ENTRY O2273 20201209 O081O227300000001 SUBENT O2273001 20201209 O081O227300100001 BIB 10 28 O227300100002 TITLE 12C+p resonant elastic scattering in the Maya active O227300100003 target. O227300100004 AUTHOR (S.Sambi,R.Raabe,M.J.G.Borge,M.Caamano,S.Damoy, O227300100005 B.Fernandez-Dominguez,F.Flavigny,H.Fynbo,J.Gibelin, O227300100006 G.F.Grinyer,A.Heinz,B.Jonson,M.Khodery,T.Nilsson, O227300100007 R.Orlandi,J.Pancin,D.Perez-Loureiro,G.Randisi, O227300100008 G.Ribeiro,T.Roger,D.Suzuki,O.Tengblad,R.Thies,U.Datta) O227300100009 REFERENCE (J,EPJ/A,51,25,2015) O227300100010 INSTITUTE (2BLGLEU,2ZZZCER,2SPNSAU,2FR GAN,2DENAAU,2FR CAE, O227300100011 2SWDCTH,2SPNIEM,2JPNJAE,2FR PAR,3INDSAH) O227300100012 FACILITY (CYCTM,2FR GAN) the SPIRAL facility based on the O227300100013 Isotope Separation on Line (ISOL) technique of beam O227300100014 production. O227300100015 INC-SOURCE The 12Be beam, produced at ISOLDE, bunched and O227300100016 accelerated up to 2.85 MeV/nucleon, had an intensity O227300100017 of approx.45 pps in Maya. O227300100018 SAMPLE A isobutane (C4H10) gas target. In the present O227300100019 experiment, the isobutane was at a pressure of 160 mbarO227300100020 METHOD (EDE) O227300100021 DETECTOR (TELES,SI) O227300100022 The Maya detector is a gaseous active target, the O227300100023 volume of the active zone is 28*25*20 cm**3 O227300100024 (DRFTC) a thin drift chamber was placed at the end of O227300100025 the active volume right before the Si detectors, O227300100026 surrounded by the gas of Maya. O227300100027 HISTORY (20151108C) SB O227300100028 (20201209U) SD: INSTITUTE code modified O227300100029 (2SPNPCM -> 2SPNIEM).O227300100030 ENDBIB 28 0 O227300100031 NOCOMMON 0 0 O227300100032 ENDSUBENT 31 0 O227300199999 SUBENT O2273002 20151108 O055O227300200001 BIB 3 10 O227300200002 REACTION 1(6-C-12(P,EL),,WID) O227300200003 2(6-C-12(P,0),,J) O227300200004 3(6-C-12(P,0),,PTY) O227300200005 ERR-ANALYS (DATA-ERR).No information on source of uncertainty O227300200006 (EN-RES-ERR).The estimated uncertainty depends on the O227300200007 energy resolution of the silicon detectors and on the O227300200008 possibility of correctly fitting the particle O227300200009 trajectory, from which was extract the proton O227300200010 scattering angle. O227300200011 STATUS (TABLE).Table 1 of J,EPJ/A,51,25,2015 O227300200012 ENDBIB 10 0 O227300200013 NOCOMMON 0 0 O227300200014 DATA 6 3 O227300200015 EN-RES-CM EN-RES-ERR DATA-CM 1DATA-ERR 1DATA 2DATA 3O227300200016 KEV KEV KEV KEV NO-DIM NO-DIM O227300200017 421.4 0.6 18. 13. 0.5 1. O227300200018 1559. 2. 28. 13. 1.5 -1. O227300200019 1604. 4. 48. 8. 2.5 1. O227300200020 ENDDATA 5 0 O227300200021 ENDSUBENT 20 0 O227300299999 ENDENTRY 2 0 O227399999999