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FGS Astrometry in 2 Gyro Mode E. P. Nelan STScI B. E. McArthur McDonald Observatory, U. of Texas.

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FGS Astrometry in 2 Gyro Mode E. P. Nelan STScI B. E. McArthur McDonald Observatory, U. of Texas
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Page 1: FGS Astrometry in 2 Gyro Mode E. P. Nelan STScI B. E. McArthur McDonald Observatory, U. of Texas.

FGS Astrometry in 2 Gyro Mode

E. P. Nelan

STScI

B. E. McArthur

McDonald Observatory, U. of Texas

Page 2: FGS Astrometry in 2 Gyro Mode E. P. Nelan STScI B. E. McArthur McDonald Observatory, U. of Texas.

Astrometry with the HST Fine Guidance Sensors

The Fine Guidance Sensors aboard HST are white-light interferometers. Their ability to provide precision tracking of guide stars also enables them to perform as a precision astrometric science instrument.

FGS1r has been calibrated to enable its use as a science instrument. Two observing modes:

• Transfer mode (fringe scanning, high angular resolution)• Position mode (fringe tracking, relative astrometry)

This presentation addresses performance of FGS1r in Position mode under two gyro operations.

Page 3: FGS Astrometry in 2 Gyro Mode E. P. Nelan STScI B. E. McArthur McDonald Observatory, U. of Texas.

FGS 1r Fringes

Position mode “locks” on to the zero point crossing of a star’s

interference fringes in both “x” and “y”. Star’s position in FGS FOV

is measured to a per observation precision of ~1 mas.

Page 4: FGS Astrometry in 2 Gyro Mode E. P. Nelan STScI B. E. McArthur McDonald Observatory, U. of Texas.

FGS Fine Lock

Page 5: FGS Astrometry in 2 Gyro Mode E. P. Nelan STScI B. E. McArthur McDonald Observatory, U. of Texas.

FGS Fine Lock

Page 6: FGS Astrometry in 2 Gyro Mode E. P. Nelan STScI B. E. McArthur McDonald Observatory, U. of Texas.

FGS Fine Lock

Page 7: FGS Astrometry in 2 Gyro Mode E. P. Nelan STScI B. E. McArthur McDonald Observatory, U. of Texas.

Error Sources for FGS Astrometry3 Gyro Mode

Error (per observation) Affect, before calibration (mas)

jitter 0.5

photometric 0.2

HST drift 20

Diff Vel Aberration 20

OFAD 1500

Scientific objective of astrometric programs is to achieve an accuracy of 0.2 mas.

Can this be done in 2-gyro mode?

Only jitter is an issue if different than 3-gyro mode.

Page 8: FGS Astrometry in 2 Gyro Mode E. P. Nelan STScI B. E. McArthur McDonald Observatory, U. of Texas.

Is Jitter Different in 2-gyro mode?

Page 9: FGS Astrometry in 2 Gyro Mode E. P. Nelan STScI B. E. McArthur McDonald Observatory, U. of Texas.

Is Jitter Different in 2-gyro mode?

Page 10: FGS Astrometry in 2 Gyro Mode E. P. Nelan STScI B. E. McArthur McDonald Observatory, U. of Texas.

Is Jitter Different in 2-gyro mode?

Page 11: FGS Astrometry in 2 Gyro Mode E. P. Nelan STScI B. E. McArthur McDonald Observatory, U. of Texas.

Is Jitter Different in 2-gyro mode?

Page 12: FGS Astrometry in 2 Gyro Mode E. P. Nelan STScI B. E. McArthur McDonald Observatory, U. of Texas.

Is Jitter Different in 2-gyro mode?

Page 13: FGS Astrometry in 2 Gyro Mode E. P. Nelan STScI B. E. McArthur McDonald Observatory, U. of Texas.

Is Jitter Different in 2-gyro mode?

Page 14: FGS Astrometry in 2 Gyro Mode E. P. Nelan STScI B. E. McArthur McDonald Observatory, U. of Texas.

Jitter is Different in 2-Gyro Mode

• Does it matter for FGS astrometry?– Amplitude is small (~2 mas 1-at 40 Hz), nearly the same as in 3-gyro

mode.– Jitter is well correlated across the 3 FGSs, guide star data can be used to

eliminate jitter in astrometer.

• Only the accuracy of the centroids on time scales of ~20 seconds is of importance to astrometry (median filter eliminates outliers)

Page 15: FGS Astrometry in 2 Gyro Mode E. P. Nelan STScI B. E. McArthur McDonald Observatory, U. of Texas.

Guide Star Jitter of 30 sec Centroids

Page 16: FGS Astrometry in 2 Gyro Mode E. P. Nelan STScI B. E. McArthur McDonald Observatory, U. of Texas.

Guide Star Jitter of 30 sec Centroids

easily removed during calibration

Page 17: FGS Astrometry in 2 Gyro Mode E. P. Nelan STScI B. E. McArthur McDonald Observatory, U. of Texas.

Jitter is Different in 2-Gyro Mode

• Does it matter for FGS astrometry?– Amplitude is small (~2 mas 1-s), nearly the same as in 3-gyro mode.

– Jitter is well correlated across the 3 FGSs, guide star data can be used to eliminate jitter in astrometer.

• Only the accuracy of the centroids on time scales of ~20 seconds is of importance to astrometry (median filter eliminates outliers)

• Conclude that jitter induced under 2-gyro mode does not degrade FGS1r astrometric performance.

Page 18: FGS Astrometry in 2 Gyro Mode E. P. Nelan STScI B. E. McArthur McDonald Observatory, U. of Texas.

However ……• Scheduling is heavily impacted.

– Parallax programs no longer can observe target fields at both epochs of maximum parallax factor.

– Scheduling constraints make observations of binary systems with optimal phase coverage more challenging.

– Calibration monitoring programs impacted.

– The requirement to use guide star pairs further exasperates scheduling opportunities.

• Fortunately, scheduling issues have had minor impact on continuing parallax programs. Most are in third (and last) cycle, final observation cans be made at either parallax factor.

Page 19: FGS Astrometry in 2 Gyro Mode E. P. Nelan STScI B. E. McArthur McDonald Observatory, U. of Texas.

Scheduling Impact

Page 20: FGS Astrometry in 2 Gyro Mode E. P. Nelan STScI B. E. McArthur McDonald Observatory, U. of Texas.

Conclusions

• Jitter environment in 2-gyro mode has no degrading impact on FGS astrometry;– Position mode

– Transfer mode (also unscathed)

• Scheduling impacts are significant– Made more difficult due to the requirement to have a guide star

pair.


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