1. TESLA R&D: Forward Region Achim Stahl DESY Zeuthen Cracow Tel Aviv Minsk Prague Colorado Protvino UC London Dubna

2. GeV The Forward Region  maximum hermiticity  precision luminosity  shield tracking volumne  monitor beamstrahlung TDR design

3. GeV The Forward Region  maximum hermiticity  precision luminosity  monitor beamstrahlung  shield tracking volumne small bunches  high electric fields  huge beamstrahlung ≈ 20 TeV per side

4. Proposal: 2-Year R&D Program Instrumentation of the very forward region LumCal Design & Simulation Exp. Limitations Physics Needs BeamCal Lab Tests & Simulation Identify most suitable technology

5. Lumi: Detector Requirements Goal: ΔL/L: 10 -4 (exp.) ΔL/L: 10 -4 (theo.) Ref: OPAL (LEP) ΔL/L: 3.4 x 10 -4 (exp.) ΔL/L: 5.4 x 10 -4 (theo.) LumCal IP < 4.5 μm < 0.7 mm

6. LumCal Design TDR design: ΔL/L 10 -4 impossible cut-off 5 MeV

7. New Design LumCal BeamCal LumCal BeamCal LumCal BeamCal

8. Lumi Simulations Full detector simulation Event reconstruction center-of-gravity algorithm necessary segmentation:  32 rings in polar angle  48 sectors in azimuth  30 segments in depth

9. Lumi Simulations Realistic Monte Carlo  rad. corrections (BHWIDE)  beamstrahlung (CIRCE)  full detector simulation  reconstruction of events

10. Laser Alignment System New collaborator: Jagiellonian Univ. Cracow Photonics Group Work just started: reconstruction of Ne-Ne laser spot on CCD camera

11. Substantial effort to improve prediction Goal: complete, massive 2-loop calculation Bhabha Cross Section: Theory Collaboration: Tord Riemann with Jochem Fleischer Janusz Gluza Alejandro Lorca Oleg Tarasov Anja Werthenbach Good progress:  1-loop done (in SM) working FORTRAN code  2-loop: |1-loop| 2 + |Born x 2-loop| 2 |1-loop| 2 near to finished numerically 2-loop under study, some progress  real corrections: interest from Jadach/Waş

12. GeV Beam Monitoring Beamstrahlung is sensitive to the machine parameters  e + e - pairs in BeamCal  photons downstream Advantage of cold technology : large bunch spacing information can be used for feedback

13. nominal our precisionBeam Diag. Bunch width x Ave. Diff. 553 nm 1.2 nm 2.8 nm ~ 10 % Bunch width y Ave. Diff. 5.0 nm 0.1 nm Shintake Monitor Bunch length z Ave. Diff. 300 μm 4.3 μm 2.6 μm ~ 10 % Emittance in x Ave. Diff. 10.0 mm mrad 1.0 mm mrad 0.4 mm mrad ? Emittance in y Ave. Diff. 0.03 mm mrad0.001 mm mrad ? Beam offset in x Beam offset in y 0 7 nm 0.2 nm 5 nm 0.1 nm Horizontal waist shift Vertical waist shift 0 μm 360 μm 80 μm 20 μm None First Results (over optimistic!) detector: realistic segmentation, ideal resolution single parameter analysis, bunch by bunch resolution

14. Hermeticity: 2-photon-veto Simulation: identify electrons close to the beam in the presence of large beamstrahlung min. detectable energy: 100 GeV for 250 GeV beam analysis with realistic beam background including ground motion & feed back

15. Technologies for BeamCal  Sandwich: W / Si  Sandwich: W / diamond  Sandwich: W / gas ionisation chambers  Xtals with ultrathin phototriodes  Xtals with fiber readout radiation hardness ?  next slides good progress, better suited for  -detection? waiting for funding (UK) no funding @ DESY, looking for new collaborator

16. Gas Calo: Beamtests sampling calorimeter  tungsten absorbers  gas ionisation chambers  extreme radiation hardness  detect beamstrahlung on downstream collimator

17. Diamond Sensors 12 samples (12 x 12 mm) Frauenhofer Inst. Freiburg measured: I-V characteristics charge collection distance to be done: homogeniety 1 st mono-crystal (2 x 3 mm) Almazot / Minsk under investigation expect diamonds from Dubna soon

18. SensorR(Average) ccd Up 500V ccd Up 800V ccd Down 500V ccd Down 800V 114.60E+1337 35 123.20E+1427303543 138.88E+1121 2533 215.92E+1417 24 227.39E+14910 (700V)911 233.93E+141013912 311.04E+1133 (400V) 28 325.12E+1350 57 334.63E+1352584954 415.12E+1148 45 (400 V) 424.35E+14 435.24E+13606554 Charge Collection Distance

19. Conclusions Good progress in most areas