How to measure Magnetic Anisotropy Constants · 1 MINT Seminar How to measure Magnetic Anisotropy...

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1 MINT Seminar How to measure Magnetic Anisotropy Constants Takao Suzuki MINT Center THE UNIVERSITY OF ALABAMA MINT Center for Materials for INformation Technology MINT Center, Univ.Alabama March 8, 2013 ([email protected])

Transcript of How to measure Magnetic Anisotropy Constants · 1 MINT Seminar How to measure Magnetic Anisotropy...

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    MINT Seminar

    How to measure Magnetic Anisotropy Constants

    Takao SuzukiMINT Center

    THE UNIVERSITY OF ALABAMA MINT

    Center for Materials for INformation TechnologyMINT Center, Univ.Alabama March 8, 2013 ([email protected])

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    Contents

    1. Magnetic Anisotropy

    2. Stoner-Wohlfarth Model

    3. Torque Measurements

    3.1 Rotational hysteresis loss

    3.2 Torque analysis

    3.3 45 Torque method

    4. Our new torque magnetometer

    5. Users Guideline

    THE UNIVERSITY OF ALABAMA MINT

    Center for Materials for INformation TechnologyMINT Center, Univ.Alabama March 8, 2013 ([email protected])

  • 3MINT Center, Univ.Alabama

    1 kA/m= 1 emu/cm3

    1 kA/m = 12.57 Oe

    1. Magnetic Anisotropy

    Magnetic anisotropy K = Ms x Hs = (1,400 emu/cc x 6.5kOe) = 5 x 106 erg/cc

    E.A.

    E.A. E.A.

    H.A.

    H.A. H.A.

    1. Example

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    1. Magnetic Anisotropy

    2. Magnitude

    K1 (Ni): 4 x 104 erg/cc (0.2 eV/atom)K1 (Fe): 5 x 105 erg/cc (2 eV/atom) Ku1 (Co): 5 x 106 erg/cc (20 eV/atom)

  • MINT Center, Univ.Alabama 5

    200 400 600 800 1000 1200 1400

    106

    107

    108 CoPt

    Fe3Pt

    Co

    NdFeBFePt

    SmCo5

    Co3Pt

    FePdMnAl

    CoPtCr

    K U

    (erg/

    cc)

    MS (emu/cc)

    MnBi MnAlMnBi

    Hk (= 2Ku/Ms) : 4 20 T

    3. Materials1. Magnetic Anisotropy

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    1. Magnetic Anisotropy

    4. Origin4.1 Magneto-crystalline anisotropy (Intrinsic)

    4.2 Induced magnetic anisotropy (Extrinsic)- Pair-ordering- Shape anisotropy- Stress induced anisotropy- Surface/interface anisotropy

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    Magneto-crystalline Anisotropy

    Spin Angular Moment

    Orbital Angular

    MomentumLattice

    Spin Angular Moment

    Orbital Angular

    MomentumLattice

    3d elementsFe, Ni, Co

    RE elementsTb, Dy, Nd

    S CouplingCrystalline field

    S L

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    1. Magnetic Anisotropy

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  • 8MINT Center, Univ.Alabama

    1. Magnetic Anisotropy

    4. Origin

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  • 9MINT Center, Univ.Alabama Hiroaki Yamamoto and Takao Suzuki: Unexpectedly Large Magnetic Anisotropy of Fe3Pt Alloy Thin Films with Various Crystallographical Orientations IEEE Trans.Mag., 44, No.11, 2868 (2008).

    1. Magnetic Anisotropy

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    4. Origin4.2 Induced magnetic anisotropy (Extrinsic)

    - Surface/interface anisotropy

    THE UNIVERSITY OF ALABAMA MINT

    Center for Materials for INformation TechnologyMINT Center, Univ.Alabama

    1. Magnetic Anisotropy

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    1. Magnetic Anisotropy

    5. Phenomenological expression

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  • -6 -4 -2 0 2 4 6

    -5

    0

    5

    -6 -4 -2 0 2 4 6

    -5

    0

    5

    E=K1(122232)+K2(1222+ 2232 + 3212)+.

    Magnetic anisotropy constants of Fe3Pt/MgO

    K1= 4106 erg/cc

    K2= 2107 erg/cc

    Magnetic anisotropy energy in Cubic

    is the easy axis, since those K1 and K2 fulfill the condition

    K2 > 9/4K1

    K2=9K1

    K2=9/4K1

    K1

    K2

    H(kOe)

    M (1

    0-3 e

    mu)

    Substrate : MgO(100)Deposition temperature : 400 Thickness : 500

    0 15 30 45 60 75 901.2

    1.4

    1.6

    1.8

    angle,

    Hc

    (kO

    e)Magnetic Anisotropy

    MINT Center, Univ.Alabama 12Hiroaki Yamamoto and Takao Suzuki: Unexpectedly Large Magnetic Anisotropy of Fe3Pt Alloy Thin Films with Various Crystallographical Orientations IEEE Trans.Mag., 44, No.11, 2868 (2008).

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    Ku1 and Ku2 vs T for h.c.p. Co

    M.Takahashi and T.Suzuki; Jap. J.Apply.Phys.18, No6, 1071-1078 (1979).

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    2. Stoner Wolfarth Model

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    Note: In reality, unless H > Hk

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    2. Stoner-Wohlfarth Model

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    h//2/3 + h 2/3 = 1

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    Two angles ( = ,) for stable M direction when h (= H/Hk) < 1.

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    3. Torque Magnetometer

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    Center for Materials for INformation TechnologyMINT Center, Univ.Alabama

    L = M x H

    0 90 180 270 360

    -5

    0

    515kOe

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    Torque Analysis -1-Rotational hysteresis-

    THE UNIVERSITY OF ALABAMA MINT

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    Calculation Experimental0.489

    0.415

    0.369

    0.738

    0.553

    0.0.521

    5.45

    1.20

    0.922

    0.5+

    0.5-

    0.3

    0.8

    0.7

    0.6

    >>

    1.0

    0.9

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    Floyd.B. Humphrey: JPL Research summary No.36-13 (1962)

  • Torque Analysis -1-Rotational hysteresis-

    William D. Doyle Torque and Rotational Hysteresis in fcc Single Crystal Cobalt Films J. Appl. Phys. 35, 929 (1964).

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    Bi-axial anisotropy of fcc Co film

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    Torque Analysis -245 Torque Method

    E = KV sin2 MVH cos ( )L = MVH sin ( )

    THE UNIVERSITY OF ALABAMA MINT

    Center for Materials for INformation Technology

    M

    H

    E.A.

    H.A.(L/H)2 = - (M2V/2K)L + (MV)2

    (L/H)2

    L

    (M2V/2K)

    (MV)2

    K and Ms can be estimated directly !

    For = 45,

    H.Miyajima, K.Sato and T. Mizoguchi: Simple analysis of torque measurement of magnetic thin films J.Appl.Phys. 47, No10, 4669-4671 (1976).

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    K

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  • 0 90 180 270 360-20

    -10

    0

    10

    20 15kOe

    0 90 180 270 360

    -5

    0

    515kOe

    () ()

    Fe3Pt (001)/MgO(100) Fe3Pt (111)/MgO(111)

    Easy Axis Easy Axis

    Lin=(1/18)K2sin6Torque, Lin=(1/2)K1sin4

    Torque curves of different crystallographycal orientationTo

    rque

    , L(d

    yne-

    cm)

    Lin=L1sin+L2sin2+L4sin4+..+L6sin6+...

    TS:4000C

    sample

    Mirror DL

    N S

    Torque Analysis -3Fourier Analysis Method

    L() (H) Lin()Hiroaki Yamamoto and Takao Suzuki: Unexpectedly Large Magnetic Anisotropy of Fe3Pt Alloy Thin Films with Various Crystallographical Orientations IEEE Trans.Mag., 44, No.11, 2868 (2008).MINT Center, Univ.Alabama 21March 8, 2013 ([email protected])

  • 22THE UNIVERSITY OF ALABAMA MINT

    Center for Materials for INformation Technology

    Torque Analysis - 3Fourier Analysis Method

    Experimental torque curves;

    L(,Ho) = L1sin + L2sin2 + L3sin 3 +L4sin 4 + . ,Where L1, L2, L3, L4 .. can be obtained from the Fourier Decomposition of the torque curves as a function of Ho.

    Two-fold component K1 or Ku1

    Four-fold component K2 or Ku2

    L2L4

    1/Ho

    Torq

    ue A

    mpl

    itude Ku1

    Ku2

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  • MINT Center, Univ.Alabama 23

    90 kOe (9T)10-7 emu2 ~400 KTorque mag

    4. Our new Torque magnetometer

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  • THE UNIVERSITY OF ALABAMA MINT

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    Magnetic Anisotropy - 1

    1. Header (36)1.1 sub header (32)

    Text font (24)

    1.1.1 sub sub header (28)

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    Magnetic Anisotropy - 1

    THE UNIVERSITY OF ALABAMA MINT

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  • 28THE UNIVERSITY OF ALABAMA MINT

    Center for Materials for INformation Technology

    300 K 2 K

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    Users Guideline

    Users must have- Understanding of basic principle of

    operation- Training for how to operate- Report each time in logbook- Report any problems to Mr. John

    Hawkins and Mr. Jason Foster, as well as your adviser

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  • MINT Center, Univ.Alabama 30March 8, 2013 ([email protected])

    Slide Number 1Slide Number 21. Magnetic Anisotropy Slide Number 4Slide Number 5Slide Number 6Magneto-crystalline Anisotropy1. Magnetic Anisotropy1. Magnetic AnisotropySlide Number 10Slide Number 11Slide Number 12Ku1 and Ku2 vs T for h.c.p. CoSlide Number 14Slide Number 15Slide Number 16Slide Number 17Torque Analysis -1-Rotational hysteresis-Slide Number 19Slide Number 20Slide Number 21Slide Number 22Slide Number 23Slide Number 24Slide Number 25Slide Number 26Slide Number 27Slide Number 28Slide Number 29Slide Number 30