QCD PERTURBATION THEORY FOR CONFINED QUARKS AND NUCLEI——(2) THE STRUCTURE OF THE NUCLEON-MESON COUPLING

HE HAN-XING; ZHUO YI-ZHONG; SA BEN-HAO

Chinese Physics C> 1982, Vol. 6> Issue(2) : 231-242

QCD PERTURBATION THEORY FOR CONFINED QUARKS AND NUCLEI——(2) THE STRUCTURE OF THE NUCLEON-MESON COUPLING

Abstract
HTML
Reference
Related

PDF

Abstract：
The structure of the nucleon-meson coupling is discussed on the basis of QCDperturbation theory. The transition amplitude for the Nucleon-Nucleon (Baryon) +Meson is obtained in the spherical cavity approximation of MIT bag model. From theanalysis of these amplitude (probability) it shows that the exchange of heavy mesonsof the first excited state (B, δ, A₁,...) and the 2π exchange (intermediate states N^*.△^*) are important in the zero range N-N interaction. However, the one-pion and onep、ω. etc do not appear.

References

[1]

G.E.Brown and A. D. Jackson, 1976, The Nucleon-Nucleon Interaction (North-Holland, Arnste-dam).[2] T. D. Lee, Phys. Rev., D19 (1978), 1802.[3] 何汉新,卓益忠,萨本豪,"QCD微扰理论和原子核(1)强子的能级移动和质量差”《高能物理与核物理》,1(1982), 69.[4] I. Duek, Phys. Lett., 77B(1978), 223.[5]A. Chode, et al., Phys. Rev., D9 (1974), 3471. T. Degrand,, et al, Phys. Rev., D12 (1975), 2060.[6] T. D. Bjokem snd S. D. Drell, "Relativistic Quantum Fields" (McGraw-Hill Book ,Company)1965.[7] T. D. DeGrand, R. L. Jaffe, Ann. Phys., (N. F.), 100 (1976), 425.[8] J. F. Donoghue, E. Golowich, Phys. Rev., D15 (1977), 3421.[9 ] R. L. Jaffe, Lectures at the 1979 Erice Summear School, MIT-CTP-814 (1979).

[1]	FU Zi-Wen . I=1/2 low-lying mesons in lattice QCD. Chinese Physics C, 2015, 39(8): 083101. doi: 10.1088/1674-1137/39/8/083101
[2]	GAO Yong-Hua , DUAN Chun-Gui , HOU Zhao-Yu , HE Zhen-Min . Nuclear Density Empicical Formula of the Nucleus and the Nuclear Effect of the Nucleon Structure Function. Chinese Physics C, 2004, 28(3): 290-293.
[3]	ZHANG Sheng-Qun , ZHOU Shan-Gui , XU Fu-Rong . Systematic Relation between Quadrupole Deformation β and Valence Nucleon Product (N_pN_n)^1/2. Chinese Physics C, 2004, 28(5): 516-520.
[4]	LIU Jian-Ye , GUO Wen-Jun , ZHAO Qiang , YANG Yan-Fang , ZUO Wei . Nuclear Stopping as a Probe to Nucleon-Nucleon Cross Section in Heavy Ion Collisions. Chinese Physics C, 2001, 25(4): 336-342.
[5]	MENG Jie , LONG Wen-Hui . Relativistic Continuum Hartree-Bogoliubov Theory Aims at Unstable Nuclei. Chinese Physics C, 2000, 24(S1): 59-64.
[6]	LONG Gui-Lu , SUN Hong-Zhou , ZHAO En-Guang , ZHU Sheng-Jiang , RUAN Dong , LIU Feng-Ying , JI Hua-Ying , LI Yan-Song , YAN Hai-Yang , TU Chang-Cun , ZHANG Wei-Lin , Pak Jae-Yon , . Some Recent Development in Nuclear Structure Studies. Chinese Physics C, 2000, 24(S1): 38-44.
[7]	MENG Jie , WU Chong-Shi , ZENG Jin-Yan . SU_q(2) Analysis of Nuclear Rotational Spectra. Chinese Physics C, 1992, 16(1): 90-96.
[8]	LI Qing-Run , ZHOU Jin-Li . A Test of the α-Particle Structure of ¹⁶O by Means of the Proton Scattering. Chinese Physics C, 1992, 16(3): 229-234.
[9]	DOU Zhi-Guo , JING Xiao-Gong , ZHAO Guo-Quan . SINGLE-PARTICLE AND SINGLE-HOLE ENERGIES IN THE ⁴⁰Ca REGION. Chinese Physics C, 1990, 14(11): 1031-1038.
[10]	CAO Zhi-Jun , SHEN Jian-Ping , LI Guang-Lie . THE ROLE OF NUCLEON-NUCLEON SHORT-RANGE CORRELATIONS IN THE UNCLEAR STRUCTURE FUNCTION IN THE X>1 REGION. Chinese Physics C, 1989, 13(10): 924-929.
[11]	HUO Yu-Kun , PAN Zheng-Ying . INTERACTIONS OF NUCLEI AND LASER (2) ——LASER ENHANCED EFFECTIVE NEUTRON WIDTH FOR NUCLEAR RESONANCE. Chinese Physics C, 1989, 13(9): 856-859.
[12]	TANG Xiao-Wei . ON THE SPONTANEOUS PION EMISSION BY HEAVY NUCLEI. Chinese Physics C, 1988, 12(5): 584-586.
[13]	GU Jin-Nan . THE R(π/2) INVARIANCE OF NUCLEI. Chinese Physics C, 1986, 10(2): 223-230.
[14]	LIU Xian-Hui , WANG De-Mao , ZHANG Zhen-Qiu . INELASTIC SCATTERING OF PION AND KAON MESONS ON Ca NUCLEUS. Chinese Physics C, 1985, 9(1): 62-70.
[15]	ZHUO YI-ZHONG , SA BEN-HAO . QCD PERTURBATION THEORY AND NUCLEI (1) THE ENERGY SHIFTS OF HADRENS AND HADRONS MASS DIFFERENCE MASS DIFFERENCE. Chinese Physics C, 1982, 6(1): 69-76.
[16]	Zhang Qi-ren . SCALAR MESON FIELD AND THE AVERAGE PROPERTIES OF ATOMIC NUCLEI. Chinese Physics C, 1980, 4(5): 576-578.
[17]	ZHANG QI-REN . SURFACE ENERGIES OF ATOMIC NUCLEI AND THE MASS OF THE SCALAR MESON. Chinese Physics C, 1979, 3(1): 75-79.
[18]	YU YOU-WEN . THE INTERACTION OF ANTINUCLEON WITH NUCLEUS. Chinese Physics C, 1979, 3(6): 676-680.
[19]	LIAO JI-ZHI . SHELL MODEL CALCULATIONS ON 1f_7/2 NUCLEI. Chinese Physics C, 1979, 3(6): 734-748.
[20]	LI YANG-GUO , ZHANG YU-SHUN , LIN CHUN-CAN . SPIN EFFECTS IN HIGH-ENERGY NUCLEONNUCLEUS SCATTERING. Chinese Physics C, 1978, 2(6): 526-533.

Access

Get Citation

HE HAN-XING, ZHUO YI-ZHONG and SA BEN-HAO. QCD PERTURBATION THEORY FOR CONFINED QUARKS AND NUCLEI——(2) THE STRUCTURE OF THE NUCLEON-MESON COUPLING[J]. Chinese Physics C, 1982, 6(2): 231-242.

HE HAN-XING, ZHUO YI-ZHONG and SA BEN-HAO. QCD PERTURBATION THEORY FOR CONFINED QUARKS AND NUCLEI——(2) THE STRUCTURE OF THE NUCLEON-MESON COUPLING[J]. Chinese Physics C, 1982, 6(2): 231-242. shu

RIS(for EndNote,Reference Manager,ProCite)

BibTex

Txt

Milestone

Received: 1981-06-09
Revised: 1900-01-01

Article Metric

Article Views(1975)
PDF Downloads(245)
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

QCD PERTURBATION THEORY FOR CONFINED QUARKS AND NUCLEI——(2) THE STRUCTURE OF THE NUCLEON-MESON COUPLING

Received Date: 1981-06-09
Accepted Date: 1900-01-01
Available Online: 1982-04-05

Abstract: The structure of the nucleon-meson coupling is discussed on the basis of QCDperturbation theory. The transition amplitude for the Nucleon-Nucleon (Baryon) +Meson is obtained in the spherical cavity approximation of MIT bag model. From theanalysis of these amplitude (probability) it shows that the exchange of heavy mesonsof the first excited state (B, δ, A₁,...) and the 2π exchange (intermediate states N^*.△^*) are important in the zero range N-N interaction. However, the one-pion and onep、ω. etc do not appear.