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 |
|---|---|---|---|---|---|---|
710.2553 | Capacity of Linear Two-hop Mesh Networks with Rate Splitting,
Decode-and-forward Relaying and Cooperation | A linear mesh network is considered in which a single user per cell
communicates to a local base station via a dedicated relay (two-hop
communication). Exploiting the possibly relevant inter-cell channel gains, rate
splitting with successive cancellation in both hops is investigated as a
promising solution to improve... | cs.IT math.IT | a linear mesh network is considered in which a single user per cell communicates to a local base station via a dedicated relay twohop communication exploiting the possibly relevant intercell channel gains rate splitting with successive cancellation in both hops is investigated as a promising solution to improve the rat... | [['a', 'linear', 'mesh', 'network', 'is', 'considered', 'in', 'which', 'a', 'single', 'user', 'per', 'cell', 'communicates', 'to', 'a', 'local', 'base', 'station', 'via', 'a', 'dedicated', 'relay', 'twohop', 'communication', 'exploiting', 'the', 'possibly', 'relevant', 'intercell', 'channel', 'gains', 'rate', 'splittin... | [-0.2748537105147425, -0.007391739766909511, -0.007180927573821284, -0.003036003846357065, -0.09284871596019899, -0.2677183041257233, 0.19073111985311647, 0.34707861274979274, -0.3126817383396793, -0.23319595602905036, 0.056553305927696834, -0.2352623220001885, -0.16555599941754004, 0.10601794979744919, -0.086486222524... |
710.2554 | A Chiral Schwinger model, its Constraint Structure and Applications to
its Quantization | The Jackiw-Rajaraman version of the chiral Schwinger model is studied as a
function of the renormalization parameter. The constraints are obtained and
they are used to carry out canonical quantization of the model by means of
Dirac brackets. By introducing an additional scalar field, it is shown that the
model can be... | math-ph math.MP | the jackiwrajaraman version of the chiral schwinger model is studied as a function of the renormalization parameter the constraints are obtained and they are used to carry out canonical quantization of the model by means of dirac brackets by introducing an additional scalar field it is shown that the model can be made ... | [['the', 'jackiwrajaraman', 'version', 'of', 'the', 'chiral', 'schwinger', 'model', 'is', 'studied', 'as', 'a', 'function', 'of', 'the', 'renormalization', 'parameter', 'the', 'constraints', 'are', 'obtained', 'and', 'they', 'are', 'used', 'to', 'carry', 'out', 'canonical', 'quantization', 'of', 'the', 'model', 'by', '... | [-0.16836796434430512, 0.19193684431080235, -0.13073437568994287, 0.08588830472226852, -0.0902605423470959, -0.14276373700405925, -0.0017041496884746428, 0.3433379250793503, -0.24741441326645705, -0.3242279385956816, 0.04596201982796909, -0.22502384435098904, -0.1734834724249175, 0.1315316289352874, 0.00810082240077929... |
710.2555 | Geometric Aspects of Biological Sequence Comparison | We propose a general framework for converting global and local similarities
between biological sequences to quasi-metrics. In contrast to previous works,
our formulation allows asymmetric distances, originating from uneven weighting
of strings, that may induce non-trivial partial orders on sets of biosequences.
Furth... | q-bio.QM | we propose a general framework for converting global and local similarities between biological sequences to quasimetrics in contrast to previous works our formulation allows asymmetric distances originating from uneven weighting of strings that may induce nontrivial partial orders on sets of biosequences furthermore th... | [['we', 'propose', 'a', 'general', 'framework', 'for', 'converting', 'global', 'and', 'local', 'similarities', 'between', 'biological', 'sequences', 'to', 'quasimetrics', 'in', 'contrast', 'to', 'previous', 'works', 'our', 'formulation', 'allows', 'asymmetric', 'distances', 'originating', 'from', 'uneven', 'weighting',... | [-0.08473781881484148, 0.07476923742112429, -0.05858574000497659, 0.1650594072599037, -0.11736209695592668, -0.13708045107641204, 0.055647117591362594, 0.41619709064709204, -0.2777204685844481, -0.31498923809632806, 0.056165497034432035, -0.27558884314303034, -0.14852494695315174, 0.23121183226798095, -0.10716676113067... |
710.2556 | Continuum of consciousness: Mind uploading and resurrection of human
consciousness. Is there a place for physics, neuroscience and computers? | In this paper, I perform mental experiment to analyze hypothetical process of
mind uploading. That process suggested as a way to achieve resurrection of
human consciousness. Mind uploading can be seen as a migration process of the
core mental functions, which migrate from a human brain to an artificial
environment. T... | physics.gen-ph | in this paper i perform mental experiment to analyze hypothetical process of mind uploading that process suggested as a way to achieve resurrection of human consciousness mind uploading can be seen as a migration process of the core mental functions which migrate from a human brain to an artificial environment to simul... | [['in', 'this', 'paper', 'i', 'perform', 'mental', 'experiment', 'to', 'analyze', 'hypothetical', 'process', 'of', 'mind', 'uploading', 'that', 'process', 'suggested', 'as', 'a', 'way', 'to', 'achieve', 'resurrection', 'of', 'human', 'consciousness', 'mind', 'uploading', 'can', 'be', 'seen', 'as', 'a', 'migration', 'pr... | [-0.07246754736746702, 0.06144005941855257, -0.15843786941470364, 0.08472153961484821, -0.11705376589423523, -0.14027015896992082, 0.0061045844852589525, 0.3496735733892538, -0.29365525135473736, -0.321533716666982, 0.07159302848910468, -0.2513059010003916, -0.20535001016749416, 0.15445840338747785, -0.1079545824384663... |
710.2557 | The Nearby and Extremely Metal-Poor Galaxy CGCG 269-049 | We present Hubble Space Telescope (HST) and Spitzer Space Telescope images
and photometry of the extremely metal-poor (Z = 0.03 Z_sol) blue dwarf galaxy
CGCG 269-049. The HST images reveal a large population of red giant and
asymptotic giant branch stars, ruling out the possibility that the galaxy has
recently formed... | astro-ph | we present hubble space telescope hst and spitzer space telescope images and photometry of the extremely metalpoor z 003 z_sol blue dwarf galaxy cgcg 269049 the hst images reveal a large population of red giant and asymptotic giant branch stars ruling out the possibility that the galaxy has recently formed from the mag... | [['we', 'present', 'hubble', 'space', 'telescope', 'hst', 'and', 'spitzer', 'space', 'telescope', 'images', 'and', 'photometry', 'of', 'the', 'extremely', 'metalpoor', 'z', '003', 'z_sol', 'blue', 'dwarf', 'galaxy', 'cgcg', '269049', 'the', 'hst', 'images', 'reveal', 'a', 'large', 'population', 'of', 'red', 'giant', 'a... | [-0.031058900597448993, 0.11574641157325657, -0.08765020842390285, 0.08308255172420681, -0.13086260700051042, -0.0475376358551472, 0.08018540702340904, 0.44734856906519116, -0.09250896583946855, -0.3867735300672139, 0.0166275447512584, -0.3261297099232691, -0.019900269765556918, 0.18630726885445575, -0.0390043209386345... |
710.2558 | A Unified Theory for the Atmospheres of the Hot and Very Hot Jupiters:
Two Classes of Irradiated Atmospheres | We highlight the importance of gaseous TiO and VO opacity on the highly
irradiated close-in giant planets. The atmospheres of these planets naturally
fall into two classes that are somewhat analogous to the M- and L-type dwarfs.
Those that are warm enough to have appreciable opacity due to TiO and VO gases
we term th... | astro-ph | we highlight the importance of gaseous tio and vo opacity on the highly irradiated closein giant planets the atmospheres of these planets naturally fall into two classes that are somewhat analogous to the m and ltype dwarfs those that are warm enough to have appreciable opacity due to tio and vo gases we term the pm cl... | [['we', 'highlight', 'the', 'importance', 'of', 'gaseous', 'tio', 'and', 'vo', 'opacity', 'on', 'the', 'highly', 'irradiated', 'closein', 'giant', 'planets', 'the', 'atmospheres', 'of', 'these', 'planets', 'naturally', 'fall', 'into', 'two', 'classes', 'that', 'are', 'somewhat', 'analogous', 'to', 'the', 'm', 'and', 'l... | [-0.10188597225372738, 0.23543993504443017, -0.03971510738601764, 0.07860317752641588, -0.1014947333197862, -0.12771994058718059, 0.06478124516208508, 0.4408857580154062, -0.1755227114201087, -0.33806822391577424, 0.024389756125624797, -0.32693792297590757, -0.05870200284392439, 0.21056662470263832, -0.1039078515194823... |
710.2559 | Products in Hopf-Cyclic Cohomology | We construct several pairings in Hopf-cyclic cohomology of (co)module
(co)algebras with arbitrary coefficients. The key ideas instrumental in
constructing these pairings are the derived functor interpretation of
Hopf-cyclic and equivariant cyclic (co)homology, and the Yoneda interpretation
of Ext-groups. As a special... | math.KT math.QA | we construct several pairings in hopfcyclic cohomology of comodule coalgebras with arbitrary coefficients the key ideas instrumental in constructing these pairings are the derived functor interpretation of hopfcyclic and equivariant cyclic cohomology and the yoneda interpretation of extgroups as a special case of one o... | [['we', 'construct', 'several', 'pairings', 'in', 'hopfcyclic', 'cohomology', 'of', 'comodule', 'coalgebras', 'with', 'arbitrary', 'coefficients', 'the', 'key', 'ideas', 'instrumental', 'in', 'constructing', 'these', 'pairings', 'are', 'the', 'derived', 'functor', 'interpretation', 'of', 'hopfcyclic', 'and', 'equivaria... | [-0.21703714090154358, 0.0368157984786912, -0.07949223417886778, 0.12913895999694144, -0.09192373823178442, -0.16244661146774889, -0.048097346036841994, 0.35755484413943794, -0.4275602200901822, -0.20562235053236547, 0.08410686932038516, -0.15652067738793496, -0.16481600622156342, 0.17824885868743112, -0.17717402443093... |
710.256 | Error Channels and the Threshold for Fault-tolerant Quantum Computation | This dissertation treats the topics of threshold calculation, ancilla
construction, and non-standard error models. Chapter 2 introduces background
material ranging from quantum mechanics to classical coding to thresholds for
quantum computation. In Chapter 3 numerical and analytical means are used to
generate estimat... | quant-ph | this dissertation treats the topics of threshold calculation ancilla construction and nonstandard error models chapter 2 introduces background material ranging from quantum mechanics to classical coding to thresholds for quantum computation in chapter 3 numerical and analytical means are used to generate estimates of a... | [['this', 'dissertation', 'treats', 'the', 'topics', 'of', 'threshold', 'calculation', 'ancilla', 'construction', 'and', 'nonstandard', 'error', 'models', 'chapter', '2', 'introduces', 'background', 'material', 'ranging', 'from', 'quantum', 'mechanics', 'to', 'classical', 'coding', 'to', 'thresholds', 'for', 'quantum',... | [-0.06795645014208276, 0.11704407435972826, -0.01882004107348621, 0.06644697315525264, -0.03176050734240562, -0.21069976522121578, 0.0558464629529044, 0.3158036693045869, -0.24256743935402483, -0.3298686083033681, 0.11106168131693267, -0.24044671449344604, -0.19312626138795166, 0.23153078066185118, -0.10089352516195504... |
710.2561 | Crystallography without crystals I: the common-line method for
assembling a 3D intensity volume from single-particle scattering | We demonstrate that a common-line method can assemble a 3D oversampled
diffracted intensity distribution suitable for high-resolution structure
solution from a set of measured 2D diffraction patterns, as proposed in
experiments with an X-ray free electron laser (XFEL) (Neutze {\it et al.},
2000). Even for a flat Ewal... | q-bio.BM | we demonstrate that a commonline method can assemble a 3d oversampled diffracted intensity distribution suitable for highresolution structure solution from a set of measured 2d diffraction patterns as proposed in experiments with an xray free electron laser xfel neutze it et al 2000 even for a flat ewald sphere we show... | [['we', 'demonstrate', 'that', 'a', 'commonline', 'method', 'can', 'assemble', 'a', '3d', 'oversampled', 'diffracted', 'intensity', 'distribution', 'suitable', 'for', 'highresolution', 'structure', 'solution', 'from', 'a', 'set', 'of', 'measured', '2d', 'diffraction', 'patterns', 'as', 'proposed', 'in', 'experiments', ... | [-0.04836625409306689, 0.17977690964123766, -0.0404692619347816, 0.07090536498540789, -0.03355347518018394, -0.11889085846912092, 0.0610111689446904, 0.44095288125106935, -0.23655756001225994, -0.41504809921446295, 0.07938328191986507, -0.3194526952747021, -0.020237410523044237, 0.23863586751047122, -0.0348624532138811... |
710.2562 | Flow of a non-Newtonian fluids on a flat plate: I. boundary layer | This paper has been withdrawn by the authors as requested by the journal.
| math-ph math.MP | this paper has been withdrawn by the authors as requested by the journal | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'authors', 'as', 'requested', 'by', 'the', 'journal']] | [-0.051849561815078445, -0.0056348205902255494, -0.07618304599936192, -0.1004991584833568, -0.1393480429855677, -0.049276651814579964, 0.04166958718381535, 0.2856891883107332, -0.2531938112627428, -0.44801925466610837, 0.13133096007200387, -0.2939828304717174, -0.14337604048733527, 0.06278734553891879, -0.3007121467246... |
710.2563 | Scaling laws of solar and stellar flares | In this study we compile for the first time comprehensive data sets of solar
and stellar flare parameters, including flare peak temperatures T_p, flare peak
volume emission measures EM_p, and flare durations t_f from both solar and
stellar data, as well as flare length scales L from solar data. Key results are
that b... | astro-ph | in this study we compile for the first time comprehensive data sets of solar and stellar flare parameters including flare peak temperatures t_p flare peak volume emission measures em_p and flare durations t_f from both solar and stellar data as well as flare length scales l from solar data key results are that both the... | [['in', 'this', 'study', 'we', 'compile', 'for', 'the', 'first', 'time', 'comprehensive', 'data', 'sets', 'of', 'solar', 'and', 'stellar', 'flare', 'parameters', 'including', 'flare', 'peak', 'temperatures', 't_p', 'flare', 'peak', 'volume', 'emission', 'measures', 'em_p', 'and', 'flare', 'durations', 't_f', 'from', 'b... | [-0.022675297473151567, 0.24450357938715542, -0.02366760999337761, 0.16960880514418725, -0.022207223766455703, -0.08016276243258047, 0.06718469605813411, 0.42971976897172115, -0.14855176343647117, -0.399778558353958, 0.03909622331548685, -0.32058240686275874, -0.028814742078838666, 0.2653328419229624, -0.01468377892737... |
710.2564 | Slonczewski windmill with dissipation and asymmetry | J. Slonczewski invented spin-transfer effect in layered systems in 1996.
Among his first predictions was the regime of ``windmill motion'' of a
perfectly symmetric spin valve where the magnetizations of the layers rotate in
a fixed plane keeping the angle between them constant. Since ``windmill'' was
predicted to hap... | cond-mat.mtrl-sci | j slonczewski invented spintransfer effect in layered systems in 1996 among his first predictions was the regime of windmill motion of a perfectly symmetric spin valve where the magnetizations of the layers rotate in a fixed plane keeping the angle between them constant since windmill was predicted to happen in the cas... | [['j', 'slonczewski', 'invented', 'spintransfer', 'effect', 'in', 'layered', 'systems', 'in', '1996', 'among', 'his', 'first', 'predictions', 'was', 'the', 'regime', 'of', 'windmill', 'motion', 'of', 'a', 'perfectly', 'symmetric', 'spin', 'valve', 'where', 'the', 'magnetizations', 'of', 'the', 'layers', 'rotate', 'in',... | [-0.20260044072520222, 0.18439779835069306, -0.010076421658163304, 0.020003350854564745, -0.08149940350379509, -0.15391378200424094, 0.0259152909193735, 0.3631671813245003, -0.2686131383834563, -0.3020305267137873, 0.04755540162005781, -0.2908790657586594, -0.1398877663345734, 0.2010052856448647, -0.007486271284442473,... |
710.2565 | The chiral transition on a 24^3x10 lattice with N_f=2 clover sea quarks
studied by overlap valence quarks | Overlap fermions are particularly well suited to study the finite temperature
dynamics of the chiral symmetry restoration transition of QCD, which might be
just an analytic crossover. Using gauge field configurations on a 24^3x10
lattice with N_f=2 flavours of dynamical Wilson-clover quarks generated by the
DIK colla... | hep-lat | overlap fermions are particularly well suited to study the finite temperature dynamics of the chiral symmetry restoration transition of qcd which might be just an analytic crossover using gauge field configurations on a 243x10 lattice with n_f2 flavours of dynamical wilsonclover quarks generated by the dik collaboratio... | [['overlap', 'fermions', 'are', 'particularly', 'well', 'suited', 'to', 'study', 'the', 'finite', 'temperature', 'dynamics', 'of', 'the', 'chiral', 'symmetry', 'restoration', 'transition', 'of', 'qcd', 'which', 'might', 'be', 'just', 'an', 'analytic', 'crossover', 'using', 'gauge', 'field', 'configurations', 'on', 'a',... | [-0.14575656629464598, 0.29516910424611825, -0.08366144551594819, 0.0939318148593884, -0.052249155046107866, -0.07490900146391748, 0.06138663485762663, 0.3729834364494309, -0.18757941177803636, -0.26373405921428156, 0.0651004383059141, -0.28310756727296393, -0.12810906563754543, 0.020659814258882154, 0.0819220377743477... |
710.2566 | Coherent Spin Manipulations of a Polarized Beam With a Localized RF
Magnetic Field | The coherent manipulation of spin observables in storage rings provides
opportunities to test the application of some fundamental dynamical principles.
In this context, it is possible to confirm, using gauge invariance and Lorentz
invariance, a conjecture framed by A. M. Kondratenko concerning the "natural"
or "intri... | hep-ph | the coherent manipulation of spin observables in storage rings provides opportunities to test the application of some fundamental dynamical principles in this context it is possible to confirm using gauge invariance and lorentz invariance a conjecture framed by a m kondratenko concerning the natural or intrinsic resona... | [['the', 'coherent', 'manipulation', 'of', 'spin', 'observables', 'in', 'storage', 'rings', 'provides', 'opportunities', 'to', 'test', 'the', 'application', 'of', 'some', 'fundamental', 'dynamical', 'principles', 'in', 'this', 'context', 'it', 'is', 'possible', 'to', 'confirm', 'using', 'gauge', 'invariance', 'and', 'l... | [-0.1847748153287774, 0.18716733075598313, -0.049278483484298564, 0.04565014431360536, -0.09750950634658623, -0.11600024161900645, 0.040628143904121734, 0.33655482867302805, -0.26559821798358685, -0.3013577643208779, 0.05441062230518302, -0.20180368939047463, -0.12019462458780393, 0.23012348802205032, -0.00505295761663... |
710.2567 | Electronic States of Magnetic Quantum Dots | We study quantum states of electrons in magnetically doped quantum dots as a
function of exchange coupling between electron and impurity spins, the strength
of Coulomb interaction, confining potential, and the number of electrons. The
magnetic phase diagram of quantum dots, doped with a large number of magnetic
Mn im... | cond-mat.mes-hall cond-mat.str-el | we study quantum states of electrons in magnetically doped quantum dots as a function of exchange coupling between electron and impurity spins the strength of coulomb interaction confining potential and the number of electrons the magnetic phase diagram of quantum dots doped with a large number of magnetic mn impuritie... | [['we', 'study', 'quantum', 'states', 'of', 'electrons', 'in', 'magnetically', 'doped', 'quantum', 'dots', 'as', 'a', 'function', 'of', 'exchange', 'coupling', 'between', 'electron', 'and', 'impurity', 'spins', 'the', 'strength', 'of', 'coulomb', 'interaction', 'confining', 'potential', 'and', 'the', 'number', 'of', 'e... | [-0.17360423073511233, 0.2710256061506119, 0.007473789659949641, 0.03706212901284523, 0.045882828496608206, -0.18131242367213196, 0.0864768126004051, 0.37699860241264105, -0.2684488437971044, -0.36349275205848797, -0.07614553809275315, -0.3145836318250407, -0.07112964234230193, 0.16558282838950894, 0.0666298377045402, ... |
710.2568 | Phase transition between non-extremal and extremal Reissner-Nordstr\"om
black holes | We discuss the phase transition between non-extremal and extremal
Reissner-Nordstr\"om black holes. This transition is considered as the
$T \to 0$ limit of the transition between the non-extremal and near-extremal
black holes.
We show that an evaporating process from non-extremal black hole to extremal
one is pos... | gr-qc | we discuss the phase transition between nonextremal and extremal reissnernordstrom black holes this transition is considered as the t to 0 limit of the transition between the nonextremal and nearextremal black holes we show that an evaporating process from nonextremal black hole to extremal one is possible to occur but... | [['we', 'discuss', 'the', 'phase', 'transition', 'between', 'nonextremal', 'and', 'extremal', 'reissnernordstrom', 'black', 'holes', 'this', 'transition', 'is', 'considered', 'as', 'the', 't', 'to', '0', 'limit', 'of', 'the', 'transition', 'between', 'the', 'nonextremal', 'and', 'nearextremal', 'black', 'holes', 'we', ... | [-0.14184775192609705, 0.16191139703847368, -0.02450886404330141, 0.1735292232252106, -0.05331130457644382, -0.17872430082264074, 0.06366602034213838, 0.31789769329067863, -0.1644315838897496, -0.2705337038012535, 0.10568617869644646, -0.3801480287141847, -0.1374726849241873, 0.14128341178378362, -0.057062251231727305,... |
710.2569 | Graphical Representation of SUSY and Application to QFT | We present a graphical representation of the supersymmetry and the graphical
calculation. Calculation is demonstrated for 4D Wess-Zumino model and for Super
QED. The chiral operators are graphically expressed in an illuminating way. The
tedious part of SUSY calculation, due to manipulating chiral suffixes, reduces
co... | hep-th | we present a graphical representation of the supersymmetry and the graphical calculation calculation is demonstrated for 4d wesszumino model and for super qed the chiral operators are graphically expressed in an illuminating way the tedious part of susy calculation due to manipulating chiral suffixes reduces considerab... | [['we', 'present', 'a', 'graphical', 'representation', 'of', 'the', 'supersymmetry', 'and', 'the', 'graphical', 'calculation', 'calculation', 'is', 'demonstrated', 'for', '4d', 'wesszumino', 'model', 'and', 'for', 'super', 'qed', 'the', 'chiral', 'operators', 'are', 'graphically', 'expressed', 'in', 'an', 'illuminating... | [-0.09936330527067185, 0.14235268780292246, -0.019800668731331825, 0.10050067748408764, -0.12004594497848302, -0.12880937016569077, -0.04644941339734942, 0.36623986646533013, -0.17948531076312066, -0.3068831600365229, 0.05245054904138669, -0.24533631490543484, -0.20594964813441038, 0.11969588933046907, -0.0506216094037... |
710.257 | The separability of tripartite Gaussian state with amplification and
amplitude damping | Tripartite three mode Gaussian state undergoes parametric amplification and
amplitude damping as well as thermal noise is studied. In the case of a state
totally symmetrically interacting with the environment, the time dependent
correlation matrix of the state in evolution is given. The conditions for fully
separabil... | quant-ph | tripartite three mode gaussian state undergoes parametric amplification and amplitude damping as well as thermal noise is studied in the case of a state totally symmetrically interacting with the environment the time dependent correlation matrix of the state in evolution is given the conditions for fully separability a... | [['tripartite', 'three', 'mode', 'gaussian', 'state', 'undergoes', 'parametric', 'amplification', 'and', 'amplitude', 'damping', 'as', 'well', 'as', 'thermal', 'noise', 'is', 'studied', 'in', 'the', 'case', 'of', 'a', 'state', 'totally', 'symmetrically', 'interacting', 'with', 'the', 'environment', 'the', 'time', 'depe... | [-0.16279623244476857, 0.225353603083335, -0.07783114470419336, 0.020514059309908725, 0.019059763950311014, -0.17955823718249553, -0.009369325366054402, 0.36234017504287547, -0.23532141192403974, -0.22970715944166678, 0.12416155538884312, -0.2657338288597396, -0.07997594018787389, 0.11245793968316961, 0.057851437143370... |
710.2571 | Rigidity of graph products of abelian groups | We show that if $G$ is a group and $G$ has a graph-product decomposition with
finitely-generated abelian vertex groups, then $G$ has two canonical
decompositions as a graph product of groups: a unique decomposition in which
each vertex group is a directly-indecomposable cyclic group, and a unique
decomposition in whi... | math.GR | we show that if g is a group and g has a graphproduct decomposition with finitelygenerated abelian vertex groups then g has two canonical decompositions as a graph product of groups a unique decomposition in which each vertex group is a directlyindecomposable cyclic group and a unique decomposition in which each vertex... | [['we', 'show', 'that', 'if', 'g', 'is', 'a', 'group', 'and', 'g', 'has', 'a', 'graphproduct', 'decomposition', 'with', 'finitelygenerated', 'abelian', 'vertex', 'groups', 'then', 'g', 'has', 'two', 'canonical', 'decompositions', 'as', 'a', 'graph', 'product', 'of', 'groups', 'a', 'unique', 'decomposition', 'in', 'whic... | [-0.17387769210177498, 0.11217718370057442, -0.1942004468040289, -0.028263889242127235, -0.16758469947789972, -0.13162521686329431, 0.023040923365467304, 0.41765401525913765, -0.3085153576590725, -0.20027718898160635, 0.1312373293315161, -0.2716481376036599, -0.1490167824400438, 0.13040653925791784, -0.097264619531563,... |
710.2572 | Flow of a non-Newtonian fluids on a flat plate: II. heat transfer | This paper has been withdrawn by the authors as requested by the journal.
| math-ph math.MP | this paper has been withdrawn by the authors as requested by the journal | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'authors', 'as', 'requested', 'by', 'the', 'journal']] | [-0.051849561815078445, -0.0056348205902255494, -0.07618304599936192, -0.1004991584833568, -0.1393480429855677, -0.049276651814579964, 0.04166958718381535, 0.2856891883107332, -0.2531938112627428, -0.44801925466610837, 0.13133096007200387, -0.2939828304717174, -0.14337604048733527, 0.06278734553891879, -0.3007121467246... |
710.2573 | On the automorphisms of a graph product of abelian groups | We study the automorphisms of a graph product of finitely-generated abelian
groups W. More precisely, we study a natural subgroup Aut* W of Aut W, with
Aut* W = Aut W whenever vertex groups are finite and in a number of other
cases. We prove a number of structure results, including a semi-direct product
decomposition... | math.GR | we study the automorphisms of a graph product of finitelygenerated abelian groups w more precisely we study a natural subgroup aut w of aut w with aut w aut w whenever vertex groups are finite and in a number of other cases we prove a number of structure results including a semidirect product decomposition of aut w in ... | [['we', 'study', 'the', 'automorphisms', 'of', 'a', 'graph', 'product', 'of', 'finitelygenerated', 'abelian', 'groups', 'w', 'more', 'precisely', 'we', 'study', 'a', 'natural', 'subgroup', 'aut', 'w', 'of', 'aut', 'w', 'with', 'aut', 'w', 'aut', 'w', 'whenever', 'vertex', 'groups', 'are', 'finite', 'and', 'in', 'a', 'n... | [-0.19165766213991448, 0.15873657859046944, -0.06278044250793754, -0.017615924838173667, -0.10616467780782841, -0.12263090152991936, 0.030124583560973407, 0.39804914803244174, -0.3418706958240364, -0.23775117257609962, 0.10908242032310227, -0.2791918602772057, -0.1036795993873966, 0.23417536881752313, -0.08311107626650... |
710.2574 | A Comparison Theorem and A Sharp Bound via the Ricci Flow | We prove a comparison theorem for the compact surfaces with negative Euler
characteristic via the Ricci flow.
| math.DG math.AP | we prove a comparison theorem for the compact surfaces with negative euler characteristic via the ricci flow | [['we', 'prove', 'a', 'comparison', 'theorem', 'for', 'the', 'compact', 'surfaces', 'with', 'negative', 'euler', 'characteristic', 'via', 'the', 'ricci', 'flow']] | [-0.21107274047372973, 0.0600630516624626, -0.19132035343414722, 0.11347092249814202, -0.11353965563809171, -0.19982262895278194, -0.11809201275601107, 0.31849457192070346, -0.2616009953267434, -0.17823426808942766, 0.11045698665411156, -0.2427311328047996, -0.10441640567253618, 0.2718716169543126, -0.05824161868761567... |
710.2575 | Scattering of a Klein-Gordon particle by a Hulth\'en potential | The Klein-Gordon equation in the presence of a spatially one-dimensional
Hulth\'en potential is solved exactly and the scattering solutions are obtained
in terms of hypergeometric functions. The transmission coefficient is derived
by the matching conditions on the wavefunctions and the condition for the
existence of ... | quant-ph | the kleingordon equation in the presence of a spatially onedimensional hulthen potential is solved exactly and the scattering solutions are obtained in terms of hypergeometric functions the transmission coefficient is derived by the matching conditions on the wavefunctions and the condition for the existence of transmi... | [['the', 'kleingordon', 'equation', 'in', 'the', 'presence', 'of', 'a', 'spatially', 'onedimensional', 'hulthen', 'potential', 'is', 'solved', 'exactly', 'and', 'the', 'scattering', 'solutions', 'are', 'obtained', 'in', 'terms', 'of', 'hypergeometric', 'functions', 'the', 'transmission', 'coefficient', 'is', 'derived',... | [-0.19070301136733697, 0.0744714641367041, -0.06713879123211854, 0.06364436672135655, -0.022816007199238927, -0.1459142068910989, -0.04548247560991773, 0.3286296163818666, -0.24512061290442944, -0.24570783836737511, 0.10609759672337936, -0.29141009801496115, -0.17071729308615127, 0.18078053284377332, 0.0196849386991253... |
710.2576 | Transmission resonances for a Dirac particle in a one-dimensional
Hulth\'en potential | We have solved exactly the two-component Dirac equation in the presence of a
spatially one-dimensional Hulth\'en potential, and presented the Dirac spinors
of scattering states in terms of hypergeometric functions. We have calculated
the reflection and transmission coefficients by the matching conditions on the
wavef... | math-ph math.MP nucl-th quant-ph | we have solved exactly the twocomponent dirac equation in the presence of a spatially onedimensional hulthen potential and presented the dirac spinors of scattering states in terms of hypergeometric functions we have calculated the reflection and transmission coefficients by the matching conditions on the wavefunctions... | [['we', 'have', 'solved', 'exactly', 'the', 'twocomponent', 'dirac', 'equation', 'in', 'the', 'presence', 'of', 'a', 'spatially', 'onedimensional', 'hulthen', 'potential', 'and', 'presented', 'the', 'dirac', 'spinors', 'of', 'scattering', 'states', 'in', 'terms', 'of', 'hypergeometric', 'functions', 'we', 'have', 'calc... | [-0.18537219392432683, 0.0938358382537853, -0.0729324792822202, 0.04040539402352727, -0.015879236036857616, -0.1438439163831535, 0.008852862088225675, 0.35879703554446285, -0.2122895433365003, -0.2581416633573995, 0.05727215428782654, -0.2776229999338587, -0.1752187776433277, 0.14705229088987992, 0.045084819913018444, ... |
710.2577 | Observation of anomalous Upsilon(1S)pi+pi- and Upsilon(2S)pi+pi-
production near the Upsilon(5S) resonance | We report the first observation of e+e- -> Upsilon(1S)pi+pi-,
Upsilon(2S)pi+pi-, and first evidence for e+e- -> Upsilon(3S)pi+pi-,
Upsilon(1S)K+K-, near the peak of the Upsilon(5S) resonance at sqrt{s}~10.87
GeV. The results are based on a data sample of 21.7 fb^-1 collected with the
Belle detector at the KEKB e+e- c... | hep-ex | we report the first observation of ee upsilon1spipi upsilon2spipi and first evidence for ee upsilon3spipi upsilon1skk near the peak of the upsilon5s resonance at sqrts1087 gev the results are based on a data sample of 217 fb1 collected with the belle detector at the kekb ee collider attributing the signals to the upsil... | [['we', 'report', 'the', 'first', 'observation', 'of', 'ee', 'upsilon1spipi', 'upsilon2spipi', 'and', 'first', 'evidence', 'for', 'ee', 'upsilon3spipi', 'upsilon1skk', 'near', 'the', 'peak', 'of', 'the', 'upsilon5s', 'resonance', 'at', 'sqrts1087', 'gev', 'the', 'results', 'are', 'based', 'on', 'a', 'data', 'sample', '... | [-0.07343612551472455, 0.16840934389591272, -0.0467196314199136, 0.10347213999525008, -0.002430775265628933, -0.09242502150430094, 0.07658304740204522, 0.3183840913479078, -0.09442771627512382, -0.3394051332782843, -0.07391634133948695, -0.5120068535503774, 0.13326570347394093, 0.19013873463044736, 0.12067678484991931,... |
710.2578 | The Lightest Higgs Boson and Relic Neutralino in the MSSM with CP
Violation | In a minimal supersymmetric extension of the standard model (MSSM) with
explicit CP violation a mass of the lightest Higgs boson H_1 in the range 7
GeV} < M_{H_1} < 10 GeV is experimentally allowed by present accelerator
limits. In the same scenario a lightest neutralino as light as 2.9 GeV can be a
viable dark matte... | hep-ph | in a minimal supersymmetric extension of the standard model mssm with explicit cp violation a mass of the lightest higgs boson h_1 in the range 7 gev m_h_1 10 gev is experimentally allowed by present accelerator limits in the same scenario a lightest neutralino as light as 29 gev can be a viable dark matter candidate p... | [['in', 'a', 'minimal', 'supersymmetric', 'extension', 'of', 'the', 'standard', 'model', 'mssm', 'with', 'explicit', 'cp', 'violation', 'a', 'mass', 'of', 'the', 'lightest', 'higgs', 'boson', 'h_1', 'in', 'the', 'range', '7', 'gev', 'm_h_1', '10', 'gev', 'is', 'experimentally', 'allowed', 'by', 'present', 'accelerator'... | [-0.08484341061973412, 0.3068218215767826, -0.030292049336380193, 0.24248763328817274, -0.10588735368634973, -0.21012556339348, 0.05714141147410763, 0.2864374034771962, -0.17102948125850942, -0.38120319795395646, 0.01243047375464812, -0.23603251016964868, 0.05770118960312435, 0.16000314807752147, 0.03538615122504, 0.07... |
710.2579 | Baryons and the Chern-Simons term in holographic QCD with three flavors | We study dynamical baryons in the holographic QCD model of Sakai and Sugimoto
in the case of three flavors and with special interest in the construction of
the Chern-Simons (CS) term. The baryon classical solution in this model is
given by the BPST instanton, and we carry out the collective coordinate
quantization of... | hep-th hep-ph | we study dynamical baryons in the holographic qcd model of sakai and sugimoto in the case of three flavors and with special interest in the construction of the chernsimons cs term the baryon classical solution in this model is given by the bpst instanton and we carry out the collective coordinate quantization of the so... | [['we', 'study', 'dynamical', 'baryons', 'in', 'the', 'holographic', 'qcd', 'model', 'of', 'sakai', 'and', 'sugimoto', 'in', 'the', 'case', 'of', 'three', 'flavors', 'and', 'with', 'special', 'interest', 'in', 'the', 'construction', 'of', 'the', 'chernsimons', 'cs', 'term', 'the', 'baryon', 'classical', 'solution', 'in... | [-0.13374366909265517, 0.12403618590001965, -0.07526144015469721, 0.029607922039992574, -0.08688410885099854, -0.13944484730932993, 0.036625740880845116, 0.2626155349026833, -0.1981985048349348, -0.2636397925338575, 0.06902252308791504, -0.2637315494357608, -0.1403360446382846, 0.05513408700769235, -0.05911274096662444... |
710.258 | Thermodynamic Studies on Non Centrosymmetric Superconductors by AC
Calorimetry under High Pressures | We investigated the non centrosymmetric superconductors CePt$_3$Si and UIr by
the ac heat capacity measurement under pressures. We determined the pressure
phase diagrams of these compounds. In CePt$_3$Si, the N\'{e}el temperature
$T_{\rm N}$ = 2.2 K decreases with increasing pressure and becomes zero at the
critical ... | cond-mat.str-el cond-mat.supr-con | we investigated the non centrosymmetric superconductors cept_3si and uir by the ac heat capacity measurement under pressures we determined the pressure phase diagrams of these compounds in cept_3si the neel temperature t_rm n 22 k decreases with increasing pressure and becomes zero at the critical pressure p_rm af sime... | [['we', 'investigated', 'the', 'non', 'centrosymmetric', 'superconductors', 'cept_3si', 'and', 'uir', 'by', 'the', 'ac', 'heat', 'capacity', 'measurement', 'under', 'pressures', 'we', 'determined', 'the', 'pressure', 'phase', 'diagrams', 'of', 'these', 'compounds', 'in', 'cept_3si', 'the', 'neel', 'temperature', 't_rm'... | [-0.2158920838145187, 0.29040294858395765, -0.026045939082758048, -0.06429124117413586, -0.04049098975201314, -0.1544035572004882, 0.17092874469109684, 0.3768666025452517, -0.22841960149943022, -0.29127019137345456, 0.06135966737056151, -0.38543382905222273, -0.015607215199820898, 0.1771870633385874, 0.0615703185502678... |
710.2581 | Quantum criticality of the Lipkin-Meshkov-Glick Model in terms of
fidelity susceptibility | We study the critical properties of the Lipkin-Meshkov-Glick Model in terms
of the fidelity susceptibility. By using the Holstein-Primakoff transformation,
we obtain explicitly the critical exponent of the fidelity susceptibility
around the second-order quantum phase transition point. Our results provide a
rare analy... | quant-ph | we study the critical properties of the lipkinmeshkovglick model in terms of the fidelity susceptibility by using the holsteinprimakoff transformation we obtain explicitly the critical exponent of the fidelity susceptibility around the secondorder quantum phase transition point our results provide a rare analytical cas... | [['we', 'study', 'the', 'critical', 'properties', 'of', 'the', 'lipkinmeshkovglick', 'model', 'in', 'terms', 'of', 'the', 'fidelity', 'susceptibility', 'by', 'using', 'the', 'holsteinprimakoff', 'transformation', 'we', 'obtain', 'explicitly', 'the', 'critical', 'exponent', 'of', 'the', 'fidelity', 'susceptibility', 'ar... | [-0.19246589151521523, 0.16522038287172716, -0.057506061322055754, 0.0334575701955085, 0.036136030463967475, -0.1401784273671607, 0.11256481158857544, 0.3169741973731046, -0.1969773395607869, -0.2273628773788611, 0.07679504168840746, -0.338718796869119, -0.20750471596916517, 0.22229771243718763, 0.057412851291398205, 0... |
710.2582 | Poisson statistics of eigenvalues in the hierarchical Anderson model | We study the eigenvalue statistics for the hieracharchial Anderson model of
Molchanov. We prove Poisson fluctuations at arbitrary disorder, when the the
model has spectral dimension d<1. The proof is based on Minami's technique and
we give an elementary exposition of the probabilistic arguments.
| math-ph math.MP | we study the eigenvalue statistics for the hieracharchial anderson model of molchanov we prove poisson fluctuations at arbitrary disorder when the the model has spectral dimension d1 the proof is based on minamis technique and we give an elementary exposition of the probabilistic arguments | [['we', 'study', 'the', 'eigenvalue', 'statistics', 'for', 'the', 'hieracharchial', 'anderson', 'model', 'of', 'molchanov', 'we', 'prove', 'poisson', 'fluctuations', 'at', 'arbitrary', 'disorder', 'when', 'the', 'the', 'model', 'has', 'spectral', 'dimension', 'd1', 'the', 'proof', 'is', 'based', 'on', 'minamis', 'techn... | [-0.0888395588628428, 0.08513367184753216, -0.1628329927903102, 0.12005650842573147, -0.03500877254707522, -0.17020579648399076, 0.013297598798174498, 0.31760242139530737, -0.1983655893005604, -0.23482961069012798, 0.09522383942723621, -0.2787888660420512, -0.17550748826118273, 0.13922713810664622, -0.06474734836279653... |
710.2583 | Martingales, the Efficient Market Hypothesis, and Spurious Stylized
Facts | The condition for stationary increments, not scaling, detemines long time
pair autocorrelations. An incorrect assumption of stationary increments
generates spurious stylized facts, fat tails and a Hurst exponent H_s=1/2, when
the increments are nonstationary, as they are in FX markets. The
nonstationarity arises from... | q-fin.ST physics.data-an physics.soc-ph | the condition for stationary increments not scaling detemines long time pair autocorrelations an incorrect assumption of stationary increments generates spurious stylized facts fat tails and a hurst exponent h_s12 when the increments are nonstationary as they are in fx markets the nonstationarity arises from systematic... | [['the', 'condition', 'for', 'stationary', 'increments', 'not', 'scaling', 'detemines', 'long', 'time', 'pair', 'autocorrelations', 'an', 'incorrect', 'assumption', 'of', 'stationary', 'increments', 'generates', 'spurious', 'stylized', 'facts', 'fat', 'tails', 'and', 'a', 'hurst', 'exponent', 'h_s12', 'when', 'the', 'i... | [-0.1106398261456368, 0.1343697031665993, -0.16153236632800602, 0.1653664326120297, -0.09916547867920347, -0.14324180391008798, 0.02908277582287024, 0.390389548641538, -0.30923363181487845, -0.19027533028792923, 0.13966621774357454, -0.30883012728151904, -0.15246059858600872, 0.20761607771448662, -0.11568670505065622, ... |
710.2584 | Single Pion production from Nuclei | We have studied charged current one pion production induced by
$\nu_\mu(\bar\nu_\mu)$ from some nuclei. The calculations have been done for
the incoherent pion production processes from these nuclear targets in the
$\Delta$ dominance model and take into account the effect of Pauli blocking,
Fermi motion and renormali... | nucl-th | we have studied charged current one pion production induced by nu_mubarnu_mu from some nuclei the calculations have been done for the incoherent pion production processes from these nuclear targets in the delta dominance model and take into account the effect of pauli blocking fermi motion and renormalization of delta ... | [['we', 'have', 'studied', 'charged', 'current', 'one', 'pion', 'production', 'induced', 'by', 'nu_mubarnu_mu', 'from', 'some', 'nuclei', 'the', 'calculations', 'have', 'been', 'done', 'for', 'the', 'incoherent', 'pion', 'production', 'processes', 'from', 'these', 'nuclear', 'targets', 'in', 'the', 'delta', 'dominance'... | [-0.023541743210101926, 0.2222178433514615, -0.12165306328097358, 0.09406954596870311, 0.010508126150447838, -0.08288121637473307, 0.04026240124228862, 0.3437648785881477, -0.18151497857479176, -0.2831126649190884, 0.00040022214289090716, -0.37976043333649856, -0.010815600265223201, 0.1696191919773891, 0.08716414437288... |
710.2585 | Conformal Dirichlet-Neumann Maps and Poincar\'e-Einstein Manifolds | A conformal description of Poincare-Einstein manifolds is developed: these
structures are seen to be a special case of a natural weakening of the Einstein
condition termed an almost Einstein structure. This is used for two purposes:
to shed light on the relationship between the scattering construction of
Graham-Zwors... | math.DG math-ph math.MP | a conformal description of poincareeinstein manifolds is developed these structures are seen to be a special case of a natural weakening of the einstein condition termed an almost einstein structure this is used for two purposes to shed light on the relationship between the scattering construction of grahamzworski and ... | [['a', 'conformal', 'description', 'of', 'poincareeinstein', 'manifolds', 'is', 'developed', 'these', 'structures', 'are', 'seen', 'to', 'be', 'a', 'special', 'case', 'of', 'a', 'natural', 'weakening', 'of', 'the', 'einstein', 'condition', 'termed', 'an', 'almost', 'einstein', 'structure', 'this', 'is', 'used', 'for', ... | [-0.1448271083517944, 0.07351743140236366, -0.08946154452860355, 0.10129937428298522, -0.16157941798016123, -0.14219942761661664, -0.08252862661005292, 0.32347023407992437, -0.2488491799593074, -0.23431425033877157, 0.11244146300046003, -0.25774128525198936, -0.19984151059378907, 0.17005615507903166, -0.067131267630890... |
710.2586 | Mode entanglement of an electron in one-dimensional determined and
random potentials | By using the measure of concurrence, mode entanglement of an electron moving
in four kinds of one-dimensional determined and random potentials is studied
numerically. The extended and local- ized states can be distinguished by mode
entanglement. There are sharp transitions in concurrence at mobility edges. It
provide... | quant-ph | by using the measure of concurrence mode entanglement of an electron moving in four kinds of onedimensional determined and random potentials is studied numerically the extended and local ized states can be distinguished by mode entanglement there are sharp transitions in concurrence at mobility edges it provides that t... | [['by', 'using', 'the', 'measure', 'of', 'concurrence', 'mode', 'entanglement', 'of', 'an', 'electron', 'moving', 'in', 'four', 'kinds', 'of', 'onedimensional', 'determined', 'and', 'random', 'potentials', 'is', 'studied', 'numerically', 'the', 'extended', 'and', 'local', 'ized', 'states', 'can', 'be', 'distinguished',... | [-0.1524746291222982, 0.2607794462647386, -0.08936643250441799, 0.046927645005052906, 0.06674517169594765, -0.2273351308424026, 0.04781848606799031, 0.39221140344937644, -0.23203450484822194, -0.2366794217688342, 0.05186872346481929, -0.30079636865605913, -0.1050092247625192, 0.16966434557301302, 0.008352010929957032, ... |
710.2587 | Origin of the anomalous magnetic circular dichroism spectral shape in
ferromagnetic (Ga,Mn)As: Impurity bands inside the band gap | The electronic structure of a prototype dilute magnetic semiconductor (DMS),
Ga1-xMnxAs, is studied by magnetic circular dichroism (MCD) spectroscopy. We
prove that the optical transitions originated from impurity bands cause the
strong positive MCD background. The MCD signal due to the E0 transition from
the valence... | cond-mat.mtrl-sci | the electronic structure of a prototype dilute magnetic semiconductor dms ga1xmnxas is studied by magnetic circular dichroism mcd spectroscopy we prove that the optical transitions originated from impurity bands cause the strong positive mcd background the mcd signal due to the e0 transition from the valence band to th... | [['the', 'electronic', 'structure', 'of', 'a', 'prototype', 'dilute', 'magnetic', 'semiconductor', 'dms', 'ga1xmnxas', 'is', 'studied', 'by', 'magnetic', 'circular', 'dichroism', 'mcd', 'spectroscopy', 'we', 'prove', 'that', 'the', 'optical', 'transitions', 'originated', 'from', 'impurity', 'bands', 'cause', 'the', 'st... | [-0.1417574536036512, 0.15850739525584034, 0.0059859201310889214, 0.10396334122998094, -0.04600362270256749, -0.16236429274872397, 0.08245247239341037, 0.43326282471117344, -0.29669770111113486, -0.2952963035080977, -0.013182293581352993, -0.3784453652874388, -0.13775399997077806, 0.09414015618162323, 0.092256431223241... |
710.2588 | Phase space constraints and statistical jet studies in heavy-ion
collisions | The effect of the correlation induced by global momentum conservation on the
two-particle distribution in nucleus-nucleus collisions is discussed, with a
focus on the generic case of collisions with a non-vanishing impact parameter.
| nucl-th | the effect of the correlation induced by global momentum conservation on the twoparticle distribution in nucleusnucleus collisions is discussed with a focus on the generic case of collisions with a nonvanishing impact parameter | [['the', 'effect', 'of', 'the', 'correlation', 'induced', 'by', 'global', 'momentum', 'conservation', 'on', 'the', 'twoparticle', 'distribution', 'in', 'nucleusnucleus', 'collisions', 'is', 'discussed', 'with', 'a', 'focus', 'on', 'the', 'generic', 'case', 'of', 'collisions', 'with', 'a', 'nonvanishing', 'impact', 'par... | [-0.1828923374978882, 0.19302143337148608, -0.14627670654744812, 0.08779020914031814, 0.013873248050610224, -0.033820841715417126, -0.09505240277697642, 0.26650451668397046, -0.1810948665846478, -0.2441621252871824, -0.016621874380772086, -0.3266825426765012, -0.03319581225514412, 0.11849777592402516, 0.067228720198865... |
710.2589 | 1-loop Corrections to the \rho Parameter in the Left-Right Twin Higgs
Model | We implement a one-loop analysis of the $\rho$ parameter in the Left Right
Twin Higgs model, including the logarithmically enhanced contributions from
both fermion and scalar loops. Numerical results show that the one-loop
contributions are dominant over the tree level corrections in most regions of
parameter space. ... | hep-ph | we implement a oneloop analysis of the rho parameter in the left right twin higgs model including the logarithmically enhanced contributions from both fermion and scalar loops numerical results show that the oneloop contributions are dominant over the tree level corrections in most regions of parameter space the experi... | [['we', 'implement', 'a', 'oneloop', 'analysis', 'of', 'the', 'rho', 'parameter', 'in', 'the', 'left', 'right', 'twin', 'higgs', 'model', 'including', 'the', 'logarithmically', 'enhanced', 'contributions', 'from', 'both', 'fermion', 'and', 'scalar', 'loops', 'numerical', 'results', 'show', 'that', 'the', 'oneloop', 'co... | [-0.10518363550786049, 0.24700407328845192, -0.026689388248468598, 0.13885568488909994, -0.07601909339427948, -0.13115812492336557, 0.031641922801011996, 0.31910753864995256, -0.20200328289666364, -0.2978200379118163, 0.05837189985228883, -0.3075728559846519, -0.03222179675464749, 0.22290631393922034, 0.083598669908780... |
710.259 | Geometries with Killing Spinors and Supersymmetric AdS Solutions | The seven and nine dimensional geometries associated with certain classes of
supersymmetric $AdS_3$ and $AdS_2$ solutions of type IIB and D=11 supergravity,
respectively, have many similarities with Sasaki-Einstein geometry. We further
elucidate their properties and also generalise them to higher odd dimensions by
in... | hep-th math-ph math.DG math.MP | the seven and nine dimensional geometries associated with certain classes of supersymmetric ads_3 and ads_2 solutions of type iib and d11 supergravity respectively have many similarities with sasakieinstein geometry we further elucidate their properties and also generalise them to higher odd dimensions by introducing a... | [['the', 'seven', 'and', 'nine', 'dimensional', 'geometries', 'associated', 'with', 'certain', 'classes', 'of', 'supersymmetric', 'ads_3', 'and', 'ads_2', 'solutions', 'of', 'type', 'iib', 'and', 'd11', 'supergravity', 'respectively', 'have', 'many', 'similarities', 'with', 'sasakieinstein', 'geometry', 'we', 'further'... | [-0.15657606083694978, 0.1325320146964691, 0.0236799747266985, 0.09846693039987342, -0.08188155466725336, -0.20924815680197578, -0.053920852339080144, 0.35422084894995637, -0.12594238072567693, -0.27004160938110755, 0.11939083868270271, -0.25798790336830923, -0.20551912421327587, 0.16379714151514127, -0.053736458552327... |
710.2591 | Von Neumann entropy and localization-delocalization transition of
electron states in quantum small-world networks | The von Neumann entropy for an electron in periodic, disorder and
quasiperiodic quantum small-world networks(QSWNs) are studied numerically. For
the disorder QSWNs, the derivative of the spectrum averaged von Neumann entropy
is maximal at a certain density of shortcut links p*, which can be as a
signature of the loca... | quant-ph | the von neumann entropy for an electron in periodic disorder and quasiperiodic quantum smallworld networksqswns are studied numerically for the disorder qswns the derivative of the spectrum averaged von neumann entropy is maximal at a certain density of shortcut links p which can be as a signature of the localization d... | [['the', 'von', 'neumann', 'entropy', 'for', 'an', 'electron', 'in', 'periodic', 'disorder', 'and', 'quasiperiodic', 'quantum', 'smallworld', 'networksqswns', 'are', 'studied', 'numerically', 'for', 'the', 'disorder', 'qswns', 'the', 'derivative', 'of', 'the', 'spectrum', 'averaged', 'von', 'neumann', 'entropy', 'is', ... | [-0.16404864993676835, 0.2180847159334899, -0.07286357801914324, 0.08867547506644555, 0.06210566366858342, -0.1763488158821037, 0.019635884303544814, 0.3405233548871954, -0.23752818204572096, -0.2091661730744675, 0.06752796512891483, -0.337354833698448, -0.12498871154864044, 0.19490130915872605, -0.007773593214212679, ... |
710.2592 | von Neumann entropy and localization properties of two interacting
particles in one-dimensional nonuniform systems | With the help of von Neumann entropy, we study numerically the localization
properties of two interacting particles (TIP) with on-site interactions in
one-dimensional disordered, quasiperiodic, and slowly varying potential
systems, respectively. We find that for TIP in disordered and slowly varying
potential systems,... | quant-ph | with the help of von neumann entropy we study numerically the localization properties of two interacting particles tip with onsite interactions in onedimensional disordered quasiperiodic and slowly varying potential systems respectively we find that for tip in disordered and slowly varying potential systems the spectru... | [['with', 'the', 'help', 'of', 'von', 'neumann', 'entropy', 'we', 'study', 'numerically', 'the', 'localization', 'properties', 'of', 'two', 'interacting', 'particles', 'tip', 'with', 'onsite', 'interactions', 'in', 'onedimensional', 'disordered', 'quasiperiodic', 'and', 'slowly', 'varying', 'potential', 'systems', 'res... | [-0.13091798471286892, 0.1882372500155515, -0.04645128361164377, 0.015791266853025614, 0.03139944552229001, -0.19927158487172655, 0.04222274258231314, 0.33699001386367644, -0.24575320228647726, -0.24543127280731614, 0.014120672238417543, -0.37069739897090653, -0.11376594487900057, 0.1868757199970647, -0.024119242209081... |
710.2593 | The Self-dual String Soliton in AdS_4\times S^7 spacetime | We construct self-dual string soliton solutions in $AdS_4\times
S^7$ spacetime, starting from the covariant equations of motion of M5-brane.
We study the properties of the solutions and find that their action are
linearized, indicating the BPS nature of the solutions, and they have the same
electric and magnetic ch... | hep-th | we construct selfdual string soliton solutions in ads_4times s7 spacetime starting from the covariant equations of motion of m5brane we study the properties of the solutions and find that their action are linearized indicating the bps nature of the solutions and they have the same electric and magnetic charge the strai... | [['we', 'construct', 'selfdual', 'string', 'soliton', 'solutions', 'in', 'ads_4times', 's7', 'spacetime', 'starting', 'from', 'the', 'covariant', 'equations', 'of', 'motion', 'of', 'm5brane', 'we', 'study', 'the', 'properties', 'of', 'the', 'solutions', 'and', 'find', 'that', 'their', 'action', 'are', 'linearized', 'in... | [-0.1887443703200136, 0.09384500153274053, -0.09636780466174795, 0.056520457539175235, -0.09027001059481075, -0.15195292224220577, -0.04223426456917964, 0.3255064870629992, -0.19296006938619983, -0.2265760357037098, 0.10448487910796844, -0.3206940305020128, -0.1389053132739805, 0.09918135185504244, -0.05032435284949661... |
710.2594 | Rotation of easy axis in training effect and recovery of exchange bias
in ferromagnet/antiferromagnet bilayers | For ferromagnet/antiferromagnet bilayers, rotation of the easy axis has been
\textit{for the first time} observed during measurements of training effect and
the recovery of exchange bias using FeNi/FeMn system. These salient phenomena
strongly suggest irreversible motion of antiferromagnet spins during subsequent
mea... | cond-mat.mtrl-sci physics.soc-ph physics.space-ph | for ferromagnetantiferromagnet bilayers rotation of the easy axis has been textitfor the first time observed during measurements of training effect and the recovery of exchange bias using fenifemn system these salient phenomena strongly suggest irreversible motion of antiferromagnet spins during subsequent measurements... | [['for', 'ferromagnetantiferromagnet', 'bilayers', 'rotation', 'of', 'the', 'easy', 'axis', 'has', 'been', 'textitfor', 'the', 'first', 'time', 'observed', 'during', 'measurements', 'of', 'training', 'effect', 'and', 'the', 'recovery', 'of', 'exchange', 'bias', 'using', 'fenifemn', 'system', 'these', 'salient', 'phenom... | [-0.18358461977913976, 0.1682516709449427, -0.06270648644524901, 0.028957115344169056, -0.09338323195012943, -0.11665654904893874, 0.04549432527410852, 0.4182868520181407, -0.2793077982359511, -0.3414377602200736, 0.10897230041925521, -0.24757751948474085, -0.10715974876931046, 0.19303619417854967, 0.019299339694792732... |
710.2595 | The process of coevolutionary competitive exclusion: speciation,
multifractality and power-laws in correlation | Competitive exclusion, a key principle of ecology, can be generalized to
understand many other complex systems. Individuals under surviving pressure
tend to be different from others, and correlations among them change
correspondingly to the updating of their states. We show with numerical
simulation that these aptitu... | physics.data-an physics.soc-ph | competitive exclusion a key principle of ecology can be generalized to understand many other complex systems individuals under surviving pressure tend to be different from others and correlations among them change correspondingly to the updating of their states we show with numerical simulation that these aptitudes can... | [['competitive', 'exclusion', 'a', 'key', 'principle', 'of', 'ecology', 'can', 'be', 'generalized', 'to', 'understand', 'many', 'other', 'complex', 'systems', 'individuals', 'under', 'surviving', 'pressure', 'tend', 'to', 'be', 'different', 'from', 'others', 'and', 'correlations', 'among', 'them', 'change', 'correspond... | [-0.11096488491953264, 0.1739402321852847, -0.10451104498847767, 0.10459584997451438, -0.0675871157565982, -0.17253953780271802, 0.09921171950150488, 0.40646651991711996, -0.3156592422553028, -0.3243522902743684, 0.0381153628027446, -0.279957509573756, -0.2030746188226018, 0.10493763590973147, -0.022365874369387275, 0.... |
710.2596 | Sub-Poissonian laser emission from a single-electron permanently
interacting with a single-mode cavity | Quiet (or sub-Poissonian) oscillators generate a number of dissipation events
whose variance is less than the mean. It was shown in 1984 by Golubev and
Sokolov that lasers driven by regular pumps are quiet in that sense. The
purpose of this paper is to show that, as long as the laser-detector system is
strictly stati... | quant-ph | quiet or subpoissonian oscillators generate a number of dissipation events whose variance is less than the mean it was shown in 1984 by golubev and sokolov that lasers driven by regular pumps are quiet in that sense the purpose of this paper is to show that as long as the laserdetector system is strictly stationary qua... | [['quiet', 'or', 'subpoissonian', 'oscillators', 'generate', 'a', 'number', 'of', 'dissipation', 'events', 'whose', 'variance', 'is', 'less', 'than', 'the', 'mean', 'it', 'was', 'shown', 'in', '1984', 'by', 'golubev', 'and', 'sokolov', 'that', 'lasers', 'driven', 'by', 'regular', 'pumps', 'are', 'quiet', 'in', 'that', ... | [-0.11192880321981474, 0.2012756279333919, -0.058518181478946794, 0.053320270147313976, -0.031431881767906705, -0.17960246358713022, 0.03402358297255448, 0.3894539419434914, -0.2087880537946563, -0.3010998063651072, 0.07328232395427846, -0.29029034322672553, -0.1393705843583535, 0.22596422384958714, -0.0910021475560608... |
710.2597 | Wheeler's delayed-choice thought experiment: Experimental realization
and theoretical analysis | Wheeler has strikingly illustrated the wave-particle duality by the
delayed-choice thought experiment, in which the configuration of a 2-path
interferometer is chosen after a single-photon light-pulsed has entered it. We
present a quantitative theoretical analysis of an experimental realization of
Wheeler's proposal.... | quant-ph | wheeler has strikingly illustrated the waveparticle duality by the delayedchoice thought experiment in which the configuration of a 2path interferometer is chosen after a singlephoton lightpulsed has entered it we present a quantitative theoretical analysis of an experimental realization of wheelers proposal | [['wheeler', 'has', 'strikingly', 'illustrated', 'the', 'waveparticle', 'duality', 'by', 'the', 'delayedchoice', 'thought', 'experiment', 'in', 'which', 'the', 'configuration', 'of', 'a', '2path', 'interferometer', 'is', 'chosen', 'after', 'a', 'singlephoton', 'lightpulsed', 'has', 'entered', 'it', 'we', 'present', 'a'... | [-0.1398081104271114, 0.12465934370532235, -0.24279327268098913, 0.04336180734709359, -0.044225990202948, -0.19917984221630344, 0.04249399075875195, 0.34436388949795466, -0.13776587714191255, -0.28850470510561294, 0.03234214456354427, -0.22559637022091122, -0.16717275291704004, 0.2357338945858362, -0.08355106388377707,... |
710.2598 | BRST quantization of the pure spinor superstring | We present a derivation of the scattering amplitude prescription for the pure
spinor superstring from first principles, both in the minimal and non-minimal
formulations, and show that they are equivalent. This is achieved by first
coupling the worldsheet action to topological gravity and then proceeding to
BRST quant... | hep-th | we present a derivation of the scattering amplitude prescription for the pure spinor superstring from first principles both in the minimal and nonminimal formulations and show that they are equivalent this is achieved by first coupling the worldsheet action to topological gravity and then proceeding to brst quantize th... | [['we', 'present', 'a', 'derivation', 'of', 'the', 'scattering', 'amplitude', 'prescription', 'for', 'the', 'pure', 'spinor', 'superstring', 'from', 'first', 'principles', 'both', 'in', 'the', 'minimal', 'and', 'nonminimal', 'formulations', 'and', 'show', 'that', 'they', 'are', 'equivalent', 'this', 'is', 'achieved', '... | [-0.14689990589876883, 0.16950084772442692, -0.08913451446830456, 0.06444333597838867, -0.0958449655525579, -0.10292436982553195, 0.009510030015572456, 0.3463906629597126, -0.238935550528587, -0.26601050157854655, 0.0749407163048404, -0.23411296073604246, -0.17353645415077434, 0.12768157618923176, -0.04413901392274119,... |
710.2599 | Heavy-flavor correlation measurements via electron azimuthal
correlations with open charm mesons | We report first STAR measurement on two heavy-flavor particle correlations in
p+p collisions at RHIC. Heavy-flavor (charm and bottom) events are identified
and separated on a statistical basis by the azimuthal correlation of their
decay electrons and open charm mesons, which yield important information about
the unde... | nucl-ex | we report first star measurement on two heavyflavor particle correlations in pp collisions at rhic heavyflavor charm and bottom events are identified and separated on a statistical basis by the azimuthal correlation of their decay electrons and open charm mesons which yield important information about the underlying pr... | [['we', 'report', 'first', 'star', 'measurement', 'on', 'two', 'heavyflavor', 'particle', 'correlations', 'in', 'pp', 'collisions', 'at', 'rhic', 'heavyflavor', 'charm', 'and', 'bottom', 'events', 'are', 'identified', 'and', 'separated', 'on', 'a', 'statistical', 'basis', 'by', 'the', 'azimuthal', 'correlation', 'of', ... | [-0.06752084856129532, 0.2558084348560248, -0.18364658215291146, 0.20061455060641994, -0.020572120294390806, -0.12105764816650777, -0.03334356880480044, 0.3817873529759823, -0.2370371843407889, -0.2671402722090772, -0.07800628670301397, -0.40936985606490406, 0.0885600540967821, 0.12259807638050899, 0.12481346259852058,... |
710.26 | A Possibility of Search for New Physics at LHCb | It is interesting to search for new physics beyond the standard model at
LHCb. We suggest that weak decays of doubly charmed baryon such as
$\Xi_{cc}(3520)^+, \Xi_{cc}^{++}$ to charmless final states would be a possible
signal for new physics. In this work, we consider two models, i.e. the
unparticle and $Z'$ as exam... | hep-ph hep-ex | it is interesting to search for new physics beyond the standard model at lhcb we suggest that weak decays of doubly charmed baryon such as xi_cc3520 xi_cc to charmless final states would be a possible signal for new physics in this work we consider two models ie the unparticle and z as examples to study such possibilit... | [['it', 'is', 'interesting', 'to', 'search', 'for', 'new', 'physics', 'beyond', 'the', 'standard', 'model', 'at', 'lhcb', 'we', 'suggest', 'that', 'weak', 'decays', 'of', 'doubly', 'charmed', 'baryon', 'such', 'as', 'xi_cc3520', 'xi_cc', 'to', 'charmless', 'final', 'states', 'would', 'be', 'a', 'possible', 'signal', 'f... | [-0.0315652974758897, 0.21667270743982645, -0.07373010158791381, 0.15668401519878436, -0.09965103045421636, -0.20384201339556504, 0.029253022710721686, 0.33348849139539366, -0.24729760685714625, -0.2885184053063266, 0.05365617556292248, -0.3299924529599563, -0.0936474806680423, 0.1961211870459966, 0.05717611401756215, ... |
710.2601 | New Physics Effects in Long Baseline Experiments | We discuss the implications of new physics, which modifies the matter effect
in neutrino oscillations, to long baseline experiments, particularly the MINOS
experiment. An analytic formula in the presence of such a new physics
interaction is derived for $P(\nu_\mu\to\nu_e)$, which is exact in the limit
$\Delta m^2_{21... | hep-ph | we discuss the implications of new physics which modifies the matter effect in neutrino oscillations to long baseline experiments particularly the minos experiment an analytic formula in the presence of such a new physics interaction is derived for pnu_mutonu_e which is exact in the limit delta m2_21to0 | [['we', 'discuss', 'the', 'implications', 'of', 'new', 'physics', 'which', 'modifies', 'the', 'matter', 'effect', 'in', 'neutrino', 'oscillations', 'to', 'long', 'baseline', 'experiments', 'particularly', 'the', 'minos', 'experiment', 'an', 'analytic', 'formula', 'in', 'the', 'presence', 'of', 'such', 'a', 'new', 'phys... | [-0.12210551647262441, 0.16031508343585302, -0.09101002189434237, 0.17186803998322123, -0.11067287445896201, -0.10208810599934724, 0.02258162647485733, 0.24855589361654387, -0.2521029824184047, -0.3172364555713203, 0.05522732529013107, -0.2759045766770012, -0.1391518481903606, 0.2532387449509568, 0.037487717738582026, ... |
710.2602 | Prospects to Measure the Higgs Boson Mass and Cross Section in ee-->ZH
Using the Recoil Mass Spectrum | The process ee-->ZH allows to measure the Higgs boson in the recoil mass
spectrum against the Z boson without any assumptions on the Higgs boson decay.
We performed a full simulation and reconstruction of ee-->ZH using the MOKKA
and MARLIN packages describing the LDC detector. The Z is reconstructed from
its decays i... | hep-ex | the process eezh allows to measure the higgs boson in the recoil mass spectrum against the z boson without any assumptions on the higgs boson decay we performed a full simulation and reconstruction of eezh using the mokka and marlin packages describing the ldc detector the z is reconstructed from its decays into electr... | [['the', 'process', 'eezh', 'allows', 'to', 'measure', 'the', 'higgs', 'boson', 'in', 'the', 'recoil', 'mass', 'spectrum', 'against', 'the', 'z', 'boson', 'without', 'any', 'assumptions', 'on', 'the', 'higgs', 'boson', 'decay', 'we', 'performed', 'a', 'full', 'simulation', 'and', 'reconstruction', 'of', 'eezh', 'using'... | [-0.023432469328067133, 0.22155792487215617, -0.06032240790390999, 0.14809878020882097, -0.03347710311342725, -0.1338863596510218, 0.03814619118751654, 0.354719371991042, -0.20686297284971392, -0.3311133778330927, -0.010634430471513117, -0.3235157635183209, 0.1384122785827031, 0.19399921408048426, 0.09653625321783582, ... |
710.2603 | Dynamics of coreless vortices and rotation-induced dissipation peak in
superfluid films on rotating porous substrates | We analyze dynamics of 3D coreless vortices in superfluid films covering
porous substrates. The 3D vortex dynamics is derived from the 2D dynamics of
the film. The motion of a 3D vortex is a sequence of jumps between neighboring
substrate cells, which can be described, nevertheless, in terms of
quasi-continuous motio... | cond-mat.soft cond-mat.mtrl-sci | we analyze dynamics of 3d coreless vortices in superfluid films covering porous substrates the 3d vortex dynamics is derived from the 2d dynamics of the film the motion of a 3d vortex is a sequence of jumps between neighboring substrate cells which can be described nevertheless in terms of quasicontinuous motion with a... | [['we', 'analyze', 'dynamics', 'of', '3d', 'coreless', 'vortices', 'in', 'superfluid', 'films', 'covering', 'porous', 'substrates', 'the', '3d', 'vortex', 'dynamics', 'is', 'derived', 'from', 'the', '2d', 'dynamics', 'of', 'the', 'film', 'the', 'motion', 'of', 'a', '3d', 'vortex', 'is', 'a', 'sequence', 'of', 'jumps', ... | [-0.12038198167442524, 0.17867844997848453, -0.0843967694256987, -0.025413009581672606, -0.006117651372083596, -0.0809125912438358, 0.006903805017682622, 0.3952620937762892, -0.27618075830533223, -0.2299651149269037, 0.04110403651735518, -0.26601457730436523, -0.11021777045200853, 0.21798791255833222, -0.02855355132120... |
710.2604 | Efficient Skyline Querying with Variable User Preferences on Nominal
Attributes | Current skyline evaluation techniques assume a fixed ordering on the
attributes. However, dynamic preferences on nominal attributes are more
realistic in known applications. In order to generate online response for any
such preference issued by a user, we propose two methods of different
characteristics. The first on... | cs.DB | current skyline evaluation techniques assume a fixed ordering on the attributes however dynamic preferences on nominal attributes are more realistic in known applications in order to generate online response for any such preference issued by a user we propose two methods of different characteristics the first one is a ... | [['current', 'skyline', 'evaluation', 'techniques', 'assume', 'a', 'fixed', 'ordering', 'on', 'the', 'attributes', 'however', 'dynamic', 'preferences', 'on', 'nominal', 'attributes', 'are', 'more', 'realistic', 'in', 'known', 'applications', 'in', 'order', 'to', 'generate', 'online', 'response', 'for', 'any', 'such', '... | [-0.09500862155608567, -0.004425940787145269, -0.06608582971883671, 0.07407057566368687, -0.12276174623319613, -0.11441863621585072, 0.07947085342769111, 0.4552141655901713, -0.24616007675150675, -0.3276848891217794, 0.09451132437679917, -0.2962000081847821, -0.18812862134405545, 0.20939065244581018, -0.056170870280558... |
710.2605 | Gravitational waves from the R^-1 high order theory of gravity | This paper is a review of a previous research on gravitational waves from the
R^-1 high order theory of gravity. It is shown that a massive scalar mode of
gravitational waves from the R^-1 theory generates a longitudinal force in
addition of the transverse one which is proper of the massless gravitational
waves and t... | astro-ph | this paper is a review of a previous research on gravitational waves from the r1 high order theory of gravity it is shown that a massive scalar mode of gravitational waves from the r1 theory generates a longitudinal force in addition of the transverse one which is proper of the massless gravitational waves and the resp... | [['this', 'paper', 'is', 'a', 'review', 'of', 'a', 'previous', 'research', 'on', 'gravitational', 'waves', 'from', 'the', 'r1', 'high', 'order', 'theory', 'of', 'gravity', 'it', 'is', 'shown', 'that', 'a', 'massive', 'scalar', 'mode', 'of', 'gravitational', 'waves', 'from', 'the', 'r1', 'theory', 'generates', 'a', 'lon... | [-0.1665862076477908, 0.130459896983299, -0.15341435502862147, 0.03489489486620445, -0.09569140123801494, -0.06213312769530836, -0.012938725717211946, 0.29322091452435617, -0.2544876391563667, -0.27091586323232825, 0.04815157283088961, -0.27389629918295855, -0.1936431656892779, 0.2061635275764408, -0.020306048656326778... |
710.2606 | The representation dimension of quantum complete intersections | We study the representation dimension of the class of algebras known as
quantum complete intersections. For such an algebra, we show that the
representation dimension is at most twice its codimension. Moreover, we show
that the representation dimension of a "homogeneous" quantum complete
intersection is strictly larg... | math.QA math.RT | we study the representation dimension of the class of algebras known as quantum complete intersections for such an algebra we show that the representation dimension is at most twice its codimension moreover we show that the representation dimension of a homogeneous quantum complete intersection is strictly larger than ... | [['we', 'study', 'the', 'representation', 'dimension', 'of', 'the', 'class', 'of', 'algebras', 'known', 'as', 'quantum', 'complete', 'intersections', 'for', 'such', 'an', 'algebra', 'we', 'show', 'that', 'the', 'representation', 'dimension', 'is', 'at', 'most', 'twice', 'its', 'codimension', 'moreover', 'we', 'show', '... | [-0.13892500322312118, 0.08395944533200236, -0.04482363567687571, 0.0586899401852861, -0.05456761912442744, -0.10800744221545756, -0.08293714710511267, 0.3229631716758013, -0.2831896490161307, -0.1411703890375793, 0.1189840509975329, -0.2880099867656827, -0.1911803836748004, 0.2065465465374291, -0.08797333602793515, -0... |
710.2607 | Localization of overlap modes and topological charge, vortices and
monopoles in SU(3) LGT | We present selected recent results of the QCDSF collaboration on the
localization and dimensionality of low overlap eigenmodes and of the
topological density in the quenched SU(3) vacuum. We discuss the correlations
between the topological structure revealed by overlap fermions without
filtering and the confining mon... | hep-lat | we present selected recent results of the qcdsf collaboration on the localization and dimensionality of low overlap eigenmodes and of the topological density in the quenched su3 vacuum we discuss the correlations between the topological structure revealed by overlap fermions without filtering and the confining monopole... | [['we', 'present', 'selected', 'recent', 'results', 'of', 'the', 'qcdsf', 'collaboration', 'on', 'the', 'localization', 'and', 'dimensionality', 'of', 'low', 'overlap', 'eigenmodes', 'and', 'of', 'the', 'topological', 'density', 'in', 'the', 'quenched', 'su3', 'vacuum', 'we', 'discuss', 'the', 'correlations', 'between'... | [-0.16785457070052093, 0.2089227056879151, -0.06372093568955149, 0.08870427420229784, -0.01491034691571258, -0.034528470964037945, 0.08594828655727074, 0.39332206354343463, -0.17721429541208117, -0.3016143323454474, 0.04687291423241342, -0.2846685172491042, -0.13641004152928612, 0.046345373981499245, 0.0574699967234794... |
710.2608 | On the conditional logistic estimator for repeated binary outcomes in
two-arm experimental studies with non-compliance | The behavior of the conditional logistic estimator is analyzed under a causal
model for two-arm experimental studies with possible non-compliance in which
the effect of the treatment is measured by a binary response variable. We show
that, when non-compliance may only be observed in the treatment arm, the effect
(mea... | math.ST stat.TH | the behavior of the conditional logistic estimator is analyzed under a causal model for twoarm experimental studies with possible noncompliance in which the effect of the treatment is measured by a binary response variable we show that when noncompliance may only be observed in the treatment arm the effect measured on ... | [['the', 'behavior', 'of', 'the', 'conditional', 'logistic', 'estimator', 'is', 'analyzed', 'under', 'a', 'causal', 'model', 'for', 'twoarm', 'experimental', 'studies', 'with', 'possible', 'noncompliance', 'in', 'which', 'the', 'effect', 'of', 'the', 'treatment', 'is', 'measured', 'by', 'a', 'binary', 'response', 'vari... | [-0.059765367986830444, 0.04084099394485269, -0.119288084317783, 0.08847779304120003, -0.07260131598572786, -0.12481056719062555, 0.07786489880251649, 0.3619516164750645, -0.21885219783963342, -0.2968402098472181, 0.13916003841992566, -0.23940493004575777, -0.1734544393851569, 0.23168847240924248, -0.10169414558791016,... |
710.2609 | Bijective 1-cocycles and classification of 3-dimensional Left-symmetric
Algebras | Left-symmetric algebras have close relations with many important fields in
mathematics and mathematical physics. Their classification is very complicated
due to the nonassociativity. In this paper, we re-study the correspondence
between left-symmetric algebras and the bijective 1-cocycles. Then a procedure
is provide... | math.QA math.RA | leftsymmetric algebras have close relations with many important fields in mathematics and mathematical physics their classification is very complicated due to the nonassociativity in this paper we restudy the correspondence between leftsymmetric algebras and the bijective 1cocycles then a procedure is provided to class... | [['leftsymmetric', 'algebras', 'have', 'close', 'relations', 'with', 'many', 'important', 'fields', 'in', 'mathematics', 'and', 'mathematical', 'physics', 'their', 'classification', 'is', 'very', 'complicated', 'due', 'to', 'the', 'nonassociativity', 'in', 'this', 'paper', 'we', 'restudy', 'the', 'correspondence', 'bet... | [-0.14404247931176514, 0.023089793181112105, -0.05339836800527392, 0.17858900355041082, -0.15994688397216977, -0.15800403125555904, -0.06552548072773567, 0.40694285185556067, -0.3828561469968973, -0.25729847046772414, 0.10872238599448324, -0.202671101083979, -0.25371658706078026, 0.20089337335560808, -0.215881257670733... |
710.261 | Solar System motions and the cosmological constant: a new approach | We use the corrections to the Newton-Einstein secular precessions of the
longitudes of perihelia of some planets (Mercury, Earth, Mars, Jupiter, Saturn)
of the Solar System, phenomenologically estimated as solve-for parameters by
the Russian astronomer E.V. Pitjeva in a global fit of almost one century of
data with t... | gr-qc astro-ph hep-ph physics.space-ph | we use the corrections to the newtoneinstein secular precessions of the longitudes of perihelia of some planets mercury earth mars jupiter saturn of the solar system phenomenologically estimated as solvefor parameters by the russian astronomer ev pitjeva in a global fit of almost one century of data with the epm2004 ep... | [['we', 'use', 'the', 'corrections', 'to', 'the', 'newtoneinstein', 'secular', 'precessions', 'of', 'the', 'longitudes', 'of', 'perihelia', 'of', 'some', 'planets', 'mercury', 'earth', 'mars', 'jupiter', 'saturn', 'of', 'the', 'solar', 'system', 'phenomenologically', 'estimated', 'as', 'solvefor', 'parameters', 'by', '... | [-0.10864660840460975, 0.14187100458009666, -0.049545090850990486, 0.10859613263164647, -0.0974008483337421, -0.08453542908982319, 0.03856194796104569, 0.2887206591994447, -0.18382801734340176, -0.3629948300567419, 0.09574476508572058, -0.2879129221900275, -0.06734056465268391, 0.23624684049076783, -0.07838109034049671... |
710.2611 | Geometric Analogue of Holographic Reduced Representation | Holographic reduced representations (HRR) are based on superpositions of
convolution-bound $n$-tuples, but the $n$-tuples cannot be regarded as vectors
since the formalism is basis dependent. This is why HRR cannot be associated
with geometric structures. Replacing convolutions by geometric products one
arrives at re... | cs.AI quant-ph | holographic reduced representations hrr are based on superpositions of convolutionbound ntuples but the ntuples cannot be regarded as vectors since the formalism is basis dependent this is why hrr cannot be associated with geometric structures replacing convolutions by geometric products one arrives at reduced represen... | [['holographic', 'reduced', 'representations', 'hrr', 'are', 'based', 'on', 'superpositions', 'of', 'convolutionbound', 'ntuples', 'but', 'the', 'ntuples', 'can', 'not', 'be', 'regarded', 'as', 'vectors', 'since', 'the', 'formalism', 'is', 'basis', 'dependent', 'this', 'is', 'why', 'hrr', 'can', 'not', 'be', 'associate... | [-0.10221205126609716, 0.1250980555691492, -0.1121261275074542, 0.10690907764755912, -0.11355626839039319, -0.1533389429834588, 0.0032400842356398256, 0.3454309992714604, -0.3188924149874209, -0.2680832823988662, 0.11624771779239762, -0.20775198708681492, -0.16081530026962926, 0.19425387921701395, -0.11252459051711276,... |
710.2612 | Involutions on tori with codimension one fixed point set | The standard P. A. Smith theory of p-group actions on spheres, disks, and
euclidean spaces is extended to the case of p-group actions on tori (i.e.,
products of circles) and coupled with topological surgery theory to give a
complete topological classification, valid in all dimensions, of the locally
linear, orientati... | math.GT | the standard p a smith theory of pgroup actions on spheres disks and euclidean spaces is extended to the case of pgroup actions on tori ie products of circles and coupled with topological surgery theory to give a complete topological classification valid in all dimensions of the locally linear orientation reversing inv... | [['the', 'standard', 'p', 'a', 'smith', 'theory', 'of', 'pgroup', 'actions', 'on', 'spheres', 'disks', 'and', 'euclidean', 'spaces', 'is', 'extended', 'to', 'the', 'case', 'of', 'pgroup', 'actions', 'on', 'tori', 'ie', 'products', 'of', 'circles', 'and', 'coupled', 'with', 'topological', 'surgery', 'theory', 'to', 'giv... | [-0.19165896209048444, 0.12419876150909018, -0.07171460289935597, 0.03750481113951775, -0.06296360962566172, -0.16222895194058778, 0.020633023701699785, 0.3443401505498857, -0.2333085020454448, -0.19615901395922802, 0.10786566364800283, -0.2900755415807982, -0.10769444525425063, 0.19395447989589856, -0.1524386875861950... |
710.2613 | High quality factor gigahertz frequencies in nanomechanical diamond
resonators | We report actuation and detection of gigahertz-range resonance frequencies in
nano-crystalline diamond mechanical resonators. High order transverse vibration
modes are measured in coupled-beam resonators exhibiting frequencies up to
1.441 GHz. The cantilever-array design of the resonators translates the
gigahertz-ran... | cond-mat.mes-hall cond-mat.mtrl-sci | we report actuation and detection of gigahertzrange resonance frequencies in nanocrystalline diamond mechanical resonators high order transverse vibration modes are measured in coupledbeam resonators exhibiting frequencies up to 1441 ghz the cantileverarray design of the resonators translates the gigahertzrange resonan... | [['we', 'report', 'actuation', 'and', 'detection', 'of', 'gigahertzrange', 'resonance', 'frequencies', 'in', 'nanocrystalline', 'diamond', 'mechanical', 'resonators', 'high', 'order', 'transverse', 'vibration', 'modes', 'are', 'measured', 'in', 'coupledbeam', 'resonators', 'exhibiting', 'frequencies', 'up', 'to', '1441... | [-0.16703458888652292, 0.22073998092061006, 0.0611956387856289, -0.12202584120003801, -0.04086153662616485, -0.13505676380897824, 0.05038157674287887, 0.47262501924445754, -0.21592331660029135, -0.3106199562843693, 0.04435380791975675, -0.307731389215118, -0.027032417519704293, 0.22844135763221665, -0.02261123670461146... |
710.2614 | Multivariate integration of functions depending explicitly on the
minimum and the maximum of the variables | By using some basic calculus of multiple integration, we provide an
alternative expression of the integral $$ \int_{]a,b[^n} f(\mathbf{x},\min
x_i,\max x_i) d\mathbf{x}, $$ in which the minimum and the maximum are replaced
with two single variables. We demonstrate the usefulness of that expression in
the computation ... | math.FA math.PR | by using some basic calculus of multiple integration we provide an alternative expression of the integral int_abn fmathbfxmin x_imax x_i dmathbfx in which the minimum and the maximum are replaced with two single variables we demonstrate the usefulness of that expression in the computation of orness and andness average ... | [['by', 'using', 'some', 'basic', 'calculus', 'of', 'multiple', 'integration', 'we', 'provide', 'an', 'alternative', 'expression', 'of', 'the', 'integral', 'int_abn', 'fmathbfxmin', 'x_imax', 'x_i', 'dmathbfx', 'in', 'which', 'the', 'minimum', 'and', 'the', 'maximum', 'are', 'replaced', 'with', 'two', 'single', 'variab... | [-0.12680528189853899, 0.052584001975940604, -0.10159464956128171, 0.04620472754218748, -0.03583235164572086, -0.06942641250123935, 0.07511606165540538, 0.3445441643142008, -0.2525856232802783, -0.3035623444643404, 0.11318291653546371, -0.24113395256655556, -0.18900934050325305, 0.2345795855990478, -0.04124137183742797... |
710.2615 | Fundamental groups of topological stacks with slice property | The main result of the paper is a formula for the fundamental group of the
coarse moduli space of a topological stack. As an application, we find simple
general formulas for the fundamental group of the coarse quotient of a group
action on a topological space in terms of the fixed point data. The formulas
seem, surpr... | math.AT | the main result of the paper is a formula for the fundamental group of the coarse moduli space of a topological stack as an application we find simple general formulas for the fundamental group of the coarse quotient of a group action on a topological space in terms of the fixed point data the formulas seem surprisingl... | [['the', 'main', 'result', 'of', 'the', 'paper', 'is', 'a', 'formula', 'for', 'the', 'fundamental', 'group', 'of', 'the', 'coarse', 'moduli', 'space', 'of', 'a', 'topological', 'stack', 'as', 'an', 'application', 'we', 'find', 'simple', 'general', 'formulas', 'for', 'the', 'fundamental', 'group', 'of', 'the', 'coarse',... | [-0.1261387793219661, 0.0844411157752939, -0.1328752426915381, 0.07059570315950997, -0.09928352929562433, -0.05666859815381978, 0.06916071881686835, 0.30467197896070675, -0.29813494125049406, -0.24708454226692245, 0.12434037633508138, -0.19777374490074914, -0.19275299690612782, 0.24736787900583793, -0.163862417360739, ... |
710.2616 | Classification of complete Finsler manifolds through a second order
differential equation | By using a certain second order differential equation, the notion of adapted
coordinates on Finsler manifolds is defined and some classifications of
complete Finsler manifolds are found. Some examples of Finsler metrics, with
positive constant sectional curvature, not necessarily of Randers type nor
projectively flat... | math.DG math.CT | by using a certain second order differential equation the notion of adapted coordinates on finsler manifolds is defined and some classifications of complete finsler manifolds are found some examples of finsler metrics with positive constant sectional curvature not necessarily of randers type nor projectively flat are f... | [['by', 'using', 'a', 'certain', 'second', 'order', 'differential', 'equation', 'the', 'notion', 'of', 'adapted', 'coordinates', 'on', 'finsler', 'manifolds', 'is', 'defined', 'and', 'some', 'classifications', 'of', 'complete', 'finsler', 'manifolds', 'are', 'found', 'some', 'examples', 'of', 'finsler', 'metrics', 'wit... | [-0.1939517924787872, 0.03297230417868405, -0.017299908340315927, 0.10182573719683921, -0.21194582525640726, -0.2202692962477379, -0.10539548020019676, 0.38907727314808377, -0.22317904443568268, -0.26269195412786567, 0.12973605188590503, -0.2891076709510702, -0.21102742956612597, 0.22457645007296267, -0.209463207897814... |
710.2617 | Cosmic Ray Propagation: Nonlinear Diffusion Parallel and Perpendicular
to Mean Magnetic Field | We consider the propagation of cosmic rays in turbulent magnetic fields. We
use the models of magnetohydrodynamic turbulence that were tested in numerical
simulations, in which the turbulence is injected on large scale and cascades to
small scales. Our attention is focused on the models of the strong turbulence,
but ... | astro-ph | we consider the propagation of cosmic rays in turbulent magnetic fields we use the models of magnetohydrodynamic turbulence that were tested in numerical simulations in which the turbulence is injected on large scale and cascades to small scales our attention is focused on the models of the strong turbulence but we als... | [['we', 'consider', 'the', 'propagation', 'of', 'cosmic', 'rays', 'in', 'turbulent', 'magnetic', 'fields', 'we', 'use', 'the', 'models', 'of', 'magnetohydrodynamic', 'turbulence', 'that', 'were', 'tested', 'in', 'numerical', 'simulations', 'in', 'which', 'the', 'turbulence', 'is', 'injected', 'on', 'large', 'scale', 'a... | [-0.1224602887329335, 0.19827466778366304, -0.0748065562702988, 0.1343580287407016, -0.07904608422564721, -0.011102143799075932, -0.04197281522333728, 0.35479097195893405, -0.30662400666927175, -0.29643588621979505, 0.023734246738391314, -0.2530212630641413, -0.08990887292978786, 0.22518790301457955, 0.0185971464967682... |
710.2618 | Probing the Intrinsic Shape and Alignment of Dark Matter Haloes using
SDSS Galaxy Groups | We study the three-dimensional and projected shapes of galaxy groups in the
Sloan Digital Sky Survey Data Release 4, and examine the alignment between the
orientation of the central galaxy and the spatial distribution of satellite
galaxies. The projected ellipticity of a group is measured using the moments of
the dis... | astro-ph | we study the threedimensional and projected shapes of galaxy groups in the sloan digital sky survey data release 4 and examine the alignment between the orientation of the central galaxy and the spatial distribution of satellite galaxies the projected ellipticity of a group is measured using the moments of the discrete... | [['we', 'study', 'the', 'threedimensional', 'and', 'projected', 'shapes', 'of', 'galaxy', 'groups', 'in', 'the', 'sloan', 'digital', 'sky', 'survey', 'data', 'release', '4', 'and', 'examine', 'the', 'alignment', 'between', 'the', 'orientation', 'of', 'the', 'central', 'galaxy', 'and', 'the', 'spatial', 'distribution', ... | [-0.10698801472466042, 0.06655125351860486, -0.11232372819386581, 0.07989229399889232, -0.06797906615810984, 0.014703901996836067, -0.02668166483673168, 0.4314850652947071, -0.136387592907673, -0.401222884876931, 0.019079475578891628, -0.308201586788005, 0.0001016415526813015, 0.16978014142728073, 0.018989930999158147,... |
710.2619 | The Effects of Fourth Generation on the double Lepton Polarization in B
\rar K \ell^+ \ell^- decay | This study investigates the influence of the fourth generation quarks on the
double lepton polarizations in B \rar K \ell^+ \ell^- decay. Taking
|V_{t's}V_{t'b}|\sim \{0.01-0.03\} with phase about 100^\circ, which is
consistent with the b\to s\ell^+\ell^- rate and the B_s mixing parameter Delta
m_{B_s}$, we obtain th... | hep-ph | this study investigates the influence of the fourth generation quarks on the double lepton polarizations in b rar k ell ell decay taking v_tsv_tbsim 001003 with phase about 100circ which is consistent with the bto sellell rate and the b_s mixing parameter delta m_b_s we obtain that the double leptonmuon and tau polariz... | [['this', 'study', 'investigates', 'the', 'influence', 'of', 'the', 'fourth', 'generation', 'quarks', 'on', 'the', 'double', 'lepton', 'polarizations', 'in', 'b', 'rar', 'k', 'ell', 'ell', 'decay', 'taking', 'v_tsv_tbsim', '001003', 'with', 'phase', 'about', '100circ', 'which', 'is', 'consistent', 'with', 'the', 'bto',... | [-0.12203728905822857, 0.2217955869420555, -0.019216857574941838, 0.1163584406611072, -0.10586739389831762, -0.15715724299381295, 0.0991774639479412, 0.2718179556036211, -0.2820526462452239, -0.283103797315474, 0.022172229483734863, -0.2915151694688542, -0.024098227109131683, 0.190318705121347, 0.10148648840251816, 0.0... |
710.262 | Generalized versus selected descriptions of quantum LC - circuits | Proofs are given that the quantum-mechanical description of the LC -circuit
with a time dependent external source can be readily established by starting
from a more general discretization rule of the electric charge. For this
purpose one resorts to an arbitrary but integer-dependent real function F(n)
instead of n. T... | cond-mat.mes-hall | proofs are given that the quantummechanical description of the lc circuit with a time dependent external source can be readily established by starting from a more general discretization rule of the electric charge for this purpose one resorts to an arbitrary but integerdependent real function fn instead of n this resul... | [['proofs', 'are', 'given', 'that', 'the', 'quantummechanical', 'description', 'of', 'the', 'lc', 'circuit', 'with', 'a', 'time', 'dependent', 'external', 'source', 'can', 'be', 'readily', 'established', 'by', 'starting', 'from', 'a', 'more', 'general', 'discretization', 'rule', 'of', 'the', 'electric', 'charge', 'for'... | [-0.09863513740019425, 0.12521023572261947, -0.07074865809452713, 0.08654360945206976, -0.07149925626310191, -0.18767467314811578, 0.03961166880737738, 0.31878703684174925, -0.2520562509894091, -0.3024180071162326, 0.07892547682044972, -0.24116097151518875, -0.10168249747029652, 0.22699945503705762, -0.0292099730139668... |
710.2621 | Absence of Wavepacket Diffusion in Disordered Nonlinear Systems | We study the spreading of an initially localized wavepacket in two nonlinear
chains (discrete nonlinear Schroedinger and quartic Klein-Gordon) with
disorder. Previous studies suggest that there are many initial conditions such
that the second moment of the norm and energy density distributions diverge as
a function o... | cond-mat.dis-nn | we study the spreading of an initially localized wavepacket in two nonlinear chains discrete nonlinear schroedinger and quartic kleingordon with disorder previous studies suggest that there are many initial conditions such that the second moment of the norm and energy density distributions diverge as a function of time... | [['we', 'study', 'the', 'spreading', 'of', 'an', 'initially', 'localized', 'wavepacket', 'in', 'two', 'nonlinear', 'chains', 'discrete', 'nonlinear', 'schroedinger', 'and', 'quartic', 'kleingordon', 'with', 'disorder', 'previous', 'studies', 'suggest', 'that', 'there', 'are', 'many', 'initial', 'conditions', 'such', 't... | [-0.1768030142545593, 0.17210076903857763, -0.11499502026939115, 0.09823978783666631, -0.025696135697243133, -0.13746767552827466, 0.005522347407971623, 0.35894091994159943, -0.25115133830339464, -0.21756100458287292, 0.09286118654715125, -0.27166923140795407, -0.1223048881574018, 0.1654965717667084, 0.0235294859434256... |
710.2622 | The escape of Lyman photons from a young starburst: the case of Haro 11 | (Abridged) Lyman-alpha (Lya) is a dominant probe of the galaxy population at
high-z. However, interpretation of data drawn from Lya alone hinges on the Lya
escape fraction which, due to the complex radiative transport, may vary
greatly. Here we map the Lya emission from local starburst Haro 11, a Lya
emitter and the ... | astro-ph | abridged lymanalpha lya is a dominant probe of the galaxy population at highz however interpretation of data drawn from lya alone hinges on the lya escape fraction which due to the complex radiative transport may vary greatly here we map the lya emission from local starburst haro 11 a lya emitter and the only known can... | [['abridged', 'lymanalpha', 'lya', 'is', 'a', 'dominant', 'probe', 'of', 'the', 'galaxy', 'population', 'at', 'highz', 'however', 'interpretation', 'of', 'data', 'drawn', 'from', 'lya', 'alone', 'hinges', 'on', 'the', 'lya', 'escape', 'fraction', 'which', 'due', 'to', 'the', 'complex', 'radiative', 'transport', 'may', ... | [-0.001875227729461975, 0.11415421255764419, -0.04611794637416356, 0.13342804516224924, -0.0878386567812413, -0.08021639642507321, 0.0790465050144121, 0.45698817277693055, -0.16577691649352866, -0.34010596568197277, -0.01489756082987047, -0.30912806260665615, -0.026571798394849924, 0.16677145618346653, 0.01527175421859... |
710.2623 | Cup products in Hopf cyclic cohomology via cyclic modules I | This is the first one in a series of two papers on the continuation of our
study in cup products in Hopf cyclic cohomology. In this note we construct
cyclic cocycles of algebras out of Hopf cyclic cocycles of algebras and
coalgebras. In the next paper we consider producing Hopf cyclic cocycle from
"equivariant" Hopf ... | math.KT math.OA | this is the first one in a series of two papers on the continuation of our study in cup products in hopf cyclic cohomology in this note we construct cyclic cocycles of algebras out of hopf cyclic cocycles of algebras and coalgebras in the next paper we consider producing hopf cyclic cocycle from equivariant hopf cyclic... | [['this', 'is', 'the', 'first', 'one', 'in', 'a', 'series', 'of', 'two', 'papers', 'on', 'the', 'continuation', 'of', 'our', 'study', 'in', 'cup', 'products', 'in', 'hopf', 'cyclic', 'cohomology', 'in', 'this', 'note', 'we', 'construct', 'cyclic', 'cocycles', 'of', 'algebras', 'out', 'of', 'hopf', 'cyclic', 'cocycles',... | [-0.21970915479926012, 0.056781179329220166, -0.07905963574966757, 0.028472524978751218, -0.06775617283037914, -0.11326320577032303, -0.033489995053969324, 0.34954077538142925, -0.4104865824262942, -0.14387551230448548, 0.18064822812604728, -0.19836990306058758, -0.1999113484015388, 0.2214179016898201, -0.1989964168338... |
710.2624 | On the use of Neumann's principle for the calculation of the
polarizability tensor of nanostructures | The polarizability measures how the system responds to an applied electrical
field. Computationally, there are many different ways to evaluate this
tensorial quantity, some of which rely on the explicit use of the external
perturbation and require several individual calculations to obtain the full
tensor. In this wor... | cond-mat.mtrl-sci | the polarizability measures how the system responds to an applied electrical field computationally there are many different ways to evaluate this tensorial quantity some of which rely on the explicit use of the external perturbation and require several individual calculations to obtain the full tensor in this work we p... | [['the', 'polarizability', 'measures', 'how', 'the', 'system', 'responds', 'to', 'an', 'applied', 'electrical', 'field', 'computationally', 'there', 'are', 'many', 'different', 'ways', 'to', 'evaluate', 'this', 'tensorial', 'quantity', 'some', 'of', 'which', 'rely', 'on', 'the', 'explicit', 'use', 'of', 'the', 'externa... | [-0.09535831458938931, 0.08595164196729067, -0.08205081986317646, 0.041225842161791273, -0.09071077852175363, -0.06346025355883593, 0.04219813243196644, 0.3739782341584129, -0.24774134556482574, -0.32452616944583584, 0.09199779093586523, -0.2583029507455931, -0.17387583221815237, 0.19619717164353911, -0.019657110252860... |
710.2625 | On two problems concerning topological centers | Let G be an infinite discrete group and bG its Cech-Stone compactification.
Using the well known fact that a free ultrafilter on an infinite set is
nonmeasurable, we show that for each element p of the remainder bG G, left
multiplication L_p:bG \to bG is not Borel measurable. Next assume that G is
abelian. Let D \sub... | math.DS | let g be an infinite discrete group and bg its cechstone compactification using the well known fact that a free ultrafilter on an infinite set is nonmeasurable we show that for each element p of the remainder bg g left multiplication l_pbg to bg is not borel measurable next assume that g is abelian let d subset ellinft... | [['let', 'g', 'be', 'an', 'infinite', 'discrete', 'group', 'and', 'bg', 'its', 'cechstone', 'compactification', 'using', 'the', 'well', 'known', 'fact', 'that', 'a', 'free', 'ultrafilter', 'on', 'an', 'infinite', 'set', 'is', 'nonmeasurable', 'we', 'show', 'that', 'for', 'each', 'element', 'p', 'of', 'the', 'remainder'... | [-0.14777639411533108, 0.13823158169062272, -0.09432417329114218, -0.014628767787228124, -0.11062405867000612, -0.11171336862831735, 0.04724446354039873, 0.34014789091709713, -0.34319792763831525, -0.17344288737513125, 0.0701794136261854, -0.31246477656162686, -0.07412740399058049, 0.18591648645770664, -0.1305606953719... |
710.2626 | Entropy, dimension, and state mixing in a class of time-delayed
dynamical systems | Time-delay systems are, in many ways, a natural set of dynamical systems for
natural scientists to study because they form an interface between abstract
mathematics and data. However, they are complicated because past states must be
sensibly incorporated into the dynamical system. The primary goal of this paper
is to... | nlin.CD | timedelay systems are in many ways a natural set of dynamical systems for natural scientists to study because they form an interface between abstract mathematics and data however they are complicated because past states must be sensibly incorporated into the dynamical system the primary goal of this paper is to begin t... | [['timedelay', 'systems', 'are', 'in', 'many', 'ways', 'a', 'natural', 'set', 'of', 'dynamical', 'systems', 'for', 'natural', 'scientists', 'to', 'study', 'because', 'they', 'form', 'an', 'interface', 'between', 'abstract', 'mathematics', 'and', 'data', 'however', 'they', 'are', 'complicated', 'because', 'past', 'state... | [-0.15726118282826268, 0.12073429976907608, -0.12579019619376508, 0.05602341952265671, -0.05586423020488417, -0.13449645433976753, 0.03487951172853177, 0.33015925156928805, -0.30412408815068076, -0.271520482364399, 0.11419671319654391, -0.2743143101983945, -0.19690874988818305, 0.21325901292292826, -0.05290133874806656... |
710.2627 | Branching integrals and Casselman phenomenon | Let $G$ be a real semisimple Lie group, $K$ its maximal complex subgroup, and
$G_C$ its complexification.
It is known that all the $K$-finite matrix elements on $G$ admit holomorphic
continuation to branching functions on $G_C$ having singularities at the a
prescribed divisor. We propose a geometric explanation of ... | math.RT math.CV | let g be a real semisimple lie group k its maximal complex subgroup and g_c its complexification it is known that all the kfinite matrix elements on g admit holomorphic continuation to branching functions on g_c having singularities at the a prescribed divisor we propose a geometric explanation of this phenomenon the n... | [['let', 'g', 'be', 'a', 'real', 'semisimple', 'lie', 'group', 'k', 'its', 'maximal', 'complex', 'subgroup', 'and', 'g_c', 'its', 'complexification', 'it', 'is', 'known', 'that', 'all', 'the', 'kfinite', 'matrix', 'elements', 'on', 'g', 'admit', 'holomorphic', 'continuation', 'to', 'branching', 'functions', 'on', 'g_c'... | [-0.2443337468107024, 0.053535684957982055, -0.12413686435181825, 0.020610679428847062, -0.2233530806214918, -0.1215753663360836, 0.04778892765679057, 0.3613665801073824, -0.3009536886617305, -0.16209402767616132, 0.09243665526931484, -0.25827308779671077, -0.21431473237536255, 0.16163808734170973, -0.11146511542536909... |
710.2628 | A Search for Single Radio Pulses and Bursts from Southern AXPs | We observed four southern AXPs in 1999 near 1400 MHz with the Parkes 64-m
radio telescope to search for periodic radio emission. No Fourier candidates
were discovered in the initial analysis, but the recent radio activity observed
for the AXP XTE J1810-197 has prompted us to revisit these data to search for
single ra... | astro-ph | we observed four southern axps in 1999 near 1400 mhz with the parkes 64m radio telescope to search for periodic radio emission no fourier candidates were discovered in the initial analysis but the recent radio activity observed for the axp xte j1810197 has prompted us to revisit these data to search for single radio pu... | [['we', 'observed', 'four', 'southern', 'axps', 'in', '1999', 'near', '1400', 'mhz', 'with', 'the', 'parkes', '64m', 'radio', 'telescope', 'to', 'search', 'for', 'periodic', 'radio', 'emission', 'no', 'fourier', 'candidates', 'were', 'discovered', 'in', 'the', 'initial', 'analysis', 'but', 'the', 'recent', 'radio', 'ac... | [-0.1236959291250914, 0.11539760162472669, -0.025305042666544143, 0.1318488126354558, -0.195169649521043, -0.14068316894800478, 0.09262627107091248, 0.4785134344732851, -0.15386178609880066, -0.3565613020638606, 0.14688687866266564, -0.32007629187826653, -0.07118618457501096, 0.290645578830622, 0.036342298944613764, -0... |
710.2629 | On cross-ratio distortion and Schwarz derivative | We prove asymptotic estimates for the cross-ratio distortion with respect to
a smooth or holomorphic function in terms of its Schwarz derivative.
| math.DS math.GM | we prove asymptotic estimates for the crossratio distortion with respect to a smooth or holomorphic function in terms of its schwarz derivative | [['we', 'prove', 'asymptotic', 'estimates', 'for', 'the', 'crossratio', 'distortion', 'with', 'respect', 'to', 'a', 'smooth', 'or', 'holomorphic', 'function', 'in', 'terms', 'of', 'its', 'schwarz', 'derivative']] | [-0.17392872853881933, -0.08001152993264524, -0.10041477837578648, 0.07805610024793581, -0.0952539358457381, -0.05242765136063099, 0.01435255885801532, 0.3366287723183632, -0.3119371341202747, -0.17760606803560883, 0.1426364817518995, -0.2794498172165318, -0.17748361619570377, 0.1716381057313728, -0.17751101696525107, ... |
710.263 | Span-program-based quantum algorithm for evaluating formulas | We give a quantum algorithm for evaluating formulas over an extended gate
set, including all two- and three-bit binary gates (e.g., NAND, 3-majority).
The algorithm is optimal on read-once formulas for which each gate's inputs are
balanced in a certain sense.
The main new tool is a correspondence between a classica... | quant-ph | we give a quantum algorithm for evaluating formulas over an extended gate set including all two and threebit binary gates eg nand 3majority the algorithm is optimal on readonce formulas for which each gates inputs are balanced in a certain sense the main new tool is a correspondence between a classical linearalgebraic ... | [['we', 'give', 'a', 'quantum', 'algorithm', 'for', 'evaluating', 'formulas', 'over', 'an', 'extended', 'gate', 'set', 'including', 'all', 'two', 'and', 'threebit', 'binary', 'gates', 'eg', 'nand', '3majority', 'the', 'algorithm', 'is', 'optimal', 'on', 'readonce', 'formulas', 'for', 'which', 'each', 'gates', 'inputs',... | [-0.1270721014454097, 0.057385250293536694, -0.054846396797971014, 0.10695316873666277, -0.07994244704225464, -0.20027586718535292, 0.10273433378323966, 0.3740598238410725, -0.2532676420599708, -0.32039620264845, 0.09490642041993747, -0.21998458463581366, -0.20204655820692796, 0.2884829171066024, -0.1005178476684639, 0... |
710.2631 | An In-Class Discussion Activity on the Nature of Science and Intelligent
Design | In this paper I describe an in-class discussion activity aimed at helping
elementary education majors in a physical science course think about issues
surrounding the inclusion of "Intelligent Design" in public school science
standards. I discuss the background instruction given, the content of the
activity and some r... | physics.ed-ph | in this paper i describe an inclass discussion activity aimed at helping elementary education majors in a physical science course think about issues surrounding the inclusion of intelligent design in public school science standards i discuss the background instruction given the content of the activity and some results ... | [['in', 'this', 'paper', 'i', 'describe', 'an', 'inclass', 'discussion', 'activity', 'aimed', 'at', 'helping', 'elementary', 'education', 'majors', 'in', 'a', 'physical', 'science', 'course', 'think', 'about', 'issues', 'surrounding', 'the', 'inclusion', 'of', 'intelligent', 'design', 'in', 'public', 'school', 'science... | [-0.050528788060512184, 0.10599907593310696, -0.06449523734209954, 0.08295198996278967, -0.15458692659465773, -0.11141773735014897, 0.053176939718091405, 0.35020429191162, -0.23607778738973276, -0.3747740970959641, 0.10053356930191787, -0.2691548101006533, -0.17854925027262103, 0.16845139999926653, -0.1650781135584386,... |
710.2632 | On the Whitham Equations for the Defocusing Complex Modified KdV
Equation | We study the Whitham equations for the defocusing complex modified KdV (mKdV)
equation. These Whitham equations are quasilinear hyperbolic equations and they
describe the averaged dynamics of the rapid oscillations which appear in the
solution of the mKdV equation when the dispersive parameter is small. The
oscillati... | nlin.SI math-ph math.MP | we study the whitham equations for the defocusing complex modified kdv mkdv equation these whitham equations are quasilinear hyperbolic equations and they describe the averaged dynamics of the rapid oscillations which appear in the solution of the mkdv equation when the dispersive parameter is small the oscillations ar... | [['we', 'study', 'the', 'whitham', 'equations', 'for', 'the', 'defocusing', 'complex', 'modified', 'kdv', 'mkdv', 'equation', 'these', 'whitham', 'equations', 'are', 'quasilinear', 'hyperbolic', 'equations', 'and', 'they', 'describe', 'the', 'averaged', 'dynamics', 'of', 'the', 'rapid', 'oscillations', 'which', 'appear... | [-0.19990931251938915, 0.10261371124523092, -0.054540316254543274, 0.1366203110009222, -0.13415836936361353, -0.15094940326648804, -0.12440037502067715, 0.25752780092617783, -0.3061409051936697, -0.182928769055649, 0.126296790575766, -0.32215989074131973, -0.20127284327935113, 0.20881064738553595, 0.014368340392715074,... |
710.2633 | X-ray Emission from Magnetically Torqued Disks of Oe/Be Stars | We focus attention on the Oe/Be stars to test the concept that the disks of
these stars form by magnetic channeling of wind material toward the equator.
Calculations are made of the X-rays expected from the Magnetically Torqued Disk
(MTD) model for Be stars discussed by Cassinelli et al. (2002), by Maheswaran
(2003),... | astro-ph | we focus attention on the oebe stars to test the concept that the disks of these stars form by magnetic channeling of wind material toward the equator calculations are made of the xrays expected from the magnetically torqued disk mtd model for be stars discussed by cassinelli et al 2002 by maheswaran 2003 and by brown ... | [['we', 'focus', 'attention', 'on', 'the', 'oebe', 'stars', 'to', 'test', 'the', 'concept', 'that', 'the', 'disks', 'of', 'these', 'stars', 'form', 'by', 'magnetic', 'channeling', 'of', 'wind', 'material', 'toward', 'the', 'equator', 'calculations', 'are', 'made', 'of', 'the', 'xrays', 'expected', 'from', 'the', 'magne... | [-0.04227134128741454, 0.13375967633846814, -0.031183001288445665, 0.033767295911093245, -0.09401799496845342, -0.05130187948816456, 0.06778649754996877, 0.3754665452754125, -0.17792124805419007, -0.3839721871598158, 0.015538483653654112, -0.28726824710320215, -0.06229249685420655, 0.20595142301754094, -0.0470259131223... |
710.2634 | The piston dispersive shock wave problem | The one-dimensional piston shock problem is a classical result of shock wave
theory. In this work, the analogous dispersive shock wave (DSW) problem for a
dispersive fluid described by the nonlinear Schr\"odinger equation is analyzed.
Asymptotic solutions are calculated using Whitham averaging theory for a
"piston" (... | nlin.PS | the onedimensional piston shock problem is a classical result of shock wave theory in this work the analogous dispersive shock wave dsw problem for a dispersive fluid described by the nonlinear schrodinger equation is analyzed asymptotic solutions are calculated using whitham averaging theory for a piston step potentia... | [['the', 'onedimensional', 'piston', 'shock', 'problem', 'is', 'a', 'classical', 'result', 'of', 'shock', 'wave', 'theory', 'in', 'this', 'work', 'the', 'analogous', 'dispersive', 'shock', 'wave', 'dsw', 'problem', 'for', 'a', 'dispersive', 'fluid', 'described', 'by', 'the', 'nonlinear', 'schrodinger', 'equation', 'is'... | [-0.12831403625127027, 0.11779347758108218, -0.12092593929888348, 0.05823520152210092, -0.10009053357810314, -0.12452173181892638, -0.02908992310118005, 0.37112205139627413, -0.2689426449318749, -0.21525397973476043, 0.09046218370245437, -0.29016599574658486, -0.12866446445488172, 0.2350236934019319, 0.0406947073726249... |
710.2635 | The CO Molecular Outflows of IRAS 16293-2422 Probed by the Submillimeter
Array | We have mapped the proto-binary source IRAS 16293-2422 in CO 2-1, 13CO 2-1,
and CO 3-2 with the Submillimeter Array (SMA). The maps with resolution of
1".5-5" reveal a single small scale (~3000 AU) bipolar molecular outflow along
the east-west direction. We found that the blueshifted emission of this small
scale outf... | astro-ph | we have mapped the protobinary source iras 162932422 in co 21 13co 21 and co 32 with the submillimeter array sma the maps with resolution of 155 reveal a single small scale 3000 au bipolar molecular outflow along the eastwest direction we found that the blueshifted emission of this small scale outflow mainly extends to... | [['we', 'have', 'mapped', 'the', 'protobinary', 'source', 'iras', '162932422', 'in', 'co', '21', '13co', '21', 'and', 'co', '32', 'with', 'the', 'submillimeter', 'array', 'sma', 'the', 'maps', 'with', 'resolution', 'of', '155', 'reveal', 'a', 'single', 'small', 'scale', '3000', 'au', 'bipolar', 'molecular', 'outflow', ... | [-0.10533145803235718, 0.11103831928127927, -0.013427118299980922, 0.028027051145138957, -0.07876862704356694, -0.09836773467952084, -0.03488638569337234, 0.4691039545269793, -0.19758102033184138, -0.3177720066091484, 0.09202879593366935, -0.29445020322557813, 0.02120480272188776, 0.1521983909941114, 0.0155657410008750... |
710.2636 | Low energy particle physics and cosmology of nonlinear supersymmetric
general relativity | We show a low energy physical meaning of nonlinear supersymmetric general
relativity (NLSUSY GR) in asymptotic Riemann-flat space-time by studying the
vacuum structure of N = 2 linear supersymmetry (LSUSY) invariant QED, which is
equivalent to N = 2 NLSUSY model, in two dimensional space-time. Two different
vacuum fi... | hep-th | we show a low energy physical meaning of nonlinear supersymmetric general relativity nlsusy gr in asymptotic riemannflat spacetime by studying the vacuum structure of n 2 linear supersymmetry lsusy invariant qed which is equivalent to n 2 nlsusy model in two dimensional spacetime two different vacuum field configuratio... | [['we', 'show', 'a', 'low', 'energy', 'physical', 'meaning', 'of', 'nonlinear', 'supersymmetric', 'general', 'relativity', 'nlsusy', 'gr', 'in', 'asymptotic', 'riemannflat', 'spacetime', 'by', 'studying', 'the', 'vacuum', 'structure', 'of', 'n', '2', 'linear', 'supersymmetry', 'lsusy', 'invariant', 'qed', 'which', 'is'... | [-0.15709840671672504, 0.23711251059775146, -0.07941609846038401, 0.1837728857906174, -0.0860442359033706, -0.2201111297864391, -0.06750760769129407, 0.27776558046723354, -0.20342765011995725, -0.31489445136774485, 0.049885499961104016, -0.20338393241281108, -0.11089034187750016, 0.07151142233502766, -0.012648148955159... |
710.2637 | Relaxation dynamics in quantum electron-glasses | It is experimentally shown that, depending on the carrier-concentration of
the system $n$, the dynamics of electron-glasses either \textit{slows down
}with increasing temperature or it is \textit{independent} of it. This also
correlates with the dependence of a typical relaxation time (or `viscosity') on
$n$. These l... | cond-mat.str-el cond-mat.dis-nn | it is experimentally shown that depending on the carrierconcentration of the system n the dynamics of electronglasses either textitslows down with increasing temperature or it is textitindependent of it this also correlates with the dependence of a typical relaxation time or viscosity on n these linked features are arg... | [['it', 'is', 'experimentally', 'shown', 'that', 'depending', 'on', 'the', 'carrierconcentration', 'of', 'the', 'system', 'n', 'the', 'dynamics', 'of', 'electronglasses', 'either', 'textitslows', 'down', 'with', 'increasing', 'temperature', 'or', 'it', 'is', 'textitindependent', 'of', 'it', 'this', 'also', 'correlates'... | [-0.1172639398901083, 0.23707162317199013, -0.12324868736322969, 0.06546215953737071, -0.027658214976933475, -0.17588334069781317, 0.005288621709041763, 0.3560017001970361, -0.26918422147476423, -0.28494667854586925, 0.0855252030196425, -0.30756787992625806, -0.1622474328178214, 0.19845174334053203, -0.0077084218598126... |
710.2638 | Coexistence of magnetism and superconductivity in a t-J bilayer | We investigate coexistence of antiferromagnetic and superconducting
correlations in bilayered materials using a two-dimensional t-J model with
couplings across the layers using variational Monte Carlo calculations. It is
found that the underdoped regime supports a coexisting phase, beyond which the
(d-wave) supercond... | cond-mat.supr-con cond-mat.str-el | we investigate coexistence of antiferromagnetic and superconducting correlations in bilayered materials using a twodimensional tj model with couplings across the layers using variational monte carlo calculations it is found that the underdoped regime supports a coexisting phase beyond which the dwave superconducting st... | [['we', 'investigate', 'coexistence', 'of', 'antiferromagnetic', 'and', 'superconducting', 'correlations', 'in', 'bilayered', 'materials', 'using', 'a', 'twodimensional', 'tj', 'model', 'with', 'couplings', 'across', 'the', 'layers', 'using', 'variational', 'monte', 'carlo', 'calculations', 'it', 'is', 'found', 'that',... | [-0.20353150984738022, 0.2619811207354109, 0.018017855010412892, 0.07381565061654767, 0.003457655083259632, -0.19062479596448548, 0.10886256274735105, 0.36627943727091467, -0.2709177139086713, -0.27486025283819643, -0.012779849516388414, -0.38824490275362444, -0.07020842646216524, 0.15028663963914432, 0.124421794297462... |
710.2639 | Heavy Quarkonium States with the Holographic Potential | The quarkonium states in a quark-gluon plasma is examined with the heavy
quark potential implied by the holographic principle. Both the vanila
AdS-Schwarzschild metric and the one with an infrared cutoff are considered.
The dissociation temperature is calculated by solving the Schr\"o dinger
equation of the potential... | hep-ph hep-th | the quarkonium states in a quarkgluon plasma is examined with the heavy quark potential implied by the holographic principle both the vanila adsschwarzschild metric and the one with an infrared cutoff are considered the dissociation temperature is calculated by solving the schro dinger equation of the potential model i... | [['the', 'quarkonium', 'states', 'in', 'a', 'quarkgluon', 'plasma', 'is', 'examined', 'with', 'the', 'heavy', 'quark', 'potential', 'implied', 'by', 'the', 'holographic', 'principle', 'both', 'the', 'vanila', 'adsschwarzschild', 'metric', 'and', 'the', 'one', 'with', 'an', 'infrared', 'cutoff', 'are', 'considered', 'th... | [-0.06746333321678408, 0.18232662861191784, -0.11622760346203688, 0.07447642419165709, 0.012808016700936216, -0.11411970690824091, 0.006498495116829872, 0.34457825819429544, -0.16786586792607391, -0.2366428582685157, 0.029794303109935884, -0.33422599194039193, -0.013821078641783623, 0.14181810438389048, 0.0342116657439... |
710.264 | Time-dependent AdS/CFT Duality II: Holographic Reconstruction of Bulk
Metric and Possible Resolution of Singularity | We continue the studies of our earlier proposal for an AdS/CFT correspondence
for time-dependent supergravity backgrounds. We note that by performing a
suitable change of variables, the dual super Yang-Mills theory lives on a flat
base space, and the time-dependence of the supergravity background is entirely
encoded ... | hep-th | we continue the studies of our earlier proposal for an adscft correspondence for timedependent supergravity backgrounds we note that by performing a suitable change of variables the dual super yangmills theory lives on a flat base space and the timedependence of the supergravity background is entirely encoded in the ti... | [['we', 'continue', 'the', 'studies', 'of', 'our', 'earlier', 'proposal', 'for', 'an', 'adscft', 'correspondence', 'for', 'timedependent', 'supergravity', 'backgrounds', 'we', 'note', 'that', 'by', 'performing', 'a', 'suitable', 'change', 'of', 'variables', 'the', 'dual', 'super', 'yangmills', 'theory', 'lives', 'on', ... | [-0.10956157359384722, 0.1369923802641889, -0.14448327942405859, 0.12504013072353817, -0.11148815257775206, -0.1072695843004171, 0.012455504768407873, 0.33203239548170277, -0.18955169412037057, -0.27296640259108595, 0.07733947425825341, -0.27379633757415334, -0.20564298281416057, 0.11084396616826134, -0.078816149963606... |
710.2641 | Deformations of Border Bases | Here we study the problem of generalizing one of the main tools of Groebner
basis theory, namely the flat deformation to the leading term ideal, to the
border basis setting. After showing that the straightforward approach based on
the deformation to the degree form ideal works only under additional
hypotheses, we int... | math.AC math.AG | here we study the problem of generalizing one of the main tools of groebner basis theory namely the flat deformation to the leading term ideal to the border basis setting after showing that the straightforward approach based on the deformation to the degree form ideal works only under additional hypotheses we introduce... | [['here', 'we', 'study', 'the', 'problem', 'of', 'generalizing', 'one', 'of', 'the', 'main', 'tools', 'of', 'groebner', 'basis', 'theory', 'namely', 'the', 'flat', 'deformation', 'to', 'the', 'leading', 'term', 'ideal', 'to', 'the', 'border', 'basis', 'setting', 'after', 'showing', 'that', 'the', 'straightforward', 'ap... | [-0.12837850767142184, 0.04798268244068148, -0.0991589783404309, 0.06344799419142097, -0.07596532993956462, -0.12295998025594371, 0.06175155948987556, 0.3443898416793469, -0.3314233397856563, -0.2082726942738388, 0.15047161373671247, -0.18573365686786966, -0.19107703608623544, 0.19557438344512318, -0.053522287734452036... |
710.2642 | Comment on: Stochastic local operations and classical communication
Invariant and the residual entanglement for n qubits | In a recent paper [Phys. Rev. A 76, 032304(2007)], Li et al. proposed the
definition of the residual entanglement for n qubits by means of the Stochastic
local operations and classical communication. Here we argue that their
definition is not suitable for the case of odd-n qubits.
| quant-ph | in a recent paper phys rev a 76 0323042007 li et al proposed the definition of the residual entanglement for n qubits by means of the stochastic local operations and classical communication here we argue that their definition is not suitable for the case of oddn qubits | [['in', 'a', 'recent', 'paper', 'phys', 'rev', 'a', '76', '0323042007', 'li', 'et', 'al', 'proposed', 'the', 'definition', 'of', 'the', 'residual', 'entanglement', 'for', 'n', 'qubits', 'by', 'means', 'of', 'the', 'stochastic', 'local', 'operations', 'and', 'classical', 'communication', 'here', 'we', 'argue', 'that', '... | [-0.12550495748987683, 0.13526350929928216, -0.0007490050452558891, -0.07086275953991825, -0.003948447942409826, -0.1124654961142527, 0.12397534417686984, 0.2959700085263213, -0.17311161155205057, -0.3345658232093505, -0.03671395601502255, -0.2258583924571133, -0.21869093799740885, 0.18640943345330332, -0.1627414993962... |
710.2643 | Solutions of Adler's lattice equation associated with 2-cycles of the
Backlund transformation | The BT of Adler's lattice equation is inherent in the equation itself by
virtue of its multidimensional consistency. We refer to a solution of the
equation that is related to itself by the composition of two BTs (with
different Backlund parameters) as a 2-cycle of the BT. In this article we will
show that such soluti... | nlin.SI | the bt of adlers lattice equation is inherent in the equation itself by virtue of its multidimensional consistency we refer to a solution of the equation that is related to itself by the composition of two bts with different backlund parameters as a 2cycle of the bt in this article we will show that such solutions are ... | [['the', 'bt', 'of', 'adlers', 'lattice', 'equation', 'is', 'inherent', 'in', 'the', 'equation', 'itself', 'by', 'virtue', 'of', 'its', 'multidimensional', 'consistency', 'we', 'refer', 'to', 'a', 'solution', 'of', 'the', 'equation', 'that', 'is', 'related', 'to', 'itself', 'by', 'the', 'composition', 'of', 'two', 'bts... | [-0.17312211434503919, 0.07456007098877117, -0.07142139461234603, 0.02600425903342272, -0.0994889707941758, -0.11099990239660991, 0.018836450321893943, 0.3101122418320493, -0.32189791863294026, -0.22123679086369905, 0.13713699929465198, -0.30646577972036443, -0.18438619737954517, 0.1462022944402538, -0.0732754332123716... |
710.2644 | New physics effect on the top-Yukawa coupling at ILC | Measurement of the top-Yukawa coupling is important to understand the fermion
mass generation mechanism and dynamics of electroweak symmetry breaking. We
discuss the top quark anomalous couplings which can be described by higher
dimensional operators. We investigate the process $e^-e^+ \to W^-W^+\nu\bar\nu
\to t \bar... | hep-ph | measurement of the topyukawa coupling is important to understand the fermion mass generation mechanism and dynamics of electroweak symmetry breaking we discuss the top quark anomalous couplings which can be described by higher dimensional operators we investigate the process ee to wwnubarnu to t bar t nubarnu to study ... | [['measurement', 'of', 'the', 'topyukawa', 'coupling', 'is', 'important', 'to', 'understand', 'the', 'fermion', 'mass', 'generation', 'mechanism', 'and', 'dynamics', 'of', 'electroweak', 'symmetry', 'breaking', 'we', 'discuss', 'the', 'top', 'quark', 'anomalous', 'couplings', 'which', 'can', 'be', 'described', 'by', 'h... | [-0.13338999091697637, 0.2418500442778872, -0.017094184812258488, 0.13548448611679, -0.09571755722775975, -0.131109972764808, 0.027568662989764445, 0.28234412737431064, -0.27580107204235527, -0.3100828589290701, 0.008542628488152898, -0.34131694087378117, -0.02564650610269558, 0.11423468338425762, 0.09888438185957331, ... |
710.2645 | Origins and breadth of the theory of higher homotopies | Higher homotopies are nowadays playing a prominent role in mathematics as
well as in certain branches of theoretical physics. We recall some of the
connections between the past and the present developments. Higher homotopies
were isolated within algebraic topology at least as far back as the 1940's.
Prompted by the f... | math.AT math.AG | higher homotopies are nowadays playing a prominent role in mathematics as well as in certain branches of theoretical physics we recall some of the connections between the past and the present developments higher homotopies were isolated within algebraic topology at least as far back as the 1940s prompted by the failure... | [['higher', 'homotopies', 'are', 'nowadays', 'playing', 'a', 'prominent', 'role', 'in', 'mathematics', 'as', 'well', 'as', 'in', 'certain', 'branches', 'of', 'theoretical', 'physics', 'we', 'recall', 'some', 'of', 'the', 'connections', 'between', 'the', 'past', 'and', 'the', 'present', 'developments', 'higher', 'homoto... | [-0.12724687773431026, 0.08787559977932423, -0.12050705916868482, 0.13681850684548003, -0.10613617681188088, -0.1523799462372373, 0.012890366876187423, 0.3466009796165301, -0.3098142399645314, -0.29871063229183653, 0.13208805492336922, -0.21845488869615204, -0.1846197587527135, 0.18863336186236265, -0.1376902547761284,... |
710.2646 | Fast projectile stopping power of two-dimensional strongly correlated
electron liquids | We study the high-velocity-projectile limit of the polarizational
contribution to the in-plane stopping power in a strongly coupled
two-dimensional electron liquid. The dielectric formalism based on the method
of moments is employed. The frequency moments of the loss function are
calculated using the model Hamiltonia... | cond-mat.str-el | we study the highvelocityprojectile limit of the polarizational contribution to the inplane stopping power in a strongly coupled twodimensional electron liquid the dielectric formalism based on the method of moments is employed the frequency moments of the loss function are calculated using the model hamiltonian includ... | [['we', 'study', 'the', 'highvelocityprojectile', 'limit', 'of', 'the', 'polarizational', 'contribution', 'to', 'the', 'inplane', 'stopping', 'power', 'in', 'a', 'strongly', 'coupled', 'twodimensional', 'electron', 'liquid', 'the', 'dielectric', 'formalism', 'based', 'on', 'the', 'method', 'of', 'moments', 'is', 'emplo... | [-0.12277695167108209, 0.1181056263626783, -0.06860365510567443, 0.05470773259891415, -0.010015684503505562, -0.09060864788540579, 0.0030460252196757823, 0.33790738676227144, -0.2697739349557208, -0.24612394169497595, 0.007287438266438904, -0.3398489339107817, -0.12956139350358348, 0.1475422051886411, 0.062810056981957... |
710.2647 | Search for GMSB NLSPs at LHC | NLSP - LSP decays could have dramatic influence on SUSY phenomenology at LHC.
NLSP could have significant lifetime and could be charged. In at least two
scenarios detectors must be used in a special way. They were not optimized for
detection of heavy (semi)stable charged particles and decaying in flight
(neutral or c... | hep-ph | nlsp lsp decays could have dramatic influence on susy phenomenology at lhc nlsp could have significant lifetime and could be charged in at least two scenarios detectors must be used in a special way they were not optimized for detection of heavy semistable charged particles and decaying in flight neutral or charged nls... | [['nlsp', 'lsp', 'decays', 'could', 'have', 'dramatic', 'influence', 'on', 'susy', 'phenomenology', 'at', 'lhc', 'nlsp', 'could', 'have', 'significant', 'lifetime', 'and', 'could', 'be', 'charged', 'in', 'at', 'least', 'two', 'scenarios', 'detectors', 'must', 'be', 'used', 'in', 'a', 'special', 'way', 'they', 'were', '... | [-0.047456743332799776, 0.3186227278018447, -0.09105371049771162, 0.14085526624056574, -0.03965831391054065, -0.2796635219176644, -0.05595400248261883, 0.38953092843549303, -0.17702287519095491, -0.37408171239474863, 0.08597921252997005, -0.31914916964030937, 0.03648746527463504, 0.15995041984579947, -0.002942582327642... |
710.2648 | Hopf algebras and characters of classical groups | Schur functions provide an integral basis of the ring of symmetric functions.
It is shown that this ring has a natural Hopf algebra structure by identifying
the appropriate product, coproduct, unit, counit and antipode, and their
properties. Characters of covariant tensor irreducible representations of the
classical ... | math.RT math.RA | schur functions provide an integral basis of the ring of symmetric functions it is shown that this ring has a natural hopf algebra structure by identifying the appropriate product coproduct unit counit and antipode and their properties characters of covariant tensor irreducible representations of the classical groups g... | [['schur', 'functions', 'provide', 'an', 'integral', 'basis', 'of', 'the', 'ring', 'of', 'symmetric', 'functions', 'it', 'is', 'shown', 'that', 'this', 'ring', 'has', 'a', 'natural', 'hopf', 'algebra', 'structure', 'by', 'identifying', 'the', 'appropriate', 'product', 'coproduct', 'unit', 'counit', 'and', 'antipode', '... | [-0.19744242397166836, 0.04982542680326698, -0.07983210899381556, 0.045943569179035276, -0.1357880593675515, -0.09460643265380436, -0.027486015883330096, 0.36798613149131465, -0.3840854575491359, -0.12971163352426046, 0.13638566463437474, -0.20193657702487758, -0.18995971811346263, 0.14696901321856895, -0.0499538355785... |
710.2649 | Geometry of Multiplicative Preprojective Algebra | Crawley-Boevey and Shaw recently introduced a certain multiplicative analogue
of the deformed preprojective algebra, which they called the multiplicative
preprojective algebra. In this paper we study the moduli space of (semi)stable
representations of such an algebra (the multiplicative quiver variety), which
in fact... | math.SG math.AG | crawleyboevey and shaw recently introduced a certain multiplicative analogue of the deformed preprojective algebra which they called the multiplicative preprojective algebra in this paper we study the moduli space of semistable representations of such an algebra the multiplicative quiver variety which in fact has many ... | [['crawleyboevey', 'and', 'shaw', 'recently', 'introduced', 'a', 'certain', 'multiplicative', 'analogue', 'of', 'the', 'deformed', 'preprojective', 'algebra', 'which', 'they', 'called', 'the', 'multiplicative', 'preprojective', 'algebra', 'in', 'this', 'paper', 'we', 'study', 'the', 'moduli', 'space', 'of', 'semistable... | [-0.17664877491713057, 0.05901308837034224, -0.09902868703099303, 0.056041799855922336, -0.16063905791303174, -0.1519866997727239, -0.05817805498468186, 0.35087084654169004, -0.43770415015274383, -0.1731733781281767, 0.07914574442958063, -0.17425424557515098, -0.25562576857990904, 0.16397227507970127, -0.22484908270893... |
710.265 | Memory Effects in the Standard Model for Glasses | The standard model of glasses is an ensemble of two-level systems interacting
with a thermal bath. The general origin of memory effects in this model is a
quasi-stationary but non-equilibrium state of a single two-level system, which
is realized due to a finite-rate cooling and very slow thermally activated
relaxatio... | cond-mat.dis-nn | the standard model of glasses is an ensemble of twolevel systems interacting with a thermal bath the general origin of memory effects in this model is a quasistationary but nonequilibrium state of a single twolevel system which is realized due to a finiterate cooling and very slow thermally activated relaxation we show... | [['the', 'standard', 'model', 'of', 'glasses', 'is', 'an', 'ensemble', 'of', 'twolevel', 'systems', 'interacting', 'with', 'a', 'thermal', 'bath', 'the', 'general', 'origin', 'of', 'memory', 'effects', 'in', 'this', 'model', 'is', 'a', 'quasistationary', 'but', 'nonequilibrium', 'state', 'of', 'a', 'single', 'twolevel'... | [-0.11522099803939151, 0.25052265223954845, -0.11930822209881929, 0.048659556648150706, 0.005474349930106352, -0.18950060557884474, 0.04121369641313019, 0.34037136550371844, -0.2783323069297088, -0.2445878035699328, 0.06067781165669051, -0.2608411478654792, -0.11664672182717671, 0.1572921013799108, -0.01629085664559776... |
710.2651 | Groupoid Extensions of Mapping Class Representations for Bordered
Surfaces | The mapping class group of a surface with one boundary component admits
numerous interesting representations including as a group of automorphisms of a
free group and as a group of symplectic transformations. Insofar as the mapping
class group can be identified with the fundamental group of Riemann's moduli
space, it... | math.GT | the mapping class group of a surface with one boundary component admits numerous interesting representations including as a group of automorphisms of a free group and as a group of symplectic transformations insofar as the mapping class group can be identified with the fundamental group of riemanns moduli space it is f... | [['the', 'mapping', 'class', 'group', 'of', 'a', 'surface', 'with', 'one', 'boundary', 'component', 'admits', 'numerous', 'interesting', 'representations', 'including', 'as', 'a', 'group', 'of', 'automorphisms', 'of', 'a', 'free', 'group', 'and', 'as', 'a', 'group', 'of', 'symplectic', 'transformations', 'insofar', 'as... | [-0.12909744627491182, 0.07268346347374087, -0.10780445885701248, 0.05575593523621464, -0.1567777927773885, -0.09965133493264708, 0.04074644556609341, 0.3813945770613913, -0.382610329396975, -0.2512533570272633, 0.1229611216714948, -0.2342907557797292, -0.18627159781684366, 0.21596629764490688, -0.13363706894690552, -0... |
710.2652 | Renormalization of Orientable Non-Commutative Complex $\Phi^6_3$ Model | In this paper we prove that the Grosse-Wulkenhaar type non-commutative
orientable complex scalar $\phi^6_3$ theory, with two non-commutative
coordinates and the third one commuting with the other two, is renormalizable
to all orders in perturbation theory. Our proof relies on a multiscale analysis
in x space.
| hep-th | in this paper we prove that the grossewulkenhaar type noncommutative orientable complex scalar phi6_3 theory with two noncommutative coordinates and the third one commuting with the other two is renormalizable to all orders in perturbation theory our proof relies on a multiscale analysis in x space | [['in', 'this', 'paper', 'we', 'prove', 'that', 'the', 'grossewulkenhaar', 'type', 'noncommutative', 'orientable', 'complex', 'scalar', 'phi6_3', 'theory', 'with', 'two', 'noncommutative', 'coordinates', 'and', 'the', 'third', 'one', 'commuting', 'with', 'the', 'other', 'two', 'is', 'renormalizable', 'to', 'all', 'orde... | [-0.1552096301275823, 0.11713963778359661, -0.08333741240203381, 0.07537475942323606, -0.08456356660980317, -0.1433250236324966, -0.06554436907430904, 0.27979864676793414, -0.24634791852699386, -0.230702755600214, 0.07217248594647066, -0.28932175394147636, -0.21959120738837454, 0.16748673849635654, -0.08453252429349555... |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.