id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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709.1235 | Monotonicity for entrywise functions of matrices | We characterize real functions $f$ on an interval $(-\alpha,\alpha)$ for
which the entrywise matrix function $[a_{ij}] \mapsto [f(a_{ij})]$ is positive,
monotone and convex, respectively, in the positive semidefiniteness order.
Fractional power functions are exemplified and related weak majorizations are
shown.
| math.FA | we characterize real functions f on an interval alphaalpha for which the entrywise matrix function a_ij mapsto fa_ij is positive monotone and convex respectively in the positive semidefiniteness order fractional power functions are exemplified and related weak majorizations are shown | [['we', 'characterize', 'real', 'functions', 'f', 'on', 'an', 'interval', 'alphaalpha', 'for', 'which', 'the', 'entrywise', 'matrix', 'function', 'a_ij', 'mapsto', 'fa_ij', 'is', 'positive', 'monotone', 'and', 'convex', 'respectively', 'in', 'the', 'positive', 'semidefiniteness', 'order', 'fractional', 'power', 'functi... | [-0.14406293838615775, 0.1023551669913056, 0.053950028775848057, 0.10056133113960784, -0.007466345474025921, -0.15567001465119815, -0.06459976585679933, 0.41238140657936273, -0.3506570491743715, -0.14898220324692757, 0.12052733857662563, -0.3624750655144453, -0.19403738832395329, 0.16152586827152654, -0.031972831703330... |
709.1236 | The metal abundance of circumnuclear star forming regions in early type
spirals. Spectrophotometric observations | We have obtained long-slit observations in the optical and near infrared of
12 circumnuclear HII regions (CNSFR) in the early type spiral galaxies NGC
2903, NGC 3351 and NGC 3504 with the aim of deriving their chemical abundances.
Only for one of the regions, the [SIII] $\lambda$ 6312 \AA was detected
providing, toge... | astro-ph | we have obtained longslit observations in the optical and near infrared of 12 circumnuclear hii regions cnsfr in the early type spiral galaxies ngc 2903 ngc 3351 and ngc 3504 with the aim of deriving their chemical abundances only for one of the regions the siii lambda 6312 aa was detected providing together with the n... | [['we', 'have', 'obtained', 'longslit', 'observations', 'in', 'the', 'optical', 'and', 'near', 'infrared', 'of', '12', 'circumnuclear', 'hii', 'regions', 'cnsfr', 'in', 'the', 'early', 'type', 'spiral', 'galaxies', 'ngc', '2903', 'ngc', '3351', 'and', 'ngc', '3504', 'with', 'the', 'aim', 'of', 'deriving', 'their', 'che... | [-0.008169223026909152, 0.07968573534919676, 0.015173672779876688, 0.062235040043589276, 0.0013719211821131107, -0.058831408636586015, 0.04458014592016742, 0.4451349352991768, -0.09912287331532871, -0.3514484076013145, -0.0007731154145497511, -0.3017047670222986, 0.034164285546193746, 0.17575760659628084, -0.0580866840... |
709.1237 | Transition rates for a S \ge 1 model coupled to a phonon bath | We investigate transition rates between different spin configurations for $S
\ge 1$ spins weakly coupled to a $d$-dimensional phonon bath. This study is
motivated by understanding observed magnetization relaxation as a function of
temperature in diverse magnetic systems such as arrays of magnetic
nanoparticles and ma... | cond-mat.mtrl-sci | we investigate transition rates between different spin configurations for s ge 1 spins weakly coupled to a ddimensional phonon bath this study is motivated by understanding observed magnetization relaxation as a function of temperature in diverse magnetic systems such as arrays of magnetic nanoparticles and magnetic mo... | [['we', 'investigate', 'transition', 'rates', 'between', 'different', 'spin', 'configurations', 'for', 's', 'ge', '1', 'spins', 'weakly', 'coupled', 'to', 'a', 'ddimensional', 'phonon', 'bath', 'this', 'study', 'is', 'motivated', 'by', 'understanding', 'observed', 'magnetization', 'relaxation', 'as', 'a', 'function', '... | [-0.16602299131675444, 0.21680846654490593, -0.03702205637428187, 0.052642946618618396, -0.012669468993571267, -0.14848045064414392, 0.061214994146275466, 0.38353155367539743, -0.2816552132430639, -0.27284230412776345, 0.047404282292541094, -0.29035436154218086, -0.07908143953707496, 0.18641322440426075, 0.074353732898... |
709.1238 | Corrections to the fine structure constant in higher dimensional global
monopole spacetime | In this paper we use the Generalized Uncertainty Principle in order to obtain
the corrections to the fine structure constant in (D+1)-dimensional global
monopole spacetime. The result is particularized to D-dimensional spacetime. We
also discuss the particular case D=3 corresponding to the (3+1)-dimensional
global mo... | gr-qc hep-th | in this paper we use the generalized uncertainty principle in order to obtain the corrections to the fine structure constant in d1dimensional global monopole spacetime the result is particularized to ddimensional spacetime we also discuss the particular case d3 corresponding to the 31dimensional global monopole spaceti... | [['in', 'this', 'paper', 'we', 'use', 'the', 'generalized', 'uncertainty', 'principle', 'in', 'order', 'to', 'obtain', 'the', 'corrections', 'to', 'the', 'fine', 'structure', 'constant', 'in', 'd1dimensional', 'global', 'monopole', 'spacetime', 'the', 'result', 'is', 'particularized', 'to', 'ddimensional', 'spacetime',... | [-0.1110986966194342, 0.06435043314907132, -0.05008881482417169, 0.132190250751117, -0.10248104888824341, -0.060805700415664396, -0.04206046771571931, 0.3087775896546309, -0.2246330090717453, -0.24827112273677535, 0.07629920156804197, -0.22572418261805308, -0.16218319381384746, 0.05680773633977641, -0.10239859714942134... |
709.1239 | Bridging over p-wave pi-production and weak processes in few-nucleon
systems with chiral perturbation theory | I study an aspect of chiral perturbation theory (\chi PT) which enables one
to ``bridge'' different reactions. That is, an operator fixed in one of the
reactions can then be used to predict the other. For this purpose, I calculate
the partial wave amplitude for the p-wave pion production (pp\to pn\pi^+) using
the pio... | nucl-th | i study an aspect of chiral perturbation theory chi pt which enables one to bridge different reactions that is an operator fixed in one of the reactions can then be used to predict the other for this purpose i calculate the partial wave amplitude for the pwave pion production ppto pnpi using the pion production operato... | [['i', 'study', 'an', 'aspect', 'of', 'chiral', 'perturbation', 'theory', 'chi', 'pt', 'which', 'enables', 'one', 'to', 'bridge', 'different', 'reactions', 'that', 'is', 'an', 'operator', 'fixed', 'in', 'one', 'of', 'the', 'reactions', 'can', 'then', 'be', 'used', 'to', 'predict', 'the', 'other', 'for', 'this', 'purpos... | [-0.08414500419815034, 0.14645774999965647, -0.08419302431167526, 0.08198295818043755, -0.0597151876528906, -0.09958975032728377, 0.0370797057916699, 0.30286805319506266, -0.2532280715564713, -0.219714082419612, 0.03718998960186788, -0.33026795386942714, -0.0878473297584109, 0.12452578088309307, 0.06600253590012546, 0.... |
709.124 | Generalized Second Law and phantom Cosmology: accreting black holes | The accretion of phantom fields by black holes within a thermodynamic context
is addressed. For a fluid violating the dominant energy condition, case of a
phantom fluid, the Euler and Gibbs relations permit two different possibilities
for the entropy and temperature: a situation in which the entropy is negative
and t... | gr-qc astro-ph | the accretion of phantom fields by black holes within a thermodynamic context is addressed for a fluid violating the dominant energy condition case of a phantom fluid the euler and gibbs relations permit two different possibilities for the entropy and temperature a situation in which the entropy is negative and the tem... | [['the', 'accretion', 'of', 'phantom', 'fields', 'by', 'black', 'holes', 'within', 'a', 'thermodynamic', 'context', 'is', 'addressed', 'for', 'a', 'fluid', 'violating', 'the', 'dominant', 'energy', 'condition', 'case', 'of', 'a', 'phantom', 'fluid', 'the', 'euler', 'and', 'gibbs', 'relations', 'permit', 'two', 'differe... | [-0.13317119726149815, 0.2061466019274327, -0.0631169257447613, 0.13488834460761867, -0.047867876079858, -0.18295126289034086, 0.02655680444988891, 0.2569408166038729, -0.1975252976841599, -0.272007056131252, 0.1163503785794397, -0.2889588328714, -0.03288848606876376, 0.19258438459815064, -0.027175808252331658, 0.01119... |
709.1241 | Homotopically non-trivial maps with small k-dilation | We construct homotopically non-trivial maps from S^m to S^n with arbitrarily
small 3-dilation for certain pairs (m,n). The simplest example is m=4, n=3.
Other examples include arbitrarily large values of m and n. We show that a
homotopy class in pi_7(S^4) can be represented by maps with arbitrarily small
4-dilation i... | math.DG | we construct homotopically nontrivial maps from sm to sn with arbitrarily small 3dilation for certain pairs mn the simplest example is m4 n3 other examples include arbitrarily large values of m and n we show that a homotopy class in pi_7s4 can be represented by maps with arbitrarily small 4dilation if and only if the c... | [['we', 'construct', 'homotopically', 'nontrivial', 'maps', 'from', 'sm', 'to', 'sn', 'with', 'arbitrarily', 'small', '3dilation', 'for', 'certain', 'pairs', 'mn', 'the', 'simplest', 'example', 'is', 'm4', 'n3', 'other', 'examples', 'include', 'arbitrarily', 'large', 'values', 'of', 'm', 'and', 'n', 'we', 'show', 'that... | [-0.14672874283384194, 0.19624605209312657, 0.03421601029959592, 0.09312851251610978, -0.04829030326482925, -0.2539234786463732, -0.023013710162856364, 0.3861399095166813, -0.27094269198450177, -0.31745620244605977, 0.07693317295263775, -0.29406250864267347, -0.15954153975048527, 0.19825702597048472, -0.079660123759161... |
709.1242 | Noise from metallic surfaces -- effects of charge diffusion | Non-local electrodynamic models are developed for describing metallic
surfaces for a diffusive metal. The electric field noise at a distance z_0 from
the surface is evaluated and compared with data from ion chips that show
anomalous heating with a noise power decaying as z_0^{-4}. We find that high
surface diffusion ... | quant-ph | nonlocal electrodynamic models are developed for describing metallic surfaces for a diffusive metal the electric field noise at a distance z_0 from the surface is evaluated and compared with data from ion chips that show anomalous heating with a noise power decaying as z_04 we find that high surface diffusion can accou... | [['nonlocal', 'electrodynamic', 'models', 'are', 'developed', 'for', 'describing', 'metallic', 'surfaces', 'for', 'a', 'diffusive', 'metal', 'the', 'electric', 'field', 'noise', 'at', 'a', 'distance', 'z_0', 'from', 'the', 'surface', 'is', 'evaluated', 'and', 'compared', 'with', 'data', 'from', 'ion', 'chips', 'that', ... | [-0.08051336005499417, 0.16473734607412058, -0.06283154051581567, 0.07834195305635645, 0.01045073106969622, -0.2167406783947213, -0.022047020139342004, 0.3674155941571702, -0.23689315258101984, -0.3059181253341111, 0.03360712866044857, -0.3375270690091632, -0.11142581220377576, 0.2595110078426925, -0.004539356634698130... |
709.1243 | The existence of two closed geodesics on every Finsler 2-sphere | In this paper, we prove that for every Finsler metric on the 2-dimensional
sphere there exist at least two distinct prime closed geodesics. For the case
of the two-sphere, this solves an open problem posed by D. V. Anosov in 1974.
| math.SG math.DS | in this paper we prove that for every finsler metric on the 2dimensional sphere there exist at least two distinct prime closed geodesics for the case of the twosphere this solves an open problem posed by d v anosov in 1974 | [['in', 'this', 'paper', 'we', 'prove', 'that', 'for', 'every', 'finsler', 'metric', 'on', 'the', '2dimensional', 'sphere', 'there', 'exist', 'at', 'least', 'two', 'distinct', 'prime', 'closed', 'geodesics', 'for', 'the', 'case', 'of', 'the', 'twosphere', 'this', 'solves', 'an', 'open', 'problem', 'posed', 'by', 'd', '... | [-0.2372205517277485, 0.08541292482284295, -0.014028779969255372, 0.04628419188396415, -0.034158347469822666, -0.20571485125437017, -0.03503424144724793, 0.3369054333193273, -0.27798414843656666, -0.1987535330444211, 0.06161693911204433, -0.32192039339825873, -0.16969599741760913, 0.21488781818529454, -0.14691048354001... |
709.1244 | Scaling of Anisotropic Flows and Nuclear Equation of State in
Intermediate Energy Heavy Ion Collisions | Elliptic flow ($v_2$) and hexadecupole flow ($v_4$) of light clusters have
been studied in details for 25 MeV/nucleon $^{86}$Kr + $^{124}$Sn at large
impact parameters by Quantum Molecular Dynamics model with different potential
parameters. Four parameter sets which include soft or hard equation of state
(EOS) with/w... | nucl-th | elliptic flow v_2 and hexadecupole flow v_4 of light clusters have been studied in details for 25 mevnucleon 86kr 124sn at large impact parameters by quantum molecular dynamics model with different potential parameters four parameter sets which include soft or hard equation of state eos withwithout symmetry energy term... | [['elliptic', 'flow', 'v_2', 'and', 'hexadecupole', 'flow', 'v_4', 'of', 'light', 'clusters', 'have', 'been', 'studied', 'in', 'details', 'for', '25', 'mevnucleon', '86kr', '124sn', 'at', 'large', 'impact', 'parameters', 'by', 'quantum', 'molecular', 'dynamics', 'model', 'with', 'different', 'potential', 'parameters', ... | [-0.11045912224638822, 0.21030729518689473, -0.11153582176514741, 0.05835839935642635, -0.03974338687859989, -0.1377560602717808, -0.024137737415730953, 0.3574810900051018, -0.22124413711757496, -0.34939877047717316, 0.05013548966721985, -0.31752713600751653, -0.027077005590023153, 0.19267725801047195, 0.05702220279209... |
709.1245 | Comparison of elastic electron or positron scattering from proton-rich
nuclei | We investigate the cross sections of the elastic electron or positron
scattering from $^{208}$Pb, $^{12}$C, $^{12,16}$O and $^{28, 32}$S by the
relativistic partial-wave expansion method using the static charge density
distribution from the self-consistent relativistic mean field model and also
calculate the charge f... | nucl-th | we investigate the cross sections of the elastic electron or positron scattering from 208pb 12c 1216o and 28 32s by the relativistic partialwave expansion method using the static charge density distribution from the selfconsistent relativistic mean field model and also calculate the charge form factor for 12 16o and 28... | [['we', 'investigate', 'the', 'cross', 'sections', 'of', 'the', 'elastic', 'electron', 'or', 'positron', 'scattering', 'from', '208pb', '12c', '1216o', 'and', '28', '32s', 'by', 'the', 'relativistic', 'partialwave', 'expansion', 'method', 'using', 'the', 'static', 'charge', 'density', 'distribution', 'from', 'the', 'se... | [0.0012186298405544626, 0.16870824764482678, -0.072276649168796, 0.130069568215145, 0.0737297425719185, -0.047169532518212993, 0.017051372449431154, 0.34462570481830174, -0.17040513943259913, -0.31462774013386174, -0.03675110275960631, -0.37319890146868095, -0.017389729391369554, 0.14700577488789957, 0.1540868176147341... |
709.1246 | Andreev Reflection in Heavy-Fermion Superconductors and Order Parameter
Symmetry in CeCoIn_5 | Differential conductance spectra are obtained from nanoscale junctions on the
heavy-fermion superconductor CeCoIn$_5$ along three major crystallographic
orientations. Consistency and reproducibility of characteristic features among
the junctions ensure their spectroscopic nature. All junctions show a similar
conducta... | cond-mat.supr-con cond-mat.str-el | differential conductance spectra are obtained from nanoscale junctions on the heavyfermion superconductor cecoin_5 along three major crystallographic orientations consistency and reproducibility of characteristic features among the junctions ensure their spectroscopic nature all junctions show a similar conductance asy... | [['differential', 'conductance', 'spectra', 'are', 'obtained', 'from', 'nanoscale', 'junctions', 'on', 'the', 'heavyfermion', 'superconductor', 'cecoin_5', 'along', 'three', 'major', 'crystallographic', 'orientations', 'consistency', 'and', 'reproducibility', 'of', 'characteristic', 'features', 'among', 'the', 'junctio... | [-0.18145899816246872, 0.09149813722006829, -0.0905920247377997, 0.06528081856667996, -0.05186419283378531, -0.18190986059013414, 0.06411568642678586, 0.3568172899498181, -0.20919756818224083, -0.3302130440758033, -0.059409990650601686, -0.3627877122510902, -0.10879319698803804, 0.1904319212115793, 0.04730613815852187,... |
709.1247 | The Hopf invariant and simplex straightening | Let M be a closed 3-manifold which can be triangulated with N simplices. We
prove that any map from M to a genus 2 surface has Hopf invariant at most C^N.
Let X be a closed oriented hyperbolic 3-manifold with injectivity radius less
than epsilon at one point. If there is a degree non-zero map from M to X, then
we pro... | math.DG | let m be a closed 3manifold which can be triangulated with n simplices we prove that any map from m to a genus 2 surface has hopf invariant at most cn let x be a closed oriented hyperbolic 3manifold with injectivity radius less than epsilon at one point if there is a degree nonzero map from m to x then we prove that ep... | [['let', 'm', 'be', 'a', 'closed', '3manifold', 'which', 'can', 'be', 'triangulated', 'with', 'n', 'simplices', 'we', 'prove', 'that', 'any', 'map', 'from', 'm', 'to', 'a', 'genus', '2', 'surface', 'has', 'hopf', 'invariant', 'at', 'most', 'cn', 'let', 'x', 'be', 'a', 'closed', 'oriented', 'hyperbolic', '3manifold', 'w... | [-0.21112953635918744, 0.13604651942766985, -0.10702539264799699, -0.017748377775526878, -0.05360130543875344, -0.26810221497298165, -0.017326240126481828, 0.3775547497412738, -0.30649379388299114, -0.23591844173257842, 0.08638000426649609, -0.3176597598940134, -0.1069727598258075, 0.16270567304523223, -0.1411397122531... |
709.1248 | Gli Strumenti Scientifici di Interesse Storico di tre antiche Scuole
Medie Superiori di Bergamo ("Lussana", "Vittorio Emanuele", e "Quarenghi") | Wherever old Universities exist [in Europe, for example: Italy being not the
last one], there can be found Scientific Instruments of Historical Interest,
e.g., for Physics -which is the case we are concerned with here;- even if
proper attention has been paid to such an exceptional heritage only during the
last half a... | physics.ed-ph physics.hist-ph | wherever old universities exist in europe for example italy being not the last one there can be found scientific instruments of historical interest eg for physics which is the case we are concerned with here even if proper attention has been paid to such an exceptional heritage only during the last half a century we st... | [['wherever', 'old', 'universities', 'exist', 'in', 'europe', 'for', 'example', 'italy', 'being', 'not', 'the', 'last', 'one', 'there', 'can', 'be', 'found', 'scientific', 'instruments', 'of', 'historical', 'interest', 'eg', 'for', 'physics', 'which', 'is', 'the', 'case', 'we', 'are', 'concerned', 'with', 'here', 'even... | [-0.06941656518405567, 0.11912727504798701, -0.04587575783415769, 0.09193071044519074, -0.10562860082112044, -0.12142158623856421, 0.051841476367187354, 0.34424867765925876, -0.19246132368094881, -0.3546344466361712, 0.16554397175420674, -0.35157646573314744, -0.07847733336168673, 0.20888786158610748, -0.11609268193361... |
709.1249 | Emergence of Symmetry in Complex Networks | Many real networks have been found to have a rich degree of symmetry, which
is a very important structural property of complex network, yet has been rarely
studied so far. And where does symmetry comes from has not been explained. To
explore the mechanism underlying symmetry of the networks, we studied
statistics of ... | physics.soc-ph | many real networks have been found to have a rich degree of symmetry which is a very important structural property of complex network yet has been rarely studied so far and where does symmetry comes from has not been explained to explore the mechanism underlying symmetry of the networks we studied statistics of certain... | [['many', 'real', 'networks', 'have', 'been', 'found', 'to', 'have', 'a', 'rich', 'degree', 'of', 'symmetry', 'which', 'is', 'a', 'very', 'important', 'structural', 'property', 'of', 'complex', 'network', 'yet', 'has', 'been', 'rarely', 'studied', 'so', 'far', 'and', 'where', 'does', 'symmetry', 'comes', 'from', 'has',... | [-0.1519595087492609, 0.07346377526204485, -0.08791970247094628, 0.11137295915550031, -0.09347020943909336, -0.15163033000220927, -0.00849829297786688, 0.39767546843573015, -0.26364427986417843, -0.28880899380344677, 0.06115186742339146, -0.2265243144664804, -0.2511618314858745, 0.09953280661412624, -0.0426920952946495... |
709.125 | Strongly Resonant Transmission of Electromagnetic Radiation in Periodic
Anisotropic Layered Media | The electromagnetic dispersion in periodic layered media can be tailored and
their resonant properties can be considerably improved by utilizing anisotropic
materials. Periodic structures with a photonic band edge split into two parts,
or so-called split band edge, exhibit superior resonant properties including
excep... | physics.optics | the electromagnetic dispersion in periodic layered media can be tailored and their resonant properties can be considerably improved by utilizing anisotropic materials periodic structures with a photonic band edge split into two parts or socalled split band edge exhibit superior resonant properties including exceptional... | [['the', 'electromagnetic', 'dispersion', 'in', 'periodic', 'layered', 'media', 'can', 'be', 'tailored', 'and', 'their', 'resonant', 'properties', 'can', 'be', 'considerably', 'improved', 'by', 'utilizing', 'anisotropic', 'materials', 'periodic', 'structures', 'with', 'a', 'photonic', 'band', 'edge', 'split', 'into', '... | [-0.2084393132938428, 0.1751160383563923, -0.007507735910417324, -0.008345087725941218, -0.07238428852405776, -0.18818867190615432, 0.038177926731662135, 0.47037182919932213, -0.26984124080267513, -0.31020146332945403, 0.07537531626709669, -0.28850265730465396, -0.13952768692129364, 0.19491789846555488, 0.0115433270922... |
709.1251 | Geomagnetic Field Effects on the Imaging Air Shower Cherenkov Technique | Imaging Air Cherenkov Telescopes (IACTs) detect the Cherenkov light flashes
of Extended Air Showers (EAS) triggered by very high energy (VHE) gamma-rays
impinging on the Earth's atmosphere. Due to the overwhelming background from
hadron induced EAS, the discrimination of the rare gamma-like events is rather
difficult... | astro-ph | imaging air cherenkov telescopes iacts detect the cherenkov light flashes of extended air showers eas triggered by very high energy vhe gammarays impinging on the earths atmosphere due to the overwhelming background from hadron induced eas the discrimination of the rare gammalike events is rather difficult in particula... | [['imaging', 'air', 'cherenkov', 'telescopes', 'iacts', 'detect', 'the', 'cherenkov', 'light', 'flashes', 'of', 'extended', 'air', 'showers', 'eas', 'triggered', 'by', 'very', 'high', 'energy', 'vhe', 'gammarays', 'impinging', 'on', 'the', 'earths', 'atmosphere', 'due', 'to', 'the', 'overwhelming', 'background', 'from'... | [-0.04777796968789069, 0.2966883904865383, -0.04115749231081397, 0.178874215680278, -0.04148923462840714, -0.0348015470496778, 0.008366382222563501, 0.4456138015828199, -0.1906632133279114, -0.4235489626104633, 0.03169442074824243, -0.32512129799255896, -0.037323543203196356, 0.255217373160468, 0.005108018368778247, -0... |
709.1252 | The Geometry of Toric Hyperk\"ahler Varieties | In this survey article we describe the geometry of toric hyperk\"ahler
varieties, which are hyperk\"ahler quotients of the quaternionic vector spaces
by tori. In particular, we discuss the Betti numbers, the cohomology ring, and
variation of hyperk\"ahler structures of these spaces with many improved
results and proo... | math.DG math.SG | in this survey article we describe the geometry of toric hyperkahler varieties which are hyperkahler quotients of the quaternionic vector spaces by tori in particular we discuss the betti numbers the cohomology ring and variation of hyperkahler structures of these spaces with many improved results and proofs | [['in', 'this', 'survey', 'article', 'we', 'describe', 'the', 'geometry', 'of', 'toric', 'hyperkahler', 'varieties', 'which', 'are', 'hyperkahler', 'quotients', 'of', 'the', 'quaternionic', 'vector', 'spaces', 'by', 'tori', 'in', 'particular', 'we', 'discuss', 'the', 'betti', 'numbers', 'the', 'cohomology', 'ring', 'an... | [-0.2088601241579299, 0.032578298861676076, -0.04808715880016222, 0.169151234963136, -0.10971713622913082, -0.08375086359917483, -0.05888195908529327, 0.3474229193352004, -0.30330817555969064, -0.2142265884483114, 0.15461351233534515, -0.2142310494239977, -0.2080986688230583, 0.18587554440377874, -0.24050975432421298, ... |
709.1253 | The Entire Cyclic Cohomology of Noncommutative 2-Tori | Our aim in this paper is to compute the entire cyclic cohomology of
noncommutative 2-tori. First of all, we clarify their algebraic structure of
noncommutative 2-tori as a $F^*$-algebra, according to the idea of
Elliott-Evans. Actually, they are the inductive limit of subhomogeneous
$F^*$-algebras. Using such a resul... | math.KT math.QA | our aim in this paper is to compute the entire cyclic cohomology of noncommutative 2tori first of all we clarify their algebraic structure of noncommutative 2tori as a falgebra according to the idea of elliottevans actually they are the inductive limit of subhomogeneous falgebras using such a result we compute their en... | [['our', 'aim', 'in', 'this', 'paper', 'is', 'to', 'compute', 'the', 'entire', 'cyclic', 'cohomology', 'of', 'noncommutative', '2tori', 'first', 'of', 'all', 'we', 'clarify', 'their', 'algebraic', 'structure', 'of', 'noncommutative', '2tori', 'as', 'a', 'falgebra', 'according', 'to', 'the', 'idea', 'of', 'elliottevans'... | [-0.18946015826211526, 0.09402084015309811, -0.10933542666383661, 0.10350490469539252, -0.12509726150534473, -0.0781518964884946, 0.007983914524531708, 0.35484976911774047, -0.372490518912673, -0.20401825291606096, 0.1500456369893912, -0.1904512324155523, -0.19010729377086347, 0.16339664742923699, -0.1448672906567271, ... |
709.1254 | Z+(4430) as a cusp in D*(2010)Dbar_1(2420) | The Z^+(4430) observed by Belle is explained naturally as a threshold cusp in
the D*(2010)Dbar_1(2420) system.
| hep-ph | the z4430 observed by belle is explained naturally as a threshold cusp in the d2010dbar_12420 system | [['the', 'z4430', 'observed', 'by', 'belle', 'is', 'explained', 'naturally', 'as', 'a', 'threshold', 'cusp', 'in', 'the', 'd2010dbar_12420', 'system']] | [-0.1625451066841682, 0.16812174456814924, -0.11097620005408923, 0.20831138147817305, -0.05434021838009358, -0.13574856367583077, 0.08657616687317689, 0.22906298111192883, -0.20093017915884653, -0.2843533232808113, -0.015591993749452134, -0.27562439665198324, -0.17756979341308277, 0.1752214789390564, 0.0109657064701120... |
709.1255 | Local structure of algebraic monoids | We describe the local structure of an irreducible algebraic monoid $M$ at an
idempotent element $e$. When $e$ is minimal, we show that $M$ is an induced
variety over the kernel $MeM$ (a homogeneous space) with fibre the two-sided
stabilizer $M_e$ (a connected affine monoid having a zero element and a dense
unit group... | math.AG | we describe the local structure of an irreducible algebraic monoid m at an idempotent element e when e is minimal we show that m is an induced variety over the kernel mem a homogeneous space with fibre the twosided stabilizer m_e a connected affine monoid having a zero element and a dense unit group this yields the irr... | [['we', 'describe', 'the', 'local', 'structure', 'of', 'an', 'irreducible', 'algebraic', 'monoid', 'm', 'at', 'an', 'idempotent', 'element', 'e', 'when', 'e', 'is', 'minimal', 'we', 'show', 'that', 'm', 'is', 'an', 'induced', 'variety', 'over', 'the', 'kernel', 'mem', 'a', 'homogeneous', 'space', 'with', 'fibre', 'the'... | [-0.20847169009000793, 0.11282635450804852, -0.06846751457573298, -0.0286185584389422, -0.08925782922911, -0.10428916205487707, -0.0153006886556635, 0.4120385556472648, -0.37460482872876466, -0.1526980012399601, 0.0911417865769609, -0.24923808716566248, -0.10036510301699095, 0.21199530591119958, -0.13035077699368783, -... |
709.1256 | Experiments needed in Meson and Baryon Spectroscopy | Three (or four) straightforward experiments would contribute greatly to
completing the spectroscopy of baryons and light mesons. In the baryon sector,
data are needed on inelastic reactions from a polarised target with pi and kaon
beams up to 3 GeV/c. Similar data are needed in the light meson sector for
pbar-p inter... | hep-ex | three or four straightforward experiments would contribute greatly to completing the spectroscopy of baryons and light mesons in the baryon sector data are needed on inelastic reactions from a polarised target with pi and kaon beams up to 3 gevc similar data are needed in the light meson sector for pbarp interactions i... | [['three', 'or', 'four', 'straightforward', 'experiments', 'would', 'contribute', 'greatly', 'to', 'completing', 'the', 'spectroscopy', 'of', 'baryons', 'and', 'light', 'mesons', 'in', 'the', 'baryon', 'sector', 'data', 'are', 'needed', 'on', 'inelastic', 'reactions', 'from', 'a', 'polarised', 'target', 'with', 'pi', '... | [-0.016944923522797497, 0.3196492302654819, -0.05945019169435413, 0.12346525040882339, -0.02804932904560581, -0.15302231508761274, 0.04521502869988769, 0.4121904796843748, -0.20403432124486762, -0.28986816040494223, -0.03880651751706331, -0.37922117063267663, 0.08758048637200547, 0.17980374384686842, 0.0799602697481216... |
709.1257 | Projective superspace and hyperkahler sigma models on cotangent bundles
of Hermitian symmetric spaces | We review the projective-superspace construction of four-dimensional N=2
supersymmetric sigma models on (co)tangent bundles of the classical Hermitian
symmetric spaces.
| hep-th | we review the projectivesuperspace construction of fourdimensional n2 supersymmetric sigma models on cotangent bundles of the classical hermitian symmetric spaces | [['we', 'review', 'the', 'projectivesuperspace', 'construction', 'of', 'fourdimensional', 'n2', 'supersymmetric', 'sigma', 'models', 'on', 'cotangent', 'bundles', 'of', 'the', 'classical', 'hermitian', 'symmetric', 'spaces']] | [-0.1584899197332561, 0.11496157858928199, 0.0204453619197011, 0.12463589604012668, -0.09964987933635712, -0.18683570981957018, -0.10960367321968079, 0.3217012070119381, -0.11426758291199804, -0.12547189388424157, 0.11232104861992412, -0.24728486090898513, -0.2503329586237669, 0.08851425278699025, -0.15808376409113406,... |
709.1258 | Fermi-point scenario for emergent gravity | Let us assume that gravity is an emergent low-energy phenomenon arising from
a topologically stable defect in momentum space -- the Fermi point. What are
the consequences? We discuss the natural values of fermion masses and
cosmological constant; flatness of the Universe; bounds on Lorentz violation;
etc.
| gr-qc cond-mat.stat-mech hep-ph | let us assume that gravity is an emergent lowenergy phenomenon arising from a topologically stable defect in momentum space the fermi point what are the consequences we discuss the natural values of fermion masses and cosmological constant flatness of the universe bounds on lorentz violation etc | [['let', 'us', 'assume', 'that', 'gravity', 'is', 'an', 'emergent', 'lowenergy', 'phenomenon', 'arising', 'from', 'a', 'topologically', 'stable', 'defect', 'in', 'momentum', 'space', 'the', 'fermi', 'point', 'what', 'are', 'the', 'consequences', 'we', 'discuss', 'the', 'natural', 'values', 'of', 'fermion', 'masses', 'a... | [-0.18353546844066485, 0.25256767692126625, -0.10034307614778695, 0.14248813993712564, -0.12815893052712732, -0.1305254654371706, 0.02152110765809598, 0.2846618568443734, -0.24828264844077436, -0.265328130117901, 0.03517518775365518, -0.26129240757259337, -0.10059272474609315, 0.1665520946211789, -0.047542729111307344,... |
709.1259 | Light-induced disassembly of dusty bodies in inner protoplanetary discs:
implications for the formation of planets | Laboratory experiments show that a solid-state greenhouse effect in
combination with thermophoresis can efficiently erode a dust bed in a
low-pressure gaseous environment. The surface of an illuminated, light
absorbing dusty body is cooler than the dust below the surface (solidstate
greenhouse effect). This temperatu... | astro-ph | laboratory experiments show that a solidstate greenhouse effect in combination with thermophoresis can efficiently erode a dust bed in a lowpressure gaseous environment the surface of an illuminated light absorbing dusty body is cooler than the dust below the surface solidstate greenhouse effect this temperature gradie... | [['laboratory', 'experiments', 'show', 'that', 'a', 'solidstate', 'greenhouse', 'effect', 'in', 'combination', 'with', 'thermophoresis', 'can', 'efficiently', 'erode', 'a', 'dust', 'bed', 'in', 'a', 'lowpressure', 'gaseous', 'environment', 'the', 'surface', 'of', 'an', 'illuminated', 'light', 'absorbing', 'dusty', 'bod... | [-0.04866418144656232, 0.23027892471189793, -0.06519102553652245, 0.04444838353358158, -0.060567320949447, -0.06426812665110929, 0.0014448925121762764, 0.3859693455728533, -0.21178167781260934, -0.3001139271695182, 0.0569024402992272, -0.28213730965164086, -0.03362355380307747, 0.18817517495627406, -0.07950031273404136... |
709.126 | Algebraic structures on parallel M2-branes | In the course of closing supersymmetry on parallel M2 branes up to a gauge
transformation, following the suggestion in hep-th/0611108 of incorporating a
gauge field which only has topological degrees of freedom, we are led to assume
a certain algebraic structure for the low energy theory supposedly living on
parallel... | hep-th | in the course of closing supersymmetry on parallel m2 branes up to a gauge transformation following the suggestion in hepth0611108 of incorporating a gauge field which only has topological degrees of freedom we are led to assume a certain algebraic structure for the low energy theory supposedly living on parallel m2 br... | [['in', 'the', 'course', 'of', 'closing', 'supersymmetry', 'on', 'parallel', 'm2', 'branes', 'up', 'to', 'a', 'gauge', 'transformation', 'following', 'the', 'suggestion', 'in', 'hepth0611108', 'of', 'incorporating', 'a', 'gauge', 'field', 'which', 'only', 'has', 'topological', 'degrees', 'of', 'freedom', 'we', 'are', '... | [-0.20601273189052283, 0.20963328795544073, -0.08712594148100299, 0.03516048919774738, -0.11409651557914913, -0.1447458355322334, 0.031306777635644024, 0.3046682153773658, -0.18586686352158294, -0.31581951319879176, 0.06119215282538504, -0.22953662475315378, -0.09770555102138542, 0.10140747816174053, -0.093519767161970... |
709.1261 | L^2-spectral invariants and convergent sequences of finite graphs | Using the spectral theory of weakly convergent sequences of finite graphs, we
prove the uniform existence of the integrated density of states for a large
class of infinite graphs.
| math.SP math.CO | using the spectral theory of weakly convergent sequences of finite graphs we prove the uniform existence of the integrated density of states for a large class of infinite graphs | [['using', 'the', 'spectral', 'theory', 'of', 'weakly', 'convergent', 'sequences', 'of', 'finite', 'graphs', 'we', 'prove', 'the', 'uniform', 'existence', 'of', 'the', 'integrated', 'density', 'of', 'states', 'for', 'a', 'large', 'class', 'of', 'infinite', 'graphs']] | [-0.172582836356014, 0.18397419503087115, -0.11030321934356771, 0.08418428547808836, 0.002255455622899121, -0.03260354055412885, 0.022985772630159648, 0.34366968749412174, -0.268756034784019, -0.23269991545359894, 0.1171244909617536, -0.25208195690707913, -0.06707086905451684, 0.14941034623389615, -0.023483146014141625... |
709.1262 | An O(2,n) formulation of invariant theory for elliptic Weyl group | In this paper, we give a new formulation of invariant theory for elliptic
Weyl group using the group O(2,n). As an elliptic Weyl group quotient, we
define a suitable $\C^*$-bundle. We show that it has a conformal Frobenius
structure which we define in this paper. Then its good section could be
identified with a Frobe... | math.AG math.RT | in this paper we give a new formulation of invariant theory for elliptic weyl group using the group o2n as an elliptic weyl group quotient we define a suitable cbundle we show that it has a conformal frobenius structure which we define in this paper then its good section could be identified with a frobenius manifold wh... | [['in', 'this', 'paper', 'we', 'give', 'a', 'new', 'formulation', 'of', 'invariant', 'theory', 'for', 'elliptic', 'weyl', 'group', 'using', 'the', 'group', 'o2n', 'as', 'an', 'elliptic', 'weyl', 'group', 'quotient', 'we', 'define', 'a', 'suitable', 'cbundle', 'we', 'show', 'that', 'it', 'has', 'a', 'conformal', 'froben... | [-0.18115942070726304, 0.05409578691299733, -0.18922145189717413, 0.044797678256873044, -0.13146718768402935, -0.12392701189188908, -0.032051908797196424, 0.3655713649156193, -0.3380835079898437, -0.22607153987822434, 0.07623826303558114, -0.2091197623560826, -0.23606622591614723, 0.14930988621587554, -0.14417529872929... |
709.1263 | Enumerating the Nash equilibria of rank 1-games | A bimatrix game $(A,B)$ is called a game of rank $k$ if the rank of the
matrix $A+B$ is at most $k$. We consider the problem of enumerating the Nash
equilibria in (non-degenerate) games of rank 1. In particular, we show that
even for games of rank 1 not all equilibria can be reached by a Lemke-Howson
path and present... | cs.GT math.OC | a bimatrix game ab is called a game of rank k if the rank of the matrix ab is at most k we consider the problem of enumerating the nash equilibria in nondegenerate games of rank 1 in particular we show that even for games of rank 1 not all equilibria can be reached by a lemkehowson path and present a parametric simplex... | [['a', 'bimatrix', 'game', 'ab', 'is', 'called', 'a', 'game', 'of', 'rank', 'k', 'if', 'the', 'rank', 'of', 'the', 'matrix', 'ab', 'is', 'at', 'most', 'k', 'we', 'consider', 'the', 'problem', 'of', 'enumerating', 'the', 'nash', 'equilibria', 'in', 'nondegenerate', 'games', 'of', 'rank', '1', 'in', 'particular', 'we', '... | [-0.17515222555467566, 0.05192343247931843, -0.10249128080536857, 0.0646016125193503, 0.029344652381137405, -0.22490151407270642, 0.10172503224365707, 0.38595902557043654, -0.2838128623506667, -0.22469419704161978, 0.09738714883324544, -0.2500070701598337, -0.18232856386978374, 0.05885871769370217, -0.08037484178662692... |
709.1264 | Discrete Monodromy, Pentagrams, and the Method of Condensation | This paper considers a simple geometric construction, called the Pentagram
map. The pentagram map, performed on N-gons, gives rise to a birational mapping
on the space of all N-gons. This paper finds what conjecturally are all the
invariants for this map, and along the way relates the construction to the
monodromy of... | math.MG | this paper considers a simple geometric construction called the pentagram map the pentagram map performed on ngons gives rise to a birational mapping on the space of all ngons this paper finds what conjecturally are all the invariants for this map and along the way relates the construction to the monodromy of 3rd order... | [['this', 'paper', 'considers', 'a', 'simple', 'geometric', 'construction', 'called', 'the', 'pentagram', 'map', 'the', 'pentagram', 'map', 'performed', 'on', 'ngons', 'gives', 'rise', 'to', 'a', 'birational', 'mapping', 'on', 'the', 'space', 'of', 'all', 'ngons', 'this', 'paper', 'finds', 'what', 'conjecturally', 'are... | [-0.1616114726798101, 0.006796932454700723, -0.09539057828034415, 0.07153744273995416, -0.10385950348537529, -0.11351044920527122, 0.006067327079080948, 0.28052553885870357, -0.31983366859794565, -0.26754401663713384, 0.09802982826350314, -0.269257635033379, -0.239693257393259, 0.20631134079656366, -0.15390754496735154... |
709.1265 | NMR Study of Large Skyrmions in Al_{0.13}Ga_{0.87}As Quantum Wells | A nuclear magnetic resonance (NMR) study is reported of multiple (30)
Al$_{0.13}$Ga$_{0.87}$As quantum well (QW) sample near the Landau level filling
factor $\nu =1$. In these Al$_{0.13}$Ga$_{0.87}$As QWs the effective $g$ factor
is nearly zero. This can lead to two effects: vanishing electronic polarization
$(P)$ an... | cond-mat.mes-hall cond-mat.str-el | a nuclear magnetic resonance nmr study is reported of multiple 30 al_013ga_087as quantum well qw sample near the landau level filling factor nu 1 in these al_013ga_087as qws the effective g factor is nearly zero this can lead to two effects vanishing electronic polarization p and skyrmionic excitations composed of a hu... | [['a', 'nuclear', 'magnetic', 'resonance', 'nmr', 'study', 'is', 'reported', 'of', 'multiple', '30', 'al_013ga_087as', 'quantum', 'well', 'qw', 'sample', 'near', 'the', 'landau', 'level', 'filling', 'factor', 'nu', '1', 'in', 'these', 'al_013ga_087as', 'qws', 'the', 'effective', 'g', 'factor', 'is', 'nearly', 'zero', '... | [-0.1723826203688077, 0.2313059120762091, -0.04633938468032284, 0.06332089416991948, -0.05435527926238137, -0.1680936701814062, 0.05976472516886133, 0.3672280996834161, -0.27267100142489653, -0.3456623269303236, 0.028602267956557625, -0.2627320287956536, -0.06740236468067451, 0.18474537645670353, 0.025658977907369263, ... |
709.1266 | The LU-LC conjecture is false | The LU-LC conjecture is an important open problem concerning the structure of
entanglement of states described in the stabilizer formalism. It states that
two local unitary equivalent stabilizer states are also local Clifford
equivalent. If this conjecture were true, the local equivalence of stabilizer
states would b... | quant-ph | the lulc conjecture is an important open problem concerning the structure of entanglement of states described in the stabilizer formalism it states that two local unitary equivalent stabilizer states are also local clifford equivalent if this conjecture were true the local equivalence of stabilizer states would be extr... | [['the', 'lulc', 'conjecture', 'is', 'an', 'important', 'open', 'problem', 'concerning', 'the', 'structure', 'of', 'entanglement', 'of', 'states', 'described', 'in', 'the', 'stabilizer', 'formalism', 'it', 'states', 'that', 'two', 'local', 'unitary', 'equivalent', 'stabilizer', 'states', 'are', 'also', 'local', 'cliffo... | [-0.12116817915294734, 0.13428397507575734, -0.10773789257897685, 0.11403014766498624, 0.002569022979716667, -0.2066659434284601, 0.022898969298694283, 0.3202446498390701, -0.26830300631829435, -0.2638070022609706, 0.08547835908151076, -0.21797138251066725, -0.17025297517991728, 0.18298673853536862, -0.1323723218326146... |
709.1267 | A Survey of Local Group Galaxies Currently Forming Stars: III. A Search
for Luminous Blue Variables and Other H-alpha Emission-Lined Stars | We describe a search for H-alpha emission-lined stars in M31, M33, and seven
dwarfs in or near the Local Group (IC 10, NGC 6822, WLM, Sextans B, Sextans A,
Pegasus and the Phoenix dwarf) using interference filter imaging with the KPNO
and CTIO 4-m telescope and Mosaic cameras. The survey is aimed primarily at
identif... | astro-ph | we describe a search for halpha emissionlined stars in m31 m33 and seven dwarfs in or near the local group ic 10 ngc 6822 wlm sextans b sextans a pegasus and the phoenix dwarf using interference filter imaging with the kpno and ctio 4m telescope and mosaic cameras the survey is aimed primarily at identifying new lumino... | [['we', 'describe', 'a', 'search', 'for', 'halpha', 'emissionlined', 'stars', 'in', 'm31', 'm33', 'and', 'seven', 'dwarfs', 'in', 'or', 'near', 'the', 'local', 'group', 'ic', '10', 'ngc', '6822', 'wlm', 'sextans', 'b', 'sextans', 'a', 'pegasus', 'and', 'the', 'phoenix', 'dwarf', 'using', 'interference', 'filter', 'imag... | [-0.044175672706949304, 0.05368739753441118, -0.08115079924156067, 0.10245269229712636, -0.1538842505097444, -0.11922899652563501, 0.09968157608112532, 0.4628001431153868, -0.15300933559089624, -0.35974934604361325, 0.07876639376327683, -0.3116983164366984, -0.08265818771670798, 0.20043672849831584, -0.1116699999127925... |
709.1268 | Tensor-product vs. geometric-product coding | Quantum computation is based on tensor products and entangled states. We
discuss an alternative to the quantum framework where tensor products are
replaced by geometric products and entangled states by multivectors. The
resulting theory is analogous to quantum computation but does not involve
quantum mechanics. We di... | quant-ph | quantum computation is based on tensor products and entangled states we discuss an alternative to the quantum framework where tensor products are replaced by geometric products and entangled states by multivectors the resulting theory is analogous to quantum computation but does not involve quantum mechanics we discuss... | [['quantum', 'computation', 'is', 'based', 'on', 'tensor', 'products', 'and', 'entangled', 'states', 'we', 'discuss', 'an', 'alternative', 'to', 'the', 'quantum', 'framework', 'where', 'tensor', 'products', 'are', 'replaced', 'by', 'geometric', 'products', 'and', 'entangled', 'states', 'by', 'multivectors', 'the', 'res... | [-0.09982568749812966, 0.2153324006629679, -0.0810948419838962, 0.08584363541846936, -0.028637111970655073, -0.1543902000185193, -0.003503343560335385, 0.38483525485527226, -0.25925082231803637, -0.26917168786522094, 0.09723408653531451, -0.26662636707854886, -0.20044898391678567, 0.18583820385449543, -0.07953034505292... |
709.1269 | A criterion for the half-plane property | We establish a convenient necessary and sufficient condition for a
multiaffine real polynomial to be stable, and use it to verify that the
half-plane property holds for seven small matroids that resisted the efforts of
Choe, Oxley, Sokal, and Wagner [5].
| math.CO | we establish a convenient necessary and sufficient condition for a multiaffine real polynomial to be stable and use it to verify that the halfplane property holds for seven small matroids that resisted the efforts of choe oxley sokal and wagner 5 | [['we', 'establish', 'a', 'convenient', 'necessary', 'and', 'sufficient', 'condition', 'for', 'a', 'multiaffine', 'real', 'polynomial', 'to', 'be', 'stable', 'and', 'use', 'it', 'to', 'verify', 'that', 'the', 'halfplane', 'property', 'holds', 'for', 'seven', 'small', 'matroids', 'that', 'resisted', 'the', 'efforts', 'o... | [-0.13560427502706285, 0.053955530952207925, -0.06847953687353832, 0.11399950200646389, -0.14852031879127026, -0.18770855926431534, 0.03938903153601398, 0.34673177787080045, -0.2390129476581223, -0.22284691098214285, 0.15554816192924614, -0.17860009543961142, -0.18639130119188893, 0.2410705901182643, -0.084583910971471... |
709.127 | Divergence of a stationary random vector field can be always positive (a
Weiss' phenomenon) | The divergence of a stationary random vector field at a given point is
usually a centered (that is, zero mean) random variable. Strangely enough, it
can be equal to 1 almost surely. This fact is another form of a phenomenon
disclosed by B. Weiss in 1997.
| math.PR | the divergence of a stationary random vector field at a given point is usually a centered that is zero mean random variable strangely enough it can be equal to 1 almost surely this fact is another form of a phenomenon disclosed by b weiss in 1997 | [['the', 'divergence', 'of', 'a', 'stationary', 'random', 'vector', 'field', 'at', 'a', 'given', 'point', 'is', 'usually', 'a', 'centered', 'that', 'is', 'zero', 'mean', 'random', 'variable', 'strangely', 'enough', 'it', 'can', 'be', 'equal', 'to', '1', 'almost', 'surely', 'this', 'fact', 'is', 'another', 'form', 'of',... | [-0.15028410097179207, 0.23200530939452027, -0.15435320569161812, 0.06662167037290562, -0.07941418959070808, -0.17698799272108337, 0.08367319405078888, 0.34699275854813016, -0.29623770632821583, -0.19731392023032127, 0.1226585608294598, -0.28480583875764, -0.15206531117386793, 0.1157384562994475, -0.09423808054998517, ... |
709.1271 | On the distance of PG 1553+11. A lineless BL Lac object active in the
TeV band | Context: The redshift of PG 1553+11, a bright BL Lac object (V~14), is still
unknown. It has been recently observed in the TeV band, a fact that offers an
upper limit for the redshift z<0.4. Aims: We intend to provide a lower limit
for the distance of the object. Methods: We used a chi^2 procedure to constrain
the ap... | astro-ph | context the redshift of pg 155311 a bright bl lac object v14 is still unknown it has been recently observed in the tev band a fact that offers an upper limit for the redshift z04 aims we intend to provide a lower limit for the distance of the object methods we used a chi2 procedure to constrain the apparent magnitude o... | [['context', 'the', 'redshift', 'of', 'pg', '155311', 'a', 'bright', 'bl', 'lac', 'object', 'v14', 'is', 'still', 'unknown', 'it', 'has', 'been', 'recently', 'observed', 'in', 'the', 'tev', 'band', 'a', 'fact', 'that', 'offers', 'an', 'upper', 'limit', 'for', 'the', 'redshift', 'z04', 'aims', 'we', 'intend', 'to', 'pro... | [-0.041307720100684536, 0.08209025795050755, -0.08027149491023183, 0.14092367699153588, -0.1513541735475883, -0.09600370425808553, 0.05975348848040171, 0.44576947925989296, -0.14565918959713253, -0.3902713520718472, 0.06103234660224102, -0.3012053038470358, 0.010120750043175317, 0.21923656597971872, -0.0556308224303869... |
709.1272 | A Class of Parallel Tiled Linear Algebra Algorithms for Multicore
Architectures | As multicore systems continue to gain ground in the High Performance
Computing world, linear algebra algorithms have to be reformulated or new
algorithms have to be developed in order to take advantage of the architectural
features on these new processors. Fine grain parallelism becomes a major
requirement and introd... | cs.MS cs.DC | as multicore systems continue to gain ground in the high performance computing world linear algebra algorithms have to be reformulated or new algorithms have to be developed in order to take advantage of the architectural features on these new processors fine grain parallelism becomes a major requirement and introduces... | [['as', 'multicore', 'systems', 'continue', 'to', 'gain', 'ground', 'in', 'the', 'high', 'performance', 'computing', 'world', 'linear', 'algebra', 'algorithms', 'have', 'to', 'be', 'reformulated', 'or', 'new', 'algorithms', 'have', 'to', 'be', 'developed', 'in', 'order', 'to', 'take', 'advantage', 'of', 'the', 'archite... | [-0.15519135045232596, 0.039562902062176296, -0.08580519896242078, 0.010103951592032832, -0.07875708346312613, -0.14267582977679272, 0.03636058661684302, 0.41923347094820607, -0.3127396414918756, -0.3611560624357267, 0.14819108379679952, -0.18660283083510068, -0.1020349818756114, 0.19673859610159042, -0.104041253049846... |
709.1273 | (GL(n+1,F),GL(n,F)) is a Gelfand pair for any local field F | Let F be an arbitrary local field. Consider the standard embedding of GL(n,F)
into GL(n+1,F) and the two-sided action of GL(n,F) \times GL(n,F) on GL(n+1,F).
In this paper we show that any GL(n,F) \times GL(n,F)-invariant distribution
on GL(n+1,F) is invariant with respect to transposition.
We show that this impl... | math.RT | let f be an arbitrary local field consider the standard embedding of glnf into gln1f and the twosided action of glnf times glnf on gln1f in this paper we show that any glnf times glnfinvariant distribution on gln1f is invariant with respect to transposition we show that this implies that the pair gln1fglnf is a gelfand... | [['let', 'f', 'be', 'an', 'arbitrary', 'local', 'field', 'consider', 'the', 'standard', 'embedding', 'of', 'glnf', 'into', 'gln1f', 'and', 'the', 'twosided', 'action', 'of', 'glnf', 'times', 'glnf', 'on', 'gln1f', 'in', 'this', 'paper', 'we', 'show', 'that', 'any', 'glnf', 'times', 'glnfinvariant', 'distribution', 'on'... | [-0.1692320124278668, 0.08823568483988543, -0.13398919439181511, 0.06525146794440441, -0.06469564950418506, -0.11791933552621929, -0.05679154872412382, 0.38587036009791287, -0.2748459356642047, -0.16762901619306853, 0.044852042616734845, -0.23605095703414705, -0.12128480009972877, 0.18140617505712217, -0.12016858827582... |
709.1274 | Valley contrasting physics in graphene: magnetic moment and topological
transport | We investigate physical properties that can be used to distinguish the valley
degree of freedom in systems where inversion symmetry is broken, using graphene
systems as examples. We show that the pseudospin associated with the valley
index of carriers has an intrinsic magnetic moment, in close analogy with the
Bohr m... | cond-mat.mtrl-sci cond-mat.mes-hall | we investigate physical properties that can be used to distinguish the valley degree of freedom in systems where inversion symmetry is broken using graphene systems as examples we show that the pseudospin associated with the valley index of carriers has an intrinsic magnetic moment in close analogy with the bohr magnet... | [['we', 'investigate', 'physical', 'properties', 'that', 'can', 'be', 'used', 'to', 'distinguish', 'the', 'valley', 'degree', 'of', 'freedom', 'in', 'systems', 'where', 'inversion', 'symmetry', 'is', 'broken', 'using', 'graphene', 'systems', 'as', 'examples', 'we', 'show', 'that', 'the', 'pseudospin', 'associated', 'wi... | [-0.1712812219271395, 0.23986610746344791, -0.059975899154129104, 0.04957446327274998, -0.06665994018632253, -0.13673588900460995, 0.023408720000069088, 0.4105021559267438, -0.3042580482350396, -0.31517258998272674, 0.004459259832011802, -0.2721445117245561, -0.1579990436979902, 0.18472910357689085, -0.0153452592307335... |
709.1275 | Automated search for galactic star clusters in large multiband surveys:
I. Discovery of 15 new open clusters in the Galactic anticenter region | Aims: According to some estimations, there are as many as 100000 open
clusters in the Galaxy, but less than 2000 of them have been discovered,
measured, and cataloged. We plan to undertake data mining of multiwavelength
surveys to find new star clusters. Methods: We have developed a new method to
search automatically... | astro-ph | aims according to some estimations there are as many as 100000 open clusters in the galaxy but less than 2000 of them have been discovered measured and cataloged we plan to undertake data mining of multiwavelength surveys to find new star clusters methods we have developed a new method to search automatically for star ... | [['aims', 'according', 'to', 'some', 'estimations', 'there', 'are', 'as', 'many', 'as', '100000', 'open', 'clusters', 'in', 'the', 'galaxy', 'but', 'less', 'than', '2000', 'of', 'them', 'have', 'been', 'discovered', 'measured', 'and', 'cataloged', 'we', 'plan', 'to', 'undertake', 'data', 'mining', 'of', 'multiwavelengt... | [-0.03361567677766925, 0.060278620799482034, -0.10530629536818263, 0.08664032760808237, -0.1026689946995269, -0.054227077670337395, 0.10966030642315963, 0.4282061437050656, -0.18594724138073462, -0.40951716865807886, 0.08268680347533759, -0.2943687055691178, -0.05492805630799405, 0.2254854765918164, -0.0248292767395653... |
709.1276 | Exponential clogging time for a one dimensional DLA | When considering DLA on a cylinder it is natural to ask how many particles it
takes to clog the cylinder, e.g. modeling clogging of arteries. In this note we
formulate a very simple DLA clogging model and establish an exponential lower
bound on the number of particles arriving before clogging appears.
| math.PR math-ph math.MP | when considering dla on a cylinder it is natural to ask how many particles it takes to clog the cylinder eg modeling clogging of arteries in this note we formulate a very simple dla clogging model and establish an exponential lower bound on the number of particles arriving before clogging appears | [['when', 'considering', 'dla', 'on', 'a', 'cylinder', 'it', 'is', 'natural', 'to', 'ask', 'how', 'many', 'particles', 'it', 'takes', 'to', 'clog', 'the', 'cylinder', 'eg', 'modeling', 'clogging', 'of', 'arteries', 'in', 'this', 'note', 'we', 'formulate', 'a', 'very', 'simple', 'dla', 'clogging', 'model', 'and', 'estab... | [-0.11457975438850768, 0.1901042721186897, -0.08810056830007656, 0.09595160211228729, -0.08001792978714495, -0.18188284193256907, 0.05438398436515355, 0.33690699701215704, -0.2413756448556395, -0.2941610608615127, 0.06887421241787937, -0.27110902212706267, -0.12259407628181518, 0.18051339860768148, -0.11891904235908798... |
709.1277 | Aspetti Moderni della Fisica Greca [Modern Aspects of Ancient Greek
Physics] | Plutarchus, circa 100 AD, in his early book on "astrophysics" --in which he
exposed, in a sense, a general theory of gravitation-- wrote the noticeable
passage: <<The Moon gets the guarantee of not falling down just from its motion
and from the dash associated with its revolution, exactly as stones in slings
cannot f... | physics.ed-ph physics.pop-ph | plutarchus circa 100 ad in his early book on astrophysics in which he exposed in a sense a general theory of gravitation wrote the noticeable passage the moon gets the guarantee of not falling down just from its motion and from the dash associated with its revolution exactly as stones in slings cannot fall due to their... | [['plutarchus', 'circa', '100', 'ad', 'in', 'his', 'early', 'book', 'on', 'astrophysics', 'in', 'which', 'he', 'exposed', 'in', 'a', 'sense', 'a', 'general', 'theory', 'of', 'gravitation', 'wrote', 'the', 'noticeable', 'passage', 'the', 'moon', 'gets', 'the', 'guarantee', 'of', 'not', 'falling', 'down', 'just', 'from',... | [-0.048185013195306256, 0.1667628889905064, -0.11631400470049383, 0.0713573733775058, -0.12182833337591904, -0.13457922853158538, 0.028971486202304077, 0.343373881749712, -0.27354094921107286, -0.32814771946906657, 0.1373267231889077, -0.2960974985403029, -0.11673074857497112, 0.20108909608702502, -0.1138194322070002, ... |
709.1278 | PoGOLite - A High Sensitivity Balloon-Borne Soft Gamma-ray Polarimeter | We describe a new balloon-borne instrument (PoGOLite) capable of detecting
10% polarisation from 200mCrab point-like sources between 25 and 80keV in one 6
hour flight. Polarisation measurements in the soft gamma-ray band are expected
to provide a powerful probe into high-energy emission mechanisms as well as the
dist... | astro-ph | we describe a new balloonborne instrument pogolite capable of detecting 10 polarisation from 200mcrab pointlike sources between 25 and 80kev in one 6 hour flight polarisation measurements in the soft gammaray band are expected to provide a powerful probe into highenergy emission mechanisms as well as the distribution o... | [['we', 'describe', 'a', 'new', 'balloonborne', 'instrument', 'pogolite', 'capable', 'of', 'detecting', '10', 'polarisation', 'from', '200mcrab', 'pointlike', 'sources', 'between', '25', 'and', '80kev', 'in', 'one', '6', 'hour', 'flight', 'polarisation', 'measurements', 'in', 'the', 'soft', 'gammaray', 'band', 'are', '... | [-0.041323340122255976, 0.1591788811660485, -0.04365564600124748, 0.08583189521461329, -0.05759090120490226, -0.11632916288821164, 0.006013316715662195, 0.4254817708106539, -0.17527420158579912, -0.3966624933570899, 0.07770141111244878, -0.35405006184656584, -0.004059617737463365, 0.23395813709443988, 0.015437083862101... |
709.1279 | An Update on the 0Z Project | We give an update on our 0Z Survey to find more extremely metal poor (EMP)
stars with [Fe/H] < -3 dex through mining the database of the Hamburg/ESO
Survey. We present the most extreme such stars we have found from ~1550
moderate resolution follow up spectra. One of these, HE1424-0241, has highly
anomalous abundance ... | astro-ph | we give an update on our 0z survey to find more extremely metal poor emp stars with feh 3 dex through mining the database of the hamburgeso survey we present the most extreme such stars we have found from 1550 moderate resolution follow up spectra one of these he14240241 has highly anomalous abundance ratios not seen i... | [['we', 'give', 'an', 'update', 'on', 'our', '0z', 'survey', 'to', 'find', 'more', 'extremely', 'metal', 'poor', 'emp', 'stars', 'with', 'feh', '3', 'dex', 'through', 'mining', 'the', 'database', 'of', 'the', 'hamburgeso', 'survey', 'we', 'present', 'the', 'most', 'extreme', 'such', 'stars', 'we', 'have', 'found', 'fro... | [-0.005219848168697475, 0.09779824387638898, -0.039842073795604005, 0.07712830557057893, -0.0643536673366364, -0.10106237205502946, 0.10023823099179666, 0.43776995772005695, -0.14030404769120355, -0.38571519879362454, 0.01461615935291061, -0.3362043502196919, -0.01701744552813114, 0.18971743673625352, -0.08290327458005... |
709.128 | Comment on Theory of spin Hall effect | Chudnovsky recently proposed (arXiv: 0709.0725) a beautifully simple
mechanism for the intrinsic spin Hall effect involving an extension of the
Drude model. We point out that an equivalent proposal was made by us in an
alternative treatment of the problem in Phys.Rev. B60, 14787 (1999)
(arXiv:cond-mat/9910408, reachi... | cond-mat.mes-hall | chudnovsky recently proposed arxiv 07090725 a beautifully simple mechanism for the intrinsic spin hall effect involving an extension of the drude model we point out that an equivalent proposal was made by us in an alternative treatment of the problem in physrev b60 14787 1999 arxivcondmat9910408 reaching identical conc... | [['chudnovsky', 'recently', 'proposed', 'arxiv', '07090725', 'a', 'beautifully', 'simple', 'mechanism', 'for', 'the', 'intrinsic', 'spin', 'hall', 'effect', 'involving', 'an', 'extension', 'of', 'the', 'drude', 'model', 'we', 'point', 'out', 'that', 'an', 'equivalent', 'proposal', 'was', 'made', 'by', 'us', 'in', 'an',... | [-0.09663873018143931, 0.10339507975058951, -0.07569744614884258, 0.047891575162066144, -0.0943562627886422, -0.15519867973052898, 0.07622266658581793, 0.35254459410207345, -0.20712432670989073, -0.2955466258164961, -0.0017835713049862533, -0.28905482734553517, -0.16549250935204327, 0.20679210584785324, -0.035937606470... |
709.1281 | Relative and Discrete Utility Maximising Entropy | The notion of utility maximising entropy (u-entropy) of a probability
density, which was introduced and studied by Slomczynski and Zastawniak (Ann.
Prob 32 (2004) 2261-2285, arXiv:math.PR/0410115 v1), is extended in two
directions. First, the relative u-entropy of two probability measures in
arbitrary probability spa... | math.PR q-fin.ST | the notion of utility maximising entropy uentropy of a probability density which was introduced and studied by slomczynski and zastawniak ann prob 32 2004 22612285 arxivmathpr0410115 v1 is extended in two directions first the relative uentropy of two probability measures in arbitrary probability spaces is defined then ... | [['the', 'notion', 'of', 'utility', 'maximising', 'entropy', 'uentropy', 'of', 'a', 'probability', 'density', 'which', 'was', 'introduced', 'and', 'studied', 'by', 'slomczynski', 'and', 'zastawniak', 'ann', 'prob', '32', '2004', '22612285', 'arxivmathpr0410115', 'v1', 'is', 'extended', 'in', 'two', 'directions', 'first... | [-0.0616528268968433, 0.07431321957104658, -0.09939237466069306, 0.11891796242534405, -0.01818287075294473, -0.1161703282213282, 0.050797437160271124, 0.32096423873310387, -0.3001881563738242, -0.2539818108930778, 0.0950242315797566, -0.307454673865205, -0.14758656954956653, 0.16458603420586257, -0.15462163420153313, 0... |
709.1282 | Dynamics of Symplectic SubVolumes | In this paper we will explore fundamental constraints on the evolution of
certain symplectic subvolumes possessed by any Hamiltonian phase space. This
research has direct application to optimal control and control of conservative
mechanical systems. We relate geometric invariants of symplectic topology to
computation... | math.OC math.DS | in this paper we will explore fundamental constraints on the evolution of certain symplectic subvolumes possessed by any hamiltonian phase space this research has direct application to optimal control and control of conservative mechanical systems we relate geometric invariants of symplectic topology to computations th... | [['in', 'this', 'paper', 'we', 'will', 'explore', 'fundamental', 'constraints', 'on', 'the', 'evolution', 'of', 'certain', 'symplectic', 'subvolumes', 'possessed', 'by', 'any', 'hamiltonian', 'phase', 'space', 'this', 'research', 'has', 'direct', 'application', 'to', 'optimal', 'control', 'and', 'control', 'of', 'conse... | [-0.18156079666079145, 0.12730187468593362, -0.1271183700259544, 0.035199458522318275, -0.10105980607161744, -0.08759352613026195, 0.060038455624949284, 0.33961527791714907, -0.31288823219988726, -0.26041112419844203, 0.11916298600865644, -0.2075534550786282, -0.17094593131667482, 0.16211509610633407, -0.10282094410900... |
709.1283 | The fundamental role of the retarded potential in the electrodynamics of
superluminal sources | We calculate the gradient of the radiation field generated by a polarization
current with a superluminally rotating distribution pattern and show that the
absolute value of this gradient increases as R^(7/2) with distance R within the
sharply focused subbeams constituting the overall radiation beam. This result
not o... | astro-ph | we calculate the gradient of the radiation field generated by a polarization current with a superluminally rotating distribution pattern and show that the absolute value of this gradient increases as r72 with distance r within the sharply focused subbeams constituting the overall radiation beam this result not only sup... | [['we', 'calculate', 'the', 'gradient', 'of', 'the', 'radiation', 'field', 'generated', 'by', 'a', 'polarization', 'current', 'with', 'a', 'superluminally', 'rotating', 'distribution', 'pattern', 'and', 'show', 'that', 'the', 'absolute', 'value', 'of', 'this', 'gradient', 'increases', 'as', 'r72', 'with', 'distance', '... | [-0.14223485160971794, 0.13095607720905372, -0.0835864148996394, 0.055721415892346866, -0.08444657127971852, -0.09410601871257479, 0.017435317474775256, 0.34248607337274134, -0.2528606917245019, -0.2681713242206083, 0.09049949835263105, -0.2740364588627761, -0.09255831574696596, 0.19540494901319394, -0.0059021779834622... |
709.1284 | Spin and orbital angular momentum in gauge theories (II): QCD and
nucleon spin structure | Parallel to the construction of gauge invariant spin and orbital angular
momentum for QED in paper (I) of this series, we present here an analogous but
non-trivial solution for QCD. Explicitly gauge invariant spin and orbital
angular momentum operators of quarks and gluons are obtained. This was
previously thought to... | hep-ph | parallel to the construction of gauge invariant spin and orbital angular momentum for qed in paper i of this series we present here an analogous but nontrivial solution for qcd explicitly gauge invariant spin and orbital angular momentum operators of quarks and gluons are obtained this was previously thought to be an i... | [['parallel', 'to', 'the', 'construction', 'of', 'gauge', 'invariant', 'spin', 'and', 'orbital', 'angular', 'momentum', 'for', 'qed', 'in', 'paper', 'i', 'of', 'this', 'series', 'we', 'present', 'here', 'an', 'analogous', 'but', 'nontrivial', 'solution', 'for', 'qcd', 'explicitly', 'gauge', 'invariant', 'spin', 'and', ... | [-0.1546202060947989, 0.24086226564395474, -0.10479542336371891, 0.08692225559035946, -0.1289467092437382, -0.08567445161615443, 0.0028869603086016417, 0.3852413673611248, -0.2087175089537221, -0.2791320665171096, -0.025918733357684687, -0.2180896332857254, -0.09215002205147517, 0.16531942328712082, 0.01437156272953978... |
709.1285 | Corners and Records of the Poisson Process in Quadrant | The scale-invariant spacings lemma due to Arratia, Barbour and Tavar{\'e}
establishes the distributional identity of a self-similar Poisson process and
the set of spacings between the points of this process. In this note we connect
this result with properties of a certain set of extreme points of the unit
Poisson pro... | math.PR | the scaleinvariant spacings lemma due to arratia barbour and tavare establishes the distributional identity of a selfsimilar poisson process and the set of spacings between the points of this process in this note we connect this result with properties of a certain set of extreme points of the unit poisson process in th... | [['the', 'scaleinvariant', 'spacings', 'lemma', 'due', 'to', 'arratia', 'barbour', 'and', 'tavare', 'establishes', 'the', 'distributional', 'identity', 'of', 'a', 'selfsimilar', 'poisson', 'process', 'and', 'the', 'set', 'of', 'spacings', 'between', 'the', 'points', 'of', 'this', 'process', 'in', 'this', 'note', 'we', ... | [-0.1342486922798509, 0.056535524654794826, -0.1022822837937962, 0.03838804677622896, -0.023886886501515454, -0.05009569618850947, 0.15435602502389387, 0.3033108209767802, -0.3262939298229123, -0.22903633366592907, 0.07715897883965887, -0.2700201443777504, -0.15416631033982742, 0.13643985451622442, -0.11416172639212825... |
709.1286 | Study of a Z-form of the coordinate ring of a reductive group | We show how the theory of canonical bases in modified universal enveloping
algebras can be used to develop the theory of Chevalley groups over any
commutative ring with 1.
| math.RT | we show how the theory of canonical bases in modified universal enveloping algebras can be used to develop the theory of chevalley groups over any commutative ring with 1 | [['we', 'show', 'how', 'the', 'theory', 'of', 'canonical', 'bases', 'in', 'modified', 'universal', 'enveloping', 'algebras', 'can', 'be', 'used', 'to', 'develop', 'the', 'theory', 'of', 'chevalley', 'groups', 'over', 'any', 'commutative', 'ring', 'with', '1']] | [-0.11831203822431893, 0.06186133568528397, -0.1602419450365264, 0.059178051121276, -0.09841387115161994, -0.14842926942068954, -0.09147255810716286, 0.3542661432433745, -0.4276509988282261, -0.17954949803393463, 0.0583719755001045, -0.13447483012388492, -0.16108165048705092, 0.2120528070191885, -0.1872880840352897, -0... |
709.1287 | Finite size corrections to the blackbody radiation laws | We investigate the radiation of a blackbody in a cavity of finite size. For a
given geometry, we use semiclassical techniques to obtain explicit expressions
of the modified Planck's and Stefan-Boltzmann's blackbody radiation laws as a
function of the size and shape of the cavity. We determine the range of
parameters ... | quant-ph astro-ph cond-mat.mes-hall cond-mat.stat-mech | we investigate the radiation of a blackbody in a cavity of finite size for a given geometry we use semiclassical techniques to obtain explicit expressions of the modified plancks and stefanboltzmanns blackbody radiation laws as a function of the size and shape of the cavity we determine the range of parameters temperat... | [['we', 'investigate', 'the', 'radiation', 'of', 'a', 'blackbody', 'in', 'a', 'cavity', 'of', 'finite', 'size', 'for', 'a', 'given', 'geometry', 'we', 'use', 'semiclassical', 'techniques', 'to', 'obtain', 'explicit', 'expressions', 'of', 'the', 'modified', 'plancks', 'and', 'stefanboltzmanns', 'blackbody', 'radiation',... | [-0.07459018569549217, 0.11987355019458953, -0.08722941966398674, 0.05152504113228882, -0.06514701064237777, -0.07612413593074854, 0.036334594419938235, 0.35897091964588446, -0.23125197869889877, -0.3116517465123359, 0.06510908955653362, -0.25939709452693077, -0.06551457419991494, 0.2548990186961258, -0.036640429116018... |
709.1288 | SU(4) and SU(2) Kondo Effects in Carbon Nanotube Quantum Dots | We study the SU(4) Kondo effect in carbon nanotube quantum dots, where doubly
degenerate orbitals form 4-electron ``shells''. The SU(4) Kondo behavior is
investigated for one, two and three electrons in the topmost shell. While the
Kondo state of two electrons is quenched by magnetic field, in case of an odd
number o... | cond-mat.mes-hall cond-mat.str-el | we study the su4 kondo effect in carbon nanotube quantum dots where doubly degenerate orbitals form 4electron shells the su4 kondo behavior is investigated for one two and three electrons in the topmost shell while the kondo state of two electrons is quenched by magnetic field in case of an odd number of electrons two ... | [['we', 'study', 'the', 'su4', 'kondo', 'effect', 'in', 'carbon', 'nanotube', 'quantum', 'dots', 'where', 'doubly', 'degenerate', 'orbitals', 'form', '4electron', 'shells', 'the', 'su4', 'kondo', 'behavior', 'is', 'investigated', 'for', 'one', 'two', 'and', 'three', 'electrons', 'in', 'the', 'topmost', 'shell', 'while'... | [-0.24637396449300772, 0.27721966699406647, 0.006785413779046697, 0.0944280535610839, 0.0036343966833859063, -0.18069061829010025, -0.005079806494298585, 0.38429109738838935, -0.2321282746270299, -0.2753975192123714, -0.0345375898432394, -0.2776048131830369, -0.04798283928539604, 0.10499214819962314, 0.0825167832808801... |
709.1289 | A two-parameter generalization of the complete elliptic integral of the
second kind | The two parameter generalization of the complete elliptic integral of the
second kind discussed recently by Barsan is expressed in terms of ordinary
complete elliptic integrals.
| math-ph math.MP | the two parameter generalization of the complete elliptic integral of the second kind discussed recently by barsan is expressed in terms of ordinary complete elliptic integrals | [['the', 'two', 'parameter', 'generalization', 'of', 'the', 'complete', 'elliptic', 'integral', 'of', 'the', 'second', 'kind', 'discussed', 'recently', 'by', 'barsan', 'is', 'expressed', 'in', 'terms', 'of', 'ordinary', 'complete', 'elliptic', 'integrals']] | [-0.19941648408770563, 0.0457150910794735, -0.055074886307120326, 0.09379422361496836, -0.1342365002632141, -0.021707802191376687, -0.08742810320109129, 0.1907084560021758, -0.26753019511699677, -0.29757113456726075, 0.10420098524075001, -0.2800643629953265, -0.1526522470265627, 0.2565293578058481, -0.10044691987335681... |
709.129 | Supersymmetric version of a Gaussian irrotational compressible fluid
flow | The Lie point symmetries and corresponding invariant solutions are obtained
for a Gaussian, irrotational, compressible fluid flow. A supersymmetric
extension of this model is then formulated through the use of a superspace and
superfield formalism. The Lie superalgebra of this extended model is determined
and a class... | math-ph math.MP | the lie point symmetries and corresponding invariant solutions are obtained for a gaussian irrotational compressible fluid flow a supersymmetric extension of this model is then formulated through the use of a superspace and superfield formalism the lie superalgebra of this extended model is determined and a classificat... | [['the', 'lie', 'point', 'symmetries', 'and', 'corresponding', 'invariant', 'solutions', 'are', 'obtained', 'for', 'a', 'gaussian', 'irrotational', 'compressible', 'fluid', 'flow', 'a', 'supersymmetric', 'extension', 'of', 'this', 'model', 'is', 'then', 'formulated', 'through', 'the', 'use', 'of', 'a', 'superspace', 'a... | [-0.14696944563576345, 0.05854418759072053, -0.07988791623979472, 0.08875720666229642, -0.10070710560683621, -0.16366851012212005, -0.027798490052038195, 0.30362946527560103, -0.25797127488362237, -0.24164892476460154, 0.14971715211083464, -0.24156756622434247, -0.14861430981186, 0.14510679378414923, -0.040291454661323... |
709.1291 | On D.K. Biss' papers "The homotopy type of the matroid Grassmannian" and
"Oriented matroids, complex manifolds, and a combinatorial model for BU" | We point out a flaw in papers by Daniel Biss devoted to homotopy type of
matroid Grassmannians.
| math.CO math.AT | we point out a flaw in papers by daniel biss devoted to homotopy type of matroid grassmannians | [['we', 'point', 'out', 'a', 'flaw', 'in', 'papers', 'by', 'daniel', 'biss', 'devoted', 'to', 'homotopy', 'type', 'of', 'matroid', 'grassmannians']] | [-0.18409031870610573, -0.07492049471201266, -0.055283794289126116, 0.03037758601610275, -0.17057223826208534, -0.14201336482758908, 0.13173075984506047, 0.2803432279649903, -0.2758175849038012, -0.1723811887204647, 0.07359447293428649, -0.2573637844008558, -0.21979534264434786, 0.14258315381320083, -0.3092339486431549... |
709.1292 | A semiclassical theory of the Anderson transition | We study analytically the metal-insulator transition in a disordered
conductor by combining the self-consistent theory of localization with the one
parameter scaling theory. We provide explicit expressions of the critical
exponents and the critical disorder as a function of the spatial
dimensionality, $d$. The critic... | cond-mat.dis-nn | we study analytically the metalinsulator transition in a disordered conductor by combining the selfconsistent theory of localization with the one parameter scaling theory we provide explicit expressions of the critical exponents and the critical disorder as a function of the spatial dimensionality d the critical expone... | [['we', 'study', 'analytically', 'the', 'metalinsulator', 'transition', 'in', 'a', 'disordered', 'conductor', 'by', 'combining', 'the', 'selfconsistent', 'theory', 'of', 'localization', 'with', 'the', 'one', 'parameter', 'scaling', 'theory', 'we', 'provide', 'explicit', 'expressions', 'of', 'the', 'critical', 'exponent... | [-0.15737407881533727, 0.18369216156458737, -0.07164437915032197, 0.06868898275882072, 0.034157160064101584, -0.15294134542429155, 0.052136922664690895, 0.30168777169248123, -0.24996678639269834, -0.23893733694317884, 0.06059767370087294, -0.32033368827770964, -0.17806416084723814, 0.1573567637159223, 0.041306901008023... |
709.1293 | Weakly interacting Bose gases below the critical temperature | We consider a homogeneous non-ideal Bose gas at nonzero temperature in
equilibrium below the critical temperature $T_C$ in the framework of finite
temperature field theory. An algorithm is described in which a manageable
subset of diagrams can be considered which, coupled with a self--consistent
condition related to ... | cond-mat.other | we consider a homogeneous nonideal bose gas at nonzero temperature in equilibrium below the critical temperature t_c in the framework of finite temperature field theory an algorithm is described in which a manageable subset of diagrams can be considered which coupled with a selfconsistent condition related to the minim... | [['we', 'consider', 'a', 'homogeneous', 'nonideal', 'bose', 'gas', 'at', 'nonzero', 'temperature', 'in', 'equilibrium', 'below', 'the', 'critical', 'temperature', 't_c', 'in', 'the', 'framework', 'of', 'finite', 'temperature', 'field', 'theory', 'an', 'algorithm', 'is', 'described', 'in', 'which', 'a', 'manageable', 's... | [-0.13037633483744698, 0.19628413517975637, -0.09257287746600684, 0.045623288697899, -0.015229782883505353, -0.16304285202144844, 0.049921216891666294, 0.3309852618754643, -0.2514311541024534, -0.27971672538484704, 0.04830355195855325, -0.2277933922519938, -0.042677807781967475, 0.18223473136542273, -0.0217909371846767... |
709.1294 | Evolving small-world scale-free networks consist of cliques | We present a family of scale-free network model consisting of cliques, which
is established by a simple recursive algorithm. We investigate the networks
both analytically and numerically. The obtained analytical solutions show that
the networks follow a power-law degree distribution, with degree exponent
continuously... | physics.soc-ph | we present a family of scalefree network model consisting of cliques which is established by a simple recursive algorithm we investigate the networks both analytically and numerically the obtained analytical solutions show that the networks follow a powerlaw degree distribution with degree exponent continuously tuned b... | [['we', 'present', 'a', 'family', 'of', 'scalefree', 'network', 'model', 'consisting', 'of', 'cliques', 'which', 'is', 'established', 'by', 'a', 'simple', 'recursive', 'algorithm', 'we', 'investigate', 'the', 'networks', 'both', 'analytically', 'and', 'numerically', 'the', 'obtained', 'analytical', 'solutions', 'show',... | [-0.15212114818233957, 0.05962695983508902, -0.09324243559091482, 0.06384643020621336, -0.010268561863115118, -0.1754474362398508, 0.053941411163998386, 0.40957863244318193, -0.26281055587253743, -0.2709197470998412, 0.043155712831605186, -0.24566928410066433, -0.2732692194641918, 0.17283261719069654, 0.044213870360005... |
709.1295 | A Rationality Problem of Some Cremona Transformation | We will show the rationality of the function field of two variables under
certain Cremona transformation.
| math.AG math.RA | we will show the rationality of the function field of two variables under certain cremona transformation | [['we', 'will', 'show', 'the', 'rationality', 'of', 'the', 'function', 'field', 'of', 'two', 'variables', 'under', 'certain', 'cremona', 'transformation']] | [-0.26422192133031785, 0.08831985510187224, -0.14986077568028122, 0.024121833383105695, -0.06402091030031443, -0.030195962521247566, 0.0033360254019498825, 0.3974619684740901, -0.3696668199263513, -0.2288693634327501, 0.06159888233378297, -0.1993298212182708, -0.23701788252219558, 0.18513969611376524, -0.14074740582145... |
709.1296 | Twisted Symmetric Group Actions | We will show the raitonality of some twisted symmetric group actions.
| math.AG math.RA | we will show the raitonality of some twisted symmetric group actions | [['we', 'will', 'show', 'the', 'raitonality', 'of', 'some', 'twisted', 'symmetric', 'group', 'actions']] | [-0.3043003298342228, 0.22209749156609176, -0.12533892691135406, 0.05137750543653965, -0.15353654846549034, -0.04240074492990971, -0.02106029223650694, 0.5442333370447159, -0.2849741689860821, -0.14698389247059823, 0.19046879704110325, -0.22584692239761353, -0.24421844631433487, 0.15477382391691208, -0.1845765640959143... |
709.1297 | Reduction theorems for Noether's problem | We will give several reduction theorems for Noether's problem.
| math.RA math.AG | we will give several reduction theorems for noethers problem | [['we', 'will', 'give', 'several', 'reduction', 'theorems', 'for', 'noethers', 'problem']] | [-0.20074921598037085, 0.022119370082186326, -0.14053994965636069, 0.2190855865677198, -0.1812369173599614, -0.09748232561267084, 0.04523614376214229, 0.2725454154941771, -0.3336596108145184, -0.3581793995367156, 0.22039688870103824, -0.2648276335870226, -0.06927854919599162, 0.32506584458880955, -0.23347242259316975, ... |
709.1298 | Exponential Maps and Symmetric Transformations in Cluster-Spin System
for Lattice-Ising Models | We defined exponential maps with one parameter, associated with geodesics on
the parameter surface. By group theory we proposed a formula of the critical
points, which is a direct sum of the Lie subalgebras at the critical
temperature. We consider the self similar transformations as symmetric
operations. In the opini... | physics.gen-ph | we defined exponential maps with one parameter associated with geodesics on the parameter surface by group theory we proposed a formula of the critical points which is a direct sum of the lie subalgebras at the critical temperature we consider the self similar transformations as symmetric operations in the opinion of s... | [['we', 'defined', 'exponential', 'maps', 'with', 'one', 'parameter', 'associated', 'with', 'geodesics', 'on', 'the', 'parameter', 'surface', 'by', 'group', 'theory', 'we', 'proposed', 'a', 'formula', 'of', 'the', 'critical', 'points', 'which', 'is', 'a', 'direct', 'sum', 'of', 'the', 'lie', 'subalgebras', 'at', 'the',... | [-0.18328165651473682, 0.11790245670636068, -0.07527492568260641, 0.05357853623263509, -0.02897379312707926, -0.13311697427707259, 0.0849383129270791, 0.36467073402309325, -0.2538125047685753, -0.22225977571361, 0.10747894853830076, -0.2981813808946754, -0.151327981857321, 0.16650680913699034, -0.017562041815835983, 0.... |
709.1299 | Monovacancy and Substitutional Defects in Hexagonal Silicon Nanotubes | We present a first-principle study of geometrical and electronic structure of
hexagonal single-walled silicon nanotubes with a monovacancy or a
substitutional defect. The C, Al or P atoms are chosen as substitutional
impurities. It is found that the defect such as a monovacancy or a
substitutional impurity results in... | cond-mat.mtrl-sci | we present a firstprinciple study of geometrical and electronic structure of hexagonal singlewalled silicon nanotubes with a monovacancy or a substitutional defect the c al or p atoms are chosen as substitutional impurities it is found that the defect such as a monovacancy or a substitutional impurity results in deform... | [['we', 'present', 'a', 'firstprinciple', 'study', 'of', 'geometrical', 'and', 'electronic', 'structure', 'of', 'hexagonal', 'singlewalled', 'silicon', 'nanotubes', 'with', 'a', 'monovacancy', 'or', 'a', 'substitutional', 'defect', 'the', 'c', 'al', 'or', 'p', 'atoms', 'are', 'chosen', 'as', 'substitutional', 'impuriti... | [-0.11978012838283147, 0.16629499716727042, 0.03716384008227066, 0.011647126751138303, 0.06646164380356498, -0.18237262849706684, 0.11794344992805059, 0.4837041924996623, -0.25318424268251005, -0.2551613365481982, -0.03528809577799349, -0.36904933739282275, -0.14399364652465388, 0.05149036248471459, 0.01619226340439984... |
709.13 | Staggered t-structures on derived categories of equivariant coherent
sheaves | Let X be a scheme, and let G be an affine group scheme acting on X. Under
reasonable hypotheses on X and G, we construct a t-structure on the derived
category of G-equivariant coherent sheaves that in many ways resembles the
perverse coherent t-structure, but which incorporates additional information
from the G-actio... | math.RT math.AG | let x be a scheme and let g be an affine group scheme acting on x under reasonable hypotheses on x and g we construct a tstructure on the derived category of gequivariant coherent sheaves that in many ways resembles the perverse coherent tstructure but which incorporates additional information from the gaction under ce... | [['let', 'x', 'be', 'a', 'scheme', 'and', 'let', 'g', 'be', 'an', 'affine', 'group', 'scheme', 'acting', 'on', 'x', 'under', 'reasonable', 'hypotheses', 'on', 'x', 'and', 'g', 'we', 'construct', 'a', 'tstructure', 'on', 'the', 'derived', 'category', 'of', 'gequivariant', 'coherent', 'sheaves', 'that', 'in', 'many', 'wa... | [-0.21458068432073799, 0.0945797291329338, -0.1620235134108478, 0.08433801751664799, -0.12458519586463175, -0.19188815066287213, -0.0016351381630596259, 0.43894673527582834, -0.39607344880183204, -0.13076142327981474, 0.06818709158814391, -0.16393660100521115, -0.12740236549617964, 0.2534138924118293, -0.24921656041102... |
709.1301 | Observations of Intrahour Variable Quasars: Scattering in our Galactic
Neighbourhood | Interstellar scintillation (ISS) has been established as the cause of the
random variations seen at centimetre wavelengths in many compact radio sources
on timescales of a day or less. Observations of ISS can be used to probe
structure both in the ionized insterstellar medium of the Galaxy, and in the
extragalactic s... | astro-ph | interstellar scintillation iss has been established as the cause of the random variations seen at centimetre wavelengths in many compact radio sources on timescales of a day or less observations of iss can be used to probe structure both in the ionized insterstellar medium of the galaxy and in the extragalactic sources... | [['interstellar', 'scintillation', 'iss', 'has', 'been', 'established', 'as', 'the', 'cause', 'of', 'the', 'random', 'variations', 'seen', 'at', 'centimetre', 'wavelengths', 'in', 'many', 'compact', 'radio', 'sources', 'on', 'timescales', 'of', 'a', 'day', 'or', 'less', 'observations', 'of', 'iss', 'can', 'be', 'used',... | [-0.1073467096795913, 0.16728273037080774, -0.08762203438107882, 0.1136967293128598, -0.08620825916146621, -0.09077906806189089, -0.015830803178967193, 0.47662667927738184, -0.19525475549893692, -0.32379187910387724, 0.1590063429261462, -0.2564819072000458, -0.025056485715023696, 0.24791133821529981, -0.032379306755804... |
709.1302 | Exactly soluble spin-1/2 models on three-dimensional lattices and
non-abelian statistics of closed string excitations | Exactly soluble spin-$\frac{1}2$ models on three-dimensional lattices are
proposed by generalizing Kitaev model on honeycomb lattice to three dimensions
with proper periodic boundary conditions. The simplest example is spins on a
diamond lattice which is exactly soluble. The ground state sector of the model
may be ma... | cond-mat.str-el cond-mat.mes-hall | exactly soluble spinfrac12 models on threedimensional lattices are proposed by generalizing kitaev model on honeycomb lattice to three dimensions with proper periodic boundary conditions the simplest example is spins on a diamond lattice which is exactly soluble the ground state sector of the model may be mapped into a... | [['exactly', 'soluble', 'spinfrac12', 'models', 'on', 'threedimensional', 'lattices', 'are', 'proposed', 'by', 'generalizing', 'kitaev', 'model', 'on', 'honeycomb', 'lattice', 'to', 'three', 'dimensions', 'with', 'proper', 'periodic', 'boundary', 'conditions', 'the', 'simplest', 'example', 'is', 'spins', 'on', 'a', 'di... | [-0.19568351035548456, 0.3200737075549385, -0.059132361450969284, 0.05284055270456167, -0.06718166946579437, -0.2219929425045848, 0.05378913116613542, 0.3896188044976165, -0.2295597805085578, -0.1859704719633976, 0.08335017216298034, -0.3096395278238316, -0.12184108567855029, 0.09517029675814921, 0.04531407371900086, 0... |
709.1303 | Global coupling at 660 km is proposed to explain plate tectonics and the
generation of the earth's magnetic field | The presence of low viscosity layers in the mantle is supported by line of
geological and geophysical observations. Recent high pressure and temperature
investigations indicated that partial carbonate melt should exist at the bottom
of the lithosphere and at 660 km. The presence of few percent carbonate melt
reduces ... | physics.gen-ph | the presence of low viscosity layers in the mantle is supported by line of geological and geophysical observations recent high pressure and temperature investigations indicated that partial carbonate melt should exist at the bottom of the lithosphere and at 660 km the presence of few percent carbonate melt reduces the ... | [['the', 'presence', 'of', 'low', 'viscosity', 'layers', 'in', 'the', 'mantle', 'is', 'supported', 'by', 'line', 'of', 'geological', 'and', 'geophysical', 'observations', 'recent', 'high', 'pressure', 'and', 'temperature', 'investigations', 'indicated', 'that', 'partial', 'carbonate', 'melt', 'should', 'exist', 'at', '... | [-0.09432124895380532, 0.1700673546272178, -0.015404000194703645, 0.016065248184183492, -0.07101225080827238, -0.042251803048602335, 0.019420608204412968, 0.3144848200935104, -0.24972153711958345, -0.36061947239259035, 0.13846713932914698, -0.264960937401885, -0.04431518661305151, 0.20390625952921332, -0.02484852359762... |
709.1304 | A design principle for improved 3D AC electro-osmotic pumps | Three-dimensional (3D) AC electro-osmotic (ACEO) pumps have recently been
developed that are much faster and more robust than previous planar designs.
The basic idea is to create a ``fluid conveyor belt'' by placing opposing ACEO
slip velocities at different heights. Current designs involve electrodes with
electropla... | physics.flu-dyn | threedimensional 3d ac electroosmotic aceo pumps have recently been developed that are much faster and more robust than previous planar designs the basic idea is to create a fluid conveyor belt by placing opposing aceo slip velocities at different heights current designs involve electrodes with electroplated steps whos... | [['threedimensional', '3d', 'ac', 'electroosmotic', 'aceo', 'pumps', 'have', 'recently', 'been', 'developed', 'that', 'are', 'much', 'faster', 'and', 'more', 'robust', 'than', 'previous', 'planar', 'designs', 'the', 'basic', 'idea', 'is', 'to', 'create', 'a', 'fluid', 'conveyor', 'belt', 'by', 'placing', 'opposing', 'a... | [-0.12295368539273413, 0.21599088147626194, -0.048015244336780706, -0.03413964485189001, -0.05456044592722816, -0.1905997416176336, -0.05776396646837984, 0.4185060001909733, -0.22442173322174444, -0.3295022730435272, 0.09115247954998744, -0.2451813639711263, -0.11663874256926435, 0.24007786366889633, -0.069295816548458... |
709.1305 | Possible evidence that pulsars are quark stars | It is a pity that the real state of matter in pulsar-like stars is still not
determined confidently because of the uncertainty about cold matter at
supranuclear density, even 40 years after the discovery of pulsar. Nuclear
matter (related to neutron stars) is one of the speculations for the inner
constitution of puls... | astro-ph hep-ph | it is a pity that the real state of matter in pulsarlike stars is still not determined confidently because of the uncertainty about cold matter at supranuclear density even 40 years after the discovery of pulsar nuclear matter related to neutron stars is one of the speculations for the inner constitution of pulsars eve... | [['it', 'is', 'a', 'pity', 'that', 'the', 'real', 'state', 'of', 'matter', 'in', 'pulsarlike', 'stars', 'is', 'still', 'not', 'determined', 'confidently', 'because', 'of', 'the', 'uncertainty', 'about', 'cold', 'matter', 'at', 'supranuclear', 'density', 'even', '40', 'years', 'after', 'the', 'discovery', 'of', 'pulsar'... | [-0.04669149879867893, 0.2243127176862146, -0.1237709670930996, 0.15085565364709727, -0.1725532650475351, -0.07942821221298237, 0.07388567347505826, 0.31806290328410836, -0.1816343720098482, -0.34917049453278975, 0.059394658530872106, -0.298191594943719, -0.007971797912368472, 0.19629559737653143, -0.050811964431515255... |
709.1306 | Necessary and sufficient condition for Greenberger-Horne-Zeilinger
diagonal states to be full $N$-partite entangled | Recently, [{arXiv:0810.3134}] is accepted and published. We show that any
$N$-qubit state which is diagonal in the Greenberger-Horne-Zeilinger basis is
full $N$-qubit entangled state if and only if no partial transpose of the
multiqubit state is positive with respect to any partition.
| quant-ph | recently arxiv08103134 is accepted and published we show that any nqubit state which is diagonal in the greenbergerhornezeilinger basis is full nqubit entangled state if and only if no partial transpose of the multiqubit state is positive with respect to any partition | [['recently', 'arxiv08103134', 'is', 'accepted', 'and', 'published', 'we', 'show', 'that', 'any', 'nqubit', 'state', 'which', 'is', 'diagonal', 'in', 'the', 'greenbergerhornezeilinger', 'basis', 'is', 'full', 'nqubit', 'entangled', 'state', 'if', 'and', 'only', 'if', 'no', 'partial', 'transpose', 'of', 'the', 'multiqub... | [-0.13474474658834792, 0.19279158122593626, -0.051873305368991124, -0.0013527144966203543, -0.04265059779087702, -0.23474311977181406, 0.02808273627999283, 0.37017806131570113, -0.18366585197370677, -0.19164076243067116, 0.09593475494433992, -0.28882971964776516, -0.06747259625366755, 0.1042010842689446, -0.01940104549... |
709.1307 | MOST: detecting cancer differential gene expression | We propose a new statistics for the detection of differentially expressed
genes, when the genes are activated only in a subset of the samples. Statistics
designed for this unconventional circumstance has proved to be valuable for
most cancer studies, where oncogenes are activated for a small number of
disease samples... | stat.AP | we propose a new statistics for the detection of differentially expressed genes when the genes are activated only in a subset of the samples statistics designed for this unconventional circumstance has proved to be valuable for most cancer studies where oncogenes are activated for a small number of disease samples prev... | [['we', 'propose', 'a', 'new', 'statistics', 'for', 'the', 'detection', 'of', 'differentially', 'expressed', 'genes', 'when', 'the', 'genes', 'are', 'activated', 'only', 'in', 'a', 'subset', 'of', 'the', 'samples', 'statistics', 'designed', 'for', 'this', 'unconventional', 'circumstance', 'has', 'proved', 'to', 'be', '... | [-0.09284392566741127, 0.1160955179338027, -0.057868011648432145, 0.0687631768732811, -0.11395543249034622, -0.15568315051948128, 0.07798268432159303, 0.3509972042548787, -0.2389010785778225, -0.2835149413553401, 0.08650514936228328, -0.2990013825010906, -0.14784522733009123, 0.22637023249622976, -0.09964158563666696, ... |
709.1308 | Cirquent calculus deepened | Cirquent calculus is a new proof-theoretic and semantic framework, whose main
distinguishing feature is being based on circuits, as opposed to the more
traditional approaches that deal with tree-like objects such as formulas or
sequents. Among its advantages are greater efficiency, flexibility and
expressiveness. Thi... | cs.LO math.LO | cirquent calculus is a new prooftheoretic and semantic framework whose main distinguishing feature is being based on circuits as opposed to the more traditional approaches that deal with treelike objects such as formulas or sequents among its advantages are greater efficiency flexibility and expressiveness this paper p... | [['cirquent', 'calculus', 'is', 'a', 'new', 'prooftheoretic', 'and', 'semantic', 'framework', 'whose', 'main', 'distinguishing', 'feature', 'is', 'being', 'based', 'on', 'circuits', 'as', 'opposed', 'to', 'the', 'more', 'traditional', 'approaches', 'that', 'deal', 'with', 'treelike', 'objects', 'such', 'as', 'formulas'... | [-0.07181848537158937, 0.0096965014917376, -0.12679999355847638, 0.11202242746352194, -0.18344323543640664, -0.18241543686494996, 0.0684956199519384, 0.3434833188051692, -0.2767341541412931, -0.2974009671033575, 0.06900570678214232, -0.24313909780257978, -0.15391427217146908, 0.21304880238066498, -0.1700609656855261, 0... |
709.1309 | Bayes and empirical Bayes changepoint problems | We generalize the approach of Liu and Lawrence (1999) for multiple
changepoint problems where the number of changepoints is unknown. The approach
is based on dynamic programming recursion for efficient calculation of the
marginal probability of the data with the hidden parameters integrated out. For
the estimation of... | stat.CO stat.ME | we generalize the approach of liu and lawrence 1999 for multiple changepoint problems where the number of changepoints is unknown the approach is based on dynamic programming recursion for efficient calculation of the marginal probability of the data with the hidden parameters integrated out for the estimation of the h... | [['we', 'generalize', 'the', 'approach', 'of', 'liu', 'and', 'lawrence', '1999', 'for', 'multiple', 'changepoint', 'problems', 'where', 'the', 'number', 'of', 'changepoints', 'is', 'unknown', 'the', 'approach', 'is', 'based', 'on', 'dynamic', 'programming', 'recursion', 'for', 'efficient', 'calculation', 'of', 'the', '... | [-0.027287081192393522, 0.007565494932567895, -0.09867887585354385, 0.09432606649091606, -0.09680742428832646, -0.10447437274478265, 0.09680530665887159, 0.3876834968035457, -0.26528795887785617, -0.3414388370088566, 0.13200303747878173, -0.2697378502352469, -0.12936310253258962, 0.21931113912932462, -0.079451270352826... |
709.131 | Pairing Correlations in halo Nuclei | Paring correlations in weakly bound halo nuclei $^{6}$He and $^{11}$Li are
studied by using a three-body model with a density-dependent contact
interaction. We investigate the spatial structure of two-neutron wave function
in a Borromean nucleus $^{11}$Li.The behavior of the neutron pair at different
densities is sim... | nucl-ex | paring correlations in weakly bound halo nuclei 6he and 11li are studied by using a threebody model with a densitydependent contact interaction we investigate the spatial structure of twoneutron wave function in a borromean nucleus 11lithe behavior of the neutron pair at different densities is simulated by calculating ... | [['paring', 'correlations', 'in', 'weakly', 'bound', 'halo', 'nuclei', '6he', 'and', '11li', 'are', 'studied', 'by', 'using', 'a', 'threebody', 'model', 'with', 'a', 'densitydependent', 'contact', 'interaction', 'we', 'investigate', 'the', 'spatial', 'structure', 'of', 'twoneutron', 'wave', 'function', 'in', 'a', 'borr... | [-0.05747601766046797, 0.19907637301119083, -0.09123691162160526, 0.17436598689569463, 0.04778843985685537, -0.07348542371665702, 0.032657286497361375, 0.37801064793945205, -0.2058782874150796, -0.3051310838299229, -0.09696257698963931, -0.33567938668296693, -0.01496297713527654, 0.1289980846642127, 0.14331257659512578... |
709.1311 | Higher order terms in the condensate fraction of a homogeneous and
dilute Bose gas | The condensate fraction of a homogeneous and dilute Bose gas is expanded as a
power series of $\sqrt{n a^3}$ as $N_0/N = 1 -c_1 (n a^3)^{1/2} -c_2 (n a^3) -
c_3 (n a^3)^{3/2}\hdots.$ The coefficient $c_1$ is well-known as $8/3
\sqrt{\pi}$, but the others are unknown yet. Considering two-body contact
interactions and ... | cond-mat.stat-mech | the condensate fraction of a homogeneous and dilute bose gas is expanded as a power series of sqrtn a3 as n_0n 1 c_1 n a312 c_2 n a3 c_3 n a332hdots the coefficient c_1 is wellknown as 83 sqrtpi but the others are unknown yet considering twobody contact interactions and applying a canonical transformation method twice ... | [['the', 'condensate', 'fraction', 'of', 'a', 'homogeneous', 'and', 'dilute', 'bose', 'gas', 'is', 'expanded', 'as', 'a', 'power', 'series', 'of', 'sqrtn', 'a3', 'as', 'n_0n', '1', 'c_1', 'n', 'a312', 'c_2', 'n', 'a3', 'c_3', 'n', 'a332hdots', 'the', 'coefficient', 'c_1', 'is', 'wellknown', 'as', '83', 'sqrtpi', 'but',... | [-0.16630203739041463, 0.15760430681180237, -0.06480008622645127, 0.03617959973429713, -0.026137255953953546, -0.20312273558092248, 0.05967908771160771, 0.3296838944668279, -0.24118001651676263, -0.27266957990359514, 0.03302860117983073, -0.317301191371756, -0.1079259823925574, 0.13678618380868368, 0.03963330926044899,... |
709.1312 | Bottomed Analog of Z+(4433) | The newly observed $Z^+ (4433)$ resonance by BELLE is believed to be a
tetraquark bound state made up of $(cu)(\bar c \bar d)$. We propose the
bottomed analog of this bound state, namely, by replacing one of the charm
quarks by a bottom quark, thus forming $Z_{bc}^{0, \pm, \pm\pm}$. One of the
$Z_{bc}$ is doubly char... | hep-ph | the newly observed z 4433 resonance by belle is believed to be a tetraquark bound state made up of cubar c bar d we propose the bottomed analog of this bound state namely by replacing one of the charm quarks by a bottom quark thus forming z_bc0 pm pmpm one of the z_bc is doubly charged the predicted mass of z_bc is aro... | [['the', 'newly', 'observed', 'z', '4433', 'resonance', 'by', 'belle', 'is', 'believed', 'to', 'be', 'a', 'tetraquark', 'bound', 'state', 'made', 'up', 'of', 'cubar', 'c', 'bar', 'd', 'we', 'propose', 'the', 'bottomed', 'analog', 'of', 'this', 'bound', 'state', 'namely', 'by', 'replacing', 'one', 'of', 'the', 'charm', ... | [-0.06870859097486928, 0.3204180109760036, -0.0717567500607718, 0.11939992282904037, -0.014837016329250259, -0.16929310520139076, 0.13315813859276798, 0.28593068665055477, -0.15268709273887393, -0.2685932438172724, -0.019385386491194367, -0.31282471784431004, 0.0815486930148757, 0.0903532902750632, 0.07317189571002256,... |
709.1313 | Entanglement of Uniformly Accelerating Schrodinger, Dirac, and Scalar
Particles | We study how the entanglement of an entangled pair of particles is affected
when one or both of the pair is uniformly accelerated, while the detector
remains in an inertial frame. We find that the entanglement is unchanged if all
degrees of freedom are considered. However, particle pairs are produced when a
relativis... | quant-ph | we study how the entanglement of an entangled pair of particles is affected when one or both of the pair is uniformly accelerated while the detector remains in an inertial frame we find that the entanglement is unchanged if all degrees of freedom are considered however particle pairs are produced when a relativistic pa... | [['we', 'study', 'how', 'the', 'entanglement', 'of', 'an', 'entangled', 'pair', 'of', 'particles', 'is', 'affected', 'when', 'one', 'or', 'both', 'of', 'the', 'pair', 'is', 'uniformly', 'accelerated', 'while', 'the', 'detector', 'remains', 'in', 'an', 'inertial', 'frame', 'we', 'find', 'that', 'the', 'entanglement', 'i... | [-0.15001984616106187, 0.3004385847146958, -0.06945110255432063, 0.07636991145594393, 0.0020426354367064975, -0.16378164286646296, -0.07738097638515282, 0.3625287499310354, -0.2630350256528137, -0.26750968972820854, 0.01710527025407843, -0.3365726140248826, -0.024589986380552716, 0.15066571174765606, -0.001047833388576... |
709.1314 | Quantum metamaterials: Electromagnetic waves in a Josephson qubit line | We consider the propagation of a classical electromagnetic wave through a
transmission line, formed by identical superconducting charge qubits inside a
superconducting resonator. Since the qubits can be in a coherent superposition
of quantum states, we show that such a system demonstrates interesting new
effects, suc... | cond-mat.supr-con cond-mat.other quant-ph | we consider the propagation of a classical electromagnetic wave through a transmission line formed by identical superconducting charge qubits inside a superconducting resonator since the qubits can be in a coherent superposition of quantum states we show that such a system demonstrates interesting new effects such as a... | [['we', 'consider', 'the', 'propagation', 'of', 'a', 'classical', 'electromagnetic', 'wave', 'through', 'a', 'transmission', 'line', 'formed', 'by', 'identical', 'superconducting', 'charge', 'qubits', 'inside', 'a', 'superconducting', 'resonator', 'since', 'the', 'qubits', 'can', 'be', 'in', 'a', 'coherent', 'superposi... | [-0.24705228313570843, 0.2488242144070682, -0.027928231242112814, -0.02611954169231467, -0.020088237505406142, -0.16696686433162541, 0.05749521341160289, 0.38951692771166563, -0.2528706772439182, -0.2121099816635251, 0.007538570961914956, -0.2644124576076865, -0.1278627245919779, 0.24890735886991025, 0.0433392996701877... |
709.1315 | Recent progress in B physics | We firstly address the recent efforts on calculations of the next-to-leading
order corrections to the color-suppressed tree amplitude in QCD factorization
method which may be essential to solve the puzzles in $B\to \pi\pi$ and $\pi K$
decays. Then we discuss the polarization puzzles in $B\to \phi K^*$ and $\rho
K^*$.... | hep-ph | we firstly address the recent efforts on calculations of the nexttoleading order corrections to the colorsuppressed tree amplitude in qcd factorization method which may be essential to solve the puzzles in bto pipi and pi k decays then we discuss the polarization puzzles in bto phi k and rho k the impacts of the newly ... | [['we', 'firstly', 'address', 'the', 'recent', 'efforts', 'on', 'calculations', 'of', 'the', 'nexttoleading', 'order', 'corrections', 'to', 'the', 'colorsuppressed', 'tree', 'amplitude', 'in', 'qcd', 'factorization', 'method', 'which', 'may', 'be', 'essential', 'to', 'solve', 'the', 'puzzles', 'in', 'bto', 'pipi', 'and... | [-0.08141256883740425, 0.2311891064234078, -0.08029913627076894, 0.10390268164686858, -0.10754294272745028, -0.11716628354042768, 0.08329750466742553, 0.29186679373960944, -0.2560554015357047, -0.17757341797463597, 0.012854737989837304, -0.41258743934333325, -0.06877203351119533, 0.11368493559537456, 0.0726620957325212... |
709.1316 | A mean ergodic theorem for actions of amenable quantum groups | We prove a weak form of the mean ergodic theorem for actions of amenable
locally compact quantum groups in the von Neumann algebra setting.
| math.OA | we prove a weak form of the mean ergodic theorem for actions of amenable locally compact quantum groups in the von neumann algebra setting | [['we', 'prove', 'a', 'weak', 'form', 'of', 'the', 'mean', 'ergodic', 'theorem', 'for', 'actions', 'of', 'amenable', 'locally', 'compact', 'quantum', 'groups', 'in', 'the', 'von', 'neumann', 'algebra', 'setting']] | [-0.161040668686231, 0.15140041107467064, -0.14542095378662148, 0.10484548332169652, -0.06158568554868301, -0.1745110053840714, 0.039926937034276, 0.3460489546317452, -0.3221745854243636, -0.054411082955387734, 0.15719282479161242, -0.22262595458111414, -0.08211030714058627, 0.28098883739827824, -0.2045608851670598, 0.... |
709.1317 | Forecasting neutrino masses from combining KATRIN and the CMB:
Frequentist and Bayesian analyses | We present a showcase for deriving bounds on the neutrino masses from
laboratory experiments and cosmological observations. We compare the
frequentist and Bayesian bounds on the effective electron neutrino mass m_beta
which the KATRIN neutrino mass experiment is expected to obtain, using both an
analytical likelihood... | hep-ph astro-ph | we present a showcase for deriving bounds on the neutrino masses from laboratory experiments and cosmological observations we compare the frequentist and bayesian bounds on the effective electron neutrino mass m_beta which the katrin neutrino mass experiment is expected to obtain using both an analytical likelihood fun... | [['we', 'present', 'a', 'showcase', 'for', 'deriving', 'bounds', 'on', 'the', 'neutrino', 'masses', 'from', 'laboratory', 'experiments', 'and', 'cosmological', 'observations', 'we', 'compare', 'the', 'frequentist', 'and', 'bayesian', 'bounds', 'on', 'the', 'effective', 'electron', 'neutrino', 'mass', 'm_beta', 'which',... | [-0.05313479816091961, 0.12663426968190158, -0.08303020248983793, 0.13371212028739926, -0.03972719751563169, -0.09680544075362271, 0.10753506602752519, 0.3488660065060113, -0.17278513561716766, -0.3794292269196588, 0.0708184408577665, -0.3433014421255758, 0.010717324348790618, 0.23404822156996216, 0.008113796641898867,... |
709.1318 | Timelike Boundary Sine-Gordon Theory and Two-Component Plasma | It has long been known that there is a relation between boundary sine-Gordon
theory and thermodynamics of charge neutral two-component Coulomb plasma on a
unit circle. On the other hand, recently it was found that open string
worldsheet description of brane decay can be related to a sequence of points of
thermodynami... | hep-th cond-mat.stat-mech | it has long been known that there is a relation between boundary sinegordon theory and thermodynamics of charge neutral twocomponent coulomb plasma on a unit circle on the other hand recently it was found that open string worldsheet description of brane decay can be related to a sequence of points of thermodynamic equi... | [['it', 'has', 'long', 'been', 'known', 'that', 'there', 'is', 'a', 'relation', 'between', 'boundary', 'sinegordon', 'theory', 'and', 'thermodynamics', 'of', 'charge', 'neutral', 'twocomponent', 'coulomb', 'plasma', 'on', 'a', 'unit', 'circle', 'on', 'the', 'other', 'hand', 'recently', 'it', 'was', 'found', 'that', 'op... | [-0.14645674791698512, 0.18467579885828692, -0.1286502327831065, 0.08018783774362225, -0.03271134577111387, -0.18032642085578476, 0.026899483405076516, 0.34888505037171674, -0.26690377855719233, -0.22293229417142565, 0.06397891445009068, -0.2863010596102256, -0.09870309239161797, 0.1499016159595769, 0.00261345708391583... |
709.1319 | A Thermodynamic Interpretation of Time for Superstring Rolling Tachyons | Rolling tachyon backgrounds, arising from open strings on unstable branes in
bosonic string theory, can be related to a simple statistical mechanical model
- Coulomb gas of point charges in two dimensions confined to a circle, the
Dyson gas. In this letter we describe a statistical system that is dual to
non-BPS bran... | hep-th | rolling tachyon backgrounds arising from open strings on unstable branes in bosonic string theory can be related to a simple statistical mechanical model coulomb gas of point charges in two dimensions confined to a circle the dyson gas in this letter we describe a statistical system that is dual to nonbps branes in sup... | [['rolling', 'tachyon', 'backgrounds', 'arising', 'from', 'open', 'strings', 'on', 'unstable', 'branes', 'in', 'bosonic', 'string', 'theory', 'can', 'be', 'related', 'to', 'a', 'simple', 'statistical', 'mechanical', 'model', 'coulomb', 'gas', 'of', 'point', 'charges', 'in', 'two', 'dimensions', 'confined', 'to', 'a', '... | [-0.14970806049669602, 0.22143940872439508, -0.10729779418704383, 0.11244946375640967, -0.005808798355584064, -0.18047474600437485, 0.04248820481497501, 0.2846880778670311, -0.2432046935611059, -0.22988659050315619, 0.03946763875480909, -0.30085581499204206, -0.12051273658714687, 0.10829453138121811, -0.100481409239425... |
709.132 | CANGAROO-III Search for Gamma Rays from SN 1987A and the Surrounding
Field | Optical images of SN 1987A show a triple ring structure. The inner (dust)
ring has recently increased in brightness and in the number of hot spots
suggesting that the supernova shock wave has collided with the dense
pre-existing circumstellar medium, a scenario supported by radio and X-ray
observations. Such a shocke... | astro-ph | optical images of sn 1987a show a triple ring structure the inner dust ring has recently increased in brightness and in the number of hot spots suggesting that the supernova shock wave has collided with the dense preexisting circumstellar medium a scenario supported by radio and xray observations such a shocked environ... | [['optical', 'images', 'of', 'sn', '1987a', 'show', 'a', 'triple', 'ring', 'structure', 'the', 'inner', 'dust', 'ring', 'has', 'recently', 'increased', 'in', 'brightness', 'and', 'in', 'the', 'number', 'of', 'hot', 'spots', 'suggesting', 'that', 'the', 'supernova', 'shock', 'wave', 'has', 'collided', 'with', 'the', 'de... | [-0.1064965017979369, 0.11608864685685254, -0.050067768921619474, 0.08031751284198392, -0.0915839045742514, -0.05832054039311348, 0.05918939381863187, 0.4298564086281726, -0.19006402941727948, -0.3427077984551386, 0.07285868087672584, -0.29178546475195866, -0.0008290425437141438, 0.2145959353106109, 0.00476013719370322... |
709.1321 | WKB approximation in deformed space with minimal length and minimal
momentum | A Bohr-Sommerfeld quantization rule is generalized for the case of the
deformed commutation relation leading to minimal uncertainties in both
coordinate and momentum operators. The correctness of the rule is verified by
comparing obtained results with exact expressions for corresponding spectra.
| quant-ph | a bohrsommerfeld quantization rule is generalized for the case of the deformed commutation relation leading to minimal uncertainties in both coordinate and momentum operators the correctness of the rule is verified by comparing obtained results with exact expressions for corresponding spectra | [['a', 'bohrsommerfeld', 'quantization', 'rule', 'is', 'generalized', 'for', 'the', 'case', 'of', 'the', 'deformed', 'commutation', 'relation', 'leading', 'to', 'minimal', 'uncertainties', 'in', 'both', 'coordinate', 'and', 'momentum', 'operators', 'the', 'correctness', 'of', 'the', 'rule', 'is', 'verified', 'by', 'com... | [-0.12356851754210345, 0.06780126525895534, -0.08520400408291962, 0.12768733231691506, -0.0826365856351558, -0.12947929356383478, 0.08284762787360062, 0.32270561530050346, -0.21603586738247696, -0.2556285869000798, 0.06300595603463036, -0.2703811964020133, -0.09312404828464113, 0.2054086281895274, -0.05136677025385746,... |
709.1322 | Scaling properties at the interface between different critical
subsystems: The Ashkin-Teller model | We consider two critical semi-infinite subsystems with different critical
exponents and couple them through their surfaces. The critical behavior at the
interface, influenced by the critical fluctuations of the two subsystems, can
be quite rich. In order to examine the various possibilities, we study a system
compose... | cond-mat.stat-mech | we consider two critical semiinfinite subsystems with different critical exponents and couple them through their surfaces the critical behavior at the interface influenced by the critical fluctuations of the two subsystems can be quite rich in order to examine the various possibilities we study a system composed of two... | [['we', 'consider', 'two', 'critical', 'semiinfinite', 'subsystems', 'with', 'different', 'critical', 'exponents', 'and', 'couple', 'them', 'through', 'their', 'surfaces', 'the', 'critical', 'behavior', 'at', 'the', 'interface', 'influenced', 'by', 'the', 'critical', 'fluctuations', 'of', 'the', 'two', 'subsystems', 'c... | [-0.2142133710421319, 0.2090340879730638, -0.057365032980536544, 0.03892193660158967, 0.011706572328883459, -0.21019438347907934, 0.04111808218342078, 0.3204895186841836, -0.274717389310642, -0.2996560646811636, 0.07883048724909351, -0.3201531421003212, -0.1496726323649802, 0.18506540255215279, 0.07405047117906614, 0.0... |
709.1323 | Reducing the magnetic susceptibility of parts in a magnetic gradiometer | In this paper we report a detailed investigation of a number of different
materials commonly used in precision instrumentation in the view of using them
as critical components in the magnetic gradiometer. The materials requirement
inside a magnetic gradiometer is stringent because the presence of magnetic
susceptible... | cond-mat.mtrl-sci | in this paper we report a detailed investigation of a number of different materials commonly used in precision instrumentation in the view of using them as critical components in the magnetic gradiometer the materials requirement inside a magnetic gradiometer is stringent because the presence of magnetic susceptible ma... | [['in', 'this', 'paper', 'we', 'report', 'a', 'detailed', 'investigation', 'of', 'a', 'number', 'of', 'different', 'materials', 'commonly', 'used', 'in', 'precision', 'instrumentation', 'in', 'the', 'view', 'of', 'using', 'them', 'as', 'critical', 'components', 'in', 'the', 'magnetic', 'gradiometer', 'the', 'materials'... | [-0.11334744564840528, 0.16304419588725055, -0.0106677012073715, -0.017436978753784117, -0.045434774477248085, -0.09817161211630202, 0.062935555859412, 0.3694174161735382, -0.23170919932481895, -0.3873456629945804, 0.10526275205361935, -0.30434848102634304, -0.11484697645970883, 0.21068581802955338, -0.0730477870186037... |
709.1324 | High-Energy Limit of Massless Dirac Fermions in Multilayer Graphene
using Magneto-Optical Transmission Spectroscopy | We have investigated the absorption spectrum of multilayer graphene in high
magnetic fields. The low energy part of the spectrum of electrons in graphene
is well described by the relativistic Dirac equation with a linear dispersion
relation. However, at higher energies (>500 meV) a deviation from the ideal
behavior o... | cond-mat.mes-hall cond-mat.other | we have investigated the absorption spectrum of multilayer graphene in high magnetic fields the low energy part of the spectrum of electrons in graphene is well described by the relativistic dirac equation with a linear dispersion relation however at higher energies 500 mev a deviation from the ideal behavior of dirac ... | [['we', 'have', 'investigated', 'the', 'absorption', 'spectrum', 'of', 'multilayer', 'graphene', 'in', 'high', 'magnetic', 'fields', 'the', 'low', 'energy', 'part', 'of', 'the', 'spectrum', 'of', 'electrons', 'in', 'graphene', 'is', 'well', 'described', 'by', 'the', 'relativistic', 'dirac', 'equation', 'with', 'a', 'li... | [-0.1329536438182307, 0.17588570552607052, -0.05463862537908426, 0.09988848455517048, -0.011315626393601027, -0.11682759842976036, 0.035086406836247384, 0.37814696847150725, -0.2534840079946055, -0.3728690145944711, -0.0577659218821888, -0.36903064309929806, -0.0593667837480704, 0.18394488958923225, 0.06042903324851068... |
709.1325 | Dynamics of interacting particle systems: stochastic process and field
theory | We present an approach to the dynamics of interacting particle systems, which
allows to derive path integral formulas from purely stochastic considerations.
We show that the resulting field theory is a dual version of the standard
theory of Doi and Peliti. This clarify both the origin of the Cole-Hopf map
between the... | cond-mat.stat-mech | we present an approach to the dynamics of interacting particle systems which allows to derive path integral formulas from purely stochastic considerations we show that the resulting field theory is a dual version of the standard theory of doi and peliti this clarify both the origin of the colehopf map between the two a... | [['we', 'present', 'an', 'approach', 'to', 'the', 'dynamics', 'of', 'interacting', 'particle', 'systems', 'which', 'allows', 'to', 'derive', 'path', 'integral', 'formulas', 'from', 'purely', 'stochastic', 'considerations', 'we', 'show', 'that', 'the', 'resulting', 'field', 'theory', 'is', 'a', 'dual', 'version', 'of', ... | [-0.1171400176256667, 0.061087324052522846, -0.1488848183380098, 0.0660617328814104, -0.06978331557570064, -0.07203553550002374, 0.015837387129550382, 0.3048567983573683, -0.2835953261166317, -0.268545600243521, 0.07306037624889263, -0.26476060604092744, -0.22034942202403077, 0.19958695084003883, -0.0361388231078531, 0... |
709.1326 | Weak antilocalization in high mobility Ga(x)In(1-x)As/InP
two-dimensional electron gases with strong spin-orbit coupling | We have studied the spin-orbit interaction in a high mobility two-dimensional
electron gas in a GaInAs/InP heterostructure as a function of an applied gate
voltage as well as a function of temperature. Highly sensitive magnetotransport
measurements of weak antilocalization as well as measurements of Shubnikov--de
Haa... | cond-mat.mes-hall | we have studied the spinorbit interaction in a high mobility twodimensional electron gas in a gainasinp heterostructure as a function of an applied gate voltage as well as a function of temperature highly sensitive magnetotransport measurements of weak antilocalization as well as measurements of shubnikovde haas oscill... | [['we', 'have', 'studied', 'the', 'spinorbit', 'interaction', 'in', 'a', 'high', 'mobility', 'twodimensional', 'electron', 'gas', 'in', 'a', 'gainasinp', 'heterostructure', 'as', 'a', 'function', 'of', 'an', 'applied', 'gate', 'voltage', 'as', 'well', 'as', 'a', 'function', 'of', 'temperature', 'highly', 'sensitive', '... | [-0.1817583429847504, 0.17380212220802987, -0.036106422591849034, 0.015691659609500155, 0.005175369993765962, -0.15077468487814819, 0.07353745247881696, 0.3259014959458801, -0.21521806490824283, -0.36342406041521885, -0.023657190349134587, -0.27476271870985347, -0.11254442828771828, 0.28929197390815653, 0.0006304480686... |
709.1327 | The Steady State Fluctuation Relation for the Dissipation Function | We give a proof of transient fluctuation relations for the entropy production
(dissipation function) in nonequilibrium systems, which is valid for most time
reversible dynamics. We then consider the conditions under which a transient
fluctuation relation yields a steady state fluctuation relation for driven
nonequili... | cond-mat.stat-mech | we give a proof of transient fluctuation relations for the entropy production dissipation function in nonequilibrium systems which is valid for most time reversible dynamics we then consider the conditions under which a transient fluctuation relation yields a steady state fluctuation relation for driven nonequilibrium ... | [['we', 'give', 'a', 'proof', 'of', 'transient', 'fluctuation', 'relations', 'for', 'the', 'entropy', 'production', 'dissipation', 'function', 'in', 'nonequilibrium', 'systems', 'which', 'is', 'valid', 'for', 'most', 'time', 'reversible', 'dynamics', 'we', 'then', 'consider', 'the', 'conditions', 'under', 'which', 'a',... | [-0.15452777678699636, 0.16031634841217762, -0.15061349475831545, 0.10034313301656941, 0.005551850124535085, -0.12020689964228583, 0.04681508028832725, 0.28962159613053307, -0.30179011725851174, -0.23081780398955964, 0.11813846947401856, -0.23960488576987626, -0.10306162447809722, 0.1985495440759508, 0.0031017491739770... |
709.1328 | On the efficiency of field star capture by star clusters | An exciting recent finding regarding scaling relations among globular
clusters is the so-called 'blue tilt': clusters of the blue sub-population
follow a trend of redder colour with increasing luminosity. In this paper we
evaluate to which extent field star capture over a Hubble time may explain the
'blue tilt'. We p... | astro-ph | an exciting recent finding regarding scaling relations among globular clusters is the socalled blue tilt clusters of the blue subpopulation follow a trend of redder colour with increasing luminosity in this paper we evaluate to which extent field star capture over a hubble time may explain the blue tilt we perform coll... | [['an', 'exciting', 'recent', 'finding', 'regarding', 'scaling', 'relations', 'among', 'globular', 'clusters', 'is', 'the', 'socalled', 'blue', 'tilt', 'clusters', 'of', 'the', 'blue', 'subpopulation', 'follow', 'a', 'trend', 'of', 'redder', 'colour', 'with', 'increasing', 'luminosity', 'in', 'this', 'paper', 'we', 'ev... | [-0.11403696009268363, 0.16165067154700713, -0.10101518514911058, 0.08705005544729325, -0.09350332084146362, 0.010337798109416057, 0.06242625402605713, 0.4054932470260947, -0.1849478140671703, -0.3737402287311852, -0.009395447300953997, -0.2639472529016159, -0.04023815224430075, 0.1964070143773117, -0.04216883384096608... |
709.1329 | Auger recombination and carrier multiplication in embedded silicon and
germanium nanocrystals | For Si and Ge nanocrystals (NCs) embedded in wide band-gap matrices, Auger
recombination (AR) and carrier multiplication (CM) lifetimes are computed
exactly in a three-dimensional real space grid using empirical pseudopotential
wave functions. Our results in support of recent experimental data offer new
predictions. ... | cond-mat.mtrl-sci | for si and ge nanocrystals ncs embedded in wide bandgap matrices auger recombination ar and carrier multiplication cm lifetimes are computed exactly in a threedimensional real space grid using empirical pseudopotential wave functions our results in support of recent experimental data offer new predictions we extract si... | [['for', 'si', 'and', 'ge', 'nanocrystals', 'ncs', 'embedded', 'in', 'wide', 'bandgap', 'matrices', 'auger', 'recombination', 'ar', 'and', 'carrier', 'multiplication', 'cm', 'lifetimes', 'are', 'computed', 'exactly', 'in', 'a', 'threedimensional', 'real', 'space', 'grid', 'using', 'empirical', 'pseudopotential', 'wave'... | [-0.05497854981804266, 0.12637277538039296, 0.028874526526002833, 0.06362852564391991, 0.020883914946656052, -0.12951295991272976, 0.06884106375218835, 0.4501131382305175, -0.24307169582073887, -0.3450719324600262, 0.015114727291317347, -0.32686213696324556, -0.07392457230016589, 0.23475578622552953, -0.003756980357381... |
709.133 | Fine-tuning the functional properties of carbon nanotubes via the
interconversion of encapsulated molecules | Tweaking the properties of carbon nanotubes is a prerequisite for their
practical applications. Here we demonstrate fine-tuning the electronic
properties of single-wall carbon nanotubes via filling with ferrocene
molecules. The evolution of the bonding and charge transfer within the tube is
demonstrated via chemical ... | cond-mat.mtrl-sci | tweaking the properties of carbon nanotubes is a prerequisite for their practical applications here we demonstrate finetuning the electronic properties of singlewall carbon nanotubes via filling with ferrocene molecules the evolution of the bonding and charge transfer within the tube is demonstrated via chemical reacti... | [['tweaking', 'the', 'properties', 'of', 'carbon', 'nanotubes', 'is', 'a', 'prerequisite', 'for', 'their', 'practical', 'applications', 'here', 'we', 'demonstrate', 'finetuning', 'the', 'electronic', 'properties', 'of', 'singlewall', 'carbon', 'nanotubes', 'via', 'filling', 'with', 'ferrocene', 'molecules', 'the', 'evo... | [-0.11173037584332457, 0.15170325944200158, 0.00549335752197272, -0.029108652303623687, 0.038657371313816094, -0.10367244030966098, 0.10599389210405075, 0.4595003931233323, -0.255925445699593, -0.2857771580028965, -0.001585496112659394, -0.2584353373666485, -0.13208273274218102, 0.10262876605974083, 0.02682532076106732... |
709.1331 | Mean time exit and isoperimetric inequalities \\for minimal submanifolds
of $N\times \mathbb{R}$ | Based on Markvorsen and Palmer's work on mean time exit and isoperimetric
inequalities we establish slightly better isoperimetric inequalities and mean
time exit estimates for minimal submanifolds of $N\times\mathbb{R}$. We also
prove isoperimetric inequalities for submanifolds of Hadamard spaces with tamed
second fu... | math.DG | based on markvorsen and palmers work on mean time exit and isoperimetric inequalities we establish slightly better isoperimetric inequalities and mean time exit estimates for minimal submanifolds of ntimesmathbbr we also prove isoperimetric inequalities for submanifolds of hadamard spaces with tamed second fundamental ... | [['based', 'on', 'markvorsen', 'and', 'palmers', 'work', 'on', 'mean', 'time', 'exit', 'and', 'isoperimetric', 'inequalities', 'we', 'establish', 'slightly', 'better', 'isoperimetric', 'inequalities', 'and', 'mean', 'time', 'exit', 'estimates', 'for', 'minimal', 'submanifolds', 'of', 'ntimesmathbbr', 'we', 'also', 'pro... | [-0.12221951304046913, 0.04847280623737809, -0.09890762883303471, 0.17567139695030312, -0.071737767695341, -0.2291165593318468, 0.036226001351551955, 0.34136655202222077, -0.24822658061071537, -0.2676198269392169, 0.18404596690954858, -0.2661288636195105, -0.1385433042291985, 0.21555209220495336, -0.19567354335341341, ... |
709.1332 | High-energy scattering and Euclidean-Minkowskian duality | We shall discuss how some relevant analyticity and crossing-symmetry
properties of the "eikonal scattering amplitudes" of two Wilson loops in QCD,
when going from Euclidean to Minkowskian theory, can be related to the still
unsolved problem of the asymptotic s-dependence of the hadron-hadron total
cross-sections. In ... | hep-ph | we shall discuss how some relevant analyticity and crossingsymmetry properties of the eikonal scattering amplitudes of two wilson loops in qcd when going from euclidean to minkowskian theory can be related to the still unsolved problem of the asymptotic sdependence of the hadronhadron total crosssections in particular ... | [['we', 'shall', 'discuss', 'how', 'some', 'relevant', 'analyticity', 'and', 'crossingsymmetry', 'properties', 'of', 'the', 'eikonal', 'scattering', 'amplitudes', 'of', 'two', 'wilson', 'loops', 'in', 'qcd', 'when', 'going', 'from', 'euclidean', 'to', 'minkowskian', 'theory', 'can', 'be', 'related', 'to', 'the', 'still... | [-0.0895030062039575, 0.17498188986191673, -0.14200778163614727, 0.17749145961669643, -0.07426577507858238, -0.06620645370068294, 0.03033307415529317, 0.3618447986682729, -0.29173692169466187, -0.21281953958705777, 0.11255139487218999, -0.287687603295559, -0.1859679210280615, 0.1459671443121301, -0.06018945653664155, 0... |
709.1333 | R&D Status of ATF2 IP Beam Size Monitor (Shintake Monitor) | Shintake monitor is a nanometer-scale electron beam size monitor. It probes a
electron beam by an interference fringe pattern formed by split laser beams.
Minimum measurable beam size by this method is less than 1/10 of laser
wavelength. In ATF2, Shintake monitor will be used for the IP beam size monitor
to measure 3... | physics.acc-ph | shintake monitor is a nanometerscale electron beam size monitor it probes a electron beam by an interference fringe pattern formed by split laser beams minimum measurable beam size by this method is less than 110 of laser wavelength in atf2 shintake monitor will be used for the ip beam size monitor to measure 37 nm des... | [['shintake', 'monitor', 'is', 'a', 'nanometerscale', 'electron', 'beam', 'size', 'monitor', 'it', 'probes', 'a', 'electron', 'beam', 'by', 'an', 'interference', 'fringe', 'pattern', 'formed', 'by', 'split', 'laser', 'beams', 'minimum', 'measurable', 'beam', 'size', 'by', 'this', 'method', 'is', 'less', 'than', '110', ... | [-0.11703714138168968, 0.2548524475399093, -0.061367030768247136, 0.025434717737410344, -0.006241053311426318, -0.21380542453085438, 0.01176851290916459, 0.4687868588462765, -0.2309930466084082, -0.35096445673386034, 0.07124144046729577, -0.2784955782313528, 0.04815719866329867, 0.24413064276810023, -0.0431391858506236... |
709.1334 | Le degre de la variete des courbes de Poncelet | We compute the degree of the projective variety of Poncelet curves of degree
$n$. This variety is irreducible of dimension $2 n + 5$, and lies inside the
projective space of degree $n$ plane curves. It is classically defined as the
closure on this projective space of the locally closed subset of curves passing
throug... | math.AG | we compute the degree of the projective variety of poncelet curves of degree n this variety is irreducible of dimension 2 n 5 and lies inside the projective space of degree n plane curves it is classically defined as the closure on this projective space of the locally closed subset of curves passing through the vertice... | [['we', 'compute', 'the', 'degree', 'of', 'the', 'projective', 'variety', 'of', 'poncelet', 'curves', 'of', 'degree', 'n', 'this', 'variety', 'is', 'irreducible', 'of', 'dimension', '2', 'n', '5', 'and', 'lies', 'inside', 'the', 'projective', 'space', 'of', 'degree', 'n', 'plane', 'curves', 'it', 'is', 'classically', '... | [-0.21855200719928924, 0.058090153410305066, -0.03924112409570968, 0.0508352231261526, -0.09675278663090975, -0.1638942507137968, 0.0023458928607597756, 0.3252977868300173, -0.31398582338149866, -0.2230297103524208, 0.09833131892404023, -0.26823470800171617, -0.13721883545823202, 0.22933913712683074, -0.126194479118850... |
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