Аннотация:
The aim of the talk is to classify binary forms, whose coefficients
depend on control parameter, with respect to the action of some
pseudogroup. We solve this problem in two steps. Firstly, we
consider the action of our pseudogroup on the infinite prolongation
of the differential Euler equation and find differential invariant
algebra of this action. Secondly, using methods from geometric
theory of differential equations, we prove that three dependencies
between basic differential invariants and their invariant
derivatives uniquely define the equivalent class of binary forms
with control parameter.
Let us consider the space $V_n(u)$ of binary forms, whose
coefficients depend on the control parameter:
$$
f(x,y;u)=\sum\limits_{i=0}^n a_i(u)x^iy^{n-i}, \quad \text{where
$a_i$ are holomorphic functions.}
$$
The pseudogroup $G:=\mathrm{SL}_2\leftthreetimes
(\mathcal{F}(u)\times \mathrm{T}(u))$ acts on the space $V_n(u)$ in
the following way:
1) “semisimple part” $\mathrm{SL}_2$ acts by linear transformations of
the coordinates $(x,y)$:
$$
\mathrm{SL}_2\ni A\colon \left(
\begin{matrix} x\\y \end{matrix}\right)\mapsto A^{-1}\left(
\begin{matrix} x\\y \end{matrix}\right);
$$
2) “functional part” $\mathcal{F}(u)$ acts by holomorphic transformations
of the control parameter: $u\mapsto \varphi(u)$;
3) “torus” $\mathrm{T}(u)$ acts by multiplications on the holomorphic
functions on the control parameter: $f\mapsto \lambda(u) f$.
Consider space $\mathbb{C}^3$ with coordinates $(x,y,u)$ and $k$-jet
space $J^k$ of functions on it (all necessary definitions and facts
can be found in [1]). Denote by $(x,y,u,h,
h_x,h_y,h_u,\ldots)$ the coordinates in $k$-jet space.
Binary forms with control parameter can be considered as solutions
of the Euler differential equation $$
\mathcal{E}:=\{x h_x+y h_y=nh\}\subset J^1$$ (see also [2]). The action of the
pseudogroup $G$ on 0-jet space $J^0$ prolongs to the action on all
prolongations $\mathcal{E}^{(k-1)}\subset J^k$
(see [1]).
$ $ Definition 1.Differential invariant of the action of pseudogroup$G$of
order$k$ is $G$-invariant function on manifold
$\mathcal{E}^{(k-1)}$, which is polynomial in derivatives
$h_\sigma$, $h^{-1}$ and $(h_xh_{yu}-h_yh_{xu})^{-1}$ (see
Theorem 1).
$ $ Remark.
Function $h_xh_{yu}-h_yh_{xu}$ is “total Poisson bracket” $\{h, h_u\}$.
Hence this function is a differential semi–invariant of pseudogroup $G$
(see [3]).
$ $ Definition 2.Invariant derivative is a combination of total derivatives,
which commutes with the action of group $G$.
$ $ Theorem 1.Differential invariant algebra of the action of pseudogroup$G$on
the manifold$\mathcal{E}^{(\infty)}$is freely generated by
differential invariant $$
H:=\frac{h_{xx}h_{yy}-h^2_{xy}}{h^2}$$ of order 2 and by invariant
derivatives $$\nabla_1:=\frac{h_y}{h}D_x-\frac{h_x}{h}D_y \quad \text{and} \quad
\nabla_2:=\frac{h^2}{h_xh_{yu}-h_yh_{xu}}\cdot D_u
$$ (where$D_x$,
$D_y$, $D_u$are total derivative operators with respect to
variables$x$, $y$, $u$correspondingly).
$ $ Definition 3.
Binary form $f\in V_n(u)$ is said to be regular, if the
restrictions of the invariants $H$, $H_1$ and $H_2$ on form $f$ are
functionally independent in points of some domain $\Omega\subset
\mathbb{C}^3$ (here indexes denote the corresponding invariant
derivatives $\nabla_1$ and $\nabla_2$).
$ $ Consider the regular binary form $f$. Then the restrictions of
invariants $H_{11}$, $H_{12}$ and $H_{22}$ on form $f$ can be
extended through the restrictions of the invariants $H$, $H_1$ and
$H_2$ on $f$:
$$
H_{11}=A(H,H_1,H_2), \;\;H_{12}=B(H,H_1,H_2),
\;\;H_{22}=C(H,H_1,H_2).
$$
The triple $(A,B,C)$ is said to be triple of dependencies of
form $f$.
$ $ Theorem 2.Two regular binary forms$f$and$\widetilde{f}$with control
parameters are$G$-equivalent iff the triples of dependencies
coincide: $$
(A,B,C)=(\widetilde{A},\widetilde{B},\widetilde{C}).
$$
$ $ The author is supported by RFBR, grand mol_a-14-01-31045.
Alekseevskii D., Vinogradov A., Lychagin V. Basic ideas and concepts of differential geometry. VINITI, vol. 28, 1988. English translation in Geometry I. Encycl. Math. Sci., 28, 1991.
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