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  1. 1161
    por Singh, Vishwanath P., Badiger, N. M.
    Publicado 2014
    “…It was found that the effective atomic numbers computed by Auto-Z(eff), direct and interpolation methods were in good agreement for intermediate energy region (0.1 MeV < E < 5 MeV) where the Compton interaction dominates. A large difference in effective atomic numbers by direct method and Auto-Z(eff) was observed in photo-electric and pair-production regions. …”
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    Effective atomic numbers of some tissue substitutes by different methods: A comparative study
  2. 1162
    “…The properties of a 50 mm × 50 mm × 30 mm monolithic LaBr(3):Ce scintillator crystal coupled to a position-sensitive multi-anode photomultiplier (PMT, Hamamatsu H9500), representing the absorbing detector of a Compton camera under study for online ion (proton) beam range verification in hadron therapy, was evaluated in combination with either absorptive or reflective crystal surface coating. …”
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    Comparative Characterization Study of a LaBr(3)(Ce) Scintillation Crystal in Two Surface Wrapping Scenarios: Absorptive and Reflective
  3. 1163
    “…Further, it was possible to obtain useful tissue structural information from the ratio of the tomogram of photon flux behind the sample to the tomogram of Compton scattering. The micro-X-ray fluorescence tomograms showed that As predominantly accumulated in the nucleus of the epidermal cells in young mature leaves exposed to sublethal 1 µM As. …”
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    Analysis of sublethal arsenic toxicity to Ceratophyllum demersum: subcellular distribution of arsenic and inhibition of chlorophyll biosynthesis
  4. 1164
    “…With a unique laser-based Compact Light Source using inverse Compton scattering, we investigated the translation of this promising radiotherapy technique to a machine of future clinical relevance. …”
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    Increased cell survival and cytogenetic integrity by spatial dose redistribution at a compact synchrotron X-ray source
  5. 1165
    “…The resulting images then show a contrast that is influenced either by the atomic number of the elements in the sample (photoelectric interactions) or by the mass density (Compton scattering). For better visualization, those images can be combined to a color image where different materials can easily be distinguished. …”
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    Novel multi-energy X-ray imaging methods: Experimental results of new image processing techniques to improve material separation in computed tomography and direct radiography
  6. 1166
    por Noori-Asl, Mahsa
    Publicado 2020
    “…INTRODUCTION: Detection of compton scattered photons is one of the most important factors affecting the quality of single-photon emission computed tomography (SPECT) images. …”
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    Assessment of Four Scatter Correction Methods in In-111 SPECT Imaging: A Simulation Study
  7. 1167
    “…Yet engaging AYA early in their trajectory of substance use offers an invaluable opportunity to minimize the short-term and long-term consequences of use (Compton et al., 2019; Levy, Williams, & Prevention, C. on S. …”
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    A commentary on the impact of COVID-19 on engagement of youth with substance use and co-occurring psychiatric disorders
  8. 1168
    “…Instrumentation developments always occurred during the search to improving devices’ sensitivity and included advances in detector technology (with the introduction of cadmium zinc telluride and digital Positron Emission Tomography—PET-devices with silicon photomultipliers), design (total body PET) and configuration (ring-shaped, Single-Photon Emission Computed Tomography (SPECT), Compton camera). In the field of radionuclide development, we observed the continual changing of clinically used radionuclides, which is sometimes influenced by instrumentation technology but also driven by availability, patient safety and clinical questions. …”
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    New Radionuclides and Technological Advances in SPECT and PET Scanners
  9. 1169
    por Aleksić, J., Ansoldi, S., Antonelli, L.A., Antoranz, P., Babic, A., Bangale, P., Barrio, J.A., Becerra González, J., Bednarek, W., Bernardini, E., Biasuzzi, B., Biland, A., Blanch, O., Bonnefoy, S., Bonnoli, G., Borracci, F., Bretz, T., Carmona, E., Carosi, A., Colin, P., Colombo, E., Contreras, J.L., Cortina, J., Covino, S., Da Vela, P., Dazzi, F., De Angelis, A., De Caneva, G., De Lotto, B., Wilhelmi, E. de Oña, Delgado Mendez, C., Dominis Prester, D., Dorner, D., Doro, M., Einecke, S., Eisenacher, D., Elsaesser, D., Fidalgo, D., Fonseca, M.V., Font, L., Frantzen, K., Fruck, C., Galindo, D., López, R. J. García, Garczarczyk, M., Garrido Terrats, D., Gaug, M., Godinović, N., González Muñoz, A., Gozzini, S.R., Hadasch, D., Hanabata, Y., Hayashida, M., Herrera, J., Hose, J., Hrupec, D., Idec, W., Kadenius, V., Kellermann, H., Knoetig, M.L., Kodani, K., Konno, Y., Krause, J., Kubo, H., Kushida, J., La Barbera, A., Lelas, D., Lewandowska, N., Lindfors, E., Lombardi, S., Longo, F., López, M., López-Coto, R., López-Oramas, A., Lorenz, E., Lozano, I., Makariev, M., Mallot, K., Maneva, G., Mannheim, K., Maraschi, L., Marcote, B., Mariotti, M., Martínez, M., Mazin, D., Menzel, U., Miranda, J.M., Mirzoyan, R., Moralejo, A., Munar-Adrover, P., Nakajima, D., Neustroev, V., Niedzwiecki, A., Nilsson, K., Nishijima, K., Noda, K., Orito, R., Overkemping, A., Paiano, S., Palatiello, M., Paneque, D., Paoletti, R., Paredes, J.M., Paredes-Fortuny, X., Persic, M., Poutanen, J., Prada Moroni, P. G., Prandini, E., Puljak, I., Reinthal, R., Rhode, W., Ribó, M., Rico, J., Rodriguez Garcia, J., Rügamer, S., Saito, T., Saito, K., Satalecka, K., Scalzotto, V., Scapin, V., Schultz, C., Schweizer, T., Sillanpää, A., Sitarek, J., Snidaric, I., Sobczynska, D., Spanier, F., Stamerra, A., Steinbring, T., Storz, J., Strzys, M., Takalo, L., Takami, H., Tavecchio, F., Temnikov, P., Terzić, T., Tescaro, D., Teshima, M., Thaele, J., Tibolla, O., Torres, D.F., Toyama, T., Treves, A., Vogler, P., Will, M., Zanin, R., D'Ammando, F., Buson, S., Lähteenmäki, A., Tornikoski, M., Hovatta, T., Readhead, A.C.S., Max-Moerbeck, W., Richards, J.L.
    Publicado 2014
    “…Finally, we find that the synchrotron self-Compton (SSC) model gives a satisfactory description of the observed multi-wavelength spectral energy distribution during the flare.…”
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    Probing the very-high-energy gamma-ray spectral curvature in the blazar PG 1553+113 with the MAGIC telescopes
  10. 1170
    por Akhunzyanov, R., Alexeev, M.G., Alexeev, G.D., Amoroso, A., Andrieux, V., Anfimov, N.V., Anosov, V., Antoshkin, A., Augsten, K., Augustyniak, W., Austregesilo, A., Azevedo, C.D.R., Badełek, B., Balestra, F., Ball, M., Barth, J., Beck, R., Bedfer, Y., Bernhard, J., Bicker, K., Bielert, E.R., Birsa, R., Bodlak, M., Bordalo, P., Bradamante, F., Bressan, A., Büchele, M., Burtin, E., Burtsev, V.E., Chang, W.-C., Chatterjee, C., Chiosso, M., Choi, I., Chumakov, A.G., Chung, S.-U., Cicuttin, A., Crespo, M.L., Dalla Torre, S., Dasgupta, S.S., Dasgupta, S., Denisov, O.Yu., Dhara, L., Donskov, S.V., Doshita, N., Dreisbach, Ch., Dünnweber, W., Dusaev, R.R., Dziewiecki, M., Efremov, A., Eversheim, P.D., Faessler, M., Ferrero, A., Finger, M., Finger, Michael, Jr., Fischer, H., Franco, C., du Fresne von Hohenesche, N., Friedrich, J.M., Frolov, V., Fuchey, E., Gautheron, F., Gavrichtchouk, O.P., Gerassimov, S., Giarra, J., Gnesi, I., Gorzellik, M., Grasso, A., Gridin, A., Grosse Perdekamp, M., Grube, B., Grussenmeyer, T., Guskov, A., Hahne, D., Hamar, G., von Harrach, D., Heitz, R., Herrmann, F., Horikawa, N., d'Hose, N., Hsieh, C.-Y., Huber, S., Ishimoto, S., Ivanov, A., Ivanshin, Yu., Iwata, T., Jary, V., Joosten, R., Jörg, P., Juraskova, K., Kabuß, E., Kerbizi, A., Ketzer, B., Khaustov, G.V., Khokhlov, Yu.A., Kisselev, Yu., Klein, F., Koivuniemi, J.H., Kolosov, V.N., Kondo, K., Konorov, I., Konstantinov, V.F., Kotzinian, A.M., Kouznetsov, O.M., Kral, Z., Krämer, M., Krinner, F., Kroumchtein, Z.V., Kulinich, Y., Kunne, F., Kurek, K., Kurjata, R.P., Kuznetsov, I.I., Kveton, A., Lednev, A.A., Levchenko, E.A., Levillain, M., Levorato, S., Lian, Y.-S., Lichtenstadt, J., Longo, R., Lyubovitskij, V.E., Maggiora, A., Magnon, A., Makins, N., Makke, N., Mallot, G.K., Mamon, S.A., Marianski, B., Martin, A., Marzec, J., Matoušek, J., Matsuda, H., Matsuda, T., Meshcheryakov, G.V., Meyer, M., Meyer, W., Mikhailov, Yu.V., Mikhasenko, M., Mitrofanov, E., Mitrofanov, N., Miyachi, Y., Moretti, A., Nagaytsev, A., Nerling, F., Neyret, D., Nový, J., Nowak, W.-D., Nukazuka, G., Nunes, A.S., Olshevsky, A.G., Orlov, I., Ostrick, M., Panzieri, D., Parsamyan, B., Paul, S., Peng, J.-C., Pereira, F., Pešek, M., Pešková, M., Peshekhonov, D.V., Pierre, N., Platchkov, S., Pochodzalla, J., Polyakov, V.A., Pretz, J., Quaresma, M., Quintans, C., Ramos, S., Regali, C., Reicherz, G., Riedl, C., Rogacheva, N.S., Ryabchikov, D.I., Rybnikov, A., Rychter, A., Salac, R., Samoylenko, V.D., Sandacz, A., Santos, C., Sarkar, S., Savin, I.A., Sawada, T., Sbrizzai, G., Schiavon, P., Schmieden, H., Schönning, K., Seder, E., Selyunin, A., Silva, L., Sinha, L., Sirtl, S., Slunecka, M., Smolik, J., Srnka, A., Steffen, D., Stolarski, M., Subrt, O., Sulc, M., Suzuki, H., Szabelski, A., Szameitat, T., Sznajder, P., Tasevsky, M., Tessaro, S., Tessarotto, F., Thiel, A., Tomsa, J., Tosello, F., Tskhay, V., Uhl, S., Vasilishin, B.I., Vauth, A., Veit, B.M., Veloso, J., Vidon, A., Virius, M., Wallner, S., Wilfert, M., ter Wolbeek, J., Zaremba, K., Zavada, P., Zavertyaev, M., Zemlyanichkina, E., Zhuravlev, N., Ziembicki, M.
    Publicado 2018
    “…We determine the dependence of the average of the measured $\mu^+$ and $\mu^-$ cross sections for deeply virtual Compton scattering on the squared four-momentum transfer $t$ from the initial to the final final proton. …”
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    Transverse extension of partons in the proton probed in the sea-quark range by measuring the DVCS cross section
  11. 1171
    “…This concept has two main advantages: (1) The parallax error is reduced to a minimum and is equal for the whole field of view (FOV). (2) The P01 and its energy deposit is known in all three dimension with a high resolution, allowing for the reconstruction of Compton scattered gamma-rays. Point (1) leads to a uniform point source resolution (PSR) distribution over the whole FOV, and also allows to place the detector close to the object being imaged. …”
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    Characterization of a high resolution and high sensitivity pre-clinical PET scanner with 3D event reconstruction
  12. 1172
    “…In parallel to the ATF2 LW, the PETRA3 laserwire has developed the use of fibre lasers for Compton scattering and the progress using fibre lasers is reported.…”
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    info:eu-repo/semantics/article
    Laser Wire and Beam Position Monitor tests
  13. 1173
    por Mustafa, Munshi G., Thoma, Markus H.
    Publicado 2000
    “…Furthermore the photon production due to bremsstrahlung from the chemically nonequilibrated plasma dominates over the emission from Compton scattering and quark-antiquark annihilation at LHC energies, whereas the both processes are of the same order at RHIC energies.…”
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    Bremsstrahlung from an Equilibrating Quark-Gluon Plasma
  14. 1174
    por Zimmermann, Frank
    Publicado 2018
    “…Raimondi et al.], (2) laser/FEL-Compton back-scattering off high-energy proton beams circulating in the LHC or FCC-hh [L. …”
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    LHC/FCC-based muon colliders
  15. 1175
    por Serafini, L, Bacci, A, Bellandi, A, Bertucci, M, Bolognesi, M, Bosotti, A, Broggi, F, Calandrino, R, Camera, F, Canella, F, Capra, S, Cardarelli, P, Carrara, M, Cassou, K, Castoldi, A, Castriconi, R, Cattaneo, G M, Cialdi, S, Cianchi, A, Coluccelli, N, Curatolo, C, Del Vecchio, A, Di Mitri, S, Drebot, I, Dupraz, K, Esposito, A, Faillace, L, Ferrario, M, Fiorini, C, Galzerano, G, Gambaccini, M, Ghiringhelli, G, Giannotti, D, Giove, D, Groppi, F, Guazzoni, C, Laporta, P, Leoni, S, Loria, A, Mangili, P, Martens, A, Mazza, T, Mazzotta, Z, Meroni, C, Mettivier, G, Michelato, P, Monaco, L, Morante, S, Moretti Sala, M, Nutarelli, D, Olivares, S, Onida, G, Opromolla, M, Pagani, C, Paparella, R, Paris, M G A, Paroli, B, Paternò, G, Paulin, C, Perini, L, Petrarca, M, Petrillo, V, Pinotti, E, Piseri, P, Potenza, M A C, Prelz, F, Pullia, A, Puppin, E, Ragusa, F, Ramponi, R, Romè, M, Rossetti Conti, M, Rossi, A R, Rossi, L, Ruijter, M, Russo, P, Samsam, S, Sarno, A, Sertore, D, Sorbi, M, Spataro, B, Statera, M, Stellato, F, Suerra, E, Tagliaferri, A, Taibi, A, Torri, V, Turchetti, G, Vaccarezza, C, Valdagni, R, Vanzulli, A, Zomer, F, Rossi, G
    Publicado 2019
    “…The accelerator complex includes an early stage that supports an advanced inverse Compton source of very high-flux hard X-rays of energies up to 180 keV that is well adapted for large area radiological imaging, realizing a broad science programme and serving a multidisciplinary user community, covering fundamental science of matter and application to life sciences, including health at preclinical and clinical level.…”
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    MariX, an advanced MHz-class repetition rate X-ray source for linear regime time-resolved spectroscopy and photon scattering
  16. 1176
    por Jovančević, N, Lebois, M, Wilson, J N, Thisse, D, Qi, L, Matea, I, Ibrahim, F, Verney, D, Babo, M, Delafosse, C, Adsley, F, Tocabens, G, Gottardo, A, Popovitch, Y, Nemer, J, Canavan, R, Rudigier, M, Belvedere, K, Boso, A, Regan, P, Podolyak, Zs, Shearman, R, Buncec, M, Inavov, P, Oberstedt, S, Lopez-Martens, A, Hauschild, K, Ljungvall, J, Chakma, R, Lozeva, R, Söderström, P -A, Oberstedt, A, Etasse, D, Ralet, D, Blazhev, A, Gerst, R -B, Hafner, G, Cieplicka-Oryńczak, N, Iskra, Ł W, Fornal, B, Benzoni, G, Leoni, S, Bottoni, S, Henrich, C, Koseoglou, P, Wiederhold, J, Homm, I, Surder, C, Kroll, T, Knezevic, D, Dragic, A, Cortes, L, Warr, N, Miernik, K, Adamska, E, Piersa, M, Rezynkina, K, Fraile, L, Garcia, J Benito, Sanchez, V, Algora, A, Davies, P, Guadilla-Gomez, V, Fallot, M, Kurtukian-Nieto, T, Schmitt, C, Heine, M, Tello, D Reygadas, Yavachova, M, Diakaki, M, Zeiser, F, Paulson, W, Gestvang, D
    Publicado 2019
    “…The $\nu$-ball is a high-efficiency hybrid spectrometer which consists of both germanium (Ge) detectors and associated anti-Compton BGO shields, coupled to lanthanum bromide (LaBr$_3$) detectors. …”
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    Spectroscopy of Neutron Induced Reactions with the $\nu $-ball Spectrometer
  17. 1177
    “…This was caused by the Compton electrons due to the   60 Co gamma radiation. …”
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    Charge collection study with the ATLAS ITk prototype silicon strip sensors ATLAS17LS
  18. 1178
    “…CONCLUSIONS/SIGNIFICANCE: We propose that due to melanin's numerous aromatic oligomers containing multiple π-electron system, a generated Compton recoil electron gradually loses energy while passing through the pigment, until its energy is sufficiently low that it can be trapped by stable free radicals present in the pigment. …”
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    Physico-Chemical Evaluation of Rationally Designed Melanins as Novel Nature-Inspired Radioprotectors
  19. 1179
    “…Here we present spectrally resolved x-ray scattering measurements from plasmons in dynamically compressed deuterium. Combined with Compton scattering, and velocity interferometry to determine shock pressure and mass density, this allows us to extract ionization state as a function of compression. …”
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    X-ray scattering measurements of dissociation-induced metallization of dynamically compressed deuterium
  20. 1180
    “…However, (18)F has a short half-life, and 511 keV Compton-scattered photons are detected in the (99m)Tc energy window. …”
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    Evaluation of Simultaneous Dual-radioisotope SPECT Imaging Using (18)F-fluorodeoxyglucose and (99m)Tc-tetrofosmin
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