ENTRY C2953 20230524 C295300000001 SUBENT C2953001 20230524 20250110 C295300100001 BIB 9 12 C295300100002 TITLE Reorientation-Effect Measurements on Cd114 C295300100003 AUTHOR (J.X.Saladin,J.E.Glenn,R.J.Pryor) C295300100004 INSTITUTE (1USAPUP) C295300100005 REFERENCE (J,PR,186,1241,1969) C295300100006 #doi:10.1103/PhysRev.186.1241 C295300100007 FACILITY (VDGT,1USAPUP) C295300100008 INC-SOURCE O16 beam carrying a charge of +6e. The 016 beams was C295300100009 about 0.6 mu-A, that of the alpha beam about 0.3 mu-A. C295300100010 DETECTOR (MAGSP,PS) Three position-sensitive detectors placed C295300100011 in the focal plane of the spectrograph. C295300100012 METHOD (EXTB) C295300100013 HISTORY (20230524C) OG C295300100014 ENDBIB 12 0 C295300100015 NOCOMMON 0 0 C295300100016 ENDSUBENT 15 0 C295300199999 SUBENT C2953002 20230524 20250110 C295300200001 BIB 7 19 C295300200002 REACTION ((48-CD-114(8-O-16,INL)48-CD-114,PAR,DA)/ C295300200003 (48-CD-114(8-O-16,EL)48-CD-114,,DA)) C295300200004 EN-SEC (E-LVL1,48-CD-114) C295300200005 (E-LVL2,8-O-16) C295300200006 LEVEL-PROP (48-CD-114,E-LVL=0.5578,SPIN=2.,PARITY=+1.) C295300200007 SAMPLE The Cd targets were prepared by dissociating in C295300200008 vacuum isotopically enriched (99.09%) CdO through C295300200009 resistive heating. The evolving cadmium was then C295300200010 allowed to condense on 10-mu-g/cm2 carbon backings. C295300200011 Targets varied in thickness from 10 to 20 mu-g/cm2 of C295300200012 Cd114. C295300200013 (48-CD-114,ENR=0.9909) C295300200014 CORRECTION The subtractions of contributions from isotopic C295300200015 impurities, using the Oak Ridge isotopic abundance C295300200016 analyses. C295300200017 ERR-ANALYS (DATA-ERR) No information on source of uncertainties C295300200018 (ERR-1,,0.002) The error due to the exclusion of chargeC295300200019 states smaller than +6e is less than 0.2%. C295300200020 STATUS (TABLE,,J.X.Saladin+,J,PR,186,1241,1969) Tab.I (p.1244)C295300200021 ENDBIB 19 0 C295300200022 COMMON 5 3 C295300200023 EN EN-ERR E-LVL1 E-LVL2 ANG-ERR C295300200024 MEV KEV MEV MEV ADEG C295300200025 42.0 10. 0.5578 0. 0.15 C295300200026 ENDCOMMON 3 0 C295300200027 DATA 3 7 C295300200028 ANG DATA DATA-ERR C295300200029 ADEG NO-DIM NO-DIM C295300200030 45. 0.00907 0.00006 C295300200031 59.4 0.02004 0.00022 C295300200032 89.4 0.05259 0.00036 C295300200033 119.4 0.08456 0.00075 C295300200034 133.8 0.09548 0.00091 C295300200035 134.2 0.09702 0.00113 C295300200036 142.8 0.1020 0.0010 C295300200037 ENDDATA 9 0 C295300200038 ENDSUBENT 37 0 C295300299999 SUBENT C2953003 20230524 20250110 C295300300001 BIB 5 15 C295300300002 REACTION ((48-CD-114(A,INL)48-CD-114,PAR,DA)/ C295300300003 (48-CD-114(A,EL)48-CD-114,,DA)) C295300300004 LEVEL-PROP (48-CD-114,E-LVL=0.5578,SPIN=2.,PARITY=+1.) C295300300005 SAMPLE The Cd targets were prepared by dissociating in C295300300006 vacuum isotopically enriched (99.09%) CdO through C295300300007 resistive heating. The evolving cadmium was then C295300300008 allowed to condense on 20-mu-g/cm2 carbon backings. C295300300009 Targets varied in thickness from 20 to 60 mu-g/cm2 of C295300300010 Cd114. C295300300011 (48-CD-114,ENR=0.9909) C295300300012 ERR-ANALYS (DATA-ERR) At energies below 9 MeV, the accuracy of theC295300300013 data is limited by ambiguities in background C295300300014 subtraction. Above 9 MeV, the accuracy of the data is C295300300015 limited by statistics. C295300300016 STATUS (TABLE,,J.X.Saladin+,J,PR,186,1241,1969) Tab.I (p.1244)C295300300017 ENDBIB 15 0 C295300300018 COMMON 3 3 C295300300019 ANG E-LVL EN-ERR C295300300020 ADEG MEV KEV C295300300021 135. 0.5578 2. C295300300022 ENDCOMMON 3 0 C295300300023 DATA 3 7 C295300300024 EN DATA DATA-ERR C295300300025 MEV NO-DIM NO-DIM C295300300026 8. 0.00244 0.00005 C295300300027 8.5 0.00338 0.00007 C295300300028 9. 0.00438 0.00009 C295300300029 10. 0.00699 0.00014 C295300300030 11. 0.0106 0.0002 C295300300031 12. 0.0147 0.0003 C295300300032 13. 0.0198 0.0004 C295300300033 ENDDATA 9 0 C295300300034 ENDSUBENT 33 0 C295300399999 ENDENTRY 3 0 C295399999999