ENTRY D0969 20200113 D125D096900000001 SUBENT D0969001 20200113 D125D096900100001 BIB 12 35 D096900100002 TITLE Experimental cross section and angular distribution D096900100003 of the 2H(p,g)3He reaction at Big-Bang D096900100004 nucleosynthesis energies D096900100005 AUTHOR (I.Tisma, M.Lipoglavsek, M.Mihovilovic, S.Markelj, D096900100006 M.Vencelj, J.Vesic) D096900100007 INSTITUTE (3SLNIJS,2GERMNZ,2GERGSI) D096900100008 (3SLNSLN) University of Ljublijana, Ljublijana D096900100009 REFERENCE (J,EPJ/A,55,137,2019) D096900100010 FACILITY (VDGT,3SLNIJS) 2 MV Tandetron accelerator D096900100011 SAMPLE Deuterons implanted into two Ti sheets, and their D096900100012 depth profiles were studied by 2H(3He,p)4He reactions.D096900100013 - Thick sample irradiated by proton beam at 260 keV D096900100014 for cross section below 163 keV. D096900100015 - Thin sample irradiated by proton beam at 260 to D096900100016 321 keV for cross section above 163 keV. D096900100017 The cross sections from both measurements were D096900100018 normalized at 163 keV. D096900100019 DETECTOR (HPGE) Two HPGe detector at D096900100020 - 135+/-12.3 deg and 57 mm from the target, relative D096900100021 efficiency of 53% at 1.33 MeV. D096900100022 - 90+/-10.2 deg and 122 mm from the target, relative D096900100023 efficiency of 40% at 1.33 MeV. D096900100024 The relative efficiencies were obtained with 152Eu D096900100025 decay gamma and 19F(p,ag)16O 6.1 MeV gamma-ray. D096900100026 METHOD (BCINT) Electrically insulated target chamber acted D096900100027 as a Faraday cup. D096900100028 ANALYSIS Incident energy of proton at reaction was determined D096900100029 was determined from the outgoing gamma energy. D096900100030 ERR-ANALYS Uncertainties in beam current and stopping power are D096900100031 negligible. D096900100032 (ERR-1) detector efficiency (4%) D096900100033 (ERR-2) NRA spectrum fit (~8%) D096900100034 STATUS (APRVD) Proof-read by Isabel Tisma (2020-01-15) D096900100035 HISTORY (20200111C) On D096900100036 (20200113R) On. Data received from Isabel Tisma. D096900100037 ENDBIB 35 0 D096900100038 COMMON 3 3 D096900100039 EN-RSL ERR-1 ERR-2 D096900100040 KEV PER-CENT PER-CENT D096900100041 1. 4. 8. D096900100042 ENDCOMMON 3 0 D096900100043 ENDSUBENT 42 0 D096900199999 SUBENT D0969002 20200113 D125D096900200001 BIB 3 3 D096900200002 REACTION (1-H-2(P,G)2-HE-3,,DA) D096900200003 ERR-ANALYS (ERR-S) Counting statistics D096900200004 STATUS (TABLE) Fig.8 of Eur.Phys.J.A55(2019)137 D096900200005 ENDBIB 3 0 D096900200006 COMMON 2 3 D096900200007 ANG ANG-RSL-HW D096900200008 ADEG ADEG D096900200009 135. 12.3 D096900200010 ENDCOMMON 3 0 D096900200011 DATA 3 14 D096900200012 EN-CM DATA ERR-S D096900200013 KEV NB/SR NB/SR D096900200014 47. 1.33105E+1 2.23579E+0 D096900200015 74. 2.44330E+1 3.92307E+0 D096900200016 97. 3.81165E+1 5.98622E+0 D096900200017 119. 5.17384E+1 8.08581E+0 D096900200018 140. 6.31261E+1 9.54318E+0 D096900200019 163. 7.67178E+1 1.12911E+1 D096900200020 166. 7.73274E+1 2.38557E+0 D096900200021 170. 7.98265E+1 1.46114E+1 D096900200022 175. 7.65077E+1 8.97137E+0 D096900200023 181. 8.02671E+1 7.85061E+0 D096900200024 190. 8.07130E+1 1.27475E+1 D096900200025 196. 8.24358E+1 8.16408E+0 D096900200026 204. 8.69361E+1 9.11246E+0 D096900200027 210. 8.84344E+1 4.35838E+0 D096900200028 ENDDATA 16 0 D096900200029 ENDSUBENT 28 0 D096900299999 SUBENT D0969003 20200113 D125D096900300001 BIB 4 6 D096900300002 REACTION (1-H-2(P,G)2-HE-3,,DA,,RS) D096900300003 CORRECTION Corrected for solid angle attenuation (0.99 at 90 deg, D096900300004 1.00 at 135 deg) D096900300005 ERR-ANALYS (DATA-ERR) Counting statistics and relative efficiency D096900300006 curve D096900300007 STATUS (TABLE) Fig.9 of Eur.Phys.J.A55(2019)137 D096900300008 ENDBIB 6 0 D096900300009 NOCOMMON 0 0 D096900300010 DATA 5 4 D096900300011 EN-CM ANG ANG-RSL-HW DATA DATA-ERR D096900300012 KEV ADEG ADEG NO-DIM NO-DIM D096900300013 170. 90. 10.2 1.4291342 0.06514962 D096900300014 170. 135. 12.3 0.78543291 0.06514962 D096900300015 210. 90. 10.2 1.5232677 0.09991902 D096900300016 210. 135. 12.3 0.73836617 0.09991902 D096900300017 ENDDATA 6 0 D096900300018 ENDSUBENT 17 0 D096900399999 SUBENT D0969004 20200113 D125D096900400001 BIB 3 4 D096900400002 REACTION (1-H-2(P,G)2-HE-3,,DA,,LEG/RS) D096900400003 ERR-ANALYS (DATA-ERR) No information on the source of uncertainty D096900400004 STATUS (TABLE) Text (p.6) of Eur.Phys.J.A55(2019)137 D096900400005 (DEP,D0969004) Angular distribution D096900400006 ENDBIB 4 0 D096900400007 COMMON 1 3 D096900400008 NUMBER D096900400009 NO-DIM D096900400010 1. D096900400011 ENDCOMMON 3 0 D096900400012 DATA 3 2 D096900400013 EN-CM DATA DATA-ERR D096900400014 KEV NO-DIM NO-DIM D096900400015 170. -0.87 0.07 D096900400016 210. -1.06 0.10 D096900400017 ENDDATA 4 0 D096900400018 ENDSUBENT 17 0 D096900499999 SUBENT D0969005 20200113 D125D096900500001 BIB 3 3 D096900500002 REACTION (1-H-2(P,G)2-HE-3,,SIG,,SFC) D096900500003 ERR-ANALYS (ERR-S) Counting statistics D096900500004 STATUS (CURVE) Fig.10 of Eur.Phys.J.A55(2019)137 D096900500005 ENDBIB 3 0 D096900500006 NOCOMMON 0 0 D096900500007 DATA 3 4 D096900500008 EN-CM DATA ERR-S D096900500009 KEV B*EV B*EV D096900500010 97. 0.78111693 0.13045707 D096900500011 119. 1.0104971 0.16803717 D096900500012 170. 1.565835 0.25806931 D096900500013 210. 1.8542257 0.26704461 D096900500014 ENDDATA 6 0 D096900500015 ENDSUBENT 14 0 D096900599999 ENDENTRY 5 0 D096999999999