Equivalence and symmetries of first order differential equations

Equivalence and symmetries of first order differential equations

Peer-reviewed article not indexed in WoS or Scopus

In this article, the equivalence and symmetries of underdetermined differential equations and differential equations with deviations of the first order are considered with respect to the pseudogroup of transformations $\bar x=\varphi (x),$ $\bar y=\bar y(\bar x)=L(x)y(x).$ That means, the transformed unknown function $\bar y$ is obtained by means of the change of the independent variable and subsequent multiplication by a~nonvanishing factor. Instead of the common direct calculations, we use some more advanced tools from differential geometry, however, exposition is self--contained and only the most fundamental properties of differential forms are employed. We refer to analogous achievements in the literature. In particular, the generalized higher symmetry problem involving a~finite number of invariants of the kind $F^j=a_j y\, \Pi |z_i|^{k^j_i}=a_j y |z_1|^{k^j_1} \ldots |z_m|^{k^j_m}=a_j(x)y|y(\xi_1)|^{k^j_1}\ldots |y(\xi_m)|^{k^j_m}$ is compared to similar results obtained by means of auxiliary functional equations.

In this article, the equivalence and symmetries of underdetermined differential equations and differential equations with deviations of the first order are considered with respect to the pseudogroup of transformations $\bar x=\varphi (x),$ $\bar y=\bar y(\bar x)=L(x)y(x).$ That means, the transformed unknown function $\bar y$ is obtained by means of the change of the independent variable and subsequent multiplication by a~nonvanishing factor. Instead of the common direct calculations, we use some more advanced tools from differential geometry, however, exposition is self--contained and only the most fundamental properties of differential forms are employed. We refer to analogous achievements in the literature. In particular, the generalized higher symmetry problem involving a~finite number of invariants of the kind $F^j=a_j y\, \Pi |z_i|^{k^j_i}=a_j y |z_1|^{k^j_1} \ldots |z_m|^{k^j_m}=a_j(x)y|y(\xi_1)|^{k^j_1}\ldots |y(\xi_m)|^{k^j_m}$ is compared to similar results obtained by means of auxiliary functional equations.

differential equations with deviations, equivalence of differential equations, symmetry of differential equation, differential invariants, moving frames

differential equations with deviations, equivalence of differential equations, symmetry of differential equation, differential invariants, moving frames

TRYHUK, V.

2010

01.10.2008

ČSAV

Praha

0011-4642

CZECHOSLOVAK MATHEMATICAL JOURNAL

58

133

Czech Republic

605

635

31