Effectiveness Of Phase Dispersion Minimization In Gyrochronology By: Jeremy Stone
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Transcript of Effectiveness Of Phase Dispersion Minimization In Gyrochronology By: Jeremy Stone
Effectiveness Of Phase Dispersion Minimization In Gyrochronology
By: Jeremy Stone
Introduction
Simulated Data
Barry Lutz Telescope (BLT) Data
Catalina Sky Survey Data
Example Light Curve
• Period = 7 days
• Amplitude = .05
• Random error = 2%M
agni
tude
Period (Minutes)0 1 2 3 4 5 6 7 8 9 101112131415161718192021222324252627282930
2.94
2.96
2.98
3
3.02
3.04
3.06
3.08
Light Curve
0 1 2 3 4 5 6 7 8 9 10 11 122.94
2.96
2.98
3
3.02
3.04
3.06
Period (Days)
Mag
nitu
de
Period
0 2 4 6 8 10 Period (days)
1
.9
.8
Thet
a
HIP 19859
Target Star
HIP 19859 Light Curve
2455980 2455985 2455990 2455995 2456000 2456005 2456010 24560152.1
2.2
2.3
2.4
2.5
2.6
2.7
2.8
2.9
3
Date (HJD)
Rel
ativ
e M
agni
tude
HIP 19859 Period
0 2 4 6 8 10
Period (Days)
1
.8
.6
.4
.2
Thet
a
Problems and Difficulties
Weather
Technical Issues
Errors
Catalina Sky Survey
Catalina Sky Survey
Started in 2005
Searching for near Earth objects
Photometry on 198 million objects
HIP 3998 Light Curve
PDM
.4 .6 .8 1 Period (Days)
1.5
1
.95
.9
.85
Thet
a
Comparing Ages
Collected ages from published papers
Gyrochonology equation P(B-V,t) = f(B-V) * g(t)
Where f(B-V) = (0.7725 ± 0.011) (B-V0-0.4)0.601±0.024
And g(t)=t0.5189±0.0070
Thanks
NASA Space Grant
Northern Arizona University
Dr. Koerner
Dr. Barlow and Kathleen Stigmon