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L2 limits of spherical Gaussian multiplicative chaos test functionals
Statement
Assume the covariance and smoothing conventions of the spherical Gaussian free field and its normalized chaos regularization defined earlier on this page. For and every real continuous on , the scalar random variables
converge in as . Their limit is unchanged when one smoothing family is replaced by another. For real continuous , the limiting functionals satisfy
The statement concerns scalar test-function limits; it does not assert a Radon-measure-valued version for the full range .
Statement references
Facts & Assumptions
Given: is a centered Gaussian random distribution on the compact sphere, has the logarithmic singularity specified by the GFF definition, and is its normalized regularization.
Gaussian free field on the Riemann sphere in the Liouville convention: the covariance is , paired on tests against the smooth round area measure ; the GMC integration measure remains ; every pair of admitted smoothings has mixed covariance converging off the diagonal and bounded above by uniformly.
, so .
Proof
The covariance bound in [F1] implies for a constant independent of the two smoothing parameters. The background density is continuous and bounded in every compact chart, so near the diagonal its integral is bounded by a constant times by [A1]; away from the diagonal it is bounded.
If are jointly centered Gaussian, their moment-generating function gives . Fubini applied to the absolutely integrable kernel bound in step 1.1 therefore gives .
The off-diagonal covariance convergence in [F1], the integrable bound in step 1.1, and dominated convergence show that the moment in step 2.1 tends to as . Taking in the same Gaussian exponential identity gives for every .
Expand into two self terms and two mixed terms. By step 3.1 each term tends to with its indicated sign, so the limit is . Thus the regularized scalar functionals are Cauchy in the complete space and have an limit.
For two smoothing families, the same uniform covariance bound and off-diagonal limit in [F1] give the same mixed second-moment limit in step 3.1. Repeating the four-term difference calculation of step 4.1 shows that their scalar limits agree. The limits have the first and second moments asserted in the Statement by step 3.1.
Remarks
The proof stops at scalar limits. Turning the simultaneous family of limits into a finite Radon random measure, and extending existence and mollifier-independence to , require additional arguments. The cited lecture notes prove the L2 case and refer elsewhere for the remaining subcritical interval; they are not treated as supplying those local arguments.