2,082 research outputs found
USp(2k) Matrix Model: F Theory Connection
We present a zero dimensional matrix model based on with
supermultiplets in symmetric, antisymmetric and fundamental representations.
The four dimensional compactification of this model naturally captures the
exact results of Sen \cite{Sen} in theory. Eight dynamical and eight
kinematical supercharges are found, which is required for critical string
interpretation. Classical vacuum has ten coordinates and is equipped with
orbifold structure. We clarify the issue of spacetime dimensions which
theory represented by this matrix model produces.Comment: 11 pages, Latex: interpretation as large T^{6}/Z^{2} IIB orientifold
added, the final version to appear in Progress of Theoretical Physic
Influence of length and measurement geometry on magnetoimpedance in La0.7Sr0.3MnO3
We show that ac magnetoresistance at room temperature in La0.7Sr0.3MnO3 is
extremely high (= 47% in H = 100 mT, f = 3-5 MHz), and magnetic field
dependence of reactance exhibits a double peak behavior. However, magnitudes of
the ac magnetoresistance and magnetoreactance for a fixed length of the sample
(li) decrease with decreasing separation (lv) between voltage probes unlike the
dc magnetoresistance. On the contrary, change in li has a negligible influence
on magnetoimpedance when lv is fixed. Our results indicate that high frequency
electrical transport is sensitive to local variations in the magnetic
permeability.Comment: 12 pages, 3 figure
Coexistence of long-ranged charge and orbital order and spin-glass state in single-layered manganites with weak quenched disorder
The relationship between orbital and spin degrees of freedom in the
single-crystals of the hole-doped PrCaMnO, 0.3
0.7, has been investigated by means of ac-magnetometry and charge
transport. Even though there is no cation ordering on the -site, the
quenched disorder is extremely weak in this system due to the very similar
ionic size of Pr and Ca. A clear asymmetric response of the
system to the under- (respective over-) hole doping was observed. The
long-ranged charge-orbital order established for half doping (=0.5) subsists
in the over-doping case ( 0.5), albeit rearranged to accommodate the
extra holes introduced in the structure. The charge-orbital order is however
destabilized by the presence of extra localized electrons (under-doping,
0.5), leading to its disappearance below =0.35. We show that in an
intermediate under-doped region, with 0.35 0.5, the
``orbital-master spin-slave'' relationship commonly observed in half-doped
manganites does not take place. The long-ranged charge-orbital order is not
accompanied by an antiferromagnetic transition at low temperatures, but by a
frustrated short-ranged magnetic state bringing forth a spin-glass phase. We
discuss in detail the nature and origin of this spin-glass state, which, as in
the half-doped manganites with large quenched disorder, is not related to the
macroscopic phase separation observed in crystals with minor defects or
impurities.Comment: EPL style; 6 pages, 5 figure
Temperature-dependent photoemission spectral weight transfer and chemical potential shift in PrCaMnO : Implications for charge density modulation
We have studied the temperature dependence of the photoemission spectra of
PrCaMnO (PCMO) with , 0.3 and 0.5. For and 0.5,
we observed a gap in the low-temperature CE-type charge-ordered (CO) phase and
a pseudogap with a finite intensity at the Fermi level () in the
high-temperature paramagnetic insulating (PI) phase. Within the CO phase, the
spectral intensity near gradually increased with temperature. These
observations are consistent with the results of Monte Carlo simulations on a
model including charge ordering and ferromagnetic fluctuations [H. Aliaga {\it
et al.} Phys. Rev. B {\bf 68}, 104405 (2003)]. For , on the other hand,
little temperature dependence was observed within the low-temperature
ferromagnetic insulating (FI) phase and the intensity at remained low in
the high-temperature PI phase. We attribute the difference in the temperature
dependence near between the CO and FI phases to the different correlation
lengths of orbital order between both phases. Furthermore, we observed a
chemical potential shift with temperature due to the opening of the gap in the
FI and CO phases. The doping dependent chemical potential shift was recovered
at low temperatures, corresponding to the disappearance of the doping dependent
change of the modulation wave vector. Spectral weight transfer with hole
concentration was clearly observed at high temperatures but was suppressed at
low temperatures. We attribute this observation to the fixed periodicity with
hole doping in PCMO at low temperatures.Comment: 5pages, 7figure
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