I have only recently begun following this forum, and I find the ideas shared here very interesting.
Dr. Brian Kloppenborg suggested that I share this approach here with the Smart Telescope Working Group.
I also own a Celestron Origin telescope, which I primarily use for live online astronomy presentations. Recently, however, I have started experimenting with photometric observations using the Origin, mainly targeting RR Lyrae and δ Cephei type variables.
In parallel with this, I continue to perform photometric measurements using Newtonian telescopes mounted on equatorial mounts, equipped with a monochrome CMOS camera (ZWO ASI1600MM Pro), ASIAIR control, and non-standard (ZWO New LRGB) filters. During the reduction of these observations, I developed a method to convert instrumental magnitudes into standard magnitudes.
The essence of the method is the following:
For each image series, I perform ensemble differential photometry on all stars within the field of view that have known standard magnitudes listed on AAVSO charts, and I determine their instrumental magnitudes.
For the non-variable stars, the instrumental magnitudes obtained from the ensemble photometry are averaged over the entire duration of the observing sequence. Since these stars are constant in time, averaging reduces measurement noise, while the standard deviation provides a useful characterization of the internal stability of the observing sequence and the observing conditions.
Each star thus contributes a single data point consisting of its averaged instrumental magnitude and its corresponding standard magnitude. These data points form the basis of a linear regression. From this regression, I determine the transformation equation valid for the given observing sequence, which I then directly use to convert the variable star’s instrumental magnitude into a standard magnitude.
The primary goal of this approach is to determine the standard magnitude of the observed variable star within a given observing sequence with the highest possible internal consistency.
The correlation coefficient obtained from the linear regression and the residual scatter provide immediate, quantitative feedback on the internal precision of the observing sequence and indicate the level of scientific use for which the results may be suitable.
In this approach, I do not treat the transformation as a constant system parameter, but rather as a local fitting problem: for each observing sequence, I determine an empirical relationship fitted to the standard stars present in the field of view.
Conceptually, this sequence-level fitting may be related to the nightly coefficient strategies currently discussed within the STWG, although implemented here at the level of a single observed field.
I would be interested to learn whether similar sequence-specific transformation strategies are being considered within the current STWG workflow.
If this is of interest, I would be happy to return with a more detailed and mathematically
Best regards,
Vilmos Tekler