ADOPTED LEVELS, GAMMAS for 45Ca
Author: T. W. Burrows | Citation: Nucl. Data Sheets 109, 171 (2008) | Cutoff date: 30-Oct-2007
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=259.0 keV 8 | S(n)= 7414.81 keV 17 | S(p)= 12319.6 keV 6 | Q(α)= -10169.6 keV 5 | ||
Reference: 2012WA38 |
References: | |||
A | 45K β- decay | B | 36S(14C,NAG) |
C | 44Ca(pol n,γ),(n,γ) E=THERMAL | D | 44Ca(n,γ) E=10-60 KEV RES |
E | 44Ca(d,p) | F | 44Ca(d,pγ) |
G | 46Ca(d,t),(3He,α) | H | 48Ca(3He,6He) |
I | 48Ti(n,αγ) |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
0.0 | ABCDEFGHI | 7/2- | 162.61 d 9 % β- = 100 | |||||
174.25 4 | A CDEFGHI | 5/2- | 0.40 ns 4 | 174.259 47 | 100 | (M1) | 0.0 | 7/2- |
1434.77 6 | A CDEFGH | 3/2- | 1.10 ps +22-16 | 1260.58 7 1434.72 13 | 100 3 49 3 | M1+E2 (E2) | 174.25 0.0 | 5/2- 7/2- |
1554.37 8 | B H | (11/2-) | > 2.1 ps | 1554.34 8 | 100 | (E2(+M3)) | 0.0 | 7/2- |
1558 10 | E | |||||||
1584 6 | E | |||||||
1879.89 16 | A C EFG | 3/2+ | 0.05 ps 3 | 1705.6 2 1879.9 3 | 100.000 30 0.0371 30 | (E1) (M2) | 174.25 0.0 | 5/2- 7/2- |
1884.4 4 | C E GH | 1710.1 4 | 100 | 174.25 | 5/2- | |||
1899.92 6 | A CDEFGH | 3/2- | 1.12 ps +11-9 | 464.96 12 1725.68 7 1900.13 18 | 9.4 12 100 3 36.9 75 | (M1+E2) M1+E2 (E2) | 1434.77 174.25 0.0 | 3/2- 5/2- 7/2- |
1940.19 7 ? | B | 385.74 8 ? | 100 | 1554.37 | (11/2-) | |||
1973 6 | E | 5/2-,7/2- | ||||||
2249.10 7 | A CDEF | 1/2- | 0.43 ps +7-6 | 349.11 10 814.51 10 2074.71 9 | 53.2 76 60.8 89 100.0 16 | (M1) (M1) (E2) | 1899.92 1434.77 174.25 | 3/2- 3/2- 5/2- |
2353.81 16 | A E | 1/2+,3/2+,5/2+ | 4.7 ns 11 | 453.9 3 919.3 3 2179.4 3 2353.6 5 | 0.30 6 6.14 45 6.93 57 100.0 11 | (M2) (E1,M2) (M2) (E1,M2,E3) | 1899.92 1434.77 174.25 0.0 | 3/2- 3/2- 5/2- 7/2- |
2392.29 14 | A C EFGH | 1/2+ | 0.19 ps 4 | 492.5 2 512 1 957.5 2 2217.3 6 2392.0 4 | 17.3 13 16.0 53 100.0 53 0.27 13 0.13 13 | (E1) (M1) (E1) (M2) [E3] | 1899.92 1879.89 1434.77 174.25 0.0 | 3/2- 3/2+ 3/2- 5/2- 7/2- |
2523.1 4 ? | A | (3/2,5/2,7/2) | 623.4 6 ? 2349 1 ? 2522.7 6 ? | 10.8 41 100 11 24.3 14 | 1899.92 174.25 0.0 | 3/2- 5/2- 7/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
2599 6 | E | |||||||
2675.1 10 | C EF | (3/2,5/2) | 2675 | | 0.0 | 7/2- | ||
2771.10 15 | A E | 1/2+,3/2+,5/2+ | 417.4 3 522.4 8 871.3 5 891.3 4 1336.4 8 2596.7 2 2769.9 10 | 13.6 17 0.17 14 4.767 17 21.4 24 98 17 100 12 0.71 24 | 2353.81 2249.10 1899.92 1879.89 1434.77 174.25 0.0 | 1/2+,3/2+,5/2+ 1/2- 3/2- 3/2+ 3/2- 5/2- 7/2- | ||
2786 12 ? | H | |||||||
2842.05 16 | A CDEFG | 3/2- | 22 fs 6 | 942.7 10 ? 957.8 3 ? 2667.7 2 2842.2 3 | 9.1 61 30 16 100 15 84 11 | D,E2 (E1) D,E2 (E2) | 1899.92 1884.4 174.25 0.0 | 3/2- 5/2- 7/2- |
2877.99 12 | B H | (15/2-) | > 2.1 ps | 1323.60 9 | 100 | (E2(+M3)) | 1554.37 | (11/2-) |
2953 6 | E | |||||||
2976.8 5 | A EF | 5/2- | 42 fs 19 | 2802.4 6 2976.7 6 | 100.0 26 28.28 26 | D,E2 (E2) | 174.25 0.0 | 5/2- 7/2- |
3023.6 4 | A | 1/2,3/2,5/2 | 2849.3 4 | 100 | 174.25 | 5/2- | ||
3035 6 ? | E H | |||||||
3151 6 | E | |||||||
3241.27 24 | CDEF | 3/2- | 36 fs 12 | 565.6 10 ? 992? 3066.9 4 3241? | 23 15 100 15 | D D,E2 | 2675.1 2249.10 174.25 0.0 | (3/2,5/2) 1/2- 5/2- 7/2- |
3278 6 | E | |||||||
3294.5 3 | A E | (3/2+,5/2+) | 771.4 8 ? 1860.4 12 3120.2 4 3294.3 4 | 35.6 44 15.6 22 100.0 44 68.9 44 | 2523.1 1434.77 174.25 0.0 | (3/2,5/2,7/2) 3/2- 5/2- 7/2- | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
3322 6 | E | 5/2-,7/2- | ||||||
3348 12 | H | |||||||
3418.46 14 | CD F | 1/2- | 35 fs 7 | 576.4 5 1026.0 6 ? 1169.66 24 1983.7 4 3243.5 3 | 18 10 10 5 100 15 25 8 60 10 | (M1) (E1) (M1) (M1) (E2) | 2842.05 2392.29 2249.10 1434.77 174.25 | 3/2- 1/2+ 1/2- 3/2- 5/2- |
3442 10 | E | 1/2-,3/2- | ||||||
3463 10 | E | |||||||
3490.7 5 | A H | 3/2-,5/2+ | 1098.0 6 3491.0 6 | 100 9 85 9 | 2392.29 0.0 | 1/2+ 7/2- | ||
3556.01 10 ? | B | 2001.48 10 ? | 100 | 1554.37 | (11/2-) | |||
3560 10 | G | (1/2+) | ||||||
3654.0 5 ? | A | 1/2,3/2,5/2 | 3479.9 8 ? 3653.8 6 ? | 100 5 28 5 | 174.25 0.0 | 5/2- 7/2- | ||
3675 12 ? | H | |||||||
3705.0 6 | A E | 1/2,3/2,5/2 | 3704.8 6 | 100 | 0.0 | 7/2- | ||
3753 10 | E | |||||||
3783.22 22 | CDEF | 1/2-,3/2- | < 26 fs | 3609.3 3 | 100 | D,E2 | 174.25 | 5/2- |
3838.00 20 | CDEF H | (1/2)- | < 15 fs | 1938.1 5 2403.3 3 | 50 10 100 20 | (M1) (M1) | 1899.92 1434.77 | 3/2- 3/2- |
3941.83 14 | B | 385.74 8 ? 1063.83 6 2001.48 10 ? | 83 43 100 50 83 25 | 3556.01 2877.99 1940.19 | (15/2-) | |||
3993 10 | E G | 5/2-,7/2- | ||||||
4048 10 | E | |||||||
4115 10 | E | |||||||
4177 10 | E | 5/2-,7/2- | ||||||
4258 10 | E | |||||||
4286 10 | E H | |||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
4312 10 | E | (1/2-,3/2-) | ||||||
4388 10 | E | |||||||
4421 10 | E | |||||||
4467.7 10 | C E | 1/2-,3/2- | ||||||
4511 10 | E | (1/2-,3/2-) | ||||||
4559 10 | E | |||||||
4615.72 15 | C EF | 1/2- | < 12 fs | 2716.0 3 3180.8 3 | 100 19 44 13 | (M1) (M1) | 1899.92 1434.77 | 3/2- 3/2- |
4695 10 | E | (5/2-,7/2,9/2+) | ||||||
4750 10 | E | 3/2+,5/2+ | ||||||
4762 10 | E | 1/2+ | ||||||
4810 10 | E | 1/2-,3/2- | ||||||
4837 10 | E | 3/2+,5/2+ | ||||||
4885 10 | E | (5/2-,7/2-) | ||||||
4919 10 | E | 1/2+ | ||||||
4981 10 | E | 1/2+ | ||||||
4999.74 19 | C EF | (1/2)- | < 9.7 fs | 2608.2 15 3099.7 4 3565.0 3 | 100 55 82 18 27 18 | [E1] [M1] [M1] | 2392.29 1899.92 1434.77 | 1/2+ 3/2- 3/2- |
5047 10 | E | 1/2+ | ||||||
5079 10 | E | |||||||
5128 10 | E | (1/2+) | ||||||
5164 10 | E | |||||||
5201 10 | E | 1/2+ | ||||||
5237 3 | C E | 1/2-,3/2- | ||||||
5285 10 | E | |||||||
5309 10 | E | |||||||
5324 10 | E | 3/2+,5/2+ | ||||||
5352 10 | E | 1/2+ | ||||||
5373 10 | E | 1/2-,3/2- | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
5390 10 | E | 7/2+,9/2+ | ||||||
5417 10 | E | 3/2+,5/2+ | ||||||
5440 10 | E | 1/2-,3/2- | ||||||
5479 10 | E | 1/2+ | ||||||
5521 10 | E | 7/2+,9/2+ | ||||||
5551 10 | E | |||||||
5569 10 | E | |||||||
5598 10 | E | |||||||
5629 10 | E | |||||||
5687 10 | E | |||||||
5716 10 | E | |||||||
5742 10 | E | (3/2+,5/2+) | ||||||
5764 10 | E | 5/2-,7/2- | ||||||
5792 10 | E | |||||||
5818 10 | E | 1/2+ | ||||||
5846 10 | E | 1/2-,3/2- | ||||||
5892 10 | E | 3/2+,5/2+ | ||||||
5915 10 | E | |||||||
5948 10 | E | |||||||
5967 10 | E | |||||||
5990 10 | E | |||||||
6018 10 | E | |||||||
6051 10 | E | |||||||
6077 10 | E | |||||||
6106 10 | E | |||||||
6234 10 | E | |||||||
6301 10 | E |
E(level): For states connected by gammas from least-squares fit to Eγ’s assuming ΔE(γ)=1 keV; capture-state energy held fixed in the fit. Other excitation energies are from (d,p) except as indicated in the XREF column
Jπ(level): From angular momentum transfer in (d,p), except as noted
T1/2(level): From DSAM in (d,pγ), except as noted
E(γ): From β- decay, except as noted
I(γ): From β- decay branching ratios in Table IV of 1980Hu10, except as noted
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 1 - (ν f7/2)-3 MULTIPLET. | |||||||
174.25 4 | 5/2- | 0.40 ns 4 | |||||
1434.77 6 | 3/2- | 1.10 ps +22-16 | 1260.58 7 1434.72 13 | 100 3 49 3 | M1+E2 (E2) | 174.25 0.0 | 5/2- 7/2- |
1554.37 8 | (11/2-) | > 2.1 ps | 1554.34 8 | 100 | (E2(+M3)) | 0.0 | 7/2- |
2877.99 12 | (15/2-) | > 2.1 ps | 1323.60 9 | 100 | (E2(+M3)) | 1554.37 | (11/2-) |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
174.25 | 5/2- | 0.40 ns 4 | 174.259 47 | (M1) | 0.00326 | B(M1)(W.u.)=0.0104 11, α=0.00326 5, α(K)=0.00297 5, α(L)=0.000259 4, α(M)=3.08×10-5 5, α(N)=1.727E-6 25, α(N+)=1.727E-6 25 | |
1434.77 | 3/2- | 1.10 ps +22-16 | 1260.58 7 | M1+E2 | 6.6×10-5 | α=6.6×10-5 8, α(K)=4.4E-5 5, α(L)=3.8E-6 4, α(M)=4.5E-7 5, α(N)=2.6E-8 3, α(N+)=1.7E-5 4 | |
3/2- | 1.10 ps +22-16 | 1434.72 13 | (E2) | 0.0001060 | B(E2)(W.u.)=2.9 +5-7, α=0.0001060 15, α(K)=3.70E-5 6, α(L)=3.18E-6 5, α(M)=3.77E-7 6, α(N)=2.14E-8 3, α(N+)=6.53E-5 10 | ||
1554.37 | (11/2-) | > 2.1 ps | 1554.34 8 | (E2(+M3)) | 0.00 6 | 0.0001440 | B(E2)(W.u.)<3.1, α=0.0001440 21, α(K)=3.14E-5 5, α(L)=2.70E-6 5, α(M)=3.20E-7 5, α(N)=1.82E-8 3, α(N+)=0.0001097 16 |
1879.89 | 3/2+ | 0.05 ps 3 | 1705.6 2 | (E1) | 0.000441 | B(E1)(W.u.)=0.0022 13, α=0.000441 7, α(K)=1.457E-5 21, α(L)=1.247E-6 18, α(M)=1.481E-7 21, α(N)=8.42E-9 12, α(N+)=0.000425 6 | |
3/2+ | 0.05 ps 3 | 1879.9 3 | (M2) | 0.0001380 | B(M2)(W.u.)=0.8 5, α=0.0001380 20, α(K)=3.35×10-5 5, α(L)=2.88E-6 4, α(M)=3.42E-7 5, α(N)=1.94E-8 3, α(N+)=0.0001011 15 | ||
1899.92 | 3/2- | 1.12 ps +11-9 | 464.96 12 | (M1+E2) | 0.0006 | α=0.0006 3, α(K)=0.00054 24, α(L)=4.6×10-5 21, α(M)=5.5E-6 25, α(N)=3.1E-7 14, α(N+)=3.1E-7 14 | |
3/2- | 1.12 ps +11-9 | 1725.68 7 | M1+E2 | +0.34 4 | 1.70×10-4 | B(E2)(W.u.)=0.25 6, B(M1)(W.u.)=0.00234 +25-28, α=1.70E-4 3, α(K)=2.31E-5 4, α(L)=1.98E-6 3, α(M)=2.35E-7 4, α(N)=1.338E-8 19, α(N+)=0.0001449 23 | |
3/2- | 1.12 ps +11-9 | 1900.13 18 | (E2) | 0.000289 | B(E2)(W.u.)=0.54 13, α=0.000289 5, α(K)=2.13E-5 3, α(L)=1.82E-6 3, α(M)=2.17E-7 3, α(N)=1.232E-8 18, α(N+)=0.000265 4 | ||
2249.10 | 1/2- | 0.43 ps +7-6 | 349.11 10 | (M1) | 0.000626 | B(M1)(W.u.)=0.30 7, α=0.000626 9, α(K)=0.000570 8, α(L)=4.94×10-5 7, α(M)=5.86E-6 9, α(N)=3.31E-7 5, α(N+)=3.31E-7 5 | |
1/2- | 0.43 ps +7-6 | 814.51 10 | (M1) | 0.0001020 | B(M1)(W.u.)=0.027 6, α=0.0001020 15, α(K)=9.26×10-5 13, α(L)=7.96E-6 12, α(M)=9.45E-7 14, α(N)=5.37E-8 8, α(N+)=5.37E-8 8 | ||
1/2- | 0.43 ps +7-6 | 2074.71 9 | (E2) | 0.000371 | B(E2)(W.u.)=1.7 3, α=0.000371 6, α(K)=1.81E-5 3, α(L)=1.553E-6 22, α(M)=1.84E-7 3, α(N)=1.049E-8 15, α(N+)=0.000351 5 | ||
2353.81 | 1/2+,3/2+,5/2+ | 4.7 ns 11 | 453.9 3 | (M2) | 0.001160 | B(M2)(W.u.)=0.072 22, α=0.001160 17, α(K)=0.001060 15, α(L)=9.27×10-5 13, α(M)=1.100E-5 16, α(N)=6.19E-7 9, α(N+)=6.19E-7 9 | |
1/2+,3/2+,5/2+ | 4.7 ns 11 | 919.3 3 | (E1,M2) | 0.00011 | B(E1)(W.u.)<7.9E-9 20, B(M2)(W.u.)<0.043 11, α=0.00011 7, α(K)=0.00010 7, α(L)=9.E-6 6, α(M)=1.1E-6 7, α(N)=6.E-8 4, α(N+)=6.E-8 4 | ||
1/2+,3/2+,5/2+ | 4.7 ns 11 | 2179.4 3 | (M2) | 0.000214 | B(M2)(W.u.)=0.00065 17, α=0.000214 3, α(K)=2.49×10-5 4, α(L)=2.14E-6 3, α(M)=2.54E-7 4, α(N)=1.446E-8 21, α(N+)=0.000187 3 | ||
1/2+,3/2+,5/2+ | 4.7 ns 11 | 2353.6 5 | (E1,M2,E3) | 0.0006 | B(E1)(W.u.)<7.7E-9 18, B(E3)(W.u.)<4.7 12, B(M2)(W.u.)<0.0064 15, α=0.0006 4, α(K)=1.5E-5 7, α(L)=1.3E-6 6, α(M)=1.6E-7 7, α(N)=9.E-9 4, α(N+)=0.0006 4 | ||
2392.29 | 1/2+ | 0.19 ps 4 | 492.5 2 | (E1) | 0.000198 | B(E1)(W.u.)=0.0030 7, α=0.000198 3, α(K)=0.000180 3, α(L)=1.549E-5 22, α(M)=1.84E-6 3, α(N)=1.039E-7 15, α(N+)=1.039E-7 15 | |
1/2+ | 0.19 ps 4 | 512 1 | (M1) | 0.000267 | B(M1)(W.u.)=0.10 4, α=0.000267 4, α(K)=0.000244 4, α(L)=2.10×10-5 3, α(M)=2.49E-6 4, α(N)=1.413E-7 21, α(N+)=1.413E-7 21 | ||
1/2+ | 0.19 ps 4 | 957.5 2 | (E1) | 4.37×10-5 | B(E1)(W.u.)=0.0024 6, α=4.37E-5 7, α(K)=3.98E-5 6, α(L)=3.41E-6 5, α(M)=4.05E-7 6, α(N)=2.30E-8 4, α(N+)=2.30E-8 4 | ||
1/2+ | 0.19 ps 4 | 2217.3 6 | (M2) | 0.000225 | B(M2)(W.u.)=0.5 3, α=0.000225 4, α(K)=2.41×10-5 4, α(L)=2.07E-6 3, α(M)=2.46E-7 4, α(N)=1.398E-8 20, α(N+)=0.000198 3 | ||
1/2+ | 0.19 ps 4 | 2392.0 4 | [E3] | 0.000336 | B(E3)(W.u.)≤2.4×102, α=0.000336 5, α(K)=2.14E-5 3, α(L)=1.84E-6 3, α(M)=2.18E-7 3, α(N)=1.240E-8 18, α(N+)=0.000313 5 | ||
2842.05 | 3/2- | 22 fs 6 | 957.8 3 | (E1) | 4.36×10-5 | B(E1)(W.u.)=0.0037 23, α=4.36E-5 7, α(K)=3.98E-5 6, α(L)=3.41E-6 5, α(M)=4.05E-7 6, α(N)=2.30E-8 4, α(N+)=2.30E-8 4 | |
3/2- | 22 fs 6 | 2842.2 3 | (E2) | 0.000726 | B(E2)(W.u.)=5.5 18, α=0.000726 11, α(K)=1.061E-5 15, α(L)=9.07E-7 13, α(M)=1.078E-7 15, α(N)=6.14E-9 9, α(N+)=0.000714 10 | ||
2877.99 | (15/2-) | > 2.1 ps | 1323.60 9 | (E2(+M3)) | 0.00 6 | 8.28×10-5 | B(E2)(W.u.)<7.0, α=8.28E-5 12, α(K)=4.40E-5 7, α(L)=3.77E-6 6, α(M)=4.48E-7 7, α(N)=2.54E-8 4, α(N+)=3.47E-5 5 |
2976.8 | 5/2- | 42 fs 19 | 2976.7 6 | (E2) | 0.000785 | B(E2)(W.u.)=1.3 6, α=0.000785 11, α(K)=9.85E-6 14, α(L)=8.42E-7 12, α(M)=1.001E-7 14, α(N)=5.70E-9 8, α(N+)=0.000774 11 | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
3418.46 | 1/2- | 35 fs 7 | 576.4 5 | (M1) | 0.000207 | B(M1)(W.u.)=0.28 17, α=0.000207 3, α(K)=0.000189 3, α(L)=1.628×10-5 23, α(M)=1.93E-6 3, α(N)=1.096E-7 16, α(N+)=1.096E-7 16 | |
1/2- | 35 fs 7 | 1026.0 6 | (E1) | 3.82×10-5 | B(E1)(W.u.)=0.0007 4, α=3.82E-5 6, α(K)=3.48E-5 5, α(L)=2.99E-6 5, α(M)=3.54E-7 5, α(N)=2.01E-8 3, α(N+)=2.01E-8 3 | ||
1/2- | 35 fs 7 | 1169.66 24 | (M1) | 5.40×10-5 | B(M1)(W.u.)=0.18 5, α=5.40×10-5 8, α(K)=4.59E-5 7, α(L)=3.94E-6 6, α(M)=4.68E-7 7, α(N)=2.66E-8 4, α(N+)=3.63E-6 6 | ||
1/2- | 35 fs 7 | 1983.7 4 | (M1) | 0.000262 | B(M1)(W.u.)=0.009 4, α=0.000262 4, α(K)=1.80×10-5 3, α(L)=1.542E-6 22, α(M)=1.83E-7 3, α(N)=1.043E-8 15, α(N+)=0.000242 4 | ||
1/2- | 35 fs 7 | 3243.5 3 | (E2) | 0.000895 | B(E2)(W.u.)=1.3 4, α=0.000895 13, α(K)=8.60E-6 12, α(L)=7.36E-7 11, α(M)=8.74E-8 13, α(N)=4.98E-9 7, α(N+)=0.000886 13 | ||
3838.00 | (1/2)- | < 15 fs | 1938.1 5 | (M1) | 0.000244 | B(M1)(W.u.)>0.067, α=0.000244 4, α(K)=1.87×10-5 3, α(L)=1.604E-6 23, α(M)=1.91E-7 3, α(N)=1.085E-8 16, α(N+)=0.000223 4 | |
(1/2)- | < 15 fs | 2403.3 3 | (M1) | 0.000434 | B(M1)(W.u.)>0.070, α=0.000434 7, α(K)=1.316×10-5 19, α(L)=1.126E-6 16, α(M)=1.337E-7 19, α(N)=7.62E-9 11, α(N+)=0.000419 6 | ||
4615.72 | 1/2- | < 12 fs | 2716.0 3 | (M1) | 0.000564 | B(M1)(W.u.)>0.064, α=0.000564 8, α(K)=1.084×10-5 16, α(L)=9.27E-7 13, α(M)=1.102E-7 16, α(N)=6.28E-9 9, α(N+)=0.000553 8 | |
1/2- | < 12 fs | 3180.8 3 | (M1) | 0.000749 | B(M1)(W.u.)>0.017, α=0.000749 11, α(K)=8.51×10-6 12, α(L)=7.28E-7 11, α(M)=8.64E-8 13, α(N)=4.92E-9 7, α(N+)=0.000739 11 | ||
4999.74 | (1/2)- | < 9.7 fs | 2608.2 15 | [E1] | 0.001030 | B(E1)(W.u.)>0.0015, α=0.001030 15, α(K)=7.92E-6 12, α(L)=6.77E-7 10, α(M)=8.04E-8 12, α(N)=4.58E-9 7, α(N+)=0.001025 15 | |
(1/2)- | < 9.7 fs | 3099.7 4 | [M1] | 0.000717 | B(M1)(W.u.)>0.030, α=0.000717 11, α(K)=8.85×10-6 13, α(L)=7.57E-7 11, α(M)=8.99E-8 13, α(N)=5.12E-9 8, α(N+)=0.000708 10 | ||
(1/2)- | < 9.7 fs | 3565.0 3 | [M1] | 0.000892 | B(M1)(W.u.)>0.0065, α=0.000892 13, α(K)=7.18×10-6 10, α(L)=6.14E-7 9, α(M)=7.29E-8 11, α(N)=4.16E-9 6, α(N+)=0.000884 13 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0.0 | 7/2- | 162.61 d 9 % β- = 100 | μ=-1.3274 14 (2005St24,1983Ar25,1980Be13), Q=+0.046 14 (2005St24,1983Ar25,1981Ar15,1980Be13) E(level): Weighted ave. (ext.) of 174.24 4 (1971BiZH) and 174.01 9 (2003ChZS) from (n,γ) E=thermal and 174.28 3 from β- decay, 1704.01 24 from (n,γ) E=thermal and 1705.6 3 from β- decay, and 1900.20 12 from (n,γ) E=thermal and 1899.7 3 from β- decay. Jπ(level): Main components of the wave functions are (ν 1f7/2)5 and ((ν 1f7/2)4 (ν 2p3/2)) (1969Gr21). |
174.25 | 5/2- | 0.40 ns 4 | E(level): Weighted ave. (ext.) of 174.24 4 (1971BiZH) and 174.01 9 (2003ChZS) from (n,γ) E=thermal and 174.28 3 from β- decay, 1704.01 24 from (n,γ) E=thermal and 1705.6 3 from β- decay, and 1900.20 12 from (n,γ) E=thermal and 1899.7 3 from β- decay. (ν f7/2)-3 MULTIPLET. Jπ(level): Main components of the wave functions are (ν 1f7/2)5 and ((ν 1f7/2)4 (ν 2p3/2)) (1969Gr21). |
1434.77 | 3/2- | 1.10 ps +22-16 | E(level): Weighted ave. (ext.) of 174.24 4 (1971BiZH) and 174.01 9 (2003ChZS) from (n,γ) E=thermal and 174.28 3 from β- decay, 1704.01 24 from (n,γ) E=thermal and 1705.6 3 from β- decay, and 1900.20 12 from (n,γ) E=thermal and 1899.7 3 from β- decay. (ν f7/2)-3 MULTIPLET. From (n,γ). Jπ(level): Main components of the wave functions are (ν 1f7/2)5 and ((ν 1f7/2)4 (ν 2p3/2)) (1969Gr21). L(d,p)=1. d,E2 γ to 7/2-. |
1554.37 | (11/2-) | > 2.1 ps | XREF: H(1562). E(level): (ν f7/2)-3 MULTIPLET. Jπ(level): Stretched quadrupole cascade in (14C,nαγ). Large angular momentum transfer in (3He,6He). T1/2(level): From DSAM in (14C,nαγ). |
1558 | This state which is observed in (d,p) at 7 MeV is probably not the same as the 1554-keV state observed in (14C,nαγ) and (3He,6He) since the (d,p) reaction at 7 MeV is unlikely to populate an 11/2- state (L=5 required). E(level): This state which is observed in (d,p) at 7 MeV is probably not the same as the 1554-keV state observed in (14C,nαγ) and (3He,6He) since the (d,p) reaction at 7 MeV is unlikely to populate an 11/2- state (L=5 required). | ||
1879.89 | 3/2+ | 0.05 ps 3 | E(level): From (14C,nαγ). Identified as the same state in β- decay, (n,γ), and (d,pγ); however, based on the large discrepancy in the Eγ to the 5/2- between β- decay and (d,pγ) and (n,γ), the evaluator proposes two states. Jπ(level): L(d,p)=2 for doublet. |
1884.4 | E(level): From (14C,nαγ). Identified as the same state in β- decay, (n,γ), and (d,pγ); however, based on the large discrepancy in the Eγ to the 5/2- between β- decay and (d,pγ) and (n,γ), the evaluator proposes two states. Jπ(level): L(d,p)=2 for doublet. | ||
1899.92 | 3/2- | 1.12 ps +11-9 | E(level): Weighted ave. (ext.) of 174.24 4 (1971BiZH) and 174.01 9 (2003ChZS) from (n,γ) E=thermal and 174.28 3 from β- decay, 1704.01 24 from (n,γ) E=thermal and 1705.6 3 from β- decay, and 1900.20 12 from (n,γ) E=thermal and 1899.7 3 from β- decay. From (n,γ). Jπ(level): Main components of the wave functions are (ν 1f7/2)5 and ((ν 1f7/2)4 (ν 2p3/2)) (1969Gr21). L(d,p)=1. d,E2 γ to 7/2-. |
2249.10 | 1/2- | 0.43 ps +7-6 | E(level): Weighted ave. (ext.) of 174.24 4 (1971BiZH) and 174.01 9 (2003ChZS) from (n,γ) E=thermal and 174.28 3 from β- decay, 1704.01 24 from (n,γ) E=thermal and 1705.6 3 from β- decay, and 1900.20 12 from (n,γ) E=thermal and 1899.7 3 from β- decay. Jπ(level): Main components of the wave functions are (ν 1f7/2)5 and ((ν 1f7/2)4 (ν 2p3/2)) (1969Gr21). From circular polarization in (pol n,γ). |
2353.81 | 1/2+,3/2+,5/2+ | 4.7 ns 11 | E(level): See footnote on associated state. Jπ(level): log ft=5.8 via 3/2+ parent. |
2771.10 | 1/2+,3/2+,5/2+ | E(level): See footnote on associated state. Jπ(level): log ft=5.8 via 3/2+ parent. | |
2786 | May Be the same as the previous state; however, the large L transfer noted in (3He,6He) would indicate that it is not. | ||
2842.05 | 3/2- | 22 fs 6 | Jπ(level): From circular polarization in (pol n,γ). |
2877.99 | (15/2-) | > 2.1 ps | E(level): (ν f7/2)-3 MULTIPLET. Jπ(level): Stretched quadrupole cascade in (14C,nαγ). Large angular momentum transfer in (3He,6He). T1/2(level): From DSAM in (14C,nαγ). |
3023.6 | 1/2,3/2,5/2 | Jπ(level): log ft=6.3-7.3 via 3/2+ parent. | |
3035 | May Be the same as the 3024 state. | ||
3241.27 | 3/2- | 36 fs 12 | Jπ(level): From circular polarization in (pol n,γ). |
3418.46 | 1/2- | 35 fs 7 | Jπ(level): From circular polarization in (pol n,γ). |
3490.7 | 3/2-,5/2+ | Jπ(level): γ’s to 1/2+ and 7/2-. | |
3560 | (1/2+) | Jπ(level): L(d,t)=(0). | |
3654.0 | 1/2,3/2,5/2 | Jπ(level): log ft=6.3-7.3 via 3/2+ parent. | |
3705.0 | 1/2,3/2,5/2 | Jπ(level): log ft=6.3-7.3 via 3/2+ parent. | |
3838.00 | (1/2)- | < 15 fs | E(level): From (d,pγ). Jπ(level): L(d,p)=1. (1/2-) from circular polarization in (pol n,γ). |
4615.72 | 1/2- | < 12 fs | Jπ(level): From circular polarization in (pol n,γ). |
4999.74 | (1/2)- | < 9.7 fs | E(level): From (d,pγ). Jπ(level): L(d,p)=1. (1/2-) from circular polarization in (pol n,γ). |
E(level) | E(gamma) | Comments |
174.25 | 174.259 | E(γ): Weighted ave. (ext.) of 174.24 4 (1971BiZH) and 174.01 9 (2003ChZS) from (n,γ) E=thermal and 174.28 3 from β- decay, 1704.01 24 from (n,γ) E=thermal and 1705.6 3 from β- decay, and 1900.20 12 from (n,γ) E=thermal and 1899.7 3 from β- decay M(γ): d from comparison to RUL. M1 from Δπ=no |
1434.77 | 1260.58 | E(γ): From (n,γ) M(γ): D+Q from γγ(θ). Ne E1+M2 from δ’s and comparison to RUL | 1434.72 | E(γ): From (n,γ) M(γ): d,E2 from comparison to RUL. E2 from ΔJ=2 |
1554.37 | 1554.34 | E(γ): From (14C,nαγ). Identified as the same state in β- decay, (n,γ), and (d,pγ); however, based on the large discrepancy in the Eγ to the 5/2- between β- decay and (d,pγ) and (n,γ), the evaluator proposes two states I(γ): From (14C,nαγ) M(γ): Q(+O) from γ(θ) in (14C,nαγ); stretched quadrupole cascade. E2(+M3) from ΔJπ=2,no |
1879.89 | 1705.6 | E(γ): Weighted ave. (ext.) of 174.24 4 (1971BiZH) and 174.01 9 (2003ChZS) from (n,γ) E=thermal and 174.28 3 from β- decay, 1704.01 24 from (n,γ) E=thermal and 1705.6 3 from β- decay, and 1900.20 12 from (n,γ) E=thermal and 1899.7 3 from β- decay. See footnote on associated state M(γ): d,E2 from comparison to RUL. E1 from Δπ=yes | 1879.9 | M(γ): d,Q from comparison to RUL. M2 from ΔJπ=2,yes |
1884.4 | 1710.1 | E(γ): From (n,γ). See footnote on associated state |
1899.92 | 464.96 | E(γ): From (n,γ) I(γ): weighted ave. (ext.) from (n,γ) E=thermal and β- decay branching ratios in Table IV of 1980Hu10 M(γ): D+Q from γ(θ) in (n,γ). M1+E2 from Δπ=no | 1725.68 | E(γ): From (n,γ) I(γ): weighted ave. (int.) from (n,γ) E=thermal and β- decay branching ratios in Table IV of 1980Hu10 M(γ): D+Q from γγ(θ). Ne E1+M2 from δ and comparison to RUL | 1900.13 | E(γ): Weighted ave. (ext.) of 174.24 4 (1971BiZH) and 174.01 9 (2003ChZS) from (n,γ) E=thermal and 174.28 3 from β- decay, 1704.01 24 from (n,γ) E=thermal and 1705.6 3 from β- decay, and 1900.20 12 from (n,γ) E=thermal and 1899.7 3 from β- decay I(γ): weighted ave. (ext.) from (n,γ) E=thermal and β- decay branching ratios in Table IV of 1980Hu10 M(γ): d,E2 from comparison to RUL. E2 from ΔJ=2 |
1940.19 | 385.74 | E(γ): Multiply placed with undivided intensity. From (14C,nαγ). Identified as the same state in β- decay, (n,γ), and (d,pγ); however, based on the large discrepancy in the Eγ to the 5/2- between β- decay and (d,pγ) and (n,γ), the evaluator proposes two states I(γ): Multiply placed with undivided intensity. From (14C,nαγ) |
2249.10 | 349.11 | E(γ): From (n,γ) I(γ): From (n,γ) M(γ): d from comparison to RUL. M1 from Δπ=no | 814.51 | E(γ): From (n,γ) I(γ): From (n,γ) M(γ): d,E2 from comparison to RUL. M1 from ΔJπ|<1,no involving 1/2 state | 2074.71 | E(γ): From (n,γ) I(γ): From (n,γ) M(γ): d,E2 from comparison to RUL. E2 from ΔJ=2 |
2353.81 | 453.9 | M(γ): d,Q from comparison to RUL. E1,M2 from Δπ=yes. Probably not E1 since B(E1)|_(W.u.)=3.2×10-9 10 is ≈1 order of magnitude less than values previously compiled (Cf. Fig. 1 of 1979En04) | 919.3 | M(γ): d,Q from comparison to RUL. E1,M2 from Δπ=yes | 2179.4 | M(γ): d,Q,E3 from comparison to RUL. E1,M2 from ΔJπ|<2,yes. Probably not E1 since B(E1)|_(W.u.)=6.7×10-10 17 is ≈1 order of magnitude less than values previously compiled (Cf. Fig. 1 of 1979En04) | 2353.6 | M(γ): d,Q,E3 from comparison to RUL. Δπ=yes |
2392.29 | 492.5 | M(γ): d from comparison to RUL. E1 from Δπ=yes | 512 | M(γ): d from comparison to RUL. M1 from Δπ=no | 957.5 | M(γ): d,E2 from comparison to RUL. E1 from Δπ=yes | 2217.3 | M(γ): d,Q from comparison to RUL. M2 from Δπ=2,yes |
2675.1 | 2675 | E(γ): From (d,pγ) |
2842.05 | 942.7 | E(γ): From (n,γ) I(γ): From (n,γ) M(γ): From comparison to RUL | 957.8 | E(γ): From (n,γ) I(γ): From (n,γ) M(γ): d,E2 from comparison to RUL. E1 from Δπ=yes | 2667.7 | E(γ): From (n,γ) I(γ): From (n,γ) M(γ): From comparison to RUL | 2842.2 | E(γ): From (n,γ) I(γ): From (n,γ) M(γ): d,E2 from comparison to RUL. E2 from ΔJ=2 |
E(level) | E(gamma) | Comments |
2877.99 | 1323.60 | E(γ): From (14C,nαγ). Identified as the same state in β- decay, (n,γ), and (d,pγ); however, based on the large discrepancy in the Eγ to the 5/2- between β- decay and (d,pγ) and (n,γ), the evaluator proposes two states I(γ): From (14C,nαγ) M(γ): Q(+O) from γ(θ) in (14C,nαγ); stretched quadrupole cascade. E2(+M3) from ΔJπ=2,no |
2976.8 | 2802.4 | M(γ): From comparison to RUL | 2976.7 | M(γ): d,E2 from comparison to RUL. E2 from ΔJ=2 |
3241.27 | 565.6 | E(γ): From (n,γ) I(γ): From (n,γ) M(γ): From comparison to RUL | 992 | E(γ): From (d,pγ) | 3066.9 | E(γ): From (n,γ) I(γ): From (n,γ) M(γ): From comparison to RUL | 3241 | E(γ): From (d,pγ) |
3418.46 | 576.4 | E(γ): From (n,γ) I(γ): From (n,γ) M(γ): d from comparison to RUL. M1 from Δπ=no | 1026.0 | E(γ): From (n,γ) I(γ): From (n,γ) M(γ): d,E2 from comparison to RUL. E1 from Δπ=yes | 1169.66 | E(γ): From (n,γ) I(γ): From (n,γ) M(γ): d,E2 from comparison to RUL. M1 from ΔJπ|<1,no involving 1/2 state | 1983.7 | E(γ): From (n,γ) I(γ): From (n,γ) M(γ): d,E2 from comparison to RUL. M1 from ΔJπ|<1,no involving 1/2 state | 3243.5 | E(γ): From (n,γ) I(γ): From (n,γ) M(γ): d,E2 from comparison to RUL. E2 from ΔJ=2 |
3556.01 | 2001.48 | E(γ): Multiply placed with undivided intensity. From (14C,nαγ). Identified as the same state in β- decay, (n,γ), and (d,pγ); however, based on the large discrepancy in the Eγ to the 5/2- between β- decay and (d,pγ) and (n,γ), the evaluator proposes two states I(γ): Multiply placed with undivided intensity. From (14C,nαγ) |
3783.22 | 3609.3 | E(γ): From (n,γ) I(γ): From (n,γ) M(γ): From comparison to RUL |
3838.00 | 1938.1 | E(γ): From (n,γ) I(γ): From (n,γ) M(γ): d,E2 from comparison to RUL. M1 from (1/2)-|)3/2- | 2403.3 | E(γ): From (n,γ) I(γ): From (n,γ) M(γ): d,E2 from comparison to RUL. M1 from (1/2)-|)3/2- |
3941.83 | 385.74 | E(γ): Multiply placed with undivided intensity. From (14C,nαγ). Identified as the same state in β- decay, (n,γ), and (d,pγ); however, based on the large discrepancy in the Eγ to the 5/2- between β- decay and (d,pγ) and (n,γ), the evaluator proposes two states I(γ): Multiply placed with undivided intensity. From (14C,nαγ) | 1063.83 | E(γ): From (14C,nαγ). Identified as the same state in β- decay, (n,γ), and (d,pγ); however, based on the large discrepancy in the Eγ to the 5/2- between β- decay and (d,pγ) and (n,γ), the evaluator proposes two states I(γ): From (14C,nαγ) | 2001.48 | E(γ): Multiply placed with undivided intensity. From (14C,nαγ). Identified as the same state in β- decay, (n,γ), and (d,pγ); however, based on the large discrepancy in the Eγ to the 5/2- between β- decay and (d,pγ) and (n,γ), the evaluator proposes two states I(γ): Multiply placed with undivided intensity. From (14C,nαγ) |
4615.72 | 2716.0 | E(γ): From (n,γ) I(γ): From (n,γ) M(γ): d,E2 from comparison to RUL. M1 from (1/2)-|)3/2- | 3180.8 | E(γ): From (n,γ) I(γ): From (n,γ) M(γ): d,E2 from comparison to RUL. M1 from (1/2)-|)3/2- |
4999.74 | 2608.2 | E(γ): From (n,γ) I(γ): From (n,γ) | 3099.7 | E(γ): From (n,γ) I(γ): From (n,γ) | 3565.0 | E(γ): From (n,γ) I(γ): From (n,γ) |
Levels: Resonance properties: see 2006MuZX
Gammas: See β- decay and (pol n,γ),(n,γ) for unplaced γ’s
Q-value: Note: Current evaluation has used the following Q record 255.8 8 7414.79 1712290 40-10169.45 2003Au03