ENTRY C1831 20111206 C112C183100000001 SUBENT C1831001 20111206 C112C183100100001 BIB 11 31 C183100100002 TITLE Fusion Reactions with the One-Neutron Halo Nucleus 15C C183100100003 AUTHOR (M.Alcorta,K.E.Rehm,B.B.Back,S.Bedoor,P.F.Bertone, C183100100004 C.M.Deibel,B.Digiovine,H.Esbensen,J.P.Greene, C183100100005 C.R.Hoffmann,C.L.Jiang,J.C.Lighthall,S.T.Marley, C183100100006 R.C.Pardo,M.Paul,A.M.Rogers,C.Ugalde,A.H.Wuosmaa) C183100100007 INSTITUTE (1USAANL,1USAWMU,1USAMSU,3ISLHEB,1USACHI) C183100100008 REFERENCE (J,PRL,106,172701,2011) C183100100009 FACILITY (LINAC,1USAANL) Experiment performed at ATLAS C183100100010 facility at Argonne National Laboratory C183100100011 SAMPLE 232Th sample with thickness of 640 mu-g/cm2 C183100100012 DETECTOR (SIBAR) Four 5 x 5 cm2 Si surface barrier detectors C183100100013 subdivided into four quadrants surrounded the 232Th C183100100014 target with two pairs opposite to each other, C183100100015 covering the angular range between 25deg and 70deg C183100100016 and between 115deg and 160deg. C183100100017 INC-SOURCE The 15C beam was produced via the in-flight technique C183100100018 by bombarding a cryogenically cooled gas cell filled C183100100019 with deuterium at 1.4 atm with an intense (100 pnA) C183100100020 14C beam delivered by the ATLAS accelerator. The 15C C183100100021 ions produced via the d(14C,15C)p reaction were C183100100022 focused with a superconducting solenoid located C183100100023 behind the gas cell and rebunched with a C183100100024 superconducting resonator.Energy changes for C183100100025 excitation function measurement were achieved by Au C183100100026 energy degrading foils. C183100100027 ERR-ANALYS (DATA-ERR) No information given C183100100028 ANALYSIS Relative normalization of 13,14,15C measurements C183100100029 was achieved by using elastically scattered particles C183100100030 detected by Si detectors at forward angles of 35 deg. C183100100031 HISTORY (20110523C) Compiled by S.H. C183100100032 (20111107A) OS. Author's name corr. C183100100033 ENDBIB 31 0 C183100100034 NOCOMMON 0 0 C183100100035 ENDSUBENT 34 0 C183100199999 SUBENT C1831002 20110523 C108C183100200001 BIB 4 6 C183100200002 REACTION (90-TH-232(6-C-13,F),,SIG) C183100200003 STATUS (TABLE) Data taken from tab. 1 of the reference C183100200004 MONITOR (90-TH-232(6-C-13,F),,SIG) Monitor was used to C183100200005 determine overall efficiency of experimental setup C183100200006 MONIT-REF (D6042003,B.P.Ajith Kumar+,J,PR/C,72,067601,2005) C183100200007 (,B.P.Ajith Kumar+,J,PR/C,73,039901,2006) C183100200008 ENDBIB 6 0 C183100200009 NOCOMMON 0 0 C183100200010 DATA 4 4 C183100200011 EN-CM EN-ERR DATA DATA-ERR C183100200012 MEV MEV MB MB C183100200013 69.7 0.1 549.0 13.0 C183100200014 64.7 0.2 279.0 9.0 C183100200015 60.1 0.2 46.0 4.0 C183100200016 56.5 0.2 5.4 5.0 C183100200017 ENDDATA 6 0 C183100200018 ENDSUBENT 17 0 C183100299999 SUBENT C1831003 20110523 C108C183100300001 BIB 4 4 C183100300002 REACTION (90-TH-232(6-C-14,F),,SIG) C183100300003 STATUS (TABLE) Data taken from tab. 1 of the reference C183100300004 MONITOR (90-TH-232(6-C-13,F),,SIG) C183100300005 MONIT-REF (C1831002,M.Alcorta+,J,PRL,106,172701,2011) C183100300006 ENDBIB 4 0 C183100300007 NOCOMMON 0 0 C183100300008 DATA 4 4 C183100300009 EN-CM EN-ERR DATA DATA-ERR C183100300010 MEV MEV MB MB C183100300011 68.4 0.2 581.0 8.0 C183100300012 63.3 0.2 214.0 6.0 C183100300013 58.5 0.2 21.0 1.0 C183100300014 54.6 0.2 1.0 1.0 C183100300015 ENDDATA 6 0 C183100300016 ENDSUBENT 15 0 C183100399999 SUBENT C1831004 20110523 C108C183100400001 BIB 4 4 C183100400002 REACTION (90-TH-232(6-C-15,F),,SIG) C183100400003 STATUS (TABLE) Data taken from tab. 1 of the reference C183100400004 MONITOR (90-TH-232(6-C-13,F),,SIG) C183100400005 MONIT-REF (C1831002,M.Alcorta+,J,PRL,106,172701,2011) C183100400006 ENDBIB 4 0 C183100400007 NOCOMMON 0 0 C183100400008 DATA 4 5 C183100400009 EN-CM EN-ERR DATA DATA-ERR C183100400010 MEV MEV MB MB C183100400011 69.8 0.2 655.0 21.0 C183100400012 65.4 0.3 369.0 22.0 C183100400013 60.4 0.3 81.0 8.0 C183100400014 56.5 0.3 18.0 4.0 C183100400015 54.4 0.3 6.5 2.2 C183100400016 ENDDATA 7 0 C183100400017 ENDSUBENT 16 0 C183100499999 ENDENTRY 4 0 C183199999999