This charge multiplication is proportional to the confinement time. Previous work used higher gap superconductors for confinement. In this work, the counterelectrode is terminated by a long, narrow wire made of the same material. We find 1 due to the slow out-diffusion of the quasiparticles down the wire. The wire dimensions and diffusion constant were chosen to engineer the backtunneling multiplication. For large backtunneling, the signal-to-noise of our spectrometer is increased.