Let G∕H be a
compactly causal symmetric space with causal compactification Φ : G∕H →Š1,
where Š1 is the Bergman-Šilov boundary of a tube type domain G1∕K1.
The Hardy space H2(C) of G∕H is the space of holomorphic functions on a
domain Ξ(Co) ⊂ Gℂ∕Hℂ with L2-boundary values on G∕H. We extend Φ
to imbed Ξ(Co) into G1∕K1, such that Ξ(Co) = {z ∈ G1∕K1∣ψm(z)≠0},
with ψm explicitly known. We use this to construct an isometry I of the
classical Hardy space Hcl on G1∕K1 into H2(C) or into a Hardy space H2(C)
defined on a covering Ξ(Co) of Ξ(Co). We describe the image of I in terms of
the highest weight modulus occuring in the decomposition of the Hardy
space.