Effects ofLi6excitation inZn64(d→,6Li)60Ni at low energies

Cross sections and the analyzing powers ${\mathit{A}}_{\mathit{y}}$, ${\mathit{A}}_{\mathit{y}\mathit{y}}$, and ${\mathit{A}}_{\mathit{x}\mathit{x}}$ for the ${}_{}{}^{64}{}_{}{}^{}\mathrm{Zn}$(d${,}^6$Li${)}^{60}$Ni reaction forming the ground and first-excited states of ${}_{}{}^{60}{}_{}{}^{}\mathrm{Ni}$ are measured in 5° steps from ${\mathrm{\theta }}_{\mathrm{lab}}$=25° to 80° using a 16.4-MeV vector- and tensor-polarized deuteron beam. The ${}_{}{}^6{}_{}{}^{}\mathrm{Li}$ ground state and seven other states, each representing ${}_{}{}^6{}_{}{}^{}\mathrm{Li}$ continuum states of a given spin and internal orbital angular momentum, are included in finite-range, coupled-channel Born approximation (CCBA) calculations for ${}_{}{}^{64}{}_{}{}^{}\mathrm{Zn}$(d${,}^6$Li${)}^{60}$Ni. The CCBA calculations demonstrate that α transfers forming these continuum states, particularly those forming the first $3^{+}$ state in ${}_{}{}^6{}_{}{}^{}\mathrm{Li}$, affect the ${}_{}{}^{64}{}_{}{}^{}\mathrm{Zn}$(d${,}^6$Li${)}^{60}$Ni cross sections and analyzing powers strongly.