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[Rivet-svn] r2249 - in trunk: data/anainfo docblackhole at projects.hepforge.org blackhole at projects.hepforge.orgWed Feb 10 16:22:39 GMT 2010
Author: hoeth Date: Wed Feb 10 16:22:39 2010 New Revision: 2249 Log: Fixing some obvious things in the documentation Modified: trunk/data/anainfo/ALEPH_1991_S2435284.info trunk/data/anainfo/ALEPH_1996_S3196992.info trunk/data/anainfo/CDF_1988_S1865951.info trunk/data/anainfo/CDF_1990_S2089246.info trunk/data/anainfo/CDF_1998_S3618439.info trunk/data/anainfo/CDF_2002_S4796047.info trunk/data/anainfo/CDF_2008_S7540469.info trunk/data/anainfo/D0_2007_S7075677.info trunk/data/anainfo/D0_2008_S7554427.info trunk/data/anainfo/D0_2008_S7837160.info trunk/data/anainfo/PDG_HADRON_MULTIPLICITIES_RATIOS.info trunk/data/anainfo/STAR_2006_S6860818.info trunk/doc/mk-analysis-latex trunk/doc/rivet-manual.tex Modified: trunk/data/anainfo/ALEPH_1991_S2435284.info ============================================================================== --- trunk/data/anainfo/ALEPH_1991_S2435284.info Tue Feb 9 17:18:25 2010 (r2248) +++ trunk/data/anainfo/ALEPH_1991_S2435284.info Wed Feb 10 16:22:39 2010 (r2249) @@ -17,7 +17,7 @@ The charged particle multiplicity distribution of hadronic Z decays, as measured on the peak of the Z resonance using the ALEPH detector at LEP. The unfolding procedure was model independent, and the - distribution was found to have a mean of 20.85+-0.24, Comparison with + distribution was found to have a mean of $20.85 \pm 0.24$, Comparison with lower energy data supports the KNO scaling hypothesis. The shape of the multiplicity distribution is well described by a log-normal distribution, as predicted from a cascading model for multi-particle Modified: trunk/data/anainfo/ALEPH_1996_S3196992.info ============================================================================== --- trunk/data/anainfo/ALEPH_1996_S3196992.info Tue Feb 9 17:18:25 2010 (r2248) +++ trunk/data/anainfo/ALEPH_1996_S3196992.info Wed Feb 10 16:22:39 2010 (r2249) @@ -19,7 +19,7 @@ attributed to radiation from primary quark pairs, have been extended in the ALEPH experiment to include hard photon production inside hadron jets. Events are selected where all particles combine democratically to form hadron jets, - one of which contains a photon with a fractional energy z > 0.7. After + one of which contains a photon with a fractional energy $z > 0.7$. After statistical subtraction of non-prompt photons, the quark-to-photon - fragmentation function, D(z), is extracted directly from the measured 2-jet + fragmentation function, $D(z)$, is extracted directly from the measured 2-jet rate. Modified: trunk/data/anainfo/CDF_1988_S1865951.info ============================================================================== --- trunk/data/anainfo/CDF_1988_S1865951.info Tue Feb 9 17:18:25 2010 (r2248) +++ trunk/data/anainfo/CDF_1988_S1865951.info Wed Feb 10 16:22:39 2010 (r2249) @@ -14,5 +14,5 @@ References: - Phys.Rev.Lett.61:1819,1988 - doi:10.1103/PhysRevLett.61.1819 -RunInfo: QCD min bias events at sqrtS = 630 GeV and 1800 GeV, |eta| < 1.0. +RunInfo: QCD min bias events at sqrtS = 630 GeV and 1800 GeV, $|\eta| < 1.0$. Energies: [630,1800] Modified: trunk/data/anainfo/CDF_1990_S2089246.info ============================================================================== --- trunk/data/anainfo/CDF_1990_S2089246.info Tue Feb 9 17:18:25 2010 (r2248) +++ trunk/data/anainfo/CDF_1990_S2089246.info Wed Feb 10 16:22:39 2010 (r2249) @@ -12,7 +12,7 @@ - doi:10.1103/PhysRevD.41.2330 RunInfo: QCD min bias events at sqrt(s) = 630 and 1800 GeV. - Particles with ctau > 10cm should be set stable. + Particles with $c \tau > 10$mm should be set stable. NumEvents: 1000000 PtCuts: [0] Energies: [630, 1800] Modified: trunk/data/anainfo/CDF_1998_S3618439.info ============================================================================== --- trunk/data/anainfo/CDF_1998_S3618439.info Tue Feb 9 17:18:25 2010 (r2248) +++ trunk/data/anainfo/CDF_1998_S3618439.info Wed Feb 10 16:22:39 2010 (r2249) @@ -11,7 +11,7 @@ - Phys.Rev.Lett.80:3461-3466,1998 - 10.1103/PhysRevLett.80.3461 RunInfo: - QCD events at Tevatron with $\sqrt{s}=1.8 TeV$ without MPI. + QCD events at Tevatron with $\sqrt{s}=1.8$ TeV without MPI. NumEvents: 1000000 PtCuts: [0] Description: Modified: trunk/data/anainfo/CDF_2002_S4796047.info ============================================================================== --- trunk/data/anainfo/CDF_2002_S4796047.info Tue Feb 9 17:18:25 2010 (r2248) +++ trunk/data/anainfo/CDF_2002_S4796047.info Wed Feb 10 16:22:39 2010 (r2249) @@ -20,8 +20,8 @@ using a minimum bias trigger in which the data set is divided into two classes corresponding to `soft' and `hard' interactions. For each subsample, the analysis includes measurements of the multiplicity, - transverse momentum (pT) spectra, and the average pT and event-by- - event pT dispersion as a function of multiplicity. A comparison of + transverse momentum (pT) spectra, and the average pT and event-by-event + pT dispersion as a function of multiplicity. A comparison of results shows distinct differences in the behavior of the two samples as a function of the center of mass energy. The properties of the soft sample are invariant as a function of c.m. energy. Modified: trunk/data/anainfo/CDF_2008_S7540469.info ============================================================================== --- trunk/data/anainfo/CDF_2008_S7540469.info Tue Feb 9 17:18:25 2010 (r2248) +++ trunk/data/anainfo/CDF_2008_S7540469.info Wed Feb 10 16:22:39 2010 (r2249) @@ -12,7 +12,7 @@ - arXiv:0711.3717 [hep-ex] RunInfo: ppbar -> e+ e- + jets at 1960 GeV. Needs mass cut on lepton pair to - avoid photon singularity, $m$ in range $66 < m_ee < 116$ + avoid photon singularity, $m$ in range $66 < m_{ee} < 116$ NumEvents: 1000000 PtCuts: [0] Description: Modified: trunk/data/anainfo/D0_2007_S7075677.info ============================================================================== --- trunk/data/anainfo/D0_2007_S7075677.info Tue Feb 9 17:18:25 2010 (r2248) +++ trunk/data/anainfo/D0_2007_S7075677.info Wed Feb 10 16:22:39 2010 (r2249) @@ -15,7 +15,7 @@ RunInfo: Drell-Yan $Z/\gamma*$ + jets events in ppbar collisions at sqrt(s) = 1960 GeV. Needs mass cut on lepton pair to avoid photon - singularity --- $m$ in range $71 < m_ee < 111$ + singularity --- $m$ in range $71 < m_{ee} < 111$ NumEvents: 1000000 PtCuts: [0] Description: Modified: trunk/data/anainfo/D0_2008_S7554427.info ============================================================================== --- trunk/data/anainfo/D0_2008_S7554427.info Tue Feb 9 17:18:25 2010 (r2248) +++ trunk/data/anainfo/D0_2008_S7554427.info Wed Feb 10 16:22:39 2010 (r2249) @@ -12,7 +12,7 @@ - arXiv:0712.0803 RunInfo: "ppbar -> e+ e- + jets at 1960 GeV. Needs mass cut on lepton pair to - avoid photon singularity: $m$ in range $40 < m_ee < 200$ GeV" + avoid photon singularity: $m$ in range $40 < m_{ee} < 200$ GeV" NumEvents: 1000000 PtCuts: [0] Description: Modified: trunk/data/anainfo/D0_2008_S7837160.info ============================================================================== --- trunk/data/anainfo/D0_2008_S7837160.info Tue Feb 9 17:18:25 2010 (r2248) +++ trunk/data/anainfo/D0_2008_S7837160.info Wed Feb 10 16:22:39 2010 (r2249) @@ -19,8 +19,8 @@ NumEvents: 1000000 PtCuts: [0] Description: - Measurement of the electron charge asymmetry in p pbar -> W + X -> e - nu_e + X events at a center of mass energy of 1.96 TeV. The asymmetry + Measurement of the electron charge asymmetry in $p \bar p \to W + X \to + e \nu_e + X$ events at a center of mass energy of 1.96 TeV. The asymmetry is measured as a function of the electron transverse momentum and pseudorapidity in the interval (-3.2, 3.2). This data is sensitive to proton parton distribution functions due to the valence asymmetry in Modified: trunk/data/anainfo/PDG_HADRON_MULTIPLICITIES_RATIOS.info ============================================================================== --- trunk/data/anainfo/PDG_HADRON_MULTIPLICITIES_RATIOS.info Tue Feb 9 17:18:25 2010 (r2248) +++ trunk/data/anainfo/PDG_HADRON_MULTIPLICITIES_RATIOS.info Wed Feb 10 16:22:39 2010 (r2249) @@ -14,10 +14,10 @@ NumEvents: 1000000 PtCuts: [0] Description: - Ratios (w.r.t. $pi^+/pi^-$) of hadron multiplicities in hadronic $e^+e^-$ + Ratios (w.r.t. $\pi^+/\pi^-$) of hadron multiplicities in hadronic $e^+e^-$ events, taken from Review of Particle Properties 2008, table 40.1, page 355. Average hadron multiplicities per hadronic $e^+e^-$ - annihilation event at $\sqrt{s} \approx {}$ 10, 29--35, 91, and 130-- - 200 GeV,normalised to the pion multiplicity. The numbers are averages + annihilation event at $\sqrt{s} \approx$ 10, 29--35, 91, and + 130--200 GeV,normalised to the pion multiplicity. The numbers are averages from various experiments. Correlations of the systematic uncertainties were considered for the calculation of the averages. Modified: trunk/data/anainfo/STAR_2006_S6860818.info ============================================================================== --- trunk/data/anainfo/STAR_2006_S6860818.info Tue Feb 9 17:18:25 2010 (r2248) +++ trunk/data/anainfo/STAR_2006_S6860818.info Wed Feb 10 16:22:39 2010 (r2249) @@ -17,5 +17,5 @@ Description: pT distributions of identified strange particles in pp collisions at $\sqrt{s} = 200$ GeV, measured by the STAR experiment at RHIC in - non-single-diffractive minbias events. WARNING The <pT> vs. particle - mass plot is not validated yet and might be wrong. + non-single-diffractive minbias events. WARNING The $\langle pT \rangle$ vs. + particle mass plot is not validated yet and might be wrong. Modified: trunk/doc/mk-analysis-latex ============================================================================== --- trunk/doc/mk-analysis-latex Tue Feb 9 17:18:25 2010 (r2248) +++ trunk/doc/mk-analysis-latex Wed Feb 10 16:22:39 2010 (r2249) @@ -60,7 +60,7 @@ ## Build analysis pages all_analyses = rivet.AnalysisLoader.analysisNames() -pages = { "LEP":[], "Tevatron":[], "HERA":[], "Monte Carlo":[], "Example":[], "Misc.":[] } +pages = { "LEP":[], "Tevatron":[], "HERA":[], "RHIC":[], "Monte Carlo":[], "Example":[], "Misc.":[] } ## Use list(...) ctor for 2.3 compatibility for aname in sorted(list(all_analyses)): page = "" @@ -157,6 +157,8 @@ pages["Tevatron"].append(page) elif "HERA" in ana.collider(): pages["HERA"].append(page) + elif "RHIC" in ana.collider(): + pages["RHIC"].append(page) elif "EXAMPLE" in ana.name().upper(): pages["Example"].append(page) else: @@ -189,6 +191,7 @@ groups["LEP"] + "\n\n" + \ groups["Tevatron"] + "\n\n" + \ groups["HERA"] + "\n\n" + \ + groups["RHIC"] + "\n\n" + \ groups["Monte Carlo"] + "\n\n" + \ groups["Example"] + "\n\n" + \ groups["Misc."] + "\n\n" Modified: trunk/doc/rivet-manual.tex ============================================================================== --- trunk/doc/rivet-manual.tex Tue Feb 9 17:18:25 2010 (r2248) +++ trunk/doc/rivet-manual.tex Wed Feb 10 16:22:39 2010 (r2249) @@ -217,7 +217,7 @@ running a generator like Sherpa or Herwig++ which provides its own native way to make HepMC output, or a generator like Cascade or PHOJET which is not currently supported by AGILe, then substitute the appropriate command in what follows. -We'll discuss using these commands in detail in \SectionRef{sec:rivetgun}. +We'll discuss using these commands in detail in \SectionRef{sec:agile-runmc}. \subsection{Getting generators for AGILe} @@ -225,7 +225,7 @@ One last thing before continuing, though: the generators themselves. Again, if you're running on a system with the CERN LCG AFS area mounted, then -\kbd{rivetgun} will attempt to automatically use the generators packaged by the +\kbd{agile-runmc} will attempt to automatically use the generators packaged by the LCG Genser team. Otherwise, you'll have to build your own mirror of the LCG generators. This @@ -271,7 +271,7 @@ \section{Running Rivet analyses} -\label{sec:rivetgun} +\label{sec:agile-runmc} The \kbd{rivet} executable is the easiest way to use Rivet, and will be our example throughout this manual. This command reads HepMC events in the standard @@ -354,8 +354,8 @@ \item \paragraph{Fine-grained logging:}{\kbd{rivet in.hepmc -A -l~Rivet.Analysis=DEBUG~\cmdbreak -l~Rivet.Projection=DEBUG - -l~Rivet.Projection.FinalState=TRACE~\cmdbreak -l~RivetGun=WARN - -l~NEvt=WARN} analyse events as before, but will print different status + -l~Rivet.Projection.FinalState=TRACE~\cmdbreak -l~NEvt=WARN} + analyse events as before, but will print different status information as the run progresses. Hierarchical logging control is possible down to the level of individual analyses and projections as shown above; this is useful for debugging without getting overloaded with debug @@ -433,12 +433,13 @@ this case $x$ would be a leading jet \pT. \subsection{Normalising histograms} -\newcommand{\normhisto}{\kbd{rivet-normalise-histos }} Sometimes you want to +\newcommand{\normhisto}{\kbd{rivet-rescale }} Sometimes you want to use histograms normalised to, e.g., the generator cross-section or the area of a reference-data histogram. The script \normhisto was designed for these purposes. The usage is the following: \kbd{\normhisto -O observables -r RIVETDATA -o normalised Rivet.aida} + By default, the normalised histograms are written to file in the AIDA-XML format. You can also give the {-f} switch on the command line to produce flat histograms. @@ -479,14 +480,14 @@ Rivet comes with two commands --- \kbd{compare-histos} and \kbd{make-plots} --- for comparing and plotting data files. These commands produce nice comparison plots of publication quality from the YODA format text files, e.g.:\\ -\inp{compare-plots path/to/CDF_2001_S4751469.aida py.aida:'Pythia 6.418' \cmdbreak hw.aida:'Herwig++ 2.3.0'} +\inp{compare-histos path/to/CDF_2001_S4751469.aida py.aida:'Pythia 6.418' \cmdbreak hw.aida:'Herwig++ 2.3.0'} This command will have compared the three named data files (ending in \kbd{.aida}), identified which plots are available in them, and combined the MC and reference plots appropriately into a set of plot data files ending with \kbd{.dat}. The strings after the ":" for the MC files are specifying ID strings to -appear in the plot legends. You can also run compare-plots to just compare MC--MC -data files. More options are described by running \kbd{compare-histos --help}. +appear in the plot legends. You can also run \kbd{compare-histos} to just compare +MC--MC data files. More options are described by running \kbd{compare-histos --help}. Incidentally, the reference files for each Rivet analysis are to be found in the installed Rivet shared data directory, \kbd{\val{installdir}/share/Rivet}. You @@ -1073,19 +1074,19 @@ the Rivet website: \url{http://projects.hepforge.org/rivet/trac/wiki/} -\cleardoublepage -\part{How Rivet \emph{really} works} -\label{part:internals} - -In time this will be the place to look for all the nitty gritty on what Rivet is -doing internally. Not very many people need to know that, and the few that do -currently don't need a manual for it! - -\section{Projection caching} -\TODO{TODO} - -\subsection{Writing a Projection comparison operator} -\TODO{TODO} +% \cleardoublepage +% \part{How Rivet \emph{really} works} +% \label{part:internals} +% +% In time this will be the place to look for all the nitty gritty on what Rivet is +% doing internally. Not very many people need to know that, and the few that do +% currently don't need a manual for it! +% +% \section{Projection caching} +% \TODO{TODO} +% +% \subsection{Writing a Projection comparison operator} +% \TODO{TODO}
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