75 research outputs found
Evidence for field-induced excitations in low-temperature thermal conductivity of Bi_2Sr_2CaCu_2O_8
The thermal conductivity ,, of Bi_2Sr_2CaCu_2O_8 was studied as a
function of magnetic field. Above 5 K, after an initial decrease,
presents a kink followed by a plateau, as recently reported by Krishana et al..
By contrast, below 1K, the thermal conductivity was found to \emph{increase}
with increasing field. This behavior is indicative of a finite density of
states and is not compatible with the existence of a field-induced fully gapped
state which was recently proposed to describe the
plateau regime. Our low-temperature results are in agreement with recent works
predicting a field-induced enhancement of thermal conductivity by Doppler shift
of quasi-particle spectrum.Comment: 4 pages including 4 eps figures, submitted to Phys. Rev. Let
Quasiparticle thermal Hall angle and magnetoconductance in YBa_2Cu_3O_x
We present a way to extract the quasiparticle (qp) thermal conductivity
Kappa_e and mean-free-path in YBa_2Cu_3O_x, using the thermal Hall effect and
the magnetoconductance of Kappa_e. The results are very consistent with heat
capacity experiments. Moreover, we find a simple relation between the thermal
Hall angle Theta_Q and the H-dependence of Kappa_e, as well as numerical
equality between Theta_Q and the electrical Hall angle. The findings also
reveal an anomalously anisotropic scattering process in the normal state.Comment: 4 pages in Tex, 5 figures in EPS; replaced on 5/12/99, minor change
Separation of Quasiparticle and Phononic Heat Currents in YBCO
Measurements of the transverse (k_{xy}) and longitudinal (k_{xx}) thermal
conductivity in high magnetic fields are used to separate the quasiparticle
thermal conductivity (k_{xx}^{el}) of the CuO_2-planes from the phononic
thermal conductivity in YBa_2Cu_3O_{7-\delta}. k_{xx}^{el} is found to display
a pronounced maximum below T_c. Our data analysis reveals distinct transport
(\tau) and Hall (\tau_H) relaxation times below T_c: Whereas \tau is strongly
enhanced, \tau_H follows the same temperature dependence as above T_c
Mixed-state quasiparticle transport in high-T_c cuprates: localization by magnetic field
Theory of quasiparticle transport in the mixed state of a d-wave
superconductor is developed under the assumption of disordered vortex array. A
novel universal regime is identified at fields above H*= c*H_{c2}(T/T_c)^2,
characterized by a field-independent longitudinal thermal conductivity. It is
argued that this behavior is responsible for the high-field plateau in the
thermal conductivity experimentally observed in cuprates by Krishana, Ong and
co-workers.Comment: 4 pages REVTeX + 1 PostScript figure. Final version to appear in PRL.
Several changes in response to referee comments. For related work and info
visit http://www.pha.jhu.edu/~fran
Time reversal symmetry breaking superconductivity
We study time reversal symmetry breaking superconductivity with ( or )
symmetries. It is shown that the behavior of such superconductors could be {\em
qualitatively} different depending on the minor components () and its
phase at lower temperatures. It is argued that such {\em qualitatively
different} behaviors in thermal as well as in angular dependencies could be a
{\em source} of consequences in transport and Josephson physics.
Orthorhombicity is found to be a strong mechanism for mixed phase (in case of
). We show that due to electron correlation the order parameter is
more like a pure symmetry near optimum doping.Comment: 5 pages, 5 figures (attached), to be published in Physical Review
Dirac Nodes and Quantized Thermal Hall Effect in the Mixed State of d-wave Superconductors
We consider the vortex state of d-wave superconductors in the clean limit.
Within the linearized approximation the quasiparticle bands obtained are found
to posess Dirac cone dispersion (band touchings) at special points in the
Brillouin zone. They are protected by a symmetry of the linearized Hamiltonian
that we call T_Dirac. Moreover, for vortex lattices that posess inversion
symmetry, it is shown that there is always a Dirac cone centered at zero energy
within the linearized theory. On going beyond the linearized approximation and
including the effect of the smaller curvature terms (that break T_Dirac), the
Dirac cone dispersions are found to acquire small gaps (0.5 K/Tesla in YBCO)
that scale linearly with the applied magnetic field. When the chemical
potential for quasiparticles lies within the gap, quantization of the
thermal-Hall conductivity is expected at low temperatures i.e. kappa_{xy}/T =
n[(pi k_B)^2/(3h)] with the integer `n' taking on values n=+2, -2, 0. This
quantization could be seen in low temperature thermal transport measurements of
clean d-wave superconductors with good vortex lattices.Comment: (23 pages in all [7 pages in appendices], 9 figures
Ground State Vortex Lattice Structures in d-wave Superconductors
We show in a realistic symmetry gap model for a cuprate
superconductor that the clean vortex lattice has discontinuous structural
transitions (at and near T=0), as a function of the magnetic field along
the c-axis. The transitions arise from the singular nonlocal and anisotropic
susceptibility of the superconductor to the perturbation
caused by supercurrents associated with vortices. The susceptibility, due to
virtual Dirac quasiparticle-hole excitation, is calculated carefully, and leads
to a ground state transition for the triangular lattice from an orientation
along one of the crystal axis to one at 45 to them, i.e, along the gap zero
direction. The field scale is seen to be 5 Tesla , where is the gap maximum, is the
nearest neighbour hopping, is the lattice constant, and is the
flux quantum. At much higher fields () there is a discontinuous
transition to a centred square structure. The source of the differences from
existing calculations, and experimental observability are discussed, the latter
especially in view of the very small (a few degrees per vortex) differences
in the ground state energy.Comment: To be published in Phys. Rev.
The Haldane-Rezayi Quantum Hall State and Magnetic Flux
We consider the general abelian background configurations for the
Haldane-Rezayi quantum Hall state. We determine the stable configurations to be
the ones with the spontaneous flux of with .
This gives the physical mechanism by which the edge theory of the state becomes
identical to the one for the 331 state. It also provides a new experimental
consequence which can be tested in the enigmatic plateau in a single
layer system.Comment: RevTex, 5 pages, 2 figures. v2:minor corrections. v4: published
version. Discussion on the thermodynamic limit adde
Thermal Conductivity Tensor in YBaCuO: Effects of a Planar Magnetic Field
We have measured the thermal conductivity tensor of a twinned
YBaCuO single crystal as a function of angle between
the magnetic field applied parallel to the CuO planes and the heat current
direction, at different magnetic fields and at T=13.8 K. Clear fourfold and
twofold variations in the field-angle dependence of and
were respectively recorded in accordance with the d-wave pairing
symmetry of the order parameter. The oscillation amplitude of the transverse
thermal conductivity was found to be larger than the
longitudinal one in the range of magnetic field studied here
(). From our data we obtain quantities that are free
from non-electronic contributions and they allow us a comparison of the
experimental results with current models for the quasiparticle transport in the
mixed state.Comment: 9 Figures, Phys. Rev. B(in press
Low temperature superfluid stiffness of d-wave superconductor in a magnetic field
The temperature and field dependence of the superfluid density in
the vortex state of a d-wave superconductor are calculated using a microscopic
model in the quasiclassical approximation. We show that at temperatures below
T^{*} \varpropto \sqrt{H}$, the linear T dependence of rho_s crosses over to a
T^2 dependence differently from the behavior of the effective penetration
depth, lambda_eff^{-2}(T). We point out that the expected dependences could be
probed by a mutual-inductance technique experiment.Comment: 4 pages, RevTeX4, 2 EPS figures; minor revisions made and 1 new
reference added; final version published in PR
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