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 |
|---|---|---|---|---|---|---|
708.0849 | The mass-critical nonlinear Schr\"odinger equation with radial data in
dimensions three and higher | We establish global well-posedness and scattering for solutions to the
mass-critical nonlinear Schr\"odinger equation $iu_t + \Delta u = \pm |u|^{4/d}
u$ for large spherically symmetric L^2_x(R^d) initial data in dimensions $d\geq
3$. In the focusing case we require that the mass is strictly less than that of
the gro... | math.AP | we establish global wellposedness and scattering for solutions to the masscritical nonlinear schrodinger equation iu_t delta u pm u4d u for large spherically symmetric l2_xrd initial data in dimensions dgeq 3 in the focusing case we require that the mass is strictly less than that of the ground state as a consequence w... | [['we', 'establish', 'global', 'wellposedness', 'and', 'scattering', 'for', 'solutions', 'to', 'the', 'masscritical', 'nonlinear', 'schrodinger', 'equation', 'iu_t', 'delta', 'u', 'pm', 'u4d', 'u', 'for', 'large', 'spherically', 'symmetric', 'l2_xrd', 'initial', 'data', 'in', 'dimensions', 'dgeq', '3', 'in', 'the', 'fo... | [-0.16047223136070873, 0.07664057585809912, -0.02683347945597458, 0.07241293778128971, -0.03338257503973973, -0.1674163856954834, -0.028026683243934983, 0.304575047939532, -0.1960009199796946, -0.21144533090825593, 0.16745722875174426, -0.3395301584251128, -0.04211812179729149, 0.12935427635569463, 0.029504162307780284... |
708.085 | Relations between random coding exponents and the statistical physics of
random codes | The partition function pertaining to finite--temperature decoding of a
(typical) randomly chosen code is known to have three types of behavior,
corresponding to three phases in the plane of rate vs. temperature: the {\it
ferromagnetic phase}, corresponding to correct decoding, the {\it paramagnetic
phase}, of complet... | cs.IT math.IT | the partition function pertaining to finitetemperature decoding of a typical randomly chosen code is known to have three types of behavior corresponding to three phases in the plane of rate vs temperature the it ferromagnetic phase corresponding to correct decoding the it paramagnetic phase of complete disorder which i... | [['the', 'partition', 'function', 'pertaining', 'to', 'finitetemperature', 'decoding', 'of', 'a', 'typical', 'randomly', 'chosen', 'code', 'is', 'known', 'to', 'have', 'three', 'types', 'of', 'behavior', 'corresponding', 'to', 'three', 'phases', 'in', 'the', 'plane', 'of', 'rate', 'vs', 'temperature', 'the', 'it', 'fer... | [-0.1328966960042961, 0.18538250064018527, -0.08441192355613171, 0.08230659354122286, -0.00978898688604976, -0.18311577122702422, 0.10939793367342988, 0.34941268072656867, -0.2950031632999011, -0.2454624605312381, 0.10363831827834354, -0.2950749893185138, -0.15277872190982067, 0.17049173224840383, -0.040943905000601244... |
708.0851 | Towards linear phononics and nonlocality tests in ion traps | We explore the possibility to manipulate massive, i.e. motional, degrees of
freedom of trapped ions. In particular, we demonstrate that, if local control
of the trapping frequencies is achieved, one can reproduce the full toolbox of
linear optics on radial modes. Furthermore, assuming only global control of the
trapp... | quant-ph | we explore the possibility to manipulate massive ie motional degrees of freedom of trapped ions in particular we demonstrate that if local control of the trapping frequencies is achieved one can reproduce the full toolbox of linear optics on radial modes furthermore assuming only global control of the trapping potentia... | [['we', 'explore', 'the', 'possibility', 'to', 'manipulate', 'massive', 'ie', 'motional', 'degrees', 'of', 'freedom', 'of', 'trapped', 'ions', 'in', 'particular', 'we', 'demonstrate', 'that', 'if', 'local', 'control', 'of', 'the', 'trapping', 'frequencies', 'is', 'achieved', 'one', 'can', 'reproduce', 'the', 'full', 't... | [-0.15712984573096037, 0.19058206184456747, -0.06938042910769582, -0.015747949647096297, -0.036638496170441306, -0.1614374737193187, 0.04257203532382846, 0.3688693328946829, -0.2613507972533504, -0.28955269674460093, 0.05354195903831472, -0.23181710949788492, -0.08735297151501678, 0.1802326769878467, -0.021260854701201... |
708.0852 | Starbursts in the Local Universe: new HST/ACS observations of the
irregular galaxy NGC 4449 | We present photometry with the Advanced Camera for Surveys (ACS) on the
Hubble Space Telescope (HST) of stars in the Magellanic starburst galaxy NGC
4449. The galaxy has been imaged in the F435W (B), F555W (V) and F814W (I)
broad-band filters, and in the F658N (Halpha) narrow-band filter. Our
photometry includes ~300... | astro-ph | we present photometry with the advanced camera for surveys acs on the hubble space telescope hst of stars in the magellanic starburst galaxy ngc 4449 the galaxy has been imaged in the f435w b f555w v and f814w i broadband filters and in the f658n halpha narrowband filter our photometry includes 300000 objects in the b ... | [['we', 'present', 'photometry', 'with', 'the', 'advanced', 'camera', 'for', 'surveys', 'acs', 'on', 'the', 'hubble', 'space', 'telescope', 'hst', 'of', 'stars', 'in', 'the', 'magellanic', 'starburst', 'galaxy', 'ngc', '4449', 'the', 'galaxy', 'has', 'been', 'imaged', 'in', 'the', 'f435w', 'b', 'f555w', 'v', 'and', 'f8... | [-0.02861568080003893, 0.07111913522295743, -0.11155203641660941, 0.05681948814800797, -0.12252871799103629, -0.050130503862881315, 0.06775391861223258, 0.49686993200045365, -0.14228726818468063, -0.35601147262160127, 0.021625060269322535, -0.3082485372531944, -0.010870863369200378, 0.17475197312014643, -0.102145337718... |
708.0853 | Embeddings of discrete groups and the speed of random walks | For a finitely generated group G and a banach space X let \alpha^*_X(G)
(respectively \alpha^#_X(G)) be the supremum over all \alpha\ge 0 such that
there exists a Lipschitz mapping (respectively an equivariant mapping) f:G\to X
and c>0 such that for all x,y\in G we have \|f(x)-f(y)\|\ge c\cdot
d_G(x,y)^\alpha. In par... | math.MG math.FA math.GR | for a finitely generated group g and a banach space x let alpha_xg respectively alpha_xg be the supremum over all alphage 0 such that there exists a lipschitz mapping respectively an equivariant mapping fgto x and c0 such that for all xyin g we have fxfyge ccdot d_gxyalpha in particular the hilbert compression exponent... | [['for', 'a', 'finitely', 'generated', 'group', 'g', 'and', 'a', 'banach', 'space', 'x', 'let', 'alpha_xg', 'respectively', 'alpha_xg', 'be', 'the', 'supremum', 'over', 'all', 'alphage', '0', 'such', 'that', 'there', 'exists', 'a', 'lipschitz', 'mapping', 'respectively', 'an', 'equivariant', 'mapping', 'fgto', 'x', 'an... | [-0.13370318607334433, 0.13271921163689804, -0.05360923443932503, 0.02003284771028226, -0.05015701168343324, -0.1722873799866104, 0.06604848926910102, 0.38894250836074584, -0.3231061923248052, -0.2174628346045482, 0.09666055192083074, -0.29220170481710145, -0.14194152404890392, 0.18879377130898203, -0.11078286794481869... |
708.0854 | On the point spectrum of some perturbed differential operators with
periodic coefficients | Finiteness of the point spectrum of linear operators acting in a Banach space
is investigated from point of view of perturbation theory. In the first part of
the paper we present an abstract result based on analytical continuation of the
resolvent function through continuous spectrum. In the second part, the
abstract... | math.SP math.FA | finiteness of the point spectrum of linear operators acting in a banach space is investigated from point of view of perturbation theory in the first part of the paper we present an abstract result based on analytical continuation of the resolvent function through continuous spectrum in the second part the abstract resu... | [['finiteness', 'of', 'the', 'point', 'spectrum', 'of', 'linear', 'operators', 'acting', 'in', 'a', 'banach', 'space', 'is', 'investigated', 'from', 'point', 'of', 'view', 'of', 'perturbation', 'theory', 'in', 'the', 'first', 'part', 'of', 'the', 'paper', 'we', 'present', 'an', 'abstract', 'result', 'based', 'on', 'ana... | [-0.12327433472499251, 0.05016804201256794, -0.11475219960014026, 0.04017961672507227, -0.08371499951307972, -0.03079199851800998, -0.022598837378124396, 0.3003905405973395, -0.33873683502276736, -0.19753553330898285, 0.14163057606201618, -0.2938056563710173, -0.1894366931108137, 0.19888020100692907, -0.076678949228177... |
708.0855 | Kinetic corrections to B -> X_c l nu at one loop | We evaluate the one-loop corrections to the Wilson coefficient of the kinetic
operator in the operator product expansion of the differential B -> X_c l nu
decay rate. With a moderate cut on the lepton energy, the one-loop terms change
the kinetic operator contributions to spectral moments by about 20%. This
amounts t... | hep-ph | we evaluate the oneloop corrections to the wilson coefficient of the kinetic operator in the operator product expansion of the differential b x_c l nu decay rate with a moderate cut on the lepton energy the oneloop terms change the kinetic operator contributions to spectral moments by about 20 this amounts to a small c... | [['we', 'evaluate', 'the', 'oneloop', 'corrections', 'to', 'the', 'wilson', 'coefficient', 'of', 'the', 'kinetic', 'operator', 'in', 'the', 'operator', 'product', 'expansion', 'of', 'the', 'differential', 'b', 'x_c', 'l', 'nu', 'decay', 'rate', 'with', 'a', 'moderate', 'cut', 'on', 'the', 'lepton', 'energy', 'the', 'on... | [-0.10444607321253938, 0.19241737184917007, -0.03415594117958908, 0.09308925294418535, -0.04472944255027434, -0.06682423045453818, 0.0734243387842308, 0.26748072339788725, -0.21113416469939378, -0.26364441637111746, 0.05408190599055556, -0.35687129909739546, -0.014488035553823346, 0.12626788373226705, 0.064264607316125... |
708.0856 | Triple oscillating field technique for accurate measurements of
couplings in homonuclear spin systems | We present a new concept for homonuclear dipolar recoupling in
magic-angle-spinning (MAS) solid-state NMR experiments which avoids the problem
of dipolar truncation. This is accomplished through the introduction of a new
NMR pulse sequence design principle: the triple oscillating field technique. We
demonstrate this ... | quant-ph | we present a new concept for homonuclear dipolar recoupling in magicanglespinning mas solidstate nmr experiments which avoids the problem of dipolar truncation this is accomplished through the introduction of a new nmr pulse sequence design principle the triple oscillating field technique we demonstrate this technique ... | [['we', 'present', 'a', 'new', 'concept', 'for', 'homonuclear', 'dipolar', 'recoupling', 'in', 'magicanglespinning', 'mas', 'solidstate', 'nmr', 'experiments', 'which', 'avoids', 'the', 'problem', 'of', 'dipolar', 'truncation', 'this', 'is', 'accomplished', 'through', 'the', 'introduction', 'of', 'a', 'new', 'nmr', 'pu... | [-0.14537586402292688, 0.19502535846423846, -0.04492445396040055, 0.0011025106707975442, -0.03812672580340662, -0.15839049860167537, 0.04471234724698104, 0.42320175701483137, -0.27219628979791105, -0.29109470454324576, -0.027696221925565877, -0.2367805104091699, -0.10678498703189668, 0.20543017546307143, 0.040495278534... |
708.0857 | The effects of clumping on wind line variability | We review the effects of clumping on the profiles of resonance doublets. By
allowing the ratio of the doublet oscillator strenghts to be a free parameter,
we demonstrate that doublet profiles contain more information than is normally
utilized. In clumped (or porous) winds, this ratio can lies between unity and
the ra... | astro-ph | we review the effects of clumping on the profiles of resonance doublets by allowing the ratio of the doublet oscillator strenghts to be a free parameter we demonstrate that doublet profiles contain more information than is normally utilized in clumped or porous winds this ratio can lies between unity and the ratio of t... | [['we', 'review', 'the', 'effects', 'of', 'clumping', 'on', 'the', 'profiles', 'of', 'resonance', 'doublets', 'by', 'allowing', 'the', 'ratio', 'of', 'the', 'doublet', 'oscillator', 'strenghts', 'to', 'be', 'a', 'free', 'parameter', 'we', 'demonstrate', 'that', 'doublet', 'profiles', 'contain', 'more', 'information', '... | [-0.08291376903756954, 0.1100713824200782, -0.06662538634304693, 0.031511266877471356, -0.07834640683481695, -0.12373934225861434, 0.043602662064783144, 0.3919283469225381, -0.21631664249476543, -0.3413150863615191, 0.06962232255884061, -0.2588085094763405, -0.06494451087460539, 0.17016681326126123, -0.0205045444045548... |
708.0858 | Fermi-surface calculation of the anomalous Hall conductivity | While the intrinsic anomalous Hall conductivity is normally written in terms
of an integral of the electronic Berry curvature over the occupied portions of
the Brillouin zone, Haldane has recently pointed out that this quantity (or
more precisely, its ``non-quantized part'') may alternatively be expressed as a
Fermi-... | cond-mat.mtrl-sci | while the intrinsic anomalous hall conductivity is normally written in terms of an integral of the electronic berry curvature over the occupied portions of the brillouin zone haldane has recently pointed out that this quantity or more precisely its nonquantized part may alternatively be expressed as a fermisurface prop... | [['while', 'the', 'intrinsic', 'anomalous', 'hall', 'conductivity', 'is', 'normally', 'written', 'in', 'terms', 'of', 'an', 'integral', 'of', 'the', 'electronic', 'berry', 'curvature', 'over', 'the', 'occupied', 'portions', 'of', 'the', 'brillouin', 'zone', 'haldane', 'has', 'recently', 'pointed', 'out', 'that', 'this'... | [-0.1823795018412122, 0.15319748097786795, -0.07535273877575117, 0.05080870649360154, -0.048653755758412826, -0.07368698812667196, 0.06850226714520197, 0.3754163405297501, -0.26379710557655645, -0.2579302972227933, 0.0469011893370547, -0.3120240127969095, -0.13870203176806195, 0.19518939059488982, 0.029466042851363373,... |
708.0859 | Exponential Separation of Quantum and Classical Non-Interactive
Multi-Party Communication Complexity | We give the first exponential separation between quantum and classical
multi-party communication complexity in the (non-interactive) one-way and
simultaneous message passing settings.
For every k, we demonstrate a relational communication problem between k
parties that can be solved exactly by a quantum simultaneou... | quant-ph | we give the first exponential separation between quantum and classical multiparty communication complexity in the noninteractive oneway and simultaneous message passing settings for every k we demonstrate a relational communication problem between k parties that can be solved exactly by a quantum simultaneous message p... | [['we', 'give', 'the', 'first', 'exponential', 'separation', 'between', 'quantum', 'and', 'classical', 'multiparty', 'communication', 'complexity', 'in', 'the', 'noninteractive', 'oneway', 'and', 'simultaneous', 'message', 'passing', 'settings', 'for', 'every', 'k', 'we', 'demonstrate', 'a', 'relational', 'communicatio... | [-0.26946465801247343, 0.1022311569058827, -0.04199591805277172, 0.04053556936873143, -0.0018357832425384111, -0.35318345652132105, 0.16778416418400344, 0.34539485911047585, -0.3455809518214195, -0.32901778376551083, 0.03349148598249241, -0.2371038063329154, -0.08627710297894013, 0.17266207234182906, -0.075958535145287... |
708.086 | Establishing the nature of companion candidates to X-ray emitting late
B-type stars | The most favored interpretation for the detection of X-ray emission from late
B-type stars is that these stars have a yet undiscovered late-type companion
(or an unbound nearby late-type star) that produces the X-rays. Several faint
IR objects at (sub)-arcsecond separation from B-type stars have been uncovered
in our... | astro-ph | the most favored interpretation for the detection of xray emission from late btype stars is that these stars have a yet undiscovered latetype companion or an unbound nearby latetype star that produces the xrays several faint ir objects at subarcsecond separation from btype stars have been uncovered in our earlier adapt... | [['the', 'most', 'favored', 'interpretation', 'for', 'the', 'detection', 'of', 'xray', 'emission', 'from', 'late', 'btype', 'stars', 'is', 'that', 'these', 'stars', 'have', 'a', 'yet', 'undiscovered', 'latetype', 'companion', 'or', 'an', 'unbound', 'nearby', 'latetype', 'star', 'that', 'produces', 'the', 'xrays', 'seve... | [-0.036329995407672816, 0.10394924947006505, -0.11269284752623168, 0.08593546353488339, -0.1461960725293505, -0.10100172585006603, 0.048483718587811635, 0.466912140669201, -0.11244994728457963, -0.372518871793203, 0.09078772042900504, -0.32704416932838576, -0.029057994375996772, 0.21080014854419216, -0.0498897145947902... |
708.0861 | Shot-Noise-Limited Operation of a Fast Quantum-Point-Contact Charge
Sensor | We have operated a quantum point contact (QPC) charge detector in a radio
frequency (RF) mode that allows fast charge detection in a bandwidth of tens of
megahertz. We find that the charge sensitivity of the RF-QPC is limited not by
the noise of a secondary amplifier, but by non-equilibrium noise f the QPC
itself. We... | cond-mat.mes-hall | we have operated a quantum point contact qpc charge detector in a radio frequency rf mode that allows fast charge detection in a bandwidth of tens of megahertz we find that the charge sensitivity of the rfqpc is limited not by the noise of a secondary amplifier but by nonequilibrium noise f the qpc itself we have perfo... | [['we', 'have', 'operated', 'a', 'quantum', 'point', 'contact', 'qpc', 'charge', 'detector', 'in', 'a', 'radio', 'frequency', 'rf', 'mode', 'that', 'allows', 'fast', 'charge', 'detection', 'in', 'a', 'bandwidth', 'of', 'tens', 'of', 'megahertz', 'we', 'find', 'that', 'the', 'charge', 'sensitivity', 'of', 'the', 'rfqpc'... | [-0.18423174555831845, 0.1464676103601907, -0.05499074513165621, -0.0012726128671615236, 0.010501133291509705, -0.1393472716090796, 0.11683556874218545, 0.3817815447320649, -0.2263203458185645, -0.3022541355723819, 0.024877494190941037, -0.30426936359256523, -0.12918006378374453, 0.20290928795778504, -0.042410838264175... |
708.0862 | Reliability of temporal coding on pulse-coupled networks of oscillators | We study the reliability of spike output in a general class of pulse-coupled
oscillators receiving a fluctuating input. Showing that this problem is
equivalent to noise-induced synchronization between identical networks of
oscillators, we employ the phase reduction method to analytically derive the
average Lyapunov e... | nlin.AO cond-mat.dis-nn q-bio.NC | we study the reliability of spike output in a general class of pulsecoupled oscillators receiving a fluctuating input showing that this problem is equivalent to noiseinduced synchronization between identical networks of oscillators we employ the phase reduction method to analytically derive the average lyapunov exponen... | [['we', 'study', 'the', 'reliability', 'of', 'spike', 'output', 'in', 'a', 'general', 'class', 'of', 'pulsecoupled', 'oscillators', 'receiving', 'a', 'fluctuating', 'input', 'showing', 'that', 'this', 'problem', 'is', 'equivalent', 'to', 'noiseinduced', 'synchronization', 'between', 'identical', 'networks', 'of', 'osci... | [-0.19650560308693218, 0.15408309281338006, -0.04217921330532788, 0.04157338661531432, -0.037108860720763914, -0.18149340409866493, 0.13218893937807044, 0.38268790074178705, -0.24692453792996946, -0.27339419863599923, 0.0380791677731474, -0.26434359130950685, -0.2500661857750105, 0.16770173186871587, -0.046396853321272... |
708.0863 | Enhance synchronizability via age-based coupling | In this brief report, we study the synchronization of growing scale-free
networks. An asymmetrical age-based coupling method is proposed with only one
free parameter $\alpha$. Although the coupling matrix is asymmetric, our
coupling method could guarantee that all the eigenvalues are non-negative
reals. The eignerati... | cond-mat.dis-nn cond-mat.stat-mech | in this brief report we study the synchronization of growing scalefree networks an asymmetrical agebased coupling method is proposed with only one free parameter alpha although the coupling matrix is asymmetric our coupling method could guarantee that all the eigenvalues are nonnegative reals the eigneratio r will appr... | [['in', 'this', 'brief', 'report', 'we', 'study', 'the', 'synchronization', 'of', 'growing', 'scalefree', 'networks', 'an', 'asymmetrical', 'agebased', 'coupling', 'method', 'is', 'proposed', 'with', 'only', 'one', 'free', 'parameter', 'alpha', 'although', 'the', 'coupling', 'matrix', 'is', 'asymmetric', 'our', 'coupli... | [-0.20982031612233681, 0.1369235762926771, -0.030580551134930415, 0.00782439886719327, -0.06038307963277806, -0.18450145447118715, -0.012435507198626345, 0.3834964795498474, -0.2566917243074964, -0.2631847065619447, 0.07579687287268991, -0.2802025509320877, -0.19896002168005164, 0.14049031815745613, -0.0194366460412063... |
708.0864 | The Local Void is Really Empty | Are voids in the distribution of galaxies only places with reduced matter
density and low star formation efficiency or are they empty of matter? There is
now compelling evidence of expansion away from the Local Void at very high
velocities. The motion is most reasonably interpreted as an evacuation of the
void, which... | astro-ph | are voids in the distribution of galaxies only places with reduced matter density and low star formation efficiency or are they empty of matter there is now compelling evidence of expansion away from the local void at very high velocities the motion is most reasonably interpreted as an evacuation of the void which requ... | [['are', 'voids', 'in', 'the', 'distribution', 'of', 'galaxies', 'only', 'places', 'with', 'reduced', 'matter', 'density', 'and', 'low', 'star', 'formation', 'efficiency', 'or', 'are', 'they', 'empty', 'of', 'matter', 'there', 'is', 'now', 'compelling', 'evidence', 'of', 'expansion', 'away', 'from', 'the', 'local', 'vo... | [-0.08358265616236225, 0.146212513981958, -0.1193796522944929, 0.09772718097970244, -0.07836214991449009, -0.04290797885152556, 0.029208282910523905, 0.38322625190965715, -0.18113913376157778, -0.3664616630782211, 0.10258710012394226, -0.2681821613676018, -0.02128323368240325, 0.14363793997345345, -0.009608380866074373... |
708.0865 | The effect of memory on functional large deviations of infinite moving
average processes | The large deviations of an infinite moving average process with exponentially
light tails are very similar to those of an i.i.d. sequence as long as the
coefficients decay fast enough. If they do not, the large deviations change
dramatically. We study this phenomenon in the context of functional large,
moderate and h... | math.PR | the large deviations of an infinite moving average process with exponentially light tails are very similar to those of an iid sequence as long as the coefficients decay fast enough if they do not the large deviations change dramatically we study this phenomenon in the context of functional large moderate and huge devia... | [['the', 'large', 'deviations', 'of', 'an', 'infinite', 'moving', 'average', 'process', 'with', 'exponentially', 'light', 'tails', 'are', 'very', 'similar', 'to', 'those', 'of', 'an', 'iid', 'sequence', 'as', 'long', 'as', 'the', 'coefficients', 'decay', 'fast', 'enough', 'if', 'they', 'do', 'not', 'the', 'large', 'dev... | [-0.09682581940217426, 0.2193107286309694, -0.09627586944649617, 0.14442954453359022, -0.04883719201165217, -0.11116518497605014, 0.047400501560467226, 0.35506673167563146, -0.3387750747303168, -0.31091195851978326, 0.1322353807325406, -0.2982358087557023, -0.11030733814092215, 0.1802340806138495, -0.08640905753364442,... |
708.0866 | Singular Potentials in Quantum Mechanics and Ambiguity in the
Self-Adjoint Hamiltonian | For a class of singular potentials, including the Coulomb potential (in three
and less dimensions) and $V(x) = g/x^2$ with the coefficient $g$ in a certain
range ($x$ being a space coordinate in one or more dimensions), the
corresponding Schr\"odinger operator is not automatically self-adjoint on its
natural domain. ... | quant-ph | for a class of singular potentials including the coulomb potential in three and less dimensions and vx gx2 with the coefficient g in a certain range x being a space coordinate in one or more dimensions the corresponding schrodinger operator is not automatically selfadjoint on its natural domain such operators admit mor... | [['for', 'a', 'class', 'of', 'singular', 'potentials', 'including', 'the', 'coulomb', 'potential', 'in', 'three', 'and', 'less', 'dimensions', 'and', 'vx', 'gx2', 'with', 'the', 'coefficient', 'g', 'in', 'a', 'certain', 'range', 'x', 'being', 'a', 'space', 'coordinate', 'in', 'one', 'or', 'more', 'dimensions', 'the', '... | [-0.10829307555061167, 0.09236147702904418, -0.05853128511938197, 0.0839271393766168, -0.11742187845138416, -0.14707959037440926, -0.0331298992960408, 0.3442318579321032, -0.24614056204654164, -0.23150988662643218, 0.1261952594313562, -0.30206625238616963, -0.1489025428561049, 0.19708955845163106, -0.07119266165128506,... |
708.0867 | Gauge Theory Model of the Neutrino and New Physics Beyond the Standard
Model | Majorana features of neutrinos and SO(3) gauge symmetry of three families
enable us to construct a gauge model of neutrino for understanding naturally
the observed smallness of neutrino masses and the nearly tri-bimaximal neutrino
mixing when combining together with the mechanism of approximate global U(1)
family sym... | hep-ph | majorana features of neutrinos and so3 gauge symmetry of three families enable us to construct a gauge model of neutrino for understanding naturally the observed smallness of neutrino masses and the nearly tribimaximal neutrino mixing when combining together with the mechanism of approximate global u1 family symmetry t... | [['majorana', 'features', 'of', 'neutrinos', 'and', 'so3', 'gauge', 'symmetry', 'of', 'three', 'families', 'enable', 'us', 'to', 'construct', 'a', 'gauge', 'model', 'of', 'neutrino', 'for', 'understanding', 'naturally', 'the', 'observed', 'smallness', 'of', 'neutrino', 'masses', 'and', 'the', 'nearly', 'tribimaximal', ... | [-0.1374109909107398, 0.35229722241556083, 0.009430347926794522, 0.18341942548079626, -0.11921052690294962, -0.2090947989847571, -0.006852689972748199, 0.3401020266089378, -0.21912241047773992, -0.3006485580436645, 0.04735813068222224, -0.2585955200108489, -0.04950818752930049, 0.07074211598298843, 0.09301169182834847,... |
708.0868 | An Improved Semi-Analytical Spherical Collapse Model for Non-linear
Density Evolution | We derive a semi-analytical extension of the spherical collapse model of
structure formation that takes account of the effects of deviations from
spherical symmetry and shell crossing which are important in the non-linear
regime. Our model is designed so that it predicts a relation between the
peculiar velocity and d... | astro-ph gr-qc | we derive a semianalytical extension of the spherical collapse model of structure formation that takes account of the effects of deviations from spherical symmetry and shell crossing which are important in the nonlinear regime our model is designed so that it predicts a relation between the peculiar velocity and densit... | [['we', 'derive', 'a', 'semianalytical', 'extension', 'of', 'the', 'spherical', 'collapse', 'model', 'of', 'structure', 'formation', 'that', 'takes', 'account', 'of', 'the', 'effects', 'of', 'deviations', 'from', 'spherical', 'symmetry', 'and', 'shell', 'crossing', 'which', 'are', 'important', 'in', 'the', 'nonlinear',... | [-0.06283793081235055, 0.07926453287458488, -0.16715034826433864, 0.1296914169235669, -0.07287355389809985, -0.11958401938151011, -0.00413251239485268, 0.3434468249137374, -0.21572560129082366, -0.3107975973565688, 0.08677629003938202, -0.2241885608795431, -0.12118226864599976, 0.17740256143947955, 0.024757891131502084... |
708.0869 | Asymptotic Curvature Decay and Removal of Singularities of Bach-Flat
Metrics | We prove a removal of singularities result for Bach-flat metrics in dimension
4 under the assumption of bounded L^2 norm of curvature, bounded Sobolev
constant and a volume growth bound. This result extends the removal of
singularities result for special classes of Bach-flat metrics obtained in
\cite{TVMOD}. For the ... | math.DG math.AP | we prove a removal of singularities result for bachflat metrics in dimension 4 under the assumption of bounded l2 norm of curvature bounded sobolev constant and a volume growth bound this result extends the removal of singularities result for special classes of bachflat metrics obtained in citetvmod for the proof we an... | [['we', 'prove', 'a', 'removal', 'of', 'singularities', 'result', 'for', 'bachflat', 'metrics', 'in', 'dimension', '4', 'under', 'the', 'assumption', 'of', 'bounded', 'l2', 'norm', 'of', 'curvature', 'bounded', 'sobolev', 'constant', 'and', 'a', 'volume', 'growth', 'bound', 'this', 'result', 'extends', 'the', 'removal'... | [-0.16415935042362237, 0.04174951865510612, -0.08665612143417581, 0.10019222226776375, -0.038662514961372636, -0.12701847539139316, -0.014109904378575762, 0.2996972262734528, -0.2608075737089072, -0.2031085567450458, 0.13350630704596753, -0.2702146309365509, -0.1347623030395852, 0.17626770608098313, -0.1291027655248943... |
708.087 | Milky Way Kinematics: Measurements at the Subcentral Point of the Fourth
Quadrant | We use atomic hydrogen (HI) data from the Southern Galactic Plane Survey to
study the kinematics of the fourth quadrant of the Milky Way. By measuring the
terminal velocity as a function of longitude throughout the fourth Galactic
quadrant we have derived the most densely sampled rotation curve available for
the Milk... | astro-ph | we use atomic hydrogen hi data from the southern galactic plane survey to study the kinematics of the fourth quadrant of the milky way by measuring the terminal velocity as a function of longitude throughout the fourth galactic quadrant we have derived the most densely sampled rotation curve available for the milky way... | [['we', 'use', 'atomic', 'hydrogen', 'hi', 'data', 'from', 'the', 'southern', 'galactic', 'plane', 'survey', 'to', 'study', 'the', 'kinematics', 'of', 'the', 'fourth', 'quadrant', 'of', 'the', 'milky', 'way', 'by', 'measuring', 'the', 'terminal', 'velocity', 'as', 'a', 'function', 'of', 'longitude', 'throughout', 'the'... | [-0.10177175682738877, 0.08975983857448254, -0.05063374170486755, 0.030033547529691264, -0.11207364293148936, -0.06355967685297613, 0.029634879487311812, 0.41394127810846515, -0.2677659341000919, -0.32545519670221346, 0.057324712979607284, -0.3032811427841065, -0.009923008926194254, 0.18967455478190487, 0.0054268699570... |
708.0871 | Discovery of Four Gravitationally Lensed Quasars from the Sloan Digital
Sky Survey | We present the discovery of four gravitationally lensed quasars selected from
the spectroscopic quasar catalog of the Sloan Digital Sky Survey. We describe
imaging and spectroscopic follow-up observations that support the lensing
interpretation of the following four quasars: SDSS J0832+0404 (image separation
\theta=1... | astro-ph | we present the discovery of four gravitationally lensed quasars selected from the spectroscopic quasar catalog of the sloan digital sky survey we describe imaging and spectroscopic followup observations that support the lensing interpretation of the following four quasars sdss j08320404 image separation theta198 source... | [['we', 'present', 'the', 'discovery', 'of', 'four', 'gravitationally', 'lensed', 'quasars', 'selected', 'from', 'the', 'spectroscopic', 'quasar', 'catalog', 'of', 'the', 'sloan', 'digital', 'sky', 'survey', 'we', 'describe', 'imaging', 'and', 'spectroscopic', 'followup', 'observations', 'that', 'support', 'the', 'lens... | [-0.046017851755023, -0.019943816512823107, -0.061554997069761155, 0.08845046831876971, -0.24441483036614955, -0.06760320292320103, -0.018094434852246197, 0.42720503829419615, -0.0816223369538784, -0.307828823113814, 0.034843885111622515, -0.4256616493500769, -0.03406856957823038, 0.2285291302204132, -0.037309087859466... |
708.0872 | Decay of massive hair on brane black hole | We study analytically the intermediate and late-time behaviour of the massive
scalar field in the background of static spherically symmetric brane black hole
solutions. The intermediate behavoiur of the scalar field reveals the
dependence on the field's parameter mass as well as the multiple moment l,
while the late-... | hep-th gr-qc | we study analytically the intermediate and latetime behaviour of the massive scalar field in the background of static spherically symmetric brane black hole solutions the intermediate behavoiur of the scalar field reveals the dependence on the fields parameter mass as well as the multiple moment l while the latetime be... | [['we', 'study', 'analytically', 'the', 'intermediate', 'and', 'latetime', 'behaviour', 'of', 'the', 'massive', 'scalar', 'field', 'in', 'the', 'background', 'of', 'static', 'spherically', 'symmetric', 'brane', 'black', 'hole', 'solutions', 'the', 'intermediate', 'behavoiur', 'of', 'the', 'scalar', 'field', 'reveals', ... | [-0.19125934327342387, 0.13074680443467765, -0.08811564166259406, 0.1289043853958619, -0.07291677413138978, -0.11127241935324052, -0.022778807138694963, 0.29618679059284003, -0.16876476776689806, -0.293892290667984, 0.08588095104466353, -0.26641128010493864, -0.07783431620015924, 0.13668848121346072, 0.0789646061201547... |
708.0873 | Momentum transfer to small particles by aloof electron beams | The force exerted on nanoparticles and atomic clusters by fast passing
electrons like those employed in transmission electron microscopes are
calculated and integrated over time to yield the momentum transferred from the
electrons to the particles. Numerical results are offered for metallic and
dielectric particles o... | cond-mat.other | the force exerted on nanoparticles and atomic clusters by fast passing electrons like those employed in transmission electron microscopes are calculated and integrated over time to yield the momentum transferred from the electrons to the particles numerical results are offered for metallic and dielectric particles of d... | [['the', 'force', 'exerted', 'on', 'nanoparticles', 'and', 'atomic', 'clusters', 'by', 'fast', 'passing', 'electrons', 'like', 'those', 'employed', 'in', 'transmission', 'electron', 'microscopes', 'are', 'calculated', 'and', 'integrated', 'over', 'time', 'to', 'yield', 'the', 'momentum', 'transferred', 'from', 'the', '... | [-0.06658778926161787, 0.2391932472395145, -0.034725464869586525, 0.035879231753289074, 0.035912076063523785, -0.13580045301606444, -0.004488996397616847, 0.45516708662089345, -0.2558188545387064, -0.3322379030545664, -0.027425574348743344, -0.34212742376828864, -0.006638057520134357, 0.2757286175511011, 0.019413098762... |
708.0874 | XMM-Newton discovery of 217 s pulsations in the brightest persistent
supersoft X-ray source in M31 | We report on the discovery of a periodic modulation in the bright supersoft
X-ray source XMMU J004252.5+411540 detected in the 2000-2004 XMM-Newton
observations of M31. The source exhibits X-ray pulsations with a period P~217.7
s and a quasi-sinusoidal pulse shape and pulsed fraction ~7-11%. We did not
detect statist... | astro-ph | we report on the discovery of a periodic modulation in the bright supersoft xray source xmmu j0042525411540 detected in the 20002004 xmmnewton observations of m31 the source exhibits xray pulsations with a period p2177 s and a quasisinusoidal pulse shape and pulsed fraction 711 we did not detect statistically significa... | [['we', 'report', 'on', 'the', 'discovery', 'of', 'a', 'periodic', 'modulation', 'in', 'the', 'bright', 'supersoft', 'xray', 'source', 'xmmu', 'j0042525411540', 'detected', 'in', 'the', '20002004', 'xmmnewton', 'observations', 'of', 'm31', 'the', 'source', 'exhibits', 'xray', 'pulsations', 'with', 'a', 'period', 'p2177... | [-0.08960018910993742, 0.15296050130914, -0.08706986830298001, 0.10672494198661298, -0.14207636683483812, -0.101560222751425, 0.11014724014998442, 0.4833828464845923, -0.17888823906039666, -0.34686009637519816, 0.09793711698797927, -0.352984215157874, 0.004328282266933183, 0.2614409247265385, -0.06859410361510745, -0.0... |
708.0875 | The Yale Lar TPC | In this paper we give a concise description of a liquid argon time projection
chamber (LAr TPC) developed at Yale, and present results from its first
calibration run with cosmic rays.
| physics.ins-det hep-ex | in this paper we give a concise description of a liquid argon time projection chamber lar tpc developed at yale and present results from its first calibration run with cosmic rays | [['in', 'this', 'paper', 'we', 'give', 'a', 'concise', 'description', 'of', 'a', 'liquid', 'argon', 'time', 'projection', 'chamber', 'lar', 'tpc', 'developed', 'at', 'yale', 'and', 'present', 'results', 'from', 'its', 'first', 'calibration', 'run', 'with', 'cosmic', 'rays']] | [0.026942410311030764, 0.14220817222432683, -0.18261247580390302, -0.055847682077587855, 0.0021685495251609435, -0.1024634589501206, -0.03304975278930919, 0.36190613863929627, -0.19238291544118716, -0.33225840588490807, 0.07893750515781463, -0.27764635677299193, 0.02201367848582806, 0.18787856841640127, -0.044356784873... |
708.0876 | Plasmons in nearly touching metallic nanoparticles: singular response in
the limit of touching dimers | The response of gold nanoparticle dimers is studied theoretically near and
beyond the limit where the particles are touching. As the particles approach
each other, a dominant dipole feature is observed that is pushed into the
infrared due to interparticle coupling and that is associated with a large
pileup of induced... | cond-mat.other | the response of gold nanoparticle dimers is studied theoretically near and beyond the limit where the particles are touching as the particles approach each other a dominant dipole feature is observed that is pushed into the infrared due to interparticle coupling and that is associated with a large pileup of induced cha... | [['the', 'response', 'of', 'gold', 'nanoparticle', 'dimers', 'is', 'studied', 'theoretically', 'near', 'and', 'beyond', 'the', 'limit', 'where', 'the', 'particles', 'are', 'touching', 'as', 'the', 'particles', 'approach', 'each', 'other', 'a', 'dominant', 'dipole', 'feature', 'is', 'observed', 'that', 'is', 'pushed', '... | [-0.15883685418971114, 0.2206279656897208, -0.04973797629630558, 0.02955144957624875, -0.022070899000871426, -0.17042418233042142, 0.024149655664493282, 0.37534414199132893, -0.2548509549215129, -0.270089793978523, -0.008838272561708023, -0.34415591460143785, -0.12001370472987134, 0.1534171133240944, 0.0398537878030503... |
708.0877 | A Portal Analysis for the Design of a Collaborative Research Environment
for Students and Supervisors (CRESS) within the CSCR Domain | In a previous paper the CSCR domain was defined. Here this is taken to the
next stage where we consider the design of a particular Collaborative Research
Environment to support Students and Supervisors CRESS. Following the CSCR
structure a preliminary design for CRESS has been established and a portal
framework analy... | cs.HC | in a previous paper the cscr domain was defined here this is taken to the next stage where we consider the design of a particular collaborative research environment to support students and supervisors cress following the cscr structure a preliminary design for cress has been established and a portal framework analysis ... | [['in', 'a', 'previous', 'paper', 'the', 'cscr', 'domain', 'was', 'defined', 'here', 'this', 'is', 'taken', 'to', 'the', 'next', 'stage', 'where', 'we', 'consider', 'the', 'design', 'of', 'a', 'particular', 'collaborative', 'research', 'environment', 'to', 'support', 'students', 'and', 'supervisors', 'cress', 'followin... | [-0.09493569317132686, 0.010551958881092794, -0.093899121042341, 0.018824867657244657, -0.14414335906533807, -0.0952939184622444, 0.04512728072145502, 0.3993331887618159, -0.2128879279974199, -0.2863422997408744, 0.15682560786477884, -0.2249600784006444, -0.16712150779185872, 0.1561489129777659, -0.06558637800062019, 0... |
708.0878 | Double Boundary and Parity Doubling in Hadrons | A new mechanism for the parity doublers in hadrons is suggested.
| physics.gen-ph | a new mechanism for the parity doublers in hadrons is suggested | [['a', 'new', 'mechanism', 'for', 'the', 'parity', 'doublers', 'in', 'hadrons', 'is', 'suggested']] | [-0.15235924602232195, 0.3013758324086666, -0.16069257219152694, 0.18575482482132924, -0.10851553615859964, -0.17929236417297612, 0.07065032896670428, 0.2817476053129543, -0.20239720222624866, -0.23734582452611488, -0.06387104818978431, -0.21819799681278793, -0.044587206772782585, 0.08418457684191791, -0.01579945153472... |
708.0879 | Sub-Lorentzian Geometry on Anti-De Sitter Space | Sub-Riemannian Geometry is proved to play an important role in many
applications, e.g., Mathematical Physics and Control Theory. The simplest
example of sub-Riemannian structure is provided by the 3-D Heisenberg group.
Sub-Riemannian Geometry enjoys major differences from the Riemannian being a
generalisation of the ... | math.DG math-ph math.MP | subriemannian geometry is proved to play an important role in many applications eg mathematical physics and control theory the simplest example of subriemannian structure is provided by the 3d heisenberg group subriemannian geometry enjoys major differences from the riemannian being a generalisation of the latter at th... | [['subriemannian', 'geometry', 'is', 'proved', 'to', 'play', 'an', 'important', 'role', 'in', 'many', 'applications', 'eg', 'mathematical', 'physics', 'and', 'control', 'theory', 'the', 'simplest', 'example', 'of', 'subriemannian', 'structure', 'is', 'provided', 'by', 'the', '3d', 'heisenberg', 'group', 'subriemannian'... | [-0.12723749784581032, 0.07596568345014518, -0.07701876396105192, 0.14755269881876384, -0.15896820207256512, -0.136804920704463, -0.09311749032560694, 0.39548017581477346, -0.2644146336346615, -0.24430066983439236, 0.10393349652070626, -0.2881830569367086, -0.17854228485687818, 0.22040779241256667, -0.12605310448018742... |
708.088 | Eriksson's numbers game on certain edge-weighted three-node cyclic
graphs | The numbers game is a one-player game played on a finite simple graph with
certain ``amplitudes'' assigned to its edges and with an initial assignment of
real numbers to its nodes. The moves of the game successively transform the
numbers at the nodes using the amplitudes in a certain way. This game and its
interactio... | math.CO | the numbers game is a oneplayer game played on a finite simple graph with certain amplitudes assigned to its edges and with an initial assignment of real numbers to its nodes the moves of the game successively transform the numbers at the nodes using the amplitudes in a certain way this game and its interactions with c... | [['the', 'numbers', 'game', 'is', 'a', 'oneplayer', 'game', 'played', 'on', 'a', 'finite', 'simple', 'graph', 'with', 'certain', 'amplitudes', 'assigned', 'to', 'its', 'edges', 'and', 'with', 'an', 'initial', 'assignment', 'of', 'real', 'numbers', 'to', 'its', 'nodes', 'the', 'moves', 'of', 'the', 'game', 'successively... | [-0.2102940401008768, 0.14329474487215474, -0.12114236191486297, 0.06853654429906135, -0.08489051163732576, -0.14567355620976297, 0.0709070584472108, 0.3747209152139777, -0.2782480048029114, -0.3038110158158292, 0.09817779478751015, -0.26457729938326124, -0.1858972804872118, 0.12072589309390286, -0.1079757391347838, 0.... |
708.0881 | Direct measurement of a pure spin current by a polarized light beam | The photon helicity may be mapped to a spin-1/2, whereby we put forward an
intrinsic interaction between a polarized light beam as a ``photon spin
current'' and a pure spin current in a semiconductor, which arises from the
spin-orbit coupling in valence bands as a pure relativity effect without
involving the Rashba o... | cond-mat.mes-hall | the photon helicity may be mapped to a spin12 whereby we put forward an intrinsic interaction between a polarized light beam as a photon spin current and a pure spin current in a semiconductor which arises from the spinorbit coupling in valence bands as a pure relativity effect without involving the rashba or the dress... | [['the', 'photon', 'helicity', 'may', 'be', 'mapped', 'to', 'a', 'spin12', 'whereby', 'we', 'put', 'forward', 'an', 'intrinsic', 'interaction', 'between', 'a', 'polarized', 'light', 'beam', 'as', 'a', 'photon', 'spin', 'current', 'and', 'a', 'pure', 'spin', 'current', 'in', 'a', 'semiconductor', 'which', 'arises', 'fro... | [-0.1705768891298113, 0.22801463129856508, -0.055176188716011, 0.05258703304756869, -0.1145838160028166, -0.1682451721726659, 0.046712085137767916, 0.39382998827111687, -0.27531444935246985, -0.2822211385045716, -0.006391225584554783, -0.25712303354583205, -0.040684136029511216, 0.18646765001702736, 0.04577499377402536... |
708.0882 | Quantum Brownian Motion of a Macroscopic Object in a General Environment | For the purpose of understanding the quantum behavior such as quantum
decoherence, fluctuations, dissipation, entanglement and teleportation of a
mesoscopic or macroscopic object interacting with a general environment, we
derive here a set of exact master equations for the reduced density matrix of
$N$ interacting ha... | quant-ph | for the purpose of understanding the quantum behavior such as quantum decoherence fluctuations dissipation entanglement and teleportation of a mesoscopic or macroscopic object interacting with a general environment we derive here a set of exact master equations for the reduced density matrix of n interacting harmonic o... | [['for', 'the', 'purpose', 'of', 'understanding', 'the', 'quantum', 'behavior', 'such', 'as', 'quantum', 'decoherence', 'fluctuations', 'dissipation', 'entanglement', 'and', 'teleportation', 'of', 'a', 'mesoscopic', 'or', 'macroscopic', 'object', 'interacting', 'with', 'a', 'general', 'environment', 'we', 'derive', 'he... | [-0.12760115093470825, 0.20419906532257995, -0.10778624956587578, 0.05413404824225652, -0.020611368758991534, -0.16007600482176407, 0.009861918002760005, 0.31858096107022266, -0.27410770831979553, -0.2966788981346726, 0.055962269191732465, -0.24801237950359897, -0.12310637806870603, 0.20679572476020266, -0.042532760832... |
708.0883 | The complete LQG propagator: I. Difficulties with the Barrett-Crane
vertex | Some components of the graviton two-point function have been recently
computed in the context of loop quantum gravity, using the spinfoam
Barrett-Crane vertex. We complete the calculation of the remaining components.
We find that, under our assumptions, the Barrett-Crane vertex does not yield
the correct long distanc... | gr-qc | some components of the graviton twopoint function have been recently computed in the context of loop quantum gravity using the spinfoam barrettcrane vertex we complete the calculation of the remaining components we find that under our assumptions the barrettcrane vertex does not yield the correct long distance limit we... | [['some', 'components', 'of', 'the', 'graviton', 'twopoint', 'function', 'have', 'been', 'recently', 'computed', 'in', 'the', 'context', 'of', 'loop', 'quantum', 'gravity', 'using', 'the', 'spinfoam', 'barrettcrane', 'vertex', 'we', 'complete', 'the', 'calculation', 'of', 'the', 'remaining', 'components', 'we', 'find',... | [-0.11537610878697549, 0.09665681424108569, -0.1239230598539415, 0.11551533735855812, -0.11019726682717752, -0.09863276465447864, 0.024800197511789097, 0.3299662009107344, -0.25127180915024844, -0.24928405015221375, 0.051656904496308984, -0.24499230416058893, -0.2026476227593693, 0.11739206140992617, -0.097585609982335... |
708.0884 | A New Model of Agegraphic Dark Energy | In this note, we propose a new model of agegraphic dark energy based on the
K\'{a}rolyh\'{a}zy relation, where the time scale is chosen to be the conformal
time $\eta$ of the Friedmann-Robertson-Walker (FRW) universe. We find that in
the radiation-dominated epoch, the equation-of-state parameter of the new
agegraphic... | astro-ph gr-qc hep-th | in this note we propose a new model of agegraphic dark energy based on the karolyhazy relation where the time scale is chosen to be the conformal time eta of the friedmannrobertsonwalker frw universe we find that in the radiationdominated epoch the equationofstate parameter of the new agegraphic dark energy w_q13 where... | [['in', 'this', 'note', 'we', 'propose', 'a', 'new', 'model', 'of', 'agegraphic', 'dark', 'energy', 'based', 'on', 'the', 'karolyhazy', 'relation', 'where', 'the', 'time', 'scale', 'is', 'chosen', 'to', 'be', 'the', 'conformal', 'time', 'eta', 'of', 'the', 'friedmannrobertsonwalker', 'frw', 'universe', 'we', 'find', 't... | [-0.11688817158196267, 0.17096973551050215, -0.1702803627787424, 0.13151852591431928, -0.09319184743496892, -0.1609965815320732, -0.06996644425883213, 0.28471604153640906, -0.22942332019908473, -0.36307179807555295, -0.04798607955998197, -0.2401795278654083, -0.051508313837134605, 0.1012295084497468, 0.0091225004984767... |
708.0885 | Massive Lyman Break Galaxies at z~3 in the Spitzer Extragalactic First
Look Survey | We investigate the properties of 1088 Lyman Break Galaxies (LBGs) at z~3
selected from a ~2.63$ deg2 sub-region of the First Look Survey field using the
ground-based multi-color data and the Spitzer Space Telescope mid-infrared data
at 3--8 and 24 um. With the wide area and the broad wavelength coverage, we
sample a ... | astro-ph | we investigate the properties of 1088 lyman break galaxies lbgs at z3 selected from a 263 deg2 subregion of the first look survey field using the groundbased multicolor data and the spitzer space telescope midinfrared data at 38 and 24 um with the wide area and the broad wavelength coverage we sample a large number of ... | [['we', 'investigate', 'the', 'properties', 'of', '1088', 'lyman', 'break', 'galaxies', 'lbgs', 'at', 'z3', 'selected', 'from', 'a', '263', 'deg2', 'subregion', 'of', 'the', 'first', 'look', 'survey', 'field', 'using', 'the', 'groundbased', 'multicolor', 'data', 'and', 'the', 'spitzer', 'space', 'telescope', 'midinfrar... | [-0.03342772163049623, 0.08960986264175226, -0.022353026405477726, 0.11663638732930207, -0.06364997819813453, -0.02778545401583449, 0.08819275399857834, 0.44901586039101377, -0.042753571177785825, -0.3767670917856906, 0.04965112344048792, -0.3056188554056928, 0.02075730644224188, 0.1568362011022459, -0.0038844313511151... |
708.0886 | Deep u*- and g-band Imaging of the Spitzer Space Telescope First Look
Survey Field : Observations and Source Catalogs | We present deep u*-, and g-band images taken with the MegaCam on the 3.6 m
Canada-France-Hawaii Telescope (CFHT) to support the extragalactic component of
the Spitzer First Look Survey (hereafter, FLS). In this paper we outline the
observations, present source catalogs and characterize the completeness,
reliability, ... | astro-ph | we present deep u and gband images taken with the megacam on the 36 m canadafrancehawaii telescope cfht to support the extragalactic component of the spitzer first look survey hereafter fls in this paper we outline the observations present source catalogs and characterize the completeness reliability astrometric accura... | [['we', 'present', 'deep', 'u', 'and', 'gband', 'images', 'taken', 'with', 'the', 'megacam', 'on', 'the', '36', 'm', 'canadafrancehawaii', 'telescope', 'cfht', 'to', 'support', 'the', 'extragalactic', 'component', 'of', 'the', 'spitzer', 'first', 'look', 'survey', 'hereafter', 'fls', 'in', 'this', 'paper', 'we', 'outli... | [-0.03987935306899742, 0.015970367043817806, -0.05104396330085056, 0.08026228101544064, -0.08006851127116396, -0.04268338327501452, 0.08255087748611399, 0.4669315131943462, -0.14876121249849433, -0.41703259209742033, 0.12194011209780825, -0.35797576454274777, 0.02440218078653451, 0.2122811419485172, -0.0725805008927259... |
708.0887 | Volume-preserving mean curvature flow of revolution hypersurfaces in a
Rotationally Symmetric Space | In an ambient space with rotational symmetry around an axis (which include
the Hyperbolic and Euclidean spaces), we study the evolution under the
volume-preserving mean curvature flow of a revolution hypersurface M generated
by a graph over the axis of revolution and with boundary in two totally
geodesic hypersurface... | math.DG | in an ambient space with rotational symmetry around an axis which include the hyperbolic and euclidean spaces we study the evolution under the volumepreserving mean curvature flow of a revolution hypersurface m generated by a graph over the axis of revolution and with boundary in two totally geodesic hypersurfaces tgh ... | [['in', 'an', 'ambient', 'space', 'with', 'rotational', 'symmetry', 'around', 'an', 'axis', 'which', 'include', 'the', 'hyperbolic', 'and', 'euclidean', 'spaces', 'we', 'study', 'the', 'evolution', 'under', 'the', 'volumepreserving', 'mean', 'curvature', 'flow', 'of', 'a', 'revolution', 'hypersurface', 'm', 'generated'... | [-0.24442754122796223, 0.1393208711756176, -0.08994270857472561, 0.01291437854984236, -0.0723026517325228, -0.11330406367778778, -0.011086248498989, 0.38327580782290743, -0.27798562898839774, -0.21576861679357917, 0.14335050753250375, -0.2535610134210928, -0.052005559374504774, 0.1775921359826737, -0.09020490951431719,... |
708.0888 | An Action For Chan-Paton Factors | We show that Chan-Paton factors can be derived from a classical action
describing the dynamics of a new group-valued degree of freedom attached to the
boundary of an open bosonic string. We discuss the free and the interacting
string in the oriented and unoriented cases, as well as the coupling of the
string to an ex... | hep-th | we show that chanpaton factors can be derived from a classical action describing the dynamics of a new groupvalued degree of freedom attached to the boundary of an open bosonic string we discuss the free and the interacting string in the oriented and unoriented cases as well as the coupling of the string to an external... | [['we', 'show', 'that', 'chanpaton', 'factors', 'can', 'be', 'derived', 'from', 'a', 'classical', 'action', 'describing', 'the', 'dynamics', 'of', 'a', 'new', 'groupvalued', 'degree', 'of', 'freedom', 'attached', 'to', 'the', 'boundary', 'of', 'an', 'open', 'bosonic', 'string', 'we', 'discuss', 'the', 'free', 'and', 't... | [-0.15440976412289523, 0.18715285786090657, -0.068004220815827, 0.06754100662620852, -0.05207047006820865, -0.11794105531986464, 0.006630388444825781, 0.3166353992948478, -0.2878484523671707, -0.29636439523010544, 0.07173507670505029, -0.22793413855304773, -0.18563495056393245, 0.1561010468214976, -0.07340221506345904,... |
708.0889 | Improved Photometric Calibrations for Red Stars Observed with the SDSS
Photometric Telescope | We present a new set of photometric transformations for red stars observed
with the Sloan Digital Sky Survey (SDSS) 0.5-m Photometric Telescope (PT) and
the SDSS 2.5-m telescope at the Apache Point Observatory in New Mexico. Nightly
PT observations of US Naval Observatory standards are used to determine
extinction co... | astro-ph | we present a new set of photometric transformations for red stars observed with the sloan digital sky survey sdss 05m photometric telescope pt and the sdss 25m telescope at the apache point observatory in new mexico nightly pt observations of us naval observatory standards are used to determine extinction corrections a... | [['we', 'present', 'a', 'new', 'set', 'of', 'photometric', 'transformations', 'for', 'red', 'stars', 'observed', 'with', 'the', 'sloan', 'digital', 'sky', 'survey', 'sdss', '05m', 'photometric', 'telescope', 'pt', 'and', 'the', 'sdss', '25m', 'telescope', 'at', 'the', 'apache', 'point', 'observatory', 'in', 'new', 'mex... | [-0.026428718504405792, 0.07874946801082021, -0.09019513862027276, 0.07651493929687046, -0.184721525782539, -0.08010301064444525, 0.09297723841793354, 0.42278085987894765, -0.11867326927040854, -0.41457964952494347, 0.07480540918712053, -0.42357272204732704, -0.014635191623482011, 0.23471647942018126, -0.08824998911229... |
708.089 | Operational Semantics and Type Soundness of Quantum Programming Language
LanQ | We present an imperative quantum programming language LanQ which was designed
to support combination of quantum and classical programming and basic process
operations - process creation and interprocess communication. The language can
thus be used for implementing both classical and quantum algorithms and
protocols. ... | quant-ph | we present an imperative quantum programming language lanq which was designed to support combination of quantum and classical programming and basic process operations process creation and interprocess communication the language can thus be used for implementing both classical and quantum algorithms and protocols its sy... | [['we', 'present', 'an', 'imperative', 'quantum', 'programming', 'language', 'lanq', 'which', 'was', 'designed', 'to', 'support', 'combination', 'of', 'quantum', 'and', 'classical', 'programming', 'and', 'basic', 'process', 'operations', 'process', 'creation', 'and', 'interprocess', 'communication', 'the', 'language', ... | [-0.09603651612811286, 0.03510722240582951, -0.09783588622280574, 0.09776055776320448, -0.16371879117325583, -0.21323739726869193, 0.07412887779386476, 0.38654260289795855, -0.3262353613972664, -0.31602933287541285, 0.08195714023524023, -0.20294034517707027, -0.155174739232802, 0.21561383238022633, -0.11161822253005936... |
708.0891 | Operad of formal homogeneous spaces and Bernoulli numbers | It is shown that for any morphism, i: g --> h, of Lie algebras the vector
space underlying the Lie algebra h is canonically a g-homogeneous formal
manifold with the action of g being highly nonlinear and twisted by Bernoulli
numbers. This fact is obtained from the study of a 2-coloured operad of formal
homogeneous sp... | math.QA math.AG | it is shown that for any morphism i g h of lie algebras the vector space underlying the lie algebra h is canonically a ghomogeneous formal manifold with the action of g being highly nonlinear and twisted by bernoulli numbers this fact is obtained from the study of a 2coloured operad of formal homogeneous spaces and its... | [['it', 'is', 'shown', 'that', 'for', 'any', 'morphism', 'i', 'g', 'h', 'of', 'lie', 'algebras', 'the', 'vector', 'space', 'underlying', 'the', 'lie', 'algebra', 'h', 'is', 'canonically', 'a', 'ghomogeneous', 'formal', 'manifold', 'with', 'the', 'action', 'of', 'g', 'being', 'highly', 'nonlinear', 'and', 'twisted', 'by... | [-0.18894200249508555, 0.05768096868747047, -0.07463423259378898, 0.07351652418728918, -0.18013089263279522, -0.13973331428354696, -0.045126350665287605, 0.389552546137323, -0.40262197527502264, -0.22634344579918045, 0.1183580129451695, -0.18446858309741532, -0.16388851872068785, 0.17021593166781324, -0.143192940675431... |
708.0892 | Nonlinear screening and ballistic transport in a graphene p-n junction | We study the charge density distribution, the electric field profile, and the
resistance of an electrostatically created lateral p-n junction in graphene. We
show that the electric field at the interface of the electron and hole regions
is strongly enhanced due to limited screening capacity of Dirac quasiparticles.
A... | cond-mat.mes-hall cond-mat.mtrl-sci | we study the charge density distribution the electric field profile and the resistance of an electrostatically created lateral pn junction in graphene we show that the electric field at the interface of the electron and hole regions is strongly enhanced due to limited screening capacity of dirac quasiparticles accordin... | [['we', 'study', 'the', 'charge', 'density', 'distribution', 'the', 'electric', 'field', 'profile', 'and', 'the', 'resistance', 'of', 'an', 'electrostatically', 'created', 'lateral', 'pn', 'junction', 'in', 'graphene', 'we', 'show', 'that', 'the', 'electric', 'field', 'at', 'the', 'interface', 'of', 'the', 'electron', ... | [-0.21835189337952662, 0.14592441914319967, -0.026211256958481113, 0.016791913015136526, 0.006318882155090065, -0.12959964846466052, 0.07143148287373075, 0.37133495635905506, -0.21581816993716915, -0.3310364163086071, -0.04419998843933187, -0.30980861205923355, -0.1015322223597727, 0.17118575613377457, -0.0252571658752... |
708.0893 | Uniform Sobolev inequalities for manifolds evolving by Ricci flow | Let M be a compact n-dimensional manifold, $n\ge 2$, with metric g(t)
evolving by the Ricci flow $\partial g_{ij}/\partial t=-2R_{ij}$ in (0,T) for
some $T\in\Bbb{R}^+\cup\{\infty\}$ with $g(0)=g_0$. Let $\lambda_0(g_0)$ be the
first eigenvalue of the operator $-\Delta_{g_0} +\frac{R(g_0)}{4}$ with respect
to g_0. We... | math.DG | let m be a compact ndimensional manifold nge 2 with metric gt evolving by the ricci flow partial g_ijpartial t2r_ij in 0t for some tinbbbrcupinfty with g0g_0 let lambda_0g_0 be the first eigenvalue of the operator delta_g_0 fracrg_04 with respect to g_0 we extend a recent result of r ye and prove uniform logarithmic so... | [['let', 'm', 'be', 'a', 'compact', 'ndimensional', 'manifold', 'nge', '2', 'with', 'metric', 'gt', 'evolving', 'by', 'the', 'ricci', 'flow', 'partial', 'g_ijpartial', 't2r_ij', 'in', '0t', 'for', 'some', 'tinbbbrcupinfty', 'with', 'g0g_0', 'let', 'lambda_0g_0', 'be', 'the', 'first', 'eigenvalue', 'of', 'the', 'operato... | [-0.16531646834930988, 0.12220007305108764, -0.06765917599709197, 0.010816521387584883, -0.075886533482734, -0.2109890101392838, -0.08313462600397709, 0.3126605659854984, -0.2621878633143926, -0.19236526678074056, 0.16849931543739982, -0.31245294469173507, -0.05059142643820984, 0.16070922816200464, -0.09031081326644529... |
708.0894 | Density-Matrix Renormalization Group Study of Trapped Imbalanced Fermi
Condensates | The density-matrix renormalization group is employed to investigate a
harmonically-trapped imbalanced Fermi condensate based on a one-dimensional
attractive Hubbard model. The obtained density profile shows a flattened
population difference of spin-up and spin-down components at the center of the
trap, and exhibits p... | cond-mat.str-el | the densitymatrix renormalization group is employed to investigate a harmonicallytrapped imbalanced fermi condensate based on a onedimensional attractive hubbard model the obtained density profile shows a flattened population difference of spinup and spindown components at the center of the trap and exhibits phase sepa... | [['the', 'densitymatrix', 'renormalization', 'group', 'is', 'employed', 'to', 'investigate', 'a', 'harmonicallytrapped', 'imbalanced', 'fermi', 'condensate', 'based', 'on', 'a', 'onedimensional', 'attractive', 'hubbard', 'model', 'the', 'obtained', 'density', 'profile', 'shows', 'a', 'flattened', 'population', 'differe... | [-0.16507596559471116, 0.2128875655350539, -0.070463192130808, 0.05862882061760416, 0.006640196584586827, -0.14475641107924705, 0.09296642032777012, 0.3608019765255586, -0.22699200053795962, -0.2906898966515964, -0.016452595020451072, -0.3178821922684053, -0.03584709727064759, 0.1308912603461342, 0.06329309267325783, 0... |
708.0895 | Generation and detection of non-Abelian matrix Berry phases through
manipulation of electric confinement potential of a semiconductor quantum dot | A matrix Berry phase can be generated and detected by {\it all electric
means} in II-VI or III-V n-type semiconductor quantum dots by changing the
shape of the confinement potential. This follows from general symmetry
considerations in the presence of spin-orbit coupling terms. The resulting 2 x
2 matrix Berry phase ... | cond-mat.mes-hall quant-ph | a matrix berry phase can be generated and detected by it all electric means in iivi or iiiv ntype semiconductor quantum dots by changing the shape of the confinement potential this follows from general symmetry considerations in the presence of spinorbit coupling terms the resulting 2 x 2 matrix berry phase can be char... | [['a', 'matrix', 'berry', 'phase', 'can', 'be', 'generated', 'and', 'detected', 'by', 'it', 'all', 'electric', 'means', 'in', 'iivi', 'or', 'iiiv', 'ntype', 'semiconductor', 'quantum', 'dots', 'by', 'changing', 'the', 'shape', 'of', 'the', 'confinement', 'potential', 'this', 'follows', 'from', 'general', 'symmetry', 'c... | [-0.17843211860169753, 0.26039241850164463, -0.05254429845478047, 0.012865979567074894, -0.023894339032598178, -0.1502655358212492, 0.04644086509837176, 0.39920981897210533, -0.30672883395825257, -0.32789646891284396, 0.05496185021183919, -0.25627513926222245, -0.22013784654766574, 0.16444507080119697, -0.0399907534010... |
708.0896 | Long term dynamics of the splitting of a doubly quantized vortex in a
two-dimensional condensate | We study the nonlinear dynamics of the splitting of a doubly quantized vortex
in a trapped condensate. The dynamics is studied in detail by solving the
Gross-Pitaevskii equation. The main dynamical features are explained in terms
of a nonlinear three-level system. We find an analytical solution for the
characteristic... | cond-mat.other | we study the nonlinear dynamics of the splitting of a doubly quantized vortex in a trapped condensate the dynamics is studied in detail by solving the grosspitaevskii equation the main dynamical features are explained in terms of a nonlinear threelevel system we find an analytical solution for the characteristics of th... | [['we', 'study', 'the', 'nonlinear', 'dynamics', 'of', 'the', 'splitting', 'of', 'a', 'doubly', 'quantized', 'vortex', 'in', 'a', 'trapped', 'condensate', 'the', 'dynamics', 'is', 'studied', 'in', 'detail', 'by', 'solving', 'the', 'grosspitaevskii', 'equation', 'the', 'main', 'dynamical', 'features', 'are', 'explained'... | [-0.20372348117896102, 0.12927619747189328, -0.07901181021777841, 0.08179471397004393, 0.006908676623330488, -0.09387752530316205, -0.051091065104179954, 0.28002129426201827, -0.30232464362468037, -0.23447424427352168, 0.08210418182999718, -0.2687537291558919, -0.17207145059553833, 0.16950893281148627, 0.04427401323397... |
708.0897 | Brane World Inflation with Scalar and Tachyon Fields | We present inflationary models of the early universe in the braneworld
scenario considering both scalar field and tachyon field separately. The
technique of Chervon and Zhuravlev to obtain inflationary cosmological models
without restrictions on a scalar field potential is employed here. We note that
like scalar fiel... | hep-th | we present inflationary models of the early universe in the braneworld scenario considering both scalar field and tachyon field separately the technique of chervon and zhuravlev to obtain inflationary cosmological models without restrictions on a scalar field potential is employed here we note that like scalar field th... | [['we', 'present', 'inflationary', 'models', 'of', 'the', 'early', 'universe', 'in', 'the', 'braneworld', 'scenario', 'considering', 'both', 'scalar', 'field', 'and', 'tachyon', 'field', 'separately', 'the', 'technique', 'of', 'chervon', 'and', 'zhuravlev', 'to', 'obtain', 'inflationary', 'cosmological', 'models', 'wit... | [-0.15007174925944, 0.1679437474925643, -0.13161115564830733, 0.09791480096183684, -0.13563159469049424, -0.2160353620430422, -0.07403151380519073, 0.3389466049051599, -0.17167909012029045, -0.2847053767427018, 0.09073518779794604, -0.1780494053096494, -0.1402683627154482, 0.17102496543482534, -0.0018390688244580176, -... |
708.0898 | Optimisation of the 3-body dynamics applied to extra-solar planetary
systems | The body of work presented here revolves around the investigation of the
existence and nature of extra-solar planetary systems. The fitting of stellar
radial velocity time series data is attempted by constructing a model to
quantify the orbital properties of a star-planetary system. This is achieved
with the Planetar... | astro-ph | the body of work presented here revolves around the investigation of the existence and nature of extrasolar planetary systems the fitting of stellar radial velocity time series data is attempted by constructing a model to quantify the orbital properties of a starplanetary system this is achieved with the planetary orbi... | [['the', 'body', 'of', 'work', 'presented', 'here', 'revolves', 'around', 'the', 'investigation', 'of', 'the', 'existence', 'and', 'nature', 'of', 'extrasolar', 'planetary', 'systems', 'the', 'fitting', 'of', 'stellar', 'radial', 'velocity', 'time', 'series', 'data', 'is', 'attempted', 'by', 'constructing', 'a', 'model... | [-0.10369988771223386, 0.03704227314642594, -0.12504526496528948, 0.048127456677065084, -0.09122782149643172, -0.11235496889821661, 0.0044536732517978335, 0.31380501242529135, -0.2616903395210102, -0.32798980199640937, 0.11639731135376981, -0.2168098626777919, -0.12750307575091333, 0.2379027018408427, -0.02834687165401... |
708.0899 | Self-similar carpets over finite fields | Some linear dynamical systems over finite fields are studied and the
self-similar character of their development is proved. Connections with
aperiodic tilings, Delanoy numbers and other topics are also proved. The prime
fields F_p have a canonical presentation as sets of self-similar carpets. The
multiplicative inver... | math.NT math.CO | some linear dynamical systems over finite fields are studied and the selfsimilar character of their development is proved connections with aperiodic tilings delanoy numbers and other topics are also proved the prime fields f_p have a canonical presentation as sets of selfsimilar carpets the multiplicative inverse corre... | [['some', 'linear', 'dynamical', 'systems', 'over', 'finite', 'fields', 'are', 'studied', 'and', 'the', 'selfsimilar', 'character', 'of', 'their', 'development', 'is', 'proved', 'connections', 'with', 'aperiodic', 'tilings', 'delanoy', 'numbers', 'and', 'other', 'topics', 'are', 'also', 'proved', 'the', 'prime', 'field... | [-0.1980949120091585, 0.19807295047212392, -0.09335307233656447, 0.13972086960226685, -0.0913329382116596, -0.10743078246256725, -0.04813498972604672, 0.36168804838477325, -0.32588029278364655, -0.20430493819488524, 0.11465947749093175, -0.2848478729914253, -0.17113838845398277, 0.2925914094278899, -0.06103033271695798... |
708.09 | Spin-down of compact stars and energy release of a first-order phase
transition | The deconfinement phase transition from hadronic matter to quark matter can
continuously occur during spins down of neutron stars. It will lead to the
release of latent heat if the transition is the first-order one. We have
investigated the energy release of such deconfinement phase transition for
rotating hybrid sta... | astro-ph | the deconfinement phase transition from hadronic matter to quark matter can continuously occur during spins down of neutron stars it will lead to the release of latent heat if the transition is the firstorder one we have investigated the energy release of such deconfinement phase transition for rotating hybrid stars mo... | [['the', 'deconfinement', 'phase', 'transition', 'from', 'hadronic', 'matter', 'to', 'quark', 'matter', 'can', 'continuously', 'occur', 'during', 'spins', 'down', 'of', 'neutron', 'stars', 'it', 'will', 'lead', 'to', 'the', 'release', 'of', 'latent', 'heat', 'if', 'the', 'transition', 'is', 'the', 'firstorder', 'one', ... | [-0.0656292094527004, 0.32425319446929707, -0.09709716617852171, 0.0725469995618921, -0.1127826541522953, -0.04749106782462413, 0.1158220989664442, 0.34517893038481196, -0.23639804459063807, -0.3190394765479821, 0.049153280949272286, -0.2950096157179258, -0.002351582485520951, 0.10598751468905987, 0.07005125176483573, ... |
708.0901 | The Statistical Mechanics of Microscopic Long-Range Bulk-Boundary
Dependence in Black-Hole Physics and Holography | We argue in the following that the entropy-area law of black-hole physics and
the various holographic bounds are the consequences of the microscopic dynamics
of elementary degrees of freedom living on or near the Planck scale. We locate
them both in the interior and on the boundary of, for example, the black hole
wit... | hep-th gr-qc quant-ph | we argue in the following that the entropyarea law of blackhole physics and the various holographic bounds are the consequences of the microscopic dynamics of elementary degrees of freedom living on or near the planck scale we locate them both in the interior and on the boundary of for example the black hole with the s... | [['we', 'argue', 'in', 'the', 'following', 'that', 'the', 'entropyarea', 'law', 'of', 'blackhole', 'physics', 'and', 'the', 'various', 'holographic', 'bounds', 'are', 'the', 'consequences', 'of', 'the', 'microscopic', 'dynamics', 'of', 'elementary', 'degrees', 'of', 'freedom', 'living', 'on', 'or', 'near', 'the', 'plan... | [-0.14631546581736232, 0.16617401118573571, -0.10898787617238599, 0.10171462183549482, -0.06712978051057947, -0.0863195728471234, 0.045179196862754095, 0.2941482273574492, -0.23877469427126058, -0.31917399359839177, 0.07157472796061665, -0.2980951915607459, -0.14187248777343303, 0.18389285080695517, -0.0289497577274839... |
708.0902 | Quantum multiparty key distribution protocol without use of entanglement | We propose a quantum key distribution (QKD) protocol that enables three
parties agree at once on a shared common random bit string in presence of an
eavesdropper without use of entanglement. We prove its unconditional security
and analyze the key rate.
| quant-ph | we propose a quantum key distribution qkd protocol that enables three parties agree at once on a shared common random bit string in presence of an eavesdropper without use of entanglement we prove its unconditional security and analyze the key rate | [['we', 'propose', 'a', 'quantum', 'key', 'distribution', 'qkd', 'protocol', 'that', 'enables', 'three', 'parties', 'agree', 'at', 'once', 'on', 'a', 'shared', 'common', 'random', 'bit', 'string', 'in', 'presence', 'of', 'an', 'eavesdropper', 'without', 'use', 'of', 'entanglement', 'we', 'prove', 'its', 'unconditional'... | [-0.24691280467072274, 0.07399801911378745, -0.09971668202111997, 0.06787141457926936, 0.054122098380836044, -0.31831528683670046, 0.1376691195920746, 0.35933841219762475, -0.22617154116401586, -0.21620759063559333, 0.04798787601417067, -0.23660002841909483, -0.08276749506774472, 0.1748193327064921, -0.1812095456506784... |
708.0903 | Percolation of Vortices in the 3D Abelian Lattice Higgs Model | The compact Abelian Higgs model is simulated on a cubic lattice where it
possesses vortex lines and pointlike magnetic monopoles as topological defects.
The focus of this high-precision Monte Carlo study is on the vortex network,
which is investigated by means of percolation observables. In the region of the
phase di... | hep-lat | the compact abelian higgs model is simulated on a cubic lattice where it possesses vortex lines and pointlike magnetic monopoles as topological defects the focus of this highprecision monte carlo study is on the vortex network which is investigated by means of percolation observables in the region of the phase diagram ... | [['the', 'compact', 'abelian', 'higgs', 'model', 'is', 'simulated', 'on', 'a', 'cubic', 'lattice', 'where', 'it', 'possesses', 'vortex', 'lines', 'and', 'pointlike', 'magnetic', 'monopoles', 'as', 'topological', 'defects', 'the', 'focus', 'of', 'this', 'highprecision', 'monte', 'carlo', 'study', 'is', 'on', 'the', 'vor... | [-0.14680450841976853, 0.23619714330432687, -0.07412079887890673, 0.06691559075116979, -0.016479015406485355, -0.12827279086469123, 0.039966334334528404, 0.3584941051320787, -0.251284931026769, -0.22045493802280292, 0.10087503013052443, -0.29486375619122324, -0.13113538934089614, 0.11125426226401212, 0.0293345735550788... |
708.0904 | Improving HTc Josephson Junctions (HTc JJ) by annealing: the role of
vacancy-interstitial annihilation | We have studied the annealing effect in transport properties of High
temperature Josephson Junctions (HTc JJ) made by ion irradiation. Low
temperature annealing (80 degrees Celsius) increases the JJ transition
temperature (TJ) and the Ic.Rn product, where Ic is the critical current and Rn
the normal resistance. We fo... | cond-mat.supr-con | we have studied the annealing effect in transport properties of high temperature josephson junctions htc jj made by ion irradiation low temperature annealing 80 degrees celsius increases the jj transition temperature tj and the icrn product where ic is the critical current and rn the normal resistance we found that the... | [['we', 'have', 'studied', 'the', 'annealing', 'effect', 'in', 'transport', 'properties', 'of', 'high', 'temperature', 'josephson', 'junctions', 'htc', 'jj', 'made', 'by', 'ion', 'irradiation', 'low', 'temperature', 'annealing', '80', 'degrees', 'celsius', 'increases', 'the', 'jj', 'transition', 'temperature', 'tj', 'a... | [-0.14352640197047908, 0.2509028991048443, -0.04017059998868993, 0.03303623815120984, 0.03695036938667975, -0.1640139572237703, 0.07777495691882014, 0.40949252710649464, -0.2592342264498725, -0.30554300332159706, 0.06196915139702873, -0.2825266494970731, -0.0407946329055862, 0.17452206781529117, 0.019365956042563977, 0... |
708.0905 | Permutation Decoding and the Stopping Redundancy Hierarchy of Cyclic and
Extended Cyclic Codes | We introduce the notion of the stopping redundancy hierarchy of a linear
block code as a measure of the trade-off between performance and complexity of
iterative decoding for the binary erasure channel. We derive lower and upper
bounds for the stopping redundancy hierarchy via Lovasz's Local Lemma and
Bonferroni-type... | cs.IT math.IT | we introduce the notion of the stopping redundancy hierarchy of a linear block code as a measure of the tradeoff between performance and complexity of iterative decoding for the binary erasure channel we derive lower and upper bounds for the stopping redundancy hierarchy via lovaszs local lemma and bonferronitype inequ... | [['we', 'introduce', 'the', 'notion', 'of', 'the', 'stopping', 'redundancy', 'hierarchy', 'of', 'a', 'linear', 'block', 'code', 'as', 'a', 'measure', 'of', 'the', 'tradeoff', 'between', 'performance', 'and', 'complexity', 'of', 'iterative', 'decoding', 'for', 'the', 'binary', 'erasure', 'channel', 'we', 'derive', 'lowe... | [-0.19287167538699884, 0.05273682005156786, -0.09785758681478096, 0.08515142116751001, -0.07059682224278006, -0.2429914011463679, 0.1435424812655844, 0.3466805534541503, -0.3271817382070125, -0.29832739356279997, 0.11455658517152696, -0.22813028859632364, -0.16838225427285566, 0.16173341603448185, -0.1340085894872363, ... |
708.0906 | Spectroscopic analysis of finite size effects around a Kondo quantum dot | We consider a simple setup in which a small quantum dot is strongly connected
to a finite size box. This box can be either a metallic box or a finite size
quantum wire.The formation of the Kondo screening cloud in the box strongly
depends on the ratio between the Kondo temperature and the box level spacing.
By weakly... | cond-mat.mes-hall cond-mat.str-el | we consider a simple setup in which a small quantum dot is strongly connected to a finite size box this box can be either a metallic box or a finite size quantum wirethe formation of the kondo screening cloud in the box strongly depends on the ratio between the kondo temperature and the box level spacing by weakly conn... | [['we', 'consider', 'a', 'simple', 'setup', 'in', 'which', 'a', 'small', 'quantum', 'dot', 'is', 'strongly', 'connected', 'to', 'a', 'finite', 'size', 'box', 'this', 'box', 'can', 'be', 'either', 'a', 'metallic', 'box', 'or', 'a', 'finite', 'size', 'quantum', 'wirethe', 'formation', 'of', 'the', 'kondo', 'screening', '... | [-0.16403518238858808, 0.19007658489794094, -0.07053450611198232, 0.04856585540941783, -0.01941216594672629, -0.19912938531044694, 0.07951674953413507, 0.32854120429560896, -0.26393953088138783, -0.24215560319523016, 0.07949684184887225, -0.30827990195816496, -0.04012113093575906, 0.1706228164135523, -0.000701428845613... |
708.0907 | Permanents of Circulants: a Transfer Matrix Approach (Expanded Version) | Calculating the permanent of a (0,1) matrix is a #P-complete problem but
there are some classes of structured matrices for which the permanent is
calculable in polynomial time. The most well-known example is the fixed-jump
(0,1) circulant matrix which, using algebraic techniques, was shown by Minc to
satisfy a consta... | math.CO | calculating the permanent of a 01 matrix is a pcomplete problem but there are some classes of structured matrices for which the permanent is calculable in polynomial time the most wellknown example is the fixedjump 01 circulant matrix which using algebraic techniques was shown by minc to satisfy a constantcoefficient f... | [['calculating', 'the', 'permanent', 'of', 'a', '01', 'matrix', 'is', 'a', 'pcomplete', 'problem', 'but', 'there', 'are', 'some', 'classes', 'of', 'structured', 'matrices', 'for', 'which', 'the', 'permanent', 'is', 'calculable', 'in', 'polynomial', 'time', 'the', 'most', 'wellknown', 'example', 'is', 'the', 'fixedjump'... | [-0.11464575518957304, 0.11075222894699091, -0.061582614164699845, 0.09508354090287278, -0.10662527699621126, -0.1369821219954062, -0.001892989644541699, 0.3665317139802451, -0.32080036256136124, -0.29714622290277065, 0.13543331748395063, -0.24122866983201732, -0.20060935783863595, 0.19747002347108514, -0.0733087963622... |
708.0908 | Periodic-orbit determination of dynamical correlations in stochastic
processes | It is shown that large deviation statistical quantities of the discrete time,
finite state Markov process $P_{n+1}^{(j)}=\sum_{k=1}^NH_{jk}P_n^{(k)}$, where
P_n^{(j)} is the probability for the j-state at the time step n and H_{jk} is
the transition probability, completely coincides with those from the Kalman map
cor... | nlin.CD | it is shown that large deviation statistical quantities of the discrete time finite state markov process p_n1jsum_k1nh_jkp_nk where p_nj is the probability for the jstate at the time step n and h_jk is the transition probability completely coincides with those from the kalman map corresponding to the above markov proce... | [['it', 'is', 'shown', 'that', 'large', 'deviation', 'statistical', 'quantities', 'of', 'the', 'discrete', 'time', 'finite', 'state', 'markov', 'process', 'p_n1jsum_k1nh_jkp_nk', 'where', 'p_nj', 'is', 'the', 'probability', 'for', 'the', 'jstate', 'at', 'the', 'time', 'step', 'n', 'and', 'h_jk', 'is', 'the', 'transitio... | [-0.054943959576485214, 0.1781990326519008, -0.08522623032913543, 0.08462124996754028, 0.019482540956232697, -0.11882024890510365, 0.01770817638898734, 0.4042352386051789, -0.3289306595921516, -0.21605834866059012, 0.13196227487496798, -0.26083778361789883, -0.1194558436080115, 0.17479183823452332, -0.03497225728351623... |
708.0909 | On the Self-stabilization of Mobile Robots in Graphs | Self-stabilization is a versatile technique to withstand any transient fault
in a distributed system. Mobile robots (or agents) are one of the emerging
trends in distributed computing as they mimic autonomous biologic entities. The
contribution of this paper is threefold. First, we present a new model for
studying mo... | cs.DS cs.DC | selfstabilization is a versatile technique to withstand any transient fault in a distributed system mobile robots or agents are one of the emerging trends in distributed computing as they mimic autonomous biologic entities the contribution of this paper is threefold first we present a new model for studying mobile enti... | [['selfstabilization', 'is', 'a', 'versatile', 'technique', 'to', 'withstand', 'any', 'transient', 'fault', 'in', 'a', 'distributed', 'system', 'mobile', 'robots', 'or', 'agents', 'are', 'one', 'of', 'the', 'emerging', 'trends', 'in', 'distributed', 'computing', 'as', 'they', 'mimic', 'autonomous', 'biologic', 'entitie... | [-0.15830442769591638, 0.06019712614084091, -0.06264701147038648, 0.0367656279815995, -0.10275305026493213, -0.20225775244824112, 0.08334708225509607, 0.4106658911803103, -0.28535988767373754, -0.35123636522930995, 0.10636860437099382, -0.2553867640028252, -0.1803949501469454, 0.16872095892037403, -0.12640836517490012,... |
708.091 | Charge-Ordered State versus Dimer-Mott Insulator at Finite Temperatures | We theoretically investigate the competition between charge-ordered state and
Mott insulating state at finite temperatures in quarter-filled
quasi-one-dimensional electron systems, by studying dimerized extended Hubbard
chains with interchain Coulomb interactions. In order to take into account
one-dimensional fluctua... | cond-mat.str-el | we theoretically investigate the competition between chargeordered state and mott insulating state at finite temperatures in quarterfilled quasionedimensional electron systems by studying dimerized extended hubbard chains with interchain coulomb interactions in order to take into account onedimensional fluctuations pro... | [['we', 'theoretically', 'investigate', 'the', 'competition', 'between', 'chargeordered', 'state', 'and', 'mott', 'insulating', 'state', 'at', 'finite', 'temperatures', 'in', 'quarterfilled', 'quasionedimensional', 'electron', 'systems', 'by', 'studying', 'dimerized', 'extended', 'hubbard', 'chains', 'with', 'interchai... | [-0.1767672954038495, 0.26126323685706926, -0.024773972954911492, 0.11193409736844756, 0.002143176802478376, -0.17905159422329495, 0.12756510914436409, 0.3947870241211993, -0.26466013567211727, -0.20811101406191787, 0.003907355070779366, -0.32435207617735223, -0.14751824972530206, 0.07432060409337282, 0.100831395260978... |
708.0911 | Extra Dimensions and the Cosmological Constant Problem | This article reviews the arguments why extra dimensions provide a unique
opportunity for progress on the cosmological constant problem, and updates the
status of -- and the objections to (with replies) -- the specific proposal
using supersymmetric large extra dimensions (SLED).
| hep-ph | this article reviews the arguments why extra dimensions provide a unique opportunity for progress on the cosmological constant problem and updates the status of and the objections to with replies the specific proposal using supersymmetric large extra dimensions sled | [['this', 'article', 'reviews', 'the', 'arguments', 'why', 'extra', 'dimensions', 'provide', 'a', 'unique', 'opportunity', 'for', 'progress', 'on', 'the', 'cosmological', 'constant', 'problem', 'and', 'updates', 'the', 'status', 'of', 'and', 'the', 'objections', 'to', 'with', 'replies', 'the', 'specific', 'proposal', '... | [-0.0850021244214776, 0.07538764221737018, -0.032467954368211135, 0.07996416859364566, -0.16135072502761316, -0.21186441969938385, 0.09460364480335744, 0.3072961251705121, -0.15853427797078323, -0.3490240269173414, 0.14507499953749806, -0.28303278791598785, -0.1403740472996082, 0.08302899521703903, -0.08151288920392592... |
708.0912 | Evidence for dust accumulation just outside the orbit of Venus | To contribute to the knowledge of dynamics of interplanetary dust we are
searching for structures in the spatial distribution of interplanetary dust
near the orbit of Venus. To this end we study the radial gradient of zodiacal
light brightness, as observed by the zodiacal light photometer on board the
Helios space pr... | astro-ph | to contribute to the knowledge of dynamics of interplanetary dust we are searching for structures in the spatial distribution of interplanetary dust near the orbit of venus to this end we study the radial gradient of zodiacal light brightness as observed by the zodiacal light photometer on board the helios space probes... | [['to', 'contribute', 'to', 'the', 'knowledge', 'of', 'dynamics', 'of', 'interplanetary', 'dust', 'we', 'are', 'searching', 'for', 'structures', 'in', 'the', 'spatial', 'distribution', 'of', 'interplanetary', 'dust', 'near', 'the', 'orbit', 'of', 'venus', 'to', 'this', 'end', 'we', 'study', 'the', 'radial', 'gradient',... | [-0.07348908340082244, 0.14652249669838657, -0.11073819759332039, 0.07247034215746462, -0.03258125469284622, -0.026230086208342163, 0.030527937933242412, 0.3914917162024325, -0.2255834440028477, -0.3573678076635745, 0.08812275592629847, -0.29586347490829185, -0.07318108005071045, 0.23410589541343593, -0.121706423083107... |
708.0913 | An explicit estimate on multiplicity truncation in the second main
theorem for holomorphic curves encountering hypersurfaces in general position
in projective space | Yan and Chen proved a weak Cartan-type second main theorem for holomorphic
curves meeting hypersurfaces in projective space that included truncated
counting functions. Here we give an explicit estimate for the level of
truncation.
| math.CV | yan and chen proved a weak cartantype second main theorem for holomorphic curves meeting hypersurfaces in projective space that included truncated counting functions here we give an explicit estimate for the level of truncation | [['yan', 'and', 'chen', 'proved', 'a', 'weak', 'cartantype', 'second', 'main', 'theorem', 'for', 'holomorphic', 'curves', 'meeting', 'hypersurfaces', 'in', 'projective', 'space', 'that', 'included', 'truncated', 'counting', 'functions', 'here', 'we', 'give', 'an', 'explicit', 'estimate', 'for', 'the', 'level', 'of', 't... | [-0.17148187942802906, 0.00046316177202457124, -0.09043552948381095, 0.1291938631192726, -0.06235241172287394, -0.10943153499187354, 0.03797952948576387, 0.27640871262616096, -0.21076762528323076, -0.2058328775524655, 0.0717252492733464, -0.2120028378250187, -0.12197147470878382, 0.2358931178391418, -0.1834659771582878... |
708.0914 | Transverse Energy per Charged Particle and Freeze-Out Criteria in
Heavy-Ion Collisions | In relativistic nucleus-nucleus collisions the transverse energy per charged
particle, E_T/N_ch, increases rapidly with beam energy and remains
approximately constant at about 800 MeV for beam energies from SPS to RHIC. It
is shown that the hadron resonance gas model describes the energy dependence,
as well as the la... | hep-ph | in relativistic nucleusnucleus collisions the transverse energy per charged particle e_tn_ch increases rapidly with beam energy and remains approximately constant at about 800 mev for beam energies from sps to rhic it is shown that the hadron resonance gas model describes the energy dependence as well as the lack of ce... | [['in', 'relativistic', 'nucleusnucleus', 'collisions', 'the', 'transverse', 'energy', 'per', 'charged', 'particle', 'e_tn_ch', 'increases', 'rapidly', 'with', 'beam', 'energy', 'and', 'remains', 'approximately', 'constant', 'at', 'about', '800', 'mev', 'for', 'beam', 'energies', 'from', 'sps', 'to', 'rhic', 'it', 'is'... | [-0.032420048878217735, 0.28589851116865045, -0.11865646685732321, 0.16643359890602166, 0.012050809242888741, -0.13898127870116797, -0.07044677745499131, 0.3421653537855794, -0.21353266118482375, -0.37255958571202225, -0.09888804156960557, -0.3578622503620055, 0.14650953678776407, 0.1649342242599232, 0.0984513511001649... |
708.0915 | Two particles on a star graph I | We consider a two particle system on a star graph with $\delta$-function
interaction. A class of eigensolutions is described which are constructed from
appropriate one particle solutions, and hence are parametrised by two momenta.
These solutions include a family of solutions with discontinuous derivative on
the diag... | math-ph math.MP math.SP | we consider a two particle system on a star graph with deltafunction interaction a class of eigensolutions is described which are constructed from appropriate one particle solutions and hence are parametrised by two momenta these solutions include a family of solutions with discontinuous derivative on the diagonal | [['we', 'consider', 'a', 'two', 'particle', 'system', 'on', 'a', 'star', 'graph', 'with', 'deltafunction', 'interaction', 'a', 'class', 'of', 'eigensolutions', 'is', 'described', 'which', 'are', 'constructed', 'from', 'appropriate', 'one', 'particle', 'solutions', 'and', 'hence', 'are', 'parametrised', 'by', 'two', 'mo... | [-0.16244037084757013, 0.12950171285526865, -0.040748710850590564, 0.05664491603160871, -0.08378947585662629, -0.17573594196917527, -0.046709475801029104, 0.3454813096434512, -0.22237222239454377, -0.2755997303001424, 0.1252163179823138, -0.32307555780131764, -0.1064656816145524, 0.17841137702418294, 0.0213153911160027... |
708.0916 | Higgs Decay to Gluons at NNLO | We present an analytical calculation of the next-to-next-to-leading order
corrections to the partial decay width $H\to gg$ for a Higgs boson in the
intermediate mass range. We apply an asymptotic expansion for $M_H\ll 2M_t$ and
compute three terms in the expansion. The leading term confirms the results
present in the... | hep-ph | we present an analytical calculation of the nexttonexttoleading order corrections to the partial decay width hto gg for a higgs boson in the intermediate mass range we apply an asymptotic expansion for m_hll 2m_t and compute three terms in the expansion the leading term confirms the results present in the literature it... | [['we', 'present', 'an', 'analytical', 'calculation', 'of', 'the', 'nexttonexttoleading', 'order', 'corrections', 'to', 'the', 'partial', 'decay', 'width', 'hto', 'gg', 'for', 'a', 'higgs', 'boson', 'in', 'the', 'intermediate', 'mass', 'range', 'we', 'apply', 'an', 'asymptotic', 'expansion', 'for', 'm_hll', '2m_t', 'an... | [-0.08615435655916702, 0.1245506999064012, -0.06030147504696453, 0.1256442139671311, -0.043715515597300095, -0.04013466351369226, 0.023969936089336195, 0.3127845518756658, -0.1794588894488036, -0.27472021243407985, 0.039693007803924214, -0.3050713535313579, -0.026387897066094658, 0.17233923295597461, 0.0380577158331024... |
708.0917 | Test of pulse shape analysis using single Compton scattering events | Compton scattering is one of the dominant interaction processes in germanium
for photons with an energy of around two MeV. If a photon scatters only once
inside a germanium detector, the resulting event contains only one electron
which normally deposits its energy within a mm range. Such events are similar
to Ge-76 n... | nucl-ex | compton scattering is one of the dominant interaction processes in germanium for photons with an energy of around two mev if a photon scatters only once inside a germanium detector the resulting event contains only one electron which normally deposits its energy within a mm range such events are similar to ge76 neutrin... | [['compton', 'scattering', 'is', 'one', 'of', 'the', 'dominant', 'interaction', 'processes', 'in', 'germanium', 'for', 'photons', 'with', 'an', 'energy', 'of', 'around', 'two', 'mev', 'if', 'a', 'photon', 'scatters', 'only', 'once', 'inside', 'a', 'germanium', 'detector', 'the', 'resulting', 'event', 'contains', 'only'... | [-0.07071276082852095, 0.215519301770154, -0.035743210292765774, 0.093310693530152, 0.011735419022146261, -0.16165389232242441, 0.01756009655263351, 0.3675390680615163, -0.22472717276565274, -0.35528618392857664, 0.04073599660151391, -0.4234533593467228, 0.00984655299499555, 0.1970763020496578, 0.04677424180304764, 0.0... |
708.0918 | A spherical model with directional interactions: I. Static properties | We introduce a simple spherical model whose structural properties are similar
to the ones generated by models with directional interactions, by employing a
binary mixture of large and small hard spheres, with a square-well attraction
acting only between particles of different size. The small particles provide
the bon... | cond-mat.dis-nn cond-mat.soft | we introduce a simple spherical model whose structural properties are similar to the ones generated by models with directional interactions by employing a binary mixture of large and small hard spheres with a squarewell attraction acting only between particles of different size the small particles provide the bonds bet... | [['we', 'introduce', 'a', 'simple', 'spherical', 'model', 'whose', 'structural', 'properties', 'are', 'similar', 'to', 'the', 'ones', 'generated', 'by', 'models', 'with', 'directional', 'interactions', 'by', 'employing', 'a', 'binary', 'mixture', 'of', 'large', 'and', 'small', 'hard', 'spheres', 'with', 'a', 'squarewel... | [-0.1124533035983859, 0.2053006207315775, -0.07256094271406255, 0.0349659058015277, -0.0011679828767228173, -0.12683608486804587, 0.06235327885588049, 0.36099101761737984, -0.24635825542645762, -0.3241927068847872, 0.05053561413433272, -0.2818630595356808, -0.11427237491989217, 0.10255031707038142, 0.04714176814968596,... |
708.0919 | On the superfluidity of classical liquid in nanotubes | In 2001, the author proposed the ultra second quantization method. The ultra
second quantization of the Schr\"odinger equation, as well as its ordinary
second quantization, is a representation of the N-particle Schr\"odinger
equation, and this means that basically the ultra second quantization of the
equation is the ... | math-ph cond-mat.other math.MP | in 2001 the author proposed the ultra second quantization method the ultra second quantization of the schrodinger equation as well as its ordinary second quantization is a representation of the nparticle schrodinger equation and this means that basically the ultra second quantization of the equation is the same as the ... | [['in', '2001', 'the', 'author', 'proposed', 'the', 'ultra', 'second', 'quantization', 'method', 'the', 'ultra', 'second', 'quantization', 'of', 'the', 'schrodinger', 'equation', 'as', 'well', 'as', 'its', 'ordinary', 'second', 'quantization', 'is', 'a', 'representation', 'of', 'the', 'nparticle', 'schrodinger', 'equat... | [-0.14382993549875928, 0.17672042646077707, -0.09505318394420963, 0.03858955790105698, -0.07842890936023507, -0.12150755356139455, 0.025923443654870714, 0.2948910092665373, -0.24118401270090162, -0.2488576596369967, 0.07072556430801724, -0.30047837404632255, -0.1396903421363229, 0.13534893332000233, -0.0304265675735414... |
708.092 | Planar graphs and covers | Planar locally finite graphs which are almost vertex transitive are
discussed. If the graph is 3-connected and has at most one end then the group
of automorphisms is a planar discontinuous group and its structure is
well-known. A general result is obtained for such graphs where no restriction
is put on the number of ... | math.GR | planar locally finite graphs which are almost vertex transitive are discussed if the graph is 3connected and has at most one end then the group of automorphisms is a planar discontinuous group and its structure is wellknown a general result is obtained for such graphs where no restriction is put on the number of ends i... | [['planar', 'locally', 'finite', 'graphs', 'which', 'are', 'almost', 'vertex', 'transitive', 'are', 'discussed', 'if', 'the', 'graph', 'is', '3connected', 'and', 'has', 'at', 'most', 'one', 'end', 'then', 'the', 'group', 'of', 'automorphisms', 'is', 'a', 'planar', 'discontinuous', 'group', 'and', 'its', 'structure', 'i... | [-0.13655896058976447, 0.1580885384375086, -0.0828997700597968, 0.012810452429291148, -0.1479063009444092, -0.13910845876927233, -0.025064955723912014, 0.4326327364932705, -0.2858475613430818, -0.25362871248520663, 0.15859956013238324, -0.31378669444225976, -0.1426717309002345, 0.20564443206383878, -0.08917957646669922... |
708.0921 | Evidence for gap anisotropy in CaC6 from directional point-contact
spectroscopy | We present the first results of directional point-contact spectroscopy in
high quality CaC6 samples both along the ab plane and in the c-axis direction.
The superconducting order parameter \Delta(0), obtained by fitting the
Andreev-reflection (AR) conductance curves at temperatures down to 400 mK with
the single-band... | cond-mat.supr-con | we present the first results of directional pointcontact spectroscopy in high quality cac6 samples both along the ab plane and in the caxis direction the superconducting order parameter delta0 obtained by fitting the andreevreflection ar conductance curves at temperatures down to 400 mk with the singleband 3d blonderti... | [['we', 'present', 'the', 'first', 'results', 'of', 'directional', 'pointcontact', 'spectroscopy', 'in', 'high', 'quality', 'cac6', 'samples', 'both', 'along', 'the', 'ab', 'plane', 'and', 'in', 'the', 'caxis', 'direction', 'the', 'superconducting', 'order', 'parameter', 'delta0', 'obtained', 'by', 'fitting', 'the', 'a... | [-0.11498742051480804, 0.14416126061526788, -0.03346923387531812, -0.003932930141066511, 0.005973296366998208, -0.13129643013235182, 0.08067072001237345, 0.4734758445993066, -0.21387356636114419, -0.35539368968845036, -0.02656743630965745, -0.3743738543125801, -0.041160240667522885, 0.2200034329095312, 0.05566101315586... |
708.0922 | Star Formation in NGC 5194 (M51a). II. The Spatially-Resolved Star
Formation Law | We have studied the relationship between the star formation rate (SFR)
surface density and gas surface density in the spiral galaxy M51a (NGC 5194),
using multi-wavelength data obtained as part of the Spitzer Infrared Nearby
Galaxies Survey (SINGS). We introduce a new SFR index based on a linear
combination of H-alph... | astro-ph | we have studied the relationship between the star formation rate sfr surface density and gas surface density in the spiral galaxy m51a ngc 5194 using multiwavelength data obtained as part of the spitzer infrared nearby galaxies survey sings we introduce a new sfr index based on a linear combination of halpha emissionli... | [['we', 'have', 'studied', 'the', 'relationship', 'between', 'the', 'star', 'formation', 'rate', 'sfr', 'surface', 'density', 'and', 'gas', 'surface', 'density', 'in', 'the', 'spiral', 'galaxy', 'm51a', 'ngc', '5194', 'using', 'multiwavelength', 'data', 'obtained', 'as', 'part', 'of', 'the', 'spitzer', 'infrared', 'nea... | [-0.04098550224515465, 0.06789754652643631, -0.11528084422538026, 0.08994896465065111, -0.04672371199951873, -0.04554603729381791, 0.058771649944275375, 0.4385453587947566, -0.1698306632289266, -0.3667938081646857, 0.020992930307240056, -0.26010565775385525, -0.04382399299285054, 0.15641514588072017, -0.031222636924749... |
708.0923 | Spherical Nilpotent Orbits in Positive Characteristic | Let G be a connected reductive linear algebraic group defined over an
algebraically closed field of characteristic p. Assume that p is good for G. In
this note we classify all the spherical nilpotent G-orbits in the Lie algebra
of G. The classification is the same as in the characteristic zero case
obtained by D.I. P... | math.GR math.RA | let g be a connected reductive linear algebraic group defined over an algebraically closed field of characteristic p assume that p is good for g in this note we classify all the spherical nilpotent gorbits in the lie algebra of g the classification is the same as in the characteristic zero case obtained by di panyushev... | [['let', 'g', 'be', 'a', 'connected', 'reductive', 'linear', 'algebraic', 'group', 'defined', 'over', 'an', 'algebraically', 'closed', 'field', 'of', 'characteristic', 'p', 'assume', 'that', 'p', 'is', 'good', 'for', 'g', 'in', 'this', 'note', 'we', 'classify', 'all', 'the', 'spherical', 'nilpotent', 'gorbits', 'in', '... | [-0.21233347675568143, 0.0952752726330208, -0.0889537640533215, -0.015140083262447788, -0.11038150520843648, -0.1487664091400802, -0.06842096466137919, 0.3482365677523058, -0.32400495350647845, -0.21165461671473676, 0.05452699772336758, -0.22499264179469022, -0.08815019975178116, 0.21348837574640678, -0.114880525822437... |
708.0924 | Modified non-local-F(R) gravity as the key for the inflation and dark
energy | We consider FRW cosmology in non-local modified gravity. Its local
scalar-tensor formulation is developed. It is explicitly demonstrated that such
theory may lead to the unification of early-time inflation with late-time
cosmic acceleration. The quintessence or phantom era may emerge for specific
form of the action. ... | hep-th astro-ph gr-qc | we consider frw cosmology in nonlocal modified gravity its local scalartensor formulation is developed it is explicitly demonstrated that such theory may lead to the unification of earlytime inflation with latetime cosmic acceleration the quintessence or phantom era may emerge for specific form of the action the couple... | [['we', 'consider', 'frw', 'cosmology', 'in', 'nonlocal', 'modified', 'gravity', 'its', 'local', 'scalartensor', 'formulation', 'is', 'developed', 'it', 'is', 'explicitly', 'demonstrated', 'that', 'such', 'theory', 'may', 'lead', 'to', 'the', 'unification', 'of', 'earlytime', 'inflation', 'with', 'latetime', 'cosmic', ... | [-0.1408550676647932, 0.16267414301490554, -0.15106264649866483, 0.1625643587516, -0.14225437656904644, -0.19945913113247699, -0.15090548967829165, 0.3170561609410633, -0.23033220017663178, -0.30999924481297153, 0.039249356088335983, -0.20897315572708464, -0.13440968623110214, 0.15052331858374274, -0.05747448701936847,... |
708.0925 | Emergence of communities in weighted networks | Topology and weights are closely related in weighted complex networks and
this is reflected in their modular structure. We present a simple network model
where the weights are generated dynamically and they shape the developing
topology. By tuning a model parameter governing the importance of weights, the
resulting n... | physics.soc-ph | topology and weights are closely related in weighted complex networks and this is reflected in their modular structure we present a simple network model where the weights are generated dynamically and they shape the developing topology by tuning a model parameter governing the importance of weights the resulting networ... | [['topology', 'and', 'weights', 'are', 'closely', 'related', 'in', 'weighted', 'complex', 'networks', 'and', 'this', 'is', 'reflected', 'in', 'their', 'modular', 'structure', 'we', 'present', 'a', 'simple', 'network', 'model', 'where', 'the', 'weights', 'are', 'generated', 'dynamically', 'and', 'they', 'shape', 'the', ... | [-0.14316708434564182, 0.13393674896230015, -0.0426987974547396, 0.07633089436552463, -0.0939921394456178, -0.1352842426043562, 0.02634540550971929, 0.4236825234137284, -0.3759528847817236, -0.2804262193803413, 0.0682122124484382, -0.24708778546072352, -0.2875818269781004, 0.1485120758611279, -0.03485802601640805, 0.01... |
708.0926 | Dynamical Lower Bounds for 1D Dirac Operators | Quantum dynamical lower bounds for continuous and discrete one-dimensional
Dirac operators are established in terms of transfer matrices. Then such
results are applied to various models, including the Bernoulli-Dirac one and,
in contrast to the discrete case, critical energies are also found for the
continuous Dirac ... | math-ph math.FA math.MP | quantum dynamical lower bounds for continuous and discrete onedimensional dirac operators are established in terms of transfer matrices then such results are applied to various models including the bernoullidirac one and in contrast to the discrete case critical energies are also found for the continuous dirac case wit... | [['quantum', 'dynamical', 'lower', 'bounds', 'for', 'continuous', 'and', 'discrete', 'onedimensional', 'dirac', 'operators', 'are', 'established', 'in', 'terms', 'of', 'transfer', 'matrices', 'then', 'such', 'results', 'are', 'applied', 'to', 'various', 'models', 'including', 'the', 'bernoullidirac', 'one', 'and', 'in'... | [-0.05734750843720929, 0.19105145071956273, 0.011079050600528717, 0.11402672755398921, -0.017620911902500962, -0.15918961489734676, -0.010082284601557315, 0.364309553437087, -0.23612888302768067, -0.2745315947151762, 0.12820482084394566, -0.30034685621456225, -0.15611810685724628, 0.262533849238285, 0.00472013489818390... |
708.0927 | Modeling Visual Information Processing in Brain: A Computer Vision Point
of View and Approach | We live in the Information Age, and information has become a critically
important component of our life. The success of the Internet made huge amounts
of it easily available and accessible to everyone. To keep the flow of this
information manageable, means for its faultless circulation and effective
handling have bec... | cs.AI cs.CV | we live in the information age and information has become a critically important component of our life the success of the internet made huge amounts of it easily available and accessible to everyone to keep the flow of this information manageable means for its faultless circulation and effective handling have become ur... | [['we', 'live', 'in', 'the', 'information', 'age', 'and', 'information', 'has', 'become', 'a', 'critically', 'important', 'component', 'of', 'our', 'life', 'the', 'success', 'of', 'the', 'internet', 'made', 'huge', 'amounts', 'of', 'it', 'easily', 'available', 'and', 'accessible', 'to', 'everyone', 'to', 'keep', 'the',... | [-0.06241647209071517, 0.07533598325595513, -0.11583304247675251, 0.10575394247327259, -0.17421317550895818, -0.17218544769948765, 0.03144941490956707, 0.37498717969607803, -0.2908885425086416, -0.3486547308570858, 0.12109100471531037, -0.27326851382629197, -0.18349456974184744, 0.17161522168418236, -0.1906086381719406... |
708.0928 | Dual Bosonic Thermal Green Function and Fermion Correlators of the
Massive Thirring Model at a Finite Temperature | The Euclidian thermal Green function of the two-dimensional (2D) free
massless scalar field in coordinate space is written as the real part of a
complex analytic function of a variable that conformally maps the infinite
strip $-\infty<x<\infty$ ($0<\tau<\beta$) of the $z=x+i\tau$ ($\tau$: imaginary
time) plane into t... | hep-th | the euclidian thermal green function of the twodimensional 2d free massless scalar field in coordinate space is written as the real part of a complex analytic function of a variable that conformally maps the infinite strip inftyxinfty 0taubeta of the zxitau tau imaginary time plane into the upperhalfplane using this fa... | [['the', 'euclidian', 'thermal', 'green', 'function', 'of', 'the', 'twodimensional', '2d', 'free', 'massless', 'scalar', 'field', 'in', 'coordinate', 'space', 'is', 'written', 'as', 'the', 'real', 'part', 'of', 'a', 'complex', 'analytic', 'function', 'of', 'a', 'variable', 'that', 'conformally', 'maps', 'the', 'infinit... | [-0.1489743243485767, 0.09924051636714164, -0.10840480636882906, 0.08255837516238292, -0.07835786897339858, -0.050964194970826306, -0.01875676156487316, 0.328325519086017, -0.23763006458951472, -0.19017894546656558, 0.10490333363001507, -0.24481981105539793, -0.17788540904681818, 0.16452451939646076, 0.0621277804214817... |
708.0929 | Relativity without tears | Special relativity is no longer a new revolutionary theory but a firmly
established cornerstone of modern physics. The teaching of special relativity,
however, still follows its presentation as it unfolded historically, trying to
convince the audience of this teaching that Newtonian physics is natural but
incorrect a... | physics.ed-ph hep-th physics.gen-ph | special relativity is no longer a new revolutionary theory but a firmly established cornerstone of modern physics the teaching of special relativity however still follows its presentation as it unfolded historically trying to convince the audience of this teaching that newtonian physics is natural but incorrect and spe... | [['special', 'relativity', 'is', 'no', 'longer', 'a', 'new', 'revolutionary', 'theory', 'but', 'a', 'firmly', 'established', 'cornerstone', 'of', 'modern', 'physics', 'the', 'teaching', 'of', 'special', 'relativity', 'however', 'still', 'follows', 'its', 'presentation', 'as', 'it', 'unfolded', 'historically', 'trying',... | [-0.07248836397118266, 0.07524091735127338, -0.1389290095746307, 0.18293910869115573, -0.18938691304966568, -0.20549395125764872, 0.02820263365415045, 0.27524198880494244, -0.2285988350227971, -0.31386937804880644, 0.06860197095140334, -0.1968291376101514, -0.1662077200411248, 0.20607805357975584, -0.16706867845759035,... |
708.093 | Violation of Porod law in a freely cooling granular gas in one dimension | We study a model of freely cooling inelastic granular gas in one dimension,
with a restitution coefficient which approaches the elastic limit below a
relative velocity scale v. While at early times (t << 1/v) the gas behaves as a
completely inelastic sticky gas conforming to predictions of earlier studies,
at late ti... | cond-mat.stat-mech | we study a model of freely cooling inelastic granular gas in one dimension with a restitution coefficient which approaches the elastic limit below a relative velocity scale v while at early times t 1v the gas behaves as a completely inelastic sticky gas conforming to predictions of earlier studies at late times t 1v it... | [['we', 'study', 'a', 'model', 'of', 'freely', 'cooling', 'inelastic', 'granular', 'gas', 'in', 'one', 'dimension', 'with', 'a', 'restitution', 'coefficient', 'which', 'approaches', 'the', 'elastic', 'limit', 'below', 'a', 'relative', 'velocity', 'scale', 'v', 'while', 'at', 'early', 'times', 't', '1v', 'the', 'gas', '... | [-0.10908967354121611, 0.17097755308589144, -0.11610548033819797, 0.08324036538913732, -0.004411849827782912, -0.14663422619035282, 0.057979135098689384, 0.34136336236811804, -0.30094772615676163, -0.25012982623893343, 0.01724651833651374, -0.33032819489372595, -0.06833486616227577, 0.08034925075525148, 0.0879167764117... |
708.0931 | Spectroscopy of the a^3\Sigma_u^+ state and the coupling to the
X^1\Sigma_g^+ state of K_2 | We report on high resolution Fourier-transform spectroscopy of fluorescence
to the a^3\Sigma_u^+ state excited by two-photon or two-step excitation from
the X^1\Sigma_g^+ state to the 2^3\Pi_g state in the molecule K_2. These
spectroscopic data are combined with recent results of Feshbach resonances and
two-color pho... | physics.atom-ph | we report on high resolution fouriertransform spectroscopy of fluorescence to the a3sigma_u state excited by twophoton or twostep excitation from the x1sigma_g state to the 23pi_g state in the molecule k_2 these spectroscopic data are combined with recent results of feshbach resonances and twocolor photoassociation spe... | [['we', 'report', 'on', 'high', 'resolution', 'fouriertransform', 'spectroscopy', 'of', 'fluorescence', 'to', 'the', 'a3sigma_u', 'state', 'excited', 'by', 'twophoton', 'or', 'twostep', 'excitation', 'from', 'the', 'x1sigma_g', 'state', 'to', 'the', '23pi_g', 'state', 'in', 'the', 'molecule', 'k_2', 'these', 'spectrosc... | [-0.07320612084453668, 0.15162159279140272, -0.04515785264320732, 0.009774289519821362, 0.056498929456906107, -0.13332431365894834, 0.11729560216237617, 0.4122837288532315, -0.2071194945970868, -0.3044368757677503, 0.0045280142515004285, -0.3223325611069435, 0.058512416318043825, 0.1429359413308614, 0.06724129883360451... |
708.0932 | Inflating Fat Bubbles in Clusters of Galaxies by Precessing Massive Slow
Jets | We conduct hydrodynamical numerical simulations and find that precessing
massive slow jets can inflate fat bubbles, i.e., more or less spherical
bubbles, that are attached to the center of clusters of galaxies. To inflate a
fat bubble the jet should precess fast. The precessing angle $\theta$ should be
large, or chan... | astro-ph | we conduct hydrodynamical numerical simulations and find that precessing massive slow jets can inflate fat bubbles ie more or less spherical bubbles that are attached to the center of clusters of galaxies to inflate a fat bubble the jet should precess fast the precessing angle theta should be large or change over a lar... | [['we', 'conduct', 'hydrodynamical', 'numerical', 'simulations', 'and', 'find', 'that', 'precessing', 'massive', 'slow', 'jets', 'can', 'inflate', 'fat', 'bubbles', 'ie', 'more', 'or', 'less', 'spherical', 'bubbles', 'that', 'are', 'attached', 'to', 'the', 'center', 'of', 'clusters', 'of', 'galaxies', 'to', 'inflate', ... | [-0.15168938902134857, 0.2003564403254401, -0.03601993512459973, 0.07606506318480558, -0.10269572145455046, -0.0996442042409017, 0.0021988116556859033, 0.41319485411139917, -0.21928419129359594, -0.3040862931513492, 0.08777902127720738, -0.28399197279510124, 0.031054233884967773, 0.23264677792408126, -0.026371825528460... |
708.0933 | How not to discard half of the cases in QKD | All known QKD protocols require the parties to discard the results when they
have chosen differen bases. In this paper we show that it is not necessary. We
give examples of QKD protocols that are as safe as standard ones but do not
involve the discarding the results when the bases are different or even that do
not re... | quant-ph | all known qkd protocols require the parties to discard the results when they have chosen differen bases in this paper we show that it is not necessary we give examples of qkd protocols that are as safe as standard ones but do not involve the discarding the results when the bases are different or even that do not requir... | [['all', 'known', 'qkd', 'protocols', 'require', 'the', 'parties', 'to', 'discard', 'the', 'results', 'when', 'they', 'have', 'chosen', 'differen', 'bases', 'in', 'this', 'paper', 'we', 'show', 'that', 'it', 'is', 'not', 'necessary', 'we', 'give', 'examples', 'of', 'qkd', 'protocols', 'that', 'are', 'as', 'safe', 'as',... | [-0.11683278416499629, 0.11040719673370145, -0.12034547489020042, 0.11640214358132132, -0.09732919069938362, -0.24054281313770584, 0.06055063354974014, 0.4095016668018486, -0.23145168463919877, -0.2675534176690105, 0.13413538797405117, -0.23932686311724996, -0.16750543208036106, 0.22779751454280422, -0.1455643101029896... |
708.0934 | Generalized Cherednik-Macdonald identities | We derive generalizations of the Cherednik-Macdonald constant term identities
associated to root systems which depend, besides on the usual multiplicity
function, symmetrically on two quasi-periods. They are natural analogues of the
Cherednik-Macdonald constant term q-identities in which the deformation
parameter q i... | math.QA math.CA | we derive generalizations of the cherednikmacdonald constant term identities associated to root systems which depend besides on the usual multiplicity function symmetrically on two quasiperiods they are natural analogues of the cherednikmacdonald constant term qidentities in which the deformation parameter q is allowed... | [['we', 'derive', 'generalizations', 'of', 'the', 'cherednikmacdonald', 'constant', 'term', 'identities', 'associated', 'to', 'root', 'systems', 'which', 'depend', 'besides', 'on', 'the', 'usual', 'multiplicity', 'function', 'symmetrically', 'on', 'two', 'quasiperiods', 'they', 'are', 'natural', 'analogues', 'of', 'the... | [-0.1708693753601983, 0.13309300100430846, -0.06018154927975653, 0.07030401745500664, -0.15769549870863556, -0.18761273756623267, -0.023068878427147867, 0.27192659545689823, -0.33866569091565907, -0.2555164992343634, 0.10552175385101388, -0.27020791730533045, -0.18019040212035178, 0.1706935316355278, -0.099172598694761... |
708.0935 | Thermodynamical quantities for overlap fermions with chemical potential | Recently a formulation of overlap fermions at finite density based on an
analytic continuation of the sign function was proposed. We study this proposal
by analyzing the energy and number densities for free fermions as a function of
the chemical potential and the temperature. Our results show that overlap
fermions wi... | hep-lat | recently a formulation of overlap fermions at finite density based on an analytic continuation of the sign function was proposed we study this proposal by analyzing the energy and number densities for free fermions as a function of the chemical potential and the temperature our results show that overlap fermions with c... | [['recently', 'a', 'formulation', 'of', 'overlap', 'fermions', 'at', 'finite', 'density', 'based', 'on', 'an', 'analytic', 'continuation', 'of', 'the', 'sign', 'function', 'was', 'proposed', 'we', 'study', 'this', 'proposal', 'by', 'analyzing', 'the', 'energy', 'and', 'number', 'densities', 'for', 'free', 'fermions', '... | [-0.09429174638353288, 0.12716563864208486, -0.1357992082601413, 0.041326361217458425, -0.030301606406768163, -0.06089524080355962, 0.08654584862136593, 0.3427747568115592, -0.165282640994216, -0.33600533930584786, 0.015153137524612248, -0.2612476160749793, -0.15903418435094258, 0.13441102708068986, 0.02749293946350614... |
708.0936 | Couplings of the Rho Meson in a Holographic dual of QCD with Regge
Trajectories | The couplings $g_{\rho HH}$ of the $\rho$ meson with any hadron H are
calculated in a holographic dual of QCD where the Regge trajectories for mesons
are manifest. The resulting couplings grow linearly with the exciting number of
H, thus are far from universal. A simple argument has been given for this
behavior based... | hep-ph | the couplings g_rho hh of the rho meson with any hadron h are calculated in a holographic dual of qcd where the regge trajectories for mesons are manifest the resulting couplings grow linearly with the exciting number of h thus are far from universal a simple argument has been given for this behavior based on quasiclas... | [['the', 'couplings', 'g_rho', 'hh', 'of', 'the', 'rho', 'meson', 'with', 'any', 'hadron', 'h', 'are', 'calculated', 'in', 'a', 'holographic', 'dual', 'of', 'qcd', 'where', 'the', 'regge', 'trajectories', 'for', 'mesons', 'are', 'manifest', 'the', 'resulting', 'couplings', 'grow', 'linearly', 'with', 'the', 'exciting',... | [-0.11123308792656703, 0.25474722937365873, -0.13363586433429486, 0.087765611966958, -0.07084864097741171, -0.14918838483917948, 0.01764051477498502, 0.3264464386504331, -0.18908223666572313, -0.20974779422830442, 0.014088924831824659, -0.30049550526594515, -0.06799676993915396, 0.12019369468803136, 0.0725054271592886,... |
708.0937 | U-boson and the HyperCP exotic events | We show that the very light spin-1 gauge U-boson of the extra $U(1)'$ gauge
model in the framework of the supersymmetric standard model extension can be a
good candidate of the new light particle suggested by the HyperCP experiment.
We demonstrate that the flavor changing neutral currents (FCNCs) for the
HyperCP even... | hep-ph hep-ex | we show that the very light spin1 gauge uboson of the extra u1 gauge model in the framework of the supersymmetric standard model extension can be a good candidate of the new light particle suggested by the hypercp experiment we demonstrate that the flavor changing neutral currents fcncs for the hypercp events in the de... | [['we', 'show', 'that', 'the', 'very', 'light', 'spin1', 'gauge', 'uboson', 'of', 'the', 'extra', 'u1', 'gauge', 'model', 'in', 'the', 'framework', 'of', 'the', 'supersymmetric', 'standard', 'model', 'extension', 'can', 'be', 'a', 'good', 'candidate', 'of', 'the', 'new', 'light', 'particle', 'suggested', 'by', 'the', '... | [-0.10127354600195977, 0.27177635735521716, -0.05502741814406047, 0.14358390753524022, -0.06805218265438122, -0.17026273859664798, 0.04420576114636839, 0.3198955954706415, -0.2062662629483281, -0.2892623633915783, 0.01261771257127906, -0.27775794914956636, -0.10813269888526424, 0.13592399857238147, 0.04364024394469217,... |
708.0938 | Cavity cooling of translational and ro-vibrational motion of molecules:
ab initio-based simulations for OH and NO | We present detailed calculations at the basis of our recent proposal for
simultaneous cooling the rotational, vibrational and external molecular degrees
of freedom. In this method, the molecular rovibronic states are coupled by an
intense laser and an optical cavity via coherent Raman processes enhanced by
the strong... | quant-ph | we present detailed calculations at the basis of our recent proposal for simultaneous cooling the rotational vibrational and external molecular degrees of freedom in this method the molecular rovibronic states are coupled by an intense laser and an optical cavity via coherent raman processes enhanced by the strong coup... | [['we', 'present', 'detailed', 'calculations', 'at', 'the', 'basis', 'of', 'our', 'recent', 'proposal', 'for', 'simultaneous', 'cooling', 'the', 'rotational', 'vibrational', 'and', 'external', 'molecular', 'degrees', 'of', 'freedom', 'in', 'this', 'method', 'the', 'molecular', 'rovibronic', 'states', 'are', 'coupled', ... | [-0.13493973014467373, 0.1533772064000463, -0.03489450589995983, -0.030512272171123424, 0.008153264884026797, -0.08680722869675213, 0.0874401447495703, 0.4262701990499305, -0.24289671460363438, -0.27520036067419906, 0.038912212746823584, -0.23201450167935553, -0.08022130867163461, 0.18468617021515057, 0.047113289640141... |
708.0939 | Spin and charge orders and their hole-doping dependence in single
layered cobaltate La2-xCaxCoO4(0.3<x<0.8) | Neutron scattering experiments were performed on single crystals of layered
cobalt-oxides La2-xCaxCoO4 (LCCO) to characterize the charge and spin orders in
a wide hole-doping range of 0.3<x<0.8. For a commensurate value of x=0.5 in
(H,0,L) plane, two types of superlattice reflections concomitantly appear at
low tempe... | cond-mat.str-el | neutron scattering experiments were performed on single crystals of layered cobaltoxides la2xcaxcoo4 lcco to characterize the charge and spin orders in a wide holedoping range of 03x08 for a commensurate value of x05 in h0l plane two types of superlattice reflections concomitantly appear at low temperature one correspo... | [['neutron', 'scattering', 'experiments', 'were', 'performed', 'on', 'single', 'crystals', 'of', 'layered', 'cobaltoxides', 'la2xcaxcoo4', 'lcco', 'to', 'characterize', 'the', 'charge', 'and', 'spin', 'orders', 'in', 'a', 'wide', 'holedoping', 'range', 'of', '03x08', 'for', 'a', 'commensurate', 'value', 'of', 'x05', 'i... | [-0.19495316007588473, 0.25424288604828893, 0.006630389767491983, 0.04399643965945062, -0.012487924979844441, -0.10035034391718606, 0.06445106740187233, 0.42384752705693246, -0.27647769873599626, -0.30503880500586494, 0.0225029606022872, -0.33969063217906903, -0.07111293798370752, 0.15424004021430543, 0.075168675647970... |
708.094 | Charged-Higgs Collider Signals with or without Flavor | A charged Higgs boson is a clear signal for an extended Higgs sector, as for
example predicted by supersymmetry. Squark mixing can significantly change the
pattern of charged-Higgs production and most notably circumvent the chiral
suppression for single Higgs production. We evaluate the LHC discovery
potential in the... | hep-ph | a charged higgs boson is a clear signal for an extended higgs sector as for example predicted by supersymmetry squark mixing can significantly change the pattern of chargedhiggs production and most notably circumvent the chiral suppression for single higgs production we evaluate the lhc discovery potential in the light... | [['a', 'charged', 'higgs', 'boson', 'is', 'a', 'clear', 'signal', 'for', 'an', 'extended', 'higgs', 'sector', 'as', 'for', 'example', 'predicted', 'by', 'supersymmetry', 'squark', 'mixing', 'can', 'significantly', 'change', 'the', 'pattern', 'of', 'chargedhiggs', 'production', 'and', 'most', 'notably', 'circumvent', 't... | [-0.0994798512198031, 0.29141895993877065, -0.03499317298798511, 0.20069896440351537, -0.1102329804833668, -0.21850017381366343, 0.09744039956713095, 0.31126512920406335, -0.20857243432619726, -0.29121735446775954, 0.04306850176556812, -0.2650543610720585, -0.004250562531524338, 0.1242298333386619, 0.04824387821524093,... |
708.0941 | An entire function with simply and multiply connected wandering domains | We modify a construction of Kisaka and Shishikura to show that there exists
an entire function which has both a simply connected and a multiply connected
wandering domain. Moreover, these domains are contained in the set of fast
escaping points.
| math.CV math.DS | we modify a construction of kisaka and shishikura to show that there exists an entire function which has both a simply connected and a multiply connected wandering domain moreover these domains are contained in the set of fast escaping points | [['we', 'modify', 'a', 'construction', 'of', 'kisaka', 'and', 'shishikura', 'to', 'show', 'that', 'there', 'exists', 'an', 'entire', 'function', 'which', 'has', 'both', 'a', 'simply', 'connected', 'and', 'a', 'multiply', 'connected', 'wandering', 'domain', 'moreover', 'these', 'domains', 'are', 'contained', 'in', 'the'... | [-0.1780268907164916, 0.11223664916551804, -0.059511616079805374, 0.011628390934604865, -0.09027703072971259, -0.07380657512933397, 0.07757310396155868, 0.39814654030860996, -0.2896968296323067, -0.1890398519925582, 0.12376354485212897, -0.28164765764123356, -0.16822329822641152, 0.24574335811373132, -0.060421615158422... |
708.0942 | Evolution of supermassive black holes | The cosmological evolution of supermassive black holes (SMBHs) seems to be
intimately linked to their host galaxies. Active galactic nuclei (AGN) can be
probed by deep X-ray surveys. We review results from large X-ray selected
samples including first results from the XMM-Newton COSMOS survey. A new
picture arises fro... | astro-ph | the cosmological evolution of supermassive black holes smbhs seems to be intimately linked to their host galaxies active galactic nuclei agn can be probed by deep xray surveys we review results from large xray selected samples including first results from the xmmnewton cosmos survey a new picture arises from the fact t... | [['the', 'cosmological', 'evolution', 'of', 'supermassive', 'black', 'holes', 'smbhs', 'seems', 'to', 'be', 'intimately', 'linked', 'to', 'their', 'host', 'galaxies', 'active', 'galactic', 'nuclei', 'agn', 'can', 'be', 'probed', 'by', 'deep', 'xray', 'surveys', 'we', 'review', 'results', 'from', 'large', 'xray', 'selec... | [-0.04628222472174972, 0.09564676838443738, -0.059934674652363615, 0.1608719889147049, -0.12720632086560693, -0.053209988373981894, 0.0448343290816685, 0.40955831258961894, -0.14168681113383258, -0.34286016803059094, 0.07247823550704129, -0.32126810450221077, -0.014747021907889988, 0.21214569868840594, -0.0259501525345... |
708.0943 | Kinematics of the Scorpius-Centaurus OB Association | A fine structure related to the kinematic peculiarities of three components
of the Scorpius-Centaurus association (LCC, UCL, and US) has been revealed in
the UV-velocity distribution of Gould Belt stars. We have been able to identify
the most likely members of these groups by applying the method of analyzing the
two-... | astro-ph | a fine structure related to the kinematic peculiarities of three components of the scorpiuscentaurus association lcc ucl and us has been revealed in the uvvelocity distribution of gould belt stars we have been able to identify the most likely members of these groups by applying the method of analyzing the twodimensiona... | [['a', 'fine', 'structure', 'related', 'to', 'the', 'kinematic', 'peculiarities', 'of', 'three', 'components', 'of', 'the', 'scorpiuscentaurus', 'association', 'lcc', 'ucl', 'and', 'us', 'has', 'been', 'revealed', 'in', 'the', 'uvvelocity', 'distribution', 'of', 'gould', 'belt', 'stars', 'we', 'have', 'been', 'able', '... | [-0.11474379447311665, 0.08777539191299412, -0.1458205045158032, 0.02898733784227512, -0.10412491614604655, 0.003795631704109212, 0.02603542378195133, 0.3945398934734014, -0.2323808777724547, -0.32580625582943484, 0.05460133780711016, -0.21634734527099353, -0.06384989816018385, 0.19198646871987274, -0.0413570637683287,... |
708.0944 | Highly efficient single photon emission from single quantum dots within
a two-dimensional photonic bandgap | We report highly efficient single photon generation from InGaAs
self-assembled quantum dots emitting within a two-dimensional photonic bandgap.
A strongly suppressed multiphoton probability is obtained for single quantum
dots in bulk GaAs and those emitting into the photonic bandgap. In the latter
case, photoluminesc... | cond-mat.mtrl-sci cond-mat.other | we report highly efficient single photon generation from ingaas selfassembled quantum dots emitting within a twodimensional photonic bandgap a strongly suppressed multiphoton probability is obtained for single quantum dots in bulk gaas and those emitting into the photonic bandgap in the latter case photoluminescence sa... | [['we', 'report', 'highly', 'efficient', 'single', 'photon', 'generation', 'from', 'ingaas', 'selfassembled', 'quantum', 'dots', 'emitting', 'within', 'a', 'twodimensional', 'photonic', 'bandgap', 'a', 'strongly', 'suppressed', 'multiphoton', 'probability', 'is', 'obtained', 'for', 'single', 'quantum', 'dots', 'in', 'b... | [-0.07634117863379604, 0.21980601422522844, -0.0025873655022298995, -0.0037129484569222845, 0.03811211450110105, -0.2309109215001183, 0.06415393140382511, 0.49116667926557794, -0.22126573398093546, -0.30702105941143165, -0.02217609176319862, -0.31491945968740737, -0.05284998637300816, 0.3025183532202293, -0.00251767910... |
708.0945 | An iterative tomogravity algorithm for the estimation of network traffic | This paper introduces an iterative tomogravity algorithm for the estimation
of a network traffic matrix based on one snapshot observation of the link loads
in the network. The proposed method does not require complete observation of
the total load on individual edge links or proper tuning of a penalty parameter
as ex... | stat.AP | this paper introduces an iterative tomogravity algorithm for the estimation of a network traffic matrix based on one snapshot observation of the link loads in the network the proposed method does not require complete observation of the total load on individual edge links or proper tuning of a penalty parameter as exist... | [['this', 'paper', 'introduces', 'an', 'iterative', 'tomogravity', 'algorithm', 'for', 'the', 'estimation', 'of', 'a', 'network', 'traffic', 'matrix', 'based', 'on', 'one', 'snapshot', 'observation', 'of', 'the', 'link', 'loads', 'in', 'the', 'network', 'the', 'proposed', 'method', 'does', 'not', 'require', 'complete',... | [-0.15527826729555463, 0.0027252866652710257, -0.06992270603646027, 0.014347052491313322, -0.1075359415046351, -0.16412682858360714, 0.11413922336434426, 0.4198352095865926, -0.2461741131318863, -0.36354248175874004, 0.14134667542367785, -0.22356163015112626, -0.17435711291131326, 0.1908764375934139, -0.124772251055705... |
708.0946 | Asymptotics for Hermite-Pade rational approximants for two analytic
functions with separated pairs of branch points (case of genus 0) | We investigate the asymptotic behavior for type II Hermite-Pade approximation
to two functions, where each function has two branch points and the pairs of
branch points are separated. We give a classification of the cases such that
the limiting counting measures for the poles of the Hermite-Pade approximants
are desc... | math.CA math.CV | we investigate the asymptotic behavior for type ii hermitepade approximation to two functions where each function has two branch points and the pairs of branch points are separated we give a classification of the cases such that the limiting counting measures for the poles of the hermitepade approximants are described ... | [['we', 'investigate', 'the', 'asymptotic', 'behavior', 'for', 'type', 'ii', 'hermitepade', 'approximation', 'to', 'two', 'functions', 'where', 'each', 'function', 'has', 'two', 'branch', 'points', 'and', 'the', 'pairs', 'of', 'branch', 'points', 'are', 'separated', 'we', 'give', 'a', 'classification', 'of', 'the', 'ca... | [-0.15996421877764636, 0.011622773634551957, -0.10941716157705397, 0.1266823493443463, -0.025098045339791087, -0.13442003853233145, 0.06687595425089737, 0.3043459468764496, -0.2595147616890687, -0.21576053652543206, 0.11525001379318833, -0.30556695242118725, -0.18001778269404764, 0.16197755849744017, -0.030679422577524... |
708.0947 | Rational semigroup automata | We show that for any monoid M, the family of languages accepted by M-automata
(or equivalently, generated by regular valence grammars over M) is completely
determined by that part of M which lies outside the maximal ideal. Hence, every
such family arises as the family of languages accepted by N-automata where N is
a ... | math.RA | we show that for any monoid m the family of languages accepted by mautomata or equivalently generated by regular valence grammars over m is completely determined by that part of m which lies outside the maximal ideal hence every such family arises as the family of languages accepted by nautomata where n is a simple or ... | [['we', 'show', 'that', 'for', 'any', 'monoid', 'm', 'the', 'family', 'of', 'languages', 'accepted', 'by', 'mautomata', 'or', 'equivalently', 'generated', 'by', 'regular', 'valence', 'grammars', 'over', 'm', 'is', 'completely', 'determined', 'by', 'that', 'part', 'of', 'm', 'which', 'lies', 'outside', 'the', 'maximal',... | [-0.13092572953695814, 0.1345452430573727, -0.02371642744972133, 0.07757120099415046, -0.09429190716222294, -0.12213910137321435, 0.05746653701313406, 0.33250045089745056, -0.3530040422828831, -0.22092426702033216, 0.09763377814613027, -0.2782191658774465, -0.1063780745014311, 0.20946597877556605, -0.09968726688598775,... |
708.0948 | Pricing, Hedging and Optimally Designing Derivatives Via Minimization of
Risk Measures | The question of pricing and hedging a given contingent claim has a unique
solution in a complete market framework. When some incompleteness is
introduced, the problem becomes however more difficult. Several approaches have
been adopted in the literature to provide a satisfactory answer to this
problem, for a particul... | math.PR | the question of pricing and hedging a given contingent claim has a unique solution in a complete market framework when some incompleteness is introduced the problem becomes however more difficult several approaches have been adopted in the literature to provide a satisfactory answer to this problem for a particular cho... | [['the', 'question', 'of', 'pricing', 'and', 'hedging', 'a', 'given', 'contingent', 'claim', 'has', 'a', 'unique', 'solution', 'in', 'a', 'complete', 'market', 'framework', 'when', 'some', 'incompleteness', 'is', 'introduced', 'the', 'problem', 'becomes', 'however', 'more', 'difficult', 'several', 'approaches', 'have',... | [-0.07612615976926909, -0.010900723685469474, -0.10142704729722547, 0.17323111704840533, -0.11473384071901745, -0.1567747539660076, 0.11434729235325179, 0.39532935941515834, -0.2739746114809294, -0.26619904314652465, 0.14547498475336137, -0.26180994184687734, -0.16876337448211046, 0.17411120090044427, -0.19550538741584... |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.