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E. Tcherniaev

Bio: E. Tcherniaev is an academic researcher from CERN. The author has contributed to research in topics: Physics & Particle physics. The author has an hindex of 15, co-authored 19 publications receiving 21881 citations.

Papers published on a yearly basis

Papers
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Journal ArticleDOI
S. Agostinelli1, John Allison2, K. Amako3, J. Apostolakis4, Henrique Araujo5, P. Arce4, Makoto Asai6, D. Axen4, S. Banerjee7, G. Barrand, F. Behner4, Lorenzo Bellagamba8, J. Boudreau9, L. Broglia10, A. Brunengo8, H. Burkhardt4, Stephane Chauvie, J. Chuma11, R. Chytracek4, Gene Cooperman12, G. Cosmo4, P. V. Degtyarenko13, Andrea Dell'Acqua4, G. Depaola14, D. Dietrich15, R. Enami, A. Feliciello, C. Ferguson16, H. Fesefeldt4, Gunter Folger4, Franca Foppiano, Alessandra Forti2, S. Garelli, S. Gianì4, R. Giannitrapani17, D. Gibin4, J. J. Gomez Y Cadenas4, I. González4, G. Gracia Abril4, G. Greeniaus18, Walter Greiner15, Vladimir Grichine, A. Grossheim4, Susanna Guatelli, P. Gumplinger11, R. Hamatsu19, K. Hashimoto, H. Hasui, A. Heikkinen20, A. S. Howard5, Vladimir Ivanchenko4, A. Johnson6, F.W. Jones11, J. Kallenbach, Naoko Kanaya4, M. Kawabata, Y. Kawabata, M. Kawaguti, S.R. Kelner21, Paul R. C. Kent22, A. Kimura23, T. Kodama24, R. P. Kokoulin21, M. Kossov13, Hisaya Kurashige25, E. Lamanna26, Tapio Lampén20, V. Lara4, Veronique Lefebure4, F. Lei16, M. Liendl4, W. S. Lockman, Francesco Longo27, S. Magni, M. Maire, E. Medernach4, K. Minamimoto24, P. Mora de Freitas, Yoshiyuki Morita3, K. Murakami3, M. Nagamatu24, R. Nartallo28, Petteri Nieminen28, T. Nishimura, K. Ohtsubo, M. Okamura, S. W. O'Neale29, Y. Oohata19, K. Paech15, J Perl6, Andreas Pfeiffer4, Maria Grazia Pia, F. Ranjard4, A.M. Rybin, S.S Sadilov4, E. Di Salvo8, Giovanni Santin27, Takashi Sasaki3, N. Savvas2, Y. Sawada, Stefan Scherer15, S. Sei24, V. Sirotenko4, David J. Smith6, N. Starkov, H. Stoecker15, J. Sulkimo20, M. Takahata23, Satoshi Tanaka30, E. Tcherniaev4, E. Safai Tehrani6, M. Tropeano1, P. Truscott31, H. Uno24, L. Urbán, P. Urban32, M. Verderi, A. Walkden2, W. Wander33, H. Weber15, J.P. Wellisch4, Torre Wenaus34, D.C. Williams, Douglas Wright6, T. Yamada24, H. Yoshida24, D. Zschiesche15 
TL;DR: The Gelfant 4 toolkit as discussed by the authors is a toolkit for simulating the passage of particles through matter, including a complete range of functionality including tracking, geometry, physics models and hits.
Abstract: G eant 4 is a toolkit for simulating the passage of particles through matter. It includes a complete range of functionality including tracking, geometry, physics models and hits. The physics processes offered cover a comprehensive range, including electromagnetic, hadronic and optical processes, a large set of long-lived particles, materials and elements, over a wide energy range starting, in some cases, from 250 eV and extending in others to the TeV energy range. It has been designed and constructed to expose the physics models utilised, to handle complex geometries, and to enable its easy adaptation for optimal use in different sets of applications. The toolkit is the result of a worldwide collaboration of physicists and software engineers. It has been created exploiting software engineering and object-oriented technology and implemented in the C++ programming language. It has been used in applications in particle physics, nuclear physics, accelerator design, space engineering and medical physics.

18,904 citations

Journal ArticleDOI
TL;DR: GeGeant4 as mentioned in this paper is a software toolkit for the simulation of the passage of particles through matter, it is used by a large number of experiments and projects in a variety of application domains, including high energy physics, astrophysics and space science, medical physics and radiation protection.
Abstract: Geant4 is a software toolkit for the simulation of the passage of particles through matter. It is used by a large number of experiments and projects in a variety of application domains, including high energy physics, astrophysics and space science, medical physics and radiation protection. Its functionality and modeling capabilities continue to be extended, while its performance is enhanced. An overview of recent developments in diverse areas of the toolkit is presented. These include performance optimization for complex setups; improvements for the propagation in fields; new options for event biasing; and additions and improvements in geometry, physics processes and interactive capabilities

6,063 citations

Journal ArticleDOI
M. G. Catanesi, M. T. Muciaccia, E. Radicioni, S. Simone, Rob Edgecock1, Malcolm Ellis1, S. Robbins1, F. J. P. Soler1, Claus Gößling2, M. Mass2, S.A. Bunyatov3, Artem Chukanov3, O.L. Klimov3, I. Krasin3, Alexey Krasnoperov3, D. Kustov3, B. A. Popov3, V. Serdiouk3, V. Tereshchenko3, V. Carassiti, E. Di Capua, F. Evangelisti, G. Vidal-Sitjes, A. Artamonov4, P. Arce4, R. Brocard4, G. Decreuse4, B. Friend4, S. Giani4, Simone Gilardoni4, P. Gorbunov4, A. Grant4, A. Grossheim4, P. Gruber4, Vladimir Ivanchenko4, J.-C. Legrand4, A. Kayis-Topaksu4, J. Panman4, Ioannis Papadopoulos4, J. Pasternak4, E. Tcherniaev4, Ilya Tsukerman4, R. van der Vlugt4, Rob Veenhof4, C. Wiebusch4, P. Zucchelli4, A. Blondel5, Silvia Borghi5, Manuela Campanelli5, A. Cervera-Villanueva5, M. C. Morone5, G. Prior5, R. Schroeter5, I. Kato6, U. Gastaldi, G.B. Mills7, J.S. Graulich8, Ghislain Grégoire8, M. Bonesini, F. Chignoli, Federico Ferri, F. Paleari, Mikhail Kirsanov, V. Postoev, A. Bagulya9, V. Grichine9, N. G. Polukhina9, V. Palladino, L. Coney10, D. W. Schmitz10, G.D. Barr11, A. De Santo11, C. Pattison11, Kai Zuber11, G. Barichello, F. Bobisut, D. Gibin, A. Guglielmi, Marco Laveder, Alessandro Menegolli, M. Mezzetto, A. Pepato, J. Dumarchez, S. Troquereau, F. Vannucci, U. Dore12, A. Iaciofano, M. Lobello, F. Marinilli, Domizia Orestano, D. Panayotov, M. Pasquali, Fr Pastore, A. Tonazzo, L. Tortora, C. N. Booth13, Craig Buttar13, Paul Hodgson13, L. Howlett13, R. Nicholson13, M. Bogomilov14, K. Burin14, M. Chizhov14, D. Kolev14, P. Petev14, I. Rusinov14, R. Tsenov14, S. Piperov15, Petar Temnikov15, M. Apollonio, P. Chimenti, G. Giannini, Giovanni Santin, Jordi Burguet-Castell16, J.J. Gómez-Cadenas16, P. Novella16, M. Sorel16, A. Tornero16 
TL;DR: HARP as mentioned in this paper is a large solid angle experiment to measure hadron production using proton and pion beams with momenta between 1.5 and 15 GeV/c impinging on many different solid and liquid targets from low to high Z.
Abstract: HARP is a high-statistics, large solid angle experiment to measure hadron production using proton and pion beams with momenta between 1.5 and 15 GeV/c impinging on many different solid and liquid targets from low to high Z. The experiment, located in the T9 beam of the CERN PS, took data in 2001 and 2002. For the measurement of momenta of produced particles and for the identification of particle types, the experiment includes a large-angle spectrometer, based on a Time Projection Chamber and a system of Resistive Plate Chambers, and a forward spectrometer equipped with a set of large drift chambers, a threshold Cherenkov detector, a time-of-flight wall and an electromagnetic calorimeter. The large angle system uses a solenoidal magnet, while the forward spectrometer is based on a dipole magnet. Redundancy in particle identification has been sought, to enable the cross-calibration of efficiencies and to obtain a few percent overall accuracy in the cross-section measurements. Detector construction, operation and initial physics performances are reported. In addition, the full chain for data recording and analysis, from trigger to the software framework, is described.

80 citations

Journal ArticleDOI
E. Radicioni, Rob Edgecock1, Malcolm Ellis1, S. Robbins1, F. J. P. Soler2, F. J. P. Soler1, Claus Gößling3, S.A. Bunyatov4, G. A. Chelkov4, D. Dedovitch4, M. I. Gostkin4, A. Guskov4, D. Khartchenko4, Alexey Krasnoperov4, Z.V. Kroumchtein4, Yu. Nefedov4, B. A. Popov4, V. Serdiouk4, V. Tereshchenko4, Alexey Zhemchugov4, E. Di Capua, G. Vidal-Sitjes5, A. Artamonov6, Pedro Arce6, Pedro Arce7, S. Gianì6, Simone Gilardoni6, P. Gorbunov6, A. Grant6, A. Grossheim8, A. Grossheim6, P. Gruber9, P. Gruber6, Vladimir Ivanchenko6, Vladimir Ivanchenko10, A. Kayis-Topaksu11, A. Kayis-Topaksu6, J. Panman6, Ioannis Papadopoulos6, J. Pasternak6, E. Tcherniaev6, Ilya Tsukerman6, Rob Veenhof6, C. Wiebusch12, C. Wiebusch6, P. Zucchelli6, A. Blondel13, Silvia Borghi6, Silvia Borghi13, Manuela Campanelli13, M. C. Morone13, G. Prior13, G. Prior14, R. Schroeter13, Ralph Engel15, C. Meurer15, I. Kato16, U. Gastaldi, G.B. Mills17, J.S. Graulich18, J.S. Graulich14, Ghislain Grégoire19, M. Bonesini20, A. De Min20, Federico Ferri20, Marco Paganoni20, F. Paleari20, Mikhail Kirsanov, A. Bagulya21, V. Grichine21, N. G. Polukhina21, V. Palladino, L. Coney22, D. W. Schmitz22, G.D. Barr23, A. De Santo13, A. De Santo23, C. Pattison23, Kai Zuber23, Kai Zuber24, F. Bobisut, D. Gibin, A. Guglielmi, M. Mezzetto, J. Dumarchez, F. Vannucci, V. V. Ammosov, V. I. Koreshev, A. Semak, V. G. Zaets, U. Dore25, Domizia Orestano, Fr Pastore, A. Tonazzo, L. Tortora, C. N. Booth26, Craig Buttar26, Paul Hodgson26, L. Howlett26, M. Bogomilov27, M. Chizhov27, D. Kolev27, R. Tsenov27, S. Piperov28, Petar Temnikov28, M. Apollonio, P. Chimenti, G. Giannini, Giovanni Santin29, Jordi Burguet-Castell7, A. Cervera-Villanueva7, J.J. Gómez-Cadenas7, J. Martín-Albo7, P. Novella7, M. Sorel7, A. Tornero7 
TL;DR: In this article, the double-differential production cross-section of positive pions, d^2σπ+}/d pdΩ, measured in the HARP experiment is presented.
Abstract: The double-differential production cross-section of positive pions, d^2σ^{π+}/d pdΩ, measured in the HARP experiment is presented. The incident particles are 8.9 GeV/c protons directed onto a beryllium target with a thickness of 5% of a nuclear interaction length. The measured cross-section has a direct impact on the prediction of neutrino fluxes for the MiniBooNE and SciBooNE experiments at Fermilab. After cuts, 13 million protons on target produced about 96000 reconstructed secondary tracks which were used in this analysis. Cross-section results are presented in the kinematic range 0.75 GeV/c≤pπ≤ 6.5 GeV/c and 30 mrad≤θπ≤ 210 mrad in the laboratory frame.

68 citations

Journal ArticleDOI
M. G. Catanesi, M. T. Muciaccia, E. Radicioni, S. Simone, Rob Edgecock1, Malcolm Ellis1, S. Robbins1, F. J. P. Soler1, Claus Gößling2, M. Mass2, S.A. Bunyatov3, Artem Chukanov3, D. Dedovitch3, A. Elagin3, Mikhail Ivanovitch Gostkin3, A. Guskov3, D. Khartchenko3, O. Klimov3, A. Krasnoperov3, D. Kustov3, K. Nikolaev3, B. A. Popov3, V. Serdiouk3, V. Tereshchenko3, Alexey Zhemchugov3, E. Di Capua, G. Vidal-Sitjes, A. Artamonov4, P. Arce4, S. Gianì4, Simone Gilardoni4, P. Gorbunov4, A. Grant4, A. Grossheim4, P M Gruber4, Vladimir Ivanchenko4, A. Kayis-Topaksu4, L. Linssen4, J. Panman4, Ioannis Papadopoulos4, J. Pasternak4, E. Tcherniaev4, Ilya Tsukerman4, Rob Veenhof4, C. Wiebusch4, P. Zucchelli4, A. Blondel5, Silvia Borghi5, Manuela Campanelli5, A. Cervera-Villanueva5, M. C. Morone5, G. Prior5, R. Schroeter5, I. Kato6, Tsuyoshi Nakaya6, K. Nishikawa6, S. Ueda6, V. Ableev, U. Gastaldi, G.B. Mills7, J.S. Graulich8, Ghislain Grégoire8, M. Bonesini, Marta Calvi, A. De Min, Federico Ferri, Marco Paganoni, F. Paleari, Mikhail Kirsanov, A. Bagulya9, V. Grichine9, N. G. Polukhina9, V. Palladino, L. Coney10, D. W. Schmitz10, G.D. Barr11, A. De Santo11, C. Pattison11, Kai Zuber11, F. Bobisut, D. Gibin, A. Guglielmi, Marco Laveder, Alessandro Menegolli, M. Mezzetto, J. Dumarchez, S. Troquereau, F. Vannucci, V. V. Ammosov, V. A. Gapienko, V. I. Koreshev, A. Semak, Yu M. Sviridov, V. G. Zaets, U. Dore12, Domizia Orestano, M. Pasquali, Fr Pastore, A. Tonazzo, L. Tortora, C. N. Booth13, Craig Buttar13, Paul Hodgson13, L. Howlett13, M. Bogomilov14, M. Chizhov14, D. Kolev14, R. Tsenov14, S. Piperov15, Petar Temnikov15, M. Apollonio, P. Chimenti, G. Giannini, Giovanni Santin, Y. Hayato16, A. Ichikawa16, Takashi Kobayashi16, Jordi Burguet-Castell17, J.J. Gómez-Cadenas17, P. Novella17, M. Sorel17, A. Tornero17 
TL;DR: In this paper, the PS detector design, construction, commissioning, and operation is described and the authors gratefully acknowledge the help and support of the PS beam staff and of the numerous technical collaborators who contributed to the detector design and construction.

66 citations


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Georges Aad1, T. Abajyan2, Brad Abbott3, Jalal Abdallah4  +2964 moreInstitutions (200)
TL;DR: In this article, a search for the Standard Model Higgs boson in proton-proton collisions with the ATLAS detector at the LHC is presented, which has a significance of 5.9 standard deviations, corresponding to a background fluctuation probability of 1.7×10−9.

9,282 citations

Journal ArticleDOI
TL;DR: In this paper, results from searches for the standard model Higgs boson in proton-proton collisions at 7 and 8 TeV in the CMS experiment at the LHC, using data samples corresponding to integrated luminosities of up to 5.8 standard deviations.

8,857 citations

Journal ArticleDOI
TL;DR: The Pythia program as mentioned in this paper can be used to generate high-energy-physics ''events'' (i.e. sets of outgoing particles produced in the interactions between two incoming particles).
Abstract: The Pythia program can be used to generate high-energy-physics ''events'', i.e. sets of outgoing particles produced in the interactions between two incoming particles. The objective is to provide as accurate as possible a representation of event properties in a wide range of reactions, within and beyond the Standard Model, with emphasis on those where strong interactions play a role, directly or indirectly, and therefore multihadronic final states are produced. The physics is then not understood well enough to give an exact description; instead the program has to be based on a combination of analytical results and various QCD-based models. This physics input is summarized here, for areas such as hard subprocesses, initial- and final-state parton showers, underlying events and beam remnants, fragmentation and decays, and much more. Furthermore, extensive information is provided on all program elements: subroutines and functions, switches and parameters, and particle and process data. This should allow the user to tailor the generation task to the topics of interest.

6,300 citations

Journal ArticleDOI
TL;DR: GeGeant4 as mentioned in this paper is a software toolkit for the simulation of the passage of particles through matter, it is used by a large number of experiments and projects in a variety of application domains, including high energy physics, astrophysics and space science, medical physics and radiation protection.
Abstract: Geant4 is a software toolkit for the simulation of the passage of particles through matter. It is used by a large number of experiments and projects in a variety of application domains, including high energy physics, astrophysics and space science, medical physics and radiation protection. Its functionality and modeling capabilities continue to be extended, while its performance is enhanced. An overview of recent developments in diverse areas of the toolkit is presented. These include performance optimization for complex setups; improvements for the propagation in fields; new options for event biasing; and additions and improvements in geometry, physics processes and interactive capabilities

6,063 citations

Journal ArticleDOI
W. B. Atwood1, A. A. Abdo2, A. A. Abdo3, Markus Ackermann4  +289 moreInstitutions (37)
TL;DR: The Large Area Telescope (Fermi/LAT) as mentioned in this paper is the primary instrument on the Fermi Gamma-ray Space Telescope, which is an imaging, wide field-of-view, high-energy gamma-ray telescope, covering the energy range from below 20 MeV to more than 300 GeV.
Abstract: (Abridged) The Large Area Telescope (Fermi/LAT, hereafter LAT), the primary instrument on the Fermi Gamma-ray Space Telescope (Fermi) mission, is an imaging, wide field-of-view, high-energy gamma-ray telescope, covering the energy range from below 20 MeV to more than 300 GeV. This paper describes the LAT, its pre-flight expected performance, and summarizes the key science objectives that will be addressed. On-orbit performance will be presented in detail in a subsequent paper. The LAT is a pair-conversion telescope with a precision tracker and calorimeter, each consisting of a 4x4 array of 16 modules, a segmented anticoincidence detector that covers the tracker array, and a programmable trigger and data acquisition system. Each tracker module has a vertical stack of 18 x,y tracking planes, including two layers (x and y) of single-sided silicon strip detectors and high-Z converter material (tungsten) per tray. Every calorimeter module has 96 CsI(Tl) crystals, arranged in an 8 layer hodoscopic configuration with a total depth of 8.6 radiation lengths. The aspect ratio of the tracker (height/width) is 0.4 allowing a large field-of-view (2.4 sr). Data obtained with the LAT are intended to (i) permit rapid notification of high-energy gamma-ray bursts (GRBs) and transients and facilitate monitoring of variable sources, (ii) yield an extensive catalog of several thousand high-energy sources obtained from an all-sky survey, (iii) measure spectra from 20 MeV to more than 50 GeV for several hundred sources, (iv) localize point sources to 0.3 - 2 arc minutes, (v) map and obtain spectra of extended sources such as SNRs, molecular clouds, and nearby galaxies, (vi) measure the diffuse isotropic gamma-ray background up to TeV energies, and (vii) explore the discovery space for dark matter.

3,666 citations