1991
DOI: 10.1016/0550-3213(91)90148-q
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Extrinsic geometry of strings and W-gravities

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Cited by 31 publications
(14 citation statements)
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“…Further argument with currents and a gauge fixing leaves T zz unfixed and the condition h √ g = 1 (or any constant) then singles out a certain class of surfaces (cf. also [46,47] where light cone gauge is used). In the conformal gauge √ g = exp(ξ) where ξ is the Liouville mode.…”
Section: Conformal Immersionsmentioning
confidence: 99%
“…Further argument with currents and a gauge fixing leaves T zz unfixed and the condition h √ g = 1 (or any constant) then singles out a certain class of surfaces (cf. also [46,47] where light cone gauge is used). In the conformal gauge √ g = exp(ξ) where ξ is the Liouville mode.…”
Section: Conformal Immersionsmentioning
confidence: 99%
“…A simple way to see why one has doubling of the Virasaro algebra in R 4 is to observe that G 2,4 ≃ CP 1 ⊗ CP 1 , while G 2,3 ≃ CP 1 . For surfaces immersed in R n (n > 4) not much is known although it is expected that one would find W-gravities in certain type of surfaces [6].…”
Section: Introductionmentioning
confidence: 99%
“…One can find an appropriate``gauge transformation'' that maps the DS gauge in a gauge where all W s are primary fields (see [25,Sect. 4] for the A 3 -case).…”
Section: N+1 -Algebrasmentioning
confidence: 99%