27,964 research outputs found
Magnetic susceptibility study of hydrated and non-hydrated NaxCoO2-yH2O single crystals
We have measured the magnetic susceptibility of single crystal samples of
non-hydrated NaxCoO2 (x ~ 0.75, 0.67, 0.5, and 0.3) and hydrated Na0.3CoO2-yH2O
(y ~ 0, 0.6, 1.3). Our measurements reveal considerable anisotropy between the
susceptibilities with H||c and H||ab. The derived anisotropic g-factor ratio
(g_ab/g_c) decreases significantly as the composition is changed from the
Curie-Weiss metal with x = 0.75 to the paramagnetic metal with x = 0.3. Fully
hydrated Na0.3CoO2-1.3H2O samples have a larger susceptibility than
non-hydrated Na0.3CoO2 samples, as well as a higher degree of anisotropy. In
addition, the fully hydrated compound contains a small additional fraction of
anisotropic localized spins.Comment: 6 pages, 5 figure
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Development Of Third Harmonic Generation As A Short Pulse Probe Of Shock Heated Material
We are studying high-pressure laser produced shock waves in silicon (100). To examine the material dynamics, we are performing pump-probe style experiments utilizing 600 ps and 40 fs laser pulses from a Ti:sapphire laser. Two-dimensional interferometry reveals information about the shock breakout, while third harmonic light generated at the rear surface is used to infer the crystalline state of the material as a function of time. Sustained third harmonic generation (THG) during a similar to 100 kbar shock breakout indicate that the rear surface remains crystalline for at least 3 ns. However, a decrease in THG during a similar to 300 kbar shock breakout suggests a different behavior, which could include a change in crystalline structure.Mechanical Engineerin
Vacuumless kinks systems from vacuum ones, an example
Some years ago, Cho and Vilenkin, introduced a model which presents
topological solutions, despite not having degenerate vacua as is usually
expected. Here we present a new model with topological defects, connecting
degenerate vacua but which in a certain limit recovers precisely the one
proposed originally by Cho and Vilenkin. In other words, we found a kind of
parent model for the so called vacuumless model. Then the idea is extended to a
model recently introduced by Bazeia et al. Finally, we trace some comments the
case of the Liouville model.Comment: 11 pages, 4 figure
Geometrization of the Gauge Connection within a Kaluza-Klein Theory
Within the framework of a Kaluza-Klein theory, we provide the geometrization
of a generic (Abelian and non-Abelian) gauge coupling, which comes out by
choosing a suitable matter fields dependence on the extra-coordinates.
We start by the extension of the Nother theorem to a multidimensional
spacetime being the direct sum of a 4-dimensional Minkowski space and of a
compact homogeneous manifold (whose isometries reflect the gauge symmetry); we
show, how on such a ``vacuum'' configuration, the extra-dimensional components
of the field momentum correspond to the gauge charges. Then we analyze the
structure of a Dirac algebra as referred to a spacetime with the Kaluza-Klein
restrictions and, by splitting the corresponding free-field Lagrangian, we show
how the gauge coupling terms outcome.Comment: 10 pages, no figure, to appear on Int. Journ. Theor. Phy
An Experimental and Semi-Empirical Method to Determine the Pauli-Limiting Field in Quasi 2D Superconductors as applied to -(BEDT-TTF)Cu(NCS): Strong Evidence of a FFLO State
We present upper critical field data for -(BEDT-TTF)Cu(NCS)
with the magnetic field close to parallel and parallel to the conducting
layers. We show that we can eliminate the effect of vortex dynamics in these
layered materials if the layers are oriented within 0.3 degrees of parallel to
the applied magnetic field. Eliminating vortex effects leaves one remaining
feature in the data that corresponds to the Pauli paramagnetic limit ().
We propose a semi-empirical method to calculate the in quasi 2D
superconductors. This method takes into account the energy gap of each of the
quasi 2D superconductors, which is calculated from specific heat data, and the
influence of many body effects. The calculated Pauli paramagnetic limits are
then compared to critical field data for the title compound and other organic
conductors. Many of the examined quasi 2D superconductors, including the above
organic superconductors and CeCoIn, exhibit upper critical fields that
exceed their calculated suggesting unconventional superconductivity. We
show that the high field low temperature state in
-(BEDT-TTF)Cu(NCS) is consistent with the Fulde Ferrell Larkin
Ovchinnikov state.Comment: 8 pages, 9 figures, 10 years of dat
Effective Lagrangian from Higher Curvature Terms: Absence of vDVZ Discontinuity in AdS Space
We argue that the van Dam-Veltman-Zakharov discontinuity arising in the limit of the massive graviton through an explicit Pauli-Fierz mass term
could be absent in anti de Sitter space. This is possible if the graviton can
acquire mass spontaneously from the higher curvature terms or/and the massless
limit is attained faster than the cosmological constant . We discuss the effects of higher-curvature couplings and of an explicit
cosmological term () on stability of such continuity and of massive
excitations.Comment: 23 pages, Latex, the version to appear in Class. Quant. Gra
Quantum Entanglement in the Two Impurity Kondo Model
In order to quantify quantum entanglement in two impurity Kondo systems, we
calculate the concurrence, negativity, and von Neumann entropy. The
entanglement of the two Kondo impurities is shown to be determined by two
competing many-body effects, the Kondo effect and the
Ruderman-Kittel-Kasuya-Yosida (RKKY) interaction, . Due to the
spin-rotational invariance of the ground state, the concurrence and negativity
are uniquely determined by the spin-spin correlation between the impurities. It
is found that there exists a critical minimum value of the antiferromagnetic
correlation between the impurity spins which is necessary for entanglement of
the two impurity spins. The critical value is discussed in relation with the
unstable fixed point in the two impurity Kondo problem. Specifically, at the
fixed point there is no entanglement between the impurity spins. Entanglement
will only be created (and quantum information processing (QIP) be possible) if
the RKKY interaction exchange energy, , is at least several times larger
than the Kondo temperature, . Quantitative criteria for QIP are given in
terms of the impurity spin-spin correlation.Comment: 7 pages, 3 figures, 1 tabl
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