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Existence and geometry of Hermitian metrics with constant second scalar curvature

T0 review · 2 major / 3 minor · reviewed 2026-08-15 · deepseek-v4-flash

Pith's one-line read The paper shows that the existence of Hermitian metrics with constant second Chern or Bismut scalar curvature within a conformal class is governed by the sign of a conformal invariant, the second Gauduchon degree, with unique solutions in…

desk verdict New conformal formulas and examples, but the two main existence proofs have real maximum-principle errors; worth peer review but not acceptance as written. read the letter →

arxiv 2601.20572 v2 pith:PW6USKXW submitted 2026-01-28 math.DG

classification math.DG MSC 53C5553C21
keywords secondscalarcurvatureHermitianmetricsBismutconnectionChernGauduchonmetricconformalclassYamabe-typeproblemdegree
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 asks whether a compact Hermitian manifold, a complex manifold with a metric that need not be Kähler, can be conformally deformed to a metric whose second scalar curvature is constant, where this curvature is a torsion-sensitive trace of the Chern or Bismut connection. The central claim is that the answer is controlled by a conformal invariant, the second Gauduchon degree: the total integral of the second Chern scalar curvature of the canonical Gauduchon metric in the class. When that invariant is zero, there is a unique conformal metric with vanishing second Chern scalar curvature; when it is negative, a unique conformal metric with constant negative second Chern scalar curvature, and in balanced classes the anti-canonical bundle is not pseudo-effective. For the Bismut connection, the paper proves existence of a constant second scalar curvature metric in every conformal class on manifolds with vanishing first Betti number. A final rigidity result shows that compact pluriclosed Gauduchon metrics satisfying a weak Einstein-type condition have constant second Chern scalar curvature, leading to a dichotomy with Kähler–Einstein metrics.

What carries the argument

The key object is the second Gauduchon degree $\Gamma^{(2)}_M(\{\omega\})$, the total integral of the second Chern scalar curvature $S^{(2)}_C$ of the unique Gauduchon metric in the conformal class; it is a conformal invariant that plays the role of a torsion-aware Yamabe invariant. The load-bearing identity is the conformal transformation formula $S^{(2)}_C(\omega_f)=e^{-f}\left(S^{(2)}_C(\omega)-\Delta^C_\omega f\right)$ for the Chern connection, and the analogous formula (3.16) for the second Bismut scalar curvature $S^{(2)}_B$; these convert the geometric problem into solvable semilinear elliptic equations. The Bismut existence proceeds through the functional $Y_q(\varphi)$ (4.3) and the equation $\square_{\omega_B}\varphi=N_1\mu_q\varphi^{q-1}$, while the negative Chern case uses a continuity method with maximum-principle a priori estimates and a uniqueness argument by comparison. The rigidity section uses the sum of the third and fourth Chern–Ricci curvatures $\Theta^{(3)}(\omega)+\Theta^{(4)}(\omega)$, whose $\partial\bar\partial$-closedness yields a linear elliptic equation $\Diamond_\omega f=0$ with only constant solutions on compact pluriclosed Gauduchon manifolds.

What would settle it

Compute the left-hand side of (5.9) at a minimum point $q$ of a solution $f_a$ for $a=1$: the maximum principle gives $S^{(2)}_C(\omega')(q)-\lambda e^{f_1(q)}\ge 0$, i.e. $e^{f_1(q)}\ge S^{(2)}_C(\omega')(q)/\lambda$. Choose a conformal class whose second Chern scalar curvature $S^{(2)}_C(\omega')$ is negative and nonconstant with $S^{(2)}_C(\omega')(q)/\lambda<1$ at the minimum point; then $f_1(q)\le \log(S^{(2)}_C(\omega')(q)/\lambda)<0$, contradicting the asserted uniform lower bound $f_a\ge 0$ in Lemma 5.3.

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Extended reading notes

Core claim

The paper's central discovery is that within a fixed Hermitian conformal class the existence and uniqueness of constant second Chern scalar curvature is decided by the sign of the second Gauduchon degree $\Gamma^{(2)}_M(\{\omega\})=\int_M S^{(2)}_C(\omega_G)\,\omega_G^n/n!$, a conformal invariant computed from the Gauduchon representative $\omega_G$ of the class. If $\Gamma^{(2)}_M(\{\omega\})=0$, the linear equation $\Delta^C_{\omega_G}f=S^{(2)}_C(\omega_G)$ is solvable, producing a unique (up to scaling) metric $\omega_a\in\{\omega\}$ with $S^{(2)}_C(\omega_a)=0$, and the paper derives that either $\kappa(M)=-\infty$ or $\kappa(M)=0$ with $K_M^{\otimes m}=\mathcal{O}_M$ for some $m\in\mathbb{Z}_+$. If $\Gamma^{(2)}_M(\{\omega\})<0$, the nonlinear equation $\Delta^C_{\omega'}f=-\lambda e^f+S^{(2)}_C(\omega')$, with $\lambda=\Gamma^{(2)}_M(\{\omega\})\mathrm{Vol}(M,\omega_G)^{-1}$, is solved by a continuity method, giving a unique conformal metric $\omega_c$ with $S^{(2)}_C(\omega_c)=\lambda<0$; in balanced classes the same method yields a metric with that constant as its first Chern scalar curvature and implies $K_M^{-1}$ is not pseudo-effective. For the Bismut connection, the paper proves that when $b_1(M)=0$ the Gauduchon metric is conformal to a balanced metric, and a variational argument on the functional $Y_q$ produces a smooth solution of the corresponding equation, hence a conformal metric of constant second Bismut scalar curvature. Finally, for a pluriclosed Gauduchon metric satisfying the weak second Hermitian–Einstein condition $\Theta^{(3)}(\omega)+\Theta^{(4)}(\omega)=f\omega$, the paper proves $S^{(2)}_C(\omega)$ is constant by showing the defining function $f$ solves a linear elliptic equation whose only solutions are constants; the surface case then forces either $S^{(2)}_C(\omega)\equiv 0$ or a Kähler–Einstein metric with negative scalar curvature.

Load-bearing premise

The negative-case existence theorem rests on a uniform a priori bound for the approximating solutions of the continuity method, and the paper's derivation of that bound (the lower half of Lemma 5.3) is not correct as written, leaving the closedness step dependent on an unproved estimate.

Editorial extensions

If this is right

  • If $\Gamma^{(2)}_M(\{\omega\})<0$, every Hermitian conformal class contains a unique constant-negative second Chern scalar curvature metric, and in balanced classes the same constant is realized as the first Chern scalar curvature of a conformal metric while $K_M^{-1}$ is not pseudo-effective.
  • If $\Gamma^{(2)}_M(\{\omega\})=0$, the unique conformal metric with $S^{(2)}_C=0$ forces the Kodaira dimension to be either $-\infty$ or $0$ with a torsion canonical bundle.
  • On any compact complex manifold with $b_1(M)=0$, including the non-Kähler Calabi–Eckmann manifolds in dimensions $n\ge 3$, every Hermitian conformal class contains a metric of constant second Bismut scalar curvature.
  • A compact pluriclosed Gauduchon metric satisfying the weak second Hermitian–Einstein condition must have constant second Chern scalar curvature; on surfaces this gives a strict alternative between $S^{(2)}_C\equiv 0$ and negative Kähler–Einstein.
  • The explicit examples (Hopf manifolds, non-Kähler properly elliptic surfaces, Inoue surfaces) show that constant second Chern scalar curvature is not a Kähler-only phenomenon.

Reading between the lines

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

  • The second Gauduchon degree $\Gamma^{(2)}_M(\{\omega\})$ behaves like a conformal 'charge' whose sign may classify Hermitian conformal classes; the positive case is left open in this paper, and Theorem 5.5 suggests it forces $\kappa(M)=-\infty$ and yields constant positive scalar curvature metrics on products with a high-genus curve.
  • The a priori lower bound $f_a\ge 0$ in Lemma 5.3 appears incorrect as written: the maximum principle at a minimum point gives $e^{f_a}\ge aS/\lambda+1-a$, which allows negative values, so a corrected uniform $C^0$ bound would be needed to make the closedness step of Theorem 1.5 fully rigorous as presented.
  • The rigidity dichotomy (zero second Chern scalar curvature or Kähler–Einstein) suggests that weak second Hermitian–Einstein metrics form a bridge between Chern–Einstein and Kähler–Einstein geometry; one might test whether the non-positivity of $f$ in Corollary 1.9 can be relaxed to bounded-below $f$.
  • Because the examples include non-Kähler surfaces with $b_1=1$ (Inoue surfaces), the Bismut theorem's condition $b_1(M)=0$ is sufficient but not necessary; finding the sharp topological condition for Bismut constant scalar curvature would be a natural next step.
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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 / 3 minor

Summary. The paper studies Hermitian metrics with constant second scalar curvature on compact complex manifolds. In a fixed Hermitian conformal class, it derives conformal transformation formulas for the curvatures of the Gauduchon connections, defines a new conformal invariant called the second Gauduchon degree, and proves existence and uniqueness theorems for constant second Chern scalar curvature whose sign is controlled by this degree. It also treats a Yamabe-type problem for the second Bismut scalar curvature under the assumption b_1(M)=0, proving that the conformal class contains a metric with constant second Bismut scalar curvature. Finally, under a weak Einstein-type condition involving the third and fourth Chern-Ricci curvatures, it shows that the second Chern scalar curvature is constant, and it gives non-Kahler examples of metrics with constant second Chern scalar curvature.

Significance. If the proofs are completed, the paper would meaningfully extend the Chern-Yamabe theory to second scalar curvatures, introduce a useful conformal invariant, and provide concrete non-Kahler examples. The paper is clearly organized, the computations are explicit, and the use of external results such as Gauduchon's theorem and Yang's Kodaira-dimension criteria is appropriate. However, two load-bearing analytic steps in the main existence proofs are invalid as written, so the significance of the results is currently conditional on a repaired argument.

major comments (2)
  1. [Section 5, Lemmas 5.3-5.4] The two-sided estimate (5.10) is not a consequence of (5.9), and the proof of closedness of the set A therefore breaks. Evaluating (5.9) at a maximum p and a minimum q gives, with S_C^(2)(omega')=lambda e^{-u}, only e^{f_a(p)} <= 1-a+a e^{-u(p)} and e^{f_a(q)} >= 1-a+a e^{-u(q)}. These imply uniform bounds of the form f_a <= max(0, -min_M u) and f_a >= min(0, -max_M u), but they do not imply f_a >= 0 nor the upper bound log(1+min_M S/lambda). The lower bound is in fact false on the local branch through a=0: differentiating F(a,f_a)=0 at a=0 gives (Delta+lambda)w = lambda(e^{-u}-1), where w = df_a/da at a=0. Since lambda<0 and Delta+lambda is negative definite, w is negative wherever u>0, so f_a<0 for small positive a. Lemma 5.4 uses the uniform C^0 estimate from Lemma 5.3 to obtain W^{2,p} and Schauder estimates, so Theorem 1.5 is not established as written. The defect is local: the corrected inequalities above still yield a uniform C^0 bound, so a revision can repair the argument.
  2. [Section 4, Theorem 4.3] The proof that the weak minimizer phi_q is strictly positive is invalid. The argument chooses a>0 such that psi=-phi_q satisfies Delta psi + a psi <= 0 and then invokes the strong maximum principle. For an operator with a positive zeroth-order coefficient this conclusion is false: on S^1, psi = -(sin x)^4 is nonpositive with interior zeros and satisfies psi'' + a psi <= 0 for a >= 4. The coefficient in the equation actually satisfied by phi_q has uncontrolled sign, so the maximum principle cannot be applied in this way. A correct proof requires a Harnack-type inequality, a Moser iteration, or a subcritical approximation argument. Since Theorem 1.1 and Corollary 1.3 use the existence of a smooth positive solution of (4.2), the Bismut-Yamabe existence claim is not proved as written. In addition, the passage from the W^{1,2} weak solution to a smooth solution is not the immediate bootstrap claimed, because the right-hand side phi_q^{q-1} initially lies only in L^{q/(q-1)}; an iterative estimate is needed.
minor comments (3)
  1. [Section 1, Corollary 1.3] The sentence 'Theorem 1.6 admits the following corollary' should refer to Theorem 1.1, not Theorem 1.6.
  2. [Throughout] There are numerous typographical errors, including 'Hermtian', 'compacr', 'ans astheno', and 'Var' in the references; these should be corrected in a revised version.
  3. [Section 7, Example 7.4] In equations (7.11) and (7.16), the notation S_C^(1)(omega_1) appears where the metric in Example 7.4 is omega_2; the labels should be made consistent.

Circularity Check

0 steps flagged · score 0.0 of 10

No circularity: the existence proofs are genuine PDE constructions from external curvature formulas, and the target constants are conformal invariants rather than fitted inputs.

full rationale

The paper's central results are existence and uniqueness of conformal Hermitian metrics with prescribed constant second scalar curvature. The prescribed constants are the conformal invariants Gamma_M^(2)({omega}) Vol(M, omega_G)^{-1}, defined by integrating S_C^(2)(omega_G); they are not parameters fitted to a subset of the data being predicted. Equations (3.14), (4.1), (4.2), and (5.6) are derived by explicit conformal-transformation computations from the curvature identities of [42] (Lemma 2.2) and standard elliptic theory, so the continuity-method and variational solutions are actual constructions rather than restatements of the inputs. The citations to Gauduchon [21], Wang-Yang [42], Yang [44], Angella-Calamai-Spotti [1], and Tosatti-Weinkove [38] are external results whose assumptions do not include the target theorems; none is a same-author uniqueness theorem invoked to forbid alternatives. The reference [47] supplies a computational formula for conformal changes of curvature and an adjoint identity; the paper also re-derives the relevant formulas (Proposition 3.1, Corollary 3.2), so even if [47] is regarded as a self-citation it is not load-bearing. The externally noted false lower-bound step in Lemma 5.3 is a correctness defect in the closedness proof of the continuity method, not a circularity: the maximum-principle computation does not reduce the theorem to its conclusion, it simply fails to give the claimed bound as written. Overall the derivation chain is self-contained with respect to circularity.

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

The central results are existence theorems, so there are no data-fit parameters. The hypotheses (b_1=0, sign of Gamma^(2), f<=0) are domain assumptions on the manifold and metric, not free constants. The paper relies on standard elliptic theory and on several external results from the literature, including Gauduchon's theorem, curvature identities from Wang-Yang [42], and Kodaira-dimension criteria from Yang [44]. The new definitions (second Gauduchon degree, weak second Hermitian-Einstein) are not independently evidenced but are defined constructs with no falsifiable handle.

assumptions (5)
  • standard math In every Hermitian conformal class there is a unique Gauduchon representative (up to scaling).
    Invoked in Section 4 and Section 5 to fix omega_G and to define Gamma^(2); from Gauduchon [21].
  • standard math The curvature identity (2.7) from Wang-Yang [42] for Gauduchon connections.
    Used throughout Section 3 to derive conformal transformation formulas.
  • standard math Elliptic regularity, Sobolev embedding, and the maximum principle on compact manifolds.
    Used in Theorem 4.3 and Lemmas 5.2 to 5.4; the paper's application in Theorem 4.3 is questionable.
  • domain assumption b_1(M)=0 implies the Lee form of omega_G is d-exact.
    Hypothesis for Theorem 1.1 and Corollary 1.3; follows from Hodge theory as stated.
  • standard math Kodaira dimension and pseudo-effectivity criteria from Yang [44].
    Used in Theorems 1.4, 1.5, and 5.5 to convert scalar curvature sign into geometric conclusions.

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Pith. "Pith review of Existence and geometry of Hermitian metrics with constant second scalar curvature." pith.science (2026). https://pith.science/paper/PW6USKXW

@misc{pith2026260120572,
  author       = {Pith},
  title        = {Pith review of: Existence and geometry of Hermitian metrics with constant second scalar curvature},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/PW6USKXW}},
  note         = {Machine review of arXiv:2601.20572}
}
read the original abstract

We study Hermitian metrics with constant second scalar curvature on compact manifolds. We first consider a Yamabe-type problem for the second Bismut scalar curvature within balanced Hermitian conformal classes, and then analyze elliptic equations arising from constant second Chern scalar curvature within a fixed Hermitian conformal class and derive geometric consequences. Finally, under an Einstein-type condition on the second Chern curvature, a pluriclosed Gauduchon Hermitian metric has constant second Chern scalar curvature, which in certain cases further implies the existence of a K\"ahler-Einstein metric.

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