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TheoremStatement: AI-adaptedProof: AI-adaptedprecheck passaudited 2026-08-31
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Equality in Minkowski's inequality for 1<p<

Statement

Let 1<p< and let f,gLp(μ). Then equality holds in Minkowski's inequality

f+gp=fp+gp

if and only if at least one of f,g is zero almost everywhere, or there is a constant λ>0 such that

f=λgμ-almost everywhere.

Facts & Assumptions

Given: An exponent 1<p< and functions f,gLp(μ).

[L1]

Minkowski's inequality has already been proved (Minkowski's inequality for integrals, including p=).

[L2]

The equality case in Holder has already been proved (Equality in Holder's inequality for 1<p<).

[L3]

A nonnegative measurable function has integral 0 exactly when it vanishes almost everywhere (A nonnegative measurable function has integral 0 exactly when it vanishes almost everywhere).

[L4]

The nonnegative integral is additive (Additivity of the nonnegative Lebesgue integral).

Proof

Proof technique: Examine the Holder step in the standard proof of Minkowski. Equality forces the nonnegative functions f and g to be proportional almost everywhere, and the pointwise triangle inequality then forces the same sign.

1.1

If at least one of f,g is zero almost everywhere, then equality is immediate.

L1given
1.2

If f=λg almost everywhere for some λ>0, then [L1, given] f+g=(λ+1)g almost everywhere, so f+gp=(λ+1)gp=fp+gp.

1.3

Conversely, assume equality in Minkowski and that neither f nor g is zero almost everywhere. [L1, L2, L3, L4] The proof of [L1] showed that equality in Minkowski can only occur when both inequalities f+gf+g and ff+gp1dμfpf+gpp1 and its g-analogue are equalities. The second and third equalities force the pairs (f,f+gp1) and (g,f+gp1) to satisfy Holder equality. By [L2], this makes f and g proportional almost everywhere. The first inequality then forces (f+g)f+g to have integral 0; [L3] and [L4] therefore give f+g=f+gμ-almost everywhere.

2.1

Let f=cg almost everywhere with c>0. Then [step 1.3, algebra] on the set where g0, step 1.3 gives equality in the real triangle inequality for f and g, so they have the same sign there. Hence f=cg almost everywhere on {g0}, and on {g=0} both sides vanish. Thus f=λg almost everywhere for λ=c>0.

3.1

Steps 1.1 and 1.2 prove sufficiency, while steps 1.3 and 2.1 prove necessity.

step 1.1step 1.2step 1.3step 2.1

Depends on

Used by

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Sources