2009Ta24, 2009Ta05: ⁶²Ti identified by fragmentation of ⁷⁶Ge beam at 132 MeV/nucleon with Be and W targets at NSCL facility using A1900 fragment separator combined with S800 analysis beam line to form a two- stage separator system. The transmitted fragments were analyzed event-by-event in terms of momentum and particle identification. The nuclei of interest were stopped in eight Si PIN diodes (50x50 mm²) which provided measurement of energy loss, nuclear charge and total kinetic energy. The time-of-flight of each particle that reached the detector stack was measured in four different ways using plastic scintillators, Si detectors, and parallel-plate avalanche counters. The simultaneous measurement of ΔE signals, magnetic rigidity, total kinetic energy and time-of-flight (ToF) provided unambiguous identification of the atomic number, charge state and mass number.

2020Mi13: measured mass excess using time-of-flight magnetic-rigidity technique at RIBF-RIKEN facility.

Theoretical nuclear structure calculations:

2022Ho02: calculated quadrupole deformation parameter β₂, S(2n), rms matter radius, hexadecapole deformation parameter β₄, difference of the charge square radii, diffuseness parameters, occupation of highly elongated intruder orbitals and effect on quadrupole and hexadecapole deformations using Skyrme-Hartree-Fock method in three-dimensional coordinate space.

2022Ko04: calculated ground state energy, charge rms radius using coupled cluster (α) and ab-initio density functional theory, extended to open-shell deformed nuclei.

2022Ya23: theory: structure: calculated binding energy, charge radius, quadrupole deformation, and pairing energy using relativistic mean-field (RMF) formalism

2021Co14: calculated S(2n), energy of the first 2⁺ state, effective single-particle energies (ESPEs), neutron-neutron monopole matrix elements using shell-model with an effective Hamiltonian from many-body perturbation theory using ⁴⁰Ca as a closed core, and three-body contributions through density-dependent two-body matrix elements (TBME) derived within a microscopic approach from chiral forces.

2018Sa40: calculated potential energy curves, T_1/2, Q(β^-), β^-n probability, Gamow-Teller strength distributions using constrained HF+BCS with Skyrme force SLy4.

2015Wa11: calculated potential energy surfaces, S(2p), excitation energies and B(E2), Jπ, neutron and proton single-particle levels using relativistic mean-field + BCS method with α(p)-PK1 functional.

2014Co04: calculated energies and B(E2) values of first 2⁺ state using realistic shell-model calculations with two different model spaces.

Theoretical calculations: consult the NSR database at for 16 primary references for nuclear structure, and two for decay modes and half-life.

2012Ca30: calculated energy levels, Jπ, electric quadrupole and dipole magnetic moments using shell model with FPD6 and GXPF1 interactions.

2010Le20: calculated levels, Jπ, B(E2), quadrupole moment, occupation of the neutron intruder orbitals and percentage of particle-hole excitations using interacting shell-model framework in full pf valence space based on ⁴⁸Ca core and effective interaction based on γ matrix; discussed shell evolution and island of inversion around n=40.

2009Ga41: calculated single-particle energies, Nilsson diagrams, potential energy curves, neutron and proton pairing energy curves, excitation energies, spectroscopic quadrupole moments, and B(E2) using Hartree-Fock-Bogoliubov (HFB) approach with Gogny D1S effective interaction

2008Gu03: calculated potential energy surfaces and ground state deformation using relativistic mean field theory.

Other theory references: 12 for structure and two for decay in the NSR database, also listed in this dataset as ’document’ records.

Q-value: Estimated uncertainties (2021Wa16): 480 for Q(β^-), 500 for S(n), 720 for S(p), 640 for Q(α)

Q-value: S(2n)=6240 470, S(2p)=37780 810, Q(β^-n)=9910 460 (syst,2021Wa16). Q(β^-2n)=4750 440, Q(β^-3n)=1200 420 (syst, deduced by evaluator from relevant mass excesses in 2021Wa16)