• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2007년도 하계학술대회 논문집 Vol.8
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• pp.222-222
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• 2007

RF circuit을 구현하는데 있어서 기판의 전기적 특성을 정확하게 아는 것은 원하는 결과를 추출하기 위해 매우 중요하다. 본 연구에서는 현재 사용되고 있는 PI 기판의 전기적인 특성인 유효 유전율과 loss tangent 값을 T-resonator률 이용해 정확하게 측정하고자 했다. T-resonator는 microstrip 구조로 구현 되었으며 conductor material은 Cu를 사용하였다. PI 기판의 두께는 25um, Cu의 두께는 PI 기판의 종류에 따라 12um 와 18um, T-resonator line width는 50um로 구현하였다. 또한 공진 주파수에 따라 stub 길이가 다른 10개의 T-resonator를 제작하였다. PI 기판의 유효 유전율을 구하기 위해 stub 길이의 open-end effect와 T-junction effect를 고려하였으며 수식을 통해 정확한 유효 유전률을 추출하였다. 또한 PI 기판의 loss tangent 추출에 필요한 dielectric loss를 추출하기 위해 unload quality factor를 분석하였다. Unload quality factor는 dielectric loss, conductor loss, radiation loss를 구성되며 conductor loss와 radiation loss를 수식에 의해 구하고 dielectric loss를 추출 하였다. 추출 된 dielectric loss를 통해 각각의 T-resonator의 loss tangent 값을 구하였다. T-resonator를 이용한 PI 기판의 측정은 비교적 복잡한 수식에 의해 이루어지지만 정확한 data를 얻을 수 있고 다른 재료의 전기적 특성을 추출하는데 응용이 가능하다.

• 한국전자파학회논문지
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• 제10권4호
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• pp.582-593
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• 1999

본 논문에서는 무궁화 III호 위성체용 Ka-밴드 다이플렉서의 설계를 위해 모드매칭법에 의해 산란행렬을 계산하여 설계한 필터의 전달특성을 분석하고, 대칭적 유도성 아이리스 구조와 전계면 금속삽입 구조로 설계된 2개의 대역통과 필터를 자계면 T-접합에 의한 합성방법으로 Ka 밴드 위성체용 다이플렉서를 설계, 제작 하여 그 설계 방법에 대한 타당성 여부를 검증하였다 제작된 다이플렉서는 위성체에서 송.수선 펼터의 개별 사용에 따른 크기 및 무게의 증가를 효과적으로 감소시킬 수 있으며, 송선필터의 경우 아이리스를 도파관 자계변 외벽으로 돌출시키는 구조로 설계함으로써 펼터 자체가 방열판 구실을 하여 고전력 전송에 따른 펼터 의 특성 변화를 최소화하였다. 또한 대부분의 도파관 펼터에서 동작특성을 보정하기 위해 사용되는 미세 보정 나사의 사용을 배제함으로써 제작의 단순화와 위성체용으로서의 내구성과 선뢰도를 향상시켰다. 제작된 Ka-밴드 위성체용 다이플렉서는 2개의 펼터(Rx : $30.485\pm0.4 GHz$, Tx : $20.755\pm0.4 GHz$) 모두 통과대역에 서 1.2 dB 미만의 삽입손실(insertion loss)과 15dB 보다 좋은 반사손실(return loss) 특성을 얻었고, 송.수신 필터간 65dB 이상의 분리도(isolation)를 나타내었다.

• Transactions on Electrical and Electronic Materials
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• 제14권4호
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• pp.177-181
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• 2013

In this paper, silicon solar cells are analyzed regarding power conversion efficiency by changed capacitance in the depletion region. For the capacitance control in the depletion region of silicon solar cell was applied for 10, 20, 40, 80, 160 and 320 Hz frequency band character and alternating current(AC) voltage with square wave of 0.2~1.4 V. Academically, symmetry formation of positive and negative change of the p-n junction is similar to the physical effect of capacitance. According to the experiment result, because input of square wave with alternating current(AC) voltage could be observed to changed capacitance effect by indirectly method through non-linear power conversion (Voltage-Current) output. In addition, when input alternating current(AC) voltage in the silicon solar cell, changed capacitance of depletion region with the forward bias condition and reverse bias condition gave a direct effect to the charge mobility.

• Journal of Electrical Engineering and Technology
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• 제4권2호
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• pp.211-218
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• 2009

This paper presents a voltage and frequency controller (VFC) for a 4-wire stand-alone wind energy conversion system (WECS) employing an asynchronous generator. The proposed VF con-troller consists of a three leg IGBT (Insulated Gate Bipolar Junction Transistor) based voltage source converter and a battery at its DC bus. The neutral terminal for the consumer loads is created using a T-connected transformer, which consists of only two single phase transformers. The control algorithm of the VF controller is developed for the bidirectional flow capability of the active power and reactive power control by which it controls the WECS voltage and frequency under different dynamic conditions, such as varying consumer loads and varying wind speeds. The WECS is modeled and simulated in MATLAB using Simulink and PSB toolboxes. Extensive results are presented to demonstrate the capability of the VF controller as a harmonic eliminator, a load balancer, a neutral current compensator as well as a voltage and frequency controller.

• Journal of Korean Neurosurgical Society
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• 제29권2호
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• pp.255-260
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• 2000

The authors report a posttraumatic syringomyelia in a 30-year-old man who has complained pain, weakness of upper arm and dissociation sensory loss since 2 months before. He was underwent by decompressive laminectomy from T12 to L1, reduction of encroached bony fragments, transpedicular screw fixation from T12 to L2 and posterolateral bony fusion due to burst fracture of L1 at other hospital 3 years ago. Preoperative spinal MRI was highly suggestive of wide-spread, multiseptated syringomyelia from C3 to thoracolumbar junction. We performed wide decompressive laminectomy from T10 to L2 and subarachnoid space reconstrucion composed of microdissection of meningeal fibrosis widely, iatrogenic meningocele formation with lefting the dura mater opened for treatment of spinal-spinal pressure dissociation. Clinical manifestations and radiological findings of the patient were improved after the operation. This technique was thought to be superior to shunting procedures in cases of wide-spread, multiseptated post-traumatic syringomyelia.

• Progress in Superconductivity
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• 제5권1호
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• pp.45-49
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• 2003

We have designed and fabricated the single-layer high $T_{c}$ SQUID magnetometer consisting of a directly coupled grain boundary junction SQUID with an inductance of 100 pH and 16 nested parallel pickup coils with the outermost dimension of 8.8 mm ${\times}$ 8.8 mm. The magnetometer was formed from a YBCO thin film deposited on an STO(100) bicrystal substrate with a misorientation angle of $30^{\circ}$. The SQUID magnetometer was further improved by optimizing the multi-loop pickup coil design for use in unshielded environments. Typical characteristics of the dc SQUID magnetometer had a modulation voltage of 40 $\mu\textrm{V}$ and a white noise of $30fT/Hz^{1}$2/. The SQUID magnetometer exhibited a 1/f noise level at 10 Hz reduced by a factor of about 3 compared with that of the conventional solid type pickup coil magnetometers and a very stable flux locked loop operation in magnetically disturbed environments.s.

• 대한전기학회:학술대회논문집
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• 대한전기학회 1988년도 추계학술대회 논문집 학회본부
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• pp.168-171
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• 1988

The p-n homo junction diode of the III-V ternary alloy semiconductor $In_{1-x}Ga_xP$ : S grown by the temperature gradient solution (TGS) was fabricated by Zn-diffusion, and it's characteristics was investigated. The carrier concentration of $In_{1-x}Ga_xP$ doped with sulfur, 0.5 mol %, was $1{\times}10^{17}cm^{-3}$ and the mobility was varied with the composition. In the case that the diffusion time was constant as 30 minutes. The temperature dependence of diffusion coefficient was decreased from D= $4.2{\times}10^{-5}$ exp (-1.74/$k_{B}T$) to D= $2.5{\times}10^{-5}$ exp (-3.272/$k_{B}T$) with increasing of composition $\times$ from 0.43 to 0.98. The major peak of E.L spectrum was due to D-A pair recombination and the peak intensity was increased with the increasing of input current. And the E.L intensity was decreased with the increasing temperature, and shift to the long wavelength. The luminescence efficiencies measured at $5^{\circ}C$, atmosphere temperature, was decreased from $2.6{\times}10^{-4}$% to $9.49{\times}10^{-6}$ % with increasing of composition it from 0.39, direct transition region, to 0.98, indirect transition region.

• The Journal of Korean Physical Therapy
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• 제13권1호
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• pp.237-243
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• 2001

Skeletal muscle cells are activated by ${\alpha}$-motorneurons which release acetylcholine at the neuromuscular junction. This results in a local depolarization of surface membrane which triggers an action potential. The action potential propagates along the surface membrane and also into the T-tubule system. In the triads T-tubules are in close connection with the terminal cisternae of the sarcoplasmic reticulum(SR). The action potential activaies T-tubule voltage sensors(DHP receptors). which activates SR Ca$^{2+}$ release channels(ryanodinc receptors). Ca$^{2+}$ have a key role in skeletal muscle in that an increase of free myoplasmic Ca$^{2+}$ concentration. The process of coupling chemical and electrical signals at the cell surface to the intracellular release of Ca$^{2+}$and ultimate contraction of muscle fibers is termed excitation-contraction coupling(ECC). Coupling of cel1 surface signals to intracellular Ca$^{2+}$ release proceeds by several mechanisms in skeletal muscle cells. This review focus on sarcopiasmic reticulum(SR) Ca$^{2+}$ releasing mechanisms from sarcoplasmic reticulum in the skeletal muscle. The mechanisms include DCCR, CICR, and HCR.

• 한국초전도학회:학술대회논문집
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• 한국초전도학회 2000년도 High Temperature Superconductivity Vol.X
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• pp.155-159
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• 2000

YBCO step-edge dc SQUID magnetometers on sapphire substrates have been fabricated. CeO2 buffer layer and YBCO films were deposited in situ on the low angle (${\sim}$35$^{\circ}$) steps formed on the sapphire substrates. Typical 5-${\mu}$m-wide junction has R$_n$ of 5 ${\omega}$ and I$_c$ of 50 ${\mu}$A with large I$_c$R$_n$ product of 250 ${\mu}$V at 77K. According to applied bias current, depth of voltage modulation was changed and maximum voltage was measured 16 ${\mu}$V. Field noise of do SQUID was measured 100${\sim}$300 fT/${\surd}^{Hz}$ in the 1 $^{kHz}$, and about 1.5 pT/${\surd}^{Hz}$ in the 1/f region. For ac bias reversal method, field noise was decreased in the 1/f region. The QRS peak of magnetocardiogram was measured 50 pT in the magnetically shielded room.

• Progress in Superconductivity
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• 제1권1호
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• pp.20-25
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• 1999

We constructed a high-$T_c$ scanning SQUID microscope (SSM) operating in the liquid nitrogen. We used a washer-type YBCO SQUID with inner and outer dimensions of $12{\mu}m$ and $36{\mu}m$, respectively, which was grown on the $SrTiO^3$ bicrystal substrate. The sample, rather than SQUID, was scanned using two stepping motors. We also developed readout electronics, stepping motor controller, and the software for system control and data display. We took images of various samples using our SSM and found that the spatial resolution is about $40{\mu}m$ and noise level is lower than $10^{-7}T/{\surd}Hz$ at 100 Hz and higher at lower frequencies. The noise level was much higher than that of a typical SQUID due to the other coupling from the electric parts. We present a simple argument on the inductive coupling between the sample and the SQUID which should be under-stood for the proper interpretation of the obtained images. By comparing the measured data with the simulation results the gap between the SQUID and the sample is estimated to be $40{\mu}m$.