Twistor theory

In theoretical and mathematical physics, twistor theory maps the geometric objects of conventional 3+1 space-time (Minkowski space) into geometric objects in a 4-dimensional space with a Hermitian form of signature (2,2). This space is called twistor space, and its complex valued coordinates are called "twistors."

Twistor theory was first proposed by Roger Penrose in 1967,[1] as a possible path to a theory of quantum gravity. The twistor approach is especially natural for solving the equations of motion of massless fields of arbitrary spin.

In 2003, Edward Witten[2] proposed uniting twistor and string theory by embedding the topological B model of string theory in twistor space. His objective was to model certain Yang–Mills amplitudes. The resulting model has come to be known as twistor string theory (read below). Simone Speziale and collaborators have also applied it to loop quantum gravity.[3]

Details

Penrose's original version of twistor theory is uniquely adapted to four-dimensional Minkowski space, with its signature (3,1) metric (although some of the most profound work in pure mathematics growing out of these ideas has actually occurred in other signatures, and even in other dimensions). At the heart of twistor theory lies the isomorphism between the conformal group Spin(4,2) and SU(2,2), which is the group of unitary transformations of determinant 1 over a four-dimensional complex vector space that leave invariant a Hermitian form of signature (2,2), see classical group.

, , and are all homogeneous spaces of the conformal group.

admits a conformal metric (i.e., an equivalence class of metric tensors under Weyl rescalings) with signature (+++−). Straight null rays map to straight null rays under a conformal transformation and there is a unique canonical isomorphism between null rays in and points in respecting the conformal group.

In , it is the case that positive and negative frequency solutions cannot be locally separated. However, this is possible in twistor space.

Twistor string theory

Main article: Twistor string theory

For many years after Penrose's foundational 1967 paper, twistor theory progressed slowly, in part because of mathematical challenges. Twistor theory also seemed unrelated to ideas in mainstream physics. While twistor theory appeared to say something about quantum gravity, its potential contributions to understanding the other fundamental interactions and particle physics were less obvious.

Witten (2003) proposed a connection between string theory and twistor geometry, called twistor string theory. Witten (2004)[2] built on this insight to propose a way to do string theory in twistor space, whose dimensionality is necessarily the same as that of 3+1 Minkowski spacetime. Although Witten has said that "I think twistor string theory is something that only partly works," his work has given new life to the twistor research program. For example, twistor string theory may simplify calculating scattering amplitudes from Feynman diagrams by using a geometric structure called an amplituhedron.

Supertwistors

Witten's twistor string theory is defined on the supertwistor space . Supertwistors are a supersymmetric extension of twistors introduced by Alan Ferber in 1978.[4] Along with the standard twistor degrees of freedom, a supertwistor contains N fermionic scalars, where N is the number of supersymmetries. The superconformal algebra can be realized on supertwistor space.

See also

Notes

  1. Penrose, R. (1967). "Twistor Algebra". Journal of Mathematical Physics. 8 (2): 345. Bibcode:1967JMP.....8..345P. doi:10.1063/1.1705200.
  2. 1 2 Witten, Edward (7 October 2004). "Perturbative Gauge Theory as a String Theory in Twistor Space". Communications in Mathematical Physics. 252 (1-3): 189–258. arXiv:hep-th/0312171Freely accessible. Bibcode:2004CMaPh.252..189W. doi:10.1007/s00220-004-1187-3.
  3. Freidel, Laurent; Speziale, Simone (25 October 2010). "Twistors to twisted geometries". Physical Review D. 82 (8). arXiv:1006.0199Freely accessible. Bibcode:2010PhRvD..82h4041F. doi:10.1103/PhysRevD.82.084041.
  4. Ferber, A (1978), "Supertwistors and conformal supersymmetry", Nuclear Physics B, 132: 55–64, Bibcode:1978NuPhB.132...55F, doi:10.1016/0550-3213(78)90257-2.

Further reading

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