Impact factor of Chinese Physics C is 3.6 in 2023 Impact factor of Chinese Physics C is 3.6 in 2022 2021 Impact Factor 2.944
Advanced Search
×
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> 2015, Vol. 39> Issue(9) : 094001 DOI: 10.1088/1674-1137/39/9/094001

Pion emission in α-particle interactions with varioustargets of nuclear emulsion detector

  • The behavior of relativistic hadron multiplicity for 4He-nucleus interactions is investigated. The experiment is carried out at 2.1 A and 3.7 A GeV (Dubna energy) to search for the incident energy effect on the interactions inside different emulsion target nuclei. Data are presented in terms of the number of emitted relativistic hadrons in both forward and backward angular zones. The dependence on the target size is presented. For this purpose the statistical events are discriminated into groups according to the interactions with H, CNO, Em, and AgBr target nuclei. The separation of events, into the mentioned groups, is executed based on Glauber's multiple scattering theory approach. Features suggestive of a decay mechanism seem to be a characteristic of the backward emission of relativistic hadrons. The results strongly support the assumption that the relativistic hadrons may already be emitted during the de-excitation of the excited target nucleus, in a behavior like that of compound-nucleus disintegration. Regarding the limiting fragmentation hypothesis beyond 1 A GeV, the target size is the main parameter affecting the backward production of the relativistic hadron. The incident energy is a principal factor responsible for the forward relativistic hadron production, implying that this system of particle production is a creation system. However, the target size is an effective parameter as well as the projectile size considering the geometrical concept regarded in the nuclear fireball model. The data are analyzed in the framework of the FRITIOF model.
      PCAS:
  • 加载中

  • References

    [1] Bondorf J P, Botvina A S, Iljinov A S, Mishustin I N, Sneppen K. Phys. Rep., 1995, 57: 133[2] Bondorf J P. Journal de Physique, 1976, 37/C5: 195; Proceeding of the EPS Topical Conference on Large Amplitude Collective Nuclear Motions, Keszthely, Hungary, June 1979[3] MA Y G. Phys. Rev. Lett., 1999, 83: 3617[4] D#261;browska A, Szarska M, Trzupek A, Wolter W, Wosiek B. Acta Physica Polonica B, 2001, 32: 3099[5] MA Y G et al. Phys. Rev. C, 2005, 71: 054606[6] Benecke J, CHOU T T, YANG C N, YEN E. Phys. Rev., 1969, 188: 2159[7] LIU Fu-Hu. Chinese Journal of Physics, 2002, 40: 159[8] Ahmad M S, Khan M Q R, Hasan R. Nucl. Phys. A, 1989, 499: 821[9] Webber W R. Proceedings of the International Cosmic Ray Conference, Vol. 8, P. 65, Moscow, USSR. 1987[10] Lindstorm P L, Greiner D E, Heckman H H, Cork B. Lawrence Berkeley Laboratory Report, LBL-3650. 1975[11] Olson D L, Berman B L, Grenier D E, Heckman H H, Lindstrom P J, Crawford H J. Phys. Rev. C, 1983, 28: 1602[12] El-Nagdy M S, Abdelsalam A, Abou-Moussa Z, Badawy B M. Can. J. Phys., 2013, 91: 737[13] Abdelsalam A, Metwalli N, Kamel S, Aboullela M, Badawy B M, Abdallah N. Can. J. Phys., 2013, 91: 438[14] Abdelsalam A, Badawy B M, Hafiz M. J. Phys. G: Nucl. Part. Phys.,2012, 39: 105104[15] Powell C F, Fowler F H, Perkins D H. The Study of Elementary Particles by the Photographic Method, Pergamon Press. London; New York, Paris, Los Angles, 474. 1958[16] Barkas H. Nuclear Research Emulsion, Vol. I, Technique and Theory Academic Press Inc., 1963[17] Shmakov S Yu, Uzhinskii V V. Com. Phys. Comm., 1989, 54: 125[18] Florian J R et al. Report Submitted to the Meeting of Division of Particles and Fields, Berkeley, California. 1973[19] Abdelsalam A. JINR Report (Dubna), 1981, E1-81-623[20] Abdrahmanov E O et al. Z. Phys. C, 1980, 5: 1[21] Adamovich M I et al. (for EMU01 collaboration). Lund University Report, Sweden, LUIP 8904. 1989[22] Andersson B Gustafson G, Nilsson-Almqvist B. Nucl. Phys. B,1987, 281: 289[23] Nilsson-Almqvist B, Stenlund E. Comp. Phys. Comm., 1987, 43: 387[24] Abdelsalam A, Shaat E A, Ali-Mossa N, Abou-Mousa Z, Osman O M, Rashed N, Osman W, Badawy B M, El-Falaky E. J. Phys. G: Nucl. Part. Phys., 2002, 28: 1375[25] Abdelsalam A, Badawy B M, El-Falaky E. Can. J. Phys., 2007, 85: 837[26] Abdelsalam A, El-Nagdy M S, Badawy B M; Can. J. Phys., 2011, 89: 261

  • Access

    加载中

Get Citation
Z. Abou-Moussa, N. Rashed, B. M. Badawy, H. A. Amer, W. Osman and M. M. El-Ashmawy. Pion emission in α-particle interactions with varioustargets of nuclear emulsion detector[J]. Chinese Physics C, 2015, 39(9): 094001. doi: 10.1088/1674-1137/39/9/094001
Z. Abou-Moussa, N. Rashed, B. M. Badawy, H. A. Amer, W. Osman and M. M. El-Ashmawy. Pion emission in α-particle interactions with varioustargets of nuclear emulsion detector[J]. Chinese Physics C, 2015, 39(9): 094001.  doi: 10.1088/1674-1137/39/9/094001 shu
Milestone
Received: 2015-02-06
Revised: 1900-01-01
Article Metric

Article Views(1805)
PDF Downloads(125)
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

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Email This Article

Title:
Email:

Pion emission in α-particle interactions with varioustargets of nuclear emulsion detector

    Corresponding author: B. M. Badawy,
  • Received Date: 2015-02-06
  • Accepted Date: 1900-01-01
  • Available Online: 2015-09-05

Abstract: The behavior of relativistic hadron multiplicity for 4He-nucleus interactions is investigated. The experiment is carried out at 2.1 A and 3.7 A GeV (Dubna energy) to search for the incident energy effect on the interactions inside different emulsion target nuclei. Data are presented in terms of the number of emitted relativistic hadrons in both forward and backward angular zones. The dependence on the target size is presented. For this purpose the statistical events are discriminated into groups according to the interactions with H, CNO, Em, and AgBr target nuclei. The separation of events, into the mentioned groups, is executed based on Glauber's multiple scattering theory approach. Features suggestive of a decay mechanism seem to be a characteristic of the backward emission of relativistic hadrons. The results strongly support the assumption that the relativistic hadrons may already be emitted during the de-excitation of the excited target nucleus, in a behavior like that of compound-nucleus disintegration. Regarding the limiting fragmentation hypothesis beyond 1 A GeV, the target size is the main parameter affecting the backward production of the relativistic hadron. The incident energy is a principal factor responsible for the forward relativistic hadron production, implying that this system of particle production is a creation system. However, the target size is an effective parameter as well as the projectile size considering the geometrical concept regarded in the nuclear fireball model. The data are analyzed in the framework of the FRITIOF model.

    HTML

Reference (1)

目录

Link
IOPScience
SCOAP3
arXiv
Chinese Physical Society
Journal information
Introduction
Editorial Board
Others
Subscribe
Contact us
QQ: 1307685413
Tel: +86-010-88235947
Fax: +86-010-88233126
E-mail: cpc@ihep.ac.cn

  • CPC Website

  • IOP Website

  • CPC WeChat

Copyright © Institute of High Energy Physics, Chinese Academy of Sciences, 19B Yuquan Road, Beijing 100049, China 京ICP备05002789号-1

Supported by: Beijing Renhe Information Technology Co. Ltd  E-mail: info@rhhz.net

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return