We demonstrated terahertz wave parametric wavelength conversion between frequency controlled infrared (stabilized pumping and tunable seeding) beams and terahertz wave in a nonlinear crystal. The pumping beam is generated using a PPLN-OPG seeded by a stabilized laser beam as traceable to the national standard. The generated pulses are amplified by a KTA-OPA pumped by a SLM Nd:YAG MOPA system. The wavelength of seeding beam is monitored by a “spectral drill” cavity as intensity error signal. We expect that these methods will open up new fields.
We demonstrated frequency controlled terahertz wave generation based on parametric wavelength conversion in a nonlinear MgO:LiNbO3 crystal. The pumping beam is generated using a PPLN-OPG seeded by a stabilized laser beam as traceable to the national standard. The generated pulses are amplified by a KTA-OPA pumped by a SLM Nd:YAG MOPA system. The seeding beam is monitored and controlled by a “spectral drill” cavity. The frequency of seeding beam is observed as intensity error signal. We expect that these methods will open up new fields.
We report for the first time, to the best of our knowledge, a simple single pixel imaging (SPI) scheme with high singalto- noise ratio (SNR) in an entire THz frequency region (1 - 15 THz) by employing a thin metallic ring with a series of random masks directly perforated, that is a ‘metallic randon ring’. This SPI scheme allows us to reconstruct highresolution images (320 x 320 pixels), and it offers potentially advanced THz imaging technologies, such as non-invasive assignment of biomaterials.
We have developed a thin THz-wave planar lens based on the phase-patterned Fresnel zone plate (FZP) concept to obtain a high transmittance and short focal length in free space. The FZP lens was designed for focusing THz waves at 1.0 THz (λ=300 μm) with a transmittance of more than 80% and a focal length of 24 mm (80λ). The developed FZP lens was made of polymer BCB as a flexible film substrate with concentric zones of metamaterial-based phase shifter patterns with a subwavelength thickness of approximately 48 μm (0.16λ). To obtain the THz-wave phase retardation of π/2 compared to the naked polymer substrate, we employed the metamaterial unit structure consisting of double-layer unsplit ring resonators (USRRs) with a 32-μm distance between the two layers. The experimental result confirms that the FZP lens creates a focus by constructive interference of incident THz waves through concentric zones of metamaterial-patterned and un-patterned regions. By using a narrowband THz-wave beam from an injection-seeded THz-wave parametric generator, the measured focus spot size of 0.57 mm at full width at half maximum was obtained at the designed frequency of 1.0 THz. Using this FZP lens, the THz-wave imaging test in transmission geometry has also been demonstrated.
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