/* 2012-01-30 File is generated by HENDEL. */ \\BIB,1[8; D#=D2347; TITLE=/ The 150Nd(3He,t) and 150Sm(t,3He) reactions with applications to double beta decay of 150Nd /; PURPOSE=/ To shed light on the nuclear structure relevant for studies of double beta decay of 150Nd /; ATH=(C.J.GUESS'1,2,3', T.ADACHI'4', H.AKIMUNE'5', A.ALGORA'6,7', S.M.AUSTIN'1,3', D.BAZIN'1', B.A.BROWN'1,2,3', C.CAESAR'1,8', J.M.DEAVEN'1,2,3', H.EJIRI'4,9', E.ESTEVEZ'6', D.FANG'10', A.FAESSLER'10', D.FREKERS'11', H.FUJITA'4', Y.FUJITA'12', M.FUJIWARA'4,13', G.F.GRINYER'1', M.N.HARAKEH'14', K.HATANAKA'4', C.HERLITZIUS'1,8', K.HIROTA'4', G.W.HITT'1,2,3', D.ISHIKAWA'4', H.MATSUBARA'4', R.MEHARCHAND'1,2,3', F.MOLINA'6', H.OKAMURA'4', H.J.ONG'4', G.PERDIKAKIS'1,3', V.RODIN'10', B.RUBIO'6', Y.SHIMBARA'15', G.SUSOY'16', T.SUZUKI'4', A.TAMII'4', J.H.THIES'11', C.TUR'1,3', N.VERHANOVITZ'1', M.YOSOI'4', J.YURKON'1', R.G.T.ZEGERS'1,2,3', J.ZENIHIRO'4'); INST-ATH=(1USAMSU'1', 1USAMSU'2', 1USAMSU'3', 2JPNRCN'4', 2JPNKON'5', 2SPNVAL'6', 3HUNDEB'7', 2GERMNZ'8', 3CZRCTI'9', 2GERTUE'10', 2GERMST'11', 2JPNOSA'12', 2JPNJAE'13', 2NEDGRN'14', 2JPNNII'15', 2TUKSTU'16'); /* '1' National Superconducting Cyclotron Laboratory */ /* '2' Department of Physics and Astronomy */ /* '3' Joint Institute for Nuclear Astrophysics */ /* '5' Department of Physics */ /* '6' Instituto de Fisica Corpuscular */ /* '9' Nuclear Science */ /* '10' Institut fur Theoretische Physik */ /* '11' Institut fur Kernphysik */ /* '12' Department of Physics */ /* '13' Quantum Beam Science Directorate */ /* '14' Kernfysisch Versneller Instituut */ /* '15' Graduate School of Science and Technology */ /* '16' Faculty of Science */ REF=PR/C; VLP=83(2011)064318; RCTS=150ND(3HE,T)150PM; PHQS=(DBL-DIFF-XSECTN, ANGL-DSTRN); \\EXP,1[8; /* 2011-10-20 : Compiled+Checked, MA and Nf */ ENR=96%; CHM=ELM; PHYS-FORM=SLD; THK-TGT=1.0MG/CM**2; POL-TGT=0%; ALGN-TGT=0%; ACC=CYC'17'; /* '17' AVF and Ring cyclotrons */ INST-ACC=2JPNRCN; INC-ENGY-LAB-RANGE=140MEV/A; BEAM-INTNSTY=5.0e+10PPS; CHRG-INC-ION=+2; POL-PRJ=0%; DET-PARTCL=T; COINC=NO; ANT-COINC=NO; DET-SYS=(MAG'18',MWDC'18',SCT'18'); /* '18' Grand Raiden spectrometer */ ERS-DET=33KEV'19'; /* '19' The excitation-energy resolution at full width at half maximum (FWHM) */ \\DATA,1[8; INC-ENGY-LAB=140MEV/A; \\EXP,1; RCT=150ND(3HE,T)150PM; PHQ=DBL-DIFF-XSECTN; \\DATA,1; THTC-MIN=0DEG; THTC-MAX=0.5DEG; DELTA-THTL=0.42DEG'20'; /* '20' Resolution of the reconstructed laboratory scattering angle */ \DATA; EXC-ENGY DSIGMA/DOMEGA/DE (MEV) (MB/SR/KEV) /* Fig. 1 of J */ \END; /* Fig.1 of J,PR/C,83,(6),064318,2011 */ \\EXP,2; RCT=150ND(3HE,T)150PM; PHQ=DBL-DIFF-XSECTN; \\DATA,2; THTC-MIN=1DEG; THTC-MAX=1.5DEG; DELTA-THTL=0.42DEG'21'; /* '21' Resolution of the reconstructed laboratory scattering angle */ \DATA; EXC-ENGY DSIGMA/DOMEGA/DE (MEV) (MB/SR/KEV) /* Fig. 1 of J */ \END; /* Fig.1 of J,PR/C,83,(6),064318,2011 */ \\EXP,3; RCT=150ND(3HE,T)150PM; PHQ=DBL-DIFF-XSECTN; \\DATA,3; THTC-MIN=2DEG; THTC-MAX=2.5DEG; DELTA-THTL=0.42DEG'22'; /* '22' Resolution of the reconstructed laboratory scattering angle */ \DATA; EXC-ENGY DSIGMA/DOMEGA/DE (MEV) (MB/SR/KEV) /* Fig. 1 of J */ \END; /* Fig.1 of J,PR/C,83,(6),064318,2011 */ \\EXP,4; RCT=150ND(3HE,T)150PM; PHQ=ANGL-DSTRN; \\DATA,4; EXC-ENGY=0MEV; DELTA-THTL=0.42DEG'23'; /* '23' Resolution of the reconstructed laboratory scattering angle */ \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 2.467E-01 9.383E-03 +-1.831E-03 7.626E-01 3.919E-02 +-2.092E-03 1.278E+00 5.657E-02 +-2.877E-03 1.792E+00 5.891E-02 +-3.007E-03 2.299E+00 4.641E-02 +-2.740E-03 2.818E+00 2.908E-02 +-1.831E-03 3.331E+00 2.619E-02 +-2.092E-03 3.845E+00 2.278E-02 +-1.700E-03 4.356E+00 1.542E-02 +-NEGLIGIBLE 4.872E+00 1.060E-02 +-NEGLIGIBLE \END; /* Fig.4(a) of J,PR/C,83,(6),064318,2011 */ \\EXP,5; RCT=150ND(3HE,T)150PM; PHQ=ANGL-DSTRN; \\DATA,5; EXC-ENGY=0.11MEV; DELTA-THTL=0.42DEG'24'; /* '24' Resolution of the reconstructed laboratory scattering angle */ \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 2.550E-01 6.491E-01 +-1.453E-02 7.666E-01 5.461E-01 +-NEGLIGIBLE 1.278E+00 3.959E-01 +-NEGLIGIBLE 1.790E+00 3.038E-01 +-NEGLIGIBLE 2.301E+00 2.541E-01 +-NEGLIGIBLE 2.813E+00 1.910E-01 +-NEGLIGIBLE 3.325E+00 1.232E-01 +-NEGLIGIBLE 3.844E+00 7.346E-02 +-NEGLIGIBLE 4.349E+00 5.039E-02 +-NEGLIGIBLE 4.861E+00 4.186E-02 +-NEGLIGIBLE \END; /* Fig.4(b) of J,PR/C,83,(6),064318,2011 */ \\EXP,6; RCT=150ND(3HE,T)150PM; PHQ=ANGL-DSTRN; \\DATA,6; EXC-ENGY=14.35MEV; DELTA-THTL=0.42DEG'25'; /* '25' Resolution of the reconstructed laboratory scattering angle */ \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 2.523E-01 9.565E+00 +-2.843E-01 7.643E-01 6.806E+00 +-NEGLIGIBLE 1.276E+00 3.695E+00 +-NEGLIGIBLE 1.788E+00 1.254E+00 +-NEGLIGIBLE 2.293E+00 2.339E-01 +-NEGLIGIBLE 2.812E+00 6.687E-01 +-NEGLIGIBLE 3.324E+00 9.195E-01 +-NEGLIGIBLE 3.837E+00 1.003E+00 +-NEGLIGIBLE 4.341E+00 7.021E-01 +-NEGLIGIBLE 4.853E+00 3.342E-01 +-NEGLIGIBLE \END; /* Fig.4(c) of J,PR/C,83,(6),064318,2011 */ \\EXP,7; RCT=150ND(3HE,T)150PM; PHQ=DBL-DIFF-XSECTN; \\DATA,7; THTC-MIN=0DEG; THTC-MAX=0.5DEG; DELTA-THTL=0.42DEG'26'; /* '26' Resolution of the reconstructed laboratory scattering angle */ \DATA; EXC-ENGY DSIGMA/DOMEGA/DE (MEV) (MB/SR/MEV) 1.507E+00 2.138E+00 2.458E+00 2.615E+00 3.521E+00 3.238E+00 4.511E+00 3.903E+00 5.485E+00 4.065E+00 6.501E+00 4.226E+00 7.500E+00 4.848E+00 8.484E+00 5.834E+00 9.508E+00 7.078E+00 1.049E+01 8.374E+00 1.150E+01 9.732E+00 1.250E+01 1.213E+01 1.352E+01 1.635E+01 1.549E+01 2.180E+01 1.649E+01 2.015E+01 1.750E+01 1.706E+01 1.849E+01 1.429E+01 1.951E+01 1.299E+01 2.051E+01 1.220E+01 2.148E+01 1.230E+01 2.253E+01 1.220E+01 2.353E+01 1.196E+01 2.452E+01 1.202E+01 2.550E+01 1.193E+01 2.656E+01 1.178E+01 2.753E+01 1.157E+01 2.851E+01 1.151E+01 \END; /* Fig.6(a) of J,PR/C,83,(6),064318,2011 */ \\EXP,8; RCT=150ND(3HE,T)150PM; PHQ=DBL-DIFF-XSECTN; \\DATA,8; THTC-MIN=1.5DEG; THTC-MAX=2DEG; DELTA-THTL=0.42DEG'27'; /* '27' Resolution of the reconstructed laboratory scattering angle */ \DATA; EXC-ENGY DSIGMA/DOMEGA/DE (MEV) (MB/SR/MEV) 1.516E+00 2.226E+00 2.532E+00 2.196E+00 3.549E+00 2.347E+00 4.524E+00 2.650E+00 5.541E+00 2.771E+00 6.532E+00 2.941E+00 7.557E+00 3.117E+00 8.549E+00 3.255E+00 9.565E+00 3.558E+00 1.054E+01 3.921E+00 1.152E+01 4.406E+00 1.257E+01 5.193E+00 1.355E+01 6.260E+00 1.457E+01 9.068E+00 1.554E+01 9.795E+00 1.652E+01 1.046E+01 1.757E+01 1.158E+01 1.855E+01 1.240E+01 1.956E+01 1.376E+01 2.054E+01 1.461E+01 2.152E+01 1.533E+01 2.258E+01 1.569E+01 2.359E+01 1.527E+01 2.455E+01 1.475E+01 2.554E+01 1.385E+01 2.657E+01 1.307E+01 2.759E+01 1.234E+01 2.859E+01 1.164E+01 \END; /* Fig.6(b) of J,PR/C,83,(6),064318,2011 */ \\END;