We investigate the energy distribution of the isoscalar monopole and dipole transitions in the heavy systems, such as 44Ti and Te isotopes. The macroscopic α cluster models with α+40Ca and α+Sn are applied to 44Ti and Sn isotopes, respectively. The present calculation shows that the monopole and dipole strengths are strongly enhanced by the excitation in the the α cluster degrees of freedom. The discrete and sharp strength is generated by the α cluster excitation at the excitation energy much lower than the energy for the single nucleon excitation inside of the uniform mean field potential.
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