496 Chapter 17Determinants
*The wave function of a system of bosons is totally symmetric, and the interchange of the coordinates of any
pair of identical bosons leaves the wave function unchanged.
functions. The electron is a member of the class of particles called fermions, particles
with half-integral spin (a particle with zero or integral spin is call a boson). The wave
function of a system of identical fermions is totally antisymmetric with respect to
the interchange of the coordinates (including spin) of the fermions; that is, the
interchange of the coordinates of any pair of fermions results in the change of sign
of the wave function.*This is just the property of an alternating function. Thus, if
the functionsf
1
,f
2
, =,f
n
in the determinant (17.54) represent the occupied states of
the nelectrons of a system, and ifx
1
, 1 x
2
,1=, 1 x
n
represent the nsets of coordinates
(including spin) of the electrons, then the functions are called spin-orbitals and the
determinant (17.54) is called a Slater determinant. Because the Slater determinant is
antisymmetric, the interchange (of the coordinates and spin) of any pair of electrons
results in a change of sign of the determinant. If two of the functions (spin-orbitals)
are the same then two rows of the determinant are equal and the determinant is zero.
This is an expression of the Pauli exclusion principle, that no two electrons can be in
the same state (spin-orbital).
17.8 Exercises
Section 17.1
1.Use determinants to solve the pair of equations
4 x 1 + 1 y 1 = 111
3 x 1 + 12 y 1 = 112
Evaluate:
Section 17.2
- Use determinants to solve the equations
x 1 + 1 y 1 + 1 z 1 = 16
x 1 + 12 y 1 + 13 z 1 = 114
x 1 + 14 y 1 + 19 z 1 = 136
Evaluate the determinants by expansion along (i)the first row, (ii)the second column:
- (i)Find the cofactors of all the elements of
(ii)Confirm that the same value of the determinant is obtained by expansion along every
row and every column
123
201
111
−
−
032
201
260
132
012
004
−
−
111
110
112
−
−
235
012
341
cos sin
sin cos
nn
nn
θθ
θθ
01 −
− 23
20
03