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Interlude: The Legendre Previous: The
Legendre Polynomials
The Spherical Harmonics,
, that are conventionally used are:
which is valid for
, while the eigenfunctions corresponding to negative values of m
are obtained from:
The functions
are the associated Legendre polynomials defined by:
which is valid for
, and the values for negative m given by:
(Remember
). truein
When m=0, (79) simplifies to a value
independent of the azimuthal angle
where
are the Legendre polynomials.
At the poles
and
the azimuthal angle
are indistinguishable so
cannot depend on
at these angles. Therefore the only non-zero spherical harmonics for these
two cases has to have m=0 i.e.
and
Consider two arbitrary directions in space defined respectively by the
angles
and
and call the angle between them
. The Spherical Harmonic Addition Theorem states that
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where
stands for the smaller of the two distances
and
, and
is the larger of the two distances. truein
Note that the
form a complete set of orthonormal functions, i.e.
and
This means that any function of
and
can be expanded as follows:
where
Furthermore, if
is the angular wavefunction of some state, normalised such that
then the
are the probabilities that simultaneous measurement of
and
on the state described by
yields
and
respectively.
In the Dirac notation, an arbitrary state
can be expanded as:
where with the help of the orthonormality condition
we get
These eigenstates are also complete so:
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calculate the matrix representation of
and
for the AM state 3/2. Check that the commutation relations hold.
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Find the eigenvalues of
if (a) the AM of the system is 1, (b) the AM of the system is 2.
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