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Rev. Lett."],"accepted":{"date-parts":[[2026,3,20]]},"abstract":"\n The weak binding and spatially extended neutron densities characteristic of drip-line nuclei give rise to a distinctive low-energy dipole response. The drip-line nucleus\n \n \n \n \n He<\/a:mi>\n <\/a:mrow>\n \n \n \n 8<\/a:mn>\n <\/a:mrow>\n <\/a:mmultiscripts>\n <\/a:mrow>\n <\/a:math>\n is the most neutron-rich bound nucleus with a mass-to-charge ratio of\n \n \n A<\/c:mi>\n \/<\/c:mo>\n Z<\/c:mi>\n =<\/c:mo>\n 4<\/c:mn>\n <\/c:mrow>\n <\/c:math>\n . We measure the dipole response of\n \n \n \n \n He<\/e:mi>\n <\/e:mrow>\n \n \n \n 8<\/e:mn>\n <\/e:mrow>\n <\/e:mmultiscripts>\n <\/e:mrow>\n <\/e:math>\n , including for the first time the four-neutron decay channel. A total dipole strength of\n \n \n \n \u2211<\/g:mo>\n B<\/g:mi>\n (<\/g:mo>\n E<\/g:mi>\n 1<\/g:mn>\n )<\/g:mo>\n (<\/g:mo>\n \n \n E<\/g:mi>\n <\/g:mrow>\n \n *<\/g:mo>\n <\/g:mrow>\n <\/g:msup>\n <<\/g:mo>\n 15<\/g:mn>\n <\/g:mrow>\n \u2009\u2009<\/g:mtext>\n MeV<\/g:mi>\n )<\/g:mo>\n =<\/g:mo>\n 0.95<\/g:mn>\n (<\/g:mo>\n 16<\/g:mn>\n )<\/g:mo>\n \n \n e<\/g:mi>\n <\/g:mrow>\n \n 2<\/g:mn>\n <\/g:mrow>\n <\/g:msup>\n \u2009<\/g:mtext>\n \n \n fm<\/g:mi>\n <\/g:mrow>\n \n 2<\/g:mn>\n <\/g:mrow>\n <\/g:msup>\n <\/g:mrow>\n <\/g:math>\n and a dipole polarizability of\n \n \n \n \n \u03b1<\/o:mi>\n <\/o:mrow>\n \n D<\/o:mi>\n <\/o:mrow>\n <\/o:msub>\n =<\/o:mo>\n 0.61<\/o:mn>\n (<\/o:mo>\n 1<\/o:mn>\n )<\/o:mo>\n \u2009<\/o:mtext>\n \u2009<\/o:mtext>\n \n \n fm<\/o:mi>\n <\/o:mrow>\n \n 3<\/o:mn>\n <\/o:mrow>\n <\/o:msup>\n <\/o:mrow>\n <\/o:math>\n are extracted from the differential Coulomb-excitation cross section and compared to state-of-the-art theoretical calculations employing coupled cluster and three-body approaches. We find that the dipole continuum is dominated, even at high excitation energies well above the\n \n 4<\/s:mn>\n n<\/s:mi>\n <\/s:math>\n decay threshold, by two-neutron emission, pointing to a\n \n \n \n \n \n He<\/u:mi>\n <\/u:mrow>\n \n \n \n 6<\/u:mn>\n <\/u:mrow>\n <\/u:mmultiscripts>\n <\/u:mrow>\n +<\/u:mo>\n 2<\/u:mn>\n n<\/u:mi>\n <\/u:mrow>\n <\/u:math>\n structure of the excited dipole mode. No indication was found for a\n \n 4<\/w:mn>\n n<\/w:mi>\n <\/w:math>\n final-state correlation, while pronounced\n \n n<\/y:mi>\n n<\/y:mi>\n <\/y:math>\n and\n \n \n \n \n \n He<\/ab:mi>\n <\/ab:mrow>\n \n \n \n 6<\/ab:mn>\n <\/ab:mrow>\n <\/ab:mmultiscripts>\n <\/ab:mrow>\n \u2212<\/ab:mtext>\n n<\/ab:mi>\n <\/ab:mrow>\n <\/ab:math>\n final-state correlations are apparent.\n <\/jats:p>","DOI":"10.1103\/vp3m-5rpp","type":"journal-article","created":{"date-parts":[[2026,3,20]],"date-time":"2026-03-20T17:59:56Z","timestamp":1774029596000},"update-policy":"https:\/\/doi.org\/10.1103\/crossmark-policy","source":"Crossref","is-referenced-by-count":0,"title":["Dipole Strength Distribution of\n \n \n \n \n He<\/mml:mi>\n <\/mml:mrow>\n \n \n \n 8<\/mml:mn>\n <\/mml:mrow>\n <\/mml:mmultiscripts>\n <\/mml:mrow>\n <\/mml:math>\n and Decay 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