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2000 Vol. 17, No. 1

Issue of Selected Papers for the 80th Birthday of Prof.Yang Li-ming
Anomlous Anisotropies of Fission Fragments in Near-and Sub-barrier Fusion-fission Reactions
ZHANG Huan qiao, LIU Zu hua, XU Jin cheng, LU Jun, QIAN Xin, RUAN Ming, QIAO Yu, LIN Cheng jian, XU Kan
2000, 17(1): 1-5. doi: 10.11804/NuclPhysRev.17.01.001
Abstract:
Systematic summary on the anomalous anisotropies of fission fragments in near and sub barrier fusion fission reactions is presented. A new version of the preequilibrium fission model is put forward to explain the anomalous anisotropies of fission fragments, except the bump of anomaly. Further study is still needed.
Chiral SU(3) Quark Model and Study of Six Quark States
ZHANG Zong-ye, YU You-wen, YUAN Xiu-qing
2000, 17(1): 6-9. doi: 10.11804/NuclPhysRev.17.01.006
Abstract:
An analysis is made for the (0s) 6 six quark cluster states in the chiral SU (3) quark model. The results show that for some multistrangeness states the chiral SU (3) could offer more attraction. Further RGM dynamical calculation of the multistrangeness system (ΩΩ) 0+ and (ΩΞ) 1+ has been done. It shows that (ΩΩ) 0+ is a deeply bound state in the chiral SU (3) quark model.
Nucleon Spin Structure
WANG Fan
2000, 17(1): 10-18. doi: 10.11804/NuclPhysRev.17.01.010
Abstract:
A simple introduction of the discovery of quark and the constituent quark model of nucleon have been given. The contradiction between the quark spin structure of nucleon of the constituent quark model and the measured one in the polarized deep inelastic lepton nucleon scattering has been explained in detail. It is elucidated that the so called “proton spin crisis” is due to quark spin confusion. The incompatibility between the requirement of gauge invariance and ...
New Frontiers of Nuclear Physics in 21st Century——a Preview
WANG Shun-jin
2000, 17(1): 19-21. doi: 10.11804/NuclPhysRev.17.01.019
Abstract:
Different opinions about prospects of the development of nuclear physics in the 21st century are displayed, and indicating great opportunities and challenges faced by nuclear physicists in the future are analyzed in detail.
QCD Study of Nucleon s(Hadron s) Structure and Property
HE Han-xin
2000, 17(1): 22-29. doi: 10.11804/NuclPhysRev.17.01.022
Abstract:
The nucleon (hadron) is the bound state of guarks and gluons, which is described by the quantum chromodynamics (QCD). Due to the basic properties of QCD (the asymptotic freedom at the high energy scale, the color confinement and the dynamical chiral symmetry breaking at the low energy scale), the QCD picture for the nucleon’s (hadron’s) structure and property is scale dependent. At high energy scale, the QCD parton model, which is relative to the hard process for testing the...
Reduction and Self-similarity of Quantum dynamics
ZHANG Qi-ren, GAO Chun-yuan
2000, 17(1): 30-34. doi: 10.11804/NuclPhysRev.17.01.030
Abstract:
By a generalized version of AGS reduction procedure we show that the forms of quantum dynamics at different strata are the same. This is the self similarity of quantum dynamics.
Closeness of Classical Orbits and Factorization of Radial Schroinger Equation
Wu Zuo-bing, Zeng Jin-yan
2000, 17(1): 35-38. doi: 10.11804/NuclPhysRev.17.01.035
Abstract(1778) PDF (989KB)(525)
Abstract:
It is shown that for a particle with suitable angular momenta in the screened Coulomb potential or isotropic harmonic potential, there still exists closed orbits rather than ellipse, characterized by the conserved perihelion and aphelion vectors, i.e., extended Runge Lenz vector, which implies a higher dynamical symmetry than the geometrical symmetry SO 3. For the potential, factorization of the radial Schrdinger equation to produce raising and lowering operators is also pointed out.
Estimating Magic Number Larger than 126 by Yang Liming Method
LI Xian-hui, ZHOU Zhi-ning, ZHONG Yu-shu, YANG Ze-sen
2000, 17(1): 39-42. doi: 10.11804/NuclPhysRev.17.01.039
Abstract:
Based on Fermi Yang Liming method and its improved method, magic numbers were calculated by using Woods Saxon density function. That the magic number next to 126 should be 184 was predicted.
Physics Today and Its Future
AI Xiao-bai
2000, 17(1): 43-50. doi: 10.11804/NuclPhysRev.17.01.043
Abstract:
Listing more than one hundred unanswered questions the present author claims that 1) the long standing puzzles in physics may be the signals of new physics; 2) the effort of searching for the basic natural laws of physics is always highly worthwhile.
Pomeron and Glueball
MA Wei-xing, JIANG Huang-qing, L C Liu, L S Kisslinger
2000, 17(1): 51-55. doi: 10.11804/NuclPhysRev.17.01.051
Abstract:
The pomeron in high energy hadron hadron scattering as well as the QCD nature of the pomeron are discussed. We claimed that the pomeron may be the tenser glueball ξ(2 230) with quantum number I G =0 +, J PC =2 ++ . Under this reggeized glueball model the cross section of high energy proton proton scattering and the coupling parameter of the pomeron nucleon, β , are calculated. The theoretical results of the present model are in good agreement with experimental data.
Nuclear Physics
Different Fission Behavior Induced by Heavy Ion Central and Peripheral Collisions
WU En-jiu, ZHENG Ji-wen, XIAO Zhi-gang, ZHANG Chun, TAN Ji-lian, YIN Shu-zhi, WANG Su-fang, JIN Gen-ming, YIN Xu, SONG Ming-tao, JIN Wei-yang, PENG Xing-ping, LI Zu-yu, WU He-yu, HE Zhi-yong
2000, 17(1): 56-57. doi: 10.11804/NuclPhysRev.17.01.056
Abstract(2004) PDF (656KB)(585)
Abstract:
Correlated fission fragments from the 40Ar+209Bi reaction and their further correlation with α particles have been studied for peripheral and central collisions simultaneously. The existence of different fission behavior of hot nuclei formed in central and peripheral collisions was found from the systematic analysis of the mass and energy distributions of fission fragments as a function of the initial temperature of hot fissioning nuclei.
ECR Ion Source of High Charge States
ZHANG Zi-min, LIU Zhan-wen, ZHAO Hong-wei
2000, 17(1): 58-62. doi: 10.11804/NuclPhysRev.17.01.058
Abstract:
Electron cyclotron resonance (ECR) ion source is the most efficient facility for producing highly charged ions. So far more than 1 emA of O 6+ and 0.02 eμA of U 55+ have been delivered by ECR ion source. In this paper the latest development of ECR ion source is presented and several typical ECR ion sources in the world is introduced.