Abstract

Astronomical spectropolarimeters require high accuracy polarizers with large aperture and stringent uniformity requirements. In solar applications, wire grid polarizers are often used as performance is maintained under high heat loads and temperatures over 200°C. DKIST is the NSF’s new 4-m aperture solar telescope designed to deliver accurate spectropolarimetric solar data across a wide wavelength range, covering a large field of view simultaneously using multiple facility instruments. Polarizers at 120 mm diameter are used to calibrate DKIST instruments but vary spatially in transmission, extinction ratio, and orientation of maximum extinction. We combine new spatial and spectral metrology for polarizers and retarders to simulate the accuracy losses with field angle and wavelength caused simultaneously by spatial variation of several optical parameters including beam decenter from misalignments. We also present testing of a new crystal sapphire substrate polarizer designed and fabricated to improve DKIST long wavelength calibrations. We assess spatial thickness variation of sapphire and fused silica wafer substrates using spectral interference fringes.

Highlights

  • Daniel K. Inouye Solar Telescope (DKIST) and Polarization Models for CalibrationThe National Science Foundation’s Daniel K

  • We show some examples of contrast, extinction, Mueller matrix elements, and the degree of polarization (DoP) in Appendix E

  • We presented new metrology for the DKIST polarizers and retarders on apertures larger than 90 mm diameter with thousands to tens of thousands of spatial sampling points at spectral resolving powers over a few thousand covering 390 to 1600 nm

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Summary

Introduction

This variation was included in the DKIST optical model to show polarization calibration errors as functions of field angle and wavelength. We include spatial variation across individual beam footprints in a Mueller matrix propagation simulation This simulation creates synthetic modulated data as a function of field angle and wavelength as the footprints sample the calibration optics well away from the optical bore sight. For the optical path to our NCSP and the Cryo-NIRSP, the aO and AO systems are not simultaneously sampling the coudé beam This leads to temporal drifts in the beam centering and preliminary polarization calibration errors at levels we simulate in this paper. We compile here additional information about the interference fringe properties anticipated for our polarizers

System Model for Calibration
10 States Created with a Polarizer and Retarder
Modulation Matrix
Fitting Output
Assessing Calibration Inaccuracies: the Error Matrix
Measuring Polarizer Spatial and Spectral Properties
DKIST Calibration Polarizer
CalPol1 spare: contrast and extinction orientation spectra
CalPol1 spare: mapping contrast variation across the aperture
CalPol1 spare: mapping extinction orientation variation across the aperture
CalPol1 spare: mapping transmission across the aperture
Measuring Retarder Spatial and Spectral Properties
Optically Contacted Calibration Retarder
Optically Contacted Calibration Retarder Transmission
Footprints on the DKIST Calibration Optics
Polarizer Spatial Variation Sampled by Beam Footprint
Retarder Spatial Variation Sampled by Beam Footprint
Fitting Footprint-Averaged Model Across Field
Fitted Calibrator Transmission Variable Field Dependence
Error Matrix with Field Angle
Error Matrix with Wavelength at 60 and 114 ArcSec Field Angles
Error Budget Comparison to Error Matrices
Wire Grid Polarizer Spatial and Spectral Fringes
Spectrally Resolving Fringes
Sapphire CalPol: transmission spatial fringe maps
Findings
Summary
Full Text
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