paper

How Many Strings Exist ?

arXiv:hep-th/9409020 · doi:10.1088/0264-9381/12/4/004

Abstract

Possible ways of constructing extended fermionic strings with world-sheet supersymmetry are reviewed. String theory constraints form, in general, a non-linear quasi(super)conformal algebra, and can have conformal dimensions . When , the most general quasi-superconformal algebra to consider for string theory building is $\hat{D}(1,2;\a)$, whose linearisation is the so-called `large' superconformal algebra. The $\hat{D}(1,2;\a)$ algebra has $\Hat{su(2)}_{k^+}\oplus \Hat{su(2)}_{k^-}\oplus\Hat{u(1)}$ Kač-Moody component, and $\a=k^-/k^+$. We check the Jacobi identities and construct a BRST charge for the $\hat{D}(1,2;\a)$ algebra. The quantum BRST operator can be made nilpotent only when . The algebra is actually isomorphic to the -based Bershadsky-Knizhnik non-linear quasi-superconformal algebra. We argue about the existence of a string theory associated with the latter, and propose the (non-covariant) hamiltonian action for this new string theory. Our results imply the existence of two different fermionic string theories: the old one based on the `small' linear superconformal algebra and having the total ghost central charge , and the new one with non-linearly realised supersymmetry, based on the quasi-superconformal algebra and having . Both critical string theories have negative `critical dimensions' and do not admit unitary matter representations.

31 pages, LaTeX, Hannover preprint ITP-UH-13/94, September 1994

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