Abstract

Number-resolving single-photon detectors represent a key technology for a host of quantum optics protocols, but despite significant efforts, state-of-the-art devices are limited to few photons. In contrast, state-dependent atom counting in arrays can be done with extremely high fidelity up to hundreds of atoms. We show that in waveguide QED, the problem of photon counting can be reduced to atom counting, by entangling the photonic state with an atomic array in the collective number basis. This is possible as the incoming photons couple to collective atomic states and can be achieved by engineering a second decay channel of an excited atom to a metastable state. Our scheme is robust to disorder and finite Purcell factors, and its fidelity increases with atom number. Analyzing the state of the re-emitted photons, we further show that if the initial atomic state is a symmetric Dicke state, dissipation engineering can be used to implement a nondestructive photon-number measurement, in which the incident state is scattered into the waveguide unchanged. Our results generalize to related platforms, including superconducting qubits.

Highlights

  • Single-photon detectors have a long history, with a plethora of technologies available [1]

  • We extend these concepts to a quantum nondemolition (QND) measurement in Sec

  • We have explored the use of arrays of quantum emitters coupled to waveguides for number-resolving photon detection

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Summary

INTRODUCTION

Single-photon detectors have a long history, with a plethora of technologies available [1]. This can be achieved either through continuous measurement, for example through dispersive coupling [14,15,16,17,18,19], or if the detector permanently changes its state and is read out later, as in impedancematched -systems [20,21,22,23,24,25,26]. The key idea here is to engineer atoms such that for each incident photon in the waveguide, exactly one atom changes its internal state, such that a subsequent measurement of the atomic state yields the number of photons in the scattered wave packet We do this by identifying conditions such that all photons are absorbed in one atomic transition (g → e, blue in Fig. 1) and dissipated in a different one (e → s, green).

ABSORPTION IN ATOMIC ARRAYS
Scattering theory
Complete absorption
Mirror geometry
Infinite waveguide
Chiral atom-waveguide coupling
Outline
QND measurement with Dicke states
Numerical simulation
Dicke state preparation
EXPERIMENTAL CONSIDERATIONS
Engineered decay
Engineered decay: nondestructive photon measurement
Other sources of disorder
Photon loss from coupling into the waveguide
Atom readout
CONCLUSION
Two-level systems coupled to one semi-infinite waveguide field
Three-level systems coupled to two semi-infinite waveguide fields
Strong coupling
Findings
Interaction timescales
Full Text
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