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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708.3549 | Lopsidedness and Sloshing in Centres of Advanced Mergers of Galaxies | We measure the non-axisymmetry in the luminosity distribution in the central
few kpc of a sample of advanced mergers of galaxies, by analyzing their 2MASS
images. All mergers show a high central asymmetry: the centres of isophotes
show a striking sloshing pattern with a spatial variation of upto 30 % within
the centr... | astro-ph | we measure the nonaxisymmetry in the luminosity distribution in the central few kpc of a sample of advanced mergers of galaxies by analyzing their 2mass images all mergers show a high central asymmetry the centres of isophotes show a striking sloshing pattern with a spatial variation of upto 30 within the central 1 kpc... | [['we', 'measure', 'the', 'nonaxisymmetry', 'in', 'the', 'luminosity', 'distribution', 'in', 'the', 'central', 'few', 'kpc', 'of', 'a', 'sample', 'of', 'advanced', 'mergers', 'of', 'galaxies', 'by', 'analyzing', 'their', '2mass', 'images', 'all', 'mergers', 'show', 'a', 'high', 'central', 'asymmetry', 'the', 'centres',... | [-0.10671038219394784, 0.12715745219805588, -0.07530535796346764, 0.12353043610831567, -0.003333217070515578, -0.00986343871918507, 0.03007194893822695, 0.3728938290189641, -0.23167862120705346, -0.3473789270462779, 0.07257870231017781, -0.27872918335100016, -0.006742490872663136, 0.17647972570072548, -0.03314963998879... |
708.355 | Is there a new physics between electroweak and Planck scales? | We argue that there may be no intermediate particle physics energy scale
between the Planck mass $M_{Pl}\sim 10^{19}$ GeV and the electroweak scale $M_W
\sim 100$ GeV. At the same time, the number of problems of the Standard Model
(neutrino masses and oscillations, dark matter, baryon asymmetry of the
Universe, stron... | hep-th hep-ph | we argue that there may be no intermediate particle physics energy scale between the planck mass m_plsim 1019 gev and the electroweak scale m_w sim 100 gev at the same time the number of problems of the standard model neutrino masses and oscillations dark matter baryon asymmetry of the universe strong cpproblem gauge c... | [['we', 'argue', 'that', 'there', 'may', 'be', 'no', 'intermediate', 'particle', 'physics', 'energy', 'scale', 'between', 'the', 'planck', 'mass', 'm_plsim', '1019', 'gev', 'and', 'the', 'electroweak', 'scale', 'm_w', 'sim', '100', 'gev', 'at', 'the', 'same', 'time', 'the', 'number', 'of', 'problems', 'of', 'the', 'sta... | [-0.14055058535666684, 0.3063053393459602, -0.050683480290998076, 0.22525851379897496, -0.04828667259347197, -0.1245134919693039, 0.008525992391278615, 0.29175822482117125, -0.22588182507535895, -0.4077975695600381, 0.02080573862720583, -0.2571548596276222, 0.06872449577723101, 0.1386228808897195, 0.08936670812702663, ... |
708.3551 | Theoretical analysis of the optimal conditions for photon-spin quantum
state transfer | We analyzed the yield and fidelity of the quantum state transfer (QST) from a
photon polarization qubit to an electron spin qubit in a spin-coherent photo
detector consisting of a semiconductor quantum dot. We used a model consisting
of the quantum dot, where the QST is carried out, coupled with a photonic
cavity. We... | cond-mat.other cond-mat.mes-hall | we analyzed the yield and fidelity of the quantum state transfer qst from a photon polarization qubit to an electron spin qubit in a spincoherent photo detector consisting of a semiconductor quantum dot we used a model consisting of the quantum dot where the qst is carried out coupled with a photonic cavity we determin... | [['we', 'analyzed', 'the', 'yield', 'and', 'fidelity', 'of', 'the', 'quantum', 'state', 'transfer', 'qst', 'from', 'a', 'photon', 'polarization', 'qubit', 'to', 'an', 'electron', 'spin', 'qubit', 'in', 'a', 'spincoherent', 'photo', 'detector', 'consisting', 'of', 'a', 'semiconductor', 'quantum', 'dot', 'we', 'used', 'a... | [-0.15080738417215317, 0.16576713750413652, -0.034893713357365304, -0.0304281122979078, 0.09769242266124553, -0.25903826397980617, 0.06870355096008793, 0.40592345098197896, -0.21553437808966813, -0.25393528767231416, 0.00385523443486925, -0.29389175438486476, -0.036525988965021336, 0.27625993487206013, 0.02745878936120... |
708.3552 | An order result for the exponential divisor function | The integer $d=\prod_{i=1}^s p_i^{b_i}$ is called an exponential divisor of
$n=\prod_{i=1}^s p_i^{a_i}>1$ if $b_i \mid a_i$ for every $i\in \{1,2,...,s\}$.
Let $\tau^{(e)}(n)$ denote the number of exponential divisors of $n$, where
$\tau^{(e)}(1)=1$ by convention. The aim of the present paper is to establish
an asymp... | math.NT | the integer dprod_i1s p_ib_i is called an exponential divisor of nprod_i1s p_ia_i1 if b_i mid a_i for every iin 12s let tauen denote the number of exponential divisors of n where taue11 by convention the aim of the present paper is to establish an asymptotic formula with remainder term for the rth power of the function... | [['the', 'integer', 'dprod_i1s', 'p_ib_i', 'is', 'called', 'an', 'exponential', 'divisor', 'of', 'nprod_i1s', 'p_ia_i1', 'if', 'b_i', 'mid', 'a_i', 'for', 'every', 'iin', '12s', 'let', 'tauen', 'denote', 'the', 'number', 'of', 'exponential', 'divisors', 'of', 'n', 'where', 'taue11', 'by', 'convention', 'the', 'aim', 'o... | [-0.2200364583199296, 0.1228584178855218, -0.06422761452952674, -0.03883816850686665, -0.03866867367726039, -0.18635683001347764, -0.010912134851370117, 0.259044427130207, -0.3005946797921377, -0.23575287895715413, 0.04449159483534887, -0.3241247170988251, -0.11292611069717061, 0.129076772092102, -0.08632156319971032, ... |
708.3553 | A study of the prompt and afterglow emission of the Short GRB 061201 | Our knowledge of the intrinsic properties of short duration Gamma-Ray Bursts
has relied, so far, only upon a few cases for which the estimate of the
distance and an extended, multiwavelength monitoring of the afterglow have been
obtained. We carried out multiwavelength observations of the short GRB 061201
aimed at es... | astro-ph | our knowledge of the intrinsic properties of short duration gammaray bursts has relied so far only upon a few cases for which the estimate of the distance and an extended multiwavelength monitoring of the afterglow have been obtained we carried out multiwavelength observations of the short grb 061201 aimed at estimatin... | [['our', 'knowledge', 'of', 'the', 'intrinsic', 'properties', 'of', 'short', 'duration', 'gammaray', 'bursts', 'has', 'relied', 'so', 'far', 'only', 'upon', 'a', 'few', 'cases', 'for', 'which', 'the', 'estimate', 'of', 'the', 'distance', 'and', 'an', 'extended', 'multiwavelength', 'monitoring', 'of', 'the', 'afterglow'... | [-0.08140706637960697, 0.07806926204654474, -0.09998840624898798, 0.12954138793512485, -0.09785341047819406, -0.0973386532132895, 0.08062395214335011, 0.4855138164658084, -0.18840783590513266, -0.32649747352999975, 0.08802890122714865, -0.2900678841986611, -0.023916134598246434, 0.2115592088202557, 0.003904223115918254... |
708.3554 | Time-distance helioseismology: Sensitivity of f-mode travel times to
flows | Time-distance helioseismology has shown that f-mode travel times contain
information about horizontal flows in the Sun. The purpose of this study is to
provide a simple interpretation of these travel times. We study the interaction
of surface-gravity waves with horizontal flows in an incompressible,
plane-parallel so... | astro-ph | timedistance helioseismology has shown that fmode travel times contain information about horizontal flows in the sun the purpose of this study is to provide a simple interpretation of these travel times we study the interaction of surfacegravity waves with horizontal flows in an incompressible planeparallel solar atmos... | [['timedistance', 'helioseismology', 'has', 'shown', 'that', 'fmode', 'travel', 'times', 'contain', 'information', 'about', 'horizontal', 'flows', 'in', 'the', 'sun', 'the', 'purpose', 'of', 'this', 'study', 'is', 'to', 'provide', 'a', 'simple', 'interpretation', 'of', 'these', 'travel', 'times', 'we', 'study', 'the', ... | [-0.16259567430278482, 0.14583752427600155, -0.04911758558089818, 0.0891912867768574, -0.07636434733298278, -0.03508666527811356, -0.017578749350621873, 0.38887381911538055, -0.23808814797399963, -0.26259112659146333, 0.10121959198965777, -0.2689954316930837, -0.11659403761577342, 0.23293237097146535, 0.000212988464413... |
708.3555 | Weakly anisotropic frustrated zigzag spin chain | The frustrated spin-1/2 model with weakly anisotropic ferromagnetic
nearest-neighbor and antiferromagnetic next-nearest-neighbor exchanges is
studied with use of variational mean-field approach, scaling estimates of the
infrared divergencies in the perturbation theory and finite-size calculations.
The ground state ph... | cond-mat.str-el | the frustrated spin12 model with weakly anisotropic ferromagnetic nearestneighbor and antiferromagnetic nextnearestneighbor exchanges is studied with use of variational meanfield approach scaling estimates of the infrared divergencies in the perturbation theory and finitesize calculations the ground state phase diagram... | [['the', 'frustrated', 'spin12', 'model', 'with', 'weakly', 'anisotropic', 'ferromagnetic', 'nearestneighbor', 'and', 'antiferromagnetic', 'nextnearestneighbor', 'exchanges', 'is', 'studied', 'with', 'use', 'of', 'variational', 'meanfield', 'approach', 'scaling', 'estimates', 'of', 'the', 'infrared', 'divergencies', 'i... | [-0.24036180879331276, 0.2675085577640765, -0.05846663770749222, 0.051986401499826695, -0.03222017027909243, -0.14918855079037102, 0.09007542619122122, 0.3702716723886095, -0.24791914505200296, -0.23801754665843955, 0.03309595826246976, -0.37509062584442426, -0.14681788523316006, 0.0571645100872162, 0.15280598123805433... |
708.3556 | Generalization error for multi-class margin classification | In this article, we study rates of convergence of the generalization error of
multi-class margin classifiers. In particular, we develop an upper bound theory
quantifying the generalization error of various large margin classifiers. The
theory permits a treatment of general margin losses, convex or nonconvex, in
prese... | math.ST stat.TH | in this article we study rates of convergence of the generalization error of multiclass margin classifiers in particular we develop an upper bound theory quantifying the generalization error of various large margin classifiers the theory permits a treatment of general margin losses convex or nonconvex in presence or ab... | [['in', 'this', 'article', 'we', 'study', 'rates', 'of', 'convergence', 'of', 'the', 'generalization', 'error', 'of', 'multiclass', 'margin', 'classifiers', 'in', 'particular', 'we', 'develop', 'an', 'upper', 'bound', 'theory', 'quantifying', 'the', 'generalization', 'error', 'of', 'various', 'large', 'margin', 'classi... | [-0.11544630383341624, 0.046372398485693085, -0.03183664307023289, 0.07702120604439168, -0.04700651374315062, -0.14383020563431645, 0.12040043230824453, 0.3493384177551194, -0.2657562799236026, -0.32262066179812604, 0.08670981014673147, -0.2508412073141024, -0.11122555477339374, 0.2221933795321953, -0.12666356821966318... |
708.3557 | On certain arithmetic functions involving exponential divisors, II | Asymptotic properties of certain arithmetic functions involving exponential
divisors are investigated.
| math.NT | asymptotic properties of certain arithmetic functions involving exponential divisors are investigated | [['asymptotic', 'properties', 'of', 'certain', 'arithmetic', 'functions', 'involving', 'exponential', 'divisors', 'are', 'investigated']] | [-0.30085994574156677, 0.13460294309664855, -0.18137009678916496, 0.24501234470781955, -0.03040194401348179, -0.15805752109736204, 0.004400944358415224, 0.3162124746225097, -0.28618736361915414, -0.17451965673403305, 0.1442889879372987, -0.2418005666272207, -0.1794985514557497, 0.250430780378255, -0.07113178599287164, ... |
708.3558 | Teleparallel Killing Vectors of the Einstein Universe | In this short paper we establish the definition of the Lie derivative of a
second rank tensor in the context of teleparallel theory of gravity and also
extend it for a general tensor of rank $p+q$. This definition is then used to
find Killing vectors of the Einstein universe. It turns out that Killing
vectors of the ... | gr-qc | in this short paper we establish the definition of the lie derivative of a second rank tensor in the context of teleparallel theory of gravity and also extend it for a general tensor of rank pq this definition is then used to find killing vectors of the einstein universe it turns out that killing vectors of the einstei... | [['in', 'this', 'short', 'paper', 'we', 'establish', 'the', 'definition', 'of', 'the', 'lie', 'derivative', 'of', 'a', 'second', 'rank', 'tensor', 'in', 'the', 'context', 'of', 'teleparallel', 'theory', 'of', 'gravity', 'and', 'also', 'extend', 'it', 'for', 'a', 'general', 'tensor', 'of', 'rank', 'pq', 'this', 'definit... | [-0.15303455616480538, 0.06901956026309303, -0.1071465274368945, 0.10749107713511746, -0.13985300049451846, -0.1057971899547348, -0.09273948173338015, 0.27972805088252894, -0.24518717701679893, -0.21067633127261484, 0.05822913339943625, -0.2062872430043561, -0.18833943320371743, 0.08811304170106138, -0.0666225855105689... |
708.3559 | Locally Indistinguishable Subspaces Spanned by Three-Qubit Unextendible
Product Bases | We study the local distinguishability of general multi-qubit states and show
that local projective measurements and classical communication are as powerful
as the most general local measurements and classical communication. Remarkably,
this indicates that the local distinguishability of multi-qubit states can be
deci... | quant-ph | we study the local distinguishability of general multiqubit states and show that local projective measurements and classical communication are as powerful as the most general local measurements and classical communication remarkably this indicates that the local distinguishability of multiqubit states can be decided ef... | [['we', 'study', 'the', 'local', 'distinguishability', 'of', 'general', 'multiqubit', 'states', 'and', 'show', 'that', 'local', 'projective', 'measurements', 'and', 'classical', 'communication', 'are', 'as', 'powerful', 'as', 'the', 'most', 'general', 'local', 'measurements', 'and', 'classical', 'communication', 'remar... | [-0.16053152860660244, 0.20885345026014004, -0.04799376117852442, 0.045719148718159304, -0.01961051312618874, -0.2156138082911425, 0.02260875984040253, 0.3517302866890668, -0.2675078163592065, -0.2247534076618479, 0.09123771783850967, -0.22632920912113338, -0.155833851097819, 0.19746693048531558, -0.060541038513482415,... |
708.356 | Prompt photon hadroproduction at high energies in off-shell gluon-gluon
fusion | The amplitude for production of a single photon associated with quark pair in
the fusion of two off-shell gluons is calculated. The matrix element found is
applied to the inclusive prompt photon hadroproduction at high energies in the
framework of kt-factorization QCD approach. The total and differential cross
sectio... | hep-ph | the amplitude for production of a single photon associated with quark pair in the fusion of two offshell gluons is calculated the matrix element found is applied to the inclusive prompt photon hadroproduction at high energies in the framework of ktfactorization qcd approach the total and differential cross sections are... | [['the', 'amplitude', 'for', 'production', 'of', 'a', 'single', 'photon', 'associated', 'with', 'quark', 'pair', 'in', 'the', 'fusion', 'of', 'two', 'offshell', 'gluons', 'is', 'calculated', 'the', 'matrix', 'element', 'found', 'is', 'applied', 'to', 'the', 'inclusive', 'prompt', 'photon', 'hadroproduction', 'at', 'hig... | [0.02013387719736151, 0.1736417498642012, -0.13971173131190565, 0.1564915747695562, 0.0014922530896475782, -0.07391188213470108, -0.011298908163671907, 0.3838302800512832, -0.14838116859774228, -0.26173135000078573, -0.043409522303946964, -0.3650386039248627, 0.08206799078489775, 0.16649353288761948, 0.0644522723944290... |
708.3561 | Phase transitions in a fluid surface model with a deficit angle term | Nambu-Goto model is investigated by using the canonical Monte Carlo
simulation technique on dynamically triangulated surfaces of spherical
topology. We find that the model has four distinct phases; crumpled,
branched-polymer, linear, and tubular. The linear phase and the tubular phase
appear to be separated by a firs... | cond-mat.stat-mech cond-mat.soft | nambugoto model is investigated by using the canonical monte carlo simulation technique on dynamically triangulated surfaces of spherical topology we find that the model has four distinct phases crumpled branchedpolymer linear and tubular the linear phase and the tubular phase appear to be separated by a firstorder tra... | [['nambugoto', 'model', 'is', 'investigated', 'by', 'using', 'the', 'canonical', 'monte', 'carlo', 'simulation', 'technique', 'on', 'dynamically', 'triangulated', 'surfaces', 'of', 'spherical', 'topology', 'we', 'find', 'that', 'the', 'model', 'has', 'four', 'distinct', 'phases', 'crumpled', 'branchedpolymer', 'linear'... | [-0.1781219914767214, 0.1963009190459905, -0.09187651655652603, 0.038760924094689966, -0.0244310841411458, -0.13400974493494935, 0.0003601835289208049, 0.37683063427870034, -0.2907384169732474, -0.25827255504290486, 0.08683356231763768, -0.2683574620168656, -0.1583146877608008, 0.14319519031216094, -0.02609013068534047... |
708.3562 | First Passage Densities and Boundary Crossing Probabilities for
Diffusion Processes | We consider the boundary crossing problem for time-homogeneous diffusions and
general curvilinear boundaries. Bounds are derived for the approximation error
of the one-sided (upper) boundary crossing probability when replacing the
original boundary by a different one. In doing so we establish the existence of
the fir... | math.PR | we consider the boundary crossing problem for timehomogeneous diffusions and general curvilinear boundaries bounds are derived for the approximation error of the onesided upper boundary crossing probability when replacing the original boundary by a different one in doing so we establish the existence of the firstpassag... | [['we', 'consider', 'the', 'boundary', 'crossing', 'problem', 'for', 'timehomogeneous', 'diffusions', 'and', 'general', 'curvilinear', 'boundaries', 'bounds', 'are', 'derived', 'for', 'the', 'approximation', 'error', 'of', 'the', 'onesided', 'upper', 'boundary', 'crossing', 'probability', 'when', 'replacing', 'the', 'o... | [-0.12377117309593953, 0.11119841726283014, -0.0455785048879289, 0.10879455425087005, -0.05393536311860841, -0.13442984804994643, 0.07914785460049573, 0.3382776597371468, -0.25156879793100345, -0.28061613738715935, 0.18013432499495907, -0.23770166998012707, -0.11453119448672694, 0.21700323992767012, -0.0480253178191980... |
708.3563 | Renormalization of vacuum energy in linearized quantum gravity | In linearized quantum gravity, a shift of the average energy-momentum can be
compensated by a shift of the average gravitational field. This allows a
renormalization scheme that naturally removes the contribution of quantum
vacuum fluctuations to the cosmological constant, solving the old
cosmological-constant proble... | gr-qc hep-th | in linearized quantum gravity a shift of the average energymomentum can be compensated by a shift of the average gravitational field this allows a renormalization scheme that naturally removes the contribution of quantum vacuum fluctuations to the cosmological constant solving the old cosmologicalconstant problem for w... | [['in', 'linearized', 'quantum', 'gravity', 'a', 'shift', 'of', 'the', 'average', 'energymomentum', 'can', 'be', 'compensated', 'by', 'a', 'shift', 'of', 'the', 'average', 'gravitational', 'field', 'this', 'allows', 'a', 'renormalization', 'scheme', 'that', 'naturally', 'removes', 'the', 'contribution', 'of', 'quantum'... | [-0.2282044799455131, 0.2077449590433389, -0.13730095920618623, 0.0871833753408282, -0.11841665406245738, -0.08456046569820803, 0.0005073450253500292, 0.26244884097347193, -0.28690998124269146, -0.2829127479538632, 0.015099778385774698, -0.21194824629522677, -0.09592945569117244, 0.15876519625696042, -0.024110580231839... |
708.3564 | Deciding security properties for cryptographic protocols. Application to
key cycles | There is a large amount of work dedicated to the formal verification of
security protocols. In this paper, we revisit and extend the NP-complete
decision procedure for a bounded number of sessions. We use a, now standard,
deducibility constraints formalism for modeling security protocols. Our first
contribution is to... | cs.LO cs.CR | there is a large amount of work dedicated to the formal verification of security protocols in this paper we revisit and extend the npcomplete decision procedure for a bounded number of sessions we use a now standard deducibility constraints formalism for modeling security protocols our first contribution is to give a s... | [['there', 'is', 'a', 'large', 'amount', 'of', 'work', 'dedicated', 'to', 'the', 'formal', 'verification', 'of', 'security', 'protocols', 'in', 'this', 'paper', 'we', 'revisit', 'and', 'extend', 'the', 'npcomplete', 'decision', 'procedure', 'for', 'a', 'bounded', 'number', 'of', 'sessions', 'we', 'use', 'a', 'now', 'st... | [-0.16083967202169777, 0.03305824138197051, -0.0915110074362696, 0.07029075753404, -0.10231600430534156, -0.1585394134528415, 0.1292713914790088, 0.3282853791511856, -0.2709395839686527, -0.3159024908348138, 0.11919199786931385, -0.2100005615868932, -0.11164015510964186, 0.21756366964532495, -0.1200386262539406, 0.0912... |
708.3565 | The double-mode RR Lyrae variable BS Com | We present the frequency analysis of the multicolour time series photometry
of the field RRd variable BS Comae. The large number of data points in each of
the BV(RI)_c bands and the ~0.01 magnitude accuracy of the individual
measurements allow us a high precision analysis of the properties of the
combination frequenc... | astro-ph | we present the frequency analysis of the multicolour time series photometry of the field rrd variable bs comae the large number of data points in each of the bvri_c bands and the 001 magnitude accuracy of the individual measurements allow us a high precision analysis of the properties of the combination frequencies due... | [['we', 'present', 'the', 'frequency', 'analysis', 'of', 'the', 'multicolour', 'time', 'series', 'photometry', 'of', 'the', 'field', 'rrd', 'variable', 'bs', 'comae', 'the', 'large', 'number', 'of', 'data', 'points', 'in', 'each', 'of', 'the', 'bvri_c', 'bands', 'and', 'the', '001', 'magnitude', 'accuracy', 'of', 'the'... | [-0.15764553989704816, 0.1086599100034367, -0.06751200612238113, -0.012307830355526444, -0.0717038595801259, -0.07236261174895187, 0.10943554890183534, 0.37286386853876585, -0.24584209381979197, -0.32367449382597463, 0.10668281493262645, -0.295897120213572, -0.06166321301258149, 0.2059126245056061, 0.001784982853271859... |
708.3566 | Does Sub-millisecond Pulsar XTE J1739-285 Contain a Low Magnetic Neutron
Star or Quark Star ? | With the possible detection of the fastest spinning nuclear-powered pulsar
XTE J1739-285 of frequency 1122 Hz (0.8913 ms), it arouses us to constrain the
mass and radius of its central compact object and to imply the stellar matter
compositions: neutrons or quarks. Spun-up by the accreting materials to such a
high ro... | astro-ph | with the possible detection of the fastest spinning nuclearpowered pulsar xte j1739285 of frequency 1122 hz 08913 ms it arouses us to constrain the mass and radius of its central compact object and to imply the stellar matter compositions neutrons or quarks spunup by the accreting materials to such a high rotating spee... | [['with', 'the', 'possible', 'detection', 'of', 'the', 'fastest', 'spinning', 'nuclearpowered', 'pulsar', 'xte', 'j1739285', 'of', 'frequency', '1122', 'hz', '08913', 'ms', 'it', 'arouses', 'us', 'to', 'constrain', 'the', 'mass', 'and', 'radius', 'of', 'its', 'central', 'compact', 'object', 'and', 'to', 'imply', 'the',... | [-0.12702697451309994, 0.22706348506303933, -0.04889196115217578, 0.09617785657367979, -0.1602070287305814, -0.08772209403403582, 0.08683553176561896, 0.3383687327986058, -0.165717061606791, -0.3650372575980444, 0.08883507144995607, -0.259973015039204, 0.03475533920125319, 0.2585865125501863, -0.025132655862715837, -0.... |
708.3567 | On the Distortion of the Eigenvalue Spectrum in MIMO Amplify-and-Forward
Multi-Hop Channels | Consider a wireless MIMO multi-hop channel with n_s non-cooperating source
antennas and n_d fully cooperating destination antennas, as well as L clusters
containing k non-cooperating relay antennas each. The source signal traverses
all L clusters of relay antennas, before it reaches the destination. When relay
antenn... | cs.IT math.IT | consider a wireless mimo multihop channel with n_s noncooperating source antennas and n_d fully cooperating destination antennas as well as l clusters containing k noncooperating relay antennas each the source signal traverses all l clusters of relay antennas before it reaches the destination when relay antennas within... | [['consider', 'a', 'wireless', 'mimo', 'multihop', 'channel', 'with', 'n_s', 'noncooperating', 'source', 'antennas', 'and', 'n_d', 'fully', 'cooperating', 'destination', 'antennas', 'as', 'well', 'as', 'l', 'clusters', 'containing', 'k', 'noncooperating', 'relay', 'antennas', 'each', 'the', 'source', 'signal', 'travers... | [-0.22985714477867694, 0.12262302513007509, -0.0041797496791323415, 0.011756214848260758, -0.07263251111998677, -0.2678337392679374, 0.11840247791208869, 0.3709001007852296, -0.28281443650499355, -0.24414168121614332, 0.10373957517380215, -0.31564109937604423, -0.08058892567458521, 0.0953363317312682, -0.02269393770973... |
708.3568 | A Polynomial-time Algorithm for Computing the Permanent in GF(3^q) | A polynomial-time algorithm for computing the permanent in any field of
characteristic 3 is presented in this article. The principal objects utilized
for that purpose are the Cauchy and Vandermonde matrices, the discriminant
function and their generalizations of various types. Classical theorems on the
permanent such... | cs.CC | a polynomialtime algorithm for computing the permanent in any field of characteristic 3 is presented in this article the principal objects utilized for that purpose are the cauchy and vandermonde matrices the discriminant function and their generalizations of various types classical theorems on the permanent such as th... | [['a', 'polynomialtime', 'algorithm', 'for', 'computing', 'the', 'permanent', 'in', 'any', 'field', 'of', 'characteristic', '3', 'is', 'presented', 'in', 'this', 'article', 'the', 'principal', 'objects', 'utilized', 'for', 'that', 'purpose', 'are', 'the', 'cauchy', 'and', 'vandermonde', 'matrices', 'the', 'discriminant... | [-0.11929171534306178, 0.0676227249675558, -0.06886093055481356, 0.11523896781249253, -0.06621393049135804, -0.13537588525461416, 0.017074824007840394, 0.29530625855422593, -0.29701222474240274, -0.29190076128515885, 0.1185821449226215, -0.2263965933944086, -0.15364493110076818, 0.21190890600940304, -0.0626018100596760... |
708.3569 | The role of the quark and gluon GPDs in hard vector-meson
electroproduction | Electroproduction of light vector mesons is analyzed on the basis of handbag
factorization. The required generalized parton distributions are constructed
from the CTEQ6 parton distributions with the help of double distributions. The
partonic subprocesses are calculated within the modified perturbative approach.
The p... | hep-ph | electroproduction of light vector mesons is analyzed on the basis of handbag factorization the required generalized parton distributions are constructed from the cteq6 parton distributions with the help of double distributions the partonic subprocesses are calculated within the modified perturbative approach the presen... | [['electroproduction', 'of', 'light', 'vector', 'mesons', 'is', 'analyzed', 'on', 'the', 'basis', 'of', 'handbag', 'factorization', 'the', 'required', 'generalized', 'parton', 'distributions', 'are', 'constructed', 'from', 'the', 'cteq6', 'parton', 'distributions', 'with', 'the', 'help', 'of', 'double', 'distributions'... | [-0.03559732868483192, 0.15708040458144082, -0.17171065535053218, 0.13080468443130436, -0.048823246236057265, -0.03183118801711029, -0.014304371467963057, 0.37504177542991546, -0.1865986527838303, -0.20452611210854038, -0.04401066824855087, -0.33197284571973507, -0.036689751634472294, 0.17100563722564593, 0.04741462392... |
708.357 | Coherent destruction of tunneling, dynamic localization and the
Landau-Zener formula | We clarify the internal relationship between the coherent destruction of
tunneling (CDT) for a two-state model and the dynamic localization (DL) for a
one-dimensional tight-binding model, under the periodical driving field. The
time-evolution of the tight-binding model is reproduced from that of the
two-state model b... | cond-mat.mes-hall | we clarify the internal relationship between the coherent destruction of tunneling cdt for a twostate model and the dynamic localization dl for a onedimensional tightbinding model under the periodical driving field the timeevolution of the tightbinding model is reproduced from that of the twostate model by a mapping of... | [['we', 'clarify', 'the', 'internal', 'relationship', 'between', 'the', 'coherent', 'destruction', 'of', 'tunneling', 'cdt', 'for', 'a', 'twostate', 'model', 'and', 'the', 'dynamic', 'localization', 'dl', 'for', 'a', 'onedimensional', 'tightbinding', 'model', 'under', 'the', 'periodical', 'driving', 'field', 'the', 'ti... | [-0.1538497450686901, 0.1375215591048173, -0.08667907679399241, 0.10099089199799176, 0.00301327926640227, -0.13299105013042545, 0.05014840741777449, 0.3423003105320109, -0.2929362582711919, -0.2336790116992101, 0.029337955216054343, -0.23799417592492972, -0.20295817820915898, 0.16546173152757934, -0.0011960758140437233... |
708.3571 | MAGIC multiwavelength observations: policy, and some recent results | MAGIC, 17 meters of diameter, is the world's largest single dish Imaging
Atmospheric Cherenkov Telescope, and reaches in the analysis the lowest energy
threshold (60 GeV) among the VHE gamma detectors. Completed in September 2004,
MAGIC started full operation with its first cycle of data taking in February
2005. MAGI... | astro-ph | magic 17 meters of diameter is the worlds largest single dish imaging atmospheric cherenkov telescope and reaches in the analysis the lowest energy threshold 60 gev among the vhe gamma detectors completed in september 2004 magic started full operation with its first cycle of data taking in february 2005 magic observati... | [['magic', '17', 'meters', 'of', 'diameter', 'is', 'the', 'worlds', 'largest', 'single', 'dish', 'imaging', 'atmospheric', 'cherenkov', 'telescope', 'and', 'reaches', 'in', 'the', 'analysis', 'the', 'lowest', 'energy', 'threshold', '60', 'gev', 'among', 'the', 'vhe', 'gamma', 'detectors', 'completed', 'in', 'september'... | [-0.06605909797813624, 0.1507164477495857, -0.013092824723571539, 0.12138604675294451, -0.08467853720354977, -0.0902883139068401, 0.09332834330001866, 0.40009438179894, -0.13329418094000048, -0.40649183272253925, 0.09936591662887123, -0.3614664043760508, -0.02360849688831036, 0.24294167587793963, -0.004785735262758149,... |
708.3572 | Neutrino spin-flavor oscillations in electromagnetic fields of various
configurations | We study spin-flavor oscillations of Dirac neutrinos with mixing and having
non-zero matrix of magnetic moments in magnetic fields of various
configurations. We discuss constant transversal and twisting magnetic fields.
To describe the dynamics of Dirac neutrinos we use relativistic quantum
mechanics approach based o... | hep-ph hep-th | we study spinflavor oscillations of dirac neutrinos with mixing and having nonzero matrix of magnetic moments in magnetic fields of various configurations we discuss constant transversal and twisting magnetic fields to describe the dynamics of dirac neutrinos we use relativistic quantum mechanics approach based on the ... | [['we', 'study', 'spinflavor', 'oscillations', 'of', 'dirac', 'neutrinos', 'with', 'mixing', 'and', 'having', 'nonzero', 'matrix', 'of', 'magnetic', 'moments', 'in', 'magnetic', 'fields', 'of', 'various', 'configurations', 'we', 'discuss', 'constant', 'transversal', 'and', 'twisting', 'magnetic', 'fields', 'to', 'descr... | [-0.22207707250073774, 0.2809402752450907, 0.004723773827887515, 0.1328405660521517, -0.09916076297635462, -0.08575247108602702, -0.0009083445010178569, 0.3719792880062292, -0.2143142293520105, -0.3028788589177403, -0.034542667464033436, -0.2556702840183653, -0.12028718300497354, 0.1309143313199782, 0.10033761134454564... |
708.3573 | On the Outage Capacity of a Practical Decoder Accounting for Channel
Estimation Inaccuracies | The optimal decoder achieving the outage capacity under imperfect channel
estimation is investigated. First, by searching into the family of nearest
neighbor decoders, which can be easily implemented on most practical coded
modulation systems, we derive a decoding metric that minimizes the average of
the transmission... | cs.IT math.IT | the optimal decoder achieving the outage capacity under imperfect channel estimation is investigated first by searching into the family of nearest neighbor decoders which can be easily implemented on most practical coded modulation systems we derive a decoding metric that minimizes the average of the transmission error... | [['the', 'optimal', 'decoder', 'achieving', 'the', 'outage', 'capacity', 'under', 'imperfect', 'channel', 'estimation', 'is', 'investigated', 'first', 'by', 'searching', 'into', 'the', 'family', 'of', 'nearest', 'neighbor', 'decoders', 'which', 'can', 'be', 'easily', 'implemented', 'on', 'most', 'practical', 'coded', '... | [-0.24232108697943974, 0.008398864369216804, -0.017401580305068932, 0.08876229008709426, -0.002871553340319837, -0.2730654652460656, 0.174358816997912, 0.3999998633948605, -0.2597430767537241, -0.23347273043597513, 0.11563308782721189, -0.2067403769083949, -0.16535039020772876, 0.18462311732451944, -0.1608114174117198,... |
708.3574 | Nonadiabatic charge pumping in a one-dimensional system of
noninteracting electrons by an oscillating potential | Using a tight-binding model, we study one-parameter charge pumping in a
one-dimensional system of non-interacting electrons. An oscillating potential
is applied at one site while a static potential is applied in a different
region. Using Floquet scattering theory, we calculate the current up to second
order in the os... | cond-mat.mes-hall | using a tightbinding model we study oneparameter charge pumping in a onedimensional system of noninteracting electrons an oscillating potential is applied at one site while a static potential is applied in a different region using floquet scattering theory we calculate the current up to second order in the oscillation ... | [['using', 'a', 'tightbinding', 'model', 'we', 'study', 'oneparameter', 'charge', 'pumping', 'in', 'a', 'onedimensional', 'system', 'of', 'noninteracting', 'electrons', 'an', 'oscillating', 'potential', 'is', 'applied', 'at', 'one', 'site', 'while', 'a', 'static', 'potential', 'is', 'applied', 'in', 'a', 'different', '... | [-0.15578554469160735, 0.1787162488956043, -0.06378182351278762, 0.027525183411780743, -0.009261356599939366, -0.11463567404697339, 0.10299248326802626, 0.3361241740795473, -0.24757672358925145, -0.24483412202447652, 0.07901195660776769, -0.2990110059827566, -0.10267557626745354, 0.17739780615083872, 0.0325529319139119... |
708.3575 | How really effective are Multimodal Hints in enhancing Visual Target
Spotting? Some evidence from a usability study | The main aim of the work presented here is to contribute to computer science
advances in the multimodal usability area, in-as-much as it addresses one of
the major issues relating to the generation of effective oral system messages:
how to design messages which effectively help users to locate specific
graphical obje... | cs.HC | the main aim of the work presented here is to contribute to computer science advances in the multimodal usability area inasmuch as it addresses one of the major issues relating to the generation of effective oral system messages how to design messages which effectively help users to locate specific graphical objects in... | [['the', 'main', 'aim', 'of', 'the', 'work', 'presented', 'here', 'is', 'to', 'contribute', 'to', 'computer', 'science', 'advances', 'in', 'the', 'multimodal', 'usability', 'area', 'inasmuch', 'as', 'it', 'addresses', 'one', 'of', 'the', 'major', 'issues', 'relating', 'to', 'the', 'generation', 'of', 'effective', 'oral... | [-0.08599177975897153, 0.03058648248188149, -0.06343988919264225, 0.08050868824401697, -0.1629839437845789, -0.15644505611351117, 0.07197670908256744, 0.43626883532343014, -0.25372624396832527, -0.3754678856113244, 0.10014505585836236, -0.2895467156478168, -0.15949682586080818, 0.1942201807313787, -0.12157872898387723,... |
708.3576 | Canonical Hilbert-Burch matrices for ideals of $k[x,y]$ | An Artinian ideal $I$ of $k[x,y]$ has many Hilbert-Burch matrices. We show
that there is a canonical choice. As an application, we determine the dimension
of certain affine Gr\"obner cells and their Betti strata recovering results of
Ellingsrud and Str{\o}mme, G\"ottsche and Iarrobino.
| math.AC math.AG | an artinian ideal i of kxy has many hilbertburch matrices we show that there is a canonical choice as an application we determine the dimension of certain affine grobner cells and their betti strata recovering results of ellingsrud and stromme gottsche and iarrobino | [['an', 'artinian', 'ideal', 'i', 'of', 'kxy', 'has', 'many', 'hilbertburch', 'matrices', 'we', 'show', 'that', 'there', 'is', 'a', 'canonical', 'choice', 'as', 'an', 'application', 'we', 'determine', 'the', 'dimension', 'of', 'certain', 'affine', 'grobner', 'cells', 'and', 'their', 'betti', 'strata', 'recovering', 're... | [-0.17968945482442544, 0.01912780525771966, -0.04302908709749233, 0.05653405247180354, -0.05037249593324093, -0.1640319141862524, -0.04085860472865576, 0.34117036200193473, -0.3331824820921865, -0.13673258882535752, 0.12225730053344092, -0.257055577150611, -0.2006962284619032, 0.18919635512108027, -0.19040226195614005,... |
708.3577 | An Equilibrium Balance of the Universe | An alternative cosmological model is presented, which avoids the requirement
of dark energy and dark matter. Based on the proposition that energy
conservation should be valid not only locally but also globally, the energy
tensor of general relativity has to be corrected, including potential energy of
matter explicitl... | physics.gen-ph | an alternative cosmological model is presented which avoids the requirement of dark energy and dark matter based on the proposition that energy conservation should be valid not only locally but also globally the energy tensor of general relativity has to be corrected including potential energy of matter explicitly this... | [['an', 'alternative', 'cosmological', 'model', 'is', 'presented', 'which', 'avoids', 'the', 'requirement', 'of', 'dark', 'energy', 'and', 'dark', 'matter', 'based', 'on', 'the', 'proposition', 'that', 'energy', 'conservation', 'should', 'be', 'valid', 'not', 'only', 'locally', 'but', 'also', 'globally', 'the', 'energy... | [-0.09100345349135368, 0.1677603637225203, -0.12443278408854415, 0.11778816704478998, -0.09681530569827086, -0.06941856958560254, -0.008899292017112634, 0.34943795571544845, -0.22502067439062032, -0.3343486638690688, 0.040959790062257334, -0.24423189744794446, -0.049046230012563204, 0.1521902015337745, -0.0082228716021... |
708.3578 | Relative Hyperbolicity, Trees of Spaces and Cannon-Thurston Maps | We prove the existence of continuous boundary extensions (Cannon-Thurston
maps) for the inclusion of a vertex space into a tree of (strongly) relatively
hyperbolic spaces satisfying the qi-embedded condition. This implies the same
result for inclusion of vertex (or edge) subgroups in finite graphs of
(strongly) relat... | math.GR math.GT | we prove the existence of continuous boundary extensions cannonthurston maps for the inclusion of a vertex space into a tree of strongly relatively hyperbolic spaces satisfying the qiembedded condition this implies the same result for inclusion of vertex or edge subgroups in finite graphs of strongly relatively hyperbo... | [['we', 'prove', 'the', 'existence', 'of', 'continuous', 'boundary', 'extensions', 'cannonthurston', 'maps', 'for', 'the', 'inclusion', 'of', 'a', 'vertex', 'space', 'into', 'a', 'tree', 'of', 'strongly', 'relatively', 'hyperbolic', 'spaces', 'satisfying', 'the', 'qiembedded', 'condition', 'this', 'implies', 'the', 'sa... | [-0.19396536834013295, 0.14934430023799586, -0.07603416313141795, 0.10332997658447375, -0.09581625584880231, -0.10599533248115593, 0.04945283051265378, 0.3305265159005116, -0.2749550700659903, -0.2089035996353962, 0.1265295508389794, -0.2663641609120327, -0.1211353437351981, 0.1957522849847471, -0.15707660735663498, 0.... |
708.3579 | The Nature of the Gould Belt from a Fractal Analysis of its Stellar
Population | The Gould Belt (GB) is a system of gas and young, bright stars distributed
along a plane that is inclined with respect to the main plane of the Milky Way.
Observational evidence suggests that the GB is our closest star formation
complex, but its true nature and origin remain rather controversial. In this
work we anal... | astro-ph | the gould belt gb is a system of gas and young bright stars distributed along a plane that is inclined with respect to the main plane of the milky way observational evidence suggests that the gb is our closest star formation complex but its true nature and origin remain rather controversial in this work we analyze the ... | [['the', 'gould', 'belt', 'gb', 'is', 'a', 'system', 'of', 'gas', 'and', 'young', 'bright', 'stars', 'distributed', 'along', 'a', 'plane', 'that', 'is', 'inclined', 'with', 'respect', 'to', 'the', 'main', 'plane', 'of', 'the', 'milky', 'way', 'observational', 'evidence', 'suggests', 'that', 'the', 'gb', 'is', 'our', 'c... | [-0.0912308975161674, 0.08462341332515713, -0.1047993401775048, 0.11657374684277567, -0.10146671620951522, -0.02161821720988623, 0.053404790964642804, 0.387323692157155, -0.1982409772596189, -0.3026165514178241, 0.05066369432565158, -0.24476279806500922, -0.09018953006625885, 0.19750835822418422, -0.07974803109342853, ... |
708.358 | Ambient Multimodality: an Asset for Developing Universal Access to the
Information Society | The paper tries to point out the benefits that can be derived from research
advances in the implementation of concepts such as ambient intelligence (AmI)
and ubiquitous or pervasive computing for promoting Universal Access (UA) to
the Information Society, that is, for contributing to enable everybody,
especially Phys... | cs.HC | the paper tries to point out the benefits that can be derived from research advances in the implementation of concepts such as ambient intelligence ami and ubiquitous or pervasive computing for promoting universal access ua to the information society that is for contributing to enable everybody especially physically di... | [['the', 'paper', 'tries', 'to', 'point', 'out', 'the', 'benefits', 'that', 'can', 'be', 'derived', 'from', 'research', 'advances', 'in', 'the', 'implementation', 'of', 'concepts', 'such', 'as', 'ambient', 'intelligence', 'ami', 'and', 'ubiquitous', 'or', 'pervasive', 'computing', 'for', 'promoting', 'universal', 'acce... | [-0.10590570475427588, 0.06562172191108488, -0.05635315165652529, 0.058927871067382454, -0.1648510908201823, -0.20469059196591613, 0.050398436137760357, 0.40107342658247874, -0.26027156335159973, -0.30789584294697747, 0.1185508380108421, -0.29282162126462924, -0.1274794525132798, 0.22941135993805298, -0.112092955903013... |
708.3581 | Hyper-atoms and the Kemperman's critical pair Theory | In the present work, we introduce the notion of a hyper-atom and prove their
main structure theorem. We then apply the global isoperimetric methodology to
give a new proof for
Kemperman's structure Theory and a slight improvement.
| math.NT math.CO | in the present work we introduce the notion of a hyperatom and prove their main structure theorem we then apply the global isoperimetric methodology to give a new proof for kempermans structure theory and a slight improvement | [['in', 'the', 'present', 'work', 'we', 'introduce', 'the', 'notion', 'of', 'a', 'hyperatom', 'and', 'prove', 'their', 'main', 'structure', 'theorem', 'we', 'then', 'apply', 'the', 'global', 'isoperimetric', 'methodology', 'to', 'give', 'a', 'new', 'proof', 'for', 'kempermans', 'structure', 'theory', 'and', 'a', 'sligh... | [-0.10615944513749029, -0.015450070536619908, -0.18477432543059458, 0.10112674511667039, -0.08914889954030514, -0.09587251204946959, 0.08939628338604863, 0.31421111690232884, -0.2993516946035261, -0.27819120804653374, 0.08826807016393522, -0.1703909574378584, -0.23308298490136056, 0.14776809297099308, -0.15541129159061... |
708.3582 | HORPO with Computability Closure : A Reconstruction | This paper provides a new, decidable definition of the higher- order
recursive path ordering in which type comparisons are made only when needed,
therefore eliminating the need for the computability clo- sure, and bound
variables are handled explicitly, making it possible to handle recursors for
arbitrary strictly po... | cs.LO | this paper provides a new decidable definition of the higher order recursive path ordering in which type comparisons are made only when needed therefore eliminating the need for the computability clo sure and bound variables are handled explicitly making it possible to handle recursors for arbitrary strictly positive i... | [['this', 'paper', 'provides', 'a', 'new', 'decidable', 'definition', 'of', 'the', 'higher', 'order', 'recursive', 'path', 'ordering', 'in', 'which', 'type', 'comparisons', 'are', 'made', 'only', 'when', 'needed', 'therefore', 'eliminating', 'the', 'need', 'for', 'the', 'computability', 'clo', 'sure', 'and', 'bound', '... | [-0.1259422018667873, 0.14056830564323736, -0.019122678159298946, 0.15566325927751937, -0.1736458713017708, -0.21438958658361618, 0.10957331372168372, 0.3597472226437257, -0.26145758297370403, -0.30352544541261633, 0.11438904629250495, -0.21001783370667573, -0.10674684261903167, 0.16258539103579764, -0.0898136192438553... |
708.3583 | Defining Relations of Low Degree of Invariants of Two $4 \times 4$
Matrices | Over a field K of characteristic 0, we study the algebra of invariants of the
general linear group GL(4,K) acting by simultaneous conjugation on two matrices
of order 4. It coincides with the trace algebra generated by all traces of
products of two generic matrices of order 4. It is known that the minimal
degree of t... | math.RA math.AC | over a field k of characteristic 0 we study the algebra of invariants of the general linear group gl4k acting by simultaneous conjugation on two matrices of order 4 it coincides with the trace algebra generated by all traces of products of two generic matrices of order 4 it is known that the minimal degree of the defin... | [['over', 'a', 'field', 'k', 'of', 'characteristic', '0', 'we', 'study', 'the', 'algebra', 'of', 'invariants', 'of', 'the', 'general', 'linear', 'group', 'gl4k', 'acting', 'by', 'simultaneous', 'conjugation', 'on', 'two', 'matrices', 'of', 'order', '4', 'it', 'coincides', 'with', 'the', 'trace', 'algebra', 'generated',... | [-0.15576544110181517, 0.10775034084859915, -0.036848810200322546, 0.005306683673427023, -0.05945113436961225, -0.09944581016416437, -0.0064220943875562654, 0.33483070003446835, -0.28062445619785836, -0.2937627351634076, 0.12195873499350172, -0.2530416977623927, -0.16610945725074872, 0.2067096253138453, -0.009023177164... |
708.3584 | Globular realization and cubical underlying homotopy type of time flow
of process algebra | We construct a small realization as flow of every precubical set (modeling
for example a process algebra). The realization is small in the sense that the
construction does not make use of any cofibrant replacement functor and of any
transfinite construction. In particular, if the precubical set is finite, then
the co... | math.AT math.CT | we construct a small realization as flow of every precubical set modeling for example a process algebra the realization is small in the sense that the construction does not make use of any cofibrant replacement functor and of any transfinite construction in particular if the precubical set is finite then the correspond... | [['we', 'construct', 'a', 'small', 'realization', 'as', 'flow', 'of', 'every', 'precubical', 'set', 'modeling', 'for', 'example', 'a', 'process', 'algebra', 'the', 'realization', 'is', 'small', 'in', 'the', 'sense', 'that', 'the', 'construction', 'does', 'not', 'make', 'use', 'of', 'any', 'cofibrant', 'replacement', 'f... | [-0.11842861146266971, 0.08090061103471921, -0.06150583001518888, 0.06192965850961433, -0.14289599877832057, -0.11698843760366019, -0.007486157429022049, 0.3406056794525024, -0.3621160339431039, -0.19976314683195337, 0.11592854517220985, -0.2300790896998868, -0.1348737484409607, 0.19074645181119973, -0.1538966438342218... |
708.3585 | Critical conductance of the chiral 2d random flux model | The two-terminal conductance of a random flux model defined on a square
lattice is investigated numerically at the band center using a transfer matrix
method. Due to the chiral symmetry, there exists a critical point where the
ensemble averaged mean conductance is scale independent. We also study the
conductance dist... | cond-mat.mes-hall | the twoterminal conductance of a random flux model defined on a square lattice is investigated numerically at the band center using a transfer matrix method due to the chiral symmetry there exists a critical point where the ensemble averaged mean conductance is scale independent we also study the conductance distributi... | [['the', 'twoterminal', 'conductance', 'of', 'a', 'random', 'flux', 'model', 'defined', 'on', 'a', 'square', 'lattice', 'is', 'investigated', 'numerically', 'at', 'the', 'band', 'center', 'using', 'a', 'transfer', 'matrix', 'method', 'due', 'to', 'the', 'chiral', 'symmetry', 'there', 'exists', 'a', 'critical', 'point',... | [-0.17193991566051003, 0.16476297677770532, -0.06771460239327064, 0.04544508300777697, 0.010886828703439311, -0.1530989267220893, 0.07056538907690318, 0.3546398700111442, -0.26265059111217315, -0.25683386925676904, 0.08787271374280357, -0.2990691941231489, -0.15885220550181758, 0.18027283582206885, 0.008094092770652086... |
708.3586 | Calculations of $^{6}$He+p elastic scattering cross sections using
folding approach and high-energy approximation for the optical potential | Calculations of microscopic optical potentials (OP's) (their real and
imaginary parts) are performed to analyze the $^6$He+p elastic scattering data
at a few tens of MeV/nucleon (MeV/N). The OP's and the cross sections are
calculated using three model densities of $^6$He. Effects of the regularization
of the NN force... | nucl-th | calculations of microscopic optical potentials ops their real and imaginary parts are performed to analyze the 6hep elastic scattering data at a few tens of mevnucleon mevn the ops and the cross sections are calculated using three model densities of 6he effects of the regularization of the nn forces and their dependenc... | [['calculations', 'of', 'microscopic', 'optical', 'potentials', 'ops', 'their', 'real', 'and', 'imaginary', 'parts', 'are', 'performed', 'to', 'analyze', 'the', '6hep', 'elastic', 'scattering', 'data', 'at', 'a', 'few', 'tens', 'of', 'mevnucleon', 'mevn', 'the', 'ops', 'and', 'the', 'cross', 'sections', 'are', 'calcula... | [-0.11059408863851179, 0.1182644340571844, -0.08460156567377487, 0.09266020401587917, 0.02836546444989465, -0.0424036083449782, -0.0041447111612392794, 0.38196850171381674, -0.21044621650233036, -0.3296525169301916, 0.030082405418700848, -0.3538868940193896, -0.044320677441579324, 0.1723941697812363, 0.1100750315623978... |
708.3587 | Fixed points of smooth varieties with Kodaira dimension zero | In this paper, we study the growth of the number of fixed points from
iterating an endomorphism of an abelian variety. Using the estimates obtained
on an abelian variety, we are able to extend the results to endomorphisms on
varieties of Kodaira dimension zero and more generally their periodic
subvarieties.
| math.AG | in this paper we study the growth of the number of fixed points from iterating an endomorphism of an abelian variety using the estimates obtained on an abelian variety we are able to extend the results to endomorphisms on varieties of kodaira dimension zero and more generally their periodic subvarieties | [['in', 'this', 'paper', 'we', 'study', 'the', 'growth', 'of', 'the', 'number', 'of', 'fixed', 'points', 'from', 'iterating', 'an', 'endomorphism', 'of', 'an', 'abelian', 'variety', 'using', 'the', 'estimates', 'obtained', 'on', 'an', 'abelian', 'variety', 'we', 'are', 'able', 'to', 'extend', 'the', 'results', 'to', 'e... | [-0.1451748739811592, 0.060372728135844225, -0.08107046271674336, 0.01534390366403386, -0.07642977877985686, -0.0730252532288432, 0.01631944107590243, 0.3246366510074586, -0.30531880524009464, -0.1906321842595935, 0.11895989767974242, -0.2714907593280077, -0.136727212369442, 0.2926308222860098, -0.1902088985964656, 0.0... |
708.3588 | Electron-phonon coupling in a two-dimensional inhomogeneous electron
gas: consequences for surface spectral properties | We investigate the coupling of an inhomogeneous electron system to phonons.
The properties of an electronic system composed of a mixture of microscopic
ordered and disordered islands are changed fundamentally by a phonon mode. In
high-Tc cuprates, such a phase separation scenario is supported by recent STM
and nuclea... | cond-mat.supr-con cond-mat.str-el | we investigate the coupling of an inhomogeneous electron system to phonons the properties of an electronic system composed of a mixture of microscopic ordered and disordered islands are changed fundamentally by a phonon mode in hightc cuprates such a phase separation scenario is supported by recent stm and nuclear quad... | [['we', 'investigate', 'the', 'coupling', 'of', 'an', 'inhomogeneous', 'electron', 'system', 'to', 'phonons', 'the', 'properties', 'of', 'an', 'electronic', 'system', 'composed', 'of', 'a', 'mixture', 'of', 'microscopic', 'ordered', 'and', 'disordered', 'islands', 'are', 'changed', 'fundamentally', 'by', 'a', 'phonon',... | [-0.19047713675813394, 0.20998448089369395, -0.08786690491473391, 0.06510225749197637, -0.03854143029699723, -0.14721539649624554, 0.06763997884866382, 0.37379886049089867, -0.2773210829212552, -0.24534548945458873, -0.024778206197411886, -0.30504231436976365, -0.12852994691181396, 0.16643984925134905, 0.04533226336130... |
708.3589 | A First Principles Theory of Nuclear Magnetic Resonance J-Coupling in
solid-state systems | A method to calculate NMR J-coupling constants from first principles in
extended systems is presented. It is based on density functional theory and is
formulated within a planewave-pseudopotential framework. The all-electron
properties are recovered using the projector augmented wave approach. The
method is validated... | cond-mat.mtrl-sci | a method to calculate nmr jcoupling constants from first principles in extended systems is presented it is based on density functional theory and is formulated within a planewavepseudopotential framework the allelectron properties are recovered using the projector augmented wave approach the method is validated by comp... | [['a', 'method', 'to', 'calculate', 'nmr', 'jcoupling', 'constants', 'from', 'first', 'principles', 'in', 'extended', 'systems', 'is', 'presented', 'it', 'is', 'based', 'on', 'density', 'functional', 'theory', 'and', 'is', 'formulated', 'within', 'a', 'planewavepseudopotential', 'framework', 'the', 'allelectron', 'prop... | [-0.06370393188157375, 0.017313336845541347, -0.14318277494074183, 0.0407119229287449, 0.005456048131420993, -0.10627937144802316, 0.014523136296201552, 0.39769827906528243, -0.22310009170863507, -0.3045933643706899, 0.07016091130714378, -0.26829231375882373, -0.17241167416121217, 0.22688568209001012, 0.054014004871546... |
708.359 | Torus knots are Fourier-(1,1,2) knots | Every torus knot can be represented as a Fourier-(1,1,2) knot which is the
simplest possible Fourier representation for such a knot. This answers a
question of Kauffman and confirms the conjecture made by Boocher, Daigle, Hoste
and Zheng.
In particular, the torus knot T(p,q) can be parameterized as x(t)=cos(pt),
y(... | math.GT | every torus knot can be represented as a fourier112 knot which is the simplest possible fourier representation for such a knot this answers a question of kauffman and confirms the conjecture made by boocher daigle hoste and zheng in particular the torus knot tpq can be parameterized as xtcospt ytcosqtpi2p and ztcosptpi... | [['every', 'torus', 'knot', 'can', 'be', 'represented', 'as', 'a', 'fourier112', 'knot', 'which', 'is', 'the', 'simplest', 'possible', 'fourier', 'representation', 'for', 'such', 'a', 'knot', 'this', 'answers', 'a', 'question', 'of', 'kauffman', 'and', 'confirms', 'the', 'conjecture', 'made', 'by', 'boocher', 'daigle',... | [-0.1940700698760338, 0.08925797666112582, -0.12744859545879686, 0.07594628942509492, -0.13002281608836105, -0.21276806214397462, 0.015718480009430397, 0.32647890062071383, -0.30451219806370017, -0.29998376007036615, 0.11894445081270533, -0.1715950140642235, -0.1988525919150561, 0.20441471620385224, -0.1537705208756961... |
708.3591 | Non commutative functional calculus: bounded operators | In this paper we develop a functional calculus for bounded operators defined
on quaternionic Banach spaces. This calculus is based on the notion of
slice-regularity, see \cite{gs}, and the key tools are a new resolvent operator
and a new eigenvalue problem.
| math.SP | in this paper we develop a functional calculus for bounded operators defined on quaternionic banach spaces this calculus is based on the notion of sliceregularity see citegs and the key tools are a new resolvent operator and a new eigenvalue problem | [['in', 'this', 'paper', 'we', 'develop', 'a', 'functional', 'calculus', 'for', 'bounded', 'operators', 'defined', 'on', 'quaternionic', 'banach', 'spaces', 'this', 'calculus', 'is', 'based', 'on', 'the', 'notion', 'of', 'sliceregularity', 'see', 'citegs', 'and', 'the', 'key', 'tools', 'are', 'a', 'new', 'resolvent', '... | [-0.09418229542206973, 0.036409411136992274, -0.1212709033396095, 0.14507644035329575, -0.14317681657266804, -0.09872877394082025, 0.02149101083923597, 0.3094937538728118, -0.3314145490527153, -0.16089431000873447, 0.13778593074239326, -0.25347197726368903, -0.23254705388098956, 0.18678066215943545, -0.2060735940700397... |
708.3592 | Non commutative functional calculus: unbounded operators | In a recent work, \cite{cgss}, we developed a functional calculus for bounded
operators defined on quaternionic Banach spaces. In this paper we show how the
results from \cite{cgss} can be extended to the unbounded case, and we
highlight the crucial differences between the two cases. In particular, we
deduce a new ei... | math.SP | in a recent work citecgss we developed a functional calculus for bounded operators defined on quaternionic banach spaces in this paper we show how the results from citecgss can be extended to the unbounded case and we highlight the crucial differences between the two cases in particular we deduce a new eigenvalue equat... | [['in', 'a', 'recent', 'work', 'citecgss', 'we', 'developed', 'a', 'functional', 'calculus', 'for', 'bounded', 'operators', 'defined', 'on', 'quaternionic', 'banach', 'spaces', 'in', 'this', 'paper', 'we', 'show', 'how', 'the', 'results', 'from', 'citecgss', 'can', 'be', 'extended', 'to', 'the', 'unbounded', 'case', 'a... | [-0.09420310099845502, 0.06289007124810744, -0.1022041533420335, 0.11457725483646143, -0.08246118601050172, -0.08329346895551504, 0.009301381578335344, 0.3644897519652523, -0.299141247047862, -0.2159829063813633, 0.11603599168367183, -0.2518283092041514, -0.2427531136616842, 0.22545393617517911, -0.12906935755441437, 0... |
708.3593 | A hidden solution to the mu/B_mu problem in gauge mediation | We propose a solution to the mu/B_mu problem in gauge mediation. The novel
feature of our solution is that it uses dynamics of the hidden sector, which is
often present in models with dynamical supersymmetry breaking. We give an
explicit example model of gauge mediation where a very simple messenger sector
generates ... | hep-ph hep-th | we propose a solution to the mub_mu problem in gauge mediation the novel feature of our solution is that it uses dynamics of the hidden sector which is often present in models with dynamical supersymmetry breaking we give an explicit example model of gauge mediation where a very simple messenger sector generates both m... | [['we', 'propose', 'a', 'solution', 'to', 'the', 'mub_mu', 'problem', 'in', 'gauge', 'mediation', 'the', 'novel', 'feature', 'of', 'our', 'solution', 'is', 'that', 'it', 'uses', 'dynamics', 'of', 'the', 'hidden', 'sector', 'which', 'is', 'often', 'present', 'in', 'models', 'with', 'dynamical', 'supersymmetry', 'breakin... | [-0.12754706697446774, 0.17383421906186303, -0.10050174448935484, 0.12735301806859559, -0.17263438574137221, -0.20122396347384588, 0.03788699088600521, 0.30829173964307166, -0.28413277419961314, -0.31527303206508583, 0.1064076793819285, -0.22535403850181893, -0.16257006671477223, 0.12080274176409919, -0.014754576726717... |
708.3594 | A new functional calculus for non-commuting operators | In this paper we use the notion of slice monogenic functions \cite{slicecss}
to define a new functional calculus for an $n$-tuple $T$ of not necessarily
commuting operators. This calculus is different from the one discussed in
\cite{jefferies} and it allows the explicit construction of the eigenvalue
equation for the... | math.SP | in this paper we use the notion of slice monogenic functions citeslicecss to define a new functional calculus for an ntuple t of not necessarily commuting operators this calculus is different from the one discussed in citejefferies and it allows the explicit construction of the eigenvalue equation for the ntuple t base... | [['in', 'this', 'paper', 'we', 'use', 'the', 'notion', 'of', 'slice', 'monogenic', 'functions', 'citeslicecss', 'to', 'define', 'a', 'new', 'functional', 'calculus', 'for', 'an', 'ntuple', 't', 'of', 'not', 'necessarily', 'commuting', 'operators', 'this', 'calculus', 'is', 'different', 'from', 'the', 'one', 'discussed'... | [-0.09463338906297812, 0.07523479930151135, -0.12280699868711668, 0.07628890212524582, -0.09735232578728951, -0.10482469131238759, 0.014511008660397114, 0.3122683501726872, -0.31644872550827424, -0.21839254331850522, 0.06469059363636817, -0.26646754711672094, -0.17019772919750698, 0.1721296729394109, -0.118346494383405... |
708.3595 | Slice monogenic functions | In this paper we offer a definition of monogenicity for functions defined on
$\rr^{n+1}$ with values in the Clifford algebra $\rr_n$ following an idea
inspired by the recent papers \cite{gs}, \cite{advances}. This new class of
monogenic functions contains the polynomials (and, more in general, power
series) with coef... | math.CV | in this paper we offer a definition of monogenicity for functions defined on rrn1 with values in the clifford algebra rr_n following an idea inspired by the recent papers citegs citeadvances this new class of monogenic functions contains the polynomials and more in general power series with coefficients in the clifford... | [['in', 'this', 'paper', 'we', 'offer', 'a', 'definition', 'of', 'monogenicity', 'for', 'functions', 'defined', 'on', 'rrn1', 'with', 'values', 'in', 'the', 'clifford', 'algebra', 'rr_n', 'following', 'an', 'idea', 'inspired', 'by', 'the', 'recent', 'papers', 'citegs', 'citeadvances', 'this', 'new', 'class', 'of', 'mon... | [-0.13735606269881082, 0.03980683668860598, -0.07406701052036041, 0.03188436053012712, -0.10941494625205031, -0.07759870496244194, -0.031009586204070214, 0.3110373083454294, -0.29066329057782125, -0.20335859871015716, 0.12265959812793881, -0.26921603076446515, -0.2165703129930756, 0.25447441222002876, -0.15480247564100... |
708.3596 | Chemical analysis and aqueous solution properties of Charged Amphiphilic
Block Copolymers PBA-b-PAA synthesized by MADIX | We have linked the structural and dynamic properties in aqueous solution of
amphiphilic charged diblock copolymers poly(butyl acrylate)-b-poly(acrylic
acid), PBA-b-PAA, synthesized by controlled radical polymerization, with the
physico-chemical characteristics of the samples. Despite product imperfections,
the sample... | cond-mat.soft | we have linked the structural and dynamic properties in aqueous solution of amphiphilic charged diblock copolymers polybutyl acrylatebpolyacrylic acid pbabpaa synthesized by controlled radical polymerization with the physicochemical characteristics of the samples despite product imperfections the samples selfassemble i... | [['we', 'have', 'linked', 'the', 'structural', 'and', 'dynamic', 'properties', 'in', 'aqueous', 'solution', 'of', 'amphiphilic', 'charged', 'diblock', 'copolymers', 'polybutyl', 'acrylatebpolyacrylic', 'acid', 'pbabpaa', 'synthesized', 'by', 'controlled', 'radical', 'polymerization', 'with', 'the', 'physicochemical', '... | [-0.12234210409421091, 0.21221152467478532, -0.07213732806849293, 0.01397331892621878, 0.03844668478510963, -0.16439808436795525, 0.03705405877250693, 0.39147432597261894, -0.2761253561839112, -0.3047118759665561, 0.060696091842146416, -0.30812940022830543, -0.07549979445320787, 0.059235569122696084, 0.0405474418748781... |
708.3597 | Equilibrium Configurations of Strongly Magnetized Neutron Stars with
Realistic Equations of State | We investigate equilibrium sequences of magnetized rotating stars with four
kinds of realistic equations of state (EOSs) of SLy (Douchin et al.), FPS
(Pandharipande et al.), Shen (Shen et al.), and LS (Lattimer & Swesty).
Employing the Tomimura-Eriguchi scheme to construct the equilibrium
configurations. we study the... | astro-ph gr-qc | we investigate equilibrium sequences of magnetized rotating stars with four kinds of realistic equations of state eoss of sly douchin et al fps pandharipande et al shen shen et al and ls lattimer swesty employing the tomimuraeriguchi scheme to construct the equilibrium configurations we study the basic physical propert... | [['we', 'investigate', 'equilibrium', 'sequences', 'of', 'magnetized', 'rotating', 'stars', 'with', 'four', 'kinds', 'of', 'realistic', 'equations', 'of', 'state', 'eoss', 'of', 'sly', 'douchin', 'et', 'al', 'fps', 'pandharipande', 'et', 'al', 'shen', 'shen', 'et', 'al', 'and', 'ls', 'lattimer', 'swesty', 'employing', ... | [-0.11028492808045827, 0.1794959720245209, -0.0805544614447008, 0.09435796993833316, -0.1008623047258362, -0.055744331592117204, 0.037183361700794434, 0.3087754529437136, -0.15765373744304334, -0.3608124692257977, 0.042820846142683756, -0.2451783791135716, -0.04142038424978633, 0.20346627219786642, -0.01986998427005594... |
708.3598 | Variations on Homological Reduction | In this paper, we are concerned with the BFV-reduction of first class
constraints in classsical Hamiltonian mechanics and deformation quantization.
As a result, we obtain continuous star products for certain singular reduced
symplectic quotients. We relate the notion of "irreducibility" of a constraint
to the notion ... | math.QA math-ph math.MP | in this paper we are concerned with the bfvreduction of first class constraints in classsical hamiltonian mechanics and deformation quantization as a result we obtain continuous star products for certain singular reduced symplectic quotients we relate the notion of irreducibility of a constraint to the notion of comple... | [['in', 'this', 'paper', 'we', 'are', 'concerned', 'with', 'the', 'bfvreduction', 'of', 'first', 'class', 'constraints', 'in', 'classsical', 'hamiltonian', 'mechanics', 'and', 'deformation', 'quantization', 'as', 'a', 'result', 'we', 'obtain', 'continuous', 'star', 'products', 'for', 'certain', 'singular', 'reduced', '... | [-0.18490186192314415, 0.07412912217790589, -0.07644063874750454, 0.09584549794055741, -0.1217205505927696, -0.0932919324046987, -0.012860557106871376, 0.3009275040534489, -0.32312209115308876, -0.23643680977470735, 0.1069574729703805, -0.20920573024846176, -0.17929401525265454, 0.18423585213227744, -0.1905593825285049... |
708.3599 | Enzyme localization can drastically affect signal amplification in
signal transduction pathways | Push-pull networks are ubiquitous in signal transduction pathways in both
prokaryotic and eukaryotic cells. They allow cells to strongly amplify signals
via the mechanism of zero-order ultrasensitivity. In a push-pull network, two
antagonistic enzymes control the activity of a protein by covalent
modification. These ... | q-bio.MN | pushpull networks are ubiquitous in signal transduction pathways in both prokaryotic and eukaryotic cells they allow cells to strongly amplify signals via the mechanism of zeroorder ultrasensitivity in a pushpull network two antagonistic enzymes control the activity of a protein by covalent modification these enzymes a... | [['pushpull', 'networks', 'are', 'ubiquitous', 'in', 'signal', 'transduction', 'pathways', 'in', 'both', 'prokaryotic', 'and', 'eukaryotic', 'cells', 'they', 'allow', 'cells', 'to', 'strongly', 'amplify', 'signals', 'via', 'the', 'mechanism', 'of', 'zeroorder', 'ultrasensitivity', 'in', 'a', 'pushpull', 'network', 'two... | [-0.12757720456111354, 0.20182021977222067, -0.009651305222368173, 0.052026780658943506, -0.005680677381023175, -0.15085246700972402, 0.04183975831305577, 0.42413289703975965, -0.31570551396047664, -0.23758039199668218, 0.06909652303320245, -0.24681262951344252, -0.23956148347838407, 0.19016987321066992, -0.05549996830... |
708.36 | Supersymmetric Candidates for Dark Matter (in German) | The identity of dark matter is one of the greatest puzzles of our Universe.
Its solution may be associated with supersymmetry which is a fundamental
space-time symmetry that has not been verified experimentally so far. In many
supersymmetric extensions of the Standard Model of particle physics, the
lightest supersymm... | hep-ph astro-ph hep-ex physics.pop-ph | the identity of dark matter is one of the greatest puzzles of our universe its solution may be associated with supersymmetry which is a fundamental spacetime symmetry that has not been verified experimentally so far in many supersymmetric extensions of the standard model of particle physics the lightest supersymmetric ... | [['the', 'identity', 'of', 'dark', 'matter', 'is', 'one', 'of', 'the', 'greatest', 'puzzles', 'of', 'our', 'universe', 'its', 'solution', 'may', 'be', 'associated', 'with', 'supersymmetry', 'which', 'is', 'a', 'fundamental', 'spacetime', 'symmetry', 'that', 'has', 'not', 'been', 'verified', 'experimentally', 'so', 'far... | [-0.08531606694382123, 0.21613887057935832, -0.11822257688104668, 0.16663680294672412, -0.12887207132435458, -0.17797030815032913, -0.04496233245248304, 0.28799331406377915, -0.2271803638432175, -0.34326012128251876, 0.0930767096709186, -0.2815770438625751, -0.01165030579055276, 0.18631075572510086, 0.05905076861107612... |
708.3601 | A correlated topic model of Science | Topic models, such as latent Dirichlet allocation (LDA), can be useful tools
for the statistical analysis of document collections and other discrete data.
The LDA model assumes that the words of each document arise from a mixture of
topics, each of which is a distribution over the vocabulary. A limitation of
LDA is t... | stat.AP | topic models such as latent dirichlet allocation lda can be useful tools for the statistical analysis of document collections and other discrete data the lda model assumes that the words of each document arise from a mixture of topics each of which is a distribution over the vocabulary a limitation of lda is the inabil... | [['topic', 'models', 'such', 'as', 'latent', 'dirichlet', 'allocation', 'lda', 'can', 'be', 'useful', 'tools', 'for', 'the', 'statistical', 'analysis', 'of', 'document', 'collections', 'and', 'other', 'discrete', 'data', 'the', 'lda', 'model', 'assumes', 'that', 'the', 'words', 'of', 'each', 'document', 'arise', 'from'... | [0.004895083197903096, 0.02013247632748048, -0.1104069284546345, 0.12228570866095952, -0.15010560118371083, -0.13050960724331856, 0.08904259558235234, 0.3661952343802464, -0.30212219386021155, -0.30853733211178996, 0.08479982911996771, -0.30594790628390284, -0.13561158803962928, 0.1568433422421526, -0.07161316679150036... |
708.3602 | Strain-driven elastic and orbital-ordering effects on
thickness-dependent properties of manganite thin films | We report on the structural and magnetic characterization of (110) and (001)
La2/3Ca1/3MnO3 (LCMO) epitaxial thin films simultaneously grown on (110) and
(001)SrTiO3 substrates, with thicknesses t varying between 8 nm and 150 nm. It
is found that while the in-plane interplanar distances of the (001) films are
strongl... | cond-mat.mtrl-sci | we report on the structural and magnetic characterization of 110 and 001 la23ca13mno3 lcmo epitaxial thin films simultaneously grown on 110 and 001srtio3 substrates with thicknesses t varying between 8 nm and 150 nm it is found that while the inplane interplanar distances of the 001 films are strongly clamped to those ... | [['we', 'report', 'on', 'the', 'structural', 'and', 'magnetic', 'characterization', 'of', '110', 'and', '001', 'la23ca13mno3', 'lcmo', 'epitaxial', 'thin', 'films', 'simultaneously', 'grown', 'on', '110', 'and', '001srtio3', 'substrates', 'with', 'thicknesses', 't', 'varying', 'between', '8', 'nm', 'and', '150', 'nm', ... | [-0.14247778757620963, 0.24626718288409832, -0.005714013068146988, -0.04816142424886189, -0.02485302099104339, -0.11026399280457441, 0.08677045075378755, 0.47239571753971377, -0.28674452766849934, -0.3377466827901778, 0.05545205934463471, -0.317488240151941, -0.06841148559972315, 0.21517244041056294, 0.0327834847243707... |
708.3603 | Chiral symmetry breaking and the Lorentz nature of confinement | We address the question of the Lorentz nature of the effective interquark
interaction in QCD which leads to the formation of the QCD string between
colour charges. In particular, we start from a manifestly vectorial fundamental
interaction mediated by gluons and demonstrate that, as soon as chiral symmetry
is broken ... | hep-ph | we address the question of the lorentz nature of the effective interquark interaction in qcd which leads to the formation of the qcd string between colour charges in particular we start from a manifestly vectorial fundamental interaction mediated by gluons and demonstrate that as soon as chiral symmetry is broken spont... | [['we', 'address', 'the', 'question', 'of', 'the', 'lorentz', 'nature', 'of', 'the', 'effective', 'interquark', 'interaction', 'in', 'qcd', 'which', 'leads', 'to', 'the', 'formation', 'of', 'the', 'qcd', 'string', 'between', 'colour', 'charges', 'in', 'particular', 'we', 'start', 'from', 'a', 'manifestly', 'vectorial',... | [-0.11249186024069786, 0.26496721810661256, -0.11257032592780888, 0.11019684627768583, -0.05495702361688018, -0.08544527016114443, 0.020680931074311956, 0.3245118252933025, -0.22387372840195893, -0.242526690318482, -0.020814570316579194, -0.2672301843762398, -0.12179474628530443, 0.036155140921473504, 0.073761835256591... |
708.3604 | Looking for the Kondo cloud | We study the spatial distribution of the Kondo screening cloud. We find that
in 3 D the spatial range of the cloud is limited to distances of the order of
the Fermi wavelength due to angular dispersion effects. In lower dimensions
this effect is less important and thus the Kondo length determines the
localization of ... | cond-mat.mes-hall cond-mat.str-el | we study the spatial distribution of the kondo screening cloud we find that in 3 d the spatial range of the cloud is limited to distances of the order of the fermi wavelength due to angular dispersion effects in lower dimensions this effect is less important and thus the kondo length determines the localization of the ... | [['we', 'study', 'the', 'spatial', 'distribution', 'of', 'the', 'kondo', 'screening', 'cloud', 'we', 'find', 'that', 'in', '3', 'd', 'the', 'spatial', 'range', 'of', 'the', 'cloud', 'is', 'limited', 'to', 'distances', 'of', 'the', 'order', 'of', 'the', 'fermi', 'wavelength', 'due', 'to', 'angular', 'dispersion', 'effec... | [-0.1969983441976919, 0.15097653617586254, -0.07568986124325809, 0.09200613147224344, 0.0003520346468403226, -0.08889191583952023, 0.05614606859605937, 0.3321263281916756, -0.2839598777216105, -0.3044932506668071, 0.012238407826849393, -0.281236226297915, -0.0648266517512855, 0.12886309878279764, 0.005478045273394812, ... |
708.3605 | Cosmological simulations using a static scalar-tensor theory | We present $\Lambda$CDM $N$-body cosmological simulations in the framework of
a static general scalar-tensor theory of gravity. Due to the influence of the
non-minimally coupled scalar field, the gravitational potential is modified by
a Yukawa type term, yielding a new structure formation dynamics. We present
some pr... | astro-ph | we present lambdacdm nbody cosmological simulations in the framework of a static general scalartensor theory of gravity due to the influence of the nonminimally coupled scalar field the gravitational potential is modified by a yukawa type term yielding a new structure formation dynamics we present some preliminary resu... | [['we', 'present', 'lambdacdm', 'nbody', 'cosmological', 'simulations', 'in', 'the', 'framework', 'of', 'a', 'static', 'general', 'scalartensor', 'theory', 'of', 'gravity', 'due', 'to', 'the', 'influence', 'of', 'the', 'nonminimally', 'coupled', 'scalar', 'field', 'the', 'gravitational', 'potential', 'is', 'modified', ... | [-0.18309089636784934, 0.07609808260929726, -0.10617353977073753, 0.08834460430357251, -0.12354812466554226, -0.10703965309741241, -0.06255716180229294, 0.28383590273618226, -0.19307264257850687, -0.306927221102847, 0.008904791588614147, -0.22796887833447682, -0.19141161370105922, 0.11907328342989323, 0.028506245611915... |
708.3606 | Variable Cosmological Constant model: the reconstruction equations and
constraints from current observational data | In this paper we first give a brief review of the variable cosmological
constant model and its scalar field description. We mainly discuss two types of
variable cosmological constant models: $a$ power law and $H$ power law models.
A method to obtain all of the equivalent scalar field potentials and the
effective equa... | astro-ph | in this paper we first give a brief review of the variable cosmological constant model and its scalar field description we mainly discuss two types of variable cosmological constant models a power law and h power law models a method to obtain all of the equivalent scalar field potentials and the effective equation of s... | [['in', 'this', 'paper', 'we', 'first', 'give', 'a', 'brief', 'review', 'of', 'the', 'variable', 'cosmological', 'constant', 'model', 'and', 'its', 'scalar', 'field', 'description', 'we', 'mainly', 'discuss', 'two', 'types', 'of', 'variable', 'cosmological', 'constant', 'models', 'a', 'power', 'law', 'and', 'h', 'power... | [-0.1168670150749747, 0.12213484934775286, -0.06533916801829072, 0.06769438294831717, -0.11271603980318652, -0.11545791385641087, 0.012920354450578141, 0.328736480162705, -0.23162393033836778, -0.3266913037706456, 0.08054578406253074, -0.3135441797830671, -0.09788512148514607, 0.2001606029991255, 0.03258585161077383, 0... |
708.3607 | Parametric stiffness analysis of the Orthoglide | This paper presents a parametric stiffness analysis of the Orthoglide. A
compliant modeling and a symbolic expression of the stiffness matrix are
conducted. This allows a simple systematic analysis of the influence of the
geometric design parameters and to quickly identify the critical link
parameters. Our symbolic m... | cs.RO | this paper presents a parametric stiffness analysis of the orthoglide a compliant modeling and a symbolic expression of the stiffness matrix are conducted this allows a simple systematic analysis of the influence of the geometric design parameters and to quickly identify the critical link parameters our symbolic model ... | [['this', 'paper', 'presents', 'a', 'parametric', 'stiffness', 'analysis', 'of', 'the', 'orthoglide', 'a', 'compliant', 'modeling', 'and', 'a', 'symbolic', 'expression', 'of', 'the', 'stiffness', 'matrix', 'are', 'conducted', 'this', 'allows', 'a', 'simple', 'systematic', 'analysis', 'of', 'the', 'influence', 'of', 'th... | [-0.13895768170021003, 0.04116876147498813, -0.12388749409443404, -0.02460703593855606, -0.14999642701748805, -0.15636305401361064, 0.05278515346684269, 0.3492166794647899, -0.2738458854212614, -0.3062654244654541, 0.11465251751507845, -0.1885427268654111, -0.19450235781790334, 0.2091219339171967, -0.07812801718618279,... |
708.3608 | Continuous functions taking every value a given number of times | We give necessary and sufficient conditions on a function $f:[0,1]\to
{0,1,2,...,\omega,\continuum}$ under which there exists a continuous function
$F:[0,1]\to [0,1]$ such that for every $y\in[0,1]$ we have $|F^{-1}(y)|=f(y)$.
| math.LO math.GN | we give necessary and sufficient conditions on a function f01to 012omegacontinuum under which there exists a continuous function f01to 01 such that for every yin01 we have f1yfy | [['we', 'give', 'necessary', 'and', 'sufficient', 'conditions', 'on', 'a', 'function', 'f01to', '012omegacontinuum', 'under', 'which', 'there', 'exists', 'a', 'continuous', 'function', 'f01to', '01', 'such', 'that', 'for', 'every', 'yin01', 'we', 'have', 'f1yfy']] | [-0.14160878426180437, 0.10647825180337979, -0.11359842051751912, 0.07854148473304051, 0.011581657678247072, -0.14531547372014478, 0.06364393510963194, 0.4843135787030825, -0.20904226615451849, -0.15978683889485323, 0.15632481006189033, -0.18529297984563387, -0.21664945444521996, 0.20575687239089838, -0.068900640391243... |
708.3609 | Thompson's Group F | We introduce forest diagrams and strand diagrams for elements of Thompson's
group F. A forest diagram is a pair of infinite, bounded binary forests
together with an order-preserving bijection of the leaves. Using forest
diagrams, we derive a simple length formula for elements of F, and we discuss
applications to the ... | math.GR | we introduce forest diagrams and strand diagrams for elements of thompsons group f a forest diagram is a pair of infinite bounded binary forests together with an orderpreserving bijection of the leaves using forest diagrams we derive a simple length formula for elements of f and we discuss applications to the geometry ... | [['we', 'introduce', 'forest', 'diagrams', 'and', 'strand', 'diagrams', 'for', 'elements', 'of', 'thompsons', 'group', 'f', 'a', 'forest', 'diagram', 'is', 'a', 'pair', 'of', 'infinite', 'bounded', 'binary', 'forests', 'together', 'with', 'an', 'orderpreserving', 'bijection', 'of', 'the', 'leaves', 'using', 'forest', '... | [-0.1663174604226062, 0.12835341209183582, -0.07473753432014008, 0.07954030432562642, -0.12124393979759605, -0.12094475203501236, 0.11114389631558948, 0.3910426568670444, -0.29140300200461355, -0.24706571712597925, 0.08042204849540589, -0.26563171184410883, -0.13570067308017247, 0.21335052681278507, -0.1058944587723158... |
708.361 | Heavy-heavy-light quark potential in SU(3) lattice QCD | We perform the first study for the heavy-heavy-light quark (QQq) potential in
SU(3) lattice QCD. The calculations are done with the standard gauge and
$O(a)$-improved Wilson fermion action on the $16^4$ lattice at $\beta =6.0$ at
the quenched level. We calculate the energy of QQq systems as the function of
the distan... | hep-lat | we perform the first study for the heavyheavylight quark qqq potential in su3 lattice qcd the calculations are done with the standard gauge and oaimproved wilson fermion action on the 164 lattice at beta 60 at the quenched level we calculate the energy of qqq systems as the function of the distance between the two heav... | [['we', 'perform', 'the', 'first', 'study', 'for', 'the', 'heavyheavylight', 'quark', 'qqq', 'potential', 'in', 'su3', 'lattice', 'qcd', 'the', 'calculations', 'are', 'done', 'with', 'the', 'standard', 'gauge', 'and', 'oaimproved', 'wilson', 'fermion', 'action', 'on', 'the', '164', 'lattice', 'at', 'beta', '60', 'at', ... | [-0.0907231111103075, 0.24159879992594538, -0.07787556710410053, 0.14731443637519723, -0.020043887670381344, -0.11647738424548204, 0.07990521148009144, 0.3341860690464576, -0.17513489500497995, -0.25367420120839623, -0.01936476012317302, -0.31533119081101124, -0.04170662386720811, 0.06334359393002924, 0.078515107142806... |
708.3611 | Structural and dynamical characteristics of mesoscopic H$^+$[H$_2$O]$_n$
clusters | Structural and dynamical characteristics pertaining to the solvation of an
excess proton in liquid-like nanoclusters of the type [H$_2$O]$_n$ are
investigated using Molecular Dynamics experiments. Three different aggregate
sizes were analyzed: $n=10,$ 21 and 125. The simulation experiments were
performed using a mult... | physics.chem-ph physics.atm-clus physics.comp-ph | structural and dynamical characteristics pertaining to the solvation of an excess proton in liquidlike nanoclusters of the type h_2o_n are investigated using molecular dynamics experiments three different aggregate sizes were analyzed n10 21 and 125 the simulation experiments were performed using a multistate empirical... | [['structural', 'and', 'dynamical', 'characteristics', 'pertaining', 'to', 'the', 'solvation', 'of', 'an', 'excess', 'proton', 'in', 'liquidlike', 'nanoclusters', 'of', 'the', 'type', 'h_2o_n', 'are', 'investigated', 'using', 'molecular', 'dynamics', 'experiments', 'three', 'different', 'aggregate', 'sizes', 'were', 'a... | [-0.06829086655223843, 0.1752195719697435, -0.022836883144467607, 0.08376610968550739, 0.0682324523615196, -0.10368557551707856, 0.0463340657748744, 0.4064897945829371, -0.222713660798938, -0.3304447734786212, 0.054050123855081754, -0.3303979803815253, -0.02328952084937992, 0.142709766520014, 0.04120192171774747, 0.013... |
708.3612 | CP Asymmetries in Higgs decays to ZZ at the LHC | We examine the effect of a general HZZ coupling through a study of the Higgs
decay to leptons via Z bosons at the LHC. We discuss various methods for
placing limits on additional couplings, including measurement of the partial
width, threshold scans, and asymmetries constructed from angular observables.
We find that ... | hep-ph | we examine the effect of a general hzz coupling through a study of the higgs decay to leptons via z bosons at the lhc we discuss various methods for placing limits on additional couplings including measurement of the partial width threshold scans and asymmetries constructed from angular observables we find that only th... | [['we', 'examine', 'the', 'effect', 'of', 'a', 'general', 'hzz', 'coupling', 'through', 'a', 'study', 'of', 'the', 'higgs', 'decay', 'to', 'leptons', 'via', 'z', 'bosons', 'at', 'the', 'lhc', 'we', 'discuss', 'various', 'methods', 'for', 'placing', 'limits', 'on', 'additional', 'couplings', 'including', 'measurement', ... | [-0.10689064243085929, 0.15902465034741908, -0.05551465102882289, 0.15901886326644352, -0.07667613295180832, -0.16210344050983516, 0.10072568619815524, 0.347718567970921, -0.19599842076765045, -0.2772643390002058, 0.06878449980457149, -0.28996159504715574, -0.013648074487504987, 0.1729366956210202, 0.11221529576270019,... |
708.3613 | Kinematics and Workspace Analysis of a Three-Axis Parallel Manipulator:
the Orthoglide | The paper addresses kinematic and geometrical aspects of the Orthoglide, a
three-DOF parallel mechanism. This machine consists of three fixed linear
joints, which are mounted orthogonally, three identical legs and a mobile
platform, which moves in the Cartesian x-y-z space with fixed orientation. New
solutions to sol... | cs.RO | the paper addresses kinematic and geometrical aspects of the orthoglide a threedof parallel mechanism this machine consists of three fixed linear joints which are mounted orthogonally three identical legs and a mobile platform which moves in the cartesian xyz space with fixed orientation new solutions to solve inversed... | [['the', 'paper', 'addresses', 'kinematic', 'and', 'geometrical', 'aspects', 'of', 'the', 'orthoglide', 'a', 'threedof', 'parallel', 'mechanism', 'this', 'machine', 'consists', 'of', 'three', 'fixed', 'linear', 'joints', 'which', 'are', 'mounted', 'orthogonally', 'three', 'identical', 'legs', 'and', 'a', 'mobile', 'pla... | [-0.19432696748778902, 0.05366850870125221, -0.06870829367615057, -0.034999741391264695, -0.15939226710576226, -0.21061682159250433, -0.01694988799246141, 0.38849531068946375, -0.24094723238412177, -0.3025126083133121, 0.06722730507141078, -0.2595368990194843, -0.09145482293697017, 0.1329353375247482, -0.03013554048216... |
708.3614 | Correlated $\Lambda d$ pairs from the $K^{-}_{stop} A \to \Lambda d A'$
reaction | Correlated $\Lambda d$ pairs emitted after the absorption of negative kaons
at rest $K^{-}_{stop}A\to \Lambda d A'$ in light nuclei $^6Li$ and $^{12}C$ are
studied. $\Lambda$-hyperons and deuterons are found to be preferentially
emitted in opposite directions. The $\Lambda d$ invariant mass spectrum of
$^6Li$ shows a... | nucl-ex | correlated lambda d pairs emitted after the absorption of negative kaons at rest k_stopato lambda d a in light nuclei 6li and 12c are studied lambdahyperons and deuterons are found to be preferentially emitted in opposite directions the lambda d invariant mass spectrum of 6li shows a bump whose mass is 3251pm6 mevc2 th... | [['correlated', 'lambda', 'd', 'pairs', 'emitted', 'after', 'the', 'absorption', 'of', 'negative', 'kaons', 'at', 'rest', 'k_stopato', 'lambda', 'd', 'a', 'in', 'light', 'nuclei', '6li', 'and', '12c', 'are', 'studied', 'lambdahyperons', 'and', 'deuterons', 'are', 'found', 'to', 'be', 'preferentially', 'emitted', 'in', ... | [-0.08711296995699574, 0.26768065885302017, -0.10489979970891351, 0.11080273230496376, 0.03540874400906349, -0.16374667555580594, -0.015457268747426993, 0.4073683073617179, -0.1557234074624086, -0.31214716234667733, -0.08814246351936493, -0.38848541146779264, 0.08006840147242077, 0.12252576818520372, 0.0867168434620411... |
708.3615 | Relativistic iron emission lines in neutron star low-mass X-ray binaries
as probes of neutron star radii | Using Suzaku observations of three neutron star low-mass X-ray binaries (Ser
X-1, 4U 1820-30 and GX 349+2) we have found broad, asymmetric, relativistic Fe
K emission lines in all three objects. These Fe K lines can be well fit by a
model for lines from a relativistic accretion disk ('diskline'), allowing a
measureme... | astro-ph | using suzaku observations of three neutron star lowmass xray binaries ser x1 4u 182030 and gx 3492 we have found broad asymmetric relativistic fe k emission lines in all three objects these fe k lines can be well fit by a model for lines from a relativistic accretion disk diskline allowing a measurement of the inner ra... | [['using', 'suzaku', 'observations', 'of', 'three', 'neutron', 'star', 'lowmass', 'xray', 'binaries', 'ser', 'x1', '4u', '182030', 'and', 'gx', '3492', 'we', 'have', 'found', 'broad', 'asymmetric', 'relativistic', 'fe', 'k', 'emission', 'lines', 'in', 'all', 'three', 'objects', 'these', 'fe', 'k', 'lines', 'can', 'be',... | [-0.08019854345283708, 0.13160860295321067, -0.0034370311067341277, 0.13159845013935004, -0.11938532948261127, -0.1373013465243004, 0.06244419502406757, 0.4528384424560929, -0.12263851888153864, -0.3448650275605806, 0.08022690317318745, -0.3351088267930361, 0.07222058142749418, 0.25941915817483563, -0.01321084502077898... |
708.3616 | Hydrodynamic simulations of irradiated secondaries in dwarf novae | We investigate numerically the surface flow on the secondary star during
outbursts. We use a simple model for the irradiation and the geometry of the
secondary star: the irradiation temperature is treated as a free parameter and
the secondary is replaced by a spherical star with a space-dependent Coriolis
force that ... | astro-ph | we investigate numerically the surface flow on the secondary star during outbursts we use a simple model for the irradiation and the geometry of the secondary star the irradiation temperature is treated as a free parameter and the secondary is replaced by a spherical star with a spacedependent coriolis force that mimic... | [['we', 'investigate', 'numerically', 'the', 'surface', 'flow', 'on', 'the', 'secondary', 'star', 'during', 'outbursts', 'we', 'use', 'a', 'simple', 'model', 'for', 'the', 'irradiation', 'and', 'the', 'geometry', 'of', 'the', 'secondary', 'star', 'the', 'irradiation', 'temperature', 'is', 'treated', 'as', 'a', 'free', ... | [-0.13322049646925288, 0.17437412905188435, -0.09505237308596343, 0.06173422918532436, -0.04784871641088996, -0.07989799547246085, 0.053435758253040706, 0.35720686839991495, -0.29348177934196173, -0.29646075497332375, 0.10706163618382752, -0.2524347508346852, -0.05773275463000398, 0.19364122760567912, -0.06981078933949... |
708.3617 | Spin relaxation in the impurity band of a semiconductor in the external
magnetic field | Spin relaxation in the impurity band of a 2D semiconductor with spin-split
spectrum in the external magnetic field is considered. Several mechanisms of
spin relaxation are shown to be relevant. The first one is attributed to
phonon-assisted transitions between Zeeman sublevels of the ground state of an
isolated impur... | cond-mat.mes-hall | spin relaxation in the impurity band of a 2d semiconductor with spinsplit spectrum in the external magnetic field is considered several mechanisms of spin relaxation are shown to be relevant the first one is attributed to phononassisted transitions between zeeman sublevels of the ground state of an isolated impurity wh... | [['spin', 'relaxation', 'in', 'the', 'impurity', 'band', 'of', 'a', '2d', 'semiconductor', 'with', 'spinsplit', 'spectrum', 'in', 'the', 'external', 'magnetic', 'field', 'is', 'considered', 'several', 'mechanisms', 'of', 'spin', 'relaxation', 'are', 'shown', 'to', 'be', 'relevant', 'the', 'first', 'one', 'is', 'attribu... | [-0.17640300926633087, 0.22535443259511348, 0.0016871210330065864, 0.0756067169882157, -0.008902768365854075, -0.1355228429633262, -0.008585014530603797, 0.3845191183538476, -0.29991664078610003, -0.3152920175959502, 0.03311068731579499, -0.2696646774911191, -0.050755814518317705, 0.20022122929842512, 0.057654638520695... |
708.3618 | Diffusive-Ballistic Crossover and the Persistent Spin Helix | Conventional transport theory focuses on either the diffusive or ballistic
regimes and neglects the crossover region between the two. In the presence of
spin-orbit coupling, the transport equations are known only in the diffusive
regime, where the spin precession angle is small. In this paper, we develop a
semiclassi... | cond-mat.mes-hall | conventional transport theory focuses on either the diffusive or ballistic regimes and neglects the crossover region between the two in the presence of spinorbit coupling the transport equations are known only in the diffusive regime where the spin precession angle is small in this paper we develop a semiclassical theo... | [['conventional', 'transport', 'theory', 'focuses', 'on', 'either', 'the', 'diffusive', 'or', 'ballistic', 'regimes', 'and', 'neglects', 'the', 'crossover', 'region', 'between', 'the', 'two', 'in', 'the', 'presence', 'of', 'spinorbit', 'coupling', 'the', 'transport', 'equations', 'are', 'known', 'only', 'in', 'the', 'd... | [-0.22490449492873338, 0.20818319442108846, -0.026622984271783095, 0.053426097928492636, -0.03685442048859281, -0.17999424954625562, 0.005636387618813807, 0.3131967479846655, -0.2779845559718804, -0.23063855729280755, 0.018386194136557885, -0.27414625775866, -0.15043791527904643, 0.1795309157034633, 0.04320465000273543... |
708.3619 | Explicit Evaluation of Certain Exponential Sums of Quadratic Functions
over $\Bbb F_{p^n}$, $p$ Odd | Let $p$ be an odd prime and let
$f(x)=\sum_{i=1}^ka_ix^{p^{\alpha_i}+1}\in\Bbb F_{p^n}[x]$, where $0\le
\alpha_1<...<\alpha_k$. We consider the exponential sum $S(f,n)=\sum_{x\in\Bbb
F_{p^n}}e_n(f(x))$, where $e_n(y)=e^{2\pi i\text{Tr}_n(y)/p}$, $y\in\Bbb
F_{p^n}$, $\text{Tr}_n=\text{Tr}_{\Bbb F_{p^n}/\Bbb F_p}$. The... | math.NT | let p be an odd prime and let fxsum_i1ka_ixpalpha_i1inbbb f_pnx where 0le alpha_1alpha_k we consider the exponential sum sfnsum_xinbbb f_pne_nfx where e_nye2pi itexttr_nyp yinbbb f_pn texttr_ntexttr_bbb f_pnbbb f_p there is an effective way to compute the nullity of the quadratic form texttr_mnfx for all integer m0 ass... | [['let', 'p', 'be', 'an', 'odd', 'prime', 'and', 'let', 'fxsum_i1ka_ixpalpha_i1inbbb', 'f_pnx', 'where', '0le', 'alpha_1alpha_k', 'we', 'consider', 'the', 'exponential', 'sum', 'sfnsum_xinbbb', 'f_pne_nfx', 'where', 'e_nye2pi', 'itexttr_nyp', 'yinbbb', 'f_pn', 'texttr_ntexttr_bbb', 'f_pnbbb', 'f_p', 'there', 'is', 'an'... | [-0.1592157483676967, 0.1402230288768271, -0.029987686104861272, 0.026028399546234628, -0.04491788574696048, -0.17632241072325208, -0.018969123269738535, 0.3004695412213194, -0.25465092036066594, -0.2877607196761468, 0.04855541418277726, -0.2858174374931943, -0.1457147350505993, 0.21484709258662948, -0.0676060375874830... |
708.362 | Heavy Ion Collisions and New Forms of Matter | I discuss forms of high energy density matter in QCD. These include the Color
Glass Condensate, the Glasma and the Quark Gluon Plasma. They all might be
studied in ultra-relativistic heavy ion collisions, nd the Color Glass
Condensate might also be probed in electron-hadron collisions. I present the
properties of suc... | hep-ph | i discuss forms of high energy density matter in qcd these include the color glass condensate the glasma and the quark gluon plasma they all might be studied in ultrarelativistic heavy ion collisions nd the color glass condensate might also be probed in electronhadron collisions i present the properties of such matter ... | [['i', 'discuss', 'forms', 'of', 'high', 'energy', 'density', 'matter', 'in', 'qcd', 'these', 'include', 'the', 'color', 'glass', 'condensate', 'the', 'glasma', 'and', 'the', 'quark', 'gluon', 'plasma', 'they', 'all', 'might', 'be', 'studied', 'in', 'ultrarelativistic', 'heavy', 'ion', 'collisions', 'nd', 'the', 'color... | [-0.059948654308344326, 0.3371238494892755, -0.18511118904326954, 0.15286328232163685, 0.019163758080873276, -0.07999023075606074, -0.0980474844278257, 0.39626862955910547, -0.1999082792580368, -0.23949976466716297, 0.018742538539827953, -0.30073961316637937, 0.03334793376345788, 0.03320647936702552, 0.0218306637834757... |
708.3621 | The $\mathcal{Q}_p$ Carleson Measure Problem | Let $\mu$ be a nonnegative Borel measure on the open unit disk
$\mathbb{D}\subset\mathbb{C}$. This note shows how to decide that the M\"obius
invariant space $\mathcal{Q}_p$, covering $\mathcal{BMOA}$ and $\mathcal{B}$,
is boundedly (resp., compactly) embedded in the quadratic tent-type space
$T^\infty_p(\mu)$. Inter... | math.CV math.FA | let mu be a nonnegative borel measure on the open unit disk mathbbdsubsetmathbbc this note shows how to decide that the mobius invariant space mathcalq_p covering mathcalbmoa and mathcalb is boundedly resp compactly embedded in the quadratic tenttype space tinfty_pmu interestingly the embedding result can be used to de... | [['let', 'mu', 'be', 'a', 'nonnegative', 'borel', 'measure', 'on', 'the', 'open', 'unit', 'disk', 'mathbbdsubsetmathbbc', 'this', 'note', 'shows', 'how', 'to', 'decide', 'that', 'the', 'mobius', 'invariant', 'space', 'mathcalq_p', 'covering', 'mathcalbmoa', 'and', 'mathcalb', 'is', 'boundedly', 'resp', 'compactly', 'em... | [-0.1317829526013742, 0.11105326029582549, -0.07592301839031279, 0.09503347474008293, -0.10261714377566793, -0.10077114607665245, 0.017726285608043357, 0.3758006078206887, -0.3548013013550791, -0.16002245872282478, 0.1504303593310859, -0.27368840060203725, -0.08753353590934963, 0.16315492667194645, -0.12981894576006522... |
708.3622 | On cosmological observables in a swiss-cheese universe | Photon geodesics are calculated in a swiss-cheese model, where the cheese is
made of the usual Friedmann-Robertson-Walker solution and the holes are
constructed from a Lemaitre-Tolman-Bondi solution of Einstein's equations. The
observables on which we focus are the changes in the redshift, in the
angular-diameter--di... | astro-ph gr-qc | photon geodesics are calculated in a swisscheese model where the cheese is made of the usual friedmannrobertsonwalker solution and the holes are constructed from a lemaitretolmanbondi solution of einsteins equations the observables on which we focus are the changes in the redshift in the angulardiameterdistance relatio... | [['photon', 'geodesics', 'are', 'calculated', 'in', 'a', 'swisscheese', 'model', 'where', 'the', 'cheese', 'is', 'made', 'of', 'the', 'usual', 'friedmannrobertsonwalker', 'solution', 'and', 'the', 'holes', 'are', 'constructed', 'from', 'a', 'lemaitretolmanbondi', 'solution', 'of', 'einsteins', 'equations', 'the', 'obse... | [-0.11423557400013562, 0.12324342137722896, -0.11558697430451435, 0.12015717194478867, -0.08693557566054809, -0.07155019417836296, -0.023295241260015764, 0.33227454707670356, -0.23297791995027642, -0.2934134507172362, 0.05254186574300682, -0.31041671370334323, -0.1081088976589618, 0.18080956905284024, -0.02349566416793... |
708.3623 | Derangements and Relative Derangements of Type $B$ | By introducing the notion of relative derangements of type $B$, also called
signed relative derangements, which are defined in terms of signed
permutations, we obtain a type $B$ analogue of the well-known relation between
relative derangements and the classical derangements. While this fact can be
proved by using the... | math.CO | by introducing the notion of relative derangements of type b also called signed relative derangements which are defined in terms of signed permutations we obtain a type b analogue of the wellknown relation between relative derangements and the classical derangements while this fact can be proved by using the principle ... | [['by', 'introducing', 'the', 'notion', 'of', 'relative', 'derangements', 'of', 'type', 'b', 'also', 'called', 'signed', 'relative', 'derangements', 'which', 'are', 'defined', 'in', 'terms', 'of', 'signed', 'permutations', 'we', 'obtain', 'a', 'type', 'b', 'analogue', 'of', 'the', 'wellknown', 'relation', 'between', 'r... | [-0.14556665592161672, 0.11738894579133817, -0.07984259801783732, 0.07749039281126378, -0.09249656567616123, -0.09840484293443816, 0.09965059409649776, 0.2780221781693399, -0.3453354436904192, -0.32450594870107513, 0.0559063713199326, -0.2201161294643368, -0.2142932270786592, 0.14114503317645619, -0.15277654001755372, ... |
708.3624 | Collapse models with non-white noises | We set up a general formalism for models of spontaneous wave function
collapse with dynamics represented by a stochastic differential equation driven
by general Gaussian noises, not necessarily white in time. In particular, we
show that the non-Schrodinger terms of the equation induce the collapse of the
wave functio... | quant-ph | we set up a general formalism for models of spontaneous wave function collapse with dynamics represented by a stochastic differential equation driven by general gaussian noises not necessarily white in time in particular we show that the nonschrodinger terms of the equation induce the collapse of the wave function to o... | [['we', 'set', 'up', 'a', 'general', 'formalism', 'for', 'models', 'of', 'spontaneous', 'wave', 'function', 'collapse', 'with', 'dynamics', 'represented', 'by', 'a', 'stochastic', 'differential', 'equation', 'driven', 'by', 'general', 'gaussian', 'noises', 'not', 'necessarily', 'white', 'in', 'time', 'in', 'particular'... | [-0.09599372294309327, 0.11001306422912807, -0.08960497911295874, 0.0775979479298938, -0.03205286624519784, -0.07416489771265777, 0.020603070085828037, 0.2763751208674993, -0.27197139093102957, -0.2542914756709415, 0.07641627078560992, -0.27024755581533755, -0.16734586819242553, 0.1575355161075219, -0.00041419333986026... |
708.3625 | Spin matrix elements in 2D Ising model on the finite lattice | We present explicit formulas for all spin matrix elements in the 2D Ising
model with the nearest neighbor interaction on the finite periodic square
lattice. These expressions generalize the known results [Phys. Rev. D19,
(1979), 2477--2479; hep-th/0107117; hep-th/0112167] (coincide with them in the
appropriate limits... | nlin.SI cond-mat.stat-mech hep-th math-ph math.MP | we present explicit formulas for all spin matrix elements in the 2d ising model with the nearest neighbor interaction on the finite periodic square lattice these expressions generalize the known results phys rev d19 1979 24772479 hepth0107117 hepth0112167 coincide with them in the appropriate limits and fulfill the tes... | [['we', 'present', 'explicit', 'formulas', 'for', 'all', 'spin', 'matrix', 'elements', 'in', 'the', '2d', 'ising', 'model', 'with', 'the', 'nearest', 'neighbor', 'interaction', 'on', 'the', 'finite', 'periodic', 'square', 'lattice', 'these', 'expressions', 'generalize', 'the', 'known', 'results', 'phys', 'rev', 'd19', ... | [-0.08558645498231743, 0.12374457666064026, 0.05814269835267354, 0.02657314541715163, -0.07443570094700488, -0.1627190496807021, 0.06917081593052933, 0.3855072421849602, -0.1598000769175727, -0.24821339583852225, 0.04455589089559874, -0.3075901829827301, -0.15534093897117096, 0.1617120522402089, 0.028492634229122713, 0... |
708.3626 | Total cross-section and rapidity gap survival probability at the LHC
through an eikonal with soft gluon resummation | New results are presented for total ${\rm pp}/ {\rm \bar p p}$
cross-sections, in the framework of our QCD based model (GGPS). This is an
improved eikonal mini-jet model, where soft gluon radiation tames the fast
energy rise normally present in mini-jet models. We discuss the variability in
our predictions and provid... | hep-ph | new results are presented for total rm pp rm bar p p crosssections in the framework of our qcd based model ggps this is an improved eikonal minijet model where soft gluon radiation tames the fast energy rise normally present in minijet models we discuss the variability in our predictions and provide a handy parametriza... | [['new', 'results', 'are', 'presented', 'for', 'total', 'rm', 'pp', 'rm', 'bar', 'p', 'p', 'crosssections', 'in', 'the', 'framework', 'of', 'our', 'qcd', 'based', 'model', 'ggps', 'this', 'is', 'an', 'improved', 'eikonal', 'minijet', 'model', 'where', 'soft', 'gluon', 'radiation', 'tames', 'the', 'fast', 'energy', 'ris... | [-0.010676169430371373, 0.13602828598386624, -0.1184862865775358, 0.15373811290306777, -0.05159288252471015, -0.1041338140174048, 0.014329016038391273, 0.3753381525093573, -0.20542631110947696, -0.29445164241915334, 0.0222880291448746, -0.30606439034727373, -0.05325647760764696, 0.2043100002905703, 0.003256570422672666... |
708.3627 | Optimizing Replica Exchange Moves For Molecular Dynamics | In this short note we sketch the statistical physics framework of the replica
exchange technique when applied to molecular dynamics simulations. In
particular, we draw attention to generalized move sets that allow a variety of
optimizations as well as new applications of the method.
| q-bio.QM cond-mat.stat-mech physics.comp-ph q-bio.BM | in this short note we sketch the statistical physics framework of the replica exchange technique when applied to molecular dynamics simulations in particular we draw attention to generalized move sets that allow a variety of optimizations as well as new applications of the method | [['in', 'this', 'short', 'note', 'we', 'sketch', 'the', 'statistical', 'physics', 'framework', 'of', 'the', 'replica', 'exchange', 'technique', 'when', 'applied', 'to', 'molecular', 'dynamics', 'simulations', 'in', 'particular', 'we', 'draw', 'attention', 'to', 'generalized', 'move', 'sets', 'that', 'allow', 'a', 'vari... | [-0.03817321950654415, 0.04544564903533848, -0.12967402665791186, 0.10827115475231866, -0.08728142522952774, -0.12551581811964174, 0.08208052792840383, 0.3933739579198035, -0.3222123989517885, -0.3089898352151398, 0.07057976734887977, -0.1977700024038892, -0.21190408096564087, 0.22617760982195084, -0.04585843603126705,... |
708.3628 | Recursive Structure and Bandwidth of Hales-Numbered Hypercube | The Hales numbered $n$-dimensional hypercube and the corresponding adjacency
matrix exhibit interesting recursive structures in $n$. These structures lead
to a very simple proof of the well-known bandwidth formula for hypercube, whose
proof was thought to be surprisingly difficult. A related problem called
hypercube ... | cs.DM | the hales numbered ndimensional hypercube and the corresponding adjacency matrix exhibit interesting recursive structures in n these structures lead to a very simple proof of the wellknown bandwidth formula for hypercube whose proof was thought to be surprisingly difficult a related problem called hypercube antibandwid... | [['the', 'hales', 'numbered', 'ndimensional', 'hypercube', 'and', 'the', 'corresponding', 'adjacency', 'matrix', 'exhibit', 'interesting', 'recursive', 'structures', 'in', 'n', 'these', 'structures', 'lead', 'to', 'a', 'very', 'simple', 'proof', 'of', 'the', 'wellknown', 'bandwidth', 'formula', 'for', 'hypercube', 'who... | [-0.10853459993514288, 0.07626242476865575, -0.08205622366136488, 0.13916119311675978, -0.09942373329934473, -0.1653592947199393, 0.04577137524542837, 0.35185753674629855, -0.28780599168556575, -0.2938937560436042, 0.12089426368252401, -0.2332983078325496, -0.2560647951801965, 0.19464697634034298, -0.09719528494786252,... |
708.3629 | Boundary conditions in the QCD nucleus-nucleus scattering problem | In the framework of the effective field theory for interacting BFKL pomerons,
applied to nucleus-nucleus scattering, boundary conditions for the classical
field equations are discussed. Correspondence with the QCD diagrams at the
boundary rapidities requires pomeron interaction with the participating nuclei
to be exp... | hep-ph hep-th | in the framework of the effective field theory for interacting bfkl pomerons applied to nucleusnucleus scattering boundary conditions for the classical field equations are discussed correspondence with the qcd diagrams at the boundary rapidities requires pomeron interaction with the participating nuclei to be exponenti... | [['in', 'the', 'framework', 'of', 'the', 'effective', 'field', 'theory', 'for', 'interacting', 'bfkl', 'pomerons', 'applied', 'to', 'nucleusnucleus', 'scattering', 'boundary', 'conditions', 'for', 'the', 'classical', 'field', 'equations', 'are', 'discussed', 'correspondence', 'with', 'the', 'qcd', 'diagrams', 'at', 'th... | [-0.11454885132060719, 0.1526527943018802, -0.1214753913595096, 0.12421257773003057, -0.05015293013288133, -0.13386034208202832, -0.021273093098095122, 0.32112826670404954, -0.2073371679724973, -0.277472284878468, 0.05315692708602894, -0.28174585142929914, -0.05156085956760012, 0.15593072121189525, 0.006287688392143675... |
708.363 | Floating Entanglement Witness Measure and Genetic Algorithm | In this paper based on the notion of entanglement witness, a new measure of
entanglement called floating entanglement witness measure is introduced which
satisfies some of the usual properties of a good entanglement measure. By
exploiting genetic algorithm, we introduce a classical algorithm that computes
floating en... | quant-ph | in this paper based on the notion of entanglement witness a new measure of entanglement called floating entanglement witness measure is introduced which satisfies some of the usual properties of a good entanglement measure by exploiting genetic algorithm we introduce a classical algorithm that computes floating entangl... | [['in', 'this', 'paper', 'based', 'on', 'the', 'notion', 'of', 'entanglement', 'witness', 'a', 'new', 'measure', 'of', 'entanglement', 'called', 'floating', 'entanglement', 'witness', 'measure', 'is', 'introduced', 'which', 'satisfies', 'some', 'of', 'the', 'usual', 'properties', 'of', 'a', 'good', 'entanglement', 'mea... | [-0.1349041414214298, 0.1389484471437754, -0.205138878460275, 0.0896294509202562, 0.009780694352230057, -0.22779610830912134, 0.0888646032417455, 0.3093925287066668, -0.2649235026910901, -0.24928280268795788, 0.010664995286788326, -0.22920704365242273, -0.17489661689614877, 0.21406243206001818, -0.0937456762912916, 0.1... |
708.3631 | Prediction of Fractional Processes with Long-range Dependence | We introduce a class of Gaussian processes with stationary increments which
exhibit long-range dependence. The class includes fractional Brownian motion
with Hurst parameter H>1/2 as a typical example. We establish infinite and
finite past prediction formulas for the processes in which the predictor
coefficients are ... | math.PR | we introduce a class of gaussian processes with stationary increments which exhibit longrange dependence the class includes fractional brownian motion with hurst parameter h12 as a typical example we establish infinite and finite past prediction formulas for the processes in which the predictor coefficients are given e... | [['we', 'introduce', 'a', 'class', 'of', 'gaussian', 'processes', 'with', 'stationary', 'increments', 'which', 'exhibit', 'longrange', 'dependence', 'the', 'class', 'includes', 'fractional', 'brownian', 'motion', 'with', 'hurst', 'parameter', 'h12', 'as', 'a', 'typical', 'example', 'we', 'establish', 'infinite', 'and',... | [-0.07600172703916376, 0.17046119255775755, -0.0495679610027847, 0.03664084909991785, -0.07146724723279477, -0.1295508535578847, 0.010452747615900907, 0.3841735333204269, -0.26099242825399743, -0.25177566131407564, 0.09995381165380506, -0.26033895591443235, -0.16157641857862473, 0.1879475508393212, -0.0457042626600014,... |
708.3632 | Akhet Khufu: archaeo-astronomical hints at a common project of the two
main pyramids of Giza, Egypt | The architectural complexes composed by the two main pyramids of Giza
together with their temples are investigated from an inter-disciplinary point
of view, taking into account their astronomical alignments as well as their
relationships with the visible landscape. Combining already known facts
together with new clue... | physics.hist-ph | the architectural complexes composed by the two main pyramids of giza together with their temples are investigated from an interdisciplinary point of view taking into account their astronomical alignments as well as their relationships with the visible landscape combining already known facts together with new clues the... | [['the', 'architectural', 'complexes', 'composed', 'by', 'the', 'two', 'main', 'pyramids', 'of', 'giza', 'together', 'with', 'their', 'temples', 'are', 'investigated', 'from', 'an', 'interdisciplinary', 'point', 'of', 'view', 'taking', 'into', 'account', 'their', 'astronomical', 'alignments', 'as', 'well', 'as', 'their... | [-0.07232093572383747, 0.10646029604890828, -0.08305863995337859, 0.08781858086877037, -0.09113223975873552, -0.07712015600554878, -0.010839049245987553, 0.38682070549111813, -0.2764180613376084, -0.3591808973287698, 0.1144481532392092, -0.29310868500033394, -0.16038450243740954, 0.1686690782516962, -0.0454948178376071... |
708.3633 | Quantum critical scaling behavior of deconfined spinons | We perform a renormalization group analysis of some important effective field
theoretic models for deconfined spinons. We show that deconfined spinons are
critical for an isotropic SU(N) Heisenberg antiferromagnet, if $N$ is large
enough. We argue that nonperturbatively this result should persist down to N=2
and prov... | cond-mat.str-el hep-th | we perform a renormalization group analysis of some important effective field theoretic models for deconfined spinons we show that deconfined spinons are critical for an isotropic sun heisenberg antiferromagnet if n is large enough we argue that nonperturbatively this result should persist down to n2 and provide furthe... | [['we', 'perform', 'a', 'renormalization', 'group', 'analysis', 'of', 'some', 'important', 'effective', 'field', 'theoretic', 'models', 'for', 'deconfined', 'spinons', 'we', 'show', 'that', 'deconfined', 'spinons', 'are', 'critical', 'for', 'an', 'isotropic', 'sun', 'heisenberg', 'antiferromagnet', 'if', 'n', 'is', 'la... | [-0.16985432404334194, 0.30127729245290863, -0.12678394694846254, 0.13576108063048475, -0.020786468527235445, -0.21623591744486673, 0.06483992800547354, 0.32919904174042397, -0.21736963490201605, -0.19323577383710516, 0.02966149331175019, -0.34520318204549705, -0.14146953809936688, 0.14637775164173575, 0.07912584287146... |
708.3634 | Time reflection and the dynamics of particles and antiparticles | In this paper we continue our analysis of a formulation of electrodynamics
fully covariant under the full Poincar\'e group. Transformations under the four
different components of the group force on us the introduction of particles,
either in the identification by Feynman or in the identification of Dirac.
| math-ph math.DG math.MP | in this paper we continue our analysis of a formulation of electrodynamics fully covariant under the full poincare group transformations under the four different components of the group force on us the introduction of particles either in the identification by feynman or in the identification of dirac | [['in', 'this', 'paper', 'we', 'continue', 'our', 'analysis', 'of', 'a', 'formulation', 'of', 'electrodynamics', 'fully', 'covariant', 'under', 'the', 'full', 'poincare', 'group', 'transformations', 'under', 'the', 'four', 'different', 'components', 'of', 'the', 'group', 'force', 'on', 'us', 'the', 'introduction', 'of'... | [-0.14238980412483215, 0.11032105213467111, -0.14716383281778148, -0.022658664309617844, -0.06746746187514448, -0.052634052942170106, 0.03778808257057074, 0.3062104959278665, -0.214873170262163, -0.291318380135171, 0.07868105653881471, -0.24799352258126786, -0.16183514643876634, 0.13532038194999257, -0.0397711210547292... |
708.3635 | A Multivariate Training Technique with Event Reweighting | An event reweighting technique incorporated in multivariate training
algorithm has been developed and tested using the Artificial Neural Networks
(ANN) and Boosted Decision Trees (BDT). The event reweighting training are
compared to that of the conventional equal event weighting based on the ANN and
the BDT performan... | physics.data-an | an event reweighting technique incorporated in multivariate training algorithm has been developed and tested using the artificial neural networks ann and boosted decision trees bdt the event reweighting training are compared to that of the conventional equal event weighting based on the ann and the bdt performance the ... | [['an', 'event', 'reweighting', 'technique', 'incorporated', 'in', 'multivariate', 'training', 'algorithm', 'has', 'been', 'developed', 'and', 'tested', 'using', 'the', 'artificial', 'neural', 'networks', 'ann', 'and', 'boosted', 'decision', 'trees', 'bdt', 'the', 'event', 'reweighting', 'training', 'are', 'compared', ... | [-0.004305772186603909, 0.051818294791041365, -0.1395186109653236, 0.1301709364280196, -0.07740322593599558, -0.1163406696252744, 0.022390821145153512, 0.39711979248871404, -0.20716062932293497, -0.3167262478530699, 0.07743802448442462, -0.2674485351981632, -0.14436558331819435, 0.1933775331605883, -0.01739335471910296... |
708.3636 | Evidences for two scales in hadrons | Some unusual features observed in hadronic collisions at high energies can be
understood assuming that gluons in hadrons are located within small spots
occupying only about 10% of the hadron's area. Such a conjecture about the
presence of two scales in hadrons helps to explain: why diffractive gluon
radiation so much... | hep-ph | some unusual features observed in hadronic collisions at high energies can be understood assuming that gluons in hadrons are located within small spots occupying only about 10 of the hadrons area such a conjecture about the presence of two scales in hadrons helps to explain why diffractive gluon radiation so much suppr... | [['some', 'unusual', 'features', 'observed', 'in', 'hadronic', 'collisions', 'at', 'high', 'energies', 'can', 'be', 'understood', 'assuming', 'that', 'gluons', 'in', 'hadrons', 'are', 'located', 'within', 'small', 'spots', 'occupying', 'only', 'about', '10', 'of', 'the', 'hadrons', 'area', 'such', 'a', 'conjecture', 'a... | [-0.05811100423387769, 0.32811676184819255, -0.15085076376864756, 0.2598628086630071, -0.07316400157862607, -0.1278971705648956, 0.0012944681342852153, 0.3983590799947212, -0.22283970758341898, -0.26525890115464545, -0.07235035555506195, -0.3336895003578522, 0.002039547017947943, 0.0718620273375878, 0.01222506794865806... |
708.3637 | Geometry of Two-Qubit State and Intertwining Quaternionic Conformal
Mapping Under Local Unitary Transformations | In this paper the geometry of two-qubit systems under local unitary group
$SO(2)\otimes SU(2)$ is discussed. It is shown that the quaternionic conformal
map intertwines between this local unitary subgroup of $Sp(2)$ and the
quaternionic M\"{o}bius transformation which is rather a generalization of the
results of Lee ... | quant-ph | in this paper the geometry of twoqubit systems under local unitary group so2otimes su2 is discussed it is shown that the quaternionic conformal map intertwines between this local unitary subgroup of sp2 and the quaternionic mobius transformation which is rather a generalization of the results of lee et al 2002 quantum ... | [['in', 'this', 'paper', 'the', 'geometry', 'of', 'twoqubit', 'systems', 'under', 'local', 'unitary', 'group', 'so2otimes', 'su2', 'is', 'discussed', 'it', 'is', 'shown', 'that', 'the', 'quaternionic', 'conformal', 'map', 'intertwines', 'between', 'this', 'local', 'unitary', 'subgroup', 'of', 'sp2', 'and', 'the', 'quat... | [-0.12973451998550445, 0.12051260548389771, -0.0947501280514354, 0.011946516009001326, -0.03819648338989778, -0.13806101956658742, 0.018534974328411575, 0.34843943442472003, -0.2742230899843641, -0.2255152037536556, 0.044697515351105145, -0.219415915613486, -0.2670722946185957, 0.1476917315274477, -0.14518243716183035,... |
708.3638 | Spin dynamics in a one-dimensional ferromagnetic Bose gas | We investigate the propagation of spin excitations in a one-dimensional (1D)
ferromagnetic Bose gas. While the spectrum of longitudinal spin waves in this
system is sound-like, the dispersion of transverse spin excitations is
quadratic making a direct application of the Luttinger Liquid (LL) theory
impossible. By usi... | cond-mat.other | we investigate the propagation of spin excitations in a onedimensional 1d ferromagnetic bose gas while the spectrum of longitudinal spin waves in this system is soundlike the dispersion of transverse spin excitations is quadratic making a direct application of the luttinger liquid ll theory impossible by using a combin... | [['we', 'investigate', 'the', 'propagation', 'of', 'spin', 'excitations', 'in', 'a', 'onedimensional', '1d', 'ferromagnetic', 'bose', 'gas', 'while', 'the', 'spectrum', 'of', 'longitudinal', 'spin', 'waves', 'in', 'this', 'system', 'is', 'soundlike', 'the', 'dispersion', 'of', 'transverse', 'spin', 'excitations', 'is',... | [-0.20442382198802772, 0.20311403017563168, -0.0854656426912351, 0.07417769158547301, -0.03705191888979503, -0.13910077238743682, -0.0018785646174191719, 0.32570363668104013, -0.2539111867524861, -0.21712841169819946, 0.014888098149649089, -0.3025799735848393, -0.12240800894353361, 0.18248434425331653, 0.09577124885926... |
708.3639 | Bimodality - a Sign of Critical Behavior in Nuclear Reactions | The recently discovered coexistence of multifragmentation and residue
production for the same total transverse energy of light charged particles can
be well reproduced in numerical simulations of the heavy ion reactions. A
detailed analysis shows that fluctuations (introduced by elementary
nucleon-nucleon collisions)... | nucl-th | the recently discovered coexistence of multifragmentation and residue production for the same total transverse energy of light charged particles can be well reproduced in numerical simulations of the heavy ion reactions a detailed analysis shows that fluctuations introduced by elementary nucleonnucleon collisions deter... | [['the', 'recently', 'discovered', 'coexistence', 'of', 'multifragmentation', 'and', 'residue', 'production', 'for', 'the', 'same', 'total', 'transverse', 'energy', 'of', 'light', 'charged', 'particles', 'can', 'be', 'well', 'reproduced', 'in', 'numerical', 'simulations', 'of', 'the', 'heavy', 'ion', 'reactions', 'a', ... | [-0.0863322966366208, 0.22051405470396968, -0.14066968833850252, 0.11879091076774612, 0.07187460815267903, -0.12735755247662642, -0.008858550234609061, 0.29643854148508536, -0.2485593607139197, -0.32098360676761895, -0.01654127483405838, -0.2979551930024865, -0.010594283763480018, 0.1598663334291251, 0.0653010255714651... |
708.364 | Two-integral distribution functions for axisymmetric systems | Some formulae are presented for finding two-integral distribution functions
(DFs) which depends only on the two classical integrals of the energy and the
magnitude of the angular momentum with respect to the axis of symmetry for
stellar systems with known axisymmetric densities. They come from an
combination of the i... | math-ph astro-ph math.MP | some formulae are presented for finding twointegral distribution functions dfs which depends only on the two classical integrals of the energy and the magnitude of the angular momentum with respect to the axis of symmetry for stellar systems with known axisymmetric densities they come from an combination of the ideas o... | [['some', 'formulae', 'are', 'presented', 'for', 'finding', 'twointegral', 'distribution', 'functions', 'dfs', 'which', 'depends', 'only', 'on', 'the', 'two', 'classical', 'integrals', 'of', 'the', 'energy', 'and', 'the', 'magnitude', 'of', 'the', 'angular', 'momentum', 'with', 'respect', 'to', 'the', 'axis', 'of', 'sy... | [-0.12743942102362282, 0.10842143876248143, -0.11405435476946757, 0.027851882534627163, -0.02521422447992249, -0.0201190274510208, 0.0005608607041050537, 0.33923005639610204, -0.26904448821244153, -0.2966868767036121, 0.09968371165450662, -0.23982844629742328, -0.07422155889980031, 0.19971589826692776, -0.0025601148911... |
708.3641 | Guerra's interpolation using Derrida-Ruelle cascades | New results about Poisson-Dirichlet point processes and Derrida-Ruelle
cascades allow us to express Guerra's interpolation entirely in the language of
Derrida-Ruelle cascades and to streamline Guerra's computations. Moreover, our
approach clarifies the nature of the error terms along the interpolation.
| math.PR math-ph math.MP | new results about poissondirichlet point processes and derridaruelle cascades allow us to express guerras interpolation entirely in the language of derridaruelle cascades and to streamline guerras computations moreover our approach clarifies the nature of the error terms along the interpolation | [['new', 'results', 'about', 'poissondirichlet', 'point', 'processes', 'and', 'derridaruelle', 'cascades', 'allow', 'us', 'to', 'express', 'guerras', 'interpolation', 'entirely', 'in', 'the', 'language', 'of', 'derridaruelle', 'cascades', 'and', 'to', 'streamline', 'guerras', 'computations', 'moreover', 'our', 'approac... | [-0.06288836784660816, 0.027306050166953356, -0.1588113251142204, 0.1584707693546079, -0.10312996231950819, -0.05468060227576643, 0.13303528712131082, 0.30781691391021015, -0.30966256982646884, -0.29715059567242863, 0.0658930058212718, -0.22471036752685905, -0.15866417512297631, 0.18802423003362492, -0.0697782055009156... |
708.3642 | First Run II Measurement of the W Boson Mass | We describe a measurement of the W boson mass mW using 200/pb of root-s =
1.96 TeV p-pbar collision data taken with the CDF II detector. With a sample of
63,964 W -> e nu candidates and 51,128 W -> mu nu candidates, we measure mW =
[80.413 +- 0.034 (stat) +- 0.034 (sys) = 80.413 +- 0.048] GeV/c^2. This is the
single ... | hep-ex | we describe a measurement of the w boson mass mw using 200pb of roots 196 tev ppbar collision data taken with the cdf ii detector with a sample of 63964 w e nu candidates and 51128 w mu nu candidates we measure mw 80413 0034 stat 0034 sys 80413 0048 gevc2 this is the single most precise mw measurement to date when comb... | [['we', 'describe', 'a', 'measurement', 'of', 'the', 'w', 'boson', 'mass', 'mw', 'using', '200pb', 'of', 'roots', '196', 'tev', 'ppbar', 'collision', 'data', 'taken', 'with', 'the', 'cdf', 'ii', 'detector', 'with', 'a', 'sample', 'of', '63964', 'w', 'e', 'nu', 'candidates', 'and', '51128', 'w', 'mu', 'nu', 'candidates'... | [-0.08449960081481639, 0.19508269452777358, -0.05024748913265397, 0.04059670787781799, -0.05997894981439099, -0.19426778438328593, 0.10854226356533206, 0.31378515129104073, -0.17999768809179695, -0.3833080600763177, -0.05544904465708065, -0.3685701760336941, 0.1349927804455805, 0.15133365070918736, 0.03382084704935551,... |
708.3643 | Correlation function of the two-dimensional Ising model on a finite
lattice. II | We calculate the two-point correlation function and magnetic susceptibility
in the anisotropic 2D Ising model on a lattice with one infinite and the other
finite dimension, along which periodic boundary conditions are imposed. Using
exact expressions for a part of lattice form factors, we propose the formulas
for arb... | nlin.SI cond-mat.stat-mech hep-th math-ph math.MP | we calculate the twopoint correlation function and magnetic susceptibility in the anisotropic 2d ising model on a lattice with one infinite and the other finite dimension along which periodic boundary conditions are imposed using exact expressions for a part of lattice form factors we propose the formulas for arbitrary... | [['we', 'calculate', 'the', 'twopoint', 'correlation', 'function', 'and', 'magnetic', 'susceptibility', 'in', 'the', 'anisotropic', '2d', 'ising', 'model', 'on', 'a', 'lattice', 'with', 'one', 'infinite', 'and', 'the', 'other', 'finite', 'dimension', 'along', 'which', 'periodic', 'boundary', 'conditions', 'are', 'impos... | [-0.15408271828257455, 0.15872861713983072, -0.038147174003647595, 0.07939796491736183, -0.06157644342619744, -0.13226691442087474, 0.00019675813808401184, 0.38539274418499414, -0.2031525418548504, -0.21127852923577514, 0.10928862087326352, -0.276895443999731, -0.15301616736914872, 0.16901161399579084, 0.11347882291845... |
708.3644 | Inflation from IIB Superstrings with Fluxes | We study the conditions needed to have an early epoch of inflationary
expansion with a potential coming from IIB superstring theory with fluxes
involving two moduli fields. The phenomenology of this potential is different
from the usual hybrid inflation scenario and we analize the possibility that
the system of field... | astro-ph | we study the conditions needed to have an early epoch of inflationary expansion with a potential coming from iib superstring theory with fluxes involving two moduli fields the phenomenology of this potential is different from the usual hybrid inflation scenario and we analize the possibility that the system of field eq... | [['we', 'study', 'the', 'conditions', 'needed', 'to', 'have', 'an', 'early', 'epoch', 'of', 'inflationary', 'expansion', 'with', 'a', 'potential', 'coming', 'from', 'iib', 'superstring', 'theory', 'with', 'fluxes', 'involving', 'two', 'moduli', 'fields', 'the', 'phenomenology', 'of', 'this', 'potential', 'is', 'differe... | [-0.15599608193376974, 0.14259660377407976, -0.13527347845205617, 0.06165754518799311, -0.06535510270999023, -0.10857875664312873, -0.014630144384066244, 0.29430937857156797, -0.252138102066613, -0.2879082856628473, 0.10052033184911124, -0.2112209731675384, -0.14569686970395607, 0.15723571103937442, -0.0273307254537940... |
708.3645 | Why Tau First? | Electron neutrino has been the first neutral lepton to be foreseen and
discovered last century. The un-ordered muon and its neutrino arose later by
cosmic rays. The tau discover, the heaviest, the most unstable charged lepton,
was found surprisingly on 1975. Its neutrino was hardly revealed just on 2000.
So why High ... | astro-ph hep-ph | electron neutrino has been the first neutral lepton to be foreseen and discovered last century the unordered muon and its neutrino arose later by cosmic rays the tau discover the heaviest the most unstable charged lepton was found surprisingly on 1975 its neutrino was hardly revealed just on 2000 so why high energy neu... | [['electron', 'neutrino', 'has', 'been', 'the', 'first', 'neutral', 'lepton', 'to', 'be', 'foreseen', 'and', 'discovered', 'last', 'century', 'the', 'unordered', 'muon', 'and', 'its', 'neutrino', 'arose', 'later', 'by', 'cosmic', 'rays', 'the', 'tau', 'discover', 'the', 'heaviest', 'the', 'most', 'unstable', 'charged',... | [-0.0575406298157759, 0.34068698974104855, -0.025351807100056096, 0.227553549788094, -0.08909394413266065, -0.11382880431622089, 0.006986025328625969, 0.3521350193269817, -0.23987520810970592, -0.3157906473192963, 0.0452001579012306, -0.33587484029565184, 0.010114390081504271, 0.19347568592049702, 0.049017309642208386,... |
708.3646 | Complex solitons with power law behaviour in Bose-Einstein condensates
near Feshbach resonance | Complex, localized stable solitons, characterized by a power law behaviour,
are found for a quasi-one-dimensional Bose-Einstein condensate near Feshbach
resonance. Both dark and bright solitons can be excited in the experimentally
allowed parameter domain, when two and three-body interactions are respectively
repulsi... | cond-mat.other | complex localized stable solitons characterized by a power law behaviour are found for a quasionedimensional boseeinstein condensate near feshbach resonance both dark and bright solitons can be excited in the experimentally allowed parameter domain when two and threebody interactions are respectively repulsive and attr... | [['complex', 'localized', 'stable', 'solitons', 'characterized', 'by', 'a', 'power', 'law', 'behaviour', 'are', 'found', 'for', 'a', 'quasionedimensional', 'boseeinstein', 'condensate', 'near', 'feshbach', 'resonance', 'both', 'dark', 'and', 'bright', 'solitons', 'can', 'be', 'excited', 'in', 'the', 'experimentally', '... | [-0.1842589006118942, 0.26095545776964474, -0.040473063333896185, 0.08169682518564514, -0.06799676441490494, -0.22917318657467453, -0.011167216388760911, 0.3919582962601756, -0.22591773762057224, -0.2588685629986382, 0.053147783073654864, -0.28189178387401626, -0.054754067852627486, 0.17433390123430095, 0.0906364479499... |
708.3647 | Sub-Threshold Field Emission from Thin Silicon Membranes | We report on strongly enhanced electron multiplication in thin silicon
membranes. The device is configured as a transmission-type membrane for
electron multiplication. A sub-threshold electric field applied on the emission
side of the membrane enhances the number of electrons emitted by two orders of
magnitude. This ... | cond-mat.mes-hall | we report on strongly enhanced electron multiplication in thin silicon membranes the device is configured as a transmissiontype membrane for electron multiplication a subthreshold electric field applied on the emission side of the membrane enhances the number of electrons emitted by two orders of magnitude this enhance... | [['we', 'report', 'on', 'strongly', 'enhanced', 'electron', 'multiplication', 'in', 'thin', 'silicon', 'membranes', 'the', 'device', 'is', 'configured', 'as', 'a', 'transmissiontype', 'membrane', 'for', 'electron', 'multiplication', 'a', 'subthreshold', 'electric', 'field', 'applied', 'on', 'the', 'emission', 'side', '... | [-0.16368190191038276, 0.24683824110357766, 0.010095713862582394, -0.030924896659849186, 0.019319405259591513, -0.15228569888226365, 0.022800379277517397, 0.4117062554519246, -0.24171561606066383, -0.29927522856472194, -0.03813244538901347, -0.32176159823649103, -0.0877716661957295, 0.24841554325235926, -0.019038607028... |
708.3648 | Evidence of a Broad Relativistic Iron Line from the Neutron Star
Low-Mass X-ray Binary Serpens X-1 | We report on an analysis of XMM-Newton data from the neutron star low mass
X-ray binary (LMXB) Serpens X-1 (Ser X-1). Spectral analysis of EPIC PN data
indicates that the previously known broad iron K$\alpha$ emission line from
this source has a significantly skewed structure with a moderately extended red
wing. The ... | astro-ph | we report on an analysis of xmmnewton data from the neutron star low mass xray binary lmxb serpens x1 ser x1 spectral analysis of epic pn data indicates that the previously known broad iron kalpha emission line from this source has a significantly skewed structure with a moderately extended red wing the asymmetric shap... | [['we', 'report', 'on', 'an', 'analysis', 'of', 'xmmnewton', 'data', 'from', 'the', 'neutron', 'star', 'low', 'mass', 'xray', 'binary', 'lmxb', 'serpens', 'x1', 'ser', 'x1', 'spectral', 'analysis', 'of', 'epic', 'pn', 'data', 'indicates', 'that', 'the', 'previously', 'known', 'broad', 'iron', 'kalpha', 'emission', 'lin... | [-0.07179727564299745, 0.04083644576783713, -0.05946926376782358, 0.08769476087209546, -0.1321639144671194, -0.1153939955518581, 0.0696454242270972, 0.4326946023053357, -0.18716935225363288, -0.3308863292093433, 0.07414950950159913, -0.3009235952049494, -0.0409547286767823, 0.22553992776000606, -0.04595125552732497, -0... |
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