The Detector Francesco Forti, INFN and University, Pisa F.Forti - SuperB Detector 1 Detector Babar and Belle designs have proven to be very effective for BFactory physics Follow the same ideas for SuperB detector Try to reuse same components as much as possible Main issues Machine backgrounds – not much larger than in Babar/Belle Beam energy asymmetry – a bit smaller Strong interaction with machine design Some areas require moderate R&D and engineering developments to improve performance A SuperB detector is possible with today’s technology Baseline is reusing large (expensive) parts of Babar (or Belle) Quartz bars of the DIRC Barrel EMC CsI(Tl) crystal and mechanical structure Superconducting coil and flux return yoke. Small beam pipe technology Thin silicon pixel detector for first layer Drift chamber CF mechanical structure, gas and cell size Photon detection for DIRC quartz bars Forward PID system (TOF or focusing RICH) Forward calorimeter crystals (LSO) Minos-style scintillator for Instrumented flux return Electronics and trigger – need to revise Bfactory “½-track” trigger style Computing – large data amount More details in: F.Forti - SuperB Detector www.pi.infn.it/SuperB/node/159 - SuperB Italy Meeting on detector R&D indico.lal.in2p3.fr/conferenceDisplay.py? confId=167 – Paris workshop (May 9-11) 2 Detector Layout – Reuse parts of Babar (or Belle) BASELINE OPTION F.Forti - SuperB Detector 3 SuperB Detector R&D Overall goals of detector R&D organization: Advance the R&D activity as coherently as possible, without duplication of effort and covering all relevant issues Start creating the infrastructure and doing the work needed for a Technical Design Report (time scale 1-2 years) Create the software infrastructure to perform simulations and physics studies for the optimization of the detector design Prepare the ground for the formation of a collaboration (time scale 1 year) Provide a structure to prepare funding applications Provide and entry point for new groups wishing to join F.Forti - SuperB Detector 4 R&D Organization Detector R&D Co-conveners Subsystems R&D conveners, tentative, open. Hopefully more than one convener per system F.Forti, B.N.Ratcliff MDI – Calderini SVT – Rizzo + DCH – PID – Leith + EMC – Hitlin + IFR – Calabrese + Electronics – Trigger/DAQ – Computing – Morandin + Testbeams coordinator Software coordinator F.Forti - SuperB Detector 5 Groups interests and activities System Italiani SVT PI, PV-BG, TO, MI, TS, (BO, PG, RM3) DCH LNF, (LE) PID PD Stranieri Maryland Triumph, SLAC SLAC, Ljubljana, BINP, Orsay? EMC PG, RM1 Caltech, UK, Germany?, Canada IFR FE, PD, RM1 Ohio? Trigger/DAQ BO, NA, TO SLAC + US Computing PD, FE, TO, BO, PI SLAC + US, UK, Germany ? Software RM2, FE?, PI, RM1 F.Forti - SuperB Detector ...... 6 Backgrounds Dominated by QED cross section Low currents / high luminosity Beam-gas are not a problem SR fan can be shielded F.Forti - SuperB Detector 7 We have an IR design coping with main BKG source SuperB Interaction Region 20 Radiative BhaBha B0H 10 B0L QF1 QD0H B00H B00L QD0 QD0 QF1 cm 0 3.5 -10 2 3 1.5 1 0.5 1 1.52 3 QD0H 4 2.5 3.5 0.5 4.5 5 6 6.5 2.5 QF1 QF1 -20 -3 5.5 B0H B0L -2 -1 0 m 1 2 3 M.Sullivan M.Sullivan Nov. Nov. 13, 13, 2006 2006 SB_IT_ILC_G3_300 SB_IT_ILC_G3_300 Need serious amount of shielding to prevent the produced shower from reaching the detector. F.Forti - SuperB Detector 8 Asymmetry and beam pipe radius Lower boost advantegeous for machine design 8 + 3.5 βγ=0.45 we can afford to have a lower boost only if the vertexing resolution is good: Babar: 9 + 3.1 βγ=0.56 , Belle: SuperB: 7 + 4 βγ=0.28 small radius beam pipe very little material in b.p. and first layer Vertex separation significance <Dz>/s(Dz) vs bg A b.p. with r ~1cm is highly desirable Present Babar value F.Forti - SuperB Detector 9 Beam pipe 1.0 cm inner radius Be inner wall 8 water cooled channels (0.3mm thick) Power ≈ 1kW Peek outer wall Outer radius ≈ 1.2cm Thermal simulation shows max T ≈ 55°C Issues ≈ 4um inside Au coating Connection to rest of b.p. Be corrosion Outer wall may be required to be thermally conductive to cool pixels F.Forti - SuperB Detector 10 SVT 20 cm Layer0 30 cm Baseline: use an SVT similar to the Babar one, complemented by one or two inner layers. 40 cm Question on whether it would possible/economical to add a layer between SVT and DCH, or move L5 to larger radius Cannot reuse because of radiation damage Beam pipe radius is paramount inner radius: 1.0cm, layer0 radius: 1.2cm, thickness: 0.5% X0 F.Forti - SuperB Detector 11 SVT SuperB R&D Two options for SuperB SVT Layer0 design in CDR: Basic MAPS R&D (sensor & electronics) partly included in the SLIM5 project (GRV-PRIN) Striplets option: well established technology, less robust against background occupancy. CMOS MAPS options: more robust against background occupancy but extensive R&D needed. Test of the prototype thin tracker (striplets and MAPS) in a test beam in 2008 Some aspects of Layer0 design from CDR (system/mechanical aspects) are not covered in SLIM5 (details in next slide) People involved in the project: SLIM5 group: PI, PV/BG,TS, T0, (TN), BO MI (BaBar+Citterio/Alimonti/Coelli) just joined the effort. + RM3 F.Forti - SuperB Detector 12 DCH Basic technology adequate. Cannot reuse BaBar DCH because of aging Baseline: Same gas, same cell shape Carbon fiber endplates instead of Al to reduce thickness Need to do complete background estimate Attività 2008 a LNF Options/Issues to be studied: Miniaturization and relocation of readout electronics Critical for backward calorimetric coverage Conical endplate Further optimization of cell size/gas simulare dettagliatamente i fondi attesi nella camera, e studiare con Garfield configurazioni di cella e miscele di gas alternative Testare le nuove miscele e geometrie di cella su un piccolo prototipo di camera a drift costruire un tracciatore compatto con risoluzioni spaziali O(50μm) estrapolate nel prototipo di camera, da usare anche alla Beam Test Facility (BTF) dei LNF (e± da 500 MeV/c). F.Forti - SuperB Detector 13 Particle ID Barrel PID essential for hadron PID above ~0.7GeV. DIRC baseline Quartz bars are OK and can be reused Almost irreplaceable PMTs are aging and need to be replaced Keep mechanical support Barrel Options Readout options motivated by reduction of background generated in SOB SOB: Faster PMTs using the standoff box and water coupling Smaller SOB: Pixilated MaPMTs and fused silica coupling No SOB: Focusing readout with pixilated MaPMTs Already active groups: SLAC, Ljubljana, BINP Attività a PD Test di PMT e SiPM F.Forti - SuperB Detector 14 Forward/Backward PID option Extending PID coverage to the forward and backward considered Possibly useful, physics case needs to be established quantitatively Serious interference with other systems cause displacement of front face of EMC require miniaturization and displacement of DCH electronics 2+2cm aerogel TOF seems the only viable option Technologies Aerogel-based focusing RICH 4cm aerogel single index Material in front of the EMC Needs space Focusing configuration – data May 10, 2007 SuperB V Peter Križan, Ljubljana Working device Requires significant space (>25 cm) Time of flight Need about 10ps resolution to be competitive with focusing RICH 15-20ps OK. 10ps seems to be achievable, although not easy F.Forti - SuperB Detector 15 EMC Barrel CsI(Tl) crystals Still OK and can be reused (the most expensive detector in BaBar) Baseline is to transport barrel as one device Forward Endcap EMC Various other transportation options BaBar crystal are damaged by radiation and need to be replaced Occupancy at low angle makes CsI(Tl) too slow No doubt we need a forward calorimeter Backward EMC option Because of material in front will have a degraded performance Maybe just a VETO device for rare channels such as Btn. Physics impact needs to be quantitatively assessed DIRC bars are necessarily in the middle DCH electronics relocation is critical for the perfomance Active group in CALTECH (Ren-yuan Zhu) Attività a PG + RM1 Test di PMT e SiPM F.Forti - SuperB Detector 16 Forward EMC crystals Both pure CsI and LSO could be used in the forward EMC LSO more expensive, but more light, more compact, and more radiation hard Use LSO as baseline Now LSO is available industrially Cost difference still significant, but not overwhelming. Gives better performance Leaves PID option open CsI option still open in case of cost/availability issues Baskward calorimeter Keep as an option Could be less performant Backward endcap Barrel extension Lead – scintillator ? Benchmark physics gain F.Forti - SuperB Detector 17 IFR and steel BaBar configuration has too little iron for m ID > 6.5 lI required; 4-5 available in barrel Fine segmentation overdid KL efficiency optimization Focus on m ID : fewer layers and more iron Is it possible to use the IFR in KL veto mode ? Baseline: Fill gaps in Babar IFR with more iron Leave 7-8 detection layers Need to verify structural issues Scintillator bars à la MINOS because rates in the 100Hz/cm2 range Cost effectiveness of steel reuse needs to be fully assessed F.Forti - SuperB Detector 18 IFR Cavoto Attività a FE, PD, RM1 Studi sulle fibre WLS: Tipo di fibra: circolari o quadrate ( eff. Intrappolamento 30% maggiore) Vari diametri (0.8, 1.0, 1.2 mm) e concentrazioni (150, 175, 200 ppm) Velocita’ di risposta: Kuraray-T11 (≈10 ns), Saint-Gobain-BCF 92 (≈2.7ns) Studi sui vari tipi di scintillatore: Numero di fibre minimo per la raccolta di una quantita’ sufficiente di luce Forma dello scintillatore: rettangolare con solchi in superficie o interni (co – estrusi) Studi e misure sui SiPM/MPPC: Verifica di: Guadagno, dark counts rate, stabilita’ del guadagno vs V and T Studi di invecchiamento: curva caratteristica I0-V, guadagno, dark counts misurati periodicamente (qualche giorno) dopo esposizione del dispositivo a luce verde Test di irraggiamento Misura della variazione dei vari parametri per diversi dispositivi Prime misure su sistemi completi scintillatore + fibra + photodetector con raggi cosmici/ test beam: Quantita’ di luce, efficienza di rivelazione, risoluzione temporale/spaziale F.Forti - SuperB Detector 19 Electronics and Trigger/DAQ L1 Trigger rate of 100-150KHz Unless a hardware Bhabha rejector is developed Up from 5KHz current Babar rate Some electronics could be reusable The bulk of the electronics is obsolete and unmaintainable Especially front-end cards, maybe power supplies Should be remade with state-of-theart technology Clearly a major cost driver Costed using recent experiments experience (LHC) Attività a BO + NA Requirements Architecture L1 buffer FPGA based Trigger Control L1 accept Detector FE Optical links L1 Trigger L1 Buffer F.Forti - SuperB Detector L3 Trigger IP Datagram L3 Trigger Farm 20 Computing Computing model extrapolated from Babar Scales with luminosity Requires distributed computing on the grid Attività in FE, PD, TO, BO, PI • valutazione risorse di calcolo e infrastrutture di un centroTier0 per SuperB • definizione e supporto di un insieme di strumenti collaborativi • supporto alle attività della VO SuperB in Grid • organizzazione delle risorse di calcolo per il TDR F.Forti - SuperB Detector 21 The SuperB Process International SuperB Study Group on International steering committee established, chaired by M.A.Giorgi. Members from Physics case, Machine, Detector Canada, France, Germany, Italy, Russia, Spain, UK, US Regular interaction with Japan, although not formalized Regular workshops Five workshop held (2 in Frascati, 1 in SLAC, 1 Villa Mondragone, 1 Paris) SuperB Meeting at Daresbury Accelerator retreat at SLAC in 2006 Accelerator Retreat at SLAC Sep 17-21, 2007 Conceptual Design Report Ready, printed and distributed. Describe Physics case, Accelerator, Detector, including costing International review ongoing More information: www.pi.infn.it/SuperB http://www.pi.infn.it/SuperB/seminars F.Forti - SuperB Detector 22 CDR Ready !!!! The CDR of SuperB is ready! INFN/AE-07/02, SLAC-R-856, LAL 07-15 Available at: www.pi.infn.it/SuperB arxiv.org/abs/0709.0451 476 pages Printed and available Copies can be requested from [email protected] F.Forti - SuperB Detector 23 Signatures: some numbers 320 Signatures; 85 institutions Drop Page Fields Here Signatures breakdown by country 174 Babar members 65 non Babar exper. Australia, 1 Canada, 7 Experimentalists 75% Signatures Theorists 13% USA, 70 France, 21 Germany, 11 Israel, 2 Accelerator physicists 12% UK, 24 Switzerland, 4 Spain, 12 Slovenia, 5 Italy, 137 Russia, 18 ROC, 3 Norway, 1 Japan, 4 Signatures breakdown by type Signatures by country Dropbreakdown Series Fields Here F.Forti - SuperB Detector 24 CDR Review An International Review Committee has been appointed by INFN. The review is scheduled for Nov 6-7, 2007. A first report is expected end 2007 The final report foreseen in spring 2008 After the results of the LNF test of crab waist foreseen in fall 2007 Already presented to ECFA in the summer John Dainton – UK/Daresbury, chair Jacques Lefrancois – F/Orsay Antonio Masiero – I/Padova Rolf Heuer – D/ Desy Daniel Schulte – CERN Abe Seiden – USA/UCSC Young-Kee Kim – USA/FNAL Hiroaki Aihara – Japan/Tokyo Very positive reaction Presentation to the CERN strategy group foreseen in spring 2008 Coordinates all projects in european HEP for research infrastructure INFRA-2007-2.2.1.33: Projects in the European strategy for particle physics (CERN Council) F.Forti - SuperB Detector 25