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1

Metwally, Walid A. "Existing NaI detectors; an efficient alternative to He-3 detectors." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 338 (November 2014): 48–51. http://dx.doi.org/10.1016/j.nimb.2014.08.001.

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2

Glesius, F., and T. Kniss. "He/sup 3/ neutron detectors for hostile environments." IEEE Transactions on Nuclear Science 35, no. 1 (1988): 867–71. http://dx.doi.org/10.1109/23.12849.

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3

Rees, Lawrence B., and J. Bart Czirr. "Optimizing moderation of He-3 neutron detectors for shielded fission sources." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 691 (November 2012): 72–80. http://dx.doi.org/10.1016/j.nima.2012.07.004.

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4

Manolopoulou, M., M. Fragopoulou, S. Stoulos, S. Petalas, and M. Zamani. "Monte Carlo calculation of the response of He-3 counter with Geant4." HNPS Proceedings 14 (December 5, 2019): 161. http://dx.doi.org/10.12681/hnps.2266.

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Monte Carlo calculations with Geant4 were performed to calculate the response of He-3 proportional counters for neutrons of the energy region of 230 keV – 7 MeV. The results are compared with experimental data obtained by irradiation of the detectors with monoenergetic neutron beams produced by 7Li(p,n)7Be and 2H(d,n)3He reactions in the Tandem accelerator, NSCR Demokritos Athens.
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5

Jia, Tao, Chao Wan, Limin Zhao, et al. "Temperature dependence of niobium superconducting nanowire single-photon detectors in He-3 cryocooler." Chinese Science Bulletin 59, no. 28 (2014): 3549–53. http://dx.doi.org/10.1007/s11434-014-0538-5.

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6

ALBERTINI, G., V. CALBUCCI, F. CARDONE, et al. "EVIDENCE OF ALPHA EMISSION FROM COMPRESSED STEEL BARS." International Journal of Modern Physics B 27, no. 23 (2013): 1350124. http://dx.doi.org/10.1142/s0217979213501245.

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Four cylindrical steel bars of 2 cm diameter and 20 cm height were subjected to compression cycles each of them consisting of a loading phase at fixed stress rate followed by a rapid stress release. Different compression rates were used for the same sample. The area surrounding the loaded samples was monitored in order to check whether ionizing particles were emitted. To this aim, three ZnS(Ag) detectors, a Geiger counter, and some polycarbonate CR39 detectors of alpha particles were used. An 3 He proportional detector of neutrons was also used. The whole set of results is discussed and propos
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7

Pappalardo, A., C. Vasi, and P. Finocchiaro. "Direct comparison between solid state Silicon+ 6 LiF and 3 He gas tube neutron detectors." Results in Physics 6 (2016): 12–13. http://dx.doi.org/10.1016/j.rinp.2015.11.012.

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8

Kashchuk, A. P., and O. V. Levitskaya. "Position-Sensitive Thermal and Cold Neutron Detectors with $$_{2}^{3}{\text{He}}$$ Gas Converter (Review)." Technical Physics 65, no. 4 (2020): 493–513. http://dx.doi.org/10.1134/s1063784220040118.

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9

NAKAE, L. F., G. F. CHAPLINE, A. M. GLENN, et al. "THE USE OF FAST NEUTRON DETECTION FOR MATERIALS ACCOUNTABILITY." International Journal of Modern Physics: Conference Series 27 (January 2014): 1460140. http://dx.doi.org/10.1142/s2010194514601409.

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For many years at LLNL, we have been developing time-correlated neutron detection techniques and algorithms for applications such as Arms Control, Threat Detection and Nuclear Material Assay. Many of our techniques have been developed specifically for the relatively low efficiency (a few percent) inherent in man-portable systems. Historically, thermal neutron detectors (mainly 3 He ) were used, taking advantage of the high thermal neutron interaction cross-sections, but more recently we have been investigating the use of fast neutron detection with liquid scintillators, inorganic crystals, and
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10

Ohzu, A., M. Takase, M. Haruyama, et al. "Numerical evaluation of the light transport properties of alternative He-3 neutron detectors using ceramic scintillators." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 798 (October 2015): 62–69. http://dx.doi.org/10.1016/j.nima.2015.07.020.

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11

Kifune, T. "The Prospects for Very High Energy Gamma Ray Astronomy." Australian Journal of Physics 48, no. 2 (1995): 305. http://dx.doi.org/10.1071/ph950305.

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Very-high-energy (VHE) gamma rays, with energies .<: 1 TeV = 1012 eV, are observed with ground-based telescopes using the atmospheric Cerenkov technique. This field of astronomy has recently experienced its coming of age, opening a new observational window on the universe after efforts spanning almost 30 years. Recent advances in this field have been aided by the results from satellite detectors with high-energy (HE) gamma ray 'eyes'. Satellite detectors are sensitive to HE gamma rays, up to energies of about 10 GeV = 1010 eV. In this paper, VHE gamma ray astronomy is reviewed, and the 3�8
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12

Nilsson, Jonas M. C., Robert R. Finck, and Christopher Rääf. "Investigation and optimisation of mobile NaI(Tl) and 3 He-based neutron detectors for finding point sources." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 786 (June 2015): 127–34. http://dx.doi.org/10.1016/j.nima.2015.03.013.

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13

Leder, A., A. J. Anderson, J. Billard, et al. "Unfolding neutron spectrum with Markov Chain Monte Carlo at MIT research Reactor with He-3 Neutral Current Detectors." Journal of Instrumentation 13, no. 02 (2018): P02004. http://dx.doi.org/10.1088/1748-0221/13/02/p02004.

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14

Engels, R., G. Kemmerling, H. Rongen, J. Schelten, and R. Cooper. "Comparison of neutron scintillation detectors with a /sup 3/He proportional counter for the Spallation Neutron Source (SNS)." IEEE Transactions on Nuclear Science 49, no. 3 (2002): 923–25. http://dx.doi.org/10.1109/tns.2002.1039590.

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15

Nakamura, Tatsuya, and Kentaro Toh. "Development of Position-Sensitive Scintillator Detectors and a 3He Gas-Based Micro-Pixel Neutron Detector for J-PARC/MLF." hamon 19, no. 4 (2009): 207–13. http://dx.doi.org/10.5611/hamon.19.4_207.

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16

WUENSCHEK, B. K., H. BHANG, M. CARGNELLI, et al. "STATUS AND PLANS OF EXPERIMENT E17 AT J-PARC." International Journal of Modern Physics A 26, no. 03n04 (2011): 604–6. http://dx.doi.org/10.1142/s0217751x11052177.

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X-ray spectroscopy is an advantageous tool for investigation of the shift and width of the energy levels in kaonic atoms, evoked due to strong interaction between nucleus and kaon. In order to study the 2p level shift in kaonic 3 He , the X-ray transition 3 p →2 d in liquid kaonic 3 He will be measured with a precision of <2 eV in the E17 experiment at J-PARC. To reach this desired precision, a well designed setup, in-situ calibration and state-of-the-art semiconductor detectors will be used. The idea and the preparation status of the whole setup will be reported in this article.
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17

Gonnelli, E., L. N. Pinto, H. R. Landim, R. Diniz, R. Jerez, and A. dos Santos. "A Simple Way to Overcome the Shortage of $^{3}\rm {He}$ Detectors in the IPEN/MB-01 Nuclear Reactor." IEEE Transactions on Nuclear Science 63, no. 3 (2016): 1507–12. http://dx.doi.org/10.1109/tns.2016.2568241.

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18

HAYANO, RYUGO. "KAONIC HELIUM ATOMS." International Journal of Modern Physics A 24, no. 02n03 (2009): 183–89. http://dx.doi.org/10.1142/s0217751x09043468.

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The KEK experiment E570 has measured the Balmer-series x-rays of kaonic 4 He atoms using large-area silicon drift x-ray detectors (SDDs) in order to study the low-energy [Formula: see text]-nucleus strong interaction. The energy of the 3d → 2p transition was determined to be 6467 ± 3( stat ) ± 2( syst ) eV . The resulting strong-interaction energy-level shift is in agreement with theoretical calculations, thus eliminating a long-standing discrepancy between theory and experiment. Using a similar setup, the E17 experiment at J-PARC, the first experiment to be carried out in the hadron hall of J
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19

Birch, J., J. C. Buffet, J. Correa, et al. "$^{10}{\rm B}_{4}{\rm C}$ Multi-Grid as an Alternative to $^{3}{\rm He}$ for Large Area Neutron Detectors." IEEE Transactions on Nuclear Science 60, no. 2 (2013): 871–78. http://dx.doi.org/10.1109/tns.2012.2227798.

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20

HAYANO, RYUGO S., G. BEER, H. BHANG, et al. "SOLVING THE KAONIC-HELIUM PUZZLE." Modern Physics Letters A 23, no. 27n30 (2008): 2505–11. http://dx.doi.org/10.1142/s021773230802968x.

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We have measured the Balmer-series x-rays of kaonic 4 He atoms using large-area silicon drift x-ray detectors (SDDs) in order to study the low-energy [Formula: see text]-nucleus strong interaction. The energy of the 3d → 2p transition was determined to be 6467 ± 3( stat ) ± 2( syst ) eV . The resulting strong-interaction energy-level shift is in agreement with theoretical calculations, thus eliminating a long-standing discrepancy between theory and experiment.
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21

PYATKOV, Yu V., D. V. KAMANIN, A. A. ALEXANDROV, et al. "PRESUMABLE SCENARIO OF ONE OF THE COLLINEAR CLUSTER TRI-PARTITION MODES." International Journal of Modern Physics E 20, no. 04 (2011): 1008–11. http://dx.doi.org/10.1142/s0218301311019155.

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Collinear cluster tri-partition (CCT) channel in 252 Cf ( sf ) was studied using COMETA apparatus. The setup consists of a double arm time of flight heavy ion spectrometer with two mosaic "stop" detectors. Also included in the setup is a neutron registration channel based on 3 He filled counters. Specific CCT mode manifesting itself as a rectangular structure in the mass-mass plot of detected fragments was revealed both by neutron gating and direct detection of all three decay partners. Presumable scenario which stands behind the mode observed is discussed.
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22

DIOSZEGI, ISTVAN, GRAHAM C. SMITH, NEIL A. SCHAKNOWSKI, et al. "CODED APERTURE THERMAL NEUTRON CAMERA WITH ASIC-BASED PAD READOUT." International Journal of Modern Physics: Conference Series 27 (January 2014): 1460139. http://dx.doi.org/10.1142/s2010194514601392.

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A new generation of coded aperture neutron imagers is being developed at Brookhaven National Laboratory. The detector of the camera is a position sensitive thermal neutron chamber. The new device is a 3 He -filled ionization chamber, which uses only anode and cathode planes. The anode is composed of an array of individual pads. The charge is collected on each of the individual 5 × 5 mm2 anode pads, (48 × 48 in total corresponding to a 24 × 24 cm2 sensitive area) and read out by application specific integrated circuits. The new design has several advantages for the field of coded aperture appli
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23

Galitzki, Nicholas, Peter A. R. Ade, Francesco E. Angilè, et al. "The Next Generation BLAST Experiment." Journal of Astronomical Instrumentation 03, no. 02 (2014): 1440001. http://dx.doi.org/10.1142/s2251171714400017.

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The Balloon-borne Large Aperture Submillimeter Telescope for Polarimetry (BLASTPol) was a suborbital experiment designed to map magnetic fields in order to study their role in star formation processes. BLASTPol made detailed polarization maps of a number of molecular clouds during its successful flights from Antarctica in 2010 and 2012. We present the next-generation BLASTPol instrument (BLAST-TNG) that will build off the success of the previous experiment and continue its role as a unique instrument and a test bed for new technologies. With a 16-fold increase in mapping speed, BLAST-TNG will
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24

KESHELASHVILI, IRAKLI, DOMINIK WERTHMÜLLER та LILIAN WITTHAUER. "QUASI-FREE PHOTOPRODUCTION OF η-MESONS OFF 2H AND 3He". International Journal of Modern Physics: Conference Series 26 (січень 2014): 1460114. http://dx.doi.org/10.1142/s2010194514601148.

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In this work, we are presenting a combination of two preliminary results for quasi-free photoproduction of η-mesons from the liquid deuterium and 3 He targets for incident photon energies from threshold up to 1.4 GeV. The experiments were performed at the Mainz MAMI electron accelerator, using the Glasgow tagged photon facility. Decay photons of the η-mesons and the recoil nucleons were detected with an almost 4π covering electromagnetic calorimeter combining the Crystal Ball and TAPS detectors. The data from both targets show a narrow structure in the excitation function of γ + n → n + η. The
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25

Liu, D., and B. Wang. "The formation of single neutron stars from double white-dwarf mergers via accretion-induced collapse." Monthly Notices of the Royal Astronomical Society 494, no. 3 (2020): 3422–31. http://dx.doi.org/10.1093/mnras/staa963.

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ABSTRACT The merging of double white dwarfs (WDs) may produce the events of accretion-induced collapse (AIC) and form single neutron stars (NSs). Meanwhile, it is also notable that the recently proposed WD+He subgiant scenario has a significant contribution to the production of massive double WDs, in which the primary WD grows in mass by accreting He-rich material from a He subgiant companion. In this work, we aim to study the binary population synthesis (BPS) properties of AIC events from the double WD mergers by considering the classical scenarios and also the contribution of the WD+He subgi
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26

Alattar, Adnan, Ravi Sharma, and John Scriven. "A System for Mitigating the Problem of Deepfake News Videos Using Watermarking." Electronic Imaging 2020, no. 4 (2020): 117–1. http://dx.doi.org/10.2352/issn.2470-1173.2020.4.mwsf-117.

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This paper describes how watermarking technology can be used to prevent the proliferation of Deepfake news. In the proposed system, digital watermarks are embedded in the audio and video tracks of video clips of trusted news agencies at the time the videos are captured or before they are distributed. The watermarks are detected at the social media network’s portals, nodes, and back ends. The embedded watermark imparts a unique identifier to the video, that links it to a blockchain. The watermarks also allow video source tracking, integrity verification, and alteration localization. The waterma
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27

Sion, Edward M., and Ronald A. Downes. "HST FOS Observations of KPD0005+5106: A Subluminous WN-WC Descendant by Ongoing Mass Outflow?" Symposium - International Astronomical Union 155 (1993): 498. http://dx.doi.org/10.1017/s0074180900172316.

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We report the results of spectroscopic observations of the ultra-high excitation, helium-rich, pre-white dwarf KPD0005+5106 obtained with the Hubble Space Telescope Faint Object Spectrograph (FOS) in 1991 May and July with the red (FOS/RD) and blue (FOS/BL) Digicon detectors. The data reveal a rich line spectrum both in absorption and in emission with ultra-high excitation species present including O VIII, N V, possibly C V, Fe VI, Fe VII and numerous weaker high n, low l, transitions of C IV and O VI as well as the predominant He II (3 → n) and He II (Balmer α) absorption lines. There is a st
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28

Takahashi, A., H. Miyamaru, and K. Ochiai. "Search for Enhanced D+D+D Reactions under D+ Beam Irradiation into TiDx Targets." Solid State Phenomena 107 (October 2005): 55–58. http://dx.doi.org/10.4028/www.scientific.net/ssp.107.55.

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To search possible enhancement of three-body D+D+D fusion reaction in condensed matter, we have studied for 10 years about emitted charged particle spectra from titanium-deuterate (TiDx) samples under low energy D+ beam irradiation. By gas loading technique with changing temperature, we prepared TiDx samples with x = 1.4 - 1.8. A TiDx sample was mounted in a vacuum chamber with cooling and irradiated with 70 – 300 keV D+ beam. A delta-E and E type counter telescope using two Si-SSD detectors was used for charged particle spectroscopy. Charged particles from D+D fusion reactions, e.g., 3MeV pro
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29

Piscitelli, F., A. Khaplanov, A. Devishvili, et al. "Neutron reflectometry on highly absorbing films and its application to 10 B 4 C-based neutron detectors." Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences 472, no. 2185 (2016): 20150711. http://dx.doi.org/10.1098/rspa.2015.0711.

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Neutron reflectometry is a powerful tool used for studies of surfaces and interfaces. The absorption in the typical studied materials is neglected and this technique is limited only to the reflectivity measurement. For strongly absorbing nuclei, the absorption can be directly measured by using the neutron-induced fluorescence technique which exploits the prompt particle emission of absorbing isotopes. This technique is emerging from soft matter and biology where highly absorbing nuclei, in very small quantities, are used as a label for buried layers. Nowadays, the importance of absorbing layer
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30

Barioglio, Luca. "Anti- and Hyper-Nuclei Production at the LHC with ALICE." Proceedings 10, no. 1 (2019): 47. http://dx.doi.org/10.3390/proceedings2019010047.

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At the Large Hadron Collider (LHC) a significant production of (anti-)(hyper-)nuclei is observed in proton-proton (pp), proton-lead (p-Pb) and lead-lead (Pb-Pb) collisions. The measurement of the production yields of light (anti-)nuclei is extremely important to provide insight into the production mechanisms of nuclear matter, which is still an open question in high energy physics. The outstanding particle identification (PID) capabilities of the ALICE detectors allow the identification of rarely produced particles such as deuterons, 3 He and their antiparticles. From the production spectra me
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31

Roy, Federico A., Perk Lin Chong, and Sor Heoh Saw. "Correlation of measured neon soft X-ray pulses of the INTI plasma focus with the reflected shock phase at 12KV." International Journal of Modern Physics: Conference Series 32 (January 2014): 1460327. http://dx.doi.org/10.1142/s2010194514603275.

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The six-phase Lee Model Code is used to fit the computed current waveform to the measured waveform of the INTI Plasma Focus (PF;2.2 kJ at 12 kV), a T2 PF device, operated as a source of Neon soft X-ray (SXR) with optimum yield around 2.5 - 3 Torr of neon. The characteristic He-like and H-like neon line SXR pulse is measured using a pair of SXR detectors with selected filters that, by subtraction, have a photon energy window of 900 to 1550 eV covering the region of the characteristic neon SXR lines. The aim of this paper is to investigate the correlation between the time histories of the measur
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32

Claps, G., F. Murtas, A. Pietropaolo, et al. "3 He-free triple GEM thermal neutron detector." EPL (Europhysics Letters) 105, no. 2 (2014): 22002. http://dx.doi.org/10.1209/0295-5075/105/22002.

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33

Koizumi, Mitsuo, Kaoru Sakasai, Masatoshi Kureta, and Hironobu Nakamura. "Development of alternative 3He NDA detector system." Journal of the Atomic Energy Society of Japan 58, no. 11 (2016): 642–46. http://dx.doi.org/10.3327/jaesjb.58.11_642.

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34

Sjoden, G. E. "Deterministic adjoint transport applications for He-3 neutron detector design." Annals of Nuclear Energy 29, no. 9 (2002): 1055–71. http://dx.doi.org/10.1016/s0306-4549(01)00096-2.

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35

Barquist, C. S., P. Zheng, W. G. Jiang, et al. "Development of a Spatially Resolved $$^3$$He Quasi-Particle Detector." Journal of Low Temperature Physics 183, no. 3-4 (2015): 307–12. http://dx.doi.org/10.1007/s10909-015-1371-1.

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36

Ahlstrom, S. L., D. I. Bradley, S. N. Fisher, et al. "A Quasiparticle Detector for Imaging Quantum Turbulence in Superfluid $$^3$$ 3 He-B." Journal of Low Temperature Physics 175, no. 5-6 (2014): 725–38. http://dx.doi.org/10.1007/s10909-014-1144-2.

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37

Mazzone, A., P. Finocchiaro, S. Lo Meo, and N. Colonna. "GEANT4 simulations of a novel 3 He-free thermalization neutron detector." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 889 (May 2018): 33–38. http://dx.doi.org/10.1016/j.nima.2018.02.011.

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38

Akyurek, T., L. P. Tucker, X. Liu, and S. Usman. "Portable spectroscopic fast neutron probe and 3 He detector dead-time measurements." Progress in Nuclear Energy 92 (September 2016): 15–21. http://dx.doi.org/10.1016/j.pnucene.2016.06.007.

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39

Mathis, G. L. "The effect of thermal neutron temperature upon /sup 3/He detector response." IEEE Transactions on Nuclear Science 36, no. 1 (1989): 1182–84. http://dx.doi.org/10.1109/23.34628.

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40

Oliva, Alberto. "Observation of Properties of Primary and Secondary Cosmic Rays by the Alpha Magnetic Spectrometer on the International Space Station." EPJ Web of Conferences 208 (2019): 13002. http://dx.doi.org/10.1051/epjconf/201920813002.

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The Alpha Magnetic Spectrometer (AMS-02) is a wide acceptance high-energy physics experiment installed on the International Space Station in May 2011 and operating continuously since then. With a collection rate of approximately 1.7 × 1010 events/year, and the combined identification capabilities of 5 independent detectors, AMS-02 is able to precisely separate cosmic rays light nuclei (1 ≤ Z ≤ 8). Knowledge of the precise rigidity dependence of the light nuclei fluxes is important in understanding the origin, acceleration, and propagation of cosmic rays. AMS-02 collaboration has recently relea
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41

King, Michael J., Tsahi Gozani, Robert Benetti, Donald B. Hilliard, and Bryan Benetti. "Development of a Portable $^{10}{\hbox{B}}$-Based $^{3}{\hbox{He}}$ Replacement Neutron Detector." IEEE Transactions on Nuclear Science 60, no. 2 (2013): 885–89. http://dx.doi.org/10.1109/tns.2013.2246579.

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42

Dubouloz, N., J. J. Berthelier, M. Malingre, et al. "Thermal ion measurements on board Interball Auroral Probe by the Hyperboloid experiment." Annales Geophysicae 16, no. 9 (1998): 1070–85. http://dx.doi.org/10.1007/s00585-998-1070-1.

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Abstract. Hyperboloid is a multi-directional mass spectrometer measuring ion distribution functions in the auroral and polar magnetosphere of the Earth in the thermal and suprathermal energy range. The instrument encompasses two analyzers containing a total of 26 entrance windows, and viewing in two almost mutually perpendicular half-planes. The nominal angular resolution is defined by the field of view of individual windows ≈13° × 12.5°. Energy analysis is performed using spherical electrostatic analyzers providing differential measurements between 1 and 80 eV. An ion beam emitter (RON experi
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43

Wu, Xiao-guang, Yu-bin Zhao, Hong Luo, et al. "Test of a $$^{3}$$He neutron detector readout electronics prototype for CSNS multipurpose physics neutron diffractometer." Radiation Detection Technology and Methods 5, no. 2 (2021): 200–206. http://dx.doi.org/10.1007/s41605-020-00235-4.

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44

Ильясова, М. В., А. Е. Шевелев, Е. М. Хилькевич та ін. "Измерения спектров гамма- и нейтронного излучения в ядерных реакциях с ионами -=SUP=-3-=/SUP=-He и -=SUP=-9-=/SUP=-Be". Письма в журнал технической физики 47, № 3 (2021): 3. http://dx.doi.org/10.21883/pjtf.2021.03.50565.18518.

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The results of the measurements of the neutron and gamma radiation produced in the 9 Be( 3 He,pγ) 11 B and 9 Be( 3 He,nγ) 11 C nuclear reaction at the 2.57 MeV energy of the 3 He ions are represented. The measurements were carried out with organic scintillation detector BC-501A and semiconductor HPGe spectrometers. Gamma-ray spectra were measured at 0°, 30°, 60°, 90° and 120° angles. The shapes of the gamma lines 6.9 MeV from the 9 Be( 3 He,nγ) 11 C reaction and 8.92 MeV from the 9 Be( 3 He,nγ) 11 C were obtained. The angular distribution of protons populating the 8.92 MeV energy level of the
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45

Jha, V., A. Budzanowski, A. Chatterjee та ін. "SEARCH FOR η-NUCLEUS BOUND STATE AT COSY". International Journal of Modern Physics A 22, № 02n03 (2007): 596–99. http://dx.doi.org/10.1142/s0217751x07035914.

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An experiment to search for the bound state of η meson in nuclei has been performed at COSY, Juelich using the ENSTAR detector and Big Karl magnetic spectrometer. Reaction (p,3 He ) on 27 Al target has been used to search for the η-mesic nucleus 25 Mg η in the missing mass distribution from the measured 3 He particles. A preliminary figure of 1.5 nb for the upper limit of the formation cross section of η-nucleus bound state has been determined.
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46

KOHNO, Masuchika, Koji YOSHIDA, Kimikazu MORITANI, et al. "Continuous Background Originated From Neutrons By 65Cu(p,n)65Zn Under 4 MeV Protons — A problem on detecting trace elements in old copper alloys by PIXE." International Journal of PIXE 08, no. 02n03 (1998): 175–83. http://dx.doi.org/10.1142/s0129083598000212.

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EDS-PIXE is a very useful and easy method for detecting trace elements in ancient materials. However, relatively high continuous background is observed, when old copper alloys are measured under 4 MeV protons. The background makes the detection limits of trace metallic elements such as Au , Ag , As , Sn , Sb and Pb in these alloys worse. The cause of the high background was investigated using a Si ( Li ) detector, a pure- Ge detector and a 3 He neutron counter, and it was found that the continuous background level is correlated with the amount of neutron released from 65 Cu ( p , n )65 Zn reac
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47

Privezentsev, Vladimir. "Optical and TEM characterization of phase transformation in Zn ion implanted and thermal oxidized quartz." Annales Universitatis Mariae Curie-Sklodowska, sectio AAA – Physica 71 (February 23, 2017): 71. http://dx.doi.org/10.17951/aaa.2016.71.71.

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<table class="data" width="100%"><tbody><tr valign="top"><td class="value"><p>Metal and metal oxide nanoparticles (NPs) embedded in various matrices have been the object of increasing interest due to their peculiar physical properties significantly different from the corresponding ones of bulk material. Metallic Zn NPs can be used in UV photo-detectors. Zinc oxide NPs play an important role too, since ZnO has direct band gap of 3.37eV, large exiton binding energy of 60meV, sorption effect, room temperature ferromagnetism and others. So they can be used in varies p
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48

KUPSC, ANDRZEJ. "RECENT RESULTS FROM THE WASA-at-COSY EXPERIMENT: LIGHT MESON DECAYS." International Journal of Modern Physics A 26, no. 03n04 (2011): 474–79. http://dx.doi.org/10.1142/s0217751x11051858.

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Studies of light meson decays are the key experiments for the WASA detector at COSY-Jülich. One of the world largest data samples of the η meson decays have been recently collected in the pd →3 He η and in the pp → ppη reactions. The status of the analysis of various decay channels and the further plans for the light meson decay program are presented.
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49

Calzolari, Gabriele, Alexis K. Ault, Greg Hirth, and Robert G. McDermott. "Hematite (U-Th)/He thermochronometry detects asperity flash heating during laboratory earthquakes." Geology 48, no. 5 (2020): 514–18. http://dx.doi.org/10.1130/g46965.1.

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Abstract Evidence for coseismic temperature rise that induces dynamic weakening is challenging to directly observe and quantify in natural and experimental fault rocks. Hematite (U-Th)/He (hematite He) thermochronometry may serve as a fault-slip thermometer, sensitive to transient high temperatures associated with earthquakes. We test this hypothesis with hematite deformation experiments at seismic slip rates, using a rotary-shear geometry with an annular ring of silicon carbide (SiC) sliding against a specular hematite slab. Hematite is characterized before and after sliding via textural and
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Zhu, Jin Tao, Guo Fu Liu, Jun Yang, and Lei Zhang. "Simulation Research of Charged Particle Discrimination Methods." Applied Mechanics and Materials 568-570 (June 2014): 146–51. http://dx.doi.org/10.4028/www.scientific.net/amm.568-570.146.

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A simple model was used to simulate the current pulse induced by charged particles with Si detector. With simulated current shapes of three element groups, H/D/T (6MeV), He-3/He-4 (15MeV) and Li-6/Li-7 (35MeV), three methods of pulse shape analysis (PSA), i.e. the m2-m3 method, the integration method and the second moment method, were compared and analyzed. Their discrimination performance and noise resisting property are investigated. The results show that the charge integration method and the m2-m3 method both have good discrimination performance and noise resisting property. While neither t
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