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Photorefractive Effect in Linbo 3 Photorefractive effect in LiNbO 3 -based integrated-optical circuits for continuous variable experiments François Mondain, Floriane Brunel, Xin Hua, Elie Gouzien, Alessandro Zavatta, Tommaso Lunghi, Florent Doutre, Marc de Micheli, Sébastien Tanzilli, Virginia d’Auria To cite this version: François Mondain, Floriane Brunel, Xin Hua, Elie Gouzien, Alessandro Zavatta, et al.. Photorefrac- tive effect in LiNbO 3 -based integrated-optical circuits for continuous variable experiments. Optics Express, Optical Society of America - OSA Publishing, 2020. hal-02908852 HAL Id: hal-02908852 https://hal.archives-ouvertes.fr/hal-02908852 Submitted on 29 Jul 2020 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Photorefractive effect in LiNbO3-based integrated-optical circuits for continuous variable experiments Fran¸coisMondain,1 Floriane Brunel,1 Xin Hua,1 Elie´ Gouzien,1 Alessandro Zavatta,2, 3 Tommaso Lunghi,1 Florent Doutre,1 Marc P. De Micheli,1 S´ebastienTanzilli,1 and Virginia D'Auria1, ∗ 1Universit´eC^oted'Azur, CNRS, Institut de Physique de Nice (INPHYNI), UMR 7010, Parc Valrose, 06108 Nice Cedex 2, France. 2Istituto Nazionale di Ottica (INO-CNR) Largo Enrico Fermi 6, 50125 Firenze, Italy 3LENS and Department of Physics, Universit`adi Firenze, 50019 Sesto Fiorentino, Firenze, Italy (Dated: July 23, 2020) We investigate the impact of photorefractive effect on lithium niobate integrated quantum pho- tonic circuits dedicated to continuous variable on-chip experiments. The circuit main building blocks, i.e. cavities, directional couplers, and periodically poled nonlinear waveguides are studied. This work demonstrates that, even when the effect of photorefractivity is weaker than spatial mode hopping, they might compromise the success of on-chip quantum photonics experiments. We de- scribe in detail the characterization methods leading to the identification of this possible issue. We also study to which extent device heating represents a viable solution to counter this effect. We focus on photorefractive effect induced by light at 775 nm, in the context of the generation of non-classical light at 1550 nm telecom wavelength. Keywords: Quantum communication, Continuous variables, Nonlinear integrated photonics, Lithium niobate I. INTRODUCTION resulting space-charge field leads to a refractive index modification that changes the spatial beam profile of the With the development of quantum information tech- guided mode [8]. This can cause, in multimode waveg- nologies, photonic circuits are attracting an increasing uides, a coupling between the spatial modes (mode hop- interest as platforms for future out-of-laboratory realiza- ping) [9, 10]. Metal doping (magnesium, zinc, indium, tions. Strong light confinement in waveguides guarantees or hafnium) can be employed to mitigate photorefrac- efficient quantum state generation and manipulation in tivity but the fabrication techniques are not yet mature miniaturized structures which enables a progressive in- enough for being used in complex circuits [11, 12]. Pho- crease in architecture complexity thanks to high system torefractive effect is partially or completely suppressed stability and scalability [1, 2]. by operating undoped congruent LiNbO3 at high work- ing temperatures [13], so as to increase charges' mobility. Lithium niobate (LiNbO3) waveguides are particularly well adapted to quantum photonics, featuring easy in- However, higher temperature becomes rapidly unprac- and out-coupling to single-mode fibers, high nonlinear tical and a compromise must be found between pump frequency conversion efficiencies, electro-optical proper- power and device temperature. ties, and low propagation losses [3]. Largely used in single This paper bridges material science and quantum pho- tonics aspects. It investigates LiNbO photonic circuits photon regime, LiNbO3 chips are now moving also toward 3 applications to continuous variable (CV) quantum optics, in working conditions that, although below the appear- where quantum information is coded on light continuous ance of mode hopping, are submitted to photorefrac- spectrum observables. CV quantum states produced at tive effect. We study the impact of photorefractivity telecom wavelengths (around 1550 nm) for quantum com- on the main building blocks of CV experiments in sit- munication and computing [4] can be deterministically uations where the induced alteration is weak and by performing dedicated tests on the components. We fo- produced in LiNbO3 by spontaneous parametric down conversion (SPDC) of near-infrared light (775 nm) [5] and cus on the on-chip generation and detection of squeezed arXiv:2007.11375v1 [quant-ph] 22 Jul 2020 unambiguously discriminated by on-chip homodyne de- light, i.e. of optical quantum states exhibiting a noise tection [6, 7]. In comparison to single photon regime, level below the classical limit on one of their CV observ- CV experiments require higher pump powers at the in- ables [14]. Squeezed states lie at the very heart of many CV quantum-information protocols and are crucial for put of the downconverters. In such a condition, LiNbO3 is likely to be affected by photorefractive effect: impu- the heralded generation of non-Gaussian optical states rities and defect centers in the crystal cause a small ab- as required for universal quantum computing [4]. At the sorption of the light traveling along the waveguide. The same time, they are very sensitive to losses as well as to photogenerated charges move out of the illuminated area generation or detection imperfections, hence they repre- and get trapped at the edges of the waveguide. The sent an extremely pertinent case-study for the analysis of unwanted effects occurring in integrated photonic sys- tems. In the following, we illustrate the consequences of photorefractive effect on crucial elements of squeez- ∗ [email protected] ing experiments, such as integrated cavities, directional 2 couplers, and PPLN sources, components having already been successfully implemented on LiNbO3 CV complex photonic circuits [6, 7, 15]. We will highlight, as a func- tion of the pump power level and chip temperature, the careful optimization necessary to avoid a degradation of the squeezing. FIG. 1. Schematics of the characterization setup used to in- II. SAMPLE FABRICATION AND vestigate photorefractivity in LiNbO3 quantum photonic cir- CHARACTERIZATION SETUP cuits. The probe beam is delivered by a EXFO T100S-HP tunable laser; the pump by a M-Squared SolsTiS laser. PC: Ion-diffusion currently represents the most reliable fiber polarization controllers. WDM: fiber wavelength divi- technique to fabricate photonic integrated circuits on sion multiplexer. SUT: sample under test, i.e. integrated cav- ity, directional coupler or periodically poled nonlinear waveg- LiNbO3 [16]. Depending on the specific fabrication pro- uide. Light sensors are Coherent OP-2 Vis and OP-2 IR. cedure, the sensitivity to photorefractive effect varies. Residual pump power on the probe beam detector is avoided Proton-exchanged (PE) waveguides exhibit the highest thanks to the dichroic mirror (DMLP950T-Thorlabs), whose robustness to photorefractivity but suffer from a strong transmission at 775 nm is less than 0.1%. Isolators after the degradation of electro-optic and nonlinear optic proper- probe and the pump lasers are not represented on the scheme. ties that make them not suitable for integrating complex circuits. Annealed proton-exchanged (APE) and reverse proton-exchanged (RPE) waveguides allow to partially operated in continuous wave regime (CW) and have their recover the material properties at the price of higher sen- polarization independently controlled. At the output of sitivity to photorefractive effect. Eventually, titanium in- the SUT, light is collected by a lens, its spectral compo- diffused waveguides benefit from non-degraded LiNbO3 nents separated using a dichroic mirror, and focused onto properties but are strongly affected by photorefractivity, suitable photodetectors. The temperature of the system because of lower dark conductivity [9, 17]. is stabilized by an active loop with an error of ±5 mK. In this context, soft proton exchange (SPE) technique is We note that in our working conditions, photothermal particularly convenient for quantum photonics, both in drift only induces changes of ∼ 10−7 /K in the refractive single photon [3] and CV regimes [7]: it prevents degra- index [20]; this effect can be neglected compared to the dation of the material properties during the manufac- one induced by photorefractivity, that is approximately turing process leading to nonlinear efficiency better than three order of magnitude more important (see below). those of APE structures. In addition, it allows higher refractive index jumps providing a more efficient optical confinement with respect to RPE [3]. III. CAVITY EFFECT In this work, we will explore photorefractive effects in SPE waveguides. In this regard we note that photore- fractivity of SPE structures is close to the one observed A. Waveguide cavity made of chip's end-facets in APE and RPE
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