id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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709.2135 | Coupling Superconducting Qubits via a Cavity Bus | Superconducting circuits are promising candidates for constructing quantum
bits (qubits) in a quantum computer; single-qubit operations are now routine,
and several examples of two qubit interactions and gates having been
demonstrated. These experiments show that two nearby qubits can be readily
coupled with local in... | cond-mat.mes-hall cond-mat.supr-con quant-ph | superconducting circuits are promising candidates for constructing quantum bits qubits in a quantum computer singlequbit operations are now routine and several examples of two qubit interactions and gates having been demonstrated these experiments show that two nearby qubits can be readily coupled with local interactio... | [['superconducting', 'circuits', 'are', 'promising', 'candidates', 'for', 'constructing', 'quantum', 'bits', 'qubits', 'in', 'a', 'quantum', 'computer', 'singlequbit', 'operations', 'are', 'now', 'routine', 'and', 'several', 'examples', 'of', 'two', 'qubit', 'interactions', 'and', 'gates', 'having', 'been', 'demonstrat... | [-0.1863201842052469, 0.20273407673585783, -0.01848109565200237, -0.004498770739532184, -0.011172510516226067, -0.27810808611582105, 0.0553456361249941, 0.4424082795953631, -0.22406338260101913, -0.3256322566756801, 0.01711300284901269, -0.2970722605703614, -0.09010636770919939, 0.2913293984142979, -0.00595416578384649... |
709.2136 | The Geometric Phase and Gravitational Precession of D-Branes | We study Berry's phase in the D0-D4-brane system. When a D0-brane moves in
the background of D4-branes, the first excited states undergo a holonomy
described by a non-Abelian Berry connection. At weak coupling this is an SU(2)
connection over R^5, known as the Yang monopole. At strong coupling, the
holonomy is recast... | hep-th | we study berrys phase in the d0d4brane system when a d0brane moves in the background of d4branes the first excited states undergo a holonomy described by a nonabelian berry connection at weak coupling this is an su2 connection over r5 known as the yang monopole at strong coupling the holonomy is recast as the classical... | [['we', 'study', 'berrys', 'phase', 'in', 'the', 'd0d4brane', 'system', 'when', 'a', 'd0brane', 'moves', 'in', 'the', 'background', 'of', 'd4branes', 'the', 'first', 'excited', 'states', 'undergo', 'a', 'holonomy', 'described', 'by', 'a', 'nonabelian', 'berry', 'connection', 'at', 'weak', 'coupling', 'this', 'is', 'an'... | [-0.24929833807708585, 0.21124295706960017, -0.07630939762491513, 0.08083719439010191, -0.07574633468380745, -0.09669277342036367, 0.0038275245248394854, 0.25946765055551246, -0.18962444554576102, -0.2545240340096986, 0.04753190753296675, -0.2802550995393711, -0.1923205623512759, 0.08043112205478417, -0.041820598147152... |
709.2137 | The influence of pairing on the nuclear matrix elements of the
neutrinoless double beta decays | We study in this letter the behavior of the neutrinoless double beta decay
nuclear matrix elements (NME's) in the framework of the Interacting Shell
Model. We analize them in terms of the total angular momentum of the decaying
neutron pair and as a function of the seniority truncations in the nuclear wave
functions. ... | nucl-th hep-ph | we study in this letter the behavior of the neutrinoless double beta decay nuclear matrix elements nmes in the framework of the interacting shell model we analize them in terms of the total angular momentum of the decaying neutron pair and as a function of the seniority truncations in the nuclear wave functions this po... | [['we', 'study', 'in', 'this', 'letter', 'the', 'behavior', 'of', 'the', 'neutrinoless', 'double', 'beta', 'decay', 'nuclear', 'matrix', 'elements', 'nmes', 'in', 'the', 'framework', 'of', 'the', 'interacting', 'shell', 'model', 'we', 'analize', 'them', 'in', 'terms', 'of', 'the', 'total', 'angular', 'momentum', 'of', ... | [-0.07962384932723485, 0.15660473772710193, -0.09822865800329841, 0.14461714732406244, 0.011707493135551536, -0.07083130366329972, 0.056956460689810716, 0.3394344602326365, -0.23985241653215617, -0.27004820911942007, -0.013337958195330785, -0.2740663614341135, -0.0952055363887851, 0.1307331439461279, 0.0538526460545004... |
709.2138 | Dynamical Emergence of Complex Structures in Field Theories | Nonlinear field theories can be used to study both standard physics
questions, or to study questions such as the emergence of order and complexity.
These theories are generally derived from the symmetries of a given problem and
the interactions that respect those symmetries. Formally one can then quantize
the system ... | nlin.AO nlin.PS | nonlinear field theories can be used to study both standard physics questions or to study questions such as the emergence of order and complexity these theories are generally derived from the symmetries of a given problem and the interactions that respect those symmetries formally one can then quantize the system to fi... | [['nonlinear', 'field', 'theories', 'can', 'be', 'used', 'to', 'study', 'both', 'standard', 'physics', 'questions', 'or', 'to', 'study', 'questions', 'such', 'as', 'the', 'emergence', 'of', 'order', 'and', 'complexity', 'these', 'theories', 'are', 'generally', 'derived', 'from', 'the', 'symmetries', 'of', 'a', 'given',... | [-0.10408723936416209, 0.1555545484911372, -0.103322291101886, 0.11731312681808216, -0.07953412906005004, -0.11240318381635386, 0.0134184987396854, 0.337662283830296, -0.29739651432126957, -0.3377836582732533, 0.0977914929861702, -0.2721955190577051, -0.16363419685208427, 0.1534662998534033, -0.029810726627390954, 0.02... |
709.2139 | Spectral functions for medium-sized nuclei | The spectral functions for calcium and argon are constructed. It is verified
that their predictions for the quasielastic electron-nucleus cross sections in
the energy range ~1 GeV agree with the data. The argon spectral function is
then used to obtain the quasielastic neutrino-nucleus cross section.
| nucl-th | the spectral functions for calcium and argon are constructed it is verified that their predictions for the quasielastic electronnucleus cross sections in the energy range 1 gev agree with the data the argon spectral function is then used to obtain the quasielastic neutrinonucleus cross section | [['the', 'spectral', 'functions', 'for', 'calcium', 'and', 'argon', 'are', 'constructed', 'it', 'is', 'verified', 'that', 'their', 'predictions', 'for', 'the', 'quasielastic', 'electronnucleus', 'cross', 'sections', 'in', 'the', 'energy', 'range', '1', 'gev', 'agree', 'with', 'the', 'data', 'the', 'argon', 'spectral', ... | [0.057442226090158026, 0.1320956437745028, -0.04457563599571586, 0.19932217499137753, 0.046349321016007, -0.07319651316437456, -0.048803472684489355, 0.4329472656051318, -0.19286870426601835, -0.2518929890667399, -0.04381002591560698, -0.3854189013234443, 0.0377160447028776, 0.23171049501332971, 0.11464636644555462, 0.... |
709.214 | Entanglement as a Probe of Confinement | We investigate the entanglement entropy in gravity duals of confining large
$N_c$ gauge theories using the proposal of arXiv:hep-th/0603001,
arXiv:hep-th/0605073. Dividing one of the directions of space into a line
segment of length $l$ and its complement, the entanglement entropy between the
two subspaces is given b... | hep-th | we investigate the entanglement entropy in gravity duals of confining large n_c gauge theories using the proposal of arxivhepth0603001 arxivhepth0605073 dividing one of the directions of space into a line segment of length l and its complement the entanglement entropy between the two subspaces is given by the classical... | [['we', 'investigate', 'the', 'entanglement', 'entropy', 'in', 'gravity', 'duals', 'of', 'confining', 'large', 'n_c', 'gauge', 'theories', 'using', 'the', 'proposal', 'of', 'arxivhepth0603001', 'arxivhepth0605073', 'dividing', 'one', 'of', 'the', 'directions', 'of', 'space', 'into', 'a', 'line', 'segment', 'of', 'lengt... | [-0.19196359601856205, 0.2330944018322043, -0.06021688322637983, 0.07397146552555031, -0.010776646584851446, -0.1773789072303111, 0.03457704935538935, 0.31551661241288087, -0.18607660441374685, -0.21970028006061526, 0.06336530799907511, -0.33428669453796406, -0.052797319991224556, 0.15076786175929974, -0.00344275385672... |
709.2141 | A skein approach to Bennequin type inequalities | We give a simple unified proof for several disparate bounds on
Thurston-Bennequin number for Legendrian knots and self-linking number for
transverse knots in R^3, and provide a template for possible future bounds. As
an application, we give sufficient conditions for some of these bounds to be
sharp.
| math.GT math.SG | we give a simple unified proof for several disparate bounds on thurstonbennequin number for legendrian knots and selflinking number for transverse knots in r3 and provide a template for possible future bounds as an application we give sufficient conditions for some of these bounds to be sharp | [['we', 'give', 'a', 'simple', 'unified', 'proof', 'for', 'several', 'disparate', 'bounds', 'on', 'thurstonbennequin', 'number', 'for', 'legendrian', 'knots', 'and', 'selflinking', 'number', 'for', 'transverse', 'knots', 'in', 'r3', 'and', 'provide', 'a', 'template', 'for', 'possible', 'future', 'bounds', 'as', 'an', '... | [-0.21510921001057834, 0.0752760167459665, -0.08731773858295476, 0.16116643697023392, -0.1331848912684128, -0.19034567645731124, 0.05068294366108293, 0.3614531076572677, -0.19279336073297135, -0.3559286250296901, 0.11773457250092179, -0.18500157548709117, -0.10287787153960225, 0.35300154678840584, -0.11983728383053491,... |
709.2142 | The Rotation Period of the Planet-Hosting Star HD 189733 | We present synoptic optical photometry of HD 189733, the chromospherically
active parent star of one of the most intensively studied exoplanets. We have
significantly extended the timespan of our previously reported observations and
refined the estimate of the stellar rotation period by more than an order of
magnitud... | astro-ph | we present synoptic optical photometry of hd 189733 the chromospherically active parent star of one of the most intensively studied exoplanets we have significantly extended the timespan of our previously reported observations and refined the estimate of the stellar rotation period by more than an order of magnitude p ... | [['we', 'present', 'synoptic', 'optical', 'photometry', 'of', 'hd', '189733', 'the', 'chromospherically', 'active', 'parent', 'star', 'of', 'one', 'of', 'the', 'most', 'intensively', 'studied', 'exoplanets', 'we', 'have', 'significantly', 'extended', 'the', 'timespan', 'of', 'our', 'previously', 'reported', 'observatio... | [-0.14672971339980476, 0.1503194668682654, -0.05079214522300894, 0.052156002228484905, -0.1272693934839174, -0.047796870663156174, 0.0703426685313279, 0.3929945240133857, -0.10743592721438147, -0.3772018497742443, 0.11669840692564935, -0.2548661701470973, -0.04906796449472769, 0.24420665573968317, -0.045066845249833475... |
709.2143 | Optimized Double-well quantum interferometry with Gaussian
squeezed-states | A Mach-Zender interferometer with a gaussian number-difference squeezed input
state can exhibit sub-shot-noise phase resolution over a large phase-interval.
We obtain the optimal level of squeezing for a given phase-interval
$\Delta\theta_0$ and particle number $N$, with the resulting phase-estimation
uncertainty smo... | quant-ph | a machzender interferometer with a gaussian numberdifference squeezed input state can exhibit subshotnoise phase resolution over a large phaseinterval we obtain the optimal level of squeezing for a given phaseinterval deltatheta_0 and particle number n with the resulting phaseestimation uncertainty smoothly approaching... | [['a', 'machzender', 'interferometer', 'with', 'a', 'gaussian', 'numberdifference', 'squeezed', 'input', 'state', 'can', 'exhibit', 'subshotnoise', 'phase', 'resolution', 'over', 'a', 'large', 'phaseinterval', 'we', 'obtain', 'the', 'optimal', 'level', 'of', 'squeezing', 'for', 'a', 'given', 'phaseinterval', 'deltathet... | [-0.13817666534536568, 0.20549711765014828, -0.11076523836922304, 0.006856893150446315, 0.017854402437372956, -0.20469134718959414, 0.08736570289921622, 0.36385152592908504, -0.23287148906510005, -0.3078080778941512, 0.0862646682509185, -0.2267308208186499, -0.04448076028578965, 0.2122076927953176, -0.04655976364995504... |
709.2144 | On-demand generation of entanglement of atomic qubits via optical
interferometry | The problem of on-demand generation of entanglement between single-atom
qubits via a common photonic channel is examined within the framework of
optical interferometry. As expected, for a Mach-Zehnder interferometer with
coherent laser beam as input, a high-finesse optical cavity is required to
overcome sensitivity t... | quant-ph | the problem of ondemand generation of entanglement between singleatom qubits via a common photonic channel is examined within the framework of optical interferometry as expected for a machzehnder interferometer with coherent laser beam as input a highfinesse optical cavity is required to overcome sensitivity to spontan... | [['the', 'problem', 'of', 'ondemand', 'generation', 'of', 'entanglement', 'between', 'singleatom', 'qubits', 'via', 'a', 'common', 'photonic', 'channel', 'is', 'examined', 'within', 'the', 'framework', 'of', 'optical', 'interferometry', 'as', 'expected', 'for', 'a', 'machzehnder', 'interferometer', 'with', 'coherent', ... | [-0.1043886240326051, 0.1739611099182201, -0.08294814517664398, 0.02386437556877778, 0.0014160758432892203, -0.25587076755766214, 0.07801685664885638, 0.45708220159532104, -0.22520480238678264, -0.32080468008626095, 0.07856609939206163, -0.23306018416912644, -0.09247279094862094, 0.28036212425341867, -0.059628044745022... |
709.2145 | Line emission from optically thick relativistic accretion tori | We calculate line emission from relativistic accretion tori around Kerr black
holes and investigate how the line profiles depend on the viewing inclination,
spin of the central black hole, parameters describing the shape of the tori,
and spatial distribution of line emissivity on the torus surface. We also
compare th... | astro-ph | we calculate line emission from relativistic accretion tori around kerr black holes and investigate how the line profiles depend on the viewing inclination spin of the central black hole parameters describing the shape of the tori and spatial distribution of line emissivity on the torus surface we also compare the line... | [['we', 'calculate', 'line', 'emission', 'from', 'relativistic', 'accretion', 'tori', 'around', 'kerr', 'black', 'holes', 'and', 'investigate', 'how', 'the', 'line', 'profiles', 'depend', 'on', 'the', 'viewing', 'inclination', 'spin', 'of', 'the', 'central', 'black', 'hole', 'parameters', 'describing', 'the', 'shape', ... | [-0.11224515866717917, 0.10283795966068021, -0.03374437466806694, 0.092264066327357, -0.07317918132794311, -0.1460909399375186, -0.017832454197910602, 0.4950934983372287, -0.1694184607187194, -0.31729961631635845, 0.09831560093328992, -0.2826370770161796, -0.037432037733470175, 0.20711021537207602, -0.05669006884240048... |
709.2146 | High frequency EPR on dilute solutions of the single molecule magnet
Ni$_4$ | Dilute frozen solutions of the single molecule magnet Ni$_4$ (S=4) have been
studied using high frequency D-band (130 GHz) EPR. Despite the random
orientation of the molecules, well defined EPR absorption peaks are observed,
due to the strong variation of the splittings between the different spin-states
on magnetic f... | cond-mat.other | dilute frozen solutions of the single molecule magnet ni_4 s4 have been studied using high frequency dband 130 ghz epr despite the random orientation of the molecules well defined epr absorption peaks are observed due to the strong variation of the splittings between the different spinstates on magnetic field temperatu... | [['dilute', 'frozen', 'solutions', 'of', 'the', 'single', 'molecule', 'magnet', 'ni_4', 's4', 'have', 'been', 'studied', 'using', 'high', 'frequency', 'dband', '130', 'ghz', 'epr', 'despite', 'the', 'random', 'orientation', 'of', 'the', 'molecules', 'well', 'defined', 'epr', 'absorption', 'peaks', 'are', 'observed', 'd... | [-0.13939454762491388, 0.19227912778888337, -0.0008619507670263264, 0.02359948294219848, -0.0054618666801497205, -0.14382439379571615, 0.05710153787388144, 0.4042370422508254, -0.19818843022493698, -0.36586280072556165, 0.0558364129588269, -0.29630245774914726, 0.0027363984627979936, 0.19236592999137242, 0.066654215366... |
709.2147 | Argon Abundances in the Solar Neighborhood: Non-LTE Analysis of Orion
Association B-type Stars | Argon abundances have been derived for a sample of B main-sequence stars in
the Orion association. The abundance calculations are based on NLTE metal
line-blanketed model atmospheres calculated with the NLTE code TLUSTY and an
updated and complete argon model atom. We derive an average argon abundance for
this young ... | astro-ph | argon abundances have been derived for a sample of b mainsequence stars in the orion association the abundance calculations are based on nlte metal lineblanketed model atmospheres calculated with the nlte code tlusty and an updated and complete argon model atom we derive an average argon abundance for this young popula... | [['argon', 'abundances', 'have', 'been', 'derived', 'for', 'a', 'sample', 'of', 'b', 'mainsequence', 'stars', 'in', 'the', 'orion', 'association', 'the', 'abundance', 'calculations', 'are', 'based', 'on', 'nlte', 'metal', 'lineblanketed', 'model', 'atmospheres', 'calculated', 'with', 'the', 'nlte', 'code', 'tlusty', 'a... | [0.020698126729199275, 0.13145519885994658, -0.01901844002675006, 0.06318402782525807, -0.013580458273583236, -0.06539877120126537, 0.07698604060003265, 0.41381215179378894, -0.1217239195976486, -0.3952501201753151, 0.008459531582573199, -0.28997886183865884, 0.012453033288761496, 0.17803208582740734, -0.08096545108439... |
709.2148 | New Constructions of Slice Links | We use techniques of Freedman and Teichner to prove that, under certain
circumstances, the multi-infection of a slice link is again slice (not
necessarily smoothly slice). We provide a general context for proving links are
slice that includes many of the previously known results.
| math.GT math.AT | we use techniques of freedman and teichner to prove that under certain circumstances the multiinfection of a slice link is again slice not necessarily smoothly slice we provide a general context for proving links are slice that includes many of the previously known results | [['we', 'use', 'techniques', 'of', 'freedman', 'and', 'teichner', 'to', 'prove', 'that', 'under', 'certain', 'circumstances', 'the', 'multiinfection', 'of', 'a', 'slice', 'link', 'is', 'again', 'slice', 'not', 'necessarily', 'smoothly', 'slice', 'we', 'provide', 'a', 'general', 'context', 'for', 'proving', 'links', 'ar... | [-0.15100024034117543, 0.04984870237883094, -0.13449060167510843, 0.13222300903709217, -0.10133822159408483, -0.1626220335317559, 0.03245445377691541, 0.4122466346205667, -0.2385948555067528, -0.2353218067653997, 0.1671624456770545, -0.16180969792049985, -0.18182757176285566, 0.28319010073535666, -0.16710969389871108, ... |
709.2149 | Rigid Dualizing Complexes via Differential Graded Algebras (Survey) | In this article we survey recent results on rigid dualizing complexes over
commutative algebras. We begin by recalling what are dualizing complexes. Next
we define rigid complexes, and explain their functorial properties. Due to the
possible presence of torsion, we must use differential graded algebras in the
constru... | math.AG math.AC math.CT | in this article we survey recent results on rigid dualizing complexes over commutative algebras we begin by recalling what are dualizing complexes next we define rigid complexes and explain their functorial properties due to the possible presence of torsion we must use differential graded algebras in the constructions ... | [['in', 'this', 'article', 'we', 'survey', 'recent', 'results', 'on', 'rigid', 'dualizing', 'complexes', 'over', 'commutative', 'algebras', 'we', 'begin', 'by', 'recalling', 'what', 'are', 'dualizing', 'complexes', 'next', 'we', 'define', 'rigid', 'complexes', 'and', 'explain', 'their', 'functorial', 'properties', 'due... | [-0.17047080015894814, 0.01588043232750095, -0.053817240904990425, 0.14247073598278187, -0.1142869285688224, -0.12274382799916284, -0.07584596394797341, 0.47132829975494195, -0.4598672625044702, -0.15124912487841408, 0.04754085152436205, -0.19628611195202864, -0.21220047685357046, 0.1127108610431913, -0.314427428304965... |
709.215 | A comment on "Computational periodicity as observed in a simple system,"
by Edward N. Lorenz (2006a) | This paper has been withdrawn by the authors as requested by the journal.
| nlin.CD | this paper has been withdrawn by the authors as requested by the journal | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'authors', 'as', 'requested', 'by', 'the', 'journal']] | [-0.051849561815078445, -0.0056348205902255494, -0.07618304599936192, -0.1004991584833568, -0.1393480429855677, -0.049276651814579964, 0.04166958718381535, 0.2856891883107332, -0.2531938112627428, -0.44801925466610837, 0.13133096007200387, -0.2939828304717174, -0.14337604048733527, 0.06278734553891879, -0.3007121467246... |
709.2151 | Eigenvalue estimates for the scattering problem associated to the
sine-Gordon equation | One of the difficulties associated with the scattering problems arising in
connection with integrable systems is that they are frequently
non-self-adjoint, making it difficult to determine where the spectrum lies. In
this paper, we consider the problem of locating and counting the discrete
eigenvalues associated with... | math.SP math-ph math.MP | one of the difficulties associated with the scattering problems arising in connection with integrable systems is that they are frequently nonselfadjoint making it difficult to determine where the spectrum lies in this paper we consider the problem of locating and counting the discrete eigenvalues associated with the sc... | [['one', 'of', 'the', 'difficulties', 'associated', 'with', 'the', 'scattering', 'problems', 'arising', 'in', 'connection', 'with', 'integrable', 'systems', 'is', 'that', 'they', 'are', 'frequently', 'nonselfadjoint', 'making', 'it', 'difficult', 'to', 'determine', 'where', 'the', 'spectrum', 'lies', 'in', 'this', 'pap... | [-0.11961275836260961, 0.09949393503864568, -0.07949967424960891, 0.06779506860298559, -0.08182380858916397, -0.1258419857093662, -0.011774568582168925, 0.35147097618693496, -0.28540807974585636, -0.22835854727110297, 0.13917592212548432, -0.3209986796172046, -0.19796939711460854, 0.1876191310526045, -0.069194133440266... |
709.2152 | Heating Hot Atmospheres with Active Galactic Nuclei | High resolution X-ray spectroscopy of the hot gas in galaxy clusters has
shown that the gas is not cooling to low temperatures at the predicted rates of
hundreds to thousands of solar masses per year. X-ray images have revealed
giant cavities and shock fronts in the hot gas that provide a direct and
relatively reliab... | astro-ph | high resolution xray spectroscopy of the hot gas in galaxy clusters has shown that the gas is not cooling to low temperatures at the predicted rates of hundreds to thousands of solar masses per year xray images have revealed giant cavities and shock fronts in the hot gas that provide a direct and relatively reliable me... | [['high', 'resolution', 'xray', 'spectroscopy', 'of', 'the', 'hot', 'gas', 'in', 'galaxy', 'clusters', 'has', 'shown', 'that', 'the', 'gas', 'is', 'not', 'cooling', 'to', 'low', 'temperatures', 'at', 'the', 'predicted', 'rates', 'of', 'hundreds', 'to', 'thousands', 'of', 'solar', 'masses', 'per', 'year', 'xray', 'image... | [-0.06374489145657761, 0.18954300026930665, -0.014122513212698876, 0.11796704806139409, -0.09462649463777147, -0.05687469966790598, 0.04674027575706334, 0.4323321065723734, -0.17932975763687864, -0.3686420088330203, 0.0434026258710377, -0.32167688244036347, 0.04664885860098445, 0.22523586772795962, 0.01212891666016177,... |
709.2153 | Generalized Vandermonde's system and Lagrange's interpolation | We give explicit formulas as well as a quadratic time algorithm to solve (so
called) generalized Vandermonde's systems of p linear equations and n
variables. It allows in particular to find all (so called Lagrange's)
interpolation polynoms with degree n-1 taking given values in p distinct
points.
| math.NA | we give explicit formulas as well as a quadratic time algorithm to solve so called generalized vandermondes systems of p linear equations and n variables it allows in particular to find all so called lagranges interpolation polynoms with degree n1 taking given values in p distinct points | [['we', 'give', 'explicit', 'formulas', 'as', 'well', 'as', 'a', 'quadratic', 'time', 'algorithm', 'to', 'solve', 'so', 'called', 'generalized', 'vandermondes', 'systems', 'of', 'p', 'linear', 'equations', 'and', 'n', 'variables', 'it', 'allows', 'in', 'particular', 'to', 'find', 'all', 'so', 'called', 'lagranges', 'in... | [-0.1511068449732154, 0.08628378119914139, -0.07681124207583513, 0.06537923617090316, -0.10736741810204818, -0.2192543698375688, 0.037540948018431664, 0.2866540899936189, -0.2982566711750436, -0.30036768418281, 0.04193752580520479, -0.24111954415584866, -0.20006282283290427, 0.17021960043843756, -0.039886391492240984, ... |
709.2154 | The AMS-RICH velocity and charge reconstruction | The AMS detector, to be installed on the International Space Station,
includes a Ring Imaging Cerenkov detector with two different radiators, silica
aerogel (n=1.05) and sodium fluoride (n=1.334). This detector is designed to
provide very precise measurements of velocity and electric charge in a wide
range of cosmic ... | astro-ph | the ams detector to be installed on the international space station includes a ring imaging cerenkov detector with two different radiators silica aerogel n105 and sodium fluoride n1334 this detector is designed to provide very precise measurements of velocity and electric charge in a wide range of cosmic nuclei energie... | [['the', 'ams', 'detector', 'to', 'be', 'installed', 'on', 'the', 'international', 'space', 'station', 'includes', 'a', 'ring', 'imaging', 'cerenkov', 'detector', 'with', 'two', 'different', 'radiators', 'silica', 'aerogel', 'n105', 'and', 'sodium', 'fluoride', 'n1334', 'this', 'detector', 'is', 'designed', 'to', 'prov... | [-0.06831090017313775, 0.16323990485091744, -0.05827758648420537, 0.03560305678432709, -0.03172463389101291, -0.16032454935990054, -0.030808734026657857, 0.40926682368521333, -0.1821493709913308, -0.3920932701102605, 0.08399341060277565, -0.30463811850763467, -0.0032300081986345744, 0.23636070669607234, -0.051840014501... |
709.2155 | A general learning algorithm for functions between metric spaces | In this paper we show how to approximate ("learn") a function f, where X and
Y are metric spaces.
| math.FA math.GM | in this paper we show how to approximate learn a function f where x and y are metric spaces | [['in', 'this', 'paper', 'we', 'show', 'how', 'to', 'approximate', 'learn', 'a', 'function', 'f', 'where', 'x', 'and', 'y', 'are', 'metric', 'spaces']] | [-0.08298844961743605, 0.054806141268559976, -0.11263513839558552, 0.11309953050467332, -0.08298754385721527, -0.11303156572639157, 0.048716629371292106, 0.4986174308547848, -0.372486543890677, -0.2454442860264527, 0.015152260654998062, -0.2815650899551417, -0.2710922191801824, 0.101304244544161, -0.15341979672053926, ... |
709.2156 | The Candy-Passing Game for c\geq3n-2 | We determine the behavior of Tanton's candy-passing game for all
distributions of at least 3n-2 candies, where n is the number of students.
Specifically, we show that the configuration of candy in such a game eventually
becomes fixed.
| math.CO | we determine the behavior of tantons candypassing game for all distributions of at least 3n2 candies where n is the number of students specifically we show that the configuration of candy in such a game eventually becomes fixed | [['we', 'determine', 'the', 'behavior', 'of', 'tantons', 'candypassing', 'game', 'for', 'all', 'distributions', 'of', 'at', 'least', '3n2', 'candies', 'where', 'n', 'is', 'the', 'number', 'of', 'students', 'specifically', 'we', 'show', 'that', 'the', 'configuration', 'of', 'candy', 'in', 'such', 'a', 'game', 'eventuall... | [-0.13532584966034503, 0.15447477792465203, -0.10920577578095568, 0.04914153482123102, -0.0003309891625257159, -0.170666995118498, 0.052647460384193705, 0.3421785830444581, -0.23414406060820092, -0.32335218941050303, 0.07459923673760951, -0.333103023066714, -0.15020587623144524, 0.07647685767025561, -0.0571406498878590... |
709.2157 | Spontaneous Transverse Response and Amplified Switching in
Superconductors with Honeycomb Pinning Arrays | Using numerical simulations, we show that a novel spontaneous transverse
response can appear when a longitudinal drive is applied to type-II
superconductors with honeycomb pinning arrays in a magnetic field near certain
filling fractions. This response is generated by dynamical symmetry breaking
that occurs at fields... | cond-mat.supr-con | using numerical simulations we show that a novel spontaneous transverse response can appear when a longitudinal drive is applied to typeii superconductors with honeycomb pinning arrays in a magnetic field near certain filling fractions this response is generated by dynamical symmetry breaking that occurs at fields away... | [['using', 'numerical', 'simulations', 'we', 'show', 'that', 'a', 'novel', 'spontaneous', 'transverse', 'response', 'can', 'appear', 'when', 'a', 'longitudinal', 'drive', 'is', 'applied', 'to', 'typeii', 'superconductors', 'with', 'honeycomb', 'pinning', 'arrays', 'in', 'a', 'magnetic', 'field', 'near', 'certain', 'fil... | [-0.2012648144644676, 0.2632976624399186, -0.045860794442014234, 0.05147088327592626, -0.11994644625130857, -0.13312904035677156, 0.01390870986045292, 0.431748296217163, -0.30312512918274004, -0.2520068864716162, 0.0617579876256203, -0.2303383937520482, -0.1599177757397958, 0.2430959516527629, -0.003231284107164581, -0... |
709.2158 | Branes, Anti-Branes and Brauer Algebras in Gauge-Gravity duality | We propose gauge theory operators built using a complex Matrix scalar which
are dual to brane-anti-brane systems in $AdS_5 \times S^5 $, in the zero
coupling limit of the dual Yang-Mills. The branes involved are half-BPS giant
gravitons. The proposed operators dual to giant-anti-giant configurations
satisfy the appro... | hep-th math.RT | we propose gauge theory operators built using a complex matrix scalar which are dual to braneantibrane systems in ads_5 times s5 in the zero coupling limit of the dual yangmills the branes involved are halfbps giant gravitons the proposed operators dual to giantantigiant configurations satisfy the appropriate orthogona... | [['we', 'propose', 'gauge', 'theory', 'operators', 'built', 'using', 'a', 'complex', 'matrix', 'scalar', 'which', 'are', 'dual', 'to', 'braneantibrane', 'systems', 'in', 'ads_5', 'times', 's5', 'in', 'the', 'zero', 'coupling', 'limit', 'of', 'the', 'dual', 'yangmills', 'the', 'branes', 'involved', 'are', 'halfbps', 'gi... | [-0.14384416866503794, 0.17939963949821103, -0.07470298506267462, 0.1144457786960053, -0.06364451325498521, -0.10719196697673905, -0.016331105950716535, 0.28706721939227503, -0.19870416774929311, -0.23113719931578044, 0.08122995709826858, -0.287994376187045, -0.18024354304696047, 0.10659900044021631, -0.053609440158127... |
709.2159 | On the application of the Critical Minimum Energy Subspace method to
disordered systems | We discuss the recent application to strongly disordered systems of the
Critical Minimum Energy Subspace (CMES) method, used to limit the energy
subspace of the Wang-Landau sampling. We compare with our results on the 3D
Random Field Ising Model obtained by a multi-range Wang-Landau simulation in
the whole energy ran... | cond-mat.stat-mech cond-mat.dis-nn | we discuss the recent application to strongly disordered systems of the critical minimum energy subspace cmes method used to limit the energy subspace of the wanglandau sampling we compare with our results on the 3d random field ising model obtained by a multirange wanglandau simulation in the whole energy range we poi... | [['we', 'discuss', 'the', 'recent', 'application', 'to', 'strongly', 'disordered', 'systems', 'of', 'the', 'critical', 'minimum', 'energy', 'subspace', 'cmes', 'method', 'used', 'to', 'limit', 'the', 'energy', 'subspace', 'of', 'the', 'wanglandau', 'sampling', 'we', 'compare', 'with', 'our', 'results', 'on', 'the', '3d... | [-0.10842894843301258, 0.1424358128507093, -0.05603267694508808, 0.11235455856532664, -0.014681832846002402, -0.0907699454802315, 0.07046460773091058, 0.3987611179409951, -0.26152027171809933, -0.3095848597712009, 0.07672825086754873, -0.24849938900788893, -0.1249329073958703, 0.22476669399357224, -0.02286955663254736,... |
709.216 | High-spin binary black hole mergers | We study identical mass black hole binaries with spins perpendicular to the
binary's orbital plane. These binaries have individual spins ranging from
$s/m^2=-0.90$ to 0.90, ($s_1 = s_2$ in all cases) which is near the limit
possible with standard Bowen-York puncture initial data. The extreme cases
correspond to the l... | gr-qc | we study identical mass black hole binaries with spins perpendicular to the binarys orbital plane these binaries have individual spins ranging from sm2090 to 090 s_1 s_2 in all cases which is near the limit possible with standard bowenyork puncture initial data the extreme cases correspond to the largest initial spin s... | [['we', 'study', 'identical', 'mass', 'black', 'hole', 'binaries', 'with', 'spins', 'perpendicular', 'to', 'the', 'binarys', 'orbital', 'plane', 'these', 'binaries', 'have', 'individual', 'spins', 'ranging', 'from', 'sm2090', 'to', '090', 's_1', 's_2', 'in', 'all', 'cases', 'which', 'is', 'near', 'the', 'limit', 'possi... | [-0.1136454549769676, 0.13374836041498206, -0.014440195079055406, 0.06680532991831992, -0.042220786466108016, -0.10845894718817038, 0.0543897019648679, 0.3607893733979138, -0.17765234697740093, -0.3606346012237518, 0.12498469155032707, -0.3506601451166956, -0.00013445845494667688, 0.24558705020724803, -0.02169921095013... |
709.2161 | Hyperbolic Unit Groups and Quaternion Algebras | We Classify the rational quadratic extensions K and the finite groups G for
which the group ring R[G] of G over the ring R of integers of K has the
property that the group of units of augmentation 1 of R[G] is hyperbolic. We
also construct units in a non-split quaternion algebra over R.
| math.RA math.GR | we classify the rational quadratic extensions k and the finite groups g for which the group ring rg of g over the ring r of integers of k has the property that the group of units of augmentation 1 of rg is hyperbolic we also construct units in a nonsplit quaternion algebra over r | [['we', 'classify', 'the', 'rational', 'quadratic', 'extensions', 'k', 'and', 'the', 'finite', 'groups', 'g', 'for', 'which', 'the', 'group', 'ring', 'rg', 'of', 'g', 'over', 'the', 'ring', 'r', 'of', 'integers', 'of', 'k', 'has', 'the', 'property', 'that', 'the', 'group', 'of', 'units', 'of', 'augmentation', '1', 'of'... | [-0.2750326670292351, 0.05514913423124839, -0.13339412212371826, -0.06539587671997854, -0.10209093994840428, -0.14632699520465126, -0.01575480922366734, 0.3716933588600821, -0.37724915326193525, -0.20087739328543344, 0.07947912993970224, -0.26128438653217423, -0.1172019691309995, 0.17483274050539843, -0.062050385279925... |
709.2162 | Closed-String Tachyon Condensation and the Worldsheet Super-Higgs Effect | Alternative gauge choices for worldsheet supersymmetry can elucidate
dynamical phenomena obscured in the usual superconformal gauge. In the
particular example of the tachyonic $E_8$ heterotic string, we use a judicious
gauge choice to show that the process of closed-string tachyon condensation can
be understood in te... | hep-th | alternative gauge choices for worldsheet supersymmetry can elucidate dynamical phenomena obscured in the usual superconformal gauge in the particular example of the tachyonic e_8 heterotic string we use a judicious gauge choice to show that the process of closedstring tachyon condensation can be understood in terms of ... | [['alternative', 'gauge', 'choices', 'for', 'worldsheet', 'supersymmetry', 'can', 'elucidate', 'dynamical', 'phenomena', 'obscured', 'in', 'the', 'usual', 'superconformal', 'gauge', 'in', 'the', 'particular', 'example', 'of', 'the', 'tachyonic', 'e_8', 'heterotic', 'string', 'we', 'use', 'a', 'judicious', 'gauge', 'cho... | [-0.1672700786058017, 0.2947708402734092, -0.09883331975729114, 0.1908643558666958, -0.18438477675155016, -0.17214239055199, -0.036752865898986936, 0.3422151452428858, -0.18667643126362646, -0.21115816467192391, 0.05836681994891555, -0.18752457006690157, -0.2055568412392282, 0.03645086245739203, -0.07974337559508186, -... |
709.2163 | Neutrino Oscillation Observables from Mass Matrix Structure | We present a systematic procedure to establish a connection between complex
neutrino mass matrix textures and experimental observables, including the Dirac
CP phase. In addition, we illustrate how future experimental measurements
affect the selection of textures in the (theta_13,delta_CP)-plane. For the
mixing angles... | hep-ph | we present a systematic procedure to establish a connection between complex neutrino mass matrix textures and experimental observables including the dirac cp phase in addition we illustrate how future experimental measurements affect the selection of textures in the theta_13delta_cpplane for the mixing angles we use ge... | [['we', 'present', 'a', 'systematic', 'procedure', 'to', 'establish', 'a', 'connection', 'between', 'complex', 'neutrino', 'mass', 'matrix', 'textures', 'and', 'experimental', 'observables', 'including', 'the', 'dirac', 'cp', 'phase', 'in', 'addition', 'we', 'illustrate', 'how', 'future', 'experimental', 'measurements'... | [-0.13252590780156542, 0.19156092432044122, -0.020279613886352466, 0.09763961003931321, -0.07042768287836858, -0.13831768439191838, 0.10611434742788096, 0.36595595518693974, -0.25678832728577694, -0.33935694703427344, 0.07022921896600368, -0.26579312521802345, -0.14839418267466775, 0.14725930992635372, 0.02302988609299... |
709.2164 | Extra dimensions, orthopositronium decay, and stellar cooling | In a class of extra dimensional models with a warped metric and a single
brane the photon can be localized on the brane by gravity only. An intriguing
feature of these models is the possibility of the photon escaping into the
extra dimensions. The search for this effect has motivated the present round of
precision or... | hep-ph astro-ph hep-ex hep-th | in a class of extra dimensional models with a warped metric and a single brane the photon can be localized on the brane by gravity only an intriguing feature of these models is the possibility of the photon escaping into the extra dimensions the search for this effect has motivated the present round of precision orthop... | [['in', 'a', 'class', 'of', 'extra', 'dimensional', 'models', 'with', 'a', 'warped', 'metric', 'and', 'a', 'single', 'brane', 'the', 'photon', 'can', 'be', 'localized', 'on', 'the', 'brane', 'by', 'gravity', 'only', 'an', 'intriguing', 'feature', 'of', 'these', 'models', 'is', 'the', 'possibility', 'of', 'the', 'photon... | [-0.08692313162027858, 0.18014586884831563, -0.05819672373860764, 0.07701288790946516, -0.04410256087624778, -0.10546301361949494, 0.07012505792663433, 0.3357279135069499, -0.21148297322603563, -0.29545074556566153, 0.06797846509434749, -0.2732293444064756, -0.056529296261336036, 0.22048665612237528, -0.002176532777957... |
709.2165 | Lighting the Universe with filaments | The first stars in the Universe form when chemically pristine gas heats as it
falls into dark matter potential wells, cools radiatively due to the formation
of molecular hydrogen, and becomes self-gravitating. We demonstrate with
super-computer simulations that their properties depend critically on the
currently unkn... | astro-ph hep-ph hep-th | the first stars in the universe form when chemically pristine gas heats as it falls into dark matter potential wells cools radiatively due to the formation of molecular hydrogen and becomes selfgravitating we demonstrate with supercomputer simulations that their properties depend critically on the currently unknown nat... | [['the', 'first', 'stars', 'in', 'the', 'universe', 'form', 'when', 'chemically', 'pristine', 'gas', 'heats', 'as', 'it', 'falls', 'into', 'dark', 'matter', 'potential', 'wells', 'cools', 'radiatively', 'due', 'to', 'the', 'formation', 'of', 'molecular', 'hydrogen', 'and', 'becomes', 'selfgravitating', 'we', 'demonstra... | [-0.09729400271718422, 0.23829335130365759, -0.07468050779004036, 0.12206511756341006, -0.09568008604893011, -0.013299557495990703, 0.007842361551291983, 0.332879295983705, -0.16885538543494225, -0.367193080077012, 0.014146367917319054, -0.26841247492180814, 0.0022241799867358703, 0.1450274760738529, 0.0568710714321712... |
709.2166 | Supercritical N = 2 string theory | The N=2 string is examined in dimensions above the critical dimension (D=4)
in a linear dilaton background. We demonstrate that string states in this
background propagate in a single physical time dimension, as opposed to two
such dimensions present when the dilaton gradient vanishes in D=4. We also find
exact soluti... | hep-th | the n2 string is examined in dimensions above the critical dimension d4 in a linear dilaton background we demonstrate that string states in this background propagate in a single physical time dimension as opposed to two such dimensions present when the dilaton gradient vanishes in d4 we also find exact solutions descri... | [['the', 'n2', 'string', 'is', 'examined', 'in', 'dimensions', 'above', 'the', 'critical', 'dimension', 'd4', 'in', 'a', 'linear', 'dilaton', 'background', 'we', 'demonstrate', 'that', 'string', 'states', 'in', 'this', 'background', 'propagate', 'in', 'a', 'single', 'physical', 'time', 'dimension', 'as', 'opposed', 'to... | [-0.12709875039054433, 0.22894211311865112, -0.017927064141933468, 0.12454390429311256, -0.004462058426461358, -0.19829403844736246, 0.0060789694645158624, 0.27397521825480287, -0.18737801590907402, -0.22721494047268145, 0.044981506104797016, -0.2898379291367272, -0.19416781109960182, 0.07360439661188402, -0.0163194990... |
709.2167 | The Lifetime of FRIIs in Groups and Clusters: Implications for
Radio-Mode Feedback | We determine the maximum lifetime t_max of 52 FRII radio sources found in 26
central group galaxies from cross correlation of the Berlind SDSS group catalog
with the VLA FIRST survey. Mock catalogs of FRII sources were produced to match
the selection criteria of FIRST and the redshift distribution of our parent
sampl... | astro-ph | we determine the maximum lifetime t_max of 52 frii radio sources found in 26 central group galaxies from cross correlation of the berlind sdss group catalog with the vla first survey mock catalogs of frii sources were produced to match the selection criteria of first and the redshift distribution of our parent sample w... | [['we', 'determine', 'the', 'maximum', 'lifetime', 't_max', 'of', '52', 'frii', 'radio', 'sources', 'found', 'in', '26', 'central', 'group', 'galaxies', 'from', 'cross', 'correlation', 'of', 'the', 'berlind', 'sdss', 'group', 'catalog', 'with', 'the', 'vla', 'first', 'survey', 'mock', 'catalogs', 'of', 'frii', 'sources... | [-0.07492588831455418, 0.11093594619179432, -0.048805517900945505, 0.11289609537312859, -0.07093529731214962, -0.04723338517559521, 0.06411188267775926, 0.45277369375291626, -0.15636953954756455, -0.35906387541214363, 0.07164275801379087, -0.2885571071097378, 0.02034884230631992, 0.20934127409137754, 0.0102454621401991... |
709.2168 | Bright branes for strongly coupled plasmas | We use holographic techniques to study photon production in a class of finite
temperature, strongly coupled, large-Nc SU(Nc) quark-gluon plasmas with Nf <<
Nc quark flavours. Our results are valid to leading order in the
electromagnetic coupling constant but non-perturbatively in the SU(Nc)
interactions. The spectral... | hep-th | we use holographic techniques to study photon production in a class of finite temperature strongly coupled largenc sunc quarkgluon plasmas with nf nc quark flavours our results are valid to leading order in the electromagnetic coupling constant but nonperturbatively in the sunc interactions the spectral function of ele... | [['we', 'use', 'holographic', 'techniques', 'to', 'study', 'photon', 'production', 'in', 'a', 'class', 'of', 'finite', 'temperature', 'strongly', 'coupled', 'largenc', 'sunc', 'quarkgluon', 'plasmas', 'with', 'nf', 'nc', 'quark', 'flavours', 'our', 'results', 'are', 'valid', 'to', 'leading', 'order', 'in', 'the', 'elec... | [-0.11746089457377017, 0.2989990739047893, -0.07236473159274909, 0.10155459147478853, -0.04280377945003958, -0.11881835885684598, 0.02072917557829483, 0.36796536745334213, -0.14229817802159042, -0.23713973703395044, -0.024414295084206023, -0.29556100075314573, -0.04516809469983949, 0.14790510585797684, 0.07573996567735... |
709.2169 | Basins of attraction of a nonlinear nanomechanical resonator | We present an experiment that systematically probes the basins of attraction
of two fixed points of a nonlinear nanomechanical resonator and maps them out
with high resolution. We observe a separatrix which progressively alters shape
for varying drive strength and changes the relative areas of the two basins of
attra... | cond-mat.mes-hall | we present an experiment that systematically probes the basins of attraction of two fixed points of a nonlinear nanomechanical resonator and maps them out with high resolution we observe a separatrix which progressively alters shape for varying drive strength and changes the relative areas of the two basins of attracti... | [['we', 'present', 'an', 'experiment', 'that', 'systematically', 'probes', 'the', 'basins', 'of', 'attraction', 'of', 'two', 'fixed', 'points', 'of', 'a', 'nonlinear', 'nanomechanical', 'resonator', 'and', 'maps', 'them', 'out', 'with', 'high', 'resolution', 'we', 'observe', 'a', 'separatrix', 'which', 'progressively',... | [-0.15238170044153537, 0.14306283993432053, -0.10447351771749948, 0.07682054812260168, 0.05372113710710485, -0.10762278262623831, 0.060231635123981456, 0.347335325720671, -0.2820938213875419, -0.28344771132657404, 0.016778566896621334, -0.2917117395781373, -0.13065092504808778, 0.1768136656401973, -0.04004177148331349,... |
709.217 | Physical Degrees of Freedom of the Relativistic Fluid on K\"{a}hler
Manifolds in the Symplectic Projector Approach | The paper has been withdrawn because of a more complete analysis of the
relativistic fluid including the quantization reported in arxiv:0801.3032
[hep-th].
| hep-th | the paper has been withdrawn because of a more complete analysis of the relativistic fluid including the quantization reported in arxiv08013032 hepth | [['the', 'paper', 'has', 'been', 'withdrawn', 'because', 'of', 'a', 'more', 'complete', 'analysis', 'of', 'the', 'relativistic', 'fluid', 'including', 'the', 'quantization', 'reported', 'in', 'arxiv08013032', 'hepth']] | [-0.13134448347236252, 0.01186971707890431, -0.15457907948820365, -0.01901395543522778, -0.08057769875796068, -0.09536364149036151, -0.05865403219857918, 0.2684552885946773, -0.12158301401705969, -0.32374657850180355, 0.04999766065849967, -0.29512378041233334, -0.12946697603911161, 0.1267022646608807, -0.14888071885243... |
709.2171 | Inverse spectral problems on a closed manifold | In this paper we consider two inverse problems on a closed connected
Riemannian manifold $(M,g)$. The first one is a direct analog of the Gel'fand
inverse boundary spectral problem. To formulate it, assume that $M$ is divided
by a hypersurface $\Sigma$ into two components and we know the eigenvalues
$\lambda_j$ of th... | math.AP math.DG | in this paper we consider two inverse problems on a closed connected riemannian manifold mg the first one is a direct analog of the gelfand inverse boundary spectral problem to formulate it assume that m is divided by a hypersurface sigma into two components and we know the eigenvalues lambda_j of the laplace operator ... | [['in', 'this', 'paper', 'we', 'consider', 'two', 'inverse', 'problems', 'on', 'a', 'closed', 'connected', 'riemannian', 'manifold', 'mg', 'the', 'first', 'one', 'is', 'a', 'direct', 'analog', 'of', 'the', 'gelfand', 'inverse', 'boundary', 'spectral', 'problem', 'to', 'formulate', 'it', 'assume', 'that', 'm', 'is', 'di... | [-0.1195073745540947, 0.09789429589919554, -0.019441699847108224, 0.07355236221337691, -0.07310110765284153, -0.15818601644567246, -0.01093209106449529, 0.3719434886902141, -0.2730924406262872, -0.2612740624757422, 0.15274845472163429, -0.3207505273499659, -0.10324624566243613, 0.18306857307830438, -0.05007633638368653... |
709.2172 | The influence of metallic particle size on the mechanical properties of
PTFE-Al-W powder composites | The dynamic mechanical properties of reactive materials (e.g., high density
mixtures of polytetraflouroethylene (PTFE), aluminum (Al) and tungsten (W)
powders) can be tailored by changing the morphology of the particles and
porosity. Cold isostatically pressed PTFE-Al-W powder composites with fine
metallic particles ... | cond-mat.soft cond-mat.mtrl-sci | the dynamic mechanical properties of reactive materials eg high density mixtures of polytetraflouroethylene ptfe aluminum al and tungsten w powders can be tailored by changing the morphology of the particles and porosity cold isostatically pressed ptfealw powder composites with fine metallic particles and a higher poro... | [['the', 'dynamic', 'mechanical', 'properties', 'of', 'reactive', 'materials', 'eg', 'high', 'density', 'mixtures', 'of', 'polytetraflouroethylene', 'ptfe', 'aluminum', 'al', 'and', 'tungsten', 'w', 'powders', 'can', 'be', 'tailored', 'by', 'changing', 'the', 'morphology', 'of', 'the', 'particles', 'and', 'porosity', '... | [-0.056327992469293646, 0.3104989629012353, -0.030328899349943542, -0.026527030242487124, -0.008488469356025504, -0.1747047528901165, 0.03366281900849968, 0.4334384358423476, -0.250619533978919, -0.33583516067373426, 0.026758574172946633, -0.2823997938101835, -0.09643688761066682, 0.09546953098534948, 1.192519828529641... |
709.2173 | Stabilization for mapping class groups of 3-manifolds | We prove that the homology of the mapping class group of any 3-manifold
stabilizes under connected sum and boundary connected sum with an arbitrary
3-manifold when both manifolds are compact and orientable. The stabilization
also holds for the quotient group by twists along spheres and disks, and
includes as particul... | math.GT math.AT | we prove that the homology of the mapping class group of any 3manifold stabilizes under connected sum and boundary connected sum with an arbitrary 3manifold when both manifolds are compact and orientable the stabilization also holds for the quotient group by twists along spheres and disks and includes as particular cas... | [['we', 'prove', 'that', 'the', 'homology', 'of', 'the', 'mapping', 'class', 'group', 'of', 'any', '3manifold', 'stabilizes', 'under', 'connected', 'sum', 'and', 'boundary', 'connected', 'sum', 'with', 'an', 'arbitrary', '3manifold', 'when', 'both', 'manifolds', 'are', 'compact', 'and', 'orientable', 'the', 'stabilizat... | [-0.20316049897057167, 0.11545740276838735, -0.04363886900246143, 0.02607901747174123, -0.08640062486862435, -0.1629064545583199, -0.03532825150691411, 0.38120376038200715, -0.2948465912383707, -0.24243765399407816, 0.16175422951003865, -0.2514329983140616, -0.137533135775148, 0.2212795436163159, -0.16234441997812074, ... |
709.2174 | Topological rigidity for holomorphic foliations | We study analytic deformations and unfoldings of holomorphic foliations in
complex projective plane $\mathbb{C}P(2)$. Let $\{\mathcal{F}_t\}_{t \in
\mathbb{D}_{\epsilon}}$ be topological trivial (in $\mathbb{C}^2$) analytic
deformation of a foliation $\mathcal{F}_0$ on $\mathbb{C}^2$. We show that
under some dynamica... | math.DS math.CV | we study analytic deformations and unfoldings of holomorphic foliations in complex projective plane mathbbcp2 let mathcalf_t_t in mathbbd_epsilon be topological trivial in mathbbc2 analytic deformation of a foliation mathcalf_0 on mathbbc2 we show that under some dynamical restriction on mathcalf_0 we have two possibil... | [['we', 'study', 'analytic', 'deformations', 'and', 'unfoldings', 'of', 'holomorphic', 'foliations', 'in', 'complex', 'projective', 'plane', 'mathbbcp2', 'let', 'mathcalf_t_t', 'in', 'mathbbd_epsilon', 'be', 'topological', 'trivial', 'in', 'mathbbc2', 'analytic', 'deformation', 'of', 'a', 'foliation', 'mathcalf_0', 'on... | [-0.24848944361049993, 0.036528322095212694, -0.13812314570047116, 0.04847254892471634, -0.10582117012624319, -0.12426649468761752, -0.03809440739223646, 0.38190426962197915, -0.3051428635371849, -0.1116241821970713, 0.10141957411906333, -0.2768861186632421, -0.18821773513385173, 0.2088980496652463, -0.1070705922223472... |
709.2175 | Electric-Magnetic Struggle in QGP, Deconfinement and Baryons | We argue that quite unusual properties of Quark-Gluon Plasma in the RHIC
temperature domain $T=(1-2)T_c$ are consequences of the approximate equilibrium
between electric and magnetic sectors reached above the deconfinement
temperature. Already classical study of few body motion in a electric-magnetic
plasma shows abn... | hep-ph | we argue that quite unusual properties of quarkgluon plasma in the rhic temperature domain t12t_c are consequences of the approximate equilibrium between electric and magnetic sectors reached above the deconfinement temperature already classical study of few body motion in a electricmagnetic plasma shows abnormally lar... | [['we', 'argue', 'that', 'quite', 'unusual', 'properties', 'of', 'quarkgluon', 'plasma', 'in', 'the', 'rhic', 'temperature', 'domain', 't12t_c', 'are', 'consequences', 'of', 'the', 'approximate', 'equilibrium', 'between', 'electric', 'and', 'magnetic', 'sectors', 'reached', 'above', 'the', 'deconfinement', 'temperature... | [-0.10371691694560188, 0.25587194698645654, -0.1072843740729237, 0.13669844025910544, -0.07999781500268027, -0.14864066518191948, 0.038510425919596865, 0.3736522692654814, -0.23031338631294498, -0.27465000124017996, 0.043865962026647776, -0.29764811407172476, -0.04527641217490392, 0.1307655555971625, 0.0103373870435625... |
709.2176 | Electronic pathway in the photosynthetic reaction centers and some
mutation of RC's | The reaction center of Chloroflexus aurantiacus and Rhodobacter sphaeroides
mutation of RC`s was investigated. To describe the kinetic of the Chloroflexus
aurantiacus RC's we use incoherent model of electron transfer. It was shown
that the asymmetry in electronic coupling must be included to explain the
experiments. ... | cond-mat.soft cond-mat.other | the reaction center of chloroflexus aurantiacus and rhodobacter sphaeroides mutation of rcs was investigated to describe the kinetic of the chloroflexus aurantiacus rcs we use incoherent model of electron transfer it was shown that the asymmetry in electronic coupling must be included to explain the experiments for the... | [['the', 'reaction', 'center', 'of', 'chloroflexus', 'aurantiacus', 'and', 'rhodobacter', 'sphaeroides', 'mutation', 'of', 'rcs', 'was', 'investigated', 'to', 'describe', 'the', 'kinetic', 'of', 'the', 'chloroflexus', 'aurantiacus', 'rcs', 'we', 'use', 'incoherent', 'model', 'of', 'electron', 'transfer', 'it', 'was', '... | [-0.05839297948405146, 0.17755947707220912, -0.05781117281207116, 0.16691147000179626, -0.0032805015332996847, -0.16290021685650571, 0.01530764864757657, 0.40863773407414555, -0.2788378469878808, -0.2457516910880804, 0.010411997054470703, -0.24007994825951756, -0.13796108529902995, 0.2123192560253665, -0.01059886130504... |
709.2177 | Fragmentation cross-sections and binding energies of neutron-rich nuclei | An exponential dependence of the fragmentation cross-section on the average
binding energy is observed and reproduced with a statistical model. The
observed functional dependence is robust and allows the extraction of binding
energies from measured cross-sections. From the systematics of 75,77,78,79Cu
isotope cross-s... | nucl-ex | an exponential dependence of the fragmentation crosssection on the average binding energy is observed and reproduced with a statistical model the observed functional dependence is robust and allows the extraction of binding energies from measured crosssections from the systematics of 75777879cu isotope crosssections ha... | [['an', 'exponential', 'dependence', 'of', 'the', 'fragmentation', 'crosssection', 'on', 'the', 'average', 'binding', 'energy', 'is', 'observed', 'and', 'reproduced', 'with', 'a', 'statistical', 'model', 'the', 'observed', 'functional', 'dependence', 'is', 'robust', 'and', 'allows', 'the', 'extraction', 'of', 'binding'... | [0.0025911171495625117, 0.20900176297005796, -0.052382658891271326, 0.15267191881662034, 0.047547189587754314, -0.08088355737023996, 0.06992386918948981, 0.3952517959027036, -0.1766001695486744, -0.3980555814482923, -0.04672568864799421, -0.3890414243696531, 0.08891247159652231, 0.18678815438394045, 0.06481976086472713... |
709.2178 | Long Memory and Volatility Clustering: is the empirical evidence
consistent across stock markets? | Long memory and volatility clustering are two stylized facts frequently
related to financial markets. Traditionally, these phenomena have been studied
based on conditionally heteroscedastic models like ARCH, GARCH, IGARCH and
FIGARCH, inter alia. One advantage of these models is their ability to capture
nonlinear dyn... | q-fin.ST physics.soc-ph | long memory and volatility clustering are two stylized facts frequently related to financial markets traditionally these phenomena have been studied based on conditionally heteroscedastic models like arch garch igarch and figarch inter alia one advantage of these models is their ability to capture nonlinear dynamics an... | [['long', 'memory', 'and', 'volatility', 'clustering', 'are', 'two', 'stylized', 'facts', 'frequently', 'related', 'to', 'financial', 'markets', 'traditionally', 'these', 'phenomena', 'have', 'been', 'studied', 'based', 'on', 'conditionally', 'heteroscedastic', 'models', 'like', 'arch', 'garch', 'igarch', 'and', 'figar... | [-0.03899361817305213, 0.08739618120242411, -0.12009592497471108, 0.18760982302535298, -0.050623364433813, -0.1331232208202579, 0.018676348455396216, 0.39600084819344444, -0.2744261086709909, -0.2579823857479131, 0.14758902633868493, -0.35220904388367685, -0.15864065889991932, 0.21262994765498633, -0.1108569190802692, ... |
709.2179 | Role of electrostatic forces in cluster formation in a dry ionomer | This simulation study investigates the dependence of the structure of dry
Nafion$^{\tiny\textregistered}$-like ionomers on the electrostatic interactions
between the components of the molecules. In order to speed equilibration, a
procedure was adopted which involved detaching the side chains from the
backbone and cut... | cond-mat.soft cond-mat.mtrl-sci | this simulation study investigates the dependence of the structure of dry nafiontinytextregisteredlike ionomers on the electrostatic interactions between the components of the molecules in order to speed equilibration a procedure was adopted which involved detaching the side chains from the backbone and cutting the bac... | [['this', 'simulation', 'study', 'investigates', 'the', 'dependence', 'of', 'the', 'structure', 'of', 'dry', 'nafiontinytextregisteredlike', 'ionomers', 'on', 'the', 'electrostatic', 'interactions', 'between', 'the', 'components', 'of', 'the', 'molecules', 'in', 'order', 'to', 'speed', 'equilibration', 'a', 'procedure'... | [-0.18431907893235344, 0.13940197990269831, -0.0558268305586097, -0.007014213061778885, 0.0037713368823508323, -0.08872234457312456, 0.05394262131120937, 0.35517775157795234, -0.29267570309438345, -0.2907213044761424, 0.025655254114455746, -0.28725705640329646, -0.12281659047280627, 0.12874423555141085, 0.0659770940040... |
709.218 | Effective field theories for rooted staggered fermions | We extend the construction of the Symanzik effective action to include rooted
staggered fermions, starting from a generalization of the renormalization-group
approach to rooted staggered fermions. The Symanzik action, together with the
usual construction of a partially quenched chiral effective theory from a
local, p... | hep-lat | we extend the construction of the symanzik effective action to include rooted staggered fermions starting from a generalization of the renormalizationgroup approach to rooted staggered fermions the symanzik action together with the usual construction of a partially quenched chiral effective theory from a local partiall... | [['we', 'extend', 'the', 'construction', 'of', 'the', 'symanzik', 'effective', 'action', 'to', 'include', 'rooted', 'staggered', 'fermions', 'starting', 'from', 'a', 'generalization', 'of', 'the', 'renormalizationgroup', 'approach', 'to', 'rooted', 'staggered', 'fermions', 'the', 'symanzik', 'action', 'together', 'with... | [-0.11471843462663167, 0.3075465115323437, -0.15820941667665134, 0.07445731288471232, -0.07638480821906617, -0.08213421028587177, 0.08240101162598214, 0.30970108878770564, -0.21460460287617575, -0.2487841548652134, 0.035787081035474934, -0.24222294108547043, -0.2099875440736386, 0.02797444921452552, -0.0350734569612100... |
709.2181 | A probabilistic proof of Wallis's formula for pi | Using mostly elementary results and functions from probability, we prove
Wallis's formula for pi: pi/2 = prod_n (2n * 2n) / ((2n-1) * (2n+1)). The proof
involves normalization constants and the Gamma function, Standard normal, and
the Student t-Distribution.
| math.NT math.PR | using mostly elementary results and functions from probability we prove walliss formula for pi pi2 prod_n 2n 2n 2n1 2n1 the proof involves normalization constants and the gamma function standard normal and the student tdistribution | [['using', 'mostly', 'elementary', 'results', 'and', 'functions', 'from', 'probability', 'we', 'prove', 'walliss', 'formula', 'for', 'pi', 'pi2', 'prod_n', '2n', '2n', '2n1', '2n1', 'the', 'proof', 'involves', 'normalization', 'constants', 'and', 'the', 'gamma', 'function', 'standard', 'normal', 'and', 'the', 'student'... | [-0.13154267062268712, 0.1979742373805493, -0.10662380342974383, 0.12842781654805602, -0.07283659864932655, -0.24651936419746456, 0.09066035336924388, 0.3130442291936454, -0.2535759638994932, -0.2514329908059581, -0.020918143926845753, -0.31612569345709157, -0.17479701745768955, 0.20819867637884967, 0.01285228500252260... |
709.2182 | Rheology of two-dimensional F-actin networks associated with a lipid
interface | We report on the surface rheology of cross-linked F-actin networks associated
with a lipid monolayer at the air-water interface of a Langmuir monolayer. The
rheological measurements are made using a Couette cell. These data demonstrate
that the network has a finite elastic modulus that grows as a function of the
cros... | cond-mat.soft | we report on the surface rheology of crosslinked factin networks associated with a lipid monolayer at the airwater interface of a langmuir monolayer the rheological measurements are made using a couette cell these data demonstrate that the network has a finite elastic modulus that grows as a function of the crosslinkin... | [['we', 'report', 'on', 'the', 'surface', 'rheology', 'of', 'crosslinked', 'factin', 'networks', 'associated', 'with', 'a', 'lipid', 'monolayer', 'at', 'the', 'airwater', 'interface', 'of', 'a', 'langmuir', 'monolayer', 'the', 'rheological', 'measurements', 'are', 'made', 'using', 'a', 'couette', 'cell', 'these', 'data... | [-0.1884639063899062, 0.1719222203460767, -0.12687054929004885, -0.08292997211806084, -0.00610946882883773, -0.14549165469055114, 0.018775532132406767, 0.34738838878509243, -0.30553147485969884, -0.21557415122362344, 0.05420303139927503, -0.302202715881561, -0.22165584558081863, 0.16105977963582663, -0.0016656311621007... |
709.2183 | Population inversion of a NAHS mixture adsorbed into a cylindrical pore | A cylindrical nanopore immersed in a non-additive hard sphere binary fluid is
studied by means of integral equation theories and Monte Carlo simulations. It
is found that at low and intermediate values of the bulk total number density
the more concentrated bulk species is preferentially absorbed by the pore, as
expec... | cond-mat.stat-mech cond-mat.soft | a cylindrical nanopore immersed in a nonadditive hard sphere binary fluid is studied by means of integral equation theories and monte carlo simulations it is found that at low and intermediate values of the bulk total number density the more concentrated bulk species is preferentially absorbed by the pore as expected h... | [['a', 'cylindrical', 'nanopore', 'immersed', 'in', 'a', 'nonadditive', 'hard', 'sphere', 'binary', 'fluid', 'is', 'studied', 'by', 'means', 'of', 'integral', 'equation', 'theories', 'and', 'monte', 'carlo', 'simulations', 'it', 'is', 'found', 'that', 'at', 'low', 'and', 'intermediate', 'values', 'of', 'the', 'bulk', '... | [-0.12467055566481451, 0.24413241758959664, -0.07197759027496495, 0.02559775386130084, 0.004299125198579939, -0.07591592609994756, 0.037535486008233296, 0.3421488259678128, -0.26622086171871695, -0.34163169617411393, 0.041893059861493005, -0.29549573280784336, -0.08956180822208588, 0.1263169378989601, -0.00580574347284... |
709.2184 | Irrationality measure and lower bounds for pi(x) | In this note we show how the irrationality measure of $\zeta(s) = \pi^2/6$
can be used to obtain explicit lower bounds for $\pi(x)$. We analyze the key
ingredients of the proof of the finiteness of the irrationality measure, and
show how to obtain good lower bounds for $\pi(x)$ from these arguments as well.
While ver... | math.NT | in this note we show how the irrationality measure of zetas pi26 can be used to obtain explicit lower bounds for pix we analyze the key ingredients of the proof of the finiteness of the irrationality measure and show how to obtain good lower bounds for pix from these arguments as well while versions of some of the resu... | [['in', 'this', 'note', 'we', 'show', 'how', 'the', 'irrationality', 'measure', 'of', 'zetas', 'pi26', 'can', 'be', 'used', 'to', 'obtain', 'explicit', 'lower', 'bounds', 'for', 'pix', 'we', 'analyze', 'the', 'key', 'ingredients', 'of', 'the', 'proof', 'of', 'the', 'finiteness', 'of', 'the', 'irrationality', 'measure',... | [-0.07398819355044647, 0.07756780636762935, -0.18166081649473026, 0.15535444109229415, -0.04689676615609122, -0.11797698469655145, 0.09080102509774622, 0.297917883044907, -0.21541813756560996, -0.3317376016195686, 0.1335844517660527, -0.2643511277856305, -0.15233454820104053, 0.2825716317276515, -0.11254107656644746, 0... |
709.2185 | Charmed signatures for phase transitions in heavy-ion collisions | The interplay of charmonium production and suppression in In+In and Pb+Pb
reactions at 158 AGeV and in Au+Au reactions at sqrt(s)=200 GeV is investigated
with the HSD transport approach within the `hadronic comover model' and the
`QGP melting scenario'. The results for the J/Psi suppression and the Psi' to
J/Psi rati... | nucl-th hep-ph | the interplay of charmonium production and suppression in inin and pbpb reactions at 158 agev and in auau reactions at sqrts200 gev is investigated with the hsd transport approach within the hadronic comover model and the qgp melting scenario the results for the jpsi suppression and the psi to jpsi ratio are compared t... | [['the', 'interplay', 'of', 'charmonium', 'production', 'and', 'suppression', 'in', 'inin', 'and', 'pbpb', 'reactions', 'at', '158', 'agev', 'and', 'in', 'auau', 'reactions', 'at', 'sqrts200', 'gev', 'is', 'investigated', 'with', 'the', 'hsd', 'transport', 'approach', 'within', 'the', 'hadronic', 'comover', 'model', 'a... | [-0.05391822842021401, 0.2402962693066981, -0.18596043918066874, 0.11770418115640775, 0.030498027126304804, -0.12731411155098332, -0.004405027326160612, 0.3597628748187652, -0.17151334596654544, -0.2834441050313986, -0.09916644213864437, -0.40670591493925223, 0.05870956609455439, 0.10145884645171463, 0.0861426969184182... |
709.2186 | D-Terms from Generalized NS-NS Fluxes in Type II | Orientifolds of type II string theory admit a certain set of generalized
NS-NS fluxes, including not only the three-form field strength H, but also
metric and non-geometric fluxes, which are related to H by T-duality. We
describe in general how these fluxes appear as parameters of an effective N=1
supergravity theory... | hep-th | orientifolds of type ii string theory admit a certain set of generalized nsns fluxes including not only the threeform field strength h but also metric and nongeometric fluxes which are related to h by tduality we describe in general how these fluxes appear as parameters of an effective n1 supergravity theory in four di... | [['orientifolds', 'of', 'type', 'ii', 'string', 'theory', 'admit', 'a', 'certain', 'set', 'of', 'generalized', 'nsns', 'fluxes', 'including', 'not', 'only', 'the', 'threeform', 'field', 'strength', 'h', 'but', 'also', 'metric', 'and', 'nongeometric', 'fluxes', 'which', 'are', 'related', 'to', 'h', 'by', 'tduality', 'we... | [-0.12487632784521788, 0.18094719486121433, 0.013109451380147729, 0.17279189945228637, -0.12160185311910926, -0.18749364700809282, 0.009332592296163721, 0.32609202762344675, -0.16578216638456109, -0.3229019089692062, 0.07912919304824324, -0.22537632853353537, -0.19761705402565258, 0.15950827885379074, -0.12324019158960... |
709.2187 | Manipulating atoms in an optical lattice: Fractional fermion number and
its optical quantum measurement | We provide a detailed analysis of our previously proposed scheme [Phys. Rev.
Lett. 88, 180401, (2002)] to engineer the profile of the hopping amplitudes for
atomic gases in a 1D optical lattice so that the particle number becomes
fractional. We consider a constructed system of a dilute two-species gas of
fermionic at... | cond-mat.other cond-mat.str-el hep-ph hep-th quant-ph | we provide a detailed analysis of our previously proposed scheme phys rev lett 88 180401 2002 to engineer the profile of the hopping amplitudes for atomic gases in a 1d optical lattice so that the particle number becomes fractional we consider a constructed system of a dilute twospecies gas of fermionic atoms where the... | [['we', 'provide', 'a', 'detailed', 'analysis', 'of', 'our', 'previously', 'proposed', 'scheme', 'phys', 'rev', 'lett', '88', '180401', '2002', 'to', 'engineer', 'the', 'profile', 'of', 'the', 'hopping', 'amplitudes', 'for', 'atomic', 'gases', 'in', 'a', '1d', 'optical', 'lattice', 'so', 'that', 'the', 'particle', 'num... | [-0.15357273104159813, 0.22628414771782102, -0.062469959880103294, -0.011394735236677061, -0.013191389781196864, -0.1314157162141959, 0.06930553790089194, 0.35737745766754, -0.19277524782426075, -0.2910833919897802, -0.033915271008843825, -0.29296593313066976, -0.14867559547798292, 0.16371051058369843, -0.0025750118357... |
709.2188 | L^p-estimates for the wave equation associated to the Grushin operator | Let G:=-((d/dx)^2+x^2(d/du)^2) denote the Grusin operator on R^2. Consider
the Cauchy problem for the associated wave equation on R x R^2, given by
((d/dt)^2+G)v =0, v(0,.)=f, d/dt v(0,.)=g, where t denotes time and f, g are
suitable functions. The focus of this thesis lies on smoothness properties of
the solution v ... | math.AP math.SP | let gddx2x2ddu2 denote the grusin operator on r2 consider the cauchy problem for the associated wave equation on r x r2 given by ddt2gv 0 v0f ddt v0g where t denotes time and f g are suitable functions the focus of this thesis lies on smoothness properties of the solution v for fixed time t with respect to the initial ... | [['let', 'gddx2x2ddu2', 'denote', 'the', 'grusin', 'operator', 'on', 'r2', 'consider', 'the', 'cauchy', 'problem', 'for', 'the', 'associated', 'wave', 'equation', 'on', 'r', 'x', 'r2', 'given', 'by', 'ddt2gv', '0', 'v0f', 'ddt', 'v0g', 'where', 't', 'denotes', 'time', 'and', 'f', 'g', 'are', 'suitable', 'functions', 't... | [-0.18581087805031643, 0.0801708410106545, -0.034967640448823896, 0.003897145662429559, -0.0337077631703476, -0.1356812461965928, -0.020606300259947124, 0.3256811279069333, -0.30215790519749164, -0.17016131233595597, 0.09646037504855326, -0.3221607596824204, -0.06075062843066824, 0.18897087454632686, -0.090202017758639... |
709.2189 | Graphs of Transportation Polytopes | This paper discusses properties of the graphs of 2-way and 3-way
transportation polytopes, in particular, their possible numbers of vertices and
their diameters. Our main results include a quadratic bound on the diameter of
axial 3-way transportation polytopes and a catalogue of non-degenerate
transportation polytope... | math.CO | this paper discusses properties of the graphs of 2way and 3way transportation polytopes in particular their possible numbers of vertices and their diameters our main results include a quadratic bound on the diameter of axial 3way transportation polytopes and a catalogue of nondegenerate transportation polytopes of smal... | [['this', 'paper', 'discusses', 'properties', 'of', 'the', 'graphs', 'of', '2way', 'and', '3way', 'transportation', 'polytopes', 'in', 'particular', 'their', 'possible', 'numbers', 'of', 'vertices', 'and', 'their', 'diameters', 'our', 'main', 'results', 'include', 'a', 'quadratic', 'bound', 'on', 'the', 'diameter', 'of... | [-0.17719015954528003, 0.08742597112097428, -0.03294456711038947, 0.025972662745043635, -0.07856424371711909, -0.10179589615669102, 0.08231334252166561, 0.3048839994892478, -0.26672879985533654, -0.3483441433822736, 0.09311843850882724, -0.3253098205663264, -0.1753537203418091, 0.16926005972316488, -0.15998222055844963... |
709.219 | White Dwarf Luminosity and Mass Functions from Sloan Digital Sky Survey
Spectra | We present the first phase in our ongoing work to use Sloan Digital Sky
Survey (SDSS) data to create separate white dwarf (WD) luminosity functions for
two or more different mass ranges. In this paper, we determine the completeness
of the SDSS spectroscopic white dwarf sample by comparing a proper-motion
selected sam... | astro-ph | we present the first phase in our ongoing work to use sloan digital sky survey sdss data to create separate white dwarf wd luminosity functions for two or more different mass ranges in this paper we determine the completeness of the sdss spectroscopic white dwarf sample by comparing a propermotion selected sample of wd... | [['we', 'present', 'the', 'first', 'phase', 'in', 'our', 'ongoing', 'work', 'to', 'use', 'sloan', 'digital', 'sky', 'survey', 'sdss', 'data', 'to', 'create', 'separate', 'white', 'dwarf', 'wd', 'luminosity', 'functions', 'for', 'two', 'or', 'more', 'different', 'mass', 'ranges', 'in', 'this', 'paper', 'we', 'determine'... | [-0.030398887422818103, 0.07521956148084215, -0.061488957481992526, 0.08718565799505586, -0.1540102363858176, -0.04934087191158307, 0.1445909993980374, 0.4086317798634719, -0.10993352688015684, -0.3953568145295071, 0.03698878746605015, -0.369155283499923, -0.051619848570029374, 0.21642638138925646, -0.12130476427754681... |
709.2191 | On the Localized superluminal Solutions to the Maxwell Equations | In the first part of this article the various experimental sectors of physics
in which Superluminal motions seem to appear are briefly mentioned, after a
sketchy theoretical introduction. In particular, a panoramic view is presented
of the experiments with evanescent waves (and/or tunneling photons), and with
the "Lo... | physics.class-ph physics.gen-ph physics.optics | in the first part of this article the various experimental sectors of physics in which superluminal motions seem to appear are briefly mentioned after a sketchy theoretical introduction in particular a panoramic view is presented of the experiments with evanescent waves andor tunneling photons and with the localized su... | [['in', 'the', 'first', 'part', 'of', 'this', 'article', 'the', 'various', 'experimental', 'sectors', 'of', 'physics', 'in', 'which', 'superluminal', 'motions', 'seem', 'to', 'appear', 'are', 'briefly', 'mentioned', 'after', 'a', 'sketchy', 'theoretical', 'introduction', 'in', 'particular', 'a', 'panoramic', 'view', 'i... | [-0.16160989916313856, 0.15121224133654468, -0.07757435247313187, 0.07895319162407868, -0.1536056818180825, -0.10017149589132088, -0.03314675254526616, 0.32005250633720206, -0.23130462229700827, -0.2727162700992419, 0.09005284638225705, -0.2845841005938016, -0.17985180901216002, 0.21464941299481474, -0.0332799262767917... |
709.2192 | Deepest Near-IR Surface Photometry of Galaxies in the Local Sphere of
Influence | We present near-IR, deep (4 mag deeper than 2MASS) imaging of 56 Local Volume
galaxies. Global parameters such as total magnitudes and stellar masses have
been derived and the new near-IR data combined with existing 21cm and optical
B-band data. We present multiwavelength relations such as the HI mass-to-light
ratio ... | astro-ph | we present nearir deep 4 mag deeper than 2mass imaging of 56 local volume galaxies global parameters such as total magnitudes and stellar masses have been derived and the new nearir data combined with existing 21cm and optical bband data we present multiwavelength relations such as the hi masstolight ratio and investig... | [['we', 'present', 'nearir', 'deep', '4', 'mag', 'deeper', 'than', '2mass', 'imaging', 'of', '56', 'local', 'volume', 'galaxies', 'global', 'parameters', 'such', 'as', 'total', 'magnitudes', 'and', 'stellar', 'masses', 'have', 'been', 'derived', 'and', 'the', 'new', 'nearir', 'data', 'combined', 'with', 'existing', '21... | [0.006917509586229676, 0.03785749473685368, -0.03672850293824907, 0.12330471892978569, -0.14463083357473866, -0.019634052874428817, 0.035551466345481696, 0.4759785643488657, -0.13697369416534413, -0.40449794339107686, 0.08015623774768815, -0.32628522996531156, -0.039553819186069435, 0.1733153102743882, -0.0489127808021... |
709.2193 | Radially Symmetric Nonlinear States of Harmonically Trapped
Bose-Einstein Condensates | Starting from the spectrum of the radially symmetric quantum harmonic
oscillator in two dimensions, we create a large set of nonlinear solutions. The
relevant three principal branches, with $n_r=0,1$ and 2 radial nodes
respectively, are systematically continued as a function of the chemical
potential and their linear... | cond-mat.other | starting from the spectrum of the radially symmetric quantum harmonic oscillator in two dimensions we create a large set of nonlinear solutions the relevant three principal branches with n_r01 and 2 radial nodes respectively are systematically continued as a function of the chemical potential and their linear stability... | [['starting', 'from', 'the', 'spectrum', 'of', 'the', 'radially', 'symmetric', 'quantum', 'harmonic', 'oscillator', 'in', 'two', 'dimensions', 'we', 'create', 'a', 'large', 'set', 'of', 'nonlinear', 'solutions', 'the', 'relevant', 'three', 'principal', 'branches', 'with', 'n_r01', 'and', '2', 'radial', 'nodes', 'respec... | [-0.15122707000012847, 0.222693280662828, -0.042186929824807026, 0.07376282483958428, 0.0010931505834874274, -0.15029256098535948, 0.004344779409372925, 0.3439747247559188, -0.2519212766730396, -0.2561674751632381, 0.12102390534842429, -0.2773285389094698, -0.10544282265817112, 0.17729583664384502, 0.03777320749742847,... |
709.2194 | Computing Solar Absolute Fluxes | Computed color indices and spectral shapes for individual stars are routinely
compared with observations for essentially all spectral types, but absolute
fluxes are rarely tested. We can confront observed irradiances with the
predictions from model atmospheres for a few stars with accurate angular
diameter measuremen... | astro-ph | computed color indices and spectral shapes for individual stars are routinely compared with observations for essentially all spectral types but absolute fluxes are rarely tested we can confront observed irradiances with the predictions from model atmospheres for a few stars with accurate angular diameter measurements n... | [['computed', 'color', 'indices', 'and', 'spectral', 'shapes', 'for', 'individual', 'stars', 'are', 'routinely', 'compared', 'with', 'observations', 'for', 'essentially', 'all', 'spectral', 'types', 'but', 'absolute', 'fluxes', 'are', 'rarely', 'tested', 'we', 'can', 'confront', 'observed', 'irradiances', 'with', 'the'... | [0.006091431298825357, 0.12516921108982962, -0.009687399700294695, 0.10719937279022165, -0.04178277041515982, -0.07465485913431918, 0.047698773971131564, 0.46766562980352616, -0.13099173104808648, -0.43616065782095703, 0.08901962580643974, -0.30488512811384033, -0.003845162114736681, 0.2313584637161753, -0.089420733693... |
709.2195 | Can Old Galaxies at High Redshifts and Baryon Acoustic Oscillations
Constrain H_0? | A new age-redshift test is proposed in order to constrain $H_0$ with basis on
the existence of old high redshift galaxies (OHRG). As should be expected, the
estimates of $H_0$ based on the OHRG are heavily dependent on the cosmological
description. In the flat concordance model ($\Lambda$CDM), for example, the
value ... | astro-ph gr-qc | a new ageredshift test is proposed in order to constrain h_0 with basis on the existence of old high redshift galaxies ohrg as should be expected the estimates of h_0 based on the ohrg are heavily dependent on the cosmological description in the flat concordance model lambdacdm for example the value of h_0 depends on t... | [['a', 'new', 'ageredshift', 'test', 'is', 'proposed', 'in', 'order', 'to', 'constrain', 'h_0', 'with', 'basis', 'on', 'the', 'existence', 'of', 'old', 'high', 'redshift', 'galaxies', 'ohrg', 'as', 'should', 'be', 'expected', 'the', 'estimates', 'of', 'h_0', 'based', 'on', 'the', 'ohrg', 'are', 'heavily', 'dependent', ... | [-0.07670261502840679, 0.0811330595395041, -0.08461888180720015, 0.06877721094288636, -0.1324085874313658, -0.10153629267718513, 0.02428528752138877, 0.30991280489842166, -0.1703739643448612, -0.3324057228783458, 0.07903648848918925, -0.2717715343142944, -0.03337294625328411, 0.24158699620007115, 0.008725298671182114, ... |
709.2196 | Bregman Voronoi Diagrams: Properties, Algorithms and Applications | The Voronoi diagram of a finite set of objects is a fundamental geometric
structure that subdivides the embedding space into regions, each region
consisting of the points that are closer to a given object than to the others.
We may define many variants of Voronoi diagrams depending on the class of
objects, the distan... | cs.CG | the voronoi diagram of a finite set of objects is a fundamental geometric structure that subdivides the embedding space into regions each region consisting of the points that are closer to a given object than to the others we may define many variants of voronoi diagrams depending on the class of objects the distance fu... | [['the', 'voronoi', 'diagram', 'of', 'a', 'finite', 'set', 'of', 'objects', 'is', 'a', 'fundamental', 'geometric', 'structure', 'that', 'subdivides', 'the', 'embedding', 'space', 'into', 'regions', 'each', 'region', 'consisting', 'of', 'the', 'points', 'that', 'are', 'closer', 'to', 'a', 'given', 'object', 'than', 'to'... | [-0.092787108607524, 0.06416119508868992, -0.15620211031181977, 0.16445725182152984, -0.09646707826616216, -0.08120405576434604, 0.08793716346767788, 0.39914279366662436, -0.32951597852623576, -0.25424627390341453, 0.04168299457413625, -0.29689369695393536, -0.19660156328999107, 0.16646385615718026, -0.1664011112142021... |
709.2197 | Scalar and vector meson propagation in asymmetric nuclear matter | The propagation of the scalar (\sigma and \delta) and vector (\omega and
\rho) mesons in an iso-asymmetric nuclear matter is studied in detail, using
the Walecka model. We calculate the invariant masses and spectral functions of
the mesons, including the effect of meson mixing. At finite density, the mixing
effect is... | nucl-th astro-ph hep-ph nucl-ex | the propagation of the scalar sigma and delta and vector omega and rho mesons in an isoasymmetric nuclear matter is studied in detail using the walecka model we calculate the invariant masses and spectral functions of the mesons including the effect of meson mixing at finite density the mixing effect is quite important... | [['the', 'propagation', 'of', 'the', 'scalar', 'sigma', 'and', 'delta', 'and', 'vector', 'omega', 'and', 'rho', 'mesons', 'in', 'an', 'isoasymmetric', 'nuclear', 'matter', 'is', 'studied', 'in', 'detail', 'using', 'the', 'walecka', 'model', 'we', 'calculate', 'the', 'invariant', 'masses', 'and', 'spectral', 'functions'... | [-0.13274846544954927, 0.25270704414160716, -0.09982164677348919, 0.13253995462146123, -0.023733195039676504, -0.07330098812817595, 0.004637441970407963, 0.33154895235784354, -0.24921146646374837, -0.22878581846598536, -0.009726319242327008, -0.287068765074946, -0.10182141785335261, 0.06459247739549027, 0.1009794260258... |
709.2198 | Anomalous optical transmission through a vortex lattice in a film of
type-II superconductor | We study the effect of anomalous optical transmission through an array of
vortices in a type-II superconducting film subjected to a strong magnetic
field. The mechanism responsible for this effect is resonance transmission
between two surface plasmon polaritons (SPP) in the system. The SPP band gap in
the system is s... | cond-mat.supr-con cond-mat.mes-hall | we study the effect of anomalous optical transmission through an array of vortices in a typeii superconducting film subjected to a strong magnetic field the mechanism responsible for this effect is resonance transmission between two surface plasmon polaritons spp in the system the spp band gap in the system is studied ... | [['we', 'study', 'the', 'effect', 'of', 'anomalous', 'optical', 'transmission', 'through', 'an', 'array', 'of', 'vortices', 'in', 'a', 'typeii', 'superconducting', 'film', 'subjected', 'to', 'a', 'strong', 'magnetic', 'field', 'the', 'mechanism', 'responsible', 'for', 'this', 'effect', 'is', 'resonance', 'transmission'... | [-0.2632166300102004, 0.19403471973013697, -0.032827253267168996, 0.01986199398192444, -0.03248352198196309, -0.1391992956732533, 0.05513070777856878, 0.42187397935028587, -0.2561673642535295, -0.3240961986527379, 0.023230845708998717, -0.23701447629635888, -0.16539301920150007, 0.21981748931908182, 0.04789045175670513... |
709.2199 | High pressure study on the strong-coupling superconductivity in
non-centrosymmetric compound CeIrSi_3 | We have carried out high pressure experiment on the pressure-induced
superconductor CeIrSi$_3$ without inversion center. The electrical resistivity
and ac heat capacity were measured in the same run for the same sample. The
critical pressure of the antiferromagnetic state was determined to be $P_{\rm
c}$ = 2.25 GPa. ... | cond-mat.supr-con | we have carried out high pressure experiment on the pressureinduced superconductor ceirsi_3 without inversion center the electrical resistivity and ac heat capacity were measured in the same run for the same sample the critical pressure of the antiferromagnetic state was determined to be p_rm c 225 gpa the heat capacit... | [['we', 'have', 'carried', 'out', 'high', 'pressure', 'experiment', 'on', 'the', 'pressureinduced', 'superconductor', 'ceirsi_3', 'without', 'inversion', 'center', 'the', 'electrical', 'resistivity', 'and', 'ac', 'heat', 'capacity', 'were', 'measured', 'in', 'the', 'same', 'run', 'for', 'the', 'same', 'sample', 'the', ... | [-0.18499694586709456, 0.22278540925824164, -0.006040446921836186, -0.005382545384359948, -0.04004233555078752, -0.16634194752193773, 0.17446052547785695, 0.33310050997545815, -0.2519549529984164, -0.3148622678922405, 0.02414867012385938, -0.3814893146754538, 0.004707629030662371, 0.18618450795708477, 0.068325179397993... |
709.22 | Statistical Investigation of Connected Structures of Stock Networks in
Financial Time Series | In this study, we have investigated factors of determination which can affect
the connected structure of a stock network. The representative index for
topological properties of a stock network is the number of links with other
stocks. We used the multi-factor model, extensively acknowledged in financial
literature. I... | q-fin.ST physics.data-an | in this study we have investigated factors of determination which can affect the connected structure of a stock network the representative index for topological properties of a stock network is the number of links with other stocks we used the multifactor model extensively acknowledged in financial literature in the mu... | [['in', 'this', 'study', 'we', 'have', 'investigated', 'factors', 'of', 'determination', 'which', 'can', 'affect', 'the', 'connected', 'structure', 'of', 'a', 'stock', 'network', 'the', 'representative', 'index', 'for', 'topological', 'properties', 'of', 'a', 'stock', 'network', 'is', 'the', 'number', 'of', 'links', 'w... | [-0.11410499085835872, 0.13296028001505955, -0.08042873047974587, 0.0676644534877695, -0.05503303184413748, -0.12882911253923385, 0.10102869996035674, 0.3732747373581486, -0.2499703134151895, -0.3176059252377899, 0.1123719146684974, -0.31259895896188694, -0.15686539308361636, 0.20769227560843562, -0.05553401755353454, ... |
709.2201 | A complete proof of The Graceful Tree Conjecture using the concept of
Edge Degree | We show the Graceful Tree Conjecture holds.
| cs.DM | we show the graceful tree conjecture holds | [['we', 'show', 'the', 'graceful', 'tree', 'conjecture', 'holds']] | [-0.36312728588070187, 0.18599365212555444, -0.130322075049792, 0.18909522385469504, -0.04443013668060303, -0.2547873186745814, 0.05262242736560958, 0.3909377711159842, -0.3293068941150393, -0.20885409095457622, -0.016337905677833726, -0.17229224472040577, -0.2952451567564692, 0.09270497092178889, -0.22597889069999968,... |
709.2202 | Linear maps preserving fibers | Let $G\subset\GL(V)$ be a complex reductive group where $\dim V<\infty$, and
let $\pi\colon V\to\quot VG$ be the categorical quotient. Let
$\NN:=\pi\inv\pi(0)$ be the null cone of $V$, let $H_0$ be the subgroup of
$\GL(V)$ which preserves the ideal $\I$ of $\NN$ and let $H$ be a Levi subgroup
of $H_0$ containing $G$.... | math.GR math.RT | let gsubsetglv be a complex reductive group where dim vinfty and let picolon vtoquot vg be the categorical quotient let nnpiinvpi0 be the null cone of v let h_0 be the subgroup of glv which preserves the ideal i of nn and let h be a levi subgroup of h_0 containing g we determine the identity component of h in many case... | [['let', 'gsubsetglv', 'be', 'a', 'complex', 'reductive', 'group', 'where', 'dim', 'vinfty', 'and', 'let', 'picolon', 'vtoquot', 'vg', 'be', 'the', 'categorical', 'quotient', 'let', 'nnpiinvpi0', 'be', 'the', 'null', 'cone', 'of', 'v', 'let', 'h_0', 'be', 'the', 'subgroup', 'of', 'glv', 'which', 'preserves', 'the', 'id... | [-0.1962296919130798, 0.10904948591047514, -0.10554428949399153, -0.05719878634530081, -0.13610275229196608, -0.18464938797114883, -0.03306093578673123, 0.3922664176983138, -0.36923999163263943, -0.13973398124411082, 0.054417133824851284, -0.27933721524383753, -0.0416548408077991, 0.15257684756458426, -0.11423688678769... |
709.2203 | Self-consistent triaxial de Zeeuw-Carollo Models | We use the usual method of Schwarzschild to construct self-consistent
solutions for the triaxial de Zeeuw & Carollo (1996) models with central
density cusps. ZC96 models are triaxial generalisations of spherical
$\gamma$-models of Dehnen whose densities vary as $r^{-\gamma}$ near the center
and $r^{-4}$ at large radi... | astro-ph | we use the usual method of schwarzschild to construct selfconsistent solutions for the triaxial de zeeuw carollo 1996 models with central density cusps zc96 models are triaxial generalisations of spherical gammamodels of dehnen whose densities vary as rgamma near the center and r4 at large radii and hence possess a cen... | [['we', 'use', 'the', 'usual', 'method', 'of', 'schwarzschild', 'to', 'construct', 'selfconsistent', 'solutions', 'for', 'the', 'triaxial', 'de', 'zeeuw', 'carollo', '1996', 'models', 'with', 'central', 'density', 'cusps', 'zc96', 'models', 'are', 'triaxial', 'generalisations', 'of', 'spherical', 'gammamodels', 'of', '... | [-0.10561924931573685, 0.16463912586641527, -0.06261495435137476, 0.09112169405170789, -0.00433466414870054, -0.1455578099739796, 0.0038917450951885257, 0.36901492234255784, -0.20105612244151416, -0.3273644831315323, 0.06331493167272129, -0.2904288299474729, -0.04892466999262979, 0.1891807673958965, 0.01975520017344934... |
709.2204 | Ferromagnetism of two-flavor quark matter in chiral and/or
color-superconducting phases at zero and finite temperatures | We study the phase structure of the unpolarized and polarized two-flavor
quark matters at zero and finite temperatures within the Nambu--Jona-Lasinio
(NJL) model. We focus on the region, which includes the coexisting phase of
quark-antiquark and diquark condensates. Generalizing the NJL model so as to
describe the po... | hep-ph | we study the phase structure of the unpolarized and polarized twoflavor quark matters at zero and finite temperatures within the nambujonalasinio njl model we focus on the region which includes the coexisting phase of quarkantiquark and diquark condensates generalizing the njl model so as to describe the polarized quar... | [['we', 'study', 'the', 'phase', 'structure', 'of', 'the', 'unpolarized', 'and', 'polarized', 'twoflavor', 'quark', 'matters', 'at', 'zero', 'and', 'finite', 'temperatures', 'within', 'the', 'nambujonalasinio', 'njl', 'model', 'we', 'focus', 'on', 'the', 'region', 'which', 'includes', 'the', 'coexisting', 'phase', 'of'... | [-0.16185310351620638, 0.2930378455585286, -0.05870044935119352, 0.0702282085410083, -0.04900647030531693, -0.14666930765066463, 0.10943035576701053, 0.3408773887846897, -0.19247783337539034, -0.18511496686529536, -0.00697491509290829, -0.2841403897323493, -0.022710136857245173, 0.04271824100513512, 0.10095133065961044... |
709.2205 | Newton's method on Gra{\ss}mann manifolds | A general class of Newton algorithms on Gra{\ss}mann and
Lagrange-Gra{\ss}mann manifolds is introduced, that depends on an arbitrary
pair of local coordinates. Local quadratic convergence of the algorithm is
shown under a suitable condition on the choice of coordinate systems. Our
result extends and unifies previous ... | math.OC math.DG math.NA | a general class of newton algorithms on grassmann and lagrangegrassmann manifolds is introduced that depends on an arbitrary pair of local coordinates local quadratic convergence of the algorithm is shown under a suitable condition on the choice of coordinate systems our result extends and unifies previous convergence ... | [['a', 'general', 'class', 'of', 'newton', 'algorithms', 'on', 'grassmann', 'and', 'lagrangegrassmann', 'manifolds', 'is', 'introduced', 'that', 'depends', 'on', 'an', 'arbitrary', 'pair', 'of', 'local', 'coordinates', 'local', 'quadratic', 'convergence', 'of', 'the', 'algorithm', 'is', 'shown', 'under', 'a', 'suitable... | [-0.14742817192537977, -0.015441708358771216, -0.11037404748139443, 0.019082971754810447, -0.09640487024935519, -0.14784523874351924, -0.012753578537905758, 0.3478400440185101, -0.2453825046344624, -0.25467702212997456, 0.09848063455761544, -0.19067143351625795, -0.17723513944316413, 0.2780161104588346, -0.108657505532... |
709.2206 | Strong collisionless damping of the low-velocity branch of
electromagnetic wave in plasmas with Maxwellian-like electron velocity
distribution function | After approximate replacing of Maxwellian distribution exponent with the
rational polynomial fraction we have obtained precise analytical expression for
and calculated the principal value of logarithmically divergent integral in the
electron wave dispersion equation. At the same time our calculations have shown
the p... | physics.plasm-ph | after approximate replacing of maxwellian distribution exponent with the rational polynomial fraction we have obtained precise analytical expression for and calculated the principal value of logarithmically divergent integral in the electron wave dispersion equation at the same time our calculations have shown the pres... | [['after', 'approximate', 'replacing', 'of', 'maxwellian', 'distribution', 'exponent', 'with', 'the', 'rational', 'polynomial', 'fraction', 'we', 'have', 'obtained', 'precise', 'analytical', 'expression', 'for', 'and', 'calculated', 'the', 'principal', 'value', 'of', 'logarithmically', 'divergent', 'integral', 'in', 't... | [-0.12005204338463954, 0.14957715220283718, -0.08536350668407977, 0.07772702225134707, 0.0057050266693113375, -0.07101938799023629, -0.012819337667897343, 0.3150492181722075, -0.24190683279652148, -0.2969896578928456, -0.002874367024633102, -0.3184309961553663, -0.024783450905233623, 0.18696939486777409, 0.058338378609... |
709.2207 | Relationships between the HI 21-cm line strength, MgII equivalent width
and metallicity in damped Lyman-alpha absorption systems | We present the results of a survey for 21-cm absorption in four never
previously searched damped Lyman-alpha absorption systems (DLAs) with the
Westerbork Synthesis Radio Telescope. We add our results to other recent
studies in order to address the important issues regarding the detection of
cold gas, through 21-cm a... | astro-ph | we present the results of a survey for 21cm absorption in four never previously searched damped lymanalpha absorption systems dlas with the westerbork synthesis radio telescope we add our results to other recent studies in order to address the important issues regarding the detection of cold gas through 21cm absorption... | [['we', 'present', 'the', 'results', 'of', 'a', 'survey', 'for', '21cm', 'absorption', 'in', 'four', 'never', 'previously', 'searched', 'damped', 'lymanalpha', 'absorption', 'systems', 'dlas', 'with', 'the', 'westerbork', 'synthesis', 'radio', 'telescope', 'we', 'add', 'our', 'results', 'to', 'other', 'recent', 'studie... | [-0.08862903638844012, 0.1099579244433758, -0.022531571928755243, 0.059164344942861345, -0.06247451910214712, -0.10125283923450491, 0.019921845461615958, 0.4338223084837931, -0.19619545378897826, -0.30197347463184937, 0.06456133179542166, -0.30387241561652817, -0.07571973127969464, 0.19281164585368432, 0.02338294204626... |
709.2208 | Glueball Decay in Holographic QCD | Using holographic QCD based on D4-branes and D8-anti-D8-branes, we have
computed couplings of glueballs to light mesons. We describe glueball decay by
explicitly calculating its decay widths and branching ratios. Interestingly,
while glueballs remain less well understood both theoretically and
experimentally, our res... | hep-th hep-ph nucl-th | using holographic qcd based on d4branes and d8antid8branes we have computed couplings of glueballs to light mesons we describe glueball decay by explicitly calculating its decay widths and branching ratios interestingly while glueballs remain less well understood both theoretically and experimentally our results are fo... | [['using', 'holographic', 'qcd', 'based', 'on', 'd4branes', 'and', 'd8antid8branes', 'we', 'have', 'computed', 'couplings', 'of', 'glueballs', 'to', 'light', 'mesons', 'we', 'describe', 'glueball', 'decay', 'by', 'explicitly', 'calculating', 'its', 'decay', 'widths', 'and', 'branching', 'ratios', 'interestingly', 'whil... | [-0.027801628148110293, 0.32436244918527196, -0.11723112561235047, 0.17740737255494368, -0.050910844052412425, -0.19671533538971142, 0.028267654497737448, 0.39538687868436506, -0.11452976278736289, -0.1873019226344235, -0.0064744134517723175, -0.31515166360929786, -0.04752894152090492, 0.10119686249562214, 0.0946418463... |
709.2209 | Topological Properties of Stock Networks Based on Random Matrix Theory
in Financial Time Series | We investigated the topological properties of stock networks through a
comparison of the original stock network with the estimated stock network from
the correlation matrix created by the random matrix theory (RMT). We used
individual stocks traded on the market indices of Korea, Japan, Canada, the
USA, Italy, and th... | q-fin.ST physics.data-an | we investigated the topological properties of stock networks through a comparison of the original stock network with the estimated stock network from the correlation matrix created by the random matrix theory rmt we used individual stocks traded on the market indices of korea japan canada the usa italy and the uk the r... | [['we', 'investigated', 'the', 'topological', 'properties', 'of', 'stock', 'networks', 'through', 'a', 'comparison', 'of', 'the', 'original', 'stock', 'network', 'with', 'the', 'estimated', 'stock', 'network', 'from', 'the', 'correlation', 'matrix', 'created', 'by', 'the', 'random', 'matrix', 'theory', 'rmt', 'we', 'us... | [-0.08167404642733707, 0.07219285036747654, -0.10338506477741086, 0.11784662442315914, -0.003293138816037591, -0.10137218595823137, 0.08498477662356979, 0.36254312327828225, -0.2693322411458182, -0.2774550652782607, 0.12486297803139693, -0.37052209602623454, -0.20838667016960982, 0.13089839136559228, -0.038682172892660... |
709.221 | Knot in Cen A: Stochastic Magnetic Field for Diffusive Synchrotron
Radiation? | The emission of relativistic electrons moving in the random and small-scale
magnetic field is presented by diffusive synchrotron radiation (DSR). In this
Letter, we revisit the perturbative treatment of DSR. We propose that random
and small-scale magnetic field might be generated by the turbulence. As an
example, mul... | astro-ph | the emission of relativistic electrons moving in the random and smallscale magnetic field is presented by diffusive synchrotron radiation dsr in this letter we revisit the perturbative treatment of dsr we propose that random and smallscale magnetic field might be generated by the turbulence as an example multiband radi... | [['the', 'emission', 'of', 'relativistic', 'electrons', 'moving', 'in', 'the', 'random', 'and', 'smallscale', 'magnetic', 'field', 'is', 'presented', 'by', 'diffusive', 'synchrotron', 'radiation', 'dsr', 'in', 'this', 'letter', 'we', 'revisit', 'the', 'perturbative', 'treatment', 'of', 'dsr', 'we', 'propose', 'that', '... | [-0.15299503097033246, 0.2146295054676073, -0.044438418035613415, 0.09311164236018196, -0.0648108564931503, -0.0981405034532493, -0.014145145315659588, 0.38068611769283073, -0.26636850708065196, -0.3342925090382391, -0.009603355285473802, -0.21295082759349904, -0.06739221026803902, 0.19645644546649915, -0.0162558052391... |
709.2211 | Possible time-variability of the fine-structure constant expected from
the accelerating universe | We present a theoretical calculation on the time-variability of the
fine-structure constant to fit the result of the recent precise analysis of the
measurement of the QSO absorption lines. We find the parameters and initial
values of the scalar-tensor theory to be determined much more accurately than
fitting the acce... | astro-ph | we present a theoretical calculation on the timevariability of the finestructure constant to fit the result of the recent precise analysis of the measurement of the qso absorption lines we find the parameters and initial values of the scalartensor theory to be determined much more accurately than fitting the accelerati... | [['we', 'present', 'a', 'theoretical', 'calculation', 'on', 'the', 'timevariability', 'of', 'the', 'finestructure', 'constant', 'to', 'fit', 'the', 'result', 'of', 'the', 'recent', 'precise', 'analysis', 'of', 'the', 'measurement', 'of', 'the', 'qso', 'absorption', 'lines', 'we', 'find', 'the', 'parameters', 'and', 'in... | [-0.0902221759331312, 0.057309338313250524, -0.09472588975158697, 0.0660091202290779, -0.0946885027696152, -0.0798430128771862, 0.05085696745821199, 0.34841462360644665, -0.18022911524324603, -0.35790145578416616, 0.051337056672137636, -0.25776200657207016, -0.02561111464102224, 0.1905956982542144, 0.025173228007514734... |
709.2212 | Molecular Bose-Einstein condensation in a versatile low power crossed
dipole trap | We produce Bose-Einstein condensates of 6Li2 molecules in a low power (22 W)
crossed optical dipole trap. Fermionic 6Li atoms are collected in a
magneto-optical trap from a Zeeman slowed atomic beam, then loaded into the
optical dipole trap where they are evaporatively cooled to quantum degeneracy.
Our simplified sys... | cond-mat.other | we produce boseeinstein condensates of 6li2 molecules in a low power 22 w crossed optical dipole trap fermionic 6li atoms are collected in a magnetooptical trap from a zeeman slowed atomic beam then loaded into the optical dipole trap where they are evaporatively cooled to quantum degeneracy our simplified system offer... | [['we', 'produce', 'boseeinstein', 'condensates', 'of', '6li2', 'molecules', 'in', 'a', 'low', 'power', '22', 'w', 'crossed', 'optical', 'dipole', 'trap', 'fermionic', '6li', 'atoms', 'are', 'collected', 'in', 'a', 'magnetooptical', 'trap', 'from', 'a', 'zeeman', 'slowed', 'atomic', 'beam', 'then', 'loaded', 'into', 't... | [-0.1222739541677363, 0.3110871254572306, -0.009666861472369143, -0.0041410259366261234, 0.04604398003765241, -0.28292443826230185, 0.05476343852933496, 0.4214347909402215, -0.18309583033745488, -0.237640231043439, -0.07616626128914174, -0.291449999464958, 0.06110385984577464, 0.19781462181444195, 0.043522148209652216,... |
709.2213 | Gauge fields, quantized fluxes and monopole confinement of the honeycomb
lattice | Electron hopping models on the honeycomb lattice are studied. The lattice
consists of two triangular sublattices, and it is non-Bravais. The dual space
has non-trivial topology. The gauge fields of Bloch electrons have the U(1)
symmetry and thus represent superconducting states in the dual space. Two
quantized Abriko... | cond-mat.mes-hall | electron hopping models on the honeycomb lattice are studied the lattice consists of two triangular sublattices and it is nonbravais the dual space has nontrivial topology the gauge fields of bloch electrons have the u1 symmetry and thus represent superconducting states in the dual space two quantized abrikosov fluxes ... | [['electron', 'hopping', 'models', 'on', 'the', 'honeycomb', 'lattice', 'are', 'studied', 'the', 'lattice', 'consists', 'of', 'two', 'triangular', 'sublattices', 'and', 'it', 'is', 'nonbravais', 'the', 'dual', 'space', 'has', 'nontrivial', 'topology', 'the', 'gauge', 'fields', 'of', 'bloch', 'electrons', 'have', 'the',... | [-0.20975160353232344, 0.2742655660284865, -0.033422936527828746, 0.08893653291410633, -0.08785184330299944, -0.16010647446015164, 0.0058441113328729245, 0.4043321726297526, -0.19708636687382272, -0.22764660868989794, 0.06196254642095585, -0.28681812151790337, -0.1486746119090209, 0.098445882352027, 0.00311789714864322... |
709.2214 | Rational interpolation and mixed inverse spectral problem for finite CMV
matrices | For finite dimensional CMV matrices the mixed inverse spectral problem of
reconstruction the matrix by its submatrix and a part of its spectrum is
considered. A general rational interpolation problem which arises in solving
the mixed inverse spectral problem is studied, and the description of the space
of its solutio... | math.SP math.CA | for finite dimensional cmv matrices the mixed inverse spectral problem of reconstruction the matrix by its submatrix and a part of its spectrum is considered a general rational interpolation problem which arises in solving the mixed inverse spectral problem is studied and the description of the space of its solutions i... | [['for', 'finite', 'dimensional', 'cmv', 'matrices', 'the', 'mixed', 'inverse', 'spectral', 'problem', 'of', 'reconstruction', 'the', 'matrix', 'by', 'its', 'submatrix', 'and', 'a', 'part', 'of', 'its', 'spectrum', 'is', 'considered', 'a', 'general', 'rational', 'interpolation', 'problem', 'which', 'arises', 'in', 'sol... | [-0.08474434159491977, 0.021688642656456116, -0.0792511439792914, 0.10394697049345616, -0.06472935269535711, -0.11134262249664698, -0.020914312011932265, 0.31521542241465145, -0.35804129463990464, -0.2419332136297981, 0.21998361793939944, -0.21685831085459828, -0.1467973225277989, 0.12930127941327144, -0.06285580816640... |
709.2215 | Measure of a 2-component link | A two-component link produces a torus as the product of the component knots
in a two-point configuration space of a three-sphere. This space can be
identified with a cotangent bundle and also with an indefinite Grassmannian. We
show that the integration of the absolute value of the canonical symplectic
form is equal ... | math.GT | a twocomponent link produces a torus as the product of the component knots in a twopoint configuration space of a threesphere this space can be identified with a cotangent bundle and also with an indefinite grassmannian we show that the integration of the absolute value of the canonical symplectic form is equal to the ... | [['a', 'twocomponent', 'link', 'produces', 'a', 'torus', 'as', 'the', 'product', 'of', 'the', 'component', 'knots', 'in', 'a', 'twopoint', 'configuration', 'space', 'of', 'a', 'threesphere', 'this', 'space', 'can', 'be', 'identified', 'with', 'a', 'cotangent', 'bundle', 'and', 'also', 'with', 'an', 'indefinite', 'grass... | [-0.21312969992868602, 0.061077492910714536, -0.08873060183280981, 0.033349986200367936, -0.10704777828466736, -0.08192233134085607, -0.0030499507556669414, 0.36388802235198553, -0.26515462811374546, -0.24586336764179195, 0.11338221150493298, -0.23156685192186974, -0.17363976029139994, 0.17215049316444875, -0.074048753... |
709.2216 | The stability of quantum Markov filters | When are quantum filters asymptotically independent of the initial state? We
show that this is the case for absolutely continuous initial states when the
quantum stochastic model satisfies an observability condition. When the initial
system is finite dimensional, this condition can be verified explicitly in
terms of ... | math-ph math.MP math.OA math.PR | when are quantum filters asymptotically independent of the initial state we show that this is the case for absolutely continuous initial states when the quantum stochastic model satisfies an observability condition when the initial system is finite dimensional this condition can be verified explicitly in terms of a ran... | [['when', 'are', 'quantum', 'filters', 'asymptotically', 'independent', 'of', 'the', 'initial', 'state', 'we', 'show', 'that', 'this', 'is', 'the', 'case', 'for', 'absolutely', 'continuous', 'initial', 'states', 'when', 'the', 'quantum', 'stochastic', 'model', 'satisfies', 'an', 'observability', 'condition', 'when', 't... | [-0.1466895129221181, 0.18088033656652744, -0.09709464239422232, 0.0451302116115888, -0.0022326851496472953, -0.16329358017537743, -0.041916917834896594, 0.3138214165150809, -0.2972237362836798, -0.18182652710626523, 0.15226032612651277, -0.23719633460665743, -0.1354559178153674, 0.1846732983016409, -0.0740019826684147... |
709.2217 | A classification of prime-valent regular Cayley maps on some groups | A Cayley map is a 2-cell embedding of a Cayley graph into an orientable
surface with the same local orientation induced by a cyclic permutation of
generators at each vertex. In this paper, we provide classifications of
prime-valent regular Cayley maps on abelian groups, dihedral groups and
dicyclic groups. Consequent... | math.CO | a cayley map is a 2cell embedding of a cayley graph into an orientable surface with the same local orientation induced by a cyclic permutation of generators at each vertex in this paper we provide classifications of primevalent regular cayley maps on abelian groups dihedral groups and dicyclic groups consequently we sh... | [['a', 'cayley', 'map', 'is', 'a', '2cell', 'embedding', 'of', 'a', 'cayley', 'graph', 'into', 'an', 'orientable', 'surface', 'with', 'the', 'same', 'local', 'orientation', 'induced', 'by', 'a', 'cyclic', 'permutation', 'of', 'generators', 'at', 'each', 'vertex', 'in', 'this', 'paper', 'we', 'provide', 'classifications... | [-0.19959241751095522, 0.1744772852766998, -0.045089490306766136, 0.07609114709497511, -0.13170436531831714, -0.1326867098585986, 0.009843794769435392, 0.4953059094107669, -0.28735232748010237, -0.18146754720288774, 0.13762387151338928, -0.31422123226397874, -0.17283123764260064, 0.16953956720712798, -0.126666278112679... |
709.2218 | The Approach to the Thermodynamic Limit in Lattice QCD at \mu\neq0 | The expectation value of the complex phase factor of the fermion determinant
is computed to leading order in the $p$-expansion of the chiral Lagrangian. The
computation is valid for $\mu<m_\pi/2$ and determines the dependence of the
sign problem on the volume and on the geometric shape of the volume. In the
thermodyn... | hep-lat | the expectation value of the complex phase factor of the fermion determinant is computed to leading order in the pexpansion of the chiral lagrangian the computation is valid for mum_pi2 and determines the dependence of the sign problem on the volume and on the geometric shape of the volume in the thermodynamic limit wi... | [['the', 'expectation', 'value', 'of', 'the', 'complex', 'phase', 'factor', 'of', 'the', 'fermion', 'determinant', 'is', 'computed', 'to', 'leading', 'order', 'in', 'the', 'pexpansion', 'of', 'the', 'chiral', 'lagrangian', 'the', 'computation', 'is', 'valid', 'for', 'mum_pi2', 'and', 'determines', 'the', 'dependence', ... | [-0.10093658187636925, 0.1637996782946791, -0.05193518739073507, 0.0282724371119853, -0.006157260818121534, -0.0535004565927891, 0.07981199271706564, 0.3112729996172411, -0.2186444079092208, -0.2776435242455092, 0.10452119658810026, -0.278275228924148, -0.07997297711517604, 0.16253580208567361, -0.005454000547263516, 0... |
709.2219 | Determination of S- and P-wave helicity amplitudes and non-unitary
evolution of pion creation process pi(-)p -> pi(-)pi(+)n on polarized target | We present the first model independent determination of S- and P-wave
helicity amplitudes from CERN measurements of pi(-)p -> pi(-)pi(+)n on
polarized target at small t and dipion masses 580-1080 MeV. The purely
analytical determination of the helicity amplitudes is made possible by our
finding analytical solution fo... | hep-ph | we present the first model independent determination of s and pwave helicity amplitudes from cern measurements of pip pipin on polarized target at small t and dipion masses 5801080 mev the purely analytical determination of the helicity amplitudes is made possible by our finding analytical solution for relative phase o... | [['we', 'present', 'the', 'first', 'model', 'independent', 'determination', 'of', 's', 'and', 'pwave', 'helicity', 'amplitudes', 'from', 'cern', 'measurements', 'of', 'pip', 'pipin', 'on', 'polarized', 'target', 'at', 'small', 't', 'and', 'dipion', 'masses', '5801080', 'mev', 'the', 'purely', 'analytical', 'determinati... | [-0.1806119950397349, 0.24383845163918122, -0.09049560968968563, 0.07155690335746884, -0.034296977164070465, -0.11284420997494968, 0.08210409681153734, 0.32582953903006345, -0.1916471445524111, -0.25063565961062545, -0.004778648040643553, -0.2792926243529087, -0.035744372536087546, 0.1395860966397222, 0.064954546405138... |
709.222 | Correlation between the Charged Current Interactions of Light and Heavy
Majorana Neutrinos | The evidence for neutrino oscillations implies that three neutrino flavors
(\nu_e, \nu_\mu, \nu_\tau) must have different mass states (\nu_1, \nu_2,
\nu_3). The most popular idea of generating tiny masses of \nu_i is to
introduce three heavy Majorana neutrinos N_i (for i = 1, 2, 3) into the
standard model and impleme... | hep-ph | the evidence for neutrino oscillations implies that three neutrino flavors nu_e nu_mu nu_tau must have different mass states nu_1 nu_2 nu_3 the most popular idea of generating tiny masses of nu_i is to introduce three heavy majorana neutrinos n_i for i 1 2 3 into the standard model and implement the seesaw mechanism in... | [['the', 'evidence', 'for', 'neutrino', 'oscillations', 'implies', 'that', 'three', 'neutrino', 'flavors', 'nu_e', 'nu_mu', 'nu_tau', 'must', 'have', 'different', 'mass', 'states', 'nu_1', 'nu_2', 'nu_3', 'the', 'most', 'popular', 'idea', 'of', 'generating', 'tiny', 'masses', 'of', 'nu_i', 'is', 'to', 'introduce', 'thr... | [-0.13209171843715012, 0.30910171862290653, 0.033321393413158755, 0.15604514394938532, -0.03462509314736558, -0.23397550314664842, 0.030013198036079606, 0.3252248918016752, -0.22114121216090604, -0.27482331809070376, -0.011364089120696816, -0.31956317067870665, -0.050474671396530335, 0.12611020707732273, 0.072676136195... |
709.2221 | First-order restoration of SU(Nf) x SU(Nf) chiral symmetry with large Nf
and Electroweak phase transition | It has been argued by Pisarski and Wilczek that finite temperature
restoration of the chiral symmetry SU(Nf) x SU(Nf) is first-order for Nf >=3.
This type of chiral symmetry with a large Nf may appear in the Higgs sector if
one considers models such as walking technicolor theories. We examine the
first-order restorat... | hep-ph | it has been argued by pisarski and wilczek that finite temperature restoration of the chiral symmetry sunf x sunf is firstorder for nf 3 this type of chiral symmetry with a large nf may appear in the higgs sector if one considers models such as walking technicolor theories we examine the firstorder restoration of the c... | [['it', 'has', 'been', 'argued', 'by', 'pisarski', 'and', 'wilczek', 'that', 'finite', 'temperature', 'restoration', 'of', 'the', 'chiral', 'symmetry', 'sunf', 'x', 'sunf', 'is', 'firstorder', 'for', 'nf', '3', 'this', 'type', 'of', 'chiral', 'symmetry', 'with', 'a', 'large', 'nf', 'may', 'appear', 'in', 'the', 'higgs'... | [-0.12834509461441682, 0.30197737232744193, -0.018192130244160828, 0.1119429147764537, -0.0807444358118684, -0.189591720501414, 0.019780744949506747, 0.3091522787773126, -0.19042279464444398, -0.2729696477838867, 0.08194233026871509, -0.2709822693915182, -0.07140841592808028, 0.05967041886839512, 0.06961097551912472, 0... |
709.2222 | Stochastic Variational Partitioned Runge-Kutta Integrators for
Constrained Systems | Stochastic variational integrators for constrained, stochastic mechanical
systems are developed in this paper. The main results of the paper are twofold:
an equivalence is established between a stochastic Hamilton-Pontryagin (HP)
principle in generalized coordinates and constrained coordinates via Lagrange
multiplier... | math.NA math.PR | stochastic variational integrators for constrained stochastic mechanical systems are developed in this paper the main results of the paper are twofold an equivalence is established between a stochastic hamiltonpontryagin hp principle in generalized coordinates and constrained coordinates via lagrange multipliers and va... | [['stochastic', 'variational', 'integrators', 'for', 'constrained', 'stochastic', 'mechanical', 'systems', 'are', 'developed', 'in', 'this', 'paper', 'the', 'main', 'results', 'of', 'the', 'paper', 'are', 'twofold', 'an', 'equivalence', 'is', 'established', 'between', 'a', 'stochastic', 'hamiltonpontryagin', 'hp', 'pri... | [-0.14325465653313413, 0.036410790758790904, -0.08818569785216823, 0.06684478572874684, -0.05892144167973172, -0.11626551196622174, -0.0238416092473753, 0.3704068608848112, -0.3514965854673868, -0.2776226915995635, 0.09216982823619176, -0.19628123649662094, -0.17999363800377718, 0.21122021020744883, -0.1176252498269258... |
709.2223 | Damping of field-induced chemical potential oscillations in ideal
two-band compensated metals | The field and temperature dependence of the de Haas-van Alphen oscillations
spectrum is studied for an ideal two-dimensional compensated metal. It is shown
that the chemical potential oscillations, involved in the frequency
combinations observed in the case of uncompensated orbits, are strongly damped
and can even be... | cond-mat.stat-mech | the field and temperature dependence of the de haasvan alphen oscillations spectrum is studied for an ideal twodimensional compensated metal it is shown that the chemical potential oscillations involved in the frequency combinations observed in the case of uncompensated orbits are strongly damped and can even be suppre... | [['the', 'field', 'and', 'temperature', 'dependence', 'of', 'the', 'de', 'haasvan', 'alphen', 'oscillations', 'spectrum', 'is', 'studied', 'for', 'an', 'ideal', 'twodimensional', 'compensated', 'metal', 'it', 'is', 'shown', 'that', 'the', 'chemical', 'potential', 'oscillations', 'involved', 'in', 'the', 'frequency', 'c... | [-0.21681658879496418, 0.24467784146047983, -0.03410943235855463, 0.10171844950216541, -0.029611158986077753, -0.11435078603735324, -0.003753408811293369, 0.32738153419868893, -0.23367179475378158, -0.29852311991068514, 0.0340808076847637, -0.29080084129778105, -0.12363439286127687, 0.26461927283035463, 0.0164021073277... |
709.2224 | Self-similar dilatation structures and automata | We show that on the boundary of the dyadic tree, any self-similar dilatation
structure induces a web of interacting automata. This is a short version, for
publication, of the paper arXiv:math/0612509v2
| math.MG cs.DM | we show that on the boundary of the dyadic tree any selfsimilar dilatation structure induces a web of interacting automata this is a short version for publication of the paper arxivmath0612509v2 | [['we', 'show', 'that', 'on', 'the', 'boundary', 'of', 'the', 'dyadic', 'tree', 'any', 'selfsimilar', 'dilatation', 'structure', 'induces', 'a', 'web', 'of', 'interacting', 'automata', 'this', 'is', 'a', 'short', 'version', 'for', 'publication', 'of', 'the', 'paper', 'arxivmath0612509v2']] | [-0.21138874863584836, 0.15710185204322138, -0.09147332527985176, 0.07518333091090122, -0.09891183444609244, -0.03160967550550898, 0.04020247102792685, 0.3544370343287786, -0.2816448340813319, -0.17917875976612171, 0.07751267824011544, -0.26782012892266116, -0.19400053101902207, 0.1516320690823098, -0.05143410265445709... |
709.2225 | Improved Linear Parallel Interference Cancellers | In this paper, taking the view that a linear parallel interference canceller
(LPIC) can be seen as a linear matrix filter, we propose new linear matrix
filters that can result in improved bit error performance compared to other
LPICs in the literature. The motivation for the proposed filters arises from
the possibili... | cs.IT cs.SC cs.SD cs.SE math.IT | in this paper taking the view that a linear parallel interference canceller lpic can be seen as a linear matrix filter we propose new linear matrix filters that can result in improved bit error performance compared to other lpics in the literature the motivation for the proposed filters arises from the possibility of a... | [['in', 'this', 'paper', 'taking', 'the', 'view', 'that', 'a', 'linear', 'parallel', 'interference', 'canceller', 'lpic', 'can', 'be', 'seen', 'as', 'a', 'linear', 'matrix', 'filter', 'we', 'propose', 'new', 'linear', 'matrix', 'filters', 'that', 'can', 'result', 'in', 'improved', 'bit', 'error', 'performance', 'compar... | [-0.1521900136752621, 0.03311686464990287, -0.04500419197847014, 0.02175018511277259, -0.05977344428513037, -0.23347672604267364, 0.07425256402221629, 0.402862443693954, -0.2585241028958041, -0.26308663305624025, 0.11429838495298653, -0.2293434525343954, -0.19537451111650822, 0.15601565870709475, -0.1253347955259454, 0... |
709.2226 | Discovery of Bragg confined hybrid modes with high Q-factor in a hollow
dielectric resonator | The authors report on observation of Bragg confined mode in a hollow
cylindrical dielectric cavity. A resonance was observed at 13.4 $GHz$ with an
unloaded Q-factor of order $2\times10^5$, which is more than a factor of 6
above the dielectric loss limit. Previously such modes have only been realized
from pure Transve... | physics.optics physics.ins-det | the authors report on observation of bragg confined mode in a hollow cylindrical dielectric cavity a resonance was observed at 134 ghz with an unloaded qfactor of order 2times105 which is more than a factor of 6 above the dielectric loss limit previously such modes have only been realized from pure transverse electric ... | [['the', 'authors', 'report', 'on', 'observation', 'of', 'bragg', 'confined', 'mode', 'in', 'a', 'hollow', 'cylindrical', 'dielectric', 'cavity', 'a', 'resonance', 'was', 'observed', 'at', '134', 'ghz', 'with', 'an', 'unloaded', 'qfactor', 'of', 'order', '2times105', 'which', 'is', 'more', 'than', 'a', 'factor', 'of', ... | [-0.16407874267009137, 0.20031450306644394, -0.0521004325808271, -0.04584927758612474, -0.06136582393787409, -0.11597436585610635, -0.015503039952416562, 0.42347767078562787, -0.16444785085163618, -0.3159709273004218, 0.05541168054639313, -0.2830518104528126, -0.06622063055830567, 0.17940207289433793, 0.049797667131612... |
709.2227 | On the Magnitude of Dark Energy Voids and Overdensities | We investigate the clustering of dark energy within matter overdensities and
voids. In particular, we derive an analytical expression for the dark energy
density perturbations, which is valid both in the linear, quasi-linear and
fully non-linear regime of structure formation. We also investigate the
possibility of de... | astro-ph | we investigate the clustering of dark energy within matter overdensities and voids in particular we derive an analytical expression for the dark energy density perturbations which is valid both in the linear quasilinear and fully nonlinear regime of structure formation we also investigate the possibility of detecting s... | [['we', 'investigate', 'the', 'clustering', 'of', 'dark', 'energy', 'within', 'matter', 'overdensities', 'and', 'voids', 'in', 'particular', 'we', 'derive', 'an', 'analytical', 'expression', 'for', 'the', 'dark', 'energy', 'density', 'perturbations', 'which', 'is', 'valid', 'both', 'in', 'the', 'linear', 'quasilinear',... | [-0.10495836556726841, 0.15315171299483732, -0.10627018944407353, 0.16479578797971228, -0.0677724265754505, -0.037735102177277734, -0.0770729821118893, 0.3248609118963206, -0.21860113635663922, -0.37446330497605784, 0.033182727379931345, -0.2610055731251986, -0.03343828498606918, 0.12728011309030476, 0.0679815338849268... |
709.2228 | Electronic structure of spin 1/2 Heisenberg antiferromagnetic systems:
Ba_2Cu(PO_4)_2 and Sr_2Cu(PO_4)_2 | We have employed first principles calculations to study the electronic
structure and magnetic properties of the low-dimensional phosphates,
Ba2Cu(PO4)2 and Sr2Cu(PO4)2. Using the self-consistent tight-binding lin-
earized muffin-tin orbital method and the Nth order muffin-tin orbital method,
we have calculated the va... | cond-mat.str-el | we have employed first principles calculations to study the electronic structure and magnetic properties of the lowdimensional phosphates ba2cupo42 and sr2cupo42 using the selfconsistent tightbinding lin earized muffintin orbital method and the nth order muffintin orbital method we have calculated the various intrachai... | [['we', 'have', 'employed', 'first', 'principles', 'calculations', 'to', 'study', 'the', 'electronic', 'structure', 'and', 'magnetic', 'properties', 'of', 'the', 'lowdimensional', 'phosphates', 'ba2cupo42', 'and', 'sr2cupo42', 'using', 'the', 'selfconsistent', 'tightbinding', 'lin', 'earized', 'muffintin', 'orbital', '... | [-0.1858174586383512, 0.12491829247771427, -0.019878711507079146, 0.05246221935329008, -0.029967020558776196, -0.10917319582306406, 0.06690204740964434, 0.4290714672937685, -0.2814553597954666, -0.28943846802715034, -0.036496113110682134, -0.3223012937803049, -0.14175447218672874, 0.1518591385561225, 0.1317394789067559... |
709.2229 | Novel QCD Effects from Initial and Final State Interactions | Initial-state and final-state interactions, which are conventionally
neglected in the parton model, have a profound effect in QCD hard-scattering
reactions. These effects, which arise from gluon exchange between the active
and spectator quarks, cause leading-twist single-spin asymmetries, diffractive
deep inelastic s... | hep-ph | initialstate and finalstate interactions which are conventionally neglected in the parton model have a profound effect in qcd hardscattering reactions these effects which arise from gluon exchange between the active and spectator quarks cause leadingtwist singlespin asymmetries diffractive deep inelastic scattering dif... | [['initialstate', 'and', 'finalstate', 'interactions', 'which', 'are', 'conventionally', 'neglected', 'in', 'the', 'parton', 'model', 'have', 'a', 'profound', 'effect', 'in', 'qcd', 'hardscattering', 'reactions', 'these', 'effects', 'which', 'arise', 'from', 'gluon', 'exchange', 'between', 'the', 'active', 'and', 'spec... | [-0.043051594260162605, 0.31868254958387854, -0.18858918668476365, 0.270687269019102, -0.037448880554579976, -0.06181280064890022, -0.03726319317817132, 0.3855510145815006, -0.24730888124444148, -0.16945207829295256, -0.12574197195553735, -0.33779804773781613, -0.04242302298045425, 0.053650667951720306, 0.1326704479531... |
709.223 | Hard X-ray Variability of AGN | Aims: Active Galactic Nuclei are known to be variable throughout the
electromagnetic spectrum. An energy domain poorly studied in this respect is
the hard X-ray range above 20 keV.
Methods: The first 9 months of the Swift/BAT all-sky survey are used to study
the 14 - 195 keV variability of the 44 brightest AGN. The... | astro-ph | aims active galactic nuclei are known to be variable throughout the electromagnetic spectrum an energy domain poorly studied in this respect is the hard xray range above 20 kev methods the first 9 months of the swiftbat allsky survey are used to study the 14 195 kev variability of the 44 brightest agn the sources have ... | [['aims', 'active', 'galactic', 'nuclei', 'are', 'known', 'to', 'be', 'variable', 'throughout', 'the', 'electromagnetic', 'spectrum', 'an', 'energy', 'domain', 'poorly', 'studied', 'in', 'this', 'respect', 'is', 'the', 'hard', 'xray', 'range', 'above', '20', 'kev', 'methods', 'the', 'first', '9', 'months', 'of', 'the',... | [-0.028852353319827537, 0.11911155979955597, -0.020755297689767624, 0.18850409290731746, -0.07032514020425475, -0.10396867548762304, 0.0430858624642025, 0.4783211331297126, -0.1528800859491134, -0.4060891884871159, 0.10360213791675589, -0.3674164086826042, 0.00773896393258366, 0.19676023092405456, -0.03407530337830798,... |
709.2231 | Biased random walks on complex networks: the role of local navigation
rules | We study the biased random walk process in random uncorrelated networks with
arbitrary degree distributions. In our model, the bias is defined by the
preferential transition probability, which, in recent years, has been commonly
used to study efficiency of different routing protocols in communication
networks. We der... | cond-mat.dis-nn cond-mat.stat-mech | we study the biased random walk process in random uncorrelated networks with arbitrary degree distributions in our model the bias is defined by the preferential transition probability which in recent years has been commonly used to study efficiency of different routing protocols in communication networks we derive exac... | [['we', 'study', 'the', 'biased', 'random', 'walk', 'process', 'in', 'random', 'uncorrelated', 'networks', 'with', 'arbitrary', 'degree', 'distributions', 'in', 'our', 'model', 'the', 'bias', 'is', 'defined', 'by', 'the', 'preferential', 'transition', 'probability', 'which', 'in', 'recent', 'years', 'has', 'been', 'com... | [-0.1450569286765087, 0.09772348276649913, -0.048982242233164254, 0.05328789960790129, 0.010482066594773815, -0.1255648995971396, 0.08873847005112717, 0.4017587589011306, -0.21499409606192438, -0.28791156920293964, 0.07703841380841497, -0.2470369549556857, -0.16950924400949763, 0.1794433007970275, -0.059198027849197386... |
709.2232 | Effect of SUSY-QCD corrections to neutralino annihilation on the cold
dark matter relic density in the Higgs funnel | We present a complete calculation of the QCD and SUSY-QCD corrections to
neutralino pair annihilation into bottom quark-antiquark pairs through exchange
of a pseudoscalar Higgs boson, which is the dominant process in the
cosmological A-funnel region of the mSUGRA model. We present numerical
predictions for the annihi... | hep-ph | we present a complete calculation of the qcd and susyqcd corrections to neutralino pair annihilation into bottom quarkantiquark pairs through exchange of a pseudoscalar higgs boson which is the dominant process in the cosmological afunnel region of the msugra model we present numerical predictions for the annihilation ... | [['we', 'present', 'a', 'complete', 'calculation', 'of', 'the', 'qcd', 'and', 'susyqcd', 'corrections', 'to', 'neutralino', 'pair', 'annihilation', 'into', 'bottom', 'quarkantiquark', 'pairs', 'through', 'exchange', 'of', 'a', 'pseudoscalar', 'higgs', 'boson', 'which', 'is', 'the', 'dominant', 'process', 'in', 'the', '... | [-0.09385663458877909, 0.1565884141650583, -0.0813615158067218, 0.16474333230468932, -0.08243736977622446, -0.06999288979651673, 0.0425218361163778, 0.3142146896570921, -0.18441015260427127, -0.26603298224259303, -0.03899670225468331, -0.3239863320785974, 0.047941193323848504, 0.12634801412766267, 0.1099073083368629, 0... |
709.2233 | Pseudo-maximization and self-normalized processes | Self-normalized processes are basic to many probabilistic and statistical
studies. They arise naturally in the the study of stochastic integrals,
martingale inequalities and limit theorems, likelihood-based methods in
hypothesis testing and parameter estimation, and Studentized pivots and
bootstrap-$t$ methods for co... | math.PR | selfnormalized processes are basic to many probabilistic and statistical studies they arise naturally in the the study of stochastic integrals martingale inequalities and limit theorems likelihoodbased methods in hypothesis testing and parameter estimation and studentized pivots and bootstrapt methods for confidence in... | [['selfnormalized', 'processes', 'are', 'basic', 'to', 'many', 'probabilistic', 'and', 'statistical', 'studies', 'they', 'arise', 'naturally', 'in', 'the', 'the', 'study', 'of', 'stochastic', 'integrals', 'martingale', 'inequalities', 'and', 'limit', 'theorems', 'likelihoodbased', 'methods', 'in', 'hypothesis', 'testin... | [-0.06419930225048139, 0.08398977959794658, -0.07582113939673216, 0.12114008604974787, -0.04281805029620423, -0.12277043753518996, 0.05827148144013014, 0.33636532091142823, -0.2521790572343914, -0.28036697132855043, 0.14943296771471193, -0.26168951142553976, -0.1554561306779482, 0.22413787737862542, -0.0792067110582831... |
709.2234 | Soliton percolation in random optical lattices | We introduce soliton percolation phenomena in the nonlinear transport of
light packets in suitable optical lattices with random properties.
Specifically, we address lattices with a gradient of the refractive index in
the transverse plane, featuring stochastic phase or amplitude fluctuations, and
we discover the exist... | physics.optics nlin.PS | we introduce soliton percolation phenomena in the nonlinear transport of light packets in suitable optical lattices with random properties specifically we address lattices with a gradient of the refractive index in the transverse plane featuring stochastic phase or amplitude fluctuations and we discover the existence o... | [['we', 'introduce', 'soliton', 'percolation', 'phenomena', 'in', 'the', 'nonlinear', 'transport', 'of', 'light', 'packets', 'in', 'suitable', 'optical', 'lattices', 'with', 'random', 'properties', 'specifically', 'we', 'address', 'lattices', 'with', 'a', 'gradient', 'of', 'the', 'refractive', 'index', 'in', 'the', 'tr... | [-0.18735609975500175, 0.24546839306966808, -0.061975996039855555, 0.03399973689691904, -0.02716882407474212, -0.14649502916906315, 0.07221970803295381, 0.42935297888918567, -0.2862111672353095, -0.229990100607467, 0.08604230619489382, -0.306254841052951, -0.1719790771514034, 0.1257142520073849, 0.017201938236562107, 0... |
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