4-DIMENSIONAL STRING STRING STRING TRIALITY

In six space-time dimensions, the heterotic string is dual to a Type I IA string. On further toroidal compactification to four space-time dim ensions, the heterotic string acquires an SL(2, Z)(S) strong/weak coup ling duality and an SL(2,Z)(T) x SL(2,Z)(U) target space duality actin g on the dilaton/axion, complex Kahler form and the complex structure fields S, T, U respectively. Strong/weak duality in D = 6 interchanges the roles of S and T in D = 4 yielding a Type IIA string with fields T, S, U. This suggests the existence of a third string (whose six-dime nsional interpretation is more obscure) that interchanges the roles of S and U. It corresponds in fact to a Type IIB string with fields U, T , S leading to a four-dimensional string/string/string triality. Since SL(2, Z)(S) is perturbative for the Type IIB string, this D = 4 trial ity implies S-duality for the heterotic string and thus fills a gap le ft by D = 6 duality. For all three strings the total symmetry is SL(2, Z)(S) x O(6, 22; Z)(TU). The O(6, 22; Z) is perturbative for the hete rotic string but contains the conjectured non-perturbative SL(2, Z)(X) , where X is the complex scalar of the D = 10 Type IIB string. Thus fo ur-dimensional triality also provides a (post-compactification) justif ication for this conjecture. We interpret the N = 4 Bogomol'nyi spectr um from all three points of view. In particular we generalize the Sen- Schwarz formula for short multiplets to include intermediate multiplet s also and discuss the corresponding black hole spectrum both for the N = 4 theory and for a truncated S-T-U symmetric N = 2 theory. Just as the first two strings are described by the four-dimensional elementar y and dual solitonic solutions, so the third string is described by th e stringy cosmic string solution. In three dimensions all three string s are related by O(8,24;Z) transformations.