On the basis of correcting various errors (spin-orbit coupling effects, scalar relativity effects, core-valence correlation effects and basis set truncation), the potential energy curves of 10 Λ-S states and 26 Ω states of AlH molecule are calculated using icMRCI+<i>Q</i> method. The transition dipole moments of 6 pairs of transitions between the X<sup>1</sup>∑<sup>+</sup><sub>0<sup>+</sup></sub>,a<sup>3</sup></sup>Π<sub>0<sup>+</sup></sub>,a<sup>3</sup></sup>Π<sub>1</sub>a<sup>3</sup></sup>Π<sub>2</sub>, and A<sup>1</sup>Π<sub>1</sub> states are calculated using the icMRCI/AV6Z* theory with the contain of spin-orbit coupling effects. The spectral and transition data obtained here for AlH molecule are in very good agreement with the available experimental measurements. We find that:(1) the transition intensities are relatively strong of the Q(<i>J</i><i>"</i><i></i>) branches for the (0, 0), (0, 1), (0, 2), (1, 0), (1, 1), (1, 2), (1, 3), (1, 4) and (1, 5) bands of the A<sup>1</sup>Π<sub>1</sub>-X<sup>1</sup>∑<sup>+</sup><sub>0<sup>+</sup></sub> transition, with the increase of <i>J</i><i>"</i>, the Einstein <i>A</i> coefficients and vibrational branching ratios gradually decrease, and the weighted absorption oscillator strengths gradually increases of Δ<i>υ</i>=0 bands, the Einstein <i>A</i> coefficients, vibrational branching ratios, and weighted absorption oscillator strengths gradually increase for the Δ<i>υ</i>≠0 bands; (2) the radiation lifetimes of A<sup>1</sup>Π<sub>1</sub>(<i>υ</i><i>'</i>=0, 1) increases slowly as the <i>J</i><i>'</i> increases. (3) The A<sup>1</sup>Π<sub>1</sub>(<i>υ</i><i>'</i>=0 and 1, <i>J'</i>=1, +)→X<sup>1</sup>∑<sup>+</sup><sub>0<sup>+</sup></sub>(<i>υ</i><i>"</i>=0-3, <i>J"</i>=1, -) transition of AlH molecule satisfies the criteria for laser cooling of diatomic molecules, that is, the vibrational branching ratios of the highly diagonal distribution, the extremely short radiation lifetimes of the A<sup>1</sup>Π<sub>1</sub>(<i>υ</i><i>'</i>=0 and 1, <i>J'</i>=1, +) states, and the intermediate electronic states a<sup>3</sup>Π<sub>0<sup>+</sup></sub>, a<sup>3</sup>Π<sub>1</sub>, and a<sup>3</sup>Π<sub>2</sub>do not interfere with laser cooling. Therefore, based on the cyclic transition A<sup>1</sup>Π<sub>1</sub>(<i>υ</i><i>'</i>=0and 1, <i>J'</i>=1, +)↔X<sup>1</sup>∑<sup>+</sup><sub>0<sup>+</sup></sub>(<i>υ</i><i>"</i>=0-3, <i>J''</i>=1, -), we propose a feasible scheme for laser cooling of AlH molecule. When cooling, 2.541×10<sup>4</sup> photons can be scattered using four pump lasers in the visible range, which are enough to cool AlH to the ultra-cold temperatures, and the Doppler and recoil temperatures of the main transition are in the order of μK.