The TESLA Project Ties Behnke, DESY TESLA: The machine " status of cavity development " RF system " FEL at TESLA " accelerator layout A Detector for particle physics at TESLA American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 1 TESLA TESLA The TESLA Collaboration INFN Legnaro a machine concept: superconducting acceleration modules a collaboration: build and operate a test accelerator TTF a proposal to build such a machine INR Troitsk MEPhI Moscow Uni Hamburg Uni Rostok BESSY Berlin American Linear Collider Workshop, Baltimore, March 2001 Yerevan Physics Institut Ties Behnke: The TESLA project 2 TESLA Basic Concept superconducting solid Nb cavities E(acc) ~ 25 MV/m, T=2K Long RF pulses ( ~ 1 ms) low RF peak power (200 kW/m) long bunch train with large interbunch spacing Low RF frequency (1.3 GHz) small wakefields The TESLA acceleration structures: Overall design compatible with E(cms) = 91 .... 800 GeV baseline design and parameters for 500 GeV American Linear Collider Workshop, Baltimore, March 2001 module geometry module length V(acc) Fill factor RF/module 219 9−cell structure 1.04 23.40 78.00% 4x7 superstructure 3.23 22.00 89.00% 675 Ties Behnke: The TESLA project 3 TESLA Parameters TESLA 500 GeV parameters American Linear Collider Workshop, Baltimore, March 2001 TESLA 800 GeV parameters Ties Behnke: The TESLA project 4 TESLA Bunch Structure Main characteristics: long bunch trains, even longer times between bunch trains 500 GeV 5 Hz x 2820 x 2.0 1010 800 GeV 3 Hz x 4568 x 1.4 1010 possibility of orbit corrections within single bunch train (fast feedback system) Head on collisions are possible Bunch collisions are well separated in detector American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 5 Status of Cavities Development TESLA Test Facility (TTF) Goals: Phase I: development of acceleration modules proof of principle of operation of SC linac at high (> 22.5 GeV) gradient proof of principle for SASE FEL in the VUV (60 nm) cavity performance per production series Tesla 500 American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 6 American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 7 RF Power: Klystrons TH 1801 multi beam Klystron High power (10 MW peak) Low voltage (117 kV) High efficiency (65 %) Long pulse (1.5 ms) System has been fabricated in industry Is now being used at the TTF LINAC American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 8 Lorentz Force Deformation Problem: Cavity deform under the Lorentz force at high gradient Cavity changes its shape cavity is detuned first successful test on cavity C45 at 20 MV/m solution: active compensation using piezo−crystal l = 39mm V(max)= 150 V f(max) = 500 Hz piezo actuator American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 9 The Free Electron Laser at TTF TTF LINAC is used to drive a SASE FEL Goal I: Proof of Principle for VUV FEL Goal II: Operation of user facility after 2003 American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 10 The TTF FEL February 2000: observe first lasing at <100 nm Since then: systematic studies very reliable and reproducible behaviour continuous reduction of the frequency Main radiation characteristics have been found CCD image of the FEL beam: American Linear Collider Workshop, Baltimore, March 2001 Signal development Ties Behnke: The TESLA project 11 The TTF FEL Since observation of first lasing: continuous further development of the system towards: FEL operation: brilliance vs energy Smaller wavelength better reproducibility higher brilliance Development of X−ray energy American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 12 Overall TESLA Layout TESLA tunnel: diameter 5.50 m Overall collider layout: DESY American Linear Collider Workshop, Baltimore, March 2001 Westerhorn Ties Behnke: The TESLA project 13 Collider Layout: Injector TESLA injector complex: Laser driven electron guns Three separate guns for Unpolarised Polarised FEL beam Electron polarisation is part of the baseline program American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 14 Collider Layout: Positron Source Positron source: use incoming electron beam as a source of photons produce positrons Small degradation of quality of beam is acceptable Allows very high positron currents Possibility of positron polarisation SLC TESLA No of positron per pulse 4.00E+010 5.60E+013 No of bunches per pulse 1 2820 Pulse duration 3 ps 0.95 ms Bunch spacing 8.3 ms 337 ns Repetition frequency 120 Hz 5 Hz American Linear Collider Workshop, Baltimore, March 2001 Expected positron polarisation: between 45 and 60% at (nearly) full intensity Need to build a helical undulator (technologically challenging) Positron Polarisation is not part of the baseline design Ties Behnke: The TESLA project 15 The Interaction Region Conceptual layout of the interaction region(s): 2. IR not part of baseline design IR for gamma gamma electron gamma electron electron electron positron 34 mrad crossing angle IR for primary electron positron program (or electron electron) no crossing angle American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 16 Fast Feedback at the IP Long bunch trains, long times between bunches: Feedback system within bunch train possible to stabilise the luminosity Act on angle Act on offset After about 90 bunches: reduction by factor 1000 Train to train tolerance of final doublet limiting the luminosity loss to 10%: 200nm American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 17 A TESLA Site near Hamburg American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 18 Cost Project will be presented to the public at the TESLA Colloquium on March 23/24 including cost American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 19 A Detector for TESLA Large detector for Optimal tracking Optimal energy flow High central magnetic field (4T) High granularity ECAL High granularity HCAL Both inside the coil! Instrumentation down to very small angles: hermeticity! Iron return yoke instrumented as muon system American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 20 Detector Overview Overall detector view: Enlarge view of the inner tracking system: American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 21 The VTX Detector High precision detector close to the beam pipe (R(min) = 1.5 cm) Several technologies are under discussion Active pixel sensors (a la LHC technology) CCD based sensors (SLD technology) CMOS based sensors (new development) SI ladders are "stretched" The CCD version: American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 22 Central Tracking Detector: TPC Sideview of the TPC Fieldcage / TPC vessel: Light composite walls Modelled after ALEPH / ALICE fieldcage Max Voltage: 100 kV American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 23 Readout Technology: GEMs Use GEM (or similar) system for signal amplification and readout: True 2−D readout possible Compact, thin endplates Mechanically "simple" Gains > 10000 have been observed Measured gain in a 2−GEM structure American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 24 Performance of the Tracking System Overall tracking performance: Full pattern recognition in TPC, VXT, FTD, FCH Sophisticated merging of different subdetectors Final clean−up step Based on LEP software with further developments Efficiency > 98.5% Secondary vertex finding Based on SLD ZVTOP Combined with OPAL NN approach Tuned on Z−data American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 25 Calorimetry: ECAL Both ECAL and HCAL are inside the coil ECAL: fine grained SI−W calorimeter Module length: 160 cm transverse: 1x1 cm longitudinal: 30 x 0.4 X W 12 x 1.2 X W About 30 million channels American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 26 Calorimetery: HCAL HCAL: "tile calorimeter" with iron as absorber, scintillator tiles as active medium Readout of tiles with clear fibres to a place outside the barrel 16 fold symmetry in Phi 9 longitudinal samples transverse sampling > 5x5 cm Energy resolution for tile or alternative digital option American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 27 Calorimeter Performance Thorough evaluation difficult and needs significant software development Some preliminary results: The calorimeter is optimised for the measurement of the energy flow in the event: Need exellent separation of Mass resolution of charged and neutral particles the visible mass of Excellent connection to the the Z in hadronic tracker information Z decays Excellent measurement of the longitudinal shower shape Goal: Energy flow resolution of 30% HHZ events: separation of signal and background for different energy flow resolution American Linear Collider Workshop, Baltimore, March 2001 a) LEPtype resolution 60%(1+|cos θ|) b) 30% resolution Ties Behnke: The TESLA project 28 Calorimeter Performance Separation of WWZ: " Standard performance b) resolution 60% American Linear Collider Workshop, Baltimore, March 2001 " High resolution calorimeter a) resolution 30% Performance Ties Behnke: The TESLA project 29 Backgrounds Beam Beam backgrounds: Pairs Hadronic background neutrons 10 simulated pair particles Synchroton Radiation induced backgrounds Beam gas backgrounds Muon induced backgrounds Per BX: 129000 pairs (360 TeV total energy) Some numbers: SIT/FTD: O(20) hits / detector Photons into TPC: O(1300) Occupancy O(0.1%) Particles with E>3 MeV into ECAL: O(200) Hits from pairs/ BX on the vertex detector layers American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 30 Backgrounds: Neutrons Simulation of neutron backgrounds: FLUKA2000 & Pythia Full detector model in FLUKA Cross checked with Pythia Some fluxes in the detector: VTX FTD SIT TPC ECAL HCAL Yoke <1E09 <2E09 <7E08 (1MeV)/year/cm2 15000/BX neutrons/BX <10000/BX <10000/BX ~55000/BX Fluxes are not expected to be a problem for detector components American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 31 Overall Detector Performance Two particularly challenging examples: determine the detailed properties of the Higgs Reconstruction of the Higgs branching ratio into different flavours, as a function of the Higgs mass American Linear Collider Workshop, Baltimore, March 2001 Reconstruction of the Higgs Potential via ZHH events Combination of high luminosity and high precision detector allows reconstruction of complete picture eg of the Higgs. Ties Behnke: The TESLA project 32 Detector Mechanics First conceptual version of detector moving and installation: Open the endcap Yoke Retract the endcap calorimeters Move the TPC along z Acces the inner detectors Proposed cable routes out of the detector American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 33 The TESLA Research Campus Central laboratory site at km15 HEP experiment(s) XFEL laboratory Artists drawing of the HEP hall Aerial view of Ellerhoop American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 34 TESLA: Goals and Milestones Goals: Develop superconducting technology Use LINAC as driver for X−FEL Milestones reached: Routine production of cavities with > 25MV/m Cavities with >40MV/m as single cell cavities Construction and operation of TTF I Stable operation for > 8600 h Demonstrate SASE principle at <100 nm Successful development of klystrons, RF couplers, etc Development of the Physics Case 2 ECFA/DESY workshops with large and international attendance (total >10 workshop meetings) Milestone reached: TESLA TDR Part III (physics), PartIV (detector), Part VI (other research options) Continuation for two more years to Develop the physics studies further React to new developments Continue work on the detector (R&D efforts are starting) Continue the work on machine/ detector interface American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 35 TESLA: The Next Steps Presentation to the public: TESLA Colloquium Integrated HEP and FEL laboratory with site close to Hamburg Including cost estimate Detailed costing of accelerator costs Based on industrial studies and the experience gained at TTF The next steps: Operation of TTF I, upgrade to TTF II (2003) Formal proposal (TDR) March 2001 Evaluation of proposal by German Wissenschaftsrat during 2001 ECFA/DESY study on long term perspectives of particle physics in Europe (2000/2001) with similar studies in US and Asia ICFA study of the Global Accelerator Network concept (2000/2001) Cryostat Damping Ring Input Coupler SC Magnets Cryogenics Klystrons INFN INFN IN2P3 Spain TU Dresden DESY Modulators DESY Global accelerator Network Laboratory Operation, R&D American Linear Collider Workshop, Baltimore, March 2001 Operation, R&D Operation, R&D Ties Behnke: The TESLA project 36 American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 37 Conclusions TESLA: a proposal for a new large interdisciplinary research center Most technical problem are solved 500 GeV baseline design is "conservative" Energy upgrade potential is real HEP experimentation at TESLA is challenging Needs serious and significant Detector R&D Combination of HEP and FEL offers exciting new perspectives Plans: TESLA TDR now German Wissenschaftsrat: 2002 International technical review? American Linear Collider Workshop, Baltimore, March 2001 Ties Behnke: The TESLA project 38 A Global Accelerator Network Construct and operate future large accelerators in the framework of a global network Make projects part of the national programs of the participating countries Maintain the scientific and technical culture and know how in home labes, remain attractive for young people, yet contribute to and participate in large, unique projects Maintain and run accelerators to a large extend from participating labs Pull together world−wide competence, ideas, resources Capital investment is done at home Site selections becomes a less critical issue Put accelerator close to an existing laboratory: Make optimal use of existing experience, manpower, and infrastructure Specific financial obligations for the host country ICFA study findings: Global considerations: Need laboratory structure Host nation is essential Will bear a major fraction of the cost American Linear Collider Workshop, Baltimore, March 2001 Technical considerations: Project requires central management Host lab will have safety responsibility Remote operation is in principle feasible Local staff of approx. 200 is needed Ties Behnke: The TESLA project 39