Time-dependent variational principle (TDVP) provides powerful methods in solving the timedependent Schröinger equation. As such Kan developed a TDVP (Kan 1981 Phys. Rev. A 24, 2831) and found that there is no Legendre transformation in quantum variational principle, suggesting that there is no place for the Maupertuis reduced action to appear in quantum dynamics. This claim is puzzling for the study of quantum-classical correspondence, since the Maupertuis least action principle practically sets the very basic foundation of classical mechanics. Zambrini showed within the theory of stochastic calculus of variations that the Maupertuis least action principle can lead to the Nelson stochastic quantization theory (Zambrini 1984 J. Math. Phys. 25, 1314. We here revisit the basic aspect of TDVP and reveal the hidden roles of Maupertuis-Hamilton least action in the Schrödinger wavepacket dynamics. On this basis we propose a dual least (stationary) action principle, which is composed of two variational functionals; one responsible for 'energy related dynamics' and the other for 'dynamics of wave-flow'. The former is mainly a manifestation of particle nature in wave-particle duality, while the latter represents that of matter wave. It is also shown that by representing the TDVP in terms of these inseparably linked variational functionals the problem of singularity, which is inherent to the standard TDVPs, is resolved. The structure and properties of this TDVP are also discussed.By contrast, the TDVP gives far more practical methodologies. Indeed, there have been proposed various elaborated formalisms such as those of the so-called Dirac-Frenkel, MaLachlan [16], Kan [17], Kramer and Saraceno [18], and so on. Broeckhove, Lathouwers, Kesteloot and van Leuven [19] gave a unified account over these methods. These methods and the variants are widely used in many fields of physics and chemistry. (For more recent progress in other general theories of TDVP, we refer to [20][21][22][23][24][25][26] .) Yet, it is known that the TDVP generally faces a divergence problem in handling nonlinear variational parameters, which arises from the inversion of possibly singular matrices.An overwhelming advantage of TDVP is that it transforms the Schrödinger partial differential equation to a set of coupled ordinary differential equations over the space of variational parameters. In this context, Kan [17] determinedly states in his seminal paper that 'any time-dependent description of quantum systems derived from the variational principle is equivalent to Hamilton's description of a classical system'. On the other hand, Kan has explicitly shown that there does not exist Legendre transformation in his TDVP. Lack of the Legendre transformation suggests that there is no place for the Maupertuis reduced (or abbreviated) action [27, 28] to appear, and therefore the Maupertuis-Hamilton least action principle will not have direct significance in TDVP. It is not comfortable however to accept this assertion, since the least action principle of Maupertu...