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20 April 2024 |
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Dynamics of the 16O(e, e'p) reaction at high missing energies | N Liyanage
; B D Anderson
; K A Aniol
; L Auerbach
; F T Baker
; J Berthot
; W Bertozzi
; P Y Bertin
; L Bimbot
; W U Boeglin
; E J Brash
; V Breton
; H Breuer
; E Burtin
; J R Calarco
; L Cardman
; G D Cates
; C Cavata
; C C Chang
; J P Chen
; E Cisbani
; D S Dale
; R De Leo
; A Deur
; B Diederich
; P Djawotho
; J Domingo
; B Doyle
; J E Ducret
; M B Epstein
; L A Ewell
; J M Finn
; K G Fissum
; H Fonvieille
; B Frois
; S Frullani
; J Gao
; F Garibaldi
; A Gasparian
; S Gilad
; R Gilman
; A Glamazdin
; C Glashausser
; J Gomez
; V Gorbenko
; T Gorringe
; F W Hersman
; R Holmes
; M Holtrop
; N d’Hose
; C Howell
; G M Huber
; C E Hyde-Wright
; M Iodice
; C W de Jager
; S Jaminion
; M K Jones
; K Joo
; C Jutier
; W Kahl
; S Kato
; J J Kelly
; S Kerhoas
; M Khandaker
; M Khayat
; K Kino
; W Korsch
; L Kramer
; K S Kumar
; G Kumbartzki
; G Laveissière
; A Leone
; J J LeRose
; L Levchuk
; M Liang
; R A Lindgren
; G J Lolos
; R W Lourie
; R Madey
; K Maeda
; S Malov
; D M Manley
; D J Margaziotis
; P Markowitz
; J Martino
; J S McCarthy
; K McCormick
; J McIntyre
; R L van der Meer
; Z E Meziani
; R Michaels
; J Mougey
; S Nanda
; D Neyret
; E A Offermann
; Z Papandreou
; C F Perdrisat
; R Perrino
; G G Petratos
; S Platchkov
; R Pomatsalyuk
; D L Prout
; V A Punjabi
; T Pussieux
; G Quéméner
; R D Ransome
; O Ravel
; Y Roblin
; R Roche
; D Rowntree
; G A Rutledge
; P M Rutt
; A Saha
; T Saito
; A J Sarty
; A Serdarevic-Offermann
; T P Smith
; A Soldi
; P Sorokin
; P Souder
; R Suleiman
; J A Templon
; T Terasawa
; L Todor
; H Tsubota
; H Ueno
; P E Ulmer
; G M Urciuoli
; P Vernin
; S van Verst
; B Vlahovic
; H Voskanyan
; J W Watson
; L B Weinstein
; K Wijesooriya
; R Wilson
; B Wojtsekhowski
; D G Zainea
; V Zeps
; J Zhao
; Z L Zhou
; | Date: |
18 Jun 2001 | Journal: | Phys Rev Lett, 86 (25), 5670-4 | Abstract: | We measured the cross section and response functions for the quasielastic 16O(e,e’p) reaction for missing energies 25< or =E(m)< or =120 MeV at missing momenta P(m)< or =340 MeV/c. For 25<E(m)<50 MeV and P(m) approximately 60 MeV/c, the reaction is dominated by a single 1s(1/2) proton knockout. At larger P(m), the single-particle aspects are increasingly masked by more complicated processes. Calculations which include pion exchange currents, isobar currents, and short-range correlations account for the shape and the transversity, but for only half of the magnitude of the measured cross section. | Source: | PubMed, pmid11415329 | Services: | Forum | Review | Favorites |
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