Understanding Electromagnetic Duality: From B_i to E_i Using Tensor Notation

AI Thread Summary
The discussion focuses on demonstrating electromagnetic duality by transforming B_i to E_i using tensor notation. The user attempts to derive this transformation directly from B_i but encounters discrepancies in their calculations, particularly with the Levi-Civita symbol and the indices involved. They express confusion over obtaining a result of -3/2 F_{i0} instead of the expected F_{i0} = E_i. Feedback indicates a misunderstanding of the relationship between B_i and the dual field tensor, suggesting that B_i corresponds to the 0i row in the dual tensor. Clarification on these tensor relationships is necessary to resolve the issue.
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So, I'm trying to show that by duality B_{i}\rightarrow E_{i}, using tensor notation. I've done it in a different way, and it works (starting from \overline{F}_{ij}, the dual of F_ij), but I would like to get it from B_i directly. Where am I going wrong?

This is what I did:

B_{i}=\frac{1}{2}\epsilon_{ijk}F^{jk}\rightarrow B'_{i}=\frac{1}{2}\epsilon_{ijk}(i\overline{F}^{jk})=\frac{1}{2}i\epsilon_{ijk}(-\frac{1}{2}i\epsilon^{jk\rho\sigma}F_{\rho\sigma})
=\frac{1}{4}\epsilon_{ijk}\epsilon^{jk\rho\sigma}F_{\rho\sigma}=\frac{1}{4}\epsilon_{0ijk}\epsilon^{jk0i}F_{0i}

where in the last line I have inserted an extra 0-index in the Levi-Civita symbol (although I am not sure I know how to deal with zeros with epsilon), and made the substitution (\rho,\sigma)\rightarrow(0,i).

However I calculate this to be -\frac{3}{2}F_{i0} when it should be just F_{i0}=E_{i}

Any advice?
 
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I don't understand your first equation for B'. B_i in the dual F is the 0i row, not what you write.
 
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