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Nuclear Electromagnetic Moments

Nuclear Electromagnetic Moments. Electric Multipoles. The electric energy associated with the electric charge distribution in the nucleus is determined by the interaction of the nuclear charge distribution with electric fields. Parity of V n goes as (-1) n. QM Analog for the Nucleus.

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Nuclear Electromagnetic Moments

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  1. Nuclear ElectromagneticMoments

  2. Electric Multipoles • The electric energy associated with the electric charge distribution in the nucleus is determined by the interaction of the nuclear charge distribution with electric fields.

  3. Parity of Vn goes as (-1)n

  4. QM Analog for the Nucleus • Vn is the multipole operator of order n •  is the nuclear wave function • For all fixed-parity states, the contribution from all odd multipole operators is zero!

  5. Electric Multipole Moments • All odd electric multipole momentsmust vanish for stationary states (e.g., nuclei, nucleons, etc.) • Therefore, nuclei must not have • Electric dipole moments (n = 1) • Electric octupole moments (n = 3) • Etc… • Search for electric dipole moment for neutron

  6. Electric Multipole Moments • In more general terms -- • All odd electric multipole momentsmust vanish if the nuclear system is time-reversible - i.e., if it obeys time reversal symmetry. • Find an electric dipole moment for neutron implies time reversal symmetry violation!

  7. Magnetic Multipole Moments • Classically, a circulating current induces a magnetic dipole moment -- • where A is the area enclosed by i. • If i is due to a single chargee moving with velocity v, we get --

  8. Magnetic Multipole Moments • If i is due to a single chargee moving with velocity v, we get --

  9. In the QM regime, this becomes --

  10. g-factors For the proton For the neutron

  11. g-factors For the electron For the proton For the neutron

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