35 research outputs found

    An integrated cryogenic optical modulator

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    Integrated electrical and photonic circuits (PIC) operating at cryogenic temperatures are fundamental building blocks required to achieve scalable quantum computing, and cryogenic computing technologies. Optical interconnects offer better performance and thermal insulation than electrical wires and are imperative for true quantum communication. Silicon PICs have matured for room temperature applications but their cryogenic performance is limited by the absence of efficient low temperature electro-optic (EO) modulation. While detectors and lasers perform better at low temperature, cryogenic optical switching remains an unsolved challenge. Here we demonstrate EO switching and modulation from room temperature down to 4 K by using the Pockels effect in integrated barium titanate (BaTiO3)-based devices. We report the nonlinear optical (NLO) properties of BaTiO3 in a temperature range which has previously not been explored, showing an effective Pockels coefficient of 200 pm/V at 4 K. We demonstrate the largest EO bandwidth (30 GHz) of any cryogenic switch to date, ultra-low-power tuning which is 10^9 times more efficient than thermal tuning, and high-speed data modulation at 20 Gbps. Our results demonstrate a missing component for cryogenic PICs. It removes major roadblocks for the realisation of novel cryogenic-compatible systems in the field of quantum computing and supercomputing, and for interfacing those systems with the real world at room-temperature

    Barium titanate (BaTiO3) RF characterization for application in electro-optic modulators

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    [EN] Barium titanate (BaTiO3 or BTO) is currently one of the most promising ferroelectric materials for enabling Pockels modulation that is compatible with silicon photonic circuits. The relative permittivity of BTO has been characterized in thin films deposited on a silicon-on-insulator (SOI) substrate. High values between 800 and 1600 have been estimated at 20 GHz. Furthermore, no substantial difference has been obtained by using BTO grown by molecular beam epitaxy and sputtering. The obtained permittivity has been used to properly design the RF electrodes for high-speed modulation in hybrid BTO/Si devices. Electrodes have been fabricated and the possibility of achieving modulation bandwidths up to 40 GHz has been demonstrated. The bandwidth is limited by the microwave propagation losses and, in this case, different losses have been measured depending on the BTO growth process.Financial support from European Commission under project FP7-ICT-2013-11-619456 SITOGA, and from TEC2016-76849-C2-2-R and NANOMET Conselleria de Educació, Cultura i Esport -PROMETEOII/2014 034 are acknowledged. Álvaro Rosa also acknowledges the Spanish Ministry of Economy and Competitiveness for funding his grant.Rosa Escutia, Á.; Tulli, D.; Castera-Molada, P.; Gutiérrez Campo, AM.; Griol Barres, A.; Baquero Escudero, M.; Vilquin, B.... (2017). Barium titanate (BaTiO3) RF characterization for application in electro-optic modulators. Optical Materials Express. 7(12):4328-4336. https://doi.org/10.1364/OME.7.004328S43284336712Hennings, D. (1987). Barium titanate based ceramic materials for dielectric use. International Journal of High Technology Ceramics, 3(2), 91-111. doi:10.1016/0267-3762(87)90031-2Sengupta, L., & Sengupta, S. (1997). Novel ferroelectric materials for phased array antennas. IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control, 44(4), 792-797. doi:10.1109/58.655193De Flaviis, F., Alexopoulos, N. G., & Stafsudd, O. M. (1997). Planar microwave integrated phase-shifter design with high purity ferroelectric material. IEEE Transactions on Microwave Theory and Techniques, 45(6), 963-969. doi:10.1109/22.588610Zgonik, M., Bernasconi, P., Duelli, M., Schlesser, R., Günter, P., Garrett, M. H., … Wu, X. (1994). Dielectric, elastic, piezoelectric, electro-optic, and elasto-optic tensors ofBaTiO3crystals. Physical Review B, 50(9), 5941-5949. doi:10.1103/physrevb.50.5941Reed, G. T., Mashanovich, G., Gardes, F. Y., & Thomson, D. J. (2010). Silicon optical modulators. Nature Photonics, 4(8), 518-526. doi:10.1038/nphoton.2010.179Petraru, A., Schubert, J., Schmid, M., & Buchal, C. (2002). Ferroelectric BaTiO3 thin-film optical waveguide modulators. Applied Physics Letters, 81(8), 1375-1377. doi:10.1063/1.1498151Tang, P., Towner, D. J., Hamano, T., Meier, A. L., & Wessels, B. W. (2004). Electrooptic modulation up to 40 GHz in a barium titanate thin film waveguide modulator. Optics Express, 12(24), 5962. doi:10.1364/opex.12.005962Tang, P., Meier, A. L., Towner, D. J., & Wessels, B. W. (2005). BaTiO_3 thin-film waveguide modulator with a low voltage–length product at near-infrared wavelengths of 098 and 155 µm. Optics Letters, 30(3), 254. doi:10.1364/ol.30.000254Dicken, M. J., Sweatlock, L. A., Pacifici, D., Lezec, H. J., Bhattacharya, K., & Atwater, H. A. (2008). Electrooptic Modulation in Thin Film Barium Titanate Plasmonic Interferometers. Nano Letters, 8(11), 4048-4052. doi:10.1021/nl802981qGirouard, P., Liu, Z., Chen, P., Jeong, Y. K., Tu, Y., Ho, S.-T., & Wessels, B. W. (2016). Enhancement of the pockels effect in photonic crystal modulators through slow light. Optics Letters, 41(23), 5531. doi:10.1364/ol.41.005531Abel, S., Stöferle, T., Marchiori, C., Rossel, C., Rossell, M. D., Erni, R., … Fompeyrine, J. (2013). A strong electro-optically active lead-free ferroelectric integrated on silicon. Nature Communications, 4(1). doi:10.1038/ncomms2695Xiong, C., Pernice, W. H. P., Ngai, J. H., Reiner, J. W., Kumah, D., Walker, F. J., … Tang, H. X. (2014). Active Silicon Integrated Nanophotonics: Ferroelectric BaTiO3 Devices. Nano Letters, 14(3), 1419-1425. doi:10.1021/nl404513pAbel, S., Stoferle, T., Marchiori, C., Caimi, D., Czornomaz, L., Stuckelberger, M., … Fompeyrine, J. (2016). A Hybrid Barium Titanate–Silicon Photonics Platform for Ultraefficient Electro-Optic Tuning. Journal of Lightwave Technology, 34(8), 1688-1693. doi:10.1109/jlt.2015.2510282Eltes, F., Caimi, D., Fallegger, F., Sousa, M., O’Connor, E., Rossell, M. D., … Abel, S. (2016). Low-Loss BaTiO3–Si Waveguides for Nonlinear Integrated Photonics. ACS Photonics, 3(9), 1698-1703. doi:10.1021/acsphotonics.6b00350Hsu, M.-H. M., Marinelli, A., Merckling, C., Pantouvaki, M., Van Campenhout, J., Absil, P., & Van Thourhout, D. (2017). Orientation-dependent electro-optical response of BaTiO_3 on SrTiO_3-buffered Si(001) studied via spectroscopic ellipsometry. Optical Materials Express, 7(6), 2030. doi:10.1364/ome.7.002030Rabiei, P., Ma, J., Khan, S., Chiles, J., & Fathpour, S. (2013). Heterogeneous lithium niobate photonics on silicon substrates. Optics Express, 21(21), 25573. doi:10.1364/oe.21.025573Pernice, W. H. P., Xiong, C., Walker, F. J., & Tang, H. X. (2014). Design of a Silicon Integrated Electro-Optic Modulator Using Ferroelectric BaTiO3 Films. IEEE Photonics Technology Letters, 26(13), 1344-1347. doi:10.1109/lpt.2014.2322501Hu, X., Cueff, S., Romeo, P. R., & Orobtchouk, R. (2015). Modeling the anisotropic electro-optic interaction in hybrid silicon-ferroelectric optical modulator. Optics Express, 23(2), 1699. doi:10.1364/oe.23.001699Castera, P., Tulli, D., Gutierrez, A. M., & Sanchis, P. (2015). Influence of BaTiO_3 ferroelectric orientation for electro-optic modulation on silicon. Optics Express, 23(12), 15332. doi:10.1364/oe.23.015332Castera, P., Gutierrez, A. M., Tulli, D., Cueff, S., Orobtchouk, R., Rojo Romeo, P., … Sanchis, P. (2016). Electro-Optical Modulation Based on Pockels Effect in BaTiO3With a Multi-Domain Structure. IEEE Photonics Technology Letters, 28(9), 990-993. doi:10.1109/lpt.2016.2522509Salama, C. A. T., & Siciunas, E. (1972). Characteristics of rf Sputtered Barium Titanate Films on Silicon. Journal of Vacuum Science and Technology, 9(1), 91-96. doi:10.1116/1.1316695Hayashi, T., Oji, N., & Maiwa, H. (1994). Film Thickness Dependence of Dielectric Properties ofBaTiO3Thin Films Prepared by Sol-Gel Method. Japanese Journal of Applied Physics, 33(Part 1, No. 9B), 5277-5280. doi:10.1143/jjap.33.5277Hamano, T., Towner, D. J., & Wessels, B. W. (2003). Relative dielectric constant of epitaxial BaTiO3 thin films in the GHz frequency range. Applied Physics Letters, 83(25), 5274-5276. doi:10.1063/1.1635967McKee, R. A., Walker, F. J., Conner, J. R., Specht, E. D., & Zelmon, D. E. (1991). Molecular beam epitaxy growth of epitaxial barium silicide, barium oxide, and barium titanate on silicon. Applied Physics Letters, 59(7), 782-784. doi:10.1063/1.105341Janezic, M. D., & Jargon, J. A. (1999). Complex permittivity determination from propagation constant measurements. IEEE Microwave and Guided Wave Letters, 9(2), 76-78. doi:10.1109/75.755052Engen, G. F., & Hoer, C. A. (1979). Thru-Reflect-Line: An Improved Technique for Calibrating the Dual Six-Port Automatic Network Analyzer. IEEE Transactions on Microwave Theory and Techniques, 27(12), 987-993. doi:10.1109/tmtt.1979.1129778Alferness, R. C. (1982). Waveguide Electrooptic Modulators. IEEE Transactions on Microwave Theory and Techniques, 30(8), 1121-1137. doi:10.1109/tmtt.1982.1131213Chung, H., Chang, W. S. C., & Adler, E. L. (1991). Modeling and optimization of traveling-wave LiNbO/sub 3/ interferometric modulators. IEEE Journal of Quantum Electronics, 27(3), 608-617. doi:10.1109/3.8137

    Strain-Engineered Metal-to-Insulator Transition and Orbital Polarization in Nickelate Superlattices Integrated on Silicon

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    Epitaxial growth of SrTiO3 (STO) on silicon greatly accelerates the monolithic integration of multifunctional oxides into the mainstream semiconductor electronics. However, oxide superlattices (SLs), the birthplace of many exciting discoveries, remain largely unexplored on silicon. In this work, LaNiO3/LaFeO3 SLs are synthesized on STO-buffered silicon (Si/STO) and STO single-crystal substrates, and their electronic properties are compared using dc transport and X-ray absorption spectroscopy. Both sets of SLs show a similar thickness-driven metal-to-insulator transition, albeit with resistivity and transition temperature modified by the different amounts of strain. In particular, the large tensile strain promotes a pronounced Ni (Formula presented.) orbital polarization for the SL grown on Si/STO, comparable to that reported for LaNiO3 SL epitaxially strained to DyScO3 substrate. Those results illustrate the ability to integrate oxide SLs on silicon with structure and property approaching their counterparts grown on STO single crystal, and also open up new prospects of strain engineering in functional oxides based on the Si platform. © 2020 The Authors. Advanced Materials published by Wiley-VCH Gmb

    Interactions of PAMAM dendrimers with SDS at the solid-liquid interface

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    This work addresses structural and nonequilibrium effects of the interactions between well-defined cationic poly(amidoamine) PAMAM dendrimers of generations 4 and 8 and the anionic surfactant sodium dodecyl sulfate (SDS) at the hydrophilic silica-water interface. Neutron reflectometry and quartz crystal microbalance with dissipation monitoring were used to reveal the adsorption from premixed dendrimer/surfactant solutions as well as sequential addition of the surfactant to preadsorbed layers of dendrimers. PAMAM dendrimers of both generations adsorb to hydrophilic silica as a compact monolayer, and the adsorption is irreversible upon rinsing with salt solution. SDS adsorbs on the dendrimer layer and at low bulk concentrations causes the expansion of the dendrimer layers on the surface. When the bulk concentration of SDS is increased, the surfactant layer consists of aggregates or bilayer-like structures The adsorption of surfactant is reversible upon rinsing, but slight changes of the structure of the preadsorbed PAMAM monolayer were observed The adsorption from premixed solutions close to charge neutrality results in thick multilayers, but the surface excess is lower when the bulk complexes have a net negative charge. A critical examination of the pathway of adsorption for the interactions of SDS with preadsorbed PAMAM monolayers and premixed PAMAM/SDS solutions with hydrophilic silica revealed that nonequilibrium effects are important only in the latter case, and the application of a thermodynamic model to such experimental data would be inappropriate
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