ENTRY C1645 20160701 C162C1645 0 1 SUBENT C1645001 20160701 C162C1645 1 1 BIB 9 19 C1645 1 2 TITLE Radiative Capture of Protons by C13 C1645 1 3 AUTHOR (J.D.Seagrave) C1645 1 4 REFERENCE (J,PR,85,197,1952) C1645 1 5 #doi:10.1103/PhysRev.85.197 C1645 1 6 REL-REF (O,C1647001,H.H.Woodbury+,J,PR,92,(5),1199,1953) C1645 1 7 INSTITUTE (1USACAL) C1645 1 8 FACILITY (VDG,1USACAL) California Institute of Technology 3- C1645 1 9 MeV electrostatic accelerator. C1645 1 10 DETECTOR (GEMUC) Three Geiger tubes of 30 mg/cm2 glass wall C1645 1 11 and a sensitive region 4 in. in diameter)x3.5 in. long.C1645 1 12 SAMPLE (6-C-13,ENR=0.61) The thick target was simply C1645 1 13 prepared by compressing C13-enriched lampblack into a C1645 1 14 3/8-in. recess milled in a silver blank. Preparation C1645 1 15 of very thin targets of high uniformity was achieved C1645 1 16 by "cracking" a hydrocarbon vapor or gas on a heated C1645 1 17 metal surface, leaving an adherent film of carbon. C1645 1 18 While the "background" is taken with a normal C1645 1 19 (98.9 percent C12) fraction. C1645 1 20 HISTORY (20160701C) BP C1645 1 21 ENDBIB 19 0 C1645 1 22 NOCOMMON 0 0 C1645 1 23 ENDSUBENT 22 0 C1645 199999 SUBENT C1645002 20160701 C162C1645 2 1 BIB 4 9 C1645 2 2 REACTION 1(6-C-13(P,0),,EN) C1645 2 3 2(6-C-13(P,EL),,WID) C1645 2 4 3(6-C-13(P,G),,WID,,G) C1645 2 5 METHOD In order to obtain the true widths, the principal C1645 2 6 resonances were examined with several targets and the C1645 2 7 resonance widths calculated from the yields and C1645 2 8 observed widths. C1645 2 9 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C1645 2 10 STATUS (TABLE) Table I, page 200; Table III, page 202. C1645 2 11 ENDBIB 9 0 C1645 2 12 NOCOMMON 0 0 C1645 2 13 DATA 4 5 C1645 2 14 DATA 1DATA 2DATA-ERR 2DATA 3 C1645 2 15 MEV KEV KEV EV C1645 2 16 0.55 32.5 1.0 8.6 C1645 2 17 1.16 6.0 2.0 1.3 C1645 2 18 1.25 500.0 12.8 C1645 2 19 1.76 2.1 0.2 14.8 C1645 2 20 2.10 45.0 3.0 6.15 C1645 2 21 ENDDATA 7 0 C1645 2 22 ENDSUBENT 21 0 C1645 299999 SUBENT C1645003 20160701 C162C1645 3 1 BIB 2 3 C1645 3 2 REACTION (6-C-13(P,G)7-N-14,,SIG,,RES) C1645 3 3 STATUS (DEP,C1645002) C1645 3 4 (TABLE) Table III, page 202. C1645 3 5 ENDBIB 3 0 C1645 3 6 NOCOMMON 0 0 C1645 3 7 DATA 2 5 C1645 3 8 EN DATA C1645 3 9 MEV MB C1645 3 10 0.55 1.44 C1645 3 11 1.16 0.56 C1645 3 12 1.25 0.062 C1645 3 13 1.76 12.0 C1645 3 14 2.10 1.96 C1645 3 15 ENDDATA 7 0 C1645 3 16 ENDSUBENT 15 0 C1645 399999 SUBENT C1645004 20160701 C162C1645 4 1 BIB 2 4 C1645 4 2 REACTION 1(6-C-12(P,0),,EN) C1645 4 3 2(6-C-12(P,EL),,WID) C1645 4 4 3(6-C-12(P,G),,WID,,G) C1645 4 5 STATUS (TABLE) Table III, page 202. C1645 4 6 ENDBIB 4 0 C1645 4 7 NOCOMMON 0 0 C1645 4 8 DATA 3 2 C1645 4 9 DATA 1DATA 2DATA 3 C1645 4 10 MEV KEV EV C1645 4 11 0.45 35.0 0.67 C1645 4 12 1.70 70.0 1.39 C1645 4 13 ENDDATA 4 0 C1645 4 14 ENDSUBENT 13 0 C1645 499999 SUBENT C1645005 20160701 C162C1645 5 1 BIB 2 3 C1645 5 2 REACTION (6-C-12(P,G)7-N-13,,SIG,,RES) C1645 5 3 STATUS (DEP,C1645004) C1645 5 4 (TABLE) Table III, page 202. C1645 5 5 ENDBIB 3 0 C1645 5 6 NOCOMMON 0 0 C1645 5 7 DATA 2 2 C1645 5 8 EN DATA C1645 5 9 MEV MB C1645 5 10 0.45 0.127 C1645 5 11 1.7 0.035 C1645 5 12 ENDDATA 4 0 C1645 5 13 ENDSUBENT 12 0 C1645 599999 ENDENTRY 5 0 C164599999999