ENTRY C1990 20130403 C131C199000000001 SUBENT C1990001 20130403 C131C199000100001 BIB 8 19 C199000100002 TITLE Valence neutron properties relevant to the C199000100003 neutrinoless double-beta decay of 130Te C199000100004 AUTHOR (B.P.Kay,T.Bloxham,S.A.McAllister,J.A.Clark,C.M.Deibel,C199000100005 S.J.Freedman,S.J.Freeman,K.Han,A.M.Howard,A.J.Mitchell,C199000100006 P.D.Parker,J.P.Schiffer,D.K.Sharp,J.S.Thomas) C199000100007 INSTITUTE (1USABRK,2UK MAN,1USAANL,1USAMSU,1USAYAL) C199000100008 (2UK UK) University of York, Heslington, York C199000100009 REFERENCE (J,PR/C,87,011302,2013) C199000100010 Submitted on March 14, 2013 by B. P. Kay C199000100011 FACILITY (VDGT,1USAYAL) The measurements were carried out at C199000100012 the A. W. Wright Nuclear Structure Laboratory at Yale C199000100013 University C199000100014 DETECTOR (MAGSP) Outgoing ions were analyzed by a split-pole C199000100015 magnetic spectrograph C199000100016 ERR-ANALYS (ERR-SYS) Overall systematic uncertainty C199000100017 (ERR-1) Systematic uncertainty for very weak C199000100018 transitions at higher excitation energy from possible C199000100019 contaminants or previously unidentified states C199000100020 HISTORY (20130403C) Compiled by S.H. C199000100021 ENDBIB 19 0 C199000100022 COMMON 2 3 C199000100023 ERR-SYS ERR-1 C199000100024 PER-CENT MB/SR C199000100025 7.0 0.03 C199000100026 ENDCOMMON 3 0 C199000100027 ENDSUBENT 26 0 C199000199999 SUBENT C1990002 20130403 C131C199000200001 BIB 4 7 C199000200002 REACTION (52-TE-128(P,D)52-TE-127,PAR,DA) C199000200003 SAMPLE (52-TE-128,ENR=0.992) Self-supporting target of C199000200004 thicknesses 436 mu-g/cm2 C199000200005 STATUS (TABLE) Data taken from tab. 2 of submission to XUNDL C199000200006 by B.P. Kay (March 14, 2013) C199000200007 ERR-ANALYS (ERR-S,1.0,3.0) Statistical uncertainty are less than C199000200008 1% for strong states and less than 3% for weak states C199000200009 ENDBIB 7 0 C199000200010 COMMON 2 3 C199000200011 EN EN-RSL C199000200012 MEV KEV C199000200013 23.0 30.0 C199000200014 ENDCOMMON 3 0 C199000200015 DATA 3 74 C199000200016 E-LVL ANG DATA C199000200017 KEV ADEG MB/SR C199000200018 0.0 5.0 1.280 C199000200019 0.0 20.0 2.200 C199000200020 0.0 35.0 0.710 C199000200021 0.0 42.0 0.870 C199000200022 61.0 5.0 10.400 C199000200023 61.0 20.0 1.620 C199000200024 61.0 35.0 1.040 C199000200025 61.0 42.0 0.490 C199000200026 88.0 5.0 0.300 C199000200027 88.0 20.0 0.300 C199000200028 88.0 35.0 0.570 C199000200029 88.0 42.0 0.600 C199000200030 502.0 5.0 0.047 C199000200031 502.0 20.0 0.053 C199000200032 502.0 35.0 0.014 C199000200033 502.0 42.0 0.021 C199000200034 685.0 5.0 0.041 C199000200035 685.0 20.0 0.020 C199000200036 685.0 35.0 0.020 C199000200037 685.0 42.0 0.015 C199000200038 783.0 5.0 0.580 C199000200039 783.0 20.0 1.270 C199000200040 783.0 35.0 0.390 C199000200041 783.0 42.0 0.580 C199000200042 924.0 5.0 0.069 C199000200043 924.0 20.0 0.170 C199000200044 924.0 35.0 0.240 C199000200045 924.0 42.0 0.140 C199000200046 1075.0 5.0 0.017 C199000200047 1075.0 20.0 0.025 C199000200048 1075.0 35.0 0.010 C199000200049 1075.0 42.0 0.016 C199000200050 1140.0 5.0 0.380 C199000200051 1140.0 20.0 0.710 C199000200052 1140.0 35.0 0.210 C199000200053 1140.0 42.0 0.350 C199000200054 1290.0 5.0 0.210 C199000200055 1290.0 20.0 0.360 C199000200056 1290.0 35.0 0.100 C199000200057 1290.0 42.0 0.170 C199000200058 1379.0 5.0 0.230 C199000200059 1379.0 20.0 0.390 C199000200060 1379.0 35.0 0.130 C199000200061 1379.0 42.0 0.200 C199000200062 1406.0 5.0 0.130 C199000200063 1406.0 20.0 0.052 C199000200064 1406.0 35.0 0.019 C199000200065 1406.0 42.0 0.012 C199000200066 1556.0 5.0 0.460 C199000200067 1556.0 20.0 0.760 C199000200068 1556.0 35.0 0.260 C199000200069 1556.0 42.0 0.390 C199000200070 1612.0 5.0 0.020 C199000200071 1612.0 20.0 0.030 C199000200072 1612.0 35.0 0.025 C199000200073 1612.0 42.0 0.034 C199000200074 1889.0 5.0 0.120 C199000200075 1889.0 20.0 0.076 C199000200076 1889.0 35.0 0.027 C199000200077 1889.0 42.0 0.024 C199000200078 1954.0 5.0 0.170 C199000200079 1954.0 20.0 0.084 C199000200080 1954.0 35.0 0.031 C199000200081 1954.0 42.0 0.020 C199000200082 2120.0 5.0 0.280 C199000200083 2120.0 20.0 0.097 C199000200084 2120.0 35.0 0.028 C199000200085 2120.0 42.0 0.017 C199000200086 2278.0 5.0 0.030 C199000200087 2278.0 20.0 0.020 C199000200088 2278.0 35.0 0.011 C199000200089 2278.0 42.0 0.004 C199000200090 2335.0 5.0 0.018 C199000200091 2335.0 20.0 0.006 C199000200092 ENDDATA 76 0 C199000200093 ENDSUBENT 92 0 C199000299999 SUBENT C1990003 20130403 C131C199000300001 BIB 4 7 C199000300002 REACTION (52-TE-130(P,D)52-TE-129,PAR,DA) C199000300003 SAMPLE (52-TE-130,ENR=0.994) Self-supporting target of C199000300004 thicknesses 671 mu-g/cm2 C199000300005 STATUS (TABLE) Data taken from tab. 3 of submission to XUNDL C199000300006 by B.P. Kay (March 14, 2013) C199000300007 ERR-ANALYS (ERR-S,1.0,3.0) Statistical uncertainty are less than C199000300008 1% for strong states and less than 3% for weak states C199000300009 ENDBIB 7 0 C199000300010 COMMON 2 3 C199000300011 EN EN-RSL C199000300012 MEV KEV C199000300013 23.0 30.0 C199000300014 ENDCOMMON 3 0 C199000300015 DATA 3 84 C199000300016 E-LVL ANG DATA C199000300017 KEV ADEG MB/SR C199000300018 0.0 5.0 0.110 C199000300019 0.0 20.0 0.260 C199000300020 0.0 35.0 0.310 C199000300021 0.0 42.0 0.490 C199000300022 106.0 5.0 0.360 C199000300023 106.0 20.0 0.300 C199000300024 106.0 35.0 0.560 C199000300025 106.0 42.0 0.610 C199000300026 180.0 5.0 8.300 C199000300027 180.0 20.0 1.740 C199000300028 180.0 35.0 1.100 C199000300029 180.0 42.0 0.680 C199000300030 360.0 5.0 0.015 C199000300031 360.0 20.0 0.004 C199000300032 360.0 35.0 0.008 C199000300033 545.0 5.0 0.022 C199000300034 545.0 20.0 0.026 C199000300035 545.0 35.0 0.007 C199000300036 545.0 42.0 0.012 C199000300037 760.0 5.0 0.045 C199000300038 760.0 20.0 0.064 C199000300039 760.0 35.0 0.042 C199000300040 760.0 42.0 0.045 C199000300041 813.0 35.0 0.022 C199000300042 813.0 42.0 0.014 C199000300043 872.0 5.0 0.045 C199000300044 872.0 20.0 0.066 C199000300045 872.0 35.0 0.028 C199000300046 872.0 42.0 0.041 C199000300047 967.0 5.0 1.600 C199000300048 967.0 20.0 0.440 C199000300049 967.0 35.0 0.700 C199000300050 1210.0 5.0 0.037 C199000300051 1210.0 20.0 0.160 C199000300052 1210.0 35.0 0.160 C199000300053 1210.0 42.0 0.120 C199000300054 1281.0 5.0 0.500 C199000300055 1281.0 20.0 1.030 C199000300056 1281.0 35.0 0.300 C199000300057 1281.0 42.0 0.490 C199000300058 1435.0 5.0 0.100 C199000300059 1435.0 20.0 0.190 C199000300060 1435.0 35.0 0.049 C199000300061 1435.0 42.0 0.088 C199000300062 1487.0 5.0 0.013 C199000300063 1487.0 20.0 0.029 C199000300064 1487.0 35.0 0.028 C199000300065 1487.0 42.0 0.024 C199000300066 1599.0 5.0 0.033 C199000300067 1599.0 20.0 0.054 C199000300068 1599.0 35.0 0.018 C199000300069 1599.0 42.0 0.019 C199000300070 1672.0 5.0 0.520 C199000300071 1672.0 20.0 0.940 C199000300072 1672.0 35.0 0.280 C199000300073 1672.0 42.0 0.470 C199000300074 1782.0 5.0 0.160 C199000300075 1782.0 20.0 0.260 C199000300076 1782.0 35.0 0.075 C199000300077 1782.0 42.0 0.120 C199000300078 1892.0 5.0 0.210 C199000300079 1892.0 20.0 0.160 C199000300080 1892.0 35.0 0.058 C199000300081 1892.0 42.0 0.066 C199000300082 2085.0 5.0 0.054 C199000300083 2085.0 20.0 0.023 C199000300084 2085.0 35.0 0.006 C199000300085 2085.0 42.0 0.009 C199000300086 2140.0 5.0 0.120 C199000300087 2140.0 20.0 0.051 C199000300088 2140.0 35.0 0.017 C199000300089 2140.0 42.0 0.022 C199000300090 2288.0 5.0 0.072 C199000300091 2288.0 20.0 0.031 C199000300092 2288.0 35.0 0.013 C199000300093 2288.0 42.0 0.018 C199000300094 2340.0 5.0 0.099 C199000300095 2340.0 20.0 0.040 C199000300096 2340.0 35.0 0.026 C199000300097 2340.0 42.0 0.023 C199000300098 2395.0 5.0 0.230 C199000300099 2395.0 20.0 0.090 C199000300100 2395.0 35.0 0.017 C199000300101 2395.0 42.0 0.012 C199000300102 ENDDATA 86 0 C199000300103 ENDSUBENT 102 0 C199000399999 SUBENT C1990004 20130403 C131C199000400001 BIB 4 7 C199000400002 REACTION (52-TE-128(D,P)52-TE-129,PAR,DA) C199000400003 SAMPLE (52-TE-128,ENR=0.992) Self-supporting target of C199000400004 thicknesses 436 mu-g/cm2 C199000400005 STATUS (TABLE) Data taken from tab. 4 of submission to XUNDL C199000400006 by B.P. Kay (March 14, 2013) C199000400007 ERR-ANALYS (ERR-S,1.0,3.0) Statistical uncertainty are less than C199000400008 1% for strong states and less than 3% for weak states C199000400009 ENDBIB 7 0 C199000400010 COMMON 2 3 C199000400011 EN EN-RSL C199000400012 MEV KEV C199000400013 15.0 30.0 C199000400014 ENDCOMMON 3 0 C199000400015 DATA 3 37 C199000400016 E-LVL ANG DATA C199000400017 KEV ADEG MB/SR C199000400018 0.0 7.0 0.480 C199000400019 0.0 18.0 1.350 C199000400020 0.0 34.0 0.440 C199000400021 0.0 42.0 0.610 C199000400022 106.0 7.0 0.040 C199000400023 106.0 18.0 0.140 C199000400024 106.0 34.0 0.170 C199000400025 106.0 42.0 0.180 C199000400026 180.0 7.0 2.220 C199000400027 180.0 18.0 0.095 C199000400028 180.0 34.0 0.690 C199000400029 180.0 42.0 0.290 C199000400030 545.0 18.0 0.016 C199000400031 545.0 42.0 0.007 C199000400032 634.0 18.0 0.032 C199000400033 634.0 42.0 0.013 C199000400034 813.0 18.0 0.012 C199000400035 813.0 34.0 0.014 C199000400036 813.0 42.0 0.009 C199000400037 872.0 18.0 0.031 C199000400038 872.0 34.0 0.017 C199000400039 872.0 42.0 0.014 C199000400040 967.0 7.0 0.099 C199000400041 967.0 18.0 0.290 C199000400042 967.0 34.0 0.120 C199000400043 967.0 42.0 0.120 C199000400044 1217.0 34.0 0.018 C199000400045 1217.0 42.0 0.018 C199000400046 1281.0 34.0 0.036 C199000400047 1281.0 42.0 0.048 C199000400048 1302.0 34.0 0.045 C199000400049 1302.0 42.0 0.018 C199000400050 1655.0 18.0 0.092 C199000400051 1655.0 42.0 0.035 C199000400052 1752.0 7.0 0.052 C199000400053 1752.0 18.0 0.050 C199000400054 1752.0 42.0 0.038 C199000400055 ENDDATA 39 0 C199000400056 ENDSUBENT 55 0 C199000499999 SUBENT C1990005 20130403 C131C199000500001 BIB 4 7 C199000500002 REACTION (52-TE-130(D,P)52-TE-131,PAR,DA) C199000500003 SAMPLE (52-TE-130,ENR=0.994) Self-supporting target of C199000500004 thicknesses 671 mu-g/cm2 C199000500005 STATUS (TABLE) Data taken from tab. 5 of submission to XUNDL C199000500006 by B.P. Kay (March 14, 2013) C199000500007 ERR-ANALYS (ERR-S,1.0,3.0) Statistical uncertainty are less than C199000500008 1% for strong states and less than 3% for weak states C199000500009 ENDBIB 7 0 C199000500010 COMMON 2 3 C199000500011 EN EN-RSL C199000500012 MEV KEV C199000500013 15.0 30.0 C199000500014 ENDCOMMON 3 0 C199000500015 DATA 3 27 C199000500016 E-LVL ANG DATA C199000500017 KEV ADEG MB/SR C199000500018 0.0 7.0 0.410 C199000500019 0.0 18.0 1.030 C199000500020 0.0 34.0 0.360 C199000500021 0.0 42.0 0.460 C199000500022 182.0 7.0 0.056 C199000500023 182.0 18.0 0.060 C199000500024 182.0 34.0 0.100 C199000500025 182.0 42.0 0.110 C199000500026 296.0 7.0 1.550 C199000500027 296.0 18.0 0.073 C199000500028 296.0 34.0 0.580 C199000500029 296.0 42.0 0.220 C199000500030 642.0 18.0 0.021 C199000500031 642.0 34.0 0.008 C199000500032 642.0 42.0 0.009 C199000500033 1042.0 34.0 0.019 C199000500034 1042.0 42.0 0.009 C199000500035 1207.0 7.0 0.025 C199000500036 1207.0 18.0 0.410 C199000500037 1207.0 34.0 0.075 C199000500038 1207.0 42.0 0.079 C199000500039 1399.0 34.0 0.010 C199000500040 1399.0 42.0 0.005 C199000500041 1470.0 18.0 0.089 C199000500042 1470.0 34.0 0.026 C199000500043 1470.0 42.0 0.035 C199000500044 1722.0 42.0 0.006 C199000500045 ENDDATA 29 0 C199000500046 ENDSUBENT 45 0 C199000599999 SUBENT C1990006 20130403 C131C199000600001 BIB 4 11 C199000600002 REACTION (54-XE-130(D,P)54-XE-131,PAR,DA) C199000600003 SAMPLE (54-XE-130,ENR=0.999) Cryogenically cooled, solid Xe C199000600004 target produced by spraying enriched Xe gas onto C199000600005 cryogenically cooled diamond foil with thickness of C199000600006 360mu-g/cm2. The typical thicknesses of Xe layers C199000600007 were from 200 to 1000 mu-g/cm2, determined by C199000600008 scattering measurements. C199000600009 STATUS (TABLE) Data taken from tab. 6 of submission to XUNDL C199000600010 by B.P. Kay (March 14, 2013) C199000600011 ERR-ANALYS (ERR-S,3.0,5.0) Statistical uncertainty are less than C199000600012 3% for strong states and less than 5% for weak states C199000600013 ENDBIB 11 0 C199000600014 COMMON 2 3 C199000600015 EN EN-RSL C199000600016 MEV KEV C199000600017 15.0 60.0 C199000600018 ENDCOMMON 3 0 C199000600019 DATA 3 26 C199000600020 E-LVL ANG DATA C199000600021 KEV ADEG MB/SR C199000600022 0.0 5.0 0.300 C199000600023 0.0 18.0 1.630 C199000600024 0.0 29.0 0.850 C199000600025 80.0 5.0 2.100 C199000600026 80.0 18.0 0.110 C199000600027 80.0 29.0 1.280 C199000600028 164.0 5.0 0.024 C199000600029 164.0 18.0 0.180 C199000600030 164.0 29.0 0.190 C199000600031 405.0 5.0 0.038 C199000600032 405.0 18.0 0.120 C199000600033 405.0 29.0 0.034 C199000600034 565.0 5.0 0.043 C199000600035 700.0 5.0 0.042 C199000600036 700.0 18.0 0.130 C199000600037 700.0 29.0 0.170 C199000600038 723.0 5.0 0.067 C199000600039 723.0 18.0 0.570 C199000600040 723.0 29.0 0.330 C199000600041 952.0 18.0 0.060 C199000600042 952.0 29.0 0.041 C199000600043 1035.0 18.0 0.140 C199000600044 1035.0 29.0 0.110 C199000600045 1240.0 5.0 0.310 C199000600046 1240.0 18.0 0.068 C199000600047 1240.0 29.0 0.278 C199000600048 ENDDATA 28 0 C199000600049 ENDSUBENT 48 0 C199000699999 SUBENT C1990007 20130403 C131C199000700001 BIB 4 11 C199000700002 REACTION (54-XE-132(D,P)54-XE-133,PAR,DA) C199000700003 SAMPLE (54-XE-130,ENR=0.999) Cryogenically cooled, solid Xe C199000700004 target produced by spraying enriched Xe gas onto C199000700005 cryogenically cooled diamond foil with thickness of C199000700006 360mu-g/cm2. The typical thicknesses of Xe layers C199000700007 were from 200 to 1000 mu-g/cm2, determined by C199000700008 scattering measurements. C199000700009 STATUS (TABLE) Data taken from tab. 7 of submission to XUNDL C199000700010 by B.P. Kay (March 14, 2013) C199000700011 ERR-ANALYS (ERR-S,3.0,5.0) Statistical uncertainty are less than C199000700012 3% for strong states and less than 5% for weak states C199000700013 ENDBIB 11 0 C199000700014 COMMON 2 3 C199000700015 EN EN-RSL C199000700016 MEV KEV C199000700017 15.0 60.0 C199000700018 ENDCOMMON 3 0 C199000700019 DATA 3 19 C199000700020 E-LVL ANG DATA C199000700021 KEV ADEG MB/SR C199000700022 0.0 5.0 0.160 C199000700023 0.0 18.0 1.300 C199000700024 0.0 29.0 0.460 C199000700025 233.0 18.0 0.078 C199000700026 233.0 29.0 0.110 C199000700027 263.0 5.0 0.980 C199000700028 263.0 18.0 0.100 C199000700029 263.0 29.0 0.790 C199000700030 530.0 18.0 0.041 C199000700031 530.0 29.0 0.030 C199000700032 680.0 5.0 0.019 C199000700033 680.0 18.0 0.023 C199000700034 744.0 18.0 0.045 C199000700035 744.0 29.0 0.044 C199000700036 929.0 5.0 0.075 C199000700037 929.0 29.0 0.089 C199000700038 1052.0 5.0 0.043 C199000700039 1052.0 18.0 0.280 C199000700040 1052.0 29.0 0.190 C199000700041 ENDDATA 21 0 C199000700042 ENDSUBENT 41 0 C199000799999 SUBENT C1990008 20130403 C131C199000800001 BIB 4 7 C199000800002 REACTION (52-TE-130(HE3,A)52-TE-129,PAR,DA) C199000800003 SAMPLE (52-TE-130,ENR=0.994) Self-supporting target of C199000800004 thicknesses 671 mu-g/cm2 C199000800005 STATUS (TABLE) Data taken from tab. 8 of submission to XUNDL C199000800006 by B.P. Kay (March 14, 2013) C199000800007 ERR-ANALYS (ERR-S,1.0,3.0) Statistical uncertainty are less than C199000800008 1% for strong states and less than 3% for weak states C199000800009 ENDBIB 7 0 C199000800010 COMMON 3 3 C199000800011 EN EN-RSL E-LVL C199000800012 MEV KEV KEV C199000800013 40.0 70.0 106.0 C199000800014 ENDCOMMON 3 0 C199000800015 DATA 2 2 C199000800016 ANG DATA C199000800017 ADEG MB/SR C199000800018 5.0 5.160 C199000800019 22.5 1.110 C199000800020 ENDDATA 4 0 C199000800021 ENDSUBENT 20 0 C199000899999 SUBENT C1990009 20130403 C131C199000900001 BIB 4 7 C199000900002 REACTION (52-TE-128(A,HE3)52-TE-129,PAR,DA) C199000900003 SAMPLE (52-TE-128,ENR=0.992) Self-supporting target of C199000900004 thicknesses 436 mu-g/cm2 C199000900005 STATUS (TABLE) Data taken from tab. 9 of submission to XUNDL C199000900006 by B.P. Kay (March 14, 2013) C199000900007 ERR-ANALYS (ERR-S,1.0,3.0) Statistical uncertainty are less than C199000900008 1% for strong states and less than 3% for weak states C199000900009 ENDBIB 7 0 C199000900010 COMMON 2 3 C199000900011 EN EN-RSL C199000900012 MEV KEV C199000900013 50.0 70.0 C199000900014 ENDCOMMON 3 0 C199000900015 DATA 3 11 C199000900016 E-LVL ANG DATA C199000900017 KEV ADEG MB/SR C199000900018 0.0 22.5 0.057 C199000900019 106.0 5.0 1.210 C199000900020 106.0 22.5 0.330 C199000900021 545.0 5.0 0.087 C199000900022 2108.0 22.5 0.043 C199000900023 2221.0 22.5 0.062 C199000900024 3085.0 5.0 0.120 C199000900025 3085.0 22.5 0.017 C199000900026 3655.0 5.0 0.064 C199000900027 3790.0 5.0 0.090 C199000900028 4121.0 5.0 0.610 C199000900029 ENDDATA 13 0 C199000900030 ENDSUBENT 29 0 C199000999999 SUBENT C1990010 20130403 C131C199001000001 BIB 4 7 C199001000002 REACTION (52-TE-130(A,HE3)52-TE-131,PAR,DA) C199001000003 SAMPLE (52-TE-130,ENR=0.994) Self-supporting target of C199001000004 thicknesses 671 mu-g/cm2 C199001000005 STATUS (TABLE) Data taken from tab.10 of submission to XUNDL C199001000006 by B.P. Kay (March 14, 2013) C199001000007 ERR-ANALYS (ERR-S,1.0,3.0) Statistical uncertainty are less than C199001000008 1% for strong states and less than 3% for weak states C199001000009 ENDBIB 7 0 C199001000010 COMMON 2 3 C199001000011 EN EN-RSL C199001000012 MEV KEV C199001000013 50.0 70.0 C199001000014 ENDCOMMON 3 0 C199001000015 DATA 3 14 C199001000016 E-LVL ANG DATA C199001000017 KEV ADEG MB/SR C199001000018 0.0 5.0 0.052 C199001000019 0.0 22.5 0.032 C199001000020 182.0 5.0 0.730 C199001000021 182.0 22.5 0.190 C199001000022 296.0 22.5 0.012 C199001000023 2275.0 22.5 0.087 C199001000024 2374.0 22.5 0.012 C199001000025 3054.0 22.5 0.005 C199001000026 3195.0 5.0 0.024 C199001000027 3195.0 22.5 0.025 C199001000028 4211.0 5.0 0.320 C199001000029 4211.0 22.5 0.220 C199001000030 5565.0 5.0 0.056 C199001000031 5565.0 22.5 0.022 C199001000032 ENDDATA 16 0 C199001000033 ENDSUBENT 32 0 C199001099999 SUBENT C1990011 20130403 C131C199001100001 BIB 4 11 C199001100002 REACTION (54-XE-130(A,HE3)54-XE-131,PAR,DA) C199001100003 SAMPLE (54-XE-130,ENR=0.999) Cryogenically cooled, solid Xe C199001100004 target produced by spraying enriched Xe gas onto C199001100005 cryogenically cooled diamond foil with thickness of C199001100006 360mu-g/cm2. The typical thicknesses of Xe layers C199001100007 were from 200 to 1000 mu-g/cm2, determined by C199001100008 scattering measurements. C199001100009 STATUS (TABLE) Data taken from tab.11 of submission to XUNDL C199001100010 by B.P. Kay (March 14, 2013) C199001100011 ERR-ANALYS (ERR-S,3.0,5.0) Statistical uncertainty are less than C199001100012 3% for strong states and less than 5% for weak states C199001100013 ENDBIB 11 0 C199001100014 COMMON 2 3 C199001100015 EN EN-RSL C199001100016 MEV KEV C199001100017 50.0 100.0 C199001100018 ENDCOMMON 3 0 C199001100019 DATA 3 1 C199001100020 E-LVL ANG DATA C199001100021 KEV ADEG MB/SR C199001100022 164.0 10.0 0.78 C199001100023 ENDDATA 3 0 C199001100024 ENDSUBENT 23 0 C199001199999 SUBENT C1990012 20130403 C131C199001200001 BIB 4 11 C199001200002 REACTION (54-XE-132(A,HE3)54-XE-133,PAR,DA) C199001200003 SAMPLE (54-XE-132,ENR=0.999) Cryogenically cooled, solid Xe C199001200004 target produced by spraying enriched Xe gas onto C199001200005 cryogenically cooled diamond foil with thickness of C199001200006 360mu-g/cm2. The typical thicknesses of Xe layers C199001200007 were from 200 to 1000 mu-g/cm2, determined by C199001200008 scattering measurements. C199001200009 STATUS (TABLE) Data taken from tab.11 of submission to XUNDL C199001200010 by B.P. Kay (March 14, 2013) C199001200011 ERR-ANALYS (ERR-S,3.0,5.0) Statistical uncertainty are less than C199001200012 3% for strong states and less than 5% for weak states C199001200013 ENDBIB 11 0 C199001200014 COMMON 2 3 C199001200015 EN EN-RSL C199001200016 MEV KEV C199001200017 50.0 100.0 C199001200018 ENDCOMMON 3 0 C199001200019 DATA 3 1 C199001200020 E-LVL ANG DATA C199001200021 KEV ADEG MB/SR C199001200022 233.0 5.0 0.42 C199001200023 ENDDATA 3 0 C199001200024 ENDSUBENT 23 0 C199001299999 ENDENTRY 12 0 C199099999999