{"title":"利用傅立叶变换光谱仪实现太阳 10 cm s-1 径向速度精度","authors":"M. Debus, Sebastian Schäfer, Ansgar Reiners","doi":"10.1117/1.JATIS.9.4.045003","DOIUrl":null,"url":null,"abstract":"Abstract. The Institute for Astrophysics and Geophysics solar observatory is producing high-fidelity, ultra-high-resolution spectra (R > 500000) of the spatially resolved surface of the Sun using a Fourier transform spectrometer (FTS). The radial velocity (RV) calibration of these spectra is currently performed using absorption lines from Earth’s atmosphere, limiting the precision and accuracy. To improve the frequency calibration precision and accuracy, we use a Fabry–Pérot etalon (FP) setup that is an evolution of the CARMENES FP design and an iodine cell in combination. To create an accurate wavelength solution, the iodine cell is measured in parallel with the FP. The FP is then used to transfer the accurate wavelength solution provided by the iodine via a simultaneous calibration of solar observations. To verify the stability and precision of the FTS, we perform parallel measurements of the FP and an iodine cell. The measurements show an intrinsic stability of the FTS of a level of 1 m s − 1 over 90 h. The difference between the FP RVs and the iodine cell RVs show no significant trends during the same time span. The root mean square of the RV difference between the FP and iodine cell is 10.7 cm s − 1, which can be largely attributed to the intrinsic RV precisions of the iodine cell and the FP (10.2 and 1.0 cm s − 1, respectively). This shows that we can calibrate the FTS to a level of 10 cm s − 1, competitive with current state-of-the-art precision RV instruments. Based on these results, we argue that the spectrum of iodine can be used as an absolute reference to reach an RV accuracy of 10 cm s − 1.","PeriodicalId":508807,"journal":{"name":"Journal of Astronomical Telescopes, Instruments, and Systems","volume":"98 1","pages":"045003 - 045003"},"PeriodicalIF":0.0000,"publicationDate":"2023-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Toward 10 cm s−1 radial velocity accuracy on the Sun using a Fourier transform spectrometer\",\"authors\":\"M. Debus, Sebastian Schäfer, Ansgar Reiners\",\"doi\":\"10.1117/1.JATIS.9.4.045003\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Abstract. The Institute for Astrophysics and Geophysics solar observatory is producing high-fidelity, ultra-high-resolution spectra (R > 500000) of the spatially resolved surface of the Sun using a Fourier transform spectrometer (FTS). The radial velocity (RV) calibration of these spectra is currently performed using absorption lines from Earth’s atmosphere, limiting the precision and accuracy. To improve the frequency calibration precision and accuracy, we use a Fabry–Pérot etalon (FP) setup that is an evolution of the CARMENES FP design and an iodine cell in combination. To create an accurate wavelength solution, the iodine cell is measured in parallel with the FP. The FP is then used to transfer the accurate wavelength solution provided by the iodine via a simultaneous calibration of solar observations. To verify the stability and precision of the FTS, we perform parallel measurements of the FP and an iodine cell. The measurements show an intrinsic stability of the FTS of a level of 1 m s − 1 over 90 h. The difference between the FP RVs and the iodine cell RVs show no significant trends during the same time span. The root mean square of the RV difference between the FP and iodine cell is 10.7 cm s − 1, which can be largely attributed to the intrinsic RV precisions of the iodine cell and the FP (10.2 and 1.0 cm s − 1, respectively). This shows that we can calibrate the FTS to a level of 10 cm s − 1, competitive with current state-of-the-art precision RV instruments. Based on these results, we argue that the spectrum of iodine can be used as an absolute reference to reach an RV accuracy of 10 cm s − 1.\",\"PeriodicalId\":508807,\"journal\":{\"name\":\"Journal of Astronomical Telescopes, Instruments, and Systems\",\"volume\":\"98 1\",\"pages\":\"045003 - 045003\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2023-10-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Astronomical Telescopes, Instruments, and Systems\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1117/1.JATIS.9.4.045003\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Astronomical Telescopes, Instruments, and Systems","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1117/1.JATIS.9.4.045003","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
摘要天体物理学和地球物理学研究所太阳观测站正在利用傅立叶变换光谱仪(FTS)制作高保真、超高分辨率的太阳表面空间分辨率光谱(R > 500000)。目前,这些光谱的径向速度(RV)校准是利用地球大气层的吸收线进行的,这限制了校准的精度和准确性。为了提高频率校准的精度和准确性,我们使用了法布里-佩罗等离子体(Fabry-Pérot etalon,FP)装置,它是 CARMENES FP 设计和碘池相组合的演化。为了创建精确的波长解决方案,碘电池与 FP 并行测量。然后,通过对太阳观测数据进行同步校准,利用 FP 转移碘提供的精确波长解决方案。为了验证 FTS 的稳定性和精确性,我们对 FP 和碘电池进行了并行测量。测量结果表明,在 90 小时内,FTS 的内在稳定性达到了 1 m s - 1 的水平。在相同的时间跨度内,FP RV 与碘池 RV 之间的差异没有显示出明显的趋势。FP 和碘池间 RV 差值的均方根为 10.7 cm s - 1,这主要归因于碘池和 FP 固有的 RV 精确度(分别为 10.2 和 1.0 cm s - 1)。这表明我们可以将 FTS 校准到 10 cm s - 1 的水平,与目前最先进的精密 RV 仪器相比具有竞争力。基于这些结果,我们认为碘的光谱可以作为绝对参考,以达到 10 cm s - 1 的 RV 精确度。
Toward 10 cm s−1 radial velocity accuracy on the Sun using a Fourier transform spectrometer
Abstract. The Institute for Astrophysics and Geophysics solar observatory is producing high-fidelity, ultra-high-resolution spectra (R > 500000) of the spatially resolved surface of the Sun using a Fourier transform spectrometer (FTS). The radial velocity (RV) calibration of these spectra is currently performed using absorption lines from Earth’s atmosphere, limiting the precision and accuracy. To improve the frequency calibration precision and accuracy, we use a Fabry–Pérot etalon (FP) setup that is an evolution of the CARMENES FP design and an iodine cell in combination. To create an accurate wavelength solution, the iodine cell is measured in parallel with the FP. The FP is then used to transfer the accurate wavelength solution provided by the iodine via a simultaneous calibration of solar observations. To verify the stability and precision of the FTS, we perform parallel measurements of the FP and an iodine cell. The measurements show an intrinsic stability of the FTS of a level of 1 m s − 1 over 90 h. The difference between the FP RVs and the iodine cell RVs show no significant trends during the same time span. The root mean square of the RV difference between the FP and iodine cell is 10.7 cm s − 1, which can be largely attributed to the intrinsic RV precisions of the iodine cell and the FP (10.2 and 1.0 cm s − 1, respectively). This shows that we can calibrate the FTS to a level of 10 cm s − 1, competitive with current state-of-the-art precision RV instruments. Based on these results, we argue that the spectrum of iodine can be used as an absolute reference to reach an RV accuracy of 10 cm s − 1.