ENTRY C0902 20040210 0000C090200000001 SUBENT C0902001 20040210 0000C090200100001 BIB 13 26 C090200100002 INSTITUTE (1USAORL,1USAOAU,1USAUNC,2UK EDG,1USATEN,1USATTU, C090200100003 1USAYAL,3CPRAEP) C090200100004 REFERENCE (J,PRL,89,262501,200212) C090200100005 (J,NP/A,718,590C,2003) C090200100006 AUTHOR (D.W.Bardayan,J.C.Batchelder,J.C.Blackmon, C090200100007 A.E.Champagne,T.Davinson,R.Fitzgerald,W.R.Hix, C090200100008 C.Iliadis,R.L.Kozub,Z.Ma,S.Parete-Koon,P.D.Parker, C090200100009 N.Shu,M.S.Smith,P.J.Woods) C090200100010 TITLE Strength of the 18F(p,alpha)15O Resonance at E(c.m.) = C090200100011 330 keV C090200100012 FACILITY (ACCEL,1USAORL) Holifield Radioactive Ion Beam C090200100013 Facility. C090200100014 INC-SOURCE 18F beam, 2E+5 18F/sec. 18F to 18O ratio about 0.2. C090200100015 SAMPLE Thin polypropylene target; 57 microg/cm2 thickness. C090200100016 H to C ratio in target 1.8. C090200100017 METHOD (BCINT) C090200100018 (COINC) 15 O and alphas detected in coincidence. C090200100019 DETECTOR Silicon strip detector array (SIDAR). Data measured C090200100020 at laboratory angles from 18-48 degrees. C090200100021 MONITOR (6-C-12(P,EL)6-C-12,,DA) C090200100022 CORRECTION Corrected for events caused by 18O in beam. C090200100023 STATUS Data received by email from Bardayan, 29 January 2003. C090200100024 (COREL,C0868001) C090200100025 (APRVD) Approved by D. Bardayan, 31 January 2003. C090200100026 HISTORY (20030130C) VM C090200100027 (20040210A) Reference added. C090200100028 ENDBIB 26 0 C090200100029 NOCOMMON 0 0 C090200100030 ENDSUBENT 29 0 C090200199999 SUBENT C0902002 20030130 0000C090200200001 BIB 3 7 C090200200002 REACTION (9-F-18(P,A)8-O-15,,SIG) C090200200003 ANALYSIS (INTAD) Integrated by assuming angular distribution C090200200004 calculated for resonance using R-Matrix codes MULTI C090200200005 and SAMMY. C090200200006 ERR-ANALYS (DATA-ERR) Data uncertainties are dominated by C090200200007 statistical uncertaintes, but also include other C090200200008 sources of uncertainty considered. C090200200009 ENDBIB 7 0 C090200200010 NOCOMMON 0 0 C090200200011 DATA 3 2 C090200200012 EN-CM DATA DATA-ERR C090200200013 KEV MB MB C090200200014 325. 0.44 0.13 C090200200015 374. 0.17 0.10 C090200200016 ENDDATA 4 0 C090200200017 ENDSUBENT 16 0 C090200299999 SUBENT C0902003 20030130 0000C090200300001 BIB 2 7 C090200300002 REACTION 1(9-F-18(P,0),,EN) C090200300003 2(9-F-18(P,EL),,WID) C090200300004 3(9-F-18(P,A),,WID/STR) C090200300005 ERR-ANALYS1(DATA-ERR) No information on source of uncertainty. C090200300006 2(DATA-ERR) Uncertainty includes contributions from C090200300007 cross section and target energy loss. C090200300008 3(DATA-ERR) No information on source of uncertainty. C090200300009 ENDBIB 7 0 C090200300010 NOCOMMON 0 0 C090200300011 DATA 6 1 C090200300012 DATA 1DATA-ERR 1DATA 2DATA-ERR 2DATA 3DATA-ERR 3C090200300013 KEV KEV EV EV EV EV C090200300014 332. 17. 2.22 0.69 1.48 0.46 C090200300015 ENDDATA 3 0 C090200300016 ENDSUBENT 15 0 C090200399999 SUBENT C0902004 20030130 0000C090200400001 BIB 2 4 C090200400002 REACTION (8-O-18(P,A)7-N-15,,DA) C090200400003 ERR-ANALYS (DATA-ERR) Data uncertainties are dominated by C090200400004 statistical uncertaintes, but also include other C090200400005 sources of uncertainty considered. C090200400006 ENDBIB 4 0 C090200400007 COMMON 1 3 C090200400008 ANG-CM C090200400009 ADEG C090200400010 125. C090200400011 ENDCOMMON 3 0 C090200400012 DATA 3 2 C090200400013 EN-CM DATA-CM DATA-ERR C090200400014 KEV MU-B/SR MU-B/SR C090200400015 330. 63. 9. C090200400016 378. 199. 30. C090200400017 ENDDATA 4 0 C090200400018 ENDSUBENT 17 0 C090200499999 ENDENTRY 4 0 C090299999999