MAORY design trade-off study: tomography dimensioning

Similar documents
MAORY (Multi conjugate Adaptive Optics RelaY) for E-ELT. Paolo Ciliegi. On behalf of the MAORY Consortium

The MAORY Multi-Conjugate Adaptive Optics module Emiliano Diolaiti Istituto Nazionale di Astrofisica

T-REX Operating Unit 3

Modelling the multi-conjugate adaptive optics system of the European Extremely Large Telescope

Adaptive Optics for the Giant Magellan Telescope. Marcos van Dam Flat Wavefronts, Christchurch, New Zealand

1. INTRODUCTION ABSTRACT

Telescopes & Adaptive Optics. Roberto Ragazzoni INAF Astronomical Observatory of Padova

Ten years of

Field Tests of elongated Sodium LGS wave-front sensing for the E-ELT

Roberto Ragazzoni INAF Padova (Italy) Munich, June 8th, 2009

MCAO for the European Solar Telescope: first results

Raven, a Multi-Object Adaptive Optics technology and science demonstrator

Adaptive Optics Status & Roadmap. Norbert Hubin Adaptive Optics Department European Southern Observatory November 2007

A novel laser guide star: Projected Pupil Plane Pattern

EPICS: A planet hunter for the European ELT

Presented by B. Neichel. Wide-Field Adaptive Optics for ground based telescopes: First science results and new challenges

Subaru Next Generation Wide Field AO: Ground Layer AO Simulation

Point spread function reconstruction at W.M. Keck Observatory : progress and beyond

Analysis of the Sequence Of Phase Correction in Multiconjugate Adaptive Optics

How to break the FoV versus thickness rule in MCAO

Sky Projected Shack-Hartmann Laser Guide Star

FP7-OPTICON PSF reconstruction meeting, Marseille January 14

Laboratory Experiments of Laser Tomographic Adaptive Optics at Visible Wavelengths on a 10-meter Telescope

Ground-Layer Adaptive Optics Christoph Baranec (IfA, U. Hawai`i)

Subaru GLAO Simulation. Shin Oya (Subaru Telescope) Hilo

The Adaptive Optics modes for HARMONI From Classical to Laser Assisted Tomographic AO

An Introduction to. Adaptive Optics. Presented by. Julian C. Christou Gemini Observatory

Subaru GLAO Simulation. Shin Oya (Subaru Telescope) Hilo

Lecture 15 The applications of tomography: LTAO, MCAO, MOAO, GLAO

Tomography for Raven, a Multi-Object Adaptive Optics Science and Technology Demonstrator. Kate Jackson. Carlos Correia

Preparing staff for ELT science operations activities

Performance Modeling of a Wide Field Ground Layer Adaptive Optics System

EAGLE multi-object AO concept study for the E-ELT

Comparing the performance of open loop centroiding techniques in the Raven MOAO system

Atmospheric Turbulence and its Influence on Adaptive Optics. Mike Campbell 23rd March 2009

T-REX. Renato Falomo. T-REX meeting, Bologna 14 Jan 2013

A FREQUENCY DEPENDENT PRECONDITIONED WAVELET METHOD FOR ATMOSPHERIC TOMOGRAPHY

arxiv: v2 [astro-ph.im] 15 Mar 2016

DRM Update Joe Liske

PSFs for Laser Guide Star Tomographic Adaptive Optics Systems

Sky demonstration of potential for ground layer adaptive optics correction

Efficient control schemes with limited computation complexity for Tomographic AO systems on VLTs and ELTs

Instrumentation for The European Extremely Large Telescope Science and Technology with E-ELT Erice, October 2015

Shack-Hartmann wavefront sensor sensitivity loss factor estimation in partial correction regime

Experimental results of tomographic reconstruction on ONERA laboratory MCAO bench

New challenges for adaptive optics: the OWL 1OOm telescope

AO system Design: Astronomy Olivier Guyon (University of Arizona / Subaru Telescope)

Performance Modeling for the RAVEN Multi-Object Adaptive Optics Demonstrator

- The AO modes for HARMONI - From Classical to Laser-assisted tomographic AO systems

Achieving high resolution

Adaptive Optics Systems for the Thirty Mirror Telescope

Layer Oriented Multi-Conjugate Adaptive Optics systems: Performance analysis by numerical simulations

Instruments for ESO s Extremely Large Telescope

Wavefront Sensing in Astronomy

Imaging with Micado at the E-ELT. WORKSHOP: Imaging at the E-ELT

Science with Micado. the high resolution camera for the E-ELT Renato Falomo. INAF Observatory of Padova, Italy. 25 February IASF, Milano

Visible near-diffraction-limited lucky imaging with full-sky laser-assisted adaptive optics

NEXT GENERATION ADAPTIVE OPTICS: SYSTEM DESIGN MANUAL

First evidence of the finite horizontal extent of the optical turbulence layers. Implications for new adaptive optics techniques

The AO and MCAO for the 4m European Solar Telescope

Weston, ACT 2611, Australia; ABSTRACT

Characterising daytime atmospheric conditions on La Palma

Development of Field of View for Ground-based Optical Telescopes in Adaptive Optics Xiaochun Zhong 1, 2, a, Shujuan Wang 2, b, Zhiliang Huang 3, c

NB: from now on we concentrate on seeing, as scintillation for large telescopes is unimportant

Monitoring Site Parameters for AO

Astronomie et astrophysique pour physiciens CUSO 2015

Telescope Project Development Seminar

Adaptive Optics. Dave Andersen NRC Herzberg.

MAORY Multiconjugate Adaptive Optics RelaY for E-ELT

C 2 n. profilometry from Shack-Hartmann data: model and experiment. 1 Introduction. 2 Problem statement with SH slope and scintillation correlations

Christian Marois Lawrence Livermore National Laboratory

CURRENT STATUS OF RAVEN, A MOAO SCIENCE DEMONSTRATOR FOR SUBARU

ABSTRACT 1. INTRODUCTION

CHARA Collaboration Year-Eight Science Review. VLTI update. F. Delplancke

arxiv: v1 [astro-ph.im] 1 Aug 2016

Studies for the first generation of instruments for the European ELT

On-sky MOAO performance evaluation of RAVEN

Reconstruction and Control Laws for Multi-conjugate Adaptive Optics in Astronomy

arxiv: v1 [astro-ph.im] 12 Jul 2018

E-ELT Programme; ESO Instrumentation Project Office Ground-based Instrumentation for VLT, VLTI and E-ELT

E-ELT Spectroscopic ETC: Detailed Description

A STUDY OF PYRAMID WFS BEHAVIOUR UNDER IMPERFECT ILLUMINATION

Curriculum Vitae et Studiorum LAURA SCHREIBER

PRELIMINARY PERFORMANCE ANALYSIS OF THE MULTI-CONJUGATE AO SYSTEM OF THE EUROPEAN SOLAR TELESCOPE

NA LASER GUIDE STAR AO WITH DYNAMICAL REFOCUS

arxiv: v2 [astro-ph.im] 20 Oct 2016

GEMS: FROM THE ON-SKY EXPERIMENTAL SYSTEM TO SCIENCE OPERATION: THE AO POINT OF VIEW.

Giant Magellan Telescope

Introduction to Adaptive Optics. Tim Morris

Error Budgets, and Introduction to Class Projects. Lecture 6, ASTR 289

A NEW METHOD FOR ADAPTIVE OPTICS POINT SPREAD FUNCTION RECONSTRUCTION

E-ELT PROGRAMME THE E-ELT DESIGN REFERENCE MISSION: TECHNICAL DATA USED FOR SIMULATIONS. E-TRE-ESO Issue June 2010

NGAO trade study report: LOWFS architecture KAON 487 (WBS )

Synergies between and E-ELT

Astronomical Observing Techniques 2017 Lecture 13: Twinkle, twinkle star... No more!

Stereo-SCIDAR: Instrument and First Commissioning Results

Early closed-loop results from the MMT's multi-laser guide star adaptive optics system

The Flexible Adaptive Optics Concept

Technology Developments for ESO at the IAC

Astronomical Observing Techniques Lecture 13: Adap<ve Op<cs

Transcription:

MAORY design trade-off study: tomography dimensioning Sylvain Oberti, Miska Le Louarn ESO Garching Emiliano Diolaiti, Carmelo Arcidiacono, Laura Schreiber, Matteo Lombini INAF Bologna and the rest of the MAORY consortium

Multi-conjugate Adaptive Optics RelaY for the E-ELT MAORY serves MICADO + future second port INS (TBD) Location, date 2

Outline: phase B design trade-off 1- Analysis of dimensioning parameters constrained by tomographic and generalized fitting error Number of post-focal DMs conjugated in altitude DM pitch DM altitudes LGS asterism angle Number of LGS LGS and NGS asterism geometry - not shown in this talk under some constraints Seeing Cn2 profile Zenith distance Telescope phase 1 / phase 2 Number of LGSs: 4/6 M1 central obstruction: 28%/57% 3

Driver: MAORY main specifications Performance in best conditions Q1 seeing (0.234 m) and wind, as close to zenith as possible Over 20 FoV SR > 50% @ 2.2 microns (goal 60%) Sky coverage requirement not applicable Performance in median conditions median seeing (0.157 m) and wind, as close to zenith as possible Over 1 FoV SR > 30% @ 2.2 microns (goal 50% @ 2 microns) Performance in sub optimal conditions Q3 seeing (0.139 m) and wind, zenith distance 30 degrees Over 2 FoV SR > 15% @ 2.2 microns (goal 30%) SR uniformity < 10% absolute PTV across FoV of interest Sky coverage > 50% 4

OCTOPUS end-to-end simulation Simulated MCAO WFE terms Generalized fitting Spatial aliasing Temporal error LGS WFS noise NGS WFS noise Tomographic error Command computation: high flux and no spot elongation high flux cone effect and anisoplanatism but optimal reconstruction of 35 layers Tomographic reconstruction to estimate the multi layer turbulent phase: FRIM3D/POLC with perfect priors on Cn 2 profile Projection of the estimated 3D phase onto the DMs space. The projection is optimized on a specific FoV No other error budget term 5

Typical simulated FoV MICADO small field 20 x20 MICADO large field 53 x53 6

Cn 2 profiles + other profiles measured by stereo scidar

Gen. fitting: N DMs and pitch r 0 =0.129 m, Z=30º 2 post-focal DMs: performance flat for pitch < 1.5 m 1 post-focal DM: performance flat for pitch < 2 m Strong impact from Cn2 profile 8

Benefit 2 vs. 1 post-focal DM(s) K band: 2.2 µm r 0 =0.129 m, Z=30º 2 post-focal DMs provide performance improvement of up to 25% in the science field and 100% in the technical field in K band, 250% in J band 2 post-focal DMs desirable to increase sky coverage

Benefit 2 vs. 1 post-focal DM(s) 2 post-focal DMs improve tolerance to Cn2 profile variation 10

E-ELT phase 1 / phase 2 K band M1 doughnut impact on Sr is marginal. How about NGS sky coverage? Significant impact 6 LGSs 4 LGSs E-ELT phase 1: limited by tomographic error DM pitch irrelevant 6 LGSs enable benefit from 2 post-focal DMs and finer pitch Photon noise σ 2 x3.8 long axis K band: 2.2 µm r 0 =0.129 m, Z=30º C n2 : Profile 1

E-ELT phase 1 / phase 2 J band M1 doughnut impact on Sr is not significant. How about NGS sky coverage? Dramatic impact 6 LGSs 4 LGSs Lower wavelength performance pushes for: 6 LGSs 2 post-focal DMs finer DM pitch K band: 2.2 µm r 0 =0.129 m, Z=30º C n2 : Profile 1 Photon noise σ 2 x3.8 long axis

Post-focal DM altitude: single DM K band: 2.2 µm r 0 =0.129 m, Z=30º C n2 : Profile 1 1 post-focal DM: conjugation altitude matters and should be > 14 km The conjugation altitude should be higher to cope with larger airmass cases 13

Post-focal DM altitude: 2 DMs case Results confirmed by Cn 2 sensitivity study Performance insensitive to DM1 altitude DM2 optimal altitude naturally increases with airmass 16 km conjugation is a good trade-off 16 km is also close to optimal for a single post-focal DM Upgradability 14

Sensitivity Cn 2 profile: DM2 altitude DM2 altitude should obviously be increased at larger airmass Dependency on profile is not significant Again 16 km conjugation looks like a good compromise 15

Sensitivity Cn 2 profile: DM1 altitude DM1 altitude has a weak influence No clear dependency on Cn2 profile The opto-mechanical design should drive the DM1 altitude 16

LGS asterism angle full field optim K band: 2.2 µm r 0 =0.129 m, Z=30º C n2 : Profile 1 1 radius 45 radius Tomography reconstruction maximizes performance in full field here Closer LGSs improve Sr on axis, decrease uniformity across the MICADO field and decrease the Sr in the technical field Trade-off between 45 and 1 radii other FoV optimization to check 17

LGS angle projection optimization K band: 2.2 µm, r 0 =0.157 m, C n2 : Profile1 Tomography reconstruction maximizes performance in 3 different FoVs with NGS @ 70 off axis Maximum and average Sr in MICADO field highest for LGS @ 45 off axis Average performance in 2 FoV highest for LGS @ 1 off axis Baseline: 45 radius 18

Ultimate performance in 20 square Best performance on axis (LTAO with on axis NGS) is achieved with 20 radius @ Z=60 NGS cannot be closer than 30 radius without vignetting the science FoV Confirmation that a fixed 45 radius is almost optimal for MICADO at any airmass for both small field and wide field: one single asterism configuration less complexity 19

Conclusions on design trade-off 2 post-focal DMs (baseline: 1) are desirable in order to enhance: Performance in the technical field sky coverage and robustness (acquisition) Performance in the blue for NGS sky coverage and MICADO performance Robustness to Cn2 profile variation and zenith distance DM pitch between 2m and 1.5m better for worse seeing and with 2 DMs Post-focal DMs altitude: 4-6 and 16 km to be robust to larger airmass and accommodate 2 post-focal DMs later LGS asterism angle: fixed @ 45 radius + optimization of tomography projection depending on FoV of interest E-ELT phase 1 / phase 2: M1 doughnut main impact on sky coverage and PSF shape: TBC 6 LGSs are highly desirable 20

Thank you for your attention! Location, date 21