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Absolute & Relative Normalization

Absolute & Relative Normalization. Paul E. Reimer 8 January 2009 Luminosity monitors Calibrations Targets composition Based on Theses of R. Towell and J. Webb. Luminosity and Beam Monitors. Secondary emission monitors (SEM) Primary beam intensity monitor Ion chamber (IC)

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Absolute & Relative Normalization

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  1. Absolute & Relative Normalization Paul E. Reimer 8 January 2009 Luminosity monitors Calibrations Targets composition Based on Theses of R. Towell and J. Webb

  2. Luminosity and Beam Monitors • Secondary emission monitors (SEM) • Primary beam intensity monitor • Ion chamber (IC) • Secondary monitor • Segmented wire ion chamber (SWIC) • Position and profile monitor • Scintillator telescopes (AMON, WMON) • Viewed targets at 85o in lab through hole in shielding • Absolute calibrations? Paul E. Reimer Absolute and Relative Normalization

  3. SEM vs. IC3 Approx. 2000 SEM • Not quite linear • Calibration and/or offset changes during dataset • Affects all targets in the same way. • Shifts can be isolated to particular times/jumps • Not significant problem for Ratio experiment Linear relationship Deuterium (ic3+0) Empty (ic3+2.5e4) Hydrogen (ic3+5e4) Paul E. Reimer Absolute and Relative Normalization

  4. SEM linearity check • Plot sem vs. other luminosity monitors (amon and wmon) • Perform similar test with IC3 Deuterium Empty Hydrogen Paul E. Reimer Absolute and Relative Normalization

  5. SEM Offset empirically determined • Should also be examined target-by-target Paul E. Reimer Absolute and Relative Normalization

  6. SEM absolute calibration • Difficult—6.5% systematic uncertainty for E866/NuSea • Replace target with thin Cu foil • Proton beam activates Cu foil creating 24Na • Measure rate of 1368 keV ’s emitted by the 24Na • Need 24Na production cross section • Measured at 400 GeV, not 120 or 800 GeV • 3.90 ± 0.11 mb (2.7% uncertainty already) • Can we do better???? Historic calibration data for MEast beam line Paul E. Reimer Absolute and Relative Normalization

  7. Target issues • Target Length • Measure it—Write it down—Note which target it belongs to. • Target Density from target measured target pressure (see ref. in Webb’s thesis) • Similar formula for deuterium • Approx. 2% systematic for E866/NuSea • Target attenuation length • PDG values for H2 and D2 • Also need HD for lD2 contamination Paul E. Reimer Absolute and Relative Normalization

  8. Target Contamination • Analysis of D2 gas during fill done at Argonne (black box) • Approx 1% uncertainty in Absolute Luminosity • Approx 0.61% uncertainty in Ratio • Tied with rate dependence for largest uncertainty Paul E. Reimer Absolute and Relative Normalization

  9. Conclusion • Relative uncertainty dominated by target composition • Obtain purest D2 we can get from Fermilab • Absolute uncertainty dominated by SEM calibration • Better ideas?? Paul E. Reimer Absolute and Relative Normalization

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