basic tensor (original) (raw)
The present entry employs the terminology and notation defined and described in the entry on tensor arrays. To keep things reasonably self-contained we mention that the symbol Tp,q refers to thevector space of type (p,q) tensor arrays, i.e. maps
where I is some finite list of index labels, and where 𝕂 is a field.
We say that a tensor array is a characteristic array, a.k.a. abasic tensor, if all but one of its values are 0, and the remaining non-zero value is equal to 1. For tuples A∈Ip andB∈Iq, we let
denote the characteristic array defined by
(εAB)j1…jqi1…ip={1 if (i1,…,ip)=A and (j1,…,jp)=B,0 otherwise. |
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The type (p,q) characteristic arrays form a natural basis forTp,q.
Furthermore the outer multiplication of two characteristic arrays gives a characteristic array of larger valence. In other words, for
A1∈Ip1,B1∈Iq1,A2∈Ip2,B2∈Iq2, |
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we have that
where the product on the left-hand side is performed by outer multiplication, and where A1A2 on the right-hand side refers to the element of Ip1+p2 obtained by concatenating the tuplesA1 and A2, and similarly for B1B2.
In this way we see that the type (1,0) characteristic arraysε(i),i∈I (the natural basis of 𝕂I), and the type(0,1) characteristic arrays ε(i),i∈I (the natural basis of(𝕂I)*) generate the tensor array algebra relative to the outer multiplication operation.
The just-mentioned fact gives us an alternate way of writing and thinking about tensor arrays. We introduce the basic symbols
subject to the commutation relations
ε(i)ε(i′)=ε(i′)ε(i),i,i′∈I, |
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add and multiply these symbols using coefficients in𝕂, and use
ε(j1…jp)(i1…iq),i1,…,iq,j1,…,jp∈I |
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as a handy abbreviation for
ε(i1)…ε(iq)ε(j1)…ε(jp). |
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We then interpret the resulting expressions as tensor arrays in theobvious fashion: the values of the tensor array are just the coefficients of the ε symbol matching the given index. However, note that in the ε symbols, the covariant data is written as asuperscript, and the contravariant data as a subscript. This is done to facilitate the Einstein summation convention.
By way of illustration, suppose that I=(1,2). We can now write down a type (1,0) tensor, i.e. a column vector
as
Similarly, a row-vector
can be written down as
In the case of a matrix
we would write
M=M11ε(1)(1)+M21ε(1)(2)+M12ε(2)(1)+M22ε(2)(2). |
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