A combined ab initio and experimental analysis of nuclear form factors reduces uncertainties in superallowed beta-decay rates, enabling a more precise first-row CKM unitarity test.
2210.17488
4 Pith papers cite this work. Polarity classification is still indexing.
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First laser spectroscopy measurements of charge radii in Al isotopes from 25Al to 22Al reveal a step-like increase toward the proton drip line with similar radii for 22Al and 23Al, consistent with mirror-partner proton-skin trends.
Improved leading-order lattice Hamiltonians lower the liquid-gas critical temperature of symmetric nuclear matter to 13.50(17)-13.71(19) MeV while improving zero-temperature binding energies and saturation point.
Lattice EFT calculations find no resonance signature in the tetraneutron ground-state energy, only a weak attraction in the dineutron-dineutron phase shift whose confined energy is close to the experimental low-energy peak.
citing papers explorer
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Taming nuclear size and shape effects in superallowed beta-decay
A combined ab initio and experimental analysis of nuclear form factors reduces uncertainties in superallowed beta-decay rates, enabling a more precise first-row CKM unitarity test.
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Nuclear charge radii of aluminium isotopes at the proton drip line
First laser spectroscopy measurements of charge radii in Al isotopes from 25Al to 22Al reveal a step-like increase toward the proton drip line with similar radii for 22Al and 23Al, consistent with mirror-partner proton-skin trends.
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From binding and saturation to criticality in nuclear matter with lattice effective field theory
Improved leading-order lattice Hamiltonians lower the liquid-gas critical temperature of symmetric nuclear matter to 13.50(17)-13.71(19) MeV while improving zero-temperature binding energies and saturation point.
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Searching for the Tetraneutron Resonance on the Lattice
Lattice EFT calculations find no resonance signature in the tetraneutron ground-state energy, only a weak attraction in the dineutron-dineutron phase shift whose confined energy is close to the experimental low-energy peak.