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1.
Opt Express ; 27(7): 9933-9940, 2019 Apr 01.
Artículo en Inglés | MEDLINE | ID: mdl-31045140

RESUMEN

Development of the wideband and tunable quasi-optic terahertz (THz) components is in high demand. In this work, we demonstrate a tunable achromatic quarter-wave plate (AQWP) for the THz frequency range. The phase retardation of this device can be set at 90° ± 9° from 0.20 to 0.50 THz. The operation range from 0.20 to 0.50 THz can be tuned to from 0.30 to 0.70 THz by introducing three nematic liquid crystals phase retarders, of which the birefringence can be magnetically tuned. The frequency-dependent phase retardation is in good agreement with theoretical predictions.

2.
Opt Lett ; 33(13): 1401-3, 2008 Jul 01.
Artículo en Inglés | MEDLINE | ID: mdl-18594645

RESUMEN

A broadly tunable terahertz Solc-type birefringence filter is demonstrated. The first central passband frequency of the filter can be continuously tuned from 0.176 to 0.793 THz using magnetically controlled birefringence in nematic liquid crystals. The insertion loss of the present device is about 5 dB.

3.
Opt Lett ; 33(11): 1174-6, 2008 Jun 01.
Artículo en Inglés | MEDLINE | ID: mdl-18516164

RESUMEN

A Feussner-type terahertz polarizer with a nematic liquid crystal (NLC) layer between two fused-silica prisms is demonstrated. The polarization factor and extinction ratio of the NLC-based terahertz polarizer can exceed 0.99 and 10(-5), respectively.

4.
Opt Express ; 16(5): 2995-3001, 2008 Mar 03.
Artículo en Inglés | MEDLINE | ID: mdl-18542385

RESUMEN

This investigation demonstrates the feasibility of a magnetically tunable liquid crystal phase grating for the terahertz wave. The phase grating can be used as a beam splitter. The ratio of the zeroth and first-order diffracted THz-beams (0.3 THz) polarized in a direction perpendicular to that of the grooves of the grating can be tuned from 4:1 to 1:2. When the THz wave is polarized in any other direction, this device can be operated as a polarizing beam splitter.


Asunto(s)
Cristales Líquidos/química , Cristales Líquidos/efectos de la radiación , Microondas , Refractometría/instrumentación , Diseño de Equipo , Análisis de Falla de Equipo , Estudios de Factibilidad , Rayos Infrarrojos , Refractometría/métodos
5.
Opt Lett ; 31(8): 1112-4, 2006 Apr 15.
Artículo en Inglés | MEDLINE | ID: mdl-16625920

RESUMEN

Phase shift exceeding tau/2 at 1 THz is demonstrated by using electrically controlled birefringence in a homeotropically aligned nematic liquid crystal (E7) cell, 570 microm in thickness. The driving voltage required for a phase shift of 90 degrees is 125 V (rms). We demonstrate that the phase shifter works as an electrically switchable quarter-wave plate at 1 THz. The device can also be used as an electrically tuned phase compensator around the quarter-wave point near 1 THz.

6.
Opt Express ; 13(11): 3921-30, 2005 May 30.
Artículo en Inglés | MEDLINE | ID: mdl-19495301

RESUMEN

We demonstrate frequency tuning of enhanced THz radiation transmitted through a two-dimensional metallic hole array (2D-MHA) by controlling the index of refraction of the medium filling the holes and adjacent to the 2D-MHA on one side. The medium is a nematic liquid crystal (NLC) and its index of refraction is varied using magnetically controlled birefringence of the NLC. With the NLC, the peak transmission frequency of the 2D-MHA shift to the red by 0.112 THz and can be tuned from 0.193 to 0.188 THz. The peak transmittance is as high as 70% or an enhancement of 2.42 times, considering the porosity of the 2D-MHA. As a tunable THz filter, this device exhibits a continuous tuning range of 4.7 GHz , a low insertion loss of 2.35 to 1.55 dB and a quality factor of ~ 4-5.

7.
Opt Express ; 12(12): 2625-30, 2004 Jun 14.
Artículo en Inglés | MEDLINE | ID: mdl-19475103

RESUMEN

Tunable phase shift up to 360 degrees at 1 THz is achieved with a liquid crystal (LC) device. The key to this design is (1) the use of a nematic LC, E7, which exhibits a birefringence of ~ 0.17 (0.2 - 1.2 THz); (2) a LC cell (3-mm in thickness) with sandwiched structure to increase the interaction length while minimizing interface Fresnel losses; and (3) the use of magnetic field to align the thick LC cell and achieve continuous tuning of phase from 0 to 360 degrees . This device can be operated over a broad range near room temperature.

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