1,182 research outputs found
True Dielectric and Ideal Conductor in Theory of the Dielectric Function for Coulomb System
On the basis of the exact relations the general formula for the static
dielectric permittivity e(q,0) for Coulomb system is found in the region of
small wave vectors q. The obtained formuladescribes the dielectric function
e(q,0) of the Coulomb system in both states in the "metallic" state and in the
"dielectric" one. The parameter which determines possible states of the Coulomb
system - from the "true" dielectric till the "ideal" conductor is found. The
exact relation for the pair correlation function for two-component system of
electrons and nuclei g_ei(r) is found for the arbitrary thermodynamic
parameters.Comment: 5 pages, no figure
Kramers-Kronig Relations For The Dielectric Function And The Static Conductivity Of Coulomb Systems
The mutual influence of singularities of the dielectric permittivity e(q,w)
in a Coulomb system in two limiting cases w tends to zero, q tends to zero, and
opposite q tends to zero, w tends to zero is established. It is shown that the
dielectric permittivity e(q,w) satisfies the Kramers-Kronig relations, which
possesses the singularity due to a finite value of the static conductivity.
This singularity is associated with the long "tails" of the time correlation
functions.Comment: 9 pages, 0 figure
On the Static Dielectric Permittivity for Coulomb System in the Long Wavelength Limit
On the basis of the exact relations the general formula for the static
dielectric permittivity for Coulomb system is found in the region of small wave
vectors. The obtained formula describes the dielectric function of the Coulomb
system in both limits: in the "metallic" state and in the "dielectric" one. On
this basis the determinations of the "apparent" dielectric and the "apparent"
radius of screening are introduced. In the random phase approximation (RPA) the
exact relations for the function dielectric function of the electron gas in the
long-wavelength region of the wave vectors are found for an arbitrary
degeneration of the particles.Comment: 5 pages, no figure
Investigation of the superconducting energy gap in the compound LuNiBC by the method of point contact spectroscopy: two-gap approximation
It is shown that the two-gap approximation is applicable for describing the
spectra of LuNiBC-Ag point contacts in a wide interval
of temperatures. The values and the temperature dependences of the large and
the small gaps in the plane and in the direction were estimated using
the generalized BTK model and the equations of Beloborodko. In the BCS
extrapolation the critical temperature of the small gap is 10 in the
plane and 14.5 in the direction. The absolute values of the gaps are
and . For the large gaps the
critical temperature coincides with the bulk , , and
their absolute values are very close, being about 3 in both orientations.
In the direction the contributions to the conductivity from the small and
the large gaps remain practically identical up to . In the
plane the contribution from the small gap is much smaller and decreases rapidly
as a temperature rises.Comment: 10 pages, 10 figures, submitted to Fiz. Nizk. Temp. (Low Temp. Phys.
Competition of multiband superconducting and magnetic order in ErNi2B2C observed by Andreev reflection
Point contacts (PC) Andreev reflection dV/dI spectra for the
antiferromagnetic (T_N =6K) superconductor (Tc=11K) ErNi2B2C have been measured
for the two main crystallographic directions. Observed retention of the Andreev
reflection minima in dV/dI up to Tc directly points to unusual superconducting
order parameter (OP) vanishing at Tc. Temperature dependence of OP was obtained
from dV/dI using recent theory of Andreev reflection including pair-breaking
effect. For the first time existence of a two superconducting OPs in ErNi2B2C
is shown. A distinct decrease of both OPs as temperature is lowered below T_N
is observed.Comment: 5 pages, 5 figs, to be published in Europhys. Let
Angular Schmidt Modes in Spontaneous Parametric Down-Conversion
We report a proof-of-principle experiment demonstrating that appropriately
chosen set of Hermite-Gaussian modes constitutes a Schmidt decomposition for
transverse momentum states of biphotons generated in the process of spontaneous
parametric down conversion. We experimentally realize projective measurements
in Schmidt basis and observe correlations between appropriate pairs of modes.
We perform tomographical state reconstruction in the Schmidt basis, by direct
measurement of single-photon density matrix eigenvalues.Comment: 5 pages, 4 figure
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