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Chaotic Dynamical Behaviour in Soliton Solutions for a New (2+1)-Dimensional Long Dispersive Wave System
ZHANG Jie-Fang, ZHENG Chun-Long, MENG Jian-Ping, FANG Jian-Ping
Chin. Phys. Lett. 2003, 20 (4):
448-451
.
With the help of variable separation approach, a quite general excitation of a new (2+1)-dimensional long dispersive wave system is derived. The chaotic behaviour, such as chaotic line soliton patterns, chaotic dromion patterns, chaotic-period patterns, and chaotic-chaotic patterns, in some new localized excitations are found by selecting appropriate functions.
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Lifetimes of High Spin Yrast States in Odd-Proton Nucleus 131Pr
LI Guang-Sheng, MENG Rui, ZHU Li-Hua, ZHANG Zhen-Long, WANG Yue, WANG Zhi-Min, WEN Shu-Xian, LU Jing-Bin, ZHAO Guang-Yi, LI Xian-Feng, WEN Li-Jun, ZHENG Yong-Nan, ZHENG Yong, LIU Yun-Zuo, YUAN Guan-Jun, YANG Chun-Xiang
Chin. Phys. Lett. 2003, 20 (4):
475-477
.
Lifetimes of the high spin yrast states in the odd-proton nucleus 131Pr have been determined by analysing the Doppler broadened line shapes for the de-exciting γ-rays following the 116Sn(19F, 4n)131Pr reaction at a bombarding energy of 95 MeV. The transition quadrupole moments extracted from the measured lifetimes exhibit a considerable reduction near the rotational frequency of 0.42 MeV, at which the J(1) and J(2) moments of inertia indicate a band crossing. The experimental result demonstrates occurrence of the nuclear shape change induced by band crossing associated with the alignment of a pair of h11/2 protons.
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Properties of the First 1/2+ Excitation State of 13C by 22 MeV Proton Inelastic Scattering
AN Zhu, CHEN Quan, CHENG Ye-Hao, SHEN Dong-Jun, GUO Gang
Chin. Phys. Lett. 2003, 20 (4):
478-481
.
The differential cross sections of 22 MeV proton inelastic scattering for the first 1/2+ excitation state (Ex = 3.09 MeV) of 13C have been measured between 9°and 130°. The broad peak located at ~ 120°, which has been systematically observed in the 0+ → 0-, 1/2- → 1/2+, and 1+ → 1- transitions for the 16O, 13C, and 14,15N (p,n) charge exchange reactions at Ep = 35 MeV, has been observed for the first time in the present proton inelastic scattering. The present experimental data are analysed by using microscopic distorted-wave Born approximation. From the comparison of present experimental data and theoretical results at forward angles, our analysis indicates the existence of neutron halo in the first 1/2+ excitation state of the 13C nucleus. In addition, by reasonable modification of shell model wavefunction of the first 1/2+ excitation state, we can well describe the experimental form factors of (e,e') and the experimental differential cross sections of (p,p') at incident energy of 547 MeV.
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Yb3+-Doped Four-Wavelength Double Clad Laser
XU Zhao-Wen, XIANG Yang, NING Ding, FAN Wan-De, YANG Shi-Quan, YUAN Shu-Zhong, DONG Xiao-Yi
Chin. Phys. Lett. 2003, 20 (4):
506-508
.
A novel Yb3+-doped four-wavelength double clad fibre laser based on a Fabry-Parot filter, and pumped by a 976 nm laser diode is presented. Its output laser wavelengths are 1085, 1090, 1095, and 1010 nm, respectively. The laser exhibits 0.32 nm line-width, 1.5 W laser output power, 40 dB signal-to-noise ratio and 66% slope efficiency.
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Energy Distribution of Recycling Particles in Front of the Limiter and the Wall on the HT-7 Tokamak
XU Wei, WAN Bao-Nian, ZHOU Qian, WU Zhen-Wei, MAO Jian-Shan, LI Jian-Gang
Chin. Phys. Lett. 2003, 20 (4):
547-549
.
The Hα(Dα) line shape in front of the limiter and the wall is measured by two sets of optical spectroscopy multi-channel analysers. The energy distribution is derived directly from the Hα(Dα) line shape, especially showing several molecular processes. The dissociative excitation of molecules is dominating when the local electron temperature is above 10 eV. The Dα line shape is also simulated by the Monte Carlo method, the result shows that the molecular dissociation contributes 57% neutral atoms, 53% emission intensity in front of the limiter, and 85\% neutral atoms, 82% emission intensity in front of the wall. The power loss from molecular dissociation is about 5.6 x 104kW/m-3 and the molecular dissociation is an important cooling mechanism at the plasma edge.
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Influence of Gd Doping at A Site upon the Magnetic Structure of La0.7-xGdxSr0.3MnO3 Systems
PENG Zhen-Sheng, LIU Ning, CAI Zhi-Rang, GUO Huan-Yin, TONG Wei, ZHANG Chang-Jing, ZHANG Yu-Heng
Chin. Phys. Lett. 2003, 20 (4):
564-567
.
We investigated the magnetism of systems La0.7-xGdxSr0.3MnO3 (x = 0.00, 0.10, 0.15, 0.20, 0.30, 0.40, 0.50, 0.60, 0.70) by M-T curves, M-H curves, and electron-spin-resonance (ESR) spectra. The experimental results indicate that the system is in a ferromagnetic long-range order at low-doping level; the samples of x = 0.30 and 0.40 show cluster-spin glass behaviour; and the antiferromagnetic characters are observed at ≥ 0.50. For the samples of x = 0.30 and 0.40, the ESR spectra demonstrate that the phase separation occurs above the Curie temperature.
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Nano-crystalline CNx Films and Field Electron Emission Properties
HANG Lan, MA Hui-Zhong, LI Hui-Jun, YANG Shi-E, YAO Ning, HU Huan-Ling, ZHANG Bing-Lin
Chin. Phys. Lett. 2003, 20 (4):
579-581
.
CNx films with x ≈ 0.5 were prepared onto a titanium coated ceramic substrate by using microwave plasma enhanced chemical vapor deposition. As-deposited films were studied by x-ray photoelectron spectroscopy (XPS), x-ray diffraction, and scanning electron microscopy. The films consist of nano-crystalline grains with sites in a range of 20-40nm approximately. The interplanar distance (d-value) of the nano-crystalline structure determined from the peak position of x-ray diffraction was found to be 0.336 nm. This value is consistent with the d-value of graphite. XPS measurements of the N 1 s and C 1 s core levels for the same sample demonstrate two types of bonding structures between carbon and nitrogen atoms, corresponding to sp2 C-N and sp3 C-N. It is suggested that the N atoms mainly exist in aromatic rings of the nano-graphite layers by substituting carbon positions with nitrogen. Field electron emission characteristics of the film were tested. The turn-on field of the emission was as low as 1.1V/μm.
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Energy Transfer in Isolated LHC II Studied by Femtosecond Pump-Probe Technique
YANG Yi, GUO Li-Jun, LIU Yuan, LIU Wei-Min, ZHU Rong-Yi, QIAN Shi-Xiong, XU Chun-He
Chin. Phys. Lett. 2003, 20 (4):
589-592
.
Excitation energy transfer in the isolated light-harvesting chlorophyll (Chl)-a/b protein complex of photosystem II (LHC II) was studied by the one-colour pump-probe technique with femtosecond time resolution. After exciting Chl b by 638 nm beam, the dynamic behaviour shows that the ultrafast energy transfer from Chl-b at positions of B2, B3, and B5 to the corresponding Chl-a molecules in monomeric subunit of LHC II is in the time scale of 230 fs. While with the excitation of Chl a at 678 nm, the energy transfer between excitons of Chl-a molecules has the lifetime of about 370 fs, and two other slow decay components are due to the energy transfer between different Chl-a molecules in a monomeric subunit of LHC II or in different subunits, or due to change of molecular conformation.
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44 articles
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