743 research outputs found
Anharmonicity of flux lattices and thermal fluctuations in layered superconductors
We study elasticity of a perpendicular flux lattice in a layered
superconductor with Josephson coupling between layers. We find that the energy
contains ln(flux displacement) terms, so that elastic constants cannot be
strictly defined. Instead we define effective elastic constants by a thermal
average. The tilt modulus has terms with ln(T) which for weak fields, i.e.
Josephson length smaller than the flux line spacing, lead to displacement
square average proportional to T/ln(T). The expansion parameter indicates that
the dominant low temperature phase transition is either layer decoupling at
high fields or melting at low fields.Comment: 15 pages, 2 eps figures, Revtex, submitted to Phys. Rev. B.
Sunj-class: superconductivit
Phase transitions for a collective coordinate coupled to Luttinger liquids
We study various realizations of collective coordinates, e.g. the position of
a particle, the charge of a Coulomb box or the phase of a Bose or a
superconducting condensate, coupled to Luttinger liquids (LL) with N flavors.
We find that for Luttinger parameter 1/2<K<1 there is a phase transition from a
delocalized phase into a phase with a periodic potential at strong coupling. In
the delocalized phase the dynamics is dominated by an effective mass, i.e.
diffusive in imaginary time, while on the transition line it becomes
dissipative. At K=1/2 there is an additional transition into a localized phase
with no diffusion at zero temperature.Comment: 5 pages, 2 figures, 1 table, Phys. Rev. Lett. (in press
Disorder Induced Transitions in Layered Coulomb Gases and Superconductors
A 3D layered system of charges with logarithmic interaction parallel to the
layers and random dipoles is studied via a novel variational method and an
energy rationale which reproduce the known phase diagram for a single layer.
Increasing interlayer coupling leads to successive transitions in which charge
rods correlated in N>1 neighboring layers are nucleated by weaker disorder. For
layered superconductors in the limit of only magnetic interlayer coupling, the
method predicts and locates a disorder-induced defect-unbinding transition in
the flux lattice. While N=1 charges dominate there, N>1 disorder induced defect
rods are predicted for multi-layer superconductors.Comment: 4 pages, 2 figures, RevTe
Field-induced charge transport at the surface of pentacene single crystals: a method to study charge dynamics of 2D electron systems in organic crystals
A method has been developed to inject mobile charges at the surface of
organic molecular crystals, and the DC transport of field-induced holes has
been measured at the surface of pentacene single crystals. To minimize damage
to the soft and fragile surface, the crystals are attached to a pre-fabricated
substrate which incorporates a gate dielectric (SiO_2) and four probe pads. The
surface mobility of the pentacene crystals ranges from 0.1 to 0.5 cm^2/Vs and
is nearly temperature-independent above ~150 K, while it becomes thermally
activated at lower temperatures when the induced charges become localized.
Ruling out the influence of electric contacts and crystal grain boundaries, the
results contribute to the microscopic understanding of trapping and detrapping
mechanisms in organic molecular crystals.Comment: 14 pages, 4 figures. Submitted to J. Appl. Phy
Glass phases of flux lattices in layered superconductors
We study a flux lattice which is parallel to superconducting layers, allowing
for dislocations and for disorder of both short wavelength and long wavelength.
We find that the long wavelength disorder has a significant effect on the phase
diagram -- it produces a first order transition within the Bragg glass phase
and leads to melting at strong disorder. This then allows a Friedel scenario of
2D superconductivity.Comment: 5 pages, 1 eps figure, Revte
Modern Trends in Workmen\u27s Compensation (a nation-wide review of basic principles)
National Symposium on Scientific Proof and Relations of Law and Medicine, Second Series
Quantum Hall effects in layered disordered superconductors
Layered singlet paired superconductors with disorder and broken time reversal
symmetry are studied. The phase diagram demonstrates charge-spin separation in
transport. In terms of the average intergrain transmission and the interlayer
tunnelling we find quantum Hall phases with spin Hall coefficients of 0 and 2
separated by a spin metal phase. We identify a spin metal-insulator
localization exponent as well as a spin conductivity exponent of ~0.9. In
presence of a Zeeman term an additional phase with spin Hall coefficient of 1
appears.Comment: 4 pages, 4 figure
Antiferromagnetic domain walls in lightly doped layered cuprates
Recent ESR data shows rotation of the antiferromagnetic (AF) easy axis in
lightly doped layered cuprates upon lowering the temperature. We account for
the ESR data and show that it has significant implications on spin and charge
ordering according to the following scenario: In the high temperature phase AF
domain walls coincide with (110) twin boundaries of an orthorhombic phase. A
magnetic field leads to annihilation of neighboring domain walls resulting in
antiphase boundaries. The latter are spin carriers, form ferromagnetic lines
and may become charged in the doped system. However, hole ordering at low
temperatures favors the (100) orientation, inducing a pi/4 rotation in the AF
easy axis. The latter phase has twin boundaries and AF domain walls in (100)
planes.Comment: 4 pages, 3 figures (1 eps). v2: no change in content, Tex shadow
problem cleare
Transconducting transition for a dynamic boundary coupled to several Luttinger liquids
We study a dynamic boundary, e.g. a mobile impurity, coupled to N independent
Tomonaga-Luttinger liquids (TLLs) each with interaction parameter K. We
demonstrate that for N>2 there is a quantum phase transition at K>1/2, where
the TLL phases lock together at the particle position, resulting in a non-zero
transconductance equal to e^2/Nh. The transition line terminates for strong
coupling at K=1- 1/N, consistent with results at large N. Another type of a
dynamic boundary is a superconducting (or Bose-Einstein condensate) grain
coupled to N>2 TLLs, here the transition signals also the onset of a relevant
Josephson coupling.Comment: 21 pages, 1 figur
- …