Total γ Beam Absorption Cross Section for TAC and e+e- Runs with Si Target Runs used: TAC run 065014 (with Si target) TAC run 065106 (empty target) e+e- run 065102 (with Si target and TAC in) e+e- run 065103 (empty target and TAC in) For discussion: preliminary results for the following TAC runs: 065063 (with Si target) 065064 (empty target) Overview Analyze TAC runs and e+e- runs and compare extracted total cross sections ● Total γ beam absorption cross section calculations ● Event selections to minimize biases ● Discuss the following items: - preliminary results on additional TAC runs (Si target) - TAC ADC spectrum and TAC to Tagger energy ratio for TAC run 065061 (with C target) - Monte Carlo corrections (Ilya Larin) ● Summarize results and details for future analysis Difference Between TAC and e+eRuns TAC Runs 065104 (Si target) and 065106 (empty target): ● B = ~ │0.1643│kG ● Pair Spectrometer Current = │250│A ● Beam Current = 250 pA e+e- Runs 065102 (Si target) and 065103 (empty target): ● B = ~ │1.980│kG ● Pair Spectrometer Current = │3185│A ● Beam Current = 250 pA Total γ Beam Absorption Cross Section σtot = -A/(NAρx)*ln(Nγout/Nγinc) Nγout= TAC events with Si target Nγinc= total events with Si target / absolute tagging ratio absolute tagging ratio = TAC events (empty) / total events (empty) A = Si atomic mass ( 28.0855 g/mol ) NA = Avogadro's number (6.022e23 mol-1) ρ = Si target density ( 2.316 g/cm3 ) x = Si target thickness ( 1.0015 cm ) Statistical Errors Let Nε = NST/ NTT and Nβ = NSE/ NTE NST= TAC events Si target NTT= total events Si target NSE= TAC events empty target NTE= total events empty target Let α = Nε / Nβ σ(Nε) = √ (NTTNε(1-Nε)) with error δ(Nε) = σ(Nε)/NTT σ(Nβ) = √ (NTENβ(1-Nβ)) with error δ(Nβ) = σ(Nβ)/NTE propagated error δ(α) = √( (∂α/∂Nε)2(δ(Nε))2 + (∂α/∂Nβ)2(δ(Nβ))2 ) Systematic Errors Due to an uncertainty in the amount of atoms in the Si target, there is a systematic error contribution from the density and thickness of the target. Information was obtained in PrimEx Notes 69. Fractional uncertainty for Si target measurements was found to be ± 0.35%. It should be noted that more items in systematic error budget will be added. TAC TDC counts and TAC ADC counts for Run 065106 TAC TDC and ADC counts shown for T counter 10 TAC TDC Spectrum Run 065106 TAC TDC spectrum (log scale) shown for T counter 10 Time Difference between TAC and Tagger Events were selected if time difference between TAC and Tagger TDC hits < 3 ns, to minimize accidentals TAC ADC Spectrum Run 065106 (empty target) TAC ADC spectrum shown for T counter 10 TAC Energy to Tagger Energy Ratio (empty target) Events were selected if calibrated ratio > 0.62, to minimize biases TAC Energy to Tagger Energy Ratio (with Si target) Events were selected if calibrated ratio > 0.62, to minimize biases Total γ Beam Absorption Cross Section: TAC 065104 and 065106 e+e- 065102 and 065103 Energy = 5.279 GeV Energy = 4.373 GeV *systematic errors not shown **error not shown on NIST, needs further investigation Discussion on TAC Runs 065063 and 065064 Further analysis was conducted on the following runs: TAC run 065063 (with Si target) TAC run 065064 (empty target) Total γ Beam Absorption Cross Section: TAC 065104 and 065106 TAC 065063 and 065064 Energy = 5.279 GeV For 0651064/065106 Beam current = 250 pA Energy = 4.373 GeV For 065063/065064 Beam current = 100 pA Discussion on TAC run 065061 (with C target) Comparison between TAC ADC spectrum for T counter 1 and T counter 19 Discussion on TAC run 065061 (with C target) TAC Energy to Tagger Energy Ratio Discussion of Monte Carlo Corrections (Ilya Larin) Summary 1) The total γ beam absorption cross section was extracted for each T counter (1-19) using information from TAC runs 065104 (with Si target), 065106 (empty target) and e+e- runs with TAC in 065102 (with Si target), 065103 (empty target) 2) Results were shown for TAC runs 065063 (with Si target) and 065064 (empty target), but warrant further investigation due to discrepancies between total γ beam absorption cross section values for other runs 3) Future analysis will follow a similar process for total cross section extraction from TAC and e+e- runs with the carbon target. I am currently waiting for exact measurements on carbon target used in PrimExII to proceed with this item 4) More items in systematic error budget ● ● Tagging ratio stability will be investigated and added Systematic contributions related to TAC efficiency and events 'returned' from Bremsstrahlung and Compton
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