Shielding (atomic physics)
Shielding designated in an electron - atom the reduction of the attractive interaction between an electron and the nucleus by the action of other electrons. In the central field model of the atom, the energy of an electron depends on the quantum numbers and :
- effective atomic number
- Atomic number
- Shielding constant (see below)
effective quantum number (see below)
- Principal quantum number
- Quantum defect
- Rydberg energy (there also the formula for one-electron systems for comparison ).
with the normalization factor N.
One-electron wave functions with radial components determined in this way are called Slater orbitals .
The shielding constant and the effective quantum number are determined as follows:
- Electron shells with principal quantum numbers greater than n are not taken into account.
- Each additional electron with the same n contributes 0.35 (but only 0.3 for n = 1).
- Each electron in shell n - 1 contributes to :
- for secondary quantum numbers l = 0 (s subshell) and l = 1 (p subshell): 0.85 each
- for secondary quantum numbers l = 2 (d subshell) and l = 3 (f subshell): 1.0 each.
- 4. All electrons from even deeper shells make a contribution of 1.0.
The following table follows:
To the quantum defect .
As part of the Sommerfeld atomic model, the orbital degeneration , i.e. the energy equality of states of the same principal quantum number n but different angular momentum quantum number l, is eliminated by the shielding, since the orbits of different angular momentum quantum numbers are subject to different shields.
- Shielding for spectrum, lexicon of physics