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Optimal discriminator and Jensen–Shannon divergence in the unrestricted GAN game

Statement

Let (X,A,μ) be a measure space and let P,Q be probability measures with finite-valued nonnegative measurable densities p,q relative to μ, normalized by ∫p dμ=∫q dμ=1. For every measurable discriminator D:X→[0,1], define

V(D;P,Q)=∫pln⁡D dμ+∫qln⁡(1−D) dμ,

extending ln⁡0=−∞ and making each zero-density term 0⋅(−∞) equal to 0. Let C(P,Q) be the supremum of V(D;P,Q) over all such D. Put m=(p+q)/2, r=p/m and s=q/m where m>0, set r=s=0 where m=0, define ϕ(0)=0 and ϕ(t)=tln⁡t for t>0, and set JS⁡μ(P,Q)=12∫mϕ(r) dμ+12∫mϕ(s) dμ. Then the measurable discriminator

D∗(x)={p(x)p(x)+q(x),p(x)+q(x)>0,12,p(x)+q(x)=0

maximizes V, and C(P,Q)=−ln⁡4+2JS⁡μ(P,Q). Consequently C(P,Q)≥−ln⁡4, with equality if and only if P=Q. Over the unrestricted class of probability densities, equality of the generator law with the data law is the unique global distribution optimum. This identity does not assert convergence of finite neural alternating optimization.

Facts & Assumptions

Given: A measure space (X,A,μ), probability measures P,Q with finite-valued nonnegative measurable densities p,q, and a measurable discriminator D:X→[0,1].

[F1]

GAN minimax objective and its distributional domain: V(D;P,Q)=−∫p(−ln⁡D) dμ−∫q(−ln⁡(1−D)) dμ, where 0⋅(+∞)=0, and C(P,Q) is the supremum over every measurable D:X→[0,1].

[F2]

Density-defined Jensen–Shannon divergence: with m=(p+q)/2, r=p/m, s=q/m on m>0 and r=s=0 otherwise, JS⁡μ(P,Q)=12∫mϕ(r) dμ+12∫mϕ(s) dμ.

[F3]

Nonnegativity and equality for density Jensen–Shannon divergence: the two integrands mϕ(r) and mϕ(s) are integrable, and JS⁡μ(P,Q) is finite and nonnegative, with equality exactly when P=Q.

[F4]

The natural logarithm has derivative 1/x and equals the integral from 1 to x of 1/t: ln⁡ is differentiable on (0,∞) with derivative 1/t.

[F5]

Order, continuity, range, and the product, quotient, and reciprocal laws for the natural logarithm: ln⁡ is strictly increasing, ln⁡1=0, and ln⁡(xy)=ln⁡x+ln⁡y for x,y>0.

[F7]

The Lebesgue integral is linear on L1(μ): the Lebesgue integral is linear on integrable functions.

[F8]

A map into Rn is measurable exactly when its coordinates are measurable: a map into R2 is measurable if its two coordinates are measurable.

[F9]

Composition with a Borel measurable outer map preserves measurability: composing a measurable map with a Borel map preserves measurability.

[F12]

A function differentiable at c is continuous at c: a function differentiable at every point of an open interval is continuous at every point of that interval.

[F13]

The mean value theorem, as the case g(x)=x of Cauchy's: for f continuous on [a,b] with a<b and differentiable on (a,b) there is c∈(a,b) with f(b)−f(a)=f′(c)(b−a): a function continuous on a closed interval and differentiable on its interior has a point where its derivative equals the average rate of change across the interval.

[F14]

Additivity of the nonnegative Lebesgue integral: for nonnegative measurable functions u,v, ∫(u+v) dμ=∫u dμ+∫v dμ.

Proof

1.1F8F9construct

Define F:[0,∞)2→[0,1] by F(a,b)=a/(a+b) when a+b>0 and F(0,0)=1/2. It is continuous on the Borel set {a+b>0} and constant on its singleton complement, hence Borel. By [F8], x↦(p(x),q(x)) is measurable, and [F9] makes D∗=F(p,q) measurable.

1.2givenF4F5F10F11F12F13algebra

Fix x and write a=p(x) and b=q(x). If a,b>0, the function f(y)=aln⁡y+bln⁡(1−y) on 0<y<1 is differentiable with f′(y)=a/y−b/(1−y)=(a−(a+b)y)/(y(1−y)): the derivative of 1−y is −1 by its difference quotient, [F4] differentiates ln⁡, [F10] applies the chain rule, and [F11] gives the sum and scalar rules. The denominator is positive; the numerator is positive for y<y∗:=a/(a+b) and negative for y>y∗. By [F12], f is continuous on every closed subinterval of (0,1). For any y∈(0,y∗), [F13] on [y,y∗] gives c∈(y,y∗) with f(y∗)−f(y)=f′(c)(y∗−y)>0. For any y∈(y∗,1), [F13] on [y∗,y] gives c∈(y∗,y) with f(y)−f(y∗)=f′(c)(y−y∗)<0. At y=0,1 the payoff is −∞. If a=0<b, then f(y)=bln⁡(1−y)≤0=f(0), with equality at y=0. If b=0<a, then f(y)=aln⁡y≤0=f(1), with equality at y=1. If a=b=0, every y gives value 0. In all four cases, D∗(x) maximizes the pointwise payoff.

2.1F1F6F14step 1.1step 1.2

For any measurable D, step 1.2 gives the pointwise loss inequality p(−ln⁡D)+q(−ln⁡(1−D))≥p(−ln⁡D∗)+q(−ln⁡(1−D∗)), with zero-density endpoint terms interpreted as in [F1]. These are nonnegative measurable losses by the definition and its measurability dependencies [F1]. Additivity [F14] and monotonicity [F6] therefore give ∫p(−ln⁡D) dμ+∫q(−ln⁡(1−D)) dμ≥∫p(−ln⁡D∗) dμ+∫q(−ln⁡(1−D∗)) dμ. Taking negatives and using [F1] yields V(D;P,Q)≤V(D∗;P,Q). Since D∗ is measurable by step 1.1, the supremum is attained and C(P,Q)=V(D∗;P,Q).

3.1F1F2F3F5F7step 2.1algebra

On m>0, one has p=mr, q=ms, D∗=r/2 and 1−D∗=s/2. Using 0ln⁡0=0 when r=0 or s=0, the pointwise optimized payoff is mϕ(r)+mϕ(s)−m(r+s)ln⁡2=mϕ(r)+mϕ(s)−2mln⁡2. On m=0, both densities and all displayed products are zero, so the same identity holds. The first two terms are integrable by [F3]; [F1] and [F7] give ∫m dμ=1. Hence [F7], [F2] and ln⁡4=2ln⁡2 [F5] give C(P,Q)=2JS⁡μ(P,Q)−ln⁡4.

4.1F3step 3.1algebra∎

By [F3], JS⁡μ(P,Q)≥0, and it vanishes exactly when P=Q. Step 3.1 therefore gives C(P,Q)≥−ln⁡4 with equality exactly at P=Q. The unrestricted density class contains the data law itself, so this value is attained there and no other generator law attains it. The argument establishes only the distribution-space optimum stated here.

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