ENTRY M0315 20210620 M113M0315 0 1 SUBENT M0315001 20210620 M113M0315 1 1 BIB 10 26 M0315 1 2 TITLE Ground-state photoneutron angular distribution for M0315 1 3 N-14. M0315 1 4 AUTHOR (J.W.Jury,C.K.Ross,N.K.Sherman) M0315 1 5 INSTITUTE (1CANOTC) M0315 1 6 REFERENCE (J,NP/A,337,503,1980) M0315 1 7 #doi:10.1016/0375-9474(80)90156-6 M0315 1 8 FACILITY (LINAC,1CANOTC) M0315 1 9 SAMPLE 140 g of cyanoguanidine (NCNC(NH2)2) powder containing M0315 1 10 93 g of natural nitrogen in which the abundance of M0315 1 11 N-14 is 99.6%. This sample was contained in a hollow M0315 1 12 disk (diameter = 152 mm, thickness = 12 mm) of 0.13 M0315 1 13 mm thick plastic film. The sample was oriented at 15 M0315 1 14 degrees to the direction of the photon beam. M0315 1 15 METHOD (TOF) flight path = 10 m. M0315 1 16 DETECTOR (SCIN) Each of eight neutron detectors consisted of a M0315 1 17 25 mm thick NE104 plastic scintillator of diameter M0315 1 18 125 mm viewed by two Phillips xp1040 photomultiplier M0315 1 19 tubes. M0315 1 20 ERR-ANALYS (ERR-S) Statistical errors are presented. M0315 1 21 HISTORY (19881227C) Data were compiled at SCJAD of Saratov M0315 1 22 State University. M0315 1 23 (19910202A) Corrected by V.Varlamov, V.Mclane. M0315 1 24 (20130617A) Corrected by V.Varlamov: REACTION, M0315 1 25 STATUS, HISTORY, dates, lowercase. M0315 1 26 (20210620U) Corrected by SD and VV: AUTHOR, PART-DET, M0315 1 27 EN-SEC, small corrections in several SUBENTs. M0315 1 28 ENDBIB 26 0 M0315 1 29 NOCOMMON 0 0 M0315 1 30 ENDSUBENT 29 0 M0315 199999 SUBENT M0315002 20210620 M113M0315 2 1 BIB 7 24 M0315 2 2 REACTION (7-N-14(G,X)0-NN-1,,DA/DE,,BRA/REL) M0315 2 3 Relative number of neutrons M0315 2 4 INC-SOURCE (BRST) M0315 2 5 CORRECTION The energy spectra were corrected for M0315 2 6 a) the dead time of detectors, M0315 2 7 b) the cosmic background, M0315 2 8 c) the background sample data, M0315 2 9 d) the neutron detection efficiency. M0315 2 10 ANALYSIS Each obtained laboratory-frame neutron energy M0315 2 11 spectrum was divided at each energy by the measured M0315 2 12 neutron detection efficiency and then converted to M0315 2 13 the c.m. frame. M0315 2 14 COMMENT Photoneutron energy spectra for end-point energies of M0315 2 15 20.5, 22.5, 24.5, 26.5 MeV were measured using M0315 2 16 time-of-flight techniques at eight angles from 48 to M0315 2 17 139 degrees in 13 degrees step. Ground-state angular M0315 2 18 distributions and (g,n0) cross sections were obtained M0315 2 19 from measured spectra. Coefficients of a Legendre M0315 2 20 polynomial fitted to the data were interpreted in M0315 2 21 terms of a simple single particle nuclear model. M0315 2 22 STATUS (CURVE) Data from Fig. 4 of Nucl.Phys.,A337(1980)503. M0315 2 23 HISTORY (20130617A) Corrected by V.Varlamov: BRS -> BRA. M0315 2 24 (20210620U) Corrected by SD and VV: STATUS, M0315 2 25 corrections in SUBENTs 010 and 011. M0315 2 26 ENDBIB 24 0 M0315 2 27 COMMON 1 3 M0315 2 28 EN-MAX M0315 2 29 MEV M0315 2 30 24.5 M0315 2 31 ENDCOMMON 3 0 M0315 2 32 DATA 4 136 M0315 2 33 ANG-CM E-CM DATA-CM ERR-S M0315 2 34 ADEG MEV ARB-UNITS ARB-UNITS M0315 2 35 48. 9.66 2.40 0.20 M0315 2 36 48. 9.84 2.56 0.20 M0315 2 37 48. 10.03 2.72 0.20 M0315 2 38 48. 10.21 2.80 0.20 M0315 2 39 48. 10.40 3.06 0.20 M0315 2 40 48. 10.59 3.36 0.28 M0315 2 41 48. 10.77 3.74 0.24 M0315 2 42 48. 10.96 3.92 0.28 M0315 2 43 48. 11.14 3.28 0.28 M0315 2 44 48. 11.33 2.98 0.24 M0315 2 45 48. 11.51 2.56 0.24 M0315 2 46 48. 11.70 2.06 0.20 M0315 2 47 48. 11.89 1.66 0.24 M0315 2 48 48. 12.07 0.90 0.18 M0315 2 49 48. 12.26 0.76 0.16 M0315 2 50 48. 12.44 0.40 0.12 M0315 2 51 48. 12.63 0.16 0.12 M0315 2 52 60. 9.66 2.38 0.20 M0315 2 53 60. 9.84 2.96 0.16 M0315 2 54 60. 10.03 3.10 0.20 M0315 2 55 60. 10.21 3.20 0.16 M0315 2 56 60. 10.40 3.44 0.16 M0315 2 57 60. 10.59 3.38 0.16 M0315 2 58 60. 10.77 3.72 0.16 M0315 2 59 60. 10.96 3.44 0.16 M0315 2 60 60. 11.14 3.28 0.16 M0315 2 61 60. 11.33 2.88 0.16 M0315 2 62 60. 11.51 2.60 0.18 M0315 2 63 60. 11.70 2.10 0.16 M0315 2 64 60. 11.89 1.36 0.14 M0315 2 65 60. 12.07 0.80 0.14 M0315 2 66 60. 12.26 0.68 0.12 M0315 2 67 60. 12.44 0.40 0.12 M0315 2 68 60. 12.63 0.16 0.12 M0315 2 69 72. 9.66 2.74 0.16 M0315 2 70 72. 9.84 2.72 0.16 M0315 2 71 72. 10.03 2.86 0.16 M0315 2 72 72. 10.21 2.50 0.18 M0315 2 73 72. 10.40 2.54 0.20 M0315 2 74 72. 10.59 2.72 0.20 M0315 2 75 72. 10.77 2.96 0.24 M0315 2 76 72. 10.96 2.64 0.16 M0315 2 77 72. 11.14 2.86 0.20 M0315 2 78 72. 11.33 2.86 0.18 M0315 2 79 72. 11.51 2.80 0.16 M0315 2 80 72. 11.70 2.42 0.18 M0315 2 81 72. 11.89 1.82 0.16 M0315 2 82 72. 12.07 1.36 0.18 M0315 2 83 72. 12.26 0.80 0.14 M0315 2 84 72. 12.44 0.60 0.12 M0315 2 85 72. 12.63 0.28 0.12 M0315 2 86 84. 9.66 3.02 0.18 M0315 2 87 84. 9.84 2.94 0.16 M0315 2 88 84. 10.03 3.04 0.16 M0315 2 89 84. 10.21 3.26 0.16 M0315 2 90 84. 10.40 3.10 0.18 M0315 2 91 84. 10.59 3.32 0.20 M0315 2 92 84. 10.77 3.66 0.20 M0315 2 93 84. 10.96 3.92 0.24 M0315 2 94 84. 11.14 4.00 0.24 M0315 2 95 84. 11.33 3.52 0.24 M0315 2 96 84. 11.51 2.78 0.18 M0315 2 97 84. 11.70 2.54 0.18 M0315 2 98 84. 11.89 1.94 0.18 M0315 2 99 84. 12.07 1.44 0.16 M0315 2 100 84. 12.26 1.14 0.14 M0315 2 101 84. 12.44 0.80 0.12 M0315 2 102 84. 12.63 0.40 0.12 M0315 2 103 97. 9.66 3.20 0.28 M0315 2 104 97. 9.84 2.78 0.24 M0315 2 105 97. 10.03 2.70 0.24 M0315 2 106 97. 10.21 3.28 0.24 M0315 2 107 97. 10.40 3.42 0.24 M0315 2 108 97. 10.59 3.35 0.24 M0315 2 109 97. 10.77 3.88 0.22 M0315 2 110 97. 10.96 3.92 0.22 M0315 2 111 97. 11.14 3.42 0.22 M0315 2 112 97. 11.33 3.00 0.24 M0315 2 113 97. 11.51 2.24 0.24 M0315 2 114 97. 11.70 1.84 0.22 M0315 2 115 97. 11.89 1.20 0.20 M0315 2 116 97. 12.07 1.08 0.18 M0315 2 117 97. 12.26 0.68 0.16 M0315 2 118 97. 12.44 0.55 0.12 M0315 2 119 97. 12.63 0.32 0.12 M0315 2 120 110. 9.66 2.86 0.24 M0315 2 121 110. 9.84 2.62 0.24 M0315 2 122 110. 10.03 2.46 0.24 M0315 2 123 110. 10.21 2.48 0.24 M0315 2 124 110. 10.40 2.66 0.22 M0315 2 125 110. 10.59 2.86 0.22 M0315 2 126 110. 10.77 3.10 0.24 M0315 2 127 110. 10.96 3.16 0.22 M0315 2 128 110. 11.14 3.02 0.24 M0315 2 129 110. 11.33 2.74 0.24 M0315 2 130 110. 11.51 2.68 0.24 M0315 2 131 110. 11.70 2.50 0.24 M0315 2 132 110. 11.89 1.71 0.20 M0315 2 133 110. 12.07 1.12 0.20 M0315 2 134 110. 12.26 0.74 0.14 M0315 2 135 110. 12.44 0.48 0.12 M0315 2 136 110. 12.63 0.32 0.12 M0315 2 137 124. 9.66 2.74 0.24 M0315 2 138 124. 9.84 2.36 0.24 M0315 2 139 124. 10.03 1.94 0.20 M0315 2 140 124. 10.21 1.84 0.20 M0315 2 141 124. 10.40 1.98 0.18 M0315 2 142 124. 10.59 2.54 0.18 M0315 2 143 124. 10.77 2.78 0.22 M0315 2 144 124. 10.96 2.64 0.24 M0315 2 145 124. 11.14 2.74 0.22 M0315 2 146 124. 11.33 2.72 0.22 M0315 2 147 124. 11.51 2.10 0.22 M0315 2 148 124. 11.70 1.80 0.20 M0315 2 149 124. 11.89 1.36 0.18 M0315 2 150 124. 12.07 0.94 0.16 M0315 2 151 124. 12.26 0.54 0.14 M0315 2 152 124. 12.44 0.41 0.12 M0315 2 153 124. 12.63 0.28 0.12 M0315 2 154 138. 9.66 2.14 0.22 M0315 2 155 138. 9.84 1.90 0.20 M0315 2 156 138. 10.03 1.74 0.20 M0315 2 157 138. 10.21 2.08 0.18 M0315 2 158 138. 10.40 2.04 0.18 M0315 2 159 138. 10.59 2.06 0.16 M0315 2 160 138. 10.77 2.32 0.18 M0315 2 161 138. 10.96 2.29 0.16 M0315 2 162 138. 11.14 2.02 0.18 M0315 2 163 138. 11.33 1.84 0.16 M0315 2 164 138. 11.51 1.42 0.16 M0315 2 165 138. 11.70 1.04 0.14 M0315 2 166 138. 11.89 0.80 0.12 M0315 2 167 138. 12.07 0.56 0.12 M0315 2 168 138. 12.26 0.32 0.12 M0315 2 169 138. 12.44 0.12 0.12 M0315 2 170 138. 12.63 0.00 0.12 M0315 2 171 ENDDATA 138 0 M0315 2 172 ENDSUBENT 171 0 M0315 299999 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 M113M0315 10 1 BIB 12 57 M0315 10 2 REACTION (7-N-14(G,N)7-N-13,PAR,SIG) M0315 10 3 INC-SOURCE (KINDT) M0315 10 4 MONITOR The scale of the cross section was determined M0315 10 5 relative to the value of the deuterium cross section, M0315 10 6 as calculated by Partovi and confirmed experimentally M0315 10 7 by Ahrens et al. M0315 10 8 MONIT-REF (,F.Partovi,J,AP,27,79,1964) M0315 10 9 (,J.Ahrens+,J,PL/B,52,49,1974) M0315 10 10 CORRECTION The ground-state data were corrected for the M0315 10 11 bremsstrahlung spectra. M0315 10 12 ASSUMED Only neutrons of the highest 3.5 MeV wide region near M0315 10 13 the tip of each spectrum represent purely M0315 10 14 ground-state transition because the transitions to M0315 10 15 the first excited state of N-13 at 2.36 MeV are M0315 10 16 negligible. M0315 10 17 ANALYSIS The ground-state data have been obtained by M0315 10 18 fitting of a series of Legendre polynomials to the M0315 10 19 eight highest 3.5 MeV regions of neutron spectra for M0315 10 20 each end-point measurement. The zero order M0315 10 21 coefficient of this series has been corrected by M0315 10 22 division by the photon distribution shape and has M0315 10 23 been represented as the total ground-state cross M0315 10 24 section. M0315 10 25 ADD-RES The ground-state data were compared with the results M0315 10 26 of measurement of cross-sections for N-14(g,p0) and M0315 10 27 C-13(g,p0) reaction. M0315 10 28 REL-REF (A,,J.E.E.Baglin+,J,PR/C,10,24,1974) The result of M0315 10 29 measurement of N-14(g,p0) cross section. M0315 10 30 (N,,H.R.Kissener+,J,NP/A,207,78,1973) The shell model M0315 10 31 with intermediate coupling was used to compute the M0315 10 32 cross section for the N-14(g,n0) reaction. M0315 10 33 (N,,J.D.Vergados,J,NP/A,239,271,1975) The total M0315 10 34 photon absorption strengths calculation. M0315 10 35 COMMENT For reactions to the ground state in N-13, it appears M0315 10 36 that most of the photon absorption in the giant M0315 10 37 resonance region studied forms 2- states in N-14, M0315 10 38 which are decayed by d-wave neutron emission. Some M0315 10 39 evidence was found for the existence of 0- strength M0315 10 40 at about 22.5 MeV (the peak of the cross section). M0315 10 41 The results are in general consistent with an M0315 10 42 identification of the (g,n0) process with the M0315 10 43 promotion of a p1/2 neutron to the s-d shell. Little M0315 10 44 or no E2 or M1 absorption was observed. Comparison M0315 10 45 with photoproton measurement shows some evidence for M0315 10 46 a small amount of isospin t = 0 mixing also near M0315 10 47 22.5 MeV. The results of the experiment have yielded aM0315 10 48 cross section which represents only a small fraction M0315 10 49 (17%) of the possible neutron-producing decays from M0315 10 50 the giant resonance of N-14. Comparison with M0315 10 51 calculations of the ground-state cross section shows M0315 10 52 reasonable agreement if the theoretical results are M0315 10 53 displaced upwards in energy of about 1 MeV. M0315 10 54 STATUS (CURVE) Data from Fig. 5 of Nucl.Phys.,A337(1980)503. M0315 10 55 (COREL,M0315011) Legendre coeff. M0315 10 56 HISTORY (20130617A) Corrected by V.Varlamov: BRA -> BRS. M0315 10 57 (20210620U) Corrected by SD and VV: EN-SEC deleted, M0315 10 58 REACTION, ANALYSIS, STATUS. M0315 10 59 ENDBIB 57 0 M0315 10 60 COMMON 1 3 M0315 10 61 E-LVL M0315 10 62 MEV M0315 10 63 0.0 M0315 10 64 ENDCOMMON 3 0 M0315 10 65 DATA 3 46 M0315 10 66 EN DATA ERR-S M0315 10 67 MEV MB MB M0315 10 68 17.2 0.31 0.05 M0315 10 69 17.4 0.36 0.05 M0315 10 70 17.6 0.40 0.05 M0315 10 71 17.8 0.44 0.05 M0315 10 72 18.0 0.60 0.06 M0315 10 73 18.2 0.77 0.06 M0315 10 74 18.4 0.98 0.06 M0315 10 75 18.6 1.14 0.06 M0315 10 76 18.8 1.16 0.06 M0315 10 77 19.0 1.26 0.06 M0315 10 78 19.2 1.31 0.06 M0315 10 79 19.4 1.30 0.06 M0315 10 80 19.6 1.27 0.06 M0315 10 81 19.8 1.26 0.06 M0315 10 82 20.0 1.31 0.06 M0315 10 83 20.2 1.36 0.06 M0315 10 84 20.4 1.48 0.07 M0315 10 85 20.6 1.59 0.10 M0315 10 86 20.8 1.58 0.11 M0315 10 87 21.0 1.48 0.09 M0315 10 88 21.2 1.27 0.10 M0315 10 89 21.4 1.18 0.09 M0315 10 90 21.6 1.28 0.09 M0315 10 91 21.8 1.48 0.10 M0315 10 92 22.0 1.72 0.11 M0315 10 93 22.2 2.02 0.11 M0315 10 94 22.4 2.21 0.10 M0315 10 95 22.6 2.22 0.11 M0315 10 96 22.8 2.31 0.13 M0315 10 97 23.0 2.29 0.12 M0315 10 98 23.2 2.20 0.11 M0315 10 99 23.4 1.90 0.13 M0315 10 100 23.6 1.50 0.11 M0315 10 101 23.8 1.32 0.11 M0315 10 102 24.0 1.19 0.11 M0315 10 103 24.2 1.17 0.10 M0315 10 104 24.4 1.15 0.11 M0315 10 105 24.6 1.15 0.10 M0315 10 106 24.8 1.11 0.11 M0315 10 107 25.0 0.94 0.12 M0315 10 108 25.2 0.80 0.11 M0315 10 109 25.4 0.80 0.11 M0315 10 110 25.6 0.72 0.11 M0315 10 111 25.8 0.60 0.11 M0315 10 112 26.0 0.51 0.09 M0315 10 113 26.2 0.55 0.11 M0315 10 114 ENDDATA 48 0 M0315 10 115 ENDSUBENT 114 0 M0315 1099999 SUBENT M0315011 20210620 M113M0315 11 1 BIB 10 40 M0315 11 2 REACTION (7-N-14(G,N)7-N-13,PAR,DA,,LEG/RS) M0315 11 3 INC-SOURCE (KINDT) M0315 11 4 CORRECTION The ground-state data were corrected for the M0315 11 5 bremsstrahlung spectra. M0315 11 6 ASSUMED Only neutrons of the highest 3.5 MeV wide region near M0315 11 7 the tip of each spectrum represent purely M0315 11 8 ground-state transition because the transitions to M0315 11 9 the first excited state of N-13 at 2.36 MeV are M0315 11 10 negligible. M0315 11 11 ANALYSIS The ground-state data have been obtained by M0315 11 12 fitting of a series of Legendre polynomials to the M0315 11 13 eight highest 3.5 MeV regions of neutron spectra for M0315 11 14 each end-point measurement. The zero order M0315 11 15 coefficient of this series has been corrected by M0315 11 16 division by the photon distribution shape and has M0315 11 17 been represented as the total ground-state cross M0315 11 18 section. M0315 11 19 ADD-RES The ground-state data were compared with the results M0315 11 20 of measurement of cross-sections for N-14(g,p0) and M0315 11 21 C-13(g,p0) reactions. M0315 11 22 REL-REF (A,,J.E.E.Baglin+,J,PR/C,10,24,1974) The result of M0315 11 23 measurement of N-14(g,p0) cross section. M0315 11 24 COMMENT For reactions to the ground state in N-13, it appears M0315 11 25 that most of the photon absorption in the giant M0315 11 26 resonance region studied forms 2- states in N-14, M0315 11 27 which are decayed by d-wave neutron emission. Some M0315 11 28 evidence was found for the existence of 0- strength M0315 11 29 at about 22.5 MeV (the peak of the cross section). M0315 11 30 The results are in general consistent with an M0315 11 31 identification of the (g,n0) process with the M0315 11 32 promotion of a p1/2 neutron to the s-d shell. Little M0315 11 33 or no E2 or M1 absorption was observed. Comparison M0315 11 34 with photoproton measurement shows some evidence for M0315 11 35 a small amount of isospin t=0 mixing also near 22.5 M0315 11 36 MeV. M0315 11 37 STATUS (CURVE) Fig.5 from Nucl.Phys.,A337(1980)503. M0315 11 38 (COREL,M0315010) Cross set. 4Pi x A0. M0315 11 39 HISTORY (20130617A) Corrected by V.Varlamov: BRA -> BRS. M0315 11 40 (20210620U) Corrected by SD and VV: EN-SEC deleted, M0315 11 41 REACTION, ANALYSIS, STATUS. M0315 11 42 ENDBIB 40 0 M0315 11 43 COMMON 1 3 M0315 11 44 E-LVL M0315 11 45 MEV M0315 11 46 0.0 M0315 11 47 ENDCOMMON 3 0 M0315 11 48 DATA 4 115 M0315 11 49 NUMBER EN DATA ERR-S M0315 11 50 NO-DIM MEV NO-DIM NO-DIM M0315 11 51 1. 18.2 -0.33 0.31 M0315 11 52 1. 18.4 0.05 0.14 M0315 11 53 1. 18.6 -0.05 0.13 M0315 11 54 1. 18.8 -0.16 0.13 M0315 11 55 1. 19.0 -0.10 0.13 M0315 11 56 1. 19.2 -0.04 0.13 M0315 11 57 1. 19.4 0.10 0.13 M0315 11 58 1. 19.6 0.09 0.13 M0315 11 59 1. 19.8 0.24 0.14 M0315 11 60 1. 20.0 0.24 0.14 M0315 11 61 1. 20.2 -0.08 0.15 M0315 11 62 1. 20.4 0.05 0.14 M0315 11 63 1. 20.6 0.20 0.13 M0315 11 64 1. 20.8 0.12 0.13 M0315 11 65 1. 21.0 0.10 0.13 M0315 11 66 1. 21.2 0.15 0.13 M0315 11 67 1. 21.4 0.10 0.13 M0315 11 68 1. 21.6 0.13 0.14 M0315 11 69 1. 21.8 0.31 0.13 M0315 11 70 1. 22.0 0.17 0.14 M0315 11 71 1. 22.2 0.40 0.13 M0315 11 72 1. 22.4 0.40 0.14 M0315 11 73 1. 22.6 0.31 0.13 M0315 11 74 1. 22.8 0.25 0.14 M0315 11 75 1. 23.0 0.31 0.14 M0315 11 76 1. 23.2 0.31 0.11 M0315 11 77 1. 23.4 0.26 0.14 M0315 11 78 1. 23.6 0.00 0.14 M0315 11 79 1. 23.8 0.14 0.13 M0315 11 80 1. 24.0 0.21 0.14 M0315 11 81 1. 24.2 0.26 0.13 M0315 11 82 1. 24.4 0.36 0.13 M0315 11 83 1. 24.6 0.30 0.13 M0315 11 84 1. 24.8 0.27 0.15 M0315 11 85 1. 25.0 0.17 0.15 M0315 11 86 1. 25.2 0.14 0.18 M0315 11 87 1. 25.4 0.48 0.18 M0315 11 88 1. 25.6 0.16 0.19 M0315 11 89 1. 25.8 0.06 0.20 M0315 11 90 2. 18.2 -0.70 0.20 M0315 11 91 2. 18.4 -0.83 0.18 M0315 11 92 2. 18.6 -0.76 0.17 M0315 11 93 2. 18.8 -0.78 0.15 M0315 11 94 2. 19.0 -0.70 0.15 M0315 11 95 2. 19.2 -0.85 0.15 M0315 11 96 2. 19.4 -0.60 0.14 M0315 11 97 2. 19.6 -0.57 0.15 M0315 11 98 2. 19.8 -0.63 0.17 M0315 11 99 2. 20.0 -0.75 0.15 M0315 11 100 2. 20.2 -0.80 0.15 M0315 11 101 2. 20.4 -0.63 0.17 M0315 11 102 2. 20.6 -0.41 0.11 M0315 11 103 2. 20.8 -0.45 0.17 M0315 11 104 2. 21.0 -0.35 0.17 M0315 11 105 2. 21.2 -0.42 0.19 M0315 11 106 2. 21.4 -0.51 0.18 M0315 11 107 2. 21.6 -0.55 0.17 M0315 11 108 2. 21.8 -0.23 0.18 M0315 11 109 2. 22.0 -0.39 0.15 M0315 11 110 2. 22.2 -0.14 0.15 M0315 11 111 2. 22.4 -0.10 0.14 M0315 11 112 2. 22.6 -0.33 0.15 M0315 11 113 2. 22.8 -0.36 0.13 M0315 11 114 2. 23.0 -0.36 0.15 M0315 11 115 2. 23.2 -0.54 0.14 M0315 11 116 2. 23.4 -0.49 0.15 M0315 11 117 2. 23.6 -1.00 0.15 M0315 11 118 2. 23.8 -0.97 0.14 M0315 11 119 2. 24.0 -0.63 0.15 M0315 11 120 2. 24.2 -0.71 0.18 M0315 11 121 2. 24.4 -0.60 0.18 M0315 11 122 2. 24.6 -0.57 0.18 M0315 11 123 2. 24.8 -0.59 0.19 M0315 11 124 2. 25.0 -0.75 0.19 M0315 11 125 2. 25.2 -0.88 0.20 M0315 11 126 2. 25.4 -0.55 0.19 M0315 11 127 2. 25.6 -0.90 0.18 M0315 11 128 3. 18.2 -0.11 0.24 M0315 11 129 3. 18.4 0.09 0.20 M0315 11 130 3. 18.6 -0.04 0.20 M0315 11 131 3. 18.8 -0.06 0.18 M0315 11 132 3. 19.0 -0.07 0.18 M0315 11 133 3. 19.2 -0.04 0.18 M0315 11 134 3. 19.4 0.15 0.18 M0315 11 135 3. 19.6 0.18 0.17 M0315 11 136 3. 19.8 0.31 0.18 M0315 11 137 3. 20.0 0.08 0.18 M0315 11 138 3. 20.2 -0.20 0.19 M0315 11 139 3. 20.4 0.19 0.19 M0315 11 140 3. 20.6 0.37 0.18 M0315 11 141 3. 20.8 0.36 0.19 M0315 11 142 3. 21.0 0.20 0.18 M0315 11 143 3. 21.2 0.06 0.18 M0315 11 144 3. 21.4 -0.05 0.15 M0315 11 145 3. 21.6 0.02 0.15 M0315 11 146 3. 21.8 0.15 0.17 M0315 11 147 3. 22.0 -0.09 0.15 M0315 11 148 3. 22.2 0.15 0.17 M0315 11 149 3. 22.4 0.26 0.17 M0315 11 150 3. 22.6 0.20 0.18 M0315 11 151 3. 22.8 0.14 0.15 M0315 11 152 3. 23.0 0.13 0.15 M0315 11 153 3. 23.2 0.17 0.15 M0315 11 154 3. 23.4 0.07 0.15 M0315 11 155 3. 23.6 0.04 0.15 M0315 11 156 3. 23.8 0.08 0.15 M0315 11 157 3. 24.0 0.02 0.17 M0315 11 158 3. 24.2 -0.08 0.15 M0315 11 159 3. 24.4 0.00 0.17 M0315 11 160 3. 24.6 0.01 0.15 M0315 11 161 3. 24.8 0.04 0.19 M0315 11 162 3. 25.0 -0.11 0.18 M0315 11 163 3. 25.2 -0.26 0.17 M0315 11 164 3. 25.4 0.10 0.20 M0315 11 165 3. 25.6 0.00 0.23 M0315 11 166 ENDDATA 117 0 M0315 11 167 ENDSUBENT 166 0 M0315 1199999 NOSUBENT M0315012 19910610 0000M031501200001 NOSUBENT M0315013 19910610 0000M031501300001 ENDENTRY 13 0 M031599999999