Torsion-freeness of a connection and anti-symmetrization












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Let $M$ be an Hermite manifold, and $nabla$ be the Levi-Civita connection on $TM$ and extend it to $Lambda^*_{mathbb{C}}(M)$. Then $nabla$ is torsion-free by definition. But I read from a paper that the torsion-freeness implies $dtheta_i = text{Alt}(nablatheta_i)$ where ${theta_i}$ is a local frame of $Lambda^{1,0}(M)$. As far as I know, the torsion-fressness means the torsion tensor $T(X,Y) = nabla_X Y - nabla_Y X - [X,Y]equiv 0$, so how can we deduce $dtheta_i = text{Alt}(nablatheta_i)$ from this?










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    $begingroup$


    Let $M$ be an Hermite manifold, and $nabla$ be the Levi-Civita connection on $TM$ and extend it to $Lambda^*_{mathbb{C}}(M)$. Then $nabla$ is torsion-free by definition. But I read from a paper that the torsion-freeness implies $dtheta_i = text{Alt}(nablatheta_i)$ where ${theta_i}$ is a local frame of $Lambda^{1,0}(M)$. As far as I know, the torsion-fressness means the torsion tensor $T(X,Y) = nabla_X Y - nabla_Y X - [X,Y]equiv 0$, so how can we deduce $dtheta_i = text{Alt}(nablatheta_i)$ from this?










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      0





      $begingroup$


      Let $M$ be an Hermite manifold, and $nabla$ be the Levi-Civita connection on $TM$ and extend it to $Lambda^*_{mathbb{C}}(M)$. Then $nabla$ is torsion-free by definition. But I read from a paper that the torsion-freeness implies $dtheta_i = text{Alt}(nablatheta_i)$ where ${theta_i}$ is a local frame of $Lambda^{1,0}(M)$. As far as I know, the torsion-fressness means the torsion tensor $T(X,Y) = nabla_X Y - nabla_Y X - [X,Y]equiv 0$, so how can we deduce $dtheta_i = text{Alt}(nablatheta_i)$ from this?










      share|cite|improve this question









      $endgroup$




      Let $M$ be an Hermite manifold, and $nabla$ be the Levi-Civita connection on $TM$ and extend it to $Lambda^*_{mathbb{C}}(M)$. Then $nabla$ is torsion-free by definition. But I read from a paper that the torsion-freeness implies $dtheta_i = text{Alt}(nablatheta_i)$ where ${theta_i}$ is a local frame of $Lambda^{1,0}(M)$. As far as I know, the torsion-fressness means the torsion tensor $T(X,Y) = nabla_X Y - nabla_Y X - [X,Y]equiv 0$, so how can we deduce $dtheta_i = text{Alt}(nablatheta_i)$ from this?







      differential-geometry connections






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      asked Nov 24 '18 at 12:10









      J. XUJ. XU

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          This is a fact from Riemannian geometry, yes, but has nothing to do with the Hermitian structure. The key point is that you can rephrase the torsion-free condition by working with an orthonormal coframe $theta_i$ and saying
          $$dtheta_i = sum omega_{ij}wedgetheta_j$$
          with $omega_{ij}=-omega_{ji}$. (Ordinarily, you'd have $dtheta_i = sumomega_{ij}wedgetheta_j + tau_i$, where $tau$ gives the torsion.) Here $omega_{ij}$ gives the connection form.



          Then you can check that $nabla theta_i = sum omega_{ij}otimestheta_j$, and the rest is immediate, since $dtheta_i = sumomega_{ij}wedgetheta_j = sum omega_{ij}otimestheta_j - theta_jotimesomega_{ij}$.






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            $begingroup$

            This is a fact from Riemannian geometry, yes, but has nothing to do with the Hermitian structure. The key point is that you can rephrase the torsion-free condition by working with an orthonormal coframe $theta_i$ and saying
            $$dtheta_i = sum omega_{ij}wedgetheta_j$$
            with $omega_{ij}=-omega_{ji}$. (Ordinarily, you'd have $dtheta_i = sumomega_{ij}wedgetheta_j + tau_i$, where $tau$ gives the torsion.) Here $omega_{ij}$ gives the connection form.



            Then you can check that $nabla theta_i = sum omega_{ij}otimestheta_j$, and the rest is immediate, since $dtheta_i = sumomega_{ij}wedgetheta_j = sum omega_{ij}otimestheta_j - theta_jotimesomega_{ij}$.






            share|cite|improve this answer











            $endgroup$


















              0












              $begingroup$

              This is a fact from Riemannian geometry, yes, but has nothing to do with the Hermitian structure. The key point is that you can rephrase the torsion-free condition by working with an orthonormal coframe $theta_i$ and saying
              $$dtheta_i = sum omega_{ij}wedgetheta_j$$
              with $omega_{ij}=-omega_{ji}$. (Ordinarily, you'd have $dtheta_i = sumomega_{ij}wedgetheta_j + tau_i$, where $tau$ gives the torsion.) Here $omega_{ij}$ gives the connection form.



              Then you can check that $nabla theta_i = sum omega_{ij}otimestheta_j$, and the rest is immediate, since $dtheta_i = sumomega_{ij}wedgetheta_j = sum omega_{ij}otimestheta_j - theta_jotimesomega_{ij}$.






              share|cite|improve this answer











              $endgroup$
















                0












                0








                0





                $begingroup$

                This is a fact from Riemannian geometry, yes, but has nothing to do with the Hermitian structure. The key point is that you can rephrase the torsion-free condition by working with an orthonormal coframe $theta_i$ and saying
                $$dtheta_i = sum omega_{ij}wedgetheta_j$$
                with $omega_{ij}=-omega_{ji}$. (Ordinarily, you'd have $dtheta_i = sumomega_{ij}wedgetheta_j + tau_i$, where $tau$ gives the torsion.) Here $omega_{ij}$ gives the connection form.



                Then you can check that $nabla theta_i = sum omega_{ij}otimestheta_j$, and the rest is immediate, since $dtheta_i = sumomega_{ij}wedgetheta_j = sum omega_{ij}otimestheta_j - theta_jotimesomega_{ij}$.






                share|cite|improve this answer











                $endgroup$



                This is a fact from Riemannian geometry, yes, but has nothing to do with the Hermitian structure. The key point is that you can rephrase the torsion-free condition by working with an orthonormal coframe $theta_i$ and saying
                $$dtheta_i = sum omega_{ij}wedgetheta_j$$
                with $omega_{ij}=-omega_{ji}$. (Ordinarily, you'd have $dtheta_i = sumomega_{ij}wedgetheta_j + tau_i$, where $tau$ gives the torsion.) Here $omega_{ij}$ gives the connection form.



                Then you can check that $nabla theta_i = sum omega_{ij}otimestheta_j$, and the rest is immediate, since $dtheta_i = sumomega_{ij}wedgetheta_j = sum omega_{ij}otimestheta_j - theta_jotimesomega_{ij}$.







                share|cite|improve this answer














                share|cite|improve this answer



                share|cite|improve this answer








                edited Nov 25 '18 at 1:30

























                answered Nov 24 '18 at 19:29









                Ted ShifrinTed Shifrin

                63.1k44489




                63.1k44489






























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