232 research outputs found

    Time-of-Flight Sensors in standard CMSO technologies

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    The goal of this PhD thesis is the design of time-of-flight sensors in standard CMOS technologies. For this, device level and circuit level task will be addressed. In the first case we will model and characterize the sensory structure. In the second case we will design the necessary circuitry to read the information captured by the sensors. The thesis will begin with the study of non-conventional photosensor structures in standard CMOS technologies, and will continue with the design of a specific circuitry in this technology. Finally, the selected design will be fabricated and tested

    A Bulk Driven Transimpedance CMOS Amplifier for SiPM Based Detection

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    The contribution of this work lies in the development of a bulk driven operationaltransconducctance amplifier which can be integrated with other analog circuits andphotodetectors in the same chip for compactness, miniaturization and reducing thepower. Silicon photomultipliers, also known as SiPMs, when coupled with scintillator materials are used in many imaging applications including nuclear detection. This thesis discuss the design of a bulk-driven transimpedance amplifier suitable for detectors where the front end is a SiPM. The amplifier was design and fabricated in a standard standard CMOS process and is suitable for integration with CMOS based SiPMs and commercially available SiPMs. Specifically, the amplifier was verified in simulations and experiment using circuit models for the SiPM. The bulk-driven amplifier’s performance, was compared to a commerciallyavailable amplifier with approximately the same open loop gain (70dB). Bothamplifiers were verified with two different light sources, a scintillator and a SiPM.The energy resolution using the bulk driven amplifier was 8.6% and was 14.2% forthe commercial amplifier indicating the suitability of the amplifier design for portable systems

    Single-Photon Avalanche Diodes in CMOS Technologies for Optical Communications

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    As optical communications may soon supplement Wi-Fi technologies, a concept known as visible light communications (VLC), low-cost receivers must provide extreme sensitivity to alleviate attenuation factors and overall power usage within communications link budgets. We present circuits with an advantage over conventional optical receivers, in that gain can be applied within the photodiode thus reducing the need for amplification circuits. To achieve this, single-photon avalanche diodes (SPADs) can be implemented in complementary metal-oxide-semiconductor (CMOS) technologies and have already been investigated in several topologies for VLC. The digital nature of SPADs removes the design effort used for low-noise, high-gain but high-bandwidth analogue circuits. We therefore present one of these circuit topologies, along with some common design and performance metrics. SPAD receivers are however not yet mature prompting research to take low-level parameters up to the communications level

    INTEGRATED SINGLE-PHOTON SENSING AND PROCESSING PLATFORM IN STANDARD CMOS

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    Practical implementation of large SPAD-based sensor arrays in the standard CMOS process has been fraught with challenges due to the many performance trade-offs existing at both the device and the system level [1]. At the device level the performance challenge stems from the suboptimal optical characteristics associated with the standard CMOS fabrication process. The challenge at the system level is the development of monolithic readout architecture capable of supporting the large volume of dynamic traffic, associated with multiple single-photon pixels, without limiting the dynamic range and throughput of the sensor. Due to trade-offs in both functionality and performance, no general solution currently exists for an integrated single-photon sensor in standard CMOS single photon sensing and multi-photon resolution. The research described herein is directed towards the development of a versatile high performance integrated SPAD sensor in the standard CMOS process. Towards this purpose a SPAD device with elongated junction geometry and a perimeter field gate that features a large detection area and a highly reduced dark noise has been presented and characterized. Additionally, a novel front-end system for optimizing the dynamic range and after-pulsing noise of the pixel has been developed. The pixel is also equipped with an output interface with an adjustable pulse width response. In order to further enhance the effective dynamic range of the pixel a theoretical model for accurate dead time related loss compensation has been developed and verified. This thesis also introduces a new paradigm for electrical generation and encoding of the SPAD array response that supports fully digital operation at the pixel level while enabling dynamic discrete time amplitude encoding of the array response. Thus offering a first ever system solution to simultaneously exploit both the dynamic nature and the digital profile of the SPAD response. The array interface, comprising of multiple digital inputs capacitively coupled onto a shared quasi-floating sense node, in conjunction with the integrated digital decoding and readout electronics represents the first ever solid state single-photon sensor capable of both photon counting and photon number resolution. The viability of the readout architecture is demonstrated through simulations and preliminary proof of concept measurements

    Design of CMOS Digital Silicon Photomultipliers with ToF for Positron Emission Tomography

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    This thesis presents a contribution to the design of single-photon detectors for medical imaging. Specifically, the focus has been on the development of a pixel capable of single-photon counting in CMOS technology, and the associated sensor thereof. These sensors can work under low light conditions and provide timing information to determine the time-stamp of the incoming photons. For instance, this is particularly attractive for applications that rely either on time-of-flight measurements or on exponential decay determination of the light source, like positron emission tomography or fluorescence-lifetime imaging, respectively. This thesis proposes the study of the pixel architecture to optimize its performance in terms of sensitivity, linearity and signal to noise ratio. The design of the pixel has followed a bottom-up approach, taking care of the smallest building block and studying how the different architecture choices affect performance. Among the various building blocks needed, special emphasis has been placed on the following: ‱ the Single-Photon Avalanche Diode (SPAD), a photodiode able to detect photons one by one; ‱ the front-end circuitry of this diode, commonly called quenching and recharge circuit; ‱ the Time-to-Digital Converter (TDC), which determines the timing performance of the pixel. The proposed architectural exploration provides a comprehensive insight into the design space of the pixel, allowing to determine the optimum design points in terms of sensor sensitivity, linearity or signal to noise ratio, thus helping designers to navigate through non-straightforward trade-offs. The proposed TDC is based on a voltage-controlled ring oscillator, since this architecture provides moderate time resolutions while keeping the footprint, the power, and conversion time relatively small. Two pseudo-differential delay stages have been studied, one with cross-coupled PMOS transistors and the other with cross-coupled inverters. Analytical studies and simulations have shown that cross-coupled inverters are the most appropriate to implement the TDC because they achieve better time resolution with smaller energy per conversion than cross-coupled PMOS transistor stages. A 1.3×1.3 mm2 pixel has been implemented in an 110 nm CMOS image sensor technology, to have the benefits of sub-micron technologies along with the cleanliness of CMOS image sensor technologies. The fabricated chips have been used to characterize the single-photon avalanche diodes. The results agree with expectations: a maximum photon detection probability of 46 % and a median dark count rate of 0.4 Hz/”m2 with an excess voltage of 3 V. Furthermore, the characterization of the TDC shows that the time resolution is below 100 ps, which agrees with post-layout simulations. The differential non-linearity is ±0.4LSB, and the integral non-linearity is ±6.1LSB. Photoemission occurs during characterization - an indication that the avalanches are not quenched properly. The cause of this has been identified to be in the design of the SPAD and the quenching circuit. SPADs are sensitive devices which maximum reverse current must be well defined and limited by the quenching circuit, otherwise unwanted effects like excessive cross-talk, noise, and power consumption may happen. Although this issue limits the operation of the implemented pixel, the information obtained during the characterization will help to avoid mistakes in future implementations

    A novel fully depleted monolithic active CMOS microstrip sensor

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    L'abstract Ăš presente nell'allegato / the abstract is in the attachmen

    Smart cmos image sensor for 3d measurement

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    3D measurements are concerned with extracting visual information from the geometry of visible surfaces and interpreting the 3D coordinate data thus obtained, to detect or track the position or reconstruct the profile of an object, often in real time. These systems necessitate image sensors with high accuracy of position estimation and high frame rate of data processing for handling large volumes of data. A standard imager cannot address the requirements of fast image acquisition and processing, which are the two figures of merit for 3D measurements. Hence, dedicated VLSI imager architectures are indispensable for designing these high performance sensors. CMOS imaging technology provides potential to integrate image processing algorithms on the focal plane of the device, resulting in smart image sensors, capable of achieving better processing features in handling massive image data. The objective of this thesis is to present a new architecture of smart CMOS image sensor for real time 3D measurement using the sheet-beam projection methods based on active triangulation. Proposing the vision sensor as an ensemble of linear sensor arrays, all working in parallel and processing the entire image in slices, the complexity of the image-processing task shifts from O (N 2 ) to O (N). Inherent also in the design is the high level of parallelism to achieve massive parallel processing at high frame rate, required in 3D computation problems. This work demonstrates a prototype of the smart linear sensor incorporating full testability features to test and debug both at device and system levels. The salient features of this work are the asynchronous position to pulse stream conversion, multiple images binarization, high parallelism and modular architecture resulting in frame rate and sub-pixel resolution suitable for real time 3D measurements

    Electronics for Sensors

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    The aim of this Special Issue is to explore new advanced solutions in electronic systems and interfaces to be employed in sensors, describing best practices, implementations, and applications. The selected papers in particular concern photomultiplier tubes (PMTs) and silicon photomultipliers (SiPMs) interfaces and applications, techniques for monitoring radiation levels, electronics for biomedical applications, design and applications of time-to-digital converters, interfaces for image sensors, and general-purpose theory and topologies for electronic interfaces

    Feasibility of Geiger-mode avalanche photodiodes in CMOS standard technologies for tracker detectors

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    The next generation of particle colliders will be characterized by linear lepton colliders, where the collisions between electrons and positrons will allow to study in great detail the new particle discovered at CERN in 2012 (presumably the Higgs boson). At present time, there are two alternative projects underway, namely the ILC (International Linear Collider) and CLIC (Compact LInear Collider). From the detector point of view, the physics aims at these particle colliders impose such extreme requirements, that there is no sensor technology available in the market that can fulfill all of them. As a result, several new detector systems are being developed in parallel with the accelerator. This thesis presents the development of a GAPD (Geiger-mode Avalanche PhotoDiode) pixel detector aimed mostly at particle tracking at future linear colliders. GAPDs offer outstanding qualities to meet the challenging requirements of ILC and CLIC, such as an extraordinary high sensitivity, virtually infinite gain and ultra-fast response time, apart from compatibility with standard CMOS technologies. In particular, GAPD detectors enable the direct conversion of a single particle event onto a CMOS digital pulse in the sub-nanosecond time scale without the utilization of either preamplifiers or pulse shapers. As a result, GAPDs can be read out after each single bunch crossing, a unique quality that none of its competitors can offer at the moment. In spite of all these advantages, GAPD detectors suffer from two main problems. On the one side, there exist noise phenomena inherent to the sensor, which induce noise pulses that cannot be distinguished from real particle events and also worsen the detector occupancy to unacceptable levels. On the other side, the fill-factor is too low and gives rise to a reduced detection efficiency. Solutions to the two problems commented that are compliant with the severe specifications of the next generation of particle colliders have been thoroughly investigated. The design and characterization of several single pixels and small arrays that incorporate some elements to reduce the intrinsic noise generated by the sensor are presented. The sensors and the readout circuits have been monolithically integrated in a conventional HV-CMOS 0.35 ÎŒm process. Concerning the readout circuits, both voltage-mode and current-mode options have been considered. Moreover, the time-gated operation has also been explored as an alternative to reduce the detected sensor noise. The design and thorough characterization of a prototype GAPD array, also monolithically integrated in a conventional 0.35 ÎŒm HV-CMOS process, is presented in the thesis as well. The detector consists of 10 rows x 43 columns of pixels, with a total sensitive area of 1 mm x 1 mm. The array is operated in a time-gated mode and read out sequentially by rows. The efficiency of the proposed technique to reduce the detected noise is shown with a wide variety of measurements. Further improved results are obtained with the reduction of the working temperature. Finally, the suitability of the proposed detector array for particle detection is shown with the results of a beam-test campaign conducted at CERN-SPS (European Organization for Nuclear Research-Super Proton Synchrotron). Apart from that, a series of additional approaches to improve the performance of the GAPD technology are proposed. The benefits of integrating a GAPD pixel array in a 3D process in terms of overcoming the fill-factor limitation are examined first. The design of a GAPD detector in the Global Foundries 130 nm/Tezzaron 3D process is also presented. Moreover, the possibility to obtain better results in light detection applications by means of the time-gated operation or correction techniques is analyzed too.Aquesta tesi presenta el desenvolupament d’un detector de pĂ­xels de GAPDs (Geiger-mode Avalanche PhotoDiodes) dedicat principalment a rastrejar partĂ­cules en futurs col‱lisionadors lineals. Els GAPDs ofereixen unes qualitats extraordinĂ ries per satisfer els requisits extremadament exigents d’ILC (International Linear Collider) i CLIC (Compact LInear Collider), els dos projectes per la propera generaciĂł de col‱lisionadors que s’han proposat fins a dia d’avui. Entre aquestes qualitats es troben una sensibilitat extremadament elevada, un guany virtualment infinit i una resposta molt rĂ pida, a part de ser compatibles amb les tecnologies CMOS estĂ ndard. En concret, els detectors de GAPDs fan possible la conversiĂł directa d’un esdeveniment generat per una sola partĂ­cula en un senyal CMOS digital amb un temps inferior al nanosegon. Com a resultat d’aquest fet, els GAPDs poden ser llegits desprĂ©s de cada bunch crossing (la col‱lisiĂł de les partĂ­cules), una qualitat Ășnica que cap dels seus competidors pot oferir en el moment actual. Malgrat tots aquests avantatges, els detectors de GAPDs pateixen dos grans problemes. D’una banda, existeixen fenĂČmens de soroll inherents al sensor, els quals indueixen polsos de soroll que no poden ser distingits dels esdeveniments reals generats per partĂ­cules i que a mĂ©s empitjoren l’ocupaciĂł del detector a nivells inacceptables. D’altra banda, el fill-factor (Ă©s a dir, l’àrea sensible respecte l’àrea total) Ă©s molt baix i redueix l’eficiĂšncia detectora. En aquesta tesi s’han investigat solucions als dos problemes comentats i que a mĂ©s compleixen amb les especificacions altament severes dels futurs col‱lisionadors lineals. El detector de pĂ­xels de GAPDs, el qual ha estat monolĂ­ticament integrat en un procĂ©s HV-CMOS estĂ ndard de 0.35 ÎŒm, incorpora circuits de lectura en mode voltatge que permeten operar el sensor en l’anomenat mode time-gated per tal de reduir el soroll detectat. L’eficiĂšncia de la tĂšcnica proposada queda demostrada amb la gran varietat d’experiments que s’han dut a terme. Els resultats del beam-test dut a terme al CERN indiquen la capacitat del detector de pĂ­xels de GAPDs per detectar partĂ­cules altament energĂštiques. A banda d’aixĂČ, tambĂ© s’han estudiat els beneficis d’integrar un detector de pĂ­xels de GAPDs en un procĂ©s 3D per tal d’incrementar el fill-factor. L’anĂ lisi realitzat conclou que es poden assolir fill-factors superiors al 90%

    Ultra-low noise, high-frame rate readout design for a 3D-stacked CMOS image sensor

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    Due to the switch from CCD to CMOS technology, CMOS based image sensors have become smaller, cheaper, faster, and have recently outclassed CCDs in terms of image quality. Apart from the extensive set of applications requiring image sensors, the next technological breakthrough in imaging would be to consolidate and completely shift the conventional CMOS image sensor technology to the 3D-stacked technology. Stacking is recent and an innovative technology in the imaging field, allowing multiple silicon tiers with different functions to be stacked on top of each other. The technology allows for an extreme parallelism of the pixel readout circuitry. Furthermore, the readout is placed underneath the pixel array on a 3D-stacked image sensor, and the parallelism of the readout can remain constant at any spatial resolution of the sensors, allowing extreme low noise and a high-frame rate (design) at virtually any sensor array resolution. The objective of this work is the design of ultra-low noise readout circuits meant for 3D-stacked image sensors, structured with parallel readout circuitries. The readout circuit’s key requirements are low noise, speed, low-area (for higher parallelism), and low power. A CMOS imaging review is presented through a short historical background, followed by the description of the motivation, the research goals, and the work contributions. The fundamentals of CMOS image sensors are addressed, as a part of highlighting the typical image sensor features, the essential building blocks, types of operation, as well as their physical characteristics and their evaluation metrics. Following up on this, the document pays attention to the readout circuit’s noise theory and the column converters theory, to identify possible pitfalls to obtain sub-electron noise imagers. Lastly, the fabricated test CIS device performances are reported along with conjectures and conclusions, ending this thesis with the 3D-stacked subject issues and the future work. A part of the developed research work is located in the Appendices.Devido Ă  mudança da tecnologia CCD para CMOS, os sensores de imagem em CMOS tornam se mais pequenos, mais baratos, mais rĂĄpidos, e mais recentemente, ultrapassaram os sensores CCD no que respeita Ă  qualidade de imagem. Para alĂ©m do vasto conjunto de aplicaçÔes que requerem sensores de imagem, o prĂłximo salto tecnolĂłgico no ramo dos sensores de imagem Ă© o de mudar completamente da tecnologia de sensores de imagem CMOS convencional para a tecnologia “3D-stacked”. O empilhamento de chips Ă© relativamente recente e Ă© uma tecnologia inovadora no campo dos sensores de imagem, permitindo vĂĄrios planos de silĂ­cio com diferentes funçÔes poderem ser empilhados uns sobre os outros. Esta tecnologia permite portanto, um paralelismo extremo na leitura dos sinais vindos da matriz de pĂ­xeis. AlĂ©m disso, num sensor de imagem de planos de silĂ­cio empilhados, os circuitos de leitura estĂŁo posicionados debaixo da matriz de pĂ­xeis, sendo que dessa forma, o paralelismo pode manter-se constante para qualquer resolução espacial, permitindo assim atingir um extremo baixo ruĂ­do e um alto debito de imagens, virtualmente para qualquer resolução desejada. O objetivo deste trabalho Ă© o de desenhar circuitos de leitura de coluna de muito baixo ruĂ­do, planeados para serem empregues em sensores de imagem “3D-stacked” com estruturas altamente paralelizadas. Os requisitos chave para os circuitos de leitura sĂŁo de baixo ruĂ­do, rapidez e pouca ĂĄrea utilizada, de forma a obter-se o melhor rĂĄcio. Uma breve revisĂŁo histĂłrica dos sensores de imagem CMOS Ă© apresentada, seguida da motivação, dos objetivos e das contribuiçÔes feitas. Os fundamentos dos sensores de imagem CMOS sĂŁo tambĂ©m abordados para expor as suas caracterĂ­sticas, os blocos essenciais, os tipos de operação, assim como as suas caracterĂ­sticas fĂ­sicas e suas mĂ©tricas de avaliação. No seguimento disto, especial atenção Ă© dada Ă  teoria subjacente ao ruĂ­do inerente dos circuitos de leitura e dos conversores de coluna, servindo para identificar os possĂ­veis aspetos que dificultem atingir a tĂŁo desejada performance de muito baixo ruĂ­do. Por fim, os resultados experimentais do sensor desenvolvido sĂŁo apresentados junto com possĂ­veis conjeturas e respetivas conclusĂ”es, terminando o documento com o assunto de empilhamento vertical de camadas de silĂ­cio, junto com o possĂ­vel trabalho futuro
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