Kawabata Yusuke, Katsukawa Yukio, Kubo Masahito, Anan Tetsu, Ichimoto Kiyoshi, Shinoda Kazuya, Tsuzuki Toshihiro, Uraguchi Fumihiro, Nagata Shin'ichi, Oba Takayoshi, Expósito David Hernández, Sánchez Gómez Antonio, Orozco Suárez David, Balaguer Jiménz María, Bailón Martínez Eduardo, Morales Fernández José Miguel, Moreno Mantas Antonio, Del Toro Iniesta Jose Carlos, Gandorfer Achim, Feller Alex
Appl Opt. 2022 Nov 10;61(32):9716-9736. doi: 10.1364/AO.472516.
The Sunrise chromospheric infrared spectropolarimeter (SCIP) installed in the international balloon experiment sunrise iii will perform spectropolarimetric observations in the near-infrared band to measure solar photospheric and chromospheric magnetic fields simultaneously. The main components of SCIP for polarization measurements are a rotating wave plate, polarization beam splitters, and CMOS imaging sensors. In each of the sensors, SCIP records the orthogonal linearly polarized components of light. The polarization is later demodulated on-board. Each sensor covers one of the two distinct wavelength regions centered at 770 and 850 nm. To retrieve the proper circular polarization, the new parameter , defined as the 45° phase shifted component of Stokes in the modulation curve, is introduced. SCIP is aimed at achieving high polarization precision (1<3×10 of continuum intensity) to capture weak polarization signals in the chromosphere. The objectives of the polarization calibration test presented in this paper are to determine a response matrix of SCIP and to measure its repeatability and temperature dependence to achieve the required polarization precision. Tolerances of the response matrix elements were set after considering typical photospheric and chromospheric polarization signal levels. We constructed a feed optical system such that a telecentric beam can enter SCIP with the same -number as the light distribution instrument of the sunrise iii telescope. A wire-grid linear polarizer and achromatic wave plate were placed before SCIP to produce the known polarization. The obtained response matrix was close to the values expected from the design. The wavelength and spatial variations, repeatability, and temperature dependence of the response matrix were confirmed to be smaller than tolerances.
安装在国际气球实验“日出三号”上的日出色球层红外光谱偏振仪(SCIP)将在近红外波段进行光谱偏振观测,以同时测量太阳光球层和色球层的磁场。用于偏振测量的SCIP的主要组件包括一个旋转波片、偏振分束器和互补金属氧化物半导体(CMOS)成像传感器。在每个传感器中,SCIP记录光的正交线偏振分量。偏振随后在机载设备上进行解调。每个传感器覆盖以770纳米和850纳米为中心的两个不同波长区域之一。为了获取适当的圆偏振,引入了新参数 ,定义为调制曲线中斯托克斯 的45°相移分量。SCIP旨在实现高偏振精度(连续强度的1<3×10 ),以捕获色球层中的微弱偏振信号。本文提出的偏振校准测试的目标是确定SCIP的响应矩阵,并测量其重复性和温度依赖性,以达到所需的偏振精度。在考虑了典型的光球层和色球层偏振信号水平后,设定了响应矩阵元素的公差。我们构建了一个馈送光学系统,使得远心光束能够以与“日出三号”望远镜的光分布仪器相同的 数进入SCIP。在SCIP之前放置了一个线栅线性偏振器和消色差波片,以产生已知的偏振。获得的响应矩阵接近设计预期的值。响应矩阵的波长和空间变化、重复性以及温度依赖性被证实小于公差。