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Mathematical Methods for Physicists: A concise introduction - Site Map

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SYMMETRIC AND SKEW-SYMMETRIC MATRICES<br />

so that<br />

…AB† T ˆ B T A T<br />

q:e:d:<br />

Because of (3.15), even if ~ A ˆ ~A T and ~B ˆ ~B T , … ~ A ~B† T 6ˆ ~A ~B unless the matrices<br />

commute.<br />

Symmetric and skew-symmetric matrices<br />

A square matrix ~A ˆ…a jk † is said to be symmetric if all its elements satisfy the<br />

equations<br />

a kj ˆ a jk ;<br />

that is, ~A and its transpose are equal ~A ˆ ~A T . For example,<br />

0<br />

1<br />

1 5 7<br />

B<br />

C<br />

~A ˆ @ 5 3 4 A<br />

7 4 0<br />

…3:16†<br />

is a third-order symmetric matrix: the elements of the ith row equal the elements<br />

of ith column, <strong>for</strong> all i.<br />

On the other hand, if the elements of ~A satisfy the equations<br />

a kj ˆa jk ;<br />

…3:17†<br />

then ~A is said to be skew-symmetric, or antisymmetric. Thus, <strong>for</strong> a skew-symmetric<br />

~A, its transpose equals minus ~A: ~A T ˆ~A.<br />

Since the elements a jj along the principal diagonal satisfy the equations<br />

a jj ˆa jj , it is evident that they must all vanish. For example,<br />

0<br />

1<br />

0 2 5<br />

B<br />

C<br />

~A ˆ @ 2 0 1A<br />

5 1 0<br />

is a skew-symmetric matrix.<br />

Any real square matrix ~A may be expressed as the sum of a symmetric matrix ~R<br />

and a skew-symmetric matrix ~S, where<br />

~R ˆ 1<br />

2 … ~A ‡ ~A T † and ~S ˆ 1<br />

2 … ~A ~A T †: …3:18†<br />

Example 3.7<br />

The matrix<br />

<br />

~A ˆ 2 3 <br />

5 1<br />

may be written in the <strong>for</strong>m ~A ˆ ~R ‡ ~S, where<br />

~R ˆ 1<br />

<br />

2 … ~A ‡ ~A T †ˆ 2 4 <br />

4 1<br />

~S ˆ 1<br />

<br />

2 … ~A ~A T †ˆ 0 1<br />

1 0<br />

<br />

:<br />

109

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