ENTRY C0906 20220629 C223C0906000 1 SUBENT C0906001 20220629 C223C0906001 1 BIB 8 21 C0906001 2 TITLE Total nuclear reaction probabilities and average C0906001 3 cross sections for 16 and 23 MeV 6Li in silicon C0906001 4 AUTHOR (R.E.Warner,K.M.Berland,W.F.Rulla,D.A.Francis, C0906001 5 J.J.Kolata,Z.Ayer,S.E.Darden,X.J.Kong,G.Liu,A.Morsad, C0906001 6 S.McGimpsey,A.A.Rollefson,A.Galonsky,A.Nadasen, C0906001 7 J.S.Winfield,F.D.Becchetti) C0906001 8 REFERENCE (J,NP/A,516,416,1990) C0906001 9 #doi:10.1016/0375-9474(90)90316-E C0906001 10 INSTITUTE (1USAOBR,1USANOT,1USAMSU,1USAMHG) C0906001 11 FACILITY (ACCEL,1USANOT) The University of Notre Dame FN tandem C0906001 12 accelerator. C0906001 13 INC-SOURCE 20 and 34 MeV primary 6Li beams scattered from 6Li C0906001 14 target. Secondary 6Li particle energies measured C0906001 15 using recoil telescope. C0906001 16 DETECTOR (TELES) Telescope consisting of a transmission C0906001 17 counter and and a stopping counter. C0906001 18 HISTORY (20030415C) VM C0906001 19 (20220629A) BP: Updated entry, added doi and author C0906001 20 F.D.Becchetti, digitized data (unobtainable data) per C0906001 21 an NRDC decision for data sets that were published C0906001 22 before 2000 (C32 of WP2022-01) for subentries 2,4. C0906001 23 ENDBIB 21 0 C0906001 24 NOCOMMON 0 0 C0906001 25 ENDSUBENT 24 0 C090600199999 SUBENT C0906002 20220629 C223C0906002 1 BIB 5 6 C0906002 2 REACTION (14-SI-0(3-LI-6,INL)14-SI-0,PAR,DA) C0906002 3 EN-SEC (E-LVL,3-LI-6) C0906002 4 ERR-ANALYS (ERR-S) Statistical uncertainty in measurements and C0906002 5 fitting the data. C0906002 6 STATUS (CURVE) Fig. 3, page 422 of J,NP/A,516,416,1990. C0906002 7 HISTORY (20220629A) BP: Digitized data. C0906002 8 ENDBIB 6 0 C0906002 9 COMMON 2 3 C0906002 10 EN E-LVL C0906002 11 MEV MEV C0906002 12 24. 2.184 C0906002 13 ENDCOMMON 3 0 C0906002 14 DATA 3 10 C0906002 15 ANG DATA ERR-S C0906002 16 ADEG MB/SR MB/SR C0906002 17 25.984 1.684E+01 C0906002 18 30.938 9.818E+00 C0906002 19 36.072 5.004E+00 C0906002 20 41.014 1.848E+00 C0906002 21 46.179 2.831E+00 C0906002 22 50.936 1.046E+00 C0906002 23 60.474 3.280E-01 1.691E-01 C0906002 24 70.586 2.239E-01 1.587E-01 C0906002 25 79.719 1.885E-02 1.884E-02 C0906002 26 90.070 8.887E-02 8.885E-02 C0906002 27 ENDDATA 12 0 C0906002 28 ENDSUBENT 27 0 C090600299999 SUBENT C0906003 20220629 C223C0906003 1 BIB 5 16 C0906003 2 REACTION (14-SI-0(3-LI-6,INL)14-SI-0,PAR,SIG) C0906003 3 EN-SEC (E-LVL,3-LI-6) C0906003 4 ANALYSIS (INTAD) We estimated the integrated partial cross C0906003 5 section in two ways: (i) a gaussian function was C0906003 6 empirically fitted to the data, and (ii) a C0906003 7 microscopic calculation (described later) was C0906003 8 renormalized for best fit. Both procedures gave the C0906003 9 same result: 24+-2 mb. The uncertainty reflects only C0906003 10 statistical uncertainties in fitting the data; that dueC0906003 11 to modelling assumptions (the functional form of the C0906003 12 angular distribution, and the isotropy of emission of C0906003 13 the decay products) would be harder to determine. C0906003 14 ERR-ANALYS (ERR-S) Statistical uncertainty in measurements and C0906003 15 fitting the data. C0906003 16 STATUS (DEP,C0906002) C0906003 17 (TABLE) page 422 of J,NP/A,516,416,1990. C0906003 18 ENDBIB 16 0 C0906003 19 NOCOMMON 0 0 C0906003 20 DATA 4 1 C0906003 21 EN E-LVL DATA ERR-S C0906003 22 MEV MEV MB MB C0906003 23 24. 2.184 24. 2. C0906003 24 ENDDATA 3 0 C0906003 25 ENDSUBENT 24 0 C090600399999 SUBENT C0906004 20220629 C223C0906004 1 BIB 6 9 C0906004 2 REACTION (14-SI-0(3-LI-6,D+A),,DA/DA/DE,D/A/D) C0906004 3 EN-SEC (E,D) C0906004 4 ANG-SEC (ANG1,D) C0906004 5 (ANG2,A) C0906004 6 ERR-ANALYS (ERR-S) Statistical uncertainty in measurements and C0906004 7 fitting the data. C0906004 8 STATUS (CURVE) Fig. 4, page 424 of J,NP/A,516,416,1990. C0906004 9 HISTORY (20220629A) BP: Digitized data, corrected reaction C0906004 10 string. C0906004 11 ENDBIB 9 0 C0906004 12 COMMON 3 3 C0906004 13 EN ANG1 ANG2 C0906004 14 MEV ADEG ADEG C0906004 15 24. 15.0 40.0 C0906004 16 ENDCOMMON 3 0 C0906004 17 DATA 3 10 C0906004 18 E DATA ERR-S C0906004 19 MEV MB/SR2/MEV MB/SR2/MEV C0906004 20 4.400 0.436 0.141 C0906004 21 4.859 0.227 0.128 C0906004 22 5.346 0.358 0.137 C0906004 23 5.861 0.745 0.199 C0906004 24 6.420 1.110 0.247 C0906004 25 7.023 1.536 0.300 C0906004 26 7.614 1.300 0.278 C0906004 27 8.230 1.828 0.300 C0906004 28 8.814 1.256 0.283 C0906004 29 9.412 0.340 0.146 C0906004 30 ENDDATA 12 0 C0906004 31 ENDSUBENT 30 0 C090600499999 SUBENT C0906005 20220629 C223C0906005 1 BIB 3 4 C0906005 2 REACTION (14-SI-0(3-LI-6,D+A),,SIG,,MSC) Nonspectator 6Li C0906005 3 breakup. C0906005 4 ERR-ANALYS (ERR-S) Statistical uncertainty. C0906005 5 STATUS (TABLE) Table 2, page 426 of J,NP/A,516,416,1990. C0906005 6 ENDBIB 4 0 C0906005 7 NOCOMMON 0 0 C0906005 8 DATA 4 1 C0906005 9 EN-MIN EN-MAX DATA ERR-S C0906005 10 MEV MEV MB MB C0906005 11 15.6 23.0 200. 70. C0906005 12 ENDDATA 3 0 C0906005 13 ENDSUBENT 12 0 C090600599999 SUBENT C0906006 20220629 C223C0906006 1 BIB 4 6 C0906006 2 REACTION (14-SI-0(3-LI-6,NON),,SIG,,AV,DERIV) C0906006 3 ANALYSIS Derived from measured data adding contributions for C0906006 4 missing reaction data. C0906006 5 ERR-ANALYS (DATA-ERR) No information on sources of uncertainty. C0906006 6 STATUS (DEP,C0906005) C0906006 7 (TABLE) Table 2, page 426 of J,NP/A,516,416,1990. C0906006 8 ENDBIB 6 0 C0906006 9 NOCOMMON 0 0 C0906006 10 DATA 4 1 C0906006 11 EN-MIN EN-MAX DATA DATA-ERR C0906006 12 MEV MEV MB MB C0906006 13 15.6 23.0 1197. 320. C0906006 14 ENDDATA 3 0 C0906006 15 ENDSUBENT 14 0 C090600699999 ENDENTRY 6 0 C090699999999