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The Entropy Reduction Laboratory

Double-Shell PSE: occupied electronic states of elements

f
 19
 20
 21
 22
 23
 24
 25
 26
 27
 28
 29
 30
 31
 32
 . 
 . 
 . 
 . 
 . 
 . 
 . 
 . 
 . 
 . 
 . 
 . 
 . 
 . 
 89
---
 90
---
 91
---
 92
---
 93
---
 94
---
 95
---
 96
---
 97
---
 98
---
 99
---
100
---
101
---
102
---
 57
---
 58
---
 59
---
 60
---
 61
---
 62
---
 63
---
 64
---
 65
---
 66
---
 67
---
 68
---
 69
---
 70
---


Legend:
 -O-
occupied electronic states
 ---
empty electronic states
Nucleus atomic nucleus with Z=32 protons (Germanium)
d
 3 
 4 
 5 
 6 
 7 
 8 
 9 
 10
 11
 12
 3B
 4B
 5B
 6B
 7B
 8B
 8B
 8B
 1B
 2B
103
---
104
---
105
---
106
---
107
---
108
---
109
---
110
---
111
---
112
---
 71
---
 72
---
 73
---
 74
---
 75
---
 76
---
 77
---
 78
---
 79
---
 80
---
 39
---
 40
---
 41
---
 42
---
 43
---
 44
---
 45
---
 46
---
 47
---
 48
---
 21
-O-
 22
-O-
 23
-O-
 24
-O-
 25
-O-
 26
-O-
 27
-O-
 28
-O-
 29
-O-
 30
-O-
p
 13
 14
 15
 16
 17
 18
 3A
 4A
 5A
 6A
 7A
 8A
113
---
114
---
115
---
116
---
117
---
118
---
 81
---
 82
---
 83
---
 84
---
 85
---
 86
---
 49
---
 50
---
 51
---
 52
---
 53
---
 54
---
 31
-O-
 32
-O-
 33
---
 34
---
 35
---
 36
---
 13
-O-
 14
-O-
 15
-O-
 16
-O-
 17
-O-
 18
-O-
 5 
-O-
 6 
-O-
 7 
-O-
 8 
-O-
 9 
-O-
 10
-O-
s
 1 
 2 
 1A
 2A
119
---
120
---
 87
---
 88
---
 55
---
 56
---
 37
---
 38
---
 19
-O-
 20
-O-
 11
-O-
 12
-O-
 3 
-O-
 4 
-O-
 1 
-O-
 2 
-O-
Nucleus
 
 
 
 
 
 3
 
 
 
 2
 
 
 
 1
 
 
 
 0
 
The
table
    This Table of occupied and unoccupied states of elements demonstrates the Build up Principle of the Double-Shell Periodic System of Elements (PSE). - To be definite, there are shown the occupied states for element 32, Germanium.

    The characteristics of the table (independent on the specific example) are:

  1. Columns connected to the various chemical groups are numbered according to the new (1, 2, ... 32) and old (1A, 2A, ... 8B) system of IUPAC.
  2. At the right is seen the numbering 0, 1, 2, 3 of the double-shells. These numbers indicate at the same time the maximal angular momentum lmaxoccuring in the respective double-shell.
  3. The letters s, p, d, f at the heads of the columns refer to the angular momenta l = 0, 1, 2, 3 of the boxes in the respective columns.
  4. As a consequence, the number of the boxes
    • in the double-shell #0 is 1 with lmax = 0
    • in the double-shell #1 is 2 with lmax = 1
    • in the double-shell #2 is 3 with lmax = 2
    • in the double-shell #3 is 4 with lmax = 3
    The total number of boxes up to the element 120 is 10.
  5. The lower halves of the double-shells are designated by the topical quantum number c = -1/2, the upper halves carry c = +1/2. This topical quantum number is not shown explicitly in the PSE table.
  6. The left halves of the boxes are designated by the spin quantum number s = -1/2, the right halves carry s = +1/2. This spin quantum number is not shown explicitly in the PSE table.

    Electronic states in the Double-Shell PSE are fourfold degenerate
Build up
principle
The build up (Aufbau) principle for this table is simple:
Starting from the bottom of the table, for each halve of a double shell, electrons start to occupy states of the highest angular momentum l = lmax and then proceed to states of lower angular momentum until l = 0.

In this presentation, the bottom of the table stands at the same time for the bottom of the potential well seen by the electrons. The positive charge of the nucleus provides the overall confinement of the core electrons and electric neutrality of the atom, but does not determine details of the elecronic structure. - For highly ionized atoms, the nuclear charge dominates and the build up prinziple becomes that of hydrogen.

Note This table is rather wide, for printing please use "landscape" format.
See also
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Last update of the page: Febr.10, 2003