The Saturation Phenomenon of Transverse Energy Distribution in Heavy-Ion Collisions and Multisource Modle

ZHANG Kun-Shi; LIU Lian-Shou

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2024年10月30日

Chinese Physics C> 1991, Vol. 15> Issue(7) : 615-622

The Saturation Phenomenon of Transverse Energy Distribution in Heavy-Ion Collisions and Multisource Modle

ZHANG Kun-Shi ^, ,
LIU Lian-Shou

Jinzhou Teachers College,Jinzhou,Hubei 4341001 Institute of Particle Physics,Huazhong Normal University,Wuhan 430070

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Abstract：
Based on a careful analysis of the mechanism of high energy non-equal mass nuclei collisions,the multisource modle is further developed.The transverse energy distribution in central rapidity region at both CERN and BNL energy domains are calculated.The saturation of transverse energy distribution at low energy is explained,and the minimum mass number of the target nucleus for this saturation effect (full stopping) to occur is obtained.

References

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ZHANG Kun-Shi and LIU Lian-Shou. The Saturation Phenomenon of Transverse Energy Distribution in Heavy-Ion Collisions and Multisource Modle[J]. Chinese Physics C, 1991, 15(7): 615-622.

ZHANG Kun-Shi and LIU Lian-Shou. The Saturation Phenomenon of Transverse Energy Distribution in Heavy-Ion Collisions and Multisource Modle[J]. Chinese Physics C, 1991, 15(7): 615-622. shu

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Received: 1900-01-01
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

The Saturation Phenomenon of Transverse Energy Distribution in Heavy-Ion Collisions and Multisource Modle

ZHANG Kun-Shi ^,
LIU Lian-Shou

Corresponding author: ZHANG Kun-Shi,

Jinzhou Teachers College,Jinzhou,Hubei 4341001 Institute of Particle Physics,Huazhong Normal University,Wuhan 430070

Received Date: 1900-01-01
Accepted Date: 1900-01-01
Available Online: 1991-07-05

Abstract: Based on a careful analysis of the mechanism of high energy non-equal mass nuclei collisions,the multisource modle is further developed.The transverse energy distribution in central rapidity region at both CERN and BNL energy domains are calculated.The saturation of transverse energy distribution at low energy is explained,and the minimum mass number of the target nucleus for this saturation effect (full stopping) to occur is obtained.