Here is a partial answer: Define Sp(2N,R) as the group of matrices S such that S⋅Ω⋅ST=Ω where Ωij is a non-degenerate anti-symmetric matrix. Then Ωij is an invariant tensor similar to the Kronecker delta for orthogonal transformations. I don't think there are any more (not 100% sure).
For E7: E7 may be defined to be the group that preserves a antisymmetric second-rank tensor gμν and a totally symmetric fourth-rank tensor fμνρσ with μ,ν,ρ,σ=1,2,…,56 (i.e., the 56 dimensional representation is the defining representation). In more detail:
gμ1μ2=Sμ1ν1 Sμ2ν2 gν1ν2 ,
with a similar one for the other tensor.
The E7 description is described in P. Cvitanovic's [Group Theory][1] book. You can take a look there for the supersymmetric groups for which he has an interesting approach.
[1]: http://www.nbi.dk/GroupTheory/
This post imported from StackExchange Physics at 2014-09-07 07:31 (UCT), posted by SE-user suresh