• 한국초전도ㆍ저온공학회논문지
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• 제15권3호
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• pp.5-8
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• 2013

We have studied Hall effect for potassium (K)-doped $BaFe_2As_2$ superconducting thin films by analyzing the relation between the longitudinal resistivity (${\rho}_{xx}$) and the Hall resistivity (${\rho}_{xy}$). The thin films used in this study were fabricated on $Al_2O_3$ (000l) substrates by using an ex-situ pulsed laser deposition (PLD) technique under a high-vacuum condition of ~$10^{-6}$ Torr. The samples showed the high superconducting transition temperatures ($T_c$) of ~ 40 K. The ${\rho}_{xx}$ and the ${\rho}_{xy}$ for K-doped $BaFe_2As_2$ thin films were measured by using a physical property measurement system (PPMS) with a temperature sweep (T-sweep) mode at an applied current density of $100A/cm^2$ and at magnetic fields from 0 up to 9 T. We report the T-sweep results of the ${\rho}_{xx}$and the ${\rho}_{xy}$ to investigate Hall scaling behavior on the basis of the relation of ${\rho}_{xy}={A{\rho}_{xx}}^{\beta}$. The ${\beta}$ values are $3.0{\pm}0.2$ in the c-axis-oriented K-doped $BaFe_2As_2$ thin films, whereas the thin films with various oriented-directions like a polycrystal showed slightly lower ${\beta}$ than that of c-axis-oriented thin films. Interestingly, the ${\beta}$ value is decreased with increasing magnetic fields.

• 한국초전도ㆍ저온공학회논문지
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• 제16권3호
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• pp.4-6
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• 2014

Among Fe-based superconductors, potassium doped $BaFe_2As_2$ is favorable for applications because of its relatively high transition temperature and low anisotropy. To study the superconducting properties and the applicable aspects, high quality thin films of potassium doped $BaFe_2As_2$ should be fabricate. However, the high volatility of potassium makes it difficult to fabricate thin films of this compound. In this paper, we discuss the details of the experimental conditions used to fabricate $Ba_{1-x}K_xFe_2As_2$ films by ex situ PLD method. In the first set of samples, barium ratio in the target was controlled to make films with various potassium doping rate. However, in the second set of samples, the amount of potassium was controlled to find out optimal conditions for making high quality $Ba_{1-x}K_xFe_2As_2$ films.

• Progress in Superconductivity
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• 제12권2호
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• pp.99-103
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• 2011

We performed angle resolved photoelectron spectroscopy (ARPES) studies on Ru doped $BaFe_2As_2$ with various Ru contents. Ru, which is doped into a parent compound $BaFe_2As_2$ and substitute Fe, does not donate or accept electrons. However, it induces superconductivity. From ARPES data along the high symmetry cuts and Fermi surface maps, we investigate the electron correlation and carrier density at the Fermi level. We observe that the Fermi velocity increases with Ru doping, suggesting reduction in electron correlation. In addition, we address issues on local vs. itinerant pictures for the magnetism in $BaFe_2As_2$.

• 한국초전도ㆍ저온공학회논문지
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• 제16권4호
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• pp.31-35
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• 2014

The upper critical field ($H_{c2}$) was determined by applying a magnetic field along the ab plane and c axis for two single crystals of $BaFe_{2-x}Ru_xAs_2$ (x=0.48 and 0.75). The anisotropy of the $H_{c2}(0)$, ${\gamma}(0)=H_{c2}{^{ab}}(0)/H_{c2}{^c}(0)$, was ~1.6 for x=0.48 and ~2.3 for x=0.75. The angle-dependent resistance measured below $T_c$ allowed perfect scaling features based on anisotropic Ginzburg-Landau theory, leading to consistent anisotropy values. Because only one fitting parameter ${\gamma}$ is used in the scaling for each temperature, the validity of the ${\gamma}$ value was compared with that determined from ${\gamma}=H_{c2}{^{ab}}/H_{c2}{^c}$. The ${\gamma}$ obtained at a temperature close to $T_c$ was 3.0 and decreased to 2.0 at low temperatures. Comparing to the anisotropy determined for electron- or hole-doped $BaFe_2As_2$ using the same method, the present results point to consistent anisotropy in Ru-doped $BaFe_2As_2$ with other electron- or hole-doped $BaFe_2As_2$.

• 한국초전도ㆍ저온공학회논문지
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• 제17권4호
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• pp.30-33
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• 2015

We report the synthesis of Ni-doped $BaFe_2Se_3$ single crystals by using a flux method. X-ray diffraction (XRD) of $Ba(Fe_{1-x}Ni_x)_2Se_3$ shows a gradual peak shift with an increase in the nominal Ni-doping rate, x = 0, 0.05, and 0.10, due to a decrease in unit-cell volume. All samples show a spin glass transition, and temperature dependence of magnetic susceptibility shows a negligible change in the spin-glass transition temperature ($T_g$) with Ni concentration x. The temperature dependence of electrical resistivity for $BaFe_2Se_3$ shows an insulating behavior, and the resistivity value at 295 K and the activation energy ($E_a$) obtained from the Arrhenius plot decrease with increasing x. These results suggest that the Ni doping can be effectively worked as a dopant for electron charge carriers, but is less efficient in controlling the magnetic property, such as spin glass transition, in the $BaFe_2Se_3$ compound.

• Progress in Superconductivity
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• 제12권1호
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• pp.32-35
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• 2010

Potassium doped $BaFe_2As_2$ superconducting thin films by using an ex situ pulsed laser deposition technique were fabricated in various conditions to find out an optimal growth condition. Controlled conditions were annealing temperature, annealing time, and mass of potassium. The $Ba_{1-x}K_xFe_2As_2$ thin films which has most good quality is fabricated at a condition of annealing temperature at $700^{\circ}C$, annealing time of 60 minutes, and 0.6 g of potassium lumps. In this condition we were able to fabricate good quality films with high transition temperature of ~ 39 K.

• Journal of Magnetics
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• 제21권1호
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• pp.61-64
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• 2016

In this study, we report the as-prepared MgO-doped $BaFe_{12}O_{19}$, which was prepared by calcination technique and high-energy ball milling process, as an electromagnetic wave absorber. The phase analysis of $BaFe_{12}O_{19}$ and the as-prepared MgO-doped $BaFe_{12}O_{19}$ was detected utilizing X-ray Diffractometer (XRD). The microstructure was characterized using Scanning Electron Microscope (SEM). By means of the transmission/reflection coaxial line method, the electromagnetic properties and microwave absorbing properties of the as-prepared electromagnetic wave absorber were studied. It is found that the electromagnetic wave absorber has a minimum reflection loss value of -41 dB at 4.27 GHz with a matching thickness of 2.6 mm. The experiment results revealed that the as-prepared electromagnetic wave absorber could find potential applications in many military as well as commercial industries.

• 한국초전도ㆍ저온공학회논문지
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• 제15권2호
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• pp.16-19
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• 2013

The magneto-resistivity and electric field-current density (E-J) curves were investigated up to a magnetic field 9 T in the optimally doped $BaFe_{1.8}Co_{0.2}As_2$ single crystal with a superconducting temperature ($T_c$) of 24.6 K. The E-J Scaling behaviors below and above vortex glass transition temperature ($T_g$) were found, confirming the existence of the vortex glass phase transition. The critical exponents for the diverging spatial and time correlations at $T_g$, were obtained as v = $1.1{\pm}0.1$ and z = $4.5{\pm}0.3$, respectively. The obtained critical exponents are in good agreement with the predicted values of v ~ 1 - 2 and z > 4 within the 3D vortex glass theory.

• 멤브레인
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• 제21권1호
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• pp.55-61
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• 2011

고상반응법을 이용하여 $BaCo_{0.7}Fe_{0.22}Nb_{0.08}O_{3-{\delta}}$ (BCFN) 조성의 산화물을 합성하였으며, 합성된 분말은 압축 성형 후 $1,200^{\circ}C$에서 소결하여 치밀한 세라믹 분리막을 제조하였다. 제조된 $BaCo_{0.7}Fe_{0.22}Nb_{0.08}O_{3-{\delta}}$ 분리막의 XRD 분석결과 단일상의 페롭스카이트 구조를 보였다. 밀봉재료로 glass ring을 사용하여 가스누출 실험 및 산소투과 분석을 하였으며, 산소투과 분석 결과 온도와 산소분압($Po_2$)이 증가할수록 산소투과량은 증가하였고, $Po_2$ = 0.63 atm의 경우 $950^{\circ}C$에서 $2.3mL/min{\cdot}cm^2$의 값을 나타내었다. 또한, 이산화탄소 300 ppm이 포함된 혼합공기를 사용할 경우 모사공기($Po_2$ = 0.21 atm)를 사용한 경우에 비해 산소투과량이 최대 2.9%만 감소하였다. 이는 $BaCo_{0.7}Fe_{0.22}Nb_{0.08}O_{3-{\delta}}$ 분리막이 다른 분리막에 비해 이산화탄소에 대해 안정하다는 것을 의미한다.

• 한국자기학회지
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• 제10권4호
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• pp.154-158
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• 2000

Ba-페라이트 BaF $e_{12}$ $O_{19}$에서 Fe 이온의 미량을 Co와 Ti 이온으로 치환시킨 시료인 BaF $e_{12-2x}$ $Co_{x}$ $Ti_{x}$ $O_{19}$(0.0$\leq$x$\leq$1.0)을 제조하여 Co와 Ti이온의 치환에 따른 결정학적 및 자기적 특성의 변화를 밝히기 위하여 x-선 회절기, Mossbauer분광기, 진동자력계 등을 이용한 연구를 하였다. 모든 조성비 범위에서 결정 구조는 magnetoplumbite 구조임을 알 수 있었으며, Co-Ti의 치환량이 증가함에 따라 격자상수 a는 거의 일정하였고 c는 증가하였다. BaF $e_{12-2x}$ $Co_{x}$ $Ti_{x}$ $O_{19}$ 시료에서 치환량이 증가함에 따라 포화자화 값은 약 60 emu/g 정도로 거의 변하지 않으나, 보자력은 x = 0.0과 0.2사이에서 매우 급격히 2297 kOe에서 220 kOe로 지수함수적으로 감소하고 그 이상의 조성비에서는 서서히 선형적으로 감소함을 알아냈다. 상온에서 Mossbauer spectra 분석 결과 Co-Ti은 l2k, 4 $f_{vi}$ 와 2b 자리를 선호함을 알 수 있었다. 또 Co-Ti리 치환량이 증가함에 따라 R 블럭의 c축 크기는 작아지고, 반대로 5 블럭의 c축 크기는 커짐을 알아냈다. 알아냈다.