Helper lemmas #
The function -exp(-x²/2) tends to 0 as x → ∞.
The integral of x · exp(-x²/2) over (t, ∞) equals exp(-t²/2) for t > 0.
This follows from FTC-2 applied to f(x) = -exp(-x²/2), whose derivative is
f'(x) = x · exp(-x²/2).
The function exp(-x²/2) is integrable on (t, ∞) for t > 0.
The function t⁻¹ * x * exp(-x²/2) is integrable on (t, ∞) for t > 0.
Main theorem #
Goal 0: Mills' inequality (Proposition 1.1 from Rigollet's "High Dimensional Statistics").
For t > 0, the Gaussian tail integral satisfies:
∫_t^∞ exp(-x²/2) dx ≤ (1/t) · exp(-t²/2)
This is the core integral bound underlying Proposition 1.1. The book's statement for general N(μ, σ²) reduces to this by setting μ = 0, σ² = 1.
The proof uses the key observation that for x ≥ t > 0, we have 1 ≤ x/t,
so exp(-x²/2) ≤ (x/t) · exp(-x²/2). Integrating both sides and using FTC
to evaluate ∫_t^∞ (x/t) exp(-x²/2) dx = (1/t) exp(-t²/2) gives the result.