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