Design of a tunable multi-band differential LC VCO using 0.35 mu m SiGe BiCMOS technology for multi-standard wireless communication systems

In this paper, an integrated 2.2-5.7GHz multi-band differential LC VCO for multi-standard wireless communication systems was designed utilizing 0.35 mu m SiGe BiCMOS technology. The topology, which combines the switching inductors and capacitors together in the same circuit, is a novel approach for wideband VCOs. Based on the post-layout simulation results, the VCO can be tuned using a DC voltage of 0 to 3.3 V for 5 different frequency bands (2.27-2.51 GHz, 2.48-2.78 GHz, 3.22-3.53 GHz, 3.48-3.91 GHz and 4.528-5.7 GHz) with a maximum bandwidth of 1.36 GHz and a minimum bandwidth of 300 MHz. The designed and simulated VCO can generate a differential output power between 0.992 and -6.087 dBm with an average power consumption of 44.21 mW including the buffers. The average second and third harmonics level were obtained as -37.21 and -47.6 dBm, respectively. The phase noise between -110.45 and -122.5 dBc/Hz, that was simulated at 1 MHz offset, can be obtained through the frequency of interest. Additionally, the figure of merit (FOM), that includes all important parameters such as the phase noise, the power consumption and the ratio of the operating frequency to the offset frequency, is between -176.48 and -181.16 and comparable or better than the ones with the other current VCOs. The main advantage of this study in comparison with the other VCOs, is covering 5 frequency bands starting from 2.27 up to 5.76 GHz without FOM and area abandonment. Output power of the fundamental frequency changes between -6.087 and 0.992 dBm, depending on the bias conditions (operating bands). Based on the post-layout simulation results, the core VCO circuit draws a current between 2.4-6.3 mA and between 11.4 and 15.3 mA with the buffer circuit from 3.3 V supply. The circuit occupies an area of 1.477 mm(2) on Si substrate, including DC, digital and RF pads

RF CMOS quadrature voltage-controlled oscillator design using superharmonic coupling method.

Chung, Wai Fung.Thesis (M.Phil.)--Chinese University of Hong Kong, 2007.Includes bibliographical references (leaves 98-100).Abstracts in English and Chinese.摘要 --- p.IIIACKNOWLEDGEMENT --- p.IVCONTENTS --- p.VLIST OF FIGURES --- p.VIIILIST OF TABLES --- p.XLIST OF TABLES --- p.XChapter CHAPTER 1 --- INTRODUCTION --- p.1Chapter 1.1 --- Motivation --- p.1Chapter 1.2 --- Receiver Architecture --- p.3Chapter 1.2.1 --- Zero-IF Receivers --- p.4Chapter 1.2.2 --- Low-IF Receivers --- p.6Chapter 1.2.2.1 --- Hartley Architecture --- p.7Chapter 1.2.2.2 --- Weaver Architecture --- p.9Chapter 1.3 --- Image-rejection ratio --- p.10Chapter 1.4 --- Thesis Organization --- p.12Chapter CHAPTER 2 --- FUNDAMENTALS OF OSCILLATOR --- p.13Chapter 2.1 --- Basic Oscillator Theory --- p.13Chapter 2.2 --- Varactor --- p.15Chapter 2.3 --- Inductor --- p.17Chapter 2.4 --- Phase noise --- p.22Chapter 2.4.1 --- The Leeson ´ةs phase noise expression --- p.24Chapter 2.4.2 --- Linear model --- p.25Chapter 2.4.3 --- Linear Time-Variant phase noise model --- p.28Chapter CHAPTER 3 --- FULLY-INTEGRATED CMOS OSCILLATOR DESIGN --- p.31Chapter 3.1 --- Ring oscillator --- p.31Chapter 3.2 --- LC oscillator --- p.33Chapter 3.2.1 --- LC-tank resonator --- p.34Chapter 3.2.2 --- Negative transconductance --- p.36Chapter 3.3 --- Generation of quadrature phase signals --- p.39Chapter 3.4 --- Quadrature VCO topologies --- p.41Chapter 3.4.1 --- Parallel-coupled QVCO --- p.41Chapter 3.4.2 --- Series-coupled QVCO --- p.46Chapter 3.4.3 --- QVCO with Back-gate Coupling --- p.47Chapter 3.4.4 --- QVCO using superharmonic coupling --- p.49Chapter 3.5 --- Novel QVCO using back-gate superharmonic coupling --- p.52Chapter 3.5.1 --- Tuning range --- p.54Chapter 3.5.2 --- Negative gm --- p.55Chapter 3.5.3 --- Phase noise calculation --- p.56Chapter 3.5.4 --- Coupling coefficient --- p.57Chapter 3.5.5 --- Low-voltage and low-power design --- p.59Chapter 3.5.6 --- Layout Consideration --- p.61Chapter 3.5.6.1 --- Symmetrical Layout and parasitics --- p.61Chapter 3.5.6.2 --- Metal width and number of vias --- p.63Chapter 3.5.6.3 --- Substrate contact and guard ring --- p.63Chapter 3.5.7 --- Simulation Results --- p.65Chapter 3.5.7.1 --- Frequency and output power --- p.65Chapter 3.5.7.2 --- Quadrature signal generation --- p.67Chapter 3.5.7.3 --- Tuning range --- p.67Chapter 3.5.7.4 --- Power consumption --- p.68Chapter 3.5.7.5 --- Phase noise --- p.69Chapter 3.6 --- Polyphase filter and Single-sideband mixer design --- p.70Chapter 3.6.1 --- Polyphase filter --- p.72Chapter 3.6.2 --- Layout Consideration --- p.74Chapter 3.6.3 --- Simulation results --- p.76Chapter 3.7 --- Comparison with parallel-coupled QVCO --- p.78Chapter CHAPTER 4 --- EXPERIMENTAL RESULTS --- p.80Chapter 4.1 --- Test Fixture --- p.82Chapter 4.2 --- Measurement set-up --- p.84Chapter 4.3 --- Measurement results --- p.86Chapter 4.3.1 --- Proposed QVCO using back-gate superharmonic coupling --- p.86Chapter 4.3.1.1 --- Output Spectrum --- p.86Chapter 4.3.1.2 --- Tuning range --- p.87Chapter 4.3.1.3 --- Phase noise --- p.88Chapter 4.3.1.4 --- Power consumption --- p.88Chapter 4.3.1.5 --- Image-rejection ratio --- p.89Chapter 4.3.2 --- Parallel-coupled QVCO --- p.90Chapter 4.3.2.1 --- Output spectrum --- p.90Chapter 4.3.2.2 --- Power consumption --- p.90Chapter 4.3.2.3 --- Tuning range --- p.91Chapter 4.3.2.4 --- Phase noise --- p.92Chapter 4.3.3 --- Comparison between proposed and parallel-coupled QVCO --- p.93Chapter CHAPTER 5 --- CONCLUSIONS --- p.95Chapter 5.1 --- Conclusions --- p.95Chapter 5.2 --- Future work --- p.97REFERENCES --- p.9

Analysis of the high frequency substrate noise effects on LC-VCOs

La integració de transceptors per comunicacions de radiofreqüència en CMOS pot quedar seriosament limitada per la interacció entre els seus blocs, arribant a desaconsellar la utilització de un únic dau de silici. El soroll d’alta freqüència generat per certs blocs, com l’amplificador de potencia, pot viatjar pel substrat i amenaçar el correcte funcionament de l’oscil·lador local. Trobem tres raons importants que mostren aquest risc d’interacció entre blocs i que justifiquen la necessitat d’un estudi profund per minimitzar-lo. Les característiques del substrat fan que el soroll d’alta freqüència es propagui m’és fàcilment que el de baixa freqüència. Per altra banda, les estructures de protecció perden eficiència a mesura que la freqüència augmenta. Finalment, el soroll d’alta freqüència que arriba a l’oscil·lador degrada al seu correcte comportament. El propòsit d’aquesta tesis és analitzar en profunditat la interacció entre el soroll d’alta freqüència que es propaga pel substrat i l’oscil·lador amb l’objectiu de poder predir, mitjançant un model, l’efecte que aquest soroll pot tenir sobre el correcte funcionament de l’oscil·lador. Es volen proporcionar diverses guies i normes a seguir que permeti als dissenyadors augmentar la robustesa dels oscil·ladors al soroll d’alta freqüència que viatja pel substrat. La investigació de l’efecte del soroll de substrat en oscil·ladors s’ha iniciat des d’un punt de vista empíric, per una banda, analitzant la propagació de senyals a través del substrat i avaluant l’eficiència d’estructures per bloquejar aquesta propagació, i per altra, determinant l’efecte d’un to present en el substrat en un oscil·lador. Aquesta investigació ha mostrat que la injecció d’un to d’alta freqüència en el substrat es pot propagar fins arribar a l’oscil·lador i que, a causa del ’pulling’ de freqüència, pot modular en freqüència la sortida de l’oscil·lador. A partir dels resultats de l’anàlisi empíric s’ha aportat un model matemàtic que permet predir l’efecte del soroll en l’oscil·lador. Aquest model té el principal avantatge en el fet de que està basat en paràmetres físics de l’oscil·lador o del soroll, permetent determinar les mesures que un dissenyador pot prendre per augmentar la robustesa de l’oscil·lador així com les conseqüències que aquestes mesures tenen sobre el seu funcionament global (trade-offs). El model ha estat comparat tant amb simulacions com amb mesures reals demostrant ser molt precís a l’hora de predir l’efecte del soroll de substrat. La utilitat del model com a eina de disseny s’ha demostrat en dos estudis. Primerament, les conclusions del model han estat aplicades en el procés de disseny d’un oscil·lador d’ultra baix consum a 2.5GHz, aconseguint un oscil·lador robust al soroll de substrat d’alta freqüència i amb característiques totalment compatibles amb els principals estàndards de comunicació en aquesta banda. Finalment, el model s’ha utilitzat com a eina d’anàlisi per avaluar la causa de les diferències, en termes de robustesa a soroll de substrat, mesurades en dos oscil·ladors a 60GHz amb dues diferents estratègies d’apantallament de l’inductor del tanc de ressonant, flotant en un cas i connectat a terra en l’altre. El model ha mostrat que les diferències en robustesa són causades per la millora en el factor de qualitat i en l’amplitud d’oscil·lació i no per un augment en l’aïllament entre tanc i substrat. Per altra banda, el model ha demostrat ser vàlid i molt precís inclús en aquest rang de freqüència tan extrem. el principal avantatge en el fet de que està basat en paràmetres físics de l’oscil·lador o del soroll, permetent determinar les mesures que un dissenyador pot prendre per augmentar la robustesa de l’oscil·lador així com les conseqüències que aquestes mesures tenen sobre el seu funcionament global (trade-offs). El model ha estat comparat tant amb simulacions com amb mesures reals demostrant ser molt precís a l’hora de predir l’efecte del soroll de substrat. La utilitat del model com a eina de disseny s’ha demostrat en dos estudis. Primerament, les conclusions del model han estat aplicades en el procés de disseny d’un oscil·lador d’ultra baix consum a 2.5GHz, aconseguint un oscil·lador robust al soroll de substrat d’alta freqüència i amb característiques totalment compatibles amb els principals estàndards de comunicació en aquesta banda. Finalment, el model s’ha utilitzat com a eina d’anàlisi per avaluar la causa de les diferències, en termes de robustesa a soroll de substrat, mesurades en dos oscil·ladors a 60GHz amb dues diferents estratègies d’apantallament de l’inductor del tanc de ressonant, flotant en un cas i connectat a terra en l’altre. El model ha mostrat que les diferències en robustesa són causades per la millora en el factor de qualitat i en l’amplitud d’oscil·lació i no per un augment en l’aïllament entre tanc i substrat. Per altra banda, el model ha demostrat ser vàlid i molt precís inclús en aquest rang de freqüència tan extrem.The integration of transceivers for RF communication in CMOS can be seriously limited by the interaction between their blocks, even advising against using a single silicon die. The high frequency noise generated by some of the blocks, like the power amplifier, can travel through the substrate, reaching the local oscillator and threatening its correct performance. Three important reasons can be stated that show the risk of the single die integration. Noise propagation is easier the higher the frequency. Moreover, the protection structures lose efficiency as the noise frequency increases. Finally, the high frequency noise that reaches the local oscillator degrades its performance. The purpose of this thesis is to deeply analyze the interaction between the high frequency substrate noise and the oscillator with the objective of being able to predict, thanks to a model, the effect that this noise may have over the correct behavior of the oscillator. We want to provide some guidelines to the designers to allow them to increase the robustness of the oscillator to high frequency substrate noise. The investigation of the effect of the high frequency substrate noise on oscillators has started from an empirical point of view, on one hand, analyzing the noise propagation through the substrate and evaluating the efficiency of some structures to block this propagation, and on the other hand, determining the effect on an oscillator of a high frequency noise tone present in the substrate. This investigation has shown that the injection of a high frequency tone in the substrate can reach the oscillator and, due to a frequency pulling effect, it can modulate in frequency the output of the oscillator. Based on the results obtained during the empirical analysis, a mathematical model to predict the effect of the substrate noise on the oscillator has been provided. The main advantage of this model is the fact that it is based on physical parameters of the oscillator and of the noise, allowing to determine the measures that a designer can take to increase the robustness of the oscillator as well as the consequences (trade-offs) that these measures have over its global performance. This model has been compared against both, simulations and real measurements, showing a very high accuracy to predict the effect of the high frequency substrate noise. The usefulness of the presented model as a design tool has been demonstrated in two case studies. Firstly, the conclusions obtained from the model have been applied in the design of an ultra low power consumption 2.5 GHz oscillator robust to the high frequency substrate noise with characteristics which make it compatible with the main communication standards in this frequency band. Finally, the model has been used as an analysis tool to evaluate the cause of the differences, in terms of performance degradation due to substrate noise, measured in two 60 GHz oscillators with two different tank inductor shielding strategies, floating and grounded. The model has determined that the robustness differences are caused by the improvement in the tank quality factor and in the oscillation amplitude and no by an increased isolation between the tank and the substrate. The model has shown to be valid and very accurate even in these extreme frequency range.Postprint (published version

Clock Generation Design for Continuous-Time Sigma-Delta Analog-To-Digital Converter in Communication Systems

Software defined radio, a highly digitized wireless receiver, has drawn huge attention in modern communication system because it can not only benefit from the advanced technologies but also exploit large digital calibration of digital signal processing (DSP) to optimize the performance of receivers. Continuous-time (CT) bandpass sigma-delta (ΣΔ) modulator, used as an RF-to-digital converter, has been regarded as a potential solution for software defined ratio. The demand to support multiple standards motivates the development of a broadband CT bandpass ΣΔ which can cover the most commercial spectrum of 1GHz to 4GHz in a modern communication system. Clock generation, a major building block in radio frequency (RF) integrated circuits (ICs), usually uses a phase-locked loop (PLL) to provide the required clock frequency to modulate/demodulate the informative signals. This work explores the design of clock generation in RF ICs. First, a 2-16 GHz frequency synthesizer is proposed to provide the sampling clocks for a programmable continuous-time bandpass sigma-delta (ΣΔ) modulator in a software radio receiver system. In the frequency synthesizer, a single-sideband mixer combines feed-forward and regenerative mixing techniques to achieve the wide frequency range. Furthermore, to optimize the excess loop delay in the wideband system, a phase-tunable clock distribution network and a clock-controlled quantizer are proposed. Also, the false locking of regenerative mixing is solved by controlling the self-oscillation frequency of the CML divider. The proposed frequency synthesizer performs excellent jitter performance and efficient power consumption. Phase noise and quadrature phase accuracy are the common tradeoff in a quadrature voltage-controlled oscillator. A larger coupling ratio is preferred to obtain good phase accuracy but suffer phase noise performance. To address these fundamental trade-offs, a phasor-based analysis is used to explain bi-modal oscillation and compute the quadrature phase errors given by inevitable mismatches of components. Also, the ISF is used to estimate the noise contribution of each major noise source. A CSD QVCO is first proposed to eliminate the undesired bi-modal oscillation and enhance the quadrature phase accuracy. The second work presents a DCC QVCO. The sophisticated dynamic current-clipping coupling network reduces injecting noise into LC tank at most vulnerable timings (zero crossing points). Hence, it allows the use of strong coupling ratio to minimize the quadrature phase sensitivity to mismatches without degrading the phase noise performance. The proposed DCC QVCO is implemented in a 130-nm CMOS technology. The measured phase noise is -121 dBc/Hz at 1MHz offset from a 5GHz carrier. The QVCO consumes 4.2mW with a 1-V power supply, resulting in an outstanding Figure of Merit (FoM) of 189 dBc/Hz. Frequency divider is one of the most power hungry building blocks in a PLL-based frequency synthesizer. The complementary injection-locked frequency divider is proposed to be a low-power solution. With the complimentary injection schemes, the dividers can realize both even and odd division modulus, performing a more than 100% locking range to overcome the PVT variation. The proposed dividers feature excellent phase noise. They can be used for multiple-phase generation, programmable phase-switching frequency dividers, and phase-skewing circuits

Design of frequency synthesizers for short range wireless transceivers

The rapid growth of the market for short-range wireless devices, with standards such as Bluetooth and Wireless LAN (IEEE 802.11) being the most important, has created a need for highly integrated transceivers that target drastic power and area reduction while providing a high level of integration. The radio section of the devices designed to establish communications using these standards is the limiting factor for the power reduction efforts. A key building block in a transceiver is the frequency synthesizer, since it operates at the highest frequency of the system and consumes a very large portion of the total power in the radio. This dissertation presents the basic theory and a design methodology of frequency synthesizers targeted for short-range wireless applications. Three different examples of synthesizers are presented. First a frequency synthesizer integrated in a Bluetooth receiver fabricated in 0.35μm CMOS technology. The receiver uses a low-IF architecture to downconvert the incoming Bluetooth signal to 2MHz. The second synthesizer is integrated within a dual-mode receiver capable of processing signals of the Bluetooth and Wireless LAN (IEEE 802.11b) standards. It is implemented in BiCMOS technology and operates the voltage controlled oscillator at twice the required frequency to generate quadrature signals through a divide-by-two circuit. A phase switching prescaler is featured in the synthesizer. A large capacitance is integrated on-chip using a capacitance multiplier circuit that provides a drastic area reduction while adding a negligible phase noise contribution. The third synthesizer is an extension of the second example. The operation range of the VCO is extended to cover a frequency band from 4.8GHz to 5.85GHz. By doing this, the synthesizer is capable of generating LO signals for Bluetooth and IEEE 802.11a, b and g standards. The quadrature output of the 5 - 6 GHz signal is generated through a first order RC - CR network with an automatic calibration loop. The loop uses a high frequency phase detector to measure the deviation from the 90° separation between the I and Q branches and implements an algorithm to minimize the phase errors between the I and Q branches and their differential counterparts

System-level design and RF front-end implementation for a 3-10ghz multiband-ofdm ultrawideband receiver and built-in testing techniques for analog and rf integrated circuits

This work consists of two main parts: a) Design of a 3-10GHz UltraWideBand (UWB) Receiver and b) Built-In Testing Techniques (BIT) for Analog and RF circuits. The MultiBand OFDM (MB-OFDM) proposal for UWB communications has received significant attention for the implementation of very high data rate (up to 480Mb/s) wireless devices. A wideband LNA with a tunable notch filter, a downconversion quadrature mixer, and the overall radio system-level design are proposed for an 11-band 3.4-10.3GHz direct conversion receiver for MB-OFDM UWB implemented in a 0.25mm BiCMOS process. The packaged IC includes an RF front-end with interference rejection at 5.25GHz, a frequency synthesizer generating 11 carrier tones in quadrature with fast hopping, and a linear phase baseband section with 42dB of gain programmability. The receiver IC mounted on a FR-4 substrate provides a maximum gain of 67-78dB and NF of 5-10dB across all bands while consuming 114mA from a 2.5V supply. Two BIT techniques for analog and RF circuits are developed. The goal is to reduce the test cost by reducing the use of analog instrumentation. An integrated frequency response characterization system with a digital interface is proposed to test the magnitude and phase responses at different nodes of an analog circuit. A complete prototype in CMOS 0.35mm technology employs only 0.3mm2 of area. Its operation is demonstrated by performing frequency response measurements in a range of 1 to 130MHz on 2 analog filters integrated on the same chip. A very compact CMOS RF RMS Detector and a methodology for its use in the built-in measurement of the gain and 1dB compression point of RF circuits are proposed to address the problem of on-chip testing at RF frequencies. The proposed device generates a DC voltage proportional to the RMS voltage amplitude of an RF signal. A design in CMOS 0.35mm technology presents and input capacitance <15fF and occupies and area of 0.03mm2. The application of these two techniques in combination with a loop-back test architecture significantly enhances the testability of a wireless transceiver system

Quadrature Frequency Synthesis for Wideband Wireless Transceivers

University of Minnesota Ph.D. dissertation. May 2014. Major: Electrical Engineering. Advisor: Ramesh Harjani. 1 computer file (PDF); xi, 112 pages.In this thesis, three different techniques pertinent to quadrature LO generation in high data rate and wideband RF transceivers are presented. Prototype designs are made to verify the performance of the proposed techniques, in three different technologies: IBM 130nm CMOS process, TSMC 65nm CMOS process and IBM 32nm SOI process. The three prototype designs also cover three different frequency bands, ranging from 5GHz to 74GHz. First, an LO generation scheme for a 21 GHz center-frequency, 4-GHz instantaneous bandwidth channelized receiver is presented. A single 1.33 GHz reference source is used to simultaneously generate 20 GHz and 22 GHz LOs with quadrature outputs. Injection locking is used instead of conventional PLL techniques allowing low-power quadrature generation. A harmonic-rich signal, containing both even and odd harmonics of the input reference signal, is generated using a digital pulse slimmer. Two ILO chains are used to lock on to the 10th and 11th harmonics of the reference signal generating the 20 GHz and the 22 GHz quadrature LOs respectively. The prototype design is implemented in IBM's 130 nm CMOS process, draws 110 mA from a 1.2 V supply and occupies an active area of 1.8 square-mm. Next, a wide-tuning range QVCO with a novel complimentary-coupling technique is presented. By using PMOS transistors for coupling two VCOs with NMOS gm-cells, it is shown that significant phase-noise improvement (7-9 dB) can be achieved over the traditional NMOS coupling. This breaks the trade-off between quadrature accuracy and phase-noise, allowing reasonable accuracy without a significant phase-noise hit. The proposed technique is frequency-insensitive, allowing robust coupling over a wide tuning range. A prototype design is done in TSMC 65nm process, with 4-bits of discrete tuning spanning the frequency range 4.6-7.8 GHz (52% FTR) while achieving a minimum FOM of 181.4dBc/Hz and a minimum FOMT of 196dBc/Hz. Finally, a wide tuning-range millimeter wave QVCO is presented that employs a modified transformer-based super-harmonic coupling technique. Using the proposed technique, together with custom-designed inductors and metal capacitors, a prototype is designed in IBM 32nm SOI technology with 6-bits of discrete tuning using switched capacitors. Full EM-extracted simulations show a tuning range of 53.84GHz to 73.59GHz, with an FOM of 173 dBc/Hz and an FOMT of 183 dBc/Hz. With 19.75GHz of tuning range around a 63.7GHz center frequency, the simulated FTR is 31%, surpassing all similar designs in the same band. A slight modification in the tank inductors would enable the QVCO to be employed in multiple mm-Wave bands (57-66 GHz communication band, 71-76 GHz E-band, and 76-77 GHz radar band)