Отрывок: we can write (9) in the following form: ( ) { } { }С y U exp Λy c exp Λy cλ + − = + And the derivative form: { } { }С U Λ exp Λy c Λ exp Λy cy λ + − ∂ = + ∂ Initial conditions for an incident light for first filter layer: ( ) ( ) ( ) ( ) 0 0 0 0 С U c c f С U Λc Λc g y λ λ + − + − = + = ∂ = − = ∂ (10) Constants are derived as follows: ( ) ( ) ( )( ) ( ) ( ) ( )( ) 11 11 1 11 11 1 0 0 0 0 c E ...
Полная запись метаданных
Поле DC | Значение | Язык |
---|---|---|
dc.contributor.author | Strelkov, Yu.S. | - |
dc.contributor.author | Butt, M.A. | - |
dc.date.accessioned | 2018-05-22 10:10:09 | - |
dc.date.available | 2018-05-22 10:10:09 | - |
dc.date.issued | 2018 | - |
dc.identifier | Dspace\SGAU\20180519\69700 | ru |
dc.identifier.citation | Strelkov Yu.S. Modeling of a Fabry-Perot filter based on TiO2 and air gap by using Eigenvectors and Eigenvalues approach / Yu.S. Strelkov, M.A. Butt // Сборник трудов IV международной конференции и молодежной школы «Информационные технологии и нанотехнологии» (ИТНТ-2018) - Самара: Новая техника, 2018. - С.443-447. | ru |
dc.identifier.uri | http://repo.ssau.ru/handle/Informacionnye-tehnologii-i-nanotehnologii/Modeling-of-a-FabryPerot-filter-based-on-TiO2-and-air-gap-by-using-Eigenvectors-and-Eigenvalues-approach-69700 | - |
dc.description.abstract | We used Eigenvectors and Eigenvalues method to obtain transmittance coefficients for each of an interference filter. The filter is based on titanium dioxide layer (n=2.26) and air (n=1.0). The transmission spectra of the FP filter in mid- IR region shows a characteristic peak with a maximum of 86 % at 4.70 μm which is the fundamental absorption wavelength of CO which makes it possible to work as a gas sensor. The layers are horizontally stacked on one side which makes it possible to use air as a low index material. This gives an opportunity to deposit high index material in single deposition step which transforms the layer thickness into line thickness. As a result complex filter designs can be fabricated with simple and low production cost. | ru |
dc.description.sponsorship | This work was supported by the Federal Agency of Scientific Organizations (agreement No 007-ГЗ/Ч3363/26). | ru |
dc.language.iso | en | ru |
dc.publisher | Новая техника | ru |
dc.subject | Fabry-Perot filter | ru |
dc.subject | spectral filter | ru |
dc.subject | air gap | ru |
dc.subject | Eigenvectors | ru |
dc.subject | Eigenvalues | ru |
dc.title | Modeling of a Fabry-Perot filter based on TiO2 and air gap by using Eigenvectors and Eigenvalues approach | ru |
dc.type | Article | ru |
dc.textpart | we can write (9) in the following form: ( ) { } { }С y U exp Λy c exp Λy cλ + − = + And the derivative form: { } { }С U Λ exp Λy c Λ exp Λy cy λ + − ∂ = + ∂ Initial conditions for an incident light for first filter layer: ( ) ( ) ( ) ( ) 0 0 0 0 С U c c f С U Λc Λc g y λ λ + − + − = + = ∂ = − = ∂ (10) Constants are derived as follows: ( ) ( ) ( )( ) ( ) ( ) ( )( ) 11 11 1 11 11 1 0 0 0 0 c E ... | - |
Располагается в коллекциях: | Информационные технологии и нанотехнологии |
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