Clebsch-Gordan Coefficients
Clebsch-Gordan Coefficients
This Demonstration illustrates the Clebsch–Gordan coefficients, , which give the coupling amplitudes between uncoupled and coupled representations of two angular momenta and . In the uncoupled representation, the components of each angular momentum, and , are known; in the coupled representation, the total (resultant) angular momentum and its component are known. The Clebsch–Gordan coefficients are only nonzero when and ; in the Demonstration we show these for ,≤3. The graphs give a vectorial representation of each pair, showing the actual value together with all possible values.
〈|JM〉
j
1
j
2
m
1
m
2
j
1
j
2
j
1
j
2
z
m
1
m
2
J
z
M
M+
m
1
m
2
max(M,-)≤J≤+
j
1
j
2
j
1
j
2
j
1
j
2
(j,m)
m
Details
Details
In quantum mechanics, angular momentum is quantized in units of . The allowed values are specified by the quantum number ; for a given , the corresponding total angular momentum has value . In addition, one Cartesian component—conventionally the component—can also be specified, and can take on values where . The other two components , cannot be specified individually, which is a manifestation of the uncertainty principle.
ℏ
j=1/2,1,3/2,2,…
j
j=
j(j+1)
ℏz
=mℏ
j
z
m=-j,-j+1,…,j
j
x
j
y
The Clebsch–Gordan coefficients arise in systems comprising two angular momenta, and . It is possible to define either states with well-defined individual components and (the uncoupled representation), or well-defined total angular momentum and its component (the coupled representation). Allowed values in the coupled representation are and . The amplitudes relating the two representations are the Clebsch–Gordan coefficients .
j
1
j
2
z
m
1
m
2
J
z
M
J=-,-+1,…,+
j
1
j
2
j
1
j
2
j
1
j
2
M=-J,-J+1,…,J
〈|JM〉
j
1
j
2
m
1
m
2
j
1
j
2
External Links
External Links
Permanent Citation
Permanent Citation
Peter Falloon
"Clebsch-Gordan Coefficients"
http://demonstrations.wolfram.com/ClebschGordanCoefficients/
Wolfram Demonstrations Project
Published: March 7, 2011