ENTRY D6209 20130602 D089D620900000001 SUBENT D6209001 20130602 D089D620900100001 BIB 14 43 D620900100002 TITLE Excitation function studies for the alpha induced D620900100003 reactions in Indium D620900100004 AUTHOR (M.K.Bhardwaj, I.A.Rizvi, A.K.Chaubey) D620900100005 INSTITUTE (3INDMUA) D620900100006 REFERENCE (J,IMP/E,1,389,1992) D620900100007 (R,IC-90-149,1990) similar contents with data in figs D620900100008 (C,92BOMBAY,,238,1992) See CRITIQUE D620900100009 REL-REF (N,,S.F.Mughabghab,B,NEUT.CS 1A,,1981) D620900100010 Error calculation D620900100011 FACILITY (ISOCY,3INDVEC) D620900100012 METHOD (STTA,GSPEC,ACTIV,EDEG) D620900100013 SAMPLE Samples were made from spectrograhically pure indium D620900100014 having purity better than 99.9%. D620900100015 In the preparation of the target sample, the indium D620900100016 metal of thickness 3.34 mg/cm2 was deposited onto the D620900100017 aluminium backing of thickness 6.75 mg/cm2 by vacuum D620900100018 evaporation technique. D620900100019 The indium foil was cut into pieces of size 1.5 cm x D620900100020 1.5 cm and each of them was glued to an aluminium D620900100021 frame having a circular hole of diameter 1.2 cm. D620900100022 These pieces were arranged in a stack. D620900100023 Aluminium and copper foils were also used in between D620900100024 the indium foils to get desired incident energy on D620900100025 each foil. D620900100026 DETECTOR (GELI) 100 cc ORTEC Ge(Li) detector coupled with D620900100027 precalibrated 4096 analyzer. D620900100028 ADD-RES (COMP) A computer code ALICE/LIVERMORE-82 was used D620900100029 for theoretical calculations. D620900100030 COMMENT The incident energy with their corresponding D620900100031 uncertainties are taken from the text of the article. D620900100032 CRITIQUE By Compiler (2013-06-18): D620900100033 The Bombay Conf. Proc. article gives cross sections D620900100034 labelled as 115In(a,n)116gSb, 115In(a,n)116mSb and D620900100035 their sum in a tabulated form. The 115In(a,n)116mSb D620900100036 is, however, inconsistent with 113In(a,n)116mSb D620900100037 cross sections compiled in D6209.002 (this entry) D620900100038 above 30 MeV where the contribution of 115In is D620900100039 dominant. The compiler sent the question to D620900100040 A.K.Chaubey on 18 June 2013, and decided to postpone D620900100041 compilation of the cross sections until the question D620900100042 is resolved. D620900100043 ERR-ANALYS No information on uncertainty D620900100044 HISTORY (20130429C) K.Mondal,U.S.Ghosh,G.Mukherjee D620900100045 ENDBIB 43 0 D620900100046 NOCOMMON 0 0 D620900100047 ENDSUBENT 46 0 D620900199999 SUBENT D6209002 20130602 D089D620900200001 BIB 4 5 D620900200002 REACTION ((49-IN-113(A,N)51-SB-116-M,,SIG)+ D620900200003 (49-IN-115(A,3N)51-SB-116-M,,SIG,,RAB)) D620900200004 SAMPLE (49-IN-113,NAT=0.043) D620900200005 DECAY-DATA (51-SB-116-M,60.4MIN) D620900200006 STATUS (CURVE) Fig.2 of Internat.J.Mod.Phys.E1(1992)389 D620900200007 ENDBIB 5 0 D620900200008 NOCOMMON 0 0 D620900200009 DATA 3 10 D620900200010 EN EN-ERR DATA D620900200011 MEV MEV MB D620900200012 21.4 1.4 2.910E+02 D620900200013 25.2 1.2 1.363E+02 D620900200014 29.0 1.0 6.984E+01 D620900200015 32.2 0.8 3.397E+02 D620900200016 35.1 0.8 6.529E+02 D620900200017 37.4 0.7 7.889E+02 D620900200018 40.1 0.7 5.959E+02 D620900200019 43.6 0.7 4.474E+02 D620900200020 46.8 0.6 3.284E+02 D620900200021 50. 0.5 2.596E+02 D620900200022 ENDDATA 12 0 D620900200023 ENDSUBENT 22 0 D620900299999 SUBENT D6209003 20130602 D089D620900300001 BIB 3 3 D620900300002 REACTION (49-IN-113(A,2N)51-SB-115,,SIG) D620900300003 SAMPLE (49-IN-113,NAT=0.043) D620900300004 STATUS (CURVE) Fig.2 of Internat.J.Mod.Phys.E1(1992)389. D620900300005 ENDBIB 3 0 D620900300006 NOCOMMON 0 0 D620900300007 DATA 3 10 D620900300008 EN EN-ERR DATA D620900300009 MEV MEV MB D620900300010 21.4 1.4 4.005E+02 D620900300011 25.2 1.2 6.700E+02 D620900300012 29.0 1.0 7.843E+02 D620900300013 32.2 0.8 4.438E+02 D620900300014 35.1 0.8 2.634E+02 D620900300015 37.4 0.7 1.224E+02 D620900300016 40.1 0.7 8.300E+01 D620900300017 43.6 0.7 6.288E+01 D620900300018 46.8 0.6 6.083E+01 D620900300019 50. 0.5 5.205E+01 D620900300020 ENDDATA 12 0 D620900300021 ENDSUBENT 20 0 D620900399999 SUBENT D6209004 20130602 D089D620900400001 BIB 4 4 D620900400002 REACTION (49-IN-115(A,N)51-SB-118-M,,SIG) D620900400003 SAMPLE (49-IN-115,NAT=0.957) D620900400004 DECAY-DATA (51-SB-118-M,5.0HR) D620900400005 STATUS (CURVE) Fig.3 of Internat.J.Mod.Phys.E1(1992)389 D620900400006 ENDBIB 4 0 D620900400007 NOCOMMON 0 0 D620900400008 DATA 3 5 D620900400009 EN EN-ERR DATA D620900400010 MEV MEV MB D620900400011 21.4 1.4 2.444E+02 D620900400012 25.2 1.2 1.154E+02 D620900400013 29.0 1.0 4.759E+01 D620900400014 32.2 0.8 2.330E+01 D620900400015 35.1 0.8 1.349E+01 D620900400016 ENDDATA 7 0 D620900400017 ENDSUBENT 16 0 D620900499999 SUBENT D6209005 20130602 D089D620900500001 BIB 5 6 D620900500002 REACTION (49-IN-115(A,2N)51-SB-117,,SIG) D620900500003 SAMPLE (49-IN-115,NAT=0.957) D620900500004 DECAY-DATA (51-SB-117,,DG,158.56) D620900500005 ANALYSIS (DECAY) The contribution of 117Sb was separated out D620900500006 with the help of decay analysis D620900500007 STATUS (CURVE) Fig.3 of Internat.J.Mod.Phys.E1(1992)389 D620900500008 ENDBIB 6 0 D620900500009 NOCOMMON 0 0 D620900500010 DATA 3 10 D620900500011 EN EN-ERR DATA D620900500012 MEV MEV MB D620900500013 21.4 1.4 8.356E+02 D620900500014 25.2 1.2 1.243E+03 D620900500015 29.0 1.0 8.983E+02 D620900500016 32.2 0.8 5.160E+02 D620900500017 35.1 0.8 2.243E+02 D620900500018 37.4 0.7 1.541E+02 D620900500019 40.1 0.7 1.248E+02 D620900500020 43.6 0.7 9.023E+01 D620900500021 46.8 0.6 6.961E+01 D620900500022 50. 0.5 6.224E+01 D620900500023 ENDDATA 12 0 D620900500024 ENDSUBENT 23 0 D620900599999 SUBENT D6209006 20130602 D089D620900600001 BIB 3 3 D620900600002 REACTION (49-IN-115(A,4N)51-SB-115,,SIG) D620900600003 SAMPLE (49-IN-115,NAT=0.957) D620900600004 STATUS (CURVE) Fig.3 of Internat.J.Mod.Phys.E1(1992)389 D620900600005 ENDBIB 3 0 D620900600006 NOCOMMON 0 0 D620900600007 DATA 3 6 D620900600008 EN EN-ERR DATA D620900600009 MEV MEV MB D620900600010 35.1 0.8 9.330E+00 D620900600011 37.4 0.7 1.743E+01 D620900600012 40.1 0.7 5.069E+01 D620900600013 43.6 0.7 1.826E+02 D620900600014 46.8 0.6 3.705E+02 D620900600015 50. 0.5 3.479E+02 D620900600016 ENDDATA 8 0 D620900600017 ENDSUBENT 16 0 D620900699999 SUBENT D6209007 20130602 D089D620900700001 BIB 5 6 D620900700002 REACTION (49-IN-115(A,2P)49-IN-117,,SIG) D620900700003 SAMPLE (49-IN-115,NAT=0.957) D620900700004 DECAY-DATA (49-IN-117,,DG,158.56) D620900700005 ANALYSIS (DECAY) The contribution of 117In was separated out D620900700006 with the help of decay analysis D620900700007 STATUS (CURVE) Fig.4 of Internat.J.Mod.Phys.E1(1992)389 D620900700008 ENDBIB 6 0 D620900700009 NOCOMMON 0 0 D620900700010 DATA 3 7 D620900700011 EN EN-ERR DATA D620900700012 MEV MEV MB D620900700013 32.2 0.8 3.128E+00 D620900700014 35.1 0.8 6.184E+00 D620900700015 37.4 0.7 1.060E+01 D620900700016 40.1 0.7 1.750E+01 D620900700017 43.6 0.7 2.410E+01 D620900700018 46.8 0.6 2.793E+01 D620900700019 50. 0.5 3.040E+01 D620900700020 ENDDATA 9 0 D620900700021 ENDSUBENT 20 0 D620900799999 SUBENT D6209008 20130602 D089D620900800001 BIB 3 3 D620900800002 REACTION (49-IN-115(A,2P)49-IN-117-M,,SIG) D620900800003 SAMPLE (49-IN-115,NAT=0.957) D620900800004 STATUS (CURVE) Fig.4 of Internat.J.Mod.Phys.E1(1992)389 D620900800005 ENDBIB 3 0 D620900800006 NOCOMMON 0 0 D620900800007 DATA 3 7 D620900800008 EN EN-ERR DATA D620900800009 MEV MEV MB D620900800010 32.2 0.8 1.558E+00 D620900800011 35.1 0.8 3.461E+00 D620900800012 37.4 0.7 4.950E+00 D620900800013 40.1 0.7 6.157E+00 D620900800014 43.6 0.7 7.939E+00 D620900800015 46.8 0.6 8.414E+00 D620900800016 50. 0.5 8.675E+00 D620900800017 ENDDATA 9 0 D620900800018 ENDSUBENT 17 0 D620900899999 SUBENT D6209009 20130602 D089D620900900001 BIB 3 3 D620900900002 REACTION (49-IN-115(A,2P)49-IN-117-G,,SIG) D620900900003 SAMPLE (49-IN-115,NAT=0.957) D620900900004 STATUS (CURVE) Fig.4 of Internat.J.Mod.Phys.E1(1992)389 D620900900005 ENDBIB 3 0 D620900900006 NOCOMMON 0 0 D620900900007 DATA 3 7 D620900900008 EN EN-ERR DATA D620900900009 MEV MEV MB D620900900010 32.2 0.8 1.453E+00 D620900900011 35.1 0.8 2.546E+00 D620900900012 37.4 0.7 5.691E+00 D620900900013 40.1 0.7 1.146E+01 D620900900014 43.6 0.7 1.640E+01 D620900900015 46.8 0.6 2.010E+01 D620900900016 50. 0.5 2.219E+01 D620900900017 ENDDATA 9 0 D620900900018 ENDSUBENT 17 0 D620900999999 SUBENT D6209010 20130602 D089D620901000001 BIB 5 6 D620901000002 REACTION (49-IN-115(A,X)50-SN-117-M,,SIG) D620901000003 SAMPLE (49-IN-115,NAT=0.957) D620901000004 DECAY-DATA (50-SN-117-M,,DG,158.56) D620901000005 ANALYSIS (DECAY) The contribution of 117mSn was separated out D620901000006 with the help of decay analysis D620901000007 STATUS (CURVE) Fig.5 of Internat.J.Mod.Phys.E1(1992)389 D620901000008 ENDBIB 6 0 D620901000009 NOCOMMON 0 0 D620901000010 DATA 3 10 D620901000011 EN EN-ERR DATA D620901000012 MEV MEV MB D620901000013 21.4 1.4 1.742E+01 D620901000014 25.2 1.2 4.876E+01 D620901000015 29.0 1.0 1.049E+02 D620901000016 32.2 0.8 1.552E+02 D620901000017 35.1 0.8 1.412E+02 D620901000018 37.4 0.7 1.017E+02 D620901000019 40.1 0.7 8.416E+01 D620901000020 43.6 0.7 6.975E+01 D620901000021 46.8 0.6 6.377E+01 D620901000022 50. 0.5 6.014E+01 D620901000023 ENDDATA 12 0 D620901000024 ENDSUBENT 23 0 D620901099999 ENDENTRY 10 0 D620999999999