-
3
-
-
85035257306
-
-
Note that the (Formula presented) 130 isotopes of Tellurium are 2νββ emitters and good candidates for 0νββ. From a nuclear structure point of view, the study of both EC and ββ processes can shed light on the mechanism which is at the basis of the cancellation between particle-hole and particle-particle correlations (cf. 4 5
-
Note that the (Formula presented) 130 isotopes of Tellurium are 2νββ emitters and good candidates for 0νββ. From a nuclear structure point of view, the study of both EC and ββ processes can shed light on the mechanism which is at the basis of the cancellation between particle-hole and particle-particle correlations (cf. 45 and references therein).
-
-
-
-
5
-
-
0003716254
-
-
Adam Hilger, Bristol
-
G. Grotz and H. V. Klapdor-Kleingrothaus, The Weak Interaction in Nuclear, Particle, and Astrophysics (Adam Hilger, Bristol, 1990).
-
(1990)
The Weak Interaction in Nuclear, Particle, and Astrophysics
-
-
Grotz, G.1
Klapdor-Kleingrothaus, H.V.2
-
7
-
-
0001479629
-
-
M. Baranger and E. Vogt, Plenum, New York
-
D. R. Bes and R. Sorensen, in Advances in Nuclear Physics, edited by M. Baranger and E. Vogt (Plenum, New York, 1969), Vol. 2, p. 129.
-
(1969)
Advances in Nuclear Physics
, vol.2
, pp. 129
-
-
Bes, D.R.1
Sorensen, R.2
-
8
-
-
0000779490
-
-
M. Baranger and E. Vogt, Plenum, New York
-
R. A. Broglia, O. Hansen, and C. Riedel, in Advances in Nuclear Physics, edited by M. Baranger and E. Vogt (Plenum, New York, 1972), Vol. 6, p. 287.
-
(1972)
Advances in Nuclear Physics
, vol.6
, pp. 287
-
-
Broglia, R.A.1
Hansen, O.2
Riedel, C.3
-
10
-
-
0002952960
-
-
M. Beiner, H. Flocard, N. Van Giai, and P. Quentin, Nucl. Phys. A238, 29 (1975)
-
(1975)
Nucl. Phys.
, vol.A238
, pp. 29
-
-
Beiner, M.1
Flocard, H.2
Van Giai, N.3
Quentin, P.4
-
14
-
-
85035282702
-
-
Ref. 10
-
In Ref. 10 the numerical values for (Formula presented) are not reported. We have set them equal to 1, as suggested by the systematics of the quoted values.
-
-
-
-
17
-
-
0008994208
-
-
J. R. Lien et al., Nucl. Phys. A253, 165 (1975)
-
(1975)
Nucl. Phys.
, vol.A253
, pp. 165
-
-
Lien, J.R.1
-
18
-
-
0001147314
-
-
AFYSA7
-
S. A. Hjort, Ark. Fys. 33, 183 (1967).AFYSA7
-
(1967)
Ark. Fys.
, vol.33
, pp. 183
-
-
Hjort, S.A.1
-
19
-
-
85035274266
-
-
The order of single particle levels may be deduced from one-particle transfer reactions 16 21 22 23 22
-
The order of single particle levels may be deduced from one-particle transfer reactions 16212223. In particular, we assumed a (Formula presented) configuration for the two protons out of the (Formula presented) core in the (Formula presented) ground state 22.
-
-
-
-
20
-
-
85035295558
-
-
Neutron quasiparticle energies in (Formula presented) are taken from Ref. 16 22 16 16 21 22 23
-
Neutron quasiparticle energies in (Formula presented) are taken from Ref. 16. Quasiproton energies in (Formula presented) are given in Ref. 22, and have been referred to the ground state of (Formula presented) according to the scheme followed in Ref. 16. The experimental quasiparticle occupation factors in (Formula presented) are given in Refs. 16212223 and were renormalized in each channel to sum up to the correct number of valence nucleons.
-
-
-
-
23
-
-
0001201348
-
-
S. Gales et al., Nucl. Phys. A381, 173 (1982)
-
(1982)
Nucl. Phys.
, vol.A381
, pp. 173
-
-
Gales, S.1
-
24
-
-
0009143626
-
-
J. R. Lien et al., Nucl. Phys. A281, 443 (1977)
-
(1977)
Nucl. Phys.
, vol.A281
, pp. 443
-
-
Lien, J.R.1
-
26
-
-
85035263199
-
-
It is well known that this phenomenon is associated with the appearance of a zero energy state, and is a signal of the failure of the standard pn-QRPA model, due to ground state correlations induced by the increasing particle-particle interaction
-
It is well known that this phenomenon is associated with the appearance of a zero energy state, and is a signal of the failure of the standard pn-QRPA model, due to ground state correlations induced by the increasing particle-particle interaction.
-
-
-
|