237 research outputs found
Nuclear Spin Relaxation in Hole Doped Two-Leg Ladders
The nuclear spin-lattice relaxation rate () has been measured in the
single crystals of hole doped two-leg ladder compounds
SrCaCuO and in the undoped parent material
LaCaCuO. Comparison of at the Cu and the two
distinct oxygen sites revealed that the major spectral weight of low frequency
spin fluctuations is located near for most of the
temperature and doping ranges investigated. Remarkable difference in the
temperature dependence of for the two oxygen sites in the heavily doped
=12 sample revealed reduction of singlet correlations between two legs in
place of growing antiferromagnetic correlations along the leg direction with
increasing temperature. Such behavior is most likely caused by the dissociation
of bound hole pairs.Comment: 4 pages. to appear in J. Phys. Soc. Jpn. Vol. 6
Depth profile photoemission study of thermally diffused Mn/GaAs (001) interfaces
We have performed a depth profile study of thermally diffused Mn/GaAs (001)
interfaces using photoemission spectroscopy combined with Ar-ion
sputtering. We found that Mn ion was thermally diffused into the deep region of
the GaAs substrate and completely reacted with GaAs. In the deep region, the Mn
2 core-level and Mn 3 valence-band spectra of the Mn/GaAs (001) sample
heated to 600 C were similar to those of GaMnAs,
zinc-blende-type MnAs dots, and/or interstitial Mn in tetrahedrally coordinated
by As atoms, suggesting that the Mn 3 states were essentially localized but
were hybridized with the electronic states of the host GaAs. Ferromagnetism was
observed in the dilute Mn phase.Comment: 5 pages, 4 figure
Superconductivuty versus Tunneling in a Doped Antiferromagnetic Ladder
The low-energy charge excitations of a doped antiferromagnetic ladder are
modeled by a system of interacting spinless fermions that live on the same
ladder. A relatively large spin gap is assumed to ``freeze out'' all spin
fluctuations. We find that the formation of rung hole pairs coincides with the
opening of a single-particle gap for charge excitations along chains and with
the absence of coherent tunneling in between chains. We also find that such
hole pairs condense into either a crystalline or superconducting state as a
function of the binding energy.Comment: 15 pgs. in PLAIN TeX, 2 figs. in postscript, to appear in Phys. Rev.
Quantum Spin Systems: From Spin Gaps to Pseudo Gaps
Many low dimensional spin systems with a dimerized or ladder-like
antiferromagnetic exchange coupling have a gapped excitation spectrum with
magnetic bound states within the spin gap. For spin ladders with an even number
of legs the existence of spin gaps and within the t-J model a tendency toward
superconductivity with d-wave symmetry is predicted. In the following we will
characterize the spin excitation spectra of different low dimensional spin
systems taking into account strong spin phonon interaction (),
charge ordering () and doping on chains and ladders (\ladder).
The spectroscopic characterization of the model systems mentioned above has
been performed using magnetic inelastic light scattering originating from a
spin conserving exchange scattering mechanism. This is also bound to yield more
insight into the interrelation between these spin gap excitations and the
origin of the pseudo gap in high temperature superconductors.Comment: 10 pages, 5 figure
Spin Gap and Superconductivity in Weakly Coupled Ladders: Interladder One-particle vs. Two-particle Crossover
Effects of the interladder one-particle hopping, , on the
low-energy asymptotics of a weakly coupled Hubbard ladder system have been
studied, based on the perturbative renormalization-group approach. We found
that for finite intraladder Hubbard repulsion, , there exists a crossover
value of the interladder one-particle hopping, . For
, the spin gap metal (SGM) phase of the isolated
ladder transits at a finite transition temperature, , to the d-wave
superconducting (SCd) phase via a two-particle crossover. In the temperature
region, , interladder coherent Josephson tunneling of the Cooper pairs
occurs, while the interladder coherent one-particle process is strongly
suppressed. For , around a crossover temperature,
, the system crosses over to the two-dimensional (2D) phase via a
one-particle crossover. In the temperature region, , the
interladdercoherent band motion occurs.Comment: 4 pages, 5 eps figures, uses jpsj.st
Perturbation Analysis of Superconductivity in the Trellis-Lattice Hubbard Model
We investigate pairing symmetry and transition temperature in the
trellis-lattice Hubbard model. We solve the \'Eliashberg equation using the
third-order perturbation theory with respect to the on-site repulsion . We
find that a spin-singlet state is very stable in a wide range of parameters. On
the other hand, when the electron number density is shifted from the
half-filled state and the band gap between two bands is small, a spin-triplet
superconductivity is expected. Finally, we discuss a possibility of
unconventional superconductivity and pairing symmetry in
SrCaCuO.Comment: 7pages, 10 figures. To be published in J. Phys. Soc. Jp
Nonlinear optical response and spin-charge separation in one-dimensional Mott insulators
We theoretically study the nonlinear optical response and photoexcited states
of the Mott insulators. The nonlinear optical susceptibility \chi^(3) is
calculated by using the exact diagonalization technique on small clusters. From
the systematic study of the dependence of \chi^(3) on dimensionality, we find
that the spin-charge separation plays a crucial role in enhancing \chi^(3) in
the one-dimensional (1D) Mott insulators. Based on this result, we propose a
holon-doublon model, which describes the nonlinear response in the 1D Mott
insulators. These findings show that the spin-charge separation will become a
key concept of optoelectronic devices.Comment: 5 pages with 3 figures, to appear in PRB RC, 15 August 200
Magnetic excitations and structural change in the S=1/2 quasi-one-dimensional magnet Sr_{14-x}Y_{x}Cu_{24}O_{41} (0<x<1)
Neutron scattering measurements have been performed on the S=1/2
quasi-one-dimensional system Sr_{14-x}Y_{x}Cu_{24}O_{41}, which has both simple
chains and two-leg ladders of copper ions. We observed that when a small amount
of yttrium is substituted for strontium, which is expected to reduce the number
of holes, the dimerized state and the structure in the chain are changed
drastically. The inelastic peaks originating from the dimerized state of the
chain becomes broader in energy but not in momentum space. This implies that
the dimerized state becomes unstable but the spin correlations are unchanged
with yttrium substitution. Furthermore, it was observed that nuclear Bragg peak
intensities originating from the chain show strong temperature and x
dependence, which suggests that the chains slide along the c axis as
temperature and x are varied.Comment: 5 pages, 6 figures, to appear in Phys. Rev.
Transport Properties of Doped t-J Ladders
Conductivity and Hall coefficient for various types of t-J ladders are
calculated as a function of temperature and frequency by numerical
diagonalization. A crossover from an incoherent to a coherent charge dynamics
is found at a temperature T_{coh}. There exists another crossover at T_{PG}
below which a pseudogap opens in the optical spectra, induced by the opening of
a spin gap. In the absence of the spin gap, T_{coh} and the coherent weight are
suppressed especially with increasing dimensionality. On the contrary, T_{coh}
is strongly enhanced by the pseudogap formation below T_{PG}, where the
coherent Drude weight decreases with increasing dimensionality. The Hall
coefficient shows a strong crossover at T_{PG} below which it has large
amplitude for small doping concentration.Comment: 4 pages, RevTeX, 5 PostScript figure
Charge-density wave formation in Sr_{14}Cu_{24}O_{41}
The electrodynamic response of the spin-ladder compound
SrCaCuO () has been studied from
radiofrequencies up to the infrared. At temperatures below 250 K a pronounced
absorption peak appears around 12 cm in SrCuO for
the radiation polarized along the chains/ladders ().
In addition a strongly temperature dependent dielectric relaxation is observed
in the kHz - MHz range. We explain this behavior by a charge density wave which
develops in the ladders sub-system and produces a mode pinned at 12 cm.
With increasing Ca doping the mode shifts up in frequency and eventually
disappears for because the dimensionality of the system crosses over from
one to two dimensions, giving way to the superconducting ground state under
pressure.Comment: One name added to author list 4 pages, 2 figures, email:
[email protected]
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