2006
DOI: 10.1117/12.672032
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Extreme adaptive optics for the Thirty Meter Telescope

Abstract: Direct detection of extrasolar Jovian planets is a major scientific motivation for the construction of future extremely large telescopes such as the Thirty Meter Telescope (TMT). Such detection will require dedicated high-contrast AO systems. Since the properties of Jovian planets and their parent stars vary enormously between different populations, the instrument must be designed to meet specific scientific needs rather than a simple metric such as maximum Strehl ratio. We present a design for such an instrum… Show more

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Cited by 78 publications
(46 citation statements)
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“…Following the method described in the previous two sections, we calculate a J-band ADI rotation time requirement of ∼ 2 minutes and ∼ 10 minutes for a planet at a radial separation from the parent star of 1 ′′ and 0.2 ′′ respectively; here we present the results for the latter. Using the required characteristics of the GMT/TMT/ELT (GMT 2006; Macintosh et al 2006;Kasper et al 2010), we use a residual stellar PSF of 10 −8 at the radial separation of 0.2 ′′ to simulate the very high SNR (on the order of several thousands, using the ELT ETC provided by ESO) J-band lightcurve for model B2 in the lower panel of Figure 8. As was the case for the 8m ExAO systems, the residual stellar PSF is no longer the main culprit for systematic errors.…”
Section: -M Class Telescopes With Next-generation Extreme Ao (30m+ mentioning
confidence: 99%
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“…Following the method described in the previous two sections, we calculate a J-band ADI rotation time requirement of ∼ 2 minutes and ∼ 10 minutes for a planet at a radial separation from the parent star of 1 ′′ and 0.2 ′′ respectively; here we present the results for the latter. Using the required characteristics of the GMT/TMT/ELT (GMT 2006; Macintosh et al 2006;Kasper et al 2010), we use a residual stellar PSF of 10 −8 at the radial separation of 0.2 ′′ to simulate the very high SNR (on the order of several thousands, using the ELT ETC provided by ESO) J-band lightcurve for model B2 in the lower panel of Figure 8. As was the case for the 8m ExAO systems, the residual stellar PSF is no longer the main culprit for systematic errors.…”
Section: -M Class Telescopes With Next-generation Extreme Ao (30m+ mentioning
confidence: 99%
“…To estimate the achievable photometric accuracy of the different instruments we rely on the residual radial contrast curves provided by the instrument teams: VLT/NACO at 4 µm (Kasper et al 2007(Kasper et al , 2009), VLT/SPHERE in J-band (Vigan et al 2010;Mesa et al 2011), Gemini/GPI in H-band ), TMT/PFI in H-band (Macintosh et al 2006), ELT/EPICS in J-band and JWST/NIRCAM in K-band (Green et al 2005). All contrast limits are for coronographic images.…”
Section: Targets and Instrumentsmentioning
confidence: 99%
“…ELTs will have to support a substantially heavier secondary than 8 meter class observatories do, and over larger lengths: as a consequence the relative area covered by the secondary support will increase by a factor of 10 (30 cm wide spiders, occupying ∼ 3% of the pupil diameter in the case of TMT). This will degrade the contrast of coronagraphs only designed for circularly obscured geometries by a factor ∼ 100, when the actual envisioned contrast for an ELT exo-planet imager can be as low as ∼ 10 −8 (Macintosh et al 2006). While the tradeoffs associated with minimization of spider width in the space-based case have yet to be explored, secondary support structures will certainly hamper the contrast depth of coronagraphic instruments of such observatories at levels that are well above the 10 10 contrast requirement.…”
Section: Introductionmentioning
confidence: 99%
“…1. As a consequence, a wavefront control system composed of two sequential Deformable Mirrors is currently the baseline architecture of currently envisioned coronagraphic space-based instruments Krist et al 2011) and ELT planet imagers (Macintosh et al 2006). One can thus naturally be motivated to investigate if such wavefront control systems can be used to cancel the light diffracted by secondary supports and segments in large telescopes, since such structures are amplitude errors, albeit large amplitude errors.…”
Section: Introductionmentioning
confidence: 99%
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