Can Particles Travel Backwards in Time if They Exceed the Speed of Light?

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Discussion Overview

The discussion revolves around the concept of whether particles can travel backwards in time if they exceed the speed of light. Participants explore the implications of time dilation and Lorentz transformations, examining both theoretical and mathematical aspects of faster-than-light travel.

Discussion Character

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

Main Points Raised

  • Some participants reference the time dilation equation and question the implications of a particle traveling faster than light, noting that it leads to an imaginary number for time.
  • Others assert that particles cannot exceed the speed of light, suggesting that the original question lacks meaning.
  • One participant introduces the idea that if a particle travels faster than light, it could theoretically allow for sending messages back in time, referencing the concept of tachyons.
  • Another participant discusses the relationship between imaginary mass terms in quantum field theory and the implications for particles, expressing uncertainty about the validity of these concepts.
  • Several participants elaborate on the use of Lorentz transformations to illustrate scenarios where faster-than-light travel could result in arriving at a destination before leaving, thus suggesting a form of time travel.
  • One participant emphasizes that the analysis of time travel does not rely on applying Lorentz transformations to frames moving faster than light.

Areas of Agreement / Disagreement

Participants express differing views on the feasibility and implications of faster-than-light travel. While some agree on the mathematical challenges posed by such speeds, others propose scenarios where time travel could occur, indicating that the discussion remains unresolved with multiple competing views.

Contextual Notes

Limitations include the assumption that the time dilation equation is valid only for speeds less than the speed of light, and the unresolved nature of the implications of imaginary mass in quantum field theory.

Salamon
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The equation for time dilation goes something like

t' = t/ (√(1-v2/c2)

I have heard that if a particle can travel at a speed such that v>c, then the particle will go backwards in time.

But how is this true? According to this equation, if v>c, this implies that t' is an imaginary number...not a real valued negative number.
 
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Since particles CAN'T travel faster than c, your question has no meaning other than playing games with math.
 
Salamon said:
The equation for time dilation goes something like

t' = t/ (√(1-v2/c2)

I have heard that if a particle can travel at a speed such that v>c, then the particle will go backwards in time.

But how is this true? According to this equation, if v>c, this implies that t' is an imaginary number...not a real valued negative number.

It's not true, and you're right.
 
Just to add a little, if a particle goes faster than light in one frame, then in other frames of reference, it will arrive before it left. Furthermore, under plausible assumptions, if particles can go faster than light, you can send a message and get an answer before you sent it. See:

http://en.wikipedia.org/wiki/Tachyonic_antitelephone


So, it is true that the particle won't go back in time in a frame in which it is moving faster than light; and it is true the mass is imaginary not negative. However, faster than light particles do readily lead to time travel 'paradoxes'.
 
I know very little quantum field theory. But as far as I know, when there is a field with an imaginary mass term, it means that we have to do a perturbation about some value of the field such that the resulting particle has real positive mass. For example Goldstone bosons (and Higgs bosons, I think). They have imaginary mass terms, but the associated particle(s) have real mass, because we must do the perturbation at some non-zero value of the field. It is not possible to do a perturbation around values of the field which would give 'imaginary mass' particles. Or, I think we would get a condensate at these values, which is because we cannot do a perturbation to just get single particles.

So anyway, I think that in quantum field theory, this idea of imaginary mass particles is kinda nonsensical. But I don't know for sure, I don't know much about quantum field theory, so don't take me too seriously.
 
Salamon said:
The equation for time dilation goes something like

t' = t/ (√(1-v2/c2)

I have heard that if a particle can travel at a speed such that v>c, then the particle will go backwards in time.

But how is this true? According to this equation, if v>c, this implies that t' is an imaginary number...not a real valued negative number.

The claim about time travel is not (directly, anyway) about time dilation. It's about the Lorentz transformations. To get an extreme case, let's suppose that you have a teleportation device, which from any frame allows you to teleport instantaneously (according to that frame) to any other location in the universe.

Consider two frames, F and F', where objects at rest in F' are moving at speed v in the x-direction, as measured in frame F. Then what we do is this: We have a teleporter at rest in frame F. You teleport from the point
x=0, t=0

to the point
x=L,\ \ t=0

Now, switch to frame F'. In its coordinates, the second event is:
x'=\gamma L,\ \ t' = -\gamma \dfrac{v L}{c^2}

Now, hop in a teleporter that is at rest in frame F'. Teleport back to the point x=0 where you came from. The coordinates of this point in frame F' is:

x'=\gamma \dfrac{v^2}{c^2} L,\ \ t' = -\gamma \dfrac{vL}{c^2}

The coordinates in frame F are:

x=0,\ \ t= - \dfrac{vL}{c^2}

So the round-trip brought you back to where you started (in space), but to an earlier time.

You might think this is an artifact of assuming instantaneous travel. But another exercise with Lorentz transformations shows that if travel is faster-than-light in one frame, then there is a second frame in which it is instantaneous. So a faster-than-light rocket, together with the ability to change frames (which only takes a slower-than-light rocket) will give you instantaneous travel, which can be used for back-in-time travel.

None of this analysis uses the concept of applying the Lorentz transformations to "frames" traveling faster than light.
 
stevendaryl said:
The claim about time travel is not (directly, anyway) about time dilation. It's about the Lorentz transformations. To get an extreme case, let's suppose that you have a teleportation device, which from any frame allows you to teleport instantaneously (according to that frame) to any other location in the universe.

Consider two frames, F and F', where objects at rest in F' are moving at speed v in the x-direction, as measured in frame F. Then what we do is this: We have a teleporter at rest in frame F. You teleport from the point
x=0, t=0

to the point
x=L,\ \ t=0

Now, switch to frame F'. In its coordinates, the second event is:
x'=\gamma L,\ \ t' = -\gamma \dfrac{v L}{c^2}

Now, hop in a teleporter that is at rest in frame F'. Teleport back to the point x=0 where you came from. The coordinates of this point in frame F' is:

x'=\gamma \dfrac{v^2}{c^2} L,\ \ t' = -\gamma \dfrac{vL}{c^2}

The coordinates in frame F are:

x=0,\ \ t= - \dfrac{vL}{c^2}

So the round-trip brought you back to where you started (in space), but to an earlier time.

You might think this is an artifact of assuming instantaneous travel. But another exercise with Lorentz transformations shows that if travel is faster-than-light in one frame, then there is a second frame in which it is instantaneous. So a faster-than-light rocket, together with the ability to change frames (which only takes a slower-than-light rocket) will give you instantaneous travel, which can be used for back-in-time travel.

None of this analysis uses the concept of applying the Lorentz transformations to "frames" traveling faster than light.

I see that PAllen already said this more succinctly.
 
Salamon said:
The equation for time dilation goes something like

t' = t/ (√(1-v2/c2)
This equation is valid for v<c only.
 

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