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

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《中国物理C》（英文）编辑部

2024年10月30日

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

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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

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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).

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[5]	ZHANG Jin-Yu , WAN Ling-De , WANG Xue-Lei , YANG Yue-Ling , LI Bing-Zhong . Searching for Neutral Toppion in TC2 Model via a Flavor-Changing Process. Chinese Physics C, 2002, 26(12): 1209-1213.
[6]	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.
[7]	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.
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[13]	GU Jin-Nan . THE R(π/2) INVARIANCE OF NUCLEI. Chinese Physics C, 1986, 10(2): 223-230.
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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

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

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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.