ENTRY O1599 20080526 O035O159900000001 SUBENT O1599001 20080526 O035O159900100001 BIB 13 68 O159900100002 TITLE Single-neutron transfer from Be-11(g.s) via the (p,d) O159900100003 reaction with a radioactive beam. O159900100004 AUTHOR (J.S.Winfield, S.Fortier, W.N.Catford, S.Pita, N.A.Orr,O159900100005 J.Van de Wiele, Y.Blumenfeld, R.Chapman, O159900100006 S.P.G.Chappell, N.M.Clarke, N.Curtis, M.Freer, S.Gales,O159900100007 H.Langevin-Joliot, H.Lauren, I.Lhenry, J.M.Maison, O159900100008 P.Roussel-Chomaz, M.Shawcross, K.Spohr, T.Suomijarvi, O159900100009 A.de Vismes) O159900100010 INSTITUTE (2FR PAR) O159900100011 (2UK SUR) O159900100012 (2FR CAE) O159900100013 (2UK UK) University of Paisley, Scotland,UK. O159900100014 (2UK OXF) O159900100015 (2UK BIR) O159900100016 (2FR GAN) O159900100017 REFERENCE (J,NP/A,683,48,2001) O159900100018 SAMPLE A polypropylene foil of thickness 50-mum and density O159900100019 0.896-g/cm**3 was used. O159900100020 METHOD (COINC) All the cross sections presented in this paper O159900100021 are those from the analysis of the coincidence O159900100022 spectra. O159900100023 (EDE) O159900100024 (TOF) O159900100025 FACILITY (CYCLO,2FR GAN) GANIL accelerator O159900100026 (PRJFS,2FR GAN) O159900100027 INC-SOURCE The secondary Be-11 beam was produced by fragmentation O159900100028 of a 65 MeV/nucleon 15N beam from the GANIL cyclotron, O159900100029 which bombarded a carbon target of thickness O159900100030 1.03-g/cm**2 located between the two superconducting O159900100031 solenoids of the SISSI device. The Be-11 beam was O159900100032 analyzed by the alpha spectrometer, which was operated O159900100033 as a fragment separator and had a 215-mg/cm**2 aluminumO159900100034 achromatic degrader to reject unwanted ion species. O159900100035 For the H-1(N-15,N-14)H-2 reaction, the N-15 primary O159900100036 beam was degraded in energy by a 745-mg/cm**2 carbon O159900100037 foil in SISSI to 584 MeV O159900100038 DETECTOR (MAGSP) magnetic spectrometer (SPEG) (see Nucl.Instr. O159900100039 Meth. A276 (1989) 509-520)). O159900100040 Unambiguous particle identification was achieved O159900100041 through a combination of the energy-loss signal from O159900100042 an ionisation chamber, the light output from a stoppingO159900100043 plastic scintillator. O159900100044 (IOCH) O159900100045 (SCIN) a thick plastic scintillator. O159900100046 (PS) The angles of the incident beam particles were O159900100047 measured event-by-event using two position sensitive O159900100048 drift chambers. The combined efficiency of the two O159900100049 chambers was approximately 88% for the Be-11 beam and O159900100050 96% for the N-15 beam. O159900100051 A position-sensitive microchannel detector was used as O159900100052 a diagnostic device. O159900100053 (PSSCN) The recoiling deuterons were detected in an O159900100054 array of ten position-sensitive sheet-resistive siliconO159900100055 detectors(CHARISSA). Each detector was 5*5-cm**2 in O159900100056 area and 500-mum thick. O159900100057 ADD-RES (COMP).Vibrational coupling model. O159900100058 CORRECTION Data in coincidence with the CHARISSA detector were O159900100059 corrected for the variation of geometrical deuteron O159900100060 detection efficiency as a function of the heavy ion O159900100061 laboratory angle. O159900100062 ERR-ANALYS (ERR-S).Statistical error O159900100063 (ERR-SYS). For the four most-forward angle points, O159900100064 the systematic errors arising from the uncertainties O159900100065 on the angle determination in SPEG and in the CHARISSAO159900100066 detectors and on the variation efficiency of the O159900100067 detection system as function of the scattering angle O159900100068 are estimated to be of the order of 15%. O159900100069 HISTORY (20080212C) SB O159900100070 ENDBIB 68 0 O159900100071 COMMON 1 3 O159900100072 ERR-SYS O159900100073 PER-CENT O159900100074 15. O159900100075 ENDCOMMON 3 0 O159900100076 ENDSUBENT 75 0 O159900199999 SUBENT O1599002 20080526 O035O159900200001 BIB 5 6 O159900200002 REACTION (1-H-1(7-N-15,D)7-N-14,PAR,DA) fig.6 O159900200003 EN-SEC (E-LVL,7-N-14) O159900200004 LEVEL-PROP (7-N-14,E-LVL=0.000,SPIN=1.0,PARITY=+1.) O159900200005 STATUS (CURVE).By CAJAD. O159900200006 ERR-ANALYS (ERR-DIG).Digitizing error of data. O159900200007 (ANG-ERR-D).Digitizing error of angle. O159900200008 ENDBIB 6 0 O159900200009 COMMON 4 3 O159900200010 EN E-LVL ANG-ERR-D ERR-DIG O159900200011 MEV/A MEV ADEG PER-CENT O159900200012 38.9 0.00 0.23 3. O159900200013 ENDCOMMON 3 0 O159900200014 DATA 3 6 O159900200015 ANG-CM DATA-CM ERR-S O159900200016 ADEG MB/SR PER-CENT O159900200017 4.07 6.2 29. O159900200018 7.9 8.4 10. O159900200019 12.9 10.1 6. O159900200020 18.36 6.1 10. O159900200021 23.63 2.6 15. O159900200022 29.11 2.3 30. O159900200023 ENDDATA 8 0 O159900200024 ENDSUBENT 23 0 O159900299999 SUBENT O1599003 20080526 O035O159900300001 BIB 4 5 O159900300002 REACTION (1-H-1(4-BE-11,D)4-BE-10,PAR,DA) O159900300003 EN-SEC (E-LVL,4-BE-10) O159900300004 LEVEL-PROP (4-BE-10,E-LVL=0.000,SPIN=0.0,PARITY=+1.) O159900300005 (4-BE-10,E-LVL=3.340,SPIN=2.0,PARITY=+1.) O159900300006 STATUS (TABLE) O159900300007 ENDBIB 5 0 O159900300008 COMMON 1 3 O159900300009 EN O159900300010 MEV/A O159900300011 35.3 O159900300012 ENDCOMMON 3 0 O159900300013 DATA 4 15 O159900300014 E-LVL ANG-CM DATA-CM ERR-S O159900300015 MEV ADEG MB/SR MB/SR O159900300016 0. 2.50 5.21 1.39 O159900300017 0. 5.08 5.16 0.73 O159900300018 0. 8.27 4.05 0.53 O159900300019 0. 11.60 1.30 0.27 O159900300020 0. 15.02 0.55 0.25 O159900300021 3.34 2.62 4.85 1.30 O159900300022 3.34 5.39 6.03 0.74 O159900300023 3.34 8.66 4.87 0.55 O159900300024 3.34 12.15 4.74 0.49 O159900300025 3.34 15.74 4.57 0.79 O159900300026 6. 2.73 19.54 2.54 O159900300027 6. 5.62 20.85 1.32 O159900300028 6. 9.00 17.80 0.98 O159900300029 6. 12.63 22.08 1.04 O159900300030 6. 16.39 19.47 1.42 O159900300031 ENDDATA 17 0 O159900300032 ENDSUBENT 31 0 O159900399999 ENDENTRY 3 0 O159999999999