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Schwinger's Oscillator Model for Angular Momentum

n
a
0
1
2
3
n
b
0
1
2
3
In an internal Atomic Energy Commission document published in 1952 [1], Julian Schwinger developed the quantum theory of angular momentum from the commutation relations for a pair of independent harmonic oscillators. This work has since been subsequently quoted many times [2, 3]. A simplified version of the derivation is given in the Details. This Demonstration shows the angular momentum states
j
,
m
derived from the quantum numbers
n
a
,
n
b
for a pair of harmonic oscillators, with
n
a
,
n
b
=0,1,2,
.
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