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708.3449 | On Local Behavior of Holomorphic Functions Along Complex Submanifolds of
C^N | In this paper we establish some general results on local behavior of
holomorphic functions along complex submanifolds of $\Co^{N}$. As a corollary,
we present multi-dimensional generalizations of an important result of Coman
and Poletsky on Bernstein type inequalities on transcendental curves in
$\Co^{2}$.
| math.CV math.FA | in this paper we establish some general results on local behavior of holomorphic functions along complex submanifolds of con as a corollary we present multidimensional generalizations of an important result of coman and poletsky on bernstein type inequalities on transcendental curves in co2 | [['in', 'this', 'paper', 'we', 'establish', 'some', 'general', 'results', 'on', 'local', 'behavior', 'of', 'holomorphic', 'functions', 'along', 'complex', 'submanifolds', 'of', 'con', 'as', 'a', 'corollary', 'we', 'present', 'multidimensional', 'generalizations', 'of', 'an', 'important', 'result', 'of', 'coman', 'and',... | [-0.1411762141736311, -0.008620410872999643, -0.04940392202589401, 0.12144933570295485, -0.08177637243859989, -0.0652636487448458, 0.016178882634808676, 0.3189660077264836, -0.25182877145274435, -0.18032604542582534, 0.10761899268796105, -0.2499552822650172, -0.23182582993840062, 0.29562159471733623, -0.165910165951868... |
708.345 | Mediation of Long-Range Attraction Selectively between
Negatively-Charged Colloids on Surfaces by Solvation | We propose a mean-field analytical model to account for the observed
asymmetry in the ability to form long-range attraction by the negatively
charged colloidal particles and not their equivalently charged positive
counterpart. We conjecture that this asymmetry is due to solvation effects, and
we phenomenologically ca... | cond-mat.soft cond-mat.mtrl-sci | we propose a meanfield analytical model to account for the observed asymmetry in the ability to form longrange attraction by the negatively charged colloidal particles and not their equivalently charged positive counterpart we conjecture that this asymmetry is due to solvation effects and we phenomenologically capture ... | [['we', 'propose', 'a', 'meanfield', 'analytical', 'model', 'to', 'account', 'for', 'the', 'observed', 'asymmetry', 'in', 'the', 'ability', 'to', 'form', 'longrange', 'attraction', 'by', 'the', 'negatively', 'charged', 'colloidal', 'particles', 'and', 'not', 'their', 'equivalently', 'charged', 'positive', 'counterpart'... | [-0.11789093418240858, 0.22481225229676055, -0.06094743051022912, 0.07350765722318707, 0.016270566211702923, -0.15084317175593848, 0.040787548385560514, 0.36410253022331746, -0.2554418533264349, -0.29730570927010075, -0.03267299442280394, -0.3156549892756933, -0.13265463996989033, 0.05028266044876849, 0.022369256506984... |
708.3451 | Diophantine subsets of function fields of curves | We consider diophantine subsets of function fields of curves and show,
roughly speaking, that they are either very small or very large. In particular,
this implies that the ring of polynomials $k[t]$ is a not a diophantine subset
of the field of rational functions $k(t)$ for many fields $k$.
| math.NT math.AG | we consider diophantine subsets of function fields of curves and show roughly speaking that they are either very small or very large in particular this implies that the ring of polynomials kt is a not a diophantine subset of the field of rational functions kt for many fields k | [['we', 'consider', 'diophantine', 'subsets', 'of', 'function', 'fields', 'of', 'curves', 'and', 'show', 'roughly', 'speaking', 'that', 'they', 'are', 'either', 'very', 'small', 'or', 'very', 'large', 'in', 'particular', 'this', 'implies', 'that', 'the', 'ring', 'of', 'polynomials', 'kt', 'is', 'a', 'not', 'a', 'diopha... | [-0.2529967817078744, 0.12382678786406712, -0.0912319161758131, 0.06957951514050364, -0.05408115561443324, -0.12708094738879983, 0.002580985379386313, 0.34121116724017325, -0.2995066008701616, -0.22099779759134566, 0.09569091908396127, -0.22827161073076482, -0.11433486410948847, 0.2574319802937383, -0.08897173298256737... |
708.3452 | Scattering on D3-branes | In a direct open string approach we analyze scattering of massless states on
a stack of D3-branes. First we construct vertex operators on the D-branes. The
4+6 splitting for the fermionic part is made possible by inserting
appropriately defined projection operators. With the vertex operators
constructed we compute va... | hep-th | in a direct open string approach we analyze scattering of massless states on a stack of d3branes first we construct vertex operators on the dbranes the 46 splitting for the fermionic part is made possible by inserting appropriately defined projection operators with the vertex operators constructed we compute various tr... | [['in', 'a', 'direct', 'open', 'string', 'approach', 'we', 'analyze', 'scattering', 'of', 'massless', 'states', 'on', 'a', 'stack', 'of', 'd3branes', 'first', 'we', 'construct', 'vertex', 'operators', 'on', 'the', 'dbranes', 'the', '46', 'splitting', 'for', 'the', 'fermionic', 'part', 'is', 'made', 'possible', 'by', 'i... | [-0.14543414347817338, 0.15502629099309592, -0.039691625352899884, 0.10831292237210284, -0.04723138252187422, -0.11802968610764335, 0.03730873082684794, 0.36726108293882326, -0.1805774264135643, -0.2449938855501578, 0.10807863434647995, -0.3372895723993057, -0.14887718659041352, 0.1281793100244709, -0.02221354014718121... |
708.3453 | Asymptotic behavior of the rate of adaptation | We consider the accumulation of beneficial and deleterious mutations in large
asexual populations. The rate of adaptation is affected by the total mutation
rate, proportion of beneficial mutations and population size $N$. We show that
regardless of mutation rates, as long as the proportion of beneficial mutations
is ... | math.PR | we consider the accumulation of beneficial and deleterious mutations in large asexual populations the rate of adaptation is affected by the total mutation rate proportion of beneficial mutations and population size n we show that regardless of mutation rates as long as the proportion of beneficial mutations is strictly... | [['we', 'consider', 'the', 'accumulation', 'of', 'beneficial', 'and', 'deleterious', 'mutations', 'in', 'large', 'asexual', 'populations', 'the', 'rate', 'of', 'adaptation', 'is', 'affected', 'by', 'the', 'total', 'mutation', 'rate', 'proportion', 'of', 'beneficial', 'mutations', 'and', 'population', 'size', 'n', 'we',... | [-0.1419739303357824, 0.19863147201543355, 0.017739064370592434, 0.08854681791295532, 0.004101861047210416, -0.181509359697388, 0.11255289689929347, 0.3436964187357161, -0.2710853860421915, -0.23173924524224165, 0.09791270091969784, -0.21828790110620586, -0.16812404676462817, 0.16251290235856566, -0.13081430809835742, ... |
708.3454 | First-person visualizations of the special and general theory of
relativity | Visualizations that adopt a first-person point of view allow observation and,
in the case of interactive simulations, experimentation with relativistic
scenes. This paper gives examples of three types of first-person
visualizations: watching objects that move at nearly the speed of light, being
a high-speed observer ... | physics.ed-ph | visualizations that adopt a firstperson point of view allow observation and in the case of interactive simulations experimentation with relativistic scenes this paper gives examples of three types of firstperson visualizations watching objects that move at nearly the speed of light being a highspeed observer looking at... | [['visualizations', 'that', 'adopt', 'a', 'firstperson', 'point', 'of', 'view', 'allow', 'observation', 'and', 'in', 'the', 'case', 'of', 'interactive', 'simulations', 'experimentation', 'with', 'relativistic', 'scenes', 'this', 'paper', 'gives', 'examples', 'of', 'three', 'types', 'of', 'firstperson', 'visualizations'... | [-0.06396684421298023, 0.06153106815539874, -0.12287413948215545, 0.06819622517617133, -0.14745193076176713, -0.17156337238131808, 0.04189391095838241, 0.38850782922684, -0.19693905317511123, -0.3643125665875582, 0.08824890143273828, -0.30086337551474573, -0.1549460527451279, 0.20922560421033548, -0.11723243873566389, ... |
708.3455 | On the Range of Validity of the Dipole Picture | We derive correlated bounds on ratios of deep inelastic structure functions
from the dipole picture of photon-hadron scattering at high energies. In
particular we consider ratios of the longitudinal structure function, the total
structure function and the charm part of the latter. We also consider ratios of
total str... | hep-ph hep-ex | we derive correlated bounds on ratios of deep inelastic structure functions from the dipole picture of photonhadron scattering at high energies in particular we consider ratios of the longitudinal structure function the total structure function and the charm part of the latter we also consider ratios of total structure... | [['we', 'derive', 'correlated', 'bounds', 'on', 'ratios', 'of', 'deep', 'inelastic', 'structure', 'functions', 'from', 'the', 'dipole', 'picture', 'of', 'photonhadron', 'scattering', 'at', 'high', 'energies', 'in', 'particular', 'we', 'consider', 'ratios', 'of', 'the', 'longitudinal', 'structure', 'function', 'the', 't... | [-0.09242190017886016, 0.14809518826327153, -0.07365500788381767, 0.13812352216475465, 0.002748388663998672, -0.041050425120851115, 0.037086594957924844, 0.3835255404202534, -0.23406407012260474, -0.33196049922012855, -0.010867392595779771, -0.3039461623189882, -0.057151671986849534, 0.17006188521017543, 0.086435731012... |
708.3456 | Index theorems for quantum graphs | In geometric analysis, an index theorem relates the difference of the numbers
of solutions of two differential equations to the topological structure of the
manifold or bundle concerned, sometimes using the heat kernels of two
higher-order differential operators as an intermediary. In this paper, the case
of quantum ... | math.SP math-ph math.MP | in geometric analysis an index theorem relates the difference of the numbers of solutions of two differential equations to the topological structure of the manifold or bundle concerned sometimes using the heat kernels of two higherorder differential operators as an intermediary in this paper the case of quantum graphs ... | [['in', 'geometric', 'analysis', 'an', 'index', 'theorem', 'relates', 'the', 'difference', 'of', 'the', 'numbers', 'of', 'solutions', 'of', 'two', 'differential', 'equations', 'to', 'the', 'topological', 'structure', 'of', 'the', 'manifold', 'or', 'bundle', 'concerned', 'sometimes', 'using', 'the', 'heat', 'kernels', '... | [-0.17108164151606617, 0.09887557602749439, -0.08222210524370893, 0.05234005737816915, -0.08718973204260692, -0.10416574765229597, -0.014872248632309492, 0.30655508967116474, -0.296123346015811, -0.2504296584636904, 0.12100057091622148, -0.2951620140053274, -0.14375024705077522, 0.15660547533610952, -0.0475841705134371... |
708.3457 | Enhanced Group Analysis and Exact Solutions of Variable Coefficient
Semilinear Diffusion Equations with a Power Source | A new approach to group classification problems and more general
investigations on transformational properties of classes of differential
equations is proposed. It is based on mappings between classes of differential
equations, generated by families of point transformations. A class of variable
coefficient (1+1)-dime... | math-ph math.MP nlin.SI | a new approach to group classification problems and more general investigations on transformational properties of classes of differential equations is proposed it is based on mappings between classes of differential equations generated by families of point transformations a class of variable coefficient 11dimensional s... | [['a', 'new', 'approach', 'to', 'group', 'classification', 'problems', 'and', 'more', 'general', 'investigations', 'on', 'transformational', 'properties', 'of', 'classes', 'of', 'differential', 'equations', 'is', 'proposed', 'it', 'is', 'based', 'on', 'mappings', 'between', 'classes', 'of', 'differential', 'equations',... | [-0.11854699381173735, 0.04536369040694186, -0.046310006639626075, 0.042528196898485096, -0.08411690290331056, -0.12636009770396509, -0.0016948367076876916, 0.3028640150435661, -0.30584405826306654, -0.3012989774827331, 0.1047601039306947, -0.2854935437182001, -0.17199244594544563, 0.2487031104729364, -0.03599700330462... |
708.3458 | First Law, Counterterms and Kerr-AdS_5 Black Holes | We apply the counterterm subtraction technique to calculate the action and
other quantities for the Kerr--AdS black hole in five dimensions using two
boundary metrics; the Einstein universe and rotating Einstein universe with
arbitrary angular velocity. In both cases, the resulting thermodynamic
quantities satisfy th... | hep-th | we apply the counterterm subtraction technique to calculate the action and other quantities for the kerrads black hole in five dimensions using two boundary metrics the einstein universe and rotating einstein universe with arbitrary angular velocity in both cases the resulting thermodynamic quantities satisfy the first... | [['we', 'apply', 'the', 'counterterm', 'subtraction', 'technique', 'to', 'calculate', 'the', 'action', 'and', 'other', 'quantities', 'for', 'the', 'kerrads', 'black', 'hole', 'in', 'five', 'dimensions', 'using', 'two', 'boundary', 'metrics', 'the', 'einstein', 'universe', 'and', 'rotating', 'einstein', 'universe', 'wit... | [-0.15291551055593622, 0.09484449722908604, -0.13535032450802562, 0.058785437730650425, -0.0904518694927295, -0.12634019476847133, -0.03132536784451232, 0.30251009797311235, -0.1691165145399033, -0.27034648853696436, 0.07873156412532474, -0.2916156163470995, -0.08138719628342132, 0.2018579079821292, -0.0365622589587528... |
708.3459 | Bulk viscosity of gauge theory plasma at strong coupling | We propose a lower bound on bulk viscosity of strongly coupled gauge theory
plasmas. Using explicit example of the N=2^* gauge theory plasma we show that
the bulk viscosity remains finite at a critical point with a divergent specific
heat. We present an estimate for the bulk viscosity of QGP plasma at RHIC.
| hep-th | we propose a lower bound on bulk viscosity of strongly coupled gauge theory plasmas using explicit example of the n2 gauge theory plasma we show that the bulk viscosity remains finite at a critical point with a divergent specific heat we present an estimate for the bulk viscosity of qgp plasma at rhic | [['we', 'propose', 'a', 'lower', 'bound', 'on', 'bulk', 'viscosity', 'of', 'strongly', 'coupled', 'gauge', 'theory', 'plasmas', 'using', 'explicit', 'example', 'of', 'the', 'n2', 'gauge', 'theory', 'plasma', 'we', 'show', 'that', 'the', 'bulk', 'viscosity', 'remains', 'finite', 'at', 'a', 'critical', 'point', 'with', '... | [-0.13177081010357108, 0.265662022192253, -0.13447879957702924, 0.012873559364310975, -0.03494349034186804, -0.12485995517059598, 0.015589564977178597, 0.3014772434033594, -0.21476713701520325, -0.2284928727543579, 0.037717809276831035, -0.301411790272467, -0.06406442755240209, 0.1386552106343069, 0.01751735112366249, ... |
708.346 | First-principles study of a single-molecule magnet Mn_{12} monolayer on
the Au(111) surface | The electronic structure of a monolayer of single-molecule magnets Mn$_{12}$
on a Au(111) surface is studied using spin-polarized density-functional theory.
The Mn$_{12}$ molecules are oriented such that the magnetic easy axis is normal
to the surface, and the terminating ligands in the Mn$_{12}$ are replaced by
thio... | cond-mat.mtrl-sci | the electronic structure of a monolayer of singlemolecule magnets mn_12 on a au111 surface is studied using spinpolarized densityfunctional theory the mn_12 molecules are oriented such that the magnetic easy axis is normal to the surface and the terminating ligands in the mn_12 are replaced by thiol groups sh where the... | [['the', 'electronic', 'structure', 'of', 'a', 'monolayer', 'of', 'singlemolecule', 'magnets', 'mn_12', 'on', 'a', 'au111', 'surface', 'is', 'studied', 'using', 'spinpolarized', 'densityfunctional', 'theory', 'the', 'mn_12', 'molecules', 'are', 'oriented', 'such', 'that', 'the', 'magnetic', 'easy', 'axis', 'is', 'norma... | [-0.11547203637545177, 0.18432332650000605, 0.015138278494736082, 0.028110760238773205, 0.028982339023302, -0.10087260277043178, 0.09923131937250952, 0.39279720392404943, -0.26528671476336424, -0.3477645790825287, -0.05112910997367611, -0.35670698585086746, -0.031783553657301684, 0.14220410742666245, 0.0516038596809825... |
708.3461 | Quaternion-Octonion Analyticity for Abelian and Non-Abelian Gauge
Theories of Dyons | Einstein- Schroedinger (ES) non-symmetric theory has been extended to
accommodate the Abelian and non-Abelian gauge theories of dyons in terms of the
quaternion-octonion metric realization. Corresponding covariant derivatives for
complex, quaternion and octonion spaces in internal gauge groups are shown to
describe t... | hep-th | einstein schroedinger es nonsymmetric theory has been extended to accommodate the abelian and nonabelian gauge theories of dyons in terms of the quaternionoctonion metric realization corresponding covariant derivatives for complex quaternion and octonion spaces in internal gauge groups are shown to describe the consist... | [['einstein', 'schroedinger', 'es', 'nonsymmetric', 'theory', 'has', 'been', 'extended', 'to', 'accommodate', 'the', 'abelian', 'and', 'nonabelian', 'gauge', 'theories', 'of', 'dyons', 'in', 'terms', 'of', 'the', 'quaternionoctonion', 'metric', 'realization', 'corresponding', 'covariant', 'derivatives', 'for', 'complex... | [-0.14851224517320938, 0.20669306892074368, -0.09140743951293383, 0.14637778802066448, -0.1630055127774385, -0.10835388095732382, -0.10820528591656067, 0.32149048718286954, -0.1670773177348236, -0.2656013922012867, 0.005788466647921249, -0.22460496537585525, -0.19496631040733228, 0.09316998955972017, -0.073912915558197... |
708.3462 | Search for pulsed multi-TeV gamma rays from the Crab pulsar using the
Tibet-III air shower array | We searched for pulsed gamma-ray emissions from the Crab pulsar using data of
the Tibet-III air shower array from November 1999 through November 2005. No
evidence for the pulsed emissions was found in our analysis. Upper limits at
different energies were calculated for a $3 \sigma$ confidence level in the
energy rang... | astro-ph | we searched for pulsed gammaray emissions from the crab pulsar using data of the tibetiii air shower array from november 1999 through november 2005 no evidence for the pulsed emissions was found in our analysis upper limits at different energies were calculated for a 3 sigma confidence level in the energy range of mult... | [['we', 'searched', 'for', 'pulsed', 'gammaray', 'emissions', 'from', 'the', 'crab', 'pulsar', 'using', 'data', 'of', 'the', 'tibetiii', 'air', 'shower', 'array', 'from', 'november', '1999', 'through', 'november', '2005', 'no', 'evidence', 'for', 'the', 'pulsed', 'emissions', 'was', 'found', 'in', 'our', 'analysis', 'u... | [-0.02899534219940161, 0.18412917267916531, -0.04018464185104802, 0.15814102823235865, -0.02101393596365534, -0.024193257482818746, 0.061572153747467134, 0.45825810064079947, -0.14341356036060587, -0.4712878327559808, 0.10839358306538056, -0.337628545255625, 0.055085815328719284, 0.29335943495469363, 0.0891135975172550... |
708.3463 | A Neural Networks Model of the Venezuelan Economy | Besides an indicator of the GDP, the Central Bank of Venezuela generates the
so called Monthly Economic Activity General Indicator. The a priori knowledge
of this indicator, which represents and sometimes even anticipates the
economy's fluctuations, could be helpful in developing public policies and in
investment dec... | cs.CE cs.NE | besides an indicator of the gdp the central bank of venezuela generates the so called monthly economic activity general indicator the a priori knowledge of this indicator which represents and sometimes even anticipates the economys fluctuations could be helpful in developing public policies and in investment decision m... | [['besides', 'an', 'indicator', 'of', 'the', 'gdp', 'the', 'central', 'bank', 'of', 'venezuela', 'generates', 'the', 'so', 'called', 'monthly', 'economic', 'activity', 'general', 'indicator', 'the', 'a', 'priori', 'knowledge', 'of', 'this', 'indicator', 'which', 'represents', 'and', 'sometimes', 'even', 'anticipates', ... | [-0.08039551341023884, 0.038941563830456674, -0.1291842822377619, 0.14309244263322876, -0.06924113849297435, -0.09890891495160758, 0.07034349202570554, 0.34583980359725264, -0.23323025428812558, -0.2938626630868959, 0.17443503467611185, -0.2183869673968538, -0.20056510292679855, 0.2400658596490853, -0.148684766299802, ... |
708.3464 | A Non Parametric Study of the Volatility of the Economy as a Country
Risk Predictor | This paper intends to explain Venezuela's country spread behavior through the
Neural Networks analysis of a monthly economic activity general index of
economic indicators constructed by the Central Bank of Venezuela, a measure of
the shocks affecting country risk of emerging markets and the U.S. short term
interest r... | cs.CE cs.NE | this paper intends to explain venezuelas country spread behavior through the neural networks analysis of a monthly economic activity general index of economic indicators constructed by the central bank of venezuela a measure of the shocks affecting country risk of emerging markets and the us short term interest rate th... | [['this', 'paper', 'intends', 'to', 'explain', 'venezuelas', 'country', 'spread', 'behavior', 'through', 'the', 'neural', 'networks', 'analysis', 'of', 'a', 'monthly', 'economic', 'activity', 'general', 'index', 'of', 'economic', 'indicators', 'constructed', 'by', 'the', 'central', 'bank', 'of', 'venezuela', 'a', 'meas... | [-0.10727656197651655, 0.0036313063553475504, -0.08078673589220152, 0.15149836830906807, -0.06035871377002589, -0.10725584235985446, 0.14245279078059417, 0.3516239060348348, -0.2544366589900625, -0.27980119338895704, 0.11803328634322255, -0.29792607627526113, -0.20008875398979156, 0.18646018386853835, -0.12153505360636... |
708.3465 | An Early Warning System for Bankruptcy Prediction: lessons from the
Venezuelan Bank Crisis | During 1993-94 Venezuela experienced a severe banking crisis which ended up
with 18 commercial banks intervened by the government. Here we develop an early
warning system for detecting credit related bankruptcy through discriminant
functions developed on financial and macroeconomic data predating the crisis. A
robust... | cs.CE | during 199394 venezuela experienced a severe banking crisis which ended up with 18 commercial banks intervened by the government here we develop an early warning system for detecting credit related bankruptcy through discriminant functions developed on financial and macroeconomic data predating the crisis a robustness ... | [['during', '199394', 'venezuela', 'experienced', 'a', 'severe', 'banking', 'crisis', 'which', 'ended', 'up', 'with', '18', 'commercial', 'banks', 'intervened', 'by', 'the', 'government', 'here', 'we', 'develop', 'an', 'early', 'warning', 'system', 'for', 'detecting', 'credit', 'related', 'bankruptcy', 'through', 'disc... | [-0.0568149971758764, 0.04719872825319991, -0.08715576751605619, 0.12292306988553109, -0.04580118559017966, -0.14500820020190144, 0.10732828372429255, 0.33481184006491793, -0.18008521308863087, -0.3254322118915712, 0.24319694893540744, -0.33732582265629046, -0.1450339801067227, 0.20475373614308295, -0.16254262599056657... |
708.3466 | Photoionization of Clustered Halos by the First Stars | We present numerical simulations of the photoevaporation of cosmological
halos clustered around a 120 M$_\odot$ primordial star, confining our study to
structures capable of hosting Population III star formation. The calculations
include self-consistent multifrequency conservative transfer of UV photons
together with... | astro-ph | we present numerical simulations of the photoevaporation of cosmological halos clustered around a 120 m_odot primordial star confining our study to structures capable of hosting population iii star formation the calculations include selfconsistent multifrequency conservative transfer of uv photons together with ninespe... | [['we', 'present', 'numerical', 'simulations', 'of', 'the', 'photoevaporation', 'of', 'cosmological', 'halos', 'clustered', 'around', 'a', '120', 'm_odot', 'primordial', 'star', 'confining', 'our', 'study', 'to', 'structures', 'capable', 'of', 'hosting', 'population', 'iii', 'star', 'formation', 'the', 'calculations', ... | [-0.06036907007907179, 0.17568941071671856, -0.008272906687025997, 0.10063283940504665, -0.05108929614123719, -0.07179746760732748, 0.0518421518499963, 0.40293351882560685, -0.15696523110488092, -0.36685959196580703, 0.049255081085191874, -0.2759375142060559, 0.01181943064915355, 0.14568167340476065, 0.0185459144805050... |
708.3467 | Analytical modelling of terminal properties in industrial growth | In this pedagogical study, carried out by adopting standard mathematical
methods of nonlinear dynamics, we have presented some simple analytical models
to understand terminal behaviour in industrial growth. This issue has also been
addressed from a dynamical systems perspective, with especial emphasis on the
concept ... | q-fin.GN physics.soc-ph | in this pedagogical study carried out by adopting standard mathematical methods of nonlinear dynamics we have presented some simple analytical models to understand terminal behaviour in industrial growth this issue has also been addressed from a dynamical systems perspective with especial emphasis on the concept of the... | [['in', 'this', 'pedagogical', 'study', 'carried', 'out', 'by', 'adopting', 'standard', 'mathematical', 'methods', 'of', 'nonlinear', 'dynamics', 'we', 'have', 'presented', 'some', 'simple', 'analytical', 'models', 'to', 'understand', 'terminal', 'behaviour', 'in', 'industrial', 'growth', 'this', 'issue', 'has', 'also'... | [-0.06982853265960494, 0.08880641388063454, -0.138535246065499, 0.07426121967904045, -0.08973675436065251, -0.10509134679833496, 0.040899861657104436, 0.37401513402481507, -0.23877358584799147, -0.29054005365918745, 0.14814716862161462, -0.24272033096534895, -0.19846161323655773, 0.23470526920544021, -0.073039414043907... |
708.3468 | Weak ferromagnetism and spin glass state with nano-sized nickel carbide | Ni3C nanoparticles of about 40 nm have been studied experimentally to exhibit
weak ferromagnetic (FM), spin-glass (SG) and paramagnetic (PM) properties. The
freezing temperature of the SG phase at zero applied field is determined as,
TF0 ~ 11.0 K. At T > TF0, a very weak ferromagnetism has been observed over a
PM bac... | cond-mat.mtrl-sci | ni3c nanoparticles of about 40 nm have been studied experimentally to exhibit weak ferromagnetic fm spinglass sg and paramagnetic pm properties the freezing temperature of the sg phase at zero applied field is determined as tf0 110 k at t tf0 a very weak ferromagnetism has been observed over a pm background the curie t... | [['ni3c', 'nanoparticles', 'of', 'about', '40', 'nm', 'have', 'been', 'studied', 'experimentally', 'to', 'exhibit', 'weak', 'ferromagnetic', 'fm', 'spinglass', 'sg', 'and', 'paramagnetic', 'pm', 'properties', 'the', 'freezing', 'temperature', 'of', 'the', 'sg', 'phase', 'at', 'zero', 'applied', 'field', 'is', 'determin... | [-0.15251654102842535, 0.243074923919818, -0.04080091147052665, 0.03721709159923898, -0.024831281341011487, -0.14132611680129964, 0.08071154981171863, 0.37834278285022704, -0.24054717958694505, -0.3316237421210615, 0.047566123500526435, -0.3334894076891003, 0.005480066930214244, 0.15908576542090985, 0.05427812777099109... |
708.3469 | Electronic structure of self-assembled InAs/InP quantum dots: A
Comparison with self-assembled InAs/GaAs quantum dots | We investigate the electronic structure of the InAs/InP quantum dots using an
atomistic pseudopotential method and compare them to those of the InAs/GaAs
QDs. We show that even though the InAs/InP and InAs/GaAs dots have the same dot
material, their electronic structure differ significantly in certain aspects,
especi... | cond-mat.mtrl-sci | we investigate the electronic structure of the inasinp quantum dots using an atomistic pseudopotential method and compare them to those of the inasgaas qds we show that even though the inasinp and inasgaas dots have the same dot material their electronic structure differ significantly in certain aspects especially for ... | [['we', 'investigate', 'the', 'electronic', 'structure', 'of', 'the', 'inasinp', 'quantum', 'dots', 'using', 'an', 'atomistic', 'pseudopotential', 'method', 'and', 'compare', 'them', 'to', 'those', 'of', 'the', 'inasgaas', 'qds', 'we', 'show', 'that', 'even', 'though', 'the', 'inasinp', 'and', 'inasgaas', 'dots', 'have... | [-0.11055808011681223, 0.18911960892482266, 0.01690936223961986, 0.06838220747617575, 0.11859392669120541, -0.22582233655385864, 0.030362760816485836, 0.4664612140028905, -0.21800518112543685, -0.3427890382325038, -0.03343815225809335, -0.33642422715440773, -0.015856443976577466, 0.17989250495313452, 0.0586573777577051... |
708.347 | Effects of mode degeneracy in the LIGO Livingston Observatory recycling
cavity | We analyze the electromagnetic fields in a Pound-Drever-Hall locked,
marginally unstable, Fabry-Perot cavity as a function of small changes in the
cavity length during resonance. More specifically, we compare the results of a
detailed numerical model with the behavior of the recycling cavity of the Laser
Interferomet... | gr-qc | we analyze the electromagnetic fields in a pounddreverhall locked marginally unstable fabryperot cavity as a function of small changes in the cavity length during resonance more specifically we compare the results of a detailed numerical model with the behavior of the recycling cavity of the laser interferometer gravit... | [['we', 'analyze', 'the', 'electromagnetic', 'fields', 'in', 'a', 'pounddreverhall', 'locked', 'marginally', 'unstable', 'fabryperot', 'cavity', 'as', 'a', 'function', 'of', 'small', 'changes', 'in', 'the', 'cavity', 'length', 'during', 'resonance', 'more', 'specifically', 'we', 'compare', 'the', 'results', 'of', 'a', ... | [-0.19294214807898522, 0.21712377087725135, -0.06916753249882547, -0.0034745196699277384, -0.025229084988605682, -0.15000818071856195, 0.0368530184982324, 0.4055927413628324, -0.24062426674312778, -0.25868355618421357, 0.07911469340119716, -0.265876917247814, -0.08335638372883185, 0.2220800326878696, -0.041454360231879... |
708.3471 | Structure of the Roper Resonance with Diquark Correlations | We study electromagnetic properties of the nucleon and Roper resonance in a
chiral quark-diquark model including two kinds of diquarks needed to describe
the nucleon: scalar and axial-vector diquarks. The nucleon and Roper resonance
are described as superpositions of two quark-diquark bound states of a quark
and a sc... | hep-ph | we study electromagnetic properties of the nucleon and roper resonance in a chiral quarkdiquark model including two kinds of diquarks needed to describe the nucleon scalar and axialvector diquarks the nucleon and roper resonance are described as superpositions of two quarkdiquark bound states of a quark and a scalar di... | [['we', 'study', 'electromagnetic', 'properties', 'of', 'the', 'nucleon', 'and', 'roper', 'resonance', 'in', 'a', 'chiral', 'quarkdiquark', 'model', 'including', 'two', 'kinds', 'of', 'diquarks', 'needed', 'to', 'describe', 'the', 'nucleon', 'scalar', 'and', 'axialvector', 'diquarks', 'the', 'nucleon', 'and', 'roper', ... | [-0.09440743855041701, 0.2923276584870331, -0.04466081186050049, 0.1681859197106394, -0.0717201921350618, -0.04589512487184881, 0.038195936573263284, 0.33064999258168404, -0.09862833818784211, -0.23979458995390593, -0.0810745751567571, -0.326924161888977, -0.04351821285672486, 0.05051719782186854, 0.16528220501978222, ... |
708.3472 | Empirical distributions of Chinese stock returns at different
microscopic timescales | We study the distributions of event-time returns and clock-time returns at
different microscopic timescales using ultra-high-frequency data extracted from
the limit-order books of 23 stocks traded in the Chinese stock market in 2003.
We find that the returns at the one-trade timescale obey the inverse cubic law.
For ... | q-fin.ST physics.soc-ph | we study the distributions of eventtime returns and clocktime returns at different microscopic timescales using ultrahighfrequency data extracted from the limitorder books of 23 stocks traded in the chinese stock market in 2003 we find that the returns at the onetrade timescale obey the inverse cubic law for larger tim... | [['we', 'study', 'the', 'distributions', 'of', 'eventtime', 'returns', 'and', 'clocktime', 'returns', 'at', 'different', 'microscopic', 'timescales', 'using', 'ultrahighfrequency', 'data', 'extracted', 'from', 'the', 'limitorder', 'books', 'of', '23', 'stocks', 'traded', 'in', 'the', 'chinese', 'stock', 'market', 'in',... | [-0.03367490037285452, 0.16451600936677638, -0.17298897948776243, 0.15824001220709208, -0.02683754610428233, -0.10127780104904802, 0.08224971064725961, 0.37897003123748907, -0.252998370784438, -0.30825137658504465, 0.07940004180963564, -0.3901975327466108, -0.050802324839596506, 0.19187431004417094, -0.0224470831335911... |
708.3473 | Geodesic plasma flows instabilities of Riemann twisted solar loops | Riemann and sectional curvatures of magnetic twisted flux tubes in Riemannian
manifold are computed to investigate the stability of the plasma astrophysical
tubes. The geodesic equations are used to show that in the case of thick
magnetic tubes, the curvature of planar (Frenet torsion-free) tubes have the
effect ct o... | physics.plasm-ph physics.flu-dyn | riemann and sectional curvatures of magnetic twisted flux tubes in riemannian manifold are computed to investigate the stability of the plasma astrophysical tubes the geodesic equations are used to show that in the case of thick magnetic tubes the curvature of planar frenet torsionfree tubes have the effect ct of dampi... | [['riemann', 'and', 'sectional', 'curvatures', 'of', 'magnetic', 'twisted', 'flux', 'tubes', 'in', 'riemannian', 'manifold', 'are', 'computed', 'to', 'investigate', 'the', 'stability', 'of', 'the', 'plasma', 'astrophysical', 'tubes', 'the', 'geodesic', 'equations', 'are', 'used', 'to', 'show', 'that', 'in', 'the', 'cas... | [-0.23696417245277668, 0.20392295522953505, -0.03319649540366574, 0.08401393344269431, -0.07568456049404997, -0.08494602176803034, -0.11552799293022166, 0.39389111137007204, -0.23645623072373093, -0.24812588818870776, 0.1056289744398208, -0.25134539514046433, -0.07409185061866012, 0.21389630085700218, -0.05101670331988... |
708.3474 | Nonlinear control of chaotic walking of atoms in an optical lattice | Centre-of-mass atomic motion in an optical lattice near the resonance is
shown to be a chaotic walking due to the interplay between coherent internal
atomic dynamics and spontaneous emission. Statistical properties of chaotic
atomic motion can be controlled by the single parameter, the detuning between
the atomic tra... | quant-ph | centreofmass atomic motion in an optical lattice near the resonance is shown to be a chaotic walking due to the interplay between coherent internal atomic dynamics and spontaneous emission statistical properties of chaotic atomic motion can be controlled by the single parameter the detuning between the atomic transitio... | [['centreofmass', 'atomic', 'motion', 'in', 'an', 'optical', 'lattice', 'near', 'the', 'resonance', 'is', 'shown', 'to', 'be', 'a', 'chaotic', 'walking', 'due', 'to', 'the', 'interplay', 'between', 'coherent', 'internal', 'atomic', 'dynamics', 'and', 'spontaneous', 'emission', 'statistical', 'properties', 'of', 'chaoti... | [-0.1181122288093675, 0.2597453859821033, -0.07173950693047629, 0.047580906980750494, -0.03655266547121289, -0.1111267287306851, 0.04987039969007417, 0.4176654609419951, -0.36598282995372555, -0.2865123867125409, -0.00679829748199753, -0.22816392369341196, -0.0905703525229289, 0.19100073612828897, 0.028060458288187297,... |
708.3475 | Optical sum rule anomalies in the cuprates: interplay between strong
correlation and electronic bandstructures | We theoretically analyze some of the anomalies of the optical sumrules in the
high-temperature superconductors. In particular we address the particularly
strong dependence on temperature of the sumrule in the normal state. Both
electron-electron correlations and the presence of a Van-Hove singularity have
been shown ... | cond-mat.str-el | we theoretically analyze some of the anomalies of the optical sumrules in the hightemperature superconductors in particular we address the particularly strong dependence on temperature of the sumrule in the normal state both electronelectron correlations and the presence of a vanhove singularity have been shown to enha... | [['we', 'theoretically', 'analyze', 'some', 'of', 'the', 'anomalies', 'of', 'the', 'optical', 'sumrules', 'in', 'the', 'hightemperature', 'superconductors', 'in', 'particular', 'we', 'address', 'the', 'particularly', 'strong', 'dependence', 'on', 'temperature', 'of', 'the', 'sumrule', 'in', 'the', 'normal', 'state', 'b... | [-0.13748922894970747, 0.14625450659543276, -0.0714644039911218, 0.12459360707551241, -0.029571817219257356, -0.13331906484556386, 0.051114760622149334, 0.3623511189222336, -0.2550854610092938, -0.24804081005044282, 0.06175104951951653, -0.31494267609436066, -0.16331727212294936, 0.1696289457171224, 0.03511384227051167... |
708.3476 | Mean Field Theory for Pedestrian Outflow through an Exit | An average pedestrian flow through an exit is one of the most important index
in evaluating pedestrian dynamics. In order to study the flow in detail, the
floor field model, which is a crowd model by using cellular automaton, is
extended by taking into account a realistic behavior of pedestrians around the
exit. The ... | cond-mat.stat-mech physics.soc-ph | an average pedestrian flow through an exit is one of the most important index in evaluating pedestrian dynamics in order to study the flow in detail the floor field model which is a crowd model by using cellular automaton is extended by taking into account a realistic behavior of pedestrians around the exit the model i... | [['an', 'average', 'pedestrian', 'flow', 'through', 'an', 'exit', 'is', 'one', 'of', 'the', 'most', 'important', 'index', 'in', 'evaluating', 'pedestrian', 'dynamics', 'in', 'order', 'to', 'study', 'the', 'flow', 'in', 'detail', 'the', 'floor', 'field', 'model', 'which', 'is', 'a', 'crowd', 'model', 'by', 'using', 'cel... | [-0.10733512262916467, 0.12416891486346311, -0.14453480931139795, 0.0611163778955698, -0.031188392772988863, -0.12258112495530303, 0.0321771593396591, 0.3829334553383964, -0.23758380967016263, -0.2816753471348466, 0.0978548578505146, -0.25704096023192896, -0.15061495389139765, 0.17960613148146065, -0.044576206189744616... |
708.3477 | The Church Synthesis Problem with Parameters | For a two-variable formula ψ(X,Y) of Monadic Logic of Order (MLO) the
Church Synthesis Problem concerns the existence and construction of an operator
Y=F(X) such that ψ(X,F(X)) is universally valid over Nat.
B\"{u}chi and Landweber proved that the Church synthesis problem is
decidable; moreover, they showed... | cs.LO | for a twovariable formula psixy of monadic logic of order mlo the church synthesis problem concerns the existence and construction of an operator yfx such that psixfx is universally valid over nat buchi and landweber proved that the church synthesis problem is decidable moreover they showed that if there is an operator... | [['for', 'a', 'twovariable', 'formula', 'psixy', 'of', 'monadic', 'logic', 'of', 'order', 'mlo', 'the', 'church', 'synthesis', 'problem', 'concerns', 'the', 'existence', 'and', 'construction', 'of', 'an', 'operator', 'yfx', 'such', 'that', 'psixfx', 'is', 'universally', 'valid', 'over', 'nat', 'buchi', 'and', 'landwebe... | [-0.11042912668831138, 0.09116577158573291, -0.09629942470622298, 0.11606257829177928, -0.10820881769330681, -0.16885291158139712, 0.04652814016031028, 0.3043839884186654, -0.3880637097172439, -0.24062676418352089, 0.12407914742959149, -0.2057274216449035, -0.12813889380700666, 0.22293778052277813, -0.14610290463315323... |
708.3478 | Feedback from Multiple Supernova Explosions inside a Wind-Blown Bubble | We study the evolution of multiple supernova (SN) explosions inside a
pre-exiting cavity blown by winds from massive progenitor stars. Hydrodynamic
simulations in one-dimensional spherical geometry, including radiative cooling
and thermal conduction, are carried out to follow first the development of the
wind-blown b... | astro-ph | we study the evolution of multiple supernova sn explosions inside a preexiting cavity blown by winds from massive progenitor stars hydrodynamic simulations in onedimensional spherical geometry including radiative cooling and thermal conduction are carried out to follow first the development of the windblown bubble duri... | [['we', 'study', 'the', 'evolution', 'of', 'multiple', 'supernova', 'sn', 'explosions', 'inside', 'a', 'preexiting', 'cavity', 'blown', 'by', 'winds', 'from', 'massive', 'progenitor', 'stars', 'hydrodynamic', 'simulations', 'in', 'onedimensional', 'spherical', 'geometry', 'including', 'radiative', 'cooling', 'and', 'th... | [-0.04310850572929827, 0.17373760353038656, -0.015694861014631866, 0.0991931192681072, -0.04496779988183319, -0.017312744595188678, 0.041418014119179655, 0.39152681240185844, -0.18337668729515574, -0.33929029109930825, 0.06705579500128868, -0.30014940512468335, 0.049540416963648894, 0.1875882853118961, 0.02289425286619... |
708.3479 | Possible nodeless superconductivity in the noncentrosymmetric
superconductor Mg_(12-delta)Ir_19B_16 | We measured the resistivity, diamagnetization, and low-temperature specific
heat of the newly discovered noncentrosymmetric superconductor
Mg_(12-delta)Ir_19B_16. The temperature dependence of specific heat is
consistent with the model of an isotropic s-wave gap with value Delta_0 = 0.94
meV for the sample Tc = 5.7 K... | cond-mat.supr-con | we measured the resistivity diamagnetization and lowtemperature specific heat of the newly discovered noncentrosymmetric superconductor mg_12deltair_19b_16 the temperature dependence of specific heat is consistent with the model of an isotropic swave gap with value delta_0 094 mev for the sample tc 57 k and the ratio d... | [['we', 'measured', 'the', 'resistivity', 'diamagnetization', 'and', 'lowtemperature', 'specific', 'heat', 'of', 'the', 'newly', 'discovered', 'noncentrosymmetric', 'superconductor', 'mg_12deltair_19b_16', 'the', 'temperature', 'dependence', 'of', 'specific', 'heat', 'is', 'consistent', 'with', 'the', 'model', 'of', 'a... | [-0.18612069642352583, 0.22141187254517686, -0.0072985195165368175, 0.025439868419455874, -0.06701865566372088, -0.16716096785117304, 0.16218655780617114, 0.3242067418728782, -0.22598625108006254, -0.30999001066109777, -0.04150022201207096, -0.37905099598971087, -0.037303074324849694, 0.19273660500715198, 0.08710183421... |
708.348 | On the Theory of Surfaces in the Four-dimensional Euclidean Space | For a two-dimensional surface in the four-dimensional Euclidean space we
introduce an invariant linear map of Weingarten type in the tangent space of
the surface, which generates two invariants k and kappa.
The condition k = kappa = 0 characterizes the surfaces consisting of flat
points. The minimal surfaces are ch... | math.DG | for a twodimensional surface in the fourdimensional euclidean space we introduce an invariant linear map of weingarten type in the tangent space of the surface which generates two invariants k and kappa the condition k kappa 0 characterizes the surfaces consisting of flat points the minimal surfaces are characterized b... | [['for', 'a', 'twodimensional', 'surface', 'in', 'the', 'fourdimensional', 'euclidean', 'space', 'we', 'introduce', 'an', 'invariant', 'linear', 'map', 'of', 'weingarten', 'type', 'in', 'the', 'tangent', 'space', 'of', 'the', 'surface', 'which', 'generates', 'two', 'invariants', 'k', 'and', 'kappa', 'the', 'condition',... | [-0.19047361193619416, 0.14587726395577685, -0.06543975337694588, 0.03795970158781698, -0.06603042803452176, -0.1733272406351516, 0.003473061491080197, 0.3382270838789074, -0.28654744359072676, -0.23954229676894748, 0.06675875151206313, -0.2345588350337062, -0.15440857801902091, 0.18101485964044992, -0.0785046141781850... |
708.3481 | Formation of Multipartite Entanglement Using Random Quantum Gates | The formation of multipartite quantum entanglement by repeated operation of
one and two qubit gates is examined. The resulting entanglement is evaluated
using two measures: the average bipartite entanglement and the Groverian
measure. A comparison is made between two geometries of the quantum register: a
one dimensio... | quant-ph | the formation of multipartite quantum entanglement by repeated operation of one and two qubit gates is examined the resulting entanglement is evaluated using two measures the average bipartite entanglement and the groverian measure a comparison is made between two geometries of the quantum register a one dimensional ch... | [['the', 'formation', 'of', 'multipartite', 'quantum', 'entanglement', 'by', 'repeated', 'operation', 'of', 'one', 'and', 'two', 'qubit', 'gates', 'is', 'examined', 'the', 'resulting', 'entanglement', 'is', 'evaluated', 'using', 'two', 'measures', 'the', 'average', 'bipartite', 'entanglement', 'and', 'the', 'groverian'... | [-0.15356601806957312, 0.17421037287124438, -0.04417700196704241, 0.050749775650602645, 0.050057338011013155, -0.25742984740125224, 0.051558202010770604, 0.4065162723032844, -0.20913737675557467, -0.2625539185978867, 0.059021357878647894, -0.289905638964415, -0.11311272532364589, 0.22557564748340095, -0.015565997156135... |
708.3482 | Designing a Spin Channel for Perfect Quantum Communication | We propose a scheme for using a spin chain with fixed symmetry interaction as
a channel for perfect quantum communication. The perfect quantum communication
is determined by the eigenvalues that form a special arithmetical progression,
the concrete interaction parameter $J_i$ is obtained as a function of integer
and ... | quant-ph | we propose a scheme for using a spin chain with fixed symmetry interaction as a channel for perfect quantum communication the perfect quantum communication is determined by the eigenvalues that form a special arithmetical progression the concrete interaction parameter j_i is obtained as a function of integer and perfec... | [['we', 'propose', 'a', 'scheme', 'for', 'using', 'a', 'spin', 'chain', 'with', 'fixed', 'symmetry', 'interaction', 'as', 'a', 'channel', 'for', 'perfect', 'quantum', 'communication', 'the', 'perfect', 'quantum', 'communication', 'is', 'determined', 'by', 'the', 'eigenvalues', 'that', 'form', 'a', 'special', 'arithmeti... | [-0.24354963173259006, 0.18208202766254544, -0.0674166995397007, 0.022766573668129488, -0.05616287589972754, -0.2523119679747403, 0.06002324699180794, 0.38617598405107856, -0.27517809018238704, -0.2526507412337444, 0.08452645493327343, -0.256748264049582, -0.11106227432504635, 0.16844200891103933, 0.009247285282154653,... |
708.3483 | An Ideal Channel of Long Distance Entanglement in Spin Systems | We propose a scheme for using spin chain to realize an ideal channel of long
distance entanglement. The results show that there has different entanglement
in different Hilbert subspace, the anisotropic parameter $\Delta$ will
frustrate the entanglement and the magnetic field affect the entanglement
through changing t... | quant-ph | we propose a scheme for using spin chain to realize an ideal channel of long distance entanglement the results show that there has different entanglement in different hilbert subspace the anisotropic parameter delta will frustrate the entanglement and the magnetic field affect the entanglement through changing the grou... | [['we', 'propose', 'a', 'scheme', 'for', 'using', 'spin', 'chain', 'to', 'realize', 'an', 'ideal', 'channel', 'of', 'long', 'distance', 'entanglement', 'the', 'results', 'show', 'that', 'there', 'has', 'different', 'entanglement', 'in', 'different', 'hilbert', 'subspace', 'the', 'anisotropic', 'parameter', 'delta', 'wi... | [-0.1567395680830774, 0.1916091654452935, -0.037801589673528306, 0.05741916506642746, -0.049464991471170984, -0.21270049094325966, 0.006461476630523291, 0.37595155293870175, -0.29239366802140176, -0.21917597296982047, 0.11421645675820913, -0.22569678497747478, -0.0812415479360005, 0.15789475633054334, -0.01661525543333... |
708.3484 | (p,q)-string in matrix-regularized membrane and type IIB duality | We consider a lightcone wrapped supermembrane compactified on 2-torus in the
matrix regularization. We examine the double dimensional reduction technique
and deduce the free matrix string of (p,q)-string in type IIB superstring
theory explicitly from the matrix-regularized wrapped supermembrane. In
addition we obtain... | hep-th | we consider a lightcone wrapped supermembrane compactified on 2torus in the matrix regularization we examine the double dimensional reduction technique and deduce the free matrix string of pqstring in type iib superstring theory explicitly from the matrixregularized wrapped supermembrane in addition we obtain the 21dim... | [['we', 'consider', 'a', 'lightcone', 'wrapped', 'supermembrane', 'compactified', 'on', '2torus', 'in', 'the', 'matrix', 'regularization', 'we', 'examine', 'the', 'double', 'dimensional', 'reduction', 'technique', 'and', 'deduce', 'the', 'free', 'matrix', 'string', 'of', 'pqstring', 'in', 'type', 'iib', 'superstring', ... | [-0.10440737892111594, 0.1210850442675027, -0.06846680499782616, 0.15916169637983496, -0.05654267589138313, -0.14365699422461065, -0.016333651366982272, 0.32938430332578716, -0.18785786693069068, -0.151951136846434, 0.10685580130243166, -0.2517322906377641, -0.2328172492371364, 0.04032464568418535, -0.1768088093704798,... |
708.3485 | Unparticle decay of neutrinos and it's effect on ultra high energy
neutrinos | The unparticle is proposed by Georgi as a conceptual new physics beyond the
standard model to describe the low energy sector of a nontrivial scale
invariant sector of an effective theory. We consider the neutrino decay in
unparticle scenario and investigate the effect of such decay for the case of
ultra high energy n... | hep-ph | the unparticle is proposed by georgi as a conceptual new physics beyond the standard model to describe the low energy sector of a nontrivial scale invariant sector of an effective theory we consider the neutrino decay in unparticle scenario and investigate the effect of such decay for the case of ultra high energy neut... | [['the', 'unparticle', 'is', 'proposed', 'by', 'georgi', 'as', 'a', 'conceptual', 'new', 'physics', 'beyond', 'the', 'standard', 'model', 'to', 'describe', 'the', 'low', 'energy', 'sector', 'of', 'a', 'nontrivial', 'scale', 'invariant', 'sector', 'of', 'an', 'effective', 'theory', 'we', 'consider', 'the', 'neutrino', '... | [-0.08422751991996823, 0.23063134624840442, -0.05655882864782255, 0.21840050980633713, -0.06547213648445904, -0.11308155916886378, 0.00498453578720354, 0.2707660705718684, -0.2425975973258586, -0.33234964742338, 0.0508217943484627, -0.2884641187137937, -0.08227024019427903, 0.17586703174938895, 0.06698669137254562, 0.0... |
708.3486 | On topological spaces possessing uniformly distributed sequences | Two classes of topological spaces are introduced on which every probability
Radon measure possesses a uniformly distributed sequence or a uniformly tight
uniformly distributed sequence. It is shown that these classes are stable under
multiplication by completely regular Souslin spaces
| math.GN math.PR | two classes of topological spaces are introduced on which every probability radon measure possesses a uniformly distributed sequence or a uniformly tight uniformly distributed sequence it is shown that these classes are stable under multiplication by completely regular souslin spaces | [['two', 'classes', 'of', 'topological', 'spaces', 'are', 'introduced', 'on', 'which', 'every', 'probability', 'radon', 'measure', 'possesses', 'a', 'uniformly', 'distributed', 'sequence', 'or', 'a', 'uniformly', 'tight', 'uniformly', 'distributed', 'sequence', 'it', 'is', 'shown', 'that', 'these', 'classes', 'are', 's... | [-0.1757543018058641, 0.25806225361302493, -0.08019698411226273, 0.07749544928374234, 0.026940552541054784, -0.17440423676744105, -0.004498017148580402, 0.47351925568655134, -0.38122891446109863, -0.15020303598139434, 0.14545334258582443, -0.24871796708866895, -0.1338336547894869, 0.21156455280142836, -0.15680549414828... |
708.3487 | Threadbare Parallel Port DAQ Card | A very simple Data acquisition card was developed in our under-graduate class
for interfacing with the parallel port of a standard computer. It was developed
with the intention to enable students to do various physics experiments with
the computer sparing them from knowing the details of the electronics required.
The... | physics.ed-ph | a very simple data acquisition card was developed in our undergraduate class for interfacing with the parallel port of a standard computer it was developed with the intention to enable students to do various physics experiments with the computer sparing them from knowing the details of the electronics required the arti... | [['a', 'very', 'simple', 'data', 'acquisition', 'card', 'was', 'developed', 'in', 'our', 'undergraduate', 'class', 'for', 'interfacing', 'with', 'the', 'parallel', 'port', 'of', 'a', 'standard', 'computer', 'it', 'was', 'developed', 'with', 'the', 'intention', 'to', 'enable', 'students', 'to', 'do', 'various', 'physics... | [-0.026645313534471724, 0.054376946581113667, -0.09627064886929777, 0.011856890058778744, -0.1820410511766871, -0.1875115866577188, 0.06751016361199112, 0.37729635027547676, -0.21216254871493825, -0.41259440495115185, 0.10296293229718383, -0.2774067437276244, -0.10955886366880602, 0.243413209554597, -0.1111275669859929... |
708.3488 | Magnetometry Based on Nonlinear Magneto-Optical Rotation with
Amplitude-Modulated Light | We report on an all-optical magnetometric technique based on nonlinear
magneto-optical rotation with amplitude-modulated light. The method enables
sensitive magnetic-field measurements in a broad dynamic range. We demonstrate
the sensitivity of $4.3\times10^{-9}$ G/$\sqrt{\text{Hz}}$ at 10 mG and the
magnetic field t... | physics.atom-ph physics.optics | we report on an alloptical magnetometric technique based on nonlinear magnetooptical rotation with amplitudemodulated light the method enables sensitive magneticfield measurements in a broad dynamic range we demonstrate the sensitivity of 43times109 gsqrttexthz at 10 mg and the magnetic field tracking in a range of 40 ... | [['we', 'report', 'on', 'an', 'alloptical', 'magnetometric', 'technique', 'based', 'on', 'nonlinear', 'magnetooptical', 'rotation', 'with', 'amplitudemodulated', 'light', 'the', 'method', 'enables', 'sensitive', 'magneticfield', 'measurements', 'in', 'a', 'broad', 'dynamic', 'range', 'we', 'demonstrate', 'the', 'sensit... | [-0.10727935751539565, 0.11147295764197723, 0.026450794513127016, -0.037436571869728784, -0.04153827664202019, -0.0768249613146538, 0.06700352446791986, 0.45130260841500375, -0.20897820213389012, -0.37760205792203066, 0.07551810128479114, -0.22531138446121926, -0.10245399153040301, 0.32218457409931767, -0.0083887529589... |
708.3489 | Extrema of low eigenvalues of the Dirichlet-Neumann Laplacian on a disk | We study extrema of the first and the second mixed eigenvalues of the
Laplacian on the disk among some families of Dirichlet-Neumann boundary
conditions. We show that the minimizer of the second eigenvalue among all mixed
boundary conditions lies in a compact 1-parameter family for which an explicit
description is gi... | math.SP | we study extrema of the first and the second mixed eigenvalues of the laplacian on the disk among some families of dirichletneumann boundary conditions we show that the minimizer of the second eigenvalue among all mixed boundary conditions lies in a compact 1parameter family for which an explicit description is given m... | [['we', 'study', 'extrema', 'of', 'the', 'first', 'and', 'the', 'second', 'mixed', 'eigenvalues', 'of', 'the', 'laplacian', 'on', 'the', 'disk', 'among', 'some', 'families', 'of', 'dirichletneumann', 'boundary', 'conditions', 'we', 'show', 'that', 'the', 'minimizer', 'of', 'the', 'second', 'eigenvalue', 'among', 'all',... | [-0.18133224174380302, 0.09090432949682616, -0.05539778375669437, -0.0033966532607069785, -0.08460661990513259, -0.07990576903719236, -0.0234903690569541, 0.320006226657835, -0.27967283550978583, -0.23409667788621258, 0.15906349704189993, -0.2761041071539854, -0.13147778217406833, 0.14604571665472843, -0.06713848211528... |
708.349 | Two-Dimensional Spectroscopy of Photospheric Shear Flows in a Small
delta Spot | In recent high-resolution observations of complex active regions,
long-lasting and well-defined regions of strong flows were identified in major
flares and associated with bright kernels of visible, near-infrared, and X-ray
radiation. These flows, which occurred in the proximity of the magnetic neutral
line, signific... | astro-ph | in recent highresolution observations of complex active regions longlasting and welldefined regions of strong flows were identified in major flares and associated with bright kernels of visible nearinfrared and xray radiation these flows which occurred in the proximity of the magnetic neutral line significantly contrib... | [['in', 'recent', 'highresolution', 'observations', 'of', 'complex', 'active', 'regions', 'longlasting', 'and', 'welldefined', 'regions', 'of', 'strong', 'flows', 'were', 'identified', 'in', 'major', 'flares', 'and', 'associated', 'with', 'bright', 'kernels', 'of', 'visible', 'nearinfrared', 'and', 'xray', 'radiation',... | [-0.14844201638022372, 0.18114597691302542, -0.027779347163492014, 0.06465340654332456, -0.09971684258302307, -0.06774984946969198, -0.019409827878137418, 0.4414845887014443, -0.2081512755082388, -0.33628486600355245, 0.09930007003796552, -0.27192041950287865, -0.10218443073972594, 0.21794672452129557, -0.0425696929857... |
708.3491 | Equation of State of Wet Granular Matter | A theory is derived for the nonequilibrium probability currents of the
capillary interaction which determines the pair correlation function near
contact. This yields an analytic expression for the equation of state, P =
P(N/V,T), of wet granular matter for D=2 dimensions, valid in the complete
density range from gas ... | cond-mat.soft | a theory is derived for the nonequilibrium probability currents of the capillary interaction which determines the pair correlation function near contact this yields an analytic expression for the equation of state p pnvt of wet granular matter for d2 dimensions valid in the complete density range from gas to jamming dr... | [['a', 'theory', 'is', 'derived', 'for', 'the', 'nonequilibrium', 'probability', 'currents', 'of', 'the', 'capillary', 'interaction', 'which', 'determines', 'the', 'pair', 'correlation', 'function', 'near', 'contact', 'this', 'yields', 'an', 'analytic', 'expression', 'for', 'the', 'equation', 'of', 'state', 'p', 'pnvt'... | [-0.13424596136248465, 0.23445800265713265, -0.09025853818173168, 0.011350530537027047, 0.009228601691699246, -0.12555188199209913, 0.06756335297747083, 0.3039368318938991, -0.20613230870633453, -0.268215777929418, -0.009448488581380466, -0.3016834812670401, -0.12505958608646944, 0.12711242024854916, 0.0161050729135551... |
708.3492 | The Variability of Polarized Radiation from Sgr A* | Sgr A* is variable at radio and submillimeter wavelengths on hourly time
scales showing time delays between the peaks of flare emission as well as
linearly polarized emission at millimeter and sub-mm wavelengths. To determine
the polarization characteristics of this variable source at radio frequencies,
we present VL... | astro-ph | sgr a is variable at radio and submillimeter wavelengths on hourly time scales showing time delays between the peaks of flare emission as well as linearly polarized emission at millimeter and submm wavelengths to determine the polarization characteristics of this variable source at radio frequencies we present vla obse... | [['sgr', 'a', 'is', 'variable', 'at', 'radio', 'and', 'submillimeter', 'wavelengths', 'on', 'hourly', 'time', 'scales', 'showing', 'time', 'delays', 'between', 'the', 'peaks', 'of', 'flare', 'emission', 'as', 'well', 'as', 'linearly', 'polarized', 'emission', 'at', 'millimeter', 'and', 'submm', 'wavelengths', 'to', 'de... | [-0.13153356971452013, 0.1866409816975647, -0.0259821719203804, 0.022622406038256788, -0.022986890233975526, -0.08071135388066371, 0.0673886890290305, 0.46483539137019153, -0.20326646562170936, -0.3483143128444984, 0.10097127788564346, -0.2959787674287024, -0.015506575899053132, 0.18848483688028259, 0.03305516203060203... |
708.3493 | Best network chirplet-chain: Near-optimal coherent detection of
unmodeled gravitation wave chirps with a network of detectors | The searches of impulsive gravitational waves (GW) in the data of the
ground-based interferometers focus essentially on two types of waveforms: short
unmodeled bursts and chirps from inspiralling compact binaries. There is room
for other types of searches based on different models. Our objective is to fill
this gap. ... | gr-qc | the searches of impulsive gravitational waves gw in the data of the groundbased interferometers focus essentially on two types of waveforms short unmodeled bursts and chirps from inspiralling compact binaries there is room for other types of searches based on different models our objective is to fill this gap more spec... | [['the', 'searches', 'of', 'impulsive', 'gravitational', 'waves', 'gw', 'in', 'the', 'data', 'of', 'the', 'groundbased', 'interferometers', 'focus', 'essentially', 'on', 'two', 'types', 'of', 'waveforms', 'short', 'unmodeled', 'bursts', 'and', 'chirps', 'from', 'inspiralling', 'compact', 'binaries', 'there', 'is', 'roo... | [-0.14726977614518105, 0.11158738211972068, -0.06354737338734422, 0.08088961331860016, -0.0981633685423657, -0.0969575254636843, 0.027597787601237943, 0.3913539327975166, -0.24943253571197752, -0.30119359138636637, 0.11360205329911263, -0.296316739105759, -0.12873326061455617, 0.2449365105180198, -0.01622625271250543, ... |
708.3494 | Fidelity Between Partial States as Signature of Quantum Phase
Transitions | We introduce a partial state fidelity approach to quantum phase transitions.
We consider a superconducting lattice with a magnetic impurity inserted at its
centre, and look at the fidelity between partial (either one-site or two-site)
quantum states. In the vicinity of the point of the quantum phase transition,
we ob... | quant-ph cond-mat.str-el | we introduce a partial state fidelity approach to quantum phase transitions we consider a superconducting lattice with a magnetic impurity inserted at its centre and look at the fidelity between partial either onesite or twosite quantum states in the vicinity of the point of the quantum phase transition we observe a su... | [['we', 'introduce', 'a', 'partial', 'state', 'fidelity', 'approach', 'to', 'quantum', 'phase', 'transitions', 'we', 'consider', 'a', 'superconducting', 'lattice', 'with', 'a', 'magnetic', 'impurity', 'inserted', 'at', 'its', 'centre', 'and', 'look', 'at', 'the', 'fidelity', 'between', 'partial', 'either', 'onesite', '... | [-0.14382657379211253, 0.1657642865471338, -0.0411072470148844, 0.04469310384103616, 0.04243065370864903, -0.12919872439779606, 0.12637805272783853, 0.3384427339728691, -0.26894621417519793, -0.25569737037701484, 0.07793415389209161, -0.33964854253629073, -0.11168900747120018, 0.10836686647293133, 0.023445846482006982,... |
708.3495 | Study of the young stellar population of NGC 4214 using the Hubble Space
Telescope | We present an original study of the dwarf starburst galaxy NGC 4214. We use
archival optical and UV images obtained with WFPC2 and STIS on-board the Hubble
Space Telescope. We explain the process followed to obtain high-quality
photometry and astrometry of the stellar and cluster populations of this
galaxy. We descri... | astro-ph | we present an original study of the dwarf starburst galaxy ngc 4214 we use archival optical and uv images obtained with wfpc2 and stis onboard the hubble space telescope we explain the process followed to obtain highquality photometry and astrometry of the stellar and cluster populations of this galaxy we describe the ... | [['we', 'present', 'an', 'original', 'study', 'of', 'the', 'dwarf', 'starburst', 'galaxy', 'ngc', '4214', 'we', 'use', 'archival', 'optical', 'and', 'uv', 'images', 'obtained', 'with', 'wfpc2', 'and', 'stis', 'onboard', 'the', 'hubble', 'space', 'telescope', 'we', 'explain', 'the', 'process', 'followed', 'to', 'obtain'... | [-0.03384263320382701, 0.06033086230604468, -0.12341637879113898, 0.1268653034674722, -0.09422075652464508, -0.03616596273996554, 0.0506646007240453, 0.5002855211008324, -0.14717996490948454, -0.35252007033968724, 0.041280922114413934, -0.25227879453348767, -0.0709016588760548, 0.18888767608177062, -0.09527475446031539... |
708.3496 | Threshold effect and \pi^\pm \psi(2S) peak | A resonance-like structure in the $\pi^\pm \psi(2S)$ mass spectrum arising in
$B \to K \pi^\pm \psi(2S)$ has recently been reported. It is noted that the
mass of this structure, $4433 \pm 4 \pm 1$ MeV, is not far from the threshold
for production of $D^* \bar{D}_1(2420)$. A proposed mechanism for production of
this s... | hep-ph | a resonancelike structure in the pipm psi2s mass spectrum arising in b to k pipm psi2s has recently been reported it is noted that the mass of this structure 4433 pm 4 pm 1 mev is not far from the threshold for production of d bard_12420 a proposed mechanism for production of this state is suggested and tests are sugge... | [['a', 'resonancelike', 'structure', 'in', 'the', 'pipm', 'psi2s', 'mass', 'spectrum', 'arising', 'in', 'b', 'to', 'k', 'pipm', 'psi2s', 'has', 'recently', 'been', 'reported', 'it', 'is', 'noted', 'that', 'the', 'mass', 'of', 'this', 'structure', '4433', 'pm', '4', 'pm', '1', 'mev', 'is', 'not', 'far', 'from', 'the', '... | [-0.10023213404435981, 0.18759923104701912, -0.1189690570710069, 0.06168371094272362, -0.017423875652099723, -0.10279583834679955, 0.02121843915369551, 0.30866488700701017, -0.19679215556342092, -0.3049018114678941, -0.019258000228901284, -0.33813853685002204, -0.02344643267787109, 0.16613538468935354, 0.03884533767477... |
708.3497 | A Mechanism for Kaluza-Klein Number Violation in UED and Implications
for LHC | If the Higgs does not propagate into an otherwise universal extra dimension,
then tree-level Kaluza-Klein number is not conserved in the Yukawa
interactions. This leads to mixing between zero-mode fermions and their
associated Kaluza-Klein excitations. The effect can be quite large for the top
quark, since its mass (... | hep-ph | if the higgs does not propagate into an otherwise universal extra dimension then treelevel kaluzaklein number is not conserved in the yukawa interactions this leads to mixing between zeromode fermions and their associated kaluzaklein excitations the effect can be quite large for the top quark since its mass 1714 plus o... | [['if', 'the', 'higgs', 'does', 'not', 'propagate', 'into', 'an', 'otherwise', 'universal', 'extra', 'dimension', 'then', 'treelevel', 'kaluzaklein', 'number', 'is', 'not', 'conserved', 'in', 'the', 'yukawa', 'interactions', 'this', 'leads', 'to', 'mixing', 'between', 'zeromode', 'fermions', 'and', 'their', 'associated... | [-0.10405719751973547, 0.28801003032413874, -0.039504174064568104, 0.13377531313501445, -0.07559897326497655, -0.16226612600610588, 0.031627462957273124, 0.2523776624298711, -0.21804471790551927, -0.27928273030639594, 0.009709167190010451, -0.3043803852590591, -0.020155273420567162, 0.0905883263198334, 0.04627332564201... |
708.3498 | Voltage Controlled Resistance | The paper discusses an application of the field effected transistor (FET) as
a voltage controlled resistance which can be done in under-graduate labs either
as a routine experiment or as a project.
| physics.ed-ph | the paper discusses an application of the field effected transistor fet as a voltage controlled resistance which can be done in undergraduate labs either as a routine experiment or as a project | [['the', 'paper', 'discusses', 'an', 'application', 'of', 'the', 'field', 'effected', 'transistor', 'fet', 'as', 'a', 'voltage', 'controlled', 'resistance', 'which', 'can', 'be', 'done', 'in', 'undergraduate', 'labs', 'either', 'as', 'a', 'routine', 'experiment', 'or', 'as', 'a', 'project']] | [-0.11536144139245152, 0.10634808677832552, -0.08311184163903818, -0.025640656018367736, -0.0456694855238311, -0.21165525093965698, 0.0722106074426847, 0.37672641000244766, -0.2379595210077241, -0.3542202108656056, 0.11427491415452096, -0.19280093838460743, -0.1658831159093097, 0.31449058697762666, -0.08452221017796546... |
708.3499 | Comparison of Tree-Child Phylogenetic Networks | Phylogenetic networks are a generalization of phylogenetic trees that allow
for the representation of non-treelike evolutionary events, like recombination,
hybridization, or lateral gene transfer. In this paper, we present and study a
new class of phylogenetic networks, called tree-child phylogenetic networks,
where ... | q-bio.PE cs.CE cs.DM | phylogenetic networks are a generalization of phylogenetic trees that allow for the representation of nontreelike evolutionary events like recombination hybridization or lateral gene transfer in this paper we present and study a new class of phylogenetic networks called treechild phylogenetic networks where every nonex... | [['phylogenetic', 'networks', 'are', 'a', 'generalization', 'of', 'phylogenetic', 'trees', 'that', 'allow', 'for', 'the', 'representation', 'of', 'nontreelike', 'evolutionary', 'events', 'like', 'recombination', 'hybridization', 'or', 'lateral', 'gene', 'transfer', 'in', 'this', 'paper', 'we', 'present', 'and', 'study'... | [-0.12412197976951925, 0.057361789038674484, -0.03487783784341425, 0.1151798519004652, -0.07390090317391701, -0.1419732270319683, 0.02340786042425908, 0.42627158199073906, -0.3168675158130752, -0.27393198667599233, 0.04085012373717049, -0.24784641773117663, -0.21940526282704187, 0.16609700168956512, -0.0528763298966032... |
708.35 | Monte Carlo simulation of the nuclear medium: Fermi gases, nuclei and
the role of Pauli potentials | The role of Pauli potentials in the semiclassical simulation of Fermi gases
at low temperatures is investigated. An alternative Pauli potential to the
usual bivariate Gaussian form by Dorso et al. is proposed. This new Pauli
potential allows for a simultaneous good reproduction of not only the kinetic
energy per part... | nucl-th | the role of pauli potentials in the semiclassical simulation of fermi gases at low temperatures is investigated an alternative pauli potential to the usual bivariate gaussian form by dorso et al is proposed this new pauli potential allows for a simultaneous good reproduction of not only the kinetic energy per particle ... | [['the', 'role', 'of', 'pauli', 'potentials', 'in', 'the', 'semiclassical', 'simulation', 'of', 'fermi', 'gases', 'at', 'low', 'temperatures', 'is', 'investigated', 'an', 'alternative', 'pauli', 'potential', 'to', 'the', 'usual', 'bivariate', 'gaussian', 'form', 'by', 'dorso', 'et', 'al', 'is', 'proposed', 'this', 'new... | [-0.11133638803973722, 0.19425585641408705, -0.07816686275984766, 0.14351756622544626, -0.023548495499145925, -0.12176971034897328, 0.04727969710145471, 0.33356837846917436, -0.21741188400271302, -0.28064656713344516, -0.04420099397036202, -0.2799459685984314, -0.07307930715784466, 0.14950402140350633, 0.01953303314817... |
708.3501 | The Meaning Of The Fine Structure Constant | A possible explanation is offered for the longstanding mystery surrounding
the meaning of the fine structure constant. The reasoning is based on a
discrete self-similar cosmological paradigm that has shown promise in
explaining the general scaling properties of nature's global hierarchy. The
discrete scale invariance... | physics.gen-ph | a possible explanation is offered for the longstanding mystery surrounding the meaning of the fine structure constant the reasoning is based on a discrete selfsimilar cosmological paradigm that has shown promise in explaining the general scaling properties of natures global hierarchy the discrete scale invariance of th... | [['a', 'possible', 'explanation', 'is', 'offered', 'for', 'the', 'longstanding', 'mystery', 'surrounding', 'the', 'meaning', 'of', 'the', 'fine', 'structure', 'constant', 'the', 'reasoning', 'is', 'based', 'on', 'a', 'discrete', 'selfsimilar', 'cosmological', 'paradigm', 'that', 'has', 'shown', 'promise', 'in', 'explai... | [-0.18755607728332704, 0.1382784148409348, -0.057130263574042155, 0.1179429917949127, -0.11320200888920076, -0.1005373980019472, 0.000575709771172902, 0.32450036869681986, -0.31275888036974925, -0.3271919011916082, 0.034638909184969195, -0.191633183057852, -0.12265689212819274, 0.1464761558190449, 0.05647804368690578, ... |
708.3502 | Child mortality in Penna ageing model | Assuming the deleterious mutations in the Penna ageing model to affect mainly
the young ages, we get an enhanced mortality at very young age, followed by a
minimum of the mortality, and then the usual exponential increase of mortality
with age.
| q-bio.PE | assuming the deleterious mutations in the penna ageing model to affect mainly the young ages we get an enhanced mortality at very young age followed by a minimum of the mortality and then the usual exponential increase of mortality with age | [['assuming', 'the', 'deleterious', 'mutations', 'in', 'the', 'penna', 'ageing', 'model', 'to', 'affect', 'mainly', 'the', 'young', 'ages', 'we', 'get', 'an', 'enhanced', 'mortality', 'at', 'very', 'young', 'age', 'followed', 'by', 'a', 'minimum', 'of', 'the', 'mortality', 'and', 'then', 'the', 'usual', 'exponential', ... | [0.01119458271054233, 0.2325713692787359, -0.09125225824054058, 0.15990840995729697, -0.035273865864771166, -0.12111963553172422, 0.161291268756386, 0.3595979830829381, -0.2607123053791683, -0.2932211364414997, 0.10993834829991456, -0.22354578771969166, -0.09546484975371419, 0.1505593110000851, -0.21435191371001122, -0... |
708.3503 | On the theorem of M.Golomb | Let $X_{1},...,X_{n}$ be compact spaces and $X=X_{1}\times ... \times X_{n}.$
Consider the approximation of a function $f\in C(X)$ by sums $g_{1}(x_{1})+...
g_{n}(x_{n}),$ where $g_{i}\in C(X_{i}),$ $i=1,...,n.$ In [8], M.Golomb
obtained a formula for the error of this approximation in terms of measures
constructed o... | math.FA | let x_1x_n be compact spaces and xx_1times times x_n consider the approximation of a function fin cx by sums g_1x_1 g_nx_n where g_iin cx_i i1n in 8 mgolomb obtained a formula for the error of this approximation in terms of measures constructed on special points of x called projection cycles however his proof had a gap... | [['let', 'x_1x_n', 'be', 'compact', 'spaces', 'and', 'xx_1times', 'times', 'x_n', 'consider', 'the', 'approximation', 'of', 'a', 'function', 'fin', 'cx', 'by', 'sums', 'g_1x_1', 'g_nx_n', 'where', 'g_iin', 'cx_i', 'i1n', 'in', '8', 'mgolomb', 'obtained', 'a', 'formula', 'for', 'the', 'error', 'of', 'this', 'approximati... | [-0.15899594524720062, 0.08032431699878846, -0.09681478306237194, 0.07179540017128197, -0.00872390120704141, -0.1549258624513944, 0.0685672589034463, 0.303194006656607, -0.23767291493713855, -0.2148799399431381, 0.11850185205047536, -0.24964029169900137, -0.1219181593041867, 0.20052866020964252, -0.12416500240150426, -... |
708.3504 | Anisotropic conductivity of disordered 2DEGs due to spin-orbit
interactions | We show that the conductivity tensor of a disordered two-dimensional electron
gas becomes anisotropic in the presence of both Rashba and Dresselhaus
spin-orbit interactions (SOI). This anisotropy is a mesoscopic effect and
vanishes with vanishing charge dephasing time. Using a diagrammatic approach
including zero, on... | cond-mat.mes-hall | we show that the conductivity tensor of a disordered twodimensional electron gas becomes anisotropic in the presence of both rashba and dresselhaus spinorbit interactions soi this anisotropy is a mesoscopic effect and vanishes with vanishing charge dephasing time using a diagrammatic approach including zero one and two... | [['we', 'show', 'that', 'the', 'conductivity', 'tensor', 'of', 'a', 'disordered', 'twodimensional', 'electron', 'gas', 'becomes', 'anisotropic', 'in', 'the', 'presence', 'of', 'both', 'rashba', 'and', 'dresselhaus', 'spinorbit', 'interactions', 'soi', 'this', 'anisotropy', 'is', 'a', 'mesoscopic', 'effect', 'and', 'van... | [-0.228321320671203, 0.20824819129466274, -0.042644205472265356, 0.05516542081525664, -0.05842583780579361, -0.18334022204587122, 0.00752151361954065, 0.3467392813828256, -0.26551989652216434, -0.18543554483740418, -0.02960054417439725, -0.31108740888489983, -0.12669580722986548, 0.16880400201742662, 0.0657846130039772... |
708.3505 | Gaze as a Supplementary Modality for Interacting with Ambient
Intelligence Environments | We present our current research on the implementation of gaze as an efficient
and usable pointing modality supplementary to speech, for interacting with
augmented objects in our daily environment or large displays, especially
immersive virtual reality environments, such as reality centres and caves. We
are also addre... | cs.HC | we present our current research on the implementation of gaze as an efficient and usable pointing modality supplementary to speech for interacting with augmented objects in our daily environment or large displays especially immersive virtual reality environments such as reality centres and caves we are also addressing ... | [['we', 'present', 'our', 'current', 'research', 'on', 'the', 'implementation', 'of', 'gaze', 'as', 'an', 'efficient', 'and', 'usable', 'pointing', 'modality', 'supplementary', 'to', 'speech', 'for', 'interacting', 'with', 'augmented', 'objects', 'in', 'our', 'daily', 'environment', 'or', 'large', 'displays', 'especial... | [-0.09117562274517928, 0.027438005897064167, -0.036232404626331274, 0.054094125079535975, -0.14440053348934792, -0.22755217435274352, 0.014507719079661679, 0.4746998467066504, -0.21382345297829586, -0.3533865295956159, 0.09832243365359473, -0.26921436430866574, -0.1558107233858925, 0.22563082819180366, -0.1195977835202... |
708.3506 | Stability Analysis of Continuous Waves in Nonlocal Random Nonlinear
Media | On the basis of the competing cubic-quintic nonlinearity model, stability
(instability) of continuous waves in nonlocal random non-Kerr nonlinear media
is studied analytically and numerically. Fluctuating media parameters are
modeled by the Gaussian white noise. It is shown that for different response
functions of a ... | nlin.PS nlin.CD | on the basis of the competing cubicquintic nonlinearity model stability instability of continuous waves in nonlocal random nonkerr nonlinear media is studied analytically and numerically fluctuating media parameters are modeled by the gaussian white noise it is shown that for different response functions of a medium no... | [['on', 'the', 'basis', 'of', 'the', 'competing', 'cubicquintic', 'nonlinearity', 'model', 'stability', 'instability', 'of', 'continuous', 'waves', 'in', 'nonlocal', 'random', 'nonkerr', 'nonlinear', 'media', 'is', 'studied', 'analytically', 'and', 'numerically', 'fluctuating', 'media', 'parameters', 'are', 'modeled', ... | [-0.16843202479313724, 0.16500965278107477, -0.058729835752364214, 0.07429688093713946, -0.06822210123242291, -0.09974797891855643, -0.00458539825515939, 0.32559366009894525, -0.28327316513100453, -0.21777494321367494, 0.09321811539645365, -0.2794386503079, -0.16037189460418247, 0.1863666385525485, 0.03514391057159718,... |
708.3507 | Relativistic Tunneling Through Two Successive Barriers | We study the relativistic quantum mechanical problem of a Dirac particle
tunneling through two successive electrostatic barriers. Our aim is to study
the emergence of the so-called \emph{Generalized Hartman Effect}, an effect
observed in the context of nonrelativistic tunneling as well as in its
electromagnetic count... | quant-ph | we study the relativistic quantum mechanical problem of a dirac particle tunneling through two successive electrostatic barriers our aim is to study the emergence of the socalled emphgeneralized hartman effect an effect observed in the context of nonrelativistic tunneling as well as in its electromagnetic counterparts ... | [['we', 'study', 'the', 'relativistic', 'quantum', 'mechanical', 'problem', 'of', 'a', 'dirac', 'particle', 'tunneling', 'through', 'two', 'successive', 'electrostatic', 'barriers', 'our', 'aim', 'is', 'to', 'study', 'the', 'emergence', 'of', 'the', 'socalled', 'emphgeneralized', 'hartman', 'effect', 'an', 'effect', 'o... | [-0.15183018909513274, 0.1560147374626302, -0.10770018302454529, 0.10055200271792934, -0.053821328963915054, -0.07992398839613253, 0.04470908724767717, 0.35222223031292244, -0.2591436566276984, -0.3080718037418344, 0.024037188266149975, -0.26214890222036047, -0.18108459193979137, 0.18269629361933437, -0.004184305943040... |
708.3508 | The young stellar population of NGC 4214 as observed with HST. I. Data
and methods | We present the data and methods that we have used to perform a detailed
UV-optical study of the nearby dwarf starburst galaxy NGC 4214 using
multifilter HST/WFPC2+STIS photometry. We explain the process followed to
obtain high-quality photometry and astrometry of the stellar and cluster
populations of this galaxy. We... | astro-ph | we present the data and methods that we have used to perform a detailed uvoptical study of the nearby dwarf starburst galaxy ngc 4214 using multifilter hstwfpc2stis photometry we explain the process followed to obtain highquality photometry and astrometry of the stellar and cluster populations of this galaxy we describ... | [['we', 'present', 'the', 'data', 'and', 'methods', 'that', 'we', 'have', 'used', 'to', 'perform', 'a', 'detailed', 'uvoptical', 'study', 'of', 'the', 'nearby', 'dwarf', 'starburst', 'galaxy', 'ngc', '4214', 'using', 'multifilter', 'hstwfpc2stis', 'photometry', 'we', 'explain', 'the', 'process', 'followed', 'to', 'obta... | [0.007528342825082159, -0.007463969151038178, -0.19825375766598993, 0.1280515709786039, -0.10819748902006901, -0.04920243301918519, 0.06208462939002388, 0.49556216453538116, -0.15566876435114704, -0.37408657866462913, 0.05073465203227878, -0.2513552456050055, -0.03940778450329894, 0.20827037035355575, -0.07869827802072... |
708.3509 | Modeling polymerization of microtubules: a quantum mechanical approach | In this paper a quantum mechanical description of the assembly/disassembly
process for microtubules is proposed. We introduce creation and annihilation
operators that raise or lower the microtubule length by a tubulin layer.
Following that, the Hamiltonian and corresponding equations of motion for the
quantum fields ... | q-bio.BM cond-mat.stat-mech q-bio.QM | in this paper a quantum mechanical description of the assemblydisassembly process for microtubules is proposed we introduce creation and annihilation operators that raise or lower the microtubule length by a tubulin layer following that the hamiltonian and corresponding equations of motion for the quantum fields are de... | [['in', 'this', 'paper', 'a', 'quantum', 'mechanical', 'description', 'of', 'the', 'assemblydisassembly', 'process', 'for', 'microtubules', 'is', 'proposed', 'we', 'introduce', 'creation', 'and', 'annihilation', 'operators', 'that', 'raise', 'or', 'lower', 'the', 'microtubule', 'length', 'by', 'a', 'tubulin', 'layer', ... | [-0.15729580049951292, 0.15865256659397406, -0.0941486869367861, 0.06174901377411398, -0.07362991020706813, -0.12015265661982759, -0.03992382822945083, 0.3305320520509755, -0.30485253671800056, -0.21021130893589748, 0.05747792400577436, -0.2428226737237926, -0.2346804665548036, 0.1883139782341107, 0.004745980454308372,... |
708.351 | The young stellar population of NGC 4214 as observed with HST. II.
Results | We present the results of a detailed UV-optical study of the nearby dwarf
starburst galaxy NGC 4214 using multifilter HST/WFPC2+STIS photometry. The
stellar extinction is found to be quite patchy, with some areas having values
of E(4405-5495)< 0.1 mag and others, associated with star forming regions, much
more heavil... | astro-ph | we present the results of a detailed uvoptical study of the nearby dwarf starburst galaxy ngc 4214 using multifilter hstwfpc2stis photometry the stellar extinction is found to be quite patchy with some areas having values of e44055495 01 mag and others associated with star forming regions much more heavily obscured a r... | [['we', 'present', 'the', 'results', 'of', 'a', 'detailed', 'uvoptical', 'study', 'of', 'the', 'nearby', 'dwarf', 'starburst', 'galaxy', 'ngc', '4214', 'using', 'multifilter', 'hstwfpc2stis', 'photometry', 'the', 'stellar', 'extinction', 'is', 'found', 'to', 'be', 'quite', 'patchy', 'with', 'some', 'areas', 'having', '... | [-0.025212021111510694, 0.11045333756133914, -0.07485658371448517, 0.10478913903888315, -0.08260324176959694, -0.07454324003309011, 0.05121745230816305, 0.48032132667303085, -0.10982750115916133, -0.3899275518730283, 0.037103924873284996, -0.293078411757946, -0.019856699245050548, 0.2336568986326456, -0.069120873793959... |
708.3511 | Formulation of a constrained system in terms of extended Lagrangian and
its local symmetries | It is shown that an arbitrary singular Lagrangian theory (with first and
second class constraints up to $N$-th stage in the Hamiltonian formulation) can
be reformulated as a theory with at most third-stage constraints. The
corresponding Lagrangian $\tilde L$ can be obtained by pure algebraic methods,
its manifest for... | hep-th math-ph math.MP | it is shown that an arbitrary singular lagrangian theory with first and second class constraints up to nth stage in the hamiltonian formulation can be reformulated as a theory with at most thirdstage constraints the corresponding lagrangian tilde l can be obtained by pure algebraic methods its manifest form in terms of... | [['it', 'is', 'shown', 'that', 'an', 'arbitrary', 'singular', 'lagrangian', 'theory', 'with', 'first', 'and', 'second', 'class', 'constraints', 'up', 'to', 'nth', 'stage', 'in', 'the', 'hamiltonian', 'formulation', 'can', 'be', 'reformulated', 'as', 'a', 'theory', 'with', 'at', 'most', 'thirdstage', 'constraints', 'the... | [-0.15067792061753785, 0.1274264040244168, -0.09446155485943303, 0.040754041861978244, -0.08542113561697047, -0.14008409611281308, -0.05809968704860872, 0.27065354734445096, -0.30265940770362343, -0.3243615794070493, 0.08314989463977474, -0.22627237160026428, -0.1302618923698734, 0.15923468295441962, -0.010065247288680... |
708.3512 | An estimate for the location of QCD critical end point | It is proposed that a study of the ratio of shear viscosity to entropy
density $\frac{\eta}{s}$ as a function of the baryon chemical potential
$\mu_B$, and temperature T, provides a dynamic probe for the critical end point
(CEP) in hot and dense QCD matter. An initial estimate from an elliptic flow
excitation functio... | nucl-ex | it is proposed that a study of the ratio of shear viscosity to entropy density fracetas as a function of the baryon chemical potential mu_b and temperature t provides a dynamic probe for the critical end point cep in hot and dense qcd matter an initial estimate from an elliptic flow excitation function gives mutextcep_... | [['it', 'is', 'proposed', 'that', 'a', 'study', 'of', 'the', 'ratio', 'of', 'shear', 'viscosity', 'to', 'entropy', 'density', 'fracetas', 'as', 'a', 'function', 'of', 'the', 'baryon', 'chemical', 'potential', 'mu_b', 'and', 'temperature', 't', 'provides', 'a', 'dynamic', 'probe', 'for', 'the', 'critical', 'end', 'point... | [-0.09616830932521601, 0.17347659922819642, -0.13243948694931842, 0.026800163790140663, -0.015986513855395748, -0.07531751257867166, 0.11408850830616202, 0.30299897064886444, -0.22841474133339235, -0.29804135749979715, 0.0327739879153896, -0.31208425822735925, 0.03129669287591241, 0.17328549623943684, 0.053712415100052... |
708.3513 | Computational complexity of quantum optimal control landscapes | We study the Hamiltonian-independent contribution to the complexity of
quantum optimal control problems. The optimization of controls that steer
quantum systems to desired objectives can itself be considered a classical
dynamical system that executes an analog computation. The system-independent
component of the equa... | quant-ph | we study the hamiltonianindependent contribution to the complexity of quantum optimal control problems the optimization of controls that steer quantum systems to desired objectives can itself be considered a classical dynamical system that executes an analog computation the systemindependent component of the equations ... | [['we', 'study', 'the', 'hamiltonianindependent', 'contribution', 'to', 'the', 'complexity', 'of', 'quantum', 'optimal', 'control', 'problems', 'the', 'optimization', 'of', 'controls', 'that', 'steer', 'quantum', 'systems', 'to', 'desired', 'objectives', 'can', 'itself', 'be', 'considered', 'a', 'classical', 'dynamical... | [-0.13886301618102673, 0.10283821389748482, -0.07716804322720106, 0.06556695286604476, -0.043033566452296716, -0.16740093445571672, 0.038141766326901104, 0.3148067584760221, -0.33436436614637, -0.3075771160124402, 0.10986630580903563, -0.21108026519068518, -0.1384495834154742, 0.22667666499203604, -0.07562480829614547,... |
708.3514 | Characteristic 2 approach to bivariate interpolation problems | We investigate bivariate interpolation problems in characteristic 2. Given a
nonnegative integer $t$, we describe all the sub-linear systems generated by
monomials, in which there is no curve passing through a general point with
multiplicity at least $2^t$. As an application, we show that a certain linear
system of p... | math.AG math.NA | we investigate bivariate interpolation problems in characteristic 2 given a nonnegative integer t we describe all the sublinear systems generated by monomials in which there is no curve passing through a general point with multiplicity at least 2t as an application we show that a certain linear system of plane curves w... | [['we', 'investigate', 'bivariate', 'interpolation', 'problems', 'in', 'characteristic', '2', 'given', 'a', 'nonnegative', 'integer', 't', 'we', 'describe', 'all', 'the', 'sublinear', 'systems', 'generated', 'by', 'monomials', 'in', 'which', 'there', 'is', 'no', 'curve', 'passing', 'through', 'a', 'general', 'point', '... | [-0.22167901311625252, 0.0870700050903619, -0.06707166361606173, 0.0440980651407715, -0.03716755159231916, -0.17466452948977812, 0.024111514126783924, 0.3636962527474552, -0.3189190614707114, -0.21303360907589658, 0.10967733623182173, -0.29573558483338147, -0.17385087542954766, 0.21887457705707403, -0.04963168348267413... |
708.3515 | Intransitive geometries and fused amalgams | We study geometries that arise from the natural $G_2(K)$ action on the
geometry of one-dimensional subspaces, of nonsingular two-dimensional
subspaces, and of nonsingular three-dimensional subspaces of the building
geometry of type $C_3(K)$ where $K$ is a perfect field of characteristic 2. One
of these geometries is ... | math.GR math.CO | we study geometries that arise from the natural g_2k action on the geometry of onedimensional subspaces of nonsingular twodimensional subspaces and of nonsingular threedimensional subspaces of the building geometry of type c_3k where k is a perfect field of characteristic 2 one of these geometries is intransitive in su... | [['we', 'study', 'geometries', 'that', 'arise', 'from', 'the', 'natural', 'g_2k', 'action', 'on', 'the', 'geometry', 'of', 'onedimensional', 'subspaces', 'of', 'nonsingular', 'twodimensional', 'subspaces', 'and', 'of', 'nonsingular', 'threedimensional', 'subspaces', 'of', 'the', 'building', 'geometry', 'of', 'type', 'c... | [-0.12498101469997352, 0.10666730587307965, -0.09500682117978057, 0.032040069644899985, -0.08270635541293372, -0.10262740376287872, -0.02383791850721554, 0.32836142985276806, -0.3052496129954324, -0.2153074769212783, 0.09983902326129486, -0.2163520993809532, -0.20881375501574315, 0.19745947474848877, -0.122285776531992... |
708.3516 | Annihilation Rate of Heavy 0^{++} P-wave Quarkonium in Relativistic
Salpeter Method | Two-photon and two-gluon annihilation rates of P-wave scalar charmonium and
bottomonium up to third radial excited states are estimated in the relativistic
Salpeter method. We solved the full Salpeter equation with a well defined
relativistic wave function and calculated the transition amplitude using the
Mandelstam ... | hep-ph | twophoton and twogluon annihilation rates of pwave scalar charmonium and bottomonium up to third radial excited states are estimated in the relativistic salpeter method we solved the full salpeter equation with a well defined relativistic wave function and calculated the transition amplitude using the mandelstam formal... | [['twophoton', 'and', 'twogluon', 'annihilation', 'rates', 'of', 'pwave', 'scalar', 'charmonium', 'and', 'bottomonium', 'up', 'to', 'third', 'radial', 'excited', 'states', 'are', 'estimated', 'in', 'the', 'relativistic', 'salpeter', 'method', 'we', 'solved', 'the', 'full', 'salpeter', 'equation', 'with', 'a', 'well', '... | [-0.016148524066410597, 0.23803331868768465, -0.02334583758535545, 0.19485111732785476, -0.022581255252234547, -0.1456603091380491, 0.10937556292770839, 0.4194294859700632, -0.16234889310761924, -0.30813213560457636, -0.11824154534246545, -0.31928509237562736, 0.11261156044627835, 0.14722962562483166, 0.155264120583036... |
708.3517 | Sparse inverse covariance estimation with the lasso | We consider the problem of estimating sparse graphs by a lasso penalty
applied to the inverse covariance matrix. Using a coordinate descent procedure
for the lasso, we develop a simple algorithm that is remarkably fast: in the
worst cases, it solves a 1000 node problem (~500,000 parameters) in about a
minute, and is ... | stat.ME | we consider the problem of estimating sparse graphs by a lasso penalty applied to the inverse covariance matrix using a coordinate descent procedure for the lasso we develop a simple algorithm that is remarkably fast in the worst cases it solves a 1000 node problem 500000 parameters in about a minute and is 50 to 2000 ... | [['we', 'consider', 'the', 'problem', 'of', 'estimating', 'sparse', 'graphs', 'by', 'a', 'lasso', 'penalty', 'applied', 'to', 'the', 'inverse', 'covariance', 'matrix', 'using', 'a', 'coordinate', 'descent', 'procedure', 'for', 'the', 'lasso', 'we', 'develop', 'a', 'simple', 'algorithm', 'that', 'is', 'remarkably', 'fas... | [-0.04209921157427048, 0.010576163230233648, -0.07863198005165277, 0.12173633655439016, -0.09030595375748163, -0.1768919978175689, 0.09928091992676426, 0.4140522622325447, -0.2792837196095125, -0.3220595116360804, 0.14120245164030054, -0.257959626845262, -0.19901743489369916, 0.21545943798329892, -0.0848064811827008, 0... |
708.3518 | A Look at the Abandoned Contributions to Cosmology of Dirac, Sciama and
Dicke | The separate contributions to cosmology of the above researchers are
revisited and a cosmology encompassing their basic ideas is proposed. We study
Dirac's article on the large number hypothesis (1938), Sciama's proposal of
realizing Mach's principle (1953), and Dicke's considerations (1957) on a
flat-space represent... | physics.gen-ph gr-qc | the separate contributions to cosmology of the above researchers are revisited and a cosmology encompassing their basic ideas is proposed we study diracs article on the large number hypothesis 1938 sciamas proposal of realizing machs principle 1953 and dickes considerations 1957 on a flatspace representation of general... | [['the', 'separate', 'contributions', 'to', 'cosmology', 'of', 'the', 'above', 'researchers', 'are', 'revisited', 'and', 'a', 'cosmology', 'encompassing', 'their', 'basic', 'ideas', 'is', 'proposed', 'we', 'study', 'diracs', 'article', 'on', 'the', 'large', 'number', 'hypothesis', '1938', 'sciamas', 'proposal', 'of', '... | [-0.12506864285339592, 0.12056907728089884, -0.12245014908846345, 0.08415300709292661, -0.11722620176458425, -0.13066154836349517, 0.004108703472001663, 0.2914389524388813, -0.22988030243828728, -0.31303097472454494, 0.07311533959480104, -0.2374518964552208, -0.09028058279060074, 0.17992657389693925, -0.093327859107016... |
708.3519 | Photons inside a waveguide as massive particles | In the paper, we show that there exists a close analogy between the behavior
of de Broglie matter waves and that of electromagnetic waves inside a hollow
waveguide, such that the guided photons can be treated as free massive
particles subject to a relativistic quantum-mechanical equation. Inspired by
the effective re... | quant-ph | in the paper we show that there exists a close analogy between the behavior of de broglie matter waves and that of electromagnetic waves inside a hollow waveguide such that the guided photons can be treated as free massive particles subject to a relativistic quantummechanical equation inspired by the effective rest mas... | [['in', 'the', 'paper', 'we', 'show', 'that', 'there', 'exists', 'a', 'close', 'analogy', 'between', 'the', 'behavior', 'of', 'de', 'broglie', 'matter', 'waves', 'and', 'that', 'of', 'electromagnetic', 'waves', 'inside', 'a', 'hollow', 'waveguide', 'such', 'that', 'the', 'guided', 'photons', 'can', 'be', 'treated', 'as... | [-0.1358032638988929, 0.24807157002987318, -0.10354912875473131, 0.10775945669063079, -0.10032005757553342, -0.11781130182085398, 0.01690619090790458, 0.33413243169585866, -0.2185764753397692, -0.29044110348655117, -0.03461962362412179, -0.3007060361876624, -0.1475006449783658, 0.17658952787449514, 0.004116914982413069... |
708.352 | Prisoner's Dilemma in One-Dimensional Cellular Automata: Visualization
of Evolutionary Patterns | The spatial Prisoner's Dilemma is a prototype model to show the emergence of
cooperation in very competitive environments. It considers players, at site of
lattices, that can either cooperate or defect when playing the Prisoner's
Dilemma with other z players. This model presents a rich phase diagram. Here we
consider... | physics.comp-ph physics.soc-ph | the spatial prisoners dilemma is a prototype model to show the emergence of cooperation in very competitive environments it considers players at site of lattices that can either cooperate or defect when playing the prisoners dilemma with other z players this model presents a rich phase diagram here we consider players ... | [['the', 'spatial', 'prisoners', 'dilemma', 'is', 'a', 'prototype', 'model', 'to', 'show', 'the', 'emergence', 'of', 'cooperation', 'in', 'very', 'competitive', 'environments', 'it', 'considers', 'players', 'at', 'site', 'of', 'lattices', 'that', 'can', 'either', 'cooperate', 'or', 'defect', 'when', 'playing', 'the', '... | [-0.10400546666898043, 0.10954547447157553, -0.114002545753105, 0.06112996855901636, -0.07768695760175463, -0.23302341774771257, 0.09022983813474139, 0.4254463095253763, -0.2763193280840354, -0.2953225346077438, 0.019321143043171205, -0.27520550121586823, -0.16276422585744493, 0.08595136351816889, -0.07613950897427788,... |
708.3521 | A novel operation associated with Gauss' arithmetic-geometric means | The arithmetic mean is the mean for addition and the geometric mean is that
for multiplication. Then what kind of binary operation is associated with the
arithmetic-geometric mean (AGM) due to C. F. Gauss? If it is possible to
construct an arithmetic operation such that AGM is the mean for this operation,
it can be r... | math.NT math.GM | the arithmetic mean is the mean for addition and the geometric mean is that for multiplication then what kind of binary operation is associated with the arithmeticgeometric mean agm due to c f gauss if it is possible to construct an arithmetic operation such that agm is the mean for this operation it can be regarded as... | [['the', 'arithmetic', 'mean', 'is', 'the', 'mean', 'for', 'addition', 'and', 'the', 'geometric', 'mean', 'is', 'that', 'for', 'multiplication', 'then', 'what', 'kind', 'of', 'binary', 'operation', 'is', 'associated', 'with', 'the', 'arithmeticgeometric', 'mean', 'agm', 'due', 'to', 'c', 'f', 'gauss', 'if', 'it', 'is',... | [-0.12035485501561699, 0.11683121855265659, -0.12677144253861972, 0.06205889210640185, -0.061520448554007484, -0.09227870061629634, 0.008646737587445512, 0.38317796904807805, -0.36733178434700803, -0.2894852851977807, 0.14246050857446402, -0.21638011863293266, -0.20492696535141988, 0.23785816670406137, -0.1676047351960... |
708.3522 | Bounding the Betti numbers and computing the Euler-Poincar\'e
characteristic of semi-algebraic sets defined by partly quadratic systems of
polynomials | Let $\R$ be a real closed field, $ {\mathcal Q} \subset
\R[Y_1,...,Y_\ell,X_1,...,X_k], $ with $ \deg_{Y}(Q) \leq 2, \deg_{X}(Q) \leq
d, Q \in {\mathcal Q}, #({\mathcal Q})=m,$ and $ {\mathcal P} \subset
\R[X_1,...,X_k] $ with $\deg_{X}(P) \leq d, P \in {\mathcal P}, #({\mathcal
P})=s$, and $S \subset \R^{\ell+k}$ a ... | math.AG cs.SC math.AT math.GT | let r be a real closed field mathcal q subset ry_1y_ellx_1x_k with deg_yq leq 2 deg_xq leq d q in mathcal q mathcal qm and mathcal p subset rx_1x_k with deg_xp leq d p in mathcal p mathcal ps and s subset rellk a semialgebraic set defined by a boolean formula without negations with atoms p0 p geq 0 p leq 0 p in mathcal... | [['let', 'r', 'be', 'a', 'real', 'closed', 'field', 'mathcal', 'q', 'subset', 'ry_1y_ellx_1x_k', 'with', 'deg_yq', 'leq', '2', 'deg_xq', 'leq', 'd', 'q', 'in', 'mathcal', 'q', 'mathcal', 'qm', 'and', 'mathcal', 'p', 'subset', 'rx_1x_k', 'with', 'deg_xp', 'leq', 'd', 'p', 'in', 'mathcal', 'p', 'mathcal', 'ps', 'and', 's... | [-0.23960486638551468, 0.1412926471377218, 0.007225284048164373, -0.016884417795261147, -0.002610029234989163, -0.2125708843471811, 0.03778528733528219, 0.2713263439534999, -0.33373207855380743, -0.23159797141081928, -0.024189323127810733, -0.28573175880592316, -0.054719534534824026, 0.16748417427879758, -0.09094804016... |
708.3523 | Polarized neutron scattering study on antiferromagnetic states in
CeRh0.6Co0.4In5 | Polarized neutron scattering experiments were performed on mixed compound
CeRh0.6Co0.4In5 to clarify the nature of the low-temperature ordered states.
Three nonequivalent Bragg peaks, characterized by the wave vectors of q_h ~
(1/2,1/2,0.3), q_1 ~ (1/2,1/2,0.4) and q_c=(1/2,1/2,1/2), were observed at 1.4
K. These Bra... | cond-mat.str-el | polarized neutron scattering experiments were performed on mixed compound cerh06co04in5 to clarify the nature of the lowtemperature ordered states three nonequivalent bragg peaks characterized by the wave vectors of q_h 121203 q_1 121204 and q_c121212 were observed at 14 k these bragg peaks are found to occur entirely ... | [['polarized', 'neutron', 'scattering', 'experiments', 'were', 'performed', 'on', 'mixed', 'compound', 'cerh06co04in5', 'to', 'clarify', 'the', 'nature', 'of', 'the', 'lowtemperature', 'ordered', 'states', 'three', 'nonequivalent', 'bragg', 'peaks', 'characterized', 'by', 'the', 'wave', 'vectors', 'of', 'q_h', '121203'... | [-0.21626595742213475, 0.30156533849674844, -0.05783952138399784, 0.062328174205260795, -0.0015708618456314147, -0.10494949416877229, 0.04810912586735483, 0.43086186901364526, -0.2768690031756398, -0.28930947449530514, 0.0015115233918678174, -0.36737492058793425, -0.09208628493295588, 0.12817563466944168, 0.12320744597... |
708.3524 | The nanoscale phase separation in hole-doped manganites | A macroscopic phase separation, in which ferromagnetic clusters are observed
in an insulating matrix, is sometimes observed, and believed to be essential to
the colossal magnetoresistive (CMR) properties of manganese oxides. The
application of a magnetic field may indeed trigger large magnetoresistance
effects due to... | cond-mat.mtrl-sci cond-mat.str-el | a macroscopic phase separation in which ferromagnetic clusters are observed in an insulating matrix is sometimes observed and believed to be essential to the colossal magnetoresistive cmr properties of manganese oxides the application of a magnetic field may indeed trigger large magnetoresistance effects due to the per... | [['a', 'macroscopic', 'phase', 'separation', 'in', 'which', 'ferromagnetic', 'clusters', 'are', 'observed', 'in', 'an', 'insulating', 'matrix', 'is', 'sometimes', 'observed', 'and', 'believed', 'to', 'be', 'essential', 'to', 'the', 'colossal', 'magnetoresistive', 'cmr', 'properties', 'of', 'manganese', 'oxides', 'the',... | [-0.16796182662577983, 0.21613808587021704, -0.03754861012964351, 0.04563161683632288, -0.054020275797967504, -0.11242715726015953, 0.05574486508806486, 0.3607005572582527, -0.29744349773518924, -0.30542046445898896, 0.051139184136352524, -0.28931906911340066, -0.1830193122519498, 0.15001515228891882, -0.00598989145875... |
708.3525 | Gauge invariance and time symmetry breaking | Employing an arbitrary velocity gauge transformation this contribution argues
that the breaking of time symmetry is a natural consequence of irreversibility.
| physics.gen-ph | employing an arbitrary velocity gauge transformation this contribution argues that the breaking of time symmetry is a natural consequence of irreversibility | [['employing', 'an', 'arbitrary', 'velocity', 'gauge', 'transformation', 'this', 'contribution', 'argues', 'that', 'the', 'breaking', 'of', 'time', 'symmetry', 'is', 'a', 'natural', 'consequence', 'of', 'irreversibility']] | [-0.24265752581968195, 0.24971934965149212, -0.14090583065436, 0.03164103130499522, -0.1278413536603607, -0.055288765025103374, 0.010952282874357133, 0.30069317917029065, -0.30203984926144284, -0.25398945639885606, 9.998776728198642e-05, -0.1626036156501089, -0.13610660229321747, 0.06886546446808747, -0.042816540625478... |
708.3526 | 1/N_c corrections to the magnetic susceptibility of the QCD vacuum | We investigate the magnetic susceptibility of the QCD vacuum with the $1/N_c$
corrections taken into account, based on the instanton vacuum. Starting from
the instanton liquid model we derive the gauged light-quark partition function
in the presence of the current quark mass as well as of external Abelian vector
and ... | hep-ph | we investigate the magnetic susceptibility of the qcd vacuum with the 1n_c corrections taken into account based on the instanton vacuum starting from the instanton liquid model we derive the gauged lightquark partition function in the presence of the current quark mass as well as of external abelian vector and tensor f... | [['we', 'investigate', 'the', 'magnetic', 'susceptibility', 'of', 'the', 'qcd', 'vacuum', 'with', 'the', '1n_c', 'corrections', 'taken', 'into', 'account', 'based', 'on', 'the', 'instanton', 'vacuum', 'starting', 'from', 'the', 'instanton', 'liquid', 'model', 'we', 'derive', 'the', 'gauged', 'lightquark', 'partition', ... | [-0.09573609232716834, 0.22450883345295636, -0.06511618731760539, 0.09315456998494505, -0.05263251463876911, -0.047155585799914745, 0.04445090974778211, 0.3054128466059734, -0.18695493203450703, -0.27555265699290427, 0.04610292205695588, -0.28939404739124097, -0.0490452003625273, 0.09734009089165487, 0.0749282064601961... |
708.3527 | Science-Based Comparative Culture: A New Theme of Experiment for
Freshmen in Tohoku University | In 2004, Tohoku University created a new introductory science experimental
course for freshmen. The course is a compulsory subject for students in all
natural science fields. The course is not designed for a professional
education, but as a liberal education, in which students are trained to become
familiar with natu... | physics.ed-ph physics.pop-ph physics.soc-ph | in 2004 tohoku university created a new introductory science experimental course for freshmen the course is a compulsory subject for students in all natural science fields the course is not designed for a professional education but as a liberal education in which students are trained to become familiar with nature and ... | [['in', '2004', 'tohoku', 'university', 'created', 'a', 'new', 'introductory', 'science', 'experimental', 'course', 'for', 'freshmen', 'the', 'course', 'is', 'a', 'compulsory', 'subject', 'for', 'students', 'in', 'all', 'natural', 'science', 'fields', 'the', 'course', 'is', 'not', 'designed', 'for', 'a', 'professional'... | [-0.006208618024212061, 0.1455352021742384, -0.12195957596627616, 0.1027230207804752, -0.16764743422272102, -0.1434094232640096, 0.021499174007936855, 0.3291283925158941, -0.22252891396115326, -0.39652011710770274, 0.09032199238141884, -0.2678738370993916, -0.1625939291730827, 0.22728644605079779, -0.10728925291201746,... |
708.3528 | Determination of Penetration Depth of Transverse Spin Current in
Ferromagnetic Metals by Spin Pumping | Spin pumping in nonmagnetic/ferromagnetic metal multilayers is studied both
theoretically and experimentally. We show that the line widths of the
ferromagnetic resonance (FMR) spectrum depend on the thickness of the
ferromagnetic metal layers, which must not be in resonance with the oscillating
magnetic field. We als... | cond-mat.mes-hall cond-mat.other | spin pumping in nonmagneticferromagnetic metal multilayers is studied both theoretically and experimentally we show that the line widths of the ferromagnetic resonance fmr spectrum depend on the thickness of the ferromagnetic metal layers which must not be in resonance with the oscillating magnetic field we also show t... | [['spin', 'pumping', 'in', 'nonmagneticferromagnetic', 'metal', 'multilayers', 'is', 'studied', 'both', 'theoretically', 'and', 'experimentally', 'we', 'show', 'that', 'the', 'line', 'widths', 'of', 'the', 'ferromagnetic', 'resonance', 'fmr', 'spectrum', 'depend', 'on', 'the', 'thickness', 'of', 'the', 'ferromagnetic',... | [-0.12234660823243472, 0.23234422690643186, 0.04749581997356053, -0.005374256933495151, -0.007626671145220151, -0.12913515402025053, 0.018912265532430302, 0.5207781349465753, -0.23359722560376264, -0.32575302797087125, 0.0025226786952423914, -0.295804445453909, -0.012713791823454118, 0.22814685196270434, 0.094224154132... |
708.3529 | Tuning Co valence state in cobalt oxyhydrate superconductor by post
reduction | We report a successful tuning of Co valence state in cobalt oxyhydrate
superconductor via a facile post reduction using NaOH as reducing agent. The
change in Co valence was precisely determined by measuring the volume of the
released oxygen. The possible hydronium-incorporation was greatly suppressed in
concentrated ... | cond-mat.supr-con cond-mat.str-el | we report a successful tuning of co valence state in cobalt oxyhydrate superconductor via a facile post reduction using naoh as reducing agent the change in co valence was precisely determined by measuring the volume of the released oxygen the possible hydroniumincorporation was greatly suppressed in concentrated naoh ... | [['we', 'report', 'a', 'successful', 'tuning', 'of', 'co', 'valence', 'state', 'in', 'cobalt', 'oxyhydrate', 'superconductor', 'via', 'a', 'facile', 'post', 'reduction', 'using', 'naoh', 'as', 'reducing', 'agent', 'the', 'change', 'in', 'co', 'valence', 'was', 'precisely', 'determined', 'by', 'measuring', 'the', 'volum... | [-0.07784736232410762, 0.2370307454397594, 0.020733763692468137, -0.008637993654701859, -0.012128958456395637, -0.13380429847165942, 0.21963989388729846, 0.4020442891300523, -0.21228275653820242, -0.3552605199095394, 0.011058062071069366, -0.33627297488107744, -0.03142299479804933, 0.12392076013964556, 0.01450154544519... |
708.353 | Gravity localization on thick branes: a numerical approach | We introduce a numerical procedure to investigate the spectrum of massive
modes and its contribution for gravity localization on thick branes. After
considering a model with an analytically known Schroedinger potential, we
present the method and discuss its applicability. With this procedure we can
study several mode... | hep-th | we introduce a numerical procedure to investigate the spectrum of massive modes and its contribution for gravity localization on thick branes after considering a model with an analytically known schroedinger potential we present the method and discuss its applicability with this procedure we can study several models ev... | [['we', 'introduce', 'a', 'numerical', 'procedure', 'to', 'investigate', 'the', 'spectrum', 'of', 'massive', 'modes', 'and', 'its', 'contribution', 'for', 'gravity', 'localization', 'on', 'thick', 'branes', 'after', 'considering', 'a', 'model', 'with', 'an', 'analytically', 'known', 'schroedinger', 'potential', 'we', '... | [-0.12311557965812744, 0.056974356989686184, -0.0656891649032568, 0.08215052542554868, -0.02605229236379072, -0.13592643320995879, 0.027734347634235178, 0.354719037843215, -0.2255416801320268, -0.28052261365311487, 0.11107985872485034, -0.25040211113375405, -0.20877450080467508, 0.16662411149530731, -0.0463085321395041... |
708.3531 | Networked Multiple Description Estimation and Compression with Resource
Scalability | We present a joint source-channel multiple description (JSC-MD) framework for
resource-constrained network communications (e.g., sensor networks), in which
one or many deprived encoders communicate a Markov source against bit errors
and erasure errors to many heterogeneous decoders, some powerful and some
deprived. T... | cs.IT math.IT | we present a joint sourcechannel multiple description jscmd framework for resourceconstrained network communications eg sensor networks in which one or many deprived encoders communicate a markov source against bit errors and erasure errors to many heterogeneous decoders some powerful and some deprived to keep the enco... | [['we', 'present', 'a', 'joint', 'sourcechannel', 'multiple', 'description', 'jscmd', 'framework', 'for', 'resourceconstrained', 'network', 'communications', 'eg', 'sensor', 'networks', 'in', 'which', 'one', 'or', 'many', 'deprived', 'encoders', 'communicate', 'a', 'markov', 'source', 'against', 'bit', 'errors', 'and',... | [-0.17743344975965014, 0.013377396247197334, -0.04941100018853973, 0.07555557815348461, -0.05523970418172762, -0.27545675279097365, 0.09277019108820002, 0.42686120640494146, -0.3248570362477728, -0.28230356490584435, 0.110050856754751, -0.2241155469949154, -0.13875153953010225, 0.13806172357028956, -0.1519165910165297,... |
708.3532 | Three-dimensional multi-mesh material point method for solving collision
problems | Contact algorithm between different bodies plays an important role in solving
collision problems. Usually it is not easy to be treated very well. Several
ones for material point method were proposed by Bardenhangen, Brackbill, and
Sulsky\cite{Bardenhagen2000,Bardenhagen2001}, Hu and Chen\cite{Hu_Chen2003}.
An imp... | physics.comp-ph cond-mat.mtrl-sci physics.class-ph | contact algorithm between different bodies plays an important role in solving collision problems usually it is not easy to be treated very well several ones for material point method were proposed by bardenhangen brackbill and sulskycitebardenhagen2000bardenhagen2001 hu and chencitehu_chen2003 an improved one for three... | [['contact', 'algorithm', 'between', 'different', 'bodies', 'plays', 'an', 'important', 'role', 'in', 'solving', 'collision', 'problems', 'usually', 'it', 'is', 'not', 'easy', 'to', 'be', 'treated', 'very', 'well', 'several', 'ones', 'for', 'material', 'point', 'method', 'were', 'proposed', 'by', 'bardenhangen', 'brack... | [-0.11642621410631007, 0.08098153555123566, -0.10196170652583848, 0.026642761510827215, -0.06913999652581128, -0.18278716781439827, 0.010163976862120604, 0.3800101435804011, -0.2770001136434629, -0.3216981907962295, 0.0752658021678065, -0.2729718447182044, -0.1556685934521501, 0.23664718213410157, -0.04980819792810665,... |
708.3533 | Stability and convergence of the Method of Fundamental Solutions for
Helmholtz problems on analytic domains | The Method of Fundamental Solutions (MFS) is a popular tool to solve Laplace
and Helmholtz boundary value problems. Its main drawback is that it often leads
to ill-conditioned systems of equations. In this paper we investigate for the
interior Helmholtz problem on analytic domains how the singularities (charge
points... | math.NA | the method of fundamental solutions mfs is a popular tool to solve laplace and helmholtz boundary value problems its main drawback is that it often leads to illconditioned systems of equations in this paper we investigate for the interior helmholtz problem on analytic domains how the singularities charge points of the ... | [['the', 'method', 'of', 'fundamental', 'solutions', 'mfs', 'is', 'a', 'popular', 'tool', 'to', 'solve', 'laplace', 'and', 'helmholtz', 'boundary', 'value', 'problems', 'its', 'main', 'drawback', 'is', 'that', 'it', 'often', 'leads', 'to', 'illconditioned', 'systems', 'of', 'equations', 'in', 'this', 'paper', 'we', 'in... | [-0.11255234250198363, 0.037675945490206544, -0.08115324728485, 0.08344979531585092, -0.11047862199086107, -0.09761067114917463, 0.043012108456490464, 0.37064795458787364, -0.2686029369501691, -0.2715277717546805, 0.15694762013031563, -0.24937897124519193, -0.13326262812081136, 0.24173526276932342, -0.07377876116354999... |
708.3534 | Momentum-resolved charge excitations in high-Tc cuprates studied by
resonant inelastic x-ray scattering | We report a Cu K-edge resonant inelastic x-ray scattering (RIXS) study of
high-Tc cuprates. Momentum-resolved charge excitations in the CuO2 plane are
examined from parent Mott insulators to carrier-doped superconductors. The Mott
gap excitation in undoped insulators is found to commonly show a larger
dispersion alon... | cond-mat.str-el cond-mat.supr-con | we report a cu kedge resonant inelastic xray scattering rixs study of hightc cuprates momentumresolved charge excitations in the cuo2 plane are examined from parent mott insulators to carrierdoped superconductors the mott gap excitation in undoped insulators is found to commonly show a larger dispersion along the pipi ... | [['we', 'report', 'a', 'cu', 'kedge', 'resonant', 'inelastic', 'xray', 'scattering', 'rixs', 'study', 'of', 'hightc', 'cuprates', 'momentumresolved', 'charge', 'excitations', 'in', 'the', 'cuo2', 'plane', 'are', 'examined', 'from', 'parent', 'mott', 'insulators', 'to', 'carrierdoped', 'superconductors', 'the', 'mott', ... | [-0.18987122619074723, 0.22221521756296556, -0.02297017501935489, 0.11033585963482669, -0.061003753228776034, -0.15252977290774805, 0.11285283639079939, 0.4330951652915801, -0.25557961280978586, -0.20992464077327463, -0.08438360565874757, -0.4299135416177875, -0.036412337573908146, 0.1330780653535562, 0.102779395096951... |
708.3535 | Probability, unitarity, and realism in generally covariant quantum
information | The formalism of covariant quantum theory, introduced by Reisenberger and
Rovelli, casts the description of quantum states and evolution into a framework
compatable with the principles of general relativity. The leap to this
covariant formalism, however, outstripped the standard interpretation used to
connect quantum... | quant-ph gr-qc | the formalism of covariant quantum theory introduced by reisenberger and rovelli casts the description of quantum states and evolution into a framework compatable with the principles of general relativity the leap to this covariant formalism however outstripped the standard interpretation used to connect quantum theory... | [['the', 'formalism', 'of', 'covariant', 'quantum', 'theory', 'introduced', 'by', 'reisenberger', 'and', 'rovelli', 'casts', 'the', 'description', 'of', 'quantum', 'states', 'and', 'evolution', 'into', 'a', 'framework', 'compatable', 'with', 'the', 'principles', 'of', 'general', 'relativity', 'the', 'leap', 'to', 'this... | [-0.06600797993703976, 0.09439695611635739, -0.13852635918732928, 0.09496774682312781, -0.10639781079499434, -0.16031054691708785, 0.03806525130065964, 0.29750872181120813, -0.22743868858203398, -0.28185209967460195, 0.004587552695145421, -0.25326700779249817, -0.186085728383524, 0.15629148920865873, -0.091911366785684... |
708.3536 | Suzaku Observations of Hercules X-1 : Measurements of the Two Cyclotron
Harmonics | The accretion-powered pulsar Her X-1 was observed with Suzaku twice in its
main-on state, on 2005 October 5-6 and 2006 March 29-30, for a net exposure of
30.5 ks and 34.4 ks, respectively. In the 2005 and 2006 observations, the
source was detected at an average 10-30 keV intensity of 290 mCrab and 230
mCrab, respecti... | astro-ph | the accretionpowered pulsar her x1 was observed with suzaku twice in its mainon state on 2005 october 56 and 2006 march 2930 for a net exposure of 305 ks and 344 ks respectively in the 2005 and 2006 observations the source was detected at an average 1030 kev intensity of 290 mcrab and 230 mcrab respectively the intrins... | [['the', 'accretionpowered', 'pulsar', 'her', 'x1', 'was', 'observed', 'with', 'suzaku', 'twice', 'in', 'its', 'mainon', 'state', 'on', '2005', 'october', '56', 'and', '2006', 'march', '2930', 'for', 'a', 'net', 'exposure', 'of', '305', 'ks', 'and', '344', 'ks', 'respectively', 'in', 'the', '2005', 'and', '2006', 'obse... | [-0.048649006025126375, 0.14426587929190965, -0.051874448412059584, 0.10613197153470162, -0.04354056730007119, -0.1588109524694953, 0.06756381388062362, 0.4342406379903868, -0.15837040792769014, -0.40893332267506527, 0.08756709300802502, -0.35853804387608257, 0.018591311928268867, 0.22557205996432908, -0.01095113041090... |
708.3537 | Studies on the Chazy equations | In this paper, we study the Chazy III,IX and X equations. For the Chazy III
equation, by making the birational transformations the Chazy III equation is
transformed into a third-order ordinary differential equation of rational type.
For this equation, we find its meromorphic solutions, whose free parameters are
essen... | math.AG math.CA math.DS | in this paper we study the chazy iiiix and x equations for the chazy iii equation by making the birational transformations the chazy iii equation is transformed into a thirdorder ordinary differential equation of rational type for this equation we find its meromorphic solutions whose free parameters are essentially two... | [['in', 'this', 'paper', 'we', 'study', 'the', 'chazy', 'iiiix', 'and', 'x', 'equations', 'for', 'the', 'chazy', 'iii', 'equation', 'by', 'making', 'the', 'birational', 'transformations', 'the', 'chazy', 'iii', 'equation', 'is', 'transformed', 'into', 'a', 'thirdorder', 'ordinary', 'differential', 'equation', 'of', 'ra... | [-0.2105938867594187, -0.015648388580825085, -0.11385291650748024, 0.07540421470319136, -0.15083968268277553, -0.1876581503269382, -0.029417929479565758, 0.27680832702929203, -0.3699015133799269, -0.21639428280102901, 0.11016442696086298, -0.2880891510130217, -0.18130677666706152, 0.15431596000368397, -0.05905037654133... |
708.3538 | Quark Confinement and the Fractional Quantum Hall Effect | Working in the physics of Wilson factor and Aharonov-Bohm effect, we find in
the fluxtube-quark system the topology of a baryon consisting three heavy
flavor quarks resembles that of the fractional quantum Hall effect (FQHE) in
condensed matter. This similarity yields the result that the constituent quarks
of baryon ... | hep-ph | working in the physics of wilson factor and aharonovbohm effect we find in the fluxtubequark system the topology of a baryon consisting three heavy flavor quarks resembles that of the fractional quantum hall effect fqhe in condensed matter this similarity yields the result that the constituent quarks of baryon have the... | [['working', 'in', 'the', 'physics', 'of', 'wilson', 'factor', 'and', 'aharonovbohm', 'effect', 'we', 'find', 'in', 'the', 'fluxtubequark', 'system', 'the', 'topology', 'of', 'a', 'baryon', 'consisting', 'three', 'heavy', 'flavor', 'quarks', 'resembles', 'that', 'of', 'the', 'fractional', 'quantum', 'hall', 'effect', '... | [-0.16063113540651336, 0.25361009421573716, -0.1290524400800707, 0.10092286519726278, -0.010873980740065216, -0.09555874760913592, 0.07733522719823785, 0.26676160551767836, -0.18421479023762063, -0.3212010671374618, -0.038479791249408916, -0.27811011363081234, -0.09023772087949579, 0.11398426235042593, 0.02708735867773... |
708.3539 | An EL-labeling of the subgroup lattice | In a 2001 paper, Shareshian conjectured that the subgroup lattice of a
finite, solvable group has an EL-labeling. We construct such a labeling, and
verify that our labeling has the expected properties.
| math.CO math.GR | in a 2001 paper shareshian conjectured that the subgroup lattice of a finite solvable group has an ellabeling we construct such a labeling and verify that our labeling has the expected properties | [['in', 'a', '2001', 'paper', 'shareshian', 'conjectured', 'that', 'the', 'subgroup', 'lattice', 'of', 'a', 'finite', 'solvable', 'group', 'has', 'an', 'ellabeling', 'we', 'construct', 'such', 'a', 'labeling', 'and', 'verify', 'that', 'our', 'labeling', 'has', 'the', 'expected', 'properties']] | [-0.1294606029696297, 0.059534804506711225, -0.16250528016826138, 0.011327094616717659, -0.09706169622950256, -0.06595794718305115, 0.04155413472108194, 0.41647916520014405, -0.2598930412204936, -0.24831556162098423, 0.10313181200399413, -0.268337784538744, -0.19587876636069268, 0.1541362788702827, -0.14268093039572705... |
708.354 | On the endomorphism algebra of modular Gelfand-Graev representations | We study the endomorphism algebras of a modular Gelfand-Graev representation
of a finite reductive group by investigating modular properties of
homomorphisms constructed by Curtis and Curtis-Shoji.
| math.RT | we study the endomorphism algebras of a modular gelfandgraev representation of a finite reductive group by investigating modular properties of homomorphisms constructed by curtis and curtisshoji | [['we', 'study', 'the', 'endomorphism', 'algebras', 'of', 'a', 'modular', 'gelfandgraev', 'representation', 'of', 'a', 'finite', 'reductive', 'group', 'by', 'investigating', 'modular', 'properties', 'of', 'homomorphisms', 'constructed', 'by', 'curtis', 'and', 'curtisshoji']] | [-0.24181581109762193, 0.06382452834397555, -0.21409438870847225, 0.03782917205244303, -0.1732967136800289, -0.08453198682516813, -0.038776102364063265, 0.3073387311398983, -0.4104242494702339, -0.17911529481410982, 0.10417256699874997, -0.19609192647039891, -0.1913792350515723, 0.19776574913412331, -0.1232780338823795... |
708.3541 | Degenerations of quadratic differentials on CP1 | We describe the connected components of the complement of a natural
"diagonal" of real codimension 1 in a stratum of quadratic differentials on
CP1. We establish a natural bijection between the set of these connected
components and the set of generic configurations that appear on such "flat
spheres". We also prove th... | math.GT | we describe the connected components of the complement of a natural diagonal of real codimension 1 in a stratum of quadratic differentials on cp1 we establish a natural bijection between the set of these connected components and the set of generic configurations that appear on such flat spheres we also prove that the s... | [['we', 'describe', 'the', 'connected', 'components', 'of', 'the', 'complement', 'of', 'a', 'natural', 'diagonal', 'of', 'real', 'codimension', '1', 'in', 'a', 'stratum', 'of', 'quadratic', 'differentials', 'on', 'cp1', 'we', 'establish', 'a', 'natural', 'bijection', 'between', 'the', 'set', 'of', 'these', 'connected',... | [-0.2119058667966682, 0.06389576787801667, -0.06660424436429618, 0.04487719032396045, -0.08910605678748754, -0.12199860768547903, 0.03275773596316059, 0.3472164918590958, -0.26793505708014387, -0.191761050222946, 0.08323015681202782, -0.2635579471372896, -0.19145651437186947, 0.20505614599419963, -0.08875796977210687, ... |
708.3542 | Congestion, equilibrium and learning: The minority game | The minority game is a simple congestion game in which the players' main goal
is to choose among two options the one that is adopted by the smallest number
of players. We characterize the set of Nash equilibria and the limiting
behavior of several well-known learning processes in the minority game with an
arbitrary o... | physics.soc-ph | the minority game is a simple congestion game in which the players main goal is to choose among two options the one that is adopted by the smallest number of players we characterize the set of nash equilibria and the limiting behavior of several wellknown learning processes in the minority game with an arbitrary odd nu... | [['the', 'minority', 'game', 'is', 'a', 'simple', 'congestion', 'game', 'in', 'which', 'the', 'players', 'main', 'goal', 'is', 'to', 'choose', 'among', 'two', 'options', 'the', 'one', 'that', 'is', 'adopted', 'by', 'the', 'smallest', 'number', 'of', 'players', 'we', 'characterize', 'the', 'set', 'of', 'nash', 'equilibr... | [-0.11248393603388897, 0.10167536136158918, -0.10449051118992043, 0.12386080337455496, -0.05578602537174116, -0.2099254245686373, 0.10328885773196816, 0.35769927800830564, -0.2594487980346788, -0.3279631617902355, 0.0297626368419239, -0.2737791894681074, -0.1451563313180073, 0.08477070636934403, -0.12375966890954948, -... |
708.3543 | Space-time orientations and Maxwell's equations | An analysis of the concept of orientation used in electrodynamics is
presented. At least two different versions are encountered in the literature.
Both are clearly identified and comparisons are made.
| math-ph math.DG math.MP | an analysis of the concept of orientation used in electrodynamics is presented at least two different versions are encountered in the literature both are clearly identified and comparisons are made | [['an', 'analysis', 'of', 'the', 'concept', 'of', 'orientation', 'used', 'in', 'electrodynamics', 'is', 'presented', 'at', 'least', 'two', 'different', 'versions', 'are', 'encountered', 'in', 'the', 'literature', 'both', 'are', 'clearly', 'identified', 'and', 'comparisons', 'are', 'made']] | [-0.13632552151878674, 0.07018206171972755, -0.0564075171481818, 0.08051868846717601, 0.0013862202254434426, -0.10946422419510782, -0.11940504647791386, 0.44878417340417703, -0.19720274433493615, -0.3356848961984118, 0.14489976281765848, -0.3415101740974933, -0.10385028421878814, 0.2579811987777551, -0.0310693476349115... |
708.3544 | A crystal theoretic method for finding rigged configurations from paths | The Kerov--Kirillov--Reshetikhin (KKR) bijection gives one to one
correspondences between the set of highest paths and the set of rigged
configurations. In this paper, we give a crystal theoretic reformulation of the
KKR map from the paths to rigged configurations, using the combinatorial R and
energy functions. This... | math.QA math-ph math.MP | the kerovkirillovreshetikhin kkr bijection gives one to one correspondences between the set of highest paths and the set of rigged configurations in this paper we give a crystal theoretic reformulation of the kkr map from the paths to rigged configurations using the combinatorial r and energy functions this formalism p... | [['the', 'kerovkirillovreshetikhin', 'kkr', 'bijection', 'gives', 'one', 'to', 'one', 'correspondences', 'between', 'the', 'set', 'of', 'highest', 'paths', 'and', 'the', 'set', 'of', 'rigged', 'configurations', 'in', 'this', 'paper', 'we', 'give', 'a', 'crystal', 'theoretic', 'reformulation', 'of', 'the', 'kkr', 'map',... | [-0.13057845635821336, 0.026030723133991504, -0.13125354605566325, 0.05572948451876512, -0.06418234668672085, -0.0584722062299863, 0.08596983144726154, 0.33606744304114694, -0.3150291839807198, -0.28062120985625116, -0.015296244522123116, -0.2550233229111623, -0.16437126397444257, 0.18077767588968935, -0.04139413914225... |
708.3545 | Applied statistics: A review | The main phases of applied statistical work are discussed in general terms.
The account starts with the clarification of objectives and proceeds through
study design, measurement and analysis to interpretation. An attempt is made to
extract some general notions.
| stat.AP | the main phases of applied statistical work are discussed in general terms the account starts with the clarification of objectives and proceeds through study design measurement and analysis to interpretation an attempt is made to extract some general notions | [['the', 'main', 'phases', 'of', 'applied', 'statistical', 'work', 'are', 'discussed', 'in', 'general', 'terms', 'the', 'account', 'starts', 'with', 'the', 'clarification', 'of', 'objectives', 'and', 'proceeds', 'through', 'study', 'design', 'measurement', 'and', 'analysis', 'to', 'interpretation', 'an', 'attempt', 'is... | [-0.08172540849026962, 0.0663118991819479, -0.09836534360566965, 0.06950831839826722, -0.08263062518567611, -0.12087619013320176, 0.016663927632646684, 0.32786756978394127, -0.2477376784603947, -0.31453321539820767, 0.11017632950992826, -0.24407801230270892, -0.15800344393564722, 0.14960816741371766, -0.098547765746330... |
708.3546 | Field Experimental "Star Type" Metropolitan Quantum Key Distribution
Network | Quantum key distribution (QKD) network has recently attracted growing
attentions. Due to the special characteristics of quantum information, to build
a full-connectivity QKD network without trusted relays is a stimulating
challenge. In this letter, we report on the first realization of QKD network
without trusted rel... | quant-ph | quantum key distribution qkd network has recently attracted growing attentions due to the special characteristics of quantum information to build a fullconnectivity qkd network without trusted relays is a stimulating challenge in this letter we report on the first realization of qkd network without trusted relays which... | [['quantum', 'key', 'distribution', 'qkd', 'network', 'has', 'recently', 'attracted', 'growing', 'attentions', 'due', 'to', 'the', 'special', 'characteristics', 'of', 'quantum', 'information', 'to', 'build', 'a', 'fullconnectivity', 'qkd', 'network', 'without', 'trusted', 'relays', 'is', 'a', 'stimulating', 'challenge'... | [-0.23470644417485986, 0.09851082017132651, -0.04716272810257451, -0.017534190449997236, -0.05694311712832414, -0.2695249775713382, 0.12155229360399436, 0.4102646060116037, -0.27455522695397455, -0.2746296265819507, 0.036856489303853913, -0.2813930264078514, -0.13192300730684497, 0.20481694732294525, -0.140343237011296... |
708.3547 | New Probable Dwarf Galaxies in Northern Groups of the Local Supercluster | We have searched for nearby dwarf galaxies in 27 northern groups with
characteristic distances 8-15 Mpc based on the Second Palomar Sky Survey
prints. In a total area of about 2000 square degrees, we have found 90
low-surface-brightness objects, more than 60% of which are absent from known
catalogs and lists. We have... | astro-ph | we have searched for nearby dwarf galaxies in 27 northern groups with characteristic distances 815 mpc based on the second palomar sky survey prints in a total area of about 2000 square degrees we have found 90 lowsurfacebrightness objects more than 60 of which are absent from known catalogs and lists we have classifie... | [['we', 'have', 'searched', 'for', 'nearby', 'dwarf', 'galaxies', 'in', '27', 'northern', 'groups', 'with', 'characteristic', 'distances', '815', 'mpc', 'based', 'on', 'the', 'second', 'palomar', 'sky', 'survey', 'prints', 'in', 'a', 'total', 'area', 'of', 'about', '2000', 'square', 'degrees', 'we', 'have', 'found', '9... | [-0.09233586121394875, 0.07817886556897845, -0.024171493574976922, 0.08707878729772, -0.11370835003354365, -0.0557492391073278, 0.048646996112629064, 0.43440354096570183, -0.09526446070632942, -0.422956452163912, 0.0851731197221116, -0.33901520403368135, -0.04104666658788032, 0.25210312411987357, -0.017810092511631195,... |
708.3548 | One-dimensional fermionic gases with attractive p-wave interaction in a
hard-wall trap | We investigate the ground state of the one-dimensional fermionic system
enclosed in a hard-wall trap with attractive contact p-wave interactions. Based
on the Bethe ansatz method, the explicit wave function is derived by
numerically solving the Bethe ansatz equations for the full physical regimes
($-\infty \leq c_F\l... | cond-mat.other cond-mat.str-el | we investigate the ground state of the onedimensional fermionic system enclosed in a hardwall trap with attractive contact pwave interactions based on the bethe ansatz method the explicit wave function is derived by numerically solving the bethe ansatz equations for the full physical regimes infty leq c_fleq 0 with the... | [['we', 'investigate', 'the', 'ground', 'state', 'of', 'the', 'onedimensional', 'fermionic', 'system', 'enclosed', 'in', 'a', 'hardwall', 'trap', 'with', 'attractive', 'contact', 'pwave', 'interactions', 'based', 'on', 'the', 'bethe', 'ansatz', 'method', 'the', 'explicit', 'wave', 'function', 'is', 'derived', 'by', 'nu... | [-0.15176356181252265, 0.16522963690427045, -0.09673020709435352, 0.07770457104089912, 0.021094824056382532, -0.12512592977188802, -0.012685041115791709, 0.3214790431920577, -0.2145752826291654, -0.2505454492099859, 0.03910433603536889, -0.3159459601708308, -0.0923686920992892, 0.10272302428191459, 0.11770931474381575,... |
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