AB¼C where C¼
c 1
c 2
Ais the coefficients matrix,Bis the unknowns matrix, andCis the constants
matrix. Now, if we can find a matrixA"^1 such thatA"^1 AB¼B(analogous to the
numbersa"^1 ab¼b) then
A"^1 AB¼A"^1 C i.e: B¼A"^1 C
Thus the unknowns matrix is simply the inverse of the coefficients matrix times
the constants matrix. Note that we multiplied byA"^1 on the left (A"^1 AB¼A"^1 C),
which is not the same as multiplying on the right, which would giveABA"^1 ¼
CA"^1 ; this is not necessarily the same asB.
To see that a matrix can act as an operator consider the vector from the origin to
the pointP(3,4). This can be written as a column matrix, and multiplying it by the
rotation matrix shown transforms it (rotates it) into another matrix:
vector
new, rotated
vector
x
y
x
y
3
4 –4
3
0
1
multiply on the left
by rotation matrix
0
–1
4.3.3.4 Some Important Kinds of Matrices
These matrices are particularly important in computational chemistry:
- The zero matrix (the null matrix)
- Diagonal matrices
- The unit matrix (the identity matrix)
- The inverse of another matrix
- Symmetric matrices
- The transpose of another matrix
- Orthogonal matrices
- The zero matrix or null matrix, 0 , is any matrix with all its elements zero.
Examples:
00
00
000
000
ðÞ 0000
Clearly, multiplication by the zero matrix (when the (a&b)(b&c) mnemonic
permits multiplication) gives a zero matrix.
112 4 Introduction to Quantum Mechanics in Computational Chemistry