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61.
The parent bicyclo[6.2.0]decapentaene is synthesized for the first time by thermal ring opening of its valence isomer. Thermal dimerization of the compound is also described. 相似文献
62.
63.
64.
65.
Utaro Furukane Toshiatsu Oda 《Journal of Quantitative Spectroscopy & Radiative Transfer》1985,33(6):645-651
Lasing conditions for He have been evaluated numerically. We have used a collisional radiative model to calculate overpopulation densities Δnij, which are defined as differences between population densities per unit statistical weight of the upper and lower excited levels i and j, respectively. Laser oscillations for the level pairs 21P-31S, 21P-41S, 21P-31D, 21P-41D, 31D-41F, 31P-41S, 31P-41D, and 33P-43S are possible when the electron densities are within well defined limits at low electron temperature (Te = 0.1 eV). For level pairs of the singlet state, the inversion mechanism for He is the same as for H. Only collisional processes produce population inversion in the triplet level pair 33P-43S. 相似文献
66.
R.?GilardiEmail author S.?Streule N.?Momono M.?Oda J.?Mesot 《The European Physical Journal B - Condensed Matter and Complex Systems》2005,47(2):231-237
Magnetization and ac-susceptibility measurements are used to
characterize the mixed phase of the high-temperature cuprate
superconductor La2-xSrxCuO4 over a large range of doping (0.075
0.20). The first order vortex lattice phase transition line HFOT(T), the upper
critical field Hc2(T) and the second peak Hsp(T) have been
investigated up to high magnetic fields (8 Tesla applied perpendicular to the CuO2 planes).
Our results reveal a strong doping dependence of the magnetic phase diagram, which can mainly be
explained by the increasing anisotropy with underdoping.
Within our interpretation, the first order vortex lattice phase transition is due to the sublimation (rather than melting)
of the vortex lattice into a gas of pancake vortices, whereas the second peak is related to the transition to a more disordered
vortex glass state. 相似文献
67.
A nickel catalyst coordinated by trimethylphosphine is found to effect the addition reaction of Ar-CN bonds in aromatic nitriles across alkynes to give rise to various beta-arylalkenenitriles. 相似文献
68.
Abe S Fujishima T Tsubone T Fujimura R Ono H Matoba O Oda K Shimura T Kuroda K 《Optics letters》2003,28(6):420-422
The photorefractive effect in a nominally undoped 0.91Pb(Zn1/3Nb2/3)O3-0.09PbTiO3 single crystal is measured. We report what is, to our knowledge, the first observation of the photorefractive effect in Pb-based relaxor ferroelectric crystals. The crystal is grown by the flux solution method. Then it is cut into a 2 mm x 4 mm x 8 mm piece and electrically poled along the [111] direction. The coupling constant of the two-wave mixing is 17 cm(-1), and the normalized time constant under 1-W/cm(2) illumination is 12 s at a wave-length of 476 nm. The effective trap density is calculated as 5 x 10(16) cm(-3) from the Debye screening length under the assumption of Kukhtarev's band-transport model. The dominant carrier is identified to be holes from the direction of two-wave mixing energy transfer. 相似文献
69.
The response of CR-39 detector has been obtained precisely for protons, deuterons, tritons, alpha-particles and lithiumions with energies of a few MeV/nucleon. The track etch rates were determined from the growth curves of pit radius and summarized as the response functions. The accuracy of this method is high enough to discriminate among hydrogen isotopes under a certain condition. The correlation between the response and LET with various cut-off energies has also been examined. It was found that LET is not an unique parameter describing the response function adequately for different ions by the same expression. 相似文献
70.
We show that a five-dimensional Universal Extra Dimension model, compactified on a line segment, is consistently formulated
even when the gauge symmetry is broken solely by non-zero Dirichlet boundary conditions on a bulk Higgs field, without any
quartic interaction. We find that the longitudinal W
+
W
− elastic scattering amplitude, under the absence of the Higgs zero mode, is unitarized by exchange of infinite towers of KK
Higgs bosons. Resultant amplitude scales linearly with the scattering energy μ ?s\propto\sqrt{s}, exhibiting five-dimensional nature. A tree-level partial-wave unitarity condition is satisfied up to 6.7 (5.7) TeV for the
KK scale m
KK=430 (500) GeV, favored by the electroweak data within 90% CL. 相似文献