6533b82dfe1ef96bd1291cc4

RESEARCH PRODUCT

Mechanisms in theC12(γ,pn)and(γ,pp)Reactions

J. C. McgeorgeR. SchneiderP.d. HartyJan RyckebuschT. HehlM. LiangT. LamparterJrm AnnandJohn A. MackenzieJ. AhrensP. GrabmayrM. SauerS. McallisterI. J. D. MacgregorJ. D. KellieR. BeckS.j. HallD. BranfordR.o. OwensD. P. WattsT.t.h. Yau

subject

PhysicsGeneral Physics and AstronomyPropagatorAngular dependenceAtomic physicsPhoton energy

description

${}^{12}\mathrm{C}(\ensuremath{\gamma},pn)$ and $(\ensuremath{\gamma},pp)$ cross sections have been measured in kinematics which emphasize direct $2N$ knockout for ${E}_{\ensuremath{\gamma}}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}120--400\mathrm{MeV}$ and ${\ensuremath{\theta}}_{p}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}23\ifmmode^\circ\else\textdegree\fi{}--152\ifmmode^\circ\else\textdegree\fi{}$. The cross sections for both reactions peak strongly in the $\ensuremath{\Delta}$-resonance region. Theoretical calculations that account for the medium dependence of the $\ensuremath{\Delta}$ propagator predict a similar photon energy dependence to the data and describe the general trends of the measured $(\ensuremath{\gamma},pp)/(\ensuremath{\gamma},pn)$ ratio. Both cross sections show strong angular dependence, and the large differences between the two channels indicate different microscopic reaction mechanisms.

https://doi.org/10.1103/physrevlett.80.245