“…In contrast, configuration mixing due to multi-particle-hole excitations was considered to gain an understanding of the shape coexistence phenomena by assuming different symmetry limits of the IBM for different configurations [6][7][8][9][10][11][12], which has proven to be successful in describing intruder states and shape coexistence phenomena in near closed shell nuclei, typically those around proton numbers Z~50 and Z~82 [2-4]. Recently, the intruder configuration mixing schemes with -particle and -hole configurations from up to in the U(5) (vibrational) and the O(6) (γ-unstable) limits of the IBM-I were proposed [13,14], whose simple Hamiltonians, suitable to describe the intruder and normal configuration mixing, prove to be exactly solvable based on the SU(1,1) coherent states.…”