1994
DOI: 10.1103/physrevc.49.955
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Quasielastic proton knockout fromO16

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Cited by 148 publications
(271 citation statements)
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“…[209] these wave functions have been used to analyze low Q 2 data for the 16 O(e,e ′ p) reaction [198]. These very same wave functions produce a good description of the shape of the coincidence cross section for the p-shell quasihole states at high Q 2 [259] using the same spectroscopic factors obtained from the low Q 2 data [198].…”
Section: Extraction Of Spectroscopic Information Frommentioning
confidence: 99%
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“…[209] these wave functions have been used to analyze low Q 2 data for the 16 O(e,e ′ p) reaction [198]. These very same wave functions produce a good description of the shape of the coincidence cross section for the p-shell quasihole states at high Q 2 [259] using the same spectroscopic factors obtained from the low Q 2 data [198].…”
Section: Extraction Of Spectroscopic Information Frommentioning
confidence: 99%
“…An analogous result holds for transition to the p 1/2 ground state of 15 N for which the same analysis yields a spectroscopic factor Z qh 0p1/2 = 0.644. For comparison, one may note that the use of phenomenological Woods-Saxon wave functions adjusted to fit the shape of the reduced cross section require spectroscopic factors ranging from 0.61 to 0.64 for the lowest 0p 1/2 state and from 0.50 to 0.59 for the 0p 3/2 state, respectively, depending upon the choice of the optical potential for the outgoing proton [198]. Figure 42 also contains the results for the reduced cross section derived from the variational result for overlap wave function of Pieper et al [181], who employed the Argonne v 14 potential for the NN interaction [135].…”
Section: Depletion Due To Short-range and Tensor Correlationsmentioning
confidence: 99%
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