Table 1.
Orthogonal basis tensors that we consider here.
Tensor | Index Representation | Norm2 | ϕ contr. |
---|---|---|---|
J2 | S2(δij) | 3 | δ |
J22 | S22(δijδkl) | 9 | δ2 |
J2 = 2 | ![]() |
5 | K2 |
J4 | S4(δijδkl) | 5 | L |
J3 − 3 | S33(δijδklδmn) | ![]() |
(∇δ)2 |
J3 ≡ 3 | ![]() |
7 | S3 ≡ 3 |
J24 | S24(δijδklδmn) | 15 | δL |
J2 = 4 | ![]() |
![]() |
ϕ2 = 4 |
Notes. The first column indicates the label we use for the tensor, the second column one possible way of defining it in index notation, the third column the square of its norm (as the full contraction with itself) and the last column the term that is obtained when fully contracting it with the corresponding derivatives of the potential as in the bias expansion.
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