8,445 research outputs found
He Scattering from Random Adsorbates, Disordered Compact Islands and Fractal Submonolayers: Intensity Manifestations of Surface Disorder
A theoretical study is made on He scattering from three fundamental classes
of disordered ad-layers: (a) Translationally random adsorbates, (b) disordered
compact islands and (c) fractal submonolayers. The implications of the results
to experimental studies of He scattering from disordered surfaces are
discussed, and a combined experimental-theoretical study is made for Ag
submonolayers on Pt(111). Some of the main theoretical findings are: (1)
Structural aspects of the calculated intensities from translationally random
clusters were found to be strongly correlated with those of individual
clusters. (2) Low intensity Bragg interference peaks appear even for scattering
from very small ad-islands, and contain information on the ad-island local
electron structure. (3) For fractal islands, just as for islands with a
different structure, the off-specular intensity depends on the parameters of
the He/Ag interaction, and does not follow a universal power law as previously
proposed in the literature. In the experimental-theoretical study of Ag on
Pt(111), we use first experimental He scattering data from low-coverage (single
adsorbate) systems to determine an empirical He/Ag-Pt potential of good
quality. Then, we carry out He scattering calculations for high coverage and
compare with experiments. The conclusions are that the actual experimental
phase corresponds to small compact Ag clusters of narrow size distribution,
translationally disordered on the surface.Comment: 36 double-spaced pages, 10 figures; accepted by J. Chem. Phys.,
scheduled to appear March 8. More info available at
http://www.fh.huji.ac.il/~dani
Universal temperature dependence of the conductivity of a strongly disordered granular metal
A disordered array of metal grains with large and random intergrain
conductances is studied within the one-loop accuracy renormalization group
approach. While at low level of disorder the dependence of conductivity on log
T is nonuniversal (it depends on details of the array's geometry), for strong
disorder this dependence is described by a universal nonlinear function, which
depends only on the array's dimensionality. In two dimensions this function is
found numerically. The dimensional crossover in granular films is discussed.Comment: 6 pages, 6 figures, submitted to JETP Letter
Exciton states in monolayer MoSe2: impact on interband transitions
We combine linear and non-linear optical spectroscopy at 4K with ab initio
calculations to study the electronic bandstructure of MoSe2 monolayers. In
1-photon photoluminescence excitation (PLE) and reflectivity we measure a
separation between the A- and B-exciton emission of 220 meV. In 2-photon PLE we
detect for the A- and B-exciton the 2p state 180meV above the respective 1s
state. In second harmonic generation (SHG) spectroscopy we record an
enhancement by more than 2 orders of magnitude of the SHG signal at resonances
of the charged exciton and the 1s and 2p neutral A- and B-exciton. Our
post-Density Functional Theory calculations show in the conduction band along
the direction a local minimum that is energetically and in k-space
close to the global minimum at the K-point. This has a potentially strong
impact on the polarization and energy of the excitonic states that govern the
interband transitions and marks an important difference to MoS2 and WSe2
monolayers.Comment: 8 pages, 3 figure
Variable range cotunneling and conductivity of a granular metal
The Efros-Shklovskii law for the conductivity of granular metals is
interpreted as a result of a variable range cotunneling process. The
cotunneling between distant resonant grains is predominantly elastic at low T
<< T_c, while it is inelastic (i.e., accompanied by creation of electron-hole
pairs on a string of intermediate non-resonant grains) at T > T_c. The
corresponding E-S temperature T_ES in the latter case is slightly
(logarithmically) T-dependent. The magnetoresistance in the two cases is
different: it may be relatively strong and negative at T much below T_c, while
at T>T_c it is suppressed due to inelastic processes which destroy the
interference.Comment: Submitted to JETP Letter
Negative Magnetoresistance of Granular Metals in a Strong Magnetic Field
The magnetoresistance of a granular superconductor in a strong magnetic field
destroying the gap in each grain is considered. It is assumed that the
tunneling between grains is sufficiently large such that all conventional
effects of localization can be neglected. A non-trivial sensitivity to the
magnetic field comes from superconducting fluctuations leading to the formation
of virtual Cooper pairs and reducing the density of states. At low temperature,
the pairs do not contribute to the macroscopic transport but their existence
can drastically reduce the conductivity. Growing the magnetic field one
destroys the fluctuations, which improves the metallic properties and leads to
the negative magnetoresistance.Comment: 4 pages, 1 figure, RevTe
Proximity effect in granular superconductor-normal metal structures
We fabricated three-dimensional disordered Pb-Cu granular structures, with
various metal compositions. The typical grain size of both metals is smaller
than the superconductor and normal metal coherence lengths, thus satisfying the
Cooper limit. The critical temperature of the samples was measured and compared
with the critical temperature of bilayers. We show how the proximity effect
theories, developed for bilayers, can be modified for random mixtures and we
demonstrate that our experimental data fit well the de Gennes weak coupling
limit theory in the Cooper limit. Our results indicate that, in granular
structures, the Cooper limit can be satisfied over a wide range of
concentrations.Comment: 15 pages, 4 figure
Magnetoresistance of Granular Superconducting Metals in a Strong Magnetic Field
The magnetoresistance of a granular superconductor in a strong magnetic field
is considered. It is assumed that this field destroys the superconducting gap
in each grain, such that all interesting effects considered in the paper are
due to superconducting fluctuations. The conductance of the system is assumed
to be large, which allows us to neglect all localization effects as well as the
Coulomb interaction. It is shown that at low temperatures the superconducting
fluctuations reduce the one-particle density of states but do not contribute to
transport. As a result, the resistivity of the normal state exceeds the
classical resistivity approaching the latter only in the limit of extremely
strong magnetic fields, and this leads to a negative magnetoresistance. We
present detailed calculations of physical quatities relevant for describing the
effect and make a comparison with existing experiments.Comment: 24 pages, 10 figure
Inversion of Randomly Corrugated Surfaces Structure from Atom Scattering Data
The Sudden Approximation is applied to invert structural data on randomly
corrugated surfaces from inert atom scattering intensities. Several expressions
relating experimental observables to surface statistical features are derived.
The results suggest that atom (and in particular He) scattering can be used
profitably to study hitherto unexplored forms of complex surface disorder.Comment: 10 pages, no figures. Related papers available at
http://neon.cchem.berkeley.edu/~dan
Low temperature relation for the trace of the energy-momentum tensor in QCD with light quarks
It is shown that the temperature derivatives of the anomalous and normal
(quark massive term) contributions to the trace of the energy-momentum tensor
in QCD are equal to each other in the low temperature region. The physical
consequences of this relation are discussed.Comment: RevTeX, 4 pages, no figure
Vortex lattice studies in CeCoIn5 with H perpendicular to c
We present small angle neutron scattering studies of the vortex lattice (VL)
in CeCoIn5 with magnetic fields applied parallel (H) to the antinodal [100] and
nodal [110] directions. For H || [100], a single VL orientation is observed,
while a 90 degree reorientation transition is found for H || [110]. For both
field orientations and VL configurations we find a distorted hexagonal VL with
an anisotropy, Gamma = 2.0 +/- 0.05. The VL form factor shows strong Pauli
paramagnetic effects similar to what have previously been reported for H ||
[001]. At high fields, above which the upper critical field (Hc2) becomes a
first-order transition, an increased disordering of the VL is observed.Comment: 5 pages, 4 figure
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