ENTRY C1645 20160701 C162C164500000001
SUBENT C1645001 20160701 C162C164500100001
BIB 9 19 C164500100002
TITLE Radiative Capture of Protons by C13 C164500100003
AUTHOR (J.D.Seagrave) C164500100004
REFERENCE (J,PR,85,197,1952) C164500100005
#doi:10.1103/PhysRev.85.197 C164500100006
REL-REF (O,C1647001,H.H.Woodbury+,J,PR,92,(5),1199,1953) C164500100007
INSTITUTE (1USACAL) C164500100008
FACILITY (VDG,1USACAL) California Institute of Technology 3- C164500100009
MeV electrostatic accelerator. C164500100010
DETECTOR (GEMUC) Three Geiger tubes of 30 mg/cm2 glass wall C164500100011
and a sensitive region 4 in. in diameter)x3.5 in. long.C164500100012
SAMPLE (6-C-13,ENR=0.61) The thick target was simply C164500100013
prepared by compressing C13-enriched lampblack into a C164500100014
3/8-in. recess milled in a silver blank. Preparation C164500100015
of very thin targets of high uniformity was achieved C164500100016
by "cracking" a hydrocarbon vapor or gas on a heated C164500100017
metal surface, leaving an adherent film of carbon. C164500100018
While the "background" is taken with a normal C164500100019
(98.9 percent C12) fraction. C164500100020
HISTORY (20160701C) BP C164500100021
ENDBIB 19 0 C164500100022
NOCOMMON 0 0 C164500100023
ENDSUBENT 22 0 C164500199999
SUBENT C1645002 20160701 C162C164500200001
BIB 4 9 C164500200002
REACTION 1(6-C-13(P,0),,EN) C164500200003
2(6-C-13(P,EL),,WID) C164500200004
3(6-C-13(P,G),,WID,,G) C164500200005
METHOD In order to obtain the true widths, the principal C164500200006
resonances were examined with several targets and the C164500200007
resonance widths calculated from the yields and C164500200008
observed widths. C164500200009
ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C164500200010
STATUS (TABLE) Table I, page 200; Table III, page 202. C164500200011
ENDBIB 9 0 C164500200012
NOCOMMON 0 0 C164500200013
DATA 4 5 C164500200014
DATA 1DATA 2DATA-ERR 2DATA 3 C164500200015
MEV KEV KEV EV C164500200016
0.55 32.5 1.0 8.6 C164500200017
1.16 6.0 2.0 1.3 C164500200018
1.25 500.0 12.8 C164500200019
1.76 2.1 0.2 14.8 C164500200020
2.10 45.0 3.0 6.15 C164500200021
ENDDATA 7 0 C164500200022
ENDSUBENT 21 0 C164500299999
SUBENT C1645003 20160701 C162C164500300001
BIB 2 3 C164500300002
REACTION (6-C-13(P,G)7-N-14,,SIG,,RES) C164500300003
STATUS (DEP,C1645002) C164500300004
(TABLE) Table III, page 202. C164500300005
ENDBIB 3 0 C164500300006
NOCOMMON 0 0 C164500300007
DATA 2 5 C164500300008
EN DATA C164500300009
MEV MB C164500300010
0.55 1.44 C164500300011
1.16 0.56 C164500300012
1.25 0.062 C164500300013
1.76 12.0 C164500300014
2.10 1.96 C164500300015
ENDDATA 7 0 C164500300016
ENDSUBENT 15 0 C164500399999
SUBENT C1645004 20160701 C162C164500400001
BIB 2 4 C164500400002
REACTION 1(6-C-12(P,0),,EN) C164500400003
2(6-C-12(P,EL),,WID) C164500400004
3(6-C-12(P,G),,WID,,G) C164500400005
STATUS (TABLE) Table III, page 202. C164500400006
ENDBIB 4 0 C164500400007
NOCOMMON 0 0 C164500400008
DATA 3 2 C164500400009
DATA 1DATA 2DATA 3 C164500400010
MEV KEV EV C164500400011
0.45 35.0 0.67 C164500400012
1.70 70.0 1.39 C164500400013
ENDDATA 4 0 C164500400014
ENDSUBENT 13 0 C164500499999
SUBENT C1645005 20160701 C162C164500500001
BIB 2 3 C164500500002
REACTION (6-C-12(P,G)7-N-13,,SIG,,RES) C164500500003
STATUS (DEP,C1645004) C164500500004
(TABLE) Table III, page 202. C164500500005
ENDBIB 3 0 C164500500006
NOCOMMON 0 0 C164500500007
DATA 2 2 C164500500008
EN DATA C164500500009
MEV MB C164500500010
0.45 0.127 C164500500011
1.7 0.035 C164500500012
ENDDATA 4 0 C164500500013
ENDSUBENT 12 0 C164500599999
ENDENTRY 5 0 C164599999999