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Dipole Strength Distribution of He8 and Decay Characteristics

C. Lehr1, T. Aumann1,2,3, M. Duer1,*, A. T. Saito4, T. Nakamura4, N. L. Achouri5, D. Ahn6, H. Baba6, S. Bacca7 et al.

C. A. Bertulani8, M. Böhmer9, F. Bonaiti7,10,11, K. Boretzky2, C. Caesar1,2,6, N. Chiga6, D. Cortina-Gil12, C. A. Douma13, F. Dufter9, Z. Elekes14,15, J. Feng16, B. Fernández-Domínguez12, U. Forsberg17, N. Fukuda6, I. Gasparic18,1,6, Z. Ge6, R. Gernhäuser9, J. M. Gheller19, J. Gibelin5, A. Gillibert19, K. I. Hahn20,21, Z. Halász14, M. N. Harakeh13, A. Hirayama4, M. Holl1, N. Inabe6, T. Isobe6, J. Kahlbow1, N. Kalantar-Nayestanaki13, D. Kim21, S. Kim21,1, T. Kobayashi22,†, Y. Kondo4, D. Körper2, P. Koseoglou1, Y. Kubota6, P. J. Li23,24, S. Lindberg25, Y. Liu16, F. M. Marqués5, S. Masuoka26, M. Matsumoto4, J. Mayer27, K. Miki1,22, M. Miwa6, B. Monteagudo5, A. Obertelli1,19, N. A. Orr5, H. Otsu6, V. Panin6,2, S. Y. Park20,21, M. Parlog5, S. Paschalis17,1, P. M. Potlog28, S. Reichert9, A. Revel5,29,10,30, D. M. Rossi1, R. Roth1, M. Sasano6, H. Scheit1, F. Schindler1, T. Shimada4, S. Shimoura26, H. Simon2, S. Storck Dutine1, L. Stuhl21,26, H. Suzuki6, D. Symochko1, H. Takeda6, S. Takeuchi4, J. Tanaka1,6, Y. Togano4, T. Tomai4, H. T. Törnqvist1,2, J. Tscheuschner1, T. Uesaka6, V. Wagner1, H. Yamada4, B. Yang16, L. Yang26, Z. H. Yang6, M. Yasuda4, K. Yoneda6, L. Zanetti1, and J. Zenihiro6,31

  • *Contact author: mduer@ikp.tu-darmstadt.de
  • †Deceased.

Phys. Rev. Lett. 136, 172501 – Published 1 May, 2026

DOI: https://doi.org/10.1103/vp3m-5rpp

Abstract

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 He8 is the most neutron-rich bound nucleus with a mass-to-charge ratio of A/Z=4. We measure the dipole response of He8, including for the first time the four-neutron decay channel. A total dipole strength of ∑B(E1)(E*<15  MeV)=0.95(16)e2 fm2 and a dipole polarizability of αD=0.61(1)  fm3 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 4n decay threshold, by two-neutron emission, pointing to a He6+2n structure of the excited dipole mode. No indication was found for a 4n final-state correlation, while pronounced nn and He6−n final-state correlations are apparent.

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