Status of hadron identification in semi-inclusive analysis - PowerPoint PPT Presentation

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Status of hadron identification in semi-inclusive analysis

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Hadron identification for longitudinal data. Tuning LH cuts. RICH stability (badspills) ... Status of hadron identification in SIDIS. 3. RICH code for identification ... – PowerPoint PPT presentation

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Title: Status of hadron identification in semi-inclusive analysis


1
Status of hadron identification in semi-inclusive
analysis
  • Rafal Gazda
  • SINS, Warsaw

Analysis Meeting, CERN, 5 September 2006
2
Motivation
Goal polarized strange sea quarks
distributions. One needs asymmetries of K and
K-.
Hadron identification for longitudinal data
Tuning LH cuts
RICH stability (badspills)
3
RICH code for identification
  • Two RICH methods are available
  • Chi2 and LH
  • Two codes for LH are available for different
    data(corespond to 04All-LH and 05All-LH)
  • The best results come from LH5 method, but part
    of data has only LH4
  • Only data with available LH5 was used
  • (part of 2004 and 2002 data)
  • For LH5 six likelihood values are available
  • background
  • Pion
  • Kaon
  • Proton
  • Electron
  • Muon

4
hadron identification
Standard cuts for SIDIS with Q2gt1GeV2
  • Hadrons
  • neither µB nor µ
  • Zlast lt 33m
  • zh(p)lt1
  • pions
  • LHmaxLH(p)
  • Plt50 GeV
  • LH(p)/...
  • kaons
  • LHmaxLH(K)
  • Plt50 GeV
  • LH(K)/...

5
Particle Identification
  • Main problem is to distinguish pions from kaons
  • Three cuts are tested on each kind of particle
  • K
    p
  • LH(K)/LH(p)
    LH(p)/LH(K)
  • LH(K)/LH(bg)
    LH(p)/LH(bg)
  • LH(K)/LH(2ndmax)
    LH(p)/LH(2ndmax)
  • Cuts using LH of muon and electron were tried but
    without any improvement (these particles are
    partly removed with hadron cuts)
  • Use LH of proton brings no improvement either.

6
LH distributions
p
K
7
Tuning LH cuts...
  • Tuning cuts on these parameters was done looking
    at ?-gtpp- and F -gt KK- distributions.
  • Only events with three particles from primary
    vertex were chosen µ and two oposite charged
    hadrons (identified as p or K).
  • Ratio S/(SB) is calculated for each set of cuts
    (each cut was changed from 1 to 1.3 with step
    0.01)

8
Results of tuning
Example 2004, W40
very preliminary LH(p)/LH(K) gt
1 LH(p)/LH(bg) gt 1.08 LH(p)/LH(2ndmax)
gt 1
very preliminary LH(K)/LH(p) gt 1.09
LH(K)/LH(bg) gt
1.18 LH(K)/LH(2ndmax) gt 1.01
9
Conclusions
  • Cuts on LH to identify p and K have been
    optimized using sample of ? and F mesons.
  • Cuts are not finalized yet, work is in progress
  • Also
  • RICH stability check for longitudinal data has
    been started

No conclusions yet...
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