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Low Mass Systematic

For the low mass background systematic we first estimate the background contribution (or contamination factor) to the signal reigon.  That is we integrate our simulated background to discern t

Systematics

We need to worry about a number of systematic effects that may change our measurement of ALL.  These effects can be broadly separated into two groups: backgrounds and non background

TPX high rate test

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PT scan of Pythia-filter rejection for QCD events ( Jan)

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Pythia Filer: cell>10 GeV ET, cluster >20 GeV ET , grid covers Endcap Pythia events

A_LL

The measurement of ALL for inclusive neutral pion production is seen below along with statistical error bars and a systematic error band.  This asymmetry was calculated using a clas

Combinatoric Background

The last piece of the invariant mass distribution is the combinatoric background.  This is the result of combining two non-daughter photons into a pion candidate.  Since each photon in an

Low Mass Background

The low mass background is the result of single photons being artifically split by the detector (specifically the SMD.)  The SMD fails in it's clustering algorithm and one photon is reconstruc

Eta Peak

I treat the eta peak in a similar way as the pion peak.  I throw single etas, flat in Pt from 2 - 25, and reconstruct the two-photon invariant mass distribution for the results.  The thro

Pion Peak

To study the pion peak section of the invariant mass distribution I looked at single pion simulations.  The pions were thrown with pt from 2 - 25 GeV/c flat and were reconstructed using the cu

Yield Extraction

 After all the pion candidates have been found and all the cuts applied, we need to extract the number of pions in each bin (in each spin state for ALL.)  To do this we simply

Cuts and Parameters

Here I will detail the some general information about my analysis; topics that aren't substantial enough to warrant their own page but need to be documented.

Pt Dependent Mass

The two-photon invariant mass is given (in the lab frame) by

M = Sqrt(2E1E2(1 - Cos(theta)))

Invariant Mass Distribution

The two-photon invariant mass distribution can be roughly broken up into four pieces, seen below*.

Fig. 1

List of available M-C event samples (Jan)

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M-C Event Samples Available   

evaluation of Bates minB sample (Jan)

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Evaluation of minB events ample produced by Mike at Bates in January of 2008.

Events characteristic: Pythia MinB events, sqrt(s)=500 GeV, vertex Gauss(0,60cm)

Polarization

I am using the final polarization numbers from run 6, released by A. Bazilevsky to the spin group on December 4, 2007.  The files can be found below.

Relative Luminosity

 

Run List

Below you will find the runlist I used for all of the studies leading up to a preliminary result.  For a more detailed look at how I arrived at this runlist please see my run

Towards a Preliminary A_LL

 Links for the 2006 Neutral Pion A_LL analysis

2008

Background information