I have had my Canon EOS R full-frame mirrorless camera for a few weeks now, long enough to do a whole batch of technical testing. So it's time for a review.
This is very much a technical review, so rather than describing the handling of the camera and its various features (which can all be found elsewhere) I am more concerned about the technical characteristics that will affect long exposure astrophotography. In many cases I will be comparing it to the Nikon Z6 which I also own and which has a recent Sony sensor.
This will be a fast ride, full of information, so strap yourself in and let's begin!
Introductory Comments
All my tests were done using a telescope or a (legacy) non-CPU lens. Since the lens (and telescope) is unrecognised by the camera firmware this means it is unable to make any hardcoded corrections.
For all tests, noise reduction, lens corrections and dual pixel mode were all switched off in the camera menus.
On the subject of dual pixels, the Canon EOS R mirrorless shares the same sensor as the Canon 5D mark iv DSLR, where every pixel is a dual pixel.
Since Canon's EOS Ra astro-camera is essentially the same camera but with different internal filtering (to enhance H-alpha sensitivity) I would expect my analysis to apply equally well to the (discontinued) EOS Ra.
Read Noise Gain etc.
I don't intend to duplicate Bill Claff's excellent work at PhotonsToPhotos because I obtain very similar figures:
- Read noise: https://www.photonst...14,Nikon Z 6_14
- DxOMark Derived Characteristics: https://www.photonst...14,Nikon Z 6_14
Regarding the DxOMark Derived Characteristics, note that Bill says that fitting the DXO data has its limitations, affecting estimates of gain, read noise, QE etc.
The read noise has the typical Canon characteristic of being constant for 3 consecutive ISOs. I would therefore stick to the main ISO values i.e. 100, 200, 400, 800, 1600, 3200 etc. and avoid the intermediate ones.
It's worth pointing out that the bias level at ISO 100 and ISO 200 is 512 which is different from the bias of 2048 at higher ISOs.
It can be seen from the PhotonsToPhotos that the Canon EOS R read noise is noticeably higher than the typical Sony sensor at the ISOs most likely to be used for astrophotography i.e. ISO 800/1600. However, for long exposure RGB imaging the read noise is usually swamped by the noise of the background sky so read noise is not a concern. On the other hand, low read noise might be important if short exposures are being used or if narrowband filters are being used.
Dark Current and Camera Self-Heating
My methodology for testing dark current and self-heating is to put the camera in a dark room at 20C ambient temperature and leave it to acclimatise for an hour or two. I then switch the camera on and immediately run a couple of hours of consecutive 5 minute dark frames with the rear LCD folded out from the rear of the camera to allow heat dissipation. By subtracting each frame from the previous one, the thermal noise can be calculated and ultimately converted into dark current.
Here's the result for a few cameras, measured in electrons per pixel per second:
However, a lot of the difference is caused by the size of the pixels, so I find it's more meaningful to display the graph in terms of electrons per square micron per second:
It can be seen that the EOS R has low dark current and remarkably low self-heating during an extended session of long exposures. Remember also that during an actual imaging session the self-heating should be lower because the camera is thermally attached to a potentially heavy telescope and also the wind will be circulating the air around the camera body, both of which will have a cooling effect.
However any time spent in live view will potentially heat the sensor quite rapidly so live view should be kept to an absolute minimum to prevent any heat building up. Beware if you are controlling the camera from a laptop via USB because live view will be on continually. I therefore switch the tethered camera off unless actively focusing or framing the shot.
Edited by sharkmelley, 11 September 2021 - 04:55 PM.