ENTRY E2152 20100514 E062E215200000001 SUBENT E2152001 20100514 E062E215200100001 BIB 15 51 E215200100002 TITLE Polarization transfer measurements for E215200100003 12C(p,n)12N(g.s.,1+) at 296 MeV and nuclear E215200100004 correlation effects E215200100005 AUTHOR (M.Dozono, T.Wakasa, E.Ihara, S.Asaji, K.Fujita, E215200100006 K.Hatanaka, M.Ichimura, T.Ishida, T.Kaneda, E215200100007 H.Matsubara, Y.Nagasue, T.Noro, Y.Sakemi, Y.Shimizu, E215200100008 H.Takeda, Y.Tameshige, A.Tamii, Y.Yamada) E215200100009 INSTITUTE (2JPNKYU) Department of Physics E215200100010 (2JPNOSA) Research Center for Nuclear Physics E215200100011 (2JPNHOS) Faculty of Computer and Information Sciences E215200100012 (2JPNTOH) Cyclotron and Radioisotope Center E215200100013 (2JPNTOK) Center for Nuclear Study E215200100014 REFERENCE (J,PR/C,80,(2),024319,200908) E215200100015 PART-DET (P,N) E215200100016 EN-SEC (E-LVL,7-N-12) E215200100017 LEVEL-PROP (7-N-12,E-LVL=0.,SPIN=1.,PARITY=+1.) E215200100018 INC-SOURCE Beam intensity is 500 nA. E215200100019 (POLIS) POL-BM: measured by beam-line polarimeter E215200100020 (BLP1, BLP2) via 1H(p,p)1H scattering E215200100021 SAMPLE - Target is natural. 98.9% 12C E215200100022 - Chemical-form of target is element. E215200100023 - Physical-form of target is solid. E215200100024 - Target-thickness is 89 mg/cm**2. E215200100025 METHOD (TOF) E215200100026 (COINC) Elastically scattered and recoil protons via E215200100027 1H(p,p)1H E215200100028 FACILITY (ISOCY,2JPNOSA) Research Center for Nuclear Physics E215200100029 DETECTOR - E-RSL: FWHM. Due to the target energy loss and the E215200100030 beam pulse width of about 270 and 350 keV E215200100031 - Efficiency: Efficiency of NPOL3(HD1 and HD2) was E215200100032 determined by using measurement of 7Li(p,n)7Be(g.s. E215200100033 +0.43 MeV). E215200100034 - CPV and CPD were used to veto and identify charged E215200100035 particles, respectively. E215200100036 (TELES,SCIN,SCIN) NPOL3 consists of three planes of E215200100037 scintillation detectors. 2 detectors E215200100038 (HD1, HD2) consists of 10 sets of E215200100039 one-dimensional position-sensitive E215200100040 plastic scintillation counters. NC E215200100041 is two-dimensional E215200100042 position-sensitive liquid E215200100043 scintillation counter. E215200100044 ADD-RES Angular distribution and vector analyzing power E215200100045 (E2081.002-003) E215200100046 (COMP) DWIA (Distorted wave impulse approximation) E215200100047 REL-REF (N,E2081002,T.Wakasa+,J,PL/B,656,38,2007) E215200100048 Data in Fig.4 of J,PR/C,80,024319,2009 given E215200100049 (N,E2081003,T.Wakasa+,J,PL/B,656,38,2007) E215200100050 Data in Fig.5 (Ay) of J,PR/C,80,024319,2009 given E215200100051 HISTORY (20091027C) Ayano Makinaga E215200100052 (20091114R) Received by e-mail from T.Wakasa E215200100053 ENDBIB 51 0 E215200100054 COMMON 4 3 E215200100055 EN POL-BM E-RSL-FW E-LVL E215200100056 MEV NO-DIM KEV MEV E215200100057 296. 0.7 500. 0. E215200100058 ENDCOMMON 3 0 E215200100059 ENDSUBENT 58 0 E215200199999 SUBENT E2152002 20100514 E062E215200200001 BIB 3 4 E215200200002 REACTION (6-C-12(P,N)7-N-12,NN,POL/DA,,D) E215200200003 ERR-ANALYS (ERR-T) Total uncertainty E215200200004 (ERR-S) Statistical uncertainty E215200200005 STATUS (TABLE) Plotted in Fig.5 of J,PR/C,80,024319,2009 E215200200006 ENDBIB 4 0 E215200200007 NOCOMMON 0 0 E215200200008 DATA 4 11 E215200200009 q DATA ERR-S ERR-T E215200200010 1/FM NO-DIM NO-DIM NO-DIM E215200200011 0.136 -.2178 .0256 .0270 E215200200012 0.20 -.0958 .0441 .0463 E215200200013 0.40 -.0031 .0617 .0661 E215200200014 0.60 .2974 .0956 .1019 E215200200015 0.80 .1570 .1351 .1410 E215200200016 1.00 -.5272 .1599 .1847 E215200200017 1.20 -.4377 .2015 .2918 E215200200018 1.40 -.0189 .2058 .2868 E215200200019 1.60 -.3639 .2091 .2828 E215200200020 1.80 -.4663 .2295 .3386 E215200200021 2.00 .3211 .3420 .5514 E215200200022 ENDDATA 13 0 E215200200023 ENDSUBENT 22 0 E215200299999 SUBENT E2152003 20100514 E062E215200300001 BIB 3 4 E215200300002 REACTION (6-C-12(P,N)7-N-12,SS,POL/DA,,D) E215200300003 ERR-ANALYS (ERR-T) Total uncertainty E215200300004 (ERR-S) Statistical uncertainty E215200300005 STATUS (TABLE) Plotted in Fig.5 of J,PR/C,80,024319,2009 E215200300006 ENDBIB 4 0 E215200300007 NOCOMMON 0 0 E215200300008 DATA 4 11 E215200300009 q DATA ERR-S ERR-T E215200300010 1/FM NO-DIM NO-DIM NO-DIM E215200300011 0.136 -.2660 .0370 .0386 E215200300012 0.20 -.2544 .0681 .0718 E215200300013 0.40 -.6992 .0991 .1052 E215200300014 0.60 -.7871 .1070 .1134 E215200300015 0.80 -.2669 .1739 .1822 E215200300016 1.00 .4034 .1958 .2234 E215200300017 1.20 -.0853 .2303 .3269 E215200300018 1.40 -.4124 .2267 .3286 E215200300019 1.60 -.1395 .2312 .3183 E215200300020 1.80 .3294 .2344 .3435 E215200300021 2.00 -.0022 .3208 .5031 E215200300022 ENDDATA 13 0 E215200300023 ENDSUBENT 22 0 E215200399999 SUBENT E2152004 20100514 E062E215200400001 BIB 3 4 E215200400002 REACTION (6-C-12(P,N)7-N-12,SL,POL/DA,,D) E215200400003 ERR-ANALYS (ERR-T) Total uncertainty E215200400004 (ERR-S) Statistical uncertainty E215200400005 STATUS (TABLE) Plotted in Fig.5 of J,PR/C,80,024319,2009 E215200400006 ENDBIB 4 0 E215200400007 NOCOMMON 0 0 E215200400008 DATA 4 11 E215200400009 q DATA ERR-S ERR-T E215200400010 1/FM NO-DIM NO-DIM NO-DIM E215200400011 0.136 .0616 .0375 .0391 E215200400012 0.20 .0271 .0690 .0723 E215200400013 0.40 .1825 .1007 .1072 E215200400014 0.60 .2018 .1076 .1137 E215200400015 0.80 .1745 .1743 .1827 E215200400016 1.00 -.2022 .1959 .2236 E215200400017 1.20 -.2856 .2300 .3266 E215200400018 1.40 .4314 .2258 .3262 E215200400019 1.60 .3257 .2281 .3127 E215200400020 1.80 .4253 .2361 .3459 E215200400021 2.00 1.0615 .3186 .4980 E215200400022 ENDDATA 13 0 E215200400023 ENDSUBENT 22 0 E215200499999 SUBENT E2152005 20100514 E062E215200500001 BIB 3 4 E215200500002 REACTION (6-C-12(P,N)7-N-12,LL,POL/DA,,D) E215200500003 ERR-ANALYS (ERR-T) Total uncertainty E215200500004 (ERR-S) Statistical uncertainty E215200500005 STATUS (TABLE) Plotted in Fig.5 of J,PR/C,80,024319,2009 E215200500006 ENDBIB 4 0 E215200500007 NOCOMMON 0 0 E215200500008 DATA 4 11 E215200500009 q DATA ERR-S ERR-T E215200500010 1/FM NO-DIM NO-DIM NO-DIM E215200500011 0.136 -.5236 .0321 .0333 E215200500012 0.20 -.4734 .0652 .0683 E215200500013 0.40 -.2621 .0988 .1052 E215200500014 0.60 -.3215 .1109 .1170 E215200500015 0.80 -.7887 .1838 .1925 E215200500016 1.00 -.8695 .2109 .2411 E215200500017 1.20 .1711 .2617 .3665 E215200500018 1.40 .0829 .2470 .3614 E215200500019 1.60 -.2797 .2377 .3362 E215200500020 1.80 -.6110 .2409 .3605 E215200500021 2.00 -.3053 .3293 .5541 E215200500022 ENDDATA 13 0 E215200500023 ENDSUBENT 22 0 E215200599999 SUBENT E2152006 20100514 E062E215200600001 BIB 3 4 E215200600002 REACTION (6-C-12(P,N)7-N-12,LS,POL/DA,,D) E215200600003 ERR-ANALYS (ERR-T) Total uncertainty E215200600004 (ERR-S) Statistical uncertainty E215200600005 STATUS (TABLE) Plotted in Fig.5 of J,PR/C,80,024319,2009 E215200600006 ENDBIB 4 0 E215200600007 NOCOMMON 0 0 E215200600008 DATA 4 11 E215200600009 q DATA ERR-S ERR-T E215200600010 1/FM NO-DIM NO-DIM NO-DIM E215200600011 0.136 -.0235 .0317 .0331 E215200600012 0.20 .1450 .0643 .0679 E215200600013 0.40 .5484 .0972 .1032 E215200600014 0.60 .1882 .1102 .1169 E215200600015 0.80 .1106 .1836 .1920 E215200600016 1.00 -.0563 .2107 .2408 E215200600017 1.20 -.8101 .2622 .3672 E215200600018 1.40 -.4802 .2485 .3635 E215200600019 1.60 -.4694 .2393 .3411 E215200600020 1.80 -.1988 .2411 .3643 E215200600021 2.00 .0384 .3266 .5555 E215200600022 ENDDATA 13 0 E215200600023 ENDSUBENT 22 0 E215200699999 ENDENTRY 6 0 E215299999999