Abstract

Astronomical instruments greatly improve wavelength multiplexing capabilities by using beam splitters. In the case of the 4-m National Science Foundation’s Daniel K. Inouye Solar Telescope (DKIST) solar telescope, over 70 W of optical power is distributed simultaneously to four instruments, each with multiple cameras. Many DKIST observing cases require simultaneous observations of many narrow bandpasses combined with an adaptive optics system. The facility uses five dichroic optical stations to allow at least 11 cameras and two wavefront sensors to simultaneously observe ultraviolet to infrared wavelengths with flexible reconfiguration. The DKIST dichroics required substantial development to achieve very tight specifications over very large apertures of 290 mm diameter. Coating spectral variation occurs over <1 nm wavelength, comparable with instrument bandpasses. We measure retardance spectral variation of up to a full wave and diattenuation varying over ±10 % per nm. Spatial variation of Mueller matrix elements for coatings in both transmission and reflection requires careful metrology. We demonstrate coatings from multiple vendors exhibit this behavior. We show achievement of 5-nm root mean square (RMS) reflected wavefront and 24-nm RMS power with coatings over 8 μm thick. We show mild impacts of depolarization and spectral variation of polarization on modulation efficiency caused by the dichroic coatings. We show an end-to-end system polarization model for the visible spectropolarimeter instrument, including the dichroics, grating, analyzer, and all coated optics. We show detailed performance for all DKIST dichroics for community use in planning future observations.

Highlights

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

  • We showed in Ref. 87 detection of the clocking oscillations outlined in Ref. 84 with calibrations both on-sun and with the DKIST calibration lamp

  • We show a coating model from DKIST M7 through the facility instrument distribution optics (FIDO) dichroics and all significant contributing visible spectropolarimeter (ViSP) optics using metrology at appropriate incidence angles

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Summary

Introduction

Spectral interference fringes adversely impact polarization accuracy for astronomical instruments requiring optical fringe modeling and/or removal methods through design and data processing.[52,53,64,68,69,70,71,72,73,74,75,76,77,78,79,80] In Ref. 81, we applied the Berreman calculus[82,83] to polarization fringes formed in multilayer crystals with predictions and data collected in the lab and at a solar telescope We extended this calculus in Ref. 81 to include fringe magnitude estimates in converging and diverging beams. We investigated spatial variation of retardance across multilayer retarders made of polished crystals, stretched polycarbonate, and ferroelectric liquid crystals in Ref. 85 This variation was included in the DKIST optical model to show polarization calibration errors as functions of field angle and wavelength. If care is not taken with specification, design, and metrology, issues we outline as follows can become major performance issues

DKIST Wavelength Multiplexing
Optical Layout
Science Drivers for FIDO Configurations
FIDO Example Configuration
FIDO Substrate Retardance in Transmission
FIDO Dichroic Transmitted Wavefront
FIDO Dichroic Reflected Wavefront
FIDO Dichroic Beam Splitter C-BS-950
BS-950: final coating reflection and transmission spectral features
BS-950: narrow spectral features reflection
BS-950
BS-950: transmission spatial variation in 100 mm aperture with NDSP3
Depolarization from Spatial Variation
2.10 DL-NIRSP Dichroic Beam Splitters from Alluxa Measured in NLSP
2.10.1 DL BS: Mueller matrix measured in transmission with NLSP
2.10.2 DL BS: Mueller matrix measured in reflective K-cell with NLSP
2.11 Dichroic Summary
System Model for DKIST Instruments
ViSP: Optical Overview and Deriving Modulation Matrices
ViSP: Coating Model for the Entire Optical Feed
ViSP: polycarbonate modulator
ViSP: diattenuation model for the grating
ViSP: polarizing beam splitter and beam combiner
ViSP: Modulation Matrix Summary
Summary of Coating Impacts for DKIST
ViSP: Slit Polarization
IOI Coatings
Spatial Variation of Protected Metal Coatings
Protected aluminum coatings
Protected silver coatings
Ellipsometry for DKIST M8
Spatial Variation of Bare Metal Coatings
FIDO Dichroic Beam Splitter C-BS-465
BS-465 reflection and transmission from IOI
BS-465 transmission spatial uniformity from NDSP3
BS-465 retardance and diattenuation with NLSP in transmission: as built
BS-465 retardance and diattenuation with NLSP in reflection: as built
FIDO Dichroic Beam Splitter C-BS-555
BS-555 reflection and transmission from IOI
BS-643 reflection and transmission from IOI
BS-643 retardance and diattenuation with NLSP in transmission
BS-643 retardance and diattenuation in reflection with NLSP K-cell
FIDO Dichroic Beam Splitter C-BS-680
BS-680 reflection and transmission from IOI full sized stress sample
BS-950 final coating absorption
BS-950 transmission spatial variation
Antireflection
Substrate Internal Transmittance and Fresnel Losses
7.10 Thorlabs
7.10.1 Thorlabs DMSP1000L short pass dichroic mapping at 0 deg and 45 deg incidence
Findings
7.10.2 Thorlabs DMLP567L long pass dichroic mapping at 0 deg incidence
Full Text
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