Heriot-Watt
2026 - 294 refereed papers & 61 PhD dissertations so far
" technical improvements in both hardware and software will continue indefinitely.
one rationale for the facility is to serve as a testbed for new developments in optical interferometry."
The CHARA Array is operated by the Center for High Angular Resolution Astronomy at Georgia State University in Atlanta.
The two-telescope CLASSIC beam combiner
The MIRC-X H-band combiner. A six-telescope cryogenic K-band beam combiner, MYSTIC
The upgrades to the six-telescope MIRC-X combiner
SPICA combines all six-telescopes and provides a range of spectral dispersions at visible wavelengths.
Precision Astronomical Visible Observations (PAVO) instrument
The (PAVO) visible beam combiner
the ALOHA fiber experiment.
Pushing the sensitivity limits of the Array in order to resolve the cores of Active Galactic Nuclei.
Open access time at the CHARA Array is available to the astronomical community through the National Optical-Infrared Astronomy Research Laboratory (NOIR Lab).
CHARA Science Meeting 2025 - Nice, France
CHARA/MROI Science Meeting and New Visions in Optical Interferometry Workshop 2026 - Socorro, NM
workshop supported by
Eaton Fire Jan 2025
Station Fire (2009)
Bobcat Fire (2020)
Eaton Fire (2025)
1920 - measured Betelgeuse (with Pease)
1956 - HBT effect, correlation b/t coherent photons
Intensity interferometry
details can be gained through interferometric measures
details can be gained through interferometric measures
details can be gained through interferometric measures
Image credit: ESO
Direct detection
Examples:
Labeyrie - 1975
diameter
Lawson 2003, S&T
Limb darkened vs Uniform disk
binarity
Separation
flux ratio
(B/λ)
Placement matters
The Array is capable of resolving details as small as 200 micro-arcseconds, equivalent to the angular size of a coin seen from a distance of 16,000 km.
"the CHARA Array continues to offer exceptional opportunities for scientific discovery using the longest operating baselines in the world among optical/near-IR interferometers"
Spatial resolution
• 0.20 mas at R (650 nm)
• 0.52 mas at H (1.67 μm)
• 0.66 mas at K (2.13 μm)
34 to 331m
Sigma Geminorum
TelAO
Optical Path Length Equalizers (OPLE) system
LabAO
MIRX
MYSTIC
SILMARIL
SPICA
CHARIOT
PAVO
VIS BEAMS
METROLOGY
STS/STST
BEAM SAMPLERS
BEAM Reduction
LabAO
MIRC-X
MYSTIC
(Stellar Parameters and Imaging with a Cophased Array)
The goal of the SPICA project is to provide a large and homogeneous set of stellar parameters across the HR-diagram.
spectrograph
Aug 2023 - First fringes with SPICA/MIRC-X/MYSTIC
Silmaril
(CHARA Array Integrated Optics Testbed)
collaboration with Leibniz-Institut fur Astrophysik Potsdam, University of Cologne, Heriot-Watt University
ULI optics for JHK bands
Apr 2024 - First fringes
Mobile Telescope Transport (TR116)
(CHARA Michelson Array Pathfinder)
S4
S3
ALOHA – Univ. Limoges
Single-mode PM fibers
λ=810nm, 240m long
Laying on the ground
Connect S1+S2
On-sky fringes Magri+2024
CMAP
Single-mode PM fibers
λ=1.6μm, 650m long
Trench: 18 inches deep
20 ← 34 - 331 → 579 m
S3
S4
Single-mode PM fibers
λ=1.6 μm, 650 m long
Trench: 18 inches deep
1100 m
W5
S3
S4
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.
Earliest Science
Rapid Rotators
Regulus -- Che et al. 2011, ApJ, 732, 68
Rasalhague -- Zhao et al. 2009, ApJ, 701, 209
Altair -- Monnier et al. 2007, Science, 317, 324
Alderamin -- Zhao et al. 2009, ApJ, 701, 209
Beta Cas -- Che et al. 2011, ApJ, 732, 68
Star spots
Polaris
sigma Geminorum
zeta Andromedae
Expansion curve of Nova Del 2013.
AAVSO, Hopkins et al. (2012)
Be stars
P = 12.9 d
a = 0.87 mas
Exoplanet Systems
Stellar Pulsations
Circumstellar Environments
Binary and Multiple Star Systems
angular orbit + distance estimate → total mass of components
angular orbit + radial velocity orbits → individual masses + independent distance measurement
→ stellar evolution processes and interactions between binary stars
Ashley Elliott 2024
Ashley Elliott (LSU) has compiled interferometric measurements from CHARA and more to create an empirical HR diagram.
Angular Dia. + Parallax → Linear Radius
Diameter + Bolometric Flux → Teff
interferometric angular diameters provide key benchmark data to evaluate calibrations of effective temperature from large-scale spectroscopic and photometric surveys - SED/CHARA
693 stars, σθ < 5%
Castor A and B
HD 284163
hierarchical quadruple system
Gleise 486
Interferometric observations of exoplanet host stars provide the means to determine the detailed stellar characteristics that are required to find the exoplanet properties.
Planet formation is generally considered in the context of young stars, but mass loss in older stars may also play a role in making planets at the end of a star's life.
If so, represents the first example of a polar circumbinary planet.
Image credit: Dr Mark A. Garlick / markgarlick.com
post-AGB star AC Her
→ the large cavity in the center of the circumbinary disk is not created by the tidal action of the central binary.
The process of planet formation involves the development of instabilities in the disk that can be followed through time series interferometric observations at very high angular resolutions.
luminous Herbig Be star HD 190073
V1925 Aql
NGC 4151
bright central region of the active galactic nucleus of the Seyfert galaxy NGC 4151.
Exoplanet Systems
51 Eridani system - resolved planet in 32 yr orbit, PARSEC evolutionary models → stellar mass and age, & a planetary mass of 4MJup Elliott+2024
Stellar Pulsations
Circumstellar Environments
Interferometric Methods
Anugu+2026 first experiments in dual field interferometry at the CHARA Array
→ yields measurements of the differential positions
α Psc → hierarchical triple.
Anugu et al. (2026)
ρ = 1.85"
Outer A-B
468 proposals submitted since 2010
132 unique OA PIs
90 distinct institutions
up to 300 nights over 3 years of open access time via NOIRLab
dedicated to community growth in US and beyond
staff assist new investigators with planning observations, collecting data, and reducing data
calibrated oifits files provided
open to all observers
New Fast Turnaround Snapshot Imaging Mode
Priority for observers who do not have existing time and for targets not already included in programs with awarded time.
https://chara.gsu.edu/observers/applying-for-chara-time
| Stellar AP |
| Diameters |
| Rapid Rotators |
| Surface Imaging |
| Be Stars |
|
Asterosiesmology |
|
Stellar Atmospheres |
| Disks |
| Stellar Winds |
| Limb Darkening |
| Metalicity |
| Temperature |
| Polarimetry |
| Orbits |
| Masses |
| Interacting Binaries |
| Distances |
|
Cepheid Distance |
| Trigonometric |
Exoplanets
Clusters & Ages
AGN
Engineering
<5% loss to technical issues
optimize simultaneous observations in visible + NIR
2028
2028+
Current sensitivity limits:
Visible/NIR fringe recording: 8.0 mag
Sensitivity improvements → K = 10-11 mag
Injection into fibers at telescope
STST Strehl~55–70% (H), 5-15% (R)
Next-gen AO system (planning):
CHA
20 to 1100m
• 0.06 mas at R
• 0.16 mas at H
• 0.20 mas at K
The full Michelson Array would offer 12 total positions, creating 66 possible baselines.
Image an exoplanet during transit
There are some 250 known exoplanets with host stars accessible to CHARA.
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 silhouette of the planet can be measured in long baseline observations made during transits.
HD189773
"Priorities will include stellar system evolution: planetary formation and young stellar objects, imaging the sites of planet formation in the inner region of circumstellar disks, and measuring the contraction of pre-main sequence stars."
The CHARA Array is supported by the US NSF under grants AST-2018862, 2034336, 2407956, 2511059.
The role of the CHARA Array continues to expand...
We plan to further expand new frontiers in instrumentation through collaboration and to support long-term initiatives for interferometry and the development and testing of new technologies that will provide the foundation for future very large long-baseline interferometers.
[1] Eisenhauer et al. ARA&A 61, 237–285 (Aug. 2023).
[2] Wright, H., “Explorer of the Universe,” AIP (1994).
[3] ten Brummelaar et al. ApJ 628, 453–465 (July 2005).
[4] McAlister, H. A. and McAlister, S. J., “The 2009 Station Fire Threat to Mount Wilson Observatory,” Amazon (2019).
[5] Gies et al. (SPIE) Conference Series 13095, 1309502 (Aug. 2024).
[6] Elliott et al. PASA 41, e043 (Sept. 2024).
[7] Balmer et al. ApJ 1001, L26 (Apr. 2026).
[8] Gardner et al. AJ 171, 30 (Jan. 2026).
[9] Ertel et al. PASP 137, 031001 (Mar. 2025).
[10] Evans et al. ApJ 971, 190 (Aug. 2024).
[11] Evans et al. ApJ 972, 145 (Sept. 2024).
[12] Gallenne et al. A&A 693, A111 (Jan. 2025).
[13] Chowhan et al. MNRAS 548, stag719 (May 2026).
[14] Setterholm et al. AJ 169, 318 (June 2025).
[15] Ibrahim et al. ApJ 947, 68 (Apr. 2023).
[16] Ibrahim et al. ApJ 998, 10 (Feb. 2026).
[17] Codron et al. MNRAS 541, 1600–1612 (Aug. 2025).
[18] Rivinius et al. A&A 694, A172 (Feb. 2025).
[19] Anugu et al. ApJ 973, L5 (Sept. 2024).
[20] Anugu et al. ApJ 974, 113 (Oct. 2024).
[21] Mobeen et al. A&A 686, A260 (June 2024).
[22] Aydi et al. Nature Astronomy 10, 271–280 (Feb. 2026).
[23] De Furio et al. ApJ 990, 54 (Sept. 2025).
[24] Danner et al. ApJ 988, 113 (July 2025).
[25] Torres et al. ApJ 990, 107 (Sept. 2025).
[26] Torres et al. ApJ 971, 31 (Aug. 2024).
References
[27] Richardson et al. ApJ 977, 78 (Dec. 2024).
[28] Lau et al. ApJ 963, 127 (Mar. 2024).
[29] Holdsworth et al. ApJ 977, 185 (Dec. 2024).
[30] Shepard et al. ApJ 977, 236 (Dec. 2024).
[31] Torres et al. ApJ 977, 43 (Dec. 2024)
[32] Anugu et al. JATIS 12, 015008 (Jan. 2026).
[33] Shuai et al. AJ 170, 344 (Dec. 2025).
[34] Anugu et al. AJ 171, 253 (Apr. 2026).
[35] Magri et al. MNRAS 536, 266–273 (Jan. 2025).
[36] Roettenbacher et al. Nature 533, 217–220 (May 2016).
[37] Dholakia et al. PASP 138, 054504 (May 2026).
[38] Mourard et al. A&A , submitted (2026).
[39] Anugu et al. AJ 160, 158 (Oct. 2020).
[40] Setterholm et al. JATIS 9, 025006 (Apr. 2023).
[41] Mourard et al. (SPIE) Conference Series 13095, 1309503 (Aug. 2024).
[42] Lanthermann et al. (SPIE) Conference Series 12183, 121830N (Aug. 2022).
[43] Lanthermann et al. (SPIE) Conference Series 13095, 1309505 (Aug. 2024).
[44] Anugu et al. (SPIE) Conference Series 13095, 130951B
(Aug. 2024).
[45] du Foresto et al. SPIE (2003).
[46] Lhomé et al. SPIE (2012).
[47] Scott et al. JATIS 02(02), 1340005 (2013).
[48] Scott et al. SPIE (2014).
[49] Siliprandi et al. Appl. Opt. 63, 159–166 (Jan 2024).
[50] Gies et al. [Bulletin of the American Astronomical Society], 51, 226 (Sept. 2019).
[51] Rajagopal et al. (SPIE) Conference Series 13095, 130951N (Aug. 2024).
[52] Mourard et al. A & A (2026), accepted
backup slides
Binary and Multiple Star Systems
Pleides member star, Atlas: orbit, mass, and rotational distortion of evolved primary Torres+2025
interferometry + spectroscopy of 6 solar-mass binaries in the Hyades cluster Torres+2025
Interferometric Methods
α Psc → hierarchical triple system
starspot locations on rotating stars using spherical harmonics
open-access code harmonix → reconstruct the intensity map based upon a simulation of observations Dholakia&Pope2026
Binary and Multiple Stars
Torres+2025 binary star Atlas, in the Pleiades cluster, age = 104 Myr
→ Rotational distortion of evolved primary
Relative orbit of companion to Atlas
Image Reconstruction of AZ Cyg
Norris et al. (2021)
Model Simulation
Chiavassa et al. (2010)
Giant star surfaces
These "closure phases" also yield information about source symmetry
Combine the phases measured in a closed triangle of three telescopes in a way that cancels out the atmospheric turbulence.
symmetry
Spectrally dispersed fringes produce differential visibilities and differential phases
Differential Vis and Differential Phases
Star + disk.
Exoplanet Systems
Gardner+2026 searched for the NIR signal of the hot Jupiter planet orbiting ups Andromeda
→ may indicate that the NIR flux is lower than predicted.
Ashley Elliott developed the RADPy code
→ reliable angular diameters of stars from CHARA observations
51 Eridani system
PARSEC evolutionary models
→ stellar mass and age, & a planetary mass of 4MJup
Stellar Pulsations
Evans+2024 investigated the mass of Polaris
CHARA observations made around periastron of a faint companion (2016 - 2021)
radial velocity + angular position measurement → 29.4 yr orbit + Gaia distance → Cepheid mass of 5.13 ± 0.28M⊙
similar analysis of the Cepheid AW Per
Relative orbit of Polaris companion from multiple observations
False color image of Polaris in H
Chowhan+2026 PAVO observations of the “secondary red clump” star κ Cyg that exhibits solar-like oscillations
→ mismatch - incomplete treatment of convective boundary mixing in the interior models
Gallenne+2025 triple system Cepheid SU Cyg
→ revisions to the model tracks are needed.
Stellar Pulsations II
Bras 2026 Cepheid η Aql
→ physical model of the center-to-limb intensity variations may be incomplete
Circumstellar Environments
Setterholm+2025 evolution of inner disk of Herbig Ae star HD 163296 - MIRC-X and VLTI PIONIER
> Keplerian motion at that separation
→ might be related to a tidal wake from wider proto-planet
Ibrahim+2026 H and K-band survey of 17 Herbig Be stars
→ binary disk system
Rivinius+2025 spectroscopic survey of Be stars in the post-mass transfer stage before the donor star shrinks to subdwarf
→ the smallest orbit yet resolved with the CHARA Array.
Circumstellar Environments II
hypergiant star RW Per during and after the Great Dimming
hypergiant star ρ Cas20, R = 3 AU.
→ latter range contains many CO lines, add to the overall opacity and shifts line forming region to higher in the atmosphere
Codron+2025 disk structure around T Tauri HD 143006
→ no inner binary companion is detected, so the origin of the misalignment remains a mystery
Circumstellar Environments III
2002: luminous red nova V838 Mon erupts:
high mass star + low mass companion merger → dust outflow enshrouding
Aydi et al. 2025 ToO observations with MIRC-X of 2 novae explosions in 2021
interferometric imaging + contemporary spectroscopy + high E γ-ray measurements Fermi fast nova V1674 Her
→ thermonuclear explosion on WD → fast bipolar outflow + slow equatorial expansion
slow nova V1405 Cas
→ outflow concentrated in the orbital plane and that appears smaller as the net optical depth decreases with expansion and the inner regions are revealed.
→ merger led to jet formation → bipolar structure of the dust emission
The cool hypergiant star RW Cep experienced a Great Dimming event in 2022:
Patchy appearance results from dust created by a huge ejection from the star
Illustration credit: NASA, ESA, and E. Wheatley (STScI)
Anugu and colleagues are continuing to monitor the star with CHARA to explore how the surface appearance changes as the star brightens again.
What causes 1.2 mag
drop in V-band flux?
Binary and Multiple Stars
Torres+2025 binary star Atlas, in the Pleiades cluster, age = 104 Myr
→ Rotational distortion of evolved primary
Mass - abs mag for Hyades cluster members
inset - shows how the PARSEC code tends to overestimate the V fluxes
Relative orbit of companion to Atlas
Torres+2024 interferometry + spectroscopy of 6 solar-mass binaries in the Hyades cluster
→ perhaps due to some missing component of opacity code calculation
"A gain of a single magnitude doubles the available sample of AGN."
7T Imaging improvements
The RECONS 25 Parsec Database
animation: Adric Riedel
20pc sample → 600 M dwarfs
Image an exoplanet during transit
New improvements
student Noy Hakobyan (UC Irvine)
AO Board (AOB) / Telescope Manager (TEMA) upgrades
1100m
600m
~17m
S3
S4
W5
Max spatial resolution
• 0.06 mas at R (650 nm)
• 0.16 mas at H (1.67 μm)
• 0.20 mas at K (2.13 μm)
20 to 1100m
The full Michelson Array would offer 12 total positions, creating 66 possible baselines.
PSAUM → r0, t0, isoplanetism, and isopistonic angle, and index of scintillation
PSAUM (Polar inStrument for Atmospheric tUrbulence Monitoring)