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In special and general relativity, a light cone (or null cone) is the path that a flash of light, emanating from a single event — localized to a single point in space and a single moment in time — and traveling in all directions, would take through spacetime.
Mathematical construction, Details & In general relativity
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cone light event time spacetime past events future relativity would cannot inside special minkowski given cones space also one causal
| Subject | Predicate | Object | Confidence | Src |
|---|---|---|---|---|
| Light cone | is a | boundary of its causal past.In a curved spacetime | 0.90 | text |
| Light cone | related to Details | If | 0.60 | section |
| Light cone | related to Details | The | 0.60 | section |
| Light cone | related to Details | In | 0.60 | section |
| Light cone | related to Details | This | 0.60 | section |
| Light cone | related to Details | Albert Einstein's | 0.60 | section |
| Light cone | related to Details | Hermann Minkowski | 0.60 | section |
| Light cone | related to Details | Minkowski | 0.60 | section |
| Light cone | related to Details | To | 0.60 | section |
| Light cone | related to Details | Euclidean | 0.60 | section |
| Light cone | related to External links | Physics | 0.60 | section |
| Light cone | related to External links | The Einstein-Minkowski Spacetime | 0.60 | section |
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