OceansPub Date : 2023-06-26DOI: 10.1109/CLEO/Europe-EQEC57999.2023.10232671
H. Thiem, Daniel Brauda, Markus Schütz, B. Globisch, Miroslawa Malach
{"title":"Fiber-Coupled Tapered Amplifier in a Hermetic 14-Pin Butterfly Package Emitting 3 W at 780 nm and More than 2.5 W at 850 nm","authors":"H. Thiem, Daniel Brauda, Markus Schütz, B. Globisch, Miroslawa Malach","doi":"10.1109/CLEO/Europe-EQEC57999.2023.10232671","DOIUrl":"https://doi.org/10.1109/CLEO/Europe-EQEC57999.2023.10232671","url":null,"abstract":"The wavelength range around 780 nm and 850 nm is extensively used for both high resolution spectroscopy and quantum technology (QT). For example, the D2 transition of cesium (Cs) and the D2 transition of rubidium (Rb) lie within these wavelength ranges. [1], [2] For compact spectrometers with high resolution and especially for QT of the second generation, compact and long-term stable systems are a prerequisite for the breakthrough of the technology. [3] In this paper we demonstrate a miniaturized fiber-coupled tapered amplifier (mini TA), which combines high output power, excellent beam properties $(mathrm{M}^{2} < 2)$ and high coherence in 14-pin butterfly package with collimated output beam. To the best of our knowledge this is the first time demonstration of a fiber-coupled TA in this power range with a collimated output beam in a hermetically sealed package.","PeriodicalId":19477,"journal":{"name":"Oceans","volume":"42 1","pages":"1-1"},"PeriodicalIF":0.0,"publicationDate":"2023-06-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"81354359","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
OceansPub Date : 2023-06-26DOI: 10.1109/CLEO/Europe-EQEC57999.2023.10231882
Fatima El Moussawi, Matthias Hofer, Siddharth Sivankutty, Andrea Bertoncini, D. Labat, A. Cassez, G. Bouwmans, Rosa Cossart, O. Vanvincq, C. Liberale, Hervé Rigneault, E. Andresen
{"title":"Two-Photon Lensless Endoscopes with Multicore Fibers","authors":"Fatima El Moussawi, Matthias Hofer, Siddharth Sivankutty, Andrea Bertoncini, D. Labat, A. Cassez, G. Bouwmans, Rosa Cossart, O. Vanvincq, C. Liberale, Hervé Rigneault, E. Andresen","doi":"10.1109/CLEO/Europe-EQEC57999.2023.10231882","DOIUrl":"https://doi.org/10.1109/CLEO/Europe-EQEC57999.2023.10231882","url":null,"abstract":"The lensless endoscope represents the ultimate limit in miniaturization of imaging tools: an image can be transmitted by numerical or physical inversion of the mode scrambling process through a bare optical fiber. Lensless endoscopes featuring multicore fibers and spatial light modulators are well adapted for nonlinear imaging as they minimally distort ultrashort pulses in the time domain as opposed to multimode fibers [1]. And in earlier works, we had addressed the issues of imaging artifacts and bending sensitivity with an helically twisted multicore fiber with a sparse and aperiodic core layout in the transverse plane [2]. However sufficiently irradiating the sample plane remained a major challenge - particularly for the imaging of dim and challenging samples such as neurons in scattering media.","PeriodicalId":19477,"journal":{"name":"Oceans","volume":"43 1","pages":"1-1"},"PeriodicalIF":0.0,"publicationDate":"2023-06-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"81767209","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
OceansPub Date : 2023-06-26DOI: 10.1109/CLEO/Europe-EQEC57999.2023.10232225
P. Suret, M. Dufour, G. Roberti, G. El, F. Copie, S. Randoux
{"title":"Refraction of a Soliton by a Soliton Gas in a Recirculating Fiber Loop","authors":"P. Suret, M. Dufour, G. Roberti, G. El, F. Copie, S. Randoux","doi":"10.1109/CLEO/Europe-EQEC57999.2023.10232225","DOIUrl":"https://doi.org/10.1109/CLEO/Europe-EQEC57999.2023.10232225","url":null,"abstract":"Soliton gases (SGs) represent large random soliton ensembles in physical systems that exhibit integrable dynamics at the leading order. SGs have been recently evidenced in optical and in water wave experiments [1], [2]. Nowadays, the question of the collective dynamics and statistical properties of SGs is an active research topic in statistical mechanics [3], mathematical physics [4], nonlinear physics [5] and constitutes a chapter of turbulence theory termed integrable turbulence [6].","PeriodicalId":19477,"journal":{"name":"Oceans","volume":"2 1","pages":"1-1"},"PeriodicalIF":0.0,"publicationDate":"2023-06-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"82079862","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
OceansPub Date : 2023-06-26DOI: 10.1109/CLEO/Europe-EQEC57999.2023.10231535
Clémentine Rouvière, David Barral, Antonin Grateau, Giacomo Sorelli, Ilya Karuseichyk, M. Walschaers, Nicolas Treps
{"title":"Experimental Separation Estimation of Incoherent Optical Sources Reaching the Cramér-Rao Bound","authors":"Clémentine Rouvière, David Barral, Antonin Grateau, Giacomo Sorelli, Ilya Karuseichyk, M. Walschaers, Nicolas Treps","doi":"10.1109/CLEO/Europe-EQEC57999.2023.10231535","DOIUrl":"https://doi.org/10.1109/CLEO/Europe-EQEC57999.2023.10231535","url":null,"abstract":"Resolving light sources below the diffraction limit is a fundamental task both for astronomy and microscopy. Several recent works analysed this problem through the lens of quantum parameter estimation theory and proved that the separation between two point sources can be estimated at the quantum limit using intensity measurements after spatial-mode demultiplexing. We implement this technique and provide an optimal estimator based on a linear combination of demultiplexed intensity measurements [1]–[3]. Our experimental setup (see Fig. 1 (left)) allows for the generation of the images of two sources, with tunable mutual coherence, as well as for spatial mode demultiplexing to estimate their separation [4].","PeriodicalId":19477,"journal":{"name":"Oceans","volume":"41 1","pages":"1-1"},"PeriodicalIF":0.0,"publicationDate":"2023-06-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"78822694","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
OceansPub Date : 2023-06-26DOI: 10.1109/CLEO/Europe-EQEC57999.2023.10232096
R. Duquennoy, M. Colautti, P. Lombardi, R. Emadi, C. Toninelli
{"title":"Quantum Interference with Single Molecules: Steps Towards a Competitive Single-Photon Source","authors":"R. Duquennoy, M. Colautti, P. Lombardi, R. Emadi, C. Toninelli","doi":"10.1109/CLEO/Europe-EQEC57999.2023.10232096","DOIUrl":"https://doi.org/10.1109/CLEO/Europe-EQEC57999.2023.10232096","url":null,"abstract":"Single molecules of polyaromatic hydrocarbons (PAH) in suitable host matrices are known for emitting with high quantum efficiency in very narrow and stable zero-phonon lines (ZPL) [1]. For our experiments we used dibenzotherrylene (DBT) molecule inserted as impurity in anthracene (Ac) nanocrystals, dispersed on a gold substrate and cooled down to 3 K in a closed-cycle cryostat. DBT in Ac features a single-photon dipole-allowed transition around 784 nm. Each molecule is namely identical but environmental conditions like local trapped charges or crystal strain can shift the frequency of its transition in a range of approximately 1 nm [2]. Those static differences alongside any instantaneous interaction with the environment can degrade the ability of the emitted photons to undergo two-photon interference (TPI).","PeriodicalId":19477,"journal":{"name":"Oceans","volume":"2 1","pages":"1-1"},"PeriodicalIF":0.0,"publicationDate":"2023-06-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"78946411","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
OceansPub Date : 2023-06-26DOI: 10.1109/cleo/europe-eqec57999.2023.10231441
George Kountouris, Lea Vestergaard, Anne Sofie Darket, J. Mørk, P. Kristensen
{"title":"A Lithographically Defined Quantum Dot with Simultaneous Sub-Wavelength Confinement of Light","authors":"George Kountouris, Lea Vestergaard, Anne Sofie Darket, J. Mørk, P. Kristensen","doi":"10.1109/cleo/europe-eqec57999.2023.10231441","DOIUrl":"https://doi.org/10.1109/cleo/europe-eqec57999.2023.10231441","url":null,"abstract":"Deterministic fabrication of quantum dots in optical devices is a long-standing challenge for future integrated photonics and electronics applications. Current approaches typically rely on alignment or transfer techniques [1], but the scalability is limited by the unavoidable introduction of uncertainty in both the geometry and the positioning of the dots. In this work, we present a lithographically defined quantum dot integrated with a nanostructured optical cavity with sub-wavelength confinement of light. The design is based on an optical bowtie cavity [2] in an InP dielectric membrane with an embedded InGaAsP quantum well. By modifying the central bowtie geometry, the structure can be made to support localized electron-hole states in the region of the optical hotspot. The concept is illustrated in Fig. 1.","PeriodicalId":19477,"journal":{"name":"Oceans","volume":"13 1","pages":"1-1"},"PeriodicalIF":0.0,"publicationDate":"2023-06-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"78948994","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
OceansPub Date : 2023-06-26DOI: 10.1109/CLEO/Europe-EQEC57999.2023.10231402
A. de Andres, S. Bhadoria, J. Marmolejo, A. Muschet, Peter Fischer, A. Gonoskov, Dag Hanstorp, Mattias Marklund, Laszlo Veisz
{"title":"Vacuum Laser Acceleration of Electrons Injected from Nanotips","authors":"A. de Andres, S. Bhadoria, J. Marmolejo, A. Muschet, Peter Fischer, A. Gonoskov, Dag Hanstorp, Mattias Marklund, Laszlo Veisz","doi":"10.1109/CLEO/Europe-EQEC57999.2023.10231402","DOIUrl":"https://doi.org/10.1109/CLEO/Europe-EQEC57999.2023.10231402","url":null,"abstract":"Vacuum laser acceleration (VLA) is a paradigm that utilizes the strong fields of focused laser light to accelerate electrons in vacuum. Despite its conceptual simplicity and a large existing collection of theoretical studies, realizing VLA in practice has proven remarkably challenging due to the difficulties associated with efficient injection: the electrons to be accelerated must be pre-energized and temporally compressed below an optical half-cycle before timely entering the rapidly oscillating fields of the laser. Therefore, only a handful of experiments have been published up to date, and a knowledge gap remains [1–3].","PeriodicalId":19477,"journal":{"name":"Oceans","volume":"358 1","pages":"1-1"},"PeriodicalIF":0.0,"publicationDate":"2023-06-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"76311044","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
OceansPub Date : 2023-06-26DOI: 10.1109/cleo/europe-eqec57999.2023.10232569
P. Micheletti, U. Senica, A. Forrer, S. Cibella, Guido Torrioli, Martin Frankié, J. Faist, Mattias Beckl, G. Scalari
{"title":"THz Optical Solitons in Planarized Quantum Cascade Double Ring Lasers","authors":"P. Micheletti, U. Senica, A. Forrer, S. Cibella, Guido Torrioli, Martin Frankié, J. Faist, Mattias Beckl, G. Scalari","doi":"10.1109/cleo/europe-eqec57999.2023.10232569","DOIUrl":"https://doi.org/10.1109/cleo/europe-eqec57999.2023.10232569","url":null,"abstract":"Quantum Cascade Lasers (QCL) based on cicular cavities are rapidly progressing as possible sources pf optical solitons [1], [2]. We report soliton formation in dispersion compensated THz ring QCLs [1]. The laser cavity consists of two concentric double metal ring waveguides, designed to support a symmetric and anti-symmetric super-mode where the global GVD is respectively enhanced or decreased [3](Fig. 1 a-b). The two super-modes feature different overlap factors, therefore the laser naturally selects the anti-symmetric super-mode which exhibits negative GVD.","PeriodicalId":19477,"journal":{"name":"Oceans","volume":"73 1","pages":"1-1"},"PeriodicalIF":0.0,"publicationDate":"2023-06-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"76431312","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
OceansPub Date : 2023-06-26DOI: 10.1109/CLEO/Europe-EQEC57999.2023.10232045
V. Sorianello, A. Montanaro, M. Giambra, Nadia Ligato, Wolfgang Templ, P. Galli, Marco Romagnoli
{"title":"Graphene Photonics Nested Mach-Zehnder Modulator for Advanced Modulation Formats","authors":"V. Sorianello, A. Montanaro, M. Giambra, Nadia Ligato, Wolfgang Templ, P. Galli, Marco Romagnoli","doi":"10.1109/CLEO/Europe-EQEC57999.2023.10232045","DOIUrl":"https://doi.org/10.1109/CLEO/Europe-EQEC57999.2023.10232045","url":null,"abstract":"Graphene is a 2D gapless material with electrically tunable optical properties that can operate over an ultra-wide optical spectrum. Graphene wafer scale films can be grown through chemical vapor deposition (CVD) and transferred on passive waveguide platforms at low temperature [1]. Photonic integrated devices for efficient and fast electro-absorption and electro-refraction modulation [2] have been demonstrated so far, as well as ultra-fast photodetection [3]. Graphene integrated photonics is an emerging technology with great potential for many photonic applications, from sensing to datacom/telecom [4]. Here, we show the first graphene photonic I/Q modulator based on a nested Mach-Zehnder loaded with $100 mu mathrm{m}$ long graphene EAMs, and demonstrate 40 Gb/s quadrature phase shift keying (QPSK) modulation. The device consists of a passive nested MZI where the child MZIs' arms are equipped with graphene EAMs and thermal phase shifters (TPS), while the parent arms are provided with only TPSs to set the quadrature phase shift $(pi/2)$. The principle of operation of the nested I/Q MZM consists in the generation of binary phase shift keying (BPSK) modulation at the outputs of the child MZMs obtained by driving the EAMs with differential signals [5], i.e. one with DATA signal and one with inverse DATA signal. By adding a constant $pi$ shift with the integrated TPS, the output is a perfectly symmetric BPSK. The output of the two child MZIs are then combined in the parent MZI which builds the QPSK signal from the two BPSKs after introducing a $(pi/2)$ phase shift with the TPS. We used a dual differential channels 100 GS/s DAC to generate the binary signals, properly amplified by two >40GHz dual channel driver amplifiers. Off-line DSP was performed to extract the QPSK constellation diagrams after coherent reception with a real-time oscilloscope.","PeriodicalId":19477,"journal":{"name":"Oceans","volume":"33 1","pages":"1-1"},"PeriodicalIF":0.0,"publicationDate":"2023-06-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"75968519","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
OceansPub Date : 2023-06-26DOI: 10.1109/CLEO/Europe-EQEC57999.2023.10232664
C. Sharp, Chaitanya K. Mididoddi, Philipp del Hougne, Simon Horsley, D. B. Phillips
{"title":"Steering Stable Light Fields Through Dynamic Scattering Media","authors":"C. Sharp, Chaitanya K. Mididoddi, Philipp del Hougne, Simon Horsley, D. B. Phillips","doi":"10.1109/CLEO/Europe-EQEC57999.2023.10232664","DOIUrl":"https://doi.org/10.1109/CLEO/Europe-EQEC57999.2023.10232664","url":null,"abstract":"The scattering of light was once thought to fundamentally limit imaging through opaque samples, as transmitted light becomes spatially scrambled. However, scattering effects can be captured by measurement of the Transmission Matrix (TM) - a linear matrix operator mathematically encapsulating how incident fields will be transformed into new fields on the other side of the scattering medium [1]. Knowledge of a scattering sample's TM enables the scrambling of optical fields to be reversed, and imaging through or inside opaque media becomes possible. Despite these successes, TM-based approaches generally require that the scattering medium remains completely static while the TM is measured and applied. Spatial control of light propagating through dynamic scattering systems remains a very challenging open problem [2], [3].","PeriodicalId":19477,"journal":{"name":"Oceans","volume":"81 1","pages":"1-1"},"PeriodicalIF":0.0,"publicationDate":"2023-06-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"76023457","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}