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Applications of Spin-Polarized Photoemission P. D. Johnson, Annual Rev. Mater. Sci. 25 (1995) 455-85 Combined spin –integrated/resolved detector: Giringhelli,

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Presentation on theme: "Applications of Spin-Polarized Photoemission P. D. Johnson, Annual Rev. Mater. Sci. 25 (1995) 455-85 Combined spin –integrated/resolved detector: Giringhelli,"— Presentation transcript:

1 Applications of Spin-Polarized Photoemission P. D. Johnson, Annual Rev. Mater. Sci. 25 (1995) 455-85 Combined spin –integrated/resolved detector: Giringhelli, et al., Rev. Sci. Inst. 70 (1999) 4225

2 From Velev, et al Most spintronic devices involve materials interfaces, and depend on polarization both adjacent to the interface (direct space) and Fermi level (inverse space). Example: A slight oxidation of a FM (ferromagnetic ) surface can yield huge changes in spin transport properties. Why is this?

3 Consider the oxidation of Fe: Fe  Pauli Magnetism (delecalized electrons): Ferromagnetic (FM) FeOx  We start to induce localized spins on Fe cations, and these interactions are antiferromagnetic (AF) A-A- M +x A-A- A-A- A-A- A-A- A-A- d xy d yz d xz Δ d z2, d x2-y2 Fe +3 = 3d 5

4 In transition metal and lanthanum oxides, the magnetic ions are typically separated by oxygen anions. That’s a very long distance. Metal ions can interact with each other via an intervening anion thru superexchange: M 3d O(2p) Antiferromagnetic Ordering via Superexchange: Shared covalency of metal centers with the oxygen leads to M-O spin pairing (see Cox, Electronic Structure and Chemistry of Solids (Oxford Press)

5 Two isolated atoms/ions (Curie model) with unpaired spins S i,j have a spin-spin interaction energy defined as : U = -2KS i S j J = Exchange Integral J = When the exchange energy U is < kT, the spins become disordered or ferromagnetic antiferromagnetic χ=C/Tχ=C/(T-θ) T χ θ T complex behavior χ=C/(T-θ) T AF F

6 Therefore, we expect surface magnetism to depend heaviliy on: 1.Surface oxidation and other environmental factors 2.Temperature (below or above magnetic ordering temperature)

7 Spin-polarized photoemission should therefore be a powerful probe of environmental effects on surface magnetic behavior Review: spin-polarized detector P. D. Johnson, Ann. Rev. Mat. Sci. 25 (1995) 455

8 Temp. dependence of Fe(100) magnetic polarization near Ferm. Level (Johnson, Ann. Rev. Mat. Sci.)

9 Oxidation can then induce big changes in a FM surface! Metal/FM, P > 0 + O 2 FM, P > 0 Meta ox., AF P = 0 Is this reflected in SP-photoemission??

10 SP PES of clean Fe(100) shows high polarization near E F E. Vescovo, et al. Phys. Rev. B. 47 (1993) 13051 (Rapid Comm.)

11 ~ 3 L of O 2 exposure largely destroys polarization near E F

12 Fe(100) + O 2 @ RT Anneal to 650 C

13 A real MTJ: (S. Tehrani, et al. IEEE Trans. on Magnetics 36 (2000) 272) Note, a key step is Al deposition and oxidation…

14 Note, excessive oxidation decrease MR due to oxidation of the substrate electrode! Thicker oxide, attenuates C AP Too thick, oxidizes NiFe electrode

15

16 In such a system, metallic behavior for T< T c semiconducting behavior for T> T c

17 Spin-integrated PES: Magnetic ordering yields increase in DOS near Fermi level (consistent with model)

18 Spin-polarized PES: Increased metallic nature associated with polarization near E F


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