TABLE IV: Excitation energies, γ and laboratory proton energies, branching ratios (averages from the present work, Borge et al. [8], and Schardt et al. [9]), individual B(GT) values and the summed B(GT). In cases, where the excitation energy is missing for the present work, the proton is emitted from the same level as the proton in the previous line. Proton energies labeled with # are due to protons populating the first excited state, whereas proton energies labeled with ## are due to protons populating the second excited state. Shell-model values for the excitation energies and the branching ratios are given for levels below the IAS. They were obtained using the USD effective interaction [21]. The excitation energies determined in the present work are E$_{x}$ (keV) spin/parity E$_{x}$ (keV) E$_{γ}$ (keV) BR (%) B(GT) ΣB(GT) USD shell model [19] [20] [20] (this work) E$_{x}$ (keV) BR (%) 0 3/2+ 0 0 18.7 0.0363 0.0363 0 13.7404 810.5(2) 1/2+ 810.6(2) 810.6 40.5 0.1151 0.1514 779 49.0350 2352.5(4) 3/2+ 2352.5(6) 2352.5 1.40 0.0128 0.1642 2174 5.5445 1541.4 0.60 E$_{x}$ (keV) spin/parity E$_{x}$ (keV) E$_{p}$ (keV) BR (%) B(GT) ΣB(GT) spin/parity USD shell model [19] [20] [20] (this work) (this work) E$_{x}$ (keV) BR (%) 3971.9(12) 3/2+ 3973(2) 1645 0.380 0.0069 0.1711 3667 0.3296 4112.8(8) (1/2,3/2)+ 4113(2) 1781 0.453 0.0090 0.1801 4185 0.3313 4438.2(15) 1/2+ 4442(3) 2100 2.54 0.0646 0.2447 4286 2.9158 4832(2) 3/2+ 4835(2) 2481 0.349 0.0121 0.2568 4808 0.2482 5104(2) 3/2+ 5106(3) 2744 0.0435 0.0019 0.2587 5076 0.2798 5310(4) 2941 0.0772 0.0040 0.2627 (3/2)+ 762# 0.0202 0.0010 0.2637 5544(1) 1/2+ 5549(3) 3173 31.0 0.1320 0.3957 5191 25.7003 5731(3) 1/2+ 5731(4) 3350 0.0753 0.0057 0.4014 5865(8) 1317# 0.180 0.0155 0.4169 (3/2)+ 6248(3) (1/2,3/2)+ 6253(3) 3857 0.724 0.0927 0.5097 or 6257(5) 1691# 0.0329 0.0042 0.5139 6326(5) 1764# 0.0102 0.0014 0.5153 (3/2)+ 6594(5) 2024# 0.00428 0.0008 0.5161 (3/2)+ 6951(5) 2370# 0.0159 0.0045 0.5206 (3/2)+ 7143(5) 4719 0.00079 0.0003 0.5209 7272(4) 3/2+ 7292(5) 4860 0.0108 0.0048 0.5257 (3/2)+ 2710# 0.00694 0.0031 0.5288 7405(10) 2810# 0.00141 0.0007 0.5295 (3/2)+ 7475(4) 5039 0.245 0.1398 0.6693 2886# 0.0394 0.0228 0.6921 7537(4) 5101 0.0592 0.0371 0.7292 7556(7) 2957# 0.0397 0.0256 0.7548 (3/2)+ 7666(4) 5225 0.0298 0.0226 0.7773 3066# 0.00446 0.0034 0.7807 7762(5) 5317 0.0113 0.0099 0.7907 (1/2)+ 1665## 0.00735 0.0066 0.7972 8077(4) 5623 0.155 0.2295 1.0268 3469# 0.0567 0.0853 1.1121 8132(6) 3515# 0.00886 0.0145 1.1266 (3/2)+ 8182(7) 5723 0.103 0.1833 1.3099 3576# 0.0108 0.0198 1.3297 8315(9) 5855 0.00318 0.0073 1.3370 8491(9) 6011 0.00100 0.0032 1.3401 (1/2)+ 2368## 0.00117 0.0039 1.3440 8557(5) 6100 0.0147 0.0562 1.4003 3926# 0.00911 0.0349 1.4352 8819(8) 6344 0.00054 0.0037 1.4389 8847(5) 4209# 0.00719 0.0523 1.4911 (3/2)+ 8865(10) 6389 0.00027 0.0021 1.4932 8967(6) 6480 0.0116 0.1122 1.6054 (1/2)+ 4330# 0.00167 0.0166 1.6221 9119(5) 6628 0.00173 0.0252 1.6473 4474# 0.00367 0.0549 1.7022 9152(6) 6657 0.00049 0.0077 1.7099 (3/2)+ 4505# 0.00487 0.0798 1.7897 3016## 0.00066 0.0113 1.8010 9202(9) 6715 0.00102 0.0193 1.8202 9300-9400 6800-6900 0.00023 0.0068 1.8270 9400-9500 6900-7000 0.00007 0.0030 1.8300 9500-9600 7000-7100 0.00032 0.0194 1.8494 9584(6) 4923# 0.00066 0.0459 1.8954 (3/2)+ 9600-9700 7100-7200 0.00000 0.0000 1.8954 9700-9800 7200-7300 0.00012 0.0175 1.9129 9800-9900 7300-7400 0.00010 0.0221 1.9350 9900-10000 7400-7500 0.00008 0.0315 1.9666 10000-10500 7500-8000 0.00006 0.1042 2.0708 10500-11500 8000-9000 0.00004 0.4966 2.5674 7