Measurement of the recoil polarization in the p((e)over-right-arrow, e′(p)over-right-arrow)π0 reaction at the Δ(1232) resonance

被引:103
作者
Pospischil, T [1 ]
Bartsch, P
Baumann, D
Bermuth, J
Böhm, R
Bohinc, K
Derber, S
Ding, M
Distler, M
Drechsel, D
Elsner, D
Ewald, I
Friedrich, J
Friedrich, JM
Geigers, R
Hedicke, S
Jennewein, P
Kahrau, M
Kamalov, SS
Klein, F
Krygier, KW
Lac, J
Liesenfeld, A
McIntyre, J
Merkel, H
Merle, P
Müller, U
Neuhausen, R
Potokar, M
Ransome, RD
Rohe, D
Rosner, G
Schmieden, H
Seimetz, M
Sirca, S
Sick, I
Süle, A
Tiator, L
Wagner, A
Walcher, T
Warren, GA
Weis, M
机构
[1] Univ Mainz, Inst Kernphys, D-55099 Mainz, Germany
[2] Univ Mainz, Inst Phys, D-55099 Mainz, Germany
[3] Univ Ljubljana, Jozef Stefan Inst, SI-1001 Ljubljana, Slovenia
[4] Rutgers State Univ, Piscataway, NJ USA
[5] Univ Basel, Dept Phys & Astron, CH-4056 Basel, Switzerland
[6] Joint Inst Nucl Res Dubna, Theoret Phys Lab, Dubna, Russia
关键词
D O I
10.1103/PhysRevLett.86.2959
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
The recoil proton polarization has been measured in the p((e) over right arrow, e(1)(p) over right arrow)pi (0) reaction in parallel kinematics around W = 1232 MeV, Q(2) = 0.121 (GeV/c)(2) and epsilon = 0.718 using the polarized cw electron beam of the Mainz Microtron. All three proton polarization components, P-x/P-e = (-11.4 +/- 1.3 +/- 1.4)%, P-y = (-43.1 +/- 1.3 +/- 2.2)%, and P-z/P-e = (56.2 +/- 1.5 +/- 2.6)%, could be measured simultaneously. The Coulomb quadrupole to magnetic dipole ratio, CMR = (-6.4 +/- 0.7(stat) +/- 0.8(syst))%, was determined from P-x in the framework of the Mainz Unitary Isobar Model. The consistency among the reduced polarizations and the extraction of the ratio of longitudinal-to-transverse response is discussed.
引用
收藏
页码:2959 / 2962
页数:4
相关论文
共 28 条
[1]   PIO ELECTROPRODUCTION AT FIRST RESONANCE AT MOMENTUM-TRANSFERS Q-2=0.6, 1.0 AND 1.56 GEV-2 [J].
ALDER, JC ;
BRASSE, FW ;
CHAZELAS, E ;
MERKWITZ, M ;
MAY, J ;
GAYLER, J ;
GANSSENA.E ;
VALENTIN, J ;
TRISTRAM, G ;
FEHRENBA.W ;
FRANK, KH ;
FLAUGER, W ;
KORBEL, V ;
COURAU, A .
NUCLEAR PHYSICS B, 1972, B 46 (02) :573-&
[2]   The MAMI source of polarized electrons [J].
Aulenbacher, K ;
Nachtigall, C ;
Andresen, HG ;
Bermuth, J ;
Dombo, T ;
Drescher, P ;
Euteneuer, H ;
Fischer, H ;
vonHarrach, D ;
Hartmann, P ;
Hoffmann, J ;
Jennewein, P ;
Kaiser, KH ;
Kobis, S ;
Kreidel, HJ ;
Langbein, J ;
Petri, M ;
Plutzer, S ;
Reichert, E ;
Schemies, M ;
Schope, HJ ;
Steffens, KH ;
Steigerwald, M ;
Trautner, H ;
Weis, T .
NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT, 1997, 391 (03) :498-506
[3]   PI0 ELECTROPRODUCTION AT DELTA (1236) RESONANCE AT A 4-MOMENTUM TRANSFER OF Q2 = 0.3 (GEV/C)2 [J].
BATZNER, K ;
BECK, U ;
BECKS, KH ;
DREES, J ;
KNOP, G ;
KOLANOSK.H ;
LEENEN, M ;
MOSER, K ;
NIETZEL, C ;
SCHLOSSE.E ;
STIER, HE .
NUCLEAR PHYSICS B, 1974, B 76 (01) :1-14
[4]   Determination of the E2/M1 ratio in the yN→Δ(1232) transition from a simultaneous measurement of p((γ)over-right-arrow,p)π0 and p((γ)over-right-arrow, π+)n -: art. no. 035204 [J].
Beck, R ;
Krahn, HP ;
Ahrens, J ;
Annand, JRM ;
Arends, HJ ;
Audit, G ;
Braghieri, A ;
d'Hose, N ;
Drechsel, D ;
Hanstein, O ;
McGeorge, JC ;
Owens, RO ;
Pedroni, P ;
Pinelli, T ;
Tamas, G ;
Tiator, L ;
Walcher, T .
PHYSICAL REVIEW C, 2000, 61 (03) :352041-3520414
[5]   Measurement of the E2/M1 ratio in the N->Delta transition using the reaction p((gamma)over-right-arrow,p)pi(0) [J].
Beck, R ;
Krahn, HP ;
Ahrens, J ;
Arends, HJ ;
Audit, G ;
Braghieri, A ;
dHose, N ;
Hall, SJ ;
Isbert, V ;
Kellie, JD ;
MacGregor, IJD ;
Pedroni, P ;
Pinelli, T ;
Tamas, G ;
Walcher, T ;
Wartenberg, S .
PHYSICAL REVIEW LETTERS, 1997, 78 (04) :606-609
[6]   N->Delta transition from simultaneous measurements of p((gamma)over-right-arrow,pi) and p((gamma)over-right-arrow,gamma) [J].
Blanpied, G ;
Blecher, M ;
Caracappa, A ;
Djalali, C ;
Giordano, G ;
Hicks, K ;
Hoblit, S ;
Khandaker, M ;
Kistner, OC ;
Kuczewski, A ;
Lowry, M ;
Lucas, M ;
Matone, G ;
Miceli, L ;
Preedom, B ;
Rebreyend, D ;
Sandorfi, AM ;
Schaerf, C ;
Sealock, RM ;
Stroher, H ;
Thorn, CE ;
Thornton, ST ;
Tonnison, J ;
Whisnant, CS ;
Zhang, H ;
Zhao, X .
PHYSICAL REVIEW LETTERS, 1997, 79 (22) :4337-4340
[7]   The three-spectrometer facility at the Mainz microtron MAMI [J].
Blomqvist, KI ;
Boeglin, WU ;
Bohm, R ;
Distler, M ;
Edelhoff, R ;
Friedrich, J ;
Geiges, R ;
Jennewein, P ;
Kahrau, M ;
Korn, M ;
Kramer, H ;
Krygier, KW ;
Kunde, V ;
Liesenfeld, A ;
Merkel, H ;
Merle, K ;
Muller, U ;
Neuhausen, R ;
Offermann, EAJM ;
Pospischil, T ;
Richter, AW ;
Rosner, G ;
Sauer, P ;
Schardt, S ;
Schmieden, H ;
Wagner, A ;
Walcher, T ;
Wolf, S .
NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT, 1998, 403 (2-3) :263-301
[8]   HADRON MASSES IN A GAUGE THEORY [J].
DERUJULA, A ;
GEORGI, H ;
GLASHOW, SL .
PHYSICAL REVIEW D, 1975, 12 (01) :147-162
[9]   A unitary isobar model for pion photo- and electroproduction on the proton up to 1 GeV [J].
Drechsel, D ;
Hanstein, O ;
Kamalov, SS ;
Tiator, L .
NUCLEAR PHYSICS A, 1999, 645 (01) :145-174
[10]   THRESHOLD PION-PHOTOPRODUCTION ON NUCLEONS [J].
DRECHSEL, D ;
TIATOR, L .
JOURNAL OF PHYSICS G-NUCLEAR AND PARTICLE PHYSICS, 1992, 18 (03) :449-497