ENTRY 22171 20210829 23032217100000001 SUBENT 22171001 20210829 23032217100100001 BIB 13 56 2217100100002 TITLE 7Li(n,gamma)8Li - trigger reaction to a primordial 2217100100003 r-process? 2217100100004 AUTHOR (M.Wiescher,R.Steininger,F.Kaeppeler) 2217100100005 REFERENCE (J,AJ,344,464,1989) 2217100100006 (R,INDC(GER)-0053,2021) Revised values of Karlsruhe 2217100100007 cross sections. 2217100100008 REL-REF (C,22401001,M.Heil+,J,AJ,507,997,1998) There is a 2217100100009 miscalculation of the total efficiency of the 2217100100010 ionization chamber. 2217100100011 A new analysis yields gives 57+/-9 ub at 25 keV 2217100100012 INSTITUTE (2GERKFK) R.S., F.K. and experimental site 2217100100013 (1USANOT) M.W. 2217100100014 FACILITY (VDG,2GERKFK) 3.75MV Van de Graaff accelerator. A 1 mm22217100100015 proton beam spot was swept magnetically across the 2217100100016 target to achieve homogeneous illumination. Beam 2217100100017 currents of up to 90 uA were used. The target 2217100100018 was bombarded for 5 sec intervals every 10 sec. 2217100100019 METHOD (ACTIV) 2217100100020 SAMPLE To derive the 7-Li(n,gamma) cross section from the 2217100100021 activation analysis the number of 7-Li atoms in the 2217100100022 samples had to be determined. This was done by 2217100100023 measuring the 6-Li(n,t)2-He-4 reaction. The 2217100100024 accelerator was operated in DC mode, Ep = 1.912 MeV, 2217100100025 to produce the Maxwellian kT = 25 keV spectrum, and 2217100100026 the samples positioned in close proximity to the 2217100100027 target. The proton beam intensity was reduced to 2217100100028 5 - 10 uA and the ionization chamber was used with an 2217100100029 increased gas pressure of 700 mbar. 2217100100030 Triton and alpha yields were determined by standard 2217100100031 peak analysis of the spectra, from which the Li 2217100100032 abundances and thus the sample thicknesses in atoms/b 2217100100033 could be calculated. 2217100100034 MONITOR (3-LI-6(N,T)2-HE-4,,SIG,,MXW) Data from ENDF/B-V, used 2217100100035 in determination of the number of 7-Li atoms in the 2217100100036 respective samples. 2217100100037 DETECTOR (GLASD) 6-Li glass detector to monitor neutron yield, 2217100100038 positioned on the beam axis 0.7 m from the target. 2217100100039 (GE-IN) A shielded 45 cm3 Ge detector, 1.6 keV 2217100100040 resolution at 1.33 MeV, was used to count gold monitor2217100100041 foil activity. 2217100100042 CORRECTION Background, detector efficiency. 2217100100043 ERR-ANALYS (ERR-T) Total error including 2217100100044 * statistical uncertainty and: 2217100100045 (ERR-2) Uncertainty due to neutron flux determination 2217100100046 (ERR-3) Uncertainty due to instability in neutron flux 2217100100047 (ERR-4,4.,5.) Uncertainty in number of Li atoms 2217100100048 (ERR-5) Uncertainty due to decay rate 2217100100049 HISTORY (19910220C) S.W. 2217100100050 (19910716A) S.W. Data mods, critique added, 2217100100051 Subents 002,003,005 2217100100052 (20200906A) SD:Updated to new date formats,lower case. 2217100100053 Corrections in all Subents. Part of ERR-ANALYS moved 2217100100054 to Subent 001. 2217100100055 (20201212U) SD: REL-REF added. 2217100100056 (20210829A) SD: Corrections in two Subents. Subents 2217100100057 007, 008 added. 2217100100058 ENDBIB 56 0 2217100100059 COMMON 3 3 2217100100060 ERR-2 ERR-3 ERR-5 2217100100061 PER-CENT PER-CENT PER-CENT 2217100100062 2.5 1. 1. 2217100100063 ENDCOMMON 3 0 2217100100064 ENDSUBENT 63 0 2217100199999 SUBENT 22171002 20210829 23032217100200001 BIB 13 43 2217100200002 REACTION (3-LI-7(N,G)3-LI-8,,SIG,,MXW) 2217100200003 INC-SOURCE (P-LI7) Metallic layers of natural Li, 2 mg/cm2 thick 2217100200004 and 5 mm in diam, evaporated on a 1.0 mm thick water- 2217100200005 cooled Cu backing. Using 1912 keV protons the 120 deg 2217100200006 forward cone of emitted neutrons closely approximates 2217100200007 to a Maxwellian kT = 25 keV shape. Total neutron rate 2217100200008 varied between 2.0E+8 and 7.0E+8 n/s 2217100200009 Monitor gold foils of 12.0 mm in diam. and 0.03 mm 2217100200010 thickness were attached to the copper backing. 2217100200011 INC-SPECT The neutron spectrum is closely approximated to a 2217100200012 Maxwellian shape with temperature of 25 keV. 2217100200013 SAMPLE Thin layer of LiF evaporated on the cathode of a 2-pi 2217100200014 hemispherical ionization chamber, with a maximum 2217100200015 thickness 260 ug/cm2 and in diam 25 mm. 2217100200016 DETECTOR (IOCH) 2-pi hemispherical ionization chamber, filled 2217100200017 with CF4 gas at 320 milli-bar and operated at 2217100200018 1500 volt. Efficiency determined by calculation using 2217100200019 sample parameters, tabulated alpha ranges and Monte 2217100200020 Carlo simulation. 2217100200021 RAD-DET (4-BE-8,A) 8-Be breakup 2217100200022 DECAY-DATA (4-BE-8,,A,1570.) 8-Be breakup producing 2 alphas. 2217100200023 (3-LI-8,0.840SEC,B-,12964.) 2217100200024 MONITOR ((MONIT1)79-AU-197(N,G)79-AU-198,,SIG,,MXW) 2217100200025 MONIT-REF ((MONIT1)22099003,W.Ratynski+,J,PR/C,37,595,1988) The 2217100200026 value in work 22099 has been corrected and multiplied 2217100200027 by a factor 2/(pi**0.5). 2217100200028 FLAG (1.) LiF thickness was 1.84E-06 atoms/barn 2217100200029 (2.) LiF thickness was 2.91E-06 atoms/barn 2217100200030 (3.) LiF thickness was 4.42E-06 atoms/barn. 2217100200031 (4.) LiF thickness was 4.42E-06 atoms/barn 2217100200032 (5.) Li glass (NE907), 1.87E-3 atoms/barn 2217100200033 ERR-ANALYS (ERR-6,8.,15.) LiF activity (kT=25 keV) 2217100200034 (ERR-1,2.,10.) Uncertainty due to detector efficiency 2217100200035 STATUS (TABLE) Table 2 from Astrophys.J.,344(1989)464 2217100200036 (SPSDD,22171007) Re-normalized. 2217100200037 HISTORY (19910716A) S.W. Decay-data + data mods, critique added2217100200038 (20200906A) SD: ERR-ANALYS, STATUS updated. First 2217100200039 data value moved to DATA-MAX. CRITIQUE deleted (now 2217100200040 inclusion of 2/sqrt(pi) is the standard definition of 2217100200041 MACS in EXFOR). THICKNESS moved to the FLAG (not 2217100200042 independent variable). 2217100200043 (20210829A) SD: Value 20.1 mu-b (from Subent 003) added2217100200044 to the DATA col. Subent superseded. 2217100200045 ENDBIB 43 0 2217100200046 COMMON 3 3 2217100200047 KT MONIT1 MONIT1-ERR 2217100200048 KEV MB PER-CENT 2217100200049 25. 648. 1.5 2217100200050 ENDCOMMON 3 0 2217100200051 DATA 4 5 2217100200052 DATA ERR-T DATA-MAX FLAG 2217100200053 MICRO-B PER-CENT MICRO-B NO-DIM 2217100200054 21.4 1. 2217100200055 25.2 17.0 2. 2217100200056 26.3 15.5 3. 2217100200057 28.5 15.5 4. 2217100200058 20.1 9.0 5. 2217100200059 ENDDATA 7 0 2217100200060 ENDSUBENT 59 0 2217100299999 SUBENT 22171003 20210829 23032217100300001 BIB 13 42 2217100300002 REACTION (3-LI-7(N,G)3-LI-8,,SIG,,SPA/AV) 2217100300003 ANALYSIS Average of results from several irradiations 2217100300004 INC-SOURCE (P-LI7) Metallic layers of natural Li, 2 mg/cm2 thick 2217100300005 and 5 mm in diam., evaporated on a 1.0 mm thick water-2217100300006 cooled Cu backing. Using 1912 keV protons the 120 deg 2217100300007 forward cone of emitted neutrons closely approximates 2217100300008 to a Maxwellian kT = 25 keV shape. Total neutron rate 2217100300009 varied between 2.0E+8 and 7.0E+8 n/s 2217100300010 Monitor gold foils of 12.0 mm in diam. and 0.03 mm 2217100300011 thick were attached to the copper backing. 2217100300012 INC-SPECT The neutron spectrum is closely approximated to a 2217100300013 Maxwellian shape with temperature of 25 keV. 2217100300014 SAMPLE A 1 mm thick NE907 Li-glass scintillator, 8.1% natural2217100300015 Li, 28 mm in diam. Thickness was 1.87E-03 atoms/barn. 2217100300016 DETECTOR (SCIN) A 1 mm thick NE907 Li-glass scintillator, 8.1% 2217100300017 natural Li, 28 mm in diam, contained in a 0.5 mm thick2217100300018 Al housing, with a 2.54 cm front opening and connected2217100300019 to a 5.08 cm photomultiplier. The detector was beta 2217100300020 shielded by 0.6 mm antimony-free lead. The Li in the 2217100300021 glass scintillator also constituted the activation 2217100300022 sample in this case. 2217100300023 RAD-DET (3-LI-8,B-) 2217100300024 (4-BE-8,A) 2217100300025 DECAY-DATA (3-LI-8,0.840SEC,B-,12964.) 2217100300026 (4-BE-8,,A,1570.) 8-Be breakup producing 2 alphas. 2217100300027 MONITOR ((MONIT1)79-AU-197(N,G)79-AU-198,,SIG,,MXW) 2217100300028 MONIT-REF ((MONIT1)22099003,W.Ratynski+,J,PR/C,37,595,1988) The 2217100300029 value in the Entry 22099 has been corrected and 2217100300030 multiplied by a factor 2/(pi**0.5). 2217100300031 ERR-ANALYS (ERR-6,8.,15.) LiF activity (kT=25keV) 2217100300032 (ERR-1,2.,10.) Uncertainty due to detector efficiency 2217100300033 STATUS (TABLE) Table 2 from Astrophys.J.,344(1989)464 2217100300034 (DEP,22171002) Results of individual irradiations 2217100300035 (SPSDD,22171008) Re-normalized 2217100300036 HISTORY (19910716A) S.W. Decay-data + data mods, critique added2217100300037 (20200906U) SD: ERR-ANALYS, STATUS updated. CRITIQUE 2217100300038 deleted (now inclusion of 2/sqrt(pi) is the standard 2217100300039 definition of MACS in EXFOR). THICKNESS moved to the 2217100300040 SAMPLE (not independent variable). 2217100300041 (20210829A) SD: SF8=MXW -> SPA/AV in REACTION code. 2217100300042 Value at ERR-T corrected. Subent superseded. 2217100300043 Data corrected (20.1 -> 21.0 ub) according to report. 2217100300044 ENDBIB 42 0 2217100300045 NOCOMMON 0 0 2217100300046 DATA 5 1 2217100300047 KT DATA ERR-T MONIT1 MONIT1-ERR 2217100300048 KEV MICRO-B MICRO-B MB PER-CENT 2217100300049 25. 21.0 1.9 648. 1.5 2217100300050 ENDDATA 3 0 2217100300051 ENDSUBENT 50 0 2217100399999 SUBENT 22171004 20200906 22912217100400001 BIB 4 11 2217100400002 REACTION (3-LI-7(N,G)3-LI-8,,SIG,,,DERIV) 2217100400003 ANALYSIS Calculated from the weighted average of the results 2217100400004 for kT = 25 keV and quoted as the adopted mono- 2217100400005 energetic cross section at EN = 25 keV. No details of 2217100400006 the precise weighting or analysis are given. 2217100400007 STATUS (TABLE) Table 2 from Astrophys.J.,344(1989)464 2217100400008 (DEP,22171002) 2217100400009 (DEP,22171003) 2217100400010 (SPSDD,22171006) 2217100400011 HISTORY (19910716U) S.W. 2217100400012 (20200906U) SD: STATUS updated. ERR-ANALYS deleted. 2217100400013 ENDBIB 11 0 2217100400014 NOCOMMON 0 0 2217100400015 DATA 3 1 2217100400016 EN DATA ERR-T 2217100400017 KEV MICRO-B MICRO-B 2217100400018 25. 21.0 1.9 2217100400019 ENDDATA 3 0 2217100400020 ENDSUBENT 19 0 2217100499999 SUBENT 22171005 20200906 22912217100500001 BIB 12 32 2217100500002 REACTION (3-LI-7(N,G)3-LI-8,,SIG) 2217100500003 INC-SOURCE (P-LI7) Thin 150 mu-g/cm2 LiF targets, for production 2217100500004 of fast monoenergetic neutrons. Proton energies 2217100500005 of 1926 - 2153 keV produced neutrons from 130 to 2217100500006 410 keV, the energy spread being +/- 10 keV. Total 2217100500007 neutron rate varied between 1.2E7 and 2.8E7 n/s. 2217100500008 SAMPLE A 1 mm thick NE907 Li-glass scintillator, 8.1% natural2217100500009 Li, 28 mm in diam. Thickness was 1.8700E-03 atoms/barn2217100500010 Monitor gold foils of 28.0 mm in diam. and 0.03 mm 2217100500011 thick were attached directly to the front of the glass2217100500012 scintillator. 2217100500013 METHOD (ACTIV) 2217100500014 DETECTOR (SCIN) A 1 mm thick NE907 Li-glass scintillator, 8.1% 2217100500015 natural Li, 28 mm diam., contained in a 0.5 mm thick 2217100500016 Al housing, with a 2.54 cm front opening and connected2217100500017 to a 5.08 cm photomultiplier. The detector was beta 2217100500018 shielded by 0.6 mm antimony-free lead. The Li in the 2217100500019 glass scintillator also constituted the activation 2217100500020 sample in this case. 2217100500021 PART-DET (B-,A ) Decay of 8-Li and 8-Be breakup 2217100500022 DECAY-DATA (3-LI-8,0.840SEC,B-,12964.) 2217100500023 (4-BE-8,,A,1570.) 8-Be breakup producing 2 alphas. 2217100500024 MONITOR (79-AU-197(N,G)79-AU-198,,SIG) 2217100500025 MONIT-REF (,,W,MACKLIN,1982) Cross sections normalized to 2217100500026 new value in Ratynski et al.,Phys.Rev.,C37,595 (1988).2217100500027 ERR-ANALYS (ERR-6,8.,30.) Li-glass activity (120-420keV) 2217100500028 (ERR-1,2.,10.) Uncertainty due to detector efficiency 2217100500029 STATUS (TABLE) Table 2 from Astrophys.J.,344(1989)464 2217100500030 HISTORY (19910716A) S.W. Decay-data + data mod. 2217100500031 (20200906U) SD: ERR-ANALYS, STATUS updated. THICKNESS 2217100500032 moved to the SAMPLE (not independent variable). 2217100500033 EN-ERR -> EN-RSL-HW 2217100500034 ENDBIB 32 0 2217100500035 COMMON 1 3 2217100500036 EN-RSL-HW 2217100500037 KEV 2217100500038 10. 2217100500039 ENDCOMMON 3 0 2217100500040 DATA 3 8 2217100500041 EN DATA ERR-T 2217100500042 KEV MICRO-B MICRO-B 2217100500043 130. 11.2 2.2 2217100500044 170. 10.8 1.8 2217100500045 210. 11.8 1.5 2217100500046 250. 14.4 2.1 2217100500047 290. 10.0 1.9 2217100500048 330. 8.6 1.9 2217100500049 370. 6.1 1.8 2217100500050 410. 3.8 1.3 2217100500051 ENDDATA 10 0 2217100500052 ENDSUBENT 51 0 2217100599999 SUBENT 22171006 20200906 22912217100600001 BIB 4 11 2217100600002 REACTION (3-LI-7(N,G)3-LI-8,,SIG,,,DERIV) 2217100600003 REL-REF (R,22401001,M.Heil+,J,AJ,507,997,1998) 2217100600004 In AJ,507,997,1998, page 1002, value of CS at 25 keV 2217100600005 measured in Subent 22171.004 by ionization chamber was2217100600006 re-analyzed to be 57+-9 microbarn - discrepancy was 2217100600007 mainly due to miscalculation of the total efficiency of2217100600008 the ionization chamber; new analysis of the activation 2217100600009 with Li-glass detector of this Entry was impossible, 2217100600010 because the original data could no longer be retrieved.2217100600011 STATUS (TABLE) Text on p.1002 of Astrophys.J.,507(1998)507 2217100600012 HISTORY (19910220C) SD 2217100600013 ENDBIB 11 0 2217100600014 NOCOMMON 0 0 2217100600015 DATA 3 1 2217100600016 EN DATA ERR-T 2217100600017 KEV MICRO-B MICRO-B 2217100600018 25. 57. 9. 2217100600019 ENDDATA 3 0 2217100600020 ENDSUBENT 19 0 2217100699999 SUBENT 22171007 20210829 23032217100700001 BIB 16 48 2217100700002 REACTION (3-LI-7(N,G)3-LI-8,,SIG,,MXW) 2217100700003 INC-SOURCE (P-LI7) Metallic layers of natural Li, 2 mg/cm2 thick 2217100700004 and 5 mm in diam, evaporated on a 1.0 mm thick water- 2217100700005 cooled Cu backing. Using 1912 keV protons the 120 deg 2217100700006 forward cone of emitted neutrons closely approximates 2217100700007 to a Maxwellian kT = 25 keV shape. Total neutron rate 2217100700008 varied between 2.0E+8 and 7.0E+8 n/s 2217100700009 Monitor gold foils of 12.0 mm in diam. and 0.03 mm 2217100700010 thickness were attached to the copper backing. 2217100700011 INC-SPECT The neutron spectrum is closely approximated to a 2217100700012 Maxwellian shape with temperature of 25 keV. 2217100700013 SAMPLE Thin layer of LiF evaporated on the cathode of a 2-pi 2217100700014 hemispherical ionization chamber, with a maximum 2217100700015 thickness 260 ug/cm2 and in diam 25 mm. 2217100700016 DETECTOR (IOCH) 2-pi hemispherical ionization chamber, filled 2217100700017 with CF4 gas at 320 milli-bar and operated at 2217100700018 1500 volt. Efficiency determined by calculation using 2217100700019 sample parameters, tabulated alpha ranges and Monte 2217100700020 Carlo simulation. 2217100700021 RAD-DET (4-BE-8,A) 8-Be breakup 2217100700022 DECAY-DATA (4-BE-8,,A,1570.) 8-Be breakup producing 2 alphas. 2217100700023 (3-LI-8,0.840SEC,B-,12964.) 2217100700024 MONITOR ((MONIT1)79-AU-197(N,G)79-AU-198,,SIG,,MXW) 2217100700025 MONIT-REF ((MONIT1),R.Reifarth+,J,EPJ/P,133,424,2018) 2217100700026 FLAG (1.) LiF thickness was 1.84E-06 atoms/barn 2217100700027 (2.) LiF thickness was 2.91E-06 atoms/barn 2217100700028 (3.) LiF thickness was 4.42E-06 atoms/barn. 2217100700029 (4.) LiF thickness was 4.42E-06 atoms/barn 2217100700030 (5.) Li glass (NE907), 1.87E-3 atoms/barn 2217100700031 ANALYSIS Cross section value in subentry 22171.002 is 2217100700032 renormalized: 2217100700033 a) for new gold cross section 2217100700034 b) corrected for missing line in previous data set 2217100700035 c) note that the quoted neutron energies refer to 2217100700036 the lab system; effective energies in the 2217100700037 c.m. system have to be reduced by 7/8 2217100700038 Measured quantity: cross section ratio 2217100700039 7Li/197Au = (3.24+-0.29)E-05 2217100700040 2 Weighted average of the different results obtained 2217100700041 with kT = 25 keV. 2217100700042 CORRECTION Correction for revised gold standard 681/648 =1.051 2217100700043 COMMENT 'MXW cross section must be obtained from adopted SPA 2217100700044 cross section of 21.9 mb by multiplication with 2217100700045 2/sqrt(pi)' from INDC(GER)-0053 report, p.56 2217100700046 ERR-ANALYS (ERR-6,8.,15.) LiF activity (kT=25 keV) 2217100700047 (ERR-1,2.,10.) Uncertainty due to detector efficiency 2217100700048 STATUS (TABLE) p.55 of INDC(GER)-0053 2217100700049 HISTORY (19910716C) SD 2217100700050 ENDBIB 48 0 2217100700051 COMMON 3 3 2217100700052 KT MONIT1 MONIT1-ERR 2217100700053 KEV MB PER-CENT 2217100700054 25. 681. 1. 2217100700055 ENDCOMMON 3 0 2217100700056 DATA 4 5 2217100700057 DATA ERR-T DATA-MAX FLAG 2217100700058 MICRO-B PER-CENT MICRO-B NO-DIM 2217100700059 22.5 1. 2217100700060 26.5 17.0 2. 2217100700061 27.6 15.5 3. 2217100700062 30.0 15.5 4. 2217100700063 21.1 15.5 5. 2217100700064 ENDDATA 7 0 2217100700065 ENDSUBENT 64 0 2217100799999 SUBENT 22171008 20210829 23032217100800001 BIB 14 40 2217100800002 REACTION 1((3-LI-7(N,G)3-LI-8,,SIG,,SPA/AV)/ 2217100800003 (79-AU-197(N,G)79-AU-198,,SIG,,SPA)) 2217100800004 2(3-LI-7(N,G)3-LI-8,,SIG,,SPA/AV) 2217100800005 INC-SOURCE (P-LI7) Metallic layers of natural Li, 2 mg/cm2 thick 2217100800006 and 5 mm in diam., evaporated on a 1.0 mm thick water-2217100800007 cooled Cu backing. Using 1912 keV protons the 120 deg 2217100800008 forward cone of emitted neutrons closely approximates 2217100800009 to a Maxwellian kT = 25 keV shape. Total neutron rate 2217100800010 varied between 2.0E+8 and 7.0E+8 n/s 2217100800011 Monitor gold foils of 12.0 mm in diam. and 0.03 mm 2217100800012 thick were attached to the copper backing. 2217100800013 INC-SPECT The neutron spectrum is closely approximated to a 2217100800014 Maxwellian shape with temperature of 25 keV. 2217100800015 SAMPLE A 1 mm thick NE907 Li-glass scintillator, 8.1% natural2217100800016 Li, 28 mm in diam. Thickness was 1.87E-03 atoms/barn. 2217100800017 ANALYSIS Cross section value in subentry 22171.003 is 2217100800018 renormalized: 2217100800019 a) for new gold cross section 2217100800020 b) note that the quoted neutron energies refer to 2217100800021 the lab system; effective energies in the 2217100800022 c.m. system have to be reduced by 7/8 2217100800023 2Average of results from several irradiations 2217100800024 CORRECTION Correction for revised gold standard 681/648 =1.051 2217100800025 DETECTOR (SCIN) A 1 mm thick NE907 Li-glass scintillator, 8.1% 2217100800026 natural Li, 28 mm in diam, contained in a 0.5 mm thick2217100800027 Al housing, with a 2.54 cm front opening and connected2217100800028 to a 5.08 cm photomultiplier. The detector was beta 2217100800029 shielded by 0.6 mm antimony-free lead. The Li in the 2217100800030 glass scintillator also constituted the activation 2217100800031 sample in this case. 2217100800032 RAD-DET (3-LI-8,B-) 2217100800033 (4-BE-8,A) 2217100800034 DECAY-DATA (3-LI-8,0.840SEC,B-,12964.) 2217100800035 (4-BE-8,,A,1570.) 8-Be breakup producing 2 alphas. 2217100800036 MONITOR ((MONIT1)79-AU-197(N,G)79-AU-198,,SIG,,MXW) 2217100800037 MONIT-REF ((MONIT1),R.Reifarth+,J,EPJ/P,133,424,2018) 2217100800038 ERR-ANALYS (ERR-6,8.,15.) LiF activity (kT=25keV) 2217100800039 (ERR-1,2.,10.) Uncertainty due to detector efficiency 2217100800040 STATUS (TABLE) p.56 of INDC(GER)-0053 2217100800041 HISTORY (19910716C) SD 2217100800042 ENDBIB 40 0 2217100800043 COMMON 3 3 2217100800044 KT MONIT1 MONIT1-ERR 2217100800045 KEV MB PER-CENT 2217100800046 25. 681. 1.0 2217100800047 ENDCOMMON 3 0 2217100800048 DATA 4 1 2217100800049 DATA 1ERR-T 1DATA 2ERR-T 2 2217100800050 NO-DIM NO-DIM MICRO-B MICRO-B 2217100800051 3.10E-05 0.14E-05 22.1 2.0 2217100800052 ENDDATA 3 0 2217100800053 ENDSUBENT 52 0 2217100899999 ENDENTRY 8 0 2217199999999