For every dimension , the orthogonal
group is the group
of orthogonal matrices. These matrices form a group because they are closed
under multiplication and taking inverses.
Thinking of a matrix as given by coordinate functions,
the set of matrices is identified with . The orthogonal
matrices are the solutions to the equations
 |
(1)
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where is the identity matrix, which are redundant. Only of these
are independent, leaving "free
variables." In fact, the orthogonal group is a smooth -dimensional
submanifold.
Because the orthogonal group is a group and a manifold, it is a Lie group. has a submanifold tangent space at the identity that is the Lie algebra of antisymmetric
matrices . In fact, the orthogonal group is
a compact Lie group.
The determinant of an orthogonal matrix is either 1 or , and so the orthogonal
group has two components. The component
containing the identity is the special
orthogonal group . For example, the group has group action on the plane that is a rotation:
![O(2)={[costheta -sintheta; sintheta costheta]} union {[-costheta sintheta; sintheta costheta]},](/images/equations/OrthogonalGroup/NumberedEquation2.gif) |
(2)
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where is any real number in . These matrices
preserve the quadratic form , and so they also preserve circles , which
are the group orbits.
As a manifold, consists of two disjoint copies of
the circle.
There are several generalizations of the orthogonal group. First, it is possible to define the orthogonal group for any symmetric
quadratic form with matrix signature . The group
of matrices which preserve , that is,
 |
(3)
|
is denoted . The Lorentz group is . For example,
the matrices
![A=[cosht sinht; sinht cosht]](/images/equations/OrthogonalGroup/NumberedEquation4.gif) |
(4)
|
are elements of . They preserve the quadratic form so they
preserve the hyperbolas .
Instead of using real numbers for the coefficients, it is possible to use coefficients from any field , in which case
it is denoted . The orthogonal matrices still
satisfy . For example, contains
![[11 15; 15 12],](/images/equations/OrthogonalGroup/NumberedEquation5.gif) |
(5)
|
and has 48 elements in total.
Of course, denotes the group of matrices
which preserve the symmetric
quadratic form of matrix signature , with coefficients in the field . When is not or , these are called
Lie-type groups.
When the coefficients are complex numbers, it is called the complex orthogonal group, which is much different from
the unitary group. For example,
matrices of the form
![A=[cosz -sinz; sinz cosz]](/images/equations/OrthogonalGroup/NumberedEquation6.gif) |
(6)
|
are in . In particular, is not compact. The equations defining in affine
space are polynomials of degree two. Consequently, is a linear algebraic group.
The numbers of subgroups of orders , 2, 3, ... in the orthogonal group are 1, 3, 1,
5, 1, 5, 1, 7, 1, 5, 1, 8, ... (Sloane's A001051), i.e., a repeating sequence of copies of with the
exceptions , , , , and .
This entry contributed by Todd Rowland
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