ENTRY C0109 20111117 C113C010900000001 SUBENT C0109001 20111117 C113C010900100001 BIB 12 35 C010900100002 INSTITUTE (1USALAS) C010900100003 REFERENCE (J,PR/C,41,1391,199004) C010900100004 (J,NIM/B,10-11,405,1985) prelim.results C010900100005 ((J,RE,92,45,1986)=(C,85SANTA,1,45,1985)) prelim.res. C010900100006 AUTHOR (R.E.Brown,N.Jarmie) C010900100007 TITLE Differential cross sections at low energies for C010900100008 2H(d,p)3H and 2H(d,n)3He C010900100009 FACILITY (VDGT,1USALAS) Cross-section facility LEFCS C010900100010 SAMPLE A cryogenic windowless gas target was chosen to avoid C010900100011 energy-loss uncertainty in entrance and exit foils. A C010900100012 temperature of the target chamber (10.5 K for C010900100013 deuterium and 11.2 K for tritium gas) just above the C010900100014 freezing point of the target gas gives the maximum C010900100015 target density compatible with an appropriate energy C010900100016 loss in the target. The resulting gas density is low, C010900100017 approximately 10**4 nuclei/cm3. C010900100018 REL-REF (I,,N.Jarmie+,J,PR/C,29,2031,1984) C010900100019 (I,,N.Jarmie+,J,PR/C,33,385,1986) C010900100020 METHOD (PHD) C010900100021 DETECTOR (SIBAR) Silicon surface-barrier detector. C010900100022 ERR-ANALYS (ERR-1) Scale uncertainty C010900100023 Total uncertainty is combination in quadrature of C010900100024 relative and scale uncertainties. C010900100025 Angle and energy errors are contained in relative C010900100026 uncertainty given. C010900100027 (ANG-ERR) Due to uncertainty in detector position and C010900100028 in beam direction. C010900100029 STATUS No reply to author proof received from N. Jarmie. C010900100030 HISTORY (19961203C) SD (Arzamas RFNC-VNIIEF) + VM (NNDC) C010900100031 (19970708A) Update for information received in private C010900100032 communication, N. Jarmie. C010900100033 (20111117A) SD: In Subent 003 Energy units changed: C010900100034 (MeV => keV). BIB updated: presentation of year C010900100035 in HISTORY and REFERENCE changed to four digits. C010900100036 Subents 006,007 added. C010900100037 ENDBIB 35 0 C010900100038 COMMON 5 3 C010900100039 EN-ERR EN-RSL-FW ANG-ERR ANG-RSL ERR-1 C010900100040 EV EV ADEG ADEG PER-CENT C010900100041 15. 40. 0.1 3.2 1.3 C010900100042 ENDCOMMON 3 0 C010900100043 ENDSUBENT 42 0 C010900199999 SUBENT C0109002 20111117 C113C010900200001 BIB 6 6 C010900200002 REACTION (1-H-2(D,P)1-H-3,,DA) C010900200003 PART-DET (P,T) C010900200004 FLAG (1.) Tritons detected. C010900200005 ERR-ANALYS (DATA-ERR) Relative uncertainty. C010900200006 STATUS (TABLE) Tabulated data from N. Jarmie, 1996/12/2. C010900200007 HISTORY (19970708A) Energy heading corrected, FLAG added. C010900200008 ENDBIB 6 0 C010900200009 NOCOMMON 0 0 C010900200010 DATA 5 130 C010900200011 EN ANG-CM DATA-CM DATA-ERR FLAG C010900200012 KEV ADEG MB/SR MB/SR NO-DIM C010900200013 19.944 28.0 0.0236 0.0019 1. C010900200014 19.944 45.7 0.0224 0.0017 C010900200015 19.944 46.6 0.0237 0.0019 C010900200016 19.944 55.8 0.0228 0.0026 1. C010900200017 19.944 77.0 0.0188 0.0020 C010900200018 19.944 85.5 0.0212 0.0026 1. C010900200019 19.944 91.2 0.0225 0.0021 C010900200020 19.944 99.8 0.0197 0.0022 1. C010900200021 19.944 121.4 0.0225 0.0021 C010900200022 19.944 131.1 0.0206 0.0019 C010900200023 19.944 132.0 0.0207 0.0017 C010900200024 19.944 150.4 0.0211 0.0017 C010900200025 29.935 27.4 0.1064 0.0039 1. C010900200026 29.935 46.0 0.0987 0.0038 C010900200027 29.935 46.9 0.0987 0.0039 C010900200028 29.935 54.9 0.0947 0.0046 1. C010900200029 29.935 77.4 0.0912 0.0044 C010900200030 29.935 84.4 0.0867 0.0046 1. C010900200031 29.935 91.6 0.0886 0.0044 C010900200032 29.935 98.7 0.0932 0.0045 1. C010900200033 29.935 121.7 0.0903 0.0042 C010900200034 29.935 130.3 0.0951 0.0037 C010900200035 29.935 131.2 0.0939 0.0036 C010900200036 29.935 150.5 0.1011 0.0035 C010900200037 39.927 27.0 0.2451 0.0056 1. C010900200038 39.927 46.2 0.2151 0.0053 C010900200039 39.927 47.1 0.2142 0.0053 C010900200040 39.927 54.0 0.2036 0.0065 1. C010900200041 39.927 77.7 0.1974 0.0060 C010900200042 39.927 83.5 0.1852 0.0061 1. C010900200043 39.927 91.9 0.1844 0.0058 C010900200044 39.927 97.8 0.2010 0.0062 1. C010900200045 39.927 121.9 0.2097 0.0060 C010900200046 39.927 129.6 0.2111 0.0051 C010900200047 39.927 130.5 0.2158 0.0051 C010900200048 39.927 150.7 0.2425 0.0051 C010900200049 49.922 26.5 0.4198 0.0087 1. C010900200050 49.922 46.4 0.3577 0.0076 C010900200051 49.922 47.3 0.3594 0.0077 C010900200052 49.922 53.3 0.3619 0.0098 1. C010900200053 49.922 78.0 0.3270 0.0088 C010900200054 49.922 82.6 0.3110 0.0091 1. C010900200055 49.922 92.2 0.3249 0.0089 C010900200056 49.922 97.0 0.3241 0.0089 1. C010900200057 49.922 122.2 0.3585 0.0089 C010900200058 49.922 129.0 0.3567 0.0076 C010900200059 49.922 130.0 0.3705 0.0077 C010900200060 49.922 150.8 0.4051 0.0073 C010900200061 59.917 26.2 0.620 0.012 1. C010900200062 59.917 46.6 0.549 0.011 C010900200063 59.917 47.5 0.547 0.011 C010900200064 59.917 52.7 0.537 0.014 1. C010900200065 59.917 78.2 0.459 0.012 C010900200066 59.917 81.9 0.474 0.013 1. C010900200067 59.917 92.4 0.448 0.012 C010900200068 59.917 96.3 0.491 0.013 1. C010900200069 59.917 122.4 0.505 0.012 C010900200070 59.917 128.5 0.527 0.011 C010900200071 59.917 129.4 0.541 0.011 C010900200072 59.917 151.0 0.598 0.010 C010900200073 69.914 25.8 0.831 0.013 1. C010900200074 69.914 46.7 0.726 0.011 C010900200075 69.914 47.6 0.726 0.011 C010900200076 69.914 52.1 0.711 0.015 1. C010900200077 69.914 78.4 0.605 0.012 C010900200078 69.914 81.2 0.614 0.025 1. C010900200079 69.914 92.6 0.616 0.023 C010900200080 69.914 95.6 0.616 0.013 1. C010900200081 69.914 122.6 0.672 0.013 C010900200082 69.914 128.0 0.709 0.011 C010900200083 69.914 129.0 0.720 0.011 C010900200084 69.914 151.1 0.824 0.011 C010900200085 79.912 25.5 1.063 0.017 1. C010900200086 79.912 46.9 0.953 0.014 C010900200087 79.912 47.8 0.875 0.013 C010900200088 79.912 51.5 0.853 0.018 1. C010900200089 79.912 78.6 0.784 0.015 C010900200090 79.912 80.6 0.746 0.028 1. C010900200091 79.912 92.9 0.704 0.024 C010900200092 79.912 95.0 0.763 0.015 1. C010900200093 79.912 122.8 0.835 0.015 C010900200094 79.912 127.6 0.850 0.013 C010900200095 79.912 128.5 0.886 0.013 C010900200096 79.912 151.2 1.037 0.013 C010900200097 89.911 25.2 1.297 0.010 1. C010900200098 89.911 47.0 1.099 0.008 C010900200099 89.911 47.9 1.102 0.008 C010900200100 89.911 51.0 1.057 0.011 1. C010900200101 89.911 78.8 0.910 0.012 C010900200102 89.911 80.0 0.894 0.016 1. C010900200103 89.911 93.1 0.908 0.015 C010900200104 89.911 94.4 0.902 0.009 1. C010900200105 89.911 122.9 1.022 0.009 C010900200106 89.911 127.1 1.052 0.007 C010900200107 89.911 128.1 1.069 0.008 C010900200108 89.911 151.3 1.276 0.008 C010900200109 99.909 24.9 1.516 0.024 1. C010900200110 99.909 47.2 1.290 0.018 C010900200111 99.909 48.1 1.239 0.017 C010900200112 99.909 50.5 1.223 0.025 1. C010900200113 99.909 79.0 1.078 0.019 C010900200114 99.909 79.4 1.032 0.029 1. C010900200115 99.909 93.2 1.020 0.027 C010900200116 99.909 93.9 1.040 0.020 1. C010900200117 99.909 123.1 1.188 0.020 C010900200118 99.909 126.7 1.211 0.017 C010900200119 99.909 127.7 1.208 0.017 C010900200120 99.909 151.4 1.498 0.018 C010900200121 109.909 24.6 1.725 0.025 1. C010900200122 109.909 47.3 1.420 0.018 C010900200123 109.909 48.2 1.442 0.018 C010900200124 109.909 50.1 1.391 0.027 1. C010900200125 109.909 78.9 1.168 0.032 C010900200126 109.909 79.2 1.176 0.020 1. C010900200127 109.909 93.4 1.134 0.029 C010900200128 109.909 93.4 1.194 0.021 1. C010900200129 109.909 123.3 1.360 0.021 C010900200130 109.909 126.4 1.398 0.017 C010900200131 109.909 127.3 1.381 0.017 C010900200132 109.909 151.5 1.702 0.019 C010900200133 116.909 24.5 1.917 0.034 1. C010900200134 116.909 47.4 1.574 0.026 C010900200135 116.909 48.3 1.555 0.026 C010900200136 116.909 49.8 1.542 0.040 1. C010900200137 116.909 79.3 1.249 0.028 C010900200138 116.909 93.0 1.262 0.029 1. C010900200139 116.909 123.4 1.431 0.029 C010900200140 116.909 126.1 1.452 0.024 C010900200141 116.909 127.1 1.514 0.024 C010900200142 116.909 151.5 1.890 0.027 C010900200143 ENDDATA 132 0 C010900200144 ENDSUBENT 143 0 C010900299999 SUBENT C0109003 20111117 C113C010900300001 BIB 5 6 C010900300002 REACTION (1-H-2(D,N)2-HE-3,,DA) C010900300003 PART-DET (HE3) C010900300004 ERR-ANALYS (DATA-ERR) Relative uncertainty. C010900300005 STATUS (TABLE) Tabulated data from N. Jarmie, 1996/12/2. C010900300006 HISTORY (19970708A) Energy heading corrected. C010900300007 (20111117A) SD: Energy units changed: (MeV => keV). C010900300008 ENDBIB 6 0 C010900300009 NOCOMMON 0 0 C010900300010 DATA 4 66 C010900300011 EN ANG-CM DATA-CM DATA-ERR C010900300012 KEV ADEG MB/SR MB/SR C010900300013 19.944 27.7 0.0244 0.0119 C010900300014 19.944 55.3 0.0216 0.0029 C010900300015 19.944 85.0 0.0176 0.0024 C010900300016 19.944 99.3 0.0169 0.0020 C010900300017 19.944 130.7 0.0247 0.0022 C010900300018 19.944 131.6 0.0253 0.0019 C010900300019 29.935 27.1 0.11433 0.0043 C010900300020 29.935 54.3 0.0949 0.0050 C010900300021 29.935 83.7 0.0768 0.0044 C010900300022 29.935 98.1 0.0830 0.0043 C010900300023 29.935 129.8 0.0916 0.0037 C010900300024 29.935 130.7 0.0958 0.0037 C010900300025 39.927 26.6 0.2552 0.0060 C010900300026 39.927 53.4 0.2063 0.0067 C010900300027 39.927 82.7 0.1799 0.0061 C010900300028 39.927 97.1 0.1755 0.0058 C010900300029 39.927 129.1 0.2233 0.0051 C010900300030 39.927 130.0 0.2286 0.0056 C010900300031 49.922 26.1 0.4724 0.0098 C010900300032 49.922 52.6 0.3736 0.0104 C010900300033 49.922 81.8 0.2989 0.0094 C010900300034 49.922 96.2 0.3084 0.0089 C010900300035 49.922 128.4 0.3751 0.0079 C010900300036 49.922 129.4 0.3904 0.0079 C010900300037 59.917 25.7 0.718 0.015 C010900300038 59.917 51.9 0.541 0.015 C010900300039 59.917 81.0 0.446 0.013 C010900300040 59.917 95.4 0.446 0.013 C010900300041 59.917 127.8 0.559 0.011 C010900300042 59.917 128.8 0.581 0.011 C010900300043 69.914 25.3 1.003 0.017 C010900300044 69.914 51.2 0.762 0.017 C010900300045 69.914 80.2 0.589 0.014 C010900300046 69.914 94.7 0.558 0.013 C010900300047 69.914 127.3 0.746 0.011 C010900300048 69.914 128.3 0.745 0.011 C010900300049 79.912 25.0 1.194 0.020 C010900300050 79.912 50.6 0.920 0.020 C010900300051 79.912 79.5 0.744 0.017 C010900300052 79.912 94.0 0.712 0.015 C010900300053 79.912 126.8 0.904 0.013 C010900300054 79.912 127.7 0.945 0.013 C010900300055 89.911 24.6 1.500 0.012 C010900300056 89.911 50.0 1.153 0.012 C010900300057 89.911 78.8 0.913 0.010 C010900300058 89.911 93.3 0.871 0.009 C010900300059 89.911 126.3 1.128 0.008 C010900300060 89.911 127.3 1.141 0.008 C010900300061 99.909 24.3 1.776 0.030 C010900300062 99.909 49.5 1.382 0.028 C010900300063 99.909 78.2 1.028 0.022 C010900300064 99.909 92.7 1.038 0.021 C010900300065 99.909 125.9 1.270 0.017 C010900300066 99.909 126.9 1.346 0.018 C010900300067 109.909 24.0 2.118 0.034 C010900300068 109.909 49.0 1.589 0.030 C010900300069 109.909 77.6 1.223 0.024 C010900300070 109.909 92.1 1.113 0.022 C010900300071 109.909 125.5 1.511 0.019 C010900300072 109.909 126.4 1.550 0.020 C010900300073 116.909 23.8 2.252 0.041 C010900300074 116.909 48.6 1.694 0.042 C010900300075 116.909 77.2 1.304 0.033 C010900300076 116.909 91.8 1.212 0.032 C010900300077 116.909 125.2 1.621 0.025 C010900300078 116.909 126.2 1.608 0.026 C010900300079 ENDDATA 68 0 C010900300080 ENDSUBENT 79 0 C010900399999 SUBENT C0109004 20111117 C113C010900400001 BIB 4 10 C010900400002 REACTION 1(1-H-2(D,P)1-H-3,,SIG) C010900400003 2(1-H-2(D,P)1-H-3,,SIG,,SFC) C010900400004 ANALYSIS (INTAD) C010900400005 ERR-ANALYS (DATA-ERR) Relative uncertainty. Full correlation C010900400006 among coefficients taken into account. C010900400007 STATUS (DEP,C0109006) with the coefficients a, b, and c (in C010900400008 Subent 007 marked as 0,2,4) determined from a C010900400009 least-squares fit to the data, angle-integrated cross C010900400010 section a from sig=4Pi(a + b/3 + c/5) was computed. C010900400011 (TABLE) Data taken from table II of PR/C,41,1391 C010900400012 ENDBIB 10 0 C010900400013 NOCOMMON 0 0 C010900400014 DATA 4 11 C010900400015 EN DATA 1DATA 2DATA-ERR C010900400016 KEV MB B*KEV PER-CENT C010900400017 19.94 0.2704 56.1 2.8 C010900400018 29.94 1.190 59.61 1.3 C010900400019 39.93 2.641 59.39 0.87 C010900400020 49.92 4.481 59.96 0.78 C010900400021 59.92 6.584 61.13 0.73 C010900400022 69.91 8.759 61.98 0.67 C010900400023 79.91 10.91 62.61 0.64 C010900400024 89.91 13.22 64.21 0.42 C010900400025 99.91 15.31 64.99 0.59 C010900400026 109.9 17.35 65.85 0.56 C010900400027 116.9 18.81 66.77 0.75 C010900400028 ENDDATA 13 0 C010900400029 ENDSUBENT 28 0 C010900499999 SUBENT C0109005 20111117 C113C010900500001 BIB 4 10 C010900500002 REACTION 1(1-H-2(D,N)2-HE-3,,SIG) C010900500003 2(1-H-2(D,N)2-HE-3,,SIG,,SFC) C010900500004 ANALYSIS (INTAD) C010900500005 ERR-ANALYS (DATA-ERR) Relative uncertainty. Full correlation C010900500006 among coefficients taken into account. C010900500007 STATUS (DEP,C0109007) with the coefficients a, b, and c (in C010900500008 Subent 007 marked as 0,2,4) determined from a C010900500009 least-squares fit to the data, angle-integrated cross C010900500010 section a from sig=4Pi(a + b/3 + c/5) was computed. C010900500011 (TABLE) Data taken from table II of PR/C,41,1391 C010900500012 ENDBIB 10 0 C010900500013 COMMON 1 3 C010900500014 ERR-1 C010900500015 PER-CENT C010900500016 1.3 C010900500017 ENDCOMMON 3 0 C010900500018 DATA 4 11 C010900500019 EN DATA 1DATA 2DATA-ERR C010900500020 KEV MB B*KEV PER-CENT C010900500021 19.94 0.2730 56.70 4.0 C010900500022 29.94 1.161 58.10 1.8 C010900500023 39.93 2.667 59.99 1.2 C010900500024 49.92 4.651 62.24 1.0 C010900500025 59.92 6.927 64.31 1.0 C010900500026 69.91 9.237 65.36 0.86 C010900500027 79.91 11.38 65.32 0.82 C010900500028 89.91 14.08 68.41 0.46 C010900500029 99.91 16.44 69.79 0.79 C010900500030 109.9 19.10 72.50 0.75 C010900500031 116.9 20.36 72.27 0.89 C010900500032 ENDDATA 13 0 C010900500033 ENDSUBENT 32 0 C010900599999 SUBENT C0109006 20111117 C113C010900600001 BIB 4 7 C010900600002 REACTION (1-H-2(D,P)1-H-3,,DA,,COS) C010900600003 ERR-ANALYS (DATA-ERR) Diagonal elements of the error matrix of C010900600004 the fit and, therefore, do not reflect the C010900600005 correlations among the coefficients. C010900600006 STATUS (TABLE) Tbl.1 from PR/C,41,1391 C010900600007 (DEP,C0109002) C010900600008 HISTORY (20111117C) SD C010900600009 ENDBIB 7 0 C010900600010 NOCOMMON 0 0 C010900600011 DATA 4 30 C010900600012 NUMBER EN DATA DATA-ERR C010900600013 NO-DIM KEV MB/SR MB/SR C010900600014 0. 19.944 0.0208 0.0010 C010900600015 0. 29.935 0.0886 0.0020 C010900600016 0. 39.927 0.1882 0.0028 C010900600017 0. 49.922 0.3215 0.0048 C010900600018 0. 59.917 0.4636 0.0067 C010900600019 0. 69.914 0.6055 0.0085 C010900600020 0. 79.912 0.7528 0.0099 C010900600021 0. 89.911 0.8976 0.0064 C010900600022 0. 99.909 1.041 0.012 C010900600023 0. 109.909 1.166 0.013 C010900600024 0. 116.909 1.243 0.021 C010900600025 2. 19.944 0.0023 0.0022 C010900600026 2. 29.935 0.0184 0.0044 C010900600027 2. 39.927 0.0659 0.0062 C010900600028 2. 49.922 0.076 0.027 C010900600029 2. 59.917 0.168 0.038 C010900600030 2. 69.914 0.251 0.044 C010900600031 2. 79.912 0.250 0.052 C010900600032 2. 89.911 0.378 0.032 C010900600033 2. 99.909 0.367 0.066 C010900600034 2. 109.909 0.521 0.069 C010900600035 2. 116.909 0.55 0.11 C010900600036 4. 49.922 0.048 0.034 C010900600037 4. 59.917 0.021 0.048 C010900600038 4. 69.914 0.039 0.052 C010900600039 4. 79.912 0.162 0.062 C010900600040 4. 89.911 0.142 0.037 C010900600041 4. 99.909 0.276 0.080 C010900600042 4. 109.909 0.203 0.083 C010900600043 4. 116.909 0.34 0.12 C010900600044 ENDDATA 32 0 C010900600045 ENDSUBENT 44 0 C010900699999 SUBENT C0109007 20111117 C113C010900700001 BIB 4 7 C010900700002 REACTION (1-H-2(D,N)2-HE-3,,DA,,COS) C010900700003 ERR-ANALYS (DATA-ERR) Diagonal elements of the error matrix of C010900700004 the fit and, therefore, do not reflect the C010900700005 correlations among the coefficients. C010900700006 STATUS (TABLE) Tbl.1 from PR/C,41,1391 C010900700007 (DEP,C0109003) C010900700008 HISTORY (20111117C) SD C010900700009 ENDBIB 7 0 C010900700010 NOCOMMON 0 0 C010900700011 DATA 4 29 C010900700012 NUMBER EN DATA DATA-ERR C010900700013 NO-DIM KEV MB/SR MB/SR C010900700014 0. 19.944 0.0181 0.0014 C010900700015 0. 29.935 0.0782 0.0028 C010900700016 0. 39.927 0.1780 0.0039 C010900700017 0. 49.922 0.2994 0.0059 C010900700018 0. 59.917 0.4406 0.0097 C010900700019 0. 69.914 0.564 0.010 C010900700020 0. 79.912 0.716 0.012 C010900700021 0. 89.911 0.8769 0.0072 C010900700022 0. 99.909 1.018 0.016 C010900700023 0. 109.909 1.138 0.018 C010900700024 0. 116.909 1.231 0.025 C010900700025 2. 19.944 0.0108 0.0031 C010900700026 2. 29.935 0.0425 0.0066 C010900700027 2. 39.927 0.1027 0.0091 C010900700028 2. 49.922 0.212 0.014 C010900700029 2. 59.917 0.303 0.055 C010900700030 2. 69.914 0.446 0.057 C010900700031 2. 79.912 0.537 0.068 C010900700032 2. 89.911 0.674 0.041 C010900700033 2. 99.909 0.755 0.094 C010900700034 2. 109.909 1.09 0.10 C010900700035 2. 116.909 1.05 0.14 C010900700036 4. 59.917 0.049 0.070 C010900700037 4. 69.914 0.111 0.073 C010900700038 4. 79.912 0.052 0.086 C010900700039 4. 89.911 0.095 0.051 C010900700040 4. 99.909 0.20 0.12 C010900700041 4. 109.909 0.09 0.13 C010900700042 4. 116.909 0.20 0.17 C010900700043 ENDDATA 31 0 C010900700044 ENDSUBENT 43 0 C010900799999 ENDENTRY 7 0 C010999999999