The dissociation dynamics of heteronuclear diatomic molecules induced by infrared laser pulses is investigated within the framework of the classical driven Morse oscillator. The interaction between the molecule and the laser field described in the dipole formulation is given by the product of a time-dependent external field with a position-dependent permanent dipole function. The effects of changing the spatial range of the dipole function in the classical dissociation dynamics of large ensembles of trajectories are studied. Numerical calculations have been performed for distinct amplitudes and carrier frequencies of the external pulses and also for ensembles with different initial energies. It is found that there exist a set of values of the dipole range for which the dissociation probability can be completely suppressed. The dependence of the dissociation on the dipole range is explained through the examination of the Fourier series coefficients of the dipole function in the angle variable of the free system. In particular, the suppression of dissociation corresponds to dipole ranges for which the Fourier coefficients associated with nonlinear resonances are null and the chaotic region in the phase space is reduced to thin layers. In this context, it is shown that the suppression of dissociation of heteronuclear molecules for certain frequencies of the external field is a consequence of the finite range of the corresponding permanent dipole. The classical driven Morse oscillator has been extensively applied to the study of the dissociation dynamics of heterodiatomic molecules by means of infrared laser fields [1][2][3][4][5][6][7][8][9][10][11][12]. The interaction between the molecule and the laser field is commonly given by the product of a time-dependent external field, which accounts for the electric field of the laser, with a position-dependent function, associated with the permanent dipole moment of the molecule. Consequently, the dissociation dynamics depends on both the external field and the dipole function. Understanding the role of the dipole function in the dynamics of the Morse oscillator can help to gain physical insights on the dissociation dynamics of diatomic molecules.The concept of a dipole function for a diatomic molecule arises within the Born-Oppenheimer picture [13][14][15]. In this picture, the electronic wavefunction depends parametrically on the internuclear distance for a given molecular state. The dipole moment of the molecular charge distribution can be represented by a function of the internuclear distance. Diatomic molecules possess many forms of dipole functions [16][17][18][19], which typically go asymptotically to zero for large internuclear distances. Correspondingly, one can associate an effective spatial range with a dipole function.The free Morse oscillator has two distinct energy regions. A particle placed in the bound region performs oscillatory motion, which represents the vibration of the molecule. A particle placed in the unbound region escapes to infinity and this sc...