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1

Chu, Benjamin, Renliang Xu, Tadakazu Maeda, and H. S. Dhadwal. "Prism laser light‐scattering spectrometer." Review of Scientific Instruments 59, no. 5 (May 1988): 716–24. http://dx.doi.org/10.1063/1.1139816.

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2

Choi, Sunwoong, Youngsik Kim, Jae-Hyung Lee, Hanjong You, Byung-Jun Jang, and Kyeong-Hoon Jung. "Minimizing Device-to-Device Variation in the Spectral Response of Portable Spectrometers." Journal of Sensors 2019 (January 28, 2019): 1–7. http://dx.doi.org/10.1155/2019/8392583.

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As portable spectrometers have been developed, the research of spectral analysis has evolved from a traditional laboratory-based closed environment to a network-connected open environment. Consequently, its application areas are expanding in combination with machine learning techniques. The device-to-device variation in the spectral response of portable spectrometers is a critical issue in a machine learning-based service scenario since the classification performance is highly dependent on the consistency of spectral responses from each spectrometer. To minimize device-to-device variation, a cuboid prism is employed instead of a combination of mirrors and prism to construct an optical system for the spectrometer. The spectral responses are calibrated to correct pixel shift on the image sensor. Experimental results show that the proposed method can minimize the device-to-device variation in spectral response of portable spectrometers.
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3

Hwang, Ling Chin, Marcel Leutenegger, Michael Gösch, Theo Lasser, Per Rigler, Wolfgang Meier, and Thorsten Wohland. "Prism-based multicolor fluorescence correlation spectrometer." Optics Letters 31, no. 9 (May 1, 2006): 1310. http://dx.doi.org/10.1364/ol.31.001310.

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4

Huang, Chu-Yu, and Wei-Chih Wang. "Birefringent prism based Fourier transform spectrometer." Optics Letters 37, no. 9 (May 1, 2012): 1559. http://dx.doi.org/10.1364/ol.37.001559.

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5

Narusawa, Fumio, Masayuki Harano, and Mitsuyoshi Tanaka. "Simplified spectrometer consisted of prism and CCD." JOURNAL OF THE ILLUMINATING ENGINEERING INSTITUTE OF JAPAN 78, Appendix (1994): 310. http://dx.doi.org/10.2150/jieij1980.78.appendix_310.

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6

Gruber, Alicia D., and Russell J. Hamilton. "Improvements in a simply constructed prism spectrometer." Physics Education 27, no. 1 (January 1992): 31–34. http://dx.doi.org/10.1088/0031-9120/27/1/007.

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7

Jung, Dong Geon, Su Hee Son, Sun Young Kwon, Jun Yeop Lee, and Seong Ho Kong. "Silicon Prism-based NIR Spectrometer Utilizing MEMS Technology." Journal of Sensor Science and Technology 26, no. 2 (March 31, 2017): 91–95. http://dx.doi.org/10.5369/jsst.2017.26.2.91.

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8

WANG Xin, 王欣, 丁学专 DING Xue-zhuan, 杨波 YANG Bo, 刘银年 LIU Yin-nian, and 王建宇 WANG Jian-yu. "Optical Design and Spectral Calculation of Prism Spectrometer." ACTA PHOTONICA SINICA 39, no. 7 (2010): 1334–39. http://dx.doi.org/10.3788/gzxb20103907.1334.

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9

Moyssides, P. G., S. Maltezos, and E. Fokitis. "A VUV prism spectrometer for RICH radiator refractometry." Journal of Modern Optics 47, no. 10 (August 2000): 1693–706. http://dx.doi.org/10.1080/09500340008231418.

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10

Meijer, A. S., J. J. H. Pijpers, H. K. Nienhuys, M. Bonn, and W. J. van der Zande. "A THz spectrometer based on a CsI prism." Journal of Optics A: Pure and Applied Optics 10, no. 9 (September 1, 2008): 095303. http://dx.doi.org/10.1088/1464-4258/10/9/095303.

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11

Tur’yanskii, A. G. "Ultimate characteristics of an X-ray prism spectrometer." Instruments and Experimental Techniques 52, no. 4 (July 2009): 587–94. http://dx.doi.org/10.1134/s0020441209040216.

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12

Lin, Xuling, Feng Zhou, Huan Li, and HaiBo Zhao. "Static Fourier-transform spectrometer based on Wollaston prism." Optik 125, no. 14 (July 2014): 3482–84. http://dx.doi.org/10.1016/j.ijleo.2014.01.062.

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13

Jiang, X. G. "Optimization and testing of an imaging energy spectrometer for high-resolution electron-energy-loss microanalysis." Proceedings, annual meeting, Electron Microscopy Society of America 51 (August 1, 1993): 644–45. http://dx.doi.org/10.1017/s0424820100149052.

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Electron energy loss (EEL) microanalysis is a powerful technique for studying the chemical composition of a specimen and the distribution of each constituent. The energy loss spectrum of the post-specimen electron beam, on which the technique is based, is obtained by the use of an energy spectrometer. In transmission electron microscopy, the most prevalent type of imaging energy spectrometer is the Prism-Mirror-Prism (PMP) design (Fig. 1). It is compact in size and easy to align. For an acceptance half angle (β in Fig. 1) of 10 mradian, which corresponds to the full field of view of a modified Siemens 102 microscope of our laboratory, an experimental PMP spectrometer with a straight-faced magnetic prism has an energy resolution of 25 eV at the microscope operating voltage of 80 kV. This resolution has permitted ionization energies of different elements to be resolved, thus making the elemental microanalysis possible. However, a resolution of 25 eV is inadequate for resolving and possibly imaging with characteristic molecular energy losses, that are located in the 1.5-10 eV region of the electron energy loss spectrum.
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14

Barfels, M. M. G., Y. Heng, and F. P. Ottensmeyer. "Molecular Imaging: Design of the PMP Imaging Spectrometer, Resolution Limits, and Radiation Sensitivity." Proceedings, annual meeting, Electron Microscopy Society of America 54 (August 11, 1996): 424–25. http://dx.doi.org/10.1017/s0424820100164581.

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One of the main applications of an energy filter is to obtain elemental distribution images by electron spectroscopic imaging. This technique has been pushed to the imaging of fine structure such as the sp2 and sp3 states of carbon at a sub-nanometer spatial resolution. However, low energy loss imaging in the region of the molecular excitations has largely remained unexplored due to the limitation in the energy resolution obtainable in the energy filters. Molecular absorptions in the visible and UV regions of the spectrum occur at 1.5 eV to 10 eV. Thus it would be necessary to have an energy resolution of about 1 eV or better.An optimized Prism-Mirror-Prism energy filter has been built by altering the straight faced pole pieces to circular curvatures. See Figure 1. The optimum curvatures for each of the faces were determined iteratively. In order to simulate the electron path accurately through the Prism-Mirror-Prism filter, it was necessary to calculate the magnetic fringing fields using the Boundary Element Method as outlined by Kasper. The ray-tracing procedure indicated a theoretical energy resolution of 1.3 eV for the optimized magnetic prism. This has been tested on our prototype spectrometer currently installed in the Siemens EM 102. An energy resolution of 1.1 eV was obtained.
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15

McMath, T. A., and Mario Glavacic. "A fast and accurate technique with the prism spectrometer." Physics Teacher 26, no. 7 (October 1988): 461–63. http://dx.doi.org/10.1119/1.2342576.

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16

Kudenov, Michael W. "Faceted grating prism for a computed tomographic imaging spectrometer." Optical Engineering 51, no. 4 (April 19, 2012): 044002. http://dx.doi.org/10.1117/1.oe.51.4.044002.

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17

Civitci, F., M. Hammer, and H. J. W. M. Hoekstra. "Planar prism spectrometer based on adiabatically connected waveguiding slabs." Optics Communications 365 (April 2016): 29–37. http://dx.doi.org/10.1016/j.optcom.2015.11.066.

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18

Kaan Cetindag, S., M. Fatih Toy, Onur Ferhanoglu, and Fehmi Civitci. "A Speckle-Enhanced Prism Spectrometer With High Dynamic Range." IEEE Photonics Technology Letters 30, no. 24 (December 15, 2018): 2139–42. http://dx.doi.org/10.1109/lpt.2018.2879247.

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19

Tang, Ziyao, and Herbert Gross. "Improved correction by freeform surfaces in prism spectrometer concepts." Applied Optics 60, no. 2 (January 6, 2021): 333. http://dx.doi.org/10.1364/ao.412103.

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20

Pei Linlin, 裴琳琳, 相里斌 Xiangli Bin, 吕群波 Lü Qunbo, and 邵晓鹏 Shao Xiaopeng. "Multi-Slit Polarization Imaging Spectrometer Based on Double Amici Prism." Acta Optica Sinica 37, no. 11 (2017): 1122001. http://dx.doi.org/10.3788/aos201737.1122001.

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21

Feng, Lei, Jinsong Zhou, Bin Xiangli, Juanjuan Jing, Yacan Li, Xiaoying He, Lei Yang, and Lidong Wei. "Design of a nonlinearity-corrected spectrometer based on curved prism." Optics Communications 434 (March 2019): 239–45. http://dx.doi.org/10.1016/j.optcom.2018.11.008.

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22

Beynon, John. "Comments on Schuster''s technique for focusing the prism spectrometer." Physics Education 26, no. 1 (January 1991): 66–68. http://dx.doi.org/10.1088/0031-9120/26/1/011.

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23

Yuan, Liyin, Jia’nan Xie, Zhiping He, Yueming Wang, and Jianyu Wang. "Optical design and evaluation of airborne prism-grating imaging spectrometer." Optics Express 27, no. 13 (June 12, 2019): 17686. http://dx.doi.org/10.1364/oe.27.017686.

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24

Wei, Lidong, Jinsong Zhou, Yacan Li, Lei Feng, Juanjuan Jing, Lei Yang, Boyang Nie, Li Xu, and Xiaoying He. "Wide-field grating-prism imaging spectrometer: optical design and implementation." Applied Optics 60, no. 24 (August 12, 2021): 7136. http://dx.doi.org/10.1364/ao.431143.

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25

Davis, J. A., R. G. Garces, J. Y. Diao, and F. P. Ottensmeyer. "Localization of Green Fluorescent Protein Absorbance by Energy Filtered Transmission Electron Microscopy." Microscopy and Microanalysis 6, S2 (August 2000): 324–25. http://dx.doi.org/10.1017/s1431927600034115.

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Energy filtered transmission electron microscopy has the potential to provide high resolution, spatially resolved, atomic and chemical information. However, aberrations generated by the electron spectrometer blur the energy resolution and limit the atomic or molecular distributions that can be studied. Energy absorptions corresponding to the visible light range fall below an energy loss of 5 eV. The selection of electrons that have lost an amount of energy corresponding to chromophore absorption by the sample thus requires a spectrometer with a high energy resolution over the full image plane. A corrected prism-mirror-prism filter that has a resolution of 1.1 eV, sufficient to select these low energy loss electrons, was developed and installed by us in a Zeiss EM902. Its imaging capability was verified for a number of different chromophores. The chromophore currently under study is that of the green fluorescent protein (GFP).
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26

Okamoto, Takayuki, Satoshi Kawata, and Shigeo Minami. "A Photodiode Array Fourier Transform Spectrometer Based on a Birefringent Interferometer." Applied Spectroscopy 40, no. 5 (July 1986): 691–95. http://dx.doi.org/10.1366/0003702864508494.

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A new version of the photodiode array Fourier transform spectrometer for visible spectroscopy is described. In this version, a birefringent interferometer with a Wollaston prism produces a spatial interferogram of the radiation, which is detected by a linear photodiode array. In addition to the merit of having no mechanical moving parts, this spectrometer has the beneficial advantage of the simple and rugged optical setup and alignment due to its common-path and in-line interferometer formation. These advantages lend this spectrometer to field-use applications. Emission spectra of a low-pressure mercury lamp and a light-emitting diode and an absorption spectrum of a didymium glass filter measured by the developed spectrometer are presented.
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27

Bai Xin, 白鑫, 吴海英 Wu Haiying, 李艳 Li Yan, and 郭晓虹 Guo Xiaohong. "Transmission Ratio of Glan-Taylor Prism in Polarization Interference Imaging Spectrometer." Laser & Optoelectronics Progress 51, no. 5 (2014): 053001. http://dx.doi.org/10.3788/lop51.053001.

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28

Chen Yang, 陈杨, and 王跃明 Wang Yueming. "Optical Design of Prism Spectrometer System with a Small Incident Angle." Acta Optica Sinica 33, no. 9 (2013): 0922002. http://dx.doi.org/10.3788/aos201333.0922002.

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29

Chen Hongfu, 陈洪福, 巩岩 Gong Yan, 骆聪 Luo Cong, and 彭建涛 Peng Jiantao. "Design of Prism-Grating Imaging Spectrometer with Eliminating Spectral Line Curvature." Acta Optica Sinica 34, no. 9 (2014): 0922004. http://dx.doi.org/10.3788/aos201434.0922004.

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30

Chen, Jianjun, Jin Yang, Jianan Liu, Jianli Liu, Ci Sun, Xiaotian Li, Bayanheshig, and Jicheng Cui. "Optical design of a short-wave infrared prism-grating imaging spectrometer." Applied Optics 57, no. 34 (August 23, 2018): F8. http://dx.doi.org/10.1364/ao.57.0000f8.

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31

Gall, L. N., E. M. Yakushev, L. M. Nazarenko, A. S. Antonov, A. A. Semenov, and N. R. Gall. "A Prism Mass-Spectrometer for Isotope Analysis of Hydrogen–Helium Mixtures." Technical Physics Letters 44, no. 7 (July 2018): 646–49. http://dx.doi.org/10.1134/s1063785018070209.

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32

Gao, Zhenyu, Ruidong Jia, Hao Zhang, Zhiwei Xia, and Wei Fang. "Simulation and Analysis of Spectral Response Function and Bandwidth of Spectrometer." International Journal of Aerospace Engineering 2016 (2016): 1–8. http://dx.doi.org/10.1155/2016/2759121.

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A simulation method for acquiring spectrometer’s Spectral Response Function (SRF) based on Huygens Point Spread Function (PSF) is suggested. Taking into account the effects of optical aberrations and diffraction, the method can obtain the fine SRF curve and corresponding spectral bandwidth at any nominal wavelength as early as in the design phase. A prism monochromator is proposed for illustrating the simulation procedure. For comparison, a geometrical ray-tracing method is also provided, with bandwidth deviations varying from 5% at 250 nm to 25% at 2400 nm. Further comparison with reported experiments shows that the areas of the SRF profiles agree to about 1%. However, the weak scattered background light on the level of 10−4 to 10−5 observed by experiment could not be covered by this simulation. This simulation method is a useful tool for forecasting the performance of an underdesigned spectrometer.
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33

Jia-lun, ZHANG, ZHENG Yu-quan, LIN Chao, and JI Zhen-hua. "Design of a freeform curved prism imaging spectrometer based on an anastigmatism." Chinese Optics 13, no. 4 (2020): 842–51. http://dx.doi.org/10.37188/co.2019-0049.

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34

Feng Yutao, 冯玉涛, 白清兰 Bai Qinglan, 王咏梅 Wang Yongmei, 胡炳樑 Hu Bingliang, and 王姝娜 Wang Shu′na. "Theory and Method for Designing Field-Widened Prism of Spatial Heterodyne Spectrometer." Acta Optica Sinica 32, no. 10 (2012): 1030001. http://dx.doi.org/10.3788/aos201232.1030001.

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35

Zhang Hao, 张浩, 方伟 Fang Wei, 叶新 Ye Xin, and 张广伟 Zhang Guangwei. "Design of Prism Spectrometer with Wide Spectral Coverage for Solar Spectrum Measurement." Acta Optica Sinica 33, no. 2 (2013): 0222001. http://dx.doi.org/10.3788/aos201333.0222001.

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36

Sun, Ci, Mingjia Wang, Jicheng Cui, Xuefeng Yao, and Jianjun Chen. "Comparison and analysis of wavelength calibration methods for prism – Grating imaging spectrometer." Results in Physics 12 (March 2019): 143–46. http://dx.doi.org/10.1016/j.rinp.2018.11.062.

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37

Liu, Jianan, Jianjun Chen, Jianli Liu, Shulong Feng, Xiaotian Li, and Jicheng Cui. "Optical design of a prism–grating-based lenslet array integral field spectrometer." Optics Express 26, no. 15 (July 18, 2018): 19456. http://dx.doi.org/10.1364/oe.26.019456.

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38

Komisarek, Dan, Karl Reichard, Dan Merdes, Dan Lysak, Philip Lam, Shudong Wu, and Shizhuo Yin. "High-performance nonscanning Fourier-transform spectrometer that uses a Wollaston prism array." Applied Optics 43, no. 20 (July 9, 2004): 3983. http://dx.doi.org/10.1364/ao.43.003983.

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39

Rodionov, A. A., Yu L. Khazov, M. G. Maksimov, and Yu L. Kleiman. "Design of a prism beta spectrometer for operation in the PIK reactor." Measurement Techniques 40, no. 10 (October 1997): 1003–7. http://dx.doi.org/10.1007/bf02505116.

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40

Ahn, Channing C., and Ondrej L. Krivanek. "A parallel-detection electron spectrometer using quadrupole lenses." Proceedings, annual meeting, Electron Microscopy Society of America 44 (August 1986): 618–19. http://dx.doi.org/10.1017/s042482010014453x.

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Serial detection systems that are standardly employed in electron energy loss spectrometry (EELS) only examine one energy channel at a time and are therefore inherently inefficient. Parallel detection systems using either photodiode arrays or charge-coupled devices (CCDs) promise to remove this inefficiency. However, to completely replace the serial detection systems, they will need 1) a detective quantum efficiency (DQE) approaching 100%, 2) a dynamic range sufficient to cover the range of intensities encountered in the energy loss spectra (about 106), and 3) ability to operate without any loss in energy resolution.We have constructed and tested a parallel detection system which incorporates three quadrupole lenses placed after the magnetic sector prism of the Gatan 607 spectrometer, a single crystal YAG scintillator, and a fiber-optically coupled linear photodiode array. The quadrupoles magnify the small dispersion (1.8μm per eV at 100kV primary voltage) of the spectrum produced by the magnetic sector to as high as 1 mm per eV without producing any spectrum rotation and with small power requirements.
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41

Ishida, Hatsuo, Yuichi Ishino, Henry Buijs, Carl Tripp, and Michael J. Dignam. "Polarization-Modulation FT-IR Reflection Spectroscopy Using a Polarizing Michelson Interferometer." Applied Spectroscopy 41, no. 8 (November 1987): 1288–94. http://dx.doi.org/10.1366/0003702874447167.

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We report the first results obtained on a mid-IR FT spectrometer equipped with a polarizing Michelson interferometer (PMI), and the application examples of polarization spectroscopy are illustrated. A relatively simple method for conversion of a conventional instrument to PMI operation is designed. Specular reflection spectra of poly(vinyl acetate) film on copper and ATR spectra of a Langmuir-Blodgett film on silicon prism are presented.
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42

Zhang Rui, 张锐, 巴音贺希格 Bayanheshig, 杨晋 Yang Jin, 尹禄 Yin Lu, 崔继承 Cui Jicheng, and 李晓天 Li Xiaotian. "Reduction Model of the Transmission Prism Echelle Spectrometer with the C-T Structure." Acta Optica Sinica 36, no. 7 (2016): 0723001. http://dx.doi.org/10.3788/aos201636.0723001.

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43

Hueni, A., D. Schlaepfer, M. Jehle, and M. Schaepman. "Impacts of dichroic prism coatings on radiometry of the airborne imaging spectrometer APEX." Applied Optics 53, no. 24 (August 13, 2014): 5344. http://dx.doi.org/10.1364/ao.53.005344.

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44

Chu, Benjamin, Renliang Xu, and Sulong Nyeo. "Applications of Prism-Cell Light-Scattering Spectrometer to Particle Sizing in Polymer Solutions." Particle & Particle Systems Characterization 6, no. 1-4 (1989): 34–38. http://dx.doi.org/10.1002/ppsc.19890060105.

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45

Kiyokura, Takanori, Takahiro Ito, and Renshi Sawada. "Fourier Transform Near-Infrared Spectrometer Using a Corner-Cube Integrated Prism Scanning Interferometer." Applied Spectroscopy 58, no. 12 (December 2004): 1447–51. http://dx.doi.org/10.1366/0003702042641353.

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46

Ioanoviciu, D., and C. Cuna. "Resolution test of an electric prism—oblique incidence magnet double focusing mass spectrometer." International Journal of Mass Spectrometry and Ion Processes 74, no. 1 (December 1986): 129–31. http://dx.doi.org/10.1016/0168-1176(86)85026-1.

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47

Pei, Linlin, Bin Xiangli, Qunbo Lv, and Xiaopeng Shao. "Optical system design of the Dyson imaging spectrometer based on the Fery prism." Optical Review 23, no. 4 (July 5, 2016): 695–702. http://dx.doi.org/10.1007/s10043-016-0236-4.

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48

HERRALA, ESKO, and JUKKA OKKONEN. "IMAGING SPECTROGRAPH AND CAMERA SOLUTIONS FOR INDUSTRIAL APPLICATIONS." International Journal of Pattern Recognition and Artificial Intelligence 10, no. 01 (February 1996): 43–54. http://dx.doi.org/10.1142/s0218001496000050.

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An imaging spectrometer instrument based on a prism-grating-prism (PGP) element as the dispersive component and advanced camera solutions for on-line applications are presented. The PGP element uses a volume type holographic plane transmission grating made of dichromated gelatin (DCG). Currently, spectrographs have been realized for the 400–1050 nm region but applicable spectral region of the PGP is 380–1800 nm. Spectral resolution is typically between 1.5 and 5 nm. The on-axis optical configuration and simple rugged tubular optomechanical construction of the spectrograph provides a good image quality and resistance to harsh environmental conditions. Spectrograph optics are designed to be interfaced to any standard CCD camera. Special camera structures and operating modes can be used for applications requiring on-line data interpretation and process control.
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49

Basnayake, Ranil, Erik Bollt, Nicholas Tufillaro, Jie Sun, and Michelle Gierach. "Regularization destriping of remote sensing imagery." Nonlinear Processes in Geophysics 24, no. 3 (July 20, 2017): 367–78. http://dx.doi.org/10.5194/npg-24-367-2017.

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Abstract. We illustrate the utility of variational destriping for ocean color images from both multispectral and hyperspectral sensors. In particular, we examine data from a filter spectrometer, the Visible Infrared Imaging Radiometer Suite (VIIRS) on the Suomi National Polar Partnership (NPP) orbiter, and an airborne grating spectrometer, the Jet Population Laboratory's (JPL) hyperspectral Portable Remote Imaging Spectrometer (PRISM) sensor. We solve the destriping problem using a variational regularization method by giving weights spatially to preserve the other features of the image during the destriping process. The target functional penalizes the neighborhood of stripes (strictly, directionally uniform features) while promoting data fidelity, and the functional is minimized by solving the Euler–Lagrange equations with an explicit finite-difference scheme. We show the accuracy of our method from a benchmark data set which represents the sea surface temperature off the coast of Oregon, USA. Technical details, such as how to impose continuity across data gaps using inpainting, are also described.
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50

Sakaguchi, Miyuki, Tetsunari Kimura, Takuma Nishida, Takehiko Tosha, Hiroshi Sugimoto, Yoshihiro Yamaguchi, Sachiko Yanagisawa, et al. "A nearly on-axis spectroscopic system for simultaneously measuring UV–visible absorption and X-ray diffraction in the SPring-8 structural genomics beamline." Journal of Synchrotron Radiation 23, no. 1 (January 1, 2016): 334–38. http://dx.doi.org/10.1107/s1600577515018275.

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UV–visible absorption spectroscopy is useful for probing the electronic and structural changes of protein active sites, and thus the on-line combination of X-ray diffraction and spectroscopic analysis is increasingly being applied. Herein, a novel absorption spectrometer was developed at SPring-8 BL26B2 with a nearly on-axis geometry between the X-ray and optical axes. A small prism mirror was placed near the X-ray beamstop to pass the light only 2° off the X-ray beam, enabling spectroscopic analysis of the X-ray-exposed volume of a crystal during X-ray diffraction data collection. The spectrometer was applied to NO reductase, a heme enzyme that catalyzes NO reduction to N2O. Radiation damage to the heme was monitored in real time during X-ray irradiation by evaluating the absorption spectral changes. Moreover, NO binding to the heme was probedviacaged NO photolysis with UV light, demonstrating the extended capability of the spectrometer for intermediate analysis.
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