SUBENT K2199001 20190114 K018K219900100001
BIB 12 42 K219900100002
TITLE Measurement of the 80Se(g,n) cross section using K219900100003
laser-Compton scattering gamma-rays K219900100004
AUTHOR (F.Kitatani, H.Harada, S.Goko, H.Utsunomiya, H.Akimune,K219900100005
T.Kaihori, H.Toyokawa, K.Yamada) K219900100006
INSTITUTE (2JPNJAE) K219900100007
(2JPNKON) K219900100008
(2JPNAIS) K219900100009
REFERENCE (J,NST,47,367,2010) K219900100010
PART-DET (N,G) K219900100011
INC-SOURCE Beam intensity is 80 to 230 mA. K219900100012
(LCS) Wave length of the laser beam is 532nm. K219900100013
SAMPLE - Chemical-form of target is element. K219900100014
- Physical-form of target is solid. K219900100015
METHOD (RINGR) To determine average neutron energies. 20 3He K219900100016
proportional counters coaxially embedded in K219900100017
polyethylene moderator at distance of 3.8, 7.0 K219900100018
and 10.0 cm from beam axis. K219900100019
FACILITY (SRING,2JPNAIS) To store electron beam from 547.6 to K219900100020
677.4 MeV at Tsukuba Electron Ring for K219900100021
Accelerating and Storage (TERAS) K219900100022
DETECTOR (PROPC) To detect neutron K219900100023
(HPGE,BGO) To measure the energy distribution of the K219900100024
LCS gamma-ray.Two 334 cm**3 high-purity Ge K219900100025
detectors shielded with an array of 23 K219900100026
pieces of BGO crystals (HHS) K219900100027
(NAICR) To measure the photon flux K219900100028
ERR-ANALYS (ERR-T) Total uncertainty. Difference between total K219900100029
uncertainties and quadratic sum of 7 partial K219900100030
uncertainties) attribute to total gamma K219900100031
counting K219900100032
(ERR-1) Systematic error of NaI detector K219900100033
(ERR-2) Systematic error of correcting zero point K219900100034
(ERR-3) Errors of the fraction of the gamma flux K219900100035
(ERR-4) Errors of neutron detector efficiency K219900100036
(ERR-5) Systematic error of fitting K219900100037
(ERR-6) Errors of LCS energy distribution K219900100038
(ERR-S) Errors of neutron counts K219900100039
HISTORY (20100602R) Received by e-mail from F.Kitatani K219900100040
(20100603C) Ayano Makinaga K219900100041
(20190114U) Tada. 003:(COREL,K2348004) another K219900100042
measurement (F.Kitatani, 2017-05-09) is K219900100043
added. K219900100044
ENDBIB 42 0 K219900100045
COMMON 2 3 K219900100046
ERR-1 ERR-2 K219900100047
PER-CENT PER-CENT K219900100048
3.0 2.0 K219900100049
ENDCOMMON 3 0 K219900100050
ENDSUBENT 49 0 K219900199999
SUBENT K2199002 20190114 K018K219900200001
BIB 3 7 K219900200002
REACTION (34-SE-80(G,N)34-SE-79,,SIG) K219900200003
SAMPLE Target-thickness: The pellet was 0.795+-0.001 cm in K219900200004
diameter, 2.170+-0.001 cm in thickness, and had a K219900200005
weight of 4.9821+-0.0001 g K219900200006
(34-SE-80,ENR=0.999) K219900200007
STATUS (TABLE) Plotted in Fig.11 of Journal of Nuclear K219900200008
Science and Technology 47(2010)367 K219900200009
ENDBIB 7 0 K219900200010
NOCOMMON 0 0 K219900200011
DATA 9 10 K219900200012
EN EN-ERR DATA ERR-T ERR-S ERR-3 K219900200013
ERR-4 ERR-5 ERR-6 K219900200014
MEV PER-CENT MB PER-CENT PER-CENT PER-CENT K219900200015
PER-CENT PER-CENT PER-CENT K219900200016
10.2 0.6 8.5 10.7 6.9 0.6K219900200017
3.5 5.0 3.3 K219900200018
10.5 1.2 11.6 9.6 5.3 1.0K219900200019
4.5 5.0 1.5 K219900200020
11.2 0.5 18.9 7.0 3.0 0.5K219900200021
3.7 3.0 1.6 K219900200022
11.5 0.5 20.7 6.7 2.8 0.5K219900200023
3.5 3.0 0.9 K219900200024
11.9 0.5 25.2 6.3 2.1 0.5K219900200025
3.3 3.0 0.7 K219900200026
12.3 0.5 29.3 6.5 2.2 0.5K219900200027
3.5 3.0 0.3 K219900200028
12.9 0.6 39.6 6.2 1.8 0.6K219900200029
3.3 3.0 0.4 K219900200030
13.1 0.6 41.3 6.2 1.9 0.5K219900200031
3.3 3.0 0.3 K219900200032
13.6 0.6 56.3 6.4 1.8 0.6K219900200033
3.6 3.0 0.4 K219900200034
14.6 0.8 89.2 6.4 1.5 0.8K219900200035
3.7 3.0 0.1 K219900200036
ENDDATA 24 0 K219900200037
ENDSUBENT 36 0 K219900299999