Visible Spectro-Polarimeter (ViSP)
Important note: Please refer to the latest DKIST Observing Cycle Proposal Call for the definition of available instrument modes. The information below is a summary of the instrument capabilities as designed and does not necessarily reflect the modes available.
Mission
The mission of the Visible Spectro-Polarimeter (ViSP) is to simultaneously record maps of the solar surface in up to three flexibly selectable spectral lines within the visible spectrum, with high spatial and spectral resolution, and high polarimetric precision whenever full-Stokes-polarimetry measurements are acquired.
Description
The Visible Spectro-Polarimeter (ViSP) is optically located behind the DKIST Adaptive Optics (AO) system and consists of a high-spectral-resolution single-slit diffraction-grating based spectrograph that can simultaneously observe up to three spectral lines in a wavelength range from 380-900 nm (the visible spectrum). The ViSP’s three camera arms can be moved and focused independently on an arched rail to access the selected spectral lines for a given diffraction grating angle and spectrograph order. The slit can be moved across the spectrograph’s entrance focal plane to scan maps of the solar surface. A modulator optic behind the slit assembly modulates the polarization state of the incoming light so that the full Stokes vector can be measured in the camera focal plane. Being dual beam polarimeters, each ViSP arm captures two orthogonal polarization states co-temporally on its detector to minimize crosstalk in the measurements.
ViSP can be run in parallel to all other DKIST instrumentation (VBI, VTF, DL-NISRP) apart from the Cryo-NIRSP, but only the start times of observations are synchronized.
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ViSP instrument layout with all relevant optics and motorized stages, taken from de Wijn et al., 2022, SoPh, 297, 22. |
Technical Details at a Glance
Observing Modes
Spectroscopic mode: acquisition of intensity spectra. The slit is moved continuously across the solar image at a speed that is matched to the slit width.
Polarimetric mode: acquisition of the full Stokes vector IQUV in a dual-beam configuration with a rotating retarder as polarization modulator. The spatial scanning of the solar surface is achieved by discrete stepping of the entrance slit across the solar image.
Spatial Sampling and Field of View
As a post-AO instrument, ViSP
is fully and routinely supported by the DKIST AO system, and
VISP can observe in parallel with VBI, VISP and DL-NIRSP.
NOTE: Available instrument combinations depend on the FIDO configuration.
The instrument was designed to perform at about twice the spatial diffraction limit of DKIST at most wavelengths.
Spatial (Pixel-)Sampling along slit
Camera arm 1: 0.0295 arcsec / pixel
Camera arm 2: 0.0236 arcsec / pixel
Camera arm 3: 0.0195 arcsec / pixel
Slits widths available
0.0284 arcsec
0.041 arcsec
0.054 arcsec
0.107 arcsec
0.214 arcsec
Field of View
Maximum optical field: 2×1.25 arcmin2 (full post-AO DKIST 2×2 arcmin2 field of view, restricted by the camera format)
Each of the three ViSP arms has a different magnification due to the spectrograph characteristics:
Camera arm 1: ~75 arcsec using 2560 spatial pixels
Camera arm 2: ~60 arcsec using 2560 spatial pixels
Camera arm 3: ~50 arcsec using 2560 spatial pixels
Full 2 arcmin that the ViSP light feed telescope transmits is covered through lateral spatial scanning
Spectral Range and Resolution
Spectral range
380 - 900 nm (designed range), with continuous coverage
i.e., for a ViSP configuration using just one single wavelength, any portion of the spectrum can be imaged in either of the 3 spectral arms
observe up to 3 spectral bands simultaneously
at λ = 630 nm: spectral bands are ~1 nm wide at ~1 pm / pixel spectral sampling, with 2×1000 px for dual beam polarimetry
NOTE: The actual wavelength range accessible by ViSP is potentially limited by the configuration of the Facility Instrument Distribution Optics (FIDO) in use.
Spectral resolution
Maximum resolving power better than R ~ 180000 @ λ = 630 nm
put differently: better than 3.5 pm @ λ = 630 nm (when sampling < 1.75 pm/px)
NOTE: resolving power depends on wavelength and spectrograph arm configuration
Spectrograph Lines
Diagnostic | Wavelength [nm] |
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Ca II K | 393.4 |
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Ca II H | 396.8 | includes H I 397 nm H-Epsilon in the red wing of Ca II H |
H I | 410.1 | H-Delta |
H I | 434.0 | H-Gamma |
Sr I | 460.7 |
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H I | 486.1 | H-Beta |
Mg I b2 | 517.3 |
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Fe I | 525.0 |
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Fe I | 557.6 | no Zeeman splitting, Lande factor g = 0 |
Na I D2 | 589.0 | either individually or both lines combined when centered at 589.3 nm |
Na I D1 | 589.6 | |
Fe I | 617.3 |
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Fe I | 630.2 |
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H I | 656.3 | H-Alpha |
Fe I | 709.0 | no Zeeman splitting, Lande factor g = 0 |
Ca II | 849.8 |
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Ca II | 854.2 |
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Ca II | 866.2 |
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NOTE: the available line list for a Cycle is announced in the Proposal Calls
Temporal Cadence
reconfiguration of arms: ~20 minutes (including order sorting filter change)
temporal cadences depend critically on the science use case, and resulting spectrograph configuration
cadence examples
spectroscopy: lateral FOV of 2.2×1 arcmin2 maps can be observed at about 62 seconds cadence
(λ = 630 nm: 0.054 arcsec slit width, 33 Hz exposure rate, 2.132 arcsec/px slit velocity)polarimetry: lateral FOV of 0.5×1 arcmin2 maps can be observed at about 25 minute cadence
(λ = 630 nm: 0.107 arcsec slit width, 33 Hz exposure rate, 0.0663 arcsec/slit step, 450 slit steps)NOTE: Modulation rate is driven by the slowest of the 3 camera arms
Polarimetric Capabilities
Each arm is a dual beam polarimeter
Full Stokes vector polarimetry, or Stokes-I only
polarimetric sensitivity per slit position: 10-3 Icont at λ > 450 nm (depending on instrument configuration requested)
Photometric Capabilities
Flat fields repeatable to the 2% level
Instrument Modes
Example Modes of Operation
Example 1: Spectroscopic mode with 3 wavelength channels (arms)
0.054 arcsec slit width
2.132 arcsec/px slit velocity, acquired at ~33 Hz camera exposure rate
4 maps/λ, with sizes 2.2×[1.25, 1, 0.83] arcmin2, cadence: 62 seconds / map
Arm configurations:
Arm 1: λ = 589.59 nm, ∆λ = 0.0009569 nm
(total) exposure time: 1 accumulations × 15 ms = 15 ms
Arm 2: λ = 630.15 nm, ∆λ = 0.0011478 nm
(total) exposure time: 1 accumulations × 10 ms = 10 ms
Arm 3: λ = 517.27 nm, ∆λ = 0.0011808 nm
(total) exposure time: 1 accumulation × 15 ms = 15 ms
Example 2: Spectro-Polarimetric Mode with 2 wavelength channels (arms)
0.1071 arcsec slit width
10 modulation states to retrieve full Stokes vector, acquired at ~33 Hz camera exposure rate
450 slit positions, 0.10625 arcs slit step width
1 map/λ, with sizes 0.8×[1, 0.83] arcmin2, cadence: ~25 minutes / map
Arm configurations:
Arm 2: λ = 630.15 nm, ∆λ = 0.0011478 nm
(total) exposure time: 10 accumulations × 10 ms = 100 ms
Arm 3: λ = 517.27 nm, ∆λ = 0.0011808 nm
(total) exposure time: 10 accumulation × 15 ms = 150 ms
Publications
Kuridze, D., Uitenbroek, H. Wöger, F., et al., “Insight into the Solar Plage Chromosphere with DKIST“, The Astrophysical Journal, 965, 1, 15 (2024)
Kuridze, D. Woeger, F., Fischer, C., et al., “DKIST observations of the fine-scale chromospheric structures“, American Astronomical Society, SPD Meeting #54, #407.02 (2023)
Campbell, R. J., Keys, P. H., Mathioudakis, M., et al., “DKIST Unveils the Serpentine Topology of Quiet Sun Magnetism in the Photosphere”, The Astrophysical Journal Letters, 955, 2 (2023)
da Silva Santos, J. M., Reardon, K., Cauzzi, G., et al., “Magnetic Fields in Solar Plage Regions: Insights from High-sensitivity Spectropolarimetry“, The Astrophysical Journal Letters, 954, 2 (2023)
de Wijn, A.G., Casini, R., Carlile, A. et al., “The Visible Spectro-Polarimeter of the Daniel K. Inouye Solar Telescope“, Solar Physics 297, 22 (2022).
Rimmele, T.R., Warner, M., Keil, S.L. et al., “The Daniel K. Inouye Solar Telescope – Observatory Overview“, Solar Physics 295, 172 (2020)
Rimmele, T., Tritschler, A., Parraguez, A., et al., “The US National Science Foundation Daniel K. Inouye Solar Telescope operations commissioning: results and lessons learned“, Ground-based and Airborne Telescopes X, Proc SPIE 13094: 130940Y (2024)
Rimmele, T., Warner, M., Casini, R., et al., “The National Science Foundation's Daniel K. Inouye Solar Telescope: status and first results“, Ground-based and Airborne Telescopes IX, Proc SPIE 12182: 121820Z (2022)
Rimmele, T., Woeger, F., Tritschler, A., et al., “Ground-based instrumentation and observational techniques“, 44th COSPAR Scientific Assembly, 44, E2.4-0001-22
Rimmele, T., Woeger, F., Tritschler, A., et al., “The National Science Foundation's Daniel K. Inouye Solar Telescope — Status Update“, American Astronomical Society meeting #238, #106.01 (2021)
Warner, M., Rimmele, T. R., Martinez Pillet, V., et al. “Construction update of the Daniel K. Inouye Solar Telescope project“, Ground-based and Airborne Telescopes VII, 10700: 107000V (2018)
Tritschler, A., Rimmele, T. R., Berukoff, S., et al., “Daniel K. Inouye Solar Telescope: High-resolution observing of the dynamic Sun", Astronomische Nachrichten, 337, 10 (2016)
Elmore, D. F., Rimmele, T. R., Casini, R., et al., “The Daniel K. Inouye Solar Telescope first light instruments and critical science plan“, Ground-based and Airborne Instrumentation for Astronomy V, Proc SPIE 9147: 914707 (2014)
Berger, T., and ATST Science Team, “The ATST Instrumentation suite: capabilities, synergies, and science goals“, American Astronomical Society, SPD meeting #44, #400.02 (2013)
Contact
If you have any specific question about ViSP, please use the DKIST Help Desk to post it.