Tables

 

Table 1: Parameters used to draw the potentials presented in Fig. 1. Parameters $\nu_{g{9\over2}}$ and $\nu'_{g{9\over2}}$ are used with the PTG and PTG' centrifugal barriers, respectively.

$\Lambda$	$s [\mbox{fm}^{-1}$	$\nu_{s{1\over2}}$	$\nu_{g{9\over2}}$	$\nu'_{g{9\over2}}$
1	0.2192	6.719	6.188	7.199
3	0.09259	5.165	5.470	5.176
7	0.04059	5.034	5.372	4.693

 

 

Table 2: Depth parameters of the PTG potential, for which the 3s_1/2 state is resonant, virtual, or bound, and for which the 2d_3/2 state is resonant or virtual. The other two parameters are $\Lambda$=7 and s=0.04059.

case		$\nu_{Lj}$	energy
(a)	resonant 3s1/2 state	4.882	$\epsilon_{\mbox{\scriptsize {res}}}$=(74-4225i)keV
(b)	virtual 3s1/2 state	4.972	$\epsilon_{\mbox{\scriptsize {virt}}}$=-84keV
(c)	bound 3s1/2 state	5.034	$\epsilon_{\mbox{\scriptsize {bound}}}$=-74keV
(d)	resonant 2d3/2 state	4.850	$\epsilon_{\mbox{\scriptsize {res}}}$=(649-2610i)keV
(c)	virtual 2d3/2 state	4.900	$\epsilon_{\mbox{\scriptsize {virt}}}$=(-247-1776i)keV

 

 

Table 3: Depth parameters of the PTG' potential (9) defining the neutron spectrum used in the HFB calculations. Parameters not given here are listed in Table 2.

Lj	$\nu_{Lj}$	Lj	$\nu_{Lj}$	Lj	$\nu_{Lj}$	Lj	$\nu_{Lj}$
s 1/2	Table 2	p 1/2	4.640	p 3/2	4.880	d 3/2	Table 2
d 5/2	5.180	f 5/2	4.300	f 7/2	4.720	g 7/2	4.420
g 9/2	4.800	h 9/2	4.493	h11/2	4.992	i11/2	4.493
i13/2	4.493	j13/2	4.493

 

 

Table 4: Properties of the HFB solutions obtained for the PTG' potentials which give the resonant (a), virtual (b), and weakly bound (c) 3s_1/2single-particle states, or the 2d_3/2low-energy narrow resonances at two different positions. The neutron Fermi energies $\lambda_N$ and average pairing gaps $\langle\Delta_N\rangle$ [6] are given together with the canonical energies $\epsilon_{\mbox{\scriptsize {can}}}$ [12] and occupation factors $v^2_{\mbox{\scriptsize {can}}}$. All energies are in keV.

case	$\lambda_N$	$\langle\Delta_N\rangle$	Lj	$\epsilon_{\mbox{\scriptsize {can}}}$	$v^2_{\mbox{\scriptsize {can}}}$
(a)	-314	1146	3s1/2	2148	0.0321
(b)	-384	1292		1043	0.1002
(c)	-488	1421		390	0.2083
(d)	-436	1217	2d3/2	1765	0.0548
(c)	-488	1421		1107	0.1149