Checking my understanding (re. wedge product) of a passage in Bishop & Goldberg

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The discussion centers on the interpretation of the coefficients of a skew-symmetric bilinear form as presented in Bishop & Goldberg's "Tensor Analysis on Manifolds." It establishes that the coefficients b_{ij} correspond to b(e_i, e_j) rather than 2b(e_i, e_j), clarifying the relationship between tensor products and exterior products. The rank of the bilinear form is defined consistently regardless of whether it is expressed in tensor product or wedge product terms. This conclusion is supported by the mathematical definitions and examples provided in the text.

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Rasalhague
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The rank of a skew-symmetric bilinear form is the minimum number of vectors in terms of which it can be expressed. We may think of a skew-symmetric bilinear form b on V as being in \wedge^2V^*. If b can be written in terms of \varepsilon^1...\varepsilon^r, then we may discard any independent \varepsilon^i's and extend to a basis, getting

b = b_{ij}\varepsilon^i \otimes \varepsilon^j, \enspace\enspace \text{where } b_{ij} = 0 \text{ unless } i,j \leq r,

=b_{ij}\varepsilon^i \wedge \varepsilon^j, \enspace\enspace \text{since } b_{ij} = -b_{ji},

so it does not matter, in the definition of rank, whether the mode of expressing b is in terms of tensor products or exterior products.

- Bishop & Goldberg: Tensor Analysis on Manifolds, Dover 1980, §2.23, pp. 111-112

Given that Bishop and Goldberg's definition of the exterior product is

\alpha \wedge \beta := (\alpha \otimes \beta)_a

where

\omega_a(v_1,...,v_s):=\frac{1}{s!}\sum_{(i_1,...,i_s)}\text{sgn}(i_1,...,i_s)A(v_{i_1},...v_{i_s}),

giving, in this case,

\alpha\wedge\beta=\frac{1}{2}(\alpha\otimes\beta-\beta\otimes\alpha),

am I right in thinking that the coefficients b_{ij} in the quote above are not b(e_i,e_j), but rather b_{ij} = 2b(e_i,e_j)?

By (e_i), I mean the basis for V with dual basis (\varepsilon^i).
 
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Ah, no, looking again at this, I think they must mean the usual coefficient b_{ij}=b(e_i,e_j) after all.

A factor of 2 would be needed to convert components with respect to a tensor product basis (\varepsilon^i\otimes\varepsilon^j) for T^0_2 (all permutations of the indices) to the corresponding wedge product basis (\varepsilon^i\wedge\varepsilon^j) (only increasing permutations) for \wedge^2 V^*. But in this case, I think, they're not restricting the indices to only increasing permutations.

So, for example, if \text{dim} V = 3 and b=b_{12} \varepsilon^1\otimes\varepsilon^2 + b_{21} \varepsilon^2\otimes\varepsilon^1, where b_{12}=-b_{21}, we have

b=b_{12} \varepsilon^1\otimes\varepsilon^2 + b_{21} \varepsilon^2\otimes\varepsilon^1

=b_{12} \varepsilon^1\otimes\varepsilon^2 - b_{12} \varepsilon^2\otimes\varepsilon^1

=b_{12} (\varepsilon^1\otimes\varepsilon^2 - \varepsilon^2\otimes\varepsilon^1)

=\frac{1}{2}b_{12} (2\varepsilon^1\otimes\varepsilon^2 - 2\varepsilon^2\otimes\varepsilon^1)

=\frac{1}{2}b_{12} (\varepsilon^1\otimes\varepsilon^2 - \varepsilon^2\otimes\varepsilon^1 - \varepsilon^2\otimes\varepsilon^1 + \varepsilon^1\otimes\varepsilon^2)

=\frac{1}{2}b_{12} (\varepsilon^1\otimes\varepsilon^2 - \varepsilon^2\otimes\varepsilon^1) - \frac{1}{2}b_{12}(\varepsilon^2\otimes\varepsilon^1-\varepsilon^1\otimes\varepsilon^2)

=b_{12} \, \varepsilon^1\wedge\varepsilon^2 - b_{12} \, \varepsilon^2\wedge\varepsilon^1

=b_{12} \, \varepsilon^1\wedge\varepsilon^2 + b_{21} \, \varepsilon^2\wedge\varepsilon^1,

just as they claim.
 
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