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Estimation of polarization aberrations and its effect on the point spread function of the Thirty Meter Telescope

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dc.contributor.author Ramya, M. Anche
dc.contributor.author Anupama, G. C
dc.contributor.author Sriram, S
dc.contributor.author Sankarasubramanian, K
dc.contributor.author Skidmore, W
dc.date.accessioned 2020-11-19T13:58:09Z
dc.date.available 2020-11-19T13:58:09Z
dc.date.issued 2018-07
dc.identifier.citation Proceedings of the SPIE, Vol. 10703, pp. 107034K-1- 107034K-12 en_US
dc.identifier.issn 1996-756X
dc.identifier.uri http://prints.iiap.res.in/handle/2248/7284
dc.description Restricted Access © SPIE--The International Society for Optical Engineering https://doi.org/10.1117/12.2312506 en_US
dc.description.abstract The Thirty Meter Telescope (TMT) is a future generation telescope proposed to be located in Mauna Kea, Hawaii or in La Palma in the Canary Islands. The telescope will have a segmented primary and an inclined tertiary mirror. The segmentation of the primary mirror and the inclination in the tertiary mirror can introduce significant polarization aberrations. Typically, the polarization aberrations, introduced due to the mirror coating and the high incident angles cause small modifications to the Point Spread Function (PSF). Here, we perform the polarization ray tracing for TMT using the optical design software Zemax for different input polarizations for a point source (on-axis). We calculate the diattenuation and retardance aberration maps for all the three mirrors of TMT. The coating induced astigmatism obtained from the retardance of the primary and secondary mirror is found to be of the order of 0.048 radians, whereas, the polarization induced tilt by the retardance of the tertiary mirror is in the order of 0.29 radians. The Jones pupil maps are estimated at two of the instrument ports, Wide Field Optical Spectrograph (WFOS) and Narrow Field Infrared Adaptive Optics System (NFIRAOS).The Amplitude Response Matrix (ARM) estimated at the WFOS port show the presence of ghost PSF's. The magnitude of the ghost PSF components is of the order of 2.5 x 10-5 at 1μm at WFOS port. The ARM and the Point Spread Matrix (PSM) are estimated at the focus of the NFIRAOS instrument. The Stokes PSF is shown for horizontal and vertical polarization as inputs. The Huygen's point spread function obtained from Zemax shows the variations in FWHM for unpolarized and polarized inputs. These estimations would help in the design aspects of a high contrast imaging instrument for the TMT in the future. en_US
dc.language.iso en en_US
dc.publisher SPIE--The International Society for Optical Engineering en_US
dc.subject Instrumental polarization en_US
dc.subject Point spread function en_US
dc.subject Polarization aberrations en_US
dc.subject Jones Pupil map en_US
dc.subject Point spread matrix en_US
dc.subject Thirty Meter Telescope en_US
dc.subject NFIRAOS en_US
dc.title Estimation of polarization aberrations and its effect on the point spread function of the Thirty Meter Telescope en_US
dc.type Article en_US


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