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7.2 Coordinate Changes and Pseudohomogeneous Kernels  411



                                               (x ,x − y ) ∼   k κ+j (x ,x − y )

                                            k A Φ
                                                            j≥0
                           be the pseudohomogeneous kernel expansion of the transformed Schwartz ker-
                           nel to A Φ in terms of the new coordinates. Then the parity conditions in
                           (7.2.35) are invariant under the change of coordinates, i.e.



                             k κ+j (x ,x − y )=(−1)  m−j+σ 0
                                                        k κ+j (x ,x − y ) for 0 ≤ j ≤ L. (7.2.36)

                           Proof: For the proof we employ Lemma 7.1.9. Then (7.2.35) is equivalent
                           to
                               a 0  (x, −ξ)=(−1) m−k−σ 0 0  (x, ξ)for ξ  =0 and 0 ≤ j ≤ L,
                                                       a
                                m−j                     m−j
                                                                                       (7.2.37)
                           where a 0  are the homogeneous symbols of the complete symbol expansion
                                  m−j
                           of A. Since the symbol a Φ (x ,ξ ) is given by (6.1.45) with (6.1.46), by rear-


                           ranging terms, the corresponding asymptotic homogeneous expansion of the
                           symbol reads
                                  0


                                 a Φ,m−j (x ,ξ )
                              j≥0
                                      j
                                                       α
                                                                                   x − y
                                             1      ∂        ∂Φ    −1          −1

                              =                 − i       det        Ξ (x ,y )  Ψ         ×


                                            α!     ∂y        ∂y                       ε
                                j≥0   =0 |α|=
                                                       ∂     0
                                                            α                    −1


                                                   ×        a m−j+   x, Ξ (x ,y    ξ    | y   =x   .
                                                       ∂ξ
                           We observe that (7.2.37) implies
                                ∂    0
                                    α                     −1
                                    a m−j+   x, − Ξ (x ,y    ξ


                               ∂ξ
                                                              ∂    0
                                                                  α                    −1
                                               =(−1) m−j+σ 0      a m−j+   x, Ξ (x ,y    ξ     .


                                                             ∂ξ
                           Then it follows from the above representation that
                                                                   a


                                         a 0   (x , −ξ )=(−1) m−j+σ 0 0  (x , −ξ )


                                          Φ,m−j                     Φ,m−j
                           which implies (7.2.37) by the application of Lemma 7.1.9 again.
                              To conclude this section, we observe for the Tricomi conditions, that as a
                                                                 m
                                                                                        m

                           consequence of Theorem 6.1.13 and A ∈L (Ω), we also have A ∈L (Ω ).

                                                                 c                      c
                           Hence, one may apply Theorem 7.1.7 to the kernels k κ+j and k κ+j of A

                           and A, respectively. This yields the following lemma which shows that the

                           Tricomi conditions are invariant under the change of coordinates.
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