In quantum-field theory in curved spacetime, two important physical quantities are the expectation value of the stress-energy tensor 〈Tμν〉 and of the square of the field operator 〈φ2〉. These expectation… Click to show full abstract
In quantum-field theory in curved spacetime, two important physical quantities are the expectation value of the stress-energy tensor 〈Tμν〉 and of the square of the field operator 〈φ2〉. These expectation values must be renormalized, which is usually performed via the so-called point-splitting prescription. However, the renormalization method that is usually implemented in the literature, in principle, only applies to static, spherically-symmetric spacetimes, and does not readily generalize to other types of spacetime. We present a novel implementation of the renormalization procedure which may be used in the future for more general spacetimes, such as Kerr black hole spacetime. As an example, we apply our method to the renormalization of 〈φ2〉 for a massless scalar field in Bertotti–Robinson spacetime.
               
Click one of the above tabs to view related content.