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?










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    0












    $begingroup$


    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?










    share|cite|improve this question











    $endgroup$















      0












      0








      0





      $begingroup$


      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?










      share|cite|improve this question











      $endgroup$




      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






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      edited Jan 1 at 12:02







      Quasar

















      asked Dec 30 '18 at 10:02









      QuasarQuasar

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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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            $begingroup$

            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 $sum_jdtildeomega^jotimes(sum_ia^i_je_i)=sum_j dtildeomega^jotimes f_j$.






            share|cite|improve this answer











            $endgroup$


















              1












              $begingroup$

              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 $sum_jdtildeomega^jotimes(sum_ia^i_je_i)=sum_j dtildeomega^jotimes f_j$.






              share|cite|improve this answer











              $endgroup$
















                1












                1








                1





                $begingroup$

                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 $sum_jdtildeomega^jotimes(sum_ia^i_je_i)=sum_j dtildeomega^jotimes f_j$.






                share|cite|improve this answer











                $endgroup$



                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 $sum_jdtildeomega^jotimes(sum_ia^i_je_i)=sum_j dtildeomega^jotimes f_j$.







                share|cite|improve this answer














                share|cite|improve this answer



                share|cite|improve this answer








                edited Jan 2 at 12:15

























                answered Jan 2 at 10:31









                Andreas CapAndreas Cap

                11.5k923




                11.5k923






























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