S. Dandy’s research while affiliated with California College San Diego and other places

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Publications (7)


FFREE: a Fresnel-FREE demonstrator for the common-path optics within EPICS
  • Article

October 2010

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15 Reads

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1 Citation

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The purpose of FFREE - the new optical bench devoted to experiments on high-contrast imaging at LAOG - consists in the validation of algorithms based on off-line calibration techniques and adaptive optics (AO) respectively for the wavefront measurement and its compensation. The aim is the rejection of the static speckles pattern arising in a focal plane after a diffraction suppression system (based on apodization or coronagraphy) by wavefront pre-compensation. To this aim, FFREE has been optimized to minimize Fresnel propagation over a large near infrared (NIR) bandwidth in a way allowing efficient rejection up to the AO control radius, it stands then as a demonstrator for the future implementation of the optics that will be common to the scientific instrumentation installed on EPICS


Figure 1: Perfect PSF corresponding to the selected DM pupil (8.16 mm), the images edges correspond to ± 1 arcsec. The adopted diffraction suppression system in FFREE is pupil apodization with or without the use of a Lyot Stop. The PSF apodized amplitude profile is obtained with the Gerschberg & Saxton iterative method [7]: the amplitude apodized map varies until the requested contrast gain is achieved within θ FFREE . 
Figure 2: Perfect PSF corresponding to the selected DM pupil after amplitude apodization. 
Figure 3: Normalized PSF profiles with (continues line) and without (dashed line) pupil apodization at the convergence of the Gerschberg-Saxton loop: the goal in contrast gain (10 -2 at ± 0.25 arcsec) is achieved and the coronagraphic PSF is 
Figure 4: PSF corresponding to the selected DM pupil through an out-of-pupil optics with EFFL = 75 mm and σ SE = 40 
Figure 5: PSF corresponding to the selected size pupil and the same out-of-pupil optics, but with an ideal AO compensation: aliased spatial frequencies in the sampled wavefront are perfectly filtered out. Apodization is inserted in the complex amplitude before fast Fourier transform (FFT) provides the focal image: Fresnel-induced speckles still dominate within θ FFREE . 

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FFREE: A Fresnel-free experiment for EPICS, the EELT planets imager
  • Article
  • Full-text available

September 2010

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374 Reads

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8 Citations

Proceedings of SPIE - The International Society for Optical Engineering

The purpose of FFREE - the new optical bench devoted to experiments on high-contrast imaging at LAOG - consists in the validation of algorithms based on off-line calibration techniques and adaptive optics (AO) respectively for the wavefront measurement and its compensation. The aim is the rejection of the static speckles pattern arising in a focal plane after a diffraction suppression system (based on apodization or coronagraphy) by wavefront pre-compensation. To this aim, FFREE has been optimized to minimize Fresnel propagation over a large near infrared (NIR) bandwidth in a way allowing efficient rejection up to the AO control radius, it stands then as a demonstrator for the future implementation of the optics that will be common to the scientific instrumentation installed on EPICS.

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FIG. 1. Phase Diversity principle
FIG. 2. Scheme of our wide-band correction concept. a being the real aberrations. b a Δλ being the estimated aberrations by a Classical Phase Diversity  
FIG. 5. Bias vector on 20 Zernike for 100 nm to 500 nm bandwidth. Bandwidth is centered at 1050 nm, images are Shannon sampled at 950 nm.  
FIG. 6. Matrix M Δλ with 500 nm bandwidth. Bandwidth is centered at 1050 nm, images are Shannon sampled at 950 nm. The estimated coefficient values are coded in gray-scale. Max value is 1.2 and corresponds to white, min value is −0.4 and corresponds to black. Each introduced coefficient is explained in main text.  
A simple and efficient model for polychromatic focal plane wave-front sensor

July 2010

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207 Reads

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2 Citations

Proceedings of SPIE - The International Society for Optical Engineering

Phase Diversity is a focal-plane technique which is chromatic by nature. The use of a monochromatic model on wide-band imaging results of an additional error function of the spectral range.We present here a second order modeling of the focal plane wave-front sensing error due to wide-band imaging and propose a first order correction by inverse problem and the first results of an end-to-end simulation for an iterative correction. Simulation results of 20 nm wave-front aberrations show that the reconstruction error decreases from 10 nm with classical focal-plane sensor to sub-nanometric error with optimal correction at Deltalambda = 500 nm.


Fig. 1. Evolution of the reconstruction error with the exposure time (in number of independent turbulence realizations), for several levels of AO correction. Static aberrations are randomly generated according to conditions described in Subsection 4.1. 
Sensing Quasi-Static Aberrations of Adaptive Optics Systems On-Line with Long-Exposure Phase Diversity

January 2010

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44 Reads

We validate by simulations an extension of the phase diversity technique that uses long exposure adaptive optics corrected images for sensing quasi-static aberrations during the scientific observation, in particul ar for high-contrast imaging. The principle of the method is that, for a sufficiently long exposure time, the residual turbulence is averaged into a convolutive component of the image and that phase diversity estimates the sole static aberrations of interest. The advantages of such a pro cedure, compared to the processing of short- exposure image pairs, are that the separation between static aberrat ions and turbulence-induced ones is performed by the long-exposure itself and not numerically, that only one image pair must be processed, that the estimation benefits from the high SNR of long-exposure images, and that only the static aberrations of interest are to be estimated. Long-exposure phase diversity can also be used as a phasing sensor for a segmented aperture telescope. Thus, it may be particularly useful for future planet finder projects such as EPICS on the European ELT.



Evolution of the reconstruction error with the exposure time (in number of independent turbulence realizations). Static aberrations are randomly generated according to conditions described in Subsection 4.1. AO correction is assumed to be performed by a SAXO-like system.
Evolution of the reconstruction error with the exposure time, for several levels of AO correction. Static aberrations are randomly generated according to conditions described in Subsection 4.1.
Spatial spectrum of the estimated aberrations, in the case of a NAOS-7 correction. The vertical line represents the maximum spatial frequency that is corrected by the AO system.
Spatial spectrum of the estimated aberrations, in the case of a NAOS-14 correction. The vertical line represents the maximum spatial frequency that is corrected by the AO system.
Spatial spectrum of the estimated aberrations, in the case of a SAXO/SPHERE correction. The vertical line represents the maximum spatial frequency that is corrected by the AO system.
On-Line Long-Exposure Phase Diversity: a Powerful Tool for Sensing Quasi-Static Aberrations of Extreme Adaptive Optics Imaging Systems.

October 2008

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67 Reads

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50 Citations

The phase diversity technique is a useful tool to measure and pre-compensate for quasi-static aberrations, in particular non-common path aberrations, in an adaptive optics corrected imaging system. In this paper, we propose and validate by simulations an extension of the phase diversity technique that uses long exposure adaptive optics corrected images for sensing quasi-static aberrations during the scientific observation, in particular for high-contrast imaging. The principle of the method is that, for a sufficiently long exposure time, the residual turbulence is averaged into a convolutive component of the image and that phase diversity estimates the sole static aberrations of interest. The advantages of such a procedure, compared to the processing of short-exposure image pairs, are that the separation between static aberrations and turbulence-induced ones is performed by the long-exposure itself and not numerically, that only one image pair must be processed, that the estimation benefits from the high SNR of long-exposure images, and that only the static aberrations of interest are to be estimated. Long-exposure phase diversity can also be used as a phasing sensor for a segmented aperture telescope. Thus, it may be particularly useful for future planet finder projects such as EPICS on the European ELT.


On-Line Long-Exposure Phase Diversity: a Powerful Tool for Sensing Quasi-Static Aberrations of Extreme Adaptive Optics Imaging Systems

October 2008

The phase diversity technique is a useful tool to measure and pre-compensate for quasi-static aberrations, in particular non-common path aberrations, in an adaptive optics corrected imaging system. In this paper, we propose and validate by simulations an extension of the phase diversity technique that uses long exposure adaptive optics corrected images for sensing quasi-static aberrations during the scientific observation, in particular for high-contrast imaging. The principle of the method is that, for a sufficiently long exposure time, the residual turbulence is averaged into a convolutive component of the image and that phase diversity estimates the sole static aberrations of interest. The advantages of such a procedure, compared to the processing of short-exposure image pairs, are that the separation between static aberrations and turbulence-induced ones is performed by the long-exposure itself and not numerically, that only one image pair must be processed, that the estimation benefits from the high SNR of long-exposure images, and that only the static aberrations of interest are to be estimated. Long-exposure phase diversity can also be used as a phasing sensor for a segmented aperture telescope. Thus, it may be particularly useful for future planet finder projects such as EPICS on the European ELT.

Citations (3)


... where f max denotes the maximum spatial frequency in the pupil we want to control, here 10 cycles per pupil. Each optics of our design shall be at a distance z from the pupil plane such that z z T /4, following the approach of Antichi et al. 17,18 This condition proves challenging for the optics close to MEMS DMs which have a small size (∼ 9 mm), associated with a short Talbot distance of 2.56 m. The dimensions of the testbed table set limits to the maximum size and pupil magnification factors in our design. ...

Reference:

High-contrast imager for Complex Aperture Telescopes (HiCAT): 1. Testbed design
FFREE: a Fresnel-FREE demonstrator for the common-path optics within EPICS
  • Citing Article
  • October 2010

... As a second step, we proceed to end-to-end testbed simulations with Fresnel propagation and starlight suppression algorithm to minimize amplitude-induced errors, building on previous analysis. [18][19][20] We performed several iterations for both the geometric/Talbot distances and end-to-end optimizations to obtain an optical design with optics specifications that mitigate the Talbot effects under the opto-mechanical requirements. The details of this work and results were detailed in Paper I. 5 ...

FFREE: A Fresnel-free experiment for EPICS, the EELT planets imager

Proceedings of SPIE - The International Society for Optical Engineering

... In astronomical AO systems, incoming light is usually divided into distinct optical paths: one fraction is channelled towards scientific instruments (science path), while another fraction is directed to WFSs (AO path). However, this scheme introduces a possibility for path-specific aberrations termed NCPAs (see Mugnier et al. 2008;Lee et al. 1997). For instance, aberrations that occur outside the AO optical path remain unseen by WFSs and, thus, they cannot be compensated for. ...

On-Line Long-Exposure Phase Diversity: a Powerful Tool for Sensing Quasi-Static Aberrations of Extreme Adaptive Optics Imaging Systems.