Let Gn∗ be one of the split classical groups in the source, and let σ¬ be a negative representation of Gn∗(F). Suppose
Jord(σ¬)=Jord(σsn)∪(χi,ni),(χi−1,ni):1≤i≤t.
For Gn∗=Sp2n∗ or O2n∗, write
Jord(σsn)=(λ0,2n1+1),…,(λ0,2nk+1),(1GL1,2m1+1),…,(1GL1,2ml+1).
For Gn∗=SO2n∗+1, write instead
Jord(σsn)=(λ0,2n1),…,(λ0,2nk),(1GL1,2m1),…,(1GL1,2ml).
Maximal wave front partition conjecture. If Gn∗=Sp2n∗ or O2n∗, then
pm(σ¬)={ηgn∗∨,gn∗([(j=1∏tnj2)(i=1∏l(2mi+1)s=1∏k(2ns+1))])}.
If Gn∗=SO2n∗+1, then
pm(σ¬)={ηgn∗∨,gn∗([(j=1∏tnj2)(i=1∏l(2mi)s=1∏k(2ns))])}.
Here ηgn∗∨,gn∗ is the duality map between partitions for the dual and original classical Lie algebras, and [⋅] denotes the partition notation used in the source. This conjecture predicts the unique maximal wave front partition of a negative representation from its Jordan data; its status is not resolved in the supplied source.