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Status of dE/dx Calibration

Status of dE/dx Calibration. Yuri Fisyak October 17, 2002. Outlook. Why ? What ? Where ? Conclusions. Why ?. Last calibration was done in March, 2002: σ (dE/dx)/(dE/dx) = 8.2% for 76 cm track STAR CDR (p. 4C-33) σ (dE/dx)/(dE/dx) = 0.47 N -0.46 (Ph) -0.32 , P = 1atm

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Status of dE/dx Calibration

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  1. Status of dE/dx Calibration Yuri Fisyak October 17, 2002

  2. Outlook • Why ? • What ? • Where ? • Conclusions

  3. Why ? • Last calibration was done in March, 2002: • σ(dE/dx)/(dE/dx) = 8.2% for 76 cm track • STAR CDR (p. 4C-33) • σ(dE/dx)/(dE/dx) = 0.47 N-0.46(Ph)-0.32, P = 1atm • σInner = 14.3%, h = 1.15 cm, N = 12; • σOuter = 7.7%, h = 1.95 cm, N = 32; • σ = 6.8% for 76 cm track in TPC • H.Bichsel simulation: • σ = 7.3 % for 11 * 1.2 cm + 31 * 2.0 cm • I am not happy that ~1% is missing

  4. Why (cont.) ? • Comparison new and old tcl • H.Bichsel’s calculations reproduce data only qualitatively. Is this due to calibration procedure ? • H.Bichsel claims that we have non linearity in dE measurement. Can we check this ? • Can dE/dx calibration be done in one pass? Can we move it into fast online ?

  5. What does calibration include? • Applying pad correction obtained from pulser data (Fabrice did this and I will not talk about) • For good clusters (used in fit, no overlaps) • For good global tracks (No. fit points ≥ 30, Track length in TPC > 40 cm) • Z =log[(dE/dx)measured/(dE/dx)predicted for π] • Fit Z-distribution with Gauss(μ,σ) + pol3 in +/-3σ range. It is supposed that we have ~80% π and μ corresponds to π. • μ should not depend on • Time, Pressure • Sector, row • Drift distance • …

  6. What does prediction mean ? • Hans Bichsel made presentation about his model during the last collaboration meeting. He is preparing STAR TN on this subject. • PAI model (Photo Absorption model for Ionization energy loss, V.Grishin V.Ermilova,S.Kotelnikov, NIM A309(1991) 476) gives the same predictions but PAI simulation program (provided by P.Nevski) has problem at low β (it was not tuned for this range). For this reason I will use Bichsel’s calculations. 0.45 GeV/c

  7. Resolution before calibration 9.6% @ 76 cm

  8. What does March calibration mean? • March calibration included: • The same procedure as for Year 1 data • As prediction it was used Sirrf • Calibration was done for all tracks (no restriction on momentum) • Time dependence : overall gain correction factor each few hours (1-4) • Sector and pad row correction • Drift distance correction • Result : σ = 9.6 % → σ = 8.2 %

  9. Red – 40% truncation Green – 30% truncation Black - fit 8.2% @ 76 cm

  10. New tcl a little bit worse than old one 9.7% 9.9% =>9.8% after setting convolution flag

  11. New calibration • Calibration is based on tracks with 0.4 < p < 0.5 GeV/c (~MIP for pions: βγ = p/m = 4). • Calibration has been done for new tcl only. • As prediction it was used Bichsel’s calculation with dx dependence (see next slide) i.e. Z =log[(dE/dx)measured/(dE/dx)predicted for π(βγ,dx)] • This calibration gives σ = 8.8% (instead of 8.2% obtained in March because it was done only for 0.4<p<0.5GeV/c but resolution is obtained for all momenta).

  12. Calibration done for p in [0.4,0.5] GeV/c with new tcl σ = 8.8% @76 cm

  13. Check of ADC nonlinearity For uniquely identified tracks: • σ < 15% and • v = log[(dEdx)/(dE/dx)J], where J = [e,π,K,p,d] • |v| < 3σ for only J, and • |(dE/dx)J - (dE/dx)k| >5σ, for J≠K Plot predicted dE versus measured dE Outer Inner • It is seen clean nonlinearity besides saturation (with offset ~1keV). • It is not clear what is origin for this nonlinearity: • ADC, it has to be checked with pulser data • tcl ? due to threshold effects?

  14. Time dependence Gain variation versus time. ~5% Pressure variation versus time Oxygen concentration variation versus time

  15. Time dependence (cont.) • Drift distance correction: e+AdO where A = 1.75e-6 (1/cm/ppmO2), provided by A.Lebedev (ALEPH data) d – drift distance (cm), O – concentration of Oxygen (ppm)

  16. Pressure • Both Drift distance and Pressure correction allow to removetime dependence. • TPC Gain Monitor cannot be used (at least now) because its results depend on magnetic field.

  17. < 1 %

  18. After pad level correction from pulser calibration it still exists gain variation versus sector and row

  19. Dependence of gain correction versus drift distance (after accounting absorption) for Inner rows has opposite behavior with respect to expected. ADC nonlinearity is overcorrected !?

  20. 7.4% @ 76 cm

  21. For both + and -

  22. For positive only

  23. Negative only

  24. Bichsel shapes fit by φ(μ+(1+σ)z), where φ(z) is Bichsel shape and z = log(dE/dEmost probable); Inner

  25. Outer Both inner and outer rows are reasonably well described by Bichsel shape.

  26. Conclusions • In sense of dE/dx old and new tcl give comparable results. • It is observed significant nonlinearity in dE with respect to H.Bichsel calculation. • Accounting this nonlinearity allows to improve resolution by ~1% (8.2%=>7.4%) which is matched with our expectation. • To understand the nonlinearity is necessary to get pulser data with different signal amplitudes. • If the linearity will be understood than it will be possible to move dE/dx calibration in fast online. • With new calibration the Bichsel shape of dE/dx distribution describes data pretty well. Thus we can claim that model calculations gives quantitative agreement with data.

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