id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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708.0349 | Observational Constraints on Agegraphic Dark Energy | In this paper, we use the Type Ia supernova data as well as the CMB and LSS
data to constrain the agegraphic dark energy model recently proposed by Cai.
Due to its peculiar nature, the parameter $n$ of this model cannot be well
constrained by the SNIa data, while the other parameter $\Omega_{m0}$ can be
constrained t... | astro-ph | in this paper we use the type ia supernova data as well as the cmb and lss data to constrain the agegraphic dark energy model recently proposed by cai due to its peculiar nature the parameter n of this model cannot be well constrained by the snia data while the other parameter omega_m0 can be constrained to be 034pm004... | [['in', 'this', 'paper', 'we', 'use', 'the', 'type', 'ia', 'supernova', 'data', 'as', 'well', 'as', 'the', 'cmb', 'and', 'lss', 'data', 'to', 'constrain', 'the', 'agegraphic', 'dark', 'energy', 'model', 'recently', 'proposed', 'by', 'cai', 'due', 'to', 'its', 'peculiar', 'nature', 'the', 'parameter', 'n', 'of', 'this',... | [-0.030461389118021254, 0.10396390756910764, -0.051023644983376325, 0.11829747133398134, -0.14139075359133513, -0.13480020850271868, 0.03570710109794929, 0.32999566910898703, -0.24131213763719547, -0.3738143430336526, 0.09635176971374006, -0.2787007521899221, -0.056721521467950786, 0.21231388075945065, -0.0345262338186... |
708.035 | Biaxial Strain in the Hexagonal Plane of MnAs Thin Films: The Key to
Stabilize Ferromagnetism to Higher Temperature | The alpha-beta magneto-structural phase transition in MnAs/GaAs(111)
epilayers is investigated by elastic neutron scattering. The in-plane parameter
of MnAs remains almost constant with temperature from 100 K to 420 K, following
the thermal evolution of the GaAs substrate. This induces a temperature
dependent biaxial... | cond-mat.mtrl-sci | the alphabeta magnetostructural phase transition in mnasgaas111 epilayers is investigated by elastic neutron scattering the inplane parameter of mnas remains almost constant with temperature from 100 k to 420 k following the thermal evolution of the gaas substrate this induces a temperature dependent biaxial strain tha... | [['the', 'alphabeta', 'magnetostructural', 'phase', 'transition', 'in', 'mnasgaas111', 'epilayers', 'is', 'investigated', 'by', 'elastic', 'neutron', 'scattering', 'the', 'inplane', 'parameter', 'of', 'mnas', 'remains', 'almost', 'constant', 'with', 'temperature', 'from', '100', 'k', 'to', '420', 'k', 'following', 'the... | [-0.16653663246629027, 0.273572805682202, -0.034273484915282273, -0.04041829237096073, -0.029699024897007667, -0.11869181591452511, 0.11962140103053974, 0.4225058753623581, -0.27256911927376126, -0.271401017560761, 0.0423308987767802, -0.29063700261663217, -0.08518528312895081, 0.16730271717228118, 0.09102235816144308,... |
708.0351 | Hard pion bremsstrahlung in the Coulomb region | Hard high-energy pion-nucleus bremsstrahlung, $\pi^- +A\to\pi^- +\gamma +A$,
is studied in the Coulomb region, i.e. the small-angle region where the nuclear
scattering is dominated by the Coulomb interaction. Special attention is
focussed on the possibility of measuring the pion polarizability in such
reactions. We s... | nucl-th | hard highenergy pionnucleus bremsstrahlung pi atopi gamma a is studied in the coulomb region ie the smallangle region where the nuclear scattering is dominated by the coulomb interaction special attention is focussed on the possibility of measuring the pion polarizability in such reactions we study the sensitivity to t... | [['hard', 'highenergy', 'pionnucleus', 'bremsstrahlung', 'pi', 'atopi', 'gamma', 'a', 'is', 'studied', 'in', 'the', 'coulomb', 'region', 'ie', 'the', 'smallangle', 'region', 'where', 'the', 'nuclear', 'scattering', 'is', 'dominated', 'by', 'the', 'coulomb', 'interaction', 'special', 'attention', 'is', 'focussed', 'on',... | [-0.10081866467050438, 0.21098475052236482, -0.08327336934255972, 0.1449758646081084, -0.05210835758018596, -0.0784760239459146, 0.033388703119480743, 0.36791524158298283, -0.26153497466410713, -0.23150446638464928, 0.0009592603263177577, -0.31995093198653696, -0.11610287290077186, 0.13171630613666413, 0.07690447264407... |
708.0352 | Gribov Poles in Diffractive Physics | High-energy diffractive physics has several interests for theoreticians and
experimentalists. We first remind the reader of the main characteristics of
diffraction in particles physics and present the calculation of a two-gluon
exchange in which non-perturbative effects are introduced via new singularities
from confi... | hep-ph | highenergy diffractive physics has several interests for theoreticians and experimentalists we first remind the reader of the main characteristics of diffraction in particles physics and present the calculation of a twogluon exchange in which nonperturbative effects are introduced via new singularities from confinement | [['highenergy', 'diffractive', 'physics', 'has', 'several', 'interests', 'for', 'theoreticians', 'and', 'experimentalists', 'we', 'first', 'remind', 'the', 'reader', 'of', 'the', 'main', 'characteristics', 'of', 'diffraction', 'in', 'particles', 'physics', 'and', 'present', 'the', 'calculation', 'of', 'a', 'twogluon', ... | [-0.05508409455678491, 0.18815478395269966, -0.17679274947447485, 0.13991289463457326, -0.13043380801587603, -0.11597147193022592, 0.009707759345643396, 0.32229754839872204, -0.22486023020356632, -0.2899556620003179, -0.01202935303648024, -0.33227877132594585, -0.12824065398511497, 0.1540736358336628, 0.005168504298253... |
708.0353 | The Local Fractal Properties of the Financial Time Series on the Polish
Stock Exchange Market | We investigate the local fractal properties of the financial time series
based on the evolution of the Warsaw Stock Exchange Index (WIG) connected with
the largest developing financial market in Europe. Calculating the local Hurst
exponent for the WIG time series we find an interesting dependence between the
behavior... | q-fin.ST cs.CE physics.data-an | we investigate the local fractal properties of the financial time series based on the evolution of the warsaw stock exchange index wig connected with the largest developing financial market in europe calculating the local hurst exponent for the wig time series we find an interesting dependence between the behavior of t... | [['we', 'investigate', 'the', 'local', 'fractal', 'properties', 'of', 'the', 'financial', 'time', 'series', 'based', 'on', 'the', 'evolution', 'of', 'the', 'warsaw', 'stock', 'exchange', 'index', 'wig', 'connected', 'with', 'the', 'largest', 'developing', 'financial', 'market', 'in', 'europe', 'calculating', 'the', 'lo... | [-0.1399218818562022, 0.08453948011316895, -0.1479531566090902, 0.10836359438722704, -0.04940913527693127, -0.02023266588073613, 0.0376279959559385, 0.3336082972697358, -0.29926265774767347, -0.24160393808426253, 0.1587260560003985, -0.33886187009290974, -0.17866848120048864, 0.2183199804276228, -0.0069239625286783525,... |
708.0354 | Universal Nonlinear Filtering Using Feynman Path Integrals I: The
Continuous-Discrete Model with Additive Noise | The continuous-discrete filtering problem requires the solution of a partial
differential equation known as the Fokker-Planck-Kolmogorov forward equation
(FPKfe). In this paper, the path integral formula for the fundamental solution
of the FPKfe is derived and verified for the general additive noise case (i.e.,
expli... | cond-mat.other | the continuousdiscrete filtering problem requires the solution of a partial differential equation known as the fokkerplanckkolmogorov forward equation fpkfe in this paper the path integral formula for the fundamental solution of the fpkfe is derived and verified for the general additive noise case ie explicitly timedep... | [['the', 'continuousdiscrete', 'filtering', 'problem', 'requires', 'the', 'solution', 'of', 'a', 'partial', 'differential', 'equation', 'known', 'as', 'the', 'fokkerplanckkolmogorov', 'forward', 'equation', 'fpkfe', 'in', 'this', 'paper', 'the', 'path', 'integral', 'formula', 'for', 'the', 'fundamental', 'solution', 'o... | [-0.12876037420631437, 0.023318212234268065, -0.07650682611979152, 0.09014036848307833, -0.11308888419482269, -0.15485108706879577, -0.0069033238580327875, 0.3129371564443174, -0.31798473505707653, -0.25393402218622596, 0.12885774420513035, -0.2466375139836026, -0.18506394681447236, 0.1920642183425738, -0.0656940211208... |
708.0355 | Advances in Data Combination, Analysis and Collection for System
Reliability Assessment | The systems that statisticians are asked to assess, such as nuclear weapons,
infrastructure networks, supercomputer codes and munitions, have become
increasingly complex. It is often costly to conduct full system tests. As such,
we present a review of methodology that has been proposed for addressing system
reliabili... | stat.ME | the systems that statisticians are asked to assess such as nuclear weapons infrastructure networks supercomputer codes and munitions have become increasingly complex it is often costly to conduct full system tests as such we present a review of methodology that has been proposed for addressing system reliability with l... | [['the', 'systems', 'that', 'statisticians', 'are', 'asked', 'to', 'assess', 'such', 'as', 'nuclear', 'weapons', 'infrastructure', 'networks', 'supercomputer', 'codes', 'and', 'munitions', 'have', 'become', 'increasingly', 'complex', 'it', 'is', 'often', 'costly', 'to', 'conduct', 'full', 'system', 'tests', 'as', 'such... | [-0.10360960683554224, -0.015739203630042053, -0.04101820886738116, 0.06995498155169994, -0.06639323736668276, -0.14922963096860717, 0.04676260796363847, 0.37374801970616306, -0.24276833812766474, -0.3347926433499661, 0.15165054879114434, -0.27816999728771313, -0.14829500195764594, 0.2247000203849815, -0.07321356085510... |
708.0356 | Quantum phase diffusion of a Bose system: beyond the
Hartree-Fock-Bogoliubov approximation | A diffusion process is usually assumed for the phase of the order parameter
of a Bose system of finite size. The theoretical basis is limited to the so
called Bogoliubov approximation. We show that a suitable generalization of the
Hartree-Fock-Bogoliubov approach recovers phase diffusion.
| quant-ph | a diffusion process is usually assumed for the phase of the order parameter of a bose system of finite size the theoretical basis is limited to the so called bogoliubov approximation we show that a suitable generalization of the hartreefockbogoliubov approach recovers phase diffusion | [['a', 'diffusion', 'process', 'is', 'usually', 'assumed', 'for', 'the', 'phase', 'of', 'the', 'order', 'parameter', 'of', 'a', 'bose', 'system', 'of', 'finite', 'size', 'the', 'theoretical', 'basis', 'is', 'limited', 'to', 'the', 'so', 'called', 'bogoliubov', 'approximation', 'we', 'show', 'that', 'a', 'suitable', 'ge... | [-0.1233733335340565, 0.16940282890573144, -0.1279319715262814, 0.050388907327322326, -0.07542091476815668, -0.09367644605861808, 0.07625011241444471, 0.31165481748228724, -0.2710209521888332, -0.1899020515636287, 0.057477245583537624, -0.23939532244747336, -0.13588325514204122, 0.1283516547727314, -0.02198871917260641... |
708.0357 | Analysis of Coulomb breakup experiments of 8B with a dynamical eikonal
approximation | Various measurements of the Coulomb breakup of 8B are analyzed within the
dynamical eikonal approximation using a single description of 8B. We obtain a
good agreement with experiment for different observables measured between 40
and 80 MeV per nucleon. A simple 7Be-p potential model description of 8B seems
sufficient... | nucl-th | various measurements of the coulomb breakup of 8b are analyzed within the dynamical eikonal approximation using a single description of 8b we obtain a good agreement with experiment for different observables measured between 40 and 80 mev per nucleon a simple 7bep potential model description of 8b seems sufficient to d... | [['various', 'measurements', 'of', 'the', 'coulomb', 'breakup', 'of', '8b', 'are', 'analyzed', 'within', 'the', 'dynamical', 'eikonal', 'approximation', 'using', 'a', 'single', 'description', 'of', '8b', 'we', 'obtain', 'a', 'good', 'agreement', 'with', 'experiment', 'for', 'different', 'observables', 'measured', 'betw... | [-0.07610832051917289, 0.14379980498924852, -0.07982826136358198, 0.16830158787488472, 0.005368112940292728, -0.11225323202282501, 0.05281407705624588, 0.33982557541069885, -0.19213217925668383, -0.3440193768357858, -0.05702840724940567, -0.3264680616479988, -0.025933989975601434, 0.18024766569530282, 0.026985424483427... |
708.0358 | Entanglement, BEC, and superfluid-like behavior of two-mode photon
systems | A system of two interacting photon modes, without constraints on the photon
number, in the presence of a Kerr nonlinearity, exhibits BEC if the transfer
amplitude is greater than the mode frequency. A symmetry-breaking field (SBF)
can be introduced by taking into account a classical electron current. The
ground state... | quant-ph | a system of two interacting photon modes without constraints on the photon number in the presence of a kerr nonlinearity exhibits bec if the transfer amplitude is greater than the mode frequency a symmetrybreaking field sbf can be introduced by taking into account a classical electron current the ground state in the li... | [['a', 'system', 'of', 'two', 'interacting', 'photon', 'modes', 'without', 'constraints', 'on', 'the', 'photon', 'number', 'in', 'the', 'presence', 'of', 'a', 'kerr', 'nonlinearity', 'exhibits', 'bec', 'if', 'the', 'transfer', 'amplitude', 'is', 'greater', 'than', 'the', 'mode', 'frequency', 'a', 'symmetrybreaking', 'f... | [-0.17777348926485798, 0.22780203691229328, -0.11202480226697385, 0.05013837198665467, -0.028019236083063045, -0.10774355208096925, 0.011342824238186429, 0.2955673461375657, -0.21173370277956705, -0.2313300606816314, 0.08979136408613489, -0.27301572081308034, -0.05087687594946041, 0.23797452155240748, 0.004790905509288... |
708.0359 | Geometric proof of Thom conjecture | This paper has been withdrawn by the author due a crucial sign error in
Theorem B. We present a geometric proof of Thom conjecture, which uses Khovanov
homology. Our approach doesn't use any analytic methods and is quite different
from proof given by Kronheimer and Mrowka in 1994.
| math.GT | this paper has been withdrawn by the author due a crucial sign error in theorem b we present a geometric proof of thom conjecture which uses khovanov homology our approach doesnt use any analytic methods and is quite different from proof given by kronheimer and mrowka in 1994 | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'author', 'due', 'a', 'crucial', 'sign', 'error', 'in', 'theorem', 'b', 'we', 'present', 'a', 'geometric', 'proof', 'of', 'thom', 'conjecture', 'which', 'uses', 'khovanov', 'homology', 'our', 'approach', 'doesnt', 'use', 'any', 'analytic', 'methods', 'and', 'i... | [-0.13351607920291522, -0.02885851010796614, -0.22046761447563767, 0.05647085780704705, -0.11905194073915482, -0.1825218327382269, 0.02754864529075955, 0.2914925408549607, -0.2490274440885211, -0.3245577646885067, 0.07150915164675098, -0.1747664103313582, -0.25054209551308304, 0.1603212656142811, -0.27991665721250075, ... |
708.036 | The generalized matrix valued hypergeometric equation | The matrix valued analog of the Euler's hypergeometric differential equation
was introduced by Tirao in \cite{T2}. This equation arises in the study of
matrix valued spherical functions and in the theory of matrix valued orthogonal
polynomials. The goal of this paper is to extend naturally the number of
parameters of... | math-ph math.MP math.RT | the matrix valued analog of the eulers hypergeometric differential equation was introduced by tirao in citet2 this equation arises in the study of matrix valued spherical functions and in the theory of matrix valued orthogonal polynomials the goal of this paper is to extend naturally the number of parameters of tiraos ... | [['the', 'matrix', 'valued', 'analog', 'of', 'the', 'eulers', 'hypergeometric', 'differential', 'equation', 'was', 'introduced', 'by', 'tirao', 'in', 'citet2', 'this', 'equation', 'arises', 'in', 'the', 'study', 'of', 'matrix', 'valued', 'spherical', 'functions', 'and', 'in', 'the', 'theory', 'of', 'matrix', 'valued', ... | [-0.12362026161281392, 0.0480365109162029, -0.10493946471251547, 0.08098272205769227, -0.09122379732658513, -0.08154165154645363, 0.009627646663620208, 0.2977884859742167, -0.2863584117372878, -0.1930243027790521, 0.08500166233212579, -0.25429610537069564, -0.2155402378859715, 0.16807706916454032, -0.07054412741574477,... |
708.0361 | Why the relational data model can be considered as a formal basis for
group operations in object-oriented systems | Relational data model defines a specification of a type "relation". However,
its simplicity does not mean that the system implementing this model must
operate with structures having the same simplicity. We consider two principles
allowing create a system which combines object-oriented paradigm (OOP) and
relational da... | cs.DB | relational data model defines a specification of a type relation however its simplicity does not mean that the system implementing this model must operate with structures having the same simplicity we consider two principles allowing create a system which combines objectoriented paradigm oop and relational data model r... | [['relational', 'data', 'model', 'defines', 'a', 'specification', 'of', 'a', 'type', 'relation', 'however', 'its', 'simplicity', 'does', 'not', 'mean', 'that', 'the', 'system', 'implementing', 'this', 'model', 'must', 'operate', 'with', 'structures', 'having', 'the', 'same', 'simplicity', 'we', 'consider', 'two', 'prin... | [-0.12537232168688206, 0.04709987501701107, -0.06856489360507112, 0.08491070737090922, -0.11179751673989813, -0.13201671628849, 0.04593666987057077, 0.3370643167218077, -0.3163718742252968, -0.3523038061975967, 0.11547434559179237, -0.2666678028763272, -0.12402656222911901, 0.17812110030536132, -0.06920057511888444, 0.... |
708.0362 | On the Statistical Modeling and Analysis of Repairable Systems | We review basic modeling approaches for failure and maintenance data from
repairable systems. In particular we consider imperfect repair models, defined
in terms of virtual age processes, and the trend-renewal process which extends
the nonhomogeneous Poisson process and the renewal process. In the case where
several ... | stat.ME | we review basic modeling approaches for failure and maintenance data from repairable systems in particular we consider imperfect repair models defined in terms of virtual age processes and the trendrenewal process which extends the nonhomogeneous poisson process and the renewal process in the case where several systems... | [['we', 'review', 'basic', 'modeling', 'approaches', 'for', 'failure', 'and', 'maintenance', 'data', 'from', 'repairable', 'systems', 'in', 'particular', 'we', 'consider', 'imperfect', 'repair', 'models', 'defined', 'in', 'terms', 'of', 'virtual', 'age', 'processes', 'and', 'the', 'trendrenewal', 'process', 'which', 'e... | [-0.10047131621727853, 0.0713054641083415, -0.03837384510885126, 0.09462193039340232, -0.045156702492386104, -0.10220487791313125, 0.07031530894788116, 0.3794666053195085, -0.25798236451976536, -0.2877963567884373, 0.1314895414705721, -0.276007151041579, -0.1712105776224884, 0.17930481792760214, -0.10484241620371385, 0... |
708.0363 | Cohomology and deformations of the infinite dimensional filiform Lie
algebra m_2 | Denote $\fm_2$ the infinite dimensional $\N$-graded Lie algebra defined by
the basis $e_i$ for $i\geq 1$ and by relations $[e_1,e_i]=e_{i+1}$ for all
$i\geq 2$, $[e_2,e_j]=e_{j+2}$ for all $j\geq 3$. We compute in this article
the bracket structure on $H^1(\fm_2,\fm_2)$, $H^2(\fm_2,\fm_2)$ and in relation
to this, we... | math.RT math.RA | denote fm_2 the infinite dimensional ngraded lie algebra defined by the basis e_i for igeq 1 and by relations e_1e_ie_i1 for all igeq 2 e_2e_je_j2 for all jgeq 3 we compute in this article the bracket structure on h1fm_2fm_2 h2fm_2fm_2 and in relation to this we establish that there are only finitely many true deformat... | [['denote', 'fm_2', 'the', 'infinite', 'dimensional', 'ngraded', 'lie', 'algebra', 'defined', 'by', 'the', 'basis', 'e_i', 'for', 'igeq', '1', 'and', 'by', 'relations', 'e_1e_ie_i1', 'for', 'all', 'igeq', '2', 'e_2e_je_j2', 'for', 'all', 'jgeq', '3', 'we', 'compute', 'in', 'this', 'article', 'the', 'bracket', 'structur... | [-0.16653778048184437, 0.1376329026519297, -0.024217314579380818, 0.0644322441240104, -0.05249431737674735, -0.1825640946149062, -0.0177274965084134, 0.3722151953440446, -0.3334365065376728, -0.2049294548252454, 0.1083043388222368, -0.26247791580569285, -0.15597498240188146, 0.1770150194135614, -0.04439911826585348, -0... |
708.0364 | The typical behaviour of relays | The typical behaviour of the relay-without-delay channel and its many-units
generalisation, termed the relay array, under LDPC coding, is studied using
methods of statistical mechanics. A demodulate-and-forward strategy is
analytically solved using the replica symmetric ansatz which is exact in the
studied system at ... | cond-mat.stat-mech cond-mat.other | the typical behaviour of the relaywithoutdelay channel and its manyunits generalisation termed the relay array under ldpc coding is studied using methods of statistical mechanics a demodulateandforward strategy is analytically solved using the replica symmetric ansatz which is exact in the studied system at the nishimo... | [['the', 'typical', 'behaviour', 'of', 'the', 'relaywithoutdelay', 'channel', 'and', 'its', 'manyunits', 'generalisation', 'termed', 'the', 'relay', 'array', 'under', 'ldpc', 'coding', 'is', 'studied', 'using', 'methods', 'of', 'statistical', 'mechanics', 'a', 'demodulateandforward', 'strategy', 'is', 'analytically', '... | [-0.22219751822322764, 0.0438776070737398, -0.06496513428323915, 0.030737270214135796, 0.021094635109299084, -0.24109234473287638, 0.08325209218720106, 0.3539327417670841, -0.25197730635122306, -0.25679875457738066, 0.10870245789689287, -0.22992471210547055, -0.1646389667941651, 0.14044860060471046, -0.0639316209159057... |
708.0365 | Uncollapsing the wavefunction | The undoing of quantum measurements is discussed in the broader context of
irreversibility in physics. We give explicit examples of how a wavefunction can
be uncollapsed in two solid-state experimental set-ups. Wavefunction uncollapse
shows the quantum observer paradox in a new and significantly clearer way.
| quant-ph cond-mat.mes-hall | the undoing of quantum measurements is discussed in the broader context of irreversibility in physics we give explicit examples of how a wavefunction can be uncollapsed in two solidstate experimental setups wavefunction uncollapse shows the quantum observer paradox in a new and significantly clearer way | [['the', 'undoing', 'of', 'quantum', 'measurements', 'is', 'discussed', 'in', 'the', 'broader', 'context', 'of', 'irreversibility', 'in', 'physics', 'we', 'give', 'explicit', 'examples', 'of', 'how', 'a', 'wavefunction', 'can', 'be', 'uncollapsed', 'in', 'two', 'solidstate', 'experimental', 'setups', 'wavefunction', 'u... | [-0.09933520123983423, 0.18431703355163337, -0.1526778457686305, 0.11133493025942395, -0.0629092738756703, -0.1674261251464486, 0.03134638889589243, 0.3558042405380143, -0.21958040425346959, -0.2773210585945182, 0.014654071380694708, -0.24408462655006183, -0.14365182183682917, 0.25887077624599136, -0.09042798438005978,... |
708.0366 | Tachyon solutions in boundary and cubic string field theory | We construct rolling tachyon solutions of open and boundary string field
theory (OSFT and BSFT, respectively), in the bosonic and supersymmetric (susy)
case. The wildly oscillating solution of susy OSFT is recovered, together with
a family of time-dependent BSFT solutions for the bosonic and susy string.
These are pa... | hep-th math-ph math.MP | we construct rolling tachyon solutions of open and boundary string field theory osft and bsft respectively in the bosonic and supersymmetric susy case the wildly oscillating solution of susy osft is recovered together with a family of timedependent bsft solutions for the bosonic and susy string these are parametrized b... | [['we', 'construct', 'rolling', 'tachyon', 'solutions', 'of', 'open', 'and', 'boundary', 'string', 'field', 'theory', 'osft', 'and', 'bsft', 'respectively', 'in', 'the', 'bosonic', 'and', 'supersymmetric', 'susy', 'case', 'the', 'wildly', 'oscillating', 'solution', 'of', 'susy', 'osft', 'is', 'recovered', 'together', '... | [-0.1643448883714882, 0.15333387990642677, -0.06898172345518105, 0.09191941931112524, -0.05281539545649139, -0.20655851957053528, -0.022298132968899154, 0.28598196435632417, -0.21581938231975073, -0.24963660293724388, 0.12180816793897975, -0.2682640166749479, -0.1593520119022287, 0.17124326631892473, -0.059700353667722... |
708.0367 | Surprising Evolution of Faraday Rotation Gradients in the Jet of
1803+784 | Several multi-frequency polarization studies have shown the presence of
systematic Faraday Rotation gradients across the parsec-scale jets of Active
Galactic Nuclei (AGN), taken to be due to the systematic variation of the
line-of-sight component of a helical magnetic field across the jet. Other
studies have confirme... | astro-ph | several multifrequency polarization studies have shown the presence of systematic faraday rotation gradients across the parsecscale jets of active galactic nuclei agn taken to be due to the systematic variation of the lineofsight component of a helical magnetic field across the jet other studies have confirmed the pres... | [['several', 'multifrequency', 'polarization', 'studies', 'have', 'shown', 'the', 'presence', 'of', 'systematic', 'faraday', 'rotation', 'gradients', 'across', 'the', 'parsecscale', 'jets', 'of', 'active', 'galactic', 'nuclei', 'agn', 'taken', 'to', 'be', 'due', 'to', 'the', 'systematic', 'variation', 'of', 'the', 'lin... | [-0.12937004294844467, 0.13721527979794304, -0.07993715283399458, 0.06730453203595362, -0.08970210917511491, -0.04504202392075192, 0.0029469171827328083, 0.44124387350254857, -0.2532990720409068, -0.33476803456799503, 0.08449810854842423, -0.24212800647099006, -0.04372768397419359, 0.2100505948389956, -0.00516300880099... |
708.0368 | Dynamics of Opinions and Social Structures | Social groups with widely different music tastes, political convictions, and
religious beliefs emerge and disappear on scales from extreme subcultures to
mainstream mass-cultures. Both the underlying social structure and the
formation of opinions are dynamic and changes in one affect the other. Several
positive feedb... | physics.soc-ph | social groups with widely different music tastes political convictions and religious beliefs emerge and disappear on scales from extreme subcultures to mainstream masscultures both the underlying social structure and the formation of opinions are dynamic and changes in one affect the other several positive feedback mec... | [['social', 'groups', 'with', 'widely', 'different', 'music', 'tastes', 'political', 'convictions', 'and', 'religious', 'beliefs', 'emerge', 'and', 'disappear', 'on', 'scales', 'from', 'extreme', 'subcultures', 'to', 'mainstream', 'masscultures', 'both', 'the', 'underlying', 'social', 'structure', 'and', 'the', 'format... | [-0.12098925202770765, 0.11072717655130314, -0.08963486379298595, 0.11974841902938571, -0.16897066605995487, -0.1092443302672087, 0.06854463481843606, 0.4394881919486426, -0.30209540141499547, -0.33895489845020943, 0.07134895258111856, -0.2957373932003975, -0.2687223855415163, 0.1009708198561636, -0.05756980675295085, ... |
708.0369 | A Review of Accelerated Test Models | Engineers in the manufacturing industries have used accelerated test (AT)
experiments for many decades. The purpose of AT experiments is to acquire
reliability information quickly. Test units of a material, component, subsystem
or entire systems are subjected to higher-than-usual levels of one or more
accelerating va... | stat.ME | engineers in the manufacturing industries have used accelerated test at experiments for many decades the purpose of at experiments is to acquire reliability information quickly test units of a material component subsystem or entire systems are subjected to higherthanusual levels of one or more accelerating variables su... | [['engineers', 'in', 'the', 'manufacturing', 'industries', 'have', 'used', 'accelerated', 'test', 'at', 'experiments', 'for', 'many', 'decades', 'the', 'purpose', 'of', 'at', 'experiments', 'is', 'to', 'acquire', 'reliability', 'information', 'quickly', 'test', 'units', 'of', 'a', 'material', 'component', 'subsystem', ... | [-0.04629748384909225, 0.07951053225251874, -0.0840084773660026, 0.06452088255665707, -0.039620902385760215, -0.1263096404210147, 0.043837596119659004, 0.3912701743344466, -0.23878761066707097, -0.354835586090845, 0.14239647955283277, -0.258697113614868, -0.08436806040058721, 0.217505971401356, -0.046849451138346335, 0... |
708.037 | A modified Next Reaction Method for simulating chemical systems with
time dependent propensities and delays | Chemical reaction systems with a low to moderate number of molecules are
typically modeled as discrete jump Markov processes. These systems are
oftentimes simulated with methods that produce statistically exact sample paths
such as the Gillespie Algorithm or the Next Reaction Method. In this paper we
make explicit us... | q-bio.MN q-bio.QM | chemical reaction systems with a low to moderate number of molecules are typically modeled as discrete jump markov processes these systems are oftentimes simulated with methods that produce statistically exact sample paths such as the gillespie algorithm or the next reaction method in this paper we make explicit use of... | [['chemical', 'reaction', 'systems', 'with', 'a', 'low', 'to', 'moderate', 'number', 'of', 'molecules', 'are', 'typically', 'modeled', 'as', 'discrete', 'jump', 'markov', 'processes', 'these', 'systems', 'are', 'oftentimes', 'simulated', 'with', 'methods', 'that', 'produce', 'statistically', 'exact', 'sample', 'paths',... | [-0.06637201065955273, 0.0963218063037148, -0.05002799379847494, 0.046537431767920696, -0.010658605902266326, -0.11837595295539852, 0.0787724577392633, 0.4316960720155956, -0.2811558569398693, -0.31885652187264574, 0.08663007788462722, -0.23340256671989495, -0.1614161759429469, 0.21480410541328837, -0.00937863215961951... |
708.0371 | Spectral Analysis of a Two Body Problem with Zero Range Perturbation | We consider a class of singular, zero-range perturbations of the Hamiltonian
of a quantum system composed by a test particle and a harmonic oscillators in
dimension one, two and three and we study its spectrum. In facts we give a
detailed characterization of point spectrum and its asymptotic behavior with
respect to ... | math-ph math.MP | we consider a class of singular zerorange perturbations of the hamiltonian of a quantum system composed by a test particle and a harmonic oscillators in dimension one two and three and we study its spectrum in facts we give a detailed characterization of point spectrum and its asymptotic behavior with respect to the pa... | [['we', 'consider', 'a', 'class', 'of', 'singular', 'zerorange', 'perturbations', 'of', 'the', 'hamiltonian', 'of', 'a', 'quantum', 'system', 'composed', 'by', 'a', 'test', 'particle', 'and', 'a', 'harmonic', 'oscillators', 'in', 'dimension', 'one', 'two', 'and', 'three', 'and', 'we', 'study', 'its', 'spectrum', 'in', ... | [-0.17246186937471586, 0.13839662337143507, -0.0981187867000699, 0.03367612533537405, -0.012268591865098903, -0.11626989574703787, 0.017796718838092473, 0.31861784931804454, -0.23635690132422107, -0.24058235375227274, 0.09240664362774363, -0.32390324478702887, -0.17565833646804094, 0.17816589542032618, 0.01290369941187... |
708.0372 | Interoccurrence time statistics in the two-dimensional Burridge-Knopoff
earthquake model | We have numerically investigated statistical properties of the so-called
interoccurrence time or the waiting time, i.e., the time interval between
successive earthquakes, based on the two-dimensional (2-D) spring-block
(Burridge-Knopoff) model, selecting the velocity-weakening property as the
constitutive friction la... | cond-mat.stat-mech | we have numerically investigated statistical properties of the socalled interoccurrence time or the waiting time ie the time interval between successive earthquakes based on the twodimensional 2d springblock burridgeknopoff model selecting the velocityweakening property as the constitutive friction law the statistical ... | [['we', 'have', 'numerically', 'investigated', 'statistical', 'properties', 'of', 'the', 'socalled', 'interoccurrence', 'time', 'or', 'the', 'waiting', 'time', 'ie', 'the', 'time', 'interval', 'between', 'successive', 'earthquakes', 'based', 'on', 'the', 'twodimensional', '2d', 'springblock', 'burridgeknopoff', 'model'... | [-0.10190194965409818, 0.14284362271442375, -0.14289091229804007, 0.10668638088275781, -0.026272218507787614, -0.09302454209925297, 0.03176907995343665, 0.3577465616422249, -0.27924341743118036, -0.31383420163582937, 0.07251274817241996, -0.261766600911049, -0.14715024868949994, 0.2008520351693162, -0.02616964044179493... |
708.0373 | Solutions of Higher Dimensional Gauss-Bonnet FRW Cosmology | We examine the effect on cosmological evolution of adding a Gauss-Bonnet term
to the standard Einstein-Hilbert action for a (1 + 3)+ d dimensional
Friedman-Robertson-Walker (FRW) metric. By assuming that the additional
dimensions compactify as a power law as the usual 3 spatial dimensions expand,
we solve the resulti... | gr-qc hep-th | we examine the effect on cosmological evolution of adding a gaussbonnet term to the standard einsteinhilbert action for a 1 3 d dimensional friedmanrobertsonwalker frw metric by assuming that the additional dimensions compactify as a power law as the usual 3 spatial dimensions expand we solve the resulting dynamical eq... | [['we', 'examine', 'the', 'effect', 'on', 'cosmological', 'evolution', 'of', 'adding', 'a', 'gaussbonnet', 'term', 'to', 'the', 'standard', 'einsteinhilbert', 'action', 'for', 'a', '1', '3', 'd', 'dimensional', 'friedmanrobertsonwalker', 'frw', 'metric', 'by', 'assuming', 'that', 'the', 'additional', 'dimensions', 'com... | [-0.15756754692643882, 0.12099743359722197, -0.09238925995926062, 0.08748083903143804, -0.13603254030148187, -0.18827766520436853, -0.04968048691749573, 0.2314050191640854, -0.22320673532783986, -0.26938675871739787, 0.10730846180270115, -0.27907406104107696, -0.1440805888051788, 0.08450289726878206, -0.023038482721894... |
708.0374 | Equilibrium states for potentials with $\sup\phi - \inf\phi < \htop(f)$ | In the context of smooth interval maps, we study an inducing scheme approach
to prove existence and uniqueness of equilibrium states for potentials $\phi$
with he `bounded range' condition $\sup \phi - \inf \phi < \htop$, first used
by Hofbauer and Keller. We compare our results to Hofbauer and Keller's use of
Perron... | math.DS | in the context of smooth interval maps we study an inducing scheme approach to prove existence and uniqueness of equilibrium states for potentials phi with he bounded range condition sup phi inf phi htop first used by hofbauer and keller we compare our results to hofbauer and kellers use of perronfrobenius operators we... | [['in', 'the', 'context', 'of', 'smooth', 'interval', 'maps', 'we', 'study', 'an', 'inducing', 'scheme', 'approach', 'to', 'prove', 'existence', 'and', 'uniqueness', 'of', 'equilibrium', 'states', 'for', 'potentials', 'phi', 'with', 'he', 'bounded', 'range', 'condition', 'sup', 'phi', 'inf', 'phi', 'htop', 'first', 'us... | [-0.11372507188934833, 0.06185086257337389, -0.08964590100513306, 0.06853225014056079, -0.024645741636049934, -0.12437527980655431, 0.016359622252639382, 0.3703590862569399, -0.298959075496532, -0.20473913215100764, 0.11197183940967079, -0.24465015043970198, -0.16072591049596668, 0.18305389286542778, -0.096539541007950... |
708.0375 | Controlled enhancement or suppression of exchange biasing using impurity
$\delta$-layers | The effects of inserting impurity $\delta$-layers of various elements into a
Co/IrMn exchange biased bilayer, at both the interface, and at given points
within the IrMn layer a distance from the interface, has been investigated.
Depending on the chemical species of dopant, and its position, we found that
the exchange... | cond-mat.other cond-mat.mtrl-sci | the effects of inserting impurity deltalayers of various elements into a coirmn exchange biased bilayer at both the interface and at given points within the irmn layer a distance from the interface has been investigated depending on the chemical species of dopant and its position we found that the exchange biasing can ... | [['the', 'effects', 'of', 'inserting', 'impurity', 'deltalayers', 'of', 'various', 'elements', 'into', 'a', 'coirmn', 'exchange', 'biased', 'bilayer', 'at', 'both', 'the', 'interface', 'and', 'at', 'given', 'points', 'within', 'the', 'irmn', 'layer', 'a', 'distance', 'from', 'the', 'interface', 'has', 'been', 'investig... | [-0.15694795540825984, 0.19633730673783664, -0.043204143027759205, 0.011576089757431489, -0.018358027051455516, -0.1636985053182027, 0.07656003589449861, 0.3832573605606617, -0.3162845450027262, -0.3006742062378612, 0.052932426076919094, -0.3161584833889442, -0.0871289063608116, 0.12936031449215202, 0.06936577886887589... |
708.0376 | Observation of the Decay B+ --> K+K-pi+ | We report the observation of charmless hadronic decays of charged B mesons to
the final state K+K-pi+. Using a data sample of 347.5 fb^-1 collected at the
Y(4S) resonance with the BABAR detector, we observe 429+/-43 signal events with
a significance of 9.6 sigma. We measure the inclusive branching fraction BF(B+
--> ... | hep-ex | we report the observation of charmless hadronic decays of charged b mesons to the final state kkpi using a data sample of 3475 fb1 collected at the y4s resonance with the babar detector we observe 42943 signal events with a significance of 96 sigma we measure the inclusive branching fraction bfb kkpi 5005stat05systx106... | [['we', 'report', 'the', 'observation', 'of', 'charmless', 'hadronic', 'decays', 'of', 'charged', 'b', 'mesons', 'to', 'the', 'final', 'state', 'kkpi', 'using', 'a', 'data', 'sample', 'of', '3475', 'fb1', 'collected', 'at', 'the', 'y4s', 'resonance', 'with', 'the', 'babar', 'detector', 'we', 'observe', '42943', 'signal... | [-0.10445759223754673, 0.17895486429777174, -0.1156659010919698, 0.08710043570248499, -0.06465864445393284, -0.09062290684475253, 0.13632461548245156, 0.2936543512235706, -0.13814387825273333, -0.30852978696514455, -0.05242016382232707, -0.44208517416180776, 0.058080895726258554, 0.0954284554131196, 0.11247829325674545... |
708.0377 | Incorporating postleap checks in tau-leaping | By explicitly representing the reaction times of discrete chemical systems as
the firing times of independent, unit rate Poisson processes, we develop a new
adaptive tau-leaping procedure. The procedure developed is novel in that
accuracy is guaranteed by performing postleap checks. Because the
representation we use ... | q-bio.MN q-bio.QM | by explicitly representing the reaction times of discrete chemical systems as the firing times of independent unit rate poisson processes we develop a new adaptive tauleaping procedure the procedure developed is novel in that accuracy is guaranteed by performing postleap checks because the representation we use separat... | [['by', 'explicitly', 'representing', 'the', 'reaction', 'times', 'of', 'discrete', 'chemical', 'systems', 'as', 'the', 'firing', 'times', 'of', 'independent', 'unit', 'rate', 'poisson', 'processes', 'we', 'develop', 'a', 'new', 'adaptive', 'tauleaping', 'procedure', 'the', 'procedure', 'developed', 'is', 'novel', 'in'... | [-0.09912279601253214, 0.09505007433749381, -0.11349166846595748, 0.041310460686994094, -0.030374528574092046, -0.1278822688696285, 0.11540463916247799, 0.35850350919977897, -0.2600278718707462, -0.2948955287447288, 0.09948764460915256, -0.2191217504064774, -0.14622385008704095, 0.1907304495905659, -0.07626554524703395... |
708.0378 | A Conversation With Harry Martz | Harry F. Martz was born June 16, 1942 and grew up in Cumberland, Maryland. He
received a Bachelor of Science degree in mathematics (with a minor in physics)
from Frostburg State University in 1964, and earned a Ph.D. in statistics at
Virginia Polytechnic Institute and State University in 1968. He started his
statisti... | stat.ME | harry f martz was born june 16 1942 and grew up in cumberland maryland he received a bachelor of science degree in mathematics with a minor in physics from frostburg state university in 1964 and earned a phd in statistics at virginia polytechnic institute and state university in 1968 he started his statistics career at... | [['harry', 'f', 'martz', 'was', 'born', 'june', '16', '1942', 'and', 'grew', 'up', 'in', 'cumberland', 'maryland', 'he', 'received', 'a', 'bachelor', 'of', 'science', 'degree', 'in', 'mathematics', 'with', 'a', 'minor', 'in', 'physics', 'from', 'frostburg', 'state', 'university', 'in', '1964', 'and', 'earned', 'a', 'ph... | [0.005349186256546444, 0.09696436485837613, -0.13575236413079783, 0.008960119723156919, -0.11107236741366178, -0.1585945471362994, 0.07159757837127746, 0.2655792363941983, -0.10651279900846818, -0.4122018271060949, 0.07296904975721465, -0.3645973463936305, -0.02855037525502256, 0.21181290663069988, -0.15297252038056938... |
708.0379 | Return time statistics for invariant measures for interval maps with
positive Lyapunov exponent | We prove that multimodal maps with an absolutely continuous invariant measure
have exponential return time statistics around a.e. point. We also show a
`polynomial Gibbs property' for these systems, and that the convergence to the
entropy in the Ornstein-Weiss formula has normal fluctuations. These results
are also p... | math.DS | we prove that multimodal maps with an absolutely continuous invariant measure have exponential return time statistics around ae point we also show a polynomial gibbs property for these systems and that the convergence to the entropy in the ornsteinweiss formula has normal fluctuations these results are also proved for ... | [['we', 'prove', 'that', 'multimodal', 'maps', 'with', 'an', 'absolutely', 'continuous', 'invariant', 'measure', 'have', 'exponential', 'return', 'time', 'statistics', 'around', 'ae', 'point', 'we', 'also', 'show', 'a', 'polynomial', 'gibbs', 'property', 'for', 'these', 'systems', 'and', 'that', 'the', 'convergence', '... | [-0.09269356959584084, 0.13366540166025515, -0.21393516579304228, 0.11764530390501023, 0.039001193591816856, -0.13300620306452568, 0.01751149743795395, 0.40530055768110534, -0.31628923104567963, -0.16134809498590502, 0.1187080437634987, -0.31238347149708057, -0.13816562396558849, 0.19242971517484297, -0.085938920097594... |
708.038 | Propagation of Fluctuations in Biochemical Systems, II: Nonlinear Chains | We consider biochemical reaction chains and investigate how random external
fluctuations, as characterized by variance and coefficient of variation,
propagate down the chains. We perform such a study under the assumption that
the number of molecules is high enough so that the behavior of the
concentrations of the sys... | math.PR math.DS | we consider biochemical reaction chains and investigate how random external fluctuations as characterized by variance and coefficient of variation propagate down the chains we perform such a study under the assumption that the number of molecules is high enough so that the behavior of the concentrations of the system i... | [['we', 'consider', 'biochemical', 'reaction', 'chains', 'and', 'investigate', 'how', 'random', 'external', 'fluctuations', 'as', 'characterized', 'by', 'variance', 'and', 'coefficient', 'of', 'variation', 'propagate', 'down', 'the', 'chains', 'we', 'perform', 'such', 'a', 'study', 'under', 'the', 'assumption', 'that',... | [-0.1405600184735296, 0.17618382635118907, -0.0671089590773998, 0.07932588037280044, 0.016726952524663045, -0.09640284780862517, 0.05999089905847635, 0.3491400004203977, -0.29471191884628656, -0.292483990167364, 0.1146602036495661, -0.2791399792029426, -0.1463058806441981, 0.17031401182235828, 0.014077846471477171, 0.0... |
708.0381 | On Sumsets and Spectral Gaps | It is well known that if S is a subset of the integers mod p, and if the
second-largest Fourier coefficient is ``small'' relative to the largest
coefficient, then the sumset S+S is much larger than S. We show in the present
paper that if instead of having such a large ``spectral gap'' between the
largest and second-l... | math.CO math.NT | it is well known that if s is a subset of the integers mod p and if the secondlargest fourier coefficient is small relative to the largest coefficient then the sumset ss is much larger than s we show in the present paper that if instead of having such a large spectral gap between the largest and secondlargest fourier c... | [['it', 'is', 'well', 'known', 'that', 'if', 's', 'is', 'a', 'subset', 'of', 'the', 'integers', 'mod', 'p', 'and', 'if', 'the', 'secondlargest', 'fourier', 'coefficient', 'is', 'small', 'relative', 'to', 'the', 'largest', 'coefficient', 'then', 'the', 'sumset', 'ss', 'is', 'much', 'larger', 'than', 's', 'we', 'show', '... | [-0.1319412777446531, 0.12548012525839425, -0.06959202087133146, 0.08129288392431545, -0.06063772667749006, -0.13731706148532571, 0.0247471853508614, 0.34231381410290107, -0.27151717680704884, -0.27299138589869026, 0.10199795874335696, -0.3281358133039636, -0.15209891736224965, 0.21479700372810093, -0.03504896839149296... |
708.0382 | Broken-Symmetry States of Dirac Fermions in Graphene with A Partially
Filled High Landau Level | We report on numerical study of the Dirac fermions in partially filled N=3
Landau level (LL) in graphene. At half-filling, the equal-time density-density
correlation function displays sharp peaks at nonzero wavevectors $\pm {\bf
q^{*}}$. Finite-size scaling shows that the peak value grows with electron
number and div... | cond-mat.str-el cond-mat.mes-hall | we report on numerical study of the dirac fermions in partially filled n3 landau level ll in graphene at halffilling the equaltime densitydensity correlation function displays sharp peaks at nonzero wavevectors pm bf q finitesize scaling shows that the peak value grows with electron number and diverges in the thermodyn... | [['we', 'report', 'on', 'numerical', 'study', 'of', 'the', 'dirac', 'fermions', 'in', 'partially', 'filled', 'n3', 'landau', 'level', 'll', 'in', 'graphene', 'at', 'halffilling', 'the', 'equaltime', 'densitydensity', 'correlation', 'function', 'displays', 'sharp', 'peaks', 'at', 'nonzero', 'wavevectors', 'pm', 'bf', 'q... | [-0.22182565041810215, 0.26025321886880837, -0.04799538949925092, 0.05124155283180786, 0.018159929704251548, -0.1655904479858075, 0.08224816676679879, 0.3172317469462512, -0.1979342096319963, -0.23716633358309347, 0.007221129857146392, -0.3798023209054654, -0.10639431812770424, 0.10434823363809095, 0.0934051514054919, ... |
708.0383 | Supersymmetric Models with Higher Dimensional Operators | In 4D renormalisable theories, integrating out massive states generates in
the low energy effective action higher dimensional operators (derivative or
otherwise). Using a superfield language it is shown that a 4D N=1
supersymmetric theory with higher derivative operators in either the Kahler or
the superpotential par... | hep-th hep-ph | in 4d renormalisable theories integrating out massive states generates in the low energy effective action higher dimensional operators derivative or otherwise using a superfield language it is shown that a 4d n1 supersymmetric theory with higher derivative operators in either the kahler or the superpotential part of th... | [['in', '4d', 'renormalisable', 'theories', 'integrating', 'out', 'massive', 'states', 'generates', 'in', 'the', 'low', 'energy', 'effective', 'action', 'higher', 'dimensional', 'operators', 'derivative', 'or', 'otherwise', 'using', 'a', 'superfield', 'language', 'it', 'is', 'shown', 'that', 'a', '4d', 'n1', 'supersymm... | [-0.12782840577503002, 0.18371964846301125, -0.022510341641538284, 0.11994722173537356, -0.10220282392490808, -0.1600305197299553, -0.017120241390051777, 0.3038637674442131, -0.20068402600959323, -0.2953670595675156, 0.10981325135561543, -0.28056490381618926, -0.14476456649468414, 0.08277662339316187, -0.01815105266263... |
708.0384 | Decoherence in adiabatic quantum computation | We have studied the decoherence properties of adiabatic quantum computation
(AQC) in the presence of in general non-Markovian, e.g., low-frequency, noise.
The developed description of the incoherent Landau-Zener transitions shows that
the global AQC maintains its properties even for decoherence larger than the
minimu... | cond-mat.mes-hall quant-ph | we have studied the decoherence properties of adiabatic quantum computation aqc in the presence of in general nonmarkovian eg lowfrequency noise the developed description of the incoherent landauzener transitions shows that the global aqc maintains its properties even for decoherence larger than the minimum gap at the ... | [['we', 'have', 'studied', 'the', 'decoherence', 'properties', 'of', 'adiabatic', 'quantum', 'computation', 'aqc', 'in', 'the', 'presence', 'of', 'in', 'general', 'nonmarkovian', 'eg', 'lowfrequency', 'noise', 'the', 'developed', 'description', 'of', 'the', 'incoherent', 'landauzener', 'transitions', 'shows', 'that', '... | [-0.18838534424844744, 0.15145886407267378, -0.052570898642705886, 0.07535696743997101, 0.044474007028932734, -0.13461594671951896, 0.07974600241538714, 0.3250715281771131, -0.2469754988932502, -0.33431985611864123, 0.05275412584227731, -0.22001842682048217, -0.08546405569794252, 0.1951044869234728, -0.0249344605902094... |
708.0385 | Tree-structured regression and the differentiation of integrals | This paper provides answers to questions regarding the almost sure limiting
behavior of rooted, binary tree-structured rules for regression. Examples show
that questions raised by Gordon and Olshen in 1984 have negative answers. For
these examples of regression functions and sequences of their associated binary
tree-... | math.ST stat.TH | this paper provides answers to questions regarding the almost sure limiting behavior of rooted binary treestructured rules for regression examples show that questions raised by gordon and olshen in 1984 have negative answers for these examples of regression functions and sequences of their associated binary treestructu... | [['this', 'paper', 'provides', 'answers', 'to', 'questions', 'regarding', 'the', 'almost', 'sure', 'limiting', 'behavior', 'of', 'rooted', 'binary', 'treestructured', 'rules', 'for', 'regression', 'examples', 'show', 'that', 'questions', 'raised', 'by', 'gordon', 'and', 'olshen', 'in', '1984', 'have', 'negative', 'answ... | [-0.0883060743536994, 0.04135096400728546, -0.05655413134981786, 0.1069215272460402, -0.07285583336202352, -0.14067439964536382, 0.08771085385583083, 0.3927773058069924, -0.27127950019983715, -0.2751365760610455, 0.15030144336108506, -0.2882377081490095, -0.1375312670591594, 0.15974835272087054, -0.12035542967725232, 0... |
708.0386 | Diversity of MIMO Multihop Relay Channels | We consider slow fading relay channels with a single multi-antenna
source-destination terminal pair. The source signal arrives at the destination
via N hops through N-1 layers of relays. We analyze the diversity of such
channels with fixed network size at high SNR. In the clustered case where the
relays within the sa... | cs.IT math.IT | we consider slow fading relay channels with a single multiantenna sourcedestination terminal pair the source signal arrives at the destination via n hops through n1 layers of relays we analyze the diversity of such channels with fixed network size at high snr in the clustered case where the relays within the same layer... | [['we', 'consider', 'slow', 'fading', 'relay', 'channels', 'with', 'a', 'single', 'multiantenna', 'sourcedestination', 'terminal', 'pair', 'the', 'source', 'signal', 'arrives', 'at', 'the', 'destination', 'via', 'n', 'hops', 'through', 'n1', 'layers', 'of', 'relays', 'we', 'analyze', 'the', 'diversity', 'of', 'such', '... | [-0.2818760060300216, 0.06093283795053139, -0.05572823198551002, -0.008196409621935649, -0.04929674860128822, -0.26941180458137143, 0.15077806621557102, 0.41406811859536297, -0.29460024444852023, -0.2244299216118331, 0.044050434885139114, -0.2245592690402797, -0.13995621070013536, 0.10316256181298135, -0.08910377555196... |
708.0387 | Analysis of two-point statistics of cosmic shear: III. Covariances of
shear measures made easy | In recent years cosmic shear, the weak gravitational lensing effect by the
large-scale structure of the Universe, has proven to be one of the
observational pillars on which the cosmological concordance model is founded.
Several cosmic shear statistics have been developed in order to analyze data
from surveys. For the... | astro-ph | in recent years cosmic shear the weak gravitational lensing effect by the largescale structure of the universe has proven to be one of the observational pillars on which the cosmological concordance model is founded several cosmic shear statistics have been developed in order to analyze data from surveys for the covari... | [['in', 'recent', 'years', 'cosmic', 'shear', 'the', 'weak', 'gravitational', 'lensing', 'effect', 'by', 'the', 'largescale', 'structure', 'of', 'the', 'universe', 'has', 'proven', 'to', 'be', 'one', 'of', 'the', 'observational', 'pillars', 'on', 'which', 'the', 'cosmological', 'concordance', 'model', 'is', 'founded', ... | [-0.07400840772187606, 0.02789089822973607, -0.09870061573821072, 0.12423022790867204, -0.07122577938854978, -0.06971357713287728, -0.006858904929377802, 0.3664806502263488, -0.22983076668372063, -0.28923060420616453, 0.1043671790181888, -0.25935869636157155, -0.14175021706811958, 0.22943069797672205, -0.02571539049504... |
708.0388 | Generally covariant quantum mechanics on noncommutative configuration
spaces | We generalize the previously given algebraic version of "Feynman's proof of
Maxwell's equations" to noncommutative configuration spaces. By doing so, we
also obtain an axiomatic formulation of nonrelativistic quantum mechanics over
such spaces, which, in contrast to most examples discussed in the literature,
does not... | math-ph math.MP | we generalize the previously given algebraic version of feynmans proof of maxwells equations to noncommutative configuration spaces by doing so we also obtain an axiomatic formulation of nonrelativistic quantum mechanics over such spaces which in contrast to most examples discussed in the literature does not rely on a ... | [['we', 'generalize', 'the', 'previously', 'given', 'algebraic', 'version', 'of', 'feynmans', 'proof', 'of', 'maxwells', 'equations', 'to', 'noncommutative', 'configuration', 'spaces', 'by', 'doing', 'so', 'we', 'also', 'obtain', 'an', 'axiomatic', 'formulation', 'of', 'nonrelativistic', 'quantum', 'mechanics', 'over',... | [-0.12899276297629023, 0.09219582309812652, -0.0866893010142331, 0.08679978158705545, -0.11602959473832296, -0.11353393438128898, 0.005181894951070158, 0.33962595389367867, -0.2270532252296107, -0.2538504858250515, 0.056436361974472396, -0.2570870366628067, -0.1668701808935461, 0.20724096876354173, -0.15196454564843756... |
708.0389 | Hydrogen patterning of Ga1-xMnxAs for planar spintronics | We demonstrate two patterning techniques based on hydrogen passivation of
Ga1-xMnxAs to produce isolated ferromagnetically active regions embedded
uniformly in a paramagnetic, insulating host. The first method consists of
selective hydrogenation of Ga1-xMnxAs by lithographic masking. Magnetotransport
measurements of ... | cond-mat.mtrl-sci | we demonstrate two patterning techniques based on hydrogen passivation of ga1xmnxas to produce isolated ferromagnetically active regions embedded uniformly in a paramagnetic insulating host the first method consists of selective hydrogenation of ga1xmnxas by lithographic masking magnetotransport measurements of hallbar... | [['we', 'demonstrate', 'two', 'patterning', 'techniques', 'based', 'on', 'hydrogen', 'passivation', 'of', 'ga1xmnxas', 'to', 'produce', 'isolated', 'ferromagnetically', 'active', 'regions', 'embedded', 'uniformly', 'in', 'a', 'paramagnetic', 'insulating', 'host', 'the', 'first', 'method', 'consists', 'of', 'selective',... | [-0.12063063882065542, 0.15874897783735034, -0.00883577217870025, -0.08901695774955883, 0.023661523645348622, -0.1572834467317796, 0.05949263041697894, 0.45397643529894677, -0.2728843588456088, -0.34876454195967227, 0.0405642488992519, -0.24897031746804715, -0.1245238816534931, 0.18244671689233546, 0.002169304932943884... |
708.039 | On the maximum bias functions of MM-estimates and constrained
M-estimates of regression | We derive the maximum bias functions of the MM-estimates and the constrained
M-estimates or CM-estimates of regression and compare them to the maximum bias
functions of the S-estimates and the $\tau$-estimates of regression. In these
comparisons, the CM-estimates tend to exhibit the most favorable
bias-robustness pro... | math.ST stat.TH | we derive the maximum bias functions of the mmestimates and the constrained mestimates or cmestimates of regression and compare them to the maximum bias functions of the sestimates and the tauestimates of regression in these comparisons the cmestimates tend to exhibit the most favorable biasrobustness properties also u... | [['we', 'derive', 'the', 'maximum', 'bias', 'functions', 'of', 'the', 'mmestimates', 'and', 'the', 'constrained', 'mestimates', 'or', 'cmestimates', 'of', 'regression', 'and', 'compare', 'them', 'to', 'the', 'maximum', 'bias', 'functions', 'of', 'the', 'sestimates', 'and', 'the', 'tauestimates', 'of', 'regression', 'in... | [-0.06871165012377371, 0.06691149265769823, -0.11607271474843592, 0.11125282249212219, -0.05292700418489583, -0.1182546768234008, 0.034862712738506586, 0.3687067050716759, -0.26399211944684525, -0.2994461093603829, 0.12670865910484191, -0.2760541877352897, -0.13733604064291735, 0.20460557617695518, -0.02312581857125976... |
708.0391 | Seven-color Vilnius photometry of the open cluster NGC 752 | New photoelectric seven-color observations in the Vilnius system are
presented for 65 stars in the region of the open cluster NGC 752. Based on
individual stars with accurate photometric classifications, we determine the
apparent distance modulus (m-M)=8.38 and the mean reddening to the cluster
E(Y-V)=0.027, or E(B-V... | astro-ph | new photoelectric sevencolor observations in the vilnius system are presented for 65 stars in the region of the open cluster ngc 752 based on individual stars with accurate photometric classifications we determine the apparent distance modulus mm838 and the mean reddening to the cluster eyv0027 or ebv0034 the mean phot... | [['new', 'photoelectric', 'sevencolor', 'observations', 'in', 'the', 'vilnius', 'system', 'are', 'presented', 'for', '65', 'stars', 'in', 'the', 'region', 'of', 'the', 'open', 'cluster', 'ngc', '752', 'based', 'on', 'individual', 'stars', 'with', 'accurate', 'photometric', 'classifications', 'we', 'determine', 'the', '... | [-0.004005436900626408, 0.12517360383723183, -0.12564205165925957, 0.0976227016562303, -0.10479729423257575, -0.060774904592721356, 0.12488531364975602, 0.44031043652068363, -0.14390765747913484, -0.3931402622858125, 0.016711046299216954, -0.2992465340773041, -0.0058697283574055585, 0.21936887355385284, -0.132912239939... |
708.0392 | Cancellation of nonrenormalizable hypersurface divergences and the
d-dimensional Casimir piston | Using a multidimensional cut-off technique, we obtain expressions for the
cut-off dependent part of the vacuum energy for parallelepiped geometries in
any spatial dimension d. The cut-off part yields nonrenormalizable hypersurface
divergences and we show explicitly that they cancel in the Casimir piston
scenario in a... | hep-th math-ph math.MP quant-ph | using a multidimensional cutoff technique we obtain expressions for the cutoff dependent part of the vacuum energy for parallelepiped geometries in any spatial dimension d the cutoff part yields nonrenormalizable hypersurface divergences and we show explicitly that they cancel in the casimir piston scenario in all dime... | [['using', 'a', 'multidimensional', 'cutoff', 'technique', 'we', 'obtain', 'expressions', 'for', 'the', 'cutoff', 'dependent', 'part', 'of', 'the', 'vacuum', 'energy', 'for', 'parallelepiped', 'geometries', 'in', 'any', 'spatial', 'dimension', 'd', 'the', 'cutoff', 'part', 'yields', 'nonrenormalizable', 'hypersurface',... | [-0.11895266135494846, 0.12143226945045171, -0.10589636774817243, 0.06822834711354704, -0.07626356087917557, -0.1727020180133434, -0.043203546990974784, 0.3685947047242035, -0.17808789261377966, -0.2401294271575096, 0.0789726979990239, -0.2814291450612916, -0.12664323970556068, 0.23421183972356793, -0.04445923935838017... |
708.0393 | Microcanonical model for a gaz of evaporating black holes and strings,
scattering amplitudes and mass spectrum | We study the system formed by a gaz of black holes and strings within a
microcanonical formulation. We derive the microcanonical content of the system:
entropy, equation of state, number of components N, temperature T and specific
heat. The pressure and the specific heat are negative reflecting the
gravitational unst... | hep-th astro-ph gr-qc hep-ph | we study the system formed by a gaz of black holes and strings within a microcanonical formulation we derive the microcanonical content of the system entropy equation of state number of components n temperature t and specific heat the pressure and the specific heat are negative reflecting the gravitational unstability ... | [['we', 'study', 'the', 'system', 'formed', 'by', 'a', 'gaz', 'of', 'black', 'holes', 'and', 'strings', 'within', 'a', 'microcanonical', 'formulation', 'we', 'derive', 'the', 'microcanonical', 'content', 'of', 'the', 'system', 'entropy', 'equation', 'of', 'state', 'number', 'of', 'components', 'n', 'temperature', 't', ... | [-0.15970328352903287, 0.19089526465390935, -0.09396642381470317, 0.11316440501911675, -0.006457286831607557, -0.14076941714401028, 0.059853466361279126, 0.25878495934357276, -0.2218218961167095, -0.3018299493112453, 0.07096750486881295, -0.3313835210344439, -0.06295066178189264, 0.1650887285087417, 0.01485512703376304... |
708.0394 | Spontaneous symmetry breakings in graphene subjected to in-plane
magnetic field | Application of the magnetic field parallel to the plane of the graphene sheet
leads to the formation of electron- and hole-like Fermi surfaces. Such
situation is shown to be unstable with respect to the formation of an excitonic
condensate even for an arbitrary weak magnetic field and interaction strength.
At tempera... | cond-mat.mes-hall cond-mat.str-el hep-ph | application of the magnetic field parallel to the plane of the graphene sheet leads to the formation of electron and holelike fermi surfaces such situation is shown to be unstable with respect to the formation of an excitonic condensate even for an arbitrary weak magnetic field and interaction strength at temperatures ... | [['application', 'of', 'the', 'magnetic', 'field', 'parallel', 'to', 'the', 'plane', 'of', 'the', 'graphene', 'sheet', 'leads', 'to', 'the', 'formation', 'of', 'electron', 'and', 'holelike', 'fermi', 'surfaces', 'such', 'situation', 'is', 'shown', 'to', 'be', 'unstable', 'with', 'respect', 'to', 'the', 'formation', 'of... | [-0.1849808259961015, 0.25888792524675674, -0.019022495851048357, 0.0999087221590021, -0.043180623732667456, -0.13727239348865564, 0.029038365807801093, 0.3615792333398775, -0.2591083838444163, -0.2884533108322836, 0.034751609562375455, -0.2978656600399684, -0.06902114559535778, 0.14176579708326106, 0.08584645456228886... |
708.0395 | Determination of the Critical Exponents for the Isotropic-Nematic Phase
Transition in a System of Long Rods on Two-dimensional Lattices: Universality
of the Transition | Monte Carlo simulations and finite-size scaling analysis have been carried
out to study the critical behavior and universality for the isotropic-nematic
phase transition in a system of long straight rigid rods of length $k$
($k$-mers) on two-dimensional lattices. The nematic phase, characterized by a
big domain of pa... | cond-mat.stat-mech | monte carlo simulations and finitesize scaling analysis have been carried out to study the critical behavior and universality for the isotropicnematic phase transition in a system of long straight rigid rods of length k kmers on twodimensional lattices the nematic phase characterized by a big domain of parallel kmers i... | [['monte', 'carlo', 'simulations', 'and', 'finitesize', 'scaling', 'analysis', 'have', 'been', 'carried', 'out', 'to', 'study', 'the', 'critical', 'behavior', 'and', 'universality', 'for', 'the', 'isotropicnematic', 'phase', 'transition', 'in', 'a', 'system', 'of', 'long', 'straight', 'rigid', 'rods', 'of', 'length', '... | [-0.15341451149899513, 0.243326007835567, -0.049260578629327936, 0.002342062700772658, 0.014369878377765417, -0.16385638974606992, 0.05699371220776811, 0.3726013206655625, -0.23982136095874013, -0.21274754835292697, 0.09497922224807553, -0.3261195680871606, -0.0958707126788795, 0.1241890220809728, 0.13225109213963152, ... |
708.0396 | Kinematics of the Broad Line Region in M81 | A new model is presented which explains the origin of the broad emission
lines observed in the LINER/Seyfert nucleus of M81 in terms of a steady state
spherically symmetric inflow, amounting to 1 x 10^-5 Msun/yr, which is
sufficient to explain the luminosity of the AGN. The emitting volume has an
outer radius of ~1 p... | astro-ph | a new model is presented which explains the origin of the broad emission lines observed in the linerseyfert nucleus of m81 in terms of a steady state spherically symmetric inflow amounting to 1 x 105 msunyr which is sufficient to explain the luminosity of the agn the emitting volume has an outer radius of 1 pc making i... | [['a', 'new', 'model', 'is', 'presented', 'which', 'explains', 'the', 'origin', 'of', 'the', 'broad', 'emission', 'lines', 'observed', 'in', 'the', 'linerseyfert', 'nucleus', 'of', 'm81', 'in', 'terms', 'of', 'a', 'steady', 'state', 'spherically', 'symmetric', 'inflow', 'amounting', 'to', '1', 'x', '105', 'msunyr', 'wh... | [-0.08410000282456168, 0.09174788399261441, -0.02114863572284006, 0.10508961100220823, -0.045137499815945586, -0.09606760986006031, 0.04851984980587776, 0.4084949561752952, -0.13976140745843832, -0.3217658125079022, 0.0622756675315591, -0.2570775587326632, 0.03622073233843996, 0.15033877413952723, -0.060778032001690005... |
708.0397 | A presentation for the mapping class group of the closed non-orientable
surface of genus 4 | Finite presentations for the mapping class group M(F) are known for arbitrary
orientable compact surface F. If F is non-orientable, then such presentations
are known only when F has genus at most 3 and few boundary components. In this
paper we obtain finite presentation for the mapping class group of the closed
non-o... | math.GT math.GR | finite presentations for the mapping class group mf are known for arbitrary orientable compact surface f if f is nonorientable then such presentations are known only when f has genus at most 3 and few boundary components in this paper we obtain finite presentation for the mapping class group of the closed nonorientable... | [['finite', 'presentations', 'for', 'the', 'mapping', 'class', 'group', 'mf', 'are', 'known', 'for', 'arbitrary', 'orientable', 'compact', 'surface', 'f', 'if', 'f', 'is', 'nonorientable', 'then', 'such', 'presentations', 'are', 'known', 'only', 'when', 'f', 'has', 'genus', 'at', 'most', '3', 'and', 'few', 'boundary', ... | [-0.16010983647121227, 0.17112133813583674, -0.04916616316254744, 0.05719048354555579, -0.12500550233594634, -0.1693777521209353, -0.013541925573543482, 0.40086174197494984, -0.27131397045142125, -0.2807628499097465, 0.11934748210307375, -0.2686961799147813, -0.15957355773185983, 0.25703741152948867, -0.113208790754844... |
708.0398 | Eigencone, saturation and Horn problems for symplectic and odd
orthogonal groups | We consider the eigenvalue problem and the associated intersection theory of
homogenous spaces for the symplectic and odd orthogonal groups. We solve the
Horn and saturation problems for these classical groups.
| math.RT math.AG | we consider the eigenvalue problem and the associated intersection theory of homogenous spaces for the symplectic and odd orthogonal groups we solve the horn and saturation problems for these classical groups | [['we', 'consider', 'the', 'eigenvalue', 'problem', 'and', 'the', 'associated', 'intersection', 'theory', 'of', 'homogenous', 'spaces', 'for', 'the', 'symplectic', 'and', 'odd', 'orthogonal', 'groups', 'we', 'solve', 'the', 'horn', 'and', 'saturation', 'problems', 'for', 'these', 'classical', 'groups']] | [-0.1815638871893527, 0.0693782341456221, -0.04718379324842845, 0.15799368869873784, -0.0898427474162271, -0.12668459901526088, -0.009343916298671356, 0.34376696070596097, -0.3349287350091242, -0.24131979577002988, 0.15184022872633632, -0.25400338610333784, -0.16619136406769675, 0.14387741546717384, -0.0622837728099717... |
708.0399 | Diffusion induced decoherence of stored optical vortices | We study the coherence properties of optical vortices stored in atomic
ensembles. In the presence of thermal diffusion, the topological nature of
stored optical vortices is found not to guarantee slow decoherence. Instead the
stored vortex state has decoherence surprisingly larger than the stored
Gaussian mode. Gener... | quant-ph | we study the coherence properties of optical vortices stored in atomic ensembles in the presence of thermal diffusion the topological nature of stored optical vortices is found not to guarantee slow decoherence instead the stored vortex state has decoherence surprisingly larger than the stored gaussian mode generally t... | [['we', 'study', 'the', 'coherence', 'properties', 'of', 'optical', 'vortices', 'stored', 'in', 'atomic', 'ensembles', 'in', 'the', 'presence', 'of', 'thermal', 'diffusion', 'the', 'topological', 'nature', 'of', 'stored', 'optical', 'vortices', 'is', 'found', 'not', 'to', 'guarantee', 'slow', 'decoherence', 'instead', ... | [-0.1558270918924848, 0.24143596092524292, -0.05694177914578635, 0.06983029168426387, -0.005391785614863709, -0.15185236135447347, 0.010505643291482786, 0.38419590068158804, -0.308508513293959, -0.20327542245237007, 0.09104103169945144, -0.2753782987779191, -0.0476591944493152, 0.19014421867223474, -0.00453921164142655... |
708.04 | Odd Scalar Curvature in Field-Antifield Formalism | We consider the possibility of adding a Grassmann-odd function \nu to the odd
Laplacian. Requiring the total \Delta operator to be nilpotent leads to a
differential condition for \nu, which is integrable. It turns out that the odd
function \nu is not an independent geometric object, but is instead completely
specifie... | hep-th math-ph math.MP math.SG | we consider the possibility of adding a grassmannodd function nu to the odd laplacian requiring the total delta operator to be nilpotent leads to a differential condition for nu which is integrable it turns out that the odd function nu is not an independent geometric object but is instead completely specified by the an... | [['we', 'consider', 'the', 'possibility', 'of', 'adding', 'a', 'grassmannodd', 'function', 'nu', 'to', 'the', 'odd', 'laplacian', 'requiring', 'the', 'total', 'delta', 'operator', 'to', 'be', 'nilpotent', 'leads', 'to', 'a', 'differential', 'condition', 'for', 'nu', 'which', 'is', 'integrable', 'it', 'turns', 'out', 't... | [-0.1933178500002428, 0.14257063623471408, -0.08492580384229588, 0.06509966833241118, -0.12916461167453674, -0.18301726737397778, 0.011911652506934182, 0.31050773248503544, -0.27844287817229985, -0.26335366086880113, 0.04758023144084082, -0.27320797232448296, -0.14717723238044625, 0.12179036956031326, -0.05790427534479... |
708.0401 | Algebraic Degeneracy of Non-Archimedean Analytic Maps | We prove non-Archimedean analogs of results of Noguchi and Winkelmann showing
algebraic degeneracy of rigid analytic maps to projective varieties omitting an
effective divisor with sufficiently many irreducible components relative to the
rank of the group they generate in the Neron-Severi group of the variety.
| math.AG math.CV math.NT | we prove nonarchimedean analogs of results of noguchi and winkelmann showing algebraic degeneracy of rigid analytic maps to projective varieties omitting an effective divisor with sufficiently many irreducible components relative to the rank of the group they generate in the neronseveri group of the variety | [['we', 'prove', 'nonarchimedean', 'analogs', 'of', 'results', 'of', 'noguchi', 'and', 'winkelmann', 'showing', 'algebraic', 'degeneracy', 'of', 'rigid', 'analytic', 'maps', 'to', 'projective', 'varieties', 'omitting', 'an', 'effective', 'divisor', 'with', 'sufficiently', 'many', 'irreducible', 'components', 'relative'... | [-0.20481017453389036, 0.03372232961862917, -0.14420590177178383, 0.0609672621720367, -0.08949932388754354, -0.0811063395606147, -0.026341022137138577, 0.3414784303141965, -0.3316421506305536, -0.22655937928292486, 0.07432740938901487, -0.24224050047083034, -0.13235158843712674, 0.23348933313455847, -0.1605213207296199... |
708.0402 | Recombination Ghosts in Littrow Configuration: Implications for
Spectrographs Using Volume Phase Holographic Gratings | We report the discovery of optical ghosts generated when using Volume Phase
Holographic (VPH) gratings in spectrographs employing the Littrow
configuration. The ghost is caused by light reflected off the detector surface,
recollimated by the camera, recombined by, and reflected from, the grating and
reimaged by the c... | astro-ph | we report the discovery of optical ghosts generated when using volume phase holographic vph gratings in spectrographs employing the littrow configuration the ghost is caused by light reflected off the detector surface recollimated by the camera recombined by and reflected from the grating and reimaged by the camera ont... | [['we', 'report', 'the', 'discovery', 'of', 'optical', 'ghosts', 'generated', 'when', 'using', 'volume', 'phase', 'holographic', 'vph', 'gratings', 'in', 'spectrographs', 'employing', 'the', 'littrow', 'configuration', 'the', 'ghost', 'is', 'caused', 'by', 'light', 'reflected', 'off', 'the', 'detector', 'surface', 'rec... | [-0.1089327391461263, 0.14437899204566465, -0.12600419589616052, 0.012576050945695062, -0.09412355104949875, -0.1444263574953542, -0.012682073731471587, 0.4270347575542563, -0.15653175761896118, -0.3470108431141793, 0.12012630054148937, -0.2787359927238927, -0.11602553856448408, 0.22253532720859484, -0.0844330426880929... |
708.0403 | Lifting D-Instanton Zero Modes by Recombination and Background Fluxes | We study the conditions under which D-brane instantons in Type II orientifold
compactifications generate a non-perturbative superpotential. If the instanton
is non-invariant under the orientifold action, it carries four instead of the
two Goldstone fermions required for superpotential contributions. Unless these
are ... | hep-th | we study the conditions under which dbrane instantons in type ii orientifold compactifications generate a nonperturbative superpotential if the instanton is noninvariant under the orientifold action it carries four instead of the two goldstone fermions required for superpotential contributions unless these are lifted t... | [['we', 'study', 'the', 'conditions', 'under', 'which', 'dbrane', 'instantons', 'in', 'type', 'ii', 'orientifold', 'compactifications', 'generate', 'a', 'nonperturbative', 'superpotential', 'if', 'the', 'instanton', 'is', 'noninvariant', 'under', 'the', 'orientifold', 'action', 'it', 'carries', 'four', 'instead', 'of',... | [-0.181295690423047, 0.21474653599163726, -0.03153978217203907, 0.15667598162138877, -0.10320383403823775, -0.18277821434352964, 0.020187785209624724, 0.3063368480403554, -0.187317827407689, -0.2218835200681127, 0.08682391013051159, -0.24937881467077025, -0.13712197898408987, 0.07213994955399976, -0.10678288107986915, ... |
708.0404 | Scattering mechanisms and Boltzmann transport in graphene | Different scattering mechanisms in graphene are explored and conductivity is
calculated within the Boltzmann transport theory. We provide results for
short-range scattering using the Random Phase Approximation for electron
screening, as well as analytical expressions for the dependence of conductivity
on the dielectr... | cond-mat.mes-hall | different scattering mechanisms in graphene are explored and conductivity is calculated within the boltzmann transport theory we provide results for shortrange scattering using the random phase approximation for electron screening as well as analytical expressions for the dependence of conductivity on the dielectric co... | [['different', 'scattering', 'mechanisms', 'in', 'graphene', 'are', 'explored', 'and', 'conductivity', 'is', 'calculated', 'within', 'the', 'boltzmann', 'transport', 'theory', 'we', 'provide', 'results', 'for', 'shortrange', 'scattering', 'using', 'the', 'random', 'phase', 'approximation', 'for', 'electron', 'screening... | [-0.10099980528000742, 0.18464392296504228, -0.07899961395654827, 0.07022995406412519, 0.0341478292667307, -0.1514652863284573, 0.0387271453847643, 0.39842566108331084, -0.2661884891893715, -0.25316999398637563, -0.01919377761078067, -0.34167035756632685, -0.17374741525389253, 0.20330143535742537, 0.09204188315896317, ... |
708.0405 | Variable stars in the Fornax dSph Galaxy. I. The Globular Cluster Fornax
4 | Variable stars have been identified for the first time in Fornax 4, the
globular cluster located near the center of the Fornax dwarf spheroidal galaxy.
By applying the image subtraction technique to B,V time series photometry
obtained with the MagIC camera of the 6.5-m Magellan/Clay telescope and with
the wide field ... | astro-ph | variable stars have been identified for the first time in fornax 4 the globular cluster located near the center of the fornax dwarf spheroidal galaxy by applying the image subtraction technique to bv time series photometry obtained with the magic camera of the 65m magellanclay telescope and with the wide field imager o... | [['variable', 'stars', 'have', 'been', 'identified', 'for', 'the', 'first', 'time', 'in', 'fornax', '4', 'the', 'globular', 'cluster', 'located', 'near', 'the', 'center', 'of', 'the', 'fornax', 'dwarf', 'spheroidal', 'galaxy', 'by', 'applying', 'the', 'image', 'subtraction', 'technique', 'to', 'bv', 'time', 'series', '... | [-0.06627013506415078, 0.1056878258892114, -0.10628749660291913, 0.06218267333762351, -0.12098715222691218, -0.06500654256084773, 0.14107549160265076, 0.40463621991090853, -0.12761483159297982, -0.3902260700079995, 0.046934970089016946, -0.31788137812610023, -0.024803587377336123, 0.20886548277141934, -0.10203927473063... |
708.0406 | Robust Models for Phase Shifts in Accreting Binary Stars | Radial velocity studies of accreting binary stars commonly use accretion disk
emission lines to determine the radial velocity of the primary star and
therefore the mass ratio. These emission line radial velocity curves are often
shifted in phase from the expected motion of the primary. These phase shifts
cast doubt o... | astro-ph | radial velocity studies of accreting binary stars commonly use accretion disk emission lines to determine the radial velocity of the primary star and therefore the mass ratio these emission line radial velocity curves are often shifted in phase from the expected motion of the primary these phase shifts cast doubt on th... | [['radial', 'velocity', 'studies', 'of', 'accreting', 'binary', 'stars', 'commonly', 'use', 'accretion', 'disk', 'emission', 'lines', 'to', 'determine', 'the', 'radial', 'velocity', 'of', 'the', 'primary', 'star', 'and', 'therefore', 'the', 'mass', 'ratio', 'these', 'emission', 'line', 'radial', 'velocity', 'curves', '... | [-0.07797898015410487, 0.09962687033937494, -0.054635254661575774, 0.09387424782055212, -0.09103717939437028, -0.09230575160776723, 0.05280885145077435, 0.40282172604987576, -0.2040619316293084, -0.3367197358823238, 0.09019357546068153, -0.2648778626143895, -0.06547307745850094, 0.22259383174400796, -0.0362678118819250... |
708.0407 | Discovery of Radio Jets in z~2 ULIRGs with Deep 9.7um Silicate
Absorption | Recent Spitzer observations have revealed a substantial population of z~2
ULIRGs with deep silicate absorption (\tau_{9.7}>1). This paper reports a 20cm
radio study of such a sample to elucidate their physical nature. We discover
that a substantial fraction (40%) of deep silicate absorption ULIRGs at z~2 are
moderate... | astro-ph | recent spitzer observations have revealed a substantial population of z2 ulirgs with deep silicate absorption tau_971 this paper reports a 20cm radio study of such a sample to elucidate their physical nature we discover that a substantial fraction 40 of deep silicate absorption ulirgs at z2 are moderately radioloud wit... | [['recent', 'spitzer', 'observations', 'have', 'revealed', 'a', 'substantial', 'population', 'of', 'z2', 'ulirgs', 'with', 'deep', 'silicate', 'absorption', 'tau_971', 'this', 'paper', 'reports', 'a', '20cm', 'radio', 'study', 'of', 'such', 'a', 'sample', 'to', 'elucidate', 'their', 'physical', 'nature', 'we', 'discove... | [-0.05638431995881326, 0.0831413478711373, -0.05721323306982716, 0.07330867880955338, -0.1034465403437163, -0.10817332446335279, 0.05154096178470575, 0.4968315176609339, -0.14199351010787667, -0.28080762761899014, 0.05928915135604753, -0.32385311611561163, -0.04590807700191032, 0.12383059696717695, -0.02389634950368693... |
708.0408 | Spin-Valley Kondo Effect in Multi-electron Silicon Quantum Dots | We study the spin-valley Kondo effect of a silicon quantum dot occupied by $%
\mathcal{N}$ electrons, with $\mathcal{N}$ up to four. We show that the Kondo
resonance appears in the $\mathcal{N}=1,2,3$ Coulomb blockade regimes, but not
in the $\mathcal{N}=4$ one, in contrast to the spin-1/2 Kondo effect, which
only oc... | cond-mat.mtrl-sci cond-mat.str-el | we study the spinvalley kondo effect of a silicon quantum dot occupied by mathcaln electrons with mathcaln up to four we show that the kondo resonance appears in the mathcaln123 coulomb blockade regimes but not in the mathcaln4 one in contrast to the spin12 kondo effect which only occurs at mathcaln odd assuming large ... | [['we', 'study', 'the', 'spinvalley', 'kondo', 'effect', 'of', 'a', 'silicon', 'quantum', 'dot', 'occupied', 'by', 'mathcaln', 'electrons', 'with', 'mathcaln', 'up', 'to', 'four', 'we', 'show', 'that', 'the', 'kondo', 'resonance', 'appears', 'in', 'the', 'mathcaln123', 'coulomb', 'blockade', 'regimes', 'but', 'not', 'i... | [-0.17771118866661, 0.22123087569407107, -0.051000944492657165, 0.0884103626934749, 0.012810277327545137, -0.19944202912433837, 0.05209049424812848, 0.3419670533832638, -0.2450222259093601, -0.3072037002768668, -0.020529517202306814, -0.2972231516802071, -0.09500034752101856, 0.13791683292478923, 0.037626007028024065, ... |
708.0409 | Analytical form of current-voltage characteristic of parallel-plane,
cylindrical and spherical ionization chambers with homogeneous ionization | The elementary processes taking place in the formation of charged particles
and their flow in parallel-plane, cylindrical and spherical ionization chambers
are considered. On the basis of particles and charges balance a differential
equation describing the distribution of current densities in the ionization
chamber v... | physics.gen-ph physics.plasm-ph | the elementary processes taking place in the formation of charged particles and their flow in parallelplane cylindrical and spherical ionization chambers are considered on the basis of particles and charges balance a differential equation describing the distribution of current densities in the ionization chamber volume... | [['the', 'elementary', 'processes', 'taking', 'place', 'in', 'the', 'formation', 'of', 'charged', 'particles', 'and', 'their', 'flow', 'in', 'parallelplane', 'cylindrical', 'and', 'spherical', 'ionization', 'chambers', 'are', 'considered', 'on', 'the', 'basis', 'of', 'particles', 'and', 'charges', 'balance', 'a', 'diff... | [-0.09952403448533448, 0.0922692263212833, -0.09209532512170149, 0.020973612961824983, 0.027978059858447167, -0.07636444782838225, -0.04257067883523499, 0.31466510512570783, -0.19962819684978303, -0.2978727300083492, 0.03442649067544219, -0.29159398538219494, 0.013566631073467207, 0.19205677718287562, 0.028369957131827... |
708.041 | Correlated projection operator approach to non-Markovian dynamics in
spin baths | The dynamics of an open quantum system is usually studied by performing a
weak-coupling and weak-correlation expansion in the system-bath interaction.
For systems exhibiting strong couplings and highly non-Markovian behavior this
approach is not justified. We apply a recently proposed correlated projection
superopera... | quant-ph cond-mat.mes-hall | the dynamics of an open quantum system is usually studied by performing a weakcoupling and weakcorrelation expansion in the systembath interaction for systems exhibiting strong couplings and highly nonmarkovian behavior this approach is not justified we apply a recently proposed correlated projection superoperator tech... | [['the', 'dynamics', 'of', 'an', 'open', 'quantum', 'system', 'is', 'usually', 'studied', 'by', 'performing', 'a', 'weakcoupling', 'and', 'weakcorrelation', 'expansion', 'in', 'the', 'systembath', 'interaction', 'for', 'systems', 'exhibiting', 'strong', 'couplings', 'and', 'highly', 'nonmarkovian', 'behavior', 'this', ... | [-0.10904117900912368, 0.09684322310577963, -0.08266210785870431, 0.0734141237805213, -0.028798840222282147, -0.17989743131409408, 0.008918333328713517, 0.34994476600421953, -0.2813880431098402, -0.25610202149735817, 0.06636397186837611, -0.2854100520201369, -0.12073120849907672, 0.21952064930880016, 0.0265372397010684... |
708.0411 | Energy conditions in f(R)-gravity | In order to shed some light on the current discussion about f(R)-gravity
theories we derive and discuss the bounds imposed by the energy conditions on a
general f(R) functional form. The null and strong energy conditions in this
framework are derived from the Raychaudhuri's equation along with the
requirement that gr... | astro-ph | in order to shed some light on the current discussion about frgravity theories we derive and discuss the bounds imposed by the energy conditions on a general fr functional form the null and strong energy conditions in this framework are derived from the raychaudhuris equation along with the requirement that gravity is ... | [['in', 'order', 'to', 'shed', 'some', 'light', 'on', 'the', 'current', 'discussion', 'about', 'frgravity', 'theories', 'we', 'derive', 'and', 'discuss', 'the', 'bounds', 'imposed', 'by', 'the', 'energy', 'conditions', 'on', 'a', 'general', 'fr', 'functional', 'form', 'the', 'null', 'and', 'strong', 'energy', 'conditio... | [-0.13512118419384933, 0.1053675529302609, -0.08267402474666596, 0.11232842492427153, -0.09027954267185123, -0.10461358302563895, -0.008710341920959763, 0.3211994254379533, -0.22284082648729964, -0.3193272537464509, 0.11562829169270117, -0.2037505136358959, -0.09375412441295339, 0.22196475705459306, -0.0135228648505290... |
708.0412 | Non-Fermi liquid behavior in a fluctuating valence system, the filled
skutterudite compound CeRu_{4}As_{12} | Electrical resistivity $\rho$, specific heat C, and magnetic susceptibility
$\chi$ measurements made on the filled skutterudite CeRu_4As_{12} reveal
non-Fermi liquid (NFL) T - dependences at low T, i.e., $\rho$(T) $\sim$ T^{1.4}
and weak power law or logarithmic divergences in C(T)/T and $\chi$(T).
Measurements also ... | cond-mat.str-el | electrical resistivity rho specific heat c and magnetic susceptibility chi measurements made on the filled skutterudite ceru_4as_12 reveal nonfermi liquid nfl t dependences at low t ie rhot sim t14 and weak power law or logarithmic divergences in ctt and chit measurements also show that the t dependence of the thermoel... | [['electrical', 'resistivity', 'rho', 'specific', 'heat', 'c', 'and', 'magnetic', 'susceptibility', 'chi', 'measurements', 'made', 'on', 'the', 'filled', 'skutterudite', 'ceru_4as_12', 'reveal', 'nonfermi', 'liquid', 'nfl', 't', 'dependences', 'at', 'low', 't', 'ie', 'rhot', 'sim', 't14', 'and', 'weak', 'power', 'law',... | [-0.16049217022465248, 0.2506244527434893, -0.0854658863948364, 0.036599001896224524, -0.03030034788197985, -0.2356472305316282, 0.12455194088734539, 0.2976181002162201, -0.2838356994043447, -0.2916466023282785, 0.004320037421329241, -0.44184742605215627, -0.07495832616267235, 0.1857011896705157, 0.04780967986627825, -... |
708.0413 | Non-Detection of Gravitationally Redshifted Absorption Lines in the
X-ray Burst Spectra of GS 1826-24 | During a 200 ks observation with the XMM-Newton Reflection Grating
Spectrometer, we detected 16 type-I X-ray bursts from GS 1826-24. We combined
the burst spectra in an attempt to measure the gravitational redshifts from the
surface of the neutron star. We divided the composite GS 1826-24 burst spectrum
into three gr... | astro-ph | during a 200 ks observation with the xmmnewton reflection grating spectrometer we detected 16 typei xray bursts from gs 182624 we combined the burst spectra in an attempt to measure the gravitational redshifts from the surface of the neutron star we divided the composite gs 182624 burst spectrum into three groups based... | [['during', 'a', '200', 'ks', 'observation', 'with', 'the', 'xmmnewton', 'reflection', 'grating', 'spectrometer', 'we', 'detected', '16', 'typei', 'xray', 'bursts', 'from', 'gs', '182624', 'we', 'combined', 'the', 'burst', 'spectra', 'in', 'an', 'attempt', 'to', 'measure', 'the', 'gravitational', 'redshifts', 'from', '... | [-0.07051872783221114, 0.13952638718276433, -0.1142477683770733, 0.10651261428705393, -0.11586196094942398, -0.10317072269315712, 0.09473083260206458, 0.4872271447346952, -0.16431068406344798, -0.3356315577402711, 0.06048435086641126, -0.3785077113514909, -0.015935867899455704, 0.23566484094436208, -0.00981821813501226... |
708.0414 | Modeling of Emission Signatures of Massive Black Hole Binaries: I
Methods | We model the electromagnetic signatures of massive black hole binaries
(MBHBs) with an associated gas component. The method comprises numerical
simulations of relativistic binaries and gas coupled with calculations of the
physical properties of the emitting gas. We calculate the UV/X-ray and the
Halpha light curves a... | astro-ph | we model the electromagnetic signatures of massive black hole binaries mbhbs with an associated gas component the method comprises numerical simulations of relativistic binaries and gas coupled with calculations of the physical properties of the emitting gas we calculate the uvxray and the halpha light curves and the h... | [['we', 'model', 'the', 'electromagnetic', 'signatures', 'of', 'massive', 'black', 'hole', 'binaries', 'mbhbs', 'with', 'an', 'associated', 'gas', 'component', 'the', 'method', 'comprises', 'numerical', 'simulations', 'of', 'relativistic', 'binaries', 'and', 'gas', 'coupled', 'with', 'calculations', 'of', 'the', 'physi... | [-0.1128788439077269, 0.10843187427945598, -0.07647124808337764, 0.10458700576456764, -0.05179698306162015, -0.09704296662842474, 0.05556048431908749, 0.3979645978891287, -0.18260194491370615, -0.3220620706834527, 0.08300381707659657, -0.2917408469043313, -0.039852530033473506, 0.2504106247685401, 0.03780955853093415, ... |
708.0415 | Search for Pentaquarks in the Hadronic Decays of the Z Boson with the
DELPHI Detector at LEP | The quark model does not exclude states composed of more than three quarks,
like pentaquark systems. Controversial evidence for such states has been
published in the last years, in particular: for a strange pentaquark
Theta(1540)+; for a double-strange state, the Xi(1862)--, subsequently called
Phi(1860)--; and for a... | hep-ex | the quark model does not exclude states composed of more than three quarks like pentaquark systems controversial evidence for such states has been published in the last years in particular for a strange pentaquark theta1540 for a doublestrange state the xi1862 subsequently called phi1860 and for a charmed state the the... | [['the', 'quark', 'model', 'does', 'not', 'exclude', 'states', 'composed', 'of', 'more', 'than', 'three', 'quarks', 'like', 'pentaquark', 'systems', 'controversial', 'evidence', 'for', 'such', 'states', 'has', 'been', 'published', 'in', 'the', 'last', 'years', 'in', 'particular', 'for', 'a', 'strange', 'pentaquark', 't... | [-0.121304368890501, 0.23236602955069896, -0.05583429735506306, 0.12026964712611123, 0.028698693438609306, -0.15270062409517532, 0.13190709496769626, 0.28450971122750873, -0.14733972280865182, -0.27868873068458727, 0.019239731201417493, -0.3717000430034524, 0.04600845228383519, 0.13392954144187938, 0.07464518858594946,... |
708.0416 | Simultaneous ferromagnetic metal-semiconductor transition in
electron-doped EuO | We present a general framework to describe the simultaneous
para-to-ferromagnetic and semiconductor-to-metal transition in electron-doped
EuO. The theory correctly describes detailed experimental features of the
conductivity and of the magnetization, in particular the doping dependence of
the Curie temperature. The e... | cond-mat.str-el cond-mat.mtrl-sci | we present a general framework to describe the simultaneous paratoferromagnetic and semiconductortometal transition in electrondoped euo the theory correctly describes detailed experimental features of the conductivity and of the magnetization in particular the doping dependence of the curie temperature the existence o... | [['we', 'present', 'a', 'general', 'framework', 'to', 'describe', 'the', 'simultaneous', 'paratoferromagnetic', 'and', 'semiconductortometal', 'transition', 'in', 'electrondoped', 'euo', 'the', 'theory', 'correctly', 'describes', 'detailed', 'experimental', 'features', 'of', 'the', 'conductivity', 'and', 'of', 'the', '... | [-0.13020478010634487, 0.1144372051810178, -0.0479952345408921, 0.051692530837894046, -0.013853111954511336, -0.08538748945091974, 0.11064176968044057, 0.3486334360292498, -0.2205390633646188, -0.2511589352638935, -0.019464165301782625, -0.33525192343963767, -0.12760245344900298, 0.11991864045695314, 0.0343717148632935... |
708.0417 | Disentangling the Dynamical Mechanisms for Cluster Galaxy Evolution | The determination of the dynamical causes of the morphological Butcher-Oemler
(BO) effect, or the rapid transformation of a large population of late-type
galaxies to earlier Hubble types in the rich cluster environment between
intermediate redshifts and the local universe, has been an important unsolved
problem which... | astro-ph | the determination of the dynamical causes of the morphological butcheroemler bo effect or the rapid transformation of a large population of latetype galaxies to earlier hubble types in the rich cluster environment between intermediate redshifts and the local universe has been an important unsolved problem which is cent... | [['the', 'determination', 'of', 'the', 'dynamical', 'causes', 'of', 'the', 'morphological', 'butcheroemler', 'bo', 'effect', 'or', 'the', 'rapid', 'transformation', 'of', 'a', 'large', 'population', 'of', 'latetype', 'galaxies', 'to', 'earlier', 'hubble', 'types', 'in', 'the', 'rich', 'cluster', 'environment', 'between... | [-0.07707905613973727, 0.03612375810693718, -0.12337466004728365, 0.0865825488908259, -0.11096332733711553, -0.02771036703910718, 0.054985923707366935, 0.3770157118874883, -0.25150377010660513, -0.33287259188810825, 0.06828552150172452, -0.199167747718218, -0.14982706324502865, 0.19891534268944747, -0.01544546478344176... |
708.0418 | Anomalous exciton lifetime by an electromagnetic coupling of
self-assembled quantum dots | We report on the experimental observation of a hitherto ignored long-range
electromagnetic coupling between self-assembled quantum dots. A 12 times
enhancement of the quantum dot exciton lifetime is observed by means of
time-resolved differential reflection spectroscopy. The enhancement is
explained by utilizing and ... | cond-mat.other | we report on the experimental observation of a hitherto ignored longrange electromagnetic coupling between selfassembled quantum dots a 12 times enhancement of the quantum dot exciton lifetime is observed by means of timeresolved differential reflection spectroscopy the enhancement is explained by utilizing and extendi... | [['we', 'report', 'on', 'the', 'experimental', 'observation', 'of', 'a', 'hitherto', 'ignored', 'longrange', 'electromagnetic', 'coupling', 'between', 'selfassembled', 'quantum', 'dots', 'a', '12', 'times', 'enhancement', 'of', 'the', 'quantum', 'dot', 'exciton', 'lifetime', 'is', 'observed', 'by', 'means', 'of', 'time... | [-0.1539995990187571, 0.19088229592562767, -0.034303764559393914, -0.00400964806587517, -0.009111147586321621, -0.13148237781582825, 0.06848707371350508, 0.41139825243143396, -0.222848995294618, -0.3380569042637944, -0.024009720971726142, -0.2718339556166412, -0.09268786676080995, 0.2090368313845574, 0.0424393432116822... |
708.0419 | On the Geometry of the Moduli Space of Real Binary Octics | The moduli space of smooth real binary octics has five connected components.
They parametrize the real binary octics whose defining equations have 0, 1,
..., 4 complex-conjugate pairs of roots respectively. We show that the
GIT-stable completion of each of these five components admits the structure of
an arithmetic r... | math.AG math.DG | the moduli space of smooth real binary octics has five connected components they parametrize the real binary octics whose defining equations have 0 1 4 complexconjugate pairs of roots respectively we show that the gitstable completion of each of these five components admits the structure of an arithmetic real hyperboli... | [['the', 'moduli', 'space', 'of', 'smooth', 'real', 'binary', 'octics', 'has', 'five', 'connected', 'components', 'they', 'parametrize', 'the', 'real', 'binary', 'octics', 'whose', 'defining', 'equations', 'have', '0', '1', '4', 'complexconjugate', 'pairs', 'of', 'roots', 'respectively', 'we', 'show', 'that', 'the', 'g... | [-0.23055719096294564, 0.13134112770927933, -0.10682394175091758, 0.0692068528201755, -0.13214049280276927, -0.12424472074591271, -0.025986595503206405, 0.36657387844246364, -0.2938365097380365, -0.22150224986810074, 0.12952737850339516, -0.27337969825400604, -0.19714091001989562, 0.222170421957423, -0.0800859088321094... |
708.042 | On Emerton's $p$-adic Banach spaces | The purpose of the current paper is to introduce some new methods for
studying the $p$-adic Banach spaces introduced by Emerton \cite{emerton}. We
first relate these spaces to more familiar sheaf cohomology groups. As an
application, we obtain a more general version of Emerton's spectral sequence.
We also calculate t... | math.NT | the purpose of the current paper is to introduce some new methods for studying the padic banach spaces introduced by emerton citeemerton we first relate these spaces to more familiar sheaf cohomology groups as an application we obtain a more general version of emertons spectral sequence we also calculate the spaces in ... | [['the', 'purpose', 'of', 'the', 'current', 'paper', 'is', 'to', 'introduce', 'some', 'new', 'methods', 'for', 'studying', 'the', 'padic', 'banach', 'spaces', 'introduced', 'by', 'emerton', 'citeemerton', 'we', 'first', 'relate', 'these', 'spaces', 'to', 'more', 'familiar', 'sheaf', 'cohomology', 'groups', 'as', 'an', ... | [-0.11898770958578098, 0.040716741421647384, -0.11623955669347197, 0.19371400966520014, -0.11424583333428018, -0.07851363007648615, -0.0002335301942366641, 0.3420212790078949, -0.297840368708421, -0.21794213089742698, 0.1321024779081199, -0.17542093290830962, -0.1877108663902618, 0.25963843904901296, -0.197058421676047... |
708.0421 | Contributions to the Study of Thermal States of the Bosonic String in
the TFD Formalism | We determine the local entropy of the free energy of the quantized open
bosonic string in Minkowski spacetime with the most general boundary
conditions. We formulate a finite temperature theory of the thermal closed
string excitations in anti-de Sitter spacetime within the TFD approach. We
write down the thermal stat... | hep-th | we determine the local entropy of the free energy of the quantized open bosonic string in minkowski spacetime with the most general boundary conditions we formulate a finite temperature theory of the thermal closed string excitations in antide sitter spacetime within the tfd approach we write down the thermal states an... | [['we', 'determine', 'the', 'local', 'entropy', 'of', 'the', 'free', 'energy', 'of', 'the', 'quantized', 'open', 'bosonic', 'string', 'in', 'minkowski', 'spacetime', 'with', 'the', 'most', 'general', 'boundary', 'conditions', 'we', 'formulate', 'a', 'finite', 'temperature', 'theory', 'of', 'the', 'thermal', 'closed', '... | [-0.13983908432183434, 0.2081009963074246, -0.11194545483276425, 0.09707556449103395, -0.015800493564834265, -0.07476675436781668, 0.037318721758138794, 0.2731707468676079, -0.22954518017768105, -0.2281456002462152, 0.052395689036898514, -0.2477275540649488, -0.04174975209517052, 0.0998475525112873, -0.0588951169016041... |
708.0422 | Scaling Relations of Spiral Galaxies | We construct a large data set of global structural parameters for 1300 field
and cluster spiral galaxies and explore the joint distribution of luminosity L,
optical rotation velocity V, and disk size R at I- and 2MASS K-bands. The I-
and K-band velocity-luminosity (VL) relations have log-slopes of 0.29 and 0.27,
resp... | astro-ph | we construct a large data set of global structural parameters for 1300 field and cluster spiral galaxies and explore the joint distribution of luminosity l optical rotation velocity v and disk size r at i and 2mass kbands the i and kband velocityluminosity vl relations have logslopes of 029 and 027 respectively with si... | [['we', 'construct', 'a', 'large', 'data', 'set', 'of', 'global', 'structural', 'parameters', 'for', '1300', 'field', 'and', 'cluster', 'spiral', 'galaxies', 'and', 'explore', 'the', 'joint', 'distribution', 'of', 'luminosity', 'l', 'optical', 'rotation', 'velocity', 'v', 'and', 'disk', 'size', 'r', 'at', 'i', 'and', '... | [-0.04299738174678255, 0.11028969376925787, -0.09424628277333032, 0.12239471915089627, -0.11212540827912489, -0.09076123654223761, 0.0332495962243262, 0.4483193469770851, -0.1937542096444025, -0.3542341145815967, 0.030996547341023837, -0.32510634420956247, -0.04126046631883755, 0.17551474991304644, -0.06157178683444368... |
708.0423 | Masers in AGN environments | Galactic nuclei are well known sources of OH and H2O maser emission. It
appears that intense star formation in ultra-luminous infrared galaxies drives
most OH sources. In contrast, nuclear activity appears to drive most H2O
sources. When H2O emission originates in accretion disk structures, constrained
geometry and d... | astro-ph | galactic nuclei are well known sources of oh and h2o maser emission it appears that intense star formation in ultraluminous infrared galaxies drives most oh sources in contrast nuclear activity appears to drive most h2o sources when h2o emission originates in accretion disk structures constrained geometry and dynamics ... | [['galactic', 'nuclei', 'are', 'well', 'known', 'sources', 'of', 'oh', 'and', 'h2o', 'maser', 'emission', 'it', 'appears', 'that', 'intense', 'star', 'formation', 'in', 'ultraluminous', 'infrared', 'galaxies', 'drives', 'most', 'oh', 'sources', 'in', 'contrast', 'nuclear', 'activity', 'appears', 'to', 'drive', 'most', ... | [-0.0701141652579491, 0.07719852155871475, -0.03157328950384489, 0.09752467690178981, -0.13187985872634903, -0.10272591889728434, 0.0010923571087634908, 0.43291437984086, -0.18963523925720857, -0.3358250697626947, 0.049697824395619906, -0.26213360756922227, 0.011354042718616815, 0.21771635604314865, -0.0222640020880275... |
708.0424 | Dual-Frequency Resonance-Tracking Atomic Force Microscopy | A dual-excitation method for resonant-frequency tracking in scanning probe
microscopy based on amplitude detection is developed. This method allows the
cantilever to be operated at or near resonance for techniques where standard
phase locked loops are not possible. This includes techniques with non-acoustic
driving w... | cond-mat.mtrl-sci | a dualexcitation method for resonantfrequency tracking in scanning probe microscopy based on amplitude detection is developed this method allows the cantilever to be operated at or near resonance for techniques where standard phase locked loops are not possible this includes techniques with nonacoustic driving where th... | [['a', 'dualexcitation', 'method', 'for', 'resonantfrequency', 'tracking', 'in', 'scanning', 'probe', 'microscopy', 'based', 'on', 'amplitude', 'detection', 'is', 'developed', 'this', 'method', 'allows', 'the', 'cantilever', 'to', 'be', 'operated', 'at', 'or', 'near', 'resonance', 'for', 'techniques', 'where', 'standar... | [-0.15025807145026657, 0.16579702846643798, -0.08451779495812202, -0.049234907843653836, -0.08401338626386835, -0.1829753730839881, 0.054792437836021536, 0.4407650621345379, -0.2575479314737522, -0.2590664556662508, 0.09297509519023908, -0.2408717780863482, -0.1628154695187164, 0.2535406461644968, -0.017325323843865988... |
708.0425 | Distribution of phylogenetic diversity under random extinction | Phylogenetic diversity is a measure for describing how much of an
evolutionary tree is spanned by a subset of species. If one applies this to the
(unknown) subset of current species that will still be present at some future
time, then this `future phylogenetic diversity' provides a measure of the
impact of various ex... | q-bio.SC q-bio.PE | phylogenetic diversity is a measure for describing how much of an evolutionary tree is spanned by a subset of species if one applies this to the unknown subset of current species that will still be present at some future time then this future phylogenetic diversity provides a measure of the impact of various extinction... | [['phylogenetic', 'diversity', 'is', 'a', 'measure', 'for', 'describing', 'how', 'much', 'of', 'an', 'evolutionary', 'tree', 'is', 'spanned', 'by', 'a', 'subset', 'of', 'species', 'if', 'one', 'applies', 'this', 'to', 'the', 'unknown', 'subset', 'of', 'current', 'species', 'that', 'will', 'still', 'be', 'present', 'at'... | [-0.1277961097101667, 0.13394379329632225, -0.10494402685869875, 0.10417620084550816, -0.04888730213817542, -0.09146454400007627, 0.05399042146659192, 0.3700160487735672, -0.28903502748528526, -0.26274164440110326, 0.08978950967073941, -0.22775949368169948, -0.164837529464041, 0.14350387188188954, -0.08764524764986013,... |
708.0426 | Pathways to folding, nucleation events and native geometry | We perform extensive Monte Carlo simulations of a lattice model and the Go
potential to investigate the existence of folding pathways at the level of
contact cluster formation for two native structures with markedly different
geometries. Our analysis of folding pathways revealed a common underlying
folding mechanism,... | q-bio.BM | we perform extensive monte carlo simulations of a lattice model and the go potential to investigate the existence of folding pathways at the level of contact cluster formation for two native structures with markedly different geometries our analysis of folding pathways revealed a common underlying folding mechanism bas... | [['we', 'perform', 'extensive', 'monte', 'carlo', 'simulations', 'of', 'a', 'lattice', 'model', 'and', 'the', 'go', 'potential', 'to', 'investigate', 'the', 'existence', 'of', 'folding', 'pathways', 'at', 'the', 'level', 'of', 'contact', 'cluster', 'formation', 'for', 'two', 'native', 'structures', 'with', 'markedly', ... | [-0.0964166132439124, 0.09405634200053388, -0.1264755318687285, 0.12504964125732124, -0.048278473322524836, -0.15597945380171663, 0.05949302890803665, 0.4069403133502132, -0.2947153229854609, -0.2701709992987545, 0.020015736517349357, -0.25166697670754634, -0.2513501154258847, 0.19177200752800624, 0.05279546417418475, ... |
708.0427 | Time Cycles in Indian Cosmology | In this article we review some key time cycles in ancient Indian astronomy,
especially those that have emerged from researches in the past couple of
decades expressing knowledge of the changing frame of earth's axis. The article
also briefly reviews the philosophy related to the interconnection between the
inner and ... | physics.hist-ph | in this article we review some key time cycles in ancient indian astronomy especially those that have emerged from researches in the past couple of decades expressing knowledge of the changing frame of earths axis the article also briefly reviews the philosophy related to the interconnection between the inner and the o... | [['in', 'this', 'article', 'we', 'review', 'some', 'key', 'time', 'cycles', 'in', 'ancient', 'indian', 'astronomy', 'especially', 'those', 'that', 'have', 'emerged', 'from', 'researches', 'in', 'the', 'past', 'couple', 'of', 'decades', 'expressing', 'knowledge', 'of', 'the', 'changing', 'frame', 'of', 'earths', 'axis',... | [-0.08335407149570528, 0.09334257944283308, -0.08051531610090024, 0.0614080759078206, -0.144219630779844, -0.011175971379998373, -0.03987605521632531, 0.35591746801219415, -0.24787921941606328, -0.3258085027919151, 0.13893906456360128, -0.2575219333230052, -0.1988517182326177, 0.2082513773057144, -0.08631754459929653, ... |
708.0428 | Progress Toward a VLBA Movie of the Jet Collimation Region in M87 | With its high black hole mass, proximity, and bright jet, M87 provides the
best prospect for a direct imaging study of the acceleration and collimation
region of a jet. Previous VLBI observations have shown an edge brightened
structure with a wide opening angle at small scales. An effort to measure
component speeds i... | astro-ph | with its high black hole mass proximity and bright jet m87 provides the best prospect for a direct imaging study of the acceleration and collimation region of a jet previous vlbi observations have shown an edge brightened structure with a wide opening angle at small scales an effort to measure component speeds in this ... | [['with', 'its', 'high', 'black', 'hole', 'mass', 'proximity', 'and', 'bright', 'jet', 'm87', 'provides', 'the', 'best', 'prospect', 'for', 'a', 'direct', 'imaging', 'study', 'of', 'the', 'acceleration', 'and', 'collimation', 'region', 'of', 'a', 'jet', 'previous', 'vlbi', 'observations', 'have', 'shown', 'an', 'edge',... | [-0.07568980573132023, 0.06438581243409312, -0.09746999375302857, 0.024089203135445516, -0.09964212832390947, -0.069095095167449, 0.047364145916487486, 0.4411314442438423, -0.18909446936083474, -0.36497238160125794, 0.1267457800546523, -0.2812314492344817, -0.022595386877785333, 0.22431835673611472, -0.0292533473102449... |
708.0429 | Observing the temperature of the Big Bang through large scale structure | It is widely accepted that the Universe underwent a period of thermal
equilibrium at very early times. One expects a residue of this primordial state
to be imprinted on the large scale structure of space time. In this paper we
study the morphology of this thermal residue in a universe whose early dynamics
is governed... | astro-ph gr-qc hep-ph | it is widely accepted that the universe underwent a period of thermal equilibrium at very early times one expects a residue of this primordial state to be imprinted on the large scale structure of space time in this paper we study the morphology of this thermal residue in a universe whose early dynamics is governed by ... | [['it', 'is', 'widely', 'accepted', 'that', 'the', 'universe', 'underwent', 'a', 'period', 'of', 'thermal', 'equilibrium', 'at', 'very', 'early', 'times', 'one', 'expects', 'a', 'residue', 'of', 'this', 'primordial', 'state', 'to', 'be', 'imprinted', 'on', 'the', 'large', 'scale', 'structure', 'of', 'space', 'time', 'i... | [-0.1503236950840801, 0.19443703735899664, -0.1609645254095085, 0.0917493497361041, -0.027471203787717967, -0.03781991143284055, -0.025881127559114248, 0.3012373346282402, -0.25196604638670883, -0.2838450726936571, 0.11811543194926344, -0.25919998302900543, -0.0933674579874302, 0.16662318858628472, 0.024525268461244802... |
708.043 | Diffuse Ionized Gas in the Dwarf Irregular Galaxy DDO 53 | The spectral characteristics throughout the dwarf irregular galaxy DDO 53 are
studied. The results are very similar to those for other irregular galaxies:
high excitation and low values of the [SII]/Halpha ratio. The most likely
ionization source is photon leakage from the classical HII regions, without any
other sou... | astro-ph | the spectral characteristics throughout the dwarf irregular galaxy ddo 53 are studied the results are very similar to those for other irregular galaxies high excitation and low values of the siihalpha ratio the most likely ionization source is photon leakage from the classical hii regions without any other source altho... | [['the', 'spectral', 'characteristics', 'throughout', 'the', 'dwarf', 'irregular', 'galaxy', 'ddo', '53', 'are', 'studied', 'the', 'results', 'are', 'very', 'similar', 'to', 'those', 'for', 'other', 'irregular', 'galaxies', 'high', 'excitation', 'and', 'low', 'values', 'of', 'the', 'siihalpha', 'ratio', 'the', 'most', ... | [-0.06232442391817184, 0.08226057954187341, -0.06476452107559524, 0.13417009061873508, -0.07055094622431651, -0.09825753718249354, 0.014623546105462546, 0.4433337139586608, -0.13893270473950087, -0.3399882592699107, 0.024894245347811605, -0.3045380735386382, -0.012115677127011996, 0.21893170978714183, -0.04950527854117... |
708.0431 | The Rank of the Cartier operator on cyclic covers of the projective line | We give a lower bound on the rank of the Cartier operator of Jacobian
varieties of hyperelliptic and superelliptic curves in terms of their genus.
| math.AG | we give a lower bound on the rank of the cartier operator of jacobian varieties of hyperelliptic and superelliptic curves in terms of their genus | [['we', 'give', 'a', 'lower', 'bound', 'on', 'the', 'rank', 'of', 'the', 'cartier', 'operator', 'of', 'jacobian', 'varieties', 'of', 'hyperelliptic', 'and', 'superelliptic', 'curves', 'in', 'terms', 'of', 'their', 'genus']] | [-0.23482548274099826, 0.0389229978993535, -0.13556268714368344, 0.06340709336102009, -0.07407803965732455, -0.15871965376660227, 0.05654129073023796, 0.26268571078777314, -0.26042800486087797, -0.23888673275709152, 0.06492108808364719, -0.2570119991339743, -0.1762816873192787, 0.30541527688503267, -0.2288151868060231,... |
708.0432 | Black hole entropy in modified gravity models | An analysis of some modified gravity models, based on the study of pure
Schwarzschild and of Schwarzschild-de Sitter black holes, and involving the use
of the Noether charge method, is carried out. Corrections to the classical
Einsteinian black hole entropy appear. It is shown explicitly how the condition
of positive... | hep-th | an analysis of some modified gravity models based on the study of pure schwarzschild and of schwarzschildde sitter black holes and involving the use of the noether charge method is carried out corrections to the classical einsteinian black hole entropy appear it is shown explicitly how the condition of positive entropy... | [['an', 'analysis', 'of', 'some', 'modified', 'gravity', 'models', 'based', 'on', 'the', 'study', 'of', 'pure', 'schwarzschild', 'and', 'of', 'schwarzschildde', 'sitter', 'black', 'holes', 'and', 'involving', 'the', 'use', 'of', 'the', 'noether', 'charge', 'method', 'is', 'carried', 'out', 'corrections', 'to', 'the', '... | [-0.09744128899001225, 0.0626535449939638, -0.1413670127512887, 0.16289064637749107, -0.09080496453680098, -0.16012231455533765, -0.0298932464356767, 0.2169917562569026, -0.16935678136360366, -0.2886357402021531, 0.08977699305978604, -0.30003650434082374, -0.11660128796938807, 0.18359559185046237, -0.07455873023718596,... |
708.0433 | On the emptiness formation probability of the open XXZ spin-$\tf{1}{2}$
chain | This paper is devoted to the study of the emptiness formation probability
$\tau\pa{m}$ of the open XXZ chain. We derive a closed form for $\tau\pa{m}$ at
$\Delta=\tf{1}{2}$ when the boundary field vanishes. Moreover we obtain its
leading asymptotics for an arbitrary boundary field at the free fermion point.
Finally, ... | hep-th | this paper is devoted to the study of the emptiness formation probability taupam of the open xxz chain we derive a closed form for taupam at deltatf12 when the boundary field vanishes moreover we obtain its leading asymptotics for an arbitrary boundary field at the free fermion point finally we compute the first term o... | [['this', 'paper', 'is', 'devoted', 'to', 'the', 'study', 'of', 'the', 'emptiness', 'formation', 'probability', 'taupam', 'of', 'the', 'open', 'xxz', 'chain', 'we', 'derive', 'a', 'closed', 'form', 'for', 'taupam', 'at', 'deltatf12', 'when', 'the', 'boundary', 'field', 'vanishes', 'moreover', 'we', 'obtain', 'its', 'le... | [-0.18062788791333637, 0.12834908373406506, -0.05716612630446131, 0.07776004886254669, -0.030865004161993663, -0.08578713323610525, 0.03461250121278378, 0.2966166988325616, -0.23578735508878404, -0.19790525453475613, 0.12854281742863047, -0.25065157522136966, -0.10875600934959948, 0.14140282143295432, 0.007514498223705... |
708.0434 | Reduction of the Casimir force using aerogels | By using silicon oxide based aerogels we show numerically that the Casimir
force can be reduced several orders of magnitude, making its effect negligible
in nanodevices. This decrease in the Casimir force is also present even when
the aerogels are deposited on metallic substrates. To calculate the Casimir
force we mo... | quant-ph | by using silicon oxide based aerogels we show numerically that the casimir force can be reduced several orders of magnitude making its effect negligible in nanodevices this decrease in the casimir force is also present even when the aerogels are deposited on metallic substrates to calculate the casimir force we model t... | [['by', 'using', 'silicon', 'oxide', 'based', 'aerogels', 'we', 'show', 'numerically', 'that', 'the', 'casimir', 'force', 'can', 'be', 'reduced', 'several', 'orders', 'of', 'magnitude', 'making', 'its', 'effect', 'negligible', 'in', 'nanodevices', 'this', 'decrease', 'in', 'the', 'casimir', 'force', 'is', 'also', 'pres... | [-0.08557261412109558, 0.19045987566050826, -0.08436769955248262, -0.021951354603515938, -0.012959401528253997, -0.08191329325200059, -0.012626963427464943, 0.4451362730857606, -0.2461051973126208, -0.3149857379612513, 0.029013596758886706, -0.3046509120661843, -0.1780923700959344, 0.23636411305172564, 0.01174576076058... |
708.0435 | Perfect Structure of the Special Relativity, Superluminal,
Neutrino-Photon Mass and New Entangled Interaction | First, some superluminal phenomena and experiments are introduced briefly.
Next, based on the basic principles of the special relativity, the Lorentz
transformation (LT) with smaller velocity and the general Lorentz
transformation (GLT) with larger velocity should be derived simultaneously by
the classification of th... | physics.gen-ph | first some superluminal phenomena and experiments are introduced briefly next based on the basic principles of the special relativity the lorentz transformation lt with smaller velocity and the general lorentz transformation glt with larger velocity should be derived simultaneously by the classification of the timelike... | [['first', 'some', 'superluminal', 'phenomena', 'and', 'experiments', 'are', 'introduced', 'briefly', 'next', 'based', 'on', 'the', 'basic', 'principles', 'of', 'the', 'special', 'relativity', 'the', 'lorentz', 'transformation', 'lt', 'with', 'smaller', 'velocity', 'and', 'the', 'general', 'lorentz', 'transformation', ... | [-0.13549707482420004, 0.2296674212504079, -0.10553589089286661, 0.11963154533157021, -0.14398300201457165, -0.17485534753366774, 0.006365355882144517, 0.38143478142721626, -0.22967264606489748, -0.24925851048712577, 0.09666022402766222, -0.23165239931348958, -0.11545082113143, 0.22025329046433573, -0.04745155839169124... |
708.0436 | Direct Estimation of Single- and Two-Qubit Hamiltonians and Relaxation
Rates | We provide a novel approach for characterization of quantum Hamiltonian
systems via utilizing a single measurement device. Specifically, we demonstrate
how external quantum correlations can be used for Hamiltonian identification
tasks. We explicitly introduce experimental procedures for direct estimation of
single- a... | quant-ph | we provide a novel approach for characterization of quantum hamiltonian systems via utilizing a single measurement device specifically we demonstrate how external quantum correlations can be used for hamiltonian identification tasks we explicitly introduce experimental procedures for direct estimation of single and two... | [['we', 'provide', 'a', 'novel', 'approach', 'for', 'characterization', 'of', 'quantum', 'hamiltonian', 'systems', 'via', 'utilizing', 'a', 'single', 'measurement', 'device', 'specifically', 'we', 'demonstrate', 'how', 'external', 'quantum', 'correlations', 'can', 'be', 'used', 'for', 'hamiltonian', 'identification', '... | [-0.11283487591614154, 0.08530964873260792, -0.11045588079797125, 0.0006608721497736272, -0.06141849552634461, -0.19682387498089637, 0.04638181786299094, 0.42117679739991826, -0.2437278893401568, -0.30110836422991477, 0.04854530807391837, -0.20472903420677643, -0.15927772790236377, 0.2839086700830309, -0.01305609568953... |
708.0437 | Snapshot-based Balanced Truncation for Linear Time-periodic Systems | We introduce an algorithm based on a method of snapshots for computing
approximate balanced truncations for discrete-time, stable, linear
time-periodic systems. By construction, this algorithm is applicable to very
high-dimensional systems, even with very high-dimensional outputs (or,
alternatively, very high-dimensi... | math.OC math.DS | we introduce an algorithm based on a method of snapshots for computing approximate balanced truncations for discretetime stable linear timeperiodic systems by construction this algorithm is applicable to very highdimensional systems even with very highdimensional outputs or alternatively very highdimensional inputs an ... | [['we', 'introduce', 'an', 'algorithm', 'based', 'on', 'a', 'method', 'of', 'snapshots', 'for', 'computing', 'approximate', 'balanced', 'truncations', 'for', 'discretetime', 'stable', 'linear', 'timeperiodic', 'systems', 'by', 'construction', 'this', 'algorithm', 'is', 'applicable', 'to', 'very', 'highdimensional', 'sy... | [-0.10904483008436022, 0.033938953648820255, -0.08374591451138258, 0.09323396561576745, -0.0397512571629593, -0.24338359780115437, 0.010865932206946368, 0.4114545994267172, -0.26225896293715556, -0.25505012201088273, 0.17100636059494348, -0.1486890272389413, -0.2356271019861178, 0.2970973107232047, -0.10819436647758192... |
708.0438 | Fisher's zeros of quasi-Gaussian densities of states | We discuss apparent paradoxes regarding the location of the zeros of the
partition function in the complex $\beta$ plane (Fisher's zeros) of a pure
SU(2) lattice gauge theory in 4 dimensions. We propose a new criterion to draw
the region of the complex $\beta$ plane where reweighting methods can be
trusted when the d... | hep-lat cond-mat.stat-mech hep-th | we discuss apparent paradoxes regarding the location of the zeros of the partition function in the complex beta plane fishers zeros of a pure su2 lattice gauge theory in 4 dimensions we propose a new criterion to draw the region of the complex beta plane where reweighting methods can be trusted when the density of stat... | [['we', 'discuss', 'apparent', 'paradoxes', 'regarding', 'the', 'location', 'of', 'the', 'zeros', 'of', 'the', 'partition', 'function', 'in', 'the', 'complex', 'beta', 'plane', 'fishers', 'zeros', 'of', 'a', 'pure', 'su2', 'lattice', 'gauge', 'theory', 'in', '4', 'dimensions', 'we', 'propose', 'a', 'new', 'criterion', ... | [-0.08992053796039567, 0.11058261991435847, -0.1014097337362193, 0.08677398568403175, -0.05540086672364073, -0.12211208989957476, 0.0645493003459761, 0.39081680927717105, -0.23797294887792292, -0.2506439612595407, 0.09789207248898749, -0.25340493741438136, -0.15522381013884912, 0.16243689799617322, -0.03723303337433937... |
708.0439 | Meta-Stable Brane Configurations with Seven NS5-Branes | We present the intersecting brane configurations consisting of NS-branes,
D4-branes(and anti D4-branes) and O6-plane, of type IIA string theory
corresponding to the meta-stable nonsupersymmetric vacua in four dimensional
N=1 supersymmetric SU(N_c) x SU(N_c') x SU(N_c'') gauge theory with a symmetric
tensor field, a c... | hep-th | we present the intersecting brane configurations consisting of nsbranes d4branesand anti d4branes and o6plane of type iia string theory corresponding to the metastable nonsupersymmetric vacua in four dimensional n1 supersymmetric sun_c x sun_c x sun_c gauge theory with a symmetric tensor field a conjugate symmetric ten... | [['we', 'present', 'the', 'intersecting', 'brane', 'configurations', 'consisting', 'of', 'nsbranes', 'd4branesand', 'anti', 'd4branes', 'and', 'o6plane', 'of', 'type', 'iia', 'string', 'theory', 'corresponding', 'to', 'the', 'metastable', 'nonsupersymmetric', 'vacua', 'in', 'four', 'dimensional', 'n1', 'supersymmetric'... | [-0.19628991094427278, 0.27986603211790834, -0.009156542508557176, 0.12042757352306084, -0.10167945100634236, -0.22561467366970397, -0.054169041055226415, 0.3030186475094671, -0.03719772291228627, -0.1850334471656066, 0.06278613791448262, -0.2811942523288907, -0.1357600522754394, -0.06539604293577599, -0.05316513127675... |
708.044 | Universality and diversity of folding mechanics for three-helix bundle
proteins | In this study we evaluate, at full atomic detail, the folding processes of
two small helical proteins, the B domain of protein A and the Villin headpiece.
Folding kinetics are studied by performing a large number of ab initio Monte
Carlo folding simulations using a single transferable all-atom potential. Using
these ... | q-bio.BM | in this study we evaluate at full atomic detail the folding processes of two small helical proteins the b domain of protein a and the villin headpiece folding kinetics are studied by performing a large number of ab initio monte carlo folding simulations using a single transferable allatom potential using these trajecto... | [['in', 'this', 'study', 'we', 'evaluate', 'at', 'full', 'atomic', 'detail', 'the', 'folding', 'processes', 'of', 'two', 'small', 'helical', 'proteins', 'the', 'b', 'domain', 'of', 'protein', 'a', 'and', 'the', 'villin', 'headpiece', 'folding', 'kinetics', 'are', 'studied', 'by', 'performing', 'a', 'large', 'number', '... | [-0.0925375263684262, 0.07336915317775072, -0.11105953863081641, 0.08106705387730564, -0.017477987090555522, -0.10763953002647329, 0.07169381537152311, 0.4158098959005796, -0.23777204092878562, -0.2885423444951765, 0.04160214395692142, -0.27095603325213186, -0.19399199704759015, 0.1902097503009897, 0.023661037625219577... |
708.0441 | Particle-Number Projection and the Density Functional Theory | In the framework of the Density Functional Theory for superconductors, we
study the restoration of the particle number symmetry by means of the
projection technique. Conceptual problems are outlined and numerical
difficulties are discussed. Both are related to the fact that neither the
many-body Hamiltonian nor the w... | nucl-th | in the framework of the density functional theory for superconductors we study the restoration of the particle number symmetry by means of the projection technique conceptual problems are outlined and numerical difficulties are discussed both are related to the fact that neither the manybody hamiltonian nor the wave fu... | [['in', 'the', 'framework', 'of', 'the', 'density', 'functional', 'theory', 'for', 'superconductors', 'we', 'study', 'the', 'restoration', 'of', 'the', 'particle', 'number', 'symmetry', 'by', 'means', 'of', 'the', 'projection', 'technique', 'conceptual', 'problems', 'are', 'outlined', 'and', 'numerical', 'difficulties'... | [-0.1433833762591738, 0.1404398427743997, -0.09144522683844636, 0.13219048505915063, -0.021743255228336367, -0.07772583716682026, -0.017773988347367518, 0.3359771226133619, -0.24975396956516696, -0.316416992779289, 0.06520153531704896, -0.28132536127232016, -0.2183762325240033, 0.12749193367448503, -0.01326472312211990... |
708.0442 | Large optical gain from four-wave mixing instabilities in semiconductor
quantum wells | Based on a microscopic many-particle theory, we predict large optical gain in
the probe and background-free four-wave mixing directions caused by excitonic
instabilities in semiconductor quantum wells. For a single quantum well with
radiative-decay limited dephasing in a typical pump-probe setup we discuss the
micros... | cond-mat.other | based on a microscopic manyparticle theory we predict large optical gain in the probe and backgroundfree fourwave mixing directions caused by excitonic instabilities in semiconductor quantum wells for a single quantum well with radiativedecay limited dephasing in a typical pumpprobe setup we discuss the microscopic dri... | [['based', 'on', 'a', 'microscopic', 'manyparticle', 'theory', 'we', 'predict', 'large', 'optical', 'gain', 'in', 'the', 'probe', 'and', 'backgroundfree', 'fourwave', 'mixing', 'directions', 'caused', 'by', 'excitonic', 'instabilities', 'in', 'semiconductor', 'quantum', 'wells', 'for', 'a', 'single', 'quantum', 'well',... | [-0.14529012187591028, 0.253915324298389, -0.0568841946552749, 0.06905238613210342, -0.0021949726915745822, -0.17832223592429525, 0.0805800262196162, 0.4028612185890476, -0.2780258922527234, -0.24730217429222884, -0.00023868931586750678, -0.2498032997569276, -0.14719154847854818, 0.2321716272789571, 0.02708637251311706... |
708.0443 | Avoiding small subgraphs in Achlioptas processes | For a fixed integer r, consider the following random process. At each round,
one is presented with r random edges from the edge set of the complete graph on
n vertices, and is asked to choose one of them. The selected edges are
collected into a graph, which thus grows at the rate of one edge per round.
This is a natu... | math.CO math.PR | for a fixed integer r consider the following random process at each round one is presented with r random edges from the edge set of the complete graph on n vertices and is asked to choose one of them the selected edges are collected into a graph which thus grows at the rate of one edge per round this is a natural gener... | [['for', 'a', 'fixed', 'integer', 'r', 'consider', 'the', 'following', 'random', 'process', 'at', 'each', 'round', 'one', 'is', 'presented', 'with', 'r', 'random', 'edges', 'from', 'the', 'edge', 'set', 'of', 'the', 'complete', 'graph', 'on', 'n', 'vertices', 'and', 'is', 'asked', 'to', 'choose', 'one', 'of', 'them', '... | [-0.1364094425977244, 0.11801113998554127, -0.03687640597986192, 0.018313264533460525, -0.0832368391034763, -0.15445962895241394, 0.06769646019324461, 0.3804307834435146, -0.2643718095767556, -0.2977365296632413, 0.10970825208430134, -0.30600941537097276, -0.13301813181656982, 0.10230507401781139, -0.07305747493242537,... |
708.0444 | Practical scheme for non-postselection entanglement concentration using
linear optical elements | We report a practical non-postselection entanglement concentration scheme in
which a maximally entangled Bell-state photon pair is produced from two pairs
of partially (or non-maximally) entangled photons. Since this scheme is built
only upon linear optical elements and does not require photon-number resolving
detect... | quant-ph | we report a practical nonpostselection entanglement concentration scheme in which a maximally entangled bellstate photon pair is produced from two pairs of partially or nonmaximally entangled photons since this scheme is built only upon linear optical elements and does not require photonnumber resolving detectors it ha... | [['we', 'report', 'a', 'practical', 'nonpostselection', 'entanglement', 'concentration', 'scheme', 'in', 'which', 'a', 'maximally', 'entangled', 'bellstate', 'photon', 'pair', 'is', 'produced', 'from', 'two', 'pairs', 'of', 'partially', 'or', 'nonmaximally', 'entangled', 'photons', 'since', 'this', 'scheme', 'is', 'bui... | [-0.12917966862067076, 0.22084196391752212, -0.08947336421174518, -0.008901155457074234, 0.004168876553333159, -0.28671706495490873, 0.0766114087388614, 0.45005597881341386, -0.18163099143085842, -0.2689731927841144, 0.03815989401901804, -0.29162493209212514, -0.033967670388677616, 0.2372819870292067, -0.04223166163063... |
708.0445 | Large Magellanic Cloud Distance from Cepheid Variables using Least
Squares Solutions | Distance to the Large Magellanic Cloud (LMC) is determined using the Cepheid
variables in the LMC. We combine the individual LMC Cepheid distances obtained
from the infrared surface brightness method and a dataset with a large number
of LMC Cepheids. Using the standard least squares method, the LMC distance
modulus c... | astro-ph | distance to the large magellanic cloud lmc is determined using the cepheid variables in the lmc we combine the individual lmc cepheid distances obtained from the infrared surface brightness method and a dataset with a large number of lmc cepheids using the standard least squares method the lmc distance modulus can be f... | [['distance', 'to', 'the', 'large', 'magellanic', 'cloud', 'lmc', 'is', 'determined', 'using', 'the', 'cepheid', 'variables', 'in', 'the', 'lmc', 'we', 'combine', 'the', 'individual', 'lmc', 'cepheid', 'distances', 'obtained', 'from', 'the', 'infrared', 'surface', 'brightness', 'method', 'and', 'a', 'dataset', 'with', ... | [-0.07699280071284363, 0.06382957928915425, -0.1663907161812381, 0.09824812676559322, -0.08810175748744814, -0.07804759635156629, 0.13359521937989952, 0.43375780101459804, -0.2997649956660548, -0.32316020789491656, 0.028228738088169975, -0.3031274784024399, -0.0723163305648077, 0.2285932503815851, -0.10858556568290632,... |
708.0446 | Finite dimensional Hecke algebras | These are notes prepared for ICRA workshop at Torun, Poland, August 2007. In
the first part, we explain results on canonical basic sets by Geck and Jacon
and propose a categorification framework which is suitable for our example of
Hecke algebras. In the second part, we review basics of Kashiwara crystal and
explain ... | math.RT math.QA | these are notes prepared for icra workshop at torun poland august 2007 in the first part we explain results on canonical basic sets by geck and jacon and propose a categorification framework which is suitable for our example of hecke algebras in the second part we review basics of kashiwara crystal and explain the fock... | [['these', 'are', 'notes', 'prepared', 'for', 'icra', 'workshop', 'at', 'torun', 'poland', 'august', '2007', 'in', 'the', 'first', 'part', 'we', 'explain', 'results', 'on', 'canonical', 'basic', 'sets', 'by', 'geck', 'and', 'jacon', 'and', 'propose', 'a', 'categorification', 'framework', 'which', 'is', 'suitable', 'for... | [-0.0982519229212821, 0.05764675858765117, -0.09488555256874093, 0.05915544213030885, -0.1324598905856459, -0.10203235748323422, -0.010803254972239143, 0.3185340642332307, -0.25032534182650373, -0.279103935058726, 0.12431790827529378, -0.2534128313305453, -0.18698024805816052, 0.18470991375738555, -0.18800310211400817,... |
708.0447 | Scalable scheme for entangling multiple ququarts using linear optical
elements | We report a scalable linear optical scheme for generating entangled states of
multiple ququarts in which the individual single-ququart state is prepared with
the biphoton polarization state of frequency-nondegenerate spontaneous
parametric down-conversion. The output state is calculated with the full
consideration of... | quant-ph | we report a scalable linear optical scheme for generating entangled states of multiple ququarts in which the individual singleququart state is prepared with the biphoton polarization state of frequencynondegenerate spontaneous parametric downconversion the output state is calculated with the full consideration of the h... | [['we', 'report', 'a', 'scalable', 'linear', 'optical', 'scheme', 'for', 'generating', 'entangled', 'states', 'of', 'multiple', 'ququarts', 'in', 'which', 'the', 'individual', 'singleququart', 'state', 'is', 'prepared', 'with', 'the', 'biphoton', 'polarization', 'state', 'of', 'frequencynondegenerate', 'spontaneous', '... | [-0.14843898141450845, 0.22166798547355096, -0.030095092799347727, -0.005594345589807786, -0.013429621206735498, -0.17259632044735906, 0.04424450039140769, 0.44793413151333583, -0.22161721477090424, -0.2469852899771128, 0.056498907810535785, -0.2708738913664893, -0.024707151694160732, 0.2022338664131378, 0.056809932090... |
708.0448 | An Ozsvath-Szabo Floer homology invariant of knots in a contact manifold | Using the knot Floer homology filtration, we define invariants associated to
a knot in a three-manifold possessing non-vanishing Floer co(homology) classes.
In the case of the Ozsvath-Szabo contact invariant we obtain an invariant of
knots in a contact three-manifold. This invariant provides an upper bound for
the Th... | math.GT math.SG | using the knot floer homology filtration we define invariants associated to a knot in a threemanifold possessing nonvanishing floer cohomology classes in the case of the ozsvathszabo contact invariant we obtain an invariant of knots in a contact threemanifold this invariant provides an upper bound for the thurstonbenne... | [['using', 'the', 'knot', 'floer', 'homology', 'filtration', 'we', 'define', 'invariants', 'associated', 'to', 'a', 'knot', 'in', 'a', 'threemanifold', 'possessing', 'nonvanishing', 'floer', 'cohomology', 'classes', 'in', 'the', 'case', 'of', 'the', 'ozsvathszabo', 'contact', 'invariant', 'we', 'obtain', 'an', 'invaria... | [-0.3161811880497474, 0.08406021088927501, -0.1685315963748673, 0.11881909621738349, -0.11965401684442027, -0.2432084207980414, -0.009645614617814621, 0.3152905194244037, -0.2787015828997193, -0.3190917237309005, 0.034000194248757463, -0.22999405389595212, -0.2054908306366115, 0.18495659380586763, -0.15740544114713417,... |
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