Abstract
Fundamental phase-shift detection properties of optical multimode interferometers are analyzed. Limits on perfectly distinguishable phase shifts are derived for general quantum states of a given average energy. These bounds are found to be independent of the number of interfering modes, and are consistent with the Heisenberg limit. A short discussion on the concept of well-defined relative phase is also included.
- Received 5 April 2002
DOI:https://doi.org/10.1103/PhysRevA.67.053803
©2003 American Physical Society