Originally Posted by Benjamin113
Yes, and that does make more sense. I believe now that the term "tilting" was meant to have a more...figurative...meaning than the light cone literally tilting.
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In coordinate systems in general relativity, light cones in a diagram using these coordinates may be tilted...for example, here is a diagram showing worldlines of particles and photons near the event horizon of a
black hole in Eddington-Finkelstein coordinates (the diagram is from the textbook
Gravitation by Misner/Thorne/Wheeler), you can see that if we draw in the future light cones of various events on these worldlines, they look more tilted as you approach the horizon (the grey column, the vertical axis being time):
this page has some similar diagrams at the bottom, one showing more clearly how for an event exactly on the horizon, the light cone has tilted over enough so it becomes impossible for anything in the future light cone to be outside the horizon:
Still, I don't understand what it would mean to say light cones "cannot be tilted so that they are parallel". Can you give some more context for that statement? Were they talking about general relativity or special relativity, for example?