351 research outputs found
Quantum fluctuations in the cohesive force of metallic nanowires
Based on the recent free electron model for cohesion in narrow metallic
constrictions by Stafford et al., we calculate the quantum fluctuations in the
cohesive force versus elongation. The fluctuations are dominated by states near
the Fermi energy, thus explaining their apparently universal magnitude of order
epsilon_F/lambda_F. We present numerical results for the force fluctuations in
a simple geometry and show that they are well described by the contributions of
a few classical periodic orbits in the Balian-Bloch trace formula for the
density of states of transverse motion.Comment: 4 pages, 2 figures, RevTeX, minor changes, to appear in Phys. Rev. B
Rapid. Com
Theory of RF-spectroscopy of strongly interacting Fermions
We show that strong pairing correlations in Fermi gases lead to the
appearance of a gap-like structure in the RF-spectrum, both in the balanced
superfluid and in the normal phase above the Clogston-Chandrasekhar limit. The
average RF-shift of a unitary gas is proportional to the ratio of the Fermi
velocity and the scattering length with the final state. In the strongly
imbalanced case, the RF-spectrum measures the binding energy of a minority atom
to the Fermi sea of majority atoms. Our results provide a qualitative
understanding of recent experiments by Schunck et.al.Comment: revised version, 4 pages, 3 figures, RevTex
Higgs Mode and Magnon Interactions in 2D Quantum Antiferromagnets from Raman Scattering
We present a theory for Raman scattering on 2D quantum antiferromagnets. The
microscopic Fleury-Loudon Hamiltonian is expressed in terms of an effective
- model. Well within the N\'eel ordered phase, the Raman spectrum
contains a two-magnon and a two-Higgs contribution, which are calculated
diagramatically. The vertex functions for both the Higgs and magnon
contributions are determined from a numerical solution of the corresponding
Bethe-Salpeter equation. Due to the momentum dependence of the Raman vertex in
the relevant symmetry, the contribution from the Higgs mode is
strongly suppressed. Except for intermediate values of the Higgs mass, it does
not show up as separate peak in the spectrum but gives rise to a broad
continuum above the dominant contribution from two-magnon excitations. The
latter give rise to a broad, asymmetric peak at , which
is a result of magnon-magnon interactions mediated by the Higgs mode. The full
Raman spectrum is determined completely by the antiferromagnetic exchange
coupling and a dimensionless Higgs mass. Experimental Raman spectra of
undoped cuprates turn out to be in very good agreement with the theory only
with inclusion of the Higgs contribution. They thus provide a clear signature
of the presence of a Higgs mode in spin one-half 2D quantum antiferromagnets.Comment: 12 pages, 15 figure
Density matrix renormalization group for disordered bosons in one dimension
We calculate the zero-temperature phase diagram of the disordered
Bose-Hubbard model in one dimension using the density matrix renormalization
group. For integer filling the Mott insulator is always separated from the
superfluid by a Bose glass phase. There is a reentrance of the Bose glass both
as a function of the repulsive interaction and of disorder. At half-filling
where no Mott insulator exists, the superfluid density has a maximum where the
kinetic and repulsive energies are about the same. Superfluidity is suppressed
both for small and very strong repulsion but is always monotonic in disorder.Comment: 4 pages, 2 eps figures, uses RevTe
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