Research / Geometry & moduli / Stability walls
Can finite models predict how geometry degenerates?
Toward a quantitative theory of geometric degeneration. This programme connects realizable stability chambers, collapsing spectra, metrics on bundles and moduli spaces, and geometric flows. The papers establish these connections in explicit geometric classes, with estimates that remain useful when positive scales separate arbitrarily. A singular graded example exposes a limit of the smooth description and a new asymptotic problem.
A finite spectral model
How a new zero mode appears
Before the limit
Bridge weight ε > 0
1 connected component
1 zero mode
At the limit
Bridge weight ε = 0
2 connected components
2 zero modes
Solid links have weight 1.
This illustrates one vanishing scale. The programme treats several scales and their relation to actual metrics and flows.
I · The ambition
From stability to loss of rigidity.
For a stable holomorphic bundle on a compact Kähler manifold, the Hermitian–Einstein correspondence gives a canonical metric up to scale. The quantitative question begins when a stable bundle approaches a wall: how does its metric change, which eigenvalues become small, and how does its evolution slow down? The aim is to relate these analytic effects to the algebraic geometry of the degeneration, with estimates that remain useful when several scales vanish at very different rates.
Four descriptions to connect
Algebraic geometry determines which degenerations occur. The incidence of equal-slope subobjects describes the local chamber. A finite operator records weak spectral directions. Nonlinear analysis determines the actual metrics and flows. A general theory would explain when these describe the same degeneration, and what additional data are needed to pass from one description to another.
The chamber alone need not determine the answer. Harmonic extension data can affect the leading spectrum; a flow retains information about its initial metric. When the graded sheaf is singular, even the proposed asymptotic scale can require a further correction.
Why relative accuracy matters
An error small in absolute size can overwhelm a much smaller eigenvalue. A useful comparison controls the error relative to each positive mode, even when the ratios between modes approach zero. Schematically, the spectral results have the form
λ is an actual eigenvalue, μ the corresponding eigenvalue of the finite model, and η tends to zero. In the stated families, C is independent of the ratios between positive modes.
The estimates retain the weak directions in the finite model and invert only a complementary operator with a uniform positive gap. Quotient metrics and flows require further arguments; a spectral comparison alone does not establish either.
Reading a small eigenvalue
The same error can hide the weaker mode.
An absolute bound
|λ − μ| ≤ 0.02
Normalized eigenvalue λ / μ
The bound allows the smaller mode to be zero.
A relative bound
|λ − μ| ≤ 0.2 μ
Normalized eigenvalue λ / μ
Both modes stay within 20% of the model.
II · Geometric realizability
Which degenerations can actually occur?
A finite model becomes a geometric example only when a bundle realizes its factors, extension classes and accessible slope directions. The chamber papers establish this part of the programme.
The toric tangent stability census and the blowup-and-bundle paper give explicit families and exact classifications. Local stability chambers then varies the polarization: it constructs an all-dimensional family with arbitrarily many independent chamber boundaries and determines nearby stable loci for the indecomposable strictly semistable examples in the earlier census.
Nonsimplicial tangent chambers goes beyond independent inequalities. It constructs weak-Fano tangent bundles whose local chambers have genuinely nonsimplicial geometry, with every centered slope direction accessible. Its general local normal form retains the slope directions realized by polarizations and requires no local-freeness assumption on the equal-slope subsheaves. A toric surface in the same paper supplies the singular graded object studied later.
III · Stationary metrics and spectra
What determines every weak spectral scale?
Small eigenvalues near stability walls begins with a stable subbundle extended by several stable quotient factors. The bipartite two-step theorem treats extensions between two sums of distinct stable factors. At equal limiting slopes and with connected extension support, a weighted graph Laplacian determines the small endomorphism spectrum with uniform relative error. Ranks give the vertex masses; balancing the harmonic extension data against the slope gaps gives the edge weights.
This description also identifies what the chamber forgets. On a tree, ranks and slopes determine the leading spectrum. On a cycle, harmonic extension data can survive. A spanning-tree expression controls the leading vanishing factor of the spectral determinant in the stated two-step setting.
When extensions compose
The three-step metric theorem includes nonlinear composition and its integrability relations. It treats distinct equal-slope line factors, adjacent extension classes and the prescribed quadratic coexact corrections, with no independent first-to-third-layer parameters. Under its balancing and smallness assumptions, the finite model approximates the actual Hermitian–Einstein metric and every small eigenvalue. An example on the product of three projective lines has a weak scale that its polarization parameters alone do not detect.
When factors repeat
The repeated-factor spectral theorem replaces scalar graph directions by matrix multiplicities for simple locally free two-step extensions. The later rank-five three-step paper constructs actual metrics and controls six small matrix modes in a specified deformation family on the product of three projective lines. These results admit arbitrarily separated positive scales, while retaining their respective hypotheses on factors and extensions.
IV · Metrics on moduli spaces
What happens when stabilizers change?
A metric on a bundle and a metric on its moduli space measure different things. The latter measures deformation after identifying changes induced by gauge transformations. When an object acquires more automorphisms, the orbit directions change rank; a comparison must survive this degeneration as well.
Begin with relative metric estimates near reducible Yang–Mills connections. Near a central Yang–Mills connection on a closed surface, the classical quadratic model approximates the actual quotient metric and every small gauge eigenvalue uniformly across stabilizer types and arbitrarily separated orbit scales. The paper also computes the leading metric correction.
The higher-dimensional stability-wall moduli paper retains the full analytic obstruction near a sum of four line bundles on the product of three projective lines. On smooth complex pieces, the relative metric error is quadratic in the coefficient radius, with a radius and comparison constant independent of the distance to the wall. The estimate persists as orbit and obstruction maps lose rank. Quantitative changes of chart also give comparisons of intrinsic lengths and their completions within the local domains.
The rank-five repeated-factor paper adds a noncommutative multiplicity symmetry. It compares harmonic quotient metrics on smooth pieces of the full local deformation problem and identifies the metric on a specified reducible locus with that of the remaining stable rank-four summand. These are concrete higher-dimensional theorems, with different hypotheses from the surface theorem.
The surface paper's explicit quaternionic projective and hyperbolic reductions provide a comparison with the finite-Planck Higgs quotient problem. A general quaternionic Kähler comparison across stabilizer changes remains open.
V · Metric response and evolution
Which trajectory belongs to the initial metric?
The earlier flow-spectrum paper determines small eigenvalue asymptotics along Hermitian Yang–Mills flow in its curve and two-step settings. The metric-response theorem relates sensitivity to polarization to reciprocal graph eigenvalues and constructs a finite-dimensional invariant manifold for the flow. Its tangent-bundle application connects chamber geometry, small spectra, metric response and evolution on the same family.
A reduced evolution equation does not yet identify which of its solutions represents a prescribed initial metric. The initial-condition and phase paper supplies this identification near a stable four-line family on the product of three projective lines. Relative to a chosen invariant graph, the initial metric selects a finite trajectory with exponentially decaying relative tracking error, uniformly in the weak relaxation rates. The phase depends differentiably on the initial metric at fixed bundle and polarization. A common restart brings prescribed smooth determinant-normalized initial metrics into the local regime under the theorem's neighborhood conditions.
The wall and unstable-flow paper treats acyclic connected extension data at the wall and a specified triangular unstable class with locally free Harder–Narasimhan line quotients. In moving diagonal coordinates, the harmonic coefficients remain small while the diagonal metric factors diverge. For the stated initial metrics, this gives all-time confinement and asymptotic phase; after the unstable linear drift is subtracted, a limiting residual retains three real diagonal initial coordinates.
These flow theorems require their own invariant graphs, confinement estimates and initial-metric assumptions. The stationary repeated-factor results do not yet supply a corresponding general repeated-factor dynamical theorem.
VI · A boundary of the smooth description
A singular point changes the metric away from it.
Changing stabilizers can make a moduli space singular even when the graded bundle is locally free. A graded sheaf that is itself singular presents a further problem. The programme contains an example where this second kind of singularity changes the long-time metric behavior on every region kept away from the singular point.
Two different geometric questions
Where does the singularity live?
In the moduli space
At q: extra automorphisms.
The graded bundle can remain locally free.
In the graded sheaf
At p: failure of local freeness.
The metric discrepancy persists on K, away from p.
Singular graded limits and metric growth studies a semistable tangent bundle on a smooth projective toric surface. Its graded sheaf is singular at one point. Write u(T, x) for the induced metric on its saturated equal-slope line, divided by a fixed Hermitian–Einstein line metric. For every smooth initial metric with the prescribed Hermitian–Einstein determinant,
As T tends to infinity, for every fixed compact K away from the singular point.
The iterated weight filtration of Haiden, Katzarkov, Kontsevich and Pandit, polarized by rank, assigns the squared-metric scale T−1/2, with no later nonzero weights. The strict decay above rules out the two bounded-remainder extensions tested in the paper: uniform metric-order comparison and a bounded error in a fixed-splitting matrix-log expansion. A local residue forces divergent normalized extension energy; a dissipation identity carries its effect into the flow. In the stationary limit from the stable side, the same point carries multiplicity-one curvature concentration.
VII · Toward a general theory
What would make the comparison reusable?
The papers already establish comparisons on explicit geometric classes and develop methods that can be used again: retain every weak finite direction, control the complement uniformly, and estimate the ambient metric before minimizing over gauge orbits. The singular-flow result also answers an independently motivated asymptotic question. The next steps concern the reach of these methods and the additional data their limits reveal.
| Direction | Established setting | Next question |
|---|---|---|
| Realizability and stationary comparison | Toric chamber families; two-step extensions and specified three-step models. | Which hypotheses extend the comparison to other stable factors and general filtrations, and which finite data must be retained? |
| Quotient geometry | Surface Yang–Mills quotients and the stated higher-dimensional deformation families. | When do uniform metric and chart comparisons persist for other moduli problems, including changing stabilizers and obstructions? |
| Dynamics | Two-step flows and the stated four-line stable, wall and unstable families. | How can the initial-condition-sensitive theory extend to repeated factors and more general filtrations? |
| Singular graded sheaves | A toric surface counterexample, with strict off-singular metric decay and a stationary curvature defect. | What is the replacement asymptotic law, and which singular data determine its correction? |
A further test of generality is transfer to a different geometric problem with a concrete new consequence. The programme's ambition is a common quantitative theory; its current theorems retain the geometric hypotheses stated above. The integrated result on the weak-Fano tangent family is one realization of that ambition.
VIII · Where to begin
Three routes through the programme.
The geometric idea
Start with local stability chambers, continue to the nonsimplicial examples, then read the integrated tangent-bundle application in metric response and flow. The singular-flow counterexample shows a limit of the resulting description.
The analytic mechanism
Read the two-step spectral theorem, then three-step metrics. For moduli geometry, follow surface quotient metrics, stability-wall metrics and repeated-factor moduli.
The dynamics
Begin with two-step response and flow. Use three-step metrics for the stationary setting of the later work, then read initial conditions and phase followed by flow at and beyond the wall.
At the Wall — explore chambers, weak spectra and metric response ↗
The explorer illustrates selected finite models and the two-factor flow profile. The three-step, quotient-metric and singular-flow theorems are developed in the papers. The full reading list below groups the programme by mathematical question; abstracts can be opened individually.
16 manuscripts · Reading order
The manuscripts.
Chambers and geometric realizability · 4 manuscriptsThe section ↑
- 01
Slope stability of tangent bundles of smooth toric Fano varieties
Constructions of toric Fano varieties with stable tangent bundles, compared with Kähler–Einstein conditions.
Preprint · 2026 · Abstract, PDF & citation ↗
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We construct smooth toric Fano -folds of Picard number whose tangent bundles are slope-stable with respect to the anticanonical polarization, for every . The construction gives toric fibrations with fibre the del Pezzo surface of degree six over products of projective lines, parametrized by multisets of roots of . Every nonempty multiset of nonzero roots with vanishing sum yields a stable tangent bundle. Among these multisets, the resulting variety is Kähler–Einstein if and only if the multiset is invariant under negation or under the order-three rotation of the root hexagon. We also construct stable, non-Kähler–Einstein examples with nonzero twist sum in every even dimension at least four. The proofs reduce slope inequalities and barycenter computations to integrals over the moment hexagon.
For a smooth toric Fano variety with strictly semistable tangent bundle, we prove that polystability is equivalent to decomposition as a nontrivial product of smooth toric Fano varieties with anticanonically stable tangent bundles. Exact evaluation of Klyachko’s criterion extends the stability classification to dimensions five and six, recovering the classifications of Steffens and Reynolds in dimensions three and four. Together with the product criterion, this determines polystability for all varieties in dimensions three through six, and hence the existence of Hermitian–Einstein metrics on their tangent bundles with respect to an anticanonical Kähler form.
- 02
Tangent stability on toric Fano blowups and bundles
Stability criteria for specified Fano blowups and bundles, with a complete exact census of Picard-number-ten eightfolds.
Preprint · 2026 · Abstract, PDF & citation ↗
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For Fano blowups of products of projective spaces along invariant codimension-two centres indexed by a tree, using distinct coordinate hyperplanes at each factor, anticanonical tangent stability is equivalent to one divisor-degree inequality at each vertex. The exceptional contributions are mixed intersections on the blowup centres. Stability holds for every tree of maximum degree at most three whose nonleaf factor dimensions equal their valences, with arbitrary positive leaf dimensions. For smooth toric Fano varieties that are locally trivial toric bundles with fibre a product of degree-six del Pezzo surfaces and base a product of projective spaces, the largest Picard number compatible with tangent stability in dimension is , allowing arbitrary integral twists. Every fixed tree of maximum degree at most three with an edge yields bundles attaining this bound after sufficiently long independent edge subdivisions. Their number, up to isomorphism of toric fans, is unbounded as the dimension grows through multiples of four. The proofs use relative tangent bundles, ranks of subspaces spanned by rays, and integral comparisons. The bundle existence proofs also use finite exact rational calculations with uniform error estimates and induction.
- 03
Local stability chambers for toric tangent bundles
Varying the polarization: an all-dimensional projective-bundle classification with arbitrarily many chamber boundaries, a geometric criterion, and local chambers for the 31 indecomposable semistable census cases.
Preprint · 2026 · Abstract, PDF & citation ↗
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We classify the anticanonical slope stability of the tangent bundles of , where are nonnegative integers and . The tangent bundle is stable when , strictly semistable when , and unstable otherwise. For and , the germ of the semistable polarization locus at the anticanonical class is real analytically equivalent to , with stable locus . In particular, the number of independent local chamber boundaries is unbounded.
For a smooth projective toric variety whose tangent bundle is semistable at a polarization , we describe the local chamber at by the order ideals of a finite poset determined by the equal-slope ray subspaces. If each such subspace is spanned by the rays it contains in every maximal cone, nearby stable polarizations exist precisely when the variety is not a nontrivial toric product. Applied to the existing anticanonical census in dimensions three through six, this criterion gives nearby stability in all 31 indecomposable strictly semistable cases, whose local chambers have one, two, or three independent boundaries. We determine locally free, pairwise nonisomorphic Jordan–Hölder factors both for these cases and for the family .
- 04
Nonsimplicial local stability chambers of toric tangent bundles
Geometric realization: nonsimplicial tangent chambers, positive-spanning slope access without local freeness, and an explicit Calabi–Yau conifold transition.
Preprint · 2026 · Abstract, PDF & citation ↗
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We construct smooth projective toric varieties with nonsimplicial local slope-stability chambers for their tangent bundles. In every even dimension , a fibre product of two projective-line bundles over admits an ample real class at which the tangent bundle is strictly semistable. Near this class, the semistable locus is analytically isomorphic to a pointed cone over , times a line, where denotes the -simplex. The torus-invariant saturated subsheaves of equal slope form the ideal lattice of the complete bipartite poset with two minimal and maximal elements, and the stable line factors realize every centered slope direction. These varieties are weak Fano and not Fano. The fourfold has minimal dimension and Picard rank among toric varieties with such a chamber and nearby stable polarizations. We also prove a local normal form at any ample real class where the tangent bundle of a smooth projective toric variety is semistable. It retains precisely the slope directions realized by polarizations, requires no local-freeness assumption on equal-slope subsheaves, and localizes every nearby Harder–Narasimhan filtration to their equality lattice. If the fan rays in each equal-slope subspace positively span that subspace, every centered slope direction occurs. A semistable surface satisfies this condition although one equal-slope quotient is not locally free.
Stationary metrics and small spectra · 4 manuscriptsThe section ↑
- 05
Small Dolbeault eigenvalues near stability walls
From stability chambers to the equilibrium spectrum: every small Hermitian–Einstein eigenvalue is determined to uniform relative error by ranks and slope gaps, even at arbitrarily separated scales.
Preprint · 2026 · Abstract, PDF & citation ↗
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We determine the small spectrum of the Dolbeault Laplacian on trace-free endomorphisms of Hermitian–Einstein bundles near intersections of slope-stability walls. On a compact Kähler manifold of dimension at least two, consider an extension of by , where the factors are pairwise nonisomorphic and stable of equal slope at the limiting Kähler class, and every extension component is nonzero. Write and let be the Einstein constant of minus that of the extension. In the chamber , exactly eigenvalues tend to zero. They agree, to relative error , with the eigenvalues of , where . The estimate is uniform in all positive ratios of the slope gaps. Thus the ranks and slopes determine the leading spectrum even when the gaps vanish at arbitrarily different rates.
For two factors we obtain , where is the quotient Einstein constant minus the subbundle Einstein constant and is given by the Green operator of the graded connection. After rescaling the extension and making unitary identifications with the graded limit, we determine the normalized first eigensection through order in every spatial norm. Toric tangent bundles provide examples with arbitrarily many small eigenvalues whose orders of vanishing can be prescribed independently.
- 06
Uniform Hermitian–Einstein spectra for bipartite two-step extensions
The spectral mechanism: relative estimates for every small eigenvalue on connected bipartite supports, uniformly through arbitrarily separated positive scales.
Preprint · 2026 · Abstract, PDF & citation ↗
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We determine every small eigenvalue of the Dolbeault Laplacian on trace-free endomorphisms at a Hermitian–Einstein metric near an intersection of slope-stability walls. The bundle is a fixed extension of one direct sum of stable bundles by another on a compact Kähler manifold, with pairwise nonisomorphic factors of equal slope at the reference form and a connected graph of nonzero extension components. In the stable chamber, the small spectrum is asymptotic to the nonzero spectrum of a weighted Laplacian on this graph. Its vertex masses are the factor ranks, and its edge weights balance the slope differences against the harmonic extension data. The relative error is of order the total edge weight, uniformly as positive stability margins vanish at arbitrarily different rates, and the remaining spectrum has a uniform gap. The proof uses curvature identities across graph cuts to control the nonlinear correction at each vanishing scale. As consequences, we obtain a relative approximation of the metric and a spanning-tree formula for the leading vanishing factor of the zeta-regularized determinant. For trees the leading spectrum is determined by ranks and slopes; cycles can retain dependence on the harmonic extension data.
- 07
Uniform Hermitian–Einstein spectra with repeated stable factors
Repeated stable factors: actual HE metric comparison and every small matrix mode, uniformly at arbitrarily separated positive scales.
Preprint · 2026 · Abstract, PDF & citation ↗
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We prove uniform relative asymptotics for all small positive Dolbeault eigenvalues on trace-free endomorphism-valued zero-forms for Hermitian–Einstein metrics on simple two-step extensions near an equal-slope Kähler polarization. The stable factors may occur with arbitrary fixed multiplicities, with distinct isomorphism types in the two layers. The finite comparison operator is the commutator Laplacian on the full complex multiplicity algebra, evaluated at an independently balanced representative of the extension. Every small eigenvalue has relative error bounded by a fixed multiple of the total balanced extension energy, and the remaining spectrum has a uniform positive lower bound. No lower bound on positive eigenvalue ratios or stability margins is imposed. The main estimate bounds the curvature residual against every multiplicity projection by its crossing energy; a degree argument then compares the actual metric with the balanced metric without inverting a degenerating finite Hessian. A fixed rank-five bundle on a product of four projective lines exhibits six small modes and arbitrarily separated positive scales.
- 08
Hermitian–Einstein metrics and small spectra for three-step extensions
Three-step extensions: actual metrics, every small spectral scale and intrinsic polarization response.
Preprint · 2026 · Abstract, PDF & citation ↗
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We prove uniform relative asymptotics for every small Dolbeault eigenvalue on trace-free endomorphism-valued zero-forms in a class of three-step Hermitian–Einstein extensions, allowing arbitrary separation of positive spectral scales. The graded factors are distinct line bundles of equal slope at a reference polarization on a compact Kähler manifold. Adjacent extension classes vary in fixed cohomology subspaces; the remaining terms are quadratic coexact Hodge primitives of their compositions, with no independent first-to-third-layer parameters. Assume integrability and a connected extension graph. At nearby polarizations, suppose diagonal rescaling balances the squared norms of the adjacent classes against the slope differences, with sufficiently small sum of rescaled squared norms. The rescaled split metric then approximates the Hermitian–Einstein metric with the same determinant, with logarithmic error bounded by a uniform constant times that sum. Every small eigenvalue has the same relative accuracy with respect to the corresponding eigenvalue of the graph Laplacian weighted by these squared norms; the complementary spectrum has a uniform positive gap. The proof controls curvature traces by the energy crossing each vertex cut. A family on the product of three projective lines has a spectral scale undetected by its polarization parameters. At each fixed bundle in this family, both singular values of the intrinsic metric response to the two polarization parameters agree, with the same relative accuracy, with those of the differentiated finite balancing equation.
Quotient metrics and repeated-factor moduli · 3 manuscriptsThe section ↑
- 09
Relative metric estimates near reducible Yang–Mills connections
Relative surface gauge quotient-metric and small-spectrum estimates, uniform across changing stabilizers and arbitrarily separated scales.
Preprint · 2026 · Abstract, PDF & citation ↗
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We study the natural metric near a central Yang–Mills connection on a closed surface. In the classical quadratic symplectic model, we prove a relative metric estimate with error quadratic in the harmonic deformation parameter, uniformly across all stabilizer types. We also compute the leading metric correction using the Green operators of the reference connection. The proof first eliminates the gauge directions with a fixed positive spectral gap and then minimizes over the remaining finite-dimensional orbit; it requires no lower bound on a positive orbit eigenvalue. The same argument compares every small eigenvalue of the gauge Laplacian with the infinitesimal stabilizer-action operator, including at changes of kernel dimension. As a curved finite-dimensional comparison, quaternionic projective and hyperbolic reductions admit exact orbit-metric formulas on their flat moment-map zero cone. A four-cycle is realized in both settings with independently vanishing weights. The resulting estimates distinguish uniform control of the quotient metric from estimates that depend on the smallest orbit scale.
- 10
L² metrics on Hermitian–Yang–Mills moduli spaces near a stability wall
Full local moduli near a wall: uniform relative harmonic L² metrics, chart transitions and intrinsic distance.
Preprint · 2026 · Abstract, PDF & citation ↗
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We prove a uniform relative comparison between the harmonic metric on a local Hermitian–Yang–Mills moduli space and the quotient metric of its finite-dimensional harmonic deformation model. The result concerns a rank-four family on the product of three projective lines, near a split sum of four line bundles at a stability wall. The model retains the full analytic obstruction and describes a neighborhood of the corresponding Hermitian–Einstein classes. On its smooth complex pieces, the relative metric error is quadratic in the coefficient radius. Both the comparison constant and the allowed radius are independent of the distance to the wall, even when the infinitesimal orbit map and the derivative of the obstruction lose rank. The proof estimates the ambient deformation norm before taking the quotient, avoiding inversion of either degenerating map. We also identify the transition from this wall model to the harmonic model at a reducible rank-three-plus-line endpoint, with quantitative domains of validity. These comparisons extend to intrinsic lengths and their completions; in an explicit family of stable extensions they give a joint asymptotic for the intrinsic distance to the reducible bundle.
- 11
Hermitian–Einstein metrics and moduli of three-step extensions with repeated factors
Repeated factors in three steps: actual rank-five metrics, six matrix modes and local quotient geometry.
Preprint · 2026 · Abstract, PDF & citation ↗
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We construct Hermitian–Einstein metrics and obtain relative asymptotics for all six small eigenvalues of the Dolbeault Laplacian on trace-free endomorphism-valued zero-forms in a rank-five deformation problem with a repeated line factor on the product of three projective lines. The estimates are uniform as positive spectral scales separate or vanish. At nearby product polarizations, the metric construction applies to every sufficiently small simple integrable deformation satisfying the quadratic moment-map equation at the centered slope level. Its logarithmic error relative to the split metric is quadratic in the harmonic coefficients. The key estimate uses harmonic orthogonality to eliminate cubic curvature terms and bounds the remaining error against each multiplicity projection by the energy mixing its image and kernel. This gives relative spectral comparison with the matrix commutator form without a lower bound on its positive eigenvalues. On smooth pieces of the full local Hermitian–Einstein quotient, we likewise compare the harmonic metric with the coefficient quotient metric. At a reducible locus where one copy of the repeated line splits off, the induced metric agrees with that of the remaining stable rank-four summand.
Metric response and dynamics · 4 manuscriptsThe section ↑
- 12
Small Dolbeault eigenvalues along Hermitian Yang–Mills flow
Small spectral modes along Hermitian Yang–Mills flow, described by evolving weighted graph Laplacians in specified bundle classes.
Preprint · 2026 · Abstract, PDF & citation ↗
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We study the small eigenvalues of the Dolbeault Laplacian on trace-free endomorphisms of a semistable holomorphic bundle along Hermitian Yang–Mills flow, normalized as with the mean curvature and its average. The bundles considered are simple bundles on a compact curve whose Jordan–Hölder factors are pairwise nonisomorphic, and extensions of one polystable bundle by another on compact Kähler manifolds, again with pairwise nonisomorphic stable factors. From every smooth initial metric, each small eigenvalue is asymptotic to an eigenvalue of a weighted graph Laplacian, whose conductances evolve by an explicit finite-dimensional flow; the relative error tends to zero. The graph records which stable factors are joined by nonzero extension classes. The asymptotics are governed by the weight grading of Haiden, Katzarkov, Kontsevich, and Pandit, the solution of a quadratic program on this graph. Suppose some Lagrange multiplier vector of this program is strictly positive on every active constraint. We then determine the decay exponent and the leading coefficient of every small eigenvalue, and the limits of the spectral subspaces. The eigenvalues of order have coefficients independent of the initial metric, and is always one of them. At each faster rate the coefficients depend on the initial metric, and their sum is unbounded over metrics on one fixed bundle. A key step shows that the bounded remainder in the asymptotics of the finite-dimensional flow converges. Examples include an eigenvalue decaying like and, without the positivity condition, an eigenvalue of order . We also treat families of harmonic extensions with fixed metrics, including repeated factors and recovery of the graded object, and we show that the constants in a slope inequality relating the lowest eigenvalue to the averaged trace-free mean curvature are sharp in every rank.
- 13
Metric response and Hermitian Yang–Mills flow for two-step extensions
Metrics and flows: intrinsic response, singular inverses and actual HYM comparisons, culminating in the integrated theorem on the same tangent family.
Preprint · 2026 · Abstract, PDF & citation ↗
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For two-step extensions of pairwise nonisomorphic stable bundles on a compact Kähler manifold, we quantify the degeneration of Hermitian–Einstein metrics and Hermitian Yang–Mills flow near intersecting slope-stability walls. We assume equal slopes at the reference form and connected support for the extension class. When the centered slopes provide full local parameters, every singular value of the trace-free part of , for the Hermitian–Einstein metric , is relatively asymptotic to the reciprocal of a nonzero eigenvalue of a weighted extension-graph Laplacian. The comparison uses rank-weighted slope and normalized norms and remains uniform for arbitrarily separated positive stability margins. We also construct a finite-dimensional invariant manifold of the flow and compare its solutions with flows from any smooth family of initial metrics. For each tolerance, one late time and then one parameter neighborhood give multiplicative metric comparison, up to a constant scalar, and relative accuracy for every small endomorphism Dolbeault eigenvalue for all subsequent times. The comparison applies in the stable, semistable and unstable regimes. In the two-factor case, we determine a uniform asymptotic profile for the smallest eigenvalue across the wall, including exponential decay on the unstable side. An application to explicit weak Fano toric tangent bundles connects nonsimplicial stability chambers, metric response and flow on the same bundles.
- 14
Initial conditions and asymptotic phase for Hermitian–Yang–Mills flow
Stable dynamics: differentiable initial-condition selection and uniform exponential tracking of a finite flow.
Preprint · 2026 · Abstract, PDF & citation ↗
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We prove that the initial Hermitian metric selects a finite-dimensional trajectory that tracks Hermitian–Yang–Mills flow with exponentially decaying relative metric error, uniformly as the positive relaxation rates separate or tend to zero. The result holds for a nearby stable family of deformations of a specified sum of four line bundles on the product of three projective lines, along a fixed polarization path. We construct an exact invariant graph over the full integrable harmonic deformation space. Relative to this chosen graph, the asymptotic phase is continuously differentiable in the initial metric at fixed bundle and polarization. The local theorem permits bounded diagonal metric coordinates and sufficiently small transverse displacement. A prescribed smooth determinant-normalized metric enters this regime after a common restart time, chosen before the deformation, polarization and nearby-metric neighborhoods. The proof uses a fixed complementary spectral gap and metric order, without inverting a small relaxation rate. For a three-layer family with two independent positive slope parameters, we also prove all-future comparison with a small, time-independent relative error.
- 15
Hermitian–Yang–Mills flow at and beyond a stability wall
Wall and unstable dynamics: all-time coefficient confinement, decay and a limiting residual of initial conditions.
Preprint · 2026 · Abstract, PDF & citation ↗
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We prove all-time confinement and two-sided decay estimates for Hermitian–Yang–Mills flow whose initial metric is a sufficiently small transverse perturbation of a metric on a fixed finite-dimensional invariant graph. The bundles are small integrable deformations of a specified sum of four line bundles on the product of three projective lines. At the stability wall the directed extension graph is acyclic and connected; beyond it we treat a connected triangular class with locally free Harder–Narasimhan line quotients. In a moving diagonal presentation, the harmonic coefficients remain small although the diagonal metric factors become unbounded. Their energy decays reciprocally at the wall and crosses to exponential decay on the unstable side, uniformly in the ratio of wall distance to initial energy. This confinement yields an asymptotic phase relative to a chosen invariant graph: each such initial metric selects a unique reduced trajectory with exponentially decaying relative metric error. The phase is continuously differentiable in the initial metric at fixed bundle and polarization. At each fixed nearby unstable polarization, subtracting the linear diagonal drift leaves a limiting residual that is locally invertible in the three real diagonal initial coordinates.
Singular graded limits · 1 manuscriptThe section ↑
- 16
Singular graded limits and metric growth under Hermitian–Yang–Mills flow
Singular graded sheaves: a toric surface obstruction to bounded-remainder weight-filtration metric asymptotics.
Preprint · 2026 · Abstract, PDF & citation ↗
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We construct a semistable toric tangent bundle for which the weight-filtration description of Hermitian–Yang–Mills metric growth cannot extend to singular graded sheaves with a uniformly bounded remainder. The bundle lies on a smooth projective surface, and its Jordan–Hölder graded sheaf is singular at one point. For every smooth initial metric with fixed Hermitian–Einstein determinant, the induced squared norm on its unique saturated equal-slope line subsheaf is as the flow time tends to infinity, uniformly on compact subsets away from that point. The rank-polarized iterated weight filtration of Haiden–Katzarkov–Kontsevich–Pandit instead assigns the scale , with no further nonzero weights. A splitting-independent local residue forces divergent normalized extension energy, which an exact dissipation identity converts into the strict decay estimate. Approaching the wall from the stable side, we also identify the Hermitian–Einstein limit with the reflexive graded bundle and locate its multiplicity-one curvature concentration at the same point.
The broader subject overview, including open FJRW theory and inverse moduli, is the Geometry & moduli guide.