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Irreducible Representation


An irreducible representation of a group is a nonzero group representation that has no nontrivial invariant subspaces. For example, the orthogonal group O(n) has an irreducible representation on R^n.

Every finite-dimensional complex group representation of a finite group or a connected semisimple Lie group breaks up into a direct sum of irreducible representations. But in general, this is not the case, e.g., (R,+) has a group representation on R^2 by

 phi(a)=[1 a; 0 1],
(1)

i.e., phi(a)(x,y)=(x+ay,y). But the subspace y=0 is fixed, hence phi is not irreducible, but there is no complementary invariant subspace.

The irreducible representation has a number of remarkable properties, as formalized in the group orthogonality theorem. For a finite group with complex irreducible realizations by unitary transformations, let the group order be h, and the dimension of the ith group representation (the order of each constituent matrix) be l_i (a positive integer). Let any group element be denoted R, and let the mth row and nth column of the matrix corresponding to the group element R in the ith irreducible representation be Gamma_i(R)_(mn). The following properties can be derived from the group orthogonality theorem,

 sum_(R)Gamma_i(R)_(mn)Gamma_j(R)_(m^'n^')^*=h/(sqrt(l_il_j))delta_(ij)delta_(mm^')delta_(nn^').
(2)

1. The dimensionality theorem:

 h=sum_(i)l_i^2=l_1^2+l_2^2+l_3^2+...=sum_(i)chi_i^2(I),
(3)

where each l_i must be a positive integer and chi is the group character (trace) of the group representation.

2. The sum of the squared absolute values of the group characters in any irreducible representation i equals h,

 h=sum_(R)|chi_i(R)|^2.
(4)

3. orthogonality of different representations

 sum_(R)chi_i(R)chi_j(R)^_=0  for i!=j.
(5)

4. In a given group representation, reducible or irreducible, the group characters of all matrices belonging to group elements in the same conjugacy class are identical (group characters of different group representations can coincide on a particular conjugacy class).

5. The number of irreducible representations of a group is equal to the number of conjugacy classes in the group. This number is the size of the character table, while the dimensions l_i of the individual group representations may differ.

6. A one-dimensional group representation with all 1s (totally symmetric) will always exist for any group.

7. For a matrix group representation, the determinant gives a one-dimensional group representation. Its group character, the trace, is generally not a one-dimensional group representation.

8. The multiplicity a_i of the irreducible representation with group character chi_i in a reducible group representation with group character chi is

 a_i=1/hsum_(R in G)chi(R)chi_i(R)^_=1/hsum_(R in G)chi(R)chi_i(R^(-1)),
(6)

where h is the group order of the group G. Since group characters are constant on conjugacy classes, this may be written

 a_i=1/hsum_(C)n_Cchi(C)chi_i(C)^_,
(7)

where the sum is over the conjugacy classes C and n_C is the number of elements in C.

Irreducible representations can be indicated using mulliken symbols.


See also

Character Table, Finite Group, Group, Group Character, Group Orthogonality Theorem, Group Representation, Ito's Theorem, Lie Algebra Representation, Mulliken Symbols, Orthogonal Group Representations, Semisimple Lie Group, Unitary Transformation, Vector Space, Wedderburn's Theorem

Portions of this entry contributed by Todd Rowland

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References

James, G. D. and Liebeck, M. Representations and Characters of Groups, 2nd ed. Cambridge, England: Cambridge University Press, 2001.

Referenced on Wolfram|Alpha

Irreducible Representation

Cite this as:

Weisstein, Eric W., with contributions by Todd Rowland. "Irreducible Representation." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/IrreducibleRepresentation.html

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