Beta-decay through broad resonances Karsten Riisager Aarhus University.

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Presentation transcript:

Beta-decay through broad resonances Karsten Riisager Aarhus University

The main points Occurs frequently in light nuclei No single, simple way to analyse the decays Consequences: – not unique Gamow-Teller strength (B GT ) ? – care needed when interpreting R-matrix fits

Example – 8 B(βα)

Example – 20 Na(βα) KL Laursen et al., Eur. Phys. J A (2013) 49: 79

Why are levels broad ? Strong coupling to continuum Small barrier Example: σ, elastic scattering of n I, integral of wavefunction squared inside potential

Remove “phase space” Decay rate w ≈ P l (E-E th ) f(Q-E) M GT 2 E.g. 8 B:

Do. for 6 He(βd) Data from: M. Pfützner et al., Phys. Rev. C 92, (2015)

Decay mechanism Two different approaches – Sequential through (overlapping) levels, e.g. 8 B(βα) – Direct to continuum, e.g. 6 He(βd) Does it matter ?? – Incomplete exp  model dependent results – How do you interpret “structureless” distributions? – It may influence the extracted B GT value

Sequential: R-Matrix approach MJG Borge et al., Nucl. Phys. A490 (1988) Ne(βp) Applied to beta-decay: FC Barker Internal region with levels that couple to “outside” channels. Level widths: Γ = 2 P γ 2 so levels may overlap and interfere.

R-matrix formulae where F/GT matrix element: Brune formulation, cf. S Hyldegaard, PhD thesis 2010

Problems with R-matrix – (1) 8 B Fits with 3 MeV resonance, the 16 MeV doublet and one extra 2 + level.

Problems with R-matrix – (2) 12 N Exp. spectrum indicates high-lying resonances with unrealistic parameters S. Hyldegaard et al, PRC 81 (10)

Simple model + R-matrix fits Same model as earlier, beta decay from initial states with binding energy E = 5 / 1 / 0.2 / 0.02 MeV: Differences due to contributions from extra-nuclear distances ! R-matrix: level energy depends on E + need more (unreasonable) levels…

Proposed B GT (re)definition Discrete states w = C f(Q-E) B GT, C = ln2 g A 2 /K Continuum w(E) = C f(Q-E) B GT (E) Gamow-Teller sum-rule Σ B GT - - Σ B GT + = 3(N-Z) is still ok (the sum extended with an integral) Easy for experimentalists but cannot extrapolate… Manageable for theoreticians Completeness relation: T Berggren, PL B44 (73) 23; WJ Romo, NP A237 (75) 275

Summary Conceptually: approaching reaction theory Careful when extracting B GT ! Danger of misinterpreting R-matrix fits Can 16 N(βα) be used to constrain 12 C(α,γ) ?

Thanks to many collaborators: Solveig Hyldegaard, Aksel S Jensen Maria JG Borge, Hans OU Fynbo, Björn Jonson, Olof Tengblad Christian Aa Diget, Dmitri V Fedorov, Luis M Fraile, Jacob G Johansen, Oliver S Kirsebom, Thomas Nilsson, Göran Nyman, Achim Richter Uffe Bergmann, Oliver Forstner, Henrik Jeppesen, Ari Jokinen, Kasper L Laursen Miguel Madurga, Antti Saastamoinen … More info: NP A940 (2015) 119, NP A925 (2014) (E) arXiv: , arXiv: