Abstract

When two equal photon-number states are combined on a balanced beam splitter, both output ports of the beam splitter contain only even numbers of photons. Consider the time-reversal of this interference phenomenon: the probability that a pair of photon-number-resolving detectors at the output ports of a beam splitter both detect the same number of photons depends on the overlap between the input state of the beam splitter and a state containing only even photon numbers. Here, we propose using this even-parity detection to engineer quantum states containing only even photon-number terms. As an example, we demonstrate the ability to prepare superpositions of two coherent states with opposite amplitudes, i.e. two-component Schrödinger cat states. Our scheme can prepare cat states of arbitrary size with nearly perfect fidelity. Moreover, we investigate engineering more complex even-parity states such as four-component cat states by iteratively applying our even-parity detector.

Highlights

  • The number of excitations in an optical field determines a fundamental property known as parity

  • We devised an even-parity detector by exploiting the interference phenomenon that leads to the production of Holland-Burnett states in a timereversed fashion

  • The even-parity detector is controlled by varying the photon-number distribution of an ancillary control state

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Summary

Introduction

The number of excitations in an optical field determines a fundamental property known as parity. Squeezed vacuum is a superposition of only even photon numbers and has reduced quantum fluctuations in its electric field compared to classical light [1]. This reduction in noise makes squeezed vacuum a valuable resource for optical quantum information processing [2, 3] and quantum sensing [4]. Thanks to recent advances in detector technology, it is possible to count the number of photons in an optical field using photon-number-resolving detectors [28] This advancement enables new state engineering schemes that exploit the number resolution of such detectors [29,30,31,32]. Tigate engineering four-component cat states which have applications in quantum error correction [52,53,54,55,56] and quantum sensing [57,58,59,60]

An even-parity detector
Detection efficiency
Even-parity state engineering
Two-component cat states
Four-component cat states
Experimental realizations
Summary and outlook
Findings
A Imperfect detection efficiency
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