id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
707.393 | Superfluid-Insulator and Roughening Transitions in Domain Walls | We have performed quantum Monte Carlo simulations to investigate the
superfluid behavior of one- and two-dimensional interfaces separating
checkerboard solid domains. The system is described by the hard-core
Bose-Hubbard Hamiltonian with nearest-neighbor interaction. In accordance with
Ref.1, we find that (i) the int... | cond-mat.other cond-mat.stat-mech | we have performed quantum monte carlo simulations to investigate the superfluid behavior of one and twodimensional interfaces separating checkerboard solid domains the system is described by the hardcore bosehubbard hamiltonian with nearestneighbor interaction in accordance with ref1 we find that i the interface remain... | [['we', 'have', 'performed', 'quantum', 'monte', 'carlo', 'simulations', 'to', 'investigate', 'the', 'superfluid', 'behavior', 'of', 'one', 'and', 'twodimensional', 'interfaces', 'separating', 'checkerboard', 'solid', 'domains', 'the', 'system', 'is', 'described', 'by', 'the', 'hardcore', 'bosehubbard', 'hamiltonian', ... | [-0.16405026327717948, 0.256899637656773, -0.009279021142713458, 0.03276075975579285, -0.009509678300772165, -0.20206957208076576, 0.03340244324676491, 0.3678854368794877, -0.23302027682966744, -0.24340004282625946, 0.04260940354439086, -0.3262836332474877, -0.12846107638717905, 0.10497840849665908, 0.06506495196833736... |
707.3931 | Influence of Rb, Cs and Ba on Superconductivity of Magnesium Diboride | Magnesium diboride has been thermally treated in the presence of Rb, Cs, and
Ba. Magnetic susceptibility shows onsets of superconductivity in the resulting
samples at 52K (Rb), 58K (Cs) and 45K (Ba). Room-temperature 11B NMR indicates
to cubic symmetry of the electric field gradient at boron site for the samples
reac... | cond-mat.supr-con | magnesium diboride has been thermally treated in the presence of rb cs and ba magnetic susceptibility shows onsets of superconductivity in the resulting samples at 52k rb 58k cs and 45k ba roomtemperature 11b nmr indicates to cubic symmetry of the electric field gradient at boron site for the samples reacted with rb an... | [['magnesium', 'diboride', 'has', 'been', 'thermally', 'treated', 'in', 'the', 'presence', 'of', 'rb', 'cs', 'and', 'ba', 'magnetic', 'susceptibility', 'shows', 'onsets', 'of', 'superconductivity', 'in', 'the', 'resulting', 'samples', 'at', '52k', 'rb', '58k', 'cs', 'and', '45k', 'ba', 'roomtemperature', '11b', 'nmr', ... | [-0.06310867808578122, 0.1945570562319416, 0.07043273468864047, -0.0939763103120236, 0.07783982843264109, -0.1684367269756169, 0.12955086476479968, 0.4301385620815886, -0.2010996566580919, -0.2916410591505054, -0.028500274698469892, -0.35892186867487097, -0.005453252932056785, 0.06291582855758154, 0.011530009020740787,... |
707.3932 | Photon strength distributions in stable even-even molybdenum isotopes | Electromagnetic dipole-strength distributions up to the particle separation
energies are studied for the stable even-even nuclides $^{92,94,96,98,100}$Mo
in photon scattering experiments at the superconducting electron accelerator
ELBE of the Forschungszentrum Dresden-Rossendorf. The influence of inelastic
transition... | nucl-ex | electromagnetic dipolestrength distributions up to the particle separation energies are studied for the stable eveneven nuclides 92949698100mo in photon scattering experiments at the superconducting electron accelerator elbe of the forschungszentrum dresdenrossendorf the influence of inelastic transitions to lowlying e... | [['electromagnetic', 'dipolestrength', 'distributions', 'up', 'to', 'the', 'particle', 'separation', 'energies', 'are', 'studied', 'for', 'the', 'stable', 'eveneven', 'nuclides', '92949698100mo', 'in', 'photon', 'scattering', 'experiments', 'at', 'the', 'superconducting', 'electron', 'accelerator', 'elbe', 'of', 'the',... | [-0.047473941712125545, 0.24836108008595673, -0.07276765167419064, 0.11939130490033054, 0.049955582236380955, -0.1065297532924696, 0.05560078660614396, 0.36337639226725227, -0.1669926790226447, -0.333973819233085, -0.05987100833169136, -0.3553375475500759, 0.04925999661515418, 0.1717270233521336, 0.1460417065965502, 0.... |
707.3933 | Branching ratio measurement of $K_S\to \gamma \gamma$ decay using a pure
$\ks$ beam in the KLOE detector | We have analyzed 1.62 fb$^{-1}$ of $e^{+}e^{-}$ collisions at a center of
mass energy $\sim M_{\phi}$ collected by the KLOE experiment at DA$\Phi$NE.
This sample corresponds to a production of $\sim$ 1.7 billion of $\ks$ $\kl$
pairs which allowed us to search for the rare $K_S\to \gamma\gamma$ decay.
$K_S$ are tagged... | hep-ex | we have analyzed 162 fb1 of ee collisions at a center of mass energy sim m_phi collected by the kloe experiment at daphine this sample corresponds to a production of sim 17 billion of ks kl pairs which allowed us to search for the rare k_sto gammagamma decay k_s are tagged by the k_l interaction in the calorimeter and ... | [['we', 'have', 'analyzed', '162', 'fb1', 'of', 'ee', 'collisions', 'at', 'a', 'center', 'of', 'mass', 'energy', 'sim', 'm_phi', 'collected', 'by', 'the', 'kloe', 'experiment', 'at', 'daphine', 'this', 'sample', 'corresponds', 'to', 'a', 'production', 'of', 'sim', '17', 'billion', 'of', 'ks', 'kl', 'pairs', 'which', 'a... | [-0.08053110173023015, 0.19261440412083175, -0.05366007629709202, 0.08869447661436425, -0.025716165284393355, -0.09676344829858863, 0.09047784291942662, 0.3008765353442868, -0.17008068309223745, -0.40800592241657796, -0.011483706975013774, -0.44035609003913123, 0.11889680760941701, 0.14781091416625713, 0.08195080841869... |
707.3934 | The Projected Rotational Velocity Distribution of a Sample of OB stars
from a Calibration based on Synthetic He I lines | We derive projected rotational velocities (vsini) for a sample of 156
Galactic OB star members of 35 clusters, HII regions, and associations. The HeI
lines at $\lambda\lambda$4026, 4388, and 4471A were analyzed in order to define
a calibration of the synthetic HeI full-widths at half maximum versus stellar
vsini. A g... | astro-ph | we derive projected rotational velocities vsini for a sample of 156 galactic ob star members of 35 clusters hii regions and associations the hei lines at lambdalambda4026 4388 and 4471a were analyzed in order to define a calibration of the synthetic hei fullwidths at half maximum versus stellar vsini a grid of syntheti... | [['we', 'derive', 'projected', 'rotational', 'velocities', 'vsini', 'for', 'a', 'sample', 'of', '156', 'galactic', 'ob', 'star', 'members', 'of', '35', 'clusters', 'hii', 'regions', 'and', 'associations', 'the', 'hei', 'lines', 'at', 'lambdalambda4026', '4388', 'and', '4471a', 'were', 'analyzed', 'in', 'order', 'to', '... | [0.01204846290020663, 0.08312757085181663, 0.0021770851870561822, 0.11189177127074978, -0.06456940261687348, -0.12721726024756208, 0.1295012633063267, 0.5013169595212849, -0.0868964212110128, -0.37800072109395705, -0.020319752161963096, -0.316541897236473, 0.09724369539626311, 0.19497828783264762, -0.0188499037636283, ... |
707.3935 | A Possibility of Volume Refraction of Negative Relativistic Particles in
Bent Crystals | The volume coherent deflection of high-energy positive and negative particles
in uniformly bent crystals is studied. The general analysis of potential
scattering shows that the standard screening potential for a large class of
collisions can cause the volume refraction for negative particles (antiprotons,
electrons) ... | physics.acc-ph physics.atom-ph physics.gen-ph | the volume coherent deflection of highenergy positive and negative particles in uniformly bent crystals is studied the general analysis of potential scattering shows that the standard screening potential for a large class of collisions can cause the volume refraction for negative particles antiprotons electrons instead... | [['the', 'volume', 'coherent', 'deflection', 'of', 'highenergy', 'positive', 'and', 'negative', 'particles', 'in', 'uniformly', 'bent', 'crystals', 'is', 'studied', 'the', 'general', 'analysis', 'of', 'potential', 'scattering', 'shows', 'that', 'the', 'standard', 'screening', 'potential', 'for', 'a', 'large', 'class', ... | [-0.10016930293015859, 0.2914905468760817, -0.05431962524609709, 0.1280531510473574, -0.022106887513978615, -0.1287836845806817, -0.02179686483685617, 0.32733161706063485, -0.24361282481846433, -0.25613233536757807, -0.05658143537800276, -0.37537120117081535, -0.009091273640040998, 0.18117788927284656, 0.02779018872900... |
707.3936 | Closed form solutions for symmetric water filling games | We study power control in optimization and game frameworks. In the
optimization framework there is a single decision maker who assigns network
resources and in the game framework users share the network resources according
to Nash equilibrium. The solution of these problems is based on so-called
water-filling techniq... | cs.NI cs.GT | we study power control in optimization and game frameworks in the optimization framework there is a single decision maker who assigns network resources and in the game framework users share the network resources according to nash equilibrium the solution of these problems is based on socalled waterfilling technique whi... | [['we', 'study', 'power', 'control', 'in', 'optimization', 'and', 'game', 'frameworks', 'in', 'the', 'optimization', 'framework', 'there', 'is', 'a', 'single', 'decision', 'maker', 'who', 'assigns', 'network', 'resources', 'and', 'in', 'the', 'game', 'framework', 'users', 'share', 'the', 'network', 'resources', 'accord... | [-0.1210837336826792, -0.0025325259375212554, -0.12847188602181825, 0.07332832502260646, -0.09667384980761624, -0.1842619445511794, 0.1129153649877519, 0.3766178736859497, -0.30484443372115494, -0.2902163887039778, 0.0830320100141491, -0.2535913643418524, -0.1967386937571412, 0.12283132114804331, -0.08599937758408487, ... |
707.3937 | Cohomology theories for homotopy algebras and noncommutative geometry | This paper builds a general framework in which to study cohomology theories
of strongly homotopy algebras, namely $A_\infty, C_\infty$ and
$L_\infty$-algebras. This framework is based on noncommutative geometry as
expounded by Connes and Kontsevich. The developed machinery is then used to
establish a general form of ... | math.QA math.AG math.KT | this paper builds a general framework in which to study cohomology theories of strongly homotopy algebras namely a_infty c_infty and l_inftyalgebras this framework is based on noncommutative geometry as expounded by connes and kontsevich the developed machinery is then used to establish a general form of hodge decompos... | [['this', 'paper', 'builds', 'a', 'general', 'framework', 'in', 'which', 'to', 'study', 'cohomology', 'theories', 'of', 'strongly', 'homotopy', 'algebras', 'namely', 'a_infty', 'c_infty', 'and', 'l_inftyalgebras', 'this', 'framework', 'is', 'based', 'on', 'noncommutative', 'geometry', 'as', 'expounded', 'by', 'connes',... | [-0.11688791096642398, 0.009733090551732026, -0.14612182626244274, 0.08439932186392717, -0.1478989733302075, -0.14962092963168802, -0.03971327561716401, 0.2880124363616325, -0.3427137048051193, -0.2309954053438876, 0.06853784995821668, -0.10910227962270164, -0.2538018967164174, 0.13988400874254497, -0.25862711987903586... |
707.3938 | On the conundrum of deriving exact solutions from approximate master
equations | We derive the exact time-evolution for a general quantum system under the
influence of pure phase-noise and demonstrate that for a Gaussian initial state
of the bath, the exact result can be obtained also within a perturbative
time-local master equation approach already in second order of the system-bath
coupling str... | quant-ph cond-mat.stat-mech | we derive the exact timeevolution for a general quantum system under the influence of pure phasenoise and demonstrate that for a gaussian initial state of the bath the exact result can be obtained also within a perturbative timelocal master equation approach already in second order of the systembath coupling strength w... | [['we', 'derive', 'the', 'exact', 'timeevolution', 'for', 'a', 'general', 'quantum', 'system', 'under', 'the', 'influence', 'of', 'pure', 'phasenoise', 'and', 'demonstrate', 'that', 'for', 'a', 'gaussian', 'initial', 'state', 'of', 'the', 'bath', 'the', 'exact', 'result', 'can', 'be', 'obtained', 'also', 'within', 'a',... | [-0.11396495635598534, 0.11406688827158111, -0.15553262345947144, 0.08760924788799546, -0.01731283363045716, -0.13508499988422887, 0.06676109603935534, 0.3272337818904439, -0.2696448373239169, -0.2509859845087659, 0.03733166244602194, -0.2074952735111299, -0.11678905983273757, 0.1801060520015975, 0.018688398240156834, ... |
707.3939 | Star Formation in Massive Low Surface Brightness Galaxies | Massive low surface brightness galaxies have disk central surface
brightnesses at least one magnitude fainter than the night sky, but total
magnitudes and masses that show they are among the largest galaxies known. Like
all low surface brightness (LSB) galaxies, massive LSB galaxies are often in
the midst of star for... | astro-ph | massive low surface brightness galaxies have disk central surface brightnesses at least one magnitude fainter than the night sky but total magnitudes and masses that show they are among the largest galaxies known like all low surface brightness lsb galaxies massive lsb galaxies are often in the midst of star formation ... | [['massive', 'low', 'surface', 'brightness', 'galaxies', 'have', 'disk', 'central', 'surface', 'brightnesses', 'at', 'least', 'one', 'magnitude', 'fainter', 'than', 'the', 'night', 'sky', 'but', 'total', 'magnitudes', 'and', 'masses', 'that', 'show', 'they', 'are', 'among', 'the', 'largest', 'galaxies', 'known', 'like'... | [-0.03745515468159553, 0.09430523516472292, -0.05189832724561846, 0.12214755747743226, -0.09711801031328461, -0.02566964403829641, 0.033263981839021045, 0.45812771066040214, -0.12081191008306902, -0.360041826232164, 0.08710496936864393, -0.3093570506269181, -0.06420626893156657, 0.19505758291041408, -0.0628248693800910... |
707.394 | A proposal for the missing mass: it is just the outer, far one | The paper has benn withdrawn because the computation of the external virial
contains an error which invalidate the main result.
| astro-ph | the paper has benn withdrawn because the computation of the external virial contains an error which invalidate the main result | [['the', 'paper', 'has', 'benn', 'withdrawn', 'because', 'the', 'computation', 'of', 'the', 'external', 'virial', 'contains', 'an', 'error', 'which', 'invalidate', 'the', 'main', 'result']] | [-0.1600492350757122, -0.05406952724661096, -0.09442511424422265, -0.015166631154716014, -0.05239870548248291, -0.06462686527520418, 0.009315367607632652, 0.2208967201411724, -0.24183067549020051, -0.33095440370962026, 0.11997319315560162, -0.2652361995540559, -0.08644516551867128, 0.1487858820706606, -0.21533543991245... |
707.3941 | Dynamics of the Chain of Oscillators with Long-Range Interaction: From
Synchronization to Chaos | We consider a chain of nonlinear oscillators with long-range interaction of
the type 1/l^{1+alpha}, where l is a distance between oscillators and 0< alpha
<2. In the continues limit the system's dynamics is described by the
Ginzburg-Landau equation with complex coefficients. Such a system has a new
parameter alpha th... | nlin.CD nlin.PS | we consider a chain of nonlinear oscillators with longrange interaction of the type 1l1alpha where l is a distance between oscillators and 0 alpha 2 in the continues limit the systems dynamics is described by the ginzburglandau equation with complex coefficients such a system has a new parameter alpha that is responsib... | [['we', 'consider', 'a', 'chain', 'of', 'nonlinear', 'oscillators', 'with', 'longrange', 'interaction', 'of', 'the', 'type', '1l1alpha', 'where', 'l', 'is', 'a', 'distance', 'between', 'oscillators', 'and', '0', 'alpha', '2', 'in', 'the', 'continues', 'limit', 'the', 'systems', 'dynamics', 'is', 'described', 'by', 'the... | [-0.21079308068850539, 0.19194689056334588, -0.06020964100793168, 0.021005680079694715, -0.016313544807157347, -0.1364583935547661, 0.026109456105137263, 0.3088419066721594, -0.3012691319480047, -0.2500173155586798, 0.06205972563859157, -0.2886907656441678, -0.20023102021090441, 0.18150346262564698, 0.03229161417418784... |
707.3942 | Mach Cones and Hydrodynamic Flow: Probing Big Bang Matter in the
Laboratory | A critical discussion of the present signals for the phase transition to
quark-gluon plasma (QGP) is given. Since hadronic rescattering models predict
much larger flow than observed from 1 to 50 A GeV laboratory bombarding
energies, this observation is interpreted as potential evidence for a
first-order phase transit... | hep-th | a critical discussion of the present signals for the phase transition to quarkgluon plasma qgp is given since hadronic rescattering models predict much larger flow than observed from 1 to 50 a gev laboratory bombarding energies this observation is interpreted as potential evidence for a firstorder phase transition at h... | [['a', 'critical', 'discussion', 'of', 'the', 'present', 'signals', 'for', 'the', 'phase', 'transition', 'to', 'quarkgluon', 'plasma', 'qgp', 'is', 'given', 'since', 'hadronic', 'rescattering', 'models', 'predict', 'much', 'larger', 'flow', 'than', 'observed', 'from', '1', 'to', '50', 'a', 'gev', 'laboratory', 'bombard... | [-0.096738150072679, 0.24465169756941763, -0.17134390533682328, 0.1214106965167643, -0.043931592714787505, -0.06125112460848159, -0.053698212748237384, 0.33703092007327295, -0.2244820074953568, -0.2871173571073572, -0.019442025175883743, -0.30939908030793967, 0.05848580044791766, 0.13912842701145336, 0.0600721081377480... |
707.3943 | Simulations of turbulent convection in rotating young solar-like stars:
Differential rotation and meridional circulation | We present the results of three-dimensional simulations of the deep
convective envelope of a young (10 Myr) one-solar-mass star, obtained with the
Anelastic Spherical Harmonic code. Since young stars are known to be faster
rotators than their main sequence counterparts, we have systematically studied
the impact of th... | astro-ph | we present the results of threedimensional simulations of the deep convective envelope of a young 10 myr onesolarmass star obtained with the anelastic spherical harmonic code since young stars are known to be faster rotators than their main sequence counterparts we have systematically studied the impact of the stellar ... | [['we', 'present', 'the', 'results', 'of', 'threedimensional', 'simulations', 'of', 'the', 'deep', 'convective', 'envelope', 'of', 'a', 'young', '10', 'myr', 'onesolarmass', 'star', 'obtained', 'with', 'the', 'anelastic', 'spherical', 'harmonic', 'code', 'since', 'young', 'stars', 'are', 'known', 'to', 'be', 'faster', ... | [-0.11559051026935727, 0.17770110275676712, -0.04966287391068787, 0.10708397934877006, -0.06395992721595309, -0.04372599894366316, 0.008857335163621713, 0.3769889818968007, -0.2466973465492283, -0.3273870160053084, 0.08457388093155636, -0.21564586648961942, -0.11711933680839533, 0.2222060243866714, -0.05383177817829703... |
707.3944 | Non-Relativistic Strings in Expanding Spacetime | We obtain a non-relativistic diffeomorphism invariant string action as a
special limit of the Nambu-Goto action in an FLRW background. We use this
action to study non-relativistic string dynamics in an expanding universe and
construct an analytic model describing the macroscopic properties of
non-relativistic string ... | astro-ph gr-qc hep-th | we obtain a nonrelativistic diffeomorphism invariant string action as a special limit of the nambugoto action in an flrw background we use this action to study nonrelativistic string dynamics in an expanding universe and construct an analytic model describing the macroscopic properties of nonrelativistic string network... | [['we', 'obtain', 'a', 'nonrelativistic', 'diffeomorphism', 'invariant', 'string', 'action', 'as', 'a', 'special', 'limit', 'of', 'the', 'nambugoto', 'action', 'in', 'an', 'flrw', 'background', 'we', 'use', 'this', 'action', 'to', 'study', 'nonrelativistic', 'string', 'dynamics', 'in', 'an', 'expanding', 'universe', 'a... | [-0.17156410699185892, 0.2109433984722181, -0.12159683923589207, 0.14280191083740004, -0.08037067655505252, -0.16006601731754652, -0.02241905265636429, 0.3091653737419543, -0.2372965734577229, -0.29820085628380794, -0.0022762914735064725, -0.24520990979748175, -0.05706561517612148, 0.1308789327642841, -0.00692544906535... |
707.3945 | k-Disjunctive cuts and a finite cutting plane algorithm for general
mixed integer linear programs | In this paper we give a generalization of the well known split cuts of Cook,
Kannan and Schrijver to cuts which are based on multi-term disjunctions. They
will be called k-disjunctive cuts. The starting point is the question what kind
of cuts is needed for a finite cutting plane algorithm for general mixed
integer pr... | math.OC | in this paper we give a generalization of the well known split cuts of cook kannan and schrijver to cuts which are based on multiterm disjunctions they will be called kdisjunctive cuts the starting point is the question what kind of cuts is needed for a finite cutting plane algorithm for general mixed integer programs ... | [['in', 'this', 'paper', 'we', 'give', 'a', 'generalization', 'of', 'the', 'well', 'known', 'split', 'cuts', 'of', 'cook', 'kannan', 'and', 'schrijver', 'to', 'cuts', 'which', 'are', 'based', 'on', 'multiterm', 'disjunctions', 'they', 'will', 'be', 'called', 'kdisjunctive', 'cuts', 'the', 'starting', 'point', 'is', 'th... | [-0.10210105811891425, 0.10342938235010375, -0.14239853744385475, 0.11267257979158889, -0.17490452702742876, -0.12807592187921718, 0.09657564935077596, 0.37727866221468936, -0.317627671181906, -0.3021952458129255, 0.1533184027330489, -0.24574311369473173, -0.13284371875840978, 0.18812751566712774, -0.12826693537357003,... |
707.3946 | Implementing universal quantum gates in coupled cavities | We study a linear array of coupled cavities interacting with two level
systems and show how to construct individually addressable qubits in this
system from the long-lived atom-photon excitations (polaritons) at each site.
We derive the system dynamics and show that is described by an XY Hamiltonian.
We proceed by sh... | quant-ph | we study a linear array of coupled cavities interacting with two level systems and show how to construct individually addressable qubits in this system from the longlived atomphoton excitations polaritons at each site we derive the system dynamics and show that is described by an xy hamiltonian we proceed by showing ho... | [['we', 'study', 'a', 'linear', 'array', 'of', 'coupled', 'cavities', 'interacting', 'with', 'two', 'level', 'systems', 'and', 'show', 'how', 'to', 'construct', 'individually', 'addressable', 'qubits', 'in', 'this', 'system', 'from', 'the', 'longlived', 'atomphoton', 'excitations', 'polaritons', 'at', 'each', 'site', '... | [-0.14545728599643046, 0.18368688342056463, 0.010358172898497624, 0.04378698211278498, 0.038589198965598474, -0.24086074641972935, 0.047736481487386156, 0.4131094700532015, -0.25867486942665097, -0.281470202797659, 0.01420760717598203, -0.30014104464273783, -0.159800768160194, 0.1997264147659322, 0.01731843516001353, 0... |
707.3947 | A computation of invariants of a rational self-map | I compute the dynamical degrees in C. Voisin's example of a rational self-map
of the variety of lines on a cubic fourfold.
| math.AG | i compute the dynamical degrees in c voisins example of a rational selfmap of the variety of lines on a cubic fourfold | [['i', 'compute', 'the', 'dynamical', 'degrees', 'in', 'c', 'voisins', 'example', 'of', 'a', 'rational', 'selfmap', 'of', 'the', 'variety', 'of', 'lines', 'on', 'a', 'cubic', 'fourfold']] | [-0.2783781580457633, -0.004279993813146244, -0.05756422335451299, -0.043770463967865166, -0.04729974176734686, -0.13869548752501776, 0.06451014954258096, 0.2917648262598298, -0.2744947759942575, -0.20294830171306702, 0.06589171503649348, -0.2482059895992279, -0.17799453742124818, 0.22473217259076508, -0.04072126636112... |
707.3948 | Potential density of rational points on the variety of lines of a cubic
fourfold | We prove the potential density of rational points on the variety of lines of
a sufficiently general cubic fourfold defined over a number field, where
``sufficiently general'' means that a condition of Terasoma type is satisfied.
These varieties have trivial canonical bundle and have geometric Picard group
equal to $\... | math.AG | we prove the potential density of rational points on the variety of lines of a sufficiently general cubic fourfold defined over a number field where sufficiently general means that a condition of terasoma type is satisfied these varieties have trivial canonical bundle and have geometric picard group equal to mathbbz | [['we', 'prove', 'the', 'potential', 'density', 'of', 'rational', 'points', 'on', 'the', 'variety', 'of', 'lines', 'of', 'a', 'sufficiently', 'general', 'cubic', 'fourfold', 'defined', 'over', 'a', 'number', 'field', 'where', 'sufficiently', 'general', 'means', 'that', 'a', 'condition', 'of', 'terasoma', 'type', 'is', ... | [-0.2392908018437447, 0.065213268045336, -0.08220050521194935, 0.020599913701880725, -0.0991318606864661, -0.19227762549184263, 0.030903179813176394, 0.3157303724065423, -0.2622012117318809, -0.21006859134882688, 0.07080308016389608, -0.20564219295978547, -0.1615279148425907, 0.2030693786405027, -0.10363532911986112, -... |
707.3949 | Nonequilibrium Renormalization Theory I | In the present article we consider some general class of divergent diagrams
in Keldysh diagram technique. These divergences arise for nonequilibrium matter
and closely related to the divergences in the kinetic theory of gases. We
suggest a scheme of renormalization of such divergences and illustrate it on
some exampl... | cond-mat.stat-mech math-ph math.MP | in the present article we consider some general class of divergent diagrams in keldysh diagram technique these divergences arise for nonequilibrium matter and closely related to the divergences in the kinetic theory of gases we suggest a scheme of renormalization of such divergences and illustrate it on some examples i... | [['in', 'the', 'present', 'article', 'we', 'consider', 'some', 'general', 'class', 'of', 'divergent', 'diagrams', 'in', 'keldysh', 'diagram', 'technique', 'these', 'divergences', 'arise', 'for', 'nonequilibrium', 'matter', 'and', 'closely', 'related', 'to', 'the', 'divergences', 'in', 'the', 'kinetic', 'theory', 'of', ... | [-0.11956807196694465, 0.13160666007517782, -0.18135314239542605, 0.09806416539113569, -0.0482960326504732, -0.08596571874304497, 0.055309796279627246, 0.3219747224068346, -0.28006159234022304, -0.25048288378156414, 0.042216415688287746, -0.28686447078862404, -0.20306122119053582, 0.17784537651291318, -0.08213367836919... |
707.395 | Ramanujan's Harmonic Number Expansion into Negative Powers of a
Triangular Number | An algebraic transformation of the DeTemple-Wang half-integer approximation
to the harmonic series produces the general formula and error estimate for the
Ramanujan expansion for the nth harmonic number into negative powers of the nth
triangular number. We also discuss the history of the Ramanujan expansion for
the n... | math.CA math.GM | an algebraic transformation of the detemplewang halfinteger approximation to the harmonic series produces the general formula and error estimate for the ramanujan expansion for the nth harmonic number into negative powers of the nth triangular number we also discuss the history of the ramanujan expansion for the nth ha... | [['an', 'algebraic', 'transformation', 'of', 'the', 'detemplewang', 'halfinteger', 'approximation', 'to', 'the', 'harmonic', 'series', 'produces', 'the', 'general', 'formula', 'and', 'error', 'estimate', 'for', 'the', 'ramanujan', 'expansion', 'for', 'the', 'nth', 'harmonic', 'number', 'into', 'negative', 'powers', 'of... | [-0.12673890482384356, 0.045756788604408294, -0.05969473626464605, 0.08427198774948277, -0.0945480208405677, -0.07268435759332907, 0.01311432323692476, 0.304123153197853, -0.26514559428152795, -0.27290398835697594, 0.09042257808751482, -0.3014386538279188, -0.13910965533560718, 0.2587661209879169, -0.007004410938166342... |
707.3951 | Symplectic $C_\infty$-algebras | In this paper we show that a strongly homotopy commutative (or $C_\infty$-)
algebra with an invariant inner product on its cohomology can be uniquely
extended to a symplectic $C_\infty$-algebra (an $\infty$-generalisation of a
commutative Frobenius algebra introduced by Kontsevich). This result relies on
the algebrai... | math.QA math.AG math.KT | in this paper we show that a strongly homotopy commutative or c_infty algebra with an invariant inner product on its cohomology can be uniquely extended to a symplectic c_inftyalgebra an inftygeneralisation of a commutative frobenius algebra introduced by kontsevich this result relies on the algebraic hodge decompositi... | [['in', 'this', 'paper', 'we', 'show', 'that', 'a', 'strongly', 'homotopy', 'commutative', 'or', 'c_infty', 'algebra', 'with', 'an', 'invariant', 'inner', 'product', 'on', 'its', 'cohomology', 'can', 'be', 'uniquely', 'extended', 'to', 'a', 'symplectic', 'c_inftyalgebra', 'an', 'inftygeneralisation', 'of', 'a', 'commut... | [-0.2031790829684225, 0.041938642994219046, -0.1540334206975756, 0.04729326415972243, -0.17753573660288127, -0.11914797958677574, -0.07932642839601144, 0.31760889063439063, -0.46063615285581155, -0.1869284906875222, 0.1183426664041866, -0.12257373564305805, -0.1791231057103423, 0.15071844451895525, -0.2921434846075793,... |
707.3952 | Threshold Resummation Effects in the Associated Production of Chargino
and Neutralino at Hadron Colliders | We investigate the QCD effects in the associated production of the chargino
and the neutralino, $\tilde\chi^\pm_{1}$ and $\tilde\chi^0_{2}$, in the Minimal
Supersymmetric Standard Model (MSSM) at both the Fermilab Tevatron and the CERN
Large Hadron Collider (LHC). We include the next-to-leading order (NLO) QCD
correc... | hep-ph | we investigate the qcd effects in the associated production of the chargino and the neutralino tildechipm_1 and tildechi0_2 in the minimal supersymmetric standard model mssm at both the fermilab tevatron and the cern large hadron collider lhc we include the nexttoleading order nlo qcd corrections including supersymmetr... | [['we', 'investigate', 'the', 'qcd', 'effects', 'in', 'the', 'associated', 'production', 'of', 'the', 'chargino', 'and', 'the', 'neutralino', 'tildechipm_1', 'and', 'tildechi0_2', 'in', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'mssm', 'at', 'both', 'the', 'fermilab', 'tevatron', 'and', 'the', 'cern', 'l... | [-0.013131898514035604, 0.2050229703258399, -0.080547097635091, 0.17154730994092382, 0.008824457281161154, -0.05816828348484916, -0.0017819316463841908, 0.2897978433052692, -0.14687035126152678, -0.3069435691838895, 0.021616177526268893, -0.4254676147289844, 0.07725028529007366, 0.1373520637634615, 0.0879941709285629, ... |
707.3953 | Stable modification of relative curves | We generalize theorems of Deligne-Mumford and de Jong on semi-stable
modifications of families of proper curves. The main result states that after a
generically \'etale alteration of the base any (not necessarily proper) family
of multipointed curves with semi-stable generic fiber admits a minimal
semi-stable modific... | math.AG | we generalize theorems of delignemumford and de jong on semistable modifications of families of proper curves the main result states that after a generically etale alteration of the base any not necessarily proper family of multipointed curves with semistable generic fiber admits a minimal semistable modification the l... | [['we', 'generalize', 'theorems', 'of', 'delignemumford', 'and', 'de', 'jong', 'on', 'semistable', 'modifications', 'of', 'families', 'of', 'proper', 'curves', 'the', 'main', 'result', 'states', 'that', 'after', 'a', 'generically', 'etale', 'alteration', 'of', 'the', 'base', 'any', 'not', 'necessarily', 'proper', 'fami... | [-0.18654103584301013, 0.07743923235070574, -0.1962744152930739, 0.04766637393513919, -0.1249258431124982, -0.13801222975662614, 0.0040243046414516455, 0.32701645074616914, -0.2882488697030387, -0.1747806720783586, 0.11431792824129973, -0.180958351325039, -0.13997824751812923, 0.2595789133069607, -0.20313238221537935, ... |
707.3954 | Challenging SO(10) SUSY GUTs with family symmetries through FCNC
processes | We perform a detailed analysis of the SO(10) SUSY GUT model with D3 family
symmetry of Dermisek and Raby (DR). The model is specified in terms of 24
parameters and predicts, as a function of them, the whole MSSM set of
parameters at low energy scales. Concerning the SM subset of such parameters,
the model is able to ... | hep-ph | we perform a detailed analysis of the so10 susy gut model with d3 family symmetry of dermisek and raby dr the model is specified in terms of 24 parameters and predicts as a function of them the whole mssm set of parameters at low energy scales concerning the sm subset of such parameters the model is able to give a sati... | [['we', 'perform', 'a', 'detailed', 'analysis', 'of', 'the', 'so10', 'susy', 'gut', 'model', 'with', 'd3', 'family', 'symmetry', 'of', 'dermisek', 'and', 'raby', 'dr', 'the', 'model', 'is', 'specified', 'in', 'terms', 'of', '24', 'parameters', 'and', 'predicts', 'as', 'a', 'function', 'of', 'them', 'the', 'whole', 'mss... | [-0.09056852436191294, 0.16611536475721486, -0.01579101201211817, 0.12761121708876894, -0.0586203274652795, -0.1893310083661142, 0.11198210802882216, 0.277945644042433, -0.2385118782720637, -0.3217862947649041, 0.050736604798801765, -0.25745066821271945, -0.0465229524840969, 0.1007628321948158, 0.008828431674614981, 0.... |
707.3955 | Quantum breathers in capacitively coupled Josephson junctions:
Correlations, number conservation, and entanglement | We consider the classical and quantum dynamics of excitations in a system of
two capacitively coupled Josephson junctions. In the classical case the
equations of motion admit discrete breather solutions, which are time periodic
and localized predominantly on one of the junctions. In the quantum case
breather states a... | cond-mat.mes-hall cond-mat.other | we consider the classical and quantum dynamics of excitations in a system of two capacitively coupled josephson junctions in the classical case the equations of motion admit discrete breather solutions which are time periodic and localized predominantly on one of the junctions in the quantum case breather states are fo... | [['we', 'consider', 'the', 'classical', 'and', 'quantum', 'dynamics', 'of', 'excitations', 'in', 'a', 'system', 'of', 'two', 'capacitively', 'coupled', 'josephson', 'junctions', 'in', 'the', 'classical', 'case', 'the', 'equations', 'of', 'motion', 'admit', 'discrete', 'breather', 'solutions', 'which', 'are', 'time', 'p... | [-0.23831160723903153, 0.2154693279447857, -0.06731710601922904, 0.07785212097494582, 0.028336099172985657, -0.16144180873159839, 0.03705704471821962, 0.31949438607904973, -0.24322012739342658, -0.2612483625971647, 0.014958186067646196, -0.3322743862206766, -0.08385090029332787, 0.2016055471816122, 0.04929442048007839,... |
707.3956 | On the regularity of geodesic rays associated to test configurations | Geodesic rays of class C^{1,1} are constructed for any test configuration of
a positive line bundle L on X using resolution of singularities. The
construction reduces to finding a subsolution of the corresponding Monge-Ampere
equation. Geometrically, this is accomplished by the use a positive line bundle
on the resol... | math.DG math.CV | geodesic rays of class c11 are constructed for any test configuration of a positive line bundle l on x using resolution of singularities the construction reduces to finding a subsolution of the corresponding mongeampere equation geometrically this is accomplished by the use a positive line bundle on the resolution whic... | [['geodesic', 'rays', 'of', 'class', 'c11', 'are', 'constructed', 'for', 'any', 'test', 'configuration', 'of', 'a', 'positive', 'line', 'bundle', 'l', 'on', 'x', 'using', 'resolution', 'of', 'singularities', 'the', 'construction', 'reduces', 'to', 'finding', 'a', 'subsolution', 'of', 'the', 'corresponding', 'mongeamper... | [-0.2130967133204665, -0.002797584059615538, -0.048375126301196586, 0.03714500295137169, -0.14679794888453265, -0.15546518498051323, 0.027531017496234232, 0.35021802488910525, -0.2566946314304675, -0.20406113623788483, 0.10867501855337698, -0.2591389416994756, -0.06070406006224323, 0.2075862995299854, -0.07344958076678... |
707.3957 | Stretched-exponential decay functions from a self-consistent model of
dielectric relaxation | There are many materials whose dielectric properties are described by a
stretched exponential, the so-called Kohlrausch-Williams-Watts (KWW) relaxation
function. Its physical origin and statistical-mechanical foundation have been a
matter of debate in the literature. In this paper we suggest a model of
dielectric rel... | cond-mat.mtrl-sci cond-mat.stat-mech | there are many materials whose dielectric properties are described by a stretched exponential the socalled kohlrauschwilliamswatts kww relaxation function its physical origin and statisticalmechanical foundation have been a matter of debate in the literature in this paper we suggest a model of dielectric relaxation whi... | [['there', 'are', 'many', 'materials', 'whose', 'dielectric', 'properties', 'are', 'described', 'by', 'a', 'stretched', 'exponential', 'the', 'socalled', 'kohlrauschwilliamswatts', 'kww', 'relaxation', 'function', 'its', 'physical', 'origin', 'and', 'statisticalmechanical', 'foundation', 'have', 'been', 'a', 'matter', ... | [-0.13086752908820487, 0.14424101529216551, -0.12288930278316319, 0.0811163988862052, -0.0699274543313736, -0.11558029264301421, -0.02822340225537184, 0.3455963001378913, -0.2989790921705405, -0.24326883945389685, 0.06116699826684836, -0.2606088009225317, -0.17965072756969785, 0.1608339920836355, 0.031947004207667995, ... |
707.3958 | Control parameters in turbulence, Self Organized Criticality and
ecosystems | From the starting point of the well known Reynolds number of fluid turbulence
we propose a control parameter $R$ for a wider class of systems including
avalanche models that show Self Organized Criticality (SOC) and ecosystems. $R$
is related to the driving and dissipation rates and from similarity analysis we
obtain... | physics.bio-ph physics.gen-ph | from the starting point of the well known reynolds number of fluid turbulence we propose a control parameter r for a wider class of systems including avalanche models that show self organized criticality soc and ecosystems r is related to the driving and dissipation rates and from similarity analysis we obtain a relati... | [['from', 'the', 'starting', 'point', 'of', 'the', 'well', 'known', 'reynolds', 'number', 'of', 'fluid', 'turbulence', 'we', 'propose', 'a', 'control', 'parameter', 'r', 'for', 'a', 'wider', 'class', 'of', 'systems', 'including', 'avalanche', 'models', 'that', 'show', 'self', 'organized', 'criticality', 'soc', 'and', '... | [-0.178524294133032, 0.15060139034183176, -0.07085646785174807, 0.02303373758082411, -0.022852171000669753, -0.17005716352806693, 0.05690250993661937, 0.30607411341652985, -0.28651835790702274, -0.2980878218121472, 0.06507301971682214, -0.2570907183013679, -0.1285997760193866, 0.17830060280282936, -0.026364292668932605... |
707.3959 | Four-Group Decodable Space-Time Block Codes | Two new rate-one full-diversity space-time block codes (STBC) are proposed.
They are characterized by the \emph{lowest decoding complexity} among the known
rate-one STBC, arising due to the complete separability of the transmitted
symbols into four groups for maximum likelihood detection. The first and the
second cod... | cs.IT math.IT | two new rateone fulldiversity spacetime block codes stbc are proposed they are characterized by the emphlowest decoding complexity among the known rateone stbc arising due to the complete separability of the transmitted symbols into four groups for maximum likelihood detection the first and the second codes are delayop... | [['two', 'new', 'rateone', 'fulldiversity', 'spacetime', 'block', 'codes', 'stbc', 'are', 'proposed', 'they', 'are', 'characterized', 'by', 'the', 'emphlowest', 'decoding', 'complexity', 'among', 'the', 'known', 'rateone', 'stbc', 'arising', 'due', 'to', 'the', 'complete', 'separability', 'of', 'the', 'transmitted', 's... | [-0.22799224579254182, 0.02389772083810487, 0.014952096487526025, 0.08588041112949706, -0.033843349867770184, -0.2718336311621574, 0.03982387469846442, 0.3586159056992592, -0.2581386710778227, -0.31526864921482645, 0.14040891894478805, -0.2456738586215494, -0.15011108828116662, 0.21019306081721437, -0.11721817416217283... |
707.396 | P-V-T equation of state of epsilon iron and its densities at core
conditions | The author's new p-V-T Equation of State is tested against the available
experiments of epsilon iron. The root-mean-square-deviations (RMSD) of the
molar volume, pressure, and temperature are 0.021 cm3, 2.0 GPa and 144.9 K
respectively. Separating the experiments into 200 K ranges the new EoS was
compared to the most... | physics.gen-ph | the authors new pvt equation of state is tested against the available experiments of epsilon iron the rootmeansquaredeviations rmsd of the molar volume pressure and temperature are 0021 cm3 20 gpa and 1449 k respectively separating the experiments into 200 k ranges the new eos was compared to the most widely used finit... | [['the', 'authors', 'new', 'pvt', 'equation', 'of', 'state', 'is', 'tested', 'against', 'the', 'available', 'experiments', 'of', 'epsilon', 'iron', 'the', 'rootmeansquaredeviations', 'rmsd', 'of', 'the', 'molar', 'volume', 'pressure', 'and', 'temperature', 'are', '0021', 'cm3', '20', 'gpa', 'and', '1449', 'k', 'respect... | [-0.052420866614233494, 0.13980068062503254, -0.08748507648447736, 0.06574865262599713, -0.04125017075178524, -0.1207778734226142, 0.07241820540447305, 0.3428762296680361, -0.18559846627774984, -0.3457452698364957, 0.10164254132218452, -0.32257003754946506, -0.005087160371153409, 0.20088808800048558, 0.0492431861962864... |
707.3961 | Atomistic Simulations of the Mechanical Properties of 'Super' Carbon
Nanotubes | The mechanical properties of the so-called `super' carbon nanotubes (STs) are
investigated using classical molecular dynamics simulations. The STs are built
from single walled carbon nanotubes (SWCNTs) connected by Y-like junctions
forming an ordered carbon nanotube network that is then rolled into a seamless
cylinde... | cond-mat.mtrl-sci | the mechanical properties of the socalled super carbon nanotubes sts are investigated using classical molecular dynamics simulations the sts are built from single walled carbon nanotubes swcnts connected by ylike junctions forming an ordered carbon nanotube network that is then rolled into a seamless cylinder we observ... | [['the', 'mechanical', 'properties', 'of', 'the', 'socalled', 'super', 'carbon', 'nanotubes', 'sts', 'are', 'investigated', 'using', 'classical', 'molecular', 'dynamics', 'simulations', 'the', 'sts', 'are', 'built', 'from', 'single', 'walled', 'carbon', 'nanotubes', 'swcnts', 'connected', 'by', 'ylike', 'junctions', 'f... | [-0.12903801772139362, 0.1675582109234686, -0.069534227322485, -0.018107847561318398, -0.03652607800432708, -0.15556441553037714, 0.05090195685373367, 0.43124333783178714, -0.30121949082995586, -0.27531854554104646, 0.022054256106147894, -0.27884521932920087, -0.16552949339101042, 0.19727941969459928, -0.01059764981571... |
707.3962 | Coherent Bayesian analysis of inspiral signals | We present in this paper a Bayesian parameter estimation method for the
analysis of interferometric gravitational wave observations of an inspiral of
binary compact objects using data recorded simultaneously by a network of
several interferometers at different sites. We consider neutron star or black
hole inspirals t... | gr-qc | we present in this paper a bayesian parameter estimation method for the analysis of interferometric gravitational wave observations of an inspiral of binary compact objects using data recorded simultaneously by a network of several interferometers at different sites we consider neutron star or black hole inspirals that... | [['we', 'present', 'in', 'this', 'paper', 'a', 'bayesian', 'parameter', 'estimation', 'method', 'for', 'the', 'analysis', 'of', 'interferometric', 'gravitational', 'wave', 'observations', 'of', 'an', 'inspiral', 'of', 'binary', 'compact', 'objects', 'using', 'data', 'recorded', 'simultaneously', 'by', 'a', 'network', '... | [-0.10428495702346684, 0.10535985719640545, -0.056354475161060694, 0.08171134918682381, -0.07056932278339648, -0.08564990935847164, 0.02003821314428933, 0.3987364840486811, -0.21881369299565753, -0.368816473800689, 0.1452346446768691, -0.2826021845866409, -0.12181398814621693, 0.24548578595406273, -0.02348570299283084,... |
707.3963 | On the quantization of conjugacy classes | Let G be a compact, simple, simply connected Lie group. A theorem of
Freed-Hopkins-Teleman identifies the level k fusion ring R_k(G) of G with the
twisted equivariant K-homology at level k+h, where h is the dual Coxeter
number. In this paper, we review this result using the language of
Dixmier-Douady bundles. We show... | math.DG | let g be a compact simple simply connected lie group a theorem of freedhopkinsteleman identifies the level k fusion ring r_kg of g with the twisted equivariant khomology at level kh where h is the dual coxeter number in this paper we review this result using the language of dixmierdouady bundles we show that the additi... | [['let', 'g', 'be', 'a', 'compact', 'simple', 'simply', 'connected', 'lie', 'group', 'a', 'theorem', 'of', 'freedhopkinsteleman', 'identifies', 'the', 'level', 'k', 'fusion', 'ring', 'r_kg', 'of', 'g', 'with', 'the', 'twisted', 'equivariant', 'khomology', 'at', 'level', 'kh', 'where', 'h', 'is', 'the', 'dual', 'coxeter... | [-0.22617244884371757, 0.11394360245127852, -0.06414444021259745, -0.001794170819533368, -0.11503919629380106, -0.11280921937276919, 0.00967420339739571, 0.36984705716371535, -0.34604063381751377, -0.23476555803169807, 0.05268370295253893, -0.1831718383356929, -0.14129166834056378, 0.201014789827168, -0.184932305241624... |
707.3964 | Universality in quantum chaos and the one parameter scaling theory | We adapt the one parameter scaling theory (OPT) to the context of quantum
chaos. As a result we propose a more precise characterization of the
universality classes associated to Wigner-Dyson and Poisson statistics which
takes into account Anderson localization effects. Based also on the OPT we
predict a new universal... | cond-mat.dis-nn cond-mat.mes-hall nlin.CD quant-ph | we adapt the one parameter scaling theory opt to the context of quantum chaos as a result we propose a more precise characterization of the universality classes associated to wignerdyson and poisson statistics which takes into account anderson localization effects based also on the opt we predict a new universality cla... | [['we', 'adapt', 'the', 'one', 'parameter', 'scaling', 'theory', 'opt', 'to', 'the', 'context', 'of', 'quantum', 'chaos', 'as', 'a', 'result', 'we', 'propose', 'a', 'more', 'precise', 'characterization', 'of', 'the', 'universality', 'classes', 'associated', 'to', 'wignerdyson', 'and', 'poisson', 'statistics', 'which', ... | [-0.10255122723663637, 0.16460268358098326, -0.08757817105851672, 0.10906862494416238, -0.034543065446948185, -0.18115793904536856, 0.08275929134054752, 0.31331057080059455, -0.2364333113325776, -0.2560576983950043, 0.06924495691293439, -0.25523558324944656, -0.22723603472772952, 0.20235474136311857, -0.029159014558304... |
707.3965 | Haar Wavelets and the Origin of Gravitational Inertia | Spacetime is considered to be everywhere Minkowski except at the location
where a signal wave of energy interacts with the gravitational field. The
conformal metric f[k(x-vt)]Nuv is suitably chosen to represent this
interaction, where f[k(x-vt)]is a generalized wave or signal function.
Parametrized and Taylor expande... | physics.gen-ph | spacetime is considered to be everywhere minkowski except at the location where a signal wave of energy interacts with the gravitational field the conformal metric fkxvtnuv is suitably chosen to represent this interaction where fkxvtis a generalized wave or signal function parametrized and taylor expanded at zero the s... | [['spacetime', 'is', 'considered', 'to', 'be', 'everywhere', 'minkowski', 'except', 'at', 'the', 'location', 'where', 'a', 'signal', 'wave', 'of', 'energy', 'interacts', 'with', 'the', 'gravitational', 'field', 'the', 'conformal', 'metric', 'fkxvtnuv', 'is', 'suitably', 'chosen', 'to', 'represent', 'this', 'interaction... | [-0.15739285640531417, 0.1516467955414996, -0.13458313102071937, 0.07470943401990966, -0.15097648436203598, -0.1124590072802014, -0.05582127362828363, 0.29378328217249927, -0.2929864825455077, -0.22213876534140473, 0.06090737675373076, -0.2825852124543444, -0.11761884048270682, 0.13372258934418135, 0.010304351055035086... |
707.3966 | Bose-Einstein condensation of diquark molecules in three-flavor quark
matter | We study the phase diagram of strongly interacting matter with three quark
flavors at low and intermediate densities and non-zero temperatures in the
framework of an NJL-type model with four-point interactions. At large
densities, when the interactions are weak due to asymptotic freedom, quarks
form loosely bound Coo... | nucl-th | we study the phase diagram of strongly interacting matter with three quark flavors at low and intermediate densities and nonzero temperatures in the framework of an njltype model with fourpoint interactions at large densities when the interactions are weak due to asymptotic freedom quarks form loosely bound cooper pair... | [['we', 'study', 'the', 'phase', 'diagram', 'of', 'strongly', 'interacting', 'matter', 'with', 'three', 'quark', 'flavors', 'at', 'low', 'and', 'intermediate', 'densities', 'and', 'nonzero', 'temperatures', 'in', 'the', 'framework', 'of', 'an', 'njltype', 'model', 'with', 'fourpoint', 'interactions', 'at', 'large', 'de... | [-0.15585672805072182, 0.3514705725621991, -0.05726004394245449, 0.09882117556764941, -0.001000467151867389, -0.1623808816585173, 0.08642898840034367, 0.3522306439215249, -0.17729770403736048, -0.2888176168049992, -0.025077086966824685, -0.3196454202402791, -0.03946078499357631, 0.05706625339833435, 0.10193054530987122... |
707.3967 | Curvaton reheating allows TeV Hubble scale in NO inflation | Curvaton reheating is studied in non-oscillatory (NO) models of inflation,
with the aim to obtain bounds on the parameters of curvaton models and find out
whether low scale inflation can be attained. Using a minimal curvaton model, it
is found that the allowed parameter space is considerably larger than in the
case o... | hep-ph astro-ph hep-th | curvaton reheating is studied in nonoscillatory no models of inflation with the aim to obtain bounds on the parameters of curvaton models and find out whether low scale inflation can be attained using a minimal curvaton model it is found that the allowed parameter space is considerably larger than in the case of the us... | [['curvaton', 'reheating', 'is', 'studied', 'in', 'nonoscillatory', 'no', 'models', 'of', 'inflation', 'with', 'the', 'aim', 'to', 'obtain', 'bounds', 'on', 'the', 'parameters', 'of', 'curvaton', 'models', 'and', 'find', 'out', 'whether', 'low', 'scale', 'inflation', 'can', 'be', 'attained', 'using', 'a', 'minimal', 'c... | [-0.11370004298320661, 0.2527325349834023, -0.09786462227606939, 0.19245806981214425, -0.09224978816928342, -0.2031086105077217, -0.040329615145714745, 0.2987396069090917, -0.20417095952951866, -0.3131735753785405, 0.12274580490096317, -0.17692957819801652, -0.09066911442722711, 0.22030414500881712, -0.0192497003655363... |
707.3968 | Phenomenology for Supernova Ia Data Based on a New Cosmic Time | A new phenomenological theory for the expansion of our universe is presented.
Because fundamental supporting theory is still in development, its discussion
is not presented in this paper. The theory is based on a new algebraic
expression for cosmic time G Rho t^2=3/32Pi, which correctly predicts the WMAP
measured cos... | physics.gen-ph | a new phenomenological theory for the expansion of our universe is presented because fundamental supporting theory is still in development its discussion is not presented in this paper the theory is based on a new algebraic expression for cosmic time g rho t2332pi which correctly predicts the wmap measured cosmological... | [['a', 'new', 'phenomenological', 'theory', 'for', 'the', 'expansion', 'of', 'our', 'universe', 'is', 'presented', 'because', 'fundamental', 'supporting', 'theory', 'is', 'still', 'in', 'development', 'its', 'discussion', 'is', 'not', 'presented', 'in', 'this', 'paper', 'the', 'theory', 'is', 'based', 'on', 'a', 'new',... | [-0.11462730227038265, 0.13729910933928166, -0.11493800899878677, 0.10696318616425353, -0.13169698659330606, -0.10758133431630475, 0.0007466097774782351, 0.32971920748906475, -0.18936729258192436, -0.3039547293333869, 0.03943409439109798, -0.24065810263156892, -0.06830682163259813, 0.2153743695241532, -0.00382414954315... |
707.3969 | Inference on inspiral signals using LISA MLDC data | In this paper we describe a Bayesian inference framework for analysis of data
obtained by LISA. We set up a model for binary inspiral signals as defined for
the Mock LISA Data Challenge 1.2 (MLDC), and implemented a Markov chain Monte
Carlo (MCMC) algorithm to facilitate exploration and integration of the
posterior d... | gr-qc | in this paper we describe a bayesian inference framework for analysis of data obtained by lisa we set up a model for binary inspiral signals as defined for the mock lisa data challenge 12 mldc and implemented a markov chain monte carlo mcmc algorithm to facilitate exploration and integration of the posterior distributi... | [['in', 'this', 'paper', 'we', 'describe', 'a', 'bayesian', 'inference', 'framework', 'for', 'analysis', 'of', 'data', 'obtained', 'by', 'lisa', 'we', 'set', 'up', 'a', 'model', 'for', 'binary', 'inspiral', 'signals', 'as', 'defined', 'for', 'the', 'mock', 'lisa', 'data', 'challenge', '12', 'mldc', 'and', 'implemented'... | [-0.05582575880792699, 0.057009945205070925, -0.11031281958699604, 0.10652059081741432, -0.08004758422133289, -0.052465916169170713, 0.0941584691968216, 0.40283805320534527, -0.27870057208487126, -0.37737325291278995, 0.1337731804955114, -0.23133356559172838, -0.1333406126904714, 0.2700551176720735, 0.01874170665735308... |
707.397 | Minimum-error discrimination between mixed quantum states | We derive a general lower bound on the minimum-error probability for {\it
ambiguous discrimination} between arbitrary $m$ mixed quantum states with given
prior probabilities. When $m=2$, this bound is precisely the well-known
Helstrom limit. Also, we give a general lower bound on the minimum-error
probability for dis... | quant-ph | we derive a general lower bound on the minimumerror probability for it ambiguous discrimination between arbitrary m mixed quantum states with given prior probabilities when m2 this bound is precisely the wellknown helstrom limit also we give a general lower bound on the minimumerror probability for discriminating quant... | [['we', 'derive', 'a', 'general', 'lower', 'bound', 'on', 'the', 'minimumerror', 'probability', 'for', 'it', 'ambiguous', 'discrimination', 'between', 'arbitrary', 'm', 'mixed', 'quantum', 'states', 'with', 'given', 'prior', 'probabilities', 'when', 'm2', 'this', 'bound', 'is', 'precisely', 'the', 'wellknown', 'helstro... | [-0.10260927700279217, 0.20578200001979158, -0.10302686312736399, 0.15146311983105024, 0.008554524637530652, -0.2669123276865401, 0.16931298476814918, 0.293872405914273, -0.18345402685614923, -0.32596055914958316, 0.07127463176757806, -0.20033364961570016, -0.12364688178613073, 0.17908681940357044, -0.10704458005517264... |
707.3971 | Quantum Flexoelectricity in Low Dimensional Systems | Symmetry breaking at surfaces and interfaces and the capability to support
large strain gradients in nanoscale systems enable new forms of
electromechanical coupling. Here we introduce the concept of quantum
flexoelectricity, a phenomenon that is manifested when the mechanical
deformation of non-polar quantum systems... | cond-mat.mtrl-sci | symmetry breaking at surfaces and interfaces and the capability to support large strain gradients in nanoscale systems enable new forms of electromechanical coupling here we introduce the concept of quantum flexoelectricity a phenomenon that is manifested when the mechanical deformation of nonpolar quantum systems resu... | [['symmetry', 'breaking', 'at', 'surfaces', 'and', 'interfaces', 'and', 'the', 'capability', 'to', 'support', 'large', 'strain', 'gradients', 'in', 'nanoscale', 'systems', 'enable', 'new', 'forms', 'of', 'electromechanical', 'coupling', 'here', 'we', 'introduce', 'the', 'concept', 'of', 'quantum', 'flexoelectricity', '... | [-0.16540437131375074, 0.16945116711780428, -0.03309443702921271, -0.0067298009973019365, -0.03806148122251034, -0.13352685919776558, 0.020278355196118356, 0.3685586143732071, -0.2767494263574481, -0.27996004350483417, 0.038039632637053726, -0.2702163325548172, -0.2120303163677454, 0.2031883368100971, -0.00020100433006... |
707.3972 | Learning Probabilistic Models of Word Sense Disambiguation | This dissertation presents several new methods of supervised and unsupervised
learning of word sense disambiguation models. The supervised methods focus on
performing model searches through a space of probabilistic models, and the
unsupervised methods rely on the use of Gibbs Sampling and the Expectation
Maximization... | cs.CL cs.AI | this dissertation presents several new methods of supervised and unsupervised learning of word sense disambiguation models the supervised methods focus on performing model searches through a space of probabilistic models and the unsupervised methods rely on the use of gibbs sampling and the expectation maximization em ... | [['this', 'dissertation', 'presents', 'several', 'new', 'methods', 'of', 'supervised', 'and', 'unsupervised', 'learning', 'of', 'word', 'sense', 'disambiguation', 'models', 'the', 'supervised', 'methods', 'focus', 'on', 'performing', 'model', 'searches', 'through', 'a', 'space', 'of', 'probabilistic', 'models', 'and', ... | [0.001965163609920404, -0.017086186975901887, -0.10119807093929595, 0.11000029081239915, -0.11464459401292679, -0.17480236200544125, 0.0835440910110871, 0.44740251552027005, -0.26691074448619756, -0.3060628299553616, 0.058576629732926495, -0.2248373011676356, -0.16525462538433763, 0.18929935893258795, -0.11464847738329... |
707.3973 | Transient current in a quantum dot asymmetrically coupled to metallic
leads | The time-dependent non-crossing approximation is used to study the transient
current in a single electron transistor attached asymmetrically to two leads
following a sudden change in the energy of the dot level. We show that for
asymmetric coupling, sharp features in the density of states of the leads can
induce osci... | cond-mat.str-el | the timedependent noncrossing approximation is used to study the transient current in a single electron transistor attached asymmetrically to two leads following a sudden change in the energy of the dot level we show that for asymmetric coupling sharp features in the density of states of the leads can induce oscillatio... | [['the', 'timedependent', 'noncrossing', 'approximation', 'is', 'used', 'to', 'study', 'the', 'transient', 'current', 'in', 'a', 'single', 'electron', 'transistor', 'attached', 'asymmetrically', 'to', 'two', 'leads', 'following', 'a', 'sudden', 'change', 'in', 'the', 'energy', 'of', 'the', 'dot', 'level', 'we', 'show',... | [-0.1887466559814389, 0.20805197013708362, -0.04105643596267328, 0.07282281169942248, 0.013017182171876942, -0.13184862114056678, 0.09344066649750207, 0.33372948256562396, -0.2693673682972855, -0.30300464456377085, 0.041792816968934075, -0.2912961747081551, -0.07587871048183713, 0.22663290256293425, -0.0058230885562287... |
707.3974 | Peculiar Nature of Snake States in Graphene | We study the dynamics of the electrons in a non-uniform magnetic field
applied perpendicular to a graphene sheet in the low energy limit when the
excitation states can be described by a Dirac type Hamiltonian. We show that as
compared to the two-dimensional electron gas (2DEG) snake states in graphene
exibit peculiar... | cond-mat.mes-hall | we study the dynamics of the electrons in a nonuniform magnetic field applied perpendicular to a graphene sheet in the low energy limit when the excitation states can be described by a dirac type hamiltonian we show that as compared to the twodimensional electron gas 2deg snake states in graphene exibit peculiar proper... | [['we', 'study', 'the', 'dynamics', 'of', 'the', 'electrons', 'in', 'a', 'nonuniform', 'magnetic', 'field', 'applied', 'perpendicular', 'to', 'a', 'graphene', 'sheet', 'in', 'the', 'low', 'energy', 'limit', 'when', 'the', 'excitation', 'states', 'can', 'be', 'described', 'by', 'a', 'dirac', 'type', 'hamiltonian', 'we',... | [-0.1723161732054797, 0.25870940939748216, -0.05705715791061836, 0.08071779593000568, 0.02681295510768196, -0.09975506911464667, 0.06650198801712653, 0.3410774137098658, -0.28569622351580803, -0.2734255848562945, -0.007312572955832643, -0.285318760580178, -0.1191689503671191, 0.133590401986898, 0.030162203571585527, 0.... |
707.3975 | Peeling Bifurcations of Toroidal Chaotic Attractors | Chaotic attractors with toroidal topology (van der Pol attractor) have
counterparts with symmetry that exhibit unfamiliar phenomena. We investigate
double covers of toroidal attractors, discuss changes in their morphology under
correlated peeling bifurcations, describe their topological structures and the
changes und... | nlin.CD | chaotic attractors with toroidal topology van der pol attractor have counterparts with symmetry that exhibit unfamiliar phenomena we investigate double covers of toroidal attractors discuss changes in their morphology under correlated peeling bifurcations describe their topological structures and the changes undergone ... | [['chaotic', 'attractors', 'with', 'toroidal', 'topology', 'van', 'der', 'pol', 'attractor', 'have', 'counterparts', 'with', 'symmetry', 'that', 'exhibit', 'unfamiliar', 'phenomena', 'we', 'investigate', 'double', 'covers', 'of', 'toroidal', 'attractors', 'discuss', 'changes', 'in', 'their', 'morphology', 'under', 'cor... | [-0.19712460802734963, 0.10531355012018158, -0.11116700528227554, 0.09484589694790085, -0.049771134922166865, -0.16308732125765588, 0.011945079400308659, 0.31371087185582336, -0.27716986040527725, -0.24128251374528117, 0.07887681892346021, -0.25812607865818604, -0.2423962980166686, 0.2066446120755115, -0.10441795384929... |
707.3976 | Spin transport in proximity induced ferromagnetic graphene | Magnetic gates in close proximity to graphene can induce ferromagnetic
correlations. We study the effect of such induced magnetization dependent
Zeeman splittings on the graphene transport properties. We estimate that
induced spin splittings of the order of \Delta ~ 5 meV could be achieved with
the use of magnetic in... | cond-mat.mes-hall | magnetic gates in close proximity to graphene can induce ferromagnetic correlations we study the effect of such induced magnetization dependent zeeman splittings on the graphene transport properties we estimate that induced spin splittings of the order of delta 5 mev could be achieved with the use of magnetic insulator... | [['magnetic', 'gates', 'in', 'close', 'proximity', 'to', 'graphene', 'can', 'induce', 'ferromagnetic', 'correlations', 'we', 'study', 'the', 'effect', 'of', 'such', 'induced', 'magnetization', 'dependent', 'zeeman', 'splittings', 'on', 'the', 'graphene', 'transport', 'properties', 'we', 'estimate', 'that', 'induced', '... | [-0.19853257722056963, 0.239584637894843, 0.0026758781442528263, 0.04257655426558545, -0.04069596707332119, -0.14860750782056986, 0.07337963973130922, 0.43026488553732634, -0.3123950224253349, -0.3562108121045372, -0.038705182820729746, -0.2897052177200642, -0.13232771649842, 0.2289019972770749, 0.0357861693996443, 0.0... |
707.3977 | The worm-like chain model at small and large stretch | The relation between force and stretch in the worm-like chain model of
entropic elasticity is examined. Although no closed-form expression is valid
for all values of forcing, solutions in the form of asymptotic series can be
obtained under conditions of small and large applied force. The small and large
stretch limit... | cond-mat.mtrl-sci | the relation between force and stretch in the wormlike chain model of entropic elasticity is examined although no closedform expression is valid for all values of forcing solutions in the form of asymptotic series can be obtained under conditions of small and large applied force the small and large stretch limits corre... | [['the', 'relation', 'between', 'force', 'and', 'stretch', 'in', 'the', 'wormlike', 'chain', 'model', 'of', 'entropic', 'elasticity', 'is', 'examined', 'although', 'no', 'closedform', 'expression', 'is', 'valid', 'for', 'all', 'values', 'of', 'forcing', 'solutions', 'in', 'the', 'form', 'of', 'asymptotic', 'series', 'c... | [-0.16805510830671824, 0.06903111335197967, -0.07457830032007289, 0.06533677088572, -0.04874536659827782, -0.11590484361711544, 0.023955291319523276, 0.3410504524471219, -0.2714216231186058, -0.2553555180640296, 0.1326241565690635, -0.25057118090311276, -0.13547753527299644, 0.2345650338534189, -0.004770241898590142, 0... |
707.3978 | M5-branes and Wilson Surfaces | We investigate the M5-brane description of the Wilson surface operators in
six-dimensional (2,0) superconformal field theory from AdS/CFT correspondence.
We consider the Wilson surface operators in high-dimensional representation,
whose description could be M5-brane string soliton solutions in $AdS_7\times
S^4$ backg... | hep-th | we investigate the m5brane description of the wilson surface operators in sixdimensional 20 superconformal field theory from adscft correspondence we consider the wilson surface operators in highdimensional representation whose description could be m5brane string soliton solutions in ads_7times s4 background we constru... | [['we', 'investigate', 'the', 'm5brane', 'description', 'of', 'the', 'wilson', 'surface', 'operators', 'in', 'sixdimensional', '20', 'superconformal', 'field', 'theory', 'from', 'adscft', 'correspondence', 'we', 'consider', 'the', 'wilson', 'surface', 'operators', 'in', 'highdimensional', 'representation', 'whose', 'de... | [-0.1754051908960958, 0.10069834775487452, -0.08726105640495294, 0.13689394520693704, -0.09835739213801724, -0.11054459121078253, -0.04605892515055051, 0.33149334908414047, -0.17273106861026272, -0.24500238896028972, 0.12153722121729515, -0.30768113601094993, -0.23127354669237607, 0.10419283885704844, -0.11759011750722... |
707.3979 | Clifford Algebra of the Vector Space of Conics for decision boundary
Hyperplanes in m-Euclidean Space | In this paper we embed $m$-dimensional Euclidean space in the geometric
algebra $Cl_m $ to extend the operators of incidence in ${R^m}$ to operators of
incidence in the geometric algebra to generalize the notion of separator to a
decision boundary hyperconic in the Clifford algebra of hyperconic sections
denoted as $... | cs.NE cs.CG | in this paper we embed mdimensional euclidean space in the geometric algebra cl_m to extend the operators of incidence in rm to operators of incidence in the geometric algebra to generalize the notion of separator to a decision boundary hyperconic in the clifford algebra of hyperconic sections denoted as clco_2 this al... | [['in', 'this', 'paper', 'we', 'embed', 'mdimensional', 'euclidean', 'space', 'in', 'the', 'geometric', 'algebra', 'cl_m', 'to', 'extend', 'the', 'operators', 'of', 'incidence', 'in', 'rm', 'to', 'operators', 'of', 'incidence', 'in', 'the', 'geometric', 'algebra', 'to', 'generalize', 'the', 'notion', 'of', 'separator',... | [-0.10356650963836324, 0.08006793985906471, -0.08351556277678658, 0.06856514382606191, -0.14347265454772343, -0.14614194027833743, -0.007326436616292792, 0.3574349687243941, -0.3155339801515866, -0.21980177011573687, 0.10152765294737441, -0.24291333306700835, -0.18401258506896234, 0.16192769302061708, -0.15837893691989... |
707.398 | Deep Chandra and multicolor HST observations of the jets of 3C 371 and
PKS 2201+044 | This paper presents multiwavelength imaging and broad-band spectroscopy of
the relativistic jets in the two nearby radio galaxies 3C 371 and PKS 2201+044,
acquired with Chandra, HST, VLA, and Merlin. Radio polarization images are also
available. The two sources stand out as "intermediate'' between FRIs and FRIIs;
the... | astro-ph | this paper presents multiwavelength imaging and broadband spectroscopy of the relativistic jets in the two nearby radio galaxies 3c 371 and pks 2201044 acquired with chandra hst vla and merlin radio polarization images are also available the two sources stand out as intermediate between fris and friis their cores are c... | [['this', 'paper', 'presents', 'multiwavelength', 'imaging', 'and', 'broadband', 'spectroscopy', 'of', 'the', 'relativistic', 'jets', 'in', 'the', 'two', 'nearby', 'radio', 'galaxies', '3c', '371', 'and', 'pks', '2201044', 'acquired', 'with', 'chandra', 'hst', 'vla', 'and', 'merlin', 'radio', 'polarization', 'images', ... | [-0.031584020605997035, 0.10107358023714906, -0.0725079030560994, 0.12800776855121448, -0.11990225632070449, -0.10955141173071113, -0.0005284306145278596, 0.5774211685734185, -0.16807865770261365, -0.3422344974323846, 0.04073940781190207, -0.3037526994529698, 0.07488090616285975, 0.19426672916882534, 0.0339308379174411... |
707.3981 | Representations of Clifford algebras with hyperbolic numbers | The representations of Clifford algebras and their involutions and
anti-involutions are fully investigated since decades. However, these
representations do sometimes not comply with usual conventions within physics.
A few simple examples are presented, which point out that the hyperbolic
numbers can close this gap.
| math-ph gr-qc hep-th math.MP | the representations of clifford algebras and their involutions and antiinvolutions are fully investigated since decades however these representations do sometimes not comply with usual conventions within physics a few simple examples are presented which point out that the hyperbolic numbers can close this gap | [['the', 'representations', 'of', 'clifford', 'algebras', 'and', 'their', 'involutions', 'and', 'antiinvolutions', 'are', 'fully', 'investigated', 'since', 'decades', 'however', 'these', 'representations', 'do', 'sometimes', 'not', 'comply', 'with', 'usual', 'conventions', 'within', 'physics', 'a', 'few', 'simple', 'ex... | [-0.1052503527819433, 0.16012413340715945, -0.06189817198636857, 0.1276357804970096, -0.123619555326348, -0.16560332308819686, 0.026641324321231383, 0.42141649237071926, -0.32766212666915223, -0.3042821946807883, 0.13606420155106622, -0.26448280935768376, -0.15921517287973652, 0.20836235263480127, -0.10821879782650451,... |
707.3982 | Interpretations for the X(4160) observed in the double charm production
at B factories | Belle Collaboration has recently observed a new state, the X(4160), in the
process of double charm production $e^+e^-\to J/\psi+X(4160)$ followed by
$X(4160)\to D^*\bar{D^*}$. We discuss possible interpretations for the X(4160)
based on the NRQCD calculations and the potential model estimates for the
charmonium spect... | hep-ph hep-ex | belle collaboration has recently observed a new state the x4160 in the process of double charm production eeto jpsix4160 followed by x4160to dbard we discuss possible interpretations for the x4160 based on the nrqcd calculations and the potential model estimates for the charmonium spectrum we first focus on the dwave s... | [['belle', 'collaboration', 'has', 'recently', 'observed', 'a', 'new', 'state', 'the', 'x4160', 'in', 'the', 'process', 'of', 'double', 'charm', 'production', 'eeto', 'jpsix4160', 'followed', 'by', 'x4160to', 'dbard', 'we', 'discuss', 'possible', 'interpretations', 'for', 'the', 'x4160', 'based', 'on', 'the', 'nrqcd', ... | [-0.07047344700657521, 0.2206082091933139, -0.08809531630335928, 0.15511349151675116, -0.054960150380524014, -0.15698424682098752, 0.08089559227529983, 0.32732489088946887, -0.1848211685169695, -0.23028777310779938, -0.008310997308365552, -0.33168463049353, -0.001111971534555778, 0.15039906831872132, 0.0577677296629796... |
707.3983 | Signatures of gravitational fixed points at the LHC | We study quantum-gravitational signatures at the Large Hadron Collider (LHC)
in the context of theories with extra spatial dimensions and a low fundamental
Planck scale in the TeV range. Implications of a gravitational fixed point at
high energies are worked out using Wilson's renormalisation group. We find that
rele... | hep-ph gr-qc hep-th | we study quantumgravitational signatures at the large hadron collider lhc in the context of theories with extra spatial dimensions and a low fundamental planck scale in the tev range implications of a gravitational fixed point at high energies are worked out using wilsons renormalisation group we find that relevant cro... | [['we', 'study', 'quantumgravitational', 'signatures', 'at', 'the', 'large', 'hadron', 'collider', 'lhc', 'in', 'the', 'context', 'of', 'theories', 'with', 'extra', 'spatial', 'dimensions', 'and', 'a', 'low', 'fundamental', 'planck', 'scale', 'in', 'the', 'tev', 'range', 'implications', 'of', 'a', 'gravitational', 'fix... | [-0.10393828189131828, 0.256147111276499, -0.08970835941055647, 0.17570547552522606, -0.07647753893457448, -0.13817906533129132, -0.015567794648142388, 0.30558605718975645, -0.2027425025888265, -0.29274937584518623, 0.05055551347024261, -0.29909876049854434, -0.01695943912730003, 0.19242345899916613, 0.0990048958740841... |
707.3984 | Coarse-Grained Finite-Temperature Theory for the Condensate in Optical
Lattices | In this work, we derive a coarse-grained finite-temperature theory for a Bose
condensate in a one-dimensional optical lattice, in addition to a confining
harmonic trap potential. We start from a two-particle irreducible (2PI)
effective action on the Schwinger-Keldysh closed-time contour path. In
principle, this actio... | cond-mat.other | in this work we derive a coarsegrained finitetemperature theory for a bose condensate in a onedimensional optical lattice in addition to a confining harmonic trap potential we start from a twoparticle irreducible 2pi effective action on the schwingerkeldysh closedtime contour path in principle this action involves all ... | [['in', 'this', 'work', 'we', 'derive', 'a', 'coarsegrained', 'finitetemperature', 'theory', 'for', 'a', 'bose', 'condensate', 'in', 'a', 'onedimensional', 'optical', 'lattice', 'in', 'addition', 'to', 'a', 'confining', 'harmonic', 'trap', 'potential', 'we', 'start', 'from', 'a', 'twoparticle', 'irreducible', '2pi', 'e... | [-0.1391213387903276, 0.20805866118926264, -0.13364548997836556, 0.07412179947576535, -0.021670877852517624, -0.0860026659126785, 0.039409665870570224, 0.319545290671325, -0.24207153884190077, -0.22351335004367978, -0.019872038807677204, -0.251116890311781, -0.12274747000723753, 0.11363202542660461, 0.02244240998522185... |
707.3985 | Direct Observation of Second Order Atom Tunnelling | Tunnelling of material particles through a classically impenetrable barrier
constitutes one of the hallmark effects of quantum physics. When interactions
between the particles compete with their mobility through a tunnel junction,
intriguing novel dynamical behaviour can arise where particles do not tunnel
independen... | cond-mat.other quant-ph | tunnelling of material particles through a classically impenetrable barrier constitutes one of the hallmark effects of quantum physics when interactions between the particles compete with their mobility through a tunnel junction intriguing novel dynamical behaviour can arise where particles do not tunnel independently ... | [['tunnelling', 'of', 'material', 'particles', 'through', 'a', 'classically', 'impenetrable', 'barrier', 'constitutes', 'one', 'of', 'the', 'hallmark', 'effects', 'of', 'quantum', 'physics', 'when', 'interactions', 'between', 'the', 'particles', 'compete', 'with', 'their', 'mobility', 'through', 'a', 'tunnel', 'junctio... | [-0.18311553402973169, 0.2132392018403202, -0.015440208834214982, 0.04715100390885544, -0.006489001582799987, -0.19461409655907613, 0.09841794981875203, 0.36176586652343923, -0.2697837816873057, -0.2977013705636967, -0.04237406961916184, -0.3249364838410507, -0.1004138585950502, 0.16946038847535172, 0.06171530131081288... |
707.3986 | Mixed States Markov Random Fields with Symbolic Labels and
Multidimensional Real Values | New theoretical results are presented here on the recently introduced model
called mixed states MRF. Such models were introduced in the context of image
motion analysis and are useful to represent information which can take both
discrete values accounting for symbolic states, and real values corresponding
to continuo... | math.PR | new theoretical results are presented here on the recently introduced model called mixed states mrf such models were introduced in the context of image motion analysis and are useful to represent information which can take both discrete values accounting for symbolic states and real values corresponding to continuous m... | [['new', 'theoretical', 'results', 'are', 'presented', 'here', 'on', 'the', 'recently', 'introduced', 'model', 'called', 'mixed', 'states', 'mrf', 'such', 'models', 'were', 'introduced', 'in', 'the', 'context', 'of', 'image', 'motion', 'analysis', 'and', 'are', 'useful', 'to', 'represent', 'information', 'which', 'can'... | [-0.041045349472690194, 0.11454486031462216, -0.1071715832599217, 0.09204550998706726, -0.06717421410250522, -0.12968506899972757, -0.00460239241919702, 0.33066219817847015, -0.2988594132165114, -0.30174261434447197, 0.11193081553071915, -0.22481023528435756, -0.13126867149202598, 0.18015394888463473, -0.06830934336675... |
707.3987 | Controlling passively-quenched single photon detectors by bright light | Single photon detectors based on passively-quenched avalanche photodiodes can
be temporarily blinded by relatively bright light, of intensity less than a
nanowatt. I describe a bright-light regime suitable for attacking a quantum key
distribution system containing such detectors. In this regime, all single
photon det... | quant-ph | single photon detectors based on passivelyquenched avalanche photodiodes can be temporarily blinded by relatively bright light of intensity less than a nanowatt i describe a brightlight regime suitable for attacking a quantum key distribution system containing such detectors in this regime all single photon detectors i... | [['single', 'photon', 'detectors', 'based', 'on', 'passivelyquenched', 'avalanche', 'photodiodes', 'can', 'be', 'temporarily', 'blinded', 'by', 'relatively', 'bright', 'light', 'of', 'intensity', 'less', 'than', 'a', 'nanowatt', 'i', 'describe', 'a', 'brightlight', 'regime', 'suitable', 'for', 'attacking', 'a', 'quantu... | [-0.10681700861459831, 0.17024613546467057, -0.11865278224043625, 0.06353439392538955, -0.0441093985051945, -0.33813813218148425, 0.06259280582283584, 0.3750223813888927, -0.22144213357629874, -0.31615906427517376, 0.06461022736342177, -0.3538352506730007, -0.06998026438062273, 0.2024484148114425, -0.11856647075910587,... |
707.3988 | Minimizing the ground state energy of an electron in a randomly deformed
lattice | We provide a characterization of the spectral minimum for a random
Schr\"odinger operator of the form $H=-\Delta + \sum_{i \in
\Z^d}q(x-i-\omega_i)$ in $L^2(\R^d)$, where the single site potential $q$ is
reflection symmetric, compactly supported in the unit cube centered at 0, and
the displacement parameters $\omega_... | math-ph math.MP | we provide a characterization of the spectral minimum for a random schrodinger operator of the form hdelta sum_i in zdqxiomega_i in l2rd where the single site potential q is reflection symmetric compactly supported in the unit cube centered at 0 and the displacement parameters omega_i are restricted so that adjacent si... | [['we', 'provide', 'a', 'characterization', 'of', 'the', 'spectral', 'minimum', 'for', 'a', 'random', 'schrodinger', 'operator', 'of', 'the', 'form', 'hdelta', 'sum_i', 'in', 'zdqxiomega_i', 'in', 'l2rd', 'where', 'the', 'single', 'site', 'potential', 'q', 'is', 'reflection', 'symmetric', 'compactly', 'supported', 'in'... | [-0.11804146148235152, 0.08960841412970513, -0.05038250261595892, 0.03924060665517168, -0.07010683888345176, -0.13351421973409608, 0.008874410016740142, 0.4054181401603197, -0.2962659182824214, -0.17906423024979484, 0.12026386082486898, -0.2897600915736436, -0.13119681872164157, 0.14575580362150084, -0.0621854871686996... |
707.3989 | Regularly varying multivariate time series | A multivariate, stationary time series is said to be jointly regularly
varying if all its finite-dimensional distributions are multivariate regularly
varying. This property is shown to be equivalent to weak convergence of the
conditional distribution of the rescaled series given that, at a fixed time
instant, its dis... | math.PR math.ST stat.TH | a multivariate stationary time series is said to be jointly regularly varying if all its finitedimensional distributions are multivariate regularly varying this property is shown to be equivalent to weak convergence of the conditional distribution of the rescaled series given that at a fixed time instant its distance t... | [['a', 'multivariate', 'stationary', 'time', 'series', 'is', 'said', 'to', 'be', 'jointly', 'regularly', 'varying', 'if', 'all', 'its', 'finitedimensional', 'distributions', 'are', 'multivariate', 'regularly', 'varying', 'this', 'property', 'is', 'shown', 'to', 'be', 'equivalent', 'to', 'weak', 'convergence', 'of', 'th... | [-0.10469232528303388, 0.13914393626239224, -0.15452720691229552, 0.05479252148604128, -0.05519733149096199, -0.11378584618019011, 0.04751235194115914, 0.38372972855017384, -0.32864473143393413, -0.1936180868918318, 0.12817898375703776, -0.265335301070706, -0.06732534158633638, 0.14248846135571427, -0.04318379216919874... |
707.399 | Inflatable Dome for Moon, Mars, Asteroids and Satellites | On a planet without atmosphere, sustaining human life is very difficult and
dangerous, especially during short sunlit period when low temperature prevails.
To counter these environmental stresses, the author offer an innovative
artificial "Evergreen" dome, an inflated hemisphere with interiors continuously
providing ... | physics.gen-ph physics.space-ph | on a planet without atmosphere sustaining human life is very difficult and dangerous especially during short sunlit period when low temperature prevails to counter these environmental stresses the author offer an innovative artificial evergreen dome an inflated hemisphere with interiors continuously providing a climate... | [['on', 'a', 'planet', 'without', 'atmosphere', 'sustaining', 'human', 'life', 'is', 'very', 'difficult', 'and', 'dangerous', 'especially', 'during', 'short', 'sunlit', 'period', 'when', 'low', 'temperature', 'prevails', 'to', 'counter', 'these', 'environmental', 'stresses', 'the', 'author', 'offer', 'an', 'innovative'... | [-0.10265744325649272, 0.21303260469580687, -0.06394041718831703, 0.07694830352426577, -0.08768629569233631, -0.10514864153506708, 0.06063861637801947, 0.3543715241101028, -0.19492243425990108, -0.34551234303021444, 0.1392827660927841, -0.2716857177750972, -0.11597623391625986, 0.24942877473754446, -0.13533672554863255... |
707.3991 | Tidal Debris posing as Dark Galaxies | Debris sent into the intergalactic medium during tidal collisions can tell us
about several fundamental properties of galaxies, in particular their missing
mass, both in the form of cosmological Dark Matter and so-called Lost Baryons.
High velocity encounters, which are common in clusters of galaxies, are able to
pro... | astro-ph | debris sent into the intergalactic medium during tidal collisions can tell us about several fundamental properties of galaxies in particular their missing mass both in the form of cosmological dark matter and socalled lost baryons high velocity encounters which are common in clusters of galaxies are able to produce fai... | [['debris', 'sent', 'into', 'the', 'intergalactic', 'medium', 'during', 'tidal', 'collisions', 'can', 'tell', 'us', 'about', 'several', 'fundamental', 'properties', 'of', 'galaxies', 'in', 'particular', 'their', 'missing', 'mass', 'both', 'in', 'the', 'form', 'of', 'cosmological', 'dark', 'matter', 'and', 'socalled', '... | [-0.08608459072462087, 0.09295521803042496, -0.1216134994324139, 0.134164820956855, -0.1362327770208667, -0.04536361322383296, -0.01622266452459934, 0.36476998380612863, -0.1662058194716998, -0.37256392885108724, 0.006831337281439078, -0.27940205889314124, -0.05670778566952177, 0.17151681586101966, -0.03840334052963225... |
707.3992 | Quantum Signatures of Solar System Dynamics | Let w(i) be a period of rotation of the i-th planet around the Sun (or w(j;i)
be a period of rotation of j-th satellite around the i-th planet). From
empirical observations it is known that the sum of n(i)w(i)=0 (or the sum of
n(j)w(j;i)=0) for some integers n(i) (or n(j)), different for different
satellite systems. ... | physics.gen-ph physics.space-ph | let wi be a period of rotation of the ith planet around the sun or wji be a period of rotation of jth satellite around the ith planet from empirical observations it is known that the sum of niwi0 or the sum of njwji0 for some integers ni or nj different for different satellite systems these conditions known as resonanc... | [['let', 'wi', 'be', 'a', 'period', 'of', 'rotation', 'of', 'the', 'ith', 'planet', 'around', 'the', 'sun', 'or', 'wji', 'be', 'a', 'period', 'of', 'rotation', 'of', 'jth', 'satellite', 'around', 'the', 'ith', 'planet', 'from', 'empirical', 'observations', 'it', 'is', 'known', 'that', 'the', 'sum', 'of', 'niwi0', 'or',... | [-0.11434288886495125, 0.13247064381447804, -0.07217871016031976, 0.0769188197888832, -0.06635158847117972, -0.12997133627884153, 0.02157788328989608, 0.3071724100607551, -0.22785261127815193, -0.32207698422746783, 0.07687711212923352, -0.2538492311629005, -0.12705414448606056, 0.23291536772615698, -0.10240413422863452... |
707.3993 | On the reduction of Feynman integrals to master integrals | The reduction of Feynman integrals to master integrals is an algebraic
problem that requires algorithmic approaches at the modern level of
calculations. Straightforward applications of the classical Buchberger
algorithm to construct Groebner bases seem to be inefficient. An essential
modification designed especially ... | hep-ph | the reduction of feynman integrals to master integrals is an algebraic problem that requires algorithmic approaches at the modern level of calculations straightforward applications of the classical buchberger algorithm to construct groebner bases seem to be inefficient an essential modification designed especially for ... | [['the', 'reduction', 'of', 'feynman', 'integrals', 'to', 'master', 'integrals', 'is', 'an', 'algebraic', 'problem', 'that', 'requires', 'algorithmic', 'approaches', 'at', 'the', 'modern', 'level', 'of', 'calculations', 'straightforward', 'applications', 'of', 'the', 'classical', 'buchberger', 'algorithm', 'to', 'const... | [-0.06949147905065665, -0.005019715406299031, -0.16836066250886086, 0.10685120494118039, -0.11533793278733714, -0.12610488828324096, 0.016194887931498005, 0.39416962494732627, -0.2631527920004348, -0.3029377166129334, 0.10007491704522514, -0.25776717169079144, -0.17610609445156872, 0.24585202258302313, -0.0753922778063... |
707.3994 | Phase separation in the vicinity of "quantum critical" doping
concentration: implications for high temperature superconductors | A general quantitative measure of the tendency towards phase separation is
introduced for systems exhibiting phase transitions or crossovers controlled by
charge carrier concentration. This measure is devised for the situations when
the quantitative knowledge of various contributions to free energy is
incomplete, and... | cond-mat.str-el cond-mat.stat-mech cond-mat.supr-con | a general quantitative measure of the tendency towards phase separation is introduced for systems exhibiting phase transitions or crossovers controlled by charge carrier concentration this measure is devised for the situations when the quantitative knowledge of various contributions to free energy is incomplete and is ... | [['a', 'general', 'quantitative', 'measure', 'of', 'the', 'tendency', 'towards', 'phase', 'separation', 'is', 'introduced', 'for', 'systems', 'exhibiting', 'phase', 'transitions', 'or', 'crossovers', 'controlled', 'by', 'charge', 'carrier', 'concentration', 'this', 'measure', 'is', 'devised', 'for', 'the', 'situations'... | [-0.15953069370121917, 0.23231656402087128, -0.06776185177305949, 0.07881908051745022, -0.019898011604927376, -0.14912810270726995, 0.11207188845408791, 0.3667391104702379, -0.24373919057043295, -0.29945048167776894, 0.0021239790817866966, -0.3343059185404137, -0.09389477653730609, 0.12821922464374924, 0.02249407401057... |
707.3995 | Probing Non-Abelian Statistics in nu=12/5 Quantum Hall State | The tunneling current and shot noise of the current between two Fractional
Quantum Hall (FQH) edges in the $ \nu=12/5 $ FQH state in electronic
Mach-Zehnder interferometer are studied. It is shown that the tunneling current
and shot noise can be used to probe the existence of $k=3 $ parafermion
statistics in the $ \n... | cond-mat.mes-hall | the tunneling current and shot noise of the current between two fractional quantum hall fqh edges in the nu125 fqh state in electronic machzehnder interferometer are studied it is shown that the tunneling current and shot noise can be used to probe the existence of k3 parafermion statistics in the nu125 fqh state more ... | [['the', 'tunneling', 'current', 'and', 'shot', 'noise', 'of', 'the', 'current', 'between', 'two', 'fractional', 'quantum', 'hall', 'fqh', 'edges', 'in', 'the', 'nu125', 'fqh', 'state', 'in', 'electronic', 'machzehnder', 'interferometer', 'are', 'studied', 'it', 'is', 'shown', 'that', 'the', 'tunneling', 'current', 'an... | [-0.18562667640578706, 0.21549871234068027, -0.07590783617431016, 0.07192921029689553, 0.011271680193727441, -0.16652650946299685, 0.05289039074154006, 0.30727904648378945, -0.21727737732175173, -0.31928934570345463, -0.003923036125453302, -0.27766681021911965, -0.12545553404329854, 0.17351519737999435, -0.039128495472... |
707.3996 | Stability of multiquarks in a simple string model | A simple string model inspired by the strong-coupling regime of Quantum
ChromoDynamics is used as a potential for studying the spectrum of multiquark
systems with two quarks and two antiquarks, with a careful treatment of the
four-body problem. It is found that the ground state is stable, lying below the
threshold fo... | hep-ph nucl-th | a simple string model inspired by the strongcoupling regime of quantum chromodynamics is used as a potential for studying the spectrum of multiquark systems with two quarks and two antiquarks with a careful treatment of the fourbody problem it is found that the ground state is stable lying below the threshold for disso... | [['a', 'simple', 'string', 'model', 'inspired', 'by', 'the', 'strongcoupling', 'regime', 'of', 'quantum', 'chromodynamics', 'is', 'used', 'as', 'a', 'potential', 'for', 'studying', 'the', 'spectrum', 'of', 'multiquark', 'systems', 'with', 'two', 'quarks', 'and', 'two', 'antiquarks', 'with', 'a', 'careful', 'treatment',... | [-0.1120198099759587, 0.23941709343017192, -0.12952277717883126, 0.11760846067734651, 0.023956922650860066, -0.18481314676536018, 0.0750416234552272, 0.316305670560452, -0.18427941404086978, -0.22851694136727274, 0.013094061789544005, -0.30148899055233125, -0.04393377164868932, 0.1453450244500122, 0.07973648393690064, ... |
707.3997 | Search for Bs --> mu+ mu- at D0 | We report results from a search for the decay Bs --> mu+ mu- using 1.3/fb of
pbar p collisions at sqrt(s)= 1.96 TeV collected by the D0 experiment at the
Fermilab Tevatron Collider. We find two candidate events, consistent with the
expected background of 1.24 +/- 0.99, and set an upper limit on the branching
fraction... | hep-ex | we report results from a search for the decay bs mu mu using 13fb of pbar p collisions at sqrts 196 tev collected by the d0 experiment at the fermilab tevatron collider we find two candidate events consistent with the expected background of 124 099 and set an upper limit on the branching fraction of bbs mu mu 12e7 at t... | [['we', 'report', 'results', 'from', 'a', 'search', 'for', 'the', 'decay', 'bs', 'mu', 'mu', 'using', '13fb', 'of', 'pbar', 'p', 'collisions', 'at', 'sqrts', '196', 'tev', 'collected', 'by', 'the', 'd0', 'experiment', 'at', 'the', 'fermilab', 'tevatron', 'collider', 'we', 'find', 'two', 'candidate', 'events', 'consiste... | [-0.07662101908335311, 0.1975942986527732, -0.06752982631611128, 0.07251543335376247, 0.016303423326462507, -0.11353826377871296, 0.16764206197413226, 0.2620108224030945, -0.12917080425447033, -0.3550486511460716, -0.018332254040175147, -0.46545668565217524, 0.11812116253760553, 0.1722580321215754, 0.13500189148039826,... |
707.3998 | The Spitzer Survey of the Small Magellanic Cloud: Discovery of Embedded
Protostars in the HII Region NGC 346 | We use Spitzer Space Telescope observations from the Spitzer Survey of the
Small Magellanic Cloud (S3MC) to study the young stellar content of N66, the
largest and brightest HII region in the SMC. In addition to large numbers of
normal stars, we detect a significant population of bright, red infrared
sources that we ... | astro-ph | we use spitzer space telescope observations from the spitzer survey of the small magellanic cloud s3mc to study the young stellar content of n66 the largest and brightest hii region in the smc in addition to large numbers of normal stars we detect a significant population of bright red infrared sources that we identify... | [['we', 'use', 'spitzer', 'space', 'telescope', 'observations', 'from', 'the', 'spitzer', 'survey', 'of', 'the', 'small', 'magellanic', 'cloud', 's3mc', 'to', 'study', 'the', 'young', 'stellar', 'content', 'of', 'n66', 'the', 'largest', 'and', 'brightest', 'hii', 'region', 'in', 'the', 'smc', 'in', 'addition', 'to', 'l... | [-0.0270285127253938, 0.09290134468726043, -0.06130258238489001, 0.12110956240252688, -0.10544166991182057, -0.021948638929311058, 0.08475249511920366, 0.4541969262882425, -0.11568153000924464, -0.3694352153014263, 0.05149647023625158, -0.27701357196241716, -0.0054675502148617446, 0.1384691524359494, -0.098917983393967... |
707.3999 | Quintessence, inflation and baryogenesis from a single
pseudo-Nambu-Goldstone boson | We exhibit a model in which a single pseudo-Nambu-Goldstone boson explains
dark energy, inflation and baryogenesis. The model predicts correlated signals
in future collider experiments, WIMP searches, proton decay experiments, dark
energy probes, and the PLANCK satellite CMB measurements.
| astro-ph | we exhibit a model in which a single pseudonambugoldstone boson explains dark energy inflation and baryogenesis the model predicts correlated signals in future collider experiments wimp searches proton decay experiments dark energy probes and the planck satellite cmb measurements | [['we', 'exhibit', 'a', 'model', 'in', 'which', 'a', 'single', 'pseudonambugoldstone', 'boson', 'explains', 'dark', 'energy', 'inflation', 'and', 'baryogenesis', 'the', 'model', 'predicts', 'correlated', 'signals', 'in', 'future', 'collider', 'experiments', 'wimp', 'searches', 'proton', 'decay', 'experiments', 'dark', ... | [-0.13372469308953255, 0.3084589740834557, -0.14383901172102645, 0.25922803652401155, -0.11098057057899542, -0.22753636066604835, -0.034596233730180524, 0.2899832953818334, -0.20381532915127584, -0.3424638016507603, -0.044200515338721186, -0.3650293607169237, 0.018425009285028163, 0.1800390125538867, 0.149517015959972,... |
707.4 | The LU-LC conjecture, diagonal local operations and quadratic forms over
GF(2) | We report progress on the LU-LC conjecture - an open problem in the context
of entanglement in stabilizer states (or graph states). This conjecture states
that every two stabilizer states which are related by a local unitary
operation, must also be related by a local operation within the Clifford group.
The contribut... | quant-ph | we report progress on the lulc conjecture an open problem in the context of entanglement in stabilizer states or graph states this conjecture states that every two stabilizer states which are related by a local unitary operation must also be related by a local operation within the clifford group the contribution of thi... | [['we', 'report', 'progress', 'on', 'the', 'lulc', 'conjecture', 'an', 'open', 'problem', 'in', 'the', 'context', 'of', 'entanglement', 'in', 'stabilizer', 'states', 'or', 'graph', 'states', 'this', 'conjecture', 'states', 'that', 'every', 'two', 'stabilizer', 'states', 'which', 'are', 'related', 'by', 'a', 'local', 'u... | [-0.14773636459295328, 0.11759416352734357, -0.09083717852210005, 0.05839692954362059, -0.012174070676167806, -0.14775606368357935, 0.054923656260749944, 0.2920247952391704, -0.31050154226521653, -0.25430718225116533, 0.130350383943102, -0.20853456784350177, -0.1616658939809228, 0.21392216511536388, -0.1298193476473291... |
707.4001 | Different Methods of Forming Cold Fronts in Non-Merging Clusters | Sharp edges in X-ray surface brightness with continuous gas pressure called
cold fronts have been often found in relaxed galaxy clusters such as Abell 496.
Models that explain cold fronts as surviving cores of head-on subcluster
mergers do not work well for these clusters and competing models involving gas
sloshing h... | astro-ph | sharp edges in xray surface brightness with continuous gas pressure called cold fronts have been often found in relaxed galaxy clusters such as abell 496 models that explain cold fronts as surviving cores of headon subcluster mergers do not work well for these clusters and competing models involving gas sloshing have b... | [['sharp', 'edges', 'in', 'xray', 'surface', 'brightness', 'with', 'continuous', 'gas', 'pressure', 'called', 'cold', 'fronts', 'have', 'been', 'often', 'found', 'in', 'relaxed', 'galaxy', 'clusters', 'such', 'as', 'abell', '496', 'models', 'that', 'explain', 'cold', 'fronts', 'as', 'surviving', 'cores', 'of', 'headon'... | [-0.0584768061095101, 0.11067917580668175, -0.0663328070747811, 0.07030632721844683, -0.06055566903153776, -0.06231051280121335, 0.047901448837213964, 0.4180636862582917, -0.17324333074557027, -0.34218527385674957, 0.02657557562779906, -0.2983501619759264, -0.028226794370459746, 0.1617748530168299, 0.007222242130407303... |
707.4002 | Spitzer Observations of Powerful Radio Sources | We have measured the mid-infrared radiation from an orientation-unbiased
sample of powerful 3C RR galaxies and quasars using the IRS and MIPS
instruments aboard the Spitzer Space Telescope. We fit the Spitzer data as well
as other measurements from the literature with synchrotron and dust components.
At 15 microns, q... | astro-ph | we have measured the midinfrared radiation from an orientationunbiased sample of powerful 3c rr galaxies and quasars using the irs and mips instruments aboard the spitzer space telescope we fit the spitzer data as well as other measurements from the literature with synchrotron and dust components at 15 microns quasars ... | [['we', 'have', 'measured', 'the', 'midinfrared', 'radiation', 'from', 'an', 'orientationunbiased', 'sample', 'of', 'powerful', '3c', 'rr', 'galaxies', 'and', 'quasars', 'using', 'the', 'irs', 'and', 'mips', 'instruments', 'aboard', 'the', 'spitzer', 'space', 'telescope', 'we', 'fit', 'the', 'spitzer', 'data', 'as', 'w... | [0.027309610982998632, 0.1049669522115157, -0.05533490745270123, 0.08642977340787183, -0.14212172662910932, -0.06797403903104939, 0.007677013390303518, 0.5119579321203324, -0.1014559390829303, -0.332748140512894, 0.07592078345120311, -0.3478756612793614, 0.003592773098856784, 0.2407088306499645, -0.011649807933001565, ... |
707.4003 | Symplectic $A_\infty$-algebras and string topology operations | In this paper we establish the existence of certain structures on the
ordinary and equivariant homology of the free loop space on a manifold or, more
generally, a formal Poincar\'e duality space. These structures; namely the loop
product, the loop bracket and the string bracket, were introduced and studied
by Chas an... | math.QA math.AT | in this paper we establish the existence of certain structures on the ordinary and equivariant homology of the free loop space on a manifold or more generally a formal poincare duality space these structures namely the loop product the loop bracket and the string bracket were introduced and studied by chas and sullivan... | [['in', 'this', 'paper', 'we', 'establish', 'the', 'existence', 'of', 'certain', 'structures', 'on', 'the', 'ordinary', 'and', 'equivariant', 'homology', 'of', 'the', 'free', 'loop', 'space', 'on', 'a', 'manifold', 'or', 'more', 'generally', 'a', 'formal', 'poincare', 'duality', 'space', 'these', 'structures', 'namely'... | [-0.20663476912850906, 0.12325099225006537, -0.125181155445997, 0.15925588716327407, -0.0935000021148611, -0.11894194839269291, 0.008480884823200788, 0.3278395216912031, -0.3053300559152792, -0.25195556688179943, 0.10995940722231926, -0.16526084044879233, -0.2305578792174519, 0.14961927632203348, -0.140155576399447, 0.... |
707.4004 | Vesicle shape, molecular tilt, and the suppression of necks | Can the presence of molecular-tilt order significantly affect the shapes of
lipid bilayer membranes, particularly membrane shapes with narrow necks?
Motivated by the propensity for tilt order and the common occurrence of narrow
necks in the intermediate stages of biological processes such as endocytosis
and vesicle t... | cond-mat.soft | can the presence of moleculartilt order significantly affect the shapes of lipid bilayer membranes particularly membrane shapes with narrow necks motivated by the propensity for tilt order and the common occurrence of narrow necks in the intermediate stages of biological processes such as endocytosis and vesicle traffi... | [['can', 'the', 'presence', 'of', 'moleculartilt', 'order', 'significantly', 'affect', 'the', 'shapes', 'of', 'lipid', 'bilayer', 'membranes', 'particularly', 'membrane', 'shapes', 'with', 'narrow', 'necks', 'motivated', 'by', 'the', 'propensity', 'for', 'tilt', 'order', 'and', 'the', 'common', 'occurrence', 'of', 'nar... | [-0.14980909650475294, 0.1509883152900424, -0.04452487129119659, 0.020660436142771188, -0.03843266021974418, -0.09784131978608972, 0.006310066962045748, 0.3770942337351653, -0.24989386076925163, -0.31465815616970694, 0.05001144388656878, -0.24197966087297684, -0.1527480200750593, 0.10438186896341216, -0.044255592464416... |
707.4005 | An Observed Fundamental Plane Relation for Supermassive Black Holes | We study observed correlations between supermassive black hole (BHs) and the
properties of their host galaxies, and show that the observations define a BH
'fundamental plane' (BHFP), of the form M_BH sigma^(3.0+-0.3)*R_e^(0.43+-0.19),
or M_BH M_bulge^(0.54+-0.17)*sigma^(2.2+-0.5), analogous to the FP of
elliptical ga... | astro-ph | we study observed correlations between supermassive black hole bhs and the properties of their host galaxies and show that the observations define a bh fundamental plane bhfp of the form m_bh sigma3003r_e043019 or m_bh m_bulge054017sigma2205 analogous to the fp of elliptical galaxies the bhfp is preferred over a simple... | [['we', 'study', 'observed', 'correlations', 'between', 'supermassive', 'black', 'hole', 'bhs', 'and', 'the', 'properties', 'of', 'their', 'host', 'galaxies', 'and', 'show', 'that', 'the', 'observations', 'define', 'a', 'bh', 'fundamental', 'plane', 'bhfp', 'of', 'the', 'form', 'm_bh', 'sigma3003r_e043019', 'or', 'm_bh... | [-0.13176538436630061, 0.06910135146996407, -0.04862359968105453, 0.20845614212660868, -0.07880374956353803, -0.07662987449232524, 0.0803627055747626, 0.3492618316836725, -0.097513214484832, -0.33804143530046826, 0.052707186167859514, -0.33887322685707394, -0.04863617016072167, 0.2212096105904153, -0.018730051188825446... |
707.4006 | Two-loop Gell-Mann-Low function of N=1 supersymmetric Yang-Mills theory,
regularized by higher covariant derivatives | Two-loop Gell-Mann-Low function is calculated for N=1 supersymmetric
Yang-Mills theory, regularized by higher covariant derivatives. The integrals,
which define it, are shown to be reduced to total derivatives and can be easily
calculated analytically.
| hep-th | twoloop gellmannlow function is calculated for n1 supersymmetric yangmills theory regularized by higher covariant derivatives the integrals which define it are shown to be reduced to total derivatives and can be easily calculated analytically | [['twoloop', 'gellmannlow', 'function', 'is', 'calculated', 'for', 'n1', 'supersymmetric', 'yangmills', 'theory', 'regularized', 'by', 'higher', 'covariant', 'derivatives', 'the', 'integrals', 'which', 'define', 'it', 'are', 'shown', 'to', 'be', 'reduced', 'to', 'total', 'derivatives', 'and', 'can', 'be', 'easily', 'ca... | [-0.04683212753426393, 0.1928672412519946, -0.0929324877284029, 0.1937358375152518, -0.08471440184204017, -0.13601141565424554, -0.0843606385135311, 0.3392690479864969, -0.23029995380955584, -0.27621967424912486, 0.08215880660367582, -0.27560733330970194, -0.20785334299537628, 0.11305796716581373, -0.032222389750292194... |
707.4007 | Reflection Groups and Polytopes over Finite Fields, III | When the standard representation of a crystallographic Coxeter group is
reduced modulo an odd prime p, one obtains a finite group G^p acting on some
orthogonal space over Z_p . If the Coxeter group has a string diagram, then G^p
will often be the automorphism group of a finite abstract regular polytope. In
parts I an... | math.CO math.MG | when the standard representation of a crystallographic coxeter group is reduced modulo an odd prime p one obtains a finite group gp acting on some orthogonal space over z_p if the coxeter group has a string diagram then gp will often be the automorphism group of a finite abstract regular polytope in parts i and ii we e... | [['when', 'the', 'standard', 'representation', 'of', 'a', 'crystallographic', 'coxeter', 'group', 'is', 'reduced', 'modulo', 'an', 'odd', 'prime', 'p', 'one', 'obtains', 'a', 'finite', 'group', 'gp', 'acting', 'on', 'some', 'orthogonal', 'space', 'over', 'z_p', 'if', 'the', 'coxeter', 'group', 'has', 'a', 'string', 'di... | [-0.11649669139296748, 0.10751611125044747, -0.09257992508446478, 0.04169135754909803, -0.11829993608625955, -0.10575877917653997, 0.02191895439318614, 0.3473835856857477, -0.31501039776503603, -0.23667841653514188, 0.13851095495647314, -0.22545078615075909, -0.14086910859987256, 0.19341012273798697, -0.110850564684824... |
707.4008 | GRBs and Hypernova Explosions of Some Galactic Sources | Knowing the Kerr parameters we can make quantitative calculations of the
rotational energy of black holes. We show that Nova Sco (GRO J1655 - 40), Il
Lupi (4U 1543 - 47), XTE J1550 - 564 and GS 2023 + 338 are relics of gamma-ray
burst (GRB) and Hypernova explosions. They had more than enough rotational
energy to powe... | astro-ph | knowing the kerr parameters we can make quantitative calculations of the rotational energy of black holes we show that nova sco gro j1655 40 il lupi 4u 1543 47 xte j1550 564 and gs 2023 338 are relics of gammaray burst grb and hypernova explosions they had more than enough rotational energy to power themselves in fact ... | [['knowing', 'the', 'kerr', 'parameters', 'we', 'can', 'make', 'quantitative', 'calculations', 'of', 'the', 'rotational', 'energy', 'of', 'black', 'holes', 'we', 'show', 'that', 'nova', 'sco', 'gro', 'j1655', '40', 'il', 'lupi', '4u', '1543', '47', 'xte', 'j1550', '564', 'and', 'gs', '2023', '338', 'are', 'relics', 'of... | [-0.0736371137524106, 0.17934820748840657, -0.05169754199284528, 0.15889709973612762, -0.1126920297285732, -0.13146449064362326, 0.07268472486191435, 0.3945364308667046, -0.1853624104960112, -0.36781743407601075, 0.0669920584436373, -0.3111719970534347, 0.008691838348512443, 0.2207987673990872, -0.06991845782890561, -0... |
707.4009 | Spin ice behavior in Dy2Sn2-xSbxO7+x/2 and Dy2NbScO7 | We report the magnetic and thermal properties of Dy2Sn2-xSbxO7+x/2, x = 0,
0.25, and 0.5, and Dy2NbScO7. We find evidence for Ising-like single ion ground
states in the Dy2Sn2-xSbxO7+x/2 materials. These materials possess nearly the
same zero point entropy as the canonical spin ices Ho2Ti2O7 and Dy2Ti2O7,
strongly su... | cond-mat.str-el cond-mat.mtrl-sci | we report the magnetic and thermal properties of dy2sn2xsbxo7x2 x 0 025 and 05 and dy2nbsco7 we find evidence for isinglike single ion ground states in the dy2sn2xsbxo7x2 materials these materials possess nearly the same zero point entropy as the canonical spin ices ho2ti2o7 and dy2ti2o7 strongly suggesting that they h... | [['we', 'report', 'the', 'magnetic', 'and', 'thermal', 'properties', 'of', 'dy2sn2xsbxo7x2', 'x', '0', '025', 'and', '05', 'and', 'dy2nbsco7', 'we', 'find', 'evidence', 'for', 'isinglike', 'single', 'ion', 'ground', 'states', 'in', 'the', 'dy2sn2xsbxo7x2', 'materials', 'these', 'materials', 'possess', 'nearly', 'the', ... | [-0.14007025434435388, 0.2844284391030669, -0.03647477032668958, 0.029695512801974525, 0.039024257294781435, -0.14946107384879317, 0.09057979865617632, 0.3769465427253848, -0.23943891799812875, -0.2666731161526709, 0.06348589447840491, -0.3431679547598986, -0.11194969224961143, 0.11138546814114969, 0.059789431786216866... |
707.401 | Stability of general relativistic Miyamoto-Nagai galaxies | The stability of a recently proposed general relativistic model of galaxies
is studied in some detail. This model is a general relativistic version of the
well known Miyamoto-Nagai model that represents well a thick galactic disk. The
stability of the disk is investigated under a general first order perturbation
keep... | gr-qc astro-ph | the stability of a recently proposed general relativistic model of galaxies is studied in some detail this model is a general relativistic version of the well known miyamotonagai model that represents well a thick galactic disk the stability of the disk is investigated under a general first order perturbation keeping t... | [['the', 'stability', 'of', 'a', 'recently', 'proposed', 'general', 'relativistic', 'model', 'of', 'galaxies', 'is', 'studied', 'in', 'some', 'detail', 'this', 'model', 'is', 'a', 'general', 'relativistic', 'version', 'of', 'the', 'well', 'known', 'miyamotonagai', 'model', 'that', 'represents', 'well', 'a', 'thick', 'g... | [-0.1246063834105989, 0.06311718549678844, -0.09529880909882124, 0.11904959983273762, -0.07794353199525944, -0.08145113986039769, -0.07399542715165366, 0.39543980213551266, -0.16932360734338464, -0.2459737073734077, 0.06909399556371303, -0.25671820203294454, -0.1085015239591882, 0.15450668694153066, -0.0207570239085505... |
707.4011 | Geometrically Induced Phase Transitions at Large N | Utilizing the large N dual description of a metastable system of branes and
anti-branes wrapping rigid homologous S^2's in a non-compact Calabi-Yau
threefold, we study phase transitions induced by changing the positions of the
S^2's. At leading order in 1/N the effective potential for this system is
computed by the p... | hep-th | utilizing the large n dual description of a metastable system of branes and antibranes wrapping rigid homologous s2s in a noncompact calabiyau threefold we study phase transitions induced by changing the positions of the s2s at leading order in 1n the effective potential for this system is computed by the planar limit ... | [['utilizing', 'the', 'large', 'n', 'dual', 'description', 'of', 'a', 'metastable', 'system', 'of', 'branes', 'and', 'antibranes', 'wrapping', 'rigid', 'homologous', 's2s', 'in', 'a', 'noncompact', 'calabiyau', 'threefold', 'we', 'study', 'phase', 'transitions', 'induced', 'by', 'changing', 'the', 'positions', 'of', 't... | [-0.18301571738881203, 0.22738870417071436, -0.052723206232783176, 0.10336577563449716, -0.045582373514021404, -0.15431946726990925, 0.05200705734228453, 0.32886136421971274, -0.21317397192708099, -0.2569107976460817, 0.05828937875644473, -0.24575572388384165, -0.06830925255195057, 0.07285407933269021, -0.0444179606098... |
707.4012 | Real space information from Fluctuation electron microscopy:
Applications to amorphous silicon | Ideal models of complex materials must satisfy all available information
about the system. Generally, this information consists of experimental data,
information implicit to sophisticated interatomic interactions and potentially
other {\it a priori} information. By jointly imposing first-principles or
tight-binding i... | cond-mat.dis-nn cond-mat.mtrl-sci | ideal models of complex materials must satisfy all available information about the system generally this information consists of experimental data information implicit to sophisticated interatomic interactions and potentially other it a priori information by jointly imposing firstprinciples or tightbinding information ... | [['ideal', 'models', 'of', 'complex', 'materials', 'must', 'satisfy', 'all', 'available', 'information', 'about', 'the', 'system', 'generally', 'this', 'information', 'consists', 'of', 'experimental', 'data', 'information', 'implicit', 'to', 'sophisticated', 'interatomic', 'interactions', 'and', 'potentially', 'other',... | [-0.06178357419033181, 0.10141649318229355, -0.0825629533439855, 0.03011972878643141, -0.07349052084413107, -0.1278521902334522, 0.026457249586598317, 0.44402265710703714, -0.26534556749016114, -0.33750879955084495, 0.08450266156709609, -0.3236251762792678, -0.12495149443955751, 0.15184641232497623, 0.01241783594260071... |
707.4013 | Contributions of Cherenkov Light to the Signals from Lead Tungstate
Crystals | Results are presented of detailed measurements of the signals generated by
high-energy electrons and muons in lead tungstate crystals. A significant
fraction of the light produced in these crystals and detected by
photomultiplier tubes is the result of the \v{C}erenkov mechanism. This is
concluded from the angular de... | physics.ins-det | results are presented of detailed measurements of the signals generated by highenergy electrons and muons in lead tungstate crystals a significant fraction of the light produced in these crystals and detected by photomultiplier tubes is the result of the vcerenkov mechanism this is concluded from the angular dependence... | [['results', 'are', 'presented', 'of', 'detailed', 'measurements', 'of', 'the', 'signals', 'generated', 'by', 'highenergy', 'electrons', 'and', 'muons', 'in', 'lead', 'tungstate', 'crystals', 'a', 'significant', 'fraction', 'of', 'the', 'light', 'produced', 'in', 'these', 'crystals', 'and', 'detected', 'by', 'photomult... | [-0.08576868557138369, 0.23063513748929837, -0.07848676468711346, 0.011413982936937827, -0.026480334298685192, -0.05485649994225241, 0.05345417190692388, 0.36159594589844346, -0.23169163013226352, -0.3697363764513284, 0.0703276833257405, -0.3588694907957688, -0.03943560076295398, 0.2450625680925441, 0.01267745891818776... |
707.4014 | Reversible plasticity in amorphous materials | A fundamental assumption in our understanding of material rheology is that
when microscopic deformations are reversible, the material responds elastically
to external loads. Plasticity, i.e. dissipative and irreversible macroscopic
changes in a material, is assumed to be the consequence of irreversible
microscopic ev... | cond-mat.soft cond-mat.mtrl-sci | a fundamental assumption in our understanding of material rheology is that when microscopic deformations are reversible the material responds elastically to external loads plasticity ie dissipative and irreversible macroscopic changes in a material is assumed to be the consequence of irreversible microscopic events her... | [['a', 'fundamental', 'assumption', 'in', 'our', 'understanding', 'of', 'material', 'rheology', 'is', 'that', 'when', 'microscopic', 'deformations', 'are', 'reversible', 'the', 'material', 'responds', 'elastically', 'to', 'external', 'loads', 'plasticity', 'ie', 'dissipative', 'and', 'irreversible', 'macroscopic', 'cha... | [-0.14613941433273403, 0.20062988970940018, -0.09416476108462495, 0.029808465690425067, -0.04988691514796194, -0.0913146967730284, 0.050631488657410385, 0.3759995539690934, -0.31100569060985367, -0.2694058054510285, 0.0435867324476039, -0.2673331413728495, -0.22053086244519435, 0.17515899191208767, -0.05049868008719903... |
707.4015 | Supersymmetry and Lie groups | We construct all vacuum states of $\mathcal{N}=2$ supersymmetric Yang-Mills
quantum mechanics (for SU(N) group) and discuss their origin from the SU(N)
real cohomology.
| math-ph math.MP | we construct all vacuum states of mathcaln2 supersymmetric yangmills quantum mechanics for sun group and discuss their origin from the sun real cohomology | [['we', 'construct', 'all', 'vacuum', 'states', 'of', 'mathcaln2', 'supersymmetric', 'yangmills', 'quantum', 'mechanics', 'for', 'sun', 'group', 'and', 'discuss', 'their', 'origin', 'from', 'the', 'sun', 'real', 'cohomology']] | [-0.09106927227390849, 0.23773434142703595, -0.07847939447484627, 0.15689234504395205, -0.031148392605878737, -0.12244642744569675, -0.05502394851013694, 0.3043990401632112, -0.15310875132032062, -0.2682715053467647, 0.10021048528142273, -0.27858071996951883, -0.22587492568013462, 0.06939892422245897, -0.09681001945358... |
707.4016 | Loop Corrections and Naturalness in a Chiral Effective Field Theory | The loop expansion is applied to a chiral effective hadronic lagrangian; with
the techniques of Infrared Regularization, it is possible to separate out the
short-range contributions and to write them as local products of fields that
are already present in our lagrangian. (The appropriate field variables must be
re-de... | nucl-th | the loop expansion is applied to a chiral effective hadronic lagrangian with the techniques of infrared regularization it is possible to separate out the shortrange contributions and to write them as local products of fields that are already present in our lagrangian the appropriate field variables must be redefined at... | [['the', 'loop', 'expansion', 'is', 'applied', 'to', 'a', 'chiral', 'effective', 'hadronic', 'lagrangian', 'with', 'the', 'techniques', 'of', 'infrared', 'regularization', 'it', 'is', 'possible', 'to', 'separate', 'out', 'the', 'shortrange', 'contributions', 'and', 'to', 'write', 'them', 'as', 'local', 'products', 'of'... | [-0.09125132079446507, 0.19531832107477973, -0.09591650117015947, 0.1284536241914236, -0.08521367737783059, -0.10942427468215746, -0.013913059617663103, 0.3714771621913138, -0.24976097601916522, -0.276445398918323, 0.03419640053424143, -0.31573825622758556, -0.09869264519412911, 0.09992382043912526, 0.08427606468359308... |
707.4017 | Casimir forces in a T operator approach | We explore the scattering approach to Casimir forces. Our main tool is the
description of Casimir energy in terms of transition operators, as presented in
Kenneth and Klich, Phys. Rev. Lett. 97, 160401 (2006). We study the convergence
properties of the formula and how to utilize it, together with scattering data
to c... | quant-ph cond-mat.stat-mech hep-th math-ph math.MP | we explore the scattering approach to casimir forces our main tool is the description of casimir energy in terms of transition operators as presented in kenneth and klich phys rev lett 97 160401 2006 we study the convergence properties of the formula and how to utilize it together with scattering data to compute the fo... | [['we', 'explore', 'the', 'scattering', 'approach', 'to', 'casimir', 'forces', 'our', 'main', 'tool', 'is', 'the', 'description', 'of', 'casimir', 'energy', 'in', 'terms', 'of', 'transition', 'operators', 'as', 'presented', 'in', 'kenneth', 'and', 'klich', 'phys', 'rev', 'lett', '97', '160401', '2006', 'we', 'study', '... | [-0.06844256405339955, 0.07867719332308887, -0.1001613622961136, 0.01740487308400059, -0.019177260012928764, -0.052087700506160545, 0.01273465308023023, 0.3641368075693538, -0.21167768681406524, -0.34237013789978654, -0.004756609107122071, -0.3049532780116731, -0.21492124465550042, 0.2002850237947244, -0.05217331428922... |
707.4018 | Adaptive Multigrid Algorithm for Lattice QCD | We present a new multigrid solver that is suitable for the Dirac operator in
the presence of disordered gauge fields. The key behind the success of the
algorithm is an adaptive projection onto the coarse grids that preserves the
near null space. The resulting algorithm has weak dependence on the gauge
coupling and ex... | hep-lat | we present a new multigrid solver that is suitable for the dirac operator in the presence of disordered gauge fields the key behind the success of the algorithm is an adaptive projection onto the coarse grids that preserves the near null space the resulting algorithm has weak dependence on the gauge coupling and exhibi... | [['we', 'present', 'a', 'new', 'multigrid', 'solver', 'that', 'is', 'suitable', 'for', 'the', 'dirac', 'operator', 'in', 'the', 'presence', 'of', 'disordered', 'gauge', 'fields', 'the', 'key', 'behind', 'the', 'success', 'of', 'the', 'algorithm', 'is', 'an', 'adaptive', 'projection', 'onto', 'the', 'coarse', 'grids', '... | [-0.14628033037902183, 0.14735096206381318, -0.0858277366919951, 0.055127591139624836, -0.06781839806731645, -0.1310153510119137, 0.008244166589136442, 0.36864958248742213, -0.22260242366752067, -0.231057948000463, 0.08920265047496499, -0.260057731725082, -0.1553568301794978, 0.15804635907233053, -0.016520103433641135,... |
707.4019 | Measurement of the Contribution of Neutrons to Hadron Calorimeter
Signals | The contributions of neutrons to hadronic signals from the DREAM calorimeter
are measured by analyzing the time structure of these signals. The neutrons,
which mainly originate from the evaporation stage of nuclear breakup in the
hadronic shower development process, contribute through elastic scattering off
protons i... | physics.ins-det | the contributions of neutrons to hadronic signals from the dream calorimeter are measured by analyzing the time structure of these signals the neutrons which mainly originate from the evaporation stage of nuclear breakup in the hadronic shower development process contribute through elastic scattering off protons in the... | [['the', 'contributions', 'of', 'neutrons', 'to', 'hadronic', 'signals', 'from', 'the', 'dream', 'calorimeter', 'are', 'measured', 'by', 'analyzing', 'the', 'time', 'structure', 'of', 'these', 'signals', 'the', 'neutrons', 'which', 'mainly', 'originate', 'from', 'the', 'evaporation', 'stage', 'of', 'nuclear', 'breakup'... | [-0.03580351825583867, 0.26972161631996605, -0.13845854435326918, 0.053338617400048915, -0.0120383566860461, -0.03708714569857309, -0.009504966536659817, 0.3645013225756867, -0.29876729943965263, -0.32132490546846726, 0.010710087723432566, -0.35149138664413804, 0.0029327931884184197, 0.13786796788917854, 0.024239267354... |
707.402 | Geometric measures of entanglement and the Schmidt decomposition | In the standard geometric approach to a measure of entanglement of a pure
state, $\sin^2\theta$ is used, where $\theta$ is the angle between the state to
the closest separable state of products of normalized qubit states. We consider
here a generalization of this notion to separable states consisting of products
of u... | quant-ph | in the standard geometric approach to a measure of entanglement of a pure state sin2theta is used where theta is the angle between the state to the closest separable state of products of normalized qubit states we consider here a generalization of this notion to separable states consisting of products of unnormalized s... | [['in', 'the', 'standard', 'geometric', 'approach', 'to', 'a', 'measure', 'of', 'entanglement', 'of', 'a', 'pure', 'state', 'sin2theta', 'is', 'used', 'where', 'theta', 'is', 'the', 'angle', 'between', 'the', 'state', 'to', 'the', 'closest', 'separable', 'state', 'of', 'products', 'of', 'normalized', 'qubit', 'states',... | [-0.11126267990507817, 0.14436803624982023, -0.10889296575229401, 0.02409406661221726, 0.017611722824937205, -0.0798770398517155, 0.04695383359883296, 0.32567381760957886, -0.31587684371556013, -0.23206038769508192, 0.07594330744596861, -0.2876701667210308, -0.08557632106545744, 0.11960193131245293, -0.0432789779891717... |
707.4021 | Dual-Readout Calorimetry with Lead Tungstate Crystals | Results are presented of beam tests in which a small electromagnetic
calorimeter consisting of lead tungstate crystals was exposed to 50 GeV
electrons and pions. This calorimeter was backed up by the DREAM Dual-Readout
calorimeter, which measures the scintillation and \v{C}erenkov light produced
in the shower develop... | physics.ins-det | results are presented of beam tests in which a small electromagnetic calorimeter consisting of lead tungstate crystals was exposed to 50 gev electrons and pions this calorimeter was backed up by the dream dualreadout calorimeter which measures the scintillation and vcerenkov light produced in the shower development usi... | [['results', 'are', 'presented', 'of', 'beam', 'tests', 'in', 'which', 'a', 'small', 'electromagnetic', 'calorimeter', 'consisting', 'of', 'lead', 'tungstate', 'crystals', 'was', 'exposed', 'to', '50', 'gev', 'electrons', 'and', 'pions', 'this', 'calorimeter', 'was', 'backed', 'up', 'by', 'the', 'dream', 'dualreadout',... | [-0.0441937492075331, 0.2100784165801105, -0.0855667028775059, 0.05244178955388951, -0.037596400700581886, -0.07594277609356688, -0.02084596384569858, 0.4030588048609715, -0.21360731290345922, -0.3776657406457709, 0.03462010579753342, -0.37670406266974593, -0.024640369744410792, 0.1895855962687615, -0.01169243830174786... |
707.4022 | Cluster Dual Fermion Approach to Nonlocal Correlations | We formulate a general cluster Dual Fermion Approach to nonlocal correlations
in crystals. The scheme allows the treatment of long-range correlations beyond
cluster DMFT and nonlocal effects in realistic calculations of multiorbital
systems. We show that the the simplest approximation exactly corresponds to
free clus... | cond-mat.str-el | we formulate a general cluster dual fermion approach to nonlocal correlations in crystals the scheme allows the treatment of longrange correlations beyond cluster dmft and nonlocal effects in realistic calculations of multiorbital systems we show that the the simplest approximation exactly corresponds to free cluster d... | [['we', 'formulate', 'a', 'general', 'cluster', 'dual', 'fermion', 'approach', 'to', 'nonlocal', 'correlations', 'in', 'crystals', 'the', 'scheme', 'allows', 'the', 'treatment', 'of', 'longrange', 'correlations', 'beyond', 'cluster', 'dmft', 'and', 'nonlocal', 'effects', 'in', 'realistic', 'calculations', 'of', 'multio... | [-0.09034875314682722, 0.05779218961743964, -0.11901300295361693, 0.15017736871539586, -0.005967945789380633, -0.11352715688306339, 0.06479260385679753, 0.354122055444828, -0.23596849707291298, -0.23298840101366652, -0.021638593348415242, -0.3072017836938048, -0.20401616786251364, 0.13091210507196385, 0.054809153694467... |
707.4023 | Influence of the jet opening angle on the derived kinematical parameters
of blazar jets having uniform and stratified bulk motion | We present analytical modelling of conical relativistic jets, in order to
evaluate the role of the jet opening angle on certain key parameters that are
inferred from VLBI radio observations of blazar nuclear jets. The key
parameters evaluated are the orientation angle (i.e., the viewing angle) of the
jet and the appa... | astro-ph | we present analytical modelling of conical relativistic jets in order to evaluate the role of the jet opening angle on certain key parameters that are inferred from vlbi radio observations of blazar nuclear jets the key parameters evaluated are the orientation angle ie the viewing angle of the jet and the apparent spee... | [['we', 'present', 'analytical', 'modelling', 'of', 'conical', 'relativistic', 'jets', 'in', 'order', 'to', 'evaluate', 'the', 'role', 'of', 'the', 'jet', 'opening', 'angle', 'on', 'certain', 'key', 'parameters', 'that', 'are', 'inferred', 'from', 'vlbi', 'radio', 'observations', 'of', 'blazar', 'nuclear', 'jets', 'the... | [-0.1412295782200356, 0.18791147871170102, -0.06576644294380354, 0.1026543954811324, -0.10731804189347942, -0.11035134325019742, -0.003931363703434808, 0.4626124880420483, -0.2349412903095959, -0.3201981388923061, 0.04759653762448579, -0.23087095871437113, 0.019192130317177047, 0.23418018720391356, 0.016415702948077936... |
707.4024 | Erlangen Program at Large--2: Inventing a wheel. The parabolic one | We discuss parabolic versions of Euler's identity e^{it}=cos t + i sin t. A
purely algebraic approach based on dual numbers is known to produce a very
trivial relation e^{pt} = 1+pt. Therefore we use a geometric setup of parabolic
rotations to recover the corresponding non-trivial algebraic framework. Our
main tool i... | math.GM math.RA math.RT | we discuss parabolic versions of eulers identity eitcos t i sin t a purely algebraic approach based on dual numbers is known to produce a very trivial relation ept 1pt therefore we use a geometric setup of parabolic rotations to recover the corresponding nontrivial algebraic framework our main tool is moebius transform... | [['we', 'discuss', 'parabolic', 'versions', 'of', 'eulers', 'identity', 'eitcos', 't', 'i', 'sin', 't', 'a', 'purely', 'algebraic', 'approach', 'based', 'on', 'dual', 'numbers', 'is', 'known', 'to', 'produce', 'a', 'very', 'trivial', 'relation', 'ept', '1pt', 'therefore', 'we', 'use', 'a', 'geometric', 'setup', 'of', '... | [-0.18073379062116146, 0.09259452095153765, -0.13838939718698384, 0.1089256408636291, -0.20470539182543945, -0.18369462054509383, 0.0017506291206257467, 0.29812943500777084, -0.37073075914612186, -0.24460216492223433, 0.0991227944703916, -0.21500809811569083, -0.20237559901598173, 0.22488902275187847, -0.12826621998101... |
707.4025 | On the Cohomological Derivation of Yang-Mills Theory in the Antifield
Formalism | We present a brief review of the cohomological solutions of self-coupling
interactions of the fields in the free Yang-Mills theory. All consistent
interactions among the fields have been obtained using the antifield formalism
through several order BRST deformations of the master equation. It is found
that the couplin... | physics.gen-ph | we present a brief review of the cohomological solutions of selfcoupling interactions of the fields in the free yangmills theory all consistent interactions among the fields have been obtained using the antifield formalism through several order brst deformations of the master equation it is found that the coupling defo... | [['we', 'present', 'a', 'brief', 'review', 'of', 'the', 'cohomological', 'solutions', 'of', 'selfcoupling', 'interactions', 'of', 'the', 'fields', 'in', 'the', 'free', 'yangmills', 'theory', 'all', 'consistent', 'interactions', 'among', 'the', 'fields', 'have', 'been', 'obtained', 'using', 'the', 'antifield', 'formalis... | [-0.1861328026037905, 0.15725267155386216, -0.09276837538610297, 0.07563960191328079, -0.08007546542696171, -0.07039277216226056, -0.0711692069829502, 0.2831102693453431, -0.22422055781564929, -0.27041450215431, 0.06700079205790656, -0.28537027093932615, -0.19832507118752057, 0.09171964620034416, -0.008436093143151179,... |
707.4026 | Renormalization and black hole entropy in Loop Quantum Gravity | Microscopic state counting for a black hole in Loop Quantum Gravity yields a
result proportional to horizon area, and inversely proportional to Newton's
constant and the Immirzi parameter. It is argued here that before this result
can be compared to the Bekenstein-Hawking entropy of a macroscopic black hole,
the scal... | gr-qc hep-th | microscopic state counting for a black hole in loop quantum gravity yields a result proportional to horizon area and inversely proportional to newtons constant and the immirzi parameter it is argued here that before this result can be compared to the bekensteinhawking entropy of a macroscopic black hole the scale depen... | [['microscopic', 'state', 'counting', 'for', 'a', 'black', 'hole', 'in', 'loop', 'quantum', 'gravity', 'yields', 'a', 'result', 'proportional', 'to', 'horizon', 'area', 'and', 'inversely', 'proportional', 'to', 'newtons', 'constant', 'and', 'the', 'immirzi', 'parameter', 'it', 'is', 'argued', 'here', 'that', 'before', ... | [-0.14569567758475005, 0.19200717662403613, -0.12025644887744645, 0.11244734393915644, -0.10720234033134249, -0.21279779555172557, 0.030206811680446987, 0.2418084405362606, -0.2315153328034981, -0.30821943076120484, 0.09724662393578731, -0.3132505455042845, -0.0727524692652586, 0.2253595676135134, -0.10638699562714239,... |
707.4027 | Large Kinetic Power in FRII Radio Jets | We investigate the total kinetic powers (L_{j}) and ages (t_{age}) of
powerful jets of four FR II radio sources (Cygnus A, 3C 223, 3C 284, and 3C
219) by the detail comparison of the dynamical model of expanding cocoons with
observed ones. It is found that these sources have quite large kinetic powers
with the ratio ... | astro-ph | we investigate the total kinetic powers l_j and ages t_age of powerful jets of four fr ii radio sources cygnus a 3c 223 3c 284 and 3c 219 by the detail comparison of the dynamical model of expanding cocoons with observed ones it is found that these sources have quite large kinetic powers with the ratio of l_j to the ed... | [['we', 'investigate', 'the', 'total', 'kinetic', 'powers', 'l_j', 'and', 'ages', 't_age', 'of', 'powerful', 'jets', 'of', 'four', 'fr', 'ii', 'radio', 'sources', 'cygnus', 'a', '3c', '223', '3c', '284', 'and', '3c', '219', 'by', 'the', 'detail', 'comparison', 'of', 'the', 'dynamical', 'model', 'of', 'expanding', 'coco... | [-0.10076021514832974, 0.18687340438676378, 0.005160884140059352, 0.1416297986113932, -0.04440071608017509, -0.09233892652458356, 0.023424474219791592, 0.38663986344472506, -0.18382696219099065, -0.39178792741149665, 0.027588709497164625, -0.29744591874380905, 0.054832720512058584, 0.18468493628897703, 0.05065826428278... |
707.4028 | The Symmetries and Redundancies of Terror: Patterns in the Dark, A study
of Terrorist Network Strategy and Structure | Although much political capital has been made regarding the war on terrorism,
and while appropriations have gotten underway, there has been a dearth of deep
work on counter-terrorism, and despite massive efforts by the federal
government, most cities and states do not have a robust response system. In
fact, most do n... | nlin.AO | although much political capital has been made regarding the war on terrorism and while appropriations have gotten underway there has been a dearth of deep work on counterterrorism and despite massive efforts by the federal government most cities and states do not have a robust response system in fact most do not yet ha... | [['although', 'much', 'political', 'capital', 'has', 'been', 'made', 'regarding', 'the', 'war', 'on', 'terrorism', 'and', 'while', 'appropriations', 'have', 'gotten', 'underway', 'there', 'has', 'been', 'a', 'dearth', 'of', 'deep', 'work', 'on', 'counterterrorism', 'and', 'despite', 'massive', 'efforts', 'by', 'the', '... | [-0.06635014302769883, 0.06353770581901902, -0.07309272970370431, 0.08054983933349529, -0.07670934429431024, -0.1353542093679102, 0.09305475817220416, 0.3968333354892416, -0.16937586782377265, -0.32849334191349855, 0.17223552882448226, -0.3319011481039019, -0.16829544130531657, 0.19327010373429707, -0.13841750051748627... |
707.4029 | Tetrahedron equations and nilpotent subalgebras of U_q(sl_n) | A relation between q-oscillator R-matrix of the tetrahedron equation and
decompositions of Poinkare-Birkhoff-Witt type bases for nilpotent subalgebras
of U_q(sl_n) is observed.
| math.QA | a relation between qoscillator rmatrix of the tetrahedron equation and decompositions of poinkarebirkhoffwitt type bases for nilpotent subalgebras of u_qsl_n is observed | [['a', 'relation', 'between', 'qoscillator', 'rmatrix', 'of', 'the', 'tetrahedron', 'equation', 'and', 'decompositions', 'of', 'poinkarebirkhoffwitt', 'type', 'bases', 'for', 'nilpotent', 'subalgebras', 'of', 'u_qsl_n', 'is', 'observed']] | [-0.1583893528579557, 0.026223919487425258, -0.07103343627282552, 0.06054447392290015, -0.14514123555272818, -0.16263048259896182, -0.031173699047593845, 0.3312819706542151, -0.3526465435113226, -0.17668301949188822, 0.08209583353960798, -0.30691047474032357, -0.10941109921605814, 0.18505008962182773, -0.03601504627260... |
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