Abstract
We prove a global algebraic version of the Lie–Tresse theorem which states that the algebra of differential invariants of an algebraic pseudogroup action on a differential equation is generated by a finite number of rational-polynomial differential invariants and invariant derivations.
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Notes
In the local case one restricts to a neighborhood \(\hat{U}=\pi _{\infty ,0}^{-1}(U)\subset J^\infty \) for an open set \(U\subset M\), while in the microlocal case \(\hat{U}=\pi _{\infty ,k}^{-1}(U)\subset J^\infty \) for some open set \(U\subset J^k\).
Ultimately, when \(l\rightarrow \infty \), we get functions that are smooth in the base variables and rational on the fibers. The theory applies to this class as well (and is simpler).
The equivalence problems of geometric structures on a manifold can be set up to be a partial case of our general setting for equivalence of submanifolds.
When we turn to the algebraic situation, then “open” becomes “Zariski open.”
To keep the notations simple, we denote the required subset in the set of regular points by the same symbol \({\mathcal {E}}_l''\subset {\mathcal {E}}_l'\) (we also abuse notations by redefining l several times).
Though the Lie–Tresse–Kumpera pseudogroup is not transitive (and so formally our theorems are not applicable), this is the case where our theory still works.
Over characteristic 0 this theorem states that a finite extension E of a field K is generated by one element \(E=K(\alpha )\), see, e.g., [31, V. §4: Theorem 4.6].
Here by \(\dim \mathcal {A}\) we understand the maximal number of functionally independent differential invariants (recall that any function of differential invariants is a differential invariant itself, so the dimension of \(\mathcal {A}\) as a vector space is either 1 or \(\infty \)).
The are two obvious choices for the invariant differentiations: derivatives \(\mathfrak {D}({\mathcal {E}},\tau )\) and derivations \(\mathfrak {Der}({\mathcal {E}},\tau )\). We choose the latter, because the primary goal is to generate \({\mathcal {A}}\).
Here D means a module over the algebra \(\mathfrak {Diff}({\mathcal {E}},\tau )\). Notice that the algebra \(\mathfrak {Diff}({\mathcal {E}},\tau )\) is generated by \({\mathcal {A}}\) and \(\nabla _j\), and so is finitely generated by \(I_i\) and \(\nabla _j\).
Notice that the Hilbert and Poincaré functions are related by \(H^{\mathcal {E}}_G(k)=\frac{1}{k!}\left. \frac{{\text {d}}^k}{{\text {d}}z^k}\right| _{z=0}P^{\mathcal {E}}_G(z)\).
Some people interpret them as the microlocal differential invariants, but we believe that the moduli are meant to be the actual global invariants.
This makes the group action intransitive, but it is irrelevant for this example. Simply add the sixth generator \(\partial _u\) to \({\mathfrak {g}}\), or observe that all our constructions work without this.
The condition of “no resonances” can be omitted since the functions \(I_2,I_4,\dots \) below are invariants anyway, but this condition relates them to the Birkhoff normal form and shows that no more independent invariants exist.
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Kruglikov, B., Lychagin, V. Global Lie–Tresse theorem. Sel. Math. New Ser. 22, 1357–1411 (2016). https://doi.org/10.1007/s00029-015-0220-z
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DOI: https://doi.org/10.1007/s00029-015-0220-z
Keywords
- Algebraic group
- Pseudogroup action
- Rational differential invariant
- Invariant derivation
- Tresse derivative
- Differential syzygy
- Orbits separation
- Spencer cohomology