Threshold Electrodisintegration of ^3He

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dc.creatorHicks, R. S.
dc.creatorHotta, A.
dc.creatorChurchwell, S.
dc.creatorJiang, X.
dc.creatorPeterson, G. A.
dc.creatorShaw, J.
dc.creatorAsavapibhop, B.
dc.creatorBerisso, M. C.
dc.creatorBosted, P. E.
dc.creatorBurchesky, K.
dc.creatorMiskimen, R. A.
dc.creatorRock, S. E.
dc.creatorNakagawa, I.
dc.creatorTamae, T.
dc.creatorSuda, T.
dc.creatorGolak, J.
dc.creatorSkibinski, R.
dc.creatorWitala, H.
dc.creatorCasagrande, F.
dc.creatorTurchinetz, W.
dc.creatorCichocki, A.
dc.creatorWang, K.
dc.creatorGlockle, W.
dc.creatorKamada, H.
dc.creatorKobayashi, T.
dc.creatorNogga, A.
dc.date2003-03-06
dc.date2003-05-15
dc.date.accessioned2026-07-07T10:30:26Z
dc.date.available2026-07-07T10:30:26Z
dc.descriptionCross sections were measured for the near-threshold electrodisintegration of ^3He at momentum transfer values of q=2.4, 4.4, and 4.7 fm^{-1}. From these and prior measurements the transverse and longitudinal response functions R_T and R_L were deduced. Comparisons are made against previously published and new non-relativistic A=3 calculations using the best available NN potentials. In general, for q<2 fm^{-1} these calculations accurately predict the threshold electrodisintegration of ^3He. Agreement at increasing q demands consideration of two-body terms, but discrepancies still appear at the highest momentum transfers probed, perhaps due to the neglect of relativistic dynamics, or to the underestimation of high-momentum wave-function components.
dc.description9 pages, 7 figures, 1 table, REVTEX4, submitted to Physical Review C
dc.identifierhttps://arxiv.org/abs/nucl-ex/0303003
dc.identifierhttp://arxiv.org/abs/nucl-ex/0303003
dc.identifierPhys.Rev.C67:064004,2003
dc.identifierdoi:10.1103/PhysRevC.67.064004
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/178128
dc.subjectNuclear Experiment
dc.titleThreshold Electrodisintegration of ^3He
dc.typetext

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