The CaSH molecule is an important target in the field of laser cooling of non-linear polyatomic molecules. Successful cooling of this molecule could surpass the technical limitations of diatomic and linear triatomic molecules in laser cooling. To identify the possible optical cycle in cooling CaSH, precise geometries of the CaSH ground state and the three lowest excited states, along with their excitation energies, are determined by utilizing the EA-EOM-CCSD (Electron attachment equation-of-motion coupled cluster singles and doubles) method, in combination with energy extrapolation using cc-pVXZ/cc-pCVXZ(X=T, Q) serial basis sets. Geometric parameters of the ground state $mathop Xlimits^ sim $<sup>2</sup><i>A'</i> were found to be RCaS=2.564Å; RSH=1.357Å; ∠CaSH=91.0°. Additionally, the equilibrium geometries of three excited states are also obtained. The $mathop Blimits^ sim $<sup>2</sup><i>A''</i> state has a similar equilibrium structure to the ground state, while the $mathop Alimits^ sim $<sup>2</sup><i>A'</i> and $mathop Climits^ sim $<sup>2</sup><i>A'</i> states exhibit significant conformer distortions. Specifically, the CaS bond of the $mathop Alimits^ sim $<sup>2</sup><i>A'</i> and $mathop Climits^ sim $<sup>2</sup><i>A'</i> states tend to contract, and the CaSH angel bends by 5 relative to the ground state. The vertical excitation energies from the ground state to $mathop Alimits^ sim $<sup>2</sup><i>A'</i>、$mathop Blimits^ sim $<sup>2</sup><i>A''</i> and $mathop Climits^ sim $<sup>2</sup><i>A'</i> are of 1.898eV, 1.945eV and 1.966eV, respectively, which are in good agreement with the previous experimental results. Moreover, the potential energy surfaces of the four lowest electronic states of CaSH were calculated by EA-EOM-CCSD with 3ζ level of basis sets. The nuclear equations of motion were solved to obtain the vibrational frequencies of the CaS bond stretching and CaSH bending. The vibrational frequencies of the (0,1,0) mode (the CaS stretching) of four states are 316 cm-1, 315 cm-1, 331 cm-1 and 325 cm-1, which are in close agreement with the available experimental results. The frequencies of the CaSH bending mode are presented for the first time, with the value of 357 cm-1, 396 cm-1, 384 cm-1, 411 cm-1 for the $mathop Xlimits^ sim $<sup>2</sup><i>A'</i>, $mathop Alimits^ sim $<sup>2</sup><i>A'</i>, $mathop Blimits^ sim $<sup>2</sup><i>A''</i> and $mathop Climits^ sim $<sup>2</sup><i>A'</i>states, respectively. Theoretical calculations give the Frank-Condon factors of 0.9268, 0.9958 and 0.9248 for the $mathop Xlimits^ sim $<sup>2</sup><i>A'</i>(0,0,0) to $mathop Alimits^ sim $<sup>2</sup><i>A'</i>(0,0,0), $mathop Blimits^ sim $<sup>2</sup><i>A''</i>(0,0,0) and $mathop Climits^ sim $<sup>2</sup><i>A'</i>(0,0,0) transitions. All three excited states are the bright states with considerable oscillator strength to the ground state. Based on the Frank-Condon factor and lifetime of excited states, the $mathop Xlimits^ sim $<sup>2</sup><i>A'</i>(0,0,0) → $mathop Blimits^ sim $<sup>2</sup><i>A''</i>(0,0,0) transition is suggested as the main cooling cycle for the CaSH molecule. The corresponding pump light wavelength is 678 nm. By exciting the vibrational excited states (0,1,0) and (0,0,1) of the $mathop Xlimits^ sim $<sup>2</sup><i>A'</i> state to $mathop Alimits^ sim $<sup>2</sup><i>A'</i>(0,0,0) using lasers at 664 nm and 668 nm, respectively, the optical cooling branch ratio of CaSH is expected to exceed 0.9998.