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Detection and Astrometry of the Ba–Bb Subsystem in α Piscium: First Dual-field Interferometry at the CHARA Array

  • Authors: Narsireddy Anugu, Robert Klement, John D. Monnier, Douglas R. Gies, Gail H. Schaefer, Stefan Kraus, Sebastián Carrazco-Gaxiola, Akshat S. Chaturvedi, Mayra Gutierrez, Becky Flores, Jeremy Jones, Colin Kane, Rainer Köhler, Karolina Kubiak, Olli W. Majoinen, Nicholas J. Scott, Kayvon Sharifi

Narsireddy Anugu et al 2026 The Astronomical Journal 171 .

  • Provider: AAS Journals

Caption: Figure 4.

Schematic optical layout of the CHARA dual-field mode. For clarity, we show only two telescopes and suppress the second-telescope AO/CHARA delay-line path. The ∼5″ field is acquired at the telescopes; visible light feeds the AO/Wavefront Sensor via the telescope dichroic (TelDic), while the IR beam is relayed to the beam-combiner lab and main CHARA delay lines. The full field is imaged by STST, then a small pickoff (STST-BS) sends light to MIRC-X (H band) and MYSTIC (K band). MIRC-X fringe-tracks on component A and drives the main delay lines; MYSTIC records science fringes on component B (see Figure 5). The instrument DDLs apply the additional differential delay B · θ between A and B, shifting the science beam relative to the fringe-tracking path. The fiber injection is set from the STST astrometric positions. Unlike VLTI/GRAVITY, CHARA does not have an internal metrology system; differential delays are inferred from DDL telemetry and A–B/B–A swap tests. This schematic illustrates the functional architecture rather than the full optical complexity of the six-telescope CHARA beam train.

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