Definition

Let (M4n,Q)(M^{4n},Q) be a . Its twistor space is the

π:Z=S(Q)M\pi:Z=S(Q)\longrightarrow M

whose fiber at xx is

Zx={AQx:A2=idTxM}.Z_x=\{A\in Q_x:A^2=-\operatorname{id}_{T_xM}\}.

The quaternionic algebra gives QQ a canonical Euclidean metric and orientation, so ZxZ_x is a two-sphere: after choosing a local admissible frame (I,J,K)(I,J,K), its points are aI+bJ+cKaI+bJ+cK with a2+b2+c2=1a^2+b^2+c^2=1. Although this description uses a frame, the bundle ZZ does not. Each point of ZZ records one complex structure compatible with QQ at its base point.

Canonical almost-complex structure

A quaternionic connection splits TZTZ into horizontal and vertical parts. On a horizontal vector over (x,A)(x,A), use AA; on the of ZxCP1Z_x\cong\mathbb{CP}^1, use its standard complex structure. These pieces define an on ZZ. For n2n\geq2, it is independent of the chosen torsion-free quaternionic connection and is integrable; this is the central twistor theorem in Salamon, §§3–4.

Examples and interpretation

The twistor space of quaternionic projective space HPn\mathbb H P^n is CP2n+1\mathbb{CP}^{2n+1}, with the projection arising from the inclusion of a complex line in the quaternionic line that it spans. For a , the global triple trivializes QQ, so ZZ is smoothly M×S2M\times S^2; its canonical complex structure nevertheless mixes the two factors and is not generally the product complex structure.

The twistor space packages the rotating local complex structures of quaternionic geometry into one . It should not be confused with the unit : its sphere fibers lie in QEnd(TM)Q\subseteq\operatorname{End}(TM), not in TMTM.

References
  1. Simon Salamon, “Quaternionic Kähler Manifolds,” Inventiones Mathematicae 67 (1982), 143–171. DOI record. Relevant: §§3–4, the twistor bundle and its integrable complex structure.