Abstract

Spontaneous parametric down-conversion (SPDC) is a widely used method to generate entangled photons, enabling a range of applications from secure communication to tests of quantum physics. Integrating SPDC on a chip provides interferometric stability, allows to reduce a physical footprint, and opens a pathway to true scalability. However, dealing with different photon polarizations and wavelengths on a chip presents a number of challenging problems. In this work, we demonstrate an on-chip polarization beam-splitter based on z-cut titanium-diffused lithium niobate asymmetric adiabatic couplers (AAC) designed for integration with a type-II SPDC source. Our experimental measurements reveal unique polarization beam-splitting regime with the ability to tune the splitting ratios based on wavelength. In particular, we measured a splitting ratio of 17 dB over broadband regions (>60 nm) for both H- and V-polarized lights and a specific 50%/50% splitting ratio for a cross-polarized photon pair from the AAC. The results show that such a system can be used for preparing different quantum polarization-path states that are controllable by changing the phase-matching conditions in the SPDC over a broad band. Furthermore, we propose a fully integrated electro-optically tunable type-II SPDC polarization-path-entangled state preparation circuit on a single lithium niobate photonic chip.

Highlights

  • Lithium Niobate (LiNbO3) is a ferroelectric material with relatively large nonlinear-optic and electro-optic (EO) coefficients[1] and has been widely used in numerous applications including the implementation of EO intensity/ phase modulators[2], EO polarization-mode converters (PMCs)[3], optical wavelength converters such as optical parametric oscillators[4,5] and quantum light sources[6,7,8] that open a range of useful applications of LiNbO3 in quantum optics

  • Despite LiNbO3-based broadband adiabatic couplers designed for integration with type-0/type-I Spontaneous parametric down-conversion (SPDC) sources have been proposed and demonstrated[19,20], it still remains a problem on designing both polarization- and wavelength-dependent beam splitters in a fully integrated manner for a type-II SPDC source

  • Unlike narrow-band (MHz) photon pair generations via atomic[24] and atom-like[25] media with χ(3) (or χ(3):χ(3)) nonlinearity, this work focuses on the application of the χ(2) SPDC sources to integrated optical circuits over a broader band (THz)

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Summary

Introduction

Lithium Niobate (LiNbO3) is a ferroelectric material with relatively large nonlinear-optic and electro-optic (EO) coefficients[1] and has been widely used in numerous applications including the implementation of EO intensity/ phase modulators[2], EO polarization-mode converters (PMCs)[3], optical wavelength converters such as optical parametric oscillators[4,5] and quantum light sources[6,7,8] that open a range of useful applications of LiNbO3 in quantum optics. LiNbO3 is a popular substrate for constructing low-loss, high-quality optical waveguides, advantageous for realizing those photonic devices with high-efficiency and compatibility All these attractive features of LiNbO3 make it a promising platform for developing integrated quantum photonic circuits; the reviews of several important material platforms including LiNbO3 for implementing on-chip photon-pair generators and quantum photonic systems have been made elsewhere[9,10]. Despite LiNbO3-based broadband adiabatic couplers designed for integration with type-0/type-I SPDC sources have been proposed and demonstrated[19,20], it still remains a problem on designing both polarization- and wavelength-dependent beam splitters in a fully integrated manner for a type-II SPDC source Another typical issue in type-II phase-matched SPDC lies in the temporal walk-off between signal and idler caused by the birefringence of the material. The third section is realized experimentally, while the first two stages have been shown in previous works and are simulated numerically within the framework of this paper

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