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MuKpi.C : micro-vertex code

 Brief introduction to the code

group meeting update

 Using the yield formula I showed at the last meeting, I can now generate yields for the xs data that have better-contained error bars and are also far more accurate when the signal-to-backgro

Group Meeting Update

Progress towards a measurement of A_{LL} for charged pion production opposite a trigger jet using data from the 2006 STAR run. Goal is to present this measurement as a function of z, defined here as p_{T}(pi) / p_{T}(trigger jet).

Update 2008-08-28: added data/MC comparison plots

Cuts Summary

This page summarizes the effect of each major cut in the 2006 jet+charged pion analysis. Each plot is obtained by applying all other applicable analysis cuts except the one being illustrated.

Figure 1: Black is TPC z-vertex for all BJP1-triggered events, Green is the TPC z-vertex distribution for events in BBC timebins 6-9, and Red is the TPC z-vertex distributions for all charged pion tracks (inclusive, no trigger jet requirement).

It appears at first that the vz distribution of good tracks is broader than the BBC 6-9 distribution, but that’s not actually the case. Here’s the ratio of the red and green histograms from the above plot:

Figure 1b

The following histograms use positively charged pions from any spin state. Black lines are inclusive π+ passing all cuts except the one being shown, green lines are leading π+ opposite a trigger jet, and the filled green histogram shows the π+ accepted for the asymmetry analysis.

Figure 2: |η| < 1.0

Figure 3: |dcaG| < 1.0

Figure 4: nHitsFit > 25

Figure 5: nσ(π). It’s not possible to read off the efficiency from this histo because I actually use a time-dependent cut window based on the results of fill-by-fill fits to the nσ(π) distributions. Ideal world cut shown is nσ(π) [-1,2]

Here’s the ratio of the green and black histograms from that plot. The away-side spectrum has a relative lack of electrons but an increase in the p/K contamination:

Figure 5b

I should also add some more plots here documenting the cuts on jet pT, detector η, and N.E.F.

SSA vs. z

Asymmetries are defined as (Y,B):

SSA vs. Fill

Asymmetries are defined as (Y,B):

List of Jobs for run 9 as of 8/21/08

Attached is a list of jobs for run 9 with names of those volunteering to handle tasks.

Spin asymmetry statistical errors, part 2

Updated the dE/dx cut. Previous asymmetry calculations was using +/- 3σ in dE/dx. The following has a tighter cut on the lower end, varies with momentum bins.

Isolation cut, rejection and efficiency versus cut value

Abstract:  We show what isolation cut is needed to obtain a given pi0 rejection power in each pT bin.
 

1.0 MC Event Sample

  1. Pythia event sample (pibero's gamma trees) w/ proper weighting for partonic pT bins
  2. No offline trigger simulation
  3. full EEMC acceptance

2.0 Definition of Isolation Cut

We use an isolation cut, which consists of correcting the ET of the tower which contains the photon candidate based on the position of the candidate within the tower, and dividing that corrected ET by the sum of all towers w/in R < 0.3.  The following links summarize the method.
  1. See Checking the isolation cut vs pythia events for definition of the 1-tower isolation cut and evaluation of rejection versus efficiency based on pythia events.
  2. See Isolation cut, data vs. MC, take 3 for data vs MC comparison, including trigger simulation.
The links above show plots of rejection power vs. efficiency.  It is informative to plot rejection vs. applied cut, and efficiency vs. applied cut.  See figure 1 below.
 
Figure 1 -- Rejection power (red) or photon efficiency (black) vs. isolation cut.
 

geometry used in Simulation (plain) vs. Embedding

Geometry used in simulation/embedding for hits projection

For embedding with SSD, we project GEANT hits on real geometry.