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2024-08-12T18:16:26.644295 | 2007-04-06T16:53:31 | 0704.0903 | {
"authors": "Elio Conte, Andrei Yu. Khrennikov, Joseph P. Zbilut",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:903",
"submitter": "Joseph P. Zbilut",
"url": "https://arxiv.org/abs/0704.0903"
} | arxiv-abstracts | For the first time we apply the methodologies of nonlinear analysis to
investigate atomic matter. We use these methods in the analysis of Atomic
Weights and of Mass Number of atomic nuclei. Using the AutoCorrelation Function
and Mutual Information we establish the presence of nonlinear effects in the
mechanism of increasing mass of atomic nuclei considered as a function of the
atomic number. We find that increasing mass is divergent, possibly chaotic. We
also investigate the possible existence of a Power Law for atomic nuclei and,
using also the technique of the variogram, we conclude that a fractal regime
could superintend to the mechanism of increasing mass for nuclei. Finally,
using the Hurst exponent, evidence is obtained that the mechanism of increasing
mass in atomic nuclei is in the fractional Brownian regime. The most
interesting results are obtained by using Recurrence Quantification Analysis
(RQA). New recurrences, psudoperiodicities, self-resemblance and class of
self-similarities are identified with values of determinism showing oscillating
values indicating the presence of more or less stability during the process of
increasing mass of atomic nuclei. In brief, new regimes of regularities are
identified for atomic nuclei that deserve to be studied by future researches.
In particular an accurate analysis of binding energy values by nonlinear
methods is further required.
|
2024-08-12T18:16:26.644374 | 2007-04-06T16:49:01 | 0704.0904 | {
"authors": "Robin Corbet, Richard Dubois",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:904",
"submitter": "Robin Corbet",
"url": "https://arxiv.org/abs/0704.0904"
} | arxiv-abstracts | The light curves produced by all-sky monitors, such as the Rossi X-ray Timing
Explorer All-Sky Monitor and the Swift Burst Alert Telescope (BAT), generally
have non-uniform error bars. In searching for periodic modulation in this type
of data using power spectra it can be important to use appropriate weighting of
data points to achieve the best sensitivity. It was recently demonstrated that
for Swift BAT data a simple weighting scheme can actually sometimes reduce the
sensitivity of the power spectrum depending on source brightness. Instead, a
modified weighting scheme, based on the Cochran semi-weighted mean, gives
improved results independent of source brightness. We investigate the benefits
of weighting power spectra in period searches using simulated GLAST LAT
observations of gamma-ray binaries.
|
2024-08-12T18:16:26.644435 | 2007-04-06T17:53:35 | 0704.0905 | {
"authors": "D. V. Luki\\'c, M. Schnell, D. W. Savin, C. Brandau, E. W. Schmidt, S.\n B\\\"ohm, A. M\\\"uller, S. Schippers, M. Lestinsky, F. Sprenger, A. Wolf, Z.\n Altun, N. R. Badnell",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:905",
"submitter": "Dragan Lukic",
"url": "https://arxiv.org/abs/0704.0905"
} | arxiv-abstracts | We have measured resonance strengths and energies for dielectronic
recombination (DR) of Mg-like Fe XV forming Al-like Fe XIV via N=3 -> N' = 3
core excitations in the electron-ion collision energy range 0-45 eV. All
measurements were carried out using the heavy-ion Test Storage Ring at the Max
Planck Institute for Nuclear Physics in Heidelberg, Germany. We have also
carried out new multiconfiguration Breit-Pauli (MCBP) calculations using the
AUTOSTRUCTURE code. For electron-ion collision energies < 25 eV we find poor
agreement between our experimental and theoretical resonance energies and
strengths. From 25 to 42 eV we find good agreement between the two for
resonance energies. But in this energy range the theoretical resonance
strengths are ~ 31% larger than the experimental results. This is larger than
our estimated total experimental uncertainty in this energy range of +/- 26%
(at a 90% confidence level). Above 42 eV the difference in the shape between
the calculated and measured 3s3p(^1P_1)nl DR series limit we attribute partly
to the nl dependence of the detection probabilities of high Rydberg states in
the experiment. We have used our measurements, supplemented by our
AUTOSTRUCTURE calculations, to produce a Maxwellian-averaged 3 -> 3 DR rate
coefficient for Fe XV forming Fe XIV. The resulting rate coefficient is
estimated to be accurate to better than +/- 29% (at a 90% confidence level) for
k_BT_e > 1 eV. At temperatures of k_BT_e ~ 2.5-15 eV, where Fe XV is predicted
to form in photoionized plasmas, significant discrepancies are found between
our experimentally-derived rate coefficient and previously published
theoretical results. Our new MCBP plasma rate coefficient is 19-28% smaller
than our experimental results over this temperature range.
|
2024-08-12T18:16:26.644553 | 2007-04-06T17:06:39 | 0704.0906 | {
"authors": "Bassetti Federico, Leisen Fabrizio",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:906",
"submitter": "Federico Bassetti",
"url": "https://arxiv.org/abs/0704.0906"
} | arxiv-abstracts | In this paper we study the Metropolis algorithm in connection with two
mean--field spin systems, the so called mean--field Ising model and the
Blume--Emery--Griffiths model. In both this examples the naive choice of
proposal chain gives rise, for some parameters, to a slowly mixing Metropolis
chain, that is a chain whose spectral gap decreases exponentially fast (in the
dimension $N$ of the problem). Here we show how a slight variant in the
proposal chain can avoid this problem, keeping the mean computational cost
similar to the cost of the usual Metropolis. More precisely we prove that, with
a suitable variant in the proposal, the Metropolis chain has a spectral gap
which decreases polynomially in 1/N. Using some symmetry structure of the
energy, the method rests on allowing appropriate jumps within the energy level
of the starting state.
|
2024-08-12T18:16:26.644630 | 2007-04-06T17:08:06 | 0704.0907 | {
"authors": "Eva Zakka-Bajjani (SPEC), Julien Segala (SPEC), Fabien Portier (SPEC),\n Patrice Roche (SPEC), Christian Glattli (SPEC), Antonella Cavanna (LPN), Yong\n Jin (LPN)",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:907",
"submitter": "Fabien Portier",
"url": "https://arxiv.org/abs/0704.0907"
} | arxiv-abstracts | We report on direct measurements of the electronic shot noise of a quantum
point contact at frequencies nu in the range 4-8 GHz. The very small energy
scale used ensures energy independent transmissions of the few transmitted
electronic modes and their accurate knowledge. Both the thermal energy and the
quantum point contact drain-source voltage Vds are comparable to the photon
energy hnu leading to observation of the shot noise suppression when
$V_{ds}<h\nu/e$. Our measurements provide the first complete test of the finite
frequency shot noise scattering theory without adjustable parameters.
|
2024-08-12T18:16:26.644683 | 2007-04-06T17:41:59 | 0704.0908 | {
"authors": "Lawrence Rudnick, Shea Brown, and Liliya R. Williams",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:908",
"submitter": "Lawrence Rudnick",
"url": "https://arxiv.org/abs/0704.0908"
} | arxiv-abstracts | We detect a dip of 20-45% in the surface brightness and number counts of NVSS
sources smoothed to a few degrees at the location of the WMAP cold spot. The
dip has structure on scales of approximately 1-10 degrees. Together with
independent all-sky wavelet analyses, our results suggest that the dip in
extragalactic brightness and number counts and the WMAP cold spot are
physically related, i.e., that the coincidence is neither a statistical anomaly
nor a WMAP foreground correction problem. If the cold spot does originate from
structures at modest redshifts, as we suggest, then there is no remaining need
for non-Gaussian processes at the last scattering surface of the CMB to explain
the cold spot. The late integrated Sachs-Wolfe effect, already seen
statistically for NVSS source counts, can now be seen to operate on a single
region. To create the magnitude and angular size of the WMAP cold spot requires
a ~140 Mpc radius completely empty void at z<=1 along this line of sight. This
is far outside the current expectations of the concordance cosmology, and adds
to the anomalies seen in the CMB.
|
2024-08-12T18:16:26.644767 | 2007-04-06T17:32:50 | 0704.0909 | {
"authors": "Sara Azzali",
"full_text_license": "arXiv.org - Non-exclusive license to distribute - http://arxiv.org/licenses/nonexclusive-distrib/1.0/",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:909",
"submitter": "Sara Azzali",
"url": "https://arxiv.org/abs/0704.0909"
} | arxiv-abstracts | We define the secondary invariants L^2- eta and -rho forms for families of
generalized Dirac operators on normal coverings of fibre bundles. On the
covering family we assume transversally smooth spectral projections, and
Novikov--Shubin invariants bigger than 3(dim B+1) to treat the large time
asymptotic for general operators. In the particular case of a bundle of spin
manifolds, we study the L^2- rho class in relation to the space of positive
scalar curvature vertical metrics.
|
2024-08-12T18:16:26.644820 | 2007-04-06T18:07:01 | 0704.0910 | {
"authors": "Efton Park and Jody Trout",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:910",
"submitter": "Jody Trout",
"url": "https://arxiv.org/abs/0704.0910"
} | arxiv-abstracts | An n-homomorphism between algebras is a linear map $\phi : A \to B$ such that
$\phi(a_1 ... a_n) = \phi(a_1)... \phi(a_n)$ for all elements $a_1, >..., a_n
\in A.$ Every homomorphism is an n-homomorphism, for all n >= 2, but the
converse is false, in general. Hejazian et al. [7] ask: Is every *-preserving
n-homomorphism between C*-algebras continuous? We answer their question in the
affirmative, but the even and odd n arguments are surprisingly disjoint. We
then use these results to prove stronger ones: If n >2 is even, then $\phi$ is
just an ordinary *-homomorphism. If n >= 3 is odd, then $\phi$ is a difference
of two orthogonal *-homomorphisms. Thus, there are no nontrivial *-linear
n-homomorphisms between C*-algebras.
|
2024-08-12T18:16:26.644879 | 2007-04-06T17:43:02 | 0704.0911 | {
"authors": "Debra Meloy Elmegreen (1), Bruce G. Elmegreen (2), Thomas Ferguson\n (1), Brendan Mullan (1,3) ((1) Vassar College, (2) IBM T.J. Watson Research\n Center, (3) Colgate University)",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:911",
"submitter": "Bruce Elmegreen",
"url": "https://arxiv.org/abs/0704.0911"
} | arxiv-abstracts | GEMS and GOODS fields were examined to z~1.4 for galaxy interactions and
mergers. The basic morphologies are familiar: antennae with long tidal tails,
tidal dwarfs, and merged cores; M51-type galaxies with disk spirals and tidal
arm companions; early-type galaxies with diffuse plumes; equal-mass
grazing-collisions; and thick J-shaped tails beaded with star formation and
double cores. One type is not common locally and is apparently a loose
assemblage of smaller galaxies. Photometric measurements were made of the tails
and clumps, and physical sizes were determined assuming photometric redshifts.
Antennae tails are a factor of ~3 smaller in GEMS and GOODS systems compared to
local antennae; their disks are a factor of ~2 smaller than locally. Collisions
among early type galaxies generally show no fine structure in their tails,
indicating that stellar debris is usually not unstable. One exception has a
5x10**9 Msun smooth red clump that could be a pure stellar condensation. Most
tidal dwarfs are blue and probably form by gravitational instabilities in the
gas. One tidal dwarf looks like it existed previously and was incorporated into
the arm tip by tidal forces. The star-forming regions in tidal arms are 10 to
1000 times more massive than star complexes in local galaxies, although their
separations are about the same. If they all form by gravitational
instabilities, then the gaseous velocity dispersions in interacting galaxies
have to be larger than in local galaxies by a factor of ~5 or more; the gas
column densities have to be larger by the square of this factor.
|
2024-08-12T18:16:26.644969 | 2007-04-06T18:23:55 | 0704.0912 | {
"authors": "Martin M. Boyd, Tanya Zelevinsky, Andrew D. Ludlow, Sebastian Blatt,\n Thomas Zanon-Willette, Seth M. Foreman and Jun Ye",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:912",
"submitter": "Jun Ye",
"url": "https://arxiv.org/abs/0704.0912"
} | arxiv-abstracts | We present a detailed experimental and theoretical study of the effect of
nuclear spin on the performance of optical lattice clocks. With a state-mixing
theory including spin-orbit and hyperfine interactions, we describe the origin
of the $^1S_0$-$^3P_0$ clock transition and the differential g-factor between
the two clock states for alkaline-earth(-like) atoms, using $^{87}$Sr as an
example. Clock frequency shifts due to magnetic and optical fields are
discussed with an emphasis on those relating to nuclear structure. An
experimental determination of the differential g-factor in $^{87}$Sr is
performed and is in good agreement with theory. The magnitude of the tensor
light shift on the clock states is also explored experimentally. State specific
measurements with controlled nuclear spin polarization are discussed as a
method to reduce the nuclear spin-related systematic effects to below
10$^{-17}$ in lattice clocks.
|
2024-08-12T18:16:26.645034 | 2007-04-06T18:36:28 | 0704.0913 | {
"authors": "Zhihong Lu, P. B. Visscher, and W. H. Butler",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:913",
"submitter": "Pieter Visscher",
"url": "https://arxiv.org/abs/0704.0913"
} | arxiv-abstracts | It has recently been suggested that exchange spring media offer a way to
increase media density without causing thermal instability
(superparamagnetism), by using a hard and a soft layer coupled by exchange.
Victora has suggested a figure of merit xi = 2 E_b/mu_0 m_s H_sw, the ratio of
the energy barrier to that of a Stoner-Wohlfarth system with the same switching
field, which is 1 for a Stoner-Wohlfarth (coherently switching) particle and 2
for an optimal two-layer composite medium. A number of theoretical approaches
have been used for this problem (e.g., various numbers of coupled
Stoner-Wohlfarth layers and continuum micromagnetics). In this paper we show
that many of these approaches can be regarded as special cases or
approximations to a variational formulation of the problem, in which the energy
is minimized for fixed magnetization. The results can be easily visualized in
terms of a plot of the energy as a function of magnetic moment m_z, in which
both the switching field [the maximum slope of E(m_z)] and the stability
(determined by the energy barrier E_b) are geometrically visible. In this
formulation we can prove a rigorous limit on the figure of merit xi, which can
be no higher than 4. We also show that a quadratic anistropy suggested by Suess
et al comes very close to this limit.
|
2024-08-12T18:16:26.645117 | 2007-04-06T18:44:19 | 0704.0914 | {
"authors": "Allan Greenleaf, Yaroslav Kurylev, Matti Lassas and Gunther Uhlmann",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:914",
"submitter": "Allan Greenleaf",
"url": "https://arxiv.org/abs/0704.0914"
} | arxiv-abstracts | Cloaking devices are prescriptions of electrostatic, optical or
electromagnetic parameter fields (conductivity $\sigma(x)$, index of refraction
$n(x)$, or electric permittivity $\epsilon(x)$ and magnetic permeability
$\mu(x)$) which are piecewise smooth on $\mathbb R^3$ and singular on a
hypersurface $\Sigma$, and such that objects in the region enclosed by $\Sigma$
are not detectable to external observation by waves. Here, we give related
constructions of invisible tunnels, which allow electromagnetic waves to pass
between possibly distant points, but with only the ends of the tunnels visible
to electromagnetic imaging. Effectively, these change the topology of space
with respect to solutions of Maxwell's equations, corresponding to attaching a
handlebody to $\mathbb R^3$. The resulting devices thus function as
electromagnetic wormholes.
|
2024-08-12T18:16:26.645177 | 2007-04-06T19:01:47 | 0704.0915 | {
"authors": "S. Noda, K. Hasegawa, H. Sugime, K. Kakehi, Z. Zhang, S. Maruyama, Y.\n Yamaguchi",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:915",
"submitter": "Shigeo Maruyama",
"url": "https://arxiv.org/abs/0704.0915"
} | arxiv-abstracts | A parametric study of so-called "super growth" of single-walled carbon
nanotubes(SWNTs) was done by using combinatorial libraries of iron/aluminum
oxide catalysts. Millimeter-thick forests of nanotubes grew within 10 min, and
those grown by using catalysts with a thin Fe layer (about 0.5 nm) were SWNTs.
Although nanotube forests grew under a wide range of reaction conditions such
as gas composition and temperature, the window for SWNT was narrow. Fe
catalysts rapidly grew nanotubes only when supported on aluminum oxide.
Aluminum oxide, which is a well-known catalyst in hydrocarbon reforming, plays
an essential role in enhancing the nanotube growth rates.
|
2024-08-12T18:16:26.645239 | 2007-04-06T18:47:34 | 0704.0916 | {
"authors": "A.V. Voinov, S.M. Grimes, C.R. Brune, M.J. Hornish, T.N. Massey, A.\n Salas",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:916",
"submitter": "Alexander Voinov dr",
"url": "https://arxiv.org/abs/0704.0916"
} | arxiv-abstracts | The energy spectra of neutrons, protons, and alpha-particles have been
measured from the d+59Co and 3He+58Fe reactions leading to the same compound
nucleus, 61$Ni. The experimental cross sections have been compared to
Hauser-Feshbach model calculations using different input level density models.
None of them have been found to agree with experiment. It manifests the serious
problem with available level density parameterizations especially those based
on neutron resonance spacings and density of discrete levels. New level
densities and corresponding Fermi-gas parameters have been obtained for
reaction product nuclei such as 60Ni,60Co, and 57Fe.
|
2024-08-12T18:16:26.645295 | 2007-04-06T19:28:33 | 0704.0917 | {
"authors": "Dominique Naef, Michel Mayor, Willy Benz, Francois Bouchy, Gaspare Lo\n Curto, Christophe Lovis, Claire Moutou, Francesco Pepe, Didier Queloz, Nuno\n C. Santos and Stephane Udry",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:917",
"submitter": "Dominique Naef",
"url": "https://arxiv.org/abs/0704.0917"
} | arxiv-abstracts | The HARPS high-resolution high-accuracy spectrograph is offered to the
astronomical community since the second half of 2003. Since then, we have been
using this instrument for monitoring radial velocities of a large sample of
Solar-type stars (~1400 stars) in order to search for their possible low-mass
companions. Amongst the goals of our survey, one is to significantly increase
the number of detected extra-solar planets in a volume-limited sample to
improve our knowledge of their orbital elements distributions and thus obtain
better constraints for planet-formation models.
In this paper, we present the HARPS radial-velocity data and orbital
solutions for 3 Solar-type stars: HD 100777, HD 190647, and HD 221287. The
radial-velocity data of HD 100777 is best explained by the presence of a 1.1
M_Jup planetary companion on a 384--day eccentric orbit (e=0.36). The orbital
fit obtained for the slightly evolved star HD 190647 reveals the presence of a
long-period (P=1038 d) 1.9 M_Jup planetary companion on a moderately eccentric
orbit (e=0.18). HD 221287 is hosting a 3.1 M_Jup planet on a 456--day orbit.
The shape of this orbit is not very well constrained because of our non-optimal
temporal coverage and because of the presence of abnormally large residuals. We
find clues for these large residuals to result from spectral line profile
variations probably induced by stellar activity related processes.
|
2024-08-12T18:16:26.645542 | 2007-04-06T19:14:52 | 0704.0918 | {
"authors": "Seth Sullivant",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:918",
"submitter": "Seth Sullivant",
"url": "https://arxiv.org/abs/0704.0918"
} | arxiv-abstracts | Conditional independence models in the Gaussian case are algebraic varieties
in the cone of positive definite covariance matrices. We study these varieties
in the case of Bayesian networks, with a view towards generalizing the
recursive factorization theorem to situations with hidden variables. In the
case when the underlying graph is a tree, we show that the vanishing ideal of
the model is generated by the conditional independence statements implied by
graph. We also show that the ideal of any Bayesian network is homogeneous with
respect to a multigrading induced by a collection of upstream random variables.
This has a number of important consequences for hidden variable models.
Finally, we relate the ideals of Bayesian networks to a number of classical
constructions in algebraic geometry including toric degenerations of the
Grassmannian, matrix Schubert varieties, and secant varieties.
|
2024-08-12T18:16:26.645612 | 2007-04-06T19:26:30 | 0704.0919 | {
"authors": "Oleksandr Zelyak, Ganpathy Murthy, Igor Rozhkov",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:919",
"submitter": "Ganpathy Murthy",
"url": "https://arxiv.org/abs/0704.0919"
} | arxiv-abstracts | We study a system of two quantum dots connected by a hopping bridge. Both the
dots and connecting region are assumed to be in universal crossover regimes
between Gaussian Orthogonal and Unitary ensembles. Using a diagrammatic
approach appropriate for energy separations much larger than the level spacing
we obtain the ensemble-averaged one- and two-particle Green's functions. It
turns out that the diffuson and cooperon parts of the two-particle Green's
function can be described by separate scaling functions. We then use this
information to investigate a model interacting system in which one dot has an
attractive s-wave reduced Bardeen-Cooper-Schrieffer interaction, while the
other is noninteracting but subject to an orbital magnetic field. We find that
the critical temperature is {\it nonmonotonic} in the flux through the second
dot in a certain regime of interdot coupling. Likewise, the fluctuation
magnetization above the critical temperature is also nonmonotonic in this
regime, can be either diamagnetic or paramagnetic, and can be deduced from the
cooperon scaling function.
|
2024-08-12T18:16:26.645683 | 2007-04-06T19:47:23 | 0704.0920 | {
"authors": "L.V. Grigorenko, M.V. Zhukov",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:920",
"submitter": "Leonid Grigorenko",
"url": "https://arxiv.org/abs/0704.0920"
} | arxiv-abstracts | Three-body decays of resonant states are studied using integral formulae for
decay widths. Theoretical approach with a simplified Hamiltonian allows
semianalytical treatment of the problem. The model is applied to decays of the
first excited $3/2^{-}$ state of $^{17}$Ne and the $3/2^{-}$ ground state of
$^{45}$Fe. The convergence of three-body hyperspherical model calculations to
the exact result for widths and energy distributions are studied. The
theoretical results for $^{17}$Ne and $^{45}$Fe decays are updated and
uncertainties of the derived values are discussed in detail. Correlations for
the decay of $^{17}$Ne $3/2^-$ state are also studied.
|
2024-08-12T18:16:26.645743 | 2007-04-06T19:24:22 | 0704.0921 | {
"authors": "A. P. Balachandran, S. G. Jo",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:921",
"submitter": "Sang Jo",
"url": "https://arxiv.org/abs/0704.0921"
} | arxiv-abstracts | Yang's theorem forbids the process $Z^0 \to 2\gamma$ in any Poincar\'{e}
invariant theory if photons are bosons and their two-particle states transform
under the Poincar\'{e} group in the standard way (under the standard coproduct
of the Poincar\'{e} group). This is an important result as it does not depend
on the assumptions of quantum field theory. Recent work on noncommutative
geometry requires deforming the above coproduct by the Drinfel'd twist. We
prove that $Z^0 \to 2\gamma$ is forbidden for the twisted coproduct as well.
This result is also independent of the assumptions of quantum field theory. As
an illustration of the use of our general formulae, we further show that $Z^0
\to \nu + \nu$ is forbidden for the standard or twisted coproduct of the
Poincar\'{e} group if the neutrino is massless, even if lepton number is not
conserved. This is a special case of our general result that a massive particle
of spin $j$ cannot decay into two identical massless particles of the same
helicity if $j$ is odd, regardless of the coproduct used.
|
2024-08-12T18:16:26.645810 | 2007-04-06T19:29:25 | 0704.0922 | {
"authors": "Quang-Cuong Pham (LPPA, College de France)",
"full_text_license": "arXiv.org - Non-exclusive license to distribute - http://arxiv.org/licenses/nonexclusive-distrib/1.0/",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:922",
"submitter": "Quang-Cuong Pham",
"url": "https://arxiv.org/abs/0704.0922"
} | arxiv-abstracts | We prove a variation of Gronwall's lemma.
|
2024-08-12T18:16:26.645841 | 2007-04-06T19:37:34 | 0704.0923 | {
"authors": "Steven J. Miller",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:923",
"submitter": "Steven Miller",
"url": "https://arxiv.org/abs/0704.0923"
} | arxiv-abstracts | We investigate a one-parameter family of probability densities (related to
the Pareto distribution, which describes many natural phenomena) where the
Cramer-Rao inequality provides no information.
|
2024-08-12T18:16:26.645876 | 2007-04-06T19:44:07 | 0704.0924 | {
"authors": "Steven J. Miller",
"full_text_license": "arXiv.org - Non-exclusive license to distribute - http://arxiv.org/licenses/nonexclusive-distrib/1.0/",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:924",
"submitter": "Steven Miller",
"url": "https://arxiv.org/abs/0704.0924"
} | arxiv-abstracts | The Katz-Sarnak density conjecture states that, in the limit as the
conductors tend to infinity, the behavior of normalized zeros near the central
point of families of L-functions agree with the N -> oo scaling limits of
eigenvalues near 1 of subgroups of U(N). Evidence for this has been found for
many families by studying the n-level densities; for suitably restricted test
functions the main terms agree with random matrix theory. In particular, all
one-parameter families of elliptic curves with rank r over Q(T) and the same
distribution of signs of functional equations have the same limiting behavior.
We break this universality and find family dependent lower order correction
terms in many cases; these lower order terms have applications ranging from
excess rank to modeling the behavior of zeros near the central point, and
depend on the arithmetic of the family. We derive an alternate form of the
explicit formula for GL(2) L-functions which simplifies comparisons, replacing
sums over powers of Satake parameters by sums of the moments of the Fourier
coefficients lambda_f(p). Our formula highlights the differences that we expect
to exist from families whose Fourier coefficients obey different laws (for
example, we expect Sato-Tate to hold only for non-CM families of elliptic
curves). Further, by the work of Rosen and Silverman we expect lower order
biases to the Fourier coefficients in families of elliptic curves with rank
over Q(T); these biases can be seen in our expansions. We analyze several
families of elliptic curves and see different lower order corrections,
depending on whether or not the family has complex multiplication, a forced
torsion point, or non-zero rank over Q(T).
|
2024-08-12T18:16:26.645974 | 2007-04-06T19:48:17 | 0704.0925 | {
"authors": "A.T. Black, E. Gomez, L.D. Turner, S. Jung, P.D. Lett",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:925",
"submitter": "Adam Black",
"url": "https://arxiv.org/abs/0704.0925"
} | arxiv-abstracts | We observe coherent spin oscillations in an antiferromagnetic spin-1
Bose-Einstein condensate of sodium. The variation of the spin oscillations with
magnetic field shows a clear signature of nonlinearity, in agreement with
theory, which also predicts anharmonic oscillations near a critical magnetic
field. Measurements of the magnetic phase diagram agree with predictions made
in the approximation of a single spatial mode. The oscillation period yields
the best measurement to date of the sodium spin-dependent interaction
coefficient, determining that the difference between the sodium spin-dependent
s-wave scattering lengths $a_{f=2}-a_{f=0}$ is $2.47\pm0.27$ Bohr radii.
|
2024-08-12T18:16:26.646024 | 2007-04-06T19:58:52 | 0704.0926 | {
"authors": "Q.-C. Pham, N. Tabareau, J.-J. Slotine",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:926",
"submitter": "Quang-Cuong Pham",
"url": "https://arxiv.org/abs/0704.0926"
} | arxiv-abstracts | We investigate the incremental stability properties of It\^o stochastic
dynamical systems. Specifically, we derive a stochastic version of nonlinear
contraction theory that provides a bound on the mean square distance between
any two trajectories of a stochastically contracting system. This bound can be
expressed as a function of the noise intensity and the contraction rate of the
noise-free system. We illustrate these results in the contexts of stochastic
nonlinear observers design and stochastic synchronization.
|
2024-08-12T18:16:26.646079 | 2007-04-06T19:59:58 | 0704.0927 | {
"authors": "Steven J. Miller",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:927",
"submitter": "Steven Miller",
"url": "https://arxiv.org/abs/0704.0927"
} | arxiv-abstracts | Recently Conrey, Farmer and Zirnbauer conjectured formulas for the averages
over a family of ratios of products of shifted L-functions. Their L-functions
Ratios Conjecture predicts both the main and lower order terms for many
problems, ranging from n-level correlations and densities to mollifiers and
moments to vanishing at the central point. There are now many results showing
agreement between the main terms of number theory and random matrix theory;
however, there are very few families where the lower order terms are known.
These terms often depend on subtle arithmetic properties of the family, and
provide a way to break the universality of behavior. The L-functions Ratios
Conjecture provides a powerful and tractable way to predict these terms. We
test a specific case here, that of the 1-level density for the symplectic
family of quadratic Dirichlet characters arising from even fundamental
discriminants d \le X. For test functions supported in (-1/3, 1/3) we calculate
all the lower order terms up to size O(X^{-1/2+epsilon}) and observe perfect
agreement with the conjecture (for test functions supported in (-1, 1) we show
agreement up to errors of size O(X^{-epsilon}) for any epsilon). Thus for this
family and suitably restricted test functions, we completely verify the Ratios
Conjecture's prediction for the 1-level density.
|
2024-08-12T18:16:26.646161 | 2007-04-06T20:00:10 | 0704.0928 | {
"authors": "Luis Anchordoqui, Haim Goldberg, Satoshi Nawata, Carlos Nunez",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:928",
"submitter": "Luis Anchordoqui",
"url": "https://arxiv.org/abs/0704.0928"
} | arxiv-abstracts | We explore the cosmological content of Salam-Sezgin six dimensional
supergravity, and find a solution to the field equations in qualitative
agreement with observation of distant supernovae, primordial nucleosynthesis
abundances, and recent measurements of the cosmic microwave background. The
carrier of the acceleration in the present de Sitter epoch is a quintessence
field slowly rolling down its exponential potential. Intrinsic to this model is
a second modulus which is automatically stabilized and acts as a source of cold
dark matter with a mass proportional to an exponential function of the
quintessence field (hence realizing VAMP models within a String context).
However, any attempt to saturate the present cold dark matter component in this
manner leads to unacceptable deviations from cosmological data -- a numerical
study reveals that this source can account for up to about 7% of the total cold
dark matter budget. We also show that (1) the model will support a de Sitter
energy in agreement with observation at the expense of a miniscule breaking of
supersymmetry in the compact space; (2) variations in the fine structure
constant are controlled by the stabilized modulus and are negligible; (3)
``fifth''forces are carried by the stabilized modulus and are short range; (4)
the long time behavior of the model in four dimensions is that of a
Robertson-Walker universe with a constant expansion rate (w = -1/3). Finally,
we present a String theory background by lifting our six dimensional
cosmological solution to ten dimensions.
|
2024-08-12T18:16:26.646251 | 2007-04-09T19:54:16 | 0704.0929 | {
"authors": "Hyun Seok Yang",
"full_text_license": "arXiv.org - Non-exclusive license to distribute - http://arxiv.org/licenses/nonexclusive-distrib/1.0/",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:929",
"submitter": "Hyun Seok Yang",
"url": "https://arxiv.org/abs/0704.0929"
} | arxiv-abstracts | We map noncommutative (NC) U(1) gauge theory on R^d_C X R^{2n}_{NC} to U(N ->
\infty) Yang-Mills theory on R^d_C, where R^d_C is a d-dimensional commutative
spacetime while R^{2n}_{NC} is a 2n-dimensional NC space. The resulting U(N)
Yang-Mills theory on R^d_C is equivalent to that obtained by the dimensional
reduction of (d+2n)-dimensional U(N) Yang-Mills theory onto R^d_C. We show that
the gauge-Higgs system (A_\mu,\Phi^a) in the U(N -> \infty) Yang-Mills theory
on R^d_C leads to an emergent geometry in the (d+2n)-dimensional spacetime
whose metric was determined by Ward a long time ago. In particular, the
10-dimensional gravity for d=4 and n=3 corresponds to the emergent geometry
arising from the 4-dimensional N=4 vector multiplet in the AdS/CFT duality. We
further elucidate the emergent gravity by showing that the gauge-Higgs system
(A_\mu,\Phi^a) in half-BPS configurations describes self-dual Einstein gravity.
|
2024-08-12T18:16:26.646330 | 2007-04-09T06:59:52 | 0704.0930 | {
"authors": "Theodore Erler",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:930",
"submitter": "Theodore G. Erler",
"url": "https://arxiv.org/abs/0704.0930"
} | arxiv-abstracts | We construct a class of analytic solutions of WZW-type open superstring field
theory describing marginal deformations of a reference D-brane background. The
deformations we consider are generated by on-shell vertex operators with
vanishing operator products. The superstring solution exhibits an intriguing
duality with the corresponding marginal solution of the {\it bosonic} string.
In particular, the superstring problem is ``dual'' to the problem of
re-expressing the bosonic marginal solution in pure gauge form. This represents
the first nonsingular analytic solution of open superstring field theory.
|
2024-08-12T18:16:26.646381 | 2007-04-06T20:25:00 | 0704.0931 | {
"authors": "Anna Pasquali, Frank C. van den Bosch, Hans-Walter Rix (MPIA)",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:931",
"submitter": "Frank van den Bosch",
"url": "https://arxiv.org/abs/0704.0931"
} | arxiv-abstracts | We study the dependence of the isophotal shape of early-type galaxies on
their absolute B-band magnitude, their dynamical mass, and their nuclear
activity and environment, using an unprecedented large sample of 847 early-type
galaxies identified in the SDSS by Hao et al (2006). We find that the fraction
of disky galaxies smoothly decreases with increasing luminosity. The large
sample allows us to describe these trends accurately with tight linear
relations that are statistically robust against the uncertainty in the
isophotal shape measurements. There is also a host of significant correlations
between the disky fraction and indicators of nuclear activity (both in the
optical and in the radio) and environment (soft X-rays, group mass, group
hierarchy). Our analysis shows however that these correlations can be
accurately matched by assuming that the disky fraction depends only on galaxy
luminosity or mass. We therefore conclude that neither the level of activity,
nor group mass or group hierarchy help in better predicting the isophotal shape
of early-type galaxies.
|
2024-08-12T18:16:26.646458 | 2007-04-06T20:13:20 | 0704.0932 | {
"authors": "Xi Kang, Frank C. van den Bosch, Anna Pasquali (MPIA)",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:932",
"submitter": "Frank van den Bosch",
"url": "https://arxiv.org/abs/0704.0932"
} | arxiv-abstracts | Using a semi-analytical model for galaxy formation, combined with a large
N-body simulation, we investigate the origin of the dichotomy among early-type
galaxies. We find that boxy galaxies originate from mergers with a progenitor
mass ratio $n < 2$ and with a combined cold gas mass fraction $F_{\rm cold} <
0.1$. Our model accurately reproduces the observed fraction of boxy systems as
a function of luminosity and halo mass, for both central galaxies and
satellites. After correcting for the stellar mass dependence, the properties of
the last major merger of early-type galaxies are independent of their halo
mass. This provides theoretical support for the conjecture of Pasquali et al
(2007) that the stellar mass of an early-type galaxy is the main parameter that
governs its isophotal shape. We argue that the observed dichotomy of early-type
galaxies has a natural explanation within hierarchical structure formation, and
does not require AGN feedback. Rather, we argue that it owes to the fact that
more massive systems (i) have more massive progenitors, (ii) assemble later,
and (iii) have a larger fraction of early-type progenitors. Each of these three
trends causes the cold gas mass fraction of the progenitors of more massive
early-types to be lower, so that their last major merger was dryer. Finally,
our model predicts that (i) less than 10 percent of all early-type galaxies
form in major mergers that involve two early-type progenitors, (ii) more than
95 percent of all boxy early-type galaxies with $M_* < 2 \times 10^{10} h^{-1}
\Msun$ are satellite galaxies, and (iii) about 70 percent of all low mass
early-types do not form a supermassive black hole binary at their last major
merger. The latter may help to explain why low mass early-types have central
cusps, while their massive counterparts have cores.
|
2024-08-12T18:16:26.646551 | 2007-04-06T20:06:15 | 0704.0933 | {
"authors": "Fa Wang, Ashvin Vishwanath, Yong Baek Kim",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:933",
"submitter": "Fa Wang",
"url": "https://arxiv.org/abs/0704.0933"
} | arxiv-abstracts | In Volborthite, spin-1/2 moments form a distorted Kagom\'e lattice, of corner
sharing isosceles triangles with exchange constants $J$ on two bonds and $J'$
on the third bond. We study the properties of such spin systems, and show that
despite the distortion, the lattice retains a great deal of frustration.
Although sub-extensive, the classical ground state degeneracy remains very
large, growing exponentially with the system perimeter. We consider degeneracy
lifting by thermal and quantum fluctuations. To linear (spin wave) order, the
degeneracy is found to stay intact. Two complementary approaches are therefore
introduced, appropriate to low and high temperatures, which point to the same
ordered pattern. In the low temperature limit, an effective chirality
Hamiltonian is derived from non-linear spin waves which predicts a transition
on increasing $J'/J$, from $\sqrt 3\times \sqrt 3$ type order to a new
ferrimagnetic {\em striped chirality} order with a doubled unit cell. This is
confirmed by a large-N approximation on the O($n$) model on this lattice. While
the saddle point solution produces a line degeneracy, $O(1/n)$ corrections
select the non-trivial wavevector of the striped chirality state. The quantum
limit of spin 1/2 on this lattice is studied via exact small system
diagonalization and compare well with experimental results at intermediate
temperatures. We suggest that the very low temperature spin frozen state seen
in NMR experiments may be related to the disconnected nature of classical
ground states on this lattice, which leads to a prediction for NMR line shapes.
|
2024-08-12T18:16:26.646639 | 2007-04-06T20:08:13 | 0704.0934 | {
"authors": "L.V. Grigorenko, M.V. Zhukov",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:934",
"submitter": "Leonid Grigorenko",
"url": "https://arxiv.org/abs/0704.0934"
} | arxiv-abstracts | We derive quasiclassical expressions for the three-body decay width and
define the ``preexponential'' coefficients for them. The derivation is based on
the integral formulae for the three-body width obtained in the semianalytical
approach with simplified three-body Hamiltonian [L.V. Grigorenko and M.V.\
Zhukov, arXiv:0704.0920v1]. The model is applied to the decays of the first
excited $3/2^{-}$ state of $^{17}$Ne and $3/2^{-}$ ground state of $^{45}$Fe.
Various qualitative aspects of the model and relations with the other
simplified approaches to the three-body decays are discussed.
|
2024-08-12T18:16:26.646691 | 2007-04-06T20:08:57 | 0704.0935 | {
"authors": "Alexander Dementsov, Vladimir Privman",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:935",
"submitter": "Vladimir Privman",
"url": "https://arxiv.org/abs/0704.0935"
} | arxiv-abstracts | We explore the conductance of self-healing materials as a measure of the
material integrity in the regime of the onset of the initial fatigue. Continuum
effective-field modeling and lattice numerical simulations are reported. Our
results illustrate the general features of the self-healing process: The onset
of the material fatigue is delayed, by developing a plateau-like
time-dependence of the material quality. We demonstrate that in this low-damage
regime, the changes in the conductance and similar transport/response
properties of the material can be used as measures of the material quality
degradation.
|
2024-08-12T18:16:26.646750 | 2007-04-09T17:20:58 | 0704.0936 | {
"authors": "Yuji Okawa (DESY)",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:936",
"submitter": "Yuji Okawa",
"url": "https://arxiv.org/abs/0704.0936"
} | arxiv-abstracts | We extend the calculable analytic approach to marginal deformations recently
developed in open bosonic string field theory to open superstring field theory
formulated by Berkovits. We construct analytic solutions to all orders in the
deformation parameter when operator products made of the marginal operator and
the associated superconformal primary field are regular.
|
2024-08-12T18:16:26.646789 | 2007-04-06T20:29:49 | 0704.0937 | {
"authors": "Vyacheslav Boyko, Jiri Patera and Roman Popovych",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:937",
"submitter": "Vyacheslav Boyko",
"url": "https://arxiv.org/abs/0704.0937"
} | arxiv-abstracts | Triangular Lie algebras are the Lie algebras which can be faithfully
represented by triangular matrices of any finite size over the real/complex
number field. In the paper invariants ('generalized Casimir operators') are
found for three classes of Lie algebras, namely those which are either strictly
or non-strictly triangular, and for so-called special upper triangular Lie
algebras. Algebraic algorithm of [J. Phys. A: Math. Gen., 2006, V.39, 5749;
math-ph/0602046], developed further in [J. Phys. A: Math. Theor., 2007, V.40,
113; math-ph/0606045], is used to determine the invariants. A conjecture of [J.
Phys. A: Math. Gen., 2001, V.34, 9085], concerning the number of independent
invariants and their form, is corroborated.
|
2024-08-12T18:16:26.646846 | 2007-04-06T20:32:31 | 0704.0938 | {
"authors": "Hui Wang, Kipton Barros, Harvey Gould and W. Klein",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:938",
"submitter": "Hui Wang",
"url": "https://arxiv.org/abs/0704.0938"
} | arxiv-abstracts | We investigate the approach to stable and metastable equilibrium in Ising
models using a cluster representation. The distribution of nucleation times is
determined using the Metropolis algorithm and the corresponding $\phi^{4}$
model using Langevin dynamics. We find that the nucleation rate is suppressed
at early times even after global variables such as the magnetization and energy
have apparently reached their time independent values. The mean number of
clusters whose size is comparable to the size of the nucleating droplet becomes
time independent at about the same time that the nucleation rate reaches its
constant value. We also find subtle structural differences between the
nucleating droplets formed before and after apparent metastable equilibrium has
been established.
|
2024-08-12T18:16:26.646909 | 2007-04-06T20:34:45 | 0704.0939 | {
"authors": "Giridhar Nandikotkur, Keith M. Jahoda, R. C. Hartman, R. Mukherjee, P.\n Sreekumar, M. B\\\"ottcher, R. M. Sambruna, and Jean H. Swank",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:939",
"submitter": "Giridhar Nandikotkur",
"url": "https://arxiv.org/abs/0704.0939"
} | arxiv-abstracts | The Energetic Gamma-Ray Experiment Telescope (EGRET) on the Compton Gamma-Ray
Observatory (CGRO) discovered gamma-ray emission from more than 67 blazars
during its 9 yr lifetime. We conducted an exhaustive search of the EGRET
archives and selected all the blazars that were observed multiple times and
were bright enough to enable a spectral analysis using standard power-law
models. The sample consists of 18 flat-spectrum radio quasars(FSRQs), 6
low-frequency peaked BL Lac objects (LBLs) and 2 high-frequency peaked BL Lac
objects (HBLs). We do not detect any clear pattern in the variation of spectral
index with flux. Some of the blazars do not show any statistical evidence for
spectral variability. The spectrum hardens with increasing flux in a few cases.
There is also evidence for a flux-hardness anticorrelation at low fluxes in
five blazars. The well-observed blazars (3C 279, 3C 273, PKS 0528+134, PKS
1622-297 PKS 0208-512) do not show any overall trend in the long-term spectral
dependence on flux, but the sample shows a mixture of hard and soft states. We
observed a previously unreported spectral hysteresis at weekly timescales in
all three FSRQs for which data from flares lasting for ~(3-4) weeks were
available. All three sources show a counterclockwise rotation, despite the
widely different flux profiles. We analyze the observed spectral behavior in
the context of various inverse Compton mechanisms believed to be responsible
for emission in the EGRET energy range. Our analysis uses the EGRET skymaps
that were regenerated to include the changes in performance during the mission.
|
2024-08-12T18:16:26.646996 | 2007-04-06T20:38:52 | 0704.0940 | {
"authors": "Peter Orland",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:940",
"submitter": "Peter Orland",
"url": "https://arxiv.org/abs/0704.0940"
} | arxiv-abstracts | The confinement problem has been solved in the anisotropic (2+1)-dimensional
SU(N) Yang-Mills theory at weak coupling. In this paper, we find the low-lying
spectrum for N=2. The lightest excitations are pairs of fundamental particles
of the (1+1)-dimensional SU(2)XSU(2) principal chiral sigma model bound in a
linear potential, with a specified matching condition where the particles
overlap. This matching condition can be determined from the exactly-known
S-matrix for the sigma model.
|
2024-08-12T18:16:26.647046 | 2007-04-06T20:43:29 | 0704.0941 | {
"authors": "Rita Tojeiro (IfA, Edinburgh), Alan F. Heavens (IfA, Edinburgh), Raul\n Jimenez (UPenn), Ben Panter (IfA, Edinburgh)",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:941",
"submitter": "Raul Jimenez",
"url": "https://arxiv.org/abs/0704.0941"
} | arxiv-abstracts | We introduce VErsatile SPectral Analysis (VESPA): a new method which aims to
recover robust star formation and metallicity histories from galactic spectra.
VESPA uses the full spectral range to construct a galaxy history from synthetic
models. We investigate the use of an adaptative parametrization grid to recover
reliable star formation histories on a galaxy-by-galaxy basis. Our goal is
robustness as opposed to high resolution histories, and the method is designed
to return high time resolution only where the data demand it. In this paper we
detail the method and we present our findings when we apply VESPA to synthetic
and real Sloan Digital Sky Survey (SDSS) spectroscopic data. We show that the
number of parameters that can be recovered from a spectrum depends strongly on
the signal-to-noise, wavelength coverage and presence or absence of a young
population. For a typical SDSS sample of galaxies, we can normally recover
between 2 to 5 stellar populations. We find very good agreement between VESPA
and our previous analysis of the SDSS sample with MOPED.
|
2024-08-12T18:16:26.647115 | 2007-04-06T20:45:17 | 0704.0942 | {
"authors": "Laura DeMarco and Suzanne Lynch Hruska",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:942",
"submitter": "Suzanne Lynch Hruska",
"url": "https://arxiv.org/abs/0704.0942"
} | arxiv-abstracts | A polynomial skew product of C^2 is a map of the form f(z,w) = (p(z),
q(z,w)), where p and q are polynomials, such that f is regular of degree d >=
2. For polynomial maps of C, hyperbolicity is equivalent to the condition that
the closure of the postcritical set is disjoint from the Julia set; further,
critical points either iterate to an attracting cycle or infinity. For
polynomial skew products, Jonsson (Math. Ann., 1999) established that f is
Axiom A if and only if the closure of the postcritical set is disjoint from the
right analog of the Julia set. Here we present the analogous conclusion:
critical orbits either escape to infinity or accumulate on an attracting set.
In addition, we construct new examples of Axiom A maps demonstrating various
postcritical behaviors.
|
2024-08-12T18:16:26.647175 | 2007-04-06T20:45:17 | 0704.0943 | {
"authors": "LIGO Scientific Collaboration",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:943",
"submitter": "Peter Shawhan",
"url": "https://arxiv.org/abs/0704.0943"
} | arxiv-abstracts | The fourth science run of the LIGO and GEO 600 gravitational-wave detectors,
carried out in early 2005, collected data with significantly lower noise than
previous science runs. We report on a search for short-duration
gravitational-wave bursts with arbitrary waveform in the 64-1600 Hz frequency
range appearing in all three LIGO interferometers. Signal consistency tests,
data quality cuts, and auxiliary-channel vetoes are applied to reduce the rate
of spurious triggers. No gravitational-wave signals are detected in 15.5 days
of live observation time; we set a frequentist upper limit of 0.15 per day (at
90% confidence level) on the rate of bursts with large enough amplitudes to be
detected reliably. The amplitude sensitivity of the search, characterized using
Monte Carlo simulations, is several times better than that of previous
searches. We also provide rough estimates of the distances at which
representative supernova and binary black hole merger signals could be detected
with 50% efficiency by this analysis.
|
2024-08-12T18:16:26.647244 | 2007-04-07T00:06:58 | 0704.0944 | {
"authors": "Michael Kuhlen (1), J\\\"urg Diemand (2) and Piero Madau (2, 3) ((1)\n Institute for Advanced Study, Princeton, (2) UC Santa Cruz, (3)\n Max-Planck-Institut f\\\"ur Astrophysik, Garching, Germany)",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:944",
"submitter": "Michael Kuhlen",
"url": "https://arxiv.org/abs/0704.0944"
} | arxiv-abstracts | We discuss the possibility of GLAST detecting gamma-rays from the
annihilation of neutralino dark matter in the Galactic halo. We have used "Via
Lactea", currently the highest resolution simulation of Galactic cold dark
matter substructure, to quantify the contribution of subhalos to the
annihilation signal. We present a simulated allsky map of the expected
gamma-ray counts from dark matter annihilation, assuming standard values of
particle mass and cross section. In this case GLAST should be able to detect
the Galactic center and several individual subhalos.
|
2024-08-12T18:16:26.647296 | 2007-04-06T20:53:36 | 0704.0945 | {
"authors": "Peter McCullagh, Jim Pitman, Matthias Winkel",
"full_text_license": "arXiv.org - Non-exclusive license to distribute - http://arxiv.org/licenses/nonexclusive-distrib/1.0/",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:945",
"submitter": "Peter McCullagh",
"url": "https://arxiv.org/abs/0704.0945"
} | arxiv-abstracts | We study fragmentation trees of Gibbs type. In the binary case, we identify
the most general Gibbs-type fragmentation tree with Aldous' beta-splitting
model, which has an extended parameter range $\beta>-2$ with respect to the
${\rm beta}(\beta+1,\beta+1)$ probability distributions on which it is based.
In the multifurcating case, we show that Gibbs fragmentation trees are
associated with the two-parameter Poisson--Dirichlet models for exchangeable
random partitions of $\mathbb {N}$, with an extended parameter range
$0\le\alpha\le1$, $\theta\ge-2\alpha$ and $\alpha<0$, $\theta =-m\alpha$, $m\in
\mathbb {N}$.
|
2024-08-12T18:16:26.647356 | 2007-04-09T19:40:39 | 0704.0946 | {
"authors": "Andrei Mesinger and Steven Furlanetto",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:946",
"submitter": "Andrei Mesinger",
"url": "https://arxiv.org/abs/0704.0946"
} | arxiv-abstracts | We present a method to construct semi-numerical ``simulations'', which can
efficiently generate realizations of halo distributions and ionization maps at
high redshifts. Our procedure combines an excursion-set approach with
first-order Lagrangian perturbation theory and operates directly on the linear
density and velocity fields. As such, the achievable dynamic range with our
algorithm surpasses the current practical limit of N-body codes by orders of
magnitude. This is particularly significant in studies of reionization, where
the dynamic range is the principal limiting factor. We test our halo-finding
and HII bubble-finding algorithms independently against N-body simulations with
radiative transfer and obtain excellent agreement. We compute the size
distributions of ionized and neutral regions in our maps. We find even larger
ionized bubbles than do purely analytic models at the same volume-weighted mean
hydrogen neutral fraction. We also generate maps and power spectra of 21-cm
brightness temperature fluctuations, which for the first time include
corrections due to gas bulk velocities. We find that velocities widen the tails
of the temperature distributions and increase small-scale power, though these
effects quickly diminish as reionization progresses. We also include some
preliminary results from a simulation run with the largest dynamic range to
date: a 250 Mpc box that resolves halos with masses M >~ 2.2 x10^8 M_sun. We
show that accurately modeling the late stages of reionization requires such
large scales. The speed and dynamic range provided by our semi-numerical
approach will be extremely useful in the modeling of early structure formation
and reionization.
|
2024-08-12T18:16:26.647448 | 2007-04-09T13:17:42 | 0704.0947 | {
"authors": "Satoki Matsushita, Sebastien Muller, Jeremy Lim (ASIAA)",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:947",
"submitter": "Satoki Matsushita",
"url": "https://arxiv.org/abs/0704.0947"
} | arxiv-abstracts | Previous molecular gas observations at arcsecond-scale resolution of the
Seyfert 2 galaxy M51 suggest the presence of a dense circumnuclear rotating
disk, which may be the reservoir for fueling the active nucleus and obscures it
from direct view in the optical. However, our recent interferometric CO(3-2)
observations show a hint of a velocity gradient perpendicular to the rotating
disk, which suggests a more complex structure than previously thought. To image
the putative circumnuclear molecular gas disk at sub-arcsecond resolution to
better understand both the spatial distribution and kinematics of the molecular
gas. We carried out CO(2-1) and CO(1-0) line observations of the nuclear region
of M51 with the new A configuration of the IRAM Plateau de Bure Interferometer,
yielding a spatial resolution lower than 15 pc. The high resolution images show
no clear evidence of a disk, aligned nearly east-west and perpendicular to the
radio jet axis, as suggested by previous observations, but show two separate
features located on the eastern and western sides of the nucleus. The western
feature shows an elongated structure along the jet and a good velocity
correspondence with optical emission lines associated with the jet, suggesting
that this feature is a jet-entrained gas. The eastern feature is elongated
nearly east-west ending around the nucleus. A velocity gradient appears in the
same direction with increasingly blueshifted velocities near the nucleus. This
velocity gradient is in the opposite sense of that previously inferred for the
putative circumnuclear disk. Possible explanations for the observed molecular
gas distribution and kinematics are that a rotating gas disk disturbed by the
jet, gas streaming toward the nucleus, or a ring with another smaller counter-
or Keplarian-rotating gas disk inside.
|
2024-08-12T18:16:26.647547 | 2007-04-06T21:27:31 | 0704.0948 | {
"authors": "H. A. Sheets, J. R. Thorstensen, C. J. Peters, A. B. Kapusta and C. J.\n Taylor",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:948",
"submitter": "John R. Thorstensen",
"url": "https://arxiv.org/abs/0704.0948"
} | arxiv-abstracts | We present optical spectroscopy of nine cataclysmic binary stars, mostly
dwarf novae, obtained primarily to determine orbital periods Porb. The stars
and their periods are LX And, 0.1509743(5) d; CZ Aql, 0.2005(6) d; LU Cam,
0.1499686(4) d; GZ Cnc, 0.0881(4) d; V632 Cyg, 0.06377(8) d; V1006 Cyg,
0.09903(9) d; BF Eri, 0.2708804(4) d; BI Ori, 0.1915(5) d; and FO Per, for
which Porb is either 0.1467(4) or 0.1719(5) d.
Several of the stars proved to be especially interesting. In BF Eri, we
detect the absorption spectrum of a secondary star of spectral type K3 +- 1
subclass, which leads to a distance estimate of approximately 1 kpc. However,
BF Eri has a large proper motion (100 mas/yr), and we have a preliminary
parallax measurement that confirms the large proper motion and yields only an
upper limit for the parallax. BF Eri's space velocity is evidently large, and
it appears to belong to the halo population. In CZ Aql, the emission lines have
strong wings that move with large velocity amplitude, suggesting a
magnetically-channeled accretion flow. The orbital period of V1006 Cyg places
it squarely within the 2- to 3-hour "gap" in the distribution of cataclysmic
binary orbital periods.
|
2024-08-12T18:16:26.647621 | 2007-04-06T21:31:14 | 0704.0949 | {
"authors": "Gastao S. F. Frederico, Delfim F. M. Torres",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:949",
"submitter": "Delfim F. M. Torres",
"url": "https://arxiv.org/abs/0704.0949"
} | arxiv-abstracts | The study of problems of the calculus of variations with compositions is a
quite recent subject with origin in dynamical systems governed by chaotic maps.
Available results are reduced to a generalized Euler-Lagrange equation that
contains a new term involving inverse images of the minimizing trajectories. In
this work we prove a generalization of the necessary optimality condition of
DuBois-Reymond for variational problems with compositions. With the help of the
new obtained condition, a Noether-type theorem is proved. An application of our
main result is given to a problem appearing in the chaotic setting when one
consider maps that are ergodic.
|
2024-08-12T18:16:26.647687 | 2007-04-06T22:13:45 | 0704.0950 | {
"authors": "Yogesh C. Joshi (Queen's University Belfast)",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:950",
"submitter": "Yogesh Joshi",
"url": "https://arxiv.org/abs/0704.0950"
} | arxiv-abstracts | We have carried out a comparative statistical study for the displacement of
the Sun from the Galactic plane (z_\odot) following three different methods.
The study has been done using a sample of 537 young open clusters (YOCs) with
log(Age) < 8.5 lying within a heliocentric distance of 4 kpc and 2030 OB stars
observed up to a distance of 1200 pc, all of them have distance information. We
decompose the Gould Belt's member in a statistical sense before investigating
the variation in the z_\odot estimation with different upper cut-off limits in
the heliocentric distance and distance perpendicular to the Galactic plane. We
found z_\odot varies in a range of ~ 13 - 20 pc from the analys is of YOCs and
~ 6 - 18 pc from the OB stars. A significant scatter in the z_\odot obtained
due to different cut-off values is noticed for the OB stars although no such
deviation is seen for the YOCs. We also determined scale heights of
56.9(+3.8)(-3.4} and 61.4(+2.7)(-2.4) pc for the distribution of YOCs and OB
stars respectively.
|
2024-08-12T18:16:26.647752 | 2007-04-08T00:58:26 | 0704.0951 | {
"authors": "J. A. Hoyos, Andr\\'e P. Vieira, Nicolas Laflorencie, E. Miranda",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:951",
"submitter": "Jos\\'e Abel Hoyos Neto",
"url": "https://arxiv.org/abs/0704.0951"
} | arxiv-abstracts | Using strong-disorder renormalization group, numerical exact diagonalization,
and quantum Monte Carlo methods, we revisit the random antiferromagnetic XXZ
spin-1/2 chain focusing on the long-length and ground-state behavior of the
average time-independent spin-spin correlation function C(l)=\upsilon
l^{-\eta}. In addition to the well-known universal (disorder-independent)
power-law exponent \eta=2, we find interesting universal features displayed by
the prefactor \upsilon=\upsilon_o/3, if l is odd, and \upsilon=\upsilon_e/3,
otherwise. Although \upsilon_o and \upsilon_e are nonuniversal (disorder
dependent) and distinct in magnitude, the combination \upsilon_o + \upsilon_e =
-1/4 is universal if C is computed along the symmetric (longitudinal) axis. The
origin of the nonuniversalities of the prefactors is discussed in the
renormalization-group framework where a solvable toy model is considered.
Moreover, we relate the average correlation function with the average
entanglement entropy, whose amplitude has been recently shown to be universal.
The nonuniversalities of the prefactors are shown to contribute only to surface
terms of the entropy. Finally, we discuss the experimental relevance of our
results by computing the structure factor whose scaling properties,
interestingly, depend on the correlation prefactors.
|
2024-08-12T18:16:26.647851 | 2007-04-06T21:37:52 | 0704.0952 | {
"authors": "M. Shao (JPL), G. Marcy (Univ. California), S. Unwin (JPL), R. Allen\n (STScI), C. Beichman (MSC/Caltech), J. Catanzarite (JPL), B. Chaboyer\n (Dartmouth), D. Ciardi (MSC/Caltech), S. J. Edberg (JPL), D. Gallagher (JPL),\n A. Gould (Ohio State), T. Henry (Georgia State), K. Johnston (USNO), S.\n Kulkarni (Caltech), N. Law (Caltech), S. Majewski (Univ. Virginia), J. Marr\n (JPL), N. Law (JPL), X. Pan (JPL), S. Shaklan (JPL), E. Shaya (Univ.\n Maryland), A. Tanner (JPL), J. Tomsick (Univ. California), A. Wehrle (Space\n Sci Inst), G. Worthey (Washington State Univ)",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:952",
"submitter": "Joseph Catanzarite",
"url": "https://arxiv.org/abs/0704.0952"
} | arxiv-abstracts | The past two Decadal Surveys in Astronomy and Astrophysics recommended the
completion of a space-based interferometry mission, known today as SIM
PlanetQuest, for its unique ability to detect and characterize nearby rocky
planets (Bahcall 1991, McKee & Taylor 2001), as well as contributions to a
broad range of problems in astrophysics. Numerous committees of the National
Research Council as well as NASA Roadmaps have similarly highlighted SIM as the
one technology that offers detection and characterization of rocky planets
around nearby stars and which is technically ready. To date, SIM remains the
only program with the capability of detecting and confirming rocky planets in
the habitable zones of nearby solar-type stars. Moreover, SIM measures masses
and three-dimensional orbits of habitable planets around nearby stars (within
25 pc); these are the only stars for which follow-up by other techniques is
feasible, such as space-based spectroscopy, ground-based interferometry, and of
course TPF.
|
2024-08-12T18:16:26.647936 | 2007-04-06T21:52:09 | 0704.0953 | {
"authors": "Lei Bai, Delphine Marcillac, George H. Rieke, Marcia J. Rieke, Kim-Vy\n H. Tran, Joannah L. Hinz, Gregory Rudnick, Douglas M. Kelly, Myra Blaylock",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:953",
"submitter": "Lei Bai",
"url": "https://arxiv.org/abs/0704.0953"
} | arxiv-abstracts | We study the infrared (IR) properties of galaxies in the cluster MS 1054-03
at z=0.83 by combining MIPS 24 micron data with spectra of more than 400
galaxies and a very deep K-band selected catalog. 19 IR cluster members are
selected spectroscopically, and an additional 15 are selected by their
photometric redshifts. We derive the IR luminosity function of the cluster and
find strong evolution compared to the similar-mass Coma cluster. The best
fitting Schechter function gives L*_{IR}=11.49 +0.30/-0.29 L_sun with a fixed
faint end slope, about one order of magnitude larger than that in Coma. The
rate of evolution of the IR luminosity from Coma to MS 1054-03 is consistent
with that found in field galaxies, and it suggests that some internal
mechanism, e.g., the consumption of the gas fuel, is responsible for the
general decline of the cosmic star formation rate (SFR) in different
environments. The mass-normalized integrated SFR within 0.5R_200 in MS 1054-03
also shows evolution compared with other rich clusters at lower redshifts, but
the trend is less conclusive if the mass selection effect is considered. A
nonnegligible fraction (13%) of cluster members, are forming stars actively and
the overdensity of IR galaxies is about 20 compared to the field. It is
unlikely that clusters only passively accrete star forming galaxies from the
surrounding fields and have their star formation quenched quickly afterward;
instead, many cluster galaxies still have large amounts of gas, and their star
formation may be enhanced by the interaction with the cluster.
|
2024-08-12T18:16:26.648037 | 2007-04-06T21:58:52 | 0704.0954 | {
"authors": "Soummya Kar and Jose M. F. Moura",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:954",
"submitter": "Jos\\'e M. F. Moura",
"url": "https://arxiv.org/abs/0704.0954"
} | arxiv-abstracts | In a sensor network, in practice, the communication among sensors is subject
to:(1) errors or failures at random times; (3) costs; and(2) constraints since
sensors and networks operate under scarce resources, such as power, data rate,
or communication. The signal-to-noise ratio (SNR) is usually a main factor in
determining the probability of error (or of communication failure) in a link.
These probabilities are then a proxy for the SNR under which the links operate.
The paper studies the problem of designing the topology, i.e., assigning the
probabilities of reliable communication among sensors (or of link failures) to
maximize the rate of convergence of average consensus, when the link
communication costs are taken into account, and there is an overall
communication budget constraint. To consider this problem, we address a number
of preliminary issues: (1) model the network as a random topology; (2)
establish necessary and sufficient conditions for mean square sense (mss) and
almost sure (a.s.) convergence of average consensus when network links fail;
and, in particular, (3) show that a necessary and sufficient condition for both
mss and a.s. convergence is for the algebraic connectivity of the mean graph
describing the network topology to be strictly positive. With these results, we
formulate topology design, subject to random link failures and to a
communication cost constraint, as a constrained convex optimization problem to
which we apply semidefinite programming techniques. We show by an extensive
numerical study that the optimal design improves significantly the convergence
speed of the consensus algorithm and can achieve the asymptotic performance of
a non-random network at a fraction of the communication cost.
|
2024-08-12T18:16:26.648137 | 2007-04-07T20:03:07 | 0704.0955 | {
"authors": "Nemani V. Suryanarayana and Matthias C. Wapler",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:955",
"submitter": "Matthias Wapler",
"url": "https://arxiv.org/abs/0704.0955"
} | arxiv-abstracts | We describe how to recover the quantum numbers of extremal black holes from
their near horizon geometries. This is achieved by constructing the
gravitational Noether-Wald charges which can be used for non-extremal black
holes as well. These charges are shown to be equivalent to the U(1) charges of
appropriately dimensionally reduced solutions. Explicit derivations are
provided for 10 dimensional type IIB supergravity and 5 dimensional minimal
gauged supergravity, with illustrative examples for various black hole
solutions. We also discuss how to derive the thermodynamic quantities and their
relations explicitly in the extremal limit, from the point of view of the
near-horizon geometry. We relate our results to the entropy function formalism.
|
2024-08-12T18:16:26.648192 | 2007-04-06T22:16:53 | 0704.0956 | {
"authors": "Tanmoy Das, R. S. Markiewicz, A. Bansil",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:956",
"submitter": "Tanmoy Das",
"url": "https://arxiv.org/abs/0704.0956"
} | arxiv-abstracts | We have investigated the doping dependence of the penetration depth vs.
temperature in electron doped Pr$_{2-x}$Ce$_x$CuO$_{4-\delta}$ using a model
which assumes the uniform coexistence of (mean-field) antiferromagnetism and
superconductivity. Despite the presence of a $d_{x^2-y^2}$ pairing gap in the
underlying spectrum, we find nodeless behavior of the low-$T$ penetration depth
in underdoped case, in accord with experimental results. As doping increases, a
linear-in-$T$ behavior of the penetration depth, characteristic of d-wave
pairing, emerges as the lower magnetic band crosses the Fermi level and creates
a nodal Fermi surface pocket.
|
2024-08-12T18:16:26.648242 | 2007-04-06T22:20:54 | 0704.0957 | {
"authors": "Soumik Pal and Jim Pitman",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:957",
"submitter": "Soumik Pal",
"url": "https://arxiv.org/abs/0704.0957"
} | arxiv-abstracts | We study interacting systems of linear Brownian motions whose drift vector at
every time point is determined by the relative ranks of the coordinate
processes at that time. Our main objective has been to study the long range
behavior of the spacings between the Brownian motions arranged in increasing
order. For finitely many Brownian motions interacting in this manner, we
characterize drifts for which the family of laws of the vector of spacings is
tight, and show its convergence to a unique stationary joint distribution given
by independent exponential distributions with varying means. We also study one
particular countably infinite system, where only the minimum Brownian particle
gets a constant upward drift, and prove that independent and identically
distributed exponential spacings remain stationary under the dynamics of such a
process. Some related conjectures in this direction have also been discussed.
|
2024-08-12T18:16:26.648313 | 2007-04-06T22:28:14 | 0704.0958 | {
"authors": "E. Pian (1), P. Romano (2,3), A. Treves (4), G. Ghisellini (2), S.\n Covino (2), A. Cucchiara (5), A. Dolcini (4), G. Tagliaferri (2), C.\n Markwardt (6), S. Campana (2), G. Chincarini (2,3), N. Gehrels (6), P. Giommi\n (7), L. Maraschi (8), S.D. Vergani (9,10), F.M. Zerbi (2), E. Molinari (2),\n V. Testa (11), G. Tosti (12), F. Vitali (11), L.A. Antonelli (11), P. Conconi\n (2), G. Malaspina (2), L. Nicastro (13), E. Palazzi (13), E.J.A. Meurs (9),\n L. Norci (10) ((1) INAF-Trieste, (2) INAF-Brera/Merate, (3) Univ.\n Milano-Bicocca, (4) Univ. Insubria, (5) Penn State, (6) GSFC-NASA, (7) ASI\n ASDC, (8) INAF-Brera/Milano, (9) Dunsink Obs., (10) School of Physical\n Sciences and NCPST, Dublin, (11) INAF-Rome, (12) Univ. Perugia, (13)\n INAF-IASF/Bologna)",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:958",
"submitter": "Elena Pian",
"url": "https://arxiv.org/abs/0704.0958"
} | arxiv-abstracts | The blazar PKS0537-441 has been observed by Swift between the end of 2004 and
November 2005. The BAT monitored it recurrently for a total of 2.7 Ms, and the
XRT and UVOT pointed it on seven occasions for a total of 67 ks, making it one
of the AGNs best monitored by Swift. The automatic optical and infrared
telescope REM has monitored simultaneously the source at all times. In
January-February 2005 PKS0537-441 has been detected at its brightest in optical
and X-rays: more than a factor of 2 brighter in X-rays and about a factor 60
brighter in the optical than observed in December 2004. The July 2005
observation recorded a fainter X-ray state. The simultaneous optical state,
monitored by both Swift UVOT and REM, is high, and in the VRI bands it is
comparable to what was recorded in early January 2005, before the outburst. In
November 2005, the source subsided both in X-rays and optical to a quiescent
state, having decreased by factors of ~4 and ~60 with respect to the
January-February 2005 outburst, respectively. Our monitoring shows an overall
well correlated optical and X-ray decay. On the shorter time scales (days or
hours), there is no obvious correlation between X-ray and optical variations,
but the former tend to be more pronounced, opposite to what is observed on
monthly time scales. The widely different amplitude of the long term
variability in optical and X-rays is very unusual and makes this observation a
unique case study for blazar activity. The spectral energy distributions are
interpreted in terms of the synchrotron and inverse Compton mechanisms within a
jet where the plasma radiates via internal shocks and the dissipation depends
on the distance of the emitting region from the central engine (abridged).
|
2024-08-12T18:16:26.648433 | 2007-04-06T23:22:54 | 0704.0959 | {
"authors": "Takumi Doi (Kentucky U., Riken BNL)",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:959",
"submitter": "Takumi Doi",
"url": "https://arxiv.org/abs/0704.0959"
} | arxiv-abstracts | We review the current status of the theoretical pentaquark search from the
direct QCD calculation. The works from the QCD sum rule and the lattice QCD in
the literature are carefully examined. The importance of the framework which
can distinguish the exotic pentaquark state (if any) from the NK scattering
state is emphasized.
|
2024-08-12T18:16:26.648481 | 2007-04-07T00:32:46 | 0704.0960 | {
"authors": "Wen Yi Huo and Gui Lu Long",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:960",
"submitter": "Gui Lu Long",
"url": "https://arxiv.org/abs/0704.0960"
} | arxiv-abstracts | We propose a scheme for generating squeezed states in solid state circuits
consisting of a nanomechanical resonator (NMR), a superconducting Cooper-pair
box (CPB) and a superconducting transmission line resonator (STLR). The
nonlinear interaction between the NMR and the STLR can be implemented by
setting the external biased flux of the CPB at certain values. The interaction
Hamiltonian between the NMR and the STLR is derived by performing Fr$\rm\ddot
o$hlich transformation on the total Hamiltonian of the combined system. Just by
adiabatically keeping the CPB at the ground state, we get the standard
parametric down-conversion Hamiltonian. The CPB plays the role of ``nonlinear
media", and the squeezed states of the NMR can be easily generated in a manner
similar to the three-wave mixing in quantum optics. This is the three-wave
mixing in a solid-state circuit.
|
2024-08-12T18:16:26.648548 | 2007-04-07T01:37:57 | 0704.0961 | {
"authors": "G. H. Tovmassian (1), S.V. Zharikov (1) ((1) Instituto de Astronomia,\n Universidad Nacional Autonoma de Mexico, Ensenada, Mexico)",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:961",
"submitter": "Sergei Zharikov",
"url": "https://arxiv.org/abs/0704.0961"
} | arxiv-abstracts | Context: The object HS 0922+1333 was visited briefly in 2002 in a mini survey
of low accretion rate polars (LARPs) in order to test if they undergo high
luminosity states similar to ordinary polars. On the basis of that short
observation the suspicion arose that the object might be an asynchronous polar
(Tovmassian et al. 2004). The disparity between the presumed orbital and spin
period appeared to be quite unusual. Aims: We performed follow-up observations
of the object to resolve the problem. Methods: New simultaneous spectroscopic
and photometric observations spanning several years allowed measurements of
radial velocities of emission and absorption lines from the secondary star and
brightness variations due to synchrotron emission from the primary. Results:
New observations show that the object is actually synchronous and its orbital
and spin period are equal to 4.04 hours. Conclusions: We identify the source of
confusion of previous observations to be a high velocity component of emission
line arousing from the stream of matter leaving L1 point.
|
2024-08-12T18:16:26.648615 | 2007-04-07T01:51:13 | 0704.0962 | {
"authors": "Tilman Sauer",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:962",
"submitter": "Tilman Sauer",
"url": "https://arxiv.org/abs/0704.0962"
} | arxiv-abstracts | The historical significance of the problem of relativistic rigid rotation is
reviewed in light of recently published correspondence between Einstein and the
mathematician Vladimir Varicak from the years 1909 to 1913.
|
2024-08-12T18:16:26.648660 | 2007-04-07T02:07:44 | 0704.0963 | {
"authors": "Tilman Sauer",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:963",
"submitter": "Tilman Sauer",
"url": "https://arxiv.org/abs/0704.0963"
} | arxiv-abstracts | Einstein's early calculations of gravitational lensing, contained in a
scratch notebook and dated to the spring of 1912, are reexamined. A hitherto
unknown letter by Einstein suggests that he entertained the idea of explaining
the phenomenon of new stars by gravitational lensing in the fall of 1915 much
more seriously than was previously assumed. A reexamination of the relevant
calculations by Einstein shows that, indeed, at least some of them most likely
date from early October 1915. But in support of earlier historical
interpretation of Einstein's notes, it is argued that the appearance of Nova
Geminorum 1912 (DN Gem) in March 1912 may, in fact, provide a relevant context
and motivation for Einstein's lensing calculations on the occasion of his first
meeting with Erwin Freundlich during a visit in Berlin in April 1912. We also
comment on the significance of Einstein's consideration of gravitational
lensing in the fall of 1915 for the reconstruction of Einstein's final steps in
his path towards general relativity.
|
2024-08-12T18:16:26.648728 | 2007-04-09T03:16:17 | 0704.0964 | {
"authors": "Sergey Bravyi",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:964",
"submitter": "Sergey Bravyi",
"url": "https://arxiv.org/abs/0704.0964"
} | arxiv-abstracts | We discuss upper bounds on the rate at which unitary evolution governed by a
non-local Hamiltonian can generate entanglement in a bipartite system. Given a
bipartite Hamiltonian H coupling two finite dimensional particles A and B, the
entangling rate is shown to be upper bounded by c*log(d)*norm(H), where d is
the smallest dimension of the interacting particles, norm(H) is the operator
norm of H, and c is a constant close to 1. Under certain restrictions on the
initial state we prove analogous upper bound for the ancilla-assisted
entangling rate with a constant c that does not depend upon dimensions of local
ancillas. The restriction is that the initial state has at most two distinct
Schmidt coefficients (each coefficient may have arbitrarily large
multiplicity). Our proof is based on analysis of a mixing rate -- a functional
measuring how fast entropy can be produced if one mixes a time-independent
state with a state evolving unitarily.
|
2024-08-12T18:16:26.648790 | 2007-04-07T02:40:13 | 0704.0965 | {
"authors": "Zongwen Yu and Su Hu",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:965",
"submitter": "Yu Zongwen",
"url": "https://arxiv.org/abs/0704.0965"
} | arxiv-abstracts | In this paper, we give out some effective criterions which can be used to
judge the separability of multipartite pure states. We obtain the relationship
between separability and Schmidt decomposable of multipartite pure states in
Theorem1. The first criterion derived from Theorem2 dose not need the Schmidt
decomposition which is hard to find for multipartite states. Theorem3 is more
profound which can be used to deduce Corollary1 which is one of the main
results in [1]. Finally, we give out an algorithm which can be used to judge
the separability of multipartite pure states effectively.
|
2024-08-12T18:16:26.648838 | 2007-04-07T02:48:27 | 0704.0966 | {
"authors": "B.Alver, et al, the PHOBOS Collaboration",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:966",
"submitter": "Wei Li",
"url": "https://arxiv.org/abs/0704.0966"
} | arxiv-abstracts | We present results on two-particle angular correlations in proton-proton
collisions at center of mass energies of 200 and 410 GeV. The PHOBOS experiment
at the Relativistic Heavy Ion Collider has a uniquely large coverage for
charged particles, giving the opportunity to explore the correlations at both
short- and long-range scales. At both energies, a complex two-dimensional
correlation structure in $\Delta \eta$ and $\Delta \phi$ is observed. In the
context of an independent cluster model of short-range correlations, the
cluster size and its decay width are extracted from the two-particle
pseudorapidity correlation function and compared with previous measurements in
proton-proton and proton-antiproton collisions, as well as PYTHIA and HIJING
predictions.
|
2024-08-12T18:16:26.648899 | 2007-04-07T03:18:46 | 0704.0967 | {
"authors": "Jia Liu and Y. Thomas Hou",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:967",
"submitter": "Jia Liu",
"url": "https://arxiv.org/abs/0704.0967"
} | arxiv-abstracts | MIMO technology is one of the most significant advances in the past decade to
increase channel capacity and has a great potential to improve network capacity
for mesh networks. In a MIMO-based mesh network, the links outgoing from each
node sharing the common communication spectrum can be modeled as a Gaussian
vector broadcast channel. Recently, researchers showed that ``dirty paper
coding'' (DPC) is the optimal transmission strategy for Gaussian vector
broadcast channels. So far, there has been little study on how this fundamental
result will impact the cross-layer design for MIMO-based mesh networks. To fill
this gap, we consider the problem of jointly optimizing DPC power allocation in
the link layer at each node and multihop/multipath routing in a MIMO-based mesh
networks. It turns out that this optimization problem is a very challenging
non-convex problem. To address this difficulty, we transform the original
problem to an equivalent problem by exploiting the channel duality. For the
transformed problem, we develop an efficient solution procedure that integrates
Lagrangian dual decomposition method, conjugate gradient projection method
based on matrix differential calculus, cutting-plane method, and subgradient
method. In our numerical example, it is shown that we can achieve a network
performance gain of 34.4% by using DPC.
|
2024-08-12T18:16:26.648980 | 2007-04-07T03:07:06 | 0704.0968 | {
"authors": "Cheongho Han (Chunguk Natl. Univ.)",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:968",
"submitter": "Cheongho Han",
"url": "https://arxiv.org/abs/0704.0968"
} | arxiv-abstracts | To provide criteria in the selection of target events preferable for
planetary lensing follow-up observations, we investigate the variation of the
probability of detecting planetary signals depending on the observables of the
lensing magnification and source brightness. In estimating the probability, we
consider variation of the photometric precision by using a quantity defined as
the ratio of the fractional deviation of the planetary perturbation to the
photometric precision. From this investigation, we find consistent result from
previous studies that the probability increases with the increase of the
magnification. The increase rate is boosted at a certain magnification at which
perturbations caused by central caustic begin to occur. We find this boost
occurs at moderate magnifications of $A\lesssim 20$, implying that probability
can be high even for events with moderate magnifications. The probability
increases as the source brightness increases. We find that the probability of
events associated with stars brighter than clump giants is not negligible even
at magnifications as low as $A\sim 5$. In the absence of rare the prime target
of very high-magnification events, we, therefore, recommend to observe events
with brightest source stars and highest magnifications among the alerted
events. Due to the increase of the source size with the increase of the
brightness, however, the probability rapidly drops off beyond a certain
magnification, causing detections of low mass ratio planets ($q\lesssim
10^{-4}$) difficult from the observations of events involved with giant stars
with magnifications $A\gtrsim 70$.
|
2024-08-12T18:16:26.649073 | 2007-04-07T03:20:51 | 0704.0969 | {
"authors": "Su Hu and Zongwen Yu",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:969",
"submitter": "Hu Su",
"url": "https://arxiv.org/abs/0704.0969"
} | arxiv-abstracts | In this paper, we present the necessary and sufficient conditions of
separability for bipartite pure states in infinite dimensional Hilbert spaces.
Let $M$ be the matrix of the amplitudes of $\ket\psi$, we prove $M$ is a
compact operator. We also prove $\ket\psi$ is separable if and only if $M$ is a
bounded linear operator with rank 1, that is the image of $M$ is a one
dimensional Hilbert space. So we have related the separability for bipartite
pure states in infinite dimensional Hilbert spaces to an important class of
bounded linear operators in Functional analysis which has many interesting
properties.
|
2024-08-12T18:16:26.649123 | 2007-04-07T04:41:23 | 0704.0970 | {
"authors": "Mark Wardle (Macquarie University)",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:970",
"submitter": "Mark Wardle",
"url": "https://arxiv.org/abs/0704.0970"
} | arxiv-abstracts | Magnetic fields likely play a key role in the dynamics and evolution of
protoplanetary discs. They have the potential to efficiently transport angular
momentum by MHD turbulence or via the magnetocentrifugal acceleration of
outflows from the disk surface, and magnetically-driven mixing has implications
for disk chemistry and evolution of the grain population. However, the weak
ionisation of protoplanetary discs means that magnetic fields may not be able
to effectively couple to the matter. I present calculations of the ionisation
equilibrium and magnetic diffusivity as a function of height from the disk
midplane at radii of 1 and 5 AU. Dust grains tend to suppress magnetic coupling
by soaking up electrons and ions from the gas phase and reducing the
conductivity of the gas by many orders of magnitude. However, once grains have
grown to a few microns in size their effect starts to wane and magnetic fields
can begin to couple to the gas even at the disk midplane. Because ions are
generally decoupled from the magnetic field by neutral collisions while
electrons are not, the Hall effect tends to dominate the diffusion of the
magnetic field when it is able to partially couple to the gas.
For a standard population of 0.1 micron grains the active surface layers have
a combined column of about 2 g/cm^2 at 1 AU; by the time grains have aggregated
to 3 microns the active surface density is 80 g/cm^2. In the absence of grains,
x-rays maintain magnetic coupling to 10% of the disk material at 1 AU (150
g/cm^2). At 5 AU the entire disk thickness becomes active once grains have
aggregated to 1 micron in size.
|
2024-08-12T18:16:26.649220 | 2007-04-07T06:53:26 | 0704.0971 | {
"authors": "Zhi-zhong Xing and Shun Zhou",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:971",
"submitter": "Shun Zhou",
"url": "https://arxiv.org/abs/0704.0971"
} | arxiv-abstracts | The noteworthy BaBar and Belle evidence for $D^0$-$\bar{D}^0$ mixing
motivates us to study its impact on $D^0\to K^{*\pm} K^\mp$ decays and their
CP-conjugate processes. We show that both the $D^0$-$\bar{D}^0$ mixing
parameters ($x$ and $y$) and the strong phase difference between $\bar{D}^0\to
K^{*\pm}K^\mp$ and $D^0\to K^{*\pm}K^\mp$ transitions ($\delta$) can be
determined or constrained from the time-dependent measurements of these decay
modes. On the $\psi (3770)$ and $\psi (4140)$ resonances at a $\tau$-charm
factory, it is even possible to determine or constrain $x$, $y$ and $\delta$
from the time-independent measurements of coherent $(D^0\bar{D}^0) \to
(K^{*\pm} K^\mp)(K^{*\pm} K^\mp)$ decays. If the CP-violating phase of
$D^0$-$\bar{D}^0$ mixing is significant in a scenario beyond the standard
model, it can also be extracted from the $K^{*\pm} K^\mp$ events.
|
2024-08-12T18:16:26.649278 | 2007-04-07T05:30:11 | 0704.0972 | {
"authors": "Fedor V.Prigara",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:972",
"submitter": "Fedor V. Prigara",
"url": "https://arxiv.org/abs/0704.0972"
} | arxiv-abstracts | Based on the formula for the number density of vacancies in a solid under the
stress or tension, the model of grain boundary diffusion in crystalline solids
is developed. We obtain the activation energy of grain boundary diffusion
(dependent on the surface tension or the energy of the grain boundary) and also
the distributions of vacancies and the diffusing species in the vicinity of the
grain boundary.
|
2024-08-12T18:16:26.649324 | 2007-04-07T07:24:41 | 0704.0973 | {
"authors": "Fangjun Lu, Q.Daniel Wang, E. V. Gotthelf, and Jinlu Qu",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:973",
"submitter": "Fangjun Lu",
"url": "https://arxiv.org/abs/0704.0973"
} | arxiv-abstracts | We present new X-ray timing and spectral observations of PSR J1930+1852, the
young energetic pulsar at the center of the non-thermal supernova remnant
G54.1+0.3. Using data obtained with the Rossi X-ray Timing Explorer and Chandra
X-ray observatories we have derived an updated timing ephemeris of the 136 ms
pulsar spanning 6 years. During this interval, however, the period evolution
shows significant variability from the best fit constant spin-down rate of
$\dot P = 7.5112(6) \times 10^{-13}$ s s$^{-1}$, suggesting strong timing noise
and/or glitch activity. The X-ray emission is highly pulsed ($71\pm5%$
modulation) and is characterized by an asymmetric, broad profile ($\sim 70%$
duty cycle) which is nearly twice the radio width. The spectrum of the pulsed
emission is well fitted with an absorbed power law of photon index $\Gamma =
1.2\pm0.2$; this is marginally harder than that of the unpulsed component. The
total 2-10 keV flux of the pulsar is $1.7 \times 10^{-12}$ erg cm$^{-2}$
s$^{-1}$. These results confirm PSR J1930+1852 as a typical Crab-like pulsar.
|
2024-08-12T18:16:26.649418 | 2007-04-07T07:56:25 | 0704.0974 | {
"authors": "Hikaru Kawamura and Atsushi Yamamoto",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:974",
"submitter": "Hikaru Kawamura",
"url": "https://arxiv.org/abs/0704.0974"
} | arxiv-abstracts | The ordering of the classical Heisenberg antiferromagnet on the triangular
lattice with the the bilinear-biquadratic interaction is studied by Monte Carlo
simulations. It is shown that the model exhibits a topological phase transition
at a finite-temperature driven by topologically stable vortices, while the spin
correlation length remains finite even at and below the transition point. The
relevant vortices could be of three different types, depending on the value of
the biquadratic coupling. Implications to recent experiments on the triangular
antiferromagnet NiGa$_2$S$_4$ is discussed.
|
2024-08-12T18:16:26.649475 | 2007-04-07T08:37:36 | 0704.0975 | {
"authors": "A. Sarkar, Charles L. Webber Jr., P. Barat, P. Mukherjee",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:975",
"submitter": "Apu Sarkar",
"url": "https://arxiv.org/abs/0704.0975"
} | arxiv-abstracts | Tensile tests were carried out by deforming polycrystalline samples of
Al-2.5%Mg alloy at room temperature in a wide range of strain rates where the
Portevin-Le Chatelier (PLC) effect was observed. The experimental stress-time
series data have been analyzed using the recurrence analysis technique based on
the Recurrence Plot (RP) and the Recurrence Quantification Analysis (RQA) to
study the change in the dynamical behavior of the PLC effect with the imposed
strain rate. Our study revealed that the RQA is able to detect the unique
crossover phenomenon in the PLC dynamics.
|
2024-08-12T18:16:26.649526 | 2007-04-07T08:40:38 | 0704.0976 | {
"authors": "Jean-Pierre Eckmann",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:976",
"submitter": "J.-P. Eckmann",
"url": "https://arxiv.org/abs/0704.0976"
} | arxiv-abstracts | We propose and study a model with glassy behavior. The state space of the
model is given by all triangulations of a sphere with $n$ nodes, half of which
are red and half are blue. Red nodes want to have 5 neighbors while blue ones
want 7. Energies of nodes with different numbers of neighbors are supposed to
be positive. The dynamics is that of flipping the diagonal of two adjacent
triangles, with a temperature dependent probability. We show that this system
has an approach to a steady state which is exponentially slow, and show that
the stationary state is unordered. We also study the local energy landscape and
show that it has the hierarchical structure known from spin glasses. Finally,
we show that the evolution can be described as that of a rarefied gas with
spontaneous generation of particles and annihilating collisions.
|
2024-08-12T18:16:26.649588 | 2007-04-07T08:53:17 | 0704.0977 | {
"authors": "Wei Yang, Ru-Zhi Wang, Yu-Fang Wang, Xue-Mei Song, Bo Wang, Hui Yan",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:977",
"submitter": "RuZhi Wang",
"url": "https://arxiv.org/abs/0704.0977"
} | arxiv-abstracts | Using the molecular dynamics simulations and the force constant model we have
studied the Raman-active tangential modes (TMs) of a (10, 0) single-wall carbon
nanotube (SWNT) under hydrostatic pressure. With increasing pressure, the
atomic motions in the three TMs present obvious diversities. The pressure
derivative of E1g, A1g, and E2g mode frequency shows an increased value (), a
constant value (), and a negative value () above 5.3 GPa, respectively. The
intrinsic characteristics of TMs consumedly help to understand the essence of
the experimental T band of CNT. The anomalous pressure behavior of the TMs
frequencies may be originated from the tube symmetry alteration from D10h to
D2h then to C2h.
|
2024-08-12T18:16:26.649650 | 2007-04-07T09:09:23 | 0704.0978 | {
"authors": "S. Muller, M. Guelin, F. Combes, T. Wiklind",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:978",
"submitter": "Sebastien Muller",
"url": "https://arxiv.org/abs/0704.0978"
} | arxiv-abstracts | The line of sight to the quasar B0218+357, one of the most studied lensed
systems, intercepts a z=0.68 spiral galaxy, which splits its image into two
main components A and B, separated by ca. 0.3'', and gives rise to molecular
absorption. Although the main absorption component has been shown to arise in
front of image A, it is not established whether some absorption from other
velocity components is also occuring in front of image B. To tackle this
question, we have observed the HCO+(2-1) absorption line during the
commissioning phase of the new very extended configuration of the Plateau de
Bure Interferometer, in order to trace the position of the absorption as a
function of frequency. Visibility fitting of the self-calibrated data allowed
us to achieve position accuracy between ~12 and 80 mas per velocity component.
Our results clearly demonstrate that all the different velocity components of
the HCO+(2-1) absorption arise in front of the south-west image A of the
quasar. We estimate a flux ratio fA/fB = 4.2 (-1.0;+1.8 at 106 GHz.
|
2024-08-12T18:16:26.649729 | 2007-04-07T10:48:57 | 0704.0979 | {
"authors": "Hajime Takami, Kohta Murase, Shigehiro Nagataki, and Katsuhiko Sato",
"full_text_license": "arXiv.org - Non-exclusive license to distribute - http://arxiv.org/licenses/nonexclusive-distrib/1.0/",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:979",
"submitter": "Hajime Takami",
"url": "https://arxiv.org/abs/0704.0979"
} | arxiv-abstracts | There are two promising scenarios that explain the ankle, which is a dip in
the spectrum of cosmic rays at $\sim 10^{19}$ eV. A scenario interprets the
ankle as the transition from Galactic to extragalactic cosmic rays ({\it
ankle-transition scenario}), while the other is that the dip caused by pair
production on the cosmic microwave background radiation ({\it proton-dip
scenario}). In this paper, we consider whether cosmogenic neutrinos can be a
clue to judge which scenario is favored. We calculated the fluxes of cosmogenic
neutrinos following these scenarios with plausible physical parameter sets, and
found several important features as follows. First of all, the neutrino flux at
$\sim 10^{20}$ eV becomes much higher in the ankle-transition scenario as long
as the maximum energy of the cosmic rays at sources is sufficiently high. On
the other hand, the neutrino spectrum has a characteristic peak at $\sim
10^{16}$ eV in the proton-dip scenario on the condition that extragalactic
protons significantly contribute to the observed cosmic rays down to $10^{17}$
eV. Thus, we conclude cosmogenic neutrinos should give us a clue to judge which
scenario is favored, unless these features are masked by the neutrino
background coming from possible, powerful neutrino sources such as AGNs and
GRBs. We also found an interesting feature that the neutrino flux at $\sim
10^{18}$ eV depends only on the cosmological evolution of the cosmic ray
sources. That means cosmogenic neutrinos with the energy bring us information
on the cosmological evolution of the sources of ultra-high energy cosmic rays.
Finally, we compare the fluxes of cosmogenic neutrinos with the expected
sensitivity curves of several neutrino detectors, and conclude the detection of
cosmogenic neutrinos in the near future is promising.
|
2024-08-12T18:16:26.649824 | 2007-04-07T11:27:29 | 0704.0980 | {
"authors": "A. Pfund, I. Shorubalko, K. Ensslin, R. Leturcq",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:980",
"submitter": "Renaud Leturcq",
"url": "https://arxiv.org/abs/0704.0980"
} | arxiv-abstracts | We quantify the contributions of hyperfine and spin-orbit mediated
singlet-triplet mixing in weakly coupled InAs quantum dots by electron
transport spectroscopy in the Pauli spin blockade regime. In contrast to double
dots in GaAs, the spin-orbit coupling is found to be more than two orders of
magnitudes larger than the hyperfine mixing energy. It is already effective at
magnetic fields of a few mT, where deviations from hyperfine mixing are
observed.
|
2024-08-12T18:16:26.649873 | 2007-04-07T12:06:05 | 0704.0981 | {
"authors": "Xuan Hien Nguyen",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:981",
"submitter": "Xuan Hien Nguyen",
"url": "https://arxiv.org/abs/0704.0981"
} | arxiv-abstracts | We study the Dirichlet problem associated to the equation for self-similar
surfaces for graphs over the Euclidean plane with a disk removed. We show the
existence of a solution provided the boundary conditions on the boundary circle
are small enough and satisfy some symmetries. This is the second step towards
the construction of new examples of complete embedded self similar surfaces
under mean curvature flow.
|
2024-08-12T18:16:26.649920 | 2007-04-09T11:54:10 | 0704.0982 | {
"authors": "Edward M. Drobyshevski and Mikhail E. Drobyshevski",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:982",
"submitter": "Edward M. Drobyshevski",
"url": "https://arxiv.org/abs/0704.0982"
} | arxiv-abstracts | The assumption of the capture by the Solar System of the electrically charged
Planckian DM objects (daemons) from the galactic disk is confirmed not only by
the St.Petersburg (SPb) experiments detecting particles with V<30 km/s. Here
the daemon approach is analyzed considering the positive model independent
result of the DAMA/NaI experiment. We explain the maximum in DAMA signals
observed in the May-June period to be associated with the formation behind the
Sun of a trail of daemons that the Sun captures into elongated orbits as it
moves to the apex. The range of significant 2-6-keV DAMA signals fits well the
iodine nuclei elastically knocked out of the NaI(Tl) scintillator by particles
falling on the Earth with V=30-50 km/s from strongly elongated heliocentric
orbits. The half-year periodicity of the slower daemons observed in SPb
originates from the transfer of particles that are deflected through ~90 deg
into near-Earth orbits each time the particles cross the outer reaches of the
Sun which had captured them. Their multi-loop (cross-like) trajectories
traverse many times the Earth's orbit in March and September, which increases
the probability for the particles to enter near-Earth orbits during this time.
Corroboration of celestial mechanics calculations with observations yields
~1e-19 cm2 for the cross section of daemon interaction with the solar matter.
|
2024-08-12T18:16:26.650171 | 2007-04-07T12:13:36 | 0704.0983 | {
"authors": "S. M. Gerasyuta, M. A. Durnev",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:983",
"submitter": "Michael Durnev",
"url": "https://arxiv.org/abs/0704.0983"
} | arxiv-abstracts | The electromagnetic form factors of the exotic baryons are calculated in the
framework of the relativistic quark model at small and intermediate momentum
transfer. The charge radii of the E+++ baryons are determined.
|
2024-08-12T18:16:26.650211 | 2007-04-09T19:00:30 | 0704.0984 | {
"authors": "Sougato Bose, Dimitris G. Angelakis, Daniel Burgarth",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:984",
"submitter": "Dimitris G. Angelakis",
"url": "https://arxiv.org/abs/0704.0984"
} | arxiv-abstracts | We demonstrate a scheme for quantum communication between the ends of an
array of coupled cavities. Each cavity is doped with a single two level system
(atoms or quantum dots) and the detuning of the atomic level spacing and
photonic frequency is appropriately tuned to achieve photon blockade in the
array. We show that in such a regime, the array can simulate a dual rail
quantum state transfer protocol where the arrival of quantum information at the
receiving cavity is heralded through a fluorescence measurement. Communication
is also possible between any pair of cavities of a network of connected
cavities.
|
2024-08-12T18:16:26.650261 | 2007-04-07T13:40:49 | 0704.0985 | {
"authors": "Mohd Abubakr, R.M.Vinay",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:985",
"submitter": "Mohd Abubakr",
"url": "https://arxiv.org/abs/0704.0985"
} | arxiv-abstracts | Advances in semiconductor technology are contributing to the increasing
complexity in the design of embedded systems. Architectures with novel
techniques such as evolvable nature and autonomous behavior have engrossed lot
of attention. This paper demonstrates conceptually evolvable embedded systems
can be characterized basing on acausal nature. It is noted that in acausal
systems, future input needs to be known, here we make a mechanism such that the
system predicts the future inputs and exhibits pseudo acausal nature. An
embedded system that uses theoretical framework of acausality is proposed. Our
method aims at a novel architecture that features the hardware evolability and
autonomous behavior alongside pseudo acausality. Various aspects of this
architecture are discussed in detail along with the limitations.
|
2024-08-12T18:16:26.650327 | 2007-04-07T14:17:02 | 0704.0986 | {
"authors": "J. W. Maluf, F. F. Faria and S. C. Ulhoa",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:986",
"submitter": "Jos\\'e Wadih Maluf",
"url": "https://arxiv.org/abs/0704.0986"
} | arxiv-abstracts | We consider the interpretation of tetrad fields as reference frames in
spacetime. Reference frames may be characterized by an antisymmetric
acceleration tensor, whose components are identified as the inertial
accelerations of the frame (the translational acceleration and the frequency of
rotation of the frame). This tensor is closely related to
gravitoelectromagnetic field quantities. We construct the set of tetrad fields
adapted to observers that are in free fall in the Schwarzschild spacetime, and
show that the gravitational energy-momentum constructed out of this set of
tetrad fields, in the framework of the teleparallel equivalent of general
relatrivity, vanishes. This result is in agreement with the principle of
equivalence, and may be taken as a condition for a viable definition of
gravitational energy.
|
2024-08-12T18:16:26.650392 | 2007-04-07T14:51:54 | 0704.0987 | {
"authors": "C. Munoz",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:987",
"submitter": "Carlos Munoz",
"url": "https://arxiv.org/abs/0704.0987"
} | arxiv-abstracts | We review the possibility that the Supersymmetric Standard Model arises from
orbifold constructions of the E_8 x E_8 Heterotic Superstring, and the
phenomenological properties that such a model should have. In particular,
trying to solve the discrepancy between the unification scale predicted by the
Heterotic Superstring (g_{GUT}x5.27x10^{17} GeV) and the value deduced from LEP
experiments (2x10^{16} GeV), we will predict the presence at low energies of
three families of Higgses and vector-like colour triplets. Our approach relies
on the Fayet-Iliopoulos breaking, and this is also a crucial ingredient,
together with having three Higgs families, to obtain in these models an
interesting pattern of fermion masses and mixing angles at the renormalizable
lebel. Namely, after the gauge breaking some physical particles appear combined
with other states, and the Yukawa couplings are modified in a well controlled
way. On the other hand, dangerous flavour-changing neutral currents may appear
when fermions of a given charge receive their mass through couplings with
several Higgs doublets. We will address this potential problem, finding that
viable scenarios can be obtained for a reasonable light Higgs spectrum.
|
2024-08-12T18:16:26.650473 | 2007-04-07T15:11:31 | 0704.0988 | {
"authors": "C.J. Cyganowski, C.L. Brogan, T.R. Hunter",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:988",
"submitter": "Todd Hunter",
"url": "https://arxiv.org/abs/0704.0988"
} | arxiv-abstracts | S255N is a luminous far-infrared source that contains many indications of
active star formation but lacks a prominent near-infrared stellar cluster. We
present mid-infrared through radio observations aimed at exploring the
evolutionary state of this region. Our observations include 1.3mm continuum and
spectral line data from the Submillimeter Array, VLA 3.6cm continuum and 1.3cm
water maser data, and multicolor IRAC images from the Spitzer Space Telescope.
The cometary morphology of the previously-known UCHII region G192.584-0.041 is
clearly revealed in our sensitive, multi-configuration 3.6cm images. The 1.3mm
continuum emission has been resolved into three compact cores, all of which are
dominated by dust emission and have radii < 7000AU. The mass estimates for
these cores range from 6 to 35 Msun. The centroid of the brightest dust core
(SMA1) is offset by 1.1'' (2800 AU) from the peak of the cometary UCHII region
and exhibits the strongest HC3N, CN, and DCN line emission in the region. SMA1
also exhibits compact CH3OH, SiO, and H2CO emission and likely contains a young
hot core. We find spatial and kinematic evidence that SMA1 may contain further
multiplicity, with one of the components coincident with a newly-detected H2O
maser. There are no mid-infrared point source counterparts to any of the dust
cores, further suggesting an early evolutionary phase for these objects. The
dominant mid-infrared emission is a diffuse, broadband component that traces
the surface of the cometary UCHII region but is obscured by foreground material
on its southern edge. An additional 4.5 micron linear feature emanating to the
northeast of SMA1 is aligned with a cluster of methanol masers and likely
traces a outflow from a protostar within SMA1. Our observations provide direct
evidence that S255N is forming a cluster of intermediate to high-mass stars.
|
2024-08-12T18:16:26.650573 | 2007-04-09T15:35:15 | 0704.0989 | {
"authors": "Daniel Groves, Henry Wilton",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:989",
"submitter": "Henry Wilton",
"url": "https://arxiv.org/abs/0704.0989"
} | arxiv-abstracts | We prove that the set of limit groups is recursive, answering a question of
Delzant. One ingredient of the proof is the observation that a finitely
presented group with local retractions (a la Long and Reid) is coherent and,
furthermore, there exists an algorithm that computes presentations for finitely
generated subgroups. The other main ingredient is the ability to
algorithmically calculate centralizers in relatively hyperbolic groups.
Applications include the existence of recognition algorithms for limit groups
and free groups.
|
2024-08-12T18:16:26.650631 | 2007-04-07T15:41:48 | 0704.0990 | {
"authors": "Chong-Yu Ruan, Yoshie Murooka, Ramani K. Raman, Ryan A. Murdick",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:990",
"submitter": "Chong-Yu Ruan",
"url": "https://arxiv.org/abs/0704.0990"
} | arxiv-abstracts | We report the studies of ultrafast electron nanocrystallography on
size-selected Au nanoparticles (2-20 nm) supported on a molecular interface.
Reversible surface melting, melting, and recrystallization were investigated
with dynamical full-profile radial distribution functions determined with
sub-picosecond and picometer accuracies. In an ultrafast photoinduced melting,
the nanoparticles are driven to a non-equilibrium transformation, characterized
by the initial lattice deformations, nonequilibrium electron-phonon coupling,
and upon melting, the collective bonding and debonding, transforming
nanocrystals into shelled nanoliquids. The displasive structural excitation at
premelting and the coherent transformation with crystal/liquid coexistence
during photomelting differ from the reciprocal behavior of recrystallization,
where a hot lattice forms from liquid and then thermally contracts. The degree
of structural change and the thermodynamics of melting are found to depend on
the size of nanoparticle.
|
2024-08-12T18:16:26.650699 | 2007-04-09T19:25:39 | 0704.0991 | {
"authors": "Masahiko Egami",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:991",
"submitter": "Masahiko Egami",
"url": "https://arxiv.org/abs/0704.0991"
} | arxiv-abstracts | In this paper, we propose a direct solution method for optimal switching
problems of one-dimensional diffusions. This method is free from conjectures
about the form of the value function and switching strategies, or does not
require the proof of optimality through quasi-variational inequalities. The
direct method uses a general theory of optimal stopping problems for
one-dimensional diffusions and characterizes the value function as sets of the
smallest linear majorants in their respective transformed spaces.
|
2024-08-12T18:16:26.650751 | 2007-04-09T15:38:43 | 0704.0992 | {
"authors": "Elena Magliaro, Claudio Perini, Carlo Rovelli",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:992",
"submitter": "Claudio Perini",
"url": "https://arxiv.org/abs/0704.0992"
} | arxiv-abstracts | We observe that the radial gauge can be consistently imposed \emph{together}
with the Lorenz gauge in Maxwell theory, and with the harmonic traceless gauge
in linearized general relativity. This simple observation has relevance for
some recent developments in quantum gravity where the radial gauge is
implicitly utilized.
|
2024-08-12T18:16:26.650789 | 2007-04-07T17:33:44 | 0704.0993 | {
"authors": "Piotr Bizo\\'n, Tadeusz Chmaj, Andrzej Rostworowski",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:993",
"submitter": "Piotr Bizon",
"url": "https://arxiv.org/abs/0704.0993"
} | arxiv-abstracts | We study the late-time behavior of spherically symmetric solutions of the
Yang-Mills equations on Minkowski and Schwarzschild backgrounds. Using
nonlinear perturbation theory we show in both cases that solutions having
smooth compactly supported initial data posses tails which decay as $t^{-4}$ at
timelike infinity. Moreover, for small initial data on Minkowski background we
derive the third-order formula for the amplitude of the tail and confirm
numerically its accuracy.
|
2024-08-12T18:16:26.650835 | 2007-04-07T17:45:12 | 0704.0994 | {
"authors": "J.-Cl. Falmagne, S. Ovchinnikov",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:994",
"submitter": "Sergei Ovchinnikov",
"url": "https://arxiv.org/abs/0704.0994"
} | arxiv-abstracts | Any medium can be represented as an isometric subgraph of the hypercube, with
each token of the medium represented by a particular equivalence class of arcs
of the subgraph. Such a representation, although useful, is not especially
revealing of the structure of a particular medium. We propose an axiomatic
definition of the concept of a `mediatic graph'. We prove that the graph of any
medium is a mediatic graph. We also show that, for any non-necessarily finite
set S, there exists a bijection from the collection M of all the media on a
given set S (of states) onto the collection G of all the mediatic graphs on S.
|
2024-08-12T18:16:26.650891 | 2007-04-07T17:53:32 | 0704.0995 | {
"authors": "Satish D. Joglekar",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:995",
"submitter": "Satish D. Joglekar",
"url": "https://arxiv.org/abs/0704.0995"
} | arxiv-abstracts | We study the question of whether a composite structure of elementary
particles, with a length scale $1/\Lambda$, can leave observable effects of
non-locality and causality violation at higher energies (but $\lesssim
\Lambda$). We formulate a model-independent approach based on
Bogoliubov-Shirkov formulation of causality. We analyze the relation between
the fundamental theory (of finer constituents) and the derived theory (of
composite particles). We assume that the fundamental theory is causal and
formulate a condition which must be fulfilled for the derived theory to be
causal. We analyze the condition and exhibit possibilities which fulfil and
which violate the condition. We make comments on how causality violating
amplitudes can arise.
|
2024-08-12T18:16:26.650946 | 2007-04-09T19:20:10 | 0704.0996 | {
"authors": "Anurag Sahay, Gautam Sengupta",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:996",
"submitter": "Gautam Sengupta",
"url": "https://arxiv.org/abs/0704.0996"
} | arxiv-abstracts | Five dimensional neutral rotating black rings are described from a
Randall-Sundrum brane world perspective in the bulk black string framework. To
this end we consider a rotating black string extension of a five dimensional
black ring into the bulk of a six dimensional Randall-Sundrum brane world with
a single four brane. The bulk solution intercepts the four brane in a five
dimensional black ring with the usual curvature singularity on the brane. The
bulk geodesics restricted to the plane of rotation of the black ring are
constructed and their projections on the four brane match with the usual black
ring geodesics restricted to the same plane. The asymptotic nature of the bulk
geodesics are elucidated with reference to a bulk singularity at the AdS
horizon. We further discuss the description of a brane world black ring as a
limit of a boosted bulk black 2 brane with periodic identification.
|
2024-08-12T18:16:26.651007 | 2007-04-09T19:56:55 | 0704.0997 | {
"authors": "Dan Coman and Evgeny A. Poletsky",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:997",
"submitter": "Dan Coman",
"url": "https://arxiv.org/abs/0704.0997"
} | arxiv-abstracts | Suppose that $h$ and $g$ belong to the algebra $\B$ generated by the rational
functions and an entire function $f$ of finite order on ${\Bbb C}^n$ and that
$h/g$ has algebraic polar variety. We show that either $h/g\in\B$ or
$f=q_1e^p+q_2$, where $p$ is a polynomial and $q_1,q_2$ are rational functions.
In the latter case, $h/g$ belongs to the algebra generated by the rational
functions, $e^p$ and $e^{-p}$.
|
2024-08-12T18:16:26.651063 | 2007-04-07T19:42:53 | 0704.0998 | {
"authors": "Louise Nyssen (I3M)",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:998",
"submitter": "Louise Nyssen",
"url": "https://arxiv.org/abs/0704.0998"
} | arxiv-abstracts | Let F be a finite extension of Qp and G be GL(2,F). When V is the tensor
product of three admissible, irreducible, finite dimensional representations of
G, the space of G-invariant linear forms has dimension at most one. When a non
zero linear form exists, one wants to find an element of V which is not in its
kernel: this is a test vector. Gross and Prasad found explicit test vectors for
some triple of representations. In this paper, others are found, and they
almost complete the case when the conductor of each representation is at most
1.
|
2024-08-12T18:16:26.651115 | 2007-04-07T19:43:39 | 0704.0999 | {
"authors": "G. Lusztig",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:999",
"submitter": "George Lusztig",
"url": "https://arxiv.org/abs/0704.0999"
} | arxiv-abstracts | We relate a generic character sheaf on a disconnected reductive group with a
character of a representation of the rational points of the group over a finite
field extending a result known in the connected case.
|
2024-08-12T18:16:26.651152 | 2007-04-07T20:23:54 | 0704.1000 | {
"authors": "L.M. Zhang, et al (for the Belle Collaboration)",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:1000",
"submitter": "Liming Zhang",
"url": "https://arxiv.org/abs/0704.1000"
} | arxiv-abstracts | We report a measurement of D0-D0bar mixing in D0->Ks pi+ pi- decays using a
time-dependent Dalitz plot analysis. We first assume CP conservation and
subsequently allow for CP violation. The results are based on 540 fb$^{-1}$ of
data accumulated with the Belle detector at the KEKB $e^+e^-$ collider.
Assuming negligible CP violation, we measure the mixing parameters
$x=(0.80\pm0.29^{+0.09 +0.10}_{-0.07 -0.14})%$ and $y=(0.33\pm0.24^{+0.08
+0.06}_{-0.12 -0.08})%$, where the errors are statistical, experimental
systematic, and systematic due to the Dalitz decay model, respectively.
Allowing for CP violation, we obtain the $CPV$ parameters $|q/p|=0.86^{+0.30
+0.06}_{-0.29 -0.03}\pm0.08$ and $\arg(q/p)=(-14^{+16 +5 +2}_{-18 -3
-4})^\circ$.
|
2024-08-12T18:16:26.651205 | 2007-04-07T20:51:13 | 0704.1001 | {
"authors": "A. Losev, S. Shadrin, I. Shneiberg",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:1001",
"submitter": "Sergey Shadrin",
"url": "https://arxiv.org/abs/0704.1001"
} | arxiv-abstracts | We propose a Hodge field theory construction that captures algebraic
properties of the reduction of Zwiebach invariants to Gromov-Witten invariants.
It generalizes the Barannikov-Kontsevich construction to the case of higher
genera correlators with gravitational descendants.
We prove the main theorem stating that algebraically defined Hodge field
theory correlators satisfy all tautological relations. From this perspective
the statement that Barannikov-Kontsevich construction provides a solution of
the WDVV equation looks as the simplest particular case of our theorem. Also it
generalizes the particular cases of other low-genera tautological relations
proven in our earlier works; we replace the old technical proofs by a novel
conceptual proof.
|
2024-08-12T18:16:26.651283 | 2007-04-07T20:45:59 | 0704.1002 | {
"authors": "M. Cantiello (WSU, and INAF OA-Teramo), G. Raimondo (INAF-OA Termo),\n J.P. Blakeslee (WSU), E. Brocato (INAF-OA Teramo), M. Capaccioli (Universita'\n degli Studi di Napoli)",
"full_text_license": "None",
"license": "Creative Commons Zero - Public Domain - https://creativecommons.org/publicdomain/zero/1.0/",
"provenance": "arxiv-abstracts-dolma-0000.json.gz:1002",
"submitter": "Michele Cantiello",
"url": "https://arxiv.org/abs/0704.1002"
} | arxiv-abstracts | Recent applications have proved that the Surface Brightness Fluctuations
(SBF) technique is a reliable distance indicator in a wide range of distances,
and a promising tool to analyze the physical and chemical properties of
unresolved stellar systems, in terms of their metallicity and age. We present
the preliminary results of a project aimed at studying the evolutionary
properties and distance of the stellar populations in external galaxies based
on the SBF method.
On the observational side, we have succeeded in detecting I-band SBF
gradients in six bright ellipticals imaged with the ACS, for these same objects
we are now presenting also B-band SBF data. These B-band data are the first
fluctuations magnitude measurements for galaxies beyond 10 Mpc.
To analyze the properties of stellar populations from the data, accurate SBF
models are essential. As a part of this project, we have evaluated SBF
magnitudes from Simple Stellar Population (SSP) models specifically optimized
for the purpose. A wide range of chemical compositions and ages, as well as
different choices of the photometric system have been investigated. All models
are available at the Teramo-Stellar Populations Tools web site:
www.oa-teramo.inaf.it/SPoT.
|