115 Minkowski Space

A set of events equipped with the Minkowski metric that is used to represent flat spacetime.

definition [d] (Minkowski Space = Minkowski Spacetime = Flat Spacetime) The four-dimensional flat Lorentzian manifold of special relativity, with Minkowski metric \(\eta_{\mu\nu} = \operatorname{diag}(-1,1,1,1)\) and line element

  • \(ds^{2} = -c^{2}\, dt^{2} + dx^{2} + dy^{2} + dz^{2}\) .

where

  • \(\eta_{\mu\nu}\) is the Minkowski metric tensor.
  • \(ds\) is the infinitesimal spacetime interval.
  • \(c\) is the speed of light.
  • \(t\) is time.
  • \(x, y, z\) are Cartesian spatial coordinates.
  • \(x^{\mu} = (ct,\, x,\, y,\, z)\) are spacetime coordinates of an event.

Note:

  • events are points of the manifold.
  • \(c\) is often set to \(1\).
  • the Riemann curvature vanishes.

definition [d] (Minkowski Space = Minkowski Spacetime) The same flat spacetime with the opposite metric signature \(\eta_{\mu\nu} = \operatorname{diag}(1,-1,-1,-1)\) and line element

  • \(ds^{2} = (c\, dt)^{2} - dx^{2} - dy^{2} - dz^{2}\) .

where

  • \(x^{\mu} = (ct,\, x,\, y,\, z)\) are spacetime coordinates.
  • \(\eta_{\mu\nu}\) is the Minkowski metric.
  • \(c\) is the speed of light.
  • \(ds\) is the infinitesimal spacetime interval.

Note:

  • the two signatures are a convention, not different geometries.