Why is the exterior differential independent of the chosen basis?
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Let M be as smooth manifold, W a k-dimensional vector space with basis $(e_1,...,e_k)$ and $Omega^r(M,W)$ be the differential r-form on M with values in W. Let $omega in Omega^r$ and $v_1,..., v_r in T_xM$. Then we can write $omega_x(v_1,...,v_r)$ as a linear combination of the $e_i$ as follows: $w_x(v_1,...,v_r) = omega_x^i(v_1,...,v_r)e_i$, i.e. both $omega_x$ and $omega_x^i$ are multilinear maps and $omega_i$ is a differential r-form on M. Let's now define the exterior differential as a sheaf morphism from $Omega^r(M,W) rightarrow Omega^{r+1}(M,W)$:
$$d(omega^iotimes w_i):=domega_iotimes e_i.$$
My question is now why this is independent of the basis we have chosen for W?
differential-geometry sheaf-theory exterior-derivative
$endgroup$
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$begingroup$
Let M be as smooth manifold, W a k-dimensional vector space with basis $(e_1,...,e_k)$ and $Omega^r(M,W)$ be the differential r-form on M with values in W. Let $omega in Omega^r$ and $v_1,..., v_r in T_xM$. Then we can write $omega_x(v_1,...,v_r)$ as a linear combination of the $e_i$ as follows: $w_x(v_1,...,v_r) = omega_x^i(v_1,...,v_r)e_i$, i.e. both $omega_x$ and $omega_x^i$ are multilinear maps and $omega_i$ is a differential r-form on M. Let's now define the exterior differential as a sheaf morphism from $Omega^r(M,W) rightarrow Omega^{r+1}(M,W)$:
$$d(omega^iotimes w_i):=domega_iotimes e_i.$$
My question is now why this is independent of the basis we have chosen for W?
differential-geometry sheaf-theory exterior-derivative
$endgroup$
add a comment |
$begingroup$
Let M be as smooth manifold, W a k-dimensional vector space with basis $(e_1,...,e_k)$ and $Omega^r(M,W)$ be the differential r-form on M with values in W. Let $omega in Omega^r$ and $v_1,..., v_r in T_xM$. Then we can write $omega_x(v_1,...,v_r)$ as a linear combination of the $e_i$ as follows: $w_x(v_1,...,v_r) = omega_x^i(v_1,...,v_r)e_i$, i.e. both $omega_x$ and $omega_x^i$ are multilinear maps and $omega_i$ is a differential r-form on M. Let's now define the exterior differential as a sheaf morphism from $Omega^r(M,W) rightarrow Omega^{r+1}(M,W)$:
$$d(omega^iotimes w_i):=domega_iotimes e_i.$$
My question is now why this is independent of the basis we have chosen for W?
differential-geometry sheaf-theory exterior-derivative
$endgroup$
Let M be as smooth manifold, W a k-dimensional vector space with basis $(e_1,...,e_k)$ and $Omega^r(M,W)$ be the differential r-form on M with values in W. Let $omega in Omega^r$ and $v_1,..., v_r in T_xM$. Then we can write $omega_x(v_1,...,v_r)$ as a linear combination of the $e_i$ as follows: $w_x(v_1,...,v_r) = omega_x^i(v_1,...,v_r)e_i$, i.e. both $omega_x$ and $omega_x^i$ are multilinear maps and $omega_i$ is a differential r-form on M. Let's now define the exterior differential as a sheaf morphism from $Omega^r(M,W) rightarrow Omega^{r+1}(M,W)$:
$$d(omega^iotimes w_i):=domega_iotimes e_i.$$
My question is now why this is independent of the basis we have chosen for W?
differential-geometry sheaf-theory exterior-derivative
differential-geometry sheaf-theory exterior-derivative
edited Jan 1 at 12:02
Quasar
asked Dec 30 '18 at 10:02
QuasarQuasar
1278
1278
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The reason is that the change of basis is given by constants. If you take a basis ${f_j}$ then you get an invertible matrix $A=(a_j^i)$ charakterized by the fact that $f_j=sum_i a_j^ie_i$. Then writing $omega$ as $sum_jtildeomega^jotimes f_j$ we see that $omega=sum_iomega^iotimes e_i$, where $omega^i=sum_j a^j_itildeomega^j$. But since the $a^j_i$ are constants, this implies $domega^i=sum_j a^j_idtildeomega^j$ and so $sum_idomega^iotimes e_i=sum_{i,j}a^j_idtildeomega^jotimes e_i$. But then the constants can be brought to the other factor in the tensor product (the right one) and the $dtildeomega^j$ can be taken out of the sum over $i$ to obtain $sum_jdtildeomega^jotimes(sum_ia^i_je_i)=sum_j dtildeomega^jotimes f_j$.
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1 Answer
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$begingroup$
The reason is that the change of basis is given by constants. If you take a basis ${f_j}$ then you get an invertible matrix $A=(a_j^i)$ charakterized by the fact that $f_j=sum_i a_j^ie_i$. Then writing $omega$ as $sum_jtildeomega^jotimes f_j$ we see that $omega=sum_iomega^iotimes e_i$, where $omega^i=sum_j a^j_itildeomega^j$. But since the $a^j_i$ are constants, this implies $domega^i=sum_j a^j_idtildeomega^j$ and so $sum_idomega^iotimes e_i=sum_{i,j}a^j_idtildeomega^jotimes e_i$. But then the constants can be brought to the other factor in the tensor product (the right one) and the $dtildeomega^j$ can be taken out of the sum over $i$ to obtain $sum_jdtildeomega^jotimes(sum_ia^i_je_i)=sum_j dtildeomega^jotimes f_j$.
$endgroup$
add a comment |
$begingroup$
The reason is that the change of basis is given by constants. If you take a basis ${f_j}$ then you get an invertible matrix $A=(a_j^i)$ charakterized by the fact that $f_j=sum_i a_j^ie_i$. Then writing $omega$ as $sum_jtildeomega^jotimes f_j$ we see that $omega=sum_iomega^iotimes e_i$, where $omega^i=sum_j a^j_itildeomega^j$. But since the $a^j_i$ are constants, this implies $domega^i=sum_j a^j_idtildeomega^j$ and so $sum_idomega^iotimes e_i=sum_{i,j}a^j_idtildeomega^jotimes e_i$. But then the constants can be brought to the other factor in the tensor product (the right one) and the $dtildeomega^j$ can be taken out of the sum over $i$ to obtain $sum_jdtildeomega^jotimes(sum_ia^i_je_i)=sum_j dtildeomega^jotimes f_j$.
$endgroup$
add a comment |
$begingroup$
The reason is that the change of basis is given by constants. If you take a basis ${f_j}$ then you get an invertible matrix $A=(a_j^i)$ charakterized by the fact that $f_j=sum_i a_j^ie_i$. Then writing $omega$ as $sum_jtildeomega^jotimes f_j$ we see that $omega=sum_iomega^iotimes e_i$, where $omega^i=sum_j a^j_itildeomega^j$. But since the $a^j_i$ are constants, this implies $domega^i=sum_j a^j_idtildeomega^j$ and so $sum_idomega^iotimes e_i=sum_{i,j}a^j_idtildeomega^jotimes e_i$. But then the constants can be brought to the other factor in the tensor product (the right one) and the $dtildeomega^j$ can be taken out of the sum over $i$ to obtain $sum_jdtildeomega^jotimes(sum_ia^i_je_i)=sum_j dtildeomega^jotimes f_j$.
$endgroup$
The reason is that the change of basis is given by constants. If you take a basis ${f_j}$ then you get an invertible matrix $A=(a_j^i)$ charakterized by the fact that $f_j=sum_i a_j^ie_i$. Then writing $omega$ as $sum_jtildeomega^jotimes f_j$ we see that $omega=sum_iomega^iotimes e_i$, where $omega^i=sum_j a^j_itildeomega^j$. But since the $a^j_i$ are constants, this implies $domega^i=sum_j a^j_idtildeomega^j$ and so $sum_idomega^iotimes e_i=sum_{i,j}a^j_idtildeomega^jotimes e_i$. But then the constants can be brought to the other factor in the tensor product (the right one) and the $dtildeomega^j$ can be taken out of the sum over $i$ to obtain $sum_jdtildeomega^jotimes(sum_ia^i_je_i)=sum_j dtildeomega^jotimes f_j$.
edited Jan 2 at 12:15
answered Jan 2 at 10:31
Andreas CapAndreas Cap
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