ENTRY 23030 20200909 22912303000000001 SUBENT 23030001 20200909 22912303000100001 BIB 18 195 2303000100002 TITLE 95 MeV neutron scattering on hydrogen, deuterium, 2303000100003 carbon, and oxygen 2303000100004 AUTHOR (P.Mermod, J.Blomgren, C.Johansson, A.Oehrn, 2303000100005 M.Oesterlund,S.Pomp, B.Bergenwall, J.Klug, L.Nilsson, 2303000100006 N.Olsson, U.Tippawan, P.Nadel-Turonski, O.Jonsson, 2303000100007 A.V.Prokofiev,P.-U.Renberg, Y.Maeda, H.Sakai, A.Tamii, 2303000100008 K.Amos, R.Crespo, A.M.Moro) 2303000100009 INSTITUTE (2SWDUPP)P.Mermod, J.Blomgren, C.Johansson,A.Oehrn, 2303000100010 M.Oesterlund,S.Pomp, B.Bergenwall,J.Klug, L.Nilsson, 2303000100011 N.Olsson,U.Tippawan,P.Nadel-Turonski,O.Jonsson, 2303000100012 A.V.Prokofiev,P.-U.Renberg. 2303000100013 (2GERZFK) J.Klug. 2303000100014 (2SWDFOI) N.Olsson. 2303000100015 (3TAICHM) U.Tippawan. 2303000100016 (1USAGWU) P.Nadel-Turonski. 2303000100017 (2JPNTOK) Y.Maeda, H.Sakai, A.Tamii. 2303000100018 (3AULAML) K.Amos. 2303000100019 (2PRTLIS) R.Crespo. Instituto Superior Technico,Lisboa,2303000100020 Portugal. 2303000100021 (2SPNSEU) A.Moro 2303000100022 REFERENCE (J,PR/C,74,054002,2006) 2303000100023 (T,Oehrn,2008) SCANDAL setup and exp.procedure 2303000100024 details. 2303000100025 (C,2007NICE,2,1039,2007) presentation on the Conf. 2303000100026 REL-REF (I,,S.Dangtip+,J,NIM/A,452,484,2000) MEDLEY setup 2303000100027 details. 2303000100028 (A,,C.Johansson+,J,PR/C,71,024002,2005) Data used in 2303000100029 normalization procedure. 2303000100030 FACILITY (CYCLO,2SWDUPP) Swedberg Lab.MEDLEY and SCANDAL setups.2303000100031 INC-SOURCE (P-LI7) 98 MeV proton beam of about 5 microA hitting a 2303000100032 thick lithium target enriched isotopically in Li-7 to 2303000100033 99.98%. 2303000100034 INC-SPECT Resulting neutron spectrum consisted of high-energy 2303000100035 peak at 94.8+-0.5 MeV with energy spread of 2.7 MeV 2303000100036 (FWHM) and low-energy tail, suppressed by TOF 2303000100037 technique. 2303000100038 1At MEDLEY target position 9.15m after Li target,neutron2303000100039 beam was about 8cm in diameter and intensity of about 2303000100040 5.E+4 1/s/cm**2. 2303000100041 2At SCANDAL target position 10.70m after Li target, 2303000100042 neutron beam was about 9 cm in diameter and intensity 2303000100043 about 4.E+4 1/s/cm**2. 2303000100044 DETECTOR 1(TELES) MEDLEY : 2303000100045 Vacuum chamber was cylinder of 80 cm in diameter. 2303000100046 Eight telescopes on rails emerging radially at 20 deg 2303000100047 separation on rotatable table. 2303000100048 (CSICR) Two silicon detectors (thin 50 or 60 microm and2303000100049 thick 400 or 500 microm available) and one thick CsI 2303000100050 detector(to detect protons up to 110 MeV energy) could 2303000100051 be mounted inside each telescope. 2303000100052 Uncertainty of typically 1.5% in the effective 2303000100053 detection area. 2303000100054 Two fission detectors were mounted after the 0.1 mm 2303000100055 thick stainless foil at exit of chamber for relative 2303000100056 monitoring of neutron fluence - 2303000100057 (TFBC) one based on thin-film breakdown counters, 2303000100058 (IOCH) other on ionization chamber. 2303000100059 2 SCANDAL: 2303000100060 Two identical arms rotated around target position, 2303000100061 each equipped with 2303000100062 (SCIN) 2mm thick veto scintillator for charged-particle2303000100063 rejection, two converter scintillators of 20 and 10 mm2303000100064 thickness for neutron-proton conversion, 2mm thick 2303000100065 deltaE plastic scintillator for triggering, 2303000100066 (DRFTC) two drift chambers for proton tracking, 2303000100067 another 2mm thick deltaE plastic scintillator for 2303000100068 triggering, 2303000100069 (CSICR) array of twelve CsI detectors for angular bins.2303000100070 Proton energy resolution 3.7 MeV (FWHM) average. 2303000100071 SAMPLE 1 MEDLEY: 2303000100072 Four different targets were used: 2303000100073 1) C-D2 target of 2.0cm x 4.0cm rectangle of 2303000100074 280 microm thickness. 2303000100075 2) C target of 2.5 cm in diameter disk , 150 microm 2303000100076 thickness. 2303000100077 3) C-H2 thick target of 2.5 cm in diameter disk, 2303000100078 1000 microm thickness. 2303000100079 4) C-H2 thin target of 2.0 cm x 4.0cm rectangle of 2303000100080 200 microm thickness. 2303000100081 Runs without target and with empty target 2303000100082 were performed for background subtraction. 2303000100083 2 SCANDAL: 2303000100084 Proton/deuteron detection mode: 2303000100085 Multi-target was used. 2303000100086 Three most downstream targets - 2303000100087 1) C-D2 target as disk of 7.0cm in diam., 1060 microm 2303000100088 thickness. 2303000100089 2) C target as disk of 8.0 cm in diameter, 500 microm 2303000100090 thickness. 2303000100091 3) C-H2 target as sheet covering the whole beam area, 2303000100092 of 380 microm thickness. 2303000100093 Neutron detection mode: 2303000100094 Targets were used one at a time. 2303000100095 1) H2-O target as 1 liter water contained in aluminum 2303000100096 can. 2303000100097 2) D2-O target as 1 liter of heavy water contained in 2303000100098 aluminum can. 2303000100099 3) EMPTY target as empty aluminum can of 8.5 cm in 2303000100100 diameter, 18 cm height. 2303000100101 4) C target as cylinder of 8 cm in diam., 16 cm height.2303000100102 METHOD 1 MEDLEY : ND scattering. Elastic peaks were well 2303000100103 isolated. 2303000100104 (EDE) Particle identification by deltaE/E techniques. 2303000100105 Main source of error was balance between deuteron 2303000100106 loses and proton contamination from deuteron break. 2303000100107 (TOF) Time of flight between trigger signal and 2303000100108 radio-frequency signal from cyclotron was measured to 2303000100109 reject events from low-energy neutrons. 2303000100110 Spectra obtained without target were subtracted, 2303000100111 then C spectra were subtracted from C-H2 and C-D2 2303000100112 spectra to obtain (n,p) and (n,d) elastic peaks. 2303000100113 Elastic peaks were fitted by Gaussian and integrated 2303000100114 to obtain number of elastic events. 2303000100115 2 SCANDAL: 2303000100116 Essentially the same method as for MEDLEY, performed 2303000100117 with another detector setup. 2303000100118 In proton/deuteron detection mode-multitarget was used,2303000100119 veto and converter detectors were removed. 2303000100120 nd data was normalized using (n,p) data. 2303000100121 Diameter of C-H2 target effective area was found to be2303000100122 about 9 cm. 2303000100123 For each target and each angular bin, after particle 2303000100124 identification, TOF selection, CsI window selection 2303000100125 and correction for MTGT efficiency, the accepted 2303000100126 events were projected as energy histograms, normalized2303000100127 to the same neutron fluence. 2303000100128 In neutron detection mode scattered neutrons were 2303000100129 detected by additional plastic scintillators (veto and 2303000100130 two converters) to tracking protons from (n,p)reactions2303000100131 After corrections for multiple scattering and 2303000100132 attenuation in the target, events were projected as 2303000100133 neutron energy histograms. EMPTY target spectra were 2303000100134 subtracted. To extract (n,p) and (n,d) elastic events 2303000100135 from H2-O and D2-O spectra, oxygen background have to 2303000100136 be subtracted - carbon spectra were used to simulate 2303000100137 the oxygen background in H2-O. 2303000100138 ANALYSIS 2 Spectra for collective states in C-12(n,inl) and 2303000100139 O-16(n,inl) were fitted in the range down to 20 MeV 2303000100140 below the elastic peak as the sum of four Gaussian 2303000100141 curves, corresponded to elastic peak and different 2303000100142 excited states. For carbon Gaussians at 4.4 MeV for 2303000100143 "first" level, 9.6 MeV for "second" and arbitrarily 2303000100144 set at 18 MeV to account for higher energy states. 2303000100145 For oxygen - 6.6, 10.4, 18 MeV, respectively. 2303000100146 Contribution from excited state Gaussians have been 2303000100147 subtracted, number of elastic events was obtained by 2303000100148 integrating the peaks in these spectra. 2303000100149 MONITOR 1(1-H-1(N,EL)1-H-1,,DA) for (n,p) and (n,d) scattering 2303000100150 from MEDLEY and SCANDAL proton/deuteron mode. 2303000100151 2(6-C-12(N,EL)6-C-12,,SIG) for normalization in 2303000100152 measurement at SCANDAL neutron mode. 2303000100153 Normalization to 286+-7 mb value. 2303000100154 MONIT-REF 1(22668002,J.Rahm+,J,PR/C,63,044001,2001) - Absolute 2303000100155 cross-sections are obtained by normalization to the 2303000100156 (n,p) elastic scattering differential cross-section 2303000100157 at 96 MeV of Rahm+, which in turn were re-normalized 2303000100158 by 0.7% using data of Johansson+ (see REL-REF). 2303000100159 2(22847002,J.Klug+,J,PR/C,68,064605,2003) 2303000100160 CORRECTION2 Correction for neutron multiple scattering and 2303000100161 attenuation inside targets before oxygen background 2303000100162 subtraction. Attenuation correction coefficients were 2303000100163 calculated from carbon and oxygen reaction cross 2303000100164 sections and (n,p) and (n,d) total cross-sections 2303000100165 using MC simulation. Attenuation in carbon - 17.3%, 2303000100166 in oxygen- 10.5%,in hydrogen- 1.2%, in deuterium-2.0%.2303000100167 Total attenuation effect 17.3% for C target, 2303000100168 11.5% for H2-O target, 12.3% for D2-O target. 2303000100169 Corrections for multiple scattering were typically 2%,2303000100170 with at most a 4% loss of events at smallest angle and2303000100171 50% gain at largest angle.MC and MCNPX codes were 2303000100172 used. 2303000100173 Correction for CsI efficiency. 2303000100174 Correction for inclusion of low-energy neutrons. 2303000100175 Correction for angular dependence of conversion 2303000100176 efficiency, typically 6% relative effect between small2303000100177 and large angles, with negligible systematic error. 2303000100178 ERR-ANALYS (ERR-T) Total uncertainty. 2303000100179 (ERR-1) Uncertainty in absolute normalization -4%. 2303000100180 (ERR-2) Uncertainty in correction for multiple 2303000100181 scattering was estimated to be 10% of correction 2303000100182 itself. 2303000100183 (ERR-3,2.,70.) Systematic uncertainty due to Gaussian 2303000100184 fits was evaluated to vary from 2% at small angles 2303000100185 to 70% at large angles. 2303000100186 ADD-RES (THEO) Exp. data are compared with predictions of 2303000100187 different models. 2303000100188 HISTORY (20080630C) M.M. 2303000100189 (20170825U) SD: Ref. 2007NICE,132(#435) deleted (full 2303000100190 article published in 2007NICE,2,1039,2007. 2303000100191 (20180317A) SD: Subents 008-009 added. Subents 006, 0072303000100192 corrected. ERR-ANALYS update. ANG-ERR moved to 2303000100193 Subents 002-007. Subents 004, 007 deleted. Data was 2303000100194 moved to Subents 003 and 006, correspondingly. 2303000100195 STATUS 'COREL' deleted (no alternative results). 2303000100196 (20200909A) SD: Correction in Subent 009. 2303000100197 ENDBIB 195 0 2303000100198 COMMON 7 6 2303000100199 EN EN-ERR EN-RSL-FW MONIT 2MONIT-ERR 2ERR-1 2303000100200 ERR-2 2303000100201 MEV MEV MEV MB MB PER-CENT 2303000100202 PER-CENT 2303000100203 94.8 0.5 2.7 286. 7. 4.2303000100204 10. 2303000100205 ENDCOMMON 6 0 2303000100206 ENDSUBENT 205 0 2303000199999 SUBENT 23030002 20180317 22702303000200001 BIB 4 4 2303000200002 REACTION (6-C-12(N,EL)6-C-12,,DA) 2303000200003 ERR-ANALYS (ANG-ERR) Uncertainty in neutron c.m. angle. 2303000200004 STATUS (TABLE) Table I from Phys.Rev.C74(2006)054002 2303000200005 HISTORY (20180317U) SD: ANG-ERR added. 2303000200006 ENDBIB 4 0 2303000200007 COMMON 1 3 2303000200008 ANG-ERR 2303000200009 ADEG 2303000200010 0.5 2303000200011 ENDCOMMON 3 0 2303000200012 DATA 3 18 2303000200013 ANG-CM DATA-CM ERR-T 2303000200014 ADEG MB/SR MB/SR 2303000200015 10.8 761. 31. 2303000200016 14.5 538. 23. 2303000200017 18.8 227. 12. 2303000200018 23.1 125. 7. 2303000200019 27.7 52. 4. 2303000200020 32.2 16.6 1.8 2303000200021 37.4 5.4 1.0 2303000200022 42.3 2.9 0.6 2303000200023 46.1 2.3 0.5 2303000200024 50.6 1.01 0.25 2303000200025 55.0 0.98 0.25 2303000200026 59.5 0.83 0.21 2303000200027 64.6 0.46 0.22 2303000200028 69.0 0.22 0.13 2303000200029 74.1 0.11 0.08 2303000200030 78.3 0.09 0.09 2303000200031 82.1 0.09 0.09 2303000200032 85.3 0.04 0.04 2303000200033 ENDDATA 20 0 2303000200034 ENDSUBENT 33 0 2303000299999 SUBENT 23030003 20180317 22702303000300001 BIB 5 12 2303000300002 REACTION (6-C-12(N,INL)6-C-12,PAR,DA) 2303000300003 Inelastic scattering to first excited state. 2303000300004 LEVEL-PROP (6-C-12,E-LVL=4.4,SPIN=2.,PARITY=1.) 2303000300005 Energy of "first" 2+ excited state, 2303000300006 corresponding to Gaussian at 4.4 MeV. 2303000300007 (6-C-12,E-LVL=9.6,SPIN=3.,PARITY=-1.) 2303000300008 Energy of "second" 3- excited state, 2303000300009 corresponding to Gaussian at 9.6 MeV. 2303000300010 ERR-ANALYS (ANG-ERR) Uncertainty in neutron c.m. angle. 2303000300011 STATUS (TABLE) Table I of from Phys.Rev.C74(2006)054002 2303000300012 HISTORY (20180317A) SD: ANG-ERR added. EN-SEC -> LEVEL-PROP. 2303000300013 Data from Subent 004 were added. 2303000300014 ENDBIB 12 0 2303000300015 COMMON 1 3 2303000300016 ANG-ERR 2303000300017 ADEG 2303000300018 0.5 2303000300019 ENDCOMMON 3 0 2303000300020 DATA 4 26 2303000300021 E-LVL ANG-CM DATA-CM ERR-T 2303000300022 MEV ADEG MB/SR MB/SR 2303000300023 4.4 32.2 4.0 1.8 2303000300024 4.4 37.4 3.6 0.9 2303000300025 4.4 42.3 3.0 0.8 2303000300026 4.4 46.1 1.8 0.6 2303000300027 4.4 50.6 0.92 0.26 2303000300028 4.4 55.0 0.66 0.22 2303000300029 4.4 59.5 0.48 0.16 2303000300030 4.4 64.6 0.28 0.14 2303000300031 4.4 69.0 0.22 0.11 2303000300032 4.4 74.1 0.11 0.05 2303000300033 4.4 78.3 0.05 0.03 2303000300034 4.4 82.1 0.06 0.04 2303000300035 4.4 85.3 0.04 0.03 2303000300036 9.6 32.2 4.5 1.9 2303000300037 9.6 37.4 5.0 1.2 2303000300038 9.6 42.3 2.6 0.5 2303000300039 9.6 46.1 3.1 0.7 2303000300040 9.6 50.6 1.46 0.38 2303000300041 9.6 55.0 1.96 0.51 2303000300042 9.6 59.5 1.72 0.49 2303000300043 9.6 64.6 1.36 0.54 2303000300044 9.6 69.0 0.35 0.17 2303000300045 9.6 74.1 0.18 0.10 2303000300046 9.6 78.3 0.08 0.05 2303000300047 9.6 82.1 0.02 0.02 2303000300048 9.6 85.3 0.04 0.04 2303000300049 ENDDATA 28 0 2303000300050 ENDSUBENT 49 0 2303000399999 NOSUBENT 23030004 20180317 22702303000400001 SUBENT 23030005 20180317 22702303000500001 BIB 5 8 2303000500002 REACTION (8-O-16(N,EL)8-O-16,,DA) 2303000500003 ANALYSIS O-16(n,el) distribution was extracted from H2-O and 2303000500004 D2-O measurement spectra. spectra obtained previously 2303000500005 for np and nd scattering were subtracted from H2-O and2303000500006 D2-O spectra to obtain oxygen spectra. 2303000500007 ERR-ANALYS (ANG-ERR) Uncertainty in neutron c.m. angle. 2303000500008 STATUS (TABLE) Table II from Phys.Rev.C74(2006)054002 2303000500009 HISTORY (20180317U) SD: ANG-ERR added. 2303000500010 ENDBIB 8 0 2303000500011 COMMON 1 3 2303000500012 ANG-ERR 2303000500013 ADEG 2303000500014 0.5 2303000500015 ENDCOMMON 3 0 2303000500016 DATA 3 18 2303000500017 ANG-CM DATA-CM ERR-T 2303000500018 ADEG MB/SR MB/SR 2303000500019 10.6 1087. 44. 2303000500020 14.2 708. 30. 2303000500021 18.4 256. 14. 2303000500022 22.7 131. 8. 2303000500023 27.1 39. 3. 2303000500024 31.6 11.9 1.2 2303000500025 36.5 8.0 1.5 2303000500026 41.3 5.8 1.1 2303000500027 45.2 3.4 0.7 2303000500028 49.8 1.29 0.27 2303000500029 54.0 1.13 0.26 2303000500030 58.2 0.95 0.22 2303000500031 63.5 0.51 0.20 2303000500032 67.8 0.37 0.17 2303000500033 73.0 0.13 0.07 2303000500034 77.2 0.03 0.03 2303000500035 80.8 0.02 0.02 2303000500036 84.0 0.02 0.01 2303000500037 ENDDATA 20 0 2303000500038 ENDSUBENT 37 0 2303000599999 SUBENT 23030006 20180317 22702303000600001 BIB 6 20 2303000600002 REACTION (8-O-16(N,INL)8-O-16,PAR,DA) 2303000600003 Inelastic scattering to sum of 3- and 2+ excited 2303000600004 states. 2303000600005 LEVEL-PROP (8-O-16,E-LVL=6.1,SPIN=3.,PARITY=-1.) 2303000600006 (8-O-16,E-LVL=6.9,SPIN=2.,PARITY=+1.) 2303000600007 (8-O-16,E-LVL=9.8,SPIN=2.,PARITY=1.) 2303000600008 (8-O-16,E-LVL=10.4,SPIN=4.,PARITY=1.) 2303000600009 ANALYSIS Energy of "first" excited state, corresponding to 2303000600010 Gaussian at 6.5 MeV, refers to 3- state at 6.1 MeV 2303000600011 and 2+ state at 6.9 MeV together, and probably also 2303000600012 the relatively weak 1- state at 7.1 MeV. 2303000600013 Energy of "second" excited state, corresponding to 2303000600014 Gaussian at 10.4 MeV, refers to 2+ state at 9.8 MeV 2303000600015 and 4+ state at 10.4 MeV together, where 4+ state 2303000600016 is expected to dominate. 2303000600017 ERR-ANALYS (ANG-ERR) Uncertainty in neutron c.m. angle. 2303000600018 STATUS (TABLE) Table II from Phys.Rev.C74(2006)054002 2303000600019 HISTORY (20180317A) SD: E-LVL-MEAN -> E-LVL. ANG-ERR added. 2303000600020 EN-SEC -> LEVEL-PROP. Info moved to ANALYSIS. 2303000600021 Data from Subent 007 were added. 2303000600022 ENDBIB 20 0 2303000600023 COMMON 1 3 2303000600024 ANG-ERR 2303000600025 ADEG 2303000600026 0.5 2303000600027 ENDCOMMON 3 0 2303000600028 DATA 5 24 2303000600029 E-LVL E-LVL ANG-CM DATA-CM ERR-T 2303000600030 MEV MEV ADEG MB/SR MB/SR 2303000600031 6.1 6.9 31.6 5.3 2.4 2303000600032 6.1 6.9 36.5 5.9 1.5 2303000600033 6.1 6.9 41.3 2.8 0.8 2303000600034 6.1 6.9 45.2 3.0 0.9 2303000600035 6.1 6.9 49.8 1.63 0.46 2303000600036 6.1 6.9 54.0 1.52 0.49 2303000600037 6.1 6.9 58.2 1.11 0.35 2303000600038 6.1 6.9 63.5 0.60 0.27 2303000600039 6.1 6.9 67.8 0.54 0.22 2303000600040 6.1 6.9 73.0 0.28 0.04 2303000600041 6.1 6.9 77.2 0.10 0.02 2303000600042 6.1 6.9 80.8 0.06 0.02 2303000600043 9.8 10.4 31.6 2.7 1.1 2303000600044 9.8 10.4 36.5 2.5 0.7 2303000600045 9.8 10.4 41.3 2.4 0.5 2303000600046 9.8 10.4 45.2 2.0 0.4 2303000600047 9.8 10.4 49.8 1.76 0.44 2303000600048 9.8 10.4 54.0 1.43 0.37 2303000600049 9.8 10.4 58.2 0.88 0.25 2303000600050 9.8 10.4 63.5 0.80 0.33 2303000600051 9.8 10.4 67.8 0.29 0.13 2303000600052 9.8 10.4 73.0 0.14 0.07 2303000600053 9.8 10.4 77.2 0.13 0.07 2303000600054 9.8 10.4 80.8 0.08 0.02 2303000600055 ENDDATA 26 0 2303000600056 ENDSUBENT 55 0 2303000699999 NOSUBENT 23030007 20180317 22702303000700001 SUBENT 23030008 20180317 22702303000800001 BIB 3 3 2303000800002 REACTION (6-C-12(N,EL)6-C-12,,KER) 2303000800003 STATUS (TABLE) Table V from Phys.Rev.C74(2006)054002 2303000800004 HISTORY (20180317C) SD 2303000800005 ENDBIB 3 0 2303000800006 NOCOMMON 0 0 2303000800007 DATA 2 1 2303000800008 DATA ERR-T 2303000800009 FGY*M2 FGY*M2 2303000800010 0.120 0.007 2303000800011 ENDDATA 3 0 2303000800012 ENDSUBENT 11 0 2303000899999 SUBENT 23030009 20200909 22912303000900001 BIB 4 6 2303000900002 REACTION (6-C-12(N,INL)6-C-12,PAR,KER) 2303000900003 LEVEL-PROP (6-C-12,E-LVL=4.4,SPIN=2.,PARITY=1.) 2303000900004 (6-C-12,E-LVL=9.6,SPIN=3.,PARITY=-1.) 2303000900005 STATUS (TABLE) Table V from Phys.Rev.C74(2006)054002 2303000900006 HISTORY (20180317C) SD 2303000900007 (20200909A) SD: SF3=EL -> INL in REACTION code. 2303000900008 ENDBIB 6 0 2303000900009 NOCOMMON 0 0 2303000900010 DATA 3 2 2303000900011 E-LVL DATA ERR-T 2303000900012 MEV FGY*M2 FGY*M2 2303000900013 4.4 0.018 0.005 2303000900014 9.6 0.029 0.009 2303000900015 ENDDATA 4 0 2303000900016 ENDSUBENT 15 0 2303000999999 SUBENT 23030010 20180317 22702303001000001 BIB 3 3 2303001000002 REACTION (8-O-16(N,EL)8-O-16,,KER) 2303001000003 STATUS (TABLE) Table V from Phys.Rev.C74(2006)054002 2303001000004 HISTORY (20180317C) SD 2303001000005 ENDBIB 3 0 2303001000006 NOCOMMON 0 0 2303001000007 DATA 2 1 2303001000008 DATA ERR-T 2303001000009 FGY*M2 FGY*M2 2303001000010 0.073 0.004 2303001000011 ENDDATA 3 0 2303001000012 ENDSUBENT 11 0 2303001099999 SUBENT 23030011 20180317 22702303001100001 BIB 4 9 2303001100002 REACTION (8-O-16(N,INL)8-O-16,PAR,KER) 2303001100003 Inelastic scattering to sum of 2+ and 4+ excited 2303001100004 states. 2303001100005 LEVEL-PROP (8-O-16,E-LVL=6.1,SPIN=3.,PARITY=-1.) 2303001100006 (8-O-16,E-LVL=6.9,SPIN=2.,PARITY=+1.) 2303001100007 (8-O-16,E-LVL=9.8,SPIN=2.,PARITY=1.) 2303001100008 (8-O-16,E-LVL=10.4,SPIN=4.,PARITY=1.) 2303001100009 STATUS (TABLE) Table V from Phys.Rev.C74(2006)054002 2303001100010 HISTORY (20180317C) SD 2303001100011 ENDBIB 9 0 2303001100012 NOCOMMON 0 0 2303001100013 DATA 4 2 2303001100014 E-LVL E-LVL DATA ERR-T 2303001100015 MEV MEV FGY*M2 FGY*M2 2303001100016 6.1 6.9 0.017 0.005 2303001100017 9.8 10.4 0.011 0.003 2303001100018 ENDDATA 4 0 2303001100019 ENDSUBENT 18 0 2303001199999 ENDENTRY 11 0 2303099999999