SUMMARY
The discussion centers on the radiation of light from atoms in stationary states, specifically addressing the hydrogen atom's Hamiltonian. It concludes that while stationary states are defined by a constant Hamiltonian, the introduction of the vacuum electromagnetic (EM) field alters this, leading to non-stationary states. The vacuum EM field triggers spontaneous emissions through stimulated emissions, which are facilitated by interaction terms added to the Hamiltonian, such as (1/2m)(p - eA)² + eφ. This interaction allows transitions between excited and ground states, challenging the notion that atoms remain in eigenstates of their Hamiltonian.
PREREQUISITES
- Understanding of quantum mechanics principles, particularly stationary states.
- Familiarity with Hamiltonian mechanics and its application in quantum systems.
- Knowledge of quantum electrodynamics (QED) and its implications for atomic behavior.
- Basic grasp of electromagnetic fields and their role in atomic transitions.
NEXT STEPS
- Research the role of the vacuum electromagnetic field in quantum electrodynamics.
- Study the implications of adding interaction terms to the Hamiltonian in quantum systems.
- Explore the concept of spontaneous and stimulated emissions in atomic physics.
- Investigate the differences between eigenstates of the atomic Hamiltonian and the full QED Hamiltonian.
USEFUL FOR
Physicists, quantum mechanics students, and researchers in quantum electrodynamics seeking to deepen their understanding of atomic radiation and the effects of electromagnetic fields on stationary states.