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Co-Al 시스템의 비대칭적 혼합거동에 관한 이론 및 실험적 고찰
김상필1,2, 이승철1, 이광렬1, 정용재2 1. 한국과학기술연구원 미래기술연구본부 2. 한양대학교 세라믹공학과 박재영, 황정남 연세대학교 물리학과
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Introduction Major Materials Issue is the interfacial structure
Typical structure of spintronic device Major Materials Issue is the interfacial structure and chemical diffusion in atomic scale CMSEL Hanyang Univ.
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Atomic deposition behavior
Al on Co(0001) Co on Al(111) TOP VIEW CMSEL Hanyang Univ. Simulation Results
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Calculation Methods Simulation Results
Adatom (normal incident 0.1 eV) 300K Initial Temperature 300K Constant Temperature Fixed Atom Position Co-Al eam potential* x,y-axis : Periodic Boundary Condition z-axis : Open Surface Deposition rate: × 10-1 nm/nsec MD calc. step : 0.5fs * C. Vailhe et al. J. Mater. Res., 12 No (1997). CMSEL Hanyang Univ. Simulation Results
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Thin Film Growth Behavior
Atomic configurations Layer density 3ML Al on Co(001) No mixing & Sharp Interface 3ML Co on Al(001) Mixing & Interface alloying Significantly different thin film growth behavior was reported CMSEL Hanyang Univ. Simulation Results
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Mixing Criteria Simulation Results Local Acceleration
Activation Barrier for Mixing (1) Co Al 3.5eV (2) (3) (4) (1) (2) (4) (3) Reaction Coordinate CMSEL Hanyang Univ. Simulation Results
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Ion Scattering Spectroscopy
CoAxial Impact Collision Ion Scattering Spectroscopy (CAICISS) Energy range of ~ keV → penetration depth : < 10 Å It can analyze the 3-dim. atomic structure of crystal surface and sub-surface by classical approximation of scattering (bond direction) intensity (angle) Da o a c1 c2 a c1 d A B c2 o Da Atomic geometry and shadow cone at various incident angles Variation of intensity of ions scattered by target atoms CMSEL Hanyang Univ. Experimental Evidences
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Polar [1100]; clean Co(0001) surface
× Bridge site On top site hcp site fcc site CMSEL Hanyang Univ. Experimental Evidences
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Polar scan curves Experimental Evidences along [1100] direction
Al atom(s) 1st Co layer 2nd Co layer Ah2 fcc hcp On Top site(s) Bridge Ah2’, Af2’ Ah1’, Af1’ Ah1,,Af1 1.8 ± 0.05 Å DFT calculation results CMSEL Hanyang Univ. Experimental Evidences
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Atomic deposition behavior
Al on Co(0001) CMSEL Hanyang Univ. Simulation Results
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Polar [100]; clean Al(001) surface
1st 2nd 3rd 4th 4.05 Å A130 A132 A121 A11 A122 A123 A11 (12.9°) A122 (11.52°) A122 (26.4°) A132 (20.4°) A130 (79.1°) CMSEL Hanyang Univ. Experimental Evidences
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Polar [100]: B2 structure Experimental Evidences
2nd Co 3rd A130 A131 C230 C231 C232 4.05 Å 4th 2.867 Å B2-CoAl alloy was formed on Al(001) surface CMSEL Hanyang Univ. Experimental Evidences
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Magnetic Behavior of Co-Al system
Stable intermetallic compound B2(CsCl) structure B2 - CoAl Ab-initio calculations Spin-Up Spin-Down FCC - Al B2 - CoAl HCP - Co Nonmagnetic Metal Nonmagnetic Metal Magnetic Metal The perfectly ordered B2-CoAl does not show any magnetic behavior CMSEL Hanyang Univ. Simulation Results
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(Magneto-Optic Kerr effects)
Experimental Measurement Si substrate Cu buffer layer (1500 A) Co (30 A) Al (30 A) Al (840 A) Capping layer (50 A) Capping layer (50A) MOKE (Magneto-Optic Kerr effects) CMSEL Hanyang Univ. Experimental Evidences
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Asymmetric Alloy Effect
Co Al Al Co CMSEL Hanyang Univ. Experimental Evidences
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Cap/Co/Buffer/Si(001) sample
CMSEL Hanyang Univ. Experimental Evidences
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Thickness of Mixing Region
~10 Å Co: Ferromagnetic GMR structure CoAl: Nonmagnetic Co: Ferromagnetic CMSEL Hanyang Univ. Experimental Evidences
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Conclusions Experimental Evidences Magnetic Behavior of CoAl
Deposition Behavior of Al on Co Deposition Behavior of Co on Al CMSEL Hanyang Univ. Experimental Evidences
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