Description of Charged Particle Multiplicity Distribution in High Energy Strong Interaction

  • With the assumption that the probability for n-charged particles production inhadron-hadron collision is Pn=xPn(1)+(1— x)Pn(2), whithin Pn(1)= andand proper choice of 1, 2, k and x, the true multiplicity distribution in full phase space can be described successfully at the centre fo mass energy GeV. Using the experimental data of non singe-diffractive collisions between proton and antiproton at centre of mass energies of 200 and 900GeV, the supposition had beenexamined and confirmed: it is very good to describe the facts. Had been discussed the theoretical bases of supposition.
  • 加载中
  • [1] V.Gupta and N.Sarma,Z.Phys.,C52(1991)53.[2]J.Benencke,T.T.Chou,C.N.Yang and E.Yen,Phys.Rev,188(1969)2159.[3]T.K.Gaisser et al,Phys.Lett,166B(1986)219.[4]UA5 Collaboration,G.J.Alner et al,Phys.Lett,138B(1984)304.[5]UA5 Collaboration,G.J.Alner et al,Phys.Lett,160B(1985)199.[6]UA5 Cllaboration,K.E.Ansorge et al.,CERN-EP/88-172(1988).
  • 加载中

Get Citation
Qin Keyu. Description of Charged Particle Multiplicity Distribution in High Energy Strong Interaction[J]. Chinese Physics C, 1994, 18(4): 347-352.
Qin Keyu. Description of Charged Particle Multiplicity Distribution in High Energy Strong Interaction[J]. Chinese Physics C, 1994, 18(4): 347-352. shu
Milestone
Received: 1900-01-01
Revised: 1900-01-01
Article Metric

Article Views(2254)
PDF Downloads(502)
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:

Description of Charged Particle Multiplicity Distribution in High Energy Strong Interaction

    Corresponding author: Qin Keyu,
  • Department of Physics, Yunnan Normal Untoer,ity, Kunming 650092

Abstract: With the assumption that the probability for n-charged particles production inhadron-hadron collision is Pn=xPn(1)+(1— x)Pn(2), whithin Pn(1)= andand proper choice of 1, 2, k and x, the true multiplicity distribution in full phase space can be described successfully at the centre fo mass energy GeV. Using the experimental data of non singe-diffractive collisions between proton and antiproton at centre of mass energies of 200 and 900GeV, the supposition had beenexamined and confirmed: it is very good to describe the facts. Had been discussed the theoretical bases of supposition.

    HTML

Reference (1)

目录

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return