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Pauli Paramagnetism
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Pauli’s Spin Matrices 12/7/2018 Let’s concentrate on electronic spins
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Zeeman Effect quantization of angular momentum B = 0 B 0
12/7/2018 quantization of angular momentum B = 0 B 0 B shifts the energy of each state by U ml: magnetic quantum number
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Electron Spin B = 0 B 0 Anomalous Zeeman splitting
12/7/2018 B = 0 B 0 Anomalous Zeeman splitting Stern-Gerlach experiment (1922) splitting into an even number of components (should be 2l +1) Goudsmidt and Uhlenbeck (1925): spinning on its axis Dirac’s theory (1928): existence of spin angular momentum
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Spin Angular Momentum ms: spin quantum number
12/7/2018 ms: spin quantum number ms = +1/2: “spin up” and ms = -1/2 : “spin down”
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Gyromagnetic Ratio and the Electron g-factor
12/7/2018 : gyromagnetic ratio g-factor Quantum Electrodymanics (QED)
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Spin is Purely Quantum Mechanical
12/7/2018 Orbital angular momentum: As h 0, we can keep L non-zero by increasing the size of l to infinity Spin angular momentum: As h 0, S 0
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Magnetic Susceptibility
12/7/2018 Total field [T] or [Wb/m2] Applied field [A/m] 4p × 10-7 [T-m/A] Induced field [A/m] : magnetization curve c > 0: paramagnetic c < 0: diamagnetic
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Calculate Spin c “Classically”
12/7/2018 spin “down” spin “up” Consider N electrons in volume V at temperature T in a magnetic field H, and calculate the total magnetic moment M Too large, and temperature dependent
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Pauli’s Spin Susceptibility
12/7/2018 g↓(e) 2mBm0H e spin imbalance magnetic moment per electron g↑(e) Net magnetic moment per m3:
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