Two spin-1 objects: Addition of Angular Momenta

In summary, the conversation discusses the probability of obtaining specific values of m when measuring the spin of object A in a container with two spin-1 objects. The solution involves finding the coupled state |2,1> in the uncoupled basis and using the restriction that j1+j2=2 and m1+m2=1 to determine the only possible values for m. The decomposition of the coupled state |2,1> in the uncoupled basis is |2,1> = c1|0,1> + c2|1,0>, where c1 and c2 are constants that can be solved for using the normalization condition. This leads to the probabilities of 1/2 for m=0 and
  • #1
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Homework Statement



Suppose in a container there are two spin-1 objects, A and B. It is found that ##J=j_1+j_22## and ##M=m_1+m_2=1##. What is the probability when ##J_z## is measured for A, values of m=0, m=-1 and m=+1 will be obtained?

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Homework Equations


The Attempt at a Solution



[tex]|j,j> = |2,2> = |(1,1)_A>|(1,1)_B>[/tex]

Starting:
[tex]J_{-}|2,2> = \left(J_{-}^A + J_{-}^B\right)|(1,1)_A>|(1,1)_B>[/tex]
[tex]\sqrt{2(2+1)-2(2-1)}|2,1> = \sqrt{1(1+1)-1(1-1)}\left(|(1,0)_A>|(1,1)_B> + |(1,1)_A>|(1,0)_B>\right)[/tex]
[tex]|2,1> = \frac{1}{\sqrt{2}}\left(|(1,0)_A>|(1,1)_B> + |(1,1)_A>|(1,0)_B>\right)[/tex]

For m=0, probability = 1/2
For m=1, probability = 1/2
For m=-1, probability = 0

Is this right?
 
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  • #2
I would say yes, that is correct. So essentially you are writing the coupled state |2,1> in the uncoupled basis. Since j1+j2=1+1 = 2 = J and m1+m2=1, you know that the only possible values for the mi are 0 and 1, since any other combination does not give a sum of 1.

So the coupled state |J,M> decomposed in the uncoupled basis |j1j2m1m2> → |m1m2> would usually consist of 9 terms for fixed j1 and j2 both equal to 1. But by the above restriction, the only possibilities are |0,1> and |1,0>, as you found.

So the decomposition must be |2,1> = c1|0,1> + c2|1,0>. For normalized states, |c1|2+ |c2|2 = 1 => c1 = c2 = 1/√2.

Thought I would give a more descriptive solution, which helps in understanding what you are actually doing.
 
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Related to Two spin-1 objects: Addition of Angular Momenta

1. What is the concept of spin in quantum mechanics?

Spin is an intrinsic property of subatomic particles, such as electrons and protons, that gives them a characteristic angular momentum. It is not the physical rotation of the particle, but rather a quantum mechanical property that describes its orientation and behavior in a magnetic field.

2. How does the addition of angular momenta in two spin-1 objects work?

In quantum mechanics, the total angular momentum of a system is the sum of the individual angular momenta of its components. In the case of two spin-1 objects, the addition of their angular momenta follows certain rules and results in a combined angular momentum that can take on discrete values.

3. What is the significance of the spin-1 quantum number in two spin-1 objects?

The spin-1 quantum number, also known as the spin projection quantum number, determines the possible orientations of the individual spin-1 objects. It plays a crucial role in the addition of angular momenta, as the combined angular momentum can only take on values based on the spin-1 quantum numbers of the individual objects.

4. What are the implications of the addition of angular momenta in quantum systems?

The addition of angular momenta is a fundamental concept in quantum mechanics that has important implications in various systems, such as atoms, molecules, and nuclei. It helps explain the behavior of these systems and provides insight into their properties and interactions.

5. How is the addition of angular momenta experimentally observed?

The addition of angular momenta can be observed experimentally through various techniques, such as spectroscopy and scattering experiments. These methods involve measuring the energy levels or scattering patterns of the system, which can provide information about the total angular momentum and its components.

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