Two Particles' Spin Hamiltonian Analysis?

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SUMMARY

The discussion focuses on the analysis of the Hamiltonian for two particles' spin, specifically defined as H = (S_{1z} + S_{2z}) + S_{1x}S_{2x}. The eigenvalues identified are ±ħ/2 and 0, with the basis states being |++⟩, |+-⟩, |−+⟩, and |--⟩. The user inquires about the orthogonality of the states |−+⟩ and |+-⟩, and whether the Hamiltonian's eigenvalues correspond to the basis states. The response clarifies that the states are indeed orthogonal and corrects the misunderstanding regarding the action of the spin operators on the basis kets.

PREREQUISITES
  • Understanding of bra-ket notation in quantum mechanics
  • Familiarity with spin operators S_{z} and S_{x}
  • Knowledge of Hamiltonian mechanics in quantum systems
  • Concept of orthogonality in quantum states
NEXT STEPS
  • Study the derivation of Hamiltonians in quantum mechanics
  • Learn about the implications of orthogonality in quantum states
  • Explore the role of spin operators in quantum mechanics
  • Investigate degenerate eigenvalues and their physical significance
USEFUL FOR

Students and researchers in quantum mechanics, particularly those studying spin systems and Hamiltonian analysis, will benefit from this discussion.

cacofolius
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Homework Statement


Hi, I'm trying to familiarize with the bra-ket notation and quantum mechanics. I have to find the hamiltonian's eigenvalues and eigenstates.

##H=(S_{1z}+S_{2z})+S_{1x}S_{2x}##

Homework Equations


##S_{z} \vert+\rangle =\hbar/2\vert+\rangle##

##S_{z}\vert-\rangle =-\hbar/2\vert-\rangle ##

##S_{x} \vert+\rangle =\hbar/2\vert-\rangle##

##S_{x} \vert-\rangle =\hbar/2\vert+\rangle, ##

The states basis is ##\vert++\rangle,\vert+-\rangle, \vert-+\rangle, \vert--\rangle ##

3. The Attempt at a Solution


What I did was apply the hamiltonian to each basis ket

##H\vert++\rangle =(S_{1z}+S_{2z})\vert++\rangle + S_{1x}S_{2x}\vert++\rangle
= \hbar/2\vert++\rangle + \hbar/2\vert++\rangle + \hbar/2\vert-+\rangle . \hbar/2\vert+-\rangle = \hbar/2\vert++\rangle##

##H\vert+-\rangle = 0##

##H\vert-+\rangle = 0##

##H\vert--\rangle = -\hbar/2\vert--\rangle##

My questions:
1) Is it right to consider ##\vert-+\rangle . \vert+-\rangle = 0##, (since they're orthogonal states)? Because they're both ket vectors (unlike the more familiar ##<a|b>##).

2) In that case, is the basis also the hamiltonian's, with eigenvalues ##\hbar/2, -\hbar/2, 0## (degenerate) ?
 
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Post this in the advanced physics homework section
 
cacofolius said:
Is it right to consider |−+⟩.|+−⟩=0\vert-+\rangle . \vert+-\rangle = 0,
No, that's not right. Moreover, ## S_{1x}S_{2x}|++\rangle \neq \hbar/2\vert-+\rangle . \hbar/2\vert+-\rangle ##. It's like you are producing four electrons out of two electrons. The operator of the first particle only acts on the first entry of the ket and that of the second particle acts on the second entry.
 

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