ENTRY S0233 20211203 S030S023300000001 SUBENT S0233001 20211203 S030S023300100001 BIB 12 38 S023300100002 TITLE Differential cross-section for the T(12C,T)12C S023300100003 elastic recoil reaction S023300100004 AUTHOR (Yiming Duan,Wei Ding,Weidu Wang,Wei Zhang,Liqun Shi) S023300100005 INSTITUTE (3CPRFUD,3CPRNPC) S023300100006 REFERENCE (J,NIM/B,483,1,2020) S023300100007 #doi:10.1016/j.nimb.2020.10.001 S023300100008 FACILITY (VDGT,3CPRFUD) NEC 9SDH-2 2x3 MV tandem accelerator S023300100009 INC-SOURCE The incident beam current was limited to less than 30 S023300100010 nA as monitored by a Faraday cup. During the S023300100011 experiment, the chamber was kept at a high vacuum of S023300100012 less than 3.0E-5 Pa. S023300100013 SAMPLE A thin solid target Ni/TiTx/Al2O3 was prepared by the S023300100014 conventional hydrogenation method, the atomic ratios S023300100015 of Ti, T and H is 10:8:1, and the atomic thickness of S023300100016 the TiTx layer is about 3.5E17 atoms/cm2. S023300100017 DETECTOR (SIBAR) An Au/Si surface barrier detector was S023300100018 employed to detect the backscattered ions at a S023300100019 laboratory angle of 165 deg, with a solid angle of S023300100020 0.00183 sr. At a laboratory angle of 30 deg, another S023300100021 Au/Si surface barrier detector with a solid angle of S023300100022 0.00246 sr was placed to detect the elastic recoil S023300100023 spectrum. The angular resolution of both detectors S023300100024 were approximately +-0.5 deg and the energy S023300100025 resolution of the detection system was about 30 keV S023300100026 for 12C ions. S023300100027 METHOD The relative determination method. S023300100028 ERR-ANALYS (ERR-T) The total error, 5.8% S023300100029 (ERR-1,2.,3.) The error of peak areas resulting from S023300100030 the statistics and background, 2-3% S023300100031 (ERR-2)The error of Rutherford scattering cross S023300100032 section for Ni-C(E0), 0.44% S023300100033 (ERR-3)The error of Rutherford scattering cross S023300100034 section for T-O(ER), 2.6% S023300100035 (ERR-4)The error of Rutherford scattering cross S023300100036 section for Ni-O(ER0), 0.53% S023300100037 STATUS (TABLE) Table 2 of Nuclear Inst. and Methods in S023300100038 Physics Research,B,483,1,2020. S023300100039 HISTORY (20211203C) Jimin Wang (CNDC) S023300100040 ENDBIB 38 0 S023300100041 COMMON 4 3 S023300100042 ERR-T ERR-2 ERR-3 ERR-4 S023300100043 PER-CENT PER-CENT PER-CENT PER-CENT S023300100044 5.8 0.44 2.6 0.53 S023300100045 ENDCOMMON 3 0 S023300100046 ENDSUBENT 45 0 S023300199999 SUBENT S0233002 20211203 S030S023300200001 BIB 1 1 S023300200002 REACTION (6-C-12(T,EL)6-C-12,,DA) S023300200003 ENDBIB 1 0 S023300200004 COMMON 1 3 S023300200005 ANG S023300200006 ADEG S023300200007 30. S023300200008 ENDCOMMON 3 0 S023300200009 DATA 2 31 S023300200010 EN DATA S023300200011 KEV MB/SR S023300200012 5227. 191. S023300200013 5477. 170. S023300200014 5727. 143. S023300200015 5977. 126. S023300200016 6177. 105. S023300200017 6377. 95. S023300200018 6577. 77. S023300200019 6777. 65. S023300200020 6978. 55. S023300200021 7178. 47. S023300200022 7378. 32. S023300200023 7578. 32. S023300200024 7778. 32. S023300200025 7979. 27. S023300200026 8179. 30. S023300200027 8379. 28. S023300200028 8579. 29. S023300200029 8779. 29. S023300200030 8879. 27. S023300200031 8980. 30. S023300200032 9180. 36. S023300200033 9480. 46. S023300200034 9780. 48. S023300200035 10081. 48. S023300200036 10381. 48. S023300200037 10681. 47. S023300200038 10982. 43. S023300200039 11282. 41. S023300200040 11582. 34. S023300200041 11882. 32. S023300200042 12183. 28. S023300200043 ENDDATA 33 0 S023300200044 ENDSUBENT 43 0 S023300299999 ENDENTRY 2 0 S023399999999