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Frostman inequalities and quasi-everywhere equilibrium equality
Statement
Assume the Axiom of Choice. Let be compact with and let be its equilibrium measure (Existence and uniqueness of the equilibrium measure). Then
and outside a Borel capacity-polar subset of ; the exceptional set may be taken to be a countable union of compact sets of capacity zero. Here , and cap are those of Logarithmic potential and energy of a positive compactly supported measure, Robin constant and logarithmic capacity of a compact set and the polarity convention of Capacity-polar sets, quasi-everywhere, and subharmonic polar sets.
The Axiom of Choice is spent through the equilibrium-measure existence theorem Existence and uniqueness of the equilibrium measure, applied to and to the nonpolar compact subsets of that occur in the argument, and through the Evans-potential lemma Compact capacity-zero sets and subharmonic minus-infinity loci used for the countable-union closure of the polar class; that lemma assumes only Dependent Choice, which the Axiom of Choice supplies. The potential and energy estimates themselves are choice-free.
Facts & Assumptions
Given: a nonempty compact set with , its equilibrium measure , the Axiom of Choice, and the potential, energy, capacity and polarity conventions of Logarithmic potential and energy of a positive compactly supported measure, Robin constant and logarithmic capacity of a compact set, Capacity-polar sets, quasi-everywhere, and subharmonic polar sets and Support of a finite Borel measure on the plane.
Let be finite positive Borel measures carried by a common compact set , and take . Then on . If , product measure monotonicity gives , hence which is finite when . If and have equal total mass and finite energies, Countable Choice and Strict positivity of logarithmic energy for a zero-mass signed charge give a finite mixed energy and No pointwise monotonicity is asserted: the unshifted kernel changes sign (Tonelli's theorem for nonnegative measurable functions on a sigma-finite product).
For a finite positive Borel measure of compact support, with and diagonal value , is the subharmonic normalisation, computed from the shifted nonnegative kernel for , and the mixed energy is symmetric (Logarithmic potential and energy of a positive compactly supported measure). If then on , so .
and when and otherwise; so is equivalent to (Robin constant and logarithmic capacity of a compact set).
The support of a finite positive Borel measure is closed, carries , is contained in every closed carrier, and if and only if ; in particular every ball about a point of has positive -measure (Support of a finite Borel measure on the plane).
Capacity-polar means that every compact subset has capacity zero; quasi-everywhere means outside a Borel capacity-polar set (Capacity-polar sets, quasi-everywhere, and subharmonic polar sets, Robin constant and logarithmic capacity of a compact set).
Assume the Axiom of Choice: every nonempty compact with has exactly one equilibrium measure , and ; if then and no equilibrium measure is asserted (Existence and uniqueness of the equilibrium measure).
is subharmonic on for every finite positive compactly supported , hence upper semicontinuous with values in , and is lower semicontinuous with values in ; consequently every sublevel set is closed (Distributional Laplacian of a compact logarithmic potential, Subharmonic functions on plane domains).
If is finite positive, compactly supported and on for some real , then on all of (Maximum principle for a compact logarithmic potential).
Assume Dependent Choice. A compact set has if and only if there are a complex domain and a function subharmonic on with ; and if is a specified sequence of compact sets with for every , then there is a function subharmonic on all of , not identically , with on (Compact capacity-zero sets and subharmonic minus-infinity loci).
The Axiom of Choice implies Dependent Choice, which implies Countable Choice (AC implies DC implies countable choice), the choice principle used by [F6].
Proof
By [F2] and [F5] the hypothesis gives and the equilibrium measure with ; is carried by , so by [F3] its support is a nonempty compact subset of with and for every ball about a point of .
Since the kernel is bounded below on , so [F1] gives by Tonelli and ; moreover, by [F1] with the common carrier and , every finite positive measure carried by has , and the mixed energy of two finite positive compactly supported measures with finite energy is finite; in particular for every with .
Minimality inequality: for every with and one has . Indeed, for the convex combination lies in , so by [F2] and [F5]; expanding the double integral of with [F1] gives , so subtracting , dividing by and letting yields , that is .
Claim: for every . Suppose not, and choose with (if any will do); by [F6] the set is open, so there is with on the disc ; put , so by step 1.1. If then is carried by , so by step 2.1, where is a finite real number, , a contradiction; hence . The restriction satisfies and , so has and by step 2.1, while the pointwise bound on and give contradicting step 3.1; so no such exists.
Since and on by step 4.1, the maximum principle [F7] with gives for every , which proves the first assertion and in particular gives the finiteness for every below.
For the set is compact, because is compact and is closed by [F6]; if were compact with , then [F5] applied to would give an equilibrium measure with , and steps 3.1 and 5.1 would give the contradictory chain ; hence every compact subset of has capacity zero.
By step 6.1 each has the property that every compact subset has capacity zero, in the sense of [F4]. Hence is capacity-polar: if is compact, then is a specified countable union of compact sets of capacity zero, so the specified- clause of [F8] supplies a function subharmonic on that equals on all of , and the compact clause of [F8], applied with , gives . Thus is a Borel capacity-polar subset of (it is a countable union of compact sets), and for one has for every , hence , while step 5.1 gives ; therefore on , which is the second assertion.
Remarks
Why the two halves are different. The inequality everywhere is the part that uses the minimality of through the competitor obtained by deleting a small disc of large potential; the reverse inequality needs no minimality beyond the perturbed-copy inequality of step 3.1 and in fact only holds quasi-everywhere, as the isolated-point example of Capacity-polar sets, quasi-everywhere, and subharmonic polar sets shows.
Choice. The Axiom of Choice enters through [F5] for and again for the compact sets of step 6.1, and through [F8] in step 7.1, whose Evans-potential lemma assumes only Dependent Choice; the running argument is otherwise choice-free, and [F6] needs only Countable Choice, which [F9] supplies.
Sharpness of the exceptional set. The exceptional set is a countable union of compact zero-capacity sets, and step 7.1 shows through [F8] that such a union is again capacity-polar (the definition alone tests only compact subsets and does not supply the countable-union closure); so the statement is exactly the classical "equals quasi-everywhere on ".
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
- Support of a finite Borel measure on the plane
- Capacity-polar sets, quasi-everywhere, and subharmonic polar sets
- Subharmonic functions on plane domains
- Existence and uniqueness of the equilibrium measure
- Distributional Laplacian of a compact logarithmic potential
- Strict positivity of logarithmic energy for a zero-mass signed charge
- Maximum principle for a compact logarithmic potential
- Compact capacity-zero sets and subharmonic minus-infinity loci
- AC implies DC implies countable choice
- 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)
- C. Kuehn, Introduction to Potential Theory via Applications, §2.3 (standard reference, not scraped)