Encyclopaedia Britannica, 11th Edition, "Groups, Theory of" to "Gwyniad": Volume 12, Slice 6Various
Science
Encyclopaedia Britannica, 11th Edition, "Groups, Theory of" to "Gwyniad": Volume 12, Slice 6
Various
Encyclopedias and dictionaries
The total number of permutations that can be performed on n symbols is
n!, and these necessarily constitute a group. It is known as the
_symmetric_ group of degree n, the only rational functions of the
symbols which are unaltered by all possible permutations being the
symmetric functions. When any permutation is carried out on the
product of the n(n - 1)/2, differences of the n symbols, it must
either remain unaltered or its sign must be changed. Those
permutations which leave the product unaltered constitute a group of
order n!/2, which is called the _alternating_ group of degree n; it is
a self-conjugate subgroup of the symmetric group. Except when n = 4
the alternating group is a simple group. A group of degree n, which is
not contained in the alternating group, must necessarily have a
self-conjugate subgroup of index 2, consisting of those of its
permutations which belong to the alternating group.
Groups of linear substitutions.
Among the various concrete forms in which a group of finite order can
be presented the most important is that of a group of linear
substitutions. Such groups have already been referred to in connexion
with discontinuous groups. Here the number of distinct substitutions
is necessarily finite; and to each operation S of a group G of finite
order there will correspond a linear substitution s, viz.
__j=m
x_i = \ s_(ij)x_j(i, j = 1, 2, ..., m),
/__j=1
on a set of m variables, such that if ST = U, then st = u. The linear
substitutions s, t, u, ... then constitute a group g with which G is
isomorphic; and whether the isomorphism is simple or multiple g is
said to give a "representation" of G as a group of linear
substitutions. If all the substitutions of g are transformed by the
same substitution on the m variables, the (in general) new group of
linear substitutions so constituted is said to be "equivalent" with g
as a representation of G; and two representations are called
"non-equivalent," or "distinct," when one is not capable of being
transformed into the other.
A group of linear substitutions on m variables is said to be
"reducible" when it is possible to choose m'(< m) linear functions of
the variables which are transformed among themselves by every
substitution of the group. When this cannot be done the group is
called "irreducible." It can be shown that a group of linear
substitutions, of finite order, is always either irreducible, or such
that the variables, when suitably chosen, may be divided into sets,
each set being irreducibly transformed among themselves. This being
so, it is clear that when the irreducible representations of a group
of finite order are known, all representations may be built up.
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