701 research outputs found
Luttinger-liquid-like transport in long InSb nanowires
Long nanowires of degenerate semiconductor InSb in asbestos matrix (wire
diameter is around 50 \AA, length 0.1 - 1 mm) were prepared. Electrical
conduction of these nanowires is studied over a temperature range 1.5 - 350 K.
It is found that a zero-field electrical conduction is a power function of the
temperature with the typical exponent .
Current-voltage characteristics of such nanowires are found to be nonlinear and
at sufficiently low temperatures follows the power law . It
is shown that the electrical conduction of these nanowires cannot be accounted
for in terms of ordinary single-electron theories and exhibits features
expected for impure Luttinger liquid. For a simple approximation of impure LL
as a pure one broken into drops by weak links, the estimated weak-link density
is around per cm.Comment: 5 pages, 2 figure
Diffusion and Transport Coefficients in Synthetic Opals
Opals are structures composed of the closed packing of spheres in the size
range of nano-to-micro meter. They are sintered to create small necks at the
points of contact. We have solved the diffusion problem in such structures. The
relation between the diffusion coefficient and the termal and electrical
conductivity makes possible to estimate the transport coefficients of opal
structures. We estimate this changes as function of the neck size and the
mean-free path of the carriers. The theory presented is also applicable to the
diffusion problem in other periodic structures.Comment: Submitted to PR
Optical properties of small polarons from dynamical mean-field theory
The optical properties of polarons are studied in the framework of the
Holstein model by applying the dynamical mean-field theory. This approach
allows to enlighten important quantitative and qualitative deviations from the
limiting treatments of small polaron theory, that should be considered when
interpreting experimental data. In the antiadiabatic regime, accounting on the
same footing for a finite phonon frequency and a finite electron bandwidth
allows to address the evolution of the optical absorption away from the
well-understood molecular limit. It is shown that the width of the multiphonon
peaks in the optical spectra depends on the temperature and on the frequency in
a way that contradicts the commonly accepted results, most notably in the
strong coupling case. In the adiabatic regime, on the other hand, the present
method allows to identify a wide range of parameters of experimental interest,
where the electron bandwidth is comparable or larger than the broadening of the
Franck-Condon line, leading to a strong modification of both the position and
the shape of the polaronic absorption. An analytical expression is derived in
the limit of vanishing broadening, which improves over the existing formulas
and whose validity extends to any finite-dimensional lattice. In the same
adiabatic regime, at intermediate values of the interaction strength, the
optical absorption exhibits a characteristic reentrant behavior, with the
emergence of sharp features upon increasing the temperature -- polaron
interband transitions -- which are peculiar of the polaron crossover, and for
which analytical expressions are provided.Comment: 16 pages, 6 figure
Metallic Xenon, Molecular Condensates, and Superconductivity
A possibility of explaining the light absorption observed to occur under
pressure-induced xenon metallization as due to the transition to the
superconducting state is analyzed. The mechanism of the van der Waals bonding
is discussed.Comment: LaTeX 2.09 (RevTeX), 4 pages, 4 PostScript figures included in tex
Melting Point and Lattice Parameter Shifts in Supported Metal Nanoclusters
The dependencies of the melting point and the lattice parameter of supported
metal nanoclusters as functions of clusters height are theoretically
investigated in the framework of the uniform approach. The vacancy mechanism
describing the melting point and the lattice parameter shifts in nanoclusters
with decrease of their size is proposed. It is shown that under the high vacuum
conditions (p<10^-7 torr) the essential role in clusters melting point and
lattice parameter shifts is played by the van der Waals forces of
cluster-substrate interation. The proposed model satisfactorily accounts for
the experimental data.Comment: 6 pages, 3 figures, 1 tabl
Bulk and local magnetic susceptibility of ErB12
High precision measurements of magnetoresistance ΞΟ/Ο = f(T,H) and magnetization M(T,H) were carried out on single crystals of rare-earth dodecaboride at temperatures in the interval 1.8-30 K in magnetic fields up to 70 kOe. The high accuracy of the experiments allowed us to perform numerical differentiation and analyze quantitatively the behavior of the derivative d(ΞΟ/Ο)/dH = f(T,H) and of the magnetic susceptibility Ο(T,H) = dM/dH in paramagnetic and magnetically ordered (antiferromagnetic, β 6.7 K and β 5.85 K) phases of . It was shown that negative magnetoresistance anomalies observed in present study in paramagnetic state of may be consistently interpreted in the framework of a simple relation between resistivity and magnetization -ΞΟ/Ο ~
Signatures of polaronic excitations in quasi-one-dimensional LaTiO
The optical properties of quasi-one-dimensional metallic LaTiO are
studied for the polarization along the and axes. With decreasing
temperature modes appear along both directions suggestive for a phase
transition. The broadness of these modes along the conducting axis might be due
to the coupling of the phonons to low-energy electronic excitations across an
energy gap. We observe a pronounced midinfrared band with a temperature
dependence consistent with (interacting) polaron models. The polaronic picture
is corroborated by the presence of strong electron-phonon coupling and the
temperature dependence of the dc conductivity.Comment: 5 pages, 5 figure
Rationality of the moduli spaces of plane curves of sufficiently large degree
We prove that the moduli space of plane curves of degree d is rational for
all sufficiently large d.Comment: 18 pages; 1 figure; Macaulay2 scripts used can be found at
http://www.uni-math.gwdg.de/bothmer/rationality/ or at the end of the latex
source fil
ΠΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ ΡΠ΅ΡΠ°ΠΏΠΈΠΈ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ Π²ΠΈΡΡΡΠ°Π»ΡΠ½ΠΎΠΉ ΡΠ΅Π°Π»ΡΠ½ΠΎΡΡΠΈ Ρ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² ΠΏΠΎΡΠ»Π΅ ΡΡΠ°Π²ΠΌΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ Ρ ΠΈΡΡΡΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ Π²ΠΌΠ΅ΡΠ°ΡΠ΅Π»ΡΡΡΠ²: ΠΏΡΠΎΡΠΏΠ΅ΠΊΡΠΈΠ²Π½ΠΎΠ΅ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅
ΠΠΠ’Π£ΠΠΠ¬ΠΠΠ‘Π’Π¬: ΠΠΎΡΠ»Π΅ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΎΠ½Π½Π°Ρ Π±ΠΎΠ»Ρ ΡΠ²Π»ΡΠ΅ΡΡΡ ΡΠ°ΡΠΏΡΠΎΡΡΡΠ°Π½Π΅Π½Π½ΠΎΠΉ ΠΏΡΠΎΠ±Π»Π΅ΠΌΠΎΠΉ. ΠΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ Π½Π΅ΠΌΠ΅Π΄ΠΈΠΊΠ°ΠΌΠ΅Π½ΡΠΎΠ·Π½ΡΡ
ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ² Π»Π΅ΡΠ΅Π½ΠΈΡ ΠΌΠΎΠΆΠ΅Ρ ΡΠ½ΠΈΠ·ΠΈΡΡ ΠΏΠΎΡΡΠ΅Π±Π½ΠΎΡΡΡ Π² Π»Π΅ΠΊΠ°ΡΡΡΠ²Π΅Π½Π½ΡΡ
ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΠ°Ρ
. ΠΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΡΠ΅ΡΠ°ΠΏΠΈΠΈ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ Π²ΠΈΡΡΡΠ°Π»ΡΠ½ΠΎΠΉ ΡΠ΅Π°Π»ΡΠ½ΠΎΡΡΠΈ (ΠΠ -ΡΠ΅ΡΠ°ΠΏΠΈΡ) ΡΠΈΡΠΎΠΊΠΎ ΠΈΠ·ΡΡΠ°Π΅ΡΡΡ ΠΊΠ°ΠΊ ΠΌΠ΅ΡΠΎΠ΄ Π΄ΠΎΠΏΠΎΠ»Π½ΠΈΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ Π»Π΅ΡΠ΅Π½ΠΈΡ ΠΏΡΠΈ ΠΎΡΡΡΠΎΠΉ ΠΈ Ρ
ΡΠΎΠ½ΠΈΡΠ΅ΡΠΊΠΎΠΉ Π±ΠΎΠ»ΠΈ. ΠΡΡΡΡΡΡΠ²ΠΈΠ΅ Π΄Π°Π½Π½ΡΡ
ΠΎΠ± ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠΈ Ρ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² ΠΏΠΎΡΠ»Π΅ ΡΡΠ°Π²ΠΌΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
Ρ
ΠΈΡΡΡΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
Π²ΠΌΠ΅ΡΠ°ΡΠ΅Π»ΡΡΡΠ² ΡΡΠ°Π»ΠΎ ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π΄Π»Ρ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΈΡ Π΄Π°Π½Π½ΠΎΠ³ΠΎ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ. Π¦ΠΠΠ¬ ΠΠ‘Π‘ΠΠΠΠΠΠΠΠΠ―: ΠΠΏΡΠ΅Π΄Π΅Π»ΠΈΡΡ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ ΠΠ -ΡΠ΅ΡΠ°ΠΏΠΈΠΈ ΠΊΠ°ΠΊ ΠΌΠ΅ΡΠΎΠ΄Π° Π΄ΠΎΠΏΠΎΠ»Π½ΠΈΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ Π»Π΅ΡΠ΅Π½ΠΈΡ ΠΏΠΎΡΠ»Π΅ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΎΠ½Π½ΠΎΠΉ Π±ΠΎΠ»ΠΈ Ρ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² ΠΏΠΎΡΠ»Π΅ ΡΡΠ°Π²ΠΌΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
Ρ
ΠΈΡΡΡΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
Π²ΠΌΠ΅ΡΠ°ΡΠ΅Π»ΡΡΡΠ². ΠΠΠ’ΠΠ ΠΠΠΠ« Π ΠΠΠ’ΠΠΠ«: Π ΠΏΡΠΎΡΠΏΠ΅ΠΊΡΠΈΠ²Π½ΠΎΠ΅ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ Π²ΠΊΠ»ΡΡΠ΅Π½Ρ 70Β ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ², ΠΏΠΎΡΡΡΠΏΠΈΠ²ΡΠΈΡ
Π΄Π»Ρ Π²ΡΠΏΠΎΠ»Π½Π΅Π½ΠΈΡ ΠΏΠ»Π°Π½ΠΎΠ²ΡΡ
ΡΡΠ°Π²ΠΌΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΉ. ΠΠ -ΡΠ΅ΡΠ°ΠΏΠΈΡ Π² ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ΅ Ρ ΠΌΠ΅Π΄ΠΈΠΊΠ°ΠΌΠ΅Π½ΡΠΎΠ·Π½ΡΠΌΠΈ Π°Π½Π°Π»ΡΠ³Π΅ΡΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΠ°ΠΌΠΈ ΠΏΡΠΈΠΌΠ΅Π½ΠΈΠ»ΠΈ 35Β ΠΏΠ°ΡΠΈΠ΅Π½ΡΠ°ΠΌ. Π ΠΊΠΎΠ½ΡΡΠΎΠ»ΡΠ½ΡΡ Π³ΡΡΠΏΠΏΡ Π²ΠΊΠ»ΡΡΠ΅Π½ΠΎ 35 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ², ΠΊΠΎΡΠΎΡΡΠΌ ΠΏΠΎΡΠ»Π΅ Π²ΡΠΏΠΎΠ»Π½Π΅Π½ΠΈΡ Π°Π½Π°Π»ΠΎΠ³ΠΈΡΠ½ΡΡ
Ρ
ΠΈΡΡΡΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
Π²ΠΌΠ΅ΡΠ°ΡΠ΅Π»ΡΡΡΠ² ΠΎΠ±Π΅Π·Π±ΠΎΠ»ΠΈΠ²Π°Π½ΠΈΠ΅ ΠΎΡΡΡΠ΅ΡΡΠ²Π»ΡΠ»ΠΈ ΡΠΎΠ»ΡΠΊΠΎ ΠΌΠ΅Π΄ΠΈΠΊΠ°ΠΌΠ΅Π½ΡΠΎΠ·Π½ΠΎ. Π’Π΅ΡΠ°ΠΏΠΈΡ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΠ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΡΡΡΡΠΎΠΉΡΡΠ²Π° Β«Oculus QuestΒ 2Β». Π‘Π΅Π°Π½ΡΡ ΠΏΠΎ 25Β ΠΌΠΈΠ½ Π²ΡΠΏΠΎΠ»Π½ΡΠ»ΠΈ ΡΠ΅ΡΠ΅Π· 3, 7, 12Β Ρ ΠΏΠΎΡΠ»Π΅ ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΈ. ΠΡΠ΅Π½ΠΊΡ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΏΡΠΎΡΠΈΠ²ΠΎΠ±ΠΎΠ»Π΅Π²ΠΎΠΉ ΡΠ΅ΡΠ°ΠΏΠΈΠΈ ΠΎΡΡΡΠ΅ΡΡΠ²Π»ΡΠ»ΠΈ Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΡΠΈΡΠ»ΠΎΠ²ΠΎΠΉ ΡΠ΅ΠΉΡΠΈΠ½Π³ΠΎΠ²ΠΎΠΉ ΡΠΊΠ°Π»Ρ. Π Π΅Π°ΠΊΡΠΈΡ ΡΠ½Π΄ΠΎΠΊΡΠΈΠ½Π½ΠΎ-ΠΌΠ΅ΡΠ°Π±ΠΎΠ»ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΎΡΠ²Π΅ΡΠ° Π½Π° Π±ΠΎΠ»Ρ ΠΎΡΠ΅Π½ΠΈΠ²Π°Π»ΠΈ ΠΏΠΎ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΠΈ ΠΊΠΎΡΡΠΈΠ·ΠΎΠ»Π° ΠΈ Π°Π΄ΡΠ΅Π½ΠΎΠΊΠΎΡΡΠΈΠΊΠΎΡΡΠΎΠΏΠ½ΠΎΠ³ΠΎ Π³ΠΎΡΠΌΠΎΠ½Π° (ΠΠΠ’Π). Π ΠΠΠ£ΠΠ¬Π’ΠΠ’Π«: Π’Π΅ΡΠ°ΠΏΠΈΡ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΌΠ΅Π΄ΠΈΠΊΠ°ΠΌΠ΅Π½ΡΠΎΠ·Π½ΠΎΠΉ Π°Π½Π°Π»ΡΠ³Π΅Π·ΠΈΠΈ Π² ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ΅ Ρ ΡΠ΅Π°Π½ΡΠ°ΠΌΠΈ ΠΠ ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΠ»Π° ΠΊ Π»ΡΡΡΠ΅ΠΌΡ ΠΊΠ°ΡΠ΅ΡΡΠ²Ρ ΠΎΠ±Π΅Π·Π±ΠΎΠ»ΠΈΠ²Π°Π½ΠΈΡ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² ΠΏΠΎΡΠ»Π΅ ΡΡΠ°Π²ΠΌΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΉ. ΠΠΎΡΠ»Π΅ ΡΠ΅Π°Π½ΡΠ° ΠΠ -ΡΠ΅ΡΠ°ΠΏΠΈΠΈ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΠ΅ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Π΅ΠΉ ΠΏΠΎ ΡΠΊΠ°Π»Π΅ ΡΠ°ΠΌΠΎΠΎΡΠ΅Π½ΠΊΠΈ Π±ΠΎΠ»ΠΈ ΡΠΎΡΡΠ°Π²ΠΈΠ»ΠΎ 44Β %. ΠΡΠΈ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΈ Ρ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ°ΠΌΠΈ, ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΠΌΠΈ Π½Π° ΡΠ»Π΅Π΄ΡΡΡΠΈΠΉ Π΄Π΅Π½Ρ, Π·Π½Π°ΡΠ΅Π½ΠΈΡ Π² ΠΎΡΠ½ΠΎΠ²Π½ΠΎΠΉ Π³ΡΡΠΏΠΏΠ΅ Π±ΡΠ»ΠΈ Π½ΠΈΠΆΠ΅ Π½Π° 22Β %. ΠΠΎΡΡΠΎΠ²Π΅ΡΠ½ΠΎ ΡΠ½ΠΈΠ·ΠΈΠ»Π°ΡΡ ΠΏΠΎΡΡΠ΅Π±Π½ΠΎΡΡΡ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² ΠΎΡΠ½ΠΎΠ²Π½ΠΎΠΉ Π³ΡΡΠΏΠΏΡ Π² Π½Π°ΡΠΊΠΎΡΠΈΡΠ΅ΡΠΊΠΈΡ
Π°Π½Π°Π»ΡΠ³Π΅ΡΠΈΠΊΠ°Ρ
. ΠΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΠΈ ΠΠΠ’Π ΠΊΠ°ΠΊ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Ρ ΡΠ½Π΄ΠΎΠΊΡΠΈΠ½Π½ΠΎ-ΠΌΠ΅ΡΠ°Π±ΠΎΠ»ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΎΡΠ²Π΅ΡΠ° Π² Π³ΡΡΠΏΠΏΠ΅ Ρ ΠΠ -ΡΠ΅ΡΠ°ΠΏΠΈΠ΅ΠΉ Π±ΡΠ»ΠΎ Π½Π° 18Β % ΠΌΠ΅Π½Π΅Π΅ Π²ΡΡΠ°ΠΆΠ΅Π½ΠΎ. ΠΠ«ΠΠΠΠ«: ΠΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΠΠ -ΡΠ΅ΡΠ°ΠΏΠΈΠΈ ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡ ΠΊ ΡΠΌΠ΅Π½ΡΡΠ΅Π½ΠΈΡ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Π΅ΠΉ ΠΏΠΎΡΠ»Π΅ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΎΠ½Π½ΠΎΠΉ Π±ΠΎΠ»ΠΈ, ΡΠ½Π΄ΠΎΠΊΡΠΈΠ½Π½ΠΎ-ΠΌΠ΅ΡΠ°Π±ΠΎΠ»ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΎΡΠ²Π΅ΡΠ° ΠΈ ΠΏΠΎΡΡΠ΅Π±Π½ΠΎΡΡΠΈ Π² ΠΎΠΏΠΈΠΎΠΈΠ΄Π½ΡΡ
Π°Π½Π°Π»ΡΠ³Π΅ΡΠΈΠΊΠ°Ρ
Beyond single-photon localization at the edge of a Photonic Band Gap
We study spontaneous emission in an atomic ladder system, with both
transitions coupled near-resonantly to the edge of a photonic band gap
continuum. The problem is solved through a recently developed technique and
leads to the formation of a ``two-photon+atom'' bound state with fractional
population trapping in both upper states. In the long-time limit, the atom can
be found excited in a superposition of the upper states and a ``direct''
two-photon process coexists with the stepwise one. The sensitivity of the
effect to the particular form of the density of states is also explored.Comment: to appear in Physical Review
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