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Approaching the N=20 Island of Inversion with the $^{29}$Mg(d,p)$^{30}$Mg reaction

Jul 30, 2026, 2:30 p.m.
20m
Fletcher Challenge Canada (Simon Fraser University Harbour Centre)

Fletcher Challenge Canada

Simon Fraser University Harbour Centre

515 West Hastings St, Vancouver, B.C. V6B 5K3

Speaker

Alan Wuosmaa (University of Connecticut)

Description

We have studied the $^{29}$Mg(d,p)$^{30}$Mg reaction in inverse kinematics, with the first use of a reaccelerated rare-isotope beam from FRIB delivered to the SOLARIS solenoidal spectrometer. The N=20 Island of Inversion (IoI) at $^{32}$Mg is well known, arising from a diminished gap between the $sd$ and $fp$ neutron shells. Evidence for this modification comes from a variety of studies including mass measurements [1], neutron knockout [2], Coulomb excitation [3] and proton scattering [4]. A pioneering study of the two-neutron transfer reaction $^{30}$Mg(t,p)$^{32}$Mg [5] and theoretical analyses [6] of those data suggested that the $^{32}$Mg ground state is strongly deformed with significant contributions of 2p-2h and 4p-4h neutron excitations out of the $sd$ shell. Differing interpretations of the approach to N=20 in the Mg isotopes exist, however. Coulomb-excitation work from the MINIBALL experiment suggest that $^{30}$Mg is a spherical nucleus residing fully outside of the IoI [7], while other Coulex measurements [8] indicate that $^{30}$Mg is deformed, and knockout data [9] identify non-negligible $fp$-shell strength in $^{30}$Mg that is approximately 30% of that seen in $^{32}$Mg. The question of whether the transition to N=20 IoI is sudden, or occurs more gradually, with particle-hole excitations already playing a role in the structure of low-lying states in $^{30}$Mg, can also be addressed by studying neutron transfer to the low-lying 0$^+$ states in $^{30}$Mg with the $^{29}$Mg(d,p)$^{30}$Mg reaction. Furthermore, little information exists about the negative-parity states in $^{30}$Mg, which inform us about the $fp$-shell single-particle energies. Shell-model calculations yield different predictions about the energies of negative-parity excitations, and single-neutron transfer strongly populates such states. We studied the $^{29}$Mg(d,p)$^{30}$Mg reaction in inverse kinematics using a reaccelerated $^{29}$Mg beam produced by the ReA6 facility at FRIB. The $^{29}$Mg beam, with an intensity of approximately 40000 particles per second and energy of 8.46 AMeV, bombarded a 200 μg/cm$^2$ CD$_2$ target. Protons and recoiling $^{30}$Mg nuclei were detected with SOLARIS, providing high-resolution measurements for final states in $^{30}$Mg. The data suggest significant mixing between the ground and first-excited 0$^+$ states, clear evidence for several negative-parity excitations, and one new previously unobserved state. We will present these results, and discuss comparisons of the experimental observations with predictions from shell-model calculations.

This material is based upon work supported by the U. S. Department of Energy, Office of Science, Office of Nuclear Physics, under Contract Numbers DE-SC0014552 (UCONN) and DE-AC02-6CH11357 (ANL) and used resources of the Facility for Rare Isotope Beams (FRIB) Operations, which is a DOE Office of Science User Facility under Award Number DE-SC0023633. SOLARIS is funded by the DOE Office of Science under the FRIB Cooperative Agreement DE-SC0000661.

[1] C. Thibault et al., Phys. Rev. C 12, 644 (1975).
[2] J.R. Terry et al., Phys. Rev. C 77, 014316 (2008).
[3] P. Doornenbal et al., Phys. Rev. Lett. 111, 212502 (2013), H.L. Crawford et al., Phys. Rev. C 93, 031303 (2016).
[4] S. Takeuchi et al., Phys. Rev. C 79, 054319 (2009).
[5] K. Wimmer et al., Phys. Rev. Lett. 105, 252501 (2010).
[6] A.O. Macchiavelli et al., Phys. Rev. C 94, 051303(R) (2016).
[7] O. Niedermaier et al., Phys. Rev. Lett. 94, 172501 (2005).
[8] V. Chisté et al., Phys. Lett. B 514, 233 (2001).
[9] J. R. Terry et al., Phys. Rev. C 77, 014316 (2008).

Author

Alan Wuosmaa (University of Connecticut)

Co-authors

Juliette Stecenko (University of Connecticut) Dr Daniel Bazin (Michigan State University) Dr Saul Bercerio Novo (Facility for Rare Isotope Beams) Dr Roderick Clark (Lawrence Berkley National Laboratory) Dr Calem Hoffman (Argonne National Laboratory) Dr Benjamin Kay (Argonne National Laboratory) Dr Matthew Martin (Argonne National Laboratory) Dr Jorge Pereira (Facility for Rare Isotope Beams) Daniela Ramirez (Facility for Rare Isotope Beams) Pranjal Singh (Facility for Rare Isotope Beams) Dr Tsz Leung Tang (Argonne National Laboratory) Dr Ivan A. Tolstukhin (Argonne National Laboratory) Nathan Turi (Facility for Rare Isotope Beams)

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