Non-critical string theory

Current Science

Volumn 81, Issue 12, 2001, Pages 1598-1608

  Dhar, Avinash ^a  

^a TATA INSTITUTE OF FUNDAMENTAL RESEARCH   (India)

Author keywords

[No Author keywords available]

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EID: 0442280443     PISSN: 00113891     EISSN: None     Source Type: Journal    
DOI: None     Document Type: Article

References (11)

1. That the liouville mode plays the role of an extra dimension in the target space was first discussed by Das, S. R., Naik, S. and Wadia, S. R., Mod. Phys. Lett., 1989, A4, 1033. Its role as an RG scale was first explained by Das, S. R., Dhar, A. and Wadia, S. R., Mod. Phys. Lett., 1990, A5, 799 and further discussed by Dhar, A. and Wadia, S. R., Nucl. Phys., 2000, B590, 261.
2. That the liouville mode plays the role of an extra dimension in the target space was first discussed by Das, S. R., Naik, S. and Wadia, S. R., Mod. Phys. Lett., 1989, A4, 1033. Its role as an RG scale was first explained by Das, S. R., Dhar, A. and Wadia, S. R., Mod. Phys. Lett., 1990, A5, 799 and further discussed by Dhar, A. and Wadia, S. R., Nucl. Phys., 2000, B590, 261.
3. That the liouville mode plays the role of an extra dimension in the target space was first discussed by Das, S. R., Naik, S. and Wadia, S. R., Mod. Phys. Lett., 1989, A4, 1033. Its role as an RG scale was first explained by Das, S. R., Dhar, A. and Wadia, S. R., Mod. Phys. Lett., 1990, A5, 799 and further discussed by Dhar, A. and Wadia, S. R., Nucl. Phys., 2000, B590, 261.
4. The physical phenomenon underlying this modern technical term is elucidated by the example given below, which was first discussed in Das, S. R., Dhar, A. and Wadia, S. R., Mod. Phys. Lett., 1990, A5, 799.
5. This solution was discovered by Mandal, G., Sengupta, A. and Wadia, S. R., Mod. Phys. Lett., 1991, A6, 1685 and Witten, E., Phys. Rev., 1991, D44, 314.
6. This solution was discovered by Mandal, G., Sengupta, A. and Wadia, S. R., Mod. Phys. Lett., 1991, A6, 1685 and Witten, E., Phys. Rev., 1991, D44, 314.
7. In the non-perturbative formalism, this was discovered by Avan, J. and Jevicki, A., Phys. Lett., 1991, B266, 35; Moore, G. and Seiberg, N., Int. J. Mod. Phys., 1992, A7, 2601; Das, S. R., Dhar, A., Mandal, G. and Wadia, S. R., Int. J. Mod. Phys., 1992, A7, 5165; Minic, D., Polchinski, J. and Yang, Z., Nucl. Phys., 1992, B369, 324.
8. In the non-perturbative formalism, this was discovered by Avan, J. and Jevicki, A., Phys. Lett., 1991, B266, 35; Moore, G. and Seiberg, N., Int. J. Mod. Phys., 1992, A7, 2601; Das, S. R., Dhar, A., Mandal, G. and Wadia, S. R., Int. J. Mod. Phys., 1992, A7, 5165; Minic, D., Polchinski, J. and Yang, Z., Nucl. Phys., 1992, B369, 324.
9. In the non-perturbative formalism, this was discovered by Avan, J. and Jevicki, A., Phys. Lett., 1991, B266, 35; Moore, G. and Seiberg, N., Int. J. Mod. Phys., 1992, A7, 2601; Das, S. R., Dhar, A., Mandal, G. and Wadia, S. R., Int. J. Mod. Phys., 1992, A7, 5165; Minic, D., Polchinski, J. and Yang, Z., Nucl. Phys., 1992, B369, 324.
10. In the non-perturbative formalism, this was discovered by Avan, J. and Jevicki, A., Phys. Lett., 1991, B266, 35; Moore, G. and Seiberg, N., Int. J. Mod. Phys., 1992, A7, 2601; Das, S. R., Dhar, A., Mandal, G. and Wadia, S. R., Int. J. Mod. Phys., 1992, A7, 5165; Minic, D., Polchinski, J. and Yang, Z., Nucl. Phys., 1992, B369, 324.
11. This work by Dhar, A., Mandal, G. and Wadia, S. R., Mod. Phys. Lett., 1992, A7, 3129 is the earliest known example of a string field theory based on an underlying non-commutative space, in this case the quantum phase space of a single fermion.