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Research in Optical Sciences

Polarization entanglement engineering at telecom wavelengths

Florian Kaiser, Lutfi Arif Ngah, Amandine Issautier, Olivier Alibart, Anthony Martin, Sébastien Tanzilli

Published Jan 1, 2012• 0 citations
Publisher

Abstract

We report an efficient polarization entanglement engineering scheme based on a stabilized birefringent delay line. The scheme is capable of handling ultra narrowband photons making it compatible for multiplexing and quantum memory based applications.
DOI
10.1364/qim.2012.qt5a.5

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Entanglement has evolved from being a spooky interaction towards a key resource of real-life applications such as absolute secure communication. Today, quantum networking devices are commercially available, typically taking advantage of time-bin or polarisation entanglement, the latter one doubtlessly being easier to analyse thanks to interferometer free set-ups. The communication distance of such systems is generally limited to a few hundreds of kilometres due to intrinsic fibre transmission losses and imperfect detectors. It was shown that the communication distance can be greatly increased when combining entangled pairs of photons and quantum memories. But the narrow absorption bandwidth of current quantum memories is in contrary to the widely used broadband entanglement sources based on non linear inter- actions. More precisely, there is a lack of ultra narrowband sources in the telecom C-band, where fibre losses are minimal and high performance guided-wave optics are available. Here we introduce a high quality polarisation entanglement engineering scheme based on a birefringent de- lay line (BDL). This BDL is applied to generate polarization entanglement from a high efficiency ultra narrowband tele- com photon pair source where no polarisation entanglement is available initially.
Entanglement is a key resource for quantum infor- mation protocols. Low-loss optical fibers and reliable guided-wave components make it possible to create and distribute photonic entanglement in the telecom C-band of wavelengths (1530-1565 nm). Entanglement is easily produced using spontaneous parametric down-conversion (SPDC) in nonlinear crystals. Usual observables are time-bin and polarisation, the latter being easier to analyze, thanks to simple experimental apparatus, real-time fiber birefringence compensation, and the natural design of heralded quantum memories for this observable. In quantum networks, where telecom photons are used to distribute, and quantum memories to store, entanglement, the photonic spectral and memory acceptance bandwidths have to be matched. The latter ranges from a few MHz (cold atoms) to a few GHz (solid- state). In the following, we discuss a versatile polar- isation entangling scheme based on a birefringent delay line (BDL) that can be applied to photon bandwidths down to 25 MHz. We demonstrate such versatility by violating, by large amounts, the Bell inequalities for 3 different bandwidths: 25 MHz, 500 MHz, and 100 GHz.
During the last decade, quantum entanglement has paved the way out to of the lab modern applications such as quantum computation and communication. Today, small scale quantum networks exist already, but they are limited to a few 100 km distance, due to intrinsic fiber transmission losses and non perfect detectors. These networks are typically established using photon pair sources based on spontaneous parametric down conversion (SPDC). Widely used entanglement observables are time-bin and polarization, where the latter one is undoubtedly simpler to analyze due to lack of interferometric devices. It was shown recently, that introducing quantum memories (QM) between the communication parties could increase both communication speed and distance. Such memories already exist, but their narrow absorption bandwidth does not match the broadband emission spectrum of SPDC sources. Our report is twofold. First, we introduce a new polarization entanglement scheme based on a birefringent delay line (BDL). A pair of incoming photons is projected on a polarizing beam splitter (PBS), where vertically polarized photons travel along a polarization maintaining fiber loop accumulating a delay δ compared to horizontally polarized photons, which exit the BDL directly upon reflection at the PBS. Via post selection of only simultaneously arriving photon pair events, we create entangled states of the form α|H>_1|H>_2 + e^(iφ)β|V>_1 |V>_2. The probability amplitudes α and β are simply tuned by controlling the input pair's polarization and the phase φ can be varied by piezo fiber stretcher (PZT) in the delay line. Therefore, any superposition of the polarization entangled Bell states can be created. The scheme may also be used for entanglement distillation of non maximally entangled states, e.g. emitted by quantum dots. We will introduce all requirements needed to create entanglement from such a BDL. Second, we show how to apply this scheme to produce polarization entanglement from one of the most efficient photon pair generators, namely a periodically poled Lithium Niobate waveguide structure (PPLN/W), where the quasi phase matching is optimized for the type-0 SPDC interaction. The pair's wavelength is chosen in the standardized ITU-21 channel of the low loss telecom C-band and a fiber Bragg grating is applied to reduce the initial spectral bandwidth from 5 THz to 540 MHz, which is suitable for some solid-state quantum memories. Using the BDL, we create the maximally entangled states, with near perfect quality, which is proven by a violation of the Bell's inequalities by more than 29 standard deviations. We achieve a source spectral brightness of 211 narrowband polarization entangled pairs created per second, mW of pump power, and MHz of spectral bandwidth, coupled into a single mode fiber. This is on the same level as the best time-bin entanglement sources reported to date. The source is very practical due to the use of standard telecom fiber components. Moreover the choice for polarization instead of time-bin entanglement allows for simple state analysis using only rotating PBSs. This is a non negligible advantage, especially for narrowband photons with long coherence times, where time-bin analysis requires interferometer path length differences on the order of a few meters stabilized to a few tens of nanometers. Non unit visibilities are solely explained by the nonlinear character of our photon pair source, giving rise to double pair contributions. Applying this scheme to deterministic photon pair sources should result in perfect quality entanglement. We believe that our scheme should play an important role for future quantum networking applications.