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Active Optics system for the ASTRI-2M prototype for the Cherenkov Telescope Array
Daniele Gardiol INAF – Osservatorio Astrofisico di Torino on behalf of the ASTRI Collaboration and the CTA consortium Daniele Gardiol – SPIE Advanced Telescopes and Instrumentation 2014, Montréal, Quebéc, Canada, June 23rd
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Gerardo Capobianco, Daniele Gardiol,
Active Optics team: Gerardo Capobianco, Daniele Gardiol, Davide Loreggia, Federico Russo, Antonio Volpicelli INAF – Osservatorio Astrofisico di Torino Daniela Fantinel, Enrico Giro, Luigi Lessio, Gabriele Rodeghiero INAF – Osservatorio Astronomico di Padova Daniele Gardiol – SPIE Advanced Telescopes and Instrumentation 2014, Montréal, Quebéc, Canada, June 23rd
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Overview of the talk Introduction: CTA (Cherenkov Telescope Array) and ASTRI (italian acronym…) Active Optics system of the ASTRI SST-2M prototype Kinematic model and performance prediction Active Optics system calibration Conclusions Daniele Gardiol – SPIE Advanced Telescopes and Instrumentation 2014, Montréal, Quebéc, Canada, June 23rd 3 3
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Cherenkov Telescope Array in brief
Introduction Cherenkov Telescope Array in brief Cherenkov Telescope Array is an initiative to build the next generation ground- based very high energy gamma-ray instrument LST (low energy): few 24 metre-class FoV ~ 4-5 degrees MST (medium energy range), from around 100 GeV to 1 TeV 10-12 metre-class FoV ~ 6-8 degrees. SST (high energy): a lot of 4-6 metre class FoV ~ 10 degrees. Daniele Gardiol – SPIE Advanced Telescopes and Instrumentation 2014, Montréal, Quebéc, Canada, June 23rd 4 4
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Italy within CTA: ASTRI
Introduction Italy within CTA: ASTRI ASTRI main goal is the production, within the CTA framework, of: an end-to-end prototype of the CTA SST to be placed and tested in Serra La Nave (mount Etna, Sicily), end 2014 a SST mini-array to be placed at the chosen CTA site, 2016 12 INAF Institutions IASF Milano, IASF Bologna, IASF Palermo, INAF HQ Roma, OA Brera, OA Torino, OA Padova, OA Bologna, OA Arcetri (Firenze), OA Roma, OA Capodimonte (Napoli), OA Catania 2 University partners Padova, Perugia Talk on ASTRI mini-array by G.Pareschi today at 11:40 (room 517D) Daniele Gardiol – SPIE Advanced Telescopes and Instrumentation 2014, Montréal, Quebéc, Canada, June 23rd 5 5
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ASTRI SST-2M The Prototype monolithic 1.8 m
Secondary mirror monolithic 1.8 m Telescope dual-mirror Schwarzschild- Couder FoV = 9.6° EFL = 2150 mm Primary mirror segmented 4.3 m 18 hex elements 850 mm side-to-side Focal plane camera compact (50x50x50 cm3) based on Si-PMs sensors. Daniele Gardiol – SPIE Advanced Telescopes and Instrumentation 2014, Montréal, Quebéc, Canada, June 23rd
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ASTRI SST-2M The Prototype monolithic 1.8 m
Secondary mirror monolithic 1.8 m Telescope dual-mirror Schwarzschild- Couder FoV = 9.6° EFL = 2150 mm Primary mirror segmented 4.3 m 18 hex elements 850 mm side-to-side Talk on structure and mirrors manufacturing by R.Canestrari today at 11:20 (room 517D) Focal plane camera compact (50x50x50 cm3) based on Si-PMs sensors. Poster on optics characterization and alignment by E.Giro et al. Wednesday from 18:00 to 20:00 (room 520D) Talk on ASTRI camera by O.Catalano was yesterday… Poster on SiPM detectors by G.Bonanno et al. this afternoon at 17:30 (room 516) Daniele Gardiol – SPIE Advanced Telescopes and Instrumentation 2014, Montréal, Quebéc, Canada, June 23rd
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Primary Mirror active supports
Active Optics system Primary Mirror active supports M1 segment support One fixed point Two axial actuators Total stroke > 10 mm Positioning accuracy < 3µm Prototype for lab test Daniele Gardiol – SPIE Advanced Telescopes and Instrumentation 2014, Montréal, Quebéc, Canada, June 23rd 8 8
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Secondary Mirror active support
Active Optics system Secondary Mirror active support M2 active support Three axial actuators Tilt + Focus Whiffletrees to share load Total stroke ~ 15 mm Daniele Gardiol – SPIE Advanced Telescopes and Instrumentation 2014, Montréal, Quebéc, Canada, June 23rd 9 9
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Alignment tracking system
Active Optics system Alignment tracking system Each M1 segment is equipped with a laser which beam follows the optical path of the telescope Spot position is tracked via two CCDs located at the camera edges and provides feedback on mirror tilt Daniele Gardiol – SPIE Advanced Telescopes and Instrumentation 2014, Montréal, Quebéc, Canada, June 23rd 10 10
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Active Mirror Control Unit
Active Optics system Active Mirror Control Unit Active Mirror Control Unit (dedicated PC) Telescope Control System OPC-UA Client Telescope Control Unit Twincat 3 (Beckhoff) Main OPC-UA Server DB KM ATS M1 M2 ADS Engineering interface Poster on Telescope Control Unit by E.Antolini et al. (room 516) Daniele Gardiol – SPIE Advanced Telescopes and Instrumentation 2014, Montréal, Quebéc, Canada, June 23rd 11 11
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Kinematic model Forward Analysis Segment model Geometrical model
Optical model Behaviour prediction Daniele Gardiol – SPIE Advanced Telescopes and Instrumentation 2014, Montréal, Quebéc, Canada, June 23rd 12 12
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Kinematic model Segment model 13 13
Daniele Gardiol – SPIE Advanced Telescopes and Instrumentation 2014, Montréal, Quebéc, Canada, June 23rd 13 13
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Kinematic model Geometrical model F 2 1
Provides the mirror position and tilt angles as a function of the actuator axial position for M1 for M2 Daniele Gardiol – SPIE Advanced Telescopes and Instrumentation 2014, Montréal, Quebéc, Canada, June 23rd 14 14
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Optical model - u-type movement
Kinematic model Optical model - u-type movement Δx Δy Inner circle Median circle Outer circle Daniele Gardiol – SPIE Advanced Telescopes and Instrumentation 2014, Montréal, Quebéc, Canada, June 23rd 15 15
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Optical model - v-type movement
Kinematic model Optical model - v-type movement Δx Δy Inner circle Median circle Outer circle Daniele Gardiol – SPIE Advanced Telescopes and Instrumentation 2014, Montréal, Quebéc, Canada, June 23rd 16 16
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Performance prediction vs. calibration
Kinematic model Performance prediction vs. calibration Kynematic Model M1 Comp. inv. function M2 Residual estimate Δx Δy Daniele Gardiol – SPIE Advanced Telescopes and Instrumentation 2014, Montréal, Quebéc, Canada, June 23rd 17 17
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Kinematic model System calibration p1 p2 Seventh order polynomial
Residuals Example: Seventh order polynomial Image shifts up to d= ∆𝑥 + ∆𝑦 <80 mm residuals for whole M1 (18 segments) > 99% of residuals are below the hardware positioning accuracy of actuators Daniele Gardiol – SPIE Advanced Telescopes and Instrumentation 2014, Montréal, Quebéc, Canada, June 23rd 18 18 18
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Conclusions active positioning is performed by means of axial actuators driven by stepper motors an alignment tracking system provides feedback on the mirrors alignment. It will be used also during calibrations can operate in stand alone mode or within the Telescope Control System A complete kinematic model predicts system performance, quantifying non- linearities (dominated by the M1 axial actuator behaviour) A simulation of the calibration procedure shows that it is possible to describe and correct the image shift induced by mirrors tilt over the whole range allowed by the hardware with a seventh order polynomial, being the residuals well below the mechanical accuracy positioning of the actuators Daniele Gardiol – SPIE Advanced Telescopes and Instrumentation 2014, Montréal, Quebéc, Canada, June 23rd 19 19
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Performance prediction
Kinematic model Performance prediction Δy (// El) Δx M1 Focal Plane M2 Δx Δy Daniele Gardiol – SPIE Advanced Telescopes and Instrumentation 2014, Montréal, Quebéc, Canada, June 23rd 20 20
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Polynomial interpolation up to a suitable order
Kinematic model Backward Analysis Kynematic Model (FA) Comp. inv. function Polynomial interpolation up to a suitable order Residual estimate Daniele Gardiol – SPIE Advanced Telescopes and Instrumentation 2014, Montréal, Quebéc, Canada, June 23rd 21 21
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