Twistors and Wick Rotation

Key Takeaways

• Twistor space encodes spacetime points as CP^1 lines.
• Minkowski ↔ Euclidean rotation uses SU(2,2) and SL(2,H).
• Penrose transform links massless fields to holomorphic bundles.
• SU(1,1) action on CP^1 yields discrete series representations.
• Fibered CP^3 over S^4 gives Euclidean conformal compactification.

Pulse Analysis

Twistor theory reshapes the traditional view of Wick rotation by embedding four‑dimensional spacetime into a six‑dimensional complex projective space. In this setting, a point of Minkowski space corresponds to a CP^1 line inside PT=CP^3, while the Euclidean counterpart emerges from a different real form of the complex spin group, SL(2,ℍ). This geometric shift eliminates the need to analytically continue Weyl spinors, replacing them with Dirac spinors that naturally accommodate both chiralities during the rotation. The result is a cleaner, group‑theoretic pathway between Lorentzian and Euclidean signatures.

The conformal groups play a central role: SU(2,2) governs Minkowski spacetime, acting with three orbits—PT⁺, PT⁻, and their common boundary N—while SL(2,ℍ) (the Euclidean conformal group) acts transitively on PT, fibering it over S⁴. This fiber structure identifies each Euclidean point with a CP^1 fiber, turning the Wick‑rotated space into a compactified Euclidean manifold. The boundary N, topologically S³×S², becomes a bundle of S² fibers over an S³ slice where the two signatures intersect, offering a concrete geometric picture of analytic continuation.

Beyond pure mathematics, these insights have practical implications for quantum field theory and scattering amplitude calculations. The Penrose transform maps solutions of massless wave equations in Minkowski space to cohomology classes of holomorphic line bundles on PT⁺ or PT⁻, providing a powerful tool for constructing conformally invariant amplitudes. By leveraging the twistor framework, physicists can exploit holomorphic techniques and representation theory—such as discrete series of SU(1,1)—to streamline perturbative computations and explore new dualities between Lorentzian and Euclidean regimes. This approach promises more efficient analytic methods and deeper conceptual links across high‑energy physics.