id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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707.003 | Mass Determination in SUSY-like Events with Missing Energy | We describe a kinematic method which is capable of determining the overall
mass scale in SUSY-like events at a hadron collider with two missing (dark
matter) particles. We focus on the kinematic topology in which a pair of
identical particles is produced with each decaying to two leptons and an
invisible particle (sc... | hep-ph astro-ph hep-ex | we describe a kinematic method which is capable of determining the overall mass scale in susylike events at a hadron collider with two missing dark matter particles we focus on the kinematic topology in which a pair of identical particles is produced with each decaying to two leptons and an invisible particle schematic... | [['we', 'describe', 'a', 'kinematic', 'method', 'which', 'is', 'capable', 'of', 'determining', 'the', 'overall', 'mass', 'scale', 'in', 'susylike', 'events', 'at', 'a', 'hadron', 'collider', 'with', 'two', 'missing', 'dark', 'matter', 'particles', 'we', 'focus', 'on', 'the', 'kinematic', 'topology', 'in', 'which', 'a',... | [-0.09583006963945606, 0.261854226211099, -0.05451818758791143, 0.1705245933094545, -0.0350964913134747, -0.13293662342930182, 0.008365801719196618, 0.3378010125641517, -0.23973678331324125, -0.3244905404517437, 0.011561111564484031, -0.34190739722633584, 0.05617244742975077, 0.15714740626611073, 0.03605572213941717, 0... |
707.0031 | Some Observations for Mean-Field Spin Glass Models | We obtain bounds to show that the pressure of a two-body, mean-field spin
glass is a Lipschitz function of the underlying distribution of the random
coupling constants, with respect to a particular semi-norm. This allows us to
re-derive a result of Carmona and Hu, on the universality of the SK model, by a
different p... | math-ph math.MP | we obtain bounds to show that the pressure of a twobody meanfield spin glass is a lipschitz function of the underlying distribution of the random coupling constants with respect to a particular seminorm this allows us to rederive a result of carmona and hu on the universality of the sk model by a different proof and to... | [['we', 'obtain', 'bounds', 'to', 'show', 'that', 'the', 'pressure', 'of', 'a', 'twobody', 'meanfield', 'spin', 'glass', 'is', 'a', 'lipschitz', 'function', 'of', 'the', 'underlying', 'distribution', 'of', 'the', 'random', 'coupling', 'constants', 'with', 'respect', 'to', 'a', 'particular', 'seminorm', 'this', 'allows'... | [-0.06832544006502782, 0.1288903018929319, -0.09835251811672893, 0.10201427556721605, -0.07588711521054944, -0.1513141211655596, 0.04769622268847739, 0.30793459232673687, -0.2808516938876138, -0.2486250339395319, 0.07224117953262618, -0.234477827088777, -0.15605263659555432, 0.16463602052874163, -0.07203931863117231, 0... |
707.0032 | Explicit Heegner Points: Kolyvagin's Conjecture and Non-trivial Elements
in the Shafarevich-Tate Group | Kolyvagin used Heegner points to associate a system of cohomology classes to
an elliptic curve over $\Q$ and conjectured that the system contains a
non-trivial class. His conjecture has profound implications on the structure of
Selmer groups. We provide new computational and theoretical evidence for
Kolyvagin's conje... | math.NT | kolyvagin used heegner points to associate a system of cohomology classes to an elliptic curve over q and conjectured that the system contains a nontrivial class his conjecture has profound implications on the structure of selmer groups we provide new computational and theoretical evidence for kolyvagins conjecture mor... | [['kolyvagin', 'used', 'heegner', 'points', 'to', 'associate', 'a', 'system', 'of', 'cohomology', 'classes', 'to', 'an', 'elliptic', 'curve', 'over', 'q', 'and', 'conjectured', 'that', 'the', 'system', 'contains', 'a', 'nontrivial', 'class', 'his', 'conjecture', 'has', 'profound', 'implications', 'on', 'the', 'structur... | [-0.1994628109728671, 0.0024019948556568966, -0.18130528591265363, 0.0980959630731016, -0.10111378587028089, -0.15356633326515925, -0.0014354026114398782, 0.3086456282695463, -0.297139453955672, -0.26630079932991907, 0.06531814693507916, -0.2615661698755277, -0.16530496217618304, 0.2736028112040078, -0.1356631754859050... |
707.0033 | The Existence of Type II Singularities for the Ricci Flow on $S^{n+1}$ | In this paper we prove the existence of Type II singularities for the Ricci
flow on $S^{n+1}$ for all $n\geq 2$.
| math.DG math.AP | in this paper we prove the existence of type ii singularities for the ricci flow on sn1 for all ngeq 2 | [['in', 'this', 'paper', 'we', 'prove', 'the', 'existence', 'of', 'type', 'ii', 'singularities', 'for', 'the', 'ricci', 'flow', 'on', 'sn1', 'for', 'all', 'ngeq', '2']] | [-0.20987954434184802, 0.018859287746073233, -0.005867389873379753, 0.05152877572635632, -0.03378826670259947, -0.17929330299652757, -0.10653986652669985, 0.3197820389732009, -0.22024034212032953, -0.14150915445671194, 0.17519717246094452, -0.3134646240089621, -0.1311634522640989, 0.13321557370502324, -0.11212576340351... |
707.0034 | Manifolds with Pointwise Ricci Pinched Curvature | In this paper, we proved a compactness result about Riemannian manifolds with
an arbitrary pointwisely pinched Ricci curvature tensor.
| math.DG | in this paper we proved a compactness result about riemannian manifolds with an arbitrary pointwisely pinched ricci curvature tensor | [['in', 'this', 'paper', 'we', 'proved', 'a', 'compactness', 'result', 'about', 'riemannian', 'manifolds', 'with', 'an', 'arbitrary', 'pointwisely', 'pinched', 'ricci', 'curvature', 'tensor']] | [-0.24523059896340496, 0.10913288483693338, -0.09204314305986229, 0.08193112024424695, -0.20478684072823902, -0.15940103128454403, -0.1955150347631915, 0.3848907739708298, -0.22890804472722506, -0.19971730819854297, 0.1376656638642185, -0.23330996479643018, -0.18102215257424273, 0.07838451345206092, -0.2392082292292463... |
707.0035 | A Simple Proof for the Generalized Frankel Conjecture | In this short paper, we will give a simple and transcendental proof for Mok's
theorem of the generalized Frankel conjecture. This work is based on the
maximum principle in \cite{BS2} proposed by Brendle and Schoen.
| math.DG | in this short paper we will give a simple and transcendental proof for moks theorem of the generalized frankel conjecture this work is based on the maximum principle in citebs2 proposed by brendle and schoen | [['in', 'this', 'short', 'paper', 'we', 'will', 'give', 'a', 'simple', 'and', 'transcendental', 'proof', 'for', 'moks', 'theorem', 'of', 'the', 'generalized', 'frankel', 'conjecture', 'this', 'work', 'is', 'based', 'on', 'the', 'maximum', 'principle', 'in', 'citebs2', 'proposed', 'by', 'brendle', 'and', 'schoen']] | [-0.126010348143823, 0.0335029772044543, -0.15891634256524198, 0.06972770891083843, -0.1227939527700929, -0.12054142968126517, 0.055179026282584184, 0.23663197479703846, -0.2104826731579926, -0.24637717637918233, 0.10957152479300823, -0.1883730851319235, -0.21612191485131488, 0.2581177988253972, -0.2264194712316727, -0... |
707.0036 | Analysis of Bell inequality violation in superconducting qubits | We analyze conditions for violation of the Bell inequality in the
Clauser-Horne-Shimony-Holt form, focusing on the Josephson phase qubits. We
start the analysis with maximum violation in the ideal case, and then take into
account the effects of the local measurement errors and decoherence. A special
attention is paid... | cond-mat.supr-con quant-ph | we analyze conditions for violation of the bell inequality in the clauserhorneshimonyholt form focusing on the josephson phase qubits we start the analysis with maximum violation in the ideal case and then take into account the effects of the local measurement errors and decoherence a special attention is paid to confi... | [['we', 'analyze', 'conditions', 'for', 'violation', 'of', 'the', 'bell', 'inequality', 'in', 'the', 'clauserhorneshimonyholt', 'form', 'focusing', 'on', 'the', 'josephson', 'phase', 'qubits', 'we', 'start', 'the', 'analysis', 'with', 'maximum', 'violation', 'in', 'the', 'ideal', 'case', 'and', 'then', 'take', 'into', ... | [-0.16349140603683496, 0.14707183904880494, -0.022532063172803374, 0.08306818532863665, -0.02291569173981419, -0.17492379096189611, 0.08582531269272103, 0.32778658907811503, -0.24147547086996432, -0.27339798361553175, 0.0965573155043418, -0.2701266038950467, -0.08890999738625333, 0.17640460499668525, -0.066614838850096... |
707.0037 | Optical Rankine Vortex | Rankine vortex charateristics of a partially coherent optical vortex are
explored using classical and physical optics. Unlike a perfectly coherent
vortex mode, the circulation is not quantized. Excess circulation is predicted
owing to the wave nature of the composite vortex fields. Based on these
findings we propose ... | physics.optics | rankine vortex charateristics of a partially coherent optical vortex are explored using classical and physical optics unlike a perfectly coherent vortex mode the circulation is not quantized excess circulation is predicted owing to the wave nature of the composite vortex fields based on these findings we propose a vort... | [['rankine', 'vortex', 'charateristics', 'of', 'a', 'partially', 'coherent', 'optical', 'vortex', 'are', 'explored', 'using', 'classical', 'and', 'physical', 'optics', 'unlike', 'a', 'perfectly', 'coherent', 'vortex', 'mode', 'the', 'circulation', 'is', 'not', 'quantized', 'excess', 'circulation', 'is', 'predicted', 'o... | [-0.21289226989827903, 0.21621474632810728, -0.10870424475447804, 0.07423109607542773, -0.12532705459378513, -0.12254834024454742, 0.014991528044144312, 0.37845036226744744, -0.2258627908486946, -0.23053502086915223, 0.09525292592497506, -0.16978946711648912, -0.14048233359832973, 0.22060758722763435, -0.04451076410637... |
707.0038 | Cluster-tilted algebras and slices | We give a criterion allowing to verify whether or not two tilted algebras
have the same relation-extension (thus correspond to the same cluster-tilted
algebra). This criterion is in terms of a combinatorial configuration in the
Auslander-Reiten quiver of the cluster-tilted algebra, which we call local
slice.
| math.RT math.RA | we give a criterion allowing to verify whether or not two tilted algebras have the same relationextension thus correspond to the same clustertilted algebra this criterion is in terms of a combinatorial configuration in the auslanderreiten quiver of the clustertilted algebra which we call local slice | [['we', 'give', 'a', 'criterion', 'allowing', 'to', 'verify', 'whether', 'or', 'not', 'two', 'tilted', 'algebras', 'have', 'the', 'same', 'relationextension', 'thus', 'correspond', 'to', 'the', 'same', 'clustertilted', 'algebra', 'this', 'criterion', 'is', 'in', 'terms', 'of', 'a', 'combinatorial', 'configuration', 'in... | [-0.1308343531149957, 0.032326597596208255, -0.1347409748782714, 0.09498226585694486, -0.17156264612244235, -0.18726361694021357, -0.035347837411488094, 0.37621985450387, -0.3619371644014286, -0.22652719977001348, 0.11602708217687904, -0.11297351051535871, -0.13073607110418378, 0.1194176277714885, -0.17454900582217509,... |
707.0039 | AKARI Far-Infrared Source Counts in the Lockman Hole | We report initial results of far-infrared observations of the Lockman hole
with Far-Infrared Surveyor (FIS) onboard the AKARI infrared satellite. On the
basis of slow scan observations of a 0.6 deg x 1.2 deg contiguous area, we
obtained source number counts at 65, 90 and 140 um down to 77, 26 and 194 mJy
(3 sigma), r... | astro-ph | we report initial results of farinfrared observations of the lockman hole with farinfrared surveyor fis onboard the akari infrared satellite on the basis of slow scan observations of a 06 deg x 12 deg contiguous area we obtained source number counts at 65 90 and 140 um down to 77 26 and 194 mjy 3 sigma respectively the... | [['we', 'report', 'initial', 'results', 'of', 'farinfrared', 'observations', 'of', 'the', 'lockman', 'hole', 'with', 'farinfrared', 'surveyor', 'fis', 'onboard', 'the', 'akari', 'infrared', 'satellite', 'on', 'the', 'basis', 'of', 'slow', 'scan', 'observations', 'of', 'a', '06', 'deg', 'x', '12', 'deg', 'contiguous', '... | [-0.05163072035289728, 0.07360359745798632, -0.015287528752994078, 0.08654739722036399, -0.02880164266993793, -0.05089070310171407, 0.11404028760555845, 0.39608228381436605, -0.10982562236917706, -0.462756388885184, 0.09079694977464477, -0.3616802034756312, -0.02171172908005806, 0.20699386169525005, -0.0176139737694309... |
707.004 | Explanation for Anomalous Shock Temperatures Measured by Neutron
Resonance Spectroscopy | Neutron resonance spectrometry (NRS) has been used to measure the temperature
inside Mo samples during shock loading. The temperatures obtained were
significantly higher than predicted assuming ideal hydrodynamic loading. The
effect of plastic flow and non-ideal projectile behavior were assessed. Plastic
flow was cal... | cond-mat.other cond-mat.mtrl-sci | neutron resonance spectrometry nrs has been used to measure the temperature inside mo samples during shock loading the temperatures obtained were significantly higher than predicted assuming ideal hydrodynamic loading the effect of plastic flow and nonideal projectile behavior were assessed plastic flow was calculated ... | [['neutron', 'resonance', 'spectrometry', 'nrs', 'has', 'been', 'used', 'to', 'measure', 'the', 'temperature', 'inside', 'mo', 'samples', 'during', 'shock', 'loading', 'the', 'temperatures', 'obtained', 'were', 'significantly', 'higher', 'than', 'predicted', 'assuming', 'ideal', 'hydrodynamic', 'loading', 'the', 'effec... | [-0.06474059781695377, 0.18075828547561598, -0.10605803088558291, 0.058321675347041586, -0.029222637803912786, -0.09745167562470375, 0.0163109257251225, 0.3794507082373261, -0.21603694045637362, -0.32576039373250065, 0.05684590281174145, -0.27252744199585416, -0.006458603053752467, 0.20330667586350246, 0.00877815830761... |
707.0041 | Classical bifurcations and entanglement in smooth Hamiltonian system | We study entanglement in two coupled quartic oscillators. It is shown that
the entanglement, as measured by the von Neumann entropy, increases with the
classical chaos parameter for generic chaotic eigenstates. We consider certain
isolated periodic orbits whose bifurcation sequence affects a class of quantum
eigensta... | nlin.CD quant-ph | we study entanglement in two coupled quartic oscillators it is shown that the entanglement as measured by the von neumann entropy increases with the classical chaos parameter for generic chaotic eigenstates we consider certain isolated periodic orbits whose bifurcation sequence affects a class of quantum eigenstates ca... | [['we', 'study', 'entanglement', 'in', 'two', 'coupled', 'quartic', 'oscillators', 'it', 'is', 'shown', 'that', 'the', 'entanglement', 'as', 'measured', 'by', 'the', 'von', 'neumann', 'entropy', 'increases', 'with', 'the', 'classical', 'chaos', 'parameter', 'for', 'generic', 'chaotic', 'eigenstates', 'we', 'consider', ... | [-0.21777674159178637, 0.19656564387220615, -0.09707600165410597, 0.10196268641743529, 0.03964212852971334, -0.1619231789828019, 0.042551593508403325, 0.29354149198222595, -0.27009452343743323, -0.19512011059314796, 0.0929979824940709, -0.30497226229329644, -0.209772296398668, 0.17391383304099614, -0.048783344909884875... |
707.0042 | Self force of a static electric charge near a Schwarzschild Star | When a charge is held static near a constant density spherical star, it
experiences a self-force which is significantly different from the force it
would experience when placed near a black hole of the same mass. In this paper,
an expression for the self-force (as measured by a locally inertial observer)
is given %ex... | gr-qc | when a charge is held static near a constant density spherical star it experiences a selfforce which is significantly different from the force it would experience when placed near a black hole of the same mass in this paper an expression for the selfforce as measured by a locally inertial observer is given explicitly c... | [['when', 'a', 'charge', 'is', 'held', 'static', 'near', 'a', 'constant', 'density', 'spherical', 'star', 'it', 'experiences', 'a', 'selfforce', 'which', 'is', 'significantly', 'different', 'from', 'the', 'force', 'it', 'would', 'experience', 'when', 'placed', 'near', 'a', 'black', 'hole', 'of', 'the', 'same', 'mass', ... | [-0.12481820362797896, 0.1408087787121574, -0.10463853092892236, 0.053356541919138224, -0.06465216054950827, -0.1485252118196769, 0.017557397022043078, 0.3365181738875769, -0.1929502451684719, -0.2824203079407239, 0.06997784633006919, -0.30134739603229505, -0.06646649454411438, 0.18043242211818658, -0.02732895357076818... |
707.0043 | Modified A-hypergeometric Systems | We will introduce a modified system of A-hypergeometric system (GKZ system)
by applying a change of variables for Groebner deformations and study its
Groebner basis and the indicial polynomials along the "exceptional
hypersurface".
| math.CA math.AG | we will introduce a modified system of ahypergeometric system gkz system by applying a change of variables for groebner deformations and study its groebner basis and the indicial polynomials along the exceptional hypersurface | [['we', 'will', 'introduce', 'a', 'modified', 'system', 'of', 'ahypergeometric', 'system', 'gkz', 'system', 'by', 'applying', 'a', 'change', 'of', 'variables', 'for', 'groebner', 'deformations', 'and', 'study', 'its', 'groebner', 'basis', 'and', 'the', 'indicial', 'polynomials', 'along', 'the', 'exceptional', 'hypersur... | [-0.26323365781343344, -0.028164687651124867, -0.1439228943464431, 0.021336401685733686, -0.09152456045602307, -0.13829947574854348, 0.0008420113361243045, 0.24998918968732609, -0.34745426069606433, -0.17199526320804248, 0.14490359184811963, -0.24433050090164848, -0.2211413485082713, 0.17721411269722562, -0.12135751726... |
707.0044 | Application of Geometric Phase in Quantum Computations | Geometric phase that manifests itself in number of optic and nuclear
experiments is shown to be a useful tool for realization of quantum
computations in so called holonomic quantum computer model (HQCM). This model
is considered as an externally driven quantum system with adiabatic evolution
law and finite number of ... | quant-ph | geometric phase that manifests itself in number of optic and nuclear experiments is shown to be a useful tool for realization of quantum computations in so called holonomic quantum computer model hqcm this model is considered as an externally driven quantum system with adiabatic evolution law and finite number of the e... | [['geometric', 'phase', 'that', 'manifests', 'itself', 'in', 'number', 'of', 'optic', 'and', 'nuclear', 'experiments', 'is', 'shown', 'to', 'be', 'a', 'useful', 'tool', 'for', 'realization', 'of', 'quantum', 'computations', 'in', 'so', 'called', 'holonomic', 'quantum', 'computer', 'model', 'hqcm', 'this', 'model', 'is'... | [-0.15056765730637503, 0.2146185808375555, -0.047311767136577414, 0.04666316825691988, 0.039293398478106166, -0.23119835257907775, 0.030841178783039387, 0.3488772691516961, -0.2551086475550373, -0.2985232741276205, 0.05558551689279517, -0.19939989163980795, -0.15009721646217528, 0.29308252068546387, -0.0387919420766568... |
707.0045 | The linear and non linear Rayleigh-Taylor instability for the quasi
isobaric profile | We study the stability of the system of the Euler equation in the
neighborhood of a stationary profile associated with the quasi isobaric model
in a gravity field. This stationary profile is not bounded below, hence the
operator is not coercive. We use this linear result to deduce a nonlinear
result
| math.AP | we study the stability of the system of the euler equation in the neighborhood of a stationary profile associated with the quasi isobaric model in a gravity field this stationary profile is not bounded below hence the operator is not coercive we use this linear result to deduce a nonlinear result | [['we', 'study', 'the', 'stability', 'of', 'the', 'system', 'of', 'the', 'euler', 'equation', 'in', 'the', 'neighborhood', 'of', 'a', 'stationary', 'profile', 'associated', 'with', 'the', 'quasi', 'isobaric', 'model', 'in', 'a', 'gravity', 'field', 'this', 'stationary', 'profile', 'is', 'not', 'bounded', 'below', 'henc... | [-0.16184854089264192, 0.07591635277312175, -0.12208735106476382, 0.057470082273414616, -0.06503850312940046, -0.09673011174206347, -0.00874966722639168, 0.287106005146223, -0.30746587322038765, -0.2302483826985254, 0.11140121223277175, -0.23978749921490602, -0.13384412449108912, 0.17113310536460988, -0.043237321845748... |
707.0046 | Smooth K-Theory | We construct an analytic multiplicative model of smooth K-theory. We further
introduce the notion of a smooth K-orientation of a proper submersion and
define the associated push-forward which satisfies functoriality, compatibility
with pull-back diagrams, and projection and bordism formulas. We construct a
multiplica... | math.KT math.DG | we construct an analytic multiplicative model of smooth ktheory we further introduce the notion of a smooth korientation of a proper submersion and define the associated pushforward which satisfies functoriality compatibility with pullback diagrams and projection and bordism formulas we construct a multiplicative lift ... | [['we', 'construct', 'an', 'analytic', 'multiplicative', 'model', 'of', 'smooth', 'ktheory', 'we', 'further', 'introduce', 'the', 'notion', 'of', 'a', 'smooth', 'korientation', 'of', 'a', 'proper', 'submersion', 'and', 'define', 'the', 'associated', 'pushforward', 'which', 'satisfies', 'functoriality', 'compatibility',... | [-0.21574651098377268, 0.00011524136533180225, -0.16986355964671557, 0.09736415225041795, -0.15037591786871493, -0.15223682176610323, -0.0054589822940843205, 0.30988357865094196, -0.4075168047205243, -0.17112568125758373, 0.036116041616917074, -0.17039467307942277, -0.208191132461521, 0.19265627650819508, -0.2566782941... |
707.0047 | Asymptotic Expansion of the One-Loop Approximation of the Chern-Simons
Integral in an Abstract Wiener Space Setting | In an abstract Wiener space setting, we constract a rigorous mathematical
model of the one-loop approximation of the perturbative Chern-Simons integral,
and derive its explicit asymptotic expansion for stochastic Wilson lines.
| math.DG math.PR | in an abstract wiener space setting we constract a rigorous mathematical model of the oneloop approximation of the perturbative chernsimons integral and derive its explicit asymptotic expansion for stochastic wilson lines | [['in', 'an', 'abstract', 'wiener', 'space', 'setting', 'we', 'constract', 'a', 'rigorous', 'mathematical', 'model', 'of', 'the', 'oneloop', 'approximation', 'of', 'the', 'perturbative', 'chernsimons', 'integral', 'and', 'derive', 'its', 'explicit', 'asymptotic', 'expansion', 'for', 'stochastic', 'wilson', 'lines']] | [-0.13969360910836728, 0.027975602515300946, -0.15092735599365928, 0.16831639252843394, -0.11898309040454126, -0.06853024679566583, 0.08413040866294215, 0.3030223537897391, -0.1919689647057244, -0.18637469068409934, 0.07638297794431809, -0.2247597490166945, -0.19109781663263997, 0.1137537120450889, -0.0506392878089701,... |
707.0048 | The Series Product and Its Application to Quantum Feedforward and
Feedback Networks | The purpose of this paper is to present simple and general algebraic methods
for describing series connections in quantum networks. These methods build on
and generalize existing methods for series (or cascade) connections by allowing
for more general interfaces, and by introducing an efficient algebraic tool,
the se... | quant-ph | the purpose of this paper is to present simple and general algebraic methods for describing series connections in quantum networks these methods build on and generalize existing methods for series or cascade connections by allowing for more general interfaces and by introducing an efficient algebraic tool the series pr... | [['the', 'purpose', 'of', 'this', 'paper', 'is', 'to', 'present', 'simple', 'and', 'general', 'algebraic', 'methods', 'for', 'describing', 'series', 'connections', 'in', 'quantum', 'networks', 'these', 'methods', 'build', 'on', 'and', 'generalize', 'existing', 'methods', 'for', 'series', 'or', 'cascade', 'connections',... | [-0.08277204580959616, 0.03826098462447648, -0.07341061429112056, 0.07772981039346666, -0.08444768552659848, -0.15675622677225448, 0.028658800411311518, 0.4116402499958736, -0.30575127351106307, -0.2618225800779161, 0.12526769952212008, -0.219376694923694, -0.23692597827549441, 0.25317694660096746, -0.08364760719342243... |
707.0049 | Molecular coupling of light with plasmonic waveguides | We use molecules to couple light into and out of microscale plasmonic
waveguides. Energy transfer, mediated by surface plasmons, from donor molecules
to acceptor molecules over ten micrometer distances is demonstrated. Also
surface plasmon coupled emission from the donor molecules is observed at
similar distances awa... | physics.optics physics.chem-ph | we use molecules to couple light into and out of microscale plasmonic waveguides energy transfer mediated by surface plasmons from donor molecules to acceptor molecules over ten micrometer distances is demonstrated also surface plasmon coupled emission from the donor molecules is observed at similar distances away from... | [['we', 'use', 'molecules', 'to', 'couple', 'light', 'into', 'and', 'out', 'of', 'microscale', 'plasmonic', 'waveguides', 'energy', 'transfer', 'mediated', 'by', 'surface', 'plasmons', 'from', 'donor', 'molecules', 'to', 'acceptor', 'molecules', 'over', 'ten', 'micrometer', 'distances', 'is', 'demonstrated', 'also', 's... | [-0.07478193253703212, 0.15207711208713096, -0.04257036194674113, -0.010582900020059478, -0.03403791779854975, -0.17710361746931766, 0.04694088470178093, 0.4747815780709086, -0.2213839979550871, -0.29359908438395377, -0.018635496093264342, -0.30505009581262427, -0.11693952438503909, 0.23553672740806122, 0.0134710699642... |
707.005 | Non-atomic Games for Multi-User Systems | In this contribution, the performance of a multi-user system is analyzed in
the context of frequency selective fading channels. Using game theoretic tools,
a useful framework is provided in order to determine the optimal power
allocation when users know only their own channel (while perfect channel state
information ... | cs.IT cs.GT math.IT | in this contribution the performance of a multiuser system is analyzed in the context of frequency selective fading channels using game theoretic tools a useful framework is provided in order to determine the optimal power allocation when users know only their own channel while perfect channel state information is assu... | [['in', 'this', 'contribution', 'the', 'performance', 'of', 'a', 'multiuser', 'system', 'is', 'analyzed', 'in', 'the', 'context', 'of', 'frequency', 'selective', 'fading', 'channels', 'using', 'game', 'theoretic', 'tools', 'a', 'useful', 'framework', 'is', 'provided', 'in', 'order', 'to', 'determine', 'the', 'optimal',... | [-0.1913821447661014, 0.027697921130053007, -0.06470975281970952, 0.06519574823896171, -0.0635780544017691, -0.21043118774538472, 0.10305668367772704, 0.36162327112416265, -0.2691669463589686, -0.24509775397861427, 0.09432332445625623, -0.26350308388169114, -0.14365005830195962, 0.11856692276839065, -0.0935801833796778... |
707.0051 | Q^2-evolution of nucleon-to-resonance transition form factors in a
QCD-inspired vector-meson-dominance model | We adopt the vector-meson-dominance approach to investigate Q^2-evolution of
N-R transition form factors (N denotes nucleon and R an excited resonance) in
the first and second resonance regions. The developed model is based upon
conventional NR\gamma-interaction Lagrangians, introducing three form factors
for spin-3/... | hep-ph nucl-th | we adopt the vectormesondominance approach to investigate q2evolution of nr transition form factors n denotes nucleon and r an excited resonance in the first and second resonance regions the developed model is based upon conventional nrgammainteraction lagrangians introducing three form factors for spin32 resonances an... | [['we', 'adopt', 'the', 'vectormesondominance', 'approach', 'to', 'investigate', 'q2evolution', 'of', 'nr', 'transition', 'form', 'factors', 'n', 'denotes', 'nucleon', 'and', 'r', 'an', 'excited', 'resonance', 'in', 'the', 'first', 'and', 'second', 'resonance', 'regions', 'the', 'developed', 'model', 'is', 'based', 'up... | [-0.11003271909128245, 0.16420007104898104, -0.059805742486126044, 0.09243475949594315, -0.08293475445916319, -0.1078591193284162, 0.05170427684845288, 0.3391066168120445, -0.1480736407124764, -0.2579341006885561, -0.022358587002859816, -0.3492585334143686, -0.10462945857230428, 0.11063464105056671, 0.1080327209194082,... |
707.0052 | Thermodynamics of theories with sixteen supercharges in non-trivial
vacua | We study the thermodynamics of maximally supersymmetric U(N) Yang-Mills
theory on $\mathds{R}\times S^2$ at large $N$. The model arises as a consistent
truncation of ${\cal N}=4$ super Yang-Mills on $\mathds{R}\times S^3$ and as
the continuum limit of the plane-wave matrix model expanded around the $N$
spherical memb... | hep-th | we study the thermodynamics of maximally supersymmetric un yangmills theory on mathdsrtimes s2 at large n the model arises as a consistent truncation of cal n4 super yangmills on mathdsrtimes s3 and as the continuum limit of the planewave matrix model expanded around the n spherical membrane vacuum the theory has an in... | [['we', 'study', 'the', 'thermodynamics', 'of', 'maximally', 'supersymmetric', 'un', 'yangmills', 'theory', 'on', 'mathdsrtimes', 's2', 'at', 'large', 'n', 'the', 'model', 'arises', 'as', 'a', 'consistent', 'truncation', 'of', 'cal', 'n4', 'super', 'yangmills', 'on', 'mathdsrtimes', 's3', 'and', 'as', 'the', 'continuum... | [-0.14758780490139523, 0.20221812157619518, -0.06942986734081923, 0.06589466725842358, -0.02020685127917898, -0.12014708069766036, 0.041444956546896894, 0.2845030875504753, -0.1725529730241753, -0.26271143360910093, 0.0770384566522509, -0.2797385771526944, -0.1645264792027828, 0.056830756322999776, -0.02681204370014082... |
707.0053 | Particle Motion Around Tachyon Monopole | Recently, Li and Liu have studied global monoole of tachyon in a four
dimensional static space-time. We analyze the motion of massless and massive
particles around tachyon monopole. Interestingly, for the bending of light rays
due to tachyon monopole instead of getting angle of deficit we find angle of
surplus. Also ... | gr-qc | recently li and liu have studied global monoole of tachyon in a four dimensional static spacetime we analyze the motion of massless and massive particles around tachyon monopole interestingly for the bending of light rays due to tachyon monopole instead of getting angle of deficit we find angle of surplus also we find ... | [['recently', 'li', 'and', 'liu', 'have', 'studied', 'global', 'monoole', 'of', 'tachyon', 'in', 'a', 'four', 'dimensional', 'static', 'spacetime', 'we', 'analyze', 'the', 'motion', 'of', 'massless', 'and', 'massive', 'particles', 'around', 'tachyon', 'monopole', 'interestingly', 'for', 'the', 'bending', 'of', 'light',... | [-0.18775825464861498, 0.18781527401791656, -0.0832781291729401, 0.11262329227276265, -0.09222358391280212, -0.13805943185700073, 0.02374933643769177, 0.31631719990677776, -0.15952833675380265, -0.3123507777908965, -0.04232808646915983, -0.2899419822035328, -0.15483511303595843, 0.11532083221726001, -0.0206969005769982... |
707.0054 | Mach Cones at central LHC Collisions via MACE | The shape of Mach Cones in central lead on lead collisions at $\sqrt{s_{NN}}
= 5.5$ TeV are calculated and discussed using MACE.
| nucl-th | the shape of mach cones in central lead on lead collisions at sqrts_nn 55 tev are calculated and discussed using mace | [['the', 'shape', 'of', 'mach', 'cones', 'in', 'central', 'lead', 'on', 'lead', 'collisions', 'at', 'sqrts_nn', '55', 'tev', 'are', 'calculated', 'and', 'discussed', 'using', 'mace']] | [-0.0603036643671138, 0.1993889840585845, -0.12483303455103721, 0.13409080853064856, 0.1113799060029643, -0.0986611589434601, -0.10577105584421329, 0.3778971227861586, -0.15352959522888773, -0.3741014310646625, -0.03605847369458172, -0.3377069769693272, 0.11287982744120416, 0.23457161159742446, 0.005853326459016118, 0.... |
707.0055 | The interface free energy: Comparison of accurate Monte Carlo results
for the 3D Ising model with effective interface models | We provide accurate Monte Carlo results for the free energy of interfaces
with periodic boundary conditions in the 3D Ising model. We study a large range
of inverse temperatures, allowing to control corrections to scaling. In
addition to square interfaces, we study rectangular interfaces for a large
range of aspect r... | hep-lat cond-mat.soft hep-th | we provide accurate monte carlo results for the free energy of interfaces with periodic boundary conditions in the 3d ising model we study a large range of inverse temperatures allowing to control corrections to scaling in addition to square interfaces we study rectangular interfaces for a large range of aspect ratios ... | [['we', 'provide', 'accurate', 'monte', 'carlo', 'results', 'for', 'the', 'free', 'energy', 'of', 'interfaces', 'with', 'periodic', 'boundary', 'conditions', 'in', 'the', '3d', 'ising', 'model', 'we', 'study', 'a', 'large', 'range', 'of', 'inverse', 'temperatures', 'allowing', 'to', 'control', 'corrections', 'to', 'sca... | [-0.08678852286600963, 0.09881264815215972, -0.05768580808542035, 0.08863426458977282, -0.06268579629992947, -0.13641976274827378, 0.03886210843375785, 0.4022869213305889, -0.1761596143280374, -0.3630138203858378, 0.09023013627998769, -0.3094414164302276, -0.06943960976786911, 0.250726194675774, 0.01817520866368679, 0.... |
707.0056 | The equation of state of solid nickel aluminide | The pressure-volume-temperature equation of state of the intermetallic
compound NiAl was calculated theoretically, and compared with experimental
measurements. Electron ground states were calculated for NiAl in the CsCl
structure, using density functional theory, and were used to predict the cold
compression curve an... | cond-mat.other cond-mat.mtrl-sci | the pressurevolumetemperature equation of state of the intermetallic compound nial was calculated theoretically and compared with experimental measurements electron ground states were calculated for nial in the cscl structure using density functional theory and were used to predict the cold compression curve and the de... | [['the', 'pressurevolumetemperature', 'equation', 'of', 'state', 'of', 'the', 'intermetallic', 'compound', 'nial', 'was', 'calculated', 'theoretically', 'and', 'compared', 'with', 'experimental', 'measurements', 'electron', 'ground', 'states', 'were', 'calculated', 'for', 'nial', 'in', 'the', 'cscl', 'structure', 'usin... | [-0.06711786025056955, 0.149099338351258, -0.12529490772965066, 0.027546701682135095, -0.01423432914714508, -0.0923460039787288, 0.03144527119045316, 0.41070942755953727, -0.25579716567824057, -0.30998224064047114, 0.054118375646597314, -0.30264535883505794, -0.05336545689107897, 0.2068582008916224, 0.03450474017322651... |
707.0057 | Quantum Oscillations in the Underdoped Cuprate YBa2Cu4O8 | We report the observation of quantum oscillations in the underdoped cuprate
superconductor YBa2Cu4O8 using a tunnel-diode oscillator technique in pulsed
magnetic fields up to 85T. There is a clear signal, periodic in inverse field,
with frequency 660+/-15T and possible evidence for the presence of two
components of s... | cond-mat.supr-con cond-mat.str-el | we report the observation of quantum oscillations in the underdoped cuprate superconductor yba2cu4o8 using a tunneldiode oscillator technique in pulsed magnetic fields up to 85t there is a clear signal periodic in inverse field with frequency 66015t and possible evidence for the presence of two components of slightly d... | [['we', 'report', 'the', 'observation', 'of', 'quantum', 'oscillations', 'in', 'the', 'underdoped', 'cuprate', 'superconductor', 'yba2cu4o8', 'using', 'a', 'tunneldiode', 'oscillator', 'technique', 'in', 'pulsed', 'magnetic', 'fields', 'up', 'to', '85t', 'there', 'is', 'a', 'clear', 'signal', 'periodic', 'in', 'inverse... | [-0.18560208422739222, 0.19649043664558913, -0.05203155642527196, 0.011751574081996374, -0.07134093141750149, -0.13519732457200956, 0.11554913595824948, 0.3649398767510834, -0.18093205160561332, -0.29874336919949757, 0.002514739682816941, -0.33776143051521934, -0.10909296403153111, 0.25369304925729724, -0.0002014115958... |
707.0058 | What is Special About the Planck Mass? | Planck introduced his famous units of mass, length and time a hundred years
ago. The many interesting facets of the Planck mass and length are explored.
The Planck mass ubiquitously occurs in astrophysics, cosmology, quantum
gravity, string theory, etc. Current aspects of its implications for
unification of fundament... | gr-qc | planck introduced his famous units of mass length and time a hundred years ago the many interesting facets of the planck mass and length are explored the planck mass ubiquitously occurs in astrophysics cosmology quantum gravity string theory etc current aspects of its implications for unification of fundamental interac... | [['planck', 'introduced', 'his', 'famous', 'units', 'of', 'mass', 'length', 'and', 'time', 'a', 'hundred', 'years', 'ago', 'the', 'many', 'interesting', 'facets', 'of', 'the', 'planck', 'mass', 'and', 'length', 'are', 'explored', 'the', 'planck', 'mass', 'ubiquitously', 'occurs', 'in', 'astrophysics', 'cosmology', 'qua... | [-0.1764871268375319, 0.2503135886232732, -0.021459182113669498, 0.20444527685334432, -0.08644769504918891, -0.127170247909755, -0.03181030778648426, 0.2829044476088326, -0.2814899056013358, -0.3697537626060894, 0.06627890847670703, -0.26106986187209014, -0.049019600911918336, 0.22888014007801727, 0.004050310038156428,... |
707.0059 | The squeezed generalized amplitude damping channel | Squeezing of a thermal bath introduces new features absent in an open quantum
system interacting with an uncorrelated (zero squeezing) thermal bath. The
resulting dynamics, governed by a Lindblad-type evolution, extends the concept
of a generalized amplitude damping channel, which corresponds to a dissipative
interac... | quant-ph | squeezing of a thermal bath introduces new features absent in an open quantum system interacting with an uncorrelated zero squeezing thermal bath the resulting dynamics governed by a lindbladtype evolution extends the concept of a generalized amplitude damping channel which corresponds to a dissipative interaction with... | [['squeezing', 'of', 'a', 'thermal', 'bath', 'introduces', 'new', 'features', 'absent', 'in', 'an', 'open', 'quantum', 'system', 'interacting', 'with', 'an', 'uncorrelated', 'zero', 'squeezing', 'thermal', 'bath', 'the', 'resulting', 'dynamics', 'governed', 'by', 'a', 'lindbladtype', 'evolution', 'extends', 'the', 'con... | [-0.206234409512185, 0.22250894515086925, -0.12761999275261426, 0.006139289726064924, -0.03567704834482249, -0.1696685154155335, 0.03439911824431928, 0.279574059212909, -0.32992704896365893, -0.19221971689120812, 0.049403014692806585, -0.255746877522153, -0.14157411361606242, 0.16498215108123773, -0.04267130852950846, ... |
707.006 | Global reanalysis of nPDFs | In this talk, we present the results from our recent global reanalysis of
nuclear parton distribution functions (nPDFs), where the DGLAP-evolving nPDFs
are constrained by nuclear hard process data from deep inelastic $l+A$
scattering (DIS) and the Drell-Yan (DY) process in $p+A$ collisions, and by sum
rules. The main... | hep-ph | in this talk we present the results from our recent global reanalysis of nuclear parton distribution functions npdfs where the dglapevolving npdfs are constrained by nuclear hard process data from deep inelastic la scattering dis and the drellyan dy process in pa collisions and by sum rules the main improvements over o... | [['in', 'this', 'talk', 'we', 'present', 'the', 'results', 'from', 'our', 'recent', 'global', 'reanalysis', 'of', 'nuclear', 'parton', 'distribution', 'functions', 'npdfs', 'where', 'the', 'dglapevolving', 'npdfs', 'are', 'constrained', 'by', 'nuclear', 'hard', 'process', 'data', 'from', 'deep', 'inelastic', 'la', 'sca... | [0.00027633346178555405, 0.05293533264868555, -0.16092966124752833, 0.16280243532623834, -0.03727994744153018, -0.05542313354427292, 0.02947084750453739, 0.4001707050247469, -0.2110634493401976, -0.2872082521545066, 0.04055710035490979, -0.31840703426944633, -0.03007566140613694, 0.16022219869605117, -0.013877717449086... |
707.0061 | How to create and detect N-dimensional entangled photons with an active
phase hologram | The experimental realization of multidimensional quantum states may lead to
unexplored and interesting physics, as well as advanced quantum communication
protocols. The orbital angular momentum of photons is a well suitable discrete
degree of freedom for implementing high-dimensional quantum systems. The
standard met... | quant-ph | the experimental realization of multidimensional quantum states may lead to unexplored and interesting physics as well as advanced quantum communication protocols the orbital angular momentum of photons is a well suitable discrete degree of freedom for implementing highdimensional quantum systems the standard method to... | [['the', 'experimental', 'realization', 'of', 'multidimensional', 'quantum', 'states', 'may', 'lead', 'to', 'unexplored', 'and', 'interesting', 'physics', 'as', 'well', 'as', 'advanced', 'quantum', 'communication', 'protocols', 'the', 'orbital', 'angular', 'momentum', 'of', 'photons', 'is', 'a', 'well', 'suitable', 'di... | [-0.12003692408540735, 0.2346493886757849, -0.08182129812323385, 0.05671408382046071, -0.0921198889393256, -0.19090961531253048, 0.03285788981399188, 0.39684908283460474, -0.27599521405580973, -0.3258983736935382, 0.034037746396346914, -0.23948480821598894, -0.084506435994559, 0.2377165995572728, -0.04008938280727576, ... |
707.0062 | Magnetic Single-Electron Transistor as a Tunable Model System for
Kondo-Destroying Quantum Criticality | Single-electron transistors attached to ferromagnetic leads can undergo a
continuous quantum phase transition as their gate voltage is tuned. The
corresponding quantum critical point separates a Fermi liquid phase from a
non-Fermi liquid one. Here, we expound on the physical idea proposed earlier.
The key physics is ... | cond-mat.str-el | singleelectron transistors attached to ferromagnetic leads can undergo a continuous quantum phase transition as their gate voltage is tuned the corresponding quantum critical point separates a fermi liquid phase from a nonfermi liquid one here we expound on the physical idea proposed earlier the key physics is the crit... | [['singleelectron', 'transistors', 'attached', 'to', 'ferromagnetic', 'leads', 'can', 'undergo', 'a', 'continuous', 'quantum', 'phase', 'transition', 'as', 'their', 'gate', 'voltage', 'is', 'tuned', 'the', 'corresponding', 'quantum', 'critical', 'point', 'separates', 'a', 'fermi', 'liquid', 'phase', 'from', 'a', 'nonfe... | [-0.15962542835623025, 0.21646116859544323, -0.08892790114266738, 0.06903714503296801, -0.04434856067471687, -0.1831057681101224, 0.0644086342259881, 0.3079144602851762, -0.23440062845906903, -0.23025428774436155, 0.006769878118328991, -0.2856781913778715, -0.17742058556046217, 0.19907015024744454, -0.00813144904320999... |
707.0063 | The STIRAP-based unitary decelerating and accelerating processes of a
single free atom | A STIRAP-based unitary decelerating (accelerating) process consists of a
train of the standard three-state STIRAP pulse sequences which may act as the
basic unitary decelerating (accelerating) sequences. The present work is
focused on investigating analytically and quantitatively how the momentum
distribution of a mo... | quant-ph | a stirapbased unitary decelerating accelerating process consists of a train of the standard threestate stirap pulse sequences which may act as the basic unitary decelerating accelerating sequences the present work is focused on investigating analytically and quantitatively how the momentum distribution of a momentum su... | [['a', 'stirapbased', 'unitary', 'decelerating', 'accelerating', 'process', 'consists', 'of', 'a', 'train', 'of', 'the', 'standard', 'threestate', 'stirap', 'pulse', 'sequences', 'which', 'may', 'act', 'as', 'the', 'basic', 'unitary', 'decelerating', 'accelerating', 'sequences', 'the', 'present', 'work', 'is', 'focused... | [-0.09925329251484005, 0.2424202431234293, -0.11698675419015964, 0.04084170990367006, -0.008740693633017394, -0.1549820866213616, 0.02743185690733382, 0.4417559009028274, -0.2872714779890834, -0.21836274652101031, 0.048269953534921306, -0.19274101917708822, -0.05807390732267752, 0.20807750643457398, 0.00475187839965823... |
707.0064 | Causal Propagation of Spin-Cascades | We gauge the direct product of the Proca with the Dirac equation that
describes the coupling to the electromagnetic field of the spin-cascade
(1/2,3/2) residing in the four-vector spinor and analyze propagation of its
wave fronts in terms of the Courant-Hilbert criteria. We show that the
differential equation under c... | hep-ph | we gauge the direct product of the proca with the dirac equation that describes the coupling to the electromagnetic field of the spincascade 1232 residing in the fourvector spinor and analyze propagation of its wave fronts in terms of the couranthilbert criteria we show that the differential equation under consideratio... | [['we', 'gauge', 'the', 'direct', 'product', 'of', 'the', 'proca', 'with', 'the', 'dirac', 'equation', 'that', 'describes', 'the', 'coupling', 'to', 'the', 'electromagnetic', 'field', 'of', 'the', 'spincascade', '1232', 'residing', 'in', 'the', 'fourvector', 'spinor', 'and', 'analyze', 'propagation', 'of', 'its', 'wave... | [-0.21051618951288137, 0.14288197075643852, -0.0969031830614602, 0.05260203055275435, -0.1133110717616298, -0.03580007708038796, -0.02360167202793739, 0.3155346800319173, -0.2445183494085954, -0.23024130063978107, 0.02034011629346589, -0.25025300436669073, -0.14823260734027083, 0.14835504607974806, 0.03023761633190919,... |
707.0065 | Superconducting-normal interface propagation speed in superconducting
thin films | In this paper a new approach to obtain the interface propagation speed in
superconductors by means of a variationalme thod is introduced. The results of
the approach proposed coincide with the numerical simulations. The hyperbolic
differential equations are introduced as an extension of the modelin order to
take into... | cond-mat.supr-con cond-mat.mtrl-sci | in this paper a new approach to obtain the interface propagation speed in superconductors by means of a variationalme thod is introduced the results of the approach proposed coincide with the numerical simulations the hyperbolic differential equations are introduced as an extension of the modelin order to take into acc... | [['in', 'this', 'paper', 'a', 'new', 'approach', 'to', 'obtain', 'the', 'interface', 'propagation', 'speed', 'in', 'superconductors', 'by', 'means', 'of', 'a', 'variationalme', 'thod', 'is', 'introduced', 'the', 'results', 'of', 'the', 'approach', 'proposed', 'coincide', 'with', 'the', 'numerical', 'simulations', 'the'... | [-0.13369724345403514, 0.08087232683465118, -0.09269135429299083, 0.025936684699664855, -0.08900126082629993, -0.06493290085024361, 0.01453992896733388, 0.3124950645041877, -0.27983890049930277, -0.28316479478159856, 0.059739552689154214, -0.257051275637611, -0.1726072878287784, 0.19400950460213012, -0.0467279405003927... |
707.0066 | First detection of galaxy-galaxy-galaxy lensing in RCS. A new tool for
studying the matter environment of galaxy pairs | The weak gravitational lensing effect, small coherent distortions of galaxy
images by means of a gravitational tidal field, can be used to study the
relation between the matter and galaxy distribution. In this context, weak
lensing has so far only been used for considering a second-order correlation
function that rel... | astro-ph | the weak gravitational lensing effect small coherent distortions of galaxy images by means of a gravitational tidal field can be used to study the relation between the matter and galaxy distribution in this context weak lensing has so far only been used for considering a secondorder correlation function that relates th... | [['the', 'weak', 'gravitational', 'lensing', 'effect', 'small', 'coherent', 'distortions', 'of', 'galaxy', 'images', 'by', 'means', 'of', 'a', 'gravitational', 'tidal', 'field', 'can', 'be', 'used', 'to', 'study', 'the', 'relation', 'between', 'the', 'matter', 'and', 'galaxy', 'distribution', 'in', 'this', 'context', '... | [-0.10377217380925739, 0.0415779261206683, -0.11806684584703808, 0.1394044455912366, -0.08770506175636661, -0.07783016670294399, -0.017675935176164642, 0.40386547642741716, -0.22645887088614935, -0.35436238868015946, 0.05974345695702177, -0.29509336265972724, -0.10731192812798362, 0.20757048224354638, 0.019594248588763... |
707.0067 | Multiparticle Production at High Multiplicities | Theoretical and experimental studies of high multiplicity events are
analyzed. Some interesting phenomena can be revealed at high multiplicities.
Preliminary results of project "Thermalization" are reported.
| hep-ph | theoretical and experimental studies of high multiplicity events are analyzed some interesting phenomena can be revealed at high multiplicities preliminary results of project thermalization are reported | [['theoretical', 'and', 'experimental', 'studies', 'of', 'high', 'multiplicity', 'events', 'are', 'analyzed', 'some', 'interesting', 'phenomena', 'can', 'be', 'revealed', 'at', 'high', 'multiplicities', 'preliminary', 'results', 'of', 'project', 'thermalization', 'are', 'reported']] | [-0.162818915837516, 0.19618076625136802, -0.14620899367862597, 0.16443835463947976, -0.05627022579742166, -0.12688999058893666, -0.04211071764047329, 0.41855731327086687, -0.14178605241557726, -0.36729279590340763, 0.09376819417453729, -0.3888724368925278, -0.07662043122512002, 0.27652970023112944, -0.0360385306681004... |
707.0068 | Hot Massive Stars: The Impact of HST | We review the contribution of Hubble Space Telescope to the study of hot,
luminous stars. Optical and IR imaging have permitted spatially resolved
observations of young, massive clusters within Local Group galaxies, such as
R136, NGC 3603 and Arches, revealing unprecedented concentrations of very
massive O stars. UV ... | astro-ph | we review the contribution of hubble space telescope to the study of hot luminous stars optical and ir imaging have permitted spatially resolved observations of young massive clusters within local group galaxies such as r136 ngc 3603 and arches revealing unprecedented concentrations of very massive o stars uv spectrosc... | [['we', 'review', 'the', 'contribution', 'of', 'hubble', 'space', 'telescope', 'to', 'the', 'study', 'of', 'hot', 'luminous', 'stars', 'optical', 'and', 'ir', 'imaging', 'have', 'permitted', 'spatially', 'resolved', 'observations', 'of', 'young', 'massive', 'clusters', 'within', 'local', 'group', 'galaxies', 'such', 'a... | [-0.03768182178288235, 0.09059528795342824, -0.05368356075808869, 0.1002889302333597, -0.13927706260008518, -0.05077297982950666, 0.07568196781986156, 0.4503017864797426, -0.0675091795183672, -0.35338681117741405, -0.040452296685814994, -0.30221363383067645, 0.02154374242939564, 0.17577088942083074, -0.0369991763228816... |
707.0069 | Vibrational spectra of C60C8H8 and C70C8H8 in the rotor-stator and
polymer phases | C60-C8H8 and C70-C8H8 are prototypes of rotor-stator cocrystals. We present
infrared and Raman spectra of these materials and show how the rotor-stator
nature is reflected in their vibrational properties. We measured the
vibrational spectra of the polymer phases poly(C60C8H8) and poly(C70C8H8)
resulting from a solid ... | cond-mat.mtrl-sci | c60c8h8 and c70c8h8 are prototypes of rotorstator cocrystals we present infrared and raman spectra of these materials and show how the rotorstator nature is reflected in their vibrational properties we measured the vibrational spectra of the polymer phases polyc60c8h8 and polyc70c8h8 resulting from a solid state reacti... | [['c60c8h8', 'and', 'c70c8h8', 'are', 'prototypes', 'of', 'rotorstator', 'cocrystals', 'we', 'present', 'infrared', 'and', 'raman', 'spectra', 'of', 'these', 'materials', 'and', 'show', 'how', 'the', 'rotorstator', 'nature', 'is', 'reflected', 'in', 'their', 'vibrational', 'properties', 'we', 'measured', 'the', 'vibrat... | [-0.07674401047963487, 0.16360325100527995, -0.11087948829505045, -0.02758375838469795, -0.012213242293396235, -0.06159979726552316, 0.04707492033839631, 0.4350053833838066, -0.22938274407415124, -0.25284708222455304, 0.05258138319882362, -0.3041188284025892, -0.141740802769124, 0.15028386451202727, -4.7213337181702904... |
707.007 | Quantum subgroups of a simple quantum group at roots of 1 | Let G be a connected, simply connected, simple complex algebraic group and
let e be a primitive l-th root of 1, with l odd and 3 does not divide l if G is
of type G_{2}. We determine all Hopf algebra quotients of the quantized
coordinate algebra of G at e.
| math.QA | let g be a connected simply connected simple complex algebraic group and let e be a primitive lth root of 1 with l odd and 3 does not divide l if g is of type g_2 we determine all hopf algebra quotients of the quantized coordinate algebra of g at e | [['let', 'g', 'be', 'a', 'connected', 'simply', 'connected', 'simple', 'complex', 'algebraic', 'group', 'and', 'let', 'e', 'be', 'a', 'primitive', 'lth', 'root', 'of', '1', 'with', 'l', 'odd', 'and', '3', 'does', 'not', 'divide', 'l', 'if', 'g', 'is', 'of', 'type', 'g_2', 'we', 'determine', 'all', 'hopf', 'algebra', 'q... | [-0.2811290632349019, 0.1448227893013288, -0.080441146203335, -0.0442709157348373, -0.2204238333301071, -0.25364576245420706, -0.029238355656464893, 0.3032306695685667, -0.3539557440169886, -0.22637207495669523, 0.07499218132237301, -0.2470988499037191, -0.09893569352068737, 0.15089521022038718, -0.11509589423589847, -... |
707.0071 | 2+1 Flavor QCD simulated in the epsilon-regime in different topological
sectors | We generated configurations with the parametrized fixed-point Dirac operator
D_{FP} on a (1.6 fm)^4 box at a lattice spacing a=0.13 fm. We compare the
distributions of the three lowest k=1,2,3 eigenvalues in the nu= 0,1,2
topological sectors with that of the Random Matrix Theory predictions. The
ratios of expectation... | hep-lat | we generated configurations with the parametrized fixedpoint dirac operator d_fp on a 16 fm4 box at a lattice spacing a013 fm we compare the distributions of the three lowest k123 eigenvalues in the nu 012 topological sectors with that of the random matrix theory predictions the ratios of expectation values of the lowe... | [['we', 'generated', 'configurations', 'with', 'the', 'parametrized', 'fixedpoint', 'dirac', 'operator', 'd_fp', 'on', 'a', '16', 'fm4', 'box', 'at', 'a', 'lattice', 'spacing', 'a013', 'fm', 'we', 'compare', 'the', 'distributions', 'of', 'the', 'three', 'lowest', 'k123', 'eigenvalues', 'in', 'the', 'nu', '012', 'topolo... | [-0.1273531192230021, 0.20753834760212836, -0.05801013275297319, 0.07958026010013047, 0.036574895731470686, -0.09658737963144766, 0.0749368472445875, 0.34078418786459147, -0.1912820773667339, -0.24837280628816324, 0.048708260423464184, -0.3528284956800177, -0.059045203669155215, 0.10473102200380031, 0.05825751878202279... |
707.0072 | Language simulation after a conquest | When a region is conquered by people speaking another language, we assume
within the Schulze model that at each iteration each person with probability s
shifts to the conquering language. The time needed for the conquering language
to become dominating is about 2/s for directed Barabasi-Albert networks, but
diverges ... | physics.soc-ph | when a region is conquered by people speaking another language we assume within the schulze model that at each iteration each person with probability s shifts to the conquering language the time needed for the conquering language to become dominating is about 2s for directed barabasialbert networks but diverges on the ... | [['when', 'a', 'region', 'is', 'conquered', 'by', 'people', 'speaking', 'another', 'language', 'we', 'assume', 'within', 'the', 'schulze', 'model', 'that', 'at', 'each', 'iteration', 'each', 'person', 'with', 'probability', 's', 'shifts', 'to', 'the', 'conquering', 'language', 'the', 'time', 'needed', 'for', 'the', 'co... | [-0.0860898914388152, 0.1441377506545577, -0.0044233261867136255, 0.09023308874962882, -0.07903578959893985, -0.23552728816103496, 0.09894694283329805, 0.39624466368409456, -0.2731828780569991, -0.2389459949078374, 0.052951705939762415, -0.357258729789345, -0.06871397000905431, 0.12536652581231883, -0.0623215340639915,... |
707.0073 | The Percolation Signature of the Spin Glass Transition | Magnetic ordering at low temperature for Ising ferromagnets manifests itself
within the associated Fortuin-Kasteleyn (FK) random cluster representation as
the occurrence of a single positive density percolating network. In this paper
we investigate the percolation signature for Ising spin glass ordering -- both
in sh... | cond-mat.stat-mech cond-mat.dis-nn | magnetic ordering at low temperature for ising ferromagnets manifests itself within the associated fortuinkasteleyn fk random cluster representation as the occurrence of a single positive density percolating network in this paper we investigate the percolation signature for ising spin glass ordering both in shortrange ... | [['magnetic', 'ordering', 'at', 'low', 'temperature', 'for', 'ising', 'ferromagnets', 'manifests', 'itself', 'within', 'the', 'associated', 'fortuinkasteleyn', 'fk', 'random', 'cluster', 'representation', 'as', 'the', 'occurrence', 'of', 'a', 'single', 'positive', 'density', 'percolating', 'network', 'in', 'this', 'pap... | [-0.10985108833416428, 0.19100327105758694, -0.0526010962008575, 0.07488582304733109, -0.011619478997602625, -0.13008419622314496, 0.04926960975117077, 0.3832332138876313, -0.18637496862307334, -0.2732249105719904, 0.031290400268066926, -0.29960887231728406, -0.15999041674025719, 0.08228749886281717, 0.0873787858121060... |
707.0074 | On the epistemic view of quantum states | We investigate the strengths and limitations of the Spekkens toy model, which
is a local hidden variable model that replicates many important properties of
quantum dynamics. First, we present a set of five axioms that fully encapsulate
Spekkens' toy model. We then test whether these axioms can be extended to
capture ... | quant-ph | we investigate the strengths and limitations of the spekkens toy model which is a local hidden variable model that replicates many important properties of quantum dynamics first we present a set of five axioms that fully encapsulate spekkens toy model we then test whether these axioms can be extended to capture more qu... | [['we', 'investigate', 'the', 'strengths', 'and', 'limitations', 'of', 'the', 'spekkens', 'toy', 'model', 'which', 'is', 'a', 'local', 'hidden', 'variable', 'model', 'that', 'replicates', 'many', 'important', 'properties', 'of', 'quantum', 'dynamics', 'first', 'we', 'present', 'a', 'set', 'of', 'five', 'axioms', 'that'... | [-0.09974874761314975, 0.12183542952854452, -0.11958126246854163, 0.14456741377084684, -0.04993936595750735, -0.2165665340847367, 0.059263623710221695, 0.3404670404457806, -0.2567861654026896, -0.32729291335223304, 0.07950584951791312, -0.2032369891425357, -0.16236574402166493, 0.1906233999304686, -0.09691432931604202,... |
707.0075 | Herman's Theory Revisited | We prove that a $C^{2+\alpha}$-smooth orientation-preserving circle
diffeomorphism with rotation number in Diophantine class $D_\delta$,
$0<\delta<\alpha\le1$, is $C^{1+\alpha-\delta}$-smoothly conjugate to a rigid
rotation. We also derive the most precise version of Denjoy's inequality for
such diffeomorphisms.
| math.DS | we prove that a c2alphasmooth orientationpreserving circle diffeomorphism with rotation number in diophantine class d_delta 0deltaalphale1 is c1alphadeltasmoothly conjugate to a rigid rotation we also derive the most precise version of denjoys inequality for such diffeomorphisms | [['we', 'prove', 'that', 'a', 'c2alphasmooth', 'orientationpreserving', 'circle', 'diffeomorphism', 'with', 'rotation', 'number', 'in', 'diophantine', 'class', 'd_delta', '0deltaalphale1', 'is', 'c1alphadeltasmoothly', 'conjugate', 'to', 'a', 'rigid', 'rotation', 'we', 'also', 'derive', 'the', 'most', 'precise', 'versi... | [-0.23655466029815603, 0.08387213286407517, -0.04609691204898285, 0.05909772223270865, -0.15639337880367582, -0.16159067452518325, 0.009062834041701122, 0.33852140898957395, -0.29432052088492183, -0.25390754267573357, 0.11472569682959918, -0.25277044234628027, -0.13062508596163808, 0.2222145439732368, -0.22651063683301... |
707.0076 | Collision of high-energy closed strings: Formation of a ring-like
apparent horizon | We study collisions of two high-energy closed strings in the framework of
$D$-dimensional general relativity. The model of a high-energy closed string is
introduced as a {/it pp}-wave generated by a ring-shaped source with the radius
$R$. At the instant of the collision, the positions of two strings are assumed
to co... | gr-qc hep-ph hep-th | we study collisions of two highenergy closed strings in the framework of ddimensional general relativity the model of a highenergy closed string is introduced as a it ppwave generated by a ringshaped source with the radius r at the instant of the collision the positions of two strings are assumed to coincide precisely ... | [['we', 'study', 'collisions', 'of', 'two', 'highenergy', 'closed', 'strings', 'in', 'the', 'framework', 'of', 'ddimensional', 'general', 'relativity', 'the', 'model', 'of', 'a', 'highenergy', 'closed', 'string', 'is', 'introduced', 'as', 'a', 'it', 'ppwave', 'generated', 'by', 'a', 'ringshaped', 'source', 'with', 'the... | [-0.22312709098473063, 0.12003445443627023, -0.03932866018972006, 0.10197964407953208, -0.012040740606407153, -0.14860427326940256, -0.06268101130323163, 0.342449783726499, -0.23565876052297394, -0.24397731764976674, 0.11401578808717172, -0.2709255979171601, -0.08455019551489888, 0.1778157063454775, -0.0155519514880544... |
707.0077 | Finite Sections of Weighted Carleman's Inequality | We study finite sections of weighted Carleman's inequality following the
approach of De Bruijn. Similar to the unweighted case, we obtain an asymptotic
expression for the optimal constant.
| math.CA | we study finite sections of weighted carlemans inequality following the approach of de bruijn similar to the unweighted case we obtain an asymptotic expression for the optimal constant | [['we', 'study', 'finite', 'sections', 'of', 'weighted', 'carlemans', 'inequality', 'following', 'the', 'approach', 'of', 'de', 'bruijn', 'similar', 'to', 'the', 'unweighted', 'case', 'we', 'obtain', 'an', 'asymptotic', 'expression', 'for', 'the', 'optimal', 'constant']] | [-0.11324428287168432, 0.016472189775023644, -0.13383248514894927, 0.16690736202456588, -0.07348075206391513, -0.11360306069920105, 0.049464772388871224, 0.3102307309662657, -0.22693206622664416, -0.27734211060617653, 0.054713939615924446, -0.2777635408565402, -0.16805070878139564, 0.19291064206377737, -0.1251340132605... |
707.0078 | Herman's Theory Revisited (Extension) | We prove that a $C^{3+\beta}$-smooth orientation-preserving circle
diffeomorphism with rotation number in Diophantine class $D_\delta$,
$0<\beta<\delta<1$, is $C^{2+\beta-\delta}$-smoothly conjugate to a rigid
rotation.
| math.DS | we prove that a c3betasmooth orientationpreserving circle diffeomorphism with rotation number in diophantine class d_delta 0betadelta1 is c2betadeltasmoothly conjugate to a rigid rotation | [['we', 'prove', 'that', 'a', 'c3betasmooth', 'orientationpreserving', 'circle', 'diffeomorphism', 'with', 'rotation', 'number', 'in', 'diophantine', 'class', 'd_delta', '0betadelta1', 'is', 'c2betadeltasmoothly', 'conjugate', 'to', 'a', 'rigid', 'rotation']] | [-0.31320358281955124, 0.13810044364072382, -0.038431855384260416, 0.002742986852535978, -0.2011212246492505, -0.16315846373327075, 0.00743340440094471, 0.3798925306648016, -0.338155634701252, -0.2411919854581356, 0.06933417369727976, -0.23434625752270222, -0.12518482338637113, 0.18526443764567374, -0.2777413298375905,... |
707.0079 | Five-quark picture of Lambda(1405) in anisotropic lattice QCD | Five-quark (5Q) picture of Lambda(1405) is studied using quenched lattice QCD
with an exotic 5Q operator of N\bar{K} type. To discreminate mere N\bar{K} and
\Sigma\pi scattering states, Hybrid Boundary Condition (HBC), a
flavor-dependent boundary condition, is imposed on the quark fields along
spatial direction. 5Q m... | hep-lat | fivequark 5q picture of lambda1405 is studied using quenched lattice qcd with an exotic 5q operator of nbark type to discreminate mere nbark and sigmapi scattering states hybrid boundary condition hbc a flavordependent boundary condition is imposed on the quark fields along spatial direction 5q mass m_5qsimeq 189 gev i... | [['fivequark', '5q', 'picture', 'of', 'lambda1405', 'is', 'studied', 'using', 'quenched', 'lattice', 'qcd', 'with', 'an', 'exotic', '5q', 'operator', 'of', 'nbark', 'type', 'to', 'discreminate', 'mere', 'nbark', 'and', 'sigmapi', 'scattering', 'states', 'hybrid', 'boundary', 'condition', 'hbc', 'a', 'flavordependent', ... | [-0.12189454447026506, 0.2608255511834733, -0.1272443990514736, 0.11069876496060375, -0.0839914038513947, -0.14647023069361845, 0.08511555993299216, 0.3593640082487554, -0.15784266369059832, -0.20258820050330173, 0.009225806400104605, -0.2504499289724562, -0.0064652465246241506, 0.017168593545905268, 0.0578471981150667... |
707.008 | Component sizes in networks with arbitrary degree distributions | We give an exact solution for the complete distribution of component sizes in
random networks with arbitrary degree distributions. The solution tells us the
probability that a randomly chosen node belongs to a component of size s, for
any s. We apply our results to networks with the three most commonly studied
degree... | cond-mat.stat-mech cond-mat.dis-nn | we give an exact solution for the complete distribution of component sizes in random networks with arbitrary degree distributions the solution tells us the probability that a randomly chosen node belongs to a component of size s for any s we apply our results to networks with the three most commonly studied degree dist... | [['we', 'give', 'an', 'exact', 'solution', 'for', 'the', 'complete', 'distribution', 'of', 'component', 'sizes', 'in', 'random', 'networks', 'with', 'arbitrary', 'degree', 'distributions', 'the', 'solution', 'tells', 'us', 'the', 'probability', 'that', 'a', 'randomly', 'chosen', 'node', 'belongs', 'to', 'a', 'component... | [-0.10509531517477276, 0.09216715150463502, -0.11091622535067681, 0.048737038816146265, -0.024563366615285093, -0.12308846458147925, 0.044833048682015104, 0.3580575998299397, -0.2320976272556716, -0.2526979014098358, 0.07241426382410841, -0.2867708269148492, -0.12855670208183045, 0.1332753197863125, -0.0003504732695336... |
707.0081 | Higher Derivative Corrections in Holographic QCD | We consider the effect of the R^4 term in type IIA string theory on the
supergravity background dual to N_c D4 branes compactified on a circle with
supersymmetry breaking boundary conditions. We study the dynamics of D8 branes
in this perturbed geometry in the probe approximation. This leads to an
analysis of higher ... | hep-th | we consider the effect of the r4 term in type iia string theory on the supergravity background dual to n_c d4 branes compactified on a circle with supersymmetry breaking boundary conditions we study the dynamics of d8 branes in this perturbed geometry in the probe approximation this leads to an analysis of higher deriv... | [['we', 'consider', 'the', 'effect', 'of', 'the', 'r4', 'term', 'in', 'type', 'iia', 'string', 'theory', 'on', 'the', 'supergravity', 'background', 'dual', 'to', 'n_c', 'd4', 'branes', 'compactified', 'on', 'a', 'circle', 'with', 'supersymmetry', 'breaking', 'boundary', 'conditions', 'we', 'study', 'the', 'dynamics', '... | [-0.1317148164145375, 0.16216217803060176, -0.061377381498993744, 0.1407594575756016, -0.0680085693490307, -0.11326706194139402, 0.028359048623899253, 0.2759764534805756, -0.13508940364208516, -0.2394509327452664, 0.07089599158290193, -0.325544213833407, -0.09148822023176563, 0.0610453949711465, -0.07064646679786282, 0... |
707.0082 | Minimax Robust Function Reconstruction in Reproducing Kernel Hilbert
Spaces | In this paper, we present a unified approach to function approximation in
reproducing kernel Hilbert spaces (RKHS) that establishes a previously
unrecognized optimality property for several well-known function approximation
techniques, such as minimum-norm interpolation, smoothing splines, and
pseudo-inverses. We con... | math.ST stat.TH | in this paper we present a unified approach to function approximation in reproducing kernel hilbert spaces rkhs that establishes a previously unrecognized optimality property for several wellknown function approximation techniques such as minimumnorm interpolation smoothing splines and pseudoinverses we consider the pr... | [['in', 'this', 'paper', 'we', 'present', 'a', 'unified', 'approach', 'to', 'function', 'approximation', 'in', 'reproducing', 'kernel', 'hilbert', 'spaces', 'rkhs', 'that', 'establishes', 'a', 'previously', 'unrecognized', 'optimality', 'property', 'for', 'several', 'wellknown', 'function', 'approximation', 'techniques... | [-0.05785475945388282, -0.005162001606362332, -0.11586294998244948, 0.13809814706991938, -0.09413941897060504, -0.12294207769174288, 0.06393726799747605, 0.3922514741559031, -0.3063999416328358, -0.24205287316350216, 0.148708714337581, -0.24818169617307906, -0.17441826159177992, 0.18300874616972493, -0.1203944894103768... |
707.0083 | On Sound Reflection in Superfluid | We consider reflection of the first and the second sound waves by a rigid
flat wall in superfluid. Nontrivial dependence of the reflection coefficients
on the angle of incidence is obtained. Sound conversion is predicted at slanted
incidence.
| cond-mat.supr-con cond-mat.soft | we consider reflection of the first and the second sound waves by a rigid flat wall in superfluid nontrivial dependence of the reflection coefficients on the angle of incidence is obtained sound conversion is predicted at slanted incidence | [['we', 'consider', 'reflection', 'of', 'the', 'first', 'and', 'the', 'second', 'sound', 'waves', 'by', 'a', 'rigid', 'flat', 'wall', 'in', 'superfluid', 'nontrivial', 'dependence', 'of', 'the', 'reflection', 'coefficients', 'on', 'the', 'angle', 'of', 'incidence', 'is', 'obtained', 'sound', 'conversion', 'is', 'predic... | [-0.19495139962160274, 0.20823137592034122, -0.05098747303954473, -0.005581972354679908, -0.14801906289434746, -0.07555082054367583, 0.029356880187007942, 0.39800590725223484, -0.26442938082312284, -0.2299442688879361, 0.09005602740523357, -0.27327688606946093, -0.10157616870281727, 0.19350029577157998, -0.006390275360... |
707.0084 | Gallai Multigraphs | A complete edge-colored graph or multigraph is called Gallai if it lacks
rainbow triangles. We give a construction of all finite Gallai multigraphs.
| math.CO | a complete edgecolored graph or multigraph is called gallai if it lacks rainbow triangles we give a construction of all finite gallai multigraphs | [['a', 'complete', 'edgecolored', 'graph', 'or', 'multigraph', 'is', 'called', 'gallai', 'if', 'it', 'lacks', 'rainbow', 'triangles', 'we', 'give', 'a', 'construction', 'of', 'all', 'finite', 'gallai', 'multigraphs']] | [-0.24562458511765883, 0.16232125230295502, -0.11457648986707562, 0.13931601197438556, -0.3058635394655816, -0.1771492127572065, 0.038268210366368294, 0.46173676135747327, -0.20218047272899878, -0.30206836006887583, 0.06905621114824696, -0.38427469652632007, -0.20220862556775304, -0.07473340489820618, -0.25704032004527... |
707.0085 | First Measurement of the W Boson Mass in Run II of the Tevatron | We present a measurement of the W boson mass using 200/pb of data collected
in pbar p collisions at sqrt(s) = 1.96 TeV by the CDF II detector at Run II of
the Fermilab Tevatron. With a sample of 63964 W -> e nu candidates and 51128 W
-> mu nu candidates, we measure M_W = (80413 +- 34 (stat) +- 34 (syst) = 80413
+- 48... | hep-ex | we present a measurement of the w boson mass using 200pb of data collected in pbar p collisions at sqrts 196 tev by the cdf ii detector at run ii of the fermilab tevatron with a sample of 63964 w e nu candidates and 51128 w mu nu candidates we measure m_w 80413 34 stat 34 syst 80413 48 mevc2 this is the most precise si... | [['we', 'present', 'a', 'measurement', 'of', 'the', 'w', 'boson', 'mass', 'using', '200pb', 'of', 'data', 'collected', 'in', 'pbar', 'p', 'collisions', 'at', 'sqrts', '196', 'tev', 'by', 'the', 'cdf', 'ii', 'detector', 'at', 'run', 'ii', 'of', 'the', 'fermilab', 'tevatron', 'with', 'a', 'sample', 'of', '63964', 'w', 'e... | [-0.06593536376021802, 0.1899894275314485, -0.056427162117971524, 0.044256597912559904, -0.012772175108289553, -0.20396534854080528, 0.1071395183680579, 0.27731819932038587, -0.1428910336964893, -0.3986528680090689, -0.04868860108035733, -0.4235442362777475, 0.19305540627101436, 0.1431558484295642, 0.05557877822623899,... |
707.0086 | Exploiting Nonlinear Recurrence and Fractal Scaling Properties for Voice
Disorder Detection | Voice disorders affect patients profoundly, and acoustic tools can
potentially measure voice function objectively. Nonetheless, existing tools are
limited to analysing voices displaying near periodicity, and do not account for
inherent biophysical nonlinearity and non-Gaussian randomness. They do not
directly measure... | nlin.CG nlin.CD | voice disorders affect patients profoundly and acoustic tools can potentially measure voice function objectively nonetheless existing tools are limited to analysing voices displaying near periodicity and do not account for inherent biophysical nonlinearity and nongaussian randomness they do not directly measure complex... | [['voice', 'disorders', 'affect', 'patients', 'profoundly', 'and', 'acoustic', 'tools', 'can', 'potentially', 'measure', 'voice', 'function', 'objectively', 'nonetheless', 'existing', 'tools', 'are', 'limited', 'to', 'analysing', 'voices', 'displaying', 'near', 'periodicity', 'and', 'do', 'not', 'account', 'for', 'inhe... | [-0.059729147729064735, 0.11619688120471047, -0.06485884011323963, 0.1408306239592743, -0.15276463186102254, -0.22315072110421688, 0.03997459721036389, 0.395436409611388, -0.28552390449414294, -0.294129446693114, 0.0930479822480785, -0.25450395239251, -0.18417219994589687, 0.2917535928904337, -0.1460954192493643, 0.108... |
707.0087 | Orthogonal Systems in Finite Graphs | Given a finite graph G there is a corresponding group given by the
presentation with generators the vertices of G and a relation [x,y]=1 for
generators x and y precisely when (x,y) is an edge of G. Such groups are known
as partially commutative groups (or right-angled Artin groups). In this paper
we construct orthogo... | math.GR | given a finite graph g there is a corresponding group given by the presentation with generators the vertices of g and a relation xy1 for generators x and y precisely when xy is an edge of g such groups are known as partially commutative groups or rightangled artin groups in this paper we construct orthogonality theory ... | [['given', 'a', 'finite', 'graph', 'g', 'there', 'is', 'a', 'corresponding', 'group', 'given', 'by', 'the', 'presentation', 'with', 'generators', 'the', 'vertices', 'of', 'g', 'and', 'a', 'relation', 'xy1', 'for', 'generators', 'x', 'and', 'y', 'precisely', 'when', 'xy', 'is', 'an', 'edge', 'of', 'g', 'such', 'groups',... | [-0.17601284752194973, 0.1379830865494707, -0.0843505998061079, 0.048545517468997074, -0.08848488915448441, -0.12233280503373269, 0.021917238405085696, 0.4144608633106817, -0.3368599516056154, -0.25794183890051814, 0.1067356328181315, -0.29449376427447016, -0.1272064795763151, 0.1480677182477413, -0.13118406487679432, ... |
707.0088 | Perverse coherent sheaves and the geometry of special pieces in the
unipotent variety | Let X be a scheme of finite type over a Noetherian base scheme S admitting a
dualizing complex, and let U be an open subset whose complement has codimension
at least 2. We extend the Deligne-Bezrukavnikov theory of perverse coherent
sheaves by showing that a coherent middle extension (or intersection
cohomology) func... | math.RT math.AG | let x be a scheme of finite type over a noetherian base scheme s admitting a dualizing complex and let u be an open subset whose complement has codimension at least 2 we extend the delignebezrukavnikov theory of perverse coherent sheaves by showing that a coherent middle extension or intersection cohomology functor fro... | [['let', 'x', 'be', 'a', 'scheme', 'of', 'finite', 'type', 'over', 'a', 'noetherian', 'base', 'scheme', 's', 'admitting', 'a', 'dualizing', 'complex', 'and', 'let', 'u', 'be', 'an', 'open', 'subset', 'whose', 'complement', 'has', 'codimension', 'at', 'least', '2', 'we', 'extend', 'the', 'delignebezrukavnikov', 'theory'... | [-0.19610721618552499, 0.03971971479396588, -0.13471426901772685, 0.05169530950911294, -0.10725860418095397, -0.16242887543530782, 0.016938723770938486, 0.3365272693828339, -0.36533002291974254, -0.16087225474066424, 0.08593151813356559, -0.18587458140928595, -0.12525764689473065, 0.2151837559542024, -0.205553803373423... |
707.0089 | Bayesian estimates of free energies from nonequilibrium work data in the
presence of instrument noise | The Jarzynski equality and the fluctuation theorem relate equilibrium free
energy differences to non-equilibrium measurements of the work. These relations
extend to single-molecule experiments that have probed the finite-time
thermodynamics of proteins and nucleic acids. The effects of experimental error
and instrume... | cond-mat.stat-mech cond-mat.soft | the jarzynski equality and the fluctuation theorem relate equilibrium free energy differences to nonequilibrium measurements of the work these relations extend to singlemolecule experiments that have probed the finitetime thermodynamics of proteins and nucleic acids the effects of experimental error and instrument nois... | [['the', 'jarzynski', 'equality', 'and', 'the', 'fluctuation', 'theorem', 'relate', 'equilibrium', 'free', 'energy', 'differences', 'to', 'nonequilibrium', 'measurements', 'of', 'the', 'work', 'these', 'relations', 'extend', 'to', 'singlemolecule', 'experiments', 'that', 'have', 'probed', 'the', 'finitetime', 'thermody... | [-0.08875848600814024, 0.14349815263174093, -0.12011124276651595, 0.07778196615086366, -0.0223788528655393, -0.17269504447885525, 0.07006493593246724, 0.374059396258627, -0.2449450591394009, -0.3018634462179109, 0.06335934109012716, -0.3033755372982854, -0.12951947867650931, 0.24760668598957217, -0.027969985233189967, ... |
707.009 | Calculation of local Fourier transforms for formal connections | We calculate the local Fourier transforms for formal connections. In
particular, we verify an analogous conjecture suggested in Laumon's paper:
"Transformation de Fourier, constantes d'equations fonctionnelles et conjecture
de Weil, 2.6.3".
| math.AG | we calculate the local fourier transforms for formal connections in particular we verify an analogous conjecture suggested in laumons paper transformation de fourier constantes dequations fonctionnelles et conjecture de weil 263 | [['we', 'calculate', 'the', 'local', 'fourier', 'transforms', 'for', 'formal', 'connections', 'in', 'particular', 'we', 'verify', 'an', 'analogous', 'conjecture', 'suggested', 'in', 'laumons', 'paper', 'transformation', 'de', 'fourier', 'constantes', 'dequations', 'fonctionnelles', 'et', 'conjecture', 'de', 'weil', '26... | [-0.1678989372486549, 0.014395457952031716, -0.22207700280893233, 0.11840380620091193, -0.14901690611675864, -0.06716563174080464, -0.05629262799442175, 0.2479206377850665, -0.25649305789791527, -0.21904203343775966, 0.0175972007620599, -0.20895445838029827, -0.26218314595039816, 0.18757291678940097, -0.211229506940130... |
707.0091 | Unheeded pseudo solution of Dirac-Coulomb equations with an indirect
transformation of functions | We open out one of incorrect solutions of the Driac equation in the Coulomb
field given in a published paper. By introducing a transformation of function,
the paper transformed the original radial first-order Dirac-Coulomb equation
into two second-order Dirac-Coulomb equation. However, each of the second-order
differ... | physics.gen-ph | we open out one of incorrect solutions of the driac equation in the coulomb field given in a published paper by introducing a transformation of function the paper transformed the original radial firstorder diraccoulomb equation into two secondorder diraccoulomb equation however each of the secondorder differential equa... | [['we', 'open', 'out', 'one', 'of', 'incorrect', 'solutions', 'of', 'the', 'driac', 'equation', 'in', 'the', 'coulomb', 'field', 'given', 'in', 'a', 'published', 'paper', 'by', 'introducing', 'a', 'transformation', 'of', 'function', 'the', 'paper', 'transformed', 'the', 'original', 'radial', 'firstorder', 'diraccoulomb... | [-0.1460266932658851, 0.01837901313090697, -0.1150720469094813, 0.06495607488012563, -0.0913584967656061, -0.13504277777547638, -0.011907806190817306, 0.23033570225040118, -0.28406207184617716, -0.28423043398186565, 0.0725717200168098, -0.3260878234108289, -0.1379860400656859, 0.15540568283448616, -0.006976528391242027... |
707.0092 | More Meta-Stable Brane Configurations without D6-Branes | We describe the intersecting brane configurations, consisting of NS-branes,
D4-branes(and anti-D4-branes), in type IIA string theory corresponding to the
meta-stable nonsupersymmetric vacua of N=1 SU(N_c) x SU(N_c') x SU(N_c'') gauge
theory with bifundamentals. By adding the orientifold 4-plane to these brane
configu... | hep-th | we describe the intersecting brane configurations consisting of nsbranes d4branesand antid4branes in type iia string theory corresponding to the metastable nonsupersymmetric vacua of n1 sun_c x sun_c x sun_c gauge theory with bifundamentals by adding the orientifold 4plane to these brane configurations we also discuss ... | [['we', 'describe', 'the', 'intersecting', 'brane', 'configurations', 'consisting', 'of', 'nsbranes', 'd4branesand', 'antid4branes', 'in', 'type', 'iia', 'string', 'theory', 'corresponding', 'to', 'the', 'metastable', 'nonsupersymmetric', 'vacua', 'of', 'n1', 'sun_c', 'x', 'sun_c', 'x', 'sun_c', 'gauge', 'theory', 'wit... | [-0.15396078733297494, 0.26297336995589715, -0.012354794181495285, 0.14076087494882253, -0.06737366347955778, -0.2476794722203452, 0.028096194080530833, 0.3194271536687246, -0.059822892173169516, -0.23346829939729127, 0.04787254012756957, -0.29764869058122617, -0.11444658784864423, -0.04679507433842772, -0.105862358083... |
707.0093 | Maximum overhang | How far can a stack of $n$ identical blocks be made to hang over the edge of
a table? The question dates back to at least the middle of the 19th century and
the answer to it was widely believed to be of order $\log n$. Recently,
Paterson and Zwick constructed $n$-block stacks with overhangs of order
$n^{1/3}$, expone... | math.HO math-ph math.CO math.MP | how far can a stack of n identical blocks be made to hang over the edge of a table the question dates back to at least the middle of the 19th century and the answer to it was widely believed to be of order log n recently paterson and zwick constructed nblock stacks with overhangs of order n13 exponentially better than ... | [['how', 'far', 'can', 'a', 'stack', 'of', 'n', 'identical', 'blocks', 'be', 'made', 'to', 'hang', 'over', 'the', 'edge', 'of', 'a', 'table', 'the', 'question', 'dates', 'back', 'to', 'at', 'least', 'the', 'middle', 'of', 'the', '19th', 'century', 'and', 'the', 'answer', 'to', 'it', 'was', 'widely', 'believed', 'to', '... | [-0.08809788277306195, 0.1053589030967227, -0.06324406258118827, 0.08066866274817758, -0.07451633592843011, -0.1535143693909049, 0.08225588653156246, 0.3411543123157961, -0.2989498358330734, -0.376473334440518, 0.1219043382720667, -0.29774804588495973, -0.1269200239385966, 0.17148124775294923, -0.08742006588450056, 0.0... |
707.0094 | Study of the linear ablation growth rate for the quasi isobaric model of
Euler equations with thermal conductivity | In this paper, we study a linear system related to the 2d system of Euler
equations with thermal conduction in the quasi-isobaric approximation of
Kull-Anisimov [14]. This model is used for the study of the ablation front
instability, which appears in the problem of inertial confinement fusion. This
physical system c... | math.AP | in this paper we study a linear system related to the 2d system of euler equations with thermal conduction in the quasiisobaric approximation of kullanisimov 14 this model is used for the study of the ablation front instability which appears in the problem of inertial confinement fusion this physical system contains a ... | [['in', 'this', 'paper', 'we', 'study', 'a', 'linear', 'system', 'related', 'to', 'the', '2d', 'system', 'of', 'euler', 'equations', 'with', 'thermal', 'conduction', 'in', 'the', 'quasiisobaric', 'approximation', 'of', 'kullanisimov', '14', 'this', 'model', 'is', 'used', 'for', 'the', 'study', 'of', 'the', 'ablation', ... | [-0.1751105977377544, 0.10020143218852658, -0.06360229689317445, 0.002523866752938678, -0.0008857480405519406, -0.13411745443629722, -0.006703944213222712, 0.283942716481785, -0.30276641321058073, -0.24342449940741062, 0.09532254566128055, -0.3043398524494842, -0.13819464552526672, 0.17816553308162839, -0.0254488880701... |
707.0095 | On Bernoulli Decompositions for Random Variables, Concentration Bounds,
and Spectral Localization | As was noted already by A. N. Kolmogorov, any random variable has a Bernoulli
component. This observation provides a tool for the extension of results which
are known for Bernoulli random variables to arbitrary distributions. Two
applications are provided here: i. an anti-concentration bound for a class of
functions ... | math.PR math-ph math.MP | as was noted already by a n kolmogorov any random variable has a bernoulli component this observation provides a tool for the extension of results which are known for bernoulli random variables to arbitrary distributions two applications are provided here i an anticoncentration bound for a class of functions of indepen... | [['as', 'was', 'noted', 'already', 'by', 'a', 'n', 'kolmogorov', 'any', 'random', 'variable', 'has', 'a', 'bernoulli', 'component', 'this', 'observation', 'provides', 'a', 'tool', 'for', 'the', 'extension', 'of', 'results', 'which', 'are', 'known', 'for', 'bernoulli', 'random', 'variables', 'to', 'arbitrary', 'distribu... | [-0.09207928246663262, 0.17854924786976578, -0.08712827397199968, 0.07545624266106946, -0.08862298261956311, -0.18677804379646357, 0.054897245969429305, 0.3460621326851348, -0.280866840078185, -0.23471123916873088, 0.12420109248293253, -0.24953533395892008, -0.14473772647518976, 0.21306477643665858, -0.0638302606588695... |
707.0096 | Coherent optical phase transfer over a 32-km fiber with 1-s instability
at $10^{-17}$ | The phase coherence of an ultrastable optical frequency reference is fully
maintained over actively stabilized fiber networks of lengths exceeding 30 km.
For a 7-km link installed in an urban environment, the transfer instability is
$6 \times 10^{-18}$ at 1-s. The excess phase noise of 0.15 rad, integrated from
8 mHz... | physics.atom-ph physics.optics | the phase coherence of an ultrastable optical frequency reference is fully maintained over actively stabilized fiber networks of lengths exceeding 30 km for a 7km link installed in an urban environment the transfer instability is 6 times 1018 at 1s the excess phase noise of 015 rad integrated from 8 mhz to 25 mhz yield... | [['the', 'phase', 'coherence', 'of', 'an', 'ultrastable', 'optical', 'frequency', 'reference', 'is', 'fully', 'maintained', 'over', 'actively', 'stabilized', 'fiber', 'networks', 'of', 'lengths', 'exceeding', '30', 'km', 'for', 'a', '7km', 'link', 'installed', 'in', 'an', 'urban', 'environment', 'the', 'transfer', 'ins... | [-0.217175808303485, 0.21254034414384174, -0.020326794270658866, -0.035596694010261366, 0.0516446748636857, -0.16237414003019998, 0.11226489736751925, 0.49634938811747514, -0.200350064112475, -0.31013636733890354, 0.10027902085736666, -0.26593350326099124, 0.011310127350346496, 0.28132367694828037, -0.06724779382542086... |
707.0097 | Metal-less Metamaterial for Surface Plasmon Polariton guiding and
amplification | We propose a novel metamaterial for Surface Plasmon Polarition guiding,
amplification and modulation. Specific example of AlN/GaN Quantum Cascade
Amplifier and its dispersion engineering are studied in details. The general
original concept of metamaterials based on inclusions of low-dimensional
quantum structures (ar... | cond-mat.mtrl-sci | we propose a novel metamaterial for surface plasmon polarition guiding amplification and modulation specific example of alngan quantum cascade amplifier and its dispersion engineering are studied in details the general original concept of metamaterials based on inclusions of lowdimensional quantum structures artificial... | [['we', 'propose', 'a', 'novel', 'metamaterial', 'for', 'surface', 'plasmon', 'polarition', 'guiding', 'amplification', 'and', 'modulation', 'specific', 'example', 'of', 'alngan', 'quantum', 'cascade', 'amplifier', 'and', 'its', 'dispersion', 'engineering', 'are', 'studied', 'in', 'details', 'the', 'general', 'original... | [-0.17774361251956886, 0.1787552413220207, -0.018962821850760116, 0.03647937427999245, -0.11825170061654515, -0.19158405092829425, 0.004807111672643158, 0.454773362312052, -0.24421788134301703, -0.24523676686092383, 0.007931851900907026, -0.24199477071977324, -0.2961666822847393, 0.24843523324363762, -0.049681514398091... |
707.0098 | A multi-dimensional Markov chain and the Meixner ensemble | We show that the transition probability of the Markoc chain
$(G(j,1),...,G(j,n))_{j\ge 1}$, where the $G(i,j)'s$ are certain directed
last-passage times, is given by a determinant of a special form. An analogous
formula has recently been obtained by Warren in a Brownian motion model.
Furthermore we demonstrate that t... | math.PR math-ph math.MP | we show that the transition probability of the markoc chain gj1gjn_jge 1 where the gijs are certain directed lastpassage times is given by a determinant of a special form an analogous formula has recently been obtained by warren in a brownian motion model furthermore we demonstrate that this formula leads to the meixne... | [['we', 'show', 'that', 'the', 'transition', 'probability', 'of', 'the', 'markoc', 'chain', 'gj1gjn_jge', '1', 'where', 'the', 'gijs', 'are', 'certain', 'directed', 'lastpassage', 'times', 'is', 'given', 'by', 'a', 'determinant', 'of', 'a', 'special', 'form', 'an', 'analogous', 'formula', 'has', 'recently', 'been', 'ob... | [-0.08696668862532346, 0.09591133335701531, -0.12819478363515094, 0.06484294479014352, -0.043449471346460856, -0.09420273527025412, 0.014598337484177394, 0.378608274870576, -0.25978061532936036, -0.2330792760118269, 0.08375163805426265, -0.261766351475858, -0.23921746497926039, 0.15991815117199737, -0.05939205575925417... |
707.0099 | Energy distributions from three-body decaying many-body resonances | We compute energy distributions of three particles emerging from decaying
many-body resonances. We reproduce the measured energy distributions from
decays of two archetypal states chosen as the lowest $0^{+}$ and
$1^{+}$-resonances in $^{12}$C populated in $\beta$-decays. These states are
dominated by sequential, thr... | nucl-th | we compute energy distributions of three particles emerging from decaying manybody resonances we reproduce the measured energy distributions from decays of two archetypal states chosen as the lowest 0 and 1resonances in 12c populated in betadecays these states are dominated by sequential through the 8be ground state an... | [['we', 'compute', 'energy', 'distributions', 'of', 'three', 'particles', 'emerging', 'from', 'decaying', 'manybody', 'resonances', 'we', 'reproduce', 'the', 'measured', 'energy', 'distributions', 'from', 'decays', 'of', 'two', 'archetypal', 'states', 'chosen', 'as', 'the', 'lowest', '0', 'and', '1resonances', 'in', '1... | [-0.05915718782056548, 0.28648372687387597, -0.06389409733665045, 0.1768453833470239, 0.04573209386295344, -0.09944223822389223, 0.019705931832896, 0.3568802746248585, -0.28512454505632573, -0.2921797334676302, -0.016296180208284362, -0.35081803698469943, 0.005354856765999229, 0.10956284141498088, 0.13121847046798543, ... |
707.01 | On the One-Dimensional Optimal Switching Problem | We explicitly solve the optimal switching problem for one-dimensional
diffusions by directly employing the dynamic programming principle and the
excessive characterization of the value function. The shape of the value
function and the smooth fit principle then can be proved using the properties
of concave functions.
| math.OC math.PR | we explicitly solve the optimal switching problem for onedimensional diffusions by directly employing the dynamic programming principle and the excessive characterization of the value function the shape of the value function and the smooth fit principle then can be proved using the properties of concave functions | [['we', 'explicitly', 'solve', 'the', 'optimal', 'switching', 'problem', 'for', 'onedimensional', 'diffusions', 'by', 'directly', 'employing', 'the', 'dynamic', 'programming', 'principle', 'and', 'the', 'excessive', 'characterization', 'of', 'the', 'value', 'function', 'the', 'shape', 'of', 'the', 'value', 'function', ... | [-0.04351158861232841, 0.025076923304763826, -0.11770177102121322, 0.07913303529114826, -0.1106186312339876, -0.10846255464560312, 0.06344147236592582, 0.3566007236747638, -0.3911847404163817, -0.3018922382844207, 0.15160965719057815, -0.20615972928783816, -0.1696207692603702, 0.19353697363935088, -0.03279634917397862,... |
707.0101 | Sakai-Sugimoto Brane System at High Density | The D4-D8 brane system of Sakai-Sugimoto model at high quark density is
studied in the weak coupling regime. We show that the color superconducting
phase (for Nc~3) or the chiral density wave (for Nc->infinity) disappears at
very large chemical potential, or equivalently at very large compactified
dimension that the ... | hep-th | the d4d8 brane system of sakaisugimoto model at high quark density is studied in the weak coupling regime we show that the color superconducting phase for nc3 or the chiral density wave for ncinfinity disappears at very large chemical potential or equivalently at very large compactified dimension that the model possess... | [['the', 'd4d8', 'brane', 'system', 'of', 'sakaisugimoto', 'model', 'at', 'high', 'quark', 'density', 'is', 'studied', 'in', 'the', 'weak', 'coupling', 'regime', 'we', 'show', 'that', 'the', 'color', 'superconducting', 'phase', 'for', 'nc3', 'or', 'the', 'chiral', 'density', 'wave', 'for', 'ncinfinity', 'disappears', '... | [-0.17008045964888227, 0.23338500463139655, -0.05531528393334862, 0.07166813307879631, -0.01621357120100909, -0.16468865788583434, 0.057513918644234316, 0.3448430024914499, -0.17100695193981502, -0.22918121669608266, 0.04961210957540672, -0.2882907903238909, -0.08382591619781816, 0.08173303985829229, 0.0594023334613042... |
707.0102 | Markov type of Alexandrov spaces of nonnegative curvature | We prove that Alexandrov spaces $X$ of nonnegative curvature have Markov type
2 in the sense of Ball. As a corollary, any Lipschitz continuous map from a
subset of $X$ into a 2-uniformly convex Banach space is extended as a Lipschitz
continuous map on the entire space $X$.
| math.MG math.FA | we prove that alexandrov spaces x of nonnegative curvature have markov type 2 in the sense of ball as a corollary any lipschitz continuous map from a subset of x into a 2uniformly convex banach space is extended as a lipschitz continuous map on the entire space x | [['we', 'prove', 'that', 'alexandrov', 'spaces', 'x', 'of', 'nonnegative', 'curvature', 'have', 'markov', 'type', '2', 'in', 'the', 'sense', 'of', 'ball', 'as', 'a', 'corollary', 'any', 'lipschitz', 'continuous', 'map', 'from', 'a', 'subset', 'of', 'x', 'into', 'a', '2uniformly', 'convex', 'banach', 'space', 'is', 'ext... | [-0.09851644636364654, 0.057713520499722414, -0.08012127670129605, 0.08838773640309228, -0.08585767447948456, -0.10379037540405989, 0.05245040168908114, 0.433818387798965, -0.3708800224509711, -0.07399963630208124, 0.18204758413048694, -0.24831091655263057, -0.12021185917546973, 0.1817173645249568, -0.15211175517955175... |
707.0103 | Simulation of the Polarized Fermion Decay | In this paper the modification of the method conventionally used for the
modeling of the massive fermions production and decays is proposed. The step by
step algorithm is presented. Under the strict conditions the proposed method of
modeling allow distinctly raise the efficiency of the computations.
| hep-ph | in this paper the modification of the method conventionally used for the modeling of the massive fermions production and decays is proposed the step by step algorithm is presented under the strict conditions the proposed method of modeling allow distinctly raise the efficiency of the computations | [['in', 'this', 'paper', 'the', 'modification', 'of', 'the', 'method', 'conventionally', 'used', 'for', 'the', 'modeling', 'of', 'the', 'massive', 'fermions', 'production', 'and', 'decays', 'is', 'proposed', 'the', 'step', 'by', 'step', 'algorithm', 'is', 'presented', 'under', 'the', 'strict', 'conditions', 'the', 'pro... | [-0.06604223871988285, 0.05691414954059798, -0.11510930281213444, 0.028432530120683266, -0.0020005372909667053, -0.1061038169098775, 0.035223436172363225, 0.30554101518962695, -0.2252153688231888, -0.31808896221058525, 0.05807599065693743, -0.20252427191514036, -0.14631544140612948, 0.21218203206587097, -0.017880142617... |
707.0104 | Giant Anisotropy of Magnetoresistance and "Spin Valve" effect in
Antiferromagnetic $Nd_{2-x}Ce_xCuO_{4}$ | We have studied anisotropic magnetoresistance (MR) and magnetization with
rotating magnetic field (B) within $CuO_2$ plane in lightly doped AF
$Nd_{2-x}Ce_xCuO_{4}$. \emph{A giant anisotropy} in MR is observed at low
temperature below 5 K. The c-axis resistivity can be tuned about one order of
magnitude just by chang... | cond-mat.supr-con cond-mat.str-el | we have studied anisotropic magnetoresistance mr and magnetization with rotating magnetic field b within cuo_2 plane in lightly doped af nd_2xce_xcuo_4 empha giant anisotropy in mr is observed at low temperature below 5 k the caxis resistivity can be tuned about one order of magnitude just by changing b direction withi... | [['we', 'have', 'studied', 'anisotropic', 'magnetoresistance', 'mr', 'and', 'magnetization', 'with', 'rotating', 'magnetic', 'field', 'b', 'within', 'cuo_2', 'plane', 'in', 'lightly', 'doped', 'af', 'nd_2xce_xcuo_4', 'empha', 'giant', 'anisotropy', 'in', 'mr', 'is', 'observed', 'at', 'low', 'temperature', 'below', '5',... | [-0.22016705691607463, 0.22759458884995962, 0.0017549903168978672, -0.0016833216253121102, -0.10949692045271929, -0.14296505109052218, 0.026304776894874753, 0.3921738036922992, -0.2631909456695356, -0.3535469151471579, -0.029106785105319603, -0.2841196519337476, -0.10599684216348189, 0.19335532486660495, 0.079068867109... |
707.0105 | Moduli Stabilization, Large-Volume dS Minimum Without anti-D3-Branes,
(Non-)Supersymmetric Black Hole Attractors and Two-Parameter Swiss Cheese
Calabi-Yau's | We consider issues of moduli stabilization and "area codes" for type II flux
compactifications, and the "Inverse Problem" and "Fake Superpotentials" for
extremal (non)supersymmetric black holes in type II compactifications on
(orientifold of) a compact two-parameter Calabi-Yau expressed as a degree-18
hypersurface in... | hep-th | we consider issues of moduli stabilization and area codes for type ii flux compactifications and the inverse problem and fake superpotentials for extremal nonsupersymmetric black holes in type ii compactifications on orientifold of a compact twoparameter calabiyau expressed as a degree18 hypersurface in wcp411169 which... | [['we', 'consider', 'issues', 'of', 'moduli', 'stabilization', 'and', 'area', 'codes', 'for', 'type', 'ii', 'flux', 'compactifications', 'and', 'the', 'inverse', 'problem', 'and', 'fake', 'superpotentials', 'for', 'extremal', 'nonsupersymmetric', 'black', 'holes', 'in', 'type', 'ii', 'compactifications', 'on', 'orienti... | [-0.15485659856531842, 0.0754865800163494, -0.047195575931839935, 0.1553966744236794, -0.08002856851500624, -0.15179368815950903, 0.04874261574929251, 0.2796468660819764, -0.19668168075127052, -0.2544677407791217, 0.13271781063465146, -0.2884861748026428, -0.14236683601550026, 0.15639206233397857, -0.10936010313749897,... |
707.0106 | The evolution of density perturbations in f(R) gravity | We give a rigorous and mathematically well defined presentation of the
Covariant and Gauge Invariant theory of scalar perturbations of a
Friedmann-Lemaitre-Robertson-Walker universe for Fourth Order Gravity, where
the matter is described by a perfect fluid with a barotropic equation of state.
The general perturbation... | gr-qc astro-ph hep-th | we give a rigorous and mathematically well defined presentation of the covariant and gauge invariant theory of scalar perturbations of a friedmannlemaitrerobertsonwalker universe for fourth order gravity where the matter is described by a perfect fluid with a barotropic equation of state the general perturbations equat... | [['we', 'give', 'a', 'rigorous', 'and', 'mathematically', 'well', 'defined', 'presentation', 'of', 'the', 'covariant', 'and', 'gauge', 'invariant', 'theory', 'of', 'scalar', 'perturbations', 'of', 'a', 'friedmannlemaitrerobertsonwalker', 'universe', 'for', 'fourth', 'order', 'gravity', 'where', 'the', 'matter', 'is', '... | [-0.1611821055125241, 0.15075610750470445, -0.11842804668432944, 0.09155945635037115, -0.09745121494968971, -0.13398180672044113, -0.06386005086266142, 0.25762558046370354, -0.21149569677112445, -0.27551318717839784, 0.0889116656720919, -0.27203307097956336, -0.11924057588625495, 0.14325943603244137, -0.019294740609850... |
707.0107 | Flexoelectric blue phases | We describe the occurence and properties of liquid crystal phases showing two
dimensional splay and bend distortions which are stabilised by flexoelectric
interactions. These phases are characterised by regions of locally double
splayed order separated by topological defects and are thus highly analogous to
the blue ... | cond-mat.soft | we describe the occurence and properties of liquid crystal phases showing two dimensional splay and bend distortions which are stabilised by flexoelectric interactions these phases are characterised by regions of locally double splayed order separated by topological defects and are thus highly analogous to the blue pha... | [['we', 'describe', 'the', 'occurence', 'and', 'properties', 'of', 'liquid', 'crystal', 'phases', 'showing', 'two', 'dimensional', 'splay', 'and', 'bend', 'distortions', 'which', 'are', 'stabilised', 'by', 'flexoelectric', 'interactions', 'these', 'phases', 'are', 'characterised', 'by', 'regions', 'of', 'locally', 'dou... | [-0.18556265252527226, 0.243544756335447, -0.1077529189439773, 0.018643407543514217, -0.06556447597450754, -0.11025567242896624, 0.039452366479881776, 0.42605355842394776, -0.2594511240689356, -0.27087169196038097, 0.08502757111878208, -0.2657455586399255, -0.22218375257478, 0.10608814506048567, 0.019097110633267446, -... |
707.0108 | Width and finite extinction time of Ricci flow | This is an expository article with complete proofs intended for a general
non-specialist audience. The results are two-fold. First, we discuss a
geometric invariant, that we call the width, of a manifold and show how it can
be realized as the sum of areas of minimal 2-spheres. For instance, when $M$ is
a homotopy 3-s... | math.DG math.GT | this is an expository article with complete proofs intended for a general nonspecialist audience the results are twofold first we discuss a geometric invariant that we call the width of a manifold and show how it can be realized as the sum of areas of minimal 2spheres for instance when m is a homotopy 3sphere the width... | [['this', 'is', 'an', 'expository', 'article', 'with', 'complete', 'proofs', 'intended', 'for', 'a', 'general', 'nonspecialist', 'audience', 'the', 'results', 'are', 'twofold', 'first', 'we', 'discuss', 'a', 'geometric', 'invariant', 'that', 'we', 'call', 'the', 'width', 'of', 'a', 'manifold', 'and', 'show', 'how', 'it... | [-0.14120290500607646, 0.11610605411649509, -0.11254013046132529, 0.09138789199742264, -0.15518013113338885, -0.14734976003669073, 0.006139578251569564, 0.37609584504188487, -0.27002845645946416, -0.2642675190842871, 0.11276022794732728, -0.2316345676041112, -0.15682619277002482, 0.1955034977411209, -0.1684777628799001... |
707.0109 | Optically Unseen HI Detections towards the Virgo Cluster detected in the
Arecibo Legacy Fast ALFA Survey | We report the discovery by the Arecibo Legacy Fast ALFA (ALFALFA) survey of
eight HI features not coincident with stellar counterparts in the Virgo Cluster
region. All of the HI clouds have cz < 3000 km/s and, if at the Virgo distance,
HI masses between 1.9 x 10**7 and 1.1 x 10**9 solar masses. Four of the eight
obje... | astro-ph | we report the discovery by the arecibo legacy fast alfa alfalfa survey of eight hi features not coincident with stellar counterparts in the virgo cluster region all of the hi clouds have cz 3000 kms and if at the virgo distance hi masses between 19 x 107 and 11 x 109 solar masses four of the eight objects were reported... | [['we', 'report', 'the', 'discovery', 'by', 'the', 'arecibo', 'legacy', 'fast', 'alfa', 'alfalfa', 'survey', 'of', 'eight', 'hi', 'features', 'not', 'coincident', 'with', 'stellar', 'counterparts', 'in', 'the', 'virgo', 'cluster', 'region', 'all', 'of', 'the', 'hi', 'clouds', 'have', 'cz', '3000', 'kms', 'and', 'if', '... | [-0.10669812055262314, 0.07451042890508863, -0.0277179128335998, 0.06768279812886395, -0.07563387899271108, -0.05570780405934083, 0.02722977615773359, 0.45009066480246773, -0.14842841571385543, -0.37537194149977066, 0.09670414941206096, -0.31844243891337976, -0.0627623141673518, 0.1963595627305312, -0.00145853643864836... |
707.011 | The static spherically symmetric body in relativistic elasticity | In this paper is discussed a class of static spherically symmetric solutions
of the general relativistic elasticity equations. The main point of discussion
is the comparison of two matter models given in terms of their stored energy
functionals, i.e., the rule which gives the amount of energy stored in the
system whe... | gr-qc | in this paper is discussed a class of static spherically symmetric solutions of the general relativistic elasticity equations the main point of discussion is the comparison of two matter models given in terms of their stored energy functionals ie the rule which gives the amount of energy stored in the system when it is... | [['in', 'this', 'paper', 'is', 'discussed', 'a', 'class', 'of', 'static', 'spherically', 'symmetric', 'solutions', 'of', 'the', 'general', 'relativistic', 'elasticity', 'equations', 'the', 'main', 'point', 'of', 'discussion', 'is', 'the', 'comparison', 'of', 'two', 'matter', 'models', 'given', 'in', 'terms', 'of', 'the... | [-0.1453574892913317, 0.10038449194461825, -0.057414522966796375, 0.09650255883595042, -0.012022286934037524, -0.09772617456851056, -0.020289486648615854, 0.3054181167249938, -0.2774518605950008, -0.28405526266657716, 0.08790806731831911, -0.27699302208710863, -0.12317290398886943, 0.16261298974684205, -0.0507821825217... |
707.0111 | Canonical volume forms on compact K\"{a}hler manifolds | We construct a canonical singular hermitian metric with semipositive
curvature current on the canonical line bundle of a compact K\"{a}hler manifold
with pseudoeffective canonical bundle.
| math.AG math.CV | we construct a canonical singular hermitian metric with semipositive curvature current on the canonical line bundle of a compact kahler manifold with pseudoeffective canonical bundle | [['we', 'construct', 'a', 'canonical', 'singular', 'hermitian', 'metric', 'with', 'semipositive', 'curvature', 'current', 'on', 'the', 'canonical', 'line', 'bundle', 'of', 'a', 'compact', 'kahler', 'manifold', 'with', 'pseudoeffective', 'canonical', 'bundle']] | [-0.2725489064306021, -0.03534579248167574, -0.024971109814941883, 0.0863575902581215, -0.241863401979208, -0.2586670770868659, -0.09906903699040413, 0.4380272173881531, -0.1769827626645565, -0.06386916145682335, 0.026378646772354842, -0.23608164846897126, -0.2024958935379982, 0.10568346709012985, -0.18442550353705883,... |
707.0112 | Holomorphy conditions of Fuji-Suzuki coupled Painlev\'e VI system | In this note, we give some holomorphy conditions of Fuji-Suzuki coupled
Painlev\'e VI system. We also give two translation operators acting on the
constant parameter $\eta$. We note a confluence process from the Fuji-Suzuki
system to the Noumi-Yamada system of type $A_5^{(1)}$.
| math.CA math.DS | in this note we give some holomorphy conditions of fujisuzuki coupled painleve vi system we also give two translation operators acting on the constant parameter eta we note a confluence process from the fujisuzuki system to the noumiyamada system of type a_51 | [['in', 'this', 'note', 'we', 'give', 'some', 'holomorphy', 'conditions', 'of', 'fujisuzuki', 'coupled', 'painleve', 'vi', 'system', 'we', 'also', 'give', 'two', 'translation', 'operators', 'acting', 'on', 'the', 'constant', 'parameter', 'eta', 'we', 'note', 'a', 'confluence', 'process', 'from', 'the', 'fujisuzuki', 's... | [-0.20710215566768533, 0.055845622693942415, -0.06932979834354705, 0.024716630371759016, -0.09253941773481313, -0.16710241696619915, 0.0335852327268748, 0.30138579811457367, -0.2960807810581866, -0.19507832337348235, 0.09855687994942335, -0.25890409396517844, -0.17182170794833274, 0.1757456117442676, -0.099628740278560... |
707.0113 | NGC 4254: An Act of Harassment Uncovered by the Arecibo Legacy Fast ALFA
Survey | We present an HI map constructed from the Arecibo Legacy Fast ALFA (ALFALFA)
survey of the surroundings of the strongly asymmetric Virgo cluster Sc galaxy
NGC 4254. Noted previously for its lopsided appearance, rich interstellar
medium, and extradisk HI emission, NGC 4254 is believed to be entering the
Virgo environm... | astro-ph | we present an hi map constructed from the arecibo legacy fast alfa alfalfa survey of the surroundings of the strongly asymmetric virgo cluster sc galaxy ngc 4254 noted previously for its lopsided appearance rich interstellar medium and extradisk hi emission ngc 4254 is believed to be entering the virgo environment for ... | [['we', 'present', 'an', 'hi', 'map', 'constructed', 'from', 'the', 'arecibo', 'legacy', 'fast', 'alfa', 'alfalfa', 'survey', 'of', 'the', 'surroundings', 'of', 'the', 'strongly', 'asymmetric', 'virgo', 'cluster', 'sc', 'galaxy', 'ngc', '4254', 'noted', 'previously', 'for', 'its', 'lopsided', 'appearance', 'rich', 'int... | [-0.06208381117321551, 0.04106682820845005, -0.09828092579803499, 0.06651937853469438, -0.13588691734381625, -0.02860621804421818, -0.00817950944214858, 0.4116321226028172, -0.20016838161123765, -0.32524323427099483, 0.04881852377659163, -0.263958996033447, -0.10037616798528344, 0.17858474845620426, 0.00741927065710361... |
707.0114 | Viral population estimation using pyrosequencing | The diversity of virus populations within single infected hosts presents a
major difficulty for the natural immune response as well as for vaccine design
and antiviral drug therapy. Recently developed pyrophosphate based sequencing
technologies (pyrosequencing) can be used for quantifying this diversity by
ultra-deep... | q-bio.PE | the diversity of virus populations within single infected hosts presents a major difficulty for the natural immune response as well as for vaccine design and antiviral drug therapy recently developed pyrophosphate based sequencing technologies pyrosequencing can be used for quantifying this diversity by ultradeep seque... | [['the', 'diversity', 'of', 'virus', 'populations', 'within', 'single', 'infected', 'hosts', 'presents', 'a', 'major', 'difficulty', 'for', 'the', 'natural', 'immune', 'response', 'as', 'well', 'as', 'for', 'vaccine', 'design', 'and', 'antiviral', 'drug', 'therapy', 'recently', 'developed', 'pyrophosphate', 'based', 's... | [-0.03272469642349699, 0.06792887319778544, -0.06915324249198261, 0.10393092010444753, -0.047438240452525926, -0.14901518663715813, 0.12454064351921225, 0.3468704036001431, -0.25283580577807196, -0.319033896615694, 0.10728915533820046, -0.24475307575663302, -0.196660170785675, 0.20677188363051346, -0.11110417884241659,... |
707.0115 | Higher derivatives and the inverse derivative of a tensor-valued
function of a tensor | The n-th derivative of a tensor valued function of a tensor is defined by a
finite number of coefficients each with closed form expression.
| math.SP | the nth derivative of a tensor valued function of a tensor is defined by a finite number of coefficients each with closed form expression | [['the', 'nth', 'derivative', 'of', 'a', 'tensor', 'valued', 'function', 'of', 'a', 'tensor', 'is', 'defined', 'by', 'a', 'finite', 'number', 'of', 'coefficients', 'each', 'with', 'closed', 'form', 'expression']] | [-0.24740220319169262, 0.14524882566183805, -0.059733217907099366, -0.032601386362027064, -0.13202117647354802, -0.08196895773289725, -0.06100774851317207, 0.22960354123885432, -0.28016960124174756, -0.1681045419536531, 0.0434485279644529, -0.24535190383903682, -0.22673257919571674, 0.128752273779052, 0.048413474733630... |
707.0116 | Non-Oberbeck-Boussinesq effects in two-dimensional Rayleigh-Benard
convection in glycerol | We numerically analyze Non-Oberbeck-Boussinesq (NOB) effects in
two-dimensional Rayleigh-Benard flow in glycerol, which shows a dramatic change
in the viscosity with temperature. The results are presented both as functions
of the Rayleigh number (Ra) up to $10^8$ (for fixed temperature difference
between the top and ... | physics.flu-dyn | we numerically analyze nonoberbeckboussinesq nob effects in twodimensional rayleighbenard flow in glycerol which shows a dramatic change in the viscosity with temperature the results are presented both as functions of the rayleigh number ra up to 108 for fixed temperature difference between the top and bottom plates an... | [['we', 'numerically', 'analyze', 'nonoberbeckboussinesq', 'nob', 'effects', 'in', 'twodimensional', 'rayleighbenard', 'flow', 'in', 'glycerol', 'which', 'shows', 'a', 'dramatic', 'change', 'in', 'the', 'viscosity', 'with', 'temperature', 'the', 'results', 'are', 'presented', 'both', 'as', 'functions', 'of', 'the', 'ra... | [-0.10753977965796366, 0.1974835021102703, -0.02690015993032016, -0.006095879904215077, -0.016602465282439402, -0.0917766868774044, 0.10710336564010696, 0.29025088375507807, -0.2520896361093037, -0.3191905551075347, 0.05349231408847692, -0.318602517798641, -0.04017904192625888, 0.20036414597355026, -0.00463822510485586... |
707.0117 | Complex trajectory method in time-dependent WKB | We present a significant improvement to a time-dependent WKB (TDWKB)
formulation developed by Boiron and Lombardi [JCP {\bf108}, 3431 (1998)] in
which the TDWKB equations are solved along classical trajectories that
propagate in the complex plane. Boiron and Lombardi showed that the method
gives very good agreement w... | quant-ph | we present a significant improvement to a timedependent wkb tdwkb formulation developed by boiron and lombardi jcp bf108 3431 1998 in which the tdwkb equations are solved along classical trajectories that propagate in the complex plane boiron and lombardi showed that the method gives very good agreement with the exact ... | [['we', 'present', 'a', 'significant', 'improvement', 'to', 'a', 'timedependent', 'wkb', 'tdwkb', 'formulation', 'developed', 'by', 'boiron', 'and', 'lombardi', 'jcp', 'bf108', '3431', '1998', 'in', 'which', 'the', 'tdwkb', 'equations', 'are', 'solved', 'along', 'classical', 'trajectories', 'that', 'propagate', 'in', '... | [-0.1050540022489648, 0.07084840695357084, -0.10799441213436824, 0.07797088197756759, -0.0764324666316887, -0.10975019335663612, 0.03715428768711198, 0.3552380384478186, -0.22989550838246942, -0.32739263092766385, 0.04290764219331322, -0.24876172211952507, -0.20336645492352545, 0.19452319006502097, -0.08926012087197575... |
707.0118 | Proton Structure Functions at High $Q^{2}$ and High x at HERA | Neutral and charged current deep inelastic scattering cross sections and
structure functions are presented. The review also discusses improvements to
the parton density measurements using jet cross section data and recent high
$Q^{2}$ inclusive cross section measurements. The projected parton density
uncertainties us... | hep-ex | neutral and charged current deep inelastic scattering cross sections and structure functions are presented the review also discusses improvements to the parton density measurements using jet cross section data and recent high q2 inclusive cross section measurements the projected parton density uncertainties using the e... | [['neutral', 'and', 'charged', 'current', 'deep', 'inelastic', 'scattering', 'cross', 'sections', 'and', 'structure', 'functions', 'are', 'presented', 'the', 'review', 'also', 'discusses', 'improvements', 'to', 'the', 'parton', 'density', 'measurements', 'using', 'jet', 'cross', 'section', 'data', 'and', 'recent', 'hig... | [-0.034443978863932634, 0.12207927616933982, -0.07886808039163988, 0.15423722232819773, -0.029474536559599286, -0.003247778604774937, -0.03765996775644667, 0.41172077287645903, -0.1833459144896444, -0.25068170000232903, -0.019815369134805368, -0.41360119438054516, 0.045589200567965414, 0.1424872327833345, 0.11953449789... |
707.0119 | TOF-Brho Mass Measurements of Very Exotic Nuclides for Astrophysical
Calculations at the NSCL | Atomic masses play a crucial role in many nuclear astrophysics calculations.
The lack of experimental values for relevant exotic nuclides triggered a rapid
development of new mass measurement devices around the world. The
Time-of-Flight (TOF) mass measurements offer a complementary technique to the
most precise one, ... | nucl-ex | atomic masses play a crucial role in many nuclear astrophysics calculations the lack of experimental values for relevant exotic nuclides triggered a rapid development of new mass measurement devices around the world the timeofflight tof mass measurements offer a complementary technique to the most precise one penning t... | [['atomic', 'masses', 'play', 'a', 'crucial', 'role', 'in', 'many', 'nuclear', 'astrophysics', 'calculations', 'the', 'lack', 'of', 'experimental', 'values', 'for', 'relevant', 'exotic', 'nuclides', 'triggered', 'a', 'rapid', 'development', 'of', 'new', 'mass', 'measurement', 'devices', 'around', 'the', 'world', 'the',... | [-0.057271804850872444, 0.2129111455550984, -0.05326402110816992, 0.09470472981566158, -0.010018318518996238, -0.11900314048499516, 0.08255553605520854, 0.33635100612173907, -0.15085048840846865, -0.3246886486916438, 0.03347778415570603, -0.29630313383658297, 0.058604717934909074, 0.2910814138878461, 0.0330358470119434... |
707.012 | Eikonal Approximation in AdS/CFT: Resumming the Gravitational Loop
Expansion | We derive an eikonal approximation to high energy interactions in Anti-de
Sitter spacetime, by generalizing a position space derivation of the eikonal
amplitude in flat space. We are able to resum, in terms of a generalized phase
shift, ladder and cross ladder graphs associated to the exchange of a spin j
field, to a... | hep-th | we derive an eikonal approximation to high energy interactions in antide sitter spacetime by generalizing a position space derivation of the eikonal amplitude in flat space we are able to resum in terms of a generalized phase shift ladder and cross ladder graphs associated to the exchange of a spin j field to all order... | [['we', 'derive', 'an', 'eikonal', 'approximation', 'to', 'high', 'energy', 'interactions', 'in', 'antide', 'sitter', 'spacetime', 'by', 'generalizing', 'a', 'position', 'space', 'derivation', 'of', 'the', 'eikonal', 'amplitude', 'in', 'flat', 'space', 'we', 'are', 'able', 'to', 'resum', 'in', 'terms', 'of', 'a', 'gene... | [-0.18074704922868737, 0.19153565664591599, -0.0330985585948023, 0.08168937258540301, -0.0410851027843748, -0.0728882755207309, -0.005521591612162044, 0.3362831549791547, -0.22845374427995851, -0.21454411588061914, 0.037748339704643065, -0.30706818507645617, -0.12583120291532537, 0.11520195050413007, 0.0214580361105429... |
707.0121 | Generation of primordial cosmological density inhomogeneities with scale
invariant power spectrum during the standard radiation dominated expansion of
the universe | The most distinctive feature of the primordial density inhomogeneities that
existed in the cosmic plasma at the instant of decoupling is their scale
invariant power spectrum ${\cal P}(k) \sim k$ over the range $k \ll H_{eq}$ of
modes with cosmologically large comoving wavelength. We characterize this
feature in real ... | astro-ph gr-qc hep-th | the most distinctive feature of the primordial density inhomogeneities that existed in the cosmic plasma at the instant of decoupling is their scale invariant power spectrum cal pk sim k over the range k ll h_eq of modes with cosmologically large comoving wavelength we characterize this feature in real space in terms o... | [['the', 'most', 'distinctive', 'feature', 'of', 'the', 'primordial', 'density', 'inhomogeneities', 'that', 'existed', 'in', 'the', 'cosmic', 'plasma', 'at', 'the', 'instant', 'of', 'decoupling', 'is', 'their', 'scale', 'invariant', 'power', 'spectrum', 'cal', 'pk', 'sim', 'k', 'over', 'the', 'range', 'k', 'll', 'h_eq'... | [-0.17286771582439542, 0.17309114567381945, -0.085735533118494, 0.0770561347632089, -0.016984653624020657, -0.048853301533216716, -0.04538709012229206, 0.32068756669056864, -0.25040066531828586, -0.29183378646958547, 0.028782494279406615, -0.30047925255032926, -0.06288109131087109, 0.15298765210680804, 0.01537970744758... |
707.0122 | Jet confinement by magneto-torsional oscillations | Many quasars and active galactic nuclei (AGN) appear in radio, optical, and
X-ray maps, as a bright nuclear sources from which emerge single or double
long, thin jets. When observed with high angular resolution these jets show
structure with bright knots separated by relatively dark regions. Nonthermal
nature of a je... | astro-ph | many quasars and active galactic nuclei agn appear in radio optical and xray maps as a bright nuclear sources from which emerge single or double long thin jets when observed with high angular resolution these jets show structure with bright knots separated by relatively dark regions nonthermal nature of a jet radiation... | [['many', 'quasars', 'and', 'active', 'galactic', 'nuclei', 'agn', 'appear', 'in', 'radio', 'optical', 'and', 'xray', 'maps', 'as', 'a', 'bright', 'nuclear', 'sources', 'from', 'which', 'emerge', 'single', 'or', 'double', 'long', 'thin', 'jets', 'when', 'observed', 'with', 'high', 'angular', 'resolution', 'these', 'jet... | [-0.1524823605287688, 0.250865418968515, -0.04139854802571712, 0.1215868751916387, -0.10598278422146401, -0.1367620376041093, -0.04154685527542012, 0.4244065666901516, -0.26689064737858503, -0.3523072317269043, 0.0338830138203285, -0.2238770819975869, -0.00569207406914892, 0.20581491215894301, 0.018417337767330677, -0.... |
707.0123 | Identified particle measurements at large transverse momenta in Cu+Cu
collisions at RHIC | Differential measurements of various particle species over an extended
momentum range provide a sensitive experimental tool for investigation of
energy loss mechanisms in the medium created in nucleus-nucleus collisions at
RHIC. In these proceedings, a systematic study of transverse momentum spectra
for charged pions... | nucl-ex | differential measurements of various particle species over an extended momentum range provide a sensitive experimental tool for investigation of energy loss mechanisms in the medium created in nucleusnucleus collisions at rhic in these proceedings a systematic study of transverse momentum spectra for charged pions prot... | [['differential', 'measurements', 'of', 'various', 'particle', 'species', 'over', 'an', 'extended', 'momentum', 'range', 'provide', 'a', 'sensitive', 'experimental', 'tool', 'for', 'investigation', 'of', 'energy', 'loss', 'mechanisms', 'in', 'the', 'medium', 'created', 'in', 'nucleusnucleus', 'collisions', 'at', 'rhic'... | [-0.08346522049425115, 0.20186672374127215, -0.17110136592078326, 0.14029718280797548, 0.01881452336317242, -0.0668678323802824, -0.05722650931225998, 0.3504538072807954, -0.22429912496763882, -0.3339151023416826, -0.07035792241274093, -0.37776588611212547, 0.08027510586572756, 0.19692816932243065, 0.08085813106378854,... |
707.0124 | Generalized Gevrey ultradistributions | We first introduce new algebras of generalized functions containing Gevrey
ultradistributions and then develop a Gevrey microlocal analysis suitable for
these algebras. Finally, we give an application through an extension of the
well-known H\"{o}rmander's theorem on the wave front of the product of two
distributions.... | math.FA math.AP | we first introduce new algebras of generalized functions containing gevrey ultradistributions and then develop a gevrey microlocal analysis suitable for these algebras finally we give an application through an extension of the wellknown hormanders theorem on the wave front of the product of two distributions | [['we', 'first', 'introduce', 'new', 'algebras', 'of', 'generalized', 'functions', 'containing', 'gevrey', 'ultradistributions', 'and', 'then', 'develop', 'a', 'gevrey', 'microlocal', 'analysis', 'suitable', 'for', 'these', 'algebras', 'finally', 'we', 'give', 'an', 'application', 'through', 'an', 'extension', 'of', 't... | [-0.1353688255469832, 0.026248717293169143, -0.13683550217085413, 0.1413130623391933, -0.11431968287150893, -0.04860610412433743, -0.05434203643558754, 0.331645311249627, -0.33757321449617544, -0.1208878883264131, 0.133408104079879, -0.22213370619962614, -0.18487552156051, 0.22144593571623167, -0.0742522075979246, 0.02... |
707.0125 | The importance of the initial geometry in heavy in collisions | Elliptic flow, elliptic flow fluctuations and fluctuations in the initial
geometry point to a description of nuclear collisions that is driven by the
initial geometry, a quantity which appears to be imprinted from the instant of
the collision. In these proceedings, recent results from the PHOBOS
collaboration are dis... | nucl-ex | elliptic flow elliptic flow fluctuations and fluctuations in the initial geometry point to a description of nuclear collisions that is driven by the initial geometry a quantity which appears to be imprinted from the instant of the collision in these proceedings recent results from the phobos collaboration are discussed... | [['elliptic', 'flow', 'elliptic', 'flow', 'fluctuations', 'and', 'fluctuations', 'in', 'the', 'initial', 'geometry', 'point', 'to', 'a', 'description', 'of', 'nuclear', 'collisions', 'that', 'is', 'driven', 'by', 'the', 'initial', 'geometry', 'a', 'quantity', 'which', 'appears', 'to', 'be', 'imprinted', 'from', 'the', ... | [-0.14576765190873106, 0.1607546741379646, -0.19827131061988362, 0.045399559071776854, -0.005330333154711683, -0.013241865609030602, -0.09460248899156765, 0.2750045816903397, -0.2938414531823058, -0.2850224017402378, 0.1177897528465048, -0.3210420865975952, -0.06748973382479054, 0.19315401834072704, -0.0498203937027414... |
707.0126 | Quantum wires in magnetic field: A comparative study of the Hartree-Fock
and the spin density functional approaches | We present a detailed comparison of the self-consistent calculations based on
the Hartree-Fock and the spin density functional theory for a spit-gate quantum
wire in the IQH regime. We demonstrate that both approaches provide
qualitatively (and in most cases quantitatively) similar results for the
spin-resolved elect... | cond-mat.mes-hall | we present a detailed comparison of the selfconsistent calculations based on the hartreefock and the spin density functional theory for a spitgate quantum wire in the iqh regime we demonstrate that both approaches provide qualitatively and in most cases quantitatively similar results for the spinresolved electron densi... | [['we', 'present', 'a', 'detailed', 'comparison', 'of', 'the', 'selfconsistent', 'calculations', 'based', 'on', 'the', 'hartreefock', 'and', 'the', 'spin', 'density', 'functional', 'theory', 'for', 'a', 'spitgate', 'quantum', 'wire', 'in', 'the', 'iqh', 'regime', 'we', 'demonstrate', 'that', 'both', 'approaches', 'prov... | [-0.11337238846647536, 0.15313967898262446, -0.06510346036358095, 0.11439905882818821, 0.02690909407390802, -0.11237344028057981, 0.023599805597429923, 0.3662500599549609, -0.21779707195136047, -0.32180844779525486, 0.002826114376046643, -0.283948272489798, -0.08568212080903073, 0.1585780615536554, 0.06721317311546401,... |
707.0127 | Design and Initial Performance of SHARP, a Polarimeter for the SHARC-II
Camera at the Caltech Submillimeter Observatory | We have developed a fore-optics module that converts the SHARC-II camera at
the Caltech Submillimeter Observatory into a sensitive imaging polarimeter at
wavelengths of 350 and 450 microns. We refer to this module as "SHARP". SHARP
splits the incident radiation into two orthogonally polarized beams that are
then re-i... | astro-ph | we have developed a foreoptics module that converts the sharcii camera at the caltech submillimeter observatory into a sensitive imaging polarimeter at wavelengths of 350 and 450 microns we refer to this module as sharp sharp splits the incident radiation into two orthogonally polarized beams that are then reimaged ont... | [['we', 'have', 'developed', 'a', 'foreoptics', 'module', 'that', 'converts', 'the', 'sharcii', 'camera', 'at', 'the', 'caltech', 'submillimeter', 'observatory', 'into', 'a', 'sensitive', 'imaging', 'polarimeter', 'at', 'wavelengths', 'of', '350', 'and', '450', 'microns', 'we', 'refer', 'to', 'this', 'module', 'as', 's... | [-0.0919264061593761, 0.12019066695744793, -0.07236109014600516, -0.017557748368320365, -0.0592891699851801, -0.17022662931742769, -0.0023403117852285505, 0.4703231442347169, -0.20838317995890976, -0.3198663320330282, 0.10935561991141488, -0.30734987394263347, -0.03884192448109389, 0.20902473431740268, -0.0197325787336... |
707.0128 | F-statistic search for white-dwarf binaries in the first Mock LISA Data
Challenge | The F-statistic is an optimal detection statistic for continuous
gravitational waves, i.e., long-duration (quasi-)monochromatic signals with
slowly-varying intrinsic frequency. This method was originally developed in the
context of ground-based detectors, but it is equally applicable to LISA where
many signals fall i... | gr-qc | the fstatistic is an optimal detection statistic for continuous gravitational waves ie longduration quasimonochromatic signals with slowlyvarying intrinsic frequency this method was originally developed in the context of groundbased detectors but it is equally applicable to lisa where many signals fall into this class ... | [['the', 'fstatistic', 'is', 'an', 'optimal', 'detection', 'statistic', 'for', 'continuous', 'gravitational', 'waves', 'ie', 'longduration', 'quasimonochromatic', 'signals', 'with', 'slowlyvarying', 'intrinsic', 'frequency', 'this', 'method', 'was', 'originally', 'developed', 'in', 'the', 'context', 'of', 'groundbased'... | [-0.1204490519805232, 0.10377153370075211, -0.0637030109807145, 0.1116802555987406, -0.1043886415711714, -0.09347196542254584, 0.033154104572288165, 0.3755744359800665, -0.1843221913876496, -0.31417473118136247, 0.13384243497885323, -0.258540556949424, -0.15243362489946582, 0.301509148857417, -0.03291781018506442, 0.07... |
707.0129 | Hodge-theoretic Atiyah-Meyer formulae and the stratified multiplicative
property | In this note we survey Hodge-theoretic formulae of Atiyah-Meyer type for
genera and characteristic classes of complex algebraic varieties, and derive
some new and interesting applications. We also present various extensions to
the singular setting of the Chern-Hirzebruch-Serre signature formula.
| math.AG math.AT | in this note we survey hodgetheoretic formulae of atiyahmeyer type for genera and characteristic classes of complex algebraic varieties and derive some new and interesting applications we also present various extensions to the singular setting of the chernhirzebruchserre signature formula | [['in', 'this', 'note', 'we', 'survey', 'hodgetheoretic', 'formulae', 'of', 'atiyahmeyer', 'type', 'for', 'genera', 'and', 'characteristic', 'classes', 'of', 'complex', 'algebraic', 'varieties', 'and', 'derive', 'some', 'new', 'and', 'interesting', 'applications', 'we', 'also', 'present', 'various', 'extensions', 'to',... | [-0.1508510270597119, -0.019541175174182218, -0.1083864726273245, 0.1703074690487579, -0.15788039628808437, -0.13359538965711468, 0.012995660078319671, 0.29349814237732635, -0.27676772288242846, -0.2619997691853266, 0.13590643390412688, -0.21659272899361035, -0.2570657909504677, 0.29936077215978385, -0.1385894287132511... |
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