processes', 'in', 'upcs', 'are', 'photonnucleon', 'nucleus', 'interactions', 'the', 'current', 'lhc', 'detector', 'configurations', 'can', 'explore'... | [-0.04078472517843684, 0.2631472912920969, -0.09548168945220285, 0.1689616281377482, 0.009473228682603302, -0.08555177922229847, -0.025522441587186064, 0.3910152161209454, -0.20111500541335475, -0.27777715153955473, -0.015173831826713615, -0.35232926203681186, 0.043161872634434786, 0.1638571611305084, 0.107498201559953... |
706.3357 | Primordial gas heating by dark matter and structure formation | Dark matter (DM) decays and annihilations might heat and partially reionize
the Universe at high redshift. Although this effect is not important for the
cosmic reionization, the gas heating due to DM particles might affect the
structure formation. In particular, the critical halo mass for collapse is
increased up to ... | astro-ph | dark matter dm decays and annihilations might heat and partially reionize the universe at high redshift although this effect is not important for the cosmic reionization the gas heating due to dm particles might affect the structure formation in particular the critical halo mass for collapse is increased up to a factor... | [['dark', 'matter', 'dm', 'decays', 'and', 'annihilations', 'might', 'heat', 'and', 'partially', 'reionize', 'the', 'universe', 'at', 'high', 'redshift', 'although', 'this', 'effect', 'is', 'not', 'important', 'for', 'the', 'cosmic', 'reionization', 'the', 'gas', 'heating', 'due', 'to', 'dm', 'particles', 'might', 'aff... | [-0.09390443745185621, 0.21477539033629, -0.06182954911608249, 0.15280046633677558, -0.09773449935019016, -0.016213101227767767, 0.005029147614259273, 0.2952131276077125, -0.21416321595199406, -0.3630320828250842, 0.020383019105065615, -0.2876803609961644, 0.017571791452355684, 0.15140227719559335, 0.043558904947713015... |
706.3358 | KNO scaling in processes of electron-positron annihilation to hadrons | The charged particles multiplicity distribution in the KNO form is discussed
in processes of $e^+e^-$ annihilation at energies $\sqrt{s}$ 14 -- 206.2 GeV.
The experimental data are compared to data, obtained with Monte Carlo
simulation in PYTHIA in the Lund quark string model. It is shown, that both
experimental and ... | hep-ph | the charged particles multiplicity distribution in the kno form is discussed in processes of ee annihilation at energies sqrts 14 2062 gev the experimental data are compared to data obtained with monte carlo simulation in pythia in the lund quark string model it is shown that both experimental and simulated data are de... | [['the', 'charged', 'particles', 'multiplicity', 'distribution', 'in', 'the', 'kno', 'form', 'is', 'discussed', 'in', 'processes', 'of', 'ee', 'annihilation', 'at', 'energies', 'sqrts', '14', '2062', 'gev', 'the', 'experimental', 'data', 'are', 'compared', 'to', 'data', 'obtained', 'with', 'monte', 'carlo', 'simulation... | [-0.03889957607010908, 0.21960514398682632, -0.1668853983225554, 0.21322300136204303, 0.02807041910695441, -0.08096012284542307, -0.03645475561742061, 0.3657961329560221, -0.18244935565823575, -0.3215825828137221, -0.03873830161885255, -0.3587349462265402, 0.012540729532455221, 0.17092223664929654, 0.07295196737956118,... |
706.3359 | Three-Dimensional Gravity Revisited | We consider the problem of identifying the CFT's that may be dual to pure
gravity in three dimensions with negative cosmological constant. The c-theorem
indicates that three-dimensional pure gravity is consistent only at certain
values of the coupling constant, and the relation to Chern-Simons gauge theory
hints that... | hep-th | we consider the problem of identifying the cfts that may be dual to pure gravity in three dimensions with negative cosmological constant the ctheorem indicates that threedimensional pure gravity is consistent only at certain values of the coupling constant and the relation to chernsimons gauge theory hints that these m... | [['we', 'consider', 'the', 'problem', 'of', 'identifying', 'the', 'cfts', 'that', 'may', 'be', 'dual', 'to', 'pure', 'gravity', 'in', 'three', 'dimensions', 'with', 'negative', 'cosmological', 'constant', 'the', 'ctheorem', 'indicates', 'that', 'threedimensional', 'pure', 'gravity', 'is', 'consistent', 'only', 'at', 'c... | [-0.12769009320234712, 0.15327905451624907, -0.10189553025940602, 0.07291278179988943, -0.10790568797877341, -0.1938841715765496, -0.035242216054096144, 0.2901021272240376, -0.23169856312839934, -0.26114588325109445, 0.09032876682397203, -0.2765404065675808, -0.1413417538458651, 0.1452126791926496, -0.05497244930064136... |
706.336 | Theory of ultracold Fermi gases | The physics of quantum degenerate Fermi gases in uniform as well as in
harmonically trapped configurations is reviewed from a theoretical perspective.
Emphasis is given to the effect of interactions which play a crucial role,
bringing the gas into a superfluid phase at low temperature. In these dilute
systems interac... | cond-mat.other | the physics of quantum degenerate fermi gases in uniform as well as in harmonically trapped configurations is reviewed from a theoretical perspective emphasis is given to the effect of interactions which play a crucial role bringing the gas into a superfluid phase at low temperature in these dilute systems interactions... | [['the', 'physics', 'of', 'quantum', 'degenerate', 'fermi', 'gases', 'in', 'uniform', 'as', 'well', 'as', 'in', 'harmonically', 'trapped', 'configurations', 'is', 'reviewed', 'from', 'a', 'theoretical', 'perspective', 'emphasis', 'is', 'given', 'to', 'the', 'effect', 'of', 'interactions', 'which', 'play', 'a', 'crucial... | [-0.16689237121142894, 0.24415087265391686, -0.07820856478113558, 0.06348675379628138, 0.007965888281225292, -0.11010755038785427, 0.04637544593243392, 0.2982810286986661, -0.2405341509323861, -0.27258216219720394, 0.03279395617739804, -0.30700574210106835, -0.06499602873249297, 0.18423084954294489, 0.07856359980329948... |
706.3361 | Polarized States and Domain Walls in Spinor Bose-Einstein Condensates | We study spin-polarized states and their stability in anti-ferromagnetic
states of spinor (F=1) quasi-one-dimensional Bose-Einstein condensates. Using
analytical approximations and numerical methods, we find various types of
polarized states, including: patterns of the Thomas-Fermi type; structures with
a pulse-shape... | cond-mat.other | we study spinpolarized states and their stability in antiferromagnetic states of spinor f1 quasionedimensional boseeinstein condensates using analytical approximations and numerical methods we find various types of polarized states including patterns of the thomasfermi type structures with a pulseshape in one component... | [['we', 'study', 'spinpolarized', 'states', 'and', 'their', 'stability', 'in', 'antiferromagnetic', 'states', 'of', 'spinor', 'f1', 'quasionedimensional', 'boseeinstein', 'condensates', 'using', 'analytical', 'approximations', 'and', 'numerical', 'methods', 'we', 'find', 'various', 'types', 'of', 'polarized', 'states',... | [-0.2099059209104613, 0.15327901324513843, -0.08690000594622094, 0.0678412110452084, -0.012474798058083623, -0.10200541314421868, 0.021597483119338144, 0.36917938620840407, -0.20646736199720478, -0.23791757818045361, 0.08173042268264202, -0.2977673150599003, -0.09429599203131332, 0.1803670346199972, 0.1022312027231163,... |
706.3362 | Three experimental pearls in Costas arrays | The results of 3 experiments in Costas arrays are presented, for which
theoretical explanation is still not available: the number of dots on the main
diagonal of exponential Welch arrays, the parity populations of Golomb arrays
generated in fields of characteristic 2, and the maximal cross-correlation
between pairs o... | math.CO math.NT | the results of 3 experiments in costas arrays are presented for which theoretical explanation is still not available the number of dots on the main diagonal of exponential welch arrays the parity populations of golomb arrays generated in fields of characteristic 2 and the maximal crosscorrelation between pairs of welch... | [['the', 'results', 'of', '3', 'experiments', 'in', 'costas', 'arrays', 'are', 'presented', 'for', 'which', 'theoretical', 'explanation', 'is', 'still', 'not', 'available', 'the', 'number', 'of', 'dots', 'on', 'the', 'main', 'diagonal', 'of', 'exponential', 'welch', 'arrays', 'the', 'parity', 'populations', 'of', 'golo... | [-0.22894358341000043, 0.17421405012282776, -0.01372538679788704, 0.0826635039793473, 0.002955331263365224, -0.14717487409507157, -0.013112776796333492, 0.3438758251431864, -0.21478546771686524, -0.30461617530090734, 0.12556944690186356, -0.3000630956958048, -0.09316656759256148, 0.2601402532418433, -0.0382877044321503... |
706.3363 | The binary properties of the pulsating subdwarf B eclipsing binary PG
1336-018 (NY Vir) | We present an unbiased orbit solution and mass determination of the
components of the eclipsing binary NY Vir as a critical test for the formation
scenarios of subdwarf B stars. We obtained high-resolution time series VLT/UVES
spectra and high-speed multicolour VLT/ULTRACAM photometric observations of NY
Vir, a rapid... | astro-ph | we present an unbiased orbit solution and mass determination of the components of the eclipsing binary ny vir as a critical test for the formation scenarios of subdwarf b stars we obtained highresolution time series vltuves spectra and highspeed multicolour vltultracam photometric observations of ny vir a rapidly pulsa... | [['we', 'present', 'an', 'unbiased', 'orbit', 'solution', 'and', 'mass', 'determination', 'of', 'the', 'components', 'of', 'the', 'eclipsing', 'binary', 'ny', 'vir', 'as', 'a', 'critical', 'test', 'for', 'the', 'formation', 'scenarios', 'of', 'subdwarf', 'b', 'stars', 'we', 'obtained', 'highresolution', 'time', 'series... | [-0.16233974426286296, 0.10481950546545704, -0.08860042801534292, 0.023755778368649772, -0.1165612802375108, -0.13404213185422123, 0.101408034627093, 0.3545080818235874, -0.1653002896317048, -0.3095547746983357, 0.09196761526291083, -0.3201590992626734, -0.06610884771798738, 0.2399679537047632, -0.04632402591378195, 0.... |
706.3364 | Unfolding Geometric Unification in M-Theory | By reinterpreting the familiar tools and ideas of M-theory model building, we
show how a G2-manifold locally engineered to give rise to massless matter
representations of an SU(5) grand unified model can be smoothly unfolded into a
G2-manifold giving rise to SU(3)xSU(2) gauge theory with the corresponding
matter repr... | hep-th | by reinterpreting the familiar tools and ideas of mtheory model building we show how a g2manifold locally engineered to give rise to massless matter representations of an su5 grand unified model can be smoothly unfolded into a g2manifold giving rise to su3xsu2 gauge theory with the corresponding matter representations ... | [['by', 'reinterpreting', 'the', 'familiar', 'tools', 'and', 'ideas', 'of', 'mtheory', 'model', 'building', 'we', 'show', 'how', 'a', 'g2manifold', 'locally', 'engineered', 'to', 'give', 'rise', 'to', 'massless', 'matter', 'representations', 'of', 'an', 'su5', 'grand', 'unified', 'model', 'can', 'be', 'smoothly', 'unfo... | [-0.041835022176568835, 0.18391851690474606, -0.18368381307400922, 0.15588359813765681, -0.13607788771054052, -0.19046673739943257, -0.012477768992539495, 0.2806608772222349, -0.2695900831430992, -0.33278160871184886, 0.042710628760532734, -0.214216775409481, -0.1775193049676439, 0.1695143427016174, -0.1117482461292851... |
706.3365 | Coulomb shifts and shape changes in the mass 70 region | The technique of recoil beta tagging has been developed which allows prompt
gamma decays in nuclei from excited states to be correlated with electrons from
their subsequent short-lived beta decay. This technique is ideal for studying
nuclei very far from stability and improves in sensitivity for very short-lived
deca... | nucl-ex | the technique of recoil beta tagging has been developed which allows prompt gamma decays in nuclei from excited states to be correlated with electrons from their subsequent shortlived beta decay this technique is ideal for studying nuclei very far from stability and improves in sensitivity for very shortlived decays an... | [['the', 'technique', 'of', 'recoil', 'beta', 'tagging', 'has', 'been', 'developed', 'which', 'allows', 'prompt', 'gamma', 'decays', 'in', 'nuclei', 'from', 'excited', 'states', 'to', 'be', 'correlated', 'with', 'electrons', 'from', 'their', 'subsequent', 'shortlived', 'beta', 'decay', 'this', 'technique', 'is', 'ideal... | [-0.0037908657074526503, 0.20385503341396408, -0.10788471989195655, 0.13574591574552297, 0.004245023386276982, -0.15448707841612674, 0.015593833302113193, 0.36310228120397636, -0.2532399056410348, -0.3120183602527336, 0.026901627687254438, -0.3152551605143041, -0.04188736293602873, 0.2043115301264657, 0.001953799168889... |
706.3366 | Extreme Associated Functions: Optimally Linking Local Extremes to
Large-scale Atmospheric Circulation Structures | We present a new statistical method to optimally link local weather extremes
to large-scale atmospheric circulation structures. The method is illustrated
using July-August daily mean temperature at 2m height (T2m) time-series over
the Netherlands and 500 hPa geopotential height (Z500) time-series over the
Euroatlanti... | physics.ao-ph physics.geo-ph | we present a new statistical method to optimally link local weather extremes to largescale atmospheric circulation structures the method is illustrated using julyaugust daily mean temperature at 2m height t2m timeseries over the netherlands and 500 hpa geopotential height z500 timeseries over the euroatlantic region of... | [['we', 'present', 'a', 'new', 'statistical', 'method', 'to', 'optimally', 'link', 'local', 'weather', 'extremes', 'to', 'largescale', 'atmospheric', 'circulation', 'structures', 'the', 'method', 'is', 'illustrated', 'using', 'julyaugust', 'daily', 'mean', 'temperature', 'at', '2m', 'height', 't2m', 'timeseries', 'over... | [-0.1204165758504983, 0.13507941676634214, -0.11278319082132751, 0.11604966424976386, -0.019796510913499422, -0.07160101167617305, 0.03441183332564129, 0.3545944828059404, -0.2356141775132968, -0.31665535796313515, 0.13946376767520222, -0.28544793021827636, -0.11934471090714778, 0.23854806583314653, -0.0998176972625867... |
706.3367 | Singularities of $n$-fold integrals of the Ising class and the theory of
elliptic curves | We introduce some multiple integrals that are expected to have the same
singularities as the singularities of the $ n$-particle contributions
$\chi^{(n)}$ to the susceptibility of the square lattice Ising model. We find
the Fuchsian linear differential equation satisfied by these multiple integrals
for $ n=1, 2, 3, 4... | math-ph cond-mat.stat-mech hep-th math.MP physics.comp-ph | we introduce some multiple integrals that are expected to have the same singularities as the singularities of the nparticle contributions chin to the susceptibility of the square lattice ising model we find the fuchsian linear differential equation satisfied by these multiple integrals for n1 2 3 4 and only modulo some... | [['we', 'introduce', 'some', 'multiple', 'integrals', 'that', 'are', 'expected', 'to', 'have', 'the', 'same', 'singularities', 'as', 'the', 'singularities', 'of', 'the', 'nparticle', 'contributions', 'chin', 'to', 'the', 'susceptibility', 'of', 'the', 'square', 'lattice', 'ising', 'model', 'we', 'find', 'the', 'fuchsia... | [-0.22144644577525743, 0.07349298405516042, -0.08508445880720157, 0.09728970233949699, -0.07812985839682217, -0.13354239829017647, -0.011336705643006702, 0.2819679551757872, -0.2962294062467472, -0.25790982776978877, 0.09205054747725312, -0.31459283999231213, -0.1724725264054136, 0.20272893119826443, -0.047290319338159... |
706.3368 | The dust, planetesimals and planets of HD 38529 | HD 38529 is a post-main sequence G8III/IV star (3.5 Gyr old) with a planetary
system consisting of at least two planets having Msin(i) of 0.8 MJup and 12.2
MJup, semimajor axes of 0.13 AU and 3.74 AU, and eccentricities of 0.25 and
0.35, respectively. Spitzer observations show that HD 38529 has an excess
emission abo... | astro-ph | hd 38529 is a postmain sequence g8iiiiv star 35 gyr old with a planetary system consisting of at least two planets having msini of 08 mjup and 122 mjup semimajor axes of 013 au and 374 au and eccentricities of 025 and 035 respectively spitzer observations show that hd 38529 has an excess emission above the stellar phot... | [['hd', '38529', 'is', 'a', 'postmain', 'sequence', 'g8iiiiv', 'star', '35', 'gyr', 'old', 'with', 'a', 'planetary', 'system', 'consisting', 'of', 'at', 'least', 'two', 'planets', 'having', 'msini', 'of', '08', 'mjup', 'and', '122', 'mjup', 'semimajor', 'axes', 'of', '013', 'au', 'and', '374', 'au', 'and', 'eccentricit... | [-0.11134463728943822, 0.15302747297331684, -0.046939483289435986, 0.03890442630167145, -0.008595422639750765, -0.06098791819819839, 0.055521537212830104, 0.3597824013826155, -0.1594759976125398, -0.38597623973982326, 0.03757874498949087, -0.31371249155613484, -0.04740525740882331, 0.1422441011025579, -0.06402908373154... |
706.3369 | Equilibrium properties of mesoscopic quantum conductors | Review article on equilibrium properties of mesoscopic quantum conductors.
| cond-mat.mes-hall | review article on equilibrium properties of mesoscopic quantum conductors | [['review', 'article', 'on', 'equilibrium', 'properties', 'of', 'mesoscopic', 'quantum', 'conductors']] | [-0.1897491150432163, 0.1815747581422329, -0.12774837423219448, -0.030550601943913434, 0.010452751484182145, -0.15926681458950043, 0.011839327583503392, 0.26226404392056996, -0.2273307301931911, -0.1542770608017842, -0.0193600675298108, -0.3485792858733071, -0.1794964066810078, 0.21441905117697185, -0.00983754276401466... |
706.337 | The algebro-geometric initial value problem for the Ablowitz-Ladik
hierarchy | We discuss the algebro-geometric initial value problem for the Ablowitz-Ladik
hierarchy with complex-valued initial data and prove unique solvability
globally in time for a set of initial (Dirichlet divisor) data of full measure.
To this effect we develop a new algorithm for constructing stationary
complex-valued alg... | nlin.SI math-ph math.MP | we discuss the algebrogeometric initial value problem for the ablowitzladik hierarchy with complexvalued initial data and prove unique solvability globally in time for a set of initial dirichlet divisor data of full measure to this effect we develop a new algorithm for constructing stationary complexvalued algebrogeome... | [['we', 'discuss', 'the', 'algebrogeometric', 'initial', 'value', 'problem', 'for', 'the', 'ablowitzladik', 'hierarchy', 'with', 'complexvalued', 'initial', 'data', 'and', 'prove', 'unique', 'solvability', 'globally', 'in', 'time', 'for', 'a', 'set', 'of', 'initial', 'dirichlet', 'divisor', 'data', 'of', 'full', 'measu... | [-0.11747600389671735, 0.02715785449926608, -0.05866115022319974, 0.10347151249233219, -0.14040987926388257, -0.16689369437279322, -0.014385929223618399, 0.2759750762747394, -0.3270585967216924, -0.24870112726678636, 0.13752297361208432, -0.24032796966728934, -0.130059682303898, 0.16499841063996853, -0.0728874710682583... |
706.3371 | Muon Spin Spectroscopy evidence of the violation of Anderson condition
in magnetite | We present new muon spectroscopy data on a Fe$_3$O$_4$ single crystal,
revealing different spin precession patterns in five distinct temperature
ranges. A careful analysis of the local field and its straightforward modeling
obtains surprisingly good agreement with experiments only if a very specific
model of localize... | cond-mat.str-el | we present new muon spectroscopy data on a fe_3o_4 single crystal revealing different spin precession patterns in five distinct temperature ranges a careful analysis of the local field and its straightforward modeling obtains surprisingly good agreement with experiments only if a very specific model of localized charge... | [['we', 'present', 'new', 'muon', 'spectroscopy', 'data', 'on', 'a', 'fe_3o_4', 'single', 'crystal', 'revealing', 'different', 'spin', 'precession', 'patterns', 'in', 'five', 'distinct', 'temperature', 'ranges', 'a', 'careful', 'analysis', 'of', 'the', 'local', 'field', 'and', 'its', 'straightforward', 'modeling', 'obt... | [-0.1493875207681838, 0.2231329795964933, -0.052426817470121304, 0.10277045567296203, -0.06008102500799124, -0.19537709616487484, 0.08622741828031548, 0.3549859878401478, -0.19788244736755822, -0.3084774654261865, 0.04527785178340439, -0.3165167293620187, -0.03430512069736595, 0.20693370506058556, 0.05168966569199965, ... |
706.3372 | Reciprocity of Networks with Degree Correlations and Arbitrary Degree
Sequences | Although most of the real networks contain a mixture of directed and
bidirectional (reciprocal) connections, the reciprocity $r$ has received little
attention as a subject of theoretical understanding. We study the expected
reciprocity of networks with an arbitrary degree sequence and a broad class of
degree correlat... | cond-mat.stat-mech cond-mat.dis-nn | although most of the real networks contain a mixture of directed and bidirectional reciprocal connections the reciprocity r has received little attention as a subject of theoretical understanding we study the expected reciprocity of networks with an arbitrary degree sequence and a broad class of degree correlations by ... | [['although', 'most', 'of', 'the', 'real', 'networks', 'contain', 'a', 'mixture', 'of', 'directed', 'and', 'bidirectional', 'reciprocal', 'connections', 'the', 'reciprocity', 'r', 'has', 'received', 'little', 'attention', 'as', 'a', 'subject', 'of', 'theoretical', 'understanding', 'we', 'study', 'the', 'expected', 'rec... | [-0.15281746105914784, 0.0215822187084363, -0.08272834326666982, 0.09064641037232081, -0.06935760724477207, -0.1530347649797635, 0.03452643096249591, 0.41249689338323864, -0.260783896777708, -0.30022701696124504, 0.028965335927711312, -0.26734515967394185, -0.2645321367156651, 0.17964806443120798, -0.01789805127064819,... |
706.3373 | First-order flow equations for extremal black holes in very special
geometry | We construct interpolating solutions describing single-center static extremal
non-supersymmetric black holes in four-dimensional N=2 supergravity theories
with cubic prepotentials. To this end, we derive and solve first-order flow
equations for rotating electrically charged extremal black holes in a Taub-NUT
geometry... | hep-th | we construct interpolating solutions describing singlecenter static extremal nonsupersymmetric black holes in fourdimensional n2 supergravity theories with cubic prepotentials to this end we derive and solve firstorder flow equations for rotating electrically charged extremal black holes in a taubnut geometry in five d... | [['we', 'construct', 'interpolating', 'solutions', 'describing', 'singlecenter', 'static', 'extremal', 'nonsupersymmetric', 'black', 'holes', 'in', 'fourdimensional', 'n2', 'supergravity', 'theories', 'with', 'cubic', 'prepotentials', 'to', 'this', 'end', 'we', 'derive', 'and', 'solve', 'firstorder', 'flow', 'equations... | [-0.14409492631569842, 0.08653513609368185, -0.01547383088054079, 0.16318203345696075, -0.09486077297972798, -0.2209455867114505, -0.06001948542667158, 0.27675415336323733, -0.07864277874415909, -0.2844533237600417, 0.10307616492288864, -0.381281623503927, -0.16702356609995617, 0.07745315798092633, -0.07463068931335301... |
706.3374 | Laser ablation loading of a surface-electrode ion trap | We demonstrate loading by laser ablation of $^{88}$Sr$^+$ ions into a
mm-scale surface-electrode ion trap. The laser used for ablation is a pulsed,
frequency-tripled Nd:YAG with pulse energies of 1-10 mJ and durations of 3-5
ns. An additional laser is not required to photoionize the ablated material.
The efficiency a... | quant-ph | we demonstrate loading by laser ablation of 88sr ions into a mmscale surfaceelectrode ion trap the laser used for ablation is a pulsed frequencytripled ndyag with pulse energies of 110 mj and durations of 35 ns an additional laser is not required to photoionize the ablated material the efficiency and lifetime of severa... | [['we', 'demonstrate', 'loading', 'by', 'laser', 'ablation', 'of', '88sr', 'ions', 'into', 'a', 'mmscale', 'surfaceelectrode', 'ion', 'trap', 'the', 'laser', 'used', 'for', 'ablation', 'is', 'a', 'pulsed', 'frequencytripled', 'ndyag', 'with', 'pulse', 'energies', 'of', '110', 'mj', 'and', 'durations', 'of', '35', 'ns',... | [-0.05727346980012953, 0.30826759681120164, 0.02003310231026262, -0.014372968911193312, 0.060478446089546195, -0.17868691982352175, 0.07423427224857733, 0.5131021934002638, -0.1858119688509032, -0.3735547968372703, 0.011345137049211189, -0.275486779587809, 0.10558903503231704, 0.2798003372736275, 0.012313636456383392, ... |
706.3375 | Eigenvalue Decomposition as a Generalized Synchronization Cluster
Analysis | Motivated by the recent demonstration of its use as a tool for the detection
and characterization of phase-shape correlations in multivariate time series,
we show that eigenvalue decomposition can also be applied to a matrix of
indices of bivariate phase synchronization strength. The resulting method is
able to ident... | physics.data-an | motivated by the recent demonstration of its use as a tool for the detection and characterization of phaseshape correlations in multivariate time series we show that eigenvalue decomposition can also be applied to a matrix of indices of bivariate phase synchronization strength the resulting method is able to identify c... | [['motivated', 'by', 'the', 'recent', 'demonstration', 'of', 'its', 'use', 'as', 'a', 'tool', 'for', 'the', 'detection', 'and', 'characterization', 'of', 'phaseshape', 'correlations', 'in', 'multivariate', 'time', 'series', 'we', 'show', 'that', 'eigenvalue', 'decomposition', 'can', 'also', 'be', 'applied', 'to', 'a', ... | [-0.08010751337591684, 0.036984978980475744, -0.12003111174846647, 0.030916956595747787, -0.042549686175731925, -0.09166379415766657, 0.049582136959275776, 0.368884737689455, -0.265036301433007, -0.324327493274287, 0.11587502834966265, -0.20983168202209748, -0.19552025566769748, 0.25742926096353885, -0.0379640360973274... |
706.3376 | Quantum limited measurements of atomic scattering properties | We propose a method to perform precision measurements of the interaction
parameters in systems of N ultra-cold spin 1/2 atoms. The spectroscopy is
realized by first creating a coherent spin superposition of the two relevant
internal states of each atom and then letting the atoms evolve under a
squeezing Hamiltonian. ... | cond-mat.other | we propose a method to perform precision measurements of the interaction parameters in systems of n ultracold spin 12 atoms the spectroscopy is realized by first creating a coherent spin superposition of the two relevant internal states of each atom and then letting the atoms evolve under a squeezing hamiltonian the no... | [['we', 'propose', 'a', 'method', 'to', 'perform', 'precision', 'measurements', 'of', 'the', 'interaction', 'parameters', 'in', 'systems', 'of', 'n', 'ultracold', 'spin', '12', 'atoms', 'the', 'spectroscopy', 'is', 'realized', 'by', 'first', 'creating', 'a', 'coherent', 'spin', 'superposition', 'of', 'the', 'two', 'rel... | [-0.15280994548611626, 0.2533591921647428, -0.026392559082787627, 0.0158438952772999, 0.02307618661065593, -0.1789707570507383, 0.08248480384145643, 0.36358108047310633, -0.2378849433735013, -0.2676126505639262, 0.024142337348027766, -0.29375664840758076, -0.07003044671172859, 0.167740894989857, 0.03673729223007237, 0.... |
706.3377 | Domain Structures in Confined Nanoferroelectrics: Phase Field Approach | Phase field modeling of domain structures in ferroelectrics nanorods of
different shape and sizes is presented. The vortex domain configurations in
confined ferroelectrics have been explored by varying the ratio of the energies
of electrostatic and elastic interactions. It is shown that a strong effect of
the electro... | cond-mat.mtrl-sci | phase field modeling of domain structures in ferroelectrics nanorods of different shape and sizes is presented the vortex domain configurations in confined ferroelectrics have been explored by varying the ratio of the energies of electrostatic and elastic interactions it is shown that a strong effect of the electrostat... | [['phase', 'field', 'modeling', 'of', 'domain', 'structures', 'in', 'ferroelectrics', 'nanorods', 'of', 'different', 'shape', 'and', 'sizes', 'is', 'presented', 'the', 'vortex', 'domain', 'configurations', 'in', 'confined', 'ferroelectrics', 'have', 'been', 'explored', 'by', 'varying', 'the', 'ratio', 'of', 'the', 'ene... | [-0.17134649469178098, 0.12598829782125426, -0.10135139115222558, 0.04652610141557904, -0.05873872205904387, -0.07524069833560186, -0.006978250917915291, 0.44775185422989927, -0.23577593192367732, -0.30039125878038336, 0.02441715362574453, -0.21210603184039586, -0.15439041690828587, 0.1761567832447715, 0.02376694062236... |
706.3378 | Many-body protected entanglement generation in interacting spin systems | We discuss a method to achieve decoherence resistent entanglement generation
in two level spin systems governed by gapped and multi-degenerate Hamiltonians.
In such systems, while the large number of degrees of freedom in the ground
state levels allows to create various quantum superpositions, the energy gap
prevents... | cond-mat.other | we discuss a method to achieve decoherence resistent entanglement generation in two level spin systems governed by gapped and multidegenerate hamiltonians in such systems while the large number of degrees of freedom in the ground state levels allows to create various quantum superpositions the energy gap prevents decoh... | [['we', 'discuss', 'a', 'method', 'to', 'achieve', 'decoherence', 'resistent', 'entanglement', 'generation', 'in', 'two', 'level', 'spin', 'systems', 'governed', 'by', 'gapped', 'and', 'multidegenerate', 'hamiltonians', 'in', 'such', 'systems', 'while', 'the', 'large', 'number', 'of', 'degrees', 'of', 'freedom', 'in', ... | [-0.18160177305460387, 0.23264508036610354, 0.005313647587339334, 0.05622265730565841, 0.029685659601071147, -0.17574408732422994, 0.05903842135913533, 0.37406012070698474, -0.24680987114103836, -0.3135004755528217, 0.04468526635019946, -0.2566614570631485, -0.08740573264487567, 0.18675370484167592, -0.0223577980501064... |
706.3379 | Self-Replicating Space-Cells and the Cosmological Constant | We consider what the implications would be if there were a discrete
fundamental model of physics based on locally-finite self-interacting
information, in which there is no presumption of the familiar space and laws of
physics, but from which such space and laws can nevertheless be shown to be
able to emerge stably fr... | gr-qc nlin.AO | we consider what the implications would be if there were a discrete fundamental model of physics based on locallyfinite selfinteracting information in which there is no presumption of the familiar space and laws of physics but from which such space and laws can nevertheless be shown to be able to emerge stably from suc... | [['we', 'consider', 'what', 'the', 'implications', 'would', 'be', 'if', 'there', 'were', 'a', 'discrete', 'fundamental', 'model', 'of', 'physics', 'based', 'on', 'locallyfinite', 'selfinteracting', 'information', 'in', 'which', 'there', 'is', 'no', 'presumption', 'of', 'the', 'familiar', 'space', 'and', 'laws', 'of', '... | [-0.09062033365769152, 0.1879985963161557, -0.0729081056251899, 0.07434573074609725, -0.07991916108398865, -0.17986889839427084, 0.05804919116905469, 0.3282778779239768, -0.289973022225691, -0.3106231801888436, 0.14561375985011601, -0.25671133072151303, -0.1092514881454249, 0.1907881933379357, -0.06292840531362026, -0.... |
706.338 | Transition metal oxides using quantum Monte Carlo | The transition metal-oxygen bond appears prominently throughout chemistry and
solid-state physics. Many materials, from biomolecules to ferroelectrics to the
components of supernova remnants contain this bond in some form. Many of these
materials' properties strongly depend on fine details of the TM-O bond and
intric... | cond-mat.str-el cond-mat.mtrl-sci | the transition metaloxygen bond appears prominently throughout chemistry and solidstate physics many materials from biomolecules to ferroelectrics to the components of supernova remnants contain this bond in some form many of these materials properties strongly depend on fine details of the tmo bond and intricate corre... | [['the', 'transition', 'metaloxygen', 'bond', 'appears', 'prominently', 'throughout', 'chemistry', 'and', 'solidstate', 'physics', 'many', 'materials', 'from', 'biomolecules', 'to', 'ferroelectrics', 'to', 'the', 'components', 'of', 'supernova', 'remnants', 'contain', 'this', 'bond', 'in', 'some', 'form', 'many', 'of',... | [-0.0799853664215776, 0.13861624039744927, -0.0628085990445079, 0.09961689222673668, -0.04591194978941267, -0.12272718629014252, 0.05643941428638542, 0.43079736485868414, -0.2936572322238968, -0.292353649284238, 0.017178477388676082, -0.3274187234656833, -0.18558164155894072, 0.1753787539603415, 0.05149957240846391, 0.... |
706.3381 | Integral degree of a ring and reduction numbers | The supremum of reduction numbers of ideals having principal reductions is
expressed in terms of the integral degree, a new invariant of the ring, which
is finite provided the ring has finite integral closure. As a consequence, one
obtains bounds for the Castelnuovo-Mumford regularity of the Rees algebra and
for the ... | math.AC | the supremum of reduction numbers of ideals having principal reductions is expressed in terms of the integral degree a new invariant of the ring which is finite provided the ring has finite integral closure as a consequence one obtains bounds for the castelnuovomumford regularity of the rees algebra and for the artinre... | [['the', 'supremum', 'of', 'reduction', 'numbers', 'of', 'ideals', 'having', 'principal', 'reductions', 'is', 'expressed', 'in', 'terms', 'of', 'the', 'integral', 'degree', 'a', 'new', 'invariant', 'of', 'the', 'ring', 'which', 'is', 'finite', 'provided', 'the', 'ring', 'has', 'finite', 'integral', 'closure', 'as', 'a'... | [-0.24537667551271194, 0.028313708807921636, -0.10349563625201864, 0.05560336088462961, -0.07381645091018586, -0.0736880485706453, -0.06701186591021295, 0.21145740861319146, -0.36238696784624513, -0.20803373964187108, 0.15751815918297069, -0.25205200580212306, -0.04440158928902644, 0.22454804373588763, -0.0896668866768... |
706.3382 | DLCQ Strings, Twist Fields and One-Loop Correlators on a Permutation
Orbifold | We investigate some aspects of the relationship between matrix string theory
and light-cone string field theory by analysing the correspondence between the
two-loop thermal partition function of DLCQ strings in flat space and the
integrated two-point correlator of twist fields in a symmetric product orbifold
conforma... | hep-th | we investigate some aspects of the relationship between matrix string theory and lightcone string field theory by analysing the correspondence between the twoloop thermal partition function of dlcq strings in flat space and the integrated twopoint correlator of twist fields in a symmetric product orbifold conformal fie... | [['we', 'investigate', 'some', 'aspects', 'of', 'the', 'relationship', 'between', 'matrix', 'string', 'theory', 'and', 'lightcone', 'string', 'field', 'theory', 'by', 'analysing', 'the', 'correspondence', 'between', 'the', 'twoloop', 'thermal', 'partition', 'function', 'of', 'dlcq', 'strings', 'in', 'flat', 'space', 'a... | [-0.17368654460956653, 0.1336370499782303, -0.10402448000696798, 0.16230725900735707, -0.04978381329836945, -0.1333753427894165, -0.0012911233659057568, 0.3374696507739524, -0.19331500228028745, -0.2406860912241973, 0.043057248732075094, -0.2624979856951783, -0.16859030848989884, 0.15143395201147844, -0.009199949389245... |
706.3383 | Universal behavior of baryons and mesons' transverse momentum
distributions in the framework of percolation of strings | In the framework of percolation of strings, we present predictions for the
$R_{AA}$ and $R_{CP}$ for mesons and baryons and for $\bar{p}/\pi^{0}$ ratios
at LHC energies.
| hep-ph | in the framework of percolation of strings we present predictions for the r_aa and r_cp for mesons and baryons and for barppi0 ratios at lhc energies | [['in', 'the', 'framework', 'of', 'percolation', 'of', 'strings', 'we', 'present', 'predictions', 'for', 'the', 'r_aa', 'and', 'r_cp', 'for', 'mesons', 'and', 'baryons', 'and', 'for', 'barppi0', 'ratios', 'at', 'lhc', 'energies']] | [0.002886585246485013, 0.22529079123901632, -0.1271577829387612, 0.17456831496495467, 0.10642437527600962, -0.13133029940609747, 0.035321884779617764, 0.37817010598687023, -0.128130838006305, -0.26148263472490585, -0.09555805668396015, -0.367066274325435, 0.08009805832989514, 0.11874043382704258, 0.12843172778733647, 0... |
706.3384 | Form factors of branch-point twist fields in quantum integrable models
and entanglement entropy | In this paper we compute the leading correction to the bipartite entanglement
entropy at large sub-system size, in integrable quantum field theories with
diagonal scattering matrices. We find a remarkably universal result, depending
only on the particle spectrum of the theory and not on the details of the
scattering ... | hep-th quant-ph | in this paper we compute the leading correction to the bipartite entanglement entropy at large subsystem size in integrable quantum field theories with diagonal scattering matrices we find a remarkably universal result depending only on the particle spectrum of the theory and not on the details of the scattering matrix... | [['in', 'this', 'paper', 'we', 'compute', 'the', 'leading', 'correction', 'to', 'the', 'bipartite', 'entanglement', 'entropy', 'at', 'large', 'subsystem', 'size', 'in', 'integrable', 'quantum', 'field', 'theories', 'with', 'diagonal', 'scattering', 'matrices', 'we', 'find', 'a', 'remarkably', 'universal', 'result', 'de... | [-0.13129307815000754, 0.10411827325330127, -0.09409061609714461, 0.059735414241863925, -0.023338311794213952, -0.07648935991164763, -0.0021630519366061148, 0.26812921917087146, -0.2721741352523995, -0.2497059992443114, 0.07817578672230328, -0.26271915774665433, -0.16336758952820674, 0.1556777131061112, -0.012723223237... |
706.3385 | Excitation energy dependence of symmetry energy of finite nuclei | A finite range density and momentum dependent effective interaction is used
to calculate the density and temperature dependence of the symmetry energy
coefficient Csym(rho,T) of infinite nuclear matter. This symmetry energy is
then used in the local density approximation to evaluate the excitation energy
dependence o... | nucl-th | a finite range density and momentum dependent effective interaction is used to calculate the density and temperature dependence of the symmetry energy coefficient csymrhot of infinite nuclear matter this symmetry energy is then used in the local density approximation to evaluate the excitation energy dependence of the ... | [['a', 'finite', 'range', 'density', 'and', 'momentum', 'dependent', 'effective', 'interaction', 'is', 'used', 'to', 'calculate', 'the', 'density', 'and', 'temperature', 'dependence', 'of', 'the', 'symmetry', 'energy', 'coefficient', 'csymrhot', 'of', 'infinite', 'nuclear', 'matter', 'this', 'symmetry', 'energy', 'is',... | [-0.0838482736291576, 0.2079794259117091, -0.16883974774634536, 0.12049925671094627, -0.04446328728447987, -0.03787642623050303, -0.007358786249179629, 0.3338250879056846, -0.22167522092556133, -0.3284992636829803, -0.013236039169309544, -0.3093013839701874, -0.018270309142108206, 0.09783335261141198, 0.074967374364975... |
706.3386 | XMM-Newton Observations of the Cataclysmic Variable GW Lib | XMM-Newton observations of the accreting, pulsating white dwarf in the
quiescent dwarf nova GW Librae were conducted to determine if the non-radial
pulsations present in previous UV and optical data affect the X-ray emission.
The non-radial pulsations are evident in the simultaneous Optical Monitor data
but are not d... | astro-ph | xmmnewton observations of the accreting pulsating white dwarf in the quiescent dwarf nova gw librae were conducted to determine if the nonradial pulsations present in previous uv and optical data affect the xray emission the nonradial pulsations are evident in the simultaneous optical monitor data but are not detected ... | [['xmmnewton', 'observations', 'of', 'the', 'accreting', 'pulsating', 'white', 'dwarf', 'in', 'the', 'quiescent', 'dwarf', 'nova', 'gw', 'librae', 'were', 'conducted', 'to', 'determine', 'if', 'the', 'nonradial', 'pulsations', 'present', 'in', 'previous', 'uv', 'and', 'optical', 'data', 'affect', 'the', 'xray', 'emissi... | [-0.06701651468888899, 0.1418773098470631, -0.07433398712997917, 0.11387775859541514, -0.17589596563167023, -0.11608927032317627, 0.11828005569105064, 0.4439793825220091, -0.16257293088622674, -0.31682066179840174, 0.0918510837196443, -0.34394554352867557, -0.027289457441039496, 0.2530128485540803, -0.08001058385354665... |
706.3387 | Vadim Kuznetsov. Informal Biography by Eyes of His First Adviser | The paper is dedicated to the memory of prominent theoretical physicist and
mathematician Dr. Vadim Kuznetsov who worked, in particular, in the fields of
the nonlinear dynamics, separation of variables, integrability theory, special
functions. It includes his short research biography, an account of the start of
his r... | nlin.SI math-ph math.CA math.MP | the paper is dedicated to the memory of prominent theoretical physicist and mathematician dr vadim kuznetsov who worked in particular in the fields of the nonlinear dynamics separation of variables integrability theory special functions it includes his short research biography an account of the start of his research ca... | [['the', 'paper', 'is', 'dedicated', 'to', 'the', 'memory', 'of', 'prominent', 'theoretical', 'physicist', 'and', 'mathematician', 'dr', 'vadim', 'kuznetsov', 'who', 'worked', 'in', 'particular', 'in', 'the', 'fields', 'of', 'the', 'nonlinear', 'dynamics', 'separation', 'of', 'variables', 'integrability', 'theory', 'sp... | [-0.10928606575665374, 0.05324139014232464, -0.10509929272208225, 0.08686126960243133, -0.1702112659846467, -0.15914680491443034, 0.024095408144165522, 0.2872925605452447, -0.21221931937530084, -0.2944585192879593, 0.060273982800060404, -0.3087363647754063, -0.15918831482391665, 0.17516207394914496, -0.1461196941909966... |
706.3388 | A Confining Strong First-Order Electroweak Phase Transition | In the Randall-Sundrum model where the radion is stabilized by a
Goldberger-Wise (GW) potential there is a supercooled transition from a
deconfined to a confined phase at temperatures orders of magnitude below the
typical Standard Model critical temperature. When the Higgs is localized at the
IR brane the electroweak... | hep-ph hep-th | in the randallsundrum model where the radion is stabilized by a goldbergerwise gw potential there is a supercooled transition from a deconfined to a confined phase at temperatures orders of magnitude below the typical standard model critical temperature when the higgs is localized at the ir brane the electroweak phase ... | [['in', 'the', 'randallsundrum', 'model', 'where', 'the', 'radion', 'is', 'stabilized', 'by', 'a', 'goldbergerwise', 'gw', 'potential', 'there', 'is', 'a', 'supercooled', 'transition', 'from', 'a', 'deconfined', 'to', 'a', 'confined', 'phase', 'at', 'temperatures', 'orders', 'of', 'magnitude', 'below', 'the', 'typical'... | [-0.1309560682416613, 0.3178200758870711, -0.07486869667168454, 0.10888039544665536, -0.0717946203974826, -0.1547191536361442, 0.07426227503783947, 0.30136294959754983, -0.20715983531119084, -0.27291613273340665, 0.0895070345570487, -0.2533703338336742, -0.03888052110266375, 0.13582466616186775, 0.023521881690559663, 0... |
706.3389 | Characterization of the Radon-Nikodym Property in terms of inverse
limits | We clarify the relation between inverse systems, the Radon-Nikodym property,
the Asymptotic Norming Property of James-Ho, and the GFDA spaces introduced in
our earlier paper on differentiability of Lipschitz maps into Banach spaces.
| math.FA math.MG | we clarify the relation between inverse systems the radonnikodym property the asymptotic norming property of jamesho and the gfda spaces introduced in our earlier paper on differentiability of lipschitz maps into banach spaces | [['we', 'clarify', 'the', 'relation', 'between', 'inverse', 'systems', 'the', 'radonnikodym', 'property', 'the', 'asymptotic', 'norming', 'property', 'of', 'jamesho', 'and', 'the', 'gfda', 'spaces', 'introduced', 'in', 'our', 'earlier', 'paper', 'on', 'differentiability', 'of', 'lipschitz', 'maps', 'into', 'banach', 's... | [-0.09891468839299294, 0.04373509878472936, -0.12406878870341086, 0.16807014939765777, -0.09001037700762672, -0.009287759871973146, 0.023840329636098636, 0.44245936865768126, -0.37452034652233124, -0.1078865303387565, 0.09773633941151802, -0.2773109524240417, -0.16208108610683872, 0.15268482856692805, -0.17534676236250... |
706.339 | Influence of friction on granular segregation | Vertical shaking of a mixture of small and large beads can lead to
segregation where the large beads either accumulate at the top of the sample,
the so called Brazil Nut effect (BNE), or at the bottom, the Reverse Brazil Nut
effect (RBNE). Here we demonstrate experimentally a sharp transition from the
RBNE to the BNE... | cond-mat.dis-nn cond-mat.soft | vertical shaking of a mixture of small and large beads can lead to segregation where the large beads either accumulate at the top of the sample the so called brazil nut effect bne or at the bottom the reverse brazil nut effect rbne here we demonstrate experimentally a sharp transition from the rbne to the bne when the ... | [['vertical', 'shaking', 'of', 'a', 'mixture', 'of', 'small', 'and', 'large', 'beads', 'can', 'lead', 'to', 'segregation', 'where', 'the', 'large', 'beads', 'either', 'accumulate', 'at', 'the', 'top', 'of', 'the', 'sample', 'the', 'so', 'called', 'brazil', 'nut', 'effect', 'bne', 'or', 'at', 'the', 'bottom', 'the', 're... | [-0.08956395286919647, 0.2843332026251837, -0.06307163919861379, 0.04292889878545937, -0.045023053933523204, -0.1235961966706734, 0.060413069297608576, 0.27651491002424766, -0.30258104464921515, -0.32874363476508545, 0.05023398129637108, -0.2951425003574083, -0.11794842659299704, 0.11983003130942387, -0.049662745209704... |
706.3391 | The Overdensity in Virgo, Sagittarius Debris, and the Asymmetric
Spheroid | We investigate the relationship between several previously identified
Galactic halo stellar structures in the direction of Virgo using imaging and
spectroscopic observations of F turnoff stars and blue horizontal branch stars
from the Sloan Digital Sky Survey (SDSS) and the Sloan Extension for Galactic
Understanding ... | astro-ph | we investigate the relationship between several previously identified galactic halo stellar structures in the direction of virgo using imaging and spectroscopic observations of f turnoff stars and blue horizontal branch stars from the sloan digital sky survey sdss and the sloan extension for galactic understanding and ... | [['we', 'investigate', 'the', 'relationship', 'between', 'several', 'previously', 'identified', 'galactic', 'halo', 'stellar', 'structures', 'in', 'the', 'direction', 'of', 'virgo', 'using', 'imaging', 'and', 'spectroscopic', 'observations', 'of', 'f', 'turnoff', 'stars', 'and', 'blue', 'horizontal', 'branch', 'stars',... | [-0.07727515966113885, 0.10082560771382783, -0.10283431124341844, 0.09355193925451943, -0.17904955804977807, -0.012427985904363097, 0.029104724978352228, 0.4456417842587228, -0.16405078714521662, -0.36159476683066366, 0.008456393588910536, -0.3224058627944922, -0.03136457739776442, 0.19507711419832335, -0.0519559261206... |
706.3392 | Solving SPDEs driven by colored noise: a chaos approach | An Ito-Skorokhod bi-linear equation driven by infinitely many independent
colored noises is considered in a normal triple of Hilbert spaces. The special
feature of the equation is the appearance of the Wick product in the definition
of the Ito-Skorokhod integral, requiring innovative approaches to computing the
solut... | math.PR math.AP | an itoskorokhod bilinear equation driven by infinitely many independent colored noises is considered in a normal triple of hilbert spaces the special feature of the equation is the appearance of the wick product in the definition of the itoskorokhod integral requiring innovative approaches to computing the solution a c... | [['an', 'itoskorokhod', 'bilinear', 'equation', 'driven', 'by', 'infinitely', 'many', 'independent', 'colored', 'noises', 'is', 'considered', 'in', 'a', 'normal', 'triple', 'of', 'hilbert', 'spaces', 'the', 'special', 'feature', 'of', 'the', 'equation', 'is', 'the', 'appearance', 'of', 'the', 'wick', 'product', 'in', '... | [-0.18805599145449792, 0.06692483257874404, -0.11927628216944522, 0.07774121449270015, -0.049040856824221116, -0.08232445993071681, -0.006825639954709177, 0.2823942934599104, -0.3025931405210042, -0.230474055948066, 0.14822818169995106, -0.27517902217157, -0.14980860879715485, 0.16798799117154714, -0.05062659562247086,... |
706.3393 | Towards a covariant model for cosmic self-acceleration | An explicitly covariant formulation is presented of a modified DGP scenario
proposed recently [1], to avoid the instability of the self-accelerating
branch. It is based on the introduction of a bulk scalar field with appropriate
non-minimal coupling to the bulk Einstein-Hilbert term. The method is general
and may be ... | hep-th astro-ph hep-ph | an explicitly covariant formulation is presented of a modified dgp scenario proposed recently 1 to avoid the instability of the selfaccelerating branch it is based on the introduction of a bulk scalar field with appropriate nonminimal coupling to the bulk einsteinhilbert term the method is general and may be applied to... | [['an', 'explicitly', 'covariant', 'formulation', 'is', 'presented', 'of', 'a', 'modified', 'dgp', 'scenario', 'proposed', 'recently', '1', 'to', 'avoid', 'the', 'instability', 'of', 'the', 'selfaccelerating', 'branch', 'it', 'is', 'based', 'on', 'the', 'introduction', 'of', 'a', 'bulk', 'scalar', 'field', 'with', 'app... | [-0.11689746498384258, 0.08985047573461832, -0.12718490316447886, 0.08753101361534474, -0.19352966909381478, -0.17982616517692804, -0.052616125785491685, 0.2790815110233697, -0.2224847486443733, -0.3032147190448913, 0.06570030792870304, -0.22853569042953578, -0.1849850252694027, 0.13188740059056064, -0.0716810391030528... |
706.3394 | Black Ring Deconstruction | We present a sample microstate for a black ring in four and five dimensional
language. The microstate consists of a black string microstate with an
additional D6-brane. We show that with an appropriate choice of parameters the
piece involving the black string microstate falls down a long AdS throat, whose
M-theory li... | hep-th | we present a sample microstate for a black ring in four and five dimensional language the microstate consists of a black string microstate with an additional d6brane we show that with an appropriate choice of parameters the piece involving the black string microstate falls down a long ads throat whose mtheory lift is a... | [['we', 'present', 'a', 'sample', 'microstate', 'for', 'a', 'black', 'ring', 'in', 'four', 'and', 'five', 'dimensional', 'language', 'the', 'microstate', 'consists', 'of', 'a', 'black', 'string', 'microstate', 'with', 'an', 'additional', 'd6brane', 'we', 'show', 'that', 'with', 'an', 'appropriate', 'choice', 'of', 'par... | [-0.1989486506387878, 0.09429426658971352, -0.07239410514011979, 0.07189935313586969, -0.1009966979483859, -0.15029570745537058, 0.046547576450393535, 0.29672659192091, -0.12674853420601442, -0.24970229446458128, 0.09469183839414305, -0.3110630180341944, -0.09006487425918189, 0.11838425744253282, -0.10489001873737344, ... |
706.3395 | Ion Charge States in Halo CMEs: What can we Learn about the Explosion? | We describe a new modeling approach to develop a more quantitative
understanding of the charge state distributions of the ions of various elements
detected in situ during halo Coronal Mass Ejection (CME) events by the Advanced
Composition Explorer (ACE) satellite. Using a model CME hydrodynamic evolution
based on obs... | astro-ph | we describe a new modeling approach to develop a more quantitative understanding of the charge state distributions of the ions of various elements detected in situ during halo coronal mass ejection cme events by the advanced composition explorer ace satellite using a model cme hydrodynamic evolution based on observatio... | [['we', 'describe', 'a', 'new', 'modeling', 'approach', 'to', 'develop', 'a', 'more', 'quantitative', 'understanding', 'of', 'the', 'charge', 'state', 'distributions', 'of', 'the', 'ions', 'of', 'various', 'elements', 'detected', 'in', 'situ', 'during', 'halo', 'coronal', 'mass', 'ejection', 'cme', 'events', 'by', 'the... | [-0.0608376883220053, 0.18425455618193712, -0.0590816751166055, 0.1166611237637216, -0.09123315736820313, -0.06301292229969768, 0.012989543786711527, 0.405638300321533, -0.22617235796168986, -0.38917339675823936, 0.05791627241954825, -0.2547193694102139, -0.05915216585365486, 0.17264266815995605, -0.029210349841651367,... |
706.3396 | Strings ending on branes from supergravity | We study geometries produced by brane intersections preserving eight
supercharges. Typical examples of such configurations are given by fundamental
strings ending on Dp branes and we construct gravity solutions describing such
intersections. The geometry is specified in terms of two functions obeying
coupled differen... | hep-th | we study geometries produced by brane intersections preserving eight supercharges typical examples of such configurations are given by fundamental strings ending on dp branes and we construct gravity solutions describing such intersections the geometry is specified in terms of two functions obeying coupled differential... | [['we', 'study', 'geometries', 'produced', 'by', 'brane', 'intersections', 'preserving', 'eight', 'supercharges', 'typical', 'examples', 'of', 'such', 'configurations', 'are', 'given', 'by', 'fundamental', 'strings', 'ending', 'on', 'dp', 'branes', 'and', 'we', 'construct', 'gravity', 'solutions', 'describing', 'such',... | [-0.18377785434159766, 0.11286562652263826, -0.04048199379066168, 0.11135066293057923, -0.03146904035814974, -0.18684540688539447, -0.03304763581915714, 0.2842116843755312, -0.15017146496011793, -0.2996654303889107, 0.08666996958267703, -0.30461931495375716, -0.13900300749414826, 0.13057472382319493, -0.103845473623029... |
706.3397 | Fock representation of the renormalized higher powers of white noise and
the Virasoro--Zamolodchikov--$w_{\infty} *$--Lie algebra | The identification of the $*$--Lie algebra of the renormalized higher powers
of white noise (RHPWN) and the analytic continuation of the second quantized
Virasoro--Zamolodchikov--$w_{\infty} *$--Lie algebra of conformal field theory
and high-energy physics, was recently established in \cite{id} based on results
obtai... | math-ph math.MP | the identification of the lie algebra of the renormalized higher powers of white noise rhpwn and the analytic continuation of the second quantized virasorozamolodchikovw_infty lie algebra of conformal field theory and highenergy physics was recently established in citeid based on results obtained in 1 and 2 in the pres... | [['the', 'identification', 'of', 'the', 'lie', 'algebra', 'of', 'the', 'renormalized', 'higher', 'powers', 'of', 'white', 'noise', 'rhpwn', 'and', 'the', 'analytic', 'continuation', 'of', 'the', 'second', 'quantized', 'virasorozamolodchikovw_infty', 'lie', 'algebra', 'of', 'conformal', 'field', 'theory', 'and', 'highen... | [-0.10766980933355323, 0.14509525616692068, -0.08712602906841009, 0.07891478102343778, -0.0697398566796134, -0.07457587169968367, -0.008482902900141198, 0.3645486460785226, -0.2565073420992121, -0.2269242649587492, 0.11306497020026048, -0.25000116240698844, -0.16614634989916036, 0.15821386561340964, -0.0570936624911458... |
706.3398 | The slice-ribbon conjecture for 3-stranded pretzel knots | We determine the smooth concordance order of the 3-stranded pretzel knots
P(p,q,r) with p,q,r odd. We show that each one of finite order is, in fact,
ribbon, thereby proving the slice-ribbon conjecture for this family of knots.
As corollaries we give new proofs of results first obtained by Fintushel-Stern
and Casson-... | math.GT | we determine the smooth concordance order of the 3stranded pretzel knots ppqr with pqr odd we show that each one of finite order is in fact ribbon thereby proving the sliceribbon conjecture for this family of knots as corollaries we give new proofs of results first obtained by fintushelstern and cassongordon | [['we', 'determine', 'the', 'smooth', 'concordance', 'order', 'of', 'the', '3stranded', 'pretzel', 'knots', 'ppqr', 'with', 'pqr', 'odd', 'we', 'show', 'that', 'each', 'one', 'of', 'finite', 'order', 'is', 'in', 'fact', 'ribbon', 'thereby', 'proving', 'the', 'sliceribbon', 'conjecture', 'for', 'this', 'family', 'of', '... | [-0.2205479602071493, 0.08122212933741656, -0.09203932330231457, 0.09419041667498794, -0.08721959185512627, -0.1852173823132819, -0.01122756956108645, 0.3367331068707155, -0.23821860354612856, -0.30172083431891367, 0.05599915521794602, -0.2099673973314245, -0.16638746190195283, 0.2328766462228754, -0.11064890202353983,... |
706.3399 | Penguin Loops for Nonleptonic B-Decays in the Standard Model: Is there a
Penguin Puzzle? | We compute standard model penguin amplitudes in nonleptonic B-decays to light
charmless mesons using tree amplitude data to fix hadronic parameters. The
leading calculation is carried out for the alphas(mb) penguin contributions
from charm quark, up quark, and magnetic penguin loops in the NDR and HV
renormalization ... | hep-ph | we compute standard model penguin amplitudes in nonleptonic bdecays to light charmless mesons using tree amplitude data to fix hadronic parameters the leading calculation is carried out for the alphasmb penguin contributions from charm quark up quark and magnetic penguin loops in the ndr and hv renormalization schemes ... | [['we', 'compute', 'standard', 'model', 'penguin', 'amplitudes', 'in', 'nonleptonic', 'bdecays', 'to', 'light', 'charmless', 'mesons', 'using', 'tree', 'amplitude', 'data', 'to', 'fix', 'hadronic', 'parameters', 'the', 'leading', 'calculation', 'is', 'carried', 'out', 'for', 'the', 'alphasmb', 'penguin', 'contributions... | [-0.092467143852703, 0.19546896558347485, -0.08902513875432734, 0.11011248049908318, -0.10334937342767657, -0.1310598941185986, 0.07501283559491331, 0.3105123619865275, -0.22157162887248527, -0.25682780392828203, 0.026003716890766058, -0.320778926932209, -0.0791610343418005, 0.18305085212396421, 0.02557739859692893, 0.... |
706.34 | Channel-Adapted Quantum Error Correction | Quantum error correction (QEC) is an essential concept for any quantum
information processing device. Typically, QEC is designed with minimal
assumptions about the noise process; this generic assumption exacts a high cost
in efficiency and performance. In physical systems, errors are not likely to be
arbitrary; rathe... | quant-ph | quantum error correction qec is an essential concept for any quantum information processing device typically qec is designed with minimal assumptions about the noise process this generic assumption exacts a high cost in efficiency and performance in physical systems errors are not likely to be arbitrary rather we will ... | [['quantum', 'error', 'correction', 'qec', 'is', 'an', 'essential', 'concept', 'for', 'any', 'quantum', 'information', 'processing', 'device', 'typically', 'qec', 'is', 'designed', 'with', 'minimal', 'assumptions', 'about', 'the', 'noise', 'process', 'this', 'generic', 'assumption', 'exacts', 'a', 'high', 'cost', 'in',... | [-0.1624030423281977, 0.08816864582294305, -0.059406683351406746, 0.11329779818306711, -0.0003281841940111202, -0.26409266070208043, 0.0584570046973964, 0.41825054279671836, -0.28469639154535153, -0.30405211760304296, 0.17656757326724015, -0.2109504146859623, -0.14382775801678713, 0.24490076458702484, -0.15301288835083... |
706.3401 | Measurement-based quantum computation beyond the one-way model | We introduce novel schemes for quantum computing based on local measurements
on entangled resource states. This work elaborates on the framework established
in [Phys. Rev. Lett. 98, 220503 (2007), quant-ph/0609149]. Our method makes use
of tools from many-body physics - matrix product states, finitely correlated
stat... | quant-ph | we introduce novel schemes for quantum computing based on local measurements on entangled resource states this work elaborates on the framework established in phys rev lett 98 220503 2007 quantph0609149 our method makes use of tools from manybody physics matrix product states finitely correlated states or projected ent... | [['we', 'introduce', 'novel', 'schemes', 'for', 'quantum', 'computing', 'based', 'on', 'local', 'measurements', 'on', 'entangled', 'resource', 'states', 'this', 'work', 'elaborates', 'on', 'the', 'framework', 'established', 'in', 'phys', 'rev', 'lett', '98', '220503', '2007', 'quantph0609149', 'our', 'method', 'makes',... | [-0.10642078617921746, 0.1529332554398697, -0.09028620037007266, 0.052534305705668645, -0.027266971260795126, -0.20560994749969763, 0.08103511684483079, 0.3599756527327649, -0.266832396576343, -0.293693402275929, 0.055338128469378245, -0.24858662844230622, -0.1525898522753066, 0.22516118146975161, -0.0851898985005075, ... |
706.3402 | Diffusion kinetic parameters from bulk diffusion limited gas release
processes | The diffusion of a bulk absorbed gas species out of spherical pebbles is
studied analytically, stressing the usefulness of the time integral of the
diffusion coefficient for analysis of arbitrary temperature schedule
experiments. Highly accurate approximations are introduced where the numeric
evaluation of the analyt... | cond-mat.mtrl-sci cond-mat.other | the diffusion of a bulk absorbed gas species out of spherical pebbles is studied analytically stressing the usefulness of the time integral of the diffusion coefficient for analysis of arbitrary temperature schedule experiments highly accurate approximations are introduced where the numeric evaluation of the analytic e... | [['the', 'diffusion', 'of', 'a', 'bulk', 'absorbed', 'gas', 'species', 'out', 'of', 'spherical', 'pebbles', 'is', 'studied', 'analytically', 'stressing', 'the', 'usefulness', 'of', 'the', 'time', 'integral', 'of', 'the', 'diffusion', 'coefficient', 'for', 'analysis', 'of', 'arbitrary', 'temperature', 'schedule', 'exper... | [-0.1077267693886908, 0.10908966307426621, -0.05470986768667554, 0.0009013722923680626, -0.045178706104727996, -0.09241622249627936, 0.03310983210009919, 0.31819712783841564, -0.27275023493787337, -0.2726778982464096, 0.05640750632610643, -0.2706417307169337, -0.07605915770052407, 0.19170316271938856, 0.054626438561987... |
706.3403 | Border trees of complex networks | The comprehensive characterization of the structure of complex networks is
essential to understand the dynamical processes which guide their evolution.
The discovery of the scale-free distribution and the small world property of
real networks were fundamental to stimulate more realistic models and to
understand some ... | physics.comp-ph | the comprehensive characterization of the structure of complex networks is essential to understand the dynamical processes which guide their evolution the discovery of the scalefree distribution and the small world property of real networks were fundamental to stimulate more realistic models and to understand some dyna... | [['the', 'comprehensive', 'characterization', 'of', 'the', 'structure', 'of', 'complex', 'networks', 'is', 'essential', 'to', 'understand', 'the', 'dynamical', 'processes', 'which', 'guide', 'their', 'evolution', 'the', 'discovery', 'of', 'the', 'scalefree', 'distribution', 'and', 'the', 'small', 'world', 'property', '... | [-0.16361676267739053, 0.09191605216524511, -0.014895924012221042, 0.09626553165296736, -0.07010896755742752, -0.0869020071127341, 0.06348983033482607, 0.3757664919248782, -0.3108416206620556, -0.3063680804001966, 0.14250622625556952, -0.2644488689035088, -0.2108652683839734, 0.15627224614166021, -0.02260254040759589, ... |
706.3404 | Disk-Planet Interaction Simulations: (I) Baroclinic Generation of
Vortensity and Non-Axisymmetric Rossby-Wave-Instability | We use a multi-dimensional hydrodynamics code to study the gravitational
interaction between an embedded planet and a protoplanetary disk with emphasis
on the generation of vortensity (potential vorticity) through a Baroclinic
Instability and subsequent development of Rossby-Wave-Instability (RWI). It is
found that t... | astro-ph | we use a multidimensional hydrodynamics code to study the gravitational interaction between an embedded planet and a protoplanetary disk with emphasis on the generation of vortensity potential vorticity through a baroclinic instability and subsequent development of rossbywaveinstability rwi it is found that the generat... | [['we', 'use', 'a', 'multidimensional', 'hydrodynamics', 'code', 'to', 'study', 'the', 'gravitational', 'interaction', 'between', 'an', 'embedded', 'planet', 'and', 'a', 'protoplanetary', 'disk', 'with', 'emphasis', 'on', 'the', 'generation', 'of', 'vortensity', 'potential', 'vorticity', 'through', 'a', 'baroclinic', '... | [-0.17339127592176423, 0.1377389287212407, -0.09896949579104267, 0.06351974078881603, -0.11448919909990168, -0.03458069251842219, 0.008979731006547809, 0.3031623320943066, -0.24677665226546855, -0.28921317473728336, 0.09056792959996403, -0.22797831235622087, -0.1306117481345327, 0.17863821044939587, -0.0316939701363574... |
706.3405 | On Point Coverings of Boxes in $\mathbb R^d$ | Families of boxes in $\mathbb R^d$ are considered. In the paper an upper
bound on the size of a minimum transversal in terms of the space dimension and
the independence number of the given family was improved.
| math.CO | families of boxes in mathbb rd are considered in the paper an upper bound on the size of a minimum transversal in terms of the space dimension and the independence number of the given family was improved | [['families', 'of', 'boxes', 'in', 'mathbb', 'rd', 'are', 'considered', 'in', 'the', 'paper', 'an', 'upper', 'bound', 'on', 'the', 'size', 'of', 'a', 'minimum', 'transversal', 'in', 'terms', 'of', 'the', 'space', 'dimension', 'and', 'the', 'independence', 'number', 'of', 'the', 'given', 'family', 'was', 'improved']] | [-0.1839630572074974, 0.1363940178829629, 0.029247378741667884, 0.011617528929098233, 0.006566735349494863, -0.021432623732835054, 0.008087665218595616, 0.25555645125112625, -0.19354944092196388, -0.3147791751433869, 0.1155174506758969, -0.28731076839707187, -0.08877640871985538, 0.2141570565920021, -0.1141084325625687... |
706.3406 | A Universal Interacting Crossover Regime in Two-Dimensional Quantum Dots | Interacting electrons in quantum dots with large Thouless number $g$ in the
three classical random matrix symmetry classes are well-understood. When a
specific type of spin-orbit coupling known to be dominant in two dimensional
semiconductor quantum dots is introduced, we show that a new interacting
quantum critical ... | cond-mat.mes-hall | interacting electrons in quantum dots with large thouless number g in the three classical random matrix symmetry classes are wellunderstood when a specific type of spinorbit coupling known to be dominant in two dimensional semiconductor quantum dots is introduced we show that a new interacting quantum critical crossove... | [['interacting', 'electrons', 'in', 'quantum', 'dots', 'with', 'large', 'thouless', 'number', 'g', 'in', 'the', 'three', 'classical', 'random', 'matrix', 'symmetry', 'classes', 'are', 'wellunderstood', 'when', 'a', 'specific', 'type', 'of', 'spinorbit', 'coupling', 'known', 'to', 'be', 'dominant', 'in', 'two', 'dimensi... | [-0.18473504779812616, 0.3235630869750868, -0.039554201603795476, 0.08621066948548198, -0.019999240978788108, -0.2530951654472842, -0.005602885774957637, 0.3042077401127571, -0.29095007030245584, -0.2739352564303539, -0.029131204958479755, -0.3107631296958201, -0.12082194498119254, 0.18426571062837654, 0.02783919264299... |
706.3407 | Abundances of Planetary Nebula M1-42 | The spectra of the planetary nebula M1-42 is reanalysed using spectral
measurements made in the mid-infrared with the Spitzer Space Telescope. The aim
is to determine the chemical composition of this object. We also make use of
ISO, IUE and ground based spectra. Abundances determined from the mid- and
far-infrared li... | astro-ph | the spectra of the planetary nebula m142 is reanalysed using spectral measurements made in the midinfrared with the spitzer space telescope the aim is to determine the chemical composition of this object we also make use of iso iue and ground based spectra abundances determined from the mid and farinfrared lines which ... | [['the', 'spectra', 'of', 'the', 'planetary', 'nebula', 'm142', 'is', 'reanalysed', 'using', 'spectral', 'measurements', 'made', 'in', 'the', 'midinfrared', 'with', 'the', 'spitzer', 'space', 'telescope', 'the', 'aim', 'is', 'to', 'determine', 'the', 'chemical', 'composition', 'of', 'this', 'object', 'we', 'also', 'mak... | [-0.011438247094499983, 0.1424460308999973, -0.06909146550812839, 0.041158690792077256, -0.034977068613645516, -0.06498925793732022, 0.025601713169354622, 0.40987532557689665, -0.14994794207935533, -0.36086421906028265, 0.0753236162701886, -0.30204484252730546, -0.015079448781447647, 0.19640958879464937, -0.04470343088... |
706.3408 | Current Renormalization in Finite Volume | For finite volume field theories with discrete translational invariance,
conserved currents can be additively renormalized by infrared effects. We
demonstrate this for pions using chiral perturbation theory coupled to
electromagnetism in a periodic box. Gauge invariant single particle effective
theories are construct... | hep-lat hep-ph nucl-th | for finite volume field theories with discrete translational invariance conserved currents can be additively renormalized by infrared effects we demonstrate this for pions using chiral perturbation theory coupled to electromagnetism in a periodic box gauge invariant single particle effective theories are constructed to... | [['for', 'finite', 'volume', 'field', 'theories', 'with', 'discrete', 'translational', 'invariance', 'conserved', 'currents', 'can', 'be', 'additively', 'renormalized', 'by', 'infrared', 'effects', 'we', 'demonstrate', 'this', 'for', 'pions', 'using', 'chiral', 'perturbation', 'theory', 'coupled', 'to', 'electromagneti... | [-0.15110611891658562, 0.287752857839223, -0.09200175854170488, 0.116616967022613, -0.07835609431236258, -0.16364423770897296, -0.04434421454304053, 0.3246768215257261, -0.2319170094302131, -0.26510707774044323, 0.049454888047572844, -0.3034879564398175, -0.13259017123103453, 0.08038392319091751, -0.04458115729115283, ... |
706.3409 | Spinless photon dark matter from two universal extra dimensions | We explore the properties of dark matter in theories with two universal extra
dimensions, where the lightest Kaluza-Klein state is a spin-0 neutral particle,
representing a six-dimensional photon polarized along the extra dimensions.
Annihilation of this 'spinless photon' proceeds predominantly through Higgs
boson ex... | hep-ph astro-ph | we explore the properties of dark matter in theories with two universal extra dimensions where the lightest kaluzaklein state is a spin0 neutral particle representing a sixdimensional photon polarized along the extra dimensions annihilation of this spinless photon proceeds predominantly through higgs boson exchange and... | [['we', 'explore', 'the', 'properties', 'of', 'dark', 'matter', 'in', 'theories', 'with', 'two', 'universal', 'extra', 'dimensions', 'where', 'the', 'lightest', 'kaluzaklein', 'state', 'is', 'a', 'spin0', 'neutral', 'particle', 'representing', 'a', 'sixdimensional', 'photon', 'polarized', 'along', 'the', 'extra', 'dime... | [-0.11823461790081878, 0.35013240764300346, -0.03682720630941604, 0.16218845060770554, -0.08859015177913775, -0.17372581118175032, 0.010843942091424042, 0.3207814705555037, -0.1920721542386227, -0.3347856338468954, -0.02970984161658743, -0.34726007753329363, 0.04300388059153265, 0.16702078895671107, 0.09674205487001909... |
706.341 | Noncommuting Flux Sectors in a Tabletop Experiment | We show how one can use superconductors and Josephson junctions to create a
laboratory system which can explore the groundstates of the free
electromagnetic field in a 3-manifold with torsion in its cohomology.
| hep-th | we show how one can use superconductors and josephson junctions to create a laboratory system which can explore the groundstates of the free electromagnetic field in a 3manifold with torsion in its cohomology | [['we', 'show', 'how', 'one', 'can', 'use', 'superconductors', 'and', 'josephson', 'junctions', 'to', 'create', 'a', 'laboratory', 'system', 'which', 'can', 'explore', 'the', 'groundstates', 'of', 'the', 'free', 'electromagnetic', 'field', 'in', 'a', '3manifold', 'with', 'torsion', 'in', 'its', 'cohomology']] | [-0.27059642874607537, 0.15555252002157044, -0.11013611283322627, 0.06829235685819929, -0.10955598160172954, -0.17235413669241648, -0.005288398725855531, 0.36586802983374306, -0.2748049103626699, -0.3008031554971681, -0.000640619256900567, -0.2555677049765081, -0.12982293466726938, 0.2020229302120931, -0.06633100596566... |
706.3411 | Cavity QED with a Bose-Einstein condensate | Cavity quantum electrodynamics (cavity QED) describes the coherent
interaction between matter and an electromagnetic field confined within a
resonator structure, and is providing a useful platform for developing concepts
in quantum information processing. By using high-quality resonators, a strong
coupling regime can... | quant-ph cond-mat.other | cavity quantum electrodynamics cavity qed describes the coherent interaction between matter and an electromagnetic field confined within a resonator structure and is providing a useful platform for developing concepts in quantum information processing by using highquality resonators a strong coupling regime can be reac... | [['cavity', 'quantum', 'electrodynamics', 'cavity', 'qed', 'describes', 'the', 'coherent', 'interaction', 'between', 'matter', 'and', 'an', 'electromagnetic', 'field', 'confined', 'within', 'a', 'resonator', 'structure', 'and', 'is', 'providing', 'a', 'useful', 'platform', 'for', 'developing', 'concepts', 'in', 'quantu... | [-0.15329066020220306, 0.22492241440968472, -0.06251792023339092, -0.043908488743064564, -0.022774772782549614, -0.2003798242857, 0.04141566906371529, 0.391586106793593, -0.2414399960577064, -0.2802329111890647, -0.001734101026477866, -0.27539337570536265, -0.07196450695313814, 0.2540585981523044, 0.007409875853300553,... |
706.3412 | On Canonical Forms of Complete Problems via First-order Projections | The class of problems complete for NP via first-order reductions is known to
be characterized by existential second-order sentences of a fixed form. All
such sentences are built around the so-called generalized IS-form of the
sentence that defines Independent-Set. This result can also be understood as
that every sent... | cs.CC | the class of problems complete for np via firstorder reductions is known to be characterized by existential secondorder sentences of a fixed form all such sentences are built around the socalled generalized isform of the sentence that defines independentset this result can also be understood as that every sentence that... | [['the', 'class', 'of', 'problems', 'complete', 'for', 'np', 'via', 'firstorder', 'reductions', 'is', 'known', 'to', 'be', 'characterized', 'by', 'existential', 'secondorder', 'sentences', 'of', 'a', 'fixed', 'form', 'all', 'such', 'sentences', 'are', 'built', 'around', 'the', 'socalled', 'generalized', 'isform', 'of',... | [-0.08896867416748037, 0.09404394219812329, -0.08213640345030859, 0.06722530998081207, -0.08885498574858353, -0.09924562220338341, -0.0035603495286012144, 0.35734680786167516, -0.3369362398845964, -0.27023159458087204, 0.08508779579395062, -0.23143820853087388, -0.17487043299771776, 0.23594271609124826, -0.085173705637... |
706.3413 | Orbital ordering in the ferromagnetic insulator Cs$_2$AgF$_4$ from first
principles | We found, using density-functional theory calculations within the generalized
gradient approximation, that Cs$_2$AgF$_4$ is stabilized in the insulating
orthorhombic phase rather than in the metallic tetragonal phase. The lattice
distortion present in the orthorhombic phase corresponds to the
$x^2-z^2$/$y^2-z^2$ hole... | cond-mat.mtrl-sci cond-mat.str-el | we found using densityfunctional theory calculations within the generalized gradient approximation that cs_2agf_4 is stabilized in the insulating orthorhombic phase rather than in the metallic tetragonal phase the lattice distortion present in the orthorhombic phase corresponds to the x2z2y2z2 holeorbital ordering of t... | [['we', 'found', 'using', 'densityfunctional', 'theory', 'calculations', 'within', 'the', 'generalized', 'gradient', 'approximation', 'that', 'cs_2agf_4', 'is', 'stabilized', 'in', 'the', 'insulating', 'orthorhombic', 'phase', 'rather', 'than', 'in', 'the', 'metallic', 'tetragonal', 'phase', 'the', 'lattice', 'distorti... | [-0.15938396041747183, 0.2060635255461204, -0.06325080770156569, 0.018919730130749355, -0.007459806594332414, -0.07616778937656254, 0.1365377548250503, 0.4111278394370207, -0.22622777122472013, -0.24167939244459072, 0.006184627471070382, -0.3153769704180637, -0.1499479519247654, 0.07249173758706699, 0.05512649366643191... |
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