today: calculating ccd gain aperture vs. psf …astronomy 101 lecture # 6 airmass = sec −0.0018167...
TRANSCRIPT
Today: Calculating CCD gain Photometry Aperture vs. PSF Photometry Photometric Filters Effects of Atmosphere – Airmass Differential vs. Absolute Photometry Photometry of Extended Sources SNR and Exposure Time
Reading: Ch. 7 (pp. 125–132), 10
Astronomy 101 Lecture # 6
PhotometryDirect measure of integrated flux (counts per unit time
per unit area ) received from a celestial target.●
●
●
F = specific flux from a target S = transmission function that describes
Filter passband CCD response Atmospheric transmission
F=∫0
∞
F⋅S
d
Astronomy 101 Lecture # 6
Magnitudes and Fluxes
m1−m2=2.5 log10 F2
F1 ● Bolometric Magnitude:●
●
●
●Color Magnitude: mV ,1−mV ,2=2.5 log10 FV , 2
FV ,1
Astronomy 101 Lecture # 6
How do we measure F?
●Main Methods:● 1. Aperture photometry● 2. Pointspreadfunction (PSF) ● fitting
F=∫0
∞
F⋅S
d
Astronomy 101 Lecture # 6
Aperture Photometry
Main stellar aperture
Astronomy 101 Lecture # 6
Background annulus
m=C−2.5 log10 [ N star−N sky ]
PSF PhotometryStars too close together to do a simple aperture count.
Need to do PSF fitting: modeling the radial “shape” of each stellar image.
Astronomy 101 Lecture # 6
PSF PhotometryAiry Pattern: Ideal PSF
Astronomy 101 Lecture # 6
Slide Credit: Don Hoard
PSF Photometry
Real PSFs are considerably more complicated.
Astronomy 101 Lecture # 6
Astronomy 101 Lecture # 6
PSF Photometry
Real PSFs are considerably more complicated.
Example: Hubble images of quasars from Bahcall et al.
Slide Credit: Don Hoard
Astronomy 101 Lecture # 6
PSF Photometry
Slide Credit: Don Hoard
How do we determine S?
●Main Contributions:● 1. CCD response● 2. Filter bandpass● 3. Atmospheric Transmission
F=∫0
∞
F⋅S
d
Astronomy 101 Lecture # 6
CCD Quantum Efficiency
●From Apogee Instruments
Astronomy 101 Lecture # 6
Astronomy 101 Lecture # 6
WideBand Photometric Filters
Astronomy 101 Lecture # 6
MediumBand Filters
Astronomy 101 Lecture # 6
NarrowBand Filters
Atmospheric Transmission Astronomy 101 Lecture # 6
mobs=mstar 0 sec
Astronomy 101 Lecture # 6
Airmass= sec−0.0018167 sec−1−0.002875 sec−12−0.0008083 sec −13
A better approximation:
Airmass Correction
How do we invert this equationto determine F
?
●Main Methods:● 1. Differential Photometry● 2. Absolute Photometry
F=∫0
∞
F⋅S
d
Astronomy 101 Lecture # 6
●Converting from instrumental magnitude to apparent magnitude.
Astronomy 101 Lecture # 6
m1= I1−I 2m2
mi=calibrated magnitude of star iI i=instrumental magnitude of star i
Differential Photometry
Slide Credit: Don Hoard
Astronomy 101 Lecture # 6Absolute Photometry
What if there are no calibrated stars in the same CCD frame as your target?
● Make separate observations of standard stars on the same night. Examples of star catalogs include
Landolt 1992, AJ, 104, 340 Stetson http://cadcwww.hia.nrc.ca/cadcbin/wdb/astrocat/stetson/query ● Standard star observations must span a range of airmasses (typically 1–
2.5) and a range of colors the same as that of science targets. ● Obtain observations of standard stars and targets in at least 2 filters. ● Use standard star observations to derive coefficients for the
“transformation equations” which can then be utilized to calibrate instrumental magnitudes of science targets.
Slide Credit: Don Hoard
Astronomy 101 Lecture # 6
Transformation Equations
B – V = (b–v) Tbv + Kbv X + Zbv
V – R = (v–r) Tvr + Kvr X + Zvr
R – I = (r–i) Tri + Kri X + Zri
V – I = (v–i) Tvi + Kvi X + Zvi
R = r Tr + Kr X + Zr
V = v Tv + Kv X + Zv
B, V, R, I = calibrated magnitudesb, v, r, i = instrumental magnitudesX = airmassT = color transformation coefficientsK = atmospheric extinction coefficientsZ = zero point corrections
Use IRAF package digiphot.photcal to solve for transformation coefficients and apply calibration to data.
Slide Credit: Don Hoard
Magnitude to Flux Conversion
FX = f
, X 10−m
X/2.5
FX=FX W X
Specific flux in the center of band X:
Total flux in band X:
Astronomy 101 Lecture # 6
SNR and Exposure Time
SNR=SN=
N star
N starnN skyN DN R2
Poisson Noise Limited:
Background Limited:
SN≈
N star
N star
= N star∝ F star t
SN≈
N star
n N sky
∝Fstar
Fsky
t