Luminescence dosimetry with ceramic materials for application to radiological emergencies and other incidents.

The likelihood of the occurrence of radiological accidents which can induce significant health consequences to the members of the public has raised the importance of developing a personal radiation dosimetry system applicable to populations not monitored by dedicated dosemeters. Mobile phones are personal devices with high ubiquity and great potential for accident dosimetry applications. Alumina surface mount resistors (SMRs) are abundant in the printed circuit board of mobile phones and their potential as fortuitous dosemeters has been investigated using thermoluminescence (TL) and optically stimulated luminescence (OSL) techniques. The physical mechanism of the generation of luminescence of the alumina SMRs is, however, less known. The basic luminescence defects in SMRs were identified to be F-type centres and their emission process was shown to be temperature dependent and highly quenched at room temperature (RT). The trap environment of beta irradiated SMRs includes a series of closely spaced traps covering thermal depths between 0.9-1.4 eV; predicting an average lifetime for thermal fading at RT of ca 23 years. Trapped charges evicted by thermal or optical stimulation are likely to recombine at F-type centres and contribute to the luminescence response that is likely to be thermally assisted via the vibrational modes of the lattice. A phonon-assisted de-excitation of the trapped charge population could additionally be involved in the mechanism of athermal or anomalous fading. Based on the temperature dependence of the rate of fading, a model is presented for the anomalous fading observed where phonon-assisted and tunnelling effects alternate or operate simultaneously depending on the temperature of the material. A number of aspects related to the use of SMRs in dosimetry seem to benefit from the investigation of the physical processes, although for accurate dose reconstruction it is imperative to know the energy of the ionising radiation source and the position of the mobile phone relative to the direction of the source. For example, at low-energy exposures the dose may be over-estimated, not only due to the non-flat energy response of the alumina, but also due to the presence of several parts of the mobile phone which can increase the amount of energy deposited in alumina substrates due to backscatter effects. In addition, MCNP simulations indicated that for low-energy exposures, such as for 192Ir, differences of up to an order-of-magnitude between resistor and whole body dose are expected. Finally, to specify the most appropriate dose conversion coefficients that can be applied to estimate whole body dose from OSL / TL determinations, the knowledge of the exposure geometry is crucial

Instrumentation of CdZnTe detectors for measuring prompt gamma-rays emitted during particle therapy

Background: The irradiation of cancer patients with charged particles, mainly protons and carbon ions, has become an established method for the treatment of specific types of tumors. In comparison with the use of X-rays or gamma-rays, particle therapy has the advantage that the dose distribution in the patient can be precisely controlled. Tissue or organs lying near the tumor will be spared. A verification of the treatment plan with the actual dose deposition by means of a measurement can be done through range assessment of the particle beam. For this purpose, prompt gamma-rays are detected, which are emitted by the affected target volume during irradiation. Motivation: The detection of prompt gamma-rays is a task related to radiation detection and measurement. Nuclear applications in medicine can be found in particular for in vivo diagnosis. In that respect the spatially resolved measurement of gamma-rays is an essential technique for nuclear imaging, however, technical requirements of radiation measurement during particle therapy are much more challenging than those of classical applications. For this purpose, appropriate instruments beyond the state-of-the-art need to be developed and tested for detecting prompt gamma-rays. Hence the success of a method for range assessment of particle beams is largely determined by the implementation of electronics. In practice, this means that a suitable detector material with adapted readout electronics, signal and information processing, and data interface must be utilized to solve the challenges. Thus, the parameters of the system (e.g. segmentation, time or energy resolution) can be optimized depending on the method (e.g. slit camera, time-of-flight measurement or Compton camera). Regardless of the method, the detector system must have a high count rate capability and a large measuring range (>7 MeV). For a subsequent evaluation of a suitable method for imaging, the mentioned parameters may not be restricted by the electronics. Digital signal processing is predestined for multipurpose tasks, and, in terms of the demands made, the performance of such an implementation has to be determined. Materials and methods: In this study, the instrumentation of a detector system for prompt gamma-rays emitted during particle therapy is limited to the use of a cadmium zinc telluride (CdZnTe, CZT) semiconductor detector. The detector crystal is divided into an 8x8 pixel array by segmented electrodes. Analog and digital signal processing are exemplarily tested with this type of detector and aims for application of a Compton camera to range assessment. The electronics are implemented with commercial off-the-shelf (COTS) components. If applicable, functional units of the detector system were digitalized and implemented in a field-programmable gate array (FPGA). An efficient implementation of the algorithms in terms of timing and logic utilization is fundamental to the design of digital circuits. The measurement system is characterized with radioactive sources to determine the measurement dynamic range and resolution. Finally, the performance is examined in terms of the requirements of particle therapy with experiments at particle accelerators. Results: A detector system based on a CZT pixel detector has been developed and tested. Although the use of an application-specific integrated circuit is convenient, this approach was rejected because there was no circuit available which met the requirements. Instead, a multichannel, compact, and low-noise analog amplifier circuit with COTS components has been implemented. Finally, the 65 information channels of a detector are digitized, processed and visualized. An advanced digital signal processing transforms the traditional approaches of nuclear electronics in algorithms and digital filter structures for an FPGA. With regard to the characteristic signals (e.g. varying rise times, depth-dependent energy measurement) of a CZT pixel detector, it could be shown that digital pulse processing results in a very good energy resolution (~2% FWHM at 511 keV), as well as permits a time measurement in the range of some tens of nanoseconds. Furthermore, the experimental results have shown that the dynamic range of the detector system could be significantly improved compared to the existing prototype of the Compton camera (~10 keV..7 MeV). Even count rates of ~100 kcps in a high-energy beam could be ultimately processed with the CZT pixel detector. But this is merely a limit of the detector due to its volume, and not related to electronics. In addition, the versatility of digital signal processing has been demonstrated with other detector materials (e.g. CeBr3). With foresight on high data throughput in a distributed data acquisition from multiple detectors, a Gigabit Ethernet link has been implemented as data interface. Conclusions: To fully exploit the capabilities of a CZT pixel detector, a digital signal processing is absolutely necessary. A decisive advantage of the digital approach is the ease of use in a multichannel system. Thus with digitalization, a necessary step has been done to master the complexity of a Compton camera. Furthermore, the benchmark of technology shows that a CZT pixel detector withstands the requirements of measuring prompt gamma-rays during particle therapy. The previously used orthogonal strip detector must be replaced by the pixel detector in favor of increased efficiency and improved energy resolution. With the integration of the developed digital detector system into a Compton camera, it must be ultimately proven whether this method is applicable for range assessment in particle therapy. Even if another method is more convenient in a clinical environment due to practical considerations, the detector system of that method may benefit from the shown instrumentation of a digital signal processing system for nuclear applications.:1. Introduction 1.1. Aim of this work 2. Analog front-end electronics 2.1. State-of-the-art 2.2. Basic design considerations 2.2.1. CZT detector assembly 2.2.2. Electrical characteristics of a CZT pixel detector 2.2.3. High voltage biasing and grounding 2.2.4. Signal formation in CZT detectors 2.2.5. Readout concepts 2.2.6. Operational amplifier 2.3. Circuit design of a charge-sensitive amplifier 2.3.1. Circuit analysis 2.3.2. Charge-to-voltage transfer function 2.3.3. Input coupling of the CSA 2.3.4. Noise 2.4. Implementation and Test 2.5. Results 2.5.1. Test pulse input 2.5.2. Pixel detector 2.6. Conclusion 3. Digital signal processing 3.1. Unfolding-synthesis technique 3.2. Digital deconvolution 3.2.1. Prior work 3.2.2. Discrete-time inverse amplifier transfer function 3.2.3. Application to measured signals 3.2.4. Implementation of a higher order IIR filter 3.2.5. Conclusion 3.3. Digital pulse synthesis 3.3.1. Prior work 3.3.2. FIR filter structures for FPGAs 3.3.3. Optimized fixed-point arithmetic 3.3.4. Conclusion 4. Data interface 4.1. State-of-the-art 4.2. Embedded Gigabit Ethernet protocol stack 4.3. Implementation 4.3.1. System overview 4.3.2. Media Access Control 4.3.3. Embedded protocol stack 4.3.4. Clock synchronization 4.4. Measurements and results 4.4.1. Throughput performance 4.4.2. Synchronization 4.4.3. Resource utilization 4.5. Conclusion 5. Experimental results 5.1. Digital pulse shapers 5.1.1. Spectroscopy application 5.1.2. Timing applications 5.2. Gamma-ray spectroscopy 5.2.1. Energy resolution of scintillation detectors 5.2.2. Energy resolution of a CZT pixel detector 5.3. Gamma-ray timing 5.3.1. Timing performance of scintillation detectors 5.3.2. Timing performance of CZT pixel detectors 5.4. Measurements with a particle beam 5.4.1. Bremsstrahlung Facility at ELBE 6. Discussion 7. Summary 8. ZusammenfassungHintergrund: Die Bestrahlung von Krebspatienten mit geladenen Teilchen, vor allem Protonen oder Kohlenstoffionen, ist mittlerweile eine etablierte Methode zur Behandlung von speziellen Tumorarten. Im Vergleich mit der Anwendung von Röntgen- oder Gammastrahlen hat die Teilchentherapie den Vorteil, dass die Dosisverteilung im Patienten präziser gesteuert werden kann. Dadurch werden um den Tumor liegendes Gewebe oder Organe geschont. Die messtechnische Verifikation des Bestrahlungsplans mit der tatsächlichen Dosisdeposition kann über eine Reichweitenkontrolle des Teilchenstrahls erfolgen. Für diesen Zweck werden prompte Gammastrahlen detektiert, die während der Bestrahlung vom getroffenen Zielvolumen emittiert werden. Fragestellung: Die Detektion von prompten Gammastrahlen ist eine Aufgabenstellung der Strahlenmesstechnik. Strahlenanwendungen in der Medizintechnik finden sich insbesondere in der in-vivo Diagnostik. Dabei ist die räumlich aufgelöste Messung von Gammastrahlen bereits zentraler Bestandteil der nuklearmedizinischen Bildgebung, jedoch sind die technischen Anforderungen der Strahlendetektion während der Teilchentherapie im Vergleich mit klassischen Anwendungen weitaus anspruchsvoller. Über den Stand der Technik hinaus müssen für diesen Zweck geeignete Instrumente zur Erfassung der prompten Gammastrahlen entwickelt und erprobt werden. Die elektrotechnische Realisierung bestimmt maßgeblich den Erfolg eines Verfahrens zur Reichweitenkontrolle von Teilchenstrahlen. Konkret bedeutet dies, dass ein geeignetes Detektormaterial mit angepasster Ausleseelektronik, Signal- und Informationsverarbeitung sowie Datenschnittstelle zur Problemlösung eingesetzt werden muss. Damit können die Parameter des Systems (z. B. Segmentierung, Zeit- oder Energieauflösung) in Abhängigkeit der Methode (z.B. Schlitzkamera, Flugzeitmessung oder Compton-Kamera) optimiert werden. Unabhängig vom Verfahren muss das Detektorsystem eine hohe Ratenfestigkeit und einen großen Messbereich (>7 MeV) besitzen. Für die anschließende Evaluierung eines geeigneten Verfahrens zur Bildgebung dürfen die genannten Parameter durch die Elektronik nicht eingeschränkt werden. Eine digitale Signalverarbeitung ist für universelle Aufgaben prädestiniert und die Leistungsfähigkeit einer solchen Implementierung soll hinsichtlich der gestellten Anforderungen bestimmt werden. Material und Methode: Die Instrumentierung eines Detektorsystems für prompte Gammastrahlen beschränkt sich in dieser Arbeit auf die Anwendung eines Cadmiumzinktellurid (CdZnTe, CZT) Halbleiterdetektors. Der Detektorkristall ist durch segmentierte Elektroden in ein 8x8 Pixelarray geteilt. Die analoge und digitale Signalverarbeitung wird beispielhaft mit diesem Detektortyp erprobt und zielt auf die Anwendung zur Reichweitenkontrolle mit einer Compton-Kamera. Die Elektronik wird mit seriengefertigten integrierten Schaltkreisen umgesetzt. Soweit möglich, werden die Funktionseinheiten des Detektorsystems digitalisiert und in einem field-programmable gate array (FPGA) implementiert. Eine effiziente Umsetzung der Algorithmen in Bezug auf Zeitverhalten und Logikverbrauch ist grundlegend für den Entwurf der digitalen Schaltungen. Das Messsystem wird mit radioaktiven Prüfstrahlern hinsichtlich Messbereichsdynamik und Auflösung charakterisiert. Schließlich wird die Leistungsfähigkeit hinsichtlich der Anforderungen der Teilchentherapie mit Experimenten am Teilchenbeschleuniger untersucht. Ergebnisse: Es wurde ein Detektorsystem auf Basis von CZT Pixeldetektoren entwickelt und erprobt. Obwohl der Einsatz einer anwendungsspezifischen integrierten Schaltung zweckmäßig wäre, wurde dieser Ansatz zurückgewiesen, da kein verfügbarer Schaltkreis die Anforderungen erfüllte. Stattdessen wurde eine vielkanalige, kompakte und rauscharme analoge Verstärkerschaltung mit seriengefertigten integrierten Schaltkreisen aufgebaut. Letztendlich werden die 65 Informationskanäle eines Detektors digitalisiert, verarbeitet und visualisiert. Eine fortschrittliche digitale Signalverarbeitung überführt die traditionellen Ansätze der Nuklearelektronik in Algorithmen und digitale Filterstrukturen für einen FPGA. Es konnte gezeigt werden, dass die digitale Pulsverarbeitung in Bezug auf die charakteristischen Signale (u.a. variierende Anstiegszeiten, tiefenabhängige Energiemessung) eines CZT Pixeldetektors eine sehr gute Energieauflösung (~2% FWHM at 511 keV) sowie eine Zeitmessung im Bereich von einigen 10 ns ermöglicht. Weiterhin haben die experimentellen Ergebnisse gezeigt, dass der Dynamikbereich des Detektorsystems im Vergleich zum bestehenden Prototyp der Compton-Kamera deutlich verbessert werden konnte (~10 keV..7 MeV). Nach allem konnten auch Zählraten von >100 kcps in einem hochenergetischen Strahl mit dem CZT Pixeldetektor verarbeitet werden. Dies stellt aber lediglich eine Begrenzung des Detektors aufgrund seines Volumens, nicht jedoch der Elektronik, dar. Zudem wurde die Vielseitigkeit der digitalen Signalverarbeitung auch mit anderen Detektormaterialen (u.a. CeBr3) demonstriert. Mit Voraussicht auf einen hohen Datendurchsatz in einer verteilten Datenerfassung von mehreren Detektoren, wurde als Datenschnittstelle eine Gigabit Ethernet Verbindung implementiert. Schlussfolgerung: Um die Leistungsfähigkeit eines CZT Pixeldetektors vollständig auszunutzen, ist eine digitale Signalverarbeitung zwingend notwendig. Ein entscheidender Vorteil des digitalen Ansatzes ist die einfache Handhabbarkeit in einem vielkanaligen System. Mit der Digitalisierung wurde ein notwendiger Schritt getan, um die Komplexität einer Compton-Kamera beherrschbar zu machen. Weiterhin zeigt die Technologiebewertung, dass ein CZT Pixeldetektor den Anforderungen der Teilchentherapie für die Messung prompter Gammastrahlen stand hält. Der bisher eingesetzte Streifendetektor muss zugunsten einer gesteigerten Effizienz und verbesserter Energieauflösung durch den Pixeldetektor ersetzt werden. Mit der Integration des entwickelten digitalen Detektorsystems in eine Compton-Kamera muss abschließend geprüft werden, ob dieses Verfahren für die Reichweitenkontrolle in der Teilchentherapie anwendbar ist. Auch wenn sich herausstellt, dass ein anderes Verfahren unter klinischen Bedingungen praktikabler ist, so kann auch dieses Detektorsystem von der gezeigten Instrumentierung eines digitalen Signalverarbeitungssystems profitieren.:1. Introduction 1.1. Aim of this work 2. Analog front-end electronics 2.1. State-of-the-art 2.2. Basic design considerations 2.2.1. CZT detector assembly 2.2.2. Electrical characteristics of a CZT pixel detector 2.2.3. High voltage biasing and grounding 2.2.4. Signal formation in CZT detectors 2.2.5. Readout concepts 2.2.6. Operational amplifier 2.3. Circuit design of a charge-sensitive amplifier 2.3.1. Circuit analysis 2.3.2. Charge-to-voltage transfer function 2.3.3. Input coupling of the CSA 2.3.4. Noise 2.4. Implementation and Test 2.5. Results 2.5.1. Test pulse input 2.5.2. Pixel detector 2.6. Conclusion 3. Digital signal processing 3.1. Unfolding-synthesis technique 3.2. Digital deconvolution 3.2.1. Prior work 3.2.2. Discrete-time inverse amplifier transfer function 3.2.3. Application to measured signals 3.2.4. Implementation of a higher order IIR filter 3.2.5. Conclusion 3.3. Digital pulse synthesis 3.3.1. Prior work 3.3.2. FIR filter structures for FPGAs 3.3.3. Optimized fixed-point arithmetic 3.3.4. Conclusion 4. Data interface 4.1. State-of-the-art 4.2. Embedded Gigabit Ethernet protocol stack 4.3. Implementation 4.3.1. System overview 4.3.2. Media Access Control 4.3.3. Embedded protocol stack 4.3.4. Clock synchronization 4.4. Measurements and results 4.4.1. Throughput performance 4.4.2. Synchronization 4.4.3. Resource utilization 4.5. Conclusion 5. Experimental results 5.1. Digital pulse shapers 5.1.1. Spectroscopy application 5.1.2. Timing applications 5.2. Gamma-ray spectroscopy 5.2.1. Energy resolution of scintillation detectors 5.2.2. Energy resolution of a CZT pixel detector 5.3. Gamma-ray timing 5.3.1. Timing performance of scintillation detectors 5.3.2. Timing performance of CZT pixel detectors 5.4. Measurements with a particle beam 5.4.1. Bremsstrahlung Facility at ELBE 6. Discussion 7. Summary 8. Zusammenfassun

Technical Design Report for the PANDA Micro Vertex Detector

This document illustrates the technical layout and the expected performance of the Micro Vertex Detector (MVD) of the PANDA experiment. The MVD will detect charged particles as close as possible to the interaction zone. Design criteria and the optimisation process as well as the technical solutions chosen are discussed and the results of this process are subjected to extensive Monte Carlo physics studies. The route towards realisation of the detector is outlined

Pixellated radiation detectors for scientific applications

The work in this thesis is focused on characterisation and evaluation of two classes of science grade imaging radiation detectors. The first class is Monolithic Active Pixel Sensors (MAPS). The advances in CMOS fabrication technologies over the last four decades allowed MAPS to compete with Charge-Coupled Devices (CCD) in many applications. The technology also provides relatively inexpensive ways to tailor design to suit specific application needs. It is important to understand performance capabilities of new sensor designs through characterisation and optimisation of readout parameters. In this work three MAPSs were characterised. The first one - HEPAPS4 - designed for charged particle detection, with the potential technology application in the vertex detector for the International Linear Collider. The noise of the sensor was measured to be 35±5 e, which agrees well with simulated data. The dark current was found to be 175 pA/cm2. The SNR performance for minimum ionising particles detection was demonstrated to be 40. The sensor was also evaluated for indirect detection of thermal and fast neutrons using lithium and polyethylene converters. The technology performed well in such an application with an estimated fast neutron detection efficiency of ~0.01%. The second sensor characterised – Vanilla MAPS – was designed to evaluate new techniques for fast readout, small noise and reduced image lag. The system was capable to readout 150 full frames (520x520 pixels) per second; the sensor showed 14±4 e noise and decreased image lag. The dark current was found to be ~50 pA/cm2. The back-thinned version of the sensor demonstrated dramatic improvement in quantum efficiency from 0% to 20% at 220 nm. The third device is parametric sensor eLeNA. It features 14 test structure designed to evaluated noise reduction architectures. The most promising structures showed temporal noise values as low as 6 e and 20 e fixed pattern noise. Medipix as an example of the second class of imaging detectors - hybrid pixel detectors - was evaluated in two applications. It was used as the core element of the ATLAS radiation background monitoring system. The sensors were covered with neutron converters, which extended the number of radiation types that can be detected. X-ray calibration was performed, showing excellent tolerance of all 18 devices characterised. Detection efficiencies were estimated to be ~1% for thermal and ~0.1% for fast neutrons. The second application of Medipix was mass spectrometry. The detector was place in the focal plane of a prototype mass spectrometer. 2D representation of data allowed focusing correction of the ion beam. The system was capable to detect ions in the range of 5-25 keV. The detector characterisation with broad range of ions (from Cu to Pb) showed very good abundance agreement with table data

Submicron to Nanocrystalline α-Al2O3:Mn as a Promising Red-Emitting Luminescence Phosphor Candidate

This thesis aims to provide a detailed understanding of the storage properties of the α-Al2O3:Mn powder, encompassing various techniques, including photoluminescence (PL), thermoluminescence (TL), persistent luminescence (PersL), and spectral hole-burning. The α-Al2O3:Mn³⁺ sample was prepared via an exothermic combustion reaction method at 600 °C. The structural properties and elemental composition of the powder were investigated by X-ray powder diffraction (XRD), scanning electron microscopy (SEM), transmission electron microscopy (TEM), and X-ray fluorescence (XRF). We explored the generation of Mn4+ in α-Al2O3:Mn³⁺ by soft X-ray (8 keV) exposure, focusing on its potential application in multilevel optical data storage. The small diffraction limit of the X-rays enables the implementation of an exceptionally fine pitch during the writing step. The results showed that ~100 levels can be read out, corresponding to 6-7 bits per data point encoding. The stored information (Mn⁴⁺) can be read out via the R-lines (²E → ⁴A₂) under ∼470 nm (⁴A₂ → ⁴T₂), or ∼630 nm (⁴A₂ → ²T₁) excitation. The data could be erased via exposure to blue light. We demonstrated the persistent luminescence properties of α-Al2O3:Mn⁴⁺, Mg²⁺ powder samples. We discussed factors that influence the efficiency of persistent luminescence, including dopant concentrations, temperatures, and trap levels. We also delved into the underlying principles of the persistent luminescence mechanism and studied the trap levels by analyzing the samples’ thermoluminescence glow curve. The photochemical persistent hole-burning properties in the R1 line transition were investigated in α-Al2O3:Mn³⁺ and α-Al2O3:Mn⁴⁺, Mg²⁺ powder samples. The hole-burning properties of Mn4+ ions burned via the R1 and R2 lines were measured either via the photoluminescence excitation mode by monitoring the luminescence of a vibrational sideband at ~694 nm, or in luminescence, with blue light excitation after burning. The hole widths were studied as a function of burn fluence and temperature, ranging from 2 to 90 K. We conducted an investigation into the luminescence properties of Mn4+ ions by introducing Gd3+ as co-dopants. We also performed Zeeman studies on a macroscopic crystal of Al2O3:Mn4⁺, Mg2+. Overall, this study provides an overview of the storage properties of α-Al2O3:Mn phosphors, providing valuable insights into their fundamental characteristics and practical applications

Characterization of Seamless CdTe Photon Counting X-Ray Detector

Spectrally selective X-ray imaging provides improved material and tissue discrimination in comparison with the state-of-the-art dual energy technologies that are commonly used in medical, industrial, and security applications. Cadmium telluride (CdTe)- and cadmium zinc telluride (CdZnTe)-based line scanners and small size two-dimensional X-ray sensors are emerging to the market, but the need for large-scale panels is axiomatic. In this study, a seamless CdTe tile was developed that enables the implementation of large-sized, energy selective X-ray detector panels. The developed tile consists of a 64 x 64 pixel array (with 150 mu m pitch) with a necessary substrate, ASIC, and CdTe crystal. The performance of the constructed seamless tile was characterized by focusing on spectral resolution and stability. In addition, a simple pixel trimming method that automates the equalization of each energy selective pixel was developed and analyzed. The obtained results suggest that the proposed concept of seamless (tileable) detector structures is a feasible approach to scale up panel sizes. The seamless tile shows comparable spectral resolution and stability performance with commercial CdTe sensors. The effect of tile to tile variation, the realization of a large-scale panel, as well as the charge sharing performance were left out of the scope and are to be studied in the next phase.Peer reviewe

Characterization of Seamless CdTe Photon Counting X-Ray Detector

Spectrally selective X-ray imaging provides improved material and tissue discrimination in comparison with the state-of-the-art dual energy technologies that are commonly used in medical, industrial, and security applications. Cadmium telluride (CdTe)- and cadmium zinc telluride (CdZnTe)-based line scanners and small size two-dimensional X-ray sensors are emerging to the market, but the need for large-scale panels is axiomatic. In this study, a seamless CdTe tile was developed that enables the implementation of large-sized, energy selective X-ray detector panels. The developed tile consists of a 64 x 64 pixel array (with 150 mu m pitch) with a necessary substrate, ASIC, and CdTe crystal. The performance of the constructed seamless tile was characterized by focusing on spectral resolution and stability. In addition, a simple pixel trimming method that automates the equalization of each energy selective pixel was developed and analyzed. The obtained results suggest that the proposed concept of seamless (tileable) detector structures is a feasible approach to scale up panel sizes. The seamless tile shows comparable spectral resolution and stability performance with commercial CdTe sensors. The effect of tile to tile variation, the realization of a large-scale panel, as well as the charge sharing performance were left out of the scope and are to be studied in the next phase.Peer reviewe

Electronics for Sensors

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

Belle II Technical Design Report

The Belle detector at the KEKB electron-positron collider has collected almost 1 billion Y(4S) events in its decade of operation. Super-KEKB, an upgrade of KEKB is under construction, to increase the luminosity by two orders of magnitude during a three-year shutdown, with an ultimate goal of 8E35 /cm^2 /s luminosity. To exploit the increased luminosity, an upgrade of the Belle detector has been proposed. A new international collaboration Belle-II, is being formed. The Technical Design Report presents physics motivation, basic methods of the accelerator upgrade, as well as key improvements of the detector.Comment: Edited by: Z. Dole\v{z}al and S. Un