ENTRY M0315 20210620 M113M031500000001
SUBENT M0315001 20210620 M113M031500100001
BIB 10 26 M031500100002
TITLE Ground-state photoneutron angular distribution for M031500100003
N-14. M031500100004
AUTHOR (J.W.Jury,C.K.Ross,N.K.Sherman) M031500100005
INSTITUTE (1CANOTC) M031500100006
REFERENCE (J,NP/A,337,503,1980) M031500100007
#doi:10.1016/0375-9474(80)90156-6 M031500100008
FACILITY (LINAC,1CANOTC) M031500100009
SAMPLE 140 g of cyanoguanidine (NCNC(NH2)2) powder containing M031500100010
93 g of natural nitrogen in which the abundance of M031500100011
N-14 is 99.6%. This sample was contained in a hollow M031500100012
disk (diameter = 152 mm, thickness = 12 mm) of 0.13 M031500100013
mm thick plastic film. The sample was oriented at 15 M031500100014
degrees to the direction of the photon beam. M031500100015
METHOD (TOF) flight path = 10 m. M031500100016
DETECTOR (SCIN) Each of eight neutron detectors consisted of a M031500100017
25 mm thick NE104 plastic scintillator of diameter M031500100018
125 mm viewed by two Phillips xp1040 photomultiplier M031500100019
tubes. M031500100020
ERR-ANALYS (ERR-S) Statistical errors are presented. M031500100021
HISTORY (19881227C) Data were compiled at SCJAD of Saratov M031500100022
State University. M031500100023
(19910202A) Corrected by V.Varlamov, V.Mclane. M031500100024
(20130617A) Corrected by V.Varlamov: REACTION, M031500100025
STATUS, HISTORY, dates, lowercase. M031500100026
(20210620U) Corrected by SD and VV: AUTHOR, PART-DET, M031500100027
EN-SEC, small corrections in several SUBENTs. M031500100028
ENDBIB 26 0 M031500100029
NOCOMMON 0 0 M031500100030
ENDSUBENT 29 0 M031500199999
SUBENT M0315002 20210620 M113M031500200001
BIB 7 24 M031500200002
REACTION (7-N-14(G,X)0-NN-1,,DA/DE,,BRA/REL) M031500200003
Relative number of neutrons M031500200004
INC-SOURCE (BRST) M031500200005
CORRECTION The energy spectra were corrected for M031500200006
a) the dead time of detectors, M031500200007
b) the cosmic background, M031500200008
c) the background sample data, M031500200009
d) the neutron detection efficiency. M031500200010
ANALYSIS Each obtained laboratory-frame neutron energy M031500200011
spectrum was divided at each energy by the measured M031500200012
neutron detection efficiency and then converted to M031500200013
the c.m. frame. M031500200014
COMMENT Photoneutron energy spectra for end-point energies of M031500200015
20.5, 22.5, 24.5, 26.5 MeV were measured using M031500200016
time-of-flight techniques at eight angles from 48 to M031500200017
139 degrees in 13 degrees step. Ground-state angular M031500200018
distributions and (g,n0) cross sections were obtained M031500200019
from measured spectra. Coefficients of a Legendre M031500200020
polynomial fitted to the data were interpreted in M031500200021
terms of a simple single particle nuclear model. M031500200022
STATUS (CURVE) Data from Fig. 4 of Nucl.Phys.,A337(1980)503. M031500200023
HISTORY (20130617A) Corrected by V.Varlamov: BRS -> BRA. M031500200024
(20210620U) Corrected by SD and VV: STATUS, M031500200025
corrections in SUBENTs 010 and 011. M031500200026
ENDBIB 24 0 M031500200027
COMMON 1 3 M031500200028
EN-MAX M031500200029
MEV M031500200030
24.5 M031500200031
ENDCOMMON 3 0 M031500200032
DATA 4 136 M031500200033
ANG-CM E-CM DATA-CM ERR-S M031500200034
ADEG MEV ARB-UNITS ARB-UNITS M031500200035
48. 9.66 2.40 0.20 M031500200036
48. 9.84 2.56 0.20 M031500200037
48. 10.03 2.72 0.20 M031500200038
48. 10.21 2.80 0.20 M031500200039
48. 10.40 3.06 0.20 M031500200040
48. 10.59 3.36 0.28 M031500200041
48. 10.77 3.74 0.24 M031500200042
48. 10.96 3.92 0.28 M031500200043
48. 11.14 3.28 0.28 M031500200044
48. 11.33 2.98 0.24 M031500200045
48. 11.51 2.56 0.24 M031500200046
48. 11.70 2.06 0.20 M031500200047
48. 11.89 1.66 0.24 M031500200048
48. 12.07 0.90 0.18 M031500200049
48. 12.26 0.76 0.16 M031500200050
48. 12.44 0.40 0.12 M031500200051
48. 12.63 0.16 0.12 M031500200052
60. 9.66 2.38 0.20 M031500200053
60. 9.84 2.96 0.16 M031500200054
60. 10.03 3.10 0.20 M031500200055
60. 10.21 3.20 0.16 M031500200056
60. 10.40 3.44 0.16 M031500200057
60. 10.59 3.38 0.16 M031500200058
60. 10.77 3.72 0.16 M031500200059
60. 10.96 3.44 0.16 M031500200060
60. 11.14 3.28 0.16 M031500200061
60. 11.33 2.88 0.16 M031500200062
60. 11.51 2.60 0.18 M031500200063
60. 11.70 2.10 0.16 M031500200064
60. 11.89 1.36 0.14 M031500200065
60. 12.07 0.80 0.14 M031500200066
60. 12.26 0.68 0.12 M031500200067
60. 12.44 0.40 0.12 M031500200068
60. 12.63 0.16 0.12 M031500200069
72. 9.66 2.74 0.16 M031500200070
72. 9.84 2.72 0.16 M031500200071
72. 10.03 2.86 0.16 M031500200072
72. 10.21 2.50 0.18 M031500200073
72. 10.40 2.54 0.20 M031500200074
72. 10.59 2.72 0.20 M031500200075
72. 10.77 2.96 0.24 M031500200076
72. 10.96 2.64 0.16 M031500200077
72. 11.14 2.86 0.20 M031500200078
72. 11.33 2.86 0.18 M031500200079
72. 11.51 2.80 0.16 M031500200080
72. 11.70 2.42 0.18 M031500200081
72. 11.89 1.82 0.16 M031500200082
72. 12.07 1.36 0.18 M031500200083
72. 12.26 0.80 0.14 M031500200084
72. 12.44 0.60 0.12 M031500200085
72. 12.63 0.28 0.12 M031500200086
84. 9.66 3.02 0.18 M031500200087
84. 9.84 2.94 0.16 M031500200088
84. 10.03 3.04 0.16 M031500200089
84. 10.21 3.26 0.16 M031500200090
84. 10.40 3.10 0.18 M031500200091
84. 10.59 3.32 0.20 M031500200092
84. 10.77 3.66 0.20 M031500200093
84. 10.96 3.92 0.24 M031500200094
84. 11.14 4.00 0.24 M031500200095
84. 11.33 3.52 0.24 M031500200096
84. 11.51 2.78 0.18 M031500200097
84. 11.70 2.54 0.18 M031500200098
84. 11.89 1.94 0.18 M031500200099
84. 12.07 1.44 0.16 M031500200100
84. 12.26 1.14 0.14 M031500200101
84. 12.44 0.80 0.12 M031500200102
84. 12.63 0.40 0.12 M031500200103
97. 9.66 3.20 0.28 M031500200104
97. 9.84 2.78 0.24 M031500200105
97. 10.03 2.70 0.24 M031500200106
97. 10.21 3.28 0.24 M031500200107
97. 10.40 3.42 0.24 M031500200108
97. 10.59 3.35 0.24 M031500200109
97. 10.77 3.88 0.22 M031500200110
97. 10.96 3.92 0.22 M031500200111
97. 11.14 3.42 0.22 M031500200112
97. 11.33 3.00 0.24 M031500200113
97. 11.51 2.24 0.24 M031500200114
97. 11.70 1.84 0.22 M031500200115
97. 11.89 1.20 0.20 M031500200116
97. 12.07 1.08 0.18 M031500200117
97. 12.26 0.68 0.16 M031500200118
97. 12.44 0.55 0.12 M031500200119
97. 12.63 0.32 0.12 M031500200120
110. 9.66 2.86 0.24 M031500200121
110. 9.84 2.62 0.24 M031500200122
110. 10.03 2.46 0.24 M031500200123
110. 10.21 2.48 0.24 M031500200124
110. 10.40 2.66 0.22 M031500200125
110. 10.59 2.86 0.22 M031500200126
110. 10.77 3.10 0.24 M031500200127
110. 10.96 3.16 0.22 M031500200128
110. 11.14 3.02 0.24 M031500200129
110. 11.33 2.74 0.24 M031500200130
110. 11.51 2.68 0.24 M031500200131
110. 11.70 2.50 0.24 M031500200132
110. 11.89 1.71 0.20 M031500200133
110. 12.07 1.12 0.20 M031500200134
110. 12.26 0.74 0.14 M031500200135
110. 12.44 0.48 0.12 M031500200136
110. 12.63 0.32 0.12 M031500200137
124. 9.66 2.74 0.24 M031500200138
124. 9.84 2.36 0.24 M031500200139
124. 10.03 1.94 0.20 M031500200140
124. 10.21 1.84 0.20 M031500200141
124. 10.40 1.98 0.18 M031500200142
124. 10.59 2.54 0.18 M031500200143
124. 10.77 2.78 0.22 M031500200144
124. 10.96 2.64 0.24 M031500200145
124. 11.14 2.74 0.22 M031500200146
124. 11.33 2.72 0.22 M031500200147
124. 11.51 2.10 0.22 M031500200148
124. 11.70 1.80 0.20 M031500200149
124. 11.89 1.36 0.18 M031500200150
124. 12.07 0.94 0.16 M031500200151
124. 12.26 0.54 0.14 M031500200152
124. 12.44 0.41 0.12 M031500200153
124. 12.63 0.28 0.12 M031500200154
138. 9.66 2.14 0.22 M031500200155
138. 9.84 1.90 0.20 M031500200156
138. 10.03 1.74 0.20 M031500200157
138. 10.21 2.08 0.18 M031500200158
138. 10.40 2.04 0.18 M031500200159
138. 10.59 2.06 0.16 M031500200160
138. 10.77 2.32 0.18 M031500200161
138. 10.96 2.29 0.16 M031500200162
138. 11.14 2.02 0.18 M031500200163
138. 11.33 1.84 0.16 M031500200164
138. 11.51 1.42 0.16 M031500200165
138. 11.70 1.04 0.14 M031500200166
138. 11.89 0.80 0.12 M031500200167
138. 12.07 0.56 0.12 M031500200168
138. 12.26 0.32 0.12 M031500200169
138. 12.44 0.12 0.12 M031500200170
138. 12.63 0.00 0.12 M031500200171
ENDDATA 138 0 M031500200172
ENDSUBENT 171 0 M031500299999
NOSUBENT M0315003 19910610 0000M031500300001
NOSUBENT M0315004 19910610 0000M031500400001
NOSUBENT M0315005 19910610 0000M031500500001
NOSUBENT M0315006 19910610 0000M031500600001
NOSUBENT M0315007 19910610 0000M031500700001
NOSUBENT M0315008 19910610 0000M031500800001
NOSUBENT M0315009 19910610 0000M031500900001
SUBENT M0315010 20210620 M113M031501000001
BIB 12 57 M031501000002
REACTION (7-N-14(G,N)7-N-13,PAR,SIG) M031501000003
INC-SOURCE (KINDT) M031501000004
MONITOR The scale of the cross section was determined M031501000005
relative to the value of the deuterium cross section, M031501000006
as calculated by Partovi and confirmed experimentally M031501000007
by Ahrens et al. M031501000008
MONIT-REF (,F.Partovi,J,AP,27,79,1964) M031501000009
(,J.Ahrens+,J,PL/B,52,49,1974) M031501000010
CORRECTION The ground-state data were corrected for the M031501000011
bremsstrahlung spectra. M031501000012
ASSUMED Only neutrons of the highest 3.5 MeV wide region near M031501000013
the tip of each spectrum represent purely M031501000014
ground-state transition because the transitions to M031501000015
the first excited state of N-13 at 2.36 MeV are M031501000016
negligible. M031501000017
ANALYSIS The ground-state data have been obtained by M031501000018
fitting of a series of Legendre polynomials to the M031501000019
eight highest 3.5 MeV regions of neutron spectra for M031501000020
each end-point measurement. The zero order M031501000021
coefficient of this series has been corrected by M031501000022
division by the photon distribution shape and has M031501000023
been represented as the total ground-state cross M031501000024
section. M031501000025
ADD-RES The ground-state data were compared with the results M031501000026
of measurement of cross-sections for N-14(g,p0) and M031501000027
C-13(g,p0) reaction. M031501000028
REL-REF (A,,J.E.E.Baglin+,J,PR/C,10,24,1974) The result of M031501000029
measurement of N-14(g,p0) cross section. M031501000030
(N,,H.R.Kissener+,J,NP/A,207,78,1973) The shell model M031501000031
with intermediate coupling was used to compute the M031501000032
cross section for the N-14(g,n0) reaction. M031501000033
(N,,J.D.Vergados,J,NP/A,239,271,1975) The total M031501000034
photon absorption strengths calculation. M031501000035
COMMENT For reactions to the ground state in N-13, it appears M031501000036
that most of the photon absorption in the giant M031501000037
resonance region studied forms 2- states in N-14, M031501000038
which are decayed by d-wave neutron emission. Some M031501000039
evidence was found for the existence of 0- strength M031501000040
at about 22.5 MeV (the peak of the cross section). M031501000041
The results are in general consistent with an M031501000042
identification of the (g,n0) process with the M031501000043
promotion of a p1/2 neutron to the s-d shell. Little M031501000044
or no E2 or M1 absorption was observed. Comparison M031501000045
with photoproton measurement shows some evidence for M031501000046
a small amount of isospin t = 0 mixing also near M031501000047
22.5 MeV. The results of the experiment have yielded aM031501000048
cross section which represents only a small fraction M031501000049
(17%) of the possible neutron-producing decays from M031501000050
the giant resonance of N-14. Comparison with M031501000051
calculations of the ground-state cross section shows M031501000052
reasonable agreement if the theoretical results are M031501000053
displaced upwards in energy of about 1 MeV. M031501000054
STATUS (CURVE) Data from Fig. 5 of Nucl.Phys.,A337(1980)503. M031501000055
(COREL,M0315011) Legendre coeff. M031501000056
HISTORY (20130617A) Corrected by V.Varlamov: BRA -> BRS. M031501000057
(20210620U) Corrected by SD and VV: EN-SEC deleted, M031501000058
REACTION, ANALYSIS, STATUS. M031501000059
ENDBIB 57 0 M031501000060
COMMON 1 3 M031501000061
E-LVL M031501000062
MEV M031501000063
0.0 M031501000064
ENDCOMMON 3 0 M031501000065
DATA 3 46 M031501000066
EN DATA ERR-S M031501000067
MEV MB MB M031501000068
17.2 0.31 0.05 M031501000069
17.4 0.36 0.05 M031501000070
17.6 0.40 0.05 M031501000071
17.8 0.44 0.05 M031501000072
18.0 0.60 0.06 M031501000073
18.2 0.77 0.06 M031501000074
18.4 0.98 0.06 M031501000075
18.6 1.14 0.06 M031501000076
18.8 1.16 0.06 M031501000077
19.0 1.26 0.06 M031501000078
19.2 1.31 0.06 M031501000079
19.4 1.30 0.06 M031501000080
19.6 1.27 0.06 M031501000081
19.8 1.26 0.06 M031501000082
20.0 1.31 0.06 M031501000083
20.2 1.36 0.06 M031501000084
20.4 1.48 0.07 M031501000085
20.6 1.59 0.10 M031501000086
20.8 1.58 0.11 M031501000087
21.0 1.48 0.09 M031501000088
21.2 1.27 0.10 M031501000089
21.4 1.18 0.09 M031501000090
21.6 1.28 0.09 M031501000091
21.8 1.48 0.10 M031501000092
22.0 1.72 0.11 M031501000093
22.2 2.02 0.11 M031501000094
22.4 2.21 0.10 M031501000095
22.6 2.22 0.11 M031501000096
22.8 2.31 0.13 M031501000097
23.0 2.29 0.12 M031501000098
23.2 2.20 0.11 M031501000099
23.4 1.90 0.13 M031501000100
23.6 1.50 0.11 M031501000101
23.8 1.32 0.11 M031501000102
24.0 1.19 0.11 M031501000103
24.2 1.17 0.10 M031501000104
24.4 1.15 0.11 M031501000105
24.6 1.15 0.10 M031501000106
24.8 1.11 0.11 M031501000107
25.0 0.94 0.12 M031501000108
25.2 0.80 0.11 M031501000109
25.4 0.80 0.11 M031501000110
25.6 0.72 0.11 M031501000111
25.8 0.60 0.11 M031501000112
26.0 0.51 0.09 M031501000113
26.2 0.55 0.11 M031501000114
ENDDATA 48 0 M031501000115
ENDSUBENT 114 0 M031501099999
SUBENT M0315011 20210620 M113M031501100001
BIB 10 40 M031501100002
REACTION (7-N-14(G,N)7-N-13,PAR,DA,,LEG/RS) M031501100003
INC-SOURCE (KINDT) M031501100004
CORRECTION The ground-state data were corrected for the M031501100005
bremsstrahlung spectra. M031501100006
ASSUMED Only neutrons of the highest 3.5 MeV wide region near M031501100007
the tip of each spectrum represent purely M031501100008
ground-state transition because the transitions to M031501100009
the first excited state of N-13 at 2.36 MeV are M031501100010
negligible. M031501100011
ANALYSIS The ground-state data have been obtained by M031501100012
fitting of a series of Legendre polynomials to the M031501100013
eight highest 3.5 MeV regions of neutron spectra for M031501100014
each end-point measurement. The zero order M031501100015
coefficient of this series has been corrected by M031501100016
division by the photon distribution shape and has M031501100017
been represented as the total ground-state cross M031501100018
section. M031501100019
ADD-RES The ground-state data were compared with the results M031501100020
of measurement of cross-sections for N-14(g,p0) and M031501100021
C-13(g,p0) reactions. M031501100022
REL-REF (A,,J.E.E.Baglin+,J,PR/C,10,24,1974) The result of M031501100023
measurement of N-14(g,p0) cross section. M031501100024
COMMENT For reactions to the ground state in N-13, it appears M031501100025
that most of the photon absorption in the giant M031501100026
resonance region studied forms 2- states in N-14, M031501100027
which are decayed by d-wave neutron emission. Some M031501100028
evidence was found for the existence of 0- strength M031501100029
at about 22.5 MeV (the peak of the cross section). M031501100030
The results are in general consistent with an M031501100031
identification of the (g,n0) process with the M031501100032
promotion of a p1/2 neutron to the s-d shell. Little M031501100033
or no E2 or M1 absorption was observed. Comparison M031501100034
with photoproton measurement shows some evidence for M031501100035
a small amount of isospin t=0 mixing also near 22.5 M031501100036
MeV. M031501100037
STATUS (CURVE) Fig.5 from Nucl.Phys.,A337(1980)503. M031501100038
(COREL,M0315010) Cross set. 4Pi x A0. M031501100039
HISTORY (20130617A) Corrected by V.Varlamov: BRA -> BRS. M031501100040
(20210620U) Corrected by SD and VV: EN-SEC deleted, M031501100041
REACTION, ANALYSIS, STATUS. M031501100042
ENDBIB 40 0 M031501100043
COMMON 1 3 M031501100044
E-LVL M031501100045
MEV M031501100046
0.0 M031501100047
ENDCOMMON 3 0 M031501100048
DATA 4 115 M031501100049
NUMBER EN DATA ERR-S M031501100050
NO-DIM MEV NO-DIM NO-DIM M031501100051
1. 18.2 -0.33 0.31 M031501100052
1. 18.4 0.05 0.14 M031501100053
1. 18.6 -0.05 0.13 M031501100054
1. 18.8 -0.16 0.13 M031501100055
1. 19.0 -0.10 0.13 M031501100056
1. 19.2 -0.04 0.13 M031501100057
1. 19.4 0.10 0.13 M031501100058
1. 19.6 0.09 0.13 M031501100059
1. 19.8 0.24 0.14 M031501100060
1. 20.0 0.24 0.14 M031501100061
1. 20.2 -0.08 0.15 M031501100062
1. 20.4 0.05 0.14 M031501100063
1. 20.6 0.20 0.13 M031501100064
1. 20.8 0.12 0.13 M031501100065
1. 21.0 0.10 0.13 M031501100066
1. 21.2 0.15 0.13 M031501100067
1. 21.4 0.10 0.13 M031501100068
1. 21.6 0.13 0.14 M031501100069
1. 21.8 0.31 0.13 M031501100070
1. 22.0 0.17 0.14 M031501100071
1. 22.2 0.40 0.13 M031501100072
1. 22.4 0.40 0.14 M031501100073
1. 22.6 0.31 0.13 M031501100074
1. 22.8 0.25 0.14 M031501100075
1. 23.0 0.31 0.14 M031501100076
1. 23.2 0.31 0.11 M031501100077
1. 23.4 0.26 0.14 M031501100078
1. 23.6 0.00 0.14 M031501100079
1. 23.8 0.14 0.13 M031501100080
1. 24.0 0.21 0.14 M031501100081
1. 24.2 0.26 0.13 M031501100082
1. 24.4 0.36 0.13 M031501100083
1. 24.6 0.30 0.13 M031501100084
1. 24.8 0.27 0.15 M031501100085
1. 25.0 0.17 0.15 M031501100086
1. 25.2 0.14 0.18 M031501100087
1. 25.4 0.48 0.18 M031501100088
1. 25.6 0.16 0.19 M031501100089
1. 25.8 0.06 0.20 M031501100090
2. 18.2 -0.70 0.20 M031501100091
2. 18.4 -0.83 0.18 M031501100092
2. 18.6 -0.76 0.17 M031501100093
2. 18.8 -0.78 0.15 M031501100094
2. 19.0 -0.70 0.15 M031501100095
2. 19.2 -0.85 0.15 M031501100096
2. 19.4 -0.60 0.14 M031501100097
2. 19.6 -0.57 0.15 M031501100098
2. 19.8 -0.63 0.17 M031501100099
2. 20.0 -0.75 0.15 M031501100100
2. 20.2 -0.80 0.15 M031501100101
2. 20.4 -0.63 0.17 M031501100102
2. 20.6 -0.41 0.11 M031501100103
2. 20.8 -0.45 0.17 M031501100104
2. 21.0 -0.35 0.17 M031501100105
2. 21.2 -0.42 0.19 M031501100106
2. 21.4 -0.51 0.18 M031501100107
2. 21.6 -0.55 0.17 M031501100108
2. 21.8 -0.23 0.18 M031501100109
2. 22.0 -0.39 0.15 M031501100110
2. 22.2 -0.14 0.15 M031501100111
2. 22.4 -0.10 0.14 M031501100112
2. 22.6 -0.33 0.15 M031501100113
2. 22.8 -0.36 0.13 M031501100114
2. 23.0 -0.36 0.15 M031501100115
2. 23.2 -0.54 0.14 M031501100116
2. 23.4 -0.49 0.15 M031501100117
2. 23.6 -1.00 0.15 M031501100118
2. 23.8 -0.97 0.14 M031501100119
2. 24.0 -0.63 0.15 M031501100120
2. 24.2 -0.71 0.18 M031501100121
2. 24.4 -0.60 0.18 M031501100122
2. 24.6 -0.57 0.18 M031501100123
2. 24.8 -0.59 0.19 M031501100124
2. 25.0 -0.75 0.19 M031501100125
2. 25.2 -0.88 0.20 M031501100126
2. 25.4 -0.55 0.19 M031501100127
2. 25.6 -0.90 0.18 M031501100128
3. 18.2 -0.11 0.24 M031501100129
3. 18.4 0.09 0.20 M031501100130
3. 18.6 -0.04 0.20 M031501100131
3. 18.8 -0.06 0.18 M031501100132
3. 19.0 -0.07 0.18 M031501100133
3. 19.2 -0.04 0.18 M031501100134
3. 19.4 0.15 0.18 M031501100135
3. 19.6 0.18 0.17 M031501100136
3. 19.8 0.31 0.18 M031501100137
3. 20.0 0.08 0.18 M031501100138
3. 20.2 -0.20 0.19 M031501100139
3. 20.4 0.19 0.19 M031501100140
3. 20.6 0.37 0.18 M031501100141
3. 20.8 0.36 0.19 M031501100142
3. 21.0 0.20 0.18 M031501100143
3. 21.2 0.06 0.18 M031501100144
3. 21.4 -0.05 0.15 M031501100145
3. 21.6 0.02 0.15 M031501100146
3. 21.8 0.15 0.17 M031501100147
3. 22.0 -0.09 0.15 M031501100148
3. 22.2 0.15 0.17 M031501100149
3. 22.4 0.26 0.17 M031501100150
3. 22.6 0.20 0.18 M031501100151
3. 22.8 0.14 0.15 M031501100152
3. 23.0 0.13 0.15 M031501100153
3. 23.2 0.17 0.15 M031501100154
3. 23.4 0.07 0.15 M031501100155
3. 23.6 0.04 0.15 M031501100156
3. 23.8 0.08 0.15 M031501100157
3. 24.0 0.02 0.17 M031501100158
3. 24.2 -0.08 0.15 M031501100159
3. 24.4 0.00 0.17 M031501100160
3. 24.6 0.01 0.15 M031501100161
3. 24.8 0.04 0.19 M031501100162
3. 25.0 -0.11 0.18 M031501100163
3. 25.2 -0.26 0.17 M031501100164
3. 25.4 0.10 0.20 M031501100165
3. 25.6 0.00 0.23 M031501100166
ENDDATA 117 0 M031501100167
ENDSUBENT 166 0 M031501199999
NOSUBENT M0315012 19910610 0000M031501200001
NOSUBENT M0315013 19910610 0000M031501300001
ENDENTRY 13 0 M031599999999