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Conference on Lasers and Electro-Optics Europe & European Quantum Electronics Conference (CLEO/Europe-EQEC)

Quantum state carving of two atomic qubits in an optical cavity

Stephan Welte, Bastian Hacker, Severin Daiss, Lin Li, Stephan Ritter, Gerhard Rempe

Published Jun 1, 2017• 2 citations
Publisher

Abstract

Summary form only given. Neutral atoms trapped inside an optical cavity provide an ideal platform for the implementation of quantum networks [1]. In such a network, nodes containing multiple atomic qubits are essential for the construction of a quantum repeater as they allow for entanglement swapping and thus the generation of entanglement between qubits over long distances. Here we will show the realisation of such a multi-qubit network node containing two87Rb atoms (see Figure. 1) in an optical cavity. Local entanglement between the two atoms is created with an experimental technique called quantum state carving. It relies on the reflection of weak coherent pulses from the cavity and subsequent measurement of the photons polarisation [2]. Postselection on the cases where the photon changed its linear polarisation by 90° after the reflection projects the atomic state onto an entangled state. This measurement technique is intrinsically probabilistic, but heralded. We will show the generation of all four maximally entangled atomic Bell states, a key resource for a plethora of quantum communication protocols. We will give an overview over the necessary experimental toolbox including the collective manipulation and readout of the two atomic qubits.

DOI
10.1109/cleoe-eqec.2017.8087415

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Summary form only given. Neutral atoms trapped inside an optical cavity provide an ideal platform for the implementation of quantum networks [1]. In such a network, nodes containing multiple atomic qubits are essential for the construction of a quantum repeater as they allow for entanglement swapping and thus the generation of entanglement between qubits over long distances. Here we will show the realisation of such a multi-qubit network node containing two87Rb atoms (see Figure. 1) in an optical cavity. Local entanglement between the two atoms is created with an experimental technique called quantum state carving. It relies on the reflection of weak coherent pulses from the cavity and subsequent measurement of the photons polarisation [2]. Postselection on the cases where the photon changed its linear polarisation by 90° after the reflection projects the atomic state onto an entangled state. This measurement technique is intrinsically probabilistic, but heralded. We will show the generation of all four maximally entangled atomic Bell states, a key resource for a plethora of quantum communication protocols. We will give an overview over the necessary experimental toolbox including the collective manipulation and readout of the two atomic qubits.
We demonstrate entanglement generation of two neutral atoms trapped inside an optical cavity. Entanglement is created from initially separable two-atom states through carving with weak photon pulses reflected from the cavity. A polarization rotation of the photons heralds the entanglement. We show the successful implementation of two different protocols and the generation of all four Bell states with a maximum fidelity of (90±2)%. The protocol works for any distance between cavity-coupled atoms, and no individual addressing is required. Our result constitutes an important step towards applications in quantum networks, e.g., for entanglement swapping in a quantum repeater.
Abstract One of the most fascinating aspects of quantum networks is their capability to distribute entanglement as a nonlocal communication resource1. In a first step, this requires network-ready devices that can generate and store entangled states2. Another crucial step, however, is to develop measurement techniques that allow for entanglement detection. Demonstrations for different platforms3–13 suffer from being not complete, destructive or local. Here, we demonstrate a complete and nondestructive measurement scheme14–16 that always projects any initial state of two spatially separated network nodes onto a maximally entangled state. Each node consists of an atom trapped inside an optical resonator from which two photons are successively reflected. Polarization measurements on the photons discriminate between the four maximally entangled states. Remarkably, such states are not destroyed by our measurement. In the future, our technique might serve to probe the decay of entanglement and to stabilize it against dephasing via repeated measurements17,18.
Entanglement distributed over a set of individually addressable qubit nodes is the enabling resource for a plethora of applications ranging from tests of quantum physics to secure and modular quantum information networks. Entanglement between two memory qubits has been realized on various platforms, but extension to more nodes remains rare and formidably challenging. The principal bottleneck is the efficiency of the light-matter interfaces connecting the qubit nodes to their communication channels. Here, we efficiently generate, distribute and store a three-qubit entangled state across three independent laboratories containing single atoms coupled to optical resonators. We sequentially entangle the atoms pairwise, two by heralded photonic entanglement swapping and two by heralded state transfer. We reach a three-qubit entanglement fidelity of 77(1)% and an entanglement lifetime above 200us. The observed qubit correlations violate Mermin's inequality while closing the detection loophole. Our three-qubit entanglement-generation efficiency is 0.16%. This unprecedented efficiency of our scheme establishes a clear route towards multi-node quantum networks.
Entanglement of distant quantum memories forms the building block of quantum networks. Neutral atoms with long coherence times are sought for candidates for quantum network links (QNLs). Our experiment with two nodes, 400 m apart, employs single optically trapped Rubidium-87 atoms as quantum memories. Via excitations, entanglement between the atom and spontaneously emitted single photons is created in both traps. Using single-mode fibers, the photons are interfered in a Bell-state measurement thereby swapping the entanglement from the two atom-photon pairs to the atoms with a projective measurement. A new collection setup [1] allows for an increased entanglement event rate of ∼1/20 Hz allowing detailed state analysis and reconstruction of the entangled state.
Photon entanglement is an essential ingredient for linear optics quantum computing schemes, quantum cryptographic protocols and fundamental tests of quantum mechanics. Here we describe a setup that allows for the generation of polarisation-entangled N-photon states on demand. The photons are obtained by mapping the entangled state of N atoms, each of them trapped inside an optical cavity, onto the free radiation field. The required initial state can be prepared by performing postselective measurements on the collective emission from the cavities through a multiport beamsplitter.
Atoms and photons are well-suited candidates for quantum information processing and quantum communication. While atoms can be used for storage and manipulation, photons are ideal carriers for the transfer of quantum information. Our group pursues the goal of creating a basic node of a quantum communication network by entangling two independently trapped87Rb atoms over a large distance. Besides its prospects in quantum communication (e.g. quantum repeater), this would also allow a loophole-free test of Bell's inequality which can help to conclusively answer the long-standing question about the completeness of the quantum theory. The key ingredient is atom-photon entanglement which will enable us to entangle two atoms by entanglement swapping. We plan to achieve a distance of 300m between two independent single atom traps.