An Off-Axis Hartmann Sensor for Measurement of Wavefront Distortion in Interferometric Detectors
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1 An Off-Axis Hartmann Sensor for Measurement of Wavefront Distortion in Interferometric Detectors Aidan Brooks, Peter Veitch, Jesper Munch Department of Physics, University of Adelaide
2 Outline of Talk Discuss the thermal lensing problem Off-Axis Hartmann Sensor Two Stages 1. Phase distortion measurements with a Hartmann sensor 2. Off-axis tomographic analysis of phase measurements Installation of sensor at AIGO
3 Objectives of research Improve operation of advanced interferometers by reducing thermally induced wavefront distortion. Develop a sensor to measure the distortion and correction in the ACIGA High Optical Power Test Facility.
4 Crux of thermal problem Courtesy of Ryan Lawrence and David Ottaway, MIT Absorbed power causes thermal lensing Prediction of MELODY model of Advanced LIGO Sideband power is scattered out of TEM00 Instrument failure at approximately 2 kw Adv. LIGO cannot achieve desired sensitivity unaided
5 How to maintain cavity finesse? Measure distortion with wavefront sensor Employ active compensation system Sensor cannot interfere with core optics or GWI laser beam. OFF-AXIS WAVEFRONT SENSOR
6 Why use a Hartmann wavefront Interferometry Shack-Hartmann Hartmann sensor? Easiest to align Cheap In principle, can measure a wavefront change of less than λ/1000
7 Hartmann wavefront sensor Large diameter HeNe beam Hartmann Rays. Reference. Distorted. CCD Hartmann Plate Mirror Substrate Record spot positions on CCD Wavefront changes spot positions change Gradient of wavefront change proportional to displacement of spot. Measurement of the gradient of the phase distortion allows one to reconstruct the distortion itself
8 Current Hartmann Plate Square arrangement Hole size: 150 microns Pitch: 570 microns Future plate: Hexagonal arrangement Hole size: 150 microns Pitch: 430 microns
9 Off-Axis Bench Top Test Hartmann plate
10 Hartmann Phase Reconstruction Gradient field Reconstructed phase map
11 Determine wavefront distortion using optical tomography Cylinder of transparent material with internal temperature/refractive index distribution
12 Determine wavefront distortion using optical tomography Divide into annular volume elements (voxels)
13 Determine wavefront distortion using optical tomography related spaces Original voxel uniform refractive index Phase distortion caused by this voxel - Off Axis Projection Off axis viewing angle, θ n(r, z) φ(x, y)
14 Simulation of tomography Temperature distribution in ITM of AdLIGO-like system modelled using Hello-Vinet equation Off-axis optical path distortion (OPD) through this distribution determined OPD used as input data for a least-squares-fit to voxel projections Internal temperature distribution reconstructed On-axis OPD determined from reconstruction and compared to OPD predicted by theory
15 Simulation results Original off-axis OPD Best fit with voxel projections
16 Tomographic analysis is accurate input, reconstructed difference 1000
17 Implementation of tomography Hartmann sensor used to measure OPD gradient field Gradient field used to reconstruct phase distortion (OPD) using iterative process Tomographic analysis determines temperature distribution from reconstructed OPD On-axis OPD determined from reconstructed temperature distribution
18 Installation at AIGO
19 Installation at AIGO
20 Installation at AIGO HR coating Off-axis probe beam One micron laser beam
21 Installation at AIGO - Update Interference fringes on illumination pattern. Caused by a combination of aberrations on the input beam and reflections from the vacuum tank input windows. Intensity variations adversely affect the Hartmann sensor Use a short coherence length source
22 Installation at AIGO - Update Interference fringes on illumination pattern. Caused by a combination of aberrations on the input beam and reflections from the vacuum tank input windows. Intensity variations adversely affect the Hartmann sensor Use a short coherence length source
23 Conclusion Single view, off-axis Hartmann, tomographic wavefront sensor has sufficient accuracy to measure cylindrically symmetric refractive index distributions in advanced interferometers Accuracy of ~ λ/1000 (simulation). Current precision (Adelaide) ~ λ/250 Current precision (AIGO) ~ poor. Acquire short coherence length source Acquire correct Hartmann plate Can extend to non-cylindrically symmetric distributions use multiple views and azimuthal voxelation
24 Compensation Plate Effect
25 Compensation Plate Effect
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