scaling relations and magnetic properties of nanoparticles

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    Scaling relations and magneticproperties of nanoparticles

    Universidade Federal do Rio de JaneiroInstituto de Fsica

    Jos dAlbuquerque e Castro

    PAN AMERICAN ADVANCED STUDIES INSTITUTEUltrafast and Ultrasmall; New Frontiers and AMO Physics

    March 30 - April 11, 2008

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    polycrystalline alloys of Co, Cr, and Ptwith B or Ta

    segregation of the non-magnetic elements:reduction of the coupling between grains

    net magnetization

    grain size 10 nm

    Problem:superparamagnetism limit

    100 Gbit in -2

    areal density: 50 Gbit in -2 ( year 2000)

    Magnetic storage media: thin films

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    Superparamagnetism

    m

    magnetic particle

    energy barrier E B

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    Superparamagnetism

    m

    magnetic particle

    energy barrier E B

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    Superparamagnetism

    volume: V net anisotropy: K

    m energy barrier for reversal: E B = KV

    rate of switching: 1/ = f 0 exp(- E B /kT)

    f 0 10 9 s-1

    storage time 10 years E B ~ 40 kT

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    Patterned thin films

    Nanoimprint lithography

    arrays of circular nanomagnets

    cylinders with diameter D and height H

    5 nm H 150 nm

    50 nm D 500 nm Lebib et al., JAP 89, 3892 (2001)

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    particles cannot accommodate a domain wall

    patterned thin films as recording media

    200-260 Gbit in -2

    Patterned thin films

    grains within particles are strongly coupled

    1 Tbit in-2

    periodicity 25 nm

    (periodicity 50 nm)

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    R. P. Cowburn et al. , Phys. Rev. Lett 83, 1042 (99)

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    A. Lebib et al. , J. Appl. Phys. 89, 3892 (01)

    MFM

    vortex

    single-domain

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    R. P. Cowburn et al. , Phys. Rev. Lett. 83, 1042 (99)

    experimental phase diagram

    R. P. Cowburn et al. , Phys. Rev. Lett. 83, 1042 (99)

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    IIIIII

    in-plane out-of-plane vortex

    Configurations

    core

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    Theoretical approach

    E ij = classical dipolar interaction

    i = magnetic moment on site i

    J ij = exchange coupling

    K = anisotropy constant

    { 1, 2, 3} = angles between i and theprincipal (easy) crystalline axes

    i

    configuration of lowest energy ?

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    For smaller systems ( e.g. N ~ 10 6)

    single domain configurations only Reason: strength of the exchange interaction J

    Scaling approach

    J. dA. e C., D. Altbir, J. C. Retamal, and P. Vargas, Phys. Rev. Lett. (2002)

    J = x J with x < 1

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    x = 0.04

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    x = 0.04 x = 0.06

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    x = 0.04 x = 0.06

    x = 0.08

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    x = 0.04 x = 0.06

    x = 0.08

    x = 0.10

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    triple point

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    H t (x) = H t (1) x with = 0.55

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    Scaling relations

    H(1) = H(x) / x

    D(1) = D(x) / x

    J = x J

    From the relation

    H t (x) = H t (1) x H t (1) = H t (x)/ x

    we expect to find

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    Truncated conical particles

    C. A. Ross et al., Phys. Rev. B 62, 14252 (2000)

    C. A. Ross et al., J. Appl. Phys. 89, 1310 (2001)

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    = 0.3

    x = 0.010

    x = 0.015

    x = 0.020

    J. Escrig, P. Landeros, J.C. Retamal, D. Altbir, and J. dA. C., Appl. Phys. Lett. (2003)

    Calculation for Ni particles

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    = 0.3

    = 0.55

    Calculation for Ni particles

    J. Escrig, P. Landeros, J.C. Retamal, D. Altbir, and J. dA. C., Appl. Phys. Lett. (2003)

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    Important point: value of

    Scaling relations for magnetized nanoparticles P. Landeros, J. Escrig, D. Altbir, D. Laroze, J. dA.C., and P. Vargas Phys. Rev. B 71, 094435 (2005)

    value of may depend on the model for the magneticconfigurations!

    vortex core

    model for the core

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    Fast Monte-Carlo method

    http://www.ctcms.nist.gov/~rdm/mumag.org.html

    Fast Monte-Carlo method for magnetic nanoparticles P. Vargas, D. Altbir and J. d'Albuquerque e Castro Phys. Rev. B, 73, 092417 (2006)

    Could we combine the scaling technique and theMonte-Carlo method?

    Single domain limit:size L for which the flower and vortex states haveequal energy.

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    Fast Monte-Carlo method

    Mag group (NIST)

    L 8 l ex where l ex = (2A/ 0 M 0 )1/2

    Co: l ex = 3.6 nm a 0 = 0.2 nm J 0 =2.35 x10 3 kOe/ B

    L 29 nm and N 3x10 6 atoms !

    A = exchange stiffness constant J

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    Fast Monte-Carlo method

    For given L (small): Monte-Carlo J

    Calculations: L 1 = 5 a 0 x 1 = 2.240 10 -3

    L 2 = 7 a 0 x 2 = 4.125

    10-3

    L 3 = 9 a 0 x 3 = 6.509 10 -3

    x = J/J 0 L = L/ x

    ?

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    Fast Monte-Carlo method

    Results

    L = 8.02 l ex = 0.551

    Conclusion

    It is possible to combine the Monte-Carlo methodwith the scaling technique

    fast and reliable method for investigatingthe equilibrium properties of magnetic nanoparticles