A classical condition in general relativity requiring the energy density to be non-negative along null geodesics.The null energy condition is a foundational assumption in classical general relativity. It states that the energy density measured by any observer moving at the speed of light along a null geodesic must be non-negative. In practical terms, it forbids negative energy densities along lightlike paths, which has profound implications for what kinds of spacetimes are physically allowed. This condition is one of several energy conditions used to constrain the behavior of matter and geometry in Einstein's equations.
The energy conditions were formalized in the 1960s and 1970s by physicists such as Stephen Hawking, Roger Penrose, and Robert Geroch, building on earlier work by Richard Arnowitt, Stanley Deser, and Charles Misner. The null energy condition specifically emerged as a minimal requirement for proving key theorems about singularities and black holes.
In general relativity, the stress-energy tensor describes the distribution of matter and energy. The null energy condition requires that for any null vector (representing a lightlike direction), the contraction of the stress-energy tensor with that vector twice is non-negative. This simple inequality prevents exotic phenomena like traversable wormholes, closed timelike curves, and certain types of warp drives, which would require negative energy densities. It also plays a role in singularity theorems and the behavior of black hole horizons.
The null energy condition is used in theoretical cosmology and astrophysics to test the viability of models involving dark energy, cosmic inflation, and exotic matter. It also constrains proposals for faster-than-light travel and time machines.
The null energy condition can be violated by quantum effects, such as the Casimir effect, which has led to the development of 'quantum energy inequalities' that bound the magnitude and duration of such violations.














