${}^{8}{Be}$ producing reactions in ${}^{12}C$ + ${}^{12}C$ , ${}^{16}O$ , + ${}^{16}O$ , and ${}^{28}{Si}$ + ${}^{12}C$

Publisher Website

1 January 1976

journal article
research article
Published by American Physical Society (APS) in Physical Review C

Vol. 13 (1) , 156-163
https://doi.org/10.1103/physrevc.13.156

Abstract

The

{}^{12}C

(

{}^{12}C

,

{}^{8}{Be}

),

{}^{16}O

(

{}^{16}O

,

{}^{8}{Be}

), and

{}^{28}{Si}

(

{}^{12}C

,

{}^{8}{Be}

) reactions show final state relative populations which are very similar to the corresponding (

{}^{6}{Li}, d

), (

{}^{7}{Li}, t

), (

{}^{12}C, α

), and (

{}^{16}O

,

{}^{12}C

) reactions on the same target nuclei. Selective population of final states for

{}^{12}C

and

{}^{28}{Si}

targets is accompanied by rapidly fluctuating excitation functions for the

{}^{12}C

(

{}^{12}C

,

{}^{8}{Be}

) reactions and much smoother, yet not flat, excitation functions for

{}^{28}{Si}

(

{}^{12}C

,

{}^{8}{Be}

). Angular distributions are forward peaked. The

{}^{16}O

(

{}^{16}O

,

{}^{8}{Be}

) reaction is not selective, similar to

{}^{16}O ({}^{12}C, α)

.

Keywords

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