(10) Combining these with eq.( 9), we get the constraints χ ∗ 1 =iχ2, χ∗ 2 =iχ1; χ2 = −iχ3, χ∗ 2 =iχ ∗ 3 ; χ ∗ 1 =χ3, χ∗ 3 =χ1

now gives (see appendix B) ˜χ1 = −iχ2, ˜χ2 =iχ1, χ2 = −iχ3, ˜χ2 =i ˜χ3, ˜χ1 = −χ3, ˜χ3 =χ1

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hep-th · 2019-08-21 · conditional · novelty 6.0

The authors construct the unique mass-deformed N=3 U(N) Chern-Simons-Matter action and express it in N=1 superspace.

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Mass-deformed $\mathcal{N} = 3$ Supersymmetric Chern-Simons-Matter Theory hep-th · 2019-08-21 · conditional · none · ref 6
The authors construct the unique mass-deformed N=3 U(N) Chern-Simons-Matter action and express it in N=1 superspace.