• 제목/요약/키워드: manganites

검색결과 40건 처리시간 0.029초

Local structure and transport properties of $La_{0.7}Ca_{0.3-x}Ba_{x}MnO_3$ manganites

  • A.N.Ulyanov;Yang, Dong-Seok;Yu, Seong-Cho
    • 한국자기학회:학술대회 개요집
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    • 한국자기학회 2003년도 하계학술연구발표회 및 한.일 공동심포지엄
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    • pp.62-63
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    • 2003
  • Electron-phonon interaction plays a significant role in forming of colossal magnetoresistance effect (CMR). Polaron formation was observed by neutron diffraction and by extended X-ray absorption fine structure (EXAFS) analysis. Local probe as given by the EXAFS is a useful method to study the polaronic charge and its dependence on temperature and ions size. Here we present the EXAFS study of polaronic charge in $La_{0.7}Ca_{0.3-x}Ba_{x}MnO_3$ compositions.

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Strain induced magnetic stripe domains in $La_{0.7}Sr_{0.3}MnO_3$ thin films

  • Joonghoe Dho;Kim, Y. N.;Y. S. Hwang;E. O. Chi;Kim, J. C.;Lee, E. K.;N. H. Hur
    • 한국자기학회:학술대회 개요집
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    • 한국자기학회 2002년도 동계연구발표회 논문개요집
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    • pp.84-85
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    • 2002
  • Recently doped perovskite manganites have renewed interest because they exhibit a variety of unique magnetic and electronic behaviors such as colossal magnetoresistance (CMR), percolative phase separation, spin/charge/orbital ordering, and so on. For this reason, fabrication of thin films with the best surface morphology and controlling their magneto transport properties is essential for making magneto-resistive devices. (omitted)

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Impact of Ba Substitution on the Magnetocaloric Effect in La1-xBaxMnO3 Manganites

  • Hussain, Imad;Anwar, M.S.;Kim, Eunji;Koo, Bon Heun;Lee, Chan Gyu
    • 한국재료학회지
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    • 제26권11호
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    • pp.623-627
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    • 2016
  • $La_{1-x}Ba_xMnO_3$ (x = 0.30, 0.35 and 0.40) samples have been prepared by solid-state reaction method. The X-ray diffraction (XRD) study showed that all the samples crystallized in a rhombohedral structure with an R-3c space group. Variation of the magnetization as a function of the temperature and applied magnetic field was carried out. All the samples revealed ferromagnetic to paramagnetic (FM-PM) phase transition at the Curie temperature $T_C{\sim}342K$. The magnetic entropy change was also studied through examination of the measured magnetic isotherms M(H, T) near $T_C$. The magnetocaloric effect was calculated in terms of the isothermal magnetic entropy change. The maximum entropy change reaches a value of 1.192 J/kgK under a magnetic field change of 2.5T for the $La_{0.6}Ba_{0.4}MnO_3$ composition. The relative cooling power (RCP) is 79.31 J/kg for the same applied magnetic field.

망간산화물 $La_{0.7}Ca_{0.3}MnO_3$의 거대 자기 엔트로피 효과 (Large Magnetic Entropy Change in Single Crystalline and Ploystalline $La_{0.7}Ca_{0.3}MnO_3$)

  • 신현수;주홍렬
    • 한국자기학회지
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    • 제10권4호
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    • pp.149-153
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    • 2000
  • 변하는 자기장을 단결정 및 다결정 망간 산화물 La$_{0.7}$Ca$_{0.3}$MnO$_3$에 인가하였을 때 자기 엔트로피가 크게 변하는(거대 자기 엔트로피 변화)현상이 관측되었다. 이 거대 자기 엔트로피 변화는 Curie온도에서 유사 1차상전이에 의한 자화값의 급격한 변화에 의한 것으로 추측된다. 이 거대 자기 엔트로피 변화와 망간 산화물 Curie 온도의 100 K<T<400 K 내의 조절 용이성은 상온을 포함한 넓은 온도에서 망간 산화물을 이용한 자기 냉각 기관의 개발 가능성을 제시하고 있다. 있다.

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Bi 첨가 란탄 망가나이트의 제조, 자기 및 자기저항 특성 (Fabrication, Magnetic and Magnetoresistive Properties of Bi-Doped Lanthanum Manganites)

  • 김덕실;조재경
    • 한국자기학회지
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    • 제9권5호
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    • pp.239-244
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    • 1999
  • 란탄 망가나이트에 Bi를 첨가한 벌크 시료(La0.67xBixCa0.33MnO3(x=0, 0.04, 0.1, 0.2)들을 세라믹스 제조공정을 이용하여 제조했다. 제조한 시료들의 결정성과 미세구조를 x-선 회절분석과 광현미경으로 조사하고, 자기 및 자기저항 특성을 100~300K의 온도 범위에서 0.4~0.5T의 자기장을 인가하여 진동시료형자력계와 van der Pauw법으로 조사했다. Bi를 소량(x=0.04, 0.1) 첨가한 시료의 경우 시료를 제조할 수 있었다. 또한 Bi를 소량 첨가하는 것에 의해 측정한 대부분의 온도에서 비저항이 감소하였고 자기저항비가 증가하였다. 아울러 실온에서 약한 자기장(0.4T)하에서도 큰 자기저항비(x=0.1의 경우 15%)를 나타냈다.

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X-ray Absorption and Photoemission Spectroscopy Study of Nd1/2A1/2Mn1-yCryO3(A=Ca, Sr)

  • Kang, J.S.;Kim, J.H.;Han, S.W.;Kim, K.H.;Choi, E.J.;Sekiyama, A.;Kasai, S.;Suga, S.;Kimura, T.
    • Journal of Magnetics
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    • 제8권4호
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    • pp.142-145
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    • 2003
  • Valence states and electronic structures of Cr-doped $Nd_{1/2}A_{1/2}Mn_{1-y}Cr_{y}O_3$(NAMO; A=Ca, Sr) manganites have been investigated using x-ray absorption spectroscopy (XAS) and high-resolution photoemission spectroscopy (PES). All the Cr-doped NAMO systems exhibit the clear metallic Fermi edges in the Mn $e_{g}$ PES spectra near $E_{F}$. The spectral intensity at $E_{F}$ is higher for Cr-doped N $d_{l}$ 2/S $r_{l}$ 2/Mn $O_3$(NSMO) than for Cr-doped N $d_{l}$ 2/C $a_{l}$ 2/Mn $O_3$ (NCMO), reflecting the stronger metallic nature for NSMO than for NCMO. The measured Cr 2p XAS spectra are found to be very similar to that of C $r_2$ $O_3$, indicating that Cr ions in Cr-doped NAMO are in the trivalent C states ( $t^3$$_{2g}$). The Cr 2p XAS data are consistent with the Cr 3d PES spectra located at ∼1.3 eV below $E_{F}$ and having no emission near $E_{F}$.

Electrical Transport and Magnetoresistance of La0.67Ca0.33MnO3: Agx (x = 0, 0.1, 0.2, 0.3, 0.4) Composites

  • Gencer, H.;Pektas, M.;Babur, Y.;Kolat, V.S.;Izgi, T.;Atalay, S.
    • Journal of Magnetics
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    • 제17권3호
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    • pp.176-184
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    • 2012
  • The structural, magnetic and magnetotransport properties of $La_{0.67}Ca_{0.33}MnO_3$: $Ag_x$ (x = 0, 0.1, 0.2, 0.3 and 0.4) composites were investigated systematically. X-ray and EDX analysis indicated that Ag is not substituted into the main $La_{0.67}Ca_{0.33}MnO_3$ phase and remains an additive to the second phase at the grain boundary. The Curie temperature first decreased from 269 K for x = 0 to 257 K for x = 0.1 and then remained nearly unchanged with increasing Ag content. For the x > 0.1 samples, a second transition temperature ($T_{MI2}$) was observed in the resistance curves. At temperatures below 150 K, a significant enhancement in MR was observed while high temperature MR decreased with increasing Ag content. The maximum MR was observed to be 55% in the x = 0.4 sample at 10 K and a 6T magnetic field, this value is larger than that of pure $La_{0.67}Ca_{0.33}MnO_3$ (53% at 265 K and 6 T). In addition, at low fields (H < 1T), a sharp increase in the MR was observed.

Magnetic properties and magnetocaloric effect of Sr-doped Pr0.7Ca0.3MnO3 compounds

  • Yen, Pham Duc Huyen;Dung, Nguyen Thi;Thanh, Tran Dang;Yu, Seong-Cho
    • Current Applied Physics
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    • 제18권11호
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    • pp.1280-1288
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    • 2018
  • In this work, we pointed out that Sr substitution for Ca leads to modify the magnetic and magnetocaloric properties of $Pr_{0.7}Ca_{0.3-x}Sr_xMnO_3$ compounds. Analyzing temperature dependence of magnetization, M(T), proves that the Curie temperature ($T_C$) increased with increasing Sr content (x); $T_C$ value is found to be 130-260 K for x = 0.0-0.3, respectively. Using the phenomenological model and M(T,H) data measured at several applied magnetic field, the magnetocaloric effect of $Pr_{0.7}Ca_{0.3-x}Sr_xMnO_3$ compounds has been investigated through their temperature and magnetic field dependences of magnetic entropy change ${\Delta}S_m$(T,H) and the change of the specific heat change ${\Delta}C_P$(T,H). Under an applied magnetic field change of 10 kOe, the maximum value of $-{\Delta}S_m$ is found to be about $3J/kg{\cdot}K$, and the maximum and minimum values of ${\Delta}C_P$(T) calculated to be about ${\pm}60J/kg{\cdot}K$ for x = 0.3 sample. Additionally, the critical behaviors of $Pr_{0.7}Ca_{0.3-x}Sr_xMnO_3$ compounds around their $T_C$ have been also analyzed. Results suggested a coexistence of the ferromagnetic short- and long-range interactions in samples. Moreover, Sr-doping favors establishing the short-range interactions.

Electrical and Magnetic Properties in [La0.7(Ca1-xSrx)0.3MnO3)]0.99/(BaTiO3)0.01 Composites

  • Kim, Geun-Woo;Bian, Jin-Long;Seo, Yong-Jun;Koo, Bon-Heun
    • 한국재료학회지
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    • 제21권4호
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    • pp.216-219
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    • 2011
  • Perovskite manganites such as $RE_{1-x}A_xMnO_3$ (RE = rare earth, A = Ca, Sr, Ba) have been the subject of intense research in the last few years, ever since the discovery that these systems demonstrate colossal magnetoresistance (CMR). The CMR is usually explained with the double-exchange (DE) mechanism, and CMR materials have potential applications for magnetic switching, recording devices, and more. However, the intrinsic CMR effect is usually found under the conditions of a magnetic field of several Teslas and a narrow temperature range near the Curie temperature ($T_c$). This magnetic field and temperature range make practical applications impossible. Recently, another type of MR, called the low-field magnetoresistance(LFMR), has also been a research focus. This MR is typically found in polycrystalline half-metallic ferromagnets, and is associated with the spin-dependent charge transport across grain boundaries. Composites with compositions $La_{0.7}(Ca_{1-x}Sr_x)_{0.3}MnO_3)]_{0.99}/(BaTiO_3)_{0.01}$ $[(LCSMO)_{0.99}/(BTO)_{0.01}]$were prepared with different Sr doping levels x by a standard ceramic technique, and their electrical transport and magnetoresistance (MR) properties were investigated. The structure and morphology of the composites were studied by X-ray diffraction (XRD) and scanning electronic microscopy (SEM). BTO peaks could not be found in the XRD pattern because the amount of BTO in the composites was too small. As the content of x decreased, the crystal structure changed from orthorhombic to rhombohedral. This change can be explained by the fact that the crystal structure of pure LCMO is orthorhombic and the crystal structure of pure LSMO is rhombohedral. The SEM results indicate that LCSMO and BTO coexist in the composites and BTO mostly segregates at the grain boundaries of LCSMO, which are in accordance with the results of the magnetic measurements. The resistivity of all the composites was measured in the range of 90-400K at 0T, 0.5T magnetic field. The result indicates that the MR of the composites increases systematically as the Ca concentration increases, although the transition temperature $T_c$ shifts to a lower range.

Cu가 도핑된 LSM의 구조분석과 열팽창특성 연구 (Structural analysis and thermal expansion property of Cu doped LSM for SOFCs)

  • 노태민;류지승;김진성;정철원;이희수
    • 한국결정성장학회지
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    • 제21권4호
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    • pp.175-180
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    • 2011
  • 이종 원자가를 가시는 Cu의 도핑이 LSM에 미치는 영향을 구조적인 분석과 열팽창계수를 통해서 고찰하였다. 고상반응을 이용하여 $La_{0.8}Sr_{0.2}Mn_{1-x}Cu_xO_3$($0{\leq}x{\leq}0.3$)음 제조하였으며, Cu의 도핑 함량에 따른 결정구조 및 열팽창계수를 확인하였다. Cu 함량이 증가함에 따라서 격자상수외 열팽창계수가 감소하는 경향을 나타냈지만, x = 0.3인 경우에는 증가 하였다. 이러한 격자상수와 열팽창계수의 변화는 Cu 이온의 B-site에서의 Mn 자리에 치환될 때 $0{\leq}x{\leq}0.2$의 범위에서는 $Cu^{3+}$의 존재로 인한 이온 반성의 감소에 의한 것으로 판단되었고, x=0.3인 경우에는 $Cu^{2+}$$Mn^{4+}$의 존재로 인한 산소 공공의 증가에 기인한 것이었다.