Floating material and so forth

Consider a task that computes profile parameters for a modified Lorentzian of the form

#math174#
I = #tex2html_wrap_indisplay965# (5)
where

#math175#

d1 = #tex2html_wrap_indisplay967#

#math176#

d2 = #tex2html_wrap_indisplay969#

#math177#

x1 = (x - x0)cosΘ + (y - y0)sinΘ

#math178#

y1 = - (x - x0)sinΘ + (y - y0)cosΘ

In these expressions x0,y0 is the star center, and Θ is the angle with the x axis. Results of this task are shown in table~#tbl-1#127>. It is not clear how these sorts of analyses may affect determination of M#tex2html_wrap_inline977# and #math179#M#tex2html_wrap_inline979#, but the assumption is that the alternate results should be less than 90 out of phase with previous values. We have no observations of <#130#>Ca<#130#><#131#>2<#131#>. Roughly <#132#>4<#132#><#133#>5<#133#> of the electronically submitted abstracts for AAS meetings are error-free.

We are grateful to V. Barger, T. Han, and R. J. N. Phillips for doing the math in section~#hairymath#134>.