
Setting Gain and Offset for QHY Cameras
Gain Setting
For beginner, we recommend that you set the gain to “unity-gain”. Unit-gain is the gain when system gain is 1 (1e/ADU). This number is shown in the table below, like the unity-gain of QHY168C is 10. In fact, increasing or decreasing a bit doesn’t make a big difference.
You could increase or decrease Gain according to the condition. For example, if your optical system is fast, like F2.2 to F5, or long exposure for more than 5 minutes without narrowband filters, then you can decrease GAIN to achieve a higher dynamic range and make better use of full well capacity. By doing so you can avoid overexposure.
If you use narrowband filter on a slow optical system like F6 to F10, or short exposure time, the amount of photons received will be less. In this case you can increase GAIN to make better use of characteristics of low read-out noise in high GAIN value.
OFFSET Setting
There is no fixed “best value” for OFFSET. To set OFFSET, you should take the bias frame and dark frame at a certain GAIN value, then check the histogram of the frames.
As you can see, the histogram distribution is a peak-like curve. By changing the OFFSET value, this curve will move left or right. We must guarantee the range of the whole curve is greater than 0, and it cannot be chopped off at the end. At the same time, we need to keep a bit of residue on the left side, just over 0 a bit. 100 to couple hundreds ADU are all okay. Don’t be too huge, however.
Pay attention that under different GAIN values, the width of this peak varies. The higher the GAIN is, the wider the distribution will be. So OFFSET value st low GAIN is not suitable for high GAIN, because the curve is very likely to be chopped off.
Advanced Settings
For those CMOS less than native 16-bits, the AD sampling accuracy doesn’t match perfectly with the full well capacity. At low GAIN level, the system gain will be couple electrons per ADU. The camera loses the ability to distinguish the strength of the signal because of such sampling error.
When GAIN increases, the system gain will decrease. However, increasing GAIN will limit the full charge of the well. If the system gain is 1 for a 12bit CMOS camera, the pixel will be saturated at only 4096 electrons (full well). Some bright stars will be easily saturated. This problem goes worse under fast optical system or long exposure. Over saturated objects cannot be fixed during post processing (unless you shrink stars, like in PixInsight). Also, the color saturation of the star will be affected. As result, the stars will be huge and white washed. We should decrease the gain value in this case, to gain a higher full well capacity.
Under long exposure or using fast optical system, the pixel will receive more photons. The variation of quantized noise from the photon which you can consider as natural dithering of the light intensity, will be greater than the “noise” from the sampling error. Therefore, the effect of the sampling error will diminish. By averaging multiple exposures, this will compensate the lack of depth of the picture because of the sampling error.
If the number of received photons is limited, like using narrowband filters or short exposures, we can increase the GAIN value. It is because the stars will not be easily saturated. At the same time, we limit the noise from the background cosmic radiation. Under this condition, the readout noise and quantized noise are the major factors that affect the ability to distinguish dim light or objects. By increasing the GAIN value in order to decrease the readout noise and quantized noise from sampling error, this would greatly increase the signal to noise ratio.
Model Unit Gain
600M/C 25 (Extended Full Well Mode) *
268M/C 30 (Extended Full Well Mode) *
294Pro 1600 (11MP Mode)
410C 90 (Low gain) 40 (High gain)
367C 2800
247C 2200
128C 3300
168C 10
183M/C 10
163M/C 120
174GPS 17
550P 85




QHY Color Camera Debayer Matrix
Cooled CMOS Camera Bayer
QHY600C RGGB
QHY268C RGGB
QHY410C RGGB
QHY367Pro RGGB
QHY128Pro RGGB
QHY294C RGGB
QHY247C RGGB
QHY168C RGGB
QHY165C RGGB
QHY163C GRBG
QHY183C RGGB
QHY174C RGGB
QHY178C GBRG
QHY290C GBRG
QHY224C GBRG
Planetary and Guiding Bayer
QHY5III174C RGGB
QHY5III178C GBRG
QHY5III224C GBRG
QHY5III290C GBRG
QHY5III462C GBRG
QHY5III485C RGGB
QHY5L-II-C BGGR
QHY5P-II-C GBRG
Cooled CCD Camera Bayer
QHY8L-C GBRG
QHY10-C RGGB
QHY12-C BGGR



Measuring the absolute QE of the QHY268M
Sony provides relative QE curves for the IMX571 sensor used in the QHY268M camera. However, by comparing its response with a CCD of known absolute QE, the ICX694 used in the QHY22, we can determine the absolute QE for the QHY268M. The graph below from the Sony IMX571 datasheet shows the relative QE of the IMX571.The good news here is that this curve includes the



QHY600 Linearity Test
After the launch of the QHY600 refrigerated CMOS with native 16-bit AD conversion, the QHY600 has received wide attention from astrophotography lovers. And the first batch of production products was ordered out of stock in no time. QHY600 uses SONY’s IMX455 full-frame back-illuminated chip, which provides a variety of readout modes. Therefore, in addition to astrophotography, QHY600 also provides some relatively professional functions. They