• 제목/요약/키워드: 5 nm & 7 nm technology

검색결과 667건 처리시간 0.027초

Phase-Locked Loop with Leakage and Power/Ground Noise Compensation in 32nm Technology

  • Kim, Kyung-Ki;Kim, Yong-Bin;Lee, Young-Jun
    • JSTS:Journal of Semiconductor Technology and Science
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    • 제7권4호
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    • pp.241-246
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    • 2007
  • This paper presents two novel compensation circuits for leakage current and power supply noise (PSN) in phase locked loop (PLL) using a nanometer CMOS technology. The leakage compensation circuit reduces the leakage current of the charge pump circuit and the PSN compensation circuit decreases the effect of power supply variation on the output frequency of VCO. The PLL design is based on a 32nm predictive CMOS technology and uses a 0.9 V power supply voltage. The simulation results show that the proposed PLL achieves 88% jitter reduction at 440 MHz output frequency compared to the PLL without leakage compensator and its output frequency drift is little to 20% power supply voltage variations. The PLL has an output frequency range of 40 $M{\sim}725$ MHz with a multiplication range of 1-1023, and the RMS and peak-to-peak jitter are 5psec and 42.7 psec, respectively.

Li2O가 포함된 B2O3-SiO2-La2O3계 광학 유리 특성 (The Properties of Optical Glass of B2O3-SiO2-La2O3 System with Li2O)

  • 이지선;김세훈;김진호
    • 한국재료학회지
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    • 제32권12호
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    • pp.560-564
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    • 2022
  • In this study, lanthanum boron silicate glasses were prepared with a composition of x Li2O-(60-x)B2O3-5CaO-5BaO-7ZnO-10SiO2-10La2O3-3Y2O3 where x = 1,3,5,7, and 9 mol%. Each composition was melted in a platinum crucible under atmospheric conditions at 1,400 ℃ for 2 h. Clear glasses with a transmittance exceeding 85 % were fabricated. Their optical, thermal, and physical properties, such as refractive index, Abbe number, density, glass transition (Tg) and Knoop hardness were studied. The results demonstrated that refractive index was between 1.6859 and 1.6953 at 589.3 nm. The Abbe number was calculated using an equation for 589.3 nm (nd), 656.3 nm (nf) and 486.1 nm (nc) and was observed to be in the range from 57.5 to 62.6. As the Li2O content increased, the glass transition temperature of the optical glass decreased from 608 ℃ to 564 ℃. If glass mold pressing is performed using a material with a low transition temperature and high mechanical strength, then the optical glasses developed in this study can be completely commercialized.

Aspergillus niger KUF-04가 생산하는 Catalase (Catalase from Aspergillus niger KUF-04)

  • Yang, Ho-Suk;Yang, Han-Chul;Yoshiki Tani
    • 한국미생물·생명공학회지
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    • 제16권3호
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    • pp.193-198
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    • 1988
  • Aspergillus niger KUF-04에서 얻은 catalase는 gel 여과를 포함하여 5단계를 걸쳐 정제하였으며, 9% 회수율로 64배 정제되었다. 본 효소는 406, 503, 625nm에서 흡광을 나타내었으며, 특히 406nm에서 뚜렷한 흡수대를 보여주었다. 이 효소 활성의 최적 pH와 온도는 각각 7.0과 6$0^{\circ}C$이었다. 이 효소는 pH4.0과 8.0 사이에서 안정했으며 열에 대한 안정성은 2$0^{\circ}C$에서 5$0^{\circ}C$까지는 안정했으나, 8$0^{\circ}C$에서 20분간 반응시켰을 때 효소의 활성이 전부 소실되었다. 이 효소의 활성은 주로 hydroxylamine, potassium cyanide, sodium azide에 의해 저해되었다.

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융합 LED 광선치료가 아토피 피부염에 미치는 영향 (Therapeutic Effects of LED Fusion of Two Wavelength Bands on Atopic Dermatitis of NC/Nga Mice)

  • 이상민;최지혜;구본준;권중기
    • 한국응용과학기술학회지
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    • 제39권4호
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    • pp.552-559
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    • 2022
  • 아토피 피부염(Atopic dermatitis, AD)은 주로 5세 이전에 발병하여 심한 가려움을 동반하는 만성 염증성 피부질환이다. 본 연구의 목적은 NC/Nga 마우스를 AD 유사 증상에 대한 405 nm+ 850 nm LED 광선 치료의 효과를 조사하는 것이다. 마우스는 Normal (Vehicle), 아토피성 피부염 유발군 (CON), 405 nm+ 850 nm LED 광선 치료군 (LED)으로 나누어 난괴법을 이용하여 무작위 배치하여 실험을 진행하였다. LED 실험군은 하루 10분씩 405 nm+ 850 nm 파장의 LED 치료를 7일 간 실시하였다. LED 광선치료 연구는 Dermatics 점수의 개선을 측정하고 피부염으로 인한 표피조직 두께 감소를 관찰하였다. LED 광선 요법으로 인한 혈청 IL-1𝛽의 현저한 감소와 경피 수분 손실 및 혈청 IgE 농도 결과를 바탕으로 LED 광선 치료는 아토피 유발 생쥐의 정상적인 피부 상태 회복에 도움을 주었다. 본 연구 결과는 아토피 피부염 마우스 모델에서 적외선 영역의 광선과 blue light 영역의 광선의 동시 조사치료가 아토피 피부염 치료에 뛰어난 효능을 가지며, 두 파장의 LED의 동시 사용 가능성에 대하여 시사하였다.

YAlO3:Tbx3+에서 발광소멸 곡선을 이용한 에너지 전달에 관한 연구 (A Study on the Energy Transfer of YAlO3:Tbx3+ using Decay Curves)

  • 김광철;최진수
    • 반도체디스플레이기술학회지
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    • 제14권1호
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    • pp.13-17
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    • 2015
  • $YAlO_3:Tb{_x}^{3+}$ has been synthesized by a combustion process and the concentration x of Tb was varied from 0.001 and 0.05 mol% per mole of YAlO3. The energy transfer of $^5D_3{\rightarrow}^7F_6$(385nm) and $^5D_4{\rightarrow}^7F_5$(544nm) transitions on the $YAlO_3:Tb{_x}^{3+}$(x =0.001, 0.05) have been investigated by using decay curves. The energy transfer mechanism was explained by Inokuti and Hirayama model. The results of calculation and fitting showed that values of n are 6.11(x=0.01) and 6.13(x=0.005). These indicate that the energy transfer mechanism between $Tb^{3+}$ ions is dipole-dipole interaction.

A Study of Magnetic Field Annealing on Microstructures and Magnetic Properties of Nanocomposite Sm-Co/Co Films

  • Yang, Choong-Jin;You, Cai-Yin;Zhang, Z.D.;Kim, Kyung-Soo;Han, Jong-Soo
    • Journal of Magnetics
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    • 제7권2호
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    • pp.45-50
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    • 2002
  • A magnetic field annealing is firstly used for nanostructured Sm-Co/Co films, prepared by magnetron sputtering method. The effects of magnetic field annealing on single-layered Sm-Co films are different from those on multi-layered Sm-Co/Co films. A detailed analysis of microstructures and magnetic properties is made by means of HRTEM, Auger electron spectroscopy, XRD and Physical Property Measurement System (PPMS). From magnetic properties and microstructure analysis, it was confirmed that these differences originate from the effects of magnetic field annealing on crystallization behavior of the films. The relationship between magnetic properties and microstructures explains a different demagnetization process of single-layered and multilayered films. For the single-layered Sm-Co films, magnetic-field-annealing makes the main phases change from $CaCu_5/ to Zn_2Th_{17}$ structure, resulting in a decrease of coercivity. The results show that the magnetic-field-annealing is useful to improve the properties of nanostructured Sm-Co(30 nm)/Co(10 nm) films, which ascribe to improving the pinning effectiveness in coercivity mechanism and decreasing the magnetostatic interaction of films. A very high coercivity about 0.7 T was obtained from nanoscaled multi-layered Sm-Co(30 nm)-/Co(10 nm) films.

65 nm CMOS 공정을 이용한 W-대역 전력증폭기 설계 (Design of a W-Band Power Amplifier Using 65 nm CMOS Technology)

  • 김준성;권오윤;송림;김병성
    • 한국전자파학회논문지
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    • 제27권3호
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    • pp.330-333
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    • 2016
  • 본 논문에서는 차량 충돌 방지 장거리 레이더(Long Range Radar: LRR)을 위한 77 GHz 전력증폭기를 65 nm CMOS 공정을 이용하여 설계하였다. 제안한 회로는 3단 차동 전력증폭기로 공통 소스 구조와 트랜스포머를 사용했다. 측정결과로 77 GHz에서 18.7 dB의 전압 이득과 13 GHz의 3 dB 대역폭을 얻었다. 측정된 최대 출력 전력은 10.2 dBm, 입력 $P_{1dB}$는 -12 dBm, 출력 $P_{1dB}$는 5.7 dBm이며, 측정된 최대 전력 효율은 7.2 %이다. 본 전력증폭기는 1.2 V의 공급전원으로부터 140.4 mW의 DC 전력을 소모한다.

Synthesis and Characterization of TiO2, Cu2O and Al2O3 Aerosol Nanoparticles Produced by the Multi-Spark Discharge Generator

  • Efimov, Alexey;Lizunova, Anna;Sukharev, Valentin;Ivanov, Victor
    • 한국재료학회지
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    • 제26권3호
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    • pp.123-129
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    • 2016
  • The morphology, crystal structure and size of aerosol nanoparticles generated by erosion of electrodes made of different materials (titanium, copper and aluminum) in a multi-spark discharge generator were investigated. The aerosol nanoparticle synthesis was carried out in air atmosphere at a capacitor stored energy of 6 J, a repetition rate of discharge of 0.5 Hz and a gas flow velocity of 5.4 m/s. The aerosol nanoparticles were generated in the form of oxides and had various morphologies: agglomerates of primary particles of $TiO_2$ and $Al_2O_3$ or aggregates of primary particles of $Cu_2O$. The average size of the primary nanoparticles ranged between 6.3 and 7.4 nm for the three substances studied. The average size of the agglomerates and aggregates varied in a wide interval from 24.6 nm for $Cu_2O$ to 46.1 nm for $Al_2O_3$.

Luminescent Properties of LaBO3:RE3+ (RE=Tb, Ce) Phosphors for White Light Emitting Diodes

  • Cho, Shinho
    • Current Photovoltaic Research
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    • 제2권2호
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    • pp.53-58
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    • 2014
  • $Tb^{3+}$ - or $Ce^{3+}$-doped $LaBO_3$ phosphors were synthesized by a solid-state reaction process with different concentrations of activator ions. The XRD spectra showed the monoclinic $LaBO_3$ pattern with the main peak occurring at (014) plane, irrespective of the kind of activator ions. The crystallite size was determined by using the Scherrer formula, and the maximum was obtained with an activator concentration of 0.05 mol for both phosphors. The emission spectra of $LaBO_3$ phosphors doped with $Tb^{3+}$ ions under excitation at 269 nm exhibited three major emission bands at 488, 544, and 587 nm. The strongest emission was green at 544 nm owing to the $^5D_4-^7F_5$ transition at a $Tb^{3+}$ ion concentration of 0.05 mol. For the $Ce^{3+}$-doped $LaBO_3$ phosphors, one strong blue band centered at 469 nm and weak multipeaks were observed. These results suggest that the optimum green and blue emission can be realized by controlling the concentration and type of activator ions incorporated in the host crystal.

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

  • Lim, Chang Sung
    • 분석과학
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    • 제27권6호
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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.