A flat-spacetime diagram plots one spatial coordinate x horizontally and ct vertically at equal scale. Dashed diagonal lightlike lines form future and past cones around event E. A timelike path stays inside the future cone, while a spacelike event lies outside.
Geometry also constrains causal reach. Schematic Minkowski light cone with equal coordinate scaling, not experimental data. Curved spacetimes require their own metric; this diagram illustrates the local causal distinction.
01 / The idea

A spacetime diagram is not just a map of where things are; it also specifies which events can influence one another. Light cones organize those relationships locally. A massive observer’s ordinary trajectory remains timelike, while light travels along null directions in the appropriate limit. Hill’s idea of moving between geometric points therefore needs a distinction between a point drawn on a model and an event a traveler could reach. Zooming from Earth to Alpha 1 is an explanatory interface. It does not establish a continuous, physically accessible route between the displayed levels.

Past and future are physical restrictions

In a simple flat-spacetime example, an event outside another event’s light cone cannot be reached by a signal traveling at or below the speed of light. Curved spacetime complicates global relationships but does not remove the need for a local causal specification. The project should display travel proposals with a departure event, arrival event and trajectory, along with the metric assumed. A shortcut drawn in an external embedding can be misleading if that external direction is not part of the physical spacetime.

Correlations do not erase the cones

Quantum entanglement gives nonclassical correlations, yet the standard theory does not turn them into freely controllable signals outside the ordinary causal structure. This distinction should appear wherever the atlas connects information with geometry. A proposed new channel must provide an operational protocol: what does the sender choose, what does the receiver observe, and how is the result distinguished from shared randomness? Without that protocol, a claim of instantaneous connectedness is not a demonstrated communication or travel mechanism.

Test the model before interpreting its picture

A useful research submission would compute the causal paths of a candidate metric, identify horizons or problematic regions, and state whether the spacetime admits a consistent initial-value formulation. If it contains closed timelike curves, the proposal must confront their implications rather than quietly using them as a feature. These are mathematical checks before engineering feasibility. Hill’s project can make progress by publishing failed constructions and the constraint that defeats each one. That record clarifies exactly what a later successful model would need to overcome.

The mathematical lens

ds² = −c²dt² + dx² + dy² + dz²

In flat spacetime, ds² < 0 is timelike, ds² = 0 is null and ds² > 0 is spacelike, using the stated sign convention.

Turn it into a question.

Proposed test / not a reported result
Question
Is the proposed journey a physical causal path in its own specified metric?
Method
Compute the trajectory and local light cones, identify horizons and check initial-value consistency.
What would count against it?
The route uses an embedding direction absent from the model or crosses a causal boundary without a defined mechanism.
What to carry forward

A destination in a visualization is not automatically a reachable event.

Follow the original work.

These sources support the mechanisms and limits discussed here. They do not endorse Hill’s framework. Notes distinguish research proposals, reviews, and observations.

  1. Lecture Notes on General RelativitySean M. Carroll · 1997 · arXiv:gr-qc/9712019Read original source ↗
  2. General RelativityDavid Tong · n.d. · University of Cambridge lecture notesRead original source ↗
  3. Loophole-free Bell inequality violation using electron spins separated by 1.3 kilometresB. Hensen et al. · 2015 · Nature 526, 682–686Read original source ↗

Continue the investigation

Edition 02 · 18 October 2026 · AI-assisted synthesis. See editorial method.