Spin- amplitudes in black-hole evaporation
arXiv:gr-qc/0510036 · doi:10.1088/0264-9381/22/14/010
Abstract
We extend to the fermionic spin-1/2 case earlier work on quantum amplitudes arising from gravitational collapse to a black hole. Boundary data are specified on initial and final asymptotically-flat space-like hypersurfaces , separated by a Lorentzian proper-time interval , measured at spatial infinity. Following Feynman's prescription, one makes the problem well-posed by rotating into the complex: , with . After calculating the amplitude for , one takes the 'Lorentzian limit' . In this paper, we treat quantum amplitudes for the case of fermionic massless spin-1/2 (neutrino) final boundary data; working in the holomorphic representation, we take these boundary data to be odd elements of a Grassmann algebra. Making use of boundary conditions originally developed for local supersymmetry, we find that this fermionic case can be treated in a way which parallels the bosonic case. With these boundary conditions, for , one obtains a unique fermionic classical solution, and we calculate its classical action as a functional of the fermionic data on the late-time surface ; the quantum amplitude follows straightforwardly from this.
References in corpus (3)
Cited by in corpus (9)
- Vaidya Space-Time in Black-Hole Evaporation
- Black hole evaporation in a spherically symmetric non-commutative space-time
- Gravitational amplitudes in black-hole evaporation: the effect of non-commutative geometry
- Bogoliubov transformations for amplitudes in black-hole evaporation
- Coherent and squeezed states in black-hole evaporation
- Bogoliubov transformations in black-hole evaporation
- Quantum amplitudes in black-hole evaporation: Spins 1 and 2
- Quantum amplitudes in black-hole evaporation: coherent and squeezed states
- Quantum Amplitudes in Black-Hole Evaporation: Complex Approach and Spin-0 Amplitude