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Subject: STAR task force for evaluating tracking efficiency uncertainty

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  • From: yh66 <yh66 AT rice.edu>
  • To: Petr Chaloupka <petrchal AT rcf.rhic.bnl.gov>, STAR task force for evaluating tracking efficiency uncertainty <star-tf-trkeff-l AT lists.bnl.gov>
  • Subject: Re: [Star-tf-trkeff-l] A question about the track efficiency uncertainty study
  • Date: Sat, 10 Jun 2023 17:34:53 -0500

Hi Petr,
Thank you, this is an excellent explanation. And the effect of the iTPC update may be very interesting for this study.

BW,
Yiding
Quoting Petr Chaloupka via Star-tf-trkeff-l <star-tf-trkeff-l AT lists.bnl.gov>:

Dear Yiding,

thank you for the question. Let me explain.
The discrepancy (large increase) from nhits>15 to nits>20 comes from the fact that we use charged tracks from decay K→3pi. This means that what is shown is a comparison of tracking efficiency for a tracks belonging to the primary kaon. However the primary kaon can never reach full way to the outer edge of the TPC (as most of primary tracks do) otherwise we would not be able to reconstruct its decay. In other words such track cannot have the maximum of 45 hits. In run18 (which data do you use?) we get to maximum of 30 possible hits, the average is about 25. So when you look at the results for nhits>20 it is quite an extreme cut for such tracks and hence there is a significant difference between data and simulation. One should be carefull to extrapolate to full lenght tracks (nhitPossible~45). I can argue that for a full lenght track the systematic error will not be larger that what is in the table so for example for the cut of dca<2cm and nhits>15 the 5% is reasonable upper estimate. The situation will be different for run19 with iTPC where we will have acces to tracks with more points. Then the estimates for nhits>20 should be closer to full lenght tracks.

With best regards,
Petr

On 08. 06. 23 1:08, yh66 via Star-tf-trkeff-l wrote:

Dear experts,
     This is Yiding from Rice. Recently I am working on the systematic uncertainty of di-electron analysis. I plan to add embedding/data mismatching uncertainty specifically referenced in your presentation slide available at: https://urldefense.com/v3/__https://drupal.star.bnl.gov/STAR/system/files/TrkEff.pdf__;!!BuQPrrmRaQ!hhfhZsWQCHurYChjT15Xy9i3REkW3jV-y0OLxbJY6S8R15zcOYmMDBLdqswClEKJ_udpYq2IIodkTNxLpPNGHa0PZc4aIgAi98Bal9gbZnQ$ . And I have one question about it.
     In Slide 15 of your presentation, you demonstrate the effect of different cuts on mismatching. I observed two intriguing aspects in this analysis. Firstly, the mismatching appears to be sensitive to the DCA cut, which aligns with similar observations made in various studies. However, what caught my attention is the substantial difference in mismatching between nHitsFit>15 and nHitsFit>20. To the best of my knowledge, previous di-electron analyses utilizing Run18 Au-Au 27GeV data did not report such a significant mismatching discrepancy between data and embedded electrons. Could you kindly shed some light on the underlying reasons behind this discrepancy?
     I appreciate your great study on the track efficiency uncertainty and would be grateful for any insights you can provide to help me better understand the question.

BW,
Yiding Han

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