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Re: Tech Note 97: Photometric properties of TOM1 data
Stupendous Man wrote:
> I've read several times that one ought to use these equations:
> picking stars of known magnitude -- standards -- one writes
>
> V = v + av + bv*(V - I) (1)
> I = i + ai + bi*(V - I) (2)
>
> Solve for the zeropoints av and ai, and the color terms bv and bi,
> by the method of least squares. Fine.
>
> Now, for all the stars which do NOT have known magnitudes,
> we want to calibrate the instrumental magnitudes; that is, we
> wish to turn v and i into V and I. We _must_ have some formula
> for doing so in terms of the quantities we know: the instrumental magnitudes,
> the zero points, and the color terms:
>
> V = f(v, i, av, bv, ai, bi)
> I = f(v, i, av, bv, ai, bi)
>
> The references I have found state at this point: "one must invert
> the equations (1) and (2) to solve for the standard magnitudes
> in terms of the instrumental ones." Presumably, one ends up
> with something like this:
>
> V = v + av' + bv'*(v - i) (1a)
> I = i + ai' + bi'*(v - i) (2a)
>
> where the values av', ai', bv' and bi' are related algebraically
> to their counterparts av, ai, bv and bi.
>
> So, what I have done is to skip directly to equations (1a) and (2a),
> rather than going through (1) and (2) and inverting. I understand that
> this is less desireable, because one knows the true V,I magnitudes
> of standard stars to a high accuracy, and so can derive
> _accurate_ values of the primed coefficients.
>
The way you normally do this is to solve for the color index first
and then substitute that into the magnitude equation. See the
description in my photometry book.
>
>>kv = 0.2 is too low for ground-level sites. Values of 0.3 would be closer.
>
>
> That's easy to change: it's the "fixk" parameter in the
> photom.param file. How big a difference does this make? A typical
> airmass for stars on the equator is about 1.4. Only differential
> extinction across a frame is required, and the difference in airmass
> is about 0.1 at most from the top to bottom of a Mark IV image.
> So the difference between a star at the top and a star at the
> bottom would be
>
> currently, in V: (0.1 airmass)*(0.2 mag/airmass) = 0.02 mag
> Arne's suggestion (0.1 airmass)*(0.3 mag/airmass) = 0.03 mag
>
> A difference of 0.01 mag at most. This might show up as a small systematic
> error, indeed. It would be smaller than the spatial errors I mention
> in TN 97, which are of order 0.05 mag in amplitude.
>
yup, but that is on the equator. you need to handle the general case.
>
>>What are the values for the two color terms?
>
>
> This bothers me. The terms are small, but they are NOT the same
> from one night to the next. I indeed looked at this during my
> recent work, hoping that I could derive good mean values that
> could then be fixed and used for all nights. But look at my
> results:
>
> based on all data on disk (good and bad sections of nights),
> derived one night at a time
> bv ranges -0.02 to -0.15
> bi ranges +0.03 to -0.13
>
> based only on a set of 10 good nights,
> derived one night at a time
> bv ranges -0.02 to -0.10
> bi ranges -0.07 to -0.13
>
> based on good night 606, 2745 stars total
> bv = -0.021
> bi = +0.076
>
> based on good nights 606 + 608, 3644 stars total,
> derived simultaneously
> bv = -0.049
> bi = +0.007
>
> based on good nights 606 + 608 + 609, 10821 stars total
> derived simultaneously
> bv = -0.044
> bi = +0.062
>
> based on good nights 606 + 608 + 609 + 614, 26650 stars total
> derived simultaneously
> bv = -0.032
> bi = +0.074
>
> You see? I was hoping that the values would converge, but it's not
> clear to me that they do.
>
There should be random scatter around a mean value, which is not
happening. I suspect the instrumental color problem is the root
of this.
>
>>You should *not* use the Tycho2 transformations to determine color
>>terms. The Ic values are nowhere near close enough to Landolt.
>>You should only use those Landolt standards that fall within scans
>>for that determination. So set zeropoints perhaps with Tycho2,
>>but determine coefficients separately.
>
>
> Perhaps you don't understand what's happening here. The procedure
> I followed is:
>
> - start with raw instrumental magnitudes
> - transform to Tycho2 magnitudes
> - transform AGAIN to Johnson-Cousins magnitudes
>
> I'd love to skip the intermediate step, but it's not possible:
> there is no guarantee that a Landolt standard will appear in
> every image. In fact, there is no guarantee that a Landolt
> standard will appear in an entire night!
>
So then I get confused. I understand the first two steps (but in step
two, you are transforming to the Tycho2 "BVRI" dataset, right, and
not to Bt/Vt), but don't understand how you are going from there
to the third step.
> If the Mark IV units were run like so:
>
> a) only on clear nights
> b) moving to fields with Landolt standards once per hour or so
>
> then one could reduce their data in the usual fashion, following several
> of the criticisms you have raised. I'd love to do that, of course.
> However, given that Tom collects data
>
> a) on all nights, clear or otherwise
> b) with no plan to acquired fields with Landolt standards
>
> I don't see a way to reduce his data in any other way. One could argue
> that the proper thing to do is to discard it, or perform only
> differential measurements within a single field. One might be correct.
> I'm trying to do the best job possible to place Tom's measurements
> onto the standard scale, so that they might be of use to others.
>
There are several approaches.
- leave everything instrumental for now, and calculate magnitudes
differentially with respect to local comparison stars in the
frame (an ensemble solution, but on Tom's native system).
- just convert magnitudes to Johnson/Cousins V/Ic by applying
zeropoints, but with no additional color correction. This
is the safest method.
- do your three-step method, which I think fails since it requires
the Tycho2 stars be of sufficient V/Ic accuracy.
- use the LONEOS file to obtain "standards" on about a 5-degree
grid; that may be sufficient for your calibrations
- wait for ARNE or another system to obtain reliable photometry
and reprocess the data (at the starlist level) then. That
is the approach I suggest. As soon as ARNE is ressurected
I should be able to produce a good photometric catalog.
- do a global solution. As long as frames overlap, you should
be able to transfer calibration across the sky from where
real standards reside.
Arne