• Title/Summary/Keyword: Phase excitation method

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Time Delay Focusing of Ultrasonic Array Transducers on a Defect Using the Concept of a Time Reversal Process

  • Jeong, Hyun-Jo;Lee, Jeong-Sik;Lee, Chung-Hoon;Jun, Ghi-Chan
    • Journal of the Korean Society for Nondestructive Testing
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    • v.29 no.6
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    • pp.550-556
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    • 2009
  • In an application of a time reversal(TR) focusing of array transducer on a defect inside the test material, we employ a new time delay focusing technique based the TR process. In order to realize this idea, a multi-channel ultrasonic system is constructed capable of applying necessary time delays to each channel. The TR-based focusing procedure first measures the backscattered signals after firing one of the array elements. A phase slope method is then used to determine the time-of-flights of the backscattered signals received by all elements of the array. These time delays are used to adjust the time of excitation of the elements for transmission focusing on the defect. In addition to the TR focusing, the classical phased array focusing is also considered for comparison. Experimental results show that the TR-based time delay focusing produces much stronger backscattered signals than the phased array focusing, demonstrating the enhanced capability of the TR focusing.

On a Pitch Alteration Technique in the V/UV Spectrum for High Quality Speech Synthesis Technique (고음질 합성방식용 V/UV 스펙트럼상의 피치변경법에 관한 연구)

  • Jo, Wang-Rae;Bae, Myung-Jin;Kim, Dong-Sung
    • The Journal of the Acoustical Society of Korea
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    • v.15 no.6
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    • pp.99-103
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    • 1996
  • Most waveform coding techniques attempt to reduce redundancy of speech signal while preserving the shape of the waveform. In speech synthesis, wavefrom coding methods are used to the synthesis by rule for high quality speech. However, it is difficult to apply the waveform coding to the synthesis by rule because the parameters of the wavefrom coding cannot be classified as either the excitation or the vocal tract parameters. The proposed method shows little spectrum distortion of 2.7% or less for 50% pitch changes. It also achieves smooth connection of wavefrom magnitudes among the frames by compensating the phase in time domain.

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Synthesis and Luminescence Properties of a Cyan-blue Thiosilicate-based Phosphor $SrSi_2S_5:Eu^{2+}$

  • Nakamuraa, Masayoshi;Katoa, Hideki;Takatsuka, Yuji;Petrykinc, Valery;Tezuka, Satoko;Kakihana, Masato
    • Journal of Information Display
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    • v.11 no.4
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    • pp.135-139
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    • 2010
  • A series of Sr-Si-S compounds was synthesized using an advanced chemical method in which the use of one solution-based process uniformly dispersed the $Eu^{2+}$ activators in the host crystals, to find new compositions that would suit phosphor applications. Particular focus was given to the Si-rich region. This led to the synthesis of a single-phase compound that showed an unknown X-ray diffraction pattern. This compound had a composition close to that of $SrSi_2S_5$. When this compound is activated with $Eu^{2+}$ ($SrSi_2S_5:Eu^{2+}$), it shows a cyan-blue emission with a main luminescence peak at 495 nm. This emission is excited by wavelengths of 250-440 nm and has a maximum excitation at 350 nm.

Stimulated emission from optically pumped column-III nitride semiconductors at room temperature (III족 질화물 반도체의 실온 광여기 유도방출)

  • 김선태;문동찬
    • Electrical & Electronic Materials
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    • v.8 no.3
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    • pp.272-277
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    • 1995
  • We report the properties of optically pumped stimulated emission at room temperature (RT) from column-III nitride semiconductors of GaN, AlGaN/GaN double heterostructure (DH) and AlGaN/GaInN DH which prepared on a sapphire substrate using an AIN buffer-layer by the nietalorganic vapor phase epitaxy (MOVPE) method. The peak wavelength of the stimulated emission at RT from AIGaN/GaN DH is 369nm and the threshold of excitation pumping power density (P$\_$th/) is about 84kW/cm$\^$2/, and they from AlGaN/GaInN DH are 402nm and 130kW/cm$\^$2/ at the pumping power density of 200kW/cm$\^$2/, respectively. The P$\_$th/ of AIGaN/GaN and AlGaN/GaInN DHs are lower than the single layers of GaN and GaInN due to optical confinement within the active layers of GaN and GaInN, respectively.

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Luminescence Study of Eu3+ Ions Doped BaMoO4 Nanoparticles

  • Bharat, L. Krishna;Lee, Soo Hyun;Yu, Jae Su
    • Proceedings of the Korean Vacuum Society Conference
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    • 2014.02a
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    • pp.415.2-415.2
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    • 2014
  • Cost-effective, robust devices for solid-state lighting industry that converts electricity to light revolutionize the current lighting industry. Phosphor materials used in these devices should be synthesized in a low-cost and effective method for use in WLEDs. In this presentation, the synthesis of Eu3+ ions doped BaMoO4 phosphor samples by a facile synthesis process for red component of WLEDs will be shown. The tetragonal phase of the host lattice was substantiated by the X-ray diffraction patterns. The morphological studies were carried out by using a field-emission scanning electron microscope and transmission electron microscope. These confirmed the formation of a shuttle like particles with perpendicular protrusions in the middle of the particle. The photoluminescence (PL) properties exhibited good emission with a high asymmetry ratio when excited with ultraviolet B wavelengths (~ 280-315 nm). The cathodoluminescence (CL) spectra showed similar results to the PL spectra, indicating the rich red emission. The results suggest that this phosphor is a good material as red region component in the development of tri-band UV excitation based WLEDs.

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Microwave-modified sol-gel preparation of La2(MoO4)3:Er3+/Yb3 particles and their upconversion photoluminescence properties

  • Lim, Chang Sung
    • Analytical Science and Technology
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    • v.27 no.6
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    • pp.314-320
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    • 2014
  • $La_{2-x}(MoO_4)_3:Er^{3+}/Yb^{3+}$ particles with doping concentrations of $Er^{3+}$ and $Yb^{3+}$ ($x=Er^{3+}+Yb^{3+}$, $Er^{3+}$=0.05, 0.1, 0.2 and $Yb^{3+}$ = 0.2, 0.45) were successfully prepared by the microwave-modified sol-gel method, and the upconversion photoluminescence properties were investigated. Well-crystallized particles, formed after heat-treatment at $900^{\circ}C$ for 16 h, showed a fine and homogeneous morphology with particle sizes of $2-5{\mu}m$. Under excitation at 980 nm, $La_{1.7}(MoO_4)_3:Er_{0.1}Yb_{0.2}$ and $La_{1.5}(MoO_4)_3:Er_{0.05}Yb_{0.45}$ particles exhibited a strong 525 nm emission band, a weak 550 nm emission band in the green region, and a very weak 655 nm emission band in the red region. The Raman spectra of the doped particles indicated the presence of strong peaks at higher frequencies of 752, 846, 922, 1358 and $1435cm^{-1}$ and lower frequency of $314cm^{-1}$ induced by the disorder of the $[MoO_4]^{2-}$ groups with the incorporation of the $Er^{3+}$ and $Yb^{3+}$ elements into the crystal lattice or by a new phase formation.

Modeling and analysis of radiation effects for 1-D RLH-TL (1차원 RLH-TL 방사효과 모델링 및 해석)

  • Moon, Hyo-Sang;Lee, Bom-Son
    • Journal of the Institute of Electronics Engineers of Korea TC
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    • v.44 no.12
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    • pp.8-15
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    • 2007
  • This paper presents the radiation rate formula due of a inclusion of a series capacitor and shunt inductor in a unit cell for the right/left-handed transmission line (RLH-TL). The equivalent circuit for a RLH unit cell considering radiation effects is presented and analyzed in terms of the Bloch impedance and dispersion diagram. It has been found that when two radiation rates are identical, the Blockimpedance reduces to the characteristic impedance of the host conventional RH-TL. Besides, design equations for a unit cell for a specific phase shift at a given frequency are provided. The method of realizing uniform excitation along the RLH-TL is also proposed for antenna applications.

The Synthesis of (Y,Gd)$BO_3:Eu^{3+}$Phosphor by Ultrasonic Spray and Their Photoluminance Properties (초음파 분무에 의한 (Y,Gd)$BO_3:Eu^{3+}$ 형광체의 제조와 이의 발광 특성)

  • 김대수;김성우;이임렬
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 1999.11a
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    • pp.107-110
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    • 1999
  • The ultrasonic spray method was employed to make (Y,Gd)BO$_3$:Eu Phosphor, and its optical properties under 147nm VUV and 254 nm UV excitations were characterized and then compared with that produced by the solid-state reaction. The mixed solution of acetate hydrates of Y, Gd, Eu and boric acid diluted in water or methanol was used as the precursor fur the spray. It was found that (Y,Gd)BO$_3$:Eu phosphor made by this ultrasonic spray had a spherical shape and fine particle size of 1${\mu}{\textrm}{m}$. The crystalline structure for the as-sprayed phosphor was amorphous, but it converted into the same polycrystalline phase of solid state reaction after post heat treatment at 110$0^{\circ}C$ for 2hr. The emitting intensity under VUV and UV excitations for the spray-formed (Y,Gd)BO$_3$:Eu phosphor, however, was inferior to the later one. The excitation spectra were also studied and compared under VUV and UV excitations to explain the change of emitting intensity with Gd substitution in (Y$_{1-x}$ Gd$_{x}$)BO$_3$:Eu Phosphors made by spray and solid state reaction.on.

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Experimental and numerical analysis of the global behaviour of the 1:9 scale model of the Old Bridge in Mostar

  • Kustura, Mladen;Smoljanovic, Hrvoje;Nikolic, Zeljana;Krstevska, Lidija
    • Coupled systems mechanics
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    • v.10 no.1
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    • pp.1-19
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    • 2021
  • Composite nature of the masonry structures in general causes complex and non-linear behaviour, especially in intense vibration conditions. The presence of different types and forms of structural elements and different materials is a major problem for the analysis of these type of structures. For this reason, the analysis of the behaviour of masonry structures requires a combination of experimental tests and non-linear mathematical modelling. The famous UNESCO Heritage Old Bridge in Mostar was selected as an example for the analysis of the global behaviour of reinforced stone arch masonry bridges. As part of the experimental research, a model of the Old Bridge was constructed in a scale of 1:9 and tested on a shaking table platform for different levels of seismic excitation. Non-linear mathematical modelling was performed using a combined finite-discrete element method (FDEM), including the effect of connection elements. The paper presents the horizontal displacement of the top of the arch and the failure mechanism of the Old Bridge model for the experimental and the numerical phase, as well as the comparison of the results. This research provided a clearer insight into the global behaviour of stone arch masonry structures reinforced with steel clamps and steel dowels, which is significant for the structures classified as world cultural heritage.

Validation of and HPLC Method for Nadolol in Human Plasma and Evaluation of Its Pharmacokinetics after a Single-dose in Korean Volunteers (인체 혈장 중 나돌올의 HPLC 분석법 검증 및 단회투여 후 약물동태 연구)

  • Kang, Choon-Mo;Trung, Tarn-Quoc;Kim, Kyeong-Ho;Myung, Ja-Hye;Hwang, Sung-Joo;Kim, Mi-Young;Kuh, Hyo-Jeong
    • Journal of Pharmaceutical Investigation
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    • v.35 no.6
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    • pp.431-436
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    • 2005
  • A high-performance liquid chromatographic method was validated for quantitation of nadolol in human plasma. Nadolol and internal standard, pindolol, were extracted with tert-butyl methyl ether after addition of 10 M sodium hydroxide solution. The analytes were separated on a reverse phased C18 column using a mobile phase consisting of 0.05 M ammonium phosphate monobasic buffer, acetonitrile and methanol (81: 17:2 v/v/v) and detected using a fluorescence detector (excitation wavelength 230 nm, emission wavelength 294 nm). The method was specific and sensitive enough to detect as low as 3 ng/mL of nadolol in human plasma. Linear calibration range was 3-150 ng/mL with correlation coefficient greater than 0.999. The overall accuracy was in the range of 96.8 to 103% and precision C.V.(%) 7.30 to 12.2%. The recovery was approximately 100% and stability was confirmed during storage and sample preparation. The present HPLC method was successfully applied to study bioavailability after oral administration of 80 mg of nadolol in healthy Korean subjects. The mean $AUC_{t}$ was $1968{\pm}397\;ng{\cdot}hr/mL$ and $C_{max}$ of $186{\pm}79.3\;ng/mL$ was reached at $3.5{\pm}0.76\;hr$. The mean $t_{1/2}$ of nadolol was $17.3{\pm}2.59\;hr$.