ENTRY C1855 20110924 C111C185500000001 SUBENT C1855001 20110924 C111C185500100001 BIB 9 21 C185500100002 TITLE Single-neutron energies outside 136Xe C185500100003 AUTHOR (B.P.Kay,J.P.Schiffer,S.J.Freeman,C.R.Hoffman,B.B.Back,C185500100004 S.I.Baker,S.Bedoor,T.Bloxham,J.A.Clark,C.M.Deibel, C185500100005 A.M.Howard,J.C.Lighthall,S.T.Marley,K.E.Rehm,D.K.Sharp,C185500100006 D.V.Shetty, J.S.Thomas,A.H.Wuosmaa) C185500100007 INSTITUTE (1USAANL,1USALAS,2UK MAN,1USAWMU,1USABRK,1USAMSU) C185500100008 REFERENCE (J,PR/C,84,024325,2011) C185500100009 FACILITY (LINAC,1USAANL) The measurement was performed at the C185500100010 ATLAS facility at Argonne National Laboratory. C185500100011 SAMPLE Deuterated polyethylene [(C2D4)n] targets. Several C185500100012 targets were used with thicknesses ranging between C185500100013 125 and 175 mu-g/cm2. C185500100014 DETECTOR (MAGSP) Outgoing protons, emitted at forward center- C185500100015 of-mass (c.m.) angles (theta-lab > 90.) were analyzed C185500100016 in HELIOS, at a field strength of 2 T. C185500100017 (PS,SI) Energy, distance from the target, and time of C185500100018 flight of outgoing protons were recorded by an array C185500100019 of position-sensitive Si detectors surrounding the C185500100020 magnetic axis, which corresponds to the beam axis. C185500100021 METHOD (TOF) C185500100022 HISTORY (20110924C) Compiled by S.H. C185500100023 ENDBIB 21 0 C185500100024 COMMON 1 3 C185500100025 EN C185500100026 MEV/A C185500100027 10.0 C185500100028 ENDCOMMON 3 0 C185500100029 ENDSUBENT 28 0 C185500199999 SUBENT C1855002 20110924 C111C185500200001 BIB 4 14 C185500200002 REACTION (1-H-2(54-XE-136,P)54-XE-137,PAR,DA) C185500200003 STATUS (TABLE) Data taken from tab.1 of the reference C185500200004 ERR-ANALYS (ERR-1) Systematic uncertainty in monitor detector C185500200005 solid angle C185500200006 (ERR-2) Systematic uncertainty in beam intensity) C185500200007 (ERR-3) Systematic uncertainty due to performance of C185500200008 individual position sensitive counters C185500200009 (ERR-4) Systematic uncertainty of Rutherford C185500200010 scattering C185500200011 (ERR-5) Systematic uncertainty due to background C185500200012 subtraction C185500200013 (ERR-T) Total uncertainty C185500200014 FLAG (1.0) Possibility of doublets at these energies C185500200015 cannot be ruled out C185500200016 ENDBIB 14 0 C185500200017 COMMON 6 3 C185500200018 ERR-1 ERR-2 ERR-3 ERR-4 ERR-5 ERR-T C185500200019 PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT C185500200020 11.0 5.0 7.0 3.0 5.0 15.0 C185500200021 ENDCOMMON 3 0 C185500200022 DATA 4 20 C185500200023 E-LVL ANG DATA FLAG C185500200024 KEV ADEG MB/SR NO-DIM C185500200025 0.0 15.0 18.8 C185500200026 601.0 12.0 0.6 C185500200027 986.0 17.0 2.2 C185500200028 1218.0 33.0 1.1 C185500200029 1303.0 15.0 4.4 C185500200030 1534.0 20.0 2.2 C185500200031 1590.0 33.0 0.7 C185500200032 1751.0 38.0 1.8 C185500200033 1841.0 25.0 3.9 C185500200034 1930.0 18.0 2.8 C185500200035 2025.0 20.0 2.1 C185500200036 2120.0 19.0 0.9 C185500200037 2510.0 23.0 2.0 C185500200038 2650.0 22.0 2.1 C185500200039 2905.0 16.0 0.8 1.0 C185500200040 2995.0 21.0 1.4 1.0 C185500200041 3150.0 35.0 0.3 1.0 C185500200042 3310.0 35.0 0.3 1.0 C185500200043 3470.0 34.0 0.5 1.0 C185500200044 3610.0 34.0 0.4 1.0 C185500200045 ENDDATA 22 0 C185500200046 ENDSUBENT 45 0 C185500299999 SUBENT C1855003 20110924 C111C185500300001 BIB 3 5 C185500300002 REACTION ((1-H-2(54-XE-136,P)54-XE-137,PAR,DA)= C185500300003 (54-XE-136(D,P)54-XE-137,PAR,DA)) C185500300004 STATUS (CURVE) Data presented in fig.3 of the reference C185500300005 sent by author (B.P.K.) C185500300006 ERR-ANALYS (ERR-S) Statistical uncertainty C185500300007 ENDBIB 5 0 C185500300008 NOCOMMON 0 0 C185500300009 DATA 4 101 C185500300010 E-LVL ANG-CM DATA-CM ERR-S C185500300011 KEV ADEG MB/SR MB/SR C185500300012 0.0 6.1 15.17 0.83 C185500300013 0.0 15.2 18.86 0.28 C185500300014 0.0 20.5 16.94 0.25 C185500300015 0.0 24.7 14.33 0.24 C185500300016 0.0 26.4 12.30 0.24 C185500300017 0.0 28.3 12.76 0.25 C185500300018 0.0 29.8 10.29 0.26 C185500300019 0.0 31.5 9.62 0.38 C185500300020 0.0 32.9 8.35 0.23 C185500300021 0.0 35.8 6.89 0.22 C185500300022 0.0 38.4 8.39 0.35 C185500300023 0.0 40.9 6.14 0.38 C185500300024 601.0 11.8 10.57 0.21 C185500300025 601.0 18.2 6.95 0.16 C185500300026 601.0 22.9 7.08 0.17 C185500300027 601.0 24.7 6.81 0.18 C185500300028 601.0 26.8 7.31 0.19 C185500300029 601.0 30.1 6.75 0.34 C185500300030 601.0 31.6 5.18 0.18 C185500300031 601.0 34.6 4.26 0.18 C185500300032 601.0 37.4 4.66 0.27 C185500300033 601.0 39.9 3.05 0.29 C185500300034 986.0 16.5 2.16 0.09 C185500300035 986.0 21.6 2.25 0.10 C185500300036 986.0 23.5 2.29 0.10 C185500300037 986.0 25.7 2.34 0.12 C185500300038 986.0 27.4 2.39 0.13 C185500300039 986.0 29.2 1.87 0.27 C185500300040 986.0 30.8 1.79 0.10 C185500300041 986.0 33.8 1.66 0.11 C185500300042 986.0 36.7 1.58 0.16 C185500300043 986.0 39.3 1.52 0.34 C185500300044 1218.0 15.4 0.57 0.08 C185500300045 1218.0 20.7 0.94 0.17 C185500300046 1218.0 22.8 0.91 0.22 C185500300047 1218.0 25.0 1.38 0.11 C185500300048 1218.0 26.7 1.09 0.23 C185500300049 1218.0 30.2 1.09 0.14 C185500300050 1218.0 33.3 1.14 0.15 C185500300051 1218.0 36.2 1.07 0.17 C185500300052 1218.0 38.9 0.74 0.18 C185500300053 1303.0 14.9 4.38 0.14 C185500300054 1303.0 20.4 4.10 0.18 C185500300055 1303.0 22.5 3.91 0.25 C185500300056 1303.0 24.7 3.35 0.15 C185500300057 1303.0 26.5 3.21 0.26 C185500300058 1303.0 30.0 2.81 0.14 C185500300059 1303.0 33.2 2.03 0.15 C185500300060 1303.0 36.1 2.32 0.25 C185500300061 1303.0 38.7 1.70 0.22 C185500300062 1534.0 13.6 2.40 0.09 C185500300063 1534.0 19.5 2.26 0.11 C185500300064 1534.0 21.7 1.87 0.19 C185500300065 1534.0 24.0 2.11 0.15 C185500300066 1534.0 25.8 1.70 0.15 C185500300067 1534.0 29.4 1.25 0.12 C185500300068 1534.0 32.7 1.24 0.12 C185500300069 1590.0 13.3 0.35 0.12 C185500300070 1590.0 19.3 0.59 0.11 C185500300071 1590.0 21.5 0.63 0.07 C185500300072 1590.0 23.8 0.69 0.13 C185500300073 1590.0 27.6 0.64 0.14 C185500300074 1590.0 29.3 0.57 0.11 C185500300075 1590.0 32.5 0.73 0.13 C185500300076 1590.0 35.5 0.50 0.13 C185500300077 1751.0 18.6 1.40 0.12 C185500300078 1751.0 20.9 1.90 0.24 C185500300079 1751.0 23.3 1.22 0.22 C185500300080 1751.0 25.2 1.79 0.17 C185500300081 1751.0 28.9 1.72 0.25 C185500300082 1751.0 32.2 2.12 0.34 C185500300083 1751.0 35.2 2.22 0.36 C185500300084 1751.0 37.9 2.15 0.52 C185500300085 1841.0 18.2 3.24 0.24 C185500300086 1841.0 20.5 3.92 0.23 C185500300087 1841.0 23.0 3.25 0.93 C185500300088 1841.0 24.9 4.35 0.23 C185500300089 1841.0 28.6 3.59 0.34 C185500300090 1841.0 32.0 3.13 0.29 C185500300091 1841.0 35.0 2.86 0.39 C185500300092 1841.0 37.8 2.17 0.63 C185500300093 1930.0 17.8 2.75 0.13 C185500300094 1930.0 20.2 1.78 0.22 C185500300095 1930.0 22.7 2.08 0.13 C185500300096 1930.0 24.6 2.08 0.19 C185500300097 1930.0 28.4 1.33 0.08 C185500300098 1930.0 31.8 1.41 0.27 C185500300099 2510.0 17.6 2.21 0.10 C185500300100 2510.0 20.5 2.24 0.12 C185500300101 2510.0 22.6 2.31 0.10 C185500300102 2510.0 24.9 2.34 0.28 C185500300103 2510.0 26.8 2.02 0.11 C185500300104 2510.0 30.3 1.86 0.08 C185500300105 2510.0 36.5 1.78 0.04 C185500300106 2650.0 14.0 2.44 0.45 C185500300107 2650.0 17.0 2.33 0.10 C185500300108 2650.0 22.1 2.31 0.10 C185500300109 2650.0 24.4 2.89 0.28 C185500300110 2650.0 26.3 2.02 0.11 C185500300111 2650.0 30.0 1.86 0.08 C185500300112 2650.0 36.2 1.78 0.04 C185500300113 ENDDATA 103 0 C185500300114 ENDSUBENT 113 0 C185500399999 ENDENTRY 3 0 C185599999999