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© 2002-2007 Prof. Dr. Hans Wilhelm Alt, University of Bonn, Germany

Transposed differential operator

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Definition (Transposed operator)    [sect:1-6]

Let  L : Cm(Ω; RN) → C0(Ω; RM)  be a classical linear differential operator of order  m  with  Cm -coefficients: (as in sect:1-1):
L(u) =
 
|α|≦m
aααu ,         aα∈Cm(Ω; RM×N).
Then there exists a unique classical linear differential operator  LT  : Cm(Ω; RM) → C0(Ω; RN)  of order  m  with
 
Ω
LT(v)•u dLn =
 
Ω
v•L(u) dLn
for all  u∈Cm(Ω; RN)  and all  v∈Cm0(Ω; RM) . This differential operator is given by
LT(v) =
 
|α|≦m
(-1)|α|α(aαT v) .
We call  LT  the transposed operator of  L  or the formally adjoint operator of  L .

Proof. For  u ,  v  as in the assertion
 
Ω
v•L(u) dLn
=
 
|α|≦m
 
Ω
v•(aααu) dLn
=
 
|α|≦m
 
Ω
(aαT v) •∂αu dLn
=
 
|α|≦m
(-1)|α|
 
Ω
α(aαT v)•u dLn     (partial integration)
=
 
Ω
LT(v)•u dLn
with  LT  as in the assertion. We have to show, that the differential operator  LT  has a representation as in sect:1-1. This follows using the LEIBNIZ rule (Proof see below)
α(vw) =
 
β : 0≦β≦α
(
α
β
)α-βv ∂βw
for functions  v, w∈Cm(Ω; R) , where
(
α
β
) :=
n
i=1
(
αi
βi
) .
Applying this LEIBNIZ rule to the transposed operator we obtain
LT(v)
=
 
|α|≦m
 
β : 0≦β≦α
(-1)|α| (
α
β
)   ∂α-β aTα ∂βv
=
 
|β|≦m
(
 
α : |α|≦m, α≧β
(-1)|α| (
α
β
)   ∂α-βaTα )  ∂βv ,
which is a representation of  LT  as in sect:1-1.

Remark: This also shows, that it is sufficient to assume  aα∈C|α|(Ω' ; RM×N)  (see sect:1-7-(3) below).

It remains to prove the uniqueness of  LT . For this let  M  be another operator with the same properties as  LT  in sect:1-6. Then for all  u ,  v 

 
Ω
( LT(v)-M(v) ) •u = 0 .
Using the Fundamental Lemma of the Caculus of Variations (see [Analysis III:Fundamental lemma] ) we obtain, that  LT(v)-M(v)=0  for all  v∈C0m(Ω; RM) . We claim, that this then also holds for all  v∈Cm(Ω;RM) . This would imply  LT=M .

For the proof of this claim let  v∈Cm(Ω; RM)  and  x∈Ω . Choose a function  η∈C0m(Ω)  so, that  η=1  in a small neighbourhood of  x . Then  LT(ηv)=M(ηv) . Moreover,  ∂α(ηv)(x)=∂αv(x)  for all  |α|≦m . From the representation of the operators  LT  and  M  as linear partial differential operators in sect:1-1 it therefore follows, that  LT(ηv)(x) = LT(v)(x)  and  M(ηv)(x) = M(v)(x) . Since this holds for all  x∈Ω , we have proved that  LT(v) = M(v) .

Proof of the LEIBNIZ rule. We have to show that
[eq:1-leibniz]
α(vw)=
 
0≦β≦α
(
α
β
)α-βv ∂βw .
This can be proved by induction with respect to  α : With  γ=α+ei 
iα-β v
=
γ-βv ,
iβw
=
β+ei w .
This gives
γ(vw)
=
iα(vw)
=
 
 
β: 0≦β≦α=γ-ei
(
α
β
)γ-βv ∂βw +
 
 
ei≦β≦γ
(
α
β-ei
)γ-βv ∂βw
=
 
 
β: ei≦β≦γ-ei
( (
γ-ei
β
) + (
γ-ei
β-ei
) )γ-βv ∂βw
+
 
 
β: βi=0
(
α
β
)γ-βv ∂βw +
 
 
β: βii
(
γ-ei
β-ei
)γ-βv ∂βw
=
 
 
β: ei≦β≦γ-ei
(
γ
β
)γ-βv ∂βw
+
 
 
β: βi=0
(
γ
β
)γ-βv ∂βw +
 
 
β: βii
(
γ
β
)γ-βv ∂βw
=
 
β: 0≦γ≦β
(
γ
β
)γ-βv ∂βw .

Remark    [sect:1-7]

  • [sect:1-7-(1)] Let  L(u)= (j=1N Lij(uj) ) i=1,... M . Then
    (Lij)T=(LT)ji.
  • [sect:1-7-(2)]  (LT)T=L .
  • [sect:1-7-(3)] For the existence of the transposed operator  LT  it suffices to assume that the coefficients satisfy  aα∈C|α|(Ω; RM×N) .

Proof sect:1-7-(1). By the representation of  L  in sect:1-6
Lij(w) =
 
α: |α|≦m
(aα)ijαw ,
hence
(Lij)T(w) =
 
α: |α|≦m
(-1)|α| ∂α ( (aα)ji w ) ,
and by the representation of  LT  in sect:1-6
(LT)ij(w) =
 
α: |α|≦m
(-1)|α| ∂α ( (aTα)ij w ) .
And for the coefficients  (aTα)ij=(aα)ji .
Proof sect:1-7-(2). For  u∈C0m(Ω; RN)  and  v∈C0m(Ω; RM)  by sect:1-6
 
Ω
v •L(u) dLn =
 
Ω
LT(v)•u dLn =
 
Ω
u•LT(v) dLn =
 
Ω
( LT ) T(u)•v dLn
Hence by the Fundamental Lemma in Calculus of Variations (see [Analysis III:Fundamental lemma] )
L(u) = ( LT ) T(u)     for all u∈C0m(Ω; RN) .
As in the proof of uniqueness in sect:1-6 this then follows also for all  u∈Cm(Ω; RN) , that is,  L= ( LT ) T .
Proof sect:1-7-(3). See the proof of sect:1-6.


Version 1.5
H.W. Alt - 02.01.2007

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