ENTRY C2747 20241014 C274700000001
SUBENT C2747001 20241014 20250110 C274700100001
BIB 9 29 C274700100002
TITLE First direct measurement of the 13N(alpha,p)16-O C274700100003
reaction relevant for core-collapse supernovae C274700100004
nucleosynthesis C274700100005
AUTHOR (H.Jayatissa,M.L.Avila,K.E.Rehm,R.Talwar,P.Mohr, C274700100006
K.Auranen,J.Chen,D.A.Gorelov,C.R.Hoffman,C.L.Jiang, C274700100007
B.P.Kay,S.A.Kuvin,D.Santiago-Gonzalez) C274700100008
INSTITUTE (1USAANL,3HUNDEB,1CANMNA) C274700100009
REFERENCE (J,PR/C,105,L042802,2022) C274700100010
#doi:10.1103/PhysRevC.105.L042802 C274700100011
FACILITY (LINAC,1USAANL) Experiment was carried out at the C274700100012
Argonne Tandem Linac Accelerator System at Argonne C274700100013
National Laboratory C274700100014
INC-SOURCE (KINDT) A radioactive 13N7+ beam was created with a C274700100015
50 MeV 12C5+ primary beam using the 12C(d,n)13N C274700100016
reaction via the in-flight technique. A magnet is used C274700100017
for separating the 13N beam from the primary 12C beam C274700100018
The beam energy of the secondary 13N was 34.6*-0.7 MeV C274700100019
SAMPLE Active target - the filling of MUSIC chamber was used C274700100020
as the sample. Detector was filled with He-Kr mixture C274700100021
with 95%-5% by volume. The pressure inside detector wasC274700100022
measured to be 402 torr. C274700100023
DETECTOR (IOCH) The cross section was measured using the multi- C274700100024
sampling ionization chamber.The anode is segmented C274700100025
in 18 strips, each with a width of 15.78 mm. The 16 C274700100026
center strips are subdivided in asymmetric left and C274700100027
right sections. Each strip corresponds to a different C274700100028
incident energy. C274700100029
HISTORY (20220518C) Compiled by S.H C274700100030
(20241005A) OS.RAECTION in sub.3 corrected C274700100031
ENDBIB 29 0 C274700100032
NOCOMMON 0 0 C274700100033
ENDSUBENT 32 0 C274700199999
SUBENT C2747002 20220530 20231011 C274700200001
BIB 3 4 C274700200002
REACTION ((2-HE-4(7-N-13,P)8-O-16,,SIG)= C274700200003
(7-N-13(A,P)8-O-16,,SIG)) C274700200004
ERR-ANALYS (DATA-ERR) Total uncertainty C274700200005
STATUS (TABLE) Data shown in fig.5 sent by author H.J. C274700200006
ENDBIB 4 0 C274700200007
NOCOMMON 0 0 C274700200008
DATA 4 9 C274700200009
EN-CM EN-RSL DATA DATA-ERR C274700200010
MEV MEV MB MB C274700200011
6.01518 0.153873 341.821 22.329 C274700200012
5.70378 0.157589 279.672 19.806 C274700200013
5.38467 0.161584 257.804 18.882 C274700200014
5.05727 0.165896 301.539 20.709 C274700200015
4.72085 0.170654 301.539 21.364 C274700200016
4.37433 0.176014 307.293 20.944 C274700200017
4.0165 0.181915 299.237 21.123 C274700200018
3.64652 0.188102 206.013 33.214 C274700200019
3.26394 0.194575 232.484 100.338 C274700200020
ENDDATA 11 0 C274700200021
ENDSUBENT 20 0 C274700299999
SUBENT C2747003 20241014 20250110 C274700300001
BIB 5 7 C274700300002
REACTION (7-N-13(A,P)8-O-16,,SIG,,SFC) C274700300003
ANALYSIS (DTBAL) S-factor calculated from cross sections C274700300004
measured in this work C274700300005
ERR-ANALYS (DATA-ERR) No details on sources of uncertainties C274700300006
STATUS (TABLE) Data shown in fig.4 sent by author H.J. C274700300007
(DEP,C2747002) C274700300008
HISTORY (20241005A) REACTION SF1,2,3,4 corrected C274700300009
ENDBIB 7 0 C274700300010
NOCOMMON 0 0 C274700300011
DATA 4 9 C274700300012
EN-CM EN-RSL DATA DATA-ERR C274700300013
MEV MEV B*MEV B*MEV C274700300014
3.26395 0.19455 548870. 470680. C274700300015
3.6465 0.1881 257530. 83039.2 C274700300016
4.0165 0.1819 223090. 31283.2 C274700300017
4.3743 0.176 149275. 20348.7 C274700300018
4.7208 0.1707 107322. 14436.5 C274700300019
5.05725 0.16585 74531.5 10237.7 C274700300020
5.3846 0.1616 48507. 7105.76 C274700300021
5.70375 0.15755 41360.5 5858.26 C274700300022
6.0152 0.1539 40793.5 5329.55 C274700300023
ENDDATA 11 0 C274700300024
ENDSUBENT 23 0 C274700399999
ENDENTRY 2 0 C274799999999