Definition

Let GG be a and HH a complex . Write

PU(H)=U(H)/{λI:λ=1},PU(H)=U(H)/\{\lambda I:|\lambda|=1\},

with the quotient of the on U(H)U(H). A projective unitary representation is a continuous

π:GPU(H).\overline\pi:G\longrightarrow PU(H).

Thus each gg acts by a determined only up to a scalar phase, while multiplication is exact after passing to projective classes. Equivalently, it is an action of GG on the rays of HH induced by unitaries; it need not admit a globally continuous choice of unitary representatives.

Multipliers

If representatives UgU(H)U_g\in U(H) can be chosen, then

UgUh=σ(g,h)UghU_gU_h=\sigma(g,h)U_{gh}

for phases σ(g,h)T\sigma(g,h)\in\mathbb T. Associativity gives the cocycle identity

σ(g,h)σ(gh,k)=σ(h,k)σ(g,hk).\sigma(g,h)\sigma(gh,k)=\sigma(h,k)\sigma(g,hk).

Changing representatives by Ugb(g)UgU_g\mapsto b(g)U_g changes σ\sigma by a coboundary. The resulting cohomology class records the obstruction to replacing the projective representation by a genuine one.

Lifts and central extensions

In a category where the chosen multiplier is continuous or Borel as required, the projective representation lifts to a genuine unitary representation of GG exactly when its multiplier class is trivial. Even when it does not lift on GG, it gives a genuine representation of the associated by T\mathbb T. Global lifts and continuous representatives require hypotheses beyond the bare quotient-valued definition Varadarajan, Chapter VIII.

Example

The spin-12\tfrac12 representation of SU(2)SU(2) does not descend to an ordinary representation of SO(3)=SU(2)/{±I}SO(3)=SU(2)/\{\pm I\}, because the nontrivial central element acts as I-I. After quotienting operators by phases, it does descend to a projective unitary representation of SO(3)SO(3).

References
  1. V. S. Varadarajan, Geometry of Quantum Theory, 2nd ed., Springer, 1985. DOI record. Relevant: Chapter VIII, “Multipliers.”
  2. V. Bargmann, “On Unitary Ray Representations of Continuous Groups,” Annals of Mathematics 59 (1954), 1–46. DOI record. Relevant: multipliers, ray representations, and lifting.