33 results on '"W. Baechtold"'
Search Results
2. Quasi-analytic steady-state solution of VCSEL rate equations including spatial hole burning and carrier diffusion losses
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Daniel Erni, W. Baechtold, and M. Jungo
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Physics ,Steady state ,business.industry ,Physics::Optics ,Rate equation ,Mechanics ,Laser ,Computer Science Applications ,law.invention ,Vertical-cavity surface-emitting laser ,Optics ,Laser diode rate equations ,law ,Modeling and Simulation ,Diffusion current ,Electrical and Electronic Engineering ,Current (fluid) ,Diffusion (business) ,business - Abstract
SUMMARY We propose a new set of equations describing a cylindrical vertical cavity surface emitting laser (VCSEL) cavity under CW operation, based on the rate equations including lateral carrier diffusion. The only numerical step in the calculation consists in finding the roots of a polynomial expression. This model enables a quasi-instantaneous calculation of the laser’s light-current characteristic, including such effects as spatial hole burning, current spreading, inhomogeneous optical intensity distribution, and diffusion losses. An analysis of the VCSELs threshold current and differential quantum efficiency is proposed, which illustrates the interplay between injected current profile and diffusion coefficient. Copyright # 2003 John Wiley & Sons, Ltd.
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- 2003
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3. Scaling effects on vertical-cavity surface-emitting lasers static and dynamic behavior
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M. Jungo, W. Baechtold, Daniel Erni, and Fabrice Monti di Sopra
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Materials science ,business.industry ,Relative intensity noise ,Oscillation ,General Physics and Astronomy ,Gain compression ,Distributed Bragg reflector ,Noise (electronics) ,Semiconductor laser theory ,Laser linewidth ,Optics ,Optoelectronics ,Spontaneous emission ,business - Abstract
We investigate the influence of oxide aperture size and number of top distributed Bragg reflector pairs on the performance of oxide confined vertical-cavity surface emitting lasers. Several counteracting mechanisms are shown to result in nonmonotonic behavior, which limits the performance of very small cavities. Static, dynamic, and noise behavior are considered. We examine static operation by means of steady-state measurements, whereas dynamic behavior and noise performance are described by the intrinsic relaxation oscillation frequency, damping coefficient, and Schawlow–Townes linewidth. These parameters are extracted from relative intensity noise measurements. Reducing the oxide aperture up to a given optimal diameter is shown to improve the device’s characteristics. We attribute the performance degradation below this value to increased diffraction losses, reduced confinement factor, and enhanced spontaneous emission. Similarly, increasing the number of Bragg reflector pairs first yields better overall performance as a consequence of reduced mirror losses. However, beyond an optimal value, significant reduction of the differential gain is observed that is attributed to gain compression and possibly thermal effects, degrading both the steady-state and high-frequency performance of the device.
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- 2002
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4. 2-D VCSEL model for investigation of dynamic fiber coupling and spatially filtered noise
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W. Baechtold, Daniel Erni, and M. Jungo
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Physics ,business.industry ,Relative intensity noise ,Rate equation ,Noise (electronics) ,Atomic and Molecular Physics, and Optics ,Electronic, Optical and Magnetic Materials ,law.invention ,Vertical-cavity surface-emitting laser ,Semiconductor laser theory ,Optics ,Orders of magnitude (time) ,Mode partition noise ,law ,Optical cavity ,Electrical and Electronic Engineering ,business - Abstract
We propose a set of transformed two-dimensional (2-D) rate equations, which allow the computation of dynamic gain competition resulting from inhomogeneous field and carrier spatial distributions inside a vertical cavity surface-emitting laser cavity. Any explicit spatial dependency has been removed from the modified equations, reducing the computational time by several orders of magnitude. Resulting 2-D dynamic intensity profiles allow investigating effects related to improper fiber coupling due to transverse misalignment between laser beam and fiber. Although the expected increased relative intensity noise (RIN) levels associated with mode partition noise are observed, other effects might have larger contributions to the total noise under specific conditions. We show that the minimum RIN level is not necessarily reached for zero misalignment, but at positions where modes with broad far-field profiles and low power experience important filtering.
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- 2003
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5. The Herschel-Heterodyne Instrument for the Far-Infrared (HIFI)
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Brian Jackson, B. Kopf, R. Bieber, R. Güsten, A. M. di Giorgio, J. A. Stern, Holger S. P. Müller, B. J. van Leeuwen, G. S. Liu, R. Orfei, Neal R. Erickson, R. Lai, B. Delforges, Wolfgang Wild, Christian Leinz, O. Coeur-Joly, J. Desbat, David Teyssier, S. D. Lord, Karl Jacobs, Bruce Bumble, Lorene Samoska, M. Rataj, R. H. Lin, Dominicus Kester, M. Salez, X. Tielens, Alexandre Karpov, Paolo Saraceno, K. Edwards, R. Huisman, A. Megej, K. F. Schuster, Michel Fich, L. Dubbeldam, Serguei Cherednichenko, H. Golstein, Christian Monstein, J. A. Murphy, C. van Baaren, Victor Belitsky, P. Planesas, E. Natale, Michael Olberg, Lorenzo Piazzo, T. Peacock, Martin Eggens, Emmanuel Caux, W. A. Hatch, Neil Trappe, Hubregt J. Visser, Herbert Zirath, Jaap Evers, S. Phillip-May, Alain Maestrini, Hamid Javadi, Jacob Kooi, Th. de Graauw, F. Schmülling, E. C. Honingh, C. McCoey, J. C. Pearson, W. Luinge, I. Lopez-Fernandez, W. M. Laauwen, M. Michalska, Bengt Larsson, S. Wulff, John Gill, René Liseau, Volker Ossenkopf, Colin Borys, B. Kruizenga, Rafael Teipen, C. Kramer, A. Cros, H. Goulooze, P. Cais, W. Nowosielski, Goutam Chattopadhyay, M. Stokroos, Rafael Bachiller, F. Zwart, C. Gal, Piotr Orleanski, J. Kawamura, H. Smit, O. Siebertz, H. Aarts, Francesco Nuzzolo, L. Meinsma, Jonas Zmuidzinas, R. Assendorp, D. A. Beintema, H. van de Stadt, Jesús Martín-Pintado, G. de Lange, Ryszard Szczerba, Erich Schlecht, R. Higgins, Christophe Risacher, Patrick W. Morris, H. Jacobs, Christopher Jarchow, Willem Jellema, Pieter Dieleman, Todd Gaier, B. Franke, J. Stutzki, Imran Mehdi, Th. Klein, Harald Franz Arno Merkel, T. Finn, M. Justen, P.R. Wesselius, M. Ciechanowicz, T. M. Klapwijk, Hans-Joachim Wunsch, C. Comito, P. Zaal, Erik L. Kollberg, C. Diez-Gonzalez, T. den Boggende, John Ward, Jian-Rong Gao, Pasquale Cerulli-Irelli, C. Kasemann, T. Kuhn, Frank Helmich, K. Wildeman, Henry G. LeDuc, L. Ravera, Frank Maiwald, Y. Delorme, D. Moratschke, F. Schlöder, J. M. Krieg, M. Olbrich, A. Marston, Juan Daniel Gallego, P.-P. Kooiman, E. Steinmetz, T. Gunsing, A. Naber, M. Melchior, Geert Keizer, M. Schultz, I. Peron, S. Gauffre, C. K. Wafelbakker, N. Whyborn, M. Krause, T. Tils, Alexander Loose, A. de Jonge, Pieter R. Roelfsema, Rudolf Schieder, M. Caris, S. Glenz, A. Barcia, W. Baechtold, Paul Hartogh, R. Shipman, Adwin Boogert, Arnold O. Benz, Thomas G. Phillips, California Institute of Technology (CALTECH), Laboratoire d'Astrophysique de Grenoble (LAOG), Université Joseph Fourier - Grenoble 1 (UJF)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National de la Recherche Scientifique (CNRS), Centre d'étude spatiale des rayonnements (CESR), Observatoire Midi-Pyrénées (OMP), Météo France-Centre National d'Études Spatiales [Toulouse] (CNES)-Université Fédérale Toulouse Midi-Pyrénées-Centre National de la Recherche Scientifique (CNRS)-Institut de Recherche pour le Développement (IRD)-Météo France-Centre National d'Études Spatiales [Toulouse] (CNES)-Université Fédérale Toulouse Midi-Pyrénées-Centre National de la Recherche Scientifique (CNRS)-Institut de Recherche pour le Développement (IRD)-Centre National de la Recherche Scientifique (CNRS)-Institut national des sciences de l'Univers (INSU - CNRS)-Université Toulouse III - Paul Sabatier (UT3), Université Fédérale Toulouse Midi-Pyrénées, Université Sciences et Technologies - Bordeaux 1, Observatoire aquitain des sciences de l'univers (OASU), Université Sciences et Technologies - Bordeaux 1-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National de la Recherche Scientifique (CNRS), Laboratoire d'Astrophysique de Bordeaux [Pessac] (LAB), Université de Bordeaux (UB)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National de la Recherche Scientifique (CNRS), Laboratoire d'astrodynamique, d'astrophysique et d'aéronomie de bordeaux (L3AB), Department of Microtechnology and Nanoscience (MC2), Chalmers University of Technology [Gothenburg, Sweden], Laboratoire de Cosmologie, Astrophysique Stellaire & Solaire, de Planétologie et de Mécanique des Fluides (CASSIOPEE), Université Nice Sophia Antipolis (... - 2019) (UNS), COMUE Université Côte d'Azur (2015-2019) (COMUE UCA)-COMUE Université Côte d'Azur (2015-2019) (COMUE UCA)-Institut national des sciences de l'Univers (INSU - CNRS)-Observatoire de la Côte d'Azur, COMUE Université Côte d'Azur (2015-2019) (COMUE UCA)-Université Côte d'Azur (UCA)-Université Côte d'Azur (UCA)-Centre National de la Recherche Scientifique (CNRS), Laboratoire d'Etude du Rayonnement et de la Matière en Astrophysique (LERMA), École normale supérieure - Paris (ENS Paris), Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Université Pierre et Marie Curie - Paris 6 (UPMC)-Institut national des sciences de l'Univers (INSU - CNRS)-Observatoire de Paris, Université Paris sciences et lettres (PSL)-Université de Cergy Pontoise (UCP), Université Paris-Seine-Université Paris-Seine-Centre National de la Recherche Scientifique (CNRS), Max Planck Institute for Solar System Research (MPS), Max-Planck-Gesellschaft, Jet Propulsion Laboratory (JPL), NASA-California Institute of Technology (CALTECH), Dept Pathol & Microbiol, Université de Montréal (UdeM)-Faculté de médecine vétérinaire, Leibniz Institute for Crystal Growth, Leibniz Institute, Technische Universität Darmstadt (TU Darmstadt), Instituto de RadioAstronomía Milimétrica (IRAM), Centre National de la Recherche Scientifique (CNRS), Institut für Festkörpertheorie, Westfälische Wilhelms-Universität Münster (WWU), Institute of Molecular Medicine and Cell Research (ZBMZ), University of Freiburg [Freiburg], Onsala Space Observatory, Chalmers University of Technology [Göteborg], ESO, European Southern Observatory (ESO), Istituto di Fisica dello Spazio Interplanetario (IFSI), Consiglio Nazionale delle Ricerche (CNR), Max Planck Institute for Meteorology (MPI-M), Institut für Chemie und Dynamik der Geosphäre - Troposphäre (ICG-2), Forschungszentrum Jülich GmbH | Centre de recherche de Juliers, Helmholtz-Gemeinschaft = Helmholtz Association-Helmholtz-Gemeinschaft = Helmholtz Association, Herschel Science Center [Madrid], European Space Astronomy Centre (ESAC), European Space Agency (ESA)-European Space Agency (ESA), Université Toulouse III - Paul Sabatier (UT3), Université de Toulouse (UT)-Université de Toulouse (UT)-Institut national des sciences de l'Univers (INSU - CNRS)-Observatoire Midi-Pyrénées (OMP), Institut de Recherche pour le Développement (IRD)-Université Toulouse III - Paul Sabatier (UT3), Université de Toulouse (UT)-Université de Toulouse (UT)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Météo-France -Institut de Recherche pour le Développement (IRD)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Météo-France -Centre National de la Recherche Scientifique (CNRS), Université Sciences et Technologies - Bordeaux 1 (UB), Université Sciences et Technologies - Bordeaux 1 (UB)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National de la Recherche Scientifique (CNRS), Université Nice Sophia Antipolis (1965 - 2019) (UNS), École normale supérieure - Paris (ENS-PSL), Max-Planck-Institut für Sonnensystemforschung = Max Planck Institute for Solar System Research (MPS), Technische Universität Darmstadt - Technical University of Darmstadt (TU Darmstadt), Westfälische Wilhelms-Universität Münster = University of Münster (WWU), National Research Council of Italy | Consiglio Nazionale delle Ricerche (CNR), Agence Spatiale Européenne = European Space Agency (ESA)-Agence Spatiale Européenne = European Space Agency (ESA), TNO Industrie en Techniek, and Astronomy
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Experimental Physics ,Local oscillator ,Observatories ,Orbits ,general [Submillimeter] ,01 natural sciences ,7. Clean energy ,spectroscopic [Techniques] ,law.invention ,Far infrared ,Spectrographs ,law ,spectrographs [Instrumentation] ,010303 astronomy & astrophysics ,instrumentation: spectrographs ,Physics ,Spectrometers ,submillimeter: general ,Bolometers ,Correlators ,methods: observational ,infrared: general ,Heterodyne ,Frequency band ,Submillimeter: generals ,Instantaneous phase ,Radio spectrum ,Optics ,Mixers (machinery) ,0103 physical sciences ,Frequency bands ,observational [Methods] ,010306 general physics ,Remote sensing ,techniques: spectroscopic ,Spectrometer ,business.industry ,[SDU.ASTR.SR]Sciences of the Universe [physics]/Astrophysics [astro-ph]/Solar and Stellar Astrophysics [astro-ph.SR] ,Bolometer ,generals [Submillimeter] ,Astronomy and Astrophysics ,[PHYS.ASTR.SR]Physics [physics]/Astrophysics [astro-ph]/Solar and Stellar Astrophysics [astro-ph.SR] ,Launching ,general [Infrared] ,Space and Planetary Science ,Heterodyning ,Instruments ,business - Abstract
International audience; Aims: This paper describes the Heterodyne Instrument for the Far-Infrared (HIFI) that was launched onboard ESA's Herschel Space Observatory in May 2009. Methods: The instrument is a set of 7 heterodyne receivers that are electronically tuneable, covering 480-1250 GHz with SIS mixers and the 1410-1910 GHz range with hot electron bolometer (HEB) mixers. The local oscillator (LO) subsystem comprises a Ka-band synthesizer followed by 14 chains of frequency multipliers and 2 chains for each frequency band. A pair of auto-correlators and a pair of acousto-optical spectrometers process the two IF signals from the dual-polarization, single-pixel front-ends to provide instantaneous frequency coverage of 2 × 4 GHz, with a set of resolutions (125 kHz to 1 MHz) that are better than 0.1 km s-1. Results: After a successful qualification and a pre-launch TB/TV test program, the flight instrument is now in-orbit and completed successfully the commissioning and performance verification phase. The in-orbit performance of the receivers matches the pre-launch sensitivities. We also report on the in-orbit performance of the receivers and some first results of HIFI's operations. Herschel is an ESA space observatory with science instruments provided by European-led Principal Investigator consortia and with important participation from NASA.
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- 2010
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6. Residual-carrier free, balanced optical phase locked loop for inter-satellite communications
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K. Kudielka, F. Herzog, W. Baechtold, and Daniel Erni
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Physics ,Phase-locked loop ,Optics ,business.industry ,Optical transistor ,Optical cross-connect ,Electronic engineering ,Optical modulation amplitude ,Optical performance monitoring ,business ,Optical switch ,Residual carrier ,Optical communications repeater - Abstract
We present a coherent optical commu nication system for inter-satellite links with a new type of Optical Phase Lock Loop (OPLL). The OPLL requires no residual carrier transmission, although it employs a conventional 180° 3 dB hybrid and an AC-coupled balanced front end.
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- 2006
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7. Fiber dispersion induced nonlinearity in fiber-optic links with multimode laser diodes
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W. Baechtold and S. Hunziker
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Physics ,Optical fiber ,business.industry ,Physics::Optics ,Atomic and Molecular Physics, and Optics ,Electronic, Optical and Magnetic Materials ,law.invention ,Semiconductor laser theory ,Optics ,Modulation ,law ,Dispersion (optics) ,Modal dispersion ,Optoelectronics ,Fiber ,Electrical and Electronic Engineering ,business ,Diode ,Intermodulation - Abstract
In analog RF fiber-optic (FO) links with directly modulated multimode laser diodes (LD's), nonlinear distortions of the received modulation signal occur due to fiber dispersion. Using a simple analytical two mode model, we show that the mutual compensation of strong nonlinearities between particular modes breaks down at high-modulation frequencies. The effect can be observed even in 1300-nm links with single-mode (SM) standard fibers. Simulations as well as measurements of intermodulation (IM) illustrate this argument.
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- 1997
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8. A flip-flop and logic gate with Josephson junctions
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W. Baechtold
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Josephson effect ,Physics ,Pass transistor logic ,business.industry ,Electrical engineering ,Hardware_PERFORMANCEANDRELIABILITY ,Emitter-coupled logic ,Resistor–transistor logic ,law.invention ,Pi Josephson junction ,law ,Logic gate ,Hardware_INTEGRATEDCIRCUITS ,Hardware_ARITHMETICANDLOGICSTRUCTURES ,business ,Flip-flop ,AND gate ,Hardware_LOGICDESIGN - Abstract
A complementary logic circuit with Josephson junctions has been investigated theoretically and experimentally. This paper will discuss a circuit with a measured risetime of 100 ps, a power dissipation of 16.4 μW, with the flip-flop operated with a 1500-MHz input signal.
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- 2005
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9. Realistic two-dimensional models for planar photonic crystal devices
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Daniel Erni, W. Baechtold, Jan-Robert van Look, Patric Strasser, Robert Wueest, K. Rauscher, Rik Harbers, and Franck Robin
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business.industry ,Scattering ,Chemistry ,Finite-difference time-domain method ,Physics::Optics ,Tapering ,law.invention ,Optics ,Planar ,law ,Phenomenological model ,Hexagonal lattice ,business ,Waveguide ,Photonic crystal - Abstract
We have studied tapers that couple light from a conventional ridge waveguide into a planar photonic crystal (PhC) waveguide. Tapering is achieved by changing the PhC waveguide width either in steps or gradually. Lag effects in fabrication provide an additional tapering due to the fact that the hole depths scale with the corresponding hole diameter. Our analysis deals with the out-of-plane loss that arises within such taper sections. The PhC consists of a triangular lattice of air holes introduced into an InGaAsP/InP slab structure. For conceptual studies we use the 2D multiple multipole method (MMP) in conjunction with an extended phenomenological model. This model covers the out-of-plane scattering providing a loss parameter and an effective index correction for the holes under consideration. This realistic 2D model is retrieved from full-wave 3D FDTD simulations and measurements.
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- 2004
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10. Lasing in a 2D photonic bandgap structure
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W. Baechtold, Asma Jebali, Ernst B. Kley, Gian-Luca Bona, Christian Bauer, Rainer F. Mahrt, Daniel Erni, and Nikolaj Moll
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chemistry.chemical_classification ,Materials science ,business.industry ,Physics::Optics ,Stopband ,Polymer ,engineering.material ,Grating ,Distributed Bragg reflector ,Optical pumping ,Optics ,Coating ,chemistry ,engineering ,Optoelectronics ,business ,Lasing threshold ,Photonic bandgap - Abstract
Organic two-dimensional photonic bandgap structures (2D PBG) have been fabricated by spin-coating a thin polymer film onto a nano-patterned SiO2 circular-grating surface-emitting distributed Bragg reflectors (CG-SE-DBR). When optically pumped and for certain grating parameters, these structures exhibit a peak inside the stop band that leads to lasing with a reduced threshold. An analytical model based on the transfer-matrix method has been developed to investigate the origin of this peak. The theoretical results are in excellent agreement with the experimental findings.
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- 2004
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11. Circular polarized aperture coupled patch antennas for an RFID system in the 2.4 GHz ISM band
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H. Benedickter, W. Baechtold, and M. Kossel
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Physics ,Super high frequency ,Reconfigurable antenna ,Directional antenna ,business.industry ,Reflective array antenna ,Fresnel zone antenna ,Astrophysics::Instrumentation and Methods for Astrophysics ,Slot antenna ,law.invention ,Biconical antenna ,Optics ,Horn antenna ,law ,High Energy Physics::Experiment ,Physics::Chemical Physics ,business ,Computer Science::Information Theory - Abstract
The design of aperture coupled patch (ACP) antennas for an RFID system in the 2.4 GHz ISM using circular polarization modulation is presented. Due to the requirements of the modulation scheme the ACP antennas are circularly polarized with switchable polarization sense. Four ACP antennas are compared according to their impedance and gain bandwidth, axial ratio, and crosspolarization isolation. Among the presented antennas a novel compact ACP antenna is shown that allows replacement of the conventional quadrature hybrid polarizer by /spl lambda//4 quarter transmission lines.
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- 2003
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12. GaAs device activities in Europe
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W. Baechtold
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Computer science ,law ,business.industry ,Electrical engineering ,JFET ,MESFET ,Integrated circuit ,business ,law.invention ,Processing methods - Abstract
This survey of European GaAs device activities focuses on GaAs MESFETs, HEMTs, and GaInAs JFETs. In all areas significant progress is noted and attributed to advanced processing methods. In the case of the GaInAs JFET, outstanding device results are cited. It is felt that the technology, however, is presently suited to very simple integrated circuits only and that of tools and processes similar to those for MESFETs are needed similar levels of integration to become feasible. >
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- 2003
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13. Determination of the noise source parameters in AlInAs/GaInAs HEMT heterostructures based on measured noise temperature dependence on the electric field
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C. Bergamaschi, W. Patrick, and W. Baechtold
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Noise temperature ,Materials science ,business.industry ,Astrophysics::Instrumentation and Methods for Astrophysics ,Heterojunction ,High-electron-mobility transistor ,Gallium arsenide ,chemistry.chemical_compound ,chemistry ,Electric field ,Equivalent circuit ,Optoelectronics ,business ,Noise (radio) - Abstract
The noise temperature dependence on the electric field in an AlInAs/GaInAs HEMT heterostructure has been measured. It was found that the dependence of the noise temperature on the electric field in GaAs MESFETs and in AlInAs/GaInAs HEMTs are remarkably different. For this reason a different model must be used for AlInAs/GaInAs HEMTs. Based on the measured noise temperature dependence on the electric field, am analytic noise model for the AlInAs/GaInAs HEMT has been developed. The noise source parameters were calculated and compared with extracted noise source parameters from noise measurements. >
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- 2002
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14. Approach for developing a large signal model of a 150 GHz HEMT
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B.-U.H. Klepser, W. Patrick, Christian G. Diskus, M. Schefer, C. Bergamaschi, and W. Baechtold
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Engineering ,business.industry ,Transistor ,Spice ,Hardware_PERFORMANCEANDRELIABILITY ,Large-signal model ,High-electron-mobility transistor ,computer.software_genre ,law.invention ,Simulation software ,Gallium arsenide ,chemistry.chemical_compound ,chemistry ,law ,Hardware_INTEGRATEDCIRCUITS ,Electronic engineering ,Scattering parameters ,business ,computer ,Voltage - Abstract
In this contribution the development of a large signal model describing the electrical behaviour of an InAlAs/InGaAs/InP-HEMT will be discussed. The transistors under question were fabricated at our laboratory. They revealed a transit frequency of 150 GHz, which is, to our knowledge, the best result obtained with a T-gate of 0.25 /spl mu/m footprint. The aim of this project was to develop a model of this transistor for simulating nonlinear circuits with commercial simulator software like HP-MDS or Spice. The procedure results in an easily applicable model which produces very good fits to the measured S-parameters.
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- 2002
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15. Depletion and enhancement mode InP high electron mobility transistors fabricated by a dry gate recess process
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W. Patrick, Rebecca Cheung, and W. Baechtold
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Materials science ,business.industry ,Transconductance ,Transistor ,Electrical engineering ,Cutoff frequency ,Threshold voltage ,law.invention ,chemistry.chemical_compound ,chemistry ,Etching (microfabrication) ,law ,Indium phosphide ,Optoelectronics ,Dry etching ,business ,Indium gallium arsenide - Abstract
We report depletion and enhancement mode InP high electron mobility transistors (HEMTs) fabricated using CH/sub 4//H/sub 2/ selective dry etch gate recess process. Under the etching conditions developed, the process has a In/sub 0.7/Ga/sub 0.3/As to In/sub 0.52/Al/sub 0.48/As selectivity of 130. The dc threshold voltages of the devices fabricated in this way increase from -1.3 V to 0.1 V as a function of dry etch time, with an extrinsic transconductance of 520 mS/mm in the depletion mode and 800 mS/mm in enhancement mode. The devices exhibit an extrapolated cut-off frequencies of 150 GHz. This work demonstrates the potential of the use of dry etching as a gate recess technology for the future development of high frequency InP-based circuits.
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- 2002
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16. Improvements on a GaAs MESFET model for nonlinear RF simulations
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Frank Ellinger, J. Kucera, and W. Baechtold
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Linear region ,Materials science ,business.industry ,Conductance ,Charge (physics) ,Condensed Matter::Mesoscopic Systems and Quantum Hall Effect ,Capacitance ,Gallium arsenide ,Nonlinear system ,chemistry.chemical_compound ,chemistry ,Equivalent circuit ,Optoelectronics ,MESFET ,business - Abstract
A modified GaAs MESFET-model has been developed to improve accuracy over a large bias range, particularly within the linear region. The enhancements consist of a modified Statz equation for the gate charge to improve the modeling of the gate drain capacitance, and an equation for the bias dependent drain source resistance for exact modeling of the dispersive output conductance.
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- 2002
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17. Broadband noise parameter and S-parameter measurement technique
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W. Baechtold and M.L. Schmatz
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Noise temperature ,Engineering ,Noise generator ,Noise measurement ,business.industry ,Electronic engineering ,Effective input noise temperature ,Y-factor ,Tuner ,business ,Noise figure ,Noise floor - Abstract
An accurate noise parameter measurement technique is presented that uses an amplifier/attenuator noise source, a multi-octave tuner and a directional coupler for noise injection at all tuner states. The presented concept allows measurements with more than 30 different ENR steps and the ability to calibrate the ENR during system calibration. A system that demonstrates the concept was built for the frequency range from 0.5-6.0 GHz.
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- 2002
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18. Active compensation of improper waveguide coupling through vertical-cavity surface-emitting laser electronic beam shaping
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M. Jungo, W. Baechtold, and Daniel Erni
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Distributed feedback laser ,Materials science ,business.industry ,Physics::Optics ,Statistical and Nonlinear Physics ,Beam parameter product ,Atomic and Molecular Physics, and Optics ,Vertical-cavity surface-emitting laser ,Laser linewidth ,Optics ,Quantum dot laser ,Optoelectronics ,Laser beam quality ,Laser power scaling ,business ,Tunable laser - Abstract
We propose a new asymmetric drive scheme for vertical-cavity surface-emitting lasers (VCSELs) that is expected to permit the active compensation of misalignment between laser beam and waveguide. Simulations performed with a VCSEL integrated spatiotemporal advanced simulator simulation tool indicate that driving the laser with two orthogonal, individually addressable contacts may improve coupling efficiency by selective excitation of modes with given azimuthal distributions. Besides improved and more-stable coupling efficiency, significantly lower noise levels that result from reduced mode partition noise are observed, which significantly enhance the performance of digital transmission systems. Such electronic beam shaping from the driver side may drastically reduce the system’s costs by relaxing its fabrication tolerances.
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- 2003
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19. Cellular remote antenna feeding: Optical fibre or coaxial cable?
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W. Baechtold and S. Hunziker
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Engineering ,Optical fiber ,business.industry ,Coaxial cable ,Dynamic range ,Cellular radio ,Cellular telephone ,law.invention ,law ,GSM ,Electronic engineering ,Electrical and Electronic Engineering ,Coaxial ,Antenna (radio) ,business - Abstract
Remote antennas in cellular telephone networks can be supplied by coaxial cable or optical fibre. It is useful to know which of the two technologies is more appropriate with respect to dynamic range and costs. Coaxial and optical fibre links are considered for GSM applications. The link length-dependent costs are compared for two reasonable values of the dynamic range.
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- 1998
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20. Simple model for fundamental intermodulation analysis of RF amplifiers and links
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W. Baechtold and S. Hunziker
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Third-order intercept point ,Engineering ,Optical fiber ,business.industry ,Second-order intercept point ,Amplifier ,Electrical engineering ,law.invention ,Simple (abstract algebra) ,law ,Electronic engineering ,Point (geometry) ,Limit (mathematics) ,Electrical and Electronic Engineering ,business ,Intermodulation - Abstract
In modern low cost RF amplifiers or fibre optic links, it is essential to know the limit of the third order intercept point definition to make accurate intermodulation predictions. The authors present a simple formula to calculate this limit from the data sheet parameters' third order intercept point and 1dB compression point.
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- 1996
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21. Determination of the RF-noise source parameters in AlInAs/GaInAs-HEMT heterostructures based on measured noise temperature dependence against electric field
- Author
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W. Patrick, W. Baechtold, and C. Bergamaschi
- Subjects
Noise temperature ,Rf noise ,business.industry ,Chemistry ,Astrophysics::Instrumentation and Methods for Astrophysics ,Y-factor ,Heterojunction ,High-electron-mobility transistor ,chemistry.chemical_compound ,Ternary compound ,Electric field ,Electronic engineering ,Optoelectronics ,Electrical and Electronic Engineering ,business ,Noise (radio) - Abstract
The noise temperature dependence on the electric field in an AlInAs/GaInAs-HEMT heterostructure has been measured. It was found that the dependence of the noise temperature on the electric field in GaAs-MESFETs and in AlInAs/GaInAs-HEMTs is remarkably different. For this reason a different model must be used for AlInAs/GaInAs-HEMTs. Based on the measured noise temperature dependence on the electric field, an analytic noise model for the AlInAs/GaInAs HEMT has been developed. The noise source parameters were calculated and compared with extracted noise source parameters from noise measurements.
- Published
- 1995
- Full Text
- View/download PDF
22. Computerized Calculation of Small Signal and Noise Properties of Microwave Transistors
- Author
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W. Kotyczka, M. J. O. Strutt, and W. Baechtold
- Subjects
Noise temperature ,Engineering ,Radiation ,business.industry ,Acoustics ,Y-factor ,Hardware_PERFORMANCEANDRELIABILITY ,Condensed Matter Physics ,Noise figure ,Noise (electronics) ,Burst noise ,Noise generator ,Hardware_INTEGRATEDCIRCUITS ,Electronic engineering ,Effective input noise temperature ,Flicker noise ,Electrical and Electronic Engineering ,business - Abstract
The small signal and noise equivalent circuit of a microwave transistor is evaluated using an analog simulation model. The noise figure has been determined with the same model as a function of the source admittance and the frequency. The s parameters and noise figures are compared with the results calculated on a digital computer.
- Published
- 1969
- Full Text
- View/download PDF
23. X- and Ku-band amplifiers with GaAs Schottky-barriers field-effect transistors
- Author
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W. Baechtold
- Subjects
Materials science ,business.industry ,Amplifier ,Transistor ,Schottky diode ,Transistor array ,Noise figure ,Ku band ,law.invention ,law ,Optoelectronics ,Field-effect transistor ,Electrical and Electronic Engineering ,business ,Monolithic microwave integrated circuit - Abstract
During recent years significant progress has been made in GaAs technology and the GaAs Schottky-barrier field-effect transistor now shows outstanding microwave gain and noise properties. Two experimental microwave amplifiers demonstrate that the device is very well suited for broad-band applications and that large bandwidth in the X- and Ku-band can be obtained with simple circuits. The first of the two three-stage amplifiers realized was optimized with respect to noise and a noise figure of 3.8 dB was obtained at 8 GHz; the maximum gain is 17.5 dB at 8.3 GHz and the 3-dB bandwidth is 1.3 GHz. The second amplifier has a maximum gain of 11.5 dB at 11.5 GHz. The gain is greater than 8.5 dB in the range 9.5-14.3 GHz.
- Published
- 1973
- Full Text
- View/download PDF
24. Noise behavior of GaAs field-effect transistors with short gate lengths
- Author
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W. Baechtold
- Subjects
Noise temperature ,Materials science ,Noise-figure meter ,business.industry ,Shot noise ,Y-factor ,Condensed Matter::Mesoscopic Systems and Quantum Hall Effect ,Electronic, Optical and Magnetic Materials ,Burst noise ,Noise generator ,Optoelectronics ,Flicker noise ,Electrical and Electronic Engineering ,business ,Noise (radio) - Abstract
The noise behavior of the GaAs Schottky-barrier gate field-effect transistor has been investigated theoretically and experimentally. It has been found that an additional noise source has to be taken into account in GaAs FET's biased in the pinchoff region: the intervalley scattering noise. This noise source has been investigated and a new transistor noise model is proposed. Measured and calculated noise figures show good agreement in the frequency range 2-10 GHz. It is shown that the influence of the intervalley scattering noise can be reduced by reducing the channel thickness, and that such devices show excellent gain and noise properties in the X band.
- Published
- 1972
- Full Text
- View/download PDF
25. Noise behavior of Schottky barrier gate field-effect transistors at microwave frequencies
- Author
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W. Baechtold
- Subjects
Materials science ,business.industry ,Schottky barrier ,Transistor ,Metal–semiconductor junction ,Electronic, Optical and Magnetic Materials ,law.invention ,Computer Science::Hardware Architecture ,Computer Science::Emerging Technologies ,law ,Optoelectronics ,Equivalent circuit ,Flicker noise ,Field-effect transistor ,Electrical and Electronic Engineering ,business ,Microwave ,Noise (radio) - Abstract
The noise behavior of a Schottky barrier gate field-effect transistor is investigated by the use of the noise equivalent circuit. The influence of the carrier velocity saturation is estimated. The noise parameters are calculated by taking into account the influence of parasitic resistances. Measured and calculated noise parameters show good agreement in the frequency range 2-8 GHz.
- Published
- 1971
- Full Text
- View/download PDF
26. Si and GaAs 0.5μm-gate Schottky-barrier field-effect transistors
- Author
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K. Daetwyler, Th. O. Mohr, W. Baechtold, T. Forster, P. Wolf, and W. Walter
- Subjects
Materials science ,Noise measurement ,business.industry ,Schottky barrier ,Schottky effect ,Transistor ,Y-factor ,Noise figure ,law.invention ,law ,Optoelectronics ,Field-effect transistor ,Electrical and Electronic Engineering ,business ,Noise (radio) - Abstract
Si and GaAs Schottky-barrier field-effect transistors with gate lengths of 0.5 μm have been experimentally realised. Noise and gain properties were measured in the microwave range up to 20 GHz. When compared with 1 μm-gate f.e.t.s, the devices show considerable improvements in gain and in noise figure. At 10 GHz, the following values were measured: Si m.e.s.f.e.t.: maximum available gain = 5.9 dB, noise figure = 5.8 dB; GaAs m.e.s.f.e.t.: maximum available gain = 12.8 dB, noise figure = 3.7 dB.
- Published
- 1973
- Full Text
- View/download PDF
27. X- and Ku-band amplifiers with GaAs Schottky-barrier FETS
- Author
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W. Baechtold
- Subjects
Materials science ,business.industry ,Amplifier ,Schottky barrier ,Transistor array ,Y-factor ,Noise figure ,Ku band ,Low-noise amplifier ,Gallium arsenide ,chemistry.chemical_compound ,chemistry ,Optoelectronics ,business - Abstract
This paper will report on two low-power FET amplifiers: 8.2 GHz with 17.5-dB gain and 1.3-GHz bandwidth; 9.5-14.3 GHz with 8.5-dB gain.
- Published
- 1972
- Full Text
- View/download PDF
28. An efficient system-oriented VCSEL model including 2D modal dynamics and thermal effects
- Author
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W. Baechtold, Daniel Erni, and M. Jungo
- Subjects
Physics ,Field (physics) ,business.industry ,Orders of magnitude (temperature) ,law.invention ,Vertical-cavity surface-emitting laser ,Transverse plane ,Modal ,law ,Laser diode rate equations ,Optical cavity ,Optoelectronics ,Semiconductor optical gain ,Statistical physics ,business - Abstract
We propose a new system-oriented 2D VCSEL model, which takes into account the detailed interactions between the transverse carrier and field distributions. It shows several orders of magnitude improvement in computational efficiency compared to conventional models.
29. Q band GaAs f.e.t. amplifier and oscillator
- Author
-
W. Baechtold
- Subjects
Physics ,Power gain ,Range (particle radiation) ,business.industry ,Amplifier ,Transistor ,law.invention ,Power (physics) ,Q band ,law ,Optoelectronics ,Field-effect transistor ,Electrical and Electronic Engineering ,business ,Stripline - Abstract
GaAs field-effect transistors with a Schottky-barrier gate have been investigated in the frequency range 12–20 GHz. Measurements of the maximum available gain have shown that the devices have much higher gain in this range than has been expected. A 17 GHz oscillator having an output power of 4mW and a 4-stage 14.9GHz amplifier with 16 dB of power gain have been built using stripline technique.
- Published
- 1971
- Full Text
- View/download PDF
30. Author's reply to 'Comments on 'noise behavior of GaAs field-effect transistors with short gate length''
- Author
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W. Baechtold
- Subjects
Physics ,Noise ,business.industry ,Gate length ,Electrical engineering ,Field-effect transistor ,Electrical and Electronic Engineering ,business ,Electronic, Optical and Magnetic Materials - Published
- 1973
- Full Text
- View/download PDF
31. Complementary Josephson-junction circuit: a fast flip-flop and logic gate
- Author
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W. Heuberger, Th. O. Mohr, W. Baechtold, and Th. Forster
- Subjects
Physics ,Josephson effect ,Pass transistor logic ,business.industry ,Electrical engineering ,Hardware_PERFORMANCEANDRELIABILITY ,Resistor–transistor logic ,law.invention ,law ,Logic gate ,Hardware_INTEGRATEDCIRCUITS ,Inverter ,Equivalent circuit ,Hardware_ARITHMETICANDLOGICSTRUCTURES ,Electrical and Electronic Engineering ,business ,Flip-flop ,AND gate ,Hardware_LOGICDESIGN - Abstract
A logic circuit with Josephson junctions has been developed that operates as logic gate or as a flip-flop. Despite the latching-type characteristic of the Josephson tunnel junction, the complementary logic circuit is nonlatching. The test circuit has a power dissipation of 16.4 μW and a signal risetime of approximately 60 ps has been measured.
- Published
- 1975
- Full Text
- View/download PDF
32. An improved microwave silicon MESFET
- Author
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W. Baechtold and P. Wolf
- Subjects
Materials science ,Silicon ,Equivalent series resistance ,Oscillation ,business.industry ,Transistor ,Electrical engineering ,chemistry.chemical_element ,Condensed Matter Physics ,Noise figure ,Electronic, Optical and Magnetic Materials ,law.invention ,chemistry ,law ,Materials Chemistry ,Optoelectronics ,MESFET ,Parasitic extraction ,Electrical and Electronic Engineering ,business ,Microwave - Abstract
An improved silicon MESFET with a 1; gate is described which has a maximum frequency of oscillation of 15 GHz. The improvement over previous MESFET's has been achieved by reducing the influence of the resistance of the gate metallization and by decreasing the gate-pad parasitics. Maximum available gain MAG is now 5 dB at 7 GHz and the optimum noise figure F 0 is 5 dB at 6 GHz. Below about 6 GHz the device is conditionally unstable. Unilateral gain U up to 3 GHz is 20 dB. The investigation indicates that not all parasitics have been removed. If the series resistance of the channel in the source-gate spacing could be decreased, f max should approach 35 GHz the estimated value of the intrinsic transistor.
- Published
- 1971
- Full Text
- View/download PDF
33. X and Ku band GaAs m.e.s.f.e.t
- Author
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P. Wolf, W. Baechtold, and W. Walter
- Subjects
Power gain ,Physics ,business.industry ,X band ,Optoelectronics ,MESFET ,Field-effect transistor ,Electrical and Electronic Engineering ,business ,Noise figure ,Ku band ,Noise (radio) - Abstract
A GaAs Schottky-barrier f.e.t. (m.e.s.f.e.t.) with a 1 ?m gate has been built, which is suitable for X band and Ku band applications. The unilateral power gain over the X band is above 9 dB and the noise figure is only 5 dB at 10 GHz.
- Published
- 1972
- Full Text
- View/download PDF
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