An article of the relevant literature Heliocentric Escape and Lunar Impact from Near Rectilinear Halo Orbits asserts: "As the spacecraft departs the immediate vicinity of the NRHO, the effects of the Sun become significant." (See block quote below).
I ask: why are those effects less significant in the NRHO vicinity, so that they can be treated just like a perturbation in the context of the CR3BP? If I calculated correctly, the Sun gravity acting on a spacecraft in the NRHO is stronger than the gravity pull of Earth on the same spacecraft.
Maybe the fact that the Earth-Moon-spacecraft system is in revolution around the Sun "generates" a centrifugal force that in part contrast the Sun gravity… I am trying to gain an intuitive physical understanding of the matter and I hope you can offer me some insights because I couldn't find them anywhere else.
edit: I quoted the article to better convey a doubt originated before reading the article itself. I try now to provide another formulation to my question to be more clear. Nasa chose the NRHO as an optimal solution for the orbit of the Gateway also because it requires low maintenance (it is fuel efficient; https://www.nasa.gov/missions/artemis/lunar-near-rectilinear-halo-orbit-gateway/). This means that the NRHO, which is a solution of the CR3BP of the Moon-Earth-System, is not heavily disrupted when considered in the context of a more realistic dynamics. I wonder how this can be the case just considering the influence of the Sun.
DYNAMICAL MODELS
In this investigation, three dynamical models are employed. The CR3BP5 provides a framework for investigation of departure dynamics and flow nearby the NRHO before and immediately after separation from the Gateway. In this regime, the primary gravitational influences on the spacecraft are the Earth and Moon, and the CR3BP is an effective approximation for the dynamics. As the spacecraft departs the immediate vicinity of the NRHO, the effects of the Sun become significant. Thus, the BCR4BP6 is employed to characterize the behavior of the departing spacecraft. The BCR4BP incorporates the influence of solar gravity on the Earth-Moon-spacecraft three-body system and offers an increase in fidelity over the CR3BP, while still offering insight into the underlying dynamical behavior in the system. Finally, an N-body model based on ephemeris data provides higher-fidelity analysis for particular mission scenarios.
5(CR3BP = circular restricted three body problem) Szebehely, Z., Theory of Orbits: The Restricted Problem of Three Bodies, Academic Press, New York, 1967.
6(BCR4BP = bi-circular restricted four body problem) Gomez, G., J. Llibre, R. Martinez, and C. Simo, Dynamics and Mission Design near Libration Points, Vol. 2. World Scientific, 2001.