Tungsten as HCal-material for a LC at multi-TeV energies CALICE AHCAL Meeting, DESY 17 July 2009 Christian Grefe for the Linear Collider Detector Group.

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Presentation transcript:

Tungsten as HCal-material for a LC at multi-TeV energies CALICE AHCAL Meeting, DESY 17 July 2009 Christian Grefe for the Linear Collider Detector CERN

Page 2 17 July 2009, Christian Grefe Outline Hcal with tungsten: simulation CERN Tungsten as HCal material Plans for a tungsten HCal prototype

Page 3 17 July 2009, Christian Grefe Why Tungsten? 3TeV Shorter Longitudinal Shower Size High energetic jets require more HCal material in terms of interaction lengths – to achieve better containment Strong constraints by coil – cost and feasibility Smaller Lateral Shower Size High energetic jets are more boosted PFA performance is decreasing Tungsten might solve both problems

Page 4 17 July 2009, Christian Grefe Tungsten HCal Simulations

Page 5 17 July 2009, Christian Grefe Simulation CERN Investigate what modifications are needed for the ILC-detector concepts in a CLIC-scenario For calorimeters this means calorimetric performance and in particular PFA performance Questions to answer: How many interaction lengths do we need? Which sampling frequency is optimal? Full detector and PFA studies (to be done) Readout cell sizes? Change magnetic field? Change aspect ratio of the detector?

Page 6 17 July 2009, Christian Grefe HCal-Stack Simulations Many different HCal-geometries with tungsten, steel and a combination of both, without changing the active parts (5.0 mm Scint mm G10) Dimensions: 5x5m and more than 25 λ in depths to guarantee shower containment Simulated 100k π + between 1 GeV and 300 GeV for each geometry This should cover the energy range of jet main constituents of events with #jets ≥ 3 TeV Defined active and dead layers – corresponding to different HCal, coil and tailcatcher sizes Defined simple shower variables: width, length, center, energy density, etc. Used a neural network (TMVA) to reconstruct the π + energy

Page 7 17 July 2009, Christian Grefe HCal-Stack Simulations “extremely deep”-HCal performance Linearity is better than 2% (not shown) “extremely deep”-case: Finer passive layers are better Steel performs better than tungsten CLIC-PH-Note, Speckmayer & Grefe (in preparation) TungstenSteel

Page 8 17 July 2009, Christian Grefe HCal-Stack Simulations Performance vs HCal depth (tungsten) The 4 points of each graph correspond to 6, 7, 8 and 9 λ For an HCal depth of around ~ 140 cm an absorber thickness of ~ 1 cm tungsten seems optimal This corresponds to ~ 8 λ; taking into account 1 λ of ECal, a 7 λ HCal appears to be sufficient for CLIC energies Stay away from the steep areas where leakage becomes the dominating factor CLIC-PH-Note, Speckmayer & Grefe (in preparation) E MC ~ 250 GeVE MC ~ 60 GeV

Page 9 17 July 2009, Christian Grefe HCal-Stack Simulations Performance vs HCal depth (tungsten vs steel) Steel yields a better performance than tungsten, but only for a significantly deeper HCal For a tungsten-steel sandwich structure (50% thickness each), the W-Fe- Scint case performs slightly better than the Fe-W-Scint case, because more of the electromagnetic signal reaches the active layers CLIC-PH-Note, Speckmayer & Grefe (in preparation) SteelSteel, Tungsten, Steel & Tungsten

Page July 2009, Christian Grefe HCal-Stack Simulations Impact of a Tailcatcher 0 λ implies no active material after the coil While the resolution is improved by adding a tailcatcher of ~1 λ the effect of an even bigger tailcatcher is negligible CLIC-PH-Note, Speckmayer & Grefe (in preparation) TungstenSteel

Page July 2009, Christian Grefe HCal Barrel Dimensions calculated for 18 fold symmetry ILD-flavorSiD-flavor 10mm W20 mm Fe10 mm W20 mm Fe layers R min [cm] R max [cm] Length [cm] weight [t] Channels (1cm x 1cm)3.4* * * *10 6 Channels (3cm x 3cm)3.8* * * *10 5 λ X0X

Page July 2009, Christian Grefe Properties of Tungsten

Page July 2009, Christian Grefe Tungsten Properties Pure tungsten  = 19.3 g/cm 3 λ = 9.94 cm, X 0 = 0.35 cm brittle and hard to machine Tungsten alloys with W > 90% + Cu / Ni / Fe  = 17 – 19 g/cm 3 λ ≈ 10 cm, X 0 ≈ 0.4 cm Well established production procedure Easy to machine Price ~ 70 Euro/kg (without machining)

Page July 2009, Christian Grefe Tungsten Alloys Tungsten is usually used in alloys for better mechanical properties and machinability Several ferromagnetic (W,Ni,Fe) or paramagnetic (W,Ni,Cu) alloys are available

Page July 2009, Christian Grefe Tungsten Alloys

Page July 2009, Christian Grefe Tungsten Alloys

Page July 2009, Christian Grefe Tungsten Production Starting from powder, the metal mixture is first pressed and then scintered and finally machined Each production step increases the density The main limitations are: Plate size – limited by the size of the oven Thin plates – it has to be somehow stable after pressing todays limitations are around 10 x 500 x 800 mm 3 We are in contact with Industry to address these issues

Page July 2009, Christian Grefe Tungsten HCal Prototype

Page July 2009, Christian Grefe Tungsten HCal Prototype Some questions can not be answered by simulations and need a real prototype: Physics performance: Verify GEANT4 simulations (resolution, etc.) Include noise terms – do slow neutrons spoil the signal? Test PFA performance Tungsten plate production process: Production of large and thin plates Quality of machining? Flatness of plates? Mechanical questions: Test assembly in view of a full HCal segment

Page July 2009, Christian Grefe 20 GeV π+ using 10 mm W plates Tungsten HCal Prototype If possible use existing CALICE active modules Test Scintillator and RPC together with tungsten Start with a smaller prototype (less than 1x1 m 2 plate-size) Fill up unused space with Steel plates to have a veto signal and use only fully contained showers Veto Calorimeter Beam P. Speckmayer

Page July 2009, Christian Grefe 20 GeV π+ using 10 mm W plates Tungsten HCal Prototype If possible use existing CALICE active modules Test Scintillator and RPC together with tungsten Start with a smaller prototype (less than 1x1 m 2 plate-size) Fill up unused space with Steel plates to have a veto signal and use only fully contained showers Veto Calorimeter Beam P. Speckmayer

Page July 2009, Christian Grefe Tungsten HCal Prototype Cutting on the shower size biases the physics: Small showers means high electromagnetic fraction, but we want to investigate hadronic performance! Getting the lateral size right is more important than getting the depth right Can select by first interaction without bias on the hadronic part of the shower Easy to add more layers Need to understand correlation of shower content and shower size → ongoing studies Some rough numbers: Minimum plate size seems to be 50x50 cm 2 (low energy tests) Minimum length ~50 cm

Page July 2009, Christian Grefe Conclusion

Page July 2009, Christian Grefe Conclusion and Outlook Simulations with tungsten λ total (ECal + HCal) seem to be sufficient for π + up to 300 GeV For the given HCal dimensions an ~10mm W-absorber seems optimal 1 λ Tailcatcher is useful Estimations based on “conventional” calorimetry and leakage Need to verify with PFA performance Production of the tungsten plates seems possible Tungsten HCal prototype If we seriously want to investigate a tungsten HCal option a prototype is necessary Possible extension for CALICE-program Strong interest from CERN – We need your help!