Comparing probability distributions f-divergences, optimal transport, and the objective map.
Which notion of closeness?
Motivation
Every generative model minimizes “distance from model to data.” The choice of divergence fixes the objective, the gradients, and the failure modes. Three families:
f-divergences: a convex f of the ratio p/q,
integral probability metrics: the largest mean gap,
optimal transport: the cheapest way to move mass.
01
The f-divergence family
one convex generator, many divergences
The f-divergence template
The f-divergence
D_f(P\|Q) = \mathbb{E}_{x\sim Q}\bigl[f(p/q)\bigr] for convex f with f(1)=0.
Proof thatD_f \ge 0: \mathbb{E}_Q[f(p/q)] \ge f(\mathbb{E}_Q[p/q])
= f(1) = 0. Jensen, once, for the whole family. \blacksquare
Convexity of f yields non-negativity.
Another application of Jensen gives data processing: pushing P and Q through any channel K only loses distinguishability, D_f(PK\,\|\,QK) \le D_f(P\|Q), for every f at once.
A gallery of generators
The gallery
One curve f per divergence:
KL: u\log u · reverse KL: -\log u
Pearson \chi^2: (u-1)^2
Hellinger: (\sqrt u-1)^2
total variation: \tfrac12|u-1|
Jensen–Shannon (symmetric)
\alpha-family: a parameter from reverse to forward KL; its log-transform is Rényi’sD_\alpha
Near P=Q all agree, \propto f''(1)\,\chi^2; they differ only far apart.
The gallery, numerically
The numbers
Each generator gives a different number on the same pair; KL is asymmetric, JS symmetric and capped below \log 2:
expectations only, no densities. The ordinary GAN is the Jensen–Shannon case.
Tight only at the right critic
The f-GAN
For the \chi^2 generator the bound hits the true divergence exactly at the optimal critic T^\star = f'(p/q), and any other critic falls short:
exact chi^2(P||Q) = 1.0133
bound at the optimal critic = 1.0133
bound at a perturbed critic (scale 0.5): 0.9678
bound at a perturbed critic (scale 1.0): 0.3661
bound at a perturbed critic (scale 2.0): 0.9600
An undertrained critic biases the estimate low; the adversary’s job is to make the bound tight.
Forward vs. reverse KL
Mode geometry
Same target, two optima: forward KL (maximum likelihood) must cover every mode; reverse KL (variational inference) concentrates on one, paying \log(1/0.7) nats for the mass it drops:
\mathrm{TV}(P,Q) = \sup_A|P(A)-Q(A)| = \tfrac12\|p-q\|_1. Hand a tester one sample: the best test succeeds with probability \tfrac12(1+\mathrm{TV}); in the cryptographers’ convention, an advantage of exactly \mathrm{TV}.
Pinsker: \mathrm{TV} \le \sqrt{D_{\mathrm{KL}}/2}, so a small KL bounds the distinguishing advantage of every event.
Pinsker’s constant is sharp
A stress test
Across ten thousand random pairs the ratio \mathrm{TV}/\sqrt{D_{\mathrm{KL}}/2} never exceeds 1, and near-fair coins push it to 0.999999:
max TV / sqrt(KL/2) over 10,000 random pairs: 0.9926
coins 1/2 vs 1/2+0.1: TV / sqrt(KL/2) = 0.989881
coins 1/2 vs 1/2+0.01: TV / sqrt(KL/2) = 0.999900
coins 1/2 vs 1/2+0.001: TV / sqrt(KL/2) = 0.999999
The factor \tfrac12 cannot be improved.
IPMs and the kernel trick
Sample-only
An integral probability metric is \sup_{f\in\mathcal F}\mathbb{E}_P[f]-\mathbb{E}_Q[f]. Over an RKHS ball it becomes MMD, a closed-form kernel expectation with no critic and no densities:
MMD^2, same distribution : +0.00054
MMD^2, mean shifted 0.5 : +0.05890
A half-\sigma shift jumps \mathrm{MMD}^2 by two orders of magnitude.
Optimal transport and Wasserstein
Moving mass
On disjoint supports every f-divergence is constant (zero gradient) while W_1 still moves smoothly. That is the WGAN.
Dual (Kantorovich–Rubinstein): the 1-Lipschitz critics. In one dimension, W_1 = \int|F_P - F_Q|.
One integral replaces a linear program
Wasserstein-1
The CDF formula and a 36-variable transport LP agree to ten digits:
W1 via the CDF formula : 1.7000000000
W1 via the primal LP : 1.7000000000
Beyond one dimension no such formula exists, and the LP has n^2 variables.
Sinkhorn and entropic regularization
Entropic OT
Sinkhorn’s row/column rescalings solve the -\varepsilon H(\gamma)-regularized plan on a GPU. At \varepsilon=1 the diffuse plan costs 1.77 vs 1.70; decreasing \varepsilon approaches the LP’s monotone transport plan:
the normalizer-free divergence, and the unifying table
Scores Cancel Unknown Normalizing Constants
Fisher divergence
s_P(\mathbf x) = \nabla_{\mathbf x}\log p drops the intractable Z entirely, since \nabla\log Z = 0. The Fisher divergence compares score fields, the basis of score matching and diffusion.
Normalizer-blindness, numerically
The point
Rescaling the density leaves the score unchanged to floating-point precision, and the Gaussian Fisher divergence matches its closed form:
mixture score, max |analytic - numerical|: 3.52e-04
score change from rescaling p by 2.7 : 1.82e-12
Fisher divergence N(0,1)||N(1,1): quadrature 0.500000, closed form 0.500000
This is why score matching works where density estimation cannot.
Stein’s identity and goodness of fit
KSD
For any smooth f, \mathbb{E}_P[f' + f\,s_P] = 0: a fingerprint of P that needs only its score. A systematic population violation distinguishes the distributions; a finite-sample test still requires calibration:
rng = np.random.default_rng(7)z = rng.standard_normal(1_000_000)# Stein operator for P = N(0,1): (A_P f)(x) = f'(x) - x f(x)for name, f, fprime in [('x^3', lambda t: t **3, lambda t: 3* t **2), ('sin x', np.sin, np.cos)]: val = (fprime(z) - z * f(z)).mean()print(f"E[ f'(Z) - Z f(Z) ] for f(x) = {name}: {val:+.4f}")
E[ f'(Z) - Z f(Z) ] for f(x) = x^3: +0.0020
E[ f'(Z) - Z f(Z) ] for f(x) = sin x: +0.0005
The kernel Stein discrepancy turns this identity into a test statistic; its descent direction yields SVGD.
These correspondences describe population objectives under their idealized critic and model assumptions; finite optimization can behave differently.
Divergences Encode Different Modeling Priorities
Wrap-up
f-divergence = \mathbb{E}_Q[f(p/q)]; Jensen gives D_f \ge 0and its DPI.
The \alpha/Rényi family sweeps reverse \to forward KL.
Fenchel duality turns any f into a critic game (the f-GAN); GAN is the JS case.
Forward KL tends to cover modes; reverse KL may concentrate on one.
TV is the best single-sample advantage; Pinsker bounds it by \sqrt{\mathrm{KL}/2}.
W_1 remains informative on disjoint supports (WGAN), though not necessarily smooth; Sinkhorn approaches the unregularized transport problem as regularization vanishes.
The score drops Z; the Fisher/Stein row powers diffusion and SVGD.
Next: mutual information, a divergence from independence, put to work in representation learning.