• Title/Summary/Keyword: Pinning center

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The Effect of Domain Wall on Defect Energetics in Ferroelectric LiNbO3 from Density Functional Theory Calculations

  • Lee, Donghwa
    • Journal of the Korean Ceramic Society
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    • v.53 no.3
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    • pp.312-316
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    • 2016
  • The energetics of defects in the presence of domain walls in $LiNbO_3$ are characterized using density-functional theory calculations. Domain walls show stronger interactions with antisite defects than with interstitial defects or vacancies. As a result, antisite defects act as a strong pinning center for the domain wall in $LiNbO_3$. Analysis of migration behavior of the antisite defects across the domain wall shows that the migration barrier of the antisite defects is significantly high, such that the migration of antisite defects across the domain wall is energetically not preferable. However, further study on excess electrons shows that the migration barrier of antisite defects can be lowered by changing the charge states of the antisite defects. So, excess electrons can enhance the migration of antisite defects and thus facilitate domain wall movement by weakening the pinning effect.

Electromagnetic Characteristics of Ceramics Superconductor (초전도체의 전기자기적 특성)

  • Lee, Sang-Heon;Lee, Sung-gap;Kim, Young-Kuk;Yoo, Jae-Mu;Lee, Young-Hie
    • Proceedings of the KIEE Conference
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    • 2004.11a
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    • pp.203-204
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    • 2004
  • Suspension effect has been studied by using superconductor of BiPbSrCaCuO ceramics containing $Ag_2O$. It has been cleared that $Ag_2O$ acts as pinning center which plays an important role to the suspension effect. Magnetic repulsive force which affects a superconductor located in magnetic flux from toroidal magnet has been investigated. It has been concluded that the suspension effect arises from the interaction between the pinning effect and the diamagnetic effect.

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Single Crystalline CoFe/MgO Tunnel Contact on Nondegenerate Ge with a Proper Resistance-Area Product for Efficient Spin Injection and Detection

  • Jeon, Kun-Rok;Min, Byoung-Chul;Lee, Hun-Sung;Shin, Il-Jae;Park, Chang-Yup;Shin, Sung-Chul
    • Proceedings of the Korean Magnestics Society Conference
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    • 2010.06a
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    • pp.96-96
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    • 2010
  • We report the proper resistance-area products in the single crystalline bcc CoFe/MgO tunnel contact on nondegenerate n-Ge desirable for efficient spin injection and detection at room temperature. The electric properties of the crystalline CoFe(5 nm)/MgO(1.5,2.0,2.5 nm)/n-Ge(001) tunnel contacts have been investigated by I-V-T and C-V measurements. Interestingly, the tunnel contact with the 2-nm MgO exhibits the ohmic behavior with low resistance-area products, satisfying the theoretical conditions required for significant spin injection and detection. This result is ascribed to the presence of MgO layer between CoFe and n-Ge, enhancing the Schottky pinning parameter as well as shifting the charge neutrality level.

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Numerical Formula of Depinning Fields from Notches in Ferromagnetic Permalloy Nanowire

  • Kim, Kab-Jin;You, Chun-Yeol;Choe, Sug-Bong
    • Journal of Magnetics
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    • v.13 no.4
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    • pp.136-139
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    • 2008
  • A simplified equation of depinning fields from notches of ferromagnetic Permalloy nanowires is presented. The derived equation is given in the form of an explicit function of nanowire width and thickness, and notch depth and angle. The equation agrees with all micromagnetic simulation results to an accuracy of ${\pm}$ 0.5 mT.

Domination of glassy and fluctuation behavior over thermal activation in vortex state in $MgB_2$ thin film ($MgB_2$ 박막에서의 열적 활성화에 비해 두드러진 볼텍스 유리화 및 열적 요동현상의 연구)

  • Kim, Heon-Jung;W. N. Kang;Kim, Hyeong-Jin;Park, Eun-Mi;Kim, Kijoon H. P.
    • Progress in Superconductivity
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    • v.3 no.1
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    • pp.23-27
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    • 2001
  • We have investigated the mixed-state magnetoresistance of high quality c-axis-oriented MgB2 thin film for magnetic field from 0.5 T to 5.0 T, applied normal to ab-plane. The temperature dependence of magnetoresistance was well described by vortex glass and fluctuation theories for different temperature regimes. We observed glassy exponent of v(z-1)~3 and upper critical field of $H_{c2}$(0)~35 T, which is consistent with previous data obtained from direct $H_{c2}$(0) measurements. Interestingly, the thermally activated flux flow region was observed to be very narrow, suggesting that the pinning strength of this compound is very strong. This finding is closely related to the recent reports that the bulk pinning is dominant in $MgB_2$and the critical current density of $MgB_2$ thin film is very high, comparable to that of cuprate superconductor. The present results further suggest that $MgB_2$is beneficial to technical applications.ons.

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Microstructure Analysis of Y-Ba-Cu-O thin Films Grown on STO Substrates with Controlled ZnO Nanorods (ZnO 나노막대가 형성된 STO기판에 증착한 Y-Ba-Cu-O 박막의 미세구조 분석)

  • Oh, S.K.;Jang, G.E.;Tran, H.D.;Kang, B.W.;Kim, K.W.;Lee, C.Y.;Hyun, O.B.
    • Progress in Superconductivity
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    • v.11 no.1
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    • pp.47-51
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    • 2009
  • For many large-scale applications of high-temperature superconducting materials, large critical current density ($J_c$) in high applied magnetic fields are required. A number of methods have been reported to introduce artificial pinning centers in $YBa_2Cu_3O_{7-{\delta}}$ films for enhancement of their $J_c$. We studied the microstructures and characteristic of $YBa_2Cu_3O_{7-{\delta}}$ films fabricated on $SrTiO_3$ (100) substrates with ZnO nanorods as pinning centers. Au catalyst nanoparticles were synthesized on STO substrates with self assembled monolayer to control the number of ZnO nanorods. The density of Au nanoparticles is approximately $240{\sim}260{\mu}m^{-2}$ with diameters of $41{\sim}49nm$. ZnO nanorods were grown on STO by hot-walled PLD with Au nanoparticles. Typical size of ZnO nanorod was around 179 nm in diameter and $2{\sim}6{\mu}m$ in length respectively. YBCO films deposited directly on STO substrates show the c-axis orientation, while YBCO films with ZnO nanorods exhibit any mixed phases without any typical crystal orientation.

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Sputering Pressure and Temperature Effects on Magnetization Reversal Behaviors of $Co(2\AA)/Pd(13\AA)$ Multilayers (스퍼터링압력 및 온도 효과에 의한 $Co(2\AA)/Pd(13\AA)$ 다층박막의 자화반전 거동)

  • 김성봉;정순영
    • Journal of the Korean Magnetics Society
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    • v.6 no.4
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    • pp.199-203
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    • 1996
  • To study the magnetization reversal behavior of Co/Pd multilayers, we first demagnetized the samples by the field-demagnetized method and then measured initial curves and minor loops. The coercivity and the perpendicular magnetic anisotropy were obtained from the perpendicular and parallel magnetization curves measured at different temperatures. We interpret our experimental results by applying several qualitative and semiquantative approaches. From these study, we found that the magnetization reversal behavior is dominated by the domain wall pinning for all samples and the coercivity incremental tendency can be explained by Kronmuller's formula $H_c(T)\;{\propto}\;r_0.K_u$.

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Ceramics superconducting Energy Materials (세라믹 에너지 재료)

  • Lee, Sang-Heon
    • Proceedings of the KIEE Conference
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    • 2008.07a
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    • pp.1238-1239
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    • 2008
  • The high Tc supeconductor of ceramic oxides type was studied for finding its application field. The results reportaed in this paper on the stability of the ceramic superconductors and the resistance to ripening in the BCO liquid phase at elevated temperature opens a processing window for engineering the microstructure of large superconductor at the nanoscale level. The results suggest further that the introduction of highly efficient artifical pinning center to bulk ceramics superconductor.

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Magnetic Suspension Effect of BiPbSrCaCuO Superconductor (Bi계 초전도체의 자기부양효과)

  • 이상헌;이창용
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2000.11a
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    • pp.500-502
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    • 2000
  • BiPbSrCaCuO 계 초전도체에서 관측되는 자기부양효과에 대하여 연구를 수행하였다. BiPbSrCaCuO 계 초전도체에 산화은을 첨가한 시료와 첨가하지 않은 시료의 자기적 특성을 측정하여 자기부양효과의 메카니즘에 대하여 고찰하였다. toroidal자석에서 관측되는 자기부양 효과는 자석의 중심부분에서만 발생하며, 자석의 ring 부분에서는 관측되지 않았다. 이 결과는 본 연구의 자기 부양효과의 발생에는 자석의 형상 및 자속의 분포 형태와 밀접한 관련이 있음을 의미한다.

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