The Heisenberg limit for laser coherence
- URL: http://arxiv.org/abs/2009.05296v2
- Date: Thu, 5 Nov 2020 12:59:03 GMT
- Title: The Heisenberg limit for laser coherence
- Authors: Travis J. Baker, S. N. Saadatmand, Dominic W. Berry, Howard M. Wiseman
- Abstract summary: Limit on $mathfrakC$ for an ideal laser was thought to be of order $mu2$.
We derive an upper bound: $mathfrakC = O(mu4)$.
- Score: 0.0
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: To quantify quantum optical coherence requires both the particle- and
wave-natures of light. For an ideal laser beam [1,2,3], it can be thought of
roughly as the number of photons emitted consecutively into the beam with the
same phase. This number, $\mathfrak{C}$, can be much larger than $\mu$, the
number of photons in the laser itself. The limit on $\mathfrak{C}$ for an ideal
laser was thought to be of order $\mu^2$ [4,5]. Here, assuming nothing about
the laser operation, only that it produces a beam with certain properties close
to those of an ideal laser beam, and that it does not have external sources of
coherence, we derive an upper bound: $\mathfrak{C} = O(\mu^4)$. Moreover, using
the matrix product states (MPSs) method [6,7,8,9], we find a model that
achieves this scaling, and show that it could in principle be realised using
circuit quantum electrodynamics (QED) [10]. Thus $\mathfrak{C} = O(\mu^2)$ is
only a standard quantum limit (SQL); the ultimate quantum limit, or Heisenberg
limit, is quadratically better.
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