New polarized gluon distributions in Pythia
Updated on Tue, 2007-11-13 16:19. Originally created by kocolosk on 2007-11-13 11:29.So we now have access to a wide variety of gluon polarization parameterizations in our Pythia afterburner covering the regions between GRSV -std and -max and between GRSV -zero and -min. Dave Staszak documents the details of the new distributions at
http://www.star.bnl.gov/protected/spin/staszak/2006/Sims/trigBias/trigBias.html
Here are plots of the raw charged pion asymmetries obtained from these grids (p070 excluded because of a bug on my part):
I suspect the problem with the pi-minus asymmetries can be traced to a lack of gg contributions. For more information see Agreement Between "Polarized" Pythia and NLO pQCD. In the remainder of this document I'll stick to analyzing pi-plus data.
I've attached multi-page PDF at the bottom of the page. Each page of the PDF plots, for a give input gluon polarization distribution A_{LL}(trigger) - A_{LL}(no trigger) as a function of pion p_T. There are six plots on each page; one for each trigger in (minbias, HT1, HT2, JP1, JP2) and then the raw A_{LL}(no trigger) distribution itself in the bottom right. I believe one way we can obtain a systematic uncertainty from plots such as these is to calculate a double-sided max( delta A_{LL}, uncertainty on triggered A_{LL} ) for each pT bin we use to make our measurement.
One question is which grids are appropriate ones to use for calculating the systematic. GRSV-max has been excluded in other measurements, so I don't think it's appropriate. All other grids are fair game, which means the systematic will likely be derived from GRSV-min and p070 (once I rerun; use p060 for now).
Agreement Between "Polarized" Pythia and NLO pQCD
We're using an afterburner framework that turns Pythia into something like a LO polarized event generator to study any biases introduced by our triggers on A_LL measurements. This page compares the asymmetries generated by Pythia to theoretical predictions from GRSV.
Cuts
- MC and reco vz positions inside 60 cm
- |eta| of reco primary track < 1.0
- dca of associated global < 1.0
- fit points > 25
- select pions using geant ID 8 (pi-plus) or 9 (pi-minus)
No trigger requirements are imposed.
Weighting
I combined MC samples 3_4 through 55_65 using the following cross sections and event counts
xsec = {
'3_4' : 1.287, 384593
'4_5' : 3.117*10**-1, 586568
'5_7' : 1.360*10**-1, 380791
'7_9' : 2.305*10**-2, 404272
'9_11' : 5.494*10**-3, 413651
'11_15' : 2.228*10**-3, 418547
'15_25' : 3.895*10**-4, 407427
'25_35' : 1.016*10**-5, 99998
'above_35' : 5.299*10**-7, 119995
'45_55' : 2.830*10**-8, 119995
'55_65' : 1.433*10**-9 119998
}
Plots
First off, here are the asymmetries integrated over all subprocesses. The left column is pi-plus, the right column is pi-minus. The agreement for postive charges seems basically acceptable to me, but pi-minus is off by quite a lot:
If I restrict to g-g, q-g, and q-q subprocesses individually, the difference between the two is obviously in the q-g subprocess contribution (as expected):
It seems to me that the lack of agreement between our Monte Carlo and the theoretical predictions could be due in part to a lack of gg / over-abundance of qg in the subprocess mix. Here are plots of the subprocess mix from Pythia:
compare that to the prediction from Vogelsang et al. for inclusive pi0 production, where gg is the primary contributor until ~3 GeV:
In particular, only the 3_4 GeV partonic sample has more g-g than q-g at any pion p_T. I'm going to try including the 2_3 GeV sample in my studies and see if that bolsters the gg contribution.
Data Carousel Quick Start/Tutorial
Updated on Thu, 2018-07-19 12:38 by gnigmat. Originally created by jeromel on 2007-11-12 20:45. Under:The Function of the Data Carousel
The Data Carousel should be used by STAR users to retrieve data from HPSS.
bfcca
Updated on Mon, 2025-03-03 01:13 by genevb. Originally created by jeromel on 2007-11-12 17:25. Under:This document describes the arguments for bfcca located in $STAR_SCRIPTS, a production script inter
Fast Offline
Updated on Wed, 2023-05-17 13:51. Originally created by jeromel on 2007-11-12 17:20. Under:Fast Offline documentation
- Disk space layout (where to find the data, path name convention)
Proposal for Run IV
Updated on Mon, 2007-11-12 14:29 by testadmin. Originally created by jeromel on 2007-11-12 14:23. Under:Procedure proposal for production and QA in Year4 run
Proposal and statements
Updated on Mon, 2007-11-12 14:54 by testadmin. Originally created by jeromel on 2007-11-12 14:20. Under:.
Offline QA
Offline QA Shift Resources
MINUTESUpdated on Fri, 2007-11-09 16:45. Originally created by margetis on 2007-11-09 16:41.Talk time : 13:55, Duration : 00:05 Run 8 preparation meetings #6Updated on Fri, 2007-11-09 14:06. Originally created by testadmin on 2007-11-09 13:25. 2007-11-09 15:00
2007-11-09 17:00
Etc/GMT-5
Friday, 9 November 2007 1-189, HighSpeed conference bridge, at 20:00 (GMT), duration : 02:00
Reader integration to offline? News & ETA.
STAR Mailing ListsUpdated on Fri, 2007-11-09 16:26 by margetis. Originally created by matis on 2007-11-09 13:01.Speaker : Howard MatisTalk time : 13:50, Duration : 00:05 comparison of 19.6 GeV Au and 22 GeV CuUpdated on Fri, 2007-11-09 11:25. Originally created by hbtuser on 2007-11-09 11:25.ReferenceSpeaker : debasish dasTalk time : 00:20, Duration : 00:20 Update on Pion-Proton Y4 200GeVUpdated on Fri, 2007-11-09 05:09. Originally created by zawisza on 2007-11-09 05:09.ReferenceSpeaker : Marcin Zawisza ( WUT )Talk time : 00:00, Duration : 00:20 link to talk What is next: Slow sim/GeometriesUpdated on Fri, 2007-11-09 16:26. Originally created by margetis on 2007-11-08 16:40.IST optimization-quick updateUpdated on Fri, 2007-11-09 13:26 by nieuwhzs. Originally created by margetis on 2007-11-08 16:22.Sotware work/updatesUpdated on Fri, 2007-11-09 11:52. Originally created by margetis on 2007-11-08 16:21.News-Production Checks/NewsUpdated on Fri, 2007-11-09 15:53. Originally created by margetis on 2007-11-08 16:20.Speaker : Jan/Spiros/AllTalk time : 13:00, Duration : 00:20 |