Who’s spin in the Einstein-Cartan theory? Source’s or test particle's?

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Discussion Overview

The discussion centers on the interpretation of "spin" within the context of the Einstein-Cartan theory, particularly whether it refers to the spin of the source or the spin of the test particle. Participants explore the implications of this distinction for understanding spin-orbit coupling and the differences between Einstein-Cartan theory and Gravitoelectromagnetism.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • One participant questions whether the spin in the Einstein-Cartan theory refers to the source's spin or the test particle's spin, drawing parallels to quantum mechanics and the spin-orbit interaction in hydrogen atoms.
  • Another participant notes the absence of Einstein-Cartan equations for the motion of spinning test particles, suggesting that the theory involves a "geodesic equation plus spin of the test particle" and emphasizes that the spin current acts as a source term for torsion.
  • A participant expresses confusion about how the Kerr metric, which describes rotating massive bodies, fits into the discussion, given that general relativity is said to be unable to model spin-orbit coupling.
  • It is mentioned that while general relativity can describe orbital angular momentum, it cannot account for intrinsic spin without employing the tetrad formalism, which introduces torsion and spin currents.

Areas of Agreement / Disagreement

Participants express differing views on the nature of spin in the Einstein-Cartan theory and its relationship to general relativity and Gravitoelectromagnetism. The discussion remains unresolved regarding the specific interpretation of spin and its implications.

Contextual Notes

There are limitations in the discussion regarding the assumptions made about the relationship between spin, torsion, and the equations governing motion in the Einstein-Cartan theory. The distinction between source and test particle spin is not clearly defined, leading to further questions about the applicability of existing metrics like the Kerr metric.

mings6
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Who’s “spin” is in the Einstein-Cartan theory? Source’s spin or the test particle’s spin?

I quantum mechanics, when we say spin orbit interaction, such as in hydrogen atom, it’s about the test particle's, the electron’s spin and the electron’s orbit interact to each other.

In the Einstein’s general relativity, with weak field condition, it can be described with Gravitoelectromagnetism, in which the source’s spin interacts with the test particles, that leads to the frame dragging and the Lense-Thirring effect.

Its said that “general relativity has one flaw that it cannot model spin-orbit coupling, so we need the Einstein-Cartan theory”. But who’s “spin” is here in the Einstein-Cartan theory? Source’s spin or the test particle’s spin?

From the relation,

(divergence of spin current) = P_{ab} – P_{ba} <> 0

it seems the spin is the source’s spin. Than what the difference between the Einstein-Cartan theory and Gravitoelectromagnetism? What happens if the test particle has spin?
 
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I haven't seen any Einstein-Cartan equations for motion of spinning test particles; this would be something a "geodesic equation plus spin of the test particle".

In Einstein-Cartan theory the l.h.s. of the equations is always "geometry", the r.h.s. is "matter", just like ordinary GR. Therefore the spin current is always the source term for torsion.

In general the equation for matter would of course not be the equation for a test particle i.e. a "geodesic equation plus spin of the test particle", but a field equation for the matter field coupled to spacetime = curvature + torsion, for example the Dirac equation.
 
Thanks for reply. I still do not understand, if general relativity can not model spin-orbit coupling, then how can we have the Kerr metric that describes the geometry of spacetime around a rotating massive body? And also Gravitoelectromagnetism can do some jobs for frame dragging and the Lense-Thirring effect?
 
GR in standard metric formulation can describe orbital angular momentum, but not intrinsic spin. In order to do that you need at least the tetrad formalism. Doing that one observes that it seems to unnatural to restrict the geometry to vanishing torsion. Allowing torsion automatically means introducing spin currents.
 

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