1,185 research outputs found
Born-Infeld Lagrangian using Cayley-Dickson algebras
We rewrite the Born-Infeld Lagrangian, which is originally given by the
determinant of a matrix composed of the metric tensor and the
field strength tensor , using the determinant of a matrix . If the elements of
are given by the linear combination of and , it is found, based on the
representation matrix for the multiplication operator of the Cayley-Dickson
algebras, that is distinguished by a single parameter,
where distinguished matrices are not similar matrices. We also give a
reasonable condition to fix the paramet
The Yellow Excitonic Series of Cu2O Revisited by Lyman Spectroscopy
We report on the observation of the yellow exciton Lyman series up to the
fourth term in Cu2O by time-resolved mid-infrared spectroscopy. The dependence
of the oscillator strength on the principal quantum number n can be well
reproduced using the hydrogenic model including an AC dielectric constant, and
precise information on the electronic structure of the 1s exciton state can be
obtained. A Bohr radius a_{1s}=7.9 A and a 1s-2p transition dipole moment
\mu_{1s-2p}= 4.2 eA were found
Study of ortho-to-paraexciton conversion in CuO by excitonic Lyman spectroscopy
Using time-resolved - excitonic Lyman spectroscopy, we study the
orthoexciton-to-paraexcitons transfer, following the creation of a high density
population of ultracold orthoexcitons by resonant two-photon excitation
with femtosecond pulses.
An observed fast exciton-density dependent conversion rate is attributed to
spin exchange between pairs of orthoexcitons.
Implication of these results on the feasibility of BEC of paraexcitons in
CuO is discussed
Coexistence and competition of local- and long-range polar orders in a ferroelectric relaxor
We have performed a series of neutron diffuse scattering measurements on a
single crystal of the solid solution Pb(ZnNb)O (PZN) doped
with 8% PbTiO (PT), a relaxor compound with a Curie temperature T K, in an effort to study the change in local polar orders from the polar
nanoregions (PNR) when the material enters the ferroelectric phase. The diffuse
scattering intensity increases monotonically upon cooling in zero field, while
the rate of increase varies dramatically around different Bragg peaks. These
results can be explained by assuming that corresponding changes occur in the
ratio of the optic and acoustic components of the atomic displacements within
the PNR. Cooling in the presence of a modest electric field oriented
along the [111] direction alters the shape of diffuse scattering in reciprocal
space, but does not eliminate the scattering as would be expected in the case
of a classic ferroelectric material. This suggests that a field-induced
redistribution of the PNR has taken place
Formation and decay of electron-hole droplets in diamond
We study the formation and decay of electron-hole droplets in diamonds at
both low and high temperatures under different excitations by master equations.
The calculation reveals that at low temperature the kinetics of the system
behaves as in direct-gap semiconductors, whereas at high temperature it shows
metastability as in traditional indirect-gap semiconductors. Our results at low
temperature are consistent with the experimental findings by Nagai {\em et al.}
[Phys. Rev. B {\bf 68}, 081202 (R) (2003)]. The kinetics of the e-h system in
diamonds at high temperature under both low and high excitations is also
predicted.Comment: 7 pages, 8 figures, revised with some modifications in physics
discussion, to be published in PR
An Anomalous Phase in the Relaxor Ferroelectric Pb(ZnNb)O
X-ray diffraction studies on a Pb(ZnNb)O (PZN) single
crystal sample show the presence of two different structures. An outer-layer
exists in the outer most 10 to 50~m of the crystal, and undergoes a
structural phase transition at the Curie temperature K. The
inside phase is however, very different. The lattice inside the crystal
maintains a cubic unit cell, while ferroelectric polarization develops below
. The lattice parameter of the cubic unit cell remains virtually a
constant, i.e., much less variations compared to that of a typical relaxor
ferroelectric, in a wide temperature range of 15 K to 750 K. On the other hand,
broadening of Bragg peaks and change of Bragg profile line-shapes in both
longitudinal and transverse directions at clearly indicate a structural
phase transition occurring.Comment: to be submitted for PR
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