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Tables
Table 1:
Parameters used to draw the potentials
presented in Fig. 1. Parameters
and
are used with the PTG and
PTG' centrifugal barriers, respectively.
|
|
|
|
|
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
3s1/2 state is resonant, virtual, or bound, and for which the
2d3/2 state is resonant or virtual. The other two
parameters are =7 and s=0.04059.
case |
|
|
energy |
(a) |
resonant 3s1/2 state |
4.882 |
=(74-4225i)keV |
(b) |
virtual 3s1/2 state |
4.972 |
=-84keV |
(c) |
bound 3s1/2 state |
5.034 |
=-74keV |
(d) |
resonant 2d3/2 state |
4.850 |
=(649-2610i)keV |
(c) |
virtual 2d3/2 state |
4.900 |
=(-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 |
|
Lj |
|
Lj |
|
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) 3s1/2single-particle states, or the 2d3/2low-energy narrow resonances at two different positions.
The neutron Fermi energies
and average pairing gaps
[6] are given together
with the canonical energies
[12] and occupation factors
.
All energies are in keV.
case |
|
|
Lj |
|
|
(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 |
Next: Figures
Up: Continuum effects for the
Previous: Bibliography
Jacek Dobaczewski
1999-05-16