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Name: ATLAS_2014_I1279489 | ||
Year: 2014 | ||
Summary: Measurements of the electroweak production of dijets in associated with a Z-boson and distributions sensitive to vector boson fusion | ||
Experiment: ATLAS | ||
Collider: LHC | ||
InspireID: 1279489 | ||
Status: VALIDATED | ||
Authors: | ||
- Kiran Joshi <[email protected]> | ||
#References: | ||
- JHEP 1404 (2014) 031 | ||
- arXiv:1401.7610[hep-ex] | ||
RunInfo: | ||
Generate Z+jets events at 8 TeV, with Z decaying to muons or electrons and pT(j1)>55 GeV, pT(j2)>45 GeV. | ||
NumEvents: 10000000 | ||
NeedCrossSection: no | ||
Beams: [p+, p+] | ||
Energies: [8000] | ||
PtCuts: [55, 45] | ||
Description: | ||
'Measurements differential distributions for inclusive Z-boson-plus-dijet production are performed | ||
in five fiducial regions, each with different sensitivity to the electroweak contribution. Measured distributions | ||
include the differential cross section as a function of the dijet invariant mass, the differential cross section | ||
and a function of the dijet rapidity separation, the differential cross section as a function of the number of jets | ||
in the rapidity interval bounded by the two leading jets. Other measurements include the jet veto effiency as a function | ||
of the dijet invariant mass and rapdity separation, the normalized transverse momentum balance cut efficiency, and the | ||
average number of jets falling into the rapidity interval boundd by the two leading jets, as a function of dijet invariant | ||
mass and dijet rapidity separation.' | ||
BibKey: Aad:2014dta | ||
BibTeX: '@article{Aad:2014dta, | ||
author = "Aad, Georges and others", | ||
title = "{Measurement of the electroweak production of dijets in | ||
association with a Z-boson and distributions sensitive to | ||
vector boson fusion in proton-proton collisions at | ||
$\sqrt{s} =$ 8 TeV using the ATLAS detector}", | ||
collaboration = "ATLAS Collaboration", | ||
journal = "JHEP", | ||
volume = "1404", | ||
pages = "031", | ||
doi = "10.1007/JHEP04%282014%29031, 10.1007/JHEP04(2014)031", | ||
year = "2014", | ||
eprint = "1401.7610", | ||
archivePrefix = "arXiv", | ||
primaryClass = "hep-ex", | ||
reportNumber = "CERN-PH-EP-2013-227", | ||
SLACcitation = "%%CITATION = ARXIV:1401.7610;%%", | ||
}' |
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# BEGIN PLOT /ATLAS_2014_I1279489/d0*-x0*-y0* | ||
RatioPlotMode=default | ||
# END PLOT | ||
|
||
## MJJ BASELINE | ||
# BEGIN PLOT /ATLAS_2014_I1279489/d01-x01-y01 | ||
Title=m$_{\text{jj}}$ in the baseline region | ||
XLabel=m$_{\text{jj}}$ [GeV] | ||
YLabel=$\frac{1}{\sigma} \frac{d\sigma}{dm_{\text{jj}}}$ | ||
# END PLOT | ||
|
||
# BEGIN PLOT /ATLAS_2014_I1279489/d01-x01-y02 | ||
Title=Jet veto efficiency vs. m$_{\text{jj}}$ in the baseline region | ||
XLabel=m$_{\text{jj}}$ [GeV] | ||
YLabel=Jet veto efficiency | ||
LogY=0 | ||
# END PLOT | ||
|
||
# BEGIN PLOT /ATLAS_2014_I1279489/d01-x01-y03 | ||
Title=$p_{\text{T}}^{\text{balance}}$ cut efficiency vs. m$_{\text{jj}}$ in the baseline region | ||
XLabel=m$_{\text{jj}}$ [GeV] | ||
YLabel=$p_{\text{T}}^{\text{balance}}$ | ||
LogY=0 | ||
# END PLOT | ||
|
||
# BEGIN PLOT /ATLAS_2014_I1279489/d01-x01-y04 | ||
Title=$<N_{\text{jet}}^{\text{gap}}>$ vs. m$_{\text{jj}}$ in the baseline region | ||
XLabel=m$_{\text{jj}}$ [GeV] | ||
YLabel=$<N_{\text{jet}}^{\text{gap}}>$ | ||
LogY=0 | ||
# END PLOT | ||
|
||
## DY BASELINE | ||
# BEGIN PLOT /ATLAS_2014_I1279489/d01-x02-y01 | ||
Title=$|\Delta y|$ in the baseline region | ||
XLabel=$|\Delta y|$ | ||
YLabel=$\frac{1}{\sigma} \frac{d\sigma}{d|\Delta y|}$ | ||
# END PLOT | ||
|
||
# BEGIN PLOT /ATLAS_2014_I1279489/d01-x02-y02 | ||
Title=Jet veto efficiency vs. $|\Delta y|$ in the baseline region | ||
XLabel=$|\Delta y|$ | ||
YLabel=Jet veto efficiency | ||
LogY=0 | ||
# END PLOT | ||
|
||
# BEGIN PLOT /ATLAS_2014_I1279489/d01-x02-y03 | ||
Title=$p_{\text{T}}^{\text{balance}}$ cut efficiency vs. $|\Delta y|$ in the baseline region | ||
XLabel=$|\Delta y|$ | ||
YLabel=$p_{\text{T}}^{\text{balance}}$ | ||
LogY=0 | ||
# END PLOT | ||
|
||
# BEGIN PLOT /ATLAS_2014_I1279489/d01-x02-y04 | ||
Title=$<N_{\text{jet}}^{\text{gap}}>$ vs. $|\Delta y|$ in the baseline region | ||
XLabel=$|\Delta y|$ | ||
YLabel=$<N_{\text{jet}}^{\text{gap}}>$ | ||
LogY=0 | ||
# END PLOT | ||
|
||
|
||
|
||
## MJJ HIGH-PT | ||
# BEGIN PLOT /ATLAS_2014_I1279489/d02-x01-y01 | ||
Title=m$_{\text{jj}}$ in the high-$p_{\text{T}}$ region | ||
XLabel=m$_{\text{jj}}$ [GeV] | ||
YLabel=$\frac{1}{\sigma} \frac{d\sigma}{dm_{\text{jj}}}$ | ||
# END PLOT | ||
|
||
# BEGIN PLOT /ATLAS_2014_I1279489/d02-x01-y02 | ||
Title=Jet veto efficiency vs. m$_{\text{jj}}$ in the high-$p_{\text{T}}$ region | ||
XLabel=m$_{\text{jj}}$ [GeV] | ||
YLabel=Jet veto efficiency | ||
LogY=0 | ||
# END PLOT | ||
|
||
# BEGIN PLOT /ATLAS_2014_I1279489/d02-x01-y03 | ||
Title=$p_{\text{T}}^{\text{balance}}$ cut efficiency vs. m$_{\text{jj}}$ in the high-$p_{\text{T}}$ region | ||
XLabel=m$_{\text{jj}}$ [GeV] | ||
YLabel=$p_{\text{T}}^{\text{balance}}$ | ||
LogY=0 | ||
# END PLOT | ||
|
||
# BEGIN PLOT /ATLAS_2014_I1279489/d02-x01-y04 | ||
Title=$<N_{\text{jet}}^{\text{gap}}>$ vs. m$_{\text{jj}}$ in the high-$p_{\text{T}}$ region | ||
XLabel=m$_{\text{jj}}$ [GeV] | ||
YLabel=$<N_{\text{jet}}^{\text{gap}}>$ | ||
LogY=0 | ||
# END PLOT | ||
|
||
## DY HIGH-PT | ||
# BEGIN PLOT /ATLAS_2014_I1279489/d02-x02-y01 | ||
Title=$|\Delta y|$ in the high-$p_{\text{T}}$ region | ||
XLabel=$|\Delta y|$ | ||
YLabel=$\frac{1}{\sigma} \frac{d\sigma}{d|\Delta y|}$ | ||
# END PLOT | ||
|
||
# BEGIN PLOT /ATLAS_2014_I1279489/d02-x02-y02 | ||
Title=Jet veto efficiency vs. $|\Delta y|$ in the high-$p_{\text{T}}$ region | ||
XLabel=$|\Delta y|$ | ||
YLabel=Jet veto efficiency | ||
LogY=0 | ||
# END PLOT | ||
|
||
# BEGIN PLOT /ATLAS_2014_I1279489/d02-x02-y03 | ||
Title=$p_{\text{T}}^{\text{balance}}$ cut efficiency vs. $|\Delta y|$ in the high-$p_{\text{T}}$ region | ||
XLabel=$|\Delta y|$ | ||
YLabel=$p_{\text{T}}^{\text{balance}}$ | ||
LogY=0 | ||
# END PLOT | ||
|
||
# BEGIN PLOT /ATLAS_2014_I1279489/d02-x02-y04 | ||
Title=$<N_{\text{jet}}^{\text{gap}}>$ vs. $|\Delta y|$ in the high-$p_{\text{T}}$ region | ||
XLabel=$|\Delta y|$ | ||
YLabel=$<N_{\text{jet}}^{\text{gap}}>$ | ||
LogY=0 | ||
# END PLOT | ||
|
||
|
||
## MJJ SEARCH | ||
# BEGIN PLOT /ATLAS_2014_I1279489/d03-x01-y01 | ||
Title=m$_{\text{jj}}$ in the search region | ||
XLabel=m$_{\text{jj}}$ [GeV] | ||
YLabel=$\frac{1}{\sigma} \frac{d\sigma}{dm_{\text{jj}}}$ | ||
# END PLOT | ||
|
||
## DY SEARCH | ||
# BEGIN PLOT /ATLAS_2014_I1279489/d03-x02-y01 | ||
Title=$|\Delta y|$ in the search region | ||
XLabel=$|\Delta y|$ | ||
YLabel=$\frac{1}{\sigma} \frac{d\sigma}{d|\Delta y|}$ | ||
# END PLOT | ||
|
||
|
||
## MJJ CONTROL | ||
# BEGIN PLOT /ATLAS_2014_I1279489/d04-x01-y01 | ||
Title=m$_{\text{jj}}$ in the control region | ||
XLabel=m$_{\text{jj}}$ [GeV] | ||
YLabel=$\frac{1}{\sigma} \frac{d\sigma}{dm_{\text{jj}}}$ | ||
# END PLOT | ||
|
||
## DY CONTROL | ||
# BEGIN PLOT /ATLAS_2014_I1279489/d04-x02-y01 | ||
Title=$|\Delta y|$ in the control region | ||
XLabel=$|\Delta y|$ | ||
YLabel=$\frac{1}{\sigma} \frac{d\sigma}{d|\Delta y|}$ | ||
# END PLOT | ||
|
||
## HIGH MASS PLOTS | ||
# BEGIN PLOT /ATLAS_2014_I1279489/d05-x03-y01 | ||
Title=$N_{\text{jet}}^{\text{gap}}$ in the high-mass region | ||
XLabel=$N_{\text{jet}}^{\text{gap}}$ | ||
YLabel=$\frac{1}{\sigma} \frac{d\sigma}{dN_{\text{jet}}^{\text{gap}}}$ | ||
# END PLOT | ||
|
||
# BEGIN PLOT /ATLAS_2014_I1279489/d05-x04-y01 | ||
Title=$|\Delta\phi(\text{j,j})|/\pi$ in the high-mass region | ||
XLabel=$|\Delta\phi(\text{j,j})|/\pi$ | ||
YLabel=$\frac{1}{\sigma} \frac{d\sigma}{d|\Delta\phi(\text{j,j})|}$ | ||
# END PLOT | ||
|
||
# BEGIN PLOT /ATLAS_2014_I1279489/d05-x05-y01 | ||
Title=$p_{\text{T}}^{\text{balance}}$ in the high-mass region | ||
XLabel=$p_{\text{T}}^{\text{balance}}$ | ||
YLabel=$\frac{1}{\sigma} \frac{d\sigma}{dp_{\text{T}}^{\text{balance}}}$ | ||
# END PLOT |
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