  We consider a way of defining quantum Hamiltonians involving particle
creation and annihilation based on an interior-boundary condition (IBC) on the
wave function, where the wave function is the particle-position representation
of a vector in Fock space, and the IBC relates (essentially) the values of the
wave function at any two configurations that differ only by the creation of a
particle. Here we prove, for a model of particle creation at one or more point
sources using the Laplace operator as the free Hamiltonian, that a Hamiltonian
can indeed be rigorously defined in this way without the need for any
ultraviolet regularization, and that it is self-adjoint. We prove further that
introducing an ultraviolet cut-off (thus smearing out particles over a positive
radius) and applying a certain known renormalization procedure (taking the
limit of removing the cut-off while subtracting a constant that tends to
infinity) yields, up to addition of a finite constant, the Hamiltonian defined
by the IBC.
