How Many N=4N=4 Strings Exist ?

preprint1994arXivOpen access

Abstract

Possible ways of constructing extended fermionic strings with N=4N=4 world-sheet supersymmetry are reviewed. String theory constraints form, in general, a non-linear quasi(super)conformal algebra, and can have conformal dimensions ≥1\geq 1. When N=4N=4, the most general N=4N=4 quasi-superconformal algebra to consider for string theory building is $\hat{D}(1,2;\a)$, whose linearisation is the so-called `large' N=4N=4 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 k+=k−=−2k^+=k^-=-2. The D^(1,2;1)\hat{D}(1,2;1) algebra is actually isomorphic to the SO(4)SO(4)-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 N=4N=4 string theory. Our results imply the existence of two different N=4N=4 fermionic string theories: the old one based on the `small' linear N=4N=4 superconformal algebra and having the total ghost central charge cgh=+12c_{\rm gh}=+12, and the new one with non-linearly realised N=4N=4 supersymmetry, based on the SO(4)SO(4) quasi-superconformal algebra and having cgh=+6c_{\rm gh}=+6. Both critical string theories have negative `critical dimensions' and do not admit unitary matter representations.

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