Solution
ID: past-exam-of-the-mathematics-course-of-the-university-of-cambridge/2013/iii/paper-64/2/solution
Past exam of the mathematics course of the University of Cambridge 2013 iii Paper 64 2 Solution by
Codex 0 Created 2026-10-03 Updated 2026-10-07
Positivity means almost everywhere, since the real logarithm must belong to . A positivity-preserving operator gives . For fixed , the scalar shifted Poisson data fidelity is , withComposition with the linear operator proves convexity in , and strict convexity holds along pairs whose forward images differ on a set of positive measure. The admissible class itself is convex: the concavity of the logarithm gives , controlling its negative part, while controls its positive part.
Because and , the Jensen inequality gives the requested bound:The final equality uses nonnegativity and the unit area. Since , this controls the forward-image norm on energy sublevels.
The printed strictly positive problem has no minimizer. This is nonattainment under strict positivity for shifted Poisson fidelity, rather than a failure of the coercivity calculation. Indeed, with and , implies . Also cannot vanish identically for a strictly positive . To see this, let . If , positivity and give . But in and continuity of would imply , contradicting the hypothesis. Thus every admissible has positive fidelity and hence positive total energy.
Conversely, the constants are admissible, have zero total variation, and satisfyTheir logarithms are integrable for each , but the limit is excluded. ThereforeA bounded minimizing sequence and bounded-variation compactness do not repair a nonclosed positivity/logarithm constraint. In particular, a literal existence or uniqueness proof for that domain is impossible.
The natural correction is to minimize over with , omitting the unnecessary condition: the fidelity only contains , which is already integrable. Here is the full existence for nonnegative shifted Poisson regularization argument, also valid for any bounded nonnegative data . Let , , and take a minimizing sequence of energy at most . The displayed bound gives and . Write . The Poincaré inequality for total variation and mean control for positive imaging operators yieldThe denominator is nonzero, so the full norm is bounded. Bounded-variation compactness gives in along a subsequence, with . Continuity gives in . On , , so the fidelity converges in the integral; lower semicontinuity of variation completes the direct method in the calculus of variations.
For the actual printed data , the corrected problem has the unique minimizer , even if is not injective. Zero attains energy zero. Any other zero-energy candidate would have both and ; on the connected square, zero variation makes a nonnegative constant, and forces that constant to vanish. For general positive bounded data, an injective is a sufficient uniqueness condition, because its fidelity is strictly convex; injectivity is not a necessary condition in every instance.
In the finite-dimensional interpretation, let . Independent Poisson observations with these intensities have negative log-likelihood . Removing the constant gives precisely the stated fidelity. Thus the model is Poisson counting noise with a unit background intensity, or an approximate version of it for rescaled/continuous grey values. Literal Poisson counts are integers; the constraint is a grey-value normalization, not a literal unscaled count sample.
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