Problem statement
Given the probability density $$ p(s,t|a,b,c) = \cases{Z(a,b,c)^{-1} \exp(-as-bt-cst) &if $s \geq 1$ and $t \geq 1$ \\ 0 &otherwise} \label{1} \tag{1}$$ where $$ \begin{align} Z(a,b,c) &\equiv \int \int \exp(-as-bt-cst) \ ds \ dt = \frac{1}{c} \exp\Big(\frac{ab}{c}\Big) \Gamma\Big(0,\frac{(a+c)(b+c)}{c}\Big) \\ \Gamma(0,x) &= \int_x^\infty \exp(-t) \frac{dt}{t} \end{align} $$ and $(a,b,c)$ are "admissible" such that $Z(a,b,c)$ exists, i.e., $$ c > 0, \quad a + c > 0, \quad b + c > 0.$$
Prove (or disprove) that for any such admissible $(a,b,c)$: $$ \langle st \rangle \leq \langle s \rangle \langle t \rangle. \label{2} \tag{2}$$ In other words, the random variates $(s,t)$ must be negatively correlated.
Comments
Lower bound on $\langle st \rangle$
For all $(s,t)$ in the support of \eqref{1} we have $1 \leq (s,t) \leq st$. So $1 \leq \max(\langle s \rangle, \langle t \rangle) \leq \langle st \rangle$.
The case $c=0$
If $c=0$ the random variates $(s,t)$ are independent and thus uncorrelated, such that \eqref{2} reduces to $\langle st \rangle = \langle s \rangle \langle t \rangle.$
Background
Given the constraints: $$ 1 \leq (s,t) < L, \quad \langle s \rangle = S, \quad \langle t \rangle = T, \quad \langle st \rangle = U $$ the density \eqref{1} is the maximum entropy distribution with respect to Lebesgue measure for $L \rightarrow \infty$ where $(a,b,c)$ are admissible Lagrange multipliers which solve the simultaneous equations: $$ -\nabla_{a,b,c} \log Z \equiv (\langle s \rangle, \langle t \rangle, \langle st \rangle) = (S,T,U). \label{3} \tag{3}$$ Thus by construction \eqref{1} is in the exponential family.
I implemented a numerical solver that finds admissible $(a,b,c)$ for given $(S,T,U)$ but it fails badly when $U$ is moderately larger than $ST$: it drives $c \rightarrow 0$ but cannot accurately satisfy \eqref{3}. Further numerical investigation led me to believe (95% sure) that \eqref{3} can only be solved when $U \leq ST$, but after much effort I could not prove this.
I tried several approaches to prove \eqref{2} (e.g. directly attacking \eqref{2}; bounding $\langle st \rangle$ with the moment generating function of \eqref{1}) but the only noteworthy result I could get is the following:
For $c \approx 0$, the solution to \eqref{3} is roughly: $$ a = \frac{1}{S-1}, \quad b = \frac{1}{T-1}, \quad c = -\frac{U - ST}{S^2(T-1)^2 + T^2(S-1)^2 + (S-1)^2 (T-1)^2}. $$ This can be obtained by a first-order expansion of \eqref{3} at $c = 0$ and solving for $(a,b,c)$. Since $c > 0$, we must have that $U < ST$, such that \eqref{2} holds.
I'm unsure what the significance of this result in relation to proving \eqref{2} might be.