davinci:samples
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| - | ====== Particle Samples ====== | + | ====== Particle Samples |
| - | ===== Under construction ===== | + | |
| - | Final content will be added soon, this is just a copy from different locations. | + | |
| - | < | + | |
| + | ===== Idea ===== | ||
| + | To perform an analysis in DaVinci, several types of samples can be used, which represent tighter or looser restrictions to the selection of the particles. | ||
| + | The following notes are just a copy of the comments in the '' | ||
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| - | Comment on CombinedParticleMaker and exclusive selection:\ | + | ===== No-PID particles ===== |
| - | Job option for exclusive selection of particle types. | + | These sets of particles are useful for loose stripping and |
| + | PID-studies. **NoPIDsParticleMaker** is used for creation: | ||
| + | * "/ | ||
| + | * "/ | ||
| + | * "/ | ||
| + | * "/ | ||
| + | * "/ | ||
| + | |||
| + | Note that the NoPIDsParticlreMaker uses VTT, Long and Downstream tracks by default. See **NoPIDsParticleMaker** in the DaVinci Doxygen for details. | ||
| + | |||
| + | ===== Loose PID particles ===== | ||
| + | |||
| + | CombinedParticlMaker (with " | ||
| + | |||
| + | * Muon : det=' | ||
| + | * Electron : det=' | ||
| + | * Kaon : det=' | ||
| + | * Proton | ||
| + | * Pion : No requirements | ||
| + | * VTT Pions: Made of VTT tracks | ||
| + | * Downstream Pions: Made of Downstream tracks | ||
| + | |||
| + | Containers: | ||
| + | * "/ | ||
| + | * "/ | ||
| + | * "/ | ||
| + | * "/ | ||
| + | * "/ | ||
| + | * "/ | ||
| + | |||
| + | See **CombinedParticleMaker** in the DaVinci Doxygen for details. | ||
| + | |||
| + | ===== Tight PID particles ===== | ||
| + | |||
| + | CombinedParticlMaker (with " | ||
| + | * Muon : det=' | ||
| + | * Electron : det=' | ||
| + | * Kaon : det=' | ||
| + | * Proton | ||
| + | * Pion : det=' | ||
| + | |||
| + | Containers: | ||
| + | * "/ | ||
| + | * "/ | ||
| + | * "/ | ||
| + | * "/ | ||
| + | * "/ | ||
| + | |||
| + | ===== Photons ===== | ||
| + | |||
| + | (Cnv)PhotonParticlemaker is used. | ||
| + | * non-converted photons: "/ | ||
| + | * converted photons: | ||
| + | * all photons: | ||
| + | See **PhotonParticleMaker** or **CnvPhotonParticleMaker** in the DaVinci Doxygen for details. | ||
| + | |||
| + | ===== General ===== | ||
| + | There are a set of StandardDC06 basic particle, StandardDC06 Pi0s and a set of StandardDC06 intermediate states: D0, Ds, D*, J/psi, K*, Phi. The relevant algorithms are fired on demand when one wants to read their outputlocation. See the relevant options for a complete list. | ||
| + | |||
| + | The cuts coded in this version are 'just a little tighter' | ||
| + | |||
| + | The actual definition of the cuts should be defined by the physics WG for the DC06 stripping. The present first import should be taken as an example more definitions of ' | ||
| + | |||
| + | ===== About Exclusive Selection in the CombinedParticleMaker ===== | ||
| + | |||
| + | **m_exclusive**: | ||
| PIDs are checked in some order and all tracks that are compatible with being a muon are made a muon, then an electron, proton, kaon and pion. What you get will depends on this order, which is already a good enough reason not to want that. If you do B->pipi and one pi decays to a muon, it will never be a pi candidate. Even worse, if you or someone relaxes the mu ID cuts between two jobs or two DaVinci versions, then suddenly what used to be a nice pion in one version of DV might now becomes a muon candidate. Your efficiency decreases although nothing affecting pion or kaon ID changed. That makes it very hard to estimate signal efficiencies as all efficiencies depend on everything. If you want to cut hard on PID, use PID cuts. If you don't want to use the same track several times (which is a valid point for tagging), then use the Overlap Tool and re-weight the track accordingly if needed. | PIDs are checked in some order and all tracks that are compatible with being a muon are made a muon, then an electron, proton, kaon and pion. What you get will depends on this order, which is already a good enough reason not to want that. If you do B->pipi and one pi decays to a muon, it will never be a pi candidate. Even worse, if you or someone relaxes the mu ID cuts between two jobs or two DaVinci versions, then suddenly what used to be a nice pion in one version of DV might now becomes a muon candidate. Your efficiency decreases although nothing affecting pion or kaon ID changed. That makes it very hard to estimate signal efficiencies as all efficiencies depend on everything. If you want to cut hard on PID, use PID cuts. If you don't want to use the same track several times (which is a valid point for tagging), then use the Overlap Tool and re-weight the track accordingly if needed. | ||
| + | |||
| + | ===== MC09 ===== | ||
| + | The corresponding information for MC09 samples can be found in: **$COMMONPARTICLESROOT/ | ||
| + | |||
davinci/samples.1236074357.txt.gz · Last modified: 2009/03/03 10:59 by decianm
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