“…Thus, we will consider the rotational 1/N c and linear m s corrections. The model has been successfully applied to various observables of the SU(3) baryons: for example, the electromagnetic structures [72][73][74][75][76], strange form factors [77][78][79][80][81][82][83], axial-vector form factors [84,85], tensor charges and corresponding form factors [82,83,86,87], semileptonic decays [18,88,89], radiative transition [90][91][92], the nucleon parton distributions [93][94][95][96][97][98], and the gravitational form factors [99,100] of the nucleon. In this work, we will concentrate on all possible axial-vector transitions from the baryon decuplet to the baryon octet, including both ∆S = 0 and |∆S| = 1 transitions.…”