Parallax would be the first thing to break the hoax
In our universe, "nearby" stars appear to move across the sky as compared to distant stars due to parallax and the motion of the Earth around the Sun. The effect is subtle and wasn't observed until the late 1800 to early 1900s. Using something called a filar micrometer (seen below) to make accurate angular measurements.
While the 'experimenters could simulate the annual parallax of stars, if the inhabitants of your solar system achieve technology comparable to the early 1900s, they could stumble upon the daily parallax. The daily parallax of the rotation of the Earth couldn't be simulated for everyone on Earth like the annual parallax could. For instance:
Consider an astronomer at location A on the Earth. For the hoaxers to simulate the location of a fake star over a single night, the image on the display would need to move from A' to B' as the Earth rotates the astronomer from A to B. However, a second astronomer on the opposite side of the Earth would measure the star in a different position due it's nefarious displacement across the screen. The displacement (denoted $\theta_H$) could be measured relative to a known object, (Jupiter, for instance). When the two astronomers meet up later and compare their observations, they would know something is wrong.
Appendix: Calculating the daily parallax
The current state-of-art parallax measurements have angular resolutions of around 1 milli-arcsecond (see the Hubble Telescope). The resolution of of the filar micrometers of the 1920-1930s astrometry would have been around 10 milli-arcseconds. To calculate the parallax your screen incurs, let $R$ be the radius of the Earth, $H$ the distance to the hologram (screen), and $S$ the simulated distance to the fake star.
The parallax angle the fake star creates across the diameter of the Earth is:
$$ \theta_S = \frac{2R}{S} $$
And the distance the image of the star must move across the screen (called $D$) is:
$$ D = (S - H)\theta_S = \frac{(S - H)2R}{S} = (1 - \frac{H}{S})2R $$
We see if $S$, the simulated distance to the star, is large, then $D\approx2R$; the image moves across the screen exactly the width of Earth. This is the worst-case scenario for the hoaxers.
And lastly, the parallax produced by the motion of the image on the screen will be:
$$ \theta_H = \frac{D}{H} = ( \frac{1}{H} - \frac{1}{S} ) 2R $$
$$ \theta_H \approx \frac{2R}{H}$$
For Earth, $R=6.73\times10^6$ meters. If we take your experimenter's screen to be 3-lightdays away, then $H=7.77\times10^{13}$ meters, then:
$$ \theta_H = \frac{2 6.73\times10^6}{7.77\times10^{13}}\frac{180^\circ \cdot 3600 \cdot 1000}{\pi} = 36 \text{milli-arcseconds}$$
Which is large enough to notice with 1900s technology. Note that Jupiter only moves around 7 milli-arcseconds a night.