A Fabry-Perot interferometer with wire-grid polarizers as beamsplitters at terahertz frequencies; Review of Scientific Instruments; Vol. 89, iss. 3

Bibliografiset tiedot
Parent link:Review of Scientific Instruments
Vol. 89, iss. 3.— 2018.— [035116, 9 p.]
Yhteisötekijä: Национальный исследовательский Томский политехнический университет Физико-технический институт Кафедра прикладной физики (№ 12) Международная научно-образовательная лаборатория "Рентгеновская оптика"
Muut tekijät: Harrison H., Lancaster J. Andrew, Konoplev I. V. Ivan Vasiljevich, Doucas G. George, Aryshev A. S. Aleksandr Sergeevich, Shevelev M. V. Mihail Viktorovich, Terunuma N. Nobihiro, Urakawa Ju. Junji, Huggard P. G. Peter
Yhteenveto:Title screen
The design of a compact Fabry-Perot interferometer (FPi) and results of the experimental studies ´ carried out using the device are presented. Our FPi uses freestanding wire-grid polarizers (WGPs) as beamsplitters and is suitable for use at terahertz (THz) frequencies. The FPi was studied at the LUCX facility, KEK, Japan, and an 8 MeV linear electron accelerator was used to generate coherent Smith-Purcell radiation. The FPi was designed to be easy to align and reposition for experiments at linear accelerator facilities. All of the components used were required to have a flat or well understood frequency response in the THz range. The performance of the FPi with WGPs was compared to that of a Michelson interferometer and the FPi is seen to perform well. The effectiveness of the beamsplitters used in the FPi is also investigated. Measurements made with the FPi using WGPs, the preferred beamsplitters, are compared to measurements made with the FPi using silicon wafers as alternative beamsplitters. The FPi performs well with both types of beamsplitter in the frequency range used (0.3-0.5 THz). The successful measurements taken with the FPi demonstrate a compact and adaptable interferometer that is capable of analyzing THz radiation over a broad frequency range. The scheme is particularly well suited for polarization studies of THz radiation produced in an accelerator environment.
Режим доступа: по договору с организацией-держателем ресурса
Kieli:englanti
Julkaistu: 2018
Aiheet:
Linkit:https://doi.org/10.1063/1.5018400
Aineistotyyppi: Elektroninen Kirjan osa
KOHA link:https://koha.lib.tpu.ru/cgi-bin/koha/opac-detail.pl?biblionumber=665870

MARC

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200 1 |a A Fabry-Perot interferometer with wire-grid polarizers as beamsplitters at terahertz frequencies  |f H. Harrison, J. Lancaster, I. V. Konoplev [et al.] 
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330 |a The design of a compact Fabry-Perot interferometer (FPi) and results of the experimental studies ´ carried out using the device are presented. Our FPi uses freestanding wire-grid polarizers (WGPs) as beamsplitters and is suitable for use at terahertz (THz) frequencies. The FPi was studied at the LUCX facility, KEK, Japan, and an 8 MeV linear electron accelerator was used to generate coherent Smith-Purcell radiation. The FPi was designed to be easy to align and reposition for experiments at linear accelerator facilities. All of the components used were required to have a flat or well understood frequency response in the THz range. The performance of the FPi with WGPs was compared to that of a Michelson interferometer and the FPi is seen to perform well. The effectiveness of the beamsplitters used in the FPi is also investigated. Measurements made with the FPi using WGPs, the preferred beamsplitters, are compared to measurements made with the FPi using silicon wafers as alternative beamsplitters. The FPi performs well with both types of beamsplitter in the frequency range used (0.3-0.5 THz). The successful measurements taken with the FPi demonstrate a compact and adaptable interferometer that is capable of analyzing THz radiation over a broad frequency range. The scheme is particularly well suited for polarization studies of THz radiation produced in an accelerator environment. 
333 |a Режим доступа: по договору с организацией-держателем ресурса 
461 |t Review of Scientific Instruments 
463 |t Vol. 89, iss. 3  |v [035116, 9 p.]  |d 2018 
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701 1 |a Lancaster  |b J.  |g Andrew 
701 1 |a Konoplev  |b I. V.  |g Ivan Vasiljevich 
701 1 |a Doucas  |b G.  |g George 
701 1 |a Aryshev  |b A. S.  |g Aleksandr Sergeevich 
701 1 |a Shevelev  |b M. V.  |c physicist  |c research engineer of Tomsk Polytechnic University  |f 1985-  |g Mihail Viktorovich  |3 (RuTPU)RU\TPU\pers\31529 
701 1 |a Terunuma  |b N.  |g Nobihiro 
701 1 |a Urakawa  |b Ju.  |g Junji 
701 1 |a Huggard  |b P. G.  |g Peter 
712 0 2 |a Национальный исследовательский Томский политехнический университет  |b Физико-технический институт  |b Кафедра прикладной физики (№ 12)  |b Международная научно-образовательная лаборатория "Рентгеновская оптика"  |3 (RuTPU)RU\TPU\col\19530 
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