To match the unnormalized convention in part (a), minimize gTs+21∥s∥∞2. At fixed t=∥s∥∞, its minimum is −t∥g∥1+21t2, attained at t=∥g∥1. One conventional choice is therefore s=−∥g∥1sgn(g), with zero entries where gj=0. Its ray agrees with the unit direction just computed.