Academic literature on the topic 'GAMMA-400'

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Journal articles on the topic "GAMMA-400"

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Galper, A. M., N. P. Topchiev, and Yu T. Yurkin. "GAMMA-400 Project." Astronomy Reports 62, no. 12 (December 2018): 882–89. http://dx.doi.org/10.1134/s1063772918120223.

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Topchiev, N. P., A. M. Galper, V. Bonvicini, O. Adriani, R. L. Aptekar, I. V. Arkhangelskaja, A. I. Arkhangelskiy, et al. "The GAMMA-400 gamma-ray telescope for precision gamma-ray emission investigations." Journal of Physics: Conference Series 675, no. 3 (February 5, 2016): 032009. http://dx.doi.org/10.1088/1742-6596/675/3/032009.

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Arkhangelskiy, A. I., I. V. Arkhangelskaja, M. D. Kheymits, M. F. Runtso, S. I. Suchkov, N. P. Topchiev, and Yu T. Yurkin. "The Prototype of GAMMA-400 Apparatus." Physics Procedia 74 (2015): 191–98. http://dx.doi.org/10.1016/j.phpro.2015.09.187.

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Galper, A. M., O. Adriani, R. L. Aptekar, I. V. Arkhangelskaja, A. I. Arkhangelskiy, M. Boezio, V. Bonvicini, et al. "Status of the GAMMA-400 project." Advances in Space Research 51, no. 2 (January 2013): 297–300. http://dx.doi.org/10.1016/j.asr.2012.01.019.

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Topchiev, N. P., A. M. Galper, I. V. Arkhangelskaja, A. I. Arkhangelskiy, A. V. Bakaldin, I. V. Chernysheva, O. D. Dalkarov, et al. "High-energy gamma- and cosmic-ray observations with future space-based GAMMA-400 gamma-ray telescope." EPJ Web of Conferences 208 (2019): 14004. http://dx.doi.org/10.1051/epjconf/201920814004.

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The future space-based GAMMA-400 gamma-ray telescope will be installed on the Navigator platform of the Russian Astrophysical Observatory. A highly elliptical orbit will provide observations for 7-10 years of many regions of the celestial sphere continuously for a long time (~ 100 days). GAMMA-400 will measure gamma-ray fluxes in the energy range from ~ 20 MeV to several TeV and electron + positron fluxes up to ~ 20 TeV. GAMMA-400 will have an excellent separation of gamma rays from the background of cosmic rays and electrons + positrons from protons and an unprecedented angular (~ 0.01° at Eγ = 100 GeV) and energy (~ 1% at Eγ = 100 GeV) resolutions better than for Fermi-LAT, as well as ground-based facilities, by a factor of 5-10. Observations of GAMMA-400 will provide new fundamental data on discrete sources and spectra of gamma-ray emission and electrons + positrons, as well as the nature of dark matter.
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Egorov, Andrey E., Nikolay P. Topchiev, Arkadiy M. Galper, Oleg D. Dalkarov, Alexey A. Leonov, Sergey I. Suchkov, and Yuriy T. Yurkin. "Dark matter searches by the planned gamma-ray telescope GAMMA-400." Journal of Cosmology and Astroparticle Physics 2020, no. 11 (November 24, 2020): 049. http://dx.doi.org/10.1088/1475-7516/2020/11/049.

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Mikhailova, A. V., A. V. Bakaldin, I. V. Chernysheva, A. M. Galper, M. D. Kheymits, A. A. Leonov, A. G. Mayorov, et al. "Capabilities of the GAMMA-400 gamma-ray telescope for lateral aperture." Journal of Physics: Conference Series 1690 (December 2020): 012026. http://dx.doi.org/10.1088/1742-6596/1690/1/012026.

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Topchiev, N. P., A. M. Galper, V. Bonvicini, O. Adriani, I. V. Arkhangelskaja, A. I. Arkhangelskiy, A. V. Bakaldin, et al. "High-energy gamma-ray studying with GAMMA-400 after Fermi-LAT." Journal of Physics: Conference Series 798 (January 2017): 012011. http://dx.doi.org/10.1088/1742-6596/798/1/012011.

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Chasovikov, E. N., I. V. Arkhangelskaja, A. A. Perfil‘ev, A. I. Arkhangelskiy, A. M. Galper, N. P. Topchiev, Yu V. Gusakov, M. D. Kheymits, and Yu T. Yurkin. "GAMMA-400 Space Gamma-telescope Mathematical Model with Engineering Elements Included." Physics Procedia 74 (2015): 206–11. http://dx.doi.org/10.1016/j.phpro.2015.09.198.

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Topchiev, N. P., A. M. Galper, V. Bonvicini, O. Adriani, R. L. Aptekar, I. V. Arkhangelskaja, A. I. Arkhangelskiy, et al. "The GAMMA-400 experiment: Status and prospects." Bulletin of the Russian Academy of Sciences: Physics 79, no. 3 (March 2015): 417–20. http://dx.doi.org/10.3103/s1062873815030429.

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Dissertations / Theses on the topic "GAMMA-400"

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Cumani, Paolo. "Analysis and estimation of the scientific performance of the GAMMA-400 experiment." Doctoral thesis, Università degli studi di Trieste, 2015. http://hdl.handle.net/10077/10888.

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2013/2014
Per uno studio completo che parte dalla materia oscura e va all'origine e propagazione dei raggi cosmici, quello multi canale è uno degli approcci migliori per risolvere i quesiti irrisolti della fisica delle astroparticelle. GAMMA-400, grazie alla sua natura duale, dedita allo studio di raggi cosmici (elettroni fino alle energie del TeV e protoni e nuclei fino a 10^{15}-10^{16} eV) e raggi gamma (da 50 MeV fino a qualche TeV), si dedicherà allo studio di questi problemi. Lo scopo di questa tesi è lo studio delle prestazioni di GAMMA-400 per l'osservazione dei raggi gamma. Due diverse configurazioni della geometria sono state studiate: la "baseline" e la cosiddetta configurazione "enhanced". Le principali differenze tra queste due configurazioni si trovano nel tracciatore e nel calorimetro. Il tracciatore della "baseline" è composto da dieci piani di silicio, otto dei quali comprendono anche uno strato di ~0.1 X_0 di tungsteno. Il tracciatore della configurazione "enhanced" è invece composto da 25 piani di silicio inframezzati da uno strato di tungsteno di ~0.03 X_0. Il calorimetro della "baseline" è diviso in due sezioni: una parte composta da due piani di ioduro di cesio e silicio (chiamata "pre-shower") e una seconda parte composta da 28x28x12 cubi di ioduro di cesio. Il calorimetro della configurazione "enhanced" è invece composto solo da 20x20x20 cubi di ioduro di cesio. Per stimare le prestazioni ho sviluppato un algoritmo di ricostruzione della direzione del raggio gamma incidente. La ricostruzione può fare uso delle informazioni provenienti dal tracciatore, dal "pre-shower" o dal calorimetro, sia combinandole che singolarmente. Le direzioni ottenuta grazie alle informazioni del solo "pre-shower" o del solo calorimetro, anche se di minor risoluzione, possono essere utili per aumentare il numero di fotoni visti ad alta energia e per fornire le informazioni necessarie all'osservazione di transienti con i telescopi Cherenkov a terra. La risoluzione angolare utilizzando il tracciatore è migliore nel caso della configurazione "enhanced". A basse energie ciò è possibile grazie al minore tungsteno, e di conseguenza minor "scattering" multiplo, presente all'interno del tracciatore. Il calorimetro più piccolo, e più profondo, seppur ostacolando la ricostruzione dell'energia di fotoni ad alta energia, produce anche un numero minore di particelle di "backsplash" che peggiorano la ricostruzione delle tracce. L'area efficace totale della "baseline", potendo contare su un calorimetro più grande ed il "pre-shower", è più grande rispetto alla configurazione "enhanced". La risoluzione angolare, l'area efficace e la strategia di osservazione dello strumento contribuiscono alla sensitività per sorgenti puntiformi. La sensitività totale dello strumento è migliore per la "baseline" per energie maggiori di 5 GeV. Ho implementato un set prelminare di condizioni di "trigger" per lo studio dei raggi gamma tramite l'utilizzo delle informazioni del tracciatore. La necessità di rigettare la maggior parte delle particelle cariche deriva dall'elevato fondo presente in orbita (~10^6 protoni per raggio gamma) e una capacità di "downlink" limitata (~100 GB/day). Tra le due configurazioni si nota una differenza di meno dell'1% nel numero rimanente di protoni. Seppur promettente, tale risultato deve essere migliorato e possibili miglioramenti sono descritti nella tesi. Gli algoritmi di ricostruzione e "trigger" sono applicati all'analisi della possibilità di studiare "gamma-ray burst" (GRB) con la principale strumentazione a bordo di GAMMA-400. Una stima del numero di eventi non ricostruiti, perchè avvengono nel tempo morto tra due "trigger", è effettuata tramite la simulazione di un ipotetico GRB accoppiata ai tempi di arrivo dei fotoni presi dai dati reali di due GRB osservati da Fermi. In nessuna delle due configurazioni è visibile una percentuale significativa di "pile-up". Anche aumentando il flusso dei GRB la percentuale di eventi non ricostruiti non supera mai il 6%. Nonostante questo risultato, molto dipenderà dal disegno finale dell’elettronica di lettura dei rivelatori che potrebbe aumentare i tempi morti dello strumento.
XXVII Ciclo
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Nakauchi, Daisuke. "Gamma-Ray Bursts from First Stars and Ultra-Long Gamma-Ray Bursts." 京都大学 (Kyoto University), 2015. http://hdl.handle.net/2433/199100.

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Komura, Shotaro. "Imaging Polarimeter for a Sub-MeV Gamma-Ray All-sky Survey Using an Electron-tracking Compton Camera." Kyoto University, 2018. http://hdl.handle.net/2433/230989.

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Sawano, Tatsuya. "Simulation Study on an Electron-Tracking Compton Camera for Deep Gamma-ray Burst Search." 京都大学 (Kyoto University), 2017. http://hdl.handle.net/2433/225397.

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Hotokezaka, Kenta. "Theoretical study of signals from binary neutron star mergers." 京都大学 (Kyoto University), 2014. http://hdl.handle.net/2433/188486.

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Hayakawa, Tomoyasu. "Black-Hole forming Supernovae." Kyoto University, 2020. http://hdl.handle.net/2433/253091.

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Fujibayashi, Sho. "Properties of the Ejecta from Binary Neutron Star Merger Remnants and Implications for the Electromagnetic Signal Associated with GW170817." Kyoto University, 2018. http://hdl.handle.net/2433/232244.

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Yamazaki, Ryo. "Toward the Unified Theory of Long and Short Gamma-Ray Bursts, X-Ray Rich Gamma-Ray Bursts, and X-Ray Flashes." 京都大学 (Kyoto University), 2004. http://hdl.handle.net/2433/147812.

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Ioka, Kunihito. "Relativistic jets from magnetars towards understanding Gamma-Ray Bursts." 京都大学 (Kyoto University), 2001. http://hdl.handle.net/2433/150815.

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Aoi, Junichi. "Exploring the Gamma Ray Bursts from GeV-TeV spectra." 京都大学 (Kyoto University), 2011. http://hdl.handle.net/2433/142363.

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Book chapters on the topic "GAMMA-400"

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Hicks, K. H. "Spin-Observables for the $$(\vec{p},p'\gamma )$$ Reactions at 400 MeV." In Spin Observables of Nuclear Probes, 111–17. Boston, MA: Springer US, 1988. http://dx.doi.org/10.1007/978-1-4613-0769-3_9.

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Gehrels, Neil, and John K. Cannizzo. "Gamma-ray telescopes." In 400 Years of Astronomical Telescopes, 395–406. Dordrecht: Springer Netherlands, 2009. http://dx.doi.org/10.1007/978-90-481-2233-2_27.

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Pinkau, Klaus. "History of gamma-ray telescopes and astronomy." In 400 Years of Astronomical Telescopes, 155–69. Dordrecht: Springer Netherlands, 2009. http://dx.doi.org/10.1007/978-90-481-2233-2_11.

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Völk, Heinrich J., and Konrad Bernlöhr. "Imaging very high energy gamma-ray telescopes." In 400 Years of Astronomical Telescopes, 171–89. Dordrecht: Springer Netherlands, 2009. http://dx.doi.org/10.1007/978-90-481-2233-2_12.

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Fegan, D. J., M. F. Cawley, K. Gibbs, P. W. Gorham, R. C. Lamb, N. A. Porter, P. T. Reynolds, V. J. Stenger, and T. C. Weekes. "Search for a 12.59 ms. Pulsar in Cygnus X-3 at E > 400 GeV." In Very High Energy Gamma Ray Astronomy, 111–14. Dordrecht: Springer Netherlands, 1987. http://dx.doi.org/10.1007/978-94-009-3831-1_13.

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Begum, Shamsun Nahar, Mirza Mofazzal Islam, and Rigyan Gupta. "Development of the first kabuli type chickpea mutant variety in Bangladesh." In Mutation breeding, genetic diversity and crop adaptation to climate change, 203–8. Wallingford: CABI, 2021. http://dx.doi.org/10.1079/9781789249095.0020.

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Abstract Chickpea has a high yield potential, nutritional importance and diversity of use. A mutation breeding programme was undertaken at Bangladesh Institute of Nuclear Agriculture (BINA) with a view to developing early-maturing, large-seeded and high-yielding varieties of chickpea. Seeds of the popular chickpea variety 'Desi Binasola-2' were treated with different doses of gamma-rays (200, 300 and 400 Gy). The treated seeds were grown in batches according to dose for raising the M1 generation. M2 seeds were collected from individual M1 plants and subsequently grown in plant-progeny rows in the M2 generation and selections were made from the M2 families. Only 85 plants were selected from the M2 population and these were grown in the M3 generation. The mutant 'CPM-kabuli' and 28 other mutants were selected from M3 and were grown in the M4 generation. Only five mutants, including 'CPM-kabuli', were selected from M4 and were grown in M5. The selected mutant 'CPM-kabuli' along with check varieties were put into preliminary yield trials. Finally, the mutant lines were evaluated, with respect to two check varieties, in advanced, zonal-yield, on-farm and on-station trials in successive generations. All the selected mutant lines were grown at different locations in Bangladesh to observe the yield and other characteristics. The performance of the mutants was evaluated under two management practices: research management and farmers' management. Contrary to its parent, 'CPM-kabuli' was found to be tolerant to root rot and Botrytis grey mould, and also showed greater tolerance to pod borer insect-pest infestation than other mutants and check varieties. The main improved attributes are a cream seed coat colour, which reflects kabuli type, larger seed size and higher seed yield. The mutant 'CPM-kabuli' matures in the range of 115-125 days and is high yielding (1.7 t/ha). Considering all these, the bold Kabuli type chickpea mutant 'CPM-kabuli' was registered as the variety 'Binasola-9' for commercial cultivation during 2017 and is suitable for farmers in drought-prone areas in Bangladesh.
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Emery, K. O., and David Neev. "Climate Inferred from Geology and Archaeology." In The Destruction of Sodom, Gomorrah, and Jericho. Oxford University Press, 1995. http://dx.doi.org/10.1093/oso/9780195090949.003.0006.

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Early climatic interpretations for the Lisan and later formations (Late Pleistocene and Holocene—Neev and Emery, 1967, figs. 16, 17) were supported and updated by information from additional coreholes. Although most new and old coreholes bottomed at relatively shallow depths, 20 to 30 m, four of them reached greater depths, 74, 80, 161, and 285 m beneath the 1960 floor of the Dead Sea south basin. The sequences consist of alternating layers of marl and rocksalt. Most marls were deposited from dilute brine during high lake levels and contain alternating laminae of chemical deposits of white aragonite, gray gypsum, and fine-grained detritus consisting of yellowish, brown, green, or dark gray carbonates, quartz, and clay. The detrital fraction is coarser and more dominant toward the deltas, especially near Amazyahu escarpment in the south. Rocksalt layers indicate deposition from more concentrated brine when the levels dropped to about -400 m m.s.l. Lower elevations could have been reached when the sea continued to shrink and when the runoff-to-evaporation ratio diminished, bringing the south basin to complete dessication. As neither the geochemical nature (ionic ratios) of the brines nor the physiography of the terminal water body has changed at least since Late Pleistocene or Lisan Lake time (Katz, Kolodny, and Nissenbaum, 1977), it is probable that through the past 60,000 years rocksalt was precipitated only when the water surface was at or below the critical level of -400 m m.s.l. Gamma-ray logs for some of the new coreholes provide more objective and precise depths of marl and rocksalt layers than do actual samples of sediments. Content of radiogenic minerals in the rocksalt is negligible compared with that in the marl; thus, these layers identify changing physical environments and climates as well as correlating stratigraphy. On gamma-ray logs the peaks or highest intensities of positive anomalies indicate that marl layers or wet climatic subphases and their thicknesses on the logs are proportional to their duration. Presence of negative anomalies or very low levels of gamma radiation show both the existence and thickness of rocksalt layers that denote dry climatic phases.
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"Extended Compartmental Model." In Controlling Epidemics With Mathematical and Machine Learning Models, 96–118. IGI Global, 2022. http://dx.doi.org/10.4018/978-1-7998-8343-2.ch005.

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In this chapter, a new compartmental model that extends the classical SIR model by incorporating various infectious stages of the COVID-19 epidemic in Sultanate of Oman for a period of 145 days is presented. This incorporates the various stages of infection such as mildly infected, moderately infected, hospitalized, and critically infected. The transmission stage of the disease is categorized as pre-symptomatic transmission, asymptomatic transmission, and symptomatic transmission. The various transmission as well as transition parameters are estimated during the period from June 4th – October 26th, 2020 along with the pandemic size for a period of 400 days. Sensitivity analysis is performed on transition parameters and the parameter gamma due to the contact with the symptomatic moderately infected is found to be more significant in spreading the disease. As the value of basic reproduction number (R0) is 0.6088 during the period from June 8th – October 26th, 2020, the disease-free equilibrium is stable, and isolation and tracing the contact are suggested to control the spread of disease.
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"As mentioned in the previous chapter, many experiments on food irradiation in the 1950s were carried out with spent-fuel rods from nuclear reactors. Such fuel rods contain a mixture of many fission products, with greatly differing half-lives, emitting different types of radiation with different energies. The composition of fuel rods changes all the time because the radionuclides with short half-lives disappear quickly, whereas those with longer half-lives remain. Although fuel rods are primarily a source of gamma radiation (the less penetrating alpha and beta radiation are absorbed by the steel hull of the rods) they do give off some neutrons. Since the latter can produce radioactivity when they interact with matter such as food, fuel rods have not been used for irraditation of foods since the early 1960s. Because of their constantly varying composition, fuel rods also make dosimetry difficult, and this was another reason for abandoning their use. Individual constituents of spent fuel rods can be separated in reprocessing plants by chemical methods. One of the radionuclides obtainable in this way is Cs. With a half-life of 30 years and emission of gamma radiation (0.66 MeV) and beta radiation (0.51 MeV and 1.18 MeV), '^C s decays to stable '^B a (barium). After the ,37Cs is separated from the other constituents of the fission waste in the form of CsCl it is triply encapsulated in stainless steel containers because CsCl is soluble in water. If it leaked out it could cause contamination of the environment. As provided by the Waste Encapsulation and Storage Facility (WESF) at Hanford, Washington, the 137Cs capsule is 400 mm in active length (500 mm in total length) and 67 mm in diameter. There are only a few reprocessing plants in the world and the capacity for extracting ,37Cs from spent fuel rods is very limited. Plans for building several commercial reprocessing facilities in the United States were canceled by Presi­ dent Carter’s 1977 decision that the United States would not engage in commer­ cial reprocessing of spent nuclear fuel. As a consequence, not much ,37Cs is available and there are not many gamma radiation facilities which use ,Cs. No." In Safety of Irradiated Foods, 31. CRC Press, 1995. http://dx.doi.org/10.1201/9781482273168-23.

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"where K = kelvin. Because of the low temperature elevation in the low dose range, radiation calorimetry is limited in practice to the dose range above 3 kGy. This small temperature elevation is the gross result of the complex process of radiation interaction with matter. The individual steps of this process depend on the type of radiation used. Another type of physical dose meter, one that is used more and more in research and in industrial practice, is the alanine/electron spin resonance (ESR) system. Stable free radicals produced by irradiation in a concentration propor­ tional to the radiation dose in samples of pure, dry alanine are measured by ESR spectroscopy. The alanine is usually mixed 4:1 with paraffin (26) or 1:1 with polystyrene (27) of analytical grade quality. Reproducible dose response curves are obtained in the extremely wide dose range of 1 Gy to 100 kGy. In principal, any reproducible change caused by irradiation of a medium can be used to measure the absorbed radiation dose. In practice, only those changes can be evaluated which are stable for a reasonable length of time and which can be reliably measured by standard procedures such as titration or spectrophotometry. The chemical change is usually expressed as the G value, which is a measure of the number of atoms, molecules, or ions produced ( + G) or destroyed ( -G ) by 100 eV of absorbed energy. In the new SI system of units the G value is expressed as per J instead of per 100 eV. An important reference dose meter in food irradiation is the ferrous sulfate or Fricke dose meter. It is based on the radiation-induced oxidation of ferrous ions (Fe + ) to ferric ions (Fe + ) and consists of measuring the increased optical absorbance of the ferric ions at the absorption peak of 305 nm. For 60Co gamma rays the G value for ferric ion yield is 15.6 Fe3+ ions per 100 eV, or 9.74 X 1017 ions/J; the yield for electrons at a dose rate of 108 Gy/sec is 13.0. Fricke dosimetry is useful in the range 3 Gy. The upper limit can be extended into the kGy range by adding CuS04, which reduces the G value from 15.6 to 0.65. There are many other systems, such as the ethanol-chlorobenzene dose meter, which is based on the formation of hydrochloric acid from chlorobenzene. The hydrochloric acid can be measured by titration or by its effect on the dielectric constant. The useful dose range of this system is 1-400 Gy. In the low dose range, down to 5 Gy, radiochromic dye dosimetry can be used. When the colorless solution of pararosaniline cyanide in 2-methoxyethanol and glacial acetic acid is irradiated, an intense red color develops with an absorption maximum at 549 nm. More recently proposed methods belonging to the group of liquid dose meter systems are listed in Table 3. PMA (polymethyl methacrylate) dose meters belong to the group of solid phase dose meters. Irradiation of PMMA (e.g., Perspex) induces an absorption." In Safety of Irradiated Foods, 50. CRC Press, 1995. http://dx.doi.org/10.1201/9781482273168-39.

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Conference papers on the topic "GAMMA-400"

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Topchiev, Nikolay. "GAMMA-400 gamma-ray observatory." In The 34th International Cosmic Ray Conference. Trieste, Italy: Sissa Medialab, 2016. http://dx.doi.org/10.22323/1.236.1026.

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Topchiev, Nikolay, Arkadiy Galper, Valter Bonvicini, Irina Arkhangelskaja, Andrey Arkhangelskiy, Alexey Bakaldin, Sergey Bobkov, et al. "High-energy gamma-ray studying with GAMMA-400." In 35th International Cosmic Ray Conference. Trieste, Italy: Sissa Medialab, 2017. http://dx.doi.org/10.22323/1.301.0802.

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Bongi, M. "The GAMMA-400 Space Experiment." In International Conference on Advanced Technology and Particle Physics. WORLD SCIENTIFIC, 2014. http://dx.doi.org/10.1142/9789814603164_0003.

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Spillantini, P. "The Gamma-400 space mission." In 10th International Conference on Large Scale Applications and Radiation Hardness of Semiconductor Detectors. Trieste, Italy: Sissa Medialab, 2012. http://dx.doi.org/10.22323/1.143.0012.

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Leonov, A., A. M. Galper, Oscar Adriani, R. L. Aptekar, Irina Arkhangelskaja, Andrey Arkhangelskiy, S. G. Bobkov, et al. "The GAMMA-400 gamma-ray telescope characteristics. Angular resolution and electrons/protons separation." In Science with the New Generation of High Energy Gamma-ray experiments, 10th Workshop. Trieste, Italy: Sissa Medialab, 2015. http://dx.doi.org/10.22323/1.218.0008.

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Galper, A. M., O. Adriani, R. L. Aptekar, I. V. Arkhangelskaja, A. I. Arkhangelskiy, M. Boezio, V. Bonvicini, et al. "Design and performance of the GAMMA-400 gamma-ray telescope for dark matter searches." In CENTENARY SYMPOSIUM 2012: DISCOVERY OF COSMIC RAYS. AIP, 2013. http://dx.doi.org/10.1063/1.4792586.

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Topchiev, Nikolai P., Sergey I. Suchkov, Arkady M. Galper, Alexey A. Leonov, Yury T. Yurkin, Valter Bonvicini, and Oscar Adriani. "The GAMMA-400 space mission for measuring high-energy gamma rays and cosmic rays." In Proceedings of the MG14 Meeting on General Relativity. WORLD SCIENTIFIC, 2017. http://dx.doi.org/10.1142/9789813226609_0423.

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Bakaldin, Alexey, Sergey Bobkov, Oleg Serdin, Maxim S. Gorbunov, Andrey I. Arkhangelskiy, Alexey A. Leonov, and Nikolay Topchiev. "The high-performance data acquisition system for the GAMMA-400 satellite-borne gamma-ray telescope." In 35th International Cosmic Ray Conference. Trieste, Italy: Sissa Medialab, 2017. http://dx.doi.org/10.22323/1.301.0810.

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Runtso, Mikhail, Irina Arkhangelskaja, Andrey Arkhangelskiy, A. M. Galper, Maxim Kheymits, V. A. Kaplin, A. Leonov, et al. "Implementation of silicon photomultipliers in scintillation detector systems of the GAMMA-400 space gamma-ray telescope." In International Conference on New Photo-detectors. Trieste, Italy: Sissa Medialab, 2016. http://dx.doi.org/10.22323/1.252.0008.

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Mikhailov, Vladimir, A. M. Galper, N. P. Topchiev, I. V. Arkhangelskaja, A. I. Arkhangelskiy, A. V. Bakaldin, I. V. Chernysheva, et al. "Capabilities of the GAMMA-400 gamma-ray telescope to detect electron + positron flux at TeV-energies from lateral directions." In 27th European Cosmic Ray Symposium. Trieste, Italy: Sissa Medialab, 2023. http://dx.doi.org/10.22323/1.423.0155.

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