47 research outputs found
Scintillator Pad Detector: Very Front End Electronics
El Laboratori d'Altes Energies de La Salle és un membre d'un grup acreditat per la Generalitat. Aquest grup està format per part del Departament d'Estructura i Constituents de la Matèria de la Facultat de Física de la Universitat de Barcelona, part del departament d'Electrònica de la mateixa Facultat i pel grup de La Salle. Tots ells estan involucrats en el disseny d'un subdetector en l'experiment de LHCb del CERN: el SPD (Scintillator Pad Detector). El SPD és part del Calorímetre de LHCb. Aquest sistema proporciona possibles hadrons d'alta energia, electrons i fotons pel primer nivell de trigger. El SPD està format per una làmina centellejeadora de plàstic, dividida en 600 cel.les de diferent tamany per obtenir una millor granularitat aprop del feix. Les partícules carregades que travessin el centellejador generaran una ionització del mateix, a diferència dels fotons que no la ionitzaran. Aquesta ionització, generarà un pols de llum que serà recollit per una WLS que està enrotllada dins de les cel.les centellejadores. La llum serà transmesa al sistema de lectura mitjançant fibres clares. Per reducció de costos, aquestes 6000 cel.les estan dividides en grups, usant MAPMT (fotomultiplicadors multiànode) de 64 canals per rebre la informació en el sistema de lectura. El senyal de sortida dels fotomultilplicadors és irregular degut al baix nivell de fotoestadística, uns 20-30 fotoelectrons per MIP, i degut també a la resposta de la fibra WLS, que té un temps de baixada lent. Degut a tot això, el processat del senyal, es realitza primer durant la integració de la càrrega total i finalment per la correcció de la cua que conté el senyal provinent del PMT. Aquesta Tesi està enfocada en el sistema de lectura de l'electrònica del VFE del SPD. Aquest, està format per un ASIC (dissenyat pel grup de la UB) encarregat d'integrar el senyal, compensar el senyal restant i comparar el nivell d'energia obtingut amb un llindar programable (fa la distinció entre electrons i fotons), una FPGA que programa aquests llindars i compensacions de cada ASIC i fa el mapeig de cada canal rebut en el detector i finalment usa serialitzadors LVDS per enviar la informació de sortida al trigger de primer nivell. En el disseny d'aquest tipus d'electrònica s'haurà de tenir en compte, per un costat, restriccions de tipus mecànic: l'espai disponible per l'electrònica és limitat i escàs, i per un altre costat, el nivell de radiació que deurà suportar és considerable i s'haurà de comprobar que tots els components superin un cert test de radiació, i finalment, també s'haurà de tenir en compte la distància que separa els VFE dels racks on la informació és enviada i el tipus de senyal amb el que es treballa en aquest tipus d'experiments: mixta i de poc rang.El Laboratorio de Altas Energías de la Salle es un miembro de un grupo acreditado por La Generalitat. Este grupo está formado por parte del departamento de Estructura i Constituents de la Matèria de la Facultad de Física de la Universidad de Barcelona, parte del departamento de Electrónica de la misma Facultad y el grupo de La Salle. Todos ellos están involucrados en el diseño de un subdetector en el experimento de LHCb del CERN: El SPD (Scintillator Pad Detector). El SPD es parte del Calorímetro de LHCb. Este sistema proporciona posibles hadrones de alta energía, electrones y fotones para el primer nivel de trigger.El SPD está diseñado para distinguir entre electrones y fotones para el trigger de primer nivel. Este detector está formado por una lámina centelleadora de plástico, dividida en 6000 celdas de diferente tamaño para obtener una mejor granularidad cerca del haz. Las partículas cargadas que atraviesen el centelleador generarán una ionización del mismo, a diferencia de los fotones que no la generarán. Esta ionización generará, a su vez, un pulso de luz que será recogido por una WLS que está enrollada dentro de las celdas centelleadoras. La luz será transmitida al sistema de lectura mediante fibras claras. Para reducción de costes, estas 6000 celdas están divididas en grupos, utilizando un MAPMT (fotomultiplicadores multiánodo) de 64 canales para recibir la información en el sistema de lectura. La señal de salida de los fotomultiplicadores es irregular debido al bajo nivel de fotoestadística, unos 20-30 fotoelectrones por MIP, y debido también a la respuesta de la fibra WLS, que tiene un tiempo de bajada lento. Debido a todo esto, el procesado de la señal, se realiza primero mediante la integración de la carga total y finalmente por la substracción de la señal restante fuera del período de integración. Esta Tesis está enfocada en el sistema de lectura de la electrónica del VFE del SPD. Éste, está formado por un ASIC (diseñado por el grupo de la UB) encargado de integrar la señal, compensar la señal restante y comparar el nivel de energía obtenido con un umbral programable (que distingue entre electrones y fotones), y una FPGA que programa estos umbrales y compensaciones de cada ASIC, y mapea cada uno de los canales recibidos en el detector y finalmente usa serializadores LVDS para enviar la información de salida al trigger de primer nivel. En el diseño de este tipo de electrónica se deberá tener en cuenta, por un lado, restricciones del tipo mecánico: el espacio disponible para la electrónica en sí, es limitado y escaso, por otro lado, el nivel de radiación que deberá soportar es considerable y se tendrá que comprobar que todos los componentes usado superen un cierto test de radiación, y finalmente, también se deberá tener en cuenta la distancia que separa los VFE de los racks dónde la información es enviada y el tipo de señal con el que se trabaja en este tipo de experimentos: mixta y de poco rango.Laboratory in La Salle is a member of a Credited Research Group by La Generatitat. This group is formed by a part of the ECM department, a part of the Electronics department at UB (University of Barcelona) and La Salle's group. Together, they are involved in the design of a subdetector at LHCb Experiment at CERN: the SPD (Scintillator Pad Detector). The SPD is a part of LHCb Calorimeter. That system provides high energy hadrons, electron and photons candidates for the first level trigger. The SPD is designed to distinguish electrons and photons for this first level trigger. This detector is a plastic scintillator layer, divided in about 6000 cells of different size to obtain better granularity near the beam. Charged particles will produce, and photons will not, ionisation on the scintillator. This ionisation generates a light pulse that is collected by a Wavelength Shifting (WLS) fibre that is twisted inside the scintillator cell. The light is transmitted through a clear fibre to the readout system. For cost reduction, these 6000 cells are divided in groups using a MAPMT of 64 channels for receiving information in the readout system. The signal outing the SPD PMTs is rather unpredictable as a result of the low number of photostatistics, 20-30 photoelectrons per MIP, and the due to the response of the WLS fibre, which has low decay time. Then, the signal processing must be performed by first integrating the total charge and later subtracting to avoid pile-up. This PhD is focused on the VFE (Very Front End) of SPD Readout system. It is performed by a specific ASIC (designed by the UB group) which integrates the signal, makes the pile-up compensation, and compares the level obtained to a programmable threshold (distinguishing electrons and photons), an FPGA which programs the ASIC thresholds, pile-up subtraction and mapping the channels in the detector and finally LVDS serializers, in order to send information to the first level trigger system. Not only mechanical constraints had to be taken into account in the design of the card as a result of the little space for the readout electronics but also, on one hand, the radiation quote expected in the environment and on the other hand, the distance between the VFE electronics and the racks were information is sent and the signal range that this kind of experiments usually have
High-Density Digital Links: Optimization of Signal Integrity and Noise Performance of the High-Density Digital Links of the ATLAS-TRT Readout System
The Transition Radiation Tracker (TRT) is a sub detector of the particle detector ATLAS (A Toroidal LHC ApparatuS). About 420,000 detecting elements are distributed over 22 m3. They produce each second approximately 20 Tbit of data which has to be transferred from the front-end electronics inside the detector to the back-end electronics outside the detector for further processing. The task of this thesis is to guarantee the integrity of the signals and the electromagnetic compatibility inside the TRT as well as to the aggressive surroundings. The electromagnetic environment of particle detectors in high-energy physics adds special constraints to the high data rates and the high complexity: high sensibility of the detecting elements and their pre amplifiers, confined space, limited material budget, a radioactive environment, and high static magnetic fields. Thus many industrial standard measures have to be abandoned. Special design is essential to compensate this disadvantage
Modelling of interconnects including coaxial cables and multiconductor lines
In recent years, electromagnetic compatibility (EMC) problems associated with high frequency and high speed interconnects are becoming of increasing concern. Coaxial cables are a popular form of interconnect. In this thesis, the crosstalk coupling between two parallel coaxial cables in free space and above a ground plane is investigated. The degree of coupling is usually formulated analytically in the frequency domain. In this thesis, a method for time domain simulation is proposed using the TLM technique. Results are compared with frequency domain solutions and experimental results. Also; the standard model has been improved by including the skin depth effect in the coaxial cable braid.
The crosstalk between the two coaxial cables is observed through the induced voltages on the loads of the adjacent cable, which is deemed to be the usual measureable form of cable coupling. The equivalent circuit developed for the coupling path of two coaxial cables in free space takes account of the differential mode (DM) current travelling in the braids of the cables. As for the coupling path of the cables via a ground plane, the equivalent circuit is developed based on the flow of differential mode (DM) and common mode (CM) currents in the braid, where the coaxial braid’s transfer impedance is modelled using Kley’s model.
The radiated electric (E) field from the coaxial cable above a ground plane is also deduced from the predicted cable sheath current distribution and by the Hertzian dipoles’ approach. Results are validated against the radiated electric field of a single copper wire above ground. Both the simulated and experimental results are presented in the time and frequency domains and good agreement is observed thus validating the accuracy of the model
Modelling of interconnects including coaxial cables and multiconductor lines
In recent years, electromagnetic compatibility (EMC) problems associated with high frequency and high speed interconnects are becoming of increasing concern. Coaxial cables are a popular form of interconnect. In this thesis, the crosstalk coupling between two parallel coaxial cables in free space and above a ground plane is investigated. The degree of coupling is usually formulated analytically in the frequency domain. In this thesis, a method for time domain simulation is proposed using the TLM technique. Results are compared with frequency domain solutions and experimental results. Also; the standard model has been improved by including the skin depth effect in the coaxial cable braid.
The crosstalk between the two coaxial cables is observed through the induced voltages on the loads of the adjacent cable, which is deemed to be the usual measureable form of cable coupling. The equivalent circuit developed for the coupling path of two coaxial cables in free space takes account of the differential mode (DM) current travelling in the braids of the cables. As for the coupling path of the cables via a ground plane, the equivalent circuit is developed based on the flow of differential mode (DM) and common mode (CM) currents in the braid, where the coaxial braid’s transfer impedance is modelled using Kley’s model.
The radiated electric (E) field from the coaxial cable above a ground plane is also deduced from the predicted cable sheath current distribution and by the Hertzian dipoles’ approach. Results are validated against the radiated electric field of a single copper wire above ground. Both the simulated and experimental results are presented in the time and frequency domains and good agreement is observed thus validating the accuracy of the model
Superconducting integrated THz receiver
The operation frequency of superconducting integrated THz receivers can be enhanced by replacing the commonly used elementary niobium with niobium nitride. This work presents the technology development of high-quality niobium nitride thin films and superconductor-insulator-superconductor multilayers along with the simulation and realization of high-frequency circuits for a superconducting integrated THz receiver using niobium nitride electrodes
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On the Boundary Conditions and Internal Mechanics of Parallel Wire Strands
This dissertation analyzes the internal mechanics of parallel wire strands as found in the main cables of suspension bridges. Parallel wire strands of reduced order (7-wire, 19-wire, and 61-wire strands made of steel and aluminum) are fabricated and subjected to various boundary conditions and external loads (tension, clamping, twist, etc.). Neutron diffraction is used as an elastic strain measurement tool for its ability to penetrate bulk materials and/or layers of a multi-body system without disturbing the sample. Firstly, this thesis aims to quantify the development length – the distance over which a broken wire within a strand regains near-full service strain – as a function of various boundary conditions and failure scenarios. The feasibility of using neutron diffractometers to measure in situ elastic strains on civil-engineering-scale samples under both tensile load and radial confinement is validated using strands fabricated from steel bridge wire. Results from various 7-wire strands indicate that friction and mechanical interference on the microscopic level play a significant role in the load partitioning. Furthermore, wires that have been broken – either pre-cracked or fractured live and in situ during tensile loading – are capable of regaining significant stresses from their neighbors over a distance of tens of centimeters. The contribution of both friction force and mechanical interference on elastic strain redevelopment in broken wires should be included in analytical models designed to simulate failure processes. The second part of this thesis aims to measure the internal mechanics of larger parallel wire strands in response to various confinement (clamping) forces. 19 and 61 aluminum wire strands are fabricated and the internal strains of all constituent wires mapped in three orthogonal directions under various clamping loads. The strain distributions for both 19-wire and 61-wire strands show a surprising degree of heterogeneity. An increase in clamping force homogenizes the distribution to a degree, but only at unfeasibly high clamping forces. The results suggest that microscale variations in wire diameter dominate the internal mechanics of parallel wire strands. The stochastic distribution of wire sizes due to manufacturing tolerances throughout a strand cross-section creates a randomly ordered network of over- and under-sized wires. This imperfectly packed lattice results in large wire-to-wire variations in clamping constraint. The up-scaling in strand size from 19 to 61 wires increases the resolution of the experiment but does not reduce the heterogeneity of the strain distribution. Ergo, the assumption of perfect hexagonal packing in parallel wire strands is weak, and mean field distributions do not accurately describe the internal mechanics of such structures
Integrated Application of Active Controls (IAAC) technology to an advanced subsonic transport project. ACT/Control/Guidance System study. Volume 2: Appendices
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Engineering Metamaterials
A couple of decades have passed since the advent of electromagnetic metamaterials. Although the research on artificial microwave materials dates back to the middle of the 20th century, the most prominent development in the electromagnetics of artificial media has happened in the new millennium. In the last decade, the electromagnetics of one-, two-, and three-dimensional metamaterials acquired robust characterization and design tools. Novel fabrication techniques have been developed. Many exotic effects involving metamaterials and metasurfaces, which initially belonged in a scientist’s lab, are now well understood by practicing engineers. Therefore, it is the right time for the metamaterial concepts to become a designer’s tools of choice in the landscape of electronics, microwaves, and photonics. Answering such a demand, the book “Engineering Metamaterials” focuses on the theory and applications of electromagnetic metamaterials, metasurfaces, and metamaterial transmission lines as the building blocks of present-day and future electronic, photonic, and microwave devices
Mu2e Technical Design Report
The Mu2e experiment at Fermilab will search for charged lepton flavor
violation via the coherent conversion process mu- N --> e- N with a sensitivity
approximately four orders of magnitude better than the current world's best
limits for this process. The experiment's sensitivity offers discovery
potential over a wide array of new physics models and probes mass scales well
beyond the reach of the LHC. We describe herein the preliminary design of the
proposed Mu2e experiment. This document was created in partial fulfillment of
the requirements necessary to obtain DOE CD-2 approval.Comment: compressed file, 888 pages, 621 figures, 126 tables; full resolution
available at http://mu2e.fnal.gov; corrected typo in background summary,
Table 3.