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How Many-Body Correlations and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>α</mml:mi></mml:math>Clustering Shape<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi>He</mml:mi></mml:mrow><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>6</mml:mn></mml:mrow></mml:mmultiscripts></mml:mrow></mml:math>

C. Romero-RedondoLawrence Livermore National Laboratory, P.O. Box 808, L-414, Livermore, California 94551, USASofia QuaglioniLawrence Livermore National Laboratory, P.O. Box 808, L-414, Livermore, California 94551, USAPetr NavrátilTRIUMF, 4004 Wesbrook Mall, Vancouver, British Columbia V6T 2A3, CanadaGuillaume HupinCEA, DAM, DIF, F-91297 Arpajon, France
2016lv
ABI

Аннотация

The Borromean ^{6}He nucleus is an exotic system characterized by two halo neutrons orbiting around a compact ^{4}He (or α) core, in which the binary subsystems are unbound. The simultaneous reproduction of its small binding energy and extended matter and point-proton radii has been a challenge for ab initio theoretical calculations based on traditional bound-state methods. Using soft nucleon-nucleon interactions based on chiral effective field theory potentials, we show that supplementing the model space with ^{4}He+n+n cluster degrees of freedom largely solves this issue. We analyze the role played by α clustering and many-body correlations, and study the dependence of the energy spectrum on the resolution scale of the interaction.

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