“…Specifically, M1 spin-flip excitations are analog of Gamow-Teller (GT) transitions, meaning that, at the operator level, the dominant M1 isovector component is the synonym to the zeroth component of GT transitions, and can serve as probe for calculations of inelastic neutrinonucleus cross section [8,9]. This process is hard to measure but it is essential in supernova physics, as well as in the r-process nucleosynthesis calculations [6,7,10,11]. The isovector spin-flip M1 response is also relevant for applications related to the design of nuclear reactors [12], for the understanding of single-particle properties, spinorbit interaction, and shell closures from stable nuclei toward limits of stability [13][14][15][16][17], as well as for the resolving the problem of quenching of the spin-isopin response in nuclei that is necessary for reliable description of double beta decay matrix elements [18].…”