Visible Nulling Coronagraph

Similar documents
Predicting the Performance of Space Coronagraphs. John Krist (JPL) 17 August st International Vortex Workshop

Opportunities and Challenges with Coronagraphy on WFIRST/AFTA

Matthew R. Bolcar NASA GSFC

PREPARED BY: I. Miller DATE: 2004 May 23 CO-OWNERS REVISED DATE OF ISSUE/CHANGED PAGES

Bruce Macintosh for the GPI team Presented at the Spirit of Lyot conference June 7, 2007

Laboratory Experiment of a High-contrast Imaging Coronagraph with. New Step-transmission Filters

Design and test of a high-contrast imaging coronagraph based on two. 50-step transmission filters

PREPARED BY: I. Miller DATE: 2004 May 23 CO-OWNERS REVISED DATE OF ISSUE/CHANGED PAGES

HC(ST) 2 : The High Contrast Spectroscopy Testbed for Segmented Telescopes

PREPARED BY: I. Miller DATE: 2004 May 23 CO-OWNERS REVISED DATE OF ISSUE/CHANGED PAGES

GPI INSTRUMENT PAGES

BEAM HALO OBSERVATION BY CORONAGRAPH

Speckle Phase Sensing in Vortex Coronagraphy

Recent Progress in Vector Vortex Coronagraphy

Focal Plane and non-linear Curvature Wavefront Sensing for High Contrast Coronagraphic Adaptive Optics Imaging

NGAO NGS WFS design review

CHARA AO Calibration Process

Non-adaptive Wavefront Control

Towards Contrast for Terrestrial Exoplanet Detection:

AgilOptics mirrors increase coupling efficiency into a 4 µm diameter fiber by 750%.

High-contrast imaging with E-ELT/HARMONI

Ultra-Flat Tip-Tilt-Piston MEMS Deformable Mirror

Wavefront control for highcontrast

Large-Actuator-Count MEMS. Deformable Mirror Development

arxiv: v2 [astro-ph] 7 Aug 2008

NIRCam Optical Analysis

ADVANCED OPTICS LAB -ECEN Basic Skills Lab

Optical Design. Instrument concept Foreoptics and slit viewer Spectrograph Alignment plan 3/29/13

Light gathering Power: Magnification with eyepiece:

High contrast imaging lab

Use of Computer Generated Holograms for Testing Aspheric Optics

Technology Days GSFC Optics Technologies. Dr. Petar Arsenovic

The predicted performance of the ACS coronagraph

ADVANCED OPTICS LAB -ECEN 5606

Adaptive Optics for LIGO

Apodized phase plates & Shaped pupils

Development of a Low-order Adaptive Optics System at Udaipur Solar Observatory

Department of Mechanical and Aerospace Engineering, Princeton University Department of Astrophysical Sciences, Princeton University ABSTRACT

MODULAR ADAPTIVE OPTICS TESTBED FOR THE NPOI

Dynamic Phase-Shifting Electronic Speckle Pattern Interferometer

Experiment 1: Fraunhofer Diffraction of Light by a Single Slit

System Architecting: Defining Optical and Mechanical Tolerances from an Error Budget

Integrated Micro Machines Inc.

arxiv: v1 [astro-ph.im] 15 Aug 2012

Subject headings: turbulence -- atmospheric effects --techniques: interferometric -- techniques: image processing

3.0 Alignment Equipment and Diagnostic Tools:

Starshade Technology Development Status

An overview of WFIRST-AFTA coronagraph modelling

Design of the cryo-optical test of the Planck reflectors

Lecture 2: Geometrical Optics. Geometrical Approximation. Lenses. Mirrors. Optical Systems. Images and Pupils. Aberrations.

Submillimeter Pupil-Plane Wavefront Sensing

PHY 431 Homework Set #5 Due Nov. 20 at the start of class

DESIGN NOTE: DIFFRACTION EFFECTS

Inverted-COR: Inverted-Occultation Coronagraph for Solar Orbiter

Exoplanet Imaging with the Giant Magellan Telescope

In order to get an estimate of the magnitude limits of the CHARA Array, a spread sheet

Lecture 7: Op,cal Design. Christoph U. Keller

PhD Defense. Low-order wavefront control and calibration for phase-mask coronagraphs. Garima Singh

Vibration-compensated interferometer for measuring cryogenic mirrors

Supplementary Materials

Lecture 2: Geometrical Optics. Geometrical Approximation. Lenses. Mirrors. Optical Systems. Images and Pupils. Aberrations.

SELECTION GUIDE MULTIPLE-ORDER QUARTZ WAVEPLATES ZERO-ORDER QUARTZ WAVEPLATES DUAL-WAVELENGTH WAVEPLATES... 85

NIRCam optical calibration sources

2.2 Wavefront Sensor Design. Lauren H. Schatz, Oli Durney, Jared Males

The Extreme Adaptive Optics test bench at CRAL

FRAUNHOFER AND FRESNEL DIFFRACTION IN ONE DIMENSION

EE119 Introduction to Optical Engineering Spring 2003 Final Exam. Name:

J. C. Wyant Fall, 2012 Optics Optical Testing and Testing Instrumentation

Simulations of the STIS CCD Clear Imaging Mode PSF

Anti-reflection Coatings

Ultralight Weight Optical Systems using Nano-Layered Synthesized Materials

Practical Flatness Tech Note

The 20/20 telescope: Concept for a 30 m GSMT

Growing a NASA Sponsored Metrology Project to Serve Many Applications and Industries. James Millerd President, 4D Technology

PYRAMID WAVEFRONT SENSOR PERFORMANCE WITH LASER GUIDE STARS

Reflectors vs. Refractors

Optical Telescope Design Study Results

Why is There a Black Dot when Defocus = 1λ?

arxiv: v1 [astro-ph.im] 6 Nov 2009

Fresnel interferometric Arrays as Imaging interferometers

Breadboard adaptive optical system based on 109-channel PDM: technical passport

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Electrical Engineering and Computer Science

An Achromatic Focal Plane Mask for High-Performance Broadband Coronagraphy

MACH-ZEHNDER WAVEFRONT SENSOR FOR PHASING OF SEGMENTED TELESCOPES

EVALUATION OF ASTROMETRY ERRORS DUE TO THE OPTICAL SURFACE DISTORTIONS IN ADAPTIVE OPTICS SYSTEMS and SCIENCE INSTRUMENTS

Supplementary Figure 1. Effect of the spacer thickness on the resonance properties of the gold and silver metasurface layers.

EXCEDE Technology Milestone #1: Monochromatic Contrast Demonstration

NIRCam Instrument Optics

Characteristics of point-focus Simultaneous Spatial and temporal Focusing (SSTF) as a two-photon excited fluorescence microscopy

Errors Caused by Nearly Parallel Optical Elements in a Laser Fizeau Interferometer Utilizing Strictly Coherent Imaging

Optics for the 90 GHz GBT array

DAVINCI Pupil Mask Size and Pupil Image Quality By Sean Adkins April 29, 2010

Instrument Characteristics

The performance of the CHEOPS On-Ground calibration system

Null Hartmann test for the fabrication of large aspheric surfaces

ECEN. Spectroscopy. Lab 8. copy. constituents HOMEWORK PR. Figure. 1. Layout of. of the

arxiv: v1 [astro-ph.im] 17 Jun 2014

Physics 431 Final Exam Examples (3:00-5:00 pm 12/16/2009) TIME ALLOTTED: 120 MINUTES Name: Signature:

PYRAMID WAVEFRONT SENSING UPDATE FOR MAGAO-X

Observational Astronomy

Transcription:

Brian Hicks 1 Rick Lyon 2 Matt Bolcar 2 Mark Clampin 2 Jeff Bolognese 2 Pete Dogoda 3 Daniel Dworzanski 4 Michael Helmbrecht 5 Corina Koca 2 Udayan Mallik 2 Ian Miller 6 Pete Petrone 3 1 NASA Postdoctoral Program - GSFC 2 Goddard Space Flight Center 3 Sigma Space, Inc. 4 Optimax Systems, Inc. 5 Iris AO, Inc. 6 LightMachinery, Inc. November 12, 2015

Science/Technical Objectives Hicks+, Spirit of Lyot (2015) 1 Provide a coronagraph solution for exoplanet and debris disk discovery and characterization with a future large aperture space telescope 2 Optimize target yield by maximizing throughput 3 Achieve broadband (> 10%) 10 9 raw contrasts at radial separations spanning 2.5 34λ/D 4 Relax telescope stability requirements

VNC narrowband results - TDEM Milestone #1 SPIE Proceedings: Lyon+ (2012) TDEM Milestone Report: Clampin+ (2013) Repeatability and traceability to wavefront control following telescope slew/settle demonstrated with multiple Data Collection Events (DCEs), each starting from scratch over several days

Outline: ongoing & forthcoming VNC development 1) Broadband demo 2) Segmented stimulus 1 + 2 = 3) SAINT

VNC broadband demo - TDEM Milestone #2 From Clampin, Lyon, Petrone, Mallik, Bolcar, Madison, and Helmbrecht, TDEM Milestone #1 Final Report (2013) Same as TDEM # 1, but at 1.0 10 9 over 40 nm FWHM centered on 633 nm: Left: Dark hole region overlay on simulated PSF. Center: control modes are designed to achieve 10 9 contrast over 40 nm bandpass within the wedged region with the circle of diameter 1λ/D centered at 2λ/D showing the region over which the contrast is calculated. Right: plot from left to right along the dashed line in the central panel showing the control mask extending from 4 to 1.3λ/D.

Broadband VNC Approach Use Fresnel rhomb retarders as Achromatic Phase Shifters (APS) The APS consists of two pairs of symmetric Fresnel rhombs as half wave retarders Rhomb pairs are oriented orthogonally to one another in terms of respective s- and p-planes APS chromatic leakage must not exceed 10 7 rms over 613-653 nm bandpass in order to reach final 10 9 averaged over 1λ/D diameter circular dark region centered at 2λ/D Hicks+, Proc. SPIE (2015)

Expected performance of Achromatic Phase Shifter (APS) Uncoated Fresnel rhombs selected as a buildable approach to meeting the TDEM milestone Hicks+, Proc. SPIE (2015) Plots of theoretical BK7/vacuum retardance (δ) optimized for the 613-653 nm bandpass Left: Retardance as a function of total internal reflection (TIR) angle of incidence (AOI) Center: Retardance as a function of wavelength at the design AOI Right: Chromaticity of the null Dashed lines correspond to the design AOI, dotted are +/- 15 arcsec Parallel coronagraphs or alternative approaches needed for achieving deeper nulls over a broader instrument bandpass

Background & Outline Broadband Milestone Macro-scale segmented mirror SAINT Summary Deformable mirror segment phasing: narrowband vs. broadband Scan delay line while recording intensity on each segment for fringe packet fitting and determining segment piston and tip/tilt offsets Tip/tilt on a given segment reduces fringe visibility 1, 40, and 80 nm bandpasses shown from left to right below λ2 λ 400µm 633 waves λ2 λ 10µm 16 waves λ2 λ 5µm 8 waves

Deformable mirror segment phasing: group and phase delay Fit 3-parameter Gaussian (amplitude, FWHM, offset) to signal modulus for each segment (single scan above) Use offset to determine group delay for each segment relative to average (upper right) Shift scan data by offset and determine phase residual (lower right) Calculate deformable mirror correction to last state vector and iterate

Flattened deformable mirror state vector Goal is to minimize peak-to-valley of each state vector: piston, tip, tilt Top to bottom gradient in piston map indicative of tilt between nuller arms Nearest neighbor outliers restrict solution range

DM states visualized in bright pupil and dark focal outputs Left to right: DM at system startup, after setting all segment PTT values to 0, following coarse flattening (relative to delay arm reference), and additional flattening by hand The digital mask applied in upper right corresponds to the physical Lyot mask in the dark focal output that produces the characteristic sidelobes visible at 15λ/D Dark outputs are the DM only and normalized to the brightest pixel value

Macro-scale actively controlled segmented mirror array In development to demonstrate laboratory coronagraph performance in the presence of complex diffraction and instabilities Rendering provided by C. Koca (NASA GSFC) R = 4000 mm, k = 0 surface allows multiple approaches to generating array using parent segmentation or blocking

Finite element analysis of gravity sag, thermal, and bond stress Including mounted segment surface measurements (+ environment dynamics) will allow scalable STOP model study and tuning of end-to-end active primary + DM wavefront control (forthcoming slides) Slide content courtesy of J. Bolognese (NASA GSFC)

Surface residual measurements Preliminary analysis of unblocked segment quality assurance data Left: Stitched segment data Center, Right: Piston/tip/tilt removed and 5, 10 pixel guard band, respectively Blocking stress corresponding to asymmetries in blank dimensions needs more forensics

Surface errors binned by spatial frequency Charts and table generated from vendor measurements of unblocked segment spatial wavelengths frequencies bin (mm) (cpa) 1 4.0 8.0 5-10 2 8.0 10.0 4-5 3 10.0 13.3 3-4 4 13.3-20.0 2-3 5 > 20.0 < 2 6 total < 10 a piston, tip, tilt, and power removed Surface data taken with 100 mm Zygo and bandpass filtered Excellent results surpassing mid high spatial frequency requirements Only a single out of spec point measured in the < 2 cpa bin, likely due to springing

Assembled mechanisms and fit-checking the array Design (optics, mounts, fixtures) completed early spring 2015, PO submitted 6/5/2015, mirrors received 11/3/2015, bonding process underway Tolerancing of segments and jig to achieve < 0.25 mm segment centration and < 0.5 clocking Coarse (manual) and fine (active) actuation stages tested Combined mirror + pedestal mass less than half recommended actuator load limit

Segmented Aperture Interferometric Nulling Testbed (SAINT) PI: R. Lyon - Awarded in 2014; Funding initiated 2015 Demonstrate and quantify high contrast imaging capability with an actively controlled segmented aperture by modifying an existing reconfigurable sparse aperture Maintain single mode fiber source option currently used with the VNC Fast steering mirror to be added between the segmented aperture telescope and VNC Continue incremental improvements to control routines, as well as hardware including detectors, deformable mirror(s), and nuller mechanisms

Adapting the Fizeau Interferometry Testbed (FIT) to SAINT FIT sparse aperture Filled hexagonal array is a drop-in replacement for sparse array Additional hyperbolic mirror before reaching relay collimator Periscope relay through baffled vacuum chamber window (not shown) Relay reimages segmented primary to fast steering mirror at existing VNC breadboard aperture stop location Lyon+, Proc. SPIE (2004)

A tool for studying end-to-end controls in the presence of dynamic instabilities Refine wavefront control offloading of non-common vs. common mode dynamic perturbations Study contrast control authority in the presence of diffraction from a complex aperture Mapping of primary segments to deformable mirror segments and Lyot mask

A 100% yield Iris, AO PTT489 DM is available for use with SAINT Left and center: APS-equipped 1 nm and 40 nm bandpass VNC bright output pupil images recorded June 2015 using a fully active PTT DM prior to flattening (shown without digital mask) Right: Broadband PSF of the reference (delay) arm showing the six sidelobes spaced at 60 characteristic of the 7-ring hexagonal array of circular subapertures in the physical Lyot mask

Summary of ongoing and forthcoming VNC development Complete the broadband VNC demonstration (imminent) Align segmented mirror and generate surface map of phased array (end of calendar 2015) Install 100% yield deformable mirror (early 2016 or sooner) Finish SAINT telescope, telescope to VNC relay design, and procure components (spring 2016) Design the Next Generation (summer 2016) Couple active segmented telescope to VNC, demonstrate SAINT (fall 2016) Continue testing of single mode fiber bundle arrays for full field complex wavefront control Continue work towards integrating photon counting CCDs and developing detector electronics [Mallik+ Proc. SPIE (2015)] using real-time Linux

Backup Slides

Polarization Nulling: generalized beamsplitters and retarders ( ) cosθ E 0 = E 0 sinθ ( t e iψ ) cosθ E t = E 0 t sinθ ( r e iξ ) cosθ E r = E 0 r e i(ψ+ξ ) sinθ ( t 2 E tt = E e iψ ) cosθ 0 t 2 sinθ ( t r E tr = E e iψ ) cosθ 0 t r sinθ ( r 2 e i2ξ ) cosθ E rr = E 0 r 2 ei(ψ+2ξ ) sinθ ( ) r t cosθ E rt = E 0 r t e iψ sinθ I b = E tt + E rr 2 I d = E tr + E rt 2

APS specifications and measurements Measurement Specification FR1 FR3 FR8 FR10 Comment 12.3+00/-0.05 12.28323 12.28323 12.28314 12.28314 FR8, FR3 pairs Thickness FR1 pairs with with FR10 ±20 nm precision Length 35.24+0.0/-0.1 35.20 35.20 35.24 35.24 Precision specification not met (unchamfered) ±50 nm precision Entrance/exit 15.0+0.0/-0.1 14.95±0.01 edge length Angle 55 4 48±1.0 ; 55 4 48.5 ±0.5 Measurement performed optically contacted ±0.1 precision to machining reference chuck TIR surface < 0.5; ±0.1 precision 0.12 0.17 0.20 0.15 parallelism Entrance/exit < 0.5; ±0.1 precision 1.6 0.7 5.0 2.8 Calculated from transmitted beam deviation parallelism at 633 nm Right angle ±1.0 from 90 < 0.5 < 1.0 < 1.0 < 0.5 errors P-V WFE < 43 (< λ/15 at 12, 20, 10, 11 11, 24, 12, 9 16, 31, 10, 17 21, 14, 10, 24 F, B, T, U surfaces 633 nm) RMS WFE < 13 (< λ/50 at 2, 4, 1, 2 1, 4, 2, 1 3, 4, 1, 3 4, 2, 1, 4 F, B, T, U surfaces 633 nm) P-V WFE < 159 (< λ/4 at 103 114 95 109 155 109 122 93 R, L alignment surfaces 633 nm) RMS surface < 1 0.8 (F) 0.9 (F), 0.8 (B) roughness Scratch/Dig 10/5 10/5 Entrance/exit reflectance Ravg < 0.1%, 613-653 nm < 0.1% Dimensions in mm, angles in arcseconds, and surfaces in nm unless specified

Rhomb anti-reflection coatings Require R < 0.1% over design bandpass Reflectance can be enhanced to aid in alignment

The (VNC) laboratory Optics and detectors, control software and electronics, and vacuum isolation chamber

WFC sequence