ENTRY C1298 20181107 C181C1298 0 1 SUBENT C1298001 20181107 C181C1298 1 1 BIB 10 18 C1298 1 2 INSTITUTE (1USACOL) C1298 1 3 REFERENCE (J,RSI,28,56(2),1957) C1298 1 4 AUTHOR (K.W.Jones,T.H.Kruse,J.L.Weil,J.A.Baicker,L.J.Lidofsky)C1298 1 5 TITLE Neutron production from proton and deuteron C1298 1 6 bombardment of nickel C1298 1 7 FACILITY (VDG,1USACOL) C1298 1 8 INC-SOURCE Deuteron beam, calibrated with a Ra-Be neutron source C1298 1 9 DETECTOR (LONGC) Long counter C1298 1 10 SAMPLE Natural nickel foil targets with densities of C1298 1 11 2.33 mg/cm2 and 0.60 mg/cm2, backed by a thick C1298 1 12 (580 mg/cm2) gold beam stop, were used C1298 1 13 CORRECTION The cross sections have not been corrected for any C1298 1 14 energy dependence of the long counter because of the C1298 1 15 presence of several neutron groups of different C1298 1 16 energies. C1298 1 17 HISTORY (20050805C) DR C1298 1 18 (20120624A) SD: Title was added; BIB update. C1298 1 19 (20181104U) OS. Minor BIB corrections C1298 1 20 ENDBIB 18 0 C1298 1 21 COMMON 1 3 C1298 1 22 ANG C1298 1 23 ADEG C1298 1 24 0. C1298 1 25 ENDCOMMON 3 0 C1298 1 26 ENDSUBENT 25 0 C1298 199999 SUBENT C1298002 20181107 C181C1298 2 1 BIB 3 4 C1298 2 2 REACTION (28-NI-0(D,N),,DA) C1298 2 3 ERR-ANALYS (DATA-ERR) No information on sources of uncertainties C1298 2 4 STATUS (TABLE) Data received on table from author, obtained C1298 2 5 from Fig.1 C1298 2 6 ENDBIB 4 0 C1298 2 7 COMMON 1 3 C1298 2 8 DATA-ERR C1298 2 9 PER-CENT C1298 2 10 40. C1298 2 11 ENDCOMMON 3 0 C1298 2 12 DATA 2 42 C1298 2 13 EN DATA C1298 2 14 MEV MB/SR C1298 2 15 1.095 0.016 C1298 2 16 1.190 0.048 C1298 2 17 1.310 0.088 C1298 2 18 1.540 0.016 C1298 2 19 1.650 0.032 C1298 2 20 1.690 0.016 C1298 2 21 1.755 0.016 C1298 2 22 1.890 0.024 C1298 2 23 1.990 0.032 C1298 2 24 2.090 0.088 C1298 2 25 2.215 0.184 C1298 2 26 2.275 0.152 C1298 2 27 2.355 0.216 C1298 2 28 2.420 0.200 C1298 2 29 2.510 0.416 C1298 2 30 2.585 0.320 C1298 2 31 2.745 0.272 C1298 2 32 2.855 0.336 C1298 2 33 2.950 0.656 C1298 2 34 3.045 0.496 C1298 2 35 3.150 0.520 C1298 2 36 3.260 0.832 C1298 2 37 3.360 0.776 C1298 2 38 3.470 1.27 C1298 2 39 3.560 1.19 C1298 2 40 3.670 1.62 C1298 2 41 3.750 1.70 C1298 2 42 3.860 2.04 C1298 2 43 3.960 2.66 C1298 2 44 4.075 2.55 C1298 2 45 4.180 2.73 C1298 2 46 4.275 3.12 C1298 2 47 4.380 3.42 C1298 2 48 4.485 4.00 C1298 2 49 4.590 4.16 C1298 2 50 4.700 5.22 C1298 2 51 4.820 5.46 C1298 2 52 4.900 5.93 C1298 2 53 5.005 7.06 C1298 2 54 5.120 6.68 C1298 2 55 5.235 7.27 C1298 2 56 5.305 7.57 C1298 2 57 ENDDATA 44 0 C1298 2 58 ENDSUBENT 57 0 C1298 299999 SUBENT C1298003 20181107 C181C1298 3 1 BIB 3 4 C1298 3 2 REACTION (28-NI-0(P,N),,DA) C1298 3 3 ERR-ANALYS (DATA-ERR) No information on sources of uncertainties C1298 3 4 STATUS (TABLE) Data received on table from author, obtained C1298 3 5 from Fig.2 C1298 3 6 ENDBIB 4 0 C1298 3 7 COMMON 1 3 C1298 3 8 DATA-ERR C1298 3 9 PER-CENT C1298 3 10 40. C1298 3 11 ENDCOMMON 3 0 C1298 3 12 DATA 2 93 C1298 3 13 EN DATA C1298 3 14 MEV MB/SR C1298 3 15 1.550 0.0015 C1298 3 16 1.595 0.0015 C1298 3 17 1.670 0.0015 C1298 3 18 1.740 0.0015 C1298 3 19 1.820 0.0015 C1298 3 20 1.900 0.0135 C1298 3 21 1.975 0.0075 C1298 3 22 2.060 0.0045 C1298 3 23 2.145 0.0045 C1298 3 24 2.245 0.0060 C1298 3 25 2.315 0.0135 C1298 3 26 2.395 0.0150 C1298 3 27 2.500 0.0210 C1298 3 28 2.590 0.0315 C1298 3 29 2.665 0.0390 C1298 3 30 2.770 0.0405 C1298 3 31 2.870 0.0495 C1298 3 32 2.945 0.0450 C1298 3 33 3.045 0.0510 C1298 3 34 3.135 0.0630 C1298 3 35 3.235 0.0735 C1298 3 36 3.325 0.0870 C1298 3 37 3.395 0.113 C1298 3 38 3.430 0.0975 C1298 3 39 3.490 0.0780 C1298 3 40 3.555 0.0930 C1298 3 41 3.620 0.100 C1298 3 42 3.690 0.105 C1298 3 43 3.750 0.108 C1298 3 44 3.810 0.114 C1298 3 45 3.870 0.123 C1298 3 46 3.935 0.122 C1298 3 47 4.000 0.123 C1298 3 48 4.065 0.149 C1298 3 49 4.130 0.173 C1298 3 50 4.185 0.159 C1298 3 51 4.240 0.211 C1298 3 52 4.320 0.312 C1298 3 53 4.370 0.213 C1298 3 54 4.440 0.197 C1298 3 55 4.500 0.216 C1298 3 56 4.565 0.263 C1298 3 57 4.630 0.354 C1298 3 58 4.695 0.372 C1298 3 59 4.750 0.354 C1298 3 60 4.810 0.423 C1298 3 61 4.945 0.605 C1298 3 62 5.000 0.658 C1298 3 63 5.060 0.728 C1298 3 64 5.130 0.786 C1298 3 65 5.180 0.837 C1298 3 66 5.215 0.765 C1298 3 67 5.235 0.690 C1298 3 68 5.255 0.835 C1298 3 69 5.270 0.883 C1298 3 70 5.325 0.976 C1298 3 71 5.355 1.09 C1298 3 72 5.395 1.25 C1298 3 73 5.420 1.23 C1298 3 74 5.430 1.13 C1298 3 75 5.455 1.15 C1298 3 76 5.495 1.16 C1298 3 77 5.520 1.20 C1298 3 78 5.520 1.29 C1298 3 79 5.550 1.32 C1298 3 80 5.550 1.33 C1298 3 81 5.570 1.37 C1298 3 82 5.590 1.48 C1298 3 83 5.605 1.40 C1298 3 84 5.650 1.48 C1298 3 85 5.650 1.51 C1298 3 86 5.680 1.50 C1298 3 87 5.700 1.63 C1298 3 88 5.720 1.73 C1298 3 89 5.730 1.61 C1298 3 90 5.750 1.75 C1298 3 91 5.765 1.79 C1298 3 92 5.770 1.65 C1298 3 93 5.780 1.82 C1298 3 94 5.800 1.92 C1298 3 95 5.820 1.89 C1298 3 96 5.830 1.97 C1298 3 97 5.850 2.15 C1298 3 98 5.870 2.02 C1298 3 99 5.880 2.06 C1298 3 100 5.880 2.13 C1298 3 101 5.910 2.04 C1298 3 102 5.940 2.03 C1298 3 103 5.945 1.79 C1298 3 104 5.960 2.22 C1298 3 105 5.990 2.03 C1298 3 106 6.000 2.45 C1298 3 107 6.030 2.41 C1298 3 108 ENDDATA 95 0 C1298 3 109 ENDSUBENT 108 0 C1298 399999 ENDENTRY 3 0 C129899999999