If a system is in a quantum state for a time interval Dt, then the uncertainty in the energy of that state is related to the lifetime of that state by the energy-time uncertainty principle:
The square of the magnitude of the wave function is proportional to the probability of locating the particle in a given region of space.
The quantum state of the electron in an atom can be described by four quantum numbers: principal quantum number n = 1, 2, 3, . . . orbital angular momentum quantum number
(3.0K) magnetic quantum number (4.0K) spin magnetic quantum number (1.0K)
According to the exclusion principle, no two electrons in an atom can be in the same quantum state.
The set of electron states with the same value of n is called a shell. A subshell is a unique combination of n and (0.0K) Spectroscopic notation for a subshell is the numerical value of n followed by a letter representing the value of (0.0K)
In a solid, the electron states form bands of closely spaced energy levels. Band gaps are ranges of energy in which there are no electron energy levels. Conductors, semiconductors, and insulators are distinguished by their band structure.
If an electron is in a higher energy level and a lower level is vacant, an incident photon of energy DE can stimulate the emission of a photon. The photon emitted by the atom is identical to the incident photon.
Lasers are based on stimulated emission. In order for stimulated emission to occur more often than absorption, a population inversion must exist (the state of higher energy must be more populated than the state of lower energy).
The wave function of a confined particle extends into regions where, according to classical physics, the particle can never go because it has insufficient energy. If the classically forbidden region is of finite length, tunneling can occur.
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