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Non-Smoothable Nestings of Fat Points

Updated 30 January 2026
  • The paper establishes explicit lower bounds and systematic construction methods showing that nested fat point configurations are generally non-smoothable in higher dimensions.
  • It employs nested Hilbert scheme theory alongside deformation analysis, including graded Betti numbers and Białynicki–Birula decomposition, to investigate smoothability.
  • These findings have significant implications for birational geometry, component stratification, and the reducibility of Hilbert schemes on singular hypersurfaces.

A non-smoothable nesting of fat points refers to an inclusion of two or more supported, zero-dimensional subschemes ("fat points") of a smooth quasi-projective variety XX, such that the nested configuration does not lie in the closure of the locus of reduced schemes (i.e., it cannot be approximated by configurations of distinct points). This phenomenon is rigorously captured by the theory of nested Hilbert schemes, which for a non-decreasing sequence d=(d1,,dr)\underline d=(d_1,\dots,d_r), parameterizes chains

Z(1)Z(2)Z(r)X×BZ^{(1)}\subset Z^{(2)}\subset\cdots\subset Z^{(r)}\subset X\times B

of closed subschemes, each flat over BB of relative length did_i. The existence, structure, and systematic construction of non-smoothable nestings of fat points in higher-dimensional ambient varieties reveal profound deviations from classical surface or curve cases and have major implications for the birational geometry and component structure of Hilbert schemes (Graffeo et al., 23 Jan 2026).

1. Structure and Smoothability of Nested Hilbert Schemes

A key foundational aspect is the precise definition of smoothability within the context of nested Hilbert schemes. For r=2r=2, a point of $\Hilb^{d_1,d_2}(X)$ corresponds to an inclusion [Z1Z2][Z_1\subset Z_2] where each ZiZ_i is a fat point of length did_i. This nesting is termed smoothable if it lies in the closure of the locus where d=(d1,,dr)\underline d=(d_1,\dots,d_r)0 is reduced (i.e., a disjoint union of d=(d1,,dr)\underline d=(d_1,\dots,d_r)1 distinct points). The locus of non-smoothable nestings, conversely, consists of chains of fat points that cannot be realized as a limit of nestings of distinct reduced points. These distinctions become increasingly pronounced as the ambient dimension d=(d1,,dr)\underline d=(d_1,\dots,d_r)2 grows.

2. Lower Bounds for Non-Smoothable Nestings (Theorem A)

Consider d=(d1,,dr)\underline d=(d_1,\dots,d_r)3 with d=(d1,,dr)\underline d=(d_1,\dots,d_r)4 and an integer d=(d1,,dr)\underline d=(d_1,\dots,d_r)5. The construction utilizes two d=(d1,,dr)\underline d=(d_1,\dots,d_r)6-primary ideals: d=(d1,,dr)\underline d=(d_1,\dots,d_r)7 where d=(d1,,dr)\underline d=(d_1,\dots,d_r)8 is a general linear subspace of codimension 2, and d=(d1,,dr)\underline d=(d_1,\dots,d_r)9. The corresponding nesting Z(1)Z(2)Z(r)X×BZ^{(1)}\subset Z^{(2)}\subset\cdots\subset Z^{(r)}\subset X\times B0 defines a point in Z(1)Z(2)Z(r)X×BZ^{(1)}\subset Z^{(2)}\subset\cdots\subset Z^{(r)}\subset X\times B1. Via dimension computations:

  • The expected dimension of the smoothable component is Z(1)Z(2)Z(r)X×BZ^{(1)}\subset Z^{(2)}\subset\cdots\subset Z^{(r)}\subset X\times B2.
  • The Białynicki–Birula decomposition reveals that nestings of a specific Hilbert–Samuel type occupy a stratum of dimension Z(1)Z(2)Z(r)X×BZ^{(1)}\subset Z^{(2)}\subset\cdots\subset Z^{(r)}\subset X\times B3.

The gap

Z(1)Z(2)Z(r)X×BZ^{(1)}\subset Z^{(2)}\subset\cdots\subset Z^{(r)}\subset X\times B4

is non-positive precisely for Z(1)Z(2)Z(r)X×BZ^{(1)}\subset Z^{(2)}\subset\cdots\subset Z^{(r)}\subset X\times B5 (for Z(1)Z(2)Z(r)X×BZ^{(1)}\subset Z^{(2)}\subset\cdots\subset Z^{(r)}\subset X\times B6). Therefore, generic chains of this type do not lie in the smoothable locus, demonstrating explicit lower bounds for the existence of non-smoothable nestings of fat points in higher dimensions. The proof incorporates the semicontinuity of graded Betti numbers and tangent space analysis, ensuring correct Hilbert functions and component structure.

3. Systematic Construction of Non-Reduced Elementary Components (Theorem B)

A robust method exists for systematically producing generically non-reduced elementary components from reduced ones. Given Z(1)Z(2)Z(r)X×BZ^{(1)}\subset Z^{(2)}\subset\cdots\subset Z^{(r)}\subset X\times B7 as a generically reduced elementary component (the general nested chain has TNT: Trivial Negative Tangents), one can insert a layer Z(1)Z(2)Z(r)X×BZ^{(1)}\subset Z^{(2)}\subset\cdots\subset Z^{(r)}\subset X\times B8 between two ideals Z(1)Z(2)Z(r)X×BZ^{(1)}\subset Z^{(2)}\subset\cdots\subset Z^{(r)}\subset X\times B9 satisfying BB0. Setting BB1, the multi-length sequence becomes BB2. The closure BB3 retains the reduced structure but features increased negative tangent dimension, rendering it generically non-reduced.

Deformation theory furnishes the parameter count for the new moduli: BB4 which is strictly positive given nontrivial sandwiching. In BB5 with BB6, a concrete example involves

BB7

with TNT realized on the reduced component. Inserting BB8 increases negative tangent dimension by BB9 in did_i0, verifying the generic non-reducedness.

4. Reducibility of Hilbert Schemes on Singular Hypersurfaces (Theorem C)

The phenomenon extends to Hilbert schemes of points supported on singular hypersurfaces within did_i1. For a hypersurface did_i2 with a singular point of multiplicity at least 5, one shows explicitly that fat points of Hilbert function did_i3 (with total length 22) are forced to lie on did_i4. The corresponding local 2-step stratum did_i5 has dimension matching the smoothable component (did_i6), producing a new irreducible component—the 2-step locus. Consequently, did_i7 is reducible. Earlier results by Iarrobino establish reducibility of did_i8 for multiplicity did_i9.

5. Broader Consequences and Infinitely Many Non-Smoothable Chains

The existence of infinite families of non-smoothable chains of fat points in any dimension r=2r=20 is established. The outlined systematic construction offers a practical “toolbox” for generating non-reduced elementary components from reduced ones, broadening the catalog of known components. On singular threefolds or surfaces, new reducibility phenomena emerge that are tied to local singularity multiplicities. The global picture for nested Hilbert schemes in higher dimension is marked by wild birational geometry, a proliferation of elementary components (both reduced and non-reduced), and subtle wall-crossing behavior under deformations—qualities that significantly distinguish these moduli spaces from their curve or surface analogues (Graffeo et al., 23 Jan 2026).

6. Component Structure and Deformation Theory

Component structure in nested Hilbert schemes is decoded via decomposition techniques such as the Białynicki–Birula analysis for r=2r=21-actions and deformation-theoretic studies of tangent spaces. Semicontinuity of graded Betti numbers and TNT conditions enable rigorous identification of elementary components, distinguishing between reduced and non-reduced loci of nestings. The dimension formulae and moduli parameter counts allow for explicit predictions of component stratification and smoothability, underpinning further study of nested Hilbert scheme geometry.

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