Quantum Imaging by Coherent Enhancement

Conventional wisdom dictates that to image the position of fluorescent atoms or molecules, one should stimulate as much emission and collect as many photons as possible. That is, in this classical case, it has always been assumed that the coherence time of the system should be made short, and that t...

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Bibliographic Details
Main Authors: Low, Guang Hao (Contributor), Yoder, Theodore James (Contributor), Chuang, Isaac L. (Contributor)
Other Authors: Massachusetts Institute of Technology. Department of Physics (Contributor), Massachusetts Institute of Technology. Research Laboratory of Electronics (Contributor), MIT-Harvard Center for Ultracold Atoms (Contributor)
Format: Article
Language:English
Published: American Physical Society, 2015-03-12T19:06:08Z.
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001 95994
042 |a dc 
100 1 0 |a Low, Guang Hao  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Physics  |e contributor 
100 1 0 |a Massachusetts Institute of Technology. Research Laboratory of Electronics  |e contributor 
100 1 0 |a MIT-Harvard Center for Ultracold Atoms  |e contributor 
100 1 0 |a Low, Guang Hao  |e contributor 
100 1 0 |a Yoder, Theodore James  |e contributor 
100 1 0 |a Chuang, Isaac L.  |e contributor 
700 1 0 |a Yoder, Theodore James  |e author 
700 1 0 |a Chuang, Isaac L.  |e author 
245 0 0 |a Quantum Imaging by Coherent Enhancement 
260 |b American Physical Society,   |c 2015-03-12T19:06:08Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/95994 
520 |a Conventional wisdom dictates that to image the position of fluorescent atoms or molecules, one should stimulate as much emission and collect as many photons as possible. That is, in this classical case, it has always been assumed that the coherence time of the system should be made short, and that the statistical scaling ∼1/sqrt[t] defines the resolution limit for imaging time t. However, here we show in contrast that given the same resources, a long coherence time permits a higher resolution image. In this quantum regime, we give a procedure for determining the position of a single two-level system and demonstrate that the standard errors of our position estimates scale at the Heisenberg limit as ∼1/t, a quadratic, and notably optimal, improvement over the classical case. 
520 |a MIT-Harvard Center for Ultracold Atoms MIT International Science and Technology Initiative 
520 |a National Science Foundation (U.S.). Integrative Graduate Education and Research Traineeship 
520 |a United States. Army Research Laboratory (Quantum Algorithms Program) 
546 |a en 
655 7 |a Article 
773 |t Physical Review Letters