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Reciprocity inequality for logarithmic potentials
Statement
Assume the Axiom of Choice. Let be compact with and let be its equilibrium measure. Then for every compactly supported Borel probability measure on ,
The Axiom of Choice enters only through the existence of the equilibrium measure and through Frostman's theorem; the reciprocity identity itself and the infimum estimate are choice-free.
Facts & Assumptions
Given: a compact set with , its equilibrium measure , a compactly supported Borel probability measure on , the logarithmic kernel with diagonal value , the potential and the mixed energy of Logarithmic potential and energy of a positive compactly supported measure, and the Axiom of Choice (The Axiom of Choice).
For a finite positive Borel measure of compact support, , and for one has on the product of the support with itself and , independently of ; for a pair of such measures and the same shifted kernel is nonnegative on the product of the two supports and , independently of (Logarithmic potential and energy of a positive compactly supported measure).
and when and otherwise, so is equivalent to , and then (Robin constant and logarithmic capacity of a compact set).
Assume the Axiom of Choice: a compact nonempty with has exactly one equilibrium measure , and ; the measure is a Borel probability measure carried by , so its support is a nonempty compact subset of (Existence and uniqueness of the equilibrium measure, Probability measures and probability spaces).
Assume the Axiom of Choice: with as above, for every (Frostman inequalities and quasi-everywhere equilibrium equality).
Tonelli's theorem computes the integral of a nonnegative product-measurable function on a -finite product as either iterated integral (Tonelli's theorem for nonnegative measurable functions on a sigma-finite product); the support of a finite positive Borel measure is closed, carries , and every closed set carrying contains it (Support of a finite Borel measure on the plane).
Proof
By [F2] and [F3] the hypothesis gives , the equilibrium measure , and ; since and are compact and nonempty, , and as the set is not a singleton, so ; fix .
Frostman bound. By [F4] one has pointwise on , and is a probability, so .
On one has , so the shifted kernel is a nonnegative Borel function there; Tonelli [F5] applied to the product measure therefore gives , both sides being elements of .
The infimum bound. For and , one has , including , where the kernel has value . Integrating this pointwise bound against the probability , carried by its support, gives on . Thus and : for finite , integrate against the probability carried by ; for , the potential is everywhere on and its integral is .
For each one has as extended reals, since pointwise and ; integrating against the probability gives , and symmetrically , the identities being understood in with .
Reciprocity. Comparing the two expressions for the common value in step 2.1 gives ; subtracting the finite real number yields the reciprocity identity .
Combining steps 4.1, 2.2 and 1.2, , and by [F2]; this is the assertion. The Axiom of Choice was used only through [F3] and [F4].
Remarks
What reciprocity does and does not require. The identity is a Fubini statement for the kernel on the product of the two supports; no finiteness of is assumed, and the value is allowed on both sides. The shifted kernel is nonnegative on that product, which is what makes Tonelli applicable without any integrability hypothesis.
Sharpness of the inequality. The inequality is the classical reciprocity inequality of Saff, Proposition 1.13; equality holds for whenever at every point of . Quasi-everywhere equality alone (Frostman inequalities and quasi-everywhere equilibrium equality) does not suffice for the infimum over all of : exceptional polar points may have smaller potential.
Depends on
- The Axiom of Choice
- Logarithmic potential and energy of a positive compactly supported measure
- Robin constant and logarithmic capacity of a compact set
- Probability measures and probability spaces
- Support of a finite Borel measure on the plane
- Existence and uniqueness of the equilibrium measure
- Frostman inequalities and quasi-everywhere equilibrium equality
- Tonelli's theorem for nonnegative measurable functions on a sigma-finite product
Used by
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Sources
- E. B. Saff, Logarithmic Potential Theory with Applications to Approximation Theory, §1 (standard reference, not scraped)
- B. Khoruzhenko, LTCC Potential Theory notes, §3 (standard reference, not scraped)