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941.
We found, through extensive experimental studies, that the physical aging effects are absent in the relaxation of rubbing-induced
birefringence (RIB) in polystyrene (PS), and the relaxation involves very small length scale. A phenomenological model based
on individual birefringence elements is proposed for the RIB relaxation. The relaxation times (RTs) of the elements are found
to be independent of the thermal or stress history of the samples, either before or after the formation of the birefringence.
The RTs are also independent of the molecular weight, rubbing conditions, and film thickness, while the RTs distribution function
does depend on the molecular weight and rubbing conditions. The model provides quantitative interpretations that agree very
well with all the reported experimental results, and sheds important light on the novel behaviors of the RIB relaxation. The
absence of physical aging effects is probably due to the combined effects of small length scale of the RIB relaxation, and
the accelerated aging speed in the near surface region in which the RIB concentrates. 相似文献
942.
Critical bond lengths and their role in spontaneous magnetostriction of R2Fe17CX (R=Y,Nd, Gd,Tb, Er)
N. Yang K.W. Dennis R.W. McCallum M.J. Kramer Y. Zhang P.L. Lee 《Journal of magnetism and magnetic materials》2007
High-energy high-flux synchrotron X-rays have been used to study the spontaneous magnetostriction of R2Fe17 (R=Y, Nd, Gd, Tb, Er) and their carbides in the temperature range 10–1100 K. Addition of interstitial carbon greatly increases both the Curie temperatures (TC) and the spontaneous magnetostrain of the compounds, while reduces the anisotropy of the magnetostrain by expanding the distances between rare-earth and neighboring Fe sites. The increase of TC with carbon is due to the increased spatial separation of the Fe hexagon layers. On the basal plane, the Fe hexagons are squeezed and the contribution of Fe sublattice to spontaneous magnetostriction is attenuated, while that of rare-earth sublattice is enhanced. The average bond magnetostrain around Fe sites are in linear relation with their hyperfine field intensities. 相似文献
943.
Z-pinch experiments with two arrays consisting, respectively, of 32
4-μm- and 6-μm-diameter tungsten wires have been carried out on
QiangGuang-1 facility with a current rising up to 1.5MA in 80ns. At early
time of implosion, x-ray framing images show that the initial emission comes
from the central part of arrays, and double clear emission rings, drifting
to the anode and the cathode at 5×106cm/s and 2.4×107cm/s respectively, are often produced near the electrodes. Later,
in a 4-μm-diameter tungsten wire array, filamentation caused by ohmic
heating is prominent, and more than ten filaments have been observed. A
radial inward shift of arrays starts at about 30\,ns earlier than the
occurrence of the x-ray peak power for both kinds of arrays, and the
shrinkage rate of emission region is as high as 1.7×107cm/s in
a 4-μm-diameter tungsten wire array, which is two times higher than
that in a 6-μm one. Emission from precursor plasmas is observed in
implosion of 6-μm-diameter tungsten wire arrays, but not in implosion
of a 4-μm-diameter tungsten wire array. Whereas, in a 4-μm-diameter tungsten wire array, the soft x-ray emission shows the growth of
m=1 instability in the plasma column, which is caused by current. The
reasons for the discrepancy between implosions of 4-μm- and 6-μm-diameter tungsten wire arrays are explained. 相似文献
944.
The possibility of ferromagnetic (FM) and antiferromagnetic (AFM) phase transitions in symmetric nuclear matter is analyzed
within the framework of a Fermi liquid theory with effective Gogny interaction. It is shown that, at some critical density,
nuclear matter with the D1S effective force undergoes a phase transition to the AFM spin state (opposite directions of neutron
and proton spins). The self-consistent equations of spin-polarized nuclear matter with the D1S force have no solutions corresponding
to FM spin ordering (the same direction of neutron and proton spins) and, hence, the FM transition does not appear. The AFM
spin polarization parameter is found for zero and finite temperature. It is shown that the AFM spin polarization parameter
of partially polarized nuclear matter at low enough temperatures increases with temperature. The entropy of the AFM spin state
for some temperature range is larger than the entropy of the normal state. Nevertheless, the free energy of the AFM spin state
is always less than the free energy of the normal state, and the AFM spin-polarized state is preferable for all temperatures
below the critical temperature.
The text was submitted by the authors in English. 相似文献
945.
G.-Y. Sun C.-X. Wu Y. Chen Z.-L. Yang 《The European Physical Journal B - Condensed Matter and Complex Systems》2006,49(4):459-464
Using the Keldysh nonequilibrium Green function method, we
theoretically investigate the electron transport properties of a
quantum dot coupled to two ferromagnetic electrodes, with
inelastic electron-phonon interaction and spin flip scattering
present in the quantum dot. It is found that the electron-phonon
interaction reduces the current, induces new satellite polaronic
peaks in the differential conductance spectrum, and at the same
time leads to oscillatory tunneling magnetoresistance effect. Spin
flip scattering suppresses the zero-bias conductance peak and
splits it into two, with different behaviors for parallel and
anti-parallel magnetic configuration of the two electrodes.
Consequently, a negative tunneling magnetoresistance effect may
occur in the resonant tunneling region, with increasing spin flip
scattering rate. 相似文献
946.
We developed a disk-type non-contact ultrasonic motor based on B22 vibration mode. The rotors of SU-8 photoresist are fabricated by the UV-LIGA process to control their shapes and thicknesses. So the structures of them are optimized by the experiments. It is found that the revolution speed of disk-type non-contact ultrasonic motor not only depends on the vibration amplitude of the stator, but also the weight and construction of the rotors. The maximum revolution speed of the optimal rotor is 3569 rpm at the input voltage of 20 V and the driving frequency of 45.6 kHz. The exciting principle of traveling wave is presented with theoretical equations. The electric signals applied to the piezoelectric ceramic are designed by the principle. The natural frequency and corresponding vibration mode are calculated and analyzed using finite element method. It is shown that experimental results are in good agreement with simulation, which verifies the effectiveness of the finite element model. Moreover, the levitation distance between the stator and rotor is measured by a CCD laser displacement transducer. 相似文献
947.
JU Guo-Xing XIANG Yang REN Zhong-Zhou 《理论物理通讯》2006,46(5):819-825
The properties of the 8-wave for a quasl-free partide with position-dependent mass (PDM) have been discussed in details. Differed from the system with constant mass in which the localization of the s-wave for the free quantum particle around the origin only occurs in two dimensions, the quasi-free particle with PDM can experience attractive forces in D dimensions except D = 1 when its mass function satisfies some conditions. The effective mass of a particle varying with its position can induce effective interaction, which may be attractive in some cases. The analytical expressions of the eigenfunctions and the corresponding probability densities for the 8-waves of the two- and three-dimensional systems with a special PDM are given, and the existences of localization around the origin for these systems are shown. 相似文献
948.
949.
950.
Ablation process of 1-kHz femtosecond lasers (pulse duration of 148 fs, wavelength of 775 nm) of Au film on silica substrates is studied. The thresholds for single and multi pulses can be obtained directly from the relation between the squared diameter D2 of the ablated craters and the laser fluence φo. From the plot of the accumulated laser fluence Nφth(N) and the number of laser pulses N, incubation coefficient of Au film is obtained to be 0.765. Some experimental data obtained around the single pulse threshold are in good agreement with the theoretical calculation. 相似文献