ENTRY C2403 20190715 C186C240300000001 SUBENT C2403001 20190715 C186C240300100001 BIB 9 27 C240300100002 TITLE Partial decay widths of resonances in 29P C240300100003 AUTHOR (N.Tsoupas,H.J.Hausman,N.L.Gearhart,G.H.Terry) C240300100004 REFERENCE (J,PR/C,13,510,1976) C240300100005 #doi:10.1103/PhysRevC.13.510 C240300100006 INSTITUTE (1USAOSU) C240300100007 FACILITY (VDG,1USAOSU) The Ohio State University 7MV Van de C240300100008 Graaff accelerator. C240300100009 SAMPLE Targets were prepared by electron beam evaporation of C240300100010 natural SiO2 onto thin carbon foils. For these C240300100011 measurements the target thickness was measured as C240300100012 being 45 microg/cm2. Target thicknesses were C240300100013 determined by comparison of the measured elastic C240300100014 scattering of protons at 2 MeV with the Coulomb cross C240300100015 section. C240300100016 DETECTOR (SIBAR) Six silicon surface barrier detectors were C240300100017 used to detect the scattered protons. C240300100018 METHOD The base plate of the scattering chamber could be C240300100019 rotated so that two different angular positions of C240300100020 the base plate could provide information for 12 C240300100021 scattering angles. The proton bombarding energy was C240300100022 varied from 3.0 to 5.2 MeV and 88 angular C240300100023 distributions were measured over this energy region. C240300100024 Pileup-rejection electronics were used to correct the C240300100025 recorded spectra for pileup losses. An on-line 1800 C240300100026 computer was used to collect the spectra from the six C240300100027 proton detectors. C240300100028 HISTORY (20190715C) BP C240300100029 ENDBIB 27 0 C240300100030 COMMON 1 3 C240300100031 E-LVL C240300100032 MEV C240300100033 1.78 C240300100034 ENDCOMMON 3 0 C240300100035 ENDSUBENT 34 0 C240300199999 SUBENT C2403002 20190715 C186C240300200001 BIB 3 7 C240300200002 REACTION (14-SI-28(P,INL)14-SI-28,PAR,DA) C240300200003 ERR-ANALYS (DATA-ERR) Error shown in figure (type of uncertainty C240300200004 not explained by authors) C240300200005 (ERR-1) The inelastic proton yields were converted to C240300200006 absolute cross sections with an overall uncertainty C240300200007 of +-3%. C240300200008 STATUS (CURVE) Fig. 1, page 513. C240300200009 ENDBIB 7 0 C240300200010 COMMON 2 3 C240300200011 EN ERR-1 C240300200012 MEV PER-CENT C240300200013 3.310 3. C240300200014 ENDCOMMON 3 0 C240300200015 DATA 3 11 C240300200016 ANG-CM DATA-CM DATA-ERR C240300200017 ADEG MB/SR MB/SR C240300200018 36.630 0.931 0.326 C240300200019 41.751 0.931 C240300200020 57.112 1.490 C240300200021 67.352 1.955 C240300200022 82.713 2.607 C240300200023 101.619 3.771 C240300200024 116.980 4.516 C240300200025 126.827 4.749 C240300200026 141.007 5.261 C240300200027 150.853 5.493 C240300200028 164.245 6.006 C240300200029 ENDDATA 13 0 C240300200030 ENDSUBENT 29 0 C240300299999 SUBENT C2403003 20190715 C186C240300300001 BIB 3 7 C240300300002 REACTION (14-SI-28(P,INL)14-SI-28,PAR,DA) C240300300003 ERR-ANALYS (DATA-ERR) Error shown in figure (type of uncertainty C240300300004 not explained by authors) C240300300005 (ERR-1) The inelastic proton yields were converted C240300300006 to absolute cross sections with an overall C240300300007 uncertainty of +-3%. C240300300008 STATUS (CURVE) Fig. 1, page 513. C240300300009 ENDBIB 7 0 C240300300010 COMMON 2 3 C240300300011 EN ERR-1 C240300300012 MEV PER-CENT C240300300013 3.325 3. C240300300014 ENDCOMMON 3 0 C240300300015 DATA 3 11 C240300300016 ANG-CM DATA-CM DATA-ERR C240300300017 ADEG MB/SR MB/SR C240300300018 36.236 7.635 0.372 C240300300019 41.357 7.821 0.279 C240300300020 56.718 8.333 0.279 C240300300021 66.958 8.799 0.279 C240300300022 81.926 10.289 0.326 C240300300023 101.619 12.942 0.279 C240300300024 116.980 14.153 0.419 C240300300025 126.433 14.572 0.419 C240300300026 140.613 16.434 0.419 C240300300027 150.460 16.760 0.466 C240300300028 164.245 17.132 0.559 C240300300029 ENDDATA 13 0 C240300300030 ENDSUBENT 29 0 C240300399999 SUBENT C2403004 20190715 C186C240300400001 BIB 3 7 C240300400002 REACTION (14-SI-28(P,INL)14-SI-28,PAR,DA) C240300400003 ERR-ANALYS (DATA-ERR) Error shown in figure (type of uncertainty C240300400004 not explained by authors) C240300400005 (ERR-1) The inelastic proton yields were converted C240300400006 to absolute cross sections with an overall C240300400007 uncertainty of +-3%. C240300400008 STATUS (CURVE) Fig. 1, page 513. C240300400009 ENDBIB 7 0 C240300400010 COMMON 2 3 C240300400011 EN ERR-1 C240300400012 MEV PER-CENT C240300400013 3.340 3. C240300400014 ENDCOMMON 3 0 C240300400015 DATA 3 10 C240300400016 ANG-CM DATA-CM DATA-ERR C240300400017 ADEG MB/SR MB/SR C240300400018 35.842 16.992 0.466 C240300400019 56.324 15.829 0.512 C240300400020 66.958 15.735 0.466 C240300400021 81.926 16.480 0.466 C240300400022 101.619 18.296 0.559 C240300400023 116.193 19.274 0.512 C240300400024 126.039 19.320 0.512 C240300400025 140.613 20.624 0.559 C240300400026 150.066 21.182 0.698 C240300400027 164.245 21.229 0.605 C240300400028 ENDDATA 12 0 C240300400029 ENDSUBENT 28 0 C240300499999 SUBENT C2403005 20190715 C186C240300500001 BIB 3 7 C240300500002 REACTION (14-SI-28(P,INL)14-SI-28,PAR,DA) C240300500003 ERR-ANALYS (DATA-ERR) Error shown in figure (type of uncertainty C240300500004 not explained by authors) C240300500005 (ERR-1) The inelastic proton yields were converted C240300500006 to absolute cross sections with an overall C240300500007 uncertainty of +-3%. C240300500008 STATUS (CURVE) Fig. 1, page 513. C240300500009 ENDBIB 7 0 C240300500010 COMMON 2 3 C240300500011 EN ERR-1 C240300500012 MEV PER-CENT C240300500013 3.350 3. C240300500014 ENDCOMMON 3 0 C240300500015 DATA 3 11 C240300500016 ANG-CM DATA-CM DATA-ERR C240300500017 ADEG MB/SR MB/SR C240300500018 35.449 17.505 0.605 C240300500019 40.569 15.875 0.512 C240300500020 56.718 14.711 0.466 C240300500021 66.565 12.896 0.466 C240300500022 81.926 12.011 0.419 C240300500023 102.013 11.359 0.419 C240300500024 116.980 9.963 0.326 C240300500025 126.827 9.125 0.326 C240300500026 141.007 9.451 0.372 C240300500027 150.853 8.938 0.326 C240300500028 164.639 8.194 0.279 C240300500029 ENDDATA 13 0 C240300500030 ENDSUBENT 29 0 C240300599999 SUBENT C2403006 20190715 C186C240300600001 BIB 3 7 C240300600002 REACTION (14-SI-28(P,INL)14-SI-28,PAR,DA) C240300600003 ERR-ANALYS (DATA-ERR) Error shown in figure (type of uncertainty C240300600004 not explained by authors) C240300600005 (ERR-1) The inelastic proton yields were converted to C240300600006 absolute cross sections with an overall uncertainty C240300600007 of +-3%. C240300600008 STATUS (CURVE) Fig. 1, page 513. C240300600009 ENDBIB 7 0 C240300600010 COMMON 2 3 C240300600011 EN ERR-1 C240300600012 MEV PER-CENT C240300600013 3.365 3.0 C240300600014 ENDCOMMON 3 0 C240300600015 DATA 3 11 C240300600016 ANG-CM DATA-CM DATA-ERR C240300600017 ADEG MB/SR MB/SR C240300600018 35.842 5.680 0.279 C240300600019 41.357 5.121 C240300600020 57.112 4.609 C240300600021 67.352 4.004 C240300600022 82.713 3.398 C240300600023 102.407 2.561 C240300600024 116.980 2.048 C240300600025 127.221 1.723 C240300600026 141.400 1.210 C240300600027 150.853 1.071 C240300600028 165.427 0.931 C240300600029 ENDDATA 13 0 C240300600030 ENDSUBENT 29 0 C240300699999 SUBENT C2403007 20190715 C186C240300700001 BIB 3 11 C240300700002 REACTION (14-SI-28(P,INL)14-SI-28,PAR,DA,,LEG) C240300700003 ANALYSIS At each bombarding energy the coefficients of the C240300700004 angular distributions were extracted from the C240300700005 inelastic proton angular distributions expanded in C240300700006 terms of Legendre polynomials. C240300700007 STATUS (DEP,C2403002) C240300700008 (DEP,C2403003) C240300700009 (DEP,C2403004) C240300700010 (DEP,C2403005) C240300700011 (DEP,C2403006) C240300700012 (CURVE) Fig. 3,6, pages 514,518. C240300700013 ENDBIB 11 0 C240300700014 COMMON 1 3 C240300700015 NUMBER C240300700016 NO-DIM C240300700017 0.0 C240300700018 ENDCOMMON 3 0 C240300700019 DATA 2 81 C240300700020 EN DATA C240300700021 MEV MB/SR C240300700022 3.094 9.083 C240300700023 3.106 54.397 C240300700024 3.122 16.589 C240300700025 3.293 2.252 C240300700026 3.308 2.881 C240300700027 3.332 10.786 C240300700028 3.335 16.921 C240300700029 3.342 11.811 C240300700030 3.358 2.613 C240300700031 3.386 2.363 C240300700032 3.431 3.140 C240300700033 3.479 5.196 C240300700034 3.502 8.012 C240300700035 3.522 13.385 C240300700036 3.547 21.058 C240300700037 3.562 25.407 C240300700038 3.593 19.535 C240300700039 3.621 12.895 C240300700040 3.644 11.878 C240300700041 3.669 15.718 C240300700042 3.694 24.158 C240300700043 3.766 7.049 C240300700044 3.816 4.760 C240300700045 3.864 4.515 C240300700046 3.915 4.782 C240300700047 3.961 4.792 C240300700048 4.009 4.547 C240300700049 4.057 4.558 C240300700050 4.105 4.057 C240300700051 4.156 4.580 C240300700052 4.171 4.839 C240300700053 4.194 9.189 C240300700054 4.198 26.827 C240300700055 4.213 26.319 C240300700056 4.219 16.863 C240300700057 4.221 9.195 C240300700058 4.252 5.113 C240300700059 4.275 5.373 C240300700060 4.300 6.913 C240300700061 4.323 8.196 C240300700062 4.346 12.290 C240300700063 4.371 18.686 C240300700064 4.383 22.267 C240300700065 4.419 19.208 C240300700066 4.439 15.634 C240300700067 4.467 12.317 C240300700068 4.490 10.533 C240300700069 4.515 9.517 C240300700070 4.538 9.010 C240300700071 4.558 9.015 C240300700072 4.589 8.766 C240300700073 4.665 8.299 C240300700074 4.688 14.232 C240300700075 4.736 8.090 C240300700076 4.785 7.873 C240300700077 4.824 8.362 C240300700078 4.852 8.373 C240300700079 4.865 8.615 C240300700080 4.871 12.646 C240300700081 4.878 44.876 C240300700082 4.892 29.005 C240300700083 4.900 16.449 C240300700084 4.920 12.191 C240300700085 4.940 11.488 C240300700086 4.946 15.519 C240300700087 4.953 15.048 C240300700088 4.957 12.680 C240300700089 4.963 12.445 C240300700090 4.968 11.736 C240300700091 4.979 11.977 C240300700092 5.025 14.128 C240300700093 5.073 16.517 C240300700094 5.121 16.299 C240300700095 5.146 15.835 C240300700096 5.160 16.788 C240300700097 5.165 16.553 C240300700098 5.173 17.031 C240300700099 5.180 17.507 C240300700100 5.186 29.358 C240300700101 5.189 24.146 C240300700102 5.197 17.040 C240300700103 ENDDATA 83 0 C240300700104 ENDSUBENT 103 0 C240300799999 SUBENT C2403008 20190715 C186C240300800001 BIB 3 11 C240300800002 REACTION (14-SI-28(P,INL)14-SI-28,PAR,DA,,LEG) C240300800003 ANALYSIS At each bombarding energy the coefficients of the C240300800004 angular distributions were extracted from the C240300800005 inelastic proton angular distributions expanded in C240300800006 terms of Legendre polynomials. C240300800007 STATUS (DEP,C2403002) C240300800008 (DEP,C2403003) C240300800009 (DEP,C2403004) C240300800010 (DEP,C2403005) C240300800011 (DEP,C2403006) C240300800012 (CURVE) Fig. 3,6, pages 514,518. C240300800013 ENDBIB 11 0 C240300800014 COMMON 1 3 C240300800015 NUMBER C240300800016 NO-DIM C240300800017 1.0 C240300800018 ENDCOMMON 3 0 C240300800019 DATA 2 80 C240300800020 EN DATA C240300800021 MEV MB/SR C240300800022 3.046 -0.304 C240300800023 3.094 0.302 C240300800024 3.144 -0.607 C240300800025 3.165 -0.607 C240300800026 3.194 -0.304 C240300800027 3.292 -1.819 C240300800028 3.312 -2.728 C240300800029 3.336 -5.758 C240300800030 3.339 -2.122 C240300800031 3.348 5.150 C240300800032 3.362 2.423 C240300800033 3.383 0.605 C240300800034 3.398 -0.304 C240300800035 3.430 -0.910 C240300800036 3.478 -1.213 C240300800037 3.504 -0.910 C240300800038 3.528 -2.122 C240300800039 3.554 -2.728 C240300800040 3.566 -1.516 C240300800041 3.596 -0.607 C240300800042 3.622 -1.213 C240300800043 3.646 -1.819 C240300800044 3.676 -3.940 C240300800045 3.702 -2.425 C240300800046 3.732 2.120 C240300800047 3.770 1.514 C240300800048 3.803 0.908 C240300800049 3.823 0.605 C240300800050 3.959 0.908 C240300800051 4.018 1.211 C240300800052 4.062 1.514 C240300800053 4.104 1.211 C240300800054 4.154 -0.001 C240300800055 4.178 -1.819 C240300800056 4.195 -7.879 C240300800057 4.225 -1.819 C240300800058 4.251 -0.607 C240300800059 4.275 -2.728 C240300800060 4.305 -4.546 C240300800061 4.325 -6.667 C240300800062 4.349 -8.485 C240300800063 4.373 -10.000 C240300800064 4.384 -7.879 C240300800065 4.443 4.241 C240300800066 4.467 5.453 C240300800067 4.491 5.150 C240300800068 4.517 4.847 C240300800069 4.538 4.544 C240300800070 4.562 4.847 C240300800071 4.591 4.847 C240300800072 4.664 3.902 C240300800073 4.691 0.488 C240300800074 4.737 2.927 C240300800075 4.784 1.951 C240300800076 4.824 1.707 C240300800077 4.852 0.976 C240300800078 4.861 0.732 C240300800079 4.873 0.488 C240300800080 4.881 -2.683 C240300800081 4.892 -2.439 C240300800082 4.900 0.000 C240300800083 4.920 -0.732 C240300800084 4.941 -0.488 C240300800085 4.949 -5.366 C240300800086 4.953 -5.122 C240300800087 4.959 -2.439 C240300800088 4.963 -2.195 C240300800089 4.968 -2.439 C240300800090 4.979 -2.927 C240300800091 5.028 -4.390 C240300800092 5.076 -4.878 C240300800093 5.124 -1.220 C240300800094 5.149 -1.220 C240300800095 5.164 0.976 C240300800096 5.171 0.732 C240300800097 5.177 0.244 C240300800098 5.181 -3.902 C240300800099 5.185 -5.610 C240300800100 5.192 -3.415 C240300800101 5.200 -1.463 C240300800102 ENDDATA 82 0 C240300800103 ENDSUBENT 102 0 C240300899999 SUBENT C2403009 20190715 C186C240300900001 BIB 3 11 C240300900002 REACTION (14-SI-28(P,INL)14-SI-28,PAR,DA,,LEG) C240300900003 ANALYSIS At each bombarding energy the coefficients of the C240300900004 angular distributions were extracted from the C240300900005 inelastic proton angular distributions expanded in C240300900006 terms of Legendre polynomials. C240300900007 STATUS (DEP,C2403002) C240300900008 (DEP,C2403003) C240300900009 (DEP,C2403004) C240300900010 (DEP,C2403005) C240300900011 (DEP,C2403006) C240300900012 (CURVE) Fig. 3,6, pages 514,518. C240300900013 ENDBIB 11 0 C240300900014 COMMON 1 3 C240300900015 NUMBER C240300900016 NO-DIM C240300900017 2.0 C240300900018 ENDCOMMON 3 0 C240300900019 DATA 2 78 C240300900020 EN DATA C240300900021 MEV MB/SR C240300900022 3.096 6.256 C240300900023 3.112 33.211 C240300900024 3.143 1.495 C240300900025 3.318 -0.653 C240300900026 3.341 2.004 C240300900027 3.389 -0.090 C240300900028 3.433 -0.701 C240300900029 3.483 -1.908 C240300900030 3.504 -2.805 C240300900031 3.527 -6.371 C240300900032 3.553 -14.085 C240300900033 3.565 -19.424 C240300900034 3.595 -16.177 C240300900035 3.624 -10.560 C240300900036 3.648 -7.015 C240300900037 3.672 -5.247 C240300900038 3.698 -4.073 C240300900039 3.731 -2.309 C240300900040 3.766 -2.917 C240300900041 3.802 -2.339 C240300900042 3.817 -2.345 C240300900043 3.864 -2.365 C240300900044 3.914 -1.498 C240300900045 3.964 -1.519 C240300900046 4.009 -1.538 C240300900047 4.059 -1.855 C240300900048 4.103 -1.578 C240300900049 4.156 -1.008 C240300900050 4.168 -1.013 C240300900051 4.189 -1.021 C240300900052 4.206 -6.066 C240300900053 4.218 -7.552 C240300900054 4.248 -3.120 C240300900055 4.292 -2.547 C240300900056 4.325 -2.857 C240300900057 4.345 -2.273 C240300900058 4.366 -2.282 C240300900059 4.384 -1.104 C240300900060 4.399 -0.221 C240300900061 4.413 -0.524 C240300900062 4.443 0.056 C240300900063 4.464 0.640 C240300900064 4.490 -1.149 C240300900065 4.514 -0.863 C240300900066 4.540 -2.059 C240300900067 4.564 -1.476 C240300900068 4.588 -0.894 C240300900069 4.667 -1.325 C240300900070 4.689 -3.012 C240300900071 4.737 -1.807 C240300900072 4.785 -2.289 C240300900073 4.824 -2.771 C240300900074 4.852 -2.771 C240300900075 4.864 -2.530 C240300900076 4.871 0.361 C240300900077 4.881 6.386 C240300900078 4.891 -2.289 C240300900079 4.903 -2.771 C240300900080 4.919 -5.422 C240300900081 4.940 -5.422 C240300900082 4.949 -6.145 C240300900083 4.953 -5.422 C240300900084 4.959 -4.699 C240300900085 4.961 -5.904 C240300900086 4.967 -6.386 C240300900087 4.979 -6.627 C240300900088 5.027 -7.108 C240300900089 5.075 -8.795 C240300900090 5.123 -8.554 C240300900091 5.147 -9.518 C240300900092 5.161 -7.349 C240300900093 5.167 -8.313 C240300900094 5.171 -7.349 C240300900095 5.176 -7.831 C240300900096 5.180 -13.855 C240300900097 5.187 -15.301 C240300900098 5.189 -12.410 C240300900099 5.200 -9.759 C240300900100 ENDDATA 80 0 C240300900101 ENDSUBENT 100 0 C240300999999 SUBENT C2403010 20190715 C186C240301000001 BIB 3 11 C240301000002 REACTION (14-SI-28(P,INL)14-SI-28,PAR,DA,,LEG) C240301000003 ANALYSIS At each bombarding energy the coefficients of the C240301000004 angular distributions were extracted from the C240301000005 inelastic proton angular distributions expanded in C240301000006 terms of Legendre polynomials. C240301000007 STATUS (DEP,C2403002) C240301000008 (DEP,C2403003) C240301000009 (DEP,C2403004) C240301000010 (DEP,C2403005) C240301000011 (DEP,C2403006) C240301000012 (CURVE) Fig. 3,6, pages 514,518. C240301000013 ENDBIB 11 0 C240301000014 COMMON 1 3 C240301000015 NUMBER C240301000016 NO-DIM C240301000017 3.0 C240301000018 ENDCOMMON 3 0 C240301000019 DATA 2 70 C240301000020 EN DATA C240301000021 MEV MB/SR C240301000022 3.049 -0.590 C240301000023 3.105 0.880 C240301000024 3.126 2.938 C240301000025 3.153 0.586 C240301000026 3.197 -0.590 C240301000027 3.295 -0.296 C240301000028 3.321 -0.002 C240301000029 3.336 0.586 C240301000030 3.351 1.762 C240301000031 3.368 0.292 C240301000032 3.389 -0.296 C240301000033 3.439 -0.002 C240301000034 3.489 0.586 C240301000035 3.537 0.292 C240301000036 3.554 -0.590 C240301000037 3.599 -0.590 C240301000038 3.631 -0.590 C240301000039 3.655 0.880 C240301000040 3.678 0.586 C240301000041 3.738 2.056 C240301000042 3.749 -0.002 C240301000043 3.782 0.880 C240301000044 3.820 0.880 C240301000045 3.865 0.586 C240301000046 3.921 0.586 C240301000047 3.965 1.468 C240301000048 4.012 1.174 C240301000049 4.059 0.586 C240301000050 4.178 0.292 C240301000051 4.198 0.880 C240301000052 4.201 3.820 C240301000053 4.219 3.820 C240301000054 4.251 -0.002 C240301000055 4.302 1.468 C240301000056 4.325 1.762 C240301000057 4.349 2.350 C240301000058 4.373 2.350 C240301000059 4.384 2.938 C240301000060 4.420 2.350 C240301000061 4.443 2.056 C240301000062 4.467 1.468 C240301000063 4.520 -0.002 C240301000064 4.538 0.292 C240301000065 4.570 -0.002 C240301000066 4.666 0.006 C240301000067 4.738 -0.714 C240301000068 4.865 -1.661 C240301000069 4.872 -0.908 C240301000070 4.893 0.101 C240301000071 4.901 2.603 C240301000072 4.921 0.612 C240301000073 4.942 0.621 C240301000074 4.950 3.623 C240301000075 4.954 1.876 C240301000076 4.960 0.628 C240301000077 4.964 0.380 C240301000078 4.969 0.132 C240301000079 4.978 0.886 C240301000080 5.025 4.404 C240301000081 5.076 6.175 C240301000082 5.124 4.445 C240301000083 5.148 2.206 C240301000084 5.162 4.211 C240301000085 5.168 2.714 C240301000086 5.173 3.466 C240301000087 5.178 2.219 C240301000088 5.184 -4.777 C240301000089 5.188 -1.026 C240301000090 5.192 1.475 C240301000091 5.202 0.979 C240301000092 ENDDATA 72 0 C240301000093 ENDSUBENT 92 0 C240301099999 SUBENT C2403011 20190715 C186C240301100001 BIB 3 11 C240301100002 REACTION (14-SI-28(P,INL)14-SI-28,PAR,DA,,LEG) C240301100003 ANALYSIS At each bombarding energy the coefficients of the C240301100004 angular distributions were extracted from the C240301100005 inelastic proton angular distributions expanded in C240301100006 terms of Legendre polynomials. C240301100007 STATUS (DEP,C2403002) C240301100008 (DEP,C2403003) C240301100009 (DEP,C2403004) C240301100010 (DEP,C2403005) C240301100011 (DEP,C2403006) C240301100012 (CURVE) Fig. 3,6, pages 514,518. C240301100013 ENDBIB 11 0 C240301100014 COMMON 1 3 C240301100015 NUMBER C240301100016 NO-DIM C240301100017 4.0 C240301100018 ENDCOMMON 3 0 C240301100019 DATA 2 78 C240301100020 EN DATA C240301100021 MEV MB/SR C240301100022 3.103 1.000 C240301100023 3.129 3.000 C240301100024 3.150 0.429 C240301100025 3.173 0.714 C240301100026 3.194 -0.714 C240301100027 3.297 -0.143 C240301100028 3.315 -0.429 C240301100029 3.336 -0.143 C240301100030 3.362 0.429 C240301100031 3.395 -0.429 C240301100032 3.439 -0.143 C240301100033 3.481 0.429 C240301100034 3.513 -0.143 C240301100035 3.534 -0.429 C240301100036 3.554 -2.714 C240301100037 3.572 -1.000 C240301100038 3.599 -1.286 C240301100039 3.628 -1.000 C240301100040 3.655 -0.714 C240301100041 3.678 -1.000 C240301100042 3.705 -0.714 C240301100043 3.738 -0.714 C240301100044 3.770 -0.429 C240301100045 3.808 -0.429 C240301100046 3.826 -0.714 C240301100047 3.868 -0.429 C240301100048 3.918 0.143 C240301100049 3.965 0.143 C240301100050 4.015 -0.714 C240301100051 4.059 -0.429 C240301100052 4.107 -0.714 C240301100053 4.157 -0.714 C240301100054 4.184 -0.714 C240301100055 4.201 -2.143 C240301100056 4.210 -3.857 C240301100057 4.225 -2.143 C240301100058 4.251 0.143 C240301100059 4.278 -0.143 C240301100060 4.305 -0.429 C240301100061 4.328 -0.714 C240301100062 4.352 -0.429 C240301100063 4.373 -2.143 C240301100064 4.390 -2.429 C240301100065 4.420 -1.286 C240301100066 4.441 -0.429 C240301100067 4.473 -0.714 C240301100068 4.497 -0.429 C240301100069 4.517 -0.429 C240301100070 4.544 -0.714 C240301100071 4.568 -0.714 C240301100072 4.591 0.429 C240301100073 4.664 -0.465 C240301100074 4.784 -0.930 C240301100075 4.824 -1.163 C240301100076 4.851 -0.930 C240301100077 4.861 -1.860 C240301100078 4.873 -1.395 C240301100079 4.891 -4.651 C240301100080 4.900 -0.465 C240301100081 4.920 -1.860 C240301100082 4.939 -2.093 C240301100083 4.948 -1.628 C240301100084 4.953 -1.395 C240301100085 4.960 -1.860 C240301100086 4.963 -1.860 C240301100087 4.971 -2.326 C240301100088 4.979 -2.326 C240301100089 5.076 -3.023 C240301100090 5.123 -4.186 C240301100091 5.145 -4.651 C240301100092 5.159 -2.093 C240301100093 5.165 -3.256 C240301100094 5.171 -2.791 C240301100095 5.176 -3.721 C240301100096 5.181 -10.698 C240301100097 5.185 -5.814 C240301100098 5.189 -2.791 C240301100099 5.200 -4.651 C240301100100 ENDDATA 80 0 C240301100101 ENDSUBENT 100 0 C240301199999 ENDENTRY 11 0 C240399999999