Spin Angular Momentum Dirac Equation

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SUMMARY

The discussion centers on the spin angular momentum in the context of the Dirac equation, which features a wave-function represented by four components in a matrix form. Each component does not independently possess spin angular momentum of h-bar/2; rather, the spin operator intermixes these components, indicating that spin is a collective property of all four. The relationship between the phases of these components is crucial, especially when considering spin eigenstates. The Pauli equation serves as a simpler illustration, demonstrating how spin states can be represented with two components.

PREREQUISITES
  • Understanding of the Dirac equation and its matrix representation.
  • Familiarity with spin angular momentum and its mathematical implications.
  • Knowledge of the Pauli equation and its two-component wave function.
  • Basic concepts of quantum mechanics, particularly eigenstates and operators.
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  • Study the mathematical formulation of the Dirac equation and its implications for particle physics.
  • Explore the relationship between spin and orbital angular momentum in quantum mechanics.
  • Investigate the properties of spin eigenstates and their representation in quantum systems.
  • Learn about the applications of the Pauli equation in nonrelativistic quantum mechanics.
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Physicists, quantum mechanics students, and researchers interested in the foundational aspects of spin and angular momentum in relativistic quantum theories.

Bob Dylan
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In the Dirac equation, the wave-function is broken into four wave-functions in four entries in a column of a matrix. Since there are four separate versions of the wave-function, does each version have the spin angular momentum of h-bar/2? This seems overly simplistic. How does spin angular momentum work for the Dirac equation?
 
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Bob Dylan said:
In the Dirac equation, the wave-function is broken into four wave-functions in four entries in a column of a matrix. Since there are four separate versions of the wave-function, does each version have the spin angular momentum of h-bar/2? This seems overly simplistic. How does spin angular momentum work for the Dirac equation?

The spin operator mixes the components of the Dirac wave function, so it's not a property of anyone component, but of all 4. On the other hand, orbital angular momentum does not mix the components, so it makes sense to say that a single component has an orbital angular momentum, but not to say that it has spin angular momentum.
 
Does this mean all four components share the same phase?
 
Bob Dylan said:
Does this mean all four components share the same phase?

If a particle is in a spin eigenstate, then the phases of the components must be related.

It's easiest to see with the two-component nonrelativistic limit of the Dirac equation, the Pauli equation.

With the Pauli equation, the wave function has two components: ##\psi = \left( \begin{array} \\ \alpha \\ \beta \end{array} \right)##.

If ##\psi## is spin-up in the z-direction, that means ##\left( \begin{array} \\ 1 & 0 \\ 0 & -1 \end{array} \right)
\left( \begin{array} \\ \alpha \\ \beta \end{array} \right) = +1 \left( \begin{array} \\ \alpha \\ \beta \end{array} \right)##. That implies ##\beta = 0##.

If ##\psi## is spin-up in the x-direction, that means ##\left( \begin{array} \\ 0 & 1 \\ 1 & 0 \end{array} \right)
\left( \begin{array} \\ \alpha \\ \beta \end{array} \right) = +1 \left( \begin{array} \\ \alpha \\ \beta \end{array} \right)##. That implies ##\alpha = \beta##.
 
So is h-bar (or h-bar divided by 2) a form of spin or orbital angular momentum?
 

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