• 제목/요약/키워드: PT symmetric

검색결과 16건 처리시간 0.02초

Three-dimensional Spatiotemporal Accessible Solitons in a PT-symmetric Potential

  • Zhong, Wei-Ping;Belic, Milivoj R.;Huang, Tingwen
    • Journal of the Optical Society of Korea
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    • 제16권4호
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    • pp.425-431
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    • 2012
  • Utilizing the three-dimensional Snyder-Mitchell model with a PT-symmetric potential, we study the influence of PT symmetry on beam propagation in strongly nonlocal nonlinear media. The complex Coulomb potential is used as the PT-symmetric potential. A localized spatiotemporal accessible soliton solution of the model is obtained. Specific values of the modulation depth for different soliton parameters are discussed. Our results reveal that in these media the localized solitons can exist in various shapes, such as single-layer and multi-layer disk-shaped structures, as well as vortex-ring and necklace patterns.

축대칭 이류체 분무화염의 구조에 관한 연구 (A Study on the Structure of Axial-Symmetric Two-Phase Spray and Flame)

  • 정보윤;고대권;안수길
    • 수산해양기술연구
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    • 제24권1호
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    • pp.36-43
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    • 1988
  • Boilers and diesel engines have many problems because their exhaust particles, i.e., soot have lots of bad influence on environment. And it's spray and flame have fundamentally axial symmetric shape. To investigate the relationship between fuel concentration distribution of spray and soot concentration distribution as well as temperature distribution of flame, we made a axial symmetric two phase spray-flame and analyzed the structure of is. The measuring method is the principle of the light extinction method for the spray-flame and onion peeling model is applied to analyze the radial distribution of fuel and soot concentration. The temperature of flame is measured by ø 0.4mm Pt-Pt.RH 3% thermocouple. The oils for the experiments are diesel oil and 10% water emulsified diesel oil. It was found that the soot concentration becomes higher as it comes near to the center of flame, and the fuel concentration does, too. And the soot concentration level of diesel oil is generally higher than that of the 10% water emulsified fuel. The maximum flame temperature of diesel oil is 1,17$0^{\circ}C$, however, 10% water emulsified diesel oil is 1,27$0^{\circ}C$.

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Carbon-13 Nuclear Magnetic Resonance Spectroscopic Studies of $^{13}CO$ Adsorbed on Platinum Particles in L-Zeolites

  • 한옥희;Gustavo Larsen;Gary L. Haller;Kurt W. Zilm
    • Bulletin of the Korean Chemical Society
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    • 제19권9호
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    • pp.934-942
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    • 1998
  • $^13CO$ chemisorbed on platinum particles in L-zeolite has been investigated by static and magic angle spinning NMR spectroscopy. The representative spectra are composed of a broad asymmetric peak with a center of gravity at 230±30 ppm and a sharp symmetric peak at 124±2 ppm which is tentatively assigned to physisorbed $CO_2$, on inner walls of L-zeolite. Overall, the broad resonance component is similar to our previous results of highly dispersed (80-96%) CO/Pt/silica or CO/Pt/alumina samples, still showing metallic characters. The principal difference is in the first moment value. The broad peak in the spectra is assigned to CO linearly bound to Pt particles in the L-zeolites, and indicates a distribution of isotropic shifts from bonding site to bonding site. The NMR results reported here manifest that the Pt particles inside of the L-zeolites channels are not collectively the same with the ones supported on silica or alumina with similar dispersion in terms of Pt particle shape and/or ordering of Pt atoms in a particle. As a result, Pt particles of CO/Pt/L-zeolite were agglomerated accompanying CO desorption upon annealing. There were no definite changes in the NMR spectra due to differences of exchanged cations. Comparison of our observation on CO/Pt/L-zeolite with Sharma et al.'s reveals that even when the first moment, the linewidtb, and the relaxation times of the static spectra and the dispersion measured by chemisorption are similar, the properties of Pt particles can be dramatically different. Therefore, it is essential to take advantage of the strengths of several techniques together in order to interpret data reliably, especially for the highly dispersed samples.

Revisiting $H_2$ and CO Interactions with Pt(111) Surfaces

  • Kim, Je-Heon;Jo, Sam-K.
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2011년도 제41회 하계 정기 학술대회 초록집
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    • pp.203-203
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    • 2011
  • The importance of stepped single-crystal surfaces as model catalysts has been well recognized [1]. We re-investigated the adsorption properties of $H_2$ and CO, most important species in platinum-based catalysts, on nearly defect-free and highly stepped surfaces of one and the same Pt(111) crystal. While both being symmetric and single-peaked from the nearly defect-free surface, temperature-programmed desorption (TPD) spectra from the highly stepped surface saturated at 90 K with H and CO were triply- and doubly-peaked, respectively. Once pre-adsorbed, CO preempted step and then terrace sites, inhibiting the dissociative $H_2$ adsorption completely. Pre-adsorbed H inhibited the CO adsorption on terrace sites only, leaving defect sites intact for CO adsorption even at the saturation H precoverage. On defect-free Pt(111), while pre-adsorbed CO inhibited the dissociative $H_2$ adsorption completely, pre-adsorbed H could not inhibit the CO adsorption completely. These intriguing, but interesting results are discussed in terms of energetics/kinetics and the role of surface step sites in the dissociative adsorption of $H_2$ on Pt(111) [2].

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Application of a General Gas Electrode Model to Ni-YSZ Symmetric Cells: Humidity and Current Collector Effects

  • Shin, Eui-Chol;Ahn, Pyung-An;Seo, Hyun-Ho;Lee, Jong-Sook
    • 한국세라믹학회지
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    • 제53권5호
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    • pp.511-520
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    • 2016
  • Electrolyte-supported symmetric Ni-YSZ cermet electrodes of ca. $23{\mu}m$ were prepared by screenprinting and the impedance was measured as a function of humidity from 2% to 90% balanced in $H_2$ at a total flow rate of 50 sccm. The Ni felt current collector of 1 mm thickness exhibited a Gerischer-like gas concentration impedance in the low frequency range, which was similarly observed in the cermet-supported solid oxide cells, while the Pt paste collector exhibited only electrochemical polarization. The electrochemical polarization of both samples was modeled by a non-ideal diffusion-reaction transmission line model including CPEs with ${\alpha}$= 0.5. In the case of the Pt paste collector, all the Bisquert parameters exhibited humidity dependence to the -1/2 power, supporting a non-faradaic chemical reaction mechanism at three phase boundaries. Consequently, the surface diffusivity and reaction rate increased linearly with humidity. Less pronounced humidity dependence and somewhat lower utilization length with an Ni felt collector can be attributed to the diffusion-limited gas flow through the collector.

크로스-결합구조의 부성 미분 저항 회로를 이용한 페리티-시간 대칭 구조의 비접촉 센서 구동 회로에 대한 연구 (Non-Contact Sensing Method using PT Symmetric Circuit with Cross-Coupled NDR Circuits)

  • 홍종균
    • 한국산학기술학회논문지
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    • 제22권4호
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    • pp.10-16
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    • 2021
  • 본 연구에서는 신축성 인덕터를 이용한 센서 응용을 위한 상태 감지 회로로써 패리티-시간 대칭 구조를 고려한 모델을 제안하고자 한다. 신축성 인덕터를 이용한 센서 구동 회로로써 트랜지스터를 이용한 부성 미분 저항 회로를 적용하여 신축성 인덕터를 보다 효율적으로 활용할 수 있는 방법을 제안하고, 패리티-시간 대칭 구조의 결합 공진 회로에 대한 특성 분석을 통해 고전적 공진 회로에 비해 향상된 분해능을 갖는 모델을 설계하였다. 특히, 보다 실질적인 전산모의실험결과를 얻기 위해, 신축성 인덕터 모델의 경우에는 참고문헌의 실험결과를 참고하여 본 연구 모델에 적용하였다. 전산모사를 통해 본 연구에서 사용한 부성 미분 저항 회로를 통해 저항 성분 뿐만 아니라 위상 성분도 제어됨을 확인하였으며, 이러한 결과를 통해 신축성 인덕터의 특성 변화에 따른 회로의 불균형을 부성 미분 저항 회로를 이용하여 보완할 수 있음을 고찰하였다. 이러한 특성을 이용하여 패리티-시간 대칭 구조를 구현할 수 있었으며, 이에 대한 특성에 대하여 논의하였다. 특히, 본 연구에서 제안하는 패리티-시간 대칭 구조의 센서 구동 회로에 대한 주파수 특성의 결과로부터 기존의 고전적 공진 회로에 비해 Q-factor가 최대 20배까지 커질 수 있음을 확인하였다.

Pt/$LiNbO_3$/AIN/Si(100) 구조의 전기적 특성 (Electrical Properties of Pt/$LiNbO_3$/AIN/Si(100) structures)

  • 정순원;정상현;인용일;김광호
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2001년도 하계학술대회 논문집
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    • pp.58-61
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    • 2001
  • Metal-insulator-semiconductor (MIS) C-V properties with high dielectric AIN thin films showed no hysteresis and good interface properties. The dielectric constant of the AIN film calculated from the capacitance at the accumulation region in the capacitance-voltage(C-V) characteristics was about 8. The C-V characteristics of MFIS capacitor showed a hysteresis loop due to the ferroelectric nature of the LiNbO$_3$ thin films. Typical dielectric constant value of LiNbO$_3$ film of MFIS device was about 23. The memory window width was about 1.2V at the gate voltage of $\pm$5 V ranges. Typical gate leakage current density of the MFIS structure was the order of 10$^{-9}$ A/cm$^2$ at the range of within $\pm$500 kV/cm. The ferroelectric capacitors showed no polarization degradation up to about 10$^{11}$ switching cycles when subjected to symmetric bipolar voltage pulse(peak-to-peak 8V, 50% duty cycle) in the 500kHz.

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Pt/LiNbO3/AlN/Si(100) 구조를 이용한 MFIS 커패시터의 전기적 특성 (Electric Properties of MFIS Capacitors using Pt/LiNbO3/AlN/Si(100) Structure)

  • 정순원;김광호
    • 한국전기전자재료학회논문지
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    • 제17권12호
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    • pp.1283-1288
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    • 2004
  • Metal-ferroelectric-insulator-semiconductor(WFIS) capacitors using rapid thermal annealed LiNbO$_3$/AlN/Si(100) structure were fabricated and demonstrated nonvolatile memory operations. The capacitors on highly doped Si wafer showed hysteresis behavior like a butterfly shape due to the ferroelectric nature of the LiNbO$_3$ films. The typical dielectric constant value of LiNbO$_3$ film in the MFIS device was about 27, The gate leakage current density of the MFIS capacitor was 10$^{-9}$ A/cm$^2$ order at the electric field of 500 kV/cm. The typical measured remnant polarization(2P$_{r}$) and coercive filed(Ec) values were about 1.2 $\mu$C/cm$^2$ and 120 kV/cm, respectively The ferroelectric capacitors showed no polarization degradation up to 10$^{11}$ switching cycles when subjected to symmetric bipolar voltage pulses of 1 MHz. The switching charges degraded only by 10 % of their initial values after 4 days at room temperature.e.

SOI웨이퍼를 이용한 마이크로가속도계 센서의 열응력해석(I) (Analyses Thermal Stresses for Microaccelerometer Sensors using SOI Wafer(I))

  • 김옥삼
    • 동력기계공학회지
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    • 제5권2호
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    • pp.36-42
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    • 2001
  • This paper deals with finite element analyses of residual stresses causing popping up which are induced in micromachining processes of a microaccelerometer sensors. The paddle of the micro accelerometer sensor is designed symmetric with respect to the direction of the beam. After heating the tunnel gap up to 100 degree and get it through the cooling process and the additional beam up to 80 degree and get it through the cooling process. We learn the thermal internal stresses of each shape and compare the results with each other, after heating the tunnel gap up to 400 degree during the Pt deposition process. Finally we find the optimal shape which is able to minimize the internal stresses of microaccelerometer sensor. We want to seek after the real cause of this pop up phenomenon and diminish this by change manufacturing processes of microaccelerometer sensor by electrostatic force.

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