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 |
|---|---|---|---|---|---|---|
706.1714 | Theory of nonlinear particle acceleration at shocks and self-generation
of the magnetic field | We present some recent developments in the theory of particle acceleration at
shock fronts in the presence of dynamical reaction of the accelerated particles
and self-generation of magnetic field due to streaming instability. The spectra
of accelerated particles, the velocity, magnetic field and temperature profiles
... | astro-ph | we present some recent developments in the theory of particle acceleration at shock fronts in the presence of dynamical reaction of the accelerated particles and selfgeneration of magnetic field due to streaming instability the spectra of accelerated particles the velocity magnetic field and temperature profiles can be... | [['we', 'present', 'some', 'recent', 'developments', 'in', 'the', 'theory', 'of', 'particle', 'acceleration', 'at', 'shock', 'fronts', 'in', 'the', 'presence', 'of', 'dynamical', 'reaction', 'of', 'the', 'accelerated', 'particles', 'and', 'selfgeneration', 'of', 'magnetic', 'field', 'due', 'to', 'streaming', 'instabili... | [-0.12505757894056538, 0.21795328492179322, -0.07650644953985018, 0.07998709833004679, -0.04043114162647189, -0.005573478021408216, -0.027935006260239065, 0.34681247301304186, -0.28935690630131805, -0.2980408515924445, 0.04040286600894223, -0.2464408676665372, -0.052051221886172123, 0.2133550163050994, 0.04136715763366... |
706.1715 | Search for correlation of UHECRs and BL Lacs in Pierre Auger Observatory
data | Several analyses of the data collected by other experiments have found an
excess of cosmic rays in correlation with subclasses of BL Lacs. Data from the
Pierre Auger Observatory do not support previously reported excesses. The
number of events correlated with BL Lac positions is compatible with that
expected for an i... | astro-ph | several analyses of the data collected by other experiments have found an excess of cosmic rays in correlation with subclasses of bl lacs data from the pierre auger observatory do not support previously reported excesses the number of events correlated with bl lac positions is compatible with that expected for an isotr... | [['several', 'analyses', 'of', 'the', 'data', 'collected', 'by', 'other', 'experiments', 'have', 'found', 'an', 'excess', 'of', 'cosmic', 'rays', 'in', 'correlation', 'with', 'subclasses', 'of', 'bl', 'lacs', 'data', 'from', 'the', 'pierre', 'auger', 'observatory', 'do', 'not', 'support', 'previously', 'reported', 'exc... | [-0.05311501136857946, 0.18558995709106554, -0.0031304557473873194, 0.16755977166895666, -0.10220599467953984, -0.07953438950034808, -0.013273213291540742, 0.46204128910629255, -0.14285976330767264, -0.43667721164957535, 0.004401465691186769, -0.4167916664396817, -0.003691068516587311, 0.2618254991270215, -0.0080633615... |
706.1716 | Modeling and analysis using hybrid Petri nets | This paper is devoted to the use of hybrid Petri nets (PNs) for modeling and
control of hybrid dynamic systems (HDS). Modeling, analysis and control of HDS
attract ever more of researchers' attention and several works have been devoted
to these topics. We consider in this paper the extensions of the PN formalism
(ini... | cs.IT math.IT | this paper is devoted to the use of hybrid petri nets pns for modeling and control of hybrid dynamic systems hds modeling analysis and control of hds attract ever more of researchers attention and several works have been devoted to these topics we consider in this paper the extensions of the pn formalism initially conc... | [['this', 'paper', 'is', 'devoted', 'to', 'the', 'use', 'of', 'hybrid', 'petri', 'nets', 'pns', 'for', 'modeling', 'and', 'control', 'of', 'hybrid', 'dynamic', 'systems', 'hds', 'modeling', 'analysis', 'and', 'control', 'of', 'hds', 'attract', 'ever', 'more', 'of', 'researchers', 'attention', 'and', 'several', 'works',... | [-0.1022299480129539, 0.037897490711253604, -0.09527678143800489, 0.05181654689013218, -0.08235074323910406, -0.14222371001228296, 0.00451466756786485, 0.3689343384497904, -0.253246557497919, -0.3011296061083477, 0.09736664679721738, -0.25723571981001175, -0.1429168156630341, 0.18987329454710153, -0.07867895973158617, ... |
706.1717 | Comment on the paper by Rovelli & al. about the compatibility of various
"gauge conditions" | The compatibility "demonstrated" by Rovelli & al. between various "gauge
conditions" both in Classical Electromagnetism and General Relativity can be
better understood if one distinguishes "gauge conditions" of the solution type
and "gauge conditions" of the constraint type.
| physics.class-ph | the compatibility demonstrated by rovelli al between various gauge conditions both in classical electromagnetism and general relativity can be better understood if one distinguishes gauge conditions of the solution type and gauge conditions of the constraint type | [['the', 'compatibility', 'demonstrated', 'by', 'rovelli', 'al', 'between', 'various', 'gauge', 'conditions', 'both', 'in', 'classical', 'electromagnetism', 'and', 'general', 'relativity', 'can', 'be', 'better', 'understood', 'if', 'one', 'distinguishes', 'gauge', 'conditions', 'of', 'the', 'solution', 'type', 'and', '... | [-0.12781696019039765, 0.12334535295470946, -0.08702668648313831, 0.146268134584298, -0.1442385228111635, -0.2192987105431589, -0.03802115190774202, 0.3073559216399853, -0.2406341019464103, -0.35816584844645616, 0.06793560792465468, -0.14876417110900622, -0.17942324200192014, 0.15429522775308657, -0.11639029527636799, ... |
706.1718 | The Strehl Ratio in Adaptive Optics Images: Statistics and Estimation | Statistical properties of the intensity in adaptive optics images are usually
modeled with a Rician distribution. We study the central point of the image,
where this model is inappropriate for high to very high correction levels. The
central point is an important problem because it gives the Strehl ratio
distribution... | astro-ph | statistical properties of the intensity in adaptive optics images are usually modeled with a rician distribution we study the central point of the image where this model is inappropriate for high to very high correction levels the central point is an important problem because it gives the strehl ratio distribution we s... | [['statistical', 'properties', 'of', 'the', 'intensity', 'in', 'adaptive', 'optics', 'images', 'are', 'usually', 'modeled', 'with', 'a', 'rician', 'distribution', 'we', 'study', 'the', 'central', 'point', 'of', 'the', 'image', 'where', 'this', 'model', 'is', 'inappropriate', 'for', 'high', 'to', 'very', 'high', 'correc... | [-0.10032829045622538, 0.04348276772809466, -0.1596882232106649, 0.11488787465406439, 0.021370523859961674, -0.13368111059356194, -0.007296156131017667, 0.41080547926517635, -0.29104546689643307, -0.30594582847104623, 0.09399357514563375, -0.2565084416132707, -0.11129747393469398, 0.14767811968564415, -0.12772182366595... |
706.1719 | Systematic study of atmosphere-induced influences and uncertainties on
shower reconstruction at the Pierre Auger Observatory | A wide range of atmospheric monitoring instruments is employed at the Pierre
Auger Observatory: two laser facilities, elastic lidar stations, aerosol phase
function monitors, a horizontal attenuation monitor, star monitors, weather
stations, and balloon soundings. We describe the impact of analyzed atmospheric
data o... | astro-ph | a wide range of atmospheric monitoring instruments is employed at the pierre auger observatory two laser facilities elastic lidar stations aerosol phase function monitors a horizontal attenuation monitor star monitors weather stations and balloon soundings we describe the impact of analyzed atmospheric data on the accu... | [['a', 'wide', 'range', 'of', 'atmospheric', 'monitoring', 'instruments', 'is', 'employed', 'at', 'the', 'pierre', 'auger', 'observatory', 'two', 'laser', 'facilities', 'elastic', 'lidar', 'stations', 'aerosol', 'phase', 'function', 'monitors', 'a', 'horizontal', 'attenuation', 'monitor', 'star', 'monitors', 'weather',... | [-0.09504764305208535, 0.1902814902383469, -0.07967327184993409, 0.10781650100497976, -0.003930910351211387, -0.012979856363552459, 0.005139551451886255, 0.4240405290734534, -0.18894106197152652, -0.4123383842627792, 0.08716993155437247, -0.3594758939637127, -0.05339939427543797, 0.22294688668996826, -0.035740898355987... |
706.172 | Correction of paper published in J. Combinatorial Theory 21, 1976: On
the Existence of Hadamard Matrices | In the paper On the Existence of Hadamard Matrices in J. Combinatorial Theory
21, 1976, it is shown that for a natural number q > 3, we can construct an
Hadamard Matrix of order 2^s q for s \geq t where t = [2 log_2(q-3)]. I will
show that this bound is not a consequence of the proof given in the paper and
explain th... | math.CO | in the paper on the existence of hadamard matrices in j combinatorial theory 21 1976 it is shown that for a natural number q 3 we can construct an hadamard matrix of order 2s q for s geq t where t 2 log_2q3 i will show that this bound is not a consequence of the proof given in the paper and explain the error in the arg... | [['in', 'the', 'paper', 'on', 'the', 'existence', 'of', 'hadamard', 'matrices', 'in', 'j', 'combinatorial', 'theory', '21', '1976', 'it', 'is', 'shown', 'that', 'for', 'a', 'natural', 'number', 'q', '3', 'we', 'can', 'construct', 'an', 'hadamard', 'matrix', 'of', 'order', '2s', 'q', 'for', 's', 'geq', 't', 'where', 't'... | [-0.13747520605631341, 0.1327602075376269, -0.045128120476323544, 0.042273390200341855, -0.013670399467545476, -0.1247871022699683, 0.03106337812002466, 0.30972914022365305, -0.2548904154788364, -0.29434177765594516, 0.09704696883052362, -0.251092697747729, -0.19444136392099387, 0.14631258266639302, -0.1080729172028827... |
706.1721 | Geometric Origin of Physical Constants in a Kaluza-Klein Tetrad Model | An important feature of Kaluza-Klein theories is their ability to relate
fundamental physical constants to the radii of higher dimensions. In previous
Kaluza-Klein theory, which unifies the electromagnetic field with gravity as
dimensionless components of a Kaluza-Klein metric, i) all fields have the same
physical di... | gr-qc astro-ph math-ph math.MP | an important feature of kaluzaklein theories is their ability to relate fundamental physical constants to the radii of higher dimensions in previous kaluzaklein theory which unifies the electromagnetic field with gravity as dimensionless components of a kaluzaklein metric i all fields have the same physical dimensions ... | [['an', 'important', 'feature', 'of', 'kaluzaklein', 'theories', 'is', 'their', 'ability', 'to', 'relate', 'fundamental', 'physical', 'constants', 'to', 'the', 'radii', 'of', 'higher', 'dimensions', 'in', 'previous', 'kaluzaklein', 'theory', 'which', 'unifies', 'the', 'electromagnetic', 'field', 'with', 'gravity', 'as'... | [-0.12098154925342117, 0.15611309694749903, -0.03840809070106064, 0.10152995245996863, -0.12630672583755637, -0.1863443773585771, -0.045740057722266234, 0.29080730452069214, -0.17981606300388064, -0.2978887919363167, 0.03366338247433305, -0.2012314404054944, -0.13619456001025226, 0.12792564779719603, -0.060605055503547... |
706.1722 | A kinetic approach to non resonant modes and growth rates of streaming
instability: consequences for shock acceleration | We show here that a purely kinetic approach to the excitation of waves by
cosmic rays in the vicinity of a shock front leads to predict the appearance of
a non-alfvenic fastly growing mode which is the same that was found by Bell
(2004) by treating the plasma in the MHD approximation. The kinetic approach we
present ... | astro-ph | we show here that a purely kinetic approach to the excitation of waves by cosmic rays in the vicinity of a shock front leads to predict the appearance of a nonalfvenic fastly growing mode which is the same that was found by bell 2004 by treating the plasma in the mhd approximation the kinetic approach we present is mor... | [['we', 'show', 'here', 'that', 'a', 'purely', 'kinetic', 'approach', 'to', 'the', 'excitation', 'of', 'waves', 'by', 'cosmic', 'rays', 'in', 'the', 'vicinity', 'of', 'a', 'shock', 'front', 'leads', 'to', 'predict', 'the', 'appearance', 'of', 'a', 'nonalfvenic', 'fastly', 'growing', 'mode', 'which', 'is', 'the', 'same'... | [-0.10929569851737697, 0.16078759194919612, -0.09476070201260815, 0.09258069501474227, -0.05811869593836912, -0.042760655017024495, -0.013307750220808042, 0.33025687359658173, -0.24474998336615789, -0.3025209956870573, 8.200437807273574e-05, -0.2500521774865508, -0.1013273316571807, 0.19525795579865213, 0.0175088854370... |
706.1723 | Ehrlich-Schwoebel Effect for Organic Molecules: Direct Calculation of
the Step Edge Barrier using Empirical Potentials | The step edge barrier of a prototypical organic semiconductor molecule,
3,4,9,10-perylene-tetracaboxylic-dianhydride (PTCDA) has been analysed by means
of calculations based on emperical potentials. The minimum energy path (MEP)
has been calculated for a single molecule on a substrate of three molecular
layers betwee... | cond-mat.other | the step edge barrier of a prototypical organic semiconductor molecule 34910perylenetetracaboxylicdianhydride ptcda has been analysed by means of calculations based on emperical potentials the minimum energy path mep has been calculated for a single molecule on a substrate of three molecular layers between equivalent m... | [['the', 'step', 'edge', 'barrier', 'of', 'a', 'prototypical', 'organic', 'semiconductor', 'molecule', '34910perylenetetracaboxylicdianhydride', 'ptcda', 'has', 'been', 'analysed', 'by', 'means', 'of', 'calculations', 'based', 'on', 'emperical', 'potentials', 'the', 'minimum', 'energy', 'path', 'mep', 'has', 'been', 'c... | [-0.13999266892794063, 0.10986807470908388, -0.03516334401501808, 0.037794610541216876, 0.03725185797945111, -0.17667897263891064, 0.1374642506610447, 0.4485356404281144, -0.24415034331226101, -0.3347038930951385, -0.040287064776445426, -0.3046961690415628, -0.05591833336317601, 0.1337285441380421, 0.06962279133100917,... |
706.1724 | Star formation in Perseus: III. Outflows | We present a search for outflows towards 51 submillimetre cores in Perseus.
With consistently derived outflow properties from a large homogeneous dataset
within one molecular cloud we can investigate further the mass dependence and
time evolution of protostellar mass loss. Of the 51 cores, 37 show broad
linewings ind... | astro-ph | we present a search for outflows towards 51 submillimetre cores in perseus with consistently derived outflow properties from a large homogeneous dataset within one molecular cloud we can investigate further the mass dependence and time evolution of protostellar mass loss of the 51 cores 37 show broad linewings indicati... | [['we', 'present', 'a', 'search', 'for', 'outflows', 'towards', '51', 'submillimetre', 'cores', 'in', 'perseus', 'with', 'consistently', 'derived', 'outflow', 'properties', 'from', 'a', 'large', 'homogeneous', 'dataset', 'within', 'one', 'molecular', 'cloud', 'we', 'can', 'investigate', 'further', 'the', 'mass', 'depen... | [-0.07263076081227987, 0.10998472501358665, -0.00898700707479783, 0.07131267887092664, -0.06891006995108084, -0.07119258799580262, 0.050503744655833675, 0.4462948998119286, -0.1612843435244463, -0.3799271395789948, 0.07421095884803035, -0.28258050213805697, -0.005919134141530525, 0.18796785906905059, -0.028891934091593... |
706.1725 | The two possible values of the chromatic number of a random graph | Given d \in (0,infty) let k_d be the smallest integer k such that d < 2k\log
k. We prove that the chromatic number of a random graph G(n,d/n) is either k_d
or k_d+1 almost surely.
| math.PR | given d in 0infty let k_d be the smallest integer k such that d 2klog k we prove that the chromatic number of a random graph gndn is either k_d or k_d1 almost surely | [['given', 'd', 'in', '0infty', 'let', 'k_d', 'be', 'the', 'smallest', 'integer', 'k', 'such', 'that', 'd', '2klog', 'k', 'we', 'prove', 'that', 'the', 'chromatic', 'number', 'of', 'a', 'random', 'graph', 'gndn', 'is', 'either', 'k_d', 'or', 'k_d1', 'almost', 'surely']] | [-0.28648466690245905, 0.2371305116932049, -0.053027948195284065, -0.0553575022759932, -0.0836955202235417, -0.23341277062497806, 0.030057712599183575, 0.3613406955970056, -0.3091295533107989, -0.22796167701369885, 0.07642876222433354, -0.34884748743339017, -0.14800592727084277, 0.06780587038674364, -0.0470957776503355... |
706.1726 | High Precision determination of the pi, K, D and D_s decay constants
from lattice QCD | We determine $D$ and $D_s$ decay constants from lattice QCD with 2% errors, 4
times better than experiment and previous theory: $f_{D_s}$ = 241(3) MeV, $f_D$
= 207(4) MeV and $f_{D_s}/f_D$ = 1.164(11).
We also obtain $f_K/f_{\pi}$ = 1.189(7) and $(f_{D_s}/f_D)/(f_K/f_{\pi})$ =
0.979(11). Combining with experiment g... | hep-lat hep-ph | we determine d and d_s decay constants from lattice qcd with 2 errors 4 times better than experiment and previous theory f_d_s 2413 mev f_d 2074 mev and f_d_sf_d 116411 we also obtain f_kf_pi 11897 and f_d_sf_df_kf_pi 097911 combining with experiment gives v_us0226214 and v_csv_cd of 44341 we use a highly improved quar... | [['we', 'determine', 'd', 'and', 'd_s', 'decay', 'constants', 'from', 'lattice', 'qcd', 'with', '2', 'errors', '4', 'times', 'better', 'than', 'experiment', 'and', 'previous', 'theory', 'f_d_s', '2413', 'mev', 'f_d', '2074', 'mev', 'and', 'f_d_sf_d', '116411', 'we', 'also', 'obtain', 'f_kf_pi', '11897', 'and', 'f_d_sf_... | [-0.035116832374352154, 0.289891716168748, -0.06732788288196467, 0.09991065182333367, -0.012163594219600782, -0.15110492977597142, 0.17420544667275745, 0.3646989445121068, -0.10396892312691426, -0.28833254062287184, -0.004502496436622966, -0.32863056534441293, 0.041442359233295305, 0.1478381075000431, 0.084820877747994... |
706.1727 | Comment on "Elementary Kaluza-Klein towers revisited" | Recently the spectrum of KK modes in the framework of one flat
extra-dimensional scenario was revisited in the paper Phys. Rev. D74 (2006)
124013, (hep-th/0607246) on the basis of self-adjoint extension of the quantum
mechanical operator determining the KK masses. In this Letter we note that the
range of allowed boun... | hep-th gr-qc | recently the spectrum of kk modes in the framework of one flat extradimensional scenario was revisited in the paper phys rev d74 2006 124013 hepth0607246 on the basis of selfadjoint extension of the quantum mechanical operator determining the kk masses in this letter we note that the range of allowed boundary condition... | [['recently', 'the', 'spectrum', 'of', 'kk', 'modes', 'in', 'the', 'framework', 'of', 'one', 'flat', 'extradimensional', 'scenario', 'was', 'revisited', 'in', 'the', 'paper', 'phys', 'rev', 'd74', '2006', '124013', 'hepth0607246', 'on', 'the', 'basis', 'of', 'selfadjoint', 'extension', 'of', 'the', 'quantum', 'mechanic... | [-0.1394616852586086, 0.17889753565765343, -0.04671266881319193, -0.007566969684110238, -0.07936364010048028, -0.08807625581438724, 0.059681294872783695, 0.27753469633081784, -0.16235336444448106, -0.2841931817963576, 0.013973974081902549, -0.23231811509825862, -0.11622805959330156, 0.17828808177549105, -0.087402259110... |
706.1728 | Lambda Mu Calculus and Duality: Call-by-Name and Call-by-Value | Under the extension of Curry-Howard's correspondence to classical logic,
Gentzen's NK and LK systems can be seen as syntax-directed systems of simple
types respectively for Parigot's Lambda Mu Calculus and Curien-Herbelin's
Lambda Bar Mu Mu Tidle Calculus. We aim at showing their computational
equivalence. We define ... | math.LO | under the extension of curryhowards correspondence to classical logic gentzens nk and lk systems can be seen as syntaxdirected systems of simple types respectively for parigots lambda mu calculus and curienherbelins lambda bar mu mu tidle calculus we aim at showing their computational equivalence we define translations... | [['under', 'the', 'extension', 'of', 'curryhowards', 'correspondence', 'to', 'classical', 'logic', 'gentzens', 'nk', 'and', 'lk', 'systems', 'can', 'be', 'seen', 'as', 'syntaxdirected', 'systems', 'of', 'simple', 'types', 'respectively', 'for', 'parigots', 'lambda', 'mu', 'calculus', 'and', 'curienherbelins', 'lambda',... | [-0.11088116731843911, 0.018388034101235462, -0.086668966414436, 0.157541796710575, -0.09422660007840022, -0.19982078518660273, 0.06153510930016637, 0.39064106103614904, -0.3445194067899138, -0.27227307538851164, 0.024436168767351774, -0.24255982803879306, -0.09476819592055108, 0.18313437944743782, -0.12808445166956517... |
706.1729 | Mixing angles of quarks and leptons as an outcome of SU(2) horizontal
symmetries | We show that all mixing angles are determined, within experimental
uncertainty, by a product of SU(2) horizontal symmetries intimately linked to
the algebra of weak neutral currents. This concerns: on one hand, the three
quark mixing angles; on the other hand, a neutrino-like pattern in which
theta_{23} is maximal an... | hep-ph | we show that all mixing angles are determined within experimental uncertainty by a product of su2 horizontal symmetries intimately linked to the algebra of weak neutral currents this concerns on one hand the three quark mixing angles on the other hand a neutrinolike pattern in which theta_23 is maximal and tan 2 theta_... | [['we', 'show', 'that', 'all', 'mixing', 'angles', 'are', 'determined', 'within', 'experimental', 'uncertainty', 'by', 'a', 'product', 'of', 'su2', 'horizontal', 'symmetries', 'intimately', 'linked', 'to', 'the', 'algebra', 'of', 'weak', 'neutral', 'currents', 'this', 'concerns', 'on', 'one', 'hand', 'the', 'three', 'q... | [-0.19996175926018467, 0.31643500604656755, 0.05683952269534911, 0.12184542613804981, -0.08023563503057406, -0.22262399206038125, 0.09689840908983462, 0.2748049233829783, -0.2749915083830235, -0.28256202704443406, 0.10232065397600133, -0.29995483316240773, -0.06358473460685703, 0.17705050285064405, 0.022757533845061097... |
706.173 | Global well-posedness for dissipative Korteweg-de Vries equations | This paper is devoted to the well-posedness for dissipative KdV equations
$u_t+u_{xxx}+|D_x|^{2\alpha}u+uu_x=0$, $0<\alpha\leq 1$. An optimal bilinear
estimate is obtained in Bourgain's type spaces, which provides global
well-posedness in $H^s(\R)$, $s>-3/4$ for $\alpha\leq1/2$ and
$s>-3/(5-2\alpha)$ for $\alpha>1/2$... | math.AP | this paper is devoted to the wellposedness for dissipative kdv equations u_tu_xxxd_x2alphauuu_x0 0alphaleq 1 an optimal bilinear estimate is obtained in bourgains type spaces which provides global wellposedness in hsr s34 for alphaleq12 and s352alpha for alpha12 | [['this', 'paper', 'is', 'devoted', 'to', 'the', 'wellposedness', 'for', 'dissipative', 'kdv', 'equations', 'u_tu_xxxd_x2alphauuu_x0', '0alphaleq', '1', 'an', 'optimal', 'bilinear', 'estimate', 'is', 'obtained', 'in', 'bourgains', 'type', 'spaces', 'which', 'provides', 'global', 'wellposedness', 'in', 'hsr', 's34', 'fo... | [-0.14899767546781473, 0.006583398065413348, -0.04040729983576707, 0.15247263935328062, -0.07327699911381517, -0.16515858859888144, -0.08533465989665794, 0.22491042624626842, -0.29057341494730543, -0.12205503920891456, 0.21561004266009798, -0.26518515827400346, -0.12610263837268576, 0.21312787202852113, -0.138586318107... |
706.1731 | The VLT-FLAMES survey of massive stars: Evolution of surface N
abundances and effective temperature scales in the Galaxy and Magellanic
Clouds | We present an analysis of high resolution VLT-FLAMES spectra of 61 B-type
stars with relatively narrow-lined spectra located in 4 fields centered on the
Milky Way clusters; NGC3293 & NGC4755 and the Large and Small Magellanic cloud
clusters; NGC2004 and NGC330. For each object a quantitative analysis was
carried out ... | astro-ph | we present an analysis of high resolution vltflames spectra of 61 btype stars with relatively narrowlined spectra located in 4 fields centered on the milky way clusters ngc3293 ngc4755 and the large and small magellanic cloud clusters ngc2004 and ngc330 for each object a quantitative analysis was carried out using the ... | [['we', 'present', 'an', 'analysis', 'of', 'high', 'resolution', 'vltflames', 'spectra', 'of', '61', 'btype', 'stars', 'with', 'relatively', 'narrowlined', 'spectra', 'located', 'in', '4', 'fields', 'centered', 'on', 'the', 'milky', 'way', 'clusters', 'ngc3293', 'ngc4755', 'and', 'the', 'large', 'and', 'small', 'magell... | [-0.03327870252333381, 0.13123103212306772, -0.049097990138965736, 0.09529136554672145, -0.07058273175012972, -0.05547928548889911, 0.07720733045301746, 0.43446377539514425, -0.09857611969267874, -0.38134123339848136, -0.008684760089566923, -0.3121880217676673, 0.012324808523551698, 0.2068617052624144, -0.0462861089453... |
706.1732 | GeV Seesaw, Accidentally Small Neutrino Masses, and Higgs Decays to
Neutrinos | If the Standard Model particle content is extended by gauge singlet fermions
(right-handed neutrinos), active neutrinos generically acquire (Majorana)
masses, in agreement with our current understanding of the lepton sector. If
the right-handed neutrino masses are of the same order as the electroweak
symmetry breakin... | hep-ph | if the standard model particle content is extended by gauge singlet fermions righthanded neutrinos active neutrinos generically acquire majorana masses in agreement with our current understanding of the lepton sector if the righthanded neutrino masses are of the same order as the electroweak symmetry breaking scale it ... | [['if', 'the', 'standard', 'model', 'particle', 'content', 'is', 'extended', 'by', 'gauge', 'singlet', 'fermions', 'righthanded', 'neutrinos', 'active', 'neutrinos', 'generically', 'acquire', 'majorana', 'masses', 'in', 'agreement', 'with', 'our', 'current', 'understanding', 'of', 'the', 'lepton', 'sector', 'if', 'the'... | [-0.07783009141707926, 0.4289275963619135, 0.0034746894692040346, 0.23048789068992598, -0.11502316419424768, -0.19808040709794786, 0.01798406869760453, 0.3299165910560321, -0.20321853636319634, -0.2838827081365523, 0.017861432678163588, -0.2945436944460703, 0.0077500264632083425, 0.11710311693681125, 0.0635442838675397... |
706.1733 | Magnetic fingerprint in a ferromagnetic wire: Spin torque diode effect
and induction of the DC voltage spectrum inherent in the wire under
application for RF current | We report the rectifying effect of a constant-wave radio frequency (RF)
current by a magnetic domain wall (DW) on a single-layered ferromagnetic wire.
A direct-current (DC) voltage is generated by the spin torque diode effect,
which is a consequence of magnetoresistance oscillation due to the resonant
spin wave excit... | cond-mat.mtrl-sci cond-mat.mes-hall | we report the rectifying effect of a constantwave radio frequency rf current by a magnetic domain wall dw on a singlelayered ferromagnetic wire a directcurrent dc voltage is generated by the spin torque diode effect which is a consequence of magnetoresistance oscillation due to the resonant spin wave excitation induced... | [['we', 'report', 'the', 'rectifying', 'effect', 'of', 'a', 'constantwave', 'radio', 'frequency', 'rf', 'current', 'by', 'a', 'magnetic', 'domain', 'wall', 'dw', 'on', 'a', 'singlelayered', 'ferromagnetic', 'wire', 'a', 'directcurrent', 'dc', 'voltage', 'is', 'generated', 'by', 'the', 'spin', 'torque', 'diode', 'effect... | [-0.27243909439662606, 0.20224379585124552, 0.020543210696792456, -0.07530688045535056, -0.1319464356752067, -0.11090859987136976, 0.0720098775572984, 0.40803337846769067, -0.26933011467136986, -0.2637320978158131, 0.008067598012730298, -0.21944919614711914, -0.08437822033401306, 0.2618828785219571, 0.0663328117509259,... |
706.1734 | The new very small angle neutron scattering spectrometer at Laboratoire
Leon Brillouin | The design and characteristics of the new very small angle neutron scattering
spectrometer under construction at the Laboratoire Leon Brillouin is described.
Its goal is to extend the range of scattering vectors magnitudes towards
2x10{-4} /A. The unique feature of this new spectrometer is a high resolution
two dimen... | cond-mat.soft physics.ins-det | the design and characteristics of the new very small angle neutron scattering spectrometer under construction at the laboratoire leon brillouin is described its goal is to extend the range of scattering vectors magnitudes towards 2x104 a the unique feature of this new spectrometer is a high resolution two dimensional i... | [['the', 'design', 'and', 'characteristics', 'of', 'the', 'new', 'very', 'small', 'angle', 'neutron', 'scattering', 'spectrometer', 'under', 'construction', 'at', 'the', 'laboratoire', 'leon', 'brillouin', 'is', 'described', 'its', 'goal', 'is', 'to', 'extend', 'the', 'range', 'of', 'scattering', 'vectors', 'magnitudes... | [-0.13142302729239738, 0.1383972213024626, -0.10488213662284653, -0.014327031086714988, -0.12643025607827144, -0.1550931001870226, 0.012812513030587218, 0.3992169681131034, -0.23132249793490847, -0.2927631296821543, 0.06720155221174119, -0.2776436029077583, -0.03606590898581655, 0.21369605334286854, -0.0788985922219236... |
706.1735 | Self Replication and Signalling | It is known that if one could clone an arbitrary quantum state one could send
signal faster than the speed of light. However it remains interesting to see
that if one can perfectly self replicate an arbitrary quantum state, does it
violate the no signalling principle? Here we see that perfect self replication
would a... | quant-ph | it is known that if one could clone an arbitrary quantum state one could send signal faster than the speed of light however it remains interesting to see that if one can perfectly self replicate an arbitrary quantum state does it violate the no signalling principle here we see that perfect self replication would also l... | [['it', 'is', 'known', 'that', 'if', 'one', 'could', 'clone', 'an', 'arbitrary', 'quantum', 'state', 'one', 'could', 'send', 'signal', 'faster', 'than', 'the', 'speed', 'of', 'light', 'however', 'it', 'remains', 'interesting', 'to', 'see', 'that', 'if', 'one', 'can', 'perfectly', 'self', 'replicate', 'an', 'arbitrary',... | [-0.13486476300157985, 0.21169457551914708, -0.12193025354990515, 0.08963407062672836, -0.15519236221956878, -0.3102050405627085, 0.03210624697841645, 0.3665058592618522, -0.2761739655003204, -0.2487475974327427, 0.07874006395212423, -0.25167627133807896, -0.15884483669158386, 0.21608531563463856, -0.09449023065962277,... |
706.1736 | Gilbert and Landau-Lifshitz damping in the presense of spin-torque | A recent article by Stiles et al. (cond-mat/0702020) argued in favor of the
Landau-Lifshitz damping term in the micromagnetic equations of motion over that
of the more commonly accepted Gilbert damping form. Much of their argument
revolved around spin-torque driven domain wall motion in narrow magnetic wires,
since t... | cond-mat.other | a recent article by stiles et al condmat0702020 argued in favor of the landaulifshitz damping term in the micromagnetic equations of motion over that of the more commonly accepted gilbert damping form much of their argument revolved around spintorque driven domain wall motion in narrow magnetic wires since the presence... | [['a', 'recent', 'article', 'by', 'stiles', 'et', 'al', 'condmat0702020', 'argued', 'in', 'favor', 'of', 'the', 'landaulifshitz', 'damping', 'term', 'in', 'the', 'micromagnetic', 'equations', 'of', 'motion', 'over', 'that', 'of', 'the', 'more', 'commonly', 'accepted', 'gilbert', 'damping', 'form', 'much', 'of', 'their'... | [-0.1791961819054214, 0.10870512333618805, -0.08307516832985444, 0.011076848049947048, -0.16497545263925453, -0.09681412697206308, 0.025222590561082333, 0.3245442315338202, -0.2430719440963901, -0.307196712029385, 0.010643560323651512, -0.2359412072893278, -0.1665531129628006, 0.23573243206605476, -0.05669339507944698,... |
706.1737 | Noise enhancement due to quantum coherence in coupled quantum dots | We show that the intriguing observation of noise enhancement in the charge
transport through two vertically coupled quantum dots can be explained by the
interplay of quantum coherence and strong Coulomb blockade. We demonstrate that
this novel mechanism for super-Poissonian charge transfer is very sensitive to
decohe... | cond-mat.mes-hall | we show that the intriguing observation of noise enhancement in the charge transport through two vertically coupled quantum dots can be explained by the interplay of quantum coherence and strong coulomb blockade we demonstrate that this novel mechanism for superpoissonian charge transfer is very sensitive to decoherenc... | [['we', 'show', 'that', 'the', 'intriguing', 'observation', 'of', 'noise', 'enhancement', 'in', 'the', 'charge', 'transport', 'through', 'two', 'vertically', 'coupled', 'quantum', 'dots', 'can', 'be', 'explained', 'by', 'the', 'interplay', 'of', 'quantum', 'coherence', 'and', 'strong', 'coulomb', 'blockade', 'we', 'dem... | [-0.15549167456378327, 0.2546919903974852, -0.052336843218654394, 0.09846097825030828, 0.02247089921528923, -0.18635716337453703, 0.03801498949479569, 0.37851271702875866, -0.3407237924121577, -0.300095143575414, -0.050239499547952336, -0.29647581783476573, -0.1839931301515678, 0.20673708219466538, -0.00645601736574337... |
706.1738 | Permutations with Extremal number of Fixed Points | We extend Stanley's work on alternating permutations with extremal number of
fixed points in two directions: first, alternating permutations are replaced by
permutations with a prescribed descent set; second, instead of simply counting
permutations we study their generating polynomials by number of excedances.
Severa... | math.CO | we extend stanleys work on alternating permutations with extremal number of fixed points in two directions first alternating permutations are replaced by permutations with a prescribed descent set second instead of simply counting permutations we study their generating polynomials by number of excedances several techni... | [['we', 'extend', 'stanleys', 'work', 'on', 'alternating', 'permutations', 'with', 'extremal', 'number', 'of', 'fixed', 'points', 'in', 'two', 'directions', 'first', 'alternating', 'permutations', 'are', 'replaced', 'by', 'permutations', 'with', 'a', 'prescribed', 'descent', 'set', 'second', 'instead', 'of', 'simply', ... | [-0.16738462330760887, 0.1455278535549705, -0.033117613226578045, 0.0849222633295466, -0.10816250788362546, -0.12547152909148182, 0.06966768711415194, 0.361815690088111, -0.28884891422490616, -0.30587543562256003, 0.09402380086878012, -0.27064334027897063, -0.14883790478563388, 0.22306028125505592, -0.08742393234117755... |
706.1739 | Speckle noise and dynamic range in coronagraphic images | This paper is concerned with the theoretical properties of high contrast
coronagraphic images in the context of exoplanet searches. We derive and
analyze the statistical properties of the residual starlight in coronagraphic
images, and describe the effect of a coronagraph on the speckle and photon
noise. Current obse... | astro-ph | this paper is concerned with the theoretical properties of high contrast coronagraphic images in the context of exoplanet searches we derive and analyze the statistical properties of the residual starlight in coronagraphic images and describe the effect of a coronagraph on the speckle and photon noise current observati... | [['this', 'paper', 'is', 'concerned', 'with', 'the', 'theoretical', 'properties', 'of', 'high', 'contrast', 'coronagraphic', 'images', 'in', 'the', 'context', 'of', 'exoplanet', 'searches', 'we', 'derive', 'and', 'analyze', 'the', 'statistical', 'properties', 'of', 'the', 'residual', 'starlight', 'in', 'coronagraphic',... | [-0.05956595645745199, 0.08531963820271987, -0.10535161874210792, 0.056528123898154245, -0.06957006461072898, -0.0873333284340746, -0.011400718649796455, 0.3946376080155795, -0.25765700224978544, -0.34238786998052967, 0.13867825634054284, -0.24915931878796388, -0.1892479530152541, 0.19634057199648508, -0.17601758406451... |
706.174 | On path factors of (3,4)-biregular bigraphs | A (3,4)-biregular bigraph G is a bipartite graph where all vertices in one
part have degree 3 and all vertices in the other part have degree 4. A path
factor of G is a spanning subgraph whose components are nontrivial paths. We
prove that a simple (3,4)-biregular bigraph always has a path factor such that
the endpoin... | math.CO | a 34biregular bigraph g is a bipartite graph where all vertices in one part have degree 3 and all vertices in the other part have degree 4 a path factor of g is a spanning subgraph whose components are nontrivial paths we prove that a simple 34biregular bigraph always has a path factor such that the endpoints of each p... | [['a', '34biregular', 'bigraph', 'g', 'is', 'a', 'bipartite', 'graph', 'where', 'all', 'vertices', 'in', 'one', 'part', 'have', 'degree', '3', 'and', 'all', 'vertices', 'in', 'the', 'other', 'part', 'have', 'degree', '4', 'a', 'path', 'factor', 'of', 'g', 'is', 'a', 'spanning', 'subgraph', 'whose', 'components', 'are',... | [-0.20356104671955108, 0.13834621701389552, -0.07293938376009464, -0.04548762949494024, -0.10368238911653559, -0.1217817837310334, 0.013575972574763, 0.43831564058860145, -0.2744930982713898, -0.2819360768484573, 0.0917567604004095, -0.30037500788768134, -0.19428100259353717, 0.13108195388379196, -0.02709378521889448, ... |
706.1741 | Breakdown of the Thomas Fermi approximation for polarized Fermi gases | We use Bogoliubov de-Gennes theory to show that the commonly used
Thomas-Fermi approximation (TFA) can fail in describing polarized unitary gases
in anisotropic harmonic traps. We find a magnetized superfluid region inside
the trap, with order parameter oscillations, even though there is no such
stable bulk phase. Th... | cond-mat.supr-con cond-mat.str-el | we use bogoliubov degennes theory to show that the commonly used thomasfermi approximation tfa can fail in describing polarized unitary gases in anisotropic harmonic traps we find a magnetized superfluid region inside the trap with order parameter oscillations even though there is no such stable bulk phase this leads t... | [['we', 'use', 'bogoliubov', 'degennes', 'theory', 'to', 'show', 'that', 'the', 'commonly', 'used', 'thomasfermi', 'approximation', 'tfa', 'can', 'fail', 'in', 'describing', 'polarized', 'unitary', 'gases', 'in', 'anisotropic', 'harmonic', 'traps', 'we', 'find', 'a', 'magnetized', 'superfluid', 'region', 'inside', 'the... | [-0.09166482384316624, 0.21361766517576244, -0.09128033922881716, 0.10664463899382907, -0.021650850317544407, -0.14416431007492875, 0.03614037467891144, 0.3814120787920223, -0.21956224302864738, -0.2865135216464599, -0.007097186060208413, -0.292978306259546, -0.12187789472906539, 0.18464363744068477, 0.0088597777011778... |
706.1742 | Intrinsic nanoscale inhomogeneity in ordering systems due to
elastic-mediated interactions | Phase diagram and pattern formation in two-dimensional Ising model with
coupling between order parameter and lattice vibrations is investigated by
Monte-Carlo simulations. It is shown that if the coupling is strong enough (or
phonons are soft enough) a short-range order exists in disordered phase for a
broader temper... | cond-mat.stat-mech cond-mat.mtrl-sci | phase diagram and pattern formation in twodimensional ising model with coupling between order parameter and lattice vibrations is investigated by montecarlo simulations it is shown that if the coupling is strong enough or phonons are soft enough a shortrange order exists in disordered phase for a broader temperature in... | [['phase', 'diagram', 'and', 'pattern', 'formation', 'in', 'twodimensional', 'ising', 'model', 'with', 'coupling', 'between', 'order', 'parameter', 'and', 'lattice', 'vibrations', 'is', 'investigated', 'by', 'montecarlo', 'simulations', 'it', 'is', 'shown', 'that', 'if', 'the', 'coupling', 'is', 'strong', 'enough', 'or... | [-0.17676104296035852, 0.29137065168470144, -0.04114617403617806, 0.04927002066291276, -0.03618804634474641, -0.1573273802483031, 0.05474506032822484, 0.42238697528161784, -0.2478353640657257, -0.28477696634151717, 0.08582024758586405, -0.2935999884608794, -0.11597906544920988, 0.11105943143378351, 0.09165412079627541,... |
706.1743 | Bloch vectors for qudits and geometry of entanglement | We present three different matrix bases that can be used to decompose density
matrices of d--dimensional quantum systems, so-called qudits: the generalized
Gell-Mann matrix basis, the polarization operator basis, and the Weyl operator
basis. Such a decomposition can be identified with a vector --the Bloch vector,
i.e... | quant-ph | we present three different matrix bases that can be used to decompose density matrices of ddimensional quantum systems socalled qudits the generalized gellmann matrix basis the polarization operator basis and the weyl operator basis such a decomposition can be identified with a vector the bloch vector ie a generalizati... | [['we', 'present', 'three', 'different', 'matrix', 'bases', 'that', 'can', 'be', 'used', 'to', 'decompose', 'density', 'matrices', 'of', 'ddimensional', 'quantum', 'systems', 'socalled', 'qudits', 'the', 'generalized', 'gellmann', 'matrix', 'basis', 'the', 'polarization', 'operator', 'basis', 'and', 'the', 'weyl', 'ope... | [-0.13183256109272512, 0.15575095453491752, -0.05719759105437226, 0.07050260417899527, -0.030671419726465556, -0.1592466586872059, 0.009843345803400391, 0.3306662115809398, -0.25659132481771796, -0.1969490311697454, 0.09590472239463399, -0.25288373038946543, -0.16152050460668227, 0.14835827824871933, -0.010807460676433... |
706.1744 | On a complex differential Riccati equation | We consider a nonlinear partial differential equation for complex-valued
functions which is related to the two-dimensional stationary Schrodinger
equation and enjoys many properties similar to those of the ordinary
differential Riccati equation as, e.g., the famous Euler theorems, the Picard
theorem and others. Besid... | math.AP math.CA math.CV | we consider a nonlinear partial differential equation for complexvalued functions which is related to the twodimensional stationary schrodinger equation and enjoys many properties similar to those of the ordinary differential riccati equation as eg the famous euler theorems the picard theorem and others besides these g... | [['we', 'consider', 'a', 'nonlinear', 'partial', 'differential', 'equation', 'for', 'complexvalued', 'functions', 'which', 'is', 'related', 'to', 'the', 'twodimensional', 'stationary', 'schrodinger', 'equation', 'and', 'enjoys', 'many', 'properties', 'similar', 'to', 'those', 'of', 'the', 'ordinary', 'differential', 'r... | [-0.11299012652735281, -0.004134222685131724, -0.10491241720121573, 0.12853222314151935, -0.14433030863566434, -0.158018380519934, -0.07603583230143961, 0.21870370351654642, -0.35705766377641873, -0.21772218106643243, 0.12747887072927208, -0.347560769505114, -0.19578058970407308, 0.25607641531592784, -0.073396294816013... |
706.1745 | Noether Symmetries and Conservations Laws For Non-critical Kohn-Laplace
Equations on Three-Dimensional Heisenberg Group | We show which Lie point symmetries of non-critical semilinear Kohn-Laplace
equations on the Heisenberg group $H^1$ are Noether symmetries and we establish
their respectives conservations laws.
| math.AP | we show which lie point symmetries of noncritical semilinear kohnlaplace equations on the heisenberg group h1 are noether symmetries and we establish their respectives conservations laws | [['we', 'show', 'which', 'lie', 'point', 'symmetries', 'of', 'noncritical', 'semilinear', 'kohnlaplace', 'equations', 'on', 'the', 'heisenberg', 'group', 'h1', 'are', 'noether', 'symmetries', 'and', 'we', 'establish', 'their', 'respectives', 'conservations', 'laws']] | [-0.27076311588287355, 0.11741274036467075, -0.08318075746297836, 0.10892157334834338, -0.1968860120140016, -0.10303151652216912, -0.03230563089251518, 0.2969264788925648, -0.30433150976896284, -0.203522789478302, 0.11469619167037308, -0.35493753403425216, -0.0937876383215189, 0.1312389884144068, -0.025208732783794402,... |
706.1746 | Triplet Josephson effect with magnetic feedback | We study AC Josephson effect in a superconductor-ferromagnet heterostructure
with a variable magnetic configuration. The system supports triplet proximity
correlations whose dynamics is coupled to the magnetic dynamics. This feedback
dramatically modifies the behavior of the junction. The current-phase relation
becom... | cond-mat.supr-con | we study ac josephson effect in a superconductorferromagnet heterostructure with a variable magnetic configuration the system supports triplet proximity correlations whose dynamics is coupled to the magnetic dynamics this feedback dramatically modifies the behavior of the junction the currentphase relation becomes doub... | [['we', 'study', 'ac', 'josephson', 'effect', 'in', 'a', 'superconductorferromagnet', 'heterostructure', 'with', 'a', 'variable', 'magnetic', 'configuration', 'the', 'system', 'supports', 'triplet', 'proximity', 'correlations', 'whose', 'dynamics', 'is', 'coupled', 'to', 'the', 'magnetic', 'dynamics', 'this', 'feedback... | [-0.3200321595274633, 0.20969093706639064, -0.04578826107805775, 0.054983445431946984, -0.08151735634648151, -0.1832976897487477, 0.07531366067480356, 0.37903629328995464, -0.2628847732013392, -0.28243816794166643, -0.00741599942933047, -0.28692355254597424, -0.10469557207468297, 0.1769839446360786, 0.04434604236796018... |
706.1747 | Characterization of coherent impurity effects in solid state qubits | We propose a characterisation of the effects of bistable coherent impurities
in solid state qubits. We introduce an effective impurity description in terms
of a tunable spin-boson environment and solve the dynamics for the qubit
coherences. The dominant rate characterizing the asymptotic time limit is
identified and ... | cond-mat.stat-mech cond-mat.mes-hall | we propose a characterisation of the effects of bistable coherent impurities in solid state qubits we introduce an effective impurity description in terms of a tunable spinboson environment and solve the dynamics for the qubit coherences the dominant rate characterizing the asymptotic time limit is identified and signa... | [['we', 'propose', 'a', 'characterisation', 'of', 'the', 'effects', 'of', 'bistable', 'coherent', 'impurities', 'in', 'solid', 'state', 'qubits', 'we', 'introduce', 'an', 'effective', 'impurity', 'description', 'in', 'terms', 'of', 'a', 'tunable', 'spinboson', 'environment', 'and', 'solve', 'the', 'dynamics', 'for', 't... | [-0.18469402328581103, 0.17835921304664792, -0.06797208514233882, 0.0796576763575824, 0.05039150942745921, -0.20434709867559275, 0.08103189224002326, 0.33154329047961667, -0.22521252595734867, -0.2360142632689956, 0.025705000046979298, -0.27774137418184963, -0.08828368804163554, 0.1916143273958912, -0.00561808734261370... |
706.1748 | Crystal Irradiation Stimulation of Enzyme Reactivity: An Explanation | In 1968, Sorin Comorosan first reported a phenomenon wherein irradiation of
the substrate of an enzyme reaction, in the crystalline state, for a specific
number of seconds could lead to an enhanced aqueous solution reaction rate for
the enzyme(up to 30%). Dependence on crystal irradiation time was found to be
oscilla... | q-bio.SC q-bio.BM | in 1968 sorin comorosan first reported a phenomenon wherein irradiation of the substrate of an enzyme reaction in the crystalline state for a specific number of seconds could lead to an enhanced aqueous solution reaction rate for the enzymeup to 30 dependence on crystal irradiation time was found to be oscillatory with... | [['in', '1968', 'sorin', 'comorosan', 'first', 'reported', 'a', 'phenomenon', 'wherein', 'irradiation', 'of', 'the', 'substrate', 'of', 'an', 'enzyme', 'reaction', 'in', 'the', 'crystalline', 'state', 'for', 'a', 'specific', 'number', 'of', 'seconds', 'could', 'lead', 'to', 'an', 'enhanced', 'aqueous', 'solution', 'rea... | [-0.08200104608192664, 0.1978432979073254, -0.0699722843874195, -0.012592232108170934, -0.015890321592573357, -0.14676436102565596, 0.07111904295474417, 0.37762276775070597, -0.25122137810690565, -0.31042153025124253, 0.05384962901105212, -0.272607333112915, -0.14898149095702634, 0.19276573181645396, -0.043093521551017... |
706.1749 | Studies of clustering in the arrival directions of cosmic rays detected
at the Pierre Auger Observatory above 10 EeV | If clustering of the arrival directions of ultra high energy cosmic rays is
discovered, this would provide important information about their origin,
composition, and the galactic and extragalactic magnetic fields. We present
here the analysis of the autocorrelation function of the data from the Pierre
Auger Observato... | astro-ph | if clustering of the arrival directions of ultra high energy cosmic rays is discovered this would provide important information about their origin composition and the galactic and extragalactic magnetic fields we present here the analysis of the autocorrelation function of the data from the pierre auger observatory as ... | [['if', 'clustering', 'of', 'the', 'arrival', 'directions', 'of', 'ultra', 'high', 'energy', 'cosmic', 'rays', 'is', 'discovered', 'this', 'would', 'provide', 'important', 'information', 'about', 'their', 'origin', 'composition', 'and', 'the', 'galactic', 'and', 'extragalactic', 'magnetic', 'fields', 'we', 'present', '... | [-0.10996591815374036, 0.14988622173963898, -0.1040407733829773, 0.1254606471342993, -0.07094229466241339, 0.03553531159970747, 0.020931283670032153, 0.3836870233433834, -0.255676805217197, -0.3833472757073848, 0.0663606395567025, -0.33545432431434374, -0.1015358031929835, 0.21429108897143084, 0.0849876613761096, 0.019... |
706.175 | On the Linearization of the Painleve' III-VI Equations and Reductions of
the Three-Wave Resonant System | We extend similarity reductions of the coupled (2+1)-dimensional three-wave
resonant interaction system to its Lax pair. Thus we obtain new 3x3 matrix
Fuchs--Garnier pairs for the third and fifth Painleve' equations, together with
the previously known Fuchs--Garnier pair for the fourth and sixth Painleve'
equations. ... | math.CA | we extend similarity reductions of the coupled 21dimensional threewave resonant interaction system to its lax pair thus we obtain new 3x3 matrix fuchsgarnier pairs for the third and fifth painleve equations together with the previously known fuchsgarnier pair for the fourth and sixth painleve equations these fuchsgarni... | [['we', 'extend', 'similarity', 'reductions', 'of', 'the', 'coupled', '21dimensional', 'threewave', 'resonant', 'interaction', 'system', 'to', 'its', 'lax', 'pair', 'thus', 'we', 'obtain', 'new', '3x3', 'matrix', 'fuchsgarnier', 'pairs', 'for', 'the', 'third', 'and', 'fifth', 'painleve', 'equations', 'together', 'with'... | [-0.15862807135850396, 0.01259510608978828, -0.004339639824649242, 0.06863909474676093, -0.10285458438997859, -0.16117238824587468, -0.05283951678046995, 0.29633511833157644, -0.3098138631895593, -0.24937350364371635, 0.04583635920425877, -0.3476155814969887, -0.1595165260161643, 0.17603560646019928, 0.0218826595403585... |
706.1751 | MacWilliams Identity for Codes with the Rank Metric | The MacWilliams identity, which relates the weight distribution of a code to
the weight distribution of its dual code, is useful in determining the weight
distribution of codes. In this paper, we derive the MacWilliams identity for
linear codes with the rank metric, and our identity has a different form than
that by ... | cs.IT math.IT | the macwilliams identity which relates the weight distribution of a code to the weight distribution of its dual code is useful in determining the weight distribution of codes in this paper we derive the macwilliams identity for linear codes with the rank metric and our identity has a different form than that by delsart... | [['the', 'macwilliams', 'identity', 'which', 'relates', 'the', 'weight', 'distribution', 'of', 'a', 'code', 'to', 'the', 'weight', 'distribution', 'of', 'its', 'dual', 'code', 'is', 'useful', 'in', 'determining', 'the', 'weight', 'distribution', 'of', 'codes', 'in', 'this', 'paper', 'we', 'derive', 'the', 'macwilliams'... | [-0.14533718762896866, -0.002477492539616055, -0.10825105166309569, 0.10839373068547392, -0.055595101934509825, -0.23432823092710361, 0.0189142434244852, 0.32755828887807675, -0.3605349909413202, -0.24037763157702355, 0.1196603257944022, -0.2708940644669964, -0.1767863722585411, 0.15325104216876698, -0.0814137038696243... |
706.1752 | Partial Inertial Manifolds for infinite-dimensional dynamical systems:
Example for P.D.E.s with a state-dependent delay | We propose a new notion of Partial Inertial Manifold to study the long-time
asymptotic behavior of dissipative differential equations. As shown on an
example, such manifolds may exist in the cases when the classical Inertial
manifold does not exist (or not known to exist).
| math.DS math.AP | we propose a new notion of partial inertial manifold to study the longtime asymptotic behavior of dissipative differential equations as shown on an example such manifolds may exist in the cases when the classical inertial manifold does not exist or not known to exist | [['we', 'propose', 'a', 'new', 'notion', 'of', 'partial', 'inertial', 'manifold', 'to', 'study', 'the', 'longtime', 'asymptotic', 'behavior', 'of', 'dissipative', 'differential', 'equations', 'as', 'shown', 'on', 'an', 'example', 'such', 'manifolds', 'may', 'exist', 'in', 'the', 'cases', 'when', 'the', 'classical', 'in... | [-0.1884284702060871, 0.09415429112248769, -0.08028091193938797, 0.10077692664609375, -0.10704971879551356, -0.15217307884119113, -0.0689353057267991, 0.3227294249968095, -0.2832981171615591, -0.2506605109453879, 0.11046554760965095, -0.23355970971963622, -0.21379286984764886, 0.2020034296385182, -0.1633737924699248, 0... |
706.1753 | Concentration of the Spectral Measure for Large Random Matrices with
Stable Entries | We derive concentration inequalities for functions of the empirical measure
of large random matrices with infinitely divisible entries and, in particular,
stable ones. We also give concentration results for some other functionals of
these random matrices, such as the largest eigenvalue or the largest singular
value.
| math.PR math.ST stat.TH | we derive concentration inequalities for functions of the empirical measure of large random matrices with infinitely divisible entries and in particular stable ones we also give concentration results for some other functionals of these random matrices such as the largest eigenvalue or the largest singular value | [['we', 'derive', 'concentration', 'inequalities', 'for', 'functions', 'of', 'the', 'empirical', 'measure', 'of', 'large', 'random', 'matrices', 'with', 'infinitely', 'divisible', 'entries', 'and', 'in', 'particular', 'stable', 'ones', 'we', 'also', 'give', 'concentration', 'results', 'for', 'some', 'other', 'functiona... | [-0.09534948869891789, 0.1426493029575795, -0.026213805575895567, 0.0959469132611285, 0.003798069624716173, -0.13077265836055513, 0.01767149077647406, 0.34214009668516077, -0.26250125815504755, -0.24223703755389736, 0.1597982460668351, -0.36823941427080525, -0.16731533394498832, 0.17892937311578705, -0.0381076027659456... |
706.1754 | Protein structure prediction by an iterative search method | We demonstrate a new algorithm for finding protein conformations that
minimize a non-bonded energy function. The new algorithm, called the difference
map, seeks to find an atomic configuration that is simultaneously in two
constraint spaces. The first constraint space is the space of atomic
configurations that have a... | q-bio.BM | we demonstrate a new algorithm for finding protein conformations that minimize a nonbonded energy function the new algorithm called the difference map seeks to find an atomic configuration that is simultaneously in two constraint spaces the first constraint space is the space of atomic configurations that have a valid ... | [['we', 'demonstrate', 'a', 'new', 'algorithm', 'for', 'finding', 'protein', 'conformations', 'that', 'minimize', 'a', 'nonbonded', 'energy', 'function', 'the', 'new', 'algorithm', 'called', 'the', 'difference', 'map', 'seeks', 'to', 'find', 'an', 'atomic', 'configuration', 'that', 'is', 'simultaneously', 'in', 'two', ... | [-0.14427887114203153, 0.12882764659480017, -0.09226639568292097, 0.10233948382151806, -0.013281183414887088, -0.1145959213583196, 0.06025981632496148, 0.39176643888383883, -0.2913766191101304, -0.3215082798988613, 0.028933678406140056, -0.24110650414299659, -0.12214107726536252, 0.1753186580077882, 0.00020599754198509... |
706.1755 | FreeBSD Mandatory Access Control Usage for Implementing Enterprise
Security Policies | FreeBSD was one of the first widely deployed free operating systems to
provide mandatory access control. It supports a number of classic MAC models.
This tutorial paper addresses exploiting this implementation to enforce typical
enterprise security policies of varying complexities.
| cs.CR | freebsd was one of the first widely deployed free operating systems to provide mandatory access control it supports a number of classic mac models this tutorial paper addresses exploiting this implementation to enforce typical enterprise security policies of varying complexities | [['freebsd', 'was', 'one', 'of', 'the', 'first', 'widely', 'deployed', 'free', 'operating', 'systems', 'to', 'provide', 'mandatory', 'access', 'control', 'it', 'supports', 'a', 'number', 'of', 'classic', 'mac', 'models', 'this', 'tutorial', 'paper', 'addresses', 'exploiting', 'this', 'implementation', 'to', 'enforce', ... | [-0.2229989501880482, -0.010464745451463387, -0.04833428274141625, 0.03147693098871969, -0.11717599600087851, -0.2581494222045876, 0.06979382424906362, 0.3531818331219256, -0.2736038547474891, -0.32616748875007034, 0.12384513607248664, -0.15141495438219862, -0.11122557064518332, 0.17926969258114694, -0.1680032523116096... |
706.1756 | IBM-1 description of the fission products $^{108,110,112}$Ru | IBM-1} calculations for the fission products $^{108,110,112}$Ru have been
carried out. The even-even isotopes of Ru can be described as transitional
nuclei situated between the U(5) (spherical vibrator) and SO(6)
($\gamma$-unstable rotor) symmetries of the Interacting Boson Model. At first,
a Hamiltonian with only on... | nucl-th | ibm1 calculations for the fission products 108110112ru have been carried out the eveneven isotopes of ru can be described as transitional nuclei situated between the u5 spherical vibrator and so6 gammaunstable rotor symmetries of the interacting boson model at first a hamiltonian with only one and twobody terms has bee... | [['ibm1', 'calculations', 'for', 'the', 'fission', 'products', '108110112ru', 'have', 'been', 'carried', 'out', 'the', 'eveneven', 'isotopes', 'of', 'ru', 'can', 'be', 'described', 'as', 'transitional', 'nuclei', 'situated', 'between', 'the', 'u5', 'spherical', 'vibrator', 'and', 'so6', 'gammaunstable', 'rotor', 'symme... | [-0.07092780359477426, 0.14144158893905115, -0.07863970251443485, 0.10024937761869902, 0.03538336673130592, -0.15397922911603626, 0.01587066554153959, 0.3911522055199991, -0.15032235671533273, -0.31013770250137895, -0.02188766412922026, -0.30424791344751917, -0.05346224389310616, 0.13237242714385503, 0.0475692593977631... |
706.1757 | Basis set convergence of post-CCSD contributions to molecular
atomization energies | Basis set convergence of correlation effects on molecular atomization
energies beyond the CCSD (coupled cluster with singles and doubles)
approximation has been studied near the one-particle basis set limit.
Quasiperturbative connected triple excitations, (T), converge more rapidly than
$L^{-3}$ (where $L$ is the hig... | physics.chem-ph | basis set convergence of correlation effects on molecular atomization energies beyond the ccsd coupled cluster with singles and doubles approximation has been studied near the oneparticle basis set limit quasiperturbative connected triple excitations t converge more rapidly than l3 where l is the highest angular moment... | [['basis', 'set', 'convergence', 'of', 'correlation', 'effects', 'on', 'molecular', 'atomization', 'energies', 'beyond', 'the', 'ccsd', 'coupled', 'cluster', 'with', 'singles', 'and', 'doubles', 'approximation', 'has', 'been', 'studied', 'near', 'the', 'oneparticle', 'basis', 'set', 'limit', 'quasiperturbative', 'conne... | [-0.14168837327607584, 0.13181171809271694, -0.03249254687039485, 0.055996497445414926, -0.04202544721666464, -0.1728870247978024, 0.0576203336787605, 0.3511409286279665, -0.20675935562900377, -0.27439175083756795, -0.0007935951664220801, -0.3421475689425025, -0.06055991789759245, 0.18168607633236017, 0.013282649151826... |
706.1758 | Statistics of football dynamics | We investigate the dynamics of football matches. Our goal is to characterize
statistically the temporal sequence of ball movements in this collective sport
game, searching for traits of complex behavior. Data were collected over a
variety of matches in South American, European and World championships
throughout 2005 ... | physics.data-an | we investigate the dynamics of football matches our goal is to characterize statistically the temporal sequence of ball movements in this collective sport game searching for traits of complex behavior data were collected over a variety of matches in south american european and world championships throughout 2005 and 20... | [['we', 'investigate', 'the', 'dynamics', 'of', 'football', 'matches', 'our', 'goal', 'is', 'to', 'characterize', 'statistically', 'the', 'temporal', 'sequence', 'of', 'ball', 'movements', 'in', 'this', 'collective', 'sport', 'game', 'searching', 'for', 'traits', 'of', 'complex', 'behavior', 'data', 'were', 'collected'... | [-0.11087081032805145, 0.07049691472202539, -0.15797012191265822, 0.10534223549067974, -0.07947588487295434, -0.07054733757395297, 0.04511611043126322, 0.41283228479325773, -0.23970905521069652, -0.32192626271396874, 0.08215189287438988, -0.3081382203800604, -0.17746526663191617, 0.1931175230978988, -0.1405815746216103... |
706.1759 | A generalized Petviashvili iteration method for scalar and vector
Hamiltonian equations with arbitrary form of nonlinearity | The Petviashvili's iteration method has been known as a rapidly converging
numerical algorithm for obtaining fundamental solitary wave solutions of
stationary scalar nonlinear wave equations with power-law nonlinearity: \
$-Mu+u^p=0$, where $M$ is a positive definite self-adjoint operator and $p={\rm
const}$. In this... | nlin.PS | the petviashvilis iteration method has been known as a rapidly converging numerical algorithm for obtaining fundamental solitary wave solutions of stationary scalar nonlinear wave equations with powerlaw nonlinearity muup0 where m is a positive definite selfadjoint operator and prm const in this paper we propose a syst... | [['the', 'petviashvilis', 'iteration', 'method', 'has', 'been', 'known', 'as', 'a', 'rapidly', 'converging', 'numerical', 'algorithm', 'for', 'obtaining', 'fundamental', 'solitary', 'wave', 'solutions', 'of', 'stationary', 'scalar', 'nonlinear', 'wave', 'equations', 'with', 'powerlaw', 'nonlinearity', 'muup0', 'where',... | [-0.13032633325556384, 0.06944192442815841, -0.08491797453337689, 0.04702065936886001, -0.1305109797778153, -0.223898014286533, -0.03376963072763074, 0.30556064837316915, -0.21343680949336508, -0.26021484883002394, 0.05507048805352164, -0.2756395499994297, -0.20445571796082687, 0.18276088916776112, 0.026773827985247096... |
706.176 | A Unique Determination of the Effective Potential in Terms of
Renormalization Group Functions | The perturbative effective potential V in the massless $\lambda\phi^4$ model
with a global O(N) symmetry is uniquely determined to all orders by the
renormalization group functions alone when the Coleman-Weinberg renormalization
condition $\frac{d^4V}{d\phi^4}|_{\phi = \mu} = \lambda$ is used, where $\mu$
represents ... | hep-ph | the perturbative effective potential v in the massless lambdaphi4 model with a global on symmetry is uniquely determined to all orders by the renormalization group functions alone when the colemanweinberg renormalization condition fracd4vdphi4_phi mu lambda is used where mu represents the renormalization scale systemat... | [['the', 'perturbative', 'effective', 'potential', 'v', 'in', 'the', 'massless', 'lambdaphi4', 'model', 'with', 'a', 'global', 'on', 'symmetry', 'is', 'uniquely', 'determined', 'to', 'all', 'orders', 'by', 'the', 'renormalization', 'group', 'functions', 'alone', 'when', 'the', 'colemanweinberg', 'renormalization', 'con... | [-0.1379773833232219, 0.12368766869195248, -0.11008654122485378, 0.09682619790663662, -0.05530384878560318, -0.11388991654241801, 0.046605098134104433, 0.34482157625018633, -0.23599702019410926, -0.2511895878432974, 0.02633808979793197, -0.2821604093698025, -0.13828866350511348, 0.14794597025913858, 0.03044795804018383... |
706.1761 | Extraspecial Two-Groups, Generalized Yang-Baxter Equations and Braiding
Quantum Gates | In this paper we describe connections among extraspecial 2-groups, unitary
representations of the braid group and multi-qubit braiding quantum gates. We
first construct new representations of extraspecial 2-groups. Extending the
latter by the symmetric group, we construct new unitary braid representations,
which are ... | quant-ph hep-th math-ph math.MP | in this paper we describe connections among extraspecial 2groups unitary representations of the braid group and multiqubit braiding quantum gates we first construct new representations of extraspecial 2groups extending the latter by the symmetric group we construct new unitary braid representations which are solutions ... | [['in', 'this', 'paper', 'we', 'describe', 'connections', 'among', 'extraspecial', '2groups', 'unitary', 'representations', 'of', 'the', 'braid', 'group', 'and', 'multiqubit', 'braiding', 'quantum', 'gates', 'we', 'first', 'construct', 'new', 'representations', 'of', 'extraspecial', '2groups', 'extending', 'the', 'latt... | [-0.1680754842609167, 0.21824322803446558, -0.05972555983066559, 0.048032446119002994, -0.05173553150892258, -0.19625446180254222, 0.04602043844480067, 0.3560651422291994, -0.2878594629317522, -0.26115844513103365, 0.02990046106465161, -0.21532722816243768, -0.1867427062126808, 0.19990859882533552, -0.09072165890038013... |
706.1762 | The Detailed Forms of the LMC Cepheid PL and PLC Relations | Possible deviations from linearity of the LMC Cepheid PL and PLC relations
are investigated. Two datasets are studied, respectively from the OGLE and
MACHO projects. A nonparametric test, based on linear regression residuals,
suggests that neither PL relation is linear. If colour dependence is allowed
for then the MA... | astro-ph | possible deviations from linearity of the lmc cepheid pl and plc relations are investigated two datasets are studied respectively from the ogle and macho projects a nonparametric test based on linear regression residuals suggests that neither pl relation is linear if colour dependence is allowed for then the macho pl r... | [['possible', 'deviations', 'from', 'linearity', 'of', 'the', 'lmc', 'cepheid', 'pl', 'and', 'plc', 'relations', 'are', 'investigated', 'two', 'datasets', 'are', 'studied', 'respectively', 'from', 'the', 'ogle', 'and', 'macho', 'projects', 'a', 'nonparametric', 'test', 'based', 'on', 'linear', 'regression', 'residuals'... | [-0.015095901455096596, 0.07137254935681636, -0.1653114007098875, 0.13467372491761095, -0.13116204981753204, -0.17100529723464833, 0.04703665820148881, 0.43468692437669293, -0.26469415588090656, -0.30631659266951144, 0.042808767937726845, -0.3502125068582961, -0.13794660046849339, 0.278905301446431, -0.078226186736338,... |
706.1763 | A discrete mean value of the derivative of the Riemann zeta function | In this article we compute a discrete mean value of the derivative of the
Riemann zeta function. This mean value will be important for several
applications concerning the size of $\zeta'(\rho)$ where $\zeta(s)$ is the
Riemann zeta function and $\rho$ is a non-trivial zero of the Riemann zeta
function.
| math.NT | in this article we compute a discrete mean value of the derivative of the riemann zeta function this mean value will be important for several applications concerning the size of zetarho where zetas is the riemann zeta function and rho is a nontrivial zero of the riemann zeta function | [['in', 'this', 'article', 'we', 'compute', 'a', 'discrete', 'mean', 'value', 'of', 'the', 'derivative', 'of', 'the', 'riemann', 'zeta', 'function', 'this', 'mean', 'value', 'will', 'be', 'important', 'for', 'several', 'applications', 'concerning', 'the', 'size', 'of', 'zetarho', 'where', 'zetas', 'is', 'the', 'riemann... | [-0.22096802746610983, 0.07398060201762283, -0.17700677130570902, 0.10875674973869202, -0.09282809932126987, -0.05147431834543846, 0.017349687499963507, 0.2676899213419885, -0.2858226901794575, -0.21338450519025934, 0.1231754408669373, -0.24276342395008826, -0.1763146130453643, 0.1918901457850422, -0.023947996144392053... |
706.1764 | Classical potential describes martensitic phase transformations between
the $\alpha$, $\beta$ and $\omega$ titanium phases | A description of the martensitic transformations between the $\alpha$,
$\beta$ and $\omega$ phases of titanium that includes nucleation and growth
requires an accurate classical potential. Optimization of the parameters of a
modified embedded atom potential to a database of density-functional
calculations yields an a... | cond-mat.mtrl-sci | a description of the martensitic transformations between the alpha beta and omega phases of titanium that includes nucleation and growth requires an accurate classical potential optimization of the parameters of a modified embedded atom potential to a database of densityfunctional calculations yields an accurate and tr... | [['a', 'description', 'of', 'the', 'martensitic', 'transformations', 'between', 'the', 'alpha', 'beta', 'and', 'omega', 'phases', 'of', 'titanium', 'that', 'includes', 'nucleation', 'and', 'growth', 'requires', 'an', 'accurate', 'classical', 'potential', 'optimization', 'of', 'the', 'parameters', 'of', 'a', 'modified',... | [-0.13229333023058185, 0.17028052200081462, -0.06723244755433491, 0.010415965738897043, 0.010060125276031175, -0.1315383912002421, 0.12533619402380414, 0.39520338860744364, -0.27378808743466276, -0.3229208528288606, 0.008726000856658646, -0.29837171090430165, -0.11102411544570386, 0.1559103206129666, 0.0899111446251262... |
706.1765 | Extreme values of zeta prime rho | In this article we exhibit small and large values of $\zeta'(\rho)$ by
applying Soundararajan's resonance method. Our results assume the Riemann
hypothesis.
| math.NT | in this article we exhibit small and large values of zetarho by applying soundararajans resonance method our results assume the riemann hypothesis | [['in', 'this', 'article', 'we', 'exhibit', 'small', 'and', 'large', 'values', 'of', 'zetarho', 'by', 'applying', 'soundararajans', 'resonance', 'method', 'our', 'results', 'assume', 'the', 'riemann', 'hypothesis']] | [-0.10839895379136909, 0.08684205380268395, -0.08394616221035407, 0.04364799984878945, -0.03487709774212404, -0.07929228754206137, 0.04166209780272435, 0.2922008437189189, -0.19651224311779847, -0.32494302771308203, 0.07681018251142549, -0.20621251145547087, -0.21813120498237284, 0.22642158272422172, -0.061074468307197... |
706.1766 | Orbital liquid in ferromagnetic manganites: The orbital Hubbard model
for $e_g$ electrons | We have analyzed the symmetry properties and the ground state of an orbital
Hubbard model with two orbital flavors, describing a partly filled
spin-polarized $e_g$ band on a cubic lattice, as in ferromagnetic manganites.
We demonstrate that the off-diagonal hopping responsible for transitions
between $x^2-y^2$ and $3... | cond-mat.str-el | we have analyzed the symmetry properties and the ground state of an orbital hubbard model with two orbital flavors describing a partly filled spinpolarized e_g band on a cubic lattice as in ferromagnetic manganites we demonstrate that the offdiagonal hopping responsible for transitions between x2y2 and 3z2r2 orbitals a... | [['we', 'have', 'analyzed', 'the', 'symmetry', 'properties', 'and', 'the', 'ground', 'state', 'of', 'an', 'orbital', 'hubbard', 'model', 'with', 'two', 'orbital', 'flavors', 'describing', 'a', 'partly', 'filled', 'spinpolarized', 'e_g', 'band', 'on', 'a', 'cubic', 'lattice', 'as', 'in', 'ferromagnetic', 'manganites', '... | [-0.17952664942234098, 0.22800181306935402, -0.04401755090300724, 0.11040299510133599, -0.02422650962584086, -0.14193856458216175, 0.05858724040958537, 0.36808023739642665, -0.22900199509390137, -0.2527538535502447, -0.0006781681435063993, -0.3032289276369756, -0.09440996435125057, 0.0998789260389886, 0.066240136434013... |
706.1767 | VHE astrophysics: recent developments | We review the current status, and some open issues, of VHE astrophysics.
| astro-ph | we review the current status and some open issues of vhe astrophysics | [['we', 'review', 'the', 'current', 'status', 'and', 'some', 'open', 'issues', 'of', 'vhe', 'astrophysics']] | [-0.10030728578567505, 0.15557728979426125, 0.08289100090041757, 0.17277069948613644, -0.23365758080035448, -0.08726388945554693, 0.0675175291641305, 0.37053624882052344, -0.2800061637535691, -0.3497755900025368, 0.19111815626577786, -0.29067369488378364, -0.06079309309522311, 0.2745627942495048, -0.12907481178020438, ... |
706.1768 | The black hole in the throat - thermodynamics of strongly coupled
cascading gauge theories | We numerically construct black hole solutions corresponding to the
deconfined, chirally symmetric phase of strongly coupled cascading gauge
theories at various temperatures. We compute the free energy as a function of
the temperature, and we show that it becomes positive below some critical
temperature, indicating th... | hep-th | we numerically construct black hole solutions corresponding to the deconfined chirally symmetric phase of strongly coupled cascading gauge theories at various temperatures we compute the free energy as a function of the temperature and we show that it becomes positive below some critical temperature indicating the poss... | [['we', 'numerically', 'construct', 'black', 'hole', 'solutions', 'corresponding', 'to', 'the', 'deconfined', 'chirally', 'symmetric', 'phase', 'of', 'strongly', 'coupled', 'cascading', 'gauge', 'theories', 'at', 'various', 'temperatures', 'we', 'compute', 'the', 'free', 'energy', 'as', 'a', 'function', 'of', 'the', 't... | [-0.1480589920196623, 0.26022394519439707, -0.07210608979775793, 0.0648355209490373, -0.010207776416329637, -0.13325163914215943, 0.05052364213089089, 0.33984483537515475, -0.20658919549295826, -0.25725675965585404, 0.07668199741266786, -0.322563019595922, -0.14038623555282514, 0.07652419350213474, 0.07140334831580283,... |
706.1769 | Higher Derivative Corrections, Dimensional Reduction and Ehlers Duality | Motivated by applications to black hole physics and duality, we study the
effect of higher derivative corrections on the dimensional reduction of
four-dimensional Einstein, Einstein Liouville and Einstein-Maxwell gravity to
one direction, as appropriate for stationary, spherically symmetric solutions.
We construct a ... | hep-th | motivated by applications to black hole physics and duality we study the effect of higher derivative corrections on the dimensional reduction of fourdimensional einstein einstein liouville and einsteinmaxwell gravity to one direction as appropriate for stationary spherically symmetric solutions we construct a field red... | [['motivated', 'by', 'applications', 'to', 'black', 'hole', 'physics', 'and', 'duality', 'we', 'study', 'the', 'effect', 'of', 'higher', 'derivative', 'corrections', 'on', 'the', 'dimensional', 'reduction', 'of', 'fourdimensional', 'einstein', 'einstein', 'liouville', 'and', 'einsteinmaxwell', 'gravity', 'to', 'one', '... | [-0.16877311520078334, 0.12507037684506128, -0.06415288380735885, 0.11072471895359057, -0.10144226400043108, -0.16470001031806278, -0.019773576377837127, 0.2812813785704515, -0.15219821543856102, -0.25407876558447917, 0.10221435362569341, -0.278366950209722, -0.16755077895546747, 0.12374201086003425, -0.066485092097754... |
706.177 | Cracking the Supersolid | We prepresent an overview of the status of experiment and theory on the
supersolid state of matter.
| cond-mat.supr-con cond-mat.dis-nn | we prepresent an overview of the status of experiment and theory on the supersolid state of matter | [['we', 'prepresent', 'an', 'overview', 'of', 'the', 'status', 'of', 'experiment', 'and', 'theory', 'on', 'the', 'supersolid', 'state', 'of', 'matter']] | [-0.14578859679750167, 0.17703204815279605, -0.15731901780236512, 0.017644090577960014, -0.03380917105823755, 0.004280076012946665, 0.06224308258242672, 0.30473508092109114, -0.18835075316019356, -0.3120922719826922, 0.10077984453528188, -0.3342951098456979, -0.14237489411607385, 0.14521387149579823, 0.0021761484676972... |
706.1771 | The fundamental progroupoid of a general topos | It is well known that the category of covering projections (that is, locally
constant objects) of a locally connected topos is equivalent to the classifying
topos of a strict progroupoid (or, equivalently, a localic prodiscrete
groupoid), the \emph{fundamental progroupoid}, and that this progroupoid
represents first ... | math.CT math.AT | it is well known that the category of covering projections that is locally constant objects of a locally connected topos is equivalent to the classifying topos of a strict progroupoid or equivalently a localic prodiscrete groupoid the emphfundamental progroupoid and that this progroupoid represents first degree cohomol... | [['it', 'is', 'well', 'known', 'that', 'the', 'category', 'of', 'covering', 'projections', 'that', 'is', 'locally', 'constant', 'objects', 'of', 'a', 'locally', 'connected', 'topos', 'is', 'equivalent', 'to', 'the', 'classifying', 'topos', 'of', 'a', 'strict', 'progroupoid', 'or', 'equivalently', 'a', 'localic', 'prodi... | [-0.12842154745712642, 0.1208668415626174, -0.10899531082217614, 0.0820104838007006, -0.13347555707384656, -0.09978382404359591, 0.0029377952491591026, 0.3522149413641725, -0.3478099593397725, -0.22560858083367868, 0.08710192532727977, -0.20794879039423866, -0.1299973517750761, 0.17794428456906827, -0.2534927013167343,... |
706.1772 | The GRB afterglow onset observed by REM: fireball Lorentz factor and
afterglow fluence | We report observations of the early light curves of GRB 060418 and GRB
060607A, carried out with the pink robotic telescope REM. A clear peak is
detected for both events, which is interpreted as the onset of the afterglow,
that is the time at which the fireball starts decelerating. This detection
allows to directly m... | astro-ph | we report observations of the early light curves of grb 060418 and grb 060607a carried out with the pink robotic telescope rem a clear peak is detected for both events which is interpreted as the onset of the afterglow that is the time at which the fireball starts decelerating this detection allows to directly measure ... | [['we', 'report', 'observations', 'of', 'the', 'early', 'light', 'curves', 'of', 'grb', '060418', 'and', 'grb', '060607a', 'carried', 'out', 'with', 'the', 'pink', 'robotic', 'telescope', 'rem', 'a', 'clear', 'peak', 'is', 'detected', 'for', 'both', 'events', 'which', 'is', 'interpreted', 'as', 'the', 'onset', 'of', 't... | [-0.06678591449873163, 0.17664679273035924, -0.14390894878279725, 0.13220527867141496, -0.11127053365248059, -0.10511838205996046, 0.04134072148061674, 0.4447684098385411, -0.16764365329910197, -0.30113153593665964, 0.05564395873059749, -0.2988456045621857, 0.0029506836377015903, 0.2517839870107902, -0.0048437612942941... |
706.1773 | The Stokes phenomenon in the confluence of the hypergeometric equation
using Riccati equation | In this paper we study the confluence of two regular singular points of the
hypergeometric equation into an irregular one. We study the consequence of the
divergence of solutions at the irregular singular point for the unfolded
system. Our study covers a full neighborhood of the origin in the confluence
parameter spa... | math.CA math.DS | in this paper we study the confluence of two regular singular points of the hypergeometric equation into an irregular one we study the consequence of the divergence of solutions at the irregular singular point for the unfolded system our study covers a full neighborhood of the origin in the confluence parameter space i... | [['in', 'this', 'paper', 'we', 'study', 'the', 'confluence', 'of', 'two', 'regular', 'singular', 'points', 'of', 'the', 'hypergeometric', 'equation', 'into', 'an', 'irregular', 'one', 'we', 'study', 'the', 'consequence', 'of', 'the', 'divergence', 'of', 'solutions', 'at', 'the', 'irregular', 'singular', 'point', 'for',... | [-0.18868811940774322, 0.010692620629561134, -0.09840839028851513, 0.06918601552435362, -0.03903995865188977, -0.0779404563610168, 0.03331603669417638, 0.24661802572800834, -0.3038886631674626, -0.18541120275964632, 0.12737177957862836, -0.3091826677596306, -0.17054091036210164, 0.16158414008643698, -0.0527691204018671... |
706.1774 | Functional Methods in the Generalized Dicke Model | The Dicke model describes an ensemble of N identical two-level atoms (qubits)
coupled to a single mode of a bosonic field. The fermion Dicke model should be
obtained by changing the atomic pseudo-spin operators by a linear combination
of Fermi operators. The generalized fermion Dicke model is defined introducing
diff... | quant-ph | the dicke model describes an ensemble of n identical twolevel atoms qubits coupled to a single mode of a bosonic field the fermion dicke model should be obtained by changing the atomic pseudospin operators by a linear combination of fermi operators the generalized fermion dicke model is defined introducing different co... | [['the', 'dicke', 'model', 'describes', 'an', 'ensemble', 'of', 'n', 'identical', 'twolevel', 'atoms', 'qubits', 'coupled', 'to', 'a', 'single', 'mode', 'of', 'a', 'bosonic', 'field', 'the', 'fermion', 'dicke', 'model', 'should', 'be', 'obtained', 'by', 'changing', 'the', 'atomic', 'pseudospin', 'operators', 'by', 'a',... | [-0.1754109816615521, 0.24978066821947956, -0.04267665150270621, 0.031982937363118004, -0.00868770991095818, -0.18090004649030447, 0.07153922400098242, 0.31074524969120043, -0.23194083214784686, -0.24449755171579973, 0.02119874665331233, -0.29603415349506973, -0.13371761195889506, 0.13814213573782436, 0.047701611157832... |
706.1775 | Galaxy-CMB Cross-Correlation as a Probe of Alternative Models of Gravity | Bekenstein's alternative to general relativity, TeVeS, reduces to Modified
Newtonian Dynamics (MOND) in the galactic limit. On cosmological scales, the
(potential well <-> overdensity) relationship is quite different than in
standard general relativity. Here we investigate the possibility of
cross-correlating galaxie... | astro-ph | bekensteins alternative to general relativity teves reduces to modified newtonian dynamics mond in the galactic limit on cosmological scales the potential well overdensity relationship is quite different than in standard general relativity here we investigate the possibility of crosscorrelating galaxies with the cosmic... | [['bekensteins', 'alternative', 'to', 'general', 'relativity', 'teves', 'reduces', 'to', 'modified', 'newtonian', 'dynamics', 'mond', 'in', 'the', 'galactic', 'limit', 'on', 'cosmological', 'scales', 'the', 'potential', 'well', 'overdensity', 'relationship', 'is', 'quite', 'different', 'than', 'in', 'standard', 'genera... | [-0.09980138421783016, 0.09450515768904653, -0.12629742492507728, 0.20439171693805191, -0.14288396976060339, -0.12200566122515334, -0.051633806811231704, 0.3117709017927862, -0.21077159945335652, -0.3315038525395923, -0.030653814360913304, -0.27367020903362166, -0.1268271476858192, 0.2004538488160405, -0.02352587082940... |
706.1776 | Coherence and phase synchronization: generalization to pairs of
multivariate time series, and removal of zero-lag contributions | Coherence and phase synchronization between time series corresponding to
different spatial locations are usually interpreted as indicators of the
connectivity between locations. In neurophysiology, time series of electric
neuronal activity are essential for studying brain interconnectivity. Such
signals can either be... | stat.ME stat.AP | coherence and phase synchronization between time series corresponding to different spatial locations are usually interpreted as indicators of the connectivity between locations in neurophysiology time series of electric neuronal activity are essential for studying brain interconnectivity such signals can either be inva... | [['coherence', 'and', 'phase', 'synchronization', 'between', 'time', 'series', 'corresponding', 'to', 'different', 'spatial', 'locations', 'are', 'usually', 'interpreted', 'as', 'indicators', 'of', 'the', 'connectivity', 'between', 'locations', 'in', 'neurophysiology', 'time', 'series', 'of', 'electric', 'neuronal', 'a... | [-0.12128875003557929, 0.12925165420840246, -0.045713767089306356, 0.08963758095435084, -0.05436777621111337, -0.1564643868730661, -0.005713425724311395, 0.42468900944086463, -0.28537663848317685, -0.3024544984483695, 0.1320796366790904, -0.24835655069018298, -0.18573447972575718, 0.17532968223689402, -0.07563151556334... |
706.1777 | "Hidden" Seyfert 2 Galaxies in the Chandra Deep Field North | We have compared the X-ray--to--optical flux ratios (F_x/F_opt) of absorbed
active galactic nuclei (AGNs) in the Chandra Deep Field North (CDF-N) with
those of nearby, optically classified Seyfert 2 galaxies. The comparison
provides an opportunity to explore the extent to which the local population of
absorbed AGNs c... | astro-ph | we have compared the xraytooptical flux ratios f_xf_opt of absorbed active galactic nuclei agns in the chandra deep field north cdfn with those of nearby optically classified seyfert 2 galaxies the comparison provides an opportunity to explore the extent to which the local population of absorbed agns can account for th... | [['we', 'have', 'compared', 'the', 'xraytooptical', 'flux', 'ratios', 'f_xf_opt', 'of', 'absorbed', 'active', 'galactic', 'nuclei', 'agns', 'in', 'the', 'chandra', 'deep', 'field', 'north', 'cdfn', 'with', 'those', 'of', 'nearby', 'optically', 'classified', 'seyfert', '2', 'galaxies', 'the', 'comparison', 'provides', '... | [-0.017621883614763554, 0.05818168369045788, -0.06369110429561657, 0.1391185639712748, -0.053732998938174494, -0.07004910054178361, 0.06696822922363752, 0.4964110621979006, -0.11929005828193005, -0.3796485181068297, 0.030407896400879316, -0.36201939744749617, -0.0025853051612263218, 0.1917059908243397, -0.0024747578701... |
706.1778 | KLT relations from the Einstein-Hilbert Lagrangian | The Kawai-Lewellen-Tye (KLT) relations derived from string theory tell us
that perturbative gravity amplitudes are the "square" of the corresponding
amplitudes in gauge theory. Starting from the light-cone Lagrangian for pure
gravity we make these relations manifest off-shell, for three- and
four-graviton vertices, a... | hep-th | the kawailewellentye klt relations derived from string theory tell us that perturbative gravity amplitudes are the square of the corresponding amplitudes in gauge theory starting from the lightcone lagrangian for pure gravity we make these relations manifest offshell for three and fourgraviton vertices at the level of ... | [['the', 'kawailewellentye', 'klt', 'relations', 'derived', 'from', 'string', 'theory', 'tell', 'us', 'that', 'perturbative', 'gravity', 'amplitudes', 'are', 'the', 'square', 'of', 'the', 'corresponding', 'amplitudes', 'in', 'gauge', 'theory', 'starting', 'from', 'the', 'lightcone', 'lagrangian', 'for', 'pure', 'gravit... | [-0.12655513507447072, 0.1962799308322636, -0.16797022750525145, 0.1856536971291109, -0.06939493392461113, -0.12213763263912833, 0.03236100061948658, 0.28539111659082833, -0.1943694029991724, -0.24949735463881978, -0.02035616034385273, -0.3213855082131162, -0.17139167722542675, 0.11039114000313745, 0.002671520615338671... |
706.1779 | Lookback time bounds from energy conditions | In general relativity, the energy conditions are invoked to restrict general
energy-momentum tensors on physical grounds. We show that in the standard
Friedmann-Lemaitre-Robertson-Walker (FLRW) approach to cosmological modeling,
where the energy and matter components of the cosmic fluid are unknown, the
energy condit... | astro-ph gr-qc hep-th | in general relativity the energy conditions are invoked to restrict general energymomentum tensors on physical grounds we show that in the standard friedmannlemaitrerobertsonwalker flrw approach to cosmological modeling where the energy and matter components of the cosmic fluid are unknown the energy conditions provide... | [['in', 'general', 'relativity', 'the', 'energy', 'conditions', 'are', 'invoked', 'to', 'restrict', 'general', 'energymomentum', 'tensors', 'on', 'physical', 'grounds', 'we', 'show', 'that', 'in', 'the', 'standard', 'friedmannlemaitrerobertsonwalker', 'flrw', 'approach', 'to', 'cosmological', 'modeling', 'where', 'the'... | [-0.09274130573848614, 0.13104969751077225, -0.0865609555574436, 0.08027849975710646, -0.06523619920197823, -0.047776330293886164, 0.008388390563227035, 0.36415615377985444, -0.1725801764043501, -0.3538351869839873, 0.07996097585891147, -0.2740138817226162, 0.003479317220783717, 0.21125764364645677, -0.0007918954078057... |
706.178 | Le travail collaboratif dans le cadre d'un projet architectural | The analysis of the practices and the tendencies of the users at the time of
the search for information on Internet makes it possible to highlight several
points. The search for information becomes powerful after knowledge of the
typology of the various systems of research. This typology supports the
adoption of a me... | cs.HC | the analysis of the practices and the tendencies of the users at the time of the search for information on internet makes it possible to highlight several points the search for information becomes powerful after knowledge of the typology of the various systems of research this typology supports the adoption of a method... | [['the', 'analysis', 'of', 'the', 'practices', 'and', 'the', 'tendencies', 'of', 'the', 'users', 'at', 'the', 'time', 'of', 'the', 'search', 'for', 'information', 'on', 'internet', 'makes', 'it', 'possible', 'to', 'highlight', 'several', 'points', 'the', 'search', 'for', 'information', 'becomes', 'powerful', 'after', '... | [-0.12328562836025979, 0.039198615481703336, -0.08718083820214587, 0.073022735231048, -0.09999744131692223, -0.07023099740849925, 0.0868065161435129, 0.31670098962796317, -0.26405537076346525, -0.3341354433629479, 0.12475725632304183, -0.29302526358677844, -0.16572799926690457, 0.19565166118619898, -0.04081465610810979... |
706.1781 | Superfluid and Pseudo-Goldstone Modes in Three Flavor Crystalline Color
Superconductivity | We study the bosonic excitations in the favorite cubic three flavor
crystalline LOFF phases of QCD. We calculate in the Ginzburg-Landau
approximation the masses of the eight pseudo Nambu-Goldstone Bosons (NGB)
present in the low energy theory. We also compute the decay constants of the
massless NGB Goldstones associa... | hep-ph | we study the bosonic excitations in the favorite cubic three flavor crystalline loff phases of qcd we calculate in the ginzburglandau approximation the masses of the eight pseudo nambugoldstone bosons ngb present in the low energy theory we also compute the decay constants of the massless ngb goldstones associated to s... | [['we', 'study', 'the', 'bosonic', 'excitations', 'in', 'the', 'favorite', 'cubic', 'three', 'flavor', 'crystalline', 'loff', 'phases', 'of', 'qcd', 'we', 'calculate', 'in', 'the', 'ginzburglandau', 'approximation', 'the', 'masses', 'of', 'the', 'eight', 'pseudo', 'nambugoldstone', 'bosons', 'ngb', 'present', 'in', 'th... | [-0.15252621932432237, 0.3168031348770189, -0.0747734281268516, 0.13823777750679633, -0.03800124843979663, -0.10080802014733596, 0.0578277959564996, 0.3066307338545235, -0.2022056105580726, -0.25673750460874745, 0.039773334632627666, -0.30855917685279033, -0.106531182156376, 0.05172304810229235, 0.07351603541273351, 0.... |
706.1782 | A Constant Spectral Index for Sagittarius A* During Infrared/X-ray
Intensity Variations | We report the first time-series of broadband infrared (IR) color measurements
of Sgr A*, the variable emission source associated with the supermassive black
hole at the Galactic Center. Using the laser and natural guide star AO systems
on the Keck II telescope, we imaged Sgr A* in multiple near-infrared broadband
fil... | astro-ph | we report the first timeseries of broadband infrared ir color measurements of sgr a the variable emission source associated with the supermassive black hole at the galactic center using the laser and natural guide star ao systems on the keck ii telescope we imaged sgr a in multiple nearinfrared broadband filters with a... | [['we', 'report', 'the', 'first', 'timeseries', 'of', 'broadband', 'infrared', 'ir', 'color', 'measurements', 'of', 'sgr', 'a', 'the', 'variable', 'emission', 'source', 'associated', 'with', 'the', 'supermassive', 'black', 'hole', 'at', 'the', 'galactic', 'center', 'using', 'the', 'laser', 'and', 'natural', 'guide', 's... | [-0.0598006065956212, 0.17101004621565127, -0.06100854796806718, 0.1010341796291087, -0.07105127935015768, -0.10682236015039141, 0.04389491517992008, 0.4660993596001095, -0.2103159716844716, -0.32629527554775156, 0.08955056959412488, -0.32299062046861854, -0.02494147274902248, 0.210857460899795, -0.020733408813535328, ... |
706.1783 | Scaling and Enhanced Symmetry at the Quantum Critical Point of the
Sub-Ohmic Bose-Fermi Kondo Model | We consider the finite temperature scaling properties of a Kondo-destroying
quantum critical point in the Ising-anisotropic Bose-Fermi Kondo model (BFKM).
A cluster-updating Monte Carlo approach is used, in order to reliably access a
wide temperature range. The scaling function for the two-point spin correlator
is fo... | cond-mat.str-el | we consider the finite temperature scaling properties of a kondodestroying quantum critical point in the isinganisotropic bosefermi kondo model bfkm a clusterupdating monte carlo approach is used in order to reliably access a wide temperature range the scaling function for the twopoint spin correlator is found to have ... | [['we', 'consider', 'the', 'finite', 'temperature', 'scaling', 'properties', 'of', 'a', 'kondodestroying', 'quantum', 'critical', 'point', 'in', 'the', 'isinganisotropic', 'bosefermi', 'kondo', 'model', 'bfkm', 'a', 'clusterupdating', 'monte', 'carlo', 'approach', 'is', 'used', 'in', 'order', 'to', 'reliably', 'access'... | [-0.15089931078616856, 0.1661704678634618, -0.13434011944868032, 0.09370809027391658, -0.0214933947370686, -0.1350901441081219, 0.009456908016112967, 0.32719453139619414, -0.2059365743319097, -0.2216297213024306, 0.07124580823233152, -0.26033158264873385, -0.139375658535446, 0.16933069414983604, 0.04522433358434479, 0.... |
706.1784 | Surfaces with K^2<3\chi and finite fundamental group | In this paper we continue the study of algebraic fundamentale group of
minimal surfaces of general type S satisfying K_S^2<3\chi(S). We show that, if
K_S^2= 3\chi(S)-1 and the algebraic fundamental group of S has order 8, then S
is a Campedelli surface.
In view of the results of math.AG/0512483 and math.AG/0605733,... | math.AG | in this paper we continue the study of algebraic fundamentale group of minimal surfaces of general type s satisfying k_s23chis we show that if k_s2 3chis1 and the algebraic fundamental group of s has order 8 then s is a campedelli surface in view of the results of mathag0512483 and mathag0605733 this implies that the f... | [['in', 'this', 'paper', 'we', 'continue', 'the', 'study', 'of', 'algebraic', 'fundamentale', 'group', 'of', 'minimal', 'surfaces', 'of', 'general', 'type', 's', 'satisfying', 'k_s23chis', 'we', 'show', 'that', 'if', 'k_s2', '3chis1', 'and', 'the', 'algebraic', 'fundamental', 'group', 'of', 's', 'has', 'order', '8', 't... | [-0.14339128790166358, 0.07067020353058288, -0.1115383977222995, 0.034508951522153, -0.06958152130567308, -0.12454032663111414, 0.03951475728435667, 0.33365509001506044, -0.2786271219464934, -0.2742455986906485, 0.13238511845300874, -0.27431094762066316, -0.19761902301227033, 0.2125905675568682, -0.12951345749777451, -... |
706.1785 | Maximum stabilizer dimension for nonproduct states | Composite quantum states can be classified by how they behave under local
unitary transformations. Each quantum state has a stabilizer subgroup and a
corresponding Lie algebra, the structure of which is a local unitary invariant.
In this paper, we study the structure of the stabilizer subalgebra for n-qubit
pure stat... | quant-ph | composite quantum states can be classified by how they behave under local unitary transformations each quantum state has a stabilizer subgroup and a corresponding lie algebra the structure of which is a local unitary invariant in this paper we study the structure of the stabilizer subalgebra for nqubit pure states and ... | [['composite', 'quantum', 'states', 'can', 'be', 'classified', 'by', 'how', 'they', 'behave', 'under', 'local', 'unitary', 'transformations', 'each', 'quantum', 'state', 'has', 'a', 'stabilizer', 'subgroup', 'and', 'a', 'corresponding', 'lie', 'algebra', 'the', 'structure', 'of', 'which', 'is', 'a', 'local', 'unitary',... | [-0.1287812468711223, 0.20333516084624884, -0.08375208984073411, 0.025832199341315042, 0.0035962677743827175, -0.2258888892391617, 0.03771709348771594, 0.34976770206649077, -0.27157357548419225, -0.22774725108065158, 0.09538383731264302, -0.2288331444351337, -0.07927794990121809, 0.14734531596748748, -0.065098099951815... |
706.1786 | Singular Fermi Surfaces I. General Power Counting and Higher Dimensional
Cases | We prove regularity properties of the self-energy, to all orders in
perturbation theory, for systems with singular Fermi surfaces which contain Van
Hove points where the gradient of the dispersion relation vanishes. In this
paper, we show for spatial dimensions $d \ge 3$ that despite the Van Hove
singularity, the ove... | math-ph cond-mat.str-el math.MP | we prove regularity properties of the selfenergy to all orders in perturbation theory for systems with singular fermi surfaces which contain van hove points where the gradient of the dispersion relation vanishes in this paper we show for spatial dimensions d ge 3 that despite the van hove singularity the overlapping lo... | [['we', 'prove', 'regularity', 'properties', 'of', 'the', 'selfenergy', 'to', 'all', 'orders', 'in', 'perturbation', 'theory', 'for', 'systems', 'with', 'singular', 'fermi', 'surfaces', 'which', 'contain', 'van', 'hove', 'points', 'where', 'the', 'gradient', 'of', 'the', 'dispersion', 'relation', 'vanishes', 'in', 'thi... | [-0.19724419431812648, 0.12189511378054266, -0.08637180692274814, 0.05798492760621701, -0.027080755547999782, -0.1534754005295259, 0.05672441479853458, 0.3127411516021109, -0.23331218932375863, -0.23805740724697158, -0.012473172712553706, -0.3322631909279153, -0.1598383272273673, 0.18078825513797778, -0.065606873510060... |
706.1787 | The Search for the Missing Baryons at Low Redshift | At low redshift, only about one-tenth of the known baryons lie in galaxies or
the hot gas seen in galaxy clusters and groups. Models posit that these
"missing baryons" are in gaseous form in overdense filaments that connect the
much denser virialized groups and clusters. About 30% are cool (<1E5 K) and are
detected i... | astro-ph | at low redshift only about onetenth of the known baryons lie in galaxies or the hot gas seen in galaxy clusters and groups models posit that these missing baryons are in gaseous form in overdense filaments that connect the much denser virialized groups and clusters about 30 are cool 1e5 k and are detected in ly alpha a... | [['at', 'low', 'redshift', 'only', 'about', 'onetenth', 'of', 'the', 'known', 'baryons', 'lie', 'in', 'galaxies', 'or', 'the', 'hot', 'gas', 'seen', 'in', 'galaxy', 'clusters', 'and', 'groups', 'models', 'posit', 'that', 'these', 'missing', 'baryons', 'are', 'in', 'gaseous', 'form', 'in', 'overdense', 'filaments', 'tha... | [-0.07533787281895882, 0.15978727272707108, 0.008612321478686309, 0.1100435526445141, -0.08364649762266449, -0.10269699164257921, 0.056275842098858705, 0.47742348206068935, -0.1346489079967554, -0.3505567662931722, 0.02913867791580137, -0.38850524906399364, 0.04374547301002507, 0.14798903421686935, 0.051101790942949026... |
706.1788 | Singular Fermi Surfaces II. The Two--Dimensional Case | We consider many--fermion systems with singular Fermi surfaces, which contain
Van Hove points where the gradient of the band function $k \mapsto e(k)$
vanishes. In a previous paper, we have treated the case of spatial dimension $d
\ge 3$. In this paper, we focus on the more singular case $d=2$ and establish
propertie... | math-ph cond-mat.str-el math.MP | we consider manyfermion systems with singular fermi surfaces which contain van hove points where the gradient of the band function k mapsto ek vanishes in a previous paper we have treated the case of spatial dimension d ge 3 in this paper we focus on the more singular case d2 and establish properties of the fermionic s... | [['we', 'consider', 'manyfermion', 'systems', 'with', 'singular', 'fermi', 'surfaces', 'which', 'contain', 'van', 'hove', 'points', 'where', 'the', 'gradient', 'of', 'the', 'band', 'function', 'k', 'mapsto', 'ek', 'vanishes', 'in', 'a', 'previous', 'paper', 'we', 'have', 'treated', 'the', 'case', 'of', 'spatial', 'dime... | [-0.19880250588580062, 0.08534227150984305, -0.07788576679902487, 0.04752317046465274, -0.028486071759188134, -0.11404705870275696, 0.03127832175879222, 0.34287201441798565, -0.252148467517044, -0.21169182352160634, 0.0018688079483884696, -0.3593878902740673, -0.1790668464867243, 0.14076904391792291, -0.018169043474093... |
706.1789 | B production at the LHC / QCD aspects | The LHC provides new opportunities to improve our understanding of the b
quark using high statistics data samples and the 14 TeV center-of-mass energy.
The prospects to measure the cross section for inclusive b production in events
containing jets and at least one muon are presented. Studies of detector
systematic ef... | hep-ex | the lhc provides new opportunities to improve our understanding of the b quark using high statistics data samples and the 14 tev centerofmass energy the prospects to measure the cross section for inclusive b production in events containing jets and at least one muon are presented studies of detector systematic effects ... | [['the', 'lhc', 'provides', 'new', 'opportunities', 'to', 'improve', 'our', 'understanding', 'of', 'the', 'b', 'quark', 'using', 'high', 'statistics', 'data', 'samples', 'and', 'the', '14', 'tev', 'centerofmass', 'energy', 'the', 'prospects', 'to', 'measure', 'the', 'cross', 'section', 'for', 'inclusive', 'b', 'product... | [-0.03741983339568833, 0.1789779294631444, -0.0676411145250313, 0.15577818686142564, -0.04493966066002031, -0.09085958059586119, 0.0313238934322726, 0.31575529678957537, -0.18935956159839407, -0.33696677317493595, 0.007101761102603632, -0.4247570780935348, 0.08449460261908825, 0.18679429946132586, 0.04705639054009225, ... |
706.179 | How to measure efficiency? | In the context of applied game theory in networking environments, a number of
concepts have been proposed to measure both efficiency and optimality of
resource allocations, the most famous certainly being the price of anarchy and
the Jain index. Yet, very few have tried to question these measures and compare
them one... | cs.GT | in the context of applied game theory in networking environments a number of concepts have been proposed to measure both efficiency and optimality of resource allocations the most famous certainly being the price of anarchy and the jain index yet very few have tried to question these measures and compare them one to an... | [['in', 'the', 'context', 'of', 'applied', 'game', 'theory', 'in', 'networking', 'environments', 'a', 'number', 'of', 'concepts', 'have', 'been', 'proposed', 'to', 'measure', 'both', 'efficiency', 'and', 'optimality', 'of', 'resource', 'allocations', 'the', 'most', 'famous', 'certainly', 'being', 'the', 'price', 'of', ... | [-0.0903412037049279, 0.011485222981057384, -0.11738765180802369, 0.11215623875437869, -0.06397748684905695, -0.14645287309857932, 0.08593632767830665, 0.3729056062628374, -0.24878505760782652, -0.3541149834566044, 0.12395823014737813, -0.24431402874038075, -0.15568458571832514, 0.14798981807843753, -0.1403200809815616... |
706.1791 | X-ray Luminosity Functions of Normal Galaxies in the GOODS | We present soft (0.5-2 keV) X-ray luminosity functions (XLFs) in the Great
Observatories Origins Deep Survey (GOODS) fields, derived for galaxies at
z~0.25 and 0.75. SED fitting was used to estimate photometric redshifts and
separate galaxy types, resulting in a sample of 40 early-type galaxies and 46
late-type galax... | astro-ph | we present soft 052 kev xray luminosity functions xlfs in the great observatories origins deep survey goods fields derived for galaxies at z025 and 075 sed fitting was used to estimate photometric redshifts and separate galaxy types resulting in a sample of 40 earlytype galaxies and 46 latetype galaxies we estimate kco... | [['we', 'present', 'soft', '052', 'kev', 'xray', 'luminosity', 'functions', 'xlfs', 'in', 'the', 'great', 'observatories', 'origins', 'deep', 'survey', 'goods', 'fields', 'derived', 'for', 'galaxies', 'at', 'z025', 'and', '075', 'sed', 'fitting', 'was', 'used', 'to', 'estimate', 'photometric', 'redshifts', 'and', 'sepa... | [0.0476625302748823, 0.05226894655989039, -0.08933567897194501, 0.1898653431044712, -0.0799938190414425, -0.0785461170860532, 0.07925585972106751, 0.5155915460386954, -0.08056888549904757, -0.41120316906738175, 0.003928939211118214, -0.33858964929288815, 0.02493474235674879, 0.20038501484481908, -0.01533358147017521, 0... |
706.1792 | On existence of log minimal models | In this paper, we prove that the log minimal model program in dimension $d-1$
implies the existence of log minimal models for effective lc pairs (eg of
nonnegative Kodaira dimension) in dimension $d$. In fact, we prove that the
same conclusion follows from a weaker assumption, namely, the log minimal model
program wi... | math.AG | in this paper we prove that the log minimal model program in dimension d1 implies the existence of log minimal models for effective lc pairs eg of nonnegative kodaira dimension in dimension d in fact we prove that the same conclusion follows from a weaker assumption namely the log minimal model program with scaling in ... | [['in', 'this', 'paper', 'we', 'prove', 'that', 'the', 'log', 'minimal', 'model', 'program', 'in', 'dimension', 'd1', 'implies', 'the', 'existence', 'of', 'log', 'minimal', 'models', 'for', 'effective', 'lc', 'pairs', 'eg', 'of', 'nonnegative', 'kodaira', 'dimension', 'in', 'dimension', 'd', 'in', 'fact', 'we', 'prove'... | [-0.13692627464255425, 0.06806871513477884, -0.07626149570569396, 0.10743430948395354, -0.009758542658976065, -0.22544766053593215, 0.02941544472392147, 0.28162762952986387, -0.21300838050396684, -0.2957837809360801, 0.06202286168431433, -0.28166736754624605, -0.15340391580516902, 0.17963660063777262, -0.10713485864779... |
706.1793 | The beta function of gauge theories at two loops in differential
renormalization | This PhD thesis is devoted to show that differential renormalization is a
simple and useful renormalization method that we can use when dealing with
gauge theories. In this work, it is shown how the one-loop results of
Constraint Differential Renormalization can be fruitfully applied when
renormalizing two-loop ampli... | hep-th | this phd thesis is devoted to show that differential renormalization is a simple and useful renormalization method that we can use when dealing with gauge theories in this work it is shown how the oneloop results of constraint differential renormalization can be fruitfully applied when renormalizing twoloop amplitudes ... | [['this', 'phd', 'thesis', 'is', 'devoted', 'to', 'show', 'that', 'differential', 'renormalization', 'is', 'a', 'simple', 'and', 'useful', 'renormalization', 'method', 'that', 'we', 'can', 'use', 'when', 'dealing', 'with', 'gauge', 'theories', 'in', 'this', 'work', 'it', 'is', 'shown', 'how', 'the', 'oneloop', 'results... | [-0.07222408953154028, 0.1389307926010366, -0.14204524453479525, 0.11350233946421479, -0.08555329604381014, -0.13446684198726605, -0.01903517114579899, 0.35525021445937455, -0.20735206958985455, -0.26893290880323595, 0.08212839809839795, -0.28026922427883755, -0.21119288945139, 0.15912629152852587, -0.0526248318336268,... |
706.1794 | Birational geometry | This article contains the notes of a graduate course on birational geometry
focusing on the minimal model program. Topics covered include singularities,
vanishing, nonvanishing, cone and contraction, base point freeness, finite
generation, flips, termination, minimal models and Mori fibre spaces.
| math.AG | this article contains the notes of a graduate course on birational geometry focusing on the minimal model program topics covered include singularities vanishing nonvanishing cone and contraction base point freeness finite generation flips termination minimal models and mori fibre spaces | [['this', 'article', 'contains', 'the', 'notes', 'of', 'a', 'graduate', 'course', 'on', 'birational', 'geometry', 'focusing', 'on', 'the', 'minimal', 'model', 'program', 'topics', 'covered', 'include', 'singularities', 'vanishing', 'nonvanishing', 'cone', 'and', 'contraction', 'base', 'point', 'freeness', 'finite', 'ge... | [-0.17641078187152742, 0.09547845391061856, -0.08401171544683166, 0.1295705574884778, -0.16199887632392346, -0.2045830686460249, 0.03254368440248072, 0.2771349095972255, -0.2823775718919933, -0.17357879921328276, 0.15965529039967805, -0.2822201472474262, -0.10632722635054961, 0.16044969211216084, -0.20951191820204257, ... |
706.1795 | Inverting geometric transitions: explicit Calabi-Yau metrics for the
Maldacena-Nunez solutions | Explicit Calabi-Yau metrics are derived that are argued to map to the
Maldacena-Nu\~{n}ez AdS solutions of M-theory and IIB under geometric
transitions. In each case the metrics are singular where a H^2 K\"{a}hler
two-cycle degenerates but are otherwise smooth. They are derived as the most
general Calabi-Yau solution... | hep-th | explicit calabiyau metrics are derived that are argued to map to the maldacenanunez ads solutions of mtheory and iib under geometric transitions in each case the metrics are singular where a h2 kahler twocycle degenerates but are otherwise smooth they are derived as the most general calabiyau solutions of an ansatz for... | [['explicit', 'calabiyau', 'metrics', 'are', 'derived', 'that', 'are', 'argued', 'to', 'map', 'to', 'the', 'maldacenanunez', 'ads', 'solutions', 'of', 'mtheory', 'and', 'iib', 'under', 'geometric', 'transitions', 'in', 'each', 'case', 'the', 'metrics', 'are', 'singular', 'where', 'a', 'h2', 'kahler', 'twocycle', 'degen... | [-0.1933911554045945, 0.061404626870142004, -0.05598436899233474, 0.14589914399097795, -0.11728139004797765, -0.19006634365782263, -0.05307937757630322, 0.3001716115977615, -0.13932713250453102, -0.2020668330707497, 0.17089948583100434, -0.3086926731874325, -0.18927680945865089, 0.11199270929360101, -0.1280617631611324... |
706.1796 | Project to install roman pot detectors at 220 m in ATLAS | We give a short description of the project to install roman pot detectors at
220 m from the interaction point in ATLAS. This project is dedicated to hard
diffractive measurements at high luminosity.
| physics.ins-det hep-ex | we give a short description of the project to install roman pot detectors at 220 m from the interaction point in atlas this project is dedicated to hard diffractive measurements at high luminosity | [['we', 'give', 'a', 'short', 'description', 'of', 'the', 'project', 'to', 'install', 'roman', 'pot', 'detectors', 'at', '220', 'm', 'from', 'the', 'interaction', 'point', 'in', 'atlas', 'this', 'project', 'is', 'dedicated', 'to', 'hard', 'diffractive', 'measurements', 'at', 'high', 'luminosity']] | [-0.04782897521826354, 0.1346326038862268, -0.13861080216751856, 0.09276737837177335, -0.09758235683495348, -0.1141494405526442, -0.008084943743817734, 0.4112627205975128, -0.18455611376769163, -0.4102330046395461, 0.08528766221945372, -0.41227334703911434, 0.06199304307599298, 0.13369145689560383, -0.01441067203202031... |
706.1797 | Soluble Models of Strongly Interacting Ultracold Gas Mixtures in Tight
Waveguides | A generalized Fermi-Bose mapping method is used to determine the exact ground
states of several models of mixtures of strongly interacting ultracold gases in
tight waveguides, which are generalizations of the Tonks-Girardeau (TG) gas (1D
Bose gas with point hard cores) and fermionic Tonks-Girardeau (FTG) gas (1D
spin... | cond-mat.other | a generalized fermibose mapping method is used to determine the exact ground states of several models of mixtures of strongly interacting ultracold gases in tight waveguides which are generalizations of the tonksgirardeau tg gas 1d bose gas with point hard cores and fermionic tonksgirardeau ftg gas 1d spinaligned fermi... | [['a', 'generalized', 'fermibose', 'mapping', 'method', 'is', 'used', 'to', 'determine', 'the', 'exact', 'ground', 'states', 'of', 'several', 'models', 'of', 'mixtures', 'of', 'strongly', 'interacting', 'ultracold', 'gases', 'in', 'tight', 'waveguides', 'which', 'are', 'generalizations', 'of', 'the', 'tonksgirardeau', ... | [-0.1479670585223795, 0.24724320980382308, -0.036215498789514425, 0.0945073924237549, 0.05240860027549541, -0.21906253498097042, 0.02888449842720169, 0.3859449514410401, -0.1727552640342475, -0.17263160991704965, -0.02905981833799289, -0.3286484314161724, -0.05602243708743326, 0.09926375048647149, 0.11124069729935279, ... |
706.1798 | New QCD fits to HERA data and search for exclusive events at the
Tevatron | We describe new QCD fits to diffractive proton structure functions measured
at HERA, and we use these parton densities to predict the shape of the dijet
mass fraction at the Tevatron and look for the existence of exclusive events in
the dijet channel.
| hep-ph | we describe new qcd fits to diffractive proton structure functions measured at hera and we use these parton densities to predict the shape of the dijet mass fraction at the tevatron and look for the existence of exclusive events in the dijet channel | [['we', 'describe', 'new', 'qcd', 'fits', 'to', 'diffractive', 'proton', 'structure', 'functions', 'measured', 'at', 'hera', 'and', 'we', 'use', 'these', 'parton', 'densities', 'to', 'predict', 'the', 'shape', 'of', 'the', 'dijet', 'mass', 'fraction', 'at', 'the', 'tevatron', 'and', 'look', 'for', 'the', 'existence', '... | [-0.001759962157108063, 0.18030464772654828, -0.1734778987092161, 0.21633512110904204, -0.05370802773422627, -0.022781443025451154, 0.005263328682198081, 0.4089040392793195, -0.17959396289878113, -0.22117255163530625, -0.05598492211348182, -0.32803315229627283, 0.0636492051010908, 0.0811604342834894, 0.0900789879175812... |
706.1799 | BFKL NLL phenomenology of forward jets at HERA and Mueller Navelet jets
at the Tevatron and the LHC | We perform a BFKL-NLL analysis of forward jet production at HERA which leads
to a good description of data over the full kinematical domain. We also predict
the azimuthal angle dependence of Mueller-Navelet jet production at the
Tevatron and the LHC using the BFKL NLL formalism.
| hep-ph | we perform a bfklnll analysis of forward jet production at hera which leads to a good description of data over the full kinematical domain we also predict the azimuthal angle dependence of muellernavelet jet production at the tevatron and the lhc using the bfkl nll formalism | [['we', 'perform', 'a', 'bfklnll', 'analysis', 'of', 'forward', 'jet', 'production', 'at', 'hera', 'which', 'leads', 'to', 'a', 'good', 'description', 'of', 'data', 'over', 'the', 'full', 'kinematical', 'domain', 'we', 'also', 'predict', 'the', 'azimuthal', 'angle', 'dependence', 'of', 'muellernavelet', 'jet', 'product... | [-0.03699675393808219, 0.04000433542662197, -0.2345073766178555, 0.16176560057534112, -0.09937549539738232, -0.06162926005975654, -0.016816541663784948, 0.38054582104086876, -0.2005704476705028, -0.24906364046037197, -0.038572553193403615, -0.31446404399143324, 0.08528507649898528, 0.1443404510617256, 0.135124058950330... |
706.18 | Necessary Conditions for Schur-Positivity | In recent years, there has been considerable interest in showing that certain
conditions on skew shapes A and B are sufficient for the difference s_A - s_B
of their skew Schur functions to be Schur-positive. We determine necessary
conditions for the difference to be Schur-positive. Our conditions are
motivated by tho... | math.CO | in recent years there has been considerable interest in showing that certain conditions on skew shapes a and b are sufficient for the difference s_a s_b of their skew schur functions to be schurpositive we determine necessary conditions for the difference to be schurpositive our conditions are motivated by those of rei... | [['in', 'recent', 'years', 'there', 'has', 'been', 'considerable', 'interest', 'in', 'showing', 'that', 'certain', 'conditions', 'on', 'skew', 'shapes', 'a', 'and', 'b', 'are', 'sufficient', 'for', 'the', 'difference', 's_a', 's_b', 'of', 'their', 'skew', 'schur', 'functions', 'to', 'be', 'schurpositive', 'we', 'determ... | [-0.13523312089209621, 0.12415129449721929, -0.0782271523683055, 0.08542821159888361, -0.05330105228160785, -0.1284431509635839, 0.011053608403213927, 0.40696168897321094, -0.24989829630263755, -0.24412070406047073, 0.1332285303490337, -0.24016673090502721, -0.1659419561509748, 0.24904167835877553, -0.16521910493690017... |
706.1801 | Mass-to-light Ratio of Ly-alpha Emitters: Implications of Ly-alpha
Surveys at Redshifts z=5.7, 6.5, 7, and 8.8 | Using a simple method to interpret the luminosity function of Ly-alpha
emitters, we explore properties of Ly-alpha emitters from 5.7 < z < 8.8 with
various assumptions about metallicity and stellar mass spectra. We constrain a
mass-to-'observed' light ratio, M_h/L_band. For narrow-band surveys, L_band is
simply relat... | astro-ph | using a simple method to interpret the luminosity function of lyalpha emitters we explore properties of lyalpha emitters from 57 z 88 with various assumptions about metallicity and stellar mass spectra we constrain a masstoobserved light ratio m_hl_band for narrowband surveys l_band is simply related to the intrinsic l... | [['using', 'a', 'simple', 'method', 'to', 'interpret', 'the', 'luminosity', 'function', 'of', 'lyalpha', 'emitters', 'we', 'explore', 'properties', 'of', 'lyalpha', 'emitters', 'from', '57', 'z', '88', 'with', 'various', 'assumptions', 'about', 'metallicity', 'and', 'stellar', 'mass', 'spectra', 'we', 'constrain', 'a',... | [-0.03276569918609827, 0.11964311688278456, -0.009431998850242502, 0.1329400748874407, -0.07710966759564719, -0.1067602704582429, 0.08630785904200283, 0.4779539400590334, -0.10102290749796078, -0.353187154407588, 0.007224415261673088, -0.35587813743029745, 0.007829100716059805, 0.2140518568645292, 0.04323395585973115, ... |
706.1802 | Notes on Quantum Field Theory in Curved Spacetime: Problems Relating to
the Concept of Particles and Hamiltonian Formalism | The aim of these notes is to elucidate some aspects of quantum field theory
in curved spacetime, especially those relating to the notion of particles. A
selection of issues relevant to wave-particle duality is given. The case of a
generic curved spacetime is outlined. A Hamiltonian formulation of quantum
field theory... | physics.gen-ph | the aim of these notes is to elucidate some aspects of quantum field theory in curved spacetime especially those relating to the notion of particles a selection of issues relevant to waveparticle duality is given the case of a generic curved spacetime is outlined a hamiltonian formulation of quantum field theory in cur... | [['the', 'aim', 'of', 'these', 'notes', 'is', 'to', 'elucidate', 'some', 'aspects', 'of', 'quantum', 'field', 'theory', 'in', 'curved', 'spacetime', 'especially', 'those', 'relating', 'to', 'the', 'notion', 'of', 'particles', 'a', 'selection', 'of', 'issues', 'relevant', 'to', 'waveparticle', 'duality', 'is', 'given', ... | [-0.17936725559535416, 0.14196545567531932, -0.10911839727208296, 0.11955897067301965, -0.10815422459099283, -0.160756095842597, -0.06072809570159347, 0.32825481456684624, -0.20236806483305197, -0.2397926252612725, 0.04059867672201127, -0.22024315111140938, -0.13692869613085815, 0.15476011615642843, -0.1109535949641561... |
706.1803 | Electronic stopping power in insulators from first principles | Using time-dependent density-functional theory we calculate from first
principles the rate of energy transfer from a moving proton or antiproton to
the electrons of an insulating material, LiF. The behavior of the electronic
stopping power versus projectile velocity displays an effective threshold
velocity of ~0.2 a.... | cond-mat.mtrl-sci | using timedependent densityfunctional theory we calculate from first principles the rate of energy transfer from a moving proton or antiproton to the electrons of an insulating material lif the behavior of the electronic stopping power versus projectile velocity displays an effective threshold velocity of 02 au for the... | [['using', 'timedependent', 'densityfunctional', 'theory', 'we', 'calculate', 'from', 'first', 'principles', 'the', 'rate', 'of', 'energy', 'transfer', 'from', 'a', 'moving', 'proton', 'or', 'antiproton', 'to', 'the', 'electrons', 'of', 'an', 'insulating', 'material', 'lif', 'the', 'behavior', 'of', 'the', 'electronic'... | [-0.03588035851226826, 0.1838065224972333, -0.07976230036369279, 0.06714543403420402, 0.01217383931537992, -0.09663907985423545, 0.06215415527817401, 0.37449806281610537, -0.23337629676649446, -0.3310999213766895, -0.02599474549734671, -0.34723024338875946, 0.012979657470101588, 0.16811426948314825, 0.0315798218343652,... |
706.1804 | HD 114839 - An Am star showing both delta Scuti and gamma Dor pulsations
discovered through MOST photometry | Using MOST (Microvariability and Oscillations of STars) satellite guide star
photometry, we have discovered a metallic A star showing hybrid p- and g-mode
pulsations. HD 114839 was observed nearly continuously for 10 days in March,
2005. We identify frequencies in three groups: the first centered near 2
cycles/day, i... | astro-ph | using most microvariability and oscillations of stars satellite guide star photometry we have discovered a metallic a star showing hybrid p and gmode pulsations hd 114839 was observed nearly continuously for 10 days in march 2005 we identify frequencies in three groups the first centered near 2 cyclesday in the gamma d... | [['using', 'most', 'microvariability', 'and', 'oscillations', 'of', 'stars', 'satellite', 'guide', 'star', 'photometry', 'we', 'have', 'discovered', 'a', 'metallic', 'a', 'star', 'showing', 'hybrid', 'p', 'and', 'gmode', 'pulsations', 'hd', '114839', 'was', 'observed', 'nearly', 'continuously', 'for', '10', 'days', 'in... | [-0.11885515587447687, 0.15940706631125406, -0.03101331007471958, 0.02916278205148681, -0.15007655875659873, -0.1201077172381067, 0.1316432423759685, 0.3716136960442676, -0.1694507828472334, -0.38647847477519925, 0.06920486632572097, -0.3223003585400536, -0.137897678060717, 0.24256160389631987, -0.08081102254800498, 0.... |
706.1805 | The von Neumann entropy asymptotics in multidimensional fermionic
systems | We study the von Neumann entropy asymptotics of pure translation-invariant
quasi-free states of d-dimensional fermionic systems. It is shown that the
entropic area law is violated by all these states: apart from the trivial
cases, the entropy of a cubic subsystem with edge length L cannot grow slower
than L^{d-1}ln L... | math-ph cond-mat.stat-mech math.MP quant-ph | we study the von neumann entropy asymptotics of pure translationinvariant quasifree states of ddimensional fermionic systems it is shown that the entropic area law is violated by all these states apart from the trivial cases the entropy of a cubic subsystem with edge length l cannot grow slower than ld1ln l as for the ... | [['we', 'study', 'the', 'von', 'neumann', 'entropy', 'asymptotics', 'of', 'pure', 'translationinvariant', 'quasifree', 'states', 'of', 'ddimensional', 'fermionic', 'systems', 'it', 'is', 'shown', 'that', 'the', 'entropic', 'area', 'law', 'is', 'violated', 'by', 'all', 'these', 'states', 'apart', 'from', 'the', 'trivial... | [-0.153814724284166, 0.24320328688481824, -0.10260634695296175, 0.08422147117234999, 0.01104141479008831, -0.21216133096604609, 0.03409479905385524, 0.25199052268581, -0.25066158585832454, -0.19706294436473398, 0.11665478357463144, -0.3412315655499697, -0.07304137823521159, 0.20351126543828285, -0.02539972495578695, 0.... |
706.1806 | On the asymptotic behavior of Faber polynomials for domains with
piecewise analytic boundary | For a function g(w) analytic and univalent in {w:1<|w|<\infty} with a simple
pole at \infty and a continuous extension to {w:|w|\geq 1}, we consider the
Faber polynomials F_n(z), n=0,1,2,..., associated to g(w) via their generating
function g'(w)/(g(w)-z)=\sum_{n=0}^\infty F_n(z)w^{-(n+1)}. Assuming that g(w)
maps th... | math.CA math.CV | for a function gw analytic and univalent in w1winfty with a simple pole at infty and a continuous extension to wwgeq 1 we consider the faber polynomials f_nz n012 associated to gw via their generating function gwgwzsum_n0infty f_nzwn1 assuming that gw maps the unit circle t onto a piecewise analytic curve l whose exter... | [['for', 'a', 'function', 'gw', 'analytic', 'and', 'univalent', 'in', 'w1winfty', 'with', 'a', 'simple', 'pole', 'at', 'infty', 'and', 'a', 'continuous', 'extension', 'to', 'wwgeq', '1', 'we', 'consider', 'the', 'faber', 'polynomials', 'f_nz', 'n012', 'associated', 'to', 'gw', 'via', 'their', 'generating', 'function', ... | [-0.15940215787373208, 0.03606947237488787, -0.09546740321808907, 0.0867821466049836, -0.05990773283678, -0.08118613029173652, 0.08433031879048641, 0.34010990822809883, -0.25288895743547896, -0.1853477525311049, 0.12512212322708066, -0.2914572033008225, -0.12774777534555215, 0.22413934825263063, -0.01905404375250581, 0... |
706.1807 | Generalised knot groups distinguish the square and granny knots (with an
appendix by David Savitt) | Given a knot K we may construct a group G_n(K) from the fundamental group of
K by adjoining an nth root of the meridian that commutes with the corresponding
longitude. These "generalised knot groups" were introduced independently by
Wada and Kelly, and contain the fundamental group as a subgroup. The square
knot SK a... | math.GT | given a knot k we may construct a group g_nk from the fundamental group of k by adjoining an nth root of the meridian that commutes with the corresponding longitude these generalised knot groups were introduced independently by wada and kelly and contain the fundamental group as a subgroup the square knot sk and the gr... | [['given', 'a', 'knot', 'k', 'we', 'may', 'construct', 'a', 'group', 'g_nk', 'from', 'the', 'fundamental', 'group', 'of', 'k', 'by', 'adjoining', 'an', 'nth', 'root', 'of', 'the', 'meridian', 'that', 'commutes', 'with', 'the', 'corresponding', 'longitude', 'these', 'generalised', 'knot', 'groups', 'were', 'introduced',... | [-0.2017894486728152, 0.11280651832387761, -0.10287025164284591, 0.03898705417114838, -0.10466212903865293, -0.14478475238377256, 0.03243274024145594, 0.3386818345205219, -0.2823940523858391, -0.30040143036853467, 0.10215102157941255, -0.28309029679738484, -0.1544829051152789, 0.2065841933545559, -0.10964428019751586, ... |
706.1808 | Simultaneous packing and covering in the two-dimensional Euclidean plane
II | This paper determines the optimal upper bound for the simultaneous packing
and covering constants of the two-dimensional centrally symmetric convex
domains. It solved a problem opening for more than thirty years.
| math.MG math.NT | this paper determines the optimal upper bound for the simultaneous packing and covering constants of the twodimensional centrally symmetric convex domains it solved a problem opening for more than thirty years | [['this', 'paper', 'determines', 'the', 'optimal', 'upper', 'bound', 'for', 'the', 'simultaneous', 'packing', 'and', 'covering', 'constants', 'of', 'the', 'twodimensional', 'centrally', 'symmetric', 'convex', 'domains', 'it', 'solved', 'a', 'problem', 'opening', 'for', 'more', 'than', 'thirty', 'years']] | [-0.13737493811640888, 0.11198493075226584, -0.009143529805324731, 0.06209559965082594, -0.08098677595356299, -0.15581625362016982, 0.09369734458760509, 0.354044642089115, -0.2647981189431683, -0.2802363611277073, 0.18353467026064474, -0.22616920151537465, -0.10683583170776406, 0.2637979222401496, -0.030885371980407545... |
706.1809 | The Spitzer c2d Survey of Large, Nearby, Interstellar Clouds. IV. Lupus
Observed with MIPS | We present maps of 7.78 square degrees of the Lupus molecular cloud complex
at 24, 70, and $160\:\mu$m. They were made with the Spitzer Space Telescope's
Multiband Imaging Photometer for Spitzer (MIPS) instrument as part of the
Spitzer Legacy Program, ``From Molecular Cores to Planet-Forming Disks'' (c2d).
The maps c... | astro-ph | we present maps of 778 square degrees of the lupus molecular cloud complex at 24 70 and 160mum they were made with the spitzer space telescopes multiband imaging photometer for spitzer mips instrument as part of the spitzer legacy program from molecular cores to planetforming disks c2d the maps cover three separate reg... | [['we', 'present', 'maps', 'of', '778', 'square', 'degrees', 'of', 'the', 'lupus', 'molecular', 'cloud', 'complex', 'at', '24', '70', 'and', '160mum', 'they', 'were', 'made', 'with', 'the', 'spitzer', 'space', 'telescopes', 'multiband', 'imaging', 'photometer', 'for', 'spitzer', 'mips', 'instrument', 'as', 'part', 'of'... | [0.0036963350261606637, 0.05825471620060383, -0.08055641878050782, 0.0992907403138346, -0.0821381448279886, -0.0527777808883618, 0.08769067423699814, 0.4758150880675643, -0.18841771107737817, -0.37237582098685146, 0.07147876568553564, -0.3285076643092438, -0.05751566816170159, 0.18329408172341513, -0.06557565433761356,... |
706.181 | A sufficient condition for a number to be the order of a nonsingular
derivation of a Lie algebra | A study of the set N_p of positive integers which occur as orders of
nonsingular derivations of finite-dimensional non-nilpotent Lie algebras of
characteristic p>0 was initiated by Shalev and continued by the present author.
The main goal of this paper is to show the abundance of elements of N_p. Our
main result show... | math.RA math.NT | a study of the set n_p of positive integers which occur as orders of nonsingular derivations of finitedimensional nonnilpotent lie algebras of characteristic p0 was initiated by shalev and continued by the present author the main goal of this paper is to show the abundance of elements of n_p our main result shows that ... | [['a', 'study', 'of', 'the', 'set', 'n_p', 'of', 'positive', 'integers', 'which', 'occur', 'as', 'orders', 'of', 'nonsingular', 'derivations', 'of', 'finitedimensional', 'nonnilpotent', 'lie', 'algebras', 'of', 'characteristic', 'p0', 'was', 'initiated', 'by', 'shalev', 'and', 'continued', 'by', 'the', 'present', 'auth... | [-0.1778498045479258, 0.10381996047993501, -0.07373342816717923, -0.017865219350076383, -0.03525536099785111, -0.13430217518471183, -0.007862694333824846, 0.2755077375099063, -0.264664148632437, -0.2291880018181271, 0.04662567016332307, -0.24184094516612176, -0.14714951916959965, 0.19141997896755736, -0.103127357203306... |
706.1811 | Direct determination of the epicycle frequency in the galactic disk, and
the derived rotation velocity V0 | We present a method which allows a direct measurement of the epicycle
frequency $\kappa$ in the galactic disk, using the large database on open
clusters completed by our group. The observed velocity vector (amplitude and
direction) of the clusters in the galactic plane is derived from the catalog
data. In the epicycl... | astro-ph | we present a method which allows a direct measurement of the epicycle frequency kappa in the galactic disk using the large database on open clusters completed by our group the observed velocity vector amplitude and direction of the clusters in the galactic plane is derived from the catalog data in the epicycle approxim... | [['we', 'present', 'a', 'method', 'which', 'allows', 'a', 'direct', 'measurement', 'of', 'the', 'epicycle', 'frequency', 'kappa', 'in', 'the', 'galactic', 'disk', 'using', 'the', 'large', 'database', 'on', 'open', 'clusters', 'completed', 'by', 'our', 'group', 'the', 'observed', 'velocity', 'vector', 'amplitude', 'and'... | [-0.15472391003806313, 0.1170051387038477, -0.0898958063079397, 0.018941027712902393, -0.09469122918424987, -0.03833905594144722, 0.03389532602953047, 0.36666778032226965, -0.25309365970139025, -0.29125453022358916, 0.07332984194076606, -0.2537594766199618, -0.050934029694568984, 0.22325114416404782, -0.016501777511703... |
706.1812 | Shell model study of neutron rich oxygen isotopes | Shell model calculations for low lying energy states of neutron rich oxygen
isotopes 19O, 20O, 21O, 22O, 23O, 24O, 25O, 26O have been performed using
OXBASH code. The configuration space consists of 0d5/2, 1s1/2, 0d3/2 orbital
for neutrons outside the 16O core. Different interactions namely, Wildenthal,
Preedom-Wilde... | nucl-th | shell model calculations for low lying energy states of neutron rich oxygen isotopes 19o 20o 21o 22o 23o 24o 25o 26o have been performed using oxbash code the configuration space consists of 0d52 1s12 0d32 orbital for neutrons outside the 16o core different interactions namely wildenthal preedomwildenthal wildenthalmcg... | [['shell', 'model', 'calculations', 'for', 'low', 'lying', 'energy', 'states', 'of', 'neutron', 'rich', 'oxygen', 'isotopes', '19o', '20o', '21o', '22o', '23o', '24o', '25o', '26o', 'have', 'been', 'performed', 'using', 'oxbash', 'code', 'the', 'configuration', 'space', 'consists', 'of', '0d52', '1s12', '0d32', 'orbita... | [-0.052492622812433054, 0.17122234619593346, -0.04620341597714183, 0.16893899563525613, 0.04794206371353233, -0.113191292067257, 0.06762450673370247, 0.3725293810563206, -0.15771036831247157, -0.36270830183188324, 0.013500663556127645, -0.34471453299030874, 0.009384231488610744, 0.14573502705390542, 0.07319292828211146... |
706.1813 | Uniqueness of the EPR--chemeleon model | A classical deterministic, reversible dynamical systems, reproducing the
Einstein--Podolsky--Rosen (EPR) correlations in full respect of causality and
locality and without the introduction of any ad hoc selection procedure, was
constructed in the paper [AIR02].
In the present paper we prove that the above mentioned... | quant-ph | a classical deterministic reversible dynamical systems reproducing the einsteinpodolskyrosen epr correlations in full respect of causality and locality and without the introduction of any ad hoc selection procedure was constructed in the paper air02 in the present paper we prove that the above mentioned model is unique... | [['a', 'classical', 'deterministic', 'reversible', 'dynamical', 'systems', 'reproducing', 'the', 'einsteinpodolskyrosen', 'epr', 'correlations', 'in', 'full', 'respect', 'of', 'causality', 'and', 'locality', 'and', 'without', 'the', 'introduction', 'of', 'any', 'ad', 'hoc', 'selection', 'procedure', 'was', 'constructed... | [-0.10573624580034188, 0.11061966593130207, -0.0794032915134211, 0.11636955905539383, -0.0324139581822163, -0.19196254203252835, 0.04554204342706243, 0.3257994995433457, -0.20704534207708297, -0.2747861648825406, 0.059353218170961515, -0.25795239501879835, -0.15853654565194583, 0.12643376754463784, -0.08818838924017487... |
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