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Sanford-Wang parameterisation : ウィキペディア英語版
Sanford-Wang parameterisation

The Sanford-Wang parameterisation is an empirical formula used to model the production of pions in nuclear interaction of the form p+A → \pi^++X where a beam of high-energy protons hit a material.
Its formula for the double-differential cross section with respect to momentum (p) and solid angle (\Omega) is as follows.
\frac(p,\theta) =
c_1 p^ \left(1-\frac}}-c_6\theta(p-c_7" TITLE="-c_3\frac^}-c_6\theta(p-c_7">p_ (\cos\theta)^)\right )
Where p and \theta are the momentum of the outgoing pion and its angle from the direction of the incident proton. The numbers c_1\ldots c_8 are the ''Sanford-Wang parameters'' and are typically varied to give a good fit with experimental data.
== References ==

* J. R. Sanford and C. L. Wang, Brookhaven National Laboratory, AGS internal report, 1967 (unpublished); C. L. Wang, Phys. Rev. Letters 25, 1068 (1970); ibid. 25, 1536(E) (1970).

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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