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221por Peebles, James“…--HTML--><p><span style="mso-fareast-font-family:"Times New Roman";">Lessons about research in the natural sciences can be drawn from the sociology of science. …”
Publicado 2022
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222“…Detectors with the new terminating structure are being produced now and will be installed at LHC in the Roman Pots, a special beam insertion, to allow the TOTEM experiment to detect leading protons at 10 σ from the beam. …”
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223por Mapelli, A“…Detector modules will be placed above and below the LHC beam axis in roman pot units at a distance of 240 m on each side of the ATLAS interaction point. …”
Publicado 2007
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224“…The TOTEM Roman Pot Silicon sensors will be operated in vacuum to minimise the mechanical stress of the thin metal window which separates the detector package from the ultra high vacuum of the beam. …”
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225por F\"orster, Fabian Alexander“…Each tracker and the ToF system are placed inside a Roman Pot, allowing operation in the vicinity of the LHC beam, up to 2-3 mm. …”
Publicado 2017
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226por Hohmann, Marcel“…Each station consists of a Roman Pot containing a Silicon tracker (SiT) with the far stations having an additional Time of Flight (ToF) detector. …”
Publicado 2017
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227por Antchev, G., Aspell, P., Atanassov, I., Avati, V., Baechler, J., Barrera, C.B., Berardi, V., Berretti, M., Bossini, E., Bottigli, U., Bozzo, M., Burkhardt, H., Cafagna, F.S., Catanesi, M.G., Csanád, M., Csörgő, T., Deile, M., De Leonardis, F., D'Orazio, A., Doubek, M., Druzhkin, D., Eggert, K., Eremin, V., Ferro, F., Fiergolski, A., Garcia, F., Georgiev, V., Giani, S., Grzanka, L., Hammerbauer, J., Heino, J., Helander, P., Isidori, T., Ivanchenko, V., Janda, M., Karev, A., Kašpar, J., Kopal, J., Kundrát, V., Lami, S., Latino, G., Lauhakangas, R., Linhart, R., Lindsey, C., Lokajíček, M.V., Losurdo, L., Lo Vetere, M., Lucas Rodríguez, F., Macrí, M., Malawski, M., Minafra, N., Minutoli, S., Naaranoja, T., Nemes, F., Niewiadomski, H., Novák, T., Oliveri, E., Oljemark, F., Oriunno, M., Österberg, K., Palazzi, P., Passaro, V., Peroutka, Z., Procházka, J., Quinto, M., Radermacher, E., Radicioni, E., Ravotti, F., Robutti, E., Royon, C., Ruggiero, G., Saarikko, H., Scribano, A., Siroky, J., Smajek, J., Snoeys, W., Stefanovitch, R., Sziklai, J., Taylor, C., Tcherniaev, E., Turini, N., Vacek, V., Welti, J., Williams, J., Wyszkowski, P., Zich, J., Zielinski, K.“…Using dedicated $\beta ^{*}=90~\hbox {m}$ beam optics, the Roman Pots were inserted very close to the beam. …”
Publicado 2017
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228por Baldenegro Barrera, Cristian“…We also study jet-gap-jet events where the colliding protons remain intact and are detected with the Roman pots of TOTEM. A larger fraction $f_\text{CSE}$ is found in the latter subsample.…”
Publicado 2022
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229por Mlinarevic, Toni“…We describe the ATLAS Forward Proton ‘Roman Pot’ Detectors (AFP and ALFA), including their performance and status. …”
Publicado 2023
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230“…However, the jet data from CDF with a ``Roman pot'' trigger are substantially lower than the results of our calculations; if confirmed, this would signal a breakdown of hard-scattering factorization.…”
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231por CERN. Geneva“…Besides, detectors close to the beam axis need to be installed in "Roman Pots" located about 150 m from the collision point. …”
Publicado 2000
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232por Bossini, Edoardo“…The new proton timing detector, based on Ultrafast Silicon Detectors, is installed in theTOTEM Roman Pots, at 220 meters from the interaction point 5 at LHC. …”
Publicado 2019
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233
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234por Royon, Christophe“…It installed sets ofvertical roman pot detectors at about 147 and 220-240 meters from theinteraction point that have good acceptance in detecting intact protons inelastic interactions. …”
Publicado 2020
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235por Mapelli, A, Anghinolfi, F, Ask, S, Barrillon, P, Blanchot, G, Blin, S, Braem, André, Cheiklali, C, de La Taille, C, Di Girolamo, B, Efthymiopoulos, I, Faustino, J, Fournier, D, Franz, S, Grafström, P, Gurriana, L, Haguenauer, M, Hedberg, V, Heller, M, Hoffmann, S, Iwanski, W, Joram, C, Kocnar, A, Lavigne, B, Lundberg, B, Maio, A, Maneira, M J P, Marques, C, Mjörnmark, U, Conde-Muíño, P, Puzo, P, Rijssenbeeck, M, Santos, J P, Saraiva, J G, Seguin-Moreau, N, Soares, S, Stenzel, H, Thioye, M, Valladolid-Gallego, E, Vorobel, V“…Detector modules will be placed above and below the LHC beam axis in roman pot units at a distance of 240 m on each side of the ATLAS interaction point. …”
Publicado 2007
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236por Anghinolfi, F., Ask, S., Barrillon, P., Blanchot, G., Blin, S., Braem, A., de la Taille, C., Girolamo, B.Di, Efthymiopoulos, I., Faustino, J., Fournier, D., Franz, S., Grafström, P., Gurriana, L., Haguenauer, M., Hedberg, V., Heller, M., Hoffmann, S., Iwanski, W., Joram, C., Kocnár, A., Lavigne, B., Lundberg, B., Maio, A., Maneira, M.JP., Mapelli, A., Marques, C., Mjörnmark, U., Muíño, P.Conde, Puzo, P., Rijssenbeek, M., Saraiva, J.G., Seguin-Moreau, N., Soares, S., Stenzel, H., Thioye, M., Varouchas, D., Vorobel, V.“…The tracker will be located in so-called Roman Pot units at a distance of 240 m on each side of the ATLAS interaction point. …”
Publicado 2007
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237“…We also discuss how these configurations are modified in the presence of a non-zero Romans mass.…”
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238por Oliveri, Eraldo“…To achieve optimum forward coverage for charged particles emitted by the pp collisions in the interaction point IP5, two tracking telescopes, T1 and T2, will be installed on each side in the pseudorapidity region $3.1 \leq |\eta| \leq 6.5$ and Roman Pot stations will be placed at distances of 147 m and 220 m from the Interaction Point 5 (IP5). …”
Publicado 2010
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239“…The collimation efficiency is computed by intercepting the deflected halo with a massive collimator or with an imaging device installed into a Roman Pot. The leakage of the system is evaluated in the dispersion suppressor by means of movable aperture restrictions. …”
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240“…This allowed for measurements of very forward proton-proton scattering with roman pot detectors at 3 σ from the beam axis at acceptable background levels for about an hour. …”
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