COT Simulation Validation Plots |
| current release | next release | description |
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Hit Resolution (Data versus Simulation) The default GARFIELD parameter controlling the hit resolution has been scaled by 0.4 to match the observed hit resolution. Hits over the entire cell are included in this plot. Tracks used are COT-only. |
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Hit Resolution (Data versus Simulation) Same as above but hits with drift distance between 2 and 7 mm only are included in these plots. Tracks used are COT-only. |
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need MC comparison | D0 Distribution from W Muons COT-only tracks - need MC comparison |
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need MC comparison | D0 Pull Distribution from W Muons COT-only tracks - need MC comparison |
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good as is (but need to check effect of multiple interactions at higher luminosity) |
Primary Track Spectrum in COT Primary COT tracks are selected with |d0| < 3 mm and at least 24 axial and 24 stereo COT hits. The per-event spectrum of charge-signed 1/Pt shows that the simulation models the primary track multiplicity well (given that Rick Field's Pythia tune is used here). The data were taken at low luminosity and no additional interactions were simulated. The comparison validates the W underlying event modelling (from the tracking point of view). |
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ready to go | Primary COT Track Multiplicity Same as above but showing the track multiplicity per event, modelled well by the simulation. |
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open issue - need to address | Good COT Track Spectrum
The impact parameter cut from above is removed, allowing secondary tracks.
The excess in the data, and the charge asymmetry, may suggest that secondary
interactions are under-estimated in GHEISHA. FLUKA gives similar results
to GHEISHA. The possibility that the MC deficit is all due to missing passive material is largely excluded by the fact that the muon dE/dx measurements (using J/psi fits and cosmic rays) are consistent with the simulation geometry within 5% or so. Since dE/dx scales with electron density and interaction lengths scale with nucleon density, the two are proportional for constant neutron/proton ratio. As there is some missing copper in the simulation geometry, and copper has 10% excess nucleons/electron as compared to low Z materials, a part of the MC deficit can be attributed to this. |
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open issue - need to address | Good COT Track Multiplicity Same as above, showing fewer COT tracks in simulation than data. |
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open issue - need to address | Spectrum of All Tracks COT hit requirements from above are removed, allowing also silicon standalone tracks. The deficit in the simulation gets worse. Updates to the simulation geometry to include the missing copper (based on studies of photon conversions) will allow for a better comparison. Direct mapping of secondary hadronic interactions using reconstructed secondary vertices will also be very useful. |
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open issue - need to address | Multiplicity of All Tracks COT hit requirements from above are removed, allowing also silicon standalone tracks. The deficit in the simulation gets worse. |
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Hit Width Hits with width<10 ns removed. Tail in the data at high width may be due to merged hits in the inner superlayers, due to higher occupancy (see plots above). |
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| nothing new | Mean Number of COT Hits per Superlayer on Muon Hits on inner superlayers may be obscured in the data due to higher occupancy than the simulation. |
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| nothing new | Total Number of COT Hits on Muon Track Consequence of above. |
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| nothing new | Distribution of COT Hits per Superlayer on Muon Track |
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Dimuon Z Mass (plot from Victoria Martin) |
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Dimuon Z Pt (plot from Victoria Martin) |
| current status | next release | description |
| *.tex file | nothing new | numerical comparison of SL efficiencies (at least 5 hits on muon track) no angular dependence was observed for the missed hits |
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Suggestions or contributions? Contact Ashutosh Kotwal