The dimensionless coefficient in the spin part of the electron magnetic moment. It is distinct from a gyromagnetic ratio, which has units: in the angular convention, . It is also distinct from the Landé g-factor of a combined atomic angular momentum and from a nuclear or hyperfine g-factor.
For spin one-half, the largest magnitude of a spin-component magnetic dipole moment is , not . Thus the ideal value gives one Bohr magneton. This follows directly from the spin angular momentum projections .
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