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706.4114 | Searches for New Physics at HERA | The high energy programme of the HERA collider ended in March 2007. During
the whole HERA programme, a combined total integrated luminosity of 1 fb$^{-1}$
was collected by the H1 and ZEUS experiments. In this context, an overview of
the most recent results of both experiments concerning searches for new physics
is pr... | hep-ex | the high energy programme of the hera collider ended in march 2007 during the whole hera programme a combined total integrated luminosity of 1 fb1 was collected by the h1 and zeus experiments in this context an overview of the most recent results of both experiments concerning searches for new physics is presented the ... | [['the', 'high', 'energy', 'programme', 'of', 'the', 'hera', 'collider', 'ended', 'in', 'march', '2007', 'during', 'the', 'whole', 'hera', 'programme', 'a', 'combined', 'total', 'integrated', 'luminosity', 'of', '1', 'fb1', 'was', 'collected', 'by', 'the', 'h1', 'and', 'zeus', 'experiments', 'in', 'this', 'context', 'a... | [-0.057375816770306814, 0.15887181077130486, -0.06555846224541821, 0.13549330222942843, -0.07347201278842078, -0.07142773760119225, -0.024833379563216757, 0.3258047034827674, -0.13661322508308263, -0.37676265897093025, 0.10820744131839402, -0.3705285605406616, -0.001747556893927295, 0.19292829550019033, 0.0929991029112... |
706.4115 | TMC-1C: an accreting starless core | We have mapped the starless core TMC-1C in a variety of molecular lines with
the IRAM 30m telescope. High density tracers show clear signs of
self-absorption and sub-sonic infall asymmetries are present in N2H+ (1-0) and
DCO+ (2-1) lines. The inward velocity profile in N2H+ (1-0) is extended over a
region of about 7,... | astro-ph | we have mapped the starless core tmc1c in a variety of molecular lines with the iram 30m telescope high density tracers show clear signs of selfabsorption and subsonic infall asymmetries are present in n2h 10 and dco 21 lines the inward velocity profile in n2h 10 is extended over a region of about 7000 au in radius aro... | [['we', 'have', 'mapped', 'the', 'starless', 'core', 'tmc1c', 'in', 'a', 'variety', 'of', 'molecular', 'lines', 'with', 'the', 'iram', '30m', 'telescope', 'high', 'density', 'tracers', 'show', 'clear', 'signs', 'of', 'selfabsorption', 'and', 'subsonic', 'infall', 'asymmetries', 'are', 'present', 'in', 'n2h', '10', 'and... | [-0.024203838263007052, 0.12591484549449605, -0.0011849069351356635, 0.015466633951291442, 0.012121983957116191, -0.052293416568484734, 0.05406599325819833, 0.4404624946756472, -0.16040300954291908, -0.31281652484863054, 0.07069801452363067, -0.2694937097151357, 0.0523389014825356, 0.07776818279108084, 0.02998948946183... |
706.4116 | Star Formation in Molecular Clouds? | Using studies of nearby star formation with Spitzer, I will argue that star
formation is restricted to dense cores within molecular clouds. The nature of
these dense cores and their connection to star formation will be discussed.
Their distribution over masses and over the cloud is similar to that of stars,
and their... | astro-ph | using studies of nearby star formation with spitzer i will argue that star formation is restricted to dense cores within molecular clouds the nature of these dense cores and their connection to star formation will be discussed their distribution over masses and over the cloud is similar to that of stars and their effic... | [['using', 'studies', 'of', 'nearby', 'star', 'formation', 'with', 'spitzer', 'i', 'will', 'argue', 'that', 'star', 'formation', 'is', 'restricted', 'to', 'dense', 'cores', 'within', 'molecular', 'clouds', 'the', 'nature', 'of', 'these', 'dense', 'cores', 'and', 'their', 'connection', 'to', 'star', 'formation', 'will',... | [-0.07624056734758514, 0.13363352263359746, -0.06509773979139338, 0.08395476625024152, -0.08199936845437526, 0.017835012396107186, 0.07182636376453232, 0.4221575496705262, -0.18115455620772355, -0.3167929437298041, 0.0332114271098305, -0.2554093408626276, -0.028772766042461657, 0.14720438879107, -0.031121586125435217, ... |
706.4117 | Vector-Boson Production of Light Higgs Pairs in 2-Higgs Doublet Models | At the Large Hadron Collider, we prove the feasibility to detect pair
production of the lightest CP-even Higgs boson $h$ of Type II 2-Higgs Doublet
Models through $q q^{(')}\to q q^{(')} {hh}$ (vector-boson fusion). We also
show that, through the $hh\to 4b$ decay channel in presence of heavy-flavour
tagging, further ... | hep-ph | at the large hadron collider we prove the feasibility to detect pair production of the lightest cpeven higgs boson h of type ii 2higgs doublet models through q qto q q hh vectorboson fusion we also show that through the hhto 4b decay channel in presence of heavyflavour tagging further exploiting forwardbackward jet sam... | [['at', 'the', 'large', 'hadron', 'collider', 'we', 'prove', 'the', 'feasibility', 'to', 'detect', 'pair', 'production', 'of', 'the', 'lightest', 'cpeven', 'higgs', 'boson', 'h', 'of', 'type', 'ii', '2higgs', 'doublet', 'models', 'through', 'q', 'qto', 'q', 'q', 'hh', 'vectorboson', 'fusion', 'we', 'also', 'show', 'tha... | [-0.10784235378741869, 0.19511443672106704, -0.026981576611029193, 0.12363682149185075, -0.10279372720914479, -0.282978772961845, 0.03641538350428972, 0.3314310109611445, -0.2838122280146409, -0.18934171585068624, -0.05860434192355671, -0.2684529050020501, 0.054992897177322045, 0.08259029385064626, 0.11226650277320813,... |
706.4118 | Nonlinear Schrodinger-Helmholtz Equation as Numerical Regularization of
the Nonlinear Schrodinger Equation | A regularized $\alpha-$system of the Nonlinear Schr\"{o}dinger Equation (NLS)
with $2\sigma$ nonlinear power in dimension $N$ is studied. We prove existence
and uniqueness of local solution in the case $1 \le \sigma <\frac{4}{N-2}$ and
existence and uniqueness of global solution in the case $1 \le \sigma <
\frac{4}{N... | math.AP math-ph math.MP | a regularized alphasystem of the nonlinear schrodinger equation nls with 2sigma nonlinear power in dimension n is studied we prove existence and uniqueness of local solution in the case 1 le sigma frac4n2 and existence and uniqueness of global solution in the case 1 le sigma frac4n when alpha to 0 this regularized syst... | [['a', 'regularized', 'alphasystem', 'of', 'the', 'nonlinear', 'schrodinger', 'equation', 'nls', 'with', '2sigma', 'nonlinear', 'power', 'in', 'dimension', 'n', 'is', 'studied', 'we', 'prove', 'existence', 'and', 'uniqueness', 'of', 'local', 'solution', 'in', 'the', 'case', '1', 'le', 'sigma', 'frac4n2', 'and', 'existe... | [-0.12987175820778837, 0.030741411306913578, -0.040041445101629575, 0.06260991538190008, -0.03840238711449737, -0.1644868662571717, -0.021444462541052523, 0.2732049078114477, -0.2785927697870077, -0.22140757142401793, 0.12786843752552407, -0.3345079149904789, -0.11933974532282673, 0.15179981342425533, -0.01130566559960... |
706.4119 | Relating multichannel scattering and production amplitudes in a
microscopic OZI-based model | Relations between scattering and production amplitudes are studied in a
microscopic multichannel model for meson-meson scattering, with coupling to
confined quark-antiquark channels. Overlapping resonances and a proper
threshold behaviour are treated exactly in the model. Under the spectator
assumption, it is found t... | hep-ph | relations between scattering and production amplitudes are studied in a microscopic multichannel model for mesonmeson scattering with coupling to confined quarkantiquark channels overlapping resonances and a proper threshold behaviour are treated exactly in the model under the spectator assumption it is found that the ... | [['relations', 'between', 'scattering', 'and', 'production', 'amplitudes', 'are', 'studied', 'in', 'a', 'microscopic', 'multichannel', 'model', 'for', 'mesonmeson', 'scattering', 'with', 'coupling', 'to', 'confined', 'quarkantiquark', 'channels', 'overlapping', 'resonances', 'and', 'a', 'proper', 'threshold', 'behaviou... | [-0.13747644922854801, 0.20329571275294506, -0.08006591609763829, 0.11020050760231573, -0.025973631945354018, -0.14905353685290637, 0.0003633941645437682, 0.34142524417151104, -0.2674480398778211, -0.19622357617217032, 0.008487998698414727, -0.34422505709596657, -0.14020639873871749, 0.13775713118428196, 0.075799784405... |
706.412 | Optical 'Shorting Wires' | Connecting lumped circuit elements in a conventional circuit is usually
accomplished by conducting wires that act as conduits for the conduction
currents with negligible potential drops. More challenging, however, is to
extend these concepts to optical nanocircuit elements. Here, following our
recent development of o... | cond-mat.mtrl-sci | connecting lumped circuit elements in a conventional circuit is usually accomplished by conducting wires that act as conduits for the conduction currents with negligible potential drops more challenging however is to extend these concepts to optical nanocircuit elements here following our recent development of optical ... | [['connecting', 'lumped', 'circuit', 'elements', 'in', 'a', 'conventional', 'circuit', 'is', 'usually', 'accomplished', 'by', 'conducting', 'wires', 'that', 'act', 'as', 'conduits', 'for', 'the', 'conduction', 'currents', 'with', 'negligible', 'potential', 'drops', 'more', 'challenging', 'however', 'is', 'to', 'extend'... | [-0.14504572784865338, 0.18474727818720985, 0.054588185623288155, -0.0642095242289762, -0.08392385569208398, -0.20919723753100153, 0.029991656335755842, 0.4490957819353575, -0.21504185400132475, -0.2932747921039318, 0.06186522856012158, -0.26541390011204813, -0.14515353120788504, 0.23430694475630834, -0.053509762735459... |
706.4121 | Analytic Bethe Ansatz and Baxter equations for long-range psl(2|2) spin
chain | We study the largest particle-number-preserving sector of the dilatation
operator in maximally supersymmetric gauge theory. After exploring one-loop
Bethe Ansatze for the underlying spin chain with psl(2|2) symmetry for simple
root systems related to several Kac-Dynkin diagrams, we use the analytic Bethe
Anzats to co... | hep-th | we study the largest particlenumberpreserving sector of the dilatation operator in maximally supersymmetric gauge theory after exploring oneloop bethe ansatze for the underlying spin chain with psl22 symmetry for simple root systems related to several kacdynkin diagrams we use the analytic bethe anzats to construct eig... | [['we', 'study', 'the', 'largest', 'particlenumberpreserving', 'sector', 'of', 'the', 'dilatation', 'operator', 'in', 'maximally', 'supersymmetric', 'gauge', 'theory', 'after', 'exploring', 'oneloop', 'bethe', 'ansatze', 'for', 'the', 'underlying', 'spin', 'chain', 'with', 'psl22', 'symmetry', 'for', 'simple', 'root', ... | [-0.12198586849512909, 0.1858809116407886, -0.00271791953413513, 0.12132154739936071, -0.0996503772276905, -0.13488932799239375, 0.0004940225515640312, 0.3430584405143202, -0.21940616186725354, -0.25181047449836885, 0.0897151358994124, -0.2838361855722004, -0.17606305972633005, 0.12425284112797924, -0.02351663110767379... |
706.4122 | Magnetic Energy and Helicity Budgets in the Active-Region Solar Corona.
I. Linear Force-Free Approximation | We self-consistently derive the magnetic energy and relative magnetic
helicity budgets of a three-dimensional linear force-free magnetic structure
rooted in a lower boundary plane. For the potential magnetic energy we derive a
general expression that gives results practically equivalent to those of the
magnetic Viria... | astro-ph | we selfconsistently derive the magnetic energy and relative magnetic helicity budgets of a threedimensional linear forcefree magnetic structure rooted in a lower boundary plane for the potential magnetic energy we derive a general expression that gives results practically equivalent to those of the magnetic virial theo... | [['we', 'selfconsistently', 'derive', 'the', 'magnetic', 'energy', 'and', 'relative', 'magnetic', 'helicity', 'budgets', 'of', 'a', 'threedimensional', 'linear', 'forcefree', 'magnetic', 'structure', 'rooted', 'in', 'a', 'lower', 'boundary', 'plane', 'for', 'the', 'potential', 'magnetic', 'energy', 'we', 'derive', 'a',... | [-0.1389057653674778, 0.16262853676313777, -0.025446925070718864, 0.1296298954941449, -0.09345388437116829, -0.023203697443629306, 0.047981517908435, 0.37269262922151636, -0.20836482059918732, -0.36109133350158423, 0.027783218361340307, -0.1854555147210097, -0.11253739211630696, 0.21588824624583747, -0.0203851464417918... |
706.4123 | Level crossing in the three-body problem for strongly interacting
fermions in a harmonic trap | We present a solution of the three-fermion problem in a harmonic potential
across a Feshbach resonance. We compare the spectrum with that of the two-body
problem and show that it is energetically unfavorable for the three fermions to
occupy one lattice site rather than two. We also demonstrate the existence of
an ene... | cond-mat.other | we present a solution of the threefermion problem in a harmonic potential across a feshbach resonance we compare the spectrum with that of the twobody problem and show that it is energetically unfavorable for the three fermions to occupy one lattice site rather than two we also demonstrate the existence of an energy le... | [['we', 'present', 'a', 'solution', 'of', 'the', 'threefermion', 'problem', 'in', 'a', 'harmonic', 'potential', 'across', 'a', 'feshbach', 'resonance', 'we', 'compare', 'the', 'spectrum', 'with', 'that', 'of', 'the', 'twobody', 'problem', 'and', 'show', 'that', 'it', 'is', 'energetically', 'unfavorable', 'for', 'the', ... | [-0.15931958547215672, 0.14861906241478923, -0.06772309550543941, 0.06668123451527208, -0.004336801575661837, -0.10962337257835685, 0.08813724830404773, 0.372728870214918, -0.23872011805636972, -0.2560216046728288, 0.054274768500789244, -0.2962000903826726, -0.13161716113291397, 0.15131772100288846, 0.08644637457224764... |
706.4124 | On the origin of X-ray emission in some FR Is: ADAF or jet? | We investigate the X-ray origin in FR Is using the radio, submillimetre,
optical, and {\em Chandra} X-ray data of a small sample consisting of eight FR
I sources. These sources are very dim, with X-ray luminosities $L_{\rm
X}/L_{\rm Edd} \sim 10^{-4}-10^{-8}$ ($L_{\rm X}$ is the X-ray luminosity
between 2-10 keV). We... | astro-ph | we investigate the xray origin in fr is using the radio submillimetre optical and em chandra xray data of a small sample consisting of eight fr i sources these sources are very dim with xray luminosities l_rm xl_rm edd sim 104108 l_rm x is the xray luminosity between 210 kev we try to fit the multiwaveband spectrum usi... | [['we', 'investigate', 'the', 'xray', 'origin', 'in', 'fr', 'is', 'using', 'the', 'radio', 'submillimetre', 'optical', 'and', 'em', 'chandra', 'xray', 'data', 'of', 'a', 'small', 'sample', 'consisting', 'of', 'eight', 'fr', 'i', 'sources', 'these', 'sources', 'are', 'very', 'dim', 'with', 'xray', 'luminosities', 'l_rm'... | [-0.061812213957773865, 0.129287489825752, -0.030437135390231226, 0.13651181032859835, -0.059611282198008125, -0.09137723987672502, 0.012953649450008289, 0.44127834048670006, -0.20373558976955322, -0.3093999457588188, 0.13153929081349786, -0.3531439259885719, 0.03766831168311411, 0.2558758407704576, -0.0111382684828842... |
706.4125 | Numerical Simulation of an Electroweak Oscillon | Numerical simulations of the bosonic sector of the $SU(2)\times U(1)$
electroweak Standard Model in 3+1 dimensions have demonstrated the existence of
an oscillon -- an extremely long-lived, localized, oscillatory solution to the
equations of motion -- when the Higgs mass is equal to twice the $W^\pm$ boson
mass. It c... | hep-th hep-lat hep-ph nlin.AO | numerical simulations of the bosonic sector of the su2times u1 electroweak standard model in 31 dimensions have demonstrated the existence of an oscillon an extremely longlived localized oscillatory solution to the equations of motion when the higgs mass is equal to twice the wpm boson mass it contains total energy rou... | [['numerical', 'simulations', 'of', 'the', 'bosonic', 'sector', 'of', 'the', 'su2times', 'u1', 'electroweak', 'standard', 'model', 'in', '31', 'dimensions', 'have', 'demonstrated', 'the', 'existence', 'of', 'an', 'oscillon', 'an', 'extremely', 'longlived', 'localized', 'oscillatory', 'solution', 'to', 'the', 'equations... | [-0.1512486713871892, 0.2196620648523094, -0.033979612489097887, 0.12072656306637718, -0.020702836286675717, -0.1126619384624064, -0.027747799043676684, 0.30398657601326706, -0.17693735768220253, -0.30099190685432403, 0.05923216296027282, -0.296324474470956, -0.01753277499228716, 0.14753583745166127, 0.0315799494103495... |
706.4126 | Current-voltage curves for molecular junctions: the effect of
substituents | We present current-voltage (I-V) curves for phenylene ethynylene oligomers
between two Au surfaces computed using a Density Functional Theory/Green's
Function approach. In addition to the parent molecule, two different
substituents are considered: one where all the hydrogens are replaced by
chlorines and a second whe... | cond-mat.mes-hall | we present currentvoltage iv curves for phenylene ethynylene oligomers between two au surfaces computed using a density functional theorygreens function approach in addition to the parent molecule two different substituents are considered one where all the hydrogens are replaced by chlorines and a second where one h is... | [['we', 'present', 'currentvoltage', 'iv', 'curves', 'for', 'phenylene', 'ethynylene', 'oligomers', 'between', 'two', 'au', 'surfaces', 'computed', 'using', 'a', 'density', 'functional', 'theorygreens', 'function', 'approach', 'in', 'addition', 'to', 'the', 'parent', 'molecule', 'two', 'different', 'substituents', 'are... | [-0.09981497738267159, 0.14986616156331284, 0.0029017547187009814, 0.05234962771275929, 0.014752392234446802, -0.16182952962080194, 0.08586414578106777, 0.3824194998296488, -0.2659594013895484, -0.3203243150191892, 0.02326396356001615, -0.31139938796686517, -0.07915422750880147, 0.15217976248229909, -0.0188065538669277... |
706.4127 | Semiclassical Density of States for the Quantum Asymmetric Top | In the quantization of a rotating rigid body, a {\it top,} one is concerned
with the Hamiltonian operator $L_\alpha=\alpha_0^2 L_x^2 + \alpha_1^2 L_y^2 +
\alpha_2^2 L_z^2,$ where $\alpha_0 < \alpha_1 <\alpha_2.$ An explicit formula
is known for the eigenvalues of $L_\alpha$ in the case of the spherical top
($\alpha_1... | math-ph math.MP | in the quantization of a rotating rigid body a it top one is concerned with the hamiltonian operator l_alphaalpha_02 l_x2 alpha_12 l_y2 alpha_22 l_z2 where alpha_0 alpha_1 alpha_2 an explicit formula is known for the eigenvalues of l_alpha in the case of the spherical top alpha_1 alpha_2 alpha_3 and symmetrical top alp... | [['in', 'the', 'quantization', 'of', 'a', 'rotating', 'rigid', 'body', 'a', 'it', 'top', 'one', 'is', 'concerned', 'with', 'the', 'hamiltonian', 'operator', 'l_alphaalpha_02', 'l_x2', 'alpha_12', 'l_y2', 'alpha_22', 'l_z2', 'where', 'alpha_0', 'alpha_1', 'alpha_2', 'an', 'explicit', 'formula', 'is', 'known', 'for', 'th... | [-0.1849216117819735, 0.16651389841569555, -0.021385505361464417, 0.06993818592542367, -0.035297253485588195, -0.19774316221439434, -0.016649004269743934, 0.3169118099059295, -0.16401922493467777, -0.2264722979817431, 0.02245180239760796, -0.2983536758794657, -0.13010969819745175, 0.1907812402791624, -0.012795766784461... |
706.4128 | A review of wildland fire spread modelling, 1990-present 2: Empirical
and quasi-empirical models | In recent years, advances in computational power and spatial data analysis
(GIS, remote sensing, etc) have led to an increase in attempts to model the
spread and behaviour of wildland fires across the landscape. This series of
review papers endeavours to critically and comprehensively review all types of
surface fire... | physics.geo-ph physics.ao-ph | in recent years advances in computational power and spatial data analysis gis remote sensing etc have led to an increase in attempts to model the spread and behaviour of wildland fires across the landscape this series of review papers endeavours to critically and comprehensively review all types of surface fire spread ... | [['in', 'recent', 'years', 'advances', 'in', 'computational', 'power', 'and', 'spatial', 'data', 'analysis', 'gis', 'remote', 'sensing', 'etc', 'have', 'led', 'to', 'an', 'increase', 'in', 'attempts', 'to', 'model', 'the', 'spread', 'and', 'behaviour', 'of', 'wildland', 'fires', 'across', 'the', 'landscape', 'this', 's... | [-0.058030017911126684, 0.05005172124159193, -0.07956040249458358, 0.04512540476571303, -0.05241979973248413, -0.08248940985423461, 0.05574882706423523, 0.37441096432222465, -0.2454655874106619, -0.358117764401767, 0.13822240882695447, -0.3177856697293464, -0.16873268125830995, 0.22067197903783786, -0.07617568322328022... |
706.4129 | Shape Coexistence and Mixing in 152Sm | Experimental studies of 152Sm using multiple-step Coulomb excitation and
inelastic neutron scattering provide key data that clarify the low-energy
collective structure of this nucleus. No candidates for two-phonon
beta-vibrational states are found. Experimental level energies of the
ground-state and first excited (0+... | nucl-ex | experimental studies of 152sm using multiplestep coulomb excitation and inelastic neutron scattering provide key data that clarify the lowenergy collective structure of this nucleus no candidates for twophonon betavibrational states are found experimental level energies of the groundstate and first excited 0 state rota... | [['experimental', 'studies', 'of', '152sm', 'using', 'multiplestep', 'coulomb', 'excitation', 'and', 'inelastic', 'neutron', 'scattering', 'provide', 'key', 'data', 'that', 'clarify', 'the', 'lowenergy', 'collective', 'structure', 'of', 'this', 'nucleus', 'no', 'candidates', 'for', 'twophonon', 'betavibrational', 'stat... | [-0.12972561904208976, 0.2540465954149587, 0.0012006995814811924, 0.09495524757759362, 0.03283531107919534, -0.12924469777625863, 0.09417252606995728, 0.37658281077671313, -0.21208917009947903, -0.2705947352603645, -0.04327635556135489, -0.3174742408015806, -0.05195315253070515, 0.09728082825692938, 0.13865015895419713... |
706.413 | A review of wildland fire spread modelling, 1990-present 3: Mathematical
analogues and simulation models | In recent years, advances in computational power and spatial data analysis
(GIS, remote sensing, etc) have led to an increase in attempts to model the
spread and behvaiour of wildland fires across the landscape. This series of
review papers endeavours to critically and comprehensively review all types of
surface fire... | physics.geo-ph physics.ao-ph | in recent years advances in computational power and spatial data analysis gis remote sensing etc have led to an increase in attempts to model the spread and behvaiour of wildland fires across the landscape this series of review papers endeavours to critically and comprehensively review all types of surface fire spread ... | [['in', 'recent', 'years', 'advances', 'in', 'computational', 'power', 'and', 'spatial', 'data', 'analysis', 'gis', 'remote', 'sensing', 'etc', 'have', 'led', 'to', 'an', 'increase', 'in', 'attempts', 'to', 'model', 'the', 'spread', 'and', 'behvaiour', 'of', 'wildland', 'fires', 'across', 'the', 'landscape', 'this', 's... | [-0.033361617657903804, 0.06803497242183178, -0.07737443456837141, 0.07941538758014384, -0.07041164849172621, -0.12836793092873824, 0.012500204502687077, 0.38244799973224014, -0.23433967038564493, -0.32740186592563986, 0.1516810547423494, -0.31878514504334066, -0.19880401723442928, 0.21193423332263003, -0.0935925889897... |
706.4131 | On some power sum problems of Montgomery and Turan | We use an estimate for character sums over finite fields of Katz to solve
open problems of Montgomery and Turan. Let h=>2 be an integer. We prove that
inf_{|z_k| => 1} max_{v=1,...,n^h} |sum_{k=1}^n z_k^v| <= (h-1+o(1)) sqrt n.
This gives the right order of magnitude for the quantity and improves on a
bound of Erdos-... | math.NT | we use an estimate for character sums over finite fields of katz to solve open problems of montgomery and turan let h2 be an integer we prove that inf_z_k 1 max_v1nh sum_k1n z_kv h1o1 sqrt n this gives the right order of magnitude for the quantity and improves on a bound of erdosrenyi by a factor of the order sqrt log ... | [['we', 'use', 'an', 'estimate', 'for', 'character', 'sums', 'over', 'finite', 'fields', 'of', 'katz', 'to', 'solve', 'open', 'problems', 'of', 'montgomery', 'and', 'turan', 'let', 'h2', 'be', 'an', 'integer', 'we', 'prove', 'that', 'inf_z_k', '1', 'max_v1nh', 'sum_k1n', 'z_kv', 'h1o1', 'sqrt', 'n', 'this', 'gives', 't... | [-0.14908583280790982, 0.11942117854376758, -0.062328194589193524, 0.025674034405804784, -0.024410345382859994, -0.11743704532273114, 0.029527345864937223, 0.26841559428079376, -0.26040300416984946, -0.31348691029666825, 0.06790314799431584, -0.35510965687190665, -0.0772203511994027, 0.19633457418691752, -0.06221067187... |
706.4132 | Using the Renormalization Group Functions to Uniquely Determine the
Effective Potential in Massless Scalar Electrodynamics | It has been demonstrated that the effective potential V(\phi) in a massless
O(N) \lambda \phi^4_4 model is determined completely by the renormalization
group functions provided the renormalization condition \frac{d^4V}{d
\phi^4}|_{\phi=\mu}=\lambda is used. This is shown to also hold in massless
scalar electrodynamic... | hep-th | it has been demonstrated that the effective potential vphi in a massless on lambda phi4_4 model is determined completely by the renormalization group functions provided the renormalization condition fracd4vd phi4_phimulambda is used this is shown to also hold in massless scalar electrodynamics by employing a variant of... | [['it', 'has', 'been', 'demonstrated', 'that', 'the', 'effective', 'potential', 'vphi', 'in', 'a', 'massless', 'on', 'lambda', 'phi4_4', 'model', 'is', 'determined', 'completely', 'by', 'the', 'renormalization', 'group', 'functions', 'provided', 'the', 'renormalization', 'condition', 'fracd4vd', 'phi4_phimulambda', 'is... | [-0.12001278215561002, 0.13011623522828494, -0.15355084676827704, 0.1014328914036649, -0.06758607634239727, -0.1610987790387183, -0.01861538857753788, 0.3408899653466448, -0.2010045111593273, -0.2551713965034911, 0.015934172725778014, -0.28856622698228984, -0.16836723244734228, 0.18700638095227382, 0.015624093937702359... |
706.4133 | The proper motion of the Arches cluster with Keck Laser-Guide Star
Adaptive Optics | We present the first measurement of the proper motion of the young, compact
Arches cluster near the Galactic center from near-infrared adaptive optics (AO)
data taken with the recently commissioned laser-guide star (LGS) at the Keck
10-m telescope. The excellent astrometric accuracy achieved with LGS-AO
provides the ... | astro-ph | we present the first measurement of the proper motion of the young compact arches cluster near the galactic center from nearinfrared adaptive optics ao data taken with the recently commissioned laserguide star lgs at the keck 10m telescope the excellent astrometric accuracy achieved with lgsao provides the basis for a ... | [['we', 'present', 'the', 'first', 'measurement', 'of', 'the', 'proper', 'motion', 'of', 'the', 'young', 'compact', 'arches', 'cluster', 'near', 'the', 'galactic', 'center', 'from', 'nearinfrared', 'adaptive', 'optics', 'ao', 'data', 'taken', 'with', 'the', 'recently', 'commissioned', 'laserguide', 'star', 'lgs', 'at',... | [-0.09257557815212579, 0.07200285610575992, -0.11088652186113197, 0.04362573967682382, -0.10250490283952715, -0.04666216906045687, 0.06456752341247002, 0.3999933061021485, -0.2166348616775354, -0.344424173824923, 0.06422985794774412, -0.2541166938199271, 0.00955560362227134, 0.18595389966652712, -0.03985060735232373, -... |
706.4134 | Bounds on the number of real solutions to polynomial equations | We use Gale duality for polynomial complete intersections and adapt the proof
of the fewnomial bound for positive solutions to obtain the bound (e^4+3) 2^(k
choose 2) n^k/4 for the number of non-zero real solutions to a system of n
polynomials in n variables having n+k+1 monomials whose exponent vectors
generate a su... | math.AG | we use gale duality for polynomial complete intersections and adapt the proof of the fewnomial bound for positive solutions to obtain the bound e43 2k choose 2 nk4 for the number of nonzero real solutions to a system of n polynomials in n variables having nk1 monomials whose exponent vectors generate a subgroup of zn o... | [['we', 'use', 'gale', 'duality', 'for', 'polynomial', 'complete', 'intersections', 'and', 'adapt', 'the', 'proof', 'of', 'the', 'fewnomial', 'bound', 'for', 'positive', 'solutions', 'to', 'obtain', 'the', 'bound', 'e43', '2k', 'choose', '2', 'nk4', 'for', 'the', 'number', 'of', 'nonzero', 'real', 'solutions', 'to', 'a... | [-0.2041805203032975, 0.15010692982184815, -0.044403469655662775, 0.04391233496106707, -0.042787192549085154, -0.23487569288444343, 0.0932552115523211, 0.22991519852927544, -0.2352994598629998, -0.3106992542800471, 0.09578729418770797, -0.3135838550401897, -0.11831223579952721, 0.15438985191967067, -0.01629932505283050... |
706.4135 | Simple Two-Dimensional Model for the Elastic Origin of Cooperativity
among Spin States of Spin-Crossover Complexes | We study the origin of the cooperative nature of spin crossover (SC) between
low spin (LS) and high spin (HS) states from the view point of elastic
interactions among molecules. As the size of each molecule changes depending on
its spin state, the elastic interaction among the lattice distortions provides
the coopera... | cond-mat.str-el cond-mat.stat-mech | we study the origin of the cooperative nature of spin crossover sc between low spin ls and high spin hs states from the view point of elastic interactions among molecules as the size of each molecule changes depending on its spin state the elastic interaction among the lattice distortions provides the cooperative inter... | [['we', 'study', 'the', 'origin', 'of', 'the', 'cooperative', 'nature', 'of', 'spin', 'crossover', 'sc', 'between', 'low', 'spin', 'ls', 'and', 'high', 'spin', 'hs', 'states', 'from', 'the', 'view', 'point', 'of', 'elastic', 'interactions', 'among', 'molecules', 'as', 'the', 'size', 'of', 'each', 'molecule', 'changes',... | [-0.1681169398925117, 0.1938456975941306, -0.0655831020079448, 0.02684708153678765, -0.017454951845725337, -0.11812891925294552, 0.06057077409293983, 0.33435100614423713, -0.2979626679913171, -0.27170057832864264, -0.004503400564464109, -0.30495810226326986, -0.13220574120585357, 0.08259303374929473, 0.1208522052188674... |
706.4136 | An improved method for estimating source densities using the temporal
distribution of Cosmological Transients | It has been shown that the observed temporal distribution of transient events
in the cosmos can be used to constrain their rate density. Here we show that
the peak flux--observation time relation takes the form of a power law that is
invariant to the luminosity distribution of the sources, and that the method
can be ... | astro-ph | it has been shown that the observed temporal distribution of transient events in the cosmos can be used to constrain their rate density here we show that the peak fluxobservation time relation takes the form of a power law that is invariant to the luminosity distribution of the sources and that the method can be greatl... | [['it', 'has', 'been', 'shown', 'that', 'the', 'observed', 'temporal', 'distribution', 'of', 'transient', 'events', 'in', 'the', 'cosmos', 'can', 'be', 'used', 'to', 'constrain', 'their', 'rate', 'density', 'here', 'we', 'show', 'that', 'the', 'peak', 'fluxobservation', 'time', 'relation', 'takes', 'the', 'form', 'of',... | [-0.060376102472303524, 0.11149158730641343, -0.1241407653988274, 0.12696651635870207, -0.07701792501367975, -0.07681996273526619, 0.059609517587760334, 0.4326898902681721, -0.21387622378181753, -0.3833043035959045, 0.0712145557509482, -0.2825726881599748, -0.06585541352911224, 0.24121370359843727, -0.01652337476167134... |
706.4137 | Propagation Constraints and Classical Solutions in K-essence Like
Theories | We consider two examples of solutions of the equations of motion of scalar
field theories with higher derivatives. These are the cosmology of the rolling
tachyon and static spherically symmetric solutions of the scalar field in flat
space. By requiring that the field equations always be hyperbolic and that the
speed ... | hep-th | we consider two examples of solutions of the equations of motion of scalar field theories with higher derivatives these are the cosmology of the rolling tachyon and static spherically symmetric solutions of the scalar field in flat space by requiring that the field equations always be hyperbolic and that the speed of p... | [['we', 'consider', 'two', 'examples', 'of', 'solutions', 'of', 'the', 'equations', 'of', 'motion', 'of', 'scalar', 'field', 'theories', 'with', 'higher', 'derivatives', 'these', 'are', 'the', 'cosmology', 'of', 'the', 'rolling', 'tachyon', 'and', 'static', 'spherically', 'symmetric', 'solutions', 'of', 'the', 'scalar'... | [-0.15784806915165472, 0.16465811757049684, -0.08802085304191208, 0.06184865917753557, -0.07350125214855732, -0.12235955793795915, -0.05657931583033321, 0.3346563187331475, -0.2126260708439453, -0.27109353223349897, 0.10979404991797717, -0.2522240572127289, -0.11852038507510362, 0.15813996010170928, -0.0034301020349536... |
706.4138 | Guaranteed Minimum-Rank Solutions of Linear Matrix Equations via Nuclear
Norm Minimization | The affine rank minimization problem consists of finding a matrix of minimum
rank that satisfies a given system of linear equality constraints. Such
problems have appeared in the literature of a diverse set of fields including
system identification and control, Euclidean embedding, and collaborative
filtering. Althou... | math.OC math.ST stat.TH | the affine rank minimization problem consists of finding a matrix of minimum rank that satisfies a given system of linear equality constraints such problems have appeared in the literature of a diverse set of fields including system identification and control euclidean embedding and collaborative filtering although spe... | [['the', 'affine', 'rank', 'minimization', 'problem', 'consists', 'of', 'finding', 'a', 'matrix', 'of', 'minimum', 'rank', 'that', 'satisfies', 'a', 'given', 'system', 'of', 'linear', 'equality', 'constraints', 'such', 'problems', 'have', 'appeared', 'in', 'the', 'literature', 'of', 'a', 'diverse', 'set', 'of', 'fields... | [-0.11598197966929019, 0.03500199447857377, -0.051417906497163914, 0.06903617016404844, -0.09723191993759463, -0.18048860977208356, 0.00985457380999305, 0.34428939006412057, -0.36719312287154204, -0.2638643935127299, 0.156569660609634, -0.24231950468153773, -0.19275979254751202, 0.15066152475314376, -0.1269373478408167... |
706.4139 | Short Gamma-Ray Bursts and Binary Mergers in Spiral and Elliptical
Galaxies: Redshift Distribution and Hosts | To test whether the short GRB rates, redshift distribution and host galaxies
are consistent with current theoretical predictions, we use avery large
database of population synthesis calculations to examine BH-NS and NS-NS merger
rates in the universe, factoring in (i) the star formation history of the
universe, (ii) ... | astro-ph | to test whether the short grb rates redshift distribution and host galaxies are consistent with current theoretical predictions we use avery large database of population synthesis calculations to examine bhns and nsns merger rates in the universe factoring in i the star formation history of the universe ii a heterogene... | [['to', 'test', 'whether', 'the', 'short', 'grb', 'rates', 'redshift', 'distribution', 'and', 'host', 'galaxies', 'are', 'consistent', 'with', 'current', 'theoretical', 'predictions', 'we', 'use', 'avery', 'large', 'database', 'of', 'population', 'synthesis', 'calculations', 'to', 'examine', 'bhns', 'and', 'nsns', 'mer... | [-0.0797991065112556, 0.1304440682255532, -0.0178726252024242, 0.18401350364477997, -0.12252946125367287, -0.09867841222727425, 0.057463311297579645, 0.44355262429958364, -0.1030955006855626, -0.3051068321446398, 0.04811016668333676, -0.29368701865185937, -0.003654158698316817, 0.24161123474928958, -0.00880501410958174... |
706.414 | Improbability of DUrca process constraints EOS | According to recent observational and theoretical progresses, the DUrca
process (direct Urca process) may be excluded from the category of neutron star
cooling mechanisms. This result combined with the latest nuclear symmetry
energy experiments, will provide us an independent way of testing the EOS
(equation of state... | astro-ph | according to recent observational and theoretical progresses the durca process direct urca process may be excluded from the category of neutron star cooling mechanisms this result combined with the latest nuclear symmetry energy experiments will provide us an independent way of testing the eos equation of state for sup... | [['according', 'to', 'recent', 'observational', 'and', 'theoretical', 'progresses', 'the', 'durca', 'process', 'direct', 'urca', 'process', 'may', 'be', 'excluded', 'from', 'the', 'category', 'of', 'neutron', 'star', 'cooling', 'mechanisms', 'this', 'result', 'combined', 'with', 'the', 'latest', 'nuclear', 'symmetry', ... | [-0.032701356260136503, 0.18448730313326958, -0.1421510025927583, 0.073629064959024, -0.15844065702108087, -0.08476022740856545, 0.10333462131255475, 0.33450772955280833, -0.2329607628682842, -0.3300950824221993, 0.09840741031421502, -0.23671046650556268, 0.0208593203273953, 0.21225804529061204, 0.006307900159001412, 0... |
706.4141 | Quark-Lepton Symmetry and Quartification in Five Dimensions | We outline some features of higher dimensional models possessing a
Quark-Lepton (QL) symmetry. The QL symmetric model in five dimensions is
discussed, with particular emphasis on the use of split fermions. An
interesting fermionic geography which utilises the QL symmetry to suppress the
proton decay rate and to motiv... | hep-ph | we outline some features of higher dimensional models possessing a quarklepton ql symmetry the ql symmetric model in five dimensions is discussed with particular emphasis on the use of split fermions an interesting fermionic geography which utilises the ql symmetry to suppress the proton decay rate and to motivate the ... | [['we', 'outline', 'some', 'features', 'of', 'higher', 'dimensional', 'models', 'possessing', 'a', 'quarklepton', 'ql', 'symmetry', 'the', 'ql', 'symmetric', 'model', 'in', 'five', 'dimensions', 'is', 'discussed', 'with', 'particular', 'emphasis', 'on', 'the', 'use', 'of', 'split', 'fermions', 'an', 'interesting', 'fer... | [-0.08509868027176708, 0.16972872596979868, -0.02114352017524652, 0.11498497692664386, -0.062333443250099665, -0.18156874564811004, -0.006578150670975447, 0.3303521626163274, -0.19513773900689557, -0.2604558636667207, 0.0722768315274152, -0.2844689489924349, -0.11981477280496619, 0.08769195630156901, 0.0142929864814504... |
706.4142 | Unified model of baryonic matter and dark components | We investigate an interacting two-fluid cosmological model and introduce a
scalar field representation by means of a linear combination of the individual
energy densities. Applying the integrability condition to the scalar field
equation we show that this "exotic quintessence" is driven by an exponential
potential an... | astro-ph hep-ph | we investigate an interacting twofluid cosmological model and introduce a scalar field representation by means of a linear combination of the individual energy densities applying the integrability condition to the scalar field equation we show that this exotic quintessence is driven by an exponential potential and the ... | [['we', 'investigate', 'an', 'interacting', 'twofluid', 'cosmological', 'model', 'and', 'introduce', 'a', 'scalar', 'field', 'representation', 'by', 'means', 'of', 'a', 'linear', 'combination', 'of', 'the', 'individual', 'energy', 'densities', 'applying', 'the', 'integrability', 'condition', 'to', 'the', 'scalar', 'fie... | [-0.12002713772926654, 0.1568398173680584, -0.12186935012707384, 0.07647505204497268, -0.07193305255431268, -0.09273370076294264, -0.020001399044607144, 0.3235629661746013, -0.23762972301079166, -0.344820776139386, 0.04616548846145937, -0.24162210613333931, -0.05711910388264288, 0.10682715710896042, 0.05098944957393946... |
706.4143 | Macroscopic non-equilibrium thermodynamics in dynamic calorimetry | What is really measured in dynamic calorimetric experiments is still an open
question. This paper is devoted to this question, which can be usefully
envisaged by means of macroscopic non-equilibrium thermodynamics. From the
pioneer work of De Donder on chemical reactions and with other authors along
the 20th century,... | cond-mat.soft | what is really measured in dynamic calorimetric experiments is still an open question this paper is devoted to this question which can be usefully envisaged by means of macroscopic nonequilibrium thermodynamics from the pioneer work of de donder on chemical reactions and with other authors along the 20th century the qu... | [['what', 'is', 'really', 'measured', 'in', 'dynamic', 'calorimetric', 'experiments', 'is', 'still', 'an', 'open', 'question', 'this', 'paper', 'is', 'devoted', 'to', 'this', 'question', 'which', 'can', 'be', 'usefully', 'envisaged', 'by', 'means', 'of', 'macroscopic', 'nonequilibrium', 'thermodynamics', 'from', 'the',... | [-0.06997967789714478, 0.1448277621115139, -0.10005015494269237, 0.05590504279417362, -0.08704083799302839, -0.11431014649324904, 0.056924936494365204, 0.3199269173589225, -0.2932040083360973, -0.2966284260905364, 0.08058070194327452, -0.286616221023315, -0.14109931206698284, 0.236498225627369, -0.11092847089789677, 0.... |
706.4144 | The Borel conjecture for manifolds with virtually solvable fundamental
groups | The article has been withdrawn by the author. Wolfgang Lueck and Peter
Linnell pointed out that the proof of Lemma 3.8 does not apply to the
unrestricted case of wreath product. It is not clear at this stage how to
complete the proof of Theorem 3.1 using the present version of Lemma 3.8. The
valid results originating... | math.GT math.KT | the article has been withdrawn by the author wolfgang lueck and peter linnell pointed out that the proof of lemma 38 does not apply to the unrestricted case of wreath product it is not clear at this stage how to complete the proof of theorem 31 using the present version of lemma 38 the valid results originating from th... | [['the', 'article', 'has', 'been', 'withdrawn', 'by', 'the', 'author', 'wolfgang', 'lueck', 'and', 'peter', 'linnell', 'pointed', 'out', 'that', 'the', 'proof', 'of', 'lemma', '38', 'does', 'not', 'apply', 'to', 'the', 'unrestricted', 'case', 'of', 'wreath', 'product', 'it', 'is', 'not', 'clear', 'at', 'this', 'stage',... | [-0.05699785066240314, 0.03813863408737885, -0.16727061408446797, 0.04511859909276853, -0.10889661492807652, -0.10945787655412038, 0.08536056156527362, 0.2558599273993898, -0.23178363701549304, -0.28829294499426855, 0.1472545536982118, -0.24405834426992198, -0.13843083933496209, 0.1771075421416048, -0.16686335735634636... |
706.4145 | Ordered spin-ice state in the geometrically frustrated
metallic-ferromagnet Sm2Mo2O7 | The recent discovery of Spin-ice is a spectacular example of non-coplanar
spin arrangements that can arise in the pyrochlore A2B2O7 structure. We present
magnetic and thermodynamic studies on the metallic-ferromagnet pyrochlore
Sm2Mo2O7. Our studies, carried out on oriented crystals, suggest that the Sm
spins have an... | cond-mat.str-el cond-mat.mtrl-sci | the recent discovery of spinice is a spectacular example of noncoplanar spin arrangements that can arise in the pyrochlore a2b2o7 structure we present magnetic and thermodynamic studies on the metallicferromagnet pyrochlore sm2mo2o7 our studies carried out on oriented crystals suggest that the sm spins have an ordered ... | [['the', 'recent', 'discovery', 'of', 'spinice', 'is', 'a', 'spectacular', 'example', 'of', 'noncoplanar', 'spin', 'arrangements', 'that', 'can', 'arise', 'in', 'the', 'pyrochlore', 'a2b2o7', 'structure', 'we', 'present', 'magnetic', 'and', 'thermodynamic', 'studies', 'on', 'the', 'metallicferromagnet', 'pyrochlore', '... | [-0.19529479310510617, 0.24357057840724933, 0.011519208209235864, 0.006337838817452048, -0.06590155292109683, -0.11145187620924593, 0.048460029200088746, 0.37193506988215036, -0.23073098716398316, -0.2722018323763442, 0.049822502928095515, -0.32442695528654186, -0.10672698770489158, 0.1289316131171353, 0.07995820813812... |
706.4146 | X-Ray Spectroscopy of SN 1006 with Suzaku | We report on observations of SN 1006 with the X-ray Imaging Spectrometers
(XIS) on board Suzaku. We firmly detected K-shell emission from Fe, for the
first time, and find that the Fe ionization state is quite low. The broad band
spectrum extracted from the southeast of the remnant is well fitted with a
model consisti... | astro-ph | we report on observations of sn 1006 with the xray imaging spectrometers xis on board suzaku we firmly detected kshell emission from fe for the first time and find that the fe ionization state is quite low the broad band spectrum extracted from the southeast of the remnant is well fitted with a model consisting of thre... | [['we', 'report', 'on', 'observations', 'of', 'sn', '1006', 'with', 'the', 'xray', 'imaging', 'spectrometers', 'xis', 'on', 'board', 'suzaku', 'we', 'firmly', 'detected', 'kshell', 'emission', 'from', 'fe', 'for', 'the', 'first', 'time', 'and', 'find', 'that', 'the', 'fe', 'ionization', 'state', 'is', 'quite', 'low', '... | [-0.03070030101071486, 0.19459453316477054, -0.023634473122576743, 0.055411507329768225, -0.02321403982509803, -0.11483852943389589, 0.021426103571350247, 0.42620397226996404, -0.19316867804035354, -0.3427551281822519, 0.03748960569839224, -0.34859830557774657, 0.052958089120747745, 0.1863991394529565, 0.04897072155856... |
706.4147 | Established pseudo solution of second-order Dirac-Coulomb equation with
position-dependent mass | We show that one of exact solutions of the second-order Dirac-Coulomb
equation were pseudo. In the corresponding original literature, it was
considered that the mass of the electron with a Coulomb potential was
position-dependent, but the obtained eigenvalues set was not the inevitable
mathematical deduction of the g... | physics.gen-ph | we show that one of exact solutions of the secondorder diraccoulomb equation were pseudo in the corresponding original literature it was considered that the mass of the electron with a coulomb potential was positiondependent but the obtained eigenvalues set was not the inevitable mathematical deduction of the given sec... | [['we', 'show', 'that', 'one', 'of', 'exact', 'solutions', 'of', 'the', 'secondorder', 'diraccoulomb', 'equation', 'were', 'pseudo', 'in', 'the', 'corresponding', 'original', 'literature', 'it', 'was', 'considered', 'that', 'the', 'mass', 'of', 'the', 'electron', 'with', 'a', 'coulomb', 'potential', 'was', 'positiondep... | [-0.11947351121305813, 0.093791913645289, -0.08749858193038924, 0.09685158605850112, -0.10849451152153494, -0.14036653086739947, -0.010007214112532878, 0.2753568362384065, -0.23410730917249026, -0.2969785825144954, 0.04535233218514368, -0.30358530490893904, -0.1536771745905583, 0.14251489266450326, -0.02894588169164774... |
706.4148 | Free energy density for mean field perturbation of states of a
one-dimensional spin chain | Motivated by recent developments on large deviations in states of the spin
chain, we reconsider the work of Petz, Raggio and Verbeure in 1989 on the
variational expression of free energy density in the presence of a mean field
type perturbation. We extend their results from the product state case to the
Gibbs state c... | math-ph math.MP | motivated by recent developments on large deviations in states of the spin chain we reconsider the work of petz raggio and verbeure in 1989 on the variational expression of free energy density in the presence of a mean field type perturbation we extend their results from the product state case to the gibbs state case i... | [['motivated', 'by', 'recent', 'developments', 'on', 'large', 'deviations', 'in', 'states', 'of', 'the', 'spin', 'chain', 'we', 'reconsider', 'the', 'work', 'of', 'petz', 'raggio', 'and', 'verbeure', 'in', '1989', 'on', 'the', 'variational', 'expression', 'of', 'free', 'energy', 'density', 'in', 'the', 'presence', 'of'... | [-0.1284160849845244, 0.17070494666178193, -0.05480100033714229, 0.06228035500066148, 0.0037788605731394554, -0.05321650388133195, 0.060218829793545106, 0.32877849503937695, -0.2591243832320389, -0.25738278563237854, 0.06638605525173867, -0.26692972788845915, -0.08492827561632213, 0.16881246661456922, -0.04298020270135... |
706.4149 | Integrating cavity quantum electrodynamics and ultracold-atom chips with
on-chip dielectric mirrors and temperature stabilization | We have fabricated an atom chip device which combines the circuitry for
magnetic trapping of cold atoms with high-finesse optical resonators suitable
for cavity QED in the single-atom strong coupling regime. Fabry-Perot optical
resonators with finesse F > 2 X 10^5 were formed between a micropatterned
on-chip planar m... | quant-ph | we have fabricated an atom chip device which combines the circuitry for magnetic trapping of cold atoms with highfinesse optical resonators suitable for cavity qed in the singleatom strong coupling regime fabryperot optical resonators with finesse f 2 x 105 were formed between a micropatterned onchip planar mirror with... | [['we', 'have', 'fabricated', 'an', 'atom', 'chip', 'device', 'which', 'combines', 'the', 'circuitry', 'for', 'magnetic', 'trapping', 'of', 'cold', 'atoms', 'with', 'highfinesse', 'optical', 'resonators', 'suitable', 'for', 'cavity', 'qed', 'in', 'the', 'singleatom', 'strong', 'coupling', 'regime', 'fabryperot', 'optic... | [-0.16805317315125937, 0.23472346872915392, 0.07246563542438181, -0.14918476595592342, 0.0134454364986404, -0.2947873156223642, 0.04022426404500086, 0.529905845538566, -0.1955449839759814, -0.3552213580323089, -0.007889324359252657, -0.2637086598839807, -0.02144352168236908, 0.2611652921199014, -0.011175485690565486, 0... |
706.415 | Energy gap measurement of nanostructured thin aluminium films for use in
single Cooper-pair devices | Within the context of superconducting gap engineering, Al-\alox-Al tunnel
junctions have been used to study the variation in superconducting gap,
$\Delta$, with film thickness. Films of thickness 5, 7, 10 and 30 nm were used
to form the small area superconductor-insulator-superconductor (SIS) tunnel
junctions. In agr... | cond-mat.supr-con cond-mat.mes-hall | within the context of superconducting gap engineering alaloxal tunnel junctions have been used to study the variation in superconducting gap delta with film thickness films of thickness 5 7 10 and 30 nm were used to form the small area superconductorinsulatorsuperconductor sis tunnel junctions in agreement with previou... | [['within', 'the', 'context', 'of', 'superconducting', 'gap', 'engineering', 'alaloxal', 'tunnel', 'junctions', 'have', 'been', 'used', 'to', 'study', 'the', 'variation', 'in', 'superconducting', 'gap', 'delta', 'with', 'film', 'thickness', 'films', 'of', 'thickness', '5', '7', '10', 'and', '30', 'nm', 'were', 'used', ... | [-0.1389995959595355, 0.14392692922292633, 0.013120215601072861, -0.017122000864802454, 0.025033127544368178, -0.14973387509011304, 0.08575954078298667, 0.45795465388104445, -0.2077895251349506, -0.4522249411918923, -0.005895963839143833, -0.33799456272465295, -0.019656190378034216, 0.18624564749387723, -0.018991175963... |
706.4151 | Directed percolation criticality in turbulent liquid crystals | We experimentally investigate the critical behavior of a phase transition
between two topologically different turbulent states of electrohydrodynamic
convection in nematic liquid crystals. The statistical properties of the
observed spatiotemporal intermittency regimes are carefully determined,
yielding a complete set... | cond-mat.stat-mech | we experimentally investigate the critical behavior of a phase transition between two topologically different turbulent states of electrohydrodynamic convection in nematic liquid crystals the statistical properties of the observed spatiotemporal intermittency regimes are carefully determined yielding a complete set of ... | [['we', 'experimentally', 'investigate', 'the', 'critical', 'behavior', 'of', 'a', 'phase', 'transition', 'between', 'two', 'topologically', 'different', 'turbulent', 'states', 'of', 'electrohydrodynamic', 'convection', 'in', 'nematic', 'liquid', 'crystals', 'the', 'statistical', 'properties', 'of', 'the', 'observed', ... | [-0.1758091453658907, 0.22777130357529754, -0.06266308327260624, 0.04624766338996491, -0.0008686831049425038, -0.11446646074029176, 0.06685741993255521, 0.34350032050095153, -0.21207358315855104, -0.25393664488863005, 0.009689446220076397, -0.2809196360850413, -0.1608075440775505, 0.12404396457867206, 0.050022547182283... |
706.4152 | Scaling of hysteresis loops at phase transitions into a quasiabsorbing
state | Models undergoing a phase transition to an absorbing state weakly broken by
the addition of a very low spontaneous nucleation rate are shown to exhibit
hysteresis loops whose width $\Delta\lambda$ depends algebraically on the ramp
rate $r$. Analytical arguments and numerical simulations show that
$\Delta\lambda \sim ... | cond-mat.stat-mech | models undergoing a phase transition to an absorbing state weakly broken by the addition of a very low spontaneous nucleation rate are shown to exhibit hysteresis loops whose width deltalambda depends algebraically on the ramp rate r analytical arguments and numerical simulations show that deltalambda sim rkappa with k... | [['models', 'undergoing', 'a', 'phase', 'transition', 'to', 'an', 'absorbing', 'state', 'weakly', 'broken', 'by', 'the', 'addition', 'of', 'a', 'very', 'low', 'spontaneous', 'nucleation', 'rate', 'are', 'shown', 'to', 'exhibit', 'hysteresis', 'loops', 'whose', 'width', 'deltalambda', 'depends', 'algebraically', 'on', '... | [-0.16150779890077602, 0.2395384995591788, -0.06969904478949805, 0.04444692520450594, -0.013143546528105314, -0.19389187917889406, 0.09072336417545254, 0.37560872220330765, -0.2437294151220057, -0.2598107407800853, 0.08333508999138657, -0.2664424140471965, -0.14169556429195734, 0.21829902106999524, 0.024714790657162665... |
706.4153 | Non-perturbative renormalization of static-light four-fermion operators
in quenched lattice QCD | We perform a non-perturbative study of the scale-dependent renormalization
factors of a multiplicatively renormalizable basis of $\Delta{B}=2$ parity-odd
four-fermion operators in quenched lattice QCD. Heavy quarks are treated in the
static approximation with various lattice discretizations of the static action.
Ligh... | hep-lat hep-ph | we perform a nonperturbative study of the scaledependent renormalization factors of a multiplicatively renormalizable basis of deltab2 parityodd fourfermion operators in quenched lattice qcd heavy quarks are treated in the static approximation with various lattice discretizations of the static action light quarks are d... | [['we', 'perform', 'a', 'nonperturbative', 'study', 'of', 'the', 'scaledependent', 'renormalization', 'factors', 'of', 'a', 'multiplicatively', 'renormalizable', 'basis', 'of', 'deltab2', 'parityodd', 'fourfermion', 'operators', 'in', 'quenched', 'lattice', 'qcd', 'heavy', 'quarks', 'are', 'treated', 'in', 'the', 'stat... | [-0.15169265922649125, 0.22634413793862782, -0.1236272254517596, 0.14166409523622542, -0.008358340495952257, -0.08924405410755099, 0.07998889628613956, 0.40525474523504573, -0.19592689034904828, -0.20544223527407698, 0.033553050242756545, -0.2976038171011105, -0.07626116604609579, 0.08782334866721117, 0.054789815812878... |
706.4154 | A Formation Mechanism of Collapsar Black Hole -- early evolution phase | The latest studies of massive star evolution indicate that an initially
rapidly rotating star with sufficiently low metallicity can produce a rapidly
rotating, massive stellar core that could be a progenitor of long-soft
gamma-ray bursts (LGRBs). Motivated by these studies, we follow the collapse of
a rapidly rotatin... | astro-ph | the latest studies of massive star evolution indicate that an initially rapidly rotating star with sufficiently low metallicity can produce a rapidly rotating massive stellar core that could be a progenitor of longsoft gammaray bursts lgrbs motivated by these studies we follow the collapse of a rapidly rotating massive... | [['the', 'latest', 'studies', 'of', 'massive', 'star', 'evolution', 'indicate', 'that', 'an', 'initially', 'rapidly', 'rotating', 'star', 'with', 'sufficiently', 'low', 'metallicity', 'can', 'produce', 'a', 'rapidly', 'rotating', 'massive', 'stellar', 'core', 'that', 'could', 'be', 'a', 'progenitor', 'of', 'longsoft', ... | [-0.15256500257114272, 0.17584914449130043, -0.04050656916128833, 0.12274054348015861, -0.09301590724889912, -0.06962326033022348, 0.017613803428037103, 0.37638904868778006, -0.186431184360081, -0.2827327503262097, 0.08484445814685015, -0.24881342699315714, -0.008211545073960106, 0.20629457525436334, 0.0260000202345223... |
706.4155 | Phonon-assisted decoherence in the production of polarization-entangled
photons in a single semiconductor quantum dot | We theoretically investigate the production of polarization-entangled photons
through the biexciton cascade decay in a single semiconductor quantum dot. In
the intermediate state the entanglement is encoded in the polarizations of the
first emitted photon and the exciton, where the exciton state can be
effectively ``... | cond-mat.mes-hall | we theoretically investigate the production of polarizationentangled photons through the biexciton cascade decay in a single semiconductor quantum dot in the intermediate state the entanglement is encoded in the polarizations of the first emitted photon and the exciton where the exciton state can be effectively measure... | [['we', 'theoretically', 'investigate', 'the', 'production', 'of', 'polarizationentangled', 'photons', 'through', 'the', 'biexciton', 'cascade', 'decay', 'in', 'a', 'single', 'semiconductor', 'quantum', 'dot', 'in', 'the', 'intermediate', 'state', 'the', 'entanglement', 'is', 'encoded', 'in', 'the', 'polarizations', 'o... | [-0.1401904901638435, 0.2598541592843063, -0.057923269443713205, 0.038591310185963554, 0.02375817114064835, -0.14119599291037038, 0.07143202276910011, 0.39016454918406057, -0.30598533819861634, -0.24046097442354122, 0.0021282958440463416, -0.31593756798232336, -0.05466467985096052, 0.18221857296975003, 0.03948615558599... |
706.4156 | Glitches in Anomalous X-ray Pulsars | (Abridged) We report on 8.7 and 7.6 yr of RXTE observations of the Anomalous
X-ray Pulsars (AXPs) RXS J170849.0-400910 and 1E 1841-045, respectively. These
observations, part of a larger RXTE AXP monitoring program, have allowed us to
study the long-term timing, pulsed flux, and pulse profile evolution of these
objec... | astro-ph | abridged we report on 87 and 76 yr of rxte observations of the anomalous xray pulsars axps rxs j1708490400910 and 1e 1841045 respectively these observations part of a larger rxte axp monitoring program have allowed us to study the longterm timing pulsed flux and pulse profile evolution of these objects we report on fou... | [['abridged', 'we', 'report', 'on', '87', 'and', '76', 'yr', 'of', 'rxte', 'observations', 'of', 'the', 'anomalous', 'xray', 'pulsars', 'axps', 'rxs', 'j1708490400910', 'and', '1e', '1841045', 'respectively', 'these', 'observations', 'part', 'of', 'a', 'larger', 'rxte', 'axp', 'monitoring', 'program', 'have', 'allowed'... | [-0.13598097942200293, 0.17591061916172684, -0.027859702571641134, 0.16168174053458628, -0.16314952537662672, -0.08075957277912342, 0.060284318194436276, 0.4359649521964884, -0.19359266415140608, -0.37708884861413056, 0.14614805475364562, -0.32103211390769304, -0.08929012606858386, 0.29154916783070584, -0.0823505474602... |
706.4157 | Adaptive dynamics in logistic branching populations | We consider a trait-structured population subject to mutation, birth and
competition of logistic type, where the number of coexisting types may
fluctuate. Applying a limit of rare mutations to this population while keeping
the population size finite leads to a jump process, the so-called `trait
substitution sequence'... | math.PR | we consider a traitstructured population subject to mutation birth and competition of logistic type where the number of coexisting types may fluctuate applying a limit of rare mutations to this population while keeping the population size finite leads to a jump process the socalled trait substitution sequence where evo... | [['we', 'consider', 'a', 'traitstructured', 'population', 'subject', 'to', 'mutation', 'birth', 'and', 'competition', 'of', 'logistic', 'type', 'where', 'the', 'number', 'of', 'coexisting', 'types', 'may', 'fluctuate', 'applying', 'a', 'limit', 'of', 'rare', 'mutations', 'to', 'this', 'population', 'while', 'keeping', ... | [-0.10794038767198799, 0.13570309121433866, -0.06023023516172543, 0.09206418267721261, -0.041289780330771464, -0.14912560555421805, 0.10214013769154917, 0.3444048083401867, -0.3012379889933072, -0.2340544402723026, 0.06135587712196866, -0.21576898480088857, -0.17583715237469733, 0.11536841332576842, -0.0940805235177322... |
706.4158 | Decay estimates of a tangential derivative to the light cone for the
wave equation and their application | We consider wave equations in three space dimensions, and obtain new weighted
$L^\infty$-$L^\infty$ estimates for a tangential derivative to the light cone.
As an application, we give a new proof of the global existence theorem, which
was originally proved by Klainerman and Christodoulou, for systems of nonlinear
wav... | math.AP | we consider wave equations in three space dimensions and obtain new weighted linftylinfty estimates for a tangential derivative to the light cone as an application we give a new proof of the global existence theorem which was originally proved by klainerman and christodoulou for systems of nonlinear wave equations unde... | [['we', 'consider', 'wave', 'equations', 'in', 'three', 'space', 'dimensions', 'and', 'obtain', 'new', 'weighted', 'linftylinfty', 'estimates', 'for', 'a', 'tangential', 'derivative', 'to', 'the', 'light', 'cone', 'as', 'an', 'application', 'we', 'give', 'a', 'new', 'proof', 'of', 'the', 'global', 'existence', 'theorem... | [-0.14843666904797667, 0.04907102495460148, -0.1300212151477086, 0.07973452034639195, -0.12524590721038883, -0.09676717432654079, 0.0029986044255030505, 0.23956512131125612, -0.2225202919833143, -0.2378680826000431, 0.15668552216683404, -0.2264817294472938, -0.15828060775118716, 0.23107933926889124, -0.0597739257329307... |
706.4159 | Multimode analysis of the light emitted from a pulsed optical parametric
oscillator | We present a multimode treatment of the optical parametric oscillator, which
is valid for both pulsed and continuous-wave pump fields. The two-time
correlation functions of the output field are derived, and we apply the theory
to analyze a scheme for heralded production of non-classical field states that
may be subse... | quant-ph | we present a multimode treatment of the optical parametric oscillator which is valid for both pulsed and continuouswave pump fields the twotime correlation functions of the output field are derived and we apply the theory to analyze a scheme for heralded production of nonclassical field states that may be subsequently ... | [['we', 'present', 'a', 'multimode', 'treatment', 'of', 'the', 'optical', 'parametric', 'oscillator', 'which', 'is', 'valid', 'for', 'both', 'pulsed', 'and', 'continuouswave', 'pump', 'fields', 'the', 'twotime', 'correlation', 'functions', 'of', 'the', 'output', 'field', 'are', 'derived', 'and', 'we', 'apply', 'the', '... | [-0.13622725251480006, 0.2039759194618195, -0.09985087820262249, 0.06498207567866691, 0.01009794557467103, -0.1697490942481506, 0.05232598278131003, 0.43235323548183907, -0.2332945073430892, -0.20897849693262419, 0.035135001366143115, -0.20188760210294276, -0.07274314453492739, 0.2796923182572105, 0.002607927907125226,... |
706.416 | Explicit formulas for biharmonic submanifolds in Sasakian space forms | We classify the biharmonic Legendre curves in a Sasakian space form, and
obtain their explicit parametric equations in the $(2n+1)$-dimensional unit
sphere endowed with the canonical and deformed Sasakian structures defined by
Tanno. Then, composing with the flow of the Reeb vector field, we transform a
biharmonic in... | math.DG | we classify the biharmonic legendre curves in a sasakian space form and obtain their explicit parametric equations in the 2n1dimensional unit sphere endowed with the canonical and deformed sasakian structures defined by tanno then composing with the flow of the reeb vector field we transform a biharmonic integral subma... | [['we', 'classify', 'the', 'biharmonic', 'legendre', 'curves', 'in', 'a', 'sasakian', 'space', 'form', 'and', 'obtain', 'their', 'explicit', 'parametric', 'equations', 'in', 'the', '2n1dimensional', 'unit', 'sphere', 'endowed', 'with', 'the', 'canonical', 'and', 'deformed', 'sasakian', 'structures', 'defined', 'by', 't... | [-0.22029439988218144, 0.03712646611375918, -0.046297743916511536, 0.07881309804801738, -0.15035612168918613, -0.1164817914537246, -0.08481697603063264, 0.412214461215575, -0.2633734187635947, -0.1748176499886412, 0.055794780590230415, -0.28894323380139303, -0.21293596760697767, 0.18559799415492256, -0.1432033125704652... |
706.4161 | The Domino Problem of the Hyperbolic Plane Is Undecidable | In this paper, we prove that the general tiling problem of the hyperbolic
plane is undecidable by proving a slightly stronger version using only a
regular polygon as the basic shape of the tiles. The problem was raised by a
paper of Raphael Robinson in 1971, in his famous simplified proof that the
general tiling prob... | cs.CG cs.DM | in this paper we prove that the general tiling problem of the hyperbolic plane is undecidable by proving a slightly stronger version using only a regular polygon as the basic shape of the tiles the problem was raised by a paper of raphael robinson in 1971 in his famous simplified proof that the general tiling problem i... | [['in', 'this', 'paper', 'we', 'prove', 'that', 'the', 'general', 'tiling', 'problem', 'of', 'the', 'hyperbolic', 'plane', 'is', 'undecidable', 'by', 'proving', 'a', 'slightly', 'stronger', 'version', 'using', 'only', 'a', 'regular', 'polygon', 'as', 'the', 'basic', 'shape', 'of', 'the', 'tiles', 'the', 'problem', 'was... | [-0.10489647093134513, 0.06121952109295281, -0.05669584781255411, 0.10723329676598635, -0.11331951658686866, -0.15055606111317224, 0.038954700873084905, 0.2522714990798546, -0.28724413240949315, -0.264111986707734, 0.1424253189166927, -0.2398369440039539, -0.20677041758418732, 0.17674525419547074, -0.2203391083124755, ... |
706.4162 | The entanglement of the XY spin chain in a random magnetic field | We investigate the entanglement of the ferromagnetic XY model in a random
magnetic field at zero temperature and in the uniform magnetic field at finite
temperatures. We use the concurrence to quantify the entanglement. We find
that, in the ferromagnetic region of the uniform magnetic field $h$, all the
concurrences ... | quant-ph cond-mat.dis-nn cond-mat.stat-mech | we investigate the entanglement of the ferromagnetic xy model in a random magnetic field at zero temperature and in the uniform magnetic field at finite temperatures we use the concurrence to quantify the entanglement we find that in the ferromagnetic region of the uniform magnetic field h all the concurrences are text... | [['we', 'investigate', 'the', 'entanglement', 'of', 'the', 'ferromagnetic', 'xy', 'model', 'in', 'a', 'random', 'magnetic', 'field', 'at', 'zero', 'temperature', 'and', 'in', 'the', 'uniform', 'magnetic', 'field', 'at', 'finite', 'temperatures', 'we', 'use', 'the', 'concurrence', 'to', 'quantify', 'the', 'entanglement'... | [-0.16159387523708701, 0.24902431013291343, -0.04211785603036875, 0.05092611548433636, 0.0072945475521121635, -0.09533173572925623, 0.0476647823213665, 0.3949060456729249, -0.25889718857708205, -0.2466027154832294, 0.04465093805042112, -0.273846727665187, -0.05729849502779217, 0.1468706157164681, 0.044207811971877196, ... |
706.4163 | Variational Principles for Constrained Electromagnetic Field and
Papapetrou Equation | In our previous article [4] an approach to derive Papapetrou equations for
constrained electromagnetic field was demonstrated by use of field variational
principles. The aim of current work is to present more universal technique of
deduction of the equations which could be applied to another types of
non-scalar field... | gr-qc | in our previous article 4 an approach to derive papapetrou equations for constrained electromagnetic field was demonstrated by use of field variational principles the aim of current work is to present more universal technique of deduction of the equations which could be applied to another types of nonscalar fields it i... | [['in', 'our', 'previous', 'article', '4', 'an', 'approach', 'to', 'derive', 'papapetrou', 'equations', 'for', 'constrained', 'electromagnetic', 'field', 'was', 'demonstrated', 'by', 'use', 'of', 'field', 'variational', 'principles', 'the', 'aim', 'of', 'current', 'work', 'is', 'to', 'present', 'more', 'universal', 'te... | [-0.1303162708291379, 0.05665912847958363, -0.10653152262751499, 0.0303426746390355, -0.14542473092999147, -0.09812948859256247, -0.018689221910039043, 0.28441573485084204, -0.26571104941363244, -0.29935109699549883, 0.039316597991906434, -0.21803665859434937, -0.1584397031277742, 0.19983927875190324, -0.04308360746616... |
706.4164 | Harmonic analysis of additive Levy processes | Let $X_1,...,X_N$ denote $N$ independent $d$-dimensional L\'evy processes,
and consider the $N$-parameter random field \[\X(\bm{t}):=
X_1(t_1)+...+X_N(t_N).\] First we demonstrate that for all nonrandom Borel sets
$F\subseteq\R^d$, the Minkowski sum $\X(\R^N_+)\oplus F$, of the range
$\X(\R^N_+)$ of $\X$ with $F$, ca... | math.PR | let x_1x_n denote n independent ddimensional levy processes and consider the nparameter random field xbmt x_1t_1x_nt_n first we demonstrate that for all nonrandom borel sets fsubseteqrd the minkowski sum xrn_oplus f of the range xrn_ of x with f can have positive ddimensional lebesgue measure if and only if a certain c... | [['let', 'x_1x_n', 'denote', 'n', 'independent', 'ddimensional', 'levy', 'processes', 'and', 'consider', 'the', 'nparameter', 'random', 'field', 'xbmt', 'x_1t_1x_nt_n', 'first', 'we', 'demonstrate', 'that', 'for', 'all', 'nonrandom', 'borel', 'sets', 'fsubseteqrd', 'the', 'minkowski', 'sum', 'xrn_oplus', 'f', 'of', 'th... | [-0.13719936817767142, 0.1580444053775197, -0.07847283634122547, 0.009880416929714723, -0.04989922971763285, -0.1190791170802394, 0.037261365235690735, 0.3312917310275308, -0.24055774293072124, -0.21744869323447347, 0.09854929596772204, -0.2273661946337528, -0.17175233587693736, 0.1902928443853068, -0.11403622628964541... |
706.4165 | Probing new physics in the Neutrinoless double beta decay using electron
angular correlation | The angular correlation of the electrons emitted in the neutrinoless double
beta decay ($0\nu2\beta$) is presented using a general Lorentz invariant
effective Lagrangian for the leptonic and hadronic charged weak currents. We
show that the coefficient $K$ in the angular correlation $d\Gamma/d\cos \theta
\propto (1-K\... | hep-ph hep-ex nucl-th | the angular correlation of the electrons emitted in the neutrinoless double beta decay 0nu2beta is presented using a general lorentz invariant effective lagrangian for the leptonic and hadronic charged weak currents we show that the coefficient k in the angular correlation dgammadcos theta propto 1kcos theta is essenti... | [['the', 'angular', 'correlation', 'of', 'the', 'electrons', 'emitted', 'in', 'the', 'neutrinoless', 'double', 'beta', 'decay', '0nu2beta', 'is', 'presented', 'using', 'a', 'general', 'lorentz', 'invariant', 'effective', 'lagrangian', 'for', 'the', 'leptonic', 'and', 'hadronic', 'charged', 'weak', 'currents', 'we', 'sh... | [-0.07238262819078152, 0.26199297674997446, -0.03512639187696114, 0.14658055408131396, 0.011097586586931501, -0.13764472986776993, 0.06232151494934245, 0.3141647679687526, -0.21410189211989442, -0.26931270152470316, -0.023454677658439768, -0.3185361084165358, -0.007894123008063702, 0.1852899156576416, 0.112913643668007... |
706.4166 | WMAPping the Inflationary Universe | An epoch of accelerated expansion, or inflation, in the early universe solves
several cosmological problems. While there are many models of inflation only
recently has it become possible to discriminate between some of the models
using observations of the cosmic microwave background radiation and large-scale
structur... | hep-ph astro-ph | an epoch of accelerated expansion or inflation in the early universe solves several cosmological problems while there are many models of inflation only recently has it become possible to discriminate between some of the models using observations of the cosmic microwave background radiation and largescale structure in t... | [['an', 'epoch', 'of', 'accelerated', 'expansion', 'or', 'inflation', 'in', 'the', 'early', 'universe', 'solves', 'several', 'cosmological', 'problems', 'while', 'there', 'are', 'many', 'models', 'of', 'inflation', 'only', 'recently', 'has', 'it', 'become', 'possible', 'to', 'discriminate', 'between', 'some', 'of', 'th... | [-0.1123475211724225, 0.14509158164522282, -0.09710447583347559, 0.1211497415836978, -0.0919449352659285, -0.11016301877356859, -0.0667992427220775, 0.3636278881587916, -0.2490027195825759, -0.3215712128698619, 0.16070817124111475, -0.2526242570820614, -0.10367996297686154, 0.20620099656581362, 0.008588443756000035, 0.... |
706.4167 | Study of the decay mechanism for B+ to p pbar K+ and B+ to p pbar pi+ | We study the characteristics of the low mass ppbar enhancements near
threshold in the three-body decays B+ to p pbar K+ and B+ to p pbar pi+. We
observe that the proton polar angle distributions in the ppbar helicity frame
in the two decays have the opposite polarity, and measure the forward-backward
asymmetries as a... | hep-ex | we study the characteristics of the low mass ppbar enhancements near threshold in the threebody decays b to p pbar k and b to p pbar pi we observe that the proton polar angle distributions in the ppbar helicity frame in the two decays have the opposite polarity and measure the forwardbackward asymmetries as a function ... | [['we', 'study', 'the', 'characteristics', 'of', 'the', 'low', 'mass', 'ppbar', 'enhancements', 'near', 'threshold', 'in', 'the', 'threebody', 'decays', 'b', 'to', 'p', 'pbar', 'k', 'and', 'b', 'to', 'p', 'pbar', 'pi', 'we', 'observe', 'that', 'the', 'proton', 'polar', 'angle', 'distributions', 'in', 'the', 'ppbar', 'h... | [-0.11421983633654162, 0.20295293063324749, -0.07025429340433405, 0.08714000611543292, -0.028980619866567536, -0.12227821241443355, 0.11427046363223041, 0.29501509141722104, -0.18017451634736564, -0.279035366306884, -0.08927620081817807, -0.4608828383157166, 0.08145886836800634, 0.1377334254225943, 0.1052628161340225, ... |
706.4168 | Symmetry invariance, anticommutativity and nilpotency in BRST approach
to QED: superfield formalism | We provide the geometrical interpretation for the Becchi-Rouet-Stora-Tyutin
(BRST) and anti-BRST symmetry invariance of the Lagrangian density of a four (3
+ 1)-dimensional (4D) interacting U(1) gauge theory within the framework of
superfield approach to BRST formalism. This interacting theory, where there is
an expl... | hep-th | we provide the geometrical interpretation for the becchirouetstoratyutin brst and antibrst symmetry invariance of the lagrangian density of a four 3 1dimensional 4d interacting u1 gauge theory within the framework of superfield approach to brst formalism this interacting theory where there is an explicit coupling betwe... | [['we', 'provide', 'the', 'geometrical', 'interpretation', 'for', 'the', 'becchirouetstoratyutin', 'brst', 'and', 'antibrst', 'symmetry', 'invariance', 'of', 'the', 'lagrangian', 'density', 'of', 'a', 'four', '3', '1dimensional', '4d', 'interacting', 'u1', 'gauge', 'theory', 'within', 'the', 'framework', 'of', 'superfi... | [-0.20313921373491808, 0.21318968631040935, -0.05324569458593807, 0.07156189972708366, -0.0963094576011197, -0.14005301645047655, -0.039695111347208094, 0.328785548769158, -0.2244498215218973, -0.2545880711246172, 0.004461937467567623, -0.23404150078425834, -0.14273827422145732, 0.003784496047859185, -0.063368038143466... |
706.4169 | Subsampling needlet coefficients on the sphere | In a recent paper, we analyzed the properties of a new kind of spherical
wavelets (called needlets) for statistical inference procedures on spherical
random fields; the investigation was mainly motivated by applications to
cosmological data. In the present work, we exploit the asymptotic uncorrelation
of random needl... | math.ST astro-ph math.PR stat.TH | in a recent paper we analyzed the properties of a new kind of spherical wavelets called needlets for statistical inference procedures on spherical random fields the investigation was mainly motivated by applications to cosmological data in the present work we exploit the asymptotic uncorrelation of random needlet coeff... | [['in', 'a', 'recent', 'paper', 'we', 'analyzed', 'the', 'properties', 'of', 'a', 'new', 'kind', 'of', 'spherical', 'wavelets', 'called', 'needlets', 'for', 'statistical', 'inference', 'procedures', 'on', 'spherical', 'random', 'fields', 'the', 'investigation', 'was', 'mainly', 'motivated', 'by', 'applications', 'to', ... | [-0.07162867930407325, 0.07988528372453792, -0.10996164294137131, 0.0925428188594413, -0.07632505597679742, -0.07745566843742771, 0.014696221654525115, 0.3776064434399207, -0.23181573745484155, -0.2504300346154542, 0.12567369222108807, -0.2249506686592386, -0.16661062749723593, 0.20702089690381573, -0.10593979893241166... |
706.417 | Hilbert++ Manual | We present here an installation guide, a hand-on mini-tutorial through
examples, and the theoretical foundations of the Hilbert++ code.
| cs.OH cond-mat.str-el | we present here an installation guide a handon minitutorial through examples and the theoretical foundations of the hilbert code | [['we', 'present', 'here', 'an', 'installation', 'guide', 'a', 'handon', 'minitutorial', 'through', 'examples', 'and', 'the', 'theoretical', 'foundations', 'of', 'the', 'hilbert', 'code']] | [-0.0626418325636122, 0.024344088128903724, -0.10966367574615611, 0.014927049063973956, -0.10246667348676258, -0.09848571990409659, 0.061552690070432924, 0.3623658956752883, -0.2506946631603771, -0.25816829554322696, 0.13318513724435535, -0.22955628836320507, -0.1815838211009072, 0.24678992645608056, -0.069754223882531... |
706.4171 | Local dark energy: HST evidence from the vicinity of the M 81/M 82
galaxy group | The Hubble Space Telescope observations of the nearby galaxy group M 81/M 82
and its vicinity indicate that the expansion outflow around the group is
dominated by the antigravity of the dark energy background. The local density
of dark energy in the area is estimated to be near the global dark energy
density or perha... | astro-ph | the hubble space telescope observations of the nearby galaxy group m 81m 82 and its vicinity indicate that the expansion outflow around the group is dominated by the antigravity of the dark energy background the local density of dark energy in the area is estimated to be near the global dark energy density or perhaps e... | [['the', 'hubble', 'space', 'telescope', 'observations', 'of', 'the', 'nearby', 'galaxy', 'group', 'm', '81m', '82', 'and', 'its', 'vicinity', 'indicate', 'that', 'the', 'expansion', 'outflow', 'around', 'the', 'group', 'is', 'dominated', 'by', 'the', 'antigravity', 'of', 'the', 'dark', 'energy', 'background', 'the', '... | [-0.12979959789299755, 0.0774327055143658, -0.09336690315394662, 0.06368654573016101, -0.08314700281480328, -0.01660143623012118, 0.03874649388017133, 0.3246445499360561, -0.189425909682177, -0.3846106050303206, 0.0617590488269343, -0.29919971426716074, -0.03101946731621865, 0.17030501607223414, -0.0019816395710222424,... |
706.4172 | Spin configuration in a frustrated ferromagnetic/antiferromagnetic thin
film system | We have studied the magnetic configuration in ultrathin antiferromagnetic Mn
films grown around monoatomic steps on an Fe(001) surface by spin-polarized
scanning tunneling microscopy/spectroscopy and ab-initio-parametrized
self-consistent real-space tight binding calculations in which the spin
quantization axis is in... | cond-mat.mtrl-sci | we have studied the magnetic configuration in ultrathin antiferromagnetic mn films grown around monoatomic steps on an fe001 surface by spinpolarized scanning tunneling microscopyspectroscopy and abinitioparametrized selfconsistent realspace tight binding calculations in which the spin quantization axis is independent ... | [['we', 'have', 'studied', 'the', 'magnetic', 'configuration', 'in', 'ultrathin', 'antiferromagnetic', 'mn', 'films', 'grown', 'around', 'monoatomic', 'steps', 'on', 'an', 'fe001', 'surface', 'by', 'spinpolarized', 'scanning', 'tunneling', 'microscopyspectroscopy', 'and', 'abinitioparametrized', 'selfconsistent', 'real... | [-0.19319692135468358, 0.19579328544489272, 0.04018503640691051, -0.015524475774327584, 0.009413634521479253, -0.13918069196552096, 0.10362799907488807, 0.4455007846117951, -0.27309054445140646, -0.31241232391039375, -0.028673086300841533, -0.32571618269139435, -0.042577349762723316, 0.12996410782761814, 0.083352651465... |
706.4173 | FPCP Theory Overview | We first review some aspects of the determination of the sides and angles of
the unitarity triangle. We pay particular attention to theory shortcomings, and
present many alternative proposals for the determination of |Vub| (which at
present is problematic). We then turn our attention to the more general
question: Wha... | hep-ph | we first review some aspects of the determination of the sides and angles of the unitarity triangle we pay particular attention to theory shortcomings and present many alternative proposals for the determination of vub which at present is problematic we then turn our attention to the more general question what have we ... | [['we', 'first', 'review', 'some', 'aspects', 'of', 'the', 'determination', 'of', 'the', 'sides', 'and', 'angles', 'of', 'the', 'unitarity', 'triangle', 'we', 'pay', 'particular', 'attention', 'to', 'theory', 'shortcomings', 'and', 'present', 'many', 'alternative', 'proposals', 'for', 'the', 'determination', 'of', 'vub... | [-0.03740057272319733, 0.13821212546183512, -0.07886483839388098, 0.12137327383778948, -0.14509345860742442, -0.15695125736285942, 0.11863373219838959, 0.3641607052810326, -0.2553344091789408, -0.29958214740790834, 0.10226743545506027, -0.28187351828635476, -0.11420661935859083, 0.12321985077885604, -0.0319804038064411... |
706.4174 | Lattice Boltzmann simulations of spontaneous flow in active liquid
crystals: the role of boundary conditions | Active liquid crystals or active gels are soft materials which can be
physically realised e.g. by preparing a solution of cytoskeletal filaments
interacting with molecular motors. We study the hydrodynamics of an active
liquid crystal in a slab-like geometry with various boundary conditions, by
solving numerically it... | cond-mat.soft cond-mat.stat-mech | active liquid crystals or active gels are soft materials which can be physically realised eg by preparing a solution of cytoskeletal filaments interacting with molecular motors we study the hydrodynamics of an active liquid crystal in a slablike geometry with various boundary conditions by solving numerically its equat... | [['active', 'liquid', 'crystals', 'or', 'active', 'gels', 'are', 'soft', 'materials', 'which', 'can', 'be', 'physically', 'realised', 'eg', 'by', 'preparing', 'a', 'solution', 'of', 'cytoskeletal', 'filaments', 'interacting', 'with', 'molecular', 'motors', 'we', 'study', 'the', 'hydrodynamics', 'of', 'an', 'active', 'l... | [-0.13716252524104408, 0.2262027549176684, -0.04991885886171504, -0.01600652397610247, -0.031484545157154036, -0.16197753274087412, 0.05623462744509144, 0.4240369914058486, -0.25117093671168034, -0.28789238306789605, 0.1131552491150454, -0.27600902745582384, -0.13108277338152916, 0.14634768561946282, 0.0163514308087007... |
706.4175 | Heuristics for Network Coding in Wireless Networks | Multicast is a central challenge for emerging multi-hop wireless
architectures such as wireless mesh networks, because of its substantial cost
in terms of bandwidth. In this report, we study one specific case of multicast:
broadcasting, sending data from one source to all nodes, in a multi-hop
wireless network. The b... | cs.NI | multicast is a central challenge for emerging multihop wireless architectures such as wireless mesh networks because of its substantial cost in terms of bandwidth in this report we study one specific case of multicast broadcasting sending data from one source to all nodes in a multihop wireless network the broadcast we... | [['multicast', 'is', 'a', 'central', 'challenge', 'for', 'emerging', 'multihop', 'wireless', 'architectures', 'such', 'as', 'wireless', 'mesh', 'networks', 'because', 'of', 'its', 'substantial', 'cost', 'in', 'terms', 'of', 'bandwidth', 'in', 'this', 'report', 'we', 'study', 'one', 'specific', 'case', 'of', 'multicast'... | [-0.2049966506191431, -0.013081688497516309, -0.008947407977181191, 0.013427022832622232, -0.09717063481705437, -0.22663270796631804, 0.11936957101042596, 0.4530702526710048, -0.26504246297911366, -0.29253429895764366, 0.10301025154832635, -0.23529161244445707, -0.21205137750590855, 0.18635143748461414, -0.135588147020... |
706.4176 | Entanglement Transfer Through an Antiferromagnetic Spin Chain | We study the possibility of using an uniformly coupled finite
antiferromagnetic spin-1/2 Heisenberg chain as a channel for transmitting
entanglement. One member of a pair of maximally entangled spins is initially
appended to one end of a chain in its ground state and the dynamical
propagation of this entanglement to ... | quant-ph | we study the possibility of using an uniformly coupled finite antiferromagnetic spin12 heisenberg chain as a channel for transmitting entanglement one member of a pair of maximally entangled spins is initially appended to one end of a chain in its ground state and the dynamical propagation of this entanglement to the o... | [['we', 'study', 'the', 'possibility', 'of', 'using', 'an', 'uniformly', 'coupled', 'finite', 'antiferromagnetic', 'spin12', 'heisenberg', 'chain', 'as', 'a', 'channel', 'for', 'transmitting', 'entanglement', 'one', 'member', 'of', 'a', 'pair', 'of', 'maximally', 'entangled', 'spins', 'is', 'initially', 'appended', 'to... | [-0.15341922270356498, 0.24184032391555652, -0.05368678821181295, 0.0412102671115965, -0.019534548033904562, -0.21299230017605475, 0.06720710702852081, 0.4167785710210342, -0.26786641695939784, -0.22187514503576808, 0.082453666129775, -0.32207989681046456, -0.04341367863417506, 0.14707964670899978, 0.04065495139724617,... |
706.4177 | \C-flows A^z of linear maps A expressed in terms of
A^{-1},A^{-2},...,A^{-n} and analytic functions of z | Suppose A\in GL_n(\C) has a relation A^p=c_{p-1}A^{p-1}+.... + c_1 A+ c_0I
where the c_i in \C. This article describes how to construct analytic functions
c_i(z) such that A^z=c_{p-1}(z)A^{p-1}+... + c_1(z) A+ c_0(z)I . One of the
theorems gives a possible description of the c_i(z): c_i(z)=C^z\alpha where
C\in Mat_p(... | math.AC math.AG math.CV | suppose ain gl_nc has a relation apc_p1ap1 c_1 a c_0i where the c_i in c this article describes how to construct analytic functions c_iz such that azc_p1zap1 c_1z a c_0zi one of the theorems gives a possible description of the c_iz c_izczalpha where cin mat_pc is similar to the companion matrix of xpc_p1xp1 c_1xc_0i an... | [['suppose', 'ain', 'gl_nc', 'has', 'a', 'relation', 'apc_p1ap1', 'c_1', 'a', 'c_0i', 'where', 'the', 'c_i', 'in', 'c', 'this', 'article', 'describes', 'how', 'to', 'construct', 'analytic', 'functions', 'c_iz', 'such', 'that', 'azc_p1zap1', 'c_1z', 'a', 'c_0zi', 'one', 'of', 'the', 'theorems', 'gives', 'a', 'possible',... | [-0.1554762461034462, 0.08730840096448331, -0.09603793065539225, 0.007642443430550555, -0.05070426852065832, -0.1880654896748193, 0.021264362109309817, 0.31556741821956125, -0.2737800179227711, -0.14502344381539745, 0.05009740040924875, -0.30970222526725305, -0.18210516469751267, 0.1617068414120598, -0.0815057405270636... |
706.4178 | Lattice polytopes of degree 2 | A theorem of Scott gives an upper bound for the normalized volume of lattice
polygons with exactly $i>0$ interior lattice points. We will show that the same
bound is true for the normalized volume of lattice polytopes of degree 2 even
in higher dimensions. In particular, there is only a finite number of quadratic
pol... | math.CO | a theorem of scott gives an upper bound for the normalized volume of lattice polygons with exactly i0 interior lattice points we will show that the same bound is true for the normalized volume of lattice polytopes of degree 2 even in higher dimensions in particular there is only a finite number of quadratic polynomials... | [['a', 'theorem', 'of', 'scott', 'gives', 'an', 'upper', 'bound', 'for', 'the', 'normalized', 'volume', 'of', 'lattice', 'polygons', 'with', 'exactly', 'i0', 'interior', 'lattice', 'points', 'we', 'will', 'show', 'that', 'the', 'same', 'bound', 'is', 'true', 'for', 'the', 'normalized', 'volume', 'of', 'lattice', 'polyt... | [-0.19269886978365708, 0.17350619178548435, -0.07075168981894174, 0.02954383110839196, -0.03230315653226254, -0.13343164709283772, 0.0779738111499076, 0.30311367322098126, -0.25803831657112547, -0.19248351214848686, 0.10257985161010627, -0.31383337249810045, -0.1256809000659621, 0.14985569954539338, -0.0945220612638601... |
706.4179 | Overview: Sides of the Unitarity Triangle | This is an opening talk for the workshop and is intended to be provocative.
We take a stab at the following questions: How well do we really know the sides
of the unitarity triangle? What else could we do to improve? (I propose several
new measurements). What precision should we ultimately aim at in the
determination... | hep-ph | this is an opening talk for the workshop and is intended to be provocative we take a stab at the following questions how well do we really know the sides of the unitarity triangle what else could we do to improve i propose several new measurements what precision should we ultimately aim at in the determination of ckm e... | [['this', 'is', 'an', 'opening', 'talk', 'for', 'the', 'workshop', 'and', 'is', 'intended', 'to', 'be', 'provocative', 'we', 'take', 'a', 'stab', 'at', 'the', 'following', 'questions', 'how', 'well', 'do', 'we', 'really', 'know', 'the', 'sides', 'of', 'the', 'unitarity', 'triangle', 'what', 'else', 'could', 'we', 'do',... | [-0.0352477556144869, 0.16293869537125952, -0.11972705337747529, 0.10341535937324217, -0.19630266522762138, -0.15475690905893585, 0.10534874395769392, 0.39245263200152564, -0.2999167064255154, -0.3086840384891508, 0.1115357953523336, -0.3118897289182437, -0.11880989662195379, 0.10973739998282965, -0.11527593483569452, ... |
706.418 | Universal Grammar and Consciousness | The orthodox interpretation of quantum theory treats the subject and the
object on an equal footing. It has been suggested that the cyclical-time
process, which resolves self-reference in consciousness, interconnects the
observed universe and the mind of the subject. Based on the analogy between
cryptography and lang... | physics.gen-ph | the orthodox interpretation of quantum theory treats the subject and the object on an equal footing it has been suggested that the cyclicaltime process which resolves selfreference in consciousness interconnects the observed universe and the mind of the subject based on the analogy between cryptography and language the... | [['the', 'orthodox', 'interpretation', 'of', 'quantum', 'theory', 'treats', 'the', 'subject', 'and', 'the', 'object', 'on', 'an', 'equal', 'footing', 'it', 'has', 'been', 'suggested', 'that', 'the', 'cyclicaltime', 'process', 'which', 'resolves', 'selfreference', 'in', 'consciousness', 'interconnects', 'the', 'observed... | [-0.08954647912436889, 0.09287558208986108, -0.1288626579153869, 0.07799706259467915, -0.11507762140697902, -0.13459575724167128, 0.024287585511855368, 0.3462389486324456, -0.285579727186511, -0.2943058710441821, 0.04144141299184412, -0.21637614779174327, -0.19344397466629742, 0.152347407117486, -0.12895538421451216, 0... |
706.4181 | A characterization property on field equivalent to algebraicity on
Banach spaces | In his article "A discrete form of the theorem that each field endomorphism
of $\mathbb{R}$ ($\mathbb{Q}_p$) is the identity", Tyszka introduce a logical
property which is equivalent to algebraicity in $\mathbb{R}$ and in
$\mathbb{Q}_p$. Amazingly, the property is no longer equivalent to algebraicity
in $\mathbb{C}$.... | math.NT math.LO | in his article a discrete form of the theorem that each field endomorphism of mathbbr mathbbq_p is the identity tyszka introduce a logical property which is equivalent to algebraicity in mathbbr and in mathbbq_p amazingly the property is no longer equivalent to algebraicity in mathbbc this article present a similirar p... | [['in', 'his', 'article', 'a', 'discrete', 'form', 'of', 'the', 'theorem', 'that', 'each', 'field', 'endomorphism', 'of', 'mathbbr', 'mathbbq_p', 'is', 'the', 'identity', 'tyszka', 'introduce', 'a', 'logical', 'property', 'which', 'is', 'equivalent', 'to', 'algebraicity', 'in', 'mathbbr', 'and', 'in', 'mathbbq_p', 'ama... | [-0.16356532689597872, 0.08654110928146559, -0.1305822773353645, 0.10452672876676337, -0.11877178708896224, -0.15399421228923732, -0.011388369068434392, 0.36070173758047597, -0.30882303529407507, -0.13071945058411838, 0.10601997353498721, -0.19666032836898978, -0.13839024675573097, 0.1833487897536453, -0.14967574449371... |
706.4182 | Experimental tests of small-x QCD | Current and future experimental studies of the high-energy limit of QCD,
dominated by non-linear gluon dynamics in the low-x sector of the hadron
wavefunctions, are presented. Results at HERA (proton) and RHIC (nucleus)
pointing to the possible onset of parton saturation phenomena, and perspectives
at the LHC and new... | hep-ex nucl-ex nucl-th | current and future experimental studies of the highenergy limit of qcd dominated by nonlinear gluon dynamics in the lowx sector of the hadron wavefunctions are presented results at hera proton and rhic nucleus pointing to the possible onset of parton saturation phenomena and perspectives at the lhc and new proposed dis... | [['current', 'and', 'future', 'experimental', 'studies', 'of', 'the', 'highenergy', 'limit', 'of', 'qcd', 'dominated', 'by', 'nonlinear', 'gluon', 'dynamics', 'in', 'the', 'lowx', 'sector', 'of', 'the', 'hadron', 'wavefunctions', 'are', 'presented', 'results', 'at', 'hera', 'proton', 'and', 'rhic', 'nucleus', 'pointing... | [-0.01917621604580846, 0.2714402637772124, -0.15058578468893688, 0.16573439368167547, -0.05186713821496124, -0.05647580011821076, -0.023850141347523918, 0.33924796163207954, -0.1884478040177513, -0.17391313454653654, 0.019594385398603562, -0.35372903470501854, 0.029010283381298737, 0.17556867448406088, 0.13196557717121... |
706.4183 | Infinitely generated Derksen and Makar-Limanov invariant | In this paper, we give an example of a finitely generated 3-dimensional
C-algebra which has infinitely generated Derksen invariant as well as
Makar-Limaonv invariant.
| math.AG math.AC | in this paper we give an example of a finitely generated 3dimensional calgebra which has infinitely generated derksen invariant as well as makarlimaonv invariant | [['in', 'this', 'paper', 'we', 'give', 'an', 'example', 'of', 'a', 'finitely', 'generated', '3dimensional', 'calgebra', 'which', 'has', 'infinitely', 'generated', 'derksen', 'invariant', 'as', 'well', 'as', 'makarlimaonv', 'invariant']] | [-0.12585851971222006, 0.19194254585422837, -0.10868551063796748, 0.0576378058227103, -0.02711327867987363, -0.12345450191313158, -0.1570638388587648, 0.38058208334057225, -0.34887596446534863, -0.2564373985742745, 0.10354866945366982, -0.23383164486807326, -0.2053232150071341, 0.2277427338387655, -0.14842638701362454,... |
706.4184 | Constructing (almost) rigid rings and a UFD having infinitely generated
Derksen and Makar-Limanov invariant | An example is given of a UFD which has infinitely generated Derksen
invariant. The ring is \textquotedblleft almost rigid\textquotedblright\
meaning that the Derksen invariant is equal to the Makar-Limanov invariant.
Techniques to show that a ring is (almost) rigid are discussed, among which is
a generalization of Ma... | math.AG math.AC | an example is given of a ufd which has infinitely generated derksen invariant the ring is textquotedblleft almost rigidtextquotedblright meaning that the derksen invariant is equal to the makarlimanov invariant techniques to show that a ring is almost rigid are discussed among which is a generalization of masons abcthe... | [['an', 'example', 'is', 'given', 'of', 'a', 'ufd', 'which', 'has', 'infinitely', 'generated', 'derksen', 'invariant', 'the', 'ring', 'is', 'textquotedblleft', 'almost', 'rigidtextquotedblright', 'meaning', 'that', 'the', 'derksen', 'invariant', 'is', 'equal', 'to', 'the', 'makarlimanov', 'invariant', 'techniques', 'to... | [-0.22868217714130878, 0.12848181146819115, -0.15551955272288373, 0.08272278151950256, -0.0652688824920915, -0.17263325234913887, -0.10918928772540919, 0.3641697062800328, -0.2841991863679141, -0.1935394888666148, 0.07558222867858906, -0.25797298533143476, -0.18021771065347517, 0.20021890827532238, -0.13864965492393821... |
706.4185 | Minimal Flavor Violation | If new physics is called upon to explain away fine tunings, like the
hierarchy problem, then, we argue, the principle of Minimal Flavor Violation is
inescapable. We review the principle and recent extensions to the lepton sector
and to Grand-Unified theories.
| hep-ph | if new physics is called upon to explain away fine tunings like the hierarchy problem then we argue the principle of minimal flavor violation is inescapable we review the principle and recent extensions to the lepton sector and to grandunified theories | [['if', 'new', 'physics', 'is', 'called', 'upon', 'to', 'explain', 'away', 'fine', 'tunings', 'like', 'the', 'hierarchy', 'problem', 'then', 'we', 'argue', 'the', 'principle', 'of', 'minimal', 'flavor', 'violation', 'is', 'inescapable', 'we', 'review', 'the', 'principle', 'and', 'recent', 'extensions', 'to', 'the', 'le... | [-0.05319700394643516, 0.20928342903896077, -0.04208702820057913, 0.18853497105968617, -0.18128346252005276, -0.16282824613153934, 0.06764067498194735, 0.25586591448589435, -0.3158733633051558, -0.313783660780911, 0.09880079983211146, -0.25806822003115243, -0.11006208999854762, 0.10336898326328615, -0.08537199975150388... |
706.4186 | Zero-Bidimension and Various Classes of Bitopological Spaces | The sum theorem and its corollaries are proved for a countable family of
zero-dimensional (in the sense of small and large inductive bidimensions)
p-closed sets, using a new notion of relative normality whose topological
correspondent is also new. The notion of almost $n$-dimensionality is
considered from the bitopol... | math.GN | the sum theorem and its corollaries are proved for a countable family of zerodimensional in the sense of small and large inductive bidimensions pclosed sets using a new notion of relative normality whose topological correspondent is also new the notion of almost ndimensionality is considered from the bitopological poin... | [['the', 'sum', 'theorem', 'and', 'its', 'corollaries', 'are', 'proved', 'for', 'a', 'countable', 'family', 'of', 'zerodimensional', 'in', 'the', 'sense', 'of', 'small', 'and', 'large', 'inductive', 'bidimensions', 'pclosed', 'sets', 'using', 'a', 'new', 'notion', 'of', 'relative', 'normality', 'whose', 'topological', ... | [-0.11889062383449933, 0.10692433030999382, -0.052406138681033825, 0.06925337239257753, -0.03957283669126597, -0.09818145129804876, 0.016952710264570455, 0.36788875996036097, -0.27327552792725174, -0.24899360274727594, 0.17538155604245517, -0.28637511753279005, -0.12040585810516743, 0.2302372094241907, -0.0972487558065... |
706.4187 | The Automorphism Group of Certain Factorial Threefolds and a
Cancellation Problem | The automorphism groups of certain factorial complex affine threefolds
admitting locally trivial actions of the additive group are determined. As a
consequence new counterexamples to a generalized cancellation problem are
obtained.
| math.AG math.AC | the automorphism groups of certain factorial complex affine threefolds admitting locally trivial actions of the additive group are determined as a consequence new counterexamples to a generalized cancellation problem are obtained | [['the', 'automorphism', 'groups', 'of', 'certain', 'factorial', 'complex', 'affine', 'threefolds', 'admitting', 'locally', 'trivial', 'actions', 'of', 'the', 'additive', 'group', 'are', 'determined', 'as', 'a', 'consequence', 'new', 'counterexamples', 'to', 'a', 'generalized', 'cancellation', 'problem', 'are', 'obtain... | [-0.24430220165560323, 0.10275558003735158, -0.05891401530994523, 0.1362770708698419, -0.18849641385097657, -0.18751912789359207, 0.015809423181288425, 0.36203033621272734, -0.36320570543889075, -0.21266414801920613, 0.15861673277592467, -0.2203921738471235, -0.20809849360657315, 0.22728104781239264, -0.193890144417603... |
706.4188 | Holography and Cosmological Singularities | Certain null singularities in ten dimensional supergravity have natural
holographic duals in terms of Matrix Theory and generalizations of the AdS/CFT
correspondence. In many situations the holographic duals appear to be well
defined in regions where the supergravity develops singularities. We describe
some recent pr... | hep-th | certain null singularities in ten dimensional supergravity have natural holographic duals in terms of matrix theory and generalizations of the adscft correspondence in many situations the holographic duals appear to be well defined in regions where the supergravity develops singularities we describe some recent progres... | [['certain', 'null', 'singularities', 'in', 'ten', 'dimensional', 'supergravity', 'have', 'natural', 'holographic', 'duals', 'in', 'terms', 'of', 'matrix', 'theory', 'and', 'generalizations', 'of', 'the', 'adscft', 'correspondence', 'in', 'many', 'situations', 'the', 'holographic', 'duals', 'appear', 'to', 'be', 'well'... | [-0.12035827279517737, 0.10896644494884337, -0.05660720798186958, 0.11777057641059703, -0.0871805751521606, -0.1381499272150298, -0.09512001925274187, 0.3007737267568397, -0.17756265363035104, -0.19254505548936626, 0.11247238736784008, -0.2923860943798597, -0.23149039371249577, 0.10293827361116807, -0.17749889850771675... |
706.4189 | Stable-Range Approach to the Equation of Nonstationary Transonic Gas
Flows | Using certain finite-dimensional stable range of the nonlinear terms, we
obtain large families of exact solutions parameterized by functions for the
equation of nonstationary transonic gas flows discovered by Lin, Reisner and
Tsien, and its three-dimensional generalization.
| physics.flu-dyn math-ph math.AP math.MP nlin.SI | using certain finitedimensional stable range of the nonlinear terms we obtain large families of exact solutions parameterized by functions for the equation of nonstationary transonic gas flows discovered by lin reisner and tsien and its threedimensional generalization | [['using', 'certain', 'finitedimensional', 'stable', 'range', 'of', 'the', 'nonlinear', 'terms', 'we', 'obtain', 'large', 'families', 'of', 'exact', 'solutions', 'parameterized', 'by', 'functions', 'for', 'the', 'equation', 'of', 'nonstationary', 'transonic', 'gas', 'flows', 'discovered', 'by', 'lin', 'reisner', 'and',... | [-0.13269567255661563, 0.0647145564823101, -0.000910361452649037, 0.04591730736946273, -0.04443650594395068, -0.11921332847689176, -0.005972143262624741, 0.23900590278208256, -0.3097873159891201, -0.27680849977251554, 0.12637167936190963, -0.21951616749477884, -0.14844738071163496, 0.255733963722984, -0.033924665974660... |
706.419 | SiZer for time series: A new approach to the analysis of trends | Smoothing methods and SiZer are a useful statistical tool for discovering
statistically significant structure in data. Based on scale space ideas
originally developed in the computer vision literature, SiZer (SIgnificant ZERo
crossing of the derivatives) is a graphical device to assess which observed
features are `re... | stat.ME | smoothing methods and sizer are a useful statistical tool for discovering statistically significant structure in data based on scale space ideas originally developed in the computer vision literature sizer significant zero crossing of the derivatives is a graphical device to assess which observed features are really th... | [['smoothing', 'methods', 'and', 'sizer', 'are', 'a', 'useful', 'statistical', 'tool', 'for', 'discovering', 'statistically', 'significant', 'structure', 'in', 'data', 'based', 'on', 'scale', 'space', 'ideas', 'originally', 'developed', 'in', 'the', 'computer', 'vision', 'literature', 'sizer', 'significant', 'zero', 'c... | [-0.05633192666904713, 0.015186013422936686, -0.14622048100804894, 0.13064957555947537, -0.1394805251204265, -0.1326343768704077, 0.029766881460800948, 0.3683298464894779, -0.2542675767184758, -0.3663181825503101, 0.1366258116128544, -0.2775156807525432, -0.1745427444244061, 0.2279139588117539, -0.09926318863361347, 0.... |
706.4191 | Kaluza--Klein excitations of gauge bosons at the LHC | We consider the Randall-Sundrum extra dimensional model with fields
propagating in the bulk based on an extended electroweak gauge symmetry with
specific fermion charges and localizations that allow to explain the LEP
anomaly of the forward--backward asymmetry for $b$--quarks, $A_{FB}^b$. We
study the manifestations ... | hep-ph | we consider the randallsundrum extra dimensional model with fields propagating in the bulk based on an extended electroweak gauge symmetry with specific fermion charges and localizations that allow to explain the lep anomaly of the forwardbackward asymmetry for bquarks a_fbb we study the manifestations of the stronglyi... | [['we', 'consider', 'the', 'randallsundrum', 'extra', 'dimensional', 'model', 'with', 'fields', 'propagating', 'in', 'the', 'bulk', 'based', 'on', 'an', 'extended', 'electroweak', 'gauge', 'symmetry', 'with', 'specific', 'fermion', 'charges', 'and', 'localizations', 'that', 'allow', 'to', 'explain', 'the', 'lep', 'anom... | [-0.07336965332155267, 0.31469430720913166, -0.038721937338456934, 0.13998014890759858, -0.07057787662265849, -0.1659325203988427, 0.0670703031359795, 0.3025170210355153, -0.22820605642696404, -0.24386712506705355, -0.04710716891157277, -0.3240502522068495, 0.023512932531850633, 0.06689768355178838, 0.05967401780927663... |
706.4192 | Equation of State for Macromolecules of Variable Flexibility in Good
Solvents: A Comparison of Techniques for Monte Carlo Simulations of Lattice
Models | The osmotic equation of state for the athermal bond fluctuation model on the
simple cubic lattice is obtained from extensive Monte Carlo simulations. For
short macromolecules (chain length N=20) we study the influence of various
choices for the chain stiffness on the equation of state. Three techniques are
applied an... | cond-mat.soft | the osmotic equation of state for the athermal bond fluctuation model on the simple cubic lattice is obtained from extensive monte carlo simulations for short macromolecules chain length n20 we study the influence of various choices for the chain stiffness on the equation of state three techniques are applied and compa... | [['the', 'osmotic', 'equation', 'of', 'state', 'for', 'the', 'athermal', 'bond', 'fluctuation', 'model', 'on', 'the', 'simple', 'cubic', 'lattice', 'is', 'obtained', 'from', 'extensive', 'monte', 'carlo', 'simulations', 'for', 'short', 'macromolecules', 'chain', 'length', 'n20', 'we', 'study', 'the', 'influence', 'of',... | [-0.10171640326639729, 0.11586155922415618, -0.13435432960218546, 0.06165049592496159, -0.010199361536449389, -0.09938197166648814, 0.06392264172293084, 0.35513746742483066, -0.2536578929942587, -0.2984939918134604, 0.08776696710075434, -0.2671074693840321, -0.11781533724506912, 0.14087133104887628, 0.06057711009887735... |
706.4193 | Transportation-information inequalities for Markov processes | In this paper, one investigates the following type of
transportation-information $T_cI$ inequalities: $\alpha(T_c(\nu,\mu))\le
I(\nu|\mu)$ for all probability measures $\nu$ on some metric space $(\XX, d)$,
where $\mu$ is a given probability measure, $T_c(\nu,\mu)$ is the
transportation cost from $\nu$ to $\mu$ with ... | math.PR math.FA | in this paper one investigates the following type of transportationinformation t_ci inequalities alphat_cnumule inumu for all probability measures nu on some metric space xx d where mu is a given probability measure t_cnumu is the transportation cost from nu to mu with respect to some cost function cxy on xx2 inumu is ... | [['in', 'this', 'paper', 'one', 'investigates', 'the', 'following', 'type', 'of', 'transportationinformation', 't_ci', 'inequalities', 'alphat_cnumule', 'inumu', 'for', 'all', 'probability', 'measures', 'nu', 'on', 'some', 'metric', 'space', 'xx', 'd', 'where', 'mu', 'is', 'a', 'given', 'probability', 'measure', 't_cnu... | [-0.09780764126857132, 0.10535947349653098, -0.051129317344648054, 0.08689115914586214, -0.034915191996521475, -0.18345263032724374, 0.06518601290660846, 0.3569407622281719, -0.29654499787259203, -0.18571456407843126, 0.10971185987502144, -0.34997339131599614, -0.118218038232138, 0.20096631650812924, -0.117046499127072... |
706.4194 | Kinetics of indirect excitons in the optically-induced exciton trap | We report on the kinetics of a low-temperature gas of indirect excitons in
the optically-induced exciton trap. The excitons in the region of laser
excitation are found to rapidly -- within 4 ns -- cool to the lattice
temperature T = 1.4 K, while the excitons at the trap center are found to be
cold -- essentially at t... | cond-mat.mes-hall | we report on the kinetics of a lowtemperature gas of indirect excitons in the opticallyinduced exciton trap the excitons in the region of laser excitation are found to rapidly within 4 ns cool to the lattice temperature t 14 k while the excitons at the trap center are found to be cold essentially at the lattice tempera... | [['we', 'report', 'on', 'the', 'kinetics', 'of', 'a', 'lowtemperature', 'gas', 'of', 'indirect', 'excitons', 'in', 'the', 'opticallyinduced', 'exciton', 'trap', 'the', 'excitons', 'in', 'the', 'region', 'of', 'laser', 'excitation', 'are', 'found', 'to', 'rapidly', 'within', '4', 'ns', 'cool', 'to', 'the', 'lattice', 't... | [-0.09351447336510038, 0.26060453989328103, -0.024768289959488005, 0.03700464302853036, 0.04085242589219258, -0.12473839332009308, 0.0878926237543615, 0.43963316191847507, -0.23796468093418158, -0.3148601486849097, 0.043202678124026325, -0.2497874372692492, 0.06548575627832459, 0.18738625279018797, 0.08473554332001815,... |
706.4195 | Flag Partial Differential Equations and Representations of Lie Algebras | In this paper, we solve the initial value problems of variable-coefficient
generalized wave equations associated with trees and a large family of linear
constant-coefficient partial differential equation by algebraic methods.
Moreover, we find all the polynomial solutions for a 3-dimensional
variable-coefficient flag... | math.RT math-ph math.AP math.MP nlin.SI | in this paper we solve the initial value problems of variablecoefficient generalized wave equations associated with trees and a large family of linear constantcoefficient partial differential equation by algebraic methods moreover we find all the polynomial solutions for a 3dimensional variablecoefficient flag partial ... | [['in', 'this', 'paper', 'we', 'solve', 'the', 'initial', 'value', 'problems', 'of', 'variablecoefficient', 'generalized', 'wave', 'equations', 'associated', 'with', 'trees', 'and', 'a', 'large', 'family', 'of', 'linear', 'constantcoefficient', 'partial', 'differential', 'equation', 'by', 'algebraic', 'methods', 'moreo... | [-0.16941684706136584, 0.014374318541958928, -0.04369666412472725, 0.06323950655176304, -0.21290231408085675, -0.11482995272148401, -0.08893920255708508, 0.2607786575704813, -0.3779938149265945, -0.2086261430475861, 0.15689085652003995, -0.2751346963644028, -0.21171133559197186, 0.19861389704979956, -0.0282218179013580... |
706.4196 | The paraboson Fock space and unitary irreducible representations of the
Lie superalgebra osp(1|2n) | It is known that the defining relations of the orthosymplectic Lie
superalgebra osp(1|2n) are equivalent to the defining (triple) relations of n
pairs of paraboson operators $b^\pm_i$. In particular, with the usual star
conditions, this implies that the ``parabosons of order p'' correspond to a
unitary irreducible (i... | hep-th math-ph math.GR math.MP math.RT quant-ph | it is known that the defining relations of the orthosymplectic lie superalgebra osp12n are equivalent to the defining triple relations of n pairs of paraboson operators bpm_i in particular with the usual star conditions this implies that the parabosons of order p correspond to a unitary irreducible infinitedimensional ... | [['it', 'is', 'known', 'that', 'the', 'defining', 'relations', 'of', 'the', 'orthosymplectic', 'lie', 'superalgebra', 'osp12n', 'are', 'equivalent', 'to', 'the', 'defining', 'triple', 'relations', 'of', 'n', 'pairs', 'of', 'paraboson', 'operators', 'bpm_i', 'in', 'particular', 'with', 'the', 'usual', 'star', 'condition... | [-0.14140477495275264, 0.12006081838298996, -0.058996575525088704, 0.054048385139321906, -0.10055059885780793, -0.10004342102947703, 0.001786096831347095, 0.35654399972991085, -0.25965690694574733, -0.21595678199955728, 0.0828750900553132, -0.22496588369540405, -0.1951378415353247, 0.13382678445195778, -0.0800396555593... |
706.4197 | On the Theory of Relative Bitopological and Topological Properties | In the first part of the work (Sections 2-6) a special attention is given to
relative separation axioms and relative connectedness, in particular, many
relative versions of p-T_0, p-T_1, p-T_2, (i,j)- and p-regularities, (i,j)- and
p-complete regularities, p-real normality and p-normality are discussed.
Moreover, rel... | math.GN | in the first part of the work sections 26 a special attention is given to relative separation axioms and relative connectedness in particular many relative versions of pt_0 pt_1 pt_2 ij and pregularities ij and pcomplete regularities preal normality and pnormality are discussed moreover relative properties of ij and pc... | [['in', 'the', 'first', 'part', 'of', 'the', 'work', 'sections', '26', 'a', 'special', 'attention', 'is', 'given', 'to', 'relative', 'separation', 'axioms', 'and', 'relative', 'connectedness', 'in', 'particular', 'many', 'relative', 'versions', 'of', 'pt_0', 'pt_1', 'pt_2', 'ij', 'and', 'pregularities', 'ij', 'and', 'p... | [-0.08049586490827491, 0.08327116085330152, -0.03143372398068887, 0.08976129126265815, -0.03451970025083007, -0.12848787026778433, 0.008572222465890964, 0.3620144081238003, -0.24244421898593543, -0.2410193685840332, 0.11684461849748747, -0.291103353080489, -0.11890956020082226, 0.17449655957548446, -0.11731766395356136... |
706.4198 | Cosmological constraints on neutrino plus axion hot dark matter | We use observations of the cosmological large-scale structure to derive
limits on two-component hot dark matter consisting of mass-degenerate neutrinos
and hadronic axions, both components having velocity dispersions corresponding
to their respective decoupling temperatures. We restrict the data samples to
the safely... | astro-ph hep-ph | we use observations of the cosmological largescale structure to derive limits on twocomponent hot dark matter consisting of massdegenerate neutrinos and hadronic axions both components having velocity dispersions corresponding to their respective decoupling temperatures we restrict the data samples to the safely linear... | [['we', 'use', 'observations', 'of', 'the', 'cosmological', 'largescale', 'structure', 'to', 'derive', 'limits', 'on', 'twocomponent', 'hot', 'dark', 'matter', 'consisting', 'of', 'massdegenerate', 'neutrinos', 'and', 'hadronic', 'axions', 'both', 'components', 'having', 'velocity', 'dispersions', 'corresponding', 'to'... | [-0.10599098066349738, 0.18618942724424414, 0.01494369473597356, 0.11547451164846405, -0.09267716265909759, -0.06502795653369535, 0.1314294222292715, 0.3353687270769271, -0.15528134198995822, -0.37722050315090294, 0.05394863798624258, -0.28426279348536027, 0.0770513876000066, 0.20616504235658795, 0.0764643349724918, -0... |
706.4199 | Radial and vertical angular momentum transport in protostellar discs | Angular momentum in protostellar discs can be transported either radially,
through turbulence induced by the magnetorotational instability (MRI), or
vertically, through the torque exerted by a large-scale magnetic field. We
present a model of steady-state discs where these two mechanisms operate at the
same radius an... | astro-ph | angular momentum in protostellar discs can be transported either radially through turbulence induced by the magnetorotational instability mri or vertically through the torque exerted by a largescale magnetic field we present a model of steadystate discs where these two mechanisms operate at the same radius and derive a... | [['angular', 'momentum', 'in', 'protostellar', 'discs', 'can', 'be', 'transported', 'either', 'radially', 'through', 'turbulence', 'induced', 'by', 'the', 'magnetorotational', 'instability', 'mri', 'or', 'vertically', 'through', 'the', 'torque', 'exerted', 'by', 'a', 'largescale', 'magnetic', 'field', 'we', 'present', ... | [-0.15417247860628458, 0.13680369996402203, -0.06589607686117177, 0.05972344969854271, -0.07547324363725218, -0.07855873493093798, -0.018869014238256192, 0.38503526387210113, -0.2833556072868208, -0.27748450337294206, 0.09273592119179808, -0.1936395475227663, -0.08231505600536485, 0.2092604503188396, 0.0284064553450537... |
706.42 | Few body Calculation of Neutrino Neutral Inelastic scattering on 4He | The inelastic neutral reaction of neutrino on 4He is calculated using two
modern nucleon--nucleon potentials. Full final state interaction among the four
nucleons is considered, via the Lorentz integral transform (LIT) method. The
effective interaction hyperspherical-harmonic (EIHH) approach is used to solve
the resu... | nucl-th | the inelastic neutral reaction of neutrino on 4he is calculated using two modern nucleonnucleon potentials full final state interaction among the four nucleons is considered via the lorentz integral transform lit method the effective interaction hypersphericalharmonic eihh approach is used to solve the resulting schrod... | [['the', 'inelastic', 'neutral', 'reaction', 'of', 'neutrino', 'on', '4he', 'is', 'calculated', 'using', 'two', 'modern', 'nucleonnucleon', 'potentials', 'full', 'final', 'state', 'interaction', 'among', 'the', 'four', 'nucleons', 'is', 'considered', 'via', 'the', 'lorentz', 'integral', 'transform', 'lit', 'method', 't... | [-0.07157574786708273, 0.14651843200534068, -0.11834919193793682, 0.1567414792912916, -0.05695130663185284, -0.10720729159094908, -0.027816203567359983, 0.3336482777035442, -0.22356810751531658, -0.26030721065813095, -0.039755925995795506, -0.3350552132931249, -0.07484703828933938, 0.14703191592807657, 0.13913416559005... |
706.4201 | Tree Diagram Lie Algebras of Differential Operators and Evolution
Partial Differential Equations | A tree diagram is a tree with positive integral weight on each edge, which is
a notion generalized from the Dynkin diagrams of finite-dimensional simple Lie
algebras. We introduce two nilpotent Lie algebras and their extended solvable
Lie algebras associated with each tree diagram. The solvable tree diagram Lie
algeb... | math.RT math-ph math.AP math.MP nlin.SI | a tree diagram is a tree with positive integral weight on each edge which is a notion generalized from the dynkin diagrams of finitedimensional simple lie algebras we introduce two nilpotent lie algebras and their extended solvable lie algebras associated with each tree diagram the solvable tree diagram lie algebras tu... | [['a', 'tree', 'diagram', 'is', 'a', 'tree', 'with', 'positive', 'integral', 'weight', 'on', 'each', 'edge', 'which', 'is', 'a', 'notion', 'generalized', 'from', 'the', 'dynkin', 'diagrams', 'of', 'finitedimensional', 'simple', 'lie', 'algebras', 'we', 'introduce', 'two', 'nilpotent', 'lie', 'algebras', 'and', 'their',... | [-0.1890815851863387, 0.10553074246922205, -0.04795103543979484, 0.11748047281858014, -0.27009980215748786, -0.183334206238158, 0.011806821291760881, 0.35745034173362017, -0.40064725470404294, -0.16809002695561842, 0.1522873111661206, -0.22373302933009154, -0.13738672079359607, 0.1326379586343271, -0.0989334463961278, ... |
706.4202 | Coherence and Spatial Resolution of Transport in Quantum Cascade Lasers | The method of nonequilibrium Greens functions allows for a spatial and
energetical resolution of the electron current in Quantum Cascade Lasers. While
scattering does not change the spatial position of carriers, the entire spatial
evolution of charge can be attributed to coherent transport by complex wave
functions. ... | cond-mat.mes-hall | the method of nonequilibrium greens functions allows for a spatial and energetical resolution of the electron current in quantum cascade lasers while scattering does not change the spatial position of carriers the entire spatial evolution of charge can be attributed to coherent transport by complex wave functions we di... | [['the', 'method', 'of', 'nonequilibrium', 'greens', 'functions', 'allows', 'for', 'a', 'spatial', 'and', 'energetical', 'resolution', 'of', 'the', 'electron', 'current', 'in', 'quantum', 'cascade', 'lasers', 'while', 'scattering', 'does', 'not', 'change', 'the', 'spatial', 'position', 'of', 'carriers', 'the', 'entire'... | [-0.09867607586545078, 0.15513544992786155, -0.1081918497499691, 0.10050230785209226, 0.009630746425014653, -0.08797809455467209, 0.016680134391756602, 0.3593925611205297, -0.3069959594006969, -0.2663395357611653, 0.022821855790313487, -0.2428169512695853, -0.13549967431016777, 0.16122840633233115, 0.053820315550706564... |
706.4203 | Optimal curves of low genus over finite fields | The Hasse-Weil-Serre bound is improved for curves of low genera over finite
fields with discriminant in {-3,-4,-7,-8,-11,-19} by studying optimal curves.
| math.AG math.NT | the hasseweilserre bound is improved for curves of low genera over finite fields with discriminant in 34781119 by studying optimal curves | [['the', 'hasseweilserre', 'bound', 'is', 'improved', 'for', 'curves', 'of', 'low', 'genera', 'over', 'finite', 'fields', 'with', 'discriminant', 'in', '34781119', 'by', 'studying', 'optimal', 'curves']] | [-0.18555196693265125, 0.1463937017037288, -0.1894240403841985, 0.09755949816347934, -0.020983169406750483, -0.1628342659065598, 0.08780184231306377, 0.29205132393460526, -0.22620952093826704, -0.328716993724045, 0.10546627122982356, -0.24465803870637165, -0.0969697006144806, 0.3807394922907023, -0.1332342662897549, 0.... |
706.4204 | Investigation of Pygmy Dipole Resonances in the Tin Region | The evolution of the low-energy electromagnetic dipole response with the
neutron excess is investigated along the Sn isotopic chain within an approach
incorporating Hartree-Fock-Bogoljubov (HFB) and multi-phonon
Quasiparticle-Phonon-Model (QPM) theory. General aspects of the relationship of
nuclear skins and dipole s... | nucl-th | the evolution of the lowenergy electromagnetic dipole response with the neutron excess is investigated along the sn isotopic chain within an approach incorporating hartreefockbogoljubov hfb and multiphonon quasiparticlephononmodel qpm theory general aspects of the relationship of nuclear skins and dipole sum rules are ... | [['the', 'evolution', 'of', 'the', 'lowenergy', 'electromagnetic', 'dipole', 'response', 'with', 'the', 'neutron', 'excess', 'is', 'investigated', 'along', 'the', 'sn', 'isotopic', 'chain', 'within', 'an', 'approach', 'incorporating', 'hartreefockbogoljubov', 'hfb', 'and', 'multiphonon', 'quasiparticlephononmodel', 'qp... | [-0.07125378749610502, 0.18590491989544672, -0.04288420613383572, 0.11944112498063728, -0.028470751948632477, -0.07235733154604011, 0.03564340156333942, 0.3654352393877205, -0.17057605567831724, -0.26357459203462075, -0.059136421072513, -0.3111312126829511, -0.06750803878475424, 0.11653741040416728, 0.07103511385537872... |
706.4205 | The extended Burnside ring and module categories | In this note an `extended Burnside ring' is defined, generated by classes of
semisimple module categories over Rep(G) with quasifibre functors. Here G is a
finite group and representations are taken over an algebraically closed field
of characteristic 0. It is shown that this is equivalent to a ring generated by
cent... | math.RT | in this note an extended burnside ring is defined generated by classes of semisimple module categories over repg with quasifibre functors here g is a finite group and representations are taken over an algebraically closed field of characteristic 0 it is shown that this is equivalent to a ring generated by centrally ext... | [['in', 'this', 'note', 'an', 'extended', 'burnside', 'ring', 'is', 'defined', 'generated', 'by', 'classes', 'of', 'semisimple', 'module', 'categories', 'over', 'repg', 'with', 'quasifibre', 'functors', 'here', 'g', 'is', 'a', 'finite', 'group', 'and', 'representations', 'are', 'taken', 'over', 'an', 'algebraically', '... | [-0.2548624148481877, 0.006337269007009145, -0.1849055779724838, 0.06001460248347828, -0.11755817595926323, -0.13896067651245286, -0.2657551164216153, 0.14671867690286694, -0.2342175069355349, -0.24490576892454483, 0.05426600749238527, -0.3465294657341604, -0.18999438900357987, 0.16353767926832044, -0.35123273155091295... |
706.4206 | Calorons and dyons at the thermal phase transition analyzed by overlap
fermions | In a pilot study, we use the topological charge density defined by the
eigenmodes of the overlap Dirac operator (with ultraviolet filtering by
mode-truncation) to search for lumps of topological charge in SU(2) pure gauge
theory. Augmenting this search with periodic and antiperiodic temporal boundary
conditions for t... | hep-lat hep-ph | in a pilot study we use the topological charge density defined by the eigenmodes of the overlap dirac operator with ultraviolet filtering by modetruncation to search for lumps of topological charge in su2 pure gauge theory augmenting this search with periodic and antiperiodic temporal boundary conditions for the overla... | [['in', 'a', 'pilot', 'study', 'we', 'use', 'the', 'topological', 'charge', 'density', 'defined', 'by', 'the', 'eigenmodes', 'of', 'the', 'overlap', 'dirac', 'operator', 'with', 'ultraviolet', 'filtering', 'by', 'modetruncation', 'to', 'search', 'for', 'lumps', 'of', 'topological', 'charge', 'in', 'su2', 'pure', 'gauge... | [-0.15024514769232183, 0.23184749710684022, -0.08653509341123881, 0.08481811107220975, -0.028672915534821874, -0.11722792969649715, 0.04444481224089748, 0.39322303911727485, -0.15664649715816434, -0.28050199668064263, 0.09173563779543407, -0.277068568348433, -0.1331447695777046, 0.061658674769216416, -0.008497860063939... |
706.4207 | Complex weak values in quantum measurement | In the weak measurement formalism of Y. Aharonov et al. the so-called weak
value A_w of any observable A is generally a complex number. We derive a
physical interpretation of its value in terms of the shift in the measurement
pointer's mean position and mean momentum. In particular we show that the mean
position shif... | quant-ph | in the weak measurement formalism of y aharonov et al the socalled weak value a_w of any observable a is generally a complex number we derive a physical interpretation of its value in terms of the shift in the measurement pointers mean position and mean momentum in particular we show that the mean position shift contai... | [['in', 'the', 'weak', 'measurement', 'formalism', 'of', 'y', 'aharonov', 'et', 'al', 'the', 'socalled', 'weak', 'value', 'a_w', 'of', 'any', 'observable', 'a', 'is', 'generally', 'a', 'complex', 'number', 'we', 'derive', 'a', 'physical', 'interpretation', 'of', 'its', 'value', 'in', 'terms', 'of', 'the', 'shift', 'in'... | [-0.16577693643596242, 0.13675385633798534, -0.08770444877993534, 0.039649123128722694, -0.07214199797633816, -0.07436133977573584, 0.047466302542563746, 0.31515654954401884, -0.2934113383813597, -0.28564366435303407, 0.05609890685334583, -0.2719651468426866, -0.11713179712019423, 0.14449135913404035, -0.06124620298471... |
706.4208 | Penetration of Andreev bound states into the ferromagnet in a
SrRuO$_{3}$/(110)YBa$_2$Cu$_3$O$_{7-\delta}$ bilayer: a scanning tunneling
spectroscopy study | Scanning tunneling spectroscopy of thin epitaxial
$SrRuO_{3}/(110)YBa_2Cu_3O_{7-\delta}$ ferromagnet/superconductor bilayers,
reveal a clear penetration of the Andreev bound states into the ferromagnetic
layer. The penetration is manifested in the density of states of the
ferromagnet as a split zero bias conductance ... | cond-mat.supr-con | scanning tunneling spectroscopy of thin epitaxial srruo_3110yba_2cu_3o_7delta ferromagnetsuperconductor bilayers reveal a clear penetration of the andreev bound states into the ferromagnetic layer the penetration is manifested in the density of states of the ferromagnet as a split zero bias conductance peak with an imb... | [['scanning', 'tunneling', 'spectroscopy', 'of', 'thin', 'epitaxial', 'srruo_3110yba_2cu_3o_7delta', 'ferromagnetsuperconductor', 'bilayers', 'reveal', 'a', 'clear', 'penetration', 'of', 'the', 'andreev', 'bound', 'states', 'into', 'the', 'ferromagnetic', 'layer', 'the', 'penetration', 'is', 'manifested', 'in', 'the', ... | [-0.22467750904317468, 0.17941476213048027, -0.08440065921212618, 0.04699182122623405, -0.011314151128037618, -0.1398407040307155, 0.10647996842192534, 0.3393437356138841, -0.2822018694636287, -0.3089457305912406, -0.057358534746946625, -0.3412939698363726, -0.048032443188369654, 0.19859423411962313, 0.0620992009719021... |
706.4209 | Elastic relaxation during 2D epitaxial growth: a study of in-plane
lattice spacing oscillations | The purpose of this paper is to report some new experimental and theoretical
results about the analysis of in-plane lattice spacing oscillations during
two-dimensional (2D) homo and hetero epitaxial growth. The physical origin of
these oscillations comes from the finite size of the strained islands. The 2D
islands ma... | cond-mat.mtrl-sci | the purpose of this paper is to report some new experimental and theoretical results about the analysis of inplane lattice spacing oscillations during twodimensional 2d homo and hetero epitaxial growth the physical origin of these oscillations comes from the finite size of the strained islands the 2d islands may thus r... | [['the', 'purpose', 'of', 'this', 'paper', 'is', 'to', 'report', 'some', 'new', 'experimental', 'and', 'theoretical', 'results', 'about', 'the', 'analysis', 'of', 'inplane', 'lattice', 'spacing', 'oscillations', 'during', 'twodimensional', '2d', 'homo', 'and', 'hetero', 'epitaxial', 'growth', 'the', 'physical', 'origin... | [-0.15180378694200727, 0.2293302582555154, -0.08091783243690046, 0.01699949670370271, -0.009918207184501409, -0.07181697778833963, 0.06300789085252277, 0.3714154607067972, -0.28659633663364775, -0.28355658600262845, 0.0778640428088785, -0.2962677718617665, -0.12765941807886746, 0.18336204151849872, 0.028262125025621525... |
706.421 | Automorphic Forms and Reeb-Like Foliations on Three-Manifolds | In this paper, we consider different ways of generating dynamical systems on
3-manifolds. We first derive explicit differential equations for dynamical
systems defined on generic hyperbolic 3-manifolds by using automorphic function
theory to uniformize the upper half-space model. It is achieved via the
modification o... | math.DS | in this paper we consider different ways of generating dynamical systems on 3manifolds we first derive explicit differential equations for dynamical systems defined on generic hyperbolic 3manifolds by using automorphic function theory to uniformize the upper halfspace model it is achieved via the modification of the st... | [['in', 'this', 'paper', 'we', 'consider', 'different', 'ways', 'of', 'generating', 'dynamical', 'systems', 'on', '3manifolds', 'we', 'first', 'derive', 'explicit', 'differential', 'equations', 'for', 'dynamical', 'systems', 'defined', 'on', 'generic', 'hyperbolic', '3manifolds', 'by', 'using', 'automorphic', 'function... | [-0.17002956877418218, 0.07822005985570805, -0.11494959677081733, 0.08507972945947023, -0.057635398971892536, -0.1267430494439655, 0.00859069630414957, 0.31412639523900693, -0.2908958068893602, -0.2710658099236233, 0.10662162671353491, -0.26446671961762364, -0.19390617047791325, 0.19954591384379283, -0.0840526595359690... |
706.4211 | The formation of a detached shell around the carbon star Y CVn | Y CVn is a carbon star surrounded by a detached dust shell that has been
imaged by the Infrared Space Observatory at 90 microns. With the Nancay Radio
Telescope we have studied the gaseous counterpart in the 21-cm HI emission
line. New data have been acquired and allow to improve the signal to noise
ratio on this lin... | astro-ph | y cvn is a carbon star surrounded by a detached dust shell that has been imaged by the infrared space observatory at 90 microns with the nancay radio telescope we have studied the gaseous counterpart in the 21cm hi emission line new data have been acquired and allow to improve the signal to noise ratio on this line the... | [['y', 'cvn', 'is', 'a', 'carbon', 'star', 'surrounded', 'by', 'a', 'detached', 'dust', 'shell', 'that', 'has', 'been', 'imaged', 'by', 'the', 'infrared', 'space', 'observatory', 'at', '90', 'microns', 'with', 'the', 'nancay', 'radio', 'telescope', 'we', 'have', 'studied', 'the', 'gaseous', 'counterpart', 'in', 'the', ... | [-0.0825267552240686, 0.10802601185866642, -0.04022388461042936, 0.024547305301223624, -0.05367767048748927, -0.07095211674160777, 0.053534589357859194, 0.412111793895467, -0.20326686171420777, -0.35434355144985974, 0.08355777321804243, -0.2880513122367213, 0.025112891021238353, 0.15239779957091043, -0.0103263632227959... |
706.4212 | Shear Viscosity to Entropy within a Parton Cascade | The shear viscosity is calculated by means of the perturbative kinetic
partonic cascade BAMPS with CGC initial conditons for various saturation
momentum scale Q_s. eta/s ~ 0.15 stays approximately constant when going from
RHIC to LHC.
| hep-ph | the shear viscosity is calculated by means of the perturbative kinetic partonic cascade bamps with cgc initial conditons for various saturation momentum scale q_s etas 015 stays approximately constant when going from rhic to lhc | [['the', 'shear', 'viscosity', 'is', 'calculated', 'by', 'means', 'of', 'the', 'perturbative', 'kinetic', 'partonic', 'cascade', 'bamps', 'with', 'cgc', 'initial', 'conditons', 'for', 'various', 'saturation', 'momentum', 'scale', 'q_s', 'etas', '015', 'stays', 'approximately', 'constant', 'when', 'going', 'from', 'rhic... | [-0.07423757372473899, 0.3747712003865412, -0.22792284303743923, 0.12245323957675802, -0.007745345632013466, -0.06875149124035877, -0.11543875916727951, 0.294018665594714, -0.2977444760767477, -0.22424797067152602, -0.04458459002364959, -0.3098902357476098, 0.18145546311778682, 0.09333150019603116, 0.11693866501695344,... |
706.4213 | Magneto-optic far-infrared study of Sr$_{14}$Cu$_{24}$O$_{41}$: triplet
excitations in chains | Using far-infrared spectroscopy we have studied the magnetic field and
temperature dependence of the spin gap modes in the chains of
Sr$_{14}$Cu$_{24}$O$_{41}$. Two triplet modes T$_1$ and T$_2$ were found in the
center of the Brillouin zone at $\Delta_1=9.65$ meV and $\Delta_2=10.86$ meV in
zero magnetic field. The ... | cond-mat.other | using farinfrared spectroscopy we have studied the magnetic field and temperature dependence of the spin gap modes in the chains of sr_14cu_24o_41 two triplet modes t_1 and t_2 were found in the center of the brillouin zone at delta_1965 mev and delta_21086 mev in zero magnetic field the t_1 mode was excited when the e... | [['using', 'farinfrared', 'spectroscopy', 'we', 'have', 'studied', 'the', 'magnetic', 'field', 'and', 'temperature', 'dependence', 'of', 'the', 'spin', 'gap', 'modes', 'in', 'the', 'chains', 'of', 'sr_14cu_24o_41', 'two', 'triplet', 'modes', 't_1', 'and', 't_2', 'were', 'found', 'in', 'the', 'center', 'of', 'the', 'bri... | [-0.14215522223852703, 0.23054668238499942, 0.0035701118942955113, -0.028692279416972246, -0.0335180249157696, -0.07350190294186115, 0.09521448012823477, 0.4153133938009413, -0.21560851075292492, -0.3082771846252438, -0.006503979875467336, -0.3323307591530248, -0.003096791489734354, 0.18296591272780624, 0.0622330826297... |
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