Codifferential of k-th exterior power endmorphism applied to differential form $delta(wedge^p Aalpha)$? ...
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Codifferential of k-th exterior power endmorphism applied to differential form $delta(wedge^p Aalpha)$?
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Planned maintenance scheduled April 23, 2019 at 23:30 UTC (7:30pm US/Eastern)Understanding the Definition of a Differential Form of Degree $k$Reconciling the meaning of the codifferential in two contextsIs there a codifferential for a covariant exterior derivative?What is the rank of a differential formProve that $p-$form $omega$ on $Mtimes N$ is $delta pi(alpha)$ iff $i(X)omega=0$ and $L_Xomega=0$Distinction or rule about $d$ and $delta$ in differential formsExterior Derivative and Lie DerivativeHow does the hodge codifferential operator act over a wedge product?interplay: exterior algebra, tensor algebra, differential formsCodifferential / divergence of differential form under conformal metric change
$begingroup$
Let $(M,g)$ be an $n$-dimensional smooth Riemannian manifold without boundary. Given an endomorphism $A(x) : sf T_x^*M to sf T_x^*M$ on the cotangent bundle, we can extend $A$ to an endomorphism on the $p$-th exterior power acting on a $p$-form $alpha$ by
begin{align*}
wedge^p A : wedge^p sf T_x^*M &to wedge^p sf T_x^*M\
wedge^p A(alpha_1 wedge ... wedge alpha_p) &:= Aalpha_1 wedge ... wedge Aalpha_p.
end{align*}
How can we make sense of the codifferential
$$delta(wedge^p Aalpha)?$$
The problem is that $dim wedge^p sf T_x^*M = {n choose p}$, unlike the case $dim wedge^n sf T_x^*M = {n choose n} = 1$, where $wedge^n A$ must act as a multiplication operator, i.e. the determinant.
But $delta$ is not a derivation of the algebra, i.e. there is no nice version of the Leibniz rule. Either using the definition of $delta = ast , mathbf d , ast $ directly or using the definition that it is the formal adjoint of the exterior derivative $mathbf d$, the question boils down to: What is the exterior derivative of this $k$-th power endomorphism $wedge^p A$?
differential-geometry differential-forms
$endgroup$
add a comment |
$begingroup$
Let $(M,g)$ be an $n$-dimensional smooth Riemannian manifold without boundary. Given an endomorphism $A(x) : sf T_x^*M to sf T_x^*M$ on the cotangent bundle, we can extend $A$ to an endomorphism on the $p$-th exterior power acting on a $p$-form $alpha$ by
begin{align*}
wedge^p A : wedge^p sf T_x^*M &to wedge^p sf T_x^*M\
wedge^p A(alpha_1 wedge ... wedge alpha_p) &:= Aalpha_1 wedge ... wedge Aalpha_p.
end{align*}
How can we make sense of the codifferential
$$delta(wedge^p Aalpha)?$$
The problem is that $dim wedge^p sf T_x^*M = {n choose p}$, unlike the case $dim wedge^n sf T_x^*M = {n choose n} = 1$, where $wedge^n A$ must act as a multiplication operator, i.e. the determinant.
But $delta$ is not a derivation of the algebra, i.e. there is no nice version of the Leibniz rule. Either using the definition of $delta = ast , mathbf d , ast $ directly or using the definition that it is the formal adjoint of the exterior derivative $mathbf d$, the question boils down to: What is the exterior derivative of this $k$-th power endomorphism $wedge^p A$?
differential-geometry differential-forms
$endgroup$
add a comment |
$begingroup$
Let $(M,g)$ be an $n$-dimensional smooth Riemannian manifold without boundary. Given an endomorphism $A(x) : sf T_x^*M to sf T_x^*M$ on the cotangent bundle, we can extend $A$ to an endomorphism on the $p$-th exterior power acting on a $p$-form $alpha$ by
begin{align*}
wedge^p A : wedge^p sf T_x^*M &to wedge^p sf T_x^*M\
wedge^p A(alpha_1 wedge ... wedge alpha_p) &:= Aalpha_1 wedge ... wedge Aalpha_p.
end{align*}
How can we make sense of the codifferential
$$delta(wedge^p Aalpha)?$$
The problem is that $dim wedge^p sf T_x^*M = {n choose p}$, unlike the case $dim wedge^n sf T_x^*M = {n choose n} = 1$, where $wedge^n A$ must act as a multiplication operator, i.e. the determinant.
But $delta$ is not a derivation of the algebra, i.e. there is no nice version of the Leibniz rule. Either using the definition of $delta = ast , mathbf d , ast $ directly or using the definition that it is the formal adjoint of the exterior derivative $mathbf d$, the question boils down to: What is the exterior derivative of this $k$-th power endomorphism $wedge^p A$?
differential-geometry differential-forms
$endgroup$
Let $(M,g)$ be an $n$-dimensional smooth Riemannian manifold without boundary. Given an endomorphism $A(x) : sf T_x^*M to sf T_x^*M$ on the cotangent bundle, we can extend $A$ to an endomorphism on the $p$-th exterior power acting on a $p$-form $alpha$ by
begin{align*}
wedge^p A : wedge^p sf T_x^*M &to wedge^p sf T_x^*M\
wedge^p A(alpha_1 wedge ... wedge alpha_p) &:= Aalpha_1 wedge ... wedge Aalpha_p.
end{align*}
How can we make sense of the codifferential
$$delta(wedge^p Aalpha)?$$
The problem is that $dim wedge^p sf T_x^*M = {n choose p}$, unlike the case $dim wedge^n sf T_x^*M = {n choose n} = 1$, where $wedge^n A$ must act as a multiplication operator, i.e. the determinant.
But $delta$ is not a derivation of the algebra, i.e. there is no nice version of the Leibniz rule. Either using the definition of $delta = ast , mathbf d , ast $ directly or using the definition that it is the formal adjoint of the exterior derivative $mathbf d$, the question boils down to: What is the exterior derivative of this $k$-th power endomorphism $wedge^p A$?
differential-geometry differential-forms
differential-geometry differential-forms
edited Mar 29 at 0:05
wueb
asked Mar 22 at 18:49
wuebwueb
34129
34129
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