Intensity Interferometry at Southern Connecticut State University WORKING TOWARD THE INTERFEROMETER IN A SUITCASE Elliott Horch, Southern Connecticut State.

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Intensity Interferometry at Southern Connecticut State University WORKING TOWARD THE INTERFEROMETER IN A SUITCASE Elliott Horch, Southern Connecticut State University HBT OCA

Collaborators SCSU Undergraduates: Matthew Camarata, now at Boston University A.J. Guerra Gerard van Belle (Lowell Observatory) Joe Ritter (University of Hawaii) Russ Genet (CalPoly) Bruce Holenstein (Gravic, Inc.) HBT OCA 2

Origins of Stellar Interferometry 1920’s: Albert Michelson builds first stellar interferometer by using two sub-apertures of Mt. Wilson 100-inch telescope. Measured several stellar diameters. Tried to extend the baseline, but mechanical issues prevented progress HBT OCA 3

How Optical Interferometry is Done Today… HBT OCA 4 Light is made to interfere prior to detection. (Michelson Interferometry). Higher signal-to-noise, but expensive. Certainly NOT portable. ~300 m baselines. Much Larger? Hmmm…

Intensity Interferomety There is a weak correlation in the arrival times of photons when viewed by two different detectors. “Wave Noise.” Related to beat frequencies, in the most extreme case. This effect was used in astronomy in the 1970’s to measure diameters of bright stars. One configuration of the two telescopes yields one Fourier component of the image (well, |  | 2 ). But, huge collectors were needed to detect this weak signal on the photomultiplier tubes of the day. 5 Sydney University Stellar Interferometer Photo: J. Davis P.S.: Only two stations, So no imaging! HBT OCA

“Wave Noise” HBT OCA 6

A lot has changed since 1974! S/N in Intensity Interferometry depends on telescope size AND speed of electronics. Timing capabilities today are about 1000x what they were in the 70’s. Can achieve the same result today with a much smaller telescope! (Portable Instrument!) HBT OCA

Simulation Data HBT OCA 8 Random Correlations  2 Data “Frames” ~0.4 s long (8192 elements)

Intensity Interferometry Revisited 9 Picoquant Picoharp 300 timing module. Two SPAD detectors Issues: Small size, dead time HBT OCA

Truly Portable HBT OCA m baseline SPAD Anderson Mesa (Lowell Observatory) Perkins Telescope Two runs: Dec 2011 & June 2012 Issues: Focus, Sky Position, Temp.

Lowell Set-up and Data HBT OCA 11

Big Glass is getting cheap! HBT OCA 12

Three-Station Wireless Interferometer at SCSU HBT OCA 13 GPS Computer Cards: ~0.5s synchronization

Dirty Beam Simulation HBT OCA 14 FWHM ~ 0.1 mas uv-plane coverage 6-hour observation

Kitt Peak: Another Possibility? HBT OCA 15 Mayall+WIYN (3.8m + 3.5m) ~700m baseline

SPAD Arrays Deadtime and small size can be mitigated if you have many SPADs all looking at the same source. Development of SPAD arrays is being started, e.g. the SPADlab at Everyphotoncounts.com HBT OCA 16

Optics Package for an 8-channel station HBT OCA 17 Grating Flat Coll. Lens Filter Reimager SPAD Array

Observation Time HBT OCA 18

Conclusions Intensity Interferometry Opportunity Today We’ve got intereting instrumentation for intensity interferometry: SPADs, Picoharp Large Dobsonian Telescopes are affordable for on-campus observing. Need to explore GPS Technology/atomic clocks for wireless operation. Take timing correlator and the SPAD detectors to larger telescopes. “Interferometer in a suitcase.” Lowell: Already doing this. Kitt Peak: A possibility for the future. Science: Imaging close binaries, stellar surfaces Imaging an exoplanet transit? (One fine day…) HBT OCA