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Analysis of CMS HCAL testbeam performance

Analysis of CMS HCAL testbeam performance. Philip Harris. CMS HCAL(a brief look). Designed to survive large magnetic fields Consists of crystals conducive to Parton Showers Major form of detection is amplified Cerenkov light Light signals are amplified by HPDs

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Analysis of CMS HCAL testbeam performance

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  1. Analysis of CMS HCAL testbeam performance Philip Harris

  2. CMS HCAL(a brief look) • Designed to survive large magnetic fields • Consists of crystals conducive to Parton Showers • Major form of detection is amplified Cerenkov light • Light signals are amplified by HPDs • An HPD consists of a photocathode with a small gap (with a voltage potential) that is then connected to a piece of Silicon. • If positioned correctly no Lorentz force

  3. Major Issues for the Testbeam • The most critical issue in the testbeam involves the behavior of the HPDs • Last year It was discovered that timing is non linear with energy. • Simulations showed that the detector would still be fine in the LHC • Still this remains a critical issue and is fundamentally rooted in the behavior of the HPDs

  4. A Quick look at What’s in the beam • The tests over the summer concern various energies of 3 different particles

  5. Very Low Energy • One of the most important tests that are being done this summer involve an analysis of the Very Low Energy (VLE) response of the detector • In order to do this we need a good trigger system • External separation of Muons, Pions and Electrons is essential • Many external triggers were added for this purpose

  6. VLE Beam characteristics • The problem with VLE is that it is difficult to separate out the beam perfectly • Pions in particular decay into muons and screw up the data royally • Below are a series of plots that describe this for 10 GeV we expect ~10% contamination

  7. VLE beam examples • Here are actual plots showing the VLE beam (calculations agree with reality)

  8. General detector Problems • One problem with HPDs is that they release background emission thereby changing the time. • The plot below shows a strange high Energy bump

  9. Is it a problem • Previous results showed timing shifts resulting from this effect • Plots show a shift on the order of the a ns (within statistical shifts)

  10. Pedestal Analysis • Another very interesting thing is the shift in the Pedestals when a signal comes in • Reasoning: Silicon is imperfect • 2d plots of Pedestals after signal show little correlations

  11. Energy Resolution • A major debate concerns the optimal pedestal signal • Pedestal subtraction event by event or during the whole beam is debated. Plot below might yield answer.

  12. Overall resolution • Plot below shows the whole Energy scale

  13. Other Issues • During the VLE beam gains were changed on HPDs to increase resolution. • So far no statistical change is seen in calibration pulses.

  14. Long Term • Most data has been looked at for short term, but long term remains to be fully analyzed. • Plots below show detector seems reasonably stable.

  15. Along with Analysis • There many other things to be done at a testbeam • Calibration of the detector can be tricky. • At present a code has been written to carefully select muons and ratio scale this so as to check the calibration • This will be checked with radioactive source data to see if changes in Energy have occurred.

  16. Future • Multiple particle beams as well as a thorough pedestal analysis remain to and will be looked at, to insure that the detector has reasonable behavior.

  17. Conclusions • CMS HCAL behaves quite well, but there remain minor issues that need to be settled. • There is a lot of analysis even on a simple testbeam like this. • All these plots were generated by an analysis code package that I created and might be used for realtime user analysis at CMS

  18. Acknowledgements • H2 testbeam people • Dragoslav Lazic • Pawel De Barbero • University of Michigan • CERN • The Number of Neutrino flavors

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