In this article, we prove some results concerning the truncated two-point function of the infinite-range Ising model above and below the critical temperature. More precisely, if the coupling constants are of the form $$J_{x}=\psi (x)\textsf{e}^{-\rho (x)}$$
J
x
=
ψ
(
x
)
e
-
ρ
(
x
)
with $$\rho $$
ρ
some norm and $$\psi $$
ψ
an subexponential correction, we show under appropriate assumptions that given $$s\in \mathbb {S}^{d-1}$$
s
∈
S
d
-
1
, the Laplace transform of the two-point function in the direction s is infinite for $$\beta =\beta _\textrm{sat}(s)$$
β
=
β
sat
(
s
)
(where $$\beta _\textrm{sat}(s)$$
β
sat
(
s
)
is a the biggest value such that the inverse correlation length $$\nu _{\beta }(s)$$
ν
β
(
s
)
associated to the truncated two-point function is equal to $$\rho (s)$$
ρ
(
s
)
on $$[0,\beta _\textrm{sat}(s)))$$
[
0
,
β
sat
(
s
)
)
)
. Moreover, we prove that the two-point function satisfies up-to-constants Ornstein-Zernike asymptotics for $$\beta =\beta _\textrm{sat}(s)$$
β
=
β
sat
(
s
)
on $$\mathbb {Z}$$
Z
. As far as we know, this constitutes the first result on the behaviour of the two-point function at $$\beta _\textrm{sat}(s)$$
β
sat
(
s
)
. Finally, we show that there exists $$\beta _{0}$$
β
0
such that for every $$\beta >\beta _{0}$$
β
>
β
0
, $$\nu _{\beta }(s)=\rho (s)$$
ν
β
(
s
)
=
ρ
(
s
)
. All the results are new and their proofs are built on different results and ideas developed in Duminil-Copin and Tassion (Commun Math Phys 359(2):821–822, 2018) and Aoun et al. in (Commun Math Phys 386:433–467, 2021).