Chinese Physics C > 1989, Vol. 13 > Issue(10): 942-955

A MEMORY PARTICLE MODEL IN STUDY OF PRE-EQUILIBRIUM EMISSION

MIAO Rong-Zhi^,

Institute of Modern Physics,Academia Sinica,Lanzhou

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Abstract：
Exciton of a composite system at high energy is divided into two subsystems which consist of memory particle m and non-memory particle r.After introducing a _nthe collision factor of m-particle in state n,the coupled master equitions of the occupation probability of stateangle of m-particle and r-particle are established.The expression of state density,taking into account the distinquishability between m-particle and r-particle,and the formulas of the rate of β-particle emission of m-system and r-system in state n are also given.The calculation results show that the fit with experimental data is improved conspicuously and is much better than that obtained from the generalized exciton mdel.

References

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MIAO Rong-Zhi. A MEMORY PARTICLE MODEL IN STUDY OF PRE-EQUILIBRIUM EMISSION[J]. Chinese Physics C, 1989, 13(10): 942-955.

MIAO Rong-Zhi. A MEMORY PARTICLE MODEL IN STUDY OF PRE-EQUILIBRIUM EMISSION[J]. Chinese Physics C, 1989, 13(10): 942-955. 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

A MEMORY PARTICLE MODEL IN STUDY OF PRE-EQUILIBRIUM EMISSION

MIAO Rong-Zhi^,

Corresponding author:MIAO Rong-Zhi,

Institute of Modern Physics,Academia Sinica,Lanzhou

Received Date:1900-01-01
Accepted Date:1900-01-01
Available Online:1989-10-05

Abstract:Exciton of a composite system at high energy is divided into two subsystems which consist of memory particle m and non-memory particle r.After introducing a_nthe collision factor of m-particle in state n,the coupled master equitions of the occupation probability of stateangle of m-particle and r-particle are established.The expression of state density,taking into account the distinquishability between m-particle and r-particle,and the formulas of the rate of β-particle emission of m-system and r-system in state n are also given.The calculation results show that the fit with experimental data is improved conspicuously and is much better than that obtained from the generalized exciton mdel.