ADOPTED LEVELS, GAMMAS for 227Ac
Author: Ictp-2014 Workshop Group | Citation: Nucl. Data Sheets 132, 257 (2016) | Cutoff date: 15-Jan-2016
Authors: B. Singh, I. Ami, A. Chakraborty, M. Latif, S. Rathi and D. Yang | Citation: ENSDF | Cutoff date: 15-JAN-2016
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=44.8 keV 8 | S(n)= 6531 keV 3 | S(p)= 5107.5 keV 23 | Q(α)= 5042.19 keV 14 | ||
Reference: 2012WA38 |
References: | |||
A | 227Ra β- decay (42.2 M) | B | 231Pa α decay (3.276×104 Y) |
C | 226Ra(3He,d) | D | 226Ra(α,t) |
E | 230Th(p,α) |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
0.0 | ABCD | 3/2- | 21.772 y 3 % β- = 98.6200 36 % α = 1.3800 36 | |||||
27.369 11 | ABCDE | 3/2+ | 38.3 ns 3 | 27.36 2 | 100 | E1(+M2) | 0.0 | 3/2- |
29.978 11 | ABCDE | 5/2- | 29.97 2 | 100 | M1+E2 | 0.0 | 3/2- | |
46.354 13 | ABCD | 5/2+ | 16.5 1 19.6 46.35 2 | 119 5 186 53 100 5 | [E1] [M1] (E1) | 29.978 27.369 0.0 | 5/2- 3/2+ 3/2- | |
74.149 17 | ABCD | 7/2- | 44.14 2 74.15 4 | 100 8 40.2 15 | [M1] [E2] | 29.978 0.0 | 5/2- 3/2- | |
84.544 14 | ABCD | 7/2+ | 38.20 2 54.60 2 57.19 3 | 100 3 48 3 22.6 15 | M1+E2 [E1] (E2) | 46.354 29.978 27.369 | 5/2+ 5/2- 3/2+ | |
109.992 21 | BCDE | 9/2+ | 25.48 6 35.83 3 63.64 3 | 100 11 13.6 8 37.5 13 | [M1] [E1] E2 | 84.544 74.149 46.354 | 7/2+ 7/2- 5/2+ | |
126.848 22 | BCDE | 9/2- | 52.71 3 96.84 3 | 92 5 100.0 25 | [M1] E2 | 74.149 29.978 | 7/2- 5/2- | |
148 5 | D | |||||||
160 2 | BC | |||||||
187.34 3 | BCD | 11/2+ | 60.50 3 77.34 3 102.6 5 | 9.2 12 100 3 <23 | [E1] [M1] [E2] | 126.848 109.992 84.544 | 9/2- 9/2+ 7/2+ | |
198.69 6 | BCD | 11/2- | 71.9 1 124.58 8 | 46 15 100 9 | [M1] [E2] | 126.848 74.149 | 9/2- 7/2- | |
210.84 7 | BCDE | 13/2+ | 23.6S 100.85 6 | 20 4 100 4 | [M1] [E2] | 187.34 109.992 | 11/2+ 9/2+ | |
227 2 | CD | |||||||
249 2 | CD | |||||||
271.32 7 | BCDE | (13/2-) | 72.67 6 144.40 8 161.0 10 ? | 26 6 100 9 | [M1] [E2] [M2] | 198.69 126.848 109.992 | 11/2- 9/2- 9/2+ | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
273.19 4 | ABCDE | (5/2)- | 198.89 10 226.6 1 ? 243.11 9 246.04 9 273.15 6 | 7.3 7 3.1 58 4 20 6 100.0 14 | [M1+E2] [E1] M1+E2 [E1] M1+E2 | 74.149 46.354 29.978 27.369 0.0 | 7/2- 5/2+ 5/2- 3/2+ 3/2- | |
304.73 6 | ABCD | (5/2+) | 219.90 15 230.0 10 258.37 10 277.39 10 | 10.5 70 35 100 18 145 | [M1+E2] [E1] [M1+E2] [M1+E2] | 84.544 74.149 46.354 27.369 | 7/2+ 7/2- 5/2+ 3/2+ | |
317 2 | CD | (7/2-) | ||||||
330.040 10 | ABCDE | 3/2- | < 70 ps | 57.19 3 ? 245.60 13 255.78 7 283.682 16 300.066 10 302.667 9 330.055 15 | 0.71 0.407 32 6.42 6 100 146.1 18 138 20 82.3 10 | [M1+E2] [M2] E2 E1 M1+E2 E1 M1+E2 | 273.19 84.544 74.149 46.354 29.978 27.369 0.0 | (5/2)- 7/2+ 7/2- 5/2+ 5/2- 3/2+ 3/2- |
342 5 | D | (7/2+) | ||||||
354.50 4 | AB DE | 1/2- | 24.5 1 327.14 7 354.48 5 | ≈5.1 37.4 7 100.0 14 | [M1] (E1) M1+E2 | 330.040 27.369 0.0 | 3/2- 3/2+ 3/2- | |
372 2 | CDE | (9/2-) | ||||||
387.202 15 | BCDE | 7/2- | 57.19 3 260.19 8 277.22 7 302.667 9 312.92 5 340.71 6 357.11 8 387.0 1 | 1.54 27 100.0 12 37.4 5 96 24 55.3 6 97.4 12 92.3 11 0.16 5 | E2 M1+E2 (E1+M2) E1 M1+E2 E1+M2 M1(+E2) [E2] | 330.040 126.848 109.992 84.544 74.149 46.354 29.978 0.0 | 3/2- 9/2- 9/2+ 7/2+ 7/2- 5/2+ 5/2- 3/2- | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
403 5 | CD | (9/2+) | ||||||
425.59 5 | ABC | 5/2+ | 341.1 1 ? 351.5 1 379.35 7 395.45 10 398.14 8 | 47 7.6 23 100.0 17 4.7 3 19.0 5 | [M1+E2] [E1] M1(+E2) [E1] [M1+E2] | 84.544 74.149 46.354 29.978 27.369 | 7/2+ 7/2- 5/2+ 5/2- 3/2+ | |
428.4 2 ? | A | 398.4 4 ? 428.4 2 ? | 97 100 | 29.978 0.0 | 5/2- 3/2- | |||
435.19 4 | ABCDE | 1/2+ | 390.4 6 ? 407.82 4 435.2 1 | 3.3 100.0 14 8.2 5 | M1 | 46.354 27.369 0.0 | 5/2+ 3/2+ 3/2- | |
437.94 5 | BCDE | (5/2-) | 50.83 15 363.84 10 391.61 9 410.30 12 438.01 9 | 25 4 100 3 84.5 25 23 3 57 3 | [M1] [M1+E2] [E1] [E1] [M1+E2] | 387.202 74.149 46.354 27.369 0.0 | 7/2- 7/2- 5/2+ 3/2+ 3/2- | |
469.27 9 | BCD | 9/2+ | 359.33 15 384.7 1 | 100 3 43.2 23 | [M1+E2] [M1+E2] | 109.992 84.544 | 9/2+ 7/2+ | |
501.29 8 | ABCDE | (3/2-,5/2-) | 146.9 5 ? 228.00 10 427.0 1 ? 471.3 5 501.4 1 | <29 40 26 100 | 354.50 273.19 74.149 29.978 0.0 | 1/2- (5/2)- 7/2- 5/2- 3/2- | ||
514.36 9 | A CDE | (3/2,5/2)+ | 209.6 2 468.5 5 486.98 10 | 4.4 10.8 100 | 304.73 46.354 27.369 | (5/2+) 5/2+ 3/2+ | ||
527 3 | CDE | (13/2+) | ||||||
537.02 10 | ABC E | (3/2+) | 232.20 10 490.7 5 510.0 2 | 100 50 117 50 | [M1+E2] | 304.73 46.354 27.369 | (5/2+) 5/2+ 3/2+ | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
549 3 | D | |||||||
562.78 14 | ABCDE | (3/2+,5/2) | 478.4 4 486.827 23 ? 516.2 2 535.6 2 | 8.6 113 11 100 11 45 5 | 84.544 74.149 46.354 27.369 | 7/2+ 7/2- 5/2+ 3/2+ | ||
577 | DE | (9/2-) | ||||||
592 2 | CDE | (13/2)+ | ||||||
639.09 15 | A CDE | 1/2+ | 611.4 2 639.4 2 | 100 18 | 27.369 0.0 | 3/2+ 3/2- | ||
656.4 4 | BCD | (7/2+) | 546.5 5 571.6 8 583 2 609 2 | 11.6 19 7 3 60.5 23 100 5 | 109.992 84.544 74.149 46.354 | 9/2+ 7/2+ 7/2- 5/2+ | ||
669 3 | E | |||||||
698.56 15 | A CDE | (3/2)+ | 652.2 2 671.2 2 | 100 67 | 46.354 27.369 | 5/2+ 3/2+ | ||
725 4 | E | |||||||
790.13 17 | A CDE | (1/2-,3/2,5/2) | 760.3 2 789.8 3 | 81 100 | 29.978 0.0 | 5/2- 3/2- | ||
816 4 | E | |||||||
863.64 22 | A CDE | (1/2,3/2,5/2) | 836.4 3 863.5 3 | 63 100 | 27.369 0.0 | 3/2+ 3/2- | ||
874.68 18 | A CDE | (1/2+,3/2,5/2) | 828.9 3 846.7 3 874.7 3 | 33 <67 100 20 | 46.354 27.369 0.0 | 5/2+ 3/2+ 3/2- | ||
895 2 | E | (3/2)+ | ||||||
920 2 | E | |||||||
950 4 | E | |||||||
992 3 | E | |||||||
1070 3 | CDE | |||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
1091 2 | CD | |||||||
1117 2 | E | |||||||
1148 2 | E | |||||||
1183 3 | E | |||||||
1215 3 | E | |||||||
1274 4 | E | |||||||
1311 2 | E | |||||||
1385 2 | E | |||||||
1438 2 | E | |||||||
1483 2 | E | |||||||
1550 2 | E | |||||||
1591 2 | E | |||||||
1629 4 | E |
E(level): From least-squares fit to adopted γ-ray energies, unless otherwise specified.
Jπ(level): Spin and parity assignments are based on rotational structure, γ-ray multipolarities and decay patterns, αγ(θ) data from 1971Le10, and comparison of experimental and theoretical cross sections (and spectroscopic factors) in 226Ra(α,t) reaction for band members based on Nilsson model configurations ( "finger-print " method). Nilsson orbital assignments are based on their energy systematics in neighboring odd-Z nuclei, favored α decay transitions from 231Pa parent with ground-state Jπ=3/2- and configuration of π1/2[530], and also on comparison of experimental and theoretical relative α-particle branches (1965PoZZ). Other specific arguments, based on γ transitions, are given with individual levels.
E(γ): Weighted average from 231Pa α decay and 227Ra β- decay.
I(γ): Best value from 231Pa α decay and 227Ra β- decay.
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 1 - π3/2[532] parity doublet band. | |||||||
0.0 | 3/2- | 21.772 y 3 % β- = 98.6200 36 % α = 1.3800 36 | |||||
29.978 11 | 5/2- | 29.97 2 | 100 | M1+E2 | 0.0 | 3/2- | |
74.149 17 | 7/2- | 44.14 2 74.15 4 | 100 8 40.2 15 | [M1] [E2] | 29.978 0.0 | 5/2- 3/2- | |
126.848 22 | 9/2- | 52.71 3 96.84 3 | 92 5 100.0 25 | [M1] E2 | 74.149 29.978 | 7/2- 5/2- | |
198.69 6 | 11/2- | 71.9 1 124.58 8 | 46 15 100 9 | [M1] [E2] | 126.848 74.149 | 9/2- 7/2- | |
271.32 7 | (13/2-) | 72.67 6 144.40 8 161.0 10 ? | 26 6 100 9 | [M1] [E2] [M2] | 198.69 126.848 109.992 | 11/2- 9/2- 9/2+ | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 2 - π3/2[651] parity doublet band. | |||||||
27.369 11 | 3/2+ | 38.3 ns 3 | |||||
46.354 13 | 5/2+ | 16.5 1 19.6 46.35 2 | 119 5 186 53 100 5 | [E1] [M1] (E1) | 29.978 27.369 0.0 | 5/2- 3/2+ 3/2- | |
84.544 14 | 7/2+ | 38.20 2 54.60 2 57.19 3 | 100 3 48 3 22.6 15 | M1+E2 [E1] (E2) | 46.354 29.978 27.369 | 5/2+ 5/2- 3/2+ | |
109.992 21 | 9/2+ | 25.48 6 35.83 3 63.64 3 | 100 11 13.6 8 37.5 13 | [M1] [E1] E2 | 84.544 74.149 46.354 | 7/2+ 7/2- 5/2+ | |
187.34 3 | 11/2+ | 60.50 3 77.34 3 102.6 5 | 9.2 12 100 3 <23 | [E1] [M1] [E2] | 126.848 109.992 84.544 | 9/2- 9/2+ 7/2+ | |
210.84 7 | 13/2+ | 23.6S 100.85 6 | 20 4 100 4 | [M1] [E2] | 187.34 109.992 | 11/2+ 9/2+ | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 3 - π5/2[523] parity doublet band. | |||||||
273.19 4 | (5/2)- | ||||||
317 2 | (7/2-) | ||||||
372 2 | (9/2-) | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 4 - π5/2[642] parity doublet band. | |||||||
304.73 6 | (5/2+) | ||||||
342 5 | (7/2+) | ||||||
403 5 | (9/2+) | ||||||
527 3 | (13/2+) | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 5 - π1/2[530] parity doublet band. | |||||||
330.040 10 | 3/2- | < 70 ps | |||||
354.50 4 | 1/2- | 24.5 1 327.14 7 354.48 5 | ≈5.1 37.4 7 100.0 14 | [M1] (E1) M1+E2 | 330.040 27.369 0.0 | 3/2- 3/2+ 3/2- | |
387.202 15 | 7/2- | 57.19 3 260.19 8 277.22 7 302.667 9 312.92 5 340.71 6 357.11 8 387.0 1 | 1.54 27 100.0 12 37.4 5 96 24 55.3 6 97.4 12 92.3 11 0.16 5 | E2 M1+E2 (E1+M2) E1 M1+E2 E1+M2 M1(+E2) [E2] | 330.040 126.848 109.992 84.544 74.149 46.354 29.978 0.0 | 3/2- 9/2- 9/2+ 7/2+ 7/2- 5/2+ 5/2- 3/2- | |
437.94 5 | (5/2-) | 50.83 15 363.84 10 391.61 9 410.30 12 438.01 9 | 25 4 100 3 84.5 25 23 3 57 3 | [M1] [M1+E2] [E1] [E1] [M1+E2] | 387.202 74.149 46.354 27.369 0.0 | 7/2- 7/2- 5/2+ 3/2+ 3/2- | |
577 | (9/2-) | ||||||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 6 - π1/2[660] parity doublet band. | |||||||
425.59 5 | 5/2+ | ||||||
435.19 4 | 1/2+ | 390.4 6 ? 407.82 4 435.2 1 | 3.3 100.0 14 8.2 5 | M1 | 46.354 27.369 0.0 | 5/2+ 3/2+ 3/2- | |
469.27 9 | 9/2+ | 359.33 15 384.7 1 | 100 3 43.2 23 | [M1+E2] [M1+E2] | 109.992 84.544 | 9/2+ 7/2+ | |
514.36 9 | (3/2,5/2)+ | 209.6 2 468.5 5 486.98 10 | 4.4 10.8 100 | 304.73 46.354 27.369 | (5/2+) 5/2+ 3/2+ | ||
592 2 | (13/2)+ | ||||||
656.4 4 | (7/2+) | 546.5 5 571.6 8 583 2 609 2 | 11.6 19 7 3 60.5 23 100 5 | 109.992 84.544 74.149 46.354 | 9/2+ 7/2+ 7/2- 5/2+ | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 7 - π1/2[400] band | |||||||
639.09 15 | 1/2+ | ||||||
698.56 15 | (3/2)+ | 652.2 2 671.2 2 | 100 67 | 46.354 27.369 | 5/2+ 3/2+ |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
27.369 | 3/2+ | 38.3 ns 3 | 27.36 2 | E1(+M2) | 0.0020 LT | 4.5 | B(E1)(W.u.)>3.9E-5, α=4.5 4 |
29.978 | 5/2- | 29.97 2 | M1+E2 | 0.22 3 | 2.7×102 | α=2.7×102 5, α(L)=2.0E2 4, α(M)=52 9, α(N)=13.8 23, α(O)=3.1 5, α(P)=0.52 8, α(Q)=0.0213 4 | |
46.354 | 5/2+ | 16.5 1 | [E1] | 8.58 | α=8.58 12 | ||
5/2+ | 19.6 | [M1] | 112.8 | α=112.8, α(L)=2.34 4, α(M)=82.5 12, α(N)=21.9 3, α(O)=5.09 8, α(P)=0.942 14, α(Q)=0.0840 12 | |||
5/2+ | 46.35 2 | (E1) | 0.879 | α=0.879, α(L)=0.663 10, α(M)=0.1634 23, α(N)=0.0423 6, α(O)=0.00913 13, α(P)=0.001417 20, α(Q)=5.89×10-5 9 | |||
74.149 | 7/2- | 44.14 2 | [M1] | 37.4 | α=37.4, α(L)=28.3 4, α(M)=6.80 10, α(N)=1.80 3, α(O)=0.420 6, α(P)=0.0777 11, α(Q)=0.00691 10 | ||
7/2- | 74.15 4 | [E2] | 42.5 | α=42.5, α(L)=31.2 5, α(M)=8.52 13, α(N)=2.27 4, α(O)=0.493 7, α(P)=0.0768 11, α(Q)=0.000234 4 | |||
84.544 | 7/2+ | 38.20 2 | M1+E2 | 0.19 9 | 92 | α=92 38, α(L)=69 28, α(M)=17.4 76, α(N)=4.6 20, α(O)=1.04 44, α(P)=0.180 67, α(Q)=0.0104 3 | |
7/2+ | 54.60 2 | [E1] | 0.569 | α=0.569, α(L)=0.429 6, α(M)=0.1052 15, α(N)=0.0273 4, α(O)=0.00594 9, α(P)=0.000940 14, α(Q)=4.17×10-5 6 | |||
7/2+ | 57.19 3 | (E2) | 148.0 | α=148.0, α(L)=108.5 16, α(M)=29.6 5, α(N)=7.87 12, α(O)=1.709 25, α(P)=0.266 4, α(Q)=0.000688 10 | |||
109.992 | 9/2+ | 25.48 6 | [M1] | 189 | α=189, α(L)=143.1 23, α(M)=34.5 6, α(N)=9.16 15, α(O)=2.13 4, α(P)=0.394 7, α(Q)=0.0351 6 | ||
9/2+ | 35.83 3 | [E1] | 1.742 | α=1.742, α(L)=1.310 19, α(M)=0.327 5, α(N)=0.0843 12, α(O)=0.0179 3, α(P)=0.00268 4, α(Q)=0.0001001 15 | |||
9/2+ | 63.64 3 | E2 | 88.4 | α=88.4, α(L)=64.8 10, α(M)=17.7 3, α(N)=4.70 7, α(O)=1.023 15, α(P)=0.1592 23, α(Q)=0.000437 7 | |||
126.848 | 9/2- | 52.71 3 | [M1] | 22.2 | α=22.2, α(L)=16.82 24, α(M)=4.04 6, α(N)=1.071 16, α(O)=0.249 4, α(P)=0.0461 7, α(Q)=0.00410 6 | ||
9/2- | 96.84 3 | E2 | 12.04 | α=12.04, α(L)=8.83 13, α(M)=2.41 4, α(N)=0.642 9, α(O)=0.1399 20, α(P)=0.0219 3, α(Q)=8.55×10-5 12 | |||
187.34 | 11/2+ | 60.50 3 | [E1] | 0.433 | α=0.433, α(L)=0.327 5, α(M)=0.0798 12, α(N)=0.0208 3, α(O)=0.00454 7, α(P)=0.000726 11, α(Q)=3.35×10-5 5 | ||
11/2+ | 77.34 3 | [M1] | 7.24 | α=7.24, α(L)=5.48 8, α(M)=1.315 19, α(N)=0.349 5, α(O)=0.0811 12, α(P)=0.01501 21, α(Q)=0.001334 19 | |||
11/2+ | 102.6 5 | [E2] | 9.20 | α=9.20 25, α(L)=6.74 19, α(M)=1.84 5, α(N)=0.490 14, α(O)=0.107 3, α(P)=0.0167 5, α(Q)=6.99×10-5 16 | |||
198.69 | 11/2- | 71.9 1 | [M1] | 8.96 | α=8.96, α(L)=6.78 10, α(M)=1.626 24, α(N)=0.432 7, α(O)=0.1004 15, α(P)=0.0186 3, α(Q)=0.001650 24 | ||
11/2- | 124.58 8 | [E2] | 4.04 | α=4.04, α(K)=0.285 4, α(L)=2.75 4, α(M)=0.752 11, α(N)=0.200 3, α(O)=0.0436 7, α(P)=0.00686 10, α(Q)=3.71×10-5 6 | |||
210.84 | 13/2+ | 23.6 | [M1] | 237 | α=237, α(L)=179 3, α(M)=43.3 6, α(N)=11.50 16, α(O)=2.67 4, α(P)=0.495 7, α(Q)=0.0441 7 | ||
13/2+ | 100.85 6 | [E2] | 9.96 | α=9.96, α(L)=7.30 11, α(M)=2.00 3, α(N)=0.531 8, α(O)=0.1157 17, α(P)=0.0181 3, α(Q)=7.42×10-5 11 | |||
271.32 | (13/2-) | 72.67 6 | [M1] | 8.68 | α=8.68, α(L)=6.57 10, α(M)=1.577 23, α(N)=0.418 6, α(O)=0.0973 14, α(P)=0.0180 3, α(Q)=0.001599 23 | ||
(13/2-) | 144.40 8 | [E2] | 2.18 | α=2.18, α(K)=0.263 4, α(L)=1.408 20, α(M)=0.384 6, α(N)=0.1023 15, α(O)=0.0223 4, α(P)=0.00353 5, α(Q)=2.38×10-5 4 | |||
(13/2-) | 161.0 10 | [M2] | 22.8 | α=22.8 6, α(K)=15.0 4, α(L)=5.75 17, α(M)=1.51 5, α(N)=0.408 12, α(O)=0.094 3, α(P)=0.0170 5, α(Q)=0.00133 4 | |||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
273.19 | (5/2)- | 198.89 10 | [M1+E2] | 1.53 | α=1.53 90, α(K)=1.05 90, α(L)=0.355 11, α(M)=0.091 4, α(N)=0.0241 10, α(O)=0.00543 10, α(P)=0.00093 7, α(Q)=4.9×10-5 39 | ||
(5/2)- | 226.6 1 | [E1] | 0.0688 | α=0.0688, α(K)=0.0548 8, α(L)=0.01057 15, α(M)=0.00253 4, α(N)=0.000666 10, α(O)=0.0001511 22, α(P)=2.65×10-5 4, α(Q)=1.81E-6 3 | |||
(5/2)- | 243.11 9 | M1+E2 | 1.1 3 | 0.80 | α=0.80 17, α(K)=0.56 16, α(L)=0.176 10, α(M)=0.0445 16, α(N)=0.0118 5, α(O)=0.00268 12, α(P)=0.00046 3, α(Q)=2.60×10-5 70 | ||
(5/2)- | 246.04 9 | [E1] | 0.0568 | α=0.0568, α(K)=0.0454 7, α(L)=0.00864 13, α(M)=0.00207 3, α(N)=0.000544 8, α(O)=0.0001237 18, α(P)=2.18×10-5 3, α(Q)=1.515E-6 22 | |||
(5/2)- | 273.15 6 | M1+E2 | 0.7 3 | 0.74 | α=0.74 15, α(K)=0.57 14, α(L)=0.131 11, α(M)=0.0323 21, α(N)=0.0086 6, α(O)=0.00197 15, α(P)=0.00035 4, α(Q)=2.6×10-5 6 | ||
304.73 | (5/2+) | 219.90 15 | [M1+E2] | 1.14 | α=1.14 70, α(K)=0.80 67, α(L)=0.250 25, α(M)=0.0635 25, α(N)=0.0169 7, α(O)=0.00382 25, α(P)=0.00066 9, α(Q)=3.7×10-5 30 | ||
(5/2+) | 230.0 10 | [E1] | 0.0664 | α=0.0664 12, α(K)=0.0530 10, α(L)=0.01019 18, α(M)=0.00244 5, α(N)=0.000642 12, α(O)=0.000146 3, α(P)=2.56×10-5 5, α(Q)=1.75E-6 3 | |||
(5/2+) | 258.37 10 | [M1+E2] | 0.71 | α=0.71 46, α(K)=0.52 42, α(L)=0.15 3, α(M)=0.037 6, α(N)=0.0097 14, α(O)=0.0022 4, α(P)=0.00039 9, α(Q)=2.4×10-5 19 | |||
(5/2+) | 277.39 10 | [M1+E2] | 0.58 | α=0.58 38, α(K)=0.43 35, α(L)=0.12 3, α(M)=0.029 6, α(N)=0.0077 15, α(O)=0.0018 4, α(P)=3.09×10-4 84, α(Q)=2.0E-5 16 | |||
330.040 | 3/2- | < 70 ps | 57.19 3 | [M1+E2] | 83 | α=83 66, α(L)=61 48, α(M)=16 14, α(N)=4.4 36, α(O)=0.95 76, α(P)=0.15 12, α(Q)=0.0020 13 | |
3/2- | < 70 ps | 245.60 13 | [M2] | 5.23 | α=5.23, α(K)=3.70 6, α(L)=1.141 17, α(M)=0.293 5, α(N)=0.0787 12, α(O)=0.0182 3, α(P)=0.00331 5, α(Q)=0.000268 4 | ||
3/2- | < 70 ps | 255.78 7 | E2 | 0.265 | α=0.265, α(K)=0.0993 14, α(L)=0.1218 18, α(M)=0.0328 5, α(N)=0.00872 13, α(O)=0.00192 3, α(P)=0.000310 5, α(Q)=5.37×10-6 8 | ||
3/2- | < 70 ps | 283.682 16 | E1 | 0.0410 | α=0.0410, α(K)=0.0329 5, α(L)=0.00614 9, α(M)=0.001468 21, α(N)=0.000386 6, α(O)=8.81×10-5 13, α(P)=1.561E-5 22, α(Q)=1.117E-6 16 | ||
3/2- | < 70 ps | 300.066 10 | M1+E2 | -0.12 7 | 0.764 | α=0.764 17, α(K)=0.613 15, α(L)=0.1146 20, α(M)=0.0275 5, α(N)=0.00728 12, α(O)=0.00169 3, α(P)=0.000313 6, α(Q)=2.75×10-5 7 | |
3/2- | < 70 ps | 302.667 9 | E1 | 0.0355 | α=0.0355, α(K)=0.0285 4, α(L)=0.00527 8, α(M)=0.001260 18, α(N)=0.000331 5, α(O)=7.56×10-5 11, α(P)=1.344E-5 19, α(Q)=9.74E-7 14 | ||
3/2- | < 70 ps | 330.055 15 | M1+E2 | +0.36 7 | 0.540 | α=0.540 21, α(K)=0.430 19, α(L)=0.0836 22, α(M)=0.0202 5, α(N)=0.00535 13, α(O)=0.00124 3, α(P)=0.000228 6, α(Q)=1.93×10-5 8 | |
354.50 | 1/2- | 24.5 1 | [M1] | 213 | α=213 4, α(L)=161 3, α(M)=38.8 8, α(N)=10.29 20, α(O)=2.39 5, α(P)=0.443 9, α(Q)=0.0395 8 | ||
1/2- | 327.14 7 | (E1) | 0.0298 | α=0.0298, α(K)=0.0240 4, α(L)=0.00440 7, α(M)=0.001050 15, α(N)=0.000276 4, α(O)=6.32×10-5 9, α(P)=1.125E-5 16, α(Q)=8.28E-7 12 | |||
1/2- | 354.48 5 | M1+E2 | +2.8 +14-6 | 0.143 | α=0.143 24, α(K)=0.090 21, α(L)=0.0391 24, α(M)=0.0101 5, α(N)=0.00269 14, α(O)=0.00060 4, α(P)=0.000102 7, α(Q)=4.2×10-6 9 | ||
387.202 | 7/2- | 57.19 3 | E2 | 148.0 | α=148.0, α(L)=108.5 16, α(M)=29.6 5, α(N)=7.87 12, α(O)=1.709 25, α(P)=0.266 4, α(Q)=0.000688 10 | ||
7/2- | 260.19 8 | M1+E2 | 1.5 3 | 0.53 | α=0.53 10, α(K)=0.35 9, α(L)=0.131 7, α(M)=0.0338 12, α(N)=0.0090 3, α(O)=0.00202 8, α(P)=0.000345 19, α(Q)=1.6×10-5 4 | ||
7/2- | 277.22 7 | (E1+M2) | 0.40 5 | 0.52 | α=0.52 11, α(K)=0.37 8, α(L)=0.107 23, α(M)=0.027 6, α(N)=0.0073 16, α(O)=0.0017 4, α(P)=0.00031 7, α(Q)=2.5×10-5 6 | ||
7/2- | 302.667 9 | E1 | 0.0355 | α=0.0355, α(K)=0.0285 4, α(L)=0.00527 8, α(M)=0.001260 18, α(N)=0.000331 5, α(O)=7.56×10-5 11, α(P)=1.344E-5 19, α(Q)=9.74E-7 14 | |||
7/2- | 312.92 5 | M1+E2 | 1.5 +9-5 | 0.31 | α=0.31 11, α(K)=0.216 94, α(L)=0.070 10, α(M)=0.0178 19, α(N)=0.0047 5, α(O)=0.00107 13, α(P)=0.00018 3, α(Q)=1.00×10-5 42 | ||
7/2- | 340.71 6 | E1+M2 | 0.23 4 | 0.115 | α=0.115 31, α(K)=0.086 23, α(L)=0.0215 62, α(M)=0.0054 16, α(N)=0.00144 42, α(O)=3.32×10-4 97, α(P)=6.0E-5 18, α(Q)=4.9E-6 15 | ||
7/2- | 357.11 8 | M1(+E2) | 0.8 LT | 0.40 | α=0.40 8, α(K)=0.32 7, α(L)=0.064 8, α(M)=0.0155 16, α(N)=0.0041 5, α(O)=0.00095 11, α(P)=0.000174 21, α(Q)=1.4×10-5 3 | ||
7/2- | 387.0 1 | [E2] | 0.0774 | α=0.0774, α(K)=0.0430 6, α(L)=0.0254 4, α(M)=0.00669 10, α(N)=0.001778 25, α(O)=0.000396 6, α(P)=6.58×10-5 10, α(Q)=2.09E-6 3 | |||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
425.59 | 5/2+ | 341.1 1 | [M1+E2] | 0.33 | α=0.33 22, α(K)=0.25 19, α(L)=0.061 21, α(M)=0.0150 44, α(N)=0.0040 12, α(O)=9.1×10-4 29, α(P)=1.62E-4 59, α(Q)=1.12E-5 84 | ||
5/2+ | 351.5 1 | [E1] | 0.0255 | α=0.0255, α(K)=0.0206 3, α(L)=0.00373 6, α(M)=0.000890 13, α(N)=0.000234 4, α(O)=5.36×10-5 8, α(P)=9.57E-6 14, α(Q)=7.14E-7 10 | |||
5/2+ | 379.35 7 | M1(+E2) | 1.1 LT | 0.32 | α=0.32 9, α(K)=0.250 78, α(L)=0.051 10, α(M)=0.0125 20, α(N)=0.0033 6, α(O)=0.00076 13, α(P)=0.00014 3, α(Q)=1.12×10-5 34 | ||
5/2+ | 395.45 10 | [E1] | 0.0198 | α=0.0198, α(K)=0.01603 23, α(L)=0.00287 4, α(M)=0.000682 10, α(N)=0.000180 3, α(O)=4.12×10-5 6, α(P)=7.38E-6 11, α(Q)=5.62E-7 8 | |||
5/2+ | 398.14 8 | [M1+E2] | 0.21 | α=0.21 15, α(K)=0.16 13, α(L)=0.038 15, α(M)=0.0094 34, α(N)=0.00248 88, α(O)=5.7×10-4 22, α(P)=1.02E-4 43, α(Q)=7.4E-6 55 | |||
435.19 | 1/2+ | 407.82 4 | M1 | 0.334 | α=0.334, α(K)=0.269 4, α(L)=0.0496 7, α(M)=0.01187 17, α(N)=0.00315 5, α(O)=0.000732 11, α(P)=0.0001354 19, α(Q)=1.200×10-5 17 | ||
437.94 | (5/2-) | 50.83 15 | [M1] | 24.7 | α=24.7, α(L)=18.7 3, α(M)=4.49 8, α(N)=1.192 20, α(O)=0.277 5, α(P)=0.0513 9, α(Q)=0.00456 8 | ||
(5/2-) | 363.84 10 | [M1+E2] | 0.27 | α=0.27 19, α(K)=0.21 16, α(L)=0.050 18, α(M)=0.0123 40, α(N)=0.0033 11, α(O)=7.5×10-4 26, α(P)=1.33E-4 52, α(Q)=9.4E-6 70 | |||
(5/2-) | 391.61 9 | [E1] | 0.0202 | α=0.0202, α(K)=0.01636 23, α(L)=0.00293 5, α(M)=0.000697 10, α(N)=0.000184 3, α(O)=4.21×10-5 6, α(P)=7.54E-6 11, α(Q)=5.74E-7 8 | |||
(5/2-) | 410.30 12 | [E1] | 0.0183 | α=0.0183, α(K)=0.01484 21, α(L)=0.00264 4, α(M)=0.000629 9, α(N)=0.0001656 24, α(O)=3.80×10-5 6, α(P)=6.81E-6 10, α(Q)=5.22E-7 8 | |||
(5/2-) | 438.01 9 | [M1+E2] | 0.17 | α=0.17 11, α(K)=0.128 94, α(L)=0.029 13, α(M)=0.0071 28, α(N)=0.00187 72, α(O)=4.3×10-4 18, α(P)=7.7E-5 35, α(Q)=5.7E-6 42 | |||
469.27 | 9/2+ | 359.33 15 | [M1+E2] | 0.28 | α=0.28 19, α(K)=0.21 17, α(L)=0.052 19, α(M)=0.0128 41, α(N)=0.0034 11, α(O)=7.8×10-4 26, α(P)=1.39E-4 53, α(Q)=9.7E-6 73 | ||
9/2+ | 384.7 1 | [M1+E2] | 0.24 | α=0.24 16, α(K)=0.18 14, α(L)=0.042 17, α(M)=0.0104 36, α(N)=0.00275 94, α(O)=6.3×10-4 23, α(P)=1.13E-4 46, α(Q)=8.1E-6 60 | |||
537.02 | (3/2+) | 232.20 10 | [M1+E2] | 0.97 | α=0.97 61, α(K)=0.69 57, α(L)=0.21 3, α(M)=0.053 4, α(N)=0.0140 11, α(O)=0.0032 4, α(P)=0.00055 10, α(Q)=3.2×10-5 26 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0.0 | 3/2- | 21.772 y 3 % β- = 98.6200 36 % α = 1.3800 36 | μ=+1.1 1 (1955Fr26,2014StZZ), Q=+1.7 2 (1955Fr26,2013StZZ) Configuration: α particle branching in 231Pa decay, Iα(exp)=11.0 5 agrees well with Iα(theory)=12.1 for 3/2-,3/2[532] (1969La04,1965PoZZ). The theoretical magnetic (μ=1.08) and quadrupole (Q=1.44) moments for 3/2-,3/2[532] coupled to a stable octupole deformation of ε3=0.1 agree well with the experimental values (1988Le13). E(level): Configuration: α particle branching in 231Pa decay, Iα(exp)=11.0 5 agrees well with Iα(theory)=12.1 for 3/2-,3/2[532] (1969La04,1965PoZZ). The theoretical magnetic (μ=1.08) and quadrupole (Q=1.44) moments for 3/2-,3/2[532] coupled to a stable octupole deformation of ε3=0.1 agree well with the experimental values (1988Le13). π3/2[532] parity doublet band. |
27.369 | 3/2+ | 38.3 ns 3 | Configuration: α particle branching in 231Pa decay, Iα(exp)≈2.5% disagrees with Iα(theory)=11.8 for 3/2+,3/2[651] (1969La04,1965PoZZ). Coriolis mixing with other n=6 Nilsson orbitals probably affects this branching. E(level): Configuration: α particle branching in 231Pa decay, Iα(exp)≈2.5% disagrees with Iα(theory)=11.8 for 3/2+,3/2[651] (1969La04,1965PoZZ). Coriolis mixing with other n=6 Nilsson orbitals probably affects this branching. π3/2[651] parity doublet band. |
29.978 | 5/2- | Configuration: α particle branching in 231Pa decay, Iα(exp)=20.0% 5 compares well with Iα(theory)=13.3% for 5/2-,3/2[532] (1969La04,1965PoZZ). E(level): Configuration: α particle branching in 231Pa decay, Iα(exp)=20.0% 5 compares well with Iα(theory)=13.3% for 5/2-,3/2[532] (1969La04,1965PoZZ). π3/2[532] parity doublet band. | |
46.354 | 5/2+ | The α particle branching in 231Pa decay, Iα(exp)=25.4% 5 was used by 1969La04 to normalize theory (1965PoZZ) and experiment for 5/2+,3/2[651]. E(level): π3/2[651] parity doublet band. | |
74.149 | 7/2- | Configuration: α particle branching in 231Pa decay, Iα(exp)=1.4% agrees well with Iα(theory)=1.6% for 7/2-,3/2[532] (1969La04,1965PoZZ). E(level): π3/2[532] parity doublet band. | |
84.544 | 7/2+ | Configuration: α particle branching in 231Pa decay, Iα(exp)=0.4%, as compared to Iα(theory)=1.4% for 7/2+,3/2[651] (1969La04,1965PoZZ). E(level): Configuration: α particle branching in 231Pa decay, Iα(exp)=0.4%, as compared to Iα(theory)=1.4% for 7/2+,3/2[651] (1969La04,1965PoZZ). π3/2[651] parity doublet band. | |
109.992 | 9/2+ | Configuration: α particle branching in 231Pa decay, Iα(exp)=22.8% as compared to Iα(theory)=16.9% for 9/2+,3/2[651] (1969La04,1965PoZZ). E(level): π3/2[651] parity doublet band. | |
126.848 | 9/2- | Configuration: α particle branching in 231Pa decay, Iα(exp)=3.0% agrees well with Iα(theory)=2.5% for 9/2-,3/2[532] (1969La04,1965PoZZ). E(level): Configuration: α particle branching in 231Pa decay, Iα(exp)=3.0% agrees well with Iα(theory)=2.5% for 9/2-,3/2[532] (1969La04,1965PoZZ). π3/2[532] parity doublet band. | |
160 | XREF: C(?). | ||
187.34 | 11/2+ | E(level): π3/2[651] parity doublet band. | |
198.69 | 11/2- | E(level): π3/2[532] parity doublet band. | |
210.84 | 13/2+ | E(level): π3/2[651] parity doublet band. | |
227 | XREF: C(?). | ||
249 | XREF: C(?). | ||
271.32 | (13/2-) | Configuration: α particle branching in 231Pa decay, Iα(exp)=0.04% is the same as Iα(theory)=0.04% for 13/2-,3/2[532] (1969La04,1965PoZZ). E(level): π3/2[532] parity doublet band. | |
273.19 | (5/2)- | E(level): π5/2[523] parity doublet band. | |
304.73 | (5/2+) | Level is weakly populated in 231Pa α decay. E(level): π5/2[642] parity doublet band. | |
317 | (7/2-) | E(level): π5/2[523] parity doublet band. | |
330.040 | 3/2- | < 70 ps | E(level): π1/2[530] parity doublet band. |
342 | (7/2+) | E(level): π5/2[642] parity doublet band. | |
354.50 | 1/2- | Configuration: α particle branching from 231Pa decay, Iα(exp)≈1% agrees with Iα(theory)=1.4% for 1/2-,1/2[530] (1969La04,1965PoZZ). E(level): Configuration: α particle branching from 231Pa decay, Iα(exp)≈1% agrees with Iα(theory)=1.4% for 1/2-,1/2[530] (1969La04,1965PoZZ). π1/2[530] parity doublet band. | |
372 | (9/2-) | E(level): π5/2[523] parity doublet band. | |
387.202 | 7/2- | Configuration: α particle branching from 231Pa decay, Iα(exp)=1.5% as compared to Iα(theory)=2.2% for 7/2-,1/2[530] (1969La04,1965PoZZ). E(level): Configuration: α particle branching from 231Pa decay, Iα(exp)=1.5% as compared to Iα(theory)=2.2% for 7/2-,1/2[530] (1969La04,1965PoZZ). π1/2[530] parity doublet band. | |
403 | (9/2+) | E(level): π5/2[642] parity doublet band. | |
425.59 | 5/2+ | Configuration: experimental band decoupling parameter (4.6) agrees wit with theoretical value for the 1/2[660] Nilsson orbital (1983Sh16). E(level): Configuration: experimental band decoupling parameter (4.6) agrees wit with theoretical value for the 1/2[660] Nilsson orbital (1983Sh16). π1/2[660] parity doublet band. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
435.19 | 1/2+ | E(level): π1/2[660] parity doublet band. | |
437.94 | (5/2-) | Configuration: α particle branching from 231Pa decay, Iα(exp)≈0.1% agrees with Iα(theory)=0.17 for 5/2-,1/2[530] (1969La04,1967Po05). E(level): Configuration: α particle branching from 231Pa decay, Iα(exp)≈0.1% agrees with Iα(theory)=0.17 for 5/2-,1/2[530] (1969La04,1967Po05). π1/2[530] parity doublet band. | |
469.27 | 9/2+ | E(level): π1/2[660] parity doublet band. | |
514.36 | (3/2,5/2)+ | E(level): π1/2[660] parity doublet band. | |
527 | (13/2+) | E(level): π5/2[642] parity doublet band. | |
577 | (9/2-) | E(level): π1/2[530] parity doublet band. | |
592 | (13/2)+ | XREF: C(589). E(level): π1/2[660] parity doublet band. | |
639.09 | 1/2+ | E(level): π1/2[400] band. | |
656.4 | (7/2+) | E(level): π1/2[660] parity doublet band. | |
698.56 | (3/2)+ | E(level): π1/2[400] band. |
E(level) | E(gamma) | Comments |
46.354 | 46.35 | M(γ): δ(Q/d)=+0.11 10 from γγ(θ) in 231Pa decay (1982An02), consistent with pure dipole |
84.544 | 57.19 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
271.32 | 161.0 | E(γ): evaluators treat this γ as questionable due to implied high multipolarity |
273.19 | 198.89 | I(γ): other: 3.1 in 227Ra decay | 226.6 | E(γ): From 227Ra β- decay. With the intensity reported in 227Ra decay, the γ ray should have been seen in 231Pa α decay. Evaluators treat this transition as uncertain I(γ): From 227Ra β- decay | 246.04 | I(γ): other: 3.1 in 227Ra decay |
304.73 | 219.90 | E(γ): From 227Ra β- decay I(γ): From 227Ra β- decay | 230.0 | E(γ): γ reported only in 231Pa α decay. With the intensity reported, it should have been seen in 227Ra β- decay. Evaluators treat this transition as uncertain I(γ): γ reported only in 231Pa α decay. With the intensity reported, it should have been seen in 227Ra β- decay. Evaluators treat this transition as uncertain | 277.39 | E(γ): From 227Ra β- decay I(γ): From 227Ra β- decay |
330.040 | 57.19 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided | 302.667 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
387.202 | 57.19 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided | 302.667 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
425.59 | 341.1 | E(γ): From 227Ra β- decay. With the intensity reported in 227Ra decay, the γ ray should have been seen in 231Pa α decay. Evaluators treat this transition as uncertain I(γ): From 227Ra β- decay |
428.4 | 398.4 | I(γ): doublet in 227Ra decay; intensity split based on its intensity in 231Pa decay, where the 398γ is a single line, placed from 425 level |
435.19 | 390.4 | E(γ): From 227Ra β- decay. With the intensity reported in 227Ra decay, the γ ray should have been seen in 231Pa α decay. Evaluators treat this transition as uncertain I(γ): From 227Ra β- decay |
501.29 | 146.9 | E(γ): From 227Ra β- decay I(γ): From 227Ra β- decay | 228.00 | E(γ): From 227Ra β- decay I(γ): From 227Ra β- decay | 427.0 | E(γ): γ reported only in 231Pa α decay. With the intensity reported, it should have been seen in 227Ra β- decay. Evaluators treat this transition as uncertain I(γ): 85 42 in 231Pa decay for a weak γ. γ reported only in 231Pa α decay. With the intensity reported, it should have been seen in 227Ra β- decay. Evaluators treat this transition as uncertain | 471.3 | E(γ): From 227Ra β- decay I(γ): From 227Ra β- decay | 501.4 | E(γ): From 227Ra β- decay I(γ): From 227Ra β- decay |
537.02 | 232.20 | E(γ): From 227Ra β- decay I(γ): From 227Ra β- decay | 510.0 | I(γ): value given only in 231Pa decay. |
562.78 | 478.4 | E(γ): From 227Ra β- decay I(γ): From 227Ra β- decay | 486.827 | E(γ): γ reported only in 231Pa α decay. With the intensity reported, it should have been seen in 227Ra β- decay. Evaluators treat this transition as uncertain I(γ): γ reported only in 231Pa α decay. With the intensity reported, it should have been seen in 227Ra β- decay. Evaluators treat this transition as uncertain |
E(level) | E(gamma) | Comments |
227Ac evaluated by B. Singh, I. Ami, α. Chakraborty, S. Kumar, M. Latif and d. Yang.
227Ac lies at the border of the octupole-quadrupole and pure quadrupole deformation regions. 1983Sh16 interpreted this nucleus as having a core with a "soft " octupole deformation (1990Ja11). The presence of parity doublet rotational bands, and also of K=1/2 rotational bands with decoupling parameters having opposite signs, suggests a stable octupole deformation for 227Ac (1987Le05). The level structure, (α,t) spectroscopic factors, and the ground state magnetic and quadrupole moments, have been interpreted in terms of a stable octupole deformation with ε3≈0.1 (1988Le13,1983Sh16). It should be mentioned, however, that the experimental (α,t) spectroscopic factors of 1988Ma18 agree with theoretical values based on a quadrupole deformation only.
Levels: Band assignments: parity doublet band assignments are from 1990Ja11. Although octupole deformations are small in this region, the states are not fully characterized by single Nilsson orbitals. Single-particle orbitals, however, are used here to label states rather than to accurately describe their detailed configurations
Q-value: S(2n)=11930 5, S(2p)=12548 12 (2012Wa38)