There exist cislunar and trans-lunar libration points near the Moon, which are referred as the LL 1 and LL 2 points respectively and can generate the different types of low-energy trajectories transferring from Earth to Moon. The time-dependent analytic model including the gravitational forces from the Sun, Earth and Moon is employed to investigate the energy-minimal and practical transfer trajectories. However, different from the circular restricted three-body problem, the equivalent gravitational equilibria are defined according to the geometry of instantaneous Hill's boundary due to the gravitational perturbation from the Sun. The relationship between the altitudes of periapsis and eccentricities is achieved from the Poincaré mapping for all the lunar captured trajectories, which presents the statistical feature of the fuel cost and captured orbital elements rather than generating a specified Moon-captured segment. The minimum energy required by the captured trajectory on a lunar circular orbit is deduced in the spatial bi-circular model. It is presented that the asymptotical behaviors of invariant manifolds approaching to/from the libration points or halo orbits are destroyed by the solar perturbation. In fact, the energy-minimal cislunar transfer trajectory is acquired by transiting LL 1 point, while the energy-minimal trans-lunar transfer trajectory is obtained by transiting LL 2 point. Finally, the transfer opportunities for the practical trajectories escaped from the Earth and captured by the Moon are yielded by transiting halo orbits near LL 1 and LL 2 points, which can be used to generate the whole trajectories. Conley had achieved the low-energy cislunar trajectories from the viewpoint of LL 1 point (Conley 1969). Bolt and Meiss obtained a low-energy cislunar transfer trajectory by the shooting method developed in chaotic dynamics with the total fuel consumption of V =750m/s and the flight duration of t =748 days (Bolt and Meiss 1995). Schroer and Ott improved the shooting method to achieve the transfer trajectory with similar fuel consumption but cutting off half of the transfer time (t =377.5 days) (Schroer and Ott 1997). Macau gained a transfer trajectory with a little more fuel consumption but much less transfer time than Schroer and Ott, i.e., V =767m/s and t =284 days (Macau 1998). Ross and Koon optimized the transfer time and fuel consumption to yield the better result, i.e., V =860m/s and t =65 days (Ross and Koon 2003). Topputo and Vasile employed the Lambert equation 3 in CR3BP to solve the two-point boundary problems and obtained the similar result with Ross and Koon (Topputo and Vasile 2005). Xu et al. investigated the occurrence condition for low-energy transfer and discovered that the transiting trajectories near LL 1 point are preferred to generate the low-thrust cislunar trajectory (Xu et al. 2012). On the other hands, Belbruno et al. raised a new type of trans-lunar trajectories by the numerical method, which has a great application in rescuing Japanese lunar spacecraft "Hiten" ...