Telescope Systems Scientist
TelAO
LabAO
New hires:
AO+6T observing is regular now, soon most nights may be 6T IR+VIS with MIRC-X, MYSTIC, & SPICA running simulataneously
(CHARA Michelson Array Pathfinder)
Mobile Telescope Transport (TR116)
Ligon et al. 2022
S3
S4
The full Michelson Array would offer
12 total positions, creating 66 possible baselines.
1100m
600m
~17m
S3
S4
W5
MIRX
MYSTIC
SILMARIL
SPICA
CHARIOT
PAVO
SPICA
VIS BEAMS
METROLOGY
STS/STST
BEAM SAMPLERS
BEAM SAMPLERS
BEAM SAMPLERS
Lanthermann et al. 2022
MIRC-X disperses light across several spectral channels and operates in the J and H-bands. MYSTIC operates in the K-band. MIRC-X/MYSTIC can be used simultaneously to create images of stellar surfaces and circumstellar disks. The precision closure phases are well suited to detecting faint binary companions.
Three spectral modes are currently available in the H-band: prism R=50 (8 spectral channels), prism R=102, and grism R=190. A higher resolution grism with R=1170 is available (with approval)
STS and STST
Anugu 2020
MYSTIC, the Michigan Young STar Imager at CHARA is a K-band, cryogenic, 6-beam combiner. All-in-One 6T or high sensitivity 4T gravity chip
A 4-telescope mode for MYSTIC using an integrated optics component designed for the VLTI-GRAVITY experiment is under development and will provide better sensitivity for the faintest targets.
MYSTIC is available in the K-band using a low-resolution R=49 prism. Additional spectra modes (prism R=22, grism R=278, grism R=981, grism R=1724)
Setterholm et al. 2023
Pannetier et al. 2021
(Stellar Parameters and Imaging with a Cophased Array)
SPICA-FT H-band 6-beam ABCD combiner by VLC Photonics, inspired by GRAVITY
low-resolution mode uses MIRC-X for fringe-tracking
The goal of the SPICA project is to provide a large and homogeneous set of stellar parameters across the HR-diagram. The survey aims to measure the angular diameters of 1000 stars.
Low-resolution spectrograph for measuring precise angular diameters (R=150, 50 channels over 650–950 nm).
For a sub-sample of bright stars, medium (R=4300) and high (R=13,200) spectral resolution modes will be available for spectral imaging of stellar surfaces and environments and kinematic studies.
spectrograph
(CHARA Array Integrated Optics Testbed)
collaboration with Leibniz Institute for Astrophysics Potsdam (AIP)
ULI optics for JHK bands
(Siliprandi, Labadie, Madhav, Dinkelaker, Thompson, Benoît)
Currently have two injection stages, CRED1 arrives this year
Coupling ratio evolutions of (input coupling waveguide) and R2(λ) in blue diamonds of a writing beam combiner characterized by coupling input light in the two external PT1 and PT2 inputs to obtain two experimental measurements of the 3 dB asymmetric directional coupler (a, b) and one for each photometric asymmetric Tap directional couplers, as Tap 1 (c) and Tap 2 (d)
Siliprandi et al. 2022
There are some 250 known exoplanets with host stars accessible to CHARA (Dec>-30 deg, V < 7). The new baselines will enable resolution of solar-like stars out to about 70pc in H-band. Numerical simulations of the transiting hot-Jupiter in HD189773 indicate that the shape of the silhouette of the planet can be measured in long baseline observations made during transits.
The Gaia orbits give the center-of-light motion of unresolved binaries, and a single resolved CHARA observation is sufficient to determine the full orbit and masses. High angular resolution observations also reveal how interacting stars are transformed by mass exchange.
NGC 4151
Early results from CHARA already show that the innermost dusty region in NGC 4151 is aligned perpendicularly to the jet axis.
following slides stolen from EXOPAG 23:
Narcissus Mirror for SILMARIL
up to 300 nights over three years of open access time via (NOIRLab).
Snapshot Imaging Mode to encourage new investigations.
Some thoughts from AAS 241
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[2] Beichman et al. 2006 ApJ 652
[3] Roberge et al. 2012
[4] Defrère et al. Proc. SPIE 2012
[5] Stark et al. 2014
[6] Kennedy & Wyatt 2013
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[8] Fajardo-Acosta et al. 2000
[9] Mannings & Barlow 1998
[10] Laureijs et al. 2002
[11] Lawler et al. 2009
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[13] Defrère et al. 2015
[14] Mennesson et al. 2014
[15] Absil et al. 2013
[16] Ciardi et al. 2001
[17] di Folco et al. 2004
[18] Absil et al. 2006
[19] di Folco et al. 2007
[20] Absil et al. 2008b
[23] Defrère et al. 2011
[24] Mennesson et al. 2011a
[25] Mawet et al. 2011
[26] Lisse et al. 2012
[27] Weinberger et al. 2011
[28] Defrère et al. 2012a
[29] Lisse et al. 2013
[30] Ertel et al. 2014
[31] Marion et al. 2014
[32] Nuñez et al. 2017
[33] Kral et al. 2013
[34] Krivov et al. 2006
[35] Wyatt et al. 2007 ApJ 663
[36] Defrère et al. 2012 A&A 546
[37] Marshall et al. 2016
[38] van Lieshout et al. 2014 A&A 571
[39] Jackson et al. 2012
[40] Rieke et al. 2016
[41] Su et al. 2016
[42] Wyatt et al. 2008
[43] Su et al. 2013
[44] Lebreton et al. 2013
[45] Eiroa et al. 2016, A&A 594, Oct 2016
[46] Faramaz et al. 2016
[47] Ertel et al. 2018