Upload
rhoda-lang
View
212
Download
0
Tags:
Embed Size (px)
Citation preview
Double beta decay nuclear matrix elements in deformed nuclei
O. Moreno, R. Álvarez-Rodríguez,P. Sarriguren, E. Moya de Guerra
F. Šimkovic, A. Faessler
H. Müther
Past, present and future calculations within Tübingen-Madrid collaboration
Introduction
Theoretical formalism
Results
Current work
Conclusions & outlook
Summary
Introduction
Two succesive decays through intermediate virtual states.
Second order process in weak interaction energy denominator.
One of the most rare events in nature, T1/2 ~ 1019 – 1021 s.
Observed in 48Ca 76Ge 82Se 96Zr 100Mo 116Cd 128Te 130Te 150Nd.
Strong dependence on nuclear structure, in particular nuclear deformation.
AX
AY
AZ
2 2 decay
Introduction
0 2 decay
Virtual emitted in the first decay is absorbed in the second decay.
For virtual neutrinos, (Majorana particles)
Also a very rare event, observation not yet confirmed.
Also strong dependence on nuclear structure
comparison with 22 nuclear matrix elements needed.
AX
AY
AZ
Mean field+
pairing+
proton-neutroncorrelations
Theoretical formalism
def. HF (Skyrme)
BCS (expG)
pnQRPA . (ph+pp)
Nuclear wavefunction: adiabatic + harmonic collective motionNuclear wavefunction: adiabatic + harmonic collective motion
Dynamics: Classical variational principleDynamics: Classical variational principle
Theoretical formalism
HF & RPA equations:HF & RPA equations:
Theoretical formalism
(Pairing(PairingBCS)BCS)
(Skyrme (Skyrme interactions)interactions)
++
( )j j
j
Ee
Theoretical formalism
136Xe
136Cs
136Ba
ParentDaughter
expQexp
Qexp
Alvarez-Rodriguez et al. PRC 70 (2004) 064309
Results
HF (Sk3) + BCS
Alvarez-Rodriguez et al. PRC 70 (2004) 064309
Results
Alvarez-Rodriguez et al. PRC 70 (2004) 064309
Results
Alvarez-Rodriguez et al. PRC 70 (2004) 064309
Alvarez-Rodriguez et al. PRC 70 (2004) 064309
Results
1)1) Improvement of overlap between RPA Improvement of overlap between RPA intermediate virtual states.intermediate virtual states.
2)2) Introduction of a realistic residual Introduction of a realistic residual interaction giving rise to spin-isospin interaction giving rise to spin-isospin transitions (to be treated within RPA).transitions (to be treated within RPA).
3)3) Closure approximation.Closure approximation.
Current calculations
1)1) Improvement of overlap between Improvement of overlap between RPA intermediate virtual states.RPA intermediate virtual states.
Current calculations I
136Xe
136Cs
136Ba
i fmm f ia BCS BCS
1)1) Improvement of overlap between Improvement of overlap between RPA intermediate virtual states.RPA intermediate virtual states.
where
RPA phonon operators on initial (i) and final (f) nuclei
, , , ,
, , , ,
, , , ,
, , , ,
i f i f
i f
i f i f
i f
m m m m i f i f i fm m
m m m m i f i f i fm m
a X Y u v
b X Y u v
NEW
1)1) Improvement of overlap between Improvement of overlap between RPA intermediate virtual states.RPA intermediate virtual states.
1 1
i fi f f im mm m mm O OO
F. Šimkovic, DBD06-ILIAS/N6 Collaboration meeting Valencia 2006
i fmm f iO m m
Unitarity test
1 † ?O O
2) Introduction of a realistic residual interaction 2) Introduction of a realistic residual interaction giving rise to spin-isospin transitionsgiving rise to spin-isospin transitions
Two-body matrix element of a realistic interaction V (CD Bonn, Vlow k ,…):
Introducing JT coupling:
Gamow-Teller transitions
Current calculations II
2) Introduction of a realistic residual interaction 2) Introduction of a realistic residual interaction giving rise to spin-isospin transitionsgiving rise to spin-isospin transitions
Change of basis: from original spherical harmonic oscillator w.f. to deformed HF w.f.:
Ready to be introduced in the RPA equations:
3) Closure approximation3) Closure approximation
136Xe
136Cs
136Ba
Current calculations III
3) Closure approximation3) Closure approximation
3) Closure approximation3) Closure approximation
BCS overlap for parent and daughter nuclei with different deformation:
with
3) Closure approximation3) Closure approximation
EM = GT closure
2v
Comparison 1+RPA – Closure to get energy denominator:
• Theoretical 22 decay nuclear matrix elements are essential information to study 02 decays, which give new information on character.
• Our calculations through deformed RPA intermediate virtual states show:
- a reduction effect due to deformation differences between parent and daughter nuclei.
- a good agreement with single and double beta experimental data.
Conclusions
• Current work includes:
- Improvement of RPA overlaps.
- Use of realistic spin-isospin residual interactions.
- Closure approximation.
• Get more accurate results on 22 and go to 02
Conclusions
Conclusions
Atomic nucleus
Detector of NEMO3
02 experiment
3 m 10-14 m
The best laboratory to measure neutrino properties is not necessarily very big!
Double beta decay nuclear matrix elements in deformed nuclei
O. Moreno, R. Álvarez-Rodríguez,P. Sarriguren, E. Moya de Guerra
F. Šimkovic, A. Faessler
H. Müther
Past, present and future calculations within Tübingen-Madrid collaboration
APPENDIX
Deformed Hartree-Fock with Skyrme forces
Single particle states (axially symmetric even-even nuclei)
Expansion into eigenfunctions of deformed h.o. (R,)
with
Pairing correlations in BCS approximation
and
Residual interactions consistent with the HF mean field
ph, pp
A simplified scheme
pnQRPA phonon operator for GT excitations
QRPA equations XK, Y
K
Transition amplitudes in the intrinsic frame
Average over nuclear volume
Xe isotopes in 2 processes
GT + GT +
GT –GT –
Gamow-Teller Gamow-Teller strength strength
distributionsdistributions
J = 0, 1(no 0+ 0+)
Tz = 1T = 0,1
HF + BCS(G)HF + BCS(G)+ QRPA+ QRPA
Results single Xe isotopes