Simple identity for antisymmetric tensor

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The identity \(\nabla_\mu \nabla_\nu F^{\mu\nu} = 0\) is valid for antisymmetric tensors \(F^{\mu\nu}\) when using a torsion-free connection, as the symmetrization of the covariant derivatives cancels the antisymmetric components. However, the validity can depend on the definition of the connection; for a general affine connection, the result may involve the Ricci tensor, which is symmetric and leads to zero only under specific conditions. It's noted that \(\nabla_\mu \nabla_\rho\) is not symmetric, and its antisymmetric part relates to the curvature tensor. The discussion emphasizes that the identity holds for commuting vector fields like \(\partial_\mu\) and \(\partial_\nu\). Understanding these nuances is crucial for applying the identity correctly in various contexts.
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Is it true that for all antisymmetric tensors F^{\mu\nu}
the following identity is true:
\nabla_\mu \nabla_\nu F^{\mu\nu}=0
(I've checked it but I'm not absolutely sure).
 
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hi paweld! :smile:
paweld said:
Is it true that for all antisymmetric tensors F^{\mu\nu}
the following identity is true:
\nabla_\mu \nabla_\nu F^{\mu\nu}=0
(I've checked it but I'm not absolutely sure).

yup, because ∇µρ is symmetric in µ and ρ, so it zeroes anything antisymmetric in µ and ρ :wink:
 
That depends on how you define \nabla_\mu. For a general affine connection you get, more or less, \pm R_{\mu\nu}F^{\mu\nu} (plus or minus depending on which convention is being used in the definition of the Ricci tensor). When there is no torsion, Ricci tensor is symmetric and you get zero. But not so for a general connection.
 
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Thanks, I always assume that connection is torsion-free.
 
BTW:

∇µ∇ρ is not symmetric in µ and ρ. Its antisymmetric part is related to the curvature tensor.

d493bbad067a502909d1ae33781994cc.png


The above holds for u,v commuting vector fields like \partial_\mu,\, \partial_\nu
 
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