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GS formalism

From Wikipedia, the free encyclopedia

Green–Schwarz (GS) formalism (named after Michael Green and John H. Schwarz)[1][2][3] is an attempt to introduce fermions in string theory. The theory is equivalent to RNS formalism which has been GSO projected. This theory is very hard to quantize, being straightforward to quantize only in light cone gauge.[4] A covariant quantization of spinning string, maintaining space-time supersymmetry manifest, is possible in a formalism inspired on the GS formalism, known as pure spinor formalism.[5]

See also

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Notes

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  1. ^ M. B. Green, J. H. Schwarz, J. H., "Supersymmetrical Dual String Theory," Nucl. Phys. B181 (1981), 502–530.
  2. ^ M. B. Green, J. H. Schwarz, J. H., "Supersymmetrical Dual String Theory (II): Vertices and Trees," Nucl. Phys. B198 (1982), 252–268.
  3. ^ M. B. Green, J. H. Schwarz, J. H., "Supersymmetrical Dual String Theory (III): Loops and Renormalization," Nucl. Phys. B198 (1982), 441–460.
  4. ^ Green, Michael B., and John H. Schwarz. "Covariant description of superstrings." Dynamical Groups and Spectrum Generating Algebras: (In 2 Volumes). 1988. 885-888.
  5. ^ N. Bekovits, "Super-Poincaré covariant quantization of the superstring." Journal of High Energy Physics 2000.04 (2000): 018.