id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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708.1749 | Efficiency of quantum Monte Carlo impurity solvers for dynamical
mean-field theory | Since the inception of the dynamical mean-field theory, numerous numerical
studies have relied on the Hirsch-Fye quantum Monte Carlo (HF-QMC) method for
solving the associated impurity problem. Recently developed continuous-time
algorithms (CT-QMC) avoid the Trotter discretization error and allow for faster
configura... | cond-mat.str-el | since the inception of the dynamical meanfield theory numerous numerical studies have relied on the hirschfye quantum monte carlo hfqmc method for solving the associated impurity problem recently developed continuoustime algorithms ctqmc avoid the trotter discretization error and allow for faster configuration updates ... | [['since', 'the', 'inception', 'of', 'the', 'dynamical', 'meanfield', 'theory', 'numerous', 'numerical', 'studies', 'have', 'relied', 'on', 'the', 'hirschfye', 'quantum', 'monte', 'carlo', 'hfqmc', 'method', 'for', 'solving', 'the', 'associated', 'impurity', 'problem', 'recently', 'developed', 'continuoustime', 'algori... | [-0.062163287439547917, 0.029609022103250025, -0.11508854883996879, 0.09930656827602755, -0.0362177138819414, -0.18751564841744872, 0.07959381459582159, 0.4041837931884562, -0.2016057350891916, -0.32685632300289236, 0.12321558739195633, -0.2566786251715658, -0.09269155224456507, 0.24064736664295197, -0.0180723835659377... |
708.175 | Dark-State Polaritons in Single- and Double-$\Lambda$ Media | We derive the properties of polaritons in single-$\Lambda$ and
double-$\Lambda$ media using a microscopic equation-of-motion technique. In
each case, the polaritonic dispersion relation and composition arise from a
matrix eigenvalue problem for arbitrary control field strengths. We show that
the double-$\Lambda$ medi... | physics.atom-ph | we derive the properties of polaritons in singlelambda and doublelambda media using a microscopic equationofmotion technique in each case the polaritonic dispersion relation and composition arise from a matrix eigenvalue problem for arbitrary control field strengths we show that the doublelambda medium can be used to u... | [['we', 'derive', 'the', 'properties', 'of', 'polaritons', 'in', 'singlelambda', 'and', 'doublelambda', 'media', 'using', 'a', 'microscopic', 'equationofmotion', 'technique', 'in', 'each', 'case', 'the', 'polaritonic', 'dispersion', 'relation', 'and', 'composition', 'arise', 'from', 'a', 'matrix', 'eigenvalue', 'proble... | [-0.11930950214848557, 0.23985851151333687, -0.05587379115217544, 0.05481969800336841, 0.011817234171990385, -0.1080905521199345, 0.10160294049568078, 0.38146381002870644, -0.2823039014660258, -0.2607178589220139, 0.003593884844412195, -0.27078367928736546, -0.052495708399293746, 0.15430196480667022, 0.0575977022204785... |
708.1751 | Superconducting islands, phase fluctuations and the
superconductor-insulator transition | Properties of disordered thin films are discussed based on the viewpoint that
superconducting islands are formed in the system. These lead to superconducting
correlations confined in space, which are known to form spontaneously in thin
films. Application of a perpendicular magnetic field can drive the system from
the... | cond-mat.supr-con cond-mat.dis-nn | properties of disordered thin films are discussed based on the viewpoint that superconducting islands are formed in the system these lead to superconducting correlations confined in space which are known to form spontaneously in thin films application of a perpendicular magnetic field can drive the system from the supe... | [['properties', 'of', 'disordered', 'thin', 'films', 'are', 'discussed', 'based', 'on', 'the', 'viewpoint', 'that', 'superconducting', 'islands', 'are', 'formed', 'in', 'the', 'system', 'these', 'lead', 'to', 'superconducting', 'correlations', 'confined', 'in', 'space', 'which', 'are', 'known', 'to', 'form', 'spontaneo... | [-0.21105371778236426, 0.20223656092771017, -0.04660856512751668, 0.0057224625662127705, -0.00879544808350979, -0.13364485835042247, 0.03094078455630571, 0.40447844503487046, -0.25014299998416545, -0.31666233293474355, 0.03711769668301171, -0.3253986771079771, -0.09926013022344163, 0.21556823669457215, 0.01042188197731... |
708.1752 | Validation of the new Hipparcos reduction | Context.A new reduction of the astrometric data as produced by the Hipparcos
mission has been published, claiming accuracies for nearly all stars brighter
than magnitude Hp = 8 to be better, by up to a factor 4, than in the original
catalogue. Aims.The new Hipparcos astrometric catalogue is checked for the
quality of... | astro-ph | contexta new reduction of the astrometric data as produced by the hipparcos mission has been published claiming accuracies for nearly all stars brighter than magnitude hp 8 to be better by up to a factor 4 than in the original catalogue aimsthe new hipparcos astrometric catalogue is checked for the quality of the data ... | [['contexta', 'new', 'reduction', 'of', 'the', 'astrometric', 'data', 'as', 'produced', 'by', 'the', 'hipparcos', 'mission', 'has', 'been', 'published', 'claiming', 'accuracies', 'for', 'nearly', 'all', 'stars', 'brighter', 'than', 'magnitude', 'hp', '8', 'to', 'be', 'better', 'by', 'up', 'to', 'a', 'factor', '4', 'tha... | [-0.08240039390012888, 0.06578230189576667, -0.06216351146188875, 0.09382373391727014, -0.09075758430131134, -0.035375387095181, 0.10864293771751579, 0.3725286409258842, -0.1740266346372664, -0.4163683942297385, 0.10121729435909185, -0.3070276188242826, -0.0013162517465562338, 0.26265281450469047, -0.09381944532506167,... |
708.1753 | Measurement of the $B^0\to X_{u}^- \ell^+ {\nu_\ell} $ decays near the
kinematic endpoint of the lepton spectrum and search for violation of isospin
symmetry | We present the first measurement of the $B^0\to X_{u}^- \ell^+ {\nu_\ell} $
partial branching fraction in the end-point region of the lepton momentum
spectrum, above the threshold for $B\to X_c\ell {\nu_\ell}$ decays. The
analysis is based on a sample of 383 million $\Upsilon(4S)$ decays into $B{\bar
B}$ pairs collec... | hep-ex | we present the first measurement of the b0to x_u ell nu_ell partial branching fraction in the endpoint region of the lepton momentum spectrum above the threshold for bto x_cell nu_ell decays the analysis is based on a sample of 383 million upsilon4s decays into bbar b pairs collected with the sc babar detector at the p... | [['we', 'present', 'the', 'first', 'measurement', 'of', 'the', 'b0to', 'x_u', 'ell', 'nu_ell', 'partial', 'branching', 'fraction', 'in', 'the', 'endpoint', 'region', 'of', 'the', 'lepton', 'momentum', 'spectrum', 'above', 'the', 'threshold', 'for', 'bto', 'x_cell', 'nu_ell', 'decays', 'the', 'analysis', 'is', 'based', ... | [-0.10198084663408838, 0.23441635121400498, -0.038202932500714284, 0.06046730765034532, -0.04142201332641499, -0.13892155473832019, 0.14695886921958987, 0.21154990054447181, -0.21735746679706094, -0.20988907763931136, -0.05784333722741106, -0.47307500273266934, 0.10841747842185338, 0.10181274224703217, 0.10875535570573... |
708.1754 | Treatment of Linear and Nonlinear Dielectric Property of Molecular
Monolayer and Submonolayer with Microscopic Dipole Lattice Model: I. Second
Harmonic Generation and Sum-Frequency Generation | In the currently accepted models of the nonlinear optics, the nonlinear
radiation was treated as the result of an infinitesimally thin polarization
sheet layer, and a three layer model was generally employed. The direct
consequence of this approach is that an apriori dielectric constant, which
still does not have a c... | physics.chem-ph physics.optics | in the currently accepted models of the nonlinear optics the nonlinear radiation was treated as the result of an infinitesimally thin polarization sheet layer and a three layer model was generally employed the direct consequence of this approach is that an apriori dielectric constant which still does not have a clear d... | [['in', 'the', 'currently', 'accepted', 'models', 'of', 'the', 'nonlinear', 'optics', 'the', 'nonlinear', 'radiation', 'was', 'treated', 'as', 'the', 'result', 'of', 'an', 'infinitesimally', 'thin', 'polarization', 'sheet', 'layer', 'and', 'a', 'three', 'layer', 'model', 'was', 'generally', 'employed', 'the', 'direct',... | [-0.07461973334207826, 0.12006050795535259, -0.0692409024707944, 0.02963172475370698, -0.05139307492115473, -0.10860986052649929, 0.013495749086848231, 0.41618340878823507, -0.2642000299860979, -0.2823633768374702, 0.0598655608582314, -0.2474335907733771, -0.1615582293765583, 0.19163108256406328, 0.012363742020502977, ... |
708.1755 | Biperiodic superlattices and the transparent state | Coquelin et al. studied biperiodic semiconductor superlattices, which consist
of alternating cell types, one with wide wells and the other narrow wells,
separated by equal strength barriers. If the wells were identical, it would be
a simply periodic system of $N = 2n$ half-cells. When asymmetry is introduced,
an allo... | quant-ph | coquelin et al studied biperiodic semiconductor superlattices which consist of alternating cell types one with wide wells and the other narrow wells separated by equal strength barriers if the wells were identical it would be a simply periodic system of n 2n halfcells when asymmetry is introduced an allowed band splits... | [['coquelin', 'et', 'al', 'studied', 'biperiodic', 'semiconductor', 'superlattices', 'which', 'consist', 'of', 'alternating', 'cell', 'types', 'one', 'with', 'wide', 'wells', 'and', 'the', 'other', 'narrow', 'wells', 'separated', 'by', 'equal', 'strength', 'barriers', 'if', 'the', 'wells', 'were', 'identical', 'it', 'w... | [-0.18622680581756867, 0.17256121952163994, -0.04540752344473731, 0.016193291929994302, -0.02507976148990565, -0.23296574062260333, 0.08314797314415046, 0.3990676689427346, -0.27340726918919245, -0.29904412535688607, 0.03803937636075716, -0.28261722275055945, -0.10839713261884754, 0.1591326755078626, 0.0117450626585196... |
708.1756 | Optimal execution strategies in limit order books with general shape
functions | We consider optimal execution strategies for block market orders placed in a
limit order book (LOB). We build on the resilience model proposed by Obizhaeva
and Wang (2005) but allow for a general shape of the LOB defined via a given
density function. Thus, we can allow for empirically observed LOB shapes and
obtain a... | q-fin.TR math.PR | we consider optimal execution strategies for block market orders placed in a limit order book lob we build on the resilience model proposed by obizhaeva and wang 2005 but allow for a general shape of the lob defined via a given density function thus we can allow for empirically observed lob shapes and obtain a nonlinea... | [['we', 'consider', 'optimal', 'execution', 'strategies', 'for', 'block', 'market', 'orders', 'placed', 'in', 'a', 'limit', 'order', 'book', 'lob', 'we', 'build', 'on', 'the', 'resilience', 'model', 'proposed', 'by', 'obizhaeva', 'and', 'wang', '2005', 'but', 'allow', 'for', 'a', 'general', 'shape', 'of', 'the', 'lob',... | [-0.09994371369214217, 0.030734493441257504, -0.09688806424614543, 0.09881755862009238, -0.049830391770228744, -0.09375549973348123, 0.12965668699219388, 0.3548792284526672, -0.2516912921040444, -0.29809115201742686, 0.14188297808290137, -0.23071686006614078, -0.14817144853139178, 0.16919841002046582, -0.10339901304316... |
708.1757 | The multiplicity of weights in nonprimitive pairs of weights | For each type of classical Lie algebra, we list the dominant highest weights
$\zeta$ for which $(\zeta;\mu_i)$ is not a primitive pair and the weight space
$V_{\mu_i}$ has dimension one where $\mu_i$ are the highest long and short
roots in each case. These dimension one weight spaces lead to examples of
nilmanifolds ... | math.RT | for each type of classical lie algebra we list the dominant highest weights zeta for which zetamu_i is not a primitive pair and the weight space v_mu_i has dimension one where mu_i are the highest long and short roots in each case these dimension one weight spaces lead to examples of nilmanifolds for which we cannot pr... | [['for', 'each', 'type', 'of', 'classical', 'lie', 'algebra', 'we', 'list', 'the', 'dominant', 'highest', 'weights', 'zeta', 'for', 'which', 'zetamu_i', 'is', 'not', 'a', 'primitive', 'pair', 'and', 'the', 'weight', 'space', 'v_mu_i', 'has', 'dimension', 'one', 'where', 'mu_i', 'are', 'the', 'highest', 'long', 'and', '... | [-0.15592071325296447, 0.12357861405268075, -0.02670664582697172, 0.07111064413569808, -0.12293948420500826, -0.16819151216703984, -0.003933202734010087, 0.37394853710891707, -0.30869104135375, -0.1845219497613254, 0.11912130217053114, -0.2591116999142936, -0.114204938756302, 0.19059083034609636, -0.052713761534837505,... |
708.1758 | Vanishing moment method and moment solutions for second order fully
nonlinear partial differential equations | This paper concerns with numerical approximations of solutions of second
order fully nonlinear partial differential equations (PDEs). A new notion of
weak solutions, called moment solutions, is introduced for second order fully
nonlinear PDEs. Unlike viscosity solutions, moment solutions are defined by a
constructive... | math.NA math.AP | this paper concerns with numerical approximations of solutions of second order fully nonlinear partial differential equations pdes a new notion of weak solutions called moment solutions is introduced for second order fully nonlinear pdes unlike viscosity solutions moment solutions are defined by a constructive method c... | [['this', 'paper', 'concerns', 'with', 'numerical', 'approximations', 'of', 'solutions', 'of', 'second', 'order', 'fully', 'nonlinear', 'partial', 'differential', 'equations', 'pdes', 'a', 'new', 'notion', 'of', 'weak', 'solutions', 'called', 'moment', 'solutions', 'is', 'introduced', 'for', 'second', 'order', 'fully',... | [-0.11899122820209919, 0.031077440440033872, -0.05754620724150704, 0.05783357984991097, -0.11230801300391452, -0.10398235414888607, -0.031570905364787905, 0.2818478013505228, -0.3102000973368477, -0.23569141237142807, 0.1726375961823376, -0.2833447672633661, -0.16186464099397804, 0.15739797527850088, -0.046430532406601... |
708.1759 | Blogging in the physics classroom: A research-based approach to shaping
students' attitudes towards physics | Even though there has been a tremendous amount of research done in how to
help students learn physics, students are still coming away missing a crucial
piece of the puzzle: why bother with physics? Students learn fundamental laws
and how to calculate, but come out of a general physics course without a deep
understand... | physics.ed-ph | even though there has been a tremendous amount of research done in how to help students learn physics students are still coming away missing a crucial piece of the puzzle why bother with physics students learn fundamental laws and how to calculate but come out of a general physics course without a deep understanding of... | [['even', 'though', 'there', 'has', 'been', 'a', 'tremendous', 'amount', 'of', 'research', 'done', 'in', 'how', 'to', 'help', 'students', 'learn', 'physics', 'students', 'are', 'still', 'coming', 'away', 'missing', 'a', 'crucial', 'piece', 'of', 'the', 'puzzle', 'why', 'bother', 'with', 'physics', 'students', 'learn', ... | [0.00665840693265916, 0.12825672754445253, -0.12753787846105474, 0.11154975349772085, -0.1707057905016252, -0.1881790263329545, 0.05969667572898265, 0.3724719683926266, -0.23215731918517277, -0.39859573223675865, 0.06748888756767409, -0.3155144475436268, -0.1592982767506017, 0.19903267305428918, -0.09146162941890666, -... |
708.176 | On the relativistic Vlasov-Poisson system | The Cauchy problem is revisited for the so-called relativistic Vlasov-Poisson
system in the attractive case. Global existence and uniqueness of spherical
classical solutions is proved under weaker assumptions than previously used. A
new class of blowing up solutions is found when these conditions are violated.
A new,... | math-ph math.AP math.MP | the cauchy problem is revisited for the socalled relativistic vlasovpoisson system in the attractive case global existence and uniqueness of spherical classical solutions is proved under weaker assumptions than previously used a new class of blowing up solutions is found when these conditions are violated a new nongrav... | [['the', 'cauchy', 'problem', 'is', 'revisited', 'for', 'the', 'socalled', 'relativistic', 'vlasovpoisson', 'system', 'in', 'the', 'attractive', 'case', 'global', 'existence', 'and', 'uniqueness', 'of', 'spherical', 'classical', 'solutions', 'is', 'proved', 'under', 'weaker', 'assumptions', 'than', 'previously', 'used'... | [-0.14097921784928957, 0.07619490546049244, -0.07501330457405368, 0.14591697749591417, -0.11079330234649355, -0.1834896907710762, -0.04960895628571065, 0.2567190487604977, -0.26032016411034475, -0.23143369141521294, 0.132145964203458, -0.2084413114379146, -0.09550533028069272, 0.232941316214821, -0.04683334128184022, 0... |
708.1761 | Lost Baryons at Low Redshift | We review our attempts to discover lost baryons at low redshift with ``X-ray
forest'' of absorption lines from the warm-hot intergalactic medium. We discuss
the best evidence to date along the Mrk 421 sightline. We then discuss the
missing baryons in the Local Group and the significance of the z=0 absorption
systems ... | astro-ph | we review our attempts to discover lost baryons at low redshift with xray forest of absorption lines from the warmhot intergalactic medium we discuss the best evidence to date along the mrk 421 sightline we then discuss the missing baryons in the local group and the significance of the z0 absorption systems in xray spe... | [['we', 'review', 'our', 'attempts', 'to', 'discover', 'lost', 'baryons', 'at', 'low', 'redshift', 'with', 'xray', 'forest', 'of', 'absorption', 'lines', 'from', 'the', 'warmhot', 'intergalactic', 'medium', 'we', 'discuss', 'the', 'best', 'evidence', 'to', 'date', 'along', 'the', 'mrk', '421', 'sightline', 'we', 'then'... | [-0.07179413718171418, 0.10209329351317137, -0.04068580273073166, 0.1205208692199085, -0.12447122079553083, -0.018662503473460674, 0.06827481979504228, 0.4776085074990988, -0.20846797436475753, -0.30737167277373373, 0.06009299679426476, -0.38286720758304, -0.04019468007609248, 0.14524556257762014, 0.044187544328160584,... |
708.1762 | The Classical r-matrix of AdS/CFT and its Lie Bialgebra Structure | In this paper we investigate the algebraic structure of AdS/CFT in the
strong-coupling limit. We propose an expression for the classical r-matrix with
(deformed) u(2|2) symmetry, which leads to a quasi-triangular Lie bialgebra as
the underlying symmetry algebra. On the fundamental representation our r-matrix
coincide... | hep-th math.QA nlin.SI | in this paper we investigate the algebraic structure of adscft in the strongcoupling limit we propose an expression for the classical rmatrix with deformed u22 symmetry which leads to a quasitriangular lie bialgebra as the underlying symmetry algebra on the fundamental representation our rmatrix coincides with the clas... | [['in', 'this', 'paper', 'we', 'investigate', 'the', 'algebraic', 'structure', 'of', 'adscft', 'in', 'the', 'strongcoupling', 'limit', 'we', 'propose', 'an', 'expression', 'for', 'the', 'classical', 'rmatrix', 'with', 'deformed', 'u22', 'symmetry', 'which', 'leads', 'to', 'a', 'quasitriangular', 'lie', 'bialgebra', 'as... | [-0.13637756272153226, 0.022445928940455044, -0.10542553023628469, 0.06367635156493634, -0.14835118780018025, -0.11149532802156964, 0.005435587776789688, 0.32566272052672673, -0.3507732269969189, -0.17026866592449258, 0.05072629625715737, -0.19649054872680385, -0.18405061939133788, 0.1325195785787589, -0.09000592200823... |
708.1763 | Exact asymptotics of the characteristic polynomial of the symmetric
Pascal matrix | We have obtained the exact asymptotics of the determinant $\det_{1\leq
r,s\leq L}[\binom{r+s-2}{r-1}+\exp(i\theta)\delta_{r,s}]$. Inverse symbolic
computing methods were used to obtain exact analytical expressions for all
terms up to relative order $L^{-14}$ to the leading term. This determinant is
known to give weig... | math-ph cond-mat.stat-mech math.MP | we have obtained the exact asymptotics of the determinant det_1leq rsleq lbinomrs2r1expithetadelta_rs inverse symbolic computing methods were used to obtain exact analytical expressions for all terms up to relative order l14 to the leading term this determinant is known to give weighted enumerations of cyclically symme... | [['we', 'have', 'obtained', 'the', 'exact', 'asymptotics', 'of', 'the', 'determinant', 'det_1leq', 'rsleq', 'lbinomrs2r1expithetadelta_rs', 'inverse', 'symbolic', 'computing', 'methods', 'were', 'used', 'to', 'obtain', 'exact', 'analytical', 'expressions', 'for', 'all', 'terms', 'up', 'to', 'relative', 'order', 'l14', ... | [-0.16247314432612023, 0.09429728914386569, -0.0832475175221379, 0.0847314194311949, -0.04420547196581864, -0.10672158197177431, 0.08849537537063067, 0.331459110793777, -0.2034664389450485, -0.2681958573804691, 0.12334089931428958, -0.2982083140239597, -0.1378871712188881, 0.18251447682418168, -0.026660632663734782, 0.... |
708.1764 | A discontinuity in the low-mass initial mass function | The origin of brown dwarfs (BDs) is still an unsolved mystery. While the
standard model describes the formation of BDs and stars in a similar way recent
data on the multiplicity properties of stars and BDs show them to have
different binary distribution functions. Here we show that proper treatment of
these uncovers ... | astro-ph | the origin of brown dwarfs bds is still an unsolved mystery while the standard model describes the formation of bds and stars in a similar way recent data on the multiplicity properties of stars and bds show them to have different binary distribution functions here we show that proper treatment of these uncovers a disc... | [['the', 'origin', 'of', 'brown', 'dwarfs', 'bds', 'is', 'still', 'an', 'unsolved', 'mystery', 'while', 'the', 'standard', 'model', 'describes', 'the', 'formation', 'of', 'bds', 'and', 'stars', 'in', 'a', 'similar', 'way', 'recent', 'data', 'on', 'the', 'multiplicity', 'properties', 'of', 'stars', 'and', 'bds', 'show',... | [-0.10059155766324206, 0.1491408359460344, -0.11356964408178029, 0.123744090590956, -0.08758613802345953, -0.06775590672256704, 0.10556821950241982, 0.35509470515833125, -0.16778650452514862, -0.3508085388631567, 0.05308590377094297, -0.27600945145126404, -0.09280735330553505, 0.19486488708969588, -0.07928850646974064,... |
708.1765 | Quantum phase transitions in the extended periodic Anderson model | We investigate quantum phase transitions in the extended periodic Anderson
model, which includes electron correlations within and between itinerant and
localized bands. We calculate zero and finite temperature properties of the
system using the combination of dynamical mean-field theory and the numerical
renormalizat... | cond-mat.str-el | we investigate quantum phase transitions in the extended periodic anderson model which includes electron correlations within and between itinerant and localized bands we calculate zero and finite temperature properties of the system using the combination of dynamical meanfield theory and the numerical renormalization g... | [['we', 'investigate', 'quantum', 'phase', 'transitions', 'in', 'the', 'extended', 'periodic', 'anderson', 'model', 'which', 'includes', 'electron', 'correlations', 'within', 'and', 'between', 'itinerant', 'and', 'localized', 'bands', 'we', 'calculate', 'zero', 'and', 'finite', 'temperature', 'properties', 'of', 'the',... | [-0.21541695816806708, 0.26888507479236945, -0.07138020610781731, 0.07456296934698778, 0.005379435871199584, -0.19905917255608882, 0.1422619244581761, 0.36027873667276084, -0.26991416973975935, -0.22060269720128012, 0.039682351437578395, -0.3162142221160509, -0.10450020610113386, 0.09336473616659297, 0.0720344135016030... |
708.1766 | The Oxygen Abundances of Luminous and Ultraluminous Infrared Galaxies | Luminous and ultraluminous infrared galaxies (LIRGs and ULIRGs) dominate the
star formation rate budget of the universe at z > 1, yet no local measurements
of their heavy element abundances exist. We measure nuclear or near-nuclear
oxygen abundances in a sample of 100 star-forming LIRGs and ULIRGs using new,
previous... | astro-ph | luminous and ultraluminous infrared galaxies lirgs and ulirgs dominate the star formation rate budget of the universe at z 1 yet no local measurements of their heavy element abundances exist we measure nuclear or nearnuclear oxygen abundances in a sample of 100 starforming lirgs and ulirgs using new previously publishe... | [['luminous', 'and', 'ultraluminous', 'infrared', 'galaxies', 'lirgs', 'and', 'ulirgs', 'dominate', 'the', 'star', 'formation', 'rate', 'budget', 'of', 'the', 'universe', 'at', 'z', '1', 'yet', 'no', 'local', 'measurements', 'of', 'their', 'heavy', 'element', 'abundances', 'exist', 'we', 'measure', 'nuclear', 'or', 'ne... | [-0.004025402714883783, 0.09041751997678407, -0.05434210104828685, 0.12430968606832805, -0.04705883792216083, -0.0483681601178715, 0.06527890938925048, 0.48083047606364016, -0.10171419915844913, -0.32816156398058877, -0.002908575940415451, -0.3327008036137441, 0.01461122151510203, 0.15359843112250432, -0.01920626781677... |
708.1767 | Where, oh where has the r-process gone? | We present a review of the possible sources for r-process nuclei. It is known
that there is as yet no self-consistent mechanism to provide abundant neutrons
for a robust r-process in the neutrino-driven winds from nascent neutron stars.
We consider that the heavy r-nuclei with mass numbers A>130 (Ba and above)
cannot... | astro-ph | we present a review of the possible sources for rprocess nuclei it is known that there is as yet no selfconsistent mechanism to provide abundant neutrons for a robust rprocess in the neutrinodriven winds from nascent neutron stars we consider that the heavy rnuclei with mass numbers a130 ba and above cannot be produced... | [['we', 'present', 'a', 'review', 'of', 'the', 'possible', 'sources', 'for', 'rprocess', 'nuclei', 'it', 'is', 'known', 'that', 'there', 'is', 'as', 'yet', 'no', 'selfconsistent', 'mechanism', 'to', 'provide', 'abundant', 'neutrons', 'for', 'a', 'robust', 'rprocess', 'in', 'the', 'neutrinodriven', 'winds', 'from', 'nas... | [-0.027725981237095607, 0.21341039384875832, -0.018587820003544232, 0.14755193541367034, -0.07879317106083178, -0.11885820040871814, 0.09931426732158609, 0.3854050512971549, -0.1973356385304953, -0.3174444766736579, 0.00806307150728972, -0.327864869879523, 0.026811261759478584, 0.19273845544950216, -0.00891359799397240... |
708.1768 | Cryptanalysis of shifted conjugacy authentication protocol | In this paper we present the first practical attack on the shifted
conjugacy-based authentication protocol proposed by P. Dehornoy. We discuss the
weaknesses of that primitive and propose ways to improve the protocol.
| math.GR cs.CR | in this paper we present the first practical attack on the shifted conjugacybased authentication protocol proposed by p dehornoy we discuss the weaknesses of that primitive and propose ways to improve the protocol | [['in', 'this', 'paper', 'we', 'present', 'the', 'first', 'practical', 'attack', 'on', 'the', 'shifted', 'conjugacybased', 'authentication', 'protocol', 'proposed', 'by', 'p', 'dehornoy', 'we', 'discuss', 'the', 'weaknesses', 'of', 'that', 'primitive', 'and', 'propose', 'ways', 'to', 'improve', 'the', 'protocol']] | [-0.18273396842414513, -0.022410444857086986, -0.0787242547958158, 0.0011643525322142523, -0.04093842697329819, -0.20907379681011662, 0.14887174740579212, 0.3623304731445387, -0.2924684981117025, -0.27773284330032766, 0.05074994182723458, -0.18374649973702617, -0.22633302793838084, 0.15853158272511791, -0.1931068159756... |
708.1769 | Anomalously small wave tails in higher dimensions | We consider the late-time tails of spherical waves propagating on
even-dimensional Minkowski spacetime under the influence of a long range radial
potential. We show that in six and higher even dimensions there exist
exceptional potentials for which the tail has an anomalously small amplitude
and fast decay. Along the... | gr-qc | we consider the latetime tails of spherical waves propagating on evendimensional minkowski spacetime under the influence of a long range radial potential we show that in six and higher even dimensions there exist exceptional potentials for which the tail has an anomalously small amplitude and fast decay along the way w... | [['we', 'consider', 'the', 'latetime', 'tails', 'of', 'spherical', 'waves', 'propagating', 'on', 'evendimensional', 'minkowski', 'spacetime', 'under', 'the', 'influence', 'of', 'a', 'long', 'range', 'radial', 'potential', 'we', 'show', 'that', 'in', 'six', 'and', 'higher', 'even', 'dimensions', 'there', 'exist', 'excep... | [-0.1666039259101336, 0.1405864710939708, -0.0978675263432356, 0.12239148165457524, -0.05557123425488288, -0.1101703718662835, 0.011973783395324763, 0.41011434547030007, -0.18900280960907156, -0.22462341163593988, 0.09958440671459987, -0.2681253385801728, -0.15901929078480373, 0.16803232584721767, -0.040469587380245614... |
708.177 | Large rotating AdS black holes from fluid mechanics | We use the AdS/CFT correspondence to argue that large rotating black holes in
global AdS(D) spaces are dual to stationary solutions of the relativistic
Navier-Stokes equations on S**(D-2). Reading off the equation of state of this
fluid from the thermodynamics of non-rotating black holes, we proceed to
construct the ... | hep-th | we use the adscft correspondence to argue that large rotating black holes in global adsd spaces are dual to stationary solutions of the relativistic navierstokes equations on sd2 reading off the equation of state of this fluid from the thermodynamics of nonrotating black holes we proceed to construct the nonlinear spin... | [['we', 'use', 'the', 'adscft', 'correspondence', 'to', 'argue', 'that', 'large', 'rotating', 'black', 'holes', 'in', 'global', 'adsd', 'spaces', 'are', 'dual', 'to', 'stationary', 'solutions', 'of', 'the', 'relativistic', 'navierstokes', 'equations', 'on', 'sd2', 'reading', 'off', 'the', 'equation', 'of', 'state', 'of... | [-0.12985044612648822, 0.10609659659764115, -0.04599120836915835, 0.16027778794157244, -0.053932634652328656, -0.14640271076244307, -0.033937560220149425, 0.25555567221962056, -0.13375031608654736, -0.2591422870228032, 0.11564510081654543, -0.36147990199567387, -0.07885499121679825, 0.17412871779411235, -0.087698873119... |
708.1771 | Specific Angular Momentum of Extrasolar Planetary Systems | As the number of known planetary systems increases, the ability to follow-up
and characterize the extent of any system becomes limited. This paper considers
the use of specific angular momentum as a metric to prioritize future
observations. We analyze 431 planets in 367 known extrasolar planetary systems
from Butler ... | astro-ph | as the number of known planetary systems increases the ability to followup and characterize the extent of any system becomes limited this paper considers the use of specific angular momentum as a metric to prioritize future observations we analyze 431 planets in 367 known extrasolar planetary systems from butler et al ... | [['as', 'the', 'number', 'of', 'known', 'planetary', 'systems', 'increases', 'the', 'ability', 'to', 'followup', 'and', 'characterize', 'the', 'extent', 'of', 'any', 'system', 'becomes', 'limited', 'this', 'paper', 'considers', 'the', 'use', 'of', 'specific', 'angular', 'momentum', 'as', 'a', 'metric', 'to', 'prioritiz... | [-0.15930538319091322, 0.10297909339699614, -0.037758286073503476, 0.07391611013751757, -0.1322816454878037, -0.07519416665778525, 0.04502818637880527, 0.32294963587636266, -0.19606833723348677, -0.4061826217283685, 0.06890368632163592, -0.29557131486444144, -0.08707122577470727, 0.215941010268345, -0.08563390308089795... |
708.1772 | Abelian duality, confinement, and chiral symmetry breaking in QCD(adj) | We analyze the vacuum structure of SU(2) QCD with multiple massless adjoint
representation fermions formulated on a small spatial $S^1 \times \R^3$. The
absence of thermal fluctuations, and the fact that quantum fluctuations
favoring the vacuum with unbroken center symmetry in a weakly coupled regime
renders the inte... | hep-th hep-lat hep-ph | we analyze the vacuum structure of su2 qcd with multiple massless adjoint representation fermions formulated on a small spatial s1 times r3 the absence of thermal fluctuations and the fact that quantum fluctuations favoring the vacuum with unbroken center symmetry in a weakly coupled regime renders the interesting dyna... | [['we', 'analyze', 'the', 'vacuum', 'structure', 'of', 'su2', 'qcd', 'with', 'multiple', 'massless', 'adjoint', 'representation', 'fermions', 'formulated', 'on', 'a', 'small', 'spatial', 's1', 'times', 'r3', 'the', 'absence', 'of', 'thermal', 'fluctuations', 'and', 'the', 'fact', 'that', 'quantum', 'fluctuations', 'fav... | [-0.20492766250598443, 0.27910658938769, -0.08790600760507264, 0.09190276475246287, -0.04677179170262423, -0.15944327945388587, -0.0021296581981005147, 0.3563842882258108, -0.19720287007069037, -0.2169341009797617, 0.06176563767768953, -0.24707484415349817, -0.09313262973557271, 0.013890569436452574, 0.0142814494268220... |
708.1773 | Homotopy Lie Superalgebra in Yang-Mills Theory | The Yang-Mills equations are formulated in the form of generalized
Maurer-Cartan equations, such that the corresponding algebraic operations are
shown to satisfy the defining relations of homotopy Lie superalgebra.
| hep-th math-ph math.MP math.QA | the yangmills equations are formulated in the form of generalized maurercartan equations such that the corresponding algebraic operations are shown to satisfy the defining relations of homotopy lie superalgebra | [['the', 'yangmills', 'equations', 'are', 'formulated', 'in', 'the', 'form', 'of', 'generalized', 'maurercartan', 'equations', 'such', 'that', 'the', 'corresponding', 'algebraic', 'operations', 'are', 'shown', 'to', 'satisfy', 'the', 'defining', 'relations', 'of', 'homotopy', 'lie', 'superalgebra']] | [-0.21144176190638722, 0.07679044311978565, -0.06785710798255329, 0.11604132284892016, -0.16867441142877115, -0.12305621780326655, -0.12355706320497496, 0.24259078374196744, -0.36482638364721987, -0.236314434493924, 0.08702682871933512, -0.22936991300305415, -0.21445079642380105, 0.14880471445363144, -0.101817752122236... |
708.1774 | Localization for Schrodinger operators with random vector potentials | We prove Anderson localization at the internal band-edges for periodic
magnetic Schr{\"o}dinger operators perturbed by random vector potentials of
Anderson-type. This is achieved by combining new results on the Lifshitz tails
behavior of the integrated density of states for random magnetic
Schr{\"o}dinger operators, ... | math-ph math.MP math.SP | we prove anderson localization at the internal bandedges for periodic magnetic schrodinger operators perturbed by random vector potentials of andersontype this is achieved by combining new results on the lifshitz tails behavior of the integrated density of states for random magnetic schrodinger operators thereby provid... | [['we', 'prove', 'anderson', 'localization', 'at', 'the', 'internal', 'bandedges', 'for', 'periodic', 'magnetic', 'schrodinger', 'operators', 'perturbed', 'by', 'random', 'vector', 'potentials', 'of', 'andersontype', 'this', 'is', 'achieved', 'by', 'combining', 'new', 'results', 'on', 'the', 'lifshitz', 'tails', 'behav... | [-0.12979149531539796, 0.19245747871796734, -0.05102967789363382, 0.0946482087851369, 0.0005077747544938964, -0.14781057900316746, 0.014847585669485852, 0.35599838716111015, -0.2343248658414398, -0.24071747467054852, 0.062282275633021654, -0.3037741239448743, -0.12388839285995346, 0.18086467939428985, 0.031897538433051... |
708.1775 | The Molecular Gas Environment around Two Herbig Ae/Be Stars: Resolving
the Outflows of LkHa 198 and LkHa 225S | Observations of outflows associated with pre-main-sequence stars reveal
details about morphology, binarity and evolutionary states of young stellar
objects. We present molecular line data from the Berkeley-Illinois-Maryland
Association array and Five Colleges Radio Astronomical Observatory toward the
regions containi... | astro-ph | observations of outflows associated with premainsequence stars reveal details about morphology binarity and evolutionary states of young stellar objects we present molecular line data from the berkeleyillinoismaryland association array and five colleges radio astronomical observatory toward the regions containing the h... | [['observations', 'of', 'outflows', 'associated', 'with', 'premainsequence', 'stars', 'reveal', 'details', 'about', 'morphology', 'binarity', 'and', 'evolutionary', 'states', 'of', 'young', 'stellar', 'objects', 'we', 'present', 'molecular', 'line', 'data', 'from', 'the', 'berkeleyillinoismaryland', 'association', 'arr... | [-0.08100136059280628, 0.05132941791162292, 0.02788957959026616, 0.0013532192265600484, -0.05777534598243714, -0.09970226504234957, 0.08107600915047941, 0.4967207265550335, -0.15292237814997672, -0.35884109745071807, 0.10542125194594192, -0.2941619572103829, 0.035629001070303, 0.1518239215713958, -0.010889179249695038,... |
708.1776 | Spectra of random linear combinations of matrices defined via
representations and Coxeter generators of the symmetric group | We consider the asymptotic behavior as $n\to\infty$ of the spectra of random
matrices of the form \[\frac{1}{\sqrt{n-1}}\sum_{k=1}^{n-1}Z_{nk}\rho_n
((k,k+1)),\] where for each $n$ the random variables $Z_{nk}$ are i.i.d.
standard Gaussian and the matrices $\rho_n((k,k+1))$ are obtained by applying
an irreducible uni... | math.PR math.RT | we consider the asymptotic behavior as ntoinfty of the spectra of random matrices of the form frac1sqrtn1sum_k1n1z_nkrho_n kk1 where for each n the random variables z_nk are iid standard gaussian and the matrices rho_nkk1 are obtained by applying an irreducible unitary representation rho_n of the symmetric group on 12n... | [['we', 'consider', 'the', 'asymptotic', 'behavior', 'as', 'ntoinfty', 'of', 'the', 'spectra', 'of', 'random', 'matrices', 'of', 'the', 'form', 'frac1sqrtn1sum_k1n1z_nkrho_n', 'kk1', 'where', 'for', 'each', 'n', 'the', 'random', 'variables', 'z_nk', 'are', 'iid', 'standard', 'gaussian', 'and', 'the', 'matrices', 'rho_n... | [-0.1290055209760032, 0.21911266633934232, -0.07521694678156449, 0.0075673135105154415, -0.014235441817907412, -0.1508139262939507, 0.044155166977666575, 0.35621491724872867, -0.26560731178332614, -0.19213980517075585, 0.1010294535023704, -0.3274058314374072, -0.12152708180159912, 0.09589710260870614, -0.02412424925539... |
708.1777 | Electronic Ground State of Higher Acenes | We examine the electronic ground state of acenes with different number of
fused benzene rings (up to 40) by using first principles density functional
theory. Their properties are compared with those of infinite polyacene. We find
that the ground state of acenes that consist of more than seven fused benzene
rings is a... | physics.chem-ph physics.comp-ph | we examine the electronic ground state of acenes with different number of fused benzene rings up to 40 by using first principles density functional theory their properties are compared with those of infinite polyacene we find that the ground state of acenes that consist of more than seven fused benzene rings is an anti... | [['we', 'examine', 'the', 'electronic', 'ground', 'state', 'of', 'acenes', 'with', 'different', 'number', 'of', 'fused', 'benzene', 'rings', 'up', 'to', '40', 'by', 'using', 'first', 'principles', 'density', 'functional', 'theory', 'their', 'properties', 'are', 'compared', 'with', 'those', 'of', 'infinite', 'polyacene'... | [-0.12852924484609357, 0.18409931477510072, -0.014312603606051334, 0.04299527823096341, 0.01163999509799885, -0.13115348932095452, 0.018777439594819582, 0.4379144049880485, -0.23883183640227604, -0.2956727907995403, 0.029516879405941495, -0.34374803238578383, -0.06397510547521373, 0.12969356755787376, 0.062866513060295... |
708.1778 | Pressure-Tuned Spin and Charge Ordering in an Itinerant Antiferromagnet | Elemental chromium orders antiferromagnetically near room temperature, but
the ordering temperature can be driven to zero by applying large pressures. We
combine diamond anvil cell and synchrotron x-ray diffraction techniques to
measure directly the spin and charge order in the pure metal at the approach to
its quant... | cond-mat.str-el | elemental chromium orders antiferromagnetically near room temperature but the ordering temperature can be driven to zero by applying large pressures we combine diamond anvil cell and synchrotron xray diffraction techniques to measure directly the spin and charge order in the pure metal at the approach to its quantum cr... | [['elemental', 'chromium', 'orders', 'antiferromagnetically', 'near', 'room', 'temperature', 'but', 'the', 'ordering', 'temperature', 'can', 'be', 'driven', 'to', 'zero', 'by', 'applying', 'large', 'pressures', 'we', 'combine', 'diamond', 'anvil', 'cell', 'and', 'synchrotron', 'xray', 'diffraction', 'techniques', 'to',... | [-0.09303405669071396, 0.25038626388077095, -0.030121350075957204, 0.038344558752680676, -0.03173998124851299, -0.09272024530748074, 0.09978080859931171, 0.4113391960416882, -0.31709532686778585, -0.3002613382875796, 0.04648654640571422, -0.34143465782000015, -0.05302704693672578, 0.1477182767669524, 0.0727963379778118... |
708.1779 | Twisted Poincar\'e Invariant Quantum Field Theories | It is by now well known that the Poincar\'e group acts on the Moyal plane
with a twisted coproduct. Poincar\'e invariant classical field theories can be
formulated for this twisted coproduct. In this paper we systematically study
such a twisted Poincar\'e action in quantum theories on the Moyal plane. We
develop quan... | hep-th math-ph math.MP math.QA | it is by now well known that the poincare group acts on the moyal plane with a twisted coproduct poincare invariant classical field theories can be formulated for this twisted coproduct in this paper we systematically study such a twisted poincare action in quantum theories on the moyal plane we develop quantum field t... | [['it', 'is', 'by', 'now', 'well', 'known', 'that', 'the', 'poincare', 'group', 'acts', 'on', 'the', 'moyal', 'plane', 'with', 'a', 'twisted', 'coproduct', 'poincare', 'invariant', 'classical', 'field', 'theories', 'can', 'be', 'formulated', 'for', 'this', 'twisted', 'coproduct', 'in', 'this', 'paper', 'we', 'systemati... | [-0.18930908029800966, 0.17782466939993594, -0.15066322188236211, 0.07400299044031845, -0.09427633809023782, -0.06782104295041216, -0.026352812081428343, 0.3342415447297849, -0.29905658403509544, -0.21778759456386693, 0.10458232087303737, -0.1735897467716744, -0.22277709473120538, 0.1773374178226253, -0.116653091382039... |
708.178 | Two-particle scattering on the lattice: Phase shifts, spin-orbit
coupling, and mixing angles | We determine two-particle scattering phase shifts and mixing angles for
quantum theories defined with lattice regularization. The method is suitable
for any nonrelativistic effective theory of point particles on the lattice. In
the center-of-mass frame of the two-particle system we impose a hard spherical
wall at som... | nucl-th hep-lat physics.atom-ph | we determine twoparticle scattering phase shifts and mixing angles for quantum theories defined with lattice regularization the method is suitable for any nonrelativistic effective theory of point particles on the lattice in the centerofmass frame of the twoparticle system we impose a hard spherical wall at some fixed ... | [['we', 'determine', 'twoparticle', 'scattering', 'phase', 'shifts', 'and', 'mixing', 'angles', 'for', 'quantum', 'theories', 'defined', 'with', 'lattice', 'regularization', 'the', 'method', 'is', 'suitable', 'for', 'any', 'nonrelativistic', 'effective', 'theory', 'of', 'point', 'particles', 'on', 'the', 'lattice', 'in... | [-0.14589977968108855, 0.26125721401048896, -0.0874018822879176, 0.03541258944167214, -0.030151982802147075, -0.13198212118221642, 0.021203470990624723, 0.37871372894342265, -0.26069934874314316, -0.21972047489435315, 0.04714403909530296, -0.2909334254339893, -0.06434869062009532, 0.13345793616582655, 0.083059227961956... |
708.1781 | Effects of pyruvate administration on infarct volume and neurological
deficits following permanent focal cerebral ischemia in rats | Recent experimental evidences indicate that pyruvate, the final metabolite of
glycolysis, has a remarkable protective effect against different types of brain
injury. The purpose of this study was to assess the neuroprotective effect and
the neurological outcome after pyruvate administration in a model of ischemic
str... | q-bio.TO | recent experimental evidences indicate that pyruvate the final metabolite of glycolysis has a remarkable protective effect against different types of brain injury the purpose of this study was to assess the neuroprotective effect and the neurological outcome after pyruvate administration in a model of ischemic stroke i... | [['recent', 'experimental', 'evidences', 'indicate', 'that', 'pyruvate', 'the', 'final', 'metabolite', 'of', 'glycolysis', 'has', 'a', 'remarkable', 'protective', 'effect', 'against', 'different', 'types', 'of', 'brain', 'injury', 'the', 'purpose', 'of', 'this', 'study', 'was', 'to', 'assess', 'the', 'neuroprotective',... | [-0.04297750138714179, 0.16618259336032412, 0.006931492223349565, 0.05931580084599737, 0.041339034541035255, -0.1458618399235146, 0.08980239710716904, 0.38342307151897864, -0.14259876353853365, -0.3149420499502608, 0.12379625905761678, -0.2966969700658, -0.2030396744992365, 0.17399640593223512, -0.1799477502853751, -0.... |
708.1782 | Ruthenium and hafnium abundances in giant and dwarf barium stars | We present abundances for Ru and Hf, compare them to abundances of other
heavy elements, and discuss the problems found in determining Ru and Hf
abundances with laboratory gf-values in the spectra of barium stars. We
determined Ru and Hf abundances in a sample of giant and dwarf barium stars, by
the spectral synthesi... | astro-ph | we present abundances for ru and hf compare them to abundances of other heavy elements and discuss the problems found in determining ru and hf abundances with laboratory gfvalues in the spectra of barium stars we determined ru and hf abundances in a sample of giant and dwarf barium stars by the spectral synthesis of tw... | [['we', 'present', 'abundances', 'for', 'ru', 'and', 'hf', 'compare', 'them', 'to', 'abundances', 'of', 'other', 'heavy', 'elements', 'and', 'discuss', 'the', 'problems', 'found', 'in', 'determining', 'ru', 'and', 'hf', 'abundances', 'with', 'laboratory', 'gfvalues', 'in', 'the', 'spectra', 'of', 'barium', 'stars', 'we... | [-0.0030925508486433773, 0.16217430507960287, 0.038029024316806735, 0.09705181272471683, 0.022556640140369143, -0.11144796700069778, 0.10984869984983417, 0.4129037434398605, -0.17896130173058625, -0.39638545562496835, -0.03574452871750844, -0.3717943810318646, -0.0069208083020751935, 0.15020140455382175, -0.04557034412... |
708.1783 | Constraints on the value of the fine structure constant from
gravitational thermodynamics | In this paper I show how the second law of thermodynamics, generalized to
include event horizon area, places interesting constraints on the value of the
fine structure constant. A simple analysis leads to the conclusion that
classical Dirac and point-like magnetic monopoles could be used to violate the
second law, an... | gr-qc | in this paper i show how the second law of thermodynamics generalized to include event horizon area places interesting constraints on the value of the fine structure constant a simple analysis leads to the conclusion that classical dirac and pointlike magnetic monopoles could be used to violate the second law and that ... | [['in', 'this', 'paper', 'i', 'show', 'how', 'the', 'second', 'law', 'of', 'thermodynamics', 'generalized', 'to', 'include', 'event', 'horizon', 'area', 'places', 'interesting', 'constraints', 'on', 'the', 'value', 'of', 'the', 'fine', 'structure', 'constant', 'a', 'simple', 'analysis', 'leads', 'to', 'the', 'conclusio... | [-0.11206553375715453, 0.16387382479605533, -0.10794333161754628, 0.14280962307692774, -0.1686742819403693, -0.15188220401405025, 0.05187613062039649, 0.29726844997603, -0.22175845978939432, -0.35792919999714623, 0.0754204670488203, -0.28203562509773644, -0.11177862864934791, 0.145662371574317, -0.08458350873473337, -6... |
708.1784 | The Higgs portal and an unified model for dark energy and dark matter | We examine a scenario where the Higgs boson is coupled to an additional
singlet scalar field which we identify with a quintessence field. We show that
this results in an unified picture of dark matter and dark energy, where dark
energy is the zero-mode classical field rolling the usual quintessence
potential and the ... | hep-ph astro-ph | we examine a scenario where the higgs boson is coupled to an additional singlet scalar field which we identify with a quintessence field we show that this results in an unified picture of dark matter and dark energy where dark energy is the zeromode classical field rolling the usual quintessence potential and the dark ... | [['we', 'examine', 'a', 'scenario', 'where', 'the', 'higgs', 'boson', 'is', 'coupled', 'to', 'an', 'additional', 'singlet', 'scalar', 'field', 'which', 'we', 'identify', 'with', 'a', 'quintessence', 'field', 'we', 'show', 'that', 'this', 'results', 'in', 'an', 'unified', 'picture', 'of', 'dark', 'matter', 'and', 'dark'... | [-0.14724308187858418, 0.20710363810716304, -0.13172241721230632, 0.1380535108380569, -0.12573577851677933, -0.15230804293726882, -0.052396042908255294, 0.2860671886577247, -0.22555793372269434, -0.32580360123075736, -0.03542736206257429, -0.2185160696076659, -0.04817326276157147, 0.10201168541038313, 0.032283177981391... |
708.1785 | Electroweak phase transition in MSSM with $U(1)'$ in explicit CP
violation scenario | The possibility of a strongly first-order electroweak phase transition is
established in the minimal supersymmetric standard model with an extra $U(1)'$,
where a nontrivial CP violating phase is introduced in its Higgs sector. We
find that there is a wide region in the parameter space of the model that
allows the str... | hep-ph | the possibility of a strongly firstorder electroweak phase transition is established in the minimal supersymmetric standard model with an extra u1 where a nontrivial cp violating phase is introduced in its higgs sector we find that there is a wide region in the parameter space of the model that allows the strongly firs... | [['the', 'possibility', 'of', 'a', 'strongly', 'firstorder', 'electroweak', 'phase', 'transition', 'is', 'established', 'in', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'with', 'an', 'extra', 'u1', 'where', 'a', 'nontrivial', 'cp', 'violating', 'phase', 'is', 'introduced', 'in', 'its', 'higgs', 'sector', ... | [-0.14118974339618956, 0.3176099870517463, -0.037392648754360006, 0.08787796005653553, -0.09350520121469665, -0.16159903408503898, 0.11566462013334465, 0.282224049307607, -0.21876437757700254, -0.26949475101268977, 0.06189215864245813, -0.241172044777597, -0.08701858592802565, 0.08265484091088765, 0.05498137499734244, ... |
708.1786 | Bound on the anomalous tbW coupling from two-loop contribution to
neutron electric dipole moment | The two-loop contribution to the electric dipole moment (EDM) and the chromo
electric dipole moment (CEDM) of an arbitrary fermion f induced by the most
general renormalizable tbW coupling with complex left- and right-handed
components (a_L and a_R) is calculated. The analytical expressions are
numerically evaluated ... | hep-ph | the twoloop contribution to the electric dipole moment edm and the chromo electric dipole moment cedm of an arbitrary fermion f induced by the most general renormalizable tbw coupling with complex left and righthanded components a_l and a_r is calculated the analytical expressions are numerically evaluated and the curr... | [['the', 'twoloop', 'contribution', 'to', 'the', 'electric', 'dipole', 'moment', 'edm', 'and', 'the', 'chromo', 'electric', 'dipole', 'moment', 'cedm', 'of', 'an', 'arbitrary', 'fermion', 'f', 'induced', 'by', 'the', 'most', 'general', 'renormalizable', 'tbw', 'coupling', 'with', 'complex', 'left', 'and', 'righthanded'... | [-0.14334590164833658, 0.2413235215674268, 0.03774161413977189, 0.12581684763011122, -0.08758784805069722, -0.11215651217692842, 0.01301761770515614, 0.2988338356039354, -0.19053004107471289, -0.3061589970076013, 0.005500840932308208, -0.3317473482429272, -0.044415037286290454, 0.19221031794413215, 0.09261244419030845,... |
708.1787 | Supernova SN2006gy as a first ever Quark Nova? | The most luminous Supernova SN2006gy (more than a 100 times brighter than a
typical supernova) has been a challenge to explain by standard models. For
example, pair instability supernovae which are luminous enough seem to have too
slow a rise, and core collapse supernovae do not seem to be luminous enough. We
present... | astro-ph | the most luminous supernova sn2006gy more than a 100 times brighter than a typical supernova has been a challenge to explain by standard models for example pair instability supernovae which are luminous enough seem to have too slow a rise and core collapse supernovae do not seem to be luminous enough we present an alte... | [['the', 'most', 'luminous', 'supernova', 'sn2006gy', 'more', 'than', 'a', '100', 'times', 'brighter', 'than', 'a', 'typical', 'supernova', 'has', 'been', 'a', 'challenge', 'to', 'explain', 'by', 'standard', 'models', 'for', 'example', 'pair', 'instability', 'supernovae', 'which', 'are', 'luminous', 'enough', 'seem', '... | [-0.03722125118320736, 0.141422374474272, -0.08752724459060492, 0.1588423135130702, -0.1562773697749855, -0.1200450413281289, 0.056278566210471, 0.38645226500617963, -0.15975775300802736, -0.2918241647287057, 0.08940374148108113, -0.28323482329310185, -0.053195786668369785, 0.22229153128540555, -0.03239992053484177, -0... |
708.1788 | Reionization Bias in High Redshift Quasar Near-Zones | Absorption spectra of high redshift quasars exhibit an increasingly thick
Ly-alpha forest towards z~6. However, the interpretation of these spectra is
complicated by the fact that the Ly-alpha optical depth is already large for
neutral hydrogen fractions in excess of 10^-4, and also because quasars are
expected to re... | astro-ph | absorption spectra of high redshift quasars exhibit an increasingly thick lyalpha forest towards z6 however the interpretation of these spectra is complicated by the fact that the lyalpha optical depth is already large for neutral hydrogen fractions in excess of 104 and also because quasars are expected to reside in de... | [['absorption', 'spectra', 'of', 'high', 'redshift', 'quasars', 'exhibit', 'an', 'increasingly', 'thick', 'lyalpha', 'forest', 'towards', 'z6', 'however', 'the', 'interpretation', 'of', 'these', 'spectra', 'is', 'complicated', 'by', 'the', 'fact', 'that', 'the', 'lyalpha', 'optical', 'depth', 'is', 'already', 'large', ... | [-0.00838942549087043, 0.17020799577615528, -0.001456204524006823, 0.0713032124082333, -0.018671197895410246, -0.04096888051496755, 0.05024932963163432, 0.42464734069232285, -0.16324057541065046, -0.318902014048192, 0.02731281114894704, -0.3083972623764441, -0.0028868481700744177, 0.16629369303921301, 0.023933045728078... |
708.1789 | Extensions of McCoy Rings | A ring $R$ is said to be right McCoy if the equation $f(x)g(x)=0,$ where
$f(x)$ and $g(x)$ are nonzero polynomials of $R[x],$ implies that there exists
nonzero $s \in R$ such that $f(x)s = 0$. It is proven that no proper
(triangular) matrix ring is one-sided McCoy. If there exists the classical
right quotient ring $Q... | math.RA | a ring r is said to be right mccoy if the equation fxgx0 where fx and gx are nonzero polynomials of rx implies that there exists nonzero s in r such that fxs 0 it is proven that no proper triangular matrix ring is onesided mccoy if there exists the classical right quotient ring q of a ring r then r is right mccoy if an... | [['a', 'ring', 'r', 'is', 'said', 'to', 'be', 'right', 'mccoy', 'if', 'the', 'equation', 'fxgx0', 'where', 'fx', 'and', 'gx', 'are', 'nonzero', 'polynomials', 'of', 'rx', 'implies', 'that', 'there', 'exists', 'nonzero', 's', 'in', 'r', 'such', 'that', 'fxs', '0', 'it', 'is', 'proven', 'that', 'no', 'proper', 'triangula... | [-0.2289376369112038, 0.03339910003192285, -0.05303495229777543, 0.012335930140923802, -0.08531716001462661, -0.3286197158633223, -0.138889746662198, 0.38841561642827604, -0.4305234537655566, -0.011344743802548707, 0.1696619572227492, -0.3059227930835816, -0.1004761200116462, 0.16316584305164694, -0.06302395773887196, ... |
708.179 | Observation of a resonance-like structure in the pi^+- psi' mass
distribution in exclusive B-->K pi^+- psi' decays | A distinct peak is observed in the pi^+/- psi' invariant mass distribution
near 4.43 GeV in B->K pi^+/- psi' decays. A fit using a Breit Wigner resonance
shape yields a peak mass and width of 4433+-4(stat)+-2(syst) MeV and Gamma =
45^+18_-13(stat) ^+30_-13 MeV. The product branching fraction is determined to
be Bf(B-... | hep-ex | a distinct peak is observed in the pi psi invariant mass distribution near 443 gev in bk pi psi decays a fit using a breit wigner resonance shape yields a peak mass and width of 44334stat2syst mev and gamma 4518_13stat 30_13 mev the product branching fraction is determined to be bfbkz4430xbfz4430pipsi 4110stat14systx10... | [['a', 'distinct', 'peak', 'is', 'observed', 'in', 'the', 'pi', 'psi', 'invariant', 'mass', 'distribution', 'near', '443', 'gev', 'in', 'bk', 'pi', 'psi', 'decays', 'a', 'fit', 'using', 'a', 'breit', 'wigner', 'resonance', 'shape', 'yields', 'a', 'peak', 'mass', 'and', 'width', 'of', '44334stat2syst', 'mev', 'and', 'ga... | [-0.08065222735461519, 0.17423187553181707, -0.10461156523412037, 0.11657421289914355, -0.0652729634780043, -0.11446724604087949, 0.049290687101413065, 0.34823939177332464, -0.1728879482744588, -0.31330427942202266, -0.08272986460870765, -0.4487516355182323, 0.08553943583338532, 0.17182502008676914, 0.10400989963721062... |
708.1791 | Load fluctuations drive actin network growth | The growth of actin filament networks is a fundamental biological process
that drives a variety of cellular and intracellular motions. During motility,
eukaryotic cells and intracellular pathogens are propelled by actin networks
organized by nucleation-promoting factors, which trigger the formation of
nascent filamen... | physics.bio-ph | the growth of actin filament networks is a fundamental biological process that drives a variety of cellular and intracellular motions during motility eukaryotic cells and intracellular pathogens are propelled by actin networks organized by nucleationpromoting factors which trigger the formation of nascent filaments off... | [['the', 'growth', 'of', 'actin', 'filament', 'networks', 'is', 'a', 'fundamental', 'biological', 'process', 'that', 'drives', 'a', 'variety', 'of', 'cellular', 'and', 'intracellular', 'motions', 'during', 'motility', 'eukaryotic', 'cells', 'and', 'intracellular', 'pathogens', 'are', 'propelled', 'by', 'actin', 'networ... | [-0.13230968246866456, 0.22276726527035892, -0.02483973470964733, -0.03784873359862902, -0.0200682090757848, -0.12190109283170279, 0.0244596244600467, 0.42933481115876465, -0.30192041155050464, -0.2209398873588618, 0.027775751276783407, -0.23909960966308247, -0.21123768584454122, 0.14554987391357355, -0.032229084202790... |
708.1792 | Radiative Column and Light Curve of X-Ray Binary Pulsars | We examine the published light curves (LCs) of 117 X-ray binary pulsars,
focusing on the dependence of their light curves on the observed energy bands.
It is found that the energy dependence of the LCs appears only when the X-ray
luminosity is larger than ~ 5 x 10^36 erg/s. Assuming that the behavior of
light curve i... | astro-ph | we examine the published light curves lcs of 117 xray binary pulsars focusing on the dependence of their light curves on the observed energy bands it is found that the energy dependence of the lcs appears only when the xray luminosity is larger than 5 x 1036 ergs assuming that the behavior of light curve is related to ... | [['we', 'examine', 'the', 'published', 'light', 'curves', 'lcs', 'of', '117', 'xray', 'binary', 'pulsars', 'focusing', 'on', 'the', 'dependence', 'of', 'their', 'light', 'curves', 'on', 'the', 'observed', 'energy', 'bands', 'it', 'is', 'found', 'that', 'the', 'energy', 'dependence', 'of', 'the', 'lcs', 'appears', 'only... | [-0.10672001322543817, 0.13481884379719608, -0.09111861453695586, 0.1417324062357592, -0.10943333104892695, -0.056276665095032916, 0.05266620144053983, 0.41864995249650544, -0.225254111150409, -0.35744882518580806, 0.10418050747587888, -0.28225442318620886, -0.04814769757407097, 0.23891990177152264, -0.0211139981078708... |
708.1793 | A sub-horizon framework for probing the relationship between the
cosmological matter distribution and metric perturbations | The relationship between the metric and nonrelativistic matter distribution
depends on the theory of gravity and additional fields, providing a possible
way of distinguishing competing theories. With the assumption that the geometry
and kinematics of the homogeneous universe have been measured to sufficient
accuracy,... | astro-ph gr-qc | the relationship between the metric and nonrelativistic matter distribution depends on the theory of gravity and additional fields providing a possible way of distinguishing competing theories with the assumption that the geometry and kinematics of the homogeneous universe have been measured to sufficient accuracy we p... | [['the', 'relationship', 'between', 'the', 'metric', 'and', 'nonrelativistic', 'matter', 'distribution', 'depends', 'on', 'the', 'theory', 'of', 'gravity', 'and', 'additional', 'fields', 'providing', 'a', 'possible', 'way', 'of', 'distinguishing', 'competing', 'theories', 'with', 'the', 'assumption', 'that', 'the', 'ge... | [-0.12013412417055895, 0.0981520183063157, -0.135527490288055, 0.10625854949825085, -0.1134920865118217, -0.11913540157167098, -0.01585876080297077, 0.3059649628533337, -0.2194151459942357, -0.3216692408725906, 0.05318976918016023, -0.24633231059818242, -0.10853899891058413, 0.16587037151822678, 0.005423645911594996, 0... |
708.1794 | Systems level circuit model of C. elegans undulatory locomotion:
mathematical modeling and molecular genetics | To establish the relationship between locomotory behavior and dynamics of
neural circuits in the nematode C. elegans we combined molecular and
theoretical approaches. In particular, we quantitatively analyzed the motion of
C. elegans with defective synaptic GABA and acetylcholine transmission,
defective muscle calciu... | q-bio.NC q-bio.GN | to establish the relationship between locomotory behavior and dynamics of neural circuits in the nematode c elegans we combined molecular and theoretical approaches in particular we quantitatively analyzed the motion of c elegans with defective synaptic gaba and acetylcholine transmission defective muscle calcium signa... | [['to', 'establish', 'the', 'relationship', 'between', 'locomotory', 'behavior', 'and', 'dynamics', 'of', 'neural', 'circuits', 'in', 'the', 'nematode', 'c', 'elegans', 'we', 'combined', 'molecular', 'and', 'theoretical', 'approaches', 'in', 'particular', 'we', 'quantitatively', 'analyzed', 'the', 'motion', 'of', 'c', ... | [-0.1250924926547596, 0.11530291030163177, -0.0032162708589306616, -0.017957087431825072, -0.06587483562192663, -0.20541255730270955, 0.06869003395211477, 0.4193747511240223, -0.2646546923936989, -0.22851093763707098, 0.03928555838870385, -0.2695094720749718, -0.2331490805988007, 0.1776555691382105, -0.0544219618952435... |
708.1795 | Suppression of spin-polarization in graphene nanoribbon by edge defect
and impurity | We investigate the effect of edge defects (vacancies) and impurities
(substitutional dopants) on the robustness of spin-polarization in graphene
nanoribbons (GNRs) with zigzag edges, using density-functional-theory
calculations. We found that the stability of the spin state and its magnetic
moments decrease continuou... | cond-mat.mtrl-sci | we investigate the effect of edge defects vacancies and impurities substitutional dopants on the robustness of spinpolarization in graphene nanoribbons gnrs with zigzag edges using densityfunctionaltheory calculations we found that the stability of the spin state and its magnetic moments decrease continuously with incr... | [['we', 'investigate', 'the', 'effect', 'of', 'edge', 'defects', 'vacancies', 'and', 'impurities', 'substitutional', 'dopants', 'on', 'the', 'robustness', 'of', 'spinpolarization', 'in', 'graphene', 'nanoribbons', 'gnrs', 'with', 'zigzag', 'edges', 'using', 'densityfunctionaltheory', 'calculations', 'we', 'found', 'tha... | [-0.150945325846515, 0.17999527652489294, 0.028257384032164653, 0.020919456519906593, 0.06961069614014387, -0.15458262900428213, 0.11147971347588853, 0.4336658391583058, -0.26563052808117005, -0.31365472548785284, -0.0031959382281878715, -0.40562777399786354, -0.09976592050029982, 0.0812245397924532, 0.0210612032816927... |
708.1796 | The Infrared Astronomical Mission AKARI | AKARI, the first Japanese satellite dedicated to infrared astronomy, was
launched on 2006 February 21, and started observations in May of the same year.
AKARI has a 68.5 cm cooled telescope, together with two focal-plane
instruments, which survey the sky in six wavelength bands from the mid- to
far-infrared. The inst... | astro-ph | akari the first japanese satellite dedicated to infrared astronomy was launched on 2006 february 21 and started observations in may of the same year akari has a 685 cm cooled telescope together with two focalplane instruments which survey the sky in six wavelength bands from the mid to farinfrared the instruments also ... | [['akari', 'the', 'first', 'japanese', 'satellite', 'dedicated', 'to', 'infrared', 'astronomy', 'was', 'launched', 'on', '2006', 'february', '21', 'and', 'started', 'observations', 'in', 'may', 'of', 'the', 'same', 'year', 'akari', 'has', 'a', '685', 'cm', 'cooled', 'telescope', 'together', 'with', 'two', 'focalplane',... | [-0.060294086331495925, 0.09903717270589835, -0.08646413121548505, 0.04391932120424605, -0.13405716721615868, -0.03327302926038278, 0.04438507957838294, 0.4332232828331521, -0.18015162684321517, -0.3637886432073329, 0.1843411442809511, -0.3591453788103536, -0.005791967388287913, 0.2476403369588164, -0.03900981862552282... |
708.1797 | Flight Performance of the AKARI Cryogenic System | We describe the flight performance of the cryogenic system of the infrared
astronomical satellite AKARI, which was successfully launched on 2006 February
21 (UT). AKARI carries a 68.5 cm telescope together with two focal plane
instruments, Infrared Cameras (IRC) and Far Infrared Surveyor (FIS), all of
which are coole... | astro-ph | we describe the flight performance of the cryogenic system of the infrared astronomical satellite akari which was successfully launched on 2006 february 21 ut akari carries a 685 cm telescope together with two focal plane instruments infrared cameras irc and far infrared surveyor fis all of which are cooled down to cry... | [['we', 'describe', 'the', 'flight', 'performance', 'of', 'the', 'cryogenic', 'system', 'of', 'the', 'infrared', 'astronomical', 'satellite', 'akari', 'which', 'was', 'successfully', 'launched', 'on', '2006', 'february', '21', 'ut', 'akari', 'carries', 'a', '685', 'cm', 'telescope', 'together', 'with', 'two', 'focal', ... | [-0.0991877763756091, 0.17893864269828116, -0.07655681982707185, -0.02865041960513402, -0.0562570009327529, -0.11007165807576355, 0.029644901784655602, 0.37132412087337313, -0.17653174054458196, -0.37801000551811326, 0.12100341566948845, -0.3383334928598915, -0.009617369280114203, 0.2549325679384667, -0.073998202409159... |
708.1798 | Theory of oxidation/reduction-induced chromium ion valence
transformations in Cr,Ca:YAG crystals | In their paper [Opt. Mater. 24, 333, 2003], Feldman et al conducted an
experimental study of the dynamics of chromium ion valence transformations in
Cr,Ca:YAG crystals among the trivalent Cr3+ state, and two tetravalent Cr4+
ones, of octahedral and tetrahedral coordination. The temperatures used ranged
between ~800 a... | cond-mat.mtrl-sci | in their paper opt mater 24 333 2003 feldman et al conducted an experimental study of the dynamics of chromium ion valence transformations in crcayag crystals among the trivalent cr3 state and two tetravalent cr4 ones of octahedral and tetrahedral coordination the temperatures used ranged between 800 and 1000 c the bas... | [['in', 'their', 'paper', 'opt', 'mater', '24', '333', '2003', 'feldman', 'et', 'al', 'conducted', 'an', 'experimental', 'study', 'of', 'the', 'dynamics', 'of', 'chromium', 'ion', 'valence', 'transformations', 'in', 'crcayag', 'crystals', 'among', 'the', 'trivalent', 'cr3', 'state', 'and', 'two', 'tetravalent', 'cr4', ... | [-0.062097176693051176, 0.21074224493949098, 0.02267804499801166, -0.010908399290158688, 0.07061404720606172, -0.10750861679655774, 0.1124261532430811, 0.4070122944738935, -0.22813152097275152, -0.35363674695220065, -0.0055155162576257305, -0.34613330686355337, -0.07326119534178253, 0.10601544597542242, 0.0200145140324... |
708.1799 | Shock Waves in Nanomechanical Resonators | The dream of every surfer is an extremely steep wave propagating at the
highest speed possible. The best waves for this would be shock waves, but are
very hard to surf. In the nanoscopic world the same is true: the surfers in
this case are electrons riding through nanomechanical devices on acoustic waves
[1]. Natural... | cond-mat.mes-hall | the dream of every surfer is an extremely steep wave propagating at the highest speed possible the best waves for this would be shock waves but are very hard to surf in the nanoscopic world the same is true the surfers in this case are electrons riding through nanomechanical devices on acoustic waves 1 naturally this h... | [['the', 'dream', 'of', 'every', 'surfer', 'is', 'an', 'extremely', 'steep', 'wave', 'propagating', 'at', 'the', 'highest', 'speed', 'possible', 'the', 'best', 'waves', 'for', 'this', 'would', 'be', 'shock', 'waves', 'but', 'are', 'very', 'hard', 'to', 'surf', 'in', 'the', 'nanoscopic', 'world', 'the', 'same', 'is', 't... | [-0.168260940022689, 0.1772879833079868, -0.026584361289213928, 0.008109677211096924, -0.07901389509853389, -0.126549609297783, 0.0035140156228509216, 0.3725680560662618, -0.2711750255923511, -0.2642831072469966, 0.07597437991126854, -0.2964079009136185, -0.14277075881448884, 0.25338283544923695, -0.016058070826370063,... |
708.18 | Confirming the Detection of an Intergalactic X-ray Absorber Toward PKS
2155-304 | We present new observations on PKS 2155-304 with the Chandra Low Energy
Transmission Grating Spectrometer (LETG), using the Advanced CCD Imaging
Spectrometer (ACIS). We confirm the detection of an absorption line plausibly
identified as OVIII Ly-alpha from the warm-hot intergalactic medium associated
with a small gro... | astro-ph | we present new observations on pks 2155304 with the chandra low energy transmission grating spectrometer letg using the advanced ccd imaging spectrometer acis we confirm the detection of an absorption line plausibly identified as oviii lyalpha from the warmhot intergalactic medium associated with a small group of galax... | [['we', 'present', 'new', 'observations', 'on', 'pks', '2155304', 'with', 'the', 'chandra', 'low', 'energy', 'transmission', 'grating', 'spectrometer', 'letg', 'using', 'the', 'advanced', 'ccd', 'imaging', 'spectrometer', 'acis', 'we', 'confirm', 'the', 'detection', 'of', 'an', 'absorption', 'line', 'plausibly', 'ident... | [-0.059156365060744065, 0.04051659625525872, -0.04920551174291177, 0.0407411160463198, -0.09709855714481819, -0.07665145610917534, 0.07057779031856626, 0.45673649887976353, -0.13588772435196006, -0.38190231120825047, 0.10924835074774819, -0.33552761967803235, -0.03902629144704406, 0.20490845260792412, -0.01396857926010... |
708.1801 | Polarized Structure of Nucleon in the Valon Representation | We have utilized the concept of valon model to calculate the spin structure
functions of proton, neutron and deuteron. The valon structure itself is
universal and arises from the perturbative dressing of the valence quark in
QCD. Our results agree rather well with all the relevant experimental data on
$g_{1}^{p, n, d... | hep-ph | we have utilized the concept of valon model to calculate the spin structure functions of proton neutron and deuteron the valon structure itself is universal and arises from the perturbative dressing of the valence quark in qcd our results agree rather well with all the relevant experimental data on g_1p n d and g_ag_v ... | [['we', 'have', 'utilized', 'the', 'concept', 'of', 'valon', 'model', 'to', 'calculate', 'the', 'spin', 'structure', 'functions', 'of', 'proton', 'neutron', 'and', 'deuteron', 'the', 'valon', 'structure', 'itself', 'is', 'universal', 'and', 'arises', 'from', 'the', 'perturbative', 'dressing', 'of', 'the', 'valence', 'q... | [-0.09010418585356451, 0.25157455323453715, -0.09654977557933486, 0.09879815974272788, -0.053591198144181645, -0.03606320397941292, 0.026580564078391978, 0.35567052223156265, -0.1984406406732483, -0.2464634346327296, -0.011256600864501785, -0.31591509553937264, -0.010329154577324695, 0.12815472588336876, 0.073070737825... |
708.1802 | Active elastic dimers: self-propulsion and current reversal on a
featureless track | We present a Brownian inchworm model of a self-propelled elastic dimer in the
absence of an external potential. Nonequilibrium noise together with a
stretch-dependent damping form the propulsion mechanism. Our model connects
three key nonequilibrium features -- position-velocity correlations, a nonzero
mean internal ... | cond-mat.stat-mech cond-mat.soft q-bio.BM | we present a brownian inchworm model of a selfpropelled elastic dimer in the absence of an external potential nonequilibrium noise together with a stretchdependent damping form the propulsion mechanism our model connects three key nonequilibrium features positionvelocity correlations a nonzero mean internal force and a... | [['we', 'present', 'a', 'brownian', 'inchworm', 'model', 'of', 'a', 'selfpropelled', 'elastic', 'dimer', 'in', 'the', 'absence', 'of', 'an', 'external', 'potential', 'nonequilibrium', 'noise', 'together', 'with', 'a', 'stretchdependent', 'damping', 'form', 'the', 'propulsion', 'mechanism', 'our', 'model', 'connects', '... | [-0.15719055805080148, 0.1580773387542484, -0.09340375790965151, 0.003061618973416361, -0.04442058226347647, -0.15155665365852078, 0.022124396020610056, 0.3823326495476067, -0.25066830865530804, -0.26024458850654564, -0.022516528068411968, -0.270283695500852, -0.2165551564910195, 0.18335056903941388, -0.004647795470770... |
708.1803 | Influence of finite baryon density on hadronization in nucleus-nucleus
collisions via recombination | In this paper is investigated the influence of net baryon density on baryon
and meson yields in relativistic nucleus-nucleus collisions, based on the
recombination model for hadronization. Unitarity condition is used as a
constraint on the model. Three cases with different assumptions on the
expansion of partonic sys... | nucl-th | in this paper is investigated the influence of net baryon density on baryon and meson yields in relativistic nucleusnucleus collisions based on the recombination model for hadronization unitarity condition is used as a constraint on the model three cases with different assumptions on the expansion of partonic system ar... | [['in', 'this', 'paper', 'is', 'investigated', 'the', 'influence', 'of', 'net', 'baryon', 'density', 'on', 'baryon', 'and', 'meson', 'yields', 'in', 'relativistic', 'nucleusnucleus', 'collisions', 'based', 'on', 'the', 'recombination', 'model', 'for', 'hadronization', 'unitarity', 'condition', 'is', 'used', 'as', 'a', ... | [-0.08039762004904571, 0.17732669492481185, -0.12308161040065718, 0.13309251178498763, -0.012497876053217982, -0.08557384261922514, 0.019864931040382408, 0.29511954122390904, -0.14085296624660737, -0.2358426182362877, -0.00466356336780381, -0.31268896345720915, 0.012635602791350885, 0.12396711945442147, 0.0567505758286... |
708.1804 | Discovery of a bright transient ultraluminous X-ray source Suzaku
J1305-4931 in NGC 4945 | This paper reports the discovery of a bright X-ray transient source, Suzaku
J1305-4913, in the south-west arm of the nearby Seyfert II galaxy NGC 4945. It
was detected at a 0.5 -- 10 keV flux of $2.2 \times 10^{-12}$ erg cm$^{-2}$
s$^{-1}$ during the Suzaku observation conducted on 2006 January 15 -- 17, but
was unde... | astro-ph | this paper reports the discovery of a bright xray transient source suzaku j13054913 in the southwest arm of the nearby seyfert ii galaxy ngc 4945 it was detected at a 05 10 kev flux of 22 times 1012 erg cm2 s1 during the suzaku observation conducted on 2006 january 15 17 but was undetectable in a shorter observation on... | [['this', 'paper', 'reports', 'the', 'discovery', 'of', 'a', 'bright', 'xray', 'transient', 'source', 'suzaku', 'j13054913', 'in', 'the', 'southwest', 'arm', 'of', 'the', 'nearby', 'seyfert', 'ii', 'galaxy', 'ngc', '4945', 'it', 'was', 'detected', 'at', 'a', '05', '10', 'kev', 'flux', 'of', '22', 'times', '1012', 'erg'... | [-0.09521285101610165, 0.1357619881634981, -0.005583815907952017, 0.11004674068446128, -0.03259779881381501, -0.12884837567913704, 0.052612796897077575, 0.41226936266757547, -0.09481803657959412, -0.3863615931092332, 0.10460312169340726, -0.3539278230808962, 0.07716094803942654, 0.2401040170619336, -0.03654688080378737... |
708.1805 | Schramm-Loewner Equations Driven by Symmetric Stable Processes | We consider shape, size and regularity of the hulls of the chordal
Schramm-Loewner evolution driven by a symmetric alpha-stable process. We obtain
derivative estimates, show that the complements of the hulls are Hoelder
domains, prove that the hulls have Hausdorff dimension 1, and show that the
trace is right-continu... | math.PR math-ph math.MP | we consider shape size and regularity of the hulls of the chordal schrammloewner evolution driven by a symmetric alphastable process we obtain derivative estimates show that the complements of the hulls are hoelder domains prove that the hulls have hausdorff dimension 1 and show that the trace is rightcontinuous with l... | [['we', 'consider', 'shape', 'size', 'and', 'regularity', 'of', 'the', 'hulls', 'of', 'the', 'chordal', 'schrammloewner', 'evolution', 'driven', 'by', 'a', 'symmetric', 'alphastable', 'process', 'we', 'obtain', 'derivative', 'estimates', 'show', 'that', 'the', 'complements', 'of', 'the', 'hulls', 'are', 'hoelder', 'dom... | [-0.10832325037982729, 0.1207741688251392, -0.07874225207854545, 0.058430395088180376, -0.02261046208958659, -0.08546994066003848, -0.05278961639851332, 0.41022209885219735, -0.3414758031980859, -0.11837479710164997, 0.18829681046514046, -0.3166048098527999, -0.13599574691788466, 0.17259358609509137, -0.112256213832922... |
708.1806 | Precision Test of Mass Ratio Variations with Lattice-Confined Ultracold
Molecules | We propose a precision measurement of time variations of the proton-electron
mass ratio using ultracold molecules in an optical lattice. Vibrational energy
intervals are sensitive to changes of the mass ratio. In contrast to
measurements that use hyperfine-interval-based atomic clocks, the scheme
discussed here is mo... | physics.atom-ph | we propose a precision measurement of time variations of the protonelectron mass ratio using ultracold molecules in an optical lattice vibrational energy intervals are sensitive to changes of the mass ratio in contrast to measurements that use hyperfineintervalbased atomic clocks the scheme discussed here is modelindep... | [['we', 'propose', 'a', 'precision', 'measurement', 'of', 'time', 'variations', 'of', 'the', 'protonelectron', 'mass', 'ratio', 'using', 'ultracold', 'molecules', 'in', 'an', 'optical', 'lattice', 'vibrational', 'energy', 'intervals', 'are', 'sensitive', 'to', 'changes', 'of', 'the', 'mass', 'ratio', 'in', 'contrast', ... | [-0.13725525900922916, 0.19905240488465958, -0.048955194073150285, 0.02286143438903162, -0.009452720625779114, -0.11375116830616183, 0.11757367022486555, 0.43873326666653156, -0.2346881731362963, -0.31911567971110344, 0.04478674600643383, -0.2262120988295489, -0.01848226230641877, 0.15847848238725518, -0.02952015721490... |
708.1807 | Supersolidity from defect-condensation in the extended boson Hubbard
model | We study the ground state phase diagram of the hard-core extended boson
Hubbard model on the square lattice with both nearest- (nn) and
next-nearest-neighbor (nnn) hopping and repulsion, using Gutzwiller mean field
theory and quantum Monte Carlo simulations. We observe the formation of
supersolid states with checkerb... | cond-mat.str-el cond-mat.stat-mech | we study the ground state phase diagram of the hardcore extended boson hubbard model on the square lattice with both nearest nn and nextnearestneighbor nnn hopping and repulsion using gutzwiller mean field theory and quantum monte carlo simulations we observe the formation of supersolid states with checkerboard striped... | [['we', 'study', 'the', 'ground', 'state', 'phase', 'diagram', 'of', 'the', 'hardcore', 'extended', 'boson', 'hubbard', 'model', 'on', 'the', 'square', 'lattice', 'with', 'both', 'nearest', 'nn', 'and', 'nextnearestneighbor', 'nnn', 'hopping', 'and', 'repulsion', 'using', 'gutzwiller', 'mean', 'field', 'theory', 'and',... | [-0.18750455325685575, 0.29262112024298403, -0.05490346299484372, 0.07163282435794827, -0.0039718609768897295, -0.15848160799110442, 0.12641569424782315, 0.4305998287995213, -0.27670536240995197, -0.17575401074386068, -0.003063481714759421, -0.34384008264169097, -0.12008681694214829, 0.044942563514008986, 0.17071317692... |
708.1808 | Launch of the Space experiment PAMELA | PAMELA is a satellite borne experiment designed to study with great accuracy
cosmic rays of galactic, solar, and trapped nature in a wide energy range
protons: 80 MeV-700 GeV, electrons 50 MeV-400 GeV). Main objective is the study
of the antimatter component: antiprotons (80 MeV-190 GeV), positrons (50
MeV-270 GeV) a... | astro-ph | pamela is a satellite borne experiment designed to study with great accuracy cosmic rays of galactic solar and trapped nature in a wide energy range protons 80 mev700 gev electrons 50 mev400 gev main objective is the study of the antimatter component antiprotons 80 mev190 gev positrons 50 mev270 gev and search for anti... | [['pamela', 'is', 'a', 'satellite', 'borne', 'experiment', 'designed', 'to', 'study', 'with', 'great', 'accuracy', 'cosmic', 'rays', 'of', 'galactic', 'solar', 'and', 'trapped', 'nature', 'in', 'a', 'wide', 'energy', 'range', 'protons', '80', 'mev700', 'gev', 'electrons', '50', 'mev400', 'gev', 'main', 'objective', 'is... | [-0.0931136483992133, 0.20975782737068538, -0.05515663502177136, 0.0643863245431597, -0.04258592819419558, -0.0810491181763757, 0.007743989097939424, 0.3386516606639973, -0.16814454432871895, -0.42174462664930923, 0.02611255128099949, -0.3758647666137217, 0.0546443421413137, 0.21914965263689765, -0.013277153719182453, ... |
708.1809 | Formation of bulk ferromagnetic nanostructured Fe40Ni40P14B6 alloys by
metastable liquid spinodal decomposition | Nanostructured Fe40Ni40P14B6 alloys ingots of diameter 3~5 mm could be
synthesised by a metastable liquid state spinodal decomposition method. The
molten Fe40Ni40P14B6 alloy was purified by means of the fluxing technique and
thus a large undercooling could be achieved. For undercooling Delta T > 260 K,
the microstruc... | cond-mat.mtrl-sci | nanostructured fe40ni40p14b6 alloys ingots of diameter 35 mm could be synthesised by a metastable liquid state spinodal decomposition method the molten fe40ni40p14b6 alloy was purified by means of the fluxing technique and thus a large undercooling could be achieved for undercooling delta t 260 k the microstructure of ... | [['nanostructured', 'fe40ni40p14b6', 'alloys', 'ingots', 'of', 'diameter', '35', 'mm', 'could', 'be', 'synthesised', 'by', 'a', 'metastable', 'liquid', 'state', 'spinodal', 'decomposition', 'method', 'the', 'molten', 'fe40ni40p14b6', 'alloy', 'was', 'purified', 'by', 'means', 'of', 'the', 'fluxing', 'technique', 'and',... | [-0.0860583464038262, 0.3156756440346891, -0.0954536695864575, -0.04060245340320567, 0.0034772007945493974, -0.1650031554235592, 0.061196047805003394, 0.39930086654480085, -0.27664031323780547, -0.3567510647776206, 0.08660256496509383, -0.27677576534049814, -0.017096957238006198, 0.10439254208429416, 0.0038318552638688... |
708.181 | 1+1+2 Electromagnetic perturbations on non-vacuum LRS class II
space-times: Decoupling scalar and 2-vector harmonic amplitudes | We use the covariant and gauge-invariant 1+1+2 formalism of Clarkson and
Barrett \cite{Clarkson2003} to analyze electromagnetic (EM) perturbations on
non-vacuum {\it locally rotationally symmetric} (LRS) class II space-times.
Ultimately, we show how to derive six real decoupled equations governing the
total of six EM... | gr-qc | we use the covariant and gaugeinvariant 112 formalism of clarkson and barrett citeclarkson2003 to analyze electromagnetic em perturbations on nonvacuum it locally rotationally symmetric lrs class ii spacetimes ultimately we show how to derive six real decoupled equations governing the total of six em scalar and 2vector... | [['we', 'use', 'the', 'covariant', 'and', 'gaugeinvariant', '112', 'formalism', 'of', 'clarkson', 'and', 'barrett', 'citeclarkson2003', 'to', 'analyze', 'electromagnetic', 'em', 'perturbations', 'on', 'nonvacuum', 'it', 'locally', 'rotationally', 'symmetric', 'lrs', 'class', 'ii', 'spacetimes', 'ultimately', 'we', 'sho... | [-0.16152347432899064, 0.17522148790223332, -0.030225843300336393, 0.07574133965074374, -0.08187703535217664, -0.10589463769173217, -0.0551466075944361, 0.35345383255646146, -0.21232513878012782, -0.2804723738018295, 0.07346697576135268, -0.24769369417094977, -0.19181058810831145, 0.15872996464724942, 0.009169018342448... |
708.1811 | 1+1+2 Electromagnetic perturbations on general LRS space-times:
Regge-Wheeler and Bardeen-Press equations | We use the, covariant and gauge-invariant, 1+1+2 formalism developed by
Clarkson and Barrett, and develop new techniques, to decouple electromagnetic
(EM) perturbations on arbitrary locally rotationally symmetric (LRS)
space-times. Ultimately, we derive 3 decoupled complex equations governing 3
complex scalars. One o... | gr-qc | we use the covariant and gaugeinvariant 112 formalism developed by clarkson and barrett and develop new techniques to decouple electromagnetic em perturbations on arbitrary locally rotationally symmetric lrs spacetimes ultimately we derive 3 decoupled complex equations governing 3 complex scalars one of these is a new ... | [['we', 'use', 'the', 'covariant', 'and', 'gaugeinvariant', '112', 'formalism', 'developed', 'by', 'clarkson', 'and', 'barrett', 'and', 'develop', 'new', 'techniques', 'to', 'decouple', 'electromagnetic', 'em', 'perturbations', 'on', 'arbitrary', 'locally', 'rotationally', 'symmetric', 'lrs', 'spacetimes', 'ultimately'... | [-0.13377863059548156, 0.11696114254165564, -0.10919244016292474, 0.07103424595934123, -0.17351324631160261, -0.17431489151184731, -0.02986471163762721, 0.2653783481222707, -0.26394458248631547, -0.24522207783217487, 0.06560928689621216, -0.19138937840077852, -0.19809914219026634, 0.13313908708460678, -0.00355519765112... |
708.1812 | 1+1+2 gravitational perturbations on LRS class II space-times:
Decoupling GEM tensor harmonic amplitudes | This paper considers gauge-invariant and covariant gravitational
perturbations on arbitrary vacuum locally rotationally symmetric (LRS) class II
space-times. Ultimately, we derive four decoupled equations governing four
specific combinations of the gravito-electromagnetic (GEM) 2-tensor harmonic
amplitudes. We use th... | gr-qc | this paper considers gaugeinvariant and covariant gravitational perturbations on arbitrary vacuum locally rotationally symmetric lrs class ii spacetimes ultimately we derive four decoupled equations governing four specific combinations of the gravitoelectromagnetic gem 2tensor harmonic amplitudes we use the gaugeinvari... | [['this', 'paper', 'considers', 'gaugeinvariant', 'and', 'covariant', 'gravitational', 'perturbations', 'on', 'arbitrary', 'vacuum', 'locally', 'rotationally', 'symmetric', 'lrs', 'class', 'ii', 'spacetimes', 'ultimately', 'we', 'derive', 'four', 'decoupled', 'equations', 'governing', 'four', 'specific', 'combinations'... | [-0.16154507673312943, 0.11422751956599785, -0.06561007047189282, 0.041986250753312575, -0.11419407863795132, -0.16719973181277495, -0.07594098619892022, 0.2857340701523569, -0.24066607953355343, -0.22553819944834583, 0.07621374279521145, -0.1979206700066847, -0.17376531853008417, 0.12058962192679462, -0.02782349762102... |
708.1813 | On Dissipative Quadratic Stochastic Operators | In present paper we introduce the notion of dissipative quadratic stochastic
operator and cubic stochastic operator. We prove necessary conditions for
dissipativity of quadratic stochastic operators. Besides, it is studied certain
limit behavior of such operators. Finally we prove ergodic theorem for
dissipative oper... | math.FA math.DS | in present paper we introduce the notion of dissipative quadratic stochastic operator and cubic stochastic operator we prove necessary conditions for dissipativity of quadratic stochastic operators besides it is studied certain limit behavior of such operators finally we prove ergodic theorem for dissipative operators | [['in', 'present', 'paper', 'we', 'introduce', 'the', 'notion', 'of', 'dissipative', 'quadratic', 'stochastic', 'operator', 'and', 'cubic', 'stochastic', 'operator', 'we', 'prove', 'necessary', 'conditions', 'for', 'dissipativity', 'of', 'quadratic', 'stochastic', 'operators', 'besides', 'it', 'is', 'studied', 'certain... | [-0.2162613287906755, 0.10643400241282176, -0.05183331160382791, 0.1385893837300087, -0.07399066936605694, -0.15396209391341967, -0.010375358553243463, 0.2965773345733231, -0.341939507136968, -0.13844525077464906, 0.12535113432518716, -0.26204696932638233, -0.2671146083792502, 0.1699360083915632, -0.11461778118973598, ... |
708.1814 | Galaxy growth in the concordance $\Lambda$CDM cosmology | We use galaxy and dark halo data from the public database for the Millennium
Simulation to study the growth of galaxies in the De Lucia et al. (2006) model
for galaxy formation. Previous work has shown this model to reproduce many
aspects of the systematic properties and the clustering of real galaxies, both
in the n... | astro-ph | we use galaxy and dark halo data from the public database for the millennium simulation to study the growth of galaxies in the de lucia et al 2006 model for galaxy formation previous work has shown this model to reproduce many aspects of the systematic properties and the clustering of real galaxies both in the nearby u... | [['we', 'use', 'galaxy', 'and', 'dark', 'halo', 'data', 'from', 'the', 'public', 'database', 'for', 'the', 'millennium', 'simulation', 'to', 'study', 'the', 'growth', 'of', 'galaxies', 'in', 'the', 'de', 'lucia', 'et', 'al', '2006', 'model', 'for', 'galaxy', 'formation', 'previous', 'work', 'has', 'shown', 'this', 'mod... | [-0.0512406909299359, 0.12283220325631124, -0.05224909516034165, 0.1205970260774174, -0.09047915767705828, -0.011159928074037586, -0.011230243949426545, 0.39865401541572754, -0.09638835022062132, -0.3418575417181408, 0.030801602740582353, -0.30253794461799166, -0.007601679544125175, 0.25582696793566423, 0.0248399337960... |
708.1815 | Reducing variance in univariate smoothing | A variance reduction technique in nonparametric smoothing is proposed: at
each point of estimation, form a linear combination of a preliminary estimator
evaluated at nearby points with the coefficients specified so that the
asymptotic bias remains unchanged. The nearby points are chosen to maximize the
variance reduc... | math.ST stat.TH | a variance reduction technique in nonparametric smoothing is proposed at each point of estimation form a linear combination of a preliminary estimator evaluated at nearby points with the coefficients specified so that the asymptotic bias remains unchanged the nearby points are chosen to maximize the variance reduction ... | [['a', 'variance', 'reduction', 'technique', 'in', 'nonparametric', 'smoothing', 'is', 'proposed', 'at', 'each', 'point', 'of', 'estimation', 'form', 'a', 'linear', 'combination', 'of', 'a', 'preliminary', 'estimator', 'evaluated', 'at', 'nearby', 'points', 'with', 'the', 'coefficients', 'specified', 'so', 'that', 'the... | [-0.0874439117279835, 0.0006666140630841255, -0.09260795643925666, 0.05633808420877904, -0.07110218051075935, -0.1470371965803206, 0.08003239376656711, 0.38154733341932295, -0.25219469602406025, -0.2894470510855317, 0.11857606022246182, -0.24558201425522566, -0.10505220517516137, 0.20432330959290265, -0.100326957374811... |
708.1816 | Proposal for exotic-hadron search by fragmentation functions | It is proposed that fragmentation functions should be used to identify exotic
hadrons. As an example, fragmentation functions of the scalar meson f_0(980)
are investigated. It is pointed out that the second moments and functional
forms of the u- and s-quark fragmentation functions can distinguish the
tetraquark struc... | hep-ph hep-ex nucl-ex nucl-th | it is proposed that fragmentation functions should be used to identify exotic hadrons as an example fragmentation functions of the scalar meson f_0980 are investigated it is pointed out that the second moments and functional forms of the u and squark fragmentation functions can distinguish the tetraquark structure from... | [['it', 'is', 'proposed', 'that', 'fragmentation', 'functions', 'should', 'be', 'used', 'to', 'identify', 'exotic', 'hadrons', 'as', 'an', 'example', 'fragmentation', 'functions', 'of', 'the', 'scalar', 'meson', 'f_0980', 'are', 'investigated', 'it', 'is', 'pointed', 'out', 'that', 'the', 'second', 'moments', 'and', 'f... | [-0.08983067406341433, 0.18360914002303616, -0.1355003879009746, 0.20123680168646388, -0.09161320542916655, -0.09036148578859865, 0.013623614981770515, 0.37156737205572427, -0.2443786509661004, -0.22531280270311982, 0.030963587441947313, -0.28087749615311625, -0.035758235771209, 0.1375884828111157, 0.08713712688535452,... |
708.1817 | Dark energy and cosmic curvature: Monte-Carlo Markov Chain approach | We use the Monte-Carlo Markov Chain method to explore the dark energy
property and the cosmic curvature by fitting two popular dark energy
parameterizations to the observational data. The new 182 gold supernova Ia data
and the ESSENCE data both give good constraint on the DE parameters and the
cosmic curvature for th... | astro-ph | we use the montecarlo markov chain method to explore the dark energy property and the cosmic curvature by fitting two popular dark energy parameterizations to the observational data the new 182 gold supernova ia data and the essence data both give good constraint on the de parameters and the cosmic curvature for the da... | [['we', 'use', 'the', 'montecarlo', 'markov', 'chain', 'method', 'to', 'explore', 'the', 'dark', 'energy', 'property', 'and', 'the', 'cosmic', 'curvature', 'by', 'fitting', 'two', 'popular', 'dark', 'energy', 'parameterizations', 'to', 'the', 'observational', 'data', 'the', 'new', '182', 'gold', 'supernova', 'ia', 'dat... | [-0.08592592917339897, 0.060121550845603146, -0.11089138647048981, 0.22246109294549873, -0.16059111074769292, -0.09157421853093581, -0.006339308741534579, 0.32311919405414113, -0.2502834269584253, -0.4021787651568309, 0.03256204796034372, -0.3157277539286805, 0.0400856373960088, 0.1938843192885919, 0.017433627294483542... |
708.1818 | Computational Simulation and 3D Virtual Reality Engineering Tools for
Dynamical Modeling and Imaging of Composite Nanomaterials | An adventure at engineering design and modeling is possible with a Virtual
Reality Environment (VRE) that uses multiple computer-generated media to let a
user experience situations that are temporally and spatially prohibiting. In
this paper, an approach to developing some advanced architecture and modeling
tools is ... | cs.CE cond-mat.other | an adventure at engineering design and modeling is possible with a virtual reality environment vre that uses multiple computergenerated media to let a user experience situations that are temporally and spatially prohibiting in this paper an approach to developing some advanced architecture and modeling tools is present... | [['an', 'adventure', 'at', 'engineering', 'design', 'and', 'modeling', 'is', 'possible', 'with', 'a', 'virtual', 'reality', 'environment', 'vre', 'that', 'uses', 'multiple', 'computergenerated', 'media', 'to', 'let', 'a', 'user', 'experience', 'situations', 'that', 'are', 'temporally', 'and', 'spatially', 'prohibiting'... | [-0.09120511708360672, 0.04722517658786812, -0.08680954262234487, -0.013791318141936678, -0.10568774506015685, -0.17901000091625216, -0.007005238194624414, 0.41730629638271427, -0.26405613211625556, -0.3295345985357767, 0.1066467909693935, -0.2467195672001147, -0.2093337051687961, 0.25381704712811026, -0.09313054267515... |
708.1819 | Quasi-Nilpotent Operators on Locally Convex Spaces | In this article we extend the notion of quasi-nilpotent equivalent operators,
introduced by Colojoara and Foias \cite{co1} for Banach spaces, to the class of
bounded operators on sequentially complete locally convex spaces.
| math.FA | in this article we extend the notion of quasinilpotent equivalent operators introduced by colojoara and foias citeco1 for banach spaces to the class of bounded operators on sequentially complete locally convex spaces | [['in', 'this', 'article', 'we', 'extend', 'the', 'notion', 'of', 'quasinilpotent', 'equivalent', 'operators', 'introduced', 'by', 'colojoara', 'and', 'foias', 'citeco1', 'for', 'banach', 'spaces', 'to', 'the', 'class', 'of', 'bounded', 'operators', 'on', 'sequentially', 'complete', 'locally', 'convex', 'spaces']] | [-0.054141037706886566, 0.1423156390327119, 0.016506599089611444, 0.11847845577229295, -0.09120426028065624, -0.07228707311855208, 0.02238822908651444, 0.3775891689283232, -0.32981526382988496, -0.08625970229566578, 0.13019236290241562, -0.242053366356319, -0.13597024006829148, 0.17862068032545428, -0.253057639084516, ... |
708.182 | Confidence sets for split points in decision trees | We investigate the problem of finding confidence sets for split points in
decision trees (CART). Our main results establish the asymptotic distribution
of the least squares estimators and some associated residual sum of squares
statistics in a binary decision tree approximation to a smooth regression
curve. Cube-root... | math.ST stat.TH | we investigate the problem of finding confidence sets for split points in decision trees cart our main results establish the asymptotic distribution of the least squares estimators and some associated residual sum of squares statistics in a binary decision tree approximation to a smooth regression curve cuberoot asympt... | [['we', 'investigate', 'the', 'problem', 'of', 'finding', 'confidence', 'sets', 'for', 'split', 'points', 'in', 'decision', 'trees', 'cart', 'our', 'main', 'results', 'establish', 'the', 'asymptotic', 'distribution', 'of', 'the', 'least', 'squares', 'estimators', 'and', 'some', 'associated', 'residual', 'sum', 'of', 's... | [-0.09137778249350959, 0.0367682335228892, -0.09668242761108559, 0.13927771750168177, -0.030005869049773537, -0.11650991254427936, 0.14806480805273167, 0.34860006627859547, -0.22623097355826757, -0.26386575895594433, 0.16098985342177913, -0.30472108284011484, -0.11625084334518761, 0.204969395295484, -0.0956914754817262... |
708.1821 | Preliminary Results on Vibration Damping Properties of
Nanoscale-Reinforced Composite Materials | The focus in this paper is an analysis of existing state of the arts directed
toward the development of the next generation of vibration damping systems. The
research work concentrates on an investigation related to
nanoparticles/fibres/tubes-reinforced materials and coatings dynamic
characterization and modeling of ... | cond-mat.mtrl-sci | the focus in this paper is an analysis of existing state of the arts directed toward the development of the next generation of vibration damping systems the research work concentrates on an investigation related to nanoparticlesfibrestubesreinforced materials and coatings dynamic characterization and modeling of the fu... | [['the', 'focus', 'in', 'this', 'paper', 'is', 'an', 'analysis', 'of', 'existing', 'state', 'of', 'the', 'arts', 'directed', 'toward', 'the', 'development', 'of', 'the', 'next', 'generation', 'of', 'vibration', 'damping', 'systems', 'the', 'research', 'work', 'concentrates', 'on', 'an', 'investigation', 'related', 'to'... | [-0.10944996132170708, 0.10388203566792187, -0.05354386537819807, -0.03641682908243287, -0.10353518434338213, -0.09367110129944452, 0.015561651600722782, 0.39243998626379045, -0.24607857696961347, -0.2929726050099666, 0.13328697675688736, -0.2835764240209512, -0.18586197223763648, 0.25144238445145173, -0.06112948497463... |
708.1822 | Suspension of Nanoparticles in SU-8 and Characterization of
Nanocomposite Properties | Gold nanospheres, single wall carbon nanotubes (SWNT), and diamonoids were
phyically incorporated into the negative photoresist SU-8. the mixtures were
spin cast onto silicon or aluminium coated silicon wafers. ASTM standard D638
tensile specimens were lithographically patterned in the materials and then
released fro... | cond-mat.mtrl-sci | gold nanospheres single wall carbon nanotubes swnt and diamonoids were phyically incorporated into the negative photoresist su8 the mixtures were spin cast onto silicon or aluminium coated silicon wafers astm standard d638 tensile specimens were lithographically patterned in the materials and then released from the sub... | [['gold', 'nanospheres', 'single', 'wall', 'carbon', 'nanotubes', 'swnt', 'and', 'diamonoids', 'were', 'phyically', 'incorporated', 'into', 'the', 'negative', 'photoresist', 'su8', 'the', 'mixtures', 'were', 'spin', 'cast', 'onto', 'silicon', 'or', 'aluminium', 'coated', 'silicon', 'wafers', 'astm', 'standard', 'd638',... | [-0.04468236341251343, 0.21892892310396356, -0.012686800828045566, -0.14384551880712998, 0.045504951350657005, -0.16575469077049224, 0.053094347454524335, 0.4898465611040592, -0.24204961039192444, -0.3007702351398101, 0.05291491396201309, -0.34286342158780564, -0.10722181455016003, 0.12700877085028747, -0.0088667895402... |
708.1823 | Landscape phage, phage display, stripped phage, biosensors, detection,
affinity reagent, nanotechnology, Salmonella typhimurium, Bacillus anthracis | Filamentous phage, such as fd used in this study, are thread-shaped bacterial
viruses. Their outer coat is a tube formed by thousands equal copies of the
major coat protein pVIII. We constructed libraries of random peptides fused to
all pVIII domains and selected phages that act as probes specific for a panel
of test... | cond-mat.mtrl-sci q-bio.CB | filamentous phage such as fd used in this study are threadshaped bacterial viruses their outer coat is a tube formed by thousands equal copies of the major coat protein pviii we constructed libraries of random peptides fused to all pviii domains and selected phages that act as probes specific for a panel of test antige... | [['filamentous', 'phage', 'such', 'as', 'fd', 'used', 'in', 'this', 'study', 'are', 'threadshaped', 'bacterial', 'viruses', 'their', 'outer', 'coat', 'is', 'a', 'tube', 'formed', 'by', 'thousands', 'equal', 'copies', 'of', 'the', 'major', 'coat', 'protein', 'pviii', 'we', 'constructed', 'libraries', 'of', 'random', 'pe... | [-0.07765013974744316, 0.19214818334919126, -0.0217939429247624, 0.03616566723497931, -0.03461056001091778, -0.21919671270320668, 0.055045553845440166, 0.4117452816252469, -0.24246572153688425, -0.2868080631611234, 0.07571985041317485, -0.3094138282752943, -0.18972015760350497, 0.16534098509502798, -0.08446018711672913... |
708.1824 | The deffect effect on electronic conductance in binomially tailored
quantum wire | The paper considers the effect of the defects on the electronic transmission
properties in binomially tailored waveguide quantum wires, in which each Dirac
delta function potential strength have been weight on the binomial distribution
law. We have assumed that a single free-electron channel is incident on the
struct... | cond-mat.mtrl-sci | the paper considers the effect of the defects on the electronic transmission properties in binomially tailored waveguide quantum wires in which each dirac delta function potential strength have been weight on the binomial distribution law we have assumed that a single freeelectron channel is incident on the structure a... | [['the', 'paper', 'considers', 'the', 'effect', 'of', 'the', 'defects', 'on', 'the', 'electronic', 'transmission', 'properties', 'in', 'binomially', 'tailored', 'waveguide', 'quantum', 'wires', 'in', 'which', 'each', 'dirac', 'delta', 'function', 'potential', 'strength', 'have', 'been', 'weight', 'on', 'the', 'binomial... | [-0.1213085300270468, 0.10168871748331003, -0.07274578108638526, 0.026997269775718452, -0.0181745474152267, -0.12708729191869497, 0.05233695999439806, 0.4409128195643425, -0.29583166844258085, -0.28903981317579747, -0.0041044315239414575, -0.2932726363241672, -0.1567429050132632, 0.13645296164602042, -0.029214670814573... |
708.1825 | Events and observables in generally invariant spacetime theories | We address the problem of observables in generally invariant spacetime
theories such as Einstein's general relativity. Using the refined notion of an
event as a ``point-coincidence'' between scalar fields that completely
characterise a spacetime model, we propose a generalisation of the relational
local observables t... | gr-qc | we address the problem of observables in generally invariant spacetime theories such as einsteins general relativity using the refined notion of an event as a pointcoincidence between scalar fields that completely characterise a spacetime model we propose a generalisation of the relational local observables that does n... | [['we', 'address', 'the', 'problem', 'of', 'observables', 'in', 'generally', 'invariant', 'spacetime', 'theories', 'such', 'as', 'einsteins', 'general', 'relativity', 'using', 'the', 'refined', 'notion', 'of', 'an', 'event', 'as', 'a', 'pointcoincidence', 'between', 'scalar', 'fields', 'that', 'completely', 'characteri... | [-0.16881249516547933, 0.12366697318223463, -0.10127906526464063, 0.11882661987328902, -0.0921349159404132, -0.13918310552332047, -0.05764873337151634, 0.28793763228050256, -0.23195033560733538, -0.25383941600149545, 0.06356655044569257, -0.21522690516871376, -0.1830156733583961, 0.14781109906097473, -0.085930526690758... |
708.1826 | Methods for The Testing of Nanopowder | Methods for the testing of nanopowders produced by wires electric explosion
were considered. The following characteristics were proposed for the testing of
nanopowders : main substance content, characteristic sizes of particles,
specific surface area etc..
| cond-mat.mtrl-sci | methods for the testing of nanopowders produced by wires electric explosion were considered the following characteristics were proposed for the testing of nanopowders main substance content characteristic sizes of particles specific surface area etc | [['methods', 'for', 'the', 'testing', 'of', 'nanopowders', 'produced', 'by', 'wires', 'electric', 'explosion', 'were', 'considered', 'the', 'following', 'characteristics', 'were', 'proposed', 'for', 'the', 'testing', 'of', 'nanopowders', 'main', 'substance', 'content', 'characteristic', 'sizes', 'of', 'particles', 'spe... | [-0.07001271265942384, 0.15840937087641044, -0.016105845351429546, 0.04139252817806076, 0.007931242395630655, -0.16415940393584177, 0.005034622434964951, 0.38790960204513636, -0.164503441657871, -0.3883589696796501, 0.06969988774782156, -0.2613841417409918, -0.037866825676139665, 0.21869320904507356, -0.065389699795666... |
708.1827 | Modeling Atmospheric Neutrino Interactions: Duality Constrained
Parameterization of Vector and Axial Nucleon Form Factors | We present new parameterizations of vector and axial nucleon form factors. We
maintain an excellent descriptions of the form factors at low momentum
transfers, where the spatial structure of the nucleon is important, and use the
Nachtman scaling variable \xi to relate elastic and inelastic form factors and
impose qua... | hep-ex nucl-ex | we present new parameterizations of vector and axial nucleon form factors we maintain an excellent descriptions of the form factors at low momentum transfers where the spatial structure of the nucleon is important and use the nachtman scaling variable xi to relate elastic and inelastic form factors and impose quarkhadr... | [['we', 'present', 'new', 'parameterizations', 'of', 'vector', 'and', 'axial', 'nucleon', 'form', 'factors', 'we', 'maintain', 'an', 'excellent', 'descriptions', 'of', 'the', 'form', 'factors', 'at', 'low', 'momentum', 'transfers', 'where', 'the', 'spatial', 'structure', 'of', 'the', 'nucleon', 'is', 'important', 'and'... | [-0.09074511292406864, 0.22563537698174754, -0.050810142153191885, 0.13796249873989277, -0.1039591008131474, -0.04524584434387323, 0.0831499867316891, 0.36064817267878535, -0.20242173691165813, -0.265275021001958, -0.02404355160838908, -0.2976880722205367, -0.052519798058232196, 0.14556002185124448, 0.0989656633975213,... |
708.1828 | Structure And Properties of Nanoparticles Formed under Conditions of
Wire Electrical Explosion | Structure and properties of nanoparticles formed under conditions of wire
electrical explosion were studied. It was shown that the state of WEE power
particles can be characterized as a metastable state. It leads to an increased
stability of nanopowders at normal temperatures and an increased reactivity
during heatin... | cond-mat.mtrl-sci | structure and properties of nanoparticles formed under conditions of wire electrical explosion were studied it was shown that the state of wee power particles can be characterized as a metastable state it leads to an increased stability of nanopowders at normal temperatures and an increased reactivity during heating wh... | [['structure', 'and', 'properties', 'of', 'nanoparticles', 'formed', 'under', 'conditions', 'of', 'wire', 'electrical', 'explosion', 'were', 'studied', 'it', 'was', 'shown', 'that', 'the', 'state', 'of', 'wee', 'power', 'particles', 'can', 'be', 'characterized', 'as', 'a', 'metastable', 'state', 'it', 'leads', 'to', 'a... | [-0.10408879873514372, 0.2359989221629548, -0.1017202188979769, 0.004312315001969405, 0.020249249483050222, -0.10563084379394065, 0.037787575101104094, 0.38164352857622136, -0.26087400524697285, -0.3197442536944883, 0.08360389124381502, -0.2537033319996114, -0.10452582752495482, 0.18753179120259328, -0.0154201531652034... |
708.1829 | Spatial Distributions of Cold and Warm Interstellar Dust in M101
Resolved with AKARI/Far-Infrared Surveyor (FIS) | The nearby face-on spiral galaxy M101 has been observed with the Far-Infrared
Surveyor (FIS) onboard AKARI. The far-infrared four-band images reveal fine
spatial structures of M101, which include global spiral patterns, giant HII
regions embedded in outer spiral arms, and a bar-like feature crossing the
center. The s... | astro-ph | the nearby faceon spiral galaxy m101 has been observed with the farinfrared surveyor fis onboard akari the farinfrared fourband images reveal fine spatial structures of m101 which include global spiral patterns giant hii regions embedded in outer spiral arms and a barlike feature crossing the center the spectral energy... | [['the', 'nearby', 'faceon', 'spiral', 'galaxy', 'm101', 'has', 'been', 'observed', 'with', 'the', 'farinfrared', 'surveyor', 'fis', 'onboard', 'akari', 'the', 'farinfrared', 'fourband', 'images', 'reveal', 'fine', 'spatial', 'structures', 'of', 'm101', 'which', 'include', 'global', 'spiral', 'patterns', 'giant', 'hii'... | [-0.09370177769388008, 0.04366242197471311, -0.0935448165994488, 0.05699257901581557, -0.07614069154467618, -0.007654541859052854, -0.024666794679487253, 0.44258317635348526, -0.1740665171055658, -0.3020707678769042, 0.02219191442490417, -0.28554438661304443, -0.04127040997350422, 0.11168237880914297, 0.007795035368809... |
708.183 | Time-dependent gravitating solitons in five dimensional warped
space-times | Time-dependent soliton solutions are explicitly derived in a five-dimensional
theory endowed with one (warped) extra-dimension. Some of the obtained
geometries, everywhere well defined and technically regular, smoothly
interpolate between two five-dimensional anti-de Sitter space-times for fixed
value of the conforma... | hep-th astro-ph gr-qc hep-ph | timedependent soliton solutions are explicitly derived in a fivedimensional theory endowed with one warped extradimension some of the obtained geometries everywhere well defined and technically regular smoothly interpolate between two fivedimensional antide sitter spacetimes for fixed value of the conformal time coordi... | [['timedependent', 'soliton', 'solutions', 'are', 'explicitly', 'derived', 'in', 'a', 'fivedimensional', 'theory', 'endowed', 'with', 'one', 'warped', 'extradimension', 'some', 'of', 'the', 'obtained', 'geometries', 'everywhere', 'well', 'defined', 'and', 'technically', 'regular', 'smoothly', 'interpolate', 'between', ... | [-0.20969674220308662, 0.15147311501204969, -0.04700986675918102, 0.10556680944282562, -0.0910562176327221, -0.20134603559349973, -0.09124688850560536, 0.3353529319912195, -0.18664968269566695, -0.21883543604363997, 0.12073794169041017, -0.27597108935316406, -0.11646528729548057, 0.1360574309217433, -0.0216690040503939... |
708.1831 | Ultrasonic Production of Nano-Size Dispersions and Emulsions | Ultrasound is a well-established method for particle size reduction in
dispersions and emulsions. Ultrasonic processors are used in the generation of
nano-size material slurries, dispersions and emulsions because of the potential
in the deagglomeration and the reduction of primaries. These are the mechanical
effects ... | cond-mat.mtrl-sci | ultrasound is a wellestablished method for particle size reduction in dispersions and emulsions ultrasonic processors are used in the generation of nanosize material slurries dispersions and emulsions because of the potential in the deagglomeration and the reduction of primaries these are the mechanical effects of ultr... | [['ultrasound', 'is', 'a', 'wellestablished', 'method', 'for', 'particle', 'size', 'reduction', 'in', 'dispersions', 'and', 'emulsions', 'ultrasonic', 'processors', 'are', 'used', 'in', 'the', 'generation', 'of', 'nanosize', 'material', 'slurries', 'dispersions', 'and', 'emulsions', 'because', 'of', 'the', 'potential',... | [-0.07955654719125654, 0.19028128997966548, -0.060525336866923324, 0.028235659882354578, -0.05473243696115061, -0.08456799789056832, 0.06616522313014372, 0.37178768195061873, -0.28506416859942796, -0.33968152755858916, 0.11802462004703289, -0.28650575991869975, -0.07716065709285388, 0.20699194049456426, -0.054859285386... |
708.1832 | High-frequency modes in solar-like stars | p-mode oscillations in solar-like stars are excited by the outer convection
zone in these stars and reflected close to the surface. The p-modes are trapped
inside an acoustic cavity, but the modes only stay trapped up to a given
frequency (known as the acoustic cut-off frequency) as modes with larger
frequencies are ... | astro-ph | pmode oscillations in solarlike stars are excited by the outer convection zone in these stars and reflected close to the surface the pmodes are trapped inside an acoustic cavity but the modes only stay trapped up to a given frequency known as the acoustic cutoff frequency as modes with larger frequencies are generally ... | [['pmode', 'oscillations', 'in', 'solarlike', 'stars', 'are', 'excited', 'by', 'the', 'outer', 'convection', 'zone', 'in', 'these', 'stars', 'and', 'reflected', 'close', 'to', 'the', 'surface', 'the', 'pmodes', 'are', 'trapped', 'inside', 'an', 'acoustic', 'cavity', 'but', 'the', 'modes', 'only', 'stay', 'trapped', 'up... | [-0.10979234964258, 0.24072146906496733, -0.0367778305692293, 0.05617773104280754, -0.09891621638844544, -0.09456652612635144, 0.028980728939410533, 0.36378124946107465, -0.22038376236309273, -0.319459959625493, 0.10651650777671838, -0.2938382937614848, -0.07356930611474725, 0.24546737795137707, -0.006081246928236372, ... |
708.1833 | Numerical Simulation of The Mechanical Properties of Nanoscale Metal
Clusters Using The Atomistic-Continuum Mechanics Method | A novel atomistic-continuum method (ACM) based on finite element method (FEM)
is proposed to numerically simulate the nano-scaled Poisson's ratio and Young's
modulus effect of Lithium (Li) body-centered cubic (BCC) structure. The
potential energy between Li atoms is described by the Morse potential function
[1]. The ... | cond-mat.mtrl-sci | a novel atomisticcontinuum method acm based on finite element method fem is proposed to numerically simulate the nanoscaled poissons ratio and youngs modulus effect of lithium li bodycentered cubic bcc structure the potential energy between li atoms is described by the morse potential function 1 the preforce effect wil... | [['a', 'novel', 'atomisticcontinuum', 'method', 'acm', 'based', 'on', 'finite', 'element', 'method', 'fem', 'is', 'proposed', 'to', 'numerically', 'simulate', 'the', 'nanoscaled', 'poissons', 'ratio', 'and', 'youngs', 'modulus', 'effect', 'of', 'lithium', 'li', 'bodycentered', 'cubic', 'bcc', 'structure', 'the', 'poten... | [-0.06575700770356233, 0.16053677488212723, -0.0501016735547234, -0.005194668655130494, -0.06105574829904716, -0.15893499090489518, 0.07867682428111004, 0.4125136633085299, -0.31776562974422795, -0.2792054018170773, -0.014428269436370723, -0.23942906787925505, -0.15848020268780993, 0.13973557199292544, -0.0249846754477... |
708.1834 | CMOL: Second Life for Silicon? | This report is a brief review of the recent work on architectures for the
prospective hybrid CMOS/nanowire/ nanodevice ("CMOL") circuits including
digital memories, reconfigurable Boolean-logic circuits, and mixed-signal
neuromorphic networks. The basic idea of CMOL circuits is to combine the
advantages of CMOS techn... | cond-mat.other | this report is a brief review of the recent work on architectures for the prospective hybrid cmosnanowire nanodevice cmol circuits including digital memories reconfigurable booleanlogic circuits and mixedsignal neuromorphic networks the basic idea of cmol circuits is to combine the advantages of cmos technology includi... | [['this', 'report', 'is', 'a', 'brief', 'review', 'of', 'the', 'recent', 'work', 'on', 'architectures', 'for', 'the', 'prospective', 'hybrid', 'cmosnanowire', 'nanodevice', 'cmol', 'circuits', 'including', 'digital', 'memories', 'reconfigurable', 'booleanlogic', 'circuits', 'and', 'mixedsignal', 'neuromorphic', 'networ... | [-0.1476899371406094, 0.10548325710785365, 0.014721636114580954, -0.06235274907223476, -0.034352189494816006, -0.2008324967025489, 0.050498882445056355, 0.41932639387268267, -0.2187690115285671, -0.3768376949926472, 0.1035581272969511, -0.2779880693930461, -0.1306707457520953, 0.2706822347731833, -0.1101706242494163, 0... |
708.1835 | Bottom-Up Approach to Silicon Nanoelectronics | This paper presents a brief review of our recent work investigating a novel
bottom-up approach to realize silicon based nanoelectronics. We discuss
fabrication technique, electronic properties and device applications of silicon
nanodots as a building block for nanoscale silicon devices.
| cond-mat.mtrl-sci | this paper presents a brief review of our recent work investigating a novel bottomup approach to realize silicon based nanoelectronics we discuss fabrication technique electronic properties and device applications of silicon nanodots as a building block for nanoscale silicon devices | [['this', 'paper', 'presents', 'a', 'brief', 'review', 'of', 'our', 'recent', 'work', 'investigating', 'a', 'novel', 'bottomup', 'approach', 'to', 'realize', 'silicon', 'based', 'nanoelectronics', 'we', 'discuss', 'fabrication', 'technique', 'electronic', 'properties', 'and', 'device', 'applications', 'of', 'silicon', ... | [-0.1289784073829651, 0.047393226879648864, -0.04351505651138723, -0.14880775437050034, -0.09910094228689559, -0.21476379326777534, 0.04920068329956848, 0.4713610801845789, -0.20328173477901146, -0.29358378813485614, 0.08809330395888537, -0.24501413491088897, -0.2807974238879979, 0.2570967825129628, -0.0993326960364356... |
708.1836 | Fundamental Building Blocks for The Design of A Single-electron
Nanoelectronic Processor | A single-electron random access memory array (RAM) and a single-electron
universal Fredkin gate are designed and simulated. The universality of the
Fredkin gate in combination with the RAM gives the potential of the realization
of an elementary single-electron nanoelectronic processor.
| cond-mat.other | a singleelectron random access memory array ram and a singleelectron universal fredkin gate are designed and simulated the universality of the fredkin gate in combination with the ram gives the potential of the realization of an elementary singleelectron nanoelectronic processor | [['a', 'singleelectron', 'random', 'access', 'memory', 'array', 'ram', 'and', 'a', 'singleelectron', 'universal', 'fredkin', 'gate', 'are', 'designed', 'and', 'simulated', 'the', 'universality', 'of', 'the', 'fredkin', 'gate', 'in', 'combination', 'with', 'the', 'ram', 'gives', 'the', 'potential', 'of', 'the', 'realiza... | [-0.23002465080498952, 0.1553520517572906, -0.002934252077830024, -0.007703576562926173, -0.01975562390871346, -0.28479519810061904, 0.14791710563004018, 0.4089968201704323, -0.23458902179263533, -0.3062596199568361, 0.007615479207015596, -0.2284174118656665, -0.08880868405249202, 0.28750010039657353, 0.027464256310486... |
708.1837 | Using Multi-Threshold Threshold Gates in RTD-based Logic Design. A Case
Study | The basic building blocks for Resonant Tunnelling Diode (RTD) logic circuits
are Threshold Gates (TGs) instead of the conventional Boolean gates (AND, OR,
NAND, NOR) due to the fact that, when designing with RTDs, threshold gates can
be implemented as efficiently as conventional ones, but realize more complex
functio... | cond-mat.other | the basic building blocks for resonant tunnelling diode rtd logic circuits are threshold gates tgs instead of the conventional boolean gates and or nand nor due to the fact that when designing with rtds threshold gates can be implemented as efficiently as conventional ones but realize more complex functions recently rt... | [['the', 'basic', 'building', 'blocks', 'for', 'resonant', 'tunnelling', 'diode', 'rtd', 'logic', 'circuits', 'are', 'threshold', 'gates', 'tgs', 'instead', 'of', 'the', 'conventional', 'boolean', 'gates', 'and', 'or', 'nand', 'nor', 'due', 'to', 'the', 'fact', 'that', 'when', 'designing', 'with', 'rtds', 'threshold', ... | [-0.131010324419881, 0.07818015874565944, -0.024787943344563246, -0.003904429118594398, -0.0269632202775582, -0.2459833784919718, 0.1307679844862002, 0.4132056837172612, -0.23705349942547796, -0.3461446989489638, 0.09539456583620251, -0.22208311935562802, -0.1638001181124507, 0.2686262401043559, -0.06220079977065325, 0... |
708.1838 | Fast rates for support vector machines using Gaussian kernels | For binary classification we establish learning rates up to the order of
$n^{-1}$ for support vector machines (SVMs) with hinge loss and Gaussian RBF
kernels. These rates are in terms of two assumptions on the considered
distributions: Tsybakov's noise assumption to establish a small estimation
error, and a new geome... | math.ST stat.ML stat.TH | for binary classification we establish learning rates up to the order of n1 for support vector machines svms with hinge loss and gaussian rbf kernels these rates are in terms of two assumptions on the considered distributions tsybakovs noise assumption to establish a small estimation error and a new geometric noise con... | [['for', 'binary', 'classification', 'we', 'establish', 'learning', 'rates', 'up', 'to', 'the', 'order', 'of', 'n1', 'for', 'support', 'vector', 'machines', 'svms', 'with', 'hinge', 'loss', 'and', 'gaussian', 'rbf', 'kernels', 'these', 'rates', 'are', 'in', 'terms', 'of', 'two', 'assumptions', 'on', 'the', 'considered'... | [-0.09196659732503887, 0.030886869936521295, -0.08141042242604721, 0.1543475561008989, -0.07975778000169917, -0.1841655088989418, 0.07847921391713279, 0.3806323909047472, -0.25486315137859955, -0.2934599119839789, 0.13219304532372642, -0.19429023125315015, -0.14833785378951816, 0.17097131775904306, -0.14614192415264587... |
708.1839 | A Design of an Autonomous Molecule Loading/Transporting/Unloading System
Using DNA Hybridization and Biomolecular Linear Motors | This paper describes a design of a molecular propagation system in molecular
communication. Molecular communication is a new communication paradigm where
biological and artificially-created nanomachines communicate over a short
distance using molecules. A molecular propagation system in molecular
communication direct... | physics.bio-ph q-bio.MN | this paper describes a design of a molecular propagation system in molecular communication molecular communication is a new communication paradigm where biological and artificiallycreated nanomachines communicate over a short distance using molecules a molecular propagation system in molecular communication directional... | [['this', 'paper', 'describes', 'a', 'design', 'of', 'a', 'molecular', 'propagation', 'system', 'in', 'molecular', 'communication', 'molecular', 'communication', 'is', 'a', 'new', 'communication', 'paradigm', 'where', 'biological', 'and', 'artificiallycreated', 'nanomachines', 'communicate', 'over', 'a', 'short', 'dist... | [-0.24103711708857303, 0.11705829179437276, -0.04821061245329155, -0.031664541522204354, -0.022875178433758647, -0.22647648269163542, 0.11894409772082183, 0.4281049002484794, -0.31373083718496847, -0.2193708436628967, 0.004705510529068609, -0.24628322038456404, -0.18075744953137218, 0.14366981495792666, -0.041969437830... |
708.184 | Prototyping Bio-Nanorobots using Molecular Dynamics Simulation | This paper presents a molecular mechanics study using a molecular dynamics
software (NAMD) coupled to virtual reality (VR) techniques for intuitive
Bio-NanoRobotic prototyping. Using simulated Bio-Nano environments in VR, the
operator can design and characterize through physical simulation and 3-D
visualization the b... | physics.bio-ph | this paper presents a molecular mechanics study using a molecular dynamics software namd coupled to virtual reality vr techniques for intuitive bionanorobotic prototyping using simulated bionano environments in vr the operator can design and characterize through physical simulation and 3d visualization the behavior of ... | [['this', 'paper', 'presents', 'a', 'molecular', 'mechanics', 'study', 'using', 'a', 'molecular', 'dynamics', 'software', 'namd', 'coupled', 'to', 'virtual', 'reality', 'vr', 'techniques', 'for', 'intuitive', 'bionanorobotic', 'prototyping', 'using', 'simulated', 'bionano', 'environments', 'in', 'vr', 'the', 'operator'... | [-0.11237841786103363, 0.057153093415570067, -0.07227182009832021, 0.018195511682821002, -0.03666912124769643, -0.1448261465263018, 0.008285889928377768, 0.4290008446934851, -0.2137067398016757, -0.29296493781928684, 0.054072796111985885, -0.2112598723702212, -0.25150855749590384, 0.18820447244612065, -0.03625191223530... |
708.1841 | A Framework for Computing Transport Properties of Carbon Nanotube-based
Conductance Biochemical Sensors | In this paper we present a framework for fast quantum conductance
calculations of carbon nanotube-based sensing devices targeting aromatic amino
acids within a tight binding approximation. The method begins by a novel
parameterization procedure based on isospectral matrix flows. With the properly
parameterized Hamilt... | cond-mat.mtrl-sci | in this paper we present a framework for fast quantum conductance calculations of carbon nanotubebased sensing devices targeting aromatic amino acids within a tight binding approximation the method begins by a novel parameterization procedure based on isospectral matrix flows with the properly parameterized hamiltonian... | [['in', 'this', 'paper', 'we', 'present', 'a', 'framework', 'for', 'fast', 'quantum', 'conductance', 'calculations', 'of', 'carbon', 'nanotubebased', 'sensing', 'devices', 'targeting', 'aromatic', 'amino', 'acids', 'within', 'a', 'tight', 'binding', 'approximation', 'the', 'method', 'begins', 'by', 'a', 'novel', 'param... | [-0.1343332078111799, 0.11065672107629086, -0.04628104956722573, 0.009651071905146205, 0.02959688092998572, -0.1883442717494051, 0.10742573737087169, 0.4571350929082224, -0.2475496064442651, -0.26948360708775, -0.028555561768467, -0.2691485644808333, -0.2110616863095569, 0.13591594624296321, -0.03117829323194823, 0.071... |
708.1842 | Zero temperature conductance of parallel T-shape double quantum dots | We analyze the zero temperature conductance of a parallel T-shaped double
quantum dot system. We present an analytical expression for the conductance of
the system in terms of the total number of electrons in both quantum dots. Our
results confirm that the system's conductance is strongly influenced by the dot
which ... | cond-mat.mes-hall | we analyze the zero temperature conductance of a parallel tshaped double quantum dot system we present an analytical expression for the conductance of the system in terms of the total number of electrons in both quantum dots our results confirm that the systems conductance is strongly influenced by the dot which is not... | [['we', 'analyze', 'the', 'zero', 'temperature', 'conductance', 'of', 'a', 'parallel', 'tshaped', 'double', 'quantum', 'dot', 'system', 'we', 'present', 'an', 'analytical', 'expression', 'for', 'the', 'conductance', 'of', 'the', 'system', 'in', 'terms', 'of', 'the', 'total', 'number', 'of', 'electrons', 'in', 'both', '... | [-0.19038590543549244, 0.10053710145142067, -0.03862265549914937, -0.01346624652776395, 0.03547794925389995, -0.1360279114746397, 0.047920198781533876, 0.3467176594364811, -0.23102222047221493, -0.29288793300134197, 0.005684509952093514, -0.30328248172316336, -0.20192741980435144, 0.2760275911907075, -0.058893662877380... |
708.1843 | Electrical Characterisation of Ultra-thin SAM Structures | The way of reduction of metal oxyde semiconductor (MOS) structures is going
to reach limitations and new devices have to be explored as an alternative to
MOS technology. Molecular electronic and more particularly
self-assembly-molecular technique on silicon substrate gives interesting
results as seen in the literatur... | cond-mat.mtrl-sci | the way of reduction of metal oxyde semiconductor mos structures is going to reach limitations and new devices have to be explored as an alternative to mos technology molecular electronic and more particularly selfassemblymolecular technique on silicon substrate gives interesting results as seen in the literature we ar... | [['the', 'way', 'of', 'reduction', 'of', 'metal', 'oxyde', 'semiconductor', 'mos', 'structures', 'is', 'going', 'to', 'reach', 'limitations', 'and', 'new', 'devices', 'have', 'to', 'be', 'explored', 'as', 'an', 'alternative', 'to', 'mos', 'technology', 'molecular', 'electronic', 'and', 'more', 'particularly', 'selfasse... | [-0.052805747819365936, 0.11752709310612772, -0.05891813670750708, -0.010042228678503306, -0.016958069350221195, -0.20509323841397417, 0.05916606227365264, 0.4832092479569837, -0.25832291309779976, -0.3359368305420503, 0.06598048349987948, -0.32298932526318824, -0.09038191349609406, 0.2504061884566909, -0.0418317871076... |
708.1844 | Low Temperature Investigation of Electrical Conduction in Polysilicon:
Simulation and Experiment | Investigation of electrical conduction in polysilicon nanowires (polySiNW)
with nanograins (5 to 20nm), based on Monte Carlo (MC) simulations and
electrical measurements from 4K to 300K are presented. Some irregular Coulomb
Oscillations (CO) are observed at temperatures lower than 200K showing several
period widths d... | cond-mat.mtrl-sci | investigation of electrical conduction in polysilicon nanowires polysinw with nanograins 5 to 20nm based on monte carlo mc simulations and electrical measurements from 4k to 300k are presented some irregular coulomb oscillations co are observed at temperatures lower than 200k showing several period widths due to the ra... | [['investigation', 'of', 'electrical', 'conduction', 'in', 'polysilicon', 'nanowires', 'polysinw', 'with', 'nanograins', '5', 'to', '20nm', 'based', 'on', 'monte', 'carlo', 'mc', 'simulations', 'and', 'electrical', 'measurements', 'from', '4k', 'to', '300k', 'are', 'presented', 'some', 'irregular', 'coulomb', 'oscillat... | [-0.12643315575737507, 0.21667961008311248, -0.026265050690621138, 0.025705245258286595, 0.010933231768663973, -0.16880257549136876, 0.07178991691768169, 0.434702252715826, -0.22128736646473407, -0.3838849277794361, 0.036498630048707126, -0.33327494955062864, -0.024646696742624045, 0.24678290741890668, 0.03341446676850... |
708.1845 | Measurements of CP Violation Parameters in B0 -> Kspi0pi0 and B0 -> KsKs
Decays | We present a measurement of the CP violation parameters in B0 ->Kspi0pi0 and
B0 -> KsKs decays using a data sample containing 657x10^6 BBbar pairs collected
with the Belle detector at the KEKB asymmetric-energy e+e- collider operating
at the Y(4S) resonance. We measure
SKspi0pi0 = +0.43+/-0.49+/-0.09,
AKspi0pi0 =... | hep-ex | we present a measurement of the cp violation parameters in b0 kspi0pi0 and b0 ksks decays using a data sample containing 657x106 bbbar pairs collected with the belle detector at the kekb asymmetricenergy ee collider operating at the y4s resonance we measure skspi0pi0 043049009 akspi0pi0 017024006 sksks 038077008 and ak... | [['we', 'present', 'a', 'measurement', 'of', 'the', 'cp', 'violation', 'parameters', 'in', 'b0', 'kspi0pi0', 'and', 'b0', 'ksks', 'decays', 'using', 'a', 'data', 'sample', 'containing', '657x106', 'bbbar', 'pairs', 'collected', 'with', 'the', 'belle', 'detector', 'at', 'the', 'kekb', 'asymmetricenergy', 'ee', 'collider... | [-0.10977705705137748, 0.1314257293728725, -0.0667946485907964, 0.04025352845530746, -0.06978506039452458, -0.14719784953895043, 0.11399693387112457, 0.2617288539801144, -0.16138798335813126, -0.2744805928108827, 0.0067668544053855655, -0.5265191086427361, 0.1092706064008317, 0.15238649614664884, 0.09943078969657984, 0... |
708.1846 | Tunable Integrated-Optics Nanoscaled Devices Based on Magnetic Photonic
Crystals | Magnetooptical properties of magnetic photonic crystals have been
investigated in the view of their possible applications for the modern
integrated-optics devices. A "transfer matrices" formalism was expanded for the
case of oblique light incidence on the periodic nanoscaled magnetic
multilayered systems. Several new... | cond-mat.mtrl-sci | magnetooptical properties of magnetic photonic crystals have been investigated in the view of their possible applications for the modern integratedoptics devices a transfer matrices formalism was expanded for the case of oblique light incidence on the periodic nanoscaled magnetic multilayered systems several new effect... | [['magnetooptical', 'properties', 'of', 'magnetic', 'photonic', 'crystals', 'have', 'been', 'investigated', 'in', 'the', 'view', 'of', 'their', 'possible', 'applications', 'for', 'the', 'modern', 'integratedoptics', 'devices', 'a', 'transfer', 'matrices', 'formalism', 'was', 'expanded', 'for', 'the', 'case', 'of', 'obl... | [-0.17918845917787016, 0.16071065114617036, 0.005855489949074884, 0.014626634462426106, -0.08023055666126311, -0.11703549084753224, 0.01726301149998714, 0.47678698929181945, -0.2381930003563563, -0.3136166312469868, 0.08982049725091201, -0.26280021996353753, -0.14428556929609235, 0.2949229280347936, 0.0374063503120207,... |
708.1847 | Measurements of Luminescence from Cleaved Silicon | This paper outlines the results from experiments performed to gain further
information about the structure and properties of cleaved silicon surfaces,
using vacuum cleavage luminescence detection methods. The experiments involved
detecting the luminescence produced by cleaving thin silicon plates within a
high vacuum... | cond-mat.mtrl-sci | this paper outlines the results from experiments performed to gain further information about the structure and properties of cleaved silicon surfaces using vacuum cleavage luminescence detection methods the experiments involved detecting the luminescence produced by cleaving thin silicon plates within a high vacuum by ... | [['this', 'paper', 'outlines', 'the', 'results', 'from', 'experiments', 'performed', 'to', 'gain', 'further', 'information', 'about', 'the', 'structure', 'and', 'properties', 'of', 'cleaved', 'silicon', 'surfaces', 'using', 'vacuum', 'cleavage', 'luminescence', 'detection', 'methods', 'the', 'experiments', 'involved', ... | [-0.04072559309953993, 0.13788646574962926, -0.07780976861037991, -0.032169252198913124, -0.002303487502715804, -0.09532194224778902, 0.0760088538941504, 0.4546333034607497, -0.26405689312483777, -0.3158335549926216, 0.07596803868020123, -0.32592534441500903, -0.08506579819050702, 0.21339036073874343, -0.02445594029585... |
708.1848 | Self-Organization of a 2D Lattice on a Surface of Ge Single Crystal
after Irradiation with Yag: ND Laser | Experimentally observed self-organization of a 2D lattice on the surface of
Ge single crystal after irradiation by pulsed YAG: Nd laser is repoted. The
calculation of time depended distribution of temperature in bulk of the Ge
sample show that overheating of the crystal lattice occurs at laser radiation
intensities e... | cond-mat.mtrl-sci | experimentally observed selforganization of a 2d lattice on the surface of ge single crystal after irradiation by pulsed yag nd laser is repoted the calculation of time depended distribution of temperature in bulk of the ge sample show that overheating of the crystal lattice occurs at laser radiation intensities exceed... | [['experimentally', 'observed', 'selforganization', 'of', 'a', '2d', 'lattice', 'on', 'the', 'surface', 'of', 'ge', 'single', 'crystal', 'after', 'irradiation', 'by', 'pulsed', 'yag', 'nd', 'laser', 'is', 'repoted', 'the', 'calculation', 'of', 'time', 'depended', 'distribution', 'of', 'temperature', 'in', 'bulk', 'of',... | [-0.11438979503388207, 0.312616692200579, -0.03268719306733045, -0.06505847197776246, 0.06816499540582299, -0.12354535279209139, 0.06013518543827727, 0.487891697290319, -0.2358230550394014, -0.3032827740880074, -0.004077222536714679, -0.3093699551773844, -0.0072638622562711435, 0.22878138933123815, 0.06365995779978456,... |
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