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

Plug-and-Play Generation and Manipulation of Squeezing on Chip

François Mondain, Tommaso Lunghi, Alessandro Zavatta, Élie Gouzien, Florent Doutre, Marc de Micheli, Sébastien Tanzilli, Virginia D’Auria

Published Jun 1, 2019• 0 citations
Publisher

Abstract

Summary form only given. Squeezed light is a quantum feature which exhibits noise properties below the shot noise level (SNL), i.e. the ultimate limit for classical intensity measurements. This characteristic makes squeezing a good candidate for a large variety of applications encompassing metrology, quantum processing and communication [1]. Up to date, squeezed light is mostly generated by means of bulk optical parametric oscillators, which require complex stabilisation techniques [2], and detected with bulk homodyne like interferometers in free space, thus implying delicate alignement and spatial mode-matching procedures. These constraints demand new strategies for developing compact and easy-to-align squeezing experiments [3]. Our work addresses these issues by demonstrating a compact, versatile, telecom-compliant and easy-to-handle squeezing experiment by merging integrated optics and off-the-shelf fibred optical components. The squeezing generation and the homodyne interferometric part are fully integrated on a single chip (see Fig.1(a)), with no significant loss between these two stages and no spatial mode matching concerns. Moreover, with the only exception of homodyne photodiodes, all the other building blocks of our experiment are realized by means of guided-wave components.

DOI
10.1109/cleoe-eqec.2019.8871809

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Summary form only given. Squeezed light is a quantum feature which exhibits noise properties below the shot noise level (SNL), i.e. the ultimate limit for classical intensity measurements. This characteristic makes squeezing a good candidate for a large variety of applications encompassing metrology, quantum processing and communication [1]. Up to date, squeezed light is mostly generated by means of bulk optical parametric oscillators, which require complex stabilisation techniques [2], and detected with bulk homodyne like interferometers in free space, thus implying delicate alignement and spatial mode-matching procedures. These constraints demand new strategies for developing compact and easy-to-align squeezing experiments [3]. Our work addresses these issues by demonstrating a compact, versatile, telecom-compliant and easy-to-handle squeezing experiment by merging integrated optics and off-the-shelf fibred optical components. The squeezing generation and the homodyne interferometric part are fully integrated on a single chip (see Fig.1(a)), with no significant loss between these two stages and no spatial mode matching concerns. Moreover, with the only exception of homodyne photodiodes, all the other building blocks of our experiment are realized by means of guided-wave components.
In the context of quantum communication and technologies squeezed states of light represent a crucial resource. Nevertheless, their generation and detection usually demand complex bulk systems, hardly compatible with out-of-the-laboratory realizations. In view of future practical applications, we present a compact and easy-to-use set-up exploiting the association of commercial plug-and-play fibre components and integrated optics on lithium niobate for the generation and detection of squeezed light at a telecom wavelength. Squeezed light exhibits a reduced quantum noise of -2.00 ± 0.05 dB below the shot-noise level in a single-pass configuration.
We demonstrate a squeezing experiment exploiting the association of integrated optics and telecom technology as key features for compact, stable, and practical continuous variable quantum optics. In our setup, squeezed light is generated by single pass spontaneous parametric down conversion on a lithium niobate photonic circuit and detected by an homodyne detector whose interferometric part is directly integrated on the same platform. The remaining parts of the experiment are implemented using commercial plug-and-play devices based on guided-wave technologies. We measure, for a CW pump power of 40\,mW, a squeezing level of −2.00±0.05-2.00\pm0.05−2.00±0.05\,dB, (antisqueezing +2.80±0.05+2.80\pm0.05+2.80±0.05\,dB) thus confirming the validity of our approach and opening the way toward miniaturized and easy-to-handle continuous variable based quantum systems.
Quantum optical technologies promise advances in sensing, computing, and communication. A key resource is squeezed light, where quantum noise is redistributed between optical quadratures. We introduce a monolithic, chip-scale platform that exploits the χ (2) nonlinearity of a thin-film lithium niobate (TFLN) resonator device to efficiently generate squeezed states of light. Our system integrates all essential components—except for the laser and two detectors—on a single chip with an area of one square centimeter, reducing the size, operational complexity, and power consumption associated with conventional setups. Using the balanced homodyne measurement subsystem that we implemented on the same chip, we measure a squeezing of 0.55 decibels and an anti-squeezing of 1.55 decibels. We use 20 milliwatts of input power to generate the parametric oscillator pump field by using second harmonic generation on the same chip. Our work represents a step toward compact and efficient quantum optical systems posed to leverage the rapid advances in integrated nonlinear and quantum photonics.
Squeezed light underpins quantum-enhanced sensing and continuous-variable quantum information processing, and integrated photonics offers a route to producing it at scale. Universal to these applications are squeezed-light generation and measurement. Importantly, quantum measurements serve not only as readout but also as active operations in quantum-state evolution. However, integrating squeezed-light generation and photodetection on the same photonic chip has remained challenging because they impose fundamentally conflicting material requirements: low optical loss to preserve quantum correlations, but efficient photon absorption for photodetection. Here, we demonstrate squeezed-light generation, routing, and balanced homodyne detection integrated on a single photonic chip through heterogeneous integration. A two-mode squeezed quantum microcomb comprising 34 quantum modes is measured with approximately 3 dB squeezing. Our work establishes a scalable architecture for fully integrated squeezed-light quantum photonic systems, unifying quantum-state generation, processing, and detection on a single chip.
We demonstrate, for the first time, the realization of an entirely guided-wave squeezing experiment at a telecom wavelength. The state generation relies on waveguide non-linear optics technology while squeezing collection and transmission are implemented by using only telecom fibre components. We observe up to −1.83±0.05-1.83\pm0.05−1.83±0.05 dB of squeezing emitted at 1542 nm in CW pumping regime. The compactness and stability of the experiment, compared to free-space configurations, represent a significant step towards achieving out-of-the-lab CV quantum communication, fully compatible with existing telecom fibre networks. We believe that this work stands as a promising approach for real applications as well as for "do-it-yourself" experiments
Integration of quantum optical technique on-chip is crucial for large scale applications of quantum technology, which were proven in a free space environment to be superior to the corresponding classical technology. Squeezed states of light can be used for enhancing the sensitivity of quantum sensors and for fault-tolerant quantum computing. Although chip-based squeezed light generation has advanced significantly, practical impact remains limited because coupling losses between the chip and off-chip detectors destroy delicate quantum correlations, restricting the amount of observed squeezing. Here, we overcome this limitation by implementing the idea of on-chip quantum measurement with the aid of a parametric amplifier and applying it to the squeezed state generated by a silicon nitride (SiN) microring resonator. In our scheme, two matched SiN micro-rings are sequentially constructed. The first ring generates a squeezed state, whereas the second ring acts as a high-gain parametric amplifier (PA) that measures the squeezed state before the light experiences significant off-chip loss. This architecture is inherently loss-tolerant: the amplifier elevates the quantum noise well above the vacuum level, making the measurement insensitive to downstream losses. We directly observe a quantum noise reduction of 4.6 dB from the first ring, despite a chip-to-fiber coupling loss exceeding 5 dB. This work also demonstrates the first monolithic SU(1,1) interferometer with an estimated 5 dB signal-to-noise enhancement compared to traditional linear interferometers, and thus establishes a practical pathway for chip-based quantum sensors.