Paolone, MMalace, SPStrauch, SAlbayrak, IArrington, JBerman, BLBrash, EJBriscoe, BCamsonne, AChen, J-PChristy, MEChudakov, ECisbani, ECraver, BCusanno, FEnt, RGaribaldi, FGilman, RGlamazdin, OGlister, JHiginbotham, DWHyde-Wright, CEIlieva, Yde Jager, CWJiang, XJones, MKKeppel, CEKhrosinkova, EKuchina, EKumbartzki, GLee, BLindgren, RMargaziotis, DJMeekins, DMichaels, RPark, KPentchev, LPerdrisat, CFPiasetzky, EPunjabi, VAPuckett, AJRQian, XQiang, YRansome, RDSaha, ASarty, AJSchulte, ESolvignon, PSubedi, RRTang, LTedeschi, DTvaskis, VUdias, JMUlmer, PEVignote, JRWesselmann, FRWojtsekhowski, BZhan, XE03-104 Collaboration2011-06-212011-06-212010Paolone,M.;Malace,S. P.;Strauch,S.;Albayrak,I.;Arrington,J.;Berman,B. L.;Brash,E. J.;Briscoe,B.;Camsonne,A.;Chen,J. -P;Christy,M. E.;Chudakov,E.;Cisbani,E.;Craver,B.;Cusanno,F.;Ent,R.;Garibaldi,F.;Gilman,R.;Glamazdin,O.;Glister,J.;Higinbotham,D. W.;Hyde-Wright,C. E.;Ilieva,Y.;de Jager,C. W.;Jiang,X.;Jones,M. K.;Keppel,C. E.;Khrosinkova,E.;Kuchina,E.;Kumbartzki,G.;Lee,B.;Lindgren,R.;Margaziotis,D. J.;Meekins,D.;Michaels,R.;Park,K.;Pentchev,L.;Perdrisat,C. F.;Piasetzky,E.;Punjabi,V. A.;Puckett,A. J. R.;Qian,X.;Qiang,Y.;Ransome,R. D.;Saha,A.;Sarty,A. J.;Schulte,E.;Solvignon,P.;Subedi,R. R.;Tang,L.;Tedeschi,D.;Tvaskis,V.;Udias,J. M.;Ulmer,P. E.;Vignote,J. R.;Wesselmann,F. R.;Wojtsekhowski,B.;Zhan,X.;E03-104 Collaboration. 2010. Polarization Transfer in the He-4((e)over-right-arrow, e '(p)over-right-arrow)H-3 Reaction at Q(2)=0.8 and 1.3 (GeV/c)(2). Physical Review Letters 105(7): 72001-72001.0031-9007https://hdl.handle.net/10161/4298Proton recoil polarization was measured in the quasielastic He-4((e) over right arrow, e '(p) over right arrow)H-3 reaction at Q(2) = 0.8 and 1.3 (GeV/c)(2) with unprecedented precision. The polarization-transfer coefficients are found to differ from those of the H-1((e) over right arrow, e '(p) over right arrow) reaction, contradicting a relativistic distorted-wave approximation and favoring either the inclusion of medium-modified proton form factors predicted by the quark-meson coupling model or a spin-dependent charge-exchange final-state interaction. For the first time, the polarization-transfer ratio is studied as a function of the virtuality of the proton.en-USelectromagnetic form-factorsimpulse approximationbound nucleonsscatteringphysics, multidisciplinary