12 TABLE V: Barrier penetration calculations used to tentatively assign spins to certain levels. The first column gives the excitation energy of the state, followed by the two or three proton energies from this state. The next two columns give the angular momentum used in the calculations which is deduce from the two spin possibilities of the proton emitting state, 1/2 or 3/2, given in the following column. The next column is the barrier penetration half-life calculated with the angular momentum l=0 or l=2. The sixth column is the experimental branching ratio of the two/three proton transitions from the state. These branching ratios are given only once for each proton group. For some states, in the final column, we give our tentative spin assignments. E$_{x}$ E$_{p}$ angular possible spin T$_{1}$$_{/}$$_{2}$ BR proposed (keV) (keV) momentum of level (s) (%) spin 5310 2941 l=0 1/2 0.27e-21 0.0769 3/2 762 l=2 0.58e-16 0.0201 2941 l=2 3/2 0.50e-20 762 l=0 0.74e-18 6253 3857 l=0 1/2 0.13e-21 0.722 1691 l=2 0.12e-18 0.0328 3857 l=2 3/2 0.14e-20 1691 l=0 0.29e-20 7292 4860 l=0 1/2 0.76e-22 0.0108 3/2 2710 l=2 0.75e-20 0.00691 4860 l=2 3/2 0.55e-21 2710 l=0 0.36e-21 7475 5039 l=0 1/2 0.71e-22 0.244 2886 l=2 0.55e-20 0.0392 5039 l=2 3/2 0.48e-21 2886 l=0 0.29e-21 7666 5225 l=0 1/2 0.67e-22 0.0297 3066 l=2 0.40e-20 0.00438 5225 l=2 3/2 0.42e-21 3066 l=0 0.24e-21 8077 5623 l=0 1/2 0.59e-22 0.154 3469 l=2 0.22e-20 0.0530 5623 l=2 3/2 0.32e-21 3469 l=0 0.16e-21 8179 5723 l=0 1/2 0.57e-22 0.103 1/2 3576 l=2 0.20e-20 0.0085 5723 l=2 3/2 0.30e-21 3576 l=0 0.15e-21 8557 6100 l=0 1/2 0.52e-22 0.0146 3/2 3926 l=2 0.13e-20 0.00812 6100 l=2 3/2 0.25e-21 3926 l=0 0.12e-21 8967 6480 l=0 1/2 0.48e-22 0.0103 1/2 4330 l=2 0.86e-21 0.00142 6480 l=2 3/2 0.20e-21 4330 l=0 0.96e-22 9119 6628 l=0 1/2 0.46e-22 0.00170 3/2 4474 l=2 0.75e-21 0.00360 6628 l=2 3/2 0.19e-21 4474 l=0 0.90e-22 9152 6657 l=0 1/2 0.46e-22 0.00050 3/2 4505 l=2 0.73e-21 0.00466 3016 l=0 0.25e-21 0.00066 6657 l=2 3/2 0.19e-21 4505 l=0 0.88e-22 3016 l=2 0.44e-20