Nuclear Data Sheets for A = 110 *

Nuclear Data Sheets 89, 481 (2000) doi:10.1006/ndsh.2000.0004 Nuclear Data Sheets for A = 110 * D. DE FRENNE AND E. JACOBS Vakgroep Subatomaire E(n) Stralingsfysica Proeftuinstraat 86, β 9000 Gent, Belgium (Received February 2, 1999; Revised November 12, 1999) Abstract: The 1992 evaluation on mass A=110 has been revised, taking into account all data available before January 1999. Detailed experimental information is presented from the neutron rich nucleus 110 Zr to the neutron deficient 110 Xe nucleus. Cutoff Date: January 1999. General Policies and Organization of Material: See the January issue of Nuclear Data Sheets. * Research sponsored by the fund for Scientific Research Flanders. 0090 3752/00 $35.00 Copyright 2000 by Academic Press. All rights of reproduction in any form reserved. 481

NUCLEAR DATA SHEETS Index for A = 110 Nuclide Data Type Page Nuclide Data Type Page Skeleton Scheme for A=110 484 110 Zr Adopted Levels 486 110 Nb Adopted Levels 486 110 Mo Adopted Levels 486 110 Tc Adopted Levels, Gammas 487 110 Mo β Decay 487 110 Ru Adopted Levels, Gammas 489 110 Tc β Decay 490 248 Cm, 252 Cf SF Decay 491 110 Sb Adopted Levels, Gammas 621 110 Te ε Decay 625 54 Fe( 59 Co,2pn), 56 Fe( 58 Ni,3pn) 625 110 Te Adopted Levels, Gammas 627 54 Fe( 58 Ni,2pγ) 629 58 Ni( 58 Ni,α2pγ) 631 110 I Adopted Levels 634 114 Cs α Decay 634 110 Xe Adopted Levels 634 110 Rh Adopted Levels, Gammas 494 110 Ru β Decay (11.6 s) 494 110 Pd Adopted Levels, Gammas 496 110 Rh β Decay (3.2 s) 503 110 Rh β Decay (28.5 s) 504 110 Ag ε Decay (24.6 s) 505 108 Pd(t,p) 506 110 Pd(e,e') 507 110 Pd(π,X) 507 110 Pd(n,n'γ) 507 110 Pd(p,p'),(d,d'),(pol d,d') 511 110 Pd(p,p'γ) 514 110 Pd(α,α') 515 Coulomb Excitation 515 110 Ag Adopted Levels, Gammas 520 110 Ag IT Decay (249.76 d) 524 109 Ag(n,γ) E=thermal 525 109 Ag(n,γ) E=5.2 ev Res 531 109 Ag(d,p) 531 109 Ag(d,pγ) 532 110 Pd(p,nγ) 532 110 Cd Adopted Levels, Gammas 534 110 Ag β Decay (24.6 s) 558 110 Ag β Decay (249.76 d) 559 110 In ε Decay (69.1 min) 563 110 In ε Decay (4.9 h) 567 108 Pd( 3 He,n) 570 108 Pd(α,2nγ), 110 Pd(α,4nγ) 570 109 Ag(p,p), (p,n) IAR 575 109 Ag( 3 He,d) 576 110 Cd(γ,γ') 576 110 Cd(e,e') 577 110 Cd(n,n'γ) 577 110 Cd(p,p'), 110 Pd(d,d') 582 110 Cd(p,p'γ) 583 110 Cd(α,α') 584 Coulomb Excitation 585 111 Cd(p,d) 586 111 Cd(d,t) 586 111 Cd(pol d,t) 586 112 Cd(p,t) 588 114 Sn(d, 6 Li) 588 (HI,xnγ) 588 110 In Adopted Levels, Gammas 593 110 Sn ε Decay 597 100 Mo( 14 N,4nγ) 599 107 Ag(α,nγ) 601 110 Cd(p,n) 604 110 Cd(p,nγ) 604 110 Cd(d,2n) 608 110 Sn Adopted Levels, Gammas 609 110 Sb ε Decay 611 94 Mo( 19 F,p2nγ) 613 98 Mo( 16 O,4nγ) 615 108 Cd(α,2nγ) 617 110 Cd( 3 He,3nγ), 104 Pd( 12 C,α2nγ) 619 112 Sn(p,t) 620 113 In(p,4nγ), 112 Sn(p,p2nγ) 620 113 In(p,xn), 115 In(p,xn) 620 482

NUCLEAR DATA SHEETS Skeleton Scheme for A=110 S(α) 9400 SY S(n) 3367 SY 0+ 0.0 >150 ns 11 0 4 0 Zr 70 Q unknown?% 0.0 0.17 s 11 4 0 1 Nb 69 Q =12063 SY 100% S(p) 14648 SY S(α) 8200 SY S(n) 6283 SY 0+ 0.0 0.30 s 11 0 4 2 Mo 68 100% Q =5906 SY S(p) 11406 SY S(α) 6900 SY S(n) 4566 SY (2+) 0.0 0.92 s 11 0 4 3 Tc 67 99.96% Q =8778 SY S(p) 12562 SY S(n) 7360 SY S(α) 6310 230 S(p) 9390 230 S(n) 6010 SY S(α) 5597 SY 0+ 0.0 11.6 s 11 0 4 4 Ru 66 1+ y 100% ( 4) x Q =2810 50 11 4 0 5 Rh 65 Q =5400 220 S(p) 10626 5 S(n) 8818 11 S(p) 7142.8 20 S(n) 6809.20 10 S(α) 4450 14 S(α) 3519 9 6+ 117.59 1+ 0.0 24.6 s 0+ 0.0 11 0 4 7 Ag 63 0.30% 6 99.70% 6 11 0 4 6 Pd 64 Q =2892.2 16 Q + =892 11 S(n) 9916 3 S(p) 8919.0 16 S(α) 2870 6 0+ 0.0 11 4 0 8 Cd 62 484

NUCLEAR DATA SHEETS Skeleton Scheme for A=110 (continued) S(n) 8058 13 S(p) 5255 12 S(α) 1957 13 2+ 62.1 7+ 0.0 4.9 h 11 0 4 9 In 61 100% Q + =3878 12 S(n) 11270 17 S(p) 6638 16 S(α) 1126 17 0+ 0.0 4.11 h 11 0 5 0 Sn 60 100% Q + =637 20 S(n) 9350 SY S(p) 2188 SY (3+,4+) 0.0 23.0 s 11 0 5 1 Sb 59 100% Q + =8300 SY S(n) 12775 SY S(p) 3310 SY 0+ 0.0 18.6 s 11 0 5 2 Te 58 100% 3 10 3 % Q + =5257 SY Q α =2723 16 (1+) 0.0 0.57 s 11 4 5 5 Cs 59 0.018% 6 Q α =3357 50 S(n) 10845 SY S(p) 1435 SY 0.0 11 0 5 4 Xe 56?% S(p) 63 SY Q + =8627 SY 0.0 Q α =3885 14 0.65 s 11 0 5 3 I 57 83% 4 17% 4 Q + =11929 SY Q α =3584 50 Ground State and Isomeric Level Properties Nuclide Level Jπ T 1/2 Decay Modes 110 Zr 0.0 0+ >150 ns %β =? 110 Nb 0.0 0.17 s 2 %β =100; %β n=40 8 110 Mo 0.0 0+ 0.30 s 4 %β =100 110 Tc 0.0 (2+) 0.92 s 3 %β =99.96; %β n=0.04 110 Ru 0.0 0+ 11.6 s 6 %β =100 110 Rh x ( 4) 28.5 s 15 %β =100 y 1+ 3.2 s 2 %β =100 110 Pd 0.0 0+ stable 110 Ag 0.0 1+ 24.6 s 2 %β =99.70 6; %ε=0.30 6 117.59 6+ 249.76 d 4 %β =98.64 6; %IT=1.36 6 110 Cd 0.0 0+ stable 110 In 0.0 7+ 4.9 h 1 %ε+%β + =100 62.1 2+ 69.1 min 5 %ε+%β + =100 110 Sn 0.0 0+ 4.11 h 10 %ε=100 110 Sb 0.0 (3+,4+) 23.0 s 4 %ε+%β + =100 110 Te 0.0 0+ 18.6 s 8 %ε+%β + 100; %α 3 10 3 110 I 0.0 0.65 s 2 %α=17 4; %ε+%β + =83 4; %β + p=11 3; %β + α=1.1 3 110 Xe 0.0 %α=? 114 Cs 0.0 (1+) 0.57 s 2 %α=0.018 6;... 485

110 40 Zr 11 70 NUCLEAR DATA SHEETS 0 40 Zr 70 Adopted Levels Isotope produced by fission of relativistic U ions on lead. Fission products identified using fragment separator (1997Be12). 110 Zr Levels E(level) Jπ T 1/2 Comments 0.0 0+ >150 ns T 1/2 : estimated by 1997Au04. %β =? 11 4 0 1 Nb 69 11 4 0 1 Nb 69 Adopted Levels Q(β )=12063 SY; S(n)=3367 SY; Q(α)= 9400 SY 1995Au04. Isotope produced by Pb( 238 U,F), 1994Be24; and by U(p,F), 1996Me09. 110 Nb Levels E(level) T 1/2 Comments 0.0 0.17 s 2 T 1/2 : from 1996Me09. %β =100; %β n=40 8 (1996Me09). 11 4 0 2 Mo 68 11 4 0 2 Mo 68 Adopted Levels Q(β )=5906 SY; S(n)=6283 SY; S(p)=14648 SY; Q(α)= 8200 SY 1995Au04. Isotope produced by 238 U(p,F), 1992Ay02, 1994Lh02. 110 Mo Levels E(level) Jπ T 1/2 Comments 0.0 0+ 0.30 s 4 %β =100. T 1/2 : from 1994Lh02. Other value: 0.25 s 10 from 1992Ay02 and 1992JoZU. 486

110 43 Tc 67 1 NUCLEAR DATA SHEETS 110 43 Tc 67 1 Adopted Levels, Gammas Q(β )=8778 SY; S(n)=4566 SY; S(p)=11406 SY; Q(α)= 6900 SY 1995Au04. 1969WiZX: assignment by Xγ coin in 252 Cf SF decay. 1973TrZM and 1976Tr02: assignment by chemical separation of Tc from 249 Cf(n,F) and growth decay curve analysis in A=110. 110 Tc Levels Cross Reference (XREF) Flags A 110 Mo β Decay E(level) Jπ XREF T 1/2 Comments 0.0 (2+) A 0.92 s 3 %β =99.96; %β n=0.04 (1996Me09). Jπ: Jπ=(2,3)+ from decay pattern, 142γ from (1+) in D. T 1/2 : from decay of 240γ (1990Ay02). Others: 0.9 s 1 (1987AlZZ), 0.78 s 15 (1996Me09), 1.0 s 2 (1976Tr02), 0.83 s 4 (1969WiZX). T 1/2 : from decay of 240γ (1990Ay02). Others: 0.9 s 1 (1987AlZZ), 1.0 s 2 (1976Tr02), 0.83 s 4 (1969WiZX). 39.45 24 A 53.3 2 (1+) A 142.09 18 (1+) A <10 ns T 1/2 : from 1994Lh02. 186.5 5 A 262.90 23 (1+) A 740.8 4 (1+) A Allowed β decay from 0+ with log ft<5.9. Jπ=(1+) from log ft values for allowed β transitions. γ( 110 Tc) E(level) Eγ Iγ Mult. α Comments 39.45 39.4 3 <8 E1,M1 3.0 11 Mult.: from α(k)exp=2.9 18 (1994Lh02). 53.3 53.3 2 20 4 (M1) 1.3 5 Mult.: E1,M1 from α(k)exp=1.4 7 (1994Lh02). Jπ allow only M1. 142.09 142.1 2 100 14 (M1) 0.08 3 Mult.: from T 1/2 limit, Jπ. 186.5 131.2 4 100 262.90 120.8 2 100 12 223.4 3 58 31 740.8 477.2 9 32 14 598.9 5 100 22 741.0 23 Placement of transition in the level scheme is uncertain. 110 Mo β Decay 1994Lh02 Source produced 238 U(p,F). Mass separated source. Measured βγ(t), and γγ(t). 110 Tc Levels E(level) Jπ T 1/2 0.0 (2+) 39.45 25 53.30 20 (1+) 142.08 19 (1+) <10 ns 184.5 5 262.89 24 (1+) 740.8 5 (1+) Jπ=(1+) from log ft values for allowed β transitions. 487

110 43 Tc 67 2 NUCLEAR DATA SHEETS 110 43 Tc 67 2 110 Mo β Decay 1994Lh02 (continued) β radiations Eβ E(level) Iβ Log ft (5165) 740.8 17 3 4.5 (5643) 262. 89 38 9 4.3 (5722) 184.5 8 3 5.0 (5764) 142. 08 15 9 4.8 (5853) 53. 30 17 6 4.7 Statistical feeding from unobserved levels neglected. For a preliminary calculation of log ft, M1 is assumed for the low energy gammas. For β intensity per 100 decays, multiply by 1. γ( 110 Tc) Iγ normalization: from ΣI(γ+ce)(g.s.)=100. Statistical feeding from unobserved levels neglected. g.s. β feeding assumed to be negligible. Eγ E(level) Iγ Mult. α Comments 39.4 3 39.45 <8 [M1] 4.10 α(k)exp=2.9 18. Mult.: from α(k)exp and intensity balance through 39.4 level. 53.3 2 53.30 20 4 [M1] 1.52 α(k)exp=1.4 7. Mult.: from α(k)exp. 120.8 2 262.89 48 6 [M1] 0.166 131.2 4 184.5 14 6 [M1] 0.132 142.1 2 142.08 100 14 [M1 ] 0. 106 Mult.: from RUL. 223.4 3 262.89 28 15 [M1] 0. 0318 477.2 9 740.8 7 3 598.9 5 740.8 22 5 741.0 740.8 5 For absolute intensity per 100 decays, multiply by 0.49 4. Placement of transition in the level scheme is uncertain. Decay Scheme 0+ 0.0 11 4 0 2 Mo 68 0.30 s Intensities: relative Iγ %β =100 Q (g.s.)=5906 SY Iβ 17 4.5 Log ft 741.0 5 598.9 22 477.2 7 (1+) 740.8 38 8 15 17 4.3 5.0 4.8 4.7 223.4 [M1] 28 120.8 [M1] 48 (1+) 262.89 131.2 [M1] 14 142.1 [M1] 100 184.5 (1+) 142.08 (1+) 53.30 53.3 [M1] 20 39.4 [M1] <8 39.45 (2+) 0.0 <10 ns 11 4 0 3 Tc 67 488

110 44 Ru 66 1 NUCLEAR DATA SHEETS 110 44 Ru 66 1 Adopted Levels, Gammas Q(β )=2810 50; S(n)=7360 SY; S(p)=12562 SY; Q(α)= 6.31 10 3 23 1995Au04. 110 Ru Levels Cross Reference (XREF) Flags A 248 Cm, 252 Cf SF Decay B 110 Tc β Decay E(level) Jπ XREF T 1/2 Comments 0.0 # 0+ AB 11.6 s 6 %β =100. T 1/2 : from time dependence of Eγ=112 kev (1991Jo11). Others: 15.9 s 5 (1969WiZX), 17 s 1 (1975Fe12), 14.7 s 13 (1976MaYL), and 12.6 s 5 (1978Fr16). 240.71 # 10 2+ AB 0.30 ns 2 Jπ: (E2) to g.s. based on ce data in 110 Tc β decay. T 1/2 : from 252 Cf SF decay (1980ChZM). 612.89 @ 14 (2+) B 663.31 # 23 4+ AB 859.96 @ 17 (3+) B 1084.3 @ 4 (4+) A 1239.4 # 5 6+ A 1375.4 @ 5 (5+) A 1396.40 19 (2+) B 1655.9 4 B 1684.1 @ 5 (6+) A 1820.49 23 B 1944.5 # 5 (8+) A 2020.8 @ 7 (7+) A 2046.8 4 B 2242.6 6 A 2396.9 @ 7 (8+) A 2426.2 7 A 2759.2 # 7 (10+) A 2776.7 @ 12 (9+) A 2892.9 11 A 3646.6 # 13 (12+) A 3700.0 13 A 4351.6 # 16 (14+) A 5150.2 # 19 (16+) A Based on systematics of low lying collective states in Ru isotopes, observed branching ratios and mult's based on ce data in 110 Tc β decay (1990Ay02). From observed band structure and γ(θ)'s which are consistent with stretched E2's for levels with Jπ<7 in 252 Cf SF decay (1994Sh26). From observed band structure and γ decay pattern of the levels in 252 Cf SF decay. # J=2 g.s. band. @ J=1 γ vibrational band on Jπ=2+ 612 kev level. γ( 110 Ru) E(level) Eγ Iγ Mult. α Comments 240.71 240.67 11 100 (E2) 0. 0570 Eγ: from 110 Tc β decay (1969WiZX). K/L 4.0 (1970Wa05). Mult.: from experimental K/L value (to be compared with K/L=6.9 for E2 from 1968Ha53) and γ(θ) results of 1972Wi15. B(E2)(W.u.)=70 5. B(E2)(W.u.): deduced from T 1/2 of 240.8 level (1980ChZM). 612.89 371.94 23 100 5 612.88 18 93 5 663.31 422.6 2 100 859.96 247.17 19 22 3 619.13 17 100 5 1084.3 421.2 10 49 6 471.7 3 100 13 843.5 10 17 4 Continued on next page (footnotes at end of table) 489

110 44 Ru 66 2 NUCLEAR DATA SHEETS 110 44 Ru 66 2 Adopted Levels, Gammas (continued) γ( 110 Ru) (continued) E(level) Eγ Iγ E(level) Eγ Iγ E(level) Eγ Iγ 1239.4 576.4 5 100 1375.4 515.4 3 100 8 712.5 10 17 4 1396.40 1155.8 2 100 15 1396.4 5 50 18 1655.9 796.1 5 <56 1415.1 5 100 20 1684.1 445.6 10 9.4 23 599.7 3 100 15 1021.2 10 30 15 1820.49 164.7 5 38 5 424.2 2 100 11 960.5 5 32 11 1579.0 5 48 11 1944.5 705.7 3 100 2020.8 645.4 5 100 2046.8 1186.6 5 46 18 1806.4 5 100 25 2242.6 867.2 4 100 2396.9 712.8 5 100 2426.2 1187.4 5 100 2759.2 814.7 5 100 2776.7 755.9 10 100 2892.9 948.4 10 100 3646.6 887.4 10 100 3700.0 940.8 10 100 4351.6 705.0 10 100 5150.2 798.6 10 100 Level branchings from 110 Tc β decay. Weighted average from 110 Tc β decay and 248 Cm, 252 Cf SF decay data, if available. Uncertainties estimated by the evaluators. 110 Tc β Decay 1990Ay02 1990Ay02: source: mass separated samples of 110 Tc from 235 U(p,F). Measured: β decay T 1/2, Q(β ), Eγ, Iγ, Ice, βγ, γγ. Deduced: 110 Ru levels, Jπ, level systematics. Hartree Fock potential energy calculations. Others: 1969WiZX, 1973TrZM, 1976Tr02, 1988AlZY. 110 Ru Levels E(level) Jπ T 1/2 Comments 0.0 0+ 240.67 11 2+ 0.50 ns 8 612.8 (2+) 0.09 ns 7 T 1/2 : from 1995Sc24. Average of T 1/2 of 372.1 and 613.0 γ. Jπ: based on γ branching ratio to the first 2+ and to the g.s. and on energy systematics. 663.2 4+ 860.0 (3+) 1137. 3? E(level): only observed by 1988AlZY. 1396.4 (2+) 1655.9 1820.6 2046.7 2084. 8? E(level): only observed by 1988AlZY. From adopted levels. γ( 110 Ru) Eγ E(level) Iγ Comments 164.7 5 1820.6 14.0 18 240.67 11 240. 67 1000 Eγ: from 1969WiZX. 247.1 2 860.0 31 4 372.1 2 612.8 170 9 422.6 2 663.2 42 4 424.2 2 1820.6 37 4 613.0 2 612.8 160 8 619.2 2 860.0 140 10 796.1 5 1655.9 <14 896.9 5 1137.3? 20 3 960.5 5 1820.6 12 4 1155.8 2 1396.4 34 5 1186.6 5 2046.7 13 5 1225.3 5 2084.8? 24 3 1396.4 5 1396.4 17 6 Continued on next page (footnotes at end of table) 490

110 44 Ru 66 3 NUCLEAR DATA SHEETS 110 44 Ru 66 3 110 Tc β Decay 1990Ay02 (continued) γ( 110 Ru) (continued) Eγ E(level) Iγ 1415.1 5 1655.9 25 5 1579.0 5 1820.6 18 4 1806.4 5 2046.7 28 7 From 1990Ay02, unless noted otherwise. Uncertainties not given by the authors but estimated by the evaluators. Placement of transition in the level scheme is uncertain. Decay Scheme (2+) 0.0 11 4 0 3 Tc 67 0.92 s Intensities: relative Iγ %β =100 Q =8778 SY 1225.3 24 1806.4 28 1186.6 13 1579.0 18 960.5 12 424.2 37 164.7 14.0 1415.1 25 796.1 <14 1396.4 17 1155.8 34 (2+) 1396.4 896.9 20 422.6 42 613.0 160 372.1 170 (3+) 860.0 619.2 140 247.1 31 4+ 663.2 (2+) 612.8 2+ 240.67 240.67 1000 0+ 0.0 2084.8 2046.7 1820.6 1655.9 1137.3 0.09 ns 0.50 ns 11 4 0 4 Ru 66 248 Cm, 252 Cf SF Decay 1995Lu10: 252 Cf SF decay. Measured: Eγ, Iγ, γγ, γγγ, xx, xγ, xγγ. Deduced: 110 Ru levels, Jπ. 1994Sh26: 248 Cm SF decay. Measured: Eγ, Iγ, γγγ. Deduced: 110 Ru levels, Jπ. Others: 1980ChZM (using 254 Cf SF decay), 1970Wa05, 1971Ch44, 1972Wi15, 1974JaYY, 1974ClZX, 1971Ho29, 1970Ch11, 1970Jo20. 110 Ru Levels E(level) Jπ T 1/2 Comments 0.0 0+ 240.9 3 2+ 0.30 ns 2 T 1/2 : from recoil distance Doppler shift measurements in 254 Cf SF decay (1980ChZM). Others: 0.50 ns 8 (1995Sc24), 0.34 ns 4 (1974JaYY), 0.23 ns (1972Wi15), <0.5 ns (1970Wa05). 612.6 3 2+ 663.2 4 4+ T 1/2 =13.4 ps 10 given by 1986Ma22 is a combined value for 108 Ru+ 110 Ru. 860.0 4 3+ 1084.3 4 (4+) 1238.8 4 6+ 1375.4 5 (5+) 1684.1 5 (6+) 1944.5 5 8+ 2020.8 7 (7+) 2242.6 6 2396.9 7 (8+) 2426.2 7 2759.2 7 10+ 2776.7 12 (9+) 2892.9 11 Continued on next page (footnotes at end of table) 491

110 44 Ru 66 4 NUCLEAR DATA SHEETS 110 44 Ru 66 4 248 Cm, 252 Cf SF Decay (continued) 110 Ru Levels (continued) E(level) Jπ 3646.6 13 12+ 3700.0 13 4351.6 16 14+ 5150.2 19 16+ Based on systematics of low lying collective states in Ru isotopes, γ decay pattern and the observed band structure. J=2 g.s. band. J=1 γ vibrational band built on Jπ=2+ 612 kev level. γ( 110 Ru) Eγ E(level) Iγ Mult. α Comments x 71.70 15 Eγ: from 1971Ho29. Also reported by 1970Wa05. T 1/2 =2.2 ns (1970Wa05). x 96.20 15 0.80 6 Eγ: from 1971Ho29. Also reported by 1970Jo20. T 1/2 =550 ns (1970Jo20). x 131.80 15 0.17 3 Eγ: from 1971Ho29. Also reported by 1970Jo20. T 1/2 =11 ns (1970Jo20). x 150 Reported by 1970Wa05. Tentatively assigned to 111 Ru by 1971Ho29. 196.7 10 860.0 0.41 10 x 222.5 2 0.21 2 T 1/2 =7.2 ns 5 (1974ClZX). Eγ: from 1970Jo20. Other: 1974ClZX. 240.67 11 240.9 100 (E2) 0.0570 K/L 4.0 (1970Wa05). Mult.: from experimental K/L value (to be compared with K/L=7.09 for E2 from 1968Ha53) and γ(θ) results of 1972Wi15. 247.6 5 860.0 6 2 371.6 3 612.6 12.3 20 421.2 10 1084.3 5.4 6 422.3 1 663.2 74 4 Iγ: taken from 1995Lu10, in disagreement with Iγ=54.6 20 from 1994Sh26. 445.6 10 1684.1 0.62 15 471.7 3 1084.3 11.0 14 515.4 3 1375.4 23.0 19 575.6 2 1238.8 41.0 19 599.7 3 1684.1 6.6 10 612.6 3 612.6 10.6 14 619.0 3 860.0 24 2 645.4 5 2020.8 9.0 14 705.0 10 4351.6 1.0 # 5 705.7 3 1944.5 17.2 18 712.5 10 1375.4 3.8 8 712.8 5 2396.9 2.1 5 755.9 10 2776.7 1.9 4 798.6 10 5150.2 0.7 # 4 814.7 5 2759.2 3.6 9 843.5 10 1084.3 1.9 4 867.2 4 2242.6 9 # 3 887.4 10 3646.6 2 # 1 940.8 10 3700.0 2 # 1 948.4 10 2892.9 4 # 2 1021.2 10 1684.1 2 # 1 1187.4 5 2426.2 7 # 2 From 1995Lu10. Unless noted otherwise, weighted average of data from 1995Lu10 and 1994Sh26 if available. From 1970Jo20. # From 1995Lu10, not observed by 1994Sh26. x γ ray not placed in level scheme. 492

110 44 Ru 66 5 NUCLEAR DATA SHEETS 110 44 Ru 66 5 248 Cm, 252 Cf SF Decay (continued) Level Scheme Intensities: relative I(γ+ce) 16+ 5150.2 798.6 0.7 14+ 4351.6 705.0 1.0 940.8 2 887.4 2 3700.0 12+ 3646.6 948.4 4 755.9 1.9 814.7 3.6 (9+) 2776.7 10+ 2759.2 1187.4 7 712.8 2.1 (8+) 2396.9 867.2 9 2892.9 2426.2 2242.6 (7+) 2020.8 645.4 9.0 705.7 17.2 8+ 1944.5 712.5 3.8 515.4 23.0 575.6 41.0 1021.2 2 599.7 6.6 445.6 0.62 (6+) 1684.1 843.5 1.9 471.7 11.0 421.2 5.4 (5+) 1375.4 6+ 1238.8 (4+) 1084.3 422.3 74 612.6 10.6 371.6 12.3 3+ 860.0 619.0 24 247.6 6 196.7 0.41 4+ 663.2 2+ 612.6 2+ 240.9 240.67 (E2) 106 0.30 ns 0+ 0.0 11 4 0 4 Ru 66 493

110 45 Rh 65 1 NUCLEAR DATA SHEETS 110 45 Rh 65 1 Adopted Levels, Gammas Q(β )=5400 220; S(n)=6010 SY; S(p)=9390 230; Q(α)= 5597 SY 1995Au04. Q(β ): Q(β ) is for the decay of the 28.5 s isomer. 110 Rh Levels Cross Reference (XREF) Flags A 110 Ru β Decay (11.6 s) E(level) Jπ XREF T 1/2 Comments x ( 4) A 28.5 s 15 %β =100. No isomeric transition has been observed (1991Jo11). T 1/2 : from γ(t) by 1970Pi01. Other: 34 s 4 (1970Wa28). Jπ: from log ft in β decay (1988Ay02). y 1+ A 3.2 s 2 %β =100. No isomeric transition has been observed (1991Jo11). T 1/2 : weighted average of 3.1 s 2 (β(t), 1970Pi01) and 3.3 s 3 (γ(t), 1978Fr16). Other: 1963Ka21. Jπ: from log ft to 0+ and 2+ states in 110 Rh β decay (3.16 s). 112.19+y 10 1+ A Jπ: from log ft in β decay of 110 Ru. 166.15+y 15 A 200.4+y 5 A 228.26+y 21 A 251.60+y 20 A 667.1+y 3 (1+) A Jπ: from log ft in β decay of 110 Ru. The relative position of the two 110 Rh isomers is unknown. γ( 110 Rh) E(level) Eγ Iγ Mult. α Comments 112.19+y 112.2 1 100 M1 0.250 α(k)exp=0.19 4. α(k)exp: from ce data, α(k)exp=0.22 15 from coincidence data. Mult.: from α(k)exp. 166.15+y 54.0 2 62 12 166.1 2 100 30 200.4+y 88.2 5 100 228.26+y 116.1 2 100 251.60+y 85.4 5 64 22 139.4 2 100 57 667.1+y 415.4 3 100 30 439.0 5 554.8 5 47 18 From 110 Ru β decay. 110 Ru β Decay (11.6 s) 1991Jo11 Source: mass separated source from 238 U(p,F). Measured: Q(β ), Eβ, Eγ, γγ, βγ, ce, T 1/2. Deduced: 110 Rh levels, mult, Jπ. 110 Rh Levels E(level) Jπ T 1/2 E(level) Jπ y 1+ 3.2 s 2 y+112.19 10 1+ y+166.15 15 y+200.4 5 y+228.26 21 y+251.60 20 y+667.1 3 (1+) Based on log ft for allowed transitions. 494

110 45 Rh 65 2 NUCLEAR DATA SHEETS 110 45 Rh 65 2 110 Ru β Decay (11.6 s) 1991Jo11 (continued) β radiations Based on β branching from 110 Ru g.s. to 110 Rh (Jπ=1+) of 70% 10 (1991Jo11). Eβ E(level) Iβ Log ft (2140 y 50) y+667.1 0.59 14 5.95 12 (2560 y 50) y+251.60 0.3 3 6.6 5 (2580 y 50) y+228.26 0.52 9 6.34 9 (2610 y 50) y+200.4 0.32 11 6.57 16 (2640 y 50) y+166.15 1.5 4 5.92 13 (2700 y 50) y+112.19 27 9 4.70 15 2810 50 y 70 10 4.37 8 For β intensity per 100 decays, multiply by 1.0. Estimated by assuming M1 mult for all low energy transitions. γ( 110 Rh) Eγ E(level) Iγ Mult. α Comments 54.0 2 y+166.15 16 3 [M1] 2.015 85.4 5 y+251.60 9 3 [M1] 0.540 88.2 5 y+200.4 9 3 [M1] 0.493 112.2 1 y+112. 19 1000 10 M1 0.250 α(k)exp=0.19 4. α(k)exp: from ce data, α(k)exp=0.22 15 from coincidence data. 116.1 2 y+228.26 18 3 [M1] 0. 2276 139.4 2 y+251.60 14 8 [M1] 0. 1369 166.1 2 y+166.15 26 8 [M1] 0. 0851 415.4 3 y+667.1 17 5 439.0 5 y+667.1 554.8 5 y+667.1 8 3 For absolute intensity per 100 decays, multiply by 0.025 9. Decay Scheme 0+ 0.0 11 4 0 4 Ru 66 11.6 s Intensities: I(γ+ce) per 100 parent decays %β =100 Q =2810 50 Eβ Iβ 0.59 Log ft 5.95 554.8 0.20 439.0 415.4 0.42 (1+) y+667.1 0.3 0.52 0.32 1.5 27 6.6 6.34 6.57 5.92 4.70 116.1 [M1] 0.55 88.2 [M1] 0.34 166.1 [M1] 0.7 54.0 [M1] 1.2 139.4 [M1] 0.4 85.4 [M1] 0.35 112.2 M1 31 y+251.60 y+228.26 y+200.4 y+166.15 1+ y+112.19 2810 70 4.37 1+ y 3.2 s 11 4 0 5 Rh 65 495

110 46 Pd 64 1 NUCLEAR DATA SHEETS 110 46 Pd 64 1 Adopted Levels, Gammas Q(β )= 892 11; S(n)=8818 11; S(p)=10626 5; Q(α)= 4450 14 1995Au04. Adopted B(E2) values are taken from Coul. ex. 110 Pd Levels Cross Reference (XREF) Flags A 110 Rh β Decay (3.2 s) E 110 Pd(α,α') I 110 Pd(p,p'),(d,d'),(pol d,d') B 110 Rh β Decay (28.5 s) F 110 Pd(e,e') J 110 Pd(p,p'γ) C 110 Ag ε Decay (24.6 s) G 110 Pd(π,X) K Coulomb Excitation D 108 Pd(t,p) H 110 Pd(n,n'γ) E(level) Jπ XREF T 1/2 Comments 0.0 0+ ABCDEF HIJK stable 373.80 6 2+ ABCDEF HIJK 46.5 ps 16 T 1/2 : from weighted average of B(E2)=0.82 5 (Coul.ex.) and B(E2)=0.86 4 (e,e'). µ=+0.62 6 (1989Ra17). Q= 0.72 14 (1989Ra17). 813.61 7 2+ AB DE GHIJK 17.7 ps 8 T 1/2 : from Coul. ex. (recoil distance method) (1989SvZZ). 920.77 10 4+ B DEF HIJK 4.09 ps 4 T 1/2 : from Coul. ex. (recoil distance method) (1989SvZZ). B(E4)=9.1 10 3 14 (1991We15). 946.73 # 11 0+ A D HIJK 7.9 ps 7 T 1/2 : from Coul. ex. (recoil distance method) (1989SvZZ). T 1/2 : unweighted average of 10.5 ps 6 (Coul.ex.) and 9.1 ps 6 (recoil distance) (1989SvZZ) data. Jπ: from 110 Pd(pol d,d') and band structure in Coul. ex. 1170.66 @ 11 0+ A D HI JK XREF: D(1175). Jπ: from 110 Pd(pol d,d') and band structure in Coul. ex. 1212.24 11 (3+) B H JK Jπ: γ's to 2+ and 4+ states give Jπ=2+,3,4+. From comparison of exp and calc level population in (n,n'γ), Jπ=3+ is favored. 1214.42 # 16 2+ A D F HIJK 9.1 ps 6 T 1/2 : from Coul. ex. (recoil distance method) (1989SvZZ). Jπ: from 110 Pd(pol d,d') and band structure in Coul. ex. B(E2)=0.0048 5 (1989SvZZ). 1398.24 15 4+ B F HIJK 5.1 ps 6 XREF: J(1401). T 1/2 : from Coul. ex. (recoil distance method) (1989SvZZ). Jπ: from 110 Pd(pol d,d'). B(E4) 1000 (1991We15). 1470.07 @ 10 2+ FGHIJK Jπ: from 110 Pd(pol d,d') and band structure observed in Coul. ex. 1574.04 17 6+ B HIJK 1.40 ps 14 T 1/2 : from Coul. ex. (recoil distance method) (1989SvZZ). Jπ: from level population in (n,n'γ) and band structure observed in Coul. ex. 1584 b 1 I 1641? 10 (0+) G 1719.06 # 15 4+ HIJK 2.2 ps 2 XREF: J(1713). T 1/2 : from Coul. ex. (recoil distance method) (1989SvZZ). Jπ: from 110 Pd(pol d,d') and band structure observed in Coul. ex. 1858 b 2 2+ I 1864 b 1 2+ I 1889.67 21 2+ D HIJK 1900.18 15 2+ B HI γ's to 0+ and 4+. 1934.47 @ 19 4+ DEF HIJK Jπ: from band structure observed in Coul. ex. B(E4)=5.6 10 3 13 (1991We15). 1956 c 2 4+ I 1988 b 1 4+ I 2015 b 2 (4+) I 2037.67 18 3 DEF HI JK XREF: K(2015). 2061 6+ K Jπ: from band structure in Coul. ex. 2089 (4+) K Jπ: from γ decay pattern in Coul. ex. Jπ: in 110 Pd(pol d, d') Jπ=3 for level at this energy but not confirmed by 110 Pd(p,p') and 110 Pd(d,d'). 2095 b 1 I 2125.3 3 1 HI 2140 b 1 2+ D F HI J XREF: D(2135)F(2130). E(level): from 110 Pd(pol d,d'). Jπ: from 110 Pd(pol d,d'). 2141.7 (4+) H K Jπ: from Coul. ex. 2193.0 3 2 HIJ Jπ: from 110 Pd(d,d'),(p,p') (1992Pi08). Continued on next page (footnotes at end of table) 496

110 46 Pd 64 2 NUCLEAR DATA SHEETS 110 46 Pd 64 2 Adopted Levels, Gammas (continued) 110 Pd Levels (continued) E(level) Jπ XREF Comments 2194 b 1 (6+) I 2259 b 1 I 2276.1 3 3 F HI Jπ=3 from (p,p'), (d,d') and (e,e'); Jπ=4+ from (pol d,d'). 2293.3 3 5 DE HI J XREF: D(2283)E(2290)I(2295). 2295 c 2 (4+) I 2296.0 15 8+ K Jπ: from band structure in Coul. ex. 2322.06 25 4+ HIJ 2332 # 1 6+ I K XREF: K(2335). Jπ: from band structure observed in Coul. ex. 2369.7 5 H 2422 c 2 6+ I 2428 b 1 I 2431 7 4+ D Jπ: from (t,p). 2446.54 24 4+ B F HIJ Jπ: from 110 Pd(pol d,d') but in disagreement with Jπ=3 from (e,e'). 2461 10 E 2474.2 4 1 HI Jπ: from 110 Pd(p,p'). In disagreement with Jπ=(3,4+) from 110 Pd(pol d,d'). 2490 b 1 D I Jπ: Jπ=3 from L(t,p)=3 but Jπ=(5 ) from 110 Pd(pol d,d'). 2498.7 4 2+ HI Jπ: from 110 Pd(pol d,d'). E(level): level observed at 2496 in 110 Pd(p,p') and at 2500 in 110 Pd(pol d,d')probably identical with this level. 2512 b 2 4+ I 2517 b 2 2+ D I Jπ: from 108 Pd(t,p). 2536 b 2 2+ I 2548 10 (2+) D Jπ: from 108 Pd(t,p). 2558 b 2 (3 ) I 2563.8 4 3 HI Jπ: from 110 Pd(pol d,d'). 2576 & 2 I J=(4,5,6) for unresolved doublet at 2576 kev in (pol d,d'). 2580 & 2 I 2602 b 2 I J=(1,2,3,4) from 110 Pd(pol d,d'). Might be identical with Jπ=1 level observed at 2608 from 110 Pd(p,p'). 2608 c 3 1 I 2617 b 2 (5 ) I Jπ: from 110 Pd(pol d,d'). 2637 10 (4+) D Jπ: from (t,p). 2644 & 2 (2+) I 2649 & 2 (2+) I 2658 c 3 1 D I Jπ: in disagreement with Jπ=2+ from (t,p). 2672 b 2 4+ I 2686.6 & 4 HI Jπ: Jπ=(2+) for unresolved multiplet in (pol d,d'). 2691 c 3 2+ I Jπ: unresolved multiplet observed in (pol d,d') at 2690 kev. 2695 & 2 D I J=(1,2,3) for unresolved multiplet in (pol d,d') but L(t,p)=4 for 2693 kev level. 2714.6 9 H 2721 b 2 4+ I 2737 & 2 I J=(1,2,3) for unresolved multiplet in (pol d,d'). 2741 c 3 (5 ) D I XREF: D(2744). Jπ: Jπ for unresolved multiplet in 110 Pd(pol d,d') at 2741 kev. 2759 b 2 (3 ) D I Jπ: from 110 Pd(pol d,d'). 2764 c 3 1 D I Jπ: Jπ=(1,2+) for unresolved doublet in 110 Pd(pol d,d'). 2775 8+ K Jπ: from band structure in Coul. ex. 2790.70 21 4+ B I XREF: I(2784). Jπ: Jπ=(5 ) for level at 2786 in 110 Pd(pol d,d'). 2792 b 2 3 I Jπ: from 110 Pd(pol d,d'). 2804.96 20 B I E(level): this level is probably different from the 2805.3 level observed in (n,n'γ), since it has a γ to lower lying 4+ state, while the latter one decays to a 0+ level. Jπ=(2+) for unresolved doublet in (pol d,d') at 2804 kev. 2805.2 3 H See comment on 2804.9 level. 2807 a 2 I Jπ: Jπ=(2+,6+,7 ) from (pol d,d'). 2818 b 2 2+ F I Jπ: from (e,e'). 2827 a 2 (2+,5 ) I 2845 c 3 1 I 2862 b 2 2+ I Jπ: from 110 Pd(pol d,d'). 2871 b 2 2+ I 2889 b 2 (2+) I Jπ: from 110 Pd(pol d,d'). Continued on next page (footnotes at end of table) 497

110 46 Pd 64 3 NUCLEAR DATA SHEETS 110 46 Pd 64 3 Adopted Levels, Gammas (continued) 110 Pd Levels (continued) E(level) Jπ XREF Comments 2893 c 5 3 I 2897 b 2 3 I Jπ: from 110 Pd(pol d,d'). 2903 10 K 2908 b 2 (2+) I Jπ: from 110 Pd(pol d,d'). 2912 c 3 1 I 2932 a 2 (2+) I 2937 a 2 I 2948 b 2 (4+) I Jπ: from 110 Pd(pol d,d'). 2955 2 (2+) I 2972 c 3 4+ I 2994 c 3 3 I E(level): unresolved doublet at 2994 in 110 Pd(pol d,d'). 2998 a 2 I 3002 a 2 I J=(1,2+,5 ) from (pol d,d'). 3009 b 2 E I XREF: E(3015). 3023 c 3 4+ I 3036 c 3 I 3050 b 2 I 3056 b 2 3 I 3062 b 2 I 3075 b 2 (4+) I 3079 b 2 (2+) I 3089 c 3 4+ I Jπ: from 110 Pd(pol d,d'). 3097 b 2 (3 ) I Jπ: from 110 Pd(pol d,d'). 3102 c 2 2+ I E(level): same level as 3106 kev level in 110 Pd(pol d,d'). 3109? # (8+) K Jπ: from band structure observed in Coul. ex. 3110 b 2 (2+,5 ) I Jπ: from 110 Pd(pol d,d'). 3119 c 3 3 I E(level): probably member of unresolved multiplet at 3123 kev in 110 Pd(pol d,d'). 3123 a 2 I Jπ=(2+,3 ) for unresolved multiplet. 3127 a 2 I 3131 10+ K Jπ: from band structure in Coul. ex. 3151 b 2 3 I Jπ: Jπ=(2+,3 ) from 110 Pd(pol d,d'). 3169 b 2 1 I Jπ: Jπ=(3 ) from 110 Pd(pol d,d'). 3181 b 2 (4+) I Jπ: from 110 Pd(pol d,d'). 3192 2 3 I Jπ: Jπ=(2+,3 ) from 110 Pd(pol d,d'). 3232 b 2 (1,2+,3 ) I Jπ: from 110 Pd(pol d,d'). 3240 b 2 (1,2+,3 ) I Jπ: from 110 Pd(pol d,d'). 3259 c 3 3 I E(level): probably member of unresolved doublet Jπ=(3 ) at 3262 in 110 Pd(pol d,d'). 3262 a 2 (3 ) I 3271 b 2 (2+) I Jπ: from 110 Pd(pol d,d'). 3280 c 3 1 I Jπ: doublet observed at 3279 kev in 110 Pd(pol d,d') with Jπ=(1,2+,3 ). 3288 b 2 (2+,6+) I Jπ: from 110 Pd(pol d,d'). 3303 b 3 (4+) I 3320 b 2 (4+) I Jπ: from 110 Pd(pol d,d'). 3333 b 2 ( 4+ ) I E(level): probably identical with level observed at 3339 in 110 Pd(p,p'). 3353 b 2 (2+,4+) I Jπ: from 110 Pd(pol d,d'). 3368 b 2 I 3374 c 3 2+ I Jπ: Jπ=(2+,4+) from 110 Pd(pol d,d'). 3380 b 2 I 3386 b 2 (2+) I Jπ: from 110 Pd(pol d,d'). 3407 c 3 4+ I 3413 b 2 I 3419 b 2 (2+,5 ) I Jπ: from 110 Pd(pol d,d'). 3427 & 2 I 3431 & 2 I 3435 & 2 I 3445 b 2 (2+,5 ) I Jπ: from 110 Pd(pol d,d'). 3455 a 2 I 3458 a 2 I 3471 b 2 I 3484 c 3 3 I 3489 b 2 I 3501 b 2 I 3511 c 3 3 I E(level): assumed identical with 3514 Jπ=(2+) level in 110 Pd(pol d,d'). Continued on next page (footnotes at end of table) 498

110 46 Pd 64 4 NUCLEAR DATA SHEETS 110 46 Pd 64 4 Adopted Levels, Gammas (continued) 110 Pd Levels (continued) E(level) Jπ XREF Comments 3525 b 2 (2+) I Jπ: from 110 Pd(pol d,d'). 3529 c 4 (2+) I 3535 b 2 (3 ) I Jπ: from 110 Pd(pol d,d'). 3543? (10+) K Jπ: from band structure in Coul. ex. 3561 b 2 2+ I Jπ: from 110 Pd(pol d,d'). 3570 b 2 (2,3,4,5,6) I Jπ: from 110 Pd(pol d,d'). 3575 b 2 (4+) I Jπ: from 110 Pd(pol d,d'). 3592 b 2 (1,2+,3 ) I Jπ: from 110 Pd(pol d,d'). 3607 b 2 (1,2+) I 3614 b 2 3 I Jπ: Jπ=(1,2+,3 ) from 110 Pd(pol d,d'). 3622 b 2 I 3642 c 4 4+ I E(level): assumed identical with 3638 level in 110 Pd(pol d,d'). 3653 b 2 (2+) I Jπ: from 110 Pd(pol d,d'). 3669 c 4 4+ I 3679 b 2 (4+) I Jπ: from 110 Pd(pol d,d'). 3687 b 2 I 3694 b 2 (2+,5 ) I Jπ: from 110 Pd(pol d,d'). 3700 c 2 (3 ) I 3720 b 2 I 3730 b 2 I 3738 c 4 (4+) I 3769 c 4 3 I 3789 c 4 3 I 3799 c 4 3 I 3826 c 4 (3 ) I 3854 c 4 (3 ) I 3869 c 4 3 I 3916 c 4 3 I 3955 c 4 (3 ) I 3968? # (10+) K Jπ: from band structure observed in Coul. ex. 4001 c 5 4+ I 4030 12+ K Jπ: from band structure in Coul. ex. 4037 c 5 4+ I 4065 c 5 4+ I 4154 c 5 3 I 4239 c 5 4+ I Unless noted otherwise, from comparison of experimental angular distributions with coupled channel calculations in 110 Pd(d,d'), 110 Pd(p,p'). J=2 g.s. band. J=2 γ band. # J=2 band based on Jπ=0+ 921 kev level. @ J=2 band based on Jπ=0+ 1171 kev level. & Unresolved multiplet in (pol d,d'). a b c Unresolved doublet in (pol d,d'). From 110 Pd(pol d,d') (1993He13). From 110 Pd(d,d') or 110 Pd(p,p') (1992Pi08). γ( 110 Pd) E(level) Eγ Iγ Mult. δ α Comments 373.80 373.80 7 100 [E2] 0. 0145 B(E2)(W.u.)=58 4. 813.61 439.79 7 100 6 E2+M1 4.6 +19 12 δ: from γ(θ) and γγ(θ) in Coul. ex. B(E2)(W.u.)=57 10; B(M1)(W.u.)=0.0006 +6 3. 813.52 10 37 3 [ E2 ] B(E2)(W.u.)=0.82 7. 920.77 107 # 547.04 10 100 B(E2)(W.u.)=99 13. 946.73 133 # 572.89 10 100 [ E2 ] B(E2)(W.u.)=37 7. 1170.66 356.9 2 47.8 22 [E2] 0. 0168 796.83 10 100 7 [E2] Continued on next page (footnotes at end of table) 499

110 46 Pd 64 5 NUCLEAR DATA SHEETS 110 46 Pd 64 5 Adopted Levels, Gammas (continued) γ( 110 Pd) (continued) E(level) Eγ Iγ Comments 1212.24 291.6 2 10.4 8 398.65 15 100 10 Iγ: see remark on the 838.2γ. 838.22 18 58 10 Iγ: in 110 Rh β decay (28.5 s), Iγ(838.2)/Iγ(398.7)=100/74 is given. 1214.42 44 # 267.4 3 24 4 293 # 401.0 7 28 12 840.9 7 63 16 1214.5 2 100 7 Iγ: in 110 Rh β decay (3.2 s), Iγ(840)/Iγ(1214)=100/67 is given. 1398.24 183 # 186 #@ 477.5 3 62 9 Iγ: see comment on the 584.6γ. 584.56 17 100 6 Iγ: in 110 Rh β decay (28.5 s) Iγ(584.6)/Iγ(477.8)=100/50 is given. 1024 # 1470.07 72 # 255 #@ 298.8 3 17 3 523 # 549 # 656.42 15 71 5 1096.29 13 100 7 1470.2 2 31 3 1574.04 176 #@ 653.25 14 100 Eγ: weighted average of 653.4 2 from 110 Rh β decay (28.5 s) and 653.1 2 from (n,n'γ). 1719.06 144 # 248 # 320 # 505 # 797 # 905.2 2 100 7 1345.5 2 28.0 24 1889.67 172 #@ 420 #@ 492 # 719 # 941.5 12 3.4 15 969 #@ 1076.7 8 5.1 16 1515.9 2 100 9 1890 # 1900.18 687.70 17 94 12 729.9 10 41 12 979.2 4 46 10 1526.7 4 100 12 1934.47 218 #@ 362 #@ 463.9 4 100 11 538 #@ 721 #@ 722.5 4 61 8 765 # 1014.0 5 67 17 1120.8 3 61 11 1560.8 4 78 11 1988 1641 16 100 2037.67 1224.2 3 20.0 18 1663.8 2 100 10 2061 125 # 343 #@ 487 #@ 663 # 1140 #@ 2089 371 #@ Continued on next page (footnotes at end of table) 500

110 46 Pd 64 6 NUCLEAR DATA SHEETS 110 46 Pd 64 6 Adopted Levels, Gammas (continued) γ( 110 Pd) (continued) E(level) Eγ Iγ 2089 515 # 619 #@ 691 # 874 # 877 # 1168 # 1275 # 1715 # 2125.3 1751.3 5 15 3 2125.3 3 100 10 2140 2130 20 2141.7 423 # 567 # 743 # 1220 # 1327 # 1767 # 2193.0 1378.8 4 100 16 1819.8 4 59 7 2276.1 1354.9 7 21 5 1462.5 3 100 10 2293.3 1919.5 3 100 2296.0 235 #@ 722 #@ 2322.06 1375.3 3 100 11 E(level) Eγ Iγ 2322.06 1401.2 4 14 3 1948.7 11 6 3 2322.6 10 6.2 19 2332 39 #@ 274 # 617 # 761 # 937 #@ 1414 # 2369.7 1449.5 20 27 13 1556.3 10 79 21 2369.6 6 100 23 2446.54 548 @ 1048.30 19 100 17 1525.8 10 29 15 2474.2 1076. 7 @ 8 34 11 2100.0 6 57 14 2474.4 4 100 14 2498.7 1286.7 4 100 18 1577.3 7 64 18 2563.8 2190.0 4 100 2686.6 1873.2 5 53 16 2312.7 4 100 11 2714.6 1900.2 20 56 26 2341.0 10 100 31 E(level) Eγ Iγ 2775 714 # 1201 #@ 2790.70 890.5 2 100 17 1216.5 5 27 13 1392.1 5 42 8 1579.2 10 50 25 1871.7 10 13 4 2804.96 904.5 2 100 9 1230.9 5 43 22 1406.6 5 26 13 1593.6 5 30 6 1885.1 5 19 54 2805.2 1407.1 10 14 5 1592.9 3 100 12 1859.5 11 17 5 3109? 334 #@ 774 # 813 #@ 1048 #@ 3131 835 # 3543? 412 #@ 1247 #@ 3968? 859 4030 899 1127 #@ Unless noted otherwise, from (n,n'γ) if available. Weighted average of 110 Rh β decay (28.5 s) and 110 Rh β decay (3.2 s). From 110 Rh β decay (28.5 s). # Only observed in Coulomb excitation. For B(E2) values see 1989SvZZ. No γ intensities given. @ Placement of transition in the level scheme is uncertain. 501

110 46 Pd 64 7 NUCLEAR DATA SHEETS 110 46 Pd 64 7 Adopted Levels, Gammas (continued) (A) J=2 g.s. band 12+ 4030 10+ 3131 8+ 2296.0 (B)6+ 6+ 1574.04 (B)4+ 4+ 920.77 (B)2+ 2+ 373.80 0+ 0.0 (B) J=2 γ band (10+) 3543 (A)10+ 8+ 2775 (A)8+ 6+ 2061 (D)4+ (C)4+ (A)6+ 4+ 1398.24 (C)2+ (3+) (A)4+ 2+ 813.61 (A)2+ (A)0+ (C) J=2 band based on Jπ=0+ 921 kev level (10+) 3968 (8+) 3109 (B)8+ 6+ 2332 (A)8+ (B)6+ 4+ 1719.06 (A)6+ (D)2+ (B)4+ 2+ 1214.42 (D)0+ 0+ 946.73 (A)4+ (B)2+ (A)2+ (A)0+ 11 4 0 6 Pd 64 (D) J=2 band based on Jπ=0+ 1171 kev level 4+ 1934.47 (C)4+ (A)6+ 2+ 1470.07 (B)4+ (C)2+ (3+) 0+ 1170.66 (C)0+ (A)4+ (B)2+ (A)2+ (A)0+ 502

110 46 Pd 64 8 NUCLEAR DATA SHEETS 110 46 Pd 64 8 110 Rh β Decay (3.2 s) 1988Ay02 Source: from 238 U(p,F), E(p)=20 MeV. Measured: T 1/2 (β ), Q(β ), Iγ, βce, βγ, γγ. Deduced: 110 Pd levels, Jπ, level systematics. Other: 1972PiZQ. 110 Pd Levels E(level) Jπ 0.0 0+ 373.88 21 2+ 813.63 23 2+ 946.5 4 0+ 1170.6 3 0+ 1214.40 24 2+ From adopted levels. β radiations Based on Iβ =43% 22 for β g.s. transition. Eβ E(level) Iβ Log ft Comments (4190+y 220) 1214.40 <2.6 >6.0 av Eβ=1817 48. (4230+y 220) 1170.6 <8 >5.5 av Eβ=1838 48. (4450+y 220) 946.5 <2 >6.2 av Eβ=1945 48. (4590+y 220) 813.63 <8 >5.7 av Eβ=2008 48. (5030+y 220) 373.88 40 20 5.14 23 av Eβ=2218 48. (5400+y 220) 0.0 43 22 5.25 23 av Eβ=2397 48. For β intensity per 100 decays, multiply by 1. γ( 110 Pd) Eγ E(level) Iγ Mult. α Comments 357.0 3 1170.6 3.1 9 373.8 3 373.88 100 10 (E2) 0. 0145 Mult.: conversion data consistent with mult=e2. 439.7 3 813.63 12 1 572.6 3 946.5 2.8 8 796.7 3 1170.6 9.9 13 813.7 3 813.63 4.3 5 ( E2 ) Mult.: conversion data consistent with mult=e2. 840.5 3 1214.40 2.1 8 1214.4 3 1214.40 1.4 8 ( E2 ) Mult.: conversion data consistent with mult=e2. Recalculated by the evaluators taking into account the decay scheme of 110 Rh (28.5 s) of 1988Ay02. For absolute intensity per 100 decays, multiply by 0.54 27. Decay Scheme 1+ y 3.2 s Intensities: relative Iγ 11 4 0 5 Rh 65 %β =100 Q (g.s.)=5400 220 Iβ Log ft <2.6 >6.0 <8 >5.5 <2 >6.2 <8 >5.7 40 5.14 840.5 2.1 796.7 9.9 357.0 3.1 2+ 1214.40 1214.4 (E2) 1.4 572.6 2.8 813.7 (E2) 4.3 439.7 12 0+ 1170.6 0+ 946.5 2+ 813.63 2+ 373.88 373.8 (E2) 100 43 5.25 0+ 0.0 11 4 0 6 Pd 64 503

110 46 Pd 64 9 NUCLEAR DATA SHEETS 110 46 Pd 64 9 110 Rh β Decay (28.5 s) 1972PiZQ,1988Ay02 Others: 1970Wa28, 1970Pi01. 110 Pd Levels E(level) Jπ E(level) Jπ E(level) Jπ 0.0 0+ 373.82 16 2+ 813.68 16 2+ 920.12 22 4+ 1212.09 19 (3+) 1398.54 23 4+ 1573.6 3 6+ 1900.03 23 2+ 2446.7 5 4+ 2790.6 3 4+ 2804.78 25 From adopted levels. β radiations Eβ E(level) Iβ Log ft Comments 2600 100 2790.6 27.8 24 5.04 9 av Eβ=1071 50. Eβ : from 1970Pi01. 2600 100 2804.78 57 4 4.72 8 av Eβ=1064 50. Eβ : from 1970Pi01. (2950+x 220) 2446.7 9.7 17 5.72 10 av Eβ=1231 50. (4000+x 220) 1398.54 4.8 6.6 av Eβ=1727 50. (4480+x 220) 920.12 8 6.6 av Eβ=1955 50. Calculated from Iγ imbalance at each level. For β intensity per 100 decays, multiply by 1. Existence of this branch is questionable. γ( 110 Pd) Iγ normalization: normalization to absolute Iγ is based on assumption of no β feeding to the 110 Pd g.s. Eγ E(level) Iγ # Mult. α Comments 373.8 3 373.82 100 10 (E2) 0. 0145 Mult.: conversion data consistent with mult=e2. 398.5 2 1212.09 19.9 12 440.0 2 813.68 22.7 24 478.8 5 1398.54 6.0 12 x 531.2 5 2.0 5 546.3 2 920.12 46.6 16 548 @ 2446.7 584.9 2 1398.54 12.0 12 653.4 2 1573.6 11.1 16 687.7 2 1900.03 28.3 16 813.7 2 813.68 8.8 12 ( E2 ) Mult.: conversion data consistent with mult=e2. 838.1 2 1212.09 27 3 890.5 2 2790.6 12.0 20 904.5 2 2804.78 23.1 20 979.6 5 1900.03 4.4 20 Eγ E(level) Iγ # 1048.3 5 2446.7 6.8 20 1086.5 @ 5 1900.03 3.4 10 1525.8 @ 10 2446.7 2 1 1216.5 5 2790.6 3.2 16 1579.2 10 2790.6 6 3 1230.9 5 2804.78 10 5 1593.6 @ 5 2804.78 6.9 15 1392.1 @ 5 2790.6 5.0 10 1871.7 @ 10 2790.6 1.5 5 1406.6 5 2804.78 6 3 1885.1 @ 5 2804.78 4.4 10 From 1988Ay02. From 1972PiZQ, unless noted otherwise. Not observed by 1988Ay02. # For absolute intensity per 100 decays, multiply by 0.91 1. @ Placement of transition in the level scheme is uncertain. x γ ray not placed in level scheme. 504

110 46 Pd 64 10 NUCLEAR DATA SHEETS 110 46 Pd 64 10 110 Rh β Decay (28.5 s) 1972PiZQ,1988Ay02 (continued) Decay Scheme ( 4) x 28.5 s Intensities: relative Iγ 11 4 0 5 Rh 65 %β =100 Q (g.s.)=5400 220 Eβ Iβ Log ft 2600 57 4.72 2600 27.8 5.04 9.7 5.72 4.8 6.6 8 6.6 1406.6 6 1230.9 10 904.5 23.1 1871.7 1.5 1579.2 6 1392.1 5.0 1216.5 3.2 890.5 12.0 1885.1 4.4 1593.6 6.9 1525.8 2 1048.3 6.8 548 4+ 2790.6 4+ 2446.7 478.8 6.0 838.1 27 398.5 19.9 2+ 1900.03 1086.5 3.4 979.6 4.4 687.7 28.3 6+ 1573.6 653.4 11.1 584.9 12.0 4+ 1398.54 (3+) 1212.09 546.3 46.6 813.7 (E2) 8.8 440.0 22.7 4+ 920.12 2+ 813.68 373.8 (E2) 100 2+ 373.82 0+ 0.0 2804.78 11 4 0 6 Pd 64 110 Ag ε Decay (24.6 s) 1965Fr01 Measured: E(K x ray), I(K x ray). Deduced: %ε=0.30 6. See also 110 Ag β decay (24.6 s). 110 Pd Levels E(level) Jπ T 1/2 From adopted levels. 0.0 0+ stable 373.80 7 2+ β +,ε Data Eε E(level) Iε Log ft Comments (518 11) 373.80 0.02 4.8 εk=0.8571; εl=0.1148 4; εm+=0.02809 10. Iε: estimated by evaluators from I(374γ)/I(658γ in 110 Cd), as seen in figure 1 of 1972Ka34. (892 11) 0.0 0.30 6 4.08 9 εk=0.8616; εl=0.1113; εm+=0.02709 3. Iε: from I(K x ray). For intensity per 100 decays, multiply by 1.0. γ( 110 Pd) Eγ E(level) Iγ (374) 373.80 0.02 For absolute intensity per 100 decays, multiply by 1.0. 505

110 46 Pd 64 11 NUCLEAR DATA SHEETS 110 46 Pd 64 11 110 Ag ε Decay (24.6 s) 1965Fr01 (continued) Decay Scheme Intensity: I(γ+ce) per 100 parent decays 1+ 0.0 110 4 7 Ag 63 %ε=0.30 6 Q + =892 11 24.6 s 2+ 373.80 0.02 4.8 374 0.02 Iε Log ft 0+ 0.0 stable 0.30 4.08 11 4 0 6 Pd 64 108 Pd(t,p) 1977An01 E(t)=17 MeV. Measured: σ(θ,e(p)), magnetic spectrograph, FWHM=10 15 kev. DWBA analysis. 110 Pd Levels E(level) L Comments 0.0 0 374 2 814 2 921 4 946 0 1175 0 1215 (2) Close lying doublet is observed in 110 Pd(n,n'γ). 1891 (2) 1935 (4) L: 5 or 6 not excluded. 2038 3 2135 2 2283 5 2431 4 2491 3 2517 2 2548 (2) 2637 (4) 2658 2 2693 4 2744 (5, 6) 2760 Uncertainty 2 kev for lowest levels, increasing to 10 kev for highest levels. Energy adopted for calibration purposes. 506

110 46 Pd 64 12 NUCLEAR DATA SHEETS 110 46 Pd 64 12 110 Pd(e,e') 1991We15: E=70 440 MeV. Measured: form factors for 110 Pd levels. Deduced transition charge densities. 1976Li19: E=40 110 MeV. Measured: σ. Deduced: electron scattering form factors, B(E2) values, Q. 1989Mi10: E=20 63 MeV. Measured: σ(e,θ). θ=117,141,165. Deduced: 110 Pd levels, J, π, B(M1), B(E2), transition form factors. No strong Jπ=1+ excited levels observed. 110 Pd Levels B(E2),B(E4): unless noted otherwise, from 1991We15. E(level) Jπ Comments 0.0 0+ 374 2+ B(E2)=0.86 4. B(E2): weighted average of 0.80 7 (1976Li19) and 0.87 3 (1991We15). 814 2+ B(E2)=0.012 3. B(E2): in agreement with the value of 0.0093 5 from Coulomb excitation measurements by 1989SvZZ. In disagreement with the value 0.0073 8 (1976Li19). 921 4+ E(level): from 1991We15. B(E4)=9.1 10 3 14. 1214 (2)+ 1398 4+ E(level): from 1991We15. B(E4) 1000. 1470 (2)+ 1934 4+ E(level): from 1991We15. B(E4)=5.6 10 3 13. 2038 3 2130 2+ 2276 3 2446 3 2820 2+ From adopted levels. From 1989Mi10, unless noted otherwise. No uncertainties given. The 2446, 2276 levels from authors' spectrum. 110 Pd(π,X) 1979Du06 Reaction: 110 Pd(π,X). Measured: dynamical nuclear polarization. 110 Pd Levels E(level) Jπ 1470.07 10 (2+) 1641? 10 (0+) The interference between nuclear and atomic transitions is discussed in view of the nuclear structure information, from which tentative spin assignments are proposed. From adopted levels. 110 Pd(n,n'γ) 1975Go11 Experiment used reactor fast neutrons. Measured: Eγ, Iγ. 110 Pd Levels E(level) Jπ 0.0 0+ 373.80 7 2+ 813.60 7 2+ 920.82 11 4+ 946.73 11 0+ Continued on next page (footnotes at end of table) 507

110 46 Pd 64 13 NUCLEAR DATA SHEETS 110 46 Pd 64 13 110 Pd(n,n'γ) 1975Go11 (continued) 110 Pd Levels (continued) E(level) Jπ E(level) Jπ E(level) Jπ 1170.66 11 0+ 1212.37 14 (3+) 1214.42 17 (2+) 1398.10 12 (2+,3+,4+) 1470.07 10 (1+,2+) 1573.92 23 (6+) 1719.06 16 (4+) 1889.71 21 (2+) 1900.14 23 1934.50 19 (4+) 2037.67 18 3 2125.3 3 2140.5? 2141.7? 2193.0 3 2276.1 3 2293.3 3 2322.09 25 2369.7 5 2446.41 23 2474.3 3 1 2498.8? 2563.8 4 (3 ) 2686.6 4 2714.6 9 2777.1? 2805.3 3 From adopted levels, unless noted otherwise. From level population and γ deexcitation. γ( 110 Pd) Eγ E(level) Iγ Eγ E(level) Iγ x 208.3 5 0.095 2 x 230.2 5 0.12 2 267.4 3 1214.42 0.61 10 x 275.0 3 0.23 3 291.6 2 1212.37 0.54 4 298.8 3 1470.07 0.22 4 356.9 2 1170.66 0.88 4 373.80 8 373.80 100.0 1 398.8 2 1212.37 5.2 5 401.0 7 1214.42 0.7 3 439.76 8 813.60 23.6 3 463.9 4 1934.50 0.18 2 477.5 3 1398.10 1.02 15 547.04 10 920.82 9.2 5 572.89 10 946.73 5.4 3 584.48 10 1398.10 1.65 10 x 641.0 11 0.040 15 x 648.51 16 0.51 4 653.1 2 1573.92 0.52 5 656.42 15 1470.07 0.93 6 x 672.4 11 0.039 15 687.7 3 1900.14 0.16 2 722.5 4 1934.50 0.110 15 729.9 10 1900.14 0.07 2 x 762.2 4 0.13 2 x 770.3 2 0.61 5 x 773.0 8 0.11 3 796.83 10 1170.66 1.84 12 813.52 10 813.60 4.2 3 838.5 3 1212.37 3.0 5 840.9 7 1214.42 1.6 4 905.2 2 1719.06 0.82 6 929.2 3 2141.7? 0.29 4 941.5 12 1889.71 0.031 14 978.8 5 1900.14 0.078 16 1014.0 5 1934.50 0.12 3 1048.3 2 2446.41 0.54 4 x 1065.5 4 0.10 2 1076.7 8 1889.71 0.047 15 2474.3 0.047 15 1096.29 13 1470.07 1.31 9 1120.8 3 1934.50 0.11 2 x 1150.09 16 0.38 3 1214.5 2 1214.42 2.52 16 1221.0 4 2141.7? 0.26 3 1224.2 3 2037.67 0.22 2 1286.7 4 2498.8? 0.11 2 x 1309.6 8 0.051 15 x 1322.1 7 0.057 15 1345.5 2 1719.06 0.23 2 1354.9 7 2276.1 0.062 15 1375.3 3 2322.09 0.64 7 1378.8 4 2193.0 0.44 7 x 1390.2 8 0.051 13 1401.2 4 2322.09 0.09 2 1407.1 10 2805.3 0.036 13 x 1441.6 7 0.061 15 1449.5 20 2369.7 0.019 9 1462.5 3 2276.1 0.30 3 1470.2 2 1470.07 0.40 4 1515.9 2 1889.71 0.92 8 1526.7 4 1900.14 0.17 2 x 1548.6 3 0.20 2 1556.3 10 2369.7 0.056 15 1560.8 4 1934.50 0.14 2 1577.3 7 2498.8? 0.07 2 1592.9 3 2805.3 0.25 3 x 1614.5 5 0.11 2 x 1626.3 20 0.024 10 x 1655.9 5 0.13 3 1663.8 2 2037.67 1.10 11 x 1671.4 9 0.075 2 x 1677.4 4 0.26 5 x 1681.4 6 0.16 5 1751.3 5 2125.3 0.10 2 1766.7 3 2140.5? 0.57 6 1819.8 4 2193.0 0.26 3 1830.8 11 2777.1? 0.043 15 x 1846.6 6 0.10 2 1859.5 11 2805.3 0.043 12 x 1865.0 7 0.07 2 1873.2 5 2686.6 0.10 3 1900.2 20 2714.6 0.022 10 1919.5 3 2293.3 0.28 5 1948.7 11 2322.09 0.04 2 x 1967.5 8 0.060 2 x 1978.1 13 0.038 13 x 2029.2 8 0.060 15 x 2043.8 8 0.059 15 x 2056.9 8 0.05 2 Continued on next page (footnotes at end of table) 508

110 46 Pd 64 14 NUCLEAR DATA SHEETS 110 46 Pd 64 14 110 Pd(n,n'γ) 1975Go11 (continued) γ( 110 Pd) (continued) Eγ E(level) Iγ Eγ E(level) Iγ x 2066.9 8 0.050 13 x 2092.4 4 0.14 3 2100.0 6 2474.3 0.08 2 x 2117.8 6 0.08 2 2125.3 3 2125.3 0.68 7 x 2161.0 7 0.065 15 x 2174.8 12 0.034 12 2190.0 4 2563.8 0.12 2 x 2205.9 8 0.047 13 x 2228.0 6 0.080 2 x 2237.1 13 0.029 12 x 2244.7 10 0.040 12 x 2260.6 5 0.12 2 2312.7 4 2686.6 0.19 2 2322.6 10 2322.09 0.040 12 2341.0 10 2714.6 0.039 12 x 2363.0 5 0.094 2 2369.6 6 2369.7 0.071 16 2402.8 10 2777.1? 0.038 12 x 2412.0 5 0.085 2 x 2428.8 8 0.056 14 x 2445.4 8 0.050 13 2474.4 4 2474.3 0.14 2 x 2487.1 5 0.096 2 x 2521.5 6 0.069 16 x 2567.3 6 0.071 16 x 2578.2 4 0.11 2 x 2601.5 7 0.059 14 x 2620.5 4 0.11 2 x 2649.6 9 0.045 13 x 2784.8 5 0.090 2 x 2827.8 10 0.041 12 x 2851.5 13 0.029 12 x 2896.1 7 0.072 2 x 2930.4 7 0.071 2 x 2949.2 8 0.055 2 x 2958.5 7 0.084 2 Normalized to Iγ(373.80)=100. Multiply placed; undivided intensity given. Placement of transition in the level scheme is uncertain. x γ ray not placed in level scheme. 509

110 46 Pd 64 15 NUCLEAR DATA SHEETS 110 46 Pd 64 15 110 Pd(n,n'γ) 1975Go11 (continued) Level Scheme & Multiply placed; undivided intensity given Intensities: relative Iγ (3 ) 2563.8 1 2474.3 3 2037.67 (4+) 1934.50 (2+) 1889.71 (4+) 1719.06 (6+) 1573.92 (1+,2+) 1470.07 (2+,3+,4+) 1398.10 (2+) 1214.42 (3+) 1212.37 0+ 1170.66 0+ 946.73 4+ 920.82 2+ 813.60 2805.3 2777.1 2714.6 2686.6 2498.8 2446.41 2369.7 2322.09 2293.3 2276.1 2193.0 2141.7 2140.5 2125.3 1900.14 291.6 0.54 398.8 5.2 838.5 3.0 267.4 0.61 401.0 0.7 840.9 1.6 1214.5 2.52 547.04 9.2 572.89 5.4 439.76 23.6 813.52 4.2 1407.1 0.036 1592.9 0.25 1859.5 0.043 298.8 0.22 656.42 0.93 1096.29 1.31 1470.2 0.40 356.9 0.88 796.83 1.84 1830.8 0.043 2402.8 0.038 1900.2 0.022 2341.0 0.039 477.5 1.02 584.48 1.65 1873.2 0.10 2312.7 0.19 2190.0 0.12 1286.7 0.11 1577.3 0.07 1048.3 0.54 1076.7 & 0.047 2100.0 0.08 2474.4 0.14 1449.5 0.019 1556.3 0.056 2369.6 0.071 1375.3 0.64 1401.2 0.09 1948.7 0.04 2322.6 0.040 1354.9 0.062 1462.5 0.30 1919.5 0.28 1378.8 0.44 1819.8 0.26 1751.3 0.10 2125.3 0.68 1766.7 0.57 929.2 0.29 1221.0 0.26 1224.2 0.22 1663.8 1.10 463.9 0.18 722.5 0.110 1014.0 0.12 1120.8 0.11 1560.8 0.14 941.5 0.031 1076.7 & 0.047 1515.9 0.92 687.7 0.16 729.9 0.07 978.8 0.078 1526.7 0.17 905.2 0.82 1345.5 0.23 653.1 0.52 373.80 100.0 2+ 373.80 0+ 0.0 11 4 0 6 Pd 64 510

110 46 Pd 64 16 NUCLEAR DATA SHEETS 110 46 Pd 64 16 110 Pd(p,p'),(d,d'),(pol d,d') 1992Pi08,1990Pi14,1993He13 1990Pi14,1992Pi08: E(p)=30.7 MeV. E(d)=50.7 MeV. Measured: σ(e(p),θ), σ(e(d),θ). Deduced: 110 Pd levels, J, π. IBM calc. No separate datasets given for (p,p') and (d,d') data. 1990Pi14 assume Jπ=1 for L=1, Jπ=3 for L=3 and Jπ=5 for L=5. 1993He13: pol E(d)=20 MeV. Measured: σ(pol E(d),θ). Deduced: 110 Pd levels, Jπ, IBA calc. Others: 1969Ro30, 1975Ko12. 110 Pd Levels For coupling parameters in coupled channel calc see 1990Pi14. E(level) Jπ # Comments 0.0 0+ 374 2 2+ 813 2 2+ 921 2 4+ 947 2 0+ 1170 2 0+ 1213 1 2+ Jπ: probably 2+ is Jπ value for a 1214 component of a 1214 unresolved doublet observed by 1993He13. 1398 2 4+ 1469 2 2+ 1575 2 0+, 4+, 6+ @ 1584 & 1 1720 1 4+ @ 1858? 2 2+ E(level): only mentioned in an unpublished private communication. 1864 1 2+ @ 1890 1 2+ @ 1899 2 (2+) 1933 2 4+ 1956 2 4+ 1991 2 4+ Jπ: Jπ=(2+,4+) (1993He13). 2038 2 3 2095 & 1 Jπ: J=(1,2,3,4) (1993He13). 2124 2 1 Jπ: J=(1,2,3,4) (1993He13). 2140 1 2+ 2190 2 2+ 2194 1 (6+) @ 2259 & 1 2274 2 3 Jπ: in disagreement with Jπ=4+ (1993He13). 2295 2 (4+) Jπ: J=(2,3,4,5,6) for unresolved doublet at 2293 kev (1993He13). 2295 2 5 Jπ: J=(2,3,4,5,6) for unresolved doublet at 2297 kev (1993He13). 2321 2 4+ 2332 1 6+ 2373 2 2422 2 6+ 2428 2 2446 2 4+ 2473 2 1 Jπ: Jπ=3,4+ (1993He13). 2490 1 (5 ) @ 2496 1 2+ 2511 3 4+ 2517 2 (2+) @ 2535 3 2+ 2563 2 3 @ 2575 2 4+ E(level): probably member of unresolved doublet at 2576 kev (Jπ=4,5,6) observed by 1993He13. Jπ: J=(4,5,6) suggested by 1993He13. 2580 b 2 2602 & 2 Jπ=(1,2,3,4) (1993He13). 2608 3 1 2617 2 (5 ) @ 2644 b 2 (2+) 2649 b 2 (2+) 2658 3 (1 ) 2672 3 4+ 2686 a 2 (2+) 2691 3 2+ E(level): unresolved multiplet at 2690 kev in (pol d,d'). 2695 a 2 Jπ=(1,2,3) suggested from 1993He13. 2718 3 4+ Continued on next page (footnotes at end of table) 511

110 46 Pd 64 17 NUCLEAR DATA SHEETS 110 46 Pd 64 17 110 Pd(p,p'),(d,d'),(pol d,d') 1992Pi08,1990Pi14,1993He13 (continued) 110 Pd Levels (continued) E(level) Jπ # Comments 2737 a 2 (1,2,3) 2741 a 3 (5 ) Jπ for unresolved multiplet at 2741 kev in (pol d,d'). 2744 a 2 2759 2 (3 ) @ 2764 3 1 E(level): Jπ=(1,2+) unresolved doublet at 2765 kev in (pol d,d'). 2784 3 4+ Jπ: Jπ=(5 ) from 1993He13. 2792 2 3 @ 2804 b 2 (2+) 2807 b 2 Jπ: Jπ=(2+,6+,7 ). 2818 2 (2+) @ L: Jπ=2+,4+ (1992Pi08). 2827 b 2 (2+,5 ) 2845 2 1 2862 2 2+ @ 2871 2 2+ @ 2889 2 (2+) @ 2893 3 3 2908 2 (2+) @ 2912 3 1 2932 b 2 (2+) 2937 b 2 2948 2 (4+) @ 2952 3 2+ 2972 3 4+ L: Jπ=(2,3,4) from 1993He13. 2994 3 3 E(level): probably member of unresolved doublet in 110 Pd(pol d,d'). 2998 b 2 3002 b 2 Jπ: Jπ=(1,2+,5 ) from 1993He13. 3009 2 3023 3 4+ 3036 3 3050 & 2 3058 3 3 3062 & 2 3071 3 (4+) 3075 & 2 3079 2 (2+) @ 3089 3 4+ Jπ: Jπ=(2+) (1993He13). 3097 2 (3 ) @ 3102 2 2+ Jπ: Jπ=(2) (1993He13). 3110 2 (2+,5 ) @ 3119 3 3 E(level): may be member of unresolved doublet (Jπ=2+,3 ) observed at 3123 kev in 110 Pd(pol d,d') (1993He13). 3123 b 2 (2+,3 ) 3127 & 2 3152 3 3 Jπ: Jπ=2,3 (1993He13). 3168 3 1 Jπ: Jπ=(3) (1993He13). 3181 2 (4+) @ Jπ: J=0,1,2,4 (1992Pi08). 3191 3 3 Jπ: Jπ=2+,3 (1993He13). 3232 2 (1,2+,3 ) @ 3240 2 (1,2+,3 ) @ 3259 2 3 E(level): very probably a member of the unresolved multiplet at 3262 kev observed in (pol d,d'). Jπ: from 1992Pi08. 3271 2 (2+) @ 3280 3 1 Jπ: Jπ=(1,2+,3 ) (1993He13). 3288 2 (2+,6+) @ 3301 3 (4+) 3320 2 (4+) @ 3333 2 (4+) @ E(level): assumed to be identical with Jπ=(4+) level at 3339 kev observed in 110 Pd(pol d,d'). 3353 2 (2+,4+) @ 3368 & 2 3374 2 2+ Jπ: Jπ=(2+,4+) (1993He13). 3380 & 2 3386 2 (2+) @ 3407 3 4+ Jπ: Jπ=(4+) (1993He13). Continued on next page (footnotes at end of table) 512

110 46 Pd 64 18 NUCLEAR DATA SHEETS 110 46 Pd 64 18 110 Pd(p,p'),(d,d'),(pol d,d') 1992Pi08,1990Pi14,1993He13 (continued) 110 Pd Levels (continued) E(level) Jπ # Comments 3413 & 2 3419 2 (2+,5 ) @ 3427 a 2 3431 a 2 3435 a 2 3445 2 (2+,5 ) @ 3455 b 2 3458 b 2 3471 & 2 3484 3 3 Jπ: Jπ=(3 )(1993He13). 3489 & 2 3501 & 2 3513 2 3 Jπ: Jπ=(2+)(1993He13). 3525 2 (2+) @ 3535 2 (3 ) @ 3561 2 2+ @ 3570 2 (2,3,4,5,6) @ 3575 2 (4+) @ 3592 2 1,2+,3 @ 3607 2 1,2+ @ 3614 3 3 Jπ: Jπ=(1,2+,3 ) (1993He13). 3622 & 2 3638 & 2 3642 4 4+ 3653 2 (2+) @ 3669 4 4+ Jπ: Jπ=(4+) (1993He13). 3679 2 (4+) @ 3687 & 2 3694 2 (2+,5 ) @ 3700 4 (3 ) 3720 & 2 3730 & 2 3738 4 (4+) 3769 4 3 3789 4 3 3799 4 3 3826 4 (3 ) 3854 4 (3 ) 3869 4 3 3916 4 3 3955 4 (3 ) 4001 5 4+ 4037 5 4+ 4065 5 4+ 4154 5 3 4239 5 4+ Unless noted otherwise, from 110 Pd(p,p') and 110 Pd(d,d') (1992Pi08). E estimated by the evaluators based on data from 1993He13 and 1992Pi08. From 110 Pd(pol d,d') (93he123). # From 110 Pd(p,p') and 110 Pd(d,d'), unless noted otherwise. Jπ values obtained from L values, which are not explicitely given but deduced from comparison of experimental data with coupled channel calc by as well 1990Pi14 as 1992Pi08. @ From 110 Pd(pol d,d') (93he123). & From 110 Pd(pol d,d') (93he123) but no Jπ value given. a Unresolved multiplet in 110 Pd(pol d,d') (1993He13). b Unresolved doublet in 110 Pd(pol d,d') with corresponding Jπ value for the doublet if available (1993He13). 513