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64“…This note presents results from simulations of losses on the TOTEM Roman Pot stations located close to 150m and 220m from IP5. …”
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65por Ruggiero, Gennaro“…This Technical Specification describes the main features of the Edgeless Strip Detectors (ESD) to be employed to equip the TOTEM Roman Pots. The scope of this document concerns the purchase of 200 units of ESDs (considered as the series production) and 200 test units, which will be used to benchmark some of the physical properties of the ESDs and some quality aspects of the production.…”
Publicado 2007
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66“…The number of protons with transversal coordinates greater than 10 s + 0:5 mm, that is inside the Roman Pot, is compared with the total number of protons. …”
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67por Deile, Mario, Caspers, Fritz, Kroyer, Tom, Oriunno, Marco, Radermacher, Ernst, Soter, Anna, Roncarolo, Federico“…The longitudinal and transverse beam coupling impedance of the first final TOTEM Roman Pot unit has been measured in the laboratory with the wire method. …”
Publicado 2008
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68por G. Ruggiero, G, Avati, V, Antchev, G, Deile, M, Eggert, K, Eremin, V, Kaspar, J, Niewiadomski, H, Petäjäjärvi, J, Radicioni, E, Ravotti, F, Radermacher, E, Snoeys, W, Spearman, W, Wu, J“…TOTEM Roman Pot (RP) microstrip edgeless silicon detectors, fabricated with standard planar technology, reach full sensitivity within 50 μm from the cut edge and can operate with high bias voltage at room temperature. …”
Publicado 2009
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69por Mierzejewski, Dominik“…Precise computer model of the Roman Pot detectors geometry, which is crucial to simulation and analysis of both simulated and real event data was developed. …”
Publicado 2010
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70“…The ATLAS Forward Proton (AFP) detectors are designed for tagging of forward protons and located inside Roman Pots (RP). My task as summer student is a data analysis to measure the distance between Silicon detectors and the RP floor. …”
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71“…The ATLAS Roman Pots are a part of the ATLAS Forward detector system which consists of two subsystems, the ALFA (Absolute Luminosity For ATLAS) and the ATLAS Forward Proton (AFP) detector. …”
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72por Janas, Krzysztof Wojciech“…ALFA detector is part of the ATLAS Roman Pot detector dedicated to measure protons scattered at very small angles. …”
Publicado 2019
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73por The ATLAS collaboration“…ALFA detector is part of the ATLAS Roman Pot detector dedicated to measure protons scattered at very small angles. …”
Publicado 2021
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74por Deile, Mario“…This note describes algebraic methods for calculating Roman Pot acceptance and reconstruction resolution in the kinematic variables of diffractively scattered protons. …”
Publicado 2007
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75“…This note reports on two calibrations of the conversion factor from the number of protons intercepted by a TOTEM Roman Pot (RP) to the dose measured in a Beam Loss Monitor (BLM) downstream of the RP station. …”
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76por Deile, M., Antchev, G.H., Appleby, R.B., Assmann, R.W., Atanassov, I., Avati, V., Baechler, J., Bruce, R., Dupont, M., Eggert, K., Farnham, B., Kaspar, J., Lucas Rodriguez, F., Morant, J., Niewiadomski, H., Pons, X., Radermacher, E., Ravat, S., Ravotti, F., Redaelli, S., Ruggiero, G., Sabba, H., Sapinski, M., Snoeys, W., Valentino, G., Wollmann, D.“…Since the LHC running season 2010, the TOTEM Roman Pots (RPs) are fully operational and serve for collecting elastic and diffractive proton-proton scattering data. …”
Publicado 2011
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78“…During the design phase of the TOTEM experiment, several Roman Pot detector models were simulated in FLUKA to address radiation damage and radiation protection issues as well as to define specific accidental scenarios involving beam losses in the Roman Pot components. …”
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79por Antchev, G, Aspell, P, Atanassov, I, Avati, V, Baechler, J, Berardi, V, Berretti, M, Bossini, E, Bottigli, U, Bozzo, M, Brücken, E, Buzzo, A, Cafagna, F S, Catanesi, M G, Covault, C, Csanád, M, Csörgő, T, Deile, M, Doubek, M, Eggert, K, Eremin, V, Ferro, F, Fiergolski, A, Garcia, F, Georgiev, V, Giani, S, Grzanka, L, Hammerbauer, J, Heino, J, Hilden, T, Karev, A, Kašpar, J, Kopal, J, Kundrát, V, Lami, S, Latino, G, Lauhakangas, R, Leszko, T, Lippmaa, E, Lippmaa, J, Lokajíček, M V, Losurdo, L, Lo Vetere, M, Lucas Rodríguez, F, Macrí, M, Mäki, T, Mercadante, A, Minafra, N, Minutoli, S, Nemes, F, Niewiadomski, H, Oliveri, E, Oljemark, F, Orava, R, Oriunno, M, Österberg, K, Palazzi, P, Peroutka, Z, Procházka, J, Quinto, M, Radermacher, E, Radicioni, E, Ravotti, F, Robutti, E, Ropelewski, L, Ruggiero, G, Saarikko, H, Scribano, A, Smajek, J, Snoeys, W, Sziklai, J, Taylor, C, Turini, N, Vacek, V, Welti, J, Whitmore, J, Wyszkowski, P, Zielinski, K“…Precise knowledge of the beam optics at the LHC is crucial to fulfil the physics goals of the TOTEM experiment, where the kinematics of the scattered protons is reconstructed with the near-beam telescopes -- so-called Roman Pots (RP). Before being detected, the protons' trajectories are influenced by the magnetic fields of the accelerator lattice. …”
Publicado 2014
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80“…Precise knowledge of the beam optics at the LHC is crucial to fulfill the physics goals of the TOTEM experiment, where the kinematics of the scattered protons is reconstructed with the near-beam telescopes – so-called Roman Pots (RP). Before being detected, the protons’ trajectories are influenced by the magnetic fields of the accelerator lattice. …”
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