ENTRY C1298 20181107 C181C129800000001
SUBENT C1298001 20181107 C181C129800100001
BIB 10 18 C129800100002
INSTITUTE (1USACOL) C129800100003
REFERENCE (J,RSI,28,56(2),1957) C129800100004
AUTHOR (K.W.Jones,T.H.Kruse,J.L.Weil,J.A.Baicker,L.J.Lidofsky)C129800100005
TITLE Neutron production from proton and deuteron C129800100006
bombardment of nickel C129800100007
FACILITY (VDG,1USACOL) C129800100008
INC-SOURCE Deuteron beam, calibrated with a Ra-Be neutron source C129800100009
DETECTOR (LONGC) Long counter C129800100010
SAMPLE Natural nickel foil targets with densities of C129800100011
2.33 mg/cm2 and 0.60 mg/cm2, backed by a thick C129800100012
(580 mg/cm2) gold beam stop, were used C129800100013
CORRECTION The cross sections have not been corrected for any C129800100014
energy dependence of the long counter because of the C129800100015
presence of several neutron groups of different C129800100016
energies. C129800100017
HISTORY (20050805C) DR C129800100018
(20120624A) SD: Title was added; BIB update. C129800100019
(20181104U) OS. Minor BIB corrections C129800100020
ENDBIB 18 0 C129800100021
COMMON 1 3 C129800100022
ANG C129800100023
ADEG C129800100024
0. C129800100025
ENDCOMMON 3 0 C129800100026
ENDSUBENT 25 0 C129800199999
SUBENT C1298002 20181107 C181C129800200001
BIB 3 4 C129800200002
REACTION (28-NI-0(D,N),,DA) C129800200003
ERR-ANALYS (DATA-ERR) No information on sources of uncertainties C129800200004
STATUS (TABLE) Data received on table from author, obtained C129800200005
from Fig.1 C129800200006
ENDBIB 4 0 C129800200007
COMMON 1 3 C129800200008
DATA-ERR C129800200009
PER-CENT C129800200010
40. C129800200011
ENDCOMMON 3 0 C129800200012
DATA 2 42 C129800200013
EN DATA C129800200014
MEV MB/SR C129800200015
1.095 0.016 C129800200016
1.190 0.048 C129800200017
1.310 0.088 C129800200018
1.540 0.016 C129800200019
1.650 0.032 C129800200020
1.690 0.016 C129800200021
1.755 0.016 C129800200022
1.890 0.024 C129800200023
1.990 0.032 C129800200024
2.090 0.088 C129800200025
2.215 0.184 C129800200026
2.275 0.152 C129800200027
2.355 0.216 C129800200028
2.420 0.200 C129800200029
2.510 0.416 C129800200030
2.585 0.320 C129800200031
2.745 0.272 C129800200032
2.855 0.336 C129800200033
2.950 0.656 C129800200034
3.045 0.496 C129800200035
3.150 0.520 C129800200036
3.260 0.832 C129800200037
3.360 0.776 C129800200038
3.470 1.27 C129800200039
3.560 1.19 C129800200040
3.670 1.62 C129800200041
3.750 1.70 C129800200042
3.860 2.04 C129800200043
3.960 2.66 C129800200044
4.075 2.55 C129800200045
4.180 2.73 C129800200046
4.275 3.12 C129800200047
4.380 3.42 C129800200048
4.485 4.00 C129800200049
4.590 4.16 C129800200050
4.700 5.22 C129800200051
4.820 5.46 C129800200052
4.900 5.93 C129800200053
5.005 7.06 C129800200054
5.120 6.68 C129800200055
5.235 7.27 C129800200056
5.305 7.57 C129800200057
ENDDATA 44 0 C129800200058
ENDSUBENT 57 0 C129800299999
SUBENT C1298003 20181107 C181C129800300001
BIB 3 4 C129800300002
REACTION (28-NI-0(P,N),,DA) C129800300003
ERR-ANALYS (DATA-ERR) No information on sources of uncertainties C129800300004
STATUS (TABLE) Data received on table from author, obtained C129800300005
from Fig.2 C129800300006
ENDBIB 4 0 C129800300007
COMMON 1 3 C129800300008
DATA-ERR C129800300009
PER-CENT C129800300010
40. C129800300011
ENDCOMMON 3 0 C129800300012
DATA 2 93 C129800300013
EN DATA C129800300014
MEV MB/SR C129800300015
1.550 0.0015 C129800300016
1.595 0.0015 C129800300017
1.670 0.0015 C129800300018
1.740 0.0015 C129800300019
1.820 0.0015 C129800300020
1.900 0.0135 C129800300021
1.975 0.0075 C129800300022
2.060 0.0045 C129800300023
2.145 0.0045 C129800300024
2.245 0.0060 C129800300025
2.315 0.0135 C129800300026
2.395 0.0150 C129800300027
2.500 0.0210 C129800300028
2.590 0.0315 C129800300029
2.665 0.0390 C129800300030
2.770 0.0405 C129800300031
2.870 0.0495 C129800300032
2.945 0.0450 C129800300033
3.045 0.0510 C129800300034
3.135 0.0630 C129800300035
3.235 0.0735 C129800300036
3.325 0.0870 C129800300037
3.395 0.113 C129800300038
3.430 0.0975 C129800300039
3.490 0.0780 C129800300040
3.555 0.0930 C129800300041
3.620 0.100 C129800300042
3.690 0.105 C129800300043
3.750 0.108 C129800300044
3.810 0.114 C129800300045
3.870 0.123 C129800300046
3.935 0.122 C129800300047
4.000 0.123 C129800300048
4.065 0.149 C129800300049
4.130 0.173 C129800300050
4.185 0.159 C129800300051
4.240 0.211 C129800300052
4.320 0.312 C129800300053
4.370 0.213 C129800300054
4.440 0.197 C129800300055
4.500 0.216 C129800300056
4.565 0.263 C129800300057
4.630 0.354 C129800300058
4.695 0.372 C129800300059
4.750 0.354 C129800300060
4.810 0.423 C129800300061
4.945 0.605 C129800300062
5.000 0.658 C129800300063
5.060 0.728 C129800300064
5.130 0.786 C129800300065
5.180 0.837 C129800300066
5.215 0.765 C129800300067
5.235 0.690 C129800300068
5.255 0.835 C129800300069
5.270 0.883 C129800300070
5.325 0.976 C129800300071
5.355 1.09 C129800300072
5.395 1.25 C129800300073
5.420 1.23 C129800300074
5.430 1.13 C129800300075
5.455 1.15 C129800300076
5.495 1.16 C129800300077
5.520 1.20 C129800300078
5.520 1.29 C129800300079
5.550 1.32 C129800300080
5.550 1.33 C129800300081
5.570 1.37 C129800300082
5.590 1.48 C129800300083
5.605 1.40 C129800300084
5.650 1.48 C129800300085
5.650 1.51 C129800300086
5.680 1.50 C129800300087
5.700 1.63 C129800300088
5.720 1.73 C129800300089
5.730 1.61 C129800300090
5.750 1.75 C129800300091
5.765 1.79 C129800300092
5.770 1.65 C129800300093
5.780 1.82 C129800300094
5.800 1.92 C129800300095
5.820 1.89 C129800300096
5.830 1.97 C129800300097
5.850 2.15 C129800300098
5.870 2.02 C129800300099
5.880 2.06 C129800300100
5.880 2.13 C129800300101
5.910 2.04 C129800300102
5.940 2.03 C129800300103
5.945 1.79 C129800300104
5.960 2.22 C129800300105
5.990 2.03 C129800300106
6.000 2.45 C129800300107
6.030 2.41 C129800300108
ENDDATA 95 0 C129800300109
ENDSUBENT 108 0 C129800399999
ENDENTRY 3 0 C129899999999