Understanding the Connection between Dirac Four Spinor and Spin Up

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Discussion Overview

The discussion explores the relationship between the Dirac four spinor and the concept of "spin up," questioning whether they are connected or separate entities. Participants delve into the implications of using the Dirac four spinor in relativistic calculations, particularly in the context of quantum states of the electron in hydrogen.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants assert that there is a connection between the Dirac four spinor and "spin up," suggesting that one of the components can represent the up-component of the electron or positron.
  • Others propose that the Dirac four spinor can be used in relativistic calculations of quantum states, referencing Penrose's work which describes the electron using the four spinor.
  • It is noted that the four solutions of the Dirac Equation do not correspond one-to-one with the four components of the spinor, as each solution involves all four components.
  • Participants discuss the coupling of two-spinors within the Dirac Equation and the implications for bound states in hydrogen, indicating that all four components are involved in the solution.
  • Questions are raised about the association of "spin up" with the spinors and whether interpretations can be made regarding the two-spinor Ψ1.
  • In the nonrelativistic limit, some participants describe how the relationship between the two-spinors leads to an approximation that resembles the Schrödinger-Pauli Equation.

Areas of Agreement / Disagreement

Participants express differing views on the connection between the Dirac four spinor and "spin up," with some asserting a link while others question the validity of such an association. The discussion remains unresolved regarding the implications of these interpretations and the role of the spinors in calculations.

Contextual Notes

Limitations include the dependence on specific interpretations of the Dirac spinor and the conditions under which the nonrelativistic limit is applied. The discussion also highlights the complexity of associating spin states with the components of the spinor.

galvin452
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Is there a connection between the Dirac four spinor and "spin up", i.e one of the four spinor states is spin up or are these two separate unconected things.
 
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Yes there is a connection - depending on how you write the spinor, one of the four components can be interpreted as the up-component of the electron, one as the up-component of the positron (the other two are the down components).
 
Sonderval said:
Yes there is a connection - depending on how you write the spinor, one of the four components can be interpreted as the up-component of the electron, one as the up-component of the positron (the other two are the down components).

Can't one use all of the Dirac four spinor in relativistic calculation of, e.g. the quantum states of the electron in hydrogen? Penrose in `The Road to Reality' (pg 629) specifically uses the four spinor to describe the electron only.
 
galvin452 said:
Can't one use all of the Dirac four spinor in relativistic calculation of, e.g. the quantum states of the electron in hydrogen? Penrose in `The Road to Reality' (pg 629) specifically uses the four spinor to describe the electron only.

Since the four spinor can be associated with only the electron, then if one associate a "spin up" state with one of the spinors what does one associate with the other three spinors?
 
galvin452 said:
Can't one use all of the Dirac four spinor in relativistic calculation of, e.g. the quantum states of the electron in hydrogen? Penrose in `The Road to Reality' (pg 629) specifically uses the four spinor to describe the electron only.
The Dirac Equation has both positive frequency and negative frequency solutions. The negative frequency ones are sometimes interpreted as negative energy ("hole") states. But in the normal way of writing a four-spinor, the four solutions do not one-to-one correspond to the four components of the spinor. Each solution involves all four components.

If you write the four-spinor as a pair of two-spinors, Ψ1, Ψ2 and put this into the Dirac Equation, you find they are coupled together:

(E + eφ)Ψ1 = c σ·p Ψ2
(E + eφ + 2mc22 = c σ·p Ψ1
where E is kinetic plus potential energy (relativistic energy minus mc2) and φ is the electrostatic potential. Putting φ = e/r, you can solve this pair of equations to find the bound states of the hydrogen atom. As Penrose said, all four components of the spinor are involved in the solution.
 
Bill_K said:
The Dirac Equation has both positive frequency and negative frequency solutions. The negative frequency ones are sometimes interpreted as negative energy ("hole") states. But in the normal way of writing a four-spinor, the four solutions do not one-to-one correspond to the four components of the spinor. Each solution involves all four components.

If you write the four-spinor as a pair of two-spinors, Ψ1, Ψ2 and put this into the Dirac Equation, you find they are coupled together:

(E + eφ)Ψ1 = c σ·p Ψ2
(E + eφ + 2mc22 = c σ·p Ψ1
where E is kinetic plus potential energy (relativistic energy minus mc2) and φ is the electrostatic potential. Putting φ = e/r, you can solve this pair of equations to find the bound states of the hydrogen atom. As Penrose said, all four components of the spinor are involved in the solution.

Does this mean one can not associate a "spin up" with anyone of the spinors?
Is there any interpretaion of the two-spinor Ψ1?
 
galvin452 said:
Does this mean one can not associate a "spin up" with anyone of the spinors? Is there any interpretaion of the two-spinor Ψ1?
Yes, in the nonrelativistic limit. In the second equation, (E + eφ + 2mc22 = c σ·p Ψ1, the rest energy mc2 is the largest energy, so we can approximate

2mc2Ψ2 = c σ·p Ψ1 or Ψ2 = (σ·p/2mc) Ψ1

This shows that Ψ2 << Ψ1 in this limit. Consequently Ψ1 is called the "large" component and Ψ2 the "small" component. Furthermore, we can eliminate Ψ2 in the first equation, getting an (approximate) second-order equation:

E Ψ1 = (σ·p σ·p/2m + eφ) Ψ1

This is a direct generalization of the Schrödinger Equation for a particle having spin 1/2, and is known as the Schrödinger-Pauli Equation.
 

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