Matrix associated of an application between tangent spaces











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Let $M$ be a differential manifold and $X$ a vector field over $M$ s.t. $X(p) = 0$ for some $p in M$. Let be $phi_p : T_p(M) to T_p(M)$ given as $$phi_p(v) := [Y,X](p),$$ being $Y$ another vector field of $M$ s.t. $Y(p) = v$.



For $X = sum_{i=1}^nX_ifrac{partial}{partial x_i}$ calculate the associated matrix of $phi_p$ with respect the basis ${(frac{partial}{partial x_i})}_{1 leq i leq m}$.



Can you help me, please?



And another question: Since $phi_p(v) = [Y,X](p) = Y(X(p)) - X(Y(p)) = Y(0) - X(v) = -X(v)$, can we assert that $phi_p$ does not depend of $Y$?



Thanks










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    Let $M$ be a differential manifold and $X$ a vector field over $M$ s.t. $X(p) = 0$ for some $p in M$. Let be $phi_p : T_p(M) to T_p(M)$ given as $$phi_p(v) := [Y,X](p),$$ being $Y$ another vector field of $M$ s.t. $Y(p) = v$.



    For $X = sum_{i=1}^nX_ifrac{partial}{partial x_i}$ calculate the associated matrix of $phi_p$ with respect the basis ${(frac{partial}{partial x_i})}_{1 leq i leq m}$.



    Can you help me, please?



    And another question: Since $phi_p(v) = [Y,X](p) = Y(X(p)) - X(Y(p)) = Y(0) - X(v) = -X(v)$, can we assert that $phi_p$ does not depend of $Y$?



    Thanks










    share|cite|improve this question


























      up vote
      0
      down vote

      favorite









      up vote
      0
      down vote

      favorite











      Let $M$ be a differential manifold and $X$ a vector field over $M$ s.t. $X(p) = 0$ for some $p in M$. Let be $phi_p : T_p(M) to T_p(M)$ given as $$phi_p(v) := [Y,X](p),$$ being $Y$ another vector field of $M$ s.t. $Y(p) = v$.



      For $X = sum_{i=1}^nX_ifrac{partial}{partial x_i}$ calculate the associated matrix of $phi_p$ with respect the basis ${(frac{partial}{partial x_i})}_{1 leq i leq m}$.



      Can you help me, please?



      And another question: Since $phi_p(v) = [Y,X](p) = Y(X(p)) - X(Y(p)) = Y(0) - X(v) = -X(v)$, can we assert that $phi_p$ does not depend of $Y$?



      Thanks










      share|cite|improve this question















      Let $M$ be a differential manifold and $X$ a vector field over $M$ s.t. $X(p) = 0$ for some $p in M$. Let be $phi_p : T_p(M) to T_p(M)$ given as $$phi_p(v) := [Y,X](p),$$ being $Y$ another vector field of $M$ s.t. $Y(p) = v$.



      For $X = sum_{i=1}^nX_ifrac{partial}{partial x_i}$ calculate the associated matrix of $phi_p$ with respect the basis ${(frac{partial}{partial x_i})}_{1 leq i leq m}$.



      Can you help me, please?



      And another question: Since $phi_p(v) = [Y,X](p) = Y(X(p)) - X(Y(p)) = Y(0) - X(v) = -X(v)$, can we assert that $phi_p$ does not depend of $Y$?



      Thanks







      differential-geometry manifolds tangent-spaces






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      edited yesterday









      Ethan Bolker

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      user540275

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          Your last computation is wrong (it actually doesn't make any sense to write $Y(X(p))$) and leads me to believe that the definition of $[Y,X]$ is not clear to you. Here is how it goes. Basically, you need to test how vector fields act on smooth functions. Let $fin C^infty(M)$ and let $X=X^ipartial_i$, $Y=Y^jpartial_j$, where by $partial_i$ I denote $partial/partial_{x_i}$ and I use Einstein summation convention for conciseness. Then
          $$
          begin{split}
          [Y,X](f) &= Y(X(f))-X(Y(f)) \
          &= Y^jpartial_j(X^ipartial_if)-X^ipartial_i(Y^jpartial_jf) \
          &= Y^j(partial_jX^i)partial_if-X^i(partial_iY^j)partial_jf ,
          end{split}
          $$

          because the terms involving second order derivatives of $f$ cancel by Schwarz's theorem.



          At point $p$, we have $X_p^i=0$ and $Y_p^j=v^j$, therefore only the first term remains
          $$
          [Y,X]_p = v^j(partial_jX^i)_ppartial_i .
          $$

          In particular, this shows that $[Y,X]_p$ only depends on the value of $Y$ at point $p$, which is $Y_p=v$, and not on the actual vector field itself.



          The matrix representation can be recovered from $phi_p(v) = phi_p(v)^ipartial_i$ from which
          $$
          phi_p(v)^i = (partial_jX^i)_p v^j = M^i_j v^j
          $$

          with $M^i_j=(partial_jX^i)_p$. The transformation $phi_p$ is linear and depends only on the derivatives of $X$ at $p$.






          share|cite|improve this answer























          • So you get $[Y,X](f) = sum_{j=1}^nsum_{i=1}^n v_jBigl(frac{partial X_i}{partial x_j} frac{partial}{partial x_i}Bigr)(p).$ And the matix $phi_p(v) = sum_{i=1}^nphi_p(v)_i frac{partial}{partial x_i}$, with $phi_p(v)_i = Bigl(frac{partial}{partial x_j} X_iBigr)(p)v_j$?
            – user540275
            yesterday










          • Yes. That is precisely what I wrote, apart from putting the indices in their most common position. Also, you are missing an $f$ in the r.h.s. of your first formula.
            – Federico
            yesterday










          • Ok. And $phi_p (v)_i = phi_p(v_i)$? I suppose, since $phi_p$ is linear (since the partial derivations are linears).
            – user540275
            yesterday












          • No. $v^i$ is the $i$-th component of $v$ written in the base $(partial_i)_{i=1}^m$, that is, $v=v^ipartial_i$. It doesn't make sense to write $phi_p(v_i)$. $phi_p$ requires a vector, you cannot feed it just a single coordinate. By $phi_p(v)^i$ i mean the $i$-th component of $phi_p(v)$ written in the base $(partial_i)_{i=1}^m$, that is, $phi_p(v)=phi_p(v)^ipartial_i$.
            – Federico
            yesterday











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          up vote
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          Your last computation is wrong (it actually doesn't make any sense to write $Y(X(p))$) and leads me to believe that the definition of $[Y,X]$ is not clear to you. Here is how it goes. Basically, you need to test how vector fields act on smooth functions. Let $fin C^infty(M)$ and let $X=X^ipartial_i$, $Y=Y^jpartial_j$, where by $partial_i$ I denote $partial/partial_{x_i}$ and I use Einstein summation convention for conciseness. Then
          $$
          begin{split}
          [Y,X](f) &= Y(X(f))-X(Y(f)) \
          &= Y^jpartial_j(X^ipartial_if)-X^ipartial_i(Y^jpartial_jf) \
          &= Y^j(partial_jX^i)partial_if-X^i(partial_iY^j)partial_jf ,
          end{split}
          $$

          because the terms involving second order derivatives of $f$ cancel by Schwarz's theorem.



          At point $p$, we have $X_p^i=0$ and $Y_p^j=v^j$, therefore only the first term remains
          $$
          [Y,X]_p = v^j(partial_jX^i)_ppartial_i .
          $$

          In particular, this shows that $[Y,X]_p$ only depends on the value of $Y$ at point $p$, which is $Y_p=v$, and not on the actual vector field itself.



          The matrix representation can be recovered from $phi_p(v) = phi_p(v)^ipartial_i$ from which
          $$
          phi_p(v)^i = (partial_jX^i)_p v^j = M^i_j v^j
          $$

          with $M^i_j=(partial_jX^i)_p$. The transformation $phi_p$ is linear and depends only on the derivatives of $X$ at $p$.






          share|cite|improve this answer























          • So you get $[Y,X](f) = sum_{j=1}^nsum_{i=1}^n v_jBigl(frac{partial X_i}{partial x_j} frac{partial}{partial x_i}Bigr)(p).$ And the matix $phi_p(v) = sum_{i=1}^nphi_p(v)_i frac{partial}{partial x_i}$, with $phi_p(v)_i = Bigl(frac{partial}{partial x_j} X_iBigr)(p)v_j$?
            – user540275
            yesterday










          • Yes. That is precisely what I wrote, apart from putting the indices in their most common position. Also, you are missing an $f$ in the r.h.s. of your first formula.
            – Federico
            yesterday










          • Ok. And $phi_p (v)_i = phi_p(v_i)$? I suppose, since $phi_p$ is linear (since the partial derivations are linears).
            – user540275
            yesterday












          • No. $v^i$ is the $i$-th component of $v$ written in the base $(partial_i)_{i=1}^m$, that is, $v=v^ipartial_i$. It doesn't make sense to write $phi_p(v_i)$. $phi_p$ requires a vector, you cannot feed it just a single coordinate. By $phi_p(v)^i$ i mean the $i$-th component of $phi_p(v)$ written in the base $(partial_i)_{i=1}^m$, that is, $phi_p(v)=phi_p(v)^ipartial_i$.
            – Federico
            yesterday















          up vote
          0
          down vote













          Your last computation is wrong (it actually doesn't make any sense to write $Y(X(p))$) and leads me to believe that the definition of $[Y,X]$ is not clear to you. Here is how it goes. Basically, you need to test how vector fields act on smooth functions. Let $fin C^infty(M)$ and let $X=X^ipartial_i$, $Y=Y^jpartial_j$, where by $partial_i$ I denote $partial/partial_{x_i}$ and I use Einstein summation convention for conciseness. Then
          $$
          begin{split}
          [Y,X](f) &= Y(X(f))-X(Y(f)) \
          &= Y^jpartial_j(X^ipartial_if)-X^ipartial_i(Y^jpartial_jf) \
          &= Y^j(partial_jX^i)partial_if-X^i(partial_iY^j)partial_jf ,
          end{split}
          $$

          because the terms involving second order derivatives of $f$ cancel by Schwarz's theorem.



          At point $p$, we have $X_p^i=0$ and $Y_p^j=v^j$, therefore only the first term remains
          $$
          [Y,X]_p = v^j(partial_jX^i)_ppartial_i .
          $$

          In particular, this shows that $[Y,X]_p$ only depends on the value of $Y$ at point $p$, which is $Y_p=v$, and not on the actual vector field itself.



          The matrix representation can be recovered from $phi_p(v) = phi_p(v)^ipartial_i$ from which
          $$
          phi_p(v)^i = (partial_jX^i)_p v^j = M^i_j v^j
          $$

          with $M^i_j=(partial_jX^i)_p$. The transformation $phi_p$ is linear and depends only on the derivatives of $X$ at $p$.






          share|cite|improve this answer























          • So you get $[Y,X](f) = sum_{j=1}^nsum_{i=1}^n v_jBigl(frac{partial X_i}{partial x_j} frac{partial}{partial x_i}Bigr)(p).$ And the matix $phi_p(v) = sum_{i=1}^nphi_p(v)_i frac{partial}{partial x_i}$, with $phi_p(v)_i = Bigl(frac{partial}{partial x_j} X_iBigr)(p)v_j$?
            – user540275
            yesterday










          • Yes. That is precisely what I wrote, apart from putting the indices in their most common position. Also, you are missing an $f$ in the r.h.s. of your first formula.
            – Federico
            yesterday










          • Ok. And $phi_p (v)_i = phi_p(v_i)$? I suppose, since $phi_p$ is linear (since the partial derivations are linears).
            – user540275
            yesterday












          • No. $v^i$ is the $i$-th component of $v$ written in the base $(partial_i)_{i=1}^m$, that is, $v=v^ipartial_i$. It doesn't make sense to write $phi_p(v_i)$. $phi_p$ requires a vector, you cannot feed it just a single coordinate. By $phi_p(v)^i$ i mean the $i$-th component of $phi_p(v)$ written in the base $(partial_i)_{i=1}^m$, that is, $phi_p(v)=phi_p(v)^ipartial_i$.
            – Federico
            yesterday













          up vote
          0
          down vote










          up vote
          0
          down vote









          Your last computation is wrong (it actually doesn't make any sense to write $Y(X(p))$) and leads me to believe that the definition of $[Y,X]$ is not clear to you. Here is how it goes. Basically, you need to test how vector fields act on smooth functions. Let $fin C^infty(M)$ and let $X=X^ipartial_i$, $Y=Y^jpartial_j$, where by $partial_i$ I denote $partial/partial_{x_i}$ and I use Einstein summation convention for conciseness. Then
          $$
          begin{split}
          [Y,X](f) &= Y(X(f))-X(Y(f)) \
          &= Y^jpartial_j(X^ipartial_if)-X^ipartial_i(Y^jpartial_jf) \
          &= Y^j(partial_jX^i)partial_if-X^i(partial_iY^j)partial_jf ,
          end{split}
          $$

          because the terms involving second order derivatives of $f$ cancel by Schwarz's theorem.



          At point $p$, we have $X_p^i=0$ and $Y_p^j=v^j$, therefore only the first term remains
          $$
          [Y,X]_p = v^j(partial_jX^i)_ppartial_i .
          $$

          In particular, this shows that $[Y,X]_p$ only depends on the value of $Y$ at point $p$, which is $Y_p=v$, and not on the actual vector field itself.



          The matrix representation can be recovered from $phi_p(v) = phi_p(v)^ipartial_i$ from which
          $$
          phi_p(v)^i = (partial_jX^i)_p v^j = M^i_j v^j
          $$

          with $M^i_j=(partial_jX^i)_p$. The transformation $phi_p$ is linear and depends only on the derivatives of $X$ at $p$.






          share|cite|improve this answer














          Your last computation is wrong (it actually doesn't make any sense to write $Y(X(p))$) and leads me to believe that the definition of $[Y,X]$ is not clear to you. Here is how it goes. Basically, you need to test how vector fields act on smooth functions. Let $fin C^infty(M)$ and let $X=X^ipartial_i$, $Y=Y^jpartial_j$, where by $partial_i$ I denote $partial/partial_{x_i}$ and I use Einstein summation convention for conciseness. Then
          $$
          begin{split}
          [Y,X](f) &= Y(X(f))-X(Y(f)) \
          &= Y^jpartial_j(X^ipartial_if)-X^ipartial_i(Y^jpartial_jf) \
          &= Y^j(partial_jX^i)partial_if-X^i(partial_iY^j)partial_jf ,
          end{split}
          $$

          because the terms involving second order derivatives of $f$ cancel by Schwarz's theorem.



          At point $p$, we have $X_p^i=0$ and $Y_p^j=v^j$, therefore only the first term remains
          $$
          [Y,X]_p = v^j(partial_jX^i)_ppartial_i .
          $$

          In particular, this shows that $[Y,X]_p$ only depends on the value of $Y$ at point $p$, which is $Y_p=v$, and not on the actual vector field itself.



          The matrix representation can be recovered from $phi_p(v) = phi_p(v)^ipartial_i$ from which
          $$
          phi_p(v)^i = (partial_jX^i)_p v^j = M^i_j v^j
          $$

          with $M^i_j=(partial_jX^i)_p$. The transformation $phi_p$ is linear and depends only on the derivatives of $X$ at $p$.







          share|cite|improve this answer














          share|cite|improve this answer



          share|cite|improve this answer








          edited yesterday

























          answered yesterday









          Federico

          1,99158




          1,99158












          • So you get $[Y,X](f) = sum_{j=1}^nsum_{i=1}^n v_jBigl(frac{partial X_i}{partial x_j} frac{partial}{partial x_i}Bigr)(p).$ And the matix $phi_p(v) = sum_{i=1}^nphi_p(v)_i frac{partial}{partial x_i}$, with $phi_p(v)_i = Bigl(frac{partial}{partial x_j} X_iBigr)(p)v_j$?
            – user540275
            yesterday










          • Yes. That is precisely what I wrote, apart from putting the indices in their most common position. Also, you are missing an $f$ in the r.h.s. of your first formula.
            – Federico
            yesterday










          • Ok. And $phi_p (v)_i = phi_p(v_i)$? I suppose, since $phi_p$ is linear (since the partial derivations are linears).
            – user540275
            yesterday












          • No. $v^i$ is the $i$-th component of $v$ written in the base $(partial_i)_{i=1}^m$, that is, $v=v^ipartial_i$. It doesn't make sense to write $phi_p(v_i)$. $phi_p$ requires a vector, you cannot feed it just a single coordinate. By $phi_p(v)^i$ i mean the $i$-th component of $phi_p(v)$ written in the base $(partial_i)_{i=1}^m$, that is, $phi_p(v)=phi_p(v)^ipartial_i$.
            – Federico
            yesterday


















          • So you get $[Y,X](f) = sum_{j=1}^nsum_{i=1}^n v_jBigl(frac{partial X_i}{partial x_j} frac{partial}{partial x_i}Bigr)(p).$ And the matix $phi_p(v) = sum_{i=1}^nphi_p(v)_i frac{partial}{partial x_i}$, with $phi_p(v)_i = Bigl(frac{partial}{partial x_j} X_iBigr)(p)v_j$?
            – user540275
            yesterday










          • Yes. That is precisely what I wrote, apart from putting the indices in their most common position. Also, you are missing an $f$ in the r.h.s. of your first formula.
            – Federico
            yesterday










          • Ok. And $phi_p (v)_i = phi_p(v_i)$? I suppose, since $phi_p$ is linear (since the partial derivations are linears).
            – user540275
            yesterday












          • No. $v^i$ is the $i$-th component of $v$ written in the base $(partial_i)_{i=1}^m$, that is, $v=v^ipartial_i$. It doesn't make sense to write $phi_p(v_i)$. $phi_p$ requires a vector, you cannot feed it just a single coordinate. By $phi_p(v)^i$ i mean the $i$-th component of $phi_p(v)$ written in the base $(partial_i)_{i=1}^m$, that is, $phi_p(v)=phi_p(v)^ipartial_i$.
            – Federico
            yesterday
















          So you get $[Y,X](f) = sum_{j=1}^nsum_{i=1}^n v_jBigl(frac{partial X_i}{partial x_j} frac{partial}{partial x_i}Bigr)(p).$ And the matix $phi_p(v) = sum_{i=1}^nphi_p(v)_i frac{partial}{partial x_i}$, with $phi_p(v)_i = Bigl(frac{partial}{partial x_j} X_iBigr)(p)v_j$?
          – user540275
          yesterday




          So you get $[Y,X](f) = sum_{j=1}^nsum_{i=1}^n v_jBigl(frac{partial X_i}{partial x_j} frac{partial}{partial x_i}Bigr)(p).$ And the matix $phi_p(v) = sum_{i=1}^nphi_p(v)_i frac{partial}{partial x_i}$, with $phi_p(v)_i = Bigl(frac{partial}{partial x_j} X_iBigr)(p)v_j$?
          – user540275
          yesterday












          Yes. That is precisely what I wrote, apart from putting the indices in their most common position. Also, you are missing an $f$ in the r.h.s. of your first formula.
          – Federico
          yesterday




          Yes. That is precisely what I wrote, apart from putting the indices in their most common position. Also, you are missing an $f$ in the r.h.s. of your first formula.
          – Federico
          yesterday












          Ok. And $phi_p (v)_i = phi_p(v_i)$? I suppose, since $phi_p$ is linear (since the partial derivations are linears).
          – user540275
          yesterday






          Ok. And $phi_p (v)_i = phi_p(v_i)$? I suppose, since $phi_p$ is linear (since the partial derivations are linears).
          – user540275
          yesterday














          No. $v^i$ is the $i$-th component of $v$ written in the base $(partial_i)_{i=1}^m$, that is, $v=v^ipartial_i$. It doesn't make sense to write $phi_p(v_i)$. $phi_p$ requires a vector, you cannot feed it just a single coordinate. By $phi_p(v)^i$ i mean the $i$-th component of $phi_p(v)$ written in the base $(partial_i)_{i=1}^m$, that is, $phi_p(v)=phi_p(v)^ipartial_i$.
          – Federico
          yesterday




          No. $v^i$ is the $i$-th component of $v$ written in the base $(partial_i)_{i=1}^m$, that is, $v=v^ipartial_i$. It doesn't make sense to write $phi_p(v_i)$. $phi_p$ requires a vector, you cannot feed it just a single coordinate. By $phi_p(v)^i$ i mean the $i$-th component of $phi_p(v)$ written in the base $(partial_i)_{i=1}^m$, that is, $phi_p(v)=phi_p(v)^ipartial_i$.
          – Federico
          yesterday


















           

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