ENTRY C2184 20160509 C158C218400000001 SUBENT C2184001 20160509 C158C218400100001 BIB 14 47 C218400100002 TITLE Measuring the neutron signature of the t->d+n triton C218400100003 breakup reaction, and the angle dependent C218400100004 differential cross section of 6Li(n,t)4He at 2.32 MeV C218400100005 AUTHOR (M.Drosg) C218400100006 INSTITUTE (2AUSVIE) C218400100007 REFERENCE (J,NSE,183,143,2016) C218400100008 REL-REF (O,14440001,M.Drosg,J,NSE,183,143,2016) C218400100009 6Li(n,t)4He angular differential cross section given C218400100010 (I,C0496001,M.Drosg+,R,LA-10444,1985) C218400100011 Details of the experiments at 5.95 and 19.15 MeV C218400100012 EXP-YEAR (1982) C218400100013 FACILITY (VDGT,1USALAS) LANL Ion Beam Facility (IBF) C218400100014 SAMPLE Gas target (0.49 mg/cm2) in a cell (3.0 cm length) C218400100015 with a molybdenum entrance window (5.3 mg/cm2) and a C218400100016 gold beam stop (0.076 cm thick) C218400100017 DETECTOR (SCIN) 2" x 2" liquid scintillator (NE213). C218400100018 METHOD (TOF) C218400100019 CORRECTION Background neutrons were subtracted by measuring C218400100020 1H(t,n)3He neutrons with hydrogen gas at the same C218400100021 pressure. C218400100022 Manfred Drosg (2015-09-30): C218400100023 The monoenergetic 1H(t,n)3He neutron peaks at 0, 15 C218400100024 and 30 deg are beyond 7 MeV, and their subtraction C218400100025 has no effect on the net neutron spectrum below C218400100026 3 MeV. C218400100027 ERR-ANALYS The uncertainties due to dead time correction and C218400100028 detector bias stability are disregarded. C218400100029 Energy dependence of detection efficiency: 1.5%/10 MeV C218400100030 (ERR-1,,,U) Uncertainty due to statistics, random C218400100031 background subtraction, and systematic background C218400100032 subtraction C218400100033 (ERR-2,,,F) 1H(t,n)3He standard cross section (1.5%)C218400100034 (ERR-3,,,F) Hydrogen sample mass (2.4%)C218400100035 (ERR-4,,0.1,F) 1H(t,n)3He normalization C218400100036 - charge collection (<0.1%)C218400100037 (ERR-5,,,F) 1H(t,n)3He counting (0.3%)C218400100038 (ERR-6,,,F) 1H(t,n2)3He background subtraction(1.6%)C218400100039 (ERR-7,,,F) Helium sample mass (1.0%)C218400100040 (ERR-SYS) Total scale uncertainty (3.4%)C218400100041 (ERR-8,,,U) Difference in gass pressure (0.2%)C218400100042 (ERR-9,,0.1,U) Normalization - charge collection(<0.1%)C218400100043 STATUS (APRVD) Corrected and approved by Manfred Drosg C218400100044 (2015-10-02) C218400100045 HISTORY (20150920R) On. Data received from Manfred Drosg. C218400100046 (20150930C) On C218400100047 (20151002A) Corrected by Manfred Drosg C218400100048 (20160509U) On. REFERENCE(NSE): vol,page and year addedC218400100049 ENDBIB 47 0 C218400100050 COMMON 7 6 C218400100051 ERR-2 ERR-3 ERR-5 ERR-6 ERR-7 ERR-SYS C218400100052 ERR-8 C218400100053 PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT C218400100054 PER-CENT C218400100055 1.5 2.4 0.3 1.6 1.0 3.4 C218400100056 0.2 C218400100057 ENDCOMMON 6 0 C218400100058 ENDSUBENT 57 0 C218400199999 SUBENT C2184002 20160509 C158C218400200001 BIB 4 11 C218400200002 REACTION (2-HE-4(T,N)3-LI-6,,DA) C218400200003 COMMENT Manfred Drosg (2015-09-30): C218400200004 No interference with the break-up spectrum at the low C218400200005 energy end. C218400200006 Compiler (2015-09-30): C218400200007 4He(t,n1)6Li threshold energy is 12.229 MeV. C218400200008 (c.f. Table II of the source article) C218400200009 FLAG (1.) The peak energy of 0.41 MeV is below 0.5 MeV C218400200010 which is the lower limit for reliable neutron data C218400200011 at the detector bias of 0.29 MeV C218400200012 STATUS (TABLE) Data received from Manfred Drosg C218400200013 ENDBIB 11 0 C218400200014 COMMON 2 3 C218400200015 EN EN-ERR C218400200016 MEV MEV C218400200017 11.88 0.02 C218400200018 ENDCOMMON 3 0 C218400200019 DATA 5 8 C218400200020 ANG DATA DATA-MIN ERR-1 FLAG C218400200021 ADEG MB/SR MB/SR MB/SR NO-DIM C218400200022 0.0 20.57 0.38 C218400200023 15.0 18.08 0.31 C218400200024 29.9 16.81 0.44 C218400200025 60.0 12.30 0.62 C218400200026 80.0 5.88 0.43 C218400200027 90.0 4.31 0.45 C218400200028 100.0 3.07 0.30 C218400200029 120.0 0.93 0.28 1. C218400200030 ENDDATA 10 0 C218400200031 ENDSUBENT 30 0 C218400299999 SUBENT C2184003 20160509 C158C218400300001 BIB 3 8 C218400300002 REACTION (2-HE-4(T,N+D)2-HE-4,,DA/DE,N) C218400300003 COMMENT Manfred Drosg (2015-09-30): C218400300004 No inteference with the 4He(t,n)4He spectrum at the C218400300005 high energy end. C218400300006 Compiler (2015-09-30): C218400300007 4He(t,2n+p)4He threshold energy is 14.883 MeV. C218400300008 (c.f. Table II of the source article) C218400300009 STATUS (TABLE) Data received from Manfred Drosg C218400300010 ENDBIB 8 0 C218400300011 COMMON 2 3 C218400300012 EN EN-ERR C218400300013 MEV MEV C218400300014 11.88 0.02 C218400300015 ENDCOMMON 3 0 C218400300016 DATA 5 45 C218400300017 ANG ANG-ERR E DATA ERR-1 C218400300018 ADEG ADEG MEV MB/SR/MEV MB/SR/MEV C218400300019 0.0 0.1 0.5750 3.9732 1.1206 C218400300020 0.0 0.1 0.7250 2.8563 0.9935 C218400300021 0.0 0.1 0.8750 3.1943 1.0352 C218400300022 0.0 0.1 1.0250 1.8430 1.0463 C218400300023 0.0 0.1 1.1750 1.3198 1.0433 C218400300024 0.0 0.1 1.3250 3.6098 1.0410 C218400300025 0.0 0.1 1.4750 0.8876 1.0183 C218400300026 0.0 0.1 1.6250 0.8048 0.9711 C218400300027 0.0 0.1 1.7750 1.9421 0.9593 C218400300028 0.0 0.1 1.9250 1.1984 0.9340 C218400300029 0.0 0.1 2.1000 1.4989 0.7733 C218400300030 0.0 0.1 2.3000 0.2713 0.7592 C218400300031 0.0 0.1 2.5000 1.1869 0.7183 C218400300032 0.0 0.1 2.7000 -0.2397 0.6858 C218400300033 0.0 0.1 2.9000 -1.0746 0.6501 C218400300034 15.0 0.1 0.5750 -0.1899 1.2202 C218400300035 15.0 0.1 0.7250 3.1829 1.0730 C218400300036 15.0 0.1 0.8750 2.3756 1.1179 C218400300037 15.0 0.1 1.0250 0.8853 1.1515 C218400300038 15.0 0.1 1.1750 -1.2486 1.1729 C218400300039 15.0 0.1 1.3250 1.0581 1.1150 C218400300040 15.0 0.1 1.4750 -0.6668 1.1242 C218400300041 15.0 0.1 1.6250 0.7058 1.0765 C218400300042 15.0 0.1 1.7750 1.3656 1.0497 C218400300043 15.0 0.1 1.9250 -0.4358 1.0421 C218400300044 15.0 0.1 2.1000 0.5312 0.8531 C218400300045 15.0 0.1 2.3000 -0.5918 0.8311 C218400300046 15.0 0.1 2.5000 1.0257 0.7746 C218400300047 15.0 0.1 2.7000 -0.9763 0.7503 C218400300048 15.0 0.1 2.9000 -0.3770 0.7128 C218400300049 29.9 0.1 0.5750 -0.4042 1.3230 C218400300050 29.9 0.1 0.7250 -1.2867 1.1955 C218400300051 29.9 0.1 0.8750 -0.9807 1.2559 C218400300052 29.9 0.1 1.0250 -0.1820 1.2589 C218400300053 29.9 0.1 1.1750 0.9465 1.2588 C218400300054 29.9 0.1 1.3250 -1.5248 1.2520 C218400300055 29.9 0.1 1.4750 -0.7362 1.2161 C218400300056 29.9 0.1 1.6250 1.9600 1.1737 C218400300057 29.9 0.1 1.7750 0.2473 1.1306 C218400300058 29.9 0.1 1.9250 1.0283 1.1095 C218400300059 29.9 0.1 2.1000 -1.7282 0.9456 C218400300060 29.9 0.1 2.3000 1.2197 0.8729 C218400300061 29.9 0.1 2.5000 -1.3006 0.8670 C218400300062 29.9 0.1 2.7000 -1.9871 0.8318 C218400300063 29.9 0.1 2.9000 -0.7973 0.7690 C218400300064 ENDDATA 47 0 C218400300065 ENDSUBENT 64 0 C218400399999 SUBENT C2184004 20160509 C158C218400400001 BIB 3 4 C218400400002 REACTION (2-HE-4(T,N+D)2-HE-4,,DA,N) C218400400003 ANALYSIS (INTED) C218400400004 STATUS (TABLE) Table VII of Nucl.Sci.Eng.183(2016)143 C218400400005 (DEP,C2184003) Double differential cross sections givenC218400400006 ENDBIB 4 0 C218400400007 COMMON 2 3 C218400400008 EN EN-ERR C218400400009 MEV MEV C218400400010 11.88 0.02 C218400400011 ENDCOMMON 3 0 C218400400012 DATA 4 3 C218400400013 ANG ANG-ERR DATA ERR-1 C218400400014 ADEG ADEG MB/SR MB/SR C218400400015 0.0 0.1 3.84 0.69 C218400400016 15.0 0.1 1.10 0.70 C218400400017 29.9 0.1 -0.14 0.66 C218400400018 ENDDATA 5 0 C218400400019 ENDSUBENT 18 0 C218400499999 ENDENTRY 4 0 C218499999999