• Journal of Magnetics
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• v.8 no.2
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• pp.85-88
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• 2003

The magnetic and transport properties far single crystals of Ru-doped mono-layered manganites $La_{0.5}Sr_{1.5}-Mn_{1-x}Ru_xO_4$ (0$\leq$$\chi$$\leq$0.1) have been studied using neutron diffraction and magnetization measurements. Temperature dependent magnetization data reveal that with an increase in the Ru concentration the parent charge ordered antiferromagnetic state is gradually destroyed and new ferromagnetic phase evolves. In the low Ru-doped system spin glass behavior is apparent in low temperature region, which is confirmed by ac and do magnetization measurements. The competing magnetic interaction between Mn/Mn and Mn/Ru couples is the most likely cause of the spin glass transition.

• Journal of Magnetics
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• v.9 no.3
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• pp.89-95
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• 2004

Magnetization and electrical resistivity measurements in the wide temperature and field ranges were performed on single crystals of $UGe_2$. The presence of extremely large anisotropy in the temperature dependence of the susceptibility and magnetization has confirmed the previously published results. The dependence of spontaneous magnetization, ${\sigma}_s$, on temperature has been inferred from the Arrot plot and compared to that determined from neutron diffraction data. The earlier transversal and present longitudinal results on the magnetoresistivity are discussed in the terms of possible f-electron dualism in $UGe_2$ and its connection with the occurrence of superconductivity under pressure in this compound.

• Journal of the Korean Crystal Growth and Crystal Technology
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• v.9 no.1
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• pp.132-136
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• 1999

Mechanical alloying (MA) by ball mill of $Fe_{30}Cr_{70}$ elemental powders was carried out under the nitrogen gas atmosphere. Amorphization has been observed in this case, while MA under an inert argon gas atmosphere produces the bcc solid solution. The DSC spectrum for the mechanically alloyed $(Fe_{30}Cr_{70})_{0.85}N_{0.15)$powders exhibits a sharp exothermic peak due to crystallization at about $550^{\circ}C$. Structural transformation from the bcc crystalline to amorphous states was observed through X-ray and neutron diffractions. During amorphization process the octahedral unit, which is typical of a polyhedron formed in any crystal structures, was preferentially destroyed and transformed into the tetrahedral unit. Futhermore, neutron diffraction measurements revealed that a nitrogen atom is situated at a center of the tetrahedron formed by metal atoms.

• Progress in Superconductivity
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• v.9 no.2
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• pp.167-172
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• 2008

We fabricated $YBa_2Cu_3O_{7-x}$(YBCO) films on (00l) $LaAlO_3$ substrates prepared by metal organic deposition(MOD) method using trifluoroacetate(TFA) solution. The films with various thicknesses were prepared by repeating the dip-coating and calcining processes. The effects of film thickness on phase formation, microstructures, and critical properties were evaluated by X-ray diffraction, scanning electron microscopy, and transmission electron microscopy. The microstructure and resultant critical current($I_C$) and critical current density($J_C$) varied remarkably with film thickness: The ($I_C$) value increased from 39 to 160 A/cm-width as the number of coatings increased from one to four, while the corresponding $J_C$ was measured to be in the range of $0.84-1.21\;MA/cm^2$. Both the $I_C$ and $J_C$ decreased when an additional coating was applied due to microstructural degradation, indicating that the optimum thickness is in the range of $1.1-1.8\;{\mu}m$. The possible cause for the decrease in the $I_C$ and $J_C$ value for film thicker than $1.8\;{\mu}m$ include non-uniform thickness, increased surface roughness, and the poor formability of the YBCO phase and texture arising from the insufficient heat treatment time with respect to the increased thickness.

• Journal of the Korean Magnetics Society
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• v.17 no.2
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• pp.86-89
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• 2007

[ $FeCr_2Se_4$ ] prepared under the high pressure (3 GPa) has been studied with x-ray, neutron diffraction techniques, superconducting quantum interference device (SQUID) magnetometer, resistance, and Mossbauer spectroscopy. The temperature dependence of resistance is explained by Mott-VRH and small polaron model for the regions I (T<20 K) and II (T>42 K), respectively. Neutron diffraction results show an antiferromagnetic spin-lattice coupling near the Neel temperature. So finally the distance of atom is enlarged in region (110$FeCr_2Se_4$ shows convex type of temperature dependence.

• Journal of the Korean Ceramic Society
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• v.38 no.11
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• pp.967-972
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• 2001

The crystal and defect structures of U $O_{x}$(x=2.0, 2.03, 2.14, 2.19, 2.20 and 2.26) were analysed by rietveld refinement and the results were compared to the U-O phase diagram. Neutron diffraction data were collected in the temperature range of RT~100$0^{\circ}C$. The specimens of x=2.14, 2.19, and 2.20 consisted of two phase: $UO_{2+x}$(Fm3m, a≒5.4$\AA$) and $U_4$$O_{9}$(I43d, a≒21.8$\AA$). The proportion of the $UO_{2+x}$(Fm3m) phase increased with increasing the temperature. The variation of the proportion of the two phases with temperature in the U $O_{2.2}$ and U $O_{2.18}$ samples showed some deviation from the expected values from the phase diagram especially at the high temperature range. The phase transitions ${\gamma}$longrightarrow$\beta$longrightarrow$\alpha$ of $U_4$$O_{9}$ were discussed in relation with the phase separation.eparation.ion.

• Korean Journal of Materials Research
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• v.4 no.6
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• pp.620-625
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• 1994

We recently showed from the neutron diffraction and extended X-ray absorption fine structure studies the structural evidence for the formation of an amorphous phase in immiscible Cu-Ta system subjected to mechanical alloying. In a system with a positive heat of mixing like Cu-Ta, we consider it necessary to confirm the formation of an amorphous phase not only from the structural studies but also from a change in the electronic properties. We show the electronic evidence for the formation of the chemical bonding between the unlike atoms Cu and Ta for the 120 h-milling sample through changes in superconducting transition temperature and X-ray photoemission spectroscopy valence band structure.

• Proceedings of the Materials Research Society of Korea Conference
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• 2003.03a
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• pp.112-112
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• 2003

최근 자성반도체(diluted magnetic semiconductor; DMS)를 이용한 소자 개발이 가긍해짐에 따라 국내외에서 활발한 연구가 이루어지고 있다. 본 연구실에서는 GaN-단일전구체를 이용하여 상온에서 자기적 특성을 나타내는 p-type GaMnN를 성장시켰다 극한 환경에서의 자성반도체 재료의 물성 변화를 알아보기 위해, 본 연구에서는 세계 최초로 중성자 빔의 조사에 따른 자성반도체의 구조적, 자기적 특성 및 열처리에 따른 특성 변화를 관찰 및 분석하였다. Molecular beam epitaxy(MBE)를 이용하여 Mn cell 온도가 각각 77$0^{\circ}C$, 94$0^{\circ}C$인 GaMnN 박막을 성장시켰다. 성장된 박막 시편에 한국원자력연구소 하나로 HTS공에서 중성자 빔을 각각 20min(4.17$\times$$10^{16}$n/$\textrm{cm}^2$), 24hour(3.0$\times$$10^{18}$n/$\textrm{cm}^2$)씩 조사하였다 중성자 빔을 조사한 시편은 진공분위기 하에서 100$0^{\circ}C$, 30초간 열처리하였다.(rapid thermal annealing;RTA, 승온속도: 8$^{\circ}C$/sec) 중성자 빔을 조사한 GaMnN 박막의 구조적인 특성은 X-ray diffraction(XRD) 측정을 통해 관찰하였고, 박막의 자기적 특성은 superconducting quantum interference device(SQUID)를 통해 측정하였다.

• Journal of Powder Materials
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• v.10 no.2
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• pp.83-88
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• 2003

Nanocrystalline materials of Ni and Ni-Cu alloy have been synthesized by the pulsed wire evaporation (PWE) method and these abnormal magnetic properties in the magnetic ordered state have been characterized using both VSM and SQUID in the range of high and low magnetic fields. Ni and Ni-Cu particles with an average size of 20 to 80 nm were found to influence magnetic hysterisis behavior and the results of powder neutron diffraction patterns and saturation magnetization curves are shown to indicate the absence of the NiO phase. The shifted hysterisis loop and irreversibility of the magnetization curve in the high field region were observed in the magnetic-ordered state of both Ni and Ni-Cu. The virgin magnetization curve for Ni slightly spillover on the limited hysterisis loop ($\pm$20kOe). This irreversibility in the high field of 50 kOe can be explained by non-col-linear behavior and the existence of the metastable states of the magnetization at the surface layer (or core) of the particle in the applied magnetic field. Immiscible alloy of Cu-Ni was also found to show irreversibility having two different magnetic phases.

• Journal of the Korean Chemical Society
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• v.23 no.4
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• pp.206-209
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• 1979

Empirical force-field calculations have been applied to eight 1,6-anhydropyra-noses, the crystal structures$^{13{\sim}21}$ of which have been studied by single crystal X-ray or neutron diffraction analysis. The theoretical calculations reproduce closely the variations in conformation between $^1C_4$ and $E_0$, which are observed in the pyranose rings. The smaller conformational differences in the five-membered anhydro ring are not so well predicted. The calculated C-C bond lengths agree with those observed within 0.012${\AA}$ with one exception. The C-O bond lengths show a larger deviation, 0.027${\AA}$. The non-hydrogen atom valence angles agree within 1.9$^{\circ}$.