= Solution
For
$$
f(k,\eta)=\frac{H\eta}{\sqrt{2k}}e^{-ik\eta},
$$
the specified <cosmological bulk-to-boundary propagator> is
$$
\boxed{G_R(\eta,p)=f(p,\eta_0)f^*(p,\eta)
=\frac{H^2\eta_0\eta}{2p}e^{-ip(\eta_0-\eta)}}.
$$
The right-right <cosmological bulk-to-bulk propagator> is time ordered:
$$
\boxed{G_{RR}(\eta_1,\eta_2,p)
=\frac{H^2\eta_1\eta_2}{2p}
e^{-ip|\eta_1-\eta_2|}}.
$$
The mixed <Wightman function> in the order stated in the question is
$$
\boxed{G_{LR}(\eta_1,\eta_2,p)
=f(p,\eta_1)f^*(p,\eta_2)
=\frac{H^2\eta_1\eta_2}{2p}
e^{-ip(\eta_1-\eta_2)}}.
$$
The suppressed factor in each expression is $(2\pi)^3\delta^{(3)}(\mathbf p+\mathbf p')$.
Back to article page
