ADOPTED LEVELS, GAMMAS for 49Sc
Author: T. W. Burrows | Citation: Nucl. Data Sheets 109, 1879 (2008) | Cutoff date: 14-Jul-2008
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=2002 keV 3 | S(n)= 10129 keV 6 | S(p)= 9625 keV 3 | Q(α)= -12370 keV 3 | ||
Reference: 2012WA38 |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
0.0 | ABCDEFGHIJ | 7/2- | 57.18 m 13 % β- = 100 | |||||
2228.63 22 | A C EFGH J | 1/2+ | 29.9 ns 11 | 2228.75 35 | 100 | [E3] | 0.0 | 7/2- |
2371.82 22 | A CDEFGH J | 3/2+ | 1.40 ns 9 | 143.2 2 2371.75 35 | 5.6 6 100 3 | (M1,E2) [M2] | 2228.63 0.0 | 1/2+ 7/2- |
3084.52 10 | ABCD FGH | 3/2- | 48 fs 29 | 712.6 856.1 5 3084.4 1 | 0.01 0.16 1 100.00 4 | (E1+(M2)) E2 | 2371.82 2228.63 0.0 | 3/2+ 1/2+ 7/2- |
3300? | J | |||||||
3516.7 4 | A C FGH | 3/2- | 1144.5 5 1288.4 5 | 100 25 67 25 | 2371.82 2228.63 | 3/2+ 1/2+ | ||
3521.7 7 | I | 3521.8 | | 0.0 | 7/2- | |||
3550? | J | (3/2+,5/2+) | ||||||
3581 10 | F | 7/2- | ||||||
3755 8 | F J | 3/2+,5/2+ | ||||||
3808.8 5 | BC FGH | 7/2- | 21 fs 19 | 3808.6 5 | 100 | 0.0 | 7/2- | |
3914.9 8 | B FG I | (9/2-) | 393.1 3914.9 | | 3521.7 0.0 | 7/2- | ||
3951 10 | F | |||||||
3991.0 9 | BC FG J | 1/2+ | ≥ 0.7 ns | 1620.0 15 1762 | | 2371.82 2228.63 | 3/2+ 1/2+ | |
4046.5 8 | F I | (9/2-) | 525.2 4046.0 | | 3521.7 0.0 | 7/2- | ||
4072.04 10 | ABC FGH | 5/2- | 28 fs 14 | 987.3 5 4071.9 1 | 0.95 6 100.0 3 | D,E2 D,E2 | 3084.52 0.0 | 3/2- 7/2- |
4192 10 | F | (11/2-) | ||||||
4220 8 | F | |||||||
4239.6 13 | I | 324.7 | | 3914.9 | (9/2-) | |||
4267 10 | F | (15/2-) | ||||||
4285 8 | F | (5/2+) | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
4332.2 10 | AB FG | 5/2- | 4332.0 | 100 | 0.0 | 7/2- | ||
4426 10 | F J | |||||||
4459 10 | F J | |||||||
4493.44 22 | ABC FGH J | 1/2- | ≤ 23 fs | 976.7 1408.9 2 2264.7 | 1.25 40 100.0 17 7.0 12 | D+Q | 3516.7 3084.52 2228.63 | 3/2- 3/2- 1/2+ |
4579 8 | B F J | 1/2-,3/2- | ||||||
4714.8 8 | A F | 1/2-,3/2- | 2486.3 4714.4 | 100 26 16 5 | 2228.63 0.0 | 1/2+ 7/2- | ||
4738.45 20 | ABC FG | 5/2- | ≤ 14 fs | 4738.2 2 | 100 | D,E2 | 0.0 | 7/2- |
4810 8 | F | 5/2-,7/2- | ||||||
4948 8 | F | (1/2-,3/2-) | ||||||
4987 10 | B F J | (3/2+,5/2+) | ||||||
5015 8 | B F | 1/2-,3/2- | ||||||
5022 10 ? | B F H | (1/2+) | ||||||
5030 | GH | 3/2- | ||||||
5077 8 | B FGH | 5/2- | ||||||
5142 10 | AB F | |||||||
5229 10 | A F | (9/2-,11/2-) | ||||||
5230 8 | A F J | 3/2+,5/2+ | ||||||
5269 10 | F J | |||||||
5376.3 5 | BC FGH | 5/2- | 21 fs 10 | 5376.0 5 | | 0.0 | 7/2- | |
5438 8 | F | |||||||
5460 10 | F | |||||||
5562 10 | F | (9/2-,11/2-) | ||||||
5578 8 | F J | 3/2+,5/2+ | ||||||
5632 10 | B F | (17/2+) | ||||||
5663 8 | B FG | 3/2- | ||||||
5735 10 | F | (15/2-) | ||||||
5815 8 | B FGH | 1/2- | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
5845 8 | F | |||||||
5930? | H | |||||||
5979 10 | F | |||||||
6010.7 11 | ABC F | ≤ 50 fs | 6010.3 11 | | (D,E2) | 0.0 | 7/2- | |
6014 20 | AB F | |||||||
6069 20 | A F | (3/2+,5/2+) | ||||||
6180 20 | F | 3/2+,5/2+ | ||||||
6212 10 | F J | |||||||
6250 20 | F | (7/2+) | ||||||
6266 20 | F J | |||||||
6306 2 | C F | 5/2- | 3225 6307 | | 3084.52 0.0 | 3/2- 7/2- | ||
6330 10 | F J | |||||||
6415.5 4 | C FG | 7/2- | 21 fs 9 | 6415.4 5 | 100 | D,E2 | 0.0 | 7/2- |
6451 10 | F J | |||||||
6504.5 5 | C F J | 3/2 | 2436 4275 | 100 40 53 47 | 4072.04 2228.63 | 5/2- 1/2+ | ||
6527 20 | F | |||||||
6624 10 | F | |||||||
6685 20 | F J | |||||||
6728 2 | C F J | 3/2- | 3640 | 100 | 3084.52 | 3/2- | ||
6745 10 | F J | |||||||
6816 20 | F J | 1/2-,3/2- | ||||||
6829 10 | B F J | 5/2-,7/2- | ||||||
6867 10 | B F J | |||||||
6910 20 | F | (1/2+) | ||||||
6917 10 | F | |||||||
6939 10 | F | |||||||
6985.8 4 | C F | 5/2- | ≤ 14 fs | 4614.6 5 6984 | 100 27 26 12 | (E1) | 2371.82 0.0 | 3/2+ 7/2- |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
7026 20 | F J | 1/2-,3/2- | ||||||
7041 10 | F J | |||||||
7059 20 | F J | 7/2+,9/2+ | ||||||
7062.5 5 | C F J | 1/2- | 3978 4688 | 92 43 100 43 | 3084.52 2371.82 | 3/2- 3/2+ | ||
7151 20 | F J | 5/2-,7/2- | ||||||
7172 10 | F J | |||||||
7186 20 | F J | (7/2+,9/2+) | ||||||
7193 2 | C J | 5/2 | ||||||
7228.8 6 | C F J | 5/2 | 7224 | 100 | 0.0 | 7/2- | ||
7253 20 | F | 1/2-,3/2- | ||||||
7293 10 | F J | |||||||
7320 20 | F | 1/2-,3/2- | ||||||
7342 20 | F | 5/2-,7/2- | ||||||
7375 20 | F | 5/2-,7/2- | ||||||
7421 20 | F | 5/2-,7/2- | ||||||
7442 20 | F | 1/2-,3/2- | ||||||
7483 20 | F | 5/2-,7/2- | ||||||
7500 20 | F | 1/2-,3/2- | ||||||
7529 20 | F | (7/2+,9/2+) | ||||||
7583 20 | F J | (3/2+,5/2+) | ||||||
7653 20 | F | 1/2-,3/2- | ||||||
7678 20 | F | (7/2+,9/2+) | ||||||
7723 20 | F | 1/2-,3/2- | ||||||
7746 20 | F | (7/2+,9/2+) | ||||||
7795 20 | F | (7/2+,9/2+) | ||||||
7832 20 | F | 1/2-,3/2- | ||||||
7890 20 | F | 1/2-,3/2- | ||||||
7940 20 | F | |||||||
7998 20 | F | 1/2-,3/2- | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
8029 20 | F | |||||||
8094 20 | F | 1/2-,3/2- | ||||||
8147 20 | F | 1/2-,3/2- | ||||||
8177 20 | F | (7/2+,9/2+) | ||||||
8200 20 | F | 1/2-,3/2- | ||||||
8246 20 | F | |||||||
8289 20 | F | 1/2-,3/2- | ||||||
8330 20 | F | 5/2-,7/2- | ||||||
8355 20 | F | 1/2-,3/2- | ||||||
8434 20 | F | 1/2-,3/2- | ||||||
8465 20 | F | 5/2-,7/2- | ||||||
8625 20 | F J | |||||||
8693 20 | F J | 3/2+,5/2+ | ||||||
8721 20 | F | 1/2-,3/2- | ||||||
8751 20 | F | |||||||
8781 20 | F | 1/2-,3/2- | ||||||
8813 20 | F | 1/2-,3/2- | ||||||
8848 20 | F | 1/2-,3/2- | ||||||
8900 20 | F | 3/2+,5/2+ | ||||||
8929 20 | F | 5/2-,7/2- | ||||||
8971 20 | F | (7/2+,9/2+) | ||||||
9008 20 | F | 3/2+,5/2+ | ||||||
9066 20 | F | 5/2-,7/2- | ||||||
9117 20 | F J | 3/2+,5/2+ | ||||||
9145 20 | F | (1/2-,3/2-) | ||||||
9185 20 | F | (5/2-,7/2-) | ||||||
9218 20 | F J | |||||||
9247 20 | F | 1/2-,3/2- | ||||||
9295 20 | F | 1/2-,3/2- | ||||||
9335 20 | F J | |||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
9385 20 | F | 1/2-,3/2- | ||||||
9449 20 | F | 5/2-,7/2- | ||||||
9514 20 | F | 5/2-,7/2- | ||||||
9575 20 | F | 1/2-,3/2- | ||||||
9634 20 | F | 1/2-,3/2- | ||||||
9675 20 | F | 1/2-,3/2- | ||||||
9726 20 | F | 1/2-,3/2- | ||||||
9790 20 | F | 1/2-,3/2- | ||||||
9843 20 | F | 1/2-,3/2- | ||||||
9873 20 | F | 1/2-,3/2- | ||||||
9923 20 | F | 1/2-,3/2- | ||||||
9956 20 | F | 5/2-,7/2- | ||||||
9991 20 | F | 1/2-,3/2- | ||||||
10059 20 | F | 1/2-,3/2- | ||||||
10155 20 | F | 5/2-,7/2- | ||||||
10212 20 | F | |||||||
10413 20 | F | 1/2-,3/2- | ||||||
10473 20 | F | 1/2-,3/2- | ||||||
10569 | E | 8340 | | 2228.63 | 1/2+ | |||
10617 20 | F | 1/2-,3/2- | ||||||
10690 20 | EF | 1/2-,3/2- | 8318 | | 2371.82 | 3/2+ | ||
10787 20 | F | (1/2-,3/2-) | ||||||
10870 20 | F | (1/2-,3/2-) | ||||||
10957 20 | F | (1/2-,3/2-) | ||||||
11021 20 | F | (1/2-,3/2-) | ||||||
11030 20 | F | (1/2-,3/2-) | ||||||
11138 20 | F | (1/2-,3/2-) | ||||||
11271 20 | F | (1/2-,3/2-) | ||||||
11425 20 | F | 3/2+,5/2+ | ||||||
11510 20 ? | F | |||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
11525 4 | E | 1/2- | ||||||
11534 4 | E | 1/2+ | ||||||
11538 3 | C | (3/2-) | ||||||
11543 3 | E | |||||||
11547 3 | C | 3/2- | 4354 4484 4561 4819 5042 5131 5241 6808 7475 8030 8462 9175 9318 | 44 19 78 19 100 27 57 19 59 19 72 19 35 19 50 13 41 13 9 9 15 6 73 27 35 7 | 7193 7062.5 6985.8 6728 6504.5 6415.5 6306 4738.45 4072.04 3516.7 3084.52 2371.82 2228.63 | 5/2 1/2- 5/2- 3/2- 3/2 7/2- 5/2- 5/2- 5/2- 3/2- 3/2- 3/2+ 1/2+ | ||
11548 3 | E | |||||||
11552 3 | C F | 3/2- | 4359 4489 4566 4824 5047 5136 5246 6813 7480 7561 8035 8467 9180 9323 | 43 10 57 8 100 10 67 10 50 10 67 10 29 8 21 5 35 5 9 5 12 8 16.4 23 43 15 17.0 23 | 7193 7062.5 6985.8 6728 6504.5 6415.5 6306 4738.45 4072.04 3991.0 3516.7 3084.52 2371.82 2228.63 | 5/2 1/2- 5/2- 3/2- 3/2 7/2- 5/2- 5/2- 5/2- 1/2+ 3/2- 3/2- 3/2+ 1/2+ | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
11563.2 4 | C F | 3/2- | 1.5 keV 3 % p = 79 6 % IT = 0.31 7 % n = 21 14 | 4333.1 5 4370.2 4500.7 5 4577.8 5 4835.2 5059.1 5 5147.7 5 5257.2 6824.8 7491.2 7572.2 7754.4 8041.5 8478.7 9191.4 9334.6 11563.2 | 44.4 14 41 8 55 7 100 9 72 10 90 10 48 8 11 6 30 5 43 5 24 7 24 10 10 4 5.9 27 9.8 27 13.7 13 20.9 20 | D+Q D+Q D+Q D+Q D+Q D+Q E2(+M3) D+Q D+Q D+Q (E1(+M2)) E2(+M3) D+Q D+Q (E1(+M2)) (E1+M2) (E2+M3) | 7228.8 7193 7062.5 6985.8 6728 6504.5 6415.5 6306 4738.45 4072.04 3991.0 3808.8 3521.7 3084.52 2371.82 2228.63 0.0 | 5/2 5/2 1/2- 5/2- 3/2- 3/2 7/2- 5/2- 5/2- 5/2- 1/2+ 7/2- 3/2- 3/2+ 1/2+ 7/2- |
11569 3 | C F | (3/2-) | % p ≈ 50 % n ≈ 50 | |||||
11579 3 | C | (3/2-) | 0.29 keV 14 % n = 86 13 % p = 14 13 | |||||
11583 3 | C | (3/2-) | 0.17 keV 8 % n = 88 12 % p = 12 12 | |||||
11665 20 | F | 1/2-,3/2- | ||||||
11735 20 | F | |||||||
11806 20 | F | |||||||
11911 20 | F | 1/2-,3/2- | ||||||
11976 20 | F | 1/2-,3/2- | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
12040 40 | F | 1/2-,3/2- | ||||||
12098 40 | F | |||||||
12160 40 | F | |||||||
12216 40 | F | |||||||
12281 40 | F | |||||||
12340 40 | F | |||||||
12390 40 | F | |||||||
12497 40 | F | |||||||
12607 40 | F | |||||||
12732 40 | F | |||||||
12829 40 | F | |||||||
12893 40 | F | |||||||
12992 40 | F | |||||||
13119 40 | F | |||||||
13204 40 | F | |||||||
13308 40 | F | |||||||
13358 40 | F | |||||||
13412 40 | F | |||||||
13487 40 | F | (1/2-) | ||||||
13557 40 | F | (1/2)- | ||||||
13572 5 | D F | (1/2)- | 226 keV 3 % n = 23.0 5 % p = 66.4 12 | |||||
15108 10 | D F | 5/2- | 12.8 keV 13 | |||||
15481 10 | D | (3/2)- | 19.3 keV 20 | 15481 | | 0.0 | 7/2- | |
15544 4 | E | 15544 | | 0.0 | 7/2- | |||
15563 6 | D F | 5/2- | 31 keV 8 | 12478 13191 15563 | | D,E2 (E1(+M2)) D,E2 | 3084.52 2371.82 0.0 | 3/2- 3/2+ 7/2- |
15583 4 | E | 15583 | | 0.0 | 7/2- | |||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
15600 4 | E | 15600 | | 0.0 | 7/2- | |||
15622 6 | D F | 9/2+ | 18 keV 5 | 15622 | | (E1(+M2)) | 0.0 | 7/2- |
15662 4 | E | 15662 | | 0.0 | 7/2- | |||
15878 10 | D | 3/2+ | 19.8 keV 20 | |||||
16025 10 | D | 5/2+ | 25.6 keV 26 | |||||
16509 10 | D F | 7/2+ | 14.8 keV 15 | |||||
16994 10 | D F | 9/2+ | 18.8 keV 19 | |||||
17662 10 | D F | 5/2+ | 108 keV 11 | |||||
18152 | D F | 3/2+,5/2+ | ||||||
18348 | D F | 3/2+,5/2+ |
E(level): From (d,n),(3He,d),(α,t)..., except as noted in the comments, footnotes or XREF column
Jπ(level): From angular momentum transfer in (d,n),(3He,d),(α,t)..., except as noted.
T1/2(level): T1/2’s from DSAM in (p,Xγ) IAR: 49Ca g.s. and Γ’s from (p,X): 49Ca other IAR’s, except as noted.
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
2228.63 | 1/2+ | 29.9 ns 11 | 2228.75 35 | [E3] | 0.000284 | B(E3)(W.u.)=1.04 4, α=0.000284 4, α(K)=2.85E-5 4, α(L)=2.50E-6 4, α(M)=3.09E-7 5, α(N)=1.740E-8 25, α(N+)=0.000252 4 | |
2371.82 | 3/2+ | 1.40 ns 9 | 143.2 2 | (M1,E2) | 0.04 | α=0.04 4, α(K)=0.04 4, α(L)=0.003 3, α(M)=0.0004 4, α(N)=2.2×10-5 19, α(N+)=2.2E-5 19 | |
3/2+ | 1.40 ns 9 | 2371.75 35 | [M2] | 0.000275 | B(M2)(W.u.)=0.0208 16, α=0.000275 4, α(K)=2.46×10-5 4, α(L)=2.15E-6 3, α(M)=2.67E-7 4, α(N)=1.503E-8 21, α(N+)=0.000248 4 | ||
3084.52 | 3/2- | 48 fs 29 | 856.1 5 | (E1+(M2)) | 0.082 LE | 0.00016 | B(E1)(W.u.)=2.3E-5 15, α=0.00016 10, α(K)=0.00014 9, α(L)=1.3E-5 8, α(M)=1.6E-6 10, α(N)=9.E-8 6, α(N+)=9.E-8 6 |
3/2- | 48 fs 29 | 3084.4 1 | E2 | 0.000831 | B(E2)(W.u.)=4.0 24, α=0.000831 12, α(K)=1.070E-5 15, α(L)=9.34E-7 13, α(M)=1.159E-7 17, α(N)=6.53E-9 10, α(N+)=0.000820 12 | ||
6985.8 | 5/2- | ≤ 14 fs | 4614.6 5 | (E1) | 0.00190 | B(E1)(W.u.)>0.00029, α=0.00190 3, α(K)=4.42E-6 7, α(L)=3.85E-7 6, α(M)=4.78E-8 7, α(N)=2.69E-9 4, α(N+)=0.00189 3 | |
11563.2 | 3/2- | 1.5 keV 3 % p = 79 6 % IT = 0.31 7 % n = 21 14 | 5147.7 5 | E2(+M3) | 0.001534 LE | 0.0012 | B(E2)(W.u.)=16.109 18, α=0.0012 3, α(K)=6.6E-6 16, α(L)=5.7E-7 14, α(M)=7.1E-8 17, α(N)=4.0E-9 10, α(N+)=0.0012 3 |
3/2- | 1.5 keV 3 % p = 79 6 % IT = 0.31 7 % n = 21 14 | 7572.2 | (E1(+M2)) | 0.276 LE | B(E1)(W.u.)=0.000169 5 | ||
3/2- | 1.5 keV 3 % p = 79 6 % IT = 0.31 7 % n = 21 14 | 7754.4 | E2(+M3) | B(E2)(W.u.)=0.308 12 | |||
3/2- | 1.5 keV 3 % p = 79 6 % IT = 0.31 7 % n = 21 14 | 9191.4 | (E1(+M2)) | -0.20 | B(E1)(W.u.)>5.025E-5 4 LT 6 | ||
3/2- | 1.5 keV 3 % p = 79 6 % IT = 0.31 7 % n = 21 14 | 9334.6 | (E1+M2) | +0.07 3 | B(E1)(W.u.)=0.00010 3, B(M2)(W.u.)=0.026 24 | ||
3/2- | 1.5 keV 3 % p = 79 6 % IT = 0.31 7 % n = 21 14 | 11563.2 | (E2+M3) | +0.09 5 | B(E2)(W.u.)=0.041 13, B(M3)(W.u.)=17 +20-17 | ||
15563 | 5/2- | 31 keV 8 | 13191 | (E1(+M2)) | 0.236 LE | B(E1)(W.u.)=0.000657 19 | |
15622 | 9/2+ | 18 keV 5 | 15622 | (E1(+M2)) | 0.092 LE | B(E1)(W.u.)=0.006 4 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
2228.63 | 1/2+ | 29.9 ns 11 | E(level): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. |
2371.82 | 3/2+ | 1.40 ns 9 | E(level): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. From β- decay. Jπ(level): From angular momentum transfer in (d,n),(3He,d),(α,t)... And primary γ(θ) in (p,Xγ) IAR: 49Ca g.s. |
3084.52 | 3/2- | 48 fs 29 | E(level): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. |
3300 | E(level): Existence considered doubtful due to energy resolution (FWHM=100-115 keV) in (d,3He) and lack of observance in other reactions. | ||
3516.7 | 3/2- | E(level): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. From β- decay. Jπ(level): From angular momentum transfer in (d,n),(3He,d),(α,t)... And primary γ(θ) in (p,Xγ) IAR: 49Ca g.s. | |
3550 | (3/2+,5/2+) | E(level): Existence considered doubtful due to energy resolution (FWHM=100-115 keV) in (d,3He) and lack of observance in other reactions. Jπ(level): From angular momentum transfer in (d,3He). Parentheses added by evaluator due to energy resolution (FWHM=100-115 keV). | |
3808.8 | 7/2- | 21 fs 19 | E(level): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. Jπ(level): From angular momentum in transfer (d,n),(3He,d),(α,t)... And characteristic shape of σ(θ) in (7Li,6He). Note that these results sometimes differ from what would Be expected from the dominant no-recoil L transfer in (15N,14C). See comment by evaluator in this table. |
3914.9 | (9/2-) | E(level): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. Jπ(level): Tentative assignment based on coupled-reaction-channel analysis of (α,t). See this dataset for the configurations. | |
3991.0 | 1/2+ | ≥ 0.7 ns | E(level): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. |
4046.5 | (9/2-) | E(level): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. Jπ(level): Tentative assignment based on coupled-reaction-channel analysis of (α,t). See this dataset for the configurations. | |
4072.04 | 5/2- | 28 fs 14 | E(level): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. Jπ(level): From angular momentum in transfer (d,n),(3He,d),(α,t)... And characteristic shape of σ(θ) in (7Li,6He). Note that these results sometimes differ from what would Be expected from the dominant no-recoil L transfer in (15N,14C). See comment by evaluator in this table. |
4192 | (11/2-) | Jπ(level): Tentative assignment based on coupled-reaction-channel analysis of (α,t). See this dataset for the configurations. | |
4267 | (15/2-) | Jπ(level): Tentative assignment based on coupled-reaction-channel analysis of (α,t). See this dataset for the configurations. | |
4285 | (5/2+) | Jπ(level): Tentative assignment based on coupled-reaction-channel analysis of (α,t). See this dataset for the configurations. | |
4332.2 | 5/2- | E(level): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. Jπ(level): From angular momentum in transfer (d,n),(3He,d),(α,t)... And characteristic shape of σ(θ) in (7Li,6He). Note that these results sometimes differ from what would Be expected from the dominant no-recoil L transfer in (15N,14C). See comment by evaluator in this table. | |
4493.44 | 1/2- | ≤ 23 fs | E(level): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. Jπ(level): From angular momentum in transfer (d,n),(3He,d),(α,t)... And characteristic shape of σ(θ) in (7Li,6He). Note that these results sometimes differ from what would Be expected from the dominant no-recoil L transfer in (15N,14C). See comment by evaluator in this table. |
4714.8 | 1/2-,3/2- | E(level): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. | |
4738.45 | 5/2- | ≤ 14 fs | E(level): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. Jπ(level): From angular momentum in transfer (d,n),(3He,d),(α,t)... And characteristic shape of σ(θ) in (7Li,6He). Note that these results sometimes differ from what would Be expected from the dominant no-recoil L transfer in (15N,14C). See comment by evaluator in this table. |
4987 | (3/2+,5/2+) | XREF: J(4860). | |
5230 | 3/2+,5/2+ | E(level): From (48Ca,Xγ). Jπ(level): L(d,3He)=2 for multiplet. | |
5269 | E(level): From (48Ca,Xγ). Jπ(level): L(d,3He)=2 for multiplet. | ||
5376.3 | 5/2- | 21 fs 10 | E(level): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. Jπ(level): From angular momentum in transfer (d,n),(3He,d),(α,t)... And characteristic shape of σ(θ) in (7Li,6He). Note that these results sometimes differ from what would Be expected from the dominant no-recoil L transfer in (15N,14C). See comment by evaluator in this table. |
5632 | (17/2+) | Jπ(level): Tentative assignment based on coupled-reaction-channel analysis of (α,t). See this dataset for the configurations. | |
5663 | 3/2- | Jπ(level): From angular momentum in transfer (d,n),(3He,d),(α,t)... And characteristic shape of σ(θ) in (7Li,6He). Note that these results sometimes differ from what would Be expected from the dominant no-recoil L transfer in (15N,14C). See comment by evaluator in this table. | |
5735 | (15/2-) | Jπ(level): Tentative assignment based on coupled-reaction-channel analysis of (α,t). See this dataset for the configurations. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
5815 | 1/2- | Jπ(level): From angular momentum in transfer (d,n),(3He,d),(α,t)... And characteristic shape of σ(θ) in (7Li,6He). Note that these results sometimes differ from what would Be expected from the dominant no-recoil L transfer in (15N,14C). See comment by evaluator in this table. | |
6010.7 | ≤ 50 fs | E(level): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. | |
6212 | E(level): From (48Ca,Xγ). Jπ(level): L(d,3He)=2 for multiplet. | ||
6250 | (7/2+) | Jπ(level): Tentative assignment based on coupled-reaction-channel analysis of (α,t). See this dataset for the configurations. | |
6266 | E(level): From (48Ca,Xγ). Jπ(level): L(d,3He)=2 for multiplet. | ||
6306 | 5/2- | E(level): From β- decay. Jπ(level): From angular momentum transfer in (d,n),(3He,d),(α,t)... And primary γ(θ) in (p,Xγ) IAR: 49Ca g.s. | |
6330 | E(level): From (48Ca,Xγ). Jπ(level): L(d,3He)=2 for multiplet. | ||
6415.5 | 7/2- | 21 fs 9 | E(level): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. From β- decay. Jπ(level): From angular momentum transfer in (d,n),(3He,d),(α,t)... And primary γ(θ) in (p,Xγ) IAR: 49Ca g.s. |
6451 | E(level): From (48Ca,Xγ). Jπ(level): L(d,3He)=2 for multiplet. | ||
6504.5 | 3/2 | XREF: F(6476). E(level): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. From (48Ca,Xγ). Jπ(level): L(d,3He)=2 for multiplet. | |
6728 | 3/2- | E(level): From β- decay. From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Jπ(level): From angular momentum transfer in (d,n),(3He,d),(α,t)... And primary γ(θ) in (p,Xγ) IAR: 49Ca g.s. | |
6985.8 | 5/2- | ≤ 14 fs | E(level): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. |
7062.5 | 1/2- | E(level): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. | |
7172 | E(level): From (48Ca,Xγ). Jπ(level): L(d,3He)=2 for multiplet. | ||
7186 | (7/2+,9/2+) | May correspond to 7193 state if L in (d,n),(3He,d),(α,t),... incorrect. | |
7193 | 5/2 | E(level): From (48Ca,Xγ). Jπ(level): L(d,3He)=2 for multiplet. | |
7228.8 | 5/2 | E(level): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. From (48Ca,Xγ). Jπ(level): L(d,3He)=2 for multiplet. | |
7293 | E(level): From (48Ca,Xγ). Jπ(level): L(d,3He)=2 for multiplet. | ||
7583 | (3/2+,5/2+) | Jπ(level): From angular momentum transfer in (d,3He). Parentheses added by evaluator due to energy resolution (FWHM=100-115 keV). | |
8625 | E(level): From (48Ca,Xγ). Jπ(level): L(d,3He)=2 for multiplet. | ||
8693 | 3/2+,5/2+ | E(level): From (48Ca,Xγ). Jπ(level): L(d,3He)=2 for multiplet. | |
9117 | 3/2+,5/2+ | E(level): From (48Ca,Xγ). Jπ(level): L(d,3He)=2 for multiplet. | |
9218 | E(level): From (48Ca,Xγ). Jπ(level): L(d,3He)=2 for multiplet. | ||
9335 | E(level): From (48Ca,Xγ). Jπ(level): L(d,3He)=2 for multiplet. | ||
10569 | E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. | ||
E(level) | Jπ(level) | T1/2(level) | Comments |
11510 | May correspond to 11525 state if L(d,n),(3He,d),(α,t) incorrect. | ||
11525 | 1/2- | E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. | |
11534 | 1/2+ | E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. | |
11538 | (3/2-) | Γp=50 50, Γn=70 70 E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s. Jπ(level): From analysis of elastic scattering excitation functions. | |
11543 | Γp=20 20, Γn=30 30 E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. | ||
11547 | 3/2- | Γp=0.10 5, Γn=0.40 20 E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s. Jπ(level): From analysis of elastic scattering excitation functions. | |
11548 | Γp=30 30, Γn=30 30 E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. | ||
11552 | 3/2- | Γp=0.40 10, Γn=0.22 6 E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s. Jπ(level): From analysis of elastic scattering excitation functions. | |
11563.2 | 3/2- | 1.5 keV 3 % p = 79 6 % IT = 0.31 7 % n = 21 14 | Γγ=4.8 5, Γp=1.2 3, Γn=0.32 8 E(level): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s. Jπ(level): From analysis of elastic scattering excitation functions. |
11569 | (3/2-) | % p ≈ 50 % n ≈ 50 | Γp=50 eV 50 or 70 eV 70; Γn=50 eV 50 or 100 eV 50. E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s. Jπ(level): From analysis of elastic scattering excitation functions. |
11579 | (3/2-) | 0.29 keV 14 % n = 86 13 % p = 14 13 | Γp=40 40, Γn=0.25 13 E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s. Jπ(level): From analysis of elastic scattering excitation functions. |
11583 | (3/2-) | 0.17 keV 8 % n = 88 12 % p = 12 12 | Γp=20 20, Γn=0.15 8 E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s. Jπ(level): From analysis of elastic scattering excitation functions. |
12098 | Jπ(level): See (d,n),(3He,d),(α,t)... For L to states between 12098 and 13412. | ||
12160 | Jπ(level): See (d,n),(3He,d),(α,t)... For L to states between 12098 and 13412. | ||
12216 | Jπ(level): See (d,n),(3He,d),(α,t)... For L to states between 12098 and 13412. | ||
12281 | Jπ(level): See (d,n),(3He,d),(α,t)... For L to states between 12098 and 13412. | ||
12340 | Jπ(level): See (d,n),(3He,d),(α,t)... For L to states between 12098 and 13412. | ||
12390 | Jπ(level): See (d,n),(3He,d),(α,t)... For L to states between 12098 and 13412. | ||
12497 | Jπ(level): See (d,n),(3He,d),(α,t)... For L to states between 12098 and 13412. | ||
12607 | Jπ(level): See (d,n),(3He,d),(α,t)... For L to states between 12098 and 13412. | ||
12732 | Jπ(level): See (d,n),(3He,d),(α,t)... For L to states between 12098 and 13412. | ||
12829 | Jπ(level): See (d,n),(3He,d),(α,t)... For L to states between 12098 and 13412. | ||
12893 | Jπ(level): See (d,n),(3He,d),(α,t)... For L to states between 12098 and 13412. | ||
12992 | Jπ(level): See (d,n),(3He,d),(α,t)... For L to states between 12098 and 13412. | ||
13119 | Jπ(level): See (d,n),(3He,d),(α,t)... For L to states between 12098 and 13412. | ||
E(level) | Jπ(level) | T1/2(level) | Comments |
13204 | Jπ(level): See (d,n),(3He,d),(α,t)... For L to states between 12098 and 13412. | ||
13308 | Jπ(level): See (d,n),(3He,d),(α,t)... For L to states between 12098 and 13412. | ||
13358 | Jπ(level): See (d,n),(3He,d),(α,t)... For L to states between 12098 and 13412. | ||
13412 | Jπ(level): See (d,n),(3He,d),(α,t)... For L to states between 12098 and 13412. | ||
13487 | (1/2-) | E(level): Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s. | |
13557 | (1/2)- | E(level): Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s. | |
13572 | (1/2)- | 226 keV 3 % n = 23.0 5 % p = 66.4 12 | Γp=151 2, Γn=52 1 E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s. |
15108 | 5/2- | 12.8 keV 13 | E(level): Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s. Jπ(level): L=3 in (d,n),(3He,d),(α,t)... and (p,p). (p,p’) to 48Ca 3832, 2+, indicates πp1/2 component. T1/2(level): See (p,Xγ): other 49Ca IAR’s for elastic and inelastic Γp. |
15481 | (3/2)- | 19.3 keV 20 | E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s. T1/2(level): See (p,Xγ): other 49Ca IAR’s for elastic and inelastic Γp. |
15544 | E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. | ||
15563 | 5/2- | 31 keV 8 | E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s. Jπ(level): L=3 in (d,n),(3He,d),(α,t)... and (p,p). (p,p’) to 48Ca 3832, 2+, indicates πp1/2 component. T1/2(level): See (p,Xγ): other 49Ca IAR’s for elastic and inelastic Γp. |
15583 | E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. | ||
15600 | E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. | ||
15622 | 9/2+ | 18 keV 5 | E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s. T1/2(level): See (p,Xγ): other 49Ca IAR’s for elastic and inelastic Γp. |
15662 | E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. | ||
15878 | 3/2+ | 19.8 keV 20 | E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s. T1/2(level): See (p,Xγ): other 49Ca IAR’s for elastic and inelastic Γp. |
16025 | 5/2+ | 25.6 keV 26 | E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s. T1/2(level): See (p,Xγ): other 49Ca IAR’s for elastic and inelastic Γp. |
16509 | 7/2+ | 14.8 keV 15 | E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s. T1/2(level): See (p,Xγ): other 49Ca IAR’s for elastic and inelastic Γp. |
16994 | 9/2+ | 18.8 keV 19 | E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s. T1/2(level): See (p,Xγ): other 49Ca IAR’s for elastic and inelastic Γp. |
17662 | 5/2+ | 108 keV 11 | E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s. T1/2(level): See (p,Xγ): other 49Ca IAR’s for elastic and inelastic Γp. |
18152 | 3/2+,5/2+ | E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s. | |
18348 | 3/2+,5/2+ | E(level): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s. |
E(level) | E(gamma) | Comments |
2228.63 | 2228.75 | E(γ): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis.. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. Existence considered doubtful due to energy resolution (FWHM=100-115 keV) in (d,3He) and lack of observance in other reactions I(γ): From β- decay. |
2371.82 | 143.2 | E(γ): From β- decay.. Existence considered doubtful due to energy resolution (FWHM=100-115 keV) in (d,3He) and lack of observance in other reactions I(γ): From β- decay. M(γ): d,E2 from comparison to RUL. Δπ=no from level scheme | 2371.75 | E(γ): Calculated using least-squares adjustment procedures, assuming ΔE(γ)=1 keV when not given. Only primary γ’s with a known ΔE(γ) were included in the analysis.. Weighted av (int.) of 2228.9 5 from β- decay and 2228.6 5 from (p,Xγ) and 2371.7 5 from β- decay and 2371.8 5 from (p,Xγ), respectively. Existence considered doubtful due to energy resolution (FWHM=100-115 keV) in (d,3He) and lack of observance in other reactions I(γ): From β- decay. |
3084.52 | 712.6 | E(γ): From β- decay.. Existence considered doubtful due to energy resolution (FWHM=100-115 keV) in (d,3He) and lack of observance in other reactions I(γ): From β- decay. | 856.1 | E(γ): From β- decay.. Existence considered doubtful due to energy resolution (FWHM=100-115 keV) in (d,3He) and lack of observance in other reactions I(γ): From β- decay. M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme | 3084.4 | E(γ): From β- decay.. Existence considered doubtful due to energy resolution (FWHM=100-115 keV) in (d,3He) and lack of observance in other reactions I(γ): From β- decay. M(γ): from γγ(θ) in β- decay and comparison to RUL |
3516.7 | 1144.5 | E(γ): From β- decay.. Existence considered doubtful due to energy resolution (FWHM=100-115 keV) in (d,3He) and lack of observance in other reactions I(γ): From β- decay. | 1288.4 | E(γ): From β- decay.. Existence considered doubtful due to energy resolution (FWHM=100-115 keV) in (d,3He) and lack of observance in other reactions I(γ): From β- decay. |
3521.7 | 3521.8 | E(γ): From (48Ca,Xγ) |
3914.9 | 393.1 | E(γ): From (48Ca,Xγ) | 3914.9 | E(γ): From (48Ca,Xγ) |
4046.5 | 525.2 | E(γ): From (48Ca,Xγ) | 4046.0 | E(γ): From (48Ca,Xγ) |
4072.04 | 987.3 | E(γ): From β- decay.. Existence considered doubtful due to energy resolution (FWHM=100-115 keV) in (d,3He) and lack of observance in other reactions I(γ): From β- decay. M(γ): From comparison to RUL | 4071.9 | E(γ): From β- decay.. Existence considered doubtful due to energy resolution (FWHM=100-115 keV) in (d,3He) and lack of observance in other reactions I(γ): From β- decay. M(γ): From comparison to RUL |
4239.6 | 324.7 | E(γ): From (48Ca,Xγ) |
4332.2 | 4332.0 | E(γ): From β- decay.. Existence considered doubtful due to energy resolution (FWHM=100-115 keV) in (d,3He) and lack of observance in other reactions I(γ): From β- decay. |
4493.44 | 976.7 | E(γ): From β- decay.. Existence considered doubtful due to energy resolution (FWHM=100-115 keV) in (d,3He) and lack of observance in other reactions I(γ): From β- decay. | 1408.9 | E(γ): From β- decay.. Existence considered doubtful due to energy resolution (FWHM=100-115 keV) in (d,3He) and lack of observance in other reactions I(γ): From β- decay. | 2264.7 | E(γ): From β- decay.. Existence considered doubtful due to energy resolution (FWHM=100-115 keV) in (d,3He) and lack of observance in other reactions I(γ): From β- decay. |
4714.8 | 2486.3 | E(γ): From β- decay.. Existence considered doubtful due to energy resolution (FWHM=100-115 keV) in (d,3He) and lack of observance in other reactions I(γ): From β- decay. | 4714.4 | E(γ): From β- decay.. Existence considered doubtful due to energy resolution (FWHM=100-115 keV) in (d,3He) and lack of observance in other reactions I(γ): From β- decay. |
4738.45 | 4738.2 | E(γ): From β- decay.. Existence considered doubtful due to energy resolution (FWHM=100-115 keV) in (d,3He) and lack of observance in other reactions I(γ): From β- decay. M(γ): From comparison to RUL |
6010.7 | 6010.3 | M(γ): from comparison to RUL if Iγ(6010γ)>17% |
6415.5 | 6415.4 | M(γ): From comparison to RUL |
E(level) | E(gamma) | Comments |
6985.8 | 4614.6 | M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme |
10569 | 8340 | E(γ): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies |
10690 | 8318 | E(γ): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies |
11563.2 | 7572.2 | M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme | 9191.4 | M(γ): d(+Q) from γ(θ). Δπ=yes from level scheme | 9334.6 | M(γ): D+Q from γ(θ). Δπ=no from level scheme | 11563.2 | M(γ): Q+O from γ(θ). Δπ=no from level scheme |
15481 | 15481 | E(γ): Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s |
15544 | 15544 | E(γ): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies |
15563 | 12478 | E(γ): Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s I(γ): From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s | 13191 | E(γ): Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s I(γ): From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme | 15563 | E(γ): Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s I(γ): From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s |
15583 | 15583 | E(γ): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies |
15600 | 15600 | E(γ): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies |
15622 | 15622 | E(γ): Isobaric analog states of 49Ca. See (p,X),(d,n),(3He,d),(α,t) for correspondence with parent states. From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s I(γ): From (p,Xγ): other 49Ca IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies. Γγ’s from (p,Xγ): other 49Ca IAR’s M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme |
15662 | 15662 | E(γ): From (p,X) and (p,Xγ) data. Resonance E(level)=(0.9798419 15)E(p)+S(p) with S(p)=9627.2 keV 29 (2003Au03). From (p,Xγ) res: non-IAR’s. Nominal energies calculated by the evaluator from the adopted excitation energies |
Levels: Resonance parameters: see data cited below in (p,X), (p,Xγ), and (d,n),(3He,d),(α,t)... Tables
Levels: Γp,Γn: from (p,X) and (p,Xγ). By one-channel multilevel and Breit-Wigner analysis for 49Ca g.s. IAS’s and non-IAR resonances (1972Ga09) and by analysis of the average resonance shape for the 49Ca 2023 IAS (1982Si19)
Gammas: See (p,Xγ) IAR: 49Ca g.s. for unplaced gammas
Gammas: B(E|l)(W.u.),B(M|l)(W.u.): calculated using adopted T1/2’s and γ-ray properties for secondary gammas. Primary Γγ’s were used for transitions from the 1974 resonance
Gammas: Γγ’s: from (p,Xγ) IAR: 49Ca g.s., except as noted as a a footnote on Iγ.
Q-value: Note: Current evaluation has used the following Q record 2006 4 10128 6 9627.2 29 -12369 11 2003Au03