Abstract
The differences between classical and quantum sources in the context of coincidence imaging are discussed. Consequently, a classical source must be configured to work with a particular reference geometry, whereas use of a quantum source allows the reference geometry to be chosen after the source is in place. It is shown how the fixed-basis limitation of a classical source can be compensated by a pair of lenses near the source, so that in practical terms a classical coincidence imaging setup will provide nearly the same flexibility as a quantum coincidence imaging setup.
Original language | English |
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Pages | QMH2/1-QMH2/2 |
State | Published - 2003 |
Externally published | Yes |
Event | Trends in Optics and Photonics Series: Quantum electronics and Laser Science (QELS) - Baltimore, MD., United States Duration: Jun 1 2003 → Jun 6 2003 |
Conference
Conference | Trends in Optics and Photonics Series: Quantum electronics and Laser Science (QELS) |
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Country/Territory | United States |
City | Baltimore, MD. |
Period | 06/1/03 → 06/6/03 |