ENTRY F0469 20220608 F093F046900000001 SUBENT F0469001 20220608 F093F046900100001 BIB 9 17 F046900100002 TITLE Neutron angular distributions from the F046900100003 reaction 11B(alpha,n)14N at 13.9 and 13.5 MeV F046900100004 AUTHOR (J.Kjellman) F046900100005 INSTITUTE (2UK HAR) F046900100006 REFERENCE (J,AF,21,543,1962) F046900100007 FACILITY (CYCLO,2UK HAR) F046900100008 SAMPLE 11B target was supplied from the Atomic Energy ResearchF046900100009 Establishment, Harwell, England. The backing material F046900100010 of the target was Au, thick enough to stop 14-MeV F046900100011 a-particles. Nominal thickness was 425 ug/cm2 F046900100012 METHOD (EXTB,TOF,PSD) F046900100013 DETECTOR (SOLST) Neutron detector. For monitoring of the neutronF046900100014 intensity, a stilbene detector with pulse-shape F046900100015 discrimination was used. F046900100016 HISTORY (19920914C) F046900100017 (20220608A) SD: Corrections in all Subents. F046900100018 Subent 003 added. F046900100019 ENDBIB 17 0 F046900100020 NOCOMMON 0 0 F046900100021 ENDSUBENT 20 0 F046900199999 SUBENT F0469002 20220608 F093F046900200001 BIB 4 7 F046900200002 REACTION (5-B-11(A,N)7-N-14,PAR,DA) F046900200003 ERR-ANALYS (ERR-S) Statistical error. The resulting statistical F046900200004 error in the points were 10- 20% for n0 and F046900200005 15-25% for n2. F046900200006 STATUS (CURVE) Figs 3,5 from Arkiv foer Fys.,21(1962)543 F046900200007 HISTORY (20220606A) SD: SF9=EXP deleted from REACTION code. F046900200008 ANG-ERR -> ANG-ERR-D; DATA-ERR -> ERR-S. F046900200009 ENDBIB 7 0 F046900200010 COMMON 1 3 F046900200011 ANG-ERR-D F046900200012 ADEG F046900200013 1.0 F046900200014 ENDCOMMON 3 0 F046900200015 DATA 5 70 F046900200016 E-LVL EN ANG-CM DATA-CM ERR-S F046900200017 MEV MEV ADEG MB/SR MB/SR F046900200018 0. 13.5 6.3 2.041 0.129 F046900200019 0. 13.5 12.2 1.770 0.129 F046900200020 0. 13.5 18.1 1.640 0.129 F046900200021 0. 13.5 26.1 1.240 0.116 F046900200022 0. 13.5 34.7 0.956 0.052 F046900200023 0. 13.5 43.9 0.891 0.077 F046900200024 0. 13.5 51.9 0.852 0.065 F046900200025 0. 13.5 62.6 0.607 0.077 F046900200026 0. 13.5 73.4 0.581 0.065 F046900200027 0. 13.5 84.7 0.813 0.077 F046900200028 0. 13.5 104.6 1.173 0.077 F046900200029 0. 13.5 114.2 1.251 0.077 F046900200030 0. 13.5 123.9 1.354 0.090 F046900200031 0. 13.5 132.5 1.315 0.077 F046900200032 0. 13.5 141.6 1.418 0.103 F046900200033 0. 13.5 150.8 1.701 0.090 F046900200034 0. 13.5 159.4 1.791 0.103 F046900200035 0. 13.9 6.9 1.543 0.128 F046900200036 0. 13.9 12.2 1.388 0.115 F046900200037 0. 13.9 17.6 1.273 0.128 F046900200038 0. 13.9 26.2 1.016 0.077 F046900200039 0. 13.9 34.7 0.862 0.064 F046900200040 0. 13.9 43.3 0.618 0.090 F046900200041 0. 13.9 51.4 0.964 0.236 F046900200042 0. 13.9 62.6 0.374 0.064 F046900200043 0. 13.9 73.9 0.360 0.064 F046900200044 0. 13.9 84.1 0.514 0.064 F046900200045 0. 13.9 104.5 0.654 0.077 F046900200046 0. 13.9 114.8 0.705 0.090 F046900200047 0. 13.9 123.9 0.756 0.090 F046900200048 0. 13.9 132.5 0.756 0.090 F046900200049 0. 13.9 141.6 0.999 0.090 F046900200050 0. 13.9 150.8 1.075 0.064 F046900200051 0. 13.9 159.9 1.293 0.103 F046900200052 0. 13.9 168.0 1.241 0.090 F046900200053 3.95 13.5 5.9 0.671 0.064 F046900200054 3.95 13.5 12.0 0.734 0.058 F046900200055 3.95 13.5 18.1 0.778 0.065 F046900200056 3.95 13.5 26.9 0.783 0.064 F046900200057 3.95 13.5 36.1 0.620 0.019 F046900200058 3.95 13.5 44.7 0.528 0.045 F046900200059 3.95 13.5 53.3 0.326 0.039 F046900200060 3.95 13.5 64.8 0.324 0.032 F046900200061 3.95 13.5 76.2 0.231 0.032 F046900200062 3.95 13.5 86.7 0.262 0.026 F046900200063 3.95 13.5 107.4 0.458 0.007 F046900200064 3.95 13.5 116.6 0.385 0.045 F046900200065 3.95 13.5 126.0 0.403 0.045 F046900200066 3.95 13.5 135.4 0.394 0.058 F046900200067 3.95 13.5 143.6 0.393 0.038 F046900200068 3.95 13.5 152.6 0.494 0.052 F046900200069 3.95 13.5 160.5 0.628 0.026 F046900200070 3.95 13.9 5.8 0.216 0.026 F046900200071 3.95 13.9 11.4 0.300 0.033 F046900200072 3.95 13.9 17.5 0.338 0.039 F046900200073 3.95 13.9 26.5 0.526 0.046 F046900200074 3.95 13.9 36.1 0.661 0.066 F046900200075 3.95 13.9 44.3 0.633 0.059 F046900200076 3.95 13.9 52.9 0.488 0.046 F046900200077 3.95 13.9 64.3 0.395 0.039 F046900200078 3.95 13.9 75.9 0.392 0.059 F046900200079 3.95 13.9 86.2 0.279 0.039 F046900200080 3.95 13.9 106.9 0.511 0.046 F046900200081 3.95 13.9 116.2 0.470 0.052 F046900200082 3.95 13.9 126.7 0.494 0.052 F046900200083 3.95 13.9 135.3 0.401 0.059 F046900200084 3.95 13.9 142.5 0.413 0.059 F046900200085 3.95 13.9 152.0 0.496 0.052 F046900200086 3.95 13.9 160.9 0.599 0.052 F046900200087 3.95 13.9 168.5 0.493 0.052 F046900200088 ENDDATA 72 0 F046900200089 ENDSUBENT 88 0 F046900299999 SUBENT F0469003 20220608 F093F046900300001 BIB 3 3 F046900300002 REACTION (5-B-11(A,N)7-N-14,PAR,SIG) F046900300003 STATUS (TABLE) Text on p.547 of Arkiv foer Fys.,21(1962)543 F046900300004 HISTORY (20220606C) SD F046900300005 ENDBIB 3 0 F046900300006 NOCOMMON 0 0 F046900300007 DATA 4 4 F046900300008 EN E-LVL DATA DATA-MAX F046900300009 MEV MEV MB MB F046900300010 13.5 0. 13. F046900300011 13.5 3.95 0.5 F046900300012 13.9 0. 9. F046900300013 13.9 3.95 0.5 F046900300014 ENDDATA 6 0 F046900300015 ENDSUBENT 14 0 F046900399999 ENDENTRY 3 0 F046999999999