173 research outputs found
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
Indication of antiferromagnetic interaction between paramagnetic Co ions in the diluted magnetic semiconductor ZnCoO
The magnetic properties of ZnCoO ( and 0.10) thin films,
which were homo-epitaxially grown on a ZnO(0001) substrates with varying
relatively high oxygen pressure, have been investigated using x-ray magnetic
circular dichroism (XMCD) at Co core-level absorption edge. The line
shapes of the absorption spectra are the same in all the films and indicate
that the Co ions substitute for the Zn sites. The magnetic-field and
temperature dependences of the XMCD intensity are consistent with the
magnetization measurements, indicating that except for Co there are no
additional sources for the magnetic moment, and demonstrate the coexistence of
paramagnetic and ferromagnetic components in the homo-epitaxial
ZnCoO thin films, in contrast to the ferromagnetism in the
hetero-epitaxial ZnCoO films studied previously. The analysis of
the XMCD intensities using the Curie-Weiss law reveals the presence of
antiferromagnetic interaction between the paramagnetic Co ions. Missing XMCD
intensities and magnetization signals indicate that most of Co ions are
non-magnetic probably because they are strongly coupled antiferromagnetically
with each other. Annealing in a high vacuum reduces both the paramagnetic and
ferromagnetic signals. We attribute the reductions to thermal diffusion and
aggregation of Co ions with antiferromagnetic nanoclusters in
ZnCoO.Comment: 21 pages, 7 figures, accepted for Physical Review
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
Optical and transport properties in doped two-leg ladder antiferromagnet
Within the t-J model, the optical and transport properties of the doped
two-leg ladder antiferromagnet are studied based on the fermion-spin theory. It
is shown that the optical and transport properties of the doped two-leg ladder
antiferromagnet are mainly governed by the holon scattering. The low energy
peak in the optical conductivity is located at a finite energy, while the
resistivity exhibits a crossover from the high temperature metallic-like
behavior to the low temperature insulating-like behavior, which are consistent
with the experiments.Comment: 13 pages, 5 figures, accepted for publication in Phys. Rev. B65
(2002) (April 15 issue
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
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
Charge-Density-Wave Formation in the Doped Two-Leg Extended Hubbard Ladder
We investigate electronic properties of the doped two-leg Hubbard ladder with
both the onsite and the nearest-neighbor Coulomb repulsions, by using the the
weak-coupling renormalization-group method. It is shown that, for strong
nearest-neighbor repulsions, the charge-density-wave state coexisting with the
p-density-wave state becomes dominant fluctuation where spins form intrachain
singlets. By increasing doping rate, we have also shown that the effects of the
nearest-neighbor repulsions are reduced and the system exhibits a quantum phase
transition into the d-wave-like (or rung-singlet) superconducting state. We
derive the effective fermion theory which describes the critical properties of
the transition point with the gapless excitation of magnon. The phase diagram
of the two-leg ladder compound, Sr_{14-x}Ca_xCu_{24}O_{41}, is discussed.Comment: 4 pages, 2 figure
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
Phase Diagram of Coupled Ladders
The 2-leg t-J ladder forms a spin liquid at half-filling which evolves to a
Luther-Emery liquid upon doping. Our aim is to obtain a complete phase diagram
for isotropic coupling (i.e. rungs and legs equal) as a function of electron
density n and the ratio J/t (>0). Two known limiting cases are: n<1/2 which is
a single band Luttinger liquid and small hole doping for J/t close to 0 which
is a Nagaoka ferromagnet. Using Lanczos techniques we examine the region
between the Nagaoka and Luther-Emery phases for 1>n>1/2. We find evidences for
gapless behavior in both spin and charge channels for J/t<0.3 consistent with
Luttinger liquids in both bonding and anti-bonding bands (i.e., C2S2). This
proposal is based on the behavior of spin and charge correlation functions. For
example the hole-hole correlation function which displays hole pairing at
larger J/t, shows hole-hole repulsion in this region. As a further test, we
examined the dependence of the energy on a relative phase shift between bonding
and antibonding bands. For J/t < 0.3 this is very weak, indicating a lack of
pairing between these channels.Comment: 21 pages, 18 figure
Optical conductivity of one-dimensional doped Hubbard-Mott insulator
We study the optical response of a strongly correlated electron system near
the metal-insulator transition using a mapping to the sine-Gordon model. With
semiclassical quantization, the spectral weight is distributed between a Drude
peak and absorption lines due to breathers. We calculate the Drude weight, the
optical gap, and the lineshape of breather absorption.Comment: 4 pages, 2 EPS figures, REVTEX 4, a final versio
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