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Heterodyne techniques in specialised radio instrumentationWadley, T. L. 10 July 2015 (has links)
Thesis (D.Sc.)--University of the Witwatersrand, Faculty of Science, 1959.
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Développement de récepteurs hétérodynes multi-pixels pour les futures missions spatiales / Development of multipixel heterodyne imaging arrays for future space missionsDelfini, Duccio 08 October 2018 (has links)
L'observation du milieu interstellaire est très importante aux fréquences mm / (sub) mm / Thz pour comprendre comment se forment les étoiles et les planètes. De telles observations dépendent des récepteurs hétérodynes. Ces instruments atteignent une résolution spectrale très élevée en convertissant un signal haute fréquence à une fréquence plus basse. Dans un récepteur hétérodyne, le signal collecté est superposé sur un signal artificiel, bien connu, monochromatique, généré par l'oscillateur local (OL), donc ce signal artificiel est plus-ou-moins la fréquence du signal du ciel. Le mélangeur produit le signal de la fréquence du battement. Cette fréquence est équivalente à la différence entre le OL et la fréquence du signal du ciel. Ainsi, le signal du ciel est traduit à une fréquence plus basse, pour qu'il soit facile à amplifier et détecter. Habituellement, les récepteurs hétérodynes ont seulement un pixel spatial avec de nombreux canaux en fréquences. Notre objectif est de développer des réseaux de centaines de pixels. Pour faire cela, certains composants de l'hétérodyne doivent être repensés radicalement, tels que l'antenne de réception et le diviseur de faisceau OL. En effet, l'antenne réceptrice est généralement constituée d'une antenne à double fentes sur une lentille, ou d'une antenne cornet. Par contre, ces antennes ne sont pas les meilleurs choix pour des réseaux de nombreux pixels car elles doivent être usinées et montées individuellement. Au lieu de cela, il est commode de développer des structures planaires qui peuvent être facilement produites toutes ensembles. En particulier, nous avons conçu et simulé des réseaux d'antennes patch, de réseaux de transmission, et de plaques de zone. Le réseau d'antennes patch consiste d'un réseau de patchs métalliques reliés par une ligne microruban et séparés du plan de masse par un substrat diélectrique. Cette configuration profite du facteur du réseau pour réduire la largeur de faisceau du signal collecté. Cependant, nos simulations nous montrent que la bande RF des réseaux d'antennes patch est étroite. Pour cette raison, nous avons analysé la possibilité d'utiliser une autre solution : le réseau de transmission. C'est un réseau de plusieurs cellules qui déphase une onde afin de transformer son front de phase de forme planaire en forme sphérique. Le but de la matrice de transmission est de focaliser le faisceau collecté vers une antenne et mélangeur à double fentes. La thés démontre qu'un effet de focalisation satisfaisant est atteint sur une ligne. Nous avons fabriqué un tel réseau de transmission et l'avons testé en laboratoire. En raison des petites dimensions de quelques millimètres, ces tests sont difficiles à réaliser. Au sein de l'erreur de mesure, la conception et les simulations sont cohérentes. Une troisième option (d'une lentille planaire) a été étudiée dans la thèse : la plaque de zone. C'est un type particulier de réseau de transmission qui ne présente que deux déphasages de 0 ° et 180 °. Le plaque de zone focalise bien, mais est peu efficace. La dernière partie de la thèse introduit un type de diviseur de faisceau particulier qui permet une division du faisceau du signal OL vers un réseau de quatre mélangeurs très serrés. Diviser le faisceau avec des angles suffisamment petits est très difficile avec les réseaux de Fourier et Dammann classiques. Pour cette raison la méthode que nous avons proposée pour concevoir un tel diviseur est très novatrice. En effet, il permet la formation de motifs de faisceaux de forme arbitraire, qui ne sont pas limités par les ordres de diffraction. Les simulations montrent des efficacités allant jusqu'à 80% qui sont très bonnes en comparaison avec les réseaux classiques. En résumé, dans cette thèse, j'ai essayé plusieurs moyens radicalement différents pour simplifier les récepteurs hétérodynes et ouvrir la voie aux grandes matrices hétérodynes avec des centaines de pixels. / The observation of the interstellar medium is very important at mm/(sub)mm/THz frequencies to understand how stars and planets form. Generally such observations rely on heterodyne receivers. These are instruments that achieve very high spectral resolution by down converting a high frequency signal towards a lower frequency one. In a heterodyne receiver the incoming signal is superimposed onto an artificial, well-known, monochromatic signal generated by the local oscillator (LO), chosen to be close to the frequency of the sky signal. The mixer produces the beat frequency signal. It has a frequency equivalent to the difference between the LO and sky signal frequency. Thus the sky signal is translated to a lower frequency, and it is easier to amplify and detect. Usually heterodyne receivers have only one spatial pixel with many frequency channels. Some prototypes have been realized recently with few pixels. Our objective is to develop arrays of hundreds of pixels. In order to do that, some components which compose the heterodyne receiver must be radically rethought, such as the receiving antenna and the LO beam divider.Indeed the receiving antenna generally consists of a double slot antenna on a lens, or a horn antenna. Such antennas are not the best choice for arrays of many pixels since they have to be machined and mounted individually. Instead it is convenient to develop planar structures which can be easily produced in bulk in a single process. In particular we designed and simulated arrays of patch antennas, transmit-arrays and zone plates. The array of patch antennas consists of an array of metallic patches connected via a microstrip line and separated from the ground plane by a dielectric substrate. This configuration takes advantage of the array factor to reduce the beamwidth of the incoming signal in place of the lens. However our simulations showed the array of patch antennas to be quite narrowband for a general purpose application, and quite difficult to realize. For this reason we also analyzed the possibility to use another solution such as the transmit-array. It is an array of several cells which provide a certain phase shift to an incoming wave in order to transform its phase front from planar to spherical. The purpose of the transmit-array is to focus the incoming beam towards a double slot antenna and a mixer placed below it. The simulations showed that a good focusing effect can be reached on a line. We fabricated such a transmit-array and tested it in the laboratory. Because of the small dimensions of a few millimeters these tests are difficult to carry out. Within the measurement error design and simulations are consistent. A third option of a planar lens was studied in the thesis: the zone plate. This is a particular kind of transmit-array which presents only two phase shift of 0° and 180°. The zone plates focus well, but are unfortunately not very efficient.The final part of the thesis introduces a particular kind of beam divider which allows beam splitting of the LO signal towards an array of four very closely packed mixers. To split the beam with such small relative angles is very difficult with the classical Fourier and Dammann grating, for this reason the method we proposed to design such a beam divider is very innovative. Indeed it allows the forming of arbitrary shaped beam patterns, which are not limited by the diffraction orders. Simulations show efficiencies up to 80% which are very good in comparison with classical gratings.In summary in this thesis I have tried several radically different approaches to simplify heterodyne receivers and made a first step towards for large heterodyne arrays with hundreds of pixels.
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As personagens e suas estórias: uma leitura de três narrativas de \'Corpo de Baile\', de Guimarães Rosa / The protagonists and their tales: an analyzis of three novels from the book Corpo de Baile by Guimarães RosaPassarelli, Paula 25 February 2008 (has links)
A relação entre criador e receptor se faz presente de forma peculiar em grande parte das obras de João Guimarães Rosa, inserida também intratextualmente em suas estórias. Para destacar tal relação, serão analisadas três novelas de Corpo de Baile: \"Campo Geral\", \"Cara-de-Bronze\" e \"Dão-lalalão\". Embora haja contadores ao longo de todo o ciclo novelístico, o corpus escolhido apresenta mais acentuadamente protagonistas que narram para os outros e, de certa forma, para si mesmos. Miguilim narra principalmente estórias infantis; Grivo reconta a trajetória pessoal de Cara-de-Bronze, modificando a versão inventada e vivida pelo fazendeiro, e, por fim, Soropita repassa questões pessoais por meio de devaneios. As estórias internas provocam um efeito sobre seus ouvintes, agindo ora como aprendizado, ora como impulso para buscas ou para ações distintas. A partir daí, este trabalho tem por objetivo tanto delimitar os criadores e receptores dessas estórias, refletindo acerca de seus papéis, quanto evidenciar as funções e conseqüências de tais narrativas para suas personagens, mostrando que os contadores internos auxiliam, com experiências ficcionais, não só a própria \"vivência\", mas também a de seus ouvintes. / The connection between creator and receiver is present in a peculiar way in great part of the work of João Guimarães Rosa. And this is also finded intratextually in his tales. To put this connection in relief, this study will analyze three novels from the book Corpo de Baile: \"Campo Geral\", \"Cara-de-Bronze\" and \"Dão-lalalão\". Although there are storytellers in all the novelistic cycle, the chosen corpus presents with more emphasis protagonists that narrate to others and, in a certain extent, to themselves. Miguilim narrates essencially juvenile tales; Grivo retells the personal trajectory of Cara-de-Bronze, changing the invented version and the experienced one by the farmer and, at last, Soropita examines again personal matters throught dreams. The internal tales cause an effect on the listeners sometimes operating as a way of learning and sometimes as a drive to different searches and actions. From this point, the purpose of this study is to define creators and receivers of this tales, reflecting about their roles, and also emphazise functions and consequences of these accounts to its characters, demonstrating that internal storytellers favour through fictional experiences, not only their own \"experience of life\", but also the one of the listeners.
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900MHz CMOS receiver chip.January 2000 (has links)
Hon Kwok-Wai. / Thesis (M.Phil.)--Chinese University of Hong Kong, 2000. / Includes bibliographical references (leaves 89-91). / Abstracts in English and Chinese. / Chapter 1. --- System Architecture --- p.1 / Chapter 1.1 --- Introduction --- p.1 / Chapter 1.2 --- Receiver Architectures --- p.2 / Chapter 1.2.1 --- Superheterodyne Receiver --- p.2 / Chapter 1.2.2 --- Homodyne Receiver --- p.3 / Chapter 1.2.3 --- Image-Reject Receiver --- p.5 / Chapter 1.2.4 --- Low intermediate frequency Receiver --- p.7 / Chapter 1.3 --- Double Intermediate Frequency Receivers --- p.8 / Chapter 1.3.1 --- Introduction --- p.8 / Chapter 1.3.2 --- Background Theory --- p.8 / Chapter 2. --- Receiver Fundamentals --- p.23 / Chapter 2.1 --- Noise model --- p.23 / Chapter 2.1.1 --- Thermal noise of resistors --- p.23 / Chapter 2.1.2 --- Channel noise of transistors --- p.24 / Chapter 2.2 --- Noise Figure --- p.26 / Chapter 2.3 --- Linearity --- p.26 / Chapter 2.3.1 --- 1 -dB Compression point --- p.27 / Chapter 2.3.2 --- Third Intercept point (IP3) --- p.28 / Chapter 2.3.3 --- Dynamic Range (DR) --- p.30 / Chapter 2.3.3.1 --- Spurious-Free Dynamic Range (SFDR) --- p.30 / Chapter 2.3.3.2 --- Blocking Dynamic Range (BDR) --- p.32 / Chapter 3. --- Spiral Inductor --- p.33 / Chapter 3.1 --- Spiral inductor modeling --- p.34 / Chapter 3.2 --- Spiral Inductor model parameters --- p.36 / Chapter 3.3 --- Characteristic of spiral inductor --- p.36 / Chapter 3.4 --- Inductor Design and Optimization --- p.37 / Chapter 4. --- Low Noise Amplifier (LNA) --- p.39 / Chapter 4.1 --- Introduction --- p.39 / Chapter 4.2 --- Common LNA Architectures --- p.39 / Chapter 4.2.1 --- Resistive Termination --- p.39 / Chapter 4.2.2 --- 1/gm Termination --- p.42 / Chapter 4.2.3 --- Shunt-Series Feedback --- p.43 / Chapter 4.2.4 --- Inductive Source Degeneration --- p.43 / Chapter 4.3 --- Full Schematic diagram of the Low Noise Amplifier --- p.45 / Chapter 4.4 --- Full noise analysis of the LNA using inductive source degeneration --- p.46 / Chapter 4.4.1 --- Output noise due to channel noise --- p.46 / Chapter 4.4.1.1 --- Output noise due to i2d --- p.47 / Chapter 4.4.1.2 --- "Output noise due to i2g,u" --- p.47 / Chapter 4.4.1.3 --- "Output noise due to i2g,c and i2d" --- p.49 / Chapter 4.4.2 --- "Output noise due to Rg R,l Rs" --- p.51 / Chapter 4.4.3 --- Noise factor calculation --- p.52 / Chapter 4.4.3.1 --- Rl calculation --- p.52 / Chapter 4.4.3.2 --- Rg calculation --- p.52 / Chapter 4.4.3.3 --- Ql calculation --- p.53 / Chapter 4.4.3.4 --- wT calculation --- p.53 / Chapter 4.4.3.5 --- x calculation --- p.53 / Chapter 4.5 --- Simulation Result of the low noise amplifier (100 finger gate poly) --- p.54 / Chapter 4.5 --- Experimental Result of the low noise amplifier (100 finger gate poly) --- p.56 / Chapter 5. --- Down-conversion Mixer --- p.58 / Chapter 5.1 --- Introduction --- p.58 / Chapter 5.2 --- Gilbert Cell Mixer --- p.59 / Chapter 5.2.1 --- Circuit Description --- p.59 / Chapter 5.2.2 --- Basic Operation --- p.60 / Chapter 5.2.3 --- Simulation Result of the Gilbert Cell Mixer --- p.62 / Chapter 5.3 --- Single-ended to Differential-ended Converter --- p.66 / Chapter 5.3.1 --- Simulation Result of the Single-Ended to Differential-Ended Converter --- p.68 / Chapter 5.4 --- Experimental Result of The Gilbert Cell Mixer --- p.70 / Chapter 5.4.1 --- 1-dB compression point experiment --- p.70 / Chapter 5.4.2 --- IIP3 experimental setup and result --- p.72 / Chapter 5.4.3 --- "Experimental result of 1 -dB compression point, IIP3, conversion gain, SFDR and BDR" --- p.74 / Chapter 5.4.4 --- LO power verse conversion gain --- p.75 / Chapter 5.4.5 --- Intermediate frequency verse conversion gain --- p.77 / Chapter 5.4.6 --- Experimental result of input matching and isolation --- p.78 / Chapter 6. --- Asymmetric Polyphase Network --- p.81 / Chapter 6.1 --- Introduction --- p.81 / Chapter 6.2 --- Performance of the Asymmetric Polyphase Network --- p.81 / Chapter 6.2.1 --- First Building Block --- p.82 / Chapter 6.2.2 --- Second Building Block --- p.83 / Chapter 6.2.3 --- Third Building Block --- p.84 / Chapter 6.2.4 --- Forth Building Block --- p.84 / Chapter 6.3 --- Simulation result of the asymmetric polyphase network --- p.85 / Chapter 6.4 --- Experimental result of the asymmetric polyphase network --- p.86 / Chapter 7. --- Conclusion --- p.87 / Chapter 8. --- Reference --- p.89 / Chapter 9. --- Appendix A --- p.92 / Chapter 10. --- Appendix B --- p.95 / Chapter 11. --- Appendix C --- p.98 / Chapter 12. --- Appendix D --- p.99
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The RMS phase error of a phase-locked loop FM demodulator for standard NTSC videoDubbert, Dale F January 2010 (has links)
Typescript (photocopy). / Digitized by Kansas Correctional Industries / Department: Electrical and Computer Engineering.
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An AM broadcast band receiver with digitally synthesized tuning.Stanley, Lee Gage January 1978 (has links)
Thesis (B.S.)--Massachusetts Institute of Technology, Dept. of Electrical Engineering and Computer Science, 1978. / MICROFICHE COPY AVAILABLE IN ARCHIVES AND ENGINEERING. / Includes bibliographical references. / B.S.
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Switched-Capacitor RF Receivers for High Interferer ToleranceXu, Yang January 2018 (has links)
The demand for broadband wireless communication is growing rapidly, requiring more spectrum resources. However, spectrum usage is inefficient today because different frequency bands are allocated for different communication standards and most of the bands are not highly occupied.
Cognitive radio systems with dynamic spectrum access improve spectrum efficiency, but they require wideband tunable receiver hardware. In such a system, a preselect filter is required for the RF receiver front end, because an out-of-band (OB) interferer can block the front end or cause distortion, desensitizing the receiver. In a conventional solution, off-chip passive filters, such as surface-acoustic-wave (SAW) filters, are used to reject the OB interferer. However, such passive filters are hardly tunable, have large area, and are very expensive. On-chip, high-selectivity, linearly tunable RF filters are, therefore, a hot topic in RF front-end research. Switched-capacitor (SC) RF filters, such as N-path filters, feature good linearity and tunability, making them good candidates for tunable RF filters. However, N-path filters have some drawbacks: notably, a poor harmonic response and limited close-by blocker tolerance.
This thesis presents the design and implementation of several interferer-tolerant receivers based on SC technology. We present an RF receiver with a harmonic-rejecting N-path filter to improve the harmonic response of the N-path bandpass filter. It features tunable narrowband filtering and high attenuation of the third- and fifth-order LO harmonics at the LNA output, which improves the blocker tolerance at LO harmonics. The 0.2-1 GHz RF receiver is implemented in a 65 nm CMOS process. The blocker 1 dB compression point (B1dB) is -2.4 dBm at a 20 MHz offset, and remains high at the third- and fifth-order LO harmonics. The LNA’s reverse isolation helps keep the LO emission below -90 dBm. A two-stage harmonic-rejection approach offers a > 51 dB harmonic-rejection ratio at the third- and fifth-order LO harmonics without calibration.
To improve tolerance for close-by blockers, we further present an SC RF receiver achieving high-order, tunable, highly linear RF filtering. We implement RF input impedance matching, N-path filtering, high-order discrete-time infinite-impulse response (IIR) filtering and downconversion using only switches and capacitors in a 0.1-0.7 GHz prototype with tunable center frequency, programmable filter order, and very high tolerance for OB blockers. The 40 nm CMOS receiver consumes 38.5-76.5mA, achieves 40 dB gain, 24 dBm OB IIP3, 14.7 dBm B1dB for a 30MHz blocker offset, 6.8-9.7 dB noise figure, and > 66dB calibrated harmonic rejection ratio.
The key drawback of our earlier SC receiver is the relatively high theoretical lower limit of the noise figure. To improve the noise performance, we developed a 0.1-0.6 GHz chopping SC RF receiver with an integrated blocker detector. We achieve RF impedance matching, high-order OB interferer filtering, and flicker-noise chopping with passive SC circuits only. The 34-80 mW 65 nm receiver achieves 35 dB gain, 4.6-9 dB NF, 31 dBm OB-IIP3, and 15 dBm B1dB. The 0.2 mW integrated blocker detector detects large OB blockers with only a 1 us response time. The filter order can be adapted to blocker power with the blocker detector.
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Atmospheric propagation effects on heterodyne-reception optical radarsPapurt, David Michael January 1982 (has links)
Thesis (Ph.D.)--Massachusetts Institute of Technology, Dept. of Electrical Engineering and Computer Science, 1982. / MICROFICHE COPY AVAILABLE IN ARCHIVES AND ENGINEERING. / Vita. / Includes bibliographical references. / by David Michael Papurt. / Ph.D.
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Development of a computer program to simulate a noncoherent FSK system in the presence of multipath fadingBareiss, Loren D January 2010 (has links)
Photocopy of typescript. / Digitized by Kansas Correctional Industries
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Are Larger Hearing Aid Receivers Really Noisier?Johnson, Earl E. 05 January 2012 (has links)
Question: I've been fitting a lot of receiver-in-canal (RIC) products, and when I have a patient with good low-frequency hearing, I like to use the smaller gain receiver option because I worry about the larger gain receiver being noisier. Sometimes though, use of the smaller gain receiver makes it difficult to fit prescriptive targets for moderately-severe to severe high frequency hearing loss thresholds. Should I be concerned about larger receivers being noisier?
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