Powerful Laser Guide Star (LGS) systems are standard for the next-generation of extremely large telescopes. However, modern earth-based astronomy has gone through a process of concentration on few sites with exceptional sky quality, resulting in those becoming more and more crowded. The future LGS systems encounter hence an environment of surrounding astronomical installations, some of which observing with large fields-of-view. We derive formulae to calculate the impact of LGS light on the camera of a neighbouring telescope and the probabilities for a laser crossing the camera field-of-view to occur, and apply these to the specific case of the next very-high-energy gamma-ray observatory "Cherenkov Telescope Array" (CTA). Its southern part shall be constructed in a valley of the Cerro Armazones, Chile, close to the "Very Large Telescope" (VLT) and the "European Extremely Large Telescope" (ELT), while its northern part will be located at the "Observatorio del Roque de los Muchachos", on the Canary Island of La Palma, which also hosts the "Gran Telescopio de Canarias" (GTC) and serves as an optional site for the "Thirty Meter Telescope" (TMT), both employing LGS systems. Although finding the artificial star in the field-of-view of a CTA telescope will not disturb observations considerably, the laser beam crossing the field-of-view of a CTA telescope may be critical. We find no conflict expected for the ELT lasers, however, 1% (3%) of extra-galactic and 1% (5%) of galactic observations with the CTA may be affected by the GTC (TMT) LGS lasers, unless an enhanced version of a laser tracking control system gets implemented.creation of several guide stars is also possible, to achieve asterism with a radial distance from science target ranging from 0.5 to 6 on the sky. The LGS will likely be operated regularly during observations, and their scattered light (Rayleigh and Mie) will then be seen by other telescopes until distances of several kilometers from the location of their host observatory. Assuming the close-by installation observes in a wavelength range enclosing that of the LGS lasers, the scattered laser light may then leave spurious light tracks on the cameras and affect operation in several ways: a) by generating false triggers (for installations which trigger image readout e.g. from Cherenkov light pulses) the star guider camera and the precision pointing of the telescopes, and ultimately, d) by affecting the duty cycle, if active laser avoidance is chosen. Several of the enumerated problems can be often overcome with the use of Notch-filters (Schallenberg et al. 2010) or band-pass filters (Ahnen et al. 2017;Archambault et al. 2017), however this is not always possible at a reasonable cost, particularly not in the case of the CTA, where every camera pixel would need to be covered by such a filter. Light losses at smaller wavelengths, particularly in the sensitive region from 300 nm to 500 nm need to be strictly controlled in order to ensure that sensitivity losses remain acceptable, particularly around the energ...