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 |
|---|---|---|---|---|---|---|
710.2153 | Phase Separation and Charge Transfer in a K-doped C60 Monolayer on
Ag(001) | We have performed a scanning tunneling microscopy and spectroscopy study of
potassium-doped C60 monolayers (KxC60) on Ag(001) in the regime of x ~ 1. Low
temperature annealing (640 K) leads to the formation of two well-ordered KxC60
phases that exhibit differing levels of electron charge transfer. Further
annealing (... | cond-mat.mtrl-sci | we have performed a scanning tunneling microscopy and spectroscopy study of potassiumdoped c60 monolayers kxc60 on ag001 in the regime of x 1 low temperature annealing 640 k leads to the formation of two wellordered kxc60 phases that exhibit differing levels of electron charge transfer further annealing 710 k distills ... | [['we', 'have', 'performed', 'a', 'scanning', 'tunneling', 'microscopy', 'and', 'spectroscopy', 'study', 'of', 'potassiumdoped', 'c60', 'monolayers', 'kxc60', 'on', 'ag001', 'in', 'the', 'regime', 'of', 'x', '1', 'low', 'temperature', 'annealing', '640', 'k', 'leads', 'to', 'the', 'formation', 'of', 'two', 'wellordered... | [-0.17297059461227893, 0.23498416644904543, -0.07558790634879295, -0.030180503279381595, 0.0378364862408489, -0.1906589737161994, 0.18268536623526255, 0.40382627038394703, -0.21302419090643526, -0.2932082058971419, -0.013667972458471709, -0.3479858575936626, -0.0784177483552519, 0.13582040430868372, 0.06491820303832783... |
710.2154 | Effective superpotential and partial breaking of N=2 supersymmetry | We consider the effective superpotential of N=2, U(N) gauge model where N=2
supersymmetry is spontaneously broken to N=1. By the computation of loop
diagrams, we obtain a formula for the effective superpotential which is
deformed from the well-known form of the effective superpotential of N=1, U(N)
gauge model with a... | hep-th | we consider the effective superpotential of n2 un gauge model where n2 supersymmetry is spontaneously broken to n1 by the computation of loop diagrams we obtain a formula for the effective superpotential which is deformed from the wellknown form of the effective superpotential of n1 un gauge model with a tree level sup... | [['we', 'consider', 'the', 'effective', 'superpotential', 'of', 'n2', 'un', 'gauge', 'model', 'where', 'n2', 'supersymmetry', 'is', 'spontaneously', 'broken', 'to', 'n1', 'by', 'the', 'computation', 'of', 'loop', 'diagrams', 'we', 'obtain', 'a', 'formula', 'for', 'the', 'effective', 'superpotential', 'which', 'is', 'de... | [-0.14709826228472422, 0.23312906952539705, -0.05608223499027344, 0.13290234977151003, -0.06464697050703865, -0.21953623248088472, 0.01962573025024162, 0.2639772518063491, -0.1388978696656677, -0.3279736112970156, 0.07017331235637923, -0.2373836399846763, -0.22215367959074253, -0.03436391211097252, -0.04405036541349957... |
710.2155 | Interpreting Recoil For Undergraduate Students | In this paper, I outline some problems in the students' understanding of the
explanation of recoil motion when introduced to them in the context of Newton's
third law. I propose to explain the origin of recoil from a microscopic point
of view, which emphasizes the exact mechanism leading to recoil. This mechanism
dif... | physics.ed-ph physics.class-ph | in this paper i outline some problems in the students understanding of the explanation of recoil motion when introduced to them in the context of newtons third law i propose to explain the origin of recoil from a microscopic point of view which emphasizes the exact mechanism leading to recoil this mechanism differs fro... | [['in', 'this', 'paper', 'i', 'outline', 'some', 'problems', 'in', 'the', 'students', 'understanding', 'of', 'the', 'explanation', 'of', 'recoil', 'motion', 'when', 'introduced', 'to', 'them', 'in', 'the', 'context', 'of', 'newtons', 'third', 'law', 'i', 'propose', 'to', 'explain', 'the', 'origin', 'of', 'recoil', 'fro... | [-0.06301010992600146, 0.10330883977473329, -0.13418469705336958, 0.08539824251410201, -0.14762694603088525, -0.1276914812539012, 0.06312715698144647, 0.3136984767272658, -0.30691700139928846, -0.3167926322053605, 0.036115890375227416, -0.26128247733133925, -0.1881046994939583, 0.19707148704985414, -0.10834207866392141... |
710.2156 | Collaborative OLAP with Tag Clouds: Web 2.0 OLAP Formalism and
Experimental Evaluation | Increasingly, business projects are ephemeral. New Business Intelligence
tools must support ad-lib data sources and quick perusal. Meanwhile, tag clouds
are a popular community-driven visualization technique. Hence, we investigate
tag-cloud views with support for OLAP operations such as roll-ups, slices,
dices, clust... | cs.DB | increasingly business projects are ephemeral new business intelligence tools must support adlib data sources and quick perusal meanwhile tag clouds are a popular communitydriven visualization technique hence we investigate tagcloud views with support for olap operations such as rollups slices dices clustering and drill... | [['increasingly', 'business', 'projects', 'are', 'ephemeral', 'new', 'business', 'intelligence', 'tools', 'must', 'support', 'adlib', 'data', 'sources', 'and', 'quick', 'perusal', 'meanwhile', 'tag', 'clouds', 'are', 'a', 'popular', 'communitydriven', 'visualization', 'technique', 'hence', 'we', 'investigate', 'tagclou... | [-0.10946393555840822, 0.00782900772187363, -0.04367931606463605, 0.1353504555127411, -0.18920056630978016, -0.1849806107606532, 0.0823854407170546, 0.49907939649980376, -0.2511670829241026, -0.3325842674994082, 0.14947431691581625, -0.3104063390271255, -0.14757917700680317, 0.1818100974024101, -0.08150179345695371, 0.... |
710.2157 | Ongoing Assembly of Massive Galaxies by Major Merging in Large Groups
and Clusters from the SDSS | We investigate the incidence of major mergers creating >10e11 Msun galaxies
in present-day groups and clusters more massive than 2.5e13 Msun. We identify
38 pairs of massive galaxies with mutual tidal interaction signatures selected
from >5000 galaxies with >5e10 Msun that reside in 845 such groups. We fit the
images... | astro-ph | we investigate the incidence of major mergers creating 10e11 msun galaxies in presentday groups and clusters more massive than 25e13 msun we identify 38 pairs of massive galaxies with mutual tidal interaction signatures selected from 5000 galaxies with 5e10 msun that reside in 845 such groups we fit the images of each ... | [['we', 'investigate', 'the', 'incidence', 'of', 'major', 'mergers', 'creating', '10e11', 'msun', 'galaxies', 'in', 'presentday', 'groups', 'and', 'clusters', 'more', 'massive', 'than', '25e13', 'msun', 'we', 'identify', '38', 'pairs', 'of', 'massive', 'galaxies', 'with', 'mutual', 'tidal', 'interaction', 'signatures',... | [-0.11343400876869188, 0.14709667233621765, -0.04442643861632466, 0.12265603615183354, -0.05180587113649367, -0.022742260962464202, 0.016018943839717185, 0.4364931115645771, -0.1171090727836122, -0.3694372212521418, 0.032183776258123444, -0.3232997367907872, -0.039517441215849984, 0.18449605354090076, -0.00275837385962... |
710.2158 | The double-Reissner-Nordstrom solution and the interaction force between
two spherically symmetric charged particles | The physical representation of the general double-Reissner-Nordstrom solution
is obtained by rewriting the N=2 Breton-Manko-Aguilar electrostatic solution in
the Varzugin-Chistyakov parametrization (M_i, Q_i, R). A concise analytical
formula is derived for the interaction force between two arbitrary
Reissner-Nordstro... | gr-qc | the physical representation of the general doublereissnernordstrom solution is obtained by rewriting the n2 bretonmankoaguilar electrostatic solution in the varzuginchistyakov parametrization m_i q_i r a concise analytical formula is derived for the interaction force between two arbitrary reissnernordstrom constituents... | [['the', 'physical', 'representation', 'of', 'the', 'general', 'doublereissnernordstrom', 'solution', 'is', 'obtained', 'by', 'rewriting', 'the', 'n2', 'bretonmankoaguilar', 'electrostatic', 'solution', 'in', 'the', 'varzuginchistyakov', 'parametrization', 'm_i', 'q_i', 'r', 'a', 'concise', 'analytical', 'formula', 'is... | [-0.19617014429006244, 0.12262687297568904, -0.07173370831315556, 0.0615051708075278, -0.014627614989876747, -0.1732170764702342, -0.03960315151620777, 0.2907552388046057, -0.18809778774307379, -0.31383048223271487, 0.011613584196780838, -0.2921993225632656, -0.11568285998768144, 0.11823138555571917, 0.0388848521190905... |
710.2159 | Nucleon electromagnetic form factors with Wilson fermions | The nucleon electromagnetic form factors continue to be of major interest for
experimentalists and phenomenologists alike. They provide important insights
into the structure of nuclear matter. For a range of interesting momenta they
can be calculated on the lattice. The limiting factor continues to be the value
of th... | hep-lat | the nucleon electromagnetic form factors continue to be of major interest for experimentalists and phenomenologists alike they provide important insights into the structure of nuclear matter for a range of interesting momenta they can be calculated on the lattice the limiting factor continues to be the value of the pio... | [['the', 'nucleon', 'electromagnetic', 'form', 'factors', 'continue', 'to', 'be', 'of', 'major', 'interest', 'for', 'experimentalists', 'and', 'phenomenologists', 'alike', 'they', 'provide', 'important', 'insights', 'into', 'the', 'structure', 'of', 'nuclear', 'matter', 'for', 'a', 'range', 'of', 'interesting', 'moment... | [-0.07341021215781951, 0.27375076998932624, -0.10627887087862174, 0.1185524332552002, -0.06065505333670164, -0.07344873726684362, 0.059360120012663685, 0.38592099235990107, -0.15478986487365687, -0.3154994409280614, 0.053402777062729, -0.27206944276650363, -0.025579596183095604, 0.1771877955000561, 0.07080435004303208,... |
710.216 | A search for pulsed radio emission from anomalous X-ray pulsar 4U
0142+61 at the frequency of 111 MHz | We have searched for pulsed radio emission from magnetar 4U 0142+61 at the
frequency of 111 MHz. No pulsed signal was detected from this source. Upper
limits for mean flux density are 0.9 - 9 mJy depending on assumed duty cycle
(.05 - .5) of the pulsar.
| astro-ph | we have searched for pulsed radio emission from magnetar 4u 014261 at the frequency of 111 mhz no pulsed signal was detected from this source upper limits for mean flux density are 09 9 mjy depending on assumed duty cycle 05 5 of the pulsar | [['we', 'have', 'searched', 'for', 'pulsed', 'radio', 'emission', 'from', 'magnetar', '4u', '014261', 'at', 'the', 'frequency', 'of', '111', 'mhz', 'no', 'pulsed', 'signal', 'was', 'detected', 'from', 'this', 'source', 'upper', 'limits', 'for', 'mean', 'flux', 'density', 'are', '09', '9', 'mjy', 'depending', 'on', 'ass... | [-0.12008726029760308, 0.2104716916465097, 0.036548448809319074, 0.08933439367295554, -0.08610716582172447, -0.11293281505091322, 0.15721986829820606, 0.501866822462115, -0.08869796234907376, -0.4239888446198569, 0.1303731935102001, -0.2837774999439716, 0.10258421136273278, 0.3203805390745401, 0.023126942705776955, -0.... |
710.2161 | Enhancement of surface activity in CO oxidation on Pt(110) through
spatiotemporal laser actuation | We explore the effect of spatiotemporally varying substrate temperature
profiles on the dynamics and resulting reaction rate enhancement for the
catalytic oxidation of CO on Pt(110). The catalytic surface is "addressed" by a
focused laser beam whose motion is computer-controlled. The averaged reaction
rate is observe... | nlin.PS | we explore the effect of spatiotemporally varying substrate temperature profiles on the dynamics and resulting reaction rate enhancement for the catalytic oxidation of co on pt110 the catalytic surface is addressed by a focused laser beam whose motion is computercontrolled the averaged reaction rate is observed to unde... | [['we', 'explore', 'the', 'effect', 'of', 'spatiotemporally', 'varying', 'substrate', 'temperature', 'profiles', 'on', 'the', 'dynamics', 'and', 'resulting', 'reaction', 'rate', 'enhancement', 'for', 'the', 'catalytic', 'oxidation', 'of', 'co', 'on', 'pt110', 'the', 'catalytic', 'surface', 'is', 'addressed', 'by', 'a',... | [-0.10643593590982535, 0.16317154398280695, -0.04502515260340002, 0.0025436262927811455, -0.002182132564485073, -0.10138199447918637, 0.05907690475290975, 0.4301957938084264, -0.28564793048541487, -0.2972842602312197, 0.0657247322651753, -0.24279264362965836, -0.10332624053145632, 0.23194573816187955, -0.01154874185284... |
710.2162 | Construction and Analysis of Projected Deformed Products | We introduce a deformed product construction for simple polytopes in terms of
lower-triangular block matrix representations. We further show how Gale duality
can be employed for the construction and for the analysis of deformed products
such that specified faces (e.g. all the k-faces) are ``strictly preserved''
under... | math.MG math.CO | we introduce a deformed product construction for simple polytopes in terms of lowertriangular block matrix representations we further show how gale duality can be employed for the construction and for the analysis of deformed products such that specified faces eg all the kfaces are strictly preserved under projection t... | [['we', 'introduce', 'a', 'deformed', 'product', 'construction', 'for', 'simple', 'polytopes', 'in', 'terms', 'of', 'lowertriangular', 'block', 'matrix', 'representations', 'we', 'further', 'show', 'how', 'gale', 'duality', 'can', 'be', 'employed', 'for', 'the', 'construction', 'and', 'for', 'the', 'analysis', 'of', 'd... | [-0.1003639593229189, 0.07942551730093828, -0.07786291301414207, 0.07185190224525606, -0.055174372353396575, -0.13779602346911127, 0.017646361097621802, 0.36117219557514885, -0.3071033425276055, -0.23244534063813083, 0.11789921489748899, -0.2833158708123777, -0.18292772934444576, 0.13624052658349603, -0.175774078339320... |
710.2163 | $O(p^6)$ extension of the large--$N_C$ partial wave dispersion relations | Continuing our previous work(JHEP 0706:030,2007), large--$N_C$ techniques and
partial wave dispersion relations are used to discuss $\pi\pi$ scattering
amplitudes. We get a set of predictions for $O(p^6)$ low-energy chiral
perturbation theory couplings. They are provided in terms of the masses and
decay widths of sca... | hep-ph | continuing our previous workjhep 07060302007 largen_c techniques and partial wave dispersion relations are used to discuss pipi scattering amplitudes we get a set of predictions for op6 lowenergy chiral perturbation theory couplings they are provided in terms of the masses and decay widths of scalar and vector mesons | [['continuing', 'our', 'previous', 'workjhep', '07060302007', 'largen_c', 'techniques', 'and', 'partial', 'wave', 'dispersion', 'relations', 'are', 'used', 'to', 'discuss', 'pipi', 'scattering', 'amplitudes', 'we', 'get', 'a', 'set', 'of', 'predictions', 'for', 'op6', 'lowenergy', 'chiral', 'perturbation', 'theory', 'c... | [-0.1570540382223123, 0.227449222366609, -0.06281093599112786, 0.16252526470824427, -0.07765396745146616, -0.06857606322180641, 0.043005072033417455, 0.34477729556839104, -0.18758514094287934, -0.19793615384918192, -0.003286962506219583, -0.368072880330779, -0.07916469450878061, 0.12152620228817282, 0.11346849388159487... |
710.2164 | Quantum Gravitational Collapse and Hawking Radiation in 2+1 Dimensions | We develop the canonical theory of gravitational collapse in 2+1 dimensions
with a negative cosmological constant and obtain exact solutions of the
Wheeler--DeWitt equation regularized on a lattice. We employ these solutions to
derive the Hawking radiation from black holes formed in all models of dust
collapse. We ob... | gr-qc astro-ph hep-th | we develop the canonical theory of gravitational collapse in 21 dimensions with a negative cosmological constant and obtain exact solutions of the wheelerdewitt equation regularized on a lattice we employ these solutions to derive the hawking radiation from black holes formed in all models of dust collapse we obtain an... | [['we', 'develop', 'the', 'canonical', 'theory', 'of', 'gravitational', 'collapse', 'in', '21', 'dimensions', 'with', 'a', 'negative', 'cosmological', 'constant', 'and', 'obtain', 'exact', 'solutions', 'of', 'the', 'wheelerdewitt', 'equation', 'regularized', 'on', 'a', 'lattice', 'we', 'employ', 'these', 'solutions', '... | [-0.11477000117859143, 0.07547747407172722, -0.10402953112895927, 0.11682597870050937, -0.07303204756373397, -0.1118525963427865, 0.022743178747443117, 0.2857198048319317, -0.20460247358856484, -0.2774082254857207, 0.09547015358534697, -0.323209449234936, -0.07912760918848535, 0.1392696312445606, 0.012453798886983551, ... |
710.2165 | Wide-field telescopes with a Mangin mirror | Two all-spherical catadioptric optical systems with a Mangin mirror are
described. The design A (aperture 500 mm, f/2.0) has flat field of view of 7
deg in diameter; the design B (aperture 1000 mm, f/1.7) has 10-deg flat field.
Both designs show near-diffraction-limited images. The D_80 diameter for the
design A in t... | astro-ph | two allspherical catadioptric optical systems with a mangin mirror are described the design a aperture 500 mm f20 has flat field of view of 7 deg in diameter the design b aperture 1000 mm f17 has 10deg flat field both designs show neardiffractionlimited images the d_80 diameter for the design a in the integral waveband... | [['two', 'allspherical', 'catadioptric', 'optical', 'systems', 'with', 'a', 'mangin', 'mirror', 'are', 'described', 'the', 'design', 'a', 'aperture', '500', 'mm', 'f20', 'has', 'flat', 'field', 'of', 'view', 'of', '7', 'deg', 'in', 'diameter', 'the', 'design', 'b', 'aperture', '1000', 'mm', 'f17', 'has', '10deg', 'flat... | [-0.10943201677396129, 0.10729713699259023, -0.030341821456025552, -0.042222379677944906, -0.052358429616269395, -0.15865832027724475, -0.035492367974808835, 0.45370989012667257, -0.1972989063972655, -0.34887773679513645, 0.15006216143508658, -0.25526878574433237, -0.08002283196482393, 0.2113922660947483, -0.0823087267... |
710.2166 | Local torus actions modeled on the standard representation | We introduce the notion of a local torus action modeled on the standard
representation (for simplicity, we call it a local torus action). It is a
generalization of a locally standard torus action and also an underlying
structure of a locally toric Lagrangian fibration. For a local torus action, we
define two invarian... | math.GT math.SG | we introduce the notion of a local torus action modeled on the standard representation for simplicity we call it a local torus action it is a generalization of a locally standard torus action and also an underlying structure of a locally toric lagrangian fibration for a local torus action we define two invariants calle... | [['we', 'introduce', 'the', 'notion', 'of', 'a', 'local', 'torus', 'action', 'modeled', 'on', 'the', 'standard', 'representation', 'for', 'simplicity', 'we', 'call', 'it', 'a', 'local', 'torus', 'action', 'it', 'is', 'a', 'generalization', 'of', 'a', 'locally', 'standard', 'torus', 'action', 'and', 'also', 'an', 'under... | [-0.21542895351162303, 0.057799329734369284, -0.11238998127666032, 0.09826448933296471, -0.10822116035345733, -0.16206027091498199, -0.003000143976342455, 0.34226181060423916, -0.2980998544039849, -0.21412591663598318, 0.1300570158582729, -0.20321550966614735, -0.1830129436996252, 0.1676545560699409, -0.184611433311844... |
710.2167 | The connection problem associated with a Selberg type integral and the
$q$-Racah polynomials | The connection problem associated with a Selberg type integral is solved. The
connection coefficients are given in terms of the $q$-Racah polynomials. As an
application of the explicit expression of the connection coefficients, examples
of the monodromy-invariant Hermitian form of non-diagonal type are presented.
It ... | math-ph math.CA math.MP | the connection problem associated with a selberg type integral is solved the connection coefficients are given in terms of the qracah polynomials as an application of the explicit expression of the connection coefficients examples of the monodromyinvariant hermitian form of nondiagonal type are presented it is notewort... | [['the', 'connection', 'problem', 'associated', 'with', 'a', 'selberg', 'type', 'integral', 'is', 'solved', 'the', 'connection', 'coefficients', 'are', 'given', 'in', 'terms', 'of', 'the', 'qracah', 'polynomials', 'as', 'an', 'application', 'of', 'the', 'explicit', 'expression', 'of', 'the', 'connection', 'coefficients... | [-0.19745048876142218, 0.0664285183904992, -0.007300596580737167, 0.09712859909493654, -0.11301010277950102, -0.14250248903408647, -0.08000598978140347, 0.3119567053629056, -0.2956645628880887, -0.2092696317722873, 0.12551720788894546, -0.2935202097860239, -0.28426517611221663, 0.21474981053717554, -0.03067529676777739... |
710.2168 | The (weak-$L^2$) Boundedness of The Quadratic Carleson Operator | We prove that the generalized Carleson operator with polynomial phase
function of degree two is of weak type (2,2). For this, we introduce a new
approach to the time-frequency analysis of the quadratic phase.
| math.CA | we prove that the generalized carleson operator with polynomial phase function of degree two is of weak type 22 for this we introduce a new approach to the timefrequency analysis of the quadratic phase | [['we', 'prove', 'that', 'the', 'generalized', 'carleson', 'operator', 'with', 'polynomial', 'phase', 'function', 'of', 'degree', 'two', 'is', 'of', 'weak', 'type', '22', 'for', 'this', 'we', 'introduce', 'a', 'new', 'approach', 'to', 'the', 'timefrequency', 'analysis', 'of', 'the', 'quadratic', 'phase']] | [-0.15949990392169533, 0.08576416475561392, -0.10965349848436959, 0.054348016034483033, -0.09666891790488187, -0.11641784265007385, 0.03636385911308667, 0.32136708991054225, -0.3532686519491322, -0.19771914503208415, 0.06718141363714547, -0.2091427882311537, -0.2308513248229728, 0.1791178791455048, -0.05330662719686242... |
710.2169 | On Liftings of Local Torus Actions to Fiber Bundles | In this note we define a lifting of a local torus action modeled on the
standard representation (we call it a local torus action for simplicity) to a
principal torus bundle, and show that there is an obstruction class for the
existence of liftings in the first cohomology of the fundamental group of the
orbit space wi... | math.GT math.AT | in this note we define a lifting of a local torus action modeled on the standard representation we call it a local torus action for simplicity to a principal torus bundle and show that there is an obstruction class for the existence of liftings in the first cohomology of the fundamental group of the orbit space with co... | [['in', 'this', 'note', 'we', 'define', 'a', 'lifting', 'of', 'a', 'local', 'torus', 'action', 'modeled', 'on', 'the', 'standard', 'representation', 'we', 'call', 'it', 'a', 'local', 'torus', 'action', 'for', 'simplicity', 'to', 'a', 'principal', 'torus', 'bundle', 'and', 'show', 'that', 'there', 'is', 'an', 'obstructi... | [-0.20871935721727147, 0.02390110175028601, -0.1073158835811961, 0.03979404387815345, -0.09239622322662223, -0.06762320550549175, 0.0008850142720245546, 0.3630870045012524, -0.34940245771600353, -0.18486289616914525, 0.12850007727073745, -0.17229519627477613, -0.20029694845359172, 0.18046625461729784, -0.14401894101812... |
710.217 | X-ray magnetic circular dichroism and photoemission study of the diluted
ferromagnetic semiconductor Zn$_{1-x}$Cr$_x$Te | We have performed x-ray magnetic circular dichroism (XMCD) and valence-band
photoemission studies of the diluted ferromagnetic semiconductor
Zn$_{1-x}$Cr$_x$Te. XMCD signals due to ferromagnetism were observed at the Cr
2p absorption edge. Comparison with atomic multiplet calculations suggests that
the magnetically a... | cond-mat.mtrl-sci cond-mat.str-el | we have performed xray magnetic circular dichroism xmcd and valenceband photoemission studies of the diluted ferromagnetic semiconductor zn_1xcr_xte xmcd signals due to ferromagnetism were observed at the cr 2p absorption edge comparison with atomic multiplet calculations suggests that the magnetically active component... | [['we', 'have', 'performed', 'xray', 'magnetic', 'circular', 'dichroism', 'xmcd', 'and', 'valenceband', 'photoemission', 'studies', 'of', 'the', 'diluted', 'ferromagnetic', 'semiconductor', 'zn_1xcr_xte', 'xmcd', 'signals', 'due', 'to', 'ferromagnetism', 'were', 'observed', 'at', 'the', 'cr', '2p', 'absorption', 'edge'... | [-0.12879480451406183, 0.2105098379568359, 0.05416979583020767, 0.029864120823533638, -0.014046865318011007, -0.15717336126987863, 0.05991407352216218, 0.4904987723769053, -0.2579459026455879, -0.30789837544864934, -0.09923177397855476, -0.41809628644715185, -0.06407243167252644, 0.09051509418919601, 0.1320512340702724... |
710.2171 | Physical and Geometrical Interpretation of the epsilon <= 0 Szekeres
Models | We study the properties and behaviour of the quasi-pseudospherical and
quasi-planar Szekeres models, obtain the regularity conditions, and analyse
their consequences. The quantities associated with "radius" and "mass" in the
quasi-spherical case must be understood in a different way for these cases. The
models with p... | gr-qc | we study the properties and behaviour of the quasipseudospherical and quasiplanar szekeres models obtain the regularity conditions and analyse their consequences the quantities associated with radius and mass in the quasispherical case must be understood in a different way for these cases the models with pseudospherica... | [['we', 'study', 'the', 'properties', 'and', 'behaviour', 'of', 'the', 'quasipseudospherical', 'and', 'quasiplanar', 'szekeres', 'models', 'obtain', 'the', 'regularity', 'conditions', 'and', 'analyse', 'their', 'consequences', 'the', 'quantities', 'associated', 'with', 'radius', 'and', 'mass', 'in', 'the', 'quasispheri... | [-0.12237996900696832, 0.13637602197436344, -0.12278591104927407, 0.10873672266041493, -0.08747588966265615, -0.1293041587407163, -0.05440118632764673, 0.4233287069897338, -0.22241471151732775, -0.30208884728957675, 0.1225557401407392, -0.25472283837529763, -0.1337878434200653, 0.14578874974018027, -0.0742746138142612,... |
710.2172 | Direct current voltage induced by microwave signal in a ferromagnetic
wire | Experimental results of rectification of a constant wave radio frequency (RF)
current flowing in a single-layered ferromagnetic wire are presented. We show
that a detailed external magnetic field dependence of the RF current induced a
direct-current voltage spectrum. The mechanism of the rectification is
discussed in... | cond-mat.mes-hall cond-mat.mtrl-sci | experimental results of rectification of a constant wave radio frequency rf current flowing in a singlelayered ferromagnetic wire are presented we show that a detailed external magnetic field dependence of the rf current induced a directcurrent voltage spectrum the mechanism of the rectification is discussed in a term ... | [['experimental', 'results', 'of', 'rectification', 'of', 'a', 'constant', 'wave', 'radio', 'frequency', 'rf', 'current', 'flowing', 'in', 'a', 'singlelayered', 'ferromagnetic', 'wire', 'are', 'presented', 'we', 'show', 'that', 'a', 'detailed', 'external', 'magnetic', 'field', 'dependence', 'of', 'the', 'rf', 'current'... | [-0.2710080962368892, 0.1725496519068928, 0.012802547466918375, -0.007854878525585704, -0.10566821065491315, -0.10783838228677813, 0.012916739319556766, 0.4126967508153817, -0.25177113412274527, -0.2611348899657425, 0.011607624506385824, -0.2417309760528895, -0.09069666776748508, 0.2664342808930837, 0.0942007861167346,... |
710.2173 | Nucleon and Nucleon to Delta Axial form factors from Lattice QCD | We present results on the nucleon axial vector form factors $G_A(q^2)$ and
$G_p(q^2)$ in the quenched theory and using two degenerate flavors of dynamical
Wilson fermions for momentum transfer squared from about 0.1 to about 2 GeV^2
and for pion masses in the range of 380 to 600 MeV. We also present results on
the co... | hep-lat | we present results on the nucleon axial vector form factors g_aq2 and g_pq2 in the quenched theory and using two degenerate flavors of dynamical wilson fermions for momentum transfer squared from about 01 to about 2 gev2 and for pion masses in the range of 380 to 600 mev we also present results on the corresponding n t... | [['we', 'present', 'results', 'on', 'the', 'nucleon', 'axial', 'vector', 'form', 'factors', 'g_aq2', 'and', 'g_pq2', 'in', 'the', 'quenched', 'theory', 'and', 'using', 'two', 'degenerate', 'flavors', 'of', 'dynamical', 'wilson', 'fermions', 'for', 'momentum', 'transfer', 'squared', 'from', 'about', '01', 'to', 'about',... | [-0.07692966781973536, 0.3434394578879894, -0.03264968380126236, 0.08948840506288201, -0.020524681479802766, -0.04622741811638048, 0.13942522867339077, 0.4138711046124267, -0.12209178795929738, -0.29155964202918977, 0.00699795272098421, -0.3346808589886614, -0.03465301126815638, 0.08904624872754306, 0.0820902154542679,... |
710.2174 | Polar Discontinuity Doping of the LaVO_3/SrTiO_3 Interface | We have investigated the transport properties of LaVO_3/SrTiO_3 Mott
insulator/band insulator heterointerfaces for various configurations. The
(001)-oriented n-type VO_2/LaO/TiO_2 polar discontinuity is conducting,
exhibiting a LaVO_3 thickness-dependent metal-insulator transition and low
temperature anomalous Hall e... | cond-mat.str-el | we have investigated the transport properties of lavo_3srtio_3 mott insulatorband insulator heterointerfaces for various configurations the 001oriented ntype vo_2laotio_2 polar discontinuity is conducting exhibiting a lavo_3 thicknessdependent metalinsulator transition and low temperature anomalous hall effect the 001 ... | [['we', 'have', 'investigated', 'the', 'transport', 'properties', 'of', 'lavo_3srtio_3', 'mott', 'insulatorband', 'insulator', 'heterointerfaces', 'for', 'various', 'configurations', 'the', '001oriented', 'ntype', 'vo_2laotio_2', 'polar', 'discontinuity', 'is', 'conducting', 'exhibiting', 'a', 'lavo_3', 'thicknessdepen... | [-0.2400711238551051, 0.2498953556919943, -0.018039272041685546, -0.04539609856820151, -0.007588587145307171, -0.25889200522606054, 0.12454652022431369, 0.4324482356601242, -0.27708599696269454, -0.3023546921617504, -0.012843927872408904, -0.36348262812886667, -0.1666024942116103, 0.1258593833789841, 0.0915047799640182... |
710.2175 | High-redshift voids in the excursion set formalism | Voids are a dominant feature of the low-redshift galaxy distribution. Several
recent surveys have found evidence for the existence of large-scale structure
at high redshifts as well. We present analytic estimates of galaxy void sizes
at redshifts z ~ 5 - 10 using the excursion set formalism. We find that recent
narro... | astro-ph | voids are a dominant feature of the lowredshift galaxy distribution several recent surveys have found evidence for the existence of largescale structure at high redshifts as well we present analytic estimates of galaxy void sizes at redshifts z 5 10 using the excursion set formalism we find that recent narrowband surve... | [['voids', 'are', 'a', 'dominant', 'feature', 'of', 'the', 'lowredshift', 'galaxy', 'distribution', 'several', 'recent', 'surveys', 'have', 'found', 'evidence', 'for', 'the', 'existence', 'of', 'largescale', 'structure', 'at', 'high', 'redshifts', 'as', 'well', 'we', 'present', 'analytic', 'estimates', 'of', 'galaxy', ... | [-0.08686229490150882, 0.13505030591220815, -0.05645543958199917, 0.15157209167871083, -0.09647042688279264, -0.049927261492106974, -0.005332448054105043, 0.4115928420972738, -0.14056124847499285, -0.3851047372220507, 0.06474157044290596, -0.31348787965466707, -0.00756026190314172, 0.20349849655589872, 0.04145985494754... |
710.2176 | Experimental studies of the $\pi^+\pi^-\pi^+\pi^-\pi^0$,
$K^+K^-\pi^+\pi^-\pi^0$ and $p\bar p\pi^+\pi^-\pi^0$ final states produced in
$e^+e^-$ annihilation at $\sqrt{s}=$ 3.773 and 3.650 GeV | We report measurements of the observed cross sections for $e^+e^-\to\omega
\pi^+\pi^-$, $\omega K^+K^-$, $\omega p\bar p$, $K^+K^-\rho^0\pi^0$,
$K^+K^-\rho^+\pi^-+c.c.$, $K^{*0}K^-\pi^+\pi^0+c.c.$,
$K^{*+}K^-\pi^+\pi^-+c.c.$, $\phi\pi^+\pi^-\pi^0$ and $\Lambda \bar \Lambda
\pi^0$ at $\sqrt s=$ 3.773 and 3.650 GeV. Up... | hep-ex | we report measurements of the observed cross sections for eetoomega pipi omega kk omega pbar p kkrho0pi0 kkrhopicc k0kpipi0cc kkpipicc phipipipi0 and lambda bar lambda pi0 at sqrt s 3773 and 3650 gev upper limits 90 cl are given for observed cross sections and for psi3770 decay branching fractions for production of the... | [['we', 'report', 'measurements', 'of', 'the', 'observed', 'cross', 'sections', 'for', 'eetoomega', 'pipi', 'omega', 'kk', 'omega', 'pbar', 'p', 'kkrho0pi0', 'kkrhopicc', 'k0kpipi0cc', 'kkpipicc', 'phipipipi0', 'and', 'lambda', 'bar', 'lambda', 'pi0', 'at', 'sqrt', 's', '3773', 'and', '3650', 'gev', 'upper', 'limits', ... | [-0.07624257837960613, 0.24212237823521718, -0.05339355634641833, 0.12198036148329265, 0.017349251377163456, -0.1104298313613981, 0.06741136884083972, 0.29448331048479304, -0.12492199882399291, -0.3447317067708354, -0.04974518722447101, -0.5210512192454189, 0.2384392550913617, 0.20029147044406273, 0.19759890768909827, ... |
710.2177 | QCD Analysis for Nuclear Parton Distributions in the Next to Leading
Order | A QCD analysis of the nuclear parton distributions and structure functions in
the NLO is performed by using the world data. By having bounded parton
distributions for a nuclear with atomic number A, we can obtain the nuclear
structure function in x space. Our results for nuclear structure function ratio
$F^A_2 /F^D_2... | hep-ph | a qcd analysis of the nuclear parton distributions and structure functions in the nlo is performed by using the world data by having bounded parton distributions for a nuclear with atomic number a we can obtain the nuclear structure function in x space our results for nuclear structure function ratio fa_2 fd_2 for some... | [['a', 'qcd', 'analysis', 'of', 'the', 'nuclear', 'parton', 'distributions', 'and', 'structure', 'functions', 'in', 'the', 'nlo', 'is', 'performed', 'by', 'using', 'the', 'world', 'data', 'by', 'having', 'bounded', 'parton', 'distributions', 'for', 'a', 'nuclear', 'with', 'atomic', 'number', 'a', 'we', 'can', 'obtain',... | [-0.03914711666545151, 0.11216471677746724, -0.15749315908682104, 0.11896879176414143, 0.008117389890390474, 0.008059954295891363, 0.021326114171864214, 0.42780372787367654, -0.17804466581878228, -0.27771207214509314, 0.04713356114980589, -0.3151196681239919, -0.03397822394539174, 0.17308447376598377, 0.057812026752209... |
710.2178 | Zel'dovich-Starobinsky Effect in Atomic Bose-Einstein Condensates:
Analogy to Kerr Black Hole | We consider circular motion of a heavy object in an atomic Bose-Einstein
condensate (BEC) at $T=0{\rm K}$. Even if the linear velocity of the object is
smaller than the Landau critical velocity, the object may radiate
quasiparticles and thus experience the quantum friction. The radiation process
is similar to Zel'dov... | cond-mat.other gr-qc | we consider circular motion of a heavy object in an atomic boseeinstein condensate bec at t0rm k even if the linear velocity of the object is smaller than the landau critical velocity the object may radiate quasiparticles and thus experience the quantum friction the radiation process is similar to zeldovichstarobinskii... | [['we', 'consider', 'circular', 'motion', 'of', 'a', 'heavy', 'object', 'in', 'an', 'atomic', 'boseeinstein', 'condensate', 'bec', 'at', 't0rm', 'k', 'even', 'if', 'the', 'linear', 'velocity', 'of', 'the', 'object', 'is', 'smaller', 'than', 'the', 'landau', 'critical', 'velocity', 'the', 'object', 'may', 'radiate', 'qu... | [-0.1720554864089658, 0.2114455961353413, -0.10796260308785323, 0.07441779543129468, -0.0755724283284942, -0.11835968315100936, 0.021341933368413307, 0.3150955273616892, -0.20273530402623896, -0.23076666070064947, 0.013964724688749038, -0.3106015663065795, -0.04133438042351114, 0.17212663050532453, -0.03844265260824016... |
710.2179 | Cluster simulation of two-dimensional relativistic fermions | The (discrete) Gross-Neveu model is studied in a lattice realization with an
N-component Majorana Wilson fermion field. It has an internal O(N) symmetry in
addition to the euclidean lattice symmetries. The discrete chiral symmetry for
vanishing mass is expected to emerge in the continuum limit only. The lattice
theor... | hep-lat | the discrete grossneveu model is studied in a lattice realization with an ncomponent majorana wilson fermion field it has an internal on symmetry in addition to the euclidean lattice symmetries the discrete chiral symmetry for vanishing mass is expected to emerge in the continuum limit only the lattice theory is first ... | [['the', 'discrete', 'grossneveu', 'model', 'is', 'studied', 'in', 'a', 'lattice', 'realization', 'with', 'an', 'ncomponent', 'majorana', 'wilson', 'fermion', 'field', 'it', 'has', 'an', 'internal', 'on', 'symmetry', 'in', 'addition', 'to', 'the', 'euclidean', 'lattice', 'symmetries', 'the', 'discrete', 'chiral', 'symm... | [-0.13570988231555284, 0.18014118823687014, -0.056818714138389854, 0.04422018327237745, -0.07105467657986209, -0.15964397226325558, 0.0462032891714758, 0.3669110147762786, -0.2341803456100184, -0.25711673110541916, 0.07692214897496966, -0.25897242426989403, -0.1406584877151785, 0.11821982291462661, 0.005066515072453885... |
710.218 | Critical endpoint in the Polyakov-loop extended NJL model | The critical endpoint (CEP) and the phase structure are studied in the
Polyakov-loop extended Nambu--Jona-Lasinio model in which the scalar type
eight-quark (\sigma^4) interaction and the vector type four-quark interaction
are newly added. The \sigma^4 interaction largely shifts the CEP toward higher
temperature and ... | hep-ph nucl-th | the critical endpoint cep and the phase structure are studied in the polyakovloop extended nambujonalasinio model in which the scalar type eightquark sigma4 interaction and the vector type fourquark interaction are newly added the sigma4 interaction largely shifts the cep toward higher temperature and lower chemical po... | [['the', 'critical', 'endpoint', 'cep', 'and', 'the', 'phase', 'structure', 'are', 'studied', 'in', 'the', 'polyakovloop', 'extended', 'nambujonalasinio', 'model', 'in', 'which', 'the', 'scalar', 'type', 'eightquark', 'sigma4', 'interaction', 'and', 'the', 'vector', 'type', 'fourquark', 'interaction', 'are', 'newly', '... | [-0.1530788132469752, 0.26844404321163895, -0.05905586226726882, 0.0489312962628901, -0.07570122499018908, -0.18402927084825932, 0.11446822201833129, 0.3373367660213262, -0.20286584137938918, -0.23149663761723788, 0.010564378523849883, -0.32133162012323735, -0.08548881707247347, 0.0013534726545913144, 0.121011640783399... |
710.2181 | Generalized Interpolation Material Point Approach to High Melting
Explosive with Cavities Under Shock | Criterion for contacting is critically important for the Generalized
Interpolation Material Point(GIMP) method. We present an improved criterion by
adding a switching function. With the method dynamical response of high melting
explosive(HMX) with cavities under shock is investigated. The physical model
used in the p... | cond-mat.mtrl-sci cond-mat.soft | criterion for contacting is critically important for the generalized interpolation material pointgimp method we present an improved criterion by adding a switching function with the method dynamical response of high melting explosivehmx with cavities under shock is investigated the physical model used in the present wo... | [['criterion', 'for', 'contacting', 'is', 'critically', 'important', 'for', 'the', 'generalized', 'interpolation', 'material', 'pointgimp', 'method', 'we', 'present', 'an', 'improved', 'criterion', 'by', 'adding', 'a', 'switching', 'function', 'with', 'the', 'method', 'dynamical', 'response', 'of', 'high', 'melting', '... | [-0.17202960960961208, 0.14663848065461338, -0.09412063032582096, -0.009350677909053586, -0.038391435109867304, -0.1413166530186399, 0.02945327039847456, 0.3735105634257986, -0.2704974191949183, -0.3027206604644932, 0.07104332188683903, -0.2801270150485887, -0.09141519475018695, 0.1723543392992012, -0.01394630347688992... |
710.2182 | Remarks on the 2nd order Seiberg-Witten maps | In this report, we discuss the Seiberg-Witten maps up to the second order in
the noncommutative parameter $\theta$. They add to the recently published
solutions in [1]. Expressions for the vector, fermion and Higgs fields are
given explicitly.
| hep-th hep-ph | in this report we discuss the seibergwitten maps up to the second order in the noncommutative parameter theta they add to the recently published solutions in 1 expressions for the vector fermion and higgs fields are given explicitly | [['in', 'this', 'report', 'we', 'discuss', 'the', 'seibergwitten', 'maps', 'up', 'to', 'the', 'second', 'order', 'in', 'the', 'noncommutative', 'parameter', 'theta', 'they', 'add', 'to', 'the', 'recently', 'published', 'solutions', 'in', '1', 'expressions', 'for', 'the', 'vector', 'fermion', 'and', 'higgs', 'fields', '... | [-0.1446625600617967, 0.14999442540207192, -0.030197639802568836, 0.10086912322041922, -0.09273068136290501, -0.11941881267059791, 0.02460450024687146, 0.3357374596311466, -0.24929557288506707, -0.2908707044920639, 0.0786845670479938, -0.2817561948230784, -0.15566052212134787, 0.13461253549413463, -0.05296980138672026,... |
710.2183 | Strong consistency of the maximum likelihood estimator for finite
mixtures of location-scale distributions when penalty is imposed on the
ratios of the scale parameters | In finite mixtures of location-scale distributions, if there is no constraint
or penalty on the parameters, then the maximum likelihood estimator does not
exist because the likelihood is unbounded. To avoid this problem, we consider a
penalized likelihood, where the penalty is a function of the minimum of the
ratios ... | math.ST math.PR stat.TH | in finite mixtures of locationscale distributions if there is no constraint or penalty on the parameters then the maximum likelihood estimator does not exist because the likelihood is unbounded to avoid this problem we consider a penalized likelihood where the penalty is a function of the minimum of the ratios of the s... | [['in', 'finite', 'mixtures', 'of', 'locationscale', 'distributions', 'if', 'there', 'is', 'no', 'constraint', 'or', 'penalty', 'on', 'the', 'parameters', 'then', 'the', 'maximum', 'likelihood', 'estimator', 'does', 'not', 'exist', 'because', 'the', 'likelihood', 'is', 'unbounded', 'to', 'avoid', 'this', 'problem', 'we... | [-0.08922427633117147, 0.05402184600153795, -0.12235992892061943, 0.11679094656918115, -0.12417768812891873, -0.15860816690006427, 0.07259958567977934, 0.38383136481650504, -0.28236491816466325, -0.29925889776671655, 0.17817424283142888, -0.27750541648448823, -0.10587725381285035, 0.09162504880709553, -0.12634937381269... |
710.2184 | On the Equivalence of Different Lax Pairs for the Kac-van Moerbeke
Hierarchy | We give a simple algebraic proof that the two different Lax pairs for the
Kac-van Moerbeke hierarchy, constructed from Jacobi respectively
super-symmetric Dirac-type difference operators, give rise to the same
hierarchy of evolution equations. As a byproduct we obtain some new recursions
for computing these equations... | nlin.SI math-ph math.MP | we give a simple algebraic proof that the two different lax pairs for the kacvan moerbeke hierarchy constructed from jacobi respectively supersymmetric diractype difference operators give rise to the same hierarchy of evolution equations as a byproduct we obtain some new recursions for computing these equations | [['we', 'give', 'a', 'simple', 'algebraic', 'proof', 'that', 'the', 'two', 'different', 'lax', 'pairs', 'for', 'the', 'kacvan', 'moerbeke', 'hierarchy', 'constructed', 'from', 'jacobi', 'respectively', 'supersymmetric', 'diractype', 'difference', 'operators', 'give', 'rise', 'to', 'the', 'same', 'hierarchy', 'of', 'evo... | [-0.15315937562643187, 0.08381129600836532, -0.0892382341477534, 0.1953592231983076, -0.14238967653870097, -0.18067208624890316, -0.022284199210369716, 0.23545347526669502, -0.3113037955177867, -0.296216096000179, 0.0724221414167677, -0.2522797712489315, -0.16550019966519397, 0.19992373606352054, -0.006364843767622243,... |
710.2185 | A new nucleon resonance in eta photoproduction | We present in this talk recent investigations on the nucleon-like resonance
N*(1675) newly found in eta photoproduction by the GRAAL, Tohoku LNS-gamma and
CB-ELSA collaborations. We focus on the production mechanism of the N*(1675),
examining its spin and parity theoretically within the framework of the
effective Lag... | hep-ph | we present in this talk recent investigations on the nucleonlike resonance n1675 newly found in eta photoproduction by the graal tohoku lnsgamma and cbelsa collaborations we focus on the production mechanism of the n1675 examining its spin and parity theoretically within the framework of the effective lagrangian method... | [['we', 'present', 'in', 'this', 'talk', 'recent', 'investigations', 'on', 'the', 'nucleonlike', 'resonance', 'n1675', 'newly', 'found', 'in', 'eta', 'photoproduction', 'by', 'the', 'graal', 'tohoku', 'lnsgamma', 'and', 'cbelsa', 'collaborations', 'we', 'focus', 'on', 'the', 'production', 'mechanism', 'of', 'the', 'n16... | [-0.13059369852080158, 0.20944629075299753, -0.08822274190978553, 0.12489762590651897, -0.035017713729320166, -0.09941506660429593, 0.05127932760633416, 0.3235182551933186, -0.17850120869794286, -0.2582508458885455, -0.037527105428761615, -0.3343367550830196, -0.07833936892071725, 0.12553633773643383, 0.076446960681937... |
710.2186 | Neutrino Masses and Mixings from Quark Mass Hierarchies | In SO(10) models with a vectorial fourth generation of down quarks and
leptons, the structure of the neutrino Majorana and Dirac mass matrices
generically coincide with those of up- and down-quarks, respectively. Then the
small neutrino mass hierarchy follows from the mismatch of the up and down
quark mass hierarchie... | hep-ph | in so10 models with a vectorial fourth generation of down quarks and leptons the structure of the neutrino majorana and dirac mass matrices generically coincide with those of up and downquarks respectively then the small neutrino mass hierarchy follows from the mismatch of the up and down quark mass hierarchies and we ... | [['in', 'so10', 'models', 'with', 'a', 'vectorial', 'fourth', 'generation', 'of', 'down', 'quarks', 'and', 'leptons', 'the', 'structure', 'of', 'the', 'neutrino', 'majorana', 'and', 'dirac', 'mass', 'matrices', 'generically', 'coincide', 'with', 'those', 'of', 'up', 'and', 'downquarks', 'respectively', 'then', 'the', '... | [-0.08772366992772034, 0.3746716870658406, 0.017962800619536885, 0.20755165487476815, -0.08144206219442086, -0.1504514383101096, 0.10749385851014355, 0.2598519961521897, -0.2529750776617494, -0.34451771679187626, 0.04990175728405481, -0.2867696106446626, -0.014888761750077957, 0.08536104796683952, 0.058031920445700214,... |
710.2187 | Theoretical analysis for the apparent discrepancy between pbarp and pp
data in charged particle forward-backward multiplicity correlations | The strength of charged particle forward-backward multiplicity correlation in
pbar+p and p+p collisions at s^1/2 = 200 GeV is studied by PYTHIA 6.4 and
compared to the UA5 and STAR data correspondingly. It is turned out that a
factor of 3-4 apparent discrepancy between UA5 and STAR data can be attributed
to the diffe... | nucl-th | the strength of charged particle forwardbackward multiplicity correlation in pbarp and pp collisions at s12 200 gev is studied by pythia 64 and compared to the ua5 and star data correspondingly it is turned out that a factor of 34 apparent discrepancy between ua5 and star data can be attributed to the differences in de... | [['the', 'strength', 'of', 'charged', 'particle', 'forwardbackward', 'multiplicity', 'correlation', 'in', 'pbarp', 'and', 'pp', 'collisions', 'at', 's12', '200', 'gev', 'is', 'studied', 'by', 'pythia', '64', 'and', 'compared', 'to', 'the', 'ua5', 'and', 'star', 'data', 'correspondingly', 'it', 'is', 'turned', 'out', 't... | [-0.05753049435443245, 0.167191292141797, -0.10581755539169535, 0.18413770759070758, 0.006833634054055437, -0.11662122193010874, -0.024809856785577723, 0.347032957074407, -0.21124097755891852, -0.3729969818261452, 0.005107958856387995, -0.3632200377905974, -0.004605411518423352, 0.13886305070482194, 0.07082440663943998... |
710.2188 | High temperature expansion in supersymmetric matrix quantum mechanics | We formulate the high temperature expansion in supersymmetric matrix quantum
mechanics with 4, 8 and 16 supercharges. The models can be obtained by
dimensionally reducing N=1 U(N) super Yang-Mills theory in D=4,6,10 to 1
dimension, respectively. While the non-zero frequency modes become weakly
coupled at high tempera... | hep-th hep-lat | we formulate the high temperature expansion in supersymmetric matrix quantum mechanics with 4 8 and 16 supercharges the models can be obtained by dimensionally reducing n1 un super yangmills theory in d4610 to 1 dimension respectively while the nonzero frequency modes become weakly coupled at high temperature the zero ... | [['we', 'formulate', 'the', 'high', 'temperature', 'expansion', 'in', 'supersymmetric', 'matrix', 'quantum', 'mechanics', 'with', '4', '8', 'and', '16', 'supercharges', 'the', 'models', 'can', 'be', 'obtained', 'by', 'dimensionally', 'reducing', 'n1', 'un', 'super', 'yangmills', 'theory', 'in', 'd4610', 'to', '1', 'dim... | [-0.09796203202368017, 0.2164708437516634, -0.07299926271376435, 0.033636684892299165, -0.0007911164090722982, -0.12423877566024387, 0.0026354120860013403, 0.3114653906265011, -0.2212771562905125, -0.27960880548390415, 0.08875910407989257, -0.33111564541361266, -0.10398094220776317, 0.14444354413637173, 0.0385623480496... |
710.2189 | Strong Interactive Massive Particles from a Strong Coupled Theory | Minimal walking technicolor models can provide a nontrivial solution for
cosmological dark matter, if the lightest technibaryon is doubly charged.
Technibaryon asymmetry generated in the early Universe is related to baryon
asymmetry and it is possible to create excess of techniparticles with charge
(-2). These excess... | astro-ph | minimal walking technicolor models can provide a nontrivial solution for cosmological dark matter if the lightest technibaryon is doubly charged technibaryon asymmetry generated in the early universe is related to baryon asymmetry and it is possible to create excess of techniparticles with charge 2 these excessive tech... | [['minimal', 'walking', 'technicolor', 'models', 'can', 'provide', 'a', 'nontrivial', 'solution', 'for', 'cosmological', 'dark', 'matter', 'if', 'the', 'lightest', 'technibaryon', 'is', 'doubly', 'charged', 'technibaryon', 'asymmetry', 'generated', 'in', 'the', 'early', 'universe', 'is', 'related', 'to', 'baryon', 'asy... | [-0.09617226668871642, 0.2856159566086717, -0.06293435574731451, 0.14678254743762822, -0.057509866147302094, -0.1259073335814967, -0.00027929513757540424, 0.2943677272044376, -0.2368409196740355, -0.36134577531113543, 0.020743942535641095, -0.33307261058891363, 0.014309654879616574, 0.13974251091078094, 0.0439741985830... |
710.219 | Spatially resolved spectroscopy of Coma cluster early-type galaxies IV.
Completing the dataset | The long-slit spectra obtained along the minor axis, offset major axis and
diagonal axis are presented for 12 E and S0 galaxies of the Coma cluster drawn
from a magnitude-limited sample studied before. The rotation curves, velocity
dispersion profiles and the H_3 and H_4 coefficients of the Hermite
decomposition of t... | astro-ph | the longslit spectra obtained along the minor axis offset major axis and diagonal axis are presented for 12 e and s0 galaxies of the coma cluster drawn from a magnitudelimited sample studied before the rotation curves velocity dispersion profiles and the h_3 and h_4 coefficients of the hermite decomposition of the line... | [['the', 'longslit', 'spectra', 'obtained', 'along', 'the', 'minor', 'axis', 'offset', 'major', 'axis', 'and', 'diagonal', 'axis', 'are', 'presented', 'for', '12', 'e', 'and', 's0', 'galaxies', 'of', 'the', 'coma', 'cluster', 'drawn', 'from', 'a', 'magnitudelimited', 'sample', 'studied', 'before', 'the', 'rotation', 'c... | [-0.10108679216107831, 0.056700274162818635, -0.07180047124228646, 0.05439347207270134, -0.0707145240817186, -0.07469599355584983, -0.006979634663897806, 0.4732989445988056, -0.16234797681063678, -0.2996159418366553, 0.06579607280189649, -0.27948617853586916, -0.00374666745650821, 0.205425923341469, 0.01660795384539967... |
710.2191 | Three-Dimensional Simulations of Standing Accretion Shock Instability in
Core-Collapse Supernovae | We have studied non-axisymmetric standing accretion shock instability, or
SASI, by 3D hydrodynamical simulations. This is an extention of our previous
study on axisymmetric SASI. We have prepared a spherically symmetric and steady
accretion flow through a standing shock wave onto a proto-neutron star, taking
into acc... | astro-ph | we have studied nonaxisymmetric standing accretion shock instability or sasi by 3d hydrodynamical simulations this is an extention of our previous study on axisymmetric sasi we have prepared a spherically symmetric and steady accretion flow through a standing shock wave onto a protoneutron star taking into account a re... | [['we', 'have', 'studied', 'nonaxisymmetric', 'standing', 'accretion', 'shock', 'instability', 'or', 'sasi', 'by', '3d', 'hydrodynamical', 'simulations', 'this', 'is', 'an', 'extention', 'of', 'our', 'previous', 'study', 'on', 'axisymmetric', 'sasi', 'we', 'have', 'prepared', 'a', 'spherically', 'symmetric', 'and', 'st... | [-0.12740214007814624, 0.1740422080360191, -0.06581155597102027, 0.07996009327951571, -0.06494547768945357, -0.11649162636034295, -0.05243545324033634, 0.34585262084594715, -0.20660988436002362, -0.2779826687382684, 0.10089072390293403, -0.2603283240036531, -0.06552237954065594, 0.19243030463120658, 0.03309396870303113... |
710.2192 | Quantitative estimates of unique continuation for parabolic equations,
determination of unknown time-varying boundaries and optimal stability
estimates | In this paper we will review the main results concerning the issue of
stability for the determination unknown boundary portion of a thermic
conducting body from Cauchy data for parabolic equations. We give detailed and
selfcontained proofs. We prove that such problems are severely ill-posed in the
sense that under a ... | math.AP | in this paper we will review the main results concerning the issue of stability for the determination unknown boundary portion of a thermic conducting body from cauchy data for parabolic equations we give detailed and selfcontained proofs we prove that such problems are severely illposed in the sense that under a prior... | [['in', 'this', 'paper', 'we', 'will', 'review', 'the', 'main', 'results', 'concerning', 'the', 'issue', 'of', 'stability', 'for', 'the', 'determination', 'unknown', 'boundary', 'portion', 'of', 'a', 'thermic', 'conducting', 'body', 'from', 'cauchy', 'data', 'for', 'parabolic', 'equations', 'we', 'give', 'detailed', 'a... | [-0.10352378296249051, 0.041905119388513726, -0.07555869918454576, 0.05349244800522739, -0.1362349104228211, -0.08678251238148889, 0.04725510100755024, 0.3172086701256993, -0.28976287313357546, -0.263892255263564, 0.19702342480857982, -0.2777458952716839, -0.10835555642139005, 0.20067666281290628, -0.14794591202021198,... |
710.2193 | Can low metallicity binaries avoid merging? | Rapid mass transfer in a binary system can drive the accreting star out of
thermal equilibrium, causing it to expand. This can lead to a contact system,
strong mass loss from the system and possibly merging of the two stars. In low
metallicity stars the timescale for heat transport is shorter due to the lower
opacity... | astro-ph | rapid mass transfer in a binary system can drive the accreting star out of thermal equilibrium causing it to expand this can lead to a contact system strong mass loss from the system and possibly merging of the two stars in low metallicity stars the timescale for heat transport is shorter due to the lower opacity the a... | [['rapid', 'mass', 'transfer', 'in', 'a', 'binary', 'system', 'can', 'drive', 'the', 'accreting', 'star', 'out', 'of', 'thermal', 'equilibrium', 'causing', 'it', 'to', 'expand', 'this', 'can', 'lead', 'to', 'a', 'contact', 'system', 'strong', 'mass', 'loss', 'from', 'the', 'system', 'and', 'possibly', 'merging', 'of', ... | [-0.0890290451891215, 0.1870692299351968, -0.060304764509597354, 0.10450413844615043, -0.08094778056801395, -0.08373341409172466, 0.08412331316070235, 0.40071285038473126, -0.20837441274148233, -0.3621237922826425, 0.07990663644778444, -0.25158451713542357, -0.003127408768743911, 0.22114688711008057, -0.087312164944299... |
710.2194 | Double beta decay to the excited states: experimental review | A brief review on double beta decay to excited states of daughter nuclei is
given. The ECEC(ov) transision to the excited states are discussed in
association with a possible enhancement of the decay rate by several orders of
magnitude.
| nucl-ex | a brief review on double beta decay to excited states of daughter nuclei is given the ececov transision to the excited states are discussed in association with a possible enhancement of the decay rate by several orders of magnitude | [['a', 'brief', 'review', 'on', 'double', 'beta', 'decay', 'to', 'excited', 'states', 'of', 'daughter', 'nuclei', 'is', 'given', 'the', 'ececov', 'transision', 'to', 'the', 'excited', 'states', 'are', 'discussed', 'in', 'association', 'with', 'a', 'possible', 'enhancement', 'of', 'the', 'decay', 'rate', 'by', 'several'... | [-0.11269867062770031, 0.267286338264475, 0.010267118822682548, 0.11277053093953007, 0.03480897408381507, -0.08425657307678783, 0.08875236997531878, 0.3414876956391979, -0.2336862988367274, -0.2605243755152097, 0.053357605517187434, -0.3278491037671228, -0.001120910350535367, 0.1771821745646161, 0.06756177484183698, 0.... |
710.2195 | A Statistical Description of Parametric Instabilities with an Incoherent
Pump | The effect on parametric instability growth of pump wave incoherence is
treated by deriving a set of equations governing the space-time evolution of
the ensemble-average coupled-mode amplitudes and intensities. Particular
attention is paid to establishing the regions of validity of the statistical
description. Thresh... | physics.plasm-ph | the effect on parametric instability growth of pump wave incoherence is treated by deriving a set of equations governing the spacetime evolution of the ensembleaverage coupledmode amplitudes and intensities particular attention is paid to establishing the regions of validity of the statistical description thresholds gr... | [['the', 'effect', 'on', 'parametric', 'instability', 'growth', 'of', 'pump', 'wave', 'incoherence', 'is', 'treated', 'by', 'deriving', 'a', 'set', 'of', 'equations', 'governing', 'the', 'spacetime', 'evolution', 'of', 'the', 'ensembleaverage', 'coupledmode', 'amplitudes', 'and', 'intensities', 'particular', 'attention... | [-0.17313828632428213, 0.18614714284930592, -0.06574198008440006, 0.08718264761552129, -0.03048707504660405, -0.11548370104176046, 0.022216610508788932, 0.3511726454799545, -0.23148612575819608, -0.2209019222478757, 0.11720684669703117, -0.22918754839605984, -0.0916950869984154, 0.206968499690123, 0.018200281215296394,... |
710.2196 | The value of long-range interactions parameter for some alloys | The critical behavior of some alloys are analyzed within the framework of
Heisenbergs model with long-range interaction. On based experimental values of
the critical exponent $\gamma$ we calculate the value of paerameter of
long-range interaction.
| cond-mat.stat-mech cond-mat.mtrl-sci | the critical behavior of some alloys are analyzed within the framework of heisenbergs model with longrange interaction on based experimental values of the critical exponent gamma we calculate the value of paerameter of longrange interaction | [['the', 'critical', 'behavior', 'of', 'some', 'alloys', 'are', 'analyzed', 'within', 'the', 'framework', 'of', 'heisenbergs', 'model', 'with', 'longrange', 'interaction', 'on', 'based', 'experimental', 'values', 'of', 'the', 'critical', 'exponent', 'gamma', 'we', 'calculate', 'the', 'value', 'of', 'paerameter', 'of', ... | [-0.1735297959051369, 0.17298442873117678, -0.09286631482160267, 0.06270532353835948, -0.0011770785323974183, -0.13053229341612144, 0.060409121763180286, 0.33011218423352523, -0.2228532996686066, -0.2903488993863849, 0.000847731703234946, -0.35423148330301046, -0.1521829750169726, 0.17959071300677298, 0.094643209656864... |
710.2197 | Quasi-exact Solvability of Dirac Equations | We present a general procedure for determining quasi-exact solvability of the
Dirac and the Pauli equation with an underlying $sl(2)$ symmetry. This
procedure makes full use of the close connection between quasi-exactly solvable
systems and supersymmetry. The Dirac-Pauli equation with spherical electric
field is take... | hep-th | we present a general procedure for determining quasiexact solvability of the dirac and the pauli equation with an underlying sl2 symmetry this procedure makes full use of the close connection between quasiexactly solvable systems and supersymmetry the diracpauli equation with spherical electric field is taken as an exa... | [['we', 'present', 'a', 'general', 'procedure', 'for', 'determining', 'quasiexact', 'solvability', 'of', 'the', 'dirac', 'and', 'the', 'pauli', 'equation', 'with', 'an', 'underlying', 'sl2', 'symmetry', 'this', 'procedure', 'makes', 'full', 'use', 'of', 'the', 'close', 'connection', 'between', 'quasiexactly', 'solvable... | [-0.14175379039862981, 0.05377785296038313, -0.048127474514051125, 0.09435624948057991, -0.15721422681011832, -0.1926785443748276, 0.0002625276056977992, 0.344544871029659, -0.257955311708009, -0.3055518827974223, 0.07271284767641471, -0.22685934339936537, -0.18161771761683318, 0.17038745736667457, 0.007565130111358415... |
710.2198 | Disorder-dominated phases of random systems : relations between tails
exponents and scaling exponents | We consider various random models (directed polymer, ferromagnetic random
Potts model, Ising spin-glasses) in their disorder-dominated phases, where the
free-energy cost $F(L)$ of an excitation of length $L$ present fluctuations
that grow as a power-law $\Delta F(L) \sim L^{\omega}$ with the so-called
droplet exponen... | cond-mat.dis-nn | we consider various random models directed polymer ferromagnetic random potts model ising spinglasses in their disorderdominated phases where the freeenergy cost fl of an excitation of length l present fluctuations that grow as a powerlaw delta fl sim lomega with the socalled droplet exponent omega0 we study the tails ... | [['we', 'consider', 'various', 'random', 'models', 'directed', 'polymer', 'ferromagnetic', 'random', 'potts', 'model', 'ising', 'spinglasses', 'in', 'their', 'disorderdominated', 'phases', 'where', 'the', 'freeenergy', 'cost', 'fl', 'of', 'an', 'excitation', 'of', 'length', 'l', 'present', 'fluctuations', 'that', 'grow... | [-0.15573511368495896, 0.20529173446382987, -0.09461818669813421, 0.08997228240988067, 0.006715603199367768, -0.14684277544959368, 0.053113174675762605, 0.349342508271716, -0.2821133037350704, -0.21802582780336155, 0.02792832751925115, -0.31664245943596336, -0.14547695489859003, 0.14235483259494405, 0.01316980366238657... |
710.2199 | Jets or high velocity flows revealed in high-cadence spectrometer and
imager co-observations? | We report on active region EUV dynamic events observed simultaneously at
high-cadence with SUMER/SoHO and TRACE. Although the features appear in the
TRACE Fe ix/x 171A images as jets seen in projection on the solar disk, the
SUMER spectral line profiles suggest that the plasma has been driven along a
curved large sca... | astro-ph | we report on active region euv dynamic events observed simultaneously at highcadence with sumersoho and trace although the features appear in the trace fe ixx 171a images as jets seen in projection on the solar disk the sumer spectral line profiles suggest that the plasma has been driven along a curved large scale magn... | [['we', 'report', 'on', 'active', 'region', 'euv', 'dynamic', 'events', 'observed', 'simultaneously', 'at', 'highcadence', 'with', 'sumersoho', 'and', 'trace', 'although', 'the', 'features', 'appear', 'in', 'the', 'trace', 'fe', 'ixx', '171a', 'images', 'as', 'jets', 'seen', 'in', 'projection', 'on', 'the', 'solar', 'd... | [-0.0784091746805474, 0.1818720923451914, -0.03697217440200146, 0.05332312589011645, -0.028465257754527726, -0.06586396981296021, 0.0399236639820819, 0.44528889046375486, -0.21149735806610023, -0.3850473321887643, 0.11173439922547618, -0.31635646157638103, 0.0032732711027398014, 0.2148398493097142, -0.00271793037770061... |
710.22 | Scale decomposition of molecular beam epitaxy | In this work, a study of epitaxial growth was carried out by means of
wavelets formalism. We showed the existence of a dynamic scaling form in
wavelet discriminated linear MBE equation where diffusion and noise are the
dominant effects. We determined simple and exact scaling functions involving
the scale of the wavel... | cond-mat.mtrl-sci | in this work a study of epitaxial growth was carried out by means of wavelets formalism we showed the existence of a dynamic scaling form in wavelet discriminated linear mbe equation where diffusion and noise are the dominant effects we determined simple and exact scaling functions involving the scale of the wavelets w... | [['in', 'this', 'work', 'a', 'study', 'of', 'epitaxial', 'growth', 'was', 'carried', 'out', 'by', 'means', 'of', 'wavelets', 'formalism', 'we', 'showed', 'the', 'existence', 'of', 'a', 'dynamic', 'scaling', 'form', 'in', 'wavelet', 'discriminated', 'linear', 'mbe', 'equation', 'where', 'diffusion', 'and', 'noise', 'are... | [-0.1177128339925908, 0.12269388140275529, -0.12145928779290509, 0.040135174596048505, -0.021440139719640317, -0.10250217335889135, 0.012022429541924718, 0.35795043202503535, -0.288216941334672, -0.2672833157031192, 0.10851763855166656, -0.2585939741069355, -0.1647965351549294, 0.22565718332411164, 0.005815773391040023... |
710.2201 | Heavy-strange meson decay constants in the continuum limit of quenched
QCD | We improve a previous quenched result for heavy-light pseudoscalar meson
decay constants with the light quark taken to be the strange quark. A finer
lattice resolution (a ~ 0.05 fm) in the continuum limit extrapolation of the
data computed in the static approximation is included. We also give further
details concerni... | hep-lat hep-ph | we improve a previous quenched result for heavylight pseudoscalar meson decay constants with the light quark taken to be the strange quark a finer lattice resolution a 005 fm in the continuum limit extrapolation of the data computed in the static approximation is included we also give further details concerning the tec... | [['we', 'improve', 'a', 'previous', 'quenched', 'result', 'for', 'heavylight', 'pseudoscalar', 'meson', 'decay', 'constants', 'with', 'the', 'light', 'quark', 'taken', 'to', 'be', 'the', 'strange', 'quark', 'a', 'finer', 'lattice', 'resolution', 'a', '005', 'fm', 'in', 'the', 'continuum', 'limit', 'extrapolation', 'of'... | [-0.035900414726681644, 0.2004000704972165, -0.09293056188960422, 0.12128522004035194, -0.008807444551121825, -0.08682009768739084, 0.14191552634030336, 0.33951336328612, -0.20791544184397875, -0.2777464610054997, 0.044006114441054095, -0.29669213388496857, 0.03823692376389489, 0.14237485976782857, 0.010403104065383067... |
710.2202 | Searches for Extra Dimensions and for Heavy Resonances in Dilepton,
Diphoton, Electron + Photon and Electron + Missing ET Final States with the
D0 Detector | The high mass spectrum of lepton and photon pairs is sensitive to a broad
array of new physics. Examples include searches for extra dimensions in the
dielectron and diphoton channels. A direct search for electron compositeness is
possible in the production of excited electrons decaying into an electron and a
photon. ... | hep-ex | the high mass spectrum of lepton and photon pairs is sensitive to a broad array of new physics examples include searches for extra dimensions in the dielectron and diphoton channels a direct search for electron compositeness is possible in the production of excited electrons decaying into an electron and a photon in ad... | [['the', 'high', 'mass', 'spectrum', 'of', 'lepton', 'and', 'photon', 'pairs', 'is', 'sensitive', 'to', 'a', 'broad', 'array', 'of', 'new', 'physics', 'examples', 'include', 'searches', 'for', 'extra', 'dimensions', 'in', 'the', 'dielectron', 'and', 'diphoton', 'channels', 'a', 'direct', 'search', 'for', 'electron', 'c... | [-0.060712749764647786, 0.20606281660663875, -0.025286768326733374, 0.17737644173427147, -0.04022037113000723, -0.16481246103913608, 0.02525920911769693, 0.33545303001124976, -0.1650600360713504, -0.3746995192275129, 0.017864618158482976, -0.37193284940087434, 0.09450793796162488, 0.20025114181881884, 0.058870448434997... |
710.2203 | Degree one cohomology with twisted coefficients of the mapping class
group | Let $\Gamma$ be the mapping class group of an oriented surface $\Sigma$ of
genus g with r boundary components. We prove that the first cohomology group
$H^1(\Gamma, O(M_{SL(2, C)})^*)$ is non-trivial, where the coefficient module
is the dual of the space of algebraic functions on the $SL(2, C)$ moduli space
over $\Si... | math.DG | let gamma be the mapping class group of an oriented surface sigma of genus g with r boundary components we prove that the first cohomology group h1gamma om_sl2 c is nontrivial where the coefficient module is the dual of the space of algebraic functions on the sl2 c moduli space over sigma | [['let', 'gamma', 'be', 'the', 'mapping', 'class', 'group', 'of', 'an', 'oriented', 'surface', 'sigma', 'of', 'genus', 'g', 'with', 'r', 'boundary', 'components', 'we', 'prove', 'that', 'the', 'first', 'cohomology', 'group', 'h1gamma', 'om_sl2', 'c', 'is', 'nontrivial', 'where', 'the', 'coefficient', 'module', 'is', 't... | [-0.23717498437811932, 0.09941440339767438, -0.09843772832377284, -0.052760480606344105, -0.12671267203804032, -0.13866595100319268, -0.044822306408747736, 0.3451813062397288, -0.36914251598657344, -0.1724357031212718, 0.09804119213995542, -0.24055226742490834, -0.1277527148269263, 0.19147284068715045, -0.0793079886512... |
710.2204 | Small cosmological constant in seesaw mechanism with breaking down SUSY | The observed small value of cosmological constant can be naturally related
with the scale of breaking down supersymmetry in agreement with other
evaluations in particle physics.
| hep-th gr-qc hep-ph | the observed small value of cosmological constant can be naturally related with the scale of breaking down supersymmetry in agreement with other evaluations in particle physics | [['the', 'observed', 'small', 'value', 'of', 'cosmological', 'constant', 'can', 'be', 'naturally', 'related', 'with', 'the', 'scale', 'of', 'breaking', 'down', 'supersymmetry', 'in', 'agreement', 'with', 'other', 'evaluations', 'in', 'particle', 'physics']] | [-0.07133215952378053, 0.2400495195044921, -0.023901658311772805, 0.08072021797012824, -0.08937736117066099, -0.1529950689470682, -0.05701608406021618, 0.292041304279477, -0.2755558972175305, -0.43889662623405457, 0.1200024189445405, -0.2422109325416386, -0.04318785352202562, 0.17149450023246643, -0.006990624627528282,... |
710.2205 | Stabilizing quantum metastable states in a time-periodic potential | In this talk we present a model to demonstrate how time-periodic potential
can be used to manipulate quantum metastability of a system. We study
metastability of a particle trapped in a well with a time-periodically
oscillating barrier in the Floquet formalism. It is shown that the oscillating
barrier causes the syst... | quant-ph | in this talk we present a model to demonstrate how timeperiodic potential can be used to manipulate quantum metastability of a system we study metastability of a particle trapped in a well with a timeperiodically oscillating barrier in the floquet formalism it is shown that the oscillating barrier causes the system to ... | [['in', 'this', 'talk', 'we', 'present', 'a', 'model', 'to', 'demonstrate', 'how', 'timeperiodic', 'potential', 'can', 'be', 'used', 'to', 'manipulate', 'quantum', 'metastability', 'of', 'a', 'system', 'we', 'study', 'metastability', 'of', 'a', 'particle', 'trapped', 'in', 'a', 'well', 'with', 'a', 'timeperiodically', ... | [-0.171744552157179, 0.2502421940812166, -0.12491871489744101, 0.0770441515349029, -0.01068633378201325, -0.1676748343743384, 0.09724091167195834, 0.32767895405136405, -0.3039915960814272, -0.27213097696394906, 0.07773243847935062, -0.2343962879136338, -0.12698767995295515, 0.1795203955975705, -0.0055457191116320675, 0... |
710.2206 | Shape transformation transitions of a tethered surface model | A surface model of Nambu and Goto is studied statistical mechanically by
using the canonical Monte Carlo simulation technique on a spherical meshwork.
The model is defined by the area energy term and a one-dimensional bending
energy term in the Hamiltonian. We find that the model has a large variety of
phases; the sp... | cond-mat.stat-mech cond-mat.soft | a surface model of nambu and goto is studied statistical mechanically by using the canonical monte carlo simulation technique on a spherical meshwork the model is defined by the area energy term and a onedimensional bending energy term in the hamiltonian we find that the model has a large variety of phases the spherica... | [['a', 'surface', 'model', 'of', 'nambu', 'and', 'goto', 'is', 'studied', 'statistical', 'mechanically', 'by', 'using', 'the', 'canonical', 'monte', 'carlo', 'simulation', 'technique', 'on', 'a', 'spherical', 'meshwork', 'the', 'model', 'is', 'defined', 'by', 'the', 'area', 'energy', 'term', 'and', 'a', 'onedimensional... | [-0.1673038419962765, 0.22013859201013763, -0.10830493694362796, 0.05182672111713545, 0.012614066377456221, -0.11387929210665627, 0.02137128194080335, 0.3802840874713158, -0.27992673452386513, -0.27446307614445686, 0.1004969057339792, -0.2585349209154042, -0.18504804045518983, 0.15758751758600575, 0.0141264405738014, 0... |
710.2207 | Sneutrino-antisneutrino mixing at future colliders | Sneutrino-antisneutrino mixing occurs in a supersymmetric model where
neutrinos have nonzero Majorana masses. This can lead to the sneutrino decaying
into a final state with a "wrong-sign charged lepton". In an $e^- \gamma$
collider, the signal of the associated production of an electron-sneutrino and
the lighter cha... | hep-ph | sneutrinoantisneutrino mixing occurs in a supersymmetric model where neutrinos have nonzero majorana masses this can lead to the sneutrino decaying into a final state with a wrongsign charged lepton in an e gamma collider the signal of the associated production of an electronsneutrino and the lighter chargino and their... | [['sneutrinoantisneutrino', 'mixing', 'occurs', 'in', 'a', 'supersymmetric', 'model', 'where', 'neutrinos', 'have', 'nonzero', 'majorana', 'masses', 'this', 'can', 'lead', 'to', 'the', 'sneutrino', 'decaying', 'into', 'a', 'final', 'state', 'with', 'a', 'wrongsign', 'charged', 'lepton', 'in', 'an', 'e', 'gamma', 'colli... | [-0.11097895653722234, 0.3216823220745563, -0.057779326993487264, 0.12555891944275696, -0.054955593157202415, -0.17783307709271878, -0.00036154896553529245, 0.3277369562140985, -0.25308054709832556, -0.2915873053828127, 0.06040951712710834, -0.29040456474567317, -0.011106706626253994, 0.15756005931275655, 0.01714524845... |
710.2208 | On Nurowski's conformal structure associated to a generic rank two
distribution in dimension five | For a generic distribution of rank two on a manifold $M$ of dimension five,
we introduce the notion of a generalized contact form. To such a form we
associate a generalized Reeb field and a partial connection. From these data,
we explicitly constructed a pseudo--Riemannian metric on $M$ of split
signature. We prove t... | math.DG | for a generic distribution of rank two on a manifold m of dimension five we introduce the notion of a generalized contact form to such a form we associate a generalized reeb field and a partial connection from these data we explicitly constructed a pseudoriemannian metric on m of split signature we prove that a change ... | [['for', 'a', 'generic', 'distribution', 'of', 'rank', 'two', 'on', 'a', 'manifold', 'm', 'of', 'dimension', 'five', 'we', 'introduce', 'the', 'notion', 'of', 'a', 'generalized', 'contact', 'form', 'to', 'such', 'a', 'form', 'we', 'associate', 'a', 'generalized', 'reeb', 'field', 'and', 'a', 'partial', 'connection', 'f... | [-0.1599092176344631, 0.06738987071981557, -0.10049416323328905, 0.07145598890753624, -0.137202051311635, -0.10813401138072769, -0.012081090909838355, 0.32483114918758127, -0.28057836408823217, -0.23237002026470346, 0.06703685029863445, -0.2550307171949153, -0.21860377678390722, 0.1323676679628612, -0.0748893654672429,... |
710.2209 | q-oscillator from the q-Hermite Polynomial | By factorization of the Hamiltonian describing the quantum mechanics of the
continuous q-Hermite polynomial, the creation and annihilation operators of the
q-oscillator are obtained. They satisfy a q-oscillator algebra as a consequence
of the shape-invariance of the Hamiltonian. A second set of q-oscillator is
derive... | hep-th math-ph math.CA math.MP math.QA nlin.SI quant-ph | by factorization of the hamiltonian describing the quantum mechanics of the continuous qhermite polynomial the creation and annihilation operators of the qoscillator are obtained they satisfy a qoscillator algebra as a consequence of the shapeinvariance of the hamiltonian a second set of qoscillator is derived from the... | [['by', 'factorization', 'of', 'the', 'hamiltonian', 'describing', 'the', 'quantum', 'mechanics', 'of', 'the', 'continuous', 'qhermite', 'polynomial', 'the', 'creation', 'and', 'annihilation', 'operators', 'of', 'the', 'qoscillator', 'are', 'obtained', 'they', 'satisfy', 'a', 'qoscillator', 'algebra', 'as', 'a', 'conse... | [-0.14136707102079527, 0.13206868965062313, -0.07935042914323276, 0.0735679456647631, -0.09788254715749645, -0.11872386205504881, -0.040874451984564075, 0.2489326437789714, -0.294150560250273, -0.18128269464796176, 0.08689659614537959, -0.304865853569936, -0.12410889307648176, 0.17325826128944755, 0.025924646703060716,... |
710.221 | Effects of Inflation on a Cosmic String Loop Population | We study the evolution of simple cosmic string loop solutions in an
inflationary universe. We show, for the particular case of circular loops, that
periodic solutions do exist in a de Sitter universe, below a critical loop
radius $R_c H=1/2$. On the other hand, larger loops freeze in comoving
coordinates, and we expl... | hep-ph astro-ph gr-qc hep-th | we study the evolution of simple cosmic string loop solutions in an inflationary universe we show for the particular case of circular loops that periodic solutions do exist in a de sitter universe below a critical loop radius r_c h12 on the other hand larger loops freeze in comoving coordinates and we explicitly show t... | [['we', 'study', 'the', 'evolution', 'of', 'simple', 'cosmic', 'string', 'loop', 'solutions', 'in', 'an', 'inflationary', 'universe', 'we', 'show', 'for', 'the', 'particular', 'case', 'of', 'circular', 'loops', 'that', 'periodic', 'solutions', 'do', 'exist', 'in', 'a', 'de', 'sitter', 'universe', 'below', 'a', 'critica... | [-0.18853438788157126, 0.20326462477479998, -0.07918082280931148, 0.1729333864154548, -0.06507982909679413, -0.10652585557373558, -0.0189531425754963, 0.3516609606587074, -0.17026154511523517, -0.23400259727442807, 0.10804783980446783, -0.2529282450675964, -0.11839989160864868, 0.1977243756187487, -0.03716274051165039,... |
710.2211 | A note on congruences for theta divisors | The classes of two theta divisors on an abelian variety in the naive
Grothendieck ring of varieties need not be congruent modulo the class of the
affine line.
| math.AG | the classes of two theta divisors on an abelian variety in the naive grothendieck ring of varieties need not be congruent modulo the class of the affine line | [['the', 'classes', 'of', 'two', 'theta', 'divisors', 'on', 'an', 'abelian', 'variety', 'in', 'the', 'naive', 'grothendieck', 'ring', 'of', 'varieties', 'need', 'not', 'be', 'congruent', 'modulo', 'the', 'class', 'of', 'the', 'affine', 'line']] | [-0.20213610432775958, 0.031745639883800844, -0.041862784951393096, 0.018877911314900433, -0.11942434630223683, -0.1681701825665576, -0.044382573546109985, 0.33963654642658575, -0.3915450533053705, -0.1969553689206285, 0.07238430415496364, -0.19116473011672497, -0.09188183896809018, 0.23634125461934932, -0.186143445449... |
710.2212 | Probing Universal Extra Dimensions through rare decays induced by $b \to
s$ transition | A few $B_{d,s}$ and $\Lambda_b$ decays induced by $b \to s$ transition are
studied in the Standard Model and in the framework of the Appelquist, Cheng and
Dobrescu (ACD) model, which is a New Physics scenario where a single universal
extra dimension is considered. In particular, we investigate the sensitivity of
the ... | hep-ph | a few b_ds and lambda_b decays induced by b to s transition are studied in the standard model and in the framework of the appelquist cheng and dobrescu acd model which is a new physics scenario where a single universal extra dimension is considered in particular we investigate the sensitivity of the observables to the ... | [['a', 'few', 'b_ds', 'and', 'lambda_b', 'decays', 'induced', 'by', 'b', 'to', 's', 'transition', 'are', 'studied', 'in', 'the', 'standard', 'model', 'and', 'in', 'the', 'framework', 'of', 'the', 'appelquist', 'cheng', 'and', 'dobrescu', 'acd', 'model', 'which', 'is', 'a', 'new', 'physics', 'scenario', 'where', 'a', 's... | [-0.10973363158247265, 0.17294937563052432, -0.029655156947183806, 0.07078994880048711, -0.02688458475635433, -0.1970811261429039, 0.03376810433778179, 0.2686837180250431, -0.25573706858959355, -0.271421982532703, 0.050979358504801134, -0.2630204986170179, -0.08731672204420214, 0.11126579058768808, -0.01176903438067338... |
710.2213 | Implications of Catalyzed BBN in the CMSSM with Gravitino Dark Matter | We investigate gravitino dark matter scenarios in which the primordial ^6Li
production is catalyzed by bound-state formation of long-lived negatively
charged particles X^- with ^4He. In the constrained minimal supersymmetric
Standard Model (CMSSM) with the stau^- as the X^-, the observationally inferred
bound on the ... | hep-ph astro-ph | we investigate gravitino dark matter scenarios in which the primordial 6li production is catalyzed by boundstate formation of longlived negatively charged particles x with 4he in the constrained minimal supersymmetric standard model cmssm with the stau as the x the observationally inferred bound on the primordial 6li a... | [['we', 'investigate', 'gravitino', 'dark', 'matter', 'scenarios', 'in', 'which', 'the', 'primordial', '6li', 'production', 'is', 'catalyzed', 'by', 'boundstate', 'formation', 'of', 'longlived', 'negatively', 'charged', 'particles', 'x', 'with', '4he', 'in', 'the', 'constrained', 'minimal', 'supersymmetric', 'standard'... | [-0.06464787669501257, 0.2819884117778348, -0.056304639403376426, 0.177696218264514, -0.033088597914621494, -0.16165053514742303, 0.01742387178685816, 0.2523039266006786, -0.15790053129720705, -0.333074940903776, 0.03140215991578739, -0.2479212105238406, 0.0639110110357575, 0.15047148929844642, 0.009216324554692054, 0.... |
710.2214 | Decay of Charged Higgs boson in TeV scale supersymmetric seesaw model | We discuss phenomenological consequences of some class of supersymmetric
seesaw models in which the right-handed (s)neutrino mass is given to be TeV
scale. In this scenario, scalar trilinear interaction of
Higgs-slepton-(right-handed) sneutrino is enhanced. We show that the 1-loop
correction by sneutrino exchange to ... | hep-ph | we discuss phenomenological consequences of some class of supersymmetric seesaw models in which the righthanded sneutrino mass is given to be tev scale in this scenario scalar trilinear interaction of higgssleptonrighthanded sneutrino is enhanced we show that the 1loop correction by sneutrino exchange to the lightest h... | [['we', 'discuss', 'phenomenological', 'consequences', 'of', 'some', 'class', 'of', 'supersymmetric', 'seesaw', 'models', 'in', 'which', 'the', 'righthanded', 'sneutrino', 'mass', 'is', 'given', 'to', 'be', 'tev', 'scale', 'in', 'this', 'scenario', 'scalar', 'trilinear', 'interaction', 'of', 'higgssleptonrighthanded', ... | [-0.11150525831767628, 0.31511452309386706, -0.0010645040010492648, 0.23813159508450377, -0.11952602999505177, -0.2671666360555357, -0.008551346994335613, 0.3207042572133604, -0.23059021886838701, -0.2751828626208809, -0.017560848483054708, -0.28993914250324493, -0.03157095054304728, 0.13076102030363373, 0.030106368393... |
710.2215 | Modelling the time variation of the surface differential rotation in AB
Doradus and LQ Hydrae | Sequences of Doppler images of the young, rapidly rotating late-type stars AB
Dor and LQ Hya show that their equatorial angular velocity and the amplitude of
their surface differential rotation vary versus time. Such variations can be
modelled to obtain information on the intensity of the azimuthal magnetic
stresses ... | astro-ph | sequences of doppler images of the young rapidly rotating latetype stars ab dor and lq hya show that their equatorial angular velocity and the amplitude of their surface differential rotation vary versus time such variations can be modelled to obtain information on the intensity of the azimuthal magnetic stresses withi... | [['sequences', 'of', 'doppler', 'images', 'of', 'the', 'young', 'rapidly', 'rotating', 'latetype', 'stars', 'ab', 'dor', 'and', 'lq', 'hya', 'show', 'that', 'their', 'equatorial', 'angular', 'velocity', 'and', 'the', 'amplitude', 'of', 'their', 'surface', 'differential', 'rotation', 'vary', 'versus', 'time', 'such', 'v... | [-0.11077361845399265, 0.1746441625299041, -0.06462223919761645, 0.10898652005118209, -0.09204226149270286, -0.027692810493194824, 0.05127251073687833, 0.4013178515453617, -0.26348860697312787, -0.3196548506883638, 0.03260814812028321, -0.23193449084344622, -0.10412851492753374, 0.2148073950099045, -0.10048526028691271... |
710.2216 | The dying rabbit problem revisited | In this paper we study a generalization of the Fibonacci sequence in which
rabbits are mortal and take more that two months to become mature. In
particular we give a general recurrence relation for these sequences (improving
the work in the paper Hoggatt, V. E., Jr.; Lind, D. A. "The dying rabbit
problem". Fibonacci ... | math.NT | in this paper we study a generalization of the fibonacci sequence in which rabbits are mortal and take more that two months to become mature in particular we give a general recurrence relation for these sequences improving the work in the paper hoggatt v e jr lind d a the dying rabbit problem fibonacci quart 7 1969 no ... | [['in', 'this', 'paper', 'we', 'study', 'a', 'generalization', 'of', 'the', 'fibonacci', 'sequence', 'in', 'which', 'rabbits', 'are', 'mortal', 'and', 'take', 'more', 'that', 'two', 'months', 'to', 'become', 'mature', 'in', 'particular', 'we', 'give', 'a', 'general', 'recurrence', 'relation', 'for', 'these', 'sequences... | [-0.13812107493291265, 0.09627127144401809, -0.05172396143311047, 0.09613040875253342, -0.05101841516155112, -0.11905302479863167, 0.06490908054475514, 0.2967655288709982, -0.27783267723757205, -0.2885586927804324, 0.09469732435877426, -0.2755925140054141, -0.20299844127064487, 0.18562806937591853, -0.09755696197719993... |
710.2217 | Investigations on the relationship between $T_c$ and the superconducting
gap under magnetic and non-magnetic impurity substitutions in
YBa$_2$Cu$_3$O$_{7-\delta}$ | We report electronic Raman scattering measurements on optimally doped
YBa2Cu3O7 where Zn or Ni impurities have been substituted by Cu. Using Raman
selection rules, we have probed the superconducting gap in the nodal and
antinodal regions. We show that under impurity substitutions, the energy of the
antinodal peak det... | cond-mat.supr-con cond-mat.str-el | we report electronic raman scattering measurements on optimally doped yba2cu3o7 where zn or ni impurities have been substituted by cu using raman selection rules we have probed the superconducting gap in the nodal and antinodal regions we show that under impurity substitutions the energy of the antinodal peak detected ... | [['we', 'report', 'electronic', 'raman', 'scattering', 'measurements', 'on', 'optimally', 'doped', 'yba2cu3o7', 'where', 'zn', 'or', 'ni', 'impurities', 'have', 'been', 'substituted', 'by', 'cu', 'using', 'raman', 'selection', 'rules', 'we', 'have', 'probed', 'the', 'superconducting', 'gap', 'in', 'the', 'nodal', 'and'... | [-0.20185850289251123, 0.20348402445393038, -0.012489849306820403, 0.0356347662463252, -0.026721035436327967, -0.1527096156208288, 0.20952069029056777, 0.41299561270335244, -0.2234705412183844, -0.24427686545643068, -0.04535898672350283, -0.42142300982737824, -0.0894727663735726, 0.11881828366202257, 0.0434537089296749... |
710.2218 | Instantons in Deformed Super Yang-Mills Theories | We study the instanton effective action in deformed four-dimensional N=2 and
N=4 super Yang-Mills (SYM) theories. These deformed gauge theories are defined
on the D-brane world-volume in the presence of constant, self-dual
Ramond-Ramond (R-R) 3-form field strength background $\mathcal{F}$ which is
scaled as $(2 \pi \... | hep-th | we study the instanton effective action in deformed fourdimensional n2 and n4 super yangmills sym theories these deformed gauge theories are defined on the dbrane worldvolume in the presence of constant selfdual ramondramond rr 3form field strength background mathcalf which is scaled as 2 pi alpha12 mathcalf fixed in t... | [['we', 'study', 'the', 'instanton', 'effective', 'action', 'in', 'deformed', 'fourdimensional', 'n2', 'and', 'n4', 'super', 'yangmills', 'sym', 'theories', 'these', 'deformed', 'gauge', 'theories', 'are', 'defined', 'on', 'the', 'dbrane', 'worldvolume', 'in', 'the', 'presence', 'of', 'constant', 'selfdual', 'ramondram... | [-0.175490335093322, 0.22286882314529985, -0.02733984866621669, 0.09698435120082301, -0.03920718400287583, -0.16510747020330394, -0.04373918559914925, 0.28990860375566313, -0.1355779555513326, -0.2590162388938056, 0.015892434705312205, -0.28598048097708006, -0.19810937672401918, 0.042739748907736456, -0.060393013064796... |
710.2219 | Forces and momenta caused by electromagnetic waves in magnetoelectric
media | We analyse the propagation of electromagnetic waves in magnetoelectric media.
Recently, Feigel has predicted that such a medium may ``extract momentum from
vacuum" in the sense that the total momentum of the virtual waves (vacuum
fluctuations of the electromagnetic field) is nontrivial. Our aim is to check
the feasib... | physics.class-ph cond-mat.other gr-qc physics.gen-ph | we analyse the propagation of electromagnetic waves in magnetoelectric media recently feigel has predicted that such a medium may extract momentum from vacuum in the sense that the total momentum of the virtual waves vacuum fluctuations of the electromagnetic field is nontrivial our aim is to check the feasibility of t... | [['we', 'analyse', 'the', 'propagation', 'of', 'electromagnetic', 'waves', 'in', 'magnetoelectric', 'media', 'recently', 'feigel', 'has', 'predicted', 'that', 'such', 'a', 'medium', 'may', 'extract', 'momentum', 'from', 'vacuum', 'in', 'the', 'sense', 'that', 'the', 'total', 'momentum', 'of', 'the', 'virtual', 'waves',... | [-0.17323554602391536, 0.16522796767454292, -0.09772335215451657, 0.03672446097092082, -0.09169381073806235, -0.0108717769830017, 0.027273775431357564, 0.33705801736082763, -0.2439894601652619, -0.27960455315488, 0.025289826416185185, -0.2769372718101549, -0.14440050647814348, 0.16416744584397924, 0.01566793849070241, ... |
710.222 | Quantum phases of mixtures of atoms and molecules on optical lattices | We investigate the phase diagram of a two-species Bose-Hubbard model
including a conversion term, by which two particles from the first species can
be converted into one particle of the second species, and vice-versa. The model
can be related to ultra-cold atom experiments in which a Feshbach resonance
produces long-... | cond-mat.stat-mech | we investigate the phase diagram of a twospecies bosehubbard model including a conversion term by which two particles from the first species can be converted into one particle of the second species and viceversa the model can be related to ultracold atom experiments in which a feshbach resonance produces longlived boun... | [['we', 'investigate', 'the', 'phase', 'diagram', 'of', 'a', 'twospecies', 'bosehubbard', 'model', 'including', 'a', 'conversion', 'term', 'by', 'which', 'two', 'particles', 'from', 'the', 'first', 'species', 'can', 'be', 'converted', 'into', 'one', 'particle', 'of', 'the', 'second', 'species', 'and', 'viceversa', 'the... | [-0.11397868293523275, 0.2274797785882102, -0.062038446838200534, 0.050447682909126504, 0.0037169938715284363, -0.1615277260699419, 0.05761097281185143, 0.3334537305978729, -0.26217744285959804, -0.29597168450024636, 0.02950552863031215, -0.28440543286748887, -0.09490944426643717, 0.16674491530712282, 0.066937337547321... |
710.2221 | LAMBDA: Large Area Modular BaF2 Detector Array for the measurement of
high energy gamma rays | A large BaF2 detector array along with its dedicated CAMAC electronics and
VME based data acquisition system has been designed, constructed and installed
successfully at VECC, Kolkata for studying high energy gamma rays (E>8 MeV).
The array consists of 162 detector elements. The detectors were fabricated from
bare ba... | nucl-ex | a large baf2 detector array along with its dedicated camac electronics and vme based data acquisition system has been designed constructed and installed successfully at vecc kolkata for studying high energy gamma rays e8 mev the array consists of 162 detector elements the detectors were fabricated from bare barium fluo... | [['a', 'large', 'baf2', 'detector', 'array', 'along', 'with', 'its', 'dedicated', 'camac', 'electronics', 'and', 'vme', 'based', 'data', 'acquisition', 'system', 'has', 'been', 'designed', 'constructed', 'and', 'installed', 'successfully', 'at', 'vecc', 'kolkata', 'for', 'studying', 'high', 'energy', 'gamma', 'rays', '... | [-0.06036368502180141, 0.13106803826697042, -0.04447766494899558, 0.02082249516152879, 0.01190314463553735, -0.15383342678545614, -0.0007336175538911726, 0.439335201218229, -0.18487076199952665, -0.3996042751174183, 0.057961580155799546, -0.35524865176065723, 0.024700194901404526, 0.20104968072469695, 0.012536744783616... |
710.2222 | Dielectric Susceptibility and Heat Capacity of Ultra-Cold Glasses in
Magnetic Field | Recent experiments demonstrated unexpected, even intriguing properties of
certain glassy materials in magnetic field at low temperatures. We have studied
the magnetic field dependence of the static dielectric susceptibility and the
heat capacity of glasses at low temperatures. We present a theory in which we
consider... | cond-mat.dis-nn | recent experiments demonstrated unexpected even intriguing properties of certain glassy materials in magnetic field at low temperatures we have studied the magnetic field dependence of the static dielectric susceptibility and the heat capacity of glasses at low temperatures we present a theory in which we consider the ... | [['recent', 'experiments', 'demonstrated', 'unexpected', 'even', 'intriguing', 'properties', 'of', 'certain', 'glassy', 'materials', 'in', 'magnetic', 'field', 'at', 'low', 'temperatures', 'we', 'have', 'studied', 'the', 'magnetic', 'field', 'dependence', 'of', 'the', 'static', 'dielectric', 'susceptibility', 'and', 't... | [-0.18180014507379383, 0.1661053931378634, -0.020613108513852917, 0.05322462053393396, -0.05230336044377719, -0.0760701086718398, 0.03082826343523219, 0.38213368494493455, -0.24336139821351913, -0.31526423112537044, 0.045086722822489746, -0.2905006517166606, -0.10211028813575514, 0.17721921937892404, 0.0471590355707284... |
710.2223 | Experimental determination of the absorption strength in absorbing
chaotic cavities | Due to the experimental necessity we present a formula to determine the
absorption strength by power losses inside a chaotic system (cavities, graphs,
acoustic resonators, etc) when the antenna coupling, always present in
experimental measurements, is taken into account. This is done by calculating
the average of the... | cond-mat.mes-hall | due to the experimental necessity we present a formula to determine the absorption strength by power losses inside a chaotic system cavities graphs acoustic resonators etc when the antenna coupling always present in experimental measurements is taken into account this is done by calculating the average of the absorptio... | [['due', 'to', 'the', 'experimental', 'necessity', 'we', 'present', 'a', 'formula', 'to', 'determine', 'the', 'absorption', 'strength', 'by', 'power', 'losses', 'inside', 'a', 'chaotic', 'system', 'cavities', 'graphs', 'acoustic', 'resonators', 'etc', 'when', 'the', 'antenna', 'coupling', 'always', 'present', 'in', 'ex... | [-0.185508129947727, 0.10426686055512285, -0.014950697441441072, -0.004709385143606071, -0.027760397505120073, -0.14625546645084528, 0.06149701205160941, 0.3780110300007001, -0.23135984263999362, -0.2876967797449357, 0.061860884418448725, -0.29576076100199994, -0.11813658774948456, 0.1813587603539648, 0.024691152386367... |
710.2224 | The Plancherel Formula for the Universal Covering Group of SL(2,R)
Revisited | The Plancherel formula for the universal covering group of $SL(2, R)$ derived
earlier by Pukanszky on which Herb and Wolf build their Plancherel theorem for
general semisimple groups is reconsidered. It is shown that a set of unitarily
equivalent representations is treated by these authors as distinct.
Identification... | hep-th | the plancherel formula for the universal covering group of sl2 r derived earlier by pukanszky on which herb and wolf build their plancherel theorem for general semisimple groups is reconsidered it is shown that a set of unitarily equivalent representations is treated by these authors as distinct identification of this ... | [['the', 'plancherel', 'formula', 'for', 'the', 'universal', 'covering', 'group', 'of', 'sl2', 'r', 'derived', 'earlier', 'by', 'pukanszky', 'on', 'which', 'herb', 'and', 'wolf', 'build', 'their', 'plancherel', 'theorem', 'for', 'general', 'semisimple', 'groups', 'is', 'reconsidered', 'it', 'is', 'shown', 'that', 'a', ... | [-0.10190654572873045, 0.08812856110894392, -0.16982004016397462, 0.07763554738466477, -0.07752985915642292, -0.14528188514973847, 0.0034925684993786198, 0.3358311614983024, -0.2511227509427455, -0.23023516436167543, 0.11717481796081448, -0.2131906352456539, -0.13642341050229245, 0.2338013010692873, -0.1377995344059121... |
710.2225 | Dust in the wind: Crystalline silicates, corundum and periclase in PG
2112+059 | We have determined the mineralogical composition of dust in the Broad
Absorption Line (BAL) quasar PG 2112+059 using mid-infrared spectroscopy
obtained with the Spitzer Space Telescope. From spectral fitting of the solid
state features, we find evidence for Mg-rich amorphous silicates with olivine
stoichiometry, as w... | astro-ph | we have determined the mineralogical composition of dust in the broad absorption line bal quasar pg 2112059 using midinfrared spectroscopy obtained with the spitzer space telescope from spectral fitting of the solid state features we find evidence for mgrich amorphous silicates with olivine stoichiometry as well as the... | [['we', 'have', 'determined', 'the', 'mineralogical', 'composition', 'of', 'dust', 'in', 'the', 'broad', 'absorption', 'line', 'bal', 'quasar', 'pg', '2112059', 'using', 'midinfrared', 'spectroscopy', 'obtained', 'with', 'the', 'spitzer', 'space', 'telescope', 'from', 'spectral', 'fitting', 'of', 'the', 'solid', 'state... | [0.004699438038758587, 0.11926999127189088, -0.03497735770733291, 0.004007757196695608, -0.02168023584919527, -0.05187973592614452, 0.06869319507982148, 0.44150950957013857, -0.19412414907263917, -0.35519626919656644, 0.05057853579163811, -0.29460516535991066, -0.022808161477536656, 0.12631780328770537, -0.014087285793... |
710.2226 | Functional biases in GRB's spectral parameter correlations | Gamma Ray Bursts (GRBs) show evidence of different spectral shapes, light
curves, duration, host galaxies and they explode within a wide redshift range.
However, the most of them seems to follow very tight correlations among some
observed quantities relating to their energetic. If true, these correlations
have signif... | astro-ph | gamma ray bursts grbs show evidence of different spectral shapes light curves duration host galaxies and they explode within a wide redshift range however the most of them seems to follow very tight correlations among some observed quantities relating to their energetic if true these correlations have significant impli... | [['gamma', 'ray', 'bursts', 'grbs', 'show', 'evidence', 'of', 'different', 'spectral', 'shapes', 'light', 'curves', 'duration', 'host', 'galaxies', 'and', 'they', 'explode', 'within', 'a', 'wide', 'redshift', 'range', 'however', 'the', 'most', 'of', 'them', 'seems', 'to', 'follow', 'very', 'tight', 'correlations', 'amo... | [-0.04792101596533838, 0.12064815822135036, -0.08673976900883847, 0.24475843088080484, -0.09165342214206855, -0.09947617560418116, 0.07343872151311694, 0.4641002396576934, -0.22312690543476493, -0.37297312766727475, -0.005066832192242145, -0.343584758548273, -0.03812876789002783, 0.26704221992856925, 0.0148626553691509... |
710.2227 | A System for Predicting Subcellular Localization of Yeast Genome Using
Neural Network | The subcellular location of a protein can provide valuable information about
its function. With the rapid increase of sequenced genomic data, the need for
an automated and accurate tool to predict subcellular localization becomes
increasingly important. Many efforts have been made to predict protein
subcellular local... | cs.NE cs.AI | the subcellular location of a protein can provide valuable information about its function with the rapid increase of sequenced genomic data the need for an automated and accurate tool to predict subcellular localization becomes increasingly important many efforts have been made to predict protein subcellular localizati... | [['the', 'subcellular', 'location', 'of', 'a', 'protein', 'can', 'provide', 'valuable', 'information', 'about', 'its', 'function', 'with', 'the', 'rapid', 'increase', 'of', 'sequenced', 'genomic', 'data', 'the', 'need', 'for', 'an', 'automated', 'and', 'accurate', 'tool', 'to', 'predict', 'subcellular', 'localization',... | [-0.05309934643562883, 0.04935430816636654, -0.043983630831353364, 0.09997650151490234, -0.0552741010254249, -0.13505831131711601, 0.037635657946811986, 0.415821580439806, -0.2727174025215209, -0.32913326311856506, 0.08342690183431842, -0.25251785804051907, -0.2371461238572374, 0.1893357267975807, -0.08286471563158557,... |
710.2228 | Recommendation model based on opinion diffusion | Information overload in the modern society calls for highly efficient
recommendation algorithms. In this letter we present a novel diffusion based
recommendation model, with users' ratings built into a transition matrix. To
speed up computation we introduce a Green function method. The numerical tests
on a benchmark ... | physics.soc-ph cs.CY cs.IR physics.data-an | information overload in the modern society calls for highly efficient recommendation algorithms in this letter we present a novel diffusion based recommendation model with users ratings built into a transition matrix to speed up computation we introduce a green function method the numerical tests on a benchmark databas... | [['information', 'overload', 'in', 'the', 'modern', 'society', 'calls', 'for', 'highly', 'efficient', 'recommendation', 'algorithms', 'in', 'this', 'letter', 'we', 'present', 'a', 'novel', 'diffusion', 'based', 'recommendation', 'model', 'with', 'users', 'ratings', 'built', 'into', 'a', 'transition', 'matrix', 'to', 's... | [-0.07043566173573924, -0.032657637955399894, -0.08626899193041027, 0.03409682823171429, -0.11683934801889552, -0.1726645772203298, 0.11032321084274958, 0.4249138704232745, -0.2252908446747115, -0.2891674370364823, 0.06379139620289838, -0.3089070410104626, -0.2229623757302761, 0.1966841519313028, -0.08789366263436485, ... |
710.2229 | Precision for B-meson matrix elements | We demonstrate how HQET and the Step Scaling Method for B-physics, pioneered
by the Tor Vergata group, can be combined to reach a further improved
precision. The observables considered are the mass of the b-quark and the
B_s-meson decay constant. The demonstration is carried out in quenched lattice
QCD. We start from... | hep-lat | we demonstrate how hqet and the step scaling method for bphysics pioneered by the tor vergata group can be combined to reach a further improved precision the observables considered are the mass of the bquark and the b_smeson decay constant the demonstration is carried out in quenched lattice qcd we start from a small v... | [['we', 'demonstrate', 'how', 'hqet', 'and', 'the', 'step', 'scaling', 'method', 'for', 'bphysics', 'pioneered', 'by', 'the', 'tor', 'vergata', 'group', 'can', 'be', 'combined', 'to', 'reach', 'a', 'further', 'improved', 'precision', 'the', 'observables', 'considered', 'are', 'the', 'mass', 'of', 'the', 'bquark', 'and'... | [-0.06348828264865382, 0.15897951328383636, -0.11427178259018338, 0.0969102979719976, -0.02840849802690162, -0.09206272044015684, 0.10499486608441448, 0.3673209006705418, -0.22428166494308704, -0.2630348364854681, 0.08933765324429427, -0.2645194399459609, -0.03743202445142763, 0.17368299769633716, 0.014098218449487769,... |
710.223 | Collider signatures for unparticle | We summarize the works presented in Refs. \cite{1,2} on collider
phenomenology of the unparticle physics associated with an exact scale
invariant sector possessing a non-trivial infrared fixed point at a high energy
scale. We give highlights on the motivations of unparticle and derivation of
the phase space and the u... | hep-ph | we summarize the works presented in refs cite12 on collider phenomenology of the unparticle physics associated with an exact scale invariant sector possessing a nontrivial infrared fixed point at a high energy scale we give highlights on the motivations of unparticle and derivation of the phase space and the unparticle... | [['we', 'summarize', 'the', 'works', 'presented', 'in', 'refs', 'cite12', 'on', 'collider', 'phenomenology', 'of', 'the', 'unparticle', 'physics', 'associated', 'with', 'an', 'exact', 'scale', 'invariant', 'sector', 'possessing', 'a', 'nontrivial', 'infrared', 'fixed', 'point', 'at', 'a', 'high', 'energy', 'scale', 'we... | [-0.14924064130488648, 0.18653182083539557, -0.1077894901804884, 0.1585295697399247, -0.13396990505967243, -0.1524235919420888, 0.00468648106269314, 0.30956033830452395, -0.20127158641186824, -0.28256394773587046, -0.006776190768220428, -0.3040473288688135, -0.13869740392070218, 0.1311731983077185, 0.05046822647395802,... |
710.2231 | Comparison and Combination of State-of-the-art Techniques for
Handwritten Character Recognition: Topping the MNIST Benchmark | Although the recognition of isolated handwritten digits has been a research
topic for many years, it continues to be of interest for the research community
and for commercial applications. We show that despite the maturity of the
field, different approaches still deliver results that vary enough to allow
improvements... | cs.CV | although the recognition of isolated handwritten digits has been a research topic for many years it continues to be of interest for the research community and for commercial applications we show that despite the maturity of the field different approaches still deliver results that vary enough to allow improvements by u... | [['although', 'the', 'recognition', 'of', 'isolated', 'handwritten', 'digits', 'has', 'been', 'a', 'research', 'topic', 'for', 'many', 'years', 'it', 'continues', 'to', 'be', 'of', 'interest', 'for', 'the', 'research', 'community', 'and', 'for', 'commercial', 'applications', 'we', 'show', 'that', 'despite', 'the', 'mat... | [-0.07246921657892005, 0.011280571154012113, -0.055656557371596395, 0.04212553923328718, -0.03403820066098002, -0.11590984024813557, 0.06696227591582178, 0.4067784127797566, -0.23039384976370272, -0.3305963532804371, 0.1325222714400844, -0.2936346998097363, -0.13311009023801174, 0.295167615858125, -0.08723213061008578,... |
710.2232 | The Chandra Small Magellanic Cloud Wing Survey - the search for X-ray
Binaries | We have detected 523 sources in a survey of the Small Magellanic Cloud (SMC)
Wing with Chandra. By cross-correlating the X-ray data with optical and
near-infrared catalogues we have found 300 matches. Using a technique that
combines X-ray colours and X-ray to optical flux ratios we have been able to
assign preliminar... | astro-ph | we have detected 523 sources in a survey of the small magellanic cloud smc wing with chandra by crosscorrelating the xray data with optical and nearinfrared catalogues we have found 300 matches using a technique that combines xray colours and xray to optical flux ratios we have been able to assign preliminary classific... | [['we', 'have', 'detected', '523', 'sources', 'in', 'a', 'survey', 'of', 'the', 'small', 'magellanic', 'cloud', 'smc', 'wing', 'with', 'chandra', 'by', 'crosscorrelating', 'the', 'xray', 'data', 'with', 'optical', 'and', 'nearinfrared', 'catalogues', 'we', 'have', 'found', '300', 'matches', 'using', 'a', 'technique', '... | [-0.03545483366917604, 0.1103086388669908, -0.05920967021061537, 0.11294932739558415, -0.11041851631061246, -0.08031912526617256, 0.11745209749340295, 0.503796638118533, -0.1274431660126608, -0.3986037594713987, 0.06018815198555016, -0.372012535110116, -0.0279984382697596, 0.19612680287100376, -0.039563645143061876, -0... |
710.2233 | Global classification of two-component approximately integrable
evolution equations | We globally classify two-component evolution equations, with homogeneous
diagonal linear part, admitting infinitely many approximate symmetries.
Important ingredients are the symbolic calculus of Gel'fand and Dikii, the
Skolem-Mahler-Lech theorem, results on diophantine equations in roots of unity
by F. Beukers, and ... | nlin.SI | we globally classify twocomponent evolution equations with homogeneous diagonal linear part admitting infinitely many approximate symmetries important ingredients are the symbolic calculus of gelfand and dikii the skolemmahlerlech theorem results on diophantine equations in roots of unity by f beukers and an algorithm ... | [['we', 'globally', 'classify', 'twocomponent', 'evolution', 'equations', 'with', 'homogeneous', 'diagonal', 'linear', 'part', 'admitting', 'infinitely', 'many', 'approximate', 'symmetries', 'important', 'ingredients', 'are', 'the', 'symbolic', 'calculus', 'of', 'gelfand', 'and', 'dikii', 'the', 'skolemmahlerlech', 'th... | [-0.2017937687950002, 0.036386366874406426, -0.07678147374341886, 0.08012593394766251, -0.1103410160789887, -0.15817945185634824, -0.05937624058375756, 0.23838900056564147, -0.2946626335796383, -0.1966345792843236, 0.1025481770410099, -0.2726498684949345, -0.18095054460896387, 0.19473247069658506, -0.06844805377639002,... |
710.2234 | Associated production of a Kaluza-Klein excitation of a gluon with a t
t(bar) pair at the LHC | In Randall-Sundrum models, the Kaluza-Klein (KK) excitations of the gluon,
g_{KK} have enhanced couplings to the right-handed quarks. In the absence of a
gg g_{KK} coupling in these models, the single production of a g_{KK} from an
initial gg state is not possible. The search for other production mechanisms at
the LH... | hep-ph | in randallsundrum models the kaluzaklein kk excitations of the gluon g_kk have enhanced couplings to the righthanded quarks in the absence of a gg g_kk coupling in these models the single production of a g_kk from an initial gg state is not possible the search for other production mechanisms at the lhc therefore become... | [['in', 'randallsundrum', 'models', 'the', 'kaluzaklein', 'kk', 'excitations', 'of', 'the', 'gluon', 'g_kk', 'have', 'enhanced', 'couplings', 'to', 'the', 'righthanded', 'quarks', 'in', 'the', 'absence', 'of', 'a', 'gg', 'g_kk', 'coupling', 'in', 'these', 'models', 'the', 'single', 'production', 'of', 'a', 'g_kk', 'fro... | [-0.09682325893725724, 0.2850859895253497, -0.07792184826363116, 0.128540575424519, -0.03788966643178162, -0.1247045206589664, 0.030623649960344144, 0.2989545123294947, -0.2285272190347314, -0.2585313884898069, 0.003299298785389104, -0.3054867251677082, 0.013300242556377928, 0.14685775884278515, 0.08555959778877491, 0.... |
710.2235 | Proteins in a shear flow | The conformational dynamics of a single protein molecule in a shear flow is
investigated using Brownian dynamics simulations. A structure-based coarse
grained model of a protein is used. We consider two proteins, ubiquitin and
integrin, and find that at moderate shear rates they unfold through a sequence
of metastabl... | q-bio.BM | the conformational dynamics of a single protein molecule in a shear flow is investigated using brownian dynamics simulations a structurebased coarse grained model of a protein is used we consider two proteins ubiquitin and integrin and find that at moderate shear rates they unfold through a sequence of metastable state... | [['the', 'conformational', 'dynamics', 'of', 'a', 'single', 'protein', 'molecule', 'in', 'a', 'shear', 'flow', 'is', 'investigated', 'using', 'brownian', 'dynamics', 'simulations', 'a', 'structurebased', 'coarse', 'grained', 'model', 'of', 'a', 'protein', 'is', 'used', 'we', 'consider', 'two', 'proteins', 'ubiquitin', ... | [-0.1344606532103308, 0.17944608686970387, -0.11440488787015603, 0.06565902412998652, 0.008157202219837798, -0.12350750833222296, 0.03687389335796995, 0.4045006657118159, -0.32380210377473745, -0.20454087196766868, 0.04475575812630751, -0.22619643321145425, -0.1917096095147287, 0.14512189914085036, 0.023425432595844686... |
710.2236 | Running of $\alpha_s$ in the MSSM with three-loop accuracy | The evolution of the strong coupling constant $\alpha_s$ from $M_Z$ to the
GUT scale is presented, involving three-loop running and two-loop decoupling.
Accordingly, the two-loop transition from the $\bar{\rm MS}$ to the $\bar{\rm
DR}$ scheme is properly taken into account. We find that the three-loop effects
are com... | hep-ph | the evolution of the strong coupling constant alpha_s from m_z to the gut scale is presented involving threeloop running and twoloop decoupling accordingly the twoloop transition from the barrm ms to the barrm dr scheme is properly taken into account we find that the threeloop effects are comparable to the experimental... | [['the', 'evolution', 'of', 'the', 'strong', 'coupling', 'constant', 'alpha_s', 'from', 'm_z', 'to', 'the', 'gut', 'scale', 'is', 'presented', 'involving', 'threeloop', 'running', 'and', 'twoloop', 'decoupling', 'accordingly', 'the', 'twoloop', 'transition', 'from', 'the', 'barrm', 'ms', 'to', 'the', 'barrm', 'dr', 'sc... | [-0.1147926940724978, 0.21614049204314748, -0.08937922858253673, 0.1507619285688701, -0.07421526424931707, -0.06848888996453886, 0.04454938001516792, 0.3321348986484938, -0.18565791265832055, -0.2917907493257964, 0.05767715803382022, -0.2964782950433868, 0.021031090972462186, 0.14742533883933598, 0.08586205621422441, 0... |
710.2237 | Formation, fractionation and excitation of carbon monoxide in diffuse
clouds | Aims: Our aims are threefold: a) To compare the $uv$ and mm-wave results; b)
to interpret 13CO and 12CO abundances in terms of the physical processes which
separately and jointly determine them; c) to interpret observed J=1-0
rotational excitation and line brightness in terms of ambient gas properties.
Methods: A s... | astro-ph | aims our aims are threefold a to compare the uv and mmwave results b to interpret 13co and 12co abundances in terms of the physical processes which separately and jointly determine them c to interpret observed j10 rotational excitation and line brightness in terms of ambient gas properties methods a simple phenomenolog... | [['aims', 'our', 'aims', 'are', 'threefold', 'a', 'to', 'compare', 'the', 'uv', 'and', 'mmwave', 'results', 'b', 'to', 'interpret', '13co', 'and', '12co', 'abundances', 'in', 'terms', 'of', 'the', 'physical', 'processes', 'which', 'separately', 'and', 'jointly', 'determine', 'them', 'c', 'to', 'interpret', 'observed', ... | [-0.04342723187811908, 0.09308150507627254, 0.012215810656113532, 0.08120818894516985, -0.021158435046265932, -0.10952167478570878, 0.07561722765812307, 0.4519361874757751, -0.19155675049665502, -0.30529606705350637, 0.027564843215197504, -0.22706087993218302, -0.04610639601343032, 0.14922532838999827, 0.02222331565153... |
710.2238 | Disentanglement in qubit-qutrit systems | We examine the phenomenon of {\it entanglement sudden death} (ESD) for $(2
\times 3)$-dimensional systems. As for $2 \times 2$ systems, the negativity
vanishes in finite time for some entangled pure as well as mixed states. While
locally equivalent pure states do so asymptotically. Interference between the
decay of t... | quant-ph | we examine the phenomenon of it entanglement sudden death esd for 2 times 3dimensional systems as for 2 times 2 systems the negativity vanishes in finite time for some entangled pure as well as mixed states while locally equivalent pure states do so asymptotically interference between the decay of the two upper levels ... | [['we', 'examine', 'the', 'phenomenon', 'of', 'it', 'entanglement', 'sudden', 'death', 'esd', 'for', '2', 'times', '3dimensional', 'systems', 'as', 'for', '2', 'times', '2', 'systems', 'the', 'negativity', 'vanishes', 'in', 'finite', 'time', 'for', 'some', 'entangled', 'pure', 'as', 'well', 'as', 'mixed', 'states', 'wh... | [-0.1218686730683069, 0.22287182360613608, -0.027674202718224156, 0.11995983270154444, 0.10912271276088979, -0.2085818970192443, 0.06795230877640493, 0.34263159653774516, -0.21653514366377802, -0.25384233722819344, 0.12113534174140488, -0.2822126195053844, -0.09559115538757075, 0.15515643651280484, -0.03897669992190512... |
710.2239 | Magnetic fields in noncommutative quantum mechanics | We discuss various descriptions of a quantum particle on noncommutative space
in a (possibly non-constant) magnetic field. We have tried to present the basic
facts in a unified and synthetic manner, and to clarify the relationship
between various approaches and results that are scattered in the literature.
| quant-ph | we discuss various descriptions of a quantum particle on noncommutative space in a possibly nonconstant magnetic field we have tried to present the basic facts in a unified and synthetic manner and to clarify the relationship between various approaches and results that are scattered in the literature | [['we', 'discuss', 'various', 'descriptions', 'of', 'a', 'quantum', 'particle', 'on', 'noncommutative', 'space', 'in', 'a', 'possibly', 'nonconstant', 'magnetic', 'field', 'we', 'have', 'tried', 'to', 'present', 'the', 'basic', 'facts', 'in', 'a', 'unified', 'and', 'synthetic', 'manner', 'and', 'to', 'clarify', 'the', ... | [-0.09426315871879776, 0.10541991483756995, -0.10088557813395845, 0.11120389778404793, -0.08797921174939008, -0.07444131749860466, 0.008944031574386866, 0.43469195852571346, -0.24612783363207857, -0.32394780234453524, 0.0730053426702804, -0.2711805954496277, -0.19412180000638707, 0.21439807692869625, -0.091151041057991... |
710.224 | The radiative lifetime of metastable CO ($a^3\Pi, v=0$) | We present a combined experimental and theoretical study on the radiative
lifetime of CO in the $a^3\Pi_{1,2}, v=0$ state. CO molecules in a beam are
prepared in selected rotational levels of this metastable state,
Stark-decelerated and electrostatically trapped. From the phosphorescence decay
in the trap, the radiat... | physics.atom-ph physics.chem-ph | we present a combined experimental and theoretical study on the radiative lifetime of co in the a3pi_12 v0 state co molecules in a beam are prepared in selected rotational levels of this metastable state starkdecelerated and electrostatically trapped from the phosphorescence decay in the trap the radiative lifetime is ... | [['we', 'present', 'a', 'combined', 'experimental', 'and', 'theoretical', 'study', 'on', 'the', 'radiative', 'lifetime', 'of', 'co', 'in', 'the', 'a3pi_12', 'v0', 'state', 'co', 'molecules', 'in', 'a', 'beam', 'are', 'prepared', 'in', 'selected', 'rotational', 'levels', 'of', 'this', 'metastable', 'state', 'starkdecele... | [-0.10308581117626127, 0.21057633556691663, 0.013594849671864388, 0.04240998597839391, 0.08029706683485027, -0.12139065985149723, 0.10994922225981267, 0.4142914421248193, -0.22300644742553027, -0.2875864548817733, 0.018027932879667044, -0.2772046880112315, 0.06899416272775555, 0.13534295369813942, 0.08493525541401753, ... |
710.2241 | A Catalog of Galaxy Clusters Observed by XMM-Newton | Aims: We present a uniform catalog of the images and radial profiles of the
temperature, abundance, and brightness for 70 clusters of galaxies observed by
XMM-Newton.
Methods: We use a new "first principles" approach to the modeling and removal
of the background components; the quiescent particle background, the co... | astro-ph | aims we present a uniform catalog of the images and radial profiles of the temperature abundance and brightness for 70 clusters of galaxies observed by xmmnewton methods we use a new first principles approach to the modeling and removal of the background components the quiescent particle background the cosmic diffuse e... | [['aims', 'we', 'present', 'a', 'uniform', 'catalog', 'of', 'the', 'images', 'and', 'radial', 'profiles', 'of', 'the', 'temperature', 'abundance', 'and', 'brightness', 'for', '70', 'clusters', 'of', 'galaxies', 'observed', 'by', 'xmmnewton', 'methods', 'we', 'use', 'a', 'new', 'first', 'principles', 'approach', 'to', '... | [-0.04955950143094493, 0.10109969092177619, -0.09144172315350979, 0.09702931124851794, -0.06641866492741667, -0.017281265054311677, 0.04158701754702059, 0.453623356689748, -0.16737655961065015, -0.37548934465035255, 0.03675076303280596, -0.3388137704888849, -0.04672210147040651, 0.18918830323979674, -0.0261609087649144... |
710.2242 | Non-vanishing theorems for rank 2 bundles on P^3: a simple approach
without the speciality lemma | The paper investigates vanishing conditions on the first cohomology module of
a normalized rank 2 vector bundle E on P^3 which force E to split, and finds
therefore strategic levels of non-vanishing for a non-split bundle. The present
conditions improve other conditions known in the literature and are obtained
with s... | math.AG | the paper investigates vanishing conditions on the first cohomology module of a normalized rank 2 vector bundle e on p3 which force e to split and finds therefore strategic levels of nonvanishing for a nonsplit bundle the present conditions improve other conditions known in the literature and are obtained with simple c... | [['the', 'paper', 'investigates', 'vanishing', 'conditions', 'on', 'the', 'first', 'cohomology', 'module', 'of', 'a', 'normalized', 'rank', '2', 'vector', 'bundle', 'e', 'on', 'p3', 'which', 'force', 'e', 'to', 'split', 'and', 'finds', 'therefore', 'strategic', 'levels', 'of', 'nonvanishing', 'for', 'a', 'nonsplit', 'b... | [-0.2116300125739404, 0.0318572767877153, -0.08813855469759022, 0.06389248961848872, -0.10791350654658995, -0.1768207729727562, 0.02165200601032536, 0.31040281283536125, -0.3017981003969908, -0.250108820452754, 0.08754367111749681, -0.20091714476501302, -0.1271845025409545, 0.1975473361688533, -0.11225596855261497, 0.0... |
710.2243 | Edge Local Complementation and Equivalence of Binary Linear Codes | Orbits of graphs under the operation edge local complementation (ELC) are
defined. We show that the ELC orbit of a bipartite graph corresponds to the
equivalence class of a binary linear code. The information sets and the minimum
distance of a code can be derived from the corresponding ELC orbit. By
extending earlier... | math.CO cs.IT math.IT | orbits of graphs under the operation edge local complementation elc are defined we show that the elc orbit of a bipartite graph corresponds to the equivalence class of a binary linear code the information sets and the minimum distance of a code can be derived from the corresponding elc orbit by extending earlier result... | [['orbits', 'of', 'graphs', 'under', 'the', 'operation', 'edge', 'local', 'complementation', 'elc', 'are', 'defined', 'we', 'show', 'that', 'the', 'elc', 'orbit', 'of', 'a', 'bipartite', 'graph', 'corresponds', 'to', 'the', 'equivalence', 'class', 'of', 'a', 'binary', 'linear', 'code', 'the', 'information', 'sets', 'an... | [-0.17806142924920373, 0.07868690311822676, -0.07874977351773692, 0.05806407157291213, -0.05508251134913577, -0.14917367760537434, 0.08110317450178706, 0.3913722796360557, -0.2857399542876722, -0.3137890042119619, 0.10425619490991306, -0.23892255636620457, -0.11510288219332047, 0.21891357491562224, -0.08721249398987983... |
710.2244 | Compact oscillons in the signum-Gordon model | We present explicit solutions of the signum-Gordon scalar field equation
which have finite energy and are periodic in time. Such oscillons have a
strictly finite size. They do not emit radiation.
| hep-th astro-ph cond-mat.other nlin.SI | we present explicit solutions of the signumgordon scalar field equation which have finite energy and are periodic in time such oscillons have a strictly finite size they do not emit radiation | [['we', 'present', 'explicit', 'solutions', 'of', 'the', 'signumgordon', 'scalar', 'field', 'equation', 'which', 'have', 'finite', 'energy', 'and', 'are', 'periodic', 'in', 'time', 'such', 'oscillons', 'have', 'a', 'strictly', 'finite', 'size', 'they', 'do', 'not', 'emit', 'radiation']] | [-0.17326763164131873, 0.24884207754005347, -0.11951394212402162, 0.11797002841147684, -0.12130071496170375, -0.15749572324115904, -0.07235046286856936, 0.4210613261187269, -0.18546305861203902, -0.24924285854062728, 0.11769926517585953, -0.28645236016581616, -0.06414296550135459, 0.13748330118570237, 0.008912198125354... |
710.2245 | Size, power and false discovery rates | Modern scientific technology has provided a new class of large-scale
simultaneous inference problems, with thousands of hypothesis tests to consider
at the same time. Microarrays epitomize this type of technology, but similar
situations arise in proteomics, spectroscopy, imaging, and social science
surveys. This pape... | math.ST stat.TH | modern scientific technology has provided a new class of largescale simultaneous inference problems with thousands of hypothesis tests to consider at the same time microarrays epitomize this type of technology but similar situations arise in proteomics spectroscopy imaging and social science surveys this paper uses fal... | [['modern', 'scientific', 'technology', 'has', 'provided', 'a', 'new', 'class', 'of', 'largescale', 'simultaneous', 'inference', 'problems', 'with', 'thousands', 'of', 'hypothesis', 'tests', 'to', 'consider', 'at', 'the', 'same', 'time', 'microarrays', 'epitomize', 'this', 'type', 'of', 'technology', 'but', 'similar', ... | [-0.07426977818372699, -0.019360414058507854, -0.06011390319408875, 0.13631390017608155, -0.11800298155252625, -0.1863296737002445, 0.11978313502032494, 0.3611471013700537, -0.24695953138133275, -0.34649556316107405, 0.13260617869345367, -0.2702554666977679, -0.14069077858379977, 0.2732925740182137, -0.0818741809650329... |
710.2246 | Probing the Slope of Cluster Mass Profile with Gravitational Einstein
Rings: Application to Abell 1689 | The strong lensing modelling of gravitational ``rings'' formed around massive
galaxies is sensitive to the amplitude of the external shear and convergence
produced by nearby mass condensations. In current wide field surveys, it is now
possible to find out a large number of rings, typically 10 gravitational rings
per ... | astro-ph | the strong lensing modelling of gravitational rings formed around massive galaxies is sensitive to the amplitude of the external shear and convergence produced by nearby mass condensations in current wide field surveys it is now possible to find out a large number of rings typically 10 gravitational rings per square de... | [['the', 'strong', 'lensing', 'modelling', 'of', 'gravitational', 'rings', 'formed', 'around', 'massive', 'galaxies', 'is', 'sensitive', 'to', 'the', 'amplitude', 'of', 'the', 'external', 'shear', 'and', 'convergence', 'produced', 'by', 'nearby', 'mass', 'condensations', 'in', 'current', 'wide', 'field', 'surveys', 'it... | [-0.12054899446161584, 0.05029114202958683, -0.0918778609713824, 0.10082930577356883, -0.05706734229292115, -0.062387334692103814, -0.009731182673707458, 0.3789386365727838, -0.22424979802459624, -0.34195521553482844, 0.056718881108931134, -0.2504680816478697, -0.06693334488445903, 0.21554893810815853, 0.01229914301877... |
710.2247 | New Companions for the lonely Crab? VHE emission from young pulsar wind
nebulae revealed by H.E.S.S | The deeper and more extended survey of the central parts of the Galactic
Plane by H.E.S.S. during 2005-2007 has revealed a number of new point-like, as
well as, extended sources. Two point-like sources can be associated to two
remarkable objects around "Crab-like" young and energetic pulsars in our
Galaxy: G21.5-0.9 ... | astro-ph | the deeper and more extended survey of the central parts of the galactic plane by hess during 20052007 has revealed a number of new pointlike as well as extended sources two pointlike sources can be associated to two remarkable objects around crablike young and energetic pulsars in our galaxy g21509 and kes 75 the char... | [['the', 'deeper', 'and', 'more', 'extended', 'survey', 'of', 'the', 'central', 'parts', 'of', 'the', 'galactic', 'plane', 'by', 'hess', 'during', '20052007', 'has', 'revealed', 'a', 'number', 'of', 'new', 'pointlike', 'as', 'well', 'as', 'extended', 'sources', 'two', 'pointlike', 'sources', 'can', 'be', 'associated', ... | [-0.08362505019827307, 0.10309050874510671, -0.04490559926489368, 0.14389821257003965, -0.11376121727859273, -0.06828566220835508, 0.04205619135652395, 0.4078163427355535, -0.17965302128783045, -0.37527305216473694, 0.08548966591650456, -0.31661487018744294, -0.06608859646846266, 0.25904930235051055, -0.030236482472152... |
710.2248 | RXTE confirmation of the Intermediate Polar status of Swift J0732.5-1331 | Aims. We intend to establish the X-ray properties of Swift J0732.5-1331 and
therefore confirm its status as an intermediate polar. Method. We analysed
36,240 s of X-ray data from RXTE. Frequency analysis was used to constrain
temporal variations and spectral analysis used to characterise the emission and
absorption p... | astro-ph | aims we intend to establish the xray properties of swift j073251331 and therefore confirm its status as an intermediate polar method we analysed 36240 s of xray data from rxte frequency analysis was used to constrain temporal variations and spectral analysis used to characterise the emission and absorption properties r... | [['aims', 'we', 'intend', 'to', 'establish', 'the', 'xray', 'properties', 'of', 'swift', 'j073251331', 'and', 'therefore', 'confirm', 'its', 'status', 'as', 'an', 'intermediate', 'polar', 'method', 'we', 'analysed', '36240', 's', 'of', 'xray', 'data', 'from', 'rxte', 'frequency', 'analysis', 'was', 'used', 'to', 'const... | [-0.07626292665090953, 0.12855757456019357, -0.045892983768886376, 0.07380344805161228, -0.06435845320623729, -0.10754277319797585, 0.07674884351323388, 0.4774815403976508, -0.19928287734247505, -0.3376593996297508, 0.08275046101545976, -0.3299767333683708, -0.0078098851879457795, 0.19270377106506437, -0.00139541554099... |
710.2249 | Total cross section of pp -> pK+Lambda reaction near threshold | The total cross sections of the pp -> pK+ Lambda reaction near threshold
measured at the COSY(Juelich) synchrotron using the internal target facility
COSY-11 are described in the frame of the model taking into account the one
pion and one kaon exchange as well as the final state interaction mechanisms.
| hep-ph | the total cross sections of the pp pk lambda reaction near threshold measured at the cosyjuelich synchrotron using the internal target facility cosy11 are described in the frame of the model taking into account the one pion and one kaon exchange as well as the final state interaction mechanisms | [['the', 'total', 'cross', 'sections', 'of', 'the', 'pp', 'pk', 'lambda', 'reaction', 'near', 'threshold', 'measured', 'at', 'the', 'cosyjuelich', 'synchrotron', 'using', 'the', 'internal', 'target', 'facility', 'cosy11', 'are', 'described', 'in', 'the', 'frame', 'of', 'the', 'model', 'taking', 'into', 'account', 'the'... | [-0.03289211801329286, 0.1784640354845597, -0.08618729577663507, 0.14040157434587575, 0.039602339742895294, -0.10511315781242993, 0.029453345612451737, 0.3241671291607603, -0.24627664183475534, -0.2925889992288181, -0.053340747071030946, -0.3552267885557851, 0.09369436982182824, 0.14853882637083987, 0.16961048801942746... |
710.225 | Efficient Simulations of Interstellar Gas-Grain Chemistry Using Moment
Equations | Networks of reactions on dust grain surfaces play a crucial role in the
chemistry of interstellar clouds, leading to the formation of molecular
hydrogen in diffuse clouds as well as various organic molecules in dense
molecular clouds. Due to the sub-micron size of the grains and the low flux,
the population of reacti... | astro-ph | networks of reactions on dust grain surfaces play a crucial role in the chemistry of interstellar clouds leading to the formation of molecular hydrogen in diffuse clouds as well as various organic molecules in dense molecular clouds due to the submicron size of the grains and the low flux the population of reactive spe... | [['networks', 'of', 'reactions', 'on', 'dust', 'grain', 'surfaces', 'play', 'a', 'crucial', 'role', 'in', 'the', 'chemistry', 'of', 'interstellar', 'clouds', 'leading', 'to', 'the', 'formation', 'of', 'molecular', 'hydrogen', 'in', 'diffuse', 'clouds', 'as', 'well', 'as', 'various', 'organic', 'molecules', 'in', 'dense... | [-0.09836962647822513, 0.09091504700314589, -0.04488421024923341, 0.041608647232830615, 0.0029100147326906285, -0.09479464287172534, 0.02676706340248992, 0.3358072015585121, -0.24535279288263379, -0.31840562156797525, 0.044426273560140304, -0.25529677526813427, -0.12515303966851382, 0.20377999655679316, -0.003750178622... |
710.2251 | Phenomenological applications of non-perturbative heavy quark effective
theory | We briefly review the strategy to perform non-perturbative heavy quark
effective theory computations and we specialize to the case of the b quark mass
which has recently been computed including the 1/m term.
| hep-lat | we briefly review the strategy to perform nonperturbative heavy quark effective theory computations and we specialize to the case of the b quark mass which has recently been computed including the 1m term | [['we', 'briefly', 'review', 'the', 'strategy', 'to', 'perform', 'nonperturbative', 'heavy', 'quark', 'effective', 'theory', 'computations', 'and', 'we', 'specialize', 'to', 'the', 'case', 'of', 'the', 'b', 'quark', 'mass', 'which', 'has', 'recently', 'been', 'computed', 'including', 'the', '1m', 'term']] | [-0.05299933035999085, 0.18139755152956102, -0.09968357307441307, 0.11246445535145926, -0.07262200540439649, -0.1432887055544239, 0.0683829506231246, 0.3325323529089942, -0.17034586152118264, -0.2775835268425219, 0.07647796806343125, -0.2712435218872446, -0.11921653484530521, 0.11271565514757778, -0.0075006931455749454... |
710.2252 | The Spectrum of 1ES0229 + 200 and the Cosmic Infrared Background | We examine the effect of gamma-ray absorption by the extragalactic infrared
radiation on intrinsic spectra predicted for 1ES0229+200 and compare our
results with the observational data. We find agreement with our previous
results on the shape of the IR spectral energy distribution (SED), contrary to
the recent assert... | astro-ph | we examine the effect of gammaray absorption by the extragalactic infrared radiation on intrinsic spectra predicted for 1es0229200 and compare our results with the observational data we find agreement with our previous results on the shape of the ir spectral energy distribution sed contrary to the recent assertion of t... | [['we', 'examine', 'the', 'effect', 'of', 'gammaray', 'absorption', 'by', 'the', 'extragalactic', 'infrared', 'radiation', 'on', 'intrinsic', 'spectra', 'predicted', 'for', '1es0229200', 'and', 'compare', 'our', 'results', 'with', 'the', 'observational', 'data', 'we', 'find', 'agreement', 'with', 'our', 'previous', 're... | [-0.01064998791286657, 0.09890234940235018, -0.10092635947367667, 0.13028671594616953, -0.0413940472248015, -0.07397928756582944, 0.009462343862474853, 0.4683921888507717, -0.1524312866635074, -0.42608512019210343, 0.03794847250932281, -0.3146097864469152, 0.0038827397577946457, 0.22770146639213726, -0.0044956013571299... |
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