• Title/Summary/Keyword: RF resonator

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Microwave Dual-Mode Band Pass Filter for Mobile Communication using Dielectric Resonator (유전체 공진기를 이용한 이동통신용 마이크로파 Dual-Mode 대역통과 필터)

  • Kim, Jee-Gyun;Lee, Heon-Yong;Kim, Byoung-Ho;Kim, Yu-Kyong;Lee, Byong-Hak
    • Proceedings of the KIEE Conference
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    • 2002.07c
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    • pp.1527-1529
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    • 2002
  • 본 논문은 저손실 소형 대역통과 여파기인 기지국용 RF/Microwave 수동소자의 다중 공진 모드(Multi-Mode)에 관한 연구로 한개의 유전체 공진기(Dielectric Resonator)로 두개의 공진 모드(Dual-Mode)를 형성하고 그의 결합량을 조절하여 대역통과 여파기를 설계 및 제작하고, 기지국용 Dual-Mode 대역통과 여파기의 소형화, 경량화를 50%이상 향상시켜 양질의 Dual-Mode 공진 특성을 관찰하였다.

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Characteristics of polycrystalline 3C-SiC micro resonator (다결정 3C-SiC 마이크로 공진기의 특성)

  • Lee, Tae-Won;Chung, Gwiy-Sang
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2008.06a
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    • pp.69-70
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    • 2008
  • Micro resonators have been actively investigated for bio/chemical sensors and RF M/NEMS devices. Among various materials, SiC is a very promising material for micro/nano resonators since the ratio of its Young's modulus, E, to mass density, $\rho$, is significantly higher than other semiconductor materials, such as, Si and GaAs. Polycrystalline 3C-SiC cantilever with different lengths were fabricated using a surface micromachining technique. Polycrystalline 3C-SiC micro resonators were actuated by piezoelectric element and its fundamental resonance was measured by a laser vibrometer in air and vacuum at room temperature, respectively. For the cantilever with $100{\mu}m$ length, $10{\mu}m$width and $1.3{\mu}m$ thickness, the fundamental frequency appeared at 147.2 kHz.

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A Study on the Deposition Characteristics of ZnO Piezoelectric Thin film Bulk Acoustic Resonator (FBAR 응용을 위한 ZnO 압전 박막의 증착 특성에 관한 연구)

  • 최승혁;김종성
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.16 no.8
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    • pp.716-722
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    • 2003
  • ZnO thin films were deposited on Al and Pt electrodes by an RF reactive sputtering system for the fabrication of FBAR (film bulk acoustic wave resonator), and the effect of thermal treatment temperature on their c-axis preferred orientation was investigated. SEM experiments show that columnar structure of ZnO thin films were grown with c-axis normal to electrode material, and XRD experiments show that both ZnO films were grown with (002) plane preferred orientation, but larger diffraction peak was observed with Pt electrode. The peak intensity increased with higher thermal treatment temperature, but c-axis preferred orientation was diminished. The surface roughness of Al thin film was higher than that of Pt, and these affect the surface roughness of ZnO film deposited on the electrode. Though the preferred orientation with respect to Pt(111) plane was improved with higher thermal treatment temperature, this could not improve the c-axis orientation of ZnO film.

The Improvements of FBAR Devices performances by Thermal Annealing Methods

  • Mai, Linh;Song, Hae-Il;Le, Minh-Tuan;Pham, Van-Su;Yoon, Gi-Wan
    • Proceedings of the Korean Institute of Information and Commucation Sciences Conference
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    • v.9 no.2
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    • pp.311-315
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    • 2005
  • In this paper, we emphasize the advantage of thermal annealing treatments for improvement characteristics of film bulk acoustic resonator (FBAR) devices. The FBAR devices were fabricated on multi-layer thin films, namely, Bragg reflectors. Sintering and/or annealing processes were applied in our experiments. The measurements confirm once again a considerable improvement of return loss $(S_{11})$ and quality factor $(Q_{s/p})$. these thermal treatment techniques are really promising for enhancing performance of FBAR resonators in industry fabrication of RF devices.

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Effect of Etch Hole Position and Sacrificial Layer Residue on a Novel Half-Coaxial Transmission Line Filter (에치홀의 위치와 희생층의 잔류물이 전송선 필터 응답에 미치는 영향)

  • Kim, Yong-Sung;Baek, Chang-Wook;Kim, Yong-Kweon
    • Proceedings of the KIEE Conference
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    • 2007.07a
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    • pp.284-285
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    • 2007
  • In this paper, we present the effect on a novel transmission line filter response by the etch hole position on the suspended ground and the residue on the resonator under ground plane. We defined the etch hole offset as the distance from the sidewall of the suspended ground to the nearest side of the etch holes. We simulated new filter responses to reflect the real value of the changed etch hole offset caused by characteristics of negative photoresist. Return loss is distorted by the residue on the center conductor remained after sacrificial layer removing. By comparison of simulation and measurements, we concluded the residue on the resonator distorted the RF response worse than etch hole offset variation did.

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Design of the Microwave Oscillator with the C type DGS Resonator (C형태의 DGS 공진기를 이용한 초고주파 발진기 설계)

  • Kim, Gi-Rae
    • The Journal of Korea Institute of Information, Electronics, and Communication Technology
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    • v.8 no.4
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    • pp.243-248
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    • 2015
  • Since phase noise is one of the most important parameters in the design of microwave oscillators, several methods have been proposed to reduce the phase noise. These methods have focused on improving the quality factor of resonators, which result in low phase noise oscillators. Dielectric resonators have been widely used for low phase noise in microwave oscillators due to their high quality factor. However this cannot be used in MMIC oscillators because they have a 3D structure. In this paper, to overcome this problem a novel resonator using open ring type DGS is proposed for improvement of phase noise characteristics that is weak point of oscillator using planar type microstrip line resonator, and oscillator for 5.8GHz band is designed using proposed DGS resonator. The open ring type DGS resonator is composed of DGS cell etched on ground plane under $50{\Omega}$ microstrip line. At the fundamental frequency of 5.8GHz, 6.1dBm output power and -82.7 dBc@100kHz phase noise have been measured for oscillator with ring type DGS resonator. The phase noise characteristics of oscillator is improved about 96.5dB compared to one using the general ${\lambda}/4$ microstrip resonator.

40 GHz Vertical Transition with a Dual-Mode Cavity for a Low-Temperature Co-fired Ceramic Transceiver Module

  • Byun, Woo-Jin;Kim, Bong-Su;Kim, Kwang-Seon;Eun, Ki-Chan;Song, Myung-Sun;Kulke, Reinhard;Kersten, Olaf;Mollenbeck, Gregor;Rittweger, Matthias
    • ETRI Journal
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    • v.32 no.2
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    • pp.195-203
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    • 2010
  • A new vertical transition between a substrate integrated waveguide in a low-temperature co-fired ceramic substrate and an air-filled standard waveguide is proposed in this paper. A rectangular cavity resonator with closely spaced metallic vias is designed to connect the substrate integrated waveguide to the standard air-filled waveguide. Physical characteristics of an air-filled WR-22 to WR-22 transition are compared with those of the proposed transition. Simulation and experiment demonstrate that the proposed transition shows a -1.3 dB insertion loss and 6.2 GHz bandwidth with a 10 dB return loss for the back-to-back module. A 40 GHz low-temperature co-fired ceramic module with the proposed vertical transition is also implemented. The implemented module is very compact, measuring 57 mm ${\times}$ 28 mm ${\times}$ 3.3 mm.

Comparative Study on the Power Transfer Efficiency of Magnetic Resonance and Radio Frequency Wireless Power Transmission

  • Kim, Ye-Chan;Choi, Bo-Hee;Lee, Jeong-Hae
    • Journal of electromagnetic engineering and science
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    • v.16 no.4
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    • pp.232-234
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    • 2016
  • In this paper, the power transfer efficiencies (PTEs) of magnetic resonance (MR) wireless power transmission (WPT) and radio frequency (RF) WPT are compared as a function of the distances between resonators (or antennas). The PTE of the C-loaded loop resonators during MR WPT was theoretically calculated and simulated at 6.78MHz, showing good agreement. The PTE of the patch antennas, whose area is the same as the C-loaded loop resonator during MR WPT, was theoretically calculated using the Friis equation and the equation by N. Shinohara and simulated at 5.8 GHz. The three results from the Friis equation, the equation by N. Shinohara, and from a full wave simulation are in strong agreement. The PTEs, when using the same size resonators and antennas are compared by considering the distance between the receiver and transmitter. The compared results show that the MR WPT PTE is higher than that of the RF WPT PTE when the distance (r) between the resonators (or antennas) is shorter. However, the RF WPT PTE is much higher than that of the MR WPT PTE when the distance (r) between the resonators (or antennas) is longer since the RF WPT PTE is proportional to $r^{-2}$ while the MR WPT PTE is proportional to $r^{-6}$.

A Novel RF Active Bandpass Filter with Low Noise Performance (저잡음 특성을 갖는 새로운 RF 능동 대역통과 여파기)

  • 이재룡;윤상원
    • The Journal of Korean Institute of Electromagnetic Engineering and Science
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    • v.13 no.8
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    • pp.748-753
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    • 2002
  • In this paper, a new topology of a active capacitor is proposed in order to apply the resonator in the design of RF active bandpass filters. Through the noise analysis of the active capacitor, the optimized low noise design process is also presented, Due to the low noise performance of the proposed active bandpass filter, it can be used in the RF front-end of the receivers. In designed 2-stage active bandpass filter at 1.9 GHz shows insertion loss of 0 dB, noise figure of 2.6 dB, and OIP3 of 8 dBm.

Advanced Design of Birdcage RF Coil for Various Absorption Regions at 3T MRI System

  • Lee, Jung-Woo;Choe, Bo-Young;Choi, Chi-Bong;Huh, Soon-Nyoung
    • Journal of the Korean Magnetic Resonance Society
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    • v.9 no.1
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    • pp.48-60
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    • 2005
  • Purpose: The purpose of this study was to design and build an optimized birdcage resonator configuration with a low pass filter, which would facilitate the acquisition of high-resolution 3D-image of small animals at 3T MRI system. Methods and Materials: The birdcage resonator with 12-element structures was built, in order to ensure B1 homogeneity over the image volume and maximum filling factor, and hence to maximize the signal to noise ratio (SNR) and resolution of the 3-dimensional images. The diameter and length of each element of a birdcage resonator were as follows: (1) diameter 13 cm, length 22 cm, (2) diameter 15 cm, length 22 cm, (3) diameter 17 cm, length 25 cm. Spin echo pulse sequence and fast spin echo pulse sequence were employed in obtaining MR images. The quality of the manufactured birdcage resonators wes evaluated on the basis of the return loss following matching and tuning process. Results: The experimental MR image of phantoms by the various manufactured birdcage resonators were obtained to compare the SNR in accordance with the size of objects. The size of an object to that of coil was identified by parameters that were estimated from the image of a phantom. First, the diameter of the birdcage resonator was 15cm, and the ratio of the tangerine to the birdcage resonator accounted for approximately 27%. The Q factor was 53.2 and the SNR was 150.7. Second, at the same birdcage resonator, the ratio of the orange was approximately 53%. The SNR and the Q parameter was 212.8 and 91.2, respectively. Conclusion: The present study demonstrated that if birdcage resonators have the same forms, SNR could be different depending on the size of an object, especially when the size of an object to that of coil is approximately 40~80%, the former is bigger than the latter. Therefore, when the size of an object to be observed is smaller than that of coil, the coil should be manufactured in accordance with the size of an object in order to obtain much more excellent images.

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