Arkalius
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The worldline for any object with mass must be time-like. Events that are time-like are separated by a non-zero amount of time in all reference frames, but there exists a reference frame where their spatial separation is 0. Example, you get in your car to leave your home, and 15 minutes later you arrive at your place of work. These are time-like events. For you, they occurred in the same distance from yourself (0). For an observer moving relative to you, the relative distances of the events are different. They may even record a different amount of time passing, but it will always be positive, and they will always see you arrive after you depart.
Space-like events, on the other hand, always have a non-zero amount of space separating them, but there exists a frame of reference where they are simultaneous, and there will be sets of reference frames that disagree on which event preceded the other. You leave work as before, and 5 minutes later (relative to you), the sun emits a solar flare. The sun is more than 8 light minutes away, so these events are space-like. There exist frames of reference that will observe the solar flare happen before you leave work, and one that will see them happen at the same time. There is also no way possible for you to reach the location of the solar flare when it happens from your position at home on Earth, meaning the events always have a positive separation in distance.
So what does this mean for FTL travel? Well, the departure and arrival of an FTL traveler will necessarily be space-like events. That means there exist frames of reference that will see the arrival happen before the departure. All you would have to do, then, is ensure you end up in such a frame of reference when you arrive, so that you observe your departure happening after your arrival by enough of a time margin such that you can then make the return trip with the same FTL velocity, now relative to your new rest frame, and you'll arrive before you left.
There's a formula for determining the critical subluminal velocity for this scenario. If you can travel at some multiple ##n## (greater than 1) of the speed of light, then this velocity is given by ##v = \frac {2n} {1+n^2}##. As long as the frame of reference at your arrival exceeds this velocity (relative to, and away from your departure location), then it will be possible to travel at ##n## relative to this frame back to your origin and arrive before you left. You'll see that the faster your superluminal velocity is, the slower the subluminal velocity has to be to enable this time travel.
Space-like events, on the other hand, always have a non-zero amount of space separating them, but there exists a frame of reference where they are simultaneous, and there will be sets of reference frames that disagree on which event preceded the other. You leave work as before, and 5 minutes later (relative to you), the sun emits a solar flare. The sun is more than 8 light minutes away, so these events are space-like. There exist frames of reference that will observe the solar flare happen before you leave work, and one that will see them happen at the same time. There is also no way possible for you to reach the location of the solar flare when it happens from your position at home on Earth, meaning the events always have a positive separation in distance.
So what does this mean for FTL travel? Well, the departure and arrival of an FTL traveler will necessarily be space-like events. That means there exist frames of reference that will see the arrival happen before the departure. All you would have to do, then, is ensure you end up in such a frame of reference when you arrive, so that you observe your departure happening after your arrival by enough of a time margin such that you can then make the return trip with the same FTL velocity, now relative to your new rest frame, and you'll arrive before you left.
There's a formula for determining the critical subluminal velocity for this scenario. If you can travel at some multiple ##n## (greater than 1) of the speed of light, then this velocity is given by ##v = \frac {2n} {1+n^2}##. As long as the frame of reference at your arrival exceeds this velocity (relative to, and away from your departure location), then it will be possible to travel at ##n## relative to this frame back to your origin and arrive before you left. You'll see that the faster your superluminal velocity is, the slower the subluminal velocity has to be to enable this time travel.