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Tin atoms have 50 electrons and the shell structure is 2.8.18.18.4.

The ground state electron configuration of ground state gaseous neutral tin is [Kr].4d10.5s2.5p2 and the term symbol is 3P0.

Kossel shell structure of tin
Schematic electronic configuration of tin.
Kossel shell structure of tin
The Kossel shell structure of tin.

Atomic spectrum

A representation of the atomic spectrum of tin.

Ionisation Energies and electron affinity

The electron affinity of tin is 107.3 kJ mol‑1. The ionisation energies of tin are given below.

Ionisation energies of tin
Ionisation energy number Enthalpy / kJ mol‑1
1st 708.58
2nd 1411.88
3rd 2943.4
4th 3931
5th 7432
6th 9070
7th 10890
8th 13030
9th 15050
10th 17750
11th 20070
12th 22380 (calculated)
13th 24900
14th 27200
15th 36600
16th 39300
17th 42200
18th 45000
19th 48800
20th 51800
21st 58700
Ionisation energies of tin
Ionisation energies of tin.
(追記) (追記ここまで)

Effective Nuclear Charges

The following are "Clementi-Raimondi" effective nuclear charges, Zeff. Follow the hyperlinks for more details and for graphs in various formats.

Effective nuclear charges for tin
1s 48.99
2s 36.86 2p 45.89
3s 32.42 3p 32.35 3d 35.74
4s 22.66 4p 21.27 4d 17.97 4f (no data)
5s 10.63 5p 9.10 5d (no data)
6s (no data) 6p (no data)
7s

References

These effective nuclear charges, Zeff, are adapted from the following references:

  1. E. Clementi and D.L.Raimondi, J. Chem. Phys. 1963, 38, 2686.
  2. E. Clementi, D.L.Raimondi, and W.P. Reinhardt, J. Chem. Phys. 1967, 47, 1300.

Electron binding energies

Electron binding energies for tin. All values of electron binding energies are given in eV. The binding energies are quoted relative to the vacuum level for rare gases and H2, N2, O2, F2, and Cl2 molecules; relative to the Fermi level for metals; and relative to the top of the valence band for semiconductors.
Label Orbital eV [literature reference]
K 1s 29200 [1]
L I2s 4465 [1]
L II2p1/2 4156 [1]
L III2p3/2 3929 [1]
M I3s 884.7 [3]
M II3p1/2 756.5 [3]
M III3p3/2 714.6 [3]
M IV3d3/2 493.2 [3]
M V3d5/2 484.9 [3]
N I4s 137.1 [3]
N II4p1/2 83.6 [3, one-particle approximation not valid owing to short core-hole lifetime]
N III4p3/2 83.6 [3, one-particle approximation not valid owing to short core-hole lifetime]
N IV4d3/2 24.9 [3]
N V4d5/2 23.9 [3]

Notes

I am grateful to Gwyn Williams (Jefferson Laboratory, Virginia, USA) who provided the electron binding energy data. The data are adapted from references 1-3. They are tabulated elsewhere on the WWW (reference 4) and in paper form (reference 5).

References

  1. J. A. Bearden and A. F. Burr, "Reevaluation of X-Ray Atomic Energy Levels," Rev. Mod. Phys., 1967, 39, 125.
  2. M. Cardona and L. Ley, Eds., Photoemission in Solids I: General Principles (Springer-Verlag, Berlin) with additional corrections, 1978.
  3. Gwyn Williams WWW table of values
  4. D.R. Lide, (Ed.) in Chemical Rubber Company handbook of chemistry and physics , CRC Press, Boca Raton, Florida, USA, 81st edition, 2000.
  5. J. C. Fuggle and N. Mårtensson, "Core-Level Binding Energies in Metals," J. Electron Spectrosc. Relat. Phenom., 1980, 21, 275.

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