The total angular momentum of an atomic nucleus, including the orbital and intrinsic spin contributions of its constituent nucleons.
The electric quadrupole moment of an atomic nucleus, conventionally specified in its stretched nuclear spin state. It measures a nonspherical nuclear charge distribution. Its interaction with the electronic electric-field gradient contributes to hyperfine structure and generally changes the magnetic-dipole Landé interval rule. A permanent rank-two moment vanishes for nuclear spin less than one.
The magnetic dipole moment associated with nuclear spin, using dimensionless angular momentum operators and the nuclear magneton . The quoted scalar moment is its expectation in the stretched quantum state, . In the same electronic energy level, the leading magnetic-dipole hyperfine structure constant is proportional to , apart from isotope-dependent electronic and nuclear-size corrections.
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