id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
706.4414 | Decay modes of $^{10}$C nuclei unbound state | Unbound states of $^{10}$C nuclei produced as quasi-projectiles in
$^{12}$C+$^{24}$Mg collisions at E/A = 53 and 95 MeV are studied with the Indra
detector array. Multi-particle correlation function analyses provide
experimental evidence of sequential de-excitation mechanisms through the
production of intermediate $^... | nucl-ex | unbound states of 10c nuclei produced as quasiprojectiles in 12c24mg collisions at ea 53 and 95 mev are studied with the indra detector array multiparticle correlation function analyses provide experimental evidence of sequential deexcitation mechanisms through the production of intermediate 9b 6be and 8be unbound nucl... | [['unbound', 'states', 'of', '10c', 'nuclei', 'produced', 'as', 'quasiprojectiles', 'in', '12c24mg', 'collisions', 'at', 'ea', '53', 'and', '95', 'mev', 'are', 'studied', 'with', 'the', 'indra', 'detector', 'array', 'multiparticle', 'correlation', 'function', 'analyses', 'provide', 'experimental', 'evidence', 'of', 'se... | [-0.04374831828144601, 0.2305078718068433, -0.13960376355542048, 0.21906264483723567, 0.06912101461057318, -0.10830885632839497, 0.04022360399054984, 0.34580622724301757, -0.19045403445627362, -0.321192938335506, -0.05261578432068096, -0.36340471005089403, 0.05675960953036944, 0.14656014183059424, 0.1502556553653752, 0... |
706.4415 | Labyrinthine pathways towards supercycle attractors in unimodal maps | We uncover previously unknown properties of the family of periodic
superstable cycles in unimodal maps characterized each by a Lyapunov exponent
that diverges to minus infinity. Amongst the main novel properties are the
following: i) The basins of attraction for the phases of the cycles develop
fractal boundaries of ... | cond-mat.stat-mech nlin.CD | we uncover previously unknown properties of the family of periodic superstable cycles in unimodal maps characterized each by a lyapunov exponent that diverges to minus infinity amongst the main novel properties are the following i the basins of attraction for the phases of the cycles develop fractal boundaries of incre... | [['we', 'uncover', 'previously', 'unknown', 'properties', 'of', 'the', 'family', 'of', 'periodic', 'superstable', 'cycles', 'in', 'unimodal', 'maps', 'characterized', 'each', 'by', 'a', 'lyapunov', 'exponent', 'that', 'diverges', 'to', 'minus', 'infinity', 'amongst', 'the', 'main', 'novel', 'properties', 'are', 'the', ... | [-0.18040501794858296, 0.14447574836168192, -0.1233462430421769, 0.06660736284799368, -0.01904999215283753, -0.11050607921141717, 0.06274848658861708, 0.31169276405700747, -0.3191365532028736, -0.21298171460404303, 0.1024363201009512, -0.2649014454541935, -0.19270616875283053, 0.14156927948495673, -0.03187706416337065,... |
706.4416 | Population III star formation in a Lambda CDM universe, II: Effects of a
photodissociating background | We examine aspects of primordial star formation in the presence of a
molecular hydrogen-dissociating ultraviolet background. We compare a set of AMR
hydrodynamic cosmological simulations using a single cosmological realization
but with a range of ultraviolet background strengths in the Lyman-Werner band.
This allows ... | astro-ph | we examine aspects of primordial star formation in the presence of a molecular hydrogendissociating ultraviolet background we compare a set of amr hydrodynamic cosmological simulations using a single cosmological realization but with a range of ultraviolet background strengths in the lymanwerner band this allows us to ... | [['we', 'examine', 'aspects', 'of', 'primordial', 'star', 'formation', 'in', 'the', 'presence', 'of', 'a', 'molecular', 'hydrogendissociating', 'ultraviolet', 'background', 'we', 'compare', 'a', 'set', 'of', 'amr', 'hydrodynamic', 'cosmological', 'simulations', 'using', 'a', 'single', 'cosmological', 'realization', 'bu... | [-0.09069631852464141, 0.15655955231023982, -0.008130250354605484, 0.06880664442174847, 0.002825128507948977, -0.014708637067837938, 0.056556616789762815, 0.3686768382258626, -0.1477617697544751, -0.34634343196242934, 0.03716234731893798, -0.2554623544450459, -0.0073647298696106625, 0.15231023400755606, 0.0280597237321... |
706.4417 | Some Two Color, Four Variable Rado Numbers | There exists a minimum integer $N$ such that any 2-coloring of
$\{1,2,...,N\}$ admits a monochromatic solution to $x+y+kz =\ell w$ for $k,\ell
\in \mathbb{Z}^+$, where $N$ depends on $k$ and $\ell$. We determine $N$ when
$\ell-k \in \{0,1,2,3,4,5\}$, for all $k,\ell$ for which
${1/2}((\ell-k)^2-2)(\ell-k+1)\leq k \le... | math.CO | there exists a minimum integer n such that any 2coloring of 12n admits a monochromatic solution to xykz ell w for kell in mathbbz where n depends on k and ell we determine n when ellk in 012345 for all kell for which 12ellk22ellk1leq k leq ell4 as well as for arbitrary k when ell2 | [['there', 'exists', 'a', 'minimum', 'integer', 'n', 'such', 'that', 'any', '2coloring', 'of', '12n', 'admits', 'a', 'monochromatic', 'solution', 'to', 'xykz', 'ell', 'w', 'for', 'kell', 'in', 'mathbbz', 'where', 'n', 'depends', 'on', 'k', 'and', 'ell', 'we', 'determine', 'n', 'when', 'ellk', 'in', '012345', 'for', 'al... | [-0.23078851401805878, 0.23613176587969065, 0.026010954071982548, -0.011516467238274904, -0.0042681266876080865, -0.27433001330623835, 0.06547990504903002, 0.34366887794861284, -0.2430828768007744, -0.2957535039346952, 0.05163376192257811, -0.3549106697050425, -0.04905042696583013, 0.16247087699146226, 0.05409711292192... |
706.4418 | Fermi surface pockets in ortho-II YBa$_2$Cu$_3$O$_{6.5}$: the origin of
quantum oscillations? | In this paper we explore whether the quantum oscillation signals recently
observed in ortho-II YBa$_2$Cu$_3$O$_{6.5}$ may be explained by conventional
density functional band-structure theory. Our calculations show that the Fermi
surface of YBa$_2$Cu$_3$O$_{6.5}$ is extremely sensitive to small shifts in the
relative... | cond-mat.supr-con cond-mat.str-el | in this paper we explore whether the quantum oscillation signals recently observed in orthoii yba_2cu_3o_65 may be explained by conventional density functional bandstructure theory our calculations show that the fermi surface of yba_2cu_3o_65 is extremely sensitive to small shifts in the relative positions of the bands... | [['in', 'this', 'paper', 'we', 'explore', 'whether', 'the', 'quantum', 'oscillation', 'signals', 'recently', 'observed', 'in', 'orthoii', 'yba_2cu_3o_65', 'may', 'be', 'explained', 'by', 'conventional', 'density', 'functional', 'bandstructure', 'theory', 'our', 'calculations', 'show', 'that', 'the', 'fermi', 'surface',... | [-0.16507149783593386, 0.19920592586335847, -0.04942028620515508, 0.08947210932018781, -0.0009406434217434979, -0.07972095927430524, 0.1269831477518598, 0.38318541331799943, -0.2654509038165814, -0.3087571537441979, -0.008788264528236757, -0.35286078394174275, -0.1459220503127635, 0.19944981352727145, -0.04931143052273... |
706.4419 | Fossil AGN jets as ultra high energy particle accelerators | Remnants of AGN jets and their surrounding cocoons leave colossal
magnetohydrodynamic (MHD) fossil structures storing total energies ~10^{60}
erg. The original active galacic nucleus (AGN) may be dead but the fossil will
retain its stable configuration resembling the reversed-field pinch (RFP)
encountered in laborato... | astro-ph | remnants of agn jets and their surrounding cocoons leave colossal magnetohydrodynamic mhd fossil structures storing total energies 1060 erg the original active galacic nucleus agn may be dead but the fossil will retain its stable configuration resembling the reversedfield pinch rfp encountered in laboratory mhd experim... | [['remnants', 'of', 'agn', 'jets', 'and', 'their', 'surrounding', 'cocoons', 'leave', 'colossal', 'magnetohydrodynamic', 'mhd', 'fossil', 'structures', 'storing', 'total', 'energies', '1060', 'erg', 'the', 'original', 'active', 'galacic', 'nucleus', 'agn', 'may', 'be', 'dead', 'but', 'the', 'fossil', 'will', 'retain', ... | [-0.10834873680191083, 0.2867569267579356, -0.04783412875036385, 0.15770470257996486, -0.09498535115094224, -0.045327810751140056, -0.012503656933805066, 0.39806935342297084, -0.25457590581628226, -0.3437355693421816, 0.03775828860264066, -0.30639881433048916, -0.0071145510596965075, 0.21798153712327387, 0.015892241422... |
706.442 | Bounds on Van der Waerden Numbers and Some Related Functions | For positive integers $s$ and $k_1, k_2, ..., k_s$, let $w(k_1,k_2,...,k_s)$
be the minimum integer $n$ such that any $s$-coloring $\{1,2,...,n\} \to
\{1,2,...,s\}$ admits a $k_i$-term arithmetic progression of color $i$ for some
$i$, $1 \leq i \leq s$. In the case when $k_1=k_2=...=k_s=k$ we simply write
$w(k;s)$.
... | math.CO | for positive integers s and k_1 k_2 k_s let wk_1k_2k_s be the minimum integer n such that any scoloring 12n to 12s admits a k_iterm arithmetic progression of color i for some i 1 leq i leq s in the case when k_1k_2k_sk we simply write wks that such a minimum integer exists follows from van der waerdens theorem on arith... | [['for', 'positive', 'integers', 's', 'and', 'k_1', 'k_2', 'k_s', 'let', 'wk_1k_2k_s', 'be', 'the', 'minimum', 'integer', 'n', 'such', 'that', 'any', 'scoloring', '12n', 'to', '12s', 'admits', 'a', 'k_iterm', 'arithmetic', 'progression', 'of', 'color', 'i', 'for', 'some', 'i', '1', 'leq', 'i', 'leq', 's', 'in', 'the', ... | [-0.18450729127013774, 0.1668780205455374, -0.06288037895534547, 0.05936003435018585, -0.02924481961015386, -0.21871700836345553, 0.09660299908225142, 0.2940051186058995, -0.21911624909350366, -0.321011523980732, 0.04521653925555504, -0.333527337131796, -0.12944325353336436, 0.22813271649118344, -0.04647145212176397, -... |
706.4421 | A presentation for Hilden's subgroup of the braid group | Consider the unit ball, B = D x [0,1], containing n unknotted arcs a_1, ...
a_n such that the boundary of each a_i lies in D x {0}. We give a finite
presentation for the mapping class group of B fixing the arcs {a_1, ..., a_n}
setwise and fixing D x {1} pointwise. This presentation is calculated using the
action of t... | math.GR | consider the unit ball b d x 01 containing n unknotted arcs a_1 a_n such that the boundary of each a_i lies in d x 0 we give a finite presentation for the mapping class group of b fixing the arcs a_1 a_n setwise and fixing d x 1 pointwise this presentation is calculated using the action of this group on a simplyconnect... | [['consider', 'the', 'unit', 'ball', 'b', 'd', 'x', '01', 'containing', 'n', 'unknotted', 'arcs', 'a_1', 'a_n', 'such', 'that', 'the', 'boundary', 'of', 'each', 'a_i', 'lies', 'in', 'd', 'x', '0', 'we', 'give', 'a', 'finite', 'presentation', 'for', 'the', 'mapping', 'class', 'group', 'of', 'b', 'fixing', 'the', 'arcs',... | [-0.27228524067322724, 0.1358580894448096, -0.022169433039380237, -0.04644431381348113, -0.042000599427410634, -0.23356245398463216, 0.0658132083772216, 0.3802575177978724, -0.3163815684383735, -0.14100157955545, 0.07660192495131923, -0.3130515195662156, -0.051530761124013225, 0.07826177280367119, -0.062432588420051616... |
706.4422 | Dynamics towards the Feigenbaum attractor | We expose at a previously unknown level of detail the features of the
dynamics of trajectories that either evolve towards the Feigenbaum attractor or
are captured by its matching repellor. Amongst these features are the
following: i) The set of preimages of the attractor and of the repellor are
embedded (dense) into ... | cond-mat.stat-mech nlin.CD | we expose at a previously unknown level of detail the features of the dynamics of trajectories that either evolve towards the feigenbaum attractor or are captured by its matching repellor amongst these features are the following i the set of preimages of the attractor and of the repellor are embedded dense into each ot... | [['we', 'expose', 'at', 'a', 'previously', 'unknown', 'level', 'of', 'detail', 'the', 'features', 'of', 'the', 'dynamics', 'of', 'trajectories', 'that', 'either', 'evolve', 'towards', 'the', 'feigenbaum', 'attractor', 'or', 'are', 'captured', 'by', 'its', 'matching', 'repellor', 'amongst', 'these', 'features', 'are', '... | [-0.16058200129307806, 0.113868513429843, -0.09360082997241989, 0.044125108641455885, -0.006968982872786, -0.095308210196672, 0.04315624285489321, 0.3295170127227902, -0.31696855316869915, -0.27347356018493885, 0.10488766741356813, -0.2868079148745164, -0.11480747671914288, 0.15189706604927777, -0.03686414887133651, 0.... |
706.4423 | Tuning Kinetic Magnetism of Strongly Correlated Electrons via Staggered
Flux | We explore the kinetic magnetism of the infinite-$U$ repulsive Hubbard models
at low hole densities on various lattices with nearest-neighbor hopping
integrals modulated by a staggered magnetic flux $\pm\phi$. Tuning $\phi$ from
0 to $\pi$ makes the ground state (GS) change from a Nagaoka-type ferromagnetic
state to ... | cond-mat.str-el cond-mat.stat-mech | we explore the kinetic magnetism of the infiniteu repulsive hubbard models at low hole densities on various lattices with nearestneighbor hopping integrals modulated by a staggered magnetic flux pmphi tuning phi from 0 to pi makes the ground state gs change from a nagaokatype ferromagnetic state to a haertershastrytype... | [['we', 'explore', 'the', 'kinetic', 'magnetism', 'of', 'the', 'infiniteu', 'repulsive', 'hubbard', 'models', 'at', 'low', 'hole', 'densities', 'on', 'various', 'lattices', 'with', 'nearestneighbor', 'hopping', 'integrals', 'modulated', 'by', 'a', 'staggered', 'magnetic', 'flux', 'pmphi', 'tuning', 'phi', 'from', '0', ... | [-0.20507094597345904, 0.28165861687770016, -0.0016284406969421788, 0.11079541410956728, -0.030479767166176126, -0.18523631926724002, 0.0742364038541717, 0.3787322455428933, -0.2607324430179831, -0.26848955829382726, 0.042743258353469794, -0.35598086463777645, -0.06956538654631003, 0.0941885836201867, 0.122695042364495... |
706.4424 | Steps toward a classifier for the Virtual Observatory. I. Classifying
the SDSS photometric archive | Modern photometric multiband digital surveys produce large amounts of data
that, in order to be effectively exploited, need automatic tools capable to
extract from photometric data an objective classification. We present here a
new method for classifying objects in large multi-parametric photometric data
bases, consi... | astro-ph | modern photometric multiband digital surveys produce large amounts of data that in order to be effectively exploited need automatic tools capable to extract from photometric data an objective classification we present here a new method for classifying objects in large multiparametric photometric data bases consisting o... | [['modern', 'photometric', 'multiband', 'digital', 'surveys', 'produce', 'large', 'amounts', 'of', 'data', 'that', 'in', 'order', 'to', 'be', 'effectively', 'exploited', 'need', 'automatic', 'tools', 'capable', 'to', 'extract', 'from', 'photometric', 'data', 'an', 'objective', 'classification', 'we', 'present', 'here',... | [-0.03363257622803821, -0.021188128411669695, -0.11244538655981075, 0.07260704461246902, -0.14711432465417093, -0.0545252354187501, 0.057126036441754985, 0.36435880492506334, -0.273668919841564, -0.36020335637379525, 0.14526344040073022, -0.2972272699103193, -0.14162341225350839, 0.2977457511087143, -0.0872764061259235... |
706.4425 | A simple model of Coulomb disorder and screening in graphene | We suggest a simple model of disorder in graphene assuming that there are
randomly distributed positive and negative centers with equal concentration
$N/2$ in the bulk of silicon oxide substrate. We show that at zero gate voltage
such disorder creates two-dimensional concentration $n_0 \sim N^{2/3}$ of
electrons and ... | cond-mat.mes-hall cond-mat.dis-nn | we suggest a simple model of disorder in graphene assuming that there are randomly distributed positive and negative centers with equal concentration n2 in the bulk of silicon oxide substrate we show that at zero gate voltage such disorder creates twodimensional concentration n_0 sim n23 of electrons and holes in graph... | [['we', 'suggest', 'a', 'simple', 'model', 'of', 'disorder', 'in', 'graphene', 'assuming', 'that', 'there', 'are', 'randomly', 'distributed', 'positive', 'and', 'negative', 'centers', 'with', 'equal', 'concentration', 'n2', 'in', 'the', 'bulk', 'of', 'silicon', 'oxide', 'substrate', 'we', 'show', 'that', 'at', 'zero', ... | [-0.16967985473872563, 0.24287447463055806, 0.03953776930436669, -0.0037672963170778183, 0.10790859268135614, -0.25060851407414747, 0.06760160331170828, 0.4247014436072537, -0.19235460925847292, -0.29799141987626043, -0.0366796757443808, -0.41121345668632003, -0.09891306347812392, 0.15712140886933498, -0.01126225855356... |
706.4426 | Be stars and binaries in the field of the SMC open cluster NGC330 with
VLT-FLAMES | Observations of hot stars belonging to the young cluster SMC-NGC330 and its
surrounding region were obtained with the VLT-GIRAFFE facilities in MEDUSA
mode. We investigated the B and Be star properties and proportions in this
environment of low metallicity. We also searched for rapid variability in Be
stars using pho... | astro-ph | observations of hot stars belonging to the young cluster smcngc330 and its surrounding region were obtained with the vltgiraffe facilities in medusa mode we investigated the b and be star properties and proportions in this environment of low metallicity we also searched for rapid variability in be stars using photometr... | [['observations', 'of', 'hot', 'stars', 'belonging', 'to', 'the', 'young', 'cluster', 'smcngc330', 'and', 'its', 'surrounding', 'region', 'were', 'obtained', 'with', 'the', 'vltgiraffe', 'facilities', 'in', 'medusa', 'mode', 'we', 'investigated', 'the', 'b', 'and', 'be', 'star', 'properties', 'and', 'proportions', 'in'... | [-0.05200386391903095, 0.1397534680919365, -0.06824731561008524, 0.08679777393650086, -0.10475160678021332, -0.03457014097217867, 0.1148241674143603, 0.4586193015838557, -0.16850320122977522, -0.3661476692724775, 0.08382681719562475, -0.32005617823132854, -0.03181638349679873, 0.22518143633707485, -0.07881673423841501,... |
706.4427 | Growing neutrinos and cosmological selection | The time evolution of a cosmological scalar field can be stopped by an
increasing mass of the neutrinos. This leads to a transition from a
cosmological scaling solution with dynamical dark energy at early time to a
cosmological constant dominated universe at late time. The trigger for the
transition is set at the tim... | hep-ph | the time evolution of a cosmological scalar field can be stopped by an increasing mass of the neutrinos this leads to a transition from a cosmological scaling solution with dynamical dark energy at early time to a cosmological constant dominated universe at late time the trigger for the transition is set at the time wh... | [['the', 'time', 'evolution', 'of', 'a', 'cosmological', 'scalar', 'field', 'can', 'be', 'stopped', 'by', 'an', 'increasing', 'mass', 'of', 'the', 'neutrinos', 'this', 'leads', 'to', 'a', 'transition', 'from', 'a', 'cosmological', 'scaling', 'solution', 'with', 'dynamical', 'dark', 'energy', 'at', 'early', 'time', 'to'... | [-0.1121348432265222, 0.2574312409508275, -0.09627979701384902, 0.14530136907473207, -0.06721450433880091, -0.11381702165771276, -0.008372843682765961, 0.2904664095879998, -0.24190232610050588, -0.35409941120445726, 0.06551090066414327, -0.23112452852725981, 0.01115952868014574, 0.16219970680214466, 0.058026626303792, ... |
706.4428 | Semi-analytical approach to magnetized temperature autocorrelations | The cosmic microwave background (CMB) temperature autocorrelations, induced
by a magnetized adiabatic mode of curvature inhomogeneities, are computed with
semi-analytical methods. As suggested by the latest CMB data, a nearly
scale-invariant spectrum for the adiabatic mode is consistently assumed. In
this situation, ... | astro-ph gr-qc hep-ph hep-th | the cosmic microwave background cmb temperature autocorrelations induced by a magnetized adiabatic mode of curvature inhomogeneities are computed with semianalytical methods as suggested by the latest cmb data a nearly scaleinvariant spectrum for the adiabatic mode is consistently assumed in this situation the effects ... | [['the', 'cosmic', 'microwave', 'background', 'cmb', 'temperature', 'autocorrelations', 'induced', 'by', 'a', 'magnetized', 'adiabatic', 'mode', 'of', 'curvature', 'inhomogeneities', 'are', 'computed', 'with', 'semianalytical', 'methods', 'as', 'suggested', 'by', 'the', 'latest', 'cmb', 'data', 'a', 'nearly', 'scaleinv... | [-0.14268781098229957, 0.21863475204439325, -0.0456903079909843, 0.08988123520396904, -0.07770001634721356, -0.05890947682856148, -0.030104786284384927, 0.366818997379958, -0.22734896620706269, -0.31223174130192993, 0.07949186787643124, -0.2640470805689473, -0.03410111426946302, 0.2245546778937051, 0.04156309815979421,... |
706.4429 | Observation of B^0 \to D^{*-} \tau^+ \nu_{\tau} decay at Belle | We report an observation of the decay $B^0\to D^{*-} \tau^+ \nu_{\tau}$ in a
data sample containing $535\times10^6$ $B\bar{B}$ pairs collected with the
Belle detector at the KEKB asymmetric-energy $e^+e^-$ collider. We find a
signal with a significance of 5.2 standard deviations and measure the branching
fraction $\m... | hep-ex | we report an observation of the decay b0to d tau nu_tau in a data sample containing 535times106 bbarb pairs collected with the belle detector at the kekb asymmetricenergy ee collider we find a signal with a significance of 52 standard deviations and measure the branching fraction mathcalbb0to d tau nu_tau202 040_037 st... | [['we', 'report', 'an', 'observation', 'of', 'the', 'decay', 'b0to', 'd', 'tau', 'nu_tau', 'in', 'a', 'data', 'sample', 'containing', '535times106', 'bbarb', 'pairs', 'collected', 'with', 'the', 'belle', 'detector', 'at', 'the', 'kekb', 'asymmetricenergy', 'ee', 'collider', 'we', 'find', 'a', 'signal', 'with', 'a', 'si... | [-0.13377023727890835, 0.17895392266343282, -0.07443808359093965, 0.026791584711255773, -0.028213550512945013, -0.1622705758682319, 0.10239304293811853, 0.2624944371836526, -0.17277313406978334, -0.2606062924755471, -0.059181812234289415, -0.47338860018977097, 0.0801285766730351, 0.10542953025350081, 0.0853278431243130... |
706.443 | Investigating the extended geometric scaling region at LHC with
polarized and unpolarized final states | We present predictions for charged hadron production and Lambda polarization
in p-p and p-Pb collisions at the LHC using the saturation inspired DHJ model
for the dipole cross section in the extended geometric scaling region.
| hep-ph | we present predictions for charged hadron production and lambda polarization in pp and ppb collisions at the lhc using the saturation inspired dhj model for the dipole cross section in the extended geometric scaling region | [['we', 'present', 'predictions', 'for', 'charged', 'hadron', 'production', 'and', 'lambda', 'polarization', 'in', 'pp', 'and', 'ppb', 'collisions', 'at', 'the', 'lhc', 'using', 'the', 'saturation', 'inspired', 'dhj', 'model', 'for', 'the', 'dipole', 'cross', 'section', 'in', 'the', 'extended', 'geometric', 'scaling', ... | [-0.004768651258200407, 0.17766025526715176, -0.13062327738319124, 0.14055895975657873, 0.05435633494385651, -0.1014155276119709, -0.08997184493845063, 0.2964997184263276, -0.193287265087877, -0.25195108811770167, -0.07622288725604968, -0.36072273669498306, 0.07027629259973764, 0.11644096437708608, 0.11789674535975792,... |
706.4431 | The Einstein static universe in Loop Quantum Cosmology | Loop Quantum Cosmology strongly modifies the high-energy dynamics of
Friedman-Robertson-Walker models and removes the big-bang singularity. We
investigate how LQC corrections affect the stability properties of the Einstein
static universe. In General Relativity, the Einstein static model with positive
cosmological co... | gr-qc astro-ph hep-th | loop quantum cosmology strongly modifies the highenergy dynamics of friedmanrobertsonwalker models and removes the bigbang singularity we investigate how lqc corrections affect the stability properties of the einstein static universe in general relativity the einstein static model with positive cosmological constant la... | [['loop', 'quantum', 'cosmology', 'strongly', 'modifies', 'the', 'highenergy', 'dynamics', 'of', 'friedmanrobertsonwalker', 'models', 'and', 'removes', 'the', 'bigbang', 'singularity', 'we', 'investigate', 'how', 'lqc', 'corrections', 'affect', 'the', 'stability', 'properties', 'of', 'the', 'einstein', 'static', 'unive... | [-0.18423592824655682, 0.1382838931323877, -0.14918734083202348, 0.1555709455165762, -0.10691260957895819, -0.20167310939017516, -0.09370651365424604, 0.27692285007032663, -0.22667234011494847, -0.21744356935482417, 0.04315310807502481, -0.26755727960992215, -0.0834697581021421, 0.11745308097382423, -0.0224360526928594... |
706.4432 | The minority game: An economics perspective | This paper gives a critical account of the minority game literature. The
minority game is a simple congestion game: players need to choose between two
options, and those who have selected the option chosen by the minority win. The
learning model proposed in this literature seems to differ markedly from the
learning m... | q-fin.GN physics.soc-ph | this paper gives a critical account of the minority game literature the minority game is a simple congestion game players need to choose between two options and those who have selected the option chosen by the minority win the learning model proposed in this literature seems to differ markedly from the learning models ... | [['this', 'paper', 'gives', 'a', 'critical', 'account', 'of', 'the', 'minority', 'game', 'literature', 'the', 'minority', 'game', 'is', 'a', 'simple', 'congestion', 'game', 'players', 'need', 'to', 'choose', 'between', 'two', 'options', 'and', 'those', 'who', 'have', 'selected', 'the', 'option', 'chosen', 'by', 'the', ... | [0.022329399641603232, 0.03531625956296921, -0.12140973256528377, 0.12201586719881743, -0.07872984765470029, -0.23497771365195513, 0.09458761371020227, 0.39695874594151975, -0.26424833087343724, -0.3487067951688077, 0.026513706598430872, -0.30594631616026163, -0.17540403143316508, 0.12791322688758372, -0.16750640886090... |
706.4433 | Relaxation dynamics of a quantum Brownian particle in an ideal gas | We show how the quantum analog of the Fokker-Planck equation for describing
Brownian motion can be obtained as the diffusive limit of the quantum linear
Boltzmann equation. The latter describes the quantum dynamics of a tracer
particle in a dilute, ideal gas by means of a translation-covariant master
equation. We dis... | quant-ph | we show how the quantum analog of the fokkerplanck equation for describing brownian motion can be obtained as the diffusive limit of the quantum linear boltzmann equation the latter describes the quantum dynamics of a tracer particle in a dilute ideal gas by means of a translationcovariant master equation we discuss th... | [['we', 'show', 'how', 'the', 'quantum', 'analog', 'of', 'the', 'fokkerplanck', 'equation', 'for', 'describing', 'brownian', 'motion', 'can', 'be', 'obtained', 'as', 'the', 'diffusive', 'limit', 'of', 'the', 'quantum', 'linear', 'boltzmann', 'equation', 'the', 'latter', 'describes', 'the', 'quantum', 'dynamics', 'of', ... | [-0.10181045098219442, 0.10991537727453966, -0.10455029299386691, 0.06540454261379373, -0.05783789897740809, -0.11377454134779647, -4.9079204285421325e-05, 0.2568378616484439, -0.2956283281151609, -0.23397767612321743, 0.04456749662502486, -0.2718021947909723, -0.13310278318438334, 0.2118158386024099, 0.041168909342287... |
706.4434 | Pairing of 1D Bose-Fermi mixtures with unequal masses | We have considered one-dimensional Bose-Fermi mixture with equal densities
and unequal masses using numerical density matrix renormalization group (DMRG).
For the mass ratio of K-Rb mixture and attraction between bosons and fermions,
we determined the phase diagram. For weak boson-boson interactions, there is a
direc... | cond-mat.str-el cond-mat.other | we have considered onedimensional bosefermi mixture with equal densities and unequal masses using numerical density matrix renormalization group dmrg for the mass ratio of krb mixture and attraction between bosons and fermions we determined the phase diagram for weak bosonboson interactions there is a direct transition... | [['we', 'have', 'considered', 'onedimensional', 'bosefermi', 'mixture', 'with', 'equal', 'densities', 'and', 'unequal', 'masses', 'using', 'numerical', 'density', 'matrix', 'renormalization', 'group', 'dmrg', 'for', 'the', 'mass', 'ratio', 'of', 'krb', 'mixture', 'and', 'attraction', 'between', 'bosons', 'and', 'fermio... | [-0.16796811867677264, 0.2870639321115776, -0.08773124725194734, 0.11656875193969202, 0.022395767758540606, -0.20436816260543303, 0.0784312515998037, 0.37588256814542714, -0.2021725867199925, -0.2638315352602699, 0.006888293635544427, -0.29250237505472854, -0.11003184320251329, 0.06165816456245295, 0.10702716734755886,... |
706.4435 | Discovery of Very High Energy gamma-rays from 1ES 1011+496 at z=0.212 | We report on the discovery of Very High Energy (VHE) gamma-ray emission from
the BL Lacertae object 1ES1011+496. The observation was triggered by an optical
outburst in March 2007 and the source was observed with the MAGIC telescope
from March to May 2007. Observing for 18.7 hr we find an excess of 6.2 sigma
with an ... | astro-ph | we report on the discovery of very high energy vhe gammaray emission from the bl lacertae object 1es1011496 the observation was triggered by an optical outburst in march 2007 and the source was observed with the magic telescope from march to may 2007 observing for 187 hr we find an excess of 62 sigma with an integrated... | [['we', 'report', 'on', 'the', 'discovery', 'of', 'very', 'high', 'energy', 'vhe', 'gammaray', 'emission', 'from', 'the', 'bl', 'lacertae', 'object', '1es1011496', 'the', 'observation', 'was', 'triggered', 'by', 'an', 'optical', 'outburst', 'in', 'march', '2007', 'and', 'the', 'source', 'was', 'observed', 'with', 'the'... | [-0.04074055311459124, 0.1486339864248403, -0.04006247632415559, 0.09194261947457671, -0.11695874132271997, -0.09204606713002365, 0.04893038847616741, 0.4912953571157348, -0.12093188510192349, -0.43001163557619976, 0.030621500325186134, -0.3403521925841171, 0.03245574341302639, 0.2517980731589566, -0.03965274428010435,... |
706.4436 | On the moment limit of quantum observables, with an application to the
balanced homodyne detection | We consider the moment operators of the observable (i.e. a semispectral
measure or POM) associated with the balanced homodyne detection statistics,
with paying attention to the correct domains of these unbounded operators. We
show that the high amplitude limit, when performed on the moment operators,
actually determi... | quant-ph | we consider the moment operators of the observable ie a semispectral measure or pom associated with the balanced homodyne detection statistics with paying attention to the correct domains of these unbounded operators we show that the high amplitude limit when performed on the moment operators actually determines unique... | [['we', 'consider', 'the', 'moment', 'operators', 'of', 'the', 'observable', 'ie', 'a', 'semispectral', 'measure', 'or', 'pom', 'associated', 'with', 'the', 'balanced', 'homodyne', 'detection', 'statistics', 'with', 'paying', 'attention', 'to', 'the', 'correct', 'domains', 'of', 'these', 'unbounded', 'operators', 'we',... | [-0.14085082331470278, 0.15209328379018833, -0.08727201536450555, 0.07593762489016015, -0.026947443579229964, -0.10136777491224978, 0.07845060847004846, 0.3333094901806877, -0.2530810168387477, -0.2374282463320664, 0.11378568915770976, -0.25970856338325476, -0.11900312535553462, 0.18686288086791084, -0.0450606916103482... |
706.4437 | Gravitational waves from inspiralling compact binaries: hexagonal
template placement and its efficiency in detecting physical signals | Matched filtering is used to search for gravitational waves emitted by
inspiralling compact binaries in data from the ground-based interferometers.
One of the key aspects of the detection process is the design of a template
bank that covers the astrophysically pertinent parameter space. In an earlier
paper, we descri... | gr-qc | matched filtering is used to search for gravitational waves emitted by inspiralling compact binaries in data from the groundbased interferometers one of the key aspects of the detection process is the design of a template bank that covers the astrophysically pertinent parameter space in an earlier paper we described a ... | [['matched', 'filtering', 'is', 'used', 'to', 'search', 'for', 'gravitational', 'waves', 'emitted', 'by', 'inspiralling', 'compact', 'binaries', 'in', 'data', 'from', 'the', 'groundbased', 'interferometers', 'one', 'of', 'the', 'key', 'aspects', 'of', 'the', 'detection', 'process', 'is', 'the', 'design', 'of', 'a', 'te... | [-0.1019992618346654, 0.043390354200536115, -0.059461239977514485, 0.09168244163613665, -0.10716160751260576, -0.09446921843858032, 0.04001289703135147, 0.40994072070056137, -0.18190515655452646, -0.3226085951165565, 0.12717366741679353, -0.2853347051750855, -0.15336016808982791, 0.24639415946311657, -0.030888906187488... |
706.4438 | Non-Markovian quantum jumps | Open quantum systems that interact with structured reservoirs exhibit
non-Markovian dynamics. We present a quantum jump method for treating the
dynamics of such systems. This approach is a generalization of the standard
Monte Carlo Wave Function (MCWF) method for Markovian dynamics. The MCWF method
identifies decay r... | quant-ph | open quantum systems that interact with structured reservoirs exhibit nonmarkovian dynamics we present a quantum jump method for treating the dynamics of such systems this approach is a generalization of the standard monte carlo wave function mcwf method for markovian dynamics the mcwf method identifies decay rates wit... | [['open', 'quantum', 'systems', 'that', 'interact', 'with', 'structured', 'reservoirs', 'exhibit', 'nonmarkovian', 'dynamics', 'we', 'present', 'a', 'quantum', 'jump', 'method', 'for', 'treating', 'the', 'dynamics', 'of', 'such', 'systems', 'this', 'approach', 'is', 'a', 'generalization', 'of', 'the', 'standard', 'mont... | [-0.11682292956393212, 0.13901931092423184, -0.12065728795714677, 0.10703639816929353, 0.016253004624741153, -0.21014794126385822, 0.04764911303063855, 0.36123046088032423, -0.29901332248700785, -0.20656279856339096, 0.02718606318521779, -0.25207594151142987, -0.17273301706882194, 0.2482708182069473, 0.0129294487007427... |
706.4439 | AGN Observations in the GeV/TeV Energy Range with the MAGIC Telescope | MAGIC currently is the largest imaging atmospheric Cerenkov telescope
world-wide. Since 2004, gamma-ray emission from several active galactic nuclei
in the GeV/TeV energy range has been detected, some of which were newly
discovered as very-high energy gamma-ray sources. The gamma-rays are assumed to
originate from pa... | astro-ph | magic currently is the largest imaging atmospheric cerenkov telescope worldwide since 2004 gammaray emission from several active galactic nuclei in the gevtev energy range has been detected some of which were newly discovered as veryhigh energy gammaray sources the gammarays are assumed to originate from particle accel... | [['magic', 'currently', 'is', 'the', 'largest', 'imaging', 'atmospheric', 'cerenkov', 'telescope', 'worldwide', 'since', '2004', 'gammaray', 'emission', 'from', 'several', 'active', 'galactic', 'nuclei', 'in', 'the', 'gevtev', 'energy', 'range', 'has', 'been', 'detected', 'some', 'of', 'which', 'were', 'newly', 'discov... | [-0.019737880965812676, 0.20585660544637432, -0.02700632823560434, 0.20718788296202362, -0.11734709357017581, -0.07102043672075754, -0.016936457651089643, 0.4567998662308047, -0.179438739673152, -0.4141815238031028, 0.08174276420599015, -0.32676543224650095, -0.014471449752196764, 0.25332932301083744, 0.027912093055304... |
706.444 | 2-State 3-Symbol Universal Turing Machines Do Not Exist | In this brief note, we give a simple information-theoretic proof that 2-state
3-symbol universal Turing machines cannot possibly exist, unless one loosens
the definition of "universal".
| cs.OH | in this brief note we give a simple informationtheoretic proof that 2state 3symbol universal turing machines cannot possibly exist unless one loosens the definition of universal | [['in', 'this', 'brief', 'note', 'we', 'give', 'a', 'simple', 'informationtheoretic', 'proof', 'that', '2state', '3symbol', 'universal', 'turing', 'machines', 'can', 'not', 'possibly', 'exist', 'unless', 'one', 'loosens', 'the', 'definition', 'of', 'universal']] | [-0.17511923838820723, 0.17524999659508467, -0.17545916312546642, 0.11165429014902285, -0.1655970721471089, -0.2808861775082295, 0.09789560586903934, 0.2765958428520847, -0.30480055407517487, -0.18437794388996231, 0.06441846289413257, -0.13033470249286405, -0.2039805397529293, 0.22018297596110237, -0.18996358859456247,... |
706.4441 | Free $n$-distributions: holonomy, sub-Riemannian structures, Fefferman
constructions and dual distributions | This paper analyses the parabolic geometries generated by a free
$n$-distribution in the tangent space of a manifold. It shows that certain
holonomy reductions of the associated normal Tractor connections, imply
preferred connections with special properties, along with Riemannian or
sub-Riemannian structures on the m... | math.DG math.AP math.MG | this paper analyses the parabolic geometries generated by a free ndistribution in the tangent space of a manifold it shows that certain holonomy reductions of the associated normal tractor connections imply preferred connections with special properties along with riemannian or subriemannian structures on the manifold i... | [['this', 'paper', 'analyses', 'the', 'parabolic', 'geometries', 'generated', 'by', 'a', 'free', 'ndistribution', 'in', 'the', 'tangent', 'space', 'of', 'a', 'manifold', 'it', 'shows', 'that', 'certain', 'holonomy', 'reductions', 'of', 'the', 'associated', 'normal', 'tractor', 'connections', 'imply', 'preferred', 'conn... | [-0.1619620780252571, 0.08336659368620372, -0.03410330779163293, 0.09818727011765235, -0.12685722649296366, -0.13697550658281277, -0.02485127279250114, 0.40028134049865804, -0.26483146559664056, -0.23448691292421767, 0.09820114660700693, -0.2662983037174218, -0.20442381734706605, 0.2150987411229826, -0.1280106828701727... |
706.4442 | A First Synoptic Blazar Study Comprising Thirteen Blazars Visible in
E>100 GeV Gamma-Rays | Since 2002, the number of detected blazars at E_\gamma > 100 GeV has more
than doubled. I study all currently known BL Lac-type objects with published
energy spectra. Their intrinsic energy spectra are reconstructed by removing
extragalactic background light attenuation effects. The emission properties are
then compa... | astro-ph | since 2002 the number of detected blazars at e_gamma 100 gev has more than doubled i study all currently known bl lactype objects with published energy spectra their intrinsic energy spectra are reconstructed by removing extragalactic background light attenuation effects the emission properties are then compared and co... | [['since', '2002', 'the', 'number', 'of', 'detected', 'blazars', 'at', 'e_gamma', '100', 'gev', 'has', 'more', 'than', 'doubled', 'i', 'study', 'all', 'currently', 'known', 'bl', 'lactype', 'objects', 'with', 'published', 'energy', 'spectra', 'their', 'intrinsic', 'energy', 'spectra', 'are', 'reconstructed', 'by', 'rem... | [-0.044452783691828694, 0.13714647129903326, -0.012908048804157076, 0.18516941559789454, -0.0962091782047883, -0.12960745474999458, 0.02227487209648619, 0.4383705813042094, -0.15248314589385636, -0.4258898285060989, 0.059929335587740405, -0.3494222294725941, 0.025612572883873915, 0.21624161934776776, -0.022777991023211... |
706.4443 | Thermal Dileptons at LHC | We predict dilepton invariant-mass spectra for central 5.5 ATeV Pb-Pb
collisions at LHC. Hadronic emission in the low-mass region is calculated using
in-medium spectral functions of light vector mesons within hadronic many-body
theory. In the intermediate-mass region thermal radiation from the Quark-Gluon
Plasma, eva... | hep-ph nucl-ex nucl-th | we predict dilepton invariantmass spectra for central 55 atev pbpb collisions at lhc hadronic emission in the lowmass region is calculated using inmedium spectral functions of light vector mesons within hadronic manybody theory in the intermediatemass region thermal radiation from the quarkgluon plasma evaluated pertur... | [['we', 'predict', 'dilepton', 'invariantmass', 'spectra', 'for', 'central', '55', 'atev', 'pbpb', 'collisions', 'at', 'lhc', 'hadronic', 'emission', 'in', 'the', 'lowmass', 'region', 'is', 'calculated', 'using', 'inmedium', 'spectral', 'functions', 'of', 'light', 'vector', 'mesons', 'within', 'hadronic', 'manybody', '... | [-0.005780903014729356, 0.2867831264083144, -0.1603683582234934, 0.18354973397459592, 0.021726974503850784, -0.08144395794211463, -0.04849090867421844, 0.34568355892869557, -0.15182280616665428, -0.22425623492083765, -0.1164659914989992, -0.3793570270955369, 0.13576543568210167, 0.12675168742607165, 0.10299092232682076... |
706.4444 | Automatic Active-Region Identification and Azimuth Disambiguation of the
SOLIS/VSM Full-Disk Vector Magnetograms | The Vector Spectromagnetograph (VSM) of the NSO's Synoptic Optical Long-Term
Investigations of the Sun (SOLIS) facility is now operational and obtains the
first-ever vector magnetic field measurements of the entire visible solar
hemisphere. To fully exploit the unprecedented SOLIS/VSM data, however, one
must first ad... | astro-ph | the vector spectromagnetograph vsm of the nsos synoptic optical longterm investigations of the sun solis facility is now operational and obtains the firstever vector magnetic field measurements of the entire visible solar hemisphere to fully exploit the unprecedented solisvsm data however one must first address two cri... | [['the', 'vector', 'spectromagnetograph', 'vsm', 'of', 'the', 'nsos', 'synoptic', 'optical', 'longterm', 'investigations', 'of', 'the', 'sun', 'solis', 'facility', 'is', 'now', 'operational', 'and', 'obtains', 'the', 'firstever', 'vector', 'magnetic', 'field', 'measurements', 'of', 'the', 'entire', 'visible', 'solar', ... | [-0.09636126119647906, 0.12056438068537048, -0.034394825087722646, 0.06256985064856618, -0.12665390047026379, -0.056666201797122374, 0.012760874899950895, 0.43045061156064557, -0.2271688129779611, -0.339737222291547, 0.1098035170460503, -0.23792786178352873, -0.1148332703761694, 0.22742202630574018, -0.0299992335753617... |
706.4445 | Random Fiber Laser | We investigate the effects of two dimensional confinement on the lasing
properties of a classical random laser system operating in the incoherent
feedback (diffusive) regime. A suspension of 250nm rutile (TiO2) particles in a
Rhodamine 6G solution was inserted into the hollow core of a photonic crystal
fiber (PCF) ge... | physics.optics | we investigate the effects of two dimensional confinement on the lasing properties of a classical random laser system operating in the incoherent feedback diffusive regime a suspension of 250nm rutile tio2 particles in a rhodamine 6g solution was inserted into the hollow core of a photonic crystal fiber pcf generating ... | [['we', 'investigate', 'the', 'effects', 'of', 'two', 'dimensional', 'confinement', 'on', 'the', 'lasing', 'properties', 'of', 'a', 'classical', 'random', 'laser', 'system', 'operating', 'in', 'the', 'incoherent', 'feedback', 'diffusive', 'regime', 'a', 'suspension', 'of', '250nm', 'rutile', 'tio2', 'particles', 'in', ... | [-0.16039674045236477, 0.18299357553684764, -0.07686154342927905, -0.05152221415922869, 0.019128465201965598, -0.16759222175731042, 0.02247427238238066, 0.46196223622144655, -0.22684380825782238, -0.19087369547653293, 0.025434807936530992, -0.2820038450232079, -0.11472192670077865, 0.2108640437404257, -0.02002195199290... |
706.4446 | An optimization problem with volume constrain in Orlicz spaces | We consider the optimization problem of minimizing $\int_{\Omega}G(|\nabla
u|) dx$ in the class of functions $W^{1,G}(\Omega)$, with a constrain on the
volume of $\{u>0\}$. The conditions on the function $G$ allow for a different
behavior at
0 and at $\infty$. We consider a penalization problem, and we prove that f... | math.AP | we consider the optimization problem of minimizing int_omegagnabla u dx in the class of functions w1gomega with a constrain on the volume of u0 the conditions on the function g allow for a different behavior at 0 and at infty we consider a penalization problem and we prove that for small values of the penalization para... | [['we', 'consider', 'the', 'optimization', 'problem', 'of', 'minimizing', 'int_omegagnabla', 'u', 'dx', 'in', 'the', 'class', 'of', 'functions', 'w1gomega', 'with', 'a', 'constrain', 'on', 'the', 'volume', 'of', 'u0', 'the', 'conditions', 'on', 'the', 'function', 'g', 'allow', 'for', 'a', 'different', 'behavior', 'at',... | [-0.15914025937672704, 0.0690315178129822, -0.06022626796038821, 0.03116406718327198, -0.040565741420141424, -0.1268571348453406, 0.04137990271556191, 0.36720082983374597, -0.3481932050315663, -0.19542193657252938, 0.12925160423037596, -0.28991378443315624, -0.08919948320835829, 0.1675629758145078, -0.08406026359880343... |
706.4447 | Pure motives, mixed motives and extensions of motives associated to
singular surfaces | We first recall the construction of the Chow motive modelling intersection
cohomology of a proper surface and study its fundamental properties. Using
Voevodsky's category of effective geometrical motives, we then study the motive
of the exceptional divisor in a non-singular blow-up. If all geometric
irreducible compo... | math.KT math.AG | we first recall the construction of the chow motive modelling intersection cohomology of a proper surface and study its fundamental properties using voevodskys category of effective geometrical motives we then study the motive of the exceptional divisor in a nonsingular blowup if all geometric irreducible components of... | [['we', 'first', 'recall', 'the', 'construction', 'of', 'the', 'chow', 'motive', 'modelling', 'intersection', 'cohomology', 'of', 'a', 'proper', 'surface', 'and', 'study', 'its', 'fundamental', 'properties', 'using', 'voevodskys', 'category', 'of', 'effective', 'geometrical', 'motives', 'we', 'then', 'study', 'the', 'm... | [-0.22007199423387647, 0.001870749139925465, -0.22123054882589108, 0.0511469502428857, -0.13837463916570414, -0.11185564300588642, -0.0006555515622797733, 0.2703385627440487, -0.3405547331397732, -0.17214270080633773, 0.06634668778254611, -0.1681013957545474, -0.19041179224344282, 0.18993272366545474, -0.23657905490836... |
706.4448 | Search for Anomalous Production of Multilepton Events in p-pbar
Collisions at sqrt(s) = 1.96 TeV | We report a search for the anomalous production of events with multiple
charged leptons in p-pbar collisions at sqrt{s} = 1.96 TeV using a data sample
corresponding to an integrated luminosity of 346 pb^{-1} collected by the CDF
II detector at the Fermilab Tevatron. The search is divided into three-lepton
and four-or... | hep-ex | we report a search for the anomalous production of events with multiple charged leptons in ppbar collisions at sqrts 196 tev using a data sample corresponding to an integrated luminosity of 346 pb1 collected by the cdf ii detector at the fermilab tevatron the search is divided into threelepton and fourormorelepton data... | [['we', 'report', 'a', 'search', 'for', 'the', 'anomalous', 'production', 'of', 'events', 'with', 'multiple', 'charged', 'leptons', 'in', 'ppbar', 'collisions', 'at', 'sqrts', '196', 'tev', 'using', 'a', 'data', 'sample', 'corresponding', 'to', 'an', 'integrated', 'luminosity', 'of', '346', 'pb1', 'collected', 'by', 't... | [-0.050767025405851506, 0.2080605008763307, -0.03756009241227399, 0.15192401224472138, -0.018072226673900856, -0.09685140940939274, 0.05924678179017616, 0.3267689058257295, -0.12862945935745357, -0.4179524020856303, 0.025333835955913826, -0.40772406659512356, 0.11408342583330744, 0.16817048030718457, 0.0622794609640329... |
706.4449 | Cheeger constants of surfaces and isoperimetric inequalities | We show that the Cheeger constant of compact surfaces is bounded by a
function of the area. We apply this to isoperimetric profiles of bounded genus
non-compact surfaces, to show that if their isoperimetric profile grows faster
than $\sqrt t$, then it grows at least as fast as a linear function. This
generalizes a re... | math.DG math.GR math.GT math.MG | we show that the cheeger constant of compact surfaces is bounded by a function of the area we apply this to isoperimetric profiles of bounded genus noncompact surfaces to show that if their isoperimetric profile grows faster than sqrt t then it grows at least as fast as a linear function this generalizes a result of gr... | [['we', 'show', 'that', 'the', 'cheeger', 'constant', 'of', 'compact', 'surfaces', 'is', 'bounded', 'by', 'a', 'function', 'of', 'the', 'area', 'we', 'apply', 'this', 'to', 'isoperimetric', 'profiles', 'of', 'bounded', 'genus', 'noncompact', 'surfaces', 'to', 'show', 'that', 'if', 'their', 'isoperimetric', 'profile', '... | [-0.1345185710826015, 0.13833502208632706, -0.06414433079977742, 0.07286198633265542, -0.04149742057316203, -0.16038316735519773, -0.006188121879786517, 0.36608046087213847, -0.26988571230425146, -0.2618676770882335, 0.12999395421083884, -0.3157125844710828, -0.18462527900588063, 0.1814442383026523, -0.1124545292582659... |
706.445 | Quadratic optimal functional quantization of stochastic processes and
numerical applications | In this paper, we present an overview of the recent developments of
functional quantization of stochastic processes, with an emphasis on the
quadratic case. Functional quantization is a way to approximate a process,
viewed as a Hilbert-valued random variable, using a nearest neighbour
projection on a finite codebook.... | math.PR | in this paper we present an overview of the recent developments of functional quantization of stochastic processes with an emphasis on the quadratic case functional quantization is a way to approximate a process viewed as a hilbertvalued random variable using a nearest neighbour projection on a finite codebook a specia... | [['in', 'this', 'paper', 'we', 'present', 'an', 'overview', 'of', 'the', 'recent', 'developments', 'of', 'functional', 'quantization', 'of', 'stochastic', 'processes', 'with', 'an', 'emphasis', 'on', 'the', 'quadratic', 'case', 'functional', 'quantization', 'is', 'a', 'way', 'to', 'approximate', 'a', 'process', 'viewed... | [-0.13538595532466258, 0.015214994659930068, -0.08872691968988095, 0.08199761387422769, -0.12040008522037948, -0.09315898978550519, 0.09470359384847273, 0.38827528868402755, -0.26792174210505826, -0.18932770964290416, 0.17588089248498104, -0.2557079737307504, -0.18939230191920484, 0.19007722457338658, -0.10501550111387... |
706.4451 | Turbulence models generator | In this paper we explore a possibility that all transport turbulent models
are contained in a coarse-grained kinetic equation. Building on a recent work
by H.Chen et al (2004), we account for fluctuations of a single -point
probability density in turbulence, by introducing a``two-level'' (${\bf
c,v}$)-phase-space, se... | nlin.CG physics.flu-dyn | in this paper we explore a possibility that all transport turbulent models are contained in a coarsegrained kinetic equation building on a recent work by hchen et al 2004 we account for fluctuations of a single point probability density in turbulence by introducing atwolevel bf cvphasespace separating microscopic bf ce... | [['in', 'this', 'paper', 'we', 'explore', 'a', 'possibility', 'that', 'all', 'transport', 'turbulent', 'models', 'are', 'contained', 'in', 'a', 'coarsegrained', 'kinetic', 'equation', 'building', 'on', 'a', 'recent', 'work', 'by', 'hchen', 'et', 'al', '2004', 'we', 'account', 'for', 'fluctuations', 'of', 'a', 'single',... | [-0.13468640072671914, 0.1455543170322503, -0.06857868718784736, 0.03442495155316063, -0.02105028764209385, -0.07075130650069737, -0.003617893346736944, 0.27365050789748513, -0.26249698933950344, -0.2964488618823072, 0.005578840016739356, -0.24854007227411276, -0.10299624046743956, 0.17576691818553522, -0.0135475189890... |
706.4452 | What is the Mathematical Structure of Quantum Spacetime? | We survey indications from different branches of Physics that the fine scale
structure of spacetime is not adequately described by a manifold. Based on the
hints we accumulate, we propose a new structure, which we call a quantum topos.
In the process of constructing a quantum topos for quantum gravity, we propose
a n... | gr-qc | we survey indications from different branches of physics that the fine scale structure of spacetime is not adequately described by a manifold based on the hints we accumulate we propose a new structure which we call a quantum topos in the process of constructing a quantum topos for quantum gravity we propose a new oper... | [['we', 'survey', 'indications', 'from', 'different', 'branches', 'of', 'physics', 'that', 'the', 'fine', 'scale', 'structure', 'of', 'spacetime', 'is', 'not', 'adequately', 'described', 'by', 'a', 'manifold', 'based', 'on', 'the', 'hints', 'we', 'accumulate', 'we', 'propose', 'a', 'new', 'structure', 'which', 'we', 'c... | [-0.11394609807978702, 0.11661337130950598, -0.17075145697291894, 0.08314545699509905, -0.11210820535079966, -0.12436997653810378, 0.07389728123280868, 0.30701398548870523, -0.2819078060079224, -0.2790229294119002, 0.04529136156109221, -0.20727936366478664, -0.18148258085586602, 0.17153142772237712, -0.1003186509390420... |
706.4453 | Systematic search for VHE gamma-ray emission from X-ray bright
high-frequency BL Lac objects | All but three (M87, BL Lac and 3C 279) extragalactic sources detected so far
at very high energy (VHE) gamma-rays belong to the class of high-frequency
peaked BL Lac (HBL) objects. This suggested to us a systematic scan of
candidate sources with the MAGIC telescope, based on the compilation of X-ray
blazars by Donato... | astro-ph | all but three m87 bl lac and 3c 279 extragalactic sources detected so far at very high energy vhe gammarays belong to the class of highfrequency peaked bl lac hbl objects this suggested to us a systematic scan of candidate sources with the magic telescope based on the compilation of xray blazars by donato et al 2001 th... | [['all', 'but', 'three', 'm87', 'bl', 'lac', 'and', '3c', '279', 'extragalactic', 'sources', 'detected', 'so', 'far', 'at', 'very', 'high', 'energy', 'vhe', 'gammarays', 'belong', 'to', 'the', 'class', 'of', 'highfrequency', 'peaked', 'bl', 'lac', 'hbl', 'objects', 'this', 'suggested', 'to', 'us', 'a', 'systematic', 's... | [-0.003251018974636794, 0.14986738011685674, -0.015286050031161432, 0.1687210351115924, -0.13023131646483388, -0.12378533608336517, 0.07677889595881336, 0.4990869199657316, -0.10145074371804377, -0.4565425943389896, 0.028485898446302962, -0.3490103632421152, 0.08360596727837638, 0.23510201170071346, -0.0182454561025941... |
706.4454 | Synchronization in networks of networks: the onset of coherent
collective behavior in systems of interacting populations of heterogeneous
oscillators | The onset of synchronization in networks of networks is investigated.
Specifically, we consider networks of interacting phase oscillators in which
the set of oscillators is composed of several distinct populations. The
oscillators in a given population are heterogeneous in that their natural
frequencies are drawn fro... | math.DS | the onset of synchronization in networks of networks is investigated specifically we consider networks of interacting phase oscillators in which the set of oscillators is composed of several distinct populations the oscillators in a given population are heterogeneous in that their natural frequencies are drawn from a g... | [['the', 'onset', 'of', 'synchronization', 'in', 'networks', 'of', 'networks', 'is', 'investigated', 'specifically', 'we', 'consider', 'networks', 'of', 'interacting', 'phase', 'oscillators', 'in', 'which', 'the', 'set', 'of', 'oscillators', 'is', 'composed', 'of', 'several', 'distinct', 'populations', 'the', 'oscillat... | [-0.16703558539572572, 0.1788546165617715, -0.035904311535081695, 0.020635057500164422, -0.010875286867043801, -0.1442935002568577, 0.0499608924263157, 0.3908345110980528, -0.24057312666804398, -0.2687949347176722, 0.04896910602858822, -0.30198187677721894, -0.19533669504536583, 0.17055089883922067, -0.0146702908944072... |
706.4455 | Anomalous metallic state of Cu$_{0.07}$TiSe$_2$: an optical spectroscopy
study | We report an optical spectroscopy study on the newly discovered
superconductor Cu$_{0.07}$TiSe$_2$. Consistent with the development from a
semimetal or semiconductor with a very small indirect energy gap upon doping
TiSe$_2$, it is found that the compound has a low carrier density. Most
remarkably, the study reveals ... | cond-mat.supr-con cond-mat.str-el | we report an optical spectroscopy study on the newly discovered superconductor cu_007tise_2 consistent with the development from a semimetal or semiconductor with a very small indirect energy gap upon doping tise_2 it is found that the compound has a low carrier density most remarkably the study reveals a substantial s... | [['we', 'report', 'an', 'optical', 'spectroscopy', 'study', 'on', 'the', 'newly', 'discovered', 'superconductor', 'cu_007tise_2', 'consistent', 'with', 'the', 'development', 'from', 'a', 'semimetal', 'or', 'semiconductor', 'with', 'a', 'very', 'small', 'indirect', 'energy', 'gap', 'upon', 'doping', 'tise_2', 'it', 'is'... | [-0.1554735622984931, 0.20755407024387182, -0.06047975648232181, 0.007031178108952714, -0.02510711395727339, -0.13876249013242847, 0.1474731161860006, 0.3868699228071203, -0.22734723844673635, -0.327093055095486, 0.027995818955447487, -0.3208368923185826, -0.11453983319260067, 0.15708778955446875, -0.012070599126673187... |
706.4456 | Heavy-Quark Kinetics in the QGP at LHC | We present predictions for the nuclear modification factor and elliptic flow
of D and B mesons, as well as of their decay electrons, in semicentral Pb-Pb
collisions at the LHC. Heavy quarks are propagated in a Quark-Gluon Plasma
using a relativistic Langevin simulation with drag and diffusion coefficients
from elasti... | hep-ph nucl-ex nucl-th | we present predictions for the nuclear modification factor and elliptic flow of d and b mesons as well as of their decay electrons in semicentral pbpb collisions at the lhc heavy quarks are propagated in a quarkgluon plasma using a relativistic langevin simulation with drag and diffusion coefficients from elastic inter... | [['we', 'present', 'predictions', 'for', 'the', 'nuclear', 'modification', 'factor', 'and', 'elliptic', 'flow', 'of', 'd', 'and', 'b', 'mesons', 'as', 'well', 'as', 'of', 'their', 'decay', 'electrons', 'in', 'semicentral', 'pbpb', 'collisions', 'at', 'the', 'lhc', 'heavy', 'quarks', 'are', 'propagated', 'in', 'a', 'qua... | [-0.04043496973879103, 0.3054473220636802, -0.18434509385260753, 0.09415436245866918, 0.009473168557243688, -0.14529794048784034, -0.043756888291266345, 0.3562023529516799, -0.22184533561979022, -0.23189700892461199, -0.07640172632278076, -0.391515324291374, 0.08903293480231826, 0.11451800792544548, 0.12009045193969671... |
706.4457 | Dissipation Scale Fluctuations and Chemical Reaction Rates in Turbulent
Flows | Small separation between reactants, not exceeding $10^{-8}-10^{-7}cm$, is the
necessary condition for various chemical reactions. It is shown that random
advection and stretching by turbulence leads to formation of scalar-enriched
sheets of {\it strongly fluctuating thickness} $\eta_{c}$. The molecular-level
mixing i... | nlin.CD astro-ph physics.flu-dyn | small separation between reactants not exceeding 108107cm is the necessary condition for various chemical reactions it is shown that random advection and stretching by turbulence leads to formation of scalarenriched sheets of it strongly fluctuating thickness eta_c the molecularlevel mixing is achieved by diffusion acr... | [['small', 'separation', 'between', 'reactants', 'not', 'exceeding', '108107cm', 'is', 'the', 'necessary', 'condition', 'for', 'various', 'chemical', 'reactions', 'it', 'is', 'shown', 'that', 'random', 'advection', 'and', 'stretching', 'by', 'turbulence', 'leads', 'to', 'formation', 'of', 'scalarenriched', 'sheets', 'o... | [-0.13589498463934704, 0.24593414181121018, -0.04193987392250504, 0.0506981728023349, 0.01035921031664779, -0.11146267879330345, 0.04588233820621425, 0.31243896309230756, -0.2531230393849285, -0.26675115363088564, -0.010375170514974465, -0.2610760222314231, -0.09512517313340874, 0.13890160951909344, 0.01477460739890864... |
706.4458 | The Popescu-Gabriel theorem for triangulated categories | The Popescu-Gabriel theorem states that each Grothendieck abelian category is
a localization of a module category. In this paper, we prove an analogue where
Grothendieck abelian categories are replaced by triangulated categories which
are well generated (in the sense of Neeman) and algebraic (in the sense of
Keller).... | math.KT | the popescugabriel theorem states that each grothendieck abelian category is a localization of a module category in this paper we prove an analogue where grothendieck abelian categories are replaced by triangulated categories which are well generated in the sense of neeman and algebraic in the sense of keller the role ... | [['the', 'popescugabriel', 'theorem', 'states', 'that', 'each', 'grothendieck', 'abelian', 'category', 'is', 'a', 'localization', 'of', 'a', 'module', 'category', 'in', 'this', 'paper', 'we', 'prove', 'an', 'analogue', 'where', 'grothendieck', 'abelian', 'categories', 'are', 'replaced', 'by', 'triangulated', 'categorie... | [-0.14178767393490202, 0.030990758926475934, -0.08583552378082746, 0.100434527298938, -0.041868710418623924, -0.1373584901387068, -0.09270735313092653, 0.34396907858746617, -0.3938828504791385, -0.22456600227834364, 0.0770754462282639, -0.17767082350818733, -0.14874610698193705, 0.1754603453813807, -0.27494121331868593... |
706.4459 | A note on the stability for Kawahara-KdV type equations | In this paper we establish the nonlinear stability of solitary traveling-wave
solutions for the Kawahara-KdV equation $$u_t+uu_x+u_{xxx}-\gamma_1
u_{xxxxx}=0,$$ and the modified Kawahara-KdV equation
$$u_t+3u^2u_x+u_{xxx}-\gamma_2 u_{xxxxx}=0,$$ where $\gamma_i\in\mathbb{R}$ is
a positive number when $i=1,2$. The mai... | math.AP | in this paper we establish the nonlinear stability of solitary travelingwave solutions for the kawaharakdv equation u_tuu_xu_xxxgamma_1 u_xxxxx0 and the modified kawaharakdv equation u_t3u2u_xu_xxxgamma_2 u_xxxxx0 where gamma_iinmathbbr is a positive number when i12 the main approach used to determine the stability of ... | [['in', 'this', 'paper', 'we', 'establish', 'the', 'nonlinear', 'stability', 'of', 'solitary', 'travelingwave', 'solutions', 'for', 'the', 'kawaharakdv', 'equation', 'u_tuu_xu_xxxgamma_1', 'u_xxxxx0', 'and', 'the', 'modified', 'kawaharakdv', 'equation', 'u_t3u2u_xu_xxxgamma_2', 'u_xxxxx0', 'where', 'gamma_iinmathbbr', ... | [-0.13012800654608078, 0.0753121529282494, -0.10616925286806443, 0.0615352319278331, -0.08836339755957438, -0.1324989494169131, -0.03074805359144441, 0.2340852034024217, -0.2706783781759441, -0.21472857316786592, 0.11448104444372637, -0.2621835339391096, -0.19812352117151022, 0.17050385322760453, -0.019770747791467744,... |
706.446 | Counterterms in Dimensionally Continued AdS Gravity | We revise two regularization mechanisms for Lovelock gravity with AdS
asymptotics. The first one corresponds to the Dirichlet counterterm method,
where local functionals of the boundary metric are added to the bulk action on
top of a Gibbons-Hawking-Myers term that defines the Dirichlet problem in
gravity. The genera... | hep-th gr-qc | we revise two regularization mechanisms for lovelock gravity with ads asymptotics the first one corresponds to the dirichlet counterterm method where local functionals of the boundary metric are added to the bulk action on top of a gibbonshawkingmyers term that defines the dirichlet problem in gravity the generalized g... | [['we', 'revise', 'two', 'regularization', 'mechanisms', 'for', 'lovelock', 'gravity', 'with', 'ads', 'asymptotics', 'the', 'first', 'one', 'corresponds', 'to', 'the', 'dirichlet', 'counterterm', 'method', 'where', 'local', 'functionals', 'of', 'the', 'boundary', 'metric', 'are', 'added', 'to', 'the', 'bulk', 'action',... | [-0.13538094612155505, 0.07514433031951255, -0.12300561996612777, 0.08667421541820736, -0.11246142347759389, -0.12962747890343693, -0.011530835336529986, 0.286830389749338, -0.2309859907056423, -0.25814567882210965, 0.11122585267195122, -0.26380553704963877, -0.1573420948963216, 0.1396633587886599, -0.09142515675382729... |
706.4461 | The Infrared Properties of Hickson Compact Groups | Compact groups of galaxies provide a unique environment to study the
mechanisms by which star formation occurs amid continuous gravitational
encounters. We present 2MASS (JHK), Spitzer IRAC (3.5-8 micron) and MIPS (24
micron) observations of a sample of twelve Hickson Compact Groups (HCGs 2, 7,
16, 19, 22, 31, 42, 48... | astro-ph | compact groups of galaxies provide a unique environment to study the mechanisms by which star formation occurs amid continuous gravitational encounters we present 2mass jhk spitzer irac 358 micron and mips 24 micron observations of a sample of twelve hickson compact groups hcgs 2 7 16 19 22 31 42 48 59 61 62 and 90 tha... | [['compact', 'groups', 'of', 'galaxies', 'provide', 'a', 'unique', 'environment', 'to', 'study', 'the', 'mechanisms', 'by', 'which', 'star', 'formation', 'occurs', 'amid', 'continuous', 'gravitational', 'encounters', 'we', 'present', '2mass', 'jhk', 'spitzer', 'irac', '358', 'micron', 'and', 'mips', '24', 'micron', 'ob... | [-0.04868202371682133, 0.12847024830081336, -0.07644053619909794, 0.09997877175176635, -0.07202405144181794, -0.03375396321953691, 0.0671833184056879, 0.4696442952036118, -0.12034329753666323, -0.37260795009804637, 0.05152509683443412, -0.3109010733343687, -0.04924731989678471, 0.14881758586749605, -0.04931395502178104... |
706.4462 | Disorder induced transition into a one-dimensional Wigner glass | The destruction of quasi-long range crystalline order as a consequence of
strong disorder effects is shown to accompany the strict localization of all
classical plasma modes of one-dimensional Wigner crystals at T=0. We construct
a phase diagram that relates the structural phase properties of Wigner crystals
to a pla... | cond-mat.dis-nn cond-mat.str-el | the destruction of quasilong range crystalline order as a consequence of strong disorder effects is shown to accompany the strict localization of all classical plasma modes of onedimensional wigner crystals at t0 we construct a phase diagram that relates the structural phase properties of wigner crystals to a plasmon d... | [['the', 'destruction', 'of', 'quasilong', 'range', 'crystalline', 'order', 'as', 'a', 'consequence', 'of', 'strong', 'disorder', 'effects', 'is', 'shown', 'to', 'accompany', 'the', 'strict', 'localization', 'of', 'all', 'classical', 'plasma', 'modes', 'of', 'onedimensional', 'wigner', 'crystals', 'at', 't0', 'we', 'co... | [-0.18974900208431375, 0.22894323508902578, -0.09825884811722367, 0.02260132781976393, -8.998254051019672e-05, -0.0952011504750841, 0.09392695513710322, 0.3639205396744131, -0.2596176848355823, -0.22710566200628762, 0.025610865022674317, -0.3065053836463858, -0.17475383046602133, 0.10855220936466264, 0.0398012816831327... |
706.4463 | The Nonlinear Evolution of Instabilities Driven by Magnetic Buoyancy: A
New Mechanism for the Formation of Coherent Magnetic Structures | Motivated by the problem of the formation of active regions from a
deep-seated solar magnetic field, we consider the nonlinear three-dimensional
evolution of magnetic buoyancy instabilities resulting from a smoothly
stratified horizontal magnetic field. By exploring the case for which the
instability is continuously ... | astro-ph | motivated by the problem of the formation of active regions from a deepseated solar magnetic field we consider the nonlinear threedimensional evolution of magnetic buoyancy instabilities resulting from a smoothly stratified horizontal magnetic field by exploring the case for which the instability is continuously driven... | [['motivated', 'by', 'the', 'problem', 'of', 'the', 'formation', 'of', 'active', 'regions', 'from', 'a', 'deepseated', 'solar', 'magnetic', 'field', 'we', 'consider', 'the', 'nonlinear', 'threedimensional', 'evolution', 'of', 'magnetic', 'buoyancy', 'instabilities', 'resulting', 'from', 'a', 'smoothly', 'stratified', '... | [-0.1726655152042286, 0.23627810227542612, 0.00828525683668963, 0.05118407646659762, -0.050588640652723234, -0.00972678283450462, 0.004831453753729998, 0.3099192107506728, -0.28767872390226795, -0.34569492011125813, 0.07607715035457227, -0.1661058634014453, -0.12675159117522633, 0.21759647209102573, 0.03200932094922005... |
706.4464 | The Persistence of High-Frequency Spin Fluctuations in Overdoped
La$_{2-x}$Sr$_{x}$CuO$_{4}$ ($x$=0.22) | We report a detailed inelastic neutron scattering study of the collective
magnetic excitations of overdoped superconducting La1.78Sr0.22CuO4 for the
energy range 0-160 meV. Our measurements show that overdoping suppresses the
strong response present for optimally doped La2-xSrxCuO4 which is peaked near
50 meV. The re... | cond-mat.supr-con cond-mat.str-el | we report a detailed inelastic neutron scattering study of the collective magnetic excitations of overdoped superconducting la178sr022cuo4 for the energy range 0160 mev our measurements show that overdoping suppresses the strong response present for optimally doped la2xsrxcuo4 which is peaked near 50 mev the remaining ... | [['we', 'report', 'a', 'detailed', 'inelastic', 'neutron', 'scattering', 'study', 'of', 'the', 'collective', 'magnetic', 'excitations', 'of', 'overdoped', 'superconducting', 'la178sr022cuo4', 'for', 'the', 'energy', 'range', '0160', 'mev', 'our', 'measurements', 'show', 'that', 'overdoping', 'suppresses', 'the', 'stron... | [-0.18440454202227113, 0.28976180836013177, 0.0023090992940635216, 0.08059426301965354, -0.05665642997745436, -0.13198968930533383, 0.13465495429728636, 0.39695830297906226, -0.20645999760230685, -0.2687087504011465, -0.07974575604198546, -0.40587772109841064, -0.03406280250765565, 0.18036214842052176, 0.13468994560123... |
706.4465 | Electric Flux Tube in Magnetic Plasma | In this paper we study a methodical problem related to the magnetic scenario
recently suggested and initiated by the authors \cite{Liao_ES_mono} to
understand the strongly coupled quark-gluon plasma (sQGP): the electric flux
tube in monopole plasma. A macroscopic approach, interpolating between Bose
condensed (dual s... | hep-ph | in this paper we study a methodical problem related to the magnetic scenario recently suggested and initiated by the authors citeliao_es_mono to understand the strongly coupled quarkgluon plasma sqgp the electric flux tube in monopole plasma a macroscopic approach interpolating between bose condensed dual superconducto... | [['in', 'this', 'paper', 'we', 'study', 'a', 'methodical', 'problem', 'related', 'to', 'the', 'magnetic', 'scenario', 'recently', 'suggested', 'and', 'initiated', 'by', 'the', 'authors', 'citeliao_es_mono', 'to', 'understand', 'the', 'strongly', 'coupled', 'quarkgluon', 'plasma', 'sqgp', 'the', 'electric', 'flux', 'tub... | [-0.10476544199646846, 0.22756056175378891, -0.04440491569222383, 0.06765102788812048, -0.021611374948977257, -0.08293756564433863, 0.054301188472701004, 0.34093975525020676, -0.17762609097644005, -0.3183141053879475, 0.0382978901349037, -0.2804831694202875, -0.051147895037680496, 0.14254795446203644, 0.024165621806496... |
706.4466 | Flux enhancement and multistability induced by time delays in a feedback
controlled flashing ratchet | Feedback controlled ratchets are thermal rectifiers that use information on
the state of the system to operate. We study the effects of time delays in the
feedback for a protocol that performs an instantaneous maximization of the
center-of-mass velocity in the many particle case. For small delays the
center-of-mass v... | cond-mat.stat-mech | feedback controlled ratchets are thermal rectifiers that use information on the state of the system to operate we study the effects of time delays in the feedback for a protocol that performs an instantaneous maximization of the centerofmass velocity in the many particle case for small delays the centerofmass velocity ... | [['feedback', 'controlled', 'ratchets', 'are', 'thermal', 'rectifiers', 'that', 'use', 'information', 'on', 'the', 'state', 'of', 'the', 'system', 'to', 'operate', 'we', 'study', 'the', 'effects', 'of', 'time', 'delays', 'in', 'the', 'feedback', 'for', 'a', 'protocol', 'that', 'performs', 'an', 'instantaneous', 'maximi... | [-0.2143586835399229, 0.12219341177882558, -0.04340957920194941, 0.0438962657142758, -0.02190194681036071, -0.15847211003950848, 0.06566317188476754, 0.36171956816790524, -0.2617748467108378, -0.297015151674194, 0.10188881905780144, -0.2247397088820555, -0.12579150861743224, 0.2461481085136676, -0.08241761750272977, 0.... |
706.4467 | Surface Brightness Fluctuations from archival ACS images: a stellar
population and distance study | We derive Surface Brightness Fluctuations (SBF) and integrated magnitudes in
the V- and I-bands using Advanced Camera for Surveys (ACS) archival data. The
sample includes 14 galaxies covering a wide range of physical properties:
morphology, total absolute magnitude, integrated color. We take advantage of
the latter c... | astro-ph | we derive surface brightness fluctuations sbf and integrated magnitudes in the v and ibands using advanced camera for surveys acs archival data the sample includes 14 galaxies covering a wide range of physical properties morphology total absolute magnitude integrated color we take advantage of the latter characteristic... | [['we', 'derive', 'surface', 'brightness', 'fluctuations', 'sbf', 'and', 'integrated', 'magnitudes', 'in', 'the', 'v', 'and', 'ibands', 'using', 'advanced', 'camera', 'for', 'surveys', 'acs', 'archival', 'data', 'the', 'sample', 'includes', '14', 'galaxies', 'covering', 'a', 'wide', 'range', 'of', 'physical', 'properti... | [-0.029416991515262496, 0.06824477452097372, -0.12325215890693168, 0.10702093962491269, -0.0648523918796508, -0.05093611292541027, 0.030862482026263717, 0.45732342732981557, -0.17470528495475826, -0.3695023969760985, 0.06343199804901987, -0.28149000376440764, -0.04351495676895692, 0.22347368958650068, -0.08273333131025... |
706.4468 | Experimental Results on |Vcb| and b -> c l nu Transitions | A review of recent analyses on semileptonic decays of B mesons into charmed
final states is given. |Vcb| is extracted both by the Babar and the Belle
collaboration from their datasets using inclusively and exclusively
reconstructed final states.
In addition there are recent results on the determination of exclusive... | hep-ex | a review of recent analyses on semileptonic decays of b mesons into charmed final states is given vcb is extracted both by the babar and the belle collaboration from their datasets using inclusively and exclusively reconstructed final states in addition there are recent results on the determination of exclusive branchi... | [['a', 'review', 'of', 'recent', 'analyses', 'on', 'semileptonic', 'decays', 'of', 'b', 'mesons', 'into', 'charmed', 'final', 'states', 'is', 'given', 'vcb', 'is', 'extracted', 'both', 'by', 'the', 'babar', 'and', 'the', 'belle', 'collaboration', 'from', 'their', 'datasets', 'using', 'inclusively', 'and', 'exclusively'... | [-0.05409918155955611, 0.21678372532187495, -0.056150817701151386, 0.0855898302475701, -0.0029910190712622146, -0.08668723094670736, 0.07636681126704267, 0.3097923792821845, -0.17742094265047423, -0.27845438145408313, 0.027715608573605104, -0.38715434152652156, -0.022887894677324702, 0.15329157348395778, 0.080197699852... |
706.4469 | Density Matrix Renormalization Group Study of Incompressible Fractional
Quantum Hall States | We develop the Density Matrix Renormalization Group (DMRG) technique for
numerically studying incompressible fractional quantum Hall (FQH) states on the
sphere. We calculate accurate estimates for ground state energies and
excitationgaps at FQH filling fractions \nu=1/3 and \nu=5/2 for systems that
are almost twice a... | cond-mat.mes-hall cond-mat.str-el | we develop the density matrix renormalization group dmrg technique for numerically studying incompressible fractional quantum hall fqh states on the sphere we calculate accurate estimates for ground state energies and excitationgaps at fqh filling fractions nu13 and nu52 for systems that are almost twice as large as th... | [['we', 'develop', 'the', 'density', 'matrix', 'renormalization', 'group', 'dmrg', 'technique', 'for', 'numerically', 'studying', 'incompressible', 'fractional', 'quantum', 'hall', 'fqh', 'states', 'on', 'the', 'sphere', 'we', 'calculate', 'accurate', 'estimates', 'for', 'ground', 'state', 'energies', 'and', 'excitatio... | [-0.1500875819593859, 0.1939147426567685, -0.09916537864587437, 0.10800259485870647, 0.03455531757133894, -0.15997354434922528, 0.04155336920386897, 0.33464949652075004, -0.1563686823579841, -0.303498885833109, 0.12386215072220717, -0.28228233960152677, -0.13609503290783137, 0.23598502964197018, 0.09261587074695107, 0.... |
706.447 | Two flavor QCD and confinement - II | This paper is part of a program of investigation of the chiral transition in
Nf=2 QCD, started in Phys.Rev.D72:114510,2005. Progress is reported on the
understanding of some possible systematic errors. A direct test of first order
scaling is presented.
| hep-lat | this paper is part of a program of investigation of the chiral transition in nf2 qcd started in physrevd721145102005 progress is reported on the understanding of some possible systematic errors a direct test of first order scaling is presented | [['this', 'paper', 'is', 'part', 'of', 'a', 'program', 'of', 'investigation', 'of', 'the', 'chiral', 'transition', 'in', 'nf2', 'qcd', 'started', 'in', 'physrevd721145102005', 'progress', 'is', 'reported', 'on', 'the', 'understanding', 'of', 'some', 'possible', 'systematic', 'errors', 'a', 'direct', 'test', 'of', 'firs... | [-0.1780815927409812, 0.11199991767735858, -0.10670592077076435, 0.012005971741593001, -0.08728913884413869, 0.011025235963691222, 0.07833353902127496, 0.3473277854684152, -0.13627219905978755, -0.25852505017169997, 0.12228453487133313, -0.26820788776354965, -0.14353071170319853, 0.15059082455148823, -0.000691453240027... |
706.4471 | Notes on D-branes and dualities in (p,q) minimal superstring theory | We study boundary states in (p,q) minimal superstring theory, combining the
explicit form of matter wave functions. Within the modular bootstrap framework,
Cardy states of (p,q) minimal superconformal field theory are completely
determined in both cases of the different supercharge combinations, and the
remaining con... | hep-th | we study boundary states in pq minimal superstring theory combining the explicit form of matter wave functions within the modular bootstrap framework cardy states of pq minimal superconformal field theory are completely determined in both cases of the different supercharge combinations and the remaining consistency che... | [['we', 'study', 'boundary', 'states', 'in', 'pq', 'minimal', 'superstring', 'theory', 'combining', 'the', 'explicit', 'form', 'of', 'matter', 'wave', 'functions', 'within', 'the', 'modular', 'bootstrap', 'framework', 'cardy', 'states', 'of', 'pq', 'minimal', 'superconformal', 'field', 'theory', 'are', 'completely', 'd... | [-0.1764736234785883, 0.13811239568001735, -0.07146784034746934, 0.12975041037785057, -0.035021577270822675, -0.19060108890544955, 0.005423775000490127, 0.3133180755894722, -0.17639298113517282, -0.22508380114956478, 0.11946028957476582, -0.27170750011152367, -0.14372522904484616, 0.09998139932210277, -0.04708745545041... |
706.4472 | Chaos at the border of criticality | The present paper points out to a novel scenario for formation of chaotic
attractors in a class of models of excitable cell membranes near an
Andronov-Hopf bifurcation (AHB). The mechanism underlying chaotic dynamics
admits a simple and visual description in terms of the families of
one-dimensional first-return maps,... | nlin.CD | the present paper points out to a novel scenario for formation of chaotic attractors in a class of models of excitable cell membranes near an andronovhopf bifurcation ahb the mechanism underlying chaotic dynamics admits a simple and visual description in terms of the families of onedimensional firstreturn maps which ar... | [['the', 'present', 'paper', 'points', 'out', 'to', 'a', 'novel', 'scenario', 'for', 'formation', 'of', 'chaotic', 'attractors', 'in', 'a', 'class', 'of', 'models', 'of', 'excitable', 'cell', 'membranes', 'near', 'an', 'andronovhopf', 'bifurcation', 'ahb', 'the', 'mechanism', 'underlying', 'chaotic', 'dynamics', 'admit... | [-0.1765103871257234, 0.06306879689526942, -0.09223450331887353, 0.0513932216113634, 0.004801326835650706, -0.11630184505926724, 0.058298750361567085, 0.2801531729271669, -0.3019686845120065, -0.22701675410265337, 0.11198008611999051, -0.25495449432539946, -0.23035066583734787, 0.20110974941558823, -0.03896927411115901... |
706.4473 | HyperKahler and quaternionic Kahler manifolds with S^1-symmetries | We study relations between quaternionic Riemannian manifolds admitting
different types of symmetries. We show that any hyperKahler manifold admitting
hyperKahler potential and triholomorphic action of S^1 can be constructed from
another hyperKahler manifold (of lower dimention) with an action of S^1 which
fixes one c... | math.DG math-ph math.MP | we study relations between quaternionic riemannian manifolds admitting different types of symmetries we show that any hyperkahler manifold admitting hyperkahler potential and triholomorphic action of s1 can be constructed from another hyperkahler manifold of lower dimention with an action of s1 which fixes one complex ... | [['we', 'study', 'relations', 'between', 'quaternionic', 'riemannian', 'manifolds', 'admitting', 'different', 'types', 'of', 'symmetries', 'we', 'show', 'that', 'any', 'hyperkahler', 'manifold', 'admitting', 'hyperkahler', 'potential', 'and', 'triholomorphic', 'action', 'of', 's1', 'can', 'be', 'constructed', 'from', '... | [-0.2159316166033668, 0.08145584653147937, -0.04335094438064643, 0.0839696201666068, -0.19217946770430733, -0.21869104301496858, -0.05600934065077254, 0.44048251568149493, -0.21235104441963215, -0.18122049960588174, 0.10222030630690716, -0.2864763904563201, -0.2176836548092705, 0.15816357657213204, -0.15026860971063857... |
706.4474 | F(R) gravity in purely affine formulation | The purely affine, metric-affine and purely metric formulation of general
relativity are dynamically equivalent and the relation between them is
analogous to the Legendre relation between the Lagrangian and Hamiltonian
dynamics. We show that one cannot construct a dynamically equivalent, purely
affine Lagrangian from... | gr-qc math-ph math.MP | the purely affine metricaffine and purely metric formulation of general relativity are dynamically equivalent and the relation between them is analogous to the legendre relation between the lagrangian and hamiltonian dynamics we show that one cannot construct a dynamically equivalent purely affine lagrangian from a met... | [['the', 'purely', 'affine', 'metricaffine', 'and', 'purely', 'metric', 'formulation', 'of', 'general', 'relativity', 'are', 'dynamically', 'equivalent', 'and', 'the', 'relation', 'between', 'them', 'is', 'analogous', 'to', 'the', 'legendre', 'relation', 'between', 'the', 'lagrangian', 'and', 'hamiltonian', 'dynamics',... | [-0.1505474461362896, 0.0989913336260328, -0.16489138510640647, 0.12880037457608942, -0.1848602041999778, -0.2155067998225267, -0.0922604174166133, 0.3230911757655735, -0.26948609921474304, -0.26674031719383573, 0.011220041323672937, -0.2311691497661843, -0.19889900142593792, 0.1311770930789474, -0.09835714834750096, -... |
706.4475 | Black chain of pearls in 5D de Sitter spacetime | We analyze some exact chain-shaped black hole solutions in 5-dimensional
spacetime. Unlike usual black string and black ring solutions, the topology of
the horizons of the new solutions are neither $\mathbb{R}\times R^{2}$ nor
$S^1\times S^2$ but rather like several topological spheres concatenating each
other at sin... | hep-th | we analyze some exact chainshaped black hole solutions in 5dimensional spacetime unlike usual black string and black ring solutions the topology of the horizons of the new solutions are neither mathbbrtimes r2 nor s1times s2 but rather like several topological spheres concatenating each other at single points the shape... | [['we', 'analyze', 'some', 'exact', 'chainshaped', 'black', 'hole', 'solutions', 'in', '5dimensional', 'spacetime', 'unlike', 'usual', 'black', 'string', 'and', 'black', 'ring', 'solutions', 'the', 'topology', 'of', 'the', 'horizons', 'of', 'the', 'new', 'solutions', 'are', 'neither', 'mathbbrtimes', 'r2', 'nor', 's1ti... | [-0.21319270465755835, 0.06830897983214211, -0.0641525965133358, 0.1281161850062705, -0.12389163782253214, -0.1955331659005226, 0.002595896670675796, 0.2834831665917907, -0.19934508292530867, -0.22975746101861738, 0.1649605412182965, -0.3382494937041369, -0.09568076260873805, 0.16676466515712926, -0.10071822332785181, ... |
706.4476 | Perturbative Quantum Corrections to the Supersymmetric CP^1 Kink with
Twisted Mass | We present an explicit calculation of the one-loop quantum corrections to the
mass and the two central charges of the kink solution of an N=(2,2)
supersymmetric CP^1 model with twisted mass, using supersymmetry preserving
dimensional regularization adapted to solitons. We find that the quantum
corrections of the mass... | hep-th | we present an explicit calculation of the oneloop quantum corrections to the mass and the two central charges of the kink solution of an n22 supersymmetric cp1 model with twisted mass using supersymmetry preserving dimensional regularization adapted to solitons we find that the quantum corrections of the mass and one o... | [['we', 'present', 'an', 'explicit', 'calculation', 'of', 'the', 'oneloop', 'quantum', 'corrections', 'to', 'the', 'mass', 'and', 'the', 'two', 'central', 'charges', 'of', 'the', 'kink', 'solution', 'of', 'an', 'n22', 'supersymmetric', 'cp1', 'model', 'with', 'twisted', 'mass', 'using', 'supersymmetry', 'preserving', '... | [-0.1392358790241325, 0.12863018349229466, -0.05496967070727036, 0.10407215425690923, -0.033841832021537885, -0.1489696190593979, 0.025254621835819516, 0.27419040333300543, -0.13698220227558452, -0.2914246107514303, 0.08423055513457467, -0.2892039379928834, -0.11253561386122153, 0.13460009442899787, -0.0489593665115535... |
706.4477 | On a Teichmueller functor between the categories of complex tori and the
Effros-Shen algebras | A covariant functor from the category of the complex tori to the category of
the Effros-Shen algebras is constructed. The functor maps isomorphic complex
tori to the stably isomorphic Effros-Shen algebras. Our construction is based
on the Teichmueller theory of the Riemann surfaces.
| math.AG math.OA | a covariant functor from the category of the complex tori to the category of the effrosshen algebras is constructed the functor maps isomorphic complex tori to the stably isomorphic effrosshen algebras our construction is based on the teichmueller theory of the riemann surfaces | [['a', 'covariant', 'functor', 'from', 'the', 'category', 'of', 'the', 'complex', 'tori', 'to', 'the', 'category', 'of', 'the', 'effrosshen', 'algebras', 'is', 'constructed', 'the', 'functor', 'maps', 'isomorphic', 'complex', 'tori', 'to', 'the', 'stably', 'isomorphic', 'effrosshen', 'algebras', 'our', 'construction', ... | [-0.1678552111112621, 0.0108253444479995, -0.12165365311815295, 0.10722939295120278, -0.11156773515218912, -0.08629004903635833, -0.10067288853975316, 0.32347924786424914, -0.42917983485169187, -0.11573470890695273, 0.11280402632126975, -0.22583004496829195, -0.18155431366244026, 0.2013322373115739, -0.2439189888753516... |
706.4478 | The Optimal Single Copy Measurement for the Hidden Subgroup Problem | The optimization of measurements for the state distinction problem has
recently been applied to the theory of quantum algorithms with considerable
successes, including efficient new quantum algorithms for the non-abelian
hidden subgroup problem. Previous work has identified the optimal single copy
measurement for the... | quant-ph | the optimization of measurements for the state distinction problem has recently been applied to the theory of quantum algorithms with considerable successes including efficient new quantum algorithms for the nonabelian hidden subgroup problem previous work has identified the optimal single copy measurement for the hidd... | [['the', 'optimization', 'of', 'measurements', 'for', 'the', 'state', 'distinction', 'problem', 'has', 'recently', 'been', 'applied', 'to', 'the', 'theory', 'of', 'quantum', 'algorithms', 'with', 'considerable', 'successes', 'including', 'efficient', 'new', 'quantum', 'algorithms', 'for', 'the', 'nonabelian', 'hidden',... | [-0.09745697660856252, 0.10734480835224797, -0.05953001468707391, 0.03477470908807098, -0.11060053509531345, -0.16840221963792554, 0.08895391680023867, 0.3642452605280692, -0.3269278259864607, -0.33131994062474346, 0.14342719063492174, -0.28390693178445825, -0.08504133375467567, 0.1872641312155297, -0.10884408659218409... |
706.4479 | Experimental characterization of frequency dependent squeezed light | We report on the demonstration of broadband squeezed laser beams that show a
frequency dependent orientation of the squeezing ellipse. Carrier frequency as
well as quadrature angle were stably locked to a reference laser beam at
1064nm. This frequency dependent squeezing was characterized in terms of noise
power spec... | quant-ph | we report on the demonstration of broadband squeezed laser beams that show a frequency dependent orientation of the squeezing ellipse carrier frequency as well as quadrature angle were stably locked to a reference laser beam at 1064nm this frequency dependent squeezing was characterized in terms of noise power spectra ... | [['we', 'report', 'on', 'the', 'demonstration', 'of', 'broadband', 'squeezed', 'laser', 'beams', 'that', 'show', 'a', 'frequency', 'dependent', 'orientation', 'of', 'the', 'squeezing', 'ellipse', 'carrier', 'frequency', 'as', 'well', 'as', 'quadrature', 'angle', 'were', 'stably', 'locked', 'to', 'a', 'reference', 'lase... | [-0.16941015215343214, 0.2233544329610595, -0.08046537711470592, 0.006148749361273076, -0.027832554976157553, -0.16117417327404837, 0.03965542652622389, 0.47036344604566693, -0.2150418337987503, -0.2657424032695417, 0.07896352253919758, -0.2283066914678784, -0.06017652274022112, 0.28395526874919597, -0.0197891907118901... |
706.448 | Quantum Projection in an Ising Spin Liquid | A transverse magnetic field is used to scan the diagonal and off-diagonal
susceptibility of the uniaxial quantum magnet,
$\text{LiHo}_{0.045}\text{Y}_{0.955}\text{F}_4$. Clusters of strongly-coupled
spins act as the primary source for the response functions, which result from a
field-induced quantum projection of the... | cond-mat.other cond-mat.dis-nn | a transverse magnetic field is used to scan the diagonal and offdiagonal susceptibility of the uniaxial quantum magnet textliho_0045texty_0955textf_4 clusters of stronglycoupled spins act as the primary source for the response functions which result from a fieldinduced quantum projection of the system into a classicall... | [['a', 'transverse', 'magnetic', 'field', 'is', 'used', 'to', 'scan', 'the', 'diagonal', 'and', 'offdiagonal', 'susceptibility', 'of', 'the', 'uniaxial', 'quantum', 'magnet', 'textliho_0045texty_0955textf_4', 'clusters', 'of', 'stronglycoupled', 'spins', 'act', 'as', 'the', 'primary', 'source', 'for', 'the', 'response'... | [-0.15489739917218684, 0.1859626326461633, -0.06561115262409051, 0.06114431834624459, -0.04400868062007551, -0.14208654853204886, 0.021967860429237287, 0.333967910160621, -0.2335525025303165, -0.25863425898055237, 0.03888024183611075, -0.30631984141965707, -0.07410214419758025, 0.17999060845312972, 0.10744369234889746,... |
706.4481 | Isogravity: Toward an Electroweak and Gravitational Unification | We present a model that unites the electroweak interaction with general
relativity without specifying a space-time metric. This is made possible by
embedding the kinetic terms for gravity and electroweak theory using one $\SL$
connection variable. The gauge theory is specified without relying on a
space-time metric. ... | hep-th | we present a model that unites the electroweak interaction with general relativity without specifying a spacetime metric this is made possible by embedding the kinetic terms for gravity and electroweak theory using one sl connection variable the gauge theory is specified without relying on a spacetime metric we show th... | [['we', 'present', 'a', 'model', 'that', 'unites', 'the', 'electroweak', 'interaction', 'with', 'general', 'relativity', 'without', 'specifying', 'a', 'spacetime', 'metric', 'this', 'is', 'made', 'possible', 'by', 'embedding', 'the', 'kinetic', 'terms', 'for', 'gravity', 'and', 'electroweak', 'theory', 'using', 'one', ... | [-0.1861774584910051, 0.22124018476762133, -0.08658055668354206, 0.12106491491765897, -0.1561544719205677, -0.18865156357294355, 0.006171189453292252, 0.32405226807184945, -0.21577567804133754, -0.26533678608636063, 0.03786762259986209, -0.22946962692785536, -0.13911177736075445, 0.06825055694475171, 0.0270106606827727... |
706.4482 | The Evolution of the Cosmic Microwave Background | We discuss the time dependence and future of the Cosmic Microwave Background
(CMB) in the context of the standard cosmological model, in which we are now
entering a state of endless accelerated expansion. The mean temperature will
simply decrease until it reaches the effective temperature of the de Sitter
vacuum, whi... | astro-ph | we discuss the time dependence and future of the cosmic microwave background cmb in the context of the standard cosmological model in which we are now entering a state of endless accelerated expansion the mean temperature will simply decrease until it reaches the effective temperature of the de sitter vacuum while the ... | [['we', 'discuss', 'the', 'time', 'dependence', 'and', 'future', 'of', 'the', 'cosmic', 'microwave', 'background', 'cmb', 'in', 'the', 'context', 'of', 'the', 'standard', 'cosmological', 'model', 'in', 'which', 'we', 'are', 'now', 'entering', 'a', 'state', 'of', 'endless', 'accelerated', 'expansion', 'the', 'mean', 'te... | [-0.11877721317441148, 0.1643857993733357, -0.09328453412728029, 0.10763468626434641, -0.07963102264466751, -0.03395316084737287, -0.029559758545570622, 0.3483550652204191, -0.2608205071670989, -0.28089964825879127, 0.09335965072832016, -0.3365955992348437, -0.09825998637585572, 0.19804195177138728, 0.02747099584187655... |
706.4483 | Epicyclic Oscillations of Fluid Bodies: Newtonian Nonslender Torus | We study epicyclic oscillations of fluid tori around black holes (in the
Paczynski-Wiita potential) and derive exact analytic expressions for their
radial and vertical eigenfrequencies nu_r and nu_z to second-order accuracy in
the width of the torus. We prove that pressure effects make the
eigenfrequencies smaller th... | astro-ph | we study epicyclic oscillations of fluid tori around black holes in the paczynskiwiita potential and derive exact analytic expressions for their radial and vertical eigenfrequencies nu_r and nu_z to secondorder accuracy in the width of the torus we prove that pressure effects make the eigenfrequencies smaller than thos... | [['we', 'study', 'epicyclic', 'oscillations', 'of', 'fluid', 'tori', 'around', 'black', 'holes', 'in', 'the', 'paczynskiwiita', 'potential', 'and', 'derive', 'exact', 'analytic', 'expressions', 'for', 'their', 'radial', 'and', 'vertical', 'eigenfrequencies', 'nu_r', 'and', 'nu_z', 'to', 'secondorder', 'accuracy', 'in',... | [-0.1368643848277698, 0.18006126617329526, -0.029657796617144735, 0.15398077994571982, -0.0757395949380072, -0.11291345894319292, 0.02047643629794888, 0.3351208749531864, -0.1469265372148567, -0.2875673658144878, 0.08400678493857175, -0.3054821887575786, -0.06500853820503733, 0.2635366027830952, -0.017169524202880527, ... |
706.4484 | Spectroscopic Surveys: Present | I summarize the current spectroscopic sky surveys and some of the scientific
results, emphasizing the largest sky survey to-date, the Sloan Digital Sky
Survey (SDSS). Techniques used commonly in spectral analyses are discussed,
followed by the present needs and challenges for solving some of the unknown
problems. I d... | astro-ph | i summarize the current spectroscopic sky surveys and some of the scientific results emphasizing the largest sky survey todate the sloan digital sky survey sdss techniques used commonly in spectral analyses are discussed followed by the present needs and challenges for solving some of the unknown problems i discuss how... | [['i', 'summarize', 'the', 'current', 'spectroscopic', 'sky', 'surveys', 'and', 'some', 'of', 'the', 'scientific', 'results', 'emphasizing', 'the', 'largest', 'sky', 'survey', 'todate', 'the', 'sloan', 'digital', 'sky', 'survey', 'sdss', 'techniques', 'used', 'commonly', 'in', 'spectral', 'analyses', 'are', 'discussed'... | [-0.056667650899579446, 0.03549734560862904, -0.0117110853504029, 0.10494125732070496, -0.20858097898082867, -0.03809400200242958, 0.05228861575690849, 0.382175893477735, -0.22301177584355877, -0.3266922670506662, 0.18749881711142558, -0.3797616486347491, -0.11700500379646978, 0.29109792738792395, -0.049201933479297064... |
707.0001 | Constants of Geodesic Motion in Higher-Dimensional Black-Hole Spacetimes | In [arXiv:hep-th/0611083] we announced the complete integrability of geodesic
motion in the general higher-dimensional rotating black-hole spacetimes. In the
present paper we prove all the necessary steps leading to this conclusion. In
particular, we demonstrate the independence of the constants of motion and the
fac... | hep-th gr-qc | in arxivhepth0611083 we announced the complete integrability of geodesic motion in the general higherdimensional rotating blackhole spacetimes in the present paper we prove all the necessary steps leading to this conclusion in particular we demonstrate the independence of the constants of motion and the fact that they ... | [['in', 'arxivhepth0611083', 'we', 'announced', 'the', 'complete', 'integrability', 'of', 'geodesic', 'motion', 'in', 'the', 'general', 'higherdimensional', 'rotating', 'blackhole', 'spacetimes', 'in', 'the', 'present', 'paper', 'we', 'prove', 'all', 'the', 'necessary', 'steps', 'leading', 'to', 'this', 'conclusion', '... | [-0.16274139962752088, 0.10200786805944517, -0.05344035320013063, 0.0836146876172279, -0.08081785454851342, -0.04518257284507854, -0.0017402890161974938, 0.3507775986508932, -0.26164384570438415, -0.2218698190699797, 0.07846070884079381, -0.23553836140490603, -0.17474467628744605, 0.16241831178194843, -0.12769896288955... |
707.0002 | Electromagnetic Field in Higher-Dimensional Black-Hole Spacetimes | A special test electromagnetic field in the spacetime of the
higher-dimensional generally rotating NUT-(A)dS black hole is found. It is
adjusted to the hidden symmetries of the background represented by the
principal Killing-Yano tensor. Such electromagnetic field generalizes the field
of charged black hole in four d... | hep-th gr-qc | a special test electromagnetic field in the spacetime of the higherdimensional generally rotating nutads black hole is found it is adjusted to the hidden symmetries of the background represented by the principal killingyano tensor such electromagnetic field generalizes the field of charged black hole in four dimensions... | [['a', 'special', 'test', 'electromagnetic', 'field', 'in', 'the', 'spacetime', 'of', 'the', 'higherdimensional', 'generally', 'rotating', 'nutads', 'black', 'hole', 'is', 'found', 'it', 'is', 'adjusted', 'to', 'the', 'hidden', 'symmetries', 'of', 'the', 'background', 'represented', 'by', 'the', 'principal', 'killingya... | [-0.15588987576923083, 0.15214245133693255, -0.020271977842582153, 0.12375370101515382, -0.09884765544640166, -0.13822796362792217, -0.09903492699451154, 0.29079092601462014, -0.19830673314364894, -0.2899616211357098, 0.06653848511632532, -0.24545582697638088, -0.1240155173258649, 0.16060876846313477, -0.02359875401718... |
707.0003 | The Spatial Structure of An Accretion Disk | Based on the microlensing variability of the two-image gravitational lens
HE1104-1805 observed between 0.4 and 8 microns, we have measured the size and
wavelength-dependent structure of the quasar accretion disk. Modeled as a power
law in temperature, T proportional to R^-beta, we measure a B-band (0.13
microns in th... | astro-ph | based on the microlensing variability of the twoimage gravitational lens he11041805 observed between 04 and 8 microns we have measured the size and wavelengthdependent structure of the quasar accretion disk modeled as a power law in temperature t proportional to rbeta we measure a bband 013 microns in the rest frame ha... | [['based', 'on', 'the', 'microlensing', 'variability', 'of', 'the', 'twoimage', 'gravitational', 'lens', 'he11041805', 'observed', 'between', '04', 'and', '8', 'microns', 'we', 'have', 'measured', 'the', 'size', 'and', 'wavelengthdependent', 'structure', 'of', 'the', 'quasar', 'accretion', 'disk', 'modeled', 'as', 'a',... | [-0.05780293217573602, 0.10833864397584246, -0.030562159456223106, 0.06492510361176056, -0.019681334778523216, -0.12858882016824702, 0.060128795243172835, 0.38015992470139354, -0.15867726536324392, -0.3868206645075518, 0.054374681483022866, -0.31733501069964126, 0.04717617749881286, 0.1990098568951138, -0.0520145508353... |
707.0004 | An Algorithm to Construct A Basis for the Module of Logarithmic Vector
Fields | We consider logarithmic vector fields parametrized by finite collections of
weighted hyperplanes. For a finite collection of weighted hyperplanes in a
two-dimensional vector space, it is known that the set of such vector fields is
a free module of rank two whose basis elements are homogeneous. We give an
algorithm to... | math.CO | we consider logarithmic vector fields parametrized by finite collections of weighted hyperplanes for a finite collection of weighted hyperplanes in a twodimensional vector space it is known that the set of such vector fields is a free module of rank two whose basis elements are homogeneous we give an algorithm to const... | [['we', 'consider', 'logarithmic', 'vector', 'fields', 'parametrized', 'by', 'finite', 'collections', 'of', 'weighted', 'hyperplanes', 'for', 'a', 'finite', 'collection', 'of', 'weighted', 'hyperplanes', 'in', 'a', 'twodimensional', 'vector', 'space', 'it', 'is', 'known', 'that', 'the', 'set', 'of', 'such', 'vector', '... | [-0.16878972077292614, 0.15965391710979648, -0.018372771691466713, 0.03286620453080355, -0.08639274620258346, -0.08372387945138175, -0.006113845906682023, 0.3942104595360057, -0.33465716512552623, -0.1646616693810913, 0.09124713884626419, -0.2441236313657257, -0.13684645124935899, 0.19790285616984654, -0.02664468162050... |
707.0005 | Higgs Physics as a Window Beyond the MSSM (BMSSM) | We interpret the current experimental limit on the lightest Higgs boson mass
to suggest that if nature is supersymmetric, there are additional interactions
beyond those of the MSSM coming from new degrees of freedom around the TeV
scale. Within an effective field theory analysis, the leading order corrections
to the ... | hep-ph | we interpret the current experimental limit on the lightest higgs boson mass to suggest that if nature is supersymmetric there are additional interactions beyond those of the mssm coming from new degrees of freedom around the tev scale within an effective field theory analysis the leading order corrections to the mssm ... | [['we', 'interpret', 'the', 'current', 'experimental', 'limit', 'on', 'the', 'lightest', 'higgs', 'boson', 'mass', 'to', 'suggest', 'that', 'if', 'nature', 'is', 'supersymmetric', 'there', 'are', 'additional', 'interactions', 'beyond', 'those', 'of', 'the', 'mssm', 'coming', 'from', 'new', 'degrees', 'of', 'freedom', '... | [-0.10502988145234857, 0.2245712436536514, -0.04452276027284212, 0.17208890395589393, -0.091698723637711, -0.14649761183934268, -0.0037507038634952785, 0.2953196268201354, -0.24384157533416212, -0.3366816710717607, 0.044315821454297785, -0.28305180978011524, -0.06288513842748829, 0.16792763433635863, 0.0172783233580354... |
707.0006 | Spectroscopic Analysis of H I Absorption Line Systems in 40 HIRES
Quasars | We list and analyze H I absorption lines at redshifts 2 < z < 4 with column
density (12 < log(N_HI) < 19) in 40 high-resolutional (FWHM = 8.0 km/s) quasar
spectra obtained with the Keck+HIRES. We de-blend and fit all H I lines within
1,000 km/s of 86 strong H I lines whose column densities are log(N_HI/[cm^-2])
> 15.... | astro-ph | we list and analyze h i absorption lines at redshifts 2 z 4 with column density 12 logn_hi 19 in 40 highresolutional fwhm 80 kms quasar spectra obtained with the keckhires we deblend and fit all h i lines within 1000 kms of 86 strong h i lines whose column densities are logn_hicm2 15 unlike most prior studies we use no... | [['we', 'list', 'and', 'analyze', 'h', 'i', 'absorption', 'lines', 'at', 'redshifts', '2', 'z', '4', 'with', 'column', 'density', '12', 'logn_hi', '19', 'in', '40', 'highresolutional', 'fwhm', '80', 'kms', 'quasar', 'spectra', 'obtained', 'with', 'the', 'keckhires', 'we', 'deblend', 'and', 'fit', 'all', 'h', 'i', 'line... | [-0.040039436813682466, 0.11859414199874117, 0.021405711481026535, 0.03793580691717804, -0.041768326327718534, -0.15059376798462343, 0.06485818899316906, 0.5219413522273082, -0.14139602424547057, -0.3525278030578139, 0.047445936705412466, -0.32286105036111595, 0.029230781002750096, 0.12578073759755953, 0.02779546252846... |
707.0007 | Meta-Stable Dynamical Supersymmetry Breaking Near Points of Enhanced
Symmetry | We show that metastable supersymmetry breaking is generic near certain
enhanced symmetry points of gauge theory moduli spaces. Our model consists of
two sectors coupled by a singlet and combines dynamical supersymmetry breaking
with an O'Raifeartaigh mechanism in terms of confined variables. All relevant
mass paramet... | hep-th hep-ph | we show that metastable supersymmetry breaking is generic near certain enhanced symmetry points of gauge theory moduli spaces our model consists of two sectors coupled by a singlet and combines dynamical supersymmetry breaking with an oraifeartaigh mechanism in terms of confined variables all relevant mass parameters i... | [['we', 'show', 'that', 'metastable', 'supersymmetry', 'breaking', 'is', 'generic', 'near', 'certain', 'enhanced', 'symmetry', 'points', 'of', 'gauge', 'theory', 'moduli', 'spaces', 'our', 'model', 'consists', 'of', 'two', 'sectors', 'coupled', 'by', 'a', 'singlet', 'and', 'combines', 'dynamical', 'supersymmetry', 'bre... | [-0.203047013631065, 0.29633368639301744, -0.05423833210378477, 0.1117024440525661, -0.05414100365445324, -0.15175916389594085, 0.007597929646567225, 0.3169549449972094, -0.24024309922800693, -0.2775727799545004, 0.06580823343980752, -0.22753522087092679, -0.1337257899369483, 0.07264615469994916, -0.0025383457669044193... |
707.0008 | Reliable Final Computational Results from Faulty Quantum Computation | In this paper we extend both standard fault tolerance theory and Kitaev's
model for quantum computation, combining them so as to yield quantitative
results that reveal the interplay between the two. Our analysis establishes a
methodology that allows us to quantitatively determine design parameters for a
quantum compu... | quant-ph | in this paper we extend both standard fault tolerance theory and kitaevs model for quantum computation combining them so as to yield quantitative results that reveal the interplay between the two our analysis establishes a methodology that allows us to quantitatively determine design parameters for a quantum computer t... | [['in', 'this', 'paper', 'we', 'extend', 'both', 'standard', 'fault', 'tolerance', 'theory', 'and', 'kitaevs', 'model', 'for', 'quantum', 'computation', 'combining', 'them', 'so', 'as', 'to', 'yield', 'quantitative', 'results', 'that', 'reveal', 'the', 'interplay', 'between', 'the', 'two', 'our', 'analysis', 'establish... | [-0.07204845425007599, 0.03934669259478272, -0.09097260665148496, 0.0511216551284971, -0.04663770725950599, -0.1393048300913402, 0.10171187836410744, 0.31734378754028253, -0.23971049053328378, -0.37282590661730086, 0.06568362986203283, -0.19691399139235727, -0.1423182933085731, 0.22964888095456576, -0.09532562016309905... |
707.0009 | Invariant weighted algebras $L_p^w(G)$ | The paper deals with weighted spaces $L_p^w(G)$ on a locally compact group G.
If w is a positive measurable function on G then we define the space
$L_p^w(G)$, $p\ge1$, as $L_p^w(G)=\{f:fw\in L_p(G)\}$. We consider weights such
that these weighted spaces are algebras with respect to usual convolution. It
is shown that... | math.FA | the paper deals with weighted spaces l_pwg on a locally compact group g if w is a positive measurable function on g then we define the space l_pwg pge1 as l_pwgffwin l_pg we consider weights such that these weighted spaces are algebras with respect to usual convolution it is shown that for p1 such weights exists on any... | [['the', 'paper', 'deals', 'with', 'weighted', 'spaces', 'l_pwg', 'on', 'a', 'locally', 'compact', 'group', 'g', 'if', 'w', 'is', 'a', 'positive', 'measurable', 'function', 'on', 'g', 'then', 'we', 'define', 'the', 'space', 'l_pwg', 'pge1', 'as', 'l_pwgffwin', 'l_pg', 'we', 'consider', 'weights', 'such', 'that', 'these... | [-0.13417819493527836, 0.11692817864940142, -0.07063395986516102, 0.10433868227033492, -0.13000410026414136, -0.17115070501926774, -0.029392787199421767, 0.45782844846447307, -0.33819749665117876, -0.15830632128271127, 0.1500291643406301, -0.255996573216501, -0.17262412474362873, 0.1975869185253567, -0.1669197327402584... |
707.001 | Equation-of-state model for shock compression of hot dense matter | A quantum equation-of-state model is presented and applied to the calculation
of high-pressure shock Hugoniot curves beyond the asymptotic fourfold density,
close to the maximum compression where quantum effects play a role. An
analytical estimate for the maximum attainable compression is proposed. It
gives a good ag... | physics.plasm-ph | a quantum equationofstate model is presented and applied to the calculation of highpressure shock hugoniot curves beyond the asymptotic fourfold density close to the maximum compression where quantum effects play a role an analytical estimate for the maximum attainable compression is proposed it gives a good agreement ... | [['a', 'quantum', 'equationofstate', 'model', 'is', 'presented', 'and', 'applied', 'to', 'the', 'calculation', 'of', 'highpressure', 'shock', 'hugoniot', 'curves', 'beyond', 'the', 'asymptotic', 'fourfold', 'density', 'close', 'to', 'the', 'maximum', 'compression', 'where', 'quantum', 'effects', 'play', 'a', 'role', 'a... | [-0.09706420539056554, 0.07980093423205237, -0.14737801695717315, 0.055054867872968316, -0.061040231455847915, -0.14848100444228918, 0.06387993162863102, 0.3201744420563473, -0.22261313391009382, -0.2815933254930903, 0.02573486798278549, -0.2789863430547948, -0.08602128603025432, 0.2322910414442566, 0.02405664969381748... |
707.0011 | Calculating the probability of detecting radio signals from alien
civilizations | Although it might not be self-evident, it is in fact entirely possible to
calculate the probability of detecting alien radio signals by understanding
what types of extraterrestrial radio emissions can be expected and what
properties these emissions can have. Using the Drake equation as the obvious
starting point, and... | physics.pop-ph astro-ph | although it might not be selfevident it is in fact entirely possible to calculate the probability of detecting alien radio signals by understanding what types of extraterrestrial radio emissions can be expected and what properties these emissions can have using the drake equation as the obvious starting point and logic... | [['although', 'it', 'might', 'not', 'be', 'selfevident', 'it', 'is', 'in', 'fact', 'entirely', 'possible', 'to', 'calculate', 'the', 'probability', 'of', 'detecting', 'alien', 'radio', 'signals', 'by', 'understanding', 'what', 'types', 'of', 'extraterrestrial', 'radio', 'emissions', 'can', 'be', 'expected', 'and', 'wha... | [-0.13075199653057085, 0.15451070143962684, -0.10738944448530674, 0.14508192956386862, -0.15380576879218005, -0.11945116347835763, 0.08448257595570623, 0.3866447333948336, -0.2615075391055881, -0.35664543366410595, 0.11837459987778541, -0.26291627425403485, -0.1855453663924034, 0.1802500789526148, -0.027301013483193474... |
707.0012 | Electron operator at the edge of the 1/3 fractional quantum Hall liquid | This study builds upon the work of Palacios and MacDonald (Phys. Rev. Lett.
{\bf 76}, 118 (1996)), wherein they identify the bosonic excitations of Wen's
approach for the edge of the 1/3 fractional quantum Hall state with certain
operators introduced by Stone. Using a quantum Monte Carlo method, we extend to
larger s... | cond-mat.mes-hall | this study builds upon the work of palacios and macdonald phys rev lett bf 76 118 1996 wherein they identify the bosonic excitations of wens approach for the edge of the 13 fractional quantum hall state with certain operators introduced by stone using a quantum monte carlo method we extend to larger systems containing ... | [['this', 'study', 'builds', 'upon', 'the', 'work', 'of', 'palacios', 'and', 'macdonald', 'phys', 'rev', 'lett', 'bf', '76', '118', '1996', 'wherein', 'they', 'identify', 'the', 'bosonic', 'excitations', 'of', 'wens', 'approach', 'for', 'the', 'edge', 'of', 'the', '13', 'fractional', 'quantum', 'hall', 'state', 'with',... | [-0.08265132582321688, 0.16202322910288097, -0.05941729150229524, 0.012398979621876433, -0.02368967091299694, -0.11764170074398075, 0.08170537262796299, 0.3114178740432033, -0.17278859983009562, -0.3240553551743663, 0.023968397169311, -0.31215936379708553, -0.11279317108612205, 0.21399605354117984, -0.00443272556750909... |
707.0013 | Shell-structure effects on high-pressure Rankine-Hugoniot shock adiabats | Rankine-Hugoniot shock adiabats are calculated in the pressure range 1
Mbar-10 Gbar with two atomic-structure models: the atom in a spherical cell and
the atom in a jellium of charges. These quantum self-consistent-field models
include shell effects, which have a strong impact on pressure and shock
velocity along the... | physics.plasm-ph physics.atom-ph | rankinehugoniot shock adiabats are calculated in the pressure range 1 mbar10 gbar with two atomicstructure models the atom in a spherical cell and the atom in a jellium of charges these quantum selfconsistentfield models include shell effects which have a strong impact on pressure and shock velocity along the shock adi... | [['rankinehugoniot', 'shock', 'adiabats', 'are', 'calculated', 'in', 'the', 'pressure', 'range', '1', 'mbar10', 'gbar', 'with', 'two', 'atomicstructure', 'models', 'the', 'atom', 'in', 'a', 'spherical', 'cell', 'and', 'the', 'atom', 'in', 'a', 'jellium', 'of', 'charges', 'these', 'quantum', 'selfconsistentfield', 'mode... | [-0.08950586687925077, 0.16972025443778135, -0.03907281824192682, 0.052071260181418076, -0.019226199833589586, -0.11336415581578432, 0.03367500535082505, 0.3975715004774027, -0.2101180372694724, -0.28300245187440237, 0.043547212801397193, -0.2833127248274206, -0.01975181795518607, 0.1935543068792931, 0.0442583227880721... |
707.0014 | Testing Gluino Spin with Three-Body Decays | We examine the possibility of distinguishing a supersymmetric gluino from a
Kaluza-Klein gluon of universal extra dimensions (UED) at the Large Hadron
Collider (LHC). We focus on the case when all kinematically allowed tree-level
decays of this particle are 3-body decays into two jets and a massive daughter
(typicall... | hep-ph | we examine the possibility of distinguishing a supersymmetric gluino from a kaluzaklein gluon of universal extra dimensions ued at the large hadron collider lhc we focus on the case when all kinematically allowed treelevel decays of this particle are 3body decays into two jets and a massive daughter typically weak gaug... | [['we', 'examine', 'the', 'possibility', 'of', 'distinguishing', 'a', 'supersymmetric', 'gluino', 'from', 'a', 'kaluzaklein', 'gluon', 'of', 'universal', 'extra', 'dimensions', 'ued', 'at', 'the', 'large', 'hadron', 'collider', 'lhc', 'we', 'focus', 'on', 'the', 'case', 'when', 'all', 'kinematically', 'allowed', 'treel... | [-0.08047982811623544, 0.2485151206731705, -0.06971519365563897, 0.18087518568567795, -0.047667828709904124, -0.1290327514596055, 0.006247593284201768, 0.30893943325667844, -0.17626704832116152, -0.31602740074947844, 0.04094822864345292, -0.27718671886936014, -0.010341718768632394, 0.17170914455368383, 0.04676945042007... |
707.0015 | Investigations in Two-Dimensional Quantum Field Theory by the Bootstrap
and TCSA Methods | This thesis contains three main parts, which are largely independent. In the
first part we deal with the boundary bootstrap in supersymmetric factorized
scattering theory. We give a description of supersymmetry in the case when the
space is a half-line and present rules for the determination of the
representations in... | hep-th | this thesis contains three main parts which are largely independent in the first part we deal with the boundary bootstrap in supersymmetric factorized scattering theory we give a description of supersymmetry in the case when the space is a halfline and present rules for the determination of the representations in which... | [['this', 'thesis', 'contains', 'three', 'main', 'parts', 'which', 'are', 'largely', 'independent', 'in', 'the', 'first', 'part', 'we', 'deal', 'with', 'the', 'boundary', 'bootstrap', 'in', 'supersymmetric', 'factorized', 'scattering', 'theory', 'we', 'give', 'a', 'description', 'of', 'supersymmetry', 'in', 'the', 'cas... | [-0.12127655196820754, 0.10574949144278037, -0.07986027669247198, 0.05680949519204611, -0.028238078477610458, -0.08771663000521704, 0.03842606166086848, 0.32578532321028897, -0.2415494583243811, -0.2574203152680534, 0.12445796620844725, -0.27443213847918985, -0.15248696407895548, 0.15694121288410406, 0.0020926279618879... |
707.0016 | Abstract polymer models with general pair interactions | A convergence criterion of cluster expansion is presented in the case of an
abstract polymer system with general pair interactions (i.e. not necessarily
hard core or repulsive). As a concrete example, the low temperature disordered
phase of the BEG model with infinite range interactions, decaying polynomially
as $1/r... | math-ph math.CO math.MP | a convergence criterion of cluster expansion is presented in the case of an abstract polymer system with general pair interactions ie not necessarily hard core or repulsive as a concrete example the low temperature disordered phase of the beg model with infinite range interactions decaying polynomially as 1rdlambda wit... | [['a', 'convergence', 'criterion', 'of', 'cluster', 'expansion', 'is', 'presented', 'in', 'the', 'case', 'of', 'an', 'abstract', 'polymer', 'system', 'with', 'general', 'pair', 'interactions', 'ie', 'not', 'necessarily', 'hard', 'core', 'or', 'repulsive', 'as', 'a', 'concrete', 'example', 'the', 'low', 'temperature', '... | [-0.13071060778719246, 0.2016320083699504, -0.05547399470336078, 0.07879392399598717, -0.04241818353058953, -0.2253563753055299, -0.025939122645878325, 0.3638464108876446, -0.2592144601923578, -0.2602968642889869, 0.09448386331353628, -0.28085690720335527, -0.07360279429064807, 0.11876852270763587, 0.06812462245579809,... |
707.0017 | A Morse type uniqueness theorem for non-parametric minimizing
hypersurfaces | A classical result about minimal geodesics on R^2 with Z^2 periodic metric
that goes back to H.M. Morse asserts that a minimal geodesic that is asymptotic
to a periodic minimal geodesic cannot intersect any periodic minimal geodesic
of the same period. This paper treats a similar theorem for nonparametric
minimizing ... | math.AP math.DS | a classical result about minimal geodesics on r2 with z2 periodic metric that goes back to hm morse asserts that a minimal geodesic that is asymptotic to a periodic minimal geodesic cannot intersect any periodic minimal geodesic of the same period this paper treats a similar theorem for nonparametric minimizing hypersu... | [['a', 'classical', 'result', 'about', 'minimal', 'geodesics', 'on', 'r2', 'with', 'z2', 'periodic', 'metric', 'that', 'goes', 'back', 'to', 'hm', 'morse', 'asserts', 'that', 'a', 'minimal', 'geodesic', 'that', 'is', 'asymptotic', 'to', 'a', 'periodic', 'minimal', 'geodesic', 'can', 'not', 'intersect', 'any', 'periodic... | [-0.2161891420802741, 0.10033735412923592, -0.10765119357062365, 0.12263674236166833, -0.11757685930760049, -0.2123043147791455, 0.055413966816015986, 0.302686350281114, -0.2524693680009735, -0.21832527592778206, 0.06938472317371851, -0.3107059015405934, -0.13056767780556164, 0.18138954221312678, -0.22406709170552777, ... |
707.0018 | AC susceptibility and $^{51}$V NMR study of MnV$_2$O$_4$ | We report $^{51}$V zero-field NMR of manganese vanadate spinel of
MnV$_2$O$_4$, together with both ac and dc magnetization measurements. The
field and temperature dependence of ac susceptibilities show a
reentrant-spin-glass-like behavior below the ferrimagnetic(FEM) ordering
temperature. The zero-field NMR spectrum ... | cond-mat.str-el | we report 51v zerofield nmr of manganese vanadate spinel of mnv_2o_4 together with both ac and dc magnetization measurements the field and temperature dependence of ac susceptibilities show a reentrantspinglasslike behavior below the ferrimagneticfem ordering temperature the zerofield nmr spectrum consists of multiple ... | [['we', 'report', '51v', 'zerofield', 'nmr', 'of', 'manganese', 'vanadate', 'spinel', 'of', 'mnv_2o_4', 'together', 'with', 'both', 'ac', 'and', 'dc', 'magnetization', 'measurements', 'the', 'field', 'and', 'temperature', 'dependence', 'of', 'ac', 'susceptibilities', 'show', 'a', 'reentrantspinglasslike', 'behavior', '... | [-0.2093687982764095, 0.24176934541668743, 0.0008937177434563637, -0.04428830181830563, -0.05917916200705804, -0.08938571565784514, 0.11748512359336019, 0.3800166891189292, -0.26007237285375595, -0.31490631960332394, 0.04260309624485672, -0.36801538076251744, -0.04024885765014915, 0.14377520587295295, 0.140063149146735... |
707.0019 | Probing the Dust and Gas in the Transitional Disk of CS Cha with Spitzer | Here we present the Spitzer IRS spectrum of CS Cha, a member of the ~2 Myr
old Chamaeleon star-forming region, which reveals an optically thick
circumstellar disk truncated at ~43 AU, the largest hole modeled in a
transitional disk to date. Within this inner hole, ~5x10^-5 lunar masses of
dust are located in a small ... | astro-ph | here we present the spitzer irs spectrum of cs cha a member of the 2 myr old chamaeleon starforming region which reveals an optically thick circumstellar disk truncated at 43 au the largest hole modeled in a transitional disk to date within this inner hole 5x105 lunar masses of dust are located in a small optically thi... | [['here', 'we', 'present', 'the', 'spitzer', 'irs', 'spectrum', 'of', 'cs', 'cha', 'a', 'member', 'of', 'the', '2', 'myr', 'old', 'chamaeleon', 'starforming', 'region', 'which', 'reveals', 'an', 'optically', 'thick', 'circumstellar', 'disk', 'truncated', 'at', '43', 'au', 'the', 'largest', 'hole', 'modeled', 'in', 'a',... | [-0.03147070426916685, 0.09594538597344011, -0.019141188018349468, 0.04757145270172377, -0.03433968516446613, -0.13606336160067153, 0.015465310012541748, 0.4583046831635397, -0.15997792385629753, -0.30938663040357295, 0.05714229822149547, -0.2613279560994385, -0.004549907362876247, 0.12332211509034205, -0.0520612890082... |
707.002 | Minimal Seesaw as an Ultraviolet Insensitive Cure for the Problems of
Anomaly Mediation | We show that an intermediate scale supersymmetric left-right seesaw scenario
with automatic R-parity conservation can cure the problem of tachyonic slepton
masses that arises when supersymmetry is broken by anomaly mediation, while
preserving ultraviolet insensitivity. The reason for this is the existence of
light B ... | hep-ph hep-th | we show that an intermediate scale supersymmetric leftright seesaw scenario with automatic rparity conservation can cure the problem of tachyonic slepton masses that arises when supersymmetry is broken by anomaly mediation while preserving ultraviolet insensitivity the reason for this is the existence of light b l 2 hi... | [['we', 'show', 'that', 'an', 'intermediate', 'scale', 'supersymmetric', 'leftright', 'seesaw', 'scenario', 'with', 'automatic', 'rparity', 'conservation', 'can', 'cure', 'the', 'problem', 'of', 'tachyonic', 'slepton', 'masses', 'that', 'arises', 'when', 'supersymmetry', 'is', 'broken', 'by', 'anomaly', 'mediation', 'w... | [-0.11011708268222023, 0.2852512076808241, 0.013291999990581237, 0.22449749756351786, -0.1106431250202846, -0.255977129982289, -0.02180654128777802, 0.3276868510168997, -0.20559665711319192, -0.3451989548914927, 0.05574306057260788, -0.2781984679935936, -0.062640858348459, 0.04233880280616119, -0.02833581902705965, 0.0... |
707.0021 | Towards Fault Tolerant Adiabatic Quantum Computation | I show how to protect adiabatic quantum computation (AQC) against decoherence
and certain control errors, using a hybrid methodology involving dynamical
decoupling, subsystem and stabilizer codes, and energy gaps. Corresponding
error bounds are derived. As an example I show how to perform
decoherence-protected AQC ag... | quant-ph | i show how to protect adiabatic quantum computation aqc against decoherence and certain control errors using a hybrid methodology involving dynamical decoupling subsystem and stabilizer codes and energy gaps corresponding error bounds are derived as an example i show how to perform decoherenceprotected aqc against loca... | [['i', 'show', 'how', 'to', 'protect', 'adiabatic', 'quantum', 'computation', 'aqc', 'against', 'decoherence', 'and', 'certain', 'control', 'errors', 'using', 'a', 'hybrid', 'methodology', 'involving', 'dynamical', 'decoupling', 'subsystem', 'and', 'stabilizer', 'codes', 'and', 'energy', 'gaps', 'corresponding', 'error... | [-0.14195360107204089, 0.10876853239320693, -0.09214678369663978, 0.1456521037823852, 0.05924562371980686, -0.25524436055834837, 0.050181422727361605, 0.3261651281768886, -0.32672025903817625, -0.3368819953443912, 0.10686794235012852, -0.2528450187528506, -0.14287641843279394, 0.23285198881505773, -0.07652622814986479,... |
707.0022 | Lagrangian Mechanics and Variational Integrators on Two-Spheres | Euler-Lagrange equations and variational integrators are developed for
Lagrangian mechanical systems evolving on a product of two-spheres. The
geometric structure of a product of two-spheres is carefully considered in
order to obtain global equations of motion. Both continuous equations of motion
and variational inte... | math.NA | eulerlagrange equations and variational integrators are developed for lagrangian mechanical systems evolving on a product of twospheres the geometric structure of a product of twospheres is carefully considered in order to obtain global equations of motion both continuous equations of motion and variational integrators... | [['eulerlagrange', 'equations', 'and', 'variational', 'integrators', 'are', 'developed', 'for', 'lagrangian', 'mechanical', 'systems', 'evolving', 'on', 'a', 'product', 'of', 'twospheres', 'the', 'geometric', 'structure', 'of', 'a', 'product', 'of', 'twospheres', 'is', 'carefully', 'considered', 'in', 'order', 'to', 'o... | [-0.15106119047384708, 0.04255881721526384, -0.10309522245824337, 0.10413954468537122, -0.08991602192819119, -0.08767692468315363, -0.06528982352279127, 0.3251523794233799, -0.3005647682417184, -0.3328951332569122, 0.13494553432054818, -0.22126746404916048, -0.14756716087833047, 0.1843420434873551, -0.06416206180676817... |
707.0023 | pi N to Multi-pi N Scattering in the 1/N_c Expansion | We extend the 1/N_c meson-baryon scattering formalism to pi N to multi-pi N
case. We first show that the leading-order large N_c processes proceed through
resonant intermediate states (e.g., rho N or pi Delta). We find that the pole
structure of baryon resonances can be uniquely identified by their
(non)appearance in... | hep-ph | we extend the 1n_c mesonbaryon scattering formalism to pi n to multipi n case we first show that the leadingorder large n_c processes proceed through resonant intermediate states eg rho n or pi delta we find that the pole structure of baryon resonances can be uniquely identified by their nonappearance in eta n or mixed... | [['we', 'extend', 'the', '1n_c', 'mesonbaryon', 'scattering', 'formalism', 'to', 'pi', 'n', 'to', 'multipi', 'n', 'case', 'we', 'first', 'show', 'that', 'the', 'leadingorder', 'large', 'n_c', 'processes', 'proceed', 'through', 'resonant', 'intermediate', 'states', 'eg', 'rho', 'n', 'or', 'pi', 'delta', 'we', 'find', 't... | [-0.19173496430351708, 0.2880120817106217, -0.11343131121636058, 0.08768524009113511, -0.0385143071723481, -0.12141935545951128, 0.12641543530238172, 0.2895019011572003, -0.25095522513147445, -0.22906737675269445, -0.08405177802972806, -0.3360770269297063, -0.10801360701443627, 0.019635794591158627, 0.11793455354248485... |
707.0024 | An Extensive Collection of Stellar Wind X-ray Source Region Emission
Line Parameters,Temperatures, Velocities, and Their Radial Distributions as
Obtained from Chandra Observations of 17 OB Stars | Chandra high energy resolution observations have now been obtained from
numerous non-peculiar O and early B stars. The observed X-ray emission line
properties differ from pre-launch predictions, and the interpretations are
still problematic. We present a straightforward analysis of a broad collection
of OB stellar li... | astro-ph | chandra high energy resolution observations have now been obtained from numerous nonpeculiar o and early b stars the observed xray emission line properties differ from prelaunch predictions and the interpretations are still problematic we present a straightforward analysis of a broad collection of ob stellar line profi... | [['chandra', 'high', 'energy', 'resolution', 'observations', 'have', 'now', 'been', 'obtained', 'from', 'numerous', 'nonpeculiar', 'o', 'and', 'early', 'b', 'stars', 'the', 'observed', 'xray', 'emission', 'line', 'properties', 'differ', 'from', 'prelaunch', 'predictions', 'and', 'the', 'interpretations', 'are', 'still'... | [-0.03291834693023593, 0.12383774419734603, -0.01723066635241502, 0.12875652328710863, -0.08664071743990459, -0.0983227934663913, 0.06976102510282302, 0.5060226275177484, -0.16697486508301937, -0.34381374829184536, 0.06627157412919352, -0.32758095572713053, 0.007501538775770573, 0.20105483252310966, -0.0052377620070112... |
707.0025 | On quantization of massive non-Abelian gauge fields | A simpler method of quantization is given for massive gauge theories. This
method gives the same results as those of the conventional massive gauge theory
with ghost and Higgs fields under the Higgs mass. Besides, we point out
physical importance of helicity zero states in non-Abelian gauge theories even
in massless ... | hep-ph | a simpler method of quantization is given for massive gauge theories this method gives the same results as those of the conventional massive gauge theory with ghost and higgs fields under the higgs mass besides we point out physical importance of helicity zero states in nonabelian gauge theories even in massless case f... | [['a', 'simpler', 'method', 'of', 'quantization', 'is', 'given', 'for', 'massive', 'gauge', 'theories', 'this', 'method', 'gives', 'the', 'same', 'results', 'as', 'those', 'of', 'the', 'conventional', 'massive', 'gauge', 'theory', 'with', 'ghost', 'and', 'higgs', 'fields', 'under', 'the', 'higgs', 'mass', 'besides', 'w... | [-0.1109049198782762, 0.21585250819060073, -0.0798659506986399, 0.12854956017200198, -0.10521879250162773, -0.16700026312361607, 0.031686164453112925, 0.33935373127879054, -0.141886338429379, -0.2873114543768127, 0.029017647934993833, -0.20516255187142765, -0.14489741132626038, 0.15826079353763398, -0.03229288381179062... |
707.0026 | Introducing a Probabilistic Structure on Sequential Dynamical Systems,
Simulation and Reduction of Probabilistic Sequential Networks | A probabilistic structure on sequential dynamical systems is introduced here,
the new model will be called Probabilistic Sequential Network, PSN. The
morphisms of Probabilistic Sequential Networks are defined using two algebraic
conditions. It is proved here that two homomorphic Probabilistic Sequential
Networks have... | q-bio.GN math.PR q-bio.MN | a probabilistic structure on sequential dynamical systems is introduced here the new model will be called probabilistic sequential network psn the morphisms of probabilistic sequential networks are defined using two algebraic conditions it is proved here that two homomorphic probabilistic sequential networks have the s... | [['a', 'probabilistic', 'structure', 'on', 'sequential', 'dynamical', 'systems', 'is', 'introduced', 'here', 'the', 'new', 'model', 'will', 'be', 'called', 'probabilistic', 'sequential', 'network', 'psn', 'the', 'morphisms', 'of', 'probabilistic', 'sequential', 'networks', 'are', 'defined', 'using', 'two', 'algebraic',... | [-0.16984828625691636, 0.04529877183427298, -0.09067080302011905, 0.10267399906712983, -0.07085380981419692, -0.17759936554975123, 0.007918610855252767, 0.40758259509861167, -0.42560103888224277, -0.19091033386256623, 0.11823302966409496, -0.21744261009200494, -0.1390122067116733, 0.15526648849600508, -0.12434963115528... |
707.0027 | The Boltzmann-Hamel Equations for Optimal Control | We extend the Boltzmann-Hamel equations to the optimal control setting,
producing a set of equations for both kinematic and dynamic nonholonomic
optimal control problems. In particular, we will show the dynamic optimal
control problem can be written as a minimal set of 4n-2m first order
differential equations of moti... | math.OC | we extend the boltzmannhamel equations to the optimal control setting producing a set of equations for both kinematic and dynamic nonholonomic optimal control problems in particular we will show the dynamic optimal control problem can be written as a minimal set of 4n2m first order differential equations of motion | [['we', 'extend', 'the', 'boltzmannhamel', 'equations', 'to', 'the', 'optimal', 'control', 'setting', 'producing', 'a', 'set', 'of', 'equations', 'for', 'both', 'kinematic', 'and', 'dynamic', 'nonholonomic', 'optimal', 'control', 'problems', 'in', 'particular', 'we', 'will', 'show', 'the', 'dynamic', 'optimal', 'contro... | [-0.17549528393577388, 0.032343242674114855, -0.05185700285228643, 0.05463401733481504, -0.14852141168840388, -0.08877425726027564, 0.006855954198127097, 0.30671377263051713, -0.3619974353846083, -0.3221332866777765, 0.15453279641347917, -0.2235364695475932, -0.14791249919762003, 0.2323362888332377, -0.1274547407284696... |
707.0028 | The spectral energy distribution of quiescent black hole X-ray binaries:
new constraints from Spitzer | (Abridged) Among the various issues that remain open in the field of
accretion onto black hole X-ray binaries (BHBs) is the way the gas accretes at
very low Eddington ratios, in the so-called quiescent regime. While there is
general agreement that the X-rays are produced by a population of high-energy
electrons near ... | astro-ph | abridged among the various issues that remain open in the field of accretion onto black hole xray binaries bhbs is the way the gas accretes at very low eddington ratios in the socalled quiescent regime while there is general agreement that the xrays are produced by a population of highenergy electrons near to the bh th... | [['abridged', 'among', 'the', 'various', 'issues', 'that', 'remain', 'open', 'in', 'the', 'field', 'of', 'accretion', 'onto', 'black', 'hole', 'xray', 'binaries', 'bhbs', 'is', 'the', 'way', 'the', 'gas', 'accretes', 'at', 'very', 'low', 'eddington', 'ratios', 'in', 'the', 'socalled', 'quiescent', 'regime', 'while', 't... | [-0.035699141867975785, 0.14679972850480827, -0.037130775830661086, 0.12949054790029335, -0.08312922618509729, -0.07307113531219252, 0.048778852984561756, 0.4638226417666775, -0.19494652367252224, -0.3410602314133292, 0.06689027712238416, -0.3328118849964023, 0.044336663657736225, 0.22840955096328536, -0.01281339186796... |
707.0029 | Zooming into the coexisting regime of ferromagnetism and
superconductivity in ErRh4B4 single crystals | High resolution measurements of the dynamic magnetic susceptibility are
reported for ferromagnetic re-entrant superconductor, ErRh$_{4}$B$_{4}$.
Detailed investigation of the coexisting regime reveals unusual
temperature-asymmetric and magnetically anisotropic behavior. The
superconducting phase appears via a series ... | cond-mat.str-el cond-mat.supr-con | high resolution measurements of the dynamic magnetic susceptibility are reported for ferromagnetic reentrant superconductor errh_4b_4 detailed investigation of the coexisting regime reveals unusual temperatureasymmetric and magnetically anisotropic behavior the superconducting phase appears via a series of discontinuou... | [['high', 'resolution', 'measurements', 'of', 'the', 'dynamic', 'magnetic', 'susceptibility', 'are', 'reported', 'for', 'ferromagnetic', 'reentrant', 'superconductor', 'errh_4b_4', 'detailed', 'investigation', 'of', 'the', 'coexisting', 'regime', 'reveals', 'unusual', 'temperatureasymmetric', 'and', 'magnetically', 'an... | [-0.2215529665365025, 0.21482667707922784, -0.07757413074035537, -0.010753630108383455, -0.09499669213299498, -0.14451014344354696, 0.11365408844060519, 0.34350559962066735, -0.200354677483891, -0.270882331258194, 0.048028718807141886, -0.3034875925037671, -0.13937168720594578, 0.13304800532800568, 0.07409635172789973,... |
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