Can the Graviton be faster than light?

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Discussion Overview

The discussion revolves around the hypothetical properties of the graviton, particularly whether it could be faster than light and how it might interact with photons. Participants explore concepts related to gravitational interactions, the nature of particles, and the implications of non-instantaneous action in gravitational fields.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • One participant suggests that if gravitons exist, they would need to be faster than light to interact with mass and smaller than photons, although they express uncertainty about this idea.
  • Another participant counters that hypothetical gravitons would not be faster than light and questions the expectation of such a property.
  • There is a discussion about how gravitational effects propagate, with some participants asserting that the speed of gravitational changes must be the speed of light.
  • One participant mentions that an object’s gravitational influence is based on its past position rather than its current position, leading to a discussion about the implications of non-instantaneous action.
  • Another participant elaborates on the nature of fields, suggesting that the gravitational field points to a quadratically extrapolated position rather than the retarded position of an object.
  • There is a mention of electromagnetic (E&M) analogies to clarify points about field propagation and the influence of moving charges.
  • Some participants express uncertainty about the details of how fields point during transitions and the implications of these dynamics.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the properties of gravitons or the implications of non-instantaneous action in gravitational fields. Multiple competing views remain regarding the nature of gravitational interactions and the behavior of fields.

Contextual Notes

Participants acknowledge that the discussion involves complex concepts that may depend on specific definitions and assumptions about particle properties and field dynamics. There are unresolved details regarding the extrapolation of positions in gravitational fields.

marcgrissz
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Hello everyone,
I was thinking of the 4 forces and in particular of the gravity force.
We know that black holes and their gravity force can bend light and light gets lost on black holes.
How can the ipothetic particle of the graviton interact with the photon?
I thought that if the interaction is real, the graviton must be not only faster than light to perceive the mass, but it also has to be smaller and photons should be able to interchange gravitons.
I must be wrong, I know, but could anyone explain this to me?
 
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marcgrissz said:
I thought that if the interaction is real, the graviton must be not only faster than light to perceive the mass, but it also has to be smaller
Particles do not have a size in the classical sense. No, hypothetical gravitons would not be faster than light, and I don't see why you would expect that.
marcgrissz said:
and photons should be able to interchange gravitons.
Right.
 
mfb said:
Particles do not have a size in the classical sense. No, hypothetical gravitons would not be faster than light, and I don't see why you would expect that.
Right.
The idea that some peace of rock in the universe is interacting with my shoe, for example, makes me thinking of some velocity faster than light.
 
marcgrissz said:
The idea that some peace of rock in the universe is interacting with my shoe, for example, makes me thinking of some velocity faster than light.
Your shoe won't react to the current position of that rock. It will react according to the position where the rock was at some point in the past (which depends on its distance).
 
mfb said:
Your shoe won't react to the current position of that rock. It will react according to the position where the rock was at some point in the past (which depends on its distance).

Actually this is not quite right. The shoe will react to the field that has propagated to it from the rock at previous times. However, the field does not actually point toward the retarded position of the rock. It points toward the quadratically extrapolated current position of the rock. A similar but easier example comes from E&M; the electric field of a moving charge points toward the charge's current linearly extrapolated position. For the gravitational case, see Carlip, http://arxiv.org/abs/gr-qc/9909087v2 . I have a description of the E&M version in section 10.4 of my SR book: http://www.lightandmatter.com/sr/ .
 
I didn't include velocity as this makes it more complicated. My point was the non-instantaneous action.
 
mfb said:
I didn't include velocity as this makes it more complicated. My point was the non-instantaneous action.

I don't see how the non-instantaneous action can make any difference in a frame where the source is at rest.
 
  • #10
Well, you can leave an object 1 light year away at position A for a year, then move it one light-hour in some direction during roughly an hour, then leave it at position B for a year. For one year we'll see no change. After that year, we'll see a short transition period, and then the effect of the object at rest at B.
 
  • #11
mfb said:
Well, you can leave an object 1 light year away at position A for a year, then move it one light-hour in some direction during roughly an hour, then leave it at position B for a year. For one year we'll see no change. After that year, we'll see a short transition period, and then the effect of the object at rest at B.

OK, but during the period when the information about the transition is propagating past B, the field will not point to the retarded position. In the E&M case, I believe it will point to the current linearly extrapolated position, and in the gravitational case to the quadratically extrapolated position. (I could be getting some details wrong.)
 
  • #12
Could be, but that's still a short transition period where the pointing is off in some way.
 

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