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Leaps in Integrable Derivation Modules

Updated 8 December 2025
  • The topic defines leaps as strict drops in the chain of Hasse–Schmidt-integrable derivations, typically occurring at p-power indices.
  • It demonstrates that the arithmetic of prime characteristic and binomial combinatorics control the integrability and singularity structure in commutative algebras.
  • Methodologies using combinatorial identities and Artin–Rees techniques establish finite leaps and provide effective tools for analyzing derivation modules.

A leap of modules of integrable derivations refers to a strict drop in the chain of modules of Hasse–Schmidt-integrable derivations associated to a commutative algebra over a ring of positive characteristic. This phenomenon encodes subtle invariants of the singularity structure of the algebra and is controlled by the arithmetic of the prime characteristic pp and the properties of the algebraic structure. The subject lies at the intersection of algebraic geometry, commutative algebra, and the theory of differential operators in positive characteristic, connecting module-theoretic, cohomological, and singularity-theoretic aspects.

1. Hasse–Schmidt Integrable Derivations

Let kk be a commutative ring and AA a unital commutative kk-algebra. A Hasse–Schmidt derivation of AA over kk of length mN{}m\in\mathbb{N}\cup\{\infty\} is a sequence of kk-linear endomorphisms

D=(D0,D1,,Dm)D = (D_0, D_1, \ldots, D_m)

satisfying D0=IdAD_0 = \operatorname{Id}_A and, for all a,bAa, b \in A and nmn\leq m,

Dn(ab)=i+j=nDi(a)Dj(b).D_n(ab) = \sum_{i+j=n} D_i(a) D_j(b).

The space HSk(A;m)\mathrm{HS}_k(A;m) denotes all such sequences. The first component D1D_1 is an ordinary kk-derivation; higher DnD_n are differential operators of order n\leq n, vanishing at $1$. A kk-derivation δDerk(A)\delta \in \operatorname{Der}_k(A) is called nn-integrable (nN{}n\in\mathbb{N}\cup\{\infty\}) if there exists DHSk(A;n)D\in \mathrm{HS}_k(A;n) with D1=δD_1 = \delta. This leads to the descending chain of AA-submodules:

IDerk(A;1)IDerk(A;2)IDerk(A;)\operatorname{IDer}_k(A;1) \supseteq \operatorname{IDer}_k(A;2) \supseteq \cdots \supseteq \operatorname{IDer}_k(A;\infty)

where IDerk(A;n)\operatorname{IDer}_k(A;n) consists of derivations that are nn-integrable in the Hasse–Schmidt sense (Hernández, 2019, Bravo et al., 27 Sep 2024, Miyamoto, 30 Nov 2025, Narváez-Macarro, 2011).

2. Filtration and Leaps: Definition and Characterization

A leap occurs at n>1n>1 if

IDerk(A;n1)IDerk(A;n)\operatorname{IDer}_k(A;n-1) \supsetneq \operatorname{IDer}_k(A;n)

i.e., if there exists a derivation integrable up to order n1n-1 but not to order nn. The set of such nn is denoted Leapsk(A)\operatorname{Leaps}_k(A). These inclusions generally stabilize after finitely many steps. For a scheme XX essentially of finite type over kk, there is a corresponding decreasing chain of quasi-coherent sheaves of integrable derivations:

Derk(OX)Derkp(OX)Derkp2(OX)\mathcal{D}er_k(\mathcal{O}_X) \supset \mathcal{D}er^p_k(\mathcal{O}_X) \supset \mathcal{D}er^{p^2}_k(\mathcal{O}_X) \supset \cdots

and XX “leaps” at pip^i if the inclusion at that stage is strict (Miyamoto, 30 Nov 2025, Bravo et al., 27 Sep 2024, Narváez-Macarro, 2011).

3. Restrictions on Possible Leaps: Powers of pp

A central result establishes that, for kk of characteristic p>0p>0, strict inclusions—i.e., leaps—can only occur at n=prn=p^r for r1r\geq 1. For all nn not a pure pp–power, the modules remain constant:

IDerk(A;n1)=IDerk(A;n)if n is not a power of p\operatorname{IDer}_k(A;n-1) = \operatorname{IDer}_k(A;n) \quad\text{if } n\text{ is not a power of } p

This result, proved via a sequence of combinatorial and lifting arguments, utilizes intricate binomial identities, properties of the characteristic pp residue field, and an induction on the pp–adic expansion of nn. The restriction to pp–power indices is intrinsic to the binomial combinatorics present in positive characteristic (Hernández, 2019, Miyamoto, 30 Nov 2025).

4. Finiteness of Leaps and Structural Theorems

For algebras essentially of finite type over an algebraically closed field of characteristic p>0p>0, the set of leaps is always finite. Specifically, there is some M0M\gg 0 such that

Derkm(A)=Derkm+1(A)==Derk(A)for mM\operatorname{Der}^m_k(A) = \operatorname{Der}^{m+1}_k(A) = \cdots = \operatorname{Der}^\infty_k(A) \quad\text{for } m\geq M

and

Leapsk(A){p,p2,...,pM1}\operatorname{Leaps}_k(A) \subset \{p, p^2, ..., p^{M-1}\}

The proof involves constructing and analyzing obstruction modules ObRpiTR/k1\operatorname{Ob}_R^{p^i} \subset T^1_{R/k} (where TR/k1T^1_{R/k} is the module of first cotangent cohomology), and using Artin–Rees techniques to show that, after a bounded stage, all further extension problems for integrable derivations are unobstructed (Miyamoto, 30 Nov 2025, Bravo et al., 27 Sep 2024).

Locally, the number of leaps is bounded by lengths of finite modules or dimensions of appropriate quotients; for instance,

Leapsk(Ap)dimκ(p)(Derk(Ap)/pMDerk(Ap))|\operatorname{Leaps}_k(A_\mathfrak{p})| \le \dim_{\kappa(\mathfrak{p})} \left( \operatorname{Der}_k(A_\mathfrak{p}) / \mathfrak{p}^M \operatorname{Der}_k(A_\mathfrak{p}) \right)

for minimal primes p\mathfrak{p} of the critical Fitting ideal (Bravo et al., 27 Sep 2024).

5. Role of Fitting Ideals and Singularities

Let ΩA/k\Omega_{A/k} denote the module of Kähler differentials; its Fitting ideals, specifically Jr(A)J_r(A)—the ideal of (nr)(n-r)-minors of a presenting Jacobian—play a decisive role. For (reduced) complete intersection algebras A=R/(f1,,fr)A=R/(f_1,\ldots,f_r), any derivation vanishing on Jr(A)J_r(A) is \infty-integrable; thus, the critical Fitting ideal detects loci where nontrivial leaps may occur. Singularities where the Jacobian drops rank control higher-order integrability, and the support of the successive quotients IDerk(A;m)/IDerk(A;m+1)\operatorname{IDer}_k(A;m)/\operatorname{IDer}_k(A;m+1) is contained in the singular locus (Bravo et al., 27 Sep 2024).

These conclusions extend to the context of schemes and formal power series. Localizations at minimal primes of Jr(A)J_r(A) reduce leap detection to the paper of finite-length vector space quotients. This mechanism provides effective criteria for the finiteness of leaps and explicit bounds in concrete settings.

6. Examples, Applications, and Algorithmic Aspects

Explicit examples:

  • For A=k[x]/(xp)A = k[x]/(x^p) in characteristic pp, δ=d/dx\delta = d/dx is (p1)(p-1)-integrable but not pp-integrable, so a leap occurs at pp.
  • For the plane cuspidal curve k[x,y]/(y2x3)k[x,y]/(y^2 - x^3) in p=2p=2, there is a single leap at $2$, with all higher modules stabilizing.
  • For reduced one-dimensional kk-algebras over perfect fields, leaps are always finite and concentrated at finitely many pp-powers determined by the conductor.

Computational algorithm: For a finitely presented algebra A=k[x1,,xn]/IA=k[x_1,\ldots,x_n]/I and integer N2N\geq2, an explicit finite-step algorithm determines the sets IDerk(A;m)\operatorname{IDer}_k(A;m) for all mNm\leq N and thus locates the possible leaps (Narváez-Macarro, 2011).

7. Theoretical Implications and Open Problems

Finiteness and pp–power restriction for leaps sharpen previous results of Narváez-Macarro, Molinelli, and others. These results provide a discrete invariant of singularities in positive characteristic, encoding subtle information about wild ramification and the structure of higher-order differential operators. The theory establishes a bridge between integrable-derivation modules and classical algebraic invariants such as the module of Kähler differentials and cotangent cohomology.

Open questions include explicit descriptions of the modules IDerk(A;pr)\operatorname{IDer}_k(A;p^r) in terms of singularity data, analogues for non-commutative or graded algebras, and the behavior of the gap Derk(A)/IDerk(A;pr)\operatorname{Der}_k(A)/\operatorname{IDer}_k(A;p^r) as an arithmetic measure of singularity. Another direction concerns the relation of this theory to stratification problems in arithmetic and geometric D-module theory in positive characteristic (Hernández, 2019, Miyamoto, 30 Nov 2025, Bravo et al., 27 Sep 2024).

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