1,123 research outputs found
Competing charge density waves and temperature-dependent nesting in 2H-TaSe2
Multiple charge density wave (CDW) phases in 2H-TaSe2 are investigated by
high-resolution synchrotron x-ray diffraction. In a narrow temperature range
immediately above the commensurate CDW transition, we observe a multi-q
superstructure with coexisting commensurate and incommensurate order
parameters, clearly distinct from the fully incommensurate state at higher
temperatures. This multi-q ordered phase, characterized by a temperature
hysteresis, is found both during warming and cooling, in contrast to previous
reports. In the normal state, the incommensurate superstructure reflection
gives way to a broad diffuse peak that persists nearly up to room temperature.
Its position provides a direct and accurate estimate of the Fermi surface
nesting vector, which evolves non-monotonically and approaches the commensurate
position as the temperature is increased. This behavior agrees with our recent
observations of the temperature-dependent Fermi surface in the same compound
[Phys. Rev. B 79, 125112 (2009)]
Impurity Effects on Quantum Depinning of Commensurate Charge Density Waves
We investigate quantum depinning of the one-dimensional (1D) commensurate
charge-density wave (CDW) in the presence of one impurity theoretically.
Quantum tunneling rate below but close to the threshold field is calculated at
absolute zero temperature by use of the phase Hamiltonian within the WKB
approximation. We show that the impurity can induce localized fluctuation and
enhance the quantum depinning. The electric field dependence of the tunneling
rate in the presence of the impurity is different from that in its absence.Comment: 14 pages with 13 figures. Submitted to J. Phys. Soc. Jp
Downward shift of infrared conductivity spectral weight at the DDW transition: role of anisotropy
We consider the motion of conductivity spectral weight at a
finite-temperature phase transition at which density-wave (DDW)
order develops. We show that there is a shift of spectral weight to higher
frequencies if the quasiparticle lifetime is assumed to be isotropic, but a
shift to lower frequencies if the quasiparticle lifetime is assumed to be
anisotropic. We suggest that this is consistent with recent experiments on the
pseudogap phase of the cuprate superconductors and, therefore, conclude that
the observation of a downward shift in the spectral weight at the pseudogap
temperature does not militate against the DDW theory of the pseudogap.Comment: 8 pages, 7 figures. Added reference
Self Organization and a Dynamical Transition in Traffic Flow Models
A simple model that describes traffic flow in two dimensions is studied. A
sharp {\it jamming transition } is found that separates between the low density
dynamical phase in which all cars move at maximal speed and the high density
jammed phase in which they are all stuck. Self organization effects in both
phases are studied and discussed.Comment: 6 pages, 4 figure
Spin-Peierls Quantum Phase Transitions in Coulomb Crystals
The spin-Peierls instability describes a structural transition of a crystal
due to strong magnetic interactions. Here we demonstrate that cold Coulomb
crystals of trapped ions provide an experimental testbed in which to study this
complex many-body problem and to access extreme regimes where the instability
is triggered by quantum fluctuations alone. We present a consistent analysis
based on different analytical and numerical methods, and provide a detailed
discussion of its feasibility on the basis of ion-trap experiments. Moreover,
we identify regimes where this quantum simulation may exceed the power of
classical computers.Comment: slightly longer than the published versio
Pseudogap enhancement due to magnetic impurities in d-density waves
We study the effect of quantum magnetic impurities on d-wave spin density
waves (d-SDW). The impurity spins are aligned coherently according to the spin
space anisotropy of the condensate. Both the order parameter and transition
temperature increases due to the coherent interplay between magnetic scatterers
and d-SDW. This can explain the recent experimental data on the pseudogap
enhancement of Ni substituted NdBa_2{Cu_{1-y}Ni_y}O_6.8 from Pimenov et al.
(Phys. Rev. Lett. 94, 227003 (2005)).Comment: 4 pages, 3 figure
Dynamics of photoinduced Charge Density Wave-metal phase transition in K0.3MoO3
We present first systematic studies of the photoinduced phase transition from
the ground charge density wave (CDW) state to the normal metallic (M) state in
the prototype quasi-1D CDW system K0.3MoO3. Ultrafast non-thermal CDW melting
is achieved at the absorbed energy density that corresponds to the electronic
energy difference between the metallic and CDW states. The results imply that
on the sub-picosecond timescale when melting and subsequent initial recovery of
the electronic order takes place the lattice remains unperturbed.Comment: Phys. Rev. Lett., accepted for publicatio
First-Order Type Effects in YBaCuO at the Onset of Superconductivity
We present results of Raman scattering experiments on tetragonal for doping levels between 0 and
0.07 holes/CuO. Below the onset of superconductivity at , we find evidence of a diagonal superstructure. At ,
lattice and electron dynamics change discontinuously with the charge and spin
properties being renormalized at all energy scales. The results indicate that
charge ordering is intimately related to the transition at and
that the maximal transition temperature to superconductivity at optimal doping
depends on the type of ordering at .Comment: 4 pages, 4 figure
Incommensurate spin resonance in URu2Si2
We focus on inelastic neutron scattering in and argue that
observed gap in the fermion spectrum naturally leads to the spin feature
observed at energies at momenta at \bQ^* = (1\pm 0.4,
0,0). We discuss how spin features seen in can indeed be thought
of in terms of {\em spin resonance} that develops in HO state and is {\em not
related} to superconducting transition at 1.5K. In our analysis we assume that
the HO gap is due to a particle-hole condensate that connects nested parts of
the Fermi surface with nesting vector . Within this approach we can
predicted the behavior of the spin susceptibility at \bQ^* and find it to be
is strikingly similar to the phenomenology of resonance peaks in high-T and
heavy fermion superconductors. The energy of the resonance peak scales with
. We discuss observable consequences
spin resonance will have on neutron scattering and local density of states.Comment: 8 pgaes latex, 4 fig
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