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We apply a three-dimensional (3D) approach to investigate the quasi-stationary states of well-deformed -emitters. With a splitting of the anisotropic 3D potential into internal and external parts at a separation surface, the 3D -cluster decay width is determined by the initial wave function of a true bound state of an anisotropic harmonic oscillator potential and a non-resonance scattering wave function of Coulomb potential. Substantial difference between the 1D and 3D decay width is found for typical -emitters with large quadrupole and hexadecapole deformations.

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