• Title/Summary/Keyword: Chirped Wave

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Numerical Study on Frequency Up-conversion in USPR using MATLAB

  • Roh, Young-Su
    • Journal of Electrical Engineering and Technology
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    • v.5 no.3
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    • pp.497-502
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    • 2010
  • In this paper, the O-mode ultrashort-pulse reflectometry (USPR) millimeter-wave signals that propagate into the plasma and cover a frequency bandwidth of 33-158 GHz are examined numerically using MATLAB. Two important processes are involved in the computation: the propagation of the USPR impulse signal through a waveguide and the frequency up-conversion using millimeter-wave mixers. These mixers are limited to intermediate frequency signals that are less than 500 mV; thus, it is necessary to disperse the impulse signal into a chirped waveform using the waveguide. The stationary phase method is utilized to derive a closed-form formula for a chirped waveform under the assumption that the USPR impulse is Gaussian. In the process of frequency up-conversion, the chirped waveform is mixed with the mixer LO signal, and the lower frequency components of the RF signal are removed using high pass filters.

Study on the Chirped Waveform of the USPR Pulse using the Impulse Response of a Waveguide

  • Roh, Young-Su
    • Journal of the Korean Institute of Illuminating and Electrical Installation Engineers
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    • v.24 no.3
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    • pp.20-26
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    • 2010
  • In ultrashort-pulse reflectometry (USPR), a chirped waveform transformed from the USPR source impulse signal via waveguide makes it possible to employ millimeter-wave mixers for the frequency up-conversion process. Consequently, the frequency bandwidth of the USPR system is sufficiently wide to cover a large portion of the electron density profile of the plasma. Some physical aspects of the chirped waveform, such as maximum amplitude and length, are critical factors to determine the performance of the system. In this paper, the propagation of the USPR impulse signal through a rectangular waveguide is numerically studied to derive the chirped waveform using the impulse response of the waveguide. The results of numerical computation show that the chirped waveform significantly depends on the waveguide cutoff frequency as well as the waveguide length.

Beam focusing by a single subwavelength metal slit surrounded by chirped dielectric surface gratings (금속 슬릿 주변에 유전체 chirped grating을 배열함으로써 구현한 beam focusing)

  • Kim, Se-Yun;Park, Jeong-Hyeon;Im, Yong-Jun;Kim, Hwi;Lee, Byeong-Ho
    • Proceedings of the Optical Society of Korea Conference
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    • 2007.07a
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    • pp.255-256
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    • 2007
  • We propose a novel method for the beam focusing by a single subwavelength metal slit surrounded by chirped dielectric surface gratings. In the proposed method, the period of each grating is chirped to make a focused beam at the desired position. Design of the grating structures for optimal beam focusing and the analysis of the field distribution are conducted based on the rigorous coupled wave analysis (RCWA). It is shown that the focused beam is formed at 1.5${\mu}m$ from the metal substrate and its full width at half maximum (FWHM) is 411nm.

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Femtosecond Coherent Spectroscopic Study of Zn(II)porphyrin Using Chirped Ultrashort Pulses

  • Yoon, Min-Chul;Song, Jae-Kyu;Cho, Sung;Kim, Dong-Ho
    • Bulletin of the Korean Chemical Society
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    • v.24 no.8
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    • pp.1075-1080
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    • 2003
  • We have investigated femtosecond coherent vibrational motions of Zn(II)-5,15-diphenylporphyrin in toluene using chirp-controlled ultrashort pulses. The oscillatory features superimposed on the temporal profiles of the pump-probe transient absorption signal are affected by the chirping and energy of excitation pulses. Using chirp- and excitation energy-controlled femtosecond pulses, we are able to obtain information on the structural changes between the electronic ground and excited states based on a comparative analysis of the Fouriertransformed frequency-domain spectra retrieved from the oscillatory components with the ground state resonance Raman spectra and normal mode calculations.

Design of High Efficiency Transmission Dielectric Grating for Chirped Pulse Amplification (CPA 시스템 구성을 위한 고효율 투과형 유전체 회절격자 설계)

  • Cho, Hyun-Ju;Jung, Jae-Woo;Lee, Sang-Hyun;Kim, Soojong;Lee, Jeongseop;Jin, Daehyun;Jung, Jiho;Son, Seonghyun
    • Korean Journal of Optics and Photonics
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    • v.33 no.6
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    • pp.260-266
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    • 2022
  • A diffraction grating structure composed of two matching layers and two grating layers was formed, and a diffraction grating with high transmission diffraction efficiency in the -1st order was designed through an optimization technique. The designed diffraction grating had a transverse electric wave diffraction efficiency of 99.997% at the design center wavelength, and had a wavelength width of 80 nm and an incident angle width of 20.0° that maintained a diffraction efficiency of 95% or more. By performing the grating tolerance analysis, it was confirmed that the thickness tolerance for a diffraction efficiency of 95% or more was secured to at least 60 nm, and the diffraction efficiency could be maintained even in a trapezoidal shape with an internal angle of less than 10°.

Basic Examination on 3D Measuring System Using Pulse-Compression

  • Fujimoto Ikumatsu;Ando Shigeru
    • International Journal of Precision Engineering and Manufacturing
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    • v.6 no.4
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    • pp.60-66
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    • 2005
  • In this paper, we propose the basic measurement method of a 3D digitizer using a CCD camera in detail. In the localization measurement with a CCD camera, the effect of the background light and the sensitivity consideration are always problems in realizing a high precision. In this research, a new measurement principle is proposed in which the pulse compression technique known in radar is used to eliminate the effect of background light even under a low intensity light source, and the coordinate values on the CCD camera image plane are determined accurately. From the quantitative evaluation of the S/N ratio improvement and the fundamental experiment, it is verified that a substantial improvement in the S/N ratio is realized for both the background noise and the pixel noise and that a resolution of less than the pixel is sufficiently possible.