/* 2012-10-09 File is generated by HENDEL. */ \\BIB,1[52; D#=D1686; TITLE=/ Isospin character of low-lying states in 56Fe /; ATH=(R.DE LEO'1,2', H.AKIMUNE'1', N.BLASI'3', I.DAITO'1', Y.FUJITA'4', M.FUJIWARA'1', S.I.HAYAKAWA'5', S.HATORI'6', K.HOSONO'1', H.IKEGAMI'1', T.INOMATA'1', I.KATAYAMA'1', K.KATORI'7', L.LAGAMBA'2', S.MICHELETTI'3', S.MORINOBU'1', T.NAKAGAWA'8', S.NAKAYAMA'9', A.NARITA'8', T.NORO'1', R.PERRINO'10', M.PIGNANELLI'3', H.SAKAGUCHI'6', J.TAKAMATSU'7', A.TAMII'6', K.TAMURA'1', M.TANAKA'11', A.TERAKAWA'8', T.TOHEI'8', M.TOSAKI'12', T.YAMAGATA'13', A.YAMAGOSHI'6', M.YOSIMURA'6', M.YOSOI'6'); INST-ATH=(2JPNRCN'1', 2ITYBAU'2', 2ITYMIL'3', 2JPNOSA'4', 2JPNAIT'5', 2JPNKTO'6', 2JPNOSA'7', 2JPNTOH'8', 2JPNTKS'9', 2ITYLEC'10', 2JPNKTJ'11', 2JPNKYP'12', 2JPNKON'13'); /* '2' Dipartimento di Fisica dell' Universita and Sezione INFN, Bari */ /* '3' Dipartimento di Fisica dell' Universita and Sezione INFN, Milano */ /* '4' College of General Education */ /* '6' Department of Physics */ /* '7' Department of Physics */ /* '8' Department of Physics */ /* '12' Laboratory of Applied Physics */ /* '13' Department of Physics */ REF=PR/C; VLP=53(1996)2718; RCTS=(56FE(P,P)56FE, 56FE(P,INL)56FE, 56FE(D,D)56FE, 56FE(D,INL)56FE); PHQS=(ANGL-DSTRN, VCTR-ANALPW); \\EXP,1[52; /* 2002-12-18 : Converted, Am + On. Data converted to EXFOR E1686 */ /* 2007-05-10 : Altered, On. INSTITUTE corrected */ CHM=ELM; PHYS-FORM=SLD; BAC=SELF; POL-TGT=0%; ALGN-TGT=0%; ACC=CYC'14'; /* '14' Isochronous cyclotron, AVF cyclotron */ INST-ACC=2JPNRCN; COINC=NO; ANT-COINC=NO; ANL=CC; \\EXP,1; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values */ RCT=56FE(P,P)56FE; RTY=ELA-SCATT; PHQ=ANGL-DSTRN; ENR=X%'15'; /* '15' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=65MEV; BEAM-INTNSTY=[12NA; POL-PRJ=[70%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'16',PROP-CNTR'17'); /* '16' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '17' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'18'; /* '18' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'19'; /* '19' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,1; INC-ENGY-LAB=65MEV; EXC-ENGY=0.0MEV; J-PTY=0+; \DATA; THTC DSIGMA/DOMEGA (DEG) (MB/SR) 1.416E+01 2.431E+03 1.607E+01 1.416E+03 1.819E+01 7.062E+02 2.031E+01 2.867E+02 2.137E+01 1.669E+02 2.222E+01 8.995E+01 2.328E+01 5.374E+01 2.435E+01 3.945E+01 2.541E+01 4.048E+01 2.647E+01 5.237E+01 2.838E+01 7.908E+01 3.050E+01 9.471E+01 3.305E+01 9.471E+01 3.559E+01 7.320E+01 3.814E+01 4.487E+01 4.069E+01 2.482E+01 4.302E+01 1.270E+01 4.578E+01 8.412E+00 4.811E+01 7.990E+00 5.087E+01 8.412E+00 5.342E+01 7.786E+00 5.575E+01 6.337E+00 5.809E+01 4.418E+00 6.085E+01 2.926E+00 6.339E+01 1.938E+00 6.615E+01 1.351E+00 6.849E+01 1.188E+00 7.103E+01 1.128E+00 \END; /* Scanned from Fig.2, p2720 in reference */ \\EXP,2; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=X%'20'; /* '20' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=65MEV; BEAM-INTNSTY=[12NA; POL-PRJ=[70%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'21',PROP-CNTR'22'); /* '21' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '22' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'23'; /* '23' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'24'; /* '24' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,2; INC-ENGY-LAB=65MEV; EXC-ENGY=0.846MEV; J-PTY=2+; \DATA; THTC DSIGMA/DOMEGA (DEG) (MB/SR) 1.013E+01 1.602E+01 1.327E+01 1.728E+01 1.623E+01 1.987E+01 1.920E+01 1.948E+01 2.233E+01 1.443E+01 2.545E+01 1.007E+01 2.825E+01 3.859E+00 3.155E+01 2.295E+00 3.467E+01 2.341E+00 3.747E+01 3.160E+00 4.076E+01 3.423E+00 4.373E+01 2.859E+00 4.669E+01 1.735E+00 4.982E+01 9.913E-01 5.278E+01 6.386E-01 5.591E+01 6.136E-01 5.887E+01 6.781E-01 6.184E+01 6.386E-01 6.497E+01 5.024E-01 \END; /* Scanned from Fig.2, p2720 in reference */ \\EXP,3; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=X%'25'; /* '25' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=65MEV; BEAM-INTNSTY=[12NA; POL-PRJ=[70%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'26',PROP-CNTR'27'); /* '26' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '27' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'28'; /* '28' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'29'; /* '29' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,3; INC-ENGY-LAB=65MEV; EXC-ENGY=4.510MEV; J-PTY=3-; \DATA; THTC DSIGMA/DOMEGA (DEG) (MB/SR) 1.031E+01 3.953E+00 1.327E+01 5.229E+00 1.640E+01 6.136E+00 1.936E+01 7.200E+00 2.249E+01 7.200E+00 2.562E+01 6.515E+00 2.858E+01 5.024E+00 3.171E+01 3.237E+00 3.467E+01 1.742E+00 3.764E+01 1.015E+00 4.076E+01 7.676E-01 4.389E+01 8.150E-01 4.686E+01 8.483E-01 4.998E+01 7.831E-01 5.278E+01 5.802E-01 5.591E+01 3.813E-01 5.887E+01 2.557E-01 6.200E+01 2.136E-01 6.497E+01 2.052E-01 \END; /* Scanned from Fig.2, p2720 in reference */ \\EXP,4; /* 2006-11-16 : Altered, At. Re-digitized */ RCT=56FE(P,P)56FE; RTY=ELA-SCATT; PHQ=ANGL-DSTRN; ENR=99.9%; THK-TGT=43MG/CM**2; INC-ENGY-LAB-RANGE=400MEV; BEAM-INTNSTY=[1NA; POL-PRJ=[80%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'30',SCT'31',MWDC); /* '30' Scattered protons were analyzed by using the magnetic spectrograph (Grand Raiden) operated with an opening angle of +-8.5 mrad horizontally and of +-20 mrad vertically. */ /* '31' Focal-plane counter system consists of two MWDCs to detect scattering proton [T.Noro et al., RCNP Annual Report (1991)177] and two plastic-scintillation counters placed behind the MWDCs. */ ERS-DET=[100KEV; \\DATA,4; INC-ENGY-LAB=400MEV; \DATA; THTC DSIGMA/DOMEGA (DEG) (MB/SR) 9.201E+00 2.320E+02 1.021E+01 4.289E+01 1.130E+01 1.517E+01 1.234E+01 4.278E+01 1.329E+01 5.685E+01 1.432E+01 6.988E+01 1.534E+01 5.246E+01 1.643E+01 2.884E+01 1.840E+01 9.930E+00 1.956E+01 3.165E+00 2.051E+01 1.653E+00 2.154E+01 1.784E+00 2.257E+01 3.073E+00 2.359E+01 2.767E+00 2.462E+01 3.147E+00 2.564E+01 1.601E+00 2.666E+01 1.112E+00 2.768E+01 4.715E-01 3.177E+01 1.316E-01 \END; /* Scanned from Fig.2, p2720 in reference */ \\EXP,5; /* 2006-11-16 : Altered, At. Re-digitized */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=99.9%; THK-TGT=43MG/CM**2; INC-ENGY-LAB-RANGE=400MEV; BEAM-INTNSTY=[1NA; POL-PRJ=[80%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'32',SCT'33',MWDC); /* '32' Scattered protons were analyzed by using the magnetic spectrograph (Grand Raiden) operated with an opening angle of +-8.5 mrad horizontally and of +-20 mrad vertically. */ /* '33' Focal-plane counter system consists of two MWDCs to detect scattering proton [T.Noro et al., RCNP Annual Report (1991)177] and two plastic-scintillation counters placed behind the MWDCs. */ ERS-DET=[100KEV; \\DATA,5; INC-ENGY-LAB=400MEV; EXC-ENGY=0.846MEV; J-PTY=2+; \DATA; THTC DSIGMA/DOMEGA (DEG) (MB/SR) 7.766E+00 2.232E+01 9.231E+00 2.287E+01 1.018E+01 2.226E+01 1.120E+01 1.256E+01 1.229E+01 5.327E+00 1.331E+01 1.934E+00 1.440E+01 5.703E-01 1.543E+01 9.326E-01 1.646E+01 1.977E+00 1.742E+01 2.991E+00 1.845E+01 3.975E+00 1.961E+01 2.833E+00 2.049E+01 2.240E+00 2.158E+01 1.001E+00 2.260E+01 4.961E-01 2.362E+01 1.897E-01 2.464E+01 2.048E-01 2.567E+01 1.750E-01 2.670E+01 3.711E-01 2.773E+01 3.172E-01 3.173E+01 3.662E-02 \END; /* Scanned from Fig.2, p2720 in reference */ \\EXP,6; /* 2006-11-16 : Altered, At. Re-digitized */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=99.9%; THK-TGT=43MG/CM**2; INC-ENGY-LAB-RANGE=400MEV; BEAM-INTNSTY=[1NA; POL-PRJ=[80%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'34',SCT'35',MWDC); /* '34' Scattered protons were analyzed by using the magnetic spectrograph (Grand Raiden) operated with an opening angle of +-8.5 mrad horizontally and of +-20 mrad vertically. */ /* '35' Focal-plane counter system consists of two MWDCs to detect scattering proton [T.Noro et al., RCNP Annual Report (1991)177] and two plastic-scintillation counters placed behind the MWDCs. */ ERS-DET=[100KEV; \\DATA,6; INC-ENGY-LAB=400MEV; EXC-ENGY=4.510MEV; J-PTY=3-; \DATA; THTC DSIGMA/DOMEGA (DEG) (MB/SR) 7.783E+00 5.418E+00 9.179E+00 8.629E+00 1.028E+01 1.305E+01 1.131E+01 1.116E+01 1.233E+01 1.058E+01 1.335E+01 7.944E+00 1.438E+01 5.376E+00 1.736E+01 9.915E-01 1.846E+01 8.046E-01 1.956E+01 8.463E-01 2.051E+01 1.068E+00 2.161E+01 8.665E-01 2.256E+01 9.854E-01 2.359E+01 6.331E-01 2.468E+01 4.878E-01 2.570E+01 2.356E-01 2.664E+01 7.511E-02 3.177E+01 5.328E-02 \END; /* Scanned from Fig.2, p2720 in reference */ \\EXP,7; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values, DATA-CM -> DATA */ RCT=56FE(P,P)56FE; RTY=ELA-SCATT; PHQ=VCTR-ANALPW; ENR=X%'36'; /* '36' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=65MEV; BEAM-INTNSTY=[12NA; POL-PRJ=[70%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'37',PROP-CNTR'38'); /* '37' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '38' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'39'; /* '39' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'40'; /* '40' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,7; INC-ENGY-LAB=65MEV; \DATA; THTC AY (DEG) (NODIM) 1.437E+01 -1.053E-02 1.633E+01 -5.072E-02 1.846E+01 -1.210E-01 2.026E+01 -2.315E-01 2.140E+01 -2.717E-01 2.238E+01 -1.813E-01 2.353E+01 9.556E-03 2.435E+01 5.018E-01 2.549E+01 8.031E-01 2.647E+01 8.534E-01 2.844E+01 6.725E-01 3.056E+01 5.219E-01 3.318E+01 4.013E-01 3.547E+01 3.009E-01 3.809E+01 2.004E-01 4.070E+01 2.004E-01 4.316E+01 3.511E-01 4.561E+01 7.328E-01 5.314E+01 8.634E-01 5.559E+01 8.031E-01 5.804E+01 7.027E-01 6.050E+01 6.022E-01 6.311E+01 5.721E-01 6.573E+01 6.123E-01 6.802E+01 7.228E-01 7.064E+01 8.433E-01 \END; /* Scanned from Fig.2, p2720 in reference */ \\EXP,8; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values, DATA-CM -> DATA */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=VCTR-ANALPW; ENR=X%'41'; /* '41' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=65MEV; BEAM-INTNSTY=[12NA; POL-PRJ=[70%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'42',PROP-CNTR'43'); /* '42' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '43' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'44'; /* '44' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'45'; /* '45' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,8; INC-ENGY-LAB=65MEV; EXC-ENGY=0.846MEV; J-PTY=2+; \DATA; THTC AY (DEG) (NODIM) 1.042E+01 -3.366E-02 1.353E+01 -3.366E-02 1.632E+01 -4.374E-02 1.959E+01 -5.382E-02 2.270E+01 -9.416E-02 2.582E+01 -1.042E-01 2.876E+01 -5.382E-02 3.155E+01 4.706E-01 3.482E+01 8.538E-01 3.761E+01 6.924E-01 4.072E+01 5.512E-01 4.383E+01 4.000E-01 4.678E+01 2.991E-01 4.989E+01 3.092E-01 5.284E+01 5.512E-01 5.578E+01 8.739E-01 5.873E+01 9.143E-01 6.168E+01 9.042E-01 6.495E+01 8.538E-01 \END; /* Scanned from Fig.2, p2720 in reference */ \\EXP,9; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values, DATA-CM -> DATA */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=VCTR-ANALPW; ENR=X%'46'; /* '46' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=65MEV; BEAM-INTNSTY=[12NA; POL-PRJ=[70%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'47',PROP-CNTR'48'); /* '47' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '48' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'49'; /* '49' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'50'; /* '50' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,9; INC-ENGY-LAB=65MEV; EXC-ENGY=4.510MEV; J-PTY=3-; \DATA; THTC AY (DEG) (NODIM) 1.039E+01 2.176E-02 1.351E+01 6.202E-02 1.647E+01 2.176E-02 1.959E+01 -8.444E-03 2.271E+01 -4.871E-02 2.567E+01 -7.891E-02 2.862E+01 -1.091E-01 3.158E+01 -1.091E-01 3.487E+01 -5.878E-02 3.766E+01 2.332E-01 4.078E+01 7.163E-01 4.390E+01 8.170E-01 4.669E+01 7.063E-01 4.998E+01 5.553E-01 5.277E+01 4.446E-01 5.589E+01 3.942E-01 5.901E+01 3.842E-01 6.197E+01 5.553E-01 6.493E+01 6.962E-01 \END; /* Scanned from Fig.2, p2720 in reference */ \\EXP,10; /* 2006-11-16 : Altered, At. Re-digitized */ RCT=56FE(P,P)56FE; RTY=ELA-SCATT; PHQ=VCTR-ANALPW; ENR=99.9%; THK-TGT=43MG/CM**2; INC-ENGY-LAB-RANGE=400MEV; BEAM-INTNSTY=[1NA; POL-PRJ=[80%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'51',SCT'52',MWDC); /* '51' Scattered protons were analyzed by using the magnetic spectrograph (Grand Raiden) operated with an opening angle of +-8.5 mrad horizontally and of +-20 mrad vertically. */ /* '52' Focal-plane counter system consists of two MWDCs to detect scattering proton [T.Noro et al., RCNP Annual Report (1991)177] and two plastic-scintillation counters placed behind the MWDCs. */ ERS-DET=[100KEV; \\DATA,10; INC-ENGY-LAB=400MEV; \DATA; THTC AY (DEG) (NODIM) 9.313E+00 3.814E-01 1.026E+01 2.009E-01 1.129E+01 6.601E-01 1.239E+01 9.194E-01 1.341E+01 8.189E-01 1.443E+01 7.883E-01 1.544E+01 7.177E-01 1.646E+01 5.672E-01 1.856E+01 7.623E-02 1.949E+01 -2.841E-01 2.052E+01 -1.048E-01 2.156E+01 7.042E-01 2.259E+01 8.836E-01 2.361E+01 8.430E-01 2.462E+01 7.025E-01 2.564E+01 6.319E-01 2.658E+01 3.415E-01 2.774E+01 3.100E-02 3.177E+01 7.784E-01 \END; /* Scanned from Fig.2, p2720 in reference */ \\EXP,11; /* 2006-11-16 : Altered, At. Re-digitized */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=VCTR-ANALPW; ENR=99.9%; THK-TGT=43MG/CM**2; INC-ENGY-LAB-RANGE=400MEV; BEAM-INTNSTY=[1NA; POL-PRJ=[80%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'53',SCT'54',MWDC); /* '53' Scattered protons were analyzed by using the magnetic spectrograph (Grand Raiden) operated with an opening angle of +-8.5 mrad horizontally and of +-20 mrad vertically. */ /* '54' Focal-plane counter system consists of two MWDCs to detect scattering proton [T.Noro et al., RCNP Annual Report (1991)177] and two plastic-scintillation counters placed behind the MWDCs. */ ERS-DET=[100KEV; \\DATA,11; INC-ENGY-LAB=400MEV; EXC-ENGY=0.846MEV; J-PTY=2+; \DATA; THTC AY DELTA-AY (DEG) (NODIM) (NODIM) 7.818E+00 5.319E-01 +-NEGLIGIBLE 9.273E+00 5.319E-01 +-NEGLIGIBLE 1.022E+01 5.520E-01 +-NEGLIGIBLE 1.131E+01 4.312E-01 +-NEGLIGIBLE 1.225E+01 3.406E-01 +-NEGLIGIBLE 1.327E+01 5.878E-02 +-NEGLIGIBLE 1.436E+01 -2.332E-01 +-NEGLIGIBLE 1.531E+01 8.238E-01 +-NEGLIGIBLE 1.742E+01 9.346E-01 +-NEGLIGIBLE 1.844E+01 7.735E-01 +-NEGLIGIBLE 1.938E+01 6.829E-01 +-NEGLIGIBLE 2.047E+01 4.816E-01 +-NEGLIGIBLE 2.149E+01 2.601E-01 +-NEGLIGIBLE 2.251E+01 -2.936E-01 +-NEGLIGIBLE 2.353E+01 -4.345E-01 +-NEGLIGIBLE 2.455E+01 3.507E-01 +-NEGLIGIBLE 2.556E+01 8.037E-01 +-8.053E-02 2.651E+01 8.641E-01 +-8.053E-02 2.760E+01 7.534E-01 +-NEGLIGIBLE 3.167E+01 -3.338E-01 +-NEGLIGIBLE \END; /* Scanned from Fig.2, p2720 in reference */ \\EXP,12; /* 2006-11-16 : Altered, At. Re-digitized */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=VCTR-ANALPW; ENR=99.9%; THK-TGT=43MG/CM**2; INC-ENGY-LAB-RANGE=400MEV; BEAM-INTNSTY=[1NA; POL-PRJ=[80%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'55',SCT'56',MWDC); /* '55' Scattered protons were analyzed by using the magnetic spectrograph (Grand Raiden) operated with an opening angle of +-8.5 mrad horizontally and of +-20 mrad vertically. */ /* '56' Focal-plane counter system consists of two MWDCs to detect scattering proton [T.Noro et al., RCNP Annual Report (1991)177] and two plastic-scintillation counters placed behind the MWDCs. */ ERS-DET=[100KEV; \\DATA,12; INC-ENGY-LAB=400MEV; EXC-ENGY=4.510MEV; J-PTY=3-; \DATA; THTC AY DELTA-AY (DEG) (NODIM) (NODIM) 7.813E+00 5.519E-01 +-NEGLIGIBLE 9.271E+00 5.915E-01 +-NEGLIGIBLE 1.022E+01 6.614E-01 +-NEGLIGIBLE 1.131E+01 5.906E-01 +-NEGLIGIBLE 1.233E+01 6.203E-01 +-NEGLIGIBLE 1.335E+01 5.495E-01 +-NEGLIGIBLE 1.437E+01 4.988E-01 +-NEGLIGIBLE 1.742E+01 -7.536E-02 +-NEGLIGIBLE 1.845E+01 4.569E-01 +-NEGLIGIBLE 1.947E+01 7.278E-01 +-NEGLIGIBLE 2.050E+01 7.977E-01 +-NEGLIGIBLE 2.151E+01 6.968E-01 +-NEGLIGIBLE 2.246E+01 6.461E-01 +-NEGLIGIBLE 2.355E+01 4.748E-01 +-NEGLIGIBLE 2.456E+01 2.934E-01 +-NEGLIGIBLE 2.558E+01 1.422E-01 +-NEGLIGIBLE 2.660E+01 2.120E-02 +-9.045E-02 3.171E+01 7.225E-01 +-1.508E-01 \END; /* Scanned from Fig.2, p2720 in reference */ \\EXP,13; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values */ RCT=56FE(D,D)56FE; RTY=ELA-SCATT; PHQ=ANGL-DSTRN; ENR=X%'57'; /* '57' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=56MEV; BEAM-INTNSTY=[60NA; POL-PRJ=0%; DET-PARTCL=D; DET-SYS=(MAG'58',PROP-CNTR'59'); /* '58' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '59' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'60'; /* '60' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'61'; /* '61' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,13; INC-ENGY-LAB=56MEV; EXC-ENGY=0.0MEV; J-PTY=0+; \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 1.504E+01 8.686E+01 +-1.638E+01 1.816E+01 2.978E+02 +-NEGLIGIBLE 2.110E+01 2.114E+02 +-NEGLIGIBLE 2.405E+01 6.728E+01 +-NEGLIGIBLE 2.618E+01 5.574E+00 +-NEGLIGIBLE 2.911E+01 4.833E+00 +-NEGLIGIBLE 3.120E+01 1.209E+01 +-NEGLIGIBLE 3.413E+01 9.087E+00 +-NEGLIGIBLE 3.709E+01 2.436E+00 +-NEGLIGIBLE 3.919E+01 1.335E+00 +-NEGLIGIBLE 4.106E+01 3.438E+00 +-NEGLIGIBLE 4.441E+01 5.441E+00 +-NEGLIGIBLE 4.713E+01 5.291E+00 +-NEGLIGIBLE 4.923E+01 3.348E+00 +-NEGLIGIBLE 5.217E+01 2.119E+00 +-NEGLIGIBLE 5.427E+01 1.686E+00 +-NEGLIGIBLE 5.721E+01 1.787E+00 +-NEGLIGIBLE 5.909E+01 1.688E+00 +-NEGLIGIBLE 6.203E+01 1.343E+00 +-NEGLIGIBLE \END; /* Scanned from Fig.3, p2720 in reference */ \\EXP,14; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values */ RCT=56FE(D,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=X%'62'; /* '62' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=56MEV; BEAM-INTNSTY=[60NA; POL-PRJ=0%; DET-PARTCL=D; DET-SYS=(MAG'63',PROP-CNTR'64'); /* '63' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '64' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'65'; /* '65' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'66'; /* '66' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,14; INC-ENGY-LAB=56MEV; EXC-ENGY=0.846MEV; J-PTY=2+; \DATA; THTC DSIGMA/DOMEGA (DEG) (MB/SR) 1.025E+01 2.605E+01 1.259E+01 2.038E+01 1.490E+01 8.938E+00 1.766E+01 1.841E+00 1.995E+01 3.048E+00 2.287E+01 6.349E+00 2.497E+01 6.208E+00 2.770E+01 4.207E+00 3.023E+01 1.888E+00 3.274E+01 1.889E+00 3.504E+01 2.790E+00 3.755E+01 3.059E+00 4.007E+01 2.434E+00 4.259E+01 1.576E+00 4.511E+01 1.313E+00 4.741E+01 1.407E+00 5.014E+01 1.507E+00 5.265E+01 1.315E+00 5.517E+01 9.327E-01 5.769E+01 7.089E-01 6.021E+01 6.325E-01 \END; /* Scanned from Fig.3, p2720 in reference */ \\EXP,15; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values */ RCT=56FE(D,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=X%'67'; /* '67' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=56MEV; BEAM-INTNSTY=[60NA; POL-PRJ=0%; DET-PARTCL=D; DET-SYS=(MAG'68',PROP-CNTR'69'); /* '68' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '69' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'70'; /* '70' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'71'; /* '71' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,15; INC-ENGY-LAB=56MEV; EXC-ENGY=4.510MEV; J-PTY=3-; \DATA; THTC DSIGMA/DOMEGA (DEG) (MB/SR) 1.034E+01 5.213E+00 1.285E+01 6.265E+00 1.579E+01 5.590E+00 1.831E+01 3.967E+00 2.084E+01 1.482E+00 2.338E+01 4.303E-01 2.609E+01 6.503E-01 2.860E+01 1.294E+00 3.111E+01 1.451E+00 3.384E+01 1.030E+00 3.615E+01 5.945E-01 3.909E+01 4.953E-01 4.139E+01 5.952E-01 4.411E+01 6.526E-01 4.684E+01 5.313E-01 5.188E+01 3.603E-01 5.439E+01 3.289E-01 \END; /* Scanned from Fig.3, p2720 in reference */ \\EXP,16; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values */ RCT=56FE(D,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=X%'72'; /* '72' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=56MEV; BEAM-INTNSTY=[60NA; POL-PRJ=0%; DET-PARTCL=D; DET-SYS=(MAG'73',PROP-CNTR'74'); /* '73' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '74' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'75'; /* '75' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'76'; /* '76' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,16; INC-ENGY-LAB=56MEV; EXC-ENGY=2.657MEV; J-PTY=2+; \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 1.069E+01 1.999E+00 +-NEGLIGIBLE 1.322E+01 1.677E+00 +-NEGLIGIBLE 1.550E+01 6.463E-01 +-NEGLIGIBLE 1.824E+01 1.010E-01 +-1.836E-02 2.055E+01 2.197E-01 +-NEGLIGIBLE 2.309E+01 5.987E-01 +-NEGLIGIBLE 2.540E+01 7.500E-01 +-NEGLIGIBLE 2.815E+01 5.411E-01 +-NEGLIGIBLE 3.044E+01 2.680E-01 +-NEGLIGIBLE 3.297E+01 1.886E-01 +-NEGLIGIBLE 3.573E+01 1.982E-01 +-NEGLIGIBLE 3.803E+01 2.190E-01 +-NEGLIGIBLE 4.056E+01 1.884E-01 +-NEGLIGIBLE 4.309E+01 1.541E-01 +-NEGLIGIBLE 4.560E+01 6.903E-02 +-NEGLIGIBLE 4.813E+01 5.506E-02 +-NEGLIGIBLE 5.066E+01 5.367E-02 +-NEGLIGIBLE 5.296E+01 5.501E-02 +-NEGLIGIBLE 5.549E+01 4.173E-02 +-NEGLIGIBLE 5.824E+01 3.011E-02 +-NEGLIGIBLE 6.054E+01 2.655E-02 +-NEGLIGIBLE \END; /* Scanned from Fig.3, p2720 in reference */ \\EXP,17; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values */ RCT=56FE(D,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=X%'77'; /* '77' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=56MEV; BEAM-INTNSTY=[60NA; POL-PRJ=0%; DET-PARTCL=D; DET-SYS=(MAG'78',PROP-CNTR'79'); /* '78' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '79' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'80'; /* '80' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'81'; /* '81' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,17; INC-ENGY-LAB=56MEV; EXC-ENGY=2.960MEV; J-PTY=2+; \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 1.294E+01 1.256E-01 +-NEGLIGIBLE 1.547E+01 9.062E-02 +-NEGLIGIBLE 1.799E+01 8.615E-02 +-NEGLIGIBLE 2.052E+01 6.536E-02 +-NEGLIGIBLE 2.328E+01 7.222E-02 +-NEGLIGIBLE 2.536E+01 8.823E-02 +-NEGLIGIBLE 2.812E+01 8.600E-02 +-NEGLIGIBLE 3.042E+01 8.815E-02 +-NEGLIGIBLE 3.294E+01 7.393E-02 +-NEGLIGIBLE 3.547E+01 5.334E-02 +-NEGLIGIBLE 4.052E+01 3.659E-02 +-NEGLIGIBLE 4.305E+01 3.226E-02 +-NEGLIGIBLE 4.788E+01 2.158E-02 +-NEGLIGIBLE 5.087E+01 1.856E-02 +-NEGLIGIBLE 5.293E+01 1.637E-02 +-NEGLIGIBLE 5.546E+01 1.338E-02 +-1.788E-03 5.799E+01 9.418E-03 +-1.315E-03 \END; /* Scanned from Fig.3, p2720 in reference */ \\EXP,18; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values */ RCT=56FE(D,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=X%'82'; /* '82' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=56MEV; BEAM-INTNSTY=[60NA; POL-PRJ=0%; DET-PARTCL=D; DET-SYS=(MAG'83',PROP-CNTR'84'); /* '83' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '84' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'85'; /* '85' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'86'; /* '86' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,18; INC-ENGY-LAB=56MEV; EXC-ENGY=3.370MEV; J-PTY=2+; \DATA; THTC DSIGMA/DOMEGA (DEG) (MB/SR) 1.001E+01 1.067E+00 1.232E+01 8.728E-01 1.509E+01 3.999E-01 1.787E+01 1.224E-01 2.018E+01 9.763E-02 2.269E+01 2.815E-01 2.498E+01 4.215E-01 2.774E+01 3.448E-01 3.005E+01 2.364E-01 3.259E+01 1.541E-01 3.512E+01 1.261E-01 3.765E+01 1.431E-01 4.018E+01 1.396E-01 4.249E+01 9.332E-02 4.526E+01 6.901E-02 4.756E+01 5.644E-02 5.032E+01 5.648E-02 5.262E+01 5.373E-02 5.515E+01 4.622E-02 5.769E+01 3.169E-02 6.022E+01 2.527E-02 \END; /* Scanned from Fig.3, p2720 in reference */ \\EXP,19; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values */ RCT=56FE(D,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=X%'87'; /* '87' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=56MEV; BEAM-INTNSTY=[60NA; POL-PRJ=0%; DET-PARTCL=D; DET-SYS=(MAG'88',PROP-CNTR'89'); /* '88' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '89' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'90'; /* '90' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'91'; /* '91' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,19; INC-ENGY-LAB=56MEV; EXC-ENGY=3.602MEV; J-PTY=2+; \DATA; THTC DSIGMA/DOMEGA (DEG) (MB/SR) 1.007E+01 5.884E-01 1.260E+01 4.693E-01 1.515E+01 2.319E-01 1.770E+01 5.658E-02 2.000E+01 6.262E-02 2.274E+01 1.674E-01 2.504E+01 2.324E-01 2.780E+01 1.554E-01 3.011E+01 9.393E-02 3.265E+01 6.441E-02 3.518E+01 6.777E-02 3.771E+01 7.132E-02 4.001E+01 7.136E-02 4.255E+01 5.277E-02 4.531E+01 3.902E-02 4.761E+01 3.904E-02 5.037E+01 4.661E-02 5.267E+01 4.111E-02 5.521E+01 2.136E-02 5.775E+01 1.580E-02 6.028E+01 1.292E-02 \END; /* Scanned from Fig.3, p2720 in reference */ \\EXP,20; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values */ RCT=56FE(D,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=X%'92'; /* '92' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=56MEV; BEAM-INTNSTY=[60NA; POL-PRJ=0%; DET-PARTCL=D; DET-SYS=(MAG'93',PROP-CNTR'94'); /* '93' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '94' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'95'; /* '95' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'96'; /* '96' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,20; INC-ENGY-LAB=56MEV; EXC-ENGY=3.832MEV; J-PTY=2+; \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 1.000E+01 4.467E-01 +-NEGLIGIBLE 1.254E+01 3.302E-01 +-NEGLIGIBLE 1.511E+01 1.399E-01 +-NEGLIGIBLE 1.770E+01 3.069E-02 +-6.863E-03 1.998E+01 5.227E-02 +-7.366E-03 2.270E+01 1.301E-01 +-NEGLIGIBLE 2.500E+01 1.405E-01 +-NEGLIGIBLE 2.754E+01 1.121E-01 +-NEGLIGIBLE 3.010E+01 5.253E-02 +-8.611E-03 3.265E+01 3.171E-02 +-5.150E-03 3.517E+01 4.089E-02 +-6.629E-03 3.770E+01 4.307E-02 +-5.802E-03 4.023E+01 4.536E-02 +-7.423E-03 4.253E+01 3.709E-02 +-9.715E-03 4.532E+01 1.783E-02 +-3.633E-03 4.763E+01 1.655E-02 +-3.371E-03 5.017E+01 1.254E-02 +-2.298E-03 5.524E+01 8.604E-03 +-1.752E-03 5.778E+01 7.591E-03 +-1.547E-03 6.031E+01 6.698E-03 +-1.364E-03 \END; /* Scanned from Fig.3, p2720 in reference */ \\EXP,21; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=X%'97'; /* '97' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=65MEV; BEAM-INTNSTY=[12NA; POL-PRJ=[70%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'98',PROP-CNTR'99'); /* '98' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '99' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'100'; /* '100' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'101'; /* '101' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,21; INC-ENGY-LAB=65MEV; EXC-ENGY=2.657MEV; J-PTY=2+; \DATA; THTC DSIGMA/DOMEGA (DEG) (MB/SR) 9.744E+00 1.870E+00 1.274E+01 1.590E+00 1.591E+01 1.458E+00 1.907E+01 1.253E+00 2.207E+01 8.045E-01 2.523E+01 3.899E-01 2.823E+01 1.226E-01 3.122E+01 7.538E-02 3.439E+01 1.660E-01 3.739E+01 2.642E-01 4.039E+01 2.880E-01 4.339E+01 2.422E-01 4.639E+01 1.505E-01 4.955E+01 8.863E-02 5.255E+01 5.567E-02 5.554E+01 5.051E-02 5.871E+01 4.996E-02 6.171E+01 5.567E-02 6.454E+01 4.682E-02 \END; /* Scanned from Fig.4, p2721 in reference */ \\EXP,22; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2011-02-14 : Altered, Nf. Heading corrected */ /* 2012-07-31 : Altered, VD. Corrected isotopic abundance values */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=X%'102'; /* '102' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=65MEV; BEAM-INTNSTY=[12NA; POL-PRJ=[70%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'103',PROP-CNTR'104'); /* '103' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '104' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'105'; /* '105' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'106'; /* '106' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,22; INC-ENGY-LAB=65MEV; EXC-ENGY=2.960MEV; J-PTY=2+; \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 9.731E+00 1.795E-01 +-NEGLIGIBLE 1.290E+01 1.446E-01 +-NEGLIGIBLE 1.606E+01 1.152E-01 +-NEGLIGIBLE 1.906E+01 1.190E-01 +-NEGLIGIBLE 2.206E+01 1.256E-01 +-NEGLIGIBLE 2.506E+01 1.270E-01 +-NEGLIGIBLE 2.822E+01 1.243E-01 +-NEGLIGIBLE 3.105E+01 1.057E-01 +-NEGLIGIBLE 3.438E+01 7.395E-02 +-NEGLIGIBLE 3.738E+01 5.065E-02 +-NEGLIGIBLE 4.038E+01 4.036E-02 +-NEGLIGIBLE 4.354E+01 3.742E-02 +-NEGLIGIBLE 4.654E+01 3.080E-02 +-NEGLIGIBLE 5.270E+01 2.227E-02 +-NEGLIGIBLE 5.570E+01 1.627E-02 +-NEGLIGIBLE 5.870E+01 1.067E-02 +-1.091E-03 6.470E+01 9.274E-03 +-8.598E-04 \END; /* Scanned from Fig.4, p2721 in reference */ \\EXP,23; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2011-02-14 : Altered, Nf. Heading corrected */ /* 2012-07-31 : Altered, VD. Corrected isotopic abundance values */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=X%'107'; /* '107' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=65MEV; BEAM-INTNSTY=[12NA; POL-PRJ=[70%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'108',PROP-CNTR'109'); /* '108' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '109' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'110'; /* '110' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'111'; /* '111' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,23; INC-ENGY-LAB=65MEV; EXC-ENGY=3.370MEV; J-PTY=2+; \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 9.724E+00 1.267E+00 +-NEGLIGIBLE 1.289E+01 1.090E+00 +-NEGLIGIBLE 1.605E+01 1.067E+00 +-NEGLIGIBLE 1.889E+01 1.033E+00 +-NEGLIGIBLE 2.205E+01 8.235E-01 +-NEGLIGIBLE 2.505E+01 5.771E-01 +-4.191E-02 2.821E+01 3.090E-01 +-NEGLIGIBLE 3.121E+01 1.363E-01 +-9.897E-03 3.437E+01 1.019E-01 +-NEGLIGIBLE 3.737E+01 1.250E-01 +-NEGLIGIBLE 4.037E+01 1.654E-01 +-NEGLIGIBLE 4.337E+01 1.765E-01 +-NEGLIGIBLE 4.653E+01 1.453E-01 +-NEGLIGIBLE 4.953E+01 1.135E-01 +-NEGLIGIBLE 5.253E+01 1.098E-01 +-NEGLIGIBLE 5.569E+01 7.373E-02 +-NEGLIGIBLE 5.869E+01 6.692E-02 +-NEGLIGIBLE 6.169E+01 6.073E-02 +-NEGLIGIBLE 6.469E+01 5.112E-02 +-NEGLIGIBLE \END; /* Scanned from Fig.4, p2721 in reference */ \\EXP,24; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=X%'112'; /* '112' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=65MEV; BEAM-INTNSTY=[12NA; POL-PRJ=[70%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'113',PROP-CNTR'114'); /* '113' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '114' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'115'; /* '115' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'116'; /* '116' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,24; INC-ENGY-LAB=65MEV; EXC-ENGY=3.602MEV; J-PTY=2+; \DATA; THTC DSIGMA/DOMEGA (DEG) (MB/SR) 1.005E+01 8.042E-01 1.305E+01 6.991E-01 1.621E+01 6.991E-01 1.921E+01 7.066E-01 2.221E+01 5.340E-01 2.537E+01 3.508E-01 2.837E+01 2.004E-01 3.137E+01 1.208E-01 3.453E+01 1.108E-01 3.753E+01 1.419E-01 4.053E+01 1.514E-01 4.353E+01 1.419E-01 4.669E+01 9.028E-02 4.969E+01 5.995E-02 5.268E+01 3.814E-02 5.885E+01 3.244E-02 6.185E+01 3.041E-02 6.501E+01 2.731E-02 \END; /* Scanned from Fig.4, p2721 in reference */ \\EXP,25; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=X%'117'; /* '117' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=65MEV; BEAM-INTNSTY=[12NA; POL-PRJ=[70%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'118',PROP-CNTR'119'); /* '118' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '119' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'120'; /* '120' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'121'; /* '121' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,25; INC-ENGY-LAB=65MEV; EXC-ENGY=3.832MEV; J-PTY=2+; \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 1.004E+01 3.317E-01 +-3.706E-02 1.303E+01 2.617E-01 +-2.673E-02 1.620E+01 2.427E-01 +-2.712E-02 1.920E+01 2.021E-01 +-2.064E-02 2.220E+01 1.416E-01 +-1.446E-02 2.552E+01 8.003E-02 +-6.607E-03 2.835E+01 3.847E-02 +-4.839E-03 3.135E+01 3.645E-02 +-4.420E-03 3.452E+01 5.257E-02 +-5.368E-03 3.769E+01 6.735E-02 +-6.061E-03 4.068E+01 7.184E-02 +-6.465E-03 4.385E+01 5.792E-02 +-7.022E-03 4.685E+01 4.059E-02 +-5.681E-03 5.001E+01 2.197E-02 +-3.575E-03 5.317E+01 1.215E-02 +-2.032E-03 5.600E+01 9.793E-03 +-2.066E-03 6.183E+01 9.792E-03 +-1.982E-03 6.517E+01 1.215E-02 +-2.354E-03 \END; /* Scanned from Fig.4, p2721 in reference */ \\EXP,26; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values, DATA-CM -> DATA */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=VCTR-ANALPW; ENR=X%'122'; /* '122' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=65MEV; BEAM-INTNSTY=[12NA; POL-PRJ=[70%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'123',PROP-CNTR'124'); /* '123' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '124' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'125'; /* '125' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'126'; /* '126' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,26; INC-ENGY-LAB=65MEV; EXC-ENGY=2.657MEV; J-PTY=2+; \DATA; THTC AY (DEG) (NODIM) 1.030E+01 7.890E-02 1.328E+01 6.551E-02 1.643E+01 4.557E-02 1.941E+01 -6.971E-03 2.256E+01 -3.343E-02 2.554E+01 -6.640E-02 2.853E+01 -2.107E-02 3.172E+01 5.267E-01 3.469E+01 3.632E-01 3.767E+01 2.454E-01 4.081E+01 8.845E-02 4.379E+01 6.854E-02 4.677E+01 -6.884E-02 4.992E+01 -1.047E-02 5.294E+01 3.872E-01 5.596E+01 9.611E-01 5.895E+01 9.412E-01 6.193E+01 9.474E-01 6.507E+01 8.100E-01 \END; /* Scanned from Fig.4, p2721 in reference */ \\EXP,27; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values, DATA-CM -> DATA */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=VCTR-ANALPW; ENR=X%'127'; /* '127' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=65MEV; BEAM-INTNSTY=[12NA; POL-PRJ=[70%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'128',PROP-CNTR'129'); /* '128' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '129' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'130'; /* '130' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'131'; /* '131' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,27; INC-ENGY-LAB=65MEV; EXC-ENGY=2.960MEV; J-PTY=2+; \DATA; THTC AY DELTA-AY (DEG) (NODIM) (NODIM) 1.038E+01 -6.681E-03 +-8.469E-02 1.354E+01 -1.325E-02 +-7.818E-02 1.636E+01 6.240E-03 +-6.515E-02 1.951E+01 -1.336E-02 +-5.863E-02 2.267E+01 -8.508E-02 +-NEGLIGIBLE 2.549E+01 -1.763E-01 +-NEGLIGIBLE 2.848E+01 -1.438E-01 +-NEGLIGIBLE 3.180E+01 -9.828E-02 +-NEGLIGIBLE 3.479E+01 5.151E-02 +-5.211E-02 3.778E+01 2.795E-01 +-5.864E-02 4.077E+01 5.465E-01 +-5.863E-02 4.392E+01 5.530E-01 +-6.515E-02 4.691E+01 5.529E-01 +-7.166E-02 5.305E+01 4.160E-01 +-5.863E-02 5.604E+01 2.856E-01 +-8.469E-02 5.902E+01 4.289E-01 +-1.107E-01 \END; /* Scanned from Fig.4, p2721 in reference */ \\EXP,28; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values, DATA-CM -> DATA */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=VCTR-ANALPW; ENR=X%'132'; /* '132' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=65MEV; BEAM-INTNSTY=[12NA; POL-PRJ=[70%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'133',PROP-CNTR'134'); /* '133' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '134' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'135'; /* '135' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'136'; /* '136' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,28; INC-ENGY-LAB=65MEV; EXC-ENGY=3.370MEV; J-PTY=2+; \DATA; THTC AY (DEG) (NODIM) 1.027E+01 -2.443E-02 1.343E+01 -6.997E-02 1.626E+01 -8.949E-02 1.942E+01 -1.090E-01 2.258E+01 -1.546E-01 2.557E+01 -2.196E-01 2.857E+01 -1.936E-01 3.173E+01 -5.052E-02 3.456E+01 4.893E-01 3.772E+01 5.673E-01 4.071E+01 3.852E-01 4.387E+01 2.096E-01 4.687E+01 9.251E-02 4.986E+01 2.746E-02 5.302E+01 2.291E-01 5.585E+01 3.461E-01 5.901E+01 5.933E-01 6.217E+01 6.778E-01 6.500E+01 7.103E-01 \END; /* Scanned from Fig.4, p2721 in reference */ \\EXP,29; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values, DATA-CM -> DATA */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=VCTR-ANALPW; ENR=X%'137'; /* '137' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=65MEV; BEAM-INTNSTY=[12NA; POL-PRJ=[70%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'138',PROP-CNTR'139'); /* '138' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '139' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'140'; /* '140' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'141'; /* '141' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,29; INC-ENGY-LAB=65MEV; EXC-ENGY=3.602MEV; J-PTY=2+; \DATA; THTC AY DELTA-AY (DEG) (NODIM) (NODIM) 1.017E+01 -1.028E-01 +-NEGLIGIBLE 1.317E+01 -8.322E-02 +-NEGLIGIBLE 1.617E+01 -7.669E-02 +-NEGLIGIBLE 1.934E+01 -1.028E-01 +-NEGLIGIBLE 2.250E+01 -1.028E-01 +-NEGLIGIBLE 2.550E+01 -1.550E-01 +-NEGLIGIBLE 2.850E+01 -1.224E-01 +-NEGLIGIBLE 3.167E+01 9.296E-02 +-NEGLIGIBLE 3.467E+01 4.584E-01 +-5.220E-02 3.750E+01 4.975E-01 +-NEGLIGIBLE 4.083E+01 4.192E-01 +-NEGLIGIBLE 4.383E+01 3.213E-01 +-NEGLIGIBLE 4.683E+01 2.365E-01 +-NEGLIGIBLE 4.983E+01 3.213E-01 +-5.220E-02 5.283E+01 4.518E-01 +-6.525E-02 5.917E+01 8.825E-01 +-NEGLIGIBLE 6.200E+01 8.303E-01 +-6.525E-02 6.517E+01 9.217E-01 +-NEGLIGIBLE \END; /* Scanned from Fig.4, p2721 in reference */ \\EXP,30; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values, DATA-CM -> DATA */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=VCTR-ANALPW; ENR=X%'142'; /* '142' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=65MEV; BEAM-INTNSTY=[12NA; POL-PRJ=[70%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'143',PROP-CNTR'144'); /* '143' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '144' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'145'; /* '145' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'146'; /* '146' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,30; INC-ENGY-LAB=65MEV; EXC-ENGY=3.832MEV; J-PTY=2+; \DATA; THTC AY DELTA-AY (DEG) (NODIM) (NODIM) 1.033E+01 4.439E-02 +-NEGLIGIBLE 1.350E+01 1.847E-02 +-NEGLIGIBLE 1.650E+01 -7.443E-03 +-NEGLIGIBLE 1.950E+01 8.974E-02 +-NEGLIGIBLE 2.250E+01 6.382E-02 +-NEGLIGIBLE 2.567E+01 3.143E-02 +-NEGLIGIBLE 2.867E+01 -1.500E-01 +-8.422E-02 3.167E+01 8.974E-02 +-9.718E-02 3.483E+01 1.351E-01 +-6.479E-02 3.767E+01 1.286E-01 +-5.831E-02 4.100E+01 -7.443E-03 +-NEGLIGIBLE 4.400E+01 1.847E-02 +-NEGLIGIBLE 4.700E+01 -7.223E-02 +-6.479E-02 4.983E+01 -2.795E-01 +-9.070E-02 5.300E+01 -3.055E-01 +-1.620E-01 5.600E+01 1.221E-01 +-1.425E-01 6.217E+01 1.286E-01 +-1.425E-01 6.533E+01 7.030E-02 +-1.166E-01 \END; /* Scanned from Fig.4, p2721 in reference */ \\EXP,31; /* 2006-11-16 : Altered, At. Re-digitized */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=99.9%; THK-TGT=43MG/CM**2; INC-ENGY-LAB-RANGE=400MEV; BEAM-INTNSTY=[1NA; POL-PRJ=[80%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'147',SCT'148',MWDC); /* '147' Scattered protons were analyzed by using the magnetic spectrograph (Grand Raiden) operated with an opening angle of +-8.5 mrad horizontally and of +-20 mrad vertically. */ /* '148' Focal-plane counter system consists of two MWDCs to detect scattering proton [T.Noro et al., RCNP Annual Report (1991)177] and two plastic-scintillation counters placed behind the MWDCs. */ ERS-DET=[100KEV; \\DATA,31; INC-ENGY-LAB=400MEV; EXC-ENGY=2.657MEV; J-PTY=2+; \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 7.235E+00 7.935E-01 +-7.741E-02 8.768E+00 1.117E+00 +-NEGLIGIBLE 9.764E+00 7.756E-01 +-NEGLIGIBLE 1.084E+01 3.451E-01 +-NEGLIGIBLE 1.191E+01 1.103E-01 +-9.620E-03 1.298E+01 2.839E-02 +-7.684E-03 1.390E+01 8.682E-02 +-NEGLIGIBLE 1.498E+01 1.702E-01 +-NEGLIGIBLE 1.590E+01 2.315E-01 +-NEGLIGIBLE 1.697E+01 2.942E-01 +-NEGLIGIBLE 1.804E+01 3.044E-01 +-NEGLIGIBLE 1.912E+01 2.019E-01 +-NEGLIGIBLE 2.011E+01 1.484E-01 +-1.233E-02 2.111E+01 5.565E-02 +-NEGLIGIBLE 2.226E+01 2.209E-02 +-3.260E-03 2.325E+01 1.193E-02 +-1.526E-03 2.425E+01 2.592E-02 +-NEGLIGIBLE 2.532E+01 2.087E-02 +-2.521E-03 2.632E+01 3.447E-02 +-NEGLIGIBLE 2.732E+01 2.938E-02 +-3.464E-03 \END; /* Scanned from Fig.5, p2721 in reference */ \\EXP,32; /* 2006-11-16 : Altered, At. Re-digitized */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=99.9%; THK-TGT=43MG/CM**2; INC-ENGY-LAB-RANGE=400MEV; BEAM-INTNSTY=[1NA; POL-PRJ=[80%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'149',SCT'150',MWDC); /* '149' Scattered protons were analyzed by using the magnetic spectrograph (Grand Raiden) operated with an opening angle of +-8.5 mrad horizontally and of +-20 mrad vertically. */ /* '150' Focal-plane counter system consists of two MWDCs to detect scattering proton [T.Noro et al., RCNP Annual Report (1991)177] and two plastic-scintillation counters placed behind the MWDCs. */ ERS-DET=[100KEV; \\DATA,32; INC-ENGY-LAB=400MEV; EXC-ENGY=2.960MEV; J-PTY=2+; \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 7.388E+00 7.289E-02 +-1.216E-02 8.844E+00 2.675E-01 +-NEGLIGIBLE 9.994E+00 3.598E-01 +-NEGLIGIBLE 1.091E+01 2.998E-01 +-3.232E-02 1.191E+01 2.768E-01 +-NEGLIGIBLE 1.306E+01 2.204E-01 +-NEGLIGIBLE 1.398E+01 1.412E-01 +-NEGLIGIBLE 1.513E+01 7.805E-02 +-NEGLIGIBLE 1.919E+01 3.513E-02 +-NEGLIGIBLE 2.027E+01 6.143E-02 +-NEGLIGIBLE 2.126E+01 6.807E-02 +-NEGLIGIBLE 2.233E+01 9.052E-02 +-NEGLIGIBLE 2.333E+01 4.515E-02 +-NEGLIGIBLE 2.440E+01 3.848E-02 +-NEGLIGIBLE 2.540E+01 1.149E-02 +-1.916E-03 2.640E+01 6.798E-03 +-1.448E-03 2.747E+01 5.350E-03 +-1.042E-03 3.161E+01 7.115E-03 +-1.050E-03 \END; /* Scanned from Fig.5, p2721 in reference */ \\EXP,33; /* 2006-11-16 : Altered, At. Re-digitized */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=99.9%; THK-TGT=43MG/CM**2; INC-ENGY-LAB-RANGE=400MEV; BEAM-INTNSTY=[1NA; POL-PRJ=[80%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'151',SCT'152',MWDC); /* '151' Scattered protons were analyzed by using the magnetic spectrograph (Grand Raiden) operated with an opening angle of +-8.5 mrad horizontally and of +-20 mrad vertically. */ /* '152' Focal-plane counter system consists of two MWDCs to detect scattering proton [T.Noro et al., RCNP Annual Report (1991)177] and two plastic-scintillation counters placed behind the MWDCs. */ ERS-DET=[100KEV; \\DATA,33; INC-ENGY-LAB=400MEV; EXC-ENGY=3.370MEV; J-PTY=2+; \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 7.464E+00 9.880E-01 +-NEGLIGIBLE 8.998E+00 1.557E+00 +-NEGLIGIBLE 9.994E+00 1.725E+00 +-NEGLIGIBLE 1.099E+01 1.011E+00 +-NEGLIGIBLE 1.206E+01 5.923E-01 +-NEGLIGIBLE 1.314E+01 2.702E-01 +-NEGLIGIBLE 1.413E+01 8.568E-02 +-1.093E-02 1.521E+01 6.022E-02 +-5.859E-03 1.620E+01 1.233E-01 +-NEGLIGIBLE 1.720E+01 2.011E-01 +-NEGLIGIBLE 1.827E+01 2.828E-01 +-NEGLIGIBLE 1.927E+01 2.960E-01 +-NEGLIGIBLE 2.034E+01 3.279E-01 +-NEGLIGIBLE 2.126E+01 2.057E-01 +-NEGLIGIBLE 2.241E+01 1.754E-01 +-NEGLIGIBLE 2.341E+01 8.375E-02 +-7.284E-03 2.448E+01 7.307E-02 +-NEGLIGIBLE 2.548E+01 6.161E-02 +-NEGLIGIBLE 2.647E+01 3.569E-02 +-NEGLIGIBLE 2.755E+01 2.843E-02 +-2.766E-03 3.169E+01 7.346E-03 +-1.691E-03 \END; /* Scanned from Fig.5, p2721 in reference */ \\EXP,34; /* 2006-11-16 : Altered, At. Re-digitized */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=99.9%; THK-TGT=43MG/CM**2; INC-ENGY-LAB-RANGE=400MEV; BEAM-INTNSTY=[1NA; POL-PRJ=[80%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'153',SCT'154',MWDC); /* '153' Scattered protons were analyzed by using the magnetic spectrograph (Grand Raiden) operated with an opening angle of +-8.5 mrad horizontally and of +-20 mrad vertically. */ /* '154' Focal-plane counter system consists of two MWDCs to detect scattering proton [T.Noro et al., RCNP Annual Report (1991)177] and two plastic-scintillation counters placed behind the MWDCs. */ ERS-DET=[100KEV; \\DATA,34; INC-ENGY-LAB=400MEV; EXC-ENGY=3.602MEV; J-PTY=2+; \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 7.618E+00 4.914E-01 +-4.270E-02 8.998E+00 8.872E-01 +-NEGLIGIBLE 1.007E+01 1.276E+00 +-NEGLIGIBLE 1.107E+01 6.098E-01 +-1.294E-01 1.214E+01 3.155E-01 +-NEGLIGIBLE 1.314E+01 1.301E-01 +-NEGLIGIBLE 1.421E+01 2.871E-02 +-5.573E-03 1.528E+01 4.732E-02 +-NEGLIGIBLE 1.628E+01 4.224E-02 +-6.212E-03 1.728E+01 8.740E-02 +-7.593E-03 1.835E+01 1.651E-01 +-NEGLIGIBLE 1.935E+01 1.013E-01 +-NEGLIGIBLE 2.042E+01 1.135E-01 +-NEGLIGIBLE 2.142E+01 5.676E-02 +-NEGLIGIBLE 2.256E+01 4.176E-02 +-3.457E-03 2.348E+01 1.211E-02 +-2.570E-03 2.762E+01 2.287E-02 +-NEGLIGIBLE 3.176E+01 1.922E-03 +-6.899E-04 \END; /* Scanned from Fig.5, p2721 in reference */ \\EXP,35; /* 2006-11-16 : Altered, At. Re-digitized */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=99.9%; THK-TGT=43MG/CM**2; INC-ENGY-LAB-RANGE=400MEV; BEAM-INTNSTY=[1NA; POL-PRJ=[80%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'155',SCT'156',MWDC); /* '155' Scattered protons were analyzed by using the magnetic spectrograph (Grand Raiden) operated with an opening angle of +-8.5 mrad horizontally and of +-20 mrad vertically. */ /* '156' Focal-plane counter system consists of two MWDCs to detect scattering proton [T.Noro et al., RCNP Annual Report (1991)177] and two plastic-scintillation counters placed behind the MWDCs. */ ERS-DET=[100KEV; \\DATA,35; INC-ENGY-LAB=400MEV; EXC-ENGY=3.832MEV; J-PTY=2+; \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 7.694E+00 1.683E-01 +-NEGLIGIBLE 9.151E+00 2.838E-01 +-NEGLIGIBLE 1.015E+01 4.574E-01 +-NEGLIGIBLE 1.107E+01 2.112E-01 +-1.031E-01 1.536E+01 2.893E-02 +-3.107E-03 1.636E+01 2.524E-02 +-5.358E-03 1.735E+01 4.662E-02 +-6.401E-03 1.942E+01 4.209E-02 +-NEGLIGIBLE 2.050E+01 6.193E-02 +-NEGLIGIBLE 2.157E+01 3.631E-02 +-3.154E-03 2.256E+01 4.609E-02 +-6.778E-03 2.364E+01 2.993E-02 +-NEGLIGIBLE 2.463E+01 3.470E-02 +-NEGLIGIBLE 2.571E+01 1.879E-02 +-2.017E-03 2.670E+01 1.621E-02 +-2.065E-03 \END; /* Scanned from Fig.5, p2721 in reference */ \\EXP,36; /* 2006-11-16 : Altered, At. Re-digitized */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=VCTR-ANALPW; ENR=99.9%; THK-TGT=43MG/CM**2; INC-ENGY-LAB-RANGE=400MEV; BEAM-INTNSTY=[1NA; POL-PRJ=[80%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'157',SCT'158',MWDC); /* '157' Scattered protons were analyzed by using the magnetic spectrograph (Grand Raiden) operated with an opening angle of +-8.5 mrad horizontally and of +-20 mrad vertically. */ /* '158' Focal-plane counter system consists of two MWDCs to detect scattering proton [T.Noro et al., RCNP Annual Report (1991)177] and two plastic-scintillation counters placed behind the MWDCs. */ ERS-DET=[100KEV; \\DATA,36; INC-ENGY-LAB=400MEV; EXC-ENGY=2.657MEV; J-PTY=2+; \DATA; THTC AY DELTA-AY (DEG) (NODIM) (NODIM) 7.670E+00 4.685E-01 +-1.298E-01 9.198E+00 5.591E-01 +-6.487E-02 1.027E+01 5.524E-01 +-7.136E-02 1.126E+01 3.771E-01 +-7.788E-02 1.224E+01 1.238E-01 +-1.168E-01 1.330E+01 -2.786E-01 +-2.466E-01 1.432E+01 9.540E-01 +-2.920E-01 1.539E+01 8.306E-01 +-1.038E-01 1.638E+01 7.785E-01 +-1.233E-01 1.737E+01 7.523E-01 +-5.840E-02 1.844E+01 5.640E-01 +-5.838E-02 1.943E+01 4.989E-01 +-5.191E-02 2.049E+01 3.300E-01 +-5.838E-02 2.155E+01 9.626E-02 +-6.487E-02 2.253E+01 -6.890E-01 +-9.084E-02 2.353E+01 -2.220E-01 +-1.233E-01 2.455E+01 7.511E-01 +-1.427E-01 2.554E+01 8.937E-01 +-1.362E-01 2.661E+01 9.584E-01 +-1.492E-01 2.767E+01 6.078E-01 +-1.233E-01 \END; /* Scanned from Fig.5, p2721 in reference */ \\EXP,37; /* 2006-11-16 : Altered, At. Re-digitized */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=VCTR-ANALPW; ENR=99.9%; THK-TGT=43MG/CM**2; INC-ENGY-LAB-RANGE=400MEV; BEAM-INTNSTY=[1NA; POL-PRJ=[80%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'159',SCT'160',MWDC); /* '159' Scattered protons were analyzed by using the magnetic spectrograph (Grand Raiden) operated with an opening angle of +-8.5 mrad horizontally and of +-20 mrad vertically. */ /* '160' Focal-plane counter system consists of two MWDCs to detect scattering proton [T.Noro et al., RCNP Annual Report (1991)177] and two plastic-scintillation counters placed behind the MWDCs. */ ERS-DET=[100KEV; \\DATA,37; INC-ENGY-LAB=400MEV; EXC-ENGY=2.960MEV; J-PTY=2+; \DATA; THTC AY DELTA-AY (DEG) (NODIM) (NODIM) 9.176E+00 4.569E-01 +-1.177E-01 1.032E+01 4.368E-01 +-1.177E-01 1.124E+01 3.187E-01 +-9.807E-02 1.224E+01 4.685E-01 +-7.846E-02 1.331E+01 4.027E-01 +-1.307E-01 1.438E+01 3.172E-01 +-1.046E-01 1.536E+01 7.492E-02 +-1.046E-01 1.954E+01 7.657E-01 +-1.700E-01 2.054E+01 8.045E-01 +-1.111E-01 2.161E+01 8.236E-01 +-9.150E-02 2.260E+01 7.250E-01 +-1.177E-01 2.359E+01 6.461E-01 +-1.373E-01 2.465E+01 4.038E-01 +-1.242E-01 2.564E+01 2.922E-01 +-2.614E-01 2.666E+01 -5.644E-01 +-1.634E-01 2.770E+01 1.213E-01 +-2.549E-01 3.180E+01 7.272E-01 +-2.744E-01 \END; /* Scanned from Fig.5, p2721 in reference */ \\EXP,38; /* 2006-11-16 : Altered, At. Re-digitized */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=VCTR-ANALPW; ENR=99.9%; THK-TGT=43MG/CM**2; INC-ENGY-LAB-RANGE=400MEV; BEAM-INTNSTY=[1NA; POL-PRJ=[80%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'161',SCT'162',MWDC); /* '161' Scattered protons were analyzed by using the magnetic spectrograph (Grand Raiden) operated with an opening angle of +-8.5 mrad horizontally and of +-20 mrad vertically. */ /* '162' Focal-plane counter system consists of two MWDCs to detect scattering proton [T.Noro et al., RCNP Annual Report (1991)177] and two plastic-scintillation counters placed behind the MWDCs. */ ERS-DET=[100KEV; \\DATA,38; INC-ENGY-LAB=400MEV; EXC-ENGY=3.370MEV; J-PTY=2+; \DATA; THTC AY DELTA-AY (DEG) (NODIM) (NODIM) 7.669E+00 5.639E-01 +-1.559E-01 9.281E+00 5.636E-01 +-7.145E-02 1.028E+01 5.828E-01 +-5.844E-02 1.127E+01 4.397E-01 +-5.195E-02 1.227E+01 4.200E-01 +-5.844E-02 1.334E+01 2.963E-01 +-9.095E-02 1.433E+01 -8.713E-02 +-1.559E-01 1.534E+01 3.933E-01 +-1.949E-01 1.643E+01 8.932E-01 +-1.624E-01 1.751E+01 8.280E-01 +-1.624E-01 1.850E+01 7.888E-01 +-6.494E-02 1.957E+01 6.912E-01 +-NEGLIGIBLE 2.057E+01 5.285E-01 +-NEGLIGIBLE 2.149E+01 4.764E-01 +-7.147E-02 2.256E+01 3.072E-01 +-7.145E-02 2.362E+01 5.367E-02 +-7.795E-02 2.470E+01 2.093E-01 +-7.147E-02 2.570E+01 2.351E-01 +-7.795E-02 2.670E+01 3.518E-01 +-1.364E-01 2.771E+01 4.815E-01 +-1.234E-01 3.183E+01 -9.758E-02 +-2.338E-01 \END; /* Scanned from Fig.5, p2721 in reference */ \\EXP,39; /* 2006-11-16 : Altered, At. Re-digitized */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=VCTR-ANALPW; ENR=99.9%; THK-TGT=43MG/CM**2; INC-ENGY-LAB-RANGE=400MEV; BEAM-INTNSTY=[1NA; POL-PRJ=[80%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'163',SCT'164',MWDC); /* '163' Scattered protons were analyzed by using the magnetic spectrograph (Grand Raiden) operated with an opening angle of +-8.5 mrad horizontally and of +-20 mrad vertically. */ /* '164' Focal-plane counter system consists of two MWDCs to detect scattering proton [T.Noro et al., RCNP Annual Report (1991)177] and two plastic-scintillation counters placed behind the MWDCs. */ ERS-DET=[100KEV; \\DATA,39; INC-ENGY-LAB=400MEV; EXC-ENGY=3.602MEV; J-PTY=2+; \DATA; THTC AY DELTA-AY (DEG) (NODIM) (NODIM) 7.709E+00 4.586E-01 +-3.317E-01 9.241E+00 4.713E-01 +-7.152E-02 1.024E+01 5.751E-01 +-7.806E-02 1.123E+01 4.123E-01 +-8.455E-02 1.230E+01 3.991E-01 +-7.803E-02 1.329E+01 2.168E-01 +-1.301E-01 1.435E+01 -2.322E-01 +-2.146E-01 1.544E+01 2.683E-01 +-1.431E-01 1.637E+01 7.884E-01 +-3.122E-01 1.745E+01 7.361E-01 +-1.756E-01 1.844E+01 7.359E-01 +-9.104E-02 1.951E+01 6.706E-01 +-9.104E-02 2.043E+01 4.948E-01 +-8.455E-02 2.157E+01 3.710E-01 +-9.754E-02 2.256E+01 1.366E-01 +-1.691E-01 2.362E+01 -2.083E-01 +-2.276E-01 2.770E+01 4.152E-01 +-1.301E-01 3.181E+01 -4.573E-01 +-2.732E-01 \END; /* Scanned from Fig.5, p2721 in reference */ \\EXP,40; /* 2006-11-16 : Altered, At. Re-digitized */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=VCTR-ANALPW; ENR=99.9%; THK-TGT=43MG/CM**2; INC-ENGY-LAB-RANGE=400MEV; BEAM-INTNSTY=[1NA; POL-PRJ=[80%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'165',SCT'166',MWDC); /* '165' Scattered protons were analyzed by using the magnetic spectrograph (Grand Raiden) operated with an opening angle of +-8.5 mrad horizontally and of +-20 mrad vertically. */ /* '166' Focal-plane counter system consists of two MWDCs to detect scattering proton [T.Noro et al., RCNP Annual Report (1991)177] and two plastic-scintillation counters placed behind the MWDCs. */ ERS-DET=[100KEV; \\DATA,40; INC-ENGY-LAB=400MEV; EXC-ENGY=3.832MEV; J-PTY=2+; \DATA; THTC AY DELTA-AY (DEG) (NODIM) (NODIM) 7.776E+00 7.125E-01 +-2.995E-01 9.286E+00 4.576E-01 +-1.041E-01 1.029E+01 5.091E-01 +-1.042E-01 1.127E+01 3.001E-01 +-1.107E-01 1.240E+01 1.691E-01 +-2.278E-01 1.544E+01 7.402E-01 +-2.149E-01 1.658E+01 5.702E-01 +-NEGLIGIBLE 1.751E+01 6.738E-01 +-2.736E-01 1.956E+01 4.511E-01 +-1.302E-01 2.057E+01 6.393E-01 +-1.172E-01 2.155E+01 4.694E-01 +-1.498E-01 2.262E+01 4.427E-01 +-1.758E-01 2.369E+01 4.289E-01 +-1.628E-01 2.467E+01 1.874E-01 +-1.042E-01 2.563E+01 -1.453E-01 +-1.106E-01 2.674E+01 2.447E-01 +-2.148E-01 \END; /* Scanned from Fig.5, p2721 in reference */ \\EXP,41; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=X%'167'; /* '167' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=65MEV; BEAM-INTNSTY=[12NA; POL-PRJ=[70%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'168',PROP-CNTR'169'); /* '168' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '169' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'170'; /* '170' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'171'; /* '171' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,41; INC-ENGY-LAB=65MEV; EXC-ENGY=2.085MEV; J-PTY=4+; \DATA; THTC DSIGMA/DOMEGA (DEG) (MB/SR) 1.036E+01 1.185E-01 1.339E+01 8.112E-02 1.641E+01 5.737E-02 1.946E+01 6.322E-02 2.249E+01 5.911E-02 2.553E+01 5.176E-02 2.872E+01 4.174E-02 3.159E+01 3.777E-02 3.461E+01 2.158E-02 3.765E+01 2.498E-02 4.393E+01 5.389E-02 4.665E+01 6.137E-02 5.289E+01 5.921E-02 5.592E+01 4.855E-02 5.880E+01 4.393E-02 6.183E+01 3.910E-02 6.487E+01 3.480E-02 \END; /* Scanned from Fig.6, p2722 in reference */ \\EXP,42; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=X%'172'; /* '172' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=65MEV; BEAM-INTNSTY=[12NA; POL-PRJ=[70%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'173',PROP-CNTR'174'); /* '173' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '174' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'175'; /* '175' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'176'; /* '176' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,42; INC-ENGY-LAB=65MEV; EXC-ENGY=3.123MEV; J-PTY=4+; \DATA; THTC DSIGMA/DOMEGA (DEG) (MB/SR) 1.030E+01 5.672E-01 1.335E+01 6.815E-01 1.639E+01 7.569E-01 1.944E+01 9.839E-01 2.248E+01 1.246E+00 2.537E+01 1.497E+00 2.858E+01 1.578E+00 3.162E+01 1.537E+00 3.467E+01 1.279E+00 3.772E+01 9.584E-01 4.076E+01 6.466E-01 4.397E+01 4.033E-01 4.685E+01 2.793E-01 4.990E+01 2.206E-01 5.295E+01 1.788E-01 5.599E+01 1.412E-01 5.904E+01 9.782E-02 6.208E+01 7.525E-02 6.513E+01 4.453E-02 \END; /* Scanned from Fig.6, p2722 in reference */ \\EXP,43; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values */ RCT=56FE(D,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=X%'177'; /* '177' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=56MEV; BEAM-INTNSTY=[60NA; POL-PRJ=0%; DET-PARTCL=D; DET-SYS=(MAG'178',PROP-CNTR'179'); /* '178' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '179' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'180'; /* '180' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'181'; /* '181' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,43; INC-ENGY-LAB=56MEV; EXC-ENGY=2.085MEV; J-PTY=4+; \DATA; THTC DSIGMA/DOMEGA (DEG) (MB/SR) 1.040E+01 3.050E-01 1.296E+01 2.845E-01 1.552E+01 2.546E-01 1.808E+01 2.067E-01 2.080E+01 1.566E-01 2.336E+01 1.254E-01 2.592E+01 1.107E-01 2.848E+01 1.272E-01 3.104E+01 1.107E-01 3.360E+01 8.500E-02 3.616E+01 6.807E-02 3.872E+01 8.153E-02 4.144E+01 8.383E-02 4.400E+01 8.153E-02 4.640E+01 6.807E-02 4.896E+01 5.682E-02 5.152E+01 5.085E-02 5.408E+01 5.085E-02 5.664E+01 4.810E-02 5.920E+01 4.550E-02 6.160E+01 3.799E-02 \END; /* Scanned from Fig.6, p2722 in reference */ \\EXP,44; /* 2006-11-16 : Altered, At. Re-digitized */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=99.9%; THK-TGT=43MG/CM**2; INC-ENGY-LAB-RANGE=400MEV; BEAM-INTNSTY=[1NA; POL-PRJ=[80%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'182',SCT'183',MWDC); /* '182' Scattered protons were analyzed by using the magnetic spectrograph (Grand Raiden) operated with an opening angle of +-8.5 mrad horizontally and of +-20 mrad vertically. */ /* '183' Focal-plane counter system consists of two MWDCs to detect scattering proton [T.Noro et al., RCNP Annual Report (1991)177] and two plastic-scintillation counters placed behind the MWDCs. */ ERS-DET=[100KEV; \\DATA,44; INC-ENGY-LAB=400MEV; EXC-ENGY=2.085MEV; J-PTY=4+; \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 7.786E+00 2.125E-01 +-NEGLIGIBLE 9.227E+00 3.024E-01 +-NEGLIGIBLE 1.029E+01 3.516E-01 +-NEGLIGIBLE 1.127E+01 5.401E-01 +-1.126E-01 1.233E+01 2.463E-01 +-NEGLIGIBLE 1.330E+01 7.683E-02 +-1.919E-02 1.443E+01 3.685E-02 +-NEGLIGIBLE 1.541E+01 2.110E-02 +-NEGLIGIBLE 1.647E+01 1.722E-02 +-3.332E-03 1.746E+01 3.674E-02 +-NEGLIGIBLE 1.845E+01 8.900E-02 +-NEGLIGIBLE 1.951E+01 9.838E-02 +-NEGLIGIBLE 2.050E+01 1.630E-01 +-NEGLIGIBLE 2.155E+01 1.233E-01 +-NEGLIGIBLE 2.254E+01 1.232E-01 +-NEGLIGIBLE 2.352E+01 7.054E-02 +-NEGLIGIBLE 2.450E+01 6.055E-02 +-NEGLIGIBLE 2.559E+01 1.942E-02 +-3.421E-03 2.668E+01 1.465E-02 +-NEGLIGIBLE 2.766E+01 1.053E-02 +-NEGLIGIBLE 3.175E+01 1.697E-02 +-NEGLIGIBLE \END; /* Scanned from Fig.6, p2721 in reference */ \\EXP,45; /* 2006-11-16 : Altered, At. Re-digitized */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=99.9%; THK-TGT=43MG/CM**2; INC-ENGY-LAB-RANGE=400MEV; BEAM-INTNSTY=[1NA; POL-PRJ=[80%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'184',SCT'185',MWDC); /* '184' Scattered protons were analyzed by using the magnetic spectrograph (Grand Raiden) operated with an opening angle of +-8.5 mrad horizontally and of +-20 mrad vertically. */ /* '185' Focal-plane counter system consists of two MWDCs to detect scattering proton [T.Noro et al., RCNP Annual Report (1991)177] and two plastic-scintillation counters placed behind the MWDCs. */ ERS-DET=[100KEV; \\DATA,45; INC-ENGY-LAB=400MEV; EXC-ENGY=3.123MEV; J-PTY=4+; \DATA; THTC DSIGMA/DOMEGA (DEG) (MB/SR) 7.697E+00 2.590E-01 9.189E+00 7.375E-01 1.023E+01 1.443E+00 1.120E+01 1.739E+00 1.223E+01 2.097E+00 1.333E+01 1.985E+00 1.430E+01 2.208E+00 1.533E+01 1.779E+00 1.637E+01 1.220E+00 1.740E+01 1.065E+00 1.843E+01 6.924E-01 1.946E+01 3.439E-01 2.055E+01 1.708E-01 2.152E+01 8.039E-02 2.255E+01 1.139E-01 2.352E+01 1.138E-01 2.463E+01 1.795E-01 2.566E+01 1.135E-01 2.669E+01 9.396E-02 2.766E+01 6.799E-02 3.178E+01 7.885E-03 \END; /* Scanned from Fig.6, p2721 in reference */ \\EXP,46; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values, DATA-CM -> DATA */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=VCTR-ANALPW; ENR=X%'186'; /* '186' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=65MEV; BEAM-INTNSTY=[12NA; POL-PRJ=[70%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'187',PROP-CNTR'188'); /* '187' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '188' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'189'; /* '189' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'190'; /* '190' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,46; INC-ENGY-LAB=65MEV; EXC-ENGY=2.085MEV; J-PTY=4+; \DATA; THTC AY DELTA-AY (DEG) (NODIM) (NODIM) 1.026E+01 1.413E-01 +-9.641E-02 1.324E+01 -7.849E-02 +-1.028E-01 1.627E+01 3.857E-03 +-1.028E-01 1.945E+01 9.900E-02 +-7.708E-02 2.257E+01 -5.653E-02 +-7.070E-02 2.560E+01 6.536E-03 +-7.081E-02 2.863E+01 3.103E-02 +-7.081E-02 3.165E+01 3.625E-02 +-7.070E-02 3.472E+01 3.050E-01 +-1.028E-01 3.788E+01 3.744E-01 +-9.004E-02 4.404E+01 2.820E-01 +-NEGLIGIBLE 4.705E+01 2.422E-01 +-NEGLIGIBLE 5.309E+01 2.398E-01 +-NEGLIGIBLE 5.613E+01 3.607E-01 +-NEGLIGIBLE 5.916E+01 3.916E-01 +-NEGLIGIBLE 6.234E+01 5.510E-01 +-NEGLIGIBLE 6.540E+01 7.748E-01 +-NEGLIGIBLE \END; /* Scanned from Fig.6, p2722 in reference */ \\EXP,47; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values, DATA-CM -> DATA */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=VCTR-ANALPW; ENR=X%'191'; /* '191' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=65MEV; BEAM-INTNSTY=[12NA; POL-PRJ=[70%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'192',PROP-CNTR'193'); /* '192' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '193' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'194'; /* '194' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'195'; /* '195' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,47; INC-ENGY-LAB=65MEV; EXC-ENGY=3.123MEV; J-PTY=4+; \DATA; THTC AY (DEG) (NODIM) 1.027E+01 -1.815E-01 1.340E+01 -1.622E-01 1.639E+01 -1.751E-01 1.952E+01 -1.105E-01 2.252E+01 -1.041E-01 2.551E+01 -1.105E-01 2.864E+01 -1.428E-01 3.163E+01 -1.622E-01 3.476E+01 -2.009E-01 3.776E+01 -2.267E-01 4.061E+01 -2.074E-01 4.374E+01 -1.041E-01 4.673E+01 1.863E-01 4.986E+01 6.381E-01 5.286E+01 8.382E-01 5.571E+01 8.769E-01 5.871E+01 8.575E-01 6.184E+01 7.349E-01 6.483E+01 5.219E-01 \END; /* Scanned from Fig.6, p2722 in reference */ \\EXP,48; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values */ RCT=56FE(D,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=X%'196'; /* '196' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=56MEV; BEAM-INTNSTY=[60NA; POL-PRJ=0%; DET-PARTCL=D; DET-SYS=(MAG'197',PROP-CNTR'198'); /* '197' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '198' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'199'; /* '199' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'200'; /* '200' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,48; INC-ENGY-LAB=56MEV; EXC-ENGY=3.123MEV; J-PTY=4+; \DATA; THTC DSIGMA/DOMEGA (DEG) (MB/SR) 1.058E+01 9.068E-01 1.318E+01 1.027E+00 1.577E+01 1.024E+00 1.837E+01 1.098E+00 2.095E+01 8.792E-01 2.352E+01 5.863E-01 2.606E+01 2.972E-01 2.874E+01 1.426E-01 3.135E+01 1.676E-01 3.369E+01 2.198E-01 3.641E+01 2.112E-01 3.899E+01 1.660E-01 4.156E+01 1.148E-01 4.401E+01 1.008E-01 4.659E+01 8.677E-02 4.905E+01 9.832E-02 5.178E+01 9.277E-02 5.409E+01 7.992E-02 5.693E+01 5.526E-02 5.937E+01 4.345E-02 6.209E+01 3.607E-02 \END; /* Scanned from Fig.6, p2722 in reference */ \\EXP,49; /* 2006-11-16 : Altered, At. Re-digitized */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=VCTR-ANALPW; ENR=99.9%; THK-TGT=43MG/CM**2; INC-ENGY-LAB-RANGE=400MEV; BEAM-INTNSTY=[1NA; POL-PRJ=[80%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'201',SCT'202',MWDC); /* '201' Scattered protons were analyzed by using the magnetic spectrograph (Grand Raiden) operated with an opening angle of +-8.5 mrad horizontally and of +-20 mrad vertically. */ /* '202' Focal-plane counter system consists of two MWDCs to detect scattering proton [T.Noro et al., RCNP Annual Report (1991)177] and two plastic-scintillation counters placed behind the MWDCs. */ ERS-DET=[100KEV; \\DATA,49; INC-ENGY-LAB=400MEV; EXC-ENGY=2.085MEV; J-PTY=4+; \DATA; THTC AY DELTA-AY (DEG) (NODIM) (NODIM) 7.840E+00 5.640E-01 +-3.551E-01 9.250E+00 4.531E-01 +-1.356E-01 1.030E+01 6.588E-01 +-3.292E-01 1.135E+01 8.258E-01 +-1.549E-01 1.238E+01 8.701E-01 +-4.132E-01 1.340E+01 6.498E-01 +-4.647E-01 1.443E+01 6.166E-01 +-3.033E-01 1.540E+01 -3.626E-02 +-1.611E-01 1.651E+01 9.119E-01 +-4.132E-01 1.857E+01 8.520E-01 +-1.614E-01 1.960E+01 8.124E-01 +-7.096E-02 2.063E+01 7.406E-01 +-8.381E-02 2.165E+01 6.364E-01 +-7.741E-02 2.268E+01 5.129E-01 +-1.226E-01 2.370E+01 3.829E-01 +-1.032E-01 2.470E+01 9.155E-02 +-8.392E-02 2.566E+01 -6.175E-02 +-7.269E-02 2.678E+01 -4.916E-01 +-1.164E-01 2.781E+01 2.245E-01 +-1.045E-01 3.190E+01 5.375E-01 +-2.128E-01 \END; /* Scanned from Fig.6, p2722 in reference */ \\EXP,50; /* 2006-11-16 : Altered, At. Re-digitized */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=VCTR-ANALPW; ENR=99.9%; THK-TGT=43MG/CM**2; INC-ENGY-LAB-RANGE=400MEV; BEAM-INTNSTY=[1NA; POL-PRJ=[80%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'203',SCT'204',MWDC); /* '203' Scattered protons were analyzed by using the magnetic spectrograph (Grand Raiden) operated with an opening angle of +-8.5 mrad horizontally and of +-20 mrad vertically. */ /* '204' Focal-plane counter system consists of two MWDCs to detect scattering proton [T.Noro et al., RCNP Annual Report (1991)177] and two plastic-scintillation counters placed behind the MWDCs. */ ERS-DET=[100KEV; \\DATA,50; INC-ENGY-LAB=400MEV; EXC-ENGY=3.123MEV; J-PTY=4+; \DATA; THTC AY DELTA-AY (DEG) (NODIM) (NODIM) 7.834E+00 3.836E-01 +-1.301E-01 9.371E+00 5.776E-01 +-7.220E-02 1.039E+01 6.564E-01 +-7.199E-02 1.140E+01 6.123E-01 +-NEGLIGIBLE 1.235E+01 7.056E-01 +-NEGLIGIBLE 1.344E+01 6.687E-01 +-NEGLIGIBLE 1.446E+01 6.824E-01 +-NEGLIGIBLE 1.547E+01 6.023E-01 +-NEGLIGIBLE 1.647E+01 5.004E-01 +-7.947E-02 1.756E+01 4.274E-01 +-NEGLIGIBLE 1.848E+01 1.739E-01 +-NEGLIGIBLE 1.949E+01 2.144E-02 +-NEGLIGIBLE 2.054E+01 -4.345E-01 +-NEGLIGIBLE 2.163E+01 -3.774E-01 +-NEGLIGIBLE 2.257E+01 5.106E-01 +-9.397E-02 2.367E+01 7.410E-01 +-1.012E-01 2.470E+01 8.848E-01 +-8.664E-02 2.563E+01 7.613E-01 +-5.780E-02 2.670E+01 5.221E-01 +-1.012E-01 2.771E+01 3.697E-01 +-7.957E-02 3.181E+01 -1.028E-01 +-1.445E-01 \END; /* Scanned from Fig.6, p2722 in reference */ \\EXP,51; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=X%'205'; /* '205' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=65MEV; BEAM-INTNSTY=[12NA; POL-PRJ=[70%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'206',PROP-CNTR'207'); /* '206' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '207' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'208'; /* '208' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'209'; /* '209' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,51; INC-ENGY-LAB=65MEV; EXC-ENGY=(2.960MEV,2.942MEV); J-PTY=(2+,0+); \DATA; THTC DSIGMA/DOMEGA (DEG) (MB/SR) 1.002E+01 1.626E-01 1.326E+01 1.311E-01 1.633E+01 1.037E-01 1.924E+01 1.074E-01 2.248E+01 1.133E-01 2.556E+01 1.132E-01 2.863E+01 1.132E-01 3.170E+01 9.624E-02 3.460E+01 6.839E-02 3.784E+01 4.605E-02 4.091E+01 3.711E-02 4.381E+01 3.390E-02 4.705E+01 2.781E-02 5.302E+01 2.011E-02 5.609E+01 1.481E-02 5.916E+01 9.798E-03 6.530E+01 8.326E-03 \END; /* Scanned from Fig.8, p2725 in reference */ \\EXP,52; /* 2006-11-16 : Altered, At. Re-digitized */ /* 2012-07-31 : Altered, VD.Corrected isotopic abundance values, DATA-CM -> DATA */ RCT=56FE(P,INL)56FE; RTY=INEL-SCATT; PHQ=VCTR-ANALPW; ENR=X%'210'; /* '210' Isotopic enrichment greater than 99% */ THK-TGT=1.05MG/CM**2; INC-ENGY-LAB-RANGE=65MEV; BEAM-INTNSTY=[12NA; POL-PRJ=[70%; ION-SOURCE=/ Polarized ion source /; DET-PARTCL=P; DET-SYS=(MAG'211',PROP-CNTR'212'); /* '211' To analyze scattering particle, Magnetic spectrograph [H.Ikegami et al., Nucl. Instrum. Methods 217(1983)441]. */ /* '212' To detect scattering particle two-dimensional position-sensitive proportional counter [Y. Fujita et al., Nucl. Instrum. Methods 217(1983)441]. */ SOLID-ANGL=3.2MSR'213'; /* '213' The solid angle of spectrograph was set to maximize the energy resolution. */ ERS-DET=[30KEV'214'; /* '214' full width at half maximum (FWHM), for proton and deuteron */ \\DATA,52; INC-ENGY-LAB=65MEV; EXC-ENGY=(2.960MEV,2.942MEV); J-PTY=(2+,0+); \DATA; THTC AY DELTA-AY (DEG) (NODIM) (NODIM) 1.024E+01 -1.667E-02 +-8.318E-02 1.330E+01 -1.204E-02 +-7.394E-02 1.635E+01 -2.802E-03 +-7.856E-02 1.924E+01 -1.667E-02 +-5.083E-02 2.247E+01 -8.598E-02 +-4.621E-02 2.536E+01 -1.877E-01 +-4.159E-02 2.858E+01 -1.461E-01 +-3.697E-02 3.147E+01 -9.523E-02 +-5.083E-02 3.470E+01 5.265E-02 +-5.083E-02 3.759E+01 2.698E-01 +-6.008E-02 4.064E+01 5.517E-01 +-6.470E-02 4.370E+01 5.471E-01 +-6.470E-02 4.676E+01 5.610E-01 +-6.932E-02 5.287E+01 4.039E-01 +-7.856E-02 5.576E+01 2.791E-01 +-9.242E-02 5.899E+01 4.270E-01 +-1.155E-01 \END; /* Scanned from Fig.8, p2725 in reference */ \\END;