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REVIEW 2 major objections 6 minor

Some Integrability Properties of $m$-Subharmonic Functions

T0 review · 2 major / 6 minor · reviewed 2026-08-01 · deepseek-v4-flash

Pith's one-line read For every m-subharmonic function, the normalized ball maximum at a point always equals the m-Lelong number, and a new capacity-decay condition yields the conjectured L^p range for a large class of such functions.

desk verdict Solid paper with real results, but the proof of the main maximum-identity theorem leans on an unstated tangent-uniqueness theorem that needs verification before publication. read the letter →

arxiv 2607.21144 v2 pith:CCBSDMYH submitted 2026-07-23 math.CV

classification math.CV MSC 32U0532U2532W2035J60
keywords m-subharmonicfunctionsm-LelongnumberHessiancapacityintegrabilityexponentssharpconjecturestrongopennessradialsingularitiespower-logarithmicmodels
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The reading

This paper establishes that for every m-subharmonic function — the class between subharmonic and plurisubharmonic in C^n, defined by a Hessian eigenvalue condition — the normalized limit of the maximum value on shrinking balls equals the m-Lelong number, a measure of singularity strength. It also introduces a scale of local Hessian-capacity conditions: if the capacity of deep sublevel sets decays like t^{-(m+δ)}, then the function is locally integrable with every power s < (m+δ)n/(n-m). At the critical case δ=0, this condition is satisfied by compact singularities, local energy classes, and radial germs, giving precisely the strict subcritical range predicted by the long-standing sharp integrability conjecture for these classes. The paper further gives explicit radial examples showing that the direct strong-openness analogue and the direct exponential-integrability analogue from the plurisubharmonic case both fail when m

What carries the argument

The main device is a scale of local Hessian-capacity conditions C_{m,δ}. For a compact set K inside a bounded m-hyperconvex domain D, the relative Hessian capacity Cap_m(E,D) is defined by a supremum of Hessian masses of comparison functions; the condition asks that the capacity of K∩{u<A-t} decays at least like t^{-(m+δ)}. Combined with a volume-capacity inequality and the layer-cake formula, this decay forces L^s integrability with the stated range. The second load-bearing object is the ball-maximum limit ℓ_u(a)=2 lim M(u,a,r)/φ_m(r), which is shown to equal the m-Lelong number by a tangent-rescaling argument. The radial Hessian test and the classification of power-logarithmic singularitie

What would settle it

Take any local m-subharmonic germ with positive m-Lelong number at 0 and compute both 2 lim_{r↓0} M(u,0,r)/φ_m(r) and the spherical-mean limit defining the m-Lelong number. The theorem predicts they are exactly equal; any germ where these differ — for instance one whose rescalings r^{2q}u(rw) converge to a non-radial limit with the same spherical mean but different maximum — would falsify it. Equivalently, checking whether the rescaled sequence always has an L1_loc limit of the form -ν/(2q)|w|^{-2q} settles the issue.

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Extended reading notes

Core claim

The paper's central identity is ν_u(a) = 2 lim_{r↓0} M(u,a,r)/φ_m(r), valid for every m-subharmonic function u at a point a, where M is the maximum over the ball of radius r and φ_m is the model function (-(r^{2q})/(q))^{-1} with q=(n-m)/m. The proof rescales u by r^{2q}, using a strong uniqueness theorem for tangents to force the rescaled functions to converge in L1_loc to the model singularity -ν/(2q)|w|^{-2q}; then the spherical-mean formula and a maximum principle squeeze the normalized maximum to the same limit. The paper's second main result is the capacity-decay criterion: if u satisfies C_{m,δ}, namely Cap_m(K∩{u<A-t},D) ≤ C t^{-(m+δ)} locally, then u ∈ L^s_loc for every s < (m+δ)n/(

Load-bearing premise

The proof of the ball-maximum identity relies on a strong uniqueness theorem for tangents of m-subharmonic functions whose precise hypotheses are not reproduced; if some local germ admits a non-radial tangent outside that theorem, the equality could fail.

Editorial extensions

If this is right

  • The equality between ball-maximum limit and m-Lelong number gives a practical way to read singularity strength from supremum asymptotics, without computing spherical means.
  • For radial m-subharmonic germs, the maximum identity turns into a direct verification of C_m, yielding the full strict range p < nm/(n-m) for all such germs.
  • Energy classes of finite Hessian mass automatically satisfy C_{m,p}, recovering known Sobolev-type integrability exponents and going beyond the critical range.
  • The counterexamples show that the classical route from bounded exponents to exponential integrability is blocked when m<n; a substitute must involve capacity or tangent profiles rather than only the m-Lelong number.
  • If the critical capacity condition C_m were proved for every local m-subharmonic germ, the long-standing sharp integrability conjecture would follow for all m between 1 and n.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • The capacity scale may be nearly necessary: it appears plausible that a germ satisfying the sharp L^p range with quantitative control on tails forces sublevel capacity decay of order at least m, so C_m could characterize the conjecture's range (a testable direction).
  • The failure of lower semicontinuity in the L1_loc topology is tied to the topology; stronger metrics based on capacities or energies might restore semicontinuity for the integrability-exponent functional and could be worth investigating.
  • Because radial germs satisfy C_m, a promising test toward the full conjecture is whether sums or convex combinations of radial singularities still satisfy C_m; a counterexample there would reveal an intrinsically non-radial obstruction.
  • The ball-maximum identity may extend to directional refinements — replacing balls with sectors or ellipsoids could yield directional m-Lelong numbers and sharp directional integrability, though the radial rigidity of tangents would be lost.
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Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

2 major / 6 minor

Summary. The paper studies local L^p integrability of m-subharmonic functions for 1≤m<n. It classifies radial power-logarithmic singularities u_{α,β}, determines their m-subharmonicity and exact L^p intervals, and uses them to show that the direct Guan–Zhou strong-openness statement and the direct Skoda criterion in terms of the m-Lelong number both fail in the range m<n. It proves upper/lower semicontinuity properties of the local integrability exponent, including a failure of lower semicontinuity in the function variable on SH_m and a closed endpoint example. It introduces a Hessian-capacity scale (C_{m,δ}) and proves, via the Dinew–Kołodziej volume-capacity inequality and layer-cake formula, that C_{m,δ} implies u∈L^s_loc for every s<(m+δ)n/(n-m); energy classes E_{p,m} are shown to satisfy C_{m,p}. It also answers Benali–Ghiloufi Problem 1 by proving the normalized ball-maximum limit equals the m-Lelong number, using the strong uniqueness theorem for tangents as cited from Dinew–Kołodziej, and shows that radial germs satisfy C_m. The paper is clearly written and the explicit computations are checkable, but the proof of the ball-maximum formula depends on an externally cited tangent-uniqueness theorem whose statement and hypotheses are not reproduced.

Significance. If correct, the paper resolves two open problems of Benali–Ghiloufi and gives a useful capacity-based route toward Błocki's conjecture. The explicit radial counterexamples to direct strong openness and direct Skoda-type criteria are valuable and carefully computed; the endpoint classification of power-logarithmic models is a solid contribution. The capacity criterion (C_{m,δ}) and its application to energy classes are clean and constitute the strongest self-contained part of the paper. However, the central equality in Theorem 8.1 is not self-contained: it rests on the strong uniqueness theorem for tangents, which is neither stated nor verified for arbitrary m-subharmonic germs. The paper is honest about what remains open, and the radial C_m theorem is a nice positive use of the Benali–Ghiloufi mean-value machinery. Overall the manuscript deserves publication after the missing tangent-uniqueness input is made precise.

major comments (2)
  1. [§8.1, Eq. (8.2)] The proof of Theorem 8.1 rests entirely on the assertion that the rescalings u_r(w)=r^{2q}u(rw) converge in L1_loc to U(w)=-ν_u(0)|w|^{-2q}/(2q) (or 0), attributed to [6, Thm 3.1]. The statement and hypotheses of that theorem are not reproduced. Is convergence for all r>0 or only along subsequences? Does it require u to have finite Hessian mass, a tame singularity, or a special normalization? If any extra hypothesis is needed, it must be verified for arbitrary u∈SH_m with u(0)=-∞. Without (8.2), the Hartogs bound (8.3) fails and the reverse inequality ℓ_u(a)≥ν_u(a) is unproved. Please quote the theorem and explain why non-radial homogeneous tangents (possible for m=n, e.g., log|z1z2| under the logarithmic scaling) are excluded when 1≤m<n.
  2. [§9.1, Theorem 9.1] The verification of (C_m) for radial germs depends on the ball-capacity formula Cap_m(B(a,ρ),B(a,R0))=c_{n,m}(ρ^{-2q}-R0^{-2q})^{-m}. The text says 'Computing the Hessian mass of this radial extremal function gives...' but gives no computation or reference. This estimate is load-bearing: together with ρ~(A/(qt))^{1/(2q)} it yields the t^{-m} decay that defines C_m. Please include the Hessian-mass computation of h_ρ, check admissibility (-1≤h_ρ≤0), and justify monotonicity of relative capacity in the comparison. A reference to a standard capacitary estimate for balls would also suffice.
minor comments (6)
  1. [Abstract] Typo: 'partial comfirmation' should be 'partial confirmation'.
  2. [§3 and later] Cross-references are inconsistent: 'Theorem 2.1' in the proof of Theorem 3.1 should be 'Lemma 2.1'; 'Theorem 3.2' in Proposition 5.2 and Theorem 8.3 should be 'Proposition 3.2'.
  3. [§6] The sentence 'No counterexample is neither known in those sources' has a double negative and should be rephrased, e.g., 'No counterexample is known in those sources.'
  4. [§8.3] The phrase 'Part (i) is Theorem 5.1' should refer to 'Proposition 5.1'.
  5. [§9.1] In the convexity computation, F(s)=f(φ_m^{-1}(s)) relies on φ_m^{-1}(s) being positive; the notation is understandable but should be stated explicitly to avoid confusion.
  6. [Table 1] The last row label 'Condition C_{m,δ} below' appears to mean 'above' (since the condition is introduced in Section 7, not below the table). Please correct.

Circularity Check

0 steps flagged · score 0.0 of 10

No significant circularity: central claims reduce to external theorems and direct computations, not to the paper's own assumptions.

full rationale

The derivation chain is not circular. Theorem 8.1's equality between the m-Lelong number and the normalized ball-maximum limit is obtained by combining the external strong-uniqueness theorem of Harvey-Lawson / Dinew-Kołodziej (eq. (8.2)) with the Benali-Ghiloufi spherical-mean formula (4.1) and Hartogs' lemma; the coefficient in U is fixed by the definition of ν_u, and the convergence assertion is an imported external result, not an assumption equivalent to the conclusion. The capacity-integrability results (Theorem 7.2, Proposition 7.3) rest on the Dinew-Kołodziej volume-capacity inequality and the Åhag-Czyż sublevel estimate (7.4), quoted from prior work, then apply a standard layer-cake argument; no fitted parameter is renamed as a prediction. The power-logarithmic classification is an explicit calculation. The only self-reference, [10], appears in Remark 4.3 and Section 10 as methodological motivation for replacing Skoda-type exponential integrability with capacity estimates; it is not used to prove Theorem 8.1, Theorem 7.2, or any central integrability statement. A possible correctness concern is that the paper does not reproduce the hypotheses of [6, Thm 3.1] before invoking (8.2), but a missing or unverified external hypothesis is a correctness risk, not circularity.

Assumptions & free parameters 0 free parameters · 5 assumptions · 0 invented entities

The central new results are obtained by combining cited external theorems (tangent uniqueness, volume-capacity, sublevel estimates) with explicit radial calculations. No free parameters are fitted, and no new entities are postulated. The main unverified external input is the strong uniqueness theorem [6, Thm 3.1], which is load-bearing for Theorem 8.1.

assumptions (5)
  • domain assumption Strong uniqueness theorem for tangents of Harvey–Lawson, as stated for m-subharmonic functions by Dinew–Kołodziej [6, Theorem 3.1]: the rescalings u_r(w)=r^{2q}u(rw) converge in L^1_loc to U(w) = -ν_u(0)/(2q)|w|^{-2q} (or 0 if ν=0).
    Used in the proof of Theorem 8.1 (Section 8.1, eq. (8.2)) to identify the tangent at a point with a multiple of the fundamental solution. If this theorem is false or has additional hypotheses, the equality (8.1) fails.
  • domain assumption Dinew–Kołodziej volume-capacity inequality: Vol(E) ≤ C_{D,K,τ} Cap_m(E,D)^τ for 1<τ<n/(n-m) (eq. (7.1)).
    Input to Theorem 7.2; converts capacity decay of sublevel sets into volume decay and hence L^s integrability.
  • domain assumption Åhag–Czyż sublevel estimate: Cap_m({u<-2t},D) ≤ 2^{m+p} e_{p,m}(u) t^{-(m+p)} [1, Lemma 5.2].
    Used in Proposition 7.3 to show energy classes satisfy C_{m,p}.
  • domain assumption Benali–Ghiloufi spherical-mean formula and convexity of M(u,a,·) with respect to φ_m [2].
    Used in the definition of ν_u (eq. (4.1)) and in Sections 8–9; the maximum convexity is used in Theorem 9.1.
  • standard math Standard stability properties of SH_m: stability under finite maxima, decreasing limits, and extension across points where u→-∞ (Lemma 2.2).
    Used throughout; these are established in [4, Proposition 3.1] and [2, Proposition 1(6)].

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Pith. "Pith review of Some Integrability Properties of $m$-Subharmonic Functions." pith.science (2026). https://pith.science/paper/CCBSDMYH

@misc{pith2026260721144,
  author       = {Pith},
  title        = {Pith review of: Some Integrability Properties of $m$-Subharmonic Functions},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/CCBSDMYH}},
  note         = {Machine review of arXiv:2607.21144}
}
abstract

Let $1\le m<n$ and let $u$ be an $m$-subharmonic function on a domain in $\mathbb{C}^n$. We study local exponential and polynomial integrability, with particular attention to the sharp polynomial exponent predicted by B{\l}ocki's conjecture. Explicit radial examples show that direct analogues of the Guan--Zhou strong openness theorem and Skoda's integrability criterion formulated in terms of the $m$-Lelong number fail when $m<n$. We classify a family of radial power-logarithmic singularities and determine the exact $L^p$-integrability range for each member, including endpoint behavior. We resolve two problems posed by Benali--Ghiloufi. The normalized limit of the ball maximum always equals the $m$-Lelong number; this follows by combining their spherical-mean formula with the strong uniqueness theorem for tangents. The pointwise integrability exponent is lower semicontinuous in the base point. However, even when restricted to $SH_m$, it is not lower semicontinuous with respect to the $L^1_{\loc}$ topology. We also disprove their polynomial openness conjecture using an explicit power-logarithmic endpoint example. Finally, we introduce a scale of local Hessian-capacity conditions, denoted by $C_{m,\delta}$. The volume-capacity inequality and the layer-cake formula yield $$u\in L^s_{loc}\quad\text{for every}\quad s<\frac{(m+\delta)n}{n-m}.$$ The critical condition $\mathrm C_{m,0}=\mathrm C_m$ holds for negative functions of finite total Hessian mass with relatively compact deep sublevel sets, and for radial functions. More generally, functions in the energy class $\mathcal E_{p,m}$ satisfy $\mathrm C_{m,p}$, recovering the full {\AA}hag--Czy{\.z} Sobolev exponent. These results provide partial progress toward B{\l}ocki's conjecture, which has remained open for more than two decades.

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