ENTRY C0906 20220629 C090600000001 SUBENT C0906001 20220629 20231011 C090600100001 BIB 8 21 C090600100002 TITLE Total nuclear reaction probabilities and average C090600100003 cross sections for 16 and 23 MeV 6Li in silicon C090600100004 AUTHOR (R.E.Warner,K.M.Berland,W.F.Rulla,D.A.Francis, C090600100005 J.J.Kolata,Z.Ayer,S.E.Darden,X.J.Kong,G.Liu,A.Morsad, C090600100006 S.McGimpsey,A.A.Rollefson,A.Galonsky,A.Nadasen, C090600100007 J.S.Winfield,F.D.Becchetti) C090600100008 REFERENCE (J,NP/A,516,416,1990) C090600100009 #doi:10.1016/0375-9474(90)90316-E C090600100010 INSTITUTE (1USAOBR,1USANOT,1USAMSU,1USAMHG) C090600100011 FACILITY (ACCEL,1USANOT) The University of Notre Dame FN tandem C090600100012 accelerator. C090600100013 INC-SOURCE 20 and 34 MeV primary 6Li beams scattered from 6Li C090600100014 target. Secondary 6Li particle energies measured C090600100015 using recoil telescope. C090600100016 DETECTOR (TELES) Telescope consisting of a transmission C090600100017 counter and and a stopping counter. C090600100018 HISTORY (20030415C) VM C090600100019 (20220629A) BP: Updated entry, added doi and author C090600100020 F.D.Becchetti, digitized data (unobtainable data) per C090600100021 an NRDC decision for data sets that were published C090600100022 before 2000 (C32 of WP2022-01) for subentries 2,4. C090600100023 ENDBIB 21 0 C090600100024 NOCOMMON 0 0 C090600100025 ENDSUBENT 24 0 C090600199999 SUBENT C0906002 20220629 20231011 C090600200001 BIB 5 6 C090600200002 REACTION (14-SI-0(3-LI-6,INL)14-SI-0,PAR,DA) C090600200003 EN-SEC (E-LVL,3-LI-6) C090600200004 ERR-ANALYS (ERR-S) Statistical uncertainty in measurements and C090600200005 fitting the data. C090600200006 STATUS (CURVE) Fig. 3, page 422 of J,NP/A,516,416,1990. C090600200007 HISTORY (20220629A) BP: Digitized data. C090600200008 ENDBIB 6 0 C090600200009 COMMON 2 3 C090600200010 EN E-LVL C090600200011 MEV MEV C090600200012 24. 2.184 C090600200013 ENDCOMMON 3 0 C090600200014 DATA 3 10 C090600200015 ANG DATA ERR-S C090600200016 ADEG MB/SR MB/SR C090600200017 25.984 1.684E+01 C090600200018 30.938 9.818E+00 C090600200019 36.072 5.004E+00 C090600200020 41.014 1.848E+00 C090600200021 46.179 2.831E+00 C090600200022 50.936 1.046E+00 C090600200023 60.474 3.280E-01 1.691E-01 C090600200024 70.586 2.239E-01 1.587E-01 C090600200025 79.719 1.885E-02 1.884E-02 C090600200026 90.070 8.887E-02 8.885E-02 C090600200027 ENDDATA 12 0 C090600200028 ENDSUBENT 27 0 C090600299999 SUBENT C0906003 20220629 20231011 C090600300001 BIB 5 16 C090600300002 REACTION (14-SI-0(3-LI-6,INL)14-SI-0,PAR,SIG) C090600300003 EN-SEC (E-LVL,3-LI-6) C090600300004 ANALYSIS (INTAD) We estimated the integrated partial cross C090600300005 section in two ways: (i) a gaussian function was C090600300006 empirically fitted to the data, and (ii) a C090600300007 microscopic calculation (described later) was C090600300008 renormalized for best fit. Both procedures gave the C090600300009 same result: 24+-2 mb. The uncertainty reflects only C090600300010 statistical uncertainties in fitting the data; that dueC090600300011 to modelling assumptions (the functional form of the C090600300012 angular distribution, and the isotropy of emission of C090600300013 the decay products) would be harder to determine. C090600300014 ERR-ANALYS (ERR-S) Statistical uncertainty in measurements and C090600300015 fitting the data. C090600300016 STATUS (DEP,C0906002) C090600300017 (TABLE) page 422 of J,NP/A,516,416,1990. C090600300018 ENDBIB 16 0 C090600300019 NOCOMMON 0 0 C090600300020 DATA 4 1 C090600300021 EN E-LVL DATA ERR-S C090600300022 MEV MEV MB MB C090600300023 24. 2.184 24. 2. C090600300024 ENDDATA 3 0 C090600300025 ENDSUBENT 24 0 C090600399999 SUBENT C0906004 20220629 20231011 C090600400001 BIB 6 9 C090600400002 REACTION (14-SI-0(3-LI-6,D+A),,DA/DA/DE,D/A/D) C090600400003 EN-SEC (E,D) C090600400004 ANG-SEC (ANG1,D) C090600400005 (ANG2,A) C090600400006 ERR-ANALYS (ERR-S) Statistical uncertainty in measurements and C090600400007 fitting the data. C090600400008 STATUS (CURVE) Fig. 4, page 424 of J,NP/A,516,416,1990. C090600400009 HISTORY (20220629A) BP: Digitized data, corrected reaction C090600400010 string. C090600400011 ENDBIB 9 0 C090600400012 COMMON 3 3 C090600400013 EN ANG1 ANG2 C090600400014 MEV ADEG ADEG C090600400015 24. 15.0 40.0 C090600400016 ENDCOMMON 3 0 C090600400017 DATA 3 10 C090600400018 E DATA ERR-S C090600400019 MEV MB/SR2/MEV MB/SR2/MEV C090600400020 4.400 0.436 0.141 C090600400021 4.859 0.227 0.128 C090600400022 5.346 0.358 0.137 C090600400023 5.861 0.745 0.199 C090600400024 6.420 1.110 0.247 C090600400025 7.023 1.536 0.300 C090600400026 7.614 1.300 0.278 C090600400027 8.230 1.828 0.300 C090600400028 8.814 1.256 0.283 C090600400029 9.412 0.340 0.146 C090600400030 ENDDATA 12 0 C090600400031 ENDSUBENT 30 0 C090600499999 SUBENT C0906005 20220629 20231011 C090600500001 BIB 3 4 C090600500002 REACTION (14-SI-0(3-LI-6,D+A),,SIG,,MSC) Nonspectator 6Li C090600500003 breakup. C090600500004 ERR-ANALYS (ERR-S) Statistical uncertainty. C090600500005 STATUS (TABLE) Table 2, page 426 of J,NP/A,516,416,1990. C090600500006 ENDBIB 4 0 C090600500007 NOCOMMON 0 0 C090600500008 DATA 4 1 C090600500009 EN-MIN EN-MAX DATA ERR-S C090600500010 MEV MEV MB MB C090600500011 15.6 23.0 200. 70. C090600500012 ENDDATA 3 0 C090600500013 ENDSUBENT 12 0 C090600599999 SUBENT C0906006 20220629 20231011 C090600600001 BIB 4 6 C090600600002 REACTION (14-SI-0(3-LI-6,NON),,SIG,,AV,DERIV) C090600600003 ANALYSIS Derived from measured data adding contributions for C090600600004 missing reaction data. C090600600005 ERR-ANALYS (DATA-ERR) No information on sources of uncertainty. C090600600006 STATUS (DEP,C0906005) C090600600007 (TABLE) Table 2, page 426 of J,NP/A,516,416,1990. C090600600008 ENDBIB 6 0 C090600600009 NOCOMMON 0 0 C090600600010 DATA 4 1 C090600600011 EN-MIN EN-MAX DATA DATA-ERR C090600600012 MEV MEV MB MB C090600600013 15.6 23.0 1197. 320. C090600600014 ENDDATA 3 0 C090600600015 ENDSUBENT 14 0 C090600699999 ENDENTRY 6 0 C090699999999