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?
differential-geometry connections
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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?
differential-geometry connections
$endgroup$
add a comment |
$begingroup$
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?
differential-geometry connections
$endgroup$
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
differential-geometry connections
asked Nov 24 '18 at 12:10
J. XUJ. XU
431214
431214
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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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1 Answer
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1 Answer
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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 $dtheta_i = sumomega_{ij}wedgetheta_j = sum omega_{ij}otimestheta_j - theta_jotimesomega_{ij}$.
$endgroup$
add a comment |
$begingroup$
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 $dtheta_i = sumomega_{ij}wedgetheta_j = sum omega_{ij}otimestheta_j - theta_jotimesomega_{ij}$.
$endgroup$
add a comment |
$begingroup$
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 $dtheta_i = sumomega_{ij}wedgetheta_j = sum omega_{ij}otimestheta_j - theta_jotimesomega_{ij}$.
$endgroup$
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 $dtheta_i = sumomega_{ij}wedgetheta_j = sum omega_{ij}otimestheta_j - theta_jotimesomega_{ij}$.
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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