Relativistic Energies and Scattering Phase Shifts for the Fermionic Particles Scattered by Hyperbolical Potential with the Pseudo(spin) Symmetry

Table 3

Nonrelativistic energies at the poles of -matrix (in units fm⁻¹) for the hyperbolical potential as a function of positive potential parameter for different states in atomic units , , and in all the calculations.

			States	for	for	for	for
0	1	0.10	2p	2.61890	3.90580	5.00395	5.88694
		0.15		1.68043	2.57796	3.43332	4.21023
		0.20		1.20892	1.86672	2.52064	3.14766
1	1	0.10	3p	4.73556	6.04579	6.91727	7.48500
		0.15		3.46030	4.62316	5.50084	6.15070
		0.20		2.68324	3.67163	4.46580	5.09331
0	2	0.10	3d	3.62747	5.29513	6.47684	7.25824
		0.15		2.27024	3.56732	4.69715	5.59908
		0.20		1.57921	2.54881	3.48311	4.31406
2	1	0.10	4p	6.00303	7.11562	7.71968	8.02132
		0.15		4.66775	5.80666	6.52479	6.95757
		0.20		3.75708	4.81251	5.53175	6.00386
1	2	0.10	4d	5.33170	6.73691	7.54672	7.97921
		0.15		3.85825	5.19508	6.13602	6.75665
		0.20		2.95305	4.10518	5.00371	5.66610
0	3	0.10	4f	4.69061	6.43208	7.43782	7.98144
		0.15		3.00365	4.60199	5.79916	6.61027
		0.20		2.07438	3.35838	4.47793	5.35424