Background: In highly deformed nuclei, there is a noticeable coupling of the Isoscalar Giant Monopole Resonance (ISGMR) and $K = 0$ component Quadrupole (ISGQR), which results in double peak structure isoscalar monopole (IS0) strength (a narrow low-energy deformation-induced main broad ISGMR part). The energy low-lying IS0 sensitive to both incompressibility modulus $K_\infty$ between quadrupol...
