Here is a report I wrote on June 26, 2000 on this attempt:

CX 6.26.00

This is an update of the progress in the task of 1-d fittings of the bright stars. The results (including this
report) can be found in skywave: /data3/2mass/ray2/results
(1) Profiles of five more stars have been provided by Raymond. All have CIO K mags
       (from K=-1.2 to   K=1.5), and 4 have CIO J mags (from J=-1.1 to J=1.7).
(2) By fitting the profiles of these very bright stars, I found that the function I used in the
       begining (two exponentials) is not a good shot.
(3) After talking to Gene Kopan and Bill Wheaton, I decided to use the so called
      'Voigt function' (in "Astrophysical Formulae", K.R. Lang, p220). Since this is an integral
      function and not very easy to use, I found, with some experiments, the following  approximation
      of the function which seems good enough for our purpose:
          H(a,b)  =  exp(-bv^2) + 3.1*av/(sqrt(3.1416)*bv^2+3.1416)
      where:
                      av = sqrt(log(2))*dv_l/(2*dv_d)
      and
                      bv = 2*sqrt(log(2))*x/dv_d
      (dv_d and dv_l are the FWHMs of the central Gaussian and of the Lorentz  wing, respectively).
(4) The fitting function is then the following 3 parameter (a(0), a(1) and a(2))  function:
                   s = exp(a(0)-bv^2) + exp(a(0))*3.1*av/(sqrt(3.1416)*bv^2+3.1416)
       where:
                      bv=2.*sqrt(alog(2.))*x/a(1)
        and
                     av=sqrt(log(2))*a(2)/(2*a(1)) .
(5) After some experimenting, I found that I can further reduce the number of parameters from
       3 to 2, becuase there is a strong correlation between a(2) and a(1). This indicates that,
       for our data, the amplitude of the central Gaussian and that of the Lorentz wing is highly
       correlated. In fact, the parameter av is found to follow the relation: av=exp(-a(0)*0.5+1.5).
      This relation eliminates the need for the third parameter a(2).
(6) The results  are given in the table, and in the gif plots found in this directory.
(7) Notes:
      1) The amplitude is parameterized as exp(a(0)). This is to ensure that it is always > 0.
      2) There seems to be a good correlation between CIO mags and mags from these fits,
           though the relation is not really linear.
      3) The fit can still be improved. But it takes a lot of time.
      4) This algorithm needs to be tested with more stars.
 

Cong
 
 
 

                                                                        Table: Results

star#       J-CIO        J_fit         a_j(0)        a_j(1)       K_CIO       K_fit       a_k(0)       a_k(1)        H_CIO
1                -1.1        -0.73         18.48           2.07           -1.2         -1.65         15.50           2.15            -1.3
2                 0.6            0.49         15.68           1.84            -0.1           0.52         13.35           2.27             -0.1
3                                   1.31         14.81           1.94              0.1           1.50         12.30            2.41
4                 1.7            2.52          13.70          1.92              0.5            1.74         12.18           2.28
5                 1.5            2.29          14.20          1.67              1.5            2.55         11.67           1.99               1.6
 

Figures:
fit_star1_j.gif 
fit_star1_k.gif
fit_star2_j.gif
fit_star2_k.gif
fit_star3_j.gif
fit_star3_k.gif
fit_star4_j.gif
fit_star4_k.gif
fit_star5_j.gif
fit_star5_k.gif