Parity Nonconservation in Atomic Phenomena
Khriplovich (physics, Novosibirsk U., USSR) describes his own work and that of others in demonstrating the first decisive confirmations of the unified model of atomic electroweak interactions. The studies of weak interaction by optical methods, at the boundary between elementary particle physics and atomic spectroscopy, have revealed parity nonconservation in atomic transitions. He considers the effects of space-inversion and time-reversal violations in atoms, molecules, and condensed matter. First published in Russian in 1981, and translated from the 1988 second edition. Annotation copyrighted by Book News, Inc., Portland, OR
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The general structure of weak electronnucleon interactions
Qualitative consideration of parity nonconservation effects
The hydrogen atom
Calculation of the mixing of oppositeparity levels
Optical highly forbidden Ml transitions in heavy atoms
Optical activity of heavymetal vapours General considerations
Observation of optical activity of heavymetal vapours
Podd nuclear forces another source of parity violation
Bloch domain walls in ferromagnetic films
Phase transition between gyrotropic and nongyrotropic structures
Electromagnetic waves in metals
Podd current in ferromagnetic materials in a magnetic field
Parity nonconservation in photogalvanic effects
Weak interactions and low temperatures
Electric dipole moment in the Bphase of superfluid 3He
Searching for Tinvariance violation in atoms and molecules
What else can be discovered about weak interactions from
Parity nonconservation effects in diatomic molecules
How can weak charges of protons and neutrons be measured?
Anticrossing of levels caused by the weak interaction
Weak interactions and optical isomers
Mossbauer effect and optical isomers
Are oscillations of optical activity observable?
Parity nonconservation and asymmetry of biological molecules
Parity nonconservation in crystals
Can parity nonconservation be observed in phase transitions?
Limits on the Todd weak interaction constants for neutral currents
Screening of electric dipole moments in an atom By what can it be violated?
Proton EDM Magnetic quadrupole and Schiff moments of the nucleus
Tinvariance nonconservation in nucleonnucleon inter action and Todd nuclear moments
absorption accuracy admixed El amplitude admixture anapole approximation arises bismuth caesium circular polarization compared configuration considered constant contribution Cooper pair coordinate correction corresponding Coulomb degree of circular density dependence dipole dipole moment discussed electric field electromagnetic energy enhancement estimate experiment experimental data expression external field factor Faraday Faraday effect formula Hamiltonian Hartree-Fock heavy atoms helical helix hyperfine hyperfine structure induced isotope left-handed limit magnetic field matrix element measurements Ml amplitude Ml transition molecular molecule momenta neutral currents neutron non-relativistic noted Novosibirsk nuclear spin nucleon nucleus obtained operator optical activity order of magnitude P-odd P-odd effects P-odd interaction parameters parity nonconservation effects particle polarizability potential proton quadrupole radial integral relativistic result rotation angle samarium sin2 spin-orbit interaction splitting standard model structure T-invariance T-odd tensor term thallium theoretical tion total angular momentum vapours vector wave function weak interaction zero
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