Changes between Version 8 and Version 9 of WikiStart


Ignore:
Timestamp:
Jun 24, 2013, 12:57:19 AM (12 years ago)
Author:
Gustavo Gil Da Silveira
Comment:

writing some text and including all plots

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  • WikiStart

    v8 v9  
    33== Introduction ==
    44
    5 This study is meant to investigate the parton distribution function in [[http://www.desy.de/~heramc/programs/lpair/lpair.pdf|LPAIR Monte Carlo generator]] w.r.t. the inelastic collision when the incoming proton breaks up into a hadronic final state.
    6 
    7 The built-in options in LPAIR make use of two parametrizations for the parton densities inside the proton, namely:
    8 
    9 1. BRASSE [[http://www.sciencedirect.com/science/article/pii/0550321376902315|DESY 76/11 (1976)]] with option 12 in the LPAIR card; and
    10 
    11 2. SURI-YENNIE [[http://www.sciencedirect.com/science/article/pii/0003491672902424|Ann. of Phys. 72 (1972) 243]] with option 11.
    12 
     5This investigation is meant to study the parton distribution functions (`PDF`) being used in the [[http://www.desy.de/~heramc/programs/lpair/lpair.pdf|LPAIR Monte Carlo generator]] w.r.t. the inelastic collision when the incoming proton breaks up into a hadronic final state. This analysis was motivated by the observation of a deficit on the number of events in the transverse momentum (p,,T,,) distributions of dimuons from data when compated to the predictions from `LPAIR` (Figure 6 in [[http://arxiv.org/abs/arXiv:1305.5596|CMS-FSQ-12-010]]). A possible reason for such disagreement may be related to the PDF being employed by `LPAIR` to compute the contribution of proton dissociation.
     6
     7There are currently two versions of this Monte Carlo generator (which can be found [[http://cmssw.cvs.cern.ch/cgi-bin/cmssw.cgi/UserCode/Forthomme/lpair/|here]]) studying two different kind of processes:
     8
     91. `DESY` version: developed for electron-proton collisions in HERA, with built-in option for proton-proton collisions as "test". This version allows one to study elastic and inelastic (single dissociation) processes for the production of dileptons; and
     10
     112. `CDF` version: improved version which allows one to study elastic and double dissociation processes with more phase-space cuts available.
     12
     13In this current analysis, we focus in the exclusive dimuon production, gamma-gamma -> mu+ mu-, in inelastic collisions (single dissociation). LPAIR makes use of the [[http://home.thep.lu.se/~torbjorn/pythiaaux/introduction.html|JetSet]] library present in [[http://home.thep.lu.se/~torbjorn/pythiaaux/present.html|Pythia]] in order to perform the hadronization of the proton remnants.
     14
     15The built-in options for proton dissociation in LPAIR make use of two parametrizations for the parton densities inside the proton, namely:
     16
     171. `SURI-YENNIE` [[http://www.sciencedirect.com/science/article/pii/0003491672902424|Ann. of Phys. 72 (1972) 243]] with option `11`; and
     18
     192. `BRASSE` [[http://www.sciencedirect.com/science/article/pii/0550321376902315|DESY 76/11 (1976)]] with option `12` in the `LPAIR` card. This parametrization is restricted: M,,X,, < 2 GeV and Q^2^ < 5 GeV^2^.
     20
     21Due to the larger hadronic masses and p,,T,, distributions of the dimuon pair probed in the LHC kinematical regime, we employ SURI-YENNIE in this analysis.
     22
     23Following the implementation made by Dariusz Bocian (IFJ-PAN, Krakow) [[http://th-www.if.uj.edu.pl/acta/vol35/abs/v35p2417.htm|Acta Phys.Polon. B35 (2004) 2417-2424]], the current `LPAIR` code (`DESY` version) was modified in order to account for the proton-nucleus collisions from previous studies. Then, LPAIR samples are produced as `HBOOK` files, which have to be converted to `ROOT` files using the [[http://root.cern.ch/root/HowtoConvert.html|h2root]] script provided by [[http://root.cern.ch/drupal/|ROOT]].
     24
     25In case one has several `ROOT` files to merge, the [[http://root.cern.ch/drupal/content/how-merge-histogram-files|hadd]] script is employed.
     26
     27
     28== Set up ==
     29
     30=== Event samples ===
     31
     32The samples are produced with 1 million (1M) events, to check the shape of all kinematic distributions, and 5 million (5M) events in order to have enough statistics for high-p,,T,, dimuons. For the former, the samples are produced by merging ten sub-samples containing 100k events, which are obtained by running `LPAIR` at a time. while for the latter, five samples of 1M events by applying cuts on Q^2^: 0-1, 1-5, 5-20, 20-50, and 50-100 GeV^2^. The production of each of the sample with 1M events follows the same procedure as for 1M events for the whole Q^2^ range.
     33
     34It is worth to notice that the histograms in the distributions with 5M events are **stacked**, and each individual set of events can be distinguished by the lines crossing vertically the histogram.
     35
     36
     37=== Structure functions ===
     38
     39The built-in PDFs in `LPAIR` are replaced by two paramatrizations for the parton densities:
     40
     411. Gluck-Reya-Vogt (`GRV`) [[http://dx.doi.org/10.1007/s100520050289|Eur.Phys.J. C5 (1998) 461-470]]
     42{{{
     43* * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * *
     44*                                                                   *
     45*     G R V  -  P R O T O N  - P A R A M E T R I Z A T I O N S      *
     46*                                                                   *
     47*                          1998 UPDATE                              *
     48*                                                                   *
     49*                  For a detailed explanation see                   *
     50*                   M. Glueck, E. Reya, A. Vogt :                   *
     51*        hep-ph/9806404  =  DO-TH 98/07  =  WUE-ITP-98-019          *
     52*                  (To appear in Eur. Phys. J. C)                   *
     53*                                                                   *
     54*   This package contains subroutines returning the light-parton    *
     55*   distributions in NLO (for the MSbar and DIS schemes) and LO;    *
     56*   the respective light-parton, charm, and bottom contributions    *
     57*   to F2(electromagnetic); and the scale dependence of alpha_s.    *
     58*                                                                   *
     59*   The parton densities and F2 values are calculated from inter-   *
     60*   polation grids covering the regions                             *
     61*         Q^2/GeV^2  between   0.8   and  1.E6 ( 1.E4 for F2 )      *
     62*            x       between  1.E-9  and   1.                       *
     63*   Any call outside these regions stops the program execution.     *
     64*                                                                   *
     65*   At Q^2 = MZ^2, alpha_s reads  0.114 (0.125) in NLO (LO); the    *
     66*   heavy quark thresholds, QH^2 = mh^2, in the beta function are   *
     67*            mc = 1.4 GeV,  mb = 4.5 GeV,  mt = 175 GeV.            *
     68*   Note that the NLO alpha_s running is different from GRV(94).    *
     69*                                                                   *
     70*    Questions, comments etc to:  avogt@physik.uni-wuerzburg.de     *
     71*                                                                   *
     72* * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * *
     73}}}
     74
     752. Parametrization by Fiore et al.
     76
     77To be added
     78
     79== Results ==
     80
     81The kinematic distributions are presented below for the sets of 1M and 5M events considering the possibilities for the parton densities.
     82
     83//(Right-click on the images and select 'Open in a new Tab' in order to enlarge them)//
     84
     85=== No experimental cuts ===
     86
     87||||||= **1M events** =||
     88||= **`SURI-YENNIE`** =||= **`GRV`** =||= **`FIORE`** =||
     89|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_contour.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_contour.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_contour.png, 500px)]] ||
     90|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_contourlarge.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_contourlarge.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_contourlarge.png, 500px)]] ||
     91|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_contourx.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_contourx.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_contourx.png, 500px)]] ||
     92|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_etapair.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_etapair.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_etapair.png, 500px)]] ||
     93|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_etarem.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_etarem.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_etarem.png, 500px)]] ||
     94|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_invm.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_invm.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_invm.png, 500px)]] ||
     95|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_invmlarge.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_invmlarge.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_invmlarge.png, 500px)]] ||
     96|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_lego.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_lego.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_lego.png, 500px)]] ||
     97|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_legolarge.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_legolarge.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_legolarge.png, 500px)]] ||
     98|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_legox.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_legox.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_legox.png, 500px)]] ||
     99|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_legoxlarge.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_legoxlarge.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_legoxlarge.png, 500px)]] ||
     100|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_mx.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_mx.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_mx.png, 500px)]] ||
     101|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_mx_zoom.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_mx_zoom.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_mx_zoom.png, 500px)]] ||
     102|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_mx_zoom2.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_mx_zoom2.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_mx_zoom2.png, 500px)]] ||
     103|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_mx2_zoom.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_mx2_zoom.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_mx2_zoom.png, 500px)]] ||
     104|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_mx2_zoom2.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_mx2_zoom2.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_mx2_zoom2.png, 500px)]] ||
     105|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_ptpair.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_ptpair.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_ptpair.png, 500px)]] ||
     106|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_ptpairlarge.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_ptpairlarge.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_ptpairlarge.png, 500px)]] ||
     107|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_Q2.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_Q2.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_Q2.png, 500px)]] ||
     108|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_Q2large.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_Q2large.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_Q2large.png, 500px)]] ||
     109|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_x.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_x.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_x.png, 500px)]] ||
     110|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_xi.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_xi.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_xi.png, 500px)]] ||
     111|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_xilog.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_xilog.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_xilog.png, 500px)]] ||
     112|| [[Image(source:/trunk/plots/no_cuts/1M_evt/SURI_1Mevt_ypair.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/1M_evt/GRV_1Mevt_ypair.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/1M_evt/FIORE_1Mevt_ypair.png, 500px)]] ||
     113
     114
     115||||||= **5M events** =||
     116||= **`SURI-YENNIE`** =||= **`GRV`** =||= **`FIORE`** =||
     117|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_contour.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_contour.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_contour.png, 500px)]] ||
     118|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_contourlarge.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_contourlarge.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_contourlarge.png, 500px)]] ||
     119|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_contourx.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_contourx.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_contourx.png, 500px)]] ||
     120|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_etapair.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_etapair.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_etapair.png, 500px)]] ||
     121|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_etarem.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_etarem.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_etarem.png, 500px)]] ||
     122|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_invm.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_invm.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_invm.png, 500px)]] ||
     123|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_invmlarge.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_invmlarge.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_invmlarge.png, 500px)]] ||
     124|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_lego.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_lego.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_lego.png, 500px)]] ||
     125|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_legolarge.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_legolarge.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_legolarge.png, 500px)]] ||
     126|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_legox.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_legox.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_legox.png, 500px)]] ||
     127|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_legoxlarge.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_legoxlarge.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_legoxlarge.png, 500px)]] ||
     128|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_mx.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_mx.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_mx.png, 500px)]] ||
     129|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_mx_zoom.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_mx_zoom.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_mx_zoom.png, 500px)]] ||
     130|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_mx_zoom2.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_mx_zoom2.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_mx_zoom2.png, 500px)]] ||
     131|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_mx2_zoom.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_mx2_zoom.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_mx2_zoom.png, 500px)]] ||
     132|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_mx2_zoom2.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_mx2_zoom2.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_mx2_zoom2.png, 500px)]] ||
     133|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_ptpair.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_ptpair.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_ptpair.png, 500px)]] ||
     134|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_ptpairlarge.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_ptpairlarge.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_ptpairlarge.png, 500px)]] ||
     135|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_Q2.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_Q2.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_Q2.png, 500px)]] ||
     136|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_Q2large.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_Q2large.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_Q2large.png, 500px)]] ||
     137|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_x.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_x.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_x.png, 500px)]] ||
     138|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_xi.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_xi.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_xi.png, 500px)]] ||
     139|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_xilog.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_xilog.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_xilog.png, 500px)]] ||
     140|| [[Image(source:/trunk/plots/no_cuts/5M_evt/SURI_5Mevt_ypair.png, 500px)]] ||  [[Image(source:/trunk/plots/no_cuts/5M_evt/GRV_5Mevt_ypair.png, 500px)]]  || [[Image(source:/trunk/plots/no_cuts/5M_evt/FIORE_5Mevt_ypair.png, 500px)]] ||
     141
     142
     143=== Experimental cuts ===
     144
     145In order to have results closer to the observed results in the data analysis, event samples are produced within the experimental acceptance used for at trigger level in CMS:
     146
     1471. p,,T,,(mu) < 3 GeV;
     148
     1492. |η(mu)| < 2.4.
     150
     1513. p,,T,,(mu^+^mu^-^) > 10 GeV.
     152
     153The first set of plots shows the events restricted to a hadronic system with mass lower than **100 GeV**, while the second consider masses up to 300 GeV.
     154
     155||||||= **1M events** =||
     156||||||= **M,,X,, < 100 GeV** =||
     157||= **`SURI-YENNIE`** =||= **`GRV`** =||
     158|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_contour_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_contour_Q2_nocut_exp_accp_MXmax_100.png, 500px)]]  ||
     159|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_contourlarge_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_contourlarge_Q2_nocut_exp_accp_MXmax_100.png, 500px)]]  ||
     160|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_contourx_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_contourx_Q2_nocut_exp_accp_MXmax_100.png, 500px)]]  ||
     161|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_etapair_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_etapair_Q2_nocut_exp_accp_MXmax_100.png, 500px)]]  ||
     162|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_etarem_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_etarem_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||
     163|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_invm_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_invm_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||
     164|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_invmlarge_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_invmlarge_Q2_nocut_exp_accp_MXmax_100.png, 500px)]]  ||
     165|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_lego_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_lego_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||
     166|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_legolarge_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_legolarge_Q2_nocut_exp_accp_MXmax_100.png, 500px)]]  ||
     167|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_legox_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_legox_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||
     168|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_legoxlarge_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_legoxlarge_Q2_nocut_exp_accp_MXmax_100.png, 500px)]]  ||
     169|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_mx_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_mx_Q2_nocut_exp_accp_MXmax_100.png, 500px)]]  ||
     170|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_mx_zoom_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_mx_zoom_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||
     171|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_mx_zoom2_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_mx_zoom2_Q2_nocut_exp_accp_MXmax_100.png, 500px)]]  ||
     172|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_mx2_zoom_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_mx2_zoom_Q2_nocut_exp_accp_MXmax_100.png, 500px)]]  ||
     173|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_mx2_zoom2_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_mx2_zoom2_Q2_nocut_exp_accp_MXmax_100.png, 500px)]]  ||
     174|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_ptpair_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_ptpair_Q2_nocut_exp_accp_MXmax_100.png, 500px)]]  ||
     175|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_ptpairlarge_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_ptpairlarge_Q2_nocut_exp_accp_MXmax_100.png, 500px)]]  ||
     176|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_Q2_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_Q2_Q2_nocut_exp_accp_MXmax_100.png, 500px)]]  ||
     177|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_Q2large_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_Q2large_Q2_nocut_exp_accp_MXmax_100.png, 500px)]]  ||
     178|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_x_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_x_Q2_nocut_exp_accp_MXmax_100.png, 500px)]]  ||
     179|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_xi_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_xi_Q2_nocut_exp_accp_MXmax_100.png, 500px)]]  ||
     180|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_xilog_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_xilog_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||
     181|| [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/SURI_1Mevt_ypair_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_100GeV/GRV_1Mevt_ypair_Q2_nocut_exp_accp_MXmax_100.png, 500px)]] ||
     182
     183
     184||||||= **1M events** =||
     185||||||= **M,,X,, < 300 GeV** =||
     186||= **`SURI-YENNIE`** =||= **`GRV`** =||
     187|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_contour_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_contour_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     188|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_contourlarge_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_contourlarge_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     189|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_contourx_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_contourx_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     190|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_etapair_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_etapair_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     191|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_etarem_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_etarem_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     192|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_invm_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_invm_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     193|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_invmlarge_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_invmlarge_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     194|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_lego_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_lego_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     195|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_legolarge_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_legolarge_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     196|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_legox_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_legox_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     197|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_legoxlarge_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_legoxlarge_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     198|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_mx_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_mx_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     199|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_mx_zoom_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_mx_zoom_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||
     200|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_mx_zoom2_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_mx_zoom2_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     201|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_mx2_zoom_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_mx2_zoom_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     202|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_mx2_zoom2_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_mx2_zoom2_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     203|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_ptpair_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_ptpair_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     204|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_ptpairlarge_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_ptpairlarge_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     205|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_Q2_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_Q2_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     206|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_Q2large_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_Q2large_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     207|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_x_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_x_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     208|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_xi_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_xi_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     209|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_xilog_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_xilog_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||
     210|| [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/SURI_1Mevt_ypair_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/MXmax_300GeV/GRV_1Mevt_ypair_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||
     211
     212
     213=== Ratio ===
     214
     215The comparisons are performed by, first, the ratio between the distributions with and without experimental acceptance and, next, the `SURI-YENNIE` and `GRV` parametrizations.
     216
     217||||||= **1M events** =||
     218||||||= **M,,X,, < 300 GeV** =||
     219||= **`SURI-YENNIE`** =||= **`GRV`** =||
     220|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI:cuts-nocuts_1Mevt_etapair_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_GRV:cuts-nocuts_1Mevt_etapair_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     221|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI:cuts-nocuts_1Mevt_etarem_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_GRV:cuts-nocuts_1Mevt_etarem_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     222|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI:cuts-nocuts_1Mevt_invm_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_GRV:cuts-nocuts_1Mevt_invm_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     223|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI:cuts-nocuts_1Mevt_invmlarge_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_GRV:cuts-nocuts_1Mevt_invmlarge_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     224|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI:cuts-nocuts_1Mevt_mx_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_GRV:cuts-nocuts_1Mevt_mx_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     225|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI:cuts-nocuts_1Mevt_mx_zoom_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_GRV:cuts-nocuts_1Mevt_mx_zoom_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||
     226|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI:cuts-nocuts_1Mevt_mx_zoom2_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_GRV:cuts-nocuts_1Mevt_mx_zoom2_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     227|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI:cuts-nocuts_1Mevt_mx2_zoom_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_GRV:cuts-nocuts_1Mevt_mx2_zoom_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     228|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI:cuts-nocuts_1Mevt_mx2_zoom2_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_GRV:cuts-nocuts_1Mevt_mx2_zoom2_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     229|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI:cuts-nocuts_1Mevt_ptpair_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_GRV:cuts-nocuts_1Mevt_ptpair_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     230|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI:cuts-nocuts_1Mevt_ptpairlarge_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_GRV:cuts-nocuts_1Mevt_ptpairlarge_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     231|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI:cuts-nocuts_1Mevt_Q2_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_GRV:cuts-nocuts_1Mevt_Q2_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     232|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI:cuts-nocuts_1Mevt_Q2large_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_GRV:cuts-nocuts_1Mevt_Q2large_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     233|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI:cuts-nocuts_1Mevt_x_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_GRV:cuts-nocuts_1Mevt_x_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     234|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI:cuts-nocuts_1Mevt_xi_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_GRV:cuts-nocuts_1Mevt_xi_Q2_nocut_exp_accp_MXmax_300.png, 500px)]]  ||
     235|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI:cuts-nocuts_1Mevt_xilog_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_GRV:cuts-nocuts_1Mevt_xilog_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||
     236|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI:cuts-nocuts_1Mevt_ypair_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||  [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_GRV:cuts-nocuts_1Mevt_ypair_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||
     237
     238||||||= **1M events** =||
     239||||||= **M,,X,, < 300 GeV** =||
     240||= **`RATIO SURI-GRV`** =||
     241|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI-GRV_1Mevt_etapair_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] || [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI-GRV_1Mevt_etarem_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] || [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI-GRV_1Mevt_invm_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||
     242|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI-GRV_1Mevt_invmlarge_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] || [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI-GRV_1Mevt_mx_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] || [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI-GRV_1Mevt_mx_zoom_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||
     243|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI-GRV_1Mevt_mx_zoom2_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] || [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI-GRV_1Mevt_mx2_zoom_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] || [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI-GRV_1Mevt_mx2_zoom2_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||
     244|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI-GRV_1Mevt_ptpair_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] || [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI-GRV_1Mevt_ptpairlarge_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] || [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI-GRV_1Mevt_Q2_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||
     245|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI-GRV_1Mevt_Q2large_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] || [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI-GRV_1Mevt_x_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] || [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI-GRV_1Mevt_xi_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||
     246|| [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI-GRV_1Mevt_xilog_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] || [[Image(source:/trunk/plots/exp_cuts/ratio_MXmax_300GeV/RATIO_SURI-GRV_1Mevt_ypair_Q2_nocut_exp_accp_MXmax_300.png, 500px)]] ||||