'Hyperfine' diaporamas de présentation

S=1/2 systems

S=1/2 systems. PRINCIPLE. h ?. Energy. B 0. B r. z. y. x. EPR of isotrope systems: the g-value. For a bound electron: additional magnetic field ? B. In EPR:. EPR of isotrope systems. ? E. Energy. B 0 = 0. B 0 > 0. 1 mT. EXAMPLE.

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Quantum phase transitions in anisotropic dipolar magnets

Quantum phase transitions in anisotropic dipolar magnets. Moshe Schechter. University of British Columbia. In collaboration with: Philip Stamp, Nicolas laflorencie. LiHoY F. x. 1-x. 4. 1. Transverse field Ising model:. LiHoY F. x. 1-x. 4. 1. Transverse field Ising model:.

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Tunable Molecular Many-Body Physics and the Hyperfine Molecular Hubbard Hamiltonian

Tunable Molecular Many-Body Physics and the Hyperfine Molecular Hubbard Hamiltonian. Michael L. Wall Department of Physics Colorado School of Mines in collaboration with Lincoln D. Carr. Motivation: Ultracold atoms in optical lattices. Trapping in optical potential

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Electron Spin Resonance Spectroscopy

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