6533b839fe1ef96bd12a59c4

RESEARCH PRODUCT

Pion electroproduction in the 3He(e,é π+)3H reaction at intermediate energies

Achim RichterB. VodenikJ.m. FriedrichK. W. KrygierS. SchardtA.w. RichterP. SauerE. A. J. M. OffermannK. MerleA. LiesenfeldTh. WalcherM. KornV. KundeM. KussChary RangacharyuluR. NeuhausenM. PotokarS. WolfJ.m. LagetR. BöhmA. RokavecH. KramerS.s. KamalovM. KohlToshio SudaMariana KirchbachR. GeigesM. O. DistlerG. SchriederA. WagnerM. KahrauW.u. BoeglinR. EdelhoffK. I. BlomqvistG. RosnerL. TiatorTh. Pospischil

subject

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryParticle acceleratorResonance (particle physics)law.inventionNuclear physicsCross section (physics)AmplitudePionCoincidentlawHigh Energy Physics::ExperimentNuclear ExperimentWave functionMicrotron

description

Abstract The differential coincident pion electroproduction cross section in the 3 He(e,e π + ) 3 H reaction has been measured with high resolution with the three-spectrometer set-up at the Mainz Microtron (MAMI) electron accelerator. Measurements were performed at the four incident energies E 0 = 855, 675, 600, and 555 MeV at fixed four-momentum transfer Q 2 = 0.045 GeV 2 , with the pions detected in parallel kinematics. This enables a separation of the measured cross section into the transverse and longitudinal structure functions by means of the Rosenbluth method. The experimental data are compared to model calculations, in which the elementary pion production amplitude includes the standard Born-amplitudes and also delta and higher resonance terms. Three-body Fadeev wave functions are used and the final state interaction of the outgoing pion is taken into account. The calculation describes the data only after medium modifications of the delta and of the pion are included.

https://doi.org/10.1016/s0375-9474(97)00463-6