6533b7ddfe1ef96bd1275131
RESEARCH PRODUCT
Measurement of the Longitudinal, Transverse, and Longitudinal-Transverse Structure Functions in theH2(e,e′p)nReaction
R. A. MiskimenWilliam BertozziD. J. MargaziotisW. KimS. DolfiniS. DolfiniM. EpsteinS. PennS. PennW.w. SappJ. GörgenR. BeckR. BeckShalev GiladK. JooW. TurchinetzK. A. DowRicardo AlarconA. J. SartyLarry WeinsteinLarry WeinsteinD. MartinezC. TschalaerJiahao ChenJiahao ChenD. S. DaleD. S. DaleD. JordanD. JordanR. M. LaszewskiJ. KelseyGlen A. WarrenM. HoltropJ. DzengeleskiJoseph B. MandevilleJoseph B. MandevilleR.w. LourieW. BoeglinW. BoeglinM. FarkhondehS. E. WilliamsonG. W. DodsonCostas N. PapanicolasCostas N. PapanicolasD. R. TiegerV. BhushanT. McilvainT. Mcilvainsubject
PhysicsTransverse planeMesonCondensed matter physicsStructure functionIsobarGeneral Physics and AstronomyAtomic physicsOmegadescription
We have separated the longitudinal ({ital f}{sub 00}), transverse ({ital f}{sub 11}), and longitudinal-transverse interference ({ital f}{sub 01}) structure functions in the {sup 2}H({ital e},{ital e}{prime}{ital p}){ital n} reaction at {ital q}{searrow}{parallel}{approx_equal} 400 MeV/{ital c} and {omega}{approx_equal}110 MeV. A nonrelativistic calculation which includes effects due to final state interactions, meson exchange currents, and isobar configurations agrees with the measured {ital f}{sub 11} and {ital f}{sub 01} but overpredicts {ital f}{sub 00} by 25{percent} (2{sigma}). The data are also compared to the results of previous structure function measurements. {copyright} {ital 1996 The American Physical Society.}
| year | journal | country | edition | language |
|---|---|---|---|---|
| 1996-03-04 | Physical Review Letters |