The SHiP Collaboration

C. Ahdida, A. Akmete,R. Albanese, A. Alexandrov,A. Anokhina,S. Aoki,G. Arduini,E. Atkin, N. Azorskiy,J. J. Back, A. Bagulya,F. Baaltasar Dos Santos,A. Baranov, F. Bardou,G. J. Barker, M. Battistin,J. Bauche,A. Bay, V. Bayliss,G. Bencivenni,A. Y. Berdnikov,Y. A. Berdnikov,M. Bertani,C. Betancourt, I. Bezshyiko, O. Bezshyyko,D. Bick, S. Bieschke,A. Blanco, J. Boehm,M. Bogomilov, I. Boiarska, K. Bondarenko,W. M. Bonivento,J. Borburgh,A. Boyarsky,R. Brenner, D. Breton,V. Büscher,A. Buonaura,S. Buontempo,S. Cadeddu,A. Calcaterra,M. Calviani,M. Campanelli,M. Casolino,N. Charitonidis, P. Chau,J. Chauveau,A. Chepurnov, M. Chernyavskiy, K.-Y. Choi, A. Chumakov,P. Ciambrone, V. Cicero,L. Congedo,K. Cornelis,M. Cristinziani, A. Crupano,G. M. Dallavalle, A. Datwyler, N. D’Ambrosio, G. D’Appollonio,R. de Asmundis,J. De Carvalho Saraiva,G. De Lellis,M. de Magistris,A. De Roeck,M. De Serio,D. De Simone, L. Dedenko, P. Dergachev,A. Di Crescenzo,L. Di Giulio,N. Di Marco,C. Dib,H. Dijkstra, V. Dmitrenko, S. Dmitrievskiy,L. A. Dougherty, A. Dolmatov,D. Domenici, S. Donskov, V. Drohan, A. Dubreuil, O. Durhan, M. Ehlert, E. Elikkaya, T. Enik,A. Etenko,F. Fabbri,O. Fedin, F. Fedotovs,G. Felici,M. Ferrillo,M. Ferro-Luzzi, K. Filippov,R. A. Fini,P. Fonte,C. Franco, M. Fraser, R. Fresa, R. Froeschl,T. Fukuda,G. Galati, J. Gall,L. Gatignon,G. Gavrilov, V. Gentile,B. Goddard, L. Golinka-Bezshyyko, A. Golovatiuk,D. Golubkov,A. Golutvin,P. Gorbounov, D. Gorbunov,S. Gorbunov, V. Gorkavenko,Y. Gornushkin, M. Gorshenkov, V. Grachev,A. L. Grandchamp,E. Graverini, J.-L. Grenard, D. Grenier, V. Grichine, N. Gruzinskii,A. M. Guler,Yu. Guz,G. J. Haefeli,C. Hagner,H. Hakobyan,I. W. Harris,E. van Herwijnen,C. Hessler, A. Hollnagel, B. Hosseini,M. Hushchyn,G. Iaselli, A. Iuliano,R. Jacobsson, D. Joković,M. Jonker,I. Kadenko,V. Kain, B. Kaiser, C. Kamiscioglu, D. Karpenkov, K. Kershaw,M. Khabibullin, E. Khalikov, G. Khaustov,G. Khoriauli, A. Khotyantsev,S. H. Kim,Y. G. Kim,V. Kim, N. Kitagawa, J.-W. Ko,K. Kodama, A. Kolesnikov,D. I. Kolev, V. Kolosov,M. Komatsu, A. Kono, N. Konovalova, S. Kormannshaus, I. Korol, I. Korol’ko,A. Korzenev, V. Kostyukhin,E. Koukovini Platia,S. Kovalenko, I. Krasilnikova,Y. Kudenko, E. Kurbatov, P. Kurbatov, V. Kurochka,E. Kuznetsova,H. M. Lacker,M. Lamont,G. Lanfranchi,O. Lantwin, A. Lauria,K. S. Lee,K. Y. Lee,J.-M. Lévy,V. P. Loschiavo,L. Lopes,E. Lopez Sola, V. Lyubovitskij, J. Maalmi, A. Magnan, V. Maleev,A. Malinin, Y. Manabe,A. K. Managadze, M. Manfredi, S. Marsh,A. M. Marshall, A. Mefodev,P. Mermod, A. Miano,S. Mikado,Yu. Mikhaylov,D. A. Milstead,O. Mineev,A. Montanari,M. C. Montesi,K. Morishima, S. Movchan, Y. Muttoni,N. Naganawa,M. Nakamura,T. Nakano, S. Nasybulin, P. Ninin, A. Nishio, A. Novikov, B. Obinyakov,S. Ogawa, N. Okateva,B. Opitz, J. Osborne, M. Ovchynnikov, N. Owtscharenko,P. H. Owen, P. Pacholek,A. Paoloni,B. D. Park,S. K. Park,A. Pastore,M. Patel, D. Pereyma, A. Perillo-Marcone,G. L. Petkov,K. Petridis,A. Petrov, D. Podgrudkov, V. Poliakov,N. Polukhina,J. Prieto Prieto, M. Prokudin,A. Prota, A. Quercia,A. Rademakers, A. Rakai,F. Ratnikov, T. Rawlings,F. Redi,S. Ricciardi, M. Rinaldesi,Volodymyr Rodin,Viktor Rodin,P. Robbe,A. B. Rodrigues Cavalcante,T. Roganova, H. Rokujo,G. Rosa,T. Rovelli, O. Ruchayskiy,T. Ruf, V. Samoylenko,V. Samsonov,F. Sanchez Galan,P. Santos Diaz,A. Sanz Ull,A. Saputi,O. Sato,E. S. Savchenko,J. S. Schliwinski,W. Schmidt-Parzefall,N. Serra, S. Sgobba,O. Shadura, A. Shakin, M. Shaposhnikov,P. Shatalov, T. Shchedrina,L. Shchutska,H. Shibuya, L. Shihora, S. Shirobokov, A. Shustov,S. B. Silverstein,S. Simone,R. Simoniello,M. Skorokhvatov, S. Smirnov,J. Y. Sohn, A. Sokolenko, E. Solodko,N. Starkov, L. Stoel,M. E. Stramaglia

semanticscholar(2019)

Cited 1|Views8
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Abstract
We propose to build and operate a detector that, for the first time, will measure the process pp → νX at the LHC and search for feebly interacting particles (FIPs) in an unexplored domain. The TI18 tunnel has been identified as a suitable site to perform these measurements due to very low machine-induced background. The detector will be off-axis with respect to the ATLAS interaction point (IP1) and, given the pseudo-rapidity range accessible, the corresponding neutrinos will mostly come from charm decays: the proposed experiment will thus make the first test of the heavy flavour production in a pseudo-rapidity range that is not accessible by the current LHC detectors. In order to efficiently reconstruct neutrino interactions and identify their flavour, the detector will combine in the target region nuclear emulsion technology with scintillating fibre tracking layers and it will adopt a muon identification system based on scintillating bars that will also play the role of a hadronic calorimeter. The time of flight measurement will be achieved thanks to a dedicated timing detector. The detector will be a small-scale prototype of the scattering and neutrino detector (SND) of the SHiP experiment: the operation of this detector will provide an important test of the neutrino reconstruction in a high occupancy environment. ar X iv :2 00 2. 08 72 2v 1 [ ph ys ic s. in sde t] 2 0 Fe b 20 20
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