Normal Forms for Rigid C2,1\mathfrak{C}_{2,1} Hypersurfaces M5⊂C3M^5 \subset \mathbb{C}^3

preprint2020arXivOpen access

Abstract

Consider a 22-nondegenerate constant Levi rank 11 rigid Cω\mathcal{C}^ω hypersurface M5⊂C3M^5 \subset \mathbb{C}^3 in coordinates (z,ζ,w=u+iv)(z, ζ, w = u + iv): u=F(z,ζ,zˉ,ζˉ). u = F\big(z,ζ,\bar{z},\barζ\big). The Gaussier-Merker model u=zzˉ+12z2ζˉ+12zˉ2ζ1−ζζˉu=\frac{z\bar{z}+ \frac{1}{2}z^2\barζ+\frac{1}{2} \bar{z}^2 ζ}{1-ζ\barζ} was shown by Fels-Kaup 2007 to be locally CR-equivalent to the light cone {x12+x22−x32=0}\{x_1^2+x_2^2-x_3^2=0\}. Another representation is the tube u=x21−yu=\frac{x^2}{1-y}. Inspired by Alexander Isaev, we study rigid biholomorphisms: (z,ζ,w)⟼(f(z,ζ),g(z,ζ),ρ w+h(z,ζ))=:(z′,ζ′,w′). (z,ζ,w) \longmapsto \big( f(z,ζ), g(z,ζ), ρ\,w+h(z,ζ) \big) =: (z',ζ',w'). The G-M model has 7-dimensional rigid automorphisms group. A Cartan-type reduction to an e-structure was done by Foo-Merker-Ta in 1904.02562. Three relative invariants appeared: V0V_0, I0I_0 (primary) and Q0Q_0 (derived). In Pocchiola's formalism, Section 8 provides a finalized expression for Q0Q_0. The goal is to establish the Poincaré-Moser complete normal form: u=zzˉ+12 z2ζˉ+12 zˉ2ζ1−ζζˉ+∑a,b,c,da+c⩾3 Ga,b,c,d zaζbzˉcζˉd, u = \frac{z\bar{z}+\frac{1}{2}\,z^2\barζ +\frac{1}{2}\,\bar{z}^2ζ}{ 1-ζ\barζ} + \sum_{a,b,c,d \atop a+c\geqslant 3}\, G_{a,b,c,d}\, z^aζ^b\bar{z}^c\barζ^d, with 0=Ga,b,0,0=Ga,b,1,0=Ga,b,2,00 = G_{a,b,0,0} = G_{a,b,1,0} = G_{a,b,2,0} and 0=G3,0,0,1=Im G3,0,1,10 = G_{3,0,0,1} = {\rm Im}\, G_{3,0,1,1}. We apply the method of Chen-Merker 1908.07867 to catch (relative) invariants at every point, not only at the central point, as the coefficients G0,1,4,0G_{0,1,4,0}, G0,2,3,0G_{0, 2, 3, 0}, ReG3,0,1,1{\rm Re} G_{3,0,1,1}. With this, a brige Poincaré ⟷\longleftrightarrow Cartan is constructed. In terms of FF, the numerators of V0V_0, I0I_0, Q0Q_0 incorporate 11, 52, 824 differential monomials.

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