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- | ===== Themis Adaptive Optics | ||
- | ** Themis Adaptive Optics (TAO)** is a single conjugate adaptive optics (AO) system with only one **[[themis: | ||
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- | TAO is inserted in the light path after the telescope and the transfer relay optics, between the (intermediate) F2' focus and the F2 focus at the spectrograph entry (Fig. 1). The TAO layout requires two horizontal folds of the beam, then returning it to a vertical path on the same downstream axis (Fig. 2). A beam splitter (with some power) feeding the **[[themis: | ||
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- | Fig.1: Telescope layout showing the TAO instrument between the transfer relay optics and the spectrograph (not shown here) | ||
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- | Fig.2: TAO zemax layout showing the main beam leading to the spectrograph entry, and the wavefront sensor branch, fed through a beam splitter from the main beam. | ||
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- | The field of view of the wavefront sensor, of 11", is a trade-off between a larger fov (for better correlation of solar surface features) and the available processing speed (limiting the amount of pixels to process given our computing power). The deformable mirror specs are also a trade-off that includes the small available physical volume that limits the pupil size to 10-20 mm, the simultaneous needs for large stroke and fast response time to allow only one mirror for both the tip-tilt and the higher order corrections, | ||
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- | Fig.3: TAO geometry showing 97 actuators on a 11 × 11 grid, and 76 subapertures on a 10 × 10 grid. The red circles mark the pupil imprint with its central obscuration, | ||
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- | The combination of DM/ | ||
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- | ====Deformable mirror==== | ||
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- | We are using an [[https:// | ||
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- | Fig.4: The ALPAO DM97-15 in the sunlight. The visible notch in the pupil comes from an inclined guide mirror which is removed when the AO system runs. | ||
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- | This mirror has 97 actuators set on square grid pitched at 1.5mm, and provides 13.5 mm of useful reflective area in factory settings. We did request a custom setup to allow using a 15mm reflective area better suited to our final WFS geometry.\\ | ||
- | A specific challenge we had to figure out immediately has been the flux load on the deformable mirror: one 15 mm pupil receiving the full telescope heat-load has the same kind of concentration of power as our F1 focus (e.g. about 9 times the natural sunlight). While this mirror is used in several other solar telescopes (Hida Observatory DST, VTT at OT ...), none of these are comparable to THEMIS in collecting power. Since 2018 we have not noticed any ageing of the DM reflective part and we have checked that the static and dynamic DM specs are not changed under that solar flux, confirming this model is suitable for our observations. | ||
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- | ====Wavefront sensor==== | ||
- | The wavefront sensor (WFS) is fed from the main beam trough a 92-8 % beam splitter. Space considerations forced us to relocate it outside of the spectrograph enclosure (where is the main path located), so that the WFS bench is setup vertically on an extra optical table hanging on the spectrograph external wall. \\ | ||
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- | The WFS is a classical Shack-Hartmann type using [[https:// | ||
- | The subpupils created at the focus of the microlens array are then scaled and re-imaged over the fast camera/ | ||
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- | Fig.5: TAO WFS being integrated at CRAL | ||
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- | Fig.6: TAO WFS zemax layout | ||
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- | Fig.7: TAO WFS optical bench on the telescope | ||
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- | Our camera is a [[https:// | ||
- | - 68 SUB-IMAGES of 29x29 pixels (11.5x11.5arcsec2) | ||
- | - scale: 0.4 arcsec/ | ||
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- | The WFS can work in several modes : | ||
- | * Solar wavefront sensing (main mode) | ||
- | * F2' pinhole with solar light (soon to become a laser pinhole), for zero reference, interaction matrix and non-common path abberration (NCPA) calibrations. | ||
- | * F1 laser mode (as an alternative to the F2' calibrations) | ||
- | Differences in flux between these modes are handled with a variable neutral density plate.\\ | ||
- | Fig. 8 & 9 show the actual output of the WFS camera. | ||
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- | Fig.8: TAO WFS over solar features | ||
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- | Fig.9: TAO WFS for the 2019 Mercury transit | ||
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- | ====Integration and tests==== | ||
- | Between 2016 and 2018, the complete AO bench has been first integrated and tested at the CRAL in Lyon, in the same configuration as it would be on the telescope, but for the spatial orientation of the whole setup which was horizontal on an optical table at CRAL, while it is vertical in the telescope. The setup included: | ||
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- | * a red laser/ color tunable light source simulator, including a realistic THEMIS telescope pupil | ||
- | * the main TAO path as described above | ||
- | * the wavefront sensor branch fed through a beam splitter, as above | ||
- | * the WFS and field cameras and their computer interfaces | ||
- | * The instrument CPU | ||
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- | Fig.10: TAO in the integration hall at CRAL | ||
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- | Fig.11: TAO@CRAL panoramic full view | ||
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- | ==== Computer and software ==== | ||
- | The wavefront sensing and mirror commanding software runs on a typical high-end desktop PC using a Linux (Mint) kernel 3.19.8-031908-lowlatency x86_64 operating system, and featuring: | ||
- | * Mobo: ASUSTeK model: Z97-A | ||
- | * Quad core Intel Core i7-4790K (-MCP-) cache: 8192 KB clock speed max: 4400 MHz | ||
- | * 16 GB DDR3 DIMM speed: 2400 MHz type | ||
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- | The real-time software is built using a Toolkit for Adaptive Optics developed at CRAL. | ||
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- | ==== To go further ==== | ||
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- | The full technical library is on the [[proj:AO project library| AO project library webpage]]. \\ | ||
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