in a recent Letter l have studied the role of the hyperfine tensor interaction in quark shell models within the context of the longitudinal and scalar quadrupole transition amplitudes in y v N-+ A. One of the two models studied was that of Vento, Baym, and Jackson 2 (VBJ). Certain conclusions as to the shortcoming of this model were reached. In this Comment we point to an unfortunate error in the VBJ wave functions used by these authors; because of this the conclusions regarding this model will have to be modified.The VBJ wave functions as used by these authors are(2)Here | A)# is in error. The correct VBJ wave functionThe important point to note is that the magnitude of the normalization for the two D states in | A) is the same. This arises due to the special nature of the operator 6 D [Eq. (4), Ref. 2] which induces the Z>-state admixtures. It was therein suggested that this arises due to the exchange of pions between quarks; not due to one-gluon exchange as viewed by these authors. x In fact, the wave function (2) can be justified on the basis of the onegluon-exchange model. But this is not what was used and advocated by VBJ. 2 Also, it has been emphasized 3 that the tensor term arising from one-gluon exchange is too weak to induce a Z>-state admixture of more than a few percent-certainly not -22% as is needed to explain the relevant experimental quantities in this picture. The incompatibility of the wave functions (2) and (3) would lead to significant differences in the physical quantities under investigation. For example, the pion-nucle-on-isobar coupling constant (i.e., the ratio of the ;r7VA to TTNN coupling constants denoted by r nNA ), is found to be 2 fxNA -
25[*(l-r)] l/2 +(yy/4) 1/2 1-fr (4) where x = l -2/3\ y=P' when the correct VBJ wave function (3) is used and x -1 -3/3, y =p when the wave function (2) is used. The advantage of the VBJ wave function is that the same value of y-0.22 fits g A (the axial-vector coupling constant), ju p /jLi n (the ratio of the proton and neutron magnetic moments), the D/F ratio, and r"iv A . It has also been recently found 4 that the same value of y (i.e., -0.22) fits all the experimental values of gA known in the study of the semileptonic decays of baryons belonging to the j + octet. Good fits to the magnetic moments of 3 He and 3 H are also obtained within this picture. 5 In view of these comments the conclusions regarding the VBJ model ] will have to be modified, perhaps quite significantly.