First, express the event M^2 > m in terms of U and V, then use the joint density to set up a double integral over the region where the condition holds. Evaluate the integral by splitting into cases or using symmetry to simplify, and finally compute the closed-form probability.
Pro tip: Leverage the symmetry between U and V by assuming U > V (so M=U, m=V) and then multiplying by 2, which simplifies the region and integral. Also, sketch the unit square and shade the region to visualize the bounds.
Since M = max(U,V) and m = min(U,V), the condition M^2 > m means that the larger value squared exceeds the smaller value. Consider the two cases: U > V and V > U.
Use the joint density f(u,v)=1 on [0,1]^2. For U > V, the condition becomes U^2 > V, so the region is {0 ≤ v ≤ u ≤ 1, v < u^2}. The integral is ∫_{u=0}^1 ∫_{v=0}^{min(u, u^2)} dv du. By symmetry, multiply by 2 for the other case.
For 0 ≤ u ≤ 1, min(u, u^2) = u^2 because u^2 ≤ u. So the inner integral is ∫_0^{u^2} dv = u^2. Thus the integral for U > V is ∫_0^1 u^2 du = 1/3.
By symmetry, the total probability is 2 * (1/3) = 2/3. Verify that the regions for U > V and V > U are disjoint and cover the event, so no overlap.
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