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[Rivet-svn] r2490 - in trunk: doc src/Analyses src/Tools
blackhole at projects.hepforge.org
blackhole at projects.hepforge.org
Sat Jun 19 22:17:25 BST 2010
Author: buckley
Date: Sat Jun 19 22:17:26 2010
New Revision: 2490
Log:
Cosmetics, just to clear my working dir ;)
Modified:
trunk/doc/analyses.bib
trunk/doc/analyses.tex
trunk/src/Analyses/CDF_1994_S2952106.cc
trunk/src/Tools/RivetAIDA.cc
Modified: trunk/doc/analyses.bib
==============================================================================
--- trunk/doc/analyses.bib Sat Jun 19 15:19:03 2010 (r2489)
+++ trunk/doc/analyses.bib Sat Jun 19 22:17:26 2010 (r2490)
@@ -190,6 +190,9 @@
% Adams:2006nd
@Article{Adams:2006nd, author = "Adams, John and others", collaboration = "STAR", title = "{Identified hadron spectra at large transverse momentum in p + p and d + Au collisions at s(NN)**(1/2) = 200-GeV}", journal = "Phys. Lett.", volume = "B637", year = "2006", pages = "161-169", eprint = "nucl-ex/0601033", archivePrefix = "arXiv", doi = "10.1016/j.physletb.2006.04.032", SLACcitation = "%%CITATION = NUCL-EX/0601033;%%" }
+% Alner:1987wb
+ at Article{Alner:1987wb, author = "Alner, G. J. and others", collaboration = "UA5", title = "{UA5: A general study of proton-antiproton physics at $\sqrt{s}$ = 546-GeV}", journal = "Phys. Rept.", volume = "154", year = "1987", pages = "247-383", doi = "10.1016/0370-1573(87)90130-X", SLACcitation = "%%CITATION = PRPLC,154,247;%%" }
+
% Affolder:1999ua
@Article{Affolder:1999ua, author = "Affolder, Anthony Allen and others", collaboration = "CDF", title = "{A measurement of the differential dijet mass cross section in $p\bar{p}$ collisions at $\sqrt{s} = 1.8$ TeV}", journal = "Phys. Rev.", volume = "D61", year = "2000", pages = "091101", eprint = "hep-ex/9912022", archivePrefix = "arXiv", doi = "10.1103/PhysRevD.61.091101", SLACcitation = "%%CITATION = HEP-EX/9912022;%%" }
@@ -199,6 +202,9 @@
% Abachi:1995zv
@Article{Abachi:1995zv, author = "Abachi, S. and others", collaboration = "D0", title = "{Studies of Topological Distributions of the Three- and Four-Jet Events in $\bar{p}p$ Collisions at $\sqrt{s}=1800$ GeV with the D\O\\ Detector}", journal = "Phys. Rev.", volume = "D53", year = "1996", pages = "6000-6016", eprint = "hep-ex/9509005", archivePrefix = "arXiv", doi = "10.1103/PhysRevD.53.6000", SLACcitation = "%%CITATION = HEP-EX/9509005;%%" }
+% Abbiendi:2001qn
+ at Article{Abbiendi:2001qn, author = "Abbiendi, G. and others", collaboration = "OPAL", title = "{A simultaneous measurement of the QCD colour factors and the strong coupling}", journal = "Eur. Phys. J.", volume = "C20", year = "2001", pages = "601-615", eprint = "hep-ex/0101044", archivePrefix = "arXiv", doi = "10.1007/s100520100699", SLACcitation = "%%CITATION = HEP-EX/0101044;%%" }
+
% Aaltonen:2009ty
@Article{Aaltonen:2009ty, author = "Aaltonen, T. and others", collaboration = "CDF", title = "{Measurement of the Inclusive Isolated Prompt Photon Cross Section in ppbar Collisions at sqrt{s} = 1.96 TeV using the CDF Detector}", journal = "Phys. Rev.", volume = "D80", year = "2009", pages = "111106", eprint = "0910.3623", archivePrefix = "arXiv", primaryClass = "hep-ex", doi = "10.1103/PhysRevD.80.111106", SLACcitation = "%%CITATION = 0910.3623;%%" }
Modified: trunk/doc/analyses.tex
==============================================================================
--- trunk/doc/analyses.tex Sat Jun 19 15:19:03 2010 (r2489)
+++ trunk/doc/analyses.tex Sat Jun 19 22:17:26 2010 (r2490)
@@ -303,6 +303,37 @@
\clearpage
+\typeout{Handling analysis OPAL_2001_S4553896}
+\subsection[OPAL\_2001\_S4553896]{OPAL\_2001\_S4553896\,\cite{Abbiendi:2001qn}}
+\textbf{Four-jet angles using Durham algorithm}\newline
+\textbf{Experiment:} OPAL (LEP Run 1) \newline
+\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+4553896}{4553896}\newline
+\textbf{Status:} VALIDATED\newline
+\textbf{Authors:}
+ \penalty 100
+\begin{itemize}
+ \item Frank Siegert $\langle\,$\href{mailto:frank.siegert at cern.ch}{frank.siegert at cern.ch}$\,\rangle$;
+\end{itemize}
+\textbf{References:}
+ \penalty 100
+\begin{itemize}
+ \item Eur.Phys.J.C20:601-615,2001
+ \item DOI: \href{http://dx.doi.org/10.1007/s100520100699}{10.1007/s100520100699}
+ \item arXiv: \href{http://arxiv.org/abs/hep-ex/0101044}{hep-ex/0101044}
+\end{itemize}
+\textbf{Run details:}
+ \penalty 100
+\begin{itemize}
+
+ \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV) Hadronisation should be turned off because the data is corrected back to the parton level.\end{itemize}
+
+\noindent Angles between the leading (in energy) four jets defined using the Durham algorithm with $y_\mathrm{cut}=0.008$. The data is presented at the parton level and includes the Bengtsson-Zerwas, Korner-Schierholz-Willrodt and Nachtmann-Reiter angles as well as the angle between the two softest jets.
+
+\clearpage
+
+
+\clearpage
+
\typeout{Handling analysis OPAL_2004_S6132243}
\subsection[OPAL\_2004\_S6132243]{OPAL\_2004\_S6132243\,\cite{Abbiendi:2004qz}}
\textbf{Event shape distributions and moments in $e^+ e^-$ \ensuremath{\to} hadrons at 91--209 GeV}\newline
@@ -1247,6 +1278,36 @@
\clearpage
+\typeout{Handling analysis CDF_2009_NOTE_9936}
+\subsection{CDF\_2009\_NOTE\_9936}
+\textbf{CDF Run 2 min bias charged multiplicity analysis}\newline
+\textbf{Experiment:} CDF (Tevatron Run 2) \newline
+\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+None}{None}\newline
+\textbf{Status:} VALIDATED\newline
+\textbf{Authors:}
+ \penalty 100
+\begin{itemize}
+ \item Holger Schulz $\langle\,$\href{mailto:holger.schulz at physik.hu-berlin.de}{holger.schulz at physik.hu-berlin.de}$\,\rangle$;
+\end{itemize}
+\textbf{References:}
+ \penalty 100
+\begin{itemize}
+ \item CDF public note 9936
+ \item http://www-cdf.fnal.gov/physics/new/qcd/minbias_mult09/multpage.html
+\end{itemize}
+\textbf{Run details:}
+ \penalty 100
+\begin{itemize}
+
+ \item $p\bar{p}$ QCD interactions at 1960~GeV. Particles with $c \\tau > {}$10 mm should be set stable.\end{itemize}
+
+\noindent Niccolo Moggi's min bias analysis. Minimum bias events are used to measure the charged multiplicity distribution. The multiplicity distribution was not published in S8233977 but the numbers and a public note are available from the CDF website given above. Note: the systematic and statistical errors in Rivet were added in quadrature.
+
+\clearpage
+
+
+\clearpage
+
\typeout{Handling analysis CDF_2009_S8233977}
\subsection[CDF\_2009\_S8233977]{CDF\_2009\_S8233977\,\cite{Aaltonen:2009ne}}
\textbf{CDF Run 2 min bias cross-section analysis}\newline
@@ -2038,12 +2099,41 @@
\clearpage
+\typeout{Handling analysis UA5_1987_S1640666}
+\subsection[UA5\_1987\_S1640666]{UA5\_1987\_S1640666\,\cite{Alner:1987wb}}
+\textbf{UA5 charged multiplicity measurements at 546 GeV}\newline
+\textbf{Experiment:} UA5 (CERN SPS) \newline
+\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+1640666}{1640666}\newline
+\textbf{Status:} VALIDATED\newline
+\textbf{Authors:}
+ \penalty 100
+\begin{itemize}
+ \item Holger Schulz $\langle\,$\href{mailto:holger.schulz at physik.hu-berlin.de}{holger.schulz at physik.hu-berlin.de}$\,\rangle$;
+\end{itemize}
+\textbf{References:}
+ \penalty 100
+\begin{itemize}
+ \item Phys.Rept.154:247-383,1987
+\end{itemize}
+\textbf{Run details:}
+ \penalty 100
+\begin{itemize}
+
+ \item QCD and diffractive events at 546 GeV\end{itemize}
+
+\noindent Charged particle multiplicity measurement.
+
+\clearpage
+
+
+\clearpage
+
\typeout{Handling analysis UA5_1988_S1867512}
\subsection[UA5\_1988\_S1867512]{UA5\_1988\_S1867512\,\cite{Ansorge:1988fg}}
-\textbf{Charged particle correlations in ppbar non-single-diffractive events of the UA5 detector at \ensuremath{\sqrt{s}} = 200, 546 and 900 GeV.}\newline
+\textbf{Charged particle correlations in UA5 $p \\bar{p}$ NSD events at \ensuremath{\sqrt{s}} = 200, 546 and 900 GeV.}\newline
\textbf{Experiment:} UA5 (CERN SPS) \newline
\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+1867512}{1867512}\newline
-\textbf{Status:} UNVALIDATED\newline
+\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
\penalty 100
\begin{itemize}
@@ -2058,9 +2148,9 @@
\penalty 100
\begin{itemize}
- \item ppbar events. Non-single diffractive events need to be switched on. The trigger implementation is the same as in UA5_1989_S1926373.\end{itemize}
+ \item ppbar events. Non-single diffractive events need to be switched on. The trigger implementation is the same as in UA5_1989_S1926373. Important: Only the correlation strengths with symmetric eta bins should be used for tuning.\end{itemize}
-\noindent Data on two-particle pseudorapidity and multiplicity correlations of charged particles for non single-diffractive $\bar{p}p$ collisions at c.m. energies of 200, 546 and 900 GeV. Pseudorapidity correlations interpreted in terms of a cluster model, which has been motivated by this and other experiments, require on average about two charged particles per cluster. The decay width of the clusters in pseudorapidity is approximately independent of multiplicity and of c.m. energy. The investigations of correlations in terms of pseudorapidity gaps confirm the picture of cluster production. The strength of forward-backward multiplicity correlations increases linearly with ins and depends strongly on position and size of the pseudorapidity gap separating the forward and backward interval. All our correlation studies can be understood in terms of a cluster model in which clusters contain on average about two charged particles, i.e. are of similar magnitude to earlier estimates
from the ISR.
+\noindent Data on two-particle pseudorapidity and multiplicity correlations of charged particles for non single-diffractive $ar{p}p$ collisions at c.m. energies of 200, 546 and 900 GeV. Pseudorapidity correlations interpreted in terms of a cluster model, which has been motivated by this and other experiments, require on average about two charged particles per cluster. The decay width of the clusters in pseudorapidity is approximately independent of multiplicity and of c.m. energy. The investigations of correlations in terms of pseudorapidity gaps confirm the picture of cluster production. The strength of forward-backward multiplicity correlations increases linearly with ins and depends strongly on position and size of the pseudorapidity gap separating the forward and backward interval. All our correlation studies can be understood in terms of a cluster model in which clusters contain on average about two charged particles, i.e. are of similar magnitude to earlier estimates
from the ISR.
\clearpage
Modified: trunk/src/Analyses/CDF_1994_S2952106.cc
==============================================================================
--- trunk/src/Analyses/CDF_1994_S2952106.cc Sat Jun 19 15:19:03 2010 (r2489)
+++ trunk/src/Analyses/CDF_1994_S2952106.cc Sat Jun 19 22:17:26 2010 (r2490)
@@ -125,7 +125,7 @@
_Et_cosphi_sum = jets[i].momentum().Et() * sin(jets[i].phi());
_Et_sum = jets[i].momentum().Et() * sin(jets[i].phi());
}
- if (sqrt(_Et_sinphi_sum*_Et_sinphi_sum + _Et_cosphi_sum*_Et_cosphi_sum)/_Et_sum > 6.0)
+ if (sqrt(_Et_sinphi_sum*_Et_sinphi_sum + _Et_cosphi_sum*_Et_cosphi_sum)/_Et_sum > 6.0)
vetoEvent;
// Check jet requirements
@@ -276,7 +276,7 @@
//AIDA::IHistogramFactory& hf = histogramFactory();
- AIDA::IDataPointSetFactory& hf = datapointsetFactory();
+ //AIDA::IDataPointSetFactory& hf = datapointsetFactory();
/// @todo Histo factory output paths don't work this way
//hf.multiply(histoDir() + "/d03-x01-y01", *_histJet3eta, *_histEta3Corr);
Modified: trunk/src/Tools/RivetAIDA.cc
==============================================================================
--- trunk/src/Tools/RivetAIDA.cc Sat Jun 19 15:19:03 2010 (r2489)
+++ trunk/src/Tools/RivetAIDA.cc Sat Jun 19 22:17:26 2010 (r2490)
@@ -46,7 +46,7 @@
const map<string, vector<DPSXPoint> > getDPSXValsErrs(string papername) {
// Get filename
const string xmlfile = getDatafilePath(papername);
-
+
// Open AIDA XML file
TiXmlDocument doc(xmlfile);
doc.LoadFile();
@@ -56,10 +56,10 @@
cerr << err << endl;
throw Error(err);
}
-
+
// Return value, to be populated
map<string, vector<DPSXPoint> > rtn;
-
+
try {
// Walk down tree to get to the <paper> element
const TiXmlNode* aidaN = doc.FirstChild("aida");
@@ -73,7 +73,7 @@
cerr << "Skipping non-reference histogram " << plotname << endl;
continue;
}
-
+
/// @todo Check that "path" matches filename
vector<DPSXPoint> points;
for (const TiXmlNode* dpN = dpsN->FirstChild("dataPoint"); dpN; dpN = dpN->NextSibling()) {
@@ -99,11 +99,11 @@
/// @todo Throw an exception here?
}
}
-
+
// Add to the map
rtn[plotname] = points;
}
-
+
}
// Write out the error
/// @todo Rethrow as a general XML failure.
@@ -111,11 +111,11 @@
cerr << e.what() << endl;
throw;
}
-
+
// Return
return rtn;
}
-
+
const map<string, BinEdges>
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