id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
710.3753 | A very faint core-collapse supernova in M85 | An anomalous transient in the early Hubble-type (S0) galaxy Messier 85 (M85)
in the Virgo cluster was discovered by Kulkarni et al. (2007) on 7 January 2006
that had very low luminosity (peak absolute R-band magnitude MR of about -12)
that was constant over more than 80 days, red colour and narrow spectral lines,
whi... | astro-ph | an anomalous transient in the early hubbletype s0 galaxy messier 85 m85 in the virgo cluster was discovered by kulkarni et al 2007 on 7 january 2006 that had very low luminosity peak absolute rband magnitude mr of about 12 that was constant over more than 80 days red colour and narrow spectral lines which seem inconsis... | [['an', 'anomalous', 'transient', 'in', 'the', 'early', 'hubbletype', 's0', 'galaxy', 'messier', '85', 'm85', 'in', 'the', 'virgo', 'cluster', 'was', 'discovered', 'by', 'kulkarni', 'et', 'al', '2007', 'on', '7', 'january', '2006', 'that', 'had', 'very', 'low', 'luminosity', 'peak', 'absolute', 'rband', 'magnitude', 'm... | [-0.039939500960948254, 0.07990028515038526, -0.08539580372550214, 0.1366407959535233, -0.16152661408220106, -0.08849182205740362, 0.029536168642031648, 0.4261737024722, -0.0687783168987759, -0.4046747458012154, 0.08041449442874485, -0.3082655417228428, -0.1053027749604856, 0.20341248104341503, -0.11155343404971063, -0... |
710.3754 | Mid-Infrared Photometry and Spectra of Three High Mass Protostellar
Candidates at IRAS 18151-1208 and IRAS 20343+4129 | We present arcsecond-scale mid-ir photometry (in the 10.5 micron N band and
at 24.8 microns), and low resolution spectra in the N band (R~100) of a
candidate high mass protostellar object (HMPO) in IRAS 18151-1208 and of two
HMPO candidates in IRAS 20343+4129, IRS 1 and IRS 3. In addition we present
high resolution m... | astro-ph | we present arcsecondscale midir photometry in the 105 micron n band and at 248 microns and low resolution spectra in the n band r100 of a candidate high mass protostellar object hmpo in iras 181511208 and of two hmpo candidates in iras 203434129 irs 1 and irs 3 in addition we present high resolution midir spectra r8000... | [['we', 'present', 'arcsecondscale', 'midir', 'photometry', 'in', 'the', '105', 'micron', 'n', 'band', 'and', 'at', '248', 'microns', 'and', 'low', 'resolution', 'spectra', 'in', 'the', 'n', 'band', 'r100', 'of', 'a', 'candidate', 'high', 'mass', 'protostellar', 'object', 'hmpo', 'in', 'iras', '181511208', 'and', 'of',... | [-0.02550702466058198, 0.07369133682943864, -0.023063765100993994, 0.019148889006532426, -0.06153788719310014, -0.11691458691398851, 0.012639267031688156, 0.5228344156368917, -0.07385789820190714, -0.32796296583445267, 0.07322064369272571, -0.29728283825178825, 0.05631973985196795, 0.0735594593313371, -0.06064653085026... |
710.3755 | The Standard Model Higgs boson as the inflaton | We argue that the Higgs boson of the Standard Model can lead to inflation and
produce cosmological perturbations in accordance with observations. An
essential requirement is the non-minimal coupling of the Higgs scalar field to
gravity; no new particle besides already present in the electroweak theory is
required.
| hep-th astro-ph hep-ph | we argue that the higgs boson of the standard model can lead to inflation and produce cosmological perturbations in accordance with observations an essential requirement is the nonminimal coupling of the higgs scalar field to gravity no new particle besides already present in the electroweak theory is required | [['we', 'argue', 'that', 'the', 'higgs', 'boson', 'of', 'the', 'standard', 'model', 'can', 'lead', 'to', 'inflation', 'and', 'produce', 'cosmological', 'perturbations', 'in', 'accordance', 'with', 'observations', 'an', 'essential', 'requirement', 'is', 'the', 'nonminimal', 'coupling', 'of', 'the', 'higgs', 'scalar', 'f... | [-0.13801346272036122, 0.2294877524379141, -0.09260741912294179, 0.1430338124288634, -0.12337940849829465, -0.18855043624838194, -0.07307527663215296, 0.29348832617203396, -0.17470963933737949, -0.30432468571234494, 0.02631150920691046, -0.2162138884984112, -0.10600008411953847, 0.13379351690673502, -0.0314706440937394... |
710.3756 | Complex Langevin Equations and Schwinger-Dyson Equations | Stationary distributions of complex Langevin equations are shown to be the
complexified path integral solutions of the Schwinger-Dyson equations of the
associated quantum field theory. Specific examples in zero dimensions and on a
lattice are given. Relevance to the study of quantum field theory phase space
is discus... | hep-th hep-lat hep-ph | stationary distributions of complex langevin equations are shown to be the complexified path integral solutions of the schwingerdyson equations of the associated quantum field theory specific examples in zero dimensions and on a lattice are given relevance to the study of quantum field theory phase space is discussed | [['stationary', 'distributions', 'of', 'complex', 'langevin', 'equations', 'are', 'shown', 'to', 'be', 'the', 'complexified', 'path', 'integral', 'solutions', 'of', 'the', 'schwingerdyson', 'equations', 'of', 'the', 'associated', 'quantum', 'field', 'theory', 'specific', 'examples', 'in', 'zero', 'dimensions', 'and', '... | [-0.16713200965265665, 0.17472999956225976, -0.09385045792441815, 0.0787836460537316, -0.09582042857073247, -0.09825725173383641, -0.037484112443053164, 0.3363885753788054, -0.25445980912384886, -0.1911206275302296, 0.09115756887816436, -0.2834952479461208, -0.19804098433814943, 0.1865353835746646, -0.03351763921091333... |
710.3757 | Inferring the conditional mean | Consider a stationary real-valued time series $\{X_n\}_{n=0}^{\infty}$ with a
priori unknown distribution. The goal is to estimate the conditional
expectation $E(X_{n+1}|X_0,..., X_n)$ based on the observations $(X_0,...,
X_n)$ in a pointwise consistent way. It is well known that this is not possible
at all values of... | math.PR cs.IT math.IT | consider a stationary realvalued time series x_n_n0infty with a priori unknown distribution the goal is to estimate the conditional expectation ex_n1x_0 x_n based on the observations x_0 x_n in a pointwise consistent way it is well known that this is not possible at all values of n we will estimate it along stopping ti... | [['consider', 'a', 'stationary', 'realvalued', 'time', 'series', 'x_n_n0infty', 'with', 'a', 'priori', 'unknown', 'distribution', 'the', 'goal', 'is', 'to', 'estimate', 'the', 'conditional', 'expectation', 'ex_n1x_0', 'x_n', 'based', 'on', 'the', 'observations', 'x_0', 'x_n', 'in', 'a', 'pointwise', 'consistent', 'way'... | [-0.12358329793051728, 0.11426269496738348, -0.10435561196140523, 0.0656905144778133, -0.06989407854787302, -0.11463494399421902, 0.03923146092807347, 0.42603681728524984, -0.2711828367736296, -0.21309616824366012, 0.1434959592802872, -0.2757608166913379, -0.09066369676004814, 0.15899491748983427, -0.10046135398717422,... |
710.3758 | Heating mechanism affects equipartition in a binary granular system | Two species of particles in a binary granular system typically do not have
the same mean kinetic energy, in contrast to the equipartition of energy
required in equilibrium. We investigate the role of the heating mechanism in
determining the extent of this non-equipartition of kinetic energy. In most
experiments, diff... | cond-mat.soft | two species of particles in a binary granular system typically do not have the same mean kinetic energy in contrast to the equipartition of energy required in equilibrium we investigate the role of the heating mechanism in determining the extent of this nonequipartition of kinetic energy in most experiments different s... | [['two', 'species', 'of', 'particles', 'in', 'a', 'binary', 'granular', 'system', 'typically', 'do', 'not', 'have', 'the', 'same', 'mean', 'kinetic', 'energy', 'in', 'contrast', 'to', 'the', 'equipartition', 'of', 'energy', 'required', 'in', 'equilibrium', 'we', 'investigate', 'the', 'role', 'of', 'the', 'heating', 'me... | [-0.1501323247507718, 0.19190527742067653, -0.061967218575450865, 0.09433588885980088, 0.021385217509833316, -0.06759118040527907, 0.019237193648868632, 0.3334092697008483, -0.2570542078775038, -0.3368698083795607, 0.04788030518290226, -0.27668623410676035, -0.060969612454139295, 0.14523280895457813, 0.0086204063244945... |
710.3759 | Selective Reflection Spectroscopy at the Interface between a Calcium
Fluoride Window and Cs Vapour | A special vapour cell has been built, that allows the measurement of the
atom-surface van der Waals interaction exerted by a CaF2 window at the
interface with Cs vapour. Mechanical and thermal fragility of fluoride windows
make common designs of vapour cells unpractical, so that we have developed an
all-sapphire seal... | physics.atom-ph | a special vapour cell has been built that allows the measurement of the atomsurface van der waals interaction exerted by a caf2 window at the interface with cs vapour mechanical and thermal fragility of fluoride windows make common designs of vapour cells unpractical so that we have developed an allsapphire sealed cell... | [['a', 'special', 'vapour', 'cell', 'has', 'been', 'built', 'that', 'allows', 'the', 'measurement', 'of', 'the', 'atomsurface', 'van', 'der', 'waals', 'interaction', 'exerted', 'by', 'a', 'caf2', 'window', 'at', 'the', 'interface', 'with', 'cs', 'vapour', 'mechanical', 'and', 'thermal', 'fragility', 'of', 'fluoride', '... | [-0.11467481443922921, 0.16130563948913565, -0.0500141919941216, -0.08074537404729513, -0.008053203722761, -0.1992933972520225, 0.08815177172899569, 0.3941460930926288, -0.2070575758791816, -0.29142103580482026, 0.00565521315280578, -0.31925907024237354, -0.11153260122317775, 0.16891250339693126, -0.023774863237998, 0.... |
710.376 | Guessing the output of a stationary binary time series | The forward prediction problem for a binary time series
$\{X_n\}_{n=0}^{\infty}$ is to estimate the probability that $X_{n+1}=1$ based
on the observations $X_i$, $0\le i\le n$ without prior knowledge of the
distribution of the process $\{X_n\}$. It is known that this is not possible if
one estimates at all values of ... | math.PR cs.IT math.IT | the forward prediction problem for a binary time series x_n_n0infty is to estimate the probability that x_n11 based on the observations x_i 0le ile n without prior knowledge of the distribution of the process x_n it is known that this is not possible if one estimates at all values of n we present a simple procedure whi... | [['the', 'forward', 'prediction', 'problem', 'for', 'a', 'binary', 'time', 'series', 'x_n_n0infty', 'is', 'to', 'estimate', 'the', 'probability', 'that', 'x_n11', 'based', 'on', 'the', 'observations', 'x_i', '0le', 'ile', 'n', 'without', 'prior', 'knowledge', 'of', 'the', 'distribution', 'of', 'the', 'process', 'x_n', ... | [-0.0911991841324112, 0.10020227358840844, -0.10360087243401829, 0.038102488923130506, -0.049520746952689744, -0.14424268360633183, 0.07955875552040251, 0.40752596048199957, -0.263274987217258, -0.27331441429388875, 0.14244925763238878, -0.2822093375136747, -0.0868142751572818, 0.16109873689163257, -0.03832477982539464... |
710.3761 | Extraordinary surface voltage effect in the invisibility cloak with an
active device inside | The electromagnetic field solution for a spherical invisibility cloak with an
active device inside is established. Extraordinary electric and magnetic
surface voltages are induced at the inner boundary of a spherical cloak, which
prevent electromagnetic waves from going out. The phase and handness of
polarized waves ... | physics.optics | the electromagnetic field solution for a spherical invisibility cloak with an active device inside is established extraordinary electric and magnetic surface voltages are induced at the inner boundary of a spherical cloak which prevent electromagnetic waves from going out the phase and handness of polarized waves obliq... | [['the', 'electromagnetic', 'field', 'solution', 'for', 'a', 'spherical', 'invisibility', 'cloak', 'with', 'an', 'active', 'device', 'inside', 'is', 'established', 'extraordinary', 'electric', 'and', 'magnetic', 'surface', 'voltages', 'are', 'induced', 'at', 'the', 'inner', 'boundary', 'of', 'a', 'spherical', 'cloak', ... | [-0.18441978969684478, 0.20144575522732502, -0.03903451862253165, -0.002871973307939309, -0.10233211804055765, -0.10374373196509112, 0.0019522620616166779, 0.40157130957068354, -0.24205936026874553, -0.2811425214298488, 0.06043594584570088, -0.28855436490430086, -0.11989157868737585, 0.1933421293336354, 0.0038825442835... |
710.3762 | Exponential decay in a spin bath | We show that the coherence of an electron spin interacting with a bath of
nuclear spins can exhibit a well-defined purely exponential decay for special
(`narrowed') bath initial conditions in the presence of a strong applied
magnetic field. This is in contrast to the typical case, where spin-bath
dynamics have been i... | cond-mat.mes-hall quant-ph | we show that the coherence of an electron spin interacting with a bath of nuclear spins can exhibit a welldefined purely exponential decay for special narrowed bath initial conditions in the presence of a strong applied magnetic field this is in contrast to the typical case where spinbath dynamics have been investigate... | [['we', 'show', 'that', 'the', 'coherence', 'of', 'an', 'electron', 'spin', 'interacting', 'with', 'a', 'bath', 'of', 'nuclear', 'spins', 'can', 'exhibit', 'a', 'welldefined', 'purely', 'exponential', 'decay', 'for', 'special', 'narrowed', 'bath', 'initial', 'conditions', 'in', 'the', 'presence', 'of', 'a', 'strong', '... | [-0.13380980564074385, 0.2455429431123506, -0.06203543291323715, 0.10261446748497999, 0.02068430911404667, -0.156292546281798, -0.01849442519920154, 0.38358971252347585, -0.22518991856594328, -0.24564786858563484, 0.005556920490494964, -0.26439190438853716, -0.048094283131865305, 0.19051230241570416, 0.0884101890605287... |
710.3763 | Supernova rates from the Southern inTermediate Redshift ESO Supernova
Search (STRESS) | To measure the supernova (SN) rates at intermediate redshift we performed the
Southern inTermediate Redshift ESO Supernova Search (STRESS). Unlike most of
the current high redshift SN searches, this survey was specifically designed to
estimate the rate for both type Ia and core collapse (CC) SNe. We counted the
SNe d... | astro-ph | to measure the supernova sn rates at intermediate redshift we performed the southern intermediate redshift eso supernova search stress unlike most of the current high redshift sn searches this survey was specifically designed to estimate the rate for both type ia and core collapse cc sne we counted the sne discovered i... | [['to', 'measure', 'the', 'supernova', 'sn', 'rates', 'at', 'intermediate', 'redshift', 'we', 'performed', 'the', 'southern', 'intermediate', 'redshift', 'eso', 'supernova', 'search', 'stress', 'unlike', 'most', 'of', 'the', 'current', 'high', 'redshift', 'sn', 'searches', 'this', 'survey', 'was', 'specifically', 'desi... | [-0.04604650118543456, 0.04902460577645494, -0.025164828648169834, 0.1116147298606423, -0.0849682635627687, -0.10905696531059221, 0.13652832473628224, 0.44750010387351113, -0.13926202829151105, -0.28044972028544485, 0.05333735645477039, -0.3290131234905372, 0.03520501762997204, 0.21234134071894611, -0.00809306549296404... |
710.3764 | Design of a Distributed Reachability Algorithm for Analysis of Linear
Hybrid Automata | This paper presents the design of a novel distributed algorithm d-IRA for the
reachability analysis of linear hybrid automata. Recent work on iterative
relaxation abstraction (IRA) is leveraged to distribute the computational
problem among multiple computational nodes in a non-redundant manner by
performing careful i... | cs.LO | this paper presents the design of a novel distributed algorithm dira for the reachability analysis of linear hybrid automata recent work on iterative relaxation abstraction ira is leveraged to distribute the computational problem among multiple computational nodes in a nonredundant manner by performing careful infeasib... | [['this', 'paper', 'presents', 'the', 'design', 'of', 'a', 'novel', 'distributed', 'algorithm', 'dira', 'for', 'the', 'reachability', 'analysis', 'of', 'linear', 'hybrid', 'automata', 'recent', 'work', 'on', 'iterative', 'relaxation', 'abstraction', 'ira', 'is', 'leveraged', 'to', 'distribute', 'the', 'computational', ... | [-0.15460375402098855, -0.023352202287731834, -0.08326893058629373, 0.04118431775751583, -0.1272869703706163, -0.18215460896205443, 0.14098196300134683, 0.35438558210929233, -0.300695139884901, -0.327394388234004, 0.07531248819148646, -0.21903305863722777, -0.2038100313466902, 0.19442785958735606, -0.0958843362183334, ... |
710.3765 | Determinants of rational knots | We study the Fox coloring invariants of rational knots. We express the
propagation of the colors down the twists of these knots and ultimately the
determinant of them with the help of finite increasing sequences whose terms of
even order are even and whose terms of odd order are odd.
| math.GT math.CO | we study the fox coloring invariants of rational knots we express the propagation of the colors down the twists of these knots and ultimately the determinant of them with the help of finite increasing sequences whose terms of even order are even and whose terms of odd order are odd | [['we', 'study', 'the', 'fox', 'coloring', 'invariants', 'of', 'rational', 'knots', 'we', 'express', 'the', 'propagation', 'of', 'the', 'colors', 'down', 'the', 'twists', 'of', 'these', 'knots', 'and', 'ultimately', 'the', 'determinant', 'of', 'them', 'with', 'the', 'help', 'of', 'finite', 'increasing', 'sequences', 'w... | [-0.2420514215528965, 0.16963119838386775, -0.06197957668453455, 0.0820961932092905, -0.05969483099877834, -0.092950926644844, 0.02171517925802618, 0.34460729867219925, -0.2680847936868668, -0.3754019112884998, 0.12234180657193065, -0.2827858216315508, -0.1558594772964716, 0.1087723577208817, -0.03824322309345007, 0.02... |
710.3766 | Equivariant $K$-theory of quaternionic flag manifolds | We consider the manifold $Fl_n(\mathbb{H})=Sp(n)/Sp(1)^n$ of all complete
flags in $\mathbb{H}^n$, where $\mathbb{H}$ is the skew-field of quaternions.
We study its equivariant $K$-theory rings with respect to the action of two
groups: $Sp(1)^n$ and a certain canonical subgroup $T:=(S^1)^n\subset Sp(1)^n$
(a maximal ... | math.AT | we consider the manifold fl_nmathbbhspnsp1n of all complete flags in mathbbhn where mathbbh is the skewfield of quaternions we study its equivariant ktheory rings with respect to the action of two groups sp1n and a certain canonical subgroup ts1nsubset sp1n a maximal torus for the first group action we obtain a goresky... | [['we', 'consider', 'the', 'manifold', 'fl_nmathbbhspnsp1n', 'of', 'all', 'complete', 'flags', 'in', 'mathbbhn', 'where', 'mathbbh', 'is', 'the', 'skewfield', 'of', 'quaternions', 'we', 'study', 'its', 'equivariant', 'ktheory', 'rings', 'with', 'respect', 'to', 'the', 'action', 'of', 'two', 'groups', 'sp1n', 'and', 'a'... | [-0.23093576572835445, 0.009531767790516217, -0.06773947785298029, 0.04990528492024168, -0.10795662391930819, -0.09416836908708016, -0.04515712895275404, 0.35557122467706603, -0.3273255518637598, -0.17220516425014162, 0.1593697338970378, -0.22111053589188184, -0.15473649663229783, 0.1965466113264362, -0.151775308065116... |
710.3767 | Magnetism and structure of LixCoO2 and comparison to NaxCoO2 | The magnetic properties and structure of LixCoO2 for x between 0.5 and 1.0
are reported. Co4+ is found to be high-spin in LixCoO2 for x between 0.94 and
1.0 and low-spin for x between 0.50 and 0.78. Weak antiferromagnetic coupling
is observed, increasing in strength as more Co4+ is introduced. At an x value
of about ... | cond-mat.str-el | the magnetic properties and structure of lixcoo2 for x between 05 and 10 are reported co4 is found to be highspin in lixcoo2 for x between 094 and 10 and lowspin for x between 050 and 078 weak antiferromagnetic coupling is observed increasing in strength as more co4 is introduced at an x value of about 065 the temperat... | [['the', 'magnetic', 'properties', 'and', 'structure', 'of', 'lixcoo2', 'for', 'x', 'between', '05', 'and', '10', 'are', 'reported', 'co4', 'is', 'found', 'to', 'be', 'highspin', 'in', 'lixcoo2', 'for', 'x', 'between', '094', 'and', '10', 'and', 'lowspin', 'for', 'x', 'between', '050', 'and', '078', 'weak', 'antiferrom... | [-0.1350407349531429, 0.20031578311639164, 0.022583672146295537, 0.016063801027394783, -0.011937680386689416, -0.11265070312685385, 0.08934882084364708, 0.4235037956271112, -0.27514433443129804, -0.3101024665806142, 0.01342764612278606, -0.38745075996722217, -0.07686310593524705, 0.1609305634122828, 0.03384351824346629... |
710.3768 | Atom Interferometry tests of the isotropy of post-Newtonian gravity | We present a test of the local Lorentz invariance of post-Newtonian gravity
by monitoring Earth's gravity with a Mach-Zehnder atom interferometer that
features a resolution of about 8*10^(-9)g/Hz^(1/2), the highest reported thus
far. Expressed within the standard model extension (SME) or Nordtvedt's
anisotropic unive... | gr-qc physics.atom-ph | we present a test of the local lorentz invariance of postnewtonian gravity by monitoring earths gravity with a machzehnder atom interferometer that features a resolution of about 8109ghz12 the highest reported thus far expressed within the standard model extension sme or nordtvedts anisotropic universe model the analys... | [['we', 'present', 'a', 'test', 'of', 'the', 'local', 'lorentz', 'invariance', 'of', 'postnewtonian', 'gravity', 'by', 'monitoring', 'earths', 'gravity', 'with', 'a', 'machzehnder', 'atom', 'interferometer', 'that', 'features', 'a', 'resolution', 'of', 'about', '8109ghz12', 'the', 'highest', 'reported', 'thus', 'far', ... | [-0.11840987565691571, 0.10694363408059959, -0.0964207202981574, 0.07880522573860474, -0.04169139907280185, -0.1314703616178987, -0.02072983672449657, 0.3005253376596304, -0.19994885260127035, -0.3467816945659109, 0.04380665945046278, -0.2756177201777337, -0.0924721347555204, 0.15891800012091645, 0.027263066995081055, ... |
710.3769 | Exact Wave Solutions to 6D Gauged Chiral Supergravity | We describe a broad class of time-dependent exact wave solutions to 6D gauged
chiral supergravity with two compact dimensions. These 6D solutions are
nontrivial warped generalizations of 4D pp-waves and Kundt class solutions and
describe how a broad class of previously-static compactifications from 6D to 4D
(sourced ... | hep-th astro-ph gr-qc | we describe a broad class of timedependent exact wave solutions to 6d gauged chiral supergravity with two compact dimensions these 6d solutions are nontrivial warped generalizations of 4d ppwaves and kundt class solutions and describe how a broad class of previouslystatic compactifications from 6d to 4d sourced by two ... | [['we', 'describe', 'a', 'broad', 'class', 'of', 'timedependent', 'exact', 'wave', 'solutions', 'to', '6d', 'gauged', 'chiral', 'supergravity', 'with', 'two', 'compact', 'dimensions', 'these', '6d', 'solutions', 'are', 'nontrivial', 'warped', 'generalizations', 'of', '4d', 'ppwaves', 'and', 'kundt', 'class', 'solutions... | [-0.1167968698665762, 0.15185151087828505, 0.010531153743037246, 0.10464120096146641, -0.11519755217620552, -0.15911738231489567, -0.043097869680192594, 0.316413797021673, -0.17978290331379418, -0.2677150574909576, 0.13202488417310876, -0.31063863114309564, -0.1598582175284834, 0.15222115814685822, -0.07598540208853362... |
710.377 | Cohomogeneity one manifolds and selfmaps of nontrivial degree | We construct natural selfmaps of compact cohomgeneity one manifolds with
finite Weyl group and compute their degrees and Lefschetz numbers. On manifolds
with simple cohomology rings this yields in certain cases relations between the
order of the Weyl group and the Euler characteristic of a principal orbit. We
apply o... | math.DG math.AT | we construct natural selfmaps of compact cohomgeneity one manifolds with finite weyl group and compute their degrees and lefschetz numbers on manifolds with simple cohomology rings this yields in certain cases relations between the order of the weyl group and the euler characteristic of a principal orbit we apply our c... | [['we', 'construct', 'natural', 'selfmaps', 'of', 'compact', 'cohomgeneity', 'one', 'manifolds', 'with', 'finite', 'weyl', 'group', 'and', 'compute', 'their', 'degrees', 'and', 'lefschetz', 'numbers', 'on', 'manifolds', 'with', 'simple', 'cohomology', 'rings', 'this', 'yields', 'in', 'certain', 'cases', 'relations', 'b... | [-0.24601736074585592, 0.10415714136419656, -0.0861772596522161, 0.017981224184531425, -0.11090228268144171, -0.08982448372466678, -1.807990117689197e-05, 0.33902486509988816, -0.29453859646187236, -0.21333761921864045, 0.08998723768006509, -0.2704360888868026, -0.13141957927871956, 0.16637395099433286, -0.091960944946... |
710.3771 | Wilson Loops in Non-Compact U(1) Gauge Theories at Criticality | We study the properties of Wilson loops in three dimensional non-compact U(1)
gauge theories with global abelian symmetries. We use duality in the continuum
and on the lattice, to argue that close to the critical point between the Higgs
and Coulomb phases, all correlators of the Wilson loops are periodic functions
of... | hep-th hep-lat hep-ph | we study the properties of wilson loops in three dimensional noncompact u1 gauge theories with global abelian symmetries we use duality in the continuum and on the lattice to argue that close to the critical point between the higgs and coulomb phases all correlators of the wilson loops are periodic functions of the wil... | [['we', 'study', 'the', 'properties', 'of', 'wilson', 'loops', 'in', 'three', 'dimensional', 'noncompact', 'u1', 'gauge', 'theories', 'with', 'global', 'abelian', 'symmetries', 'we', 'use', 'duality', 'in', 'the', 'continuum', 'and', 'on', 'the', 'lattice', 'to', 'argue', 'that', 'close', 'to', 'the', 'critical', 'poin... | [-0.191973882803914, 0.23714963856036775, -0.05110356888067863, 0.10528725168918945, -0.07050474062807073, -0.14845999270849125, 0.030505371277716842, 0.35859962204765333, -0.1842427811199358, -0.24319697214339517, 0.087519578242025, -0.25247937135741505, -0.15521542446099615, 0.12605273433789416, -0.012265232799109071... |
710.3772 | Oscillations in Procyon A: First results from a multi-site campaign | Procyon A is a bright F5IV star in a binary system. Although the distance,
mass and angular diameter of this star are all known with high precision, the
exact evolutionary state is still unclear. Evolutionary tracks with different
ages and different mass fractions of hydrogen in the core pass, within the
errors, thro... | astro-ph | procyon a is a bright f5iv star in a binary system although the distance mass and angular diameter of this star are all known with high precision the exact evolutionary state is still unclear evolutionary tracks with different ages and different mass fractions of hydrogen in the core pass within the errors through the ... | [['procyon', 'a', 'is', 'a', 'bright', 'f5iv', 'star', 'in', 'a', 'binary', 'system', 'although', 'the', 'distance', 'mass', 'and', 'angular', 'diameter', 'of', 'this', 'star', 'are', 'all', 'known', 'with', 'high', 'precision', 'the', 'exact', 'evolutionary', 'state', 'is', 'still', 'unclear', 'evolutionary', 'tracks'... | [-0.10859313212867693, 0.1562795280060636, -0.06345523752740578, 0.0955273004396523, -0.07525508839938187, -0.08291705090184501, 0.10226430513053954, 0.41346543523187407, -0.20489505553774223, -0.38013191154633763, 0.13603468442720523, -0.2707762692908235, -0.03169993508218866, 0.19474147136942177, -0.05956363360241368... |
710.3773 | Limitations on intermittent forecasting | Bailey showed that the general pointwise forecasting for stationary and
ergodic time series has a negative solution. However, it is known that for
Markov chains the problem can be solved. Morvai showed that there is a stopping
time sequence $\{\lambda_n\}$ such that
$P(X_{\lambda_n+1}=1|X_0,...,X_{\lambda_n}) $ can b... | math.PR cs.IT math.IT | bailey showed that the general pointwise forecasting for stationary and ergodic time series has a negative solution however it is known that for markov chains the problem can be solved morvai showed that there is a stopping time sequence lambda_n such that px_lambda_n11x_0x_lambda_n can be estimated from samples x_0x_l... | [['bailey', 'showed', 'that', 'the', 'general', 'pointwise', 'forecasting', 'for', 'stationary', 'and', 'ergodic', 'time', 'series', 'has', 'a', 'negative', 'solution', 'however', 'it', 'is', 'known', 'that', 'for', 'markov', 'chains', 'the', 'problem', 'can', 'be', 'solved', 'morvai', 'showed', 'that', 'there', 'is', ... | [-0.10028974702969815, 0.1542030101797233, -0.10500029867204527, 0.11599273798346985, -0.015502896683756262, -0.13974863496065762, 0.0742080807161983, 0.42425515766565997, -0.3303255885529021, -0.20848813802876975, 0.16683228964199467, -0.2704756131085257, -0.11651053239183966, 0.2217229918227531, -0.045908970343104254... |
710.3774 | Wave breaking and particle jets in intense inhomogeneous charged beams | This work analyzes the dynamics of inhomogeneous, magnetically focused
high-intensity beams of charged particles. While for homogeneous beams the
whole system oscillates with a single frequency, any inhomogeneity leads to
propagating transverse density waves which eventually result in a singular
density build up, cau... | physics.plasm-ph physics.acc-ph physics.flu-dyn | this work analyzes the dynamics of inhomogeneous magnetically focused highintensity beams of charged particles while for homogeneous beams the whole system oscillates with a single frequency any inhomogeneity leads to propagating transverse density waves which eventually result in a singular density build up causing wa... | [['this', 'work', 'analyzes', 'the', 'dynamics', 'of', 'inhomogeneous', 'magnetically', 'focused', 'highintensity', 'beams', 'of', 'charged', 'particles', 'while', 'for', 'homogeneous', 'beams', 'the', 'whole', 'system', 'oscillates', 'with', 'a', 'single', 'frequency', 'any', 'inhomogeneity', 'leads', 'to', 'propagati... | [-0.15942840987475276, 0.22494917059556976, -0.09231091033215497, 0.03163306840861419, -0.034538165988898514, -0.09728068160815256, 0.0039854653555401924, 0.317382091508791, -0.2251994426104028, -0.27502601142018335, 0.024296234313417042, -0.2308955994115665, -0.020983972926140015, 0.1361903132188438, 0.061526495124222... |
710.3775 | On classifying processes | We prove several results concerning classifications, based on successive
observations $(X_1,..., X_n)$ of an unknown stationary and ergodic process, for
membership in a given class of processes, such as the class of all finite order
Markov chains.
| math.PR cs.IT math.IT | we prove several results concerning classifications based on successive observations x_1 x_n of an unknown stationary and ergodic process for membership in a given class of processes such as the class of all finite order markov chains | [['we', 'prove', 'several', 'results', 'concerning', 'classifications', 'based', 'on', 'successive', 'observations', 'x_1', 'x_n', 'of', 'an', 'unknown', 'stationary', 'and', 'ergodic', 'process', 'for', 'membership', 'in', 'a', 'given', 'class', 'of', 'processes', 'such', 'as', 'the', 'class', 'of', 'all', 'finite', '... | [-0.14078348467277513, 0.12651514637361067, -0.020417522412498255, 0.0326862855568293, -0.027288216883568344, -0.08687383801097402, 0.07367040252161992, 0.42661604204693354, -0.31486734969390406, -0.18528539838420377, 0.17603002426629835, -0.2590063797259653, -0.10315928044351372, 0.2178481576360158, -0.055765671970171... |
710.3776 | Structure and Evolution of the Opacity of Spiral Disks | The opacity of a spiral disk due to dust absorption influences every
measurement we make of it in the UV and optical. Two separate techniques
directly measure the total absorption by dust in the disk: calibrated distant
galaxy counts and overlapping galaxy pairs. The main results from both so far
are a semi-transpare... | astro-ph | the opacity of a spiral disk due to dust absorption influences every measurement we make of it in the uv and optical two separate techniques directly measure the total absorption by dust in the disk calibrated distant galaxy counts and overlapping galaxy pairs the main results from both so far are a semitransparent dis... | [['the', 'opacity', 'of', 'a', 'spiral', 'disk', 'due', 'to', 'dust', 'absorption', 'influences', 'every', 'measurement', 'we', 'make', 'of', 'it', 'in', 'the', 'uv', 'and', 'optical', 'two', 'separate', 'techniques', 'directly', 'measure', 'the', 'total', 'absorption', 'by', 'dust', 'in', 'the', 'disk', 'calibrated', ... | [-0.03733929318100722, 0.05811428456012197, -0.10567739146357083, 0.08709675439391192, -0.11874306013788839, -0.02409126561116239, 0.035815989371680776, 0.4582622672497022, -0.17968984669535373, -0.3326864916398519, 0.023384882454675706, -0.2926170044493946, -0.024451173691436498, 0.20279677496279938, -0.02618645685677... |
710.3777 | A Deterministic Approach to Wireless Relay Networks | We present a deterministic channel model which captures several key features
of multiuser wireless communication. We consider a model for a wireless network
with nodes connected by such deterministic channels, and present an exact
characterization of the end-to-end capacity when there is a single source and a
single ... | cs.IT cs.DM math.IT math.PR | we present a deterministic channel model which captures several key features of multiuser wireless communication we consider a model for a wireless network with nodes connected by such deterministic channels and present an exact characterization of the endtoend capacity when there is a single source and a single destin... | [['we', 'present', 'a', 'deterministic', 'channel', 'model', 'which', 'captures', 'several', 'key', 'features', 'of', 'multiuser', 'wireless', 'communication', 'we', 'consider', 'a', 'model', 'for', 'a', 'wireless', 'network', 'with', 'nodes', 'connected', 'by', 'such', 'deterministic', 'channels', 'and', 'present', 'a... | [-0.19300258799252668, 0.029461936866790966, -0.02988501224431327, 0.026736661164898253, -0.012781211702238726, -0.23396849677758827, 0.11480347405257367, 0.36109980968785227, -0.29192725368828953, -0.253441484594161, 0.08090731961018374, -0.24572656043649962, -0.21536497813890335, 0.1778436469023876, -0.09633489506287... |
710.3778 | Critical points of 2d disordered Dirac fermions: the Quantum Hall
Transitions revisited | We propose a resolution of the renormalization group flow for the disordered
Dirac fermion theories describing the quantum Hall transition (QHT) and spin
Quantum Hall transition (SQHT), which previously revealed no perturbative fixed
points at 1-loop and higher. The approach involves carrying out the flow in 2
stages... | cond-mat.mes-hall cond-mat.dis-nn hep-th math-ph math.MP | we propose a resolution of the renormalization group flow for the disordered dirac fermion theories describing the quantum hall transition qht and spin quantum hall transition sqht which previously revealed no perturbative fixed points at 1loop and higher the approach involves carrying out the flow in 2 stages the firs... | [['we', 'propose', 'a', 'resolution', 'of', 'the', 'renormalization', 'group', 'flow', 'for', 'the', 'disordered', 'dirac', 'fermion', 'theories', 'describing', 'the', 'quantum', 'hall', 'transition', 'qht', 'and', 'spin', 'quantum', 'hall', 'transition', 'sqht', 'which', 'previously', 'revealed', 'no', 'perturbative',... | [-0.16551558666686023, 0.18870674292222153, -0.08305446171503075, 0.019515113561152438, -0.02825201274461898, -0.1507876806594188, 0.03427522151835196, 0.2902143230323917, -0.22088844939043709, -0.2705570249848701, 0.07709894709979957, -0.2993844420332583, -0.14395090863960824, 0.1508083351114704, 0.01612603271629637, ... |
710.3779 | Testing D-Sequences for their Randomness | This paper examines the randomness of d-sequences, which are decimal
sequences to an arbitrary base. Our motivation is to check their suitability
for application to cryptography, spread-spectrum systems and use as
pseudorandom sequence.
| cs.CR | this paper examines the randomness of dsequences which are decimal sequences to an arbitrary base our motivation is to check their suitability for application to cryptography spreadspectrum systems and use as pseudorandom sequence | [['this', 'paper', 'examines', 'the', 'randomness', 'of', 'dsequences', 'which', 'are', 'decimal', 'sequences', 'to', 'an', 'arbitrary', 'base', 'our', 'motivation', 'is', 'to', 'check', 'their', 'suitability', 'for', 'application', 'to', 'cryptography', 'spreadspectrum', 'systems', 'and', 'use', 'as', 'pseudorandom', ... | [-0.16416615281592717, 0.01255311144235417, -0.0702831437952365, 0.08130951282201392, -0.05449392985213886, -0.12384155162638336, 0.06272069365491695, 0.36480568902510585, -0.30020993897183373, -0.29560139255993295, 0.14157632563376066, -0.23909110722668242, -0.19191167411874188, 0.2391614897007292, -0.1876226457287416... |
710.378 | The Galaxy Content of SDSS Clusters and Groups | Imaging data from the Sloan Digital Sky Survey are used to characterize the
population of galaxies in groups and clusters detected with the MaxBCG
algorithm. We investigate the dependence of Brightest Cluster Galaxy (BCG)
luminosity, and the distributions of satellite galaxy luminosity and satellite
color, on cluster... | astro-ph | imaging data from the sloan digital sky survey are used to characterize the population of galaxies in groups and clusters detected with the maxbcg algorithm we investigate the dependence of brightest cluster galaxy bcg luminosity and the distributions of satellite galaxy luminosity and satellite color on cluster proper... | [['imaging', 'data', 'from', 'the', 'sloan', 'digital', 'sky', 'survey', 'are', 'used', 'to', 'characterize', 'the', 'population', 'of', 'galaxies', 'in', 'groups', 'and', 'clusters', 'detected', 'with', 'the', 'maxbcg', 'algorithm', 'we', 'investigate', 'the', 'dependence', 'of', 'brightest', 'cluster', 'galaxy', 'bcg... | [-0.022496054168524487, 0.1100913814513716, -0.08226143698189027, 0.11789220291836074, -0.10036805081466327, -0.017016861877613226, 0.05651427540852099, 0.48691695098366056, -0.11628180569303888, -0.39565183577336827, 0.01589028104255926, -0.36200583909064465, 0.019125221797018026, 0.22051645066156716, -0.0332674589359... |
710.3781 | Wireless Network Information Flow | We present an achievable rate for general deterministic relay networks, with
broadcasting at the transmitters and interference at the receivers. In
particular we show that if the optimizing distribution for the
information-theoretic cut-set bound is a product distribution, then we have a
complete characterization of ... | cs.IT cs.DM math.IT math.PR | we present an achievable rate for general deterministic relay networks with broadcasting at the transmitters and interference at the receivers in particular we show that if the optimizing distribution for the informationtheoretic cutset bound is a product distribution then we have a complete characterization of the ach... | [['we', 'present', 'an', 'achievable', 'rate', 'for', 'general', 'deterministic', 'relay', 'networks', 'with', 'broadcasting', 'at', 'the', 'transmitters', 'and', 'interference', 'at', 'the', 'receivers', 'in', 'particular', 'we', 'show', 'that', 'if', 'the', 'optimizing', 'distribution', 'for', 'the', 'informationtheo... | [-0.18603048548556683, 0.028118498278561718, -0.0450597207016516, 0.06207032828370291, -0.01383936169511843, -0.19569376485263248, 0.12116767345535819, 0.3710108198816093, -0.2835201312242666, -0.21720820669902535, 0.11442991317442913, -0.2548107097788555, -0.19820959172098013, 0.17674547728014792, -0.09732030934040867... |
710.3782 | On the localization theorem for F-pure rings | We solve Grothendieck's localization problem for certain class of rings
arising from the tight closure theory. The idea of the proof depends heavily on
the study of the relative version of the Frobenius map.
| math.AC math.AG | we solve grothendiecks localization problem for certain class of rings arising from the tight closure theory the idea of the proof depends heavily on the study of the relative version of the frobenius map | [['we', 'solve', 'grothendiecks', 'localization', 'problem', 'for', 'certain', 'class', 'of', 'rings', 'arising', 'from', 'the', 'tight', 'closure', 'theory', 'the', 'idea', 'of', 'the', 'proof', 'depends', 'heavily', 'on', 'the', 'study', 'of', 'the', 'relative', 'version', 'of', 'the', 'frobenius', 'map']] | [-0.14401972933453233, -0.025211423717658308, -0.07875153389485444, 0.09471664312021698, -0.04306865272605244, -0.08221116763375261, 0.01346312984755701, 0.2185294360251111, -0.3882585313061581, -0.274343067451435, 0.1259837943362072, -0.21571364445502267, -0.1769072842948577, 0.2379129143048297, -0.15201739013633309, ... |
710.3783 | Search for axion-like particles using a variable baseline photon
regeneration technique | We report the first results of the GammeV experiment, a search for milli-eV
mass particles with axion-like couplings to two photons. The search is
performed using a "light shining through a wall" technique where incident
photons oscillate into new weakly interacting particles that are able to pass
through the wall an... | hep-ex astro-ph gr-qc | we report the first results of the gammev experiment a search for milliev mass particles with axionlike couplings to two photons the search is performed using a light shining through a wall technique where incident photons oscillate into new weakly interacting particles that are able to pass through the wall and subseq... | [['we', 'report', 'the', 'first', 'results', 'of', 'the', 'gammev', 'experiment', 'a', 'search', 'for', 'milliev', 'mass', 'particles', 'with', 'axionlike', 'couplings', 'to', 'two', 'photons', 'the', 'search', 'is', 'performed', 'using', 'a', 'light', 'shining', 'through', 'a', 'wall', 'technique', 'where', 'incident'... | [-0.07952993276359682, 0.311481920202178, -0.08044156485623469, 0.08647986349268731, -0.10274607237343761, -0.16225106366063383, 0.08345664942806418, 0.35774686978283254, -0.16973287927156144, -0.3636641166765581, 0.006161304363261231, -0.3302954013882713, 0.010956156461245634, 0.19312493176389994, 0.08810054327530617,... |
710.3784 | Evolution of Complexity | The evolution of complexity has been a central theme for Biology [2] and
Artificial Life research [1]. It is generally agreed that complexity has
increased in our universe, giving way to life, multi-cellularity, societies,
and systems of higher complexities. However, the mechanisms behind the
complexification and its... | q-bio.PE | the evolution of complexity has been a central theme for biology 2 and artificial life research 1 it is generally agreed that complexity has increased in our universe giving way to life multicellularity societies and systems of higher complexities however the mechanisms behind the complexification and its relation to e... | [['the', 'evolution', 'of', 'complexity', 'has', 'been', 'a', 'central', 'theme', 'for', 'biology', '2', 'and', 'artificial', 'life', 'research', '1', 'it', 'is', 'generally', 'agreed', 'that', 'complexity', 'has', 'increased', 'in', 'our', 'universe', 'giving', 'way', 'to', 'life', 'multicellularity', 'societies', 'an... | [-0.08146856356353506, 0.12269958743722889, -0.08517644171581024, 0.1298917970923824, -0.07427223169017495, -0.09551936764211401, 0.025876961731879904, 0.3932181492037191, -0.27653162412374743, -0.37369264313203143, 0.10779556275554383, -0.2296571959262461, -0.19479145144669735, 0.20276173193137872, -0.0889493802591689... |
710.3785 | Outflow and Accretion in Massive Star Forming Regions | In order to distinguish between the various components of massive star
forming regions (i.e. infalling, outflowing and rotating gas structures) within
our own Galaxy, we require high angular resolution observations which are
sensitive to structures on all size scales. To this end, we present
observations of the molec... | astro-ph | in order to distinguish between the various components of massive star forming regions ie infalling outflowing and rotating gas structures within our own galaxy we require high angular resolution observations which are sensitive to structures on all size scales to this end we present observations of the molecular and i... | [['in', 'order', 'to', 'distinguish', 'between', 'the', 'various', 'components', 'of', 'massive', 'star', 'forming', 'regions', 'ie', 'infalling', 'outflowing', 'and', 'rotating', 'gas', 'structures', 'within', 'our', 'own', 'galaxy', 'we', 'require', 'high', 'angular', 'resolution', 'observations', 'which', 'are', 'se... | [-0.05285521356291288, 0.09988484427477458, -0.011584772438471837, 0.015912636527941833, -0.07314233647719506, -0.06537268849600467, 0.029456452866114917, 0.41470768330318314, -0.16897526556971454, -0.36425394923576426, 0.10115448709412088, -0.27664933491408106, -0.032263684241221315, 0.11158052032302705, 0.02553092543... |
710.3786 | Reducible And Finite Dehn Fillings | We show that the distance between a finite filling slope and a reducible
filling slope on the boundary of a hyperbolic knot manifold is at most one.
| math.GT | we show that the distance between a finite filling slope and a reducible filling slope on the boundary of a hyperbolic knot manifold is at most one | [['we', 'show', 'that', 'the', 'distance', 'between', 'a', 'finite', 'filling', 'slope', 'and', 'a', 'reducible', 'filling', 'slope', 'on', 'the', 'boundary', 'of', 'a', 'hyperbolic', 'knot', 'manifold', 'is', 'at', 'most', 'one']] | [-0.23763698991388083, 0.13762620012103408, -0.15834500807923851, 0.08635317067253506, -0.09047875170492464, -0.19768179665078167, 0.06563327406291608, 0.3684184537269175, -0.24092182039748877, -0.22597269610398346, 0.09462532951255087, -0.2930954487787353, -0.1527994764899766, 0.1927840316116258, -0.07113302371430176,... |
710.3787 | Quantum Stress Tensor Fluctuations and their Physical Effects | We summarize several aspects of recent work on quantum stress tensor
fluctuations and their role in driving fluctuations of the gravitational field.
The role of correlations and anticorrelations is emphasized. We begin with a
review of the properties of the stress tensor correlation function. We next
consider some il... | gr-qc | we summarize several aspects of recent work on quantum stress tensor fluctuations and their role in driving fluctuations of the gravitational field the role of correlations and anticorrelations is emphasized we begin with a review of the properties of the stress tensor correlation function we next consider some illumin... | [['we', 'summarize', 'several', 'aspects', 'of', 'recent', 'work', 'on', 'quantum', 'stress', 'tensor', 'fluctuations', 'and', 'their', 'role', 'in', 'driving', 'fluctuations', 'of', 'the', 'gravitational', 'field', 'the', 'role', 'of', 'correlations', 'and', 'anticorrelations', 'is', 'emphasized', 'we', 'begin', 'with... | [-0.19261923437553077, 0.20848549814582945, -0.13653742781366798, 0.1169344886107235, -0.05426175526587823, -0.0449946652577576, -0.0656149739102986, 0.32485955165355734, -0.23218566835623797, -0.2771954768923939, 0.08950846256654418, -0.28125853849161614, -0.1485532141607983, 0.14339776374477706, -0.03064481775775843,... |
710.3788 | Instanton Packet Formation via a Wormhole Bridge between a Prior to our
Present Universe, and criteria for their possible break up | We present a criteria for necessary conditions for instanton formation of an
energy packet from a prior to our present universe, using the
Reissnor-Nordstrom metric which is congruent with Crowell's pseudo time
evolution version of Wheeler De Witt equation. This is based upon Wesson's
(1999) treatment of instanton fo... | physics.gen-ph | we present a criteria for necessary conditions for instanton formation of an energy packet from a prior to our present universe using the reissnornordstrom metric which is congruent with crowells pseudo time evolution version of wheeler de witt equation this is based upon wessons 1999 treatment of instanton formation i... | [['we', 'present', 'a', 'criteria', 'for', 'necessary', 'conditions', 'for', 'instanton', 'formation', 'of', 'an', 'energy', 'packet', 'from', 'a', 'prior', 'to', 'our', 'present', 'universe', 'using', 'the', 'reissnornordstrom', 'metric', 'which', 'is', 'congruent', 'with', 'crowells', 'pseudo', 'time', 'evolution', '... | [-0.10360227901451659, 0.0728738288163717, -0.18788163459371074, 0.08794699407166497, -0.10407818069838283, -0.1185909742097564, 0.026444654148717474, 0.3020913458825781, -0.21704433657376482, -0.315553663810254, 0.07329560486406161, -0.19441023681659741, -0.11722046145154993, 0.14583054554445835, -0.08285051501254634,... |
710.3789 | Frequency Analysis of Decoupling Capacitors for Three Voltage Supplies
in SoC | Reduction in power consumption has become a major criterion of design in
modern ICs. One such scheme to reduce power consumption by an IC is the use of
multiple power supplies for critical and non-critical paths. To maintain the
impedance of a power distribution system below a specified level, multiple
decoupling cap... | cs.AR | reduction in power consumption has become a major criterion of design in modern ics one such scheme to reduce power consumption by an ic is the use of multiple power supplies for critical and noncritical paths to maintain the impedance of a power distribution system below a specified level multiple decoupling capacitor... | [['reduction', 'in', 'power', 'consumption', 'has', 'become', 'a', 'major', 'criterion', 'of', 'design', 'in', 'modern', 'ics', 'one', 'such', 'scheme', 'to', 'reduce', 'power', 'consumption', 'by', 'an', 'ic', 'is', 'the', 'use', 'of', 'multiple', 'power', 'supplies', 'for', 'critical', 'and', 'noncritical', 'paths', ... | [-0.20098583699106726, 0.07589383317783575, -0.02556645572046513, 0.0004946718621415212, -0.03918883836925475, -0.1578779242786843, 0.043905267576207475, 0.33159235253914454, -0.2886002969775182, -0.3261465548273565, 0.11288779856569356, -0.2962245408779205, -0.06335360144695906, 0.24447044282812805, -0.090617511852352... |
710.379 | f(R)-Brane | We investigate the existence of brane solutions in braneworld scenarios
described by real scalar field in the presence of modified $f(R)$ gravity with
a single extra dimension. In the case of constant curvature, we obtain
first-order differential equations which solve the equations of motion and ease
the search for e... | hep-th | we investigate the existence of brane solutions in braneworld scenarios described by real scalar field in the presence of modified fr gravity with a single extra dimension in the case of constant curvature we obtain firstorder differential equations which solve the equations of motion and ease the search for explicit a... | [['we', 'investigate', 'the', 'existence', 'of', 'brane', 'solutions', 'in', 'braneworld', 'scenarios', 'described', 'by', 'real', 'scalar', 'field', 'in', 'the', 'presence', 'of', 'modified', 'fr', 'gravity', 'with', 'a', 'single', 'extra', 'dimension', 'in', 'the', 'case', 'of', 'constant', 'curvature', 'we', 'obtain... | [-0.1791219179615823, 0.02800731333111649, -0.011853881652897863, 0.075954673839594, -0.10823827223685473, -0.15626174495763964, -0.049341925805601386, 0.2639409783087782, -0.20654938007885618, -0.3170280501441057, 0.111008864163713, -0.24374676357482128, -0.16157000614747183, 0.17330098268575966, -0.03583105713295848,... |
710.3791 | New constraints on supersymmetric models from b -> s gamma | We provide an analysis of the parameter space of several supersymmetry
breaking scenarios such as the minimal supergravity (mSUGRA) model and the non
universal Higgs mass (NUHM) framework, as well as the Anomaly Mediated
Supersymmetry Breaking (AMSB) and the Gauge Mediated Supersymmetry Breaking
(GMSB) models, in the... | hep-ph | we provide an analysis of the parameter space of several supersymmetry breaking scenarios such as the minimal supergravity msugra model and the non universal higgs mass nuhm framework as well as the anomaly mediated supersymmetry breaking amsb and the gauge mediated supersymmetry breaking gmsb models in the light of a ... | [['we', 'provide', 'an', 'analysis', 'of', 'the', 'parameter', 'space', 'of', 'several', 'supersymmetry', 'breaking', 'scenarios', 'such', 'as', 'the', 'minimal', 'supergravity', 'msugra', 'model', 'and', 'the', 'non', 'universal', 'higgs', 'mass', 'nuhm', 'framework', 'as', 'well', 'as', 'the', 'anomaly', 'mediated', ... | [-0.13755116616777177, 0.22410013896246553, -0.0015614158983727725, 0.1279990460619266, -0.08639302787788469, -0.16260992607487174, 0.09371164880195183, 0.3243520662316988, -0.1971417347097705, -0.28962812222026546, 0.07956874791757557, -0.24680563857586219, -0.07630044505128573, 0.13070646533100255, 0.0359852735571370... |
710.3792 | Approximating critical parameters of branching random walks | Given a branching random walk on a graph, we consider two kinds of
truncations: by inhibiting the reproduction outside a subset of vertices and by
allowing at most $m$ particles per site. We investigate the convergence of weak
and strong critical parameters of these truncated branching random walks to the
analogous p... | math.PR | given a branching random walk on a graph we consider two kinds of truncations by inhibiting the reproduction outside a subset of vertices and by allowing at most m particles per site we investigate the convergence of weak and strong critical parameters of these truncated branching random walks to the analogous paramete... | [['given', 'a', 'branching', 'random', 'walk', 'on', 'a', 'graph', 'we', 'consider', 'two', 'kinds', 'of', 'truncations', 'by', 'inhibiting', 'the', 'reproduction', 'outside', 'a', 'subset', 'of', 'vertices', 'and', 'by', 'allowing', 'at', 'most', 'm', 'particles', 'per', 'site', 'we', 'investigate', 'the', 'convergenc... | [-0.12534727166599496, 0.1999306844697259, -0.02706732794150025, 0.031724252577485706, -0.03796133305877447, -0.12482091809098406, 0.18127124392609487, 0.35091576117208634, -0.24000554475745978, -0.19539997220606725, 0.09898893984205935, -0.25290543111790525, -0.1250191811129622, 0.12641482476690977, -0.015107454346685... |
710.3793 | Depressed Surface Magnetization in Thin La0.8MnO3 Films | A systematic study the magnetization in La0.8.MnO3 films of thickness varying
from ultra-thin to bulk-like has been conducted. The study reveals suppression
of the bulk magnetization for films up to at least 1600 A. In addition, the
surface (top 50 A) of all films exhibits depressed magnetization as observed by
x-ray... | cond-mat.str-el | a systematic study the magnetization in la08mno3 films of thickness varying from ultrathin to bulklike has been conducted the study reveals suppression of the bulk magnetization for films up to at least 1600 a in addition the surface top 50 a of all films exhibits depressed magnetization as observed by xray magnetic ci... | [['a', 'systematic', 'study', 'the', 'magnetization', 'in', 'la08mno3', 'films', 'of', 'thickness', 'varying', 'from', 'ultrathin', 'to', 'bulklike', 'has', 'been', 'conducted', 'the', 'study', 'reveals', 'suppression', 'of', 'the', 'bulk', 'magnetization', 'for', 'films', 'up', 'to', 'at', 'least', '1600', 'a', 'in', ... | [-0.1448408718897055, 0.18229478787732858, -0.033161091127062906, -0.03753020145375384, -0.03100935608301669, -0.07818328204551993, 0.07629344824778095, 0.42540830668470225, -0.26540522963727176, -0.3486761533438343, 0.016164532974234796, -0.34281964791453867, -0.0439251181446271, 0.20830825900607933, 0.070042399338714... |
710.3794 | Curve complexes are rigid | Any quasi-isometry of the complex of curves is bounded distance from a
simplicial automorphism. As a consequence, the quasi-isometry type of the curve
complex determines the homeomorphism type of the surface.
| math.GT | any quasiisometry of the complex of curves is bounded distance from a simplicial automorphism as a consequence the quasiisometry type of the curve complex determines the homeomorphism type of the surface | [['any', 'quasiisometry', 'of', 'the', 'complex', 'of', 'curves', 'is', 'bounded', 'distance', 'from', 'a', 'simplicial', 'automorphism', 'as', 'a', 'consequence', 'the', 'quasiisometry', 'type', 'of', 'the', 'curve', 'complex', 'determines', 'the', 'homeomorphism', 'type', 'of', 'the', 'surface']] | [-0.21481500632099568, 0.07714570707250987, -0.1170141285345439, 0.07308059271740457, -0.13201332990560802, -0.1311192289896069, 0.03608304661728682, 0.3119996008613417, -0.437217706574067, -0.2197917035270122, 0.09937729172769093, -0.26168186025273416, -0.18921586654839978, 0.22174315043394605, -0.21150413906622317, -... |
710.3795 | Localizing coalescing massive black hole binaries with gravitational
waves | Massive black hole binary coalescences are prime targets for space-based
gravitational wave (GW) observatories such as {\it LISA}. GW measurements can
localize the position of a coalescing binary on the sky to an ellipse with a
major axis of a few tens of arcminutes to a few degrees, depending on source
redshift, and... | astro-ph gr-qc | massive black hole binary coalescences are prime targets for spacebased gravitational wave gw observatories such as it lisa gw measurements can localize the position of a coalescing binary on the sky to an ellipse with a major axis of a few tens of arcminutes to a few degrees depending on source redshift and a minor ax... | [['massive', 'black', 'hole', 'binary', 'coalescences', 'are', 'prime', 'targets', 'for', 'spacebased', 'gravitational', 'wave', 'gw', 'observatories', 'such', 'as', 'it', 'lisa', 'gw', 'measurements', 'can', 'localize', 'the', 'position', 'of', 'a', 'coalescing', 'binary', 'on', 'the', 'sky', 'to', 'an', 'ellipse', 'w... | [-0.12566074021534085, 0.12758427942858067, -0.0314471009616508, 0.1142581077681937, -0.09915900045494094, -0.07569805325291822, 0.04425989448986058, 0.3867157515863103, -0.20408821002653332, -0.35774182324828546, 0.1145025703693667, -0.3162336366079468, -0.013973494300319982, 0.2488924525972176, -0.005309258123586406,... |
710.3796 | Sweet Spot Supersymmetry and Composite Messengers | Sweet spot supersymmetry is a phenomenologically and cosmologically perfect
framework to realize a supersymmetric world at short distance. We discuss a
class of dynamical models of supersymmetry breaking and its mediation whose
low-energy effective description falls into this framework. Hadron fields in
the dynamical... | hep-ph hep-th | sweet spot supersymmetry is a phenomenologically and cosmologically perfect framework to realize a supersymmetric world at short distance we discuss a class of dynamical models of supersymmetry breaking and its mediation whose lowenergy effective description falls into this framework hadron fields in the dynamical mode... | [['sweet', 'spot', 'supersymmetry', 'is', 'a', 'phenomenologically', 'and', 'cosmologically', 'perfect', 'framework', 'to', 'realize', 'a', 'supersymmetric', 'world', 'at', 'short', 'distance', 'we', 'discuss', 'a', 'class', 'of', 'dynamical', 'models', 'of', 'supersymmetry', 'breaking', 'and', 'its', 'mediation', 'who... | [-0.1680068111579333, 0.2711814472128694, -0.061131994596359374, 0.18219429352653346, -0.07841352977770932, -0.13912761759735187, 0.009262485692173014, 0.33381885432695246, -0.19715884397737682, -0.3708225410355597, 0.09154925804005518, -0.2078322632076713, -0.09186814695226067, 0.1452064428915631, -0.01453601891098886... |
710.3797 | Two-dimensional magnetoexcitons in the presence of spin-orbit coupling | We study theoretically the effect of spin-orbit coupling on quantum well
excitons in a strong magnetic field. We show that, in the presence of an
in-plane field component, the excitonic absorption spectrum develops a
double-peak structure due to hybridization of bright and dark magnetoexcitons.
If the Rashba and Dres... | cond-mat.mes-hall | we study theoretically the effect of spinorbit coupling on quantum well excitons in a strong magnetic field we show that in the presence of an inplane field component the excitonic absorption spectrum develops a doublepeak structure due to hybridization of bright and dark magnetoexcitons if the rashba and dresselhaus s... | [['we', 'study', 'theoretically', 'the', 'effect', 'of', 'spinorbit', 'coupling', 'on', 'quantum', 'well', 'excitons', 'in', 'a', 'strong', 'magnetic', 'field', 'we', 'show', 'that', 'in', 'the', 'presence', 'of', 'an', 'inplane', 'field', 'component', 'the', 'excitonic', 'absorption', 'spectrum', 'develops', 'a', 'dou... | [-0.2473044905345887, 0.17876150351717282, -0.030054968711165538, 0.05895954478290622, -0.07724731290471498, -0.09430949990120199, -0.005066150580575966, 0.4474425268256002, -0.3019060907299044, -0.3301396443836253, -0.09228718654183601, -0.2538942824359293, -0.11651553432629616, 0.20683678124030982, 0.0814620261339263... |
710.3798 | The moduli space of parallelizable 4-manifolds | In this paper we construct the space of smooth 4-manifolds and find the
homotopy model for the connected components of the complement to the
discriminant.
The discriminant of this space is a singular hypersurface and its generic
points correspond to manifolds with isolated Morse singularities.
These spaces can be... | math.GT math-ph math.MP | in this paper we construct the space of smooth 4manifolds and find the homotopy model for the connected components of the complement to the discriminant the discriminant of this space is a singular hypersurface and its generic points correspond to manifolds with isolated morse singularities these spaces can be consider... | [['in', 'this', 'paper', 'we', 'construct', 'the', 'space', 'of', 'smooth', '4manifolds', 'and', 'find', 'the', 'homotopy', 'model', 'for', 'the', 'connected', 'components', 'of', 'the', 'complement', 'to', 'the', 'discriminant', 'the', 'discriminant', 'of', 'this', 'space', 'is', 'a', 'singular', 'hypersurface', 'and'... | [-0.1559146071431806, 0.07861797056731931, -0.12496406175531782, 0.07430675254950116, -0.07780238962522498, -0.1037461642209474, -0.012215232128394884, 0.30141562804881783, -0.2815564473470052, -0.2472430015536579, 0.1044884918012178, -0.25455331543108095, -0.1731281402501957, 0.1947194744669203, -0.13010712960516815, ... |
710.3799 | On the Physics Case of a Super Flavour Factory | We summarize the physics case of a high-luminosity e+e- flavour factory
collecting an integrated luminosity of 50-75 ab^(-1). Many New Physics
sensitive measurements involving B and D mesons and tau leptons, unique to a
Super Flavour Factory, can be performed with excellent sensitivity to new
particles with masses up... | hep-ph hep-ex | we summarize the physics case of a highluminosity ee flavour factory collecting an integrated luminosity of 5075 ab1 many new physics sensitive measurements involving b and d mesons and tau leptons unique to a super flavour factory can be performed with excellent sensitivity to new particles with masses up to 100 or ev... | [['we', 'summarize', 'the', 'physics', 'case', 'of', 'a', 'highluminosity', 'ee', 'flavour', 'factory', 'collecting', 'an', 'integrated', 'luminosity', 'of', '5075', 'ab1', 'many', 'new', 'physics', 'sensitive', 'measurements', 'involving', 'b', 'and', 'd', 'mesons', 'and', 'tau', 'leptons', 'unique', 'to', 'a', 'super... | [-0.04599209921015007, 0.2710320498546017, -0.05888374715724641, 0.12885814054915262, -0.09076827975107474, -0.24462424668793878, 0.02773076156364032, 0.29881968975553774, -0.2361358755555524, -0.3446126261910608, 0.09362009610836017, -0.32747449598333855, 0.06622300617059122, 0.16189693806793642, 0.04947723405486023, ... |
710.38 | Community Detection via Facility Location | In this paper we apply theoretical and practical results from facility
location theory to the problem of community detection in networks. The result
is an algorithm that computes bounds on a minimization variant of local
modularity. We also define the concept of an edge support and a new measure of
the goodness of co... | physics.soc-ph physics.data-an | in this paper we apply theoretical and practical results from facility location theory to the problem of community detection in networks the result is an algorithm that computes bounds on a minimization variant of local modularity we also define the concept of an edge support and a new measure of the goodness of commun... | [['in', 'this', 'paper', 'we', 'apply', 'theoretical', 'and', 'practical', 'results', 'from', 'facility', 'location', 'theory', 'to', 'the', 'problem', 'of', 'community', 'detection', 'in', 'networks', 'the', 'result', 'is', 'an', 'algorithm', 'that', 'computes', 'bounds', 'on', 'a', 'minimization', 'variant', 'of', 'l... | [-0.08536385828241085, 0.0041562117957154344, -0.12489615033458297, 0.0351870042165198, -0.09955809588751031, -0.07377919535307835, 0.05988037593003052, 0.4127994163427502, -0.2891376630286686, -0.3107409237458746, 0.09009877014452489, -0.24622099064031822, -0.2462669180887234, 0.21396025634991625, -0.1199016193956292,... |
710.3801 | Levi-flat hypersurfaces with real analytic boundary | Let $X$ be a Stein manifold of dimension at least 3. Given a compact
codimension 2 real analytic submanifold $M$ of $X$, that is the boundary of a
compact Levi-flat hypersurface $H$, we study the regularity of $H$. Suppose
that the CR singularities of $M$ are an $\mathcal{O}(X)$-convex set. For
example, suppose $M$ h... | math.CV math.AP | let x be a stein manifold of dimension at least 3 given a compact codimension 2 real analytic submanifold m of x that is the boundary of a compact leviflat hypersurface h we study the regularity of h suppose that the cr singularities of m are an mathcaloxconvex set for example suppose m has only finitely many cr singul... | [['let', 'x', 'be', 'a', 'stein', 'manifold', 'of', 'dimension', 'at', 'least', '3', 'given', 'a', 'compact', 'codimension', '2', 'real', 'analytic', 'submanifold', 'm', 'of', 'x', 'that', 'is', 'the', 'boundary', 'of', 'a', 'compact', 'leviflat', 'hypersurface', 'h', 'we', 'study', 'the', 'regularity', 'of', 'h', 'sup... | [-0.2237110094312605, 0.04419653589355492, -0.1018968711224061, 0.0767227566498827, -0.09501270877844686, -0.1745325217571717, -0.0579313291963322, 0.3389115092536131, -0.24557859498135587, -0.1691393464876352, 0.10939242361288465, -0.2839925761552567, -0.15351533488839442, 0.2145777291945241, -0.12350004276009739, -0.... |
710.3802 | A Posteriori Equivalence: A New Perspective for Design of Optimal
Channel Shortening Equalizers | The problem of channel shortening equalization for optimal detection in ISI
channels is considered. The problem is to choose a linear equalizer and a
partial response target filter such that the combination produces the best
detection performance. Instead of using the traditional approach of MMSE
equalization, we dir... | cs.IT math.IT | the problem of channel shortening equalization for optimal detection in isi channels is considered the problem is to choose a linear equalizer and a partial response target filter such that the combination produces the best detection performance instead of using the traditional approach of mmse equalization we directly... | [['the', 'problem', 'of', 'channel', 'shortening', 'equalization', 'for', 'optimal', 'detection', 'in', 'isi', 'channels', 'is', 'considered', 'the', 'problem', 'is', 'to', 'choose', 'a', 'linear', 'equalizer', 'and', 'a', 'partial', 'response', 'target', 'filter', 'such', 'that', 'the', 'combination', 'produces', 'the... | [-0.11390476570435701, -0.009973418955009297, -0.06308408248885256, 0.06079987000270579, -0.07671292716302493, -0.1927617606041687, 0.09160799495575409, 0.42866641532818567, -0.26688575050965263, -0.2676747398169857, 0.10803226238032931, -0.2527821834632603, -0.180785461726989, 0.14925871825399314, -0.11439098978698391... |
710.3803 | Massive expanding torus and fast outflow in planetary nebula NGC 6302 | We present interferometric observations of $^{12}$CO and $^{13}$CO $J$=2$-$1
emission from the butterfly-shaped, young planetary nebula NGC 6302. The high
angular resolution and high sensitivity achieved in our observations allow us
to resolve the nebula into two distinct kinematic components: (1) a massive
expanding... | astro-ph | we present interferometric observations of 12co and 13co j21 emission from the butterflyshaped young planetary nebula ngc 6302 the high angular resolution and high sensitivity achieved in our observations allow us to resolve the nebula into two distinct kinematic components 1 a massive expanding torus seen almost edgeo... | [['we', 'present', 'interferometric', 'observations', 'of', '12co', 'and', '13co', 'j21', 'emission', 'from', 'the', 'butterflyshaped', 'young', 'planetary', 'nebula', 'ngc', '6302', 'the', 'high', 'angular', 'resolution', 'and', 'high', 'sensitivity', 'achieved', 'in', 'our', 'observations', 'allow', 'us', 'to', 'reso... | [-0.08694135099448536, 0.07400192371445947, 0.016112370461851887, 0.026122577854151945, -0.06552536287901313, -0.08462396118093479, -0.03265547834656642, 0.5038914595590492, -0.178189286067917, -0.31287477212361536, 0.02946518778242583, -0.2343000225636251, 0.03317428906051549, 0.17072769079720024, 0.00956667216782627,... |
710.3804 | Random subcubes as a toy model for constraint satisfaction problems | We present an exactly solvable random-subcube model inspired by the structure
of hard constraint satisfaction and optimization problems. Our model reproduces
the structure of the solution space of the random k-satisfiability and
k-coloring problems, and undergoes the same phase transitions as these
problems. The comp... | cs.CC cond-mat.dis-nn | we present an exactly solvable randomsubcube model inspired by the structure of hard constraint satisfaction and optimization problems our model reproduces the structure of the solution space of the random ksatisfiability and kcoloring problems and undergoes the same phase transitions as these problems the comparison b... | [['we', 'present', 'an', 'exactly', 'solvable', 'randomsubcube', 'model', 'inspired', 'by', 'the', 'structure', 'of', 'hard', 'constraint', 'satisfaction', 'and', 'optimization', 'problems', 'our', 'model', 'reproduces', 'the', 'structure', 'of', 'the', 'solution', 'space', 'of', 'the', 'random', 'ksatisfiability', 'an... | [-0.10359169897175842, 0.08426694306654571, -0.08629909575638639, 0.12513682098194426, -0.049919161522252994, -0.12251380405860482, 0.03631744999136147, 0.35698094905970934, -0.3395883096502973, -0.3235993342982097, 0.11555066410687982, -0.26598875918848947, -0.1866073033639363, 0.15817801727211805, -0.0131318930887266... |
710.3805 | Cherenkov Flashes and Fluorescence Flares on Telescopes: New lights on
UHECR Spectroscopy while unveiling Neutrinos Astronomy | Cherenkov Telescopes (as Magic, Hess and Veritas), while pointing
horizontally should reveal also the fluorescence flare tails of nearby
down-going air-showers. Such air-showers, born at higher (tens km) altitudes,
are growing and extending up to lowest atmospheres (EeVs) or up to higher (few
km) quotas (PeVs). Vicev... | astro-ph hep-ph | cherenkov telescopes as magic hess and veritas while pointing horizontally should reveal also the fluorescence flare tails of nearby downgoing airshowers such airshowers born at higher tens km altitudes are growing and extending up to lowest atmospheres eevs or up to higher few km quotas pevs viceversa as it has been f... | [['cherenkov', 'telescopes', 'as', 'magic', 'hess', 'and', 'veritas', 'while', 'pointing', 'horizontally', 'should', 'reveal', 'also', 'the', 'fluorescence', 'flare', 'tails', 'of', 'nearby', 'downgoing', 'airshowers', 'such', 'airshowers', 'born', 'at', 'higher', 'tens', 'km', 'altitudes', 'are', 'growing', 'and', 'ex... | [-0.07861938461476614, 0.26457965319345067, -0.011375860272606543, 0.15819237029472413, -0.11899556804155885, -0.09306946035266724, -0.016898346379830325, 0.44439509916787945, -0.20452257461676543, -0.42042968409859444, 0.07120043573244898, -0.33754689732474114, -0.014350776427833379, 0.2072254314783899, -0.00649467468... |
710.3806 | Internal shocks in relativistic jets with time--dependent sources | We present a ballistic description of the formation and propagation of the
working surface of a relativistic jet. Using simple laws of conservation of
mass and linear momentum at the working surface, we obtain a full description
of the working surface flow parametrised by the initial velocity and mass
injection rate.... | astro-ph | we present a ballistic description of the formation and propagation of the working surface of a relativistic jet using simple laws of conservation of mass and linear momentum at the working surface we obtain a full description of the working surface flow parametrised by the initial velocity and mass injection rate this... | [['we', 'present', 'a', 'ballistic', 'description', 'of', 'the', 'formation', 'and', 'propagation', 'of', 'the', 'working', 'surface', 'of', 'a', 'relativistic', 'jet', 'using', 'simple', 'laws', 'of', 'conservation', 'of', 'mass', 'and', 'linear', 'momentum', 'at', 'the', 'working', 'surface', 'we', 'obtain', 'a', 'fu... | [-0.0926268213608813, 0.10923404861842433, -0.12087818745884203, 0.06386116139080016, -0.056646167676174836, -0.09142520828773418, 0.03930951937612507, 0.3619255952056377, -0.22454842601211802, -0.3289962972784715, 0.038109009000923365, -0.22792383464778052, -0.0577060921598346, 0.24910275264673176, -0.0091135591764243... |
710.3807 | Directed destabilization of lysozyme in protic ionic liquids reveals a
compact, low energy, soluble, reversibly-unfolding (pre-fibril) state | Recent demonstrations of extraordinary stabilization of proteins in mobile
protic [1] and aprotic [2] ionic liquid solutions at ambient temperatures have
raised hopes of new biopreservation and drug transportation technologies. Here
we examine the relation of folded protein stability to the state of the
transferred p... | physics.bio-ph physics.chem-ph | recent demonstrations of extraordinary stabilization of proteins in mobile protic 1 and aprotic 2 ionic liquid solutions at ambient temperatures have raised hopes of new biopreservation and drug transportation technologies here we examine the relation of folded protein stability to the state of the transferred proton 1... | [['recent', 'demonstrations', 'of', 'extraordinary', 'stabilization', 'of', 'proteins', 'in', 'mobile', 'protic', '1', 'and', 'aprotic', '2', 'ionic', 'liquid', 'solutions', 'at', 'ambient', 'temperatures', 'have', 'raised', 'hopes', 'of', 'new', 'biopreservation', 'and', 'drug', 'transportation', 'technologies', 'here... | [-0.11595014737462563, 0.19447452084106218, -0.03180635747629286, 0.02181213885089032, 0.019385317866289557, -0.13880162042124652, 0.05783850941514066, 0.36802644352891195, -0.26933297604963874, -0.2968334558648088, 0.07018845437737552, -0.27369109235876643, -0.11511201797275256, 0.14261282991543905, -0.018636202396491... |
710.3808 | Finite Mirror Effects in Advanced Interferometric Gravitational Wave
Detectors | Thermal noise is expected to be the dominant source of noise in the most
sensitive frequency band of second generation ground based gravitational wave
detectors. Reshaping the beam to a flatter wider profile which probes more of
the mirror surface reduces this noise. The "Mesa" beam shape has been proposed
for this p... | gr-qc | thermal noise is expected to be the dominant source of noise in the most sensitive frequency band of second generation ground based gravitational wave detectors reshaping the beam to a flatter wider profile which probes more of the mirror surface reduces this noise the mesa beam shape has been proposed for this purpose... | [['thermal', 'noise', 'is', 'expected', 'to', 'be', 'the', 'dominant', 'source', 'of', 'noise', 'in', 'the', 'most', 'sensitive', 'frequency', 'band', 'of', 'second', 'generation', 'ground', 'based', 'gravitational', 'wave', 'detectors', 'reshaping', 'the', 'beam', 'to', 'a', 'flatter', 'wider', 'profile', 'which', 'pr... | [-0.08838328744959936, 0.15944696780964676, -0.10263773489978718, 0.07701367544554015, -0.05430947547249986, -0.15222925020085332, 0.04049613838290286, 0.39731452513444254, -0.26091572756445597, -0.32261179449281635, 0.06816773835463276, -0.28284625029386745, -0.07522171000856584, 0.19149068107499795, -0.05078506262248... |
710.3809 | A precessing jet model for the PN K 3-35: simulated radio-continuum
emission | The bipolar morphology of the planetary nebula (PN) K 3-35 observed in
radio-continuum images was modelled with 3D hydrodynamic simulations with the
adaptive grid code yguazu-a. We find that the observed morphology of this PN
can be reproduced considering a precessing jet evolving in a dense AGB
circumstellar medium,... | astro-ph | the bipolar morphology of the planetary nebula pn k 335 observed in radiocontinuum images was modelled with 3d hydrodynamic simulations with the adaptive grid code yguazua we find that the observed morphology of this pn can be reproduced considering a precessing jet evolving in a dense agb circumstellar medium given by... | [['the', 'bipolar', 'morphology', 'of', 'the', 'planetary', 'nebula', 'pn', 'k', '335', 'observed', 'in', 'radiocontinuum', 'images', 'was', 'modelled', 'with', '3d', 'hydrodynamic', 'simulations', 'with', 'the', 'adaptive', 'grid', 'code', 'yguazua', 'we', 'find', 'that', 'the', 'observed', 'morphology', 'of', 'this',... | [-0.1302996341427185, 0.09016146578846111, -0.056237262918231945, 0.023752939655351715, -0.043941899983332956, -0.06884185011706336, 0.006948712709018116, 0.44021829072278823, -0.20236099322440385, -0.3293014254266892, 0.05037874386230443, -0.24821615521963553, -0.006927223368581358, 0.21406161333576662, -0.00345355269... |
710.381 | On the number of tetrahedra with minimum, unit, and distinct volumes in
three-space | We formulate and give partial answers to several combinatorial problems on
volumes of simplices determined by $n$ points in 3-space, and in general in $d$
dimensions. (i) The number of tetrahedra of minimum (nonzero) volume spanned by
$n$ points in $\RR^3$ is at most ${2/3}n^3-O(n^2)$, and there are point sets
for wh... | math.CO | we formulate and give partial answers to several combinatorial problems on volumes of simplices determined by n points in 3space and in general in d dimensions i the number of tetrahedra of minimum nonzero volume spanned by n points in rr3 is at most 23n3on2 and there are point sets for which this number is 316n3on2 we... | [['we', 'formulate', 'and', 'give', 'partial', 'answers', 'to', 'several', 'combinatorial', 'problems', 'on', 'volumes', 'of', 'simplices', 'determined', 'by', 'n', 'points', 'in', '3space', 'and', 'in', 'general', 'in', 'd', 'dimensions', 'i', 'the', 'number', 'of', 'tetrahedra', 'of', 'minimum', 'nonzero', 'volume', ... | [-0.21712410381723266, 0.14888032732125783, 0.04143907979813329, -0.007129860273996217, 0.016356642619758752, -0.14615533742417366, 0.11896560058107611, 0.3160025814247335, -0.23643444519365633, -0.28752971275692213, 0.07636123624129904, -0.36025360999455364, -0.12429430807929093, 0.15014686119440446, -0.10473088225384... |
710.3811 | Coherent population oscillation from a Fermi atom-molecule dark state | We show that a robust macroscopic atom-molecule dark state can exist in
fermionic systems, which represents a coherent superposition between the ground
molecular BEC and the atomic BCS paired state. We take advantage of the
tunability offered by external laser fields, and explore this superposition for
demonstrating ... | cond-mat.other | we show that a robust macroscopic atommolecule dark state can exist in fermionic systems which represents a coherent superposition between the ground molecular bec and the atomic bcs paired state we take advantage of the tunability offered by external laser fields and explore this superposition for demonstrating cohere... | [['we', 'show', 'that', 'a', 'robust', 'macroscopic', 'atommolecule', 'dark', 'state', 'can', 'exist', 'in', 'fermionic', 'systems', 'which', 'represents', 'a', 'coherent', 'superposition', 'between', 'the', 'ground', 'molecular', 'bec', 'and', 'the', 'atomic', 'bcs', 'paired', 'state', 'we', 'take', 'advantage', 'of',... | [-0.2121454912370869, 0.24491971152435457, -0.08600142929436905, 0.09595377013985333, 0.003824466573340552, -0.11238668354760323, 0.1031086569252823, 0.35100286512502604, -0.255963747815362, -0.271612318046391, -0.07650246839371642, -0.22960325098663037, -0.059160855043280336, 0.16689329051545687, 0.06766280294063368, ... |
710.3812 | Flow- and Diffusion Distributed Structures with noise at the inlet | Flow and Diffusion Distributed Structures (FDS) are stationary spatially
periodic patterns that can be observed in reaction-diffusion-advection systems.
These structures arise when the flow rate exceeds a certain bifurcation point
provided that concentrations of interacting species at the inlet differ from
steady sta... | nlin.PS | flow and diffusion distributed structures fds are stationary spatially periodic patterns that can be observed in reactiondiffusionadvection systems these structures arise when the flow rate exceeds a certain bifurcation point provided that concentrations of interacting species at the inlet differ from steady state valu... | [['flow', 'and', 'diffusion', 'distributed', 'structures', 'fds', 'are', 'stationary', 'spatially', 'periodic', 'patterns', 'that', 'can', 'be', 'observed', 'in', 'reactiondiffusionadvection', 'systems', 'these', 'structures', 'arise', 'when', 'the', 'flow', 'rate', 'exceeds', 'a', 'certain', 'bifurcation', 'point', 'p... | [-0.20544998353320487, 0.20997674259215157, -0.05010073430314185, 0.0817699148742316, 0.01562993012362747, -0.14265774285634328, 0.009492883013092741, 0.33671025922937187, -0.30654717786652835, -0.24984744997030706, 0.1361477155798963, -0.2699635383750128, -0.1200637689637388, 0.1848567602266172, -0.035683247616668794,... |
710.3813 | Shape transformations of a compartmentalized fluid surface | A surface model on compartmentalized spheres is studied by using the Monte
Carlo simulation technique with dynamical triangulations. We found that the
model exhibits a variety of phases: the spherical phase, the tubular phase, the
planar phase, the wormlike planar phase, the wormlike long phase, the wormlike
short ph... | cond-mat.stat-mech cond-mat.soft | a surface model on compartmentalized spheres is studied by using the monte carlo simulation technique with dynamical triangulations we found that the model exhibits a variety of phases the spherical phase the tubular phase the planar phase the wormlike planar phase the wormlike long phase the wormlike short phase and t... | [['a', 'surface', 'model', 'on', 'compartmentalized', 'spheres', 'is', 'studied', 'by', 'using', 'the', 'monte', 'carlo', 'simulation', 'technique', 'with', 'dynamical', 'triangulations', 'we', 'found', 'that', 'the', 'model', 'exhibits', 'a', 'variety', 'of', 'phases', 'the', 'spherical', 'phase', 'the', 'tubular', 'p... | [-0.1692528833437041, 0.23922277814333365, -0.08505029963296756, 0.000913197718961001, -0.015559882199261011, -0.10140500019259523, 0.01994550384973225, 0.4320549369838677, -0.2971302849289618, -0.25749589997882905, 0.09150792666090031, -0.2770835422142817, -0.21663989558031685, 0.12639998026567986, 0.03662070698102757... |
710.3814 | Finsleroid-Finsler Space of Involutive Case | The Finsleroid-Finsler space is constructed over an underlying Riemannian
space by the help of a scalar $g(x)$ and an input 1-form $b$ of unit length.
Explicit form of the entailed tensors, as well as the respective spray
coefficients, is evaluated. The involutive case means the framework in which
the characteristic ... | math.DG math-ph math.MP | the finsleroidfinsler space is constructed over an underlying riemannian space by the help of a scalar gx and an input 1form b of unit length explicit form of the entailed tensors as well as the respective spray coefficients is evaluated the involutive case means the framework in which the characteristic scalar gx may ... | [['the', 'finsleroidfinsler', 'space', 'is', 'constructed', 'over', 'an', 'underlying', 'riemannian', 'space', 'by', 'the', 'help', 'of', 'a', 'scalar', 'gx', 'and', 'an', 'input', '1form', 'b', 'of', 'unit', 'length', 'explicit', 'form', 'of', 'the', 'entailed', 'tensors', 'as', 'well', 'as', 'the', 'respective', 'spr... | [-0.1816962521675299, 0.128317232151893, -0.041910715743199045, 0.03805428326613623, -0.12238917992876251, -0.1416768213777348, -0.0615710641596784, 0.36869733906242735, -0.2890995115965836, -0.22182818540812346, 0.070218027765184, -0.24674178023512164, -0.18234226771796397, 0.12807155608121926, -0.016050822365047165, ... |
710.3815 | Eigenmodes of elastic vibrations of quaking neutron star encoded in QPOs
on light curves of SGR flares | The Newtonian solid-mechanical theory of nodeless spheroidal and torsional of
elastic seismic vibrations trapped in the crust of a quaking neutron star is
outlined and applied to the modal classification of the quasi-periodic
oscillations (QPOs) of X-ray luminosity in the aftermath of giant flares in SGR
1806-20 and ... | astro-ph | the newtonian solidmechanical theory of nodeless spheroidal and torsional of elastic seismic vibrations trapped in the crust of a quaking neutron star is outlined and applied to the modal classification of the quasiperiodic oscillations qpos of xray luminosity in the aftermath of giant flares in sgr 180620 and sgr 1900... | [['the', 'newtonian', 'solidmechanical', 'theory', 'of', 'nodeless', 'spheroidal', 'and', 'torsional', 'of', 'elastic', 'seismic', 'vibrations', 'trapped', 'in', 'the', 'crust', 'of', 'a', 'quaking', 'neutron', 'star', 'is', 'outlined', 'and', 'applied', 'to', 'the', 'modal', 'classification', 'of', 'the', 'quasiperiod... | [-0.1381458219420165, 0.1557714792972062, -0.048047006878380975, 0.06671397470093021, -0.20077090767522654, -0.04944593116951485, 0.059916105900580684, 0.36427195366472004, -0.1783416065449516, -0.27473966454466187, 0.0398221286564755, -0.28293036806086697, -0.055126961986728326, 0.2631633692964291, -0.0389578534266911... |
710.3816 | Uniting the Quiescent Emission and Burst Spectra of Magnetar Candidates | Spectral studies of quiescent emission and bursts of magnetar candidates
using XMM-Newton, Chandra and Swift data are presented. Spectra of both the
quiescent emission and the bursts for most magnetar candidates are reproduced
by a photoelectrically absorbed two blackbody function (2BB). There is a strong
correlation... | astro-ph | spectral studies of quiescent emission and bursts of magnetar candidates using xmmnewton chandra and swift data are presented spectra of both the quiescent emission and the bursts for most magnetar candidates are reproduced by a photoelectrically absorbed two blackbody function 2bb there is a strong correlation between... | [['spectral', 'studies', 'of', 'quiescent', 'emission', 'and', 'bursts', 'of', 'magnetar', 'candidates', 'using', 'xmmnewton', 'chandra', 'and', 'swift', 'data', 'are', 'presented', 'spectra', 'of', 'both', 'the', 'quiescent', 'emission', 'and', 'the', 'bursts', 'for', 'most', 'magnetar', 'candidates', 'are', 'reproduc... | [-0.07624330838983197, 0.17379828726117877, -0.04112989275984923, 0.1746285823017654, -0.10662504295795792, -0.1335969863845626, 0.05699615030430212, 0.4523010713434437, -0.1359102247238852, -0.3817356927661089, 0.08003000487082229, -0.3498430274449652, -0.010880293906666338, 0.2475886656476821, -0.0076730060469211514,... |
710.3817 | A Note on Comparison of Error Correction Codes | Use of an error correction code in a given transmission channel can be
regarded as the statistical experiment. Therefore, powerful results from the
theory of comparison of experiments can be applied to compare the performances
of different error correction codes. We present results on the comparison of
block error co... | cs.IT math.IT math.ST stat.TH | use of an error correction code in a given transmission channel can be regarded as the statistical experiment therefore powerful results from the theory of comparison of experiments can be applied to compare the performances of different error correction codes we present results on the comparison of block error correct... | [['use', 'of', 'an', 'error', 'correction', 'code', 'in', 'a', 'given', 'transmission', 'channel', 'can', 'be', 'regarded', 'as', 'the', 'statistical', 'experiment', 'therefore', 'powerful', 'results', 'from', 'the', 'theory', 'of', 'comparison', 'of', 'experiments', 'can', 'be', 'applied', 'to', 'compare', 'the', 'per... | [-0.0980086334090194, -0.014952109121267036, -0.07270763909606182, 0.11619033690886167, 0.020577756025949898, -0.16728489300964966, 0.045891550953661944, 0.3763077852356693, -0.26754962665879206, -0.28452112952895137, 0.1613537348493043, -0.2698169596493244, -0.13631712180440841, 0.23939599485500998, -0.069004604609116... |
710.3818 | Improved Factorization Method in Studying B-meson Decays | B decays are a subject of active research since they provide useful
information on the dynamics of strong and electroweak interactions for testing
the Standard Model (SM) and models beyond and are ideally suited for a critical
analysis of CP violation phenomena. Within the standard model, there exist
certain relation... | hep-ph | b decays are a subject of active research since they provide useful information on the dynamics of strong and electroweak interactions for testing the standard model sm and models beyond and are ideally suited for a critical analysis of cp violation phenomena within the standard model there exist certain relations betw... | [['b', 'decays', 'are', 'a', 'subject', 'of', 'active', 'research', 'since', 'they', 'provide', 'useful', 'information', 'on', 'the', 'dynamics', 'of', 'strong', 'and', 'electroweak', 'interactions', 'for', 'testing', 'the', 'standard', 'model', 'sm', 'and', 'models', 'beyond', 'and', 'are', 'ideally', 'suited', 'for',... | [-0.08221449844476178, 0.18828254896058624, -0.06830349789650049, 0.10975247522555112, -0.07032342581978239, -0.17004061225297804, 0.12486806068488437, 0.3228594512017309, -0.227825495592152, -0.2607759596456004, 0.047797859564832984, -0.3204271970609212, -0.09032580888141757, 0.1535893302131894, 0.048689908809186035, ... |
710.3819 | B \to K^{*} \gamma Decay within MSSM | The paper deals with a next-to-leading order analysis of the radiative $B \to
K^* \gamma$ decay. Working in a PQCD approach, we compute the correction to the
essential form factor, coming from a single gluon exchange with the spectator.
We investigate the supersymmetry effects on the branching ratio and direct CP
asy... | hep-ph | the paper deals with a nexttoleading order analysis of the radiative b to k gamma decay working in a pqcd approach we compute the correction to the essential form factor coming from a single gluon exchange with the spectator we investigate the supersymmetry effects on the branching ratio and direct cp asymmetry and con... | [['the', 'paper', 'deals', 'with', 'a', 'nexttoleading', 'order', 'analysis', 'of', 'the', 'radiative', 'b', 'to', 'k', 'gamma', 'decay', 'working', 'in', 'a', 'pqcd', 'approach', 'we', 'compute', 'the', 'correction', 'to', 'the', 'essential', 'form', 'factor', 'coming', 'from', 'a', 'single', 'gluon', 'exchange', 'wit... | [-0.11702121869391954, 0.18463613935906825, -0.06896940650868005, 0.097766442569615, -0.08643424197838738, -0.08888344178056537, 0.08560038638373452, 0.2938635092357109, -0.24244924069478593, -0.25664451377915926, 0.011409079176293493, -0.2890628126875401, -0.005251561556461042, 0.07581584059215825, 0.08856436268201676... |
710.382 | A Brief Introduction to PYTHIA 8.1 | The PYTHIA program is a standard tool for the generation of high-energy
collisions, comprising a coherent set of physics models for the evolution from
a few-body hard process to a complex multihadronic final state. It contains a
library of hard processes and models for initial- and final-state parton
showers, multipl... | hep-ph | the pythia program is a standard tool for the generation of highenergy collisions comprising a coherent set of physics models for the evolution from a fewbody hard process to a complex multihadronic final state it contains a library of hard processes and models for initial and finalstate parton showers multiple partonp... | [['the', 'pythia', 'program', 'is', 'a', 'standard', 'tool', 'for', 'the', 'generation', 'of', 'highenergy', 'collisions', 'comprising', 'a', 'coherent', 'set', 'of', 'physics', 'models', 'for', 'the', 'evolution', 'from', 'a', 'fewbody', 'hard', 'process', 'to', 'a', 'complex', 'multihadronic', 'final', 'state', 'it',... | [-0.05313566179287563, 0.14113053825085375, -0.1266096533504528, 0.16341684407424656, -0.07789233776399482, -0.1424053096752756, -0.02480499683399436, 0.3728568449559558, -0.24304649093053268, -0.30298012941551417, 0.05180653737847274, -0.3119802610594993, -0.007782633899789275, 0.2017870501780399, 0.03522613855391627,... |
710.3821 | Torsion, Scalar Field and f(\mathcal{R}) Gravity | The role of torsion and a scalar field $\phi$ in gravitation in the
background of a particular class of the Riemann-Cartan geometry is considered
here. Some times ago, a Lagrangian density with Lagrange multipliers has been
proposed by the author which has been obtained by picking some particular terms
from the SO(4,... | astro-ph | the role of torsion and a scalar field phi in gravitation in the background of a particular class of the riemanncartan geometry is considered here some times ago a lagrangian density with lagrange multipliers has been proposed by the author which has been obtained by picking some particular terms from the so41 pontryag... | [['the', 'role', 'of', 'torsion', 'and', 'a', 'scalar', 'field', 'phi', 'in', 'gravitation', 'in', 'the', 'background', 'of', 'a', 'particular', 'class', 'of', 'the', 'riemanncartan', 'geometry', 'is', 'considered', 'here', 'some', 'times', 'ago', 'a', 'lagrangian', 'density', 'with', 'lagrange', 'multipliers', 'has', ... | [-0.19591524142103836, 0.1448798500062169, -0.14053858573669972, 0.03841856223551313, -0.12985455452909936, -0.11713436585243629, -0.09558487668653708, 0.2730771743328027, -0.2117401762339084, -0.2751044494221392, 0.05585406120846291, -0.23025896753305974, -0.17443262663791362, 0.10993380679384522, -0.04493776512048814... |
710.3822 | Explicit approximation of the sum of the reciprocal of the imaginary
parts of the zeta zeros | In this note, we give some explicit upper and lower bounds for the summation
$\sum_{0<\gamma\leq T}\frac{1}{\gamma}$, where $\gamma$ is the imaginary part
of nontrivial zeros $\rho=\beta+i\gamma$ of $\zeta(s)$.
| math.NT math.GM | in this note we give some explicit upper and lower bounds for the summation sum_0gammaleq tfrac1gamma where gamma is the imaginary part of nontrivial zeros rhobetaigamma of zetas | [['in', 'this', 'note', 'we', 'give', 'some', 'explicit', 'upper', 'and', 'lower', 'bounds', 'for', 'the', 'summation', 'sum_0gammaleq', 'tfrac1gamma', 'where', 'gamma', 'is', 'the', 'imaginary', 'part', 'of', 'nontrivial', 'zeros', 'rhobetaigamma', 'of', 'zetas']] | [-0.23010551370680332, 0.09862738694995642, -0.1362009503878653, 0.1128948526084423, -0.14494206665083767, -0.06780517190694808, 0.13019537821412086, 0.25903229251503945, -0.15458398818969726, -0.23957694366574286, 0.13413917161058633, -0.2816847146488726, -0.1771106257289648, 0.26228739961981773, 0.014844308122992516,... |
710.3823 | Eccentric binary black-hole mergers: The transition from inspiral to
plunge in general relativity | We study the transition from inspiral to plunge in general relativity by
computing gravitational waveforms of non-spinning, equal-mass black-hole
binaries. We consider three sequences of simulations, starting with a
quasi-circular inspiral completing 1.5, 2.3 and 9.6 orbits, respectively, prior
to coalescence of the ... | gr-qc astro-ph hep-th | we study the transition from inspiral to plunge in general relativity by computing gravitational waveforms of nonspinning equalmass blackhole binaries we consider three sequences of simulations starting with a quasicircular inspiral completing 15 23 and 96 orbits respectively prior to coalescence of the holes for each ... | [['we', 'study', 'the', 'transition', 'from', 'inspiral', 'to', 'plunge', 'in', 'general', 'relativity', 'by', 'computing', 'gravitational', 'waveforms', 'of', 'nonspinning', 'equalmass', 'blackhole', 'binaries', 'we', 'consider', 'three', 'sequences', 'of', 'simulations', 'starting', 'with', 'a', 'quasicircular', 'ins... | [-0.20576966582496026, 0.1873154806531066, -0.05641042687682714, 0.0900075645506571, -0.09067910756681852, -0.06393559089668346, -0.012011881029977944, 0.31192273564258777, -0.1444145175797082, -0.3226827933787085, 0.03130869631225846, -0.31344652586000193, -0.04000182829376598, 0.2237389439633701, -0.01169954654693171... |
710.3824 | Deterministic Secure Positioning in Wireless Sensor Networks | Properly locating sensor nodes is an important building block for a large
subset of wireless sensor networks (WSN) applications. As a result, the
performance of the WSN degrades significantly when misbehaving nodes report
false location and distance information in order to fake their actual location.
In this paper we... | cs.CR cs.DC cs.DS cs.NI | properly locating sensor nodes is an important building block for a large subset of wireless sensor networks wsn applications as a result the performance of the wsn degrades significantly when misbehaving nodes report false location and distance information in order to fake their actual location in this paper we propos... | [['properly', 'locating', 'sensor', 'nodes', 'is', 'an', 'important', 'building', 'block', 'for', 'a', 'large', 'subset', 'of', 'wireless', 'sensor', 'networks', 'wsn', 'applications', 'as', 'a', 'result', 'the', 'performance', 'of', 'the', 'wsn', 'degrades', 'significantly', 'when', 'misbehaving', 'nodes', 'report', '... | [-0.18532348004643556, 0.05402133759884133, -0.025699314880937206, -0.012703277094403534, -0.08520504209623717, -0.2403763673150318, 0.09769235067852411, 0.4033682414830772, -0.22259567831805602, -0.3179906576429087, 0.0920565096614679, -0.3173324274525502, -0.15106147855487714, 0.20092195763220141, -0.1587748732987189... |
710.3825 | Product and anti-Hermitian structures on the tangent space | Noting that the complete lift of a Rimannian metric defined on a
differentiable manifold is not 0-homogeneous on the fibers of the tangent
bundle . In this paper we introduce a new lift which is 0-homogeneous. It
determines on slit tangent bundle a pseudo-Riemannian metric, which depends
only on the metric . We study... | math.DG math-ph math.MP | noting that the complete lift of a rimannian metric defined on a differentiable manifold is not 0homogeneous on the fibers of the tangent bundle in this paper we introduce a new lift which is 0homogeneous it determines on slit tangent bundle a pseudoriemannian metric which depends only on the metric we study some of th... | [['noting', 'that', 'the', 'complete', 'lift', 'of', 'a', 'rimannian', 'metric', 'defined', 'on', 'a', 'differentiable', 'manifold', 'is', 'not', '0homogeneous', 'on', 'the', 'fibers', 'of', 'the', 'tangent', 'bundle', 'in', 'this', 'paper', 'we', 'introduce', 'a', 'new', 'lift', 'which', 'is', '0homogeneous', 'it', 'd... | [-0.17971725798478083, 0.04920323055315142, -0.09211367823272235, 0.051767900408733455, -0.16210608301861656, -0.08326700555958919, -0.024086561518266707, 0.3920647708166923, -0.30905527277805267, -0.18120617333001324, 0.08398209816438057, -0.21233888058174802, -0.2443606109646637, 0.1581541576555797, -0.14253958839080... |
710.3826 | R fluids | A theory of collisionless fluids is developed in a unified picture, where
nonrotating figures with anisotropic random velocity component distributions
and rotating figures with isotropic random velocity component distributions,
make adjoints configurations to the same system. R fluids are defined and mean
and rms ang... | astro-ph | a theory of collisionless fluids is developed in a unified picture where nonrotating figures with anisotropic random velocity component distributions and rotating figures with isotropic random velocity component distributions make adjoints configurations to the same system r fluids are defined and mean and rms angular ... | [['a', 'theory', 'of', 'collisionless', 'fluids', 'is', 'developed', 'in', 'a', 'unified', 'picture', 'where', 'nonrotating', 'figures', 'with', 'anisotropic', 'random', 'velocity', 'component', 'distributions', 'and', 'rotating', 'figures', 'with', 'isotropic', 'random', 'velocity', 'component', 'distributions', 'make... | [-0.15238361454066762, 0.16466400068071607, -0.09066482234516116, 0.028031680727124808, -0.09454630995151092, -0.06445219534180069, -0.019636370455600627, 0.3663870655291248, -0.2710954590993424, -0.32201523861294845, 0.025819539056101348, -0.23838721104107208, -0.021759985544122173, 0.1564581816601276, -0.023557106294... |
710.3827 | Topological Born-Infeld-dilaton black holes | We construct a new analytic solution of Einstein-Born-Infeld-dilaton theory
in the presence of Liouville-type potentials for the dilaton field. These
solutions describe dilaton black holes with nontrivial topology and nonlinear
electrodynamics. Black hole horizons and cosmological horizons in these
spacetimes, can be... | hep-th | we construct a new analytic solution of einsteinborninfelddilaton theory in the presence of liouvilletype potentials for the dilaton field these solutions describe dilaton black holes with nontrivial topology and nonlinear electrodynamics black hole horizons and cosmological horizons in these spacetimes can be a twodim... | [['we', 'construct', 'a', 'new', 'analytic', 'solution', 'of', 'einsteinborninfelddilaton', 'theory', 'in', 'the', 'presence', 'of', 'liouvilletype', 'potentials', 'for', 'the', 'dilaton', 'field', 'these', 'solutions', 'describe', 'dilaton', 'black', 'holes', 'with', 'nontrivial', 'topology', 'and', 'nonlinear', 'elec... | [-0.20444124421543058, 0.09050109960577067, -0.08732646378305028, 0.14903852141133564, -0.10330762585953754, -0.21737322015139987, -0.030776589589796084, 0.28211972187547124, -0.16194978711359642, -0.24358727602589436, 0.12521938192658127, -0.3610812306842383, -0.14458397968453082, 0.15937040745938086, -0.0375317542868... |
710.3828 | Masses and magnetic moments of heavy flavour baryons in hyper central
model | We employ the hyper central approach to study the masses and magnetic moments
of the baryons constituting single charm and beauty quark. The confinement
potential is assumed in the hyper central co-ordinates of the coulomb plus
power potential form.
| hep-ph | we employ the hyper central approach to study the masses and magnetic moments of the baryons constituting single charm and beauty quark the confinement potential is assumed in the hyper central coordinates of the coulomb plus power potential form | [['we', 'employ', 'the', 'hyper', 'central', 'approach', 'to', 'study', 'the', 'masses', 'and', 'magnetic', 'moments', 'of', 'the', 'baryons', 'constituting', 'single', 'charm', 'and', 'beauty', 'quark', 'the', 'confinement', 'potential', 'is', 'assumed', 'in', 'the', 'hyper', 'central', 'coordinates', 'of', 'the', 'co... | [-0.09033801048420943, 0.13702588826895523, -0.08762771987284605, 0.11619142576968536, -0.02494953594242151, -0.0703979339928199, 0.04857631925588999, 0.29872935313062793, -0.20336611385051256, -0.2958426446868823, -0.04667267803019152, -0.3273368732860455, -0.005342652424214742, 0.03811651888566139, 0.0716577841876409... |
710.3829 | Multi-scale Entanglement Renormalization Ansatz in Two Dimensions:
Quantum Ising Model | We propose a symmetric version of the multi-scale entanglement
renormalization Ansatz (MERA) in two spatial dimensions (2D) and use this
Ansatz to find an unknown ground state of a 2D quantum system. Results in the
simple 2D quantum Ising model on the $8\times8$ square lattice are found to be
very accurate even with ... | cond-mat.other cond-mat.mes-hall cond-mat.stat-mech cond-mat.str-el physics.comp-ph quant-ph | we propose a symmetric version of the multiscale entanglement renormalization ansatz mera in two spatial dimensions 2d and use this ansatz to find an unknown ground state of a 2d quantum system results in the simple 2d quantum ising model on the 8times8 square lattice are found to be very accurate even with the smalles... | [['we', 'propose', 'a', 'symmetric', 'version', 'of', 'the', 'multiscale', 'entanglement', 'renormalization', 'ansatz', 'mera', 'in', 'two', 'spatial', 'dimensions', '2d', 'and', 'use', 'this', 'ansatz', 'to', 'find', 'an', 'unknown', 'ground', 'state', 'of', 'a', '2d', 'quantum', 'system', 'results', 'in', 'the', 'sim... | [-0.12612459497076683, 0.1398214777986266, -0.06002326926280712, 0.04644238424350925, -0.028831822701312345, -0.204186644373012, -0.024460274653894633, 0.3705979295974148, -0.21518179510944876, -0.24432657078582923, 0.09124918325788117, -0.2409638827987786, -0.1767184929922223, 0.11999148544293411, 0.03529863754801195,... |
710.383 | Spin-Dependent Mass Enhancement under Magnetic Field in the Periodic
Anderson Model | In order to study the mechanism of the mass enhancement in heavy fermion
compounds in the presence of magnetic field, we study the periodic Anderson
model using the fluctuation exchange approximation. The resulting value of the
mass enhancement factor z^{-1} can become up to 10, which is significantly
larger than tha... | cond-mat.str-el | in order to study the mechanism of the mass enhancement in heavy fermion compounds in the presence of magnetic field we study the periodic anderson model using the fluctuation exchange approximation the resulting value of the mass enhancement factor z1 can become up to 10 which is significantly larger than that in the ... | [['in', 'order', 'to', 'study', 'the', 'mechanism', 'of', 'the', 'mass', 'enhancement', 'in', 'heavy', 'fermion', 'compounds', 'in', 'the', 'presence', 'of', 'magnetic', 'field', 'we', 'study', 'the', 'periodic', 'anderson', 'model', 'using', 'the', 'fluctuation', 'exchange', 'approximation', 'the', 'resulting', 'value... | [-0.13963763668434695, 0.22912814759183675, 0.011345899958784381, 0.07590029656615419, -0.003281996996762852, -0.09193920866431048, 0.08104110146135403, 0.32832042551599444, -0.21179067509559293, -0.32558199763298035, -0.03205781889652523, -0.33777082185260954, -0.08194138146936894, 0.19850909842255834, 0.0540175681778... |
710.3831 | A truth about Brownian motion in gases and in general | Real thermal motion of gas molecules, free electrons, etc., at long time
intervals (much greater than mean free-flight time) possesses, contrary to its
popular mathematical models, essentially non-Gaussian statistics. A simple
proof of this statement is suggested basing on only the determinism and
reversibility of mi... | cond-mat.stat-mech | real thermal motion of gas molecules free electrons etc at long time intervals much greater than mean freeflight time possesses contrary to its popular mathematical models essentially nongaussian statistics a simple proof of this statement is suggested basing on only the determinism and reversibility of microscopic dyn... | [['real', 'thermal', 'motion', 'of', 'gas', 'molecules', 'free', 'electrons', 'etc', 'at', 'long', 'time', 'intervals', 'much', 'greater', 'than', 'mean', 'freeflight', 'time', 'possesses', 'contrary', 'to', 'its', 'popular', 'mathematical', 'models', 'essentially', 'nongaussian', 'statistics', 'a', 'simple', 'proof', ... | [-0.10287281486389768, 0.1434221749584521, -0.16859042234418373, 0.11752515245649603, -0.05698235981887387, -0.14742100458862561, 0.06551819582349591, 0.34009177816070374, -0.24201046079096775, -0.25128897887864904, 0.04556624339743247, -0.24377502866780326, -0.058968895051117624, 0.18377672395135666, -0.03253991511319... |
710.3832 | Superfield Formulation of Nonlinear N=4 Supermultiplets | We propose a unified superfield formulation of N=4 off-shell supermultiplets
in one spacetime dimension using the standard N=4 superspace. The main idea of
our approach is a "gluing" together of two linear supermultiplets along their
fermions. The functions defining such a gluing obey a system of equations. Each
solu... | hep-th | we propose a unified superfield formulation of n4 offshell supermultiplets in one spacetime dimension using the standard n4 superspace the main idea of our approach is a gluing together of two linear supermultiplets along their fermions the functions defining such a gluing obey a system of equations each solution of th... | [['we', 'propose', 'a', 'unified', 'superfield', 'formulation', 'of', 'n4', 'offshell', 'supermultiplets', 'in', 'one', 'spacetime', 'dimension', 'using', 'the', 'standard', 'n4', 'superspace', 'the', 'main', 'idea', 'of', 'our', 'approach', 'is', 'a', 'gluing', 'together', 'of', 'two', 'linear', 'supermultiplets', 'al... | [-0.1586193364563879, 0.1333339147355758, -0.0631599800947767, 0.06545686177208324, -0.13554877845140603, -0.2086543317495303, -0.07863883895205927, 0.30557493869583685, -0.1904235325016818, -0.23209910563213731, 0.07147401315671811, -0.2830608795898465, -0.23616999069429936, 0.0879536733455997, -0.0660537723554196, 0.... |
710.3833 | A silence black hole: Hawking radiation at the Hagedorn temperature | We compute semi-classically the Hawking emission for different types of black
hole in type II string theory. In particular we analyze the thermal transition
between NS5 branes and Little String Theory, finding compelling evidence for
information recovering. We find that once the near horizon limit is taken the
emissi... | hep-th | we compute semiclassically the hawking emission for different types of black hole in type ii string theory in particular we analyze the thermal transition between ns5 branes and little string theory finding compelling evidence for information recovering we find that once the near horizon limit is taken the emission of ... | [['we', 'compute', 'semiclassically', 'the', 'hawking', 'emission', 'for', 'different', 'types', 'of', 'black', 'hole', 'in', 'type', 'ii', 'string', 'theory', 'in', 'particular', 'we', 'analyze', 'the', 'thermal', 'transition', 'between', 'ns5', 'branes', 'and', 'little', 'string', 'theory', 'finding', 'compelling', '... | [-0.11650107519623513, 0.14481549650965328, -0.10297077171573485, 0.18764851038684827, -0.08314144625156014, -0.16579533483902062, 0.01872058449144889, 0.3270315397358327, -0.19937591246518963, -0.28158066971270646, 0.08496603706993887, -0.32284090652872155, -0.12469934629000447, 0.14441383485164908, -0.046109106477901... |
710.3834 | Trace ideals for Fourier integral operators with non-smooth symbols II | We consider Fourier integral operators with symbols in modulation spaces and
non-smooth phase functions whose second orders of derivatives belong to certain
types of modulation space. We establish continuity and Schatten-von Neumann
properties of such operators when acting on modulation spaces.
| math.AP math.FA | we consider fourier integral operators with symbols in modulation spaces and nonsmooth phase functions whose second orders of derivatives belong to certain types of modulation space we establish continuity and schattenvon neumann properties of such operators when acting on modulation spaces | [['we', 'consider', 'fourier', 'integral', 'operators', 'with', 'symbols', 'in', 'modulation', 'spaces', 'and', 'nonsmooth', 'phase', 'functions', 'whose', 'second', 'orders', 'of', 'derivatives', 'belong', 'to', 'certain', 'types', 'of', 'modulation', 'space', 'we', 'establish', 'continuity', 'and', 'schattenvon', 'ne... | [-0.19490214805232314, 0.13352220396443112, -0.018445717397986387, 0.09962216324013907, -0.12908462545175742, -0.07306993316586424, -0.006480475759883298, 0.3843962988282395, -0.3461903666668549, -0.16033844995062527, 0.2002408637000793, -0.27360042200491924, -0.16425541715651024, 0.20577295815072408, -0.12336963237399... |
710.3835 | The lessons from the running of the tensor-to-scalar ratio | We derive a simple consistency relation from the running of the
tensor-to-scalar ratio. This new relation is first order in the slow-roll
approximation. While for single field models we can obtain what can be found by
using other observables, multi-field cases in general give non-trivial
contributions dependent on th... | astro-ph gr-qc hep-ph hep-th | we derive a simple consistency relation from the running of the tensortoscalar ratio this new relation is first order in the slowroll approximation while for single field models we can obtain what can be found by using other observables multifield cases in general give nontrivial contributions dependent on the geometry... | [['we', 'derive', 'a', 'simple', 'consistency', 'relation', 'from', 'the', 'running', 'of', 'the', 'tensortoscalar', 'ratio', 'this', 'new', 'relation', 'is', 'first', 'order', 'in', 'the', 'slowroll', 'approximation', 'while', 'for', 'single', 'field', 'models', 'we', 'can', 'obtain', 'what', 'can', 'be', 'found', 'by... | [-0.13886956226197072, 0.15128744039684533, -0.12408111898694188, 0.1106585668560001, -0.09510393707314506, -0.13903034759568983, -0.0005915036934311501, 0.3340135260950774, -0.23773283897608052, -0.35062711792998014, 0.07073395679763053, -0.1884458718355745, -0.13359088998986407, 0.21228532317327337, -0.00654320911271... |
710.3836 | Noncommutative real scalar field theory in 2+1 dimensions at finite
temperature | We study thermal effects for a noncommutative real scalar field in 2+1
dimensions including a Grosse-Wulkenhaar term. Using a perturbative expansion
for the free energy, we deduce some general properties of the corresponding
contributions, in the thermodynamic limit. We show that the model can be
consistently interpr... | hep-th | we study thermal effects for a noncommutative real scalar field in 21 dimensions including a grossewulkenhaar term using a perturbative expansion for the free energy we deduce some general properties of the corresponding contributions in the thermodynamic limit we show that the model can be consistently interpreted as ... | [['we', 'study', 'thermal', 'effects', 'for', 'a', 'noncommutative', 'real', 'scalar', 'field', 'in', '21', 'dimensions', 'including', 'a', 'grossewulkenhaar', 'term', 'using', 'a', 'perturbative', 'expansion', 'for', 'the', 'free', 'energy', 'we', 'deduce', 'some', 'general', 'properties', 'of', 'the', 'corresponding'... | [-0.11300879490912938, 0.16141921386421376, -0.10042249629670968, 0.12434266342163147, -0.0340542852130459, -0.04023133105689996, -0.00664900539473432, 0.27445478449178645, -0.2657533398539316, -0.25972911442217766, 0.10853181819462018, -0.23292021996906545, -0.13879474380710086, 0.19325774390113037, -0.028366514504505... |
710.3837 | Potential for regulatory genetic networks of gene expression near a
stable point | A description for regulatory genetic network based on generalized potential
energy is constructed. The potential energy is derived from the steady state
solution of linearized Fokker-Plank equation, and the result is shown to be
equivalent to the system of coupled oscillators. The correspondence between the
quantitie... | physics.bio-ph q-bio.MN | a description for regulatory genetic network based on generalized potential energy is constructed the potential energy is derived from the steady state solution of linearized fokkerplank equation and the result is shown to be equivalent to the system of coupled oscillators the correspondence between the quantities from... | [['a', 'description', 'for', 'regulatory', 'genetic', 'network', 'based', 'on', 'generalized', 'potential', 'energy', 'is', 'constructed', 'the', 'potential', 'energy', 'is', 'derived', 'from', 'the', 'steady', 'state', 'solution', 'of', 'linearized', 'fokkerplank', 'equation', 'and', 'the', 'result', 'is', 'shown', 't... | [-0.13244704247743902, 0.10068012538548803, -0.07442257340962642, 0.07088636503572289, -0.03125025017326263, -0.15489943192784336, 0.001380345096515718, 0.29282142981782416, -0.29311535981370607, -0.26015587420437797, 0.048569006674540026, -0.295707415750198, -0.16854852989150612, 0.200195449656833, -0.0021527874409699... |
710.3838 | Momentum and excitation energy dependence of the "waterfalls" in
cuprates | Using high-resolution angle-resolved photoemission spectroscopy we have
studied the momentum and photon energy dependence of the anomalous high-energy
dispersion, termed "waterfalls", between the Fermi level and 1 eV binding
energy in several high-Tc superconductors. We observe strong changes of the
dispersion betwee... | cond-mat.supr-con cond-mat.str-el | using highresolution angleresolved photoemission spectroscopy we have studied the momentum and photon energy dependence of the anomalous highenergy dispersion termed waterfalls between the fermi level and 1 ev binding energy in several hightc superconductors we observe strong changes of the dispersion between different... | [['using', 'highresolution', 'angleresolved', 'photoemission', 'spectroscopy', 'we', 'have', 'studied', 'the', 'momentum', 'and', 'photon', 'energy', 'dependence', 'of', 'the', 'anomalous', 'highenergy', 'dispersion', 'termed', 'waterfalls', 'between', 'the', 'fermi', 'level', 'and', '1', 'ev', 'binding', 'energy', 'in... | [-0.11830576736974763, 0.1710565167460345, -0.09823929690901423, 0.09937220468418673, -0.04864197064307518, -0.07609495610631711, 0.11083920257442514, 0.40899148400785634, -0.28788733936380595, -0.3253008806177604, -0.05034145490753872, -0.36549706051300745, -0.08178385351584438, 0.1820795618914417, 0.04219767861468426... |
710.3839 | Dissipative dynamics of the semiconductor-cavity QED with q-deformed
bosons in the dispersive approximation | In this paper we give fully analytical description of the dynamics of a
collection of $N$-Frenkel excitons in high density regime dispersively coupled
to a single mode cavity field, in the presence of both exciton and cavity-field
dissipations. By using excitonic operators as q-deformed bosonic operators for
the syst... | quant-ph | in this paper we give fully analytical description of the dynamics of a collection of nfrenkel excitons in high density regime dispersively coupled to a single mode cavity field in the presence of both exciton and cavityfield dissipations by using excitonic operators as qdeformed bosonic operators for the system we sol... | [['in', 'this', 'paper', 'we', 'give', 'fully', 'analytical', 'description', 'of', 'the', 'dynamics', 'of', 'a', 'collection', 'of', 'nfrenkel', 'excitons', 'in', 'high', 'density', 'regime', 'dispersively', 'coupled', 'to', 'a', 'single', 'mode', 'cavity', 'field', 'in', 'the', 'presence', 'of', 'both', 'exciton', 'an... | [-0.1684723297437427, 0.17299382124364263, -0.0571991372659492, 0.022819893994672, -0.0004234249865862005, -0.10570565809823827, 0.03340175511248438, 0.3117570730532999, -0.25152583168043446, -0.2684107268666566, 0.033127400598128916, -0.2828498985080373, -0.13274344488639722, 0.18780804405722654, 0.03901525413631603, ... |
710.384 | Challenge on Ca-48 enrichment for CANDLES double beta decay experiment | Chemical isotope effects of calcium were studied by liquid-liquid extraction
using a crown ether of dicyclohexano-18-crown-6 for the purpose of finding a
cost-effective and efficient way of enrichment of Ca-48 towards the study of
the neutrinoless double beta decay of Ca-48. We evaluated each contribution
ratio of th... | nucl-ex | chemical isotope effects of calcium were studied by liquidliquid extraction using a crown ether of dicyclohexano18crown6 for the purpose of finding a costeffective and efficient way of enrichment of ca48 towards the study of the neutrinoless double beta decay of ca48 we evaluated each contribution ratio of the field sh... | [['chemical', 'isotope', 'effects', 'of', 'calcium', 'were', 'studied', 'by', 'liquidliquid', 'extraction', 'using', 'a', 'crown', 'ether', 'of', 'dicyclohexano18crown6', 'for', 'the', 'purpose', 'of', 'finding', 'a', 'costeffective', 'and', 'efficient', 'way', 'of', 'enrichment', 'of', 'ca48', 'towards', 'the', 'study... | [-0.0781509392739584, 0.18662738790153527, -0.02547328672371805, 0.03749048546839428, 0.001518067013239488, -0.0781428046990186, 0.08203673982255472, 0.3605745844232539, -0.21600585452979432, -0.2905956177972257, 0.0183296720701037, -0.2621491583064198, -0.08573825028336918, 0.17928440077230334, 0.042108580719498905, -... |
710.3841 | Gravitational and Inertial Mass of Casimir Energy | It has been demonstrated, using variational methods, that quantum vacuum
energy gravitates according to the equivalence principle, at least for the
finite Casimir energies associated with perfectly conducting parallel plates.
This conclusion holds independently of the orientation of the plates. We review
these argume... | hep-th gr-qc quant-ph | it has been demonstrated using variational methods that quantum vacuum energy gravitates according to the equivalence principle at least for the finite casimir energies associated with perfectly conducting parallel plates this conclusion holds independently of the orientation of the plates we review these arguments and... | [['it', 'has', 'been', 'demonstrated', 'using', 'variational', 'methods', 'that', 'quantum', 'vacuum', 'energy', 'gravitates', 'according', 'to', 'the', 'equivalence', 'principle', 'at', 'least', 'for', 'the', 'finite', 'casimir', 'energies', 'associated', 'with', 'perfectly', 'conducting', 'parallel', 'plates', 'this'... | [-0.1745951771660475, 0.15202662790194155, -0.08659775874926709, 0.0233990891079884, -0.04436220112955198, -0.12657180279027672, -0.008751371875405312, 0.3468842156045139, -0.21435795770958066, -0.28717678526882084, 0.033362371465773324, -0.2594314557593316, -0.07002434456138872, 0.18148562845075503, -0.013306528214598... |
710.3842 | Global Existence Theorem for the Solutions of 3d Navier-Stokes System on
T3 for small initial data from the space P(a) | We consider 3d Navier-Stokes system with periodic boundary conditions for
small initial data from the space of Pseudomeasures. We provide asymptotic
behavior for the coefficients in the perturbation series for the solution of
this system.
| math.AP math-ph math.MP | we consider 3d navierstokes system with periodic boundary conditions for small initial data from the space of pseudomeasures we provide asymptotic behavior for the coefficients in the perturbation series for the solution of this system | [['we', 'consider', '3d', 'navierstokes', 'system', 'with', 'periodic', 'boundary', 'conditions', 'for', 'small', 'initial', 'data', 'from', 'the', 'space', 'of', 'pseudomeasures', 'we', 'provide', 'asymptotic', 'behavior', 'for', 'the', 'coefficients', 'in', 'the', 'perturbation', 'series', 'for', 'the', 'solution', '... | [-0.19930309200925486, 0.01897714664893491, -0.10399883165955544, 0.012708502033326243, -0.01385624909640423, -0.08293258954903909, -0.012657177641189524, 0.292480389082006, -0.2776902083839689, -0.2323137794754335, 0.20334019276113915, -0.2687332872567432, -0.12123603959168706, 0.19505503113780703, -0.0553157438124929... |
710.3843 | H and A Discrimination using Linear Polarization of Photons at the PLC | First realistic estimate of the usefulness of the Photon Linear Collider with
linearly polarized photons as analyzer of the CP-parity of Higgs bosons is
presented. MSSM Higgs bosons H and A with 300 GeV mass, for the model
parameters corresponding to the so called "LHC wedge" region, are considered.
When switching fr... | hep-ph | first realistic estimate of the usefulness of the photon linear collider with linearly polarized photons as analyzer of the cpparity of higgs bosons is presented mssm higgs bosons h and a with 300 gev mass for the model parameters corresponding to the so called lhc wedge region are considered when switching from circul... | [['first', 'realistic', 'estimate', 'of', 'the', 'usefulness', 'of', 'the', 'photon', 'linear', 'collider', 'with', 'linearly', 'polarized', 'photons', 'as', 'analyzer', 'of', 'the', 'cpparity', 'of', 'higgs', 'bosons', 'is', 'presented', 'mssm', 'higgs', 'bosons', 'h', 'and', 'a', 'with', '300', 'gev', 'mass', 'for', ... | [-0.0634750296594575, 0.3238925962788543, -0.024857141449230544, 0.12310233680233196, -0.060794120221480466, -0.2103042121151495, 0.00797393910276393, 0.33687986690028193, -0.19943935419187733, -0.28197935277906555, -0.013198060255187253, -0.31061885629274083, 0.05773285086207468, 0.16384024040164882, 0.085746442553691... |
710.3844 | A new class of examples of group-valued moment maps | The purpose of this paper is to construct new examples of group-valued moment
maps. As the main tool for construction of such examples we use
quasi-symplectic implosion which was introduced in [HJS06]. More precisely we
show that there are certain strata of $D{\bf Sp}(n)_{\rm impl}$, the universal
imploded space, whe... | math.SG | the purpose of this paper is to construct new examples of groupvalued moment maps as the main tool for construction of such examples we use quasisymplectic implosion which was introduced in hjs06 more precisely we show that there are certain strata of dbf spn_rm impl the universal imploded space where it is singular bu... | [['the', 'purpose', 'of', 'this', 'paper', 'is', 'to', 'construct', 'new', 'examples', 'of', 'groupvalued', 'moment', 'maps', 'as', 'the', 'main', 'tool', 'for', 'construction', 'of', 'such', 'examples', 'we', 'use', 'quasisymplectic', 'implosion', 'which', 'was', 'introduced', 'in', 'hjs06', 'more', 'precisely', 'we',... | [-0.123145968595054, 0.11835949724510071, -0.06514407006362753, 0.07985856956727203, -0.0875305147215371, -0.10001389583903214, -0.04369560058224916, 0.353123449029461, -0.25523260650375196, -0.21272885239675582, 0.12409296232808922, -0.19150859403664305, -0.2440181085539441, 0.22845537822333076, -0.13961772405872902, ... |
710.3845 | Symmetry properties of Penrose type tilings | The Penrose tiling is directly related to the atomic structure of certain
decagonal quasicrystals and, despite its aperiodicity, is highly symmetric. It
is known that the numbers 1, $-\tau $, $(-\tau)^2$, $(-\tau)^3$, ..., where
$\tau =(1+\sqrt{5})/2$, are scaling factors of the Penrose tiling. We show that
the set o... | math-ph cond-mat.mtrl-sci math.MP | the penrose tiling is directly related to the atomic structure of certain decagonal quasicrystals and despite its aperiodicity is highly symmetric it is known that the numbers 1 tau tau2 tau3 where tau 1sqrt52 are scaling factors of the penrose tiling we show that the set of scaling factors is much larger and for most ... | [['the', 'penrose', 'tiling', 'is', 'directly', 'related', 'to', 'the', 'atomic', 'structure', 'of', 'certain', 'decagonal', 'quasicrystals', 'and', 'despite', 'its', 'aperiodicity', 'is', 'highly', 'symmetric', 'it', 'is', 'known', 'that', 'the', 'numbers', '1', 'tau', 'tau2', 'tau3', 'where', 'tau', '1sqrt52', 'are',... | [-0.1338402499465949, 0.21392326763033812, -0.05021674848147527, 0.11027975808158799, -0.08056555792802211, -0.10663864477255354, 0.01511809229850769, 0.33305367172667477, -0.30515863342302374, -0.24607798220081764, 0.13827547480380445, -0.3037222503599795, -0.1585928341056305, 0.18112634573922012, -0.01517269672882376... |
710.3846 | Cells and Constructible Representations in type B | We examine the partition of a finite Coxeter group of type $B$ into cells
determined by a weight function $L$. The main objective of these notes is to
reconcile Lusztig's description of constructible representations in this
setting with conjectured combinatorial descriptions of cells.
| math.RT math.CO | we examine the partition of a finite coxeter group of type b into cells determined by a weight function l the main objective of these notes is to reconcile lusztigs description of constructible representations in this setting with conjectured combinatorial descriptions of cells | [['we', 'examine', 'the', 'partition', 'of', 'a', 'finite', 'coxeter', 'group', 'of', 'type', 'b', 'into', 'cells', 'determined', 'by', 'a', 'weight', 'function', 'l', 'the', 'main', 'objective', 'of', 'these', 'notes', 'is', 'to', 'reconcile', 'lusztigs', 'description', 'of', 'constructible', 'representations', 'in', ... | [-0.13815506751280884, 0.09972395118174338, -0.10009078477877517, 0.06307142236551573, -0.08651326016284698, -0.12581627727161313, 0.07107426252129466, 0.30368769688661706, -0.32340131493198665, -0.2370801824469899, 0.0019211272768632963, -0.20202751708931702, -0.16687773774529613, 0.12280486545763737, -0.1906233616606... |
710.3847 | Coherent transfer of light polarization to electron spins in a
semiconductor | We demonstrate that the superposition of light polarization states is
coherently transferred to electron spins in a semiconductor quantum well. By
using time-resolved Kerr rotation we observe the initial phase of Larmor
precession of electron spins whose coherence is transferred from light. To
break the electron-hole... | quant-ph | we demonstrate that the superposition of light polarization states is coherently transferred to electron spins in a semiconductor quantum well by using timeresolved kerr rotation we observe the initial phase of larmor precession of electron spins whose coherence is transferred from light to break the electronhole spin ... | [['we', 'demonstrate', 'that', 'the', 'superposition', 'of', 'light', 'polarization', 'states', 'is', 'coherently', 'transferred', 'to', 'electron', 'spins', 'in', 'a', 'semiconductor', 'quantum', 'well', 'by', 'using', 'timeresolved', 'kerr', 'rotation', 'we', 'observe', 'the', 'initial', 'phase', 'of', 'larmor', 'pre... | [-0.13265079276703567, 0.3022323427497443, -0.046129151925596086, 0.0746300122111542, 0.011447130309709584, -0.19395349938871273, 0.05690662242354354, 0.4201231855697122, -0.26157241637807294, -0.30479084441707616, -0.08163597298707499, -0.343638530562082, 0.006246821191835116, 0.24100299904414688, 0.003655299779970243... |
710.3848 | Andreev reflection and Klein tunneling in graphene | This is a colloquium-style introduction to two electronic processes in a
carbon monolayer (graphene), each having an analogue in relativistic quantum
mechanics. Both processes couple electron-like and hole-like states, through
the action of either a superconducting pair potential or an electrostatic
potential. The fi... | cond-mat.mes-hall | this is a colloquiumstyle introduction to two electronic processes in a carbon monolayer graphene each having an analogue in relativistic quantum mechanics both processes couple electronlike and holelike states through the action of either a superconducting pair potential or an electrostatic potential the first process... | [['this', 'is', 'a', 'colloquiumstyle', 'introduction', 'to', 'two', 'electronic', 'processes', 'in', 'a', 'carbon', 'monolayer', 'graphene', 'each', 'having', 'an', 'analogue', 'in', 'relativistic', 'quantum', 'mechanics', 'both', 'processes', 'couple', 'electronlike', 'and', 'holelike', 'states', 'through', 'the', 'a... | [-0.2430035715845103, 0.1522473256245333, -0.05758583258488215, 0.032607669809488773, -0.0970809577902158, -0.26855187898501753, 0.09732411159202456, 0.35503436697646973, -0.24780558158953986, -0.26420591976493596, -0.09613335596164689, -0.33338933750366173, -0.13327847133080165, 0.1682366484000037, 0.01999637843109667... |
710.3849 | Fractal Analysis of Discharge Current Fluctuations | We use the multifractal detrended fluctuation analysis (MF-DFA) to study the
electrical discharge current fluctuations in plasma and show that it has
multifractal properties and behaves as a weak anti-correlated process.
Comparison of the MF-DFA results for the original series with those for the
shuffled and surrogat... | cond-mat.stat-mech | we use the multifractal detrended fluctuation analysis mfdfa to study the electrical discharge current fluctuations in plasma and show that it has multifractal properties and behaves as a weak anticorrelated process comparison of the mfdfa results for the original series with those for the shuffled and surrogate series... | [['we', 'use', 'the', 'multifractal', 'detrended', 'fluctuation', 'analysis', 'mfdfa', 'to', 'study', 'the', 'electrical', 'discharge', 'current', 'fluctuations', 'in', 'plasma', 'and', 'show', 'that', 'it', 'has', 'multifractal', 'properties', 'and', 'behaves', 'as', 'a', 'weak', 'anticorrelated', 'process', 'comparis... | [-0.08521847009615158, 0.11457403162057744, -0.17237136535550235, 0.13475671155097757, 0.03526653106473532, -0.08700977745320415, 0.0016307103214785457, 0.3480869801423978, -0.27006405871361494, -0.2279121415776899, 0.0872712777909328, -0.3899506028392352, -0.17428524009301327, 0.24841957091121003, 0.02105332193605136,... |
710.385 | Detection of Acetylene toward Cepheus A East with Spitzer | The first map of interstellar acetylene (C2H2) has been obtained with the
infrared spectrograph onboard the Spitzer Space Telescope. A spectral line map
of the $\nu_5$ vibration-rotation band at 13.7 microns carried out toward the
star-forming region Cepheus A East, shows that the C2H2 emission peaks in a few
localiz... | astro-ph | the first map of interstellar acetylene c2h2 has been obtained with the infrared spectrograph onboard the spitzer space telescope a spectral line map of the nu_5 vibrationrotation band at 137 microns carried out toward the starforming region cepheus a east shows that the c2h2 emission peaks in a few localized clumps wh... | [['the', 'first', 'map', 'of', 'interstellar', 'acetylene', 'c2h2', 'has', 'been', 'obtained', 'with', 'the', 'infrared', 'spectrograph', 'onboard', 'the', 'spitzer', 'space', 'telescope', 'a', 'spectral', 'line', 'map', 'of', 'the', 'nu_5', 'vibrationrotation', 'band', 'at', '137', 'microns', 'carried', 'out', 'toward... | [-0.044015469164393535, 0.14094355191086327, 0.011466096344196961, -0.014852592731929487, 0.023791909047092, -0.07199728393202855, 0.04872802365053859, 0.4547514293420439, -0.18809631706875127, -0.34134107417743914, 0.042261006881017235, -0.30315761896134874, 0.03925975697735946, 0.12834210832887846, 0.0296801572403637... |
710.3851 | A(4) Symmetry and Neutrinos | I recount briefly the history of neutrino tribimaximal mixing and the use of
the discrete family symmetry A(4) in obtaining it.
| hep-ph | i recount briefly the history of neutrino tribimaximal mixing and the use of the discrete family symmetry a4 in obtaining it | [['i', 'recount', 'briefly', 'the', 'history', 'of', 'neutrino', 'tribimaximal', 'mixing', 'and', 'the', 'use', 'of', 'the', 'discrete', 'family', 'symmetry', 'a4', 'in', 'obtaining', 'it']] | [-0.06495992351500761, 0.2292767424313795, 0.0036402581525700434, 0.15957187302410603, -0.120572268253281, -0.12397523987151328, 0.03250240729678245, 0.34375305970509845, -0.28989933821417035, -0.23824128552916504, 0.14889682866522067, -0.23372229170941172, -0.14107812036361014, 0.06921603969697442, 0.00057814864530449... |
710.3852 | Quantum Antiferromagnetism of Fermions in Optical Lattices with
Half-filled p-band | We study Fermi gases in a three-dimensional optical lattice with five
fermions per site, i.e. the s-band is completely filled and the p-band with
three-fold degeneracy is half filled. We show that, for repulsive interaction
between fermions, the system will exhibit spin-3/2 antiferromagnetic order at
low temperature.... | cond-mat.str-el cond-mat.supr-con | we study fermi gases in a threedimensional optical lattice with five fermions per site ie the sband is completely filled and the pband with threefold degeneracy is half filled we show that for repulsive interaction between fermions the system will exhibit spin32 antiferromagnetic order at low temperature this conclusio... | [['we', 'study', 'fermi', 'gases', 'in', 'a', 'threedimensional', 'optical', 'lattice', 'with', 'five', 'fermions', 'per', 'site', 'ie', 'the', 'sband', 'is', 'completely', 'filled', 'and', 'the', 'pband', 'with', 'threefold', 'degeneracy', 'is', 'half', 'filled', 'we', 'show', 'that', 'for', 'repulsive', 'interaction'... | [-0.18645586785733184, 0.2543309777840569, 0.005476005179729282, 0.048844102726067505, -0.00226790233546508, -0.19404003965597943, 0.06924140515459404, 0.38296537823630733, -0.2069026705918505, -0.26020946262106925, 0.00885734917838596, -0.37820502937215716, -0.09704836281094731, 0.13314070086730564, 0.0873565174680312... |
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