7 research outputs found
Study of terahertz spoof surface plasmons on subwavelength gratings with dielectric substance in grooves
Terahertz (THz) plasmonic devises based on periodical corrugated structures are promising for sensing applications in biology and medicine but have not been developed so far because spoof surface plasmons (SSPs) on such structures were studied insufficiently in the THz spectral range. In the paper, the propagation of THz SSPs along one-dimensional subwavelength rectangular plane gratings with a dielectric substance in the grooves was studied and optimal parameters of gratings (period, aspect ratio and groove depth) for sensing of dielectric were found. First grating samples were made and tested using the THz radiation of the Novosibirsk free electron laser.The investigations were supported by the Russian Science Foundation (grant No. 14-50-00080) and Russian Foundation for Basic Research (grant No. 16-32-00678). The Siberian Synchrotron and Terahertz Radiation Center equipment and free electron laser were employed in the experiments
Liga method of forming high-contrast collimators and anti-scatter grids with high aspect ratio
The article deals with creation and application of high-contrast anti-scatter X-ray grids for X-ray imaging in the range of 20β200 keV from microfocus X-ray tubes. A prototype high-aspect-ratio nickel grid structure is used to consider the impact of anti-scatter grid on the directional patterns of the IMA-2-150D X-ray tube. The suppression of scattered radiation and narrowing of the directional radiation pattern are demonstrated. The contrast of the nickel prototype is apparently insuffi cient. The article presents LIGA methods for manufacturing anti-scatter X-ray grids made of gold in Siberian Synchrotron and Terahertz Radiation Centre. A method for forming resistive grid structures using deep X-ray lithography is described and test structures are shown. The development of manufacturing technology for anti-scatter X-ray grids is in progress
Terahertz localized surface plasmons on subwave metal structures
ΠΠΎΠ·Π±ΡΠΆΠ΄Π΅Π½ΠΈΠ΅ ΠΌΡΠ»ΡΡΠΈΠΏΠΎΠ»ΡΠ½ΡΡ
Π»ΠΎΠΊΠ°Π»ΠΈΠ·ΠΎΠ²Π°Π½Π½ΡΡ
ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠ½ΡΡ
ΡΠ΅Π·ΠΎΠ½Π°Π½ΡΠΎΠ² (ΠΠΠ ) Π½Π° ΡΡΠ±Π²ΠΎΠ»Π½ΠΎΠ²ΡΡ
ΡΡΡΡΠΊΡΡΡΠ°Ρ
ΠΌΠΎΠΆΠ΅Ρ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎ ΡΠ°ΡΡΠΈΡΠΈΡΡ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΠΈ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΏΠ»Π°Π·ΠΌΠΎΠ½Π½ΡΡ
Π±ΠΈΠΎΡΠ΅Π½ΡΠΎΡΠΎΠ². Π ΡΠ°Π±ΠΎΡΠ΅ Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΡΠΈΡΠ»Π΅Π½Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΎ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΠΠ Π½Π° Π³ΠΎΡΡΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΠΌΠ΅ΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΈΡ
Π΄ΠΈΡΠΊΠ°Ρ
Π² ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΠΈ Ρ Π‘-ΠΎΠ±ΡΠ°Π·Π½ΡΠΌ ΡΠ΅Π·ΠΎΠ½Π°ΡΠΎΡΠΎΠΌ Π² ΠΈΠ½ΡΡΠ°ΠΊΡΠ°ΡΠ½ΠΎΠΌ ΠΈ ΡΠ΅ΡΠ°Π³Π΅ΡΡΠΎΠ²ΠΎΠΌ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π°Ρ
. ΠΠ°ΠΉΠ΄Π΅Π½Ρ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΡ ΡΡΡΡΠΊΡΡΡ, ΠΏΡΠΈ ΠΊΠΎΡΠΎΡΡΡ
Π²ΠΎΠ·Π±ΡΠΆΠ΄Π°ΡΡΡΡ ΠΌΡΠ»ΡΡΠΈΠΏΠΎΠ»ΡΠ½ΡΠ΅ ΡΠ΅Π·ΠΎΠ½Π°Π½ΡΡ. ΠΠΎΡΡΠ΄ΠΎΠΊ ΠΈ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΡ ΡΠ΅Π·ΠΎΠ½Π°Π½ΡΠ° Π·Π°Π²ΠΈΡΡΡ ΠΎΡ Π²Π΅Π»ΠΈΡΠΈΠ½Ρ Π΄ΠΈΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΏΡΠΎΠ½ΠΈΡΠ°Π΅ΠΌΠΎΡΡΠΈ ΠΌΠ΅ΡΠ°Π»Π»Π°. Excitation of multipole localized surface plasmon resonances (SPR) can greatly expand the potential of application of plasmonic biosensors. In the paper we studied the SPR on corrugated metal disks in conjunction with a C-shaped resonator in the infrared and terahertz ranges using numerical simulations. The parameters of the structures for which
multipole resonances are excited were found. The order and intensity of the resonances
depends on the dielectric permittivity of the metal.Π Π°Π±ΠΎΡΠ° Π²ΡΠΏΠΎΠ»Π½Π΅Π½Π° ΠΏΡΠΈ ΠΏΠΎΠ΄Π΄Π΅ΡΠΆΠΊΠ΅ Π³ΡΠ°Π½ΡΠ° Π ΠΠ€ (No 14-50-00080, Π° ΡΠ°ΠΊΠΆΠ΅ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΎΠ±ΠΎΡΡΠ΄ΠΎΠ²Π°Π½ΠΈΡ ΠΠΎΠ²ΠΎΡΠΈΠ±ΠΈΡΡΠΊΠΎΠ³ΠΎ Π¦ΠΠ Π¦Π‘Π’Π