HPO

Astronomy

Hopkins Phoenix
Observatory


Photoelectric Photometry

 

White Paper

Extinction

J and H Band Extinction

Introduction
When doing system calibration or all-sky photometry it is essential to know the extinction coefficients. The following explains three methods of determining the extinction coefficients.

Differential Photometry Method I
This method is used for differential photometry. The comparison star is used as the star for determining the extinction coefficients and is measured through a range of air masses.

Note: Due to the nature of these bands, extinction is very low and for differential photometry can usually be ignored.

System Calibration Method II
This method uses multiple stars with (J-H) ~ 0.00 at significantly different air masses. This method is used when calibrating the system.

All-Sky Photometry Method III
THis method uses multiple stars of any color, but at significantly different air masses. This method is used when doing all-sky photometry.

Objective

To determine extinction coefficients kj and kjh. Determining the extinction coefficients and zero points depends on using the equation for a straight line Y = MX + B where M is the slope and B is the Y intercept (point where line crosses the Y axis when
X = 0.

The key is to get the coefficient equations in the form of Y= MX + B.

Note: Some books use the Gewwk letters epsilon and mu for the color transformation coefficients for J and (J - H) bands. Because the symbols are used in the UBV bands the symbols rho and lambda are used in this paper for the color transformation coefficients for J and (J - H) respectively.

Note: Air Mass X of each observation must be determined. Determining air mass is somewhat involved and covered in another white paper.


Method I
Differential Photometry

Using the Comparison Star measure J and H magnitude values of the Comparison Star through a wide range of air masses. Note the air mass X of the observation and calculate instrumental magnitudes j and h.

Corrected counts are counts normalized to 1 second integration and unity gain. Sky readings have been subtracted.

j = - 2.5 log10 (J corrected counts) Equation 1

h= - 2.5 log10 (H corrected counts) Equation 2

The values jo and ho are the extra-atmospheric magnitudes.


Note: The Y intercepts are not used in this method and do not represent the zero points.

Method II
For System Calibration when system rho and lambda are unknown.

Use multiple stars with (J - H)~ 0.00 .

Measure J and H magnitude values of standard stars with (J - H)~ 0.00 at a wide range of air masses.

Note: Corrected counts are counts normalized to 1 second integration and unity gain. Sky readings have been subtracted.

j = - 2.5 log10 (J corrected counts) Equation 1

h= - 2.5 log10 (H corrected counts) Equation 2

Note: The air mass X of the observation and calculate instrumental magnitudes j and h. By doing this the observation time can be short as the stars do not have to travel through a range of air masses. Different stars should be at different air masses.


Method III
All Sky-Photometry Multiple stars of any color with known system rho and lambda.

Use multiple stars of any color.

Measure J and H magnitude values of standard stars of any color at a wide range of air masses. Note the air mass X of the observation and calculate instrumental magnitudes j and h.

Note: Corrected counts are counts normalized to 1 second integration and unity gain. Sky readings have been subtracted.


Return

Present Page Version as of 1 November 2006

phxjeff@hposoft.com
www.hposoft.com