Partial masslessness of higher spins in (A)dS

• Published in: Nuclear physics. B Vol. 607; no. 3; pp. 577 - 604
• Main Authors: Deser, S., Waldron, A.
• Format: Journal Article
• Language: English
• Published: Elsevier B.V 30-07-2001
• Subjects: 03.70.+k; 04.62.+v; 04.65.+e; 03.65.Pm
• ISSN: 0550-3213; 1873-1562
• DOI: 10.1016/S0550-3213(01)00212-7

Massive spin
s⩾3/2 fields can become partially massless in cosmological backgrounds. In the plane spanned by
m
2 and
Λ, there are lines where new gauge invariances permit intermediate sets of higher helicities, rather than the usual flat space extremes of all 2
s+1 massive or just 2 massless helicities. These gauge lines divide the (
m
2,
Λ) plane into unitarily allowed or forbidden intermediate regions where all 2
s+1 massive helicities propagate but lower helicity states can have negative norms. We derive these consequences for
s=3/2,2 by studying both their canonical (anti)commutators and the transmutation of massive constraints to partially massless Bianchi identities. For
s=2, a Hamiltonian analysis exhibits the absence of zero helicity modes in the partially massless sector. For
s=5/2,3 we derive Bianchi identities and their accompanying gauge invariances for the various partially massless theories with propagating helicities (±5/2,±3/2) and (±3,±2), (±3,±2,±1), respectively. Of these, only the
s=3 models are unitary. To these ends, we also provide the half integer generalization of the integer spin wave operators of Lichnerowicz. Partial masslessness applies to all higher spins in (A)dS as seen by their degree of freedom counts. Finally a derivation of massive
d=4 constraints by dimensional reduction from their
d=5 massless Bianchi identity ancestors is given.