Why Don't L2 and Ly Commute When L2 and Lx Do?

In summary, the conversation discusses the commutativity of operators in a spin-1/2 system and the relationship between their eigenbases. It is noted that the identity operator commutes with all other operators and shares an eigenbasis with them. However, it is also mentioned that two operators may have a common eigenbasis, but their commutativity does not guarantee a shared eigenbasis with a third operator. This is demonstrated in the example of the angular momentum operators, Lx and Ly, which have a common eigenbasis with L2, but do not commute with each other.
  • #1
dyn
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Hi.
To show that [ L2 , L+ ] uses the following commutators [ L2 , Lx ] = 0 and [ L2 , Ly ] = 0 . But if [ L2 , Lx ] = 0 this shows that L2 and Lx have simultaneous eigenstates ; but then should L2 and Ly not commute ?
Thanks
 
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  • #2
dyn said:
Hi.
To show that [ L2 , L+ ] uses the following commutators [ L2 , Lx ] = 0 and [ L2 , Ly ] = 0 . But if [ L2 , Lx ] = 0 this shows that L2 and Lx have simultaneous eigenstates ; but then should L2 and Ly not commute ?
Thanks
No. If A and B commute so have a common eigenbasis and B and C commute so have a different common eigenbasis, it does not follow that A and C commute and have a common eigenbasis.
 
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  • #3
Thanks. So L2 and Lx have a common eigenbasis as the 2 operators commute and L2 and Ly have a different common eigenbasis. But as Lx and Ly do not commute these 2 sets of eigenbases can never be the same ?
 
  • #4
dyn said:
Thanks. So L2 and Lx have a common eigenbasis as the 2 operators commute and L2 and Ly have a different common eigenbasis. But as Lx and Ly do not commute these 2 sets of eigenbases can never be the same ?

A spin-1/2 system is useful because the operators are simple 2x2 matrices. I suggest you work through this example for these AM operators.

Note that the identity operator, ##I##, commutes with everything (and every vector is an eigenvector of ##I##). So, ##I## has a shared eigenbasis with all operators that have an eigenbasis (such as Hermitian operators).
 

Related to Why Don't L2 and Ly Commute When L2 and Lx Do?

1. What is angular momentum commutator?

Angular momentum commutator is a mathematical tool used to calculate the relationship between two angular momentum operators. It represents the difference between the product of two angular momentum operators and the product of the same operators in reverse order.

2. Why is angular momentum commutator important in quantum mechanics?

Angular momentum commutator is important in quantum mechanics because it helps us understand the behavior of particles at the atomic and subatomic level. It allows us to predict the outcomes of measurements and determine the state of a quantum system.

3. How is angular momentum commutator calculated?

The angular momentum commutator is calculated using the commutator formula [A, B] = AB - BA, where A and B are angular momentum operators. This formula gives the difference between the product of the two operators and the product in reverse order.

4. What is the physical interpretation of the angular momentum commutator?

The physical interpretation of the angular momentum commutator is that it represents the uncertainty in measuring the angular momentum of a particle. A smaller commutator value indicates a more certain measurement, while a larger commutator value indicates a more uncertain measurement.

5. How does the angular momentum commutator affect the behavior of quantum particles?

The angular momentum commutator affects the behavior of quantum particles by determining the possible values of angular momentum that can be measured. It also plays a crucial role in the Heisenberg uncertainty principle, which states that the more precisely we know the angular momentum of a particle, the less precisely we can know its position, and vice versa.

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