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Published byKornelia Bednarek Modified over 5 years ago
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2D Ising model Monte-Carlo (Metropolis) method
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2D Ising model Monte-Carlo (Metropolis) method
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Some Ferromagnetic Elements Some Paramagnetic Elements
• Iron • Uranium • Nickel • Platinum • Cobalt • Aluminum • Gadolinium • Sodium • Dysprosium • Oxygen
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Magnetic dipole–dipole interaction
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Energy Magnetization
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T<<Tc T ~Tc T>> Tc
Almost at the Close to the phase High temperature ground state transition (no correlation between spins) Single large cluster Broad distribution All clusters of like of ordered spins of clusters spins are small with small clusters of opposite spins
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Monte-Carlo method
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Onsanger exact result H=0, kB=1, J=1
for critical temperature T~Tc=2.269 T<<Tc T>>Tc
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The mean average over all configurations=
Yang exact result for H=0 forr magnetization Ergodic principle After thermalization The mean average over all configurations= The mean time average over 1 configuration
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The thermalization depends on
the size of the lattice and the number of steps
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A new look on the two-dimensional Ising model: thermal artificial spins amorphous Co68Fe24Zr8 NxN lattice , N=10487
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