Detector Technologies for CLIC
- Abusleme Hoffman, A.
- Parès, G.
- Fritzsch, T.
- Rothermund, M.
- Jansen, H.
- Krüger, K.
- Sefkow, F.
- Velyka, A.
- Schwandt, J.
- Perić, I.
- Emberger, L.
- Graf, C.
- Macchiolo, A.
- Simon, F.
- Szalay, M.
- van der Kolk, N.
- Abramowicz, H.
- Benhammou, Y.
- Borysov, O.
- Borysova, M.
- Joffe, A.
- Kananov, S.
- Levy, A.
- Levy, I.
- Eigen, G.
- Bugiel, R.
- Bugiel, S.
- Firlej, M.
- Fiutowski, T.
- Idzik, M.
- Moroń, J.
- Świentek, K.
- Terlecki, P.
- Brückman de Renstrom, P.
- Turbiarz, B.
- Wojtoń, T.
- Zawiejski, L.
- Firu, E.
- Ghenescu, V.
- Neagu, A.
- Preda, T.
- Boyko, I.
- Nefedov, Y.
- Rymbekova, A.
- Sapronov, A.
- Shelkov, G.
- Zhemchugov, A.
- Ruiz-Jimeno, A.
- Vila, I.
- Fullana, E.
- Fuster, J.
- Gomis Lopez, P.
- Perelló, M.
- Villarejo, M.
- Vos, M.
- Alozy, J.
- Alipour Tehrani, N.
- Arominski, D.
- Ballabriga Sune, R.
- Boyer, F.
- Brondolin, E.
- Buckland, M.
- Campbell, M.
- Dannheim, D.
- Dette, K.
- Duarte Ramos, F.
- Egidos Plaja, N.
- Elsener, K.
- Fiergolski, A.
- Fuentes Rojas, C.
- Grefe, C.
- Hynds, D.
- Klempt, W.
- Kremastiotis, I.
- Kröger, J.
- Kulis, S.
- Leogrande, E.
- Linssen, L.
- Llopart Cudie, X.
- Lucaci-Timoce, A.
- Munker, M.
- Musa, L.
- Nürnberg, A.
- Nuiry, F.
- Perez Codina, E.
- Pernegger, H.
- Petrič, M.
- Pitters, F.
- Quast, T.
- Redford, S.
- Riedler, P.
- Roloff, P.
- Sailer, A.
- Santin, E.
- Schnoor, U.
- Sicking, E.
- Sielewicz, K.
- Simoniello, R.
- Snoeys, W.
- Spannagel, S.
- Sroka, S.
- Ström, R.
- Valerio, P.
- van Dam, S.
- van der Kraaij, E.
- Vǎnát, T.
- Viazlo, O.
- Vicente Barreto Pinto, M.
- Weber, M.
- Williams, M.
- Wolters, K.
- Benoit, M.
- Iacobucci, G.
- Sultan, D.
- Bosley, R.
- Price, T.
- Watson, M.
- Watson, N.
- Winter, A.
- Goldstein, J.
- Green, S.
- Marshall, J.
- Thomson, M.
- Xu, B.
- Casse, G.
- Vossebeld, J.
- Coates, T.
- Salvatore, F.
- Repond, J.
- Xia, L.
- Kenney, C.
- Tomada, A.
DOIAbstract
The Compact Linear Collider (CLIC) is a high-energy high-luminosity linear electron-positron collider under development. It is foreseen to be built and operated in three stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively. It offers a rich physics program including direct searches as well as the probing of new physics through a broad set of precision measurements of Standard Model processes, particularly in the Higgs-boson and top-quark sectors. The precision required for such measurements and the specific conditions imposed by the beam dimensions and time structure put strict requirements on the detector design and technology. This includes low-mass vertexing and tracking systems with small cells, highly granular...
Add to ORKG