Difference: GlobalHeavyIonResults (1 vs. 12)

Revision 122010-12-06 - PatrickJussel

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Global Variables Results

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Revision 112010-10-11 - AdamTrzupek

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  • Transverse momentum dependence of the resolution corrected reconstructed v2 with standard method (triangles), two-particle azimuthal correlations method (stars), compared to the generated v2(pT) (filled circles) for events with b = 2.3 fm (a) and b = 10.7 fm (b). For standard method the event plane is determined from the first layer of the forward calorimeter (FCAL0), while the elliptic flow signal is calculated for the azimuthal angles of the reconstructed tracks. For two-particle correlations method the elliptic flow is calculated for the reconstructed tracks as well.
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  • Fig. 5.15 from PPR. Transverse momentum dependence of the reconstructed v2 from the event plane method (squares), two-particle correlations (stars) and the Lee-Yang Zeros method (triangles) for Pb+Pb collisions with (a) b = 2.3, (b) 7.0 and (c) 10.7 fm.
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  • Distribution of the difference between the event plane angle and the true reaction plane, where the event plane angle is determined from the first barrel layer of the electromagnetic calorimeter - EMB1 (a), the first layer of the forward calorimeter - FCAL0 (b), the innermost layer of the pixel detector (c) and also calculated from the reconstructed tracks with pT > 0.5 Gev/c (d). For all distributions sample with constant flow 5% and b = 10-12 fm is used.

Revision 102010-05-10 - PatrickJussel

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Global Variables Results

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Revision 92009-11-25 - AdamTrzupek

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Fig5_9v3.jpg

* Fig. 5.15 from PPR. Transverse momentum dependence of the reconstructed v2 from the event plane method (squares), two-particle correlations (stars) and the Lee-Yang Zeros method (triangles) for Pb+Pb collisions with (a) b = 2.3, (b) 7.0 and (c) 10.7 fm.

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  • Distribution of the difference between the event plane angle and the true reaction plane, where the event plane angle is determined from the first barrel layer of the electromagnetic calorimeter - EMB1 (a), the first layer of the forward calorimeter - FCAL0 (b), the innermost layer of the pixel detector (c) and also calculated from the reconstructed tracks with pT > 0.5 Gev/c (d). For all distributions sample with constant flow 5% and b = 10-12 fm is used.
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  • The resolution correction and reconstructed elliptic flow parameters with different detector combination: table_PPR.pdf
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  • Pseudo-rapidity dependence of the reconstructed elliptic flow signal calculated from reconstructed tracks (left) and from pixel clusters and forward calorimetric cells (right) for a sample of peripheral events (b = 10 − 12 fm) with input flow of 5%. The reaction plane was estimated from signals in the first layer of forward calorimeters.

Fig5_12a.jpgpdf Fig5_12b.jpgpdf

  • Correlation functions for samples with input flow of 5% and impact parameter range (a) b = 10 − 12 fm, (b) b = 6 − 8 fm and (c) b = 2 − 4 fm.
Fig5_14.jpgpdf

  • |G^theta(ir)| versus r for peripheral samples (b = 10 − 12 fm) with the generated v2 of 3% (a), 5% (b) and 10% (c). In each plot the curves are calculated for different q values as indicated in the legend.
Fig5_15.jpgpdf

  • The same as in the previous figure for samples with constant input flow of 5% and different centralities: b = 2 − 4 fm (a), b = 6 − 8 fm (b) and b = 10 − 12 fm (c).
Fig5_16.jpgpdf
 
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Revision 82009-11-25 - AdamTrzupek

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Charged Particle Multiplicity (Si Hits)

  • multiplicity reconstruction from pixel cluster for a single HIJING events, histogram: true dN/deta, points: reconstruction results obtained using pixel cluster from one pixel detector layer: layer 1 (black), layer 2 (blue), layer 3 (red).
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    • plot for b=2.3 fm, multiplicity (left), correction factors (right):
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      layer 1 C, pdf layer 2C, pdf
    • plot for b=10.7 fm, C, pdf
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Charged Particle Multiplicity (Tracklets)

 
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  • Distribution of dNch/deta from HIJING events (histogram) and reconstructed using the tracklet method event-byevent, but without efficiency corrections (points with error bars).
 
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* (left) Tracklet reconstruction efficiency at |eta| < 1 for raw MC and reconstructed simulation data. (right) Resolution of the event-by-event charged particle multiplicity measurements.

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Charged Particle Multiplicity (Tracklets)

 

Transverse Energy

  • This figure shows the total reconstructed transverse energy ETRec calculated by means of the [MissingET] package (Athena 12.0.3) vs the true ET also calculated by the same package.
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Revision 72009-11-24 - PatrickJussel

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Global Variables Results

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Revision 62009-10-28 - unknown

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EtRecEtTrue.jpg
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  • This figure shows the reconstructed pseudorapidity transverse energy distribution (red crosses, obtained with a "toy reconstruction" described here) compared to the true data shown by black histogram.
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  • This figure shows (left) the reconstructed pseudorapidity transverse energy distribution (red crosses, obtained with a "toy reconstruction" described here) compared to the true data shown by black histogram and correction factor (right) used to obtain the reconstructed distribution from cell transverse energies.
 
    • data source: one event from run5, described at AOAtlasHIMC
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OneEventEtRec.jpg

Flow

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OneEventEtRec.jpg OneEventEtRec.pdf, OneEventEtRec.C c_factor.gif c_factor.C

Flow

 
  • Transverse momentum dependence of the resolution corrected reconstructed v2 with standard method (triangles), two-particle azimuthal correlations method (stars), compared to the generated v2(pT) (filled circles) for events with b = 2.3 fm (a) and b = 10.7 fm (b). For standard method the event plane is determined from the first layer of the forward calorimeter (FCAL0), while the elliptic flow signal is calculated for the azimuthal angles of the reconstructed tracks. For two-particle correlations method the elliptic flow is calculated for the reconstructed tracks as well.
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Revision 52009-07-09 - AdamTrzupek

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  • This figure shows correlations between total transverse energy ET (in EMC, FCAL and HAD calorimeters) and the number of collisions (Ncoll), number of participants (Npart) and impact parameter (b).
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Correl.gif
  • The same type of plot as above but now with higher statystics (6500 events) and for the total transverse energy CorrelETOT.eps, CorrelETOT.C
CorrelETOT.gif
  • This figure shows relative RMS of the number of collisions (Ncoll), number of participants (Npart) and impact parameter for 20 centrality bins, each cantaining 5% of events, selected by cutting on distribution of ETOT in EMC (open squares), ETOT in FCAL (+) and ETOT in HADC (x). Full points represent "truth" relative RMS obtained by direct cut on Ncoll, Npart and b. RelCentCuts5p.eps, RelCentCuts5p.C
    RelCentCuts5p.gif
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Correl.jpg
  • The same type of plot as above but now with higher statystics (6500 events) and for the total transverse energy CorrelETOT.pdf, CorrelETOT.C
CorrelETOT.jpg
  • This figure shows relative RMS of the number of collisions (Ncoll), number of participants (Npart) and impact parameter for 20 centrality bins, each cantaining 5% of events, selected by cutting on distribution of ETOT in EMC (open squares), ETOT in FCAL (+) and ETOT in HADC (x). Full points represent "truth" relative RMS obtained by direct cut on Ncoll, Npart and b. RelCentCuts5p.pdf, RelCentCuts5p.C
    RelCentCuts5p.jpg
 

Charged Particle Multiplicity (Si Hits)

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    • plot for b=2.3 fm, multiplicity (left), correction factors (right):


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Charged Particle Multiplicity (Tracklets)

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  • This figure shows the total reconstructed transverse energy ETRec calculated by means of the [MissingET] package (Athena 12.0.3) vs the true ET also calculated by the same package.
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EtRecEtTrue.gif
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EtRecEtTrue.jpg
 
  • This figure shows the reconstructed pseudorapidity transverse energy distribution (red crosses, obtained with a "toy reconstruction" described here) compared to the true data shown by black histogram.
    • data source: one event from run5, described at AOAtlasHIMC
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OneEventEtRec.gif
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OneEventEtRec.jpg
 

Flow

  • Transverse momentum dependence of the resolution corrected reconstructed v2 with standard method (triangles), two-particle azimuthal correlations method (stars), compared to the generated v2(pT) (filled circles) for events with b = 2.3 fm (a) and b = 10.7 fm (b). For standard method the event plane is determined from the first layer of the forward calorimeter (FCAL0), while the elliptic flow signal is calculated for the azimuthal angles of the reconstructed tracks. For two-particle correlations method the elliptic flow is calculated for the reconstructed tracks as well.
    • data source: all events from run7, described at AOAtlasHIMC
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  * Fig. 5.15 from PPR. Transverse momentum dependence of the reconstructed v2 from the event plane method (squares), two-particle correlations (stars) and the Lee-Yang Zeros method (triangles) for Pb+Pb collisions with (a) b = 2.3, (b) 7.0 and (c) 10.7 fm.
layer 1
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  • Distribution of the difference between the event plane angle and the true reaction plane, where the event plane angle is determined from the first barrel layer of the electromagnetic calorimeter - EMB1 (a), the first layer of the forward calorimeter - FCAL0 (b), the innermost layer of the pixel detector (c) and also calculated from the reconstructed tracks with pT > 0.5 Gev/c (d). For all distributions sample with constant flow 5% and b = 10-12 fm is used.
    • data source: all events from run7, described at AOAtlasHIMC
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  • The azimuthal angle distributions of the pixel clusters (innermost layer) measured with respect to event plane angle obtained from EMB1 (upper plots) and from FCAL0 (lower plots) for the simulated data with 3%, 5% and 10% (respectively from left side) constant input flow.
    • data source: all events from run9, run3, run8 described at AOAtlasHIMC
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  • The resolution correction and reconstructed elliptic flow parameters with different detector combination: table_PPR.pdf
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Revision 42009-07-07 - AdamTrzupek

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META TOPICPARENT name="HeavyIonsPublicResults"
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* Fig. 5.15 from PPR. Transverse momentum dependence of the reconstructed v2 from the event plane method (squares), two-particle correlations (stars) and the Lee-Yang Zeros method (triangles) for Pb+Pb collisions with (a) b = 2.3, (b) 7.0 and (c) 10.7 fm.
layer 1
pdf
 
  • Distribution of the difference between the event plane angle and the true reaction plane, where the event plane angle is determined from the first barrel layer of the electromagnetic calorimeter - EMB1 (a), the first layer of the forward calorimeter - FCAL0 (b), the innermost layer of the pixel detector (c) and also calculated from the reconstructed tracks with pT > 0.5 Gev/c (d). For all distributions sample with constant flow 5% and b = 10-12 fm is used.
Line: 123 to 128
 
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META FILEATTACHMENT attachment="Fig5_17.jpg" attr="" comment="" date="1246975431" name="Fig5_17.jpg" path="Fig5_17.jpg" size="67681" stream="Fig5_17.jpg" user="Main.AdamTrzupek" version="1"
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Revision 32009-01-14 - AdamTrzupek

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META TOPICPARENT name="HeavyIonsPublicResults"
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    • plot for b=2.3 fm, multiplicity (left), correction factors (right):


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layer 1
  C, eps, gif layer 2
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C, eps, gif
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C, eps, gif
 

* plot for b=10.7 fm, C, eps, gif

Line: 62 to 62
 
  • Transverse momentum dependence of the resolution corrected reconstructed v2 with standard method (triangles), two-particle azimuthal correlations method (stars), compared to the generated v2(pT) (filled circles) for events with b = 2.3 fm (a) and b = 10.7 fm (b). For standard method the event plane is determined from the first layer of the forward calorimeter (FCAL0), while the elliptic flow signal is calculated for the azimuthal angles of the reconstructed tracks. For two-particle correlations method the elliptic flow is calculated for the reconstructed tracks as well.
Changed:
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Fig5_9v3.gif
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Fig5_9v3.gif
 
  • Distribution of the difference between the event plane angle and the true reaction plane, where the event plane angle is determined from the first barrel layer of the electromagnetic calorimeter - EMB1 (a), the first layer of the forward calorimeter - FCAL0 (b), the innermost layer of the pixel detector (c) and also calculated from the reconstructed tracks with pT > 0.5 Gev/c (d). For all distributions sample with constant flow 5% and b = 10-12 fm is used.
    • data source: all events from run7, described at AOAtlasHIMC
Line: 120 to 120
 
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Revision 22009-01-14 - AdamTrzupek

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Correl.gif
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  • The same type of plot as above but now with higher statystics (6500 events) and for the total transverse energy CorrelETOT.eps, CorrelETOT.C
CorrelETOT.gif
  • This figure shows relative RMS of the number of collisions (Ncoll), number of participants (Npart) and impact parameter for 20 centrality bins, each cantaining 5% of events, selected by cutting on distribution of ETOT in EMC (open squares), ETOT in FCAL (+) and ETOT in HADC (x). Full points represent "truth" relative RMS obtained by direct cut on Ncoll, Npart and b. RelCentCuts5p.eps, RelCentCuts5p.C
    RelCentCuts5p.gif
 
Changed:
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  • This figure shows RMS of the number of collisions (Ncoll), number of participants (Npart) and impact parameter (b) for 0-15%, 15-30%,30-50%,50-70% and 70-100% central events, selected by cutting on distribution of ET in EMC (open squares), ET in FCAL (+) and ET in HADC (x). Full points represent "truth" RMS obtain by direct cut on Ncoll, Npart and b.
cent4_all.gif
>
>

Charged Particle Multiplicity (Si Hits)

 
Added:
>
>
  • multiplicity reconstruction from pixel cluster for a single HIJING events, histogram: true dN/deta, points: reconstruction results obtained using pixel cluster from one pixel detector layer: layer 1 (black), layer 2 (blue), layer 3 (red).
    • plot for b=2.3 fm, multiplicity (left), correction factors (right):
 
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layer 1 C, eps, gif layer 2 C, eps, gif
 
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Charged Particle Multiplicity (Si Hits)

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* plot for b=10.7 fm, C, eps, gif
 
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  • multiplicity reconstruction from pixel cluster for a single most central HIJING event, histogram: true dN/deta, points: reconstruction results obtained using pixel cluster from one pixel detector layer: layer 1 (black), layer 2 (blue), layer 3 (red).
 
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layer 1 layer 2 layer 3
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layer 1
 

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More detailed explanations, more figures and additional results (including LOI figures based on ATLSIM) are available in "this page",
 

Charged Particle Multiplicity (Tracklets)

Transverse Energy

Deleted:
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  • This figure shows total transverse energy ET calculated as a sum over all (Calo) cells in EMB+PEMB (red), EME+PEMEC (green) and HEC (blue), FCAL (white) and Tile (other colors). Thin histogram is sum over all generated particles pT (but neutrinos).
EtvsEta.gif
 
  • This figure shows the total reconstructed transverse energy ETRec calculated by means of the [MissingET] package (Athena 12.0.3) vs the true ET also calculated by the same package.
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 Last reviewed by: Never reviewed
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Revision 12009-01-13 - AdamTrzupek

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Added:
>
>
META TOPICPARENT name="HeavyIonsPublicResults"
<!-- /ActionTrackerPlugin -->

<!-- This is the default ATLAS template. 
Please modify it in the sections indicated to create your topic! In particular, notice that at the bottom there are some sections that must be filled for publicly accessible pages.
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<!-- By default the title is the WikiWord used to create this topic !-->
<!-- if you want to modify it to something more meaningful, just replace GlobalHeavyIonResults below with i.e "My Topic"!-->
<!---------------------------------------------------------  snip snip ----------------------------------------------------------------->

Global Variables Results

<!--optional-->

Introduction

At this page you will find data on global variables including:

Centrality

<!--Add the main topic here. i.e. create some new headings as follows:!-->
  • This figure shows correlations between total transverse energy ET (in EMC, FCAL and HAD calorimeters) and the number of collisions (Ncoll), number of participants (Npart) and impact parameter (b).
Correl.gif

  • This figure shows RMS of the number of collisions (Ncoll), number of participants (Npart) and impact parameter (b) for 0-15%, 15-30%,30-50%,50-70% and 70-100% central events, selected by cutting on distribution of ET in EMC (open squares), ET in FCAL (+) and ET in HADC (x). Full points represent "truth" RMS obtain by direct cut on Ncoll, Npart and b.
cent4_all.gif

Charged Particle Multiplicity (Si Hits)

  • multiplicity reconstruction from pixel cluster for a single most central HIJING event, histogram: true dN/deta, points: reconstruction results obtained using pixel cluster from one pixel detector layer: layer 1 (black), layer 2 (blue), layer 3 (red).

More detailed explanations, more figures and additional results (including LOI figures based on ATLSIM) are available in "this page",

Charged Particle Multiplicity (Tracklets)

Transverse Energy

  • This figure shows total transverse energy ET calculated as a sum over all (Calo) cells in EMB+PEMB (red), EME+PEMEC (green) and HEC (blue), FCAL (white) and Tile (other colors). Thin histogram is sum over all generated particles pT (but neutrinos).
EtvsEta.gif

  • This figure shows the total reconstructed transverse energy ETRec calculated by means of the [MissingET] package (Athena 12.0.3) vs the true ET also calculated by the same package.
EtRecEtTrue.gif

OneEventEtRec.gif

Flow

  • Transverse momentum dependence of the resolution corrected reconstructed v2 with standard method (triangles), two-particle azimuthal correlations method (stars), compared to the generated v2(pT) (filled circles) for events with b = 2.3 fm (a) and b = 10.7 fm (b). For standard method the event plane is determined from the first layer of the forward calorimeter (FCAL0), while the elliptic flow signal is calculated for the azimuthal angles of the reconstructed tracks. For two-particle correlations method the elliptic flow is calculated for the reconstructed tracks as well.

  • Distribution of the difference between the event plane angle and the true reaction plane, where the event plane angle is determined from the first barrel layer of the electromagnetic calorimeter - EMB1 (a), the first layer of the forward calorimeter - FCAL0 (b), the innermost layer of the pixel detector (c) and also calculated from the reconstructed tracks with pT > 0.5 Gev/c (d). For all distributions sample with constant flow 5% and b = 10-12 fm is used.

  • The azimuthal angle distributions of the pixel clusters (innermost layer) measured with respect to event plane angle obtained from EMB1 (upper plots) and from FCAL0 (lower plots) for the simulated data with 3%, 5% and 10% (respectively from left side) constant input flow.
Fig5_8v1.gif

  • The resolution correction and reconstructed elliptic flow parameters with different detector combination: table_PPR.pdf

<!--***********************************************************-->
<!--Do NOT remove the remaining lines, but add requested info as appropriate-->
<!--***********************************************************-->


<!--For significant updates to the topic, consider adding your 'signature' (beneath this editing box)-->
Major updates:
-- AdamTrzupek - 14 Dec 2007

<!--Please add the name of someone who is responsible for this page so that he/she can be contacted if changes are needed.
The creator's name will be added by default, but this can be replaced if appropriate.
Put the name first, without dashes.-->
Responsible: AdamTrzupek
<!--Once this page has been reviewed, please add the name and the date e.g. StephenHaywood - 31 Oct 2006 -->
Last reviewed by: Never reviewed
 
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