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| The twistor approach appears to be especially natural for solving the equations of motion of ] of arbitrary ]. | The twistor approach appears to be especially natural for solving the equations of motion of ] of arbitrary ]. | ||
| Recently, ] used twistor theory to understand certain ] ], by relating them to a certain ], the ] B model, embedded in twistor space. This field has come to be known as |
Recently, ] used twistor theory to understand certain ] ], by relating them to a certain ], the ] B model, embedded in twistor space. This field has come to be known as ]. | ||
| ==See also== | ==See also== | ||
Revision as of 10:01, 19 June 2006
The twistor theory, originally developed by Roger Penrose in 1967, is the mathematical theory which maps the geometric objects of the four dimensional space-time (Minkowski space) into the geometric objects in the 4-dimensional complex space with the metric signature (2,2).
The coordinates in such a space are called twistors.
For some time there was hope that the twistor theory may be the right approach towards solving quantum gravity, but this is now considered unlikely.
The twistor approach appears to be especially natural for solving the equations of motion of massless fields of arbitrary spin.
Recently, Edward Witten used twistor theory to understand certain Yang-Mills amplitudes, by relating them to a certain string theory, the topological B model, embedded in twistor space. This field has come to be known as twistor string theory.
See also
External links
- Twistor Theory and the Twistor Programme
- MathWorld - Twistors
- Roger Penrose - On the Origins of Twistor Theory
- Roger Penrose - The Central Programme of Twistor Theory
- Richard Jozsa - Applications of Sheaf Cohomology in Twistor Theory
- Fedja Hadrovich - Twistor primer