Understanding Basis Choices in Quantum Mechanics

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In summary, the conversation discusses a problem involving hyperfine interaction between two spin 1 particles and determining the corresponding columns of the Hamiltonian matrix. The question is whether these columns can be chosen arbitrarily and the concern is that without a clear way to distinguish between them, the experiment may become problematic. It is mentioned that the choice of basis may be arbitrary and that the numbers used to describe eigenstates may no longer be applicable in the case of hyperfine interaction. The individual clarifies their question and acknowledges that it can be easily answered.
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Homework Statement


Alright, so this is not exactly a guided homework question. It is a rather intricate problem consisting of many steps, but one of these steps comes down to working out the hyperfine interaction between two spin 1 particles, from a hamiltonian point of view. From what I have been given, in this particular setup it can be simplified to the equation below:

Homework Equations


[itex]H = A S_{z}⊗I_{z}[/itex]

where S and Z are angular momentum operators corresponding to the Z axis.

The Attempt at a Solution


Alright, so my problem is how I go about knowing which column of each matrix correspons to what. Does the first column correspond to the spin being 0, 1 or -1, basically. I have illustrated my question with the picture below, working out a specific case, where I indicate the spin of the first particle by mS and the spin of the second particle by mI. The reason for why the ordering is important to me is because I want to perform an experiment in which I have to be able to distinguish between the second particle being spin 1, 0 or -1, and the only way I can think of doing so in my specific setup is if I know which values of the hamiltonian correspond to which combination of (spin particle 1, spin particle 2)

2z6zbqa.jpg


Somehow I seem to remember that this choice of basis is arbitrary, which means that no specific one corresponds to spin 1, 0, or -1. This would be problematic, as I need a clear way to distinguish them from one another.

Edit: I understand that my question is a bit vague. It basically boils down to if the numbers I put under the matrix are set, or if they can be chosen arbitrarily.
 
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I don't understand where you are going with this. By if you have hyperfine interaction, then ##m_S## and ##m_I## are no longer good quantum numbers and cannot be used to describe eigenstates of the system.
 
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Hmm. Well, I suppose I should have added more context, as looking back at it it is indeed not clear at all what I am trying to say. In the end my question boiled down to which eigenvectors corresponded to what columns of the pauli matrices for a spin 1 particle, which is easily answered. But thank you for giving my question some thought, and I apologize for wasting your time!
 

FAQ: Understanding Basis Choices in Quantum Mechanics

What is a basis and why is it important?

A basis is a set of linearly independent vectors that span a vector space. It is important because it provides a framework for representing and manipulating vectors in a vector space.

How do I know which basis to choose?

The choice of basis depends on the specific problem being solved. It is often helpful to choose a basis that is aligned with the problem's underlying structure or symmetry.

Can I choose any set of vectors as a basis?

No, a basis must meet two criteria: linear independence and span. This means that the vectors must be independent of each other and must be able to generate all possible vectors in the vector space.

What are some common bases used in mathematics and science?

Some common bases include the standard basis (i.e. the unit vectors), the natural basis (i.e. the basis of eigenvectors), and the Fourier basis (i.e. the basis of sinusoidal functions).

Are there any techniques for choosing a good basis?

Yes, there are various techniques such as Gram-Schmidt orthogonalization and principal component analysis that can help in choosing a good basis for a specific problem.

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