• 제목/요약/키워드: neutron diffraction

검색결과 123건 처리시간 0.03초

중성자회절법을 이용한 $(Fe_{0.61}Ni_{0.39})_3V$ 합금의 규칙- 불규칙 상전이 연구 (Study of Order-Disorder Phase Transition of $(Fe_{0.61}Ni_{0.39})_3V$V Alloy by Neutron Diffraction Method)

  • 이정수;이창희
    • 한국결정학회지
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    • 제13권1호
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    • pp.36-40
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    • 2002
  • 중성자회절법을 이용하여 여러 다른 조건으로 열처리한 (Fe/sub 0.61/Ni/sub 0.39/)₃V 합금 분말시료의 장거리 규칙도를 측정하여 규칙-불규칙 상전이의 정도를 조사하였다. 조사 결과 680℃-94 h 열처리 시료는 완전 불규칙 상태로 상전이가 발생하지 않았으며 면심입방구조를 보였다. T < 640℃의 조건에서 열처리한 시료들은 모두 장거리 규칙도 0 < S < 1으로 면심입방구조의 일부가 단순입방구조로 상전이 함을 보여주었다. 또한 Cowley의 S-T/T/sub c/ 관계식으로부터 465℃-144 h 으로 열처리한 시료가 열평형상태에 가장 근접하였음을 확인하였다

Crystal Structure of High Temperature Phase in ${Bi_2}{O_2}$-layered Perovskites ${ABi_2}{M_2}{O_9}$(A=Pb, Sr, M=Nb, Ta)

  • Kim, Jeong-Seog;Cheon, Chae-il;Lee, Chang-Hee;Choo, Woong-Gil
    • 한국세라믹학회지
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    • 제38권11호
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    • pp.962-966
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    • 2001
  • Crystal structure of PbBi$_2$Nb$_2$$O_{9}$ and $Sr_{1.2}$$Bi_{1.8}$Ta$_2$$O_{9}$ were determined by Rietveld method using neutron diffraction data in the temperature range of 300 K~1273K. Phase transition temperature were measured from the dielectric permittivitytemperature curve. The PbBi$_2$Nb$_2$$O_{9}$ showed a phase transition at about 810 K. In the Sr-excess compound $Sr_{1.2}$$Bi_{1.8}$Ta$_2$$O_{9}$ the phase transition was suppressed down to room temperature. Several structural models were tested by the Rietiveld refinement. Based on the \`R\` values and the structural parameters, the B2cb model is judged to be the most feasible one for the high temperature phase at above 810 K of the PbBi$_2$Nb$_2$$O_{9}$. The $Sr_{1.2}$$Bi_{1.8}$Ta$_2$$O_{9}$ sample was refined to show the most reliable results by the Am2m model.sults by the Am2m model.

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고 분해능 중성자 회절 실험에 의한 YMn2-xFexO5 (x = 0.00, 0.01)의 다강체 특성 연구 (The Multiferroic Properties Study of YMn2-xFexO5 (x=0.00, 0.01) by Neutron Diffraction)

  • 김동현;김철성
    • 한국자기학회지
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    • 제17권5호
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    • pp.183-187
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    • 2007
  • 다강체 물질인 망간 산화물 $YMn_{2-x}Fe_xO_5$ (x = 0.00, 0.01)를 졸-겔법을 이용하여 합성하였다. 결정학적 및 자기적 성질을 알아보기 위해 x-선 회절기, 고 분해능 중성자 분말 회절기, 진동 자화율 측정기를 이용하였으며, 전기적 성질은 Physical Property Measurement System(PPMS)를 사용하여 연구하였다. x-선 회절 분석 결과 $YMn_2O_5$ 시료의 결정구조는 격자상수 $a_0=7.275\;{\AA},\;b_0=8.487\;{\AA},\;c_0=5.674\;{\AA}$을 갖는 단일상의 orthorhombic 구조로 분석 되었고, Fe가 치환됨에 따른 격자상수의 변화는 없었다. $YMn_2O_5$의 중성자 회절 실험 결과 다강체 특성이 발현되는 온도($T_2=18K$)에서 격자상수의 변화 및 자기 구조에 의해 나타나는 회절 피크가 변화하는 모습을 확인하였다. 또한 우리는 뫼스바우어 분광법을 이용한 전기 사중극자 분열값의 확인을 위하여 $YMn_{1.99}Fe_{0.01}O_5$를 합성하였고 $YMn_2O_5$$YMn_{1.99}Fe_{0.01}O_5$의 물리적 특성의 변화는 없는 것으로 확인하였다[1]. $T_2$에서 전기 사중 극자 분열값의 변화가 확인된 $YMn_{1.99}Fe_{0.01}O_5$ 시료의 유전상수 및 자화율 그래프를 통하여 다강체 특성이 서로 연관되어 상호작용을 함을 알 수 있었다.

Soild-state reaction in Ti/Ni multilayers

  • 이주열;이영백;김태하;김기원
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 1999년도 제17회 학술발표회 논문개요집
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    • pp.140-140
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    • 1999
  • Ti/Ni multilayered films (MLF) are ideal for neutron optics particularly in neutron guides and focusing devices. This system also possesses the tendency of amorphization through a solid-state reaction (SSR). This behaviors are closely related to the electronic structures and both magneto-optical (MO) and optical properties of metals depend strongly on their electron energy structures. Mutual inter-diffusion of the Tin and Ni atoms in the MLF caused by a low temperature annealing should decrease the thickness of pure Ni, as well as change the chemical and atomic order in the reactive zone. The application of the MO spectroscopy to the study of SSR in the MLF allows us to obtain an additional information on the changes in the atomic and chemical orders in the interface region. The optical one has no restriction on the magnetic state of the constituent sublayers. Therefore, the changes in magnetic, MO and optical properties of the Ti/Ni MLF due to SSR can be expected. To the best of our knowledge, the MO and optical spectroscopies were not used for this purpose. SSR has been studied in the series of the Ti/Ni MLFs with bilayer periods of 0.65-22.2nm and constant ratio of the Ti to Ni sublayers thickness by using MO and optical spectroscopies as well as an x-ray diffraction. The experimental MO and optical spectra are compared with the computer-simulated spectra, assuming various interface models. The relative changes in the x-ray diffraction spectra and MO properties of the Ti/Ni MLF caused by annealing are bigger for the multilayers with "thick" sublayers, or the SSR with the formation of amorphous alloy takes place mainly in the Ti/Ni multilayers with "thick" sublayers, while in the nominal threshold thickness of the Ni-sublayer for the observation of the equatorial Kerr effect in the as-deposited and annealed Ti/Ni MLFs of about 3.0 and 4.5nm thick is explained by the formation of amorphous alloy during the deposition or the formation of the nonmagnetic alloyed regions between pure components as a result of the SSR. For the case of Ti/Ni MLF the MO approach is more sensitive for the determination of the thickness of the reacted zone, while x-ray diffraction is more useful for structural analyses.structural analyses.

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MgB2 초전도 특성에 대한 나노 FexC 첨가 효과 (Effects of Nano FexC Addition on Superconducting Properties of MgB2)

  • 이동건;이지현;전병혁;박순동;엄영랑;박해웅;김찬중
    • 한국분말재료학회지
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    • 제19권2호
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    • pp.146-150
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    • 2012
  • The effects of nano $Fe_xC$ addition to superconducting properties of $in$ $situ$ processed $MgB_2$ superconductors was examined. 0.1 wt.% and 1 wt.% nano $Fe_xC$ powders were mixed with boron and magnesium powders by ball milling. The powder mixtures were made into pellets by uniaxial pressing. The pellets were heat-treated at $700^{\circ}C-900^{\circ}C$ in argon atmosphere for $MgB_2$ formation. It was found by powder X-ray diffraction that the raw powders were completely converted into $MgB_2$ after the heat treatment. The superconducting transition temperature ($T_c$) and critical current density ($J_c$), estimated from susceptibility-temperature and $M-H$ curves, were decreased by nano $Fe_xC$ addition. The $T_c$ and $J_c$ decrease by nano $Fe_xC$ addition are attributed to the incorporation of iron and carbon with $MgB_2$ lattices (Fe substitution for Mg and C substitution for B) due to the high reactivity of the nano $Fe_xC$ powder.

중성자를 이용한 리튬이온 이차전지 전극 구조분석 (Structure Analysis of Li-ion Battery Using Neutron Beam Source)

  • 김창섭;박헌용;양연화;김지영;성백석;김건
    • 전기화학회지
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    • 제10권1호
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    • pp.20-24
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    • 2007
  • 최근 높은 에너지 밀도를 갖고 있는 리튬 이온 이차전지에 대한 관심이 높다. 리튬 이온 이차전지는 이미 휴대용 기기로 널리 적용되고 있으며, 하이브리드 전기자동차와 같은 고출력 전지시스템에 적용을 위해 연구되고 있다. 리튬 이온 이차전지의 전극 소재는 리튬 이온의 이동에 의해서 충전 및 방전되는 현상을 활용한다. 전극으로부터 리튬 이온이 이동될 때 전극내의 구조 변화가 발생한다. 전극의 구조분석은 중성자 또는 X-선을 이용하여 분석할 수 있다. X-선은 분석 시간이 짧고, 쉽게 분석할 수 있다는 장점이 있으나 원자내의 전자구름과의 산란을 응용하므로 전자가 적은 가벼운 원소의 경우 분석이 어려운 단점이 있다. 리튬도 원자량이 작아서 X-선 만으로는 리튬의 정확한 위치에 대한 분석이 어렵다. 중성자 분석기술은 이에 대한 해답이 될 것이다. 본 자료에서는 중성자를 활용한 전극물질의 구조 분석 사례 및 그 원리에 대해서 논의하고자 한다.

Development of liquid target for beam-target neutron source & two-channel prototype ITER vacuum ultraviolet spectrometer

  • Ahn, B.N.;Lee, Y.M.;Dang, J.J.;Hwang, Y.S.;Seon, C.R.;Lee, H.G.;Biel, W.;Barnsley, R.;Kim, D.E.;Kim, J.G.
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2011년도 제40회 동계학술대회 초록집
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    • pp.421-422
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    • 2011
  • The first part is about development of a liquid target for a neutron source, which is designed to overcome many of the limitations of traditional beam-target neutron generators by utilizing a liquid target neutron source. One of the most critical aspects of the beam-target neutron generator is the target integrity under the beam exposure. A liquid target can be a good solution to overcome damage to the target such as target erosion and depletion of hydrogen isotopes in the active layer, especially for the one operating at high neutron fluxes with no need for water cooling. There is no inherent target lifetime for the liquid target neutron generator when used with continuous refreshment of the target surface exposed to the energetic beam. In this work, liquid target containing hydrogen has been developed and tested in vacuum environment. Potentially, liquid targets could allow a point neutron source whose spatial extension is on the order of 1 to $10{\mu}m$. And the second is about the vacuum ultraviolet (VUV) spectrometer which is designed as a five-channel spectral system for ITER main plasma measurement. To develop and verify the design, a two-channel prototype system was fabricated with No. 3 (14.4 nm~31.8 nm) and No. 4 (29.0 nm~60.0 nm) among the five channels. For test of the prototype system, a hollow cathode lamp is used as a light source. The system is composed of a collimating mirror to collect the light from source to slit, and two holographic diffraction gratings with toroidal geometry to diffract and also to collimate the light from the common slit to detectors. The two gratings are positioned at different optical distances and heights as designed. To study the appropriate detector for ITER VUV system, two different electronic detectors of the back-illuminated charge coupled device and the micro-channel plate electron multiplier were installed and the performance has been investigated and compared in the same experimental conditions. The overall system performance was verified by measuring the spectrums.

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The Determination of Stress Distribution in WC-Ni Cemented Carbide Composites by Neutron Diffraction

  • Seol, Kyeongwon
    • 한국재료학회지
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    • 제5권2호
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    • pp.232-238
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    • 1995
  • The thermal stress distribution of WC and Ni binder phases In WC-26st.%Ni and WC-6wt.%Ni composites has been investigated over the temperature range 100-900 K using a time-of-flight neutron diffractometer. To determine the stress distribution, the breadths of WC and Ni peaks in the reference powder and the composites were analyzed. The peak breadths were corrected for particle size effect using a procedure based on the integral peak breadth method of particle size-strain analysis. The result shows a broad range of strain, and thus stress, is present in the WC and Ni binder phases of the composites. The strain distribution of both phases broadens as the temperature decreases, and some fraction of total strain distribution of the WC phase remains tensile regardless of the temperature. The strain distribution of the WC phase broadens as the binder content increases, and that of Ni binder phase broadens as the binder content decreases, which means the strain distribution broadens as the absolute value of residual stress increase.

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MONTE-CARLO SIMULATION OF NEUTRON STAR ORBITS IN THE GALAXY

  • TAANI, ALI
    • 천문학논총
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    • 제30권2호
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    • pp.583-584
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    • 2015
  • In this paper, the numerical results concerning different orbits of a 3D axisymmetric non-rotating galactic potential are presented. We use $Paczy{\acute{n}}ski^{\prime}s$ gravitational potential with different birth velocity distributions for the isolated old Neutron Star (NS) population. We note some smooth non-constant segments corresponding to regular orbits as well as the characterization of their chaoticity. This is strongly related to the effect of different kick velocities due to supernovae mass-loss and natal kicks to the newly-formed NS. We further confirm that the dynamical motion of the isolated old NSs in the gravitational field becomes obvious, with some significant diffraction in the symmetry of their orbital characteristics.

기계적 합금화에 의한 Cr-N계 합금의 비정질화 과정 (Amorphization Process of Cr-N Alloy System by Mechanical Alloying)

  • 이충효;이성희;이상진;권영순
    • 한국분말재료학회지
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    • 제10권4호
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    • pp.288-293
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    • 2003
  • Mechanical alloying (MA) by high energy ball mill of Pure chromium Powders was carried out under the nitrogen gas atmosphere. Cr-N amorphous alloy powders have been produced through the solid-gas reaction subjected to MA. The atomic structure during amorphization process was observed by X-ray and neutron diffractions. An advantage of the neutron diffraction technique allows us to observe the local atomic structure surrounding a nitrogen atom. The coordination number of metal atoms around a N atom turns out to be 5.5 atoms. This implies that a nitrogen atom is located at both of centers of the tetrahedron and octahedron formed by metal atoms to stabilize an amorphous Cr-N structure. Also, we have revealed that a Cr-N amorphous alloy may produced from a mixture of pure Cr and Cr nitrides powders by solid-solid reaction during mechanical alloying.