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706.4214 | Dynamical Systems On Three Manifolds Part II: 3-Manifolds,Heegaard
Splittings and Three-Dimensional Systems | The global behaviour of nonlinear systems is extremely important in control
and systems theory since the usual local theories will only give information
about a system in some neighbourhood of an operating point. Away from that
point, the system may have totally different behaviour and so the theory
developed for the... | math.DS | the global behaviour of nonlinear systems is extremely important in control and systems theory since the usual local theories will only give information about a system in some neighbourhood of an operating point away from that point the system may have totally different behaviour and so the theory developed for the loc... | [['the', 'global', 'behaviour', 'of', 'nonlinear', 'systems', 'is', 'extremely', 'important', 'in', 'control', 'and', 'systems', 'theory', 'since', 'the', 'usual', 'local', 'theories', 'will', 'only', 'give', 'information', 'about', 'a', 'system', 'in', 'some', 'neighbourhood', 'of', 'an', 'operating', 'point', 'away',... | [-0.19116171034834079, 0.12840272430361027, -0.12048138019764015, 0.09400232168733172, -0.017654566327109933, -0.14903392787316755, 0.022788982289174812, 0.3293625839174755, -0.2806575836974286, -0.2909273892761238, 0.15082727371519733, -0.2683977258669573, -0.1921194977232165, 0.20190397297471552, -0.07609032470340495... |
706.4215 | Polyakov loop and the color-flavor locked phase of Quantum
Chromodynamics | We consider the Polyakov Nambu Jona Lasinio model with three massless quarks
at high density and moderate temperature in the superconductive color flavor
locking phase. We compute the critical temperature $T_c$ as a function of the
baryonic chemical potential for the phase transition from the superconductive
state to... | hep-ph | we consider the polyakov nambu jona lasinio model with three massless quarks at high density and moderate temperature in the superconductive color flavor locking phase we compute the critical temperature t_c as a function of the baryonic chemical potential for the phase transition from the superconductive state to the ... | [['we', 'consider', 'the', 'polyakov', 'nambu', 'jona', 'lasinio', 'model', 'with', 'three', 'massless', 'quarks', 'at', 'high', 'density', 'and', 'moderate', 'temperature', 'in', 'the', 'superconductive', 'color', 'flavor', 'locking', 'phase', 'we', 'compute', 'the', 'critical', 'temperature', 't_c', 'as', 'a', 'funct... | [-0.1206413503347453, 0.2599765702865077, -0.057372598230694107, 0.049630431319333757, -0.03157840513237707, -0.11217322758878175, 0.13133059994507473, 0.36023937515661264, -0.18079851367013547, -0.25546055420491737, 0.03381885346070438, -0.3278020890520036, -0.10014494803725081, 0.08261088644000657, 0.0345739005947286... |
706.4216 | Entropy production in ac-calorimetry | In calorimetry and particularly in heat capacity measurements, different
characteristic relaxation time constants may perturb the experiment which
cannot be considered at thermodynamic equilibrium. In this case, thermodynamics
of irreversible processes has to be taken into account and the calorimetric
measurements mu... | cond-mat.other | in calorimetry and particularly in heat capacity measurements different characteristic relaxation time constants may perturb the experiment which cannot be considered at thermodynamic equilibrium in this case thermodynamics of irreversible processes has to be taken into account and the calorimetric measurements must be... | [['in', 'calorimetry', 'and', 'particularly', 'in', 'heat', 'capacity', 'measurements', 'different', 'characteristic', 'relaxation', 'time', 'constants', 'may', 'perturb', 'the', 'experiment', 'which', 'can', 'not', 'be', 'considered', 'at', 'thermodynamic', 'equilibrium', 'in', 'this', 'case', 'thermodynamics', 'of', ... | [-0.12632597936538367, 0.18954009587063803, -0.08193954853399928, 0.025923089269839047, -0.06981245322223706, -0.12424174566381858, 0.08434862278687733, 0.34896045138092735, -0.3178325841509843, -0.25662914972495926, 0.09228701241641553, -0.2807760440355426, -0.0989454413213048, 0.23067569753886025, -0.0157122134770372... |
706.4217 | W4 thermochemistry of P_2 and P_4. Is the CODATA heat of formation of
phosphorus atom correct? | The high-accuracy W4 computational thermochemistry protocol, and several
post-W4 methods, have been applied to the P$_2$ and P$_4$ molecules. Contrary
to previous studies, we find the experimental thermochemistry to be
fundamentally sound. The reaction enthalpy for P$_4\to 2$P$_2$ has a very
significant contribution ... | physics.chem-ph physics.atm-clus physics.comp-ph | the highaccuracy w4 computational thermochemistry protocol and several postw4 methods have been applied to the p_2 and p_4 molecules contrary to previous studies we find the experimental thermochemistry to be fundamentally sound the reaction enthalpy for p_4to 2p_2 has a very significant contribution from postccsdt cor... | [['the', 'highaccuracy', 'w4', 'computational', 'thermochemistry', 'protocol', 'and', 'several', 'postw4', 'methods', 'have', 'been', 'applied', 'to', 'the', 'p_2', 'and', 'p_4', 'molecules', 'contrary', 'to', 'previous', 'studies', 'we', 'find', 'the', 'experimental', 'thermochemistry', 'to', 'be', 'fundamentally', 's... | [-0.06232455002277025, 0.08227550451244627, -0.05959766615955492, 0.06316078374428409, 0.005114603721137557, -0.11096923126439963, 0.12718794883361884, 0.3933561970213694, -0.20081729539337434, -0.32772738936224155, 0.008213381254712918, -0.34470368969653337, -0.02311956182654415, 0.21594422414699302, 0.007595505212832... |
706.4218 | Association of heteronuclear molecules in a harmonic oscillator well | We describe the collisional interaction between two different atoms that are
trapped in a harmonic potential. The atoms are exposed to a magnetic field,
which is modulated in the vicinity of an s-wave Feshbach resonance, and we
study the formation of molecular bound states and excited states of the trapped
system wit... | cond-mat.other quant-ph | we describe the collisional interaction between two different atoms that are trapped in a harmonic potential the atoms are exposed to a magnetic field which is modulated in the vicinity of an swave feshbach resonance and we study the formation of molecular bound states and excited states of the trapped system with nont... | [['we', 'describe', 'the', 'collisional', 'interaction', 'between', 'two', 'different', 'atoms', 'that', 'are', 'trapped', 'in', 'a', 'harmonic', 'potential', 'the', 'atoms', 'are', 'exposed', 'to', 'a', 'magnetic', 'field', 'which', 'is', 'modulated', 'in', 'the', 'vicinity', 'of', 'an', 'swave', 'feshbach', 'resonanc... | [-0.20507535834542728, 0.2576531593372982, -0.026537858085198835, 0.057460699427280236, 0.05780471197583459, -0.13731067707254127, 0.007059563831849532, 0.3862041060897437, -0.23048901307311925, -0.2773531398312612, -0.05078178001144393, -0.32495830736377024, -0.05823148597370494, 0.13203491902148182, 0.105298719618638... |
706.4219 | Effect of physical inactivity on the oxidation of saturated and
monounsaturated dietary Fatty acids: results of a randomized trial | OBJECTIVES: Changes in the way dietary fat is metabolized can be considered
causative in obesity. The role of sedentary behavior in this defect has not
been determined. We hypothesized that physical inactivity partitions dietary
fats toward storage and that a resistance exercise training program mitigates
storage.
| q-bio.PE | objectives changes in the way dietary fat is metabolized can be considered causative in obesity the role of sedentary behavior in this defect has not been determined we hypothesized that physical inactivity partitions dietary fats toward storage and that a resistance exercise training program mitigates storage | [['objectives', 'changes', 'in', 'the', 'way', 'dietary', 'fat', 'is', 'metabolized', 'can', 'be', 'considered', 'causative', 'in', 'obesity', 'the', 'role', 'of', 'sedentary', 'behavior', 'in', 'this', 'defect', 'has', 'not', 'been', 'determined', 'we', 'hypothesized', 'that', 'physical', 'inactivity', 'partitions', '... | [-0.12171591570317421, 0.14327271816411824, -0.10673034178983906, 0.07794681863616341, -0.07048322875862537, -0.1577155312988907, 0.07512162814584925, 0.3925210677249276, -0.25868593739426654, -0.29640401620417833, 0.07921741891945915, -0.2671011269912529, -0.1849513745907208, 0.13526027153610534, -0.20894373078709064,... |
706.422 | Temperature micro-Raman study of lysozyme crystals | We have performed for the first time micro-Raman studies of lysozyme crystals
for the temperatures lower than the room one (in the range 282-300K). Anomalous
temperature dependence of the positions of Raman scattering bands has been
detected and discussed, which corresponds to the crystalline lysozyme structure
in th... | cond-mat.soft cond-mat.mtrl-sci | we have performed for the first time microraman studies of lysozyme crystals for the temperatures lower than the room one in the range 282300k anomalous temperature dependence of the positions of raman scattering bands has been detected and discussed which corresponds to the crystalline lysozyme structure in the vicini... | [['we', 'have', 'performed', 'for', 'the', 'first', 'time', 'microraman', 'studies', 'of', 'lysozyme', 'crystals', 'for', 'the', 'temperatures', 'lower', 'than', 'the', 'room', 'one', 'in', 'the', 'range', '282300k', 'anomalous', 'temperature', 'dependence', 'of', 'the', 'positions', 'of', 'raman', 'scattering', 'bands... | [-0.09983701095441166, 0.15108493539951362, -0.08036251316721342, -0.025982977594343985, 0.020785393269390474, -0.08011356446587918, 0.07165308897288478, 0.43043455109000206, -0.18591328298825086, -0.30104284294481787, 0.06377033806139869, -0.336702930607966, -0.06378413090596394, 0.20410216652921268, 0.095949446136245... |
706.4221 | Thermal instability of an expanding dusty plasma with equilibrium
cooling | We present an analysis of radiation induced instabilities in an expanding
plasma with considerable presence of dust particles and equilibrium cooling. We
have shown that the equilibrium expansion and cooling destabilize the radiation
condensation modes and the presence of dust particles enhances this effect. We
have ... | physics.plasm-ph | we present an analysis of radiation induced instabilities in an expanding plasma with considerable presence of dust particles and equilibrium cooling we have shown that the equilibrium expansion and cooling destabilize the radiation condensation modes and the presence of dust particles enhances this effect we have exam... | [['we', 'present', 'an', 'analysis', 'of', 'radiation', 'induced', 'instabilities', 'in', 'an', 'expanding', 'plasma', 'with', 'considerable', 'presence', 'of', 'dust', 'particles', 'and', 'equilibrium', 'cooling', 'we', 'have', 'shown', 'that', 'the', 'equilibrium', 'expansion', 'and', 'cooling', 'destabilize', 'the',... | [-0.11326060267421811, 0.1746341410209918, -0.10734322114050451, 0.06430303314069317, -0.029044535973945917, -0.051445131059893866, 0.0016315826984374957, 0.35671002858207895, -0.20408253650915004, -0.28062832824514894, 0.07539398016771144, -0.28022223827823745, -0.07802962312096004, 0.16839160553526955, -0.00895856618... |
706.4222 | Polarized and unpolarized $\mu$-pair meson-induced Drell--Yan production
and the pion distribution amplitude | We present a detailed analysis of meson-induced massive lepton (muon)
Drell--Yan production for the process $\pi^{-}N\to\mu^{+}\mu^{-}X$, considering
both an unpolarized nucleon target and longitudinally polarized protons. Using
a QCD framework, we focus on the angular distribution of $\mu^+$, which is
sensitive to t... | hep-ph | we present a detailed analysis of mesoninduced massive lepton muon drellyan production for the process pintomumux considering both an unpolarized nucleon target and longitudinally polarized protons using a qcd framework we focus on the angular distribution of mu which is sensitive to the shape of the pion distribution ... | [['we', 'present', 'a', 'detailed', 'analysis', 'of', 'mesoninduced', 'massive', 'lepton', 'muon', 'drellyan', 'production', 'for', 'the', 'process', 'pintomumux', 'considering', 'both', 'an', 'unpolarized', 'nucleon', 'target', 'and', 'longitudinally', 'polarized', 'protons', 'using', 'a', 'qcd', 'framework', 'we', 'f... | [-0.07571122021302774, 0.19340724092050246, -0.10465290551655926, 0.1524288172763022, -0.04783123092784081, -0.07392201264156029, 0.01494067355330723, 0.39722311093161505, -0.15522402709757444, -0.22784131704247557, -0.002769714320796387, -0.32501636919914745, 0.02142100108418769, 0.16110101412050426, 0.094873005063467... |
706.4223 | Emergence of a flux tube through a partially ionised solar atmosphere | For a magnetic flux tube, or indeed any flux, to emerge into the Solar corona
from the convection zone it must pass through the partially ionised layers of
the lower atmosphere: the photosphere and the chromosphere. In such regions the
ion-neutral collisions lead to an increased resistivity for currents flowing
acros... | astro-ph | for a magnetic flux tube or indeed any flux to emerge into the solar corona from the convection zone it must pass through the partially ionised layers of the lower atmosphere the photosphere and the chromosphere in such regions the ionneutral collisions lead to an increased resistivity for currents flowing across magne... | [['for', 'a', 'magnetic', 'flux', 'tube', 'or', 'indeed', 'any', 'flux', 'to', 'emerge', 'into', 'the', 'solar', 'corona', 'from', 'the', 'convection', 'zone', 'it', 'must', 'pass', 'through', 'the', 'partially', 'ionised', 'layers', 'of', 'the', 'lower', 'atmosphere', 'the', 'photosphere', 'and', 'the', 'chromosphere'... | [-0.1082277009581131, 0.17822499249951443, 0.002638155372724647, 0.06907734608789705, -0.06468701041384209, -0.07277729359830355, 0.021448800763119318, 0.36485744541051324, -0.24790201245028992, -0.31635666213268454, 0.0567084042787818, -0.24716023330725892, -0.05905162615669932, 0.18236040982550808, -0.017238718191175... |
706.4224 | User driven applications - new design paradigm | Programs for complicated engineering and scientific tasks always have to deal
with a problem of showing numerous graphical results. The limits of the screen
space and often opposite requirements from different users are the cause of the
infinite discussions between designers and users, but the source of this
ongoing ... | cs.GR cs.HC | programs for complicated engineering and scientific tasks always have to deal with a problem of showing numerous graphical results the limits of the screen space and often opposite requirements from different users are the cause of the infinite discussions between designers and users but the source of this ongoing conf... | [['programs', 'for', 'complicated', 'engineering', 'and', 'scientific', 'tasks', 'always', 'have', 'to', 'deal', 'with', 'a', 'problem', 'of', 'showing', 'numerous', 'graphical', 'results', 'the', 'limits', 'of', 'the', 'screen', 'space', 'and', 'often', 'opposite', 'requirements', 'from', 'different', 'users', 'are', ... | [-0.06891515169648782, 0.0626528782900149, -0.07752537165823228, 0.05814133526086259, -0.1779482819044086, -0.17588991206515964, 0.03400965176303597, 0.39490812085568905, -0.2756246008725344, -0.36025628701728934, 0.1383969581055948, -0.24745299089973902, -0.15739534472060554, 0.26268931089297815, -0.12668403123560198,... |
706.4225 | Topology of the regular part for infinitely renormalizable quadratic
polynomials | In this paper we describe the well studied process of renormalization of
quadratic polynomials from the point of view of their natural extensions. In
particular, we describe the topology of the inverse limit of infinitely
renormalizable quadratic polynomials and prove that when they satisfy a-priori
bounds, the topol... | math.DS math.GT | in this paper we describe the well studied process of renormalization of quadratic polynomials from the point of view of their natural extensions in particular we describe the topology of the inverse limit of infinitely renormalizable quadratic polynomials and prove that when they satisfy apriori bounds the topology is... | [['in', 'this', 'paper', 'we', 'describe', 'the', 'well', 'studied', 'process', 'of', 'renormalization', 'of', 'quadratic', 'polynomials', 'from', 'the', 'point', 'of', 'view', 'of', 'their', 'natural', 'extensions', 'in', 'particular', 'we', 'describe', 'the', 'topology', 'of', 'the', 'inverse', 'limit', 'of', 'infini... | [-0.15687853926880602, 0.09582427140536173, -0.10443389257591851, 0.10693794057198898, -0.07333889429650779, -0.09840407161885556, 0.03786662897701323, 0.2940702961652346, -0.3774421585477748, -0.23486112121422337, 0.09782761851554068, -0.25028052005284235, -0.22222619246744182, 0.17241337308484428, -0.1097936612413317... |
706.4226 | On the methods to construct UFD counterexamples to a cancellation
problem | In a previous paper, the author together with prof. dr. Finston constructed a
class of UFDs A_{n,m} where n,m\in \N^*. These rings are all stably equivalent
(A_{n,m}[T]\cong A_{p,q}[T] for all n,m,p,q) but are only isomorphic themselves
if (n,m)=(p,q). These examples are the first UFD examples over a
characteristical... | math.AG math.AC | in a previous paper the author together with prof dr finston constructed a class of ufds a_nm where nmin n these rings are all stably equivalent a_nmtcong a_pqt for all nmpq but are only isomorphic themselves if nmpq these examples are the first ufd examples over a characteristically closed field satisfying this behavi... | [['in', 'a', 'previous', 'paper', 'the', 'author', 'together', 'with', 'prof', 'dr', 'finston', 'constructed', 'a', 'class', 'of', 'ufds', 'a_nm', 'where', 'nmin', 'n', 'these', 'rings', 'are', 'all', 'stably', 'equivalent', 'a_nmtcong', 'a_pqt', 'for', 'all', 'nmpq', 'but', 'are', 'only', 'isomorphic', 'themselves', '... | [-0.10528423640789697, 0.08870863516349345, -0.045741683375672436, 0.06525747021405551, -0.08521727608167566, -0.15004595891223288, -0.037058667428209444, 0.3945444154785946, -0.25106814813334494, -0.25008084753644655, 0.11351031995582161, -0.2737506844336167, -0.20344333551765886, 0.24074022064451128, -0.1115073922963... |
706.4227 | Angles from B Decays with Charm: Summary of Working Group 5 of the CKM
Workshop 2006 | We summarize the results presented in Working Group 5 (WG5) of the CKM 2006
Workshop in Nagoya. The charge of WG5 was to discuss the measurements of
unitarity triangle angles $\beta/\phi_1$ and $\gamma/\phi_3$ from $B$-meson
decays containing charm quark(s) in the final states.
| hep-ph hep-ex | we summarize the results presented in working group 5 wg5 of the ckm 2006 workshop in nagoya the charge of wg5 was to discuss the measurements of unitarity triangle angles betaphi_1 and gammaphi_3 from bmeson decays containing charm quarks in the final states | [['we', 'summarize', 'the', 'results', 'presented', 'in', 'working', 'group', '5', 'wg5', 'of', 'the', 'ckm', '2006', 'workshop', 'in', 'nagoya', 'the', 'charge', 'of', 'wg5', 'was', 'to', 'discuss', 'the', 'measurements', 'of', 'unitarity', 'triangle', 'angles', 'betaphi_1', 'and', 'gammaphi_3', 'from', 'bmeson', 'dec... | [-0.07049184655997812, 0.2705529606901109, -0.0800483131372347, 0.02983759482186742, -0.04304805334952728, -0.08981003868961479, 0.1065642067895657, 0.2587537323011131, -0.17392344687917702, -0.27090058711970727, 0.035830501918453814, -0.38986934894673164, 0.01238908172335203, 0.12121364892255969, -0.007723806448644254... |
706.4228 | Piezooptic Coefficients and Acoustic Wave Velocities in Sn2P2S6 Crystals | Piezooptic coefficients of Sn2P2S6 crystals are experimentally determined for
l=623.8 nm and T=293 K with the aid of interferometric technique. The
components of the elastic stiffness tensor for these crystals are calculated on
the basis of studies for the acoustic wave velocities. It is shown that
acoustooptic figur... | physics.optics physics.gen-ph | piezooptic coefficients of sn2p2s6 crystals are experimentally determined for l6238 nm and t293 k with the aid of interferometric technique the components of the elastic stiffness tensor for these crystals are calculated on the basis of studies for the acoustic wave velocities it is shown that acoustooptic figure of me... | [['piezooptic', 'coefficients', 'of', 'sn2p2s6', 'crystals', 'are', 'experimentally', 'determined', 'for', 'l6238', 'nm', 'and', 't293', 'k', 'with', 'the', 'aid', 'of', 'interferometric', 'technique', 'the', 'components', 'of', 'the', 'elastic', 'stiffness', 'tensor', 'for', 'these', 'crystals', 'are', 'calculated', '... | [-0.13949460683088227, 0.1998143447889832, -0.0465927066020014, -0.0769071159618825, -0.06402794206351564, -0.12000681141293362, -0.023347662157264717, 0.4400999168293518, -0.2079231466183014, -0.273013907991219, 0.0724181570766265, -0.30138738061252396, -0.11222806795124422, 0.2898709911918431, 0.06941841941392213, 0.... |
706.4229 | Classification of Graded Left-symmetric Algebra Structures on Witt and
Virasoro Algebras | We find that a compatible graded left-symmetric algebra structure on the Witt
algebra induces an indecomposable module of the Witt algebra with 1-dimensional
weight spaces by its left multiplication operators. From the classification of
such modules of the Witt algebra, the compatible graded left-symmetric algebra
st... | math.QA math-ph math.MP | we find that a compatible graded leftsymmetric algebra structure on the witt algebra induces an indecomposable module of the witt algebra with 1dimensional weight spaces by its left multiplication operators from the classification of such modules of the witt algebra the compatible graded leftsymmetric algebra structure... | [['we', 'find', 'that', 'a', 'compatible', 'graded', 'leftsymmetric', 'algebra', 'structure', 'on', 'the', 'witt', 'algebra', 'induces', 'an', 'indecomposable', 'module', 'of', 'the', 'witt', 'algebra', 'with', '1dimensional', 'weight', 'spaces', 'by', 'its', 'left', 'multiplication', 'operators', 'from', 'the', 'class... | [-0.2017554625564692, 0.02915278149009041, -0.025282442968870913, 0.06233399440249314, -0.20695806448395382, -0.1461333524321719, -0.13470125331172758, 0.3788630626715568, -0.4704679173930567, -0.15047248416789333, 0.15352738138326272, -0.22720624243930262, -0.18217354524246304, 0.2030785231641969, -0.1764526707452855,... |
706.423 | On the set of complex points of a 2-sphere | Let $G$ be a strictly pseudoconvex domain in $\mathbb{C}^2$ with
$C^\infty$-smooth boundary $\partial G$. Let $S$ be a 2-dimensional sphere
embedded into $\partial G$. Denote by $\mathcal{E}$ the set of all complex
points on $S$. We study how the structure of the set $\mathcal{E}$ depends on
the smoothness of $S$
| math.CV | let g be a strictly pseudoconvex domain in mathbbc2 with cinftysmooth boundary partial g let s be a 2dimensional sphere embedded into partial g denote by mathcale the set of all complex points on s we study how the structure of the set mathcale depends on the smoothness of s | [['let', 'g', 'be', 'a', 'strictly', 'pseudoconvex', 'domain', 'in', 'mathbbc2', 'with', 'cinftysmooth', 'boundary', 'partial', 'g', 'let', 's', 'be', 'a', '2dimensional', 'sphere', 'embedded', 'into', 'partial', 'g', 'denote', 'by', 'mathcale', 'the', 'set', 'of', 'all', 'complex', 'points', 'on', 's', 'we', 'study', ... | [-0.24320177104324103, 0.07795197011902928, -0.04446698306128383, -0.08807529179379343, -0.1342368123214692, -0.11752726355567575, -0.0020057747140526773, 0.32072170995175836, -0.32181894455105065, -0.17207998158410193, 0.08388097695773468, -0.2968271164596081, -0.0631408173777163, 0.16842799618840218, -0.0949832347407... |
706.4231 | Un coronographe interf\'erentiel achromatique coaxial | On-axis achromatic interfero-coronagraph. We present a new type of stellar
interfero-coronagraph, the "CIAXE", which is a variant of the "AIC", the
Achromatic Interfero-Coronagraph [3,4]. The CIAXE is characterized by a very
simple, compact and fully coaxial optical combination. Indeed, contrarily to
the classical AI... | astro-ph | onaxis achromatic interferocoronagraph we present a new type of stellar interferocoronagraph the ciaxe which is a variant of the aic the achromatic interferocoronagraph 34 the ciaxe is characterized by a very simple compact and fully coaxial optical combination indeed contrarily to the classical aic which has a michels... | [['onaxis', 'achromatic', 'interferocoronagraph', 'we', 'present', 'a', 'new', 'type', 'of', 'stellar', 'interferocoronagraph', 'the', 'ciaxe', 'which', 'is', 'a', 'variant', 'of', 'the', 'aic', 'the', 'achromatic', 'interferocoronagraph', '34', 'the', 'ciaxe', 'is', 'characterized', 'by', 'a', 'very', 'simple', 'compa... | [-0.19594885003043397, 0.059620103448252665, -0.1628032006765454, 0.07160166986456686, -0.11935174219718064, -0.174967608227541, -0.10029209534156272, 0.202429127081538, -0.12867356812122954, -0.2838092521094623, 0.07012036418361757, -0.32476952116350444, -0.16248794329834035, 0.16318680542283115, -0.23981159473664723,... |
706.4232 | Slippery or sticky ! Control of wrinkling patterns by selective adhesion | Wrinkling patterns at the metallized surface of thin polymer films are shown
to be sensitive to the sticky or slippery character of the polymer/substrate
interface (titanium coating, polystyrene film and coated silicon substrate).
Selective prefered wrinkle orientation and amplitude are achieved. Existing
theoretical... | cond-mat.soft | wrinkling patterns at the metallized surface of thin polymer films are shown to be sensitive to the sticky or slippery character of the polymersubstrate interface titanium coating polystyrene film and coated silicon substrate selective prefered wrinkle orientation and amplitude are achieved existing theoretical models ... | [['wrinkling', 'patterns', 'at', 'the', 'metallized', 'surface', 'of', 'thin', 'polymer', 'films', 'are', 'shown', 'to', 'be', 'sensitive', 'to', 'the', 'sticky', 'or', 'slippery', 'character', 'of', 'the', 'polymersubstrate', 'interface', 'titanium', 'coating', 'polystyrene', 'film', 'and', 'coated', 'silicon', 'subst... | [-0.09011960821838952, 0.19586931943501296, -0.06575910251162816, -0.05669287846243957, -0.06787346394552865, -0.2604055179001175, 0.00540655883633646, 0.5384267983598667, -0.2737774073816182, -0.28413879642622514, 0.06540584172073163, -0.28763892163375493, -0.13102276133487753, 0.15594721563990643, -0.0792668160181819... |
706.4233 | Symmetry in semidefinite programs | This paper is a tutorial in a general and explicit procedure to simplify
semidefinite programs which are invariant under the action of a symmetry group.
The procedure is based on basic notions of representation theory of finite
groups. As an example we derive the block diagonalization of the Terwilliger
algebra of th... | math.OC math.CO | this paper is a tutorial in a general and explicit procedure to simplify semidefinite programs which are invariant under the action of a symmetry group the procedure is based on basic notions of representation theory of finite groups as an example we derive the block diagonalization of the terwilliger algebra of the bi... | [['this', 'paper', 'is', 'a', 'tutorial', 'in', 'a', 'general', 'and', 'explicit', 'procedure', 'to', 'simplify', 'semidefinite', 'programs', 'which', 'are', 'invariant', 'under', 'the', 'action', 'of', 'a', 'symmetry', 'group', 'the', 'procedure', 'is', 'based', 'on', 'basic', 'notions', 'of', 'representation', 'theor... | [-0.16181489579778696, 0.06798924715777892, -0.15015470795333385, 0.05252925880652453, -0.12236294218538595, -0.1374774280935526, 0.049066855432465674, 0.37508239640987345, -0.3251486658484542, -0.21173088445461222, 0.14976581384627416, -0.19311775688215027, -0.23552708981026496, 0.1492457562691665, -0.0933057474305055... |
706.4234 | Indicative Surfaces for Crystal Optical Effects | This paper has mainly a pedagogical meaning. Our aim is to demonstrate a
correct general approach for constructing indicative surfaces of higher-rank
tensors. We reconstruct the surfaces of piezo-optic tensor for beta-BaB2O4 and
LiNbO3 crystals, which have been incorrectly presented in our recent papers.
| physics.optics physics.gen-ph | this paper has mainly a pedagogical meaning our aim is to demonstrate a correct general approach for constructing indicative surfaces of higherrank tensors we reconstruct the surfaces of piezooptic tensor for betabab2o4 and linbo3 crystals which have been incorrectly presented in our recent papers | [['this', 'paper', 'has', 'mainly', 'a', 'pedagogical', 'meaning', 'our', 'aim', 'is', 'to', 'demonstrate', 'a', 'correct', 'general', 'approach', 'for', 'constructing', 'indicative', 'surfaces', 'of', 'higherrank', 'tensors', 'we', 'reconstruct', 'the', 'surfaces', 'of', 'piezooptic', 'tensor', 'for', 'betabab2o4', 'a... | [-0.060613184976814824, 0.06645829721607945, -0.10078484200957147, 0.004938258778896521, -0.12846644303168764, -0.0991673872763799, -0.044754765956895426, 0.3941655300388282, -0.1824790743518282, -0.2672894009473649, 0.07261347620144741, -0.2752778097479181, -0.22643456121229313, 0.1574558953712271, -0.1080781954382969... |
706.4235 | Effect of hydrostatic pressure on elastic properties of ZDTP tribofilms | Previous studies have shown that the elastic properties of Zinc
Dialkyl-dithiophosphate (ZDTP) tribofilms measured by nanoindentation increase
versus applied pressure (Anvil effect) [1, 2]. The aim of this paper is to
demonstrate that, up to 8 GPa, this increase is a reversible phenomenon. A ZDTP
tribofilm has been p... | physics.class-ph | previous studies have shown that the elastic properties of zinc dialkyldithiophosphate zdtp tribofilms measured by nanoindentation increase versus applied pressure anvil effect 1 2 the aim of this paper is to demonstrate that up to 8 gpa this increase is a reversible phenomenon a zdtp tribofilm has been produced on ais... | [['previous', 'studies', 'have', 'shown', 'that', 'the', 'elastic', 'properties', 'of', 'zinc', 'dialkyldithiophosphate', 'zdtp', 'tribofilms', 'measured', 'by', 'nanoindentation', 'increase', 'versus', 'applied', 'pressure', 'anvil', 'effect', '1', '2', 'the', 'aim', 'of', 'this', 'paper', 'is', 'to', 'demonstrate', '... | [-0.07130846906729421, 0.13564645879885215, -0.1086997988851306, -0.025188048041152385, -0.022524863615364373, -0.06802791222918801, 0.06838609272137307, 0.4213762005824529, -0.2374173707578298, -0.3127868594978183, 0.08795794348572632, -0.31368933378127656, -0.09703082328628816, 0.1821105172578803, -0.0493713234255681... |
706.4236 | t-J model then and now: A personal perspective from the pioneering times | In this overview I sketch briefly the path to the so-called {\em t-J model}
derived for the first time 30 years ago and provide its original meaning within
the theory of strongly correlated magnetic metals with a non-Fermi (non-Landau)
liquid ground state. An emergence of the concept of {\em real space pairing},
is d... | cond-mat.str-el | in this overview i sketch briefly the path to the socalled em tj model derived for the first time 30 years ago and provide its original meaning within the theory of strongly correlated magnetic metals with a nonfermi nonlandau liquid ground state an emergence of the concept of em real space pairing is discussed in a hi... | [['in', 'this', 'overview', 'i', 'sketch', 'briefly', 'the', 'path', 'to', 'the', 'socalled', 'em', 'tj', 'model', 'derived', 'for', 'the', 'first', 'time', '30', 'years', 'ago', 'and', 'provide', 'its', 'original', 'meaning', 'within', 'the', 'theory', 'of', 'strongly', 'correlated', 'magnetic', 'metals', 'with', 'a',... | [-0.10594856649637223, 0.1570299487830198, -0.09474213745677844, 0.12523716067575152, -0.08970724025508389, -0.12614666743203998, 0.04259330162894912, 0.3268696088064462, -0.2634976903535426, -0.26963790625333783, 0.07967826415784657, -0.25900360053870825, -0.16765404734760522, 0.15952411938924344, -0.0699056027107872,... |
706.4237 | On-sky observations with an achromatic hybrid phase knife coronagraph in
the visible | CONTEXT: The four-quadrant phase mask stellar coronagraph, introduced by D.
Rouan et al., is capable of achieving very high dynamical range imaging and was
studied in the context of the direct detection of extra-solar planets.
Achromatic four-quadrant phase mask is currently being developed for broadband
IR applicati... | astro-ph | context the fourquadrant phase mask stellar coronagraph introduced by d rouan et al is capable of achieving very high dynamical range imaging and was studied in the context of the direct detection of extrasolar planets achromatic fourquadrant phase mask is currently being developed for broadband ir applications aims we... | [['context', 'the', 'fourquadrant', 'phase', 'mask', 'stellar', 'coronagraph', 'introduced', 'by', 'd', 'rouan', 'et', 'al', 'is', 'capable', 'of', 'achieving', 'very', 'high', 'dynamical', 'range', 'imaging', 'and', 'was', 'studied', 'in', 'the', 'context', 'of', 'the', 'direct', 'detection', 'of', 'extrasolar', 'plan... | [-0.10494050901647119, 0.07532970728940967, -0.10509256089858232, 0.02984600525768349, -0.1038560004902376, -0.14405114987160372, 0.016752888190804078, 0.4501837453341739, -0.17154520210302013, -0.3740981584614053, 0.1647787995189478, -0.21119928232986818, -0.1856667936336309, 0.24763200750928074, -0.1319358929005616, ... |
706.4238 | Immediate Calculation of some Poisson Type Integrals Using
Supermathematics Circular Ex-Centric Functions | This article presents two methods, in parallel, of solving more complex
integrals, among which is the Poisson's integral, in order to emphasize the
obvious advantages of a new method of integration, which uses the
supermathematics circular ex-centric functions.
| math.GM | this article presents two methods in parallel of solving more complex integrals among which is the poissons integral in order to emphasize the obvious advantages of a new method of integration which uses the supermathematics circular excentric functions | [['this', 'article', 'presents', 'two', 'methods', 'in', 'parallel', 'of', 'solving', 'more', 'complex', 'integrals', 'among', 'which', 'is', 'the', 'poissons', 'integral', 'in', 'order', 'to', 'emphasize', 'the', 'obvious', 'advantages', 'of', 'a', 'new', 'method', 'of', 'integration', 'which', 'uses', 'the', 'superma... | [-0.1540666521193359, -0.011004253617815069, -0.12969676549294712, 0.031331164611352456, -0.13560280755061555, -0.09095577335589237, -0.02373752208124544, 0.3755866912118084, -0.2790667818406144, -0.27246426901704557, 0.044536540781877736, -0.23113321825056463, -0.20679112342563835, 0.24624289798776847, -0.039488947295... |
706.4239 | Quantum Unique Ergodicity for Eisenstein Series on the Hilbert Modular
Group over a Totally Real Field | W. Luo and P. Sarnak have proved the quantum unique ergodicity property for
Eisenstein series on $\rm{PSL}(2,\mathbb{Z}) \backslash H$. We extend their
result to Eisenstein series on $\rm{PSL}(2,O) \backslash H^n$, where $O$ is the
ring of integers in a totally real field of degree $n$ over $Q$ with narrow
class numb... | math.NT | w luo and p sarnak have proved the quantum unique ergodicity property for eisenstein series on rmpsl2mathbbz backslash h we extend their result to eisenstein series on rmpsl2o backslash hn where o is the ring of integers in a totally real field of degree n over q with narrow class number one using the eisenstein series... | [['w', 'luo', 'and', 'p', 'sarnak', 'have', 'proved', 'the', 'quantum', 'unique', 'ergodicity', 'property', 'for', 'eisenstein', 'series', 'on', 'rmpsl2mathbbz', 'backslash', 'h', 'we', 'extend', 'their', 'result', 'to', 'eisenstein', 'series', 'on', 'rmpsl2o', 'backslash', 'hn', 'where', 'o', 'is', 'the', 'ring', 'of'... | [-0.21882370524729292, 0.05352846113518656, -0.098878939760228, -0.0014754113291079798, -0.08247923012822866, -0.1527154141354064, -0.01038757749988387, 0.3061818875124057, -0.29756700426340105, -0.18004009480277697, 0.031309120215009895, -0.2752065856382251, -0.14185421355379124, 0.23175577639291683, -0.09977431830018... |
706.424 | High-temperature excess current and quantum suppression of electronic
backscattering in a 1-D system | We consider the electronic current through a one-dimensional conductor in the
ballistic transport regime and show that the quantum oscillations of a weakly
pinned single scattering target results in a temperature- and bias-voltage
independent excess current at large bias voltages. This is a genuine effect on
transpor... | cond-mat.mes-hall | we consider the electronic current through a onedimensional conductor in the ballistic transport regime and show that the quantum oscillations of a weakly pinned single scattering target results in a temperature and biasvoltage independent excess current at large bias voltages this is a genuine effect on transport that... | [['we', 'consider', 'the', 'electronic', 'current', 'through', 'a', 'onedimensional', 'conductor', 'in', 'the', 'ballistic', 'transport', 'regime', 'and', 'show', 'that', 'the', 'quantum', 'oscillations', 'of', 'a', 'weakly', 'pinned', 'single', 'scattering', 'target', 'results', 'in', 'a', 'temperature', 'and', 'biasv... | [-0.15428591739544842, 0.20066164119975355, -0.0534665494371232, 0.030100368362924096, 0.019137207164382893, -0.13309217742082816, 0.0988060922794546, 0.3449091271015135, -0.29673220897555774, -0.2444957790612276, 0.01824470062522178, -0.3195730644469777, -0.1235549744278034, 0.19625931983840064, 0.009487044330395706, ... |
706.4241 | The role of thermal pressure in jet launching | I present and discuss a unified scheme for jet launching that is based on
stochastic dissipation of the accretion disk kinetic energy, mainly via shock
waves. In this scheme, termed thermally-launched jet model, the kinetic energy
of the accreted mass is transferred to internal energy, e.g., heat or magnetic
energy. ... | astro-ph | i present and discuss a unified scheme for jet launching that is based on stochastic dissipation of the accretion disk kinetic energy mainly via shock waves in this scheme termed thermallylaunched jet model the kinetic energy of the accreted mass is transferred to internal energy eg heat or magnetic energy the internal... | [['i', 'present', 'and', 'discuss', 'a', 'unified', 'scheme', 'for', 'jet', 'launching', 'that', 'is', 'based', 'on', 'stochastic', 'dissipation', 'of', 'the', 'accretion', 'disk', 'kinetic', 'energy', 'mainly', 'via', 'shock', 'waves', 'in', 'this', 'scheme', 'termed', 'thermallylaunched', 'jet', 'model', 'the', 'kine... | [-0.12594671445959904, 0.2003630715338752, -0.035747113942097015, 0.12141609160893588, -0.12377646300368585, -0.06908737680015083, 0.011853647525780477, 0.357111590108476, -0.22573575582011984, -0.3314939345030162, 0.033885669973619185, -0.22867544028215492, 0.031965257305926524, 0.21338487567696482, -0.001475860588610... |
706.4242 | An application of transverse-momentum-dependent evolution equations in
QCD | The properties and behaviour of the solutions of the recently obtained
$k_t$-dependent evolution equations are investigated. When used to reproduce
transverse momentum spectra of hadrons in Semi-Inclusive DIS, an encouraging
agreement with data is found. The present analysis also supports at the
phenomenological leve... | hep-ph | the properties and behaviour of the solutions of the recently obtained k_tdependent evolution equations are investigated when used to reproduce transverse momentum spectra of hadrons in semiinclusive dis an encouraging agreement with data is found the present analysis also supports at the phenomenological level the fac... | [['the', 'properties', 'and', 'behaviour', 'of', 'the', 'solutions', 'of', 'the', 'recently', 'obtained', 'k_tdependent', 'evolution', 'equations', 'are', 'investigated', 'when', 'used', 'to', 'reproduce', 'transverse', 'momentum', 'spectra', 'of', 'hadrons', 'in', 'semiinclusive', 'dis', 'an', 'encouraging', 'agreemen... | [-0.05153861152264627, 0.09242876447873034, -0.16458971818666096, 0.13576781272759958, -0.025779159037747246, 0.00065798736244872, -0.07564663619437403, 0.34230397873814555, -0.19073635337037453, -0.2428123030703569, 0.020247404703168548, -0.3420143786115923, -0.06273812420661579, 0.19142532273047214, 0.052042494055585... |
706.4243 | Massless Wave States of Two-Fermion Systems | It is known that in the ladder approximation the relativistic two-fermion
bound-state equation of Bethe and Salpeter has solutions corresponding to the
binding energy equal to the total mass of the particles. The study of these
massless states has been carried out only for the bound system at rest. Of
course, such co... | hep-th | it is known that in the ladder approximation the relativistic twofermion boundstate equation of bethe and salpeter has solutions corresponding to the binding energy equal to the total mass of the particles the study of these massless states has been carried out only for the bound system at rest of course such composite... | [['it', 'is', 'known', 'that', 'in', 'the', 'ladder', 'approximation', 'the', 'relativistic', 'twofermion', 'boundstate', 'equation', 'of', 'bethe', 'and', 'salpeter', 'has', 'solutions', 'corresponding', 'to', 'the', 'binding', 'energy', 'equal', 'to', 'the', 'total', 'mass', 'of', 'the', 'particles', 'the', 'study', ... | [-0.1388776618166871, 0.21625943002519696, -0.09069913657580878, 0.09561954530654475, -0.04963294011984198, -0.12336237391323916, 0.008035419606381938, 0.334800207774554, -0.2120004238560796, -0.29365767667158726, 0.030952321909301514, -0.2948021787440493, -0.046285424144783364, 0.15193591258832298, 0.08886666537839033... |
706.4244 | Behind Pvlas | We offer a detailed review of the physics behind the PVLAS experiment. We
also address some laboratory and astrophysical cross-checks for the recent
claim concerning a signal consistent with an Axion-Like Particle. Our aim is
that the leading role played by Emilio (Mimmo) Zavattini in this field of
research will beco... | hep-ph | we offer a detailed review of the physics behind the pvlas experiment we also address some laboratory and astrophysical crosschecks for the recent claim concerning a signal consistent with an axionlike particle our aim is that the leading role played by emilio mimmo zavattini in this field of research will become appar... | [['we', 'offer', 'a', 'detailed', 'review', 'of', 'the', 'physics', 'behind', 'the', 'pvlas', 'experiment', 'we', 'also', 'address', 'some', 'laboratory', 'and', 'astrophysical', 'crosschecks', 'for', 'the', 'recent', 'claim', 'concerning', 'a', 'signal', 'consistent', 'with', 'an', 'axionlike', 'particle', 'our', 'aim... | [-0.09448732377961278, 0.1482097943246481, -0.12671775301918387, 0.10475163334980607, -0.12325090704485774, -0.06856523146852851, 0.015493242386728525, 0.33337121706455947, -0.16387422680854796, -0.3267054582759738, 0.09897933828411624, -0.2800695788860321, -0.14331809194758535, 0.2434581317869015, -0.04340270139276981... |
706.4245 | Conformal Invariance = Finiteness and Beta Deformed N=4 SYM Theory | We claim that if by a choice of the couplings the theory can be made
conformally invariant (vanishing of the beta functions) it is automatically
finite and vice versa. This is demonstrated by explicit example in
supersymmetric gauge theory. The formalism is then applied to the beta deformed
${\cal N}=4$ SYM theory an... | hep-th | we claim that if by a choice of the couplings the theory can be made conformally invariant vanishing of the beta functions it is automatically finite and vice versa this is demonstrated by explicit example in supersymmetric gauge theory the formalism is then applied to the beta deformed cal n4 sym theory and it is show... | [['we', 'claim', 'that', 'if', 'by', 'a', 'choice', 'of', 'the', 'couplings', 'the', 'theory', 'can', 'be', 'made', 'conformally', 'invariant', 'vanishing', 'of', 'the', 'beta', 'functions', 'it', 'is', 'automatically', 'finite', 'and', 'vice', 'versa', 'this', 'is', 'demonstrated', 'by', 'explicit', 'example', 'in', '... | [-0.09257940768374182, 0.23430537102588764, -0.10496701756104206, 0.09958624499429586, -0.08126442522431414, -0.1746683184044539, -0.040093518119344175, 0.35486982863706845, -0.22433204920445052, -0.22637652529131932, 0.09319294173716723, -0.23428445972967893, -0.22525084049751362, 0.1174056802281282, -0.05150081803246... |
706.4246 | High-Speed Optical Spectroscopy | The large surveys and sensitive instruments of modern astronomy are turning
ever more examples of variable objects, many of which are extending the
parameter space to testing theories of stellar evolution and accretion. Future
projects such as the Laser Interferometer Space Antenna (LISA) and the Large
Synoptic Surve... | astro-ph | the large surveys and sensitive instruments of modern astronomy are turning ever more examples of variable objects many of which are extending the parameter space to testing theories of stellar evolution and accretion future projects such as the laser interferometer space antenna lisa and the large synoptic survey tele... | [['the', 'large', 'surveys', 'and', 'sensitive', 'instruments', 'of', 'modern', 'astronomy', 'are', 'turning', 'ever', 'more', 'examples', 'of', 'variable', 'objects', 'many', 'of', 'which', 'are', 'extending', 'the', 'parameter', 'space', 'to', 'testing', 'theories', 'of', 'stellar', 'evolution', 'and', 'accretion', '... | [-0.08763958114422306, 0.12892337192157757, -0.05564670509390407, 0.08774020266423191, -0.17266220402098814, -0.13434377142624787, -0.0033204248273682037, 0.397322529548053, -0.2305019768744202, -0.3926210687140603, 0.15817156346550337, -0.3019355738188251, -0.14610412103613302, 0.30797317052670453, -0.0622432435669352... |
706.4247 | Subgroup separability in residually free groups | We prove that the finitely presentable subgroups of residually free groups
are separable and that the subgroups of type $\mathrm{FP}_\infty$ are virtual
retracts. We describe a uniform solution to the membership problem for finitely
presentable subgroups of residually free groups.
| math.GR | we prove that the finitely presentable subgroups of residually free groups are separable and that the subgroups of type mathrmfp_infty are virtual retracts we describe a uniform solution to the membership problem for finitely presentable subgroups of residually free groups | [['we', 'prove', 'that', 'the', 'finitely', 'presentable', 'subgroups', 'of', 'residually', 'free', 'groups', 'are', 'separable', 'and', 'that', 'the', 'subgroups', 'of', 'type', 'mathrmfp_infty', 'are', 'virtual', 'retracts', 'we', 'describe', 'a', 'uniform', 'solution', 'to', 'the', 'membership', 'problem', 'for', 'f... | [-0.14896555192386493, 0.195763620094229, -0.11585102760447906, 0.127175506681968, -0.1253753169797934, -0.12643999805769476, 0.016504677920005262, 0.49157974391411513, -0.41941901907706874, -0.16165678571455944, 0.10258587065319984, -0.2673407781105011, 0.02193678051042251, 0.2688655306895574, -0.23018351475445506, -0... |
706.4248 | Gap Formation in the Dust Layer of 3D Protoplanetary Disks | We numerically model the evolution of dust in a protoplanetary disk using a
two-phase (gas+dust) Smoothed Particle Hydrodynamics (SPH) code, which is
non-self-gravitating and locally isothermal. The code follows the three
dimensional distribution of dust in a protoplanetary disk as it interacts with
the gas via aerod... | astro-ph | we numerically model the evolution of dust in a protoplanetary disk using a twophase gasdust smoothed particle hydrodynamics sph code which is nonselfgravitating and locally isothermal the code follows the three dimensional distribution of dust in a protoplanetary disk as it interacts with the gas via aerodynamic drag ... | [['we', 'numerically', 'model', 'the', 'evolution', 'of', 'dust', 'in', 'a', 'protoplanetary', 'disk', 'using', 'a', 'twophase', 'gasdust', 'smoothed', 'particle', 'hydrodynamics', 'sph', 'code', 'which', 'is', 'nonselfgravitating', 'and', 'locally', 'isothermal', 'the', 'code', 'follows', 'the', 'three', 'dimensional'... | [-0.08039673659484833, 0.14261883964147679, -0.06453824869708115, 0.06024991275949611, -0.042580896778446106, -0.04343641850683424, -0.015664880680334236, 0.3758909638153596, -0.22587662372531161, -0.3325219033948249, 0.07519897798128013, -0.2199959670338366, -0.059781392245656914, 0.1573238673304311, -0.05924227319256... |
706.4249 | Solution of the Unanimity Rule on exponential, uniform and scalefree
networks: A simple model for biodiversity collapse in foodwebs | We solve the Unanimity Rule on networks with exponential, uniform and
scalefree degree distributions. In particular we arrive at equations relating
the asymptotic number of nodes in one of two states to the initial fraction of
nodes in this state. The solutions for exponential and uniform networks are
exact, the appr... | physics.bio-ph q-bio.PE | we solve the unanimity rule on networks with exponential uniform and scalefree degree distributions in particular we arrive at equations relating the asymptotic number of nodes in one of two states to the initial fraction of nodes in this state the solutions for exponential and uniform networks are exact the approximat... | [['we', 'solve', 'the', 'unanimity', 'rule', 'on', 'networks', 'with', 'exponential', 'uniform', 'and', 'scalefree', 'degree', 'distributions', 'in', 'particular', 'we', 'arrive', 'at', 'equations', 'relating', 'the', 'asymptotic', 'number', 'of', 'nodes', 'in', 'one', 'of', 'two', 'states', 'to', 'the', 'initial', 'fr... | [-0.12855051914889332, 0.0656391989431484, -0.08888078568527986, 0.0715024804385313, -0.028438538156317927, -0.11768165720725614, 0.0790948309864544, 0.3621446983146984, -0.22359000406005478, -0.29596480589145713, 0.08947557559344027, -0.29450362372488725, -0.1201344059076597, 0.16290600378420697, -0.020253094770343958... |
706.425 | n alpha Resonating-Group Calculation with a Quark-Model G-Matrix NN
Interaction | We calculate n alpha phase-shifts and scattering observables in the
resonating-group method, using the nuclear-matter G-matrix of an SU_6
quark-model NN interaction. The G-matrix is generated in the recent
energy-independent procedure of the quark-model NN interaction with the
continuous prescription for intermediate... | nucl-th | we calculate n alpha phaseshifts and scattering observables in the resonatinggroup method using the nuclearmatter gmatrix of an su_6 quarkmodel nn interaction the gmatrix is generated in the recent energyindependent procedure of the quarkmodel nn interaction with the continuous prescription for intermediate spectra by ... | [['we', 'calculate', 'n', 'alpha', 'phaseshifts', 'and', 'scattering', 'observables', 'in', 'the', 'resonatinggroup', 'method', 'using', 'the', 'nuclearmatter', 'gmatrix', 'of', 'an', 'su_6', 'quarkmodel', 'nn', 'interaction', 'the', 'gmatrix', 'is', 'generated', 'in', 'the', 'recent', 'energyindependent', 'procedure',... | [-0.15721978836241493, 0.17224005211599633, -0.10285494894116397, 0.11328059966687365, 0.001415726691598724, -0.119241612280599, -0.015993569636191786, 0.3615858868061582, -0.21549036280691988, -0.2790050564985151, -0.1113339686434876, -0.3195441770767279, -0.0759143742084206, 0.1117057762754384, 0.14827667357845722, 0... |
706.4251 | Gradient expansion approach to multiple-band Fermi liquids | Promoted by the recent progress of Berry phase physics in spin
galvanomagnetic communities, we develop a systematic derivation of the reduced
Keldysh equation (RKE) which captures the low-energy dynamics of
quasi-particles constrained within doubly degenerate bands forming a single
Fermi surface. Specifically, we pro... | cond-mat.str-el cond-mat.mes-hall | promoted by the recent progress of berry phase physics in spin galvanomagnetic communities we develop a systematic derivation of the reduced keldysh equation rke which captures the lowenergy dynamics of quasiparticles constrained within doubly degenerate bands forming a single fermi surface specifically we project out ... | [['promoted', 'by', 'the', 'recent', 'progress', 'of', 'berry', 'phase', 'physics', 'in', 'spin', 'galvanomagnetic', 'communities', 'we', 'develop', 'a', 'systematic', 'derivation', 'of', 'the', 'reduced', 'keldysh', 'equation', 'rke', 'which', 'captures', 'the', 'lowenergy', 'dynamics', 'of', 'quasiparticles', 'constr... | [-0.18351789595777387, 0.19547658960918607, -0.10977683881316586, 0.05965889539141711, -0.0302538918918586, -0.10292955441964131, 0.07966321949985482, 0.31467534175461476, -0.2802766813804303, -0.258224890558972, -0.0005219290064446426, -0.30238274060323966, -0.13716377328026216, 0.1088671162724495, 0.03875608942660226... |
706.4252 | Mach cones in Heavy Ion Collisions | MACE, a model for the propagation of mach cones in the velocity field of
heavy ion collisions (as created by hydrodynamical models) is explained. It is
tested on an analytical test case (static medium) and applied to velocity
fields created by the Particle-in-Cell model from LHC and RHIC initial
conditions.
| nucl-th | mace a model for the propagation of mach cones in the velocity field of heavy ion collisions as created by hydrodynamical models is explained it is tested on an analytical test case static medium and applied to velocity fields created by the particleincell model from lhc and rhic initial conditions | [['mace', 'a', 'model', 'for', 'the', 'propagation', 'of', 'mach', 'cones', 'in', 'the', 'velocity', 'field', 'of', 'heavy', 'ion', 'collisions', 'as', 'created', 'by', 'hydrodynamical', 'models', 'is', 'explained', 'it', 'is', 'tested', 'on', 'an', 'analytical', 'test', 'case', 'static', 'medium', 'and', 'applied', 't... | [-0.08440527610480786, 0.19211018159316154, -0.1365423958003521, 0.10171192972455173, 0.014712328505702317, -0.1284266025852412, -0.08722213835455478, 0.3753278425335884, -0.2250522879138589, -0.297558329552412, 0.008121093071531504, -0.23034910339862108, 0.04593918074853718, 0.21653424714691938, 0.06857050670310855, 0... |
706.4253 | Exact ground state density functional theory for impurity models coupled
to external reservoirs and transport calculations | A method is presented, which employs the density matrix renormalization group
technique in order to construct exact ground state exchange correlation
functionals for models of correlated electron systems coupled to external
reservoirs. The technique is applied to the M-site resonant level model. We
calculate its exac... | cond-mat.mes-hall cond-mat.str-el | a method is presented which employs the density matrix renormalization group technique in order to construct exact ground state exchange correlation functionals for models of correlated electron systems coupled to external reservoirs the technique is applied to the msite resonant level model we calculate its exact kubo... | [['a', 'method', 'is', 'presented', 'which', 'employs', 'the', 'density', 'matrix', 'renormalization', 'group', 'technique', 'in', 'order', 'to', 'construct', 'exact', 'ground', 'state', 'exchange', 'correlation', 'functionals', 'for', 'models', 'of', 'correlated', 'electron', 'systems', 'coupled', 'to', 'external', 'r... | [-0.0978300598975046, 0.11689911905876142, -0.12458084399918182, 0.11619353385082752, 0.007525456131704702, -0.14042615395151828, 0.07090460664933335, 0.37802540827792563, -0.23909709319447311, -0.32134568588745677, 0.010493974238102818, -0.33564056507343015, -0.11281908722281855, 0.15371932444224587, 0.036472625478839... |
706.4254 | X-ray Tail in NGC 7619 | We present new observational results of NGC 7619, an elliptical galaxy with a
prominent X-ray tail and a dominant member of the Pegasus group. With Chandra
and XMM-Newton observations, we confirm the presence of a long X-ray tail in
the SW direction; moreover, we identify for the first time a sharp
discontinuity of t... | astro-ph | we present new observational results of ngc 7619 an elliptical galaxy with a prominent xray tail and a dominant member of the pegasus group with chandra and xmmnewton observations we confirm the presence of a long xray tail in the sw direction moreover we identify for the first time a sharp discontinuity of the xray su... | [['we', 'present', 'new', 'observational', 'results', 'of', 'ngc', '7619', 'an', 'elliptical', 'galaxy', 'with', 'a', 'prominent', 'xray', 'tail', 'and', 'a', 'dominant', 'member', 'of', 'the', 'pegasus', 'group', 'with', 'chandra', 'and', 'xmmnewton', 'observations', 'we', 'confirm', 'the', 'presence', 'of', 'a', 'lon... | [-0.08912837097236916, 0.07409938145672659, -0.1195222501912471, 0.04588153092237898, -0.09092258054557431, -0.029252463318218434, 0.02059489818937547, 0.41850204659900087, -0.20573146292835776, -0.2905575239151565, 0.06565071081123339, -0.3123761289682107, -0.021835760575090415, 0.1608473281742447, -0.0016686076648192... |
706.4255 | Quantum key distribution over 25 km with an all-fiber
continuous-variable system | We report on the implementation of a reverse-reconciliated coherent-state
continuous-variable quantum key distribution system, with which we generated
secret keys at a rate of more than 2 kb/s over 25 km of optical fiber. Time
multiplexing is used to transmit both the signal and phase reference in the
same optical fi... | quant-ph | we report on the implementation of a reversereconciliated coherentstate continuousvariable quantum key distribution system with which we generated secret keys at a rate of more than 2 kbs over 25 km of optical fiber time multiplexing is used to transmit both the signal and phase reference in the same optical fiber our ... | [['we', 'report', 'on', 'the', 'implementation', 'of', 'a', 'reversereconciliated', 'coherentstate', 'continuousvariable', 'quantum', 'key', 'distribution', 'system', 'with', 'which', 'we', 'generated', 'secret', 'keys', 'at', 'a', 'rate', 'of', 'more', 'than', '2', 'kbs', 'over', '25', 'km', 'of', 'optical', 'fiber', ... | [-0.20811872790354868, 0.06653377277213206, -0.07977671570857459, 0.011895112831283498, 0.03208183234465527, -0.23978958368577338, 0.08353002181414652, 0.4230314656448217, -0.23977793921015145, -0.26416669928549247, 0.1191925485589668, -0.2142131004344534, -0.08144450618850964, 0.3008970720291046, -0.08131034562456203,... |
706.4256 | Double-gap superconducting proximity effect in nanotubes | We theoretically explore the possibility of a superconducting proximity
effect in single-walled metallic carbon nanotubes due to the presence of a
superconducting substrate. An unconventional double-gap situation can arise in
the two bands for nanotubes of large radius wherein the tunneling is (almost)
symmetric in t... | cond-mat.str-el cond-mat.supr-con | we theoretically explore the possibility of a superconducting proximity effect in singlewalled metallic carbon nanotubes due to the presence of a superconducting substrate an unconventional doublegap situation can arise in the two bands for nanotubes of large radius wherein the tunneling is almost symmetric in the two ... | [['we', 'theoretically', 'explore', 'the', 'possibility', 'of', 'a', 'superconducting', 'proximity', 'effect', 'in', 'singlewalled', 'metallic', 'carbon', 'nanotubes', 'due', 'to', 'the', 'presence', 'of', 'a', 'superconducting', 'substrate', 'an', 'unconventional', 'doublegap', 'situation', 'can', 'arise', 'in', 'the'... | [-0.21396830489292093, 0.18071431913122069, -0.01591237159980902, 0.0569594373309013, -0.009364888199564556, -0.1500830985524732, 0.12191821095412192, 0.42174401840438014, -0.2464686125030984, -0.26355337818031727, -0.01390187498688212, -0.2940151079335129, -0.13930964546035166, 0.13763647143445584, 0.00311619509618891... |
706.4257 | Isoperimetric profile and random walks on locally compact solvable
groups | We study a large class of amenable locally compact groups containing all
solvable algebraic groups over a local field and their discrete subgroups. We
show that the isoperimetric profile of these groups is in some sense optimal
among amenable groups. We use this fact to compute the probability of return of
symmetric ... | math.GR math.MG | we study a large class of amenable locally compact groups containing all solvable algebraic groups over a local field and their discrete subgroups we show that the isoperimetric profile of these groups is in some sense optimal among amenable groups we use this fact to compute the probability of return of symmetric rand... | [['we', 'study', 'a', 'large', 'class', 'of', 'amenable', 'locally', 'compact', 'groups', 'containing', 'all', 'solvable', 'algebraic', 'groups', 'over', 'a', 'local', 'field', 'and', 'their', 'discrete', 'subgroups', 'we', 'show', 'that', 'the', 'isoperimetric', 'profile', 'of', 'these', 'groups', 'is', 'in', 'some', ... | [-0.14284301188472712, 0.12368364187455932, -0.10858574899202081, 0.10221900079976505, -0.11876114752655192, -0.11789582710398334, 0.05417386420123594, 0.4482682614888943, -0.3207182361331152, -0.2591897282408367, 0.1627787165294572, -0.22146067492873736, -0.14569873117487614, 0.22669372315728434, -0.10149119514971972,... |
706.4258 | Characterization of two-dimensional fermionic insulating states | Inspired by the duality picture between superconductivity and insulator in
two spatial dimension, we conjecture that the order parameter, suitable for
characterizing 2D fermionic insulating state, is the disorder operator, usually
known in the context of statistical transformation. Namely, the change of the
phase of ... | cond-mat.str-el cond-mat.stat-mech | inspired by the duality picture between superconductivity and insulator in two spatial dimension we conjecture that the order parameter suitable for characterizing 2d fermionic insulating state is the disorder operator usually known in the context of statistical transformation namely the change of the phase of the diso... | [['inspired', 'by', 'the', 'duality', 'picture', 'between', 'superconductivity', 'and', 'insulator', 'in', 'two', 'spatial', 'dimension', 'we', 'conjecture', 'that', 'the', 'order', 'parameter', 'suitable', 'for', 'characterizing', '2d', 'fermionic', 'insulating', 'state', 'is', 'the', 'disorder', 'operator', 'usually'... | [-0.143448708508744, 0.1865112100179856, -0.07107429906735244, 0.06836860991508967, -0.04697744478588577, -0.16506141805834132, 0.04947522762301729, 0.3398434814760677, -0.24790398296361893, -0.2387891959483225, 0.0674721882906719, -0.2757568217003156, -0.1501013982640907, 0.11499539921680306, -0.010109841919518145, 0.... |
706.4259 | Quiver Gauge Theory and Conformality at the TeV Scale | This review describes the conformality approach to extending the standard
model of particle phenomenology using an assumption of no conformal anomaly at
high energy. Topics include quiver gauge theory, the conformality approach to
phenomenology, strong-electroweak unification at 4 TeV, cancellation of
quadratic diver... | hep-ph astro-ph gr-qc hep-th | this review describes the conformality approach to extending the standard model of particle phenomenology using an assumption of no conformal anomaly at high energy topics include quiver gauge theory the conformality approach to phenomenology strongelectroweak unification at 4 tev cancellation of quadratic divergences ... | [['this', 'review', 'describes', 'the', 'conformality', 'approach', 'to', 'extending', 'the', 'standard', 'model', 'of', 'particle', 'phenomenology', 'using', 'an', 'assumption', 'of', 'no', 'conformal', 'anomaly', 'at', 'high', 'energy', 'topics', 'include', 'quiver', 'gauge', 'theory', 'the', 'conformality', 'approac... | [-0.13786860017213398, 0.1625274061340091, -0.12579004375080471, 0.17186481954055266, -0.1423010028934536, -0.1814326695076978, -0.01834018803604592, 0.28637776892775524, -0.217744304995554, -0.37117491114454776, 0.029535671615471635, -0.2893516239710152, -0.1250997049948917, 0.028674004431545306, -0.02637473957684751,... |
706.426 | Ultracold Bose gases in time-dependent 1D superlattices: response and
quasimomentum structure | The response of ultracold atomic Bose gases in time-dependent optical
lattices is discussed based on direct simulations of the time-evolution of the
many-body state in the framework of the Bose-Hubbard model. We focus on
small-amplitude modulations of the lattice potential as implemented in several
recent experiment ... | cond-mat.stat-mech | the response of ultracold atomic bose gases in timedependent optical lattices is discussed based on direct simulations of the timeevolution of the manybody state in the framework of the bosehubbard model we focus on smallamplitude modulations of the lattice potential as implemented in several recent experiment and stud... | [['the', 'response', 'of', 'ultracold', 'atomic', 'bose', 'gases', 'in', 'timedependent', 'optical', 'lattices', 'is', 'discussed', 'based', 'on', 'direct', 'simulations', 'of', 'the', 'timeevolution', 'of', 'the', 'manybody', 'state', 'in', 'the', 'framework', 'of', 'the', 'bosehubbard', 'model', 'we', 'focus', 'on', ... | [-0.17935654326469044, 0.14683677061376246, -0.08461692054247992, 0.05419933487110856, 0.03116952045397325, -0.07496401662514969, 0.055217118527401576, 0.3911932993680239, -0.24973863459784876, -0.24239164302125574, 0.03811053490710699, -0.2627751847136427, -0.13730706362138417, 0.1692796466512267, 0.08858932894416449,... |
706.4261 | Free flux flow magneto-resistance of single crystal BSCCO | Measurement of the free flux flow resistance in monocrystalline highly
anisotropic BSCCO reveals a low field magneto-resistive effect nearly 100 times
that expected from a naive application of the Bardeen-Stephen rule R/Rn =
B/Bc2. Furthermore in the vortex solid phase it saturates to a constant value
at about Hc2/10... | cond-mat.supr-con | measurement of the free flux flow resistance in monocrystalline highly anisotropic bscco reveals a low field magnetoresistive effect nearly 100 times that expected from a naive application of the bardeenstephen rule rrn bbc2 furthermore in the vortex solid phase it saturates to a constant value at about hc2100 as if th... | [['measurement', 'of', 'the', 'free', 'flux', 'flow', 'resistance', 'in', 'monocrystalline', 'highly', 'anisotropic', 'bscco', 'reveals', 'a', 'low', 'field', 'magnetoresistive', 'effect', 'nearly', '100', 'times', 'that', 'expected', 'from', 'a', 'naive', 'application', 'of', 'the', 'bardeenstephen', 'rule', 'rrn', 'b... | [-0.15574935738030554, 0.2220801015252672, -0.053223493845522905, 0.01058204225244924, -0.05721632391214371, -0.15005599666864244, 0.09283579411762845, 0.3620444299230556, -0.24593490189990075, -0.2816193135173506, 0.07005870194045216, -0.28965889139711354, -0.0670907387212545, 0.17254947840643092, 0.00861974956248613,... |
706.4262 | The Heisenberg group and conformal field theory | A mathematical construction of the conformal field theory (CFT) associated to
a compact torus, also called the "nonlinear Sigma-model" or "lattice-CFT", is
given. Underlying this approach to CFT is a unitary modular functor, the
construction of which follows from a "Quantization commutes with reduction"-
type of theo... | math-ph math.MP | a mathematical construction of the conformal field theory cft associated to a compact torus also called the nonlinear sigmamodel or latticecft is given underlying this approach to cft is a unitary modular functor the construction of which follows from a quantization commutes with reduction type of theorem for unitary q... | [['a', 'mathematical', 'construction', 'of', 'the', 'conformal', 'field', 'theory', 'cft', 'associated', 'to', 'a', 'compact', 'torus', 'also', 'called', 'the', 'nonlinear', 'sigmamodel', 'or', 'latticecft', 'is', 'given', 'underlying', 'this', 'approach', 'to', 'cft', 'is', 'a', 'unitary', 'modular', 'functor', 'the',... | [-0.1644558787201753, 0.11139787040329316, -0.1312376098441226, 0.0829188866870633, -0.13757710136650575, -0.14846741139245706, -0.012341022573222983, 0.3043586879059495, -0.3060283132252239, -0.16585115566184477, 0.09724128664293814, -0.20165489486299476, -0.2145899341225491, 0.20057945908878796, -0.18809852914308153,... |
706.4263 | CP violation in the B0s system | In this paper the most recent Tevatron results concerning CP violation in the
B0s system are reviewed. These are the measurement of the direct CP asymmetry
in the B0s->K-\pi+ decay performed by CDF and the measurement of \Delta\Gamma_s
and \phi_s performed by D0 in the B0s->J/\psi\phi decay.
| hep-ex | in this paper the most recent tevatron results concerning cp violation in the b0s system are reviewed these are the measurement of the direct cp asymmetry in the b0skpi decay performed by cdf and the measurement of deltagamma_s and phi_s performed by d0 in the b0sjpsiphi decay | [['in', 'this', 'paper', 'the', 'most', 'recent', 'tevatron', 'results', 'concerning', 'cp', 'violation', 'in', 'the', 'b0s', 'system', 'are', 'reviewed', 'these', 'are', 'the', 'measurement', 'of', 'the', 'direct', 'cp', 'asymmetry', 'in', 'the', 'b0skpi', 'decay', 'performed', 'by', 'cdf', 'and', 'the', 'measurement'... | [-0.12768271784815524, 0.19816038878634573, -0.05232627818153964, 0.033361459903729455, 0.0019411920259396235, -0.11776096334473954, 0.08437585572246462, 0.2478395567999946, -0.23362500314962947, -0.2721659596595499, 0.07470202495654424, -0.3412164581525657, -0.0019310627339614761, 0.17185383035490912, 0.06982335721453... |
706.4264 | Upper and lower bounds for the large polaron dispersion in $D=1,2,3$
dimensions | Numerical results for the polaron dispersion are presented for an arbitrary
number of space dimensions. Upper and lower bounds are calculated for the
dispersion curves. They are rather close to each other in the cases of small
electron-phonon couplings usual for real polar materials. To describe the
dispersion in oth... | cond-mat.other | numerical results for the polaron dispersion are presented for an arbitrary number of space dimensions upper and lower bounds are calculated for the dispersion curves they are rather close to each other in the cases of small electronphonon couplings usual for real polar materials to describe the dispersion in other mat... | [['numerical', 'results', 'for', 'the', 'polaron', 'dispersion', 'are', 'presented', 'for', 'an', 'arbitrary', 'number', 'of', 'space', 'dimensions', 'upper', 'and', 'lower', 'bounds', 'are', 'calculated', 'for', 'the', 'dispersion', 'curves', 'they', 'are', 'rather', 'close', 'to', 'each', 'other', 'in', 'the', 'cases... | [-0.10919622786471392, 0.13080856719482523, -0.05050387257729106, 0.0944778649136424, -0.1145681408899171, -0.17925458128697105, 0.05759438716958524, 0.41099501823132134, -0.21597581505490354, -0.3013500000863355, 0.06439158500276734, -0.2609612956662111, -0.12157452186778644, 0.3141354704251969, 0.013275044666109036, ... |
706.4265 | ASTE Submillimeter Observations of a Young Stellar Object Condensation
in Cederblad 110 | We present results of submillimeter observations of a low-mass young stellar
objects (YSOs) condensation in the Cederblad 110 region of the Chamaeleon I
dark cloud with Atacama Submillimeter Telescope Experiment. Our HCO+(J=4-3) map
reveals a dense molecular gas with an extent of ~ 0.1 pc, which is a complex of
two e... | astro-ph | we present results of submillimeter observations of a lowmass young stellar objects ysos condensation in the cederblad 110 region of the chamaeleon i dark cloud with atacama submillimeter telescope experiment our hcoj43 map reveals a dense molecular gas with an extent of 01 pc which is a complex of two envelopes associ... | [['we', 'present', 'results', 'of', 'submillimeter', 'observations', 'of', 'a', 'lowmass', 'young', 'stellar', 'objects', 'ysos', 'condensation', 'in', 'the', 'cederblad', '110', 'region', 'of', 'the', 'chamaeleon', 'i', 'dark', 'cloud', 'with', 'atacama', 'submillimeter', 'telescope', 'experiment', 'our', 'hcoj43', 'm... | [-0.07300229151223903, 0.102621956787425, -0.028426223908172687, 0.04910786889813608, -0.0772594264104555, -0.07734818529279437, 0.011144204541051295, 0.4707859977381304, -0.13188890035962686, -0.3246036650554743, 0.07297225042420905, -0.28597290604375303, -0.005177790293237195, 0.1644787722871115, -0.02679515855597856... |
706.4266 | Fluctuating initial conditions in heavy-ion collisions from the Glauber
approach | In the framework of the Glauber approach we analyze the shape parameters of
the early-formed system and their event-by-event fluctuations. We test a
variety of models: the conventional wounded nucleon model, a model admixing
binary collisions to the wounded nucleons, a model with hot spots, as well as
the hot-spot mo... | nucl-th hep-ph nucl-ex | in the framework of the glauber approach we analyze the shape parameters of the earlyformed system and their eventbyevent fluctuations we test a variety of models the conventional wounded nucleon model a model admixing binary collisions to the wounded nucleons a model with hot spots as well as the hotspot model where t... | [['in', 'the', 'framework', 'of', 'the', 'glauber', 'approach', 'we', 'analyze', 'the', 'shape', 'parameters', 'of', 'the', 'earlyformed', 'system', 'and', 'their', 'eventbyevent', 'fluctuations', 'we', 'test', 'a', 'variety', 'of', 'models', 'the', 'conventional', 'wounded', 'nucleon', 'model', 'a', 'model', 'admixing... | [-0.08763685812483783, 0.12466646620790318, -0.12186312046747103, 0.12353208908828459, 0.00659229313713257, -0.06664227484466714, 0.0012071730504329833, 0.3376682715697421, -0.23414051793170748, -0.31110525414934037, 0.026220882376138534, -0.3214933420876386, -0.014644891266814536, 0.16928580857002762, 0.00064871167263... |
706.4267 | A mixed problem for the infinity laplacian via Tug-of-War games | In this paper we prove that a function $ u\in\mathcal{C}(\bar{\Omega})$ is
the continuous value of the Tug-of-War game described in \cite{PSSW} if and
only if it is the unique viscosity solution to the infinity laplacian with
mixed boundary conditions
{-\Delta_{\infty}u(x)=0\quad & \text{in} \Omega,
\frac{\partia... | math.AP | in this paper we prove that a function uinmathcalcbaromega is the continuous value of the tugofwar game described in citepssw if and only if it is the unique viscosity solution to the infinity laplacian with mixed boundary conditions delta_inftyux0quad textin omega fracpartial upartial nx0quad texton gamma_n uxfxquad t... | [['in', 'this', 'paper', 'we', 'prove', 'that', 'a', 'function', 'uinmathcalcbaromega', 'is', 'the', 'continuous', 'value', 'of', 'the', 'tugofwar', 'game', 'described', 'in', 'citepssw', 'if', 'and', 'only', 'if', 'it', 'is', 'the', 'unique', 'viscosity', 'solution', 'to', 'the', 'infinity', 'laplacian', 'with', 'mixe... | [-0.12315779247266405, 0.04477640237549649, -0.09938683937961126, -0.015327615459340022, -0.09871312347788583, -0.15630746035672285, -0.047605695212533806, 0.3168953855686328, -0.3672000714084681, -0.1541813546243836, 0.18217311363242678, -0.3745973753140253, -0.12949152869336744, 0.09959615638671333, -0.11059138925800... |
706.4268 | Theory of the Siegel Modular Variety | In this paper, we discuss the theory of the Siegel modular variety in the
aspects of arithmetic and geometry. This article covers the theory of Siegel
modular forms, the Hecke theory, a lifting of elliptic cusp forms, geometric
properties of the Siegel modular variety, (hypothetical) motives attached to
Siegel modula... | math.NT math.AG | in this paper we discuss the theory of the siegel modular variety in the aspects of arithmetic and geometry this article covers the theory of siegel modular forms the hecke theory a lifting of elliptic cusp forms geometric properties of the siegel modular variety hypothetical motives attached to siegel modular forms an... | [['in', 'this', 'paper', 'we', 'discuss', 'the', 'theory', 'of', 'the', 'siegel', 'modular', 'variety', 'in', 'the', 'aspects', 'of', 'arithmetic', 'and', 'geometry', 'this', 'article', 'covers', 'the', 'theory', 'of', 'siegel', 'modular', 'forms', 'the', 'hecke', 'theory', 'a', 'lifting', 'of', 'elliptic', 'cusp', 'fo... | [-0.27669396829965004, -0.0057038971069032105, -0.2343374520295568, 0.04508565078584193, -0.14182105409454995, -0.04036405639943935, -0.0585898268549561, 0.16466269607387357, -0.3980383404483229, -0.2441846065349498, 0.06274971146909994, -0.19345097540546272, -0.2883285333923364, 0.2756840636859001, -0.1681049494230646... |
706.4269 | Exploring the Di-Photon Decay of a Light Higgs Boson in the MSSM With
Explicit CP Violation | The di-photon decay channel of the lightest Higgs boson is considerd as a
probe to explore CP violation in the Minimal Supersymmetric Standard Model
(MSSM). The scalar/pseudo-scalar mixing is considered along with CP violation
entering through the Higgs-sfermion-sfermion couplings, with and without light
sparticles. ... | hep-ph | the diphoton decay channel of the lightest higgs boson is considerd as a probe to explore cp violation in the minimal supersymmetric standard model mssm the scalarpseudoscalar mixing is considered along with cp violation entering through the higgssfermionsfermion couplings with and without light sparticles the impact o... | [['the', 'diphoton', 'decay', 'channel', 'of', 'the', 'lightest', 'higgs', 'boson', 'is', 'considerd', 'as', 'a', 'probe', 'to', 'explore', 'cp', 'violation', 'in', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'mssm', 'the', 'scalarpseudoscalar', 'mixing', 'is', 'considered', 'along', 'with', 'cp', 'violati... | [-0.09825342627899612, 0.2868909629907052, -0.015634891201405467, 0.13479205170710692, -0.10160878706457359, -0.22173387169477946, 0.10709643165557449, 0.3331092008596928, -0.22952323368977473, -0.27615558736401946, 0.07736097755274508, -0.281392718508777, -0.004585486754555912, 0.14772412288707032, 0.04409552450847475... |
706.427 | Coherent Magnetization Precession in GaMnAs induced by Ultrafast Optical
Excitation | We use femtosecond optical pulses to induce, control and monitor
magnetization precession in ferromagnetic Ga0.965Mn0.035As. At temperatures
below ~40 K we observe coherent oscillations of the local Mn spins, triggered
by an ultrafast photoinduced reorientation of the in-plane easy axis. The
amplitude saturation of t... | cond-mat.mtrl-sci | we use femtosecond optical pulses to induce control and monitor magnetization precession in ferromagnetic ga0965mn0035as at temperatures below 40 k we observe coherent oscillations of the local mn spins triggered by an ultrafast photoinduced reorientation of the inplane easy axis the amplitude saturation of the oscilla... | [['we', 'use', 'femtosecond', 'optical', 'pulses', 'to', 'induce', 'control', 'and', 'monitor', 'magnetization', 'precession', 'in', 'ferromagnetic', 'ga0965mn0035as', 'at', 'temperatures', 'below', '40', 'k', 'we', 'observe', 'coherent', 'oscillations', 'of', 'the', 'local', 'mn', 'spins', 'triggered', 'by', 'an', 'ul... | [-0.2362928298816673, 0.29854051129736225, -0.031453933669744354, 0.03531784549183947, -0.08322733321080082, -0.13234771132885823, 0.08443901327340618, 0.47504181720708544, -0.29691176743883835, -0.27400474016995807, 0.002248057232875573, -0.22635718520828768, -0.051641617553602706, 0.25546248318921577, 0.0512405169784... |
706.4271 | Characteristic Time and Maximum Mixedness: Single Mode Gaussian States
in Dissipative Channels | We derive an upper limit for the mixedness of single bosonic mode gaussian
states propagating in dissipative channels. It is a function of the initial
squeezing and temperature of the channel only. Moreover the time at which von
Neumann's entropy reaches its maximum value coincides with that of complete
loss of coher... | quant-ph | we derive an upper limit for the mixedness of single bosonic mode gaussian states propagating in dissipative channels it is a function of the initial squeezing and temperature of the channel only moreover the time at which von neumanns entropy reaches its maximum value coincides with that of complete loss of coherence ... | [['we', 'derive', 'an', 'upper', 'limit', 'for', 'the', 'mixedness', 'of', 'single', 'bosonic', 'mode', 'gaussian', 'states', 'propagating', 'in', 'dissipative', 'channels', 'it', 'is', 'a', 'function', 'of', 'the', 'initial', 'squeezing', 'and', 'temperature', 'of', 'the', 'channel', 'only', 'moreover', 'the', 'time',... | [-0.16392071896412394, 0.20878017138462032, -0.12432669255710942, 0.007993858505710306, 0.02771934415132069, -0.16947382048850781, 0.1145456699621782, 0.2955344823401487, -0.27653728199616207, -0.20151025433452768, 0.07824874644600704, -0.2801683002984838, -0.03604900155608591, 0.17525976207189, -0.029622550555423163, ... |
706.4272 | On the principle of relativity and electrostatics in a flat spacetime
with a compact spatial dimension | We study a flat spacetime with a compact spatial dimension and dispute the
claim of Bansal, Laing, and Sriharan that a local experiment can determine
whether or not an inertial observer is "privileged" in this spacetime.
| gr-qc | we study a flat spacetime with a compact spatial dimension and dispute the claim of bansal laing and sriharan that a local experiment can determine whether or not an inertial observer is privileged in this spacetime | [['we', 'study', 'a', 'flat', 'spacetime', 'with', 'a', 'compact', 'spatial', 'dimension', 'and', 'dispute', 'the', 'claim', 'of', 'bansal', 'laing', 'and', 'sriharan', 'that', 'a', 'local', 'experiment', 'can', 'determine', 'whether', 'or', 'not', 'an', 'inertial', 'observer', 'is', 'privileged', 'in', 'this', 'spacet... | [-0.14546884271715368, 0.1100651575422879, -0.17093641425349881, 0.06462900063821247, -0.10731807429609554, -0.17774164800399117, 0.0027463922277092935, 0.3787457720509597, -0.21070985347032548, -0.2654311542099874, 0.09890439406236899, -0.20319131644708768, -0.12918791289973472, 0.1016785045487008, -0.1351061686341251... |
706.4273 | Drift and Diffusion of Spins Generated by the Spin Hall Effect | Electrically generated spin accumulation due to the spin Hall effect is
imaged in n-GaAs channels using Kerr rotation microscopy, focusing on its
spatial distribution and time-averaged behavior in a magnetic field.
Spatially-resolved imaging reveals that spin accumulation observed in
transverse arms develops due to l... | cond-mat.mes-hall cond-mat.mtrl-sci | electrically generated spin accumulation due to the spin hall effect is imaged in ngaas channels using kerr rotation microscopy focusing on its spatial distribution and timeaveraged behavior in a magnetic field spatiallyresolved imaging reveals that spin accumulation observed in transverse arms develops due to longitud... | [['electrically', 'generated', 'spin', 'accumulation', 'due', 'to', 'the', 'spin', 'hall', 'effect', 'is', 'imaged', 'in', 'ngaas', 'channels', 'using', 'kerr', 'rotation', 'microscopy', 'focusing', 'on', 'its', 'spatial', 'distribution', 'and', 'timeaveraged', 'behavior', 'in', 'a', 'magnetic', 'field', 'spatiallyreso... | [-0.1639627398501034, 0.17720806415309198, -0.07868148475536145, 0.03253126859490294, -0.08386190507153515, -0.10253496832447126, -0.05133162120255293, 0.39335636855103073, -0.26080665801418945, -0.29188999373000113, 0.0388021477861912, -0.27955208359635436, -0.09091757057467476, 0.21604301375336946, 0.0253414764185436... |
706.4274 | Mixing-induced global modes in open active flow | We describe how a convectively unstable active field in an open flow
configuration becomes absolutely unstable due to local mixing. A representation
of the mixing region as those with locally enhanced effective diffusion allows
us to find the linear transition point to unstable global mode analytically. We
derive the... | nlin.PS | we describe how a convectively unstable active field in an open flow configuration becomes absolutely unstable due to local mixing a representation of the mixing region as those with locally enhanced effective diffusion allows us to find the linear transition point to unstable global mode analytically we derive the cri... | [['we', 'describe', 'how', 'a', 'convectively', 'unstable', 'active', 'field', 'in', 'an', 'open', 'flow', 'configuration', 'becomes', 'absolutely', 'unstable', 'due', 'to', 'local', 'mixing', 'a', 'representation', 'of', 'the', 'mixing', 'region', 'as', 'those', 'with', 'locally', 'enhanced', 'effective', 'diffusion',... | [-0.14482994182575223, 0.19044331331130798, -0.10041963279355264, 0.07893929966603933, -0.049091268699460976, -0.1600748635356085, 0.044933466905512025, 0.3147841325380664, -0.3254500429139243, -0.20322920086429172, 0.12403833193778721, -0.24449882236080736, -0.1613367879088374, 0.1634643043330668, 0.027144497283650024... |
706.4275 | Boltzmann equation for dissipative gases in homogeneous states with
nonlinear friction | Combining analytical and numerical methods, we study within the framework of
the homogeneous non-linear Boltzmann equation, a broad class of models relevant
for the dynamics of dissipative fluids, including granular gases. We use the
new method presented in a previous paper [J. Stat. Phys. 124, 549 (2006)] and
extend... | cond-mat.stat-mech | combining analytical and numerical methods we study within the framework of the homogeneous nonlinear boltzmann equation a broad class of models relevant for the dynamics of dissipative fluids including granular gases we use the new method presented in a previous paper j stat phys 124 549 2006 and extend our results to... | [['combining', 'analytical', 'and', 'numerical', 'methods', 'we', 'study', 'within', 'the', 'framework', 'of', 'the', 'homogeneous', 'nonlinear', 'boltzmann', 'equation', 'a', 'broad', 'class', 'of', 'models', 'relevant', 'for', 'the', 'dynamics', 'of', 'dissipative', 'fluids', 'including', 'granular', 'gases', 'we', '... | [-0.09777379401873612, 0.08791396083600872, -0.10283279313263319, 0.06598015269347143, -0.04429668788996307, -0.1593754776945034, 0.020848048286981457, 0.30286994183201554, -0.2349980991797733, -0.27196434858182433, 0.038683050470624834, -0.27424517750710325, -0.13784015001993336, 0.22281064180300592, -0.02173197665251... |
706.4276 | Fermi pockets and correlation effects in underdoped YBa2Cu3O6.5 | The detection of quantum oscillations in the electrical resistivity of
YBa2Cu3O6.5 provides direct evidence for the existence of Fermi surface pockets
in an underdoped cuprate. We present a theoretical study of the electronic
structure of YBa2Cu3O7-d (YBCO) aiming at establishing the nature of these
Fermi pockets, i.... | cond-mat.str-el | the detection of quantum oscillations in the electrical resistivity of yba2cu3o65 provides direct evidence for the existence of fermi surface pockets in an underdoped cuprate we present a theoretical study of the electronic structure of yba2cu3o7d ybco aiming at establishing the nature of these fermi pockets ie cuo2 pl... | [['the', 'detection', 'of', 'quantum', 'oscillations', 'in', 'the', 'electrical', 'resistivity', 'of', 'yba2cu3o65', 'provides', 'direct', 'evidence', 'for', 'the', 'existence', 'of', 'fermi', 'surface', 'pockets', 'in', 'an', 'underdoped', 'cuprate', 'we', 'present', 'a', 'theoretical', 'study', 'of', 'the', 'electron... | [-0.2067875117617881, 0.17121946307365543, -0.049984654605699085, 0.09063375129231385, -0.06903863827964025, -0.10600838640017346, 0.10604236143297471, 0.3398577371346099, -0.24277001400367312, -0.2633162557058746, -0.02844771664517577, -0.4029553371171157, -0.10500352888733946, 0.18419446634028905, 0.07053645201432075... |
706.4277 | On the Wilsonian renormalization group equation for nuclear current
operators | We present the solution to the recently derived Wilsonian renormalization
group (RG) equation for nuclear current operators. In order to eliminate the
present ambiguity in the RG equation itself, we introduce a new condition
specifying the cutoff independence of the five point Green function
corresponding to the two-... | nucl-th | we present the solution to the recently derived wilsonian renormalization group rg equation for nuclear current operators in order to eliminate the present ambiguity in the rg equation itself we introduce a new condition specifying the cutoff independence of the five point green function corresponding to the twobody pr... | [['we', 'present', 'the', 'solution', 'to', 'the', 'recently', 'derived', 'wilsonian', 'renormalization', 'group', 'rg', 'equation', 'for', 'nuclear', 'current', 'operators', 'in', 'order', 'to', 'eliminate', 'the', 'present', 'ambiguity', 'in', 'the', 'rg', 'equation', 'itself', 'we', 'introduce', 'a', 'new', 'conditi... | [-0.12786713769455674, 0.0937840139187756, -0.15073430843185634, 0.08223536994337337, -0.14398744954378345, -0.12780542845430318, 0.04404020734291407, 0.2865194554440677, -0.2876538597047329, -0.26268280455842613, 0.07367273314448539, -0.28871795563027264, -0.12348684184253216, 0.08352904156781733, -0.03486639165785164... |
706.4278 | The minimal principals of Hermitian matrices and the negativity of
bipartite of qubit states | Quantum entanglement is an enigmatic and powerful property that has attracted
much attention due to its usefulness in new ways of communications, like
quantum teleportation and quantum key distribution. Much effort has been done
to quantify entanglement. Indeed, there exist some well-established
separability criterio... | quant-ph | quantum entanglement is an enigmatic and powerful property that has attracted much attention due to its usefulness in new ways of communications like quantum teleportation and quantum key distribution much effort has been done to quantify entanglement indeed there exist some wellestablished separability criterion and a... | [['quantum', 'entanglement', 'is', 'an', 'enigmatic', 'and', 'powerful', 'property', 'that', 'has', 'attracted', 'much', 'attention', 'due', 'to', 'its', 'usefulness', 'in', 'new', 'ways', 'of', 'communications', 'like', 'quantum', 'teleportation', 'and', 'quantum', 'key', 'distribution', 'much', 'effort', 'has', 'been... | [-0.11552004827832689, 0.11990842329025178, -0.09290377030206122, 0.07292441635069494, -0.032131370123741884, -0.18213641870177674, 0.01864120036681962, 0.35148269571458957, -0.2424462745441314, -0.2556264203669009, 0.10689076160232784, -0.3012480758871807, -0.17164918179243652, 0.15756579230026324, -0.0749625772734027... |
706.4279 | Diagonal fibrations are pointwise fibrations | On the category of bisimplicial sets there are different Quillen closed model
structures associated to various definitions of fibrations. In one of them,
which is due to Bousfield and Kan and that consists of seeing a bisimplicial
set as a simplicial object in the category of simplicial sets, fibrations are
those bis... | math.AT | on the category of bisimplicial sets there are different quillen closed model structures associated to various definitions of fibrations in one of them which is due to bousfield and kan and that consists of seeing a bisimplicial set as a simplicial object in the category of simplicial sets fibrations are those bisimpli... | [['on', 'the', 'category', 'of', 'bisimplicial', 'sets', 'there', 'are', 'different', 'quillen', 'closed', 'model', 'structures', 'associated', 'to', 'various', 'definitions', 'of', 'fibrations', 'in', 'one', 'of', 'them', 'which', 'is', 'due', 'to', 'bousfield', 'and', 'kan', 'and', 'that', 'consists', 'of', 'seeing',... | [-0.19662498110872612, 0.030486594485282376, -0.06457552844004934, 0.14299391944721146, -0.09078556235487524, -0.1492188428977929, -0.02609309421754197, 0.3819412499862282, -0.40332296957964436, -0.16346874121135394, 0.08365541921618085, -0.29237866700675924, -0.15420289925430297, 0.13088861003052443, -0.26625383464341... |
706.428 | Symmetry breaking by the sea of Dirac-Landau levels in graphene | The quantum Hall states of graphene have a filled Dirac sea of Landau levels.
The short ranged SU(4) symmetry breaking interactions can induce a staggered
polarization of the sea of Dirac-Landau levels. We study this effect in the
extended Hubbard model on a honeycomb lattice using mean field variational
wavefunction... | cond-mat.mes-hall | the quantum hall states of graphene have a filled dirac sea of landau levels the short ranged su4 symmetry breaking interactions can induce a staggered polarization of the sea of diraclandau levels we study this effect in the extended hubbard model on a honeycomb lattice using mean field variational wavefunctions we fi... | [['the', 'quantum', 'hall', 'states', 'of', 'graphene', 'have', 'a', 'filled', 'dirac', 'sea', 'of', 'landau', 'levels', 'the', 'short', 'ranged', 'su4', 'symmetry', 'breaking', 'interactions', 'can', 'induce', 'a', 'staggered', 'polarization', 'of', 'the', 'sea', 'of', 'diraclandau', 'levels', 'we', 'study', 'this', '... | [-0.20573927051771213, 0.28224352320437046, -0.05285325590452618, 0.07995283420279842, -0.006985375827507061, -0.13872181505841366, 0.0628597158829079, 0.3789536429240423, -0.2082410543663975, -0.2713053186588428, -0.007965681533438755, -0.31204502490513464, -0.12404625494690502, 0.04779538156957749, 0.0663207026088939... |
706.4281 | Riesz integral representation theory | We present a Riesz integral representation theory in which functions,
operators and measures take values in uniform commutative monoids (a
commutative monoid with a uniformity making the binary operation of the monoid
uniformly continuous). It describes the operators to which the theory can be
applied and the finitel... | math.RT | we present a riesz integral representation theory in which functions operators and measures take values in uniform commutative monoids a commutative monoid with a uniformity making the binary operation of the monoid uniformly continuous it describes the operators to which the theory can be applied and the finitelyaddit... | [['we', 'present', 'a', 'riesz', 'integral', 'representation', 'theory', 'in', 'which', 'functions', 'operators', 'and', 'measures', 'take', 'values', 'in', 'uniform', 'commutative', 'monoids', 'a', 'commutative', 'monoid', 'with', 'a', 'uniformity', 'making', 'the', 'binary', 'operation', 'of', 'the', 'monoid', 'unifo... | [-0.1293937341479028, 0.13493051209714882, -0.13834972172782461, 0.1562995305043509, -0.11244643168671556, -0.11232410061241287, -0.009480021030091249, 0.37731245331176577, -0.3732683224399097, -0.10963675717925425, 0.08595400337249086, -0.28966081364395485, -0.16868403031513457, 0.18235236747054065, -0.124717410436615... |
706.4282 | Two Gaps Make a High Temperature Superconductor? | One of the keys to the high-temperature superconductivity puzzle is the
identification of the energy scales associated with the emergence of a coherent
condensate of superconducting electron pairs. These might provide a measure of
the pairing strength and of the coherence of the superfluid, and ultimately
reveal the ... | cond-mat.supr-con cond-mat.str-el | one of the keys to the hightemperature superconductivity puzzle is the identification of the energy scales associated with the emergence of a coherent condensate of superconducting electron pairs these might provide a measure of the pairing strength and of the coherence of the superfluid and ultimately reveal the natur... | [['one', 'of', 'the', 'keys', 'to', 'the', 'hightemperature', 'superconductivity', 'puzzle', 'is', 'the', 'identification', 'of', 'the', 'energy', 'scales', 'associated', 'with', 'the', 'emergence', 'of', 'a', 'coherent', 'condensate', 'of', 'superconducting', 'electron', 'pairs', 'these', 'might', 'provide', 'a', 'mea... | [-0.23377061033572413, 0.20334075180008976, -0.0941753898330621, 0.05784176915818662, -0.0673603427906831, -0.13419247765769046, 0.13823802527979734, 0.30670658807809414, -0.2383035870040195, -0.26593723381346646, -0.01389060285260999, -0.3202036520989056, -0.06864799151866975, 0.14468337807869702, 0.03374369272639517,... |
706.4283 | Heisenberg-limited eavesdropping on the continuous-variable quantum
cryptographic protocol with no basis switching is impossible | The Gaussian quantum key distribution protocol based on coherent states and
heterodyne detection [Phys. Rev. Lett. 93, 170504 (2004)] has the advantage
that no active random basis switching is needed on the receiver's side. Its
security is, however, not very satisfyingly understood today because the bounds
on the sec... | quant-ph | the gaussian quantum key distribution protocol based on coherent states and heterodyne detection phys rev lett 93 170504 2004 has the advantage that no active random basis switching is needed on the receivers side its security is however not very satisfyingly understood today because the bounds on the secret key rate t... | [['the', 'gaussian', 'quantum', 'key', 'distribution', 'protocol', 'based', 'on', 'coherent', 'states', 'and', 'heterodyne', 'detection', 'phys', 'rev', 'lett', '93', '170504', '2004', 'has', 'the', 'advantage', 'that', 'no', 'active', 'random', 'basis', 'switching', 'is', 'needed', 'on', 'the', 'receivers', 'side', 'i... | [-0.16392920030037236, 0.06265928528054561, -0.09147640231944551, 0.029992167463647985, -0.04358997442280856, -0.23796540983978695, 0.14347202397630524, 0.36568221254883526, -0.19371741821458477, -0.29241179745365803, 0.10838654978313944, -0.2143376625064656, -0.15704034026015865, 0.2552919271853578, -0.135426641898839... |
706.4284 | Geodetic precession and frame dragging observed far from massive objects
and close to a gyroscope | Total precession (geodetic precession and frame dragging) depends on the
velocity of each source of gravitation, which means that it depends on the
choice of the coordinate system. We consider the latter as an anomaly
specifically in the Gravity Probe B experiment, we investigated it and solved
this anomaly. Thus, we... | gr-qc | total precession geodetic precession and frame dragging depends on the velocity of each source of gravitation which means that it depends on the choice of the coordinate system we consider the latter as an anomaly specifically in the gravity probe b experiment we investigated it and solved this anomaly thus we proved t... | [['total', 'precession', 'geodetic', 'precession', 'and', 'frame', 'dragging', 'depends', 'on', 'the', 'velocity', 'of', 'each', 'source', 'of', 'gravitation', 'which', 'means', 'that', 'it', 'depends', 'on', 'the', 'choice', 'of', 'the', 'coordinate', 'system', 'we', 'consider', 'the', 'latter', 'as', 'an', 'anomaly',... | [-0.1743765567386678, 0.09879319902063192, -0.07755100388390322, 0.058409451382855575, -0.11995710796366135, -0.1370125686066846, 0.015986110645656783, 0.32443523238102595, -0.2412329149742921, -0.30848702459285654, 0.09600944295991212, -0.2281507181376219, -0.11989273267487685, 0.2207140865921974, -0.06785090198119481... |
706.4285 | Decoupling of Heavy Kaluza-Klein Modes In Models With Five-Dimensional
Scalar Fields | We investigate the decoupling of heavy Kaluza-Klein modes in $\phi^{4}$
theory and scalar QED with space-time topology $\mathbb{R}^{3,1} \times S^{1}$.
We calculate the effective action due to integrating out heavy KK modes. We
construct generalized RGE's for the couplings with respect to the
compactification scale $... | hep-th | we investigate the decoupling of heavy kaluzaklein modes in phi4 theory and scalar qed with spacetime topology mathbbr31 times s1 we calculate the effective action due to integrating out heavy kk modes we construct generalized rges for the couplings with respect to the compactification scale m with the solutions to the... | [['we', 'investigate', 'the', 'decoupling', 'of', 'heavy', 'kaluzaklein', 'modes', 'in', 'phi4', 'theory', 'and', 'scalar', 'qed', 'with', 'spacetime', 'topology', 'mathbbr31', 'times', 's1', 'we', 'calculate', 'the', 'effective', 'action', 'due', 'to', 'integrating', 'out', 'heavy', 'kk', 'modes', 'we', 'construct', '... | [-0.1513764845959758, 0.24795141529770684, -0.051138016789734606, 0.10721305887725226, -0.08402740272078703, -0.16211203513745914, -0.0016214260127721618, 0.3100491255195548, -0.2064526685353074, -0.28773602656000635, 0.05829341141678035, -0.27265057036663687, -0.11233707946214803, 0.0929241694574439, -0.01317991216609... |
706.4286 | Measuring eccentricity in binary black-hole initial data | Initial data for evolving black-hole binaries can be constructed via many
techniques, and can represent a wide range of physical scenarios. However,
because of the way that different schemes parameterize the physical aspects of
a configuration, it is not alway clear what a given set of initial data
actually represent... | gr-qc | initial data for evolving blackhole binaries can be constructed via many techniques and can represent a wide range of physical scenarios however because of the way that different schemes parameterize the physical aspects of a configuration it is not alway clear what a given set of initial data actually represents this ... | [['initial', 'data', 'for', 'evolving', 'blackhole', 'binaries', 'can', 'be', 'constructed', 'via', 'many', 'techniques', 'and', 'can', 'represent', 'a', 'wide', 'range', 'of', 'physical', 'scenarios', 'however', 'because', 'of', 'the', 'way', 'that', 'different', 'schemes', 'parameterize', 'the', 'physical', 'aspects'... | [-0.1656062769066408, 0.08836649885589035, -0.12423624844609091, 0.134048910061485, -0.08180908776425926, -0.09232361806594086, -0.001280027985472807, 0.3613830477424316, -0.18164601739735856, -0.30293379517134605, 0.08437332039036406, -0.23977507825240793, -0.10543056359302078, 0.30455846375091966, -0.0882781792178925... |
706.4287 | Dyakonov-Tamm wave at the planar interface of a chiral sculptured thin
film and an isotropic dielectric material | Surface waves, named here as Dyakonov-Tamm waves, can exist at the planar
interface of an isotropic dielectric material and a chiral sculptured thin film
(STF). Due to the periodic nonhomogeneity of a chiral STF, the range of the
refractive index of the isotropic material is smaller but the range of the
propagation d... | physics.optics physics.class-ph | surface waves named here as dyakonovtamm waves can exist at the planar interface of an isotropic dielectric material and a chiral sculptured thin film stf due to the periodic nonhomogeneity of a chiral stf the range of the refractive index of the isotropic material is smaller but the range of the propagation direction ... | [['surface', 'waves', 'named', 'here', 'as', 'dyakonovtamm', 'waves', 'can', 'exist', 'at', 'the', 'planar', 'interface', 'of', 'an', 'isotropic', 'dielectric', 'material', 'and', 'a', 'chiral', 'sculptured', 'thin', 'film', 'stf', 'due', 'to', 'the', 'periodic', 'nonhomogeneity', 'of', 'a', 'chiral', 'stf', 'the', 'ra... | [-0.18475043788895987, 0.21357322593775324, -0.02500964263786695, -0.05522481925020527, -0.10491992083067696, -0.06290786263776854, -0.06411677998992327, 0.4263682739055228, -0.2636841927832436, -0.2792977710875372, 0.08274710660390112, -0.28609016903543044, -0.11240190414745095, 0.18793562890606977, 0.0581995643414778... |
706.4288 | On the Ring of Integer-valued Quasi-polynomials | The paper studies some properties of the ring of integer-valued
quasi-polynomials. On this ring, theory of generalized Euclidean division and
generalized GCD are presented. Applications to finite simple continued fraction
expansion and Smith normal form of integral matrices with integer parameters
are also given.
| math.NT math.RA | the paper studies some properties of the ring of integervalued quasipolynomials on this ring theory of generalized euclidean division and generalized gcd are presented applications to finite simple continued fraction expansion and smith normal form of integral matrices with integer parameters are also given | [['the', 'paper', 'studies', 'some', 'properties', 'of', 'the', 'ring', 'of', 'integervalued', 'quasipolynomials', 'on', 'this', 'ring', 'theory', 'of', 'generalized', 'euclidean', 'division', 'and', 'generalized', 'gcd', 'are', 'presented', 'applications', 'to', 'finite', 'simple', 'continued', 'fraction', 'expansion'... | [-0.2005294537362219, 0.09441555960273201, -0.07901257268068465, 0.024856603796996005, -0.13966598984023387, -0.10048300931653516, -0.013944752778942611, 0.32859531116925855, -0.33145744615996425, -0.15708461536136878, 0.1358593996529552, -0.23879453535615044, -0.22788486993786963, 0.19936432687311686, -0.0569366968279... |
706.4289 | A low CMB variance in the WMAP data | We have estimated the CMB variance from the three-year WMAP data, finding a
value which is significantly lower than the one expected from Gaussian
simulations using the WMAP best-fit cosmological model, at a significance level
of 98.7 per cent. This result is even more prominent if we consider only the
north ecliptic... | astro-ph | we have estimated the cmb variance from the threeyear wmap data finding a value which is significantly lower than the one expected from gaussian simulations using the wmap bestfit cosmological model at a significance level of 987 per cent this result is even more prominent if we consider only the north ecliptic hemisph... | [['we', 'have', 'estimated', 'the', 'cmb', 'variance', 'from', 'the', 'threeyear', 'wmap', 'data', 'finding', 'a', 'value', 'which', 'is', 'significantly', 'lower', 'than', 'the', 'one', 'expected', 'from', 'gaussian', 'simulations', 'using', 'the', 'wmap', 'bestfit', 'cosmological', 'model', 'at', 'a', 'significance',... | [-0.07761907108304873, 0.08950926518356576, -0.06885828888809488, 0.11479249178932452, -0.06635755321563765, -0.09356087385452685, 0.04508189669496474, 0.3204478223753326, -0.22082282717334714, -0.36758182818358914, 0.10183541984658409, -0.33779134310503056, -0.055733971835617076, 0.2127822870089807, -0.000204781772578... |
706.429 | Heterotic Kahler/non-Kahler Transitions | We show how two topologically distinct spaces - the Kahler K3 x T^2 and the
non-Kahler T^2 bundle over K3 - can be smoothly connected in heterotic string
theory. The transition occurs when the base K3 is deformed to the T^4/Z_2
orbifold limit. The orbifold theory can be mapped via duality to M-theory on K3
x K3 where... | hep-th | we show how two topologically distinct spaces the kahler k3 x t2 and the nonkahler t2 bundle over k3 can be smoothly connected in heterotic string theory the transition occurs when the base k3 is deformed to the t4z_2 orbifold limit the orbifold theory can be mapped via duality to mtheory on k3 x k3 where the transitio... | [['we', 'show', 'how', 'two', 'topologically', 'distinct', 'spaces', 'the', 'kahler', 'k3', 'x', 't2', 'and', 'the', 'nonkahler', 't2', 'bundle', 'over', 'k3', 'can', 'be', 'smoothly', 'connected', 'in', 'heterotic', 'string', 'theory', 'the', 'transition', 'occurs', 'when', 'the', 'base', 'k3', 'is', 'deformed', 'to',... | [-0.2113711656014802, 0.17170653504405037, -0.10733732490828543, 0.1379775201961765, -0.09209141995278046, -0.2563617889854041, 0.00013666959465340233, 0.34132657434339775, -0.28335441756203317, -0.19800272754351186, 0.08598038445713675, -0.2951618066114007, -0.16270328662358224, 0.143321947836684, -0.15897770937899072... |
706.4291 | Soft modes near the buckling transition of icosahedral shells | Icosahedral shells undergo a buckling transition as the ratio of Young's
modulus to bending stiffness increases. Strong bending stiffness favors smooth,
nearly spherical shapes, while weak bending stiffness leads to a sharply
faceted icosahedral shape. Based on the phonon spectrum of a simplified
mass-and-spring mode... | physics.bio-ph | icosahedral shells undergo a buckling transition as the ratio of youngs modulus to bending stiffness increases strong bending stiffness favors smooth nearly spherical shapes while weak bending stiffness leads to a sharply faceted icosahedral shape based on the phonon spectrum of a simplified massandspring model of the ... | [['icosahedral', 'shells', 'undergo', 'a', 'buckling', 'transition', 'as', 'the', 'ratio', 'of', 'youngs', 'modulus', 'to', 'bending', 'stiffness', 'increases', 'strong', 'bending', 'stiffness', 'favors', 'smooth', 'nearly', 'spherical', 'shapes', 'while', 'weak', 'bending', 'stiffness', 'leads', 'to', 'a', 'sharply', ... | [-0.13116496435861155, 0.15751791535379575, -0.06050567777490429, -0.014758135498680684, -0.0949778704707343, -0.1201031217438325, 0.020442151991644678, 0.3929265450992801, -0.26794914831841216, -0.25341594365847686, 0.04365845359153236, -0.34501322312569765, -0.18385525663551058, 0.06710821304395101, 0.009371894124319... |
706.4292 | Global perspectives on the energy landscapes of liquids, supercooled
liquids, and glassy systems: The potential energy landscape ensemble | In principle, all of the dynamical complexities of many-body systems are
encapsulated in the potential energy landscapes on which the atoms move - an
observation that suggests that the essentials of the dynamics ought to be
determined by the geometry of those landscapes. But what are the principal
geometric features ... | cond-mat.soft cond-mat.stat-mech | in principle all of the dynamical complexities of manybody systems are encapsulated in the potential energy landscapes on which the atoms move an observation that suggests that the essentials of the dynamics ought to be determined by the geometry of those landscapes but what are the principal geometric features that co... | [['in', 'principle', 'all', 'of', 'the', 'dynamical', 'complexities', 'of', 'manybody', 'systems', 'are', 'encapsulated', 'in', 'the', 'potential', 'energy', 'landscapes', 'on', 'which', 'the', 'atoms', 'move', 'an', 'observation', 'that', 'suggests', 'that', 'the', 'essentials', 'of', 'the', 'dynamics', 'ought', 'to',... | [-0.09844135808206404, 0.12510783205165824, -0.14152169596449707, 0.0806609497280621, -0.02724309267303456, -0.10659652115118073, 0.08112086004093139, 0.3630916210372121, -0.29808044920331844, -0.3021029914342498, 0.05584563304681421, -0.25664088560552045, -0.19753358711398417, 0.16623874896510143, -0.03729087897978212... |
706.4293 | Simple Picture for Neutrino Flavor Transformation in Supernovae | We can understand many recently-discovered features of flavor evolution in
dense, self-coupled supernova neutrino and antineutrino systems with a simple,
physical scheme consisting of two quasi-static solutions. One solution closely
resembles the conventional, adiabatic single neutrino
Mikheyev-Smirnov-Wolfenstein (M... | astro-ph hep-ph | we can understand many recentlydiscovered features of flavor evolution in dense selfcoupled supernova neutrino and antineutrino systems with a simple physical scheme consisting of two quasistatic solutions one solution closely resembles the conventional adiabatic single neutrino mikheyevsmirnovwolfenstein msw mechanism... | [['we', 'can', 'understand', 'many', 'recentlydiscovered', 'features', 'of', 'flavor', 'evolution', 'in', 'dense', 'selfcoupled', 'supernova', 'neutrino', 'and', 'antineutrino', 'systems', 'with', 'a', 'simple', 'physical', 'scheme', 'consisting', 'of', 'two', 'quasistatic', 'solutions', 'one', 'solution', 'closely', '... | [-0.1321153081689491, 0.23226434539897925, -0.04992030281866072, 0.1348584505240913, -0.05139696308694895, -0.1366052957918956, 0.030811838143188313, 0.34364388205264645, -0.22917379942755922, -0.2662658816702741, 0.05502449038208069, -0.2885862390232301, -0.07440934399354089, 0.1688780641212061, -0.00839130354555535, ... |
706.4294 | Cosmic Rays and Global Warming | It has been claimed by others that observed temporal correlations of
terrestrial cloud cover with `the cosmic ray intensity' are causal. The
possibility arises, therefore, of a connection between cosmic rays and Global
Warming. If true, the implications would be very great. We have examined this
claim to look for evi... | astro-ph physics.ao-ph physics.geo-ph physics.soc-ph | it has been claimed by others that observed temporal correlations of terrestrial cloud cover with the cosmic ray intensity are causal the possibility arises therefore of a connection between cosmic rays and global warming if true the implications would be very great we have examined this claim to look for evidence to c... | [['it', 'has', 'been', 'claimed', 'by', 'others', 'that', 'observed', 'temporal', 'correlations', 'of', 'terrestrial', 'cloud', 'cover', 'with', 'the', 'cosmic', 'ray', 'intensity', 'are', 'causal', 'the', 'possibility', 'arises', 'therefore', 'of', 'a', 'connection', 'between', 'cosmic', 'rays', 'and', 'global', 'warm... | [-0.07259489992702584, 0.17933915074536344, -0.07134473002952291, 0.15331768632586318, -0.0827549570822157, -0.05385371145894169, 0.02104189787132782, 0.4128477817575913, -0.23083178463275544, -0.3701867473864695, 0.11277490208522067, -0.30834047772805206, -0.14186157738959082, 0.21642363851788105, -0.07245966348637012... |
706.4295 | Global perspectives on the energy landscapes of liquids, supercooled
liquids, and glassy systems: Geodesic pathways through the potential energy
landscape | How useful it is to think about the potential energy landscape of a complex
many-body system depends in large measure on how direct the connection is to
the system's dynamics. In this paper we show that, within what we call the
potential energy landscape ensemble, it is possible to make direct connections
between the... | cond-mat.soft cond-mat.stat-mech | how useful it is to think about the potential energy landscape of a complex manybody system depends in large measure on how direct the connection is to the systems dynamics in this paper we show that within what we call the potential energy landscape ensemble it is possible to make direct connections between the geomet... | [['how', 'useful', 'it', 'is', 'to', 'think', 'about', 'the', 'potential', 'energy', 'landscape', 'of', 'a', 'complex', 'manybody', 'system', 'depends', 'in', 'large', 'measure', 'on', 'how', 'direct', 'the', 'connection', 'is', 'to', 'the', 'systems', 'dynamics', 'in', 'this', 'paper', 'we', 'show', 'that', 'within', ... | [-0.1389644219992025, 0.17973034565511625, -0.1309088375369575, 0.09550033039338687, -0.033356314724221584, -0.08937931786737041, 0.04214511946015518, 0.388359115817609, -0.32131438089763736, -0.25784471594195635, 0.06420399054055685, -0.29444687687642473, -0.21771276027043873, 0.1877600976893489, 0.0037009882551423687... |
706.4296 | Schwarzian Derivatives and Uniform Local Univalence | Quantitative estimates are obtained for the (finite) valence of functions
analytic in the unit disk with Schwarzian derivative that is bounded or of slow
growth. A harmonic mapping is shown to be uniformly locally univalent with
respect to the hyperbolic metric if and only if it has finite Schwarzian norm,
thus gener... | math.CV | quantitative estimates are obtained for the finite valence of functions analytic in the unit disk with schwarzian derivative that is bounded or of slow growth a harmonic mapping is shown to be uniformly locally univalent with respect to the hyperbolic metric if and only if it has finite schwarzian norm thus generalizin... | [['quantitative', 'estimates', 'are', 'obtained', 'for', 'the', 'finite', 'valence', 'of', 'functions', 'analytic', 'in', 'the', 'unit', 'disk', 'with', 'schwarzian', 'derivative', 'that', 'is', 'bounded', 'or', 'of', 'slow', 'growth', 'a', 'harmonic', 'mapping', 'is', 'shown', 'to', 'be', 'uniformly', 'locally', 'univ... | [-0.09789043783420723, 0.07411504360489955, -0.06879203256151052, 0.07045328734946527, -0.0902305771660519, -0.14532013715257588, -0.019649390896705733, 0.3673585581287027, -0.3146816478047061, -0.11210716788558137, 0.1297224119404484, -0.32172072053670064, -0.13238719673763502, 0.25154476569110706, -0.0853359478538575... |
706.4297 | Accelerated Projected Gradient Method for Linear Inverse Problems with
Sparsity Constraints | Regularization of ill-posed linear inverse problems via $\ell_1$ penalization
has been proposed for cases where the solution is known to be (almost) sparse.
One way to obtain the minimizer of such an $\ell_1$ penalized functional is via
an iterative soft-thresholding algorithm. We propose an alternative
implementatio... | math.NA | regularization of illposed linear inverse problems via ell_1 penalization has been proposed for cases where the solution is known to be almost sparse one way to obtain the minimizer of such an ell_1 penalized functional is via an iterative softthresholding algorithm we propose an alternative implementation to ell_1cons... | [['regularization', 'of', 'illposed', 'linear', 'inverse', 'problems', 'via', 'ell_1', 'penalization', 'has', 'been', 'proposed', 'for', 'cases', 'where', 'the', 'solution', 'is', 'known', 'to', 'be', 'almost', 'sparse', 'one', 'way', 'to', 'obtain', 'the', 'minimizer', 'of', 'such', 'an', 'ell_1', 'penalized', 'functi... | [0.0017790777748450638, -0.05525996929689427, -0.1607053224023548, 0.06384407493867911, -0.10464616698212921, -0.18326426574029028, -0.0017680389620363711, 0.4706240001693368, -0.3846474975952879, -0.24738543012179434, 0.17396514814230613, -0.22860973770730197, -0.18947290039621292, 0.18295141477137805, -0.104641267783... |
706.4298 | Unison as a Self-Stabilizing Wave Stream Algorithm in Asynchronous
Anonymous Networks | How to pass from local to global scales in anonymous networks? How to
organize a selfstabilizing propagation of information with feedback. From the
Angluin impossibility results, we cannot elect a leader in a general anonymous
network. Thus, it is impossible to build a rooted spanning tree. Many problems
can only be ... | cs.DC | how to pass from local to global scales in anonymous networks how to organize a selfstabilizing propagation of information with feedback from the angluin impossibility results we cannot elect a leader in a general anonymous network thus it is impossible to build a rooted spanning tree many problems can only be solved b... | [['how', 'to', 'pass', 'from', 'local', 'to', 'global', 'scales', 'in', 'anonymous', 'networks', 'how', 'to', 'organize', 'a', 'selfstabilizing', 'propagation', 'of', 'information', 'with', 'feedback', 'from', 'the', 'angluin', 'impossibility', 'results', 'we', 'can', 'not', 'elect', 'a', 'leader', 'in', 'a', 'general'... | [-0.2114810809036907, 0.056057529800455086, -0.08596563607226221, 0.0923481763096615, -0.14160671593862123, -0.15261315849616008, 0.09509242589024788, 0.4219154288523457, -0.363482093856651, -0.25045554811882526, 0.09958947282585436, -0.20449924965699515, -0.22584281169467282, 0.1493798642321078, -0.0961754655043379, 0... |
706.4299 | A Metric on Shape Space with Explicit Geodesics | This paper studies a specific metric on plane curves that has the property of
being isometric to classical manifold (sphere, complex projective, Stiefel,
Grassmann) modulo change of parametrization, each of these classical manifolds
being associated to specific qualifications of the space of curves
(closed-open, modu... | math.DG math.AP | this paper studies a specific metric on plane curves that has the property of being isometric to classical manifold sphere complex projective stiefel grassmann modulo change of parametrization each of these classical manifolds being associated to specific qualifications of the space of curves closedopen modulo rotation... | [['this', 'paper', 'studies', 'a', 'specific', 'metric', 'on', 'plane', 'curves', 'that', 'has', 'the', 'property', 'of', 'being', 'isometric', 'to', 'classical', 'manifold', 'sphere', 'complex', 'projective', 'stiefel', 'grassmann', 'modulo', 'change', 'of', 'parametrization', 'each', 'of', 'these', 'classical', 'mani... | [-0.166870054278294, 0.0976002597629926, -0.07997331031385743, 0.0852792779966094, -0.12724220909570394, -0.11287824285937588, -0.0002787921224361318, 0.4070043870362273, -0.2941489773521633, -0.22908472710109332, 0.10456321604974698, -0.27783909123881084, -0.17846713958741084, 0.23205884744560248, -0.1295931592538724,... |
706.43 | Morphological influence on surface--wave propagation at the planar
interface of a metal film and a columnar thin film | The selection of a higher vapor deposition angle when growing a columnar thin
film (CTF) leads to surface-wave propagation at a planar metal-CTF interface
with phase velocity of lower magnitude and shorter propagation range.
Acordingly, a higher angle of plane-wave incidence is required to excite that
surface wave in... | physics.optics physics.class-ph | the selection of a higher vapor deposition angle when growing a columnar thin film ctf leads to surfacewave propagation at a planar metalctf interface with phase velocity of lower magnitude and shorter propagation range acordingly a higher angle of planewave incidence is required to excite that surface wave in a modifi... | [['the', 'selection', 'of', 'a', 'higher', 'vapor', 'deposition', 'angle', 'when', 'growing', 'a', 'columnar', 'thin', 'film', 'ctf', 'leads', 'to', 'surfacewave', 'propagation', 'at', 'a', 'planar', 'metalctf', 'interface', 'with', 'phase', 'velocity', 'of', 'lower', 'magnitude', 'and', 'shorter', 'propagation', 'rang... | [-0.16781491808155002, 0.2619539689930046, -0.044061644596285095, -0.030359626297985075, -0.12296342727381225, -0.11837649547184508, 0.03934112554370407, 0.421704351047725, -0.237445437705473, -0.3118153085895613, 0.04246703351336513, -0.21989744527301952, -0.07901148518145669, 0.18503516511626394, 0.03168868772028124,... |
706.4301 | Searching for Gravitational-Wave Bursts with LIGO | We present recent results from searches by the LIGO Science Collaboration for
bursts of gravitational-wave radiation, as well as the status of other ongoing
searches. These include directed searches for bursts associated with observed
sources (gamma-ray bursts, soft gamma repeaters) and untriggered searches for
burst... | gr-qc | we present recent results from searches by the ligo science collaboration for bursts of gravitationalwave radiation as well as the status of other ongoing searches these include directed searches for bursts associated with observed sources gammaray bursts soft gamma repeaters and untriggered searches for bursts from un... | [['we', 'present', 'recent', 'results', 'from', 'searches', 'by', 'the', 'ligo', 'science', 'collaboration', 'for', 'bursts', 'of', 'gravitationalwave', 'radiation', 'as', 'well', 'as', 'the', 'status', 'of', 'other', 'ongoing', 'searches', 'these', 'include', 'directed', 'searches', 'for', 'bursts', 'associated', 'wit... | [-0.05212266862370251, 0.1734204164794868, -0.005138088682932513, 0.15988920952769972, -0.15299755980127624, -0.07740776621115704, 0.06422640555649109, 0.4262850123590657, -0.19807756732084922, -0.3621723981396783, 0.1005172645991912, -0.3336131827728379, -0.12067200093311146, 0.32595394156773444, 0.03200107517962655, ... |
706.4302 | Silicon beamsplitter for Fourier transform spectroscopy at far infrared
frequencies | We report the performance of a silicon wafer beamsplitter for use for low
$\Delta\nu>0.3 cm^{-1}$ resolution Fourier transform spectroscopy at far
infrared frequencies. We characterize the Si beamsplitter by comparing
throughput spectra measured with it to those measured with the standard Mylar
beamsplitters commonly... | physics.ins-det physics.optics | we report the performance of a silicon wafer beamsplitter for use for low deltanu03 cm1 resolution fourier transform spectroscopy at far infrared frequencies we characterize the si beamsplitter by comparing throughput spectra measured with it to those measured with the standard mylar beamsplitters commonly used in that... | [['we', 'report', 'the', 'performance', 'of', 'a', 'silicon', 'wafer', 'beamsplitter', 'for', 'use', 'for', 'low', 'deltanu03', 'cm1', 'resolution', 'fourier', 'transform', 'spectroscopy', 'at', 'far', 'infrared', 'frequencies', 'we', 'characterize', 'the', 'si', 'beamsplitter', 'by', 'comparing', 'throughput', 'spectr... | [-0.05960742991866188, 0.12939536008011868, -0.02048422975862837, -0.029179563409450243, 0.009050506302360994, -0.1837575794916655, 0.030395944563411725, 0.49093388385303754, -0.1950822141584735, -0.3259761450908092, 0.0691972375189995, -0.3334789467934409, -0.029353788499172556, 0.25181789494715356, -0.037976988961043... |
706.4303 | Global General Relativistic MHD Simulation of a Tilted Black-Hole
Accretion Disk | This paper presents a continuation of our efforts to numerically study
accretion disks that are misaligned (tilted) with respect to the rotation axis
of a Kerr black hole. Here we present results of a global numerical simulation
which fully incorporates the effects of the black hole spacetime as well as
magnetorotati... | astro-ph | this paper presents a continuation of our efforts to numerically study accretion disks that are misaligned tilted with respect to the rotation axis of a kerr black hole here we present results of a global numerical simulation which fully incorporates the effects of the black hole spacetime as well as magnetorotational ... | [['this', 'paper', 'presents', 'a', 'continuation', 'of', 'our', 'efforts', 'to', 'numerically', 'study', 'accretion', 'disks', 'that', 'are', 'misaligned', 'tilted', 'with', 'respect', 'to', 'the', 'rotation', 'axis', 'of', 'a', 'kerr', 'black', 'hole', 'here', 'we', 'present', 'results', 'of', 'a', 'global', 'numeric... | [-0.16946909182344475, 0.11166818751477084, -0.05852675388450734, 0.05869033264752943, -0.09080399755546223, -0.06030179451937006, -0.013547447457958403, 0.33953962433752755, -0.24449626283509837, -0.2882883267365903, 0.11084921390941035, -0.2871114369594462, -0.059574180598100344, 0.2370083919621163, -0.06976776978849... |
706.4304 | Erratum: Assessment of uncertainties in QRPA $0\nu\beta\beta$-decay
nuclear matrix elements [Nucl. Phys. A 766, 107 (2006)] | This is an erratum to our previously published paper.
| nucl-th hep-ph | this is an erratum to our previously published paper | [['this', 'is', 'an', 'erratum', 'to', 'our', 'previously', 'published', 'paper']] | [-0.034768850439124636, -0.05257687783483157, -0.12003827136423853, -0.04985809408956104, -0.19960625821517575, 0.0019351117726829317, 0.036162831833482616, 0.3147331521742874, -0.19658914829293886, -0.40963773905403084, 0.0780289171056615, -0.3127872811423408, -0.18044968363311556, 0.13541672958268058, -0.349867577768... |
706.4305 | Moments from their very truncations | It is known that positive definiteness is not enough for the multidimensional
moment problem to be solved. We would like throw in to the garden of existing
in this matter so far results one more, a result which takes into
considerations the utmost possible truncations.
| math.FA math.CA | it is known that positive definiteness is not enough for the multidimensional moment problem to be solved we would like throw in to the garden of existing in this matter so far results one more a result which takes into considerations the utmost possible truncations | [['it', 'is', 'known', 'that', 'positive', 'definiteness', 'is', 'not', 'enough', 'for', 'the', 'multidimensional', 'moment', 'problem', 'to', 'be', 'solved', 'we', 'would', 'like', 'throw', 'in', 'to', 'the', 'garden', 'of', 'existing', 'in', 'this', 'matter', 'so', 'far', 'results', 'one', 'more', 'a', 'result', 'whi... | [-0.06355643024823318, 0.11762380929042895, -0.1253695148974657, 0.14215079398256622, -0.1504308368389805, -0.14219070022097893, 0.02758794922200549, 0.33114933810300295, -0.2967677727341652, -0.2626051439644976, 0.1583528831238962, -0.2595079622955786, -0.13629775668183963, 0.21150529359777767, -0.09537721729526917, 0... |
706.4306 | Smooth models of quiver moduli | For any moduli space of stable representations of quivers, certain smooth
varieties, compactifying projective space fibrations over the moduli space, are
constructed. The boundary of this compactification is analyzed. Explicit
formulas for the Betti numbers of the smooth models are derived. In the case of
moduli of s... | math.RT math.AG math.CO | for any moduli space of stable representations of quivers certain smooth varieties compactifying projective space fibrations over the moduli space are constructed the boundary of this compactification is analyzed explicit formulas for the betti numbers of the smooth models are derived in the case of moduli of simple re... | [['for', 'any', 'moduli', 'space', 'of', 'stable', 'representations', 'of', 'quivers', 'certain', 'smooth', 'varieties', 'compactifying', 'projective', 'space', 'fibrations', 'over', 'the', 'moduli', 'space', 'are', 'constructed', 'the', 'boundary', 'of', 'this', 'compactification', 'is', 'analyzed', 'explicit', 'formu... | [-0.21550223981190858, 0.11361330294788911, -0.0871975093212878, 0.1268099969702548, -0.09285930190877668, -0.1031623493623117, -0.045600515918741966, 0.3433181652478103, -0.31534550406424133, -0.17911285815102146, 0.13317207185800412, -0.16230265158710294, -0.14778091574633687, 0.2395955496628223, -0.17983347398167726... |
706.4307 | Sonic booms and diffusion wakes generated by a heavy quark in thermal
AdS/CFT | We evaluate the Poynting vector generated by a heavy quark moving through a
thermal state of N=4 gauge theory using AdS/CFT. A significant diffusion wake
is observed as well as a Mach cone. We discuss the ratio of the energy going
into sound modes to the energy coming in from the wake.
| hep-th hep-ph nucl-th | we evaluate the poynting vector generated by a heavy quark moving through a thermal state of n4 gauge theory using adscft a significant diffusion wake is observed as well as a mach cone we discuss the ratio of the energy going into sound modes to the energy coming in from the wake | [['we', 'evaluate', 'the', 'poynting', 'vector', 'generated', 'by', 'a', 'heavy', 'quark', 'moving', 'through', 'a', 'thermal', 'state', 'of', 'n4', 'gauge', 'theory', 'using', 'adscft', 'a', 'significant', 'diffusion', 'wake', 'is', 'observed', 'as', 'well', 'as', 'a', 'mach', 'cone', 'we', 'discuss', 'the', 'ratio', ... | [-0.10224011085945396, 0.2576782160366957, -0.09499505787299803, 0.09068736810765515, -0.05865317787258671, -0.04629765330957106, 0.044390529366725016, 0.31026624275657994, -0.27037800583415306, -0.23991513594340247, 0.04330734990295381, -0.2900236363057047, -0.04999576291391769, 0.14968035241159108, 0.0187070744398694... |
706.4308 | Reducibility of the polynomial representation of the degenerate double
affine Hecke algebra | In this note we determine the values of parameters c for which the polynomial
representation of the degenerate double affine Hecke algebra (DAHA), i.e. the
trigonometric Cherednik algebra, is reducible. Namely, we show that c is a
reducibility point for the polynomial representation of the trigonometric
Cherednik alg... | math.QA math.RT | in this note we determine the values of parameters c for which the polynomial representation of the degenerate double affine hecke algebra daha ie the trigonometric cherednik algebra is reducible namely we show that c is a reducibility point for the polynomial representation of the trigonometric cherednik algebra for a... | [['in', 'this', 'note', 'we', 'determine', 'the', 'values', 'of', 'parameters', 'c', 'for', 'which', 'the', 'polynomial', 'representation', 'of', 'the', 'degenerate', 'double', 'affine', 'hecke', 'algebra', 'daha', 'ie', 'the', 'trigonometric', 'cherednik', 'algebra', 'is', 'reducible', 'namely', 'we', 'show', 'that', ... | [-0.1698308780476033, 0.014343991631937919, -0.08777836240201353, 0.02502507092888145, -0.11188820927517018, -0.21372818267930335, -0.004244516690688155, 0.3190982614591648, -0.39257438339850054, -0.1620641554331529, 0.1301753083929402, -0.211783064825234, -0.16280341492916858, 0.20784878974484505, -0.09661484768104991... |
706.4309 | Constraints on the extra dimension from KK gravitino decay | We study the consequences of the gravitino decay into dark matter. We suppose
that the lightest neutralino is the main component of dark matter. In our
framework gravitino is heavy enough to decay before Big Bang Nucleosynthesis
starts. We consider a model coming from a five dimensional supergravity
compactified on $... | hep-ph | we study the consequences of the gravitino decay into dark matter we suppose that the lightest neutralino is the main component of dark matter in our framework gravitino is heavy enough to decay before big bang nucleosynthesis starts we consider a model coming from a five dimensional supergravity compactified on s1z_2 ... | [['we', 'study', 'the', 'consequences', 'of', 'the', 'gravitino', 'decay', 'into', 'dark', 'matter', 'we', 'suppose', 'that', 'the', 'lightest', 'neutralino', 'is', 'the', 'main', 'component', 'of', 'dark', 'matter', 'in', 'our', 'framework', 'gravitino', 'is', 'heavy', 'enough', 'to', 'decay', 'before', 'big', 'bang',... | [-0.10589802008507831, 0.21872917103166856, -0.1426377921779931, 0.10955168420241534, -0.08102889592464635, -0.12675520940319984, -0.013485082992701791, 0.29272401236448786, -0.18845357364261872, -0.287185577879427, 0.0675408447150403, -0.29310440650442615, -0.010405637471194495, 0.14269445435729722, -0.037711287783167... |
706.431 | Exotic phase diagram of a cluster charging model of bosons on the kagome
lattice | We study a model of hard-core bosons on the kagome lattice with short-range
hopping ($t$) and repulsive interactions ($V$). This model directly maps on to
an easy-axis $S=1/2$ XXZ model on the kagome lattice and is also related, at
large $V/t$, to a quantum dimer model on the triangular lattice. Using quantum
Monte C... | cond-mat.str-el | we study a model of hardcore bosons on the kagome lattice with shortrange hopping t and repulsive interactions v this model directly maps on to an easyaxis s12 xxz model on the kagome lattice and is also related at large vt to a quantum dimer model on the triangular lattice using quantum monte carlo qmc numerics we map... | [['we', 'study', 'a', 'model', 'of', 'hardcore', 'bosons', 'on', 'the', 'kagome', 'lattice', 'with', 'shortrange', 'hopping', 't', 'and', 'repulsive', 'interactions', 'v', 'this', 'model', 'directly', 'maps', 'on', 'to', 'an', 'easyaxis', 's12', 'xxz', 'model', 'on', 'the', 'kagome', 'lattice', 'and', 'is', 'also', 're... | [-0.15883999497564816, 0.2735253035008681, -0.06124851337970868, 0.01674053380117927, -0.00813720918491437, -0.18856524833722316, 0.11747236766081426, 0.3870994744547566, -0.25434612544429047, -0.22083177580689003, 0.046302131160551714, -0.36009279607230277, -0.0932825845296468, 0.07587278891329989, 0.06623035219314767... |
706.4311 | LHC Phenomenology of an Extended Standard Model with a Real Scalar
Singlet | Gauge singlet extensions of the Standard Model (SM) scalar sector may help
remedy its theoretical and phenomenological shortcomings while solving
outstanding problems in cosmology. Depending on the symmetries of the scalar
potential, such extensions may provide a viable candidate for the observed
relic density of col... | hep-ph | gauge singlet extensions of the standard model sm scalar sector may help remedy its theoretical and phenomenological shortcomings while solving outstanding problems in cosmology depending on the symmetries of the scalar potential such extensions may provide a viable candidate for the observed relic density of cold dark... | [['gauge', 'singlet', 'extensions', 'of', 'the', 'standard', 'model', 'sm', 'scalar', 'sector', 'may', 'help', 'remedy', 'its', 'theoretical', 'and', 'phenomenological', 'shortcomings', 'while', 'solving', 'outstanding', 'problems', 'in', 'cosmology', 'depending', 'on', 'the', 'symmetries', 'of', 'the', 'scalar', 'pote... | [-0.083296153838161, 0.2215381937751628, -0.0703317134824322, 0.18557729531153325, -0.10664518277893667, -0.1982282819302722, -0.02133480174456789, 0.29150610220684703, -0.21947199598595987, -0.2976323073129348, 0.04919433459331653, -0.2625493105307547, -0.028121694473325798, 0.12276529417503014, 0.09759404039636377, 0... |
706.4312 | Interacting Binaries with Eccentric Orbits. Secular Orbital Evolution
Due To Conservative Mass Transfer | We investigate the secular evolution of the orbital semi-major axis and
eccentricity due to mass transfer in eccentric binaries, assuming conservation
of total system mass and orbital angular momentum. Assuming a delta function
mass transfer rate centered at periastron, we find rates of secular change of
the orbital ... | astro-ph | we investigate the secular evolution of the orbital semimajor axis and eccentricity due to mass transfer in eccentric binaries assuming conservation of total system mass and orbital angular momentum assuming a delta function mass transfer rate centered at periastron we find rates of secular change of the orbital semima... | [['we', 'investigate', 'the', 'secular', 'evolution', 'of', 'the', 'orbital', 'semimajor', 'axis', 'and', 'eccentricity', 'due', 'to', 'mass', 'transfer', 'in', 'eccentric', 'binaries', 'assuming', 'conservation', 'of', 'total', 'system', 'mass', 'and', 'orbital', 'angular', 'momentum', 'assuming', 'a', 'delta', 'funct... | [-0.1912264990579446, 0.15839519375003874, -0.06934170205049474, 0.08719769111794835, -0.0689987980443588, -0.057208222690028475, 0.033469789963651526, 0.3836981892372739, -0.23681487907293908, -0.3563219264788712, 0.06623391773702794, -0.21683123163839288, -0.017193570816047252, 0.21778974583387337, -0.056494096437706... |
706.4313 | Rephasing Invariants of Quark and Lepton Mixing Matrices | Rephasing invariants of quark and lepton mixing matrices are obtained in the
standard model extended by the seesaw mechanism, and in its low-energy
effective theory with the dimension-five Majorana mass operator. We classify
the basic invariants, discuss non-trivial relations between them, and determine
the independe... | hep-ph | rephasing invariants of quark and lepton mixing matrices are obtained in the standard model extended by the seesaw mechanism and in its lowenergy effective theory with the dimensionfive majorana mass operator we classify the basic invariants discuss nontrivial relations between them and determine the independent invari... | [['rephasing', 'invariants', 'of', 'quark', 'and', 'lepton', 'mixing', 'matrices', 'are', 'obtained', 'in', 'the', 'standard', 'model', 'extended', 'by', 'the', 'seesaw', 'mechanism', 'and', 'in', 'its', 'lowenergy', 'effective', 'theory', 'with', 'the', 'dimensionfive', 'majorana', 'mass', 'operator', 'we', 'classify'... | [-0.13404035926479, 0.252039413232441, -0.05214682303961705, 0.15603912451346827, -0.03980749735968526, -0.1548390672806735, 0.07955230057467072, 0.29231804552149365, -0.289835468061607, -0.3008811132326214, 0.07290360922078518, -0.2441984023052183, -0.12056503043277189, 0.11728682887306521, -0.0035808279644697905, 0.0... |
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