TY - GEN

T1 - On-chip quantum state generation by means of integrated frequency combs

AU - Sciara, Stefania

AU - Kues, Michael

AU - Reimer, Christian

AU - Roztocki, Piotr

AU - Wetzel, Benjamin

AU - Bromberg, Yaron

AU - Little, Brent E.

AU - Chu, Sai T.

AU - Moss, David J.

AU - Caspani, Lucia

AU - Morandotti, Roberto

N1 - Funding Information: 1INRS-EMT, 1650 Boulevard Lionel Boulet, Varennes, Québec J3X 1S2, Canada 2 University of Palermo-Department of Energy, Information Engineering and Mathematical Methods, Palermo 90128, Italy 3School of Engineering, University of Glasgow, Rankine Building, Oakfield Avenue, Glasgow G12 8LT, Scotland 4Department of Physics and Astronomy, University of Sussex, Falmer, Brighton BN1 9RH, England 5 Racah Institute of Physics, The Hebrew University of Jerusalem, Jerusalem 91904, Israel 6 Xi’an Institute of Optics and Precision Mechanics of CAS, Xi’an, China 7Department of Physics and Material Science, City University of Hong Kong, Tat Chee Avenue, Hong Kong, China 8Centre for Micro Photonics, Swinburne University of Technology, Hawthorn, VIC, 3122 Australia 9Institute of Photonics, Department of Physics, University of Strathclyde, Glasgow G4 0NW, Scotland *michael.kues@emt.inrs.ca, **morandotti@emt.inrs.ca Publisher Copyright: © 2017 IEEE. Copyright: Copyright 2017 Elsevier B.V., All rights reserved.

PY - 2017/8/17

Y1 - 2017/8/17

N2 - Entangled photon-pair sources are key building blocks towards the realization of applications in quantum information processing [1], quantum communications [2], as well as imaging and sensing with resolutions exceeding the classical limit [3]. The generation of, e.g. polarization, time-energy and time-bin entangled photon-pairs has been demonstrated using spontaneous parametric down-conversion (SPDC) in nonlinear second-order media, as well as spontaneous four-wave mixing (SFWM) in third-order nonlinear media. Specifically, nonlinear (third-order) interactions in on-chip microring resonators have been widely used to achieve classical frequency combs [4], mode-lock lasers [5], signal processing [6], etc. Integrated photonics can also find applications for quantum state generation in compact, scalable and efficient devices, required for future optical quantum circuits. In particular, solutions focusing on an integrated (on-chip) approach have been recently investigated and developed, including integrated quantum circuits, sources and detectors [7]. In contrast to waveguides, microring resonators [8] with narrow resonances and high Q-factors, offer an improvement in photon-pair generation efficiency, as well as a narrow photon-pair bandwidth, making them compatible with quantum optical devices (e.g. high temporal-resolution single-photon detectors and quantum memories). Most importantly, in contrast to non-resonant waveguides, where individuals photon-pairs, featured by one signal/idler frequency pair, are generally produced, resonant nonlinear cavities (e.g., microring resonators) allow the generation of correlated photon-pairs on multiple signal/idler frequency channels [9], due to their periodic and equidistant resonance structure.

AB - Entangled photon-pair sources are key building blocks towards the realization of applications in quantum information processing [1], quantum communications [2], as well as imaging and sensing with resolutions exceeding the classical limit [3]. The generation of, e.g. polarization, time-energy and time-bin entangled photon-pairs has been demonstrated using spontaneous parametric down-conversion (SPDC) in nonlinear second-order media, as well as spontaneous four-wave mixing (SFWM) in third-order nonlinear media. Specifically, nonlinear (third-order) interactions in on-chip microring resonators have been widely used to achieve classical frequency combs [4], mode-lock lasers [5], signal processing [6], etc. Integrated photonics can also find applications for quantum state generation in compact, scalable and efficient devices, required for future optical quantum circuits. In particular, solutions focusing on an integrated (on-chip) approach have been recently investigated and developed, including integrated quantum circuits, sources and detectors [7]. In contrast to waveguides, microring resonators [8] with narrow resonances and high Q-factors, offer an improvement in photon-pair generation efficiency, as well as a narrow photon-pair bandwidth, making them compatible with quantum optical devices (e.g. high temporal-resolution single-photon detectors and quantum memories). Most importantly, in contrast to non-resonant waveguides, where individuals photon-pairs, featured by one signal/idler frequency pair, are generally produced, resonant nonlinear cavities (e.g., microring resonators) allow the generation of correlated photon-pairs on multiple signal/idler frequency channels [9], due to their periodic and equidistant resonance structure.

UR - http://www.scopus.com/inward/record.url?scp=85029360019&partnerID=8YFLogxK

U2 - 10.1109/PHOSST.2017.8012710

DO - 10.1109/PHOSST.2017.8012710

M3 - Conference contribution

AN - SCOPUS:85029360019

T3 - Summer Topicals Meeting Series, SUM 2017

SP - 181

EP - 182

BT - Summer Topicals Meeting Series, SUM 2017

PB - Institute of Electrical and Electronics Engineers Inc.

T2 - 2017 IEEE Photonics Society Summer Topicals Meeting Series, SUM 2017

Y2 - 10 July 2017 through 12 July 2017

ER -