Matching the dimensions of \( [M] \), \( [L] \), and \( [T] \) on both sides of \( A = G^{\alpha}M^{\beta}c^{\gamma} \) gives three equations: \( -\alpha+\beta=0 \), \( 3\alpha+\gamma=2 \), and \( -2\alpha-\gamma=0 \). We can solve these in a different order to see which set of values holds. From the mass equation, \( \beta = \alpha \). From the length equation, \( \gamma = 2-3\alpha \). Substituting this into the time equation gives \( -2\alpha-(2-3\alpha)=0 \), which simplifies to \( \alpha - 2 = 0 \), so \( \alpha = 2 \). This gives \( \beta = 2 \) and \( \gamma = 2-3(2) = -4 \).
Only option (2) is consistent with both derived relations simultaneously.
Therefore, the correct answer is \( \alpha = 2, \beta = 2, \gamma = -4 \).
Match List-I with List-II.

