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Journal articles on the topic 'Pile-up rejection'

Author: Grafiati

Published: 23 November 2024

Last updated: 31 July 2025

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1

Gurbich, A. F., and N. V. Kornilov. "Backscattering spectrometry with time-of-flight pile-up rejection." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 62, no. 1 (1991): 151–54. http://dx.doi.org/10.1016/0168-583x(91)95942-7.

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2

Wikne, J. C. "A CAMAC 32-channel pile-up detection and rejection module." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 330, no. 1-2 (1993): 210–14. http://dx.doi.org/10.1016/0168-9002(93)91324-g.

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3

Bourne, M. M., S. D. Clarke, M. Paff, A. DiFulvio, M. Norsworthy, and S. A. Pozzi. "Digital pile-up rejection for plutonium experiments with solution-grown stilbene." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 842 (January 2017): 1–6. http://dx.doi.org/10.1016/j.nima.2016.10.023.

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4

Helmbrecht, Stephan, Wolfgang Enghardt, Fine Fiedler, et al. "In-beam PET at clinical proton beams with pile-up rejection." Zeitschrift für Medizinische Physik 27, no. 3 (2017): 202–17. http://dx.doi.org/10.1016/j.zemedi.2016.07.003.

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5

Bastia, P., G. Bertuccio, F. Borghetti, et al. "An integrated reset/pulse pile-up rejection circuit for pixel readout ASICs." IEEE Transactions on Nuclear Science 53, no. 1 (2006): 414–17. http://dx.doi.org/10.1109/tns.2006.869852.

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6

Capogni, M., A. Ceccatelli, P. De Felice, and A. Fazio. "Random-summing correction and pile-up rejection in the sum-peak method." Applied Radiation and Isotopes 64, no. 10-11 (2006): 1229–33. http://dx.doi.org/10.1016/j.apradiso.2006.02.027.

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7

Hu, Kun, Feng Li, Lian Chen, Fu-Tian Liang, and Ge Jin. "An FPGA-Based Pulse Pile-up Rejection Technique for Photon Counting Imaging Detectors." Chinese Physics Letters 32, no. 3 (2015): 030701. http://dx.doi.org/10.1088/0256-307x/32/3/030701.

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8

Sjöland, K. A., and P. Kristiansson. "Pile-up and defective pulse rejection by pulse shape discrimination in surface barrier detectors." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 94, no. 3 (1994): 333–37. http://dx.doi.org/10.1016/0168-583x(94)95374-0.

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9

Iguaz, F. J., L. Bombelli, S. Meo, et al. "DANTE Digital Pulse Processor for XRF and XAS experiments." Journal of Instrumentation 18, no. 06 (2023): T06011. http://dx.doi.org/10.1088/1748-0221/18/06/t06011.

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Abstract DANTE is a new Digital Pulse Processor (DPP) developed for fluorescence detectors, like Silicon Drift Detectors (SDDs) or High Purity Germanium detectors (HPGe), used in X-ray Fluorescence (XRF) and X-ray Absorption Spectroscopy (XAS) experiments at synchrotron facilities. Its main features are its optimal energy resolution and peak stability for detector count rate values up to 1–2 Mcps, and its enhanced rejection of pile-up events. In this paper, we present the first complete evaluation of DANTE performance in SOLEIL synchrotron facility. DANTE has been tested in laboratory with an

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10

Lyon, Anne-Mazarine. "Optimisation of the CMS ECAL clustering algorithms in view of LHC-Run 3." Journal of Physics: Conference Series 2374, no. 1 (2022): 012015. http://dx.doi.org/10.1088/1742-6596/2374/1/012015.

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The Run 3 of the Large Hadron Collider (LHC) will be characterised by an enhanced level of noise in the CMS electromagnetic calorimeter (ECAL), caused by the ageing of the photosensors and the loss of crystal transparency due to radiation damage. To face these new conditions, some parameters of the clustering algorithms of the ECAL, namely the Particle-Flow Clustering and SuperClustering algorithms, are tuned to offer optimal performance in terms of signal preservation and noise and pile-up rejection. The methods used for the tuning as well as its performance are presented.

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11

Zuo, Jingxin, Jingkai Wang, Shangmian Du, et al. "A method combining pulse shape discrimination and pile-up rejection for plastic scintillator detectors based on multiresolution analysis." Journal of Instrumentation 20, no. 04 (2025): P04009. https://doi.org/10.1088/1748-0221/20/04/p04009.

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Abstract This paper introduces a new method for neutron-gamma pulse shape discrimination (PSD) and pile-up signal rejection (PUR) based on multi-resolution analysis (MRA). The method uses a fast wavelet transform to decompose the original signal, extracting approximate components through low-pass filtering and detail components through high-pass filtering. Following reconstruction, the approximate and detail components are analyzed to achieve efficient PSD and PUR, respectively. The experiments used an EJ276 plastic scintillator detector to collect neutron and gamma signals from an Am-Be sourc

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12

Zhong, Xiaodong, Lian Chen, Baochen Wang, and Ge Jin. "A spectrometer with baseline correction and fast pulse pile-up rejection for prompt gamma neutron activation analysis technology." Review of Scientific Instruments 89, no. 12 (2018): 123504. http://dx.doi.org/10.1063/1.5049517.

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13

Okuda, T., H. Yamazaki, M. Kawabata, J. Kasagi та H. Harada. "Performance of n–γ pulse-shape discrimination with simple pile-up rejection at high γ-ray count rates". Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 426, № 2-3 (1999): 497–502. http://dx.doi.org/10.1016/s0168-9002(98)01382-5.

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14

Satoh, T., K. Ishii, S. Matsuyama, et al. "INVESTIGATION ON THE INFLUENCE OF BACK SCATTERED PROTONS IN PIXE SPECTRUM." International Journal of PIXE 11, no. 01n02 (2001): 49–59. http://dx.doi.org/10.1142/s0129083501000086.

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The pre-amplifier with an active reset system was examined to carry out PIXE analysis under the condition that X-rays and back scattered protons are detected simultaneously. Rejection of false signals produced by back scattered protons is discussed, and it is confirmed that false signals can be completely rejected by using an inhibit signal of the preamplifier. Energy resolution of an X-ray detector and a live-time of measurement system were measured as a function of counting rate. As a result, energy resolution did not change and the live-time was 70 % at the high counting rate over 3kcps. Th

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15

Kim, G. B., S. Choi, F. A. Danevich, et al. "A CaMoO4Crystal Low Temperature Detector for the AMoRE Neutrinoless Double Beta Decay Search." Advances in High Energy Physics 2015 (2015): 1–7. http://dx.doi.org/10.1155/2015/817530.

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We report the development of a CaMoO4crystal low temperature detector for the AMoRE neutrinoless double beta decay(0νββ)search experiment. The prototype detector cell was composed of a 216 g CaMoO4crystal and a metallic magnetic calorimeter. An overground measurement demonstrated FWHM resolution of 6–11 keV for full absorption gamma peaks. Pulse shape discrimination was clearly demonstrated in the phonon signals, and 7.6 σof discrimination power was found for theαandβ/γseparation. The phonon signals showed rise-times of about 1 ms. It is expected that the relatively fast rise-time will increas

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16

Langrock, Gert, Norbert Wiehl, Hans-Otto Kling, et al. "Digital liquid-scintillation counting and effective pulse-shape discrimination with artificial neural networks." Radiochimica Acta 103, no. 1 (2015): 15–25. http://dx.doi.org/10.1515/ract-2014-2281.

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Abstract A typical problem in low-level liquid scintillation (LS) counting is the identification of α particles in the presence of a high background of β and γ particles. Especially the occurrence of β-β and β-γ pile-ups may prevent the unambiguous identification of an α signal by commonly used analog electronics. In this case, pulse-shape discrimination (PSD) and pile-up rejection (PUR) units show an insufficient performance. This problem was also observed in own earlier experiments on the chemical behaviour of transactinide elements using the liquid-liquid extraction system SISAK in combinat

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17

Ronchi, E., P. A. Söderström, J. Nyberg, et al. "An artificial neural network based neutron–gamma discrimination and pile-up rejection framework for the BC-501 liquid scintillation detector." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 610, no. 2 (2009): 534–39. http://dx.doi.org/10.1016/j.nima.2009.08.064.

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18

Haase, Ernst L., та I. Khubeis. "Measurement of oxygen depth profiles using the 16O(d, α)14N reaction and a fast pulse pile-up rejection circuit". Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 10-11 (травень 1985): 727–34. http://dx.doi.org/10.1016/0168-583x(85)90094-1.

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19

Mišura, Arijana Burazin, Josip Musić, Marina Prvan, and Damir Lelas. "Towards Real-Time Machine Learning-Based Signal/Background Selection in the CMS Detector Using Quantized Neural Networks and Input Data Reduction." Applied Sciences 14, no. 4 (2024): 1559. http://dx.doi.org/10.3390/app14041559.

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The Large Hadron Collider (LHC) is being prepared for an extensive upgrade to boost its particle discovery potential. The new phase, High Luminosity LHC, will operate at a factor-of-five-increased luminosity (the number proportional to the rate of collisions). Consequently, such an increase in luminosity will result in enormous quantities of generated data that cannot be transmitted or stored with the currently available resources and time. However, the vast majority of the generated data consist of uninteresting data or pile-up data containing few interesting events or electromagnetic showers

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20

M., N. Islam, and Akhter H. "Study of FPGA Based Multi Channel Analyzer for Gamma Ray and X Ray Spectrometry." International Journal of Trend in Scientific Research and Development 3, no. 3 (2019): 61–65. https://doi.org/10.31142/ijtsrd19113.

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Study of FPGA Based Multi channel Analyzer MCA for Gamma ray and X ray Spectroscopy has been presented in this article. For the systems, FPGA has been chosen as the central pulse processor. And NaI Tl scintillation counter, BF3 or Silicon Drift Detector followed by Voltage Preamplifier VPA or Fast Amplifier, Shaping Amplifier of 150 ns and 450 ns and high resolution ADC 8 12 bit, 50 MHz . Special features for the systems are Pulse Pile up Detection and Rejection, Clipping Pulses and Base line Restoration BLR . The system performance varies from 332 KCPS to 400 KCPS. Energy spectrum in the pres

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21

Martinis, John M., K. D. Irwin, D. A. Wollman, G. C. Hilton, L. L. Dulcie, and N. F. Bergren. "The Next Generation of EDS: Microcalorimeter Eds With 3 eV Energy Resolution." Microscopy and Microanalysis 4, S2 (1998): 172–73. http://dx.doi.org/10.1017/s1431927600020985.

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Semiconductor energy dispersive spectrometers (EDS), the most commonly used detectors for x-ray microanalysis, have matured to the point that significant improvement in energy resolution is not expected in the future. We believe a revolutionary advance in x-ray microanalysis will occur in the next few years due to the development of new x-ray spectrometers based on microcalorimeters. Energy resolution comparable with wavelength dispersive spectrometers, 3 eV to 10 eV, has already been achieved; future detectors may reach a fundamental limit as low as 0.5 eV to 1 eV.In a microcalorimeter, the e

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22

Song, Wen-Gang, Li-Jun Zhang, Jing Zhang, and Guan-Ying Wang. "Research on digital pulse processing techniques for silicon drift detector." Acta Physica Sinica 71, no. 1 (2022): 012903. http://dx.doi.org/10.7498/aps.71.20211062.

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Silicon drift detector (SDD) is a kind of high performance X-ray detector, which is widely used. The ray detection system based on SDD is composed of SDD device, preamplifier and pulse processing system. The now available pulse processing system has the problems of poor pulse pile-up rejection performance and being vulnerable to the parameter fluctuations of front-end system, which degrades the performance of detection system. A digital pulse processing system is proposed. In this system, analog-to-digital converter (ADC) directly samples the output signal of preamplifier, and transmits the da

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23

Wollman, D. A., G. C. Hilton, K. D. Irwin, L. L. Dulcie, Dale E. Newbury, and John M. Martinis. "High-Energy-Resolution Microcalorimeter Spectrometer for EDS X-ray Micro Analysis." Microscopy and Microanalysis 3, S2 (1997): 1073–74. http://dx.doi.org/10.1017/s1431927600012253.

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Si(Li) and Ge Energy Dispersive Spectroscopy (EDS) detectors are commonly used for x-ray microanalysis because they are easy to use, inexpensive to operate, and offer both rapid qualitative evaluation of chemical composition and accurate quantitative analysis. Unfortunately, they are limited by energy resolutions on the order of 100 eV, which is insufficient to resolve many important overlapping x-ray peaks in materials of industrial interest, such as the Si Kα and W Mα peak overlap in WSi2. Although WDS spectrometers with excellent energy resolution (typically 2 eV to 10 eV) can resolve most

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24

Fantini, G., A. Armatol, E. Armengaud, et al. "Machine Learning Techniques for Pile-Up Rejection in Cryogenic Calorimeters." Journal of Low Temperature Physics, May 27, 2022. http://dx.doi.org/10.1007/s10909-022-02741-9.

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AbstractCUORE Upgrade with Particle IDentification (CUPID) is a foreseen ton-scale array of Li2MoO4 (LMO) cryogenic calorimeters with double readout of heat and light signals. Its scientific goal is to fully explore the inverted hierarchy of neutrino masses in the search for neutrinoless double beta decay of 100Mo. Pile-up of standard double beta decay of the candidate isotope is a relevant background. We generate pile-up heat events via injection of Joule heater pulses with a programmable waveform generator in a small array of LMO crystals operated underground in the Laboratori Nazionali del

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25

Marcer, Giulia, Andrea Dal Molin, Marica Rebai, Davide Rigamonti, and Marco Tardocchi. "Degenerate Pile-up Correction in Pulse Height Spectra from Gamma-ray Spectrometers." Journal of Fusion Energy 43, no. 1 (2024). http://dx.doi.org/10.1007/s10894-024-00409-8.

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AbstractOne of the primary obstacles faced by spectrometers operating under high counting rates is pile-up, which occurs when two or more events are detected within a timelapse short enough to result in a superposition of the events waveforms. These can not hence be integrated separately in order to get their amplitudes. Piled-up events are typically identified using pile-up rejection or recovery algorithms. In the latter case, the constituent single waveforms and their amplitudes are also restored. However, there are instances in which the pulses overlap so closely that it is impossible to id

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26

Ahmine, A., A. Armatol, I. Bandac, et al. "Enhanced light signal for the suppression of pile-up events in Mo-based bolometers for the 0$$\nu \beta \beta $$ decay search." European Physical Journal C 83, no. 5 (2023). http://dx.doi.org/10.1140/epjc/s10052-023-11519-6.

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AbstractRandom coincidences of events could be one of the main sources of background in the search for neutrino-less double-beta decay of $$^{100}$$ 100 Mo with macro-bolometers, due to their modest time resolution. Scintillating bolometers as those based on Li$$_2$$ 2 MoO$$_4$$ 4 crystals and employed in the CROSS and CUPID experiments can eventually exploit the coincident fast signal detected in a light detector to reduce this background. However, the scintillation provides a modest signal-to-noise ratio, making difficult a pile-up pulse-shape recognition and rejection at timescales shorter

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27

Aaboud, M., G. Aad, B. Abbott, et al. "Identification and rejection of pile-up jets at high pseudorapidity with the ATLAS detector." European Physical Journal C 77, no. 9 (2017). http://dx.doi.org/10.1140/epjc/s10052-017-5081-5.

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28

Aaboud, M., G. Aad, B. Abbott, et al. "Correction to: Identification and rejection of pile-up jets at high pseudorapidity with the ATLAS detector." European Physical Journal C 77, no. 10 (2017). http://dx.doi.org/10.1140/epjc/s10052-017-5245-3.

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29

Albakry, M. F., I. Alkhatib, D. Alonso-González, et al. "Light dark matter constraints from SuperCDMS HVeV detectors operated underground with an anticoincidence event selection." Physical Review D 111, no. 1 (2025). https://doi.org/10.1103/physrevd.111.012006.

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This article presents constraints on dark-matter-electron interactions obtained from the first underground data-taking campaign with multiple SuperCDMS HVeV detectors operated in the same housing. An exposure of 7.63 g−days is used to set upper limits on the dark-matter-electron scattering cross section for dark matter masses between 0.5 and 1000 MeV/c2, as well as upper limits on dark photon kinetic mixing and axionlike particle axioelectric coupling for masses between 1.2 and 23.3 eV/c2. Compared to an earlier HVeV search, sensitivity was improved as a result of an increased overburden of 22

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30

Sani, Abubakar Kawuwa, and Rao Martand Singh. "Incorporating phase change materials in geothermal energy piles for thermal energy storage." Symposium on Energy Geotechnics 2023, October 2, 2023. http://dx.doi.org/10.59490/seg.2023.573.

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Introduction Geothermal energy piles (GEPs) are foundation elements that are installed in the ground to support the weight of the building to a competent strata. Energy loops are installed into the piles to allow heat rejection or extraction via the circulation of fluid through the loops. In winter, low-grade heat is extracted from the ground (source) and transferred to the building (sink) to achieve space heating. Conversely, in summer, heat is removed from the building and rejected into the ground to achieve space cooling. The system relies on the temperature gradient between the groun

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31

Aad, G., B. Abbott, D. C. Abbott, et al. "Configuration and performance of the ATLAS b-jet triggers in Run 2." European Physical Journal C 81, no. 12 (2021). http://dx.doi.org/10.1140/epjc/s10052-021-09775-5.

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AbstractSeveral improvements to the ATLAS triggers used to identify jets containing b-hadrons (b-jets) were implemented for data-taking during Run 2 of the Large Hadron Collider from 2016 to 2018. These changes include reconfiguring the b-jet trigger software to improve primary-vertex finding and allow more stable running in conditions with high pile-up, and the implementation of the functionality needed to run sophisticated taggers used by the offline reconstruction in an online environment. These improvements yielded an order of magnitude better light-flavour jet rejection for the same b-jet

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32

Seale, Kirsten. "Location, Location." M/C Journal 9, no. 5 (2006). http://dx.doi.org/10.5204/mcj.2668.

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   Last year, the ABC’s Media Watch (17 Oct. 2005) noted the continuing outrage in the tabloid media over “the dirtiest house in NSW”. The program took issue with Sydney newspaper The Daily Telegraph, and the descriptor “exclusive” attached to their article on a property in beachside Bondi (9 Oct. 2005). In fact, as Media Watch pointed out, Channel Seven’s current affairs flagship Today Tonight had already made repeat visits to the residence. A Current Affair, Channel Nine’s rival show, as well as Bondi’s local newspaper also offered coverage. However, I am interested not in

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33

Caldwell, Tracy M. "Identity Making from Soap to Nuts." M/C Journal 6, no. 1 (2003). http://dx.doi.org/10.5204/mcj.2149.

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The release of the film Fight Club (Dir. David Fincher, 1999) was met with an outpouring of contradictory reviews. From David Ansen’s [Newsweek] claim that “Fight Club is the most incendiary movie to come out of Hollywood in a long time” (Fight Club DVD insert) to LA Times’s Kenneth Turan who proclaimed Fight Club to be “…a witless mishmash of whiny, infantile philosophising and bone-crushing violence that actually thinks it’s saying something of significance” (Fight Club DVD insert), everyone, it seemed, needed to weigh in with their views. Whether you think the film is a piece of witless and

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