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Progress Update. Compact Modeling of MTJs for use in STT-MRAM. Richard Dorrance Advisor: Prof. Dejan Marković March 12, 2010. Motivation. Magnetic Tunnel Junctions (MTJs) exhibit magnetic hysteresis Excellent potential as memory Integratable with CMOS Non-volatile
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Progress Update Compact Modeling of MTJs for use in STT-MRAM Richard DorranceAdvisor: Prof. Dejan Marković March 12, 2010
Motivation • Magnetic Tunnel Junctions (MTJs)exhibit magnetic hysteresis • Excellent potential as memory • Integratable with CMOS • Non-volatile • Spin-Transfer-Torque (STT) is a recently discovered phenomena • Predicted in 1996, observed in 2000 • No good compact model currently exists • Existing models oversimplify and ignore critical nonlinearities (temperature and voltage) • Problem for simulating STT-MRAM
Spintronic Operation • Spin Injector/Polarizer • Ferromagnetic layers tend to spin-polarize a current • Spin Detector • Ferromagnetic layers tend to scatter anti-parallel currents
Compact Model Landau–Lifshitz–Gilbert Equation Julliere’s Conductance Model
Temperature Nonlinearities • Saturation Magnetization • Weiss theory of ferromagnetism • Spin-Polarization • Affects resistance and STT • Modeled by:
Voltage Nonlinearities • TMR changes for an applied bias voltage • Simple fitting function
Simulation Setup • Compare transient behavior of MTJ model with a commercially available Micromagnetic Simulator: • ±1 mA, 10 ns pulses (30 ns total) • Total simulation time: • Micromagnetic Simulator: 13.5 hours • Verilog-A Model: 0.750 seconds
Simulation Results b(θ) not implemented
Future Work • Validation/refinement of model to measured devices • Explore the use of fitted function to replace b(θ) • b(θ) currently model a simple 5-layer structure • MTJ have 20+ layers with synthetic ferromagnets • Model C-STT 3rd Magnetic Layer (Perpendicular) • easier to switch • switching has greater thermal independence
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