2026ApJ...996L..18K


Query : 2026ApJ...996L..18K

2026ApJ...996L..18K - Astrophys. J., 996, L18 (2026/January-1)

Dipole Polarizability of Finite Nuclei as a Probe of Neutron Stars.

KOLIOGIANNIS P.S., YUKSEL E., GHOSH T. and PAAR N.

Abstract (from CDS):

Nuclear ground state and collective excitation properties provide a means to probe the nuclear matter equation of state and establish connections between observables in finite nuclei and neutron stars. Specifically, the electric dipole polarizability, measured with high precision in various neutron-rich nuclei, serves as a robust constraint on the density dependence of the symmetry energy. In this Letter, we employ a class of relativistic energy density functionals in a twofold process: first, to link the electric dipole polarizability from recent experiments to the slope of the symmetry energy, and second, to translate this information into constraints on the tidal deformability and radii of neutron stars, in connection with multimessenger astrophysical observations from pulsars and binary neutron stars. We provide compelling evidence that the electric dipole polarizability represents a key nuclear observable to probe the neutron star properties. By significantly reducing the uncertainties in the mass-radius plane, our findings also align with recent multimessenger observations.

Abstract Copyright: © 2025. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Nuclear physics - Nuclear astrophysics - Neutron stars - Relativistic binary stars - Gravitational waves

Simbad objects: 6

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Number of rows : 6
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 PSR J0030+0451 Psr 00 30 27.42348 +04 51 39.7144           ~ 596 1
2 PSR J0437-47 Psr 04 37 15.7994581776 -47 15 08.544351636           DC 1032 0
3 PSR J0740+6620 Psr 07 40 45.799 +66 20 33.60           ~ 395 0
4 PSR J1231-1411 Psr 12 31 11.3069 -14 11 43.628           ~ 139 0
5 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
6 SNR G353.6-00.7 SNR 17 31 55.0 -34 42 36           ~ 172 0

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