• The Journal of Korean Institute of Electromagnetic Engineering and Science
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• v.26 no.5
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• pp.514-520
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• 2015

Sidelobe canceller(SLC) requires main beam pattern(SUM beam) and auxiliary beam patterns for rejection of sidelobe noise jammer. For best performance of sidelobe noise jamming cancellation of adaptive SLC, gain dominant region of each auxiliary beam pattern shall not be overlapped one another in elevation/azimuth regions of sidelobe of main beam, and beam patterns of auxiliary channels should have low gains in regions of mainlobe of main beam. In the monopulse radar, the difference beam patterns for monopulse processing have these properties. This paper proposes the method using data from the difference channel for monopulse processing as data from auxiliary channel for sidelobe cancellation. For the proposed SLC, the results of simulation and performance analysis was presented. If the proposed method is used in the monopulse radar, SLC can be constructed by using basic SUM and difference channels without extra channel composition.

• Proceedings of the Korean Vacuum Society Conference
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• 2013.02a
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• pp.241-241
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• 2013

PLS-II 저장링 진공시스템은 2011년 6월 설치 완료 후 2011년 7월부터 2012년 초 까지 1차 시운전을 마쳤다. PLS-II 저장링 진공시스템은 누적 전류 50 Ah 운전 후, 3 GeV, 400 mA 전자빔 운전 시 평균 진공도 $2{\times}10^{-9}$ mbar를 유지도록 설계되어 빔-기체 산란 수명을 20 시간 이상 확보하도록 설계하였다. 지금까지의 간략한 운전 이력과 진공시스템의 성능을 보고하고 최근 방사광 가속기에서 중요하게 취급하는 진공용기(특히, 빔전류 측정 진공용기)의 기계적 안정도, 변위 등과 BPM TE mode noise suppression 등을 보고하고자 한다.

• The Journal of Korean Institute of Electromagnetic Engineering and Science
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• v.22 no.7
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• pp.720-728
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• 2011

In this paper, development of the monopulse secondary surveillance radar antenna which can be used for IFF system is presented. This antenna that is passive linear array is comprised of the row-feeder and several array-elements. The row-feeder provides sum, different and SLS(Sidelobe Supression) channels which are optimized the distribution of the power and phase ratio. The azimuthe sidelobe level of the sum channel beam pattern is -20 dBc or less. The SLS channel covers the sidelobe of the sum-chanel in the whole azimuth angle range. And the difference channel is used to perform the mono-pulse function, improves the detection accuracy in the azimuth direction. Meanwhile, the arrayelement makes shaped beam in the elevation angle, in order to eliminate the clutter and multipath effects from the ground. Performance of the antenna developed is verified by the measurement of S-parameters and far-field beam pattern, and satisfies all of the development specifications well.

• Korean Journal of Optics and Photonics
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• v.35 no.4
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• pp.150-156
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• 2024

One of the key factors in research regarding long-distance laser beam propagation, as in free-space optical communication or laser power transmission, is the transmission efficiency of the laser beam. As a way to improve efficiency, we perform extensive numerical simulations of the effect of modifying the laser beam's profile, especially replacing the fundamental Gaussian beam with a super-Gaussian beam. Numerical simulations of the transmitted power in the ideal diffraction-limited beam diameter determined by the optical system of the transmitter, after about 1-km propagation, reveal that the second-order super-Gaussian beam can yield superior performance to that of the fundamental Gaussian beam, in both single-channel and coherently combined multi-channel laser transmitters. The improvement of the transmission efficiency for a 1-km propagation distance when using a second-order super-Gaussian beam, in comparison with a fundamental Gaussian beam, is estimated at over 1.2% in the singlechannel laser transmitter, and over 4.2% and over 4.6% in coherently combined 3- and 7-channel laser transmitters, respectively. For a range of the propagation distance varying from 750 to 1,250 m, the improvement in transmission efficiency by use of the second-order super-Gaussian beam is estimated at over 1.2% in the single-channel laser transmitter, and over 4.1% and over 4.0% in the coherently combined 3- and 7-channel laser transmitters, respectively. These simulation results will pave the way for future advances in the generation of higher-order super-Gaussian beams and the development of long-distance optical energy-transfer technology.

• Proceedings of the Korean Vacuum Society Conference
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• 1999.07a
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• pp.132-132
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• 1999

카본 박막은 내마모성, 내산성, 윤활성 및 높은 경도를 가지고 있어, 경질 박막 및 기능성 박막으로 주목을 받고 있으며 그 응용 분야가 매우 크다. 본 연구는 전자빔(Electron Beam)을 카본 grain을 증발시킴과 동시에 아르곤 보조 이온빔을 조사시켜 이온에너지에 따른 박막의 물성변화를 관찰하였다. 특히 본 연구에서 이용한 이온빔 증착 장치의 장점은 이온 충돌 에너지의 조절이 가능하다는 것이다. 카본 박막의 제조는 이온빔이 증착된 고진공 증착 장치를 이용하였고 이원빔원으로는 Oxford Applied Research 사의 RF 방전형 이온빔을 이용하였다. 배기장치는 유회전펌프와 터보펌프를 사용하였다. 기판은 홀더에 장착하기 전에 전처리를 거친 후 용기 내에서 이온빔에 의해 2차 청정을 하였다. 빔전압이 500V, 빔 전류는 4mA/cm2 및 RF power를 400W로 하여 기판 청정을 거친 후 전자빔을 이용하여 흑연을 증발시켜 박막을 제조하였다. 이때 이온빔 전압을 100~500V, RF power를 400~550W 으로 조절하였다. 카본 grain을 Si 및 Slide Glass 기판위에 1$\AA$/sec의 증착율을 유지하면서 증착하였다. 카본 박막의 박막은 평균두께는 0.3~0.4$\mu\textrm{m}$이며 SEM을 이용하여 단면을 관찰하였다. 라만 분광분석을 통하여 비정질 카본 박막의 결합특성을 조사하였고 scratch tester를 이용하여 박막의 밀착력을 관찰하였다. 그리고 카본 박막의 전도도 특성을 알고자 비저항을 측정하였으며, 박막의 성분 분석을 위한 AES 분석을 하였다. 1)AES 결과:표면에서와 박막 내부에서는 불순물인 산소나 질소의 함량이 거의 존재하지 않음을 관찰하였다. 2)경도:1,000~1,400kg/mm2 3)라만 분광 분석:300V의 이온 에너지를 분기로 박막 구조의 변화에 의한 스팩트럼의 변화를 보였다. 4)비저항:10-2~10-1$\Omega$.cm

• The Journal of the Acoustical Society of Korea
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• v.32 no.4
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• pp.287-293
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• 2013

We present a parametric array signal generating system using $3{\times}16$ transducer array which is composed of multi-resonant frequency transducers of 20kHz and 32.5kHz. To drive transducer array, sixteen channel amplifier using LM1875 chips is designed and implemented, and the PXI system based on the LabView 8.6 for arbitrary signal generation and analysis is used. Using the proposed system, we measure sound pressure level and beam pattern of difference frequency and verify the nonlinear effect of difference frequency. The theoretical absorption range and the Rayleigh distance are 15.51m and 1.933m, respectively and we verify that sound pressure of difference frequency is accumulated and increased at the near-field shorter than the Rayleigh distance. We verify that the beam pattern of the measured difference frequency and the beam pattern obtained by the superposition of two primary frequencies are similar, and high directional parametric signal was generated.

• The Journal of Korean Institute of Electromagnetic Engineering and Science
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• v.11 no.6
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• pp.1006-1014
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• 2000

Hemisphere type Luneberg lens antenna with a reflector(frequency : 9.375 GHz, -3 dB beam width 6$^{\circ}$, diameter 30.3 cm(about 10 A), which is miniaturized and lightweightized by attaching a reflector on a section of half the Luneberg lens antenna, is designed and fabricated on the basis of Luneberg lens antenna from which easy beam pointing is acquired only by movement of 1st radiator. Measurement shows -3dB beamwidth is 6.1$^{\circ}$ in case of E-plane and 5.5$^{\circ}$ in case of H-plane. These are good agreements with expected value. Gain of this antenna is 26dBi(Aperture efficiency for uniform distribution : $\pi$ = 44.97%) which is greater than that of 1st radiator(Rectangular microstrip antenna) by 20.4 dB. And, after calculating the approximated pattern of the 1st radiator, far-field pattern, whose source is the second aperture source farmed from the approximated pattern of the 1st radiator is computed. Comparing this far-field pattern with the expected pattern, a (relatively) good agreement is observed. Circular polarization Luneberg lens antenna is also manufactured by making 1st radiator so that it has the characteristics of LHCP and RHCP radiation. The results are as followings : -3 dB beamwidth 5.8$^{\circ}$ , side lobe level -15.3 dB, isolation between LHCP and RHCP radiation 2543, axial ratio 2 dB bandwidth about 1.4 GHz(14.9%).

• Journal of the Korean Vacuum Society
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• v.2 no.3
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• pp.304-313
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• 1993

집속 이온빔 기술은 고해상도의 이온빔 리토그라피, 마스크가 필요없는 이온주입, 그리고 Ion beam induced deposition 등 반도체 소자의 미세가공에 널리 이용되어 왔다. 좋은 안정도와 높은 전류밀도, 적은 에너지 퍼짐 그리고 낮은 에미턴스와 높은 선명도를 갖는 집속 이온빔 장비를 위한 액체 갈륨 이온원이 한국에서 개발 시업되었다. 이온빔의 전압이 15kV, 렌즈전압이 7kV 그리고 렌즈상단에 위치한 aperture의 직경이 0.2mm일 때, 0.1$mu extrm{m}$의 빔 직경으로 집속되는 정전 einzel렌즈가 설계 조립되었고, FIB 진공 chamber는 렌즈부와의 차 등 진공시스템으로 구성되어 설계제작되었다. FIB 장비가 조만간 한국에서 이온빔 밀링, ion beam induced deposition 그리고 잘못된 부분의 수정 등 반도체 제작공정에서의 응용에 큰 기여를 할 것이라 기대된다.

• Journal of the Korea Institute of Information and Communication Engineering
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• v.12 no.3
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• pp.427-437
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• 2008

In order to increase the coupling efficiency of the power and phase of the active phase array antenna, we have fabricated the active phased-array antenna which is coupled by the transmission line, and investigated the relationship between the length of the coupling transmission line and coupling power and phase. The following three types of driving method - (1) giving the frequency difference between the two active antenna, (2) applying the input signal to the one side of the two antennas, and changing the eigen frequency of the other side antenna, (3) appling the different phase inputs to the active antennas was investigated. The experimental results showed that the interval of the antenna elements has not affected the power and the phase of the antenna.

• Journal of the Korea Institute of Information and Communication Engineering
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• v.25 no.11
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• pp.1687-1695
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• 2021

In this paper, it is designed and analyzed the beamforming antenna using the butler matrix. The operating frequency of the proposed beamforing antenna is ISM band of 2.4 GHz band and the component of the beamforing antenna consisted of a 1×4 array antenna and a 4×4 butler matrix. Each output port of 4×4 butler matrix outputs the signal having a different phase, it is provided to each input port of 1×4 array antenna. The beamforming antenna with four output ports forms a total of four beams. In order to analyze the radiation pattern of the beamforming antenna, it was provided by switching the signal to the input port and proceeded the Individual analysis for the input port 1 to 4. The main beams of the proposed beamforming antenna were formed in the -12°, 40°, -40° and 12° directions according to each input port, respectively.