In the planar circular restricted three-body problem and for any value of the mass parameter $$\mu \in (0,1)$$
μ
∈
(
0
,
1
)
and $$n\ge 1$$
n
≥
1
, we prove the existence of four families of n-ejection–collision (n-EC) orbits, that is, orbits where the particle ejects from a primary, reaches n maxima in the (Euclidean) distance with respect to it and finally collides with the primary. Such EC orbits have a value of the Jacobi constant of the form $$C=3\mu +Ln^{2/3}(1-\mu )^{2/3}$$
C
=
3
μ
+
L
n
2
/
3
(
1
-
μ
)
2
/
3
, where $$L>0$$
L
>
0
is big enough but independent of $$\mu $$
μ
and n. In order to prove this optimal result, we consider Levi-Civita’s transformation to regularize the collision with one primary and a perturbative approach using an ad hoc small parameter once a suitable scale in the configuration plane and time has previously been applied. This result improves a previous work where the existence of the n-EC orbits was stated when the mass parameter $$\mu >0$$
μ
>
0
was small enough. Moreover, for decreasing values of C, there appear some bifurcations which are first numerically investigated and afterward explicit expressions for the approximation of the bifurcation values of C are discussed. Finally, a detailed analysis of the existence of n-EC orbits when $$\mu \rightarrow 1$$
μ
→
1
is also described. In a natural way, Hill’s problem shows up. For this problem, we prove an analytical result on the existence of four families of n-EC orbits, and numerically, we describe them as well as the appearing bifurcations.