ENTRY C2325 20230112 C227C2325000 1 SUBENT C2325001 20230112 C227C2325001 1 BIB 10 33 C2325001 2 TITLE Isomeric cross sections and yield ratios of (d,p) C2325001 3 reactions below 15 MeV C2325001 4 AUTHOR (J.B.Natowitz,R.L.Wolke) C2325001 5 REFERENCE (J,PR,155,1352,1967) C2325001 6 #doi:10.1103/physrev.155.1352 C2325001 7 (R,TID-21525,1965) Tabulated data. C2325001 8 INSTITUTE (1USAPUP) C2325001 9 FACILITY (CYCLO,1USAPUP) The University of Pittsburgh cyclotron.C2325001 10 SAMPLE Metal foils were used as targets whenever possible. C2325001 11 If foils were unavailable, uniform (4%) layers of C2325001 12 powdered compounds were deposited on backings of C2325001 13 glass-fiber filter paper, weighed, covered with mylar C2325001 14 tape, and assembled into stacks with Al foils as beam C2325001 15 degraders. C2325001 16 DETECTOR (PROPC,NAICR) 4pi methane-flow proportional counters C2325001 17 or with a calibrated 3 in. x 3 in. NaI(Tl) crystal and C2325001 18 a 512-channel pulse-height analyzer. C2325001 19 METHOD (CHSEP,ACTIV) After the irradiations, the targets C2325001 20 were subjected to adaptations of standard C2325001 21 radiochemical procedures. The final samples were C2325001 22 mounted either on Al cards and covered with 0.9 C2325001 23 mg/cm2 of mylar or between two films of aluminized C2325001 24 mylar on an aluminum ring. Absolute beta or gamma C2325001 25 counting was accomplished with proportional counter C2325001 26 and NaI crystal. C2325001 27 DECAY-DATA Authors are not very specific about decay data: C2325001 28 Nuclear Data Sheets, compiled by K. Way et al., C2325001 29 Printing and publishing once, National Academy of C2325001 30 Sciences-National Research Council, Washington 25, D.C.C2325001 31 HISTORY (20180618C) BP C2325001 32 (20230112A) BP: Added the report reference, updated C2325001 33 entry with tabulated data from R,TID-21525,1965. Added C2325001 34 subentries 20-25. C2325001 35 ENDBIB 33 0 C2325001 36 NOCOMMON 0 0 C2325001 37 ENDSUBENT 36 0 C232500199999 SUBENT C2325002 20230112 C227C2325002 1 BIB 4 12 C2325002 2 REACTION (27-CO-59(D,P)27-CO-60-M,,SIG) C2325002 3 ERR-ANALYS (DATA-ERR) The experimental errors shown in the C2325002 4 figures were obtained by assigning estimated errors C2325002 5 to all measured quantities and propagating C2325002 6 interactions in which only a fraction of the C2325002 7 projectile's angular momentum is transferred to the C2325002 8 target nucleus. C2325002 9 STATUS (TABLE) Table VI, page 22 of R,TID-21525,1965 C2325002 10 (absolute values). Fig. 1, page 1353 of C2325002 11 J,PR,155,1352,1967 (Errors). C2325002 12 HISTORY (20230112A) BP: partially replaced digitized with C2325002 13 tabulated data. C2325002 14 ENDBIB 12 0 C2325002 15 NOCOMMON 0 0 C2325002 16 DATA 3 10 C2325002 17 EN DATA DATA-ERR C2325002 18 MEV MB MB C2325002 19 5.80 99.0 1.104E+01 C2325002 20 6.55 140.0 1.796E+01 C2325002 21 7.00 170.0 2.198E+01 C2325002 22 8.00 160.0 1.893E+01 C2325002 23 9.40 150.0 1.934E+01 C2325002 24 10.4 130.0 1.667E+01 C2325002 25 11.2 110.0 1.305E+01 C2325002 26 12.4 98.0 1.264E+01 C2325002 27 13.0 89.0 9.822E+00 C2325002 28 13.8 75.0 9.898E+00 C2325002 29 ENDDATA 12 0 C2325002 30 ENDSUBENT 29 0 C232500299999 SUBENT C2325003 20230112 C227C2325003 1 BIB 4 12 C2325003 2 REACTION (27-CO-59(D,P)27-CO-60-G,,SIG) C2325003 3 ERR-ANALYS (DATA-ERR) The experimental errors shown in the C2325003 4 figures were obtained by assigning estimated errors C2325003 5 to all measured quantities and propagating C2325003 6 interactions in which only a fraction of the C2325003 7 projectile's angular momentum is transferred to the C2325003 8 target nucleus. C2325003 9 STATUS (TABLE) Table VI, page 22 of R,TID-21525,1965 C2325003 10 (absolute values). Fig. 1, page 1353 of C2325003 11 J,PR,155,1352,1967 (Errors). C2325003 12 HISTORY (20230112A) BP: partially replaced digitized with C2325003 13 tabulated data. C2325003 14 ENDBIB 12 0 C2325003 15 NOCOMMON 0 0 C2325003 16 DATA 3 10 C2325003 17 EN DATA DATA-ERR C2325003 18 MEV MB MB C2325003 19 5.80 86.0 16.95 C2325003 20 6.55 120.0 24.89 C2325003 21 7.00 160.0 33.85 C2325003 22 8.00 150.0 35.16 C2325003 23 9.40 120.0 24.63 C2325003 24 10.4 140.0 28.58 C2325003 25 11.2 120.0 24.11 C2325003 26 12.4 97.0 18.2 C2325003 27 13.0 100.0 20.56 C2325003 28 13.8 110.0 25.19 C2325003 29 ENDDATA 12 0 C2325003 30 ENDSUBENT 29 0 C232500399999 SUBENT C2325004 20230112 C227C2325004 1 BIB 3 8 C2325004 2 REACTION (39-Y-89(D,P)39-Y-90-M,,SIG) C2325004 3 ERR-ANALYS (DATA-ERR) The experimental errors shown in the C2325004 4 figures were obtained by assigning estimated errors C2325004 5 to all measured quantities and propagating C2325004 6 interactions in which only a fraction of the C2325004 7 projectile's angular momentum is transferred to the C2325004 8 target nucleus. C2325004 9 STATUS (CURVE) Fig. 2, page 1353 of J,PR,155,1352,1967. C2325004 10 ENDBIB 8 0 C2325004 11 NOCOMMON 0 0 C2325004 12 DATA 3 7 C2325004 13 EN DATA DATA-ERR C2325004 14 MEV MB MB C2325004 15 5.177 3.797E+00 4.495E-01 C2325004 16 8.381 1.401E+01 1.939E+00 C2325004 17 9.590 2.523E+01 2.472E+00 C2325004 18 11.837 1.412E+01 1.529E+00 C2325004 19 12.539 1.111E+01 1.431E+00 C2325004 20 14.066 1.208E+01 1.556E+00 C2325004 21 14.452 1.504E+01 1.785E+00 C2325004 22 ENDDATA 9 0 C2325004 23 ENDSUBENT 22 0 C232500499999 SUBENT C2325005 20230112 C227C2325005 1 BIB 3 8 C2325005 2 REACTION (39-Y-89(D,P)39-Y-90-G,,SIG) C2325005 3 ERR-ANALYS (DATA-ERR) The experimental errors shown in the C2325005 4 figures were obtained by assigning estimated errors C2325005 5 to all measured quantities and propagating C2325005 6 interactions in which only a fraction of the C2325005 7 projectile's angular momentum is transferred to the C2325005 8 target nucleus. C2325005 9 STATUS (CURVE) Fig. 2, page 1353 of J,PR,155,1352,1967. C2325005 10 ENDBIB 8 0 C2325005 11 NOCOMMON 0 0 C2325005 12 DATA 3 8 C2325005 13 EN DATA DATA-ERR C2325005 14 MEV MB MB C2325005 15 2.647 5.031E+00 6.471E-01 C2325005 16 5.180 1.137E+02 1.235E+01 C2325005 17 8.418 1.835E+02 1.419E+01 C2325005 18 9.586 2.750E+02 3.542E+01 C2325005 19 11.793 1.237E+02 1.217E+01 C2325005 20 12.543 1.008E+02 9.895E+00 C2325005 21 14.127 9.122E+01 1.084E+01 C2325005 22 14.464 1.123E+02 1.217E+01 C2325005 23 ENDDATA 10 0 C2325005 24 ENDSUBENT 23 0 C232500599999 SUBENT C2325006 20230112 C227C2325006 1 BIB 4 12 C2325006 2 REACTION (45-RH-103(D,P)45-RH-104-M,,SIG) C2325006 3 ERR-ANALYS (DATA-ERR) The experimental errors shown in the C2325006 4 figures were obtained by assigning estimated errors C2325006 5 to all measured quantities and propagating C2325006 6 interactions in which only a fraction of the C2325006 7 projectile's angular momentum is transferred to the C2325006 8 target nucleus. C2325006 9 STATUS Table VII, page 23 of R,TID-21525,1965 C2325006 10 (absolute values). Fig. 3, page 1354 of C2325006 11 J,PR,155,1352,1967 (Errors). C2325006 12 HISTORY (20230112A) BP: partially replaced digitized with C2325006 13 tabulated data. C2325006 14 ENDBIB 12 0 C2325006 15 NOCOMMON 0 0 C2325006 16 DATA 3 9 C2325006 17 EN DATA DATA-ERR C2325006 18 MEV MB MB C2325006 19 5.75 4.5 5.304E-01 C2325006 20 6.20 5.5 6.393E-01 C2325006 21 6.37 9.5 1.220E+00 C2325006 22 7.70 21.0 2.701E+00 C2325006 23 9.70 30.0 C2325006 24 9.90 30.0 3.830E+00 C2325006 25 12.0 35.0 3.143E+00 C2325006 26 13.6 33.0 3.842E+00 C2325006 27 14.4 32.0 3.075E+00 C2325006 28 ENDDATA 11 0 C2325006 29 ENDSUBENT 28 0 C232500699999 SUBENT C2325007 20230112 C227C2325007 1 BIB 3 8 C2325007 2 REACTION (45-RH-103(D,P)45-RH-104-G,,SIG) C2325007 3 ERR-ANALYS (DATA-ERR) The experimental errors shown in the C2325007 4 figures were obtained by assigning estimated errors C2325007 5 to all measured quantities and propagating C2325007 6 interactions in which only a fraction of the C2325007 7 projectile's angular momentum is transferred to the C2325007 8 target nucleus. C2325007 9 STATUS (CURVE) Fig. 3, page 1354 of J,PR,155,1352,1967. C2325007 10 ENDBIB 8 0 C2325007 11 NOCOMMON 0 0 C2325007 12 DATA 3 10 C2325007 13 EN DATA DATA-ERR C2325007 14 MEV MB MB C2325007 15 5.647 3.346E+01 3.896E+00 C2325007 16 6.130 3.837E+01 5.299E+00 C2325007 17 6.280 6.375E+01 8.793E+00 C2325007 18 7.668 1.359E+02 1.876E+01 C2325007 19 9.609 1.681E+02 2.502E+01 C2325007 20 9.825 1.661E+02 2.114E+01 C2325007 21 10.907 1.603E+02 2.211E+01 C2325007 22 11.990 1.508E+02 2.243E+01 C2325007 23 13.455 1.165E+02 1.732E+01 C2325007 24 14.431 1.018E+02 1.404E+01 C2325007 25 ENDDATA 12 0 C2325007 26 ENDSUBENT 25 0 C232500799999 SUBENT C2325008 20230112 C227C2325008 1 BIB 4 12 C2325008 2 REACTION (46-PD-110(D,P)46-PD-111-M,,SIG) C2325008 3 ERR-ANALYS (DATA-ERR) The experimental errors shown in the C2325008 4 figures were obtained by assigning estimated errors C2325008 5 to all measured quantities and propagating C2325008 6 interactions in which only a fraction of the C2325008 7 projectile's angular momentum is transferred to the C2325008 8 target nucleus. C2325008 9 STATUS (TABLE) Table VIII, page 24 of R,TID-21525,1965 C2325008 10 (absolute values). Fig. 4, page 1354 of C2325008 11 J,PR,155,1352,1967 (Errors). C2325008 12 HISTORY (20230112A) BP: partially replaced digitized with C2325008 13 tabulated data. C2325008 14 ENDBIB 12 0 C2325008 15 NOCOMMON 0 0 C2325008 16 DATA 3 7 C2325008 17 EN DATA DATA-ERR C2325008 18 MEV MB MB C2325008 19 4.97 1.1 1.018E-01 C2325008 20 6.90 10.0 1.027E+00 C2325008 21 7.70 16.0 1.848E+00 C2325008 22 9.98 21.0 1.978E+00 C2325008 23 11.3 20.0 2.365E+00 C2325008 24 13.0 21.0 2.006E+00 C2325008 25 14.3 18.0 1.716E+00 C2325008 26 ENDDATA 9 0 C2325008 27 ENDSUBENT 26 0 C232500899999 SUBENT C2325009 20230112 C227C2325009 1 BIB 4 12 C2325009 2 REACTION (46-PD-110(D,P)46-PD-111-G,,SIG) C2325009 3 ERR-ANALYS (DATA-ERR) The experimental errors shown in the C2325009 4 figures were obtained by assigning estimated errors C2325009 5 to all measured quantities and propagating C2325009 6 interactions in which only a fraction of the C2325009 7 projectile's angular momentum is transferred to the C2325009 8 target nucleus. C2325009 9 STATUS (TABLE) Table VIII, page 24 of R,TID-21525,1965 C2325009 10 (absolute values). Fig. 4, page 1354 of C2325009 11 J,PR,155,1352,1967 (Errors). C2325009 12 HISTORY (20230112A) BP: partially replaced digitized with C2325009 13 tabulated data. C2325009 14 ENDBIB 12 0 C2325009 15 NOCOMMON 0 0 C2325009 16 DATA 3 7 C2325009 17 EN DATA DATA-ERR C2325009 18 MEV MB MB C2325009 19 4.97 14.0 2.638E+00 C2325009 20 6.90 110.0 1.566E+01 C2325009 21 7.70 150.0 2.578E+01 C2325009 22 9.98 180.0 2.891E+01 C2325009 23 11.3 140.0 1.829E+01 C2325009 24 13.0 120.0 1.814E+01 C2325009 25 14.3 100.0 1.586E+01 C2325009 26 ENDDATA 9 0 C2325009 27 ENDSUBENT 26 0 C232500999999 SUBENT C2325010 20230112 C227C2325010 1 BIB 4 12 C2325010 2 REACTION (48-CD-114(D,P)48-CD-115-M,,SIG) C2325010 3 ERR-ANALYS (DATA-ERR) The experimental errors shown in the C2325010 4 figures were obtained by assigning estimated errors C2325010 5 to all measured quantities and propagating C2325010 6 interactions in which only a fraction of the C2325010 7 projectile's angular momentum is transferred to the C2325010 8 target nucleus. C2325010 9 STATUS (TABLE) Table IX, page 25 of R,TID-21525,1965 C2325010 10 (absolute values). Fig. 5, page 1354 of C2325010 11 J,PR,155,1352,1967 (Errors). C2325010 12 HISTORY (20230112A) BP: partially replaced digitized with C2325010 13 tabulated data. C2325010 14 ENDBIB 12 0 C2325010 15 NOCOMMON 0 0 C2325010 16 DATA 3 9 C2325010 17 EN DATA DATA-ERR C2325010 18 MEV MB MB C2325010 19 5.35 11.0 1.111E+00 C2325010 20 7.28 42.0 3.775E+00 C2325010 21 8.22 57.0 6.272E+00 C2325010 22 9.08 54.0 5.949E+00 C2325010 23 10.6 52.0 4.665E+00 C2325010 24 12.1 54.0 5.379E+00 C2325010 25 13.3 52.0 5.156E+00 C2325010 26 14.2 65.0 5.888E+00 C2325010 27 14.3 67.0 4.879E+00 C2325010 28 ENDDATA 11 0 C2325010 29 ENDSUBENT 28 0 C232501099999 SUBENT C2325011 20230112 C227C2325011 1 BIB 4 12 C2325011 2 REACTION (48-CD-114(D,P)48-CD-115-G,,SIG) C2325011 3 ERR-ANALYS (DATA-ERR) The experimental errors shown in the C2325011 4 figures were obtained by assigning estimated errors C2325011 5 to all measured quantities and propagating C2325011 6 interactions in which only a fraction of the C2325011 7 projectile's angular momentum is transferred to the C2325011 8 target nucleus. C2325011 9 STATUS (TABLE) Table IX, page 25 of R,TID-21525,1965 C2325011 10 (absolute values). Fig. 5, page 1354 of C2325011 11 J,PR,155,1352,1967 (Errors). C2325011 12 HISTORY (20230112A) BP: partially replaced digitized with C2325011 13 tabulated data. C2325011 14 ENDBIB 12 0 C2325011 15 NOCOMMON 0 0 C2325011 16 DATA 3 9 C2325011 17 EN DATA DATA-ERR C2325011 18 MEV MB MB C2325011 19 5.35 61.0 6.173E+00 C2325011 20 7.28 184.0 1.662E+01 C2325011 21 8.22 230.0 2.318E+01 C2325011 22 9.08 200.0 1.809E+01 C2325011 23 10.6 190.0 1.734E+01 C2325011 24 12.1 190.0 1.549E+01 C2325011 25 13.3 160.0 1.652E+01 C2325011 26 14.2 200.0 1.599E+01 C2325011 27 14.3 180.0 1.252E+01 C2325011 28 ENDDATA 11 0 C2325011 29 ENDSUBENT 28 0 C232501199999 SUBENT C2325012 20230112 C227C2325012 1 BIB 4 12 C2325012 2 REACTION (55-CS-133(D,P)55-CS-134-M,,SIG) C2325012 3 ERR-ANALYS (DATA-ERR) The experimental errors shown in the C2325012 4 figures were obtained by assigning estimated errors C2325012 5 to all measured quantities and propagating C2325012 6 interactions in which only a fraction of the C2325012 7 projectile's angular momentum is transferred to the C2325012 8 target nucleus. C2325012 9 STATUS (TABLE) Table X, page 26 of R,TID-21525,1965 C2325012 10 (absolute values). Fig. 6, page 1354 of C2325012 11 J,PR,155,1352,1967 (Errors). C2325012 12 HISTORY (20230112A) BP: partially replaced digitized with C2325012 13 tabulated data. C2325012 14 ENDBIB 12 0 C2325012 15 NOCOMMON 0 0 C2325012 16 DATA 3 10 C2325012 17 EN DATA DATA-ERR C2325012 18 MEV MB MB C2325012 19 2.55 1.3 1.945E-01 C2325012 20 4.08 6.1 5.951E-01 C2325012 21 5.25 5.0 1.137E+00 C2325012 22 7.62 37.0 4.858E+00 C2325012 23 8.33 38.0 4.901E+00 C2325012 24 10.4 20.0 1.963E+00 C2325012 25 11.1 37.0 4.210E+00 C2325012 26 12.3 44.0 4.295E+00 C2325012 27 14.0 41.0 5.257E+00 C2325012 28 14.0 40.0 C2325012 29 ENDDATA 12 0 C2325012 30 ENDSUBENT 29 0 C232501299999 SUBENT C2325013 20230112 C227C2325013 1 BIB 4 12 C2325013 2 REACTION (55-CS-133(D,P)55-CS-134-G,,SIG) C2325013 3 ERR-ANALYS (DATA-ERR) The experimental errors shown in the C2325013 4 figures were obtained by assigning estimated errors C2325013 5 to all measured quantities and propagating C2325013 6 interactions in which only a fraction of the C2325013 7 projectile's angular momentum is transferred to the C2325013 8 target nucleus. C2325013 9 STATUS (TABLE) Table X, page 26 of R,TID-21525,1965 C2325013 10 (absolute values). Fig. 6, page 1354 of C2325013 11 J,PR,155,1352,1967 (Errors). C2325013 12 HISTORY (20230112A) BP: partially replaced digitized with C2325013 13 tabulated data. C2325013 14 ENDBIB 12 0 C2325013 15 NOCOMMON 0 0 C2325013 16 DATA 3 9 C2325013 17 EN DATA DATA-ERR C2325013 18 MEV MB MB C2325013 19 2.55 5.8 6.576E-01 C2325013 20 4.08 28.0 2.503E+00 C2325013 21 5.25 20.0 3.147E+00 C2325013 22 7.62 150.0 1.388E+01 C2325013 23 8.33 170.0 1.826E+01 C2325013 24 10.4 74.0 7.486E+00 C2325013 25 11.1 120.0 1.159E+01 C2325013 26 12.3 160.0 1.936E+01 C2325013 27 14.0 140.0 1.447E+01 C2325013 28 ENDDATA 11 0 C2325013 29 ENDSUBENT 28 0 C232501399999 SUBENT C2325014 20230112 C227C2325014 1 BIB 4 12 C2325014 2 REACTION (73-TA-181(D,P)73-TA-182-M,,SIG) C2325014 3 ERR-ANALYS (DATA-ERR) The experimental errors shown in the C2325014 4 figures were obtained by assigning estimated errors C2325014 5 to all measured quantities and propagating C2325014 6 interactions in which only a fraction of the C2325014 7 projectile's angular momentum is transferred to the C2325014 8 target nucleus. C2325014 9 STATUS (TABLE) Table XI, page 27 of R,TID-21525,1965 C2325014 10 (absolute values). Fig. 7, page 1355 of C2325014 11 J,PR,155,1352,1967 (Errors). C2325014 12 HISTORY (20230112A) BP: partially replaced digitized with C2325014 13 tabulated data. C2325014 14 ENDBIB 12 0 C2325014 15 NOCOMMON 0 0 C2325014 16 DATA 3 12 C2325014 17 EN DATA DATA-ERR C2325014 18 MEV MB MB C2325014 19 5.73 0.015 C2325014 20 7.50 0.030 C2325014 21 8.90 0.15 2.114E-02 C2325014 22 8.98 0.91 9.76E-02 C2325014 23 9.22 0.84 8.805E-02 C2325014 24 11.0 1.9 0.1651 C2325014 25 11.9 2.9 0.3126 C2325014 26 12.4 3.2 0.3464 C2325014 27 13.1 3.8 0.3703 C2325014 28 14.0 4.0 0.3081 C2325014 29 14.7 4.5 0.4482 C2325014 30 14.8 4.6 C2325014 31 ENDDATA 14 0 C2325014 32 ENDSUBENT 31 0 C232501499999 SUBENT C2325015 20230112 C227C2325015 1 BIB 4 12 C2325015 2 REACTION (73-TA-181(D,P)73-TA-182-G,,SIG) C2325015 3 ERR-ANALYS (DATA-ERR) The experimental errors shown in the C2325015 4 figures were obtained by assigning estimated errors C2325015 5 to all measured quantities and propagating C2325015 6 interactions in which only a fraction of the C2325015 7 projectile's angular momentum is transferred to the C2325015 8 target nucleus. C2325015 9 STATUS (TABLE) Table XI, page 27 of R,TID-21525,1965 C2325015 10 (absolute values). Fig. 7, page 1355 of C2325015 11 J,PR,155,1352,1967 (Errors). C2325015 12 HISTORY (20230112A) BP: partially replaced digitized with C2325015 13 tabulated data. C2325015 14 ENDBIB 12 0 C2325015 15 NOCOMMON 0 0 C2325015 16 DATA 3 12 C2325015 17 EN DATA DATA-ERR C2325015 18 MEV MB MB C2325015 19 5.73 5.0 5.856E-01 C2325015 20 7.50 7.1 6.223E-01 C2325015 21 8.90 55.0 6.035E+00 C2325015 22 8.98 170.0 1.852E+01 C2325015 23 9.22 120.0 1.177E+01 C2325015 24 11.0 180.0 1.977E+01 C2325015 25 11.9 240.0 2.128E+01 C2325015 26 12.4 210.0 1.848E+01 C2325015 27 13.1 220.0 1.961E+01 C2325015 28 14.0 210.0 2.086E+01 C2325015 29 14.7 210.0 1.903E+01 C2325015 30 14.8 220.0 2.159E+01 C2325015 31 ENDDATA 14 0 C2325015 32 ENDSUBENT 31 0 C232501599999 SUBENT C2325016 20230112 C227C2325016 1 BIB 4 12 C2325016 2 REACTION (75-RE-187(D,P)75-RE-188-M,,SIG) C2325016 3 ERR-ANALYS (DATA-ERR) The experimental errors shown in the C2325016 4 figures were obtained by assigning estimated errors C2325016 5 to all measured quantities and propagating C2325016 6 interactions in which only a fraction of the C2325016 7 projectile's angular momentum is transferred to the C2325016 8 target nucleus. C2325016 9 STATUS (TABLE) Table XII, page 28 of R,TID-21525,1965 C2325016 10 (absolute values). Fig. 8, page 1355 of C2325016 11 J,PR,155,1352,1967 (Errors). C2325016 12 HISTORY (20230112A) BP: partially replaced digitized with C2325016 13 tabulated data. C2325016 14 ENDBIB 12 0 C2325016 15 NOCOMMON 0 0 C2325016 16 DATA 3 8 C2325016 17 EN DATA DATA-ERR C2325016 18 MEV MB MB C2325016 19 4.03 0.081 C2325016 20 7.80 1.83 1.796E-01 C2325016 21 8.35 7.14 9.258E-01 C2325016 22 9.65 10.0 7.250E-01 C2325016 23 11.0 14.0 1.649E+00 C2325016 24 12.3 17.0 2.193E+00 C2325016 25 14.1 24.0 3.119E+00 C2325016 26 14.2 25.4 2.991E+00 C2325016 27 ENDDATA 10 0 C2325016 28 ENDSUBENT 27 0 C232501699999 SUBENT C2325017 20230112 C227C2325017 1 BIB 4 12 C2325017 2 REACTION (75-RE-187(D,P)75-RE-188-G,,SIG) C2325017 3 ERR-ANALYS (DATA-ERR) The experimental errors shown in the C2325017 4 figures were obtained by assigning estimated errors C2325017 5 to all measured quantities and propagating C2325017 6 interactions in which only a fraction of the C2325017 7 projectile's angular momentum is transferred to the C2325017 8 target nucleus. C2325017 9 STATUS (TABLE) Table XII, page 28 of R,TID-21525,1965 C2325017 10 (absolute values). Fig. 8, page 1355 of C2325017 11 J,PR,155,1352,1967 (Errors). C2325017 12 HISTORY (20230112A) BP: partially replaced digitized with C2325017 13 tabulated data. C2325017 14 ENDBIB 12 0 C2325017 15 NOCOMMON 0 0 C2325017 16 DATA 3 8 C2325017 17 EN DATA DATA-ERR C2325017 18 MEV MB MB C2325017 19 4.03 1.22 1.455E-01 C2325017 20 7.80 25.6 2.875E+00 C2325017 21 8.35 119.0 1.464E+01 C2325017 22 9.65 156.0 1.625E+01 C2325017 23 11.0 194.0 1.741E+01 C2325017 24 12.3 184.0 2.302E+01 C2325017 25 14.1 189.0 2.500E+01 C2325017 26 14.2 204.0 2.613E+01 C2325017 27 ENDDATA 10 0 C2325017 28 ENDSUBENT 27 0 C232501799999 SUBENT C2325018 20230112 C227C2325018 1 BIB 4 12 C2325018 2 REACTION (78-PT-196(D,P)78-PT-197-M,,SIG) C2325018 3 ERR-ANALYS (DATA-ERR) The experimental errors shown in the C2325018 4 figures were obtained by assigning estimated errors C2325018 5 to all measured quantities and propagating C2325018 6 interactions in which only a fraction of the C2325018 7 projectile's angular momentum is transferred to the C2325018 8 target nucleus. C2325018 9 STATUS (TABLE) Table XIII, page 29 of R,TID-21525,1965 C2325018 10 (absolute values). Fig. 9, page 1355 of C2325018 11 J,PR,155,1352,1967 (Errors). C2325018 12 HISTORY (20230112A) BP: partially replaced digitized with C2325018 13 tabulated data. C2325018 14 ENDBIB 12 0 C2325018 15 NOCOMMON 0 0 C2325018 16 DATA 3 6 C2325018 17 EN DATA DATA-ERR C2325018 18 MEV MB MB C2325018 19 7.42 3.87 4.699E-01 C2325018 20 8.80 8.71 1.033E+00 C2325018 21 9.98 10.9 1.203E+00 C2325018 22 11.1 16.9 1.519E+00 C2325018 23 12.1 30.1 3.556E+00 C2325018 24 14.3 30.6 3.120E+00 C2325018 25 ENDDATA 8 0 C2325018 26 ENDSUBENT 25 0 C232501899999 SUBENT C2325019 20230112 C227C2325019 1 BIB 4 12 C2325019 2 REACTION (78-PT-196(D,P)78-PT-197-G,,SIG) C2325019 3 ERR-ANALYS (DATA-ERR) The experimental errors shown in the C2325019 4 figures were obtained by assigning estimated errors C2325019 5 to all measured quantities and propagating C2325019 6 interactions in which only a fraction of the C2325019 7 projectile's angular momentum is transferred to the C2325019 8 target nucleus. C2325019 9 STATUS (TABLE) Table XIII, page 29 of R,TID-21525,1965 C2325019 10 (absolute values). Fig. 9, page 1355 of C2325019 11 J,PR,155,1352,1967 (Errors). C2325019 12 HISTORY (20230112A) BP: partially replaced digitized with C2325019 13 tabulated data. C2325019 14 ENDBIB 12 0 C2325019 15 NOCOMMON 0 0 C2325019 16 DATA 3 6 C2325019 17 EN DATA DATA-ERR C2325019 18 MEV MB MB C2325019 19 7.42 17.8 1.985E+00 C2325019 20 8.80 55.5 6.668E+00 C2325019 21 9.98 62.6 6.856E+00 C2325019 22 11.1 81.5 9.586E+00 C2325019 23 12.1 117.0 1.407E+01 C2325019 24 14.3 111.0 1.097E+01 C2325019 25 ENDDATA 8 0 C2325019 26 ENDSUBENT 25 0 C232501999999 SUBENT C2325020 20230119 C227C2325020 1 BIB 3 3 C2325020 2 REACTION (42-MO-92(D,N)43-TC-93-M,,SIG) C2325020 3 STATUS (TABLE) Table XIV, page 30 of R,TID-21525,1965. C2325020 4 HISTORY (20230119C) BP C2325020 5 ENDBIB 3 0 C2325020 6 NOCOMMON 0 0 C2325020 7 DATA 2 11 C2325020 8 EN DATA C2325020 9 MEV MB C2325020 10 0.80 2.6 C2325020 11 4.67 23.0 C2325020 12 6.75 56.0 C2325020 13 9.05 39.0 C2325020 14 10.8 36.0 C2325020 15 11.0 40.0 C2325020 16 12.0 21.0 C2325020 17 12.4 25.0 C2325020 18 13.3 24.0 C2325020 19 13.7 24.0 C2325020 20 14.1 23.0 C2325020 21 ENDDATA 13 0 C2325020 22 ENDSUBENT 21 0 C232502099999 SUBENT C2325021 20230119 C227C2325021 1 BIB 3 3 C2325021 2 REACTION (42-MO-92(D,N)43-TC-93-G,,SIG) C2325021 3 STATUS (TABLE) Table XIV, page 30 of R,TID-21525,1965. C2325021 4 HISTORY (20230119C) BP C2325021 5 ENDBIB 3 0 C2325021 6 NOCOMMON 0 0 C2325021 7 DATA 2 11 C2325021 8 EN DATA C2325021 9 MEV MB C2325021 10 0.80 4.8 C2325021 11 4.67 44.0 C2325021 12 6.75 170.0 C2325021 13 9.05 140.0 C2325021 14 10.8 150.0 C2325021 15 11.0 150.0 C2325021 16 12.0 95.0 C2325021 17 12.4 100.0 C2325021 18 13.3 97.0 C2325021 19 13.7 110.0 C2325021 20 14.1 92.0 C2325021 21 ENDDATA 13 0 C2325021 22 ENDSUBENT 21 0 C232502199999 SUBENT C2325022 20230119 C227C2325022 1 BIB 3 3 C2325022 2 REACTION (40-ZR-94(D,N)41-NB-95-M,,SIG) C2325022 3 STATUS (TABLE) Table XV, page 31 of R,TID-21525,1965. C2325022 4 HISTORY (20230119C) BP C2325022 5 ENDBIB 3 0 C2325022 6 NOCOMMON 0 0 C2325022 7 DATA 2 9 C2325022 8 EN DATA C2325022 9 MEV MB C2325022 10 5.95 35.0 C2325022 11 7.87 52.0 C2325022 12 9.30 51.0 C2325022 13 10.7 42.0 C2325022 14 11.0 35.0 C2325022 15 11.9 36.0 C2325022 16 13.3 32.0 C2325022 17 14.3 31.0 C2325022 18 14.4 30.0 C2325022 19 ENDDATA 11 0 C2325022 20 ENDSUBENT 19 0 C232502299999 SUBENT C2325023 20230119 C227C2325023 1 BIB 3 3 C2325023 2 REACTION (40-ZR-94(D,N)41-NB-95-G,,SIG) C2325023 3 STATUS (TABLE) Table XV, page 31 of R,TID-21525,1965. C2325023 4 HISTORY (20230119C) BP C2325023 5 ENDBIB 3 0 C2325023 6 NOCOMMON 0 0 C2325023 7 DATA 2 9 C2325023 8 EN DATA C2325023 9 MEV MB C2325023 10 5.95 45.0 C2325023 11 7.87 60.0 C2325023 12 9.30 70.0 C2325023 13 10.7 52.0 C2325023 14 11.0 42.0 C2325023 15 11.9 43.0 C2325023 16 13.3 43.0 C2325023 17 14.3 40.0 C2325023 18 14.4 40.0 C2325023 19 ENDDATA 11 0 C2325023 20 ENDSUBENT 19 0 C232502399999 SUBENT C2325024 20230119 C227C2325024 1 BIB 3 3 C2325024 2 REACTION (31-GA-71(D,A)30-ZN-69-M,,SIG) C2325024 3 STATUS (TABLE) Table XVI, page 32 of R,TID-21525,1965. C2325024 4 HISTORY (20230119C) BP C2325024 5 ENDBIB 3 0 C2325024 6 NOCOMMON 0 0 C2325024 7 DATA 2 9 C2325024 8 EN DATA C2325024 9 MEV MB C2325024 10 4.52 0.13 C2325024 11 6.50 0.32 C2325024 12 6.97 0.72 C2325024 13 8.85 0.93 C2325024 14 10.4 1.2 C2325024 15 12.0 1.3 C2325024 16 12.8 1.2 C2325024 17 14.0 2.2 C2325024 18 14.5 3.1 C2325024 19 ENDDATA 11 0 C2325024 20 ENDSUBENT 19 0 C232502499999 SUBENT C2325025 20230119 C227C2325025 1 BIB 3 3 C2325025 2 REACTION (31-GA-71(D,A)30-ZN-69-G,,SIG) C2325025 3 STATUS (TABLE) Table XVI, page 32 of R,TID-21525,1965. C2325025 4 HISTORY (20230119C) BP C2325025 5 ENDBIB 3 0 C2325025 6 NOCOMMON 0 0 C2325025 7 DATA 2 9 C2325025 8 EN DATA C2325025 9 MEV MB C2325025 10 4.52 0.27 C2325025 11 6.50 0.56 C2325025 12 6.97 1.0 C2325025 13 8.85 1.1 C2325025 14 10.4 1.4 C2325025 15 12.0 1.0 C2325025 16 12.8 1.2 C2325025 17 14.0 2.0 C2325025 18 14.5 2.5 C2325025 19 ENDDATA 11 0 C2325025 20 ENDSUBENT 19 0 C232502599999 ENDENTRY 25 0 C232599999999