SND@LHC

preprint2020arXivOpen access
SHiP CollaborationC. AhdidaA. AkmeteR. AlbaneseA. AlexandrovM. AndreiniA. AnokhinaS. AokiG. ArduiniE. AtkinN. AzorskiyJ. J. BackA. BagulyaF. Baaltasar Dos SantosA. BaranovF. BardouG. J. BarkerM. BattistinJ. BaucheA. BayV. BaylissG. BencivenniA. Y. BerdnikovY. A. BerdnikovM. BertaniP. BestmannC. BetancourtI. BezshyikoO. BezshyykoD. BickS. BieschkeA. BlancoJ. BoehmM. BogomilovI. BoiarskaK. BondarenkoW. M. BoniventoJ. BorburghA. BoyarskyR. BrennerD. BretonL. R. BuonocoreV. BüscherA. BuonauraS. BuontempoS. CadedduA. CalcaterraM. CalvianiM. CampanelliV. CanaleM. CasolinoF. CeruttiN. CharitonidisP. ChauJ. ChauveauA. ChepurnovM. ChernyavskiyK. -Y. ChoiA. ChumakovP. CiambroneV. CiceroL. CongedoK. CornelisM. CristinzianiA. CrupanoG. M. DallavalleA. DatwylerN. D'AmbrosioG. D'AppollonioR. de AsmundisP. T. De Bryas Dexmiers D'ArchiacJ. De Carvalho SaraivaG. De LellisM. de MagistrisA. De RoeckM. De SerioD. De SimoneL. DedenkoP. DergachevA. Di CrescenzoL. Di GiulioN. Di MarcoC. DibH. DijkstraV. DmitrenkoS. DmitrievskiyL. A. DoughertyA. DolmatovD. DomeniciS. DonskovV. DrohanA. DubreuilO. DurhanM. EhlertE. ElikkayaT. EnikA. EtenkoF. FabbriO. FedinF. FedotovsG. FeliciM. FerrilloM. Ferro-LuzziK. FilippovR. A. FiniP. FonteC. FrancoM. FraserR. FresaR. FroeschlT. FukudaG. GalatiJ. GallL. GatignonG. GavrilovV. GentileB. GoddardL. Golinka-BezshyykoA. GolovatiukD. GolubkovA. GolutvinP. GorbounovD. GorbunovS. GorbunovV. GorkavenkoM. GorshenkovV. GrachevA. L. GrandchampE. GraveriniJ. -L. GrenardD. GrenierV. GrichineN. GruzinskiiA. M. GulerYu. GuzG. J. HaefeliC. HagnerH. HakobyanI. W. HarrisE. van HerwijnenC. HesslerA. HollnagelB. HosseiniM. HushchynG. IaselliP. IengoA. IulianoR. JacobssonD. JokovićM. JonkerI. KadenkoV. KainB. KaiserC. KamisciogluD. KarpenkovK. KershawM. KhabibullinE. KhalikovG. KhaustovG. KhoriauliA. KhotyantsevY. G. KimV. KimN. KitagawaJ. -W. KoK. KodamaA. KolesnikovD. I. KolevV. KolosovM. KomatsuA. KonoN. KonovalovaS. KormannshausI. KorolI. Korol'koA. KorzenevV. KostyukhinE. Koukovini PlatiaS. KovalenkoI. KrasilnikovaY. KudenkoE. KurbatovP. KurbatovV. KurochkaE. KuznetsovaH. M. LackerM. LamontG. LanfranchiO. LantwinA. LauriaK. S. LeeK. Y. LeeJ. -M. LévyV. P. LoschiavoL. LopesE. Lopez SolaV. LyubovitskijJ. MaalmiA. MagnanV. MaleevA. MalininY. ManabeA. K. ManagadzeM. ManfrediS. MarshA. M. MarshallA. MefodevP. MermodA. MianoS. MikadoYu. MikhaylovD. A. MilsteadO. MineevA. MontanariM. C. MontesiK. MorishimaS. MovchanY. MuttoniN. NaganawaS. NasybulinP. NininA. NishioA. NovikovB. ObinyakovS. OgawaN. OkatevaB. OpitzJ. OsborneM. OvchynnikovN. OwtscharenkoP. H. OwenP. PacholekA. PaoloniB. D. ParkG. PasseggioA. PastoreM. PatelD. PereymaA. Perillo-MarconeG. L. PetkovK. PetridisA. PetrovD. PodgrudkovV. PoliakovN. PolukhinaJ. Prieto PrietoM. ProkudinA. ProtaA. QuerciaA. RademakersA. RakaiF. RatnikovT. RawlingsF. RediS. RicciardiM. RinaldesiVolodymyr RodinViktor RodinP. RobbeA. B. Rodrigues CavalcanteT. RoganovaH. RokujoG. RosaT. RovelliO. RuchayskiyT. RufM. Sabate GilarteV. SamoylenkoV. SamsonovF. Sanchez GalanP. Santos DiazA. Sanz UllA. SaputiE. S. SavchenkoJ. S. SchliwinskiW. Schmidt-ParzefallO. SchneiderG. SekhniaidzeN. SerraS. SgobbaO. ShaduraA. ShakinM. ShaposhnikovP. ShatalovT. ShchedrinaL. ShchutskaV. ShevchenkoH. ShibuyaL. ShihoraS. ShirobokovA. ShustovS. B. SilversteinS. SimoneR. SimonielloM. SkorokhvatovS. SmirnovJ. Y. SohnA. SokolenkoE. SolodkoN. StarkovL. StoelM. E. StramagliaD. StrekalinaD. SukhonosY. SuzukiS. TakahashiJ. L. TastetP. TeterinS. Than NaingI. TimiryasovV. TioukovD. TommasiniM. ToriiN. TosiF. TramontanoD. TreilleR. TsenovS. UlinE. UrsovA. UstyuzhaninZ. UteshevG. Vankova-KirilovaF. VannucciC. VendeuvreV. VenturiS. VilchinskiHeinz VinckeHelmut VinckeC. VisoneK. VlasikA. VolkovR. VoronkovS. van WaasenR. WankeP. WertelaersO. WilliamsJ. -K. WooM. WurmS. XellaD. YilmazA. U. YilmazerC. S. YoonYu. ZaytsevJ. Zimmerman

Abstract

We propose to build and operate a detector that, for the first time, will measure the process pp→νXpp\toνX 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.

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