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708.4049 | An analysis of the durations of Swift Gamma-Ray Bursts | We report the systematic analysis of the durations for Swift gamma-ray bursts
(GRBs) and compare the results with those of pre-Swift data. For 95 GRBs with
known redshift, we show that the observed durations have two lognormal
distributions that are clearly divided at $T_{90}\simeq2$ s. This is consistent
with the ea... | astro-ph | we report the systematic analysis of the durations for swift gammaray bursts grbs and compare the results with those of preswift data for 95 grbs with known redshift we show that the observed durations have two lognormal distributions that are clearly divided at t_90simeq2 s this is consistent with the earlier batse re... | [['we', 'report', 'the', 'systematic', 'analysis', 'of', 'the', 'durations', 'for', 'swift', 'gammaray', 'bursts', 'grbs', 'and', 'compare', 'the', 'results', 'with', 'those', 'of', 'preswift', 'data', 'for', '95', 'grbs', 'with', 'known', 'redshift', 'we', 'show', 'that', 'the', 'observed', 'durations', 'have', 'two',... | [-0.06218613041627327, 0.1502355620149373, -0.08953446659787664, 0.18168348873865434, -0.0683358203035298, -0.10289090176131702, 0.036180225711928415, 0.5098079345032773, -0.1677446922274844, -0.3301933298775014, 0.01926642555615321, -0.31977182656414055, -0.014942753885016345, 0.26641510521380496, -0.03292016549998482... |
708.405 | Ni-PZT-Ni Trilayered Magnetoelectric composites Synthesized by
Electro-deposition | We report the high strength of magnetoelectric (ME) coupling of trilayered
composites prepared by electro-deposition. The ME coupling of Ni-lead zirconate
titanate (PZT)-Ni trilayered structure was measured ranged from1 kHz to 120
kHz. The trilayered composites exhibit high magnetoelectric voltage coefficient
because... | cond-mat.mtrl-sci cond-mat.other | we report the high strength of magnetoelectric me coupling of trilayered composites prepared by electrodeposition the me coupling of nilead zirconate titanate pztni trilayered structure was measured ranged from1 khz to 120 khz the trilayered composites exhibit high magnetoelectric voltage coefficient because of good bo... | [['we', 'report', 'the', 'high', 'strength', 'of', 'magnetoelectric', 'me', 'coupling', 'of', 'trilayered', 'composites', 'prepared', 'by', 'electrodeposition', 'the', 'me', 'coupling', 'of', 'nilead', 'zirconate', 'titanate', 'pztni', 'trilayered', 'structure', 'was', 'measured', 'ranged', 'from1', 'khz', 'to', '120',... | [-0.2121993387476183, 0.225313486591077, 0.08900444083011304, -0.12446414056541517, -0.15463589472720066, -0.1744802698182563, 0.08361210381516661, 0.45942900110131657, -0.26350576103999257, -0.3718909297663814, -0.032480453954448395, -0.29487879601760936, -0.1316533167189799, 0.2156084903444235, 0.04651555983731762, 0... |
708.4051 | On orthostochastic, unistochastic and qustochastic matrices | We introduce qustochastic matrices as the bistochastic matrices arising from
quaternionic unitary matrices by replacing each entry with the square of its
norm. This is the quaternionic analogue of the unistochastic matrices studied
by physicists. We also introduce quaternionic Hadamard matrices and
quaternionic mutua... | math-ph math.MP | we introduce qustochastic matrices as the bistochastic matrices arising from quaternionic unitary matrices by replacing each entry with the square of its norm this is the quaternionic analogue of the unistochastic matrices studied by physicists we also introduce quaternionic hadamard matrices and quaternionic mutually ... | [['we', 'introduce', 'qustochastic', 'matrices', 'as', 'the', 'bistochastic', 'matrices', 'arising', 'from', 'quaternionic', 'unitary', 'matrices', 'by', 'replacing', 'each', 'entry', 'with', 'the', 'square', 'of', 'its', 'norm', 'this', 'is', 'the', 'quaternionic', 'analogue', 'of', 'the', 'unistochastic', 'matrices',... | [-0.13002431748367577, 0.17314228967147044, 0.01705470511441523, 0.053024555724787426, 0.012446847503039852, -0.14712140356830086, -0.01328159831127668, 0.3603021240826831, -0.2687645103047456, -0.17067847222493715, 0.12845636045571462, -0.31899041281900853, -0.2189604868910399, 0.13876569912073214, -0.0808611291135291... |
708.4052 | Magnetoelectric Effect in Ni-PZT-Ni Cylindrical Layered Composite
Synthesized by Electro-deposition | The magnetoelectric (ME) coupling of cylindrical trilayered composite was
studied in this paper. The Ni-lead zirconate titanate (PZT)-Ni trilayered
cylindrical composite was synthesized by electro-deposition. The maximum ME
voltage coefficient of cylindrical ME composite is 35V/cm Oe, about three times
higher than th... | cond-mat.mtrl-sci | the magnetoelectric me coupling of cylindrical trilayered composite was studied in this paper the nilead zirconate titanate pztni trilayered cylindrical composite was synthesized by electrodeposition the maximum me voltage coefficient of cylindrical me composite is 35vcm oe about three times higher than that of the pla... | [['the', 'magnetoelectric', 'me', 'coupling', 'of', 'cylindrical', 'trilayered', 'composite', 'was', 'studied', 'in', 'this', 'paper', 'the', 'nilead', 'zirconate', 'titanate', 'pztni', 'trilayered', 'cylindrical', 'composite', 'was', 'synthesized', 'by', 'electrodeposition', 'the', 'maximum', 'me', 'voltage', 'coeffic... | [-0.1605998855712039, 0.18842158761082134, -0.01249665053289258, -0.08232265189185403, -0.1347620017261485, -0.15890815777356182, 0.01214081746018544, 0.3983574469019188, -0.22702922125796923, -0.3447736498763722, 0.04002002199452496, -0.26162644699634463, -0.1583498519677878, 0.15918329025336195, -0.023983031731057033... |
708.4053 | Origin of Ferromagnetism in nitrogen embedded ZnO:N thin films | Nitrogen embedded ZnO:N films prepared by pulsed laser deposition exhibit
significant ferromagnetism. The nitrogen ions contained in ZnO confirmed by
Secondary Ion Microscopic Spectrum and Raman experiments and the embedded
nitrogen ions can be regarded as defects. According to the experiment results,
a mechanism is ... | cond-mat.str-el cond-mat.mtrl-sci | nitrogen embedded znon films prepared by pulsed laser deposition exhibit significant ferromagnetism the nitrogen ions contained in zno confirmed by secondary ion microscopic spectrum and raman experiments and the embedded nitrogen ions can be regarded as defects according to the experiment results a mechanism is propos... | [['nitrogen', 'embedded', 'znon', 'films', 'prepared', 'by', 'pulsed', 'laser', 'deposition', 'exhibit', 'significant', 'ferromagnetism', 'the', 'nitrogen', 'ions', 'contained', 'in', 'zno', 'confirmed', 'by', 'secondary', 'ion', 'microscopic', 'spectrum', 'and', 'raman', 'experiments', 'and', 'the', 'embedded', 'nitro... | [-0.07657691828805853, 0.27670617979691103, 0.0257275063578073, 0.013559261770071546, 0.08879374185795183, -0.1950826961337379, 0.0808591229625063, 0.4079649924292221, -0.2303118471576421, -0.2939121264655999, -0.003480975731141731, -0.3709988764713745, -0.016293688870228088, 0.1385126227894714, 0.008043709378857334, -... |
708.4054 | Pion Form Factors in Holographic QCD | Using a holographic dual model of QCD, we compute the pion electromagnetic
form factor F_pi(Q^2) in the spacelike momentum transfer region, as well as
pion couplings to vector mesons g_rho^(n) pi pi. Spontaneous and explicit
chiral symmetry breaking are intrinsic features of this particular holographic
model. We cons... | hep-ph | using a holographic dual model of qcd we compute the pion electromagnetic form factor f_piq2 in the spacelike momentum transfer region as well as pion couplings to vector mesons g_rhon pi pi spontaneous and explicit chiral symmetry breaking are intrinsic features of this particular holographic model we consider variant... | [['using', 'a', 'holographic', 'dual', 'model', 'of', 'qcd', 'we', 'compute', 'the', 'pion', 'electromagnetic', 'form', 'factor', 'f_piq2', 'in', 'the', 'spacelike', 'momentum', 'transfer', 'region', 'as', 'well', 'as', 'pion', 'couplings', 'to', 'vector', 'mesons', 'g_rhon', 'pi', 'pi', 'spontaneous', 'and', 'explicit... | [-0.062233851084088465, 0.18034871255376322, -0.10249104117289842, 0.13110258498978938, -0.11048868885914356, -0.15540508824222557, 0.05226835705209797, 0.37512285328086686, -0.1710205409223871, -0.24715088303063942, 0.0036719786419994573, -0.30393201314419616, -0.06777280541513499, 0.09660064996569417, 0.0443324871917... |
708.4055 | Resonant Atom Traps for Electromagnetic Waves | Exitation of atomic levels due to interaction with electromagnetic waves has
been the subject of numerous works, both experimental and theoretical. This
topic became of interest in accelerator physics in relation to high efficiency
charge exchange injection into rings for high beam power applications. Taking
equation... | nlin.PS nlin.AO | exitation of atomic levels due to interaction with electromagnetic waves has been the subject of numerous works both experimental and theoretical this topic became of interest in accelerator physics in relation to high efficiency charge exchange injection into rings for high beam power applications taking equations of ... | [['exitation', 'of', 'atomic', 'levels', 'due', 'to', 'interaction', 'with', 'electromagnetic', 'waves', 'has', 'been', 'the', 'subject', 'of', 'numerous', 'works', 'both', 'experimental', 'and', 'theoretical', 'this', 'topic', 'became', 'of', 'interest', 'in', 'accelerator', 'physics', 'in', 'relation', 'to', 'high', ... | [-0.15482980976020075, 0.17667340553102312, -0.04352173340753708, 0.052259016311475, -0.04962309523827834, -0.13533139530378563, 0.028650094524267162, 0.3901354860267546, -0.22625348019604402, -0.3096627082973045, 0.05785617676384029, -0.2887372353804264, -0.08176533713185015, 0.21744044308539434, -0.01445780606752441,... |
708.4056 | Renormalization group analysis of resonantly interacting anyons | We formulate a field theory for resonantly interacting anyons, that enables
us to perform a perturbative calculation near the fermionic limit. We derive
renormalization group equations for three-body and four-body couplings at
one-loop order. In addition to two fixed points, we find a limit cycle behavior
in the four... | hep-th cond-mat.other nucl-th quant-ph | we formulate a field theory for resonantly interacting anyons that enables us to perform a perturbative calculation near the fermionic limit we derive renormalization group equations for threebody and fourbody couplings at oneloop order in addition to two fixed points we find a limit cycle behavior in the fourbody coup... | [['we', 'formulate', 'a', 'field', 'theory', 'for', 'resonantly', 'interacting', 'anyons', 'that', 'enables', 'us', 'to', 'perform', 'a', 'perturbative', 'calculation', 'near', 'the', 'fermionic', 'limit', 'we', 'derive', 'renormalization', 'group', 'equations', 'for', 'threebody', 'and', 'fourbody', 'couplings', 'at',... | [-0.20622482305759046, 0.18286203554298033, -0.1071974963453583, 0.06664001948551321, 0.005959922657729906, -0.13891425048627082, 0.12588152885398843, 0.27611780188000595, -0.19513894437018353, -0.26667001385079053, -0.013834648366757959, -0.3260206219236382, -0.10752402046756422, 0.11815550206916133, 0.070733705443925... |
708.4057 | Determination of Charm Hadronic Branching Ratios and New Modes | Recent results from CLEO-c, BABAR, and Belle on measurements of absolute
branching fractions of D and D_s mesons are reviewed.
| hep-ex | recent results from cleoc babar and belle on measurements of absolute branching fractions of d and d_s mesons are reviewed | [['recent', 'results', 'from', 'cleoc', 'babar', 'and', 'belle', 'on', 'measurements', 'of', 'absolute', 'branching', 'fractions', 'of', 'd', 'and', 'd_s', 'mesons', 'are', 'reviewed']] | [-0.0077271369664231315, 0.2656277664238587, -0.08199710166081786, -0.0032715687528252603, -0.07488432498648763, -0.13060635160654782, 0.1530009879730642, 0.2939566494897008, -0.03993649072945118, -0.15046440549194812, -0.0632270248606801, -0.5847676262259484, 0.07978449473157526, 0.21406539473682643, 0.088250468857586... |
708.4058 | Spin-dependent Hedin's equations | Hedin's equations for the electron self-energy and the vertex were originally
derived for a many-electron system with Coulomb interaction. In recent years it
has been increasingly recognized that spin interactions can play a major role
in determining physical properties of systems such as nanoscale magnets or of
inte... | cond-mat.str-el cond-mat.mtrl-sci | hedins equations for the electron selfenergy and the vertex were originally derived for a manyelectron system with coulomb interaction in recent years it has been increasingly recognized that spin interactions can play a major role in determining physical properties of systems such as nanoscale magnets or of interfaces... | [['hedins', 'equations', 'for', 'the', 'electron', 'selfenergy', 'and', 'the', 'vertex', 'were', 'originally', 'derived', 'for', 'a', 'manyelectron', 'system', 'with', 'coulomb', 'interaction', 'in', 'recent', 'years', 'it', 'has', 'been', 'increasingly', 'recognized', 'that', 'spin', 'interactions', 'can', 'play', 'a'... | [-0.1982467898058814, 0.13934556900844122, -0.04662913706852123, 0.11594718928878232, -0.017432104551245445, -0.14374392994304563, -0.06445046617383403, 0.3353840550044914, -0.2323613525035658, -0.3057841805426718, 0.009641627705498756, -0.3449488862889347, -0.16543893234550275, 0.20722105859645776, 0.11484581593109609... |
708.4059 | Asymptotic Blocking Probabilities in Loss Networks with Subexponential
Demands | The analysis of stochastic loss networks has long been of interest in
computer and communications networks and is becoming important in the areas of
service and information systems. In traditional settings, computing the well
known Erlang formula for blocking probability in these systems becomes
intractable for large... | math.PR | the analysis of stochastic loss networks has long been of interest in computer and communications networks and is becoming important in the areas of service and information systems in traditional settings computing the well known erlang formula for blocking probability in these systems becomes intractable for larger re... | [['the', 'analysis', 'of', 'stochastic', 'loss', 'networks', 'has', 'long', 'been', 'of', 'interest', 'in', 'computer', 'and', 'communications', 'networks', 'and', 'is', 'becoming', 'important', 'in', 'the', 'areas', 'of', 'service', 'and', 'information', 'systems', 'in', 'traditional', 'settings', 'computing', 'the', ... | [-0.11455862958632086, 0.040413772000085925, -0.04019820565438789, 0.135364911489207, -0.017863026083163595, -0.1716358092573026, 0.1271906688404472, 0.39526637416818866, -0.23097117920406163, -0.30978672518192424, 0.10336702772740113, -0.25679775845745334, -0.16310106880314973, 0.22766827303187354, -0.1265246482438195... |
708.406 | Invariant information and complementarity in high-dimensional states | Using a generalization of the invariant information introduced by Brukner and
Zeilinger [Phys. Rev. Lett. \textbf{83}, 3354 (1999)] to high-dimensional
systems, we introduce a complementarity relation between the local and nonlocal
information for $d\times d$ systems under the isolated environment, where $d$
is prime... | quant-ph | using a generalization of the invariant information introduced by brukner and zeilinger phys rev lett textbf83 3354 1999 to highdimensional systems we introduce a complementarity relation between the local and nonlocal information for dtimes d systems under the isolated environment where d is prime or the power of prim... | [['using', 'a', 'generalization', 'of', 'the', 'invariant', 'information', 'introduced', 'by', 'brukner', 'and', 'zeilinger', 'phys', 'rev', 'lett', 'textbf83', '3354', '1999', 'to', 'highdimensional', 'systems', 'we', 'introduce', 'a', 'complementarity', 'relation', 'between', 'the', 'local', 'and', 'nonlocal', 'infor... | [-0.16175892415095963, 0.06367977008584046, -0.08697592552691218, 0.003744099106253059, -0.025296588751277136, -0.15514601870710332, 0.06000538332568061, 0.2605521026247692, -0.23902544715712148, -0.29378213040200213, 0.01589666888861346, -0.2845837716839366, -0.19702097191475332, 0.1488681908268782, -0.133252541804986... |
708.4061 | Plasma experiments with relevance for complexity science | The goal of this paper is the identification of the physical processes at the
origin of the nonlinear behavior of a plasma conductor when an external
constraint gradually departs the system from thermal equilibrium. This reveals
the presence of a self-organization scenario whose final product depends on the
magnitude... | nlin.PS nlin.AO physics.plasm-ph | the goal of this paper is the identification of the physical processes at the origin of the nonlinear behavior of a plasma conductor when an external constraint gradually departs the system from thermal equilibrium this reveals the presence of a selforganization scenario whose final product depends on the magnitude of ... | [['the', 'goal', 'of', 'this', 'paper', 'is', 'the', 'identification', 'of', 'the', 'physical', 'processes', 'at', 'the', 'origin', 'of', 'the', 'nonlinear', 'behavior', 'of', 'a', 'plasma', 'conductor', 'when', 'an', 'external', 'constraint', 'gradually', 'departs', 'the', 'system', 'from', 'thermal', 'equilibrium', '... | [-0.15900626020356232, 0.13930054843192513, -0.08648941260696177, 0.013426201769730427, -0.04820106694409129, -0.10045028984598764, 0.06409675859800586, 0.27454854553187646, -0.3132149684275468, -0.3388652968370206, 0.10051340845468865, -0.23670671523346767, -0.13805983214919176, 0.18735117039324103, -0.036576610221364... |
708.4062 | Constraining Dark Energy and Cosmological Transition Redshift with Type
Ia Supernovae | The property of dark energy and the physical reason for acceleration of the
present universe are two of the most difficult problems in modern cosmology.
The dark energy contributes about two-thirds of the critical density of the
present universe from the observations of type-Ia supernova (SNe Ia) and
anisotropy of co... | astro-ph | the property of dark energy and the physical reason for acceleration of the present universe are two of the most difficult problems in modern cosmology the dark energy contributes about twothirds of the critical density of the present universe from the observations of typeia supernova sne ia and anisotropy of cosmic mi... | [['the', 'property', 'of', 'dark', 'energy', 'and', 'the', 'physical', 'reason', 'for', 'acceleration', 'of', 'the', 'present', 'universe', 'are', 'two', 'of', 'the', 'most', 'difficult', 'problems', 'in', 'modern', 'cosmology', 'the', 'dark', 'energy', 'contributes', 'about', 'twothirds', 'of', 'the', 'critical', 'den... | [-0.0875644467844458, 0.12388710816469092, -0.08148495449221192, 0.10169160727347279, -0.11203622560273728, -0.07572807643615315, 0.03222919892051757, 0.3625948454558464, -0.21369621943363581, -0.3427201484638528, 0.010876254118368801, -0.29876151137292534, 0.0008824160804265532, 0.18651812436779402, 0.0459813447026857... |
708.4063 | Anti-correlation between energy-gap and phonon energy for cuprate Bi2212
superconductor | Using electron-phonon mechanism, we explains very well the spatial
anti-orrelation between the energy-gap and the energy of phonon mode for
cuprate superconductor found in d^2I/dV^2 spectrum by STM measurements [Jinho
Lee, et.al Nature {\bf 442},546 (2006)], which is the direct effect of a
relation $M<\omega^{2}>\lam... | cond-mat.supr-con cond-mat.mtrl-sci | using electronphonon mechanism we explains very well the spatial antiorrelation between the energygap and the energy of phonon mode for cuprate superconductor found in d2idv2 spectrum by stm measurements jinho lee etal nature bf 442546 2006 which is the direct effect of a relation momega2lambdaconst we calculate t_c ma... | [['using', 'electronphonon', 'mechanism', 'we', 'explains', 'very', 'well', 'the', 'spatial', 'antiorrelation', 'between', 'the', 'energygap', 'and', 'the', 'energy', 'of', 'phonon', 'mode', 'for', 'cuprate', 'superconductor', 'found', 'in', 'd2idv2', 'spectrum', 'by', 'stm', 'measurements', 'jinho', 'lee', 'etal', 'na... | [-0.1716150708400227, 0.12515524563636501, -0.09729071789228454, 0.07682776567726878, -0.11676917217093809, -0.12858044451648562, 0.15297039681724434, 0.3311052232466895, -0.23132702651441675, -0.31545716492009573, -0.05228916010297514, -0.31555174536810354, -0.15944349915110345, 0.2123487508406156, 0.02435434039617920... |
708.4064 | Ball Lightning as a Self-organized Complexity | The ball lightning phenomenon is explained in the frame of a
self-organization scenario suggested by experiments performed on the
spontaneously generated complex spherical space charge configuration in plasma.
Originated in a hot plasma, suddenly created in a point where a lightning flash
strikes the Earth surface, t... | nlin.PS nlin.AO physics.plasm-ph | the ball lightning phenomenon is explained in the frame of a selforganization scenario suggested by experiments performed on the spontaneously generated complex spherical space charge configuration in plasma originated in a hot plasma suddenly created in a point where a lightning flash strikes the earth surface the bal... | [['the', 'ball', 'lightning', 'phenomenon', 'is', 'explained', 'in', 'the', 'frame', 'of', 'a', 'selforganization', 'scenario', 'suggested', 'by', 'experiments', 'performed', 'on', 'the', 'spontaneously', 'generated', 'complex', 'spherical', 'space', 'charge', 'configuration', 'in', 'plasma', 'originated', 'in', 'a', '... | [-0.11380596015450739, 0.22641137081682106, -0.08944903733595487, 0.1057572895245872, -0.04688483110968341, -0.05566329275106275, 0.029001752674478548, 0.35755780919693236, -0.2605732176308484, -0.30531526138904946, 0.053922493150638226, -0.20664665502831772, -0.12753481281444776, 0.1503156883454369, -0.074314156215540... |
708.4065 | Self-consistent theory of reversible ligand binding to a spherical cell | In this article, we study the kinetics of reversible ligand binding to
receptors on a spherical cell surface using a self-consistent stochastic
theory. Binding, dissociation, diffusion and rebinding of ligands are
incorporated into the theory in a systematic manner. We derive explicitly the
time evolution of the liga... | q-bio.SC cond-mat.stat-mech q-bio.QM | in this article we study the kinetics of reversible ligand binding to receptors on a spherical cell surface using a selfconsistent stochastic theory binding dissociation diffusion and rebinding of ligands are incorporated into the theory in a systematic manner we derive explicitly the time evolution of the ligandbound ... | [['in', 'this', 'article', 'we', 'study', 'the', 'kinetics', 'of', 'reversible', 'ligand', 'binding', 'to', 'receptors', 'on', 'a', 'spherical', 'cell', 'surface', 'using', 'a', 'selfconsistent', 'stochastic', 'theory', 'binding', 'dissociation', 'diffusion', 'and', 'rebinding', 'of', 'ligands', 'are', 'incorporated', ... | [-0.09661143128440017, 0.14525756866438314, -0.0685948446270777, 0.09301085528335534, 0.03339125977130607, -0.12496854070806876, 0.08059759343974292, 0.3470018033310771, -0.23882861797115765, -0.26983615730889143, 0.06196898491471074, -0.27536385898478327, -0.13432585214381107, 0.15686647309572435, -0.00369957840332062... |
708.4066 | On the "mystery" of differential negative resistance | Investigating the causes of the nonlinear behavior of a gaseous conductor we
identified the presence of two states of the complex space charge configuration
self-assembled in front of the anode. These states correspond to two levels of
self-organization from which the first one is related to spatial pattern
whereas t... | physics.plasm-ph nlin.AO | investigating the causes of the nonlinear behavior of a gaseous conductor we identified the presence of two states of the complex space charge configuration selfassembled in front of the anode these states correspond to two levels of selforganization from which the first one is related to spatial pattern whereas the se... | [['investigating', 'the', 'causes', 'of', 'the', 'nonlinear', 'behavior', 'of', 'a', 'gaseous', 'conductor', 'we', 'identified', 'the', 'presence', 'of', 'two', 'states', 'of', 'the', 'complex', 'space', 'charge', 'configuration', 'selfassembled', 'in', 'front', 'of', 'the', 'anode', 'these', 'states', 'correspond', 't... | [-0.1759715270956309, 0.12606498431705404, -0.05539063593707255, 0.017514707884543294, -0.01968176328369136, -0.11326253995552514, -0.0035228434999844114, 0.3432678205856276, -0.30010062715635427, -0.28510090310886066, 0.049813003371948904, -0.29036774360619994, -0.1447509237049708, 0.17569339455747343, -0.003765628700... |
708.4067 | Cell-like space charge configurations formed by selforganization in
laboratory | A phenomenological model of self-organization explaining the emergence of a
complexity with features that apparently satisfy the specific criteria usually
required for recognizing the appearance of life in laboratory is presented. The
described phenomenology, justified by laboratory experiments, is essentially
based ... | nlin.AO nlin.PS physics.plasm-ph | a phenomenological model of selforganization explaining the emergence of a complexity with features that apparently satisfy the specific criteria usually required for recognizing the appearance of life in laboratory is presented the described phenomenology justified by laboratory experiments is essentially based on loc... | [['a', 'phenomenological', 'model', 'of', 'selforganization', 'explaining', 'the', 'emergence', 'of', 'a', 'complexity', 'with', 'features', 'that', 'apparently', 'satisfy', 'the', 'specific', 'criteria', 'usually', 'required', 'for', 'recognizing', 'the', 'appearance', 'of', 'life', 'in', 'laboratory', 'is', 'presente... | [-0.12267815565868614, 0.14693083901556186, -0.11619448454956471, 0.07521369675300832, -0.0651550213030229, -0.14578287559848876, 0.04415892818252797, 0.3286494593837379, -0.24511319800153558, -0.2908520712344735, 0.06738812293725112, -0.1860786248228432, -0.16903940758403438, 0.18271591456572492, -0.0365273498205675, ... |
708.4068 | Boundaries for algebras of holomorphic functions on Banach spaces | We study the relations between boundaries for algebras of holomorphic
functions on Banach spaces and complex convexity of their balls. In addition,
we show that the Shilov boundary for algebras of holomorphic functions on an
order continuous sequence space $X$ is the unit sphere $S_X$ if $X$ is locally
c-convex. In p... | math.FA | we study the relations between boundaries for algebras of holomorphic functions on banach spaces and complex convexity of their balls in addition we show that the shilov boundary for algebras of holomorphic functions on an order continuous sequence space x is the unit sphere s_x if x is locally cconvex in particular it... | [['we', 'study', 'the', 'relations', 'between', 'boundaries', 'for', 'algebras', 'of', 'holomorphic', 'functions', 'on', 'banach', 'spaces', 'and', 'complex', 'convexity', 'of', 'their', 'balls', 'in', 'addition', 'we', 'show', 'that', 'the', 'shilov', 'boundary', 'for', 'algebras', 'of', 'holomorphic', 'functions', 'o... | [-0.18743881873691073, 0.09454181554312789, -0.05532313330401947, 0.08715609335957701, -0.07878821511494827, -0.06472321929612074, -0.026243597692641688, 0.4465460018170661, -0.34169219142521723, -0.10458718140957406, 0.12628780954786722, -0.2861333771058953, -0.13647454552891025, 0.19279775340446687, -0.12315263213163... |
708.4069 | Bishop's Theorem and Differentiability of a subspace of $C_b(K)$ | Let $K$ be a Hausdorff space and $C_b(K)$ be the Banach algebra of all
complex bounded continuous functions on $K$. We study the G\^{a}teaux and
Fr\'echet differentiability of subspaces of $C_b(K)$. Using this, we show that
the set of all strong peak functions in a nontrivial separating separable
subspace $H$ of $C_b... | math.FA | let k be a hausdorff space and c_bk be the banach algebra of all complex bounded continuous functions on k we study the gateaux and frechet differentiability of subspaces of c_bk using this we show that the set of all strong peak functions in a nontrivial separating separable subspace h of c_bk is a dense g_delta subse... | [['let', 'k', 'be', 'a', 'hausdorff', 'space', 'and', 'c_bk', 'be', 'the', 'banach', 'algebra', 'of', 'all', 'complex', 'bounded', 'continuous', 'functions', 'on', 'k', 'we', 'study', 'the', 'gateaux', 'and', 'frechet', 'differentiability', 'of', 'subspaces', 'of', 'c_bk', 'using', 'this', 'we', 'show', 'that', 'the', ... | [-0.18221674035391155, 0.09054863860097304, -0.0636610077920025, 0.06238402079467943, -0.08165824618893412, -0.06836409205219375, 0.03467653585017993, 0.38973993015088987, -0.3250215109613425, -0.12202564134034065, 0.09938650967153492, -0.27525668877796355, -0.11550680289642429, 0.1901329222161604, -0.0931324892213902,... |
708.407 | The Loewy length of the descent algebra of type D | The Loewy length of the descent algebra of type D_{2m+1} is shown to be m+2,
for m \geq 2, by providing an upper bound that agrees with the lower bound in
\cite{BonnafePfeiffer2006}. The bound is obtained by showing that the length of
the longest path in the quiver of the descent algebra of D_{2m+1} is at most
m+1. T... | math.RT math.CO | the loewy length of the descent algebra of type d_2m1 is shown to be m2 for m geq 2 by providing an upper bound that agrees with the lower bound in citebonnafepfeiffer2006 the bound is obtained by showing that the length of the longest path in the quiver of the descent algebra of d_2m1 is at most m1 to achieve this bou... | [['the', 'loewy', 'length', 'of', 'the', 'descent', 'algebra', 'of', 'type', 'd_2m1', 'is', 'shown', 'to', 'be', 'm2', 'for', 'm', 'geq', '2', 'by', 'providing', 'an', 'upper', 'bound', 'that', 'agrees', 'with', 'the', 'lower', 'bound', 'in', 'citebonnafepfeiffer2006', 'the', 'bound', 'is', 'obtained', 'by', 'showing',... | [-0.16840991973339653, 0.10920194499380119, -0.10014538527312843, 0.009283548773645045, -0.07304270181723022, -0.13631758699193597, -0.02842689641229399, 0.335112618272203, -0.3435416941154891, -0.2978423129726242, 0.11414610290679834, -0.22908871383457394, -0.11860795443427267, 0.22677178093191278, -0.1107008556456683... |
708.4071 | Shape demagnetization effect on layered magnetoelectric composites | Magnetoelectric (ME) voltage coefficient was always considered independent on
in-plane shape of plate layered magnetostrictive-piezoelectric composites due
to the oversimplification in ME theoretical models. In this article, we present
that in fact the ME voltage coefficient is largely dependent on the in-plane
shape... | cond-mat.mtrl-sci | magnetoelectric me voltage coefficient was always considered independent on inplane shape of plate layered magnetostrictivepiezoelectric composites due to the oversimplification in me theoretical models in this article we present that in fact the me voltage coefficient is largely dependent on the inplane shape owing to... | [['magnetoelectric', 'me', 'voltage', 'coefficient', 'was', 'always', 'considered', 'independent', 'on', 'inplane', 'shape', 'of', 'plate', 'layered', 'magnetostrictivepiezoelectric', 'composites', 'due', 'to', 'the', 'oversimplification', 'in', 'me', 'theoretical', 'models', 'in', 'this', 'article', 'we', 'present', '... | [-0.1501932342114203, 0.1534539177039362, -0.034069088298430736, -0.08472294801052797, -0.1596980603515274, -0.14701514046949646, 0.035623035902433375, 0.4506699734720988, -0.2705151541934659, -0.3122564300687777, 0.016077872464881727, -0.26260420669698054, -0.18495867158182794, 0.2289609940877805, -0.047562251350394, ... |
708.4072 | Autoionization of spin-polarized metastable helium in tight anisotropic
harmonic traps | Spin-dipole mediated interactions between tightly confined metastable helium
atoms couple the spin-polarized quintet ${}^{5}\Sigma^{+}_{g}$ state to the
singlet ${}^{1}\Sigma^{+}_{g}$ state from which autoionization is highly
probable, resulting in finite lifetimes for the trap eigenstates. We extend our
earlier stud... | physics.atom-ph | spindipole mediated interactions between tightly confined metastable helium atoms couple the spinpolarized quintet 5sigma_g state to the singlet 1sigma_g state from which autoionization is highly probable resulting in finite lifetimes for the trap eigenstates we extend our earlier study on spherically symmetric harmoni... | [['spindipole', 'mediated', 'interactions', 'between', 'tightly', 'confined', 'metastable', 'helium', 'atoms', 'couple', 'the', 'spinpolarized', 'quintet', '5sigma_g', 'state', 'to', 'the', 'singlet', '1sigma_g', 'state', 'from', 'which', 'autoionization', 'is', 'highly', 'probable', 'resulting', 'in', 'finite', 'lifet... | [-0.12497325955444703, 0.2759752087821455, 0.0388193177656554, 0.05027958350053624, 0.06584604081049886, -0.17287033579676694, 0.02569169936620671, 0.39415533143379117, -0.16802613317318585, -0.26805884058222823, -0.028453556585388826, -0.32177005568924155, -0.01595712707620924, 0.13388113491439624, 0.07592581697618184... |
708.4073 | Classification of uniformly outer actions of Z^2 on UHF algebras | We give a complete classification up to cocycle conjugacy of uniformly outer
actions of Z^2 on UHF algebras. In particular, it is shown that any two
uniformly outer actions of Z^2 on a UHF algebra of infinite type are cocycle
conjugate. We also classify them up to outer conjugacy.
| math.OA | we give a complete classification up to cocycle conjugacy of uniformly outer actions of z2 on uhf algebras in particular it is shown that any two uniformly outer actions of z2 on a uhf algebra of infinite type are cocycle conjugate we also classify them up to outer conjugacy | [['we', 'give', 'a', 'complete', 'classification', 'up', 'to', 'cocycle', 'conjugacy', 'of', 'uniformly', 'outer', 'actions', 'of', 'z2', 'on', 'uhf', 'algebras', 'in', 'particular', 'it', 'is', 'shown', 'that', 'any', 'two', 'uniformly', 'outer', 'actions', 'of', 'z2', 'on', 'a', 'uhf', 'algebra', 'of', 'infinite', 't... | [-0.17862382013949432, 0.12363421411386558, -0.05770001936779947, 0.027955319582750753, -0.1326260804673847, -0.15638178128901184, 0.021798314963828544, 0.4432924669616076, -0.33006468730769595, -0.1825770286044904, 0.15954557687224707, -0.2626748330587027, -0.10696426592767239, 0.210892346592582, -0.12932352687479282,... |
708.4074 | Classification of outer actions of Z^N on O_2 | We will show that any two outer actions of Z^N on O_2 are cocycle conjugate.
| math.OA | we will show that any two outer actions of zn on o_2 are cocycle conjugate | [['we', 'will', 'show', 'that', 'any', 'two', 'outer', 'actions', 'of', 'zn', 'on', 'o_2', 'are', 'cocycle', 'conjugate']] | [-0.21260637119412423, 0.24380261357873678, -0.02506363354623318, 0.010256580108155807, -0.0348689965903759, -0.12197152835627396, -0.04021764267235994, 0.5530346453189849, -0.27081662652393185, -0.13660157347718874, 0.10875034105653564, -0.32764319131771724, -0.21427167014529308, 0.21074837346871694, -0.13315259603162... |
708.4075 | Graph Isomorphism is PSPACE-complete | Combining the the results of A.R. Meyer and L.J. Stockmeyer "The Equivalence
Problem for Regular Expressions with Squaring Requires Exponential Space", and
K.S. Booth "Isomorphism testing for graphs, semigroups, and finite automata are
polynomiamlly equivalent problems" shows that graph isomorphism is
PSPACE-complete... | cs.CC | combining the the results of ar meyer and lj stockmeyer the equivalence problem for regular expressions with squaring requires exponential space and ks booth isomorphism testing for graphs semigroups and finite automata are polynomiamlly equivalent problems shows that graph isomorphism is pspacecomplete | [['combining', 'the', 'the', 'results', 'of', 'ar', 'meyer', 'and', 'lj', 'stockmeyer', 'the', 'equivalence', 'problem', 'for', 'regular', 'expressions', 'with', 'squaring', 'requires', 'exponential', 'space', 'and', 'ks', 'booth', 'isomorphism', 'testing', 'for', 'graphs', 'semigroups', 'and', 'finite', 'automata', 'a... | [-0.08941677358092331, 0.08692443108458708, -0.04830319143650008, 0.14728030509304074, -0.10974967516050106, -0.23491121401510587, 0.05033253523998144, 0.38830290207775625, -0.29425642031767385, -0.3002605153497581, 0.10284413629007048, -0.2899416267826426, -0.11551184579730034, 0.1918596736859621, -0.1195167161796878,... |
708.4076 | Holder stability of diffeomorphisms | We prove that a $C^2$ diffeomorphism $f$ of a compact manifold $M$ satisfies
Axiom A and the strong transversality condition if and only if it is H\"{o}lder
stable, that is, any $C^1$ diffeomorphism $g$ of $M$ sufficiently $C^1$ close
to $f$ is conjugate to $f$ by a homeomorphism which is H\"{o}lder on the whole
mani... | math.DS | we prove that a c2 diffeomorphism f of a compact manifold m satisfies axiom a and the strong transversality condition if and only if it is holder stable that is any c1 diffeomorphism g of m sufficiently c1 close to f is conjugate to f by a homeomorphism which is holder on the whole manifold | [['we', 'prove', 'that', 'a', 'c2', 'diffeomorphism', 'f', 'of', 'a', 'compact', 'manifold', 'm', 'satisfies', 'axiom', 'a', 'and', 'the', 'strong', 'transversality', 'condition', 'if', 'and', 'only', 'if', 'it', 'is', 'holder', 'stable', 'that', 'is', 'any', 'c1', 'diffeomorphism', 'g', 'of', 'm', 'sufficiently', 'c1'... | [-0.27812012481418524, 0.11848841863261028, -0.12020993615839291, 0.06222801140763543, -0.12399192096834832, -0.24845578416504643, 0.011977621946822514, 0.3532879134259102, -0.27491204582832074, -0.16571782444688407, 0.11179102124984969, -0.22975218804045158, -0.08742505789480426, 0.1588669512928887, -0.150347410904412... |
708.4077 | Typicality, Freak Observers and the Anthropic Principle of Existence | We propose an alternative anthropic probability for calculating the
probabilities in eternal inflation. This anthropic probability follows
naturally from the weak anthropic principle, and does not suffer the freak
observer or the typicality problems. The problem that our observed cosmological
constant is not at the p... | hep-th astro-ph gr-qc | we propose an alternative anthropic probability for calculating the probabilities in eternal inflation this anthropic probability follows naturally from the weak anthropic principle and does not suffer the freak observer or the typicality problems the problem that our observed cosmological constant is not at the peak o... | [['we', 'propose', 'an', 'alternative', 'anthropic', 'probability', 'for', 'calculating', 'the', 'probabilities', 'in', 'eternal', 'inflation', 'this', 'anthropic', 'probability', 'follows', 'naturally', 'from', 'the', 'weak', 'anthropic', 'principle', 'and', 'does', 'not', 'suffer', 'the', 'freak', 'observer', 'or', '... | [-0.0717771333754705, 0.15021485084761135, -0.14922532048236964, 0.19910280750100984, -0.14017786331282095, -0.1562080011414043, 0.11042018033612262, 0.3284433186576092, -0.27391970014713446, -0.2753304178216334, 0.05364813630525344, -0.17636898127866202, -0.09021964462490045, 0.10914636902302376, -0.1303127744267213, ... |
708.4078 | Optomechanical trapping and cooling of partially transparent mirrors | We consider the radiative trapping and cooling of a partially transmitting
mirror suspended inside an optical cavity, generalizing the case of a perfectly
reflecting mirror previously considered [M. Bhattacharya and P. Meystre, Phys.
Rev. Lett. \textbf{99}, 073601 (2007)]. This configuration was recently used in
an e... | quant-ph | we consider the radiative trapping and cooling of a partially transmitting mirror suspended inside an optical cavity generalizing the case of a perfectly reflecting mirror previously considered m bhattacharya and p meystre phys rev lett textbf99 073601 2007 this configuration was recently used in an experiment to cool ... | [['we', 'consider', 'the', 'radiative', 'trapping', 'and', 'cooling', 'of', 'a', 'partially', 'transmitting', 'mirror', 'suspended', 'inside', 'an', 'optical', 'cavity', 'generalizing', 'the', 'case', 'of', 'a', 'perfectly', 'reflecting', 'mirror', 'previously', 'considered', 'm', 'bhattacharya', 'and', 'p', 'meystre',... | [-0.12017751869060239, 0.18248343287177132, -0.06812438749673091, -0.01542221460968795, -0.057856153755349186, -0.1633209828287363, 0.044448660461103205, 0.37687185983636284, -0.20655945911944942, -0.31751264491171205, 0.031572060592167966, -0.24558766375430538, -0.1195022508900308, 0.19052749072529562, -0.127098902773... |
708.4079 | GMRT Low Frequency Observations of Extrasolar Planetary Systems | Extrasolar planets are expected to emit detectable low frequency radio
emission. In this paper we present results from new low frequency observations
of two extrasolar planetary systems (Epsilon Eridani and HD 128311) taken at
150 MHz with the Giant Metrewave Radio Telescope (GMRT). These two systems have
been chosen... | astro-ph | extrasolar planets are expected to emit detectable low frequency radio emission in this paper we present results from new low frequency observations of two extrasolar planetary systems epsilon eridani and hd 128311 taken at 150 mhz with the giant metrewave radio telescope gmrt these two systems have been chosen because... | [['extrasolar', 'planets', 'are', 'expected', 'to', 'emit', 'detectable', 'low', 'frequency', 'radio', 'emission', 'in', 'this', 'paper', 'we', 'present', 'results', 'from', 'new', 'low', 'frequency', 'observations', 'of', 'two', 'extrasolar', 'planetary', 'systems', 'epsilon', 'eridani', 'and', 'hd', '128311', 'taken'... | [-0.12718103031089623, 0.1831741946960849, -0.017707253864781867, 0.09687040527553661, -0.15076981801179729, -0.09113686672605323, 0.09897713208793783, 0.4381770195286487, -0.12843535619828364, -0.35355001608368714, 0.1254712852267245, -0.28464012485501416, -0.07390833191870563, 0.256691462727565, -0.043725401115860194... |
708.408 | Computer simulated heat flow dynamics in Silicon at low temperatures | The thermal characteristics of silicon between 15 and 300 deg K are
investigated by applying a computer program on the solution of the differential
heat diffusion equation. The computer model is linked to high-purity silicon
through a set of experimental data. The numerical results are given in graphic
form and show,... | cond-mat.mtrl-sci cond-mat.other | the thermal characteristics of silicon between 15 and 300 deg k are investigated by applying a computer program on the solution of the differential heat diffusion equation the computer model is linked to highpurity silicon through a set of experimental data the numerical results are given in graphic form and show in pa... | [['the', 'thermal', 'characteristics', 'of', 'silicon', 'between', '15', 'and', '300', 'deg', 'k', 'are', 'investigated', 'by', 'applying', 'a', 'computer', 'program', 'on', 'the', 'solution', 'of', 'the', 'differential', 'heat', 'diffusion', 'equation', 'the', 'computer', 'model', 'is', 'linked', 'to', 'highpurity', '... | [-0.11048676977710177, 0.07706439319170183, -0.052240911948805056, -0.0005751027977870157, -0.0414979150518775, -0.1425558068181595, 0.016782119676160317, 0.40137628714243573, -0.26331379016240436, -0.3564160253542165, 0.10888463784229113, -0.33403268622027504, -0.09380899351607594, 0.2956228225666564, 0.01286050634613... |
708.4081 | A recursive online algorithm for the estimation of time-varying ARCH
parameters | In this paper we propose a recursive online algorithm for estimating the
parameters of a time-varying ARCH process. The estimation is done by updating
the estimator at time point $t-1$ with observations about the time point $t$ to
yield an estimator of the parameter at time point $t$. The sampling properties
of this ... | math.ST stat.TH | in this paper we propose a recursive online algorithm for estimating the parameters of a timevarying arch process the estimation is done by updating the estimator at time point t1 with observations about the time point t to yield an estimator of the parameter at time point t the sampling properties of this estimator ar... | [['in', 'this', 'paper', 'we', 'propose', 'a', 'recursive', 'online', 'algorithm', 'for', 'estimating', 'the', 'parameters', 'of', 'a', 'timevarying', 'arch', 'process', 'the', 'estimation', 'is', 'done', 'by', 'updating', 'the', 'estimator', 'at', 'time', 'point', 't1', 'with', 'observations', 'about', 'the', 'time', ... | [-0.09287921249868528, 0.06625602017549936, -0.10558701597415564, 0.05447861620104321, -0.023181872679280083, -0.13522012802167682, 0.0652969928158104, 0.40495837682433294, -0.28764812599279377, -0.3078486229979286, 0.15968379980410663, -0.21792089499598533, -0.11275856592896673, 0.19790815365941902, -0.066212946279464... |
708.4082 | Aides en ligne \`a l'utilisation de logiciels grand public : probl\`emes
sp\'ecifiques de conception et solutions potentielles | The observation that novice users seldom consult online help was made over
twenty years ago. This observation still holds nowadays, although online help
to the use of software for the general public has greatly improved in usability
during this period. The paper first demonstrates the necessity of online help
to the ... | cs.HC | the observation that novice users seldom consult online help was made over twenty years ago this observation still holds nowadays although online help to the use of software for the general public has greatly improved in usability during this period the paper first demonstrates the necessity of online help to the use o... | [['the', 'observation', 'that', 'novice', 'users', 'seldom', 'consult', 'online', 'help', 'was', 'made', 'over', 'twenty', 'years', 'ago', 'this', 'observation', 'still', 'holds', 'nowadays', 'although', 'online', 'help', 'to', 'the', 'use', 'of', 'software', 'for', 'the', 'general', 'public', 'has', 'greatly', 'improv... | [-0.07710035072461247, 0.016528129422287284, -0.06548606296812377, 0.09662857840823486, -0.18362677875569366, -0.16393450769704787, 0.07008299197595408, 0.3985842313503529, -0.252013835233656, -0.353668748193044, 0.1435689822141517, -0.25516552948814003, -0.17706887114253092, 0.20926817986517252, -0.10936113824681477, ... |
708.4083 | Metal Abundance Properties of M81 Globular Cluster System | This paper is the third in the series of papers on M81 globular clusters. In
this paper, we present spatial and metal abundance properties of 95 M81
globular clusters, which comprise nearly half of all the M81 globular cluster
system. These globular clusters are divided into two M81 metallicity groups by
a KMM test. ... | astro-ph | this paper is the third in the series of papers on m81 globular clusters in this paper we present spatial and metal abundance properties of 95 m81 globular clusters which comprise nearly half of all the m81 globular cluster system these globular clusters are divided into two m81 metallicity groups by a kmm test our res... | [['this', 'paper', 'is', 'the', 'third', 'in', 'the', 'series', 'of', 'papers', 'on', 'm81', 'globular', 'clusters', 'in', 'this', 'paper', 'we', 'present', 'spatial', 'and', 'metal', 'abundance', 'properties', 'of', '95', 'm81', 'globular', 'clusters', 'which', 'comprise', 'nearly', 'half', 'of', 'all', 'the', 'm81', ... | [-0.054632865151676514, 0.06579898540118517, -0.11514382446685914, 0.11158283092467858, -0.08740748976087907, -0.014165810024380922, 0.043646321618394934, 0.4646680784608016, -0.1409535407189973, -0.33315100597484965, -0.032452512466173304, -0.30920667378357175, -0.03046866401094492, 0.18496323680487406, -0.06646741632... |
708.4084 | High-Temperature Expansion of the Free Energy in the Two-Dimensional XY
Model | We extend the high-temperature series of the free energy for the XY model in
two dimensions to order $\beta^{48}$ from the previous order of $\beta^{22}$ by
applying the improved algorithm of the finite lattice method. The long series
obtained enables us to conclude that the behavior of the free energy is
consistent ... | cond-mat.stat-mech | we extend the hightemperature series of the free energy for the xy model in two dimensions to order beta48 from the previous order of beta22 by applying the improved algorithm of the finite lattice method the long series obtained enables us to conclude that the behavior of the free energy is consistent in high accuracy... | [['we', 'extend', 'the', 'hightemperature', 'series', 'of', 'the', 'free', 'energy', 'for', 'the', 'xy', 'model', 'in', 'two', 'dimensions', 'to', 'order', 'beta48', 'from', 'the', 'previous', 'order', 'of', 'beta22', 'by', 'applying', 'the', 'improved', 'algorithm', 'of', 'the', 'finite', 'lattice', 'method', 'the', '... | [-0.08224396647087165, 0.13475416212874863, -0.08642370382856046, 0.03375916530078809, -0.03339646277683122, -0.07659247570804187, 0.06063497319285359, 0.3512737878731319, -0.2570379557753248, -0.2869163928819554, 0.0779110802769927, -0.2856058884944235, -0.08902553695120982, 0.1852917821346117, -0.005351195032043117, ... |
708.4085 | Multiple Quantum NMR Dynamics in Dipolar Ordered Spin Systems | We investigate analytically and numerically the Multiple Quantum (MQ) NMR
dynamics in systems of nuclear spins 1/2 coupled by the dipole-dipole
interactions in the case of the dipolar ordered initial state. We suggest two
different methods of MQ NMR. One of them is based on the measurement of the
dipolar temperature ... | cond-mat.other | we investigate analytically and numerically the multiple quantum mq nmr dynamics in systems of nuclear spins 12 coupled by the dipoledipole interactions in the case of the dipolar ordered initial state we suggest two different methods of mq nmr one of them is based on the measurement of the dipolar temperature in the q... | [['we', 'investigate', 'analytically', 'and', 'numerically', 'the', 'multiple', 'quantum', 'mq', 'nmr', 'dynamics', 'in', 'systems', 'of', 'nuclear', 'spins', '12', 'coupled', 'by', 'the', 'dipoledipole', 'interactions', 'in', 'the', 'case', 'of', 'the', 'dipolar', 'ordered', 'initial', 'state', 'we', 'suggest', 'two',... | [-0.12585819169132362, 0.21617796311786586, -0.07660596804887687, 0.04912559349332313, 0.055199484423588005, -0.12288942233436118, -0.010820448972969816, 0.38084933325679093, -0.2367472954417679, -0.29382948223347505, 0.043701152845424376, -0.2916285224953543, -0.054003819423027274, 0.23764541976092277, 0.1038403743223... |
708.4086 | Non-Markovian hole spin kinetics in $p$-type GaAs quantum wells | Based on fully microscopic kinetic spin Bloch equation approach, we show the
non-Markovian effect in spin dephasing of heavy holes in $p$-type GaAs quantum
wells. The non-Markovian effect manifests itself in spin dephasing when the
mean spin precession time is shorter than the momentum relaxation time. The
spin depha... | cond-mat.mtrl-sci | based on fully microscopic kinetic spin bloch equation approach we show the nonmarkovian effect in spin dephasing of heavy holes in ptype gaas quantum wells the nonmarkovian effect manifests itself in spin dephasing when the mean spin precession time is shorter than the momentum relaxation time the spin dephasing becom... | [['based', 'on', 'fully', 'microscopic', 'kinetic', 'spin', 'bloch', 'equation', 'approach', 'we', 'show', 'the', 'nonmarkovian', 'effect', 'in', 'spin', 'dephasing', 'of', 'heavy', 'holes', 'in', 'ptype', 'gaas', 'quantum', 'wells', 'the', 'nonmarkovian', 'effect', 'manifests', 'itself', 'in', 'spin', 'dephasing', 'wh... | [-0.17676459660602584, 0.302096115337131, -0.06980172338316569, 0.100542672156243, -0.041325766895268415, -0.1909261814796844, -0.027191797491616092, 0.37363289387242216, -0.27788813807372303, -0.1999326628960065, -0.046633213844993526, -0.27354397803444314, -0.1015035555622465, 0.2627883850269624, 0.025879924890358705... |
708.4087 | Higher loop renormalization of fermion bilinear operators | We compute the two-loop renormalization functions, in the RI' scheme, of
local bilinear quark operators $\bar\psi\Gamma\psi$, where $\Gamma$ denotes the
Scalar and Pseudoscalar Dirac matrices, in the lattice formulation of QCD. We
consider both the flavor non-singlet and singlet operators; the latter, in the
scalar c... | hep-lat | we compute the twoloop renormalization functions in the ri scheme of local bilinear quark operators barpsigammapsi where gamma denotes the scalar and pseudoscalar dirac matrices in the lattice formulation of qcd we consider both the flavor nonsinglet and singlet operators the latter in the scalar case leads directly to... | [['we', 'compute', 'the', 'twoloop', 'renormalization', 'functions', 'in', 'the', 'ri', 'scheme', 'of', 'local', 'bilinear', 'quark', 'operators', 'barpsigammapsi', 'where', 'gamma', 'denotes', 'the', 'scalar', 'and', 'pseudoscalar', 'dirac', 'matrices', 'in', 'the', 'lattice', 'formulation', 'of', 'qcd', 'we', 'consid... | [-0.1270670029177406, 0.25151702785562424, -0.0662240371850596, 0.10673012211918831, -0.05189599872352807, -0.09681209133988297, 0.053944199285438484, 0.34312968840193303, -0.1670963221003075, -0.23448791700994243, 0.011511886096716783, -0.27303639669726426, -0.11844964919775422, 0.12185587353274427, 0.0420097699451788... |
708.4088 | $pp\to pp\pi^0$ near threshold in pionless effective field theory | In this talk, we review our recent calculation for the $pp\to pp\pi^0$
reaction near threshold in pionless effective field theory with a di-baryon and
external pions.
| nucl-th | in this talk we review our recent calculation for the ppto pppi0 reaction near threshold in pionless effective field theory with a dibaryon and external pions | [['in', 'this', 'talk', 'we', 'review', 'our', 'recent', 'calculation', 'for', 'the', 'ppto', 'pppi0', 'reaction', 'near', 'threshold', 'in', 'pionless', 'effective', 'field', 'theory', 'with', 'a', 'dibaryon', 'and', 'external', 'pions']] | [-0.08455243532975706, 0.23011740300661096, -0.08235054797282479, 0.07916288209917884, -0.005751484288619115, -0.08891181341515711, 0.06710560191333151, 0.3247450840157958, -0.10014847135887696, -0.22745799086987972, -0.11412739589846191, -0.3505971011920617, -0.15353830059309706, 0.0494416510919109, 0.0768571819465320... |
708.4089 | Measurement of B -> D*- tau+ nu and B -> h(*) nu nubar Decays at Belle | We report an observation of the decay B0 -> D*- tau+ nu and a search for the
rare decays B -> h(*) nu nubar\ove, where h(*) stands for a light meson. A data
sample of 535 million BBbar pairs collected with the Belle detector at the KEKB
e+e- collider is used. We find a signal with a significance of 5.2 standard
devia... | hep-ex | we report an observation of the decay b0 d tau nu and a search for the rare decays b h nu nubarove where h stands for a light meson a data sample of 535 million bbbar pairs collected with the belle detector at the kekb ee collider is used we find a signal with a significance of 52 standard deviations on b0 d tau nu and... | [['we', 'report', 'an', 'observation', 'of', 'the', 'decay', 'b0', 'd', 'tau', 'nu', 'and', 'a', 'search', 'for', 'the', 'rare', 'decays', 'b', 'h', 'nu', 'nubarove', 'where', 'h', 'stands', 'for', 'a', 'light', 'meson', 'a', 'data', 'sample', 'of', '535', 'million', 'bbbar', 'pairs', 'collected', 'with', 'the', 'belle... | [-0.12758509768351287, 0.2437050177243128, -0.009016485023153883, 0.06906918094645502, -0.06137229354900061, -0.22393560800764736, 0.21023807482759083, 0.2147082711512945, -0.16227579334763442, -0.2424141921381764, -0.04859330419444663, -0.47415139168805004, 0.1178280543868563, 0.17771865409754573, 0.14435555615468698,... |
708.409 | NMR method for amplification of single spin state | Amplification of a single spin state using nuclear magnetic resonance (NMR)
techniques in a rotating frame is considered. The main aim is to investigate
the efficient of various schemes for quantum detection. Results of numerical
simulation of the time dependence of individual and total nuclear polarizations
for one-... | quant-ph | amplification of a single spin state using nuclear magnetic resonance nmr techniques in a rotating frame is considered the main aim is to investigate the efficient of various schemes for quantum detection results of numerical simulation of the time dependence of individual and total nuclear polarizations for one two an... | [['amplification', 'of', 'a', 'single', 'spin', 'state', 'using', 'nuclear', 'magnetic', 'resonance', 'nmr', 'techniques', 'in', 'a', 'rotating', 'frame', 'is', 'considered', 'the', 'main', 'aim', 'is', 'to', 'investigate', 'the', 'efficient', 'of', 'various', 'schemes', 'for', 'quantum', 'detection', 'results', 'of', ... | [-0.1712919089397223, 0.1248392969578633, -0.04965291872263308, 0.05312908227667855, 0.0030902652712217695, -0.10129616669668205, -0.02680743089475637, 0.3791907049458602, -0.2190589324394562, -0.2926172175091402, 0.08034725337096586, -0.24100359551737022, -0.05450418226998942, 0.26471402931251914, 0.0643306039675171, ... |
708.4091 | Non-Abelian Global Strings at Chiral Phase Transition | We construct non-Abelian global string solutions in the U(N)_L x U(N)_R
linear sigma model. These strings are the most fundamental objects which are
expected to form during the chiral phase transitions, because the Abelian eta'
string is marginally decomposed into N of them. We point out Nambu-Goldstone
modes of CP^{... | hep-ph astro-ph hep-th nucl-th | we construct nonabelian global string solutions in the un_l x un_r linear sigma model these strings are the most fundamental objects which are expected to form during the chiral phase transitions because the abelian eta string is marginally decomposed into n of them we point out nambugoldstone modes of cpn1 for breakin... | [['we', 'construct', 'nonabelian', 'global', 'string', 'solutions', 'in', 'the', 'un_l', 'x', 'un_r', 'linear', 'sigma', 'model', 'these', 'strings', 'are', 'the', 'most', 'fundamental', 'objects', 'which', 'are', 'expected', 'to', 'form', 'during', 'the', 'chiral', 'phase', 'transitions', 'because', 'the', 'abelian', ... | [-0.20376899954862893, 0.2557544364660446, -0.07033108981392745, 0.10377190722127645, -0.08396662904747895, -0.13456400065583043, 0.031023516186646054, 0.32035230692209943, -0.24831070863417284, -0.2173408553270357, 0.0848992488775236, -0.2818476671153413, -0.12198112882158187, 0.09494026360750597, 0.009879327927982169... |
708.4092 | Interactions of Non-Abelian Global Strings | Non-Abelian global strings are expected to form during the chiral phase
transition. They have orientational zero modes in the internal space,
associated with the vector-like symmetry SU(N)_{L+R} broken in the presence of
strings. The interaction among two parallel non-Abelian global strings is
derived for general rel... | hep-ph astro-ph hep-th nucl-th | nonabelian global strings are expected to form during the chiral phase transition they have orientational zero modes in the internal space associated with the vectorlike symmetry sun_lr broken in the presence of strings the interaction among two parallel nonabelian global strings is derived for general relative orienta... | [['nonabelian', 'global', 'strings', 'are', 'expected', 'to', 'form', 'during', 'the', 'chiral', 'phase', 'transition', 'they', 'have', 'orientational', 'zero', 'modes', 'in', 'the', 'internal', 'space', 'associated', 'with', 'the', 'vectorlike', 'symmetry', 'sun_lr', 'broken', 'in', 'the', 'presence', 'of', 'strings',... | [-0.21494912299034508, 0.26790240899948725, -0.06542092253020483, 0.1059098858135383, -0.06648168235952998, -0.1089350081988257, 0.008400312468313194, 0.32044298217856676, -0.25983825176633124, -0.2636276634474253, 0.04478127113543451, -0.27328694330785297, -0.09809842363706436, 0.10229501127393852, -0.0026725930531091... |
708.4093 | Limiting distributions of curves under geodesic flow on hyperbolic
manifolds | We consider the evolution of a compact segment of an analytic curve on the
unit tangent bundle of a finite volume hyperbolic $n$-manifold under the
geodesic flow. Suppose that the curve is not contained in a stable leaf of the
flow. It is shown that under the geodesic flow, the normalized parameter
measure on the cur... | math.DG math.RT | we consider the evolution of a compact segment of an analytic curve on the unit tangent bundle of a finite volume hyperbolic nmanifold under the geodesic flow suppose that the curve is not contained in a stable leaf of the flow it is shown that under the geodesic flow the normalized parameter measure on the curve gets ... | [['we', 'consider', 'the', 'evolution', 'of', 'a', 'compact', 'segment', 'of', 'an', 'analytic', 'curve', 'on', 'the', 'unit', 'tangent', 'bundle', 'of', 'a', 'finite', 'volume', 'hyperbolic', 'nmanifold', 'under', 'the', 'geodesic', 'flow', 'suppose', 'that', 'the', 'curve', 'is', 'not', 'contained', 'in', 'a', 'stabl... | [-0.20778637028945637, 0.08654538996124395, -0.12837430083225318, 0.01018190715781677, -0.10440584006186444, -0.11590117575260185, -0.01190881107109066, 0.3670941529545321, -0.31481437726103845, -0.11286738158646155, 0.13164226702745743, -0.2945557157022517, -0.09375449512570874, 0.19768262353368957, -0.188369076360776... |
708.4094 | A note on the measurement of phase space observables with an eight-port
homodyne detector | It is well known that the Husimi Q-function of the signal field can actually
be measured by the eight-port homodyne detection technique, provided that the
reference beam (used for homodyne detection) is a very strong coherent field so
that it can be treated classically. Using recent rigorous results on the
quantum th... | quant-ph | it is well known that the husimi qfunction of the signal field can actually be measured by the eightport homodyne detection technique provided that the reference beam used for homodyne detection is a very strong coherent field so that it can be treated classically using recent rigorous results on the quantum theory of ... | [['it', 'is', 'well', 'known', 'that', 'the', 'husimi', 'qfunction', 'of', 'the', 'signal', 'field', 'can', 'actually', 'be', 'measured', 'by', 'the', 'eightport', 'homodyne', 'detection', 'technique', 'provided', 'that', 'the', 'reference', 'beam', 'used', 'for', 'homodyne', 'detection', 'is', 'a', 'very', 'strong', '... | [-0.10468485063341047, 0.16431934952071264, -0.14983781780667452, 0.09046872510997654, -0.04293706644402475, -0.17512136767143194, 0.03515234446195809, 0.38709127768037876, -0.23844198061970576, -0.27062908491613913, 0.09547163260511446, -0.21617794172762303, -0.1601917779367721, 0.267917943146669, -0.06034266505371399... |
708.4095 | $L^2$-approximating pricing under restricted information | We consider the mean-variance hedging problem under partial information in
the case where the flow of observable events does not contain the full
information on the underlying asset price process. We introduce a martingale
equation of a new type and characterize the optimal strategy in terms of the
solution of this e... | q-fin.PR math.PR | we consider the meanvariance hedging problem under partial information in the case where the flow of observable events does not contain the full information on the underlying asset price process we introduce a martingale equation of a new type and characterize the optimal strategy in terms of the solution of this equat... | [['we', 'consider', 'the', 'meanvariance', 'hedging', 'problem', 'under', 'partial', 'information', 'in', 'the', 'case', 'where', 'the', 'flow', 'of', 'observable', 'events', 'does', 'not', 'contain', 'the', 'full', 'information', 'on', 'the', 'underlying', 'asset', 'price', 'process', 'we', 'introduce', 'a', 'martinga... | [-0.12269887726620904, 0.003734879954052823, -0.11182913020519274, 0.11721833092020201, -0.1239966127023633, -0.08440553661701934, 0.08612133700932775, 0.3110851666224854, -0.3666569700198514, -0.2340608880855143, 0.1602515657731731, -0.2837654422436442, -0.14880835602858236, 0.1516492435708642, -0.11521782792572464, 0... |
708.4096 | Non-Abelian Strings in High Density QCD: Zero Modes and Interactions | The most fundamental strings in high density color superconductivity are the
non-Abelian semi-superfluid strings which have color gauge flux tube but behave
as superfluid vortices in the energetic point of view. We show that in addition
to the usual translational zero modes, these vortices have normalizable
orientati... | hep-ph astro-ph cond-mat.supr-con hep-th nucl-th | the most fundamental strings in high density color superconductivity are the nonabelian semisuperfluid strings which have color gauge flux tube but behave as superfluid vortices in the energetic point of view we show that in addition to the usual translational zero modes these vortices have normalizable orientational z... | [['the', 'most', 'fundamental', 'strings', 'in', 'high', 'density', 'color', 'superconductivity', 'are', 'the', 'nonabelian', 'semisuperfluid', 'strings', 'which', 'have', 'color', 'gauge', 'flux', 'tube', 'but', 'behave', 'as', 'superfluid', 'vortices', 'in', 'the', 'energetic', 'point', 'of', 'view', 'we', 'show', 't... | [-0.2195610082496635, 0.333955571463347, -0.07977200903321717, 0.09828971654238287, -0.045771566519806205, -0.11994385751626216, 0.00491367990905342, 0.34950409189236065, -0.22535094634672118, -0.2588814771849631, 0.015860865696926008, -0.24568873703141103, -0.07995418845560433, 0.04467417238557265, -0.0337135706189250... |
708.4097 | On dynamical smash product | In the theory of dynamical Yang-Baxter equation, with any Hopf algebra $H$
and a certain $H$-module and $H$-comodule algebra $L$ (base algebra) one
associates a monoidal category. Given an algebra $A$ in that category, one can
construct an associative algebra $A\rtimes L$, which is a generalization of the
ordinary sm... | math.QA math.RA | in the theory of dynamical yangbaxter equation with any hopf algebra h and a certain hmodule and hcomodule algebra l base algebra one associates a monoidal category given an algebra a in that category one can construct an associative algebra artimes l which is a generalization of the ordinary smash product when a is an... | [['in', 'the', 'theory', 'of', 'dynamical', 'yangbaxter', 'equation', 'with', 'any', 'hopf', 'algebra', 'h', 'and', 'a', 'certain', 'hmodule', 'and', 'hcomodule', 'algebra', 'l', 'base', 'algebra', 'one', 'associates', 'a', 'monoidal', 'category', 'given', 'an', 'algebra', 'a', 'in', 'that', 'category', 'one', 'can', '... | [-0.18507425423347573, 0.031162960246745926, -0.07667640217676244, 0.03711250230225724, -0.15940893906029477, -0.15307657343827874, -0.07959091240117305, 0.3141097468778962, -0.4775215509593829, -0.1406215731825294, 0.12353094182400054, -0.22773402959279632, -0.14927395102139776, 0.14474367938036548, -0.158898519576880... |
708.4098 | Hybrid Curvatons from Broken Symmetry | We present a new general mechanism for generating curvature perturbations
after inflation. Our model is based on the simple assumption that a field that
starts to oscillate after inflation has a potential characterized by an
underlying global symmetry that is slightly or badly broken. Inhomogeneous
preheating occurs ... | hep-ph astro-ph hep-th | we present a new general mechanism for generating curvature perturbations after inflation our model is based on the simple assumption that a field that starts to oscillate after inflation has a potential characterized by an underlying global symmetry that is slightly or badly broken inhomogeneous preheating occurs due ... | [['we', 'present', 'a', 'new', 'general', 'mechanism', 'for', 'generating', 'curvature', 'perturbations', 'after', 'inflation', 'our', 'model', 'is', 'based', 'on', 'the', 'simple', 'assumption', 'that', 'a', 'field', 'that', 'starts', 'to', 'oscillate', 'after', 'inflation', 'has', 'a', 'potential', 'characterized', '... | [-0.1668280426367018, 0.23253956140371107, -0.10116109452100631, 0.11770179700492843, -0.11380208203507984, -0.17574397115739154, -0.04942881942490024, 0.3205680004244701, -0.2365691924055458, -0.23800600855992954, 0.10672212203346254, -0.202301225818686, -0.15693517670905616, 0.12519539270328633, -0.004853623835217269... |
708.4099 | Protected nodes and the collapse of the Fermi arcs in high Tc cuprates | Angle resolved photoemission on underdoped Bi2Sr2CaCu2O8 reveals that the
magnitude and d-wave anisotropy of the superconducting state energy gap are
independent of temperature all the way up to Tc. This lack of T variation of
the entire k-dependent gap is in marked contrast to mean field theory. At Tc
the point node... | cond-mat.supr-con cond-mat.str-el | angle resolved photoemission on underdoped bi2sr2cacu2o8 reveals that the magnitude and dwave anisotropy of the superconducting state energy gap are independent of temperature all the way up to tc this lack of t variation of the entire kdependent gap is in marked contrast to mean field theory at tc the point nodes of t... | [['angle', 'resolved', 'photoemission', 'on', 'underdoped', 'bi2sr2cacu2o8', 'reveals', 'that', 'the', 'magnitude', 'and', 'dwave', 'anisotropy', 'of', 'the', 'superconducting', 'state', 'energy', 'gap', 'are', 'independent', 'of', 'temperature', 'all', 'the', 'way', 'up', 'to', 'tc', 'this', 'lack', 'of', 't', 'variat... | [-0.22776831172016118, 0.2479879722457319, -0.06371475150057625, 0.018491460750209947, -0.08142368342747451, -0.12118179346584985, 0.18669995424583033, 0.37392206768435177, -0.3050016964815797, -0.30231220664716857, -0.04628524369677849, -0.34642879304385954, -0.032403159626228834, 0.13347109868153628, 0.03234948129493... |
708.41 | Specific heat of the mixed spin-1/2 and spin-S Ising model with a rope
ladder structure | The mixed spin-1/2 and spin-S (S>1/2) Ising model on a rope ladder is
examined by combining two exact analytical methods. By the decoration-iteration
mapping transformation, this mixed-spin system is firstly transformed to a
simple spin-1/2 Ising model on the two-leg ladder, which is then exactly solved
by the standa... | cond-mat.stat-mech cond-mat.mtrl-sci | the mixed spin12 and spins s12 ising model on a rope ladder is examined by combining two exact analytical methods by the decorationiteration mapping transformation this mixedspin system is firstly transformed to a simple spin12 ising model on the twoleg ladder which is then exactly solved by the standard transfermatrix... | [['the', 'mixed', 'spin12', 'and', 'spins', 's12', 'ising', 'model', 'on', 'a', 'rope', 'ladder', 'is', 'examined', 'by', 'combining', 'two', 'exact', 'analytical', 'methods', 'by', 'the', 'decorationiteration', 'mapping', 'transformation', 'this', 'mixedspin', 'system', 'is', 'firstly', 'transformed', 'to', 'a', 'simp... | [-0.11494052937136047, 0.1624228148203757, 0.018331486288280713, 0.08727533781590562, -0.057417560797480366, -0.23459148982037153, 0.004851276882820659, 0.4122368913912584, -0.24052882910011306, -0.220701115420236, 0.09695347268984372, -0.3094042505152405, -0.10055814687872217, 0.17387663090365038, 0.1064219619664881, ... |
708.4101 | General quantum phase estimation and calibration of a timepiece in a
quantum dot system | We present a physical scheme for implementing quantum phase estimation via
weakly coupled double quantum-dot molecules embedded in a microcavity. During
the same process of implementation, we can also realize the calibration of a
timepiece based on the estimated phase. We use the electron-hole pair states in
coupled ... | quant-ph | we present a physical scheme for implementing quantum phase estimation via weakly coupled double quantumdot molecules embedded in a microcavity during the same process of implementation we can also realize the calibration of a timepiece based on the estimated phase we use the electronhole pair states in coupled double ... | [['we', 'present', 'a', 'physical', 'scheme', 'for', 'implementing', 'quantum', 'phase', 'estimation', 'via', 'weakly', 'coupled', 'double', 'quantumdot', 'molecules', 'embedded', 'in', 'a', 'microcavity', 'during', 'the', 'same', 'process', 'of', 'implementation', 'we', 'can', 'also', 'realize', 'the', 'calibration', ... | [-0.11832193585441393, 0.2029120730893577, -0.041073062166105956, 0.015853307947541265, -0.0005268246017615585, -0.23521868703229462, 0.026701044288518674, 0.40169248052817935, -0.2657525132465012, -0.25423207223853644, 0.04272597272442106, -0.2446917969678693, -0.1495415275587755, 0.22620789960355442, -0.0085647516130... |
708.4102 | The spin-1/2 Ising model on the bow-tie lattice as an exactly soluble
free-fermion model | The spin-1/2 Ising model on the bow-tie lattice is exactly solved by
establishing a precise mapping relationship with its corresponding free-fermion
eight-vertex model. Ground-state and finite-temperature phase diagrams are
obtained for the anisotropic bow-tie lattice with three different exchange
interactions along ... | cond-mat.stat-mech | the spin12 ising model on the bowtie lattice is exactly solved by establishing a precise mapping relationship with its corresponding freefermion eightvertex model groundstate and finitetemperature phase diagrams are obtained for the anisotropic bowtie lattice with three different exchange interactions along three diffe... | [['the', 'spin12', 'ising', 'model', 'on', 'the', 'bowtie', 'lattice', 'is', 'exactly', 'solved', 'by', 'establishing', 'a', 'precise', 'mapping', 'relationship', 'with', 'its', 'corresponding', 'freefermion', 'eightvertex', 'model', 'groundstate', 'and', 'finitetemperature', 'phase', 'diagrams', 'are', 'obtained', 'fo... | [-0.16745185483660963, 0.19687099950646775, 0.012670149544202204, 0.06896380088033362, -0.0578271116130054, -0.265416670549247, -0.0065108769883712135, 0.4892211331261529, -0.24685511451421513, -0.2573763466854062, 0.059086202540331416, -0.3232370620386468, -0.11267040005574623, 0.11058043617134293, 0.20037215921199983... |
708.4103 | Reentrant transitions of Ising-Heisenberg ferromagnet on a triangular
lattice with diamond-like decorations | The mixed spin-1/2 and spin-1 Ising-Heisenberg ferromagnet on the decorated
triangular lattice consisting of inter-connected diamonds is investigated
within the framework of an exact decoration-iteration mapping transformation.
It is shown that the diamond-like decoration by a couple of the Heisenberg
spins gives ris... | cond-mat.stat-mech | the mixed spin12 and spin1 isingheisenberg ferromagnet on the decorated triangular lattice consisting of interconnected diamonds is investigated within the framework of an exact decorationiteration mapping transformation it is shown that the diamondlike decoration by a couple of the heisenberg spins gives rise to a div... | [['the', 'mixed', 'spin12', 'and', 'spin1', 'isingheisenberg', 'ferromagnet', 'on', 'the', 'decorated', 'triangular', 'lattice', 'consisting', 'of', 'interconnected', 'diamonds', 'is', 'investigated', 'within', 'the', 'framework', 'of', 'an', 'exact', 'decorationiteration', 'mapping', 'transformation', 'it', 'is', 'sho... | [-0.17972568889646873, 0.2244696186862073, -0.015105136817223147, 0.006968760066420624, -0.03467503920393555, -0.19270236546729216, 0.024571600018820743, 0.38679966506989377, -0.23951020931596295, -0.22659935574700826, 0.04269162306088235, -0.34320940139393014, -0.13482687958891978, 0.13840681941885696, 0.0844784183386... |
708.4104 | Wavelet block thresholding for samples with random design: a minimax
approach under the $L^p$ risk | We consider the regression model with (known) random design. We investigate
the minimax performances of an adaptive wavelet block thresholding estimator
under the $\mathbb{L}^p$ risk with $p\ge 2$ over Besov balls. We prove that it
is near optimal and that it achieves better rates of convergence than the
conventional... | math.ST stat.TH | we consider the regression model with known random design we investigate the minimax performances of an adaptive wavelet block thresholding estimator under the mathbblp risk with pge 2 over besov balls we prove that it is near optimal and that it achieves better rates of convergence than the conventional termbyterm est... | [['we', 'consider', 'the', 'regression', 'model', 'with', 'known', 'random', 'design', 'we', 'investigate', 'the', 'minimax', 'performances', 'of', 'an', 'adaptive', 'wavelet', 'block', 'thresholding', 'estimator', 'under', 'the', 'mathbblp', 'risk', 'with', 'pge', '2', 'over', 'besov', 'balls', 'we', 'prove', 'that', ... | [-0.04992836541584078, 0.0012106049022272687, -0.11593618948574898, 0.12166436846183508, -0.010988383470454588, -0.20563815409352756, 0.028372558624536363, 0.4785138649760552, -0.27397614274665993, -0.18503788204969102, 0.1874044827572158, -0.2652049767345471, -0.19563379890795024, 0.19481776237821663, -0.1816131241514... |
708.4105 | Ground-state phase diagram of geometrically frustrated Ising-Heisenberg
model on doubly decorated planar lattices | Ground-state phase diagram of the mixed spin-1/2 and spin-1 Ising-Heisenberg
model on doubly decorated planar lattices is examined using the generalized
decoration-iteration transformation. The main attention is devoted to the
comparison of the ground-state properties of the quantum Ising-Heisenberg model
and its sem... | cond-mat.stat-mech | groundstate phase diagram of the mixed spin12 and spin1 isingheisenberg model on doubly decorated planar lattices is examined using the generalized decorationiteration transformation the main attention is devoted to the comparison of the groundstate properties of the quantum isingheisenberg model and its semiclassical ... | [['groundstate', 'phase', 'diagram', 'of', 'the', 'mixed', 'spin12', 'and', 'spin1', 'isingheisenberg', 'model', 'on', 'doubly', 'decorated', 'planar', 'lattices', 'is', 'examined', 'using', 'the', 'generalized', 'decorationiteration', 'transformation', 'the', 'main', 'attention', 'is', 'devoted', 'to', 'the', 'compari... | [-0.11440226073480314, 0.164699137231542, -0.03377006851757566, 0.09959905905545585, -0.06302432641386986, -0.1880001727802058, 0.013891353639256624, 0.3940104062358538, -0.21968760366241138, -0.1654212946848323, 0.037558046562804114, -0.3161125156407555, -0.13004084291557472, 0.10976775693189766, 0.0784074509723319, 0... |
708.4106 | Biexciton stability in carbon nanotubes | We have applied the quantum Monte Carlo method and tight-binding modelling to
calculate the binding energy of biexcitons in semiconductor carbon nanotubes
for a wide range of diameters and chiralities. For typical nanotube diameters
we find that biexciton binding energies are much larger than previously
predicted fro... | cond-mat.mtrl-sci | we have applied the quantum monte carlo method and tightbinding modelling to calculate the binding energy of biexcitons in semiconductor carbon nanotubes for a wide range of diameters and chiralities for typical nanotube diameters we find that biexciton binding energies are much larger than previously predicted from va... | [['we', 'have', 'applied', 'the', 'quantum', 'monte', 'carlo', 'method', 'and', 'tightbinding', 'modelling', 'to', 'calculate', 'the', 'binding', 'energy', 'of', 'biexcitons', 'in', 'semiconductor', 'carbon', 'nanotubes', 'for', 'a', 'wide', 'range', 'of', 'diameters', 'and', 'chiralities', 'for', 'typical', 'nanotube'... | [-0.02186210940546188, 0.22153579767365925, -0.01093414198362925, 0.1293823675664722, 0.030508632374713657, -0.19283958670270981, 0.07166691298107998, 0.5209366091084285, -0.20993287475840722, -0.38901737735408254, -0.09942241893417095, -0.2796936086302654, -0.03326212761534347, 0.26448628198752394, 0.08578652204548726... |
708.4107 | The variable mass loss of the AGB star WX Psc as traced by the CO J=1-0
through 7-6 lines and the dust emission | Low and intermediate mass stars lose a significant fraction of their mass
through a dust-driven wind during the Asymptotic Giant Branch (AGB) phase.
Recent studies show that winds from late-type stars are far from being smooth.
Mass-loss variations occur on different time scales, from years to tens of
thousands of ye... | astro-ph | low and intermediate mass stars lose a significant fraction of their mass through a dustdriven wind during the asymptotic giant branch agb phase recent studies show that winds from latetype stars are far from being smooth massloss variations occur on different time scales from years to tens of thousands of years the va... | [['low', 'and', 'intermediate', 'mass', 'stars', 'lose', 'a', 'significant', 'fraction', 'of', 'their', 'mass', 'through', 'a', 'dustdriven', 'wind', 'during', 'the', 'asymptotic', 'giant', 'branch', 'agb', 'phase', 'recent', 'studies', 'show', 'that', 'winds', 'from', 'latetype', 'stars', 'are', 'far', 'from', 'being'... | [-0.07682339853799348, 0.11569513108965972, -0.06688141420291359, 0.07926086134739631, -0.06901253618174018, -0.03425160305594422, 0.08124963566909454, 0.4611377444903754, -0.2004896591678908, -0.3393799899861853, 0.12933834853459455, -0.2500619638058294, -0.03204820590802995, 0.1818292290392809, -0.05296268166872401, ... |
708.4108 | Polynomial identities and noncommutative versal torsors | To any cleft Hopf Galois object, i.e., any algebra H[t] obtained from a Hopf
algebra H by twisting its multiplication with a two-cocycle t, we attach two
"universal algebras" A(H,t) and U(H,t). The algebra A(H,t) is obtained by
twisting the multiplication of H with the most general two-cocycle u formally
cohomologous... | math.QA math.RA | to any cleft hopf galois object ie any algebra ht obtained from a hopf algebra h by twisting its multiplication with a twococycle t we attach two universal algebras aht and uht the algebra aht is obtained by twisting the multiplication of h with the most general twococycle u formally cohomologous to t the cocycle u tak... | [['to', 'any', 'cleft', 'hopf', 'galois', 'object', 'ie', 'any', 'algebra', 'ht', 'obtained', 'from', 'a', 'hopf', 'algebra', 'h', 'by', 'twisting', 'its', 'multiplication', 'with', 'a', 'twococycle', 't', 'we', 'attach', 'two', 'universal', 'algebras', 'aht', 'and', 'uht', 'the', 'algebra', 'aht', 'is', 'obtained', 'b... | [-0.16731382135157158, 0.07960765876600155, -0.09324704200816024, 0.0420295764854318, -0.14752577222404478, -0.18756193538802196, -0.037272928894646645, 0.3464654537722541, -0.40055293452901114, -0.13799594436066895, 0.13236789857444253, -0.21053888268745619, -0.1451181565485985, 0.1922386692231069, -0.1188231671293428... |
708.4109 | Finite temperature quantum field theory on non compact domains and
application to delta interactionsinteractions in three dimensions | We use relative zeta functions technique of W. Muller \cite{Mul} to extend
the classical decomposition of the zeta regularized partition function of a
finite temperature quantum field theory on a ultrastatic space-time with
compact spatial section to the case of non compact spatial section. As an
application, we stud... | math-ph hep-th math.MP | we use relative zeta functions technique of w muller citemul to extend the classical decomposition of the zeta regularized partition function of a finite temperature quantum field theory on a ultrastatic spacetime with compact spatial section to the case of non compact spatial section as an application we study the cas... | [['we', 'use', 'relative', 'zeta', 'functions', 'technique', 'of', 'w', 'muller', 'citemul', 'to', 'extend', 'the', 'classical', 'decomposition', 'of', 'the', 'zeta', 'regularized', 'partition', 'function', 'of', 'a', 'finite', 'temperature', 'quantum', 'field', 'theory', 'on', 'a', 'ultrastatic', 'spacetime', 'with', ... | [-0.1112938404767192, 0.07677972645910813, -0.08744545851368457, 0.07069336315908004, -0.05485553975813673, -0.11316942614212167, -0.000765367656640592, 0.32622836987138726, -0.2341304120782297, -0.23602274629229214, 0.05673881034454098, -0.24946744955377653, -0.14664224907755852, 0.19682121553341858, -0.03688950881769... |
708.411 | The effect of a planet on the dust distribution in a 3D protoplanetary
disk | Aims: We investigate the behaviour of dust in protoplanetary disks under the
action of gas drag in the presence of a planet. Our goal is twofold: to
determine the spatial distribution of dust depending on grain size and planet
mass, and therefore to provide a framework for interpretation of coming
observations and fu... | astro-ph | aims we investigate the behaviour of dust in protoplanetary disks under the action of gas drag in the presence of a planet our goal is twofold to determine the spatial distribution of dust depending on grain size and planet mass and therefore to provide a framework for interpretation of coming observations and future s... | [['aims', 'we', 'investigate', 'the', 'behaviour', 'of', 'dust', 'in', 'protoplanetary', 'disks', 'under', 'the', 'action', 'of', 'gas', 'drag', 'in', 'the', 'presence', 'of', 'a', 'planet', 'our', 'goal', 'is', 'twofold', 'to', 'determine', 'the', 'spatial', 'distribution', 'of', 'dust', 'depending', 'on', 'grain', 's... | [-0.09032467972488956, 0.1179213048786135, -0.08027191198123355, 0.03793328136339965, -0.037734073692276965, -0.024045315424629142, -0.005497708280957984, 0.3547855745538832, -0.22153283216317327, -0.3327707093338088, 0.0776905258555028, -0.21399689075442846, -0.06724388935613666, 0.1550699888797449, -0.059041662900451... |
708.4111 | Full Spectrum Diffused and Beamed Solar Energy Application Using Optical
Fibre | Existing solar energy application systems use small fraction of full spectrum
of solar energy. So attempts are made to show how full spectrum solar energy
can be used for diffused and beamed form of incident solar energy. Luminescent
Solar Concentrator (LSC) principle with optical fibre in diffused sun light and
diel... | physics.optics physics.soc-ph | existing solar energy application systems use small fraction of full spectrum of solar energy so attempts are made to show how full spectrum solar energy can be used for diffused and beamed form of incident solar energy luminescent solar concentrator lsc principle with optical fibre in diffused sun light and dielectric... | [['existing', 'solar', 'energy', 'application', 'systems', 'use', 'small', 'fraction', 'of', 'full', 'spectrum', 'of', 'solar', 'energy', 'so', 'attempts', 'are', 'made', 'to', 'show', 'how', 'full', 'spectrum', 'solar', 'energy', 'can', 'be', 'used', 'for', 'diffused', 'and', 'beamed', 'form', 'of', 'incident', 'solar... | [-0.10848622770741755, 0.22343049387902367, 0.041533402584697565, 0.0668541583405851, -0.0926493709950253, -0.12069200109257254, -0.04103725627172998, 0.4671603671686594, -0.215792472847889, -0.35934591301998425, 0.019150826358507105, -0.25346507754739983, -0.08477185003805993, 0.2985053505142068, -0.07724825690668292,... |
708.4112 | Phase coherence and extreme self phase modulation | I study how pulse to pulse phase coherence in a pulse train can survive
super-broadening by extreme self phase modulation (SPM). Such pulse trains have
been used in phase self-stabilizing schemes as an alternative to using a
feedback process. However, such super-broadened pulses have undergone
considerable distortion... | physics.optics | i study how pulse to pulse phase coherence in a pulse train can survive superbroadening by extreme self phase modulation spm such pulse trains have been used in phase selfstabilizing schemes as an alternative to using a feedback process however such superbroadened pulses have undergone considerable distortion and it is... | [['i', 'study', 'how', 'pulse', 'to', 'pulse', 'phase', 'coherence', 'in', 'a', 'pulse', 'train', 'can', 'survive', 'superbroadening', 'by', 'extreme', 'self', 'phase', 'modulation', 'spm', 'such', 'pulse', 'trains', 'have', 'been', 'used', 'in', 'phase', 'selfstabilizing', 'schemes', 'as', 'an', 'alternative', 'to', '... | [-0.11191409172689808, 0.1730875544476259, -0.1362622460472353, 0.10918382735354455, -0.06524668342345172, -0.18042077258273603, 0.04243134706103731, 0.5603173244744539, -0.2581845285548341, -0.25803690014540087, 0.12201488114217118, -0.23765860561425575, -0.13770855924147846, 0.198974929195607, -0.08721555867980767, 0... |
708.4113 | Conoscopic Patterns for Optically Uniaxial Gyrotropic Crystals in the
Vicinity of Isotropic Point | We have presented computer simulations of conoscopic patterns occurring in
optically uniaxial gyrotropic crystals in the vicinity of isotropic point for a
number of sets of crystal parameters and orientations. The appearance of
special directions characterized by equalization of linear and circular
birefringences has... | physics.optics | we have presented computer simulations of conoscopic patterns occurring in optically uniaxial gyrotropic crystals in the vicinity of isotropic point for a number of sets of crystal parameters and orientations the appearance of special directions characterized by equalization of linear and circular birefringences has be... | [['we', 'have', 'presented', 'computer', 'simulations', 'of', 'conoscopic', 'patterns', 'occurring', 'in', 'optically', 'uniaxial', 'gyrotropic', 'crystals', 'in', 'the', 'vicinity', 'of', 'isotropic', 'point', 'for', 'a', 'number', 'of', 'sets', 'of', 'crystal', 'parameters', 'and', 'orientations', 'the', 'appearance'... | [-0.19341583476077928, 0.15488036527581836, -0.0365405296167469, -0.08111448213458061, -0.038813673526696534, -0.09564401370311237, -0.0069473093001009975, 0.45413742578871874, -0.24434687027140803, -0.27458783614692156, 0.07131483353694658, -0.2636645896329909, -0.14011819308380719, 0.20493544866938307, 0.035358466086... |
708.4114 | Group theoretical construction of mutually unbiased bases in Hilbert
spaces of prime dimensions | Mutually unbiased bases in Hilbert spaces of finite dimensions are closely
related to the quantal notion of complementarity. An alternative proof of
existence of a maximal collection of N+1 mutually unbiased bases in Hilbert
spaces of prime dimension N is given by exploiting the finite Heisenberg group
(also called t... | quant-ph | mutually unbiased bases in hilbert spaces of finite dimensions are closely related to the quantal notion of complementarity an alternative proof of existence of a maximal collection of n1 mutually unbiased bases in hilbert spaces of prime dimension n is given by exploiting the finite heisenberg group also called the pa... | [['mutually', 'unbiased', 'bases', 'in', 'hilbert', 'spaces', 'of', 'finite', 'dimensions', 'are', 'closely', 'related', 'to', 'the', 'quantal', 'notion', 'of', 'complementarity', 'an', 'alternative', 'proof', 'of', 'existence', 'of', 'a', 'maximal', 'collection', 'of', 'n1', 'mutually', 'unbiased', 'bases', 'in', 'hil... | [-0.1863971259607392, 0.22451210816997932, -0.06619710898751713, 0.05715986005393355, -0.05268951432595333, -0.10621138597123844, 0.0027558810218388952, 0.3219916882253317, -0.2589846888643711, -0.13661713579799548, 0.1008567496211008, -0.24365174148751553, -0.0925989112800507, 0.17441693645750367, -0.09260061844576929... |
708.4115 | Thermal and Chemical Freeze-out in Spectator Fragmentation | Isotope temperatures from double ratios of hydrogen, helium, lithium,
beryllium, and carbon isotopic yields, and excited-state temperatures from
yield ratios of particle-unstable resonances in 4He, 5Li, and 8Be, were
determined for spectator fragmentation, following collisions of 197Au with
targets ranging from C to ... | nucl-ex | isotope temperatures from double ratios of hydrogen helium lithium beryllium and carbon isotopic yields and excitedstate temperatures from yield ratios of particleunstable resonances in 4he 5li and 8be were determined for spectator fragmentation following collisions of 197au with targets ranging from c to au at inciden... | [['isotope', 'temperatures', 'from', 'double', 'ratios', 'of', 'hydrogen', 'helium', 'lithium', 'beryllium', 'and', 'carbon', 'isotopic', 'yields', 'and', 'excitedstate', 'temperatures', 'from', 'yield', 'ratios', 'of', 'particleunstable', 'resonances', 'in', '4he', '5li', 'and', '8be', 'were', 'determined', 'for', 'sp... | [0.016759460254026384, 0.2789298652339427, -0.08462586109633503, 0.02128645660617956, 0.10758593962788743, -0.10683292749166574, 0.08936338684382453, 0.3722699531461059, -0.17247771833027745, -0.3196319902594062, -0.12611443666345173, -0.3685784263686202, 0.1380899842352146, 0.12764644289881677, 0.09077963841029968, 0.... |
708.4116 | Dynamical SUSY Breaking in Intersecting Brane Models | We present a simple mechanism by which supersymmetry can be dynamically
broken in intersecting brane models, naturally generating an exponentially
small scale. Rather than utilize either non-Abelian gauge dynamics or
D-instantons, our mechanism uses worldsheet instantons to generate the small
scale in a hidden sector... | hep-th hep-ph | we present a simple mechanism by which supersymmetry can be dynamically broken in intersecting brane models naturally generating an exponentially small scale rather than utilize either nonabelian gauge dynamics or dinstantons our mechanism uses worldsheet instantons to generate the small scale in a hidden sector | [['we', 'present', 'a', 'simple', 'mechanism', 'by', 'which', 'supersymmetry', 'can', 'be', 'dynamically', 'broken', 'in', 'intersecting', 'brane', 'models', 'naturally', 'generating', 'an', 'exponentially', 'small', 'scale', 'rather', 'than', 'utilize', 'either', 'nonabelian', 'gauge', 'dynamics', 'or', 'dinstantons',... | [-0.16197741056481998, 0.3200320001410243, -0.10317710074078705, 0.18838342589636645, -0.1768728101419078, -0.20096234500201213, -0.003071327233273122, 0.31381711078704233, -0.266400877179371, -0.28641190158410207, 0.08948561028939568, -0.20015368579576412, -0.15457091921836966, 0.06465030018136733, -0.0481480770640903... |
708.4117 | Quadratic operators used in deducing exact ground states for correlated
systems: ferromagnetism at half filling provided by a dispersive band | Quadratic operators are used in transforming the model Hamiltonian (H) of one
correlated and dispersive band in an unique positive semidefinite form coopting
both the kinetic and interacting part of H. The expression is used in deducing
exact ground states which are minimum energy eigenstates only of the full
Hamilto... | cond-mat.str-el | quadratic operators are used in transforming the model hamiltonian h of one correlated and dispersive band in an unique positive semidefinite form coopting both the kinetic and interacting part of h the expression is used in deducing exact ground states which are minimum energy eigenstates only of the full hamiltonian ... | [['quadratic', 'operators', 'are', 'used', 'in', 'transforming', 'the', 'model', 'hamiltonian', 'h', 'of', 'one', 'correlated', 'and', 'dispersive', 'band', 'in', 'an', 'unique', 'positive', 'semidefinite', 'form', 'coopting', 'both', 'the', 'kinetic', 'and', 'interacting', 'part', 'of', 'h', 'the', 'expression', 'is',... | [-0.1621789648698824, 0.14132735543555303, -0.017658768469926953, 0.12226481186775749, -0.028954033096346796, -0.15669045579205784, -0.0031492077622614387, 0.34914996333666043, -0.25664146737997523, -0.281649676267989, 0.06141617656168011, -0.31643449476299185, -0.1356086834631343, 0.1335751836854292, 0.063068423148555... |
708.4118 | Transformation of Morphology and Luminosity Classes of the SDSS Galaxies | We present a unified picture on the evolution of galaxy luminosity and
morphology. Galaxy morphology is found to depend critically on the local
environment set up by the nearest neighbor galaxy in addition to luminosity and
the large scale density. When a galaxy is located farther than the virial
radius from its clos... | astro-ph | we present a unified picture on the evolution of galaxy luminosity and morphology galaxy morphology is found to depend critically on the local environment set up by the nearest neighbor galaxy in addition to luminosity and the large scale density when a galaxy is located farther than the virial radius from its closest ... | [['we', 'present', 'a', 'unified', 'picture', 'on', 'the', 'evolution', 'of', 'galaxy', 'luminosity', 'and', 'morphology', 'galaxy', 'morphology', 'is', 'found', 'to', 'depend', 'critically', 'on', 'the', 'local', 'environment', 'set', 'up', 'by', 'the', 'nearest', 'neighbor', 'galaxy', 'in', 'addition', 'to', 'luminos... | [-0.06608128256423008, 0.11788193308274979, -0.07244221325006726, 0.09053503694195049, -0.07997509370474278, -0.06678986174114102, 0.02429340772572706, 0.39439182652299726, -0.22335878790942854, -0.3069871806032505, 0.07793364771666648, -0.320712778876988, -0.05324940988793969, 0.14668281781371165, 0.03445695040729294,... |
708.4119 | The early spectral evolution of SN 2004dt | Aims. We study the optical spectroscopic properties of Type Ia Supernova (SN
Ia) 2004dt, focusing our attention on the early epochs.
Methods. Observation triggered soon after the SN 2004dt discovery allowed us
to obtain a spectrophotometric coverage from day -10 to almost one year (~353
days) after the B band maxim... | astro-ph | aims we study the optical spectroscopic properties of type ia supernova sn ia 2004dt focusing our attention on the early epochs methods observation triggered soon after the sn 2004dt discovery allowed us to obtain a spectrophotometric coverage from day 10 to almost one year 353 days after the b band maximum observation... | [['aims', 'we', 'study', 'the', 'optical', 'spectroscopic', 'properties', 'of', 'type', 'ia', 'supernova', 'sn', 'ia', '2004dt', 'focusing', 'our', 'attention', 'on', 'the', 'early', 'epochs', 'methods', 'observation', 'triggered', 'soon', 'after', 'the', 'sn', '2004dt', 'discovery', 'allowed', 'us', 'to', 'obtain', 'a... | [-0.05235919958897796, 0.057639838407595935, -0.05566614276282583, 0.020005237747536007, -0.08904539428454772, -0.10888831466015185, 0.0879324932799712, 0.410868177536744, -0.19208334470588959, -0.30898398430503193, 0.06771898268658817, -0.3021474762272146, -0.028447606352085642, 0.18036129083671612, -0.016261329895456... |
708.412 | Theoretical model atmosphere spectra used for the calibration of
infrared instruments | One of the key ingredients in establishing the relation between input signal
and output flux from a spectrometer is accurate determination of the
spectrophotometric calibration. In the case of spectrometers onboard
satellites, the accuracy of this part of the calibration pedigree is ultimately
linked to the accuracy ... | astro-ph | one of the key ingredients in establishing the relation between input signal and output flux from a spectrometer is accurate determination of the spectrophotometric calibration in the case of spectrometers onboard satellites the accuracy of this part of the calibration pedigree is ultimately linked to the accuracy of t... | [['one', 'of', 'the', 'key', 'ingredients', 'in', 'establishing', 'the', 'relation', 'between', 'input', 'signal', 'and', 'output', 'flux', 'from', 'a', 'spectrometer', 'is', 'accurate', 'determination', 'of', 'the', 'spectrophotometric', 'calibration', 'in', 'the', 'case', 'of', 'spectrometers', 'onboard', 'satellites... | [0.022759237319737544, 0.07014925251842534, -0.07267038751099454, 0.10922671383116067, -0.08262285299664526, -0.07421738169729922, 0.05008612117676979, 0.4550569943430131, -0.14540177552160202, -0.3964730054107413, 0.09396103591282379, -0.3032361351713342, 0.02270944532836183, 0.23743238314218296, -0.1019445494715974, ... |
708.4121 | Estimates for parameters and characteristics of the confining
SU(3)-gluonic field in \pi^0-meson from one- and two-photon decays | On the basis of the confinement mechanism earlier proposed by author the
electric formfactor of $\pi^0$-meson is nonperturbatively calculated. The
latter is then applied to describing electromagnetic decays $\pi^0\to2\gamma$
and $\pi^0\to e^+e^-\gamma$ which entails estimates for parameters of the
confining SU(3)-glu... | hep-ph | on the basis of the confinement mechanism earlier proposed by author the electric formfactor of pi0meson is nonperturbatively calculated the latter is then applied to describing electromagnetic decays pi0to2gamma and pi0to eegamma which entails estimates for parameters of the confining su3gluonic field in pi0meson the ... | [['on', 'the', 'basis', 'of', 'the', 'confinement', 'mechanism', 'earlier', 'proposed', 'by', 'author', 'the', 'electric', 'formfactor', 'of', 'pi0meson', 'is', 'nonperturbatively', 'calculated', 'the', 'latter', 'is', 'then', 'applied', 'to', 'describing', 'electromagnetic', 'decays', 'pi0to2gamma', 'and', 'pi0to', 'e... | [-0.09667974841385518, 0.2222041691161899, -0.053425292292284585, 0.08741839443303881, -0.04241736950944104, -0.0804980748466083, 0.007298113595295165, 0.36858919638371657, -0.15717155878092087, -0.2815514530705672, -0.01242764231504961, -0.22325410698318765, -0.040635362622283754, 0.1771675217601042, 0.048173763375315... |
708.4122 | On the stability of the triangular libration points: exact results | This paper has been withdrawn by the author, due to necessity of revision.
| astro-ph | this paper has been withdrawn by the author due to necessity of revision | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'author', 'due', 'to', 'necessity', 'of', 'revision']] | [-0.07375832432164596, -0.030269107924631007, -0.10107749041456443, -0.1016718844542853, -0.20956976539813554, -0.0077370047712555295, 0.03499392055583975, 0.3010449008299754, -0.22672517569019243, -0.40683457599236417, 0.10455750602369125, -0.27558917752825296, -0.12718353090951076, 0.02892236612164057, -0.32931048609... |
708.4123 | Precision calculations for H -> WW/ZZ -> 4fermions with PROPHECY4f | PROPHECY4f is a Monte Carlo event generator for precise simulations of the
Higgs-boson decay H -> WW/ZZ -> 4fermions, supporting leptonic, semileptonic,
and four-quark final states. Both electroweak and QCD corrections are included.
Treating the intermediate gauge bosons as resonances, the calculation covers
the full... | hep-ph | prophecy4f is a monte carlo event generator for precise simulations of the higgsboson decay h wwzz 4fermions supporting leptonic semileptonic and fourquark final states both electroweak and qcd corrections are included treating the intermediate gauge bosons as resonances the calculation covers the full higgsboson mass ... | [['prophecy4f', 'is', 'a', 'monte', 'carlo', 'event', 'generator', 'for', 'precise', 'simulations', 'of', 'the', 'higgsboson', 'decay', 'h', 'wwzz', '4fermions', 'supporting', 'leptonic', 'semileptonic', 'and', 'fourquark', 'final', 'states', 'both', 'electroweak', 'and', 'qcd', 'corrections', 'are', 'included', 'treat... | [-0.053515960449274154, 0.22414549470970957, -0.0005364230223996959, 0.23300503810185572, -0.08663890854796578, -0.14251962846512317, 0.07709244873479638, 0.37881234461362934, -0.1416055727028616, -0.257790560847227, 0.009496672093723965, -0.3333567068452986, 0.024992990346861556, 0.12820546990129308, 0.102018430645407... |
708.4124 | Shell Effects in the First Sound Velocity of an Ultracold Fermi Gas | We investigate the first sound of a normal dilute and ultracold two-component
Fermi gas in a harmonic microtube, i.e. a cylinder with harmonic transverse
radial confinement in the length-scale of microns. We show that the velocity of
the sound that propagates along the axial direction strongly depends on the
dimensio... | cond-mat.stat-mech cond-mat.other | we investigate the first sound of a normal dilute and ultracold twocomponent fermi gas in a harmonic microtube ie a cylinder with harmonic transverse radial confinement in the lengthscale of microns we show that the velocity of the sound that propagates along the axial direction strongly depends on the dimensionality o... | [['we', 'investigate', 'the', 'first', 'sound', 'of', 'a', 'normal', 'dilute', 'and', 'ultracold', 'twocomponent', 'fermi', 'gas', 'in', 'a', 'harmonic', 'microtube', 'ie', 'a', 'cylinder', 'with', 'harmonic', 'transverse', 'radial', 'confinement', 'in', 'the', 'lengthscale', 'of', 'microns', 'we', 'show', 'that', 'the... | [-0.1617144745897764, 0.2450420415499112, -0.05981749047082171, -0.018545422800228868, -0.007630530066643525, -0.11634912588226709, 0.013207418889313647, 0.3815280883979884, -0.23299385543892304, -0.19936701347395885, 0.013074661324759132, -0.2814135800468401, -0.0895820700391693, 0.17715482080854855, 0.024477077308828... |
708.4125 | Comparing cosmic shear measures - Optimizing the Information content of
cosmic shear data vectors | We introduce an optimized data vector of cosmic shear measures (N). This data
vector has high information content, is not sensitive against B-mode
contamination and only shows small correlation between data points of different
angular scales. We show that a data vector of the two-point correlation
function (2PCF) in ... | astro-ph | we introduce an optimized data vector of cosmic shear measures n this data vector has high information content is not sensitive against bmode contamination and only shows small correlation between data points of different angular scales we show that a data vector of the twopoint correlation function 2pcf in general con... | [['we', 'introduce', 'an', 'optimized', 'data', 'vector', 'of', 'cosmic', 'shear', 'measures', 'n', 'this', 'data', 'vector', 'has', 'high', 'information', 'content', 'is', 'not', 'sensitive', 'against', 'bmode', 'contamination', 'and', 'only', 'shows', 'small', 'correlation', 'between', 'data', 'points', 'of', 'differ... | [-0.13168825656528105, 0.06777357044284217, -0.08341746577859459, 0.1115881903050653, -0.09663229582245013, -0.08334050177127138, -0.0021857809728991046, 0.3604044294823332, -0.24416638687308656, -0.28287674699802384, 0.09320284864880085, -0.3456842967119361, -0.08114699090170521, 0.17773961824313014, -0.01808599164093... |
708.4126 | Diffractive parton distributions: the role of the perturbative Pomeron | We consider the role of the perturbative Pomeron-to-parton splitting in the
formation of the diffractive parton distributions.
| hep-ph | we consider the role of the perturbative pomerontoparton splitting in the formation of the diffractive parton distributions | [['we', 'consider', 'the', 'role', 'of', 'the', 'perturbative', 'pomerontoparton', 'splitting', 'in', 'the', 'formation', 'of', 'the', 'diffractive', 'parton', 'distributions']] | [-0.12525453174021095, 0.17085669172229245, -0.19643396558240056, 0.20192596362903714, 0.04000256583094597, 0.11022656946443021, -0.03697137534618378, 0.36823363322764635, -0.21299182414077222, -0.19924426218494773, -0.05364691338763805, -0.23852892313152552, -0.017806311137974262, 0.03977726399898529, 0.06857729330658... |
708.4127 | The Dirichlet Casimir effect for $\phi^4$ theory in (3+1) dimensions: A
new renormalization approach | We calculate the next to the leading order Casimir effect for a real scalar
field, within $\phi^4$ theory, confined between two parallel plates in three
spatial dimensions with the Dirichlet boundary condition. In this paper we
introduce a systematic perturbation expansion in which the counterterms
automatically turn... | hep-th | we calculate the next to the leading order casimir effect for a real scalar field within phi4 theory confined between two parallel plates in three spatial dimensions with the dirichlet boundary condition in this paper we introduce a systematic perturbation expansion in which the counterterms automatically turn out to b... | [['we', 'calculate', 'the', 'next', 'to', 'the', 'leading', 'order', 'casimir', 'effect', 'for', 'a', 'real', 'scalar', 'field', 'within', 'phi4', 'theory', 'confined', 'between', 'two', 'parallel', 'plates', 'in', 'three', 'spatial', 'dimensions', 'with', 'the', 'dirichlet', 'boundary', 'condition', 'in', 'this', 'pap... | [-0.1266906511566291, 0.13621998965429763, -0.09082008849518995, 0.05508422901077817, -0.09923505968414247, -0.10911691638330619, 0.021410692712912956, 0.3404373057124515, -0.2210206655606938, -0.27975844147304696, 0.1219055154104717, -0.2555989527531589, -0.14922486293750506, 0.15141720485407859, -0.03882709864682207,... |
708.4128 | On radio emission of the Geminga pulsar and RBS 1223 at the frequency of
111 MHz | I have searched for pulsed radio emission from the Geminga pulsar and for the
nearby isolated neutron star 1RX J1308.6+2127 (RBS 1223) at the frequency of
111 MHz. No pulsed signals were detected from these sources. Upper limits for
mean flux density are 0.4 - 4 mJy for the Geminga pulsar and 1.5 - 15 mJy for
RBS 122... | astro-ph | i have searched for pulsed radio emission from the geminga pulsar and for the nearby isolated neutron star 1rx j130862127 rbs 1223 at the frequency of 111 mhz no pulsed signals were detected from these sources upper limits for mean flux density are 04 4 mjy for the geminga pulsar and 15 15 mjy for rbs 1223 depending on... | [['i', 'have', 'searched', 'for', 'pulsed', 'radio', 'emission', 'from', 'the', 'geminga', 'pulsar', 'and', 'for', 'the', 'nearby', 'isolated', 'neutron', 'star', '1rx', 'j130862127', 'rbs', '1223', 'at', 'the', 'frequency', 'of', '111', 'mhz', 'no', 'pulsed', 'signals', 'were', 'detected', 'from', 'these', 'sources', ... | [-0.08621048612632987, 0.18918326333390945, 0.03390865377503249, 0.10988163221345255, -0.08849236123602498, -0.0988957315372924, 0.1690839793476643, 0.4624190705433262, -0.10114822157827968, -0.41213337512630405, 0.13040883712175966, -0.3354623911507202, 0.10496314925452073, 0.301760064766065, 0.0332119447094473, -0.06... |
708.4129 | Lattice Supersymmetry: Equivalence between the Link Approach and
Orbifolding | We examine the relation between supersymmetric lattice gauge theories
constructed by the link approach and by orbifolding and show that they are
equivalent. We discuss the number of preserved supersymmetries.
| hep-lat hep-th | we examine the relation between supersymmetric lattice gauge theories constructed by the link approach and by orbifolding and show that they are equivalent we discuss the number of preserved supersymmetries | [['we', 'examine', 'the', 'relation', 'between', 'supersymmetric', 'lattice', 'gauge', 'theories', 'constructed', 'by', 'the', 'link', 'approach', 'and', 'by', 'orbifolding', 'and', 'show', 'that', 'they', 'are', 'equivalent', 'we', 'discuss', 'the', 'number', 'of', 'preserved', 'supersymmetries']] | [-0.14778285203501582, 0.21113766795024275, -0.013370831434925397, 0.15631905910559, -0.0019088369483749072, -0.1698289077108105, 0.030905462428927423, 0.4347528138508399, -0.21653162688016891, -0.31488381973467766, 0.0929414703277871, -0.24333268388484916, -0.24944137663890917, 0.08766707245570918, -0.0768293268357714... |
708.413 | Electrically and magnetically induced optical rotation in Pb5Ge3O11:Cr
crystals at the phase transition. 1. Electrogyration effect in Pb5Ge3O11:Cr | We present the results of studies for temperature dependences of
electrogyration (EG) effect and natural optical activity in Pb5Ge3O11:Cr
crystals. Extremely high magnitude of EG coefficient is found for these
crystals. We also demonstrate how the Curie-Weiss constant, the critical
exponents of the order parameter an... | physics.optics | we present the results of studies for temperature dependences of electrogyration eg effect and natural optical activity in pb5ge3o11cr crystals extremely high magnitude of eg coefficient is found for these crystals we also demonstrate how the curieweiss constant the critical exponents of the order parameter and the die... | [['we', 'present', 'the', 'results', 'of', 'studies', 'for', 'temperature', 'dependences', 'of', 'electrogyration', 'eg', 'effect', 'and', 'natural', 'optical', 'activity', 'in', 'pb5ge3o11cr', 'crystals', 'extremely', 'high', 'magnitude', 'of', 'eg', 'coefficient', 'is', 'found', 'for', 'these', 'crystals', 'we', 'als... | [-0.09147520335939001, 0.1730848901480546, -0.027975372203132686, -0.017669020376428413, -0.06810080454520442, -0.09284032051287153, 0.06484884693054482, 0.3912542853726978, -0.24679164399447687, -0.3258374737959136, 0.10825775931281147, -0.31929637798491645, -0.1691466969821383, 0.254902962663704, 0.039463651859584975... |
708.4131 | Full Bayesian analysis for a class of jump-diffusion models | A new Bayesian significance test is adjusted for jump detection in a
diffusion process. This is an advantageous procedure for temporal data having
extreme valued outliers, like financial data, pluvial or tectonic forces
records and others.
| stat.ME | a new bayesian significance test is adjusted for jump detection in a diffusion process this is an advantageous procedure for temporal data having extreme valued outliers like financial data pluvial or tectonic forces records and others | [['a', 'new', 'bayesian', 'significance', 'test', 'is', 'adjusted', 'for', 'jump', 'detection', 'in', 'a', 'diffusion', 'process', 'this', 'is', 'an', 'advantageous', 'procedure', 'for', 'temporal', 'data', 'having', 'extreme', 'valued', 'outliers', 'like', 'financial', 'data', 'pluvial', 'or', 'tectonic', 'forces', 'r... | [-0.060288505908101794, 0.07944130444209024, -0.12380310243793896, 0.17306728442059205, -0.14102756354425636, -0.19021522974861518, 0.07764258080029061, 0.40022830196789333, -0.25707718531734175, -0.29294890532536166, 0.16533649725772973, -0.2925098242504256, -0.11616678682954183, 0.16859375900322837, -0.13564342940226... |
708.4132 | Exploring spatial nonlinearity using additive approximation | We propose to approximate the conditional expectation of a spatial random
variable given its nearest-neighbour observations by an additive function. The
setting is meaningful in practice and requires no unilateral ordering. It is
capable of catching nonlinear features in spatial data and exploring local
dependence st... | math.ST stat.TH | we propose to approximate the conditional expectation of a spatial random variable given its nearestneighbour observations by an additive function the setting is meaningful in practice and requires no unilateral ordering it is capable of catching nonlinear features in spatial data and exploring local dependence structu... | [['we', 'propose', 'to', 'approximate', 'the', 'conditional', 'expectation', 'of', 'a', 'spatial', 'random', 'variable', 'given', 'its', 'nearestneighbour', 'observations', 'by', 'an', 'additive', 'function', 'the', 'setting', 'is', 'meaningful', 'in', 'practice', 'and', 'requires', 'no', 'unilateral', 'ordering', 'it'... | [-0.0722620394327819, 0.04629618605295863, -0.11212957807760121, 0.12055646356682038, -0.08571277852311279, -0.11096347097279222, 0.03970424184014767, 0.41448295392999146, -0.24764267961357042, -0.2871958629129398, 0.11047359954682179, -0.26106575479251193, -0.15074544317604072, 0.19559513593699332, -0.0613904869409673... |
708.4133 | Some doubts on the validity of the foreground Galactic contribution
subtraction from microwave anisotropies | The Galactic foreground contamination in CMBR anisotropies, especially from
the dust component, is not easily separable from the cosmological or
extragalactic component. In this paper, some doubts will be raised concerning
the validity of the methods used to date to remove Galactic dust emission in
order to show that... | astro-ph | the galactic foreground contamination in cmbr anisotropies especially from the dust component is not easily separable from the cosmological or extragalactic component in this paper some doubts will be raised concerning the validity of the methods used to date to remove galactic dust emission in order to show that none ... | [['the', 'galactic', 'foreground', 'contamination', 'in', 'cmbr', 'anisotropies', 'especially', 'from', 'the', 'dust', 'component', 'is', 'not', 'easily', 'separable', 'from', 'the', 'cosmological', 'or', 'extragalactic', 'component', 'in', 'this', 'paper', 'some', 'doubts', 'will', 'be', 'raised', 'concerning', 'the',... | [-0.05671710433516031, 0.06286083152517677, -0.07071507616796427, 0.08770865557611816, -0.1260756564171364, -0.05025367596600619, 0.01700928521795302, 0.3731294799632289, -0.2232887354394835, -0.32237326684925294, 0.08816519717582398, -0.3258205690400468, -0.021910638618800375, 0.20796182858654194, -0.02375001722946763... |
708.4134 | Star-gas decoupling and a non-rotating stellar core in He 2-10: Integral
field spectroscopy with FLAMES/ARGUS | We study the two-dimensional distribution and kinematics of the stellar and
gaseous components in the centre of the blue compact dwarf galaxy, He 2-10. The
aim is to compare the kinematics of gas and stars in order to determine whether
they are consistent with one another, or if stars and gas can be decoupled due
to ... | astro-ph | we study the twodimensional distribution and kinematics of the stellar and gaseous components in the centre of the blue compact dwarf galaxy he 210 the aim is to compare the kinematics of gas and stars in order to determine whether they are consistent with one another or if stars and gas can be decoupled due to gravita... | [['we', 'study', 'the', 'twodimensional', 'distribution', 'and', 'kinematics', 'of', 'the', 'stellar', 'and', 'gaseous', 'components', 'in', 'the', 'centre', 'of', 'the', 'blue', 'compact', 'dwarf', 'galaxy', 'he', '210', 'the', 'aim', 'is', 'to', 'compare', 'the', 'kinematics', 'of', 'gas', 'and', 'stars', 'in', 'orde... | [-0.04861709832655358, 0.0977847670642937, -0.07268806363598586, 0.061832929635776045, -0.08729846719107046, -0.027747048830680618, 0.012022891228699737, 0.4533117350929224, -0.18753483193729342, -0.3100722241362238, 0.053597096459172364, -0.28206982216923626, -0.002343460935302213, 0.17022169328940748, -0.022045139075... |
708.4135 | Strangeness content of the nucleon in quasielastic neutrino-nucleus
reactions | We present a systematic study of the sensitivity of quasielastic
neutrino-nucleus cross sections at intermediate energies to the strange quark
sea of the nucleon. To this end, we investigate the impact of the weak
strangeness form factors on the ratio of proton-to-neutron knockout, the ratio
of neutral-to-charged cur... | nucl-th | we present a systematic study of the sensitivity of quasielastic neutrinonucleus cross sections at intermediate energies to the strange quark sea of the nucleon to this end we investigate the impact of the weak strangeness form factors on the ratio of protontoneutron knockout the ratio of neutraltocharged current cross... | [['we', 'present', 'a', 'systematic', 'study', 'of', 'the', 'sensitivity', 'of', 'quasielastic', 'neutrinonucleus', 'cross', 'sections', 'at', 'intermediate', 'energies', 'to', 'the', 'strange', 'quark', 'sea', 'of', 'the', 'nucleon', 'to', 'this', 'end', 'we', 'investigate', 'the', 'impact', 'of', 'the', 'weak', 'stra... | [-0.06701315893503472, 0.20780649209312724, -0.08265074163460487, 0.16603537950245406, 0.0017743486363070281, -0.04338617775157012, 0.04731751623748704, 0.34013199155831203, -0.1670854380277104, -0.2577679598374673, -0.06926376468409368, -0.3455542625694726, -0.02745237637270057, 0.1350135655870445, 0.08145522516483225... |
708.4136 | Solar cell Edge shunt isolation : A simplified approach | Edge shunts are among the main factors causing reduction in solar cell open
circuit voltage that is why their isolation is one of the main steps in solar
cell manufacturing. Many techniques have been employed to achieve this goal,
e.g. plasma etching, grinding, wet etching, etc. Unfortunately, these methods
have the ... | cond-mat.other | edge shunts are among the main factors causing reduction in solar cell open circuit voltage that is why their isolation is one of the main steps in solar cell manufacturing many techniques have been employed to achieve this goal eg plasma etching grinding wet etching etc unfortunately these methods have the disadvantag... | [['edge', 'shunts', 'are', 'among', 'the', 'main', 'factors', 'causing', 'reduction', 'in', 'solar', 'cell', 'open', 'circuit', 'voltage', 'that', 'is', 'why', 'their', 'isolation', 'is', 'one', 'of', 'the', 'main', 'steps', 'in', 'solar', 'cell', 'manufacturing', 'many', 'techniques', 'have', 'been', 'employed', 'to',... | [-0.0651790685103412, 0.1512128680470885, -0.03258688565228106, -0.01194517408867803, -0.06162266650728073, -0.20530827661485287, 0.10194086761018911, 0.4217478876081548, -0.2540397590293383, -0.35258358271518186, 0.10322016379489138, -0.24418237892001174, -0.1851616536164223, 0.2326289591516635, -0.16187138908882012, ... |
708.4137 | A multiwavelength study of Galactic HII region Sh2-294 | We present the observational results of Galactic HII region S294, using
optical photometry, narrow-band imaging and radio continuum mapping at 1280
MHz, together with archival data from 2MASS, MSX and IRAS surveys. The stellar
surface density profile indicates that the radius of the cluster associated
with the S294 r... | astro-ph | we present the observational results of galactic hii region s294 using optical photometry narrowband imaging and radio continuum mapping at 1280 mhz together with archival data from 2mass msx and iras surveys the stellar surface density profile indicates that the radius of the cluster associated with the s294 region is... | [['we', 'present', 'the', 'observational', 'results', 'of', 'galactic', 'hii', 'region', 's294', 'using', 'optical', 'photometry', 'narrowband', 'imaging', 'and', 'radio', 'continuum', 'mapping', 'at', '1280', 'mhz', 'together', 'with', 'archival', 'data', 'from', '2mass', 'msx', 'and', 'iras', 'surveys', 'the', 'stell... | [-0.0490739806732097, 0.06431493072742975, -0.047366230319132334, 0.06070345900780044, -0.0526187640052065, -0.05523263392295333, 0.07401495493945169, 0.47743311570710484, -0.20313815025583093, -0.30775357653590923, 0.0315078480285181, -0.30632060224539187, 0.019353455925391585, 0.14148124165474288, -0.0164993488598404... |
708.4138 | Generalized backward doubly stochastic differential equations and SPDEs
with nonlinear Neumann boundary conditions | In this paper a new class of generalized backward doubly stochastic
differential equations is investigated. This class involves an integral with
respect to an adapted continuous increasing process. A probabilistic
representation for viscosity solutions of semi-linear stochastic partial
differential equations with a N... | math.PR math.AP | in this paper a new class of generalized backward doubly stochastic differential equations is investigated this class involves an integral with respect to an adapted continuous increasing process a probabilistic representation for viscosity solutions of semilinear stochastic partial differential equations with a neuman... | [['in', 'this', 'paper', 'a', 'new', 'class', 'of', 'generalized', 'backward', 'doubly', 'stochastic', 'differential', 'equations', 'is', 'investigated', 'this', 'class', 'involves', 'an', 'integral', 'with', 'respect', 'to', 'an', 'adapted', 'continuous', 'increasing', 'process', 'a', 'probabilistic', 'representation'... | [-0.151437032868729, 0.05636340574462938, -0.0375121916208337, 0.033358197090994045, -0.18663912111932926, -0.1475830407951899, -0.06398387955491767, 0.2458507389652523, -0.39408539433745626, -0.17152106171062692, 0.1215311563846239, -0.27871794184233917, -0.14218609530399454, 0.1815089768670658, -0.14076659346910866, ... |
708.4139 | Non-linear Equation of State, COSMIC Acceleration and Deceleration
During Phantom-Dominance | Here, RS-II model of brane-gravity is considerd for phantom universe using
non-linear equation of stste. Phantom fluid is known to violate the weak energy
condition. In this paper, it is found that this characteristic of phantom
energy is affected drastically by the negative brane-tension $\lambda$ of the
RS-II model... | gr-qc | here rsii model of branegravity is considerd for phantom universe using nonlinear equation of stste phantom fluid is known to violate the weak energy condition in this paper it is found that this characteristic of phantom energy is affected drastically by the negative branetension lambda of the rsii model it is interes... | [['here', 'rsii', 'model', 'of', 'branegravity', 'is', 'considerd', 'for', 'phantom', 'universe', 'using', 'nonlinear', 'equation', 'of', 'stste', 'phantom', 'fluid', 'is', 'known', 'to', 'violate', 'the', 'weak', 'energy', 'condition', 'in', 'this', 'paper', 'it', 'is', 'found', 'that', 'this', 'characteristic', 'of',... | [-0.1461039681751512, 0.1754958155364845, -0.08989434072763221, 0.1310494356780998, -0.09807473981429722, -0.2326088031669232, -0.05499104466500946, 0.2959582955414845, -0.21608132745085423, -0.3033085056495937, 0.04052012805800023, -0.23721236778684884, -0.043167525596439466, 0.1340588975874784, -0.003334058691124039,... |
708.414 | On E0 Transitions in even-even nuclei | The reanimation of the investigations dedicated to 0^{+} states energies and
E0 transitions between them is provoked by new and more precise experimental
techniques that not only made revision of the previous data but also gave a
possibility to obtain a great amount of new 0^{+} states energies and
conversion electro... | nucl-th | the reanimation of the investigations dedicated to 0 states energies and e0 transitions between them is provoked by new and more precise experimental techniques that not only made revision of the previous data but also gave a possibility to obtain a great amount of new 0 states energies and conversion electrons data we... | [['the', 'reanimation', 'of', 'the', 'investigations', 'dedicated', 'to', '0', 'states', 'energies', 'and', 'e0', 'transitions', 'between', 'them', 'is', 'provoked', 'by', 'new', 'and', 'more', 'precise', 'experimental', 'techniques', 'that', 'not', 'only', 'made', 'revision', 'of', 'the', 'previous', 'data', 'but', 'a... | [-0.07882336873885695, 0.159075549497937, -0.07590151450719045, 0.08156676230025525, -0.035236578005791705, -0.1584668761410873, 0.11816953740675341, 0.3618212813003497, -0.18544621579819406, -0.32402912317540006, 0.025883643596310808, -0.3150264409116723, -0.00829425859594285, 0.1554147216039851, 0.029540070436067052,... |
708.4141 | Phases of 4D Scalar-tensor black holes coupled to Born-Infeld nonlinear
electrodynamics | Recent results show that when non-linear electrodynamics is considered the
no-scalar-hair theorems in the scalar-tensor theories (STT) of gravity, which
are valid for the cases of neutral black holes and charged black holes in the
Maxwell electrodynamics, can be circumvented. What is even more, in the present
work, w... | gr-qc | recent results show that when nonlinear electrodynamics is considered the noscalarhair theorems in the scalartensor theories stt of gravity which are valid for the cases of neutral black holes and charged black holes in the maxwell electrodynamics can be circumvented what is even more in the present work we find new no... | [['recent', 'results', 'show', 'that', 'when', 'nonlinear', 'electrodynamics', 'is', 'considered', 'the', 'noscalarhair', 'theorems', 'in', 'the', 'scalartensor', 'theories', 'stt', 'of', 'gravity', 'which', 'are', 'valid', 'for', 'the', 'cases', 'of', 'neutral', 'black', 'holes', 'and', 'charged', 'black', 'holes', 'i... | [-0.18739226534598857, 0.11093447793318774, -0.05694469881127588, 0.11792951502575306, -0.06246517544204835, -0.17475730119331273, -0.03788566128641833, 0.2691562549123773, -0.16251805834826882, -0.26680598713574, 0.08551002447857173, -0.30250866731075804, -0.146430299046915, 0.18401019158773124, -0.02596325684498879, ... |
708.4142 | Terahertz conductivity of localized photoinduced carriers in Mott
insulator YTiO$_{3}$ at low excitation density, contrasted with metallic
nature in band semiconductor Si | We performed optical-pump terahertz-probe measurements of a Mott insulator
YTiO$_{3}$ and a band semiconductor Si using a laser diode (1.47 eV) and a
femtosecond pulse laser (1.55 eV). Both samples possess long energy-relaxation
times (1.5 ms for YTiO$_{3}$ and 15 $\mu$s for Si); therefore, it is possible
to extract ... | cond-mat.str-el cond-mat.mtrl-sci | we performed opticalpump terahertzprobe measurements of a mott insulator ytio_3 and a band semiconductor si using a laser diode 147 ev and a femtosecond pulse laser 155 ev both samples possess long energyrelaxation times 15 ms for ytio_3 and 15 mus for si therefore it is possible to extract terahertz complex conductivi... | [['we', 'performed', 'opticalpump', 'terahertzprobe', 'measurements', 'of', 'a', 'mott', 'insulator', 'ytio_3', 'and', 'a', 'band', 'semiconductor', 'si', 'using', 'a', 'laser', 'diode', '147', 'ev', 'and', 'a', 'femtosecond', 'pulse', 'laser', '155', 'ev', 'both', 'samples', 'possess', 'long', 'energyrelaxation', 'tim... | [-0.1362177903295121, 0.22137661532480682, -0.03588548798088719, -0.010333959546199917, 0.024004451209856642, -0.1893514192181633, 0.10819080523627043, 0.4567418468697947, -0.23015395606088698, -0.2774236082371806, 0.014629592699296519, -0.34096711177258515, -0.09077914058370198, 0.18266641546942003, 0.0335334699100428... |
708.4143 | Stephani-Schutz quantum cosmology | We study the Stephani quantum cosmological model in the presence of a
cosmological constant in radiation dominated Universe. In the present work the
Schutz's variational formalism which recovers the notion of time is applied.
This gives rise to Wheeler-DeWitt equations which can be cast in the form of
Schr\"odinger e... | gr-qc | we study the stephani quantum cosmological model in the presence of a cosmological constant in radiation dominated universe in the present work the schutzs variational formalism which recovers the notion of time is applied this gives rise to wheelerdewitt equations which can be cast in the form of schrodinger equations... | [['we', 'study', 'the', 'stephani', 'quantum', 'cosmological', 'model', 'in', 'the', 'presence', 'of', 'a', 'cosmological', 'constant', 'in', 'radiation', 'dominated', 'universe', 'in', 'the', 'present', 'work', 'the', 'schutzs', 'variational', 'formalism', 'which', 'recovers', 'the', 'notion', 'of', 'time', 'is', 'app... | [-0.11636194869788596, 0.10693418798211951, -0.11590936476318348, 0.06018863096142013, -0.06782170626684092, -0.08754855548431806, -0.0005210085710132262, 0.31275239043134206, -0.26176821331137035, -0.29031306974502513, 0.07140589229766192, -0.25627402793907095, -0.11685043577381293, 0.1332849288774014, -0.004850681063... |
708.4144 | High rate production of polarized 3He with meta-stability exchange
method | Keywords: polarized 3He, meta-stability exchange, infrared laser
| nucl-ex | keywords polarized 3he metastability exchange infrared laser | [['keywords', 'polarized', '3he', 'metastability', 'exchange', 'infrared', 'laser']] | [-0.06156376217092786, 0.5170119000332696, -0.14632590460990155, 0.20189635987792695, 0.015482636035553046, -0.13505429614867484, 0.12995636276900768, 0.5047498066643519, -0.28471347357013393, -0.11897391972265073, -0.08151949090617043, -0.392855666577816, 0.11423636440719877, 0.13327380306353526, 0.11816103264157261, ... |
708.4145 | Low Luminosity Radio Loud Active Galactic Nuclei | I review observational properties of low power radio loud AGN. High
resolution VLBI observations allow the estimate of the jet velocity and
orientation with respect to the line of sight and the determination of the
Doppler factor. These data reveal rich structures, including two-sided jets and
secondary components. N... | astro-ph | i review observational properties of low power radio loud agn high resolution vlbi observations allow the estimate of the jet velocity and orientation with respect to the line of sight and the determination of the doppler factor these data reveal rich structures including twosided jets and secondary components new resu... | [['i', 'review', 'observational', 'properties', 'of', 'low', 'power', 'radio', 'loud', 'agn', 'high', 'resolution', 'vlbi', 'observations', 'allow', 'the', 'estimate', 'of', 'the', 'jet', 'velocity', 'and', 'orientation', 'with', 'respect', 'to', 'the', 'line', 'of', 'sight', 'and', 'the', 'determination', 'of', 'the',... | [-0.11689771635780832, 0.08975138726283706, -0.02234635706390104, 0.04274897673918355, -0.19501049388876004, -0.1069752813331903, -0.003130860260904639, 0.48522321471283514, -0.18161828227100835, -0.325848874002282, 0.0858387025730354, -0.2538070588132306, -0.02200797315585547, 0.21467938878753734, -0.01186526442817863... |
708.4146 | Z_3 Polyakov Loop Models and Inverse Monte-Carlo Methods | We study effective Polyakov loop models for SU(3) Yang-Mills theory at finite
temperature. A comprehensive mean field analysis of the phase diagram is
carried out and compared to the results obtained from Monte-Carlo simulations.
We find a rich phase structure including ferromagnetic and antiferromagnetic
phases. Due... | hep-lat | we study effective polyakov loop models for su3 yangmills theory at finite temperature a comprehensive mean field analysis of the phase diagram is carried out and compared to the results obtained from montecarlo simulations we find a rich phase structure including ferromagnetic and antiferromagnetic phases due to the p... | [['we', 'study', 'effective', 'polyakov', 'loop', 'models', 'for', 'su3', 'yangmills', 'theory', 'at', 'finite', 'temperature', 'a', 'comprehensive', 'mean', 'field', 'analysis', 'of', 'the', 'phase', 'diagram', 'is', 'carried', 'out', 'and', 'compared', 'to', 'the', 'results', 'obtained', 'from', 'montecarlo', 'simula... | [-0.11042053691779423, 0.13657630918396993, -0.10034783186880175, 0.11033363958863034, -0.03602880809568998, -0.12867795428110643, 0.08432833376491085, 0.3862677098903335, -0.17766641451967785, -0.2845765479859153, 0.08307564816781028, -0.32778614353049884, -0.1535430890131704, 0.11655393902052458, 0.06691248337926362,... |
708.4147 | On Some New Proof of the Bogoliubov-Parasiuk Theorem (Nonequilibrium
Renormalization Theory II) | It is usually used a complicated combinatorics to prove the
Bogoliubov-Parasiuk theorem. In the present paper we give a proof of the
Bogoliubov-Parasiuk theorem which use a simple combinatorics. To give this
proof we interpret Feynman amplitudes as distributions on the space of
\alpha-parameters.
We will use this t... | math-ph math.MP | it is usually used a complicated combinatorics to prove the bogoliubovparasiuk theorem in the present paper we give a proof of the bogoliubovparasiuk theorem which use a simple combinatorics to give this proof we interpret feynman amplitudes as distributions on the space of alphaparameters we will use this technique in... | [['it', 'is', 'usually', 'used', 'a', 'complicated', 'combinatorics', 'to', 'prove', 'the', 'bogoliubovparasiuk', 'theorem', 'in', 'the', 'present', 'paper', 'we', 'give', 'a', 'proof', 'of', 'the', 'bogoliubovparasiuk', 'theorem', 'which', 'use', 'a', 'simple', 'combinatorics', 'to', 'give', 'this', 'proof', 'we', 'in... | [-0.08374343790323159, 0.07548910612240434, -0.22640721847278042, 0.13420450429878877, -0.11548359762575175, -0.06656714375256687, 0.0877773996719436, 0.3150341774060114, -0.25324056711601645, -0.2611878462437842, 0.09270968174442297, -0.20151967214219071, -0.19585592366402615, 0.19423566589987762, -0.14746028600210273... |
708.4148 | Electron and lattice structure of ultra thin Ag films on Si(111) and
Si(001) | We studied the low temperature (T<130K) growth of Ag on Si(001) and Si(111)
flat surfaces prepared by Si homo epitaxy with the aim to achieve thin metallic
films. The band structure and morphology of the Ag overlayers have been
investigated by means of XPS, UPS, LEED, STM and STS. Surprisingly a
(root3xroot3)R30^o LE... | cond-mat.mtrl-sci cond-mat.stat-mech | we studied the low temperature t130k growth of ag on si001 and si111 flat surfaces prepared by si homo epitaxy with the aim to achieve thin metallic films the band structure and morphology of the ag overlayers have been investigated by means of xps ups leed stm and sts surprisingly a root3xroot3r30o leed structure for ... | [['we', 'studied', 'the', 'low', 'temperature', 't130k', 'growth', 'of', 'ag', 'on', 'si001', 'and', 'si111', 'flat', 'surfaces', 'prepared', 'by', 'si', 'homo', 'epitaxy', 'with', 'the', 'aim', 'to', 'achieve', 'thin', 'metallic', 'films', 'the', 'band', 'structure', 'and', 'morphology', 'of', 'the', 'ag', 'overlayers... | [-0.06780888373726948, 0.16236022830754895, -0.1019489856496934, -0.05072326682087395, 0.06337757830868565, -0.18107781730622294, 0.09024302822748019, 0.5362725597896403, -0.24242511285889534, -0.3053314703051001, 0.028053167377478413, -0.33576822381827137, -0.10335474417454774, 0.23154434034630897, -0.0029600133879050... |
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