• 제목/요약/키워드: B1 field

검색결과 2,607건 처리시간 0.03초

초미세결정립과 비정질이 공존하는 $Fe_{73.9}$$Cu_{1.0}$$Nb_{3.5}$$Si_{14.0}$$B_{7.6}$ 합금의 자기장 중 열처리 (Heat Treatment Effects of $Fe_{73.0}Cu{1.0}Nb_{3.5}Si_{14.0}B_{7.6}$Alloy with Imbedded Nanocrystalline Phase under Magnetic Field)

  • 양재석;손대락;조육
    • 한국자기학회지
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    • 제8권1호
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    • pp.13-20
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    • 1998
  • 초미세결정립과 비정질을 동시에 포함하는 리본형 Fe73.9Cu1.0Nb3.5Si14.0B7.6 합금을 자기장 중 열처리한 시편의 결정?적 특성 및 고주파 연기자 특성을 인가 자기장과 열처리 온도에 따라하여 조사아였다. 제조된 리본의 표면에 석출된 Fe-Si 초미세결정립은 (400) 우선방위를 나타내는 동시에 리본길이방향으로 [011] 결정측이 형성되어 있음을 확인하엿다. 자기장을 인가하지 않거나 길이방향으로 자기장을 인가하여 열처리할 때 45$0^{\circ}C$에소 Fe-Si 초미세결정립이 석출되다, 폭방향의 자기장을 인가한 경우 초미세결정립의 석출은 지연되어 55$0^{\circ}C$에서 나타남을 확인하였다. 길이방향으로 자기장을 인가할 때 시편의 결정화 정도는 외부 자기장을 인가하지 않은 경우에 비해 조금 증가하였다. 그러나, 시편의 각도를 기울여 측정된 X-선 회절패턴으로부터 시편내부는 표면과 달리 결정화가 진행되고 있음을 확인하였다. 열처리한 시편의 포화자기유도는 1.3T로 비슷하였다. 열처리전 리본의 보자력의 크기는 1.06A/츠이었으나, 열처리한 시편은 열처리 온도가 40$0^{\circ}C$에서 55$0^{\circ}C$로 증가함에 따라 0.56A/cm에서 0.1A/cm로 감소하였다. 폭방향의 자기장을 인가한 경우 각형비는 자기장을 인가하지 않거나 길이방향으로 자기장을 인가하여 열처리한 시편의 각형비보다 작았다.

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단일층 $d^2B_{z}$/dxdy SQUID 2차 미분기 설계 및 제작 (Fabrication of sing1e layer $d^2B_{z}$/dxdy second-order SQUID gradiometer)

  • 황윤석;박승문;이순걸;김인선;박용기
    • Progress in Superconductivity
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    • 제4권2호
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    • pp.109-113
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    • 2003
  • We have developed a planar-type single layer second-order $high-T_{c}$ SQUID gradiometer, which can detect the $d^2$$B_{z/}$dxdy of the second-order field gradient. This SQUID gradiometer consists of four-way 'clover-leaf' pick-up loops and is coupled directly to a 4-junction dc SQUID in such a way that the coupling polarity of the two diagonal loops is opposite to that of the other two loops. The pickup loops are intrinsically balanced for both uniform field and the 1 st-order field gradient. The $YBa_2$$Cu_3$$O_{7}$ thin film was made by pulsed laser deposition method on $SrTiO_3$ single crystal substrate and patterned by photolithography with Ar ion milling technique. Response of this gradiometer was tested for both uniform field and the 2nd-order field gradient. Details of the design, fabrication, and results will be discussed.

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Magnetic Anisotropy Energy Distribution and Magnetization of CoPt Nanoparticles Encaged in Protein Shell

  • Lee, T.H.;Suh, B.J.;Jang, Z.H.
    • Journal of Magnetics
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    • 제22권1호
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    • pp.1-6
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    • 2017
  • Magnetic properties of CoPt nanoparticles (average size = 2.1 nm) encapsulated in synthesized protein shell have been investigated with SQUID (Superconducting Quantum Interference Device) magnetometer and analyzed by the recently developed non-equilibrium magnetization calculation by our group [T. H. Lee et al., Phys. Rev. B 90, 184411 (2014)]. Field dependence of magnetization measured at 2 K was successfully analyzed with modified Langevin function. In addition, small hysteresis loops having the coercive field of 890 Oe were observed at 2 K. Temperature dependence of magnetization has been measured with zero field cooled (ZFC) and field cooled (FC) protocol with slightly modified sequence in accordance with non-equilibrium magnetization calculation. The analysis on the M vs. T data revealed that the anisotropy energy barrier distribution is found to be very different from the log-normal distribution found in a size distribution. Zero temperature coercive field and Bloch coefficient have also been extracted from the analysis and the validity of those values is checked.

7T MRI에서 B1 필드 조정을 위해 페로브스카이트 재료를 이용한 자기공명영상 향상 (MRI Enhancement using Perovskite Material for B1 Field Control at 7T)

  • 김용태;김주연;백현만
    • 한국방사선학회논문지
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    • 제15권4호
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    • pp.565-573
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    • 2021
  • 인체 내 전자기장의 공간 분포는 고 유전율 재료를 사용하여 비교적 간단하게 조정할 수 있다. 이 방법은 다른 방법에 비해 보완적인 성격이 강하지만 특정 응용 분야에서 강력한 유전체 시밍용 도구로 활용될 수 있다. 기하학적으로 자유로운 형상으로 제조 가능하며 시스템의 어떠한 변경 없이 목적에 따라 제작된 패드를 적용할 수 있다. 특히 초 고자장(ultrahigh magnetic field UHF) MRI에서 높은 작동 주파수로 인해 낮은 감도 (low sensitivity)를 갖는 송신 (B1+) 및 수신 (B1-) 필드의 강도를 높이는 데 사용되는 임상목적의 고 유전율 패드는 잠재적 가치가 상당히 클 뿐만 아니라 그 효과가 클 것으로 예상되는 UHF MRI에 적용된 연구가 적기 때문에 이 연구에서는 티탄산 칼슘의 현탁액으로 제조된 고 유전율 패드를 실험실에서 직접 개발하였으며 UHF 7T 자기공명영상 MRI의 다양한 프로토콜에서 임상적으로 유용한 영상의 신호증가를 확인하였다.

$3{\beta}$-Hydroxy-12-oleanen-28-oic Acid 유도체들의 PTP-1B 저해활성에 대한 CoMFA 분석과 활성 분자들의 예측 (CoMFA Analysis on Inhibitory Effect of $3{\beta}$-Hydroxy-12-oleanen-28-oic Acid Analogues on PTP-1B Activity and Prediction of Active Compounds)

  • 김상진;김세곤;성낙도
    • 대한화장품학회지
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    • 제34권2호
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    • pp.109-115
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    • 2008
  • 기질 화합물로써 $3{\beta}$-hydroxy-12-oleanen-28-oic acid 유도체들의 치환기($R_1{\sim}R_4$)가 변화함에 따른 protein tyrosine phosphatase(PTP)-1B의 저해활성에 관한 비교 분자장 분석(CoMFA) 모델을 유도하고 정량적으로 검토하였다. 최적의 CoMFA F1 모델은 가장 높은 예측성과 상관성($r^2_{cv.}=0.654$$r^2_{ncv.}=0.995$)을 나타내었다. 저해활성에 관한 CoMFA장 기여비율(%)의 순서는 입체장(53.0%), 정전기장(36.2%) 및 소수성장(10.8%) 이었다. 등고도 분석 결과로부터 저해활성은 기질 분자 내 $R_4$-치환기에 의존적이었으며 특히 melanin 저해활성이 높은 새로운 화합물(P1 및 P2)이 예측되었다.

형광 나노포러스 박막의 온도장 가시화 (The Visualization of Temperature Field for Nanoporous Thin Film using Laser-Induced Fluorescence.)

  • 오영수;백인기;전필수;김현정;유재석
    • 대한기계학회:학술대회논문집
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    • 대한기계학회 2007년도 춘계학술대회B
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    • pp.2459-2464
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    • 2007
  • In present study, a temperature field of specimens which was coated with fluorescence dye such as Rhodamine-B(Rh-B) has been measured, based on the fluorescence intensity. Silica(SiO2) nano porous structure with 1um thickness was constructed on a cover glass, and fluorescence dye was digested into these porous thin films. To optimize manufacturing coating process, various solvents, Rh-B concentration, and other chemical materials were applied to fabricate the specimen and all specimens were measured on the various temperature conditions. For the measurement, a 14 bit cooled CCD camera with 1600 by 1200 spatial resolution is equipped with epifluorescence microscope to obtain only fluorescence intensity from 1.2 mm by 0.9 mm field of view of the illuminated coated specimen.

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Integrated-Optic Electric-Field Sensor Utilizing a Ti:LiNbO3 Y-fed Balanced-Bridge Mach-Zehnder Interferometric Modulator With a Segmented Dipole Antenna

  • Jung, Hongsik
    • Journal of the Optical Society of Korea
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    • 제18권6호
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    • pp.739-745
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    • 2014
  • We have demonstrated a $Ti:LiNbO_3$ electro-optic electric-field sensor utilizing a $1{\times}2$ Y-fed balanced-bridge Mach-Zehnder interferometric (YBB-MZI) modulator, which uses a 3-dB directional coupler at the output and has two complementary output waveguides. A dc switching voltage of ~25 V and an extinction ratio of ~12.5 dB are observed at a wavelength of $1.3{\mu}m$. For a 20 dBm rf input power, the minimum detectable electric fields are ~8.21, 7.24, and ~13.3 V/m, corresponding to dynamic ranges of ~10, ~12, and ~7 dB at frequencies of 10, 30, and 50 MHz respectively. The sensors exhibit almost linear response for an applied electric-field intensity from 0.29 V/m to 29.8 V/m.

분야연상어를 이용한 화제분야의 계산방법과 단락검색 (Passage Retrieval and Calculation Method of Topic Field by Using Field-Associated Terms)

  • 이상곤
    • 정보처리학회논문지B
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    • 제12B권1호
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    • pp.57-68
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    • 2005
  • 텍스트에 임베디드 되어 있는 부가적인 정보를 이용하여 문서의 실제적인 의미단위인 텍스트를 분리하는 단락검색은 중요한 기술이다. 본 논문에서는 문서의 분야에 적합한 단락만을 분리하여 사용자의 요구에 적합한 단락을 추출하는 기술을 설명한다. 문서에서 분야연상어론 추출하여, 각 문장마다 화제의 분야가 어떻게 커져가고, 줄어들고, 변화하여 가는지를 측정하는 방법을 실험을 통해 설명한다. 긴 문서에서 어떤 화제가 출현하는가를 파악하고, 화제가 계속되거나 혹은 전환되는 지점을 측정하고, 분야별로 단락을 구분하는 방법을 계산한다. 12,500개의 한국어 신문기사를 이용하여 실험한 결과 $88{\%}$의 정확률과 $78{\%}$의 재현율을 얻을 수 있었다.

Whole brain radiotherapy using four-field box technique with tilting baseplate for parotid gland sparing

  • Park, Jaehyeon;Yea, Ji Woon
    • Radiation Oncology Journal
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    • 제37권1호
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    • pp.22-29
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    • 2019
  • Purpose: The aim of this study is to evaluate the efficacy and feasibility of four-field box whole brain radiotherapy (FB-WBRT) with tilting baseplate by comparing bilateral WBRT (B-WBRT). Methods and Materials: Between March 2016 and September 2018, 20 patients with brain metastases underwent WBRT using the four-field box technique. WBRT is performed with a dose of 30 Gy in 10 fractions daily. Two computed tomography simulations per person were performed. One was in the traditional supine position for B-WBRT and the other by applying the tilting acrylic supine baseplate to elevate the head by 40° for FB-WBRT. The B-WBRT used the field-in-field technique, which is the most commonly used method in our institution. The FB-WBRT comprised anterior, posterior, and bilateral beams. A wedge was applied in anterior and posterior fields to compensate for skull convexity. Results: The average of Dmean of both parotid glands was 10.2 Gy (range, 3.8 to 17.8 Gy) in B-WBRT and 5.4 Gy (range, 2.0 to 11.7 Gy) in FB-WBRT (p < 0.05). Compared to B-WBRT, FB-WBRT reduced the mean dose of the right and left parotid glands from 10.1 Gy to 4.9 Gy and from 10.4 Gy to 5.8 Gy, respectively (p < 0.05). Further, V5, V10, V15, V20, and V25 for the parotid gland decreased significantly in FB-WBRT (p < 0.05). The Dmax and Dmean of lens decreased according to the dose-volume histogram. Conclusion: Compared to B-WBRT, FB-WBRT with a tilting baseplate is a simple and effective method that takes feature of noncoplanar beam to protect the parotid gland.

SQUID 센서 기반의 극저자장 자기공명 장치를 위한 사전자화코일 전류구동장치 개발 (Development of Prepolarization Coil Current Driver in SQUID Sensor-based Ultra Low-field Magnetic Resonance Apparatuses)

  • 황성민;김기웅;강찬석;이성주;이용호
    • Progress in Superconductivity
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    • 제13권2호
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    • pp.105-110
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    • 2011
  • SQUID sensor-based ultra low-field magnetic resonance apparatus with ${\mu}T$-level measurement field requires a strong prepolarization magnetic field ($B_p$) to magnetize its sample and obtain magnetic resonance signal with a high signal-to-noise ratio. This $B_p$ needs to be ramped down very quickly so that it does not interfere with signal acquisition which must take place before the sample magnetization relaxes off. A MOSFET switch-based $B_p$ coil driver has current ramp-down time ($t_{rd}$) that increases with $B_p$ current, which makes it unsuitable for driving high-field $B_p$ coil made of superconducting material. An energy cycling-type current driver has been developed for such a coil. This driver contains a storage capacitor inside a switch in IGBT-diode bridge configuration, which can manipulate how the capacitor is connected between the $B_p$ coil and its current source. The implemented circuit with 1.2 kV-tolerant devices was capable of driving 32 A current into a thick copper-wire solenoid $B_p$ coil with a 182 mm inner diameter, 0.23 H inductance, and 5.4 mT/A magnetic field-to-current ratio. The measured trd was 7.6 ms with a 160 ${\mu}F$ storage capacitor. trd was dependent only on the inductance of the coil and the capacitance of the driver capacitor. This driver is scalable to significantly higher current of superconducting $B_p$ coils without the $t_{rd}$ becoming unacceptably long with higher $B_p$ current.