Birgit Stiller’s research while affiliated with Friedrich-Alexander-University Erlangen-Nürnberg and other places

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Publications (146)


Optoacoustic Entanglement in a Continuous Brillouin-Active Solid State System
  • Article
  • Full-text available

November 2024

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8 Reads

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3 Citations

Physical Review Letters

Changlong Zhu

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Claudiu Genes

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Birgit Stiller

Entanglement in hybrid quantum systems comprised of fundamentally different degrees of freedom, such as light and mechanics, is of interest for a wide range of applications in quantum technologies. Here, we propose to engineer bipartite entanglement between traveling acoustic phonons in a Brillouin active solid state system and the accompanying light wave. The effect is achieved by applying optical pump pulses to state-of-the-art waveguides, exciting a Brillouin Stokes process. This pulsed approach, in a system operating in a regime orthogonal to standard optomechanical setups, allows for the generation of entangled photon-phonon pairs, resilient to thermal fluctuations. We propose an experimental platform where readout of the optoacoustics entanglement is done by the simultaneous detection of Stokes and anti-Stokes photons in a two-pump configuration. The proposed mechanism presents an important feature in that it does not require initial preparation of the quantum ground state of the phonon mode. Published by the American Physical Society 2024

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Brillouin-based storage of QPSK signals with fully tunable phase retrieval

October 2024

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8 Reads

Olivia Saffer

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Jesús Humberto Marines Cabello

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Steven Becker

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[...]

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Birgit Stiller

Photonic memory is an important building block to delay, route and buffer optical information, for instance in optical interconnects or for recurrent optical signal processing. Photonic-phononic memory based on stimulated Brillouin-Mandelstam scattering (SBS) has been demonstrated as a coherent optical storage approach with broad bandwidth, frequency selectivity and intrinsic nonreciprocity. Here, we experimentally demonstrated the storage of quadrature-phase encoded data at room temperature and at cryogenic temperatures. We store and retrieve the 2-bit states {00,01,10,11}\{00, 01, 10, 11\} encoded as optical pulses with the phases {0,π/2,π,3π/2}\{0, {\pi}/2 , {\pi}, 3{\pi}/2\} - a quadrature phase shift keying (QPSK) signal. The 2-bit signals are retrieved from the acoustic domain with a global phase rotation of π{\pi}, which is inherent in the process due to SBS. We also demonstrate full phase control over the retrieved data based on two different handles: by detuning slightly from the SBS resonance, or by changing the storage time in the memory scheme we can cover the full range [0,2π)[0, 2{\pi}). At a cryogenic temperature of 3.9 K, we have increased readout efficiency as well as gained access to longer storage times, which results in a detectable signal at 140 ns. All in all, the work sets the cornerstone for optoacoustic memory schemes with phase-encoded data





Brillouin light storage for 100 pulse widths

May 2024

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85 Reads

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3 Citations

Signal processing based on stimulated Brillouin scattering (SBS) is limited by the narrow linewidth of the optoacoustic response, which confines many Brillouin applications to continuous wave signals or optical pulses longer than several nanoseconds. In this work, we experimentally demonstrate Brillouin interactions at the 150 ps time scale and a delay for a record 15 ns which corresponds to a delay of 100 pulse widths. This breakthrough experimental result was enabled by the high local gain of the chalcogenide waveguides as the optoacoustic interaction length reduces with pulse width. We successfully transfer 150 ps-long pulses to traveling acoustic waves within a Brillouin-based memory setup. The information encoded in the optical pulses is stored for 15 ns in the acoustic field. We show the retrieval of eight amplitude levels, multiple consecutive pulses, and low distortion in pulse shape. The extension of Brillouin-based storage to the ultra-short pulse regime is an important step for the realization of practical Brillouin-based delay lines and other optical processing applications.


Schematic of the optoacoustic recurrent operator (OREO) and its proposed function in a recurrent optical NN
a An example of a photonic recurrent network with N layers Xⁿ, which are connected by a matrix operation Wⁿ. b The bi-directional perceptron contains an OREO and an activation function. OREO captures and links sequential information aD using a sound wave b, which is generated by SBS and controlled by an optical control pulse aC. The output of the acoustic recurrent neuron aD′\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${a}_{{{{{{{{\rm{D}}}}}}}}}^{{\prime} }$$\end{document} is fed into the next layer of the optical neural network. The blue arrow indicates the recurrent nature of one neuron. c Conceptional illustration of the SBS process with its interaction Hamiltonian Hint. The sound wave b carries the information of the neuron’s input and decays after the SBS process exponentially with the acoustic lifetime τac. d–g Illustration of three recurrent operations performed by OREO. d shows the initial situation with three data-control pulse pairs separated by a deadtime dt. The data and control pulses are launched from opposite sides into a photonic crystal fiber (PCF). e shows the system after the SBS-interaction of aD,1 and aC,1, which transfers energy from aD,1 to an acoustic wave b1. f shows the system after a second pulse pair has passed the PCF. The acoustic wave b1 connects the interaction of aD,2 and aC,2 with the previous one, while the SBS process transfers information from aD,2 into b2. g highlights the acoustic link created by OREO between three optical pulse pairs.
Observing OREO’s optoacoustic linking and recurrent dropout capabilities
a Schematic illustration of the amplitude sweep that investigates how different optical states are passed between the optical data pulses aD,i via an acoustic wave b. b–d Experimental results of the amplitude sweep. While aD,i,  i = 1, 2 is changed, its impact on the subsequent pulses aD,j,  j > i is studied for different deadtimes dt. Each SBS process creates an acoustic wave bi, which interferes with pre-exisiting ones bk,  k < i, eventually. We mark the links aD,i → aD,j with a +, −, and ⋅, when they experienced an enhancement, a reduction and an annihilation of the SBS process, respectively. We added the depletion of a single pulse interaction (SPI) as reference. e Schematic illustration of the pulse configuration used to study the OREO’s feature to implement a recurrent dropout. f–h Experimental results of OREO’s recurrent dropout capabilities.
Applying OREO as an acceptor to predict patterns of optical pulses
a Schematic illustration of how the acoustic link can be used by an optical evaluation pulse (Eval) to predict a pattern from optical pulses, which have been launched into the optical fiber before. The example shows a ab-pattern. Note that the output pulses a′\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${a}^{{\prime} }$$\end{document}, and b′\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${b}^{{\prime} }$$\end{document} are not shown. The control pulses aC,i are numbered according to the time sequence of the data pulses as they enter the sample. b, c Confusion matrix of a Random Forest classifier (RFC) which is used to classify the experimental data set with and without SBS. The RFC achieves an almost perfect classification rate as soon as OREO provides the recurrent feedback. d Schematic illustration of the three pulse pattern recognition task. This case shows the cab-pattern. Note that the output pulses c′\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${c}^{{\prime} }$$\end{document}, a′\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${a}^{{\prime} }$$\end{document}, and b′\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${b}^{{\prime} }$$\end{document} are not shown. e Shows the confusion matrix of the RFC, using 30% of the experimentally obtained data set for training. The RFC achieves an accuracy of 45% and outperforms a simple guess by 11-times. The accuracy of the RFC is mostly limited by experimental precision. f RFC confusion matrix using simulated data to study OREO’s performance with experimental optimization. In this case, we can achieve an accuracy of 92%. The simulation are based on a frequency matched SBS process and is described in more detail in the supplementary material.
An optoacoustic field-programmable perceptron for recurrent neural networks

April 2024

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74 Reads

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3 Citations

Recurrent neural networks (RNNs) can process contextual information such as time series signals and language. But their tracking of internal states is a limiting factor, motivating research on analog implementations in photonics. While photonic unidirectional feedforward neural networks (NNs) have demonstrated big leaps, bi-directional optical RNNs present a challenge: the need for a short-term memory that (i) programmable and coherently computes optical inputs, (ii) minimizes added noise, and (iii) allows scalability. Here, we experimentally demonstrate an optoacoustic recurrent operator (OREO) which meets (i, ii, iii). OREO contextualizes the information of an optical pulse sequence via acoustic waves. The acoustic waves link different optical pulses, capturing their information and using it to manipulate subsequent operations. OREO’s all-optical control on a pulse-by-pulse basis offers simple reconfigurability and is used to implement a recurrent drop-out and pattern recognition of 27 optical pulse patterns. Finally, we introduce OREO as bi-directional perceptron for new classes of optical NNs.



Eavesdropper localization for quantum and classical channels via nonlinear scattering

January 2024

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25 Reads

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2 Citations

Optical fiber networks are part of the important critical infrastructure and known to be prone to eavesdropping attacks. Hence, cryptographic methods have to be used to protect communication. Quantum key distribution (QKD), at its core, offers information theoretical security based on the laws of physics. In deployments, one has to take into account practical security and resilience. The latter includes the localization of a possible eavesdropper after an anomaly has been detected by the QKD system to avoid denial-of-service. Here, we present an approach to eavesdropper location that can be employed in quantum as well as classical channels using stimulated Brillouin scattering. The tight localization of the acoustic wave inside the fiber channel using correlated pump and probe waves allows discovery of the coordinates of a potential threat within centimeters. We demonstrate that our approach outperforms conventional optical time-domain reflectometry (OTDR) in the task of localizing an evanescent outcoupling of 1 %\,{\% } % with centimeter precision inside standard optical fibers. The system is furthermore able to clearly distinguish commercially available standard SMF28 from different manufacturers, paving the way for fingerprinted fibers in high-security environments.


Citations (37)


... To address these challenges, optomechanical cooling via sideband cooling in a continuous system has been demonstrated, using SBS to cool a continuum of traveling wave phonons in a waveguide by tens of kelvins (Otterstrom et al., 2018b). These achievements open the possibility of developing versatile light-matter interfaces (Hammerer et al., 2010) based on SBS achieving, for example, optomechanical entanglement (Zhu et al., 2024) or nonlinear photon interactions (Zoubi and Hammerer, 2017). ...

Reference:

Slow light through Brillouin scattering in continuum quantum optomechanics
Optoacoustic Entanglement in a Continuous Brillouin-Active Solid State System

Physical Review Letters

... in the previous sections. We first note (see Appendix) that the field amplitudes have all been normalised to the amplitude of the incident pump, so that an amplitude of A 0 = 1.0 corresponds to an input power of 1.0 W. Achieving powers of this order of magnitude is certainly feasible, with typical Brillouin experiments having peak powers of around 500 mW for CW or ns pulses [5], or far higher for shorter pulses [31]. The power levels discussed throughout this paper are therefore achievable in contemporary Brillouin experiments. ...

Brillouin light storage for 100 pulse widths

... The demonstrated complete control over the phase of the retrieved data can prove very useful in advanced optical signal processing schemes and neuromorphic network implementations. 39,40 This enhances the body of work surrounding Brillouin-based memory and paves the way for optical memory schemes for phase-encoded data. ...

An optoacoustic field-programmable perceptron for recurrent neural networks

... Especially due to the recent development in nanofabrication, a new breed of chip-based Brillouin-active waveguides with short length (∼cm) have been achieved experimentally [24], which enables coherent information transduction [25], information storage [26,27], and phonon cooling [28,29]. However, the next logical step after the experimental demonstration of Brillouin cooling [29][30][31] in continuum optomechanics is the observation of quantum optoacoustical entanglement. ...

Optoacoustic Cooling of Traveling Hypersound Waves

Physical Review Letters

... At the same time, quantum technology promises advanced sensing methods going strictly beyond the available methods using conventional technology [4]. Specifically in the domain of communication, the aspect of detection and localization of a possible eavesdropper has been studied from an applied perspective in the recent work [5], where the system concept is to identify the presence of an eavesdropper via a QKD protocol and then identify the location of the eavesdropper using frequency-modulated Brillouin optical correlation domain analysis. Another concept called "Quantum Alarm" has been investigated in [6], where an optical fiber data transmission system multiplexes the classical data signal stream with specific signals designed for eavesdropper detection. ...

Eavesdropper localization for quantum and classical channels via nonlinear scattering

... As described above, possible changes in the output spectra result from changes of the incoupling, which can in principle be eliminated by integrating the LCF into the fiber circuit in order to have an all-fiber system. Such integration has been recently achieved by one of the authors through a combination of liquid volume reduction by cooling, splicing and expansion 48 . This enables LCFs to be used in conventional fiber circuitry, opening up new applications in areas such as material research, life science and nonlinear optics. ...

Extreme thermodynamics in nanolitre volumes through stimulated Brillouin–Mandelstam scattering

Nature Physics

... To address this, we tapered fibers with dimensions 100/140 µm (Nexans Switzerland -1990) down to ∼57/80 µm using a heat-brush technique. Specifically, the method of manufacturing fiber tips is adapted from a conventional optical fiber tapering process for the fabrication of high transmission nanofibers [31,32]. The heat-brush technique consists of holding the 100/140 µm fiber on two plates and lighting a flame underneath to raise the temperature of the silica to its softening point. ...

Spin-orbit interaction in nanofiber-based Brillouin scattering

... Наприклад, для створення ефективних систем квантового зв'язку необхідне широке використання квантових повторювачів, здатних передавати інформацію на великі відстані без втрати якості сигналу. Також потрібно вирішити питання інтеграції квантових систем з існуючими класичними телекомунікаційними мережами [3,4]. ...

Quantum coherent control in pulsed waveguide optomechanics

Physical Review Research