SLIDE 1
Non-uniform Thickness in Two-dimensional Micromagnetic Simulation - - PowerPoint PPT Presentation
Non-uniform Thickness in Two-dimensional Micromagnetic Simulation - - PowerPoint PPT Presentation
Non-uniform Thickness in Two-dimensional Micromagnetic Simulation Don Porter Mike Donahue Information Technology Laboratory National Institute of Standards and Technology Gaithersburg, Maryland Fewer cells Less memory required 2D
SLIDE 2
SLIDE 3
2D Model Shortcomings
No variation through thickness Limited to thin films Limited to single layers Limited to uniform thickness - Why? SLIDE 4
2D Model with Variable Thickness
For each cell k, store a relative thickness- t
- 1
- t
- t
- j
- H
- M
- M
- H
SLIDE 5
Zeeman Energy
Energy density and field unchanged E k;Z =- M
- H
- 2
SLIDE 6
Anisotropy Energy (uniaxial)
Energy density and field unchanged H k;A = 2K 1- M
- u)u
- X
- M
- H
- 2
SLIDE 7
Exchange Energy
Original expression (eight-neighbor cosine) E k;ex h = A 3 2 m k- X
- m
- X
- m
- X
- m
SLIDE 8
Exchange Energy Thickness Weighting
Weights should have these properties w (t 1 ; t 2 ) = w (t 2 ; t 1 ) w (t; t) = t min (t 1 ; t 2 )- w
- max
SLIDE 9
Magnetostatic Energy
Uniform thickness: Grid is periodic Demagnetization field is convolution of magnetization. Efficient FFT techniques available Variable thickness: efficient structure lost Preserve efficiency: represent reduced thickness as reduced moment. M k ! M k t k SLIDE 10
Magnetostatic Energy
Moment reduction good “far-field” approximation. Self-demagnetization energy of a cell need correction H k = D(M k t k ) Change in moment interpreted as change in demag factors H k = (t k D)M ktrace
(t k D) = t k 6= 1 Local correction, add (1- t
as a correction to the out-of-plane demag field.
SLIDE 11
Magnetostatic Energy Adjustment Results
Represent a 100- 100
- 10 nm oblate ellipsoid with three models
– 2D uniform thickness – 2D with variable thickness adjustments – 3D using 10 layers
Cell size 1 nm for all. Check how well each produces uniform demag field. Check calculated demag factors– In-plane: 0.0696 – Out-of-plane: 0.8608
SLIDE 12
2D Uniform Thickness
In-plane: 0.1026 Out-of-plane: 0.7947 SLIDE 13
2D Variable Thickness
In-plane: 0.0635 Out-of-plane: 0.8730 SLIDE 14
3D With 10 Layers
In-plane: 0.0753 Out-of-plane: 0.8559 SLIDE 15
Shape Effects on Reversal
Compare magnetic reversal of three permalloy samples–
500- 100
- 10 nm (Std. Prob. 2,
- 19)
–
530- 130
- 10 nm
– truncated pyramid, base:
530- 130; top:
- 100 nm
SLIDE 16
530 x 130 Reversal
SLIDE 17
Magnetization Reversal Curves
−40 −1 1
Effect of size, edge taper on reversal
Bx (mT) Mx/Ms My/Ms
SLIDE 18
Truncated Pyramid Reversal
SLIDE 19
Comparison of 2D and 3D Results
- 530
- 130
- 10 nm sample
– 2D variable thickness model
H s- 25:5mT
– 3D model – 5 layers
H s- 24:5mT
– 2D variable thickness model
H s- 21:5mT
– 3D model – 5 layers
H s- 22:5mT