Antiferromagnetic/ferromagnetic coupling

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SUMMARY

Antiferromagnetic and ferromagnetic coupling are fundamental concepts in quantum magnetism, particularly relevant to two-level half-flux quantum systems, often modeled as spin 1/2 systems. The Heisenberg spin-exchange interaction, represented by the Heisenberg spin Hamiltonian H = ∑_{ij}J_{ij}S_i · S_j, defines these couplings. In antiferromagnetic systems, the coupling constant J is positive (J > 0), resulting in neighboring spins being opposite, while in ferromagnetic systems, J is negative (J < 0), leading to aligned spins. Understanding these interactions is crucial for studying the stability and energy states of quantum systems.

PREREQUISITES
  • Quantum magnetism principles
  • Heisenberg spin Hamiltonian formulation
  • Spin 1/2 system characteristics
  • Many-body physics approximations
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  • Explore the implications of the Heisenberg spin-exchange interaction in various quantum systems
  • Study the role of Coulomb and spin exchange terms in determining the coupling constant J
  • Investigate the stability conditions of quantum systems under antiferromagnetic and ferromagnetic couplings
  • Learn about advanced topics in solid state physics related to quantum magnetism
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Physicists, quantum mechanics researchers, and students studying solid state physics or quantum magnetism who seek to deepen their understanding of spin interactions and their implications in quantum systems.

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What is antiferromagnetic/ferromagnetic coupling, and what is the difference between the two? I'm referring to coupling between two two-level half-flux quantum systems for example.
 
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qubits said:
What is antiferromagnetic/ferromagnetic coupling, and what is the difference between the two? I'm referring to coupling between two two-level half-flux quantum systems for example.

I'm assuming what you meant by "half-flux quantum systems" is spin 1/2 systems.

First of all, this is a VERY difficult subject that falls into quantum magnetism. So I'm guessing you're asking this because you're studying either quantum magnetism, or solid state physics. If that is the case, then the "coupling" is the Heisenberg spin-exchange interaction, defined within the Heisenberg spin Hamiltonian as

H = \sum_{ij}J_{ij}\mathbold{S_i} \cdot \mathbold{S_j}

where J_{ij} is the Heisenberg coupling of nearest-neighbor spins. In a "simple" system (pay attention to that word), a ferromagnetic coupling implies that J < 0, whereas antiferromagnetic coupling means that J > 0. The exact determination of what J is for any given system is usually impossible to find exactly. This is where one has to make approximations within the many-body picture.

Zz.
 
Last edited:
In any physical system we are concerned with energy lowering that leads to stability of the system. So the hamiltonian that is presented above H=sum (ij) J(ij) S(i).S(j) is a simplestic one illustrating the fact.

1.For a antiferromagnetic system neighbouring spins are opposite (+1/2) and (-1/2) so J is +ve that leads to an overall -ve sign>>> means H= -ve ( ... ) this hamiltonian will have -ve eigen energy leading to a bound state.

2.For ferromagnetic spins are (+1/2) (+1/2) so by similar argument J should be -ve...

This hamiltonian is simple but it hides the actual physics. The J cointains Coulomb and spin exchange terms within it...
 

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