id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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709.4235 | Extended matter coupled to BF theory | Recently, a topological field theory of membrane-matter coupled to BF theory
in arbitrary spacetime dimensions was proposed [1]. In this paper, we discuss
various aspects of the four-dimensional theory. Firstly, we study classical
solutions leading to an interpretation of the theory in terms of strings
propagating on... | gr-qc | recently a topological field theory of membranematter coupled to bf theory in arbitrary spacetime dimensions was proposed 1 in this paper we discuss various aspects of the fourdimensional theory firstly we study classical solutions leading to an interpretation of the theory in terms of strings propagating on a flat spa... | [['recently', 'a', 'topological', 'field', 'theory', 'of', 'membranematter', 'coupled', 'to', 'bf', 'theory', 'in', 'arbitrary', 'spacetime', 'dimensions', 'was', 'proposed', '1', 'in', 'this', 'paper', 'we', 'discuss', 'various', 'aspects', 'of', 'the', 'fourdimensional', 'theory', 'firstly', 'we', 'study', 'classical... | [-0.15329907898158404, 0.13793890561852054, -0.11128342259703701, 0.07612067232359883, -0.053529264775055055, -0.0766356852410347, -0.010896010798906893, 0.29521880992723787, -0.23767891603003022, -0.26288534634309385, 0.0390556794911168, -0.27067814689868963, -0.25217507549966794, 0.10833093175710755, -0.0865801502719... |
709.4236 | HST search for M subdwarf binaries | We present HST/ACS observations of 19 nearby M subdwarfs in a search for
binary systems. Other than the wide common proper motion pair LHS 2140/2139,
none of our sdM and esdM targets are found to be binaries. Our survey is
sensitive to equal-luminosity companions at close (2-8 AU) separations, while
sub-stellar secon... | astro-ph | we present hstacs observations of 19 nearby m subdwarfs in a search for binary systems other than the wide common proper motion pair lhs 21402139 none of our sdm and esdm targets are found to be binaries our survey is sensitive to equalluminosity companions at close 28 au separations while substellar secondaries could ... | [['we', 'present', 'hstacs', 'observations', 'of', '19', 'nearby', 'm', 'subdwarfs', 'in', 'a', 'search', 'for', 'binary', 'systems', 'other', 'than', 'the', 'wide', 'common', 'proper', 'motion', 'pair', 'lhs', '21402139', 'none', 'of', 'our', 'sdm', 'and', 'esdm', 'targets', 'are', 'found', 'to', 'be', 'binaries', 'ou... | [-0.08397225089336241, 0.13895015401201685, -0.04494335262947055, 0.09164469985202225, -0.07041993004687917, -0.07348399466862625, 0.07343993615205384, 0.3820934142462491, -0.13345746669254385, -0.4096325692834437, 0.04082457169509268, -0.304364961749496, 0.0016971727519637287, 0.22152852743599724, -0.05568931623524909... |
709.4237 | Type Ia Supernova: Burning and Detonation in the Distributed Regime | A simple, semi-analytic representation is developed for nuclear burning in
Type Ia supernovae in the special case where turbulent eddies completely
disrupt the flame. The speed and width of the ``distributed'' flame front are
derived. For the conditions considered, the burning front can be considered as
a turbulent f... | astro-ph | a simple semianalytic representation is developed for nuclear burning in type ia supernovae in the special case where turbulent eddies completely disrupt the flame the speed and width of the distributed flame front are derived for the conditions considered the burning front can be considered as a turbulent flame brush ... | [['a', 'simple', 'semianalytic', 'representation', 'is', 'developed', 'for', 'nuclear', 'burning', 'in', 'type', 'ia', 'supernovae', 'in', 'the', 'special', 'case', 'where', 'turbulent', 'eddies', 'completely', 'disrupt', 'the', 'flame', 'the', 'speed', 'and', 'width', 'of', 'the', 'distributed', 'flame', 'front', 'are... | [-0.11493084149840636, 0.22998012382486444, -0.03575109450628056, 0.08383916604861642, -0.05865781401524789, -0.11266391425944712, -0.014690098061296, 0.35527589013697075, -0.27670430280917585, -0.2381636507771149, 0.09843834446502381, -0.20226635499603945, -0.015650859989580653, 0.19216250477447397, -0.046067165193469... |
709.4238 | Generic local distinguishability and completely entangled subspaces | A subspace of a multipartite Hilbert space is completely entangled if it
contains no product states. Such subspaces can be large with a known maximum
size, S, approaching the full dimension of the system, D. We show that almost
all subspaces with dimension less than or equal to S are completely entangled,
and then us... | quant-ph | a subspace of a multipartite hilbert space is completely entangled if it contains no product states such subspaces can be large with a known maximum size s approaching the full dimension of the system d we show that almost all subspaces with dimension less than or equal to s are completely entangled and then use this f... | [['a', 'subspace', 'of', 'a', 'multipartite', 'hilbert', 'space', 'is', 'completely', 'entangled', 'if', 'it', 'contains', 'no', 'product', 'states', 'such', 'subspaces', 'can', 'be', 'large', 'with', 'a', 'known', 'maximum', 'size', 's', 'approaching', 'the', 'full', 'dimension', 'of', 'the', 'system', 'd', 'we', 'sho... | [-0.14308514037605272, 0.2454031777131337, -0.06753552858845903, 0.06346865191867729, 0.0017686042328014834, -0.23234812074998787, 0.01920404438775272, 0.3513018797245731, -0.25033853954951696, -0.19985461047500236, 0.08835465045979059, -0.3102679819844817, -0.0985792781196432, 0.17511927600257918, -0.04785250495999641... |
709.4239 | An introduction to the geometry of metric spaces | These informal notes deal with some basic properties of metric spaces,
especially concerning lengths of curves.
| math.MG | these informal notes deal with some basic properties of metric spaces especially concerning lengths of curves | [['these', 'informal', 'notes', 'deal', 'with', 'some', 'basic', 'properties', 'of', 'metric', 'spaces', 'especially', 'concerning', 'lengths', 'of', 'curves']] | [-0.17854493553750217, 0.130896651869989, -0.09679733286611736, 0.22778915101662278, -0.1732296982227126, -0.15474156063282862, -0.03313698060810566, 0.4295058436691761, -0.2563018170185387, -0.22691336349816993, 0.1951260914793238, -0.3125402699224651, -0.16262467321939766, 0.266822217265144, -0.25443334912415594, 0.0... |
709.424 | The Impact of Carbon Enhancement on Extra Mixing in Metal-Poor Stars | We critically examine the constraints imposed by carbon-enhanced metal-poor
(CEMP) stars on the mixing mechanisms that operate in red giants. CEMP stars
are created when the surface layers of a metal-poor dwarf are enriched with
He-burning products via mass transfer from an evolved donor. The difference
between main ... | astro-ph | we critically examine the constraints imposed by carbonenhanced metalpoor cemp stars on the mixing mechanisms that operate in red giants cemp stars are created when the surface layers of a metalpoor dwarf are enriched with heburning products via mass transfer from an evolved donor the difference between main sequence m... | [['we', 'critically', 'examine', 'the', 'constraints', 'imposed', 'by', 'carbonenhanced', 'metalpoor', 'cemp', 'stars', 'on', 'the', 'mixing', 'mechanisms', 'that', 'operate', 'in', 'red', 'giants', 'cemp', 'stars', 'are', 'created', 'when', 'the', 'surface', 'layers', 'of', 'a', 'metalpoor', 'dwarf', 'are', 'enriched'... | [-0.03209210443758191, 0.24915818423978636, -0.029438853797574455, 0.11538697660972293, -0.11485874263318972, -0.04114056689879642, 0.1391834959822098, 0.40846688837672657, -0.15789510949443167, -0.3440354951012593, -0.016722858453151555, -0.2579725616710046, -0.035926612080612146, 0.15384510487828476, -0.1268282343006... |
709.4241 | Permutahedra and generalized associahedra | Given a finite Coxeter system $(W,S)$ and a Coxeter element $c$, we construct
a simple polytope whose outer normal fan is N. Reading's Cambrian fan $F_c$,
settling a conjecture of Reading that this is possible. We call this polytope
the $c$-generalized associahedron. Our approach generalizes Loday's realization
of th... | math.CO | given a finite coxeter system ws and a coxeter element c we construct a simple polytope whose outer normal fan is n readings cambrian fan f_c settling a conjecture of reading that this is possible we call this polytope the cgeneralized associahedron our approach generalizes lodays realization of the associahedron a typ... | [['given', 'a', 'finite', 'coxeter', 'system', 'ws', 'and', 'a', 'coxeter', 'element', 'c', 'we', 'construct', 'a', 'simple', 'polytope', 'whose', 'outer', 'normal', 'fan', 'is', 'n', 'readings', 'cambrian', 'fan', 'f_c', 'settling', 'a', 'conjecture', 'of', 'reading', 'that', 'this', 'is', 'possible', 'we', 'call', 't... | [-0.1449226163431636, 0.17507522676938347, -0.09525503018604857, -0.0018880058296157846, -0.14438421478095864, -0.13525918961968272, 0.07422367975814267, 0.3140164416416415, -0.3623011614827971, -0.17152207839701858, 0.07522281465519752, -0.26375044568142453, -0.19171189993254042, 0.13696919240589653, -0.16443112881055... |
709.4242 | Rational Expectations, psychology and inductive learning via moving
thresholds | This work suggests modifications to a previously introduced class of
heterogeneous agent models that allow for the inclusion of different types of
agent motivations and behaviours in a unified way. The agents operate within a
highly simplified environment where they are only able to be long or short one
unit of the a... | q-fin.TR physics.comp-ph | this work suggests modifications to a previously introduced class of heterogeneous agent models that allow for the inclusion of different types of agent motivations and behaviours in a unified way the agents operate within a highly simplified environment where they are only able to be long or short one unit of the asse... | [['this', 'work', 'suggests', 'modifications', 'to', 'a', 'previously', 'introduced', 'class', 'of', 'heterogeneous', 'agent', 'models', 'that', 'allow', 'for', 'the', 'inclusion', 'of', 'different', 'types', 'of', 'agent', 'motivations', 'and', 'behaviours', 'in', 'a', 'unified', 'way', 'the', 'agents', 'operate', 'wi... | [-0.10078412988919228, 0.11023307437403908, -0.09012256102329216, 0.08187697094519497, -0.10982511596743393, -0.16834732004412517, 0.10727623893477901, 0.37406352532009796, -0.3049157670190193, -0.300930178865848, 0.08187456795112855, -0.25217873655079887, -0.14015676535440358, 0.14987258050235508, -0.08401741576741074... |
709.4243 | Direct and inverse theorems in the theory of approximation by the Ritz
method | For an arbitrary self-adjoint operator $B$ in a Hilbert space $H$, we present
direct and inverse theorems establishing the relationship between the degree of
smoothness of a vector $x \in H$ with respect to the operator $B$, the rate of
convergence to zero of its best approximation by exponential-type entire
vectors ... | math.FA | for an arbitrary selfadjoint operator b in a hilbert space h we present direct and inverse theorems establishing the relationship between the degree of smoothness of a vector x in h with respect to the operator b the rate of convergence to zero of its best approximation by exponentialtype entire vectors of the operator... | [['for', 'an', 'arbitrary', 'selfadjoint', 'operator', 'b', 'in', 'a', 'hilbert', 'space', 'h', 'we', 'present', 'direct', 'and', 'inverse', 'theorems', 'establishing', 'the', 'relationship', 'between', 'the', 'degree', 'of', 'smoothness', 'of', 'a', 'vector', 'x', 'in', 'h', 'with', 'respect', 'to', 'the', 'operator',... | [-0.12678735419739406, 0.07134296328669214, -0.058550787872153814, 0.042432765156583306, -0.06403709212215719, -0.10177748327995496, 0.07151860836637462, 0.3344096869312145, -0.3209101056045556, -0.2017874150897714, 0.10951170256325546, -0.2805235220508261, -0.07215674575111204, 0.1477972959874423, -0.02598039995223939... |
709.4244 | Superconducting d-wave stripes in cuprates: Valence bond order
coexisting with nodal quasiparticles | We point out that unidirectional bond-centered charge-density-wave states in
cuprates involve electronic order in both s- and d-wave channels, with
non-local Coulomb repulsion suppressing the s-wave component. The resulting
bond-charge-density wave, coexisting with superconductivity, is compatible with
recent photoem... | cond-mat.supr-con cond-mat.str-el | we point out that unidirectional bondcentered chargedensitywave states in cuprates involve electronic order in both s and dwave channels with nonlocal coulomb repulsion suppressing the swave component the resulting bondchargedensity wave coexisting with superconductivity is compatible with recent photoemission and tunn... | [['we', 'point', 'out', 'that', 'unidirectional', 'bondcentered', 'chargedensitywave', 'states', 'in', 'cuprates', 'involve', 'electronic', 'order', 'in', 'both', 's', 'and', 'dwave', 'channels', 'with', 'nonlocal', 'coulomb', 'repulsion', 'suppressing', 'the', 'swave', 'component', 'the', 'resulting', 'bondchargedensi... | [-0.20189812658138054, 0.24673231112564978, -0.03409732682738713, 0.02827257818818569, -0.05192199278557974, -0.16066158222857602, 0.08739602848817053, 0.3534835627692383, -0.216803612753845, -0.2729545089437865, -0.0059605193754853035, -0.43170094996864017, -0.12559124948944203, 0.1049381834915081, 0.06812677340755283... |
709.4245 | Minimal conductivity in graphene: interaction corrections and
ultraviolet anomaly | Conductivity of a disorder-free intrinsic graphene is studied to the first
order in the long-range Coulomb interaction and is found to be
\sigma=\sigma_0(1+0.01 g), where 'g' is the dimensionless ("fine structure")
coupling constant. The calculations are performed using three different
methods: i) electron polarizati... | cond-mat.mes-hall | conductivity of a disorderfree intrinsic graphene is studied to the first order in the longrange coulomb interaction and is found to be sigmasigma_01001 g where g is the dimensionless fine structure coupling constant the calculations are performed using three different methods i electron polarization function ii kubo f... | [['conductivity', 'of', 'a', 'disorderfree', 'intrinsic', 'graphene', 'is', 'studied', 'to', 'the', 'first', 'order', 'in', 'the', 'longrange', 'coulomb', 'interaction', 'and', 'is', 'found', 'to', 'be', 'sigmasigma_01001', 'g', 'where', 'g', 'is', 'the', 'dimensionless', 'fine', 'structure', 'coupling', 'constant', 't... | [-0.15782597914424745, 0.16905196314829207, -0.08233055415519969, 0.06670634724811629, -0.07201076904853243, -0.1899899436420826, -0.0001496082228651747, 0.4014717163734658, -0.2538923580675971, -0.3156214648597809, -0.011045779726944517, -0.2843150063742732, -0.10784143791534007, 0.1530088878123003, 0.0592780877337899... |
709.4246 | Spin-orbital effects in magnetized quantum wires and spin chains | We present analysis of the interacting quantum wire problem in the presence
of magnetic field and spin-orbital interaction. We show that an interesting
interplay of Zeeman and spin-orbit terms, facilitated by the electron-electron
interaction, results in the spin-density wave (SDW) state when the magnetic
field and s... | cond-mat.mes-hall cond-mat.str-el | we present analysis of the interacting quantum wire problem in the presence of magnetic field and spinorbital interaction we show that an interesting interplay of zeeman and spinorbit terms facilitated by the electronelectron interaction results in the spindensity wave sdw state when the magnetic field and spinorbit ax... | [['we', 'present', 'analysis', 'of', 'the', 'interacting', 'quantum', 'wire', 'problem', 'in', 'the', 'presence', 'of', 'magnetic', 'field', 'and', 'spinorbital', 'interaction', 'we', 'show', 'that', 'an', 'interesting', 'interplay', 'of', 'zeeman', 'and', 'spinorbit', 'terms', 'facilitated', 'by', 'the', 'electronelec... | [-0.2678043364905394, 0.2158383184946545, -0.016398530620790552, 0.06155820814534449, -0.10508503506246668, -0.1088914739057565, -0.03149173728620203, 0.42409284627781463, -0.2955989249731199, -0.26444690443503743, -0.023102152432637434, -0.2624983382626222, -0.08750377226835833, 0.15746875867032661, 0.1315179171613776... |
709.4247 | Modeling the Infrared Bow Shock at delta Velorum: Implications for
Studies of Debris Disks and lambda Bootis Stars | We have discovered a bow shock shaped mid-infrared excess region in front of
delta Velorum using 24 micron observations obtained with the Multiband Imaging
Photometer for Spitzer (MIPS). The excess has been classified as a debris disk
from previous infrared observations. Although the bow shock morphology was only
det... | astro-ph | we have discovered a bow shock shaped midinfrared excess region in front of delta velorum using 24 micron observations obtained with the multiband imaging photometer for spitzer mips the excess has been classified as a debris disk from previous infrared observations although the bow shock morphology was only detected i... | [['we', 'have', 'discovered', 'a', 'bow', 'shock', 'shaped', 'midinfrared', 'excess', 'region', 'in', 'front', 'of', 'delta', 'velorum', 'using', '24', 'micron', 'observations', 'obtained', 'with', 'the', 'multiband', 'imaging', 'photometer', 'for', 'spitzer', 'mips', 'the', 'excess', 'has', 'been', 'classified', 'as',... | [-0.06427760817039241, 0.10556166530511582, -0.08183854787819908, 0.0815931923334313, -0.10259413664757261, -0.06277059015047037, 0.01641794514416775, 0.4311788843846635, -0.22000295451160468, -0.362291653275169, 0.042702289075372324, -0.28963630133125773, -0.045832717958303015, 0.15833894238538782, -0.0452388738916739... |
709.4248 | The SINFONI MgII Program for Line Emitters (SIMPLE): Discovering
starbursts near QSO sight-lines | Low-ionization transitions such as the MgII 2796/2803 doublet trace cold gas
in the vicinity of galaxies. It is not clear whether this gas is part of the
interstellar medium of large proto-disks, part of dwarfs, or part of entrained
material in supernovae-driven outflows. Studies based on MgII statistics, e.g.
stacke... | astro-ph | lowionization transitions such as the mgii 27962803 doublet trace cold gas in the vicinity of galaxies it is not clear whether this gas is part of the interstellar medium of large protodisks part of dwarfs or part of entrained material in supernovaedriven outflows studies based on mgii statistics eg stacked images and ... | [['lowionization', 'transitions', 'such', 'as', 'the', 'mgii', '27962803', 'doublet', 'trace', 'cold', 'gas', 'in', 'the', 'vicinity', 'of', 'galaxies', 'it', 'is', 'not', 'clear', 'whether', 'this', 'gas', 'is', 'part', 'of', 'the', 'interstellar', 'medium', 'of', 'large', 'protodisks', 'part', 'of', 'dwarfs', 'or', '... | [-0.04332781653785536, 0.07293030697499113, 0.010296998027679992, 0.11587290681501176, -0.05451381869076205, -0.09067698408335705, 0.028408242226979727, 0.48722553420972464, -0.09543192103906065, -0.3295964477061904, 0.020438718442917513, -0.31587949003582694, 0.02449473080823423, 0.16695997308664998, 0.020736185657432... |
709.4249 | HI Imaging Observations of Superthin Galaxies. II. IC2233 and the Blue
Compact Dwarf NGC2537 | We have used the VLA to image the HI 21-cm line emission in the edge-on Sd
galaxy IC2233 and the blue compact dwarf NGC2537. We also present new optical
B,R, and H alpha imaging of IC2233 obtained with the WIYN telescope. Despite
evidence of localized massive star formation, IC2233 has a low surface
brightness disk w... | astro-ph | we have used the vla to image the hi 21cm line emission in the edgeon sd galaxy ic2233 and the blue compact dwarf ngc2537 we also present new optical br and h alpha imaging of ic2233 obtained with the wiyn telescope despite evidence of localized massive star formation ic2233 has a low surface brightness disk with a low... | [['we', 'have', 'used', 'the', 'vla', 'to', 'image', 'the', 'hi', '21cm', 'line', 'emission', 'in', 'the', 'edgeon', 'sd', 'galaxy', 'ic2233', 'and', 'the', 'blue', 'compact', 'dwarf', 'ngc2537', 'we', 'also', 'present', 'new', 'optical', 'br', 'and', 'h', 'alpha', 'imaging', 'of', 'ic2233', 'obtained', 'with', 'the', ... | [-0.10043156690152133, 0.06859952755851402, -0.06720894099327555, 0.07727057335881941, -0.09538283308461439, -0.06371946530661693, -0.007082367730081866, 0.46293761783785986, -0.1739018995433294, -0.29241612512749016, 0.07603489930267658, -0.26697734787798766, -0.051908025298300284, 0.17469766872052692, -0.015011571897... |
709.425 | The origin of star formation since z=1 | The use of multiple integral field units with FLAMES/GIRAFFE at VLT has
revolutionized investigations of distant galaxy kinematics. This facility may
recover the velocity fields of almost all emission line galaxies with
I_(AB)<22.5 at z<0.8. We have gathered a unique sample of 63 velocity fields at
z=0.4-0.75, which ... | astro-ph | the use of multiple integral field units with flamesgiraffe at vlt has revolutionized investigations of distant galaxy kinematics this facility may recover the velocity fields of almost all emission line galaxies with i_ab225 at z08 we have gathered a unique sample of 63 velocity fields at z04075 which are representati... | [['the', 'use', 'of', 'multiple', 'integral', 'field', 'units', 'with', 'flamesgiraffe', 'at', 'vlt', 'has', 'revolutionized', 'investigations', 'of', 'distant', 'galaxy', 'kinematics', 'this', 'facility', 'may', 'recover', 'the', 'velocity', 'fields', 'of', 'almost', 'all', 'emission', 'line', 'galaxies', 'with', 'i_a... | [-0.08935389815476434, 0.10625289815542256, -0.052993056805531395, 0.04469787946516841, -0.09132960539487801, -0.043268799513642646, -0.0009683768562009108, 0.4714512684992675, -0.14177958393822712, -0.35894386352136215, 0.03665685063139696, -0.25822435801142246, 0.0076503595883219404, 0.21633697828149487, 0.0351059788... |
709.4251 | Bulk viscosity in 2SC and CFL quark matter | The bulk viscosities of two color-superconducting phases, the color-flavor
locked (CFL) phase and the 2SC phase, are computed and compared to the result
for unpaired quark matter. In the case of the CFL phase, processes involving
kaons and the superfluid mode give the largest contribution to the bulk
viscosity since ... | nucl-th astro-ph hep-ph | the bulk viscosities of two colorsuperconducting phases the colorflavor locked cfl phase and the 2sc phase are computed and compared to the result for unpaired quark matter in the case of the cfl phase processes involving kaons and the superfluid mode give the largest contribution to the bulk viscosity since all fermio... | [['the', 'bulk', 'viscosities', 'of', 'two', 'colorsuperconducting', 'phases', 'the', 'colorflavor', 'locked', 'cfl', 'phase', 'and', 'the', '2sc', 'phase', 'are', 'computed', 'and', 'compared', 'to', 'the', 'result', 'for', 'unpaired', 'quark', 'matter', 'in', 'the', 'case', 'of', 'the', 'cfl', 'phase', 'processes', '... | [-0.15747794638394463, 0.35330945648781786, -0.07449079797015334, 0.06769290915490403, -0.058690381818038165, -0.08665788699443458, 0.084925287560038, 0.2796085116565756, -0.21378854231856076, -0.2821069537985621, 0.06326235056209134, -0.28822852996118525, 0.00691945703389744, 0.12080853109921705, 0.031471485100316665,... |
709.4252 | Global Models for the Evolution of Embedded, Accreting Protostellar
Disks | Most analytic work to date on protostellar disks has focused on those in
isolation from their environments. However, observations are now beginning to
probe the earliest, most embedded phases of star formation, during which disks
are rapidly accreting from their parent cores and cannot be modeled in
isolation. We pre... | astro-ph | most analytic work to date on protostellar disks has focused on those in isolation from their environments however observations are now beginning to probe the earliest most embedded phases of star formation during which disks are rapidly accreting from their parent cores and cannot be modeled in isolation we present a ... | [['most', 'analytic', 'work', 'to', 'date', 'on', 'protostellar', 'disks', 'has', 'focused', 'on', 'those', 'in', 'isolation', 'from', 'their', 'environments', 'however', 'observations', 'are', 'now', 'beginning', 'to', 'probe', 'the', 'earliest', 'most', 'embedded', 'phases', 'of', 'star', 'formation', 'during', 'whic... | [-0.08492454725126045, 0.15719953371702336, -0.050592738996888174, 0.07582180347888504, -0.09934852825941153, -0.032329263143591205, -0.004575931414199824, 0.4148103314937587, -0.19626801602016583, -0.33917020805153336, 0.07278844153588754, -0.21825617166881062, -0.030540089623147006, 0.19769838175727455, 0.01560436737... |
709.4253 | Finitistic dimension through infinite projective dimension | We show that an artin algebra having at most three radical layers of infinite
projective dimension has finite finitistic dimension, generalizing the known
result for algebras with vanishing radical cube.
| math.RT | we show that an artin algebra having at most three radical layers of infinite projective dimension has finite finitistic dimension generalizing the known result for algebras with vanishing radical cube | [['we', 'show', 'that', 'an', 'artin', 'algebra', 'having', 'at', 'most', 'three', 'radical', 'layers', 'of', 'infinite', 'projective', 'dimension', 'has', 'finite', 'finitistic', 'dimension', 'generalizing', 'the', 'known', 'result', 'for', 'algebras', 'with', 'vanishing', 'radical', 'cube']] | [-0.15063114054501056, 0.08348243850099, -0.030762345483526587, -0.0073352511351307235, -0.06066665211692453, -0.22306531152377526, -0.13443857450038194, 0.33316332126657167, -0.3593146458772632, -0.10298832685997089, 0.11366103985346854, -0.2898342336528003, -0.06653868649154901, 0.16832685996002208, -0.11950715314596... |
709.4254 | Measurement of the muon charge asymmetry from W boson decays | We present a measurement of the muon charge asymmetry from W boson decays
using 0.3 fb^{-1} of data collected at \sqrt{s}=1.96 GeV between 2002 and 2004
with the D0 detector at the Fermilab Tevatron ppbar Collider. We compare our
findings with expectations from next-to-leading-order calculations performed
using the C... | hep-ex | we present a measurement of the muon charge asymmetry from w boson decays using 03 fb1 of data collected at sqrts196 gev between 2002 and 2004 with the d0 detector at the fermilab tevatron ppbar collider we compare our findings with expectations from nexttoleadingorder calculations performed using the cteq61m and mrst0... | [['we', 'present', 'a', 'measurement', 'of', 'the', 'muon', 'charge', 'asymmetry', 'from', 'w', 'boson', 'decays', 'using', '03', 'fb1', 'of', 'data', 'collected', 'at', 'sqrts196', 'gev', 'between', '2002', 'and', '2004', 'with', 'the', 'd0', 'detector', 'at', 'the', 'fermilab', 'tevatron', 'ppbar', 'collider', 'we', ... | [0.05663051539315627, 0.17591958225059967, -0.18133013871713327, 0.14202320757680215, -0.04646672083494755, -0.08899159907148435, 0.025974563614895137, 0.3810409010029756, -0.14537563843724247, -0.3289421666485186, -0.06706038915480558, -0.475620081447638, 0.14403728917241096, 0.1433970690633242, 0.1197039850629293, 0.... |
709.4255 | Arithmetic duality theorems for 1-motives over function fields | In this paper we obtain a Poitou-Tate exact sequence for finite and flat
group schemes over a global function field. We also extend the duality theorems
for 1-motives over number fields obtained by D.Harari and T.Szamuely to the
function field case.
| math.NT math.AG | in this paper we obtain a poitoutate exact sequence for finite and flat group schemes over a global function field we also extend the duality theorems for 1motives over number fields obtained by dharari and tszamuely to the function field case | [['in', 'this', 'paper', 'we', 'obtain', 'a', 'poitoutate', 'exact', 'sequence', 'for', 'finite', 'and', 'flat', 'group', 'schemes', 'over', 'a', 'global', 'function', 'field', 'we', 'also', 'extend', 'the', 'duality', 'theorems', 'for', '1motives', 'over', 'number', 'fields', 'obtained', 'by', 'dharari', 'and', 'tszam... | [-0.15439382224128798, 0.04128734643260638, -0.12077464662396754, 0.09336032879311973, -0.04081306448922707, -0.05577955994372948, 0.07301210273558703, 0.3861787365988279, -0.2847254056101426, -0.24647366841478893, 0.09609423221077006, -0.15023212531247201, -0.1506620770177016, 0.24929227796980205, -0.0964953298561084,... |
709.4256 | Comment on ``Elastic Stabilization of a Single-Domain Ferroelectric
State in Nanoscale Capacitors and Tunnel Junctions" [N.A. Pertsev and H.
Kohlstedt, Phys. Rev. Lett. 98, 257603 (2007).] | In a recent Letter [N.A. Pertsev and H. Kohlstedt, Phys. Rev. Lett. 98,
257603 (2007)] the authors claim that "even nanoscale capacitors and tunnel
junctions may have out of plane polarization sufficient for memory
applications." Here we show in an elementary way that this conclusion is not
substantiated by their cal... | cond-mat.mtrl-sci cond-mat.stat-mech | in a recent letter na pertsev and h kohlstedt phys rev lett 98 257603 2007 the authors claim that even nanoscale capacitors and tunnel junctions may have out of plane polarization sufficient for memory applications here we show in an elementary way that this conclusion is not substantiated by their calculations and tha... | [['in', 'a', 'recent', 'letter', 'na', 'pertsev', 'and', 'h', 'kohlstedt', 'phys', 'rev', 'lett', '98', '257603', '2007', 'the', 'authors', 'claim', 'that', 'even', 'nanoscale', 'capacitors', 'and', 'tunnel', 'junctions', 'may', 'have', 'out', 'of', 'plane', 'polarization', 'sufficient', 'for', 'memory', 'applications'... | [-0.12425897720142177, 0.10754071237099724, -0.07266947338657995, -0.05587815203433556, -0.058922352870145155, -0.10803471019701852, 0.12485171512760702, 0.4566705682795615, -0.1310515784763641, -0.33978914370339725, -0.020611987081206134, -0.2625498544544943, -0.18731587386273238, 0.1998170298907245, -0.12669075601508... |
709.4257 | Thermodynamical Analogy Between BTZ Black Holes and Effective String
Theory | In this paper we study the first law of thermodynamics for the (2+1)
dimensional BTZ rotating black hole considering a pair of thermodinamical
systems constructed with the two horizons of this solution. We show that these
two systems are similar to the right and left movers of string theory and that
the temperature a... | gr-qc | in this paper we study the first law of thermodynamics for the 21 dimensional btz rotating black hole considering a pair of thermodinamical systems constructed with the two horizons of this solution we show that these two systems are similar to the right and left movers of string theory and that the temperature associa... | [['in', 'this', 'paper', 'we', 'study', 'the', 'first', 'law', 'of', 'thermodynamics', 'for', 'the', '21', 'dimensional', 'btz', 'rotating', 'black', 'hole', 'considering', 'a', 'pair', 'of', 'thermodinamical', 'systems', 'constructed', 'with', 'the', 'two', 'horizons', 'of', 'this', 'solution', 'we', 'show', 'that', '... | [-0.15917713822397803, 0.11055605635046958, -0.04522370621562004, 0.06853391327728917, 0.019228493951128, -0.13709573415108026, -0.010889626340940595, 0.3279233289084264, -0.2276203383824655, -0.253927685400205, 0.12568391773550372, -0.3620089212964688, -0.12495984150362867, 0.19704131967654184, -0.04098490291674222, 0... |
709.4258 | Fractional statistics of topological defects in graphene and related
structures | We show that fractional charges bound to topological defects in the recently
proposed time-reversal-invariant models on honeycomb and square lattices obey
fractional statistics. The effective low-energy description is given in terms
of a `doubled' level-2 Chern-Simons field theory, which is parity and
time-reversal i... | cond-mat.str-el cond-mat.mes-hall | we show that fractional charges bound to topological defects in the recently proposed timereversalinvariant models on honeycomb and square lattices obey fractional statistics the effective lowenergy description is given in terms of a doubled level2 chernsimons field theory which is parity and timereversal invariant and... | [['we', 'show', 'that', 'fractional', 'charges', 'bound', 'to', 'topological', 'defects', 'in', 'the', 'recently', 'proposed', 'timereversalinvariant', 'models', 'on', 'honeycomb', 'and', 'square', 'lattices', 'obey', 'fractional', 'statistics', 'the', 'effective', 'lowenergy', 'description', 'is', 'given', 'in', 'term... | [-0.19257859269024005, 0.28480610584041904, -0.038922733989810304, 0.0800353603570589, -0.056324047981096165, -0.1885019639639982, 0.032860341150912326, 0.3002182638272643, -0.1857732691336423, -0.33053840468637646, -0.003293171082623303, -0.2878569237355675, -0.1887517187943948, 0.09335374385118485, -0.038948528498544... |
709.4259 | Unravelling Strings at the LHC | We construct LHC signature footprints for four semi-realistic string/$M$
theory vacua with an MSSM visible sector. We find that they all give rise to
limited regions in LHC signature space, and are qualitatively different from
each other for understandable reasons. We also propose a technique in which
correlations of... | hep-ph hep-ex hep-th | we construct lhc signature footprints for four semirealistic stringm theory vacua with an mssm visible sector we find that they all give rise to limited regions in lhc signature space and are qualitatively different from each other for understandable reasons we also propose a technique in which correlations of lhc sign... | [['we', 'construct', 'lhc', 'signature', 'footprints', 'for', 'four', 'semirealistic', 'stringm', 'theory', 'vacua', 'with', 'an', 'mssm', 'visible', 'sector', 'we', 'find', 'that', 'they', 'all', 'give', 'rise', 'to', 'limited', 'regions', 'in', 'lhc', 'signature', 'space', 'and', 'are', 'qualitatively', 'different', ... | [-0.031212807090064004, 0.15692750578018605, -0.1464375029233369, 0.2016967998468317, -0.1216707360232249, -0.212144081806764, 0.028381001662505283, 0.38709563907574523, -0.20326597092842513, -0.3206708779558539, 0.06678886989512565, -0.26109376225027847, -0.11965994009621103, 0.19383180200556208, -0.05743594845248894,... |
709.426 | Geometric resonance cooling of polarizable particles in an optical
waveguide | In the radiation field of an optical waveguide, the Rayleigh scattering of
photons is shown to result in a strongly velocity-dependent force on atoms. The
pump field, which is injected in the fundamental branch of the waveguide, is
favorably scattered by a moving atom into one of the transversely excited
branches of ... | quant-ph | in the radiation field of an optical waveguide the rayleigh scattering of photons is shown to result in a strongly velocitydependent force on atoms the pump field which is injected in the fundamental branch of the waveguide is favorably scattered by a moving atom into one of the transversely excited branches of propaga... | [['in', 'the', 'radiation', 'field', 'of', 'an', 'optical', 'waveguide', 'the', 'rayleigh', 'scattering', 'of', 'photons', 'is', 'shown', 'to', 'result', 'in', 'a', 'strongly', 'velocitydependent', 'force', 'on', 'atoms', 'the', 'pump', 'field', 'which', 'is', 'injected', 'in', 'the', 'fundamental', 'branch', 'of', 'th... | [-0.14810437998213968, 0.27159113127563617, -0.07503356216749286, -0.014748982472947854, -0.038957611071493696, -0.15577516229275395, -0.010493653352879098, 0.4071680546683424, -0.25522122252937957, -0.2241843730868662, -0.03424830057740431, -0.3118910132962115, -0.04475702859242173, 0.25559769639444047, 0.029163530205... |
709.4261 | Overview of the New Horizons Science Payload | The New Horizons mission was launched on 2006 January 19, and the spacecraft
is heading for a flyby encounter with the Pluto system in the summer of 2015.
The challenges associated with sending a spacecraft to Pluto in less than 10
years and performing an ambitious suite of scientific investigations at such
large hel... | astro-ph | the new horizons mission was launched on 2006 january 19 and the spacecraft is heading for a flyby encounter with the pluto system in the summer of 2015 the challenges associated with sending a spacecraft to pluto in less than 10 years and performing an ambitious suite of scientific investigations at such large helioce... | [['the', 'new', 'horizons', 'mission', 'was', 'launched', 'on', '2006', 'january', '19', 'and', 'the', 'spacecraft', 'is', 'heading', 'for', 'a', 'flyby', 'encounter', 'with', 'the', 'pluto', 'system', 'in', 'the', 'summer', 'of', '2015', 'the', 'challenges', 'associated', 'with', 'sending', 'a', 'spacecraft', 'to', 'p... | [-0.09492052925354354, 0.16759882307549281, -0.10527043944994847, 0.03038394557650183, -0.09324148405329861, -0.1341119419129637, -0.04595605210600367, 0.3766452409819557, -0.19552786589002397, -0.4248031477708047, 0.13142498848733689, -0.3337192263727327, -0.0589545773064646, 0.23755760530548287, -0.09926534134473723,... |
709.4262 | Nonperturbative Instability of AdS_5 x S^5/Z_k | We study the AdS/CFT correspondence with boundary conditions AdS_5 x S^5/Z_k,
where the Z_k acts freely but breaks all supersymmetry. While there are closed
string tachyons at small 't Hooft coupling, there are no tachyons at large
coupling. Nevertheless, we show that there is a nonperturbative instability
directly a... | hep-th | we study the adscft correspondence with boundary conditions ads_5 x s5z_k where the z_k acts freely but breaks all supersymmetry while there are closed string tachyons at small t hooft coupling there are no tachyons at large coupling nevertheless we show that there is a nonperturbative instability directly analogous to... | [['we', 'study', 'the', 'adscft', 'correspondence', 'with', 'boundary', 'conditions', 'ads_5', 'x', 's5z_k', 'where', 'the', 'z_k', 'acts', 'freely', 'but', 'breaks', 'all', 'supersymmetry', 'while', 'there', 'are', 'closed', 'string', 'tachyons', 'at', 'small', 't', 'hooft', 'coupling', 'there', 'are', 'no', 'tachyons... | [-0.20614165398001205, 0.24791946194600314, -0.04319715083693154, 0.10680383791186614, -0.07613788180460687, -0.19116291087702847, -0.006406674624304287, 0.3304936060332693, -0.20595676330849527, -0.19745395585196093, 0.07758111690345686, -0.27200985301751646, -0.1092580744472798, 0.11327951063867658, -0.00086822112789... |
709.4263 | On Cobweb posets tiling problem | Kwasniewski's cobweb posets uniquely represented by directed acyclic graphs
are such a generalization of the Fibonacci tree that allows joint combinatorial
interpretation for all of them under admissibility condition. This
interpretation was derived in the source papers and it entailes natural
enquieres already formu... | math.CO cs.DM | kwasniewskis cobweb posets uniquely represented by directed acyclic graphs are such a generalization of the fibonacci tree that allows joint combinatorial interpretation for all of them under admissibility condition this interpretation was derived in the source papers and it entailes natural enquieres already formulate... | [['kwasniewskis', 'cobweb', 'posets', 'uniquely', 'represented', 'by', 'directed', 'acyclic', 'graphs', 'are', 'such', 'a', 'generalization', 'of', 'the', 'fibonacci', 'tree', 'that', 'allows', 'joint', 'combinatorial', 'interpretation', 'for', 'all', 'of', 'them', 'under', 'admissibility', 'condition', 'this', 'interp... | [-0.11540669434162486, 0.0852034064669005, -0.03486536735534129, 0.1289772597486602, -0.14693946035646172, -0.10321147103109453, 0.056473309791321494, 0.37425484483590327, -0.33071566220507564, -0.30848018708358327, 0.13589176363087294, -0.24638169052669112, -0.21338243127228265, 0.17206639548516775, -0.152793088366827... |
709.4264 | Quantum trajectory approach to circuit QED: Quantum jumps and the Zeno
effect | We present a theoretical study of a superconducting charge qubit dispersively
coupled to a transmission line resonator. Starting from a master equation
description of this coupled system and using a polaron transformation, we
obtain an exact effective master equation for the qubit. We then use quantum
trajectory theo... | cond-mat.mes-hall cond-mat.supr-con quant-ph | we present a theoretical study of a superconducting charge qubit dispersively coupled to a transmission line resonator starting from a master equation description of this coupled system and using a polaron transformation we obtain an exact effective master equation for the qubit we then use quantum trajectory theory to... | [['we', 'present', 'a', 'theoretical', 'study', 'of', 'a', 'superconducting', 'charge', 'qubit', 'dispersively', 'coupled', 'to', 'a', 'transmission', 'line', 'resonator', 'starting', 'from', 'a', 'master', 'equation', 'description', 'of', 'this', 'coupled', 'system', 'and', 'using', 'a', 'polaron', 'transformation', '... | [-0.16208884170606594, 0.14763051703048405, -0.08909283288995977, -0.005530987155658228, 0.010907790589111822, -0.21126292990520595, 0.08959745517673177, 0.34468509938429903, -0.23524026453012117, -0.23722263808465666, 0.012985577284254961, -0.2844357957304628, -0.11577148032547147, 0.22758291603617922, -0.006705280800... |
709.4265 | Multi-symmetry and Multi-band Superconductivity in Filled-skutterudites
PrOs$_4$Sb$_{12}$ and PrRu$_4$Sb$_{12}$ | Thermal conductivity measurements were performed on single crystal samples of
the superconducting filled skutterudite compounds PrOs$_4$Sb$_{12}$ and
PrRu$_4$Sb$_{12}$ both as a function of temperature and magnetic field applied
perpendicular to the heat current. In zero magnetic field, the low temperature
electronic... | cond-mat.supr-con cond-mat.str-el | thermal conductivity measurements were performed on single crystal samples of the superconducting filled skutterudite compounds pros_4sb_12 and prru_4sb_12 both as a function of temperature and magnetic field applied perpendicular to the heat current in zero magnetic field the low temperature electronic thermal conduct... | [['thermal', 'conductivity', 'measurements', 'were', 'performed', 'on', 'single', 'crystal', 'samples', 'of', 'the', 'superconducting', 'filled', 'skutterudite', 'compounds', 'pros_4sb_12', 'and', 'prru_4sb_12', 'both', 'as', 'a', 'function', 'of', 'temperature', 'and', 'magnetic', 'field', 'applied', 'perpendicular', ... | [-0.1974628740250804, 0.23941407053832328, -0.017318788188073288, 0.017809065434124347, -0.05205947242455779, -0.11608758180278476, 0.11668218912921481, 0.3527018899021514, -0.23409037170683397, -0.2769648812913134, 0.008415595362112708, -0.3357338309874172, -0.046956481692101155, 0.1936930759152124, 0.0306151225133896... |
709.4266 | Ontological models and the interpretation of contextuality | Studying the extent to which realism is compatible with quantum mechanics
teaches us something about the quantum mechanical universe, regardless of the
validity of such realistic assumptions. It has also recently been appreciated
that these kinds of studies are fruitful for questions relating to quantum
information a... | quant-ph | studying the extent to which realism is compatible with quantum mechanics teaches us something about the quantum mechanical universe regardless of the validity of such realistic assumptions it has also recently been appreciated that these kinds of studies are fruitful for questions relating to quantum information and c... | [['studying', 'the', 'extent', 'to', 'which', 'realism', 'is', 'compatible', 'with', 'quantum', 'mechanics', 'teaches', 'us', 'something', 'about', 'the', 'quantum', 'mechanical', 'universe', 'regardless', 'of', 'the', 'validity', 'of', 'such', 'realistic', 'assumptions', 'it', 'has', 'also', 'recently', 'been', 'appre... | [-0.08130591903275228, 0.12272133029408362, -0.1510344660940865, 0.10042771789007161, -0.07341445130444893, -0.1691729290746833, 0.04922812641890652, 0.31556420597634766, -0.24824823576055433, -0.3295416219168466, 0.04931864928141594, -0.24536560254696954, -0.14827589810821631, 0.18858935675673086, -0.0753793305807511,... |
709.4267 | Doping Dependence of Vortex Regimes in
Y$_{1-x}$Pr$_{x}$Ba$_{2}$Cu$_{3}$O$_{7-\delta}$ Single Crystals | Magnetic relaxation measurements on a series of
Y$_{1-x}$Pr$_{x}$Ba$_{2}$Cu$_{3}$O$_{7-\delta}$ ($x = 0.13, 0.34, 0.47$) single
crystals were performed over a large field and temperature range in order to
investigate the characteristics of the vortex matter across the second
magnetization peak (SMP). The magnitude of... | cond-mat.supr-con cond-mat.str-el | magnetic relaxation measurements on a series of y_1xpr_xba_2cu_3o_7delta x 013 034 047 single crystals were performed over a large field and temperature range in order to investigate the characteristics of the vortex matter across the second magnetization peak smp the magnitude of the smp varies nonmonotonically with t... | [['magnetic', 'relaxation', 'measurements', 'on', 'a', 'series', 'of', 'y_1xpr_xba_2cu_3o_7delta', 'x', '013', '034', '047', 'single', 'crystals', 'were', 'performed', 'over', 'a', 'large', 'field', 'and', 'temperature', 'range', 'in', 'order', 'to', 'investigate', 'the', 'characteristics', 'of', 'the', 'vortex', 'matt... | [-0.17934306008610756, 0.21300920119151698, -0.059488896366540985, -0.01380131809726049, -0.02878908547209457, -0.1187553593805831, 0.07501213741933654, 0.3308775240294398, -0.28555640118577735, -0.30352525098640826, 0.018532997055815615, -0.3038711919372154, -0.029626876771283946, 0.1788151313819193, 0.054909562617803... |
709.4268 | Coherence lifetimes of excitations in an atomic condensate due to the
thin spectrum | We study the quantum coherence properties of a finite sized atomic condensate
using a toy-model and the thin spectrum model formalism. The decoherence time
for a condensate in the ground state, nominally taken as a variational symmetry
breaking state, is investigated for both zero and finite temperatures. We also
con... | quant-ph cond-mat.soft | we study the quantum coherence properties of a finite sized atomic condensate using a toymodel and the thin spectrum model formalism the decoherence time for a condensate in the ground state nominally taken as a variational symmetry breaking state is investigated for both zero and finite temperatures we also consider t... | [['we', 'study', 'the', 'quantum', 'coherence', 'properties', 'of', 'a', 'finite', 'sized', 'atomic', 'condensate', 'using', 'a', 'toymodel', 'and', 'the', 'thin', 'spectrum', 'model', 'formalism', 'the', 'decoherence', 'time', 'for', 'a', 'condensate', 'in', 'the', 'ground', 'state', 'nominally', 'taken', 'as', 'a', '... | [-0.15797342347152726, 0.26128763260417864, -0.08988709644855637, 0.09698534503603648, 0.0056848802064594466, -0.10234258939070921, 0.06092553182112935, 0.38388516171590276, -0.256549851586552, -0.2463533011608218, 0.08038891443468042, -0.2583688304220375, 0.004621665924787521, 0.1089573558983638, 0.08324650801522167, ... |
709.4269 | Electroweak Model Without A Higgs Particle | An electroweak model is formulated in a finite, four-dimensional quantum
field theory without a Higgs particle. The W and Z masses are induced from the
electroweak symmetry breaking of one-loop vacuum polarization graphs. The
theory contains only the observed particle spectrum of the standard model. In
terms of the o... | hep-ph | an electroweak model is formulated in a finite fourdimensional quantum field theory without a higgs particle the w and z masses are induced from the electroweak symmetry breaking of oneloop vacuum polarization graphs the theory contains only the observed particle spectrum of the standard model in terms of the observed ... | [['an', 'electroweak', 'model', 'is', 'formulated', 'in', 'a', 'finite', 'fourdimensional', 'quantum', 'field', 'theory', 'without', 'a', 'higgs', 'particle', 'the', 'w', 'and', 'z', 'masses', 'are', 'induced', 'from', 'the', 'electroweak', 'symmetry', 'breaking', 'of', 'oneloop', 'vacuum', 'polarization', 'graphs', 't... | [-0.11209211465732018, 0.26654094171246323, -0.058955752197117815, 0.14404366150546563, -0.04550498984111794, -0.14154063444450798, 0.014627832979908556, 0.28857024036476325, -0.21935668685901696, -0.3085690260297437, 0.003044907432504469, -0.30922343641862104, 0.009542014692032218, 0.12491361228026578, 0.0862576478621... |
709.427 | New Horizons: Anticipated Scientific Investigations at the Pluto System | The New Horizons spacecraft will achieve a wide range of measurement
objectives at the Pluto system, including color and panchromatic maps,
1.25-2.50 micron spectral images for studying surface compositions, and
measurements of Pluto's atmosphere (temperatures, composition, hazes, and the
escape rate). Additional mea... | astro-ph | the new horizons spacecraft will achieve a wide range of measurement objectives at the pluto system including color and panchromatic maps 125250 micron spectral images for studying surface compositions and measurements of plutos atmosphere temperatures composition hazes and the escape rate additional measurement object... | [['the', 'new', 'horizons', 'spacecraft', 'will', 'achieve', 'a', 'wide', 'range', 'of', 'measurement', 'objectives', 'at', 'the', 'pluto', 'system', 'including', 'color', 'and', 'panchromatic', 'maps', '125250', 'micron', 'spectral', 'images', 'for', 'studying', 'surface', 'compositions', 'and', 'measurements', 'of', ... | [-0.07039669811288894, 0.17153667641203788, -0.06838473908098067, 0.05879509047010524, -0.022240296963833818, -0.054702287918682826, 0.005031678320492728, 0.3193620734264032, -0.2350794710534609, -0.41014473610899627, 0.12369120385797726, -0.31373908953993757, -0.08318457409928916, 0.2017640736937986, -0.08413220647627... |
709.4271 | A New 3D Potential-Density Basis Set | A set of bi-orthogonal potential-density basis functions is introduced to
model the density and its associated gravitational field of three dimensional
stellar systems. Radial components of our basis functions are weighted integral
forms of spherical Bessel functions. We discuss the properties of our basis
functions ... | astro-ph | a set of biorthogonal potentialdensity basis functions is introduced to model the density and its associated gravitational field of three dimensional stellar systems radial components of our basis functions are weighted integral forms of spherical bessel functions we discuss the properties of our basis functions and de... | [['a', 'set', 'of', 'biorthogonal', 'potentialdensity', 'basis', 'functions', 'is', 'introduced', 'to', 'model', 'the', 'density', 'and', 'its', 'associated', 'gravitational', 'field', 'of', 'three', 'dimensional', 'stellar', 'systems', 'radial', 'components', 'of', 'our', 'basis', 'functions', 'are', 'weighted', 'inte... | [-0.14980627696283838, 0.07420553156090054, -0.12156828648664735, 0.08993692507501691, -0.05284878465939652, 0.037071056562391194, -0.0632691807367585, 0.3878224935721267, -0.25989365540444853, -0.192762951688333, 0.05333550311625004, -0.24126079311086374, -0.18116799374534326, 0.2340486525092274, 0.029329965287946503,... |
709.4272 | Radio Detection of Supernova 2004ip in the Circumnuclear Region of the
Luminous Infrared Galaxy IRAS 18293-3413 | We report a radio detection of supernova SN 2004ip in the circumnuclear
region of the luminous infrared galaxy IRAS 18293-3413, using Very Large Array
(VLA) observations at 8.4 GHz on 11 June 2007. SN 2004ip had been previously
discovered at near-infrared wavelengths using adaptive optics observations, but
its nature... | astro-ph | we report a radio detection of supernova sn 2004ip in the circumnuclear region of the luminous infrared galaxy iras 182933413 using very large array vla observations at 84 ghz on 11 june 2007 sn 2004ip had been previously discovered at nearinfrared wavelengths using adaptive optics observations but its nature corecolla... | [['we', 'report', 'a', 'radio', 'detection', 'of', 'supernova', 'sn', '2004ip', 'in', 'the', 'circumnuclear', 'region', 'of', 'the', 'luminous', 'infrared', 'galaxy', 'iras', '182933413', 'using', 'very', 'large', 'array', 'vla', 'observations', 'at', '84', 'ghz', 'on', '11', 'june', '2007', 'sn', '2004ip', 'had', 'bee... | [-0.031244968464263452, 0.027096687213790986, -0.055400396990004236, 0.08353492018730452, -0.15941711719019594, -0.11745125961261327, 0.0657298490628154, 0.4641583879550774, -0.09731588597983835, -0.30913263271300645, 0.11230772112574272, -0.30932796245697375, -0.0076668967122022445, 0.1863847181636798, -0.016657943861... |
709.4273 | Set Matrices and The Path/Cycle Problem | Presentation of set matrices and demonstration of their efficiency as a tool
using the path/cycle problem.
| cs.DM cs.CC cs.DS math.CO | presentation of set matrices and demonstration of their efficiency as a tool using the pathcycle problem | [['presentation', 'of', 'set', 'matrices', 'and', 'demonstration', 'of', 'their', 'efficiency', 'as', 'a', 'tool', 'using', 'the', 'pathcycle', 'problem']] | [-0.06623294157907367, -0.02567431819625199, -0.0755964527343167, 0.01868524303426966, -0.05862097511999309, -0.046173900802386925, 0.10873935744166374, 0.3455542139708996, -0.291015304508619, -0.4108572538534645, 0.17221918571158312, -0.24932458289549686, -0.168748413445428, 0.28776242723688483, -0.02130997838685289, ... |
709.4274 | Extreme gravitational lensing in vicinity of Schwarzschild-de Sitter
black holes | We have developed a realistic, fully general relativistic computer code to
simulate optical projection in a strong, spherically symmetric gravitational
field. The standard theoretical analysis of optical projection for an observer
in the vicinity of a Schwarzschild black hole is extended to black hole
spacetimes with... | astro-ph | we have developed a realistic fully general relativistic computer code to simulate optical projection in a strong spherically symmetric gravitational field the standard theoretical analysis of optical projection for an observer in the vicinity of a schwarzschild black hole is extended to black hole spacetimes with a re... | [['we', 'have', 'developed', 'a', 'realistic', 'fully', 'general', 'relativistic', 'computer', 'code', 'to', 'simulate', 'optical', 'projection', 'in', 'a', 'strong', 'spherically', 'symmetric', 'gravitational', 'field', 'the', 'standard', 'theoretical', 'analysis', 'of', 'optical', 'projection', 'for', 'an', 'observer... | [-0.13864113595199717, 0.05585500233053822, -0.08570738208329524, 0.10948123811634586, -0.09690544869312469, -0.15955531023620792, -0.053634603819398975, 0.3826985074179795, -0.20639791351962178, -0.27771546199972574, 0.09608186535479035, -0.2768987631767659, -0.02606115584871184, 0.21194377497030312, -0.00530795942776... |
709.4275 | Ullemar's formula for the moment map, II | We establish the complex analogue of Ullemar's formula for polynomial
domains. We show that the Jacobian of the complex moment mapping is equal to
the self-resultant of the defining polynomial.
| math.CV math.AC | we establish the complex analogue of ullemars formula for polynomial domains we show that the jacobian of the complex moment mapping is equal to the selfresultant of the defining polynomial | [['we', 'establish', 'the', 'complex', 'analogue', 'of', 'ullemars', 'formula', 'for', 'polynomial', 'domains', 'we', 'show', 'that', 'the', 'jacobian', 'of', 'the', 'complex', 'moment', 'mapping', 'is', 'equal', 'to', 'the', 'selfresultant', 'of', 'the', 'defining', 'polynomial']] | [-0.17490056463118112, 0.00997152372396418, -0.06815602224586266, 0.084456301913763, -0.09903204381199819, -0.06520983962608236, -0.04539550154627899, 0.2957040016938533, -0.35532644178186146, -0.19539104930923454, 0.10193508993169027, -0.2007951493807403, -0.2204805251343974, 0.22073478065431118, -0.03774881080192115,... |
709.4276 | The Integrability of Pauli System in Lorentz Violating Background | We systematically analyze the integrability of a Pauli system in Lorentz
violating background at the non-relativistic level both in two- and
three-dimensions. We consider the non-relativistic limit of the Dirac equation
from the QED sector of the so-called Standard Model Extension by keeping only
two types of backgro... | hep-th hep-ph | we systematically analyze the integrability of a pauli system in lorentz violating background at the nonrelativistic level both in two and threedimensions we consider the nonrelativistic limit of the dirac equation from the qed sector of the socalled standard model extension by keeping only two types of background coup... | [['we', 'systematically', 'analyze', 'the', 'integrability', 'of', 'a', 'pauli', 'system', 'in', 'lorentz', 'violating', 'background', 'at', 'the', 'nonrelativistic', 'level', 'both', 'in', 'two', 'and', 'threedimensions', 'we', 'consider', 'the', 'nonrelativistic', 'limit', 'of', 'the', 'dirac', 'equation', 'from', 't... | [-0.17582422058772423, 0.1851960332687856, 0.007260759564212941, 0.09012025791252481, -0.06876137209092749, -0.12997851366947952, 0.028562995088126125, 0.2846680541876061, -0.25492552884629577, -0.2661323172794976, 0.04317027755675773, -0.2882170771249642, -0.09969294036674345, 0.12867900461665002, 0.03505925796123157,... |
709.4277 | Geometric Transitions and Dynamical SUSY Breaking | We show that the physics of D-brane theories that exhibit dynamical SUSY
breaking due to stringy instanton effects is well captured by geometric
transitions, which recast the non-perturbative superpotential as a classical
flux superpotential. This allows for simple engineering of Fayet, Polonyi,
O'Raifeartaigh, and o... | hep-th | we show that the physics of dbrane theories that exhibit dynamical susy breaking due to stringy instanton effects is well captured by geometric transitions which recast the nonperturbative superpotential as a classical flux superpotential this allows for simple engineering of fayet polonyi oraifeartaigh and other canon... | [['we', 'show', 'that', 'the', 'physics', 'of', 'dbrane', 'theories', 'that', 'exhibit', 'dynamical', 'susy', 'breaking', 'due', 'to', 'stringy', 'instanton', 'effects', 'is', 'well', 'captured', 'by', 'geometric', 'transitions', 'which', 'recast', 'the', 'nonperturbative', 'superpotential', 'as', 'a', 'classical', 'fl... | [-0.11364693944587519, 0.24683355242737698, -0.09143179628115736, 0.18448877628696592, -0.09644674669068895, -0.17944109368009345, -0.038172275477432106, 0.24320830822628187, -0.28801358341680544, -0.3161506232695262, 0.09668223479744292, -0.19228861634454866, -0.17118770498353497, 0.10966426853663411, -0.0845038077279... |
709.4278 | Long-Range Reconnaissance Imager on New Horizons | The LOng-Range Reconnaissance Imager (LORRI) is the high resolution imaging
instrument for the New Horizons mission to Pluto, its giant satellite Charon,
its small moons Nix and Hydra, and the Kuiper Belt, which is the vast region of
icy bodies extending roughly from Neptune's orbit out to 50 astronomical units
(AU).... | astro-ph | the longrange reconnaissance imager lorri is the high resolution imaging instrument for the new horizons mission to pluto its giant satellite charon its small moons nix and hydra and the kuiper belt which is the vast region of icy bodies extending roughly from neptunes orbit out to 50 astronomical units au new horizons... | [['the', 'longrange', 'reconnaissance', 'imager', 'lorri', 'is', 'the', 'high', 'resolution', 'imaging', 'instrument', 'for', 'the', 'new', 'horizons', 'mission', 'to', 'pluto', 'its', 'giant', 'satellite', 'charon', 'its', 'small', 'moons', 'nix', 'and', 'hydra', 'and', 'the', 'kuiper', 'belt', 'which', 'is', 'the', '... | [-0.1251871751604098, 0.15477569616110337, -0.06273430447708525, -0.007311388161189355, -0.09344254396900392, -0.13026366491343058, 0.015805057706712394, 0.407994669485552, -0.18951986543667107, -0.40331901617472965, 0.13822346340985212, -0.29532690193619954, -0.006943074799182883, 0.23238347050439762, -0.1222802699751... |
709.4279 | ALICE: The Ultraviolet Imaging Spectrograph aboard the New Horizons
Pluto-Kuiper Belt Mission | The New Horizons ALICE instrument is a lightweight (4.4 kg), low-power (4.4
Watt) imaging spectrograph aboard the New Horizons mission to Pluto/Charon and
the Kuiper Belt. Its primary job is to determine the relative abundances of
various species in Pluto's atmosphere. ALICE will also be used to search for an
atmosph... | astro-ph | the new horizons alice instrument is a lightweight 44 kg lowpower 44 watt imaging spectrograph aboard the new horizons mission to plutocharon and the kuiper belt its primary job is to determine the relative abundances of various species in plutos atmosphere alice will also be used to search for an atmosphere around plu... | [['the', 'new', 'horizons', 'alice', 'instrument', 'is', 'a', 'lightweight', '44', 'kg', 'lowpower', '44', 'watt', 'imaging', 'spectrograph', 'aboard', 'the', 'new', 'horizons', 'mission', 'to', 'plutocharon', 'and', 'the', 'kuiper', 'belt', 'its', 'primary', 'job', 'is', 'to', 'determine', 'the', 'relative', 'abundanc... | [-0.07322560149774897, 0.16052452472680065, -0.10074173905983723, 0.04962495036549323, -0.09718097664153902, -0.14842987671727315, -0.0306762276692704, 0.41753267047655146, -0.18160464373067953, -0.3810160436939138, 0.12970816806773655, -0.32453861631802283, -0.07308467497750826, 0.22474952784129223, -0.153657397393544... |
709.428 | A converse to Moore's theorem on cellular automata | We prove a converse to Moore's ``Garden-of-Eden'' theorem: a group G is
amenable if and only if all cellular automata living on G that admit mutually
erasable patterns also admit gardens of Eden.
It had already been conjectured in that amenability could be characterized by
cellular automata. We prove the first part... | math.CO cs.IT math.DS math.GR math.IT | we prove a converse to moores gardenofeden theorem a group g is amenable if and only if all cellular automata living on g that admit mutually erasable patterns also admit gardens of eden it had already been conjectured in that amenability could be characterized by cellular automata we prove the first part of that conje... | [['we', 'prove', 'a', 'converse', 'to', 'moores', 'gardenofeden', 'theorem', 'a', 'group', 'g', 'is', 'amenable', 'if', 'and', 'only', 'if', 'all', 'cellular', 'automata', 'living', 'on', 'g', 'that', 'admit', 'mutually', 'erasable', 'patterns', 'also', 'admit', 'gardens', 'of', 'eden', 'it', 'had', 'already', 'been', ... | [-0.15200926475861873, 0.16789101853289387, -0.12128121683543379, 0.056977920397184786, -0.08262626823376526, -0.198223883963444, 0.06274527271955528, 0.38289416025985373, -0.2604327328503132, -0.16843623628162524, 0.1300188450883566, -0.21011289423754947, -0.23389154117215763, 0.20274580114267088, -0.15384307349608703... |
709.4281 | Ralph: A Visible/Infrared Imager for the New Horizons Pluto/Kuiper Belt
Mission | The New Horizons instrument named Ralph is a visible/near infrared
multi-spectral imager and a short wavelength infrared spectral imager. It is
one of the core instruments on New Horizons, NASA's first mission to the
Pluto/Charon system and the Kuiper Belt. Ralph combines panchromatic and color
imaging capabilities w... | astro-ph | the new horizons instrument named ralph is a visiblenear infrared multispectral imager and a short wavelength infrared spectral imager it is one of the core instruments on new horizons nasas first mission to the plutocharon system and the kuiper belt ralph combines panchromatic and color imaging capabilities with ir im... | [['the', 'new', 'horizons', 'instrument', 'named', 'ralph', 'is', 'a', 'visiblenear', 'infrared', 'multispectral', 'imager', 'and', 'a', 'short', 'wavelength', 'infrared', 'spectral', 'imager', 'it', 'is', 'one', 'of', 'the', 'core', 'instruments', 'on', 'new', 'horizons', 'nasas', 'first', 'mission', 'to', 'the', 'plu... | [-0.07550443721413472, 0.1231389142169365, -0.14893655507664258, 0.07592157831089921, -0.14398751492591055, -0.13174602199569904, -0.019508126114111717, 0.4121545661491153, -0.2073309904076439, -0.38652994754002956, 0.15759550637996203, -0.3028765983233592, -0.1237661152713953, 0.25697601537213177, -0.12564915789753422... |
709.4282 | Glassy protein dynamics and gigantic solvent reorganization energy of
plastocyanin | We report the results of Molecular Dynamics simulations of electron transfer
activation parameters of plastocyanin metalloprotein involved as electron
carrier in natural photosynthesis. We have discovered that slow, non-ergodic
conformational fluctuations of the protein, coupled to hydrating water, result
in a very b... | physics.bio-ph physics.chem-ph | we report the results of molecular dynamics simulations of electron transfer activation parameters of plastocyanin metalloprotein involved as electron carrier in natural photosynthesis we have discovered that slow nonergodic conformational fluctuations of the protein coupled to hydrating water result in a very broad di... | [['we', 'report', 'the', 'results', 'of', 'molecular', 'dynamics', 'simulations', 'of', 'electron', 'transfer', 'activation', 'parameters', 'of', 'plastocyanin', 'metalloprotein', 'involved', 'as', 'electron', 'carrier', 'in', 'natural', 'photosynthesis', 'we', 'have', 'discovered', 'that', 'slow', 'nonergodic', 'confo... | [-0.13470710068411956, 0.24193706175411175, -0.023540534377389122, 0.09631138981609239, 0.049196397342408694, -0.14911526744606707, 0.030833858525676824, 0.37760464372254454, -0.2914801153326125, -0.3064183930894642, -0.04259968872506623, -0.23625501235705032, -0.14283008447312046, 0.15756810195902785, 0.00621853628068... |
709.4283 | Production and detection of atomic hexadecapole at Earth's magnetic
field | Anisotropy of atomic states is characterized by population differences and
coherences between Zeeman sublevels. It can be efficiently created and probed
via resonant interactions with light, the technique which is at the heart of
modern atomic clocks and magnetometers. Recently, nonlinear magneto-optical
techniques h... | physics.atom-ph | anisotropy of atomic states is characterized by population differences and coherences between zeeman sublevels it can be efficiently created and probed via resonant interactions with light the technique which is at the heart of modern atomic clocks and magnetometers recently nonlinear magnetooptical techniques have bee... | [['anisotropy', 'of', 'atomic', 'states', 'is', 'characterized', 'by', 'population', 'differences', 'and', 'coherences', 'between', 'zeeman', 'sublevels', 'it', 'can', 'be', 'efficiently', 'created', 'and', 'probed', 'via', 'resonant', 'interactions', 'with', 'light', 'the', 'technique', 'which', 'is', 'at', 'the', 'he... | [-0.12937231133768723, 0.23344612037340834, -0.010961714289266268, 0.06449925763964919, -0.03408347438652437, -0.11474411724810744, 0.009837059280131483, 0.38212901589225284, -0.24114075817607836, -0.3167325380068927, -0.005361097402983232, -0.27068712501052655, -0.07864846116197961, 0.1910230874321884, 0.0346070304500... |
709.4284 | A squeezing formalism for finite dimensional quantum systems | This article presents a squeezing transformation for quantum systems
associated to finite vector spaces. The physical idea of squeezing here is
taken from the action of the usual squeezing operator over wave functions
defined on a real line, that is, a transformation capable to diminish (or
enhance) the mean square d... | quant-ph | this article presents a squeezing transformation for quantum systems associated to finite vector spaces the physical idea of squeezing here is taken from the action of the usual squeezing operator over wave functions defined on a real line that is a transformation capable to diminish or enhance the mean square deviatio... | [['this', 'article', 'presents', 'a', 'squeezing', 'transformation', 'for', 'quantum', 'systems', 'associated', 'to', 'finite', 'vector', 'spaces', 'the', 'physical', 'idea', 'of', 'squeezing', 'here', 'is', 'taken', 'from', 'the', 'action', 'of', 'the', 'usual', 'squeezing', 'operator', 'over', 'wave', 'functions', 'd... | [-0.1241184219574318, 0.1861951274246515, -0.08846633351021545, 0.05877854337078579, -0.08577311092472457, -0.12829922695961246, 0.00903279903503333, 0.36437129314513284, -0.28885563200418934, -0.18094443947948674, 0.11664929050219028, -0.2892748224350842, -0.1483908333008158, 0.2117745090806064, -0.05400431753096587, ... |
709.4285 | Weak convergence of Vervaat and Vervaat Error processes of long-range
dependent sequences | Following Cs\"{o}rg\H{o}, Szyszkowicz and Wang (Ann. Statist. {\bf 34},
(2006), 1013--1044) we consider a long range dependent linear sequence. We
prove weak convergence of the uniform Vervaat and the uniform Vervaat error
processes, extending their results to distributions with unbounded support and
removing normali... | math.PR | following csorgho szyszkowicz and wang ann statist bf 34 2006 10131044 we consider a long range dependent linear sequence we prove weak convergence of the uniform vervaat and the uniform vervaat error processes extending their results to distributions with unbounded support and removing normality assumption | [['following', 'csorgho', 'szyszkowicz', 'and', 'wang', 'ann', 'statist', 'bf', '34', '2006', '10131044', 'we', 'consider', 'a', 'long', 'range', 'dependent', 'linear', 'sequence', 'we', 'prove', 'weak', 'convergence', 'of', 'the', 'uniform', 'vervaat', 'and', 'the', 'uniform', 'vervaat', 'error', 'processes', 'extendi... | [-0.07731819783591411, 0.061852778286927125, -0.045487864704971966, 0.07448190958662466, -0.08615873269313438, -0.11359215691812675, 0.10005866300409914, 0.37173122844912787, -0.26695684894167987, -0.24489364293615587, 0.11303266977616162, -0.21272521941202946, -0.07479111078745601, 0.1345602590379051, -0.1583979662126... |
709.4286 | On the Radial Distribution of White Dwarfs in the Globular Cluster NGC
6397 | We have examined the radial distribution of white dwarfs over a single
HST/ACS field in the nearby globular cluster NGC 6397. In relaxed populations,
such as in a globular cluster, stellar velocity dispersion, and hence radial
distribution, is directly dependent on stellar masses. The progenitors of very
young cluste... | astro-ph | we have examined the radial distribution of white dwarfs over a single hstacs field in the nearby globular cluster ngc 6397 in relaxed populations such as in a globular cluster stellar velocity dispersion and hence radial distribution is directly dependent on stellar masses the progenitors of very young cluster white d... | [['we', 'have', 'examined', 'the', 'radial', 'distribution', 'of', 'white', 'dwarfs', 'over', 'a', 'single', 'hstacs', 'field', 'in', 'the', 'nearby', 'globular', 'cluster', 'ngc', '6397', 'in', 'relaxed', 'populations', 'such', 'as', 'in', 'a', 'globular', 'cluster', 'stellar', 'velocity', 'dispersion', 'and', 'hence'... | [-0.02095900384485032, 0.20110422299002056, -0.10432758229888148, 0.15807699952360796, -0.12050209404831683, -0.015618296719535633, 0.09322160456450311, 0.4249886900738434, -0.09748417878333755, -0.3721817130843798, 0.006341222366663041, -0.2689398415878208, -0.0084320148660077, 0.2276919944073867, -0.12415582658722997... |
709.4287 | Magnetic Field Upper Limits for Jet Formation | Context: Very high magnetic fields at the surface of neutron stars or in the
accretion disk of black holes inhibit the production of jets. Aims: We quantify
here the magnetic field strength for jet formation. Methods: By using the
Alfven Radius, R_A, we study what we call {\it the basic condition}, R_A/R_*=1
or R_A/R... | astro-ph | context very high magnetic fields at the surface of neutron stars or in the accretion disk of black holes inhibit the production of jets aims we quantify here the magnetic field strength for jet formation methods by using the alfven radius r_a we study what we call it the basic condition r_ar_1 or r_ar_lso1 lso last st... | [['context', 'very', 'high', 'magnetic', 'fields', 'at', 'the', 'surface', 'of', 'neutron', 'stars', 'or', 'in', 'the', 'accretion', 'disk', 'of', 'black', 'holes', 'inhibit', 'the', 'production', 'of', 'jets', 'aims', 'we', 'quantify', 'here', 'the', 'magnetic', 'field', 'strength', 'for', 'jet', 'formation', 'methods... | [-0.14583186158368597, 0.15328498376788352, -0.005175072257141423, 0.13465551465454054, -0.10323327586423081, -0.12006393134480647, 0.09368500269651979, 0.39560118763789026, -0.1604408532834325, -0.3216026335279745, 0.08010335426782914, -0.3100204027537611, 0.01885347876754437, 0.25575960042334017, -0.02720621912855258... |
709.4288 | The New Horizons Spacecraft | The New Horizons spacecraft was launched on 19 January 2006. The spacecraft
was designed to provide a platform for seven instruments that will collect and
return data from Pluto in 2015. The design drew on heritage from previous
missions developed at The Johns Hopkins University Applied Physics Laboratory
(APL) and o... | astro-ph | the new horizons spacecraft was launched on 19 january 2006 the spacecraft was designed to provide a platform for seven instruments that will collect and return data from pluto in 2015 the design drew on heritage from previous missions developed at the johns hopkins university applied physics laboratory apl and other m... | [['the', 'new', 'horizons', 'spacecraft', 'was', 'launched', 'on', '19', 'january', '2006', 'the', 'spacecraft', 'was', 'designed', 'to', 'provide', 'a', 'platform', 'for', 'seven', 'instruments', 'that', 'will', 'collect', 'and', 'return', 'data', 'from', 'pluto', 'in', '2015', 'the', 'design', 'drew', 'on', 'heritage... | [-0.0913530988033997, 0.1339085811146957, -0.08401228519173586, 0.02128325302800223, -0.12334495409047358, -0.1393029366079803, 0.04191702331169657, 0.35971763985206, -0.19171586655745854, -0.4382859697208217, 0.14675142815959594, -0.30820169445280343, -0.04079803904586527, 0.2728394877519586, -0.1364046187399457, 0.12... |
709.4289 | Optical limiting using Laguerre-Gaussian beams | We demonstrate optical limiting using the self-lensing effect of a
higher-order Laguerre-Gaussian beam in a thin dye-doped polymer sample, which
we find is consistent with our model using Gaussian decomposition. The peak
phase shift in the sample required for limiting is smaller than for a
fundamental Gaussian beam w... | physics.optics | we demonstrate optical limiting using the selflensing effect of a higherorder laguerregaussian beam in a thin dyedoped polymer sample which we find is consistent with our model using gaussian decomposition the peak phase shift in the sample required for limiting is smaller than for a fundamental gaussian beam with the ... | [['we', 'demonstrate', 'optical', 'limiting', 'using', 'the', 'selflensing', 'effect', 'of', 'a', 'higherorder', 'laguerregaussian', 'beam', 'in', 'a', 'thin', 'dyedoped', 'polymer', 'sample', 'which', 'we', 'find', 'is', 'consistent', 'with', 'our', 'model', 'using', 'gaussian', 'decomposition', 'the', 'peak', 'phase'... | [-0.058306464199524594, 0.1360039735231754, -0.10368991578819559, 0.004075847441152505, -0.06837549386546016, -0.12744160438202978, 0.031038831344203037, 0.45720636855591745, -0.23289490814375527, -0.26746673004099114, 0.08070528861272204, -0.24954461613122156, -0.08000043093788382, 0.20762914360281737, -0.026513039908... |
709.429 | HIP 56948: A Solar Twin With a Low Lithium Abundance | For more than a decade, 18 Sco (HD 146233) has been considered the star that
most closely resembles the Sun, even though significant differences such as its
Li content, which is about three times solar, exist. Using high resolution,
high S/N spectra obtained at McDonald Observatory, we show that the stars HIP
56948 a... | astro-ph | for more than a decade 18 sco hd 146233 has been considered the star that most closely resembles the sun even though significant differences such as its li content which is about three times solar exist using high resolution high sn spectra obtained at mcdonald observatory we show that the stars hip 56948 and hip 73815... | [['for', 'more', 'than', 'a', 'decade', '18', 'sco', 'hd', '146233', 'has', 'been', 'considered', 'the', 'star', 'that', 'most', 'closely', 'resembles', 'the', 'sun', 'even', 'though', 'significant', 'differences', 'such', 'as', 'its', 'li', 'content', 'which', 'is', 'about', 'three', 'times', 'solar', 'exist', 'using'... | [-0.045515211695445236, 0.16778287567209704, -0.06316675605828034, 0.11214664157985658, -0.1166671438337635, -0.09622327272603116, 0.04915620827121786, 0.3963243417738954, -0.1428008229068039, -0.39774117098858386, 0.09821808886388603, -0.2838963302240873, -0.09232218466710551, 0.21441930685580873, -0.13651213157447797... |
709.4291 | Affine descents and the Steinberg torus | Let $W\ltimes L$ be an irreducible affine Weyl group with Coxeter complex
$\Sigma$, where $W$ denotes the associated finite Weyl group and $L$ the
translation subgroup. The Steinberg torus is the Boolean cell complex obtained
by taking the quotient of $\Sigma$ by the lattice $L$. We show that the
ordinary and flag $h... | math.CO math.GT | let wltimes l be an irreducible affine weyl group with coxeter complex sigma where w denotes the associated finite weyl group and l the translation subgroup the steinberg torus is the boolean cell complex obtained by taking the quotient of sigma by the lattice l we show that the ordinary and flag hpolynomials of the st... | [['let', 'wltimes', 'l', 'be', 'an', 'irreducible', 'affine', 'weyl', 'group', 'with', 'coxeter', 'complex', 'sigma', 'where', 'w', 'denotes', 'the', 'associated', 'finite', 'weyl', 'group', 'and', 'l', 'the', 'translation', 'subgroup', 'the', 'steinberg', 'torus', 'is', 'the', 'boolean', 'cell', 'complex', 'obtained',... | [-0.18259941536450275, 0.10656397466893261, -0.06036157825427061, 0.021273130590863595, -0.10830517359836786, -0.16800655803160258, 0.006639971152051455, 0.33458133689472797, -0.33653552853071167, -0.14377676497248035, 0.08941335125860793, -0.26363927956360084, -0.16304983867815248, 0.17373478541978532, -0.082476373917... |
709.4292 | Reduced State Uniquely Defines Groverian Measure of Original Pure State | Groverian and Geometric entanglement measures of the n-party pure state are
expressed by the (n-1)-party reduced state density operator directly. This main
theorem derives several important consequences. First, if two pure n-qudit
states have reduced states of (n-1)-qudits, which are equivalent under local
unitary(LU... | quant-ph | groverian and geometric entanglement measures of the nparty pure state are expressed by the n1party reduced state density operator directly this main theorem derives several important consequences first if two pure nqudit states have reduced states of n1qudits which are equivalent under local unitarylu transformations ... | [['groverian', 'and', 'geometric', 'entanglement', 'measures', 'of', 'the', 'nparty', 'pure', 'state', 'are', 'expressed', 'by', 'the', 'n1party', 'reduced', 'state', 'density', 'operator', 'directly', 'this', 'main', 'theorem', 'derives', 'several', 'important', 'consequences', 'first', 'if', 'two', 'pure', 'nqudit', ... | [-0.12439605841751802, 0.1684013426273437, -0.0888766345906664, 0.10042243099199946, 0.028033375316722828, -0.20392148808830163, -0.0011178694834763354, 0.3005440308035097, -0.2658590801483528, -0.26268386127511884, 0.13824135121275585, -0.2901386920108714, -0.11796298739077016, 0.17901144459504972, -0.0261595759964124... |
709.4293 | Quark helicity flip and the transverse spin dependence of inclusive DIS | Inclusive DIS with unpolarized beam exhibits a subtle dependence on the
transverse target spin, arising from the interference of one-photon and
two-photon exchange amplitudes in the cross section. We argue that this
observable probes mainly the quark helicity-flip amplitudes induced by the
non-perturbative vacuum str... | hep-ph | inclusive dis with unpolarized beam exhibits a subtle dependence on the transverse target spin arising from the interference of onephoton and twophoton exchange amplitudes in the cross section we argue that this observable probes mainly the quark helicityflip amplitudes induced by the nonperturbative vacuum structure o... | [['inclusive', 'dis', 'with', 'unpolarized', 'beam', 'exhibits', 'a', 'subtle', 'dependence', 'on', 'the', 'transverse', 'target', 'spin', 'arising', 'from', 'the', 'interference', 'of', 'onephoton', 'and', 'twophoton', 'exchange', 'amplitudes', 'in', 'the', 'cross', 'section', 'we', 'argue', 'that', 'this', 'observabl... | [-0.12899711691790214, 0.30070319995126227, -0.1218381550743134, 0.12680212090290913, -0.06855723673035785, -0.050321249241972246, 0.020589401325905473, 0.34093720252010024, -0.20442137093050405, -0.2076612392310211, -0.05399419948206109, -0.2933182776175534, -0.023358288173705846, 0.07202507119815228, 0.07495167630949... |
709.4294 | New constraints on dark energy from the observed growth of the most
X-ray luminous galaxy clusters | We present constraints on the mean matter density, Omega_m, the normalization
of the density fluctuation power spectrum, sigma_8, and the dark-energy
equation-of-state parameter, w, obtained from measurements of the X-ray
luminosity function of the largest known galaxy clusters at redshifts z<0.7, as
compiled in the ... | astro-ph | we present constraints on the mean matter density omega_m the normalization of the density fluctuation power spectrum sigma_8 and the darkenergy equationofstate parameter w obtained from measurements of the xray luminosity function of the largest known galaxy clusters at redshifts z07 as compiled in the massive cluster... | [['we', 'present', 'constraints', 'on', 'the', 'mean', 'matter', 'density', 'omega_m', 'the', 'normalization', 'of', 'the', 'density', 'fluctuation', 'power', 'spectrum', 'sigma_8', 'and', 'the', 'darkenergy', 'equationofstate', 'parameter', 'w', 'obtained', 'from', 'measurements', 'of', 'the', 'xray', 'luminosity', 'f... | [-0.06844932711947795, 0.11792338425988089, -0.06201026091902432, 0.12372908059041947, -0.10643754940247163, -0.04275011603974483, 0.07353298528416252, 0.34637560388073324, -0.16707342281958765, -0.3877123230274513, 0.025549285651967776, -0.3608405129073865, 0.05883237821346318, 0.2266856027259068, 0.018311051821133746... |
709.4295 | NeIII/OII as an oxygen abundance indicator in the HII regions and HII
galaxies | To calibrate the relationship between Ne3O2 (Ne3O2 =
log(\neiii$\lambda3869$/\oii$\lambda3727$)) and oxygen abundances, we present a
sample of $\sim$3000 $\hii$ galaxies from the Sloan Digital Sky Survey (SDSS)
data release four. They are associated with a sample from the literature
intended to enlarge the oxygen abu... | astro-ph | to calibrate the relationship between ne3o2 ne3o2 logneiiilambda3869oiilambda3727 and oxygen abundances we present a sample of sim3000 hii galaxies from the sloan digital sky survey sdss data release four they are associated with a sample from the literature intended to enlarge the oxygen abundance region we calculated... | [['to', 'calibrate', 'the', 'relationship', 'between', 'ne3o2', 'ne3o2', 'logneiiilambda3869oiilambda3727', 'and', 'oxygen', 'abundances', 'we', 'present', 'a', 'sample', 'of', 'sim3000', 'hii', 'galaxies', 'from', 'the', 'sloan', 'digital', 'sky', 'survey', 'sdss', 'data', 'release', 'four', 'they', 'are', 'associated... | [0.02687492144476246, 0.05552628802907969, -0.05666528592112961, 0.08894173843530369, -0.04805215659437923, -0.04466034279933556, 0.11518825425698852, 0.45010840923674983, -0.1790616972651815, -0.3607971438597598, 0.011651661007549285, -0.33343449512429035, -0.018064038374417803, 0.2047444526009609, -0.0563288820424018... |
709.4296 | Chemical System Complexity and Bifurcation Point: a New Relationship | The article introduces a new relationship between the chemical system
complexity and deviation of its bifurcation point from thermodynamic
equilibrium. In the formalism of discrete thermodynamics of chemical
equilibria, simulation of numerous equilibrium cases with regards to complexity
of the reaction hosting system... | physics.chem-ph | the article introduces a new relationship between the chemical system complexity and deviation of its bifurcation point from thermodynamic equilibrium in the formalism of discrete thermodynamics of chemical equilibria simulation of numerous equilibrium cases with regards to complexity of the reaction hosting systems ha... | [['the', 'article', 'introduces', 'a', 'new', 'relationship', 'between', 'the', 'chemical', 'system', 'complexity', 'and', 'deviation', 'of', 'its', 'bifurcation', 'point', 'from', 'thermodynamic', 'equilibrium', 'in', 'the', 'formalism', 'of', 'discrete', 'thermodynamics', 'of', 'chemical', 'equilibria', 'simulation',... | [-0.1474769196676469, 0.056220078661751285, -0.15391557363845704, 0.039041326950869655, -0.00532559649814125, -0.1369366621429735, 0.1451725978455455, 0.2525684316284381, -0.3037467609833834, -0.31457007840112017, 0.07986399406122023, -0.3207350073198041, -0.1576992827621135, 0.14245425472752407, -0.048708243090864065,... |
709.4297 | Modulated Branching Processes, Origins of Power Laws and Queueing
Duality | Power law distributions have been repeatedly observed in a wide variety of
socioeconomic, biological and technological areas. In many of the observations,
e.g., city populations and sizes of living organisms, the objects of interest
evolve due to the replication of their many independent components, e.g.,
births-deat... | math.PR math.ST stat.TH | power law distributions have been repeatedly observed in a wide variety of socioeconomic biological and technological areas in many of the observations eg city populations and sizes of living organisms the objects of interest evolve due to the replication of their many independent components eg birthsdeaths of individu... | [['power', 'law', 'distributions', 'have', 'been', 'repeatedly', 'observed', 'in', 'a', 'wide', 'variety', 'of', 'socioeconomic', 'biological', 'and', 'technological', 'areas', 'in', 'many', 'of', 'the', 'observations', 'eg', 'city', 'populations', 'and', 'sizes', 'of', 'living', 'organisms', 'the', 'objects', 'of', 'i... | [-0.08558681219195326, 0.16515545011289187, -0.07866946415527275, 0.10847907444662673, -0.05315139304406734, -0.11004225076154668, 0.06783011330858076, 0.3458003884060653, -0.27426410561612874, -0.2979039841103023, 0.1341709308800529, -0.24366415496681132, -0.15072756448191488, 0.20243906831051894, -0.1521502521785873,... |
709.4298 | Observation of the Supernova Remnant IC 443 with VERITAS | Shell-type supernova remnants (SNRs) accelerate particles at the shock front
between the expanding remnant and the swept-up interstellar medium. If these
particles include protons and nuclei, very-high-energy gamma-ray emission may
result from the decay of pions produced in interactions between cosmic rays and
the lo... | astro-ph | shelltype supernova remnants snrs accelerate particles at the shock front between the expanding remnant and the sweptup interstellar medium if these particles include protons and nuclei veryhighenergy gammaray emission may result from the decay of pions produced in interactions between cosmic rays and the local insters... | [['shelltype', 'supernova', 'remnants', 'snrs', 'accelerate', 'particles', 'at', 'the', 'shock', 'front', 'between', 'the', 'expanding', 'remnant', 'and', 'the', 'sweptup', 'interstellar', 'medium', 'if', 'these', 'particles', 'include', 'protons', 'and', 'nuclei', 'veryhighenergy', 'gammaray', 'emission', 'may', 'resu... | [-0.08982784390160493, 0.21833659069060318, -0.02827979227288455, 0.13088776074863714, -0.1146788533894752, -0.06441021982269983, -0.0012521565752639167, 0.4371650302461509, -0.1867492829975351, -0.34002475235504154, -0.005282489596277304, -0.3474265291012995, 0.05408018330732981, 0.22510053543909186, 0.066673334380183... |
709.4299 | TeV and X-ray Monitoring of LS I +61 303 With VERITAS, Swift, and RXTE | Between September 2006 and February 2007, the galactic binary LS I +61 303
was monitored in the TeV band with the VERITAS array of imaging Cherenkov
telescopes. These observations confirm LS I +61 303 as a variable TeV gamma-ray
source, with emission peaking between orbital phase 0.6 and 0.7. During this
observationa... | astro-ph | between september 2006 and february 2007 the galactic binary ls i 61 303 was monitored in the tev band with the veritas array of imaging cherenkov telescopes these observations confirm ls i 61 303 as a variable tev gammaray source with emission peaking between orbital phase 06 and 07 during this observational period mo... | [['between', 'september', '2006', 'and', 'february', '2007', 'the', 'galactic', 'binary', 'ls', 'i', '61', '303', 'was', 'monitored', 'in', 'the', 'tev', 'band', 'with', 'the', 'veritas', 'array', 'of', 'imaging', 'cherenkov', 'telescopes', 'these', 'observations', 'confirm', 'ls', 'i', '61', '303', 'as', 'a', 'variabl... | [-0.07199218454770744, 0.13358100898206302, -0.03410737888022725, 0.09753889840462111, -0.07280074556557728, -0.13290390331697252, 0.06516380779711263, 0.46525581665337085, -0.2019480102841044, -0.4274710973458631, 0.13177858009003102, -0.37558745334390553, -0.009734368961237904, 0.19910082185108746, -0.003911525373613... |
709.43 | Observations of the Crab Nebula with the Whipple 10 m Telescope | Due to the strong and steady TeV gamma-ray emission from the Crab Nebula
supernova remnant, its measured flux and energy spectrum can be used to verify
the calibration and data reduction methods applied to IACT data acquired over
many observing seasons. This gives us confidence in the results obtained on
variable TeV... | astro-ph | due to the strong and steady tev gammaray emission from the crab nebula supernova remnant its measured flux and energy spectrum can be used to verify the calibration and data reduction methods applied to iact data acquired over many observing seasons this gives us confidence in the results obtained on variable tev sour... | [['due', 'to', 'the', 'strong', 'and', 'steady', 'tev', 'gammaray', 'emission', 'from', 'the', 'crab', 'nebula', 'supernova', 'remnant', 'its', 'measured', 'flux', 'and', 'energy', 'spectrum', 'can', 'be', 'used', 'to', 'verify', 'the', 'calibration', 'and', 'data', 'reduction', 'methods', 'applied', 'to', 'iact', 'dat... | [-0.06110434390232502, 0.0703635227890055, -0.06801795734670656, 0.10412479645904453, -0.053007494763942196, -0.060778701546783935, 0.07839754878693185, 0.391707128342027, -0.17766550059454386, -0.45660740705528136, 0.08932235991534103, -0.3212794127269252, 0.023035435428864312, 0.25518473916976103, -0.0737160294900123... |
709.4301 | A bright millisecond radio burst of extragalactic origin | Pulsar surveys offer one of the few opportunities to monitor even a small
fraction (~0.00001) of the radio sky for impulsive burst-like events with
millisecond durations. In analysis of archival survey data, we have discovered
a 30-Jy dispersed burst of duration <5 ms located three degrees from the Small
Magellanic C... | astro-ph | pulsar surveys offer one of the few opportunities to monitor even a small fraction 000001 of the radio sky for impulsive burstlike events with millisecond durations in analysis of archival survey data we have discovered a 30jy dispersed burst of duration 5 ms located three degrees from the small magellanic cloud the bu... | [['pulsar', 'surveys', 'offer', 'one', 'of', 'the', 'few', 'opportunities', 'to', 'monitor', 'even', 'a', 'small', 'fraction', '000001', 'of', 'the', 'radio', 'sky', 'for', 'impulsive', 'burstlike', 'events', 'with', 'millisecond', 'durations', 'in', 'analysis', 'of', 'archival', 'survey', 'data', 'we', 'have', 'discov... | [-0.16001394125182303, 0.14391085037571047, -0.07723655757839762, 0.14038257517911976, -0.10762856575104618, -0.09728561076636036, 0.08753017739077369, 0.3862086009354361, -0.21152512423483835, -0.3584471509281185, 0.10480788447837826, -0.325975781742243, -0.026815101917412494, 0.24680513680927577, -0.00067545549433317... |
709.4302 | Possibilities to verify the level density and radiative strength
functions, extracted from the two-step gamma-cascade intensities | The direct determination of the excitation level density and radiative
strength functions of their exciting gamma-transitions is impossible for the
larger part of the stable and long-life radioactive target nuclei. This
circumstance is uniquely determined by the fact, that the level spacing much
less than the resolut... | nucl-ex | the direct determination of the excitation level density and radiative strength functions of their exciting gammatransitions is impossible for the larger part of the stable and longlife radioactive target nuclei this circumstance is uniquely determined by the fact that the level spacing much less than the resolution of... | [['the', 'direct', 'determination', 'of', 'the', 'excitation', 'level', 'density', 'and', 'radiative', 'strength', 'functions', 'of', 'their', 'exciting', 'gammatransitions', 'is', 'impossible', 'for', 'the', 'larger', 'part', 'of', 'the', 'stable', 'and', 'longlife', 'radioactive', 'target', 'nuclei', 'this', 'circums... | [-0.08178475289003409, 0.15900217386861815, -0.05514790092161877, 0.09003433499791252, -0.02174927188878365, -0.06277055946100454, 0.053267224360626704, 0.34586834422200274, -0.2573601371179142, -0.3383107215561503, 0.058466364250213294, -0.2598427649936639, -0.052859927442302154, 0.1845491321572777, 0.0400253880060486... |
709.4303 | Security Analyses of One-time System | This paper has been withdrawn
| cs.CR | this paper has been withdrawn | [['this', 'paper', 'has', 'been', 'withdrawn']] | [-0.14966976195573806, -0.11479587350040674, -0.26925536394119265, -0.2174653896363452, -0.24278417900204657, -0.06483052410185337, -0.18645338097121567, 0.4360402226448059, -0.2831330731511116, -0.34362963438034055, 0.12004837393760681, -0.3683081828057766, -0.1602430183440447, -0.10558439195156097, -0.497941048443317... |
709.4304 | On the correctness of various approaches in the extraction of the
nucleus parameters on example of analysis of the two-step gamma-cascades in
163Dy compound nucleus | The model-free analysis of experimental data in the intensities of two-step
cascades into 163Dy shows, that the basically special features of the cascade
gamma-decay of its compound-state completely correspond to those observed in
other nuclei. Thus, the density of the levels in this nucleus with good
precision it is... | nucl-ex | the modelfree analysis of experimental data in the intensities of twostep cascades into 163dy shows that the basically special features of the cascade gammadecay of its compoundstate completely correspond to those observed in other nuclei thus the density of the levels in this nucleus with good precision it is reproduc... | [['the', 'modelfree', 'analysis', 'of', 'experimental', 'data', 'in', 'the', 'intensities', 'of', 'twostep', 'cascades', 'into', '163dy', 'shows', 'that', 'the', 'basically', 'special', 'features', 'of', 'the', 'cascade', 'gammadecay', 'of', 'its', 'compoundstate', 'completely', 'correspond', 'to', 'those', 'observed',... | [-0.09603953357172772, 0.16892374460579992, -0.046139910342808094, 0.07282794900034471, 0.011965381684394911, -0.06437272822299267, 0.053466334437187873, 0.340937413418411, -0.239268285066167, -0.32654417460923146, 0.017940519235866224, -0.30541255016325286, -0.07804480397574688, 0.1732647663997544, 0.01259981005261681... |
709.4305 | Measurements of the steady streaming flow around oscillating spheres
using 3D particle tracking velocimetry | Granular particles vibrated in a fluid have been found to exhibit
self-organization with attractive and repulsive interactions between the
particles. These interactions have been attributed to the steady streaming flow
around oscillating particles. Here we examine the steady streaming flow
surrounding a vertically os... | cond-mat.soft | granular particles vibrated in a fluid have been found to exhibit selforganization with attractive and repulsive interactions between the particles these interactions have been attributed to the steady streaming flow around oscillating particles here we examine the steady streaming flow surrounding a vertically oscilla... | [['granular', 'particles', 'vibrated', 'in', 'a', 'fluid', 'have', 'been', 'found', 'to', 'exhibit', 'selforganization', 'with', 'attractive', 'and', 'repulsive', 'interactions', 'between', 'the', 'particles', 'these', 'interactions', 'have', 'been', 'attributed', 'to', 'the', 'steady', 'streaming', 'flow', 'around', '... | [-0.14871199251957665, 0.23305699316201262, -0.11047835375395525, 0.026970380766412626, -0.03360330042182412, -0.15287393369958793, -0.036472746499264276, 0.3556100144836468, -0.2747243204166698, -0.2885106312537409, 0.05155656172007502, -0.3382082407261772, -0.0810296880095322, 0.14911738746864048, 0.02380823136934258... |
709.4306 | Modulation of bilayer quantum Hall states by tilted-field-induced
subband-Landau-level coupling | We study effects of tilted magnetic fields on energy levels in a
double-quantum-well (DQW) system, focusing on the coupling of subbands and
Landau levels (LLs). The subband-LL coupling induces anticrossings between LLs,
manifested directly in the magnetoresistance. The anticrossing gap becomes
larger than the spin sp... | cond-mat.mes-hall | we study effects of tilted magnetic fields on energy levels in a doublequantumwell dqw system focusing on the coupling of subbands and landau levels lls the subbandll coupling induces anticrossings between lls manifested directly in the magnetoresistance the anticrossing gap becomes larger than the spin splitting at th... | [['we', 'study', 'effects', 'of', 'tilted', 'magnetic', 'fields', 'on', 'energy', 'levels', 'in', 'a', 'doublequantumwell', 'dqw', 'system', 'focusing', 'on', 'the', 'coupling', 'of', 'subbands', 'and', 'landau', 'levels', 'lls', 'the', 'subbandll', 'coupling', 'induces', 'anticrossings', 'between', 'lls', 'manifested'... | [-0.2415981208785148, 0.2330402418587694, 0.007621298279163653, 0.09855965673943565, -0.018057805658639247, -0.16437313447160454, 0.05063054792318043, 0.35088479467507067, -0.24315626529077516, -0.33369191666936565, -0.04724565602272974, -0.28117426181340527, -0.11031764736059092, 0.2057202091372315, 0.0852792170681541... |
709.4307 | The rapid decline of the prompt emission in Gamma-Ray Bursts | Many gamma ray bursts (GRBs) have been observed with the Burst-Alert and
X-Ray telescopes of the Swift satellite. The successive `pulses' of these GRBs
end with a fast decline and a fast spectral softening, until they are overtaken
by another pulse, or the last pulse's decline is overtaken by a less
rapidly-varying `... | astro-ph | many gamma ray bursts grbs have been observed with the burstalert and xray telescopes of the swift satellite the successive pulses of these grbs end with a fast decline and a fast spectral softening until they are overtaken by another pulse or the last pulses decline is overtaken by a less rapidlyvarying afterglow the ... | [['many', 'gamma', 'ray', 'bursts', 'grbs', 'have', 'been', 'observed', 'with', 'the', 'burstalert', 'and', 'xray', 'telescopes', 'of', 'the', 'swift', 'satellite', 'the', 'successive', 'pulses', 'of', 'these', 'grbs', 'end', 'with', 'a', 'fast', 'decline', 'and', 'a', 'fast', 'spectral', 'softening', 'until', 'they', ... | [-0.04655796769333796, 0.20448566408379487, -0.11566843524471754, 0.15583891387063045, -0.09967336382854868, -0.09752028129339495, 0.01726061448506597, 0.5190940335117005, -0.20569418794130562, -0.2981804081549247, 0.05603581420965148, -0.31568710795922755, -0.01321293763100618, 0.2211271096301196, -0.02653936567906014... |
709.4308 | The Globular Cluster System of M60 (NGC 4649). I. CFHT MOS Spectroscopy
and Database | We present the measurement of radial velocities for globular clusters in M60,
giant elliptical galaxy in the Virgo cluster. Target globular cluster
candidates were selected using the Washington photometry based on the deep
$16\arcmin \times 16\arcmin$ images taken at the KPNO 4m and using the $VI$
photometry derived ... | astro-ph | we present the measurement of radial velocities for globular clusters in m60 giant elliptical galaxy in the virgo cluster target globular cluster candidates were selected using the washington photometry based on the deep 16arcmin times 16arcmin images taken at the kpno 4m and using the vi photometry derived from the hs... | [['we', 'present', 'the', 'measurement', 'of', 'radial', 'velocities', 'for', 'globular', 'clusters', 'in', 'm60', 'giant', 'elliptical', 'galaxy', 'in', 'the', 'virgo', 'cluster', 'target', 'globular', 'cluster', 'candidates', 'were', 'selected', 'using', 'the', 'washington', 'photometry', 'based', 'on', 'the', 'deep'... | [-0.048545407449217655, 0.07337464229651512, -0.0924762142587077, 0.021313426685922492, -0.07646685315166206, 0.0010667584227541317, 0.038863445000830464, 0.46506654801599395, -0.0874061057850038, -0.3994015185968377, 0.015308430745790247, -0.35946840121715257, 0.0462108296398163, 0.2347540797583441, -0.029356545122237... |
709.4309 | The Globular Cluster System of M60 (NGC 4649). II. Kinematics of the
Globular Cluster System | We present a kinematic analysis of the globular cluster (GC) system in the
giant elliptical galaxy (gE) M60 in the Virgo cluster. Using the photometric
and spectroscopic database of 121 GCs (83 blue GCs and 38 red GCs), we have
investigated the kinematics of the GC system. We have found that the M60 GC
system shows a... | astro-ph | we present a kinematic analysis of the globular cluster gc system in the giant elliptical galaxy ge m60 in the virgo cluster using the photometric and spectroscopic database of 121 gcs 83 blue gcs and 38 red gcs we have investigated the kinematics of the gc system we have found that the m60 gc system shows a significan... | [['we', 'present', 'a', 'kinematic', 'analysis', 'of', 'the', 'globular', 'cluster', 'gc', 'system', 'in', 'the', 'giant', 'elliptical', 'galaxy', 'ge', 'm60', 'in', 'the', 'virgo', 'cluster', 'using', 'the', 'photometric', 'and', 'spectroscopic', 'database', 'of', '121', 'gcs', '83', 'blue', 'gcs', 'and', '38', 'red',... | [-0.0973899567672141, 0.054293262610838444, -0.1432561820846063, 0.07952802106536602, -0.09615784661414531, -0.047618697581408645, -0.0055409713987058075, 0.46083352622241736, -0.1264613765032174, -0.34584679691873205, -0.01297468672997545, -0.2995082863027421, -0.02487511364131187, 0.22062470988972704, -0.048971347776... |
709.431 | Extensions and degenerations of spectral triples | For a unital C*-algebra A, which is equipped with a spectral triple and an
extension T of A by the compacts, we construct a family of spectral triples
associated to T and depending on the two positive parameters (s,t).
Using Rieffel's notation of quantum Gromov-Hausdorff distance between compact
quantum metric spac... | math.OA math-ph math.MP math.QA | for a unital calgebra a which is equipped with a spectral triple and an extension t of a by the compacts we construct a family of spectral triples associated to t and depending on the two positive parameters st using rieffels notation of quantum gromovhausdorff distance between compact quantum metric spaces it is possi... | [['for', 'a', 'unital', 'calgebra', 'a', 'which', 'is', 'equipped', 'with', 'a', 'spectral', 'triple', 'and', 'an', 'extension', 't', 'of', 'a', 'by', 'the', 'compacts', 'we', 'construct', 'a', 'family', 'of', 'spectral', 'triples', 'associated', 'to', 't', 'and', 'depending', 'on', 'the', 'two', 'positive', 'parameter... | [-0.1283103081604673, 0.08373083256697605, -0.0964782493473548, 0.07163380205655712, -0.05242803233623919, -0.11767730332859275, 0.039120008081146, 0.38021703510829763, -0.28963079103527384, -0.23999822804503815, 0.07860987845471956, -0.28463265743210087, -0.11563383512515833, 0.19771373121895724, -0.10309162565584605,... |
709.4311 | Bounds for the second and the third derivatives of the electron density
at the nucleus | Lower bound for ${\bar \rho}''(0)$, the second derivative of the spherically
averaged atomic electronic density at the nucleus, and upper bound for ${\bar
\rho}'''(0)$, the third derivative, are obtained respectively. It is shown
that, for the ground state, ${\bar \rho}''(0) \ge {10/3} Z^2 \rho(0)$ and
${\bar \rho}''... | physics.atom-ph physics.chem-ph | lower bound for bar rho0 the second derivative of the spherically averaged atomic electronic density at the nucleus and upper bound for bar rho0 the third derivative are obtained respectively it is shown that for the ground state bar rho0 ge 103 z2 rho0 and bar rho0 le 143z3 rho0 where z is the charge of the nucleus an... | [['lower', 'bound', 'for', 'bar', 'rho0', 'the', 'second', 'derivative', 'of', 'the', 'spherically', 'averaged', 'atomic', 'electronic', 'density', 'at', 'the', 'nucleus', 'and', 'upper', 'bound', 'for', 'bar', 'rho0', 'the', 'third', 'derivative', 'are', 'obtained', 'respectively', 'it', 'is', 'shown', 'that', 'for', ... | [-0.07785101726797004, 0.22248013727743216, -0.06140577765840172, 0.13603840682260465, 0.04667957061713542, -0.13619002209731726, 0.0638323315052372, 0.33032341425617534, -0.16758941478011283, -0.2135358734545533, -0.021225578255123563, -0.3752298815166484, 0.02763917178122534, 0.12655074348804926, 0.1267381789200384, ... |
709.4312 | Universality of quantum symplectic structure | Operating in the framework of `supmech' (a scheme of mechanics which aims at
providing a concrete setting for the axiomatization of physics and probability
theory as required in Hilbert's sixth problem; integrating noncommutative
symplectic geometry and noncommutative probability in an algebraic setting, it
associate... | math.SG math-ph math.MP math.QA quant-ph | operating in the framework of supmech a scheme of mechanics which aims at providing a concrete setting for the axiomatization of physics and probability theory as required in hilberts sixth problem integrating noncommutative symplectic geometry and noncommutative probability in an algebraic setting it associates with e... | [['operating', 'in', 'the', 'framework', 'of', 'supmech', 'a', 'scheme', 'of', 'mechanics', 'which', 'aims', 'at', 'providing', 'a', 'concrete', 'setting', 'for', 'the', 'axiomatization', 'of', 'physics', 'and', 'probability', 'theory', 'as', 'required', 'in', 'hilberts', 'sixth', 'problem', 'integrating', 'noncommutat... | [-0.1468330045637119, 0.11711941499034813, -0.0949701057755176, 0.07739702520765397, -0.06434634961432924, -0.2297733263480232, -0.027825789085973315, 0.30967244915990977, -0.31765801029018403, -0.2700680634006858, 0.09419698225591626, -0.23325672717928364, -0.16927933979885684, 0.19597895691587933, -0.1070054611844713... |
709.4313 | Schwinger Mechanism and Hawking Radiation as Quantum Tunneling | The common interpretation of the Hawking radiation as quantum tunneling has
some ambiguity such as coordinate-dependence of tunneling rate and
non-invariance of the action under canonical transformations. It is shown that
the tunneling process of black holes can be successfully described by Rindler
coordinates in ana... | hep-th | the common interpretation of the hawking radiation as quantum tunneling has some ambiguity such as coordinatedependence of tunneling rate and noninvariance of the action under canonical transformations it is shown that the tunneling process of black holes can be successfully described by rindler coordinates in analogy ... | [['the', 'common', 'interpretation', 'of', 'the', 'hawking', 'radiation', 'as', 'quantum', 'tunneling', 'has', 'some', 'ambiguity', 'such', 'as', 'coordinatedependence', 'of', 'tunneling', 'rate', 'and', 'noninvariance', 'of', 'the', 'action', 'under', 'canonical', 'transformations', 'it', 'is', 'shown', 'that', 'the',... | [-0.13953554359744233, 0.14734862805969678, -0.09923326411743218, 0.15487213020323498, -0.03914320991902765, -0.1692587279874498, 0.03490229046542142, 0.31259354123317484, -0.21613049757347177, -0.2747681705809351, 0.01569257274707918, -0.33760600740006613, -0.13154188435135492, 0.19417459908316828, -0.0531147652124958... |
709.4314 | Experimental demonstration of quantum leader election in linear optics | Linear optics is a promising candidate to enable the construction of quantum
computers. A number of quantum protocols gates based on linear optics have been
demonstrated. However, it is well-known that these gates are non-deterministic
and that higher order nonlinearity is necessary for deterministic operations.
We f... | quant-ph | linear optics is a promising candidate to enable the construction of quantum computers a number of quantum protocols gates based on linear optics have been demonstrated however it is wellknown that these gates are nondeterministic and that higher order nonlinearity is necessary for deterministic operations we found the... | [['linear', 'optics', 'is', 'a', 'promising', 'candidate', 'to', 'enable', 'the', 'construction', 'of', 'quantum', 'computers', 'a', 'number', 'of', 'quantum', 'protocols', 'gates', 'based', 'on', 'linear', 'optics', 'have', 'been', 'demonstrated', 'however', 'it', 'is', 'wellknown', 'that', 'these', 'gates', 'are', 'n... | [-0.15091100396358803, 0.14086293945828937, -0.0941403611078348, 0.0063411647283268, -0.05135384860308203, -0.31344613478812455, 0.038767789043996435, 0.38863811815438204, -0.25649168644712805, -0.29102863052426137, 0.1119015743168173, -0.21166366255803876, -0.18302604096801314, 0.30958767130664766, -0.0919269047715790... |
709.4315 | Pulsar Magnetic Field Oscillation Model and Verification Methods | We constructed the magnetic field oscillation model (hereafter the MO model)
by analogizing the periodically reversing phenomenon of the solar magnetic
field to pulsars. Almost all kinds of pulsar radiation phenomena are best
explained using the MO model, especially polarization characteristics, glitch,
generation ra... | astro-ph | we constructed the magnetic field oscillation model hereafter the mo model by analogizing the periodically reversing phenomenon of the solar magnetic field to pulsars almost all kinds of pulsar radiation phenomena are best explained using the mo model especially polarization characteristics glitch generation rate the g... | [['we', 'constructed', 'the', 'magnetic', 'field', 'oscillation', 'model', 'hereafter', 'the', 'mo', 'model', 'by', 'analogizing', 'the', 'periodically', 'reversing', 'phenomenon', 'of', 'the', 'solar', 'magnetic', 'field', 'to', 'pulsars', 'almost', 'all', 'kinds', 'of', 'pulsar', 'radiation', 'phenomena', 'are', 'bes... | [-0.11790624739073996, 0.1428673872168162, -0.005727261836543235, 0.115959749397224, -0.13892781117812855, -0.09197667532308555, 0.066181035986893, 0.4144589584737794, -0.209216953578419, -0.36158240122247987, 0.01853801215105732, -0.25097735077941985, -0.0619797660732892, 0.2823686201278287, -0.04781965884630249, -0.0... |
709.4316 | Confidence intervals for the normal mean utilizing prior information | Consider X_1,X_2,...,X_n that are independent and identically N(mu,sigma^2)
distributed. Suppose that we have uncertain prior information that mu = 0. We
answer the question: to what extent can a frequentist 1-alpha confidence
interval for mu utilize this prior information?
| math.ST stat.TH | consider x_1x_2x_n that are independent and identically nmusigma2 distributed suppose that we have uncertain prior information that mu 0 we answer the question to what extent can a frequentist 1alpha confidence interval for mu utilize this prior information | [['consider', 'x_1x_2x_n', 'that', 'are', 'independent', 'and', 'identically', 'nmusigma2', 'distributed', 'suppose', 'that', 'we', 'have', 'uncertain', 'prior', 'information', 'that', 'mu', '0', 'we', 'answer', 'the', 'question', 'to', 'what', 'extent', 'can', 'a', 'frequentist', '1alpha', 'confidence', 'interval', 'f... | [-0.11023988795617747, 0.14009106254859552, -0.08597237195165174, 0.11286726874311932, -0.14184931786479177, -0.2254839133144029, 0.14793499430792556, 0.46942068394776937, -0.29852306168224363, -0.2445337568988671, 0.1077780882840523, -0.30599095440796903, -0.05004314954291929, 0.05530529441563664, -0.14156201428960305... |
709.4317 | The connection between noise and quantum correlations in a double
quantum dot | We investigate the current and noise characteristics of a double quantum dot
system. The strong correlations induced by the Coulomb interaction create
entangled two-electron states and lead to signatures in the transport
properties. We show that the interaction parameter phi, which measures the
admixture of the doubl... | cond-mat.mes-hall | we investigate the current and noise characteristics of a double quantum dot system the strong correlations induced by the coulomb interaction create entangled twoelectron states and lead to signatures in the transport properties we show that the interaction parameter phi which measures the admixture of the doubleoccup... | [['we', 'investigate', 'the', 'current', 'and', 'noise', 'characteristics', 'of', 'a', 'double', 'quantum', 'dot', 'system', 'the', 'strong', 'correlations', 'induced', 'by', 'the', 'coulomb', 'interaction', 'create', 'entangled', 'twoelectron', 'states', 'and', 'lead', 'to', 'signatures', 'in', 'the', 'transport', 'pr... | [-0.17212967686355113, 0.20612646750440555, -0.07015017309625234, 0.09488352158639048, 0.04007148928940296, -0.15804717587307096, 0.048089741386606225, 0.32453041177775177, -0.31852012564694243, -0.2870452384863581, -0.04091609550939341, -0.3051909472261156, -0.12192423011043242, 0.15053624856684888, 0.0344533210487238... |
709.4318 | Comparative study between N-body and Fokker-Planck simulations for
rotating star clusters: I. Equal-mass system | We have carried out N-body simulations for rotating star clusters with equal
mass and compared the results with Fokker-Planck models. These two different
approaches are found to produce fairly similar results, although there are some
differences with regard to the detailed aspects. We confirmed the acceleration
of th... | astro-ph | we have carried out nbody simulations for rotating star clusters with equal mass and compared the results with fokkerplanck models these two different approaches are found to produce fairly similar results although there are some differences with regard to the detailed aspects we confirmed the acceleration of the core ... | [['we', 'have', 'carried', 'out', 'nbody', 'simulations', 'for', 'rotating', 'star', 'clusters', 'with', 'equal', 'mass', 'and', 'compared', 'the', 'results', 'with', 'fokkerplanck', 'models', 'these', 'two', 'different', 'approaches', 'are', 'found', 'to', 'produce', 'fairly', 'similar', 'results', 'although', 'there'... | [-0.11131947368637404, 0.13977771931954935, -0.13098790033466437, 0.0842516126926057, -0.04784643712495877, -0.04808582633691417, -0.014776762676509944, 0.3820068345489827, -0.20411005326208065, -0.34289598805321886, 0.04301431065594608, -0.2654886597259478, -0.008371280700984326, 0.19632614492862063, 0.004282400596209... |
709.4319 | Local density of diffeomorphisms with large centralizers | Given any compact manifold M, we construct a non-empty open subset O of the
space of C^1-diffeomorphisms of M and a dense subset D of O such that the
centralizer of every diffeomorphism in D is uncountable, hence non-trivial.
| math.DS | given any compact manifold m we construct a nonempty open subset o of the space of c1diffeomorphisms of m and a dense subset d of o such that the centralizer of every diffeomorphism in d is uncountable hence nontrivial | [['given', 'any', 'compact', 'manifold', 'm', 'we', 'construct', 'a', 'nonempty', 'open', 'subset', 'o', 'of', 'the', 'space', 'of', 'c1diffeomorphisms', 'of', 'm', 'and', 'a', 'dense', 'subset', 'd', 'of', 'o', 'such', 'that', 'the', 'centralizer', 'of', 'every', 'diffeomorphism', 'in', 'd', 'is', 'uncountable', 'henc... | [-0.26677008885412645, 0.12049039541624296, -0.014978778070937365, -0.008534030066444896, -0.062427121333968945, -0.15019147790586337, 0.07313592770160773, 0.3556089527331866, -0.25224361124520117, -0.16314330964516371, 0.07575569186920826, -0.273203176446259, -0.07399930556615193, 0.12125525701767167, -0.1115546672939... |
709.432 | Experimental observation of the Anderson transition with atomic matter
waves | We realize experimentally an atom-optics quantum chaotic system, the
quasiperiodic kicked rotor, which is equivalent to a 3D disordered system, that
allow us to demonstrate the Anderson metal-insulator transition. Sensitive
measurements of the atomic wavefunction dynamics and the use of finite-size
scaling techniques... | quant-ph cond-mat.mes-hall cond-mat.other cond-mat.stat-mech nlin.CD physics.optics | we realize experimentally an atomoptics quantum chaotic system the quasiperiodic kicked rotor which is equivalent to a 3d disordered system that allow us to demonstrate the anderson metalinsulator transition sensitive measurements of the atomic wavefunction dynamics and the use of finitesize scaling techniques make it ... | [['we', 'realize', 'experimentally', 'an', 'atomoptics', 'quantum', 'chaotic', 'system', 'the', 'quasiperiodic', 'kicked', 'rotor', 'which', 'is', 'equivalent', 'to', 'a', '3d', 'disordered', 'system', 'that', 'allow', 'us', 'to', 'demonstrate', 'the', 'anderson', 'metalinsulator', 'transition', 'sensitive', 'measureme... | [-0.10753710232184906, 0.14129024985002042, -0.08098499055976342, 0.0613464263764112, 0.001562498836919028, -0.22236775684685103, 0.06450164522117886, 0.34003886146666973, -0.23408099158519977, -0.2499379177246929, 0.05342851460016774, -0.29840096105870445, -0.1892755244258105, 0.21681649426280178, 0.029635894063271974... |
709.4321 | Chaotic scattering with direct processes: A generalization of Poisson's
kernel for non-unitary scattering matrices | The problem of chaotic scattering in presence of direct processes or prompt
responses is mapped via a transformation to the case of scattering in absence
of such processes for non-unitary scattering matrices, \tilde S. In the absence
of prompt responses, \tilde S is uniformly distributed according to its
invariant me... | cond-mat.mes-hall nlin.CD | the problem of chaotic scattering in presence of direct processes or prompt responses is mapped via a transformation to the case of scattering in absence of such processes for nonunitary scattering matrices tilde s in the absence of prompt responses tilde s is uniformly distributed according to its invariant measure in... | [['the', 'problem', 'of', 'chaotic', 'scattering', 'in', 'presence', 'of', 'direct', 'processes', 'or', 'prompt', 'responses', 'is', 'mapped', 'via', 'a', 'transformation', 'to', 'the', 'case', 'of', 'scattering', 'in', 'absence', 'of', 'such', 'processes', 'for', 'nonunitary', 'scattering', 'matrices', 'tilde', 's', '... | [-0.15148888720499978, 0.21301230011497038, -0.014832324697636068, 0.05745701148610584, -0.011110650931842365, -0.15547661244501035, 0.023609035163792935, 0.35266848744521306, -0.3022269590833593, -0.23416509794417856, 0.08991678486115212, -0.3364474699550936, -0.1325271595540175, 0.18436408968815624, -0.00150772067718... |
709.4322 | Rich methane laminar flames doped with light unsaturated hydrocarbons.
Part II: 1,3butadiene | In line with the study presented in the part I of this paper, the structure
of a laminar rich premixed methane flame doped with 1,3-butadiene has been
investigated. The flame contains 20.7% (molar) of methane, 31.4% of oxygen and
3.3% of 1,3-butadiene, corresponding to an equivalence ratio of 1.8, and a
ratio C4H6 / ... | physics.chem-ph | in line with the study presented in the part i of this paper the structure of a laminar rich premixed methane flame doped with 13butadiene has been investigated the flame contains 207 molar of methane 314 of oxygen and 33 of 13butadiene corresponding to an equivalence ratio of 18 and a ratio c4h6 ch4 of 16 the flame ha... | [['in', 'line', 'with', 'the', 'study', 'presented', 'in', 'the', 'part', 'i', 'of', 'this', 'paper', 'the', 'structure', 'of', 'a', 'laminar', 'rich', 'premixed', 'methane', 'flame', 'doped', 'with', '13butadiene', 'has', 'been', 'investigated', 'the', 'flame', 'contains', '207', 'molar', 'of', 'methane', '314', 'of',... | [-0.05309453440944679, 0.13192100487030406, -0.016542365795608718, -0.050484112020404565, 0.06230573316976901, -0.10385694443223574, 0.05539174343917578, 0.3603494464559604, -0.2011412475258112, -0.3043336606185351, 0.06413945619622985, -0.30954229832681085, -0.0254415621360143, 0.16691360987104456, 0.00633488009220590... |
709.4323 | Markov basis for design of experiments with three-level factors | We consider Markov basis arising from fractional factorial designs with
three-level factors. Once we have a Markov basis, $p$ values for various
conditional tests are estimated by the Markov chain Monte Carlo procedure. For
designed experiments with a single count observation for each run, we formulate
a generalized ... | stat.ME | we consider markov basis arising from fractional factorial designs with threelevel factors once we have a markov basis p values for various conditional tests are estimated by the markov chain monte carlo procedure for designed experiments with a single count observation for each run we formulate a generalized linear mo... | [['we', 'consider', 'markov', 'basis', 'arising', 'from', 'fractional', 'factorial', 'designs', 'with', 'threelevel', 'factors', 'once', 'we', 'have', 'a', 'markov', 'basis', 'p', 'values', 'for', 'various', 'conditional', 'tests', 'are', 'estimated', 'by', 'the', 'markov', 'chain', 'monte', 'carlo', 'procedure', 'for'... | [-0.05390941161007648, 0.12563260489300188, -0.0500286366735207, 0.10766153241563035, -0.05185925552510832, -0.1627985273008373, 0.06753146323135657, 0.4095126139645529, -0.27755409364800643, -0.29944277090011256, 0.1299785821108461, -0.25757576042030117, -0.11282544251125638, 0.17613215569526622, -0.018032575053817564... |
709.4324 | Hard Squares for z = -1 | The hard square model in statistical mechanics has been investigated for the
case when the activity z is -1. For cyclic boundary conditions, the
characteristic polynomial of the transfer matrix has an intriguingly simple
structure, all the eigenvalues $x$ being zero, roots of unity, or solutions of
x^3 = 4 cos^2 (pi*... | cond-mat.stat-mech | the hard square model in statistical mechanics has been investigated for the case when the activity z is 1 for cyclic boundary conditions the characteristic polynomial of the transfer matrix has an intriguingly simple structure all the eigenvalues x being zero roots of unity or solutions of x3 4 cos2 pimn here we tabul... | [['the', 'hard', 'square', 'model', 'in', 'statistical', 'mechanics', 'has', 'been', 'investigated', 'for', 'the', 'case', 'when', 'the', 'activity', 'z', 'is', '1', 'for', 'cyclic', 'boundary', 'conditions', 'the', 'characteristic', 'polynomial', 'of', 'the', 'transfer', 'matrix', 'has', 'an', 'intriguingly', 'simple'... | [-0.1517267832012612, 0.18144278871293917, -0.04862122199706082, 0.036129125426704226, -0.04881386611230888, -0.1785868363436854, -0.0022810241976047602, 0.4366544057226297, -0.2743100900998683, -0.22598013152974178, 0.15955860087155246, -0.28347876458202753, -0.1261064843839776, 0.15901365956897368, -0.009366683883465... |
709.4325 | Crypto-Harmonic Oscillator in Higher Dimensions: Classical and Quantum
Aspects | We study complexified Harmonic Oscillator models in two and three dimensions.
Our work is a generalization of the work of Smilga \cite{sm} who initiated the
study of these Crypto-gauge invariant models that can be related to
$PT$-symmetric models. We show that rotational symmetry in higher spatial
dimensions naturall... | hep-th math-ph math.MP quant-ph | we study complexified harmonic oscillator models in two and three dimensions our work is a generalization of the work of smilga citesm who initiated the study of these cryptogauge invariant models that can be related to ptsymmetric models we show that rotational symmetry in higher spatial dimensions naturally introduce... | [['we', 'study', 'complexified', 'harmonic', 'oscillator', 'models', 'in', 'two', 'and', 'three', 'dimensions', 'our', 'work', 'is', 'a', 'generalization', 'of', 'the', 'work', 'of', 'smilga', 'citesm', 'who', 'initiated', 'the', 'study', 'of', 'these', 'cryptogauge', 'invariant', 'models', 'that', 'can', 'be', 'relate... | [-0.10904791002842383, 0.12287488072767731, -0.05615748529537366, 0.0503815267718612, -0.07149066966907172, -0.16888964630069805, -0.04284511756274726, 0.35415929653374784, -0.21888709540100215, -0.2894264507506575, 0.07352667957784834, -0.25238558562001684, -0.2141043700170345, 0.1497514783455939, -0.07667506233389888... |
709.4326 | Some properties of group-theoretical categories | We first show that every group-theoretical category is graded by a certain
double coset ring. As a consequence, we obtain a necessary and sufficient
condition for a group-theoretical category to be nilpotent. We then give an
explicit description of the simple objects in a group-theoretical category
(following Ostrik,... | math.QA math.CT | we first show that every grouptheoretical category is graded by a certain double coset ring as a consequence we obtain a necessary and sufficient condition for a grouptheoretical category to be nilpotent we then give an explicit description of the simple objects in a grouptheoretical category following ostrik arxivmath... | [['we', 'first', 'show', 'that', 'every', 'grouptheoretical', 'category', 'is', 'graded', 'by', 'a', 'certain', 'double', 'coset', 'ring', 'as', 'a', 'consequence', 'we', 'obtain', 'a', 'necessary', 'and', 'sufficient', 'condition', 'for', 'a', 'grouptheoretical', 'category', 'to', 'be', 'nilpotent', 'we', 'then', 'giv... | [-0.1501601336935124, 0.032833911764455125, -0.10721466909223176, 0.09837896427194068, -0.17188076985479853, -0.14475332738154315, 0.03231643105542602, 0.3720729761309438, -0.35334701916541567, -0.16619690742295284, 0.09038639398497324, -0.1265128434684079, -0.16870127640084012, 0.153206379346356, -0.21718327070030008,... |
709.4327 | On and beyond entropy production: the case of Markov jump processes | How is it that entropy derivatives almost in their own are characterizing the
state of a system close to equilibrium, and what happens further away from it?
We explain within the framework of Markov jump processes why fluctuation theory
can be based on considerations involving entropy production alone when
perturbing... | cond-mat.stat-mech | how is it that entropy derivatives almost in their own are characterizing the state of a system close to equilibrium and what happens further away from it we explain within the framework of markov jump processes why fluctuation theory can be based on considerations involving entropy production alone when perturbing aro... | [['how', 'is', 'it', 'that', 'entropy', 'derivatives', 'almost', 'in', 'their', 'own', 'are', 'characterizing', 'the', 'state', 'of', 'a', 'system', 'close', 'to', 'equilibrium', 'and', 'what', 'happens', 'further', 'away', 'from', 'it', 'we', 'explain', 'within', 'the', 'framework', 'of', 'markov', 'jump', 'processes'... | [-0.11476378615420972, 0.17659313563499496, -0.15796428457303327, 0.11619066500806403, -0.03307218673709733, -0.11846724760135094, 0.051494018999930426, 0.28321806249751036, -0.31003591149479526, -0.2732676488665652, 0.09758531476541929, -0.293507080289382, -0.14448430507349533, 0.15072412388008735, -0.0307489298225109... |
709.4328 | Deeply Virtual Compton Scattering at JLab Hall A | The deeply virtual Compton scattering reaction has been investigated in the
Hall A of the Jefferson Laboratory by measuring longitudinally polarized
(e,e'gamma) cross sections, in the valence quark region, for protons and
neutrons. In the proton channel, experimental results strongly support the
factorization of the ... | nucl-ex | the deeply virtual compton scattering reaction has been investigated in the hall a of the jefferson laboratory by measuring longitudinally polarized eegamma cross sections in the valence quark region for protons and neutrons in the proton channel experimental results strongly support the factorization of the cross sect... | [['the', 'deeply', 'virtual', 'compton', 'scattering', 'reaction', 'has', 'been', 'investigated', 'in', 'the', 'hall', 'a', 'of', 'the', 'jefferson', 'laboratory', 'by', 'measuring', 'longitudinally', 'polarized', 'eegamma', 'cross', 'sections', 'in', 'the', 'valence', 'quark', 'region', 'for', 'protons', 'and', 'neutr... | [-0.04320477554279886, 0.3007497990833996, -0.11744218875537626, 0.11845817571930305, -0.021008792389302127, -0.02672848393890087, 0.0504319573210293, 0.37203882396504095, -0.21381098057933245, -0.22220451644138445, -0.09764805472090463, -0.34598984051778725, 0.08445272187973503, 0.18660144868625117, 0.0900627946671941... |
709.4329 | Detecting unambiguously non-Abelian geometric phases with trapped ions | We propose for the first time an experimentally feasible scheme to disclose
the noncommutative effects induced by a light-induced non-Abelian gauge
structure with trapped ions. Under an appropriate configuration, a true
non-Abelian gauge potential naturally arises in connection with the geometric
phase associated wit... | quant-ph | we propose for the first time an experimentally feasible scheme to disclose the noncommutative effects induced by a lightinduced nonabelian gauge structure with trapped ions under an appropriate configuration a true nonabelian gauge potential naturally arises in connection with the geometric phase associated with two d... | [['we', 'propose', 'for', 'the', 'first', 'time', 'an', 'experimentally', 'feasible', 'scheme', 'to', 'disclose', 'the', 'noncommutative', 'effects', 'induced', 'by', 'a', 'lightinduced', 'nonabelian', 'gauge', 'structure', 'with', 'trapped', 'ions', 'under', 'an', 'appropriate', 'configuration', 'a', 'true', 'nonabeli... | [-0.16735263428939828, 0.28038368444786416, -0.06694791787544843, 0.030762549200705414, -0.026246675916401476, -0.1448213980324438, 0.031381186011552424, 0.4092290704881226, -0.2835544626196397, -0.29256048444497945, 0.03236375528724928, -0.20924125564413082, -0.12942208185117562, 0.15731722389092942, -0.01750071176652... |
709.433 | Magneto-gyrotropic photogalvanic effects in GaN/AlGaN two-dimensional
systems | The magneto-gyrotropic photogalvanic and spin-galvanic effects are observed
in (0001)-oriented GaN/AlGaN heterojunctions excited by terahertz radiation. We
show that free-carrier absorption of linearly or circularly polarized terahertz
radiation in low-dimensional structures causes an electric photocurrent in the
pre... | cond-mat.mes-hall | the magnetogyrotropic photogalvanic and spingalvanic effects are observed in 0001oriented ganalgan heterojunctions excited by terahertz radiation we show that freecarrier absorption of linearly or circularly polarized terahertz radiation in lowdimensional structures causes an electric photocurrent in the presence of an... | [['the', 'magnetogyrotropic', 'photogalvanic', 'and', 'spingalvanic', 'effects', 'are', 'observed', 'in', '0001oriented', 'ganalgan', 'heterojunctions', 'excited', 'by', 'terahertz', 'radiation', 'we', 'show', 'that', 'freecarrier', 'absorption', 'of', 'linearly', 'or', 'circularly', 'polarized', 'terahertz', 'radiatio... | [-0.2143037323909464, 0.24981130876816435, 0.013019167554022661, 0.018675417833051076, -0.056518105741367855, -0.09739244155196557, -0.04230333731245639, 0.5169849721853857, -0.278225928044586, -0.24619479660889995, -0.05149015595740291, -0.32239520898672624, -0.19438193109817803, 0.2823361878373674, 0.0498133978681333... |
709.4331 | Spiral Galaxies in the SAURON Survey | We discuss some recent integral field spectroscopy using the SAURON
instrument of a sample consisting of 24 early-type spirals, part of the SAURON
Survey, and 18 late-type spirals. Using 2-dimensional maps of their stellar
radial velocity, velocity dispersion, and absorption line strength, it is now
much easier to un... | astro-ph | we discuss some recent integral field spectroscopy using the sauron instrument of a sample consisting of 24 earlytype spirals part of the sauron survey and 18 latetype spirals using 2dimensional maps of their stellar radial velocity velocity dispersion and absorption line strength it is now much easier to understand th... | [['we', 'discuss', 'some', 'recent', 'integral', 'field', 'spectroscopy', 'using', 'the', 'sauron', 'instrument', 'of', 'a', 'sample', 'consisting', 'of', '24', 'earlytype', 'spirals', 'part', 'of', 'the', 'sauron', 'survey', 'and', '18', 'latetype', 'spirals', 'using', '2dimensional', 'maps', 'of', 'their', 'stellar',... | [-0.09198817785829305, 0.024582117795944214, -0.09102602548897266, 0.10125272564589977, -0.16526699274778367, -0.02022554771353801, 0.035657195582365, 0.427976488918066, -0.16534937073166173, -0.33723762585471073, 0.036239658457537495, -0.2839971487224102, -0.11818537218806645, 0.23748256879548232, -0.02061816681409254... |
709.4332 | Sharp results in the integral-form John--Nirenberg inequality | We consider the strong form of the John-Nirenberg inequality for the
$L^2$-based BMO. We construct explicit Bellman functions for the inequality in
the continuous and dyadic settings and obtain the sharp constant as well as the
precise bound on the inequality's range of validity, both previously unknown.
The results ... | math.CA | we consider the strong form of the johnnirenberg inequality for the l2based bmo we construct explicit bellman functions for the inequality in the continuous and dyadic settings and obtain the sharp constant as well as the precise bound on the inequalitys range of validity both previously unknown the results for the two... | [['we', 'consider', 'the', 'strong', 'form', 'of', 'the', 'johnnirenberg', 'inequality', 'for', 'the', 'l2based', 'bmo', 'we', 'construct', 'explicit', 'bellman', 'functions', 'for', 'the', 'inequality', 'in', 'the', 'continuous', 'and', 'dyadic', 'settings', 'and', 'obtain', 'the', 'sharp', 'constant', 'as', 'well', '... | [-0.0910360488613757, 0.03452960895374417, -0.041175711325680216, 0.1313485320760972, -0.08740144970102443, -0.1275017953063879, 0.050972023008701704, 0.3667024883441627, -0.2754222831504497, -0.3003519440276755, 0.1374765981428532, -0.21672331764259273, -0.15542107089810694, 0.28130820768937054, -0.060342006892379785,... |
709.4333 | BAT X-ray Survey - III: X-ray Spectra and Statistical Properties | In this concluding part of the series of three papers dedicated to the
Swift/BAT hard X-ray survey (BXS), we focus on the X-ray spectral analysis and
statistical properties of the source sample. Using a dedicated method to
extract time-averaged spectra of BAT sources we show that Galactic sources
have, generally, sof... | astro-ph | in this concluding part of the series of three papers dedicated to the swiftbat hard xray survey bxs we focus on the xray spectral analysis and statistical properties of the source sample using a dedicated method to extract timeaveraged spectra of bat sources we show that galactic sources have generally softer spectra ... | [['in', 'this', 'concluding', 'part', 'of', 'the', 'series', 'of', 'three', 'papers', 'dedicated', 'to', 'the', 'swiftbat', 'hard', 'xray', 'survey', 'bxs', 'we', 'focus', 'on', 'the', 'xray', 'spectral', 'analysis', 'and', 'statistical', 'properties', 'of', 'the', 'source', 'sample', 'using', 'a', 'dedicated', 'method... | [-0.02247101798976629, 0.06689528599229373, -0.03852342741631039, 0.1496400550382237, -0.057394157532971724, -0.06446700851298734, 0.08884514468566825, 0.47825456478502937, -0.08722072798414743, -0.3849345726749717, 0.028060193786603137, -0.3979495719226228, 0.037852837165045713, 0.21104124245424713, -0.021825493458891... |
709.4334 | Noncommutative Brownian motions with Kesten distributions and related
Poisson processes | We introduce and study a noncommutative two-parameter family of
noncommutative Brownian motions in the free Fock space. They are associated
with Kesten laws and give a continuous interpolation between Brownian motions
in free probability and monotone probability. The combinatorics of our model is
based on ordered non... | math.QA math.PR | we introduce and study a noncommutative twoparameter family of noncommutative brownian motions in the free fock space they are associated with kesten laws and give a continuous interpolation between brownian motions in free probability and monotone probability the combinatorics of our model is based on ordered noncross... | [['we', 'introduce', 'and', 'study', 'a', 'noncommutative', 'twoparameter', 'family', 'of', 'noncommutative', 'brownian', 'motions', 'in', 'the', 'free', 'fock', 'space', 'they', 'are', 'associated', 'with', 'kesten', 'laws', 'and', 'give', 'a', 'continuous', 'interpolation', 'between', 'brownian', 'motions', 'in', 'fr... | [-0.11078984657208257, 0.1643874748671286, -0.08599447021870651, 0.09859522465281077, -0.07779496573909585, -0.07267796081889953, 0.05789810794383465, 0.3525733006452875, -0.32177561010411454, -0.2562921963011225, 0.0431165010391158, -0.25823949367622845, -0.12994150022015155, 0.1682222575320685, -0.08821315542029749, ... |
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