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708.3749 | Berry's phase | Berry's phase, entry in the Compendium of Quantum Physics: Concepts,
Experiments, History and Philosophy, ed. F. Weinert, K. Hentschel, D.
Greenberger and B. Falkenburg (Springer), to appear
| quant-ph | berrys phase entry in the compendium of quantum physics concepts experiments history and philosophy ed f weinert k hentschel d greenberger and b falkenburg springer to appear | [['berrys', 'phase', 'entry', 'in', 'the', 'compendium', 'of', 'quantum', 'physics', 'concepts', 'experiments', 'history', 'and', 'philosophy', 'ed', 'f', 'weinert', 'k', 'hentschel', 'd', 'greenberger', 'and', 'b', 'falkenburg', 'springer', 'to', 'appear']] | [-0.17785325332510252, 0.15818580171024357, -0.14509072463476547, -0.02178658106950698, -0.09598903675322179, -0.20737214131211792, 0.0775434628939601, 0.2226987725675658, -0.28882622215206977, -0.3225111161807069, 0.013695284185275712, -0.2921764879590935, -0.17869560958610642, 0.12127142516827141, -0.0968725879987080... |
708.375 | Entanglement and correlation functions following a local quench: a
conformal field theory approach | We show that the dynamics resulting from preparing a one-dimensional quantum
system in the ground state of two decoupled parts, then joined together and
left to evolve unitarily with a translational invariant Hamiltonian (a local
quench), can be described by means of quantum field theory. In the case when
the corresp... | cond-mat.stat-mech cond-mat.str-el hep-th quant-ph | we show that the dynamics resulting from preparing a onedimensional quantum system in the ground state of two decoupled parts then joined together and left to evolve unitarily with a translational invariant hamiltonian a local quench can be described by means of quantum field theory in the case when the corresponding t... | [['we', 'show', 'that', 'the', 'dynamics', 'resulting', 'from', 'preparing', 'a', 'onedimensional', 'quantum', 'system', 'in', 'the', 'ground', 'state', 'of', 'two', 'decoupled', 'parts', 'then', 'joined', 'together', 'and', 'left', 'to', 'evolve', 'unitarily', 'with', 'a', 'translational', 'invariant', 'hamiltonian', ... | [-0.1307366955313084, 0.20546821856834485, -0.12343092094861756, 0.047078396381326264, 0.0245730831908683, -0.1336939723655712, 0.0019076988039734332, 0.3403213129689296, -0.2879318568463388, -0.2337307230214049, 0.06597602972862915, -0.2993488553584668, -0.12867280929104277, 0.16824959864913436, 0.02536595110340338, 0... |
708.3751 | Errors and paradoxes in quantum mechanics | Errors and paradoxes in quantum mechanics, entry in the Compendium of Quantum
Physics: Concepts, Experiments, History and Philosophy, ed. F. Weinert, K.
Hentschel, D. Greenberger and B. Falkenburg (Springer), to appear
| quant-ph | errors and paradoxes in quantum mechanics entry in the compendium of quantum physics concepts experiments history and philosophy ed f weinert k hentschel d greenberger and b falkenburg springer to appear | [['errors', 'and', 'paradoxes', 'in', 'quantum', 'mechanics', 'entry', 'in', 'the', 'compendium', 'of', 'quantum', 'physics', 'concepts', 'experiments', 'history', 'and', 'philosophy', 'ed', 'f', 'weinert', 'k', 'hentschel', 'd', 'greenberger', 'and', 'b', 'falkenburg', 'springer', 'to', 'appear']] | [-0.10245427522327631, 0.1202987964835859, -0.1368786911179702, 0.031791110042362444, -0.07294269032295674, -0.22498484009936934, 0.056259437779625575, 0.21281872566549048, -0.3030278379277837, -0.3296628888816603, 0.02129310762299405, -0.3190069074832624, -0.15114570565281377, 0.153040237905037, -0.1477006546431972, 0... |
708.3752 | Contribution in combinatorics in commutative algebra.(ph-d thesis) | In the first chapter we present new results related on monomial ideals of
Borel type. Also, we introduce a new class of monomial ideals, called
$\de$-fixed ideals, which generalize the class of $p$-Borel ideals and we
extend several results to this new class.
In the second chapter, we compute the generic initial id... | math.AC | in the first chapter we present new results related on monomial ideals of borel type also we introduce a new class of monomial ideals called defixed ideals which generalize the class of pborel ideals and we extend several results to this new class in the second chapter we compute the generic initial ideal with repect t... | [['in', 'the', 'first', 'chapter', 'we', 'present', 'new', 'results', 'related', 'on', 'monomial', 'ideals', 'of', 'borel', 'type', 'also', 'we', 'introduce', 'a', 'new', 'class', 'of', 'monomial', 'ideals', 'called', 'defixed', 'ideals', 'which', 'generalize', 'the', 'class', 'of', 'pborel', 'ideals', 'and', 'we', 'ex... | [-0.12160010777354817, 0.059401608747245684, -0.040867637242780815, 0.047088926287472875, -0.100050970528301, -0.12139699984223805, -0.04216063456875469, 0.3232303886530055, -0.35097861372616507, -0.17511172007488965, 0.10009603178895958, -0.22771826547629553, -0.12717317557618232, 0.17878204766778985, -0.0787846225012... |
708.3753 | Transient growth and coupling of vortex and wave modes in
self-gravitating gaseous discs | Flow nonnormality induced linear transient phenomena in thin self-gravitating
astrophysical discs are studied in the shearing sheet approximation. The
considered system includes two modes of perturbations: vortex and (spiral
density) wave. It is shown that self-gravity considerably alters the vortex
mode dynamics -- ... | astro-ph | flow nonnormality induced linear transient phenomena in thin selfgravitating astrophysical discs are studied in the shearing sheet approximation the considered system includes two modes of perturbations vortex and spiral density wave it is shown that selfgravity considerably alters the vortex mode dynamics its transien... | [['flow', 'nonnormality', 'induced', 'linear', 'transient', 'phenomena', 'in', 'thin', 'selfgravitating', 'astrophysical', 'discs', 'are', 'studied', 'in', 'the', 'shearing', 'sheet', 'approximation', 'the', 'considered', 'system', 'includes', 'two', 'modes', 'of', 'perturbations', 'vortex', 'and', 'spiral', 'density',... | [-0.23778853855456214, 0.18287025408002816, -0.07047461919256881, 0.09959778976897798, -0.10378602025902843, -0.06442220910924347, -0.0354929106718261, 0.3055070926409776, -0.24299283492959373, -0.23785322152671393, 0.1006022219287793, -0.24361777236391727, -0.1178521830476948, 0.19595658576294575, 0.04763495563752694,... |
708.3754 | Convergence in the no-core shell model with low-momentum two-nucleon
interactions | The convergence of no-core shell model (NCSM) calculations using
renormalization group evolved low-momentum two-nucleon interactions is studied
for light nuclei up to Li-7. Because no additional transformation was used in
applying the NCSM framework, the energy calculations satisfy the variational
principle for a giv... | nucl-th | the convergence of nocore shell model ncsm calculations using renormalization group evolved lowmomentum twonucleon interactions is studied for light nuclei up to li7 because no additional transformation was used in applying the ncsm framework the energy calculations satisfy the variational principle for a given hamilto... | [['the', 'convergence', 'of', 'nocore', 'shell', 'model', 'ncsm', 'calculations', 'using', 'renormalization', 'group', 'evolved', 'lowmomentum', 'twonucleon', 'interactions', 'is', 'studied', 'for', 'light', 'nuclei', 'up', 'to', 'li7', 'because', 'no', 'additional', 'transformation', 'was', 'used', 'in', 'applying', '... | [-0.06503753476923571, 0.14612514235147642, -0.12522590486439578, 0.16208828805300723, -0.03400662523873765, -0.09174945555764054, 0.015610529937559244, 0.4042622553304248, -0.23770543890620727, -0.32040191927087414, 0.020131819996846104, -0.29921560402993763, -0.04681632287133861, 0.1048967573608041, 0.043396329994253... |
708.3755 | On derived equivalence classification of gentle two-cycle algebras | We classify, up to derived (equivalently, tilting-cotilting) equivalence all
nondegenerate gentle two-cycle algebras. We also give a partial classification
and formulate a conjecture in the degenerate case.
| math.RT | we classify up to derived equivalently tiltingcotilting equivalence all nondegenerate gentle twocycle algebras we also give a partial classification and formulate a conjecture in the degenerate case | [['we', 'classify', 'up', 'to', 'derived', 'equivalently', 'tiltingcotilting', 'equivalence', 'all', 'nondegenerate', 'gentle', 'twocycle', 'algebras', 'we', 'also', 'give', 'a', 'partial', 'classification', 'and', 'formulate', 'a', 'conjecture', 'in', 'the', 'degenerate', 'case']] | [-0.15913055761268846, 0.05019478010082686, -0.014502580105154603, 0.11968591992087939, -0.08430564222443435, -0.2183758224947033, 0.03702317260171252, 0.3454973243728832, -0.34420165481666726, -0.19133795297670145, 0.12685152935079747, -0.20793297872188743, -0.14225320014412757, 0.14802952224595678, -0.132634472653821... |
708.3756 | Discussion of "Second order topological sensitivity analysis" by J.
Rocha de Faria et al | The article by J. Rocha de Faria et al. under discussion is concerned with
the evaluation of the perturbation undergone by the potential energy of a
domain $\Omega$ (in a 2-D, scalar Laplace equation setting) when a disk
$B_{\epsilon}$ of small radius $\epsilon$ centered at a given location
$\hat{\boldsymbol{x}\in\Om... | physics.class-ph | the article by j rocha de faria et al under discussion is concerned with the evaluation of the perturbation undergone by the potential energy of a domain omega in a 2d scalar laplace equation setting when a disk b_epsilon of small radius epsilon centered at a given location hatboldsymbolxinomega is removed from omega a... | [['the', 'article', 'by', 'j', 'rocha', 'de', 'faria', 'et', 'al', 'under', 'discussion', 'is', 'concerned', 'with', 'the', 'evaluation', 'of', 'the', 'perturbation', 'undergone', 'by', 'the', 'potential', 'energy', 'of', 'a', 'domain', 'omega', 'in', 'a', '2d', 'scalar', 'laplace', 'equation', 'setting', 'when', 'a', ... | [-0.16081880481781102, 0.07264226571027797, -0.05961655931201272, 0.016076914966106415, -0.08894305413478934, -0.10515157053709522, 0.011263440408381738, 0.2864413023134047, -0.24059840309200808, -0.257509230357957, 0.1303190896481586, -0.2917157052886776, -0.11690963320951495, 0.15854566305966322, -0.08850739484639941... |
708.3757 | Interacting Convection Zones | We present results from simulations to examine how the separation between two
convectively unstable layers affect their interaction. We show that two
convectively unstable layers remain connected via the overshooting plumes even
when they are separated by several pressure scale heights.
| astro-ph | we present results from simulations to examine how the separation between two convectively unstable layers affect their interaction we show that two convectively unstable layers remain connected via the overshooting plumes even when they are separated by several pressure scale heights | [['we', 'present', 'results', 'from', 'simulations', 'to', 'examine', 'how', 'the', 'separation', 'between', 'two', 'convectively', 'unstable', 'layers', 'affect', 'their', 'interaction', 'we', 'show', 'that', 'two', 'convectively', 'unstable', 'layers', 'remain', 'connected', 'via', 'the', 'overshooting', 'plumes', 'e... | [-0.1742190386327665, 0.31084540682822104, -0.04604982491582632, 0.12027925393748574, 0.021179173414300128, -0.116576984019314, 0.00822878495517482, 0.4548055967543183, -0.3709859757161722, -0.2896593186277442, 0.11433130096098999, -0.2558910343341711, -0.1395349558442831, 0.19704084997860397, 0.024848790657592983, -0.... |
708.3758 | Numerical Color-Magnitude Diagram Analysis of SDSS Data and Application
to the New Milky Way satellites | We have tested the application to Sloan Digital Sky Survey data of the
software package MATCH, which fits color-magnitude diagrams (CMDs) to estimate
stellar population parameters and distances. These tests on a set of six
globular clusters show that these techniques recover their known properties.
New ways of using ... | astro-ph | we have tested the application to sloan digital sky survey data of the software package match which fits colormagnitude diagrams cmds to estimate stellar population parameters and distances these tests on a set of six globular clusters show that these techniques recover their known properties new ways of using the cmdf... | [['we', 'have', 'tested', 'the', 'application', 'to', 'sloan', 'digital', 'sky', 'survey', 'data', 'of', 'the', 'software', 'package', 'match', 'which', 'fits', 'colormagnitude', 'diagrams', 'cmds', 'to', 'estimate', 'stellar', 'population', 'parameters', 'and', 'distances', 'these', 'tests', 'on', 'a', 'set', 'of', 's... | [-0.025812123916087632, 0.03563573627060476, -0.11271838642035921, 0.11042710255585714, -0.1675039378444328, -0.06426210264261398, 0.08425084815179515, 0.44110350372890633, -0.1866252431047744, -0.39526603410195094, 0.032577116677809194, -0.2853192986221984, -0.0533027065220166, 0.23050024771914146, -0.0772754700479304... |
708.3759 | Roper resonances in chiral quark models | We derive a method to calculate the multi-channel K matrix applicable to a
broad class of models in which mesons linearly couple to the quark core. The
method is used to calculate pion scattering amplitudes in the energy region of
low-lying P11 and P33 resonances. A good agreement with experimental data is
achieved i... | hep-ph | we derive a method to calculate the multichannel k matrix applicable to a broad class of models in which mesons linearly couple to the quark core the method is used to calculate pion scattering amplitudes in the energy region of lowlying p11 and p33 resonances a good agreement with experimental data is achieved if in a... | [['we', 'derive', 'a', 'method', 'to', 'calculate', 'the', 'multichannel', 'k', 'matrix', 'applicable', 'to', 'a', 'broad', 'class', 'of', 'models', 'in', 'which', 'mesons', 'linearly', 'couple', 'to', 'the', 'quark', 'core', 'the', 'method', 'is', 'used', 'to', 'calculate', 'pion', 'scattering', 'amplitudes', 'in', 't... | [-0.09835133621205402, 0.1644352949636502, -0.07927150443707288, 0.11378436923167148, -0.019153256871762264, -0.13759903792720451, 0.06553787881491986, 0.3516757943444943, -0.22194926548477228, -0.22599868110867333, -0.024496460036761994, -0.3248830194857004, -0.06020917169609626, 0.12305429235587012, 0.073185773498112... |
708.376 | Interaction between ionic lattices and superconducting condensates | The interaction of the ionic lattice with the superconducting condensate is
treated in terms of the electrostatic force in superconductors. It is shown
that this force is similar but not identical to the force suggested by the
volume difference of the normal and superconducting states. The BCS theory
shows larger dev... | cond-mat.supr-con cond-mat.str-el | the interaction of the ionic lattice with the superconducting condensate is treated in terms of the electrostatic force in superconductors it is shown that this force is similar but not identical to the force suggested by the volume difference of the normal and superconducting states the bcs theory shows larger deviati... | [['the', 'interaction', 'of', 'the', 'ionic', 'lattice', 'with', 'the', 'superconducting', 'condensate', 'is', 'treated', 'in', 'terms', 'of', 'the', 'electrostatic', 'force', 'in', 'superconductors', 'it', 'is', 'shown', 'that', 'this', 'force', 'is', 'similar', 'but', 'not', 'identical', 'to', 'the', 'force', 'sugges... | [-0.15459693794096396, 0.20553695073520595, -0.09190355671400374, 0.08092277888631956, 0.003905150903896852, -0.13843444176018238, 0.022990653263828292, 0.2931968620216305, -0.21478346366096626, -0.2675513885237954, -0.05419615448283201, -0.3050902426920154, -0.0995214928957549, 0.15523670234040104, 0.00891038657335395... |
708.3761 | Multi-agent systems, Equiprobability, Gamma distributions and other
Geometrical questions | A set of many identical interacting agents obeying a global additive
constraint is considered. Under the hypothesis of equiprobability in the
high-dimensional volume delimited in phase space by the constraint, the
statistical behavior of a generic agent over the ensemble is worked out. The
asymptotic distribution of ... | nlin.CD cond-mat.stat-mech cs.MA physics.soc-ph | a set of many identical interacting agents obeying a global additive constraint is considered under the hypothesis of equiprobability in the highdimensional volume delimited in phase space by the constraint the statistical behavior of a generic agent over the ensemble is worked out the asymptotic distribution of that s... | [['a', 'set', 'of', 'many', 'identical', 'interacting', 'agents', 'obeying', 'a', 'global', 'additive', 'constraint', 'is', 'considered', 'under', 'the', 'hypothesis', 'of', 'equiprobability', 'in', 'the', 'highdimensional', 'volume', 'delimited', 'in', 'phase', 'space', 'by', 'the', 'constraint', 'the', 'statistical',... | [-0.1538651445279679, 0.09248142647406747, -0.14545442134903003, 0.087990049073743, -0.024663163203826194, -0.12340986968508812, 0.0442793410852231, 0.3122698711832204, -0.2554019966553296, -0.27313082941597505, 0.09768688177146326, -0.25127759832207874, -0.14067840032900372, 0.18313946756434135, -0.07489228321700006, ... |
708.3762 | Where is the pseudoscalar glueball ? | The pseudoscalar mesons with the masses higher than 1 GeV are assumed to
belong to the meson decuplet including the glueball as the basis state
supplementing the standard $SU(3)_F$ nonet of light $q\bar{q}$ states
$(u,d,s)$. The decuplet is investigated by means of an algebraic approach based
on hypothesis of vanishi... | hep-ph | the pseudoscalar mesons with the masses higher than 1 gev are assumed to belong to the meson decuplet including the glueball as the basis state supplementing the standard su3_f nonet of light qbarq states uds the decuplet is investigated by means of an algebraic approach based on hypothesis of vanishing the exotic su3_... | [['the', 'pseudoscalar', 'mesons', 'with', 'the', 'masses', 'higher', 'than', '1', 'gev', 'are', 'assumed', 'to', 'belong', 'to', 'the', 'meson', 'decuplet', 'including', 'the', 'glueball', 'as', 'the', 'basis', 'state', 'supplementing', 'the', 'standard', 'su3_f', 'nonet', 'of', 'light', 'qbarq', 'states', 'uds', 'the... | [-0.09573235555948599, 0.27774699864803737, -0.059247179166893905, 0.14766853789861323, -0.047112924812515215, -0.12160654930090628, 0.06322522782816638, 0.30877134429840564, -0.1649821192775037, -0.24731010773933862, -0.032615827102473335, -0.3446488741535655, -0.01478146096408252, 0.07740836957116737, 0.0972469215648... |
708.3763 | Rate of Escape on Free Products | Suppose we are given the free product $V$ of a finite family of finite or
countable sets $(V_i)_{i\in\mathcal{I}}$ and probability measures on each
$V_i$, which govern random walks on it. We consider a transient random walk on
the free product arising naturally from the random walks on the $V_i$. We prove
the existen... | math.PR | suppose we are given the free product v of a finite family of finite or countable sets v_i_iinmathcali and probability measures on each v_i which govern random walks on it we consider a transient random walk on the free product arising naturally from the random walks on the v_i we prove the existence of the rate of esc... | [['suppose', 'we', 'are', 'given', 'the', 'free', 'product', 'v', 'of', 'a', 'finite', 'family', 'of', 'finite', 'or', 'countable', 'sets', 'v_i_iinmathcali', 'and', 'probability', 'measures', 'on', 'each', 'v_i', 'which', 'govern', 'random', 'walks', 'on', 'it', 'we', 'consider', 'a', 'transient', 'random', 'walk', 'o... | [-0.12741974889006663, 0.20166814397334268, -0.04886249334698445, 0.033470035834532036, -0.027007471243115633, -0.14370238593730486, 0.06157418462741924, 0.40094365786613995, -0.3048112959551968, -0.17009889675659667, 0.11197927945146435, -0.3067216005764509, -0.11318540523367884, 0.18528019706779894, -0.03753756648266... |
708.3764 | A Radio Resource Management strategy for downlink cooperation in
distributed networks | This paper has been withdrawn by the author
| cs.IT math.IT | this paper has been withdrawn by the author | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'author']] | [-0.11762839742004871, -0.04127746832091361, -0.17016396392136812, -0.1582642109860899, -0.18072871817275882, -0.04020218155346811, -0.09601712167204823, 0.33764172717928886, -0.2455208501778543, -0.3865965995937586, 0.12438089866191149, -0.3554150704294443, -0.17133164615370333, -0.03124168887734413, -0.36054937075823... |
708.3765 | The effects of lepton KK modes on the lepton electric dipole moments in
the Randall Sundrum scenario | We study the charged lepton electric dipole moments in the Randall Sundrum
model where the leptons and the gauge fields are accessible to the extra
dimension. We observe that the electron (muon; tau) electric dipole moment
reaches to the value of the order of 10^{-26} e-cm (10^{-20} e-cm; 10^{-20}
e-cm) with the incl... | hep-ph | we study the charged lepton electric dipole moments in the randall sundrum model where the leptons and the gauge fields are accessible to the extra dimension we observe that the electron muon tau electric dipole moment reaches to the value of the order of 1026 ecm 1020 ecm 1020 ecm with the inclusion of the lepton kk m... | [['we', 'study', 'the', 'charged', 'lepton', 'electric', 'dipole', 'moments', 'in', 'the', 'randall', 'sundrum', 'model', 'where', 'the', 'leptons', 'and', 'the', 'gauge', 'fields', 'are', 'accessible', 'to', 'the', 'extra', 'dimension', 'we', 'observe', 'that', 'the', 'electron', 'muon', 'tau', 'electric', 'dipole', '... | [-0.10873023505274464, 0.3043336983577445, 0.07857944320180807, 0.11173786425256524, -0.0360551787508202, -0.08589371936074619, -0.007940474627659944, 0.29983813668890247, -0.17622844833109913, -0.32311595488211203, -0.04347243826186027, -0.31613082721315583, 0.04250536586061634, 0.05213616251672522, 0.1100062334845805... |
708.3766 | Rate of Escape on the Lamplighter Tree | Suppose we are given a homogeneous tree $\mathcal{T}_q$ of degree $q\geq 3$,
where at each vertex sits a lamp, which can be switched on or off. This
structure can be described by the wreath product $(\mathbb{Z}/2)\wr \Gamma$,
where $\Gamma=\ast_{i=1}^q \mathbb{Z}/2$ is the free product group of $q$
factors $\mathbb{Z... | math.PR | suppose we are given a homogeneous tree mathcalt_q of degree qgeq 3 where at each vertex sits a lamp which can be switched on or off this structure can be described by the wreath product mathbbz2wr gamma where gammaast_i1q mathbbz2 is the free product group of q factors mathbbz2 we consider a transient random walk on a... | [['suppose', 'we', 'are', 'given', 'a', 'homogeneous', 'tree', 'mathcalt_q', 'of', 'degree', 'qgeq', '3', 'where', 'at', 'each', 'vertex', 'sits', 'a', 'lamp', 'which', 'can', 'be', 'switched', 'on', 'or', 'off', 'this', 'structure', 'can', 'be', 'described', 'by', 'the', 'wreath', 'product', 'mathbbz2wr', 'gamma', 'wh... | [-0.1350074011242277, 0.23090814096246695, -0.0779598064958876, 0.013646245074490908, -0.07714052481555142, -0.17266104002158308, 0.11332472733243606, 0.4055675096528301, -0.30351232910572096, -0.19846811716249863, 0.13469139612713005, -0.2785772197165115, -0.0914157728128525, 0.15852906620725557, -0.03675834798838857,... |
708.3767 | Acceleration of Lamplighter Random Walks | Suppose we are given an infinite, finitely generated group $G$ and a
transient random walk on the wreath product $(\mathbb{Z}/ 2\mathbb{Z})\wr G$,
such that its projection on $G$ is transient and has finite first moment. This
random walk can be interpreted as a lamplighter random walk on $G$. Our aim is
to show that ... | math.PR | suppose we are given an infinite finitely generated group g and a transient random walk on the wreath product mathbbz 2mathbbzwr g such that its projection on g is transient and has finite first moment this random walk can be interpreted as a lamplighter random walk on g our aim is to show that the random walk on the w... | [['suppose', 'we', 'are', 'given', 'an', 'infinite', 'finitely', 'generated', 'group', 'g', 'and', 'a', 'transient', 'random', 'walk', 'on', 'the', 'wreath', 'product', 'mathbbz', '2mathbbzwr', 'g', 'such', 'that', 'its', 'projection', 'on', 'g', 'is', 'transient', 'and', 'has', 'finite', 'first', 'moment', 'this', 'ra... | [-0.1572564748831366, 0.19474767881165905, -0.07688182737011977, 0.022451748081475376, -0.10006821362634863, -0.13133984516427769, 0.048442185563470685, 0.43655728441246644, -0.32467702905291584, -0.15522277381174585, 0.1409522327850005, -0.3055061985685573, -0.11096797383019352, 0.19336746780701528, -0.100940317449318... |
708.3768 | Scenario of inflationary cosmology from the phenomenological $\Lambda$
models | Choosing the three phenomenological models of the dynamical cosmological term
$\Lambda$, viz., $\Lambda \sim (\dot a/a)^2$, $\Lambda \sim {\ddot a/a}$ and
$\Lambda \sim \rho$ where $a$ is the cosmic scale factor, it has been shown by
the method of numerical analysis that the three models are equivalent for the
flat U... | gr-qc | choosing the three phenomenological models of the dynamical cosmological term lambda viz lambda sim dot aa2 lambda sim ddot aa and lambda sim rho where a is the cosmic scale factor it has been shown by the method of numerical analysis that the three models are equivalent for the flat universe k0 the evolution plots for... | [['choosing', 'the', 'three', 'phenomenological', 'models', 'of', 'the', 'dynamical', 'cosmological', 'term', 'lambda', 'viz', 'lambda', 'sim', 'dot', 'aa2', 'lambda', 'sim', 'ddot', 'aa', 'and', 'lambda', 'sim', 'rho', 'where', 'a', 'is', 'the', 'cosmic', 'scale', 'factor', 'it', 'has', 'been', 'shown', 'by', 'the', '... | [-0.11908648721753745, 0.1441517011790546, -0.11531880421602388, 0.08424119469493666, -0.029393370152863953, -0.1640141831888558, -0.028612164108409097, 0.339064617199612, -0.23914853153155022, -0.29186979893321346, 0.06334301587386229, -0.3136904809009476, -0.03388785342589866, 0.16611155732198782, 0.10088126479945693... |
708.3769 | Ultraviolet light emission from Si in a scanning tunneling microscope | Ultraviolet and visible radiation is observed from the contacts of a scanning
tunneling microscope with Si(100) and (111) wafers. This luminescence relies on
the presence of hot electrons in silicon, which are supplied, at positive bias
on n- and p-type samples, through the injection from the tip, or, at negative
bia... | cond-mat.mtrl-sci | ultraviolet and visible radiation is observed from the contacts of a scanning tunneling microscope with si100 and 111 wafers this luminescence relies on the presence of hot electrons in silicon which are supplied at positive bias on n and ptype samples through the injection from the tip or at negative bias on psamples ... | [['ultraviolet', 'and', 'visible', 'radiation', 'is', 'observed', 'from', 'the', 'contacts', 'of', 'a', 'scanning', 'tunneling', 'microscope', 'with', 'si100', 'and', '111', 'wafers', 'this', 'luminescence', 'relies', 'on', 'the', 'presence', 'of', 'hot', 'electrons', 'in', 'silicon', 'which', 'are', 'supplied', 'at', ... | [-0.06541369417898876, 0.19101875736161547, -0.022278034315054672, 0.008280561998659787, 0.025497691792457602, -0.17301280390427903, 0.11482921979920722, 0.4190927913715673, -0.23957084951012633, -0.369304274577041, 0.001980786441911965, -0.40887642608479013, -0.05306163181139286, 0.20540174228399125, 0.026413625666633... |
708.377 | Squark and gaugino hadroproduction and decays in non-minimal flavour
violating supersymmetry | We implement non-minimal flavour violation (NMFV) in the MSSM at low scale.
In this framework, we propose benchmark points for the mSUGRA scenario
including non-minimal flavour violation by evaluating a number of experimental
low-energy, electroweak precision and cosmological constraints. We finally
discuss phenomeno... | hep-ph | we implement nonminimal flavour violation nmfv in the mssm at low scale in this framework we propose benchmark points for the msugra scenario including nonminimal flavour violation by evaluating a number of experimental lowenergy electroweak precision and cosmological constraints we finally discuss phenomenological asp... | [['we', 'implement', 'nonminimal', 'flavour', 'violation', 'nmfv', 'in', 'the', 'mssm', 'at', 'low', 'scale', 'in', 'this', 'framework', 'we', 'propose', 'benchmark', 'points', 'for', 'the', 'msugra', 'scenario', 'including', 'nonminimal', 'flavour', 'violation', 'by', 'evaluating', 'a', 'number', 'of', 'experimental',... | [-0.14086066345713796, 0.18197604533403167, -0.00508954963232908, 0.18252288528518484, -0.08802942912064729, -0.20156658649636758, 0.08327982809379815, 0.28321502458245035, -0.14752399185228915, -0.3297106499177596, 0.011399856816592908, -0.254260138719387, -0.03067444905727392, 0.12945110523807152, 0.03907697932750341... |
708.3771 | Atomic structure analysis of nanocrystalline Boehmite AlO(OH) | Nanocrystalline n-AlO(OH) (Disperal P2(R) of Sasol) was investigated by means
of the atomic pair distribution function (PDF). The PDF is derived from powder
diffraction data, an ideally resolved PDF is obtained from a synchrotron source
which provides a large maximal scattering vector length Qmax > 300 nm-1. Here,
ho... | cond-mat.mtrl-sci | nanocrystalline nalooh disperal p2r of sasol was investigated by means of the atomic pair distribution function pdf the pdf is derived from powder diffraction data an ideally resolved pdf is obtained from a synchrotron source which provides a large maximal scattering vector length qmax 300 nm1 here however we were able... | [['nanocrystalline', 'nalooh', 'disperal', 'p2r', 'of', 'sasol', 'was', 'investigated', 'by', 'means', 'of', 'the', 'atomic', 'pair', 'distribution', 'function', 'pdf', 'the', 'pdf', 'is', 'derived', 'from', 'powder', 'diffraction', 'data', 'an', 'ideally', 'resolved', 'pdf', 'is', 'obtained', 'from', 'a', 'synchrotron... | [-0.051084846651572785, 0.15846308151459346, -0.0731071794059041, 0.02600270448263388, -0.009949685194865302, -0.08522342854595018, 0.053168406558417994, 0.4093040715209966, -0.27274928251173086, -0.3289342272274066, 0.0660065760427198, -0.34186391380268993, -0.053281192188584355, 0.16949028321332027, 0.015830563465241... |
708.3772 | Discretely Holomorphic Parafermions in Lattice Z(N) Models | We construct lattice parafermions - local products of order and disorder
operators - in nearest-neighbor Z(N) models on regular isotropic planar
lattices, and show that they are discretely holomorphic, that is they satisfy
discrete Cauchy-Riemann equations, precisely at the critical
Fateev-Zamolodchikov (FZ) integrab... | math-ph cond-mat.stat-mech hep-th math.MP | we construct lattice parafermions local products of order and disorder operators in nearestneighbor zn models on regular isotropic planar lattices and show that they are discretely holomorphic that is they satisfy discrete cauchyriemann equations precisely at the critical fateevzamolodchikov fz integrable points we gen... | [['we', 'construct', 'lattice', 'parafermions', 'local', 'products', 'of', 'order', 'and', 'disorder', 'operators', 'in', 'nearestneighbor', 'zn', 'models', 'on', 'regular', 'isotropic', 'planar', 'lattices', 'and', 'show', 'that', 'they', 'are', 'discretely', 'holomorphic', 'that', 'is', 'they', 'satisfy', 'discrete',... | [-0.14812071130367085, 0.15439446073114163, -0.012473116507421115, 0.10097893891811725, -0.08465992117167584, -0.13859410470883762, -0.018378786254851592, 0.4200079618110543, -0.27291488205747944, -0.16695464938169435, 0.11702474683545352, -0.30980028630722134, -0.17037025388507615, 0.16095388155164464, 0.0210721614238... |
708.3773 | Exact density matrix of the Gutzwiller wave function: II. Minority spin
component | The density matrix, i.e. the Fourier transform of the momentum distribution,
is obtained analytically for all magnetization of the Gutzwiller wave function
in one dimension with exclusion of double occupancy per site. The present
result complements the previous analytic derivation of the density matrix for
the majori... | cond-mat.str-el cond-mat.stat-mech | the density matrix ie the fourier transform of the momentum distribution is obtained analytically for all magnetization of the gutzwiller wave function in one dimension with exclusion of double occupancy per site the present result complements the previous analytic derivation of the density matrix for the majority spin... | [['the', 'density', 'matrix', 'ie', 'the', 'fourier', 'transform', 'of', 'the', 'momentum', 'distribution', 'is', 'obtained', 'analytically', 'for', 'all', 'magnetization', 'of', 'the', 'gutzwiller', 'wave', 'function', 'in', 'one', 'dimension', 'with', 'exclusion', 'of', 'double', 'occupancy', 'per', 'site', 'the', 'p... | [-0.13836345379034157, 0.13690365002264637, -0.07880060439764043, 0.05943543115043847, -0.012545380660073732, -0.07803812706236832, 0.040544403138289435, 0.33983193384759, -0.2376484026878896, -0.23638272518016532, 0.037431715492340985, -0.3138732865759993, -0.07969271377465735, 0.15776398859590227, 0.07506262040738369... |
708.3774 | Fisher Lecture: Dimension Reduction in Regression | Beginning with a discussion of R. A. Fisher's early written remarks that
relate to dimension reduction, this article revisits principal components as a
reductive method in regression, develops several model-based extensions and
ends with descriptions of general approaches to model-based and model-free
dimension reduc... | stat.ME | beginning with a discussion of r a fishers early written remarks that relate to dimension reduction this article revisits principal components as a reductive method in regression develops several modelbased extensions and ends with descriptions of general approaches to modelbased and modelfree dimension reduction in re... | [['beginning', 'with', 'a', 'discussion', 'of', 'r', 'a', 'fishers', 'early', 'written', 'remarks', 'that', 'relate', 'to', 'dimension', 'reduction', 'this', 'article', 'revisits', 'principal', 'components', 'as', 'a', 'reductive', 'method', 'in', 'regression', 'develops', 'several', 'modelbased', 'extensions', 'and', ... | [-0.06694308702340897, 0.025793144983403824, -0.12562932995805406, 0.0742791382376762, -0.13374245045158792, -0.18475491111440695, 0.010897193369729554, 0.342032564313644, -0.23967100096976054, -0.23896330805385815, 0.1478914251414073, -0.24175897189142073, -0.18338662579874782, 0.21489794682711363, -0.1346382319215027... |
708.3775 | Decoherence of encoded quantum registers | In order to eliminate disturbing effects of decoherence, encoding of quantum
information in decoherence-free subspaces has been suggested. We analyze the
benefits of this concept for a quantum register that is realized in a spin
chain in contact with a common bosonic bath. Within a dissipation-less model we
provide e... | quant-ph | in order to eliminate disturbing effects of decoherence encoding of quantum information in decoherencefree subspaces has been suggested we analyze the benefits of this concept for a quantum register that is realized in a spin chain in contact with a common bosonic bath within a dissipationless model we provide explicit... | [['in', 'order', 'to', 'eliminate', 'disturbing', 'effects', 'of', 'decoherence', 'encoding', 'of', 'quantum', 'information', 'in', 'decoherencefree', 'subspaces', 'has', 'been', 'suggested', 'we', 'analyze', 'the', 'benefits', 'of', 'this', 'concept', 'for', 'a', 'quantum', 'register', 'that', 'is', 'realized', 'in', ... | [-0.18089082856456956, 0.14669007286066552, -0.08422248277740625, 0.06305265155100784, -0.026749446407541053, -0.1968374375266011, 0.07038199137775349, 0.34300375187938864, -0.22565717120691167, -0.22631349054153088, 0.030142971719675636, -0.25833962688996615, -0.12212701773198394, 0.1997971857154089, -0.03735370876860... |
708.3776 | Comment: Fisher Lecture: Dimension Reduction in Regression | Comment: Fisher Lecture: Dimension Reduction in Regression [arXiv:0708.3774]
| stat.ME | comment fisher lecture dimension reduction in regression arxiv07083774 | [['comment', 'fisher', 'lecture', 'dimension', 'reduction', 'in', 'regression', 'arxiv07083774']] | [-0.0180543374735862, 0.020581837045028806, -0.09514877054607496, 0.12449243548326194, -0.1400118555757217, -0.3189979321323335, -0.019820759305730462, 0.14219930957187898, -0.12936251517385244, -0.18627265794202685, 0.21493641687266063, -0.3917643390595913, -0.33059780672192574, 0.0719880061224103, -0.2476060227490961... |
708.3777 | Comment: Fisher Lecture: Dimension Reduction in Regression | Comment: Fisher Lecture: Dimension Reduction in Regression [arXiv:0708.3774]
| stat.ME | comment fisher lecture dimension reduction in regression arxiv07083774 | [['comment', 'fisher', 'lecture', 'dimension', 'reduction', 'in', 'regression', 'arxiv07083774']] | [-0.0180543374735862, 0.020581837045028806, -0.09514877054607496, 0.12449243548326194, -0.1400118555757217, -0.3189979321323335, -0.019820759305730462, 0.14219930957187898, -0.12936251517385244, -0.18627265794202685, 0.21493641687266063, -0.3917643390595913, -0.33059780672192574, 0.0719880061224103, -0.2476060227490961... |
708.3778 | Symplectic geometries on supermanifolds | Extension of symplectic geometry on manifolds to the supersymmetric case is
considered. In the even case it leads to the even symplectic geometry (or,
equivalently, to the geometry on supermanifolds endowed with a non-degenerate
Poisson bracket) or to the geometry on an even Fedosov supermanifolds. It is
proven that ... | hep-th | extension of symplectic geometry on manifolds to the supersymmetric case is considered in the even case it leads to the even symplectic geometry or equivalently to the geometry on supermanifolds endowed with a nondegenerate poisson bracket or to the geometry on an even fedosov supermanifolds it is proven that in the od... | [['extension', 'of', 'symplectic', 'geometry', 'on', 'manifolds', 'to', 'the', 'supersymmetric', 'case', 'is', 'considered', 'in', 'the', 'even', 'case', 'it', 'leads', 'to', 'the', 'even', 'symplectic', 'geometry', 'or', 'equivalently', 'to', 'the', 'geometry', 'on', 'supermanifolds', 'endowed', 'with', 'a', 'nondegen... | [-0.1955765333492309, 0.07413428695035691, -0.0598704454721883, 0.1535618824796984, -0.11721108860801906, -0.19038132423884235, -0.11099199894088088, 0.3660753514850512, -0.2586387414019555, -0.24801337398821488, 0.09247160835657268, -0.208733607432805, -0.19928640741854906, 0.21107721512089483, -0.15396264934388454, -... |
708.3779 | Comment: Fisher Lecture: Dimension Reduction in Regression | Comment: Fisher Lecture: Dimension Reduction in Regression [arXiv:0708.3774]
| stat.ME | comment fisher lecture dimension reduction in regression arxiv07083774 | [['comment', 'fisher', 'lecture', 'dimension', 'reduction', 'in', 'regression', 'arxiv07083774']] | [-0.0180543374735862, 0.020581837045028806, -0.09514877054607496, 0.12449243548326194, -0.1400118555757217, -0.3189979321323335, -0.019820759305730462, 0.14219930957187898, -0.12936251517385244, -0.18627265794202685, 0.21493641687266063, -0.3917643390595913, -0.33059780672192574, 0.0719880061224103, -0.2476060227490961... |
708.378 | The optical emission line spectrum of Mark 110 | We analyse in detail the rich emission line spectrum of Mark 110 to determine
the physical conditions in the nucleus of this object, a peculiar NLS1 without
any detectable Fe II emission associated with the broad line region and with a
$\lambda5007/H\beta$ line ratio unusually large for a NLS1. We use 24 spectra
obta... | astro-ph | we analyse in detail the rich emission line spectrum of mark 110 to determine the physical conditions in the nucleus of this object a peculiar nls1 without any detectable fe ii emission associated with the broad line region and with a lambda5007hbeta line ratio unusually large for a nls1 we use 24 spectra obtained with... | [['we', 'analyse', 'in', 'detail', 'the', 'rich', 'emission', 'line', 'spectrum', 'of', 'mark', '110', 'to', 'determine', 'the', 'physical', 'conditions', 'in', 'the', 'nucleus', 'of', 'this', 'object', 'a', 'peculiar', 'nls1', 'without', 'any', 'detectable', 'fe', 'ii', 'emission', 'associated', 'with', 'the', 'broad'... | [-0.08520598145573313, 0.07810899221129675, 0.020596446807857584, 0.062397372573639566, -0.05576454166353482, -0.1665847292577064, 0.035413281523871944, 0.4860372920851401, -0.12258005283437058, -0.3593031091493417, 0.0713343631140277, -0.28298510934221127, 0.03687763435745744, 0.17102905982326655, 0.01747297751621847,... |
708.3781 | Rejoinder: Fisher Lecture: Dimension Reduction in Regression | Rejoinder: Fisher Lecture: Dimension Reduction in Regression
[arXiv:0708.3774]
| stat.ME | rejoinder fisher lecture dimension reduction in regression arxiv07083774 | [['rejoinder', 'fisher', 'lecture', 'dimension', 'reduction', 'in', 'regression', 'arxiv07083774']] | [0.08107881131581962, -0.04717068071477115, -0.1274330923333764, 0.13871754962019622, -0.11098479590145871, -0.2860194589011371, -0.040378311881795526, 0.16192143692751415, -0.1607476221397519, -0.20769146410748363, 0.19392229737422895, -0.4410094730556011, -0.32342861592769623, 0.04440533462911844, -0.2855026838369667... |
708.3782 | QCD-resummation and non-minimal flavour-violation for supersymmetric
particle production at hadron colliders | Cross sections for supersymmetric particles production at hadron colliders
have been extensively studied in the past at leading order and also at
next-to-leading order of perturbative QCD. The radiative corrections include
large logarithms which have to be resummed to all orders in the strong coupling
constant in ord... | hep-ph | cross sections for supersymmetric particles production at hadron colliders have been extensively studied in the past at leading order and also at nexttoleading order of perturbative qcd the radiative corrections include large logarithms which have to be resummed to all orders in the strong coupling constant in order to... | [['cross', 'sections', 'for', 'supersymmetric', 'particles', 'production', 'at', 'hadron', 'colliders', 'have', 'been', 'extensively', 'studied', 'in', 'the', 'past', 'at', 'leading', 'order', 'and', 'also', 'at', 'nexttoleading', 'order', 'of', 'perturbative', 'qcd', 'the', 'radiative', 'corrections', 'include', 'larg... | [-0.06991465014124394, 0.19948996151885334, -0.04671222707564187, 0.1725036606164034, -0.06961101714855517, -0.1396174519712694, -0.0031666330837222907, 0.32268189855868806, -0.1550003027495102, -0.2794700866907765, 0.021117876232755458, -0.31081894370024354, 0.011611837704824109, 0.13102715608130103, 0.069432850283535... |
708.3783 | Resonantly damped surface and body MHD waves in a solar coronal slab
with oblique propagation | The theory of magnetohydrodynamic (MHD) waves in solar coronal slabs in a
zero-$\beta$ configuration and for parallel propagation of waves does not allow
the existence of surface waves. When oblique propagation of perturbations is
considered both surface and body waves are able to propagate. When the
perpendicular wa... | astro-ph | the theory of magnetohydrodynamic mhd waves in solar coronal slabs in a zerobeta configuration and for parallel propagation of waves does not allow the existence of surface waves when oblique propagation of perturbations is considered both surface and body waves are able to propagate when the perpendicular wave number ... | [['the', 'theory', 'of', 'magnetohydrodynamic', 'mhd', 'waves', 'in', 'solar', 'coronal', 'slabs', 'in', 'a', 'zerobeta', 'configuration', 'and', 'for', 'parallel', 'propagation', 'of', 'waves', 'does', 'not', 'allow', 'the', 'existence', 'of', 'surface', 'waves', 'when', 'oblique', 'propagation', 'of', 'perturbations'... | [-0.1973799341931885, 0.20836349002733504, -0.028450670220173786, 0.06811018222504282, -0.10145818524271843, -0.0872056274033705, -0.035402433533369956, 0.35124441274050355, -0.2457272782854304, -0.2498417051738479, 0.11876275330112127, -0.2612410667824788, -0.12368964267206257, 0.21173517066695174, 0.03658634036158522... |
708.3784 | Localization of quantum wave packets | We study the semiclassical propagation of squeezed Gau{\ss}ian states. We do
so by considering the propagation theorem introduced by Combescure and Robert
\cite{CR97} approximating the evolution generated by the Weyl-quantization of
symbols $H$. We examine the particular case when the Hessian
$H^{\prime\prime}(X_{t})... | math-ph math.MP | we study the semiclassical propagation of squeezed gaussian states we do so by considering the propagation theorem introduced by combescure and robert citecr97 approximating the evolution generated by the weylquantization of symbols h we examine the particular case when the hessian hprimeprimex_t evaluated at the corre... | [['we', 'study', 'the', 'semiclassical', 'propagation', 'of', 'squeezed', 'gaussian', 'states', 'we', 'do', 'so', 'by', 'considering', 'the', 'propagation', 'theorem', 'introduced', 'by', 'combescure', 'and', 'robert', 'citecr97', 'approximating', 'the', 'evolution', 'generated', 'by', 'the', 'weylquantization', 'of', ... | [-0.16651134102409013, 0.15597039186754091, -0.07421093596114724, 0.0881438052112406, -0.02046837722536269, -0.08519244828253739, 0.009892026903415637, 0.3539364460301547, -0.2974342939343827, -0.21235283285818132, 0.1120856646660038, -0.23430628703968706, -0.16405816410845223, 0.18616701903067961, -0.04957696233976109... |
708.3785 | Perfect Teleportation, Quantum state sharing and Superdense Coding
through a Genuinely Entangled Five-qubit State | We investigate the usefulness of a recently introduced five qubit state by
Brown $\it et al. \normalfont$ \cite{Brown} for quantum teleportation, quantum
state sharing and superdense coding. It is shown that this five-qubit state can
be utilized for perfect teleportation of arbitrary single and two qubit
systems. We ... | quant-ph | we investigate the usefulness of a recently introduced five qubit state by brown it et al normalfont citebrown for quantum teleportation quantum state sharing and superdense coding it is shown that this fivequbit state can be utilized for perfect teleportation of arbitrary single and two qubit systems we devise various... | [['we', 'investigate', 'the', 'usefulness', 'of', 'a', 'recently', 'introduced', 'five', 'qubit', 'state', 'by', 'brown', 'it', 'et', 'al', 'normalfont', 'citebrown', 'for', 'quantum', 'teleportation', 'quantum', 'state', 'sharing', 'and', 'superdense', 'coding', 'it', 'is', 'shown', 'that', 'this', 'fivequbit', 'state... | [-0.1381158823037128, 0.2045465685489992, -0.0950830386363362, 0.02473515412941771, 0.027673788233905247, -0.2971316097255208, 0.07099514973202818, 0.370906420385367, -0.2646238510643965, -0.3023630698456576, 0.0731933307307037, -0.21147431728283042, -0.12250211673396591, 0.216161222115012, -0.08349279440743358, 0.1458... |
708.3786 | Temperature and Polarization CMB Maps from Primordial non-Gaussianities
of the Local Type | The forthcoming Planck experiment will provide high sensitivity polarization
measurements that will allow us to further tighten the f_NL bounds from the
temperature data. Monte Carlo simulations of non-Gaussian CMB maps have been
used as a fundamental tool to characterize non-Gaussian signatures in the data,
as they ... | astro-ph | the forthcoming planck experiment will provide high sensitivity polarization measurements that will allow us to further tighten the f_nl bounds from the temperature data monte carlo simulations of nongaussian cmb maps have been used as a fundamental tool to characterize nongaussian signatures in the data as they allow ... | [['the', 'forthcoming', 'planck', 'experiment', 'will', 'provide', 'high', 'sensitivity', 'polarization', 'measurements', 'that', 'will', 'allow', 'us', 'to', 'further', 'tighten', 'the', 'f_nl', 'bounds', 'from', 'the', 'temperature', 'data', 'monte', 'carlo', 'simulations', 'of', 'nongaussian', 'cmb', 'maps', 'have',... | [-0.055664668770639296, 0.05960426217301614, -0.1277546135510211, 0.1064485836719402, -0.07414191234297032, -0.09769943563644189, 0.028533458313395783, 0.35592718423812403, -0.21756173310740318, -0.3374596778176155, 0.10061570941763193, -0.29268419179464866, -0.10631384666184665, 0.2539102586464641, -0.0114336560373423... |
708.3787 | Black-Hole Mass and Growth Rate at High Redshift | We present new H and K bands spectroscopy of 15 high luminosity active
galactic nuclei (AGNs) at redshifts 2.3-3.4 obtained on Gemini South. We
combined the data with spectra of additional 29 high-luminosity sources to
obtain a sample with 10^{45.2}<\lambda L_{\lambda}(5100A)<10^{47.3} ergs/sec
and black hole (BH) ma... | astro-ph | we present new h and k bands spectroscopy of 15 high luminosity active galactic nuclei agns at redshifts 2334 obtained on gemini south we combined the data with spectra of additional 29 highluminosity sources to obtain a sample with 10452lambda l_lambda5100a10473 ergssec and black hole bh mass range using reverberation... | [['we', 'present', 'new', 'h', 'and', 'k', 'bands', 'spectroscopy', 'of', '15', 'high', 'luminosity', 'active', 'galactic', 'nuclei', 'agns', 'at', 'redshifts', '2334', 'obtained', 'on', 'gemini', 'south', 'we', 'combined', 'the', 'data', 'with', 'spectra', 'of', 'additional', '29', 'highluminosity', 'sources', 'to', '... | [-0.024409491731897718, 0.08602983080826988, -0.06591307941671228, 0.14060583453038303, -0.06964455913203423, -0.11241377079139513, 0.07692049110222805, 0.4535374197285568, -0.1139233888403607, -0.3604308701624221, 0.07530577197909391, -0.34584050882463724, 0.010326381980841935, 0.24703493006673646, -0.0317313523326465... |
708.3788 | Dimensional Reduction of Conformal Tensors and Einstein-Weyl Spaces | Conformal Weyl and Cotton tensors are dimensionally reduced by a Kaluza-Klein
procedure. Explicit formulas are given for reducing from four and three
dimensions to three and two dimensions, respectively. When the higher
dimensional conformal tensor vanishes because the space is conformallly flat,
the lower-dimensiona... | math-ph gr-qc hep-th math.MP | conformal weyl and cotton tensors are dimensionally reduced by a kaluzaklein procedure explicit formulas are given for reducing from four and three dimensions to three and two dimensions respectively when the higher dimensional conformal tensor vanishes because the space is conformallly flat the lowerdimensional kaluza... | [['conformal', 'weyl', 'and', 'cotton', 'tensors', 'are', 'dimensionally', 'reduced', 'by', 'a', 'kaluzaklein', 'procedure', 'explicit', 'formulas', 'are', 'given', 'for', 'reducing', 'from', 'four', 'and', 'three', 'dimensions', 'to', 'three', 'and', 'two', 'dimensions', 'respectively', 'when', 'the', 'higher', 'dimen... | [-0.13748560154870634, 0.21759671856078408, 0.040702116825888236, 0.05165723571741593, -0.0964613653298828, -0.19169956658245815, -0.1356807189032195, 0.2822163327476911, -0.13860619816208078, -0.23179593547660438, 0.13606606478307157, -0.30267916300574377, -0.19093479665987675, 0.1378654925633342, 0.02469939707835663,... |
708.3789 | Efficient qubit detection using alkali earth metal ions and a double
STIRAP process | We present a scheme for robust and efficient projection measurement of a
qubit consisting of the two magnetic sublevels in the electronic ground state
of alkali earth metal ions. The scheme is based on two stimulated Raman
adiabatic passages (STIRAP) involving four partially coherent laser fields. We
show how the eff... | quant-ph | we present a scheme for robust and efficient projection measurement of a qubit consisting of the two magnetic sublevels in the electronic ground state of alkali earth metal ions the scheme is based on two stimulated raman adiabatic passages stirap involving four partially coherent laser fields we show how the efficienc... | [['we', 'present', 'a', 'scheme', 'for', 'robust', 'and', 'efficient', 'projection', 'measurement', 'of', 'a', 'qubit', 'consisting', 'of', 'the', 'two', 'magnetic', 'sublevels', 'in', 'the', 'electronic', 'ground', 'state', 'of', 'alkali', 'earth', 'metal', 'ions', 'the', 'scheme', 'is', 'based', 'on', 'two', 'stimula... | [-0.16256612149142735, 0.28940492052886935, 0.00048553256468998417, 0.004345130139168956, 0.022661397982439078, -0.1806205207217686, 0.10576326335541199, 0.5323597523509651, -0.2198576722923364, -0.23548441360125671, -0.04226808321215464, -0.22488307351611453, -0.016681782668456435, 0.28919710016280814, 0.0530695509027... |
708.379 | Singlet fermion dark matter and electroweak baryogenesis with radiative
neutrino mass | The model of radiative neutrino mass with dark matter proposed by one of us
is extended to include a real singlet scalar field. There are then two
important new consequences. One is the realistic possibility of having the
lightest neutral singlet fermion (instead of the lightest neutral component of
the dark scalar d... | hep-ph | the model of radiative neutrino mass with dark matter proposed by one of us is extended to include a real singlet scalar field there are then two important new consequences one is the realistic possibility of having the lightest neutral singlet fermion instead of the lightest neutral component of the dark scalar double... | [['the', 'model', 'of', 'radiative', 'neutrino', 'mass', 'with', 'dark', 'matter', 'proposed', 'by', 'one', 'of', 'us', 'is', 'extended', 'to', 'include', 'a', 'real', 'singlet', 'scalar', 'field', 'there', 'are', 'then', 'two', 'important', 'new', 'consequences', 'one', 'is', 'the', 'realistic', 'possibility', 'of', '... | [-0.08904619253455447, 0.24246548609031984, -0.05353545047677098, 0.1903123465495017, -0.11071278102313861, -0.19867786276751223, -0.055404261232186586, 0.27571726536067825, -0.17055338822329083, -0.33776379716940796, -0.003820717722798387, -0.2524380424561409, -0.009981269781024028, 0.09704604688196038, 0.111248305521... |
708.3791 | Critical phenomena in a highly constrained classical spin system: Neel
ordering from the Coulomb phase | Many classical, geometrically frustrated antiferromagnets have
macroscopically degenerate ground states. In a class of three-dimensional
systems, the set of degenerate ground states has power-law correlations and is
an example of a Coulomb phase. We investigate Neel ordering from such a Coulomb
phase, induced by weak... | cond-mat.stat-mech cond-mat.str-el | many classical geometrically frustrated antiferromagnets have macroscopically degenerate ground states in a class of threedimensional systems the set of degenerate ground states has powerlaw correlations and is an example of a coulomb phase we investigate neel ordering from such a coulomb phase induced by weak addition... | [['many', 'classical', 'geometrically', 'frustrated', 'antiferromagnets', 'have', 'macroscopically', 'degenerate', 'ground', 'states', 'in', 'a', 'class', 'of', 'threedimensional', 'systems', 'the', 'set', 'of', 'degenerate', 'ground', 'states', 'has', 'powerlaw', 'correlations', 'and', 'is', 'an', 'example', 'of', 'a'... | [-0.18058994280343707, 0.25459076650136425, -0.07129571319515393, 0.0775232547237961, -0.04438279147302224, -0.14892702969637783, 0.05901720244437456, 0.3635266762904146, -0.2870077873294411, -0.2395392092410475, 0.07620005660944364, -0.31359805046496064, -0.1566497829912061, 0.1253093940459869, 0.05993893692185256, -0... |
708.3792 | Gelfand-Dickey Algebra and Higher Spin Symmetries On $T^2=S^1\times S^1$ | We focus in this work to renew the interest in higher conformal spins
symmetries and their relations to quantum field theories and integrable models.
We consider the extension of the conformal Frappat et al. symmetries containing
the Virasoro and the Antoniadis et al. algebras as particular cases describing
geometric... | hep-th | we focus in this work to renew the interest in higher conformal spins symmetries and their relations to quantum field theories and integrable models we consider the extension of the conformal frappat et al symmetries containing the virasoro and the antoniadis et al algebras as particular cases describing geometrically ... | [['we', 'focus', 'in', 'this', 'work', 'to', 'renew', 'the', 'interest', 'in', 'higher', 'conformal', 'spins', 'symmetries', 'and', 'their', 'relations', 'to', 'quantum', 'field', 'theories', 'and', 'integrable', 'models', 'we', 'consider', 'the', 'extension', 'of', 'the', 'conformal', 'frappat', 'et', 'al', 'symmetrie... | [-0.1214084306569851, 0.12058582599274814, -0.019250426026385114, 0.08532525723516617, -0.11413938036117621, -0.1445746971749822, -0.07119578227613364, 0.32592811287664203, -0.2536754716471162, -0.2493084652106399, 0.10466371035917015, -0.2714590691612102, -0.2056559570811932, 0.15389646607471388, -0.08693629924622971,... |
708.3793 | Low upper bounds of ideals | We show that there is a low T-upper bound for the class of K-trivial sets,
namely those which are weak from the point of view of algorithmic randomness.
This result is a special case of a more general characterization of ideals in
the T-degrees below 0' for which there is a low T-upper bound.
| math.LO | we show that there is a low tupper bound for the class of ktrivial sets namely those which are weak from the point of view of algorithmic randomness this result is a special case of a more general characterization of ideals in the tdegrees below 0 for which there is a low tupper bound | [['we', 'show', 'that', 'there', 'is', 'a', 'low', 'tupper', 'bound', 'for', 'the', 'class', 'of', 'ktrivial', 'sets', 'namely', 'those', 'which', 'are', 'weak', 'from', 'the', 'point', 'of', 'view', 'of', 'algorithmic', 'randomness', 'this', 'result', 'is', 'a', 'special', 'case', 'of', 'a', 'more', 'general', 'charac... | [-0.15231255999599355, 0.11892720183603606, -0.06708366668976422, 0.08641384375492497, -0.004305959257455367, -0.1477943854582197, 0.07680688306408108, 0.2923036878401378, -0.2606114186346531, -0.24813685816589673, 0.11165194275991042, -0.2717147739120882, -0.13748966674056817, 0.24485517254556124, -0.09289137759017495... |
708.3794 | Time-optimal control of a two-level dissipative quantum system | We propose an analysis of the time-optimal control of a dissipative two-level
quantum system whose dynamics is governed by the Lindblad equation. This simple
system allows one to use tools of geometric control theory and to construct its
optimal synthesis, i.e. to determine the set of all the optimal trajectories
sta... | quant-ph | we propose an analysis of the timeoptimal control of a dissipative twolevel quantum system whose dynamics is governed by the lindblad equation this simple system allows one to use tools of geometric control theory and to construct its optimal synthesis ie to determine the set of all the optimal trajectories starting fr... | [['we', 'propose', 'an', 'analysis', 'of', 'the', 'timeoptimal', 'control', 'of', 'a', 'dissipative', 'twolevel', 'quantum', 'system', 'whose', 'dynamics', 'is', 'governed', 'by', 'the', 'lindblad', 'equation', 'this', 'simple', 'system', 'allows', 'one', 'to', 'use', 'tools', 'of', 'geometric', 'control', 'theory', 'a... | [-0.124655263974101, 0.11488970557008044, -0.11807614087217277, 0.023921434338184534, -0.03728251397028886, -0.1526268393662508, 0.05128629835853253, 0.31632880187563356, -0.3273114586919947, -0.2662670920322579, 0.11981393976051921, -0.22937752857008795, -0.1366804893859612, 0.20139868923973653, -0.06599507679516871, ... |
708.3795 | White dwarf atmosphere models with Ly-$\alpha$ opacity in the analysis
of the white dwarf cooling sequence of NGC 6397 | We discuss the importance of pure hydrogen white dwarf atmosphere models with
Ly-$\rm \alpha$ far red wing opacity in the analysis of the white dwarf cooling
sequence of the globular cluster NGC 6397. Our recently improved atmosphere
models account for the previously missing opacity from the Ly-$\rm \alpha$
hydrogen ... | astro-ph | we discuss the importance of pure hydrogen white dwarf atmosphere models with lyrm alpha far red wing opacity in the analysis of the white dwarf cooling sequence of the globular cluster ngc 6397 our recently improved atmosphere models account for the previously missing opacity from the lyrm alpha hydrogen line broadene... | [['we', 'discuss', 'the', 'importance', 'of', 'pure', 'hydrogen', 'white', 'dwarf', 'atmosphere', 'models', 'with', 'lyrm', 'alpha', 'far', 'red', 'wing', 'opacity', 'in', 'the', 'analysis', 'of', 'the', 'white', 'dwarf', 'cooling', 'sequence', 'of', 'the', 'globular', 'cluster', 'ngc', '6397', 'our', 'recently', 'impr... | [0.018277364753885195, 0.15722483122506395, -0.06391819587980326, 0.10618570099625056, -0.04532282729185401, -0.08229287311461611, 0.07515417967750601, 0.44295259167511875, -0.154178858526463, -0.3572760197902636, 0.0059076085302736964, -0.31249679148682985, -0.009717924370271738, 0.18895060967602498, -0.06050129333743... |
708.3796 | Embedding Population Dynamics Models in Inference | Increasing pressures on the environment are generating an ever-increasing
need to manage animal and plant populations sustainably, and to protect and
rebuild endangered populations. Effective management requires reliable
mathematical models, so that the effects of management action can be predicted,
and the uncertain... | stat.ME | increasing pressures on the environment are generating an everincreasing need to manage animal and plant populations sustainably and to protect and rebuild endangered populations effective management requires reliable mathematical models so that the effects of management action can be predicted and the uncertainty in t... | [['increasing', 'pressures', 'on', 'the', 'environment', 'are', 'generating', 'an', 'everincreasing', 'need', 'to', 'manage', 'animal', 'and', 'plant', 'populations', 'sustainably', 'and', 'to', 'protect', 'and', 'rebuild', 'endangered', 'populations', 'effective', 'management', 'requires', 'reliable', 'mathematical', ... | [-0.03277103097212535, 0.0880163983633759, -0.093299765671017, 0.11907130950925487, -0.06471479580979105, -0.11766628807548571, 0.07632043742298804, 0.37736702967711067, -0.2752626745927113, -0.3649433513206464, 0.12421442214399576, -0.2743691477683131, -0.1461049998407597, 0.18116298648356288, -0.14207385499375286, 0.... |
708.3797 | A General Framework for the Parametrization of Hierarchical Models | In this paper, we describe centering and noncentering methodology as
complementary techniques for use in parametrization of broad classes of
hierarchical models, with a view to the construction of effective MCMC
algorithms for exploring posterior distributions from these models. We give a
clear qualitative understand... | stat.ME | in this paper we describe centering and noncentering methodology as complementary techniques for use in parametrization of broad classes of hierarchical models with a view to the construction of effective mcmc algorithms for exploring posterior distributions from these models we give a clear qualitative understanding a... | [['in', 'this', 'paper', 'we', 'describe', 'centering', 'and', 'noncentering', 'methodology', 'as', 'complementary', 'techniques', 'for', 'use', 'in', 'parametrization', 'of', 'broad', 'classes', 'of', 'hierarchical', 'models', 'with', 'a', 'view', 'to', 'the', 'construction', 'of', 'effective', 'mcmc', 'algorithms', '... | [0.01290178520442999, 0.04539426818968344, -0.1497910213049339, 0.12085403588134795, -0.06634266667229974, -0.14482975692852684, 0.060394837212262915, 0.45318430935883003, -0.27166117733197653, -0.30714409139169296, 0.1080246037489775, -0.18656500115909655, -0.15494478129498337, 0.20580397062003614, -0.1032939124042573... |
708.3798 | Impedance-matched Hyperlens | We propose an approach to optical imaging beyond the diffraction limit, based
on transformation optics in concentric circular cylinder domains. The resulting
systems allow image magnification and minimize reflection losses due to the
impedance matching at the input or output boundaries. While perfect impedance
matchi... | physics.optics | we propose an approach to optical imaging beyond the diffraction limit based on transformation optics in concentric circular cylinder domains the resulting systems allow image magnification and minimize reflection losses due to the impedance matching at the input or output boundaries while perfect impedance matching at... | [['we', 'propose', 'an', 'approach', 'to', 'optical', 'imaging', 'beyond', 'the', 'diffraction', 'limit', 'based', 'on', 'transformation', 'optics', 'in', 'concentric', 'circular', 'cylinder', 'domains', 'the', 'resulting', 'systems', 'allow', 'image', 'magnification', 'and', 'minimize', 'reflection', 'losses', 'due', ... | [-0.1019739087140705, 0.06040527115086055, -0.04936230282247481, -0.014398008979494788, -0.07010241476301518, -0.13682451403130674, -0.0008072536826754609, 0.48722872231155634, -0.2724987624601959, -0.33170004992280155, 0.09910523333827667, -0.26632662231309545, -0.1257837214636513, 0.22864665904974876, -0.113020232186... |
708.3799 | Spatially nonuniform phases in the one-dimensional SU(n) Hubbard model
for commensurate fillings | The one-dimensional repulsive SU$(n)$ Hubbard model is investigated
analytically by bosonization approach and numerically using the density-matrix
renormalization-group (DMRG) method for $n=3,4$, and 5 for commensurate
fillings $f=p/q$ where $p$ and $q$ are relatively prime. It is shown that the
behavior of the syste... | cond-mat.str-el | the onedimensional repulsive sun hubbard model is investigated analytically by bosonization approach and numerically using the densitymatrix renormalizationgroup dmrg method for n34 and 5 for commensurate fillings fpq where p and q are relatively prime it is shown that the behavior of the system is drastically differen... | [['the', 'onedimensional', 'repulsive', 'sun', 'hubbard', 'model', 'is', 'investigated', 'analytically', 'by', 'bosonization', 'approach', 'and', 'numerically', 'using', 'the', 'densitymatrix', 'renormalizationgroup', 'dmrg', 'method', 'for', 'n34', 'and', '5', 'for', 'commensurate', 'fillings', 'fpq', 'where', 'p', 'a... | [-0.20266147494489986, 0.2726370350538224, -0.014423849243583023, 0.0661358826335437, -0.003347412498868247, -0.2319823526777327, 0.034104031156984314, 0.3573696809184231, -0.253900355906992, -0.19372127372241002, 0.08060552187328804, -0.3351960196005051, -0.08063066320028156, 0.11936144270482686, 0.08104176500434929, ... |
708.38 | Coupled quintessence and vacuum decay | We discuss observational consequences of a class of cosmological models
characterized by the dilution of pressureless matter attenuated with respect to
the usual $a^{-3}$ scaling due to the decay of vacuum energy. We carry out a
joint statistical analysis of observational data from the new \emph{gold}
sample of 182 S... | astro-ph | we discuss observational consequences of a class of cosmological models characterized by the dilution of pressureless matter attenuated with respect to the usual a3 scaling due to the decay of vacuum energy we carry out a joint statistical analysis of observational data from the new emphgold sample of 182 sne ia recent... | [['we', 'discuss', 'observational', 'consequences', 'of', 'a', 'class', 'of', 'cosmological', 'models', 'characterized', 'by', 'the', 'dilution', 'of', 'pressureless', 'matter', 'attenuated', 'with', 'respect', 'to', 'the', 'usual', 'a3', 'scaling', 'due', 'to', 'the', 'decay', 'of', 'vacuum', 'energy', 'we', 'carry', ... | [-0.07139209469535453, 0.13468863545306797, -0.08363963899218702, 0.12366423389577338, -0.11151664704887261, -0.12474840740143353, 0.03879896949390592, 0.29282981671136, -0.2337648441517276, -0.29775453228674076, 0.04997741815670201, -0.2803951843625641, -0.035822575943994114, 0.1826062315958552, -0.0006170443074520806... |
708.3801 | Heavy-quark production from Glauber-Gribov theory at LHC | We present predictions for heavy-quark production for proton-lead collisions
at LHC energy 5.5 TeV from Glauber-Gribov theory of nuclear shadowing. We have
also made predictions for baseline cold-matter (in other words inital-state)
nuclear effects in lead-lead collisions at the same energy that has to be taken
into ... | hep-ph | we present predictions for heavyquark production for protonlead collisions at lhc energy 55 tev from glaubergribov theory of nuclear shadowing we have also made predictions for baseline coldmatter in other words initalstate nuclear effects in leadlead collisions at the same energy that has to be taken into account to u... | [['we', 'present', 'predictions', 'for', 'heavyquark', 'production', 'for', 'protonlead', 'collisions', 'at', 'lhc', 'energy', '55', 'tev', 'from', 'glaubergribov', 'theory', 'of', 'nuclear', 'shadowing', 'we', 'have', 'also', 'made', 'predictions', 'for', 'baseline', 'coldmatter', 'in', 'other', 'words', 'initalstate'... | [0.02812958794061606, 0.21170384069795117, -0.2174702376930737, 0.22940230650790766, 0.012684288379900596, -0.0956334905589328, -0.09485015387911641, 0.4058750126072589, -0.1984202180276899, -0.274700397141643, -0.04987642876164732, -0.3791375952024086, 0.13391077845339097, 0.12536110718136506, 0.06211556223969834, 0.0... |
708.3802 | Unparticle physics in top pair signals at the LHC and ILC | We study the effects of unparticle physics in the pair productions of top
quarks at the LHC and ILC. By considering vector, tensor and scalar unparticle
operators, as appropriate, we compute the total cross sections for pair
production processes depending on scale dimension $d_{\U}$. We find that the
existence of unp... | hep-ph | we study the effects of unparticle physics in the pair productions of top quarks at the lhc and ilc by considering vector tensor and scalar unparticle operators as appropriate we compute the total cross sections for pair production processes depending on scale dimension d_u we find that the existence of unparticles wou... | [['we', 'study', 'the', 'effects', 'of', 'unparticle', 'physics', 'in', 'the', 'pair', 'productions', 'of', 'top', 'quarks', 'at', 'the', 'lhc', 'and', 'ilc', 'by', 'considering', 'vector', 'tensor', 'and', 'scalar', 'unparticle', 'operators', 'as', 'appropriate', 'we', 'compute', 'the', 'total', 'cross', 'sections', '... | [-0.10574087713957651, 0.25450584309298424, -0.04298736071111737, 0.176044123261338, -0.06632214072569795, -0.12977753194550481, -0.011139282746915962, 0.28193674281567005, -0.21145682691872775, -0.25549754965026955, -0.00975507205341953, -0.3618754359310145, -0.04639239954137868, 0.17475858556904963, 0.121206837358301... |
708.3803 | Multiplicity and cold-nuclear matter effects from Glauber-Gribov theory
at LHC | We present predictions for nuclear modification factor in proton-lead
collisions at LHC energy 5.5 TeV from Glauber-Gribov theory of nuclear
shadowing. We have also made predictions for baseline cold-matter nuclear
effects in lead-lead collisions at the same energy.
| hep-ph | we present predictions for nuclear modification factor in protonlead collisions at lhc energy 55 tev from glaubergribov theory of nuclear shadowing we have also made predictions for baseline coldmatter nuclear effects in leadlead collisions at the same energy | [['we', 'present', 'predictions', 'for', 'nuclear', 'modification', 'factor', 'in', 'protonlead', 'collisions', 'at', 'lhc', 'energy', '55', 'tev', 'from', 'glaubergribov', 'theory', 'of', 'nuclear', 'shadowing', 'we', 'have', 'also', 'made', 'predictions', 'for', 'baseline', 'coldmatter', 'nuclear', 'effects', 'in', '... | [0.014745383208768593, 0.19094290347719514, -0.21384647184026404, 0.2186403149688566, 0.08585979079676641, -0.07630172232165933, -0.11293403574932567, 0.40067262348492405, -0.1879722907937862, -0.3165553754346596, -0.055892357898473334, -0.3762659672144297, 0.1438555746414774, 0.12217688233264394, 0.0953897170823168, 0... |
708.3804 | Free Quarks and Antiquarks versus Hadronic Matter | Meson-meson reactions A(q_1 \bar{q}_1) + B(q_2 \bar{q}_2) to q_1 + \bar{q}_1
+ q_2 + \bar{q}_2 in high-temperature hadronic matter are found to produce an
appreciable amount of quarks and antiquarks freely moving in hadronic matter
and to establish a new mechanism for deconfinement of quarks and antiquarks in
hadroni... | hep-ph nucl-th | mesonmeson reactions aq_1 barq_1 bq_2 barq_2 to q_1 barq_1 q_2 barq_2 in hightemperature hadronic matter are found to produce an appreciable amount of quarks and antiquarks freely moving in hadronic matter and to establish a new mechanism for deconfinement of quarks and antiquarks in hadronic matter | [['mesonmeson', 'reactions', 'aq_1', 'barq_1', 'bq_2', 'barq_2', 'to', 'q_1', 'barq_1', 'q_2', 'barq_2', 'in', 'hightemperature', 'hadronic', 'matter', 'are', 'found', 'to', 'produce', 'an', 'appreciable', 'amount', 'of', 'quarks', 'and', 'antiquarks', 'freely', 'moving', 'in', 'hadronic', 'matter', 'and', 'to', 'estab... | [-0.08554480834440752, 0.43349160304040363, -0.14330251614393835, 0.13159150918099013, -0.06991881966082887, -0.12755066409326074, 0.049751668450798286, 0.3496741410344839, -0.16834301696243612, -0.21912550244649703, -0.1584685480841224, -0.32462833809073677, 0.11769386173479936, 0.0029794306240298533, 0.08455406114543... |
708.3805 | Moduli stabilization in heterotic M-theory | We reconsider the ingredients of moduli stabilization in heterotic M-theory.
On this line we close a gap in the literature deriving the Kaehler potential
dependence on vector bundle moduli and charged matter. Crucial in this
derivation is our superspace formulation of 5d heterotic M-theory taking into
account the Bia... | hep-th hep-ph | we reconsider the ingredients of moduli stabilization in heterotic mtheory on this line we close a gap in the literature deriving the kaehler potential dependence on vector bundle moduli and charged matter crucial in this derivation is our superspace formulation of 5d heterotic mtheory taking into account the bianchi i... | [['we', 'reconsider', 'the', 'ingredients', 'of', 'moduli', 'stabilization', 'in', 'heterotic', 'mtheory', 'on', 'this', 'line', 'we', 'close', 'a', 'gap', 'in', 'the', 'literature', 'deriving', 'the', 'kaehler', 'potential', 'dependence', 'on', 'vector', 'bundle', 'moduli', 'and', 'charged', 'matter', 'crucial', 'in',... | [-0.15917675515089383, 0.14589261157768743, -0.08264326953990314, 0.14065152619972485, -0.1648204744546203, -0.1601009362818005, 0.002014660556402541, 0.2901715616205039, -0.18433508887631064, -0.23770883579148364, 0.06406722691635253, -0.21878545326074117, -0.16084922450587494, 0.10171415931225278, -0.1289887426435265... |
708.3806 | Instantons in N=2 magnetized D-brane worlds | In a toroidal orbifold of type IIB string theory we study instanton effects
in N=2 super Yang-Mills theories engineered with systems of wrapped magnetized
D9 branes and Euclidean D5 branes. We analyze the various open string sectors
in this brane system and study the 1-loop amplitudes described by annulus
diagrams wi... | hep-th | in a toroidal orbifold of type iib string theory we study instanton effects in n2 super yangmills theories engineered with systems of wrapped magnetized d9 branes and euclidean d5 branes we analyze the various open string sectors in this brane system and study the 1loop amplitudes described by annulus diagrams with mix... | [['in', 'a', 'toroidal', 'orbifold', 'of', 'type', 'iib', 'string', 'theory', 'we', 'study', 'instanton', 'effects', 'in', 'n2', 'super', 'yangmills', 'theories', 'engineered', 'with', 'systems', 'of', 'wrapped', 'magnetized', 'd9', 'branes', 'and', 'euclidean', 'd5', 'branes', 'we', 'analyze', 'the', 'various', 'open'... | [-0.20168038990105625, 0.17281174201963712, -0.07192032796371242, 0.19974759931311659, -0.056056505704865506, -0.1249812422360739, -0.0037866325856631866, 0.30239132166050536, -0.1669654739124741, -0.23250972397787414, 0.07040932392397814, -0.2434786608685618, -0.21073406690974597, 0.05685219279004504, -0.1035791662643... |
708.3807 | Doniach diagram for ordered, disordered and underscreened Kondo lattices | The Doniach's diagram has been originally proposed to describe the
competition between the local Kondo effect and the intersite RKKY interactions
in cerium compounds. Here we discuss the extension of this diagram to different
variations of Kondo lattice model. We consider a) ordered cerium compounds
where the competi... | cond-mat.str-el | the doniachs diagram has been originally proposed to describe the competition between the local kondo effect and the intersite rkky interactions in cerium compounds here we discuss the extension of this diagram to different variations of kondo lattice model we consider a ordered cerium compounds where the competition b... | [['the', 'doniachs', 'diagram', 'has', 'been', 'originally', 'proposed', 'to', 'describe', 'the', 'competition', 'between', 'the', 'local', 'kondo', 'effect', 'and', 'the', 'intersite', 'rkky', 'interactions', 'in', 'cerium', 'compounds', 'here', 'we', 'discuss', 'the', 'extension', 'of', 'this', 'diagram', 'to', 'diff... | [-0.1566460368587919, 0.28861836728389356, -0.03634646677300739, 0.09642325057749353, -0.012631385728878819, -0.17354992647128908, 0.09542833220861528, 0.36826953821734565, -0.2457268794472127, -0.27662080558745755, -0.02311035070021677, -0.34812461685227314, -0.16820866196699766, 0.07508381414834572, 0.075915996963158... |
708.3808 | PAHs in the Halo of NGC 5529 | We present sensitive ISO $\lambda 6.7 \mu$m observations of the edge-on
galaxy, NGC 5529, finding an extensive MIR halo around NGC 5529. The emission
is dominated by PAHs in this band. The PAH halo has an exponential scale height
of 3.7 kpc but can still be detected as far as $\approx 10$ kpc from the plane
to the li... | astro-ph | we present sensitive iso lambda 67 mum observations of the edgeon galaxy ngc 5529 finding an extensive mir halo around ngc 5529 the emission is dominated by pahs in this band the pah halo has an exponential scale height of 37 kpc but can still be detected as far as approx 10 kpc from the plane to the limits of the high... | [['we', 'present', 'sensitive', 'iso', 'lambda', '67', 'mum', 'observations', 'of', 'the', 'edgeon', 'galaxy', 'ngc', '5529', 'finding', 'an', 'extensive', 'mir', 'halo', 'around', 'ngc', '5529', 'the', 'emission', 'is', 'dominated', 'by', 'pahs', 'in', 'this', 'band', 'the', 'pah', 'halo', 'has', 'an', 'exponential', ... | [-0.061698543377336455, 0.08919743027140357, -0.05919243689617, 0.09720904736243056, -0.08384355899007981, -0.060122019846493444, -0.0028467231340290325, 0.45716882178436985, -0.16365053480654143, -0.33960014683794854, 0.03864238668188245, -0.2943951835723471, 0.021525896649552404, 0.16888470594714475, -0.0335922730108... |
708.3809 | Design Strategies for the Geometric Synthesis of Orthoglide-type
Mechanisms | The paper addresses the geometric synthesis of Orthoglide-type mechanism, a
family of 3-DOF parallel manipulators for rapid machining applications, which
combine advantages of both serial mechanisms and parallel kinematic
architectures. These manipulators possess quasi-isotropic kinematic
performances and are made up... | cs.RO | the paper addresses the geometric synthesis of orthoglidetype mechanism a family of 3dof parallel manipulators for rapid machining applications which combine advantages of both serial mechanisms and parallel kinematic architectures these manipulators possess quasiisotropic kinematic performances and are made up of thre... | [['the', 'paper', 'addresses', 'the', 'geometric', 'synthesis', 'of', 'orthoglidetype', 'mechanism', 'a', 'family', 'of', '3dof', 'parallel', 'manipulators', 'for', 'rapid', 'machining', 'applications', 'which', 'combine', 'advantages', 'of', 'both', 'serial', 'mechanisms', 'and', 'parallel', 'kinematic', 'architecture... | [-0.18010447532012078, 0.061322227380189456, -0.034967023705279356, -0.05384406272787601, -0.1302722198165659, -0.19844926197179838, -0.0037789658073482937, 0.41838253190691926, -0.25816349495986574, -0.3263909950460258, 0.0986000012699821, -0.2029814838554318, -0.14558457124145016, 0.21088382569141687, -0.067702184354... |
708.381 | From the Planck to the Photon Scale | Using considerations from the Quantum Zero Point Field and Thermodynamics, we
show that the Planck Scale is the minimum (maximum mass) and the Photon Scale
is the maximum (minimum mass) Scale in the universe. The arguments also deduce
the residual cosmic energy of $10^{-33}eV$ observed lately.
| physics.gen-ph | using considerations from the quantum zero point field and thermodynamics we show that the planck scale is the minimum maximum mass and the photon scale is the maximum minimum mass scale in the universe the arguments also deduce the residual cosmic energy of 1033ev observed lately | [['using', 'considerations', 'from', 'the', 'quantum', 'zero', 'point', 'field', 'and', 'thermodynamics', 'we', 'show', 'that', 'the', 'planck', 'scale', 'is', 'the', 'minimum', 'maximum', 'mass', 'and', 'the', 'photon', 'scale', 'is', 'the', 'maximum', 'minimum', 'mass', 'scale', 'in', 'the', 'universe', 'the', 'argum... | [-0.12037410785484573, 0.22556773307935699, -0.12795276554179905, 0.1497951118812046, -0.054330524866995605, -0.03913362787368343, 0.04363375025011761, 0.2724021009432719, -0.2765605861483061, -0.3582232503382408, 0.10289444664807018, -0.29643679345431534, -0.04251827574942423, 0.15708399227941813, -0.00304245807068503... |
708.3811 | An Exhaustive Study of the Workspaces Tolopogies of all 3R Orthogonal
Manipulators with Geometric Simplifications | This paper proposes a classification of three-revolute orthogonal
manipulators that have at least one of their DH parameters equal to zero. This
classification is based on the topology of their workspace. The workspace is
characterized in a half-cross section by the singular curves. The workspace
topology is defined ... | cs.RO | this paper proposes a classification of threerevolute orthogonal manipulators that have at least one of their dh parameters equal to zero this classification is based on the topology of their workspace the workspace is characterized in a halfcross section by the singular curves the workspace topology is defined by the ... | [['this', 'paper', 'proposes', 'a', 'classification', 'of', 'threerevolute', 'orthogonal', 'manipulators', 'that', 'have', 'at', 'least', 'one', 'of', 'their', 'dh', 'parameters', 'equal', 'to', 'zero', 'this', 'classification', 'is', 'based', 'on', 'the', 'topology', 'of', 'their', 'workspace', 'the', 'workspace', 'is... | [-0.18668496658094227, 0.060941024140144386, -0.09803616531814138, -0.009189519321080298, -0.11547981057005624, -0.1401185974323501, -0.012204879852167021, 0.39424343607077994, -0.24412690110504628, -0.2911516479899486, 0.13174772412050514, -0.23823208414018154, -0.12828310299819956, 0.1655705586805319, -0.069044558030... |
708.3812 | Search for new charmonium states in the processes e+ e- --> J/psi D(*)
D(*) at sqrt{s} ~ 10.6 GeV | We present a study of the X(3940) state in the process e+e- -> J/psi D* Dbar.
The X(3940) mass and width are measured to be (3942 +7 -6 +- 6)MeV/c^2 and
Gamma=(37 + 26 - 15 +- 8 MeV. In the process e+e- -> J/psi D* D*bar we have
observed another charmonium-like state, which we denote as X(4160), in the
spectrum of in... | hep-ex | we present a study of the x3940 state in the process ee jpsi d dbar the x3940 mass and width are measured to be 3942 7 6 6mevc2 and gamma37 26 15 8 mev in the process ee jpsi d dbar we have observed another charmoniumlike state which we denote as x4160 in the spectrum of invariant masses of d d combinations the x4160 p... | [['we', 'present', 'a', 'study', 'of', 'the', 'x3940', 'state', 'in', 'the', 'process', 'ee', 'jpsi', 'd', 'dbar', 'the', 'x3940', 'mass', 'and', 'width', 'are', 'measured', 'to', 'be', '3942', '7', '6', '6mevc2', 'and', 'gamma37', '26', '15', '8', 'mev', 'in', 'the', 'process', 'ee', 'jpsi', 'd', 'dbar', 'we', 'have',... | [-0.10917002143967827, 0.17726446138557447, -0.05283853662183025, 0.07912502469753235, -0.01437827860084966, -0.14919066796115926, 0.07513851921410403, 0.32923944841173514, -0.13186502817121368, -0.3437775080954587, -0.024504602631269436, -0.4413474353582219, 0.06854410678217257, 0.12975156272727031, 0.1010547993808156... |
708.3813 | Non-Commutativity of Effective Space-Time Coordinates and the Minimal
Length | Considering that a position measurement can effectively involve a
momentum-dependent shift and rescaling of the "true" space-time coordinates, we
construct a set of effective space-time coordinates which are naturally
non-commutative. They lead to a minimum length and are shown to be related to
Snyder's coordinates a... | hep-th | considering that a position measurement can effectively involve a momentumdependent shift and rescaling of the true spacetime coordinates we construct a set of effective spacetime coordinates which are naturally noncommutative they lead to a minimum length and are shown to be related to snyders coordinates and the five... | [['considering', 'that', 'a', 'position', 'measurement', 'can', 'effectively', 'involve', 'a', 'momentumdependent', 'shift', 'and', 'rescaling', 'of', 'the', 'true', 'spacetime', 'coordinates', 'we', 'construct', 'a', 'set', 'of', 'effective', 'spacetime', 'coordinates', 'which', 'are', 'naturally', 'noncommutative', '... | [-0.14689663567083985, 0.14528405986187098, -0.11534005809134167, 0.11711826681092039, -0.13242996500584445, -0.14989968924170458, -0.02102854691666404, 0.31295678506629837, -0.2556444431262973, -0.29262439760158915, 0.058435662065963505, -0.214909578872673, -0.17143050769932175, 0.1430478414251028, -0.1051801395430964... |
708.3814 | Extending BCCNR flavored geometry to the negative coupling constant
region | We extend BCCNR's flavored KW and KS geometries into the negative coupling
constant region and try giving physical explanations from the dual gauge theory
side. We show that, in the extended region, except the coupling constant being
negative, all other fields of the super-gravity theory having good properties
which ... | hep-th | we extend bccnrs flavored kw and ks geometries into the negative coupling constant region and try giving physical explanations from the dual gauge theory side we show that in the extended region except the coupling constant being negative all other fields of the supergravity theory having good properties which can be d... | [['we', 'extend', 'bccnrs', 'flavored', 'kw', 'and', 'ks', 'geometries', 'into', 'the', 'negative', 'coupling', 'constant', 'region', 'and', 'try', 'giving', 'physical', 'explanations', 'from', 'the', 'dual', 'gauge', 'theory', 'side', 'we', 'show', 'that', 'in', 'the', 'extended', 'region', 'except', 'the', 'coupling'... | [-0.10744275758874469, 0.17399823984929494, -0.0684655432456306, 0.08921822868952793, -0.12351412930625624, -0.21649385965429246, 0.024535886363342536, 0.3414494462028545, -0.22087686009971158, -0.28751701435872484, 0.06065742599769562, -0.25049579083653434, -0.1352291833941958, 0.10601341864094138, -0.0006653094990594... |
708.3815 | Flavor Hierarchy Quadratic Rule and Dual Quark-Neutrino Mixing Patterns | Flavor physics is about particle mass-degeneracy-deviations (DMD) and mixing
and especially about hierarchies of those deviations. On the one hand there is
no established theory of particle flavor at present; on the other hand there
are growing data indications on interesting empirical flavor regularities that
are de... | hep-ph hep-ex | flavor physics is about particle massdegeneracydeviations dmd and mixing and especially about hierarchies of those deviations on the one hand there is no established theory of particle flavor at present on the other hand there are growing data indications on interesting empirical flavor regularities that are described ... | [['flavor', 'physics', 'is', 'about', 'particle', 'massdegeneracydeviations', 'dmd', 'and', 'mixing', 'and', 'especially', 'about', 'hierarchies', 'of', 'those', 'deviations', 'on', 'the', 'one', 'hand', 'there', 'is', 'no', 'established', 'theory', 'of', 'particle', 'flavor', 'at', 'present', 'on', 'the', 'other', 'ha... | [-0.06214105761299531, 0.311046631805754, -0.022489223992452026, 0.21775434900851298, -0.08099368136841804, -0.18812983532746633, 0.11504802834630633, 0.28051443374851565, -0.2306098256011804, -0.3193593006487936, 0.05687769413848097, -0.31624250022073586, -0.044630737040812773, 0.14789492059033363, 0.04586820145603269... |
708.3816 | Constraining the equation of state of supra-nuclear dense matter from
XMM-Newton observations of neutron stars in globular clusters | We report on the detailed modelling of the X-ray spectra of three likely
neutron stars. The neutron stars, observed with XMM-Newton are found in three
quiescent X-ray binaries in the globular clusters: omega Cen, M 13 and NGC
2808. Whether they are accreting at very low rates or radiating energy from an
accretion hea... | astro-ph | we report on the detailed modelling of the xray spectra of three likely neutron stars the neutron stars observed with xmmnewton are found in three quiescent xray binaries in the globular clusters omega cen m 13 and ngc 2808 whether they are accreting at very low rates or radiating energy from an accretion heated core t... | [['we', 'report', 'on', 'the', 'detailed', 'modelling', 'of', 'the', 'xray', 'spectra', 'of', 'three', 'likely', 'neutron', 'stars', 'the', 'neutron', 'stars', 'observed', 'with', 'xmmnewton', 'are', 'found', 'in', 'three', 'quiescent', 'xray', 'binaries', 'in', 'the', 'globular', 'clusters', 'omega', 'cen', 'm', '13',... | [-0.03347321832666128, 0.15107915776096023, -0.06588440205129545, 0.1270214088192982, -0.11710927315942216, -0.07513368002070886, 0.0824404362725412, 0.37780838915851056, -0.1541694135217723, -0.40812331918717887, 0.06678167111921783, -0.35805315224272083, 0.0604469703249179, 0.23824899137054184, -0.005022566082387618,... |
708.3817 | Fractionally Quantized Hall Effect: Liquid-Crystal Ground-State and it
Excitations | It is shown that the ground-state and the lowest excited-states of
two-dimensional electron system (2DES), with ion jellium background, correspond
to partial crystal-like (with the period $L_{x}^{\square}=\sqrt{2 m \pi}
\ell_{0}$) correlation order among $N$ electrons of the main region (MR; $L_{x}
\times L_{y}$). Ma... | cond-mat.mes-hall cond-mat.str-el | it is shown that the groundstate and the lowest excitedstates of twodimensional electron system 2des with ion jellium background correspond to partial crystallike with the period l_xsquaresqrt2 m pi ell_0 correlation order among n electrons of the main region mr l_x times l_y manybody variational groundstate wave funct... | [['it', 'is', 'shown', 'that', 'the', 'groundstate', 'and', 'the', 'lowest', 'excitedstates', 'of', 'twodimensional', 'electron', 'system', '2des', 'with', 'ion', 'jellium', 'background', 'correspond', 'to', 'partial', 'crystallike', 'with', 'the', 'period', 'l_xsquaresqrt2', 'm', 'pi', 'ell_0', 'correlation', 'order',... | [-0.18184786011761805, 0.23761188385980375, -0.016057630137907803, 0.053884391119135455, 0.047511222129345894, -0.16199264526708956, 0.054293199715742826, 0.35824374916083224, -0.2173270201438679, -0.2915898314858744, -0.03408553113641832, -0.3443885974974773, -0.04648368954637148, 0.12407008237408372, 0.08629646869640... |
708.3818 | All-sky search for periodic gravitational waves in LIGO S4 data | We report on an all-sky search with the LIGO detectors for periodic
gravitational waves in the frequency range 50-1000 Hz and with the frequency's
time derivative in the range -1.0E-8 Hz/s to zero. Data from the fourth LIGO
science run (S4) have been used in this search. Three different semi-coherent
methods of trans... | gr-qc astro-ph | we report on an allsky search with the ligo detectors for periodic gravitational waves in the frequency range 501000 hz and with the frequencys time derivative in the range 10e8 hzs to zero data from the fourth ligo science run s4 have been used in this search three different semicoherent methods of transforming and su... | [['we', 'report', 'on', 'an', 'allsky', 'search', 'with', 'the', 'ligo', 'detectors', 'for', 'periodic', 'gravitational', 'waves', 'in', 'the', 'frequency', 'range', '501000', 'hz', 'and', 'with', 'the', 'frequencys', 'time', 'derivative', 'in', 'the', 'range', '10e8', 'hzs', 'to', 'zero', 'data', 'from', 'the', 'fourt... | [-0.09393022548143579, 0.10791876203998917, -0.041585944026844596, 0.07171822441597593, -0.07445427760006901, -0.06096141055778526, 0.07597740663965522, 0.3925448421809196, -0.22059548272034235, -0.3248743821075598, 0.13647743036086563, -0.3017800777576337, -0.07452747249868658, 0.27253449510317296, -0.0111289499265726... |
708.3819 | Line shift, line asymmetry, and the 6Li/7Li isotopic ratio determination | Context: Line asymmetries are generated by convective Doppler shifts in
stellar atmospheres, especially in metal-poor stars, where convective motions
penetrate to higher atmospheric levels. Such asymmetries are usually neglected
in abundance analyses. The determination of the 6Li/7Li isotopic ratio is prone
to suffer... | astro-ph | context line asymmetries are generated by convective doppler shifts in stellar atmospheres especially in metalpoor stars where convective motions penetrate to higher atmospheric levels such asymmetries are usually neglected in abundance analyses the determination of the 6li7li isotopic ratio is prone to suffering from ... | [['context', 'line', 'asymmetries', 'are', 'generated', 'by', 'convective', 'doppler', 'shifts', 'in', 'stellar', 'atmospheres', 'especially', 'in', 'metalpoor', 'stars', 'where', 'convective', 'motions', 'penetrate', 'to', 'higher', 'atmospheric', 'levels', 'such', 'asymmetries', 'are', 'usually', 'neglected', 'in', '... | [-0.048448730447496514, 0.11093172246276155, -0.04464006457688673, 0.05093925746096263, -0.05763429598355631, -0.07136427633956356, 0.05431056782374826, 0.3809243509827076, -0.18640526480937622, -0.31981761722566276, 0.008638265039683934, -0.2918087681096469, -0.04035617164292215, 0.17281231949685738, -0.05322074476049... |
708.382 | Vacuum polarization for lukewarm black holes | We compute the renormalized expectation value of the square of a quantum
scalar field on a Reissner-Nordstrom-de Sitter black hole in which the
temperatures of the event and cosmological horizons are equal (`lukewarm' black
hole). Our numerical calculations for a thermal state at the same temperature
as the two horiz... | gr-qc | we compute the renormalized expectation value of the square of a quantum scalar field on a reissnernordstromde sitter black hole in which the temperatures of the event and cosmological horizons are equal lukewarm black hole our numerical calculations for a thermal state at the same temperature as the two horizons indic... | [['we', 'compute', 'the', 'renormalized', 'expectation', 'value', 'of', 'the', 'square', 'of', 'a', 'quantum', 'scalar', 'field', 'on', 'a', 'reissnernordstromde', 'sitter', 'black', 'hole', 'in', 'which', 'the', 'temperatures', 'of', 'the', 'event', 'and', 'cosmological', 'horizons', 'are', 'equal', 'lukewarm', 'black... | [-0.14672901035532698, 0.12836779388160868, -0.1032854341366596, 0.12973519887818002, -0.031273462825679575, -0.09167222540033446, -0.01301710867729766, 0.32188050145947045, -0.1481485610918795, -0.2472873730370882, 0.15151541823944098, -0.3425095565014936, -0.07624065863161252, 0.20495378398122374, -0.0054057800350175... |
708.3821 | Fundamental and composite scalars from extra dimensions | We discuss a scenario consisting of an effective 4D theory containing
fundamental and composite fields. The strong dynamics sector responsible for
the compositeness is assumed to be of extra dimensional origin. In the 4D
effective theory the SM fermion and gauge fields are taken as fundamental
fields. The scalar sect... | hep-ph | we discuss a scenario consisting of an effective 4d theory containing fundamental and composite fields the strong dynamics sector responsible for the compositeness is assumed to be of extra dimensional origin in the 4d effective theory the sm fermion and gauge fields are taken as fundamental fields the scalar sector of... | [['we', 'discuss', 'a', 'scenario', 'consisting', 'of', 'an', 'effective', '4d', 'theory', 'containing', 'fundamental', 'and', 'composite', 'fields', 'the', 'strong', 'dynamics', 'sector', 'responsible', 'for', 'the', 'compositeness', 'is', 'assumed', 'to', 'be', 'of', 'extra', 'dimensional', 'origin', 'in', 'the', '4d... | [-0.13934105457857263, 0.2261351942715371, -0.029492749512779068, 0.1415808891985532, -0.07102861469863993, -0.18499498429472547, 0.01223461160293208, 0.283460803134984, -0.19195441788696074, -0.29356048028938564, 0.055586102193485136, -0.2287273726156767, -0.11599679617211223, 0.12272985840177006, 0.04304287443849179,... |
708.3822 | Critical Topology for Optimization on the Symplectic Group | Optimization problems over compact Lie groups have been extensively studied
due to their broad applications in linear programming and optimal control. This
paper analyzes least square problems over a noncompact Lie group, the
symplectic group $\Sp(2N,\R)$, which can be used to assess the optimality of
control over dy... | math-ph math.MP | optimization problems over compact lie groups have been extensively studied due to their broad applications in linear programming and optimal control this paper analyzes least square problems over a noncompact lie group the symplectic group sp2nr which can be used to assess the optimality of control over dynamical tran... | [['optimization', 'problems', 'over', 'compact', 'lie', 'groups', 'have', 'been', 'extensively', 'studied', 'due', 'to', 'their', 'broad', 'applications', 'in', 'linear', 'programming', 'and', 'optimal', 'control', 'this', 'paper', 'analyzes', 'least', 'square', 'problems', 'over', 'a', 'noncompact', 'lie', 'group', 't... | [-0.16988970313589866, 0.010523685092468642, -0.10762458006360652, 0.08766959129166531, -0.10764619360108757, -0.1383373770942045, 0.01673681922370128, 0.370026261608776, -0.33588269632309675, -0.28107115623101386, 0.14683828847814262, -0.2217221548845474, -0.172324562585143, 0.2063465448639666, -0.1294520928155786, 0.... |
708.3823 | Reduction without reduction: Adding KK-monopoles to five dimensional
stationary axisymmetric solutions | We present a general method to add KK-monopole charge to any asymptotically
flat stationary axisymmetric solution of five dimensional General Relativity.
The technique exploits the underlying SL(3,R) invariance of the system by
identifying a particular element of the symmetry group which changes the
asymptotic bounda... | hep-th | we present a general method to add kkmonopole charge to any asymptotically flat stationary axisymmetric solution of five dimensional general relativity the technique exploits the underlying sl3r invariance of the system by identifying a particular element of the symmetry group which changes the asymptotic boundary cond... | [['we', 'present', 'a', 'general', 'method', 'to', 'add', 'kkmonopole', 'charge', 'to', 'any', 'asymptotically', 'flat', 'stationary', 'axisymmetric', 'solution', 'of', 'five', 'dimensional', 'general', 'relativity', 'the', 'technique', 'exploits', 'the', 'underlying', 'sl3r', 'invariance', 'of', 'the', 'system', 'by',... | [-0.13969489145943875, 0.03636369402210544, -0.1233987121952958, 0.07053480937235779, -0.10368268919848306, -0.15448413328117422, 0.03390423410762382, 0.2999998932273718, -0.22441198326326828, -0.2622239981134552, 0.11874027265816607, -0.25077487667521803, -0.15072545576940782, 0.12542352423832942, -0.04380122236707198... |
708.3824 | Radio Detection of Neutrinos from Behind a Mountain | We explore the sensitivity of a neutrino detector employing strongly
directional high gain radio antennae to detect the conversion of neutrinos
above $10^{16}$ eV in a mountain or the earth crust. The directionality of the
antennae will allow both, the low threshold and the suppression of background.
This technology ... | astro-ph | we explore the sensitivity of a neutrino detector employing strongly directional high gain radio antennae to detect the conversion of neutrinos above 1016 ev in a mountain or the earth crust the directionality of the antennae will allow both the low threshold and the suppression of background this technology would have... | [['we', 'explore', 'the', 'sensitivity', 'of', 'a', 'neutrino', 'detector', 'employing', 'strongly', 'directional', 'high', 'gain', 'radio', 'antennae', 'to', 'detect', 'the', 'conversion', 'of', 'neutrinos', 'above', '1016', 'ev', 'in', 'a', 'mountain', 'or', 'the', 'earth', 'crust', 'the', 'directionality', 'of', 'th... | [-0.09503827268859842, 0.1676905481920888, -0.05128448278272665, 0.09139211390477915, -0.11910932997031318, -0.11760077098452096, 0.06692971525493488, 0.40362263790341796, -0.1864698545666792, -0.3442139355165343, 0.09880310423441872, -0.27461145358580735, -0.07534094734908513, 0.21403780857586774, -0.02509565268873527... |
708.3825 | Stochastic Fluctuations in Epidemics on Networks | The effects of demographic stochasticity in the long term behaviour of
endemic infectious diseases have been considered for long as a necessary
addition to an underlying deterministic theory. The latter would explain the
regular behaviour of recurrent epidemics, and the former the superimposed noise
of observed incid... | q-bio.PE | the effects of demographic stochasticity in the long term behaviour of endemic infectious diseases have been considered for long as a necessary addition to an underlying deterministic theory the latter would explain the regular behaviour of recurrent epidemics and the former the superimposed noise of observed incidence... | [['the', 'effects', 'of', 'demographic', 'stochasticity', 'in', 'the', 'long', 'term', 'behaviour', 'of', 'endemic', 'infectious', 'diseases', 'have', 'been', 'considered', 'for', 'long', 'as', 'a', 'necessary', 'addition', 'to', 'an', 'underlying', 'deterministic', 'theory', 'the', 'latter', 'would', 'explain', 'the',... | [-0.13877555135785385, 0.17630547746451533, -0.09928149518985037, 0.1210661249542035, -0.04016478969693466, -0.11653733747168245, 0.05172257363615266, 0.33234283038507706, -0.2865468110553744, -0.2751676619375098, 0.11583236169888775, -0.2503633517690579, -0.20937938440449855, 0.15977861271217747, -0.06144221579894353,... |
708.3826 | Trapping radioactive ^{82}Rb in an optical dipole trap and evidence of
spontaneous spin polarization | Optical trapping of selected species of radioactive atoms has great potential
in precision measurements for testing fundamental physics such as EDM, PNC and
parity violating beta-decay asymmetry correlation coefficients. We report
trapping of 10^4 radioactive ^{82}Rb atoms (t_{1/2}=75 s) with a trap lifetime
of ~55 s... | quant-ph nucl-ex physics.atom-ph | optical trapping of selected species of radioactive atoms has great potential in precision measurements for testing fundamental physics such as edm pnc and parity violating betadecay asymmetry correlation coefficients we report trapping of 104 radioactive 82rb atoms t_1275 s with a trap lifetime of 55 seconds in an opt... | [['optical', 'trapping', 'of', 'selected', 'species', 'of', 'radioactive', 'atoms', 'has', 'great', 'potential', 'in', 'precision', 'measurements', 'for', 'testing', 'fundamental', 'physics', 'such', 'as', 'edm', 'pnc', 'and', 'parity', 'violating', 'betadecay', 'asymmetry', 'correlation', 'coefficients', 'we', 'report... | [-0.08777535287916417, 0.23646004297346657, 0.03238402658051042, -0.032975713793269315, 0.05561820367027236, -0.18096701106380508, 0.0879847377376712, 0.42018844875628536, -0.21310567165441488, -0.3014349460794145, -0.014602888279351528, -0.3186440304853022, 0.0331059560336618, 0.17189077379526166, 0.054159154965596513... |
708.3827 | Linear frictional forces cause orbits to neither circularize nor precess | For the undamped Kepler potential the lack of precession has historically
been understood in terms of the Runge-Lenz symmetry. For the damped Kepler
problem this result may be understood in terms of the generalization of Poisson
structure to damped systems suggested recently by Tarasov[1]. In this
generalized algebra... | physics.class-ph | for the undamped kepler potential the lack of precession has historically been understood in terms of the rungelenz symmetry for the damped kepler problem this result may be understood in terms of the generalization of poisson structure to damped systems suggested recently by tarasov1 in this generalized algebraic stru... | [['for', 'the', 'undamped', 'kepler', 'potential', 'the', 'lack', 'of', 'precession', 'has', 'historically', 'been', 'understood', 'in', 'terms', 'of', 'the', 'rungelenz', 'symmetry', 'for', 'the', 'damped', 'kepler', 'problem', 'this', 'result', 'may', 'be', 'understood', 'in', 'terms', 'of', 'the', 'generalization', ... | [-0.1832564883208012, 0.14533969213473885, -0.03958059992531643, 0.07740438366240329, -0.12962672987487167, -0.05992898582617807, -0.01004033480935237, 0.2711266009410953, -0.3207489837180166, -0.2831652592114337, 0.07747670584135716, -0.2254752182703027, -0.17669401736930013, 0.2217613535176497, -0.10304975149440854, ... |
708.3828 | Leptogenesis from Pseudo-Scalar Driven Inflation | We examine recent claims for a considerable amount of leptogenesis, in some
inflationary scenarios, through the gravitational anomaly in the lepton number
current. We find that when the short distances contributions are properly
included the amount of lepton number generated is actually much smaller.
| hep-th | we examine recent claims for a considerable amount of leptogenesis in some inflationary scenarios through the gravitational anomaly in the lepton number current we find that when the short distances contributions are properly included the amount of lepton number generated is actually much smaller | [['we', 'examine', 'recent', 'claims', 'for', 'a', 'considerable', 'amount', 'of', 'leptogenesis', 'in', 'some', 'inflationary', 'scenarios', 'through', 'the', 'gravitational', 'anomaly', 'in', 'the', 'lepton', 'number', 'current', 'we', 'find', 'that', 'when', 'the', 'short', 'distances', 'contributions', 'are', 'prop... | [-0.17308345349209214, 0.23121831676160748, 0.01453861433467616, 0.1498385485055306, -0.08036581621589986, -0.060976242889988826, 0.03397623081268235, 0.3284658577970483, -0.2264044095169414, -0.32627811036019755, 0.04976083168400113, -0.3154356572777033, -0.08065936258803545, 0.199865508755796, -0.03672777986238626, 0... |
708.3829 | A Non Parametric Model for the Forecasting of the Venezuelan Oil Prices | A neural net model for forecasting the prices of Venezuelan crude oil is
proposed. The inputs of the neural net are selected by reference to a dynamic
system model of oil prices by Mashayekhi (1995, 2001) and its performance is
evaluated using two criteria: the Excess Profitability test by Anatoliev and
Gerko (2005) ... | cs.CE cs.NE | a neural net model for forecasting the prices of venezuelan crude oil is proposed the inputs of the neural net are selected by reference to a dynamic system model of oil prices by mashayekhi 1995 2001 and its performance is evaluated using two criteria the excess profitability test by anatoliev and gerko 2005 and the c... | [['a', 'neural', 'net', 'model', 'for', 'forecasting', 'the', 'prices', 'of', 'venezuelan', 'crude', 'oil', 'is', 'proposed', 'the', 'inputs', 'of', 'the', 'neural', 'net', 'are', 'selected', 'by', 'reference', 'to', 'a', 'dynamic', 'system', 'model', 'of', 'oil', 'prices', 'by', 'mashayekhi', '1995', '2001', 'and', 'i... | [-0.15638071309402585, -0.004341679690405727, -0.1630724278613925, 0.11943493680842221, -0.05664996106550097, -0.17985372494161128, 0.010345898427069187, 0.2555638954639435, -0.13388698655366899, -0.29758350394666194, 0.03130027127487119, -0.33679354429990055, -0.16052882723137737, 0.11475275932997465, -0.2252377996817... |
708.383 | Entanglement and the nonlinear elastic behavior of forests of coiled
carbon nanotubes | Helical or coiled nanostructures have been object of intense experimental and
theoretical studies due to their special electronic and mechanical properties.
Recently, it was experimentally reported that the dynamical response of
foamlike forest of coiled carbon nanotubes under mechanical impact exhibits a
nonlinear, ... | cond-mat.mtrl-sci | helical or coiled nanostructures have been object of intense experimental and theoretical studies due to their special electronic and mechanical properties recently it was experimentally reported that the dynamical response of foamlike forest of coiled carbon nanotubes under mechanical impact exhibits a nonlinear nonhe... | [['helical', 'or', 'coiled', 'nanostructures', 'have', 'been', 'object', 'of', 'intense', 'experimental', 'and', 'theoretical', 'studies', 'due', 'to', 'their', 'special', 'electronic', 'and', 'mechanical', 'properties', 'recently', 'it', 'was', 'experimentally', 'reported', 'that', 'the', 'dynamical', 'response', 'of'... | [-0.11675341364688578, 0.1342194947142121, -0.09920186256841484, -0.011285116597268302, -0.056866179653072516, -0.11835079119371794, 0.02846961383567711, 0.4393075081495057, -0.21752274706465216, -0.24314517615027148, 0.06204080914839509, -0.2780567587134882, -0.2004294819590034, 0.1821939917708813, -0.0129640529641007... |
708.3831 | Twisted Alexander Polynomials and Representation Shifts | For any knot, the following are equivalent. (1) The infinite cyclic cover has
uncountably many finite covers; (2) there exists a finite-image representation
of the knot group for which the twisted Alexander polynomial vanishes; (3) the
knot group admits a finite-image representation such that the image of the
fundame... | math.GT | for any knot the following are equivalent 1 the infinite cyclic cover has uncountably many finite covers 2 there exists a finiteimage representation of the knot group for which the twisted alexander polynomial vanishes 3 the knot group admits a finiteimage representation such that the image of the fundamental group of ... | [['for', 'any', 'knot', 'the', 'following', 'are', 'equivalent', '1', 'the', 'infinite', 'cyclic', 'cover', 'has', 'uncountably', 'many', 'finite', 'covers', '2', 'there', 'exists', 'a', 'finiteimage', 'representation', 'of', 'the', 'knot', 'group', 'for', 'which', 'the', 'twisted', 'alexander', 'polynomial', 'vanishes... | [-0.27713182579193796, 0.10588366581713282, -0.1724780055295144, 0.034356419530896735, -0.11436578483719911, -0.1557491949958993, -0.01488106498228652, 0.3644978546670505, -0.341561927087605, -0.22841203710330385, 0.1382094452423709, -0.23231660606605667, -0.11442048765186752, 0.1751803626306355, -0.1473175508968, -0.0... |
708.3832 | An H2CO 6cm Maser Pinpointing a Possible Circumstellar Torus in
IRAS18566+0408 | We report observations of 6cm, 3.6cm, 1.3cm, and 7mm radio continuum,
conducted with the Very Large Array towards IRAS18566+0408, one of the few
sources known to harbor H2CO 6cm maser emission. Our observations reveal that
the emission is dominated by an ionized jet at cm wavelengths. Spitzer/IRAC
images from GLIMPSE... | astro-ph | we report observations of 6cm 36cm 13cm and 7mm radio continuum conducted with the very large array towards iras185660408 one of the few sources known to harbor h2co 6cm maser emission our observations reveal that the emission is dominated by an ionized jet at cm wavelengths spitzerirac images from glimpse support this... | [['we', 'report', 'observations', 'of', '6cm', '36cm', '13cm', 'and', '7mm', 'radio', 'continuum', 'conducted', 'with', 'the', 'very', 'large', 'array', 'towards', 'iras185660408', 'one', 'of', 'the', 'few', 'sources', 'known', 'to', 'harbor', 'h2co', '6cm', 'maser', 'emission', 'our', 'observations', 'reveal', 'that',... | [-0.05176334885875215, 0.05652298184160078, -0.00959074223989292, 0.034249158835497354, -0.10243907952270306, -0.09331496655324693, 0.01573290430721553, 0.5230646982022068, -0.1545070909675868, -0.2650548115454833, 0.08282264559581082, -0.26979823653956, 0.020341668661464665, 0.13039857446325614, 0.06437880213090519, -... |
708.3833 | The Symbiotic System SS73 17 Seen with Suzaku | We observed with Suzaku the symbiotic star SS73 17, motivated by the
discovery by the INTEGRAL satellite and the Swift BAT survey that it emits hard
X-rays. Our observations showed a highly-absorbed X-ray spectrum with NH >
10^23 cm-2, equivalent to A_V > 26, although the source has B magnitude 11.3
and is also brigh... | astro-ph | we observed with suzaku the symbiotic star ss73 17 motivated by the discovery by the integral satellite and the swift bat survey that it emits hard xrays our observations showed a highlyabsorbed xray spectrum with nh 1023 cm2 equivalent to a_v 26 although the source has b magnitude 113 and is also bright in uv the sour... | [['we', 'observed', 'with', 'suzaku', 'the', 'symbiotic', 'star', 'ss73', '17', 'motivated', 'by', 'the', 'discovery', 'by', 'the', 'integral', 'satellite', 'and', 'the', 'swift', 'bat', 'survey', 'that', 'it', 'emits', 'hard', 'xrays', 'our', 'observations', 'showed', 'a', 'highlyabsorbed', 'xray', 'spectrum', 'with',... | [-0.02592788129961708, 0.10828832756715819, -0.011908181871359166, 0.09892102924641222, -0.10827317575995739, -0.16612889453435814, 0.06459748531624304, 0.48732333744947726, -0.18931309192713217, -0.3493596380239361, 0.09552134788432896, -0.3598851954724589, -0.06977650573439222, 0.20687190206127232, -0.069180846256435... |
708.3834 | A simple evolutionary game with feedback between perception and reality | We study an evolutionary game of chance in which the probabilities for
different outcomes (e.g., heads or tails) depend on the amount wagered on those
outcomes. The game is perhaps the simplest possible probabilistic game in which
perception affects reality. By varying the `reality map', which relates the
amount wage... | physics.soc-ph | we study an evolutionary game of chance in which the probabilities for different outcomes eg heads or tails depend on the amount wagered on those outcomes the game is perhaps the simplest possible probabilistic game in which perception affects reality by varying the reality map which relates the amount wagered to the p... | [['we', 'study', 'an', 'evolutionary', 'game', 'of', 'chance', 'in', 'which', 'the', 'probabilities', 'for', 'different', 'outcomes', 'eg', 'heads', 'or', 'tails', 'depend', 'on', 'the', 'amount', 'wagered', 'on', 'those', 'outcomes', 'the', 'game', 'is', 'perhaps', 'the', 'simplest', 'possible', 'probabilistic', 'game... | [-0.07616553351951716, 0.09894807402675863, -0.14958383081576382, 0.08869778303644404, -0.05798801784194672, -0.15734066318434017, 0.14831175001051564, 0.3651989764892138, -0.2743448241112324, -0.33236057905223554, 0.0656492682120118, -0.27087428835101235, -0.15458233409608976, 0.09816017328188396, -0.15058180414474545... |
708.3835 | A 5D non compact and non Ricci flat Kaluza-Klein Cosmology | A model universe is proposed in the framework of 5-dimensional noncompact
Kaluza-Klein cosmology which is not Ricci flat. The 4D part as the
Robertson-Walker metric is coupled to conventional perfect fluid, and its
extra-dimensional part is coupled to a dark pressure through a scalar field. It
is shown that neither e... | gr-qc | a model universe is proposed in the framework of 5dimensional noncompact kaluzaklein cosmology which is not ricci flat the 4d part as the robertsonwalker metric is coupled to conventional perfect fluid and its extradimensional part is coupled to a dark pressure through a scalar field it is shown that neither early infl... | [['a', 'model', 'universe', 'is', 'proposed', 'in', 'the', 'framework', 'of', '5dimensional', 'noncompact', 'kaluzaklein', 'cosmology', 'which', 'is', 'not', 'ricci', 'flat', 'the', '4d', 'part', 'as', 'the', 'robertsonwalker', 'metric', 'is', 'coupled', 'to', 'conventional', 'perfect', 'fluid', 'and', 'its', 'extradim... | [-0.14812321521536875, 0.18455150747055038, -0.12020409569093907, 0.11680005732577646, -0.17358525094853058, -0.18861163666824232, -0.14602188506742586, 0.28747693768928984, -0.16928549161231196, -0.24989380463926322, 0.0679516706008439, -0.23828695163231445, -0.10892167670111097, 0.08489955349737224, -0.05449832174171... |
708.3836 | Inelastic scattering rates in d-wave superconductors | The inelastic scattering rates of quasiparticles in a two-dimensional d-wave
superconductor, which arise from interactions with either acoustic phonons or
other quasiparticles, are calculated within second order perturbation theory.
We discover a strong enhancement of scattering with collinear momenta, brouth
about b... | cond-mat.str-el cond-mat.supr-con | the inelastic scattering rates of quasiparticles in a twodimensional dwave superconductor which arise from interactions with either acoustic phonons or other quasiparticles are calculated within second order perturbation theory we discover a strong enhancement of scattering with collinear momenta brouth about by the sp... | [['the', 'inelastic', 'scattering', 'rates', 'of', 'quasiparticles', 'in', 'a', 'twodimensional', 'dwave', 'superconductor', 'which', 'arise', 'from', 'interactions', 'with', 'either', 'acoustic', 'phonons', 'or', 'other', 'quasiparticles', 'are', 'calculated', 'within', 'second', 'order', 'perturbation', 'theory', 'we... | [-0.17001136727706198, 0.17143149408647948, -0.07490516034369883, 0.06500342944843485, -0.05822821957765207, -0.08576289876814812, 0.05310595882098911, 0.32765106639764724, -0.2791638190993258, -0.24604414150282186, 0.008834019076124194, -0.37875501023823277, -0.09841181355859002, 0.1285363922060858, 0.0679835350076187... |
708.3837 | Possible Magnetic Activity in the Low Mass X-ray Binary EXO 0748-676 | We report evidence of magnetic activity associated with the secondary star in
the EXO 0748-676 low mass X-ray binary system. An analysis of a sequence of
five consecutive X-ray eclipses observed during December 2003 with the RXTE
satellite brings out a feature occurring during ingress we interpret as the
X-ray photoe... | astro-ph | we report evidence of magnetic activity associated with the secondary star in the exo 0748676 low mass xray binary system an analysis of a sequence of five consecutive xray eclipses observed during december 2003 with the rxte satellite brings out a feature occurring during ingress we interpret as the xray photoelectric... | [['we', 'report', 'evidence', 'of', 'magnetic', 'activity', 'associated', 'with', 'the', 'secondary', 'star', 'in', 'the', 'exo', '0748676', 'low', 'mass', 'xray', 'binary', 'system', 'an', 'analysis', 'of', 'a', 'sequence', 'of', 'five', 'consecutive', 'xray', 'eclipses', 'observed', 'during', 'december', '2003', 'wit... | [-0.12894855446956424, 0.1449025612970897, -0.08918473491422742, 0.04856892776498795, -0.04093160665543548, -0.07453104155418654, 0.10379775816782277, 0.40232114264803254, -0.24593368443065738, -0.3888682388274156, 0.10177039734932246, -0.32350199489033055, -0.07581028044897031, 0.21157539842779333, -0.0811189871718994... |
708.3838 | Spectroscopic follow-up of a cluster candidate at z = 1.45 | We have obtained deep optical spectroscopic data of the highest-redshift
cluster candidate (z ~ 1.4, CVB13) selected by Van Breukelen et al. (2006) in a
photometric optical/infrared catalogue of the Subaru XMM-Newton Deep Field. The
data, which comprise 104 targeted galaxies, were taken with the DEep Imaging
Multi-Ob... | astro-ph | we have obtained deep optical spectroscopic data of the highestredshift cluster candidate z 14 cvb13 selected by van breukelen et al 2006 in a photometric opticalinfrared catalogue of the subaru xmmnewton deep field the data which comprise 104 targeted galaxies were taken with the deep imaging multiobject spectrograph ... | [['we', 'have', 'obtained', 'deep', 'optical', 'spectroscopic', 'data', 'of', 'the', 'highestredshift', 'cluster', 'candidate', 'z', '14', 'cvb13', 'selected', 'by', 'van', 'breukelen', 'et', 'al', '2006', 'in', 'a', 'photometric', 'opticalinfrared', 'catalogue', 'of', 'the', 'subaru', 'xmmnewton', 'deep', 'field', 'th... | [-0.06872415966161743, 0.10082683091090609, -0.06813241882403766, 0.05673717652776636, -0.08402368641122335, -0.1171571592147343, 0.08010280101351734, 0.44090048377087016, -0.1582498272777626, -0.3849611252308228, 0.0920738662620201, -0.31917618846877904, 0.007233997131610303, 0.20545282149079075, 0.04226792642195259, ... |
708.3839 | Derived classification of gentle algebras with two cycles | We classify gentle algebras defined by quivers with two cycles under derived
equivalence in a non degenerate case, by using some combinatorial invariants
constructed from the quiver with relations defining these algebras. We also
present a list of normal forms; any such algebra is derived equivalent to one
of the alg... | math.RT | we classify gentle algebras defined by quivers with two cycles under derived equivalence in a non degenerate case by using some combinatorial invariants constructed from the quiver with relations defining these algebras we also present a list of normal forms any such algebra is derived equivalent to one of the algebras... | [['we', 'classify', 'gentle', 'algebras', 'defined', 'by', 'quivers', 'with', 'two', 'cycles', 'under', 'derived', 'equivalence', 'in', 'a', 'non', 'degenerate', 'case', 'by', 'using', 'some', 'combinatorial', 'invariants', 'constructed', 'from', 'the', 'quiver', 'with', 'relations', 'defining', 'these', 'algebras', 'w... | [-0.1581066599012249, 0.07608774017663328, -0.04237604677608168, 0.09550126601674559, -0.08614433187715433, -0.1864659198111406, -0.008391378175777694, 0.3481223205863326, -0.3767611925593681, -0.25586163801899936, 0.1328229587395779, -0.21519217667756257, -0.17331768006638246, 0.19138162721086432, -0.14853217741646976... |
708.384 | Formal analytical solutions for the Gross-Pitaevskii equation | Considering the Gross-Pitaevskii integral equation we are able to formally
obtain an analytical solution for the order parameter $\Phi (x)$ and for the
chemical potential $\mu $ as a function of a unique dimensionless non-linear
parameter $\Lambda $. We report solutions for different range of values for the
repulsive... | cond-mat.other | considering the grosspitaevskii integral equation we are able to formally obtain an analytical solution for the order parameter phi x and for the chemical potential mu as a function of a unique dimensionless nonlinear parameter lambda we report solutions for different range of values for the repulsive and the attractiv... | [['considering', 'the', 'grosspitaevskii', 'integral', 'equation', 'we', 'are', 'able', 'to', 'formally', 'obtain', 'an', 'analytical', 'solution', 'for', 'the', 'order', 'parameter', 'phi', 'x', 'and', 'for', 'the', 'chemical', 'potential', 'mu', 'as', 'a', 'function', 'of', 'a', 'unique', 'dimensionless', 'nonlinear'... | [-0.13733509231135774, 0.03998742097333684, -0.09763359597393863, 0.08952319006760225, -0.06767359294298984, -0.13891967544397732, 0.028411294241816227, 0.3288404290420069, -0.2527768508150754, -0.27613925072036577, 0.05641486154808532, -0.2804709563300696, -0.13271469077829953, 0.18270676708976988, 0.0709829253970947,... |
708.3841 | Mesoscopic gap fluctuations in an unconventional superconductor | We study mesoscopic disorder fluctuations in an anisotropic gap
superconductor, which lead to the spatial variations of the local pairing
temperature and formation of superconducting islands above the mean-field
transition. We derive the probability distribution function of the pairing
temperatures and superconductin... | cond-mat.supr-con cond-mat.dis-nn | we study mesoscopic disorder fluctuations in an anisotropic gap superconductor which lead to the spatial variations of the local pairing temperature and formation of superconducting islands above the meanfield transition we derive the probability distribution function of the pairing temperatures and superconducting gap... | [['we', 'study', 'mesoscopic', 'disorder', 'fluctuations', 'in', 'an', 'anisotropic', 'gap', 'superconductor', 'which', 'lead', 'to', 'the', 'spatial', 'variations', 'of', 'the', 'local', 'pairing', 'temperature', 'and', 'formation', 'of', 'superconducting', 'islands', 'above', 'the', 'meanfield', 'transition', 'we', '... | [-0.19729250495455583, 0.2666257855087358, -0.1082660739775747, 0.11097874084867619, -0.01755971694878741, -0.12819989317315905, 0.06373472920249161, 0.33311480534372523, -0.25110314803382877, -0.26438309707651464, -0.01882117177506991, -0.32501653683207493, -0.12616135879858015, 0.10161351556513075, 0.0212262840051313... |
708.3842 | Triple charged-particle decays of resonances illustrated by 12C-states | The hyperspherical adiabatic expansion is combined with complex scaling and
used to calculate the energy distributions of the particles arising from
three-body decaying low-lying $^{12}$C resonances. The large distance continuum
properties of the wavefunctions are crucial and must be accurately calculated.
The substa... | nucl-th | the hyperspherical adiabatic expansion is combined with complex scaling and used to calculate the energy distributions of the particles arising from threebody decaying lowlying 12c resonances the large distance continuum properties of the wavefunctions are crucial and must be accurately calculated the substantial chang... | [['the', 'hyperspherical', 'adiabatic', 'expansion', 'is', 'combined', 'with', 'complex', 'scaling', 'and', 'used', 'to', 'calculate', 'the', 'energy', 'distributions', 'of', 'the', 'particles', 'arising', 'from', 'threebody', 'decaying', 'lowlying', '12c', 'resonances', 'the', 'large', 'distance', 'continuum', 'proper... | [-0.04088374093001665, 0.2497909406855226, -0.06480421503561787, 0.14971339013996035, 0.040909446174885296, -0.08855786767983159, 0.020369810612633998, 0.30927568328631827, -0.29086573917938524, -0.30556476964117135, 0.014849484574623666, -0.3227996412924556, -0.024417939520072797, 0.12465013392800249, 0.10192648169779... |
708.3843 | Real-time electron dynamics with exact-exchange time-dependent
density-functional theory | The exact exchange potential in time-dependent density-functional theory is
defined as an orbital functional through the time-dependent optimized effective
potential (TDOEP) method. We numerically solve the TDOEP integral equation for
the real-time nonlinear intersubband electron dynamics in a semiconductor
quantum w... | cond-mat.mes-hall | the exact exchange potential in timedependent densityfunctional theory is defined as an orbital functional through the timedependent optimized effective potential tdoep method we numerically solve the tdoep integral equation for the realtime nonlinear intersubband electron dynamics in a semiconductor quantum well with ... | [['the', 'exact', 'exchange', 'potential', 'in', 'timedependent', 'densityfunctional', 'theory', 'is', 'defined', 'as', 'an', 'orbital', 'functional', 'through', 'the', 'timedependent', 'optimized', 'effective', 'potential', 'tdoep', 'method', 'we', 'numerically', 'solve', 'the', 'tdoep', 'integral', 'equation', 'for',... | [-0.1463814583504955, 0.10560200698470397, -0.06119608077258892, 0.12752472678811788, 0.003932012729857066, -0.16273037899821385, 0.04533880933870447, 0.3742118686284513, -0.26466612290744096, -0.3036181385539574, -0.017496576992003885, -0.3096554151493801, -0.18987249124999325, 0.1860473014873593, 0.08621130683395552,... |
708.3844 | Bubbling the False Vacuum Away | We investigate the role of nonperturbative, bubble-like inhomogeneities on
the decay rate of false-vacuum states in two and three-dimensional scalar field
theories. The inhomogeneities are induced by setting up large-amplitude
oscillations of the field about the false vacuum as, for example, after a rapid
quench or i... | hep-th cond-mat.stat-mech hep-lat nlin.PS | we investigate the role of nonperturbative bubblelike inhomogeneities on the decay rate of falsevacuum states in two and threedimensional scalar field theories the inhomogeneities are induced by setting up largeamplitude oscillations of the field about the false vacuum as for example after a rapid quench or in certain ... | [['we', 'investigate', 'the', 'role', 'of', 'nonperturbative', 'bubblelike', 'inhomogeneities', 'on', 'the', 'decay', 'rate', 'of', 'falsevacuum', 'states', 'in', 'two', 'and', 'threedimensional', 'scalar', 'field', 'theories', 'the', 'inhomogeneities', 'are', 'induced', 'by', 'setting', 'up', 'largeamplitude', 'oscill... | [-0.1630756730834643, 0.2641272700486192, -0.07035137140664502, 0.14265904683734465, -0.028780107791333095, -0.1254505900517646, 0.015372210560177547, 0.30839047499804123, -0.2458967961559909, -0.28441677410560456, 0.07301109574694672, -0.21235655231235348, -0.1133005737674598, 0.18244219482100257, 0.03791983267359868,... |
708.3845 | Non-supersymmetric microstates of the D1-D5-KK system | We construct a discrete family of smooth non-supersymmetric three charge
geometries carrying D1 brane, D5 brane and Kaluza-Klein monopole charges in
Type IIB supergravity compactified on a six-torus, which can be interpreted as
the geometric description of some special states of the brane system. These
solutions are ... | hep-th | we construct a discrete family of smooth nonsupersymmetric three charge geometries carrying d1 brane d5 brane and kaluzaklein monopole charges in type iib supergravity compactified on a sixtorus which can be interpreted as the geometric description of some special states of the brane system these solutions are asymptot... | [['we', 'construct', 'a', 'discrete', 'family', 'of', 'smooth', 'nonsupersymmetric', 'three', 'charge', 'geometries', 'carrying', 'd1', 'brane', 'd5', 'brane', 'and', 'kaluzaklein', 'monopole', 'charges', 'in', 'type', 'iib', 'supergravity', 'compactified', 'on', 'a', 'sixtorus', 'which', 'can', 'be', 'interpreted', 'a... | [-0.1619766271042247, 0.11441218038089573, -0.05094467279981942, 0.12185449367708286, -0.08619565907640443, -0.222435416548603, -0.06519589753400895, 0.30496281045376356, -0.08445330620968654, -0.22695543681883493, 0.12213969445738551, -0.3051392121349401, -0.1007327592458516, 0.1319067569894551, -0.1117366559713358, 0... |
708.3846 | Simulating Reionization: Character and Observability | In recent years there has been considerable progress in our understanding of
the nature and properties of the reionization process. In particular, the
numerical simulations of this epoch have made a qualitative leap forward,
reaching sufficiently large scales to derive the characteristic scales of the
reionization pr... | astro-ph | in recent years there has been considerable progress in our understanding of the nature and properties of the reionization process in particular the numerical simulations of this epoch have made a qualitative leap forward reaching sufficiently large scales to derive the characteristic scales of the reionization process... | [['in', 'recent', 'years', 'there', 'has', 'been', 'considerable', 'progress', 'in', 'our', 'understanding', 'of', 'the', 'nature', 'and', 'properties', 'of', 'the', 'reionization', 'process', 'in', 'particular', 'the', 'numerical', 'simulations', 'of', 'this', 'epoch', 'have', 'made', 'a', 'qualitative', 'leap', 'forw... | [-0.04413026251224062, 0.035018551621645216, -0.0880288201576424, 0.06699043345958801, -0.09948522733554008, -0.03158396754842547, 0.01891650836027804, 0.39948418890199966, -0.18498110530033177, -0.3347860281725252, 0.09554004640824768, -0.24664893361789705, -0.09024127082721818, 0.22647177852461084, 0.0728178764878225... |
708.3847 | Tropical Lines on Cubic Surfaces | Given a tropical line $L$ and a smooth tropical surface $X$, we look at the
position of $L$ on $X$. We introduce its primal and dual motif which are
respectively a decorated graph and a subcomplex of the dual triangulation of
$X$. They encode the combinatorial position of $L$ on $X$. We classify all
possible motifs o... | math.AG math.CO | given a tropical line l and a smooth tropical surface x we look at the position of l on x we introduce its primal and dual motif which are respectively a decorated graph and a subcomplex of the dual triangulation of x they encode the combinatorial position of l on x we classify all possible motifs of tropical lines on ... | [['given', 'a', 'tropical', 'line', 'l', 'and', 'a', 'smooth', 'tropical', 'surface', 'x', 'we', 'look', 'at', 'the', 'position', 'of', 'l', 'on', 'x', 'we', 'introduce', 'its', 'primal', 'and', 'dual', 'motif', 'which', 'are', 'respectively', 'a', 'decorated', 'graph', 'and', 'a', 'subcomplex', 'of', 'the', 'dual', 't... | [-0.17902256791078583, 0.05686165463442941, -0.06544511745176543, 0.07557685720465501, -0.08847706192324499, -0.15678984825537215, 0.06711632059508466, 0.35625298085766355, -0.30205288508195216, -0.22104928533478482, 0.09871544634707545, -0.25242577672084676, -0.20518014125707673, 0.18510060582491683, -0.15106031261914... |
708.3848 | The Second Stars | The ejecta of the first probably very massive stars polluted the Big Bang
primordial element mix with the first heavier elements. The resulting ultra
metal-poor abundance distribution provided the initial conditions for the
second stars of a wide range of initial masses reaching down to intermediate
and low masses. T... | astro-ph | the ejecta of the first probably very massive stars polluted the big bang primordial element mix with the first heavier elements the resulting ultra metalpoor abundance distribution provided the initial conditions for the second stars of a wide range of initial masses reaching down to intermediate and low masses the im... | [['the', 'ejecta', 'of', 'the', 'first', 'probably', 'very', 'massive', 'stars', 'polluted', 'the', 'big', 'bang', 'primordial', 'element', 'mix', 'with', 'the', 'first', 'heavier', 'elements', 'the', 'resulting', 'ultra', 'metalpoor', 'abundance', 'distribution', 'provided', 'the', 'initial', 'conditions', 'for', 'the... | [-0.037737570483785926, 0.17490566911650463, -0.07692411973578694, 0.1298233614632346, -0.08318794130076548, -0.06557197217639309, 0.04432281317369671, 0.3569847111496333, -0.19245030172230967, -0.3528621148046931, 0.08727358288467622, -0.282213466883012, -0.04922727176385983, 0.21092427172451045, -0.028443337120461605... |
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