• Title/Summary/Keyword: Fe based superconductor

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Electronic and Magnetic Structures of {Ca,Sr,Ba}$Fe_2As_2$ : Dynamical Mean Field Theory Approach ({Ca,Sr,Ba}$Fe_2As_2$의 전자 및 자성 구조: 동력학적 평균장 이론 접근)

  • Lee, Geun-Sik;Shim, Ji-Hoon
    • Progress in Superconductivity
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    • v.13 no.2
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    • pp.85-89
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    • 2011
  • Using the density functional theory and its combination to the dynamical mean field theory (DMFT), we have studied the electronic and magnetic structures of Fe-based superconductors, $AFe_2As_2$ (A=Ca, Sr, Ba). Our results for the electronic structure agree well with existing angle resolved photoemission spectroscopy (ARPES) data. The temperature dependent magnetization has been calculated using DMFT, and the magnetic transition temperatures are reasonably consistent with the experimentally observed trend for three compounds.

Growth of $FeSe_x$ Superconducting Thin Films at Various Temperatures by PLD Technique (PLD법을 이용한 다양한 온도에서의 $FeSe_x$ 초전도 박막 성장)

  • Jung, Soon-Gil;Lee, N.H.;Kang, W.N.;Hwang, Tae-Jong;Kim, D.H.
    • Progress in Superconductivity
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    • v.13 no.2
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    • pp.117-121
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    • 2011
  • We have fabricated $FeSe_x$ superconducting thin films at much different substrate temperatures of 430 and $610^{\circ}C$ on $Al_2O_3$(0001) substrates by using a pulsed laser deposition (PLD) technique. Superconducting transitions for both films were shown around 10 K, but their transition width and growth directions of grains were different. We found that superconducting tetragonal FeSe phases and non-superconducting hexagonal FeSe phases were coexisted in the sample grown at the low temperature of $430^{\circ}C$, whereas the hexagonal FeSe phase was decreased with increasing fabrication temperatures.

Existence of a vortex-glass phase transition in an optimally doped BaFe1.8Co0.2As2 single crystal

  • Choi, Ki-Young;Kim, Kee Hoon
    • Progress in Superconductivity and Cryogenics
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    • v.15 no.2
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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.

Upper critical field and superconducting anisotropy of BaFe2-xRuxAs2 (x=0.48 and 0.75) single crystals

  • Jo, Youn Jung;Eom, Man Jin;Kim, Jun Sung;Kang, W.
    • Progress in Superconductivity and Cryogenics
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    • v.16 no.4
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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 $BaFe_2As_2$.

Synthesis of the Ni-doped ternary compound Ba(Fe1-xNix)2Se3

  • Park, Hyeon Beom;Shin, Soohyeon;Jung, Soon-Gil;Hwang, Doyeon;Lee, Hyoyoung;Park, Tuson
    • Progress in Superconductivity and Cryogenics
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    • v.17 no.4
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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.

High-Pressure Synthesis of $SmFeAsO_{1-x}F_x$(x=0.2) Single Crystals ($SmFeAsO_{1-x}F_x$(x=0.2)의 고압 단결정 합성)

  • Lee, Hyun-Sook;Park, Jae-Hyun;Lee, Jae-Yeap;Kim, Ju-Young;Cho, B.K.;Jung, Chang-Uk;Lee, Hu-Jong
    • Progress in Superconductivity
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    • v.10 no.2
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    • pp.87-91
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    • 2009
  • Fluorine-doped $SmFeAsO_{1-x}F_x$ single crystals with the nominal value of x=0.2 were grown at $1350-1450^{\circ}C$ under the pressure of 3.3 GPa by using the self-flux method. Plate-shaped single crystals in the range of a few-150 ${\mu}m$ in their lateral size were obtained. The detailed crystal structure was analyzed by using the x-ray diffractometry. Superconducting transition temperature, determined by the resistive transition, of a single crystal was about 49 K with a narrow resistive transition width of ${\sim}1$ K. A relatively sharp transition, a low residual resistivity, and a large residual resistivity ratio compared with those reported for $REFeAsO_{1-x}F_x$(RE=Sm, Nd) single crystals indicate the high quality of our single crystals.

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