314 research outputs found
Interchain-Frustration-Induced Metallic State in Quasi-One-Dimensional Mott Insulators
The mechanism that drives a metal-insulator transition in an undoped
quasi-one-dimensional Mott insulator is examined in the framework of the
Hubbard model with two different hoppings t_{perp 1} and t_{perp 2} between
nearest-neighbor chains. By applying an N_{perp}-chain renormalization group
method at the two-loop level, we show how a metallic state emerges when both
t_{perp 1} and t_{perp 2} exceed critical values. In the metallic phase, the
quasiparticle weight becomes finite and develops a strong momentum dependence.
We discuss the temperature dependence of the resistivity and the impact of our
theory in the understanding of recent experiments on half-filled molecular
conductors.Comment: 4 pages, 3 figures, published versio
Mechanism of confinement in low-dimensional organic conductors
Confinement-deconfinement transition in quarter-filled two-coupled chains
comprising dimerization, repulsive interactions and interchain hopping has been
demonstrated by applying the renormalization group method to the bosonized
Hamiltonian. The confinement given by the irrelevant interchain hopping occurs
with increasing umklapp scattering which is induced by the dimerization leading
to effectively half-filling. It is shown that the transition originates in a
competition between a charge gap and the renormalized interchain hopping.Comment: 5 pages, 7 figures, Proc. CREST Int. Workshop, Nagoya 2000, submitted
to J. Phys. Chem. Solid
Spin susceptibility of interacting electrons in one dimension: Luttinger liquid and lattice effects
The temperature-dependent uniform magnetic susceptibility of interacting
electrons in one dimension is calculated using several methods. At low
temperature, the renormalization group reaveals that the Luttinger liquid spin
susceptibility approaches zero temperature with an infinite slope
in striking contrast with the Fermi liquid result and with the behavior of the
compressibility in the absence of umklapp scattering. This effect comes from
the leading marginally irrelevant operator, in analogy with the Heisenberg spin
1/2 antiferromagnetic chain. Comparisons with Monte Carlo simulations at higher
temperature reveal that non-logarithmic terms are important in that regime.
These contributions are evaluated from an effective interaction that includes
the same set of diagrams as those that give the leading logarithmic terms in
the renormalization group approach. Comments on the third law of thermodynamics
as well as reasons for the failure of approaches that work in higher dimensions
are given.Comment: 21 pages, latex including 5 eps figure
Wilson-Kadanoff Renormalization Group in Higher Orders: One-Dimensional g-ology Model as an Example
We apply the standard Wilson-Kadanoff (WK) momentum-space Renormalization
Group (RG) scheme for the g-ology model of one-dimensional fermions. By
explicitly carrying out calculations at the two-loop level, we show how the RG
flow equations can be derived from the summation of the cascades of
contractions generated by the effective action's mode elimination at each
infinitesimal step of the WK procedure. The rules for selecting these series of
cascades appear naturally as a consequence of the WK scheme ``on-shell''
kinematic constraints and conservation laws. The relation between the present
RG approach and the field-theoretic schemes used in earlier related studies is
analysed. Generalizations for other models and/or higher dimensions are
formulated.Comment: 21 pages, 5 figure
Pressure-induced Spin-Peierls to Incommensurate Charge-Density-Wave Transition in the Ground State of TiOCl
The ground state of the spin-Peierls system TiOCl was probed using
synchrotron x-ray diffraction on a single-crystal sample at T = 6 K. We tracked
the evolution of the structural superlattice peaks associated with the
dimerized ground state as a function of pressure. The dimerization along the b
axis is rapidly suppressed in the vicinity of a first-order structural phase
transition at Pc = 13.1(1) GPa. The high-pressure phase is characterized by an
incommensurate charge density wave perpendicular to the original spin chain
direction. These results show that the electronic ground state undergoes a
fundamental change in symmetry, indicating a significant change in the
principal interactions.Comment: 5 pages, 4 figure
Superconductivity and Antiferromagnetism in Quasi-one-dimensional Organic Conductors
We review the current understanding of superconductivity in the
quasi-one-dimensional organic conductors of the Bechgaard and Fabre salt
families. We discuss the interplay between superconductivity,
antiferromagnetism, and charge-density-wave fluctuations. The connection to
recent experimental observations supporting unconventional pairing and the
possibility of a triplet-spin order parameter for the superconducting phase is
also presented.Comment: (v1) 30 pages, 13 figures; Review article for the 20th anniversary of
high-Tc superconductivity, to appear in J. Low Temp. Phys. (v2) 1 Ref. adde
(Sr/Ca)_{14}Cu_{24}O_{41} spin ladders studied by NMR under pressure
(63)Cu-NMR measurements have been performed on two-leg hole-doped spin
ladders Sr_{14-x}Ca_{x}Cu_{24}O_{41} single crystals (0-x-12) at several
pressures up to the pressure domain where the stabilization of a
superconducting ground state can be achieved. The data reveal marked decrease
of the spin gap derived from Knight shift measurements upon Ca substitution and
also under pressure and confirm the onset of low lying spin excitations around
P_{c} as previously reported. The spin gap in Sr_{2}Ca_{12}Cu_{24}O_{41} is
strongly reduced above 20 kbar. However, the data of an experiment performed at
P=36 kbar where superconductivity has been detected at 6.7K by an inductive
technique have shown that a significant amount of spin excitations remains
gapped at 80K when superconductivity sets in. The standard relaxation model
with two and three-magnon modes explains fairly well the activated relaxation
data in the intermediate temperature regime corresponding to gapped spin
excitations using the spin gap data derived from Knight shift experiments.The
data of Gaussian relaxation rates of heavily doped samples support the
limitation of the coherence lenght at low temperature by the average distance
between doped holes. We discuss the interplay between superconductivity and the
spin gap and suggest that these new results support the exciting prospect of
superconductivity induced by the interladder tunnelling of preformed pairs as
long as the pressure remains lower than the pressure corresponding to the
maximum of the superconducting critical temperature.Comment: 15 pages Latex, 13 figures. to be published in Eur.Phys.Jour.B,200
Heterologous expression of peptide hormone precursors in the yeast Saccharomyces cerevisiae. Evidence for a novel prohormone endoprotease with specificity for monobasic amino acids.
The peptide somatostatin (SRIF) exists as two different molecular species. In addition to the most common form, which is a 14-residue peptide, there is also a 14-amino acid amino-terminally extended form of the tetradecapeptide, SRIF-28. Both peptides are synthesized as larger precursors containing paired basic and monobasic amino acids at their processing sites, which, upon cleavage, generate either SRIF-14 or -28, respectively. In mammals a single prepro-SRIF molecule undergoes tissue-specific processing to generate the mature hormone whereas in some species of fish separate genes encode two distinct but homologous precursors prepro-SRIF-I and -II that give rise to SRIF-14 and -28, respectively. To investigate the molecular basis for differential processing of the prohormones we introduce their cDNAs into yeast cells (Saccharomyces cerevisiae). The signal peptides of both precursors were poorly recognized by the yeast endoplasmic reticulum translocation apparatus, consequently only low levels of SRIF peptides were synthesized. To circumvent this problem a chimeric precursor consisting of the alpha-factor signal peptide plus 30 residues of the proregion was fused to pro-SRIF-II. This fusion protein was efficiently transported through the yeast secretory pathway and processed to SRIF-28 exclusively, which is identical to the processing of the native precursor in pancreatic islet D-cells. Most significantly, cleavage of the precursor to SRIF-28 was independent of the Kex 2 endoprotease since processing occurred efficiently in a kex 2 mutant strain. We conclude that in addition to the Kex 2 protease, yeast possess a distinct prohormone converting enzyme with specificity toward monobasic processing sites
Confinement-deconfinement transition in two-coupled chains with umklapp scattering
A role of umklapp scattering has been examined for two-coupled chains with
both forward and backward scatterings by applying renormalization group method
to bosonized Hamiltonian. It has been found that a state with relevant
interchain hopping changes into a state with irrelevant (confined) one when the
magnitude of umklapp scattering becomes larger than that of interchain hopping.
Critical value of umklapp scattering for such a confinement-deconfinement
transition is calculated as the function of interchain hopping and intrachain
interactions. A crossover from one-dimensional regime into that of coupled
chains is also shown with decreasing temperature.Comment: 13 pages, 7 figures, to be published in Phys. Rev.
Spin-Density-Wave Phase Transitions in Quasi-One-Dimensional Dimerized Quarter-Filled Organic Conductors
We have studied spin density wave (SDW) phase transitions in dimerized
quarter-filled Hubbard chains weakly coupled via interchain one-particle
hopping, . It is shown that there exists a critical value of ,
, between the incoherent metal regime () and the
Fermi liquid regime () in the metallic phase above the SDW
transition temperature. By using the 2-loop perturbative renormalization-group
approach together with the random-phase-approximation, we propose a SDW phase
diagram covering both of the regimes. The SDW phase transition from the
incoherent metal phase for is caused by growth of the
intrachain electron-electron umklapp scattering toward low temperatures, which
is regarded as preformation of the Mott gap. We discuss relevance of the
present result to the SDW phase transitions in the quasi-one-dimensional
dimerized quarter-filled organic conductors, (TMTTF)X and (TMTSF)X.Comment: 19 pages, 13 eps figures, uses jpsj.sty, corrected typo in the text
and figures, no changes to the paper, to appear in J. Phys. Soc. Jpn. 68,
No.8 (1999
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