Performance comparison of large-area SiPM arrays suitable for gamma ray detectors

[EN] The use of photosensors of the type Silicon Photomultpliers (SiPM) has widely been extended in recent years for multiple applications in both research and industry. However, there is a lack of comparative studies of different SiPMs under the same conditions, making it difficult to choose the most appropriate one for a specific application. SiPM arrays are suitable for gamma rays detectors, especially when covering large active areas. They are used either in clinical or pre-clinical scenarios, constituting Single-Photon Emission Computed Tomography (SPECT) and Positron Emission Tomography (PET) scanners, or just gamma cameras. The current work presents, for the first time, a comparative study between SensL, Hamamatsu Photonics and KETEK arrays of 12 x 12 SiPMs, with individual active areas of 3 mm x 3 mm, thus covering a total active area of about 5 cm x 5 cm. In this study, we have first evaluated their bias and temperature dependencies, resulting in a very similar behaviour with just a slightly larger dependency of the tested Hamamatsu parts. We also report the performance of detector blocks based on these three SiPM arrays, when coupled to pixelated crystal arrays and monolithic scintillators, in terms of photon impact estimation accuracy, as well as energy resolution. In the case of the monolithic crystals, also the depth of interaction resolution was determined. Both monolithic and pixelated blocks are nowadays widely used in academia or are commercially available for molecular imaging systems. The results obtained for the three SiPM arrays when using those crystals, are comparable, without observing any significant different among them.This project has received funding from the European Research Council (ERC) under the European Union's Horizon 2020 research and innovation program (grant agreement No 695536). It has also been supported by the Spanish Ministerio de Economia, Industria y Competitividad under Grant TEC2016-79884-C2-1-R.Gonzalez-Montoro, A.; González Martínez, AJ. (2019). Performance comparison of large-area SiPM arrays suitable for gamma ray detectors. Biomedical Physics & Engineering Express. 5(4):1-10. https://doi.org/10.1088/2057-1976/ab0f6eS11054Henseler, D., Grazioso, R., Nan Zhang, & Schmand, M. (2009). SiPM performance in PET applications: An experimental and theoretical analysis. 2009 IEEE Nuclear Science Symposium Conference Record (NSS/MIC). doi:10.1109/nssmic.2009.5402157Buzhan, P., Dolgoshein, B., Filatov, L., Ilyin, A., Kantzerov, V., Kaplin, V., … Smirnov, S. (2003). Silicon photomultiplier and its possible applications. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 504(1-3), 48-52. doi:10.1016/s0168-9002(03)00749-6Dolgoshein, B., Balagura, V., Buzhan, P., Danilov, M., Filatov, L., Garutti, E., … Tikhomirov, I. (2006). Status report on silicon photomultiplier development and its applications. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 563(2), 368-376. doi:10.1016/j.nima.2006.02.193Berard, P., Couture, M., Deschamps, P., Laforce, F., & Dautet, H. (2011). Performance measurement for a new low dark count UV-SiPM. 2011 IEEE Nuclear Science Symposium Conference Record. doi:10.1109/nssmic.2011.6154109Moliner, L., González, A. J., Soriano, A., Sánchez, F., Correcher, C., Orero, A., … Benlloch, J. M. (2012). Design and evaluation of the MAMMI dedicated breast PET. Medical Physics, 39(9), 5393-5404. doi:10.1118/1.4742850Gonzalez, A. J., Aguilar, A., Conde, P., Hernandez, L., Moliner, L., Vidal, L. F., … Benlloch, J. M. (2016). A PET Design Based on SiPM and Monolithic LYSO Crystals: Performance Evaluation. IEEE Transactions on Nuclear Science, 63(5), 2471-2477. doi:10.1109/tns.2016.2522179Gonzalez-Montoro, A., Benlloch, J. M., Gonzalez, A. J., Aguilar, A., Canizares, G., Conde, P., … Sanchez, F. (2017). Performance Study of a Large Monolithic LYSO PET Detector With Accurate Photon DOI Using Retroreflector Layers. IEEE Transactions on Radiation and Plasma Medical Sciences, 1(3), 229-237. doi:10.1109/trpms.2017.2692819González-Montoro, A., Sánchez, F., Martí, R., Hernández, L., Aguilar, A., Barberá, J., … González, A. J. (2018). Detector block performance based on a monolithic LYSO crystal using a novel signal multiplexing method. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 912, 372-377. doi:10.1016/j.nima.2017.10.098Ronzhin, A., Albrow, M., Los, S., Martens, M., Murat, P., Ramberg, E., … Ritt, S. (2013). A SiPM-based TOF-PET detector with high speed digital DRS4 readout. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 703, 109-113. doi:10.1016/j.nima.2012.11.043Kim, C., McDaniel, D., Malaney, J., McBroom, G., Peterson, W., Tran, V. H., … Ganin, A. (2012). Time-of-flight PET-MR detector development with silicon photomultiplier. 2012 IEEE Nuclear Science Symposium and Medical Imaging Conference Record (NSS/MIC). doi:10.1109/nssmic.2012.6551808Schaart, D. R., van Dam, H. T., Seifert, S., Vinke, R., Dendooven, P., Löhner, H., & Beekman, F. J. (2009). A novel, SiPM-array-based, monolithic scintillator detector for PET. Physics in Medicine and Biology, 54(11), 3501-3512. doi:10.1088/0031-9155/54/11/01

Quantum interference in the dielectronic recombination of heavy highly charged ions

Die Photorekombination hochgeladener Quecksilberionen wurde mittels einer Elektronenstrahlionenfalle (electron beam ion trap) experimentell untersucht. Ein Elektronenstrahl variabler Energie überstrich den Bereich 45-54 keV, in dem die KLL Resonanzen der Hg75+...78+ -Ionen liegen. Zum Nachweis der Photorekombination diente die dabei erzeugte Strahlung. Dies ermöglichte es, die Anregungsenergien dieser Resonanzen zustandsselektiv mit Messfehlern kleiner als ± 5 eV zu bestimmen. Diese Genauigkeit gestattete es zum ersten Mal, zwischen verschiedenen ab initio Berechnungen für eine Anzahl von Konfigurationen zu unterscheiden, wobei sich einige signifikante Abweichungen zeigten. QED-Beiträge und Kerngrösseneffekte von jeweils in etwa 160 eV und 50 eV mussten dabei berücksichtigt werden. Die hohe experimentelle Auflösung erlaubte es zudem, bei einzelnen, zustandsselektierten Resonanzen die Linienprofile genau aufzuzeichnen. Diese wiesen eindeutig durch Quanteninterferenz zwischen radiativer und dielektronischer Rekombination verursachte Asymmetrien auf. Zum ersten Mal konnte so bei hochgeladenen Ionen die diese Asymmetrie charakterisierenden Fano-Parameter mit Messfehlern von nur 6% bestimmt werden

Desempleo juvenil profesional en el sistema neoliberal San Isidro-Matagalpa 2016

El presente documento aborda los factores que inciden en el desempleo juvenil profesional en el sistema neoliberal; según la Organización Internacional del Trabajo (OIT), se estima que alrededor de 66 millones de mujeres y hombres jóvenes en el mundo estaban desempleados. Esto significaba que los jóvenes, que representaban casi un 41 por ciento de la cifra mundial de 160 millones de personas, estaban clasificadas como desempleadas (que declaran estar sin trabajo, buscando trabajo y/o dispuestos a trabajar)”. (Market.OIT, 2001). Nos enfocamos en San Isidro, Matagalpa en el periodo 2016; la muestra se hizo de forma intencional, se tomaron quince personas profesionales que estuvieran desempleados o ejerciendo otro oficio, los instrumentos aplicados fueron la escala Likert y entrevista, que eran las propicias para obtener resultados según los objetivos

Desarrollo de un equipo didáctico para prácticas en asignaturas de control e identificación

En este artículo se presentan los detalles de un equipo didáctico desarrollado por los autores bajo las especificaciones dadas por los profesores del departamento DISA de la UPCT. Se ha tratado de crear un equipo que permita realizar el más amplio abanico de prácticas en las asignaturas de regulación y control de sistemas de este departamento. Además se hizo un esfuerzo especial en conseguir un equipo sencillo de manejo, robusto, fiable, seguro, versátil y de arquitectura abierta, características que a nuestro entender hay que cumplir para conseguir un buen equipo didáctico. En este articulo se muestran los detalles constructivos así como sus posibilidades como equipo de prácticas en las asignaturas de automática.Los autores desean mostrar su agradecimiento al Departamento de Ingeniería de Sistemas y Automática de la UPCT por su apoyo y apuesta por una iniciativa de este tipo

Herramienta para la implantación hardware de controladores sobre FPGAs

Barcelona, 12-14 de septiembre de 2001Deseamos agradecerle al departamento de electrónica, tecnología de computadoras y proyectos su apoyo técnico en la realización de este proyecto. Además deseamos agradecer al CEDETEL su apoyo económico

Organ-Dedicated Molecular Imaging Systems

[EN] In this review, we will cover both clinical and technical aspects of the advantages and disadvantages of organ specific (dedicated) molecular imaging (MI) systems, namely positron emission tomography (PET) and single photon emission computed tomography, including gamma cameras. This review will start with the introduction to the organ-dedicated MI systems. Thereafter, we will describe the differences and their advantages/disadvantages when compared with the standard large size scanners. We will review time evolution of dedicated systems, from first attempts to current scanners, and the ones that ended in clinical use. We will review later the state of the art of these systems for different organs, namely: breast, brain, heart, and prostate. We will also present the advantages offered by these systems as a function of the special application or field, such as in surgery, therapy assistance and assessment, etc. Their technological evolution will be introduced for each organ-based imager. Some of the advantages of dedicated devices are: higher sensitivity by placing the detectors closer to the organ, improved spatial resolution, better image contrast recovery (by reducing the noise from other organs), and also lower cost. Designing a complete ring-shaped dedicated PET scanner is sometimes difficult and limited angle tomography systems are preferable as they have more flexibility in placing the detectors around the body/organ. Examples of these geometries will be presented for breast, prostate and heart imaging. Recently achievable excellent time of flight capabilities below 300-ps full width at half of the maximum reduce significantly the impact of missing angles on the reconstructed images.This work was supported in part by the European Research Council through the European Union's Horizon 2020 Research and Innovation Program under Grant 695536, in part by the EU through the FP7 Program under Grant 603002, and in part by the Spanish Ministerio de Economia, Industria y Competitividad through PROSPET (DTS15/00152) funded by the Ministerio de Economia y Competitividad under Grant TEC2016-79884-C2-1-R.González Martínez, AJ.; Sánchez, F.; Benlloch Baviera, JM. (2018). Organ-Dedicated Molecular Imaging Systems. IEEE Transactions on Radiation and Plasma Medical Sciences. 2(5):388-403. https://doi.org/10.1109/TRPMS.2018.2846745S3884032

In-depth evaluation of TOF-PET detectors based on crystal arrays and the TOFPET2 ASIC

[EN] In recent years high efforts have been devoted to enhance spatial and temporal resolutions of PET detectors. However, accurately combining these two main features is, in most of the cases, challenging. Typically, a compromise has to be made between the number of readout channels, scintillator type and size, and photosensors arrangement if aiming for a good system performance, while keeping a moderate cost. In this work, we have studied several detector configurations for PET based on a set of 8x8 Silicon Photomultiplier (SiPMs) of 3x3 mm(2) active area, and LYSO crystal arrays with different pixel sizes. An exhaustive evaluation in terms of spatial, energy and timing resolution was made for all detector configurations. In some cases, when using pixel sizes different than SiPM active area, a significant amount of scintillation light may spread among several SiPMs. Therefore, we made use of a calibration method considering the different SiPM timing contributions. Best Detector Time Resolution (DTR) of 156 ps FWHM was measured when using 3x3 mm(2) crystal pixels directly coupled to the 3x3 mm(2) SiPMs. However, when using 1.5 mm crystal pixels with the same photosensor array, although we could clearly resolve all crystal pixels, an average DTR of 250 ps FWHM was achieved. We also shed light in this work on the timing dependency of the crystal pixel and photosensor alignment.This project has received funding from the European Research Council (ERC) under the European Union's Horizon 2020 research and innovation program (grant agreement No. 695536) and by the Spanish Ministerio de Economia, Industria y Competitividad under Grant TEC2016-79884-C2-1-R. The first author has also been supported by Generalitat Valenciana, Spain under grant agreement GRISOLIAP-2018-026.Lamprou, E.; Sánchez Martínez, F.; Benlloch Baviera, JM.; González Martínez, AJ. (2020). In-depth evaluation of TOF-PET detectors based on crystal arrays and the TOFPET2 ASIC. Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment. 977:1-8. https://doi.org/10.1016/j.nima.2020.164295S18977Jones, T., & Townsend, D. (2017). History and future technical innovation in positron emission tomography. Journal of Medical Imaging, 4(1), 011013. doi:10.1117/1.jmi.4.1.011013Surti, S. (2014). Update on Time-of-Flight PET Imaging. Journal of Nuclear Medicine, 56(1), 98-105. doi:10.2967/jnumed.114.145029Lecoq, P. (2017). Pushing the Limits in Time-of-Flight PET Imaging. IEEE Transactions on Radiation and Plasma Medical Sciences, 1(6), 473-485. doi:10.1109/trpms.2017.2756674Surti, S., & Karp, J. S. (2016). Advances in time-of-flight PET. Physica Medica, 32(1), 12-22. doi:10.1016/j.ejmp.2015.12.007Gundacker, S., Auffray, E., Pauwels, K., & Lecoq, P. (2016). Measurement of intrinsic rise times for various L(Y)SO and LuAG scintillators with a general study of prompt photons to achieve 10 ps in TOF-PET. Physics in Medicine and Biology, 61(7), 2802-2837. doi:10.1088/0031-9155/61/7/2802González-Montoro, A., Sánchez, F., Bruyndonckx, P., Cañizares, G., Benlloch, J. M., & González, A. J. (2019). Novel method to measure the intrinsic spatial resolution in PET detectors based on monolithic crystals. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 920, 58-67. doi:10.1016/j.nima.2018.12.056Moses, W. W. (2011). Fundamental limits of spatial resolution in PET. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 648, S236-S240. doi:10.1016/j.nima.2010.11.092Lamprou, E., Gonzalez, A. J., Sanchez, F., & Benlloch, J. M. (2020). Exploring TOF capabilities of PET detector blocks based on large monolithic crystals and analog SiPMs. Physica Medica, 70, 10-18. doi:10.1016/j.ejmp.2019.12.004Lamprou, E., Aguilar, A., González-Montoro, A., Monzó, J. M., Cañizares, G., Iranzo, S., … Benlloch, J. M. (2018). PET detector block with accurate 4D capabilities. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 912, 132-136. doi:10.1016/j.nima.2017.11.002A. Di Francesco, R. Bugalho, L. Oliveira, L. Pacher, A. Rivetti, M. Rolo, et al. TOFPET2: A high-performance ASIC for time and amplitude measurements of SiPM signals in time-of-flight applications, J. Instrum. 11 (03) C03042.Van Dam, H. T., Borghi, G., Seifert, S., & Schaart, D. R. (2013). Sub-200 ps CRT in monolithic scintillator PET detectors using digital SiPM arrays and maximum likelihood interaction time estimation. Physics in Medicine and Biology, 58(10), 3243-3257. doi:10.1088/0031-9155/58/10/3243V. Nadig, D. Schug, B. Weissler, V. Schulz, Evaluation Of The PETsys TOFPET2 ASIC In Multi-Channel Coincidence Experiments, arXiv:1911.08156.Gundacker, S., Turtos, R. M., Auffray, E., Paganoni, M., & Lecoq, P. (2019). High-frequency SiPM readout advances measured coincidence time resolution limits in TOF-PET. Physics in Medicine & Biology, 64(5), 055012. doi:10.1088/1361-6560/aafd52Gundacker, S., Acerbi, F., Auffray, E., Ferri, A., Gola, A., Nemallapudi, M. V., … Lecoq, P. (2016). State of the art timing in TOF-PET detectors with LuAG, GAGG and L(Y)SO scintillators of various sizes coupled to FBK-SiPMs. Journal of Instrumentation, 11(08), P08008-P08008. doi:10.1088/1748-0221/11/08/p0800

Exploring TOF Capabilities of PET Detector Blocks Based on Large Monolithic Crystals and Analog SiPMs

[EN] Monolithic scintillators are more frequently used in PET instrumentation due to their advantages in terms of accurate position estimation of the impinging gamma rays both planar and depth of interaction, their increased efficiency, and expected timing capabilities. Such timing performance has been studied when those blocks are coupled to digital photosensors showing an excellent timing resolution. In this work we study the timing behaviour of detectors composed by monolithic crystals and analog SiPMs read out by an ASIC. The scintillation light spreads across the crystal towards the photosensors, resulting in a high number of SiPMs and ASIC channels fired. This has been studied in relation with the Coincidence Timing Resolution (CTR). We have used LYSO monolithic blocks with dimensions of 50 x 50 x 15 mm(3) coupled to SiPM arrays (8 x 8 elements with 6 x 6 mm(2) area) which compose detectors suitable for clinical applications. While a CTR as good as 186 ps FWHM was achieved for a pair of 3 x 3 x 5 mm(3) LYSO crystals, when using the monolithic block and the SiPM arrays, a raw CTR over 1 ns was observed. An optimal timestamp assignment was studied as well as compensation methods for the time-skew and time-walk errors. This work describes all steps followed to improve the CTR. Eventually, an average detector time resolution of 497 ps FWHM was measured for the whole thick monolithic block. This improves to 380 ps FWHM for a central volume of interest near the photosensors. The timing dependency with the photon depth of interaction and planar position are also included.This project has received funding from the European Research Council (ERC) under the European Union's Horizon 2020 research and innovation program (grant agreement No 695536). It has also been supported by the Spanish Ministerio de Economia, Industria y Competitividad under Grant TEC2016-79884-C2-1-R.Lamprou, E.; González Martínez, AJ.; Sánchez Martínez, F.; Benlloch Baviera, JM. (2020). Exploring TOF Capabilities of PET Detector Blocks Based on Large Monolithic Crystals and Analog SiPMs. Physica Medica. 70:10-18. https://doi.org/10.1016/j.ejmp.2019.12.004101870Surti, S. (2014). Update on Time-of-Flight PET Imaging. Journal of Nuclear Medicine, 56(1), 98-105. doi:10.2967/jnumed.114.145029Spanoudaki, V. C., & Levin, C. S. (2010). Photo-Detectors for Time of Flight Positron Emission Tomography (ToF-PET). Sensors, 10(11), 10484-10505. doi:10.3390/s101110484Szczesniak, T., Moszynski, M., Swiderski, L., Nassalski, A., Lavoute, P., & Kapusta, M. (2009). Fast Photomultipliers for TOF PET. IEEE Transactions on Nuclear Science, 56(1), 173-181. doi:10.1109/tns.2008.2008992Renker, D. (2007). New trends on photodetectors. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 571(1-2), 1-6. doi:10.1016/j.nima.2006.10.016Kim, C. L., Wang, G.-C., & Dolinsky, S. (2009). Multi-Pixel Photon Counters for TOF PET Detector and Its Challenges. IEEE Transactions on Nuclear Science, 56(5), 2580-2585. doi:10.1109/tns.2009.2028075Moses, W. W. (2002). Current trends in scintillator detectors and materials. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 487(1-2), 123-128. doi:10.1016/s0168-9002(02)00955-5Gundacker, S., Auffray, E., Pauwels, K., & Lecoq, P. (2016). Measurement of intrinsic rise times for various L(Y)SO and LuAG scintillators with a general study of prompt photons to achieve 10 ps in TOF-PET. Physics in Medicine and Biology, 61(7), 2802-2837. doi:10.1088/0031-9155/61/7/2802Gundacker, S., Acerbi, F., Auffray, E., Ferri, A., Gola, A., Nemallapudi, M. V., … Lecoq, P. (2016). State of the art timing in TOF-PET detectors with LuAG, GAGG and L(Y)SO scintillators of various sizes coupled to FBK-SiPMs. Journal of Instrumentation, 11(08), P08008-P08008. doi:10.1088/1748-0221/11/08/p08008Surti, S., & Karp, J. S. (2016). Advances in time-of-flight PET. Physica Medica, 32(1), 12-22. doi:10.1016/j.ejmp.2015.12.007Gundacker, S., Knapitsch, A., Auffray, E., Jarron, P., Meyer, T., & Lecoq, P. (2014). Time resolution deterioration with increasing crystal length in a TOF-PET system. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 737, 92-100. doi:10.1016/j.nima.2013.11.025Marcinkowski, R., España, S., Van Holen, R., & Vandenberghe, S. (2014). Optimized light sharing for high-resolution TOF PET detector based on digital silicon photomultipliers. Physics in Medicine and Biology, 59(23), 7125-7139. doi:10.1088/0031-9155/59/23/7125González-Montoro, A., Sánchez, F., Martí, R., Hernández, L., Aguilar, A., Barberá, J., … González, A. J. (2018). Detector block performance based on a monolithic LYSO crystal using a novel signal multiplexing method. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 912, 372-377. doi:10.1016/j.nima.2017.10.098Xi, D., Xie, Q., Zhu, J., Lin, L., Niu, M., Xiao, P., … Kao, C.-M. (2012). Optimization of the SiPM Pixel Size for a Monolithic PET Detector. Physics Procedia, 37, 1497-1503. doi:10.1016/j.phpro.2012.04.101Gonzalez-Montoro A, Aguilar A, Canizares G, Conde P, Hernandez L, Vidal LF, et al. Performance Study of a Large Monolithic LYSO PET Detector With Accurate Photon DOI Using Retroreflector Layers. IEEE Trans Rad Plasma Med Sci. PP. 1-1. DOI: 10.1109/TRPMS.2017.2692819.Krishnamoorthy, S., Blankemeyer, E., Mollet, P., Surti, S., Van Holen, R., & Karp, J. S. (2018). Performance evaluation of the MOLECUBES β-CUBE—a high spatial resolution and high sensitivity small animal PET scanner utilizing monolithic LYSO scintillation detectors. Physics in Medicine & Biology, 63(15), 155013. doi:10.1088/1361-6560/aacec3González-Montoro, A., Sánchez, F., Bruyndonckx, P., Cañizares, G., Benlloch, J. M., & González, A. J. (2019). Novel method to measure the intrinsic spatial resolution in PET detectors based on monolithic crystals. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 920, 58-67. doi:10.1016/j.nima.2018.12.056Van Dam, H. T., Borghi, G., Seifert, S., & Schaart, D. R. (2013). Sub-200 ps CRT in monolithic scintillator PET detectors using digital SiPM arrays and maximum likelihood interaction time estimation. Physics in Medicine and Biology, 58(10), 3243-3257. doi:10.1088/0031-9155/58/10/3243Di Francesco A, Bugalho R, Oliveira L, Pacher L, Rivetti A, Rolo M, et al. TOFPET2: A high-performance ASIC for time and amplitude measurements of SiPM signals in time-of-flight applications. Journal of Instrumentation, vol. 11, no. 03, p. C03042.TOFPET2 ASIC Evaluation kit - Hardware User Guide (v1.2), v1.2, PETsys Electronics SA., 2018.Lamprou, E., Aguilar, A., González-Montoro, A., Monzó, J. M., Cañizares, G., Iranzo, S., … Benlloch, J. M. (2018). PET detector block with accurate 4D capabilities. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 912, 132-136. doi:10.1016/j.nima.2017.11.002Acerbi, F., & Gundacker, S. (2019). Understanding and simulating SiPMs. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 926, 16-35. doi:10.1016/j.nima.2018.11.118Schug D, Nadig V, Weissler B, Gebhardt P, Schulz V. Initial Measurements with the PETsys TOFPET2 ASIC Evaluation Kit and a Characterization of the ASIC TDC IEEE Trans Rad Plasma Med Sci. PP. 1-1. DOI: 10.1109/TRPMS.2018.2884564.Seifert, S., van Dam, H. T., Vinke, R., Dendooven, P., Lohner, H., Beekman, F. J., & Schaart, D. R. (2012). A Comprehensive Model to Predict the Timing Resolution of SiPM-Based Scintillation Detectors: Theory and Experimental Validation. IEEE Transactions on Nuclear Science, 59(1), 190-204. doi:10.1109/tns.2011.2179314Vinke R, Olcott PD, Cates JW, Levin CS. The lower timing resolution bound for scintillators with non-negligible optical photon transport time in time-of-flight PET. Phys. Med. Phys. Med. Biol. 59 6215. Phys Med Biol. 2014; 59(20): 6215–29.Gonzalez AJ, Sanchez F, Benlloch JM. 2018 Organ-Dedicated Molecular Imaging Systems. IEEE Trans Ratiat Plasma Med Sci. 2017; 2(5): 388–403

Optimization and modeling of two-phase olive-oil washing wastewater integral treatment and phenolic compounds recovery by novel weak-base ion exchange resins

In light of the Circular Economy concept, recently emerged as a need for sustainable production, olive oil industry should be concerned to transform the whole process into environmentally friendly, which necessarily implies the treatment of the wastewater by-produced in olive mills. In this work, concentration and recovery of high-added value phenolic compounds from two-phase olive-oil washing wastewater (OOWW) and parallel effluent treatment by a ‘green process’ based on novel weak-base ion exchange (IE) resins was addressed. The key operating input factors of the resin process for the treatment and valorization of OOWW were studied, optimized and further modelled. A Box-Behnken design was implemented and the obtained data were analyzed by ANOVA and interpreted by RSM methodology. The process was ulteriorly modelled by a second-grade quadratic fitting equation comprising the significant operating variables. The optimization of the IE process performance (20.3 °C, pH0 6.7 and 114 g/L Mresin) ensured up to 92.5% recovery of total phenols concentration. Moreover, the purified stream presented good quality (56.6–83.7 mg L−1 total phenols), following standard recommendations by the FAO. The obtained information would be of key importance for the scale-up of the proposed IE operation. Both the treatment and revalorization of OOWW would help implement a definite sustainable production process of olive-oil.Spanish Ministry of Economy and Competitiveness is acknowledged for having funded the project CTM2014-61105-JIN ‘Design and development of an integral process for revalorization and treatment of the effluents from olive oil industry’, as well as the University of Granada