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416    8. Pseudodifferential and Boundary Integral Operators

                                                                            one has
                              For the principal symbols of the local operators A χ r

                                                                  ,m χ t (x),ξ          (8.1.8)
                                             σ A χ r ,m χ r (x),ξ = σ A χ t

                           where x = T r (  )= T t (τ ) ∈ O rt ⊂ Γ and the variables ξ and ξ in IR n−1 \{0}


                           are related by the equations
                                               n−1           n−1
                                                   ∂T t          ∂T r




                                                      (τ )ξ ι =     (  )ξ .             (8.1.9)
                                                                        ι
                                                   ∂τ ι          ∂    ι
                                               ι=1            ι=1
                                                                                        m
                                                                                     ∈L (U r )
                           Conversely, if a family of local pseudodifferential operators A χ r
                           is given satisfying (8.1.7) for the whole atlas A and satisfying the smooth-
                           ing property in Definition 8.1.1, then (8.1.6) defines a pseudodifferential
                                        m
                           operatorA ∈L (Γ).
                           Proof: The equations (8.1.6) and (8.1.7) are immediate consequences of the
                           previous definitions.
                              For the transformation proposed in (8.1.8) we employ the coordinate
                                                     (−1)
                           transformation Φ rt = χ t ◦ χ r  given in (8.1.1), apply (6.1.49) to (8.1.7)
                           and obtain

                                                              (−1)      ∂Φ rt
                                           ,m (τ ,ξ )= σ A χ r ,m Φ rt  (τ ) ,  ξ    .



                                                                        ∂
                                       σ A χ t
                           The argument in the right–hand side can be expressed component–wise as
                                                  n−1        n−1 n

                                    ∂Φ rt            ∂τ             ∂τ ∂x
                                                                      λ
                                                        ξ =
                             ξ λ :=        ξ     =     λ   ι              ξ ,λ =1,...,n − 1 .
                                                                           ι
                                     ∂        λ      ∂              ∂x   ∂
                                                  ι=1  ι     ι=1  =1     ι
                           Inserting (3.4.27) with g nλ  = 0 and the inverse γ µλ  to γ tµλ =  n    ∂x   ∂x     on
                                                                      t
                                                 t
                                                                                     ∂τ   ∂τ
                                                                                   =1  µ  λ
                           Γ (c.f. (3.4.2), (3.4.4)) we find with (3.4.24), (3.4.28):
                                       n−1 n−1 n
                                                 ∂x   ∂x    µλ

                                  ξ λ =                 γ t  ξ ι  for λ =1,...,n − 1 .  (8.1.10)
                                                 ∂τ ∂    ι

                                                   µ
                                       ι=1 µ=1  =1
                           On the other hand, if (8.1.9) is satisfied, the scalar multiplication of both
                           sides of (8.1.9) by  ∂τ   gives
                                            ∂T t
                                             µ
                                               n−1        n−1 n
                                                                 ∂x   ∂x
                                                  γ tµι ξ ι =           ξ .
                                                                        ι
                                                                 ∂  ∂τ

                                               ι=1        ι=1  =1  ι  µ
                                            µλ
                           Multiplication by γ  yields
                                            t
                                                    n−1 n−1 n
                                                              ∂x   ∂x

                                               ξ λ =                 γ t µλ   ι
                                                                        ξ ,
                                                              ∂  ∂τ

                                                    µ=1 ι=1  =1  ι  µ
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