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Journal articles on the topic 'Function detector'

Author: Grafiati

Published: 30 May 2022

Last updated: 31 July 2025

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1

Celik, Cihangir, Douglas E. Peplow, Gregory G. Davidson, and Mathew W. Swinney. "A Directional Detector Response Function for Anisotropic Detectors." Nuclear Science and Engineering 193, no. 12 (2019): 1355–70. http://dx.doi.org/10.1080/00295639.2019.1631028.

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2

Wirawan, Rahadi, M. Djamal, A. Waris, Gunawan Handayani, and Hong Joo Kim. "Response Function of Collimated Detector for Non Axial Detector-Source Geometry." Advanced Materials Research 772 (September 2013): 571–78. http://dx.doi.org/10.4028/www.scientific.net/amr.772.571.

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Response function is a fundamental parameter for all detectors in order to analyze the energy distribution of gamma ray which undergoes scattering interaction with the material. The response functions of a 3 in. x 3 in. NaI(Tl) collimated detector for non axis detector-source geometry has been calculated using a Monte Carlo approach from GEANT4 simulation code with 0.662 MeV of mono-energetic of photon gamma ray. Collimated Pb with 4 cm thickness and 2 cm of holes diameter were employed for shielding. The source was assumed as an isotropic point source and it is placed at various positions to

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3

Jeong, Seongkwon, and Jaejin Lee. "Soft-Output Detector Using Multi-Layer Perceptron for Bit-Patterned Media Recording." Applied Sciences 12, no. 2 (2022): 620. http://dx.doi.org/10.3390/app12020620.

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As conventional data storage systems are faced with critical problems such as the superparamagnetic limit, bit-patterned media recording (BPMR) has received significant attention as a promising next-generation magnetic data storage system. However, the reduced spacing between islands at increased areal density causes severe intersymbol and intertrack interference, which degrade BPMR system performance. In this study, we introduce a soft-output detector using multi-layer perceptron to predict reliable information. A received signal is equalized and detected by the MLP detector. The MLP detector

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4

Karapetyan, G. G. "Directivity function of muon detector." Astroparticle Physics 61 (February 2015): 17–21. http://dx.doi.org/10.1016/j.astropartphys.2014.06.002.

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5

Oh, Seokwon, Seungjun Yoo, Hubeom Shin, Junho Lee, Dong Uk Kim, and Ho Kyung Kim. "Signal and noise analysis of a metal oxide transistor-based flat-panel detector." Journal of Instrumentation 18, no. 10 (2023): C10016. http://dx.doi.org/10.1088/1748-0221/18/10/c10016.

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Abstract Recently, metal-oxide thin-film transistor (TFT)-based flat-panel x-ray detectors have attracted attention owing to their fast readout times and low noise characteristics. We empirically analyzed the signal and noise characteristics of an indium gallium zinc oxide (IGZO) TFT-based detector in comparison with those of a conventional hydrogenated amorphous silicon (a-Si:H) TFT-based detector. We compared the large-area signal transfer functions of the detectors as a function of air kerma at their entrance surfaces. Signal and noise performances were evaluated by measuring the modulation

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6

Abramov, Yuriy, Yaroslav Kalchenko, and Olena Liashevska. "DETERMINATION OF DYNAMIC CHARACTERISTICS OF HEAT FIRE DETECTORS." EUREKA: Physics and Engineering 3 (May 31, 2019): 50–59. http://dx.doi.org/10.21303/2461-4262.2019.00898.

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The proposed methods for determining the dynamic characteristics of heat fire detectors in the time and frequency domains, focused on the use of existing thermal chambers. The proposed method for determining the transition function of the detector is implemented as follows. Heat fire detector creates a thermal effect in the form of a linearly increasing function. The response of the output signal to the influence of this type is measured and approximated using the Heaviside function at regular intervals. It is shown that information on the transition function of a heat fire detector can be use

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7

El-Tayebany, R. A., and N. Shaaban. "Influence of dead layer on the response function of planar and coaxial Ge detector using Monte Carlo method." Nuclear Physics and Atomic Energy 24, no. 4 (2023): 388–94. http://dx.doi.org/10.15407/jnpae2023.04.388.

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Germanium crystals have a dead layer that causes a decrease in efficiency since the layer is not useful for detection but strongly attenuates photons. The thickness of this inactive layer is not well known due to the existence of a transition zone where photons are increasingly absorbed. Therefore, using data provided by manufacturers in the detector simulation model, some strong discrepancies appear by changing the dead layer. Investigations into the Ge detector response functions for gamma rays have been conducted using straightforward physical mechanisms implemented by Monte Carlo simulatio

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8

Yuriy, Abramov, Kalchenko Yaroslav, and Liashevska Olena. "DETERMINATION OF DYNAMIC CHARACTERISTICS OF HEAT FIRE DETECTORS." EUREKA: Physics and Engineering, no. 3 (May 31, 2019): 50–59. https://doi.org/10.21303/2461-4262.2019.00898.

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The proposed methods for determining the dynamic characteristics of heat fire detectors in the time and frequency domains, focused on the use of existing thermal chambers. The proposed method for determining the transition function of the detector is implemented as follows. Heat fire detector creates a thermal effect in the form of a linearly increasing function. The response of the output signal to the influence of this type is measured and approximated using the Heaviside function at regular intervals. It is shown that information on the transition function of a heat fire detector can be use

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9

Chi, Tao, та Ding Song Zhang. "Response Function Test of Marine γ-Spectrometry with Different Detector Material". Key Engineering Materials 500 (січень 2012): 108–13. http://dx.doi.org/10.4028/www.scientific.net/kem.500.108.

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The marine radioactivity measurement is the low-level radiation measurement, whose accuracy mainly depends on the material and design of the detector. However, the currently research results mainly focus on the qualitative research. In this paper, a Monte Carlo code MCNP was utilized to simulate the comparation of the energy spectra of several relevant γ rays recorded by detectors immersed in seawater, The detection efficiency and the effective detection distance of these detectors to the radionuclides of 137Cs dispersed in seawater were calculated．The results of our experiment shown that the

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10

Tavakoli-A, H., R. Izadi-Naja, and H. Miri-Hakim. "The Effect of Detector Dimensions on the NaI (Tl) Detector Response Function." Journal of Applied Sciences 9, no. 11 (2009): 2168–73. http://dx.doi.org/10.3923/jas.2009.2168.2173.

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11

Liu, Xin, and Hyoung Koo Lee. "Detector response function of an energy-resolved CdTe single photon counting detector." Journal of X-Ray Science and Technology 22, no. 6 (2014): 735–44. http://dx.doi.org/10.3233/xst-140458.

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12

Poudel, Suresh, Asita Kulshreshtha, Golam Abu Zakaria, and Günther H. Hartmann. "On correction factors for profile measurements with small solid state detectors and with small ionization chambers." Polish Journal of Medical Physics and Engineering 31, no. 1 (2025): 51–61. https://doi.org/10.2478/pjmpe-2025-0005.

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Abstract Introduction: Measured profiles, which are crucial to treatment planning system commissioning, are generally affected by averaging effect linked to the size of sensitive volume of detectors used. Such averaging leads to deviation from the true profiles in water even when small field detectors are employed. In order to have access to profile data which are free from the influence of the measuring device, a guidance is required, on when and how much correction is required for a detector in use. Material and methods: Profile correction factors were determined as the ratio between true pr

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13

TUZNIK, STANLEY L., PETER J. OLVER, and ALLEN TANNENBAUM. "Equi-affine differential invariants for invariant feature point detection." European Journal of Applied Mathematics 31, no. 2 (2019): 277–96. http://dx.doi.org/10.1017/s0956792519000020.

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Image feature points are detected as pixels which locally maximise a detector function, two commonly used examples of which are the (Euclidean) image gradient and the Harris–Stephens corner detector. A major limitation of these feature detectors is that they are only Euclidean-invariant. In this work, we demonstrate the application of a 2D equi-affine-invariant image feature point detector based on differential invariants as derived through the equivariant method of moving frames. The fundamental equi-affine differential invariants for 3D image volumes are also computed.

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14

Tursinah, Rasito, Bunawas Bunawas, and Jungho Kim. "NEUTRON RESPONSE FUNCTION OF BONNER SPHERE SPECTROMETER WITH 6LiI(Eu) DETECTOR." GANENDRA Majalah IPTEK Nuklir 20, no. 2 (2017): 65. http://dx.doi.org/10.17146/gnd.2017.20.2.3319.

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Neutron Response Function of Bonner Sphere Spectrometer With 6LiI(Eu) Detector. The detector response function was needed to measure the neutron fluence based on the count rates from Bonner Sphere Spectrometer (BSS). The determination of response function of a BSS with 6LiI(Eu) detector has been performed using Monte Carlo MCNPX code. This calculation was performed for BSS using scintillation detector of 4 mm × 4 mm 6LiI(Eu) which is placed at the center of a set of polyethylene spheres i.e bare, 2", 3", 5", 8", 10", and 12" diameters. The BSS response functions were obtained for neutron energ

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15

INAGAKI, Shintaro, Tomio YAMAURA, and Akira KOBAYASHI. "Spatial Filter Detector with Weighting Function Variability." Transactions of the Society of Instrument and Control Engineers 23, no. 6 (1987): 633–35. http://dx.doi.org/10.9746/sicetr1965.23.633.

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16

Alsaleh, Salwa. "Accelerated Detector Response Function in Squeezed Vacuum." Technologies 5, no. 2 (2017): 17. http://dx.doi.org/10.3390/technologies5020017.

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17

Luo, Heng, Ning Jie Jin, Xiao Yan Ye, Jun Chen Li, and Lu Gao. "An Indoor Multi-Function Environment Detector Model." Applied Mechanics and Materials 713-715 (January 2015): 544–47. http://dx.doi.org/10.4028/www.scientific.net/amm.713-715.544.

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Modern people spend more than 90% of their life indoors and therefore the indoor environment quality has great impact on the body health and working efficiency of human beings. A series of detectors thus been developed to evaluate the indoor environment quality. Nevertheless, these devices are either expensive or too simple. In this paper, a portable detector model, basing on the Lego Blocks Principle, is proposed. Users are able to select sensing modules according to their preference based on the precision requirements, price constraints and size limitations before piling them together like b

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18

Lutostansky, Yu S., and N. B. Shul’gina. "Strength function ofXe127and iodine-xenon neutrino detector." Physical Review Letters 67, no. 4 (1991): 430–32. http://dx.doi.org/10.1103/physrevlett.67.430.

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19

Nakamura, Kouji. "Weak Value in Wave Function of Detector." Journal of the Physical Society of Japan 79, no. 12 (2010): 125003. http://dx.doi.org/10.1143/jpsj.79.125003.

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20

Drga, Rudolf, Dagmar Janacova, and Hana Charvatova. "Simulation of the PIR detector active function." MATEC Web of Conferences 76 (2016): 04036. http://dx.doi.org/10.1051/matecconf/20167604036.

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21

Krishnamoorthy, A. V., T. K. Woodward, K. W. Goossen, et al. "Dual-Function Detector–Modulator Smart-Pixel Module." Applied Optics 36, no. 20 (1997): 4866. http://dx.doi.org/10.1364/ao.36.004866.

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22

Kim, Hyunduk, Gyuseong Cho, and Bo-Sun Kang. "Study on response function of CdTe detector." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 610, no. 1 (2009): 302–6. http://dx.doi.org/10.1016/j.nima.2009.05.097.

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23

Puc, M. D., M. Budnar, M. Kavčič, and P. Pelicon. "Detector response function for fitting PIXE spectra." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 189, no. 1-4 (2002): 123–30. http://dx.doi.org/10.1016/s0168-583x(01)01017-5.

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24

He, T., R. P. Gardner, and K. Verghese. "An improved Si(Li) detector response function." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 299, no. 1-3 (1990): 354–66. http://dx.doi.org/10.1016/0168-9002(90)90805-g.

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25

Zybov, V. N. "Simulating primary detector function in multifactor measurements." Measurement Techniques 49, no. 4 (2006): 348–56. http://dx.doi.org/10.1007/s11018-006-0113-9.

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26

Marwaha, L., and F. Tondeur. "Response function of the CdZnTe SPEAR detector." X-Ray Spectrometry 40, no. 6 (2011): 417–19. http://dx.doi.org/10.1002/xrs.1368.

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27

Melbinger, Julian, Christina Weiss, Erich Griesmayer, Erwin Jericha, and Dieter Hainz. "Diamond based neutron detector in high temperature environments of 200 °C." Journal of Instrumentation 19, no. 07 (2024): P07015. http://dx.doi.org/10.1088/1748-0221/19/07/p07015.

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Abstract The stability of the neutron response function and the detection efficiency of a sCVD diamond detector in the temperature range up to 200 °C are demonstrated in this paper. A CIVIDEC neutron detector was simultaneously heated with an AmBe neutron source. This enabled the measurement of the spectrum of the deposited energy in the diamond sensor, i.e. the neutron response function of the detector and the detection rate, which in combination represents the neutron flux as a function of temperature. The measured temperature stability of the neutron response function of the detector and de

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28

Sun, Shuai, Ruoyu Zhang, Jiaxin Peng, et al. "MO detector (MOD): a dual-function optical modulator-detector for on-chip communication." Optics Express 26, no. 7 (2018): 8252. http://dx.doi.org/10.1364/oe.26.008252.

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29

Егоров, С. Б., and Р. И. Горбачев. "Probability function of waiting for double threshold detector." MORSKIE INTELLEKTUAL`NYE TEHNOLOGII)</msg>, no. 4(58) (December 2, 2022): 156–61. http://dx.doi.org/10.37220/mit.2022.58.4.037.

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На основе «выбросовой» физической модели работы автоматического обнаружителя в режиме ожидания сигнала, когда ложное срабатывание ассоциируется с появлением «ложного выброса» помехового индикаторного процесса выше уровня обнаружения, разработана вероятностная «выбросовая» модель работы двухпорогового обнаружителя, – обнаружителя с порогами по уровню и длительности, в режиме ожидания сигнала. Модель разработана в приближении независимости вероятностных характеристик длительности ложных выбросов от числа выбросов на интервале ожидания. С помощью вероятностной модели и использования функций распр

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30

Li, Buyu, Yu Liu, and Xiaogang Wang. "Gradient Harmonized Single-Stage Detector." Proceedings of the AAAI Conference on Artificial Intelligence 33 (July 17, 2019): 8577–84. http://dx.doi.org/10.1609/aaai.v33i01.33018577.

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Despite the great success of two-stage detectors, single-stage detector is still a more elegant and efficient way, yet suffers from the two well-known disharmonies during training, i.e. the huge difference in quantity between positive and negative examples as well as between easy and hard examples. In this work, we first point out that the essential effect of the two disharmonies can be summarized in term of the gradient. Further, we propose a novel gradient harmonizing mechanism (GHM) to be a hedging for the disharmonies. The philosophy behind GHM can be easily embedded into both classificati

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31

Zhong, Bao Jiang, and Chang Li. "Robust Image Corner Detection Using Curvature Product in Direct Curvature Scale Space." Applied Mechanics and Materials 20-23 (January 2010): 725–30. http://dx.doi.org/10.4028/www.scientific.net/amm.20-23.725.

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In this paper we propose an image corner detector based on the direct curvature scale space (DCSS) technique, referred to as the curvature product DCSS (CP-DCSS) corner detector. After the contours of interested objects are extracted from a real-world image, their curvature functions are respectively convolved with the Gaussian function as its standard deviation gradually increases. By measuring the product of the curvature values computed at several given scales, true corners on the contours can be easily detected since false or insignificant corners have been effectively suppressed. A point

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32

Pfeiffer, D., F. Brunbauer, V. Cristiglio, et al. "Demonstration of Gd-GEM detector design for neutron macromolecular crystallography applications." Journal of Instrumentation 18, no. 04 (2023): P04023. http://dx.doi.org/10.1088/1748-0221/18/04/p04023.

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Abstract The European Spallation Source (ESS) in Lund, Sweden will become the world's most powerful thermal neutron source. The Macromolecular Diffractometer (NMX) at the ESS requires three 51.2 × 51.2 cm2 detectors with reasonable detection efficiency, sub-mm spatial resolution, a narrow point-spread function (PSF), and good time resolution. This work presents measurements with the improved version of the NMX detector prototype consisting of a Triple-GEM (Gas Electron Multiplier) detector with a natural Gd converter and a low material budget readout. The detector was successfully tested at th

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33

Benítez, Ricardo Betancourt, Ruola Ning, David Conover, and Shaohua Liu. "Measurements of the Modulation Transfer Function, Normalized Noise Power Spectrum and Detective Quantum Efficiency for two flat panel detectors: A Fluoroscopic and a Cone Beam Computer Tomography Flat Panel Detectors." Journal of X-Ray Science and Technology: Clinical Applications of Diagnosis and Therapeutics 17, no. 4 (2009): 279–93. http://dx.doi.org/10.3233/xst-2009-023400234.

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The physical performance of two Flat Panel Detectors has been evaluated. The first Flat Panel Detector is for Fluoroscopic applications, Varian PaxScan 2520, and the second is for Cone Beam Computer Tomography applications, Varian PaxScan 4030CB. First, the spectrum of the X-ray source was measured. Second, the linearity of the detectors was investigated by using an ionization chamber and the average ADU values of the detectors. Third, the temporal resolution was characterized by evaluating their image lag. Fourth, their spatial resolution was characterized by the pre-sampling Modulation Trans

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34

Kriegner, Dominik, Zdeněk Matěj, Radomír Kužel, and Václav Holý. "Powder diffraction in Bragg–Brentano geometry with straight linear detectors." Journal of Applied Crystallography 48, no. 2 (2015): 613–18. http://dx.doi.org/10.1107/s1600576715003465.

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A common way of speeding up powder diffraction measurements is the use of one- or two-dimensional detectors. This usually goes hand in hand with worse resolution and asymmetric peak profiles. In this work the influence of a straight linear detector on the resolution function in the Bragg–Brentano focusing geometry is discussed. Because of the straight nature of most modern detectors geometrical defocusing occurs, which heavily influences the line shape of diffraction lines at low angles. An easy approach to limit the resolution-degrading effects is presented. The presented algorithm selects an

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35

Ida, T. "Connection of segmented intensity data measured with a multiple-detector system for powder diffractometry." Journal of Applied Crystallography 38, no. 5 (2005): 795–803. http://dx.doi.org/10.1107/s0021889805021709.

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A Fourier method to connect segmented intensity data measured with a multiple-detector system (MDS) for powder diffractometry has been developed. Differences in sensitivity, slight shifts in peak positions and asymmetric instrumental broadening for different detectors are simultaneously adjusted by a Fourier-based deconvolution/convolution method. The Fourier transform of the adjustment function is evaluated as the ratio of the Fourier transforms of the intensity data sets in the overlapped region measured with the adjacent detectors. Even and odd polynomial functions with maximum order of 10

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36

Fida, M. A., Fang Liu, Min Li, Tianze Jiang, and Xiaoxue Fan. "Response Function Simulation of Labr3 (Ce) Scintillation Detector." Journal of Physics: Conference Series 1739 (January 2021): 012002. http://dx.doi.org/10.1088/1742-6596/1739/1/012002.

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37

Anosov, A. A., A. A. Sharakshane, A. S. Kazanskii, A. D. Mansfel’d, A. G. Sanin, and A. S. Sharakshane. "Instrument function of a broadband acoustic thermometric detector." Acoustical Physics 62, no. 5 (2016): 626–32. http://dx.doi.org/10.1134/s1063771016050018.

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38

Belforte, G., T. Raparelli, V. Viktorov, G. Eula, and A. Ivanov. "Frequency transfer function of an opto-pneumatic detector." Mechatronics 6, no. 8 (1996): 855–66. http://dx.doi.org/10.1016/s0957-4158(96)00031-1.

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39

Fonte, R., A. Insolia, G. Lanzanó, et al. "Response function of a BaF2 detector to electrons." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 307, no. 1 (1991): 80–82. http://dx.doi.org/10.1016/0168-9002(91)90133-b.

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40

Alamaniotis, Miltiadis, Jason Young, and Lefteri H. Tsoukalas. "Assessment of Fuzzy Logic Radioisotopic Pattern Identifier on Gamma-Ray Signals with Application to Security." International Journal of Monitoring and Surveillance Technologies Research 2, no. 1 (2014): 1–21. http://dx.doi.org/10.4018/ijmstr.2014010101.

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Analysis of acquired nuclear detector gamma-ray signals for recognition of present radioisotopic signatures is crucial to national security and security applications. Identification algorithms must be accurate and rapid. Artificial intelligence is a scientific field with a variety of tools suitable to implement automated processing of nuclear signals. The use of low resolution portable detectors to measure gamma-ray signals has found a wide use in security and safeguards applications. In this paper, the fuzzy logic based analysis methodology that has been previously developed is applied and as

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41

Dabylova, S. B., Yu N. Kopach, S. K. Sakhiyev, D. N. Grozdanov, and N. A. Fedorov. "Determination of the response function of the NaI detector for g-quanta with an energy of 4.43 MeV, formed during inelastic scattering of neutrons with an energy of 14.1 MeV on carbon nuclei." Eurasian Journal of Physics and Functional Materials 4, no. 4 (2020): 281–90. http://dx.doi.org/10.29317/ejpfm.2020040402.

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The work is devoted to determining the response function of the detector NaI(Tl) for g -quanta with energy of 4.43 MeV, formed during inelastic scattering of neutrons with energy of 14.1 MeV on the nuclei 12C. In gamma spectrometry, output pulses are recorded, the amplitudes of which are proportional to the energy lost in the detection medium by incident photons. One of the main tasks of radiation detection is to restore radiation characteristics from signals measured at the outputs of detectors. For this, it is necessary to know, first of all, the general characteristics of detectors as conve

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42

KWON, HEESUNG, NASSER M. NASRABADI, and PATTI GILLESPIE. "NONLINEAR CHEMICAL PLUME DETECTION USING KERNEL-BASED MATCHED SUBSPACE DETECTORS." International Journal of High Speed Electronics and Systems 17, no. 04 (2007): 813–26. http://dx.doi.org/10.1142/s0129156407005004.

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In this paper, we compare several detection algorithms that are based on spectral matched (subspace) filters. Nonlinear (kernel) versions of these spectral matched (subspace) detectors are also discussed and their performance is compared with the linear versions. These kernel-based detectors exploit the nonlinear correlations between the spectral bands that are ignored by the conventional detectors. Several well-known matched detectors, such as matched subspace detector, orthogonal subspace detector, spectral matched filter and adaptive subspace detector (adaptive cosine estimator) are extende

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43

Eftekhari Zadeh, E., S. A. H. Feghhi, E. Bayat, and G. H. Roshani. "Gaussian Energy Broadening Function of an HPGe Detector in the Range of 40 keV to 1.46 MeV." Journal of Experimental Physics 2014 (October 7, 2014): 1–4. http://dx.doi.org/10.1155/2014/623683.

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High-purity germanium (HPGe) detectors are widely used in nuclear spectroscopy (e.g., neutron activation analysis) due to their high resolution. Resolution function of a GMX series coaxial detector system (model number GMX40P4-83) in the range of 40 keV to 1.46 MeV has been measured using standard γ-ray sources. The energy response function also was calculated using Monte Carlo simulation through the precise modeling of the detector structure. The simulated energy response function was verified with the measured energy response function obtained using calibration sources. A new approach was us

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44

Kuleshov, D. O., V. A. Simonyan, A. A. Bogdanov, et al. "Measurement of the photon detection efficiency of silicon photomultipliers for the new detector cluster of the Cherenkov gamma-ray telescope TAIGA-IACT equipped with UV filters." Journal of Physics: Conference Series 2103, no. 1 (2021): 012036. http://dx.doi.org/10.1088/1742-6596/2103/1/012036.

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Abstract This study was devoted to measurements of the UV-range photon detection efficiency (PDE) of OnSemi MicroFJ SiPM detectors use together with custom UV filters and of the transmission coefficient of these filters at 277 nm. The final goal of these measurements was to determine feasibility of the filters for the new detector cluster of the TAIGA-IACT telescope. PicoQuant PLS-270 UV source emitting pulses at 277 nm was calibrated. The obtained dependences of the registered radiation power on the distance between the emission source and the reference detector are well approximated by the i

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45

Nakaye, Yasukazu, Takuto Sakumura, Yasutaka Sakuma, et al. "Characterization and performance evaluation of the XSPA-500k detector using synchrotron radiation." Journal of Synchrotron Radiation 28, no. 2 (2021): 439–47. http://dx.doi.org/10.1107/s1600577520016665.

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Hybrid photon counting (HPC) detectors are widely used at both synchrotron facilities and in-house laboratories. The features of HPC detectors, such as no readout noise, high dynamic range, high frame rate, excellent point spread function, no blurring etc. along with fast data acquisition, provide a high-performance detector with a low detection limit and high sensitivity. Several HPC detector systems have been developed around the world. A number of them are commercially available and used in academia and industry. One of the important features of an HPC detector is a fast readout speed. Most

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Kushoro, Matteo Hakeem, Marica Rebai, Marco Tardocchi, et al. "Detector Response to D-D Neutrons and Stability Measurements with 4H Silicon Carbide Detectors." Materials 14, no. 3 (2021): 568. http://dx.doi.org/10.3390/ma14030568.

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The use of wide-band-gap solid-state neutron detectors is expanding in environments where a compact size and high radiation hardness are needed, such as spallation neutron sources and next-generation fusion machines. Silicon carbide is a very promising material for use as a neutron detector in these fields because of its high resistance to radiation, fast response time, stability and good energy resolution. In this paper, measurements were performed with neutrons from the ISIS spallation source with two different silicon carbide detectors together with stability measurements performed in a lab

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Chesi, Giovanni, Alessia Allevi, and Maria Bondani. "Autocorrelation functions: a useful tool for both state and detector characterisation." Quantum Measurements and Quantum Metrology 6, no. 1 (2019): 1–6. http://dx.doi.org/10.1515/qmetro-2019-0001.

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Abstract The calculation of autocorrelation functions represents a routinely used tool to characterise quantum states of light. In this paper, we evaluate the g(2) function for detected photons in the case of mesoscopic multi-mode twin-beam states in order to fully investigate their statistical properties starting from measurable quantities. Moreover, we show that the second-order autocorrelation function is also useful to estimate the spurious effects affecting the employed Silicon-photomultiplier detectors.

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Gianvecchio’, Alberto. "Synthetic data for the study of the CUORE detector response function." Journal of Physics: Conference Series 2156, no. 1 (2021): 012222. http://dx.doi.org/10.1088/1742-6596/2156/1/012222.

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Abstract CUORE (Cryogenic Underground Observatory for Rare Events) is a ton-scale experiment located at LNGS (Laboratori Nazionali del Gran Sasso) in Italy whose goal is to search for neutrino-less double beta decay (0υββ) in 130Te. CUORE exploits an array of 988 TeO2 crystals operated as Low-Temperature Detectors (LTDs) at 10 mK. These detectors show an excellent energy resolution, making the experiment one of the most competitive 0υββ searches in the world. In this scenario, the proposed research deals with the generation of synthetic (mock) data for the study of the CUORE detector response

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NIU Jin, 牛津, 王劲松 WANG Jinsong, 安志勇 AN Zhiyong, and 杨海凝 YANG Haining. "Optical System Design of the Optical Multifunction Detector." ACTA PHOTONICA SINICA 42, no. 12 (2013): 1507–13. http://dx.doi.org/10.3788/gzxb20134212.1507.

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Zuo, Lei, Ming Li, Xiaowei Zhang, Yunlong Lu, and Yan Wu. "Range‐spread target detector using the frequency rate function." IET Radar, Sonar & Navigation 8, no. 7 (2014): 749–56. http://dx.doi.org/10.1049/iet-rsn.2013.0129.

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