Spin Hamiltonians
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Updated
2009-03-12 00:09
Spin Hamiltonians
Spin Hamiltonians are energy expressions used to interpret NMR (Nuclear Magnetic Resonance), ESR (Electron Spin Resonance), EPR (Electron Paramagnetic Resonance), and ENDOR spectra. They are also useful in the fields of Spintronics and Quantum Computing.
| Symbol | Explanation |
|---|---|
| H | Overall Spin Hamiltonian, generally a Hermitian matrix |
| h J S1• S2 | Isotropic Exchange Interaction between two electron spins |
| h A S • I | Isotropic Hyperfine Coupling between an electron spin and a nuclear spin |
| h [A<FONT FACE="Symbol">^</FONT>(Sx Ix + Sy Iy) + A|| Sz Iz] | Axial Hyperfine Coupling between an electron spin and a nuclear spin |
| h (Ax Sx Ix + Ay Sy Iy + Az Sz Iz) | Rhombic Hyperfine Coupling between an electron spin and a nuclear spin |
| g μB B • S | Isotropic Electron Zeeman Effect for an electron spin in a magnetic field |
| μB [g<FONT FACE="Symbol">^</FONT>(Sx Bx + Sy By) + g|| Sz Bz] | Axial Electron Zeeman Effect for an electron spin in a magnetic field |
| μB (gx Sx Bx + gy Sy By + gz Sz Bz) | Rhombic Electron Zeeman Effect for an electron spin in a magnetic field |
| -gN μB B • I | Nuclear Zeeman Effect for a nuclear spin in a magnetic field |
| μ0/(4 π R3)[μ1• μ2 - 3(μ1• r)(μ2• r)] | Dipole-Dipole Interaction between two electron magnetic moments a distance R apart where r is the unit vector between them |
| h J I1• I2 | J-Coupling or Spin-Spin Coupling between two nuclear spins |
| Quadrupole Coupling due to a nuclear spin I>1/2 | |
| Zero-Field Splitting due to an electron spin S>1/2 | |
| Spin-Orbit Coupling between an electron spin and an angular momentum | |
| Russell-Saunders Coupling between an electron spin and an angular momentum | |





