17 May 2007LCWS analysis1 LCWS physics analysis work Paul Dauncey.

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Presentation transcript:

17 May 2007LCWS analysis1 LCWS physics analysis work Paul Dauncey

17 May 2007LCWS analysis2 The list shown previously Detailed sensor level simulation Understanding of sources of resolution Variation of resolution with parameters Linearity and resolution PFA “no harm” confirmation PFA improvements using fine granularity Not many volunteers; need to assign names today Work needs to be done by at latest the weekend before LCWS Programme of studies

17 May 2007LCWS analysis3 Needed to decide on the spacing size Yoshi fixed a Mokka version Anne-Marie did spacing study and found no threshold to GEANT4 small subpixel bug Decided to stay with 5  m spacing Now allows Giulio to proceed with sensor simulation Nigel to proceed with Mokka simulation production for single photons Marcel to proceed with Mokka simulation of qq and K L,n events Assume the simulation is independent of pixel circuit type (shaper/sampler, etc) Simulation will then be some “average” of the two? Sensor simulation

17 May 2007LCWS analysis4 How does the resolution depend on the parameters of the simulation? Want to evaluate the resolution as a function of Noise Threshold Charge diffusion values Dead area Cluster algorithm Pixel size (?) We should determine the “standard” values to use for these Noise: complicated by scale discrepancy GEANT4 deposits ~3.2keV in epitaxial layer; Giulio’s simulation gives 1300e  This corresponds to ~2.5eV/ e , known silicon value ~3.6eV/ e  E.g. take 30e  noise as 30/1300 ~ of MIP or assume 3200/3.6 ~ 900e  total so noise is 30/900 if MIP? Also, use shaper or sampler noise? What are the “best” values? Parameter dependence

17 May 2007LCWS analysis5 Want to build up from SimCalorimeterHits to fully digitised MAPS in stages See where the resolution comes from Want to also compare with diode pads option If different, need to understand why Ideally, would do this comparison on the same simulated events; removes fluctuations from showers, etc. Would be possible if energy deposits in bulk silicon are stored (as planned); is this done? Should be done with “standard” set of parameters and cuts Determine resolution for at least one representative energy SimCalorimeterHits analogue sum (i.e. only sampling fraction and shower fluctuations); this will be different for MAPS (using 15  m) and diode pads (using 300 or 500  m) of silicon. It is independent of cell size Digitized diode pads analogue sum, with reasonable threshold SimCalorimeterHits discriminated hit count, for MAPS, with and without clustering Digitised MAPS hit count, with and without clustering Understanding resolution

17 May 2007LCWS analysis6 Response as a function of energy From 0.5GeV to 500GeV Non-linearity from binary readout important Can do as a function of pixel size? At least for multiples of 50  m? Both linearity and resolution will depend on clustering Expect higher rate of 8-neighbour hits at high energies Value assigned to cluster containing these pixels will have big influence Could potentially optimise clustering for linearity or resolution; not both? Leakage into HCAL important also; how to handle this? Just look at ECAL? Worse resolution Try to include HCAL? Confuses what is due to MAPS and what not Linearity and resolution

17 May 2007LCWS analysis7 “No harm” check Need to ensure MAPS used like diode pads does not degrade PFA results Do a check which ignors benefits of MAPS Worse case; can only improve later Sum pixels (with clustering; adds complications at boundaries?) over area equivalent to diode pads Make faked-up CalorimeterHits from sums, with energy proportional to number of clusters These feed directly into PandoraPFA with no further changes (except truth-reco mapping needed?) Also, try to use benefits of MAPS in PFA directly Need to adapt PFA algorithm to benefit from finer granularity Large study so may not be possible in time available PFA studies