Finite Abnormal Nuclei

ZHANG Qi-Ren; LI Xun-Gui

近期发现有不法分子冒充我刊与作者联系，借此进行欺诈等不法行为，请广大作者加以鉴别，如遇诈骗行为，请第一时间与我刊编辑部联系确认（《中国物理C》（英文）编辑部电话：010-88235947,010-88236950），并作报警处理。

本刊再次郑重声明：

（1）本刊官方网址为cpc.ihep.ac.cn和https://iopscience.iop.org/journal/1674-1137

（2）本刊采编系统作者中心是投稿的唯一路径，该系统为ScholarOne远程稿件采编系统，仅在本刊投稿网网址（https://mc03.manuscriptcentral.com/cpc）设有登录入口。本刊不接受其他方式的投稿，如打印稿投稿、E-mail信箱投稿等，若以此种方式接收投稿均为假冒。

（3）所有投稿均需经过严格的同行评议、编辑加工后方可发表，本刊不存在所谓的“编辑部内部征稿”。如果有人以“编辑部内部人员”名义帮助作者发稿，并收取发表费用，均为假冒。

《中国物理C》（英文）编辑部

2024年10月30日

Chinese Physics C> 1991, Vol. 15> Issue(11) : 1010-1014

Finite Abnormal Nuclei

ZHANG Qi-Ren ^, ,
LI Xun-Gui

Department of Technical Physics,Peking University,100871

Abstract
HTML
Reference
Related

PDF

Abstract：
We solved the problem for both the normal and abnormal finite nuclei from a simple relativistic model,and found eritical mass numbers A₁=85 and A₂=165.Only nuclei with mass numbers A≥A₁ may bave bound abnormal states,and only abnormal nuclei with mass number A≥A₂ have binding energies larger than those of corresponding normal nuclei.Abnormal nuclei become unbound again if A>3310,because of the Coulomb repulsion.

References

[1]

T.D.Lee and G.C. Wick, Phys. Rev., D9 (1974), 2291.[2] J. D.Walecka Ann., Phys.,83(1974), 491.[3] A.K.Kerman and L.D. Miller, in "Second High Energy Heavy Ion Summer Study" (1974)LBL-3675.[4] N. K. Glendenning, Nucl. Phys., A480(1988), 597.[5] J. Kunz, D. Masak and U. Post, Phys. Lett., 186B(1987), 124[6] 张启仁, 高能物理与核物理, 3(1979),75.[7] 张启仁, 高能物理与核物理, 4(1980),576.[8] Qi-ren Zhang, in Nuclear Equation of State, PtA eds. W. Greiner and H. Stoecker, (Plenum New York, 1989) p. 625.[9] A. Bohr and B. R. Mottelson, Nuclear Structure (Benjamin, New York, 1969) p. 256.[10] K. Huang and C. N. Yang, Phys. Reu., 105 (1957), 767; C. De Dominicis and P. C. Martin,Phys. Rev.105(1957). 1417.[11] W. D. Myers and W. J. Swiatecki, Ann. Phys., 84(1974), 186.

[1]	ZHOU Li-Juan , Ma Wei-xing . Nuclear Short range correlations in finite nuclei. Chinese Physics C, 2008, 32(1): 44-48. doi: 10.1088/1674-1137/32/1/010
[2]	YANG Fang , SHEN Hong . Quark-meson coupling model with a density-dependent bag constant for nuclear matter and finite nuclei. Chinese Physics C, 2006, 30(7): 620-624.
[3]	HUANG Xi , ZHANG Feng-Shou , FENG Zhao-Qing , JIN Gen-Ming . Critical Behavior of Multifragmentation in Finite Nuclei and Extraction of Critical Exponents. Chinese Physics C, 2006, 30(2): 123-127.
[4]	FENG Zhao-Qing , ZHANG Feng-Shou , HUANG Xi , JIN Gen-Ming , LI Wen-Fei . Isospin Effect of Multifragmentation and Critical Phenomena in Finite Nuclei. Chinese Physics C, 2005, 29(6): 577-582.
[5]	MAO Guang-Jun . Spectra of Anti-Nucleons in the Vacuum of Finite Nuclei. Chinese Physics C, 2004, 28(12): 1356-1360.
[6]	SHEN Hong . Quark Mean Field Model for Finite Nuclei and Hypernuclei. Chinese Physics C, 2004, 28(12): 1313-1316.
[7]	XIAO Jun , WANG En-Ke . Bremsstrahlung Radiative Correction in QED at Finite Temperature. Chinese Physics C, 2001, 25(8): 772-779.
[8]	LIU Ling , CAO Li-Gang , MA Zhong-Yu . The Effective DBHF Method for Finite Nuclei. Chinese Physics C, 2001, 25(7): 658-667.
[9]	Liu Jueping , Jin Yaping . Finite Temperature QCD Sum Rule and the ρ-Meson. Chinese Physics C, 1995, 19(12): 1108-1113.
[10]	Zheng Taiyu . Casimir Effect at Finite Temperature. Chinese Physics C, 1995, 19(3): 241-244.
[11]	Chen Baoqiu , Shi Hualin , Ma Zhongyu . N-N Correlations and Relativistic Density Dependent Mean Field Approach in Finite Nuclei. Chinese Physics C, 1995, 19(9): 852-857.
[12]	QIAN Zhi-Xin , ZHONG Wan-Heng , SU Ru-Keng . Yukawa Potential at Finite Temperature and Finite Density. Chinese Physics C, 1993, 17(5): 417-422.
[13]	ZHENG Guo-Tong , SU Ru-Keng . π AND σ MESON EXCHANGE POTENTIALS OF NUCLEON-NUCLEON INTERACTION AT FINITE TEMPERATURE. Chinese Physics C, 1990, 14(3): 220-227.
[14]	BI Pin-Zhen . KAONS CONDENSATION AT FINITE TEMPEATURE. Chinese Physics C, 1989, 13(3): 219-221.
[15]	SA Ben-Hao , ZHENG Yu-Ming , ZHANG Xiao-Ze , LU Zhao-Qi , XU Shu-Yan , , . ON THE BEHAVIOR OF PHASE TRANSITION SHOWN IN DISASSYMBLY PROCESSES OF VERY HOT AND DILUTE FINITE NUCLEAR SYSTEMS. Chinese Physics C, 1989, 13(2): 142-147.
[16]	CHEN Tao , SU Ru-Keng . THE ONE PION EXCHANGE POTENTIAL AT FINITE TEMPERATURE. Chinese Physics C, 1988, 12(1): 140-144.
[17]	YUAN Hai-Ji , YE Wei-Lei , GAO Qin , SHEN Qing-Biao . MICROSCOPIC OPTICAL POTENTIAL CALCULATIONS OF FINITE NUCLEI WITH EXTENDED SKYRME FORCES. Chinese Physics C, 1986, 10(3): 335-342.
[18]	SHI Xiang-Jun . THE APPLICATION OF OBEP IN THE HARTREE-FOCK CALCULATION FOR SOME FINITE NUCLEI. Chinese Physics C, 1983, 7(2): 223-228.
[19]	Xu Jiao-lin , Wu Yong-shi , Chen Shi , Guo Han-ying . ISOSPIN CIASSIFICATION OF HADRONS BY FINITE GROUP. Chinese Physics C, 1980, 4(2): 251-255.
[20]	Wang Ying-cai , Li Guang-lie , Zhang Zong-ye . THE π CONDENSATION EFFECTS IN FINITE NUCLEI. Chinese Physics C, 1980, 4(1): 63-72.

Access

Get Citation

ZHANG Qi-Ren and LI Xun-Gui. Finite Abnormal Nuclei[J]. Chinese Physics C, 1991, 15(11): 1010-1014.

ZHANG Qi-Ren and LI Xun-Gui. Finite Abnormal Nuclei[J]. Chinese Physics C, 1991, 15(11): 1010-1014. shu

RIS(for EndNote,Reference Manager,ProCite)

BibTex

Txt

Milestone

Received: 1900-01-01
Revised: 1900-01-01

Article Metric

Article Views(2165)
PDF Downloads(422)
Cited by(0)

Policy on re-use

To reuse of subscription content published by CPC, the users need to request permission from CPC, unless the content was published under an Open Access license which automatically permits that type of reuse.

通讯作者: 陈斌, bchen63@163.com

1.
沈阳化工大学材料科学与工程学院沈阳 110142

Finite Abnormal Nuclei

ZHANG Qi-Ren ^,
LI Xun-Gui

Corresponding author: ZHANG Qi-Ren,

Department of Technical Physics,Peking University,100871

Received Date: 1900-01-01
Accepted Date: 1900-01-01
Available Online: 1991-11-05

Abstract: We solved the problem for both the normal and abnormal finite nuclei from a simple relativistic model,and found eritical mass numbers A₁=85 and A₂=165.Only nuclei with mass numbers A≥A₁ may bave bound abnormal states,and only abnormal nuclei with mass number A≥A₂ have binding energies larger than those of corresponding normal nuclei.Abnormal nuclei become unbound again if A>3310,because of the Coulomb repulsion.