Definition
Conjugate and contragredient unitary representations
The conjugate action on the conjugate Hilbert space and the corresponding dual action on continuous linear functionals.
Definition
Let be a strongly continuous unitary representation of a group . Its conjugate representation acts on the conjugate Hilbert space by
Its contragredient representation acts on the continuous linear dual by
Both actions are strongly continuous and unitary for their natural Hilbert structures. They are canonically unitarily equivalent through the Riesz map , with the inner product taken linear in the first variable.
Coefficients
For , the matrix coefficients of the conjugate representation satisfy
Under the Riesz identification, the contragredient action sends the functional represented by to the functional represented by . This calculation is the reason the inverse occurs in the dual-action formula.
Relationship to equivalence
The representation is self-conjugate when it is unitarily equivalent to . This condition does not by itself decide whether a compatible real or quaternionic structure exists; those finer alternatives require an antiunitary intertwiner and a condition on its square. Conjugation also reverses scalar phases, which is important even when and act on Hilbert spaces of the same dimension.
Conventions and scope
For a general Banach-space representation, the dual action naturally lives on the Banach dual and need not share the Hilbert-space properties used above. In finite-dimensional algebra, “contragredient” is often written using inverse transpose matrices. The Riesz identification is conjugate-linear on but becomes linear when its source is Folland, §3.1.
References
- G. B. Folland, A Course in Abstract Harmonic Analysis, 2nd ed., CRC Press, 2016. DOI record. Relevant: §3.1 on unitary representations and their conjugates.