• 제목/요약/키워드: weak ferromagnetic

검색결과 34건 처리시간 0.024초

Formation of Au Particles in Cu2-xICu2IIO3-δ (x ≈ 0.20; δ ≈ 0.10) Oxide Matrix by Sol-Gel Growth

  • Das, Bidhu Bhusan;Palanisamy, Kuppan;venugopal, Potu;Sandeep, Eesam;Kumar, Karrothu Varun
    • 대한화학회지
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    • 제61권1호
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    • pp.29-33
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    • 2017
  • Formation of Au particles in nonstoichiometric $Cu_{2-x}{^I}Cu{_2}^{II}O_{3-{\delta}}$ ($x{\approx}0.20$; ${\delta}{\approx}0.10$) oxide from aniline + hydrochloric acid mixtures and chloroauric acid in the ratios 30 : 1; 60 : 1; 90 : 1 (S1-S3) by volume and 0.01 mol of copper acetate, $Cu(OCOCH_3)_2.H_2O$, in each case is performed by sol-gel growth. Powder x-ray diffraction (XRD) results show Au particles are dispersed in tetragonal nonstoichiometric dicopper (I) dicopper (II) oxides, $Cu_{2-x}{^I}Cu{_2}^{II}O_{3-{\delta}}$ ($x{\approx}0.20$; ${\delta}{\approx}0.10$). Average crystallite sizes of Au particles determined using Scherrer equation are found to be in the approximate ranges ${\sim}85-140{\AA}$, ${\sim}85-150{\AA}$ and ${\sim}80-150{\AA}$ in S1-S3, respectively which indicate the formation of Au nano-micro size particles in $Cu_{2-x}{^I}Cu{_2}^{II}O_{3-{\delta}}$ ($x{\approx}0.20$; ${\delta}{\approx}0.10$) oxides. Hysteresis behaviour at 300 K having low loop areas and magnetic susceptibility values ${\sim}5.835{\times}10^{-6}-9.889{\times}10^{-6}emu/gG$ in S1-S3 show weakly ferromagnetic nature of the samples. Broad and isotropic electron paramagnetic resonance (EPR) lineshapes of S1-S4 at 300, 77 and 8 K having $g_{iso}$-values ${\sim}2.053{\pm}0.008-2.304{\pm}0.008$ show rapid spin-lattice relaxation process in magnetic $Cu^{2+}$ ($3d^9$) sites as well as delocalized electrons in Au ($6s^1$) nano-micro size particles in the $Cu_{2-x}{^I}Cu{_2}^{II}O_{3-{\delta}}$ ($x{\approx}0.20$; ${\delta}{\approx}0.10$) oxides. Broad and weak UV-Vis diffuse reflectance optical absorption band ~725 nm is assigned to $^2B_{1g}{\rightarrow}^2A_{1g}$ transitions, and the weak band ~470 nm is due to $^2B_{1g}{\rightarrow}^2E_g$ transitions from the ground state $^2B_{1g}$(${\mid}d_{x^2-y^2}$>) of $Cu^{2+}$ ($3d^9$) ions in octahedral coordination having tetragonal distortion.

NiFe/FeMn 이중박막의 증착시 자기장에 의한 교환결합력 이방성 효과 (Anisotropy Effect of Exchange Bias Coupling by Unidirectional Deposition Field of NiFe/FeMn Bilayer)

  • 박영석;황도근;이상석
    • 한국자기학회지
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    • 제18권5호
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    • pp.180-184
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    • 2008
  • 이온빔 증착법으로 제작한 코닝유리(Corning glass)/Ta(5 nm)/NiFe(7 nm)/FeMn(25 nm)/Ta(5 nm) 다층박막 구조에서 반강자성체 FeMn층 증착시 인가한 일축 이방성 자기장 방향에 따른 강자성체 NiFe층의 자화 스핀배열 의존성을 조사하였다. NiFe층과 FeMn 층 증착시 인가한 자기장 방향을 달리한 각도는 각각 $0^{\circ},\;45^{\circ},\;90^{\circ}$였다. 용이축 MR(magnetoresistaice) 곡선으로부터 얻은 교환결합세기(Hex)는 증착 자기장 각도가 $45^{\circ}$일 때 40 Oe로, $90^{\circ}$일 때는 거의 0 Oe로 감소하였다. 반면에 곤란축 MR 곡선으로부터 얻은 $H_{ex}$ 값은 증착 자기장 각도가 $45^{\circ}$일 때 35 Oe로, 90o일 때는 79 Oe로 증가하였다. 강자성체 층의 용이축과 반강자성체 층의 일축 이방성 방향이 $90^{\circ}$ 차이가 나는 계면에서도 FeMn층이 NiFe층의 자기모멘트 스핀방향을 회전시켜 교환결합 이방성 효과가 발생함을 알 수 있었다.

RF 마그네트론 스퍼터링법으로 증착된 Multiferroic BiFeO3 박막의 미세구조 및 자기적 특성 (Microstructures and Magnetic Properties of Multiferroic BiFeO3 Thin Films Deposited by RF Magnetron Sputtering Method)

  • 송종한;남중희;강대식;조정호;김병익;최덕균;전명표
    • 한국자기학회지
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    • 제20권6호
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    • pp.222-227
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    • 2010
  • RF 마그네트론 스퍼터링법을 이용하여 Pt/Ti/$SiO_2$/Si(100) 기판위에 $BiFeO_3$ 박막을 증착하였고, 스퍼터링 공정에서 산소량이 $BiFeO_3$ 박막에 미치는 영향을 조사하였다. $BiFeO_3$ 박막은 XRD 회절패턴의 결과를 통하여 소량의 불순물상이 존재하는 페로브스카이트 구조로 결정화되었다. $O_2$ 가스의 유량은 박막의 미세구조 및 자기적 특성에 많은 영향을 끼친다. $O_2$ 가스의 유량이 증가함에 따라 박막의 표면 거칠기 및 grain size가 증가하였다. $BiFeO_3$ 박막은 상온에서 약자성적인 거동을 보였으며, PFM 측정을 통하여 박막의 미세구조와 압전계수와의 상관관계를 조사하였다.

Physical Properties of the Nonstoichiometric Perovskite $Dy_{1-x}Sr_xCoO_{3-y}$ System

  • 정수경;김민규;김규홍;여철현
    • Bulletin of the Korean Chemical Society
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    • 제17권9호
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    • pp.794-798
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    • 1996
  • Solid solutions of the nonstoichiometric Dy1-xSrxCoO3-y system with the compositions of x=0.00, 0.25, 0.50, 0.75, and 1.00 have been synthesized by the solid state reaction at 1000 ℃ under atmospheric air pressure. The crystallographic structures of the solid solutions are analyzed by the powder X-ray diffraction patterns at room temperature. The analyses assign the compositions of x=0.00 and 0.25 to the orthorhombic system with space group of Pbnm/D2h16, the compositions of x=0.50 and 0.75 to the tetragonal system like a typical SrCoO2.86, and the composition of x=l.00 or SrCoO2.50 to the brownmillerite type system with space group of I**a. The reduced lattice volumes increase with x value due to the larger radius of Sr2+ ion than that of Dy3+ ion. The mole ratio of Co4+ ion to total Co ion with mixed valence state between Co3+ and Co4+ ions at B sites or τ value has been determined by an iodometric titration. All the samples except for the DyCoO3 compound show the mixed valnce state and thus the composition of x=0.50 has the maximum τ value in the system. The oxygen vacancies increasing with x value are randomly distributed over the crystal lattice except for the composition of x=l.00 which have the ordering of the oxygen vacancies. The nonstoichiometric chemical formulas of the Dy1-xSrxCo3+1-τCo4+τO3-(x-τ)/2 system are formulated from the x, τ, and y values. The electrical conductivity in the temperature range of 100 to 900 K increases with τ value linearly because of positive holes of the Co4+ ions in π* band as a conducting carrier. The activation energy of the x=0.50 as Ea=0.17 eV is minimum among other compouds. Broad and high order transition due to the overlap between σ* and π* bands broadened by the thermal activation is observed near 1000 K and shows a low temperature-semiconducting behavior. Magnetic properties following the Currie-Weiss law show the low to high spin transition in the cobaltate perovskite. Especially, the composition of x=0.75 presents weak ferromagnetic behavior due to the Co3+-O2--Co4+ indirect superexchange interaction.