487 research outputs found
Ginzburg-Landau Equations for Coexistent States of Superconductivity and Antiferromagnetism in t-J model
Ginzburg-Landau (GL) equations for the coexistent state of superconductivity
and antiferromagnetism are derived microscopically from the t-J model with
extended transfer integrals. GL equations and the GL free energy, which are
obtained based on the slave-boson mean-field approximation, reflect the
electronic structure of the microscopic model, especially the evolution of the
Fermi surface due to the change of the doping rate. Thus they are suitable for
studying the material dependence of the coexistent states in high- cuprate
superconductors.Comment: 12 page
Effect of Band Structure on the Symmetry of Superconducting States
Effects of the band structure on the symmetry of superconducting (SC) states
are studied. For a square lattice system with a nearest-neighbor attractive
interaction, SC states with various symmetries are found by changing the band
structure, or, the shape of the Fermi surface. The spin-triplet (-wave) and spin-singlet (- or s-wave) SC states, and states with their
coexistence (, ) can be stabilized within the same type of
interaction. The stability of interlayer-pairing states with line nodes is also
examined, and its relation to the SC state of SrRuO is discussed.Comment: 4 pages, 4 figure
Precision measurement of vector and tensor analyzing powers in elastic deuteron-proton scattering
High precision vector and tensor analyzing powers of elastic deuteron-proton
d+p scattering have been measured at intermediate energies to investigate
effects of three-nucleon forces (3NF). Angular distribution in the range of
70-120 degree in the center-of mass frame for incident-deuteron energies of 130
and 180 MeV were obtained using the RIKEN facility. The beam polarization was
unambiguously determined by measuring the 12C(d,alpha)10B(2+) reaction at 0
degree. Results of the measurements are compared with state-of-the-art
three-nucleon calculations. The present modeling of nucleon-nucleon forces and
its extension to the three-nucleon system is not sufficient to describe the
high precision data consistently and requires, therefore, further
investigation
Shallow and diffuse spin-orbit potential for proton elastic scattering from neutron-rich helium isotopes at 71 MeV/nucleon
Vector analyzing powers for proton elastic scattering from 8He at 71
MeV/nucleon have been measured using a solid polarized proton target operated
in a low magnetic field of 0.1 T. The spin-orbit potential obtained from a
phenomenological optical model analysis is found to be significantly shallower
and more diffuse than the global systematics of stable nuclei, which is an
indication that the spin-orbit potential is modified for scattering involving
neutron-rich nuclei. A close similarity between the matter radius and the
root-mean-square radius of the spin-orbit potential is also identified.Comment: 6 pages, 4 figures, accepted for publication in Physical Review C
Rapid Communicatio
Geometrically Frustrated Crystals: Elastic Theory and Dislocations
Elastic theory of ring-(or cylinder-)shaped crystals is constructed and the
generation of edge dislocations due to geometrical frustration caused by the
bending is studied. The analogy to superconducting (or superfluid) vortex state
is pointed out and the phase diagram of the ring-crystal, which depends on
radius and thickness, is discussed.Comment: 4 pages, 3 figure
Time-reversal symmetry breaking surface states of d-wave superconductors induced by an additional order parameter with negative T_c
Surface states of d_{x^2-y^2}-wave superconductors are studied using the
Ginzburg-Landau (GL) theory. For a [110] surface it has been known that the
time-reversal symmetry (T) breaking surface state, (d+-is)-wave state, can
occur if the bare transition temperature of the s-wave order parameter (OP) is
positive. We show that even if this bare T_c is negative, it is possible to
break T because the coupling to the spontaneously generated magnetic field may
induce the s-wave OP. The T-breaking state is favored when the GL parameter
(kappa) is small.Comment: 5 pages, 7 figure
Dynamical Induction of s-wave Component in d-wave Superconductor Driven by Thermal Fluctuations
We investigated the mutual induction effects between the d-wave and the
s-wave components of order parameters due to superconducting fluctuation above
the critical temperatures and calculated its contributions to paraconductivity
and excess Hall conductivity based on the two-component stochastic TDGL
equation. It is shown that the coupling of two components increases
paraconductivity while it decreases excess Hall conductivity compared to the
cases when each component fluctuates independently. We also found the singular
behavior in the paraconductivity and the excess Hall conductivity dependence on
the coupling parameter which is consistent with the natural restriction among
the coefficients of gradient terms.Comment: 10 pages, 4 figures included, submitted to J.Phys.Soc.Jp
Effect of spin-orbit impurity scattering in the superconducting state of t-J model
We study the effect of magnetic impurities in the d_{x^2-y^2}-wave
superconducting (SC) state of the two dimensional t-J model.The spin-orbit and
the spin-exchange interactions are examined by treating the impurity as a
classical spin. The Bogoliubov de Gennes equation derived within a slave-boson
mean-field approximation is solved numerically at T = 0. The spin-exchange
scattering induces spin-triplet p-wave SC order parameters near the impurity,
while a SC state with broken time-reversal symmetry and a spontaneous current
appears in the presence of the spin-orbit interaction. When both interactions
coexist, it turns out that a state which carries a spontaneous spin current
occurs.Comment: 4 pages, 7 figure
Phase diagram and critical properties of the frustrated Kondo necklace model in a magnetic field
The critical properties of the frustrated Kondo necklace model with a half
saturation magnetization () have been studied by means of an
exact-diagonalization method. It is shown from bosonization technique that the
model can be effectively expressed as a quantum sine-Gordom model. Thus it may
show three (dimer plateau, N{\'e}el plateau and Tomonaga-Luttinger liquid)
phases due to competitions among the Ising anisotropy , and the
nearest- and next-nearest-neighbor exchange interactions and . The
boundary lines on the phase diagram separating the three
phases are determined by the method of level spectroscopy based on the
conformal field theory.Comment: 5 pages, 5 figure
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