A small correction term proportional to the logarithm of the area, added to the black hole entropy formula.The logarithmic correction is a refinement to the famous Bekenstein-Hawking entropy formula for black holes. The standard formula states that a black hole's entropy is proportional to the area of its event horizon, but quantum gravitational effects introduce a small additional term that scales with the natural logarithm of that area. This correction becomes significant only for very small black holes, where quantum effects are no longer negligible, and it provides a window into the microscopic structure of spacetime.
The logarithmic correction was first derived in the mid-1990s by several groups, including work by S. Carlip and by D. V. Fursaev, building on earlier insights from string theory and loop quantum gravity. It is now a standard prediction of any quantum theory of gravity that reproduces the Bekenstein-Hawking entropy.
In semiclassical gravity, the entropy of a black hole is computed from the partition function of quantum fields in the curved background. When one includes one-loop quantum fluctuations of matter and gravitons, the entropy acquires a logarithmic term. The coefficient of this term depends on the number and spin of the fields present, and it arises from the trace anomaly of the stress-energy tensor. For a Schwarzschild black hole, the correction is typically of the form -a ln(A), where A is the horizon area and a is a constant determined by the theory.
While not directly applied in technology, the logarithmic correction is a key test for candidate quantum gravity theories, as different approaches (e.g., loop quantum gravity, string theory) predict specific coefficients that can be compared.
The coefficient of the logarithmic correction is universal in the sense that it depends only on the low-energy particle content, not on the details of the ultraviolet completion.














