How is the anti-symmetry property used to show that the tensor product is symmetric in the free indi

How is the anti-symmetry property used to show that the tensor product is symmetric in the free indices?

The anti-symmetry property of the magnetic field tensor, Fij=Fji\mathbf{F}{ij} = -\mathbf{F}{ji}, is used to show the symmetry of the product Mik=FijFjk\mathbf{M}{ik} = \mathbf{F}{ij} \mathbf{F}{jk} by demonstrating that Mik\mathbf{M}{ik} is equal to its transpose, Mki\mathbf{M}_{ki}.

Here is the step-by-step application:

🛡️ Proof of Symmetry

  1. Define the Transpose: Start with the transpose of the tensor product, Mki\mathbf{M}_{ki}:

    Mki=FkjFji \mathbf{M}{ki} = \mathbf{F}{kj} \mathbf{F}_{ji}

  2. Apply Anti-Symmetry: Substitute the anti-symmetry relation (Fab=Fba\mathbf{F}{ab} = -\mathbf{F}{ba}) to both terms in the transpose:

    • Fkj=Fjk\mathbf{F}{kj} = -\mathbf{F}{jk}

    • Fji=Fij\mathbf{F}{ji} = -\mathbf{F}{ij}

    Substituting these gives:

    Mki=(Fjk)(Fij) \mathbf{M}{ki} = (-\mathbf{F}{jk})(-\mathbf{F}_{ij})

  3. Simplify and Reorder: The two negative signs multiply to a positive sign, and because jj is a dummy summation index, the order of multiplication of the scalar terms can be changed:

    Mki=FjkFij=FijFjk \mathbf{M}{ki} = \mathbf{F}{jk} \mathbf{F}{ij} = \mathbf{F}{ij} \mathbf{F}_{jk}

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