2 spin 1/2 particles in magnetic field

In summary, the student is having trouble solving the Hamiltonian for two particles. He has identified that he needs to solve for the total spin operator and has attempted to do so, but is not sure how to do so. He has also identified that he needs to solve for a non-diagonal entry in his basis states, and has given a hint as to which one to check.
  • #1
oww
2
0

Homework Statement


See pdf file: http://www.2shared.com/file/3469465/52e02653/q3_online.html

Its the third problem I'm having trouble with. I'm pretty sure I have the two first questions correct.

Homework Equations


1)[tex]H^{'}_{\uparrow\downarrow,\downarrow\uparrow}=<\left|\uparrow\downarrow\right\rangle\left|H^'\right|\left|\downarrow\uparrow\right\rangle[/tex]

The Attempt at a Solution



My idea was to compute the quantity given by 1), but I am not sure how to manage [tex]H^{'} =-\beta S^{(1)}.S^{(2)}=-\beta(S_x ^{(1)}S_x ^{(2)},S_y ^{(1)}S_y ^{(2)},S_z ^{(1)}S_z ^{(2)}) [/tex]

Should I try and find [tex]S_y ^{(1)}[/tex], [tex]S_y ^{(2)}[/tex] and the same for the z-spinor matrices. Or is there a smarter way of doing this?

Looking forward to all the help i can get. Oistein
 
Last edited:
Physics news on Phys.org
  • #2
You've written

[tex]H^{single-quote} =-\beta S^{(1)}.S^{(2)}=-\beta(S_x ^{(1)}S_x ^{(2)},S_y ^{(1)}S_y ^{(2)},S_z ^{(1)}S_z ^{(2)}) [/tex]

which you appear to have written as a vector, which it isn't:

[tex]\mathcal{H} = - \beta \mathbf{S}_1 \cdot \mathbf{S}_2 = -\beta \left[S_{x1}S_{x2} + S_{y1}S_{y2} + S_{z1}S_{z2}\right][/tex]

Now, you might not want to solve the hamiltonian in that form. Instead, look at:

[tex](\mathbf{S}_1 + \mathbf{S}_2)^2 = S_1^2 + S_2^2 + 2\mathbf{S}_1 \cdot \mathbf{S}_2[/tex]

Solve for the dot product and substitute that into the Hamiltonian. Having done that, your hamiltonian is expressed in terms of the total spin operator and the spin operators for particle 1 and particle two. These last two are proportional to the Pauli spin matrices, and you should know that [itex]\mathbf{\sigma}^2 = 1[/itex], so S_1^2 and S_2^2 just evaluate to the square of the proportionality factors. So, the only operator whose value you don't know before acting on it with your states to get the matrix element is the total spin operator.
 
Last edited:
  • #3
Blah, time limit to edit has expired before I was finished editing. What's left to say is that your matrix is 4x4, so to show that the hamiltonian is non-diagonal in your basis states, you just need to find a non-zero non-diagonal entry. The problem seems to tell you which element to check. Do that and you should be done.
 

FAQ: 2 spin 1/2 particles in magnetic field

How do spin 1/2 particles behave in a magnetic field?

Spin 1/2 particles, also known as fermions, have intrinsic angular momentum and behave like tiny magnets in a magnetic field. They align either parallel or anti-parallel to the field, depending on their spin orientation.

What is the significance of the number 2 in "2 spin 1/2 particles"?

The number 2 represents the number of spin states that a spin 1/2 particle can have. This is because spin 1/2 particles can have two possible spin orientations: up or down.

How does the magnetic field affect the energy levels of spin 1/2 particles?

The presence of a magnetic field causes the energy levels of spin 1/2 particles to split into two levels, known as the Zeeman effect. This is due to the interaction between the magnetic moment of the particles and the magnetic field.

Can spin 1/2 particles change their spin orientation in a magnetic field?

No, according to the laws of quantum mechanics, spin 1/2 particles cannot change their spin orientation in a magnetic field. They can only align either parallel or anti-parallel to the field.

How is the behavior of spin 1/2 particles in a magnetic field important in technology?

The behavior of spin 1/2 particles in a magnetic field is crucial for technologies such as magnetic resonance imaging (MRI) and magnetic storage devices. These technologies rely on the ability to manipulate and detect the spin orientation of particles in a magnetic field.

Similar threads

Back
Top