Can Gravitons Interact with Magnetic Fields and Explain Light Bending?

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Discussion Overview

The discussion revolves around the interaction of gravitons with magnetic fields and the implications for light bending in the context of general relativity (GR). Participants explore the nature of gravitons, photons, and their respective interactions with magnetic fields, as well as the relationship between spin and magnetic moments.

Discussion Character

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

Main Points Raised

  • Some participants suggest that the graviton, having spin 2, might interact with magnetic fields, similar to how electrons (spin 1/2) do.
  • Others argue that spin angular momentum does not determine interaction with magnetic fields, pointing out that the electron's interaction is due to its magnetic moment.
  • A participant states that photons do not "bend" but travel in straight lines in curved spacetime, challenging the idea of photon-graviton interaction in light bending.
  • Questions arise regarding the relationship between the electron's magnetic moment and its spin, with references to external resources for clarification.
  • Some participants discuss the derivation of the magnetic moment from the spin of particles, mentioning the role of quantum field theory (QFT) and minimal coupling in electromagnetic interactions.
  • There is mention of the gyrofactor of 2 for electrons, with discussions on whether this can be derived non-relativistically or if it is a relativistic effect.
  • Concerns are raised about the validity of non-relativistic derivations, with critiques of the ad-hoc nature of certain approaches to deriving the gyrofactor.

Areas of Agreement / Disagreement

Participants express disagreement on the interaction of gravitons with magnetic fields and the nature of light bending. There is no consensus on whether photons can be considered to interact with gravitons in the context of light bending, and the relationship between spin and magnetic moment remains a topic of exploration.

Contextual Notes

Limitations include unresolved assumptions regarding the nature of gravitons and their interactions, as well as the dependence on definitions related to magnetic moments and spin. The discussion also reflects varying interpretations of relativistic versus non-relativistic effects in particle physics.

kent davidge
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(I'm sorry for my poor English.) In GR the explanation for the bending of light by gravity is that gravity is a curvature in space (and time) and thus light follows the curved space. I was reading about the (undiscovered) graviton. It would have spin 2. Does it mean a graviton would interact with a magnetic field? If so, can we speak of bending of light as a photon-graviton interaction, like electrons (spin 1/2) interact with magnetic fields?
 
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kent davidge said:
(I'm sorry for my poor English.) In GR the explanation for the bending of light by gravity is that gravity is a curvature in space (and time) and thus light follows the curved space. I was reading about the (undiscovered) graviton. It would have spin 2. Does it mean a graviton would interact with a magnetic field?
No. Having spin angular momentum has no relation with interaction with a magnetic field. The electron interacts with a magnetic field because it has a magnetic moment.

kent davidge said:
If so, can we speak of bending of light as a photon-graviton interaction, like electrons (spin 1/2) interact with magnetic fields?
No. The photon doesn't "bend," it goes in a straight line in a curved space-time.
 
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DrClaude said:
No. Having spin angular momentum has no relation with interaction with a magnetic field. The electron interacts with a magnetic field because it has a magnetic moment.No. The photon doesn't "bend," it goes in a straight line in a curved space-time.
Thank you. How does the electron magnetic moment is related to its spin? And do photons and gravitons have a magnetic moment?
 
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kent davidge said:
Can you show me a derivation for the spin from the magnetic moment?
I don't know that it can be "derived." There may be something coming from QFT.

Maybe @vanhees71 can help?
 
The relation between spin and magnetic moment comes from minimal coupling of the electromagnetic field. For Dirac spinors, e.g., you start from the free-field Lagrangian
$$\mathcal{L}=\overline{\psi} (\mathrm{i} \gamma^{\mu} \partial_{\mu}-m) \psi,$$
and substitute
$$\partial_{\mu} \rightarrow D_{\mu}=\partial_{\mu} + \mathrm{i} q A_{\mu},$$
where ##A_{\mu}## is the electromagnetic field. This leads to the magnetic moment of the electron with the correct tree-level gyrofactor of 2.
 
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vanhees71 said:
The relation between spin and magnetic moment comes from minimal coupling of the electromagnetic field. For Dirac spinors, e.g., you start from the free-field Lagrangian
$$\mathcal{L}=\overline{\psi} (\mathrm{i} \gamma^{\mu} \partial_{\mu}-m) \psi,$$
and substitute
$$\partial_{\mu} \rightarrow D_{\mu}=\partial_{\mu} + \mathrm{i} q A_{\mu},$$
where ##A_{\mu}## is the electromagnetic field. This leads to the magnetic moment of the electron with the correct tree-level gyrofactor of 2.
Thank you.
 
vanhees71 said:
The relation between spin and magnetic moment comes from minimal coupling of the electromagnetic field. For Dirac spinors, e.g., you start from the free-field Lagrangian
$$\mathcal{L}=\overline{\psi} (\mathrm{i} \gamma^{\mu} \partial_{\mu}-m) \psi,$$
and substitute
$$\partial_{\mu} \rightarrow D_{\mu}=\partial_{\mu} + \mathrm{i} q A_{\mu},$$
where ##A_{\mu}## is the electromagnetic field. This leads to the magnetic moment of the electron with the correct tree-level gyrofactor of 2.
Just to add: this can also be derived non-relativistically, which shows that the gyrofactor of 2 is not a relativistic effect, as sometimes is claimed (unlike the Darwin-term and the spin-orbit coupling, which are relativistic effects). See e.g. papers by Levy-Leblond. The idea is basically to write down the Dirac equation, but demand that every spinor component obeys the Schrödinger equation instead of the Klein-Gordon equation, resulting in a "nonrelativistic Clifford algebra".
 
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Well, in the non-relativistic case it's not so convincing, because you have to write
$$\hat{\vec{p}}^2=(\vec{\sigma} \cdot \hat{\vec{p}})^2,$$
and then introduce the minimal coupling in this way ##\vec{\sigma} \cdot \hat{\vec{p}} \rightarrow \vec{\sigma}(\hat{\vec{p}}-\mathrm{i} q \hat{\vec{A}})## and then square. This is just an ad-hoc description, leading to the correct gyro factor. Why one cannot simply put the minimal substitution without introducing the Pauli matrices is not clear. In th Dirac case it's a unique procedure.
 
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