Table B.1.
Covariances of various derivatives of the potential.
Example Terms | n1 | n2 | n3 | Value |
---|---|---|---|---|
⟨ϕ112⟩ | 4 | 0 | 0 | ![]() |
⟨ϕ11ϕ22⟩, ⟨ϕ122⟩ | 2 | 2 | 0 | ![]() |
⟨ϕ1111ϕ11⟩, ⟨ϕ1112⟩ | 6 | 0 | 0 | ![]() |
⟨ϕ1111ϕ22⟩, ⟨ϕ1112ϕ12⟩, ⟨ϕ1122⟩ | 4 | 2 | 0 | ![]() |
⟨ϕ1123ϕ23⟩, ⟨ϕ1122ϕ33⟩, ⟨ϕ1232⟩ | 2 | 2 | 2 | ![]() |
⟨ϕ11111ϕ111⟩, ⟨ϕ11112⟩ | 8 | 0 | 0 | ![]() |
⟨ϕ11111ϕ122⟩, ⟨ϕ11122⟩ | 6 | 2 | 0 | ![]() |
⟨ϕ11112ϕ222⟩, ⟨ϕ1111ϕ2222⟩, ⟨ϕ11222⟩ | 4 | 4 | 0 | ![]() |
⟨ϕ11112ϕ233⟩, ⟨ϕ1112ϕ1233⟩, ⟨ϕ11232⟩ | 4 | 2 | 2 | ![]() |
Notes. The first column is an (incomplete) list of examples to give an idea of what kind of terms fall under the same combination of n1, n2 and n3. All uneven terms are omitted, because they are zero and terms containing 0th and first derivatives are omitted, because the are not Galilei-invariant.
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