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[Rivet-svn] r2322 - in trunk: data/anainfo doc
blackhole at projects.hepforge.org
blackhole at projects.hepforge.org
Tue Mar 9 17:14:32 GMT 2010
Author: buckley
Date: Tue Mar 9 17:14:32 2010
New Revision: 2322
Log:
More fixes to metadata for documentation
Modified:
trunk/data/anainfo/CDF_2000_S4155203.info
trunk/data/anainfo/CDF_2009_S8233977.info
trunk/data/anainfo/D0_2008_S7863608.info
trunk/data/anainfo/JADE_OPAL_2000_S4300807.info
trunk/data/anainfo/OPAL_2004_S6132243.info
trunk/data/anainfo/UA5_1982_S875503.info
trunk/data/anainfo/UA5_1986_S1583476.info
trunk/data/anainfo/UA5_1989_S1926373.info
trunk/doc/analyses.bib
trunk/doc/analyses.tex
trunk/doc/mk-analysis-latex
trunk/doc/rivet-manual.tex
trunk/doc/spiresbib.py
Modified: trunk/data/anainfo/CDF_2000_S4155203.info
==============================================================================
--- trunk/data/anainfo/CDF_2000_S4155203.info Tue Mar 9 15:26:46 2010 (r2321)
+++ trunk/data/anainfo/CDF_2000_S4155203.info Tue Mar 9 17:14:32 2010 (r2322)
@@ -12,8 +12,8 @@
- arXiv:hep-ex/0001021
- doi:10.1103/PhysRevLett.84.845
RunInfo:
- ppbar collisions at 1800 GeV. $Z/\gamma*$ Drell-Yan events with
- $e^+e^-$ decay mode only.
+ $p\bar{p}$ collisions at 1800 GeV.
+ $Z/\gamma^*$ Drell-Yan events with $e^+e^-$ decay mode only.
NumEvents: 1000000
PtCuts: [0]
Description:
@@ -29,5 +29,5 @@
This analysis is subject to ambiguities in the experimental Z pT
definition, since the Rivet implementation reconstructs the Z momentum from the
- dileptonpair with finite cones for photon brem summation, rather than
- YFS/shower unfolding or non-portable direct use of the Z in the event record.
+ dilepton pair with finite cones for QED bremstrahlung summation, rather than
+ non-portable direct use of the (sometimes absent) Z in the event record.
Modified: trunk/data/anainfo/CDF_2009_S8233977.info
==============================================================================
--- trunk/data/anainfo/CDF_2009_S8233977.info Tue Mar 9 15:26:46 2010 (r2321)
+++ trunk/data/anainfo/CDF_2009_S8233977.info Tue Mar 9 17:14:32 2010 (r2322)
@@ -13,8 +13,7 @@
- doi:10.1103/PhysRevD.79.112005
- arXiv:0904.1098 [hep-ex]
RunInfo:
- "* ppbar QCD interactions at 1960 GeV.
- * Particles with $c \\tau > {}$10 mm should be set stable."
+ ppbar QCD interactions at 1960 GeV. Particles with $c \\tau > {}$10 mm should be set stable.
NumEvents: 1000000
PtCuts: [0]
Description:
Modified: trunk/data/anainfo/D0_2008_S7863608.info
==============================================================================
--- trunk/data/anainfo/D0_2008_S7863608.info Tue Mar 9 15:26:46 2010 (r2321)
+++ trunk/data/anainfo/D0_2008_S7863608.info Tue Mar 9 17:14:32 2010 (r2322)
@@ -20,4 +20,4 @@
Description:
Cross sections as a function of pT and rapidity of the boson and pT
and rapidity of the leading jet in $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96
- TeV, based on an integrated luminosity of 1.0 fb$^-1$.
+ TeV, based on an integrated luminosity of 1.0 fb$^{-1}$.
Modified: trunk/data/anainfo/JADE_OPAL_2000_S4300807.info
==============================================================================
--- trunk/data/anainfo/JADE_OPAL_2000_S4300807.info Tue Mar 9 15:26:46 2010 (r2321)
+++ trunk/data/anainfo/JADE_OPAL_2000_S4300807.info Tue Mar 9 17:14:32 2010 (r2322)
@@ -1,6 +1,6 @@
Name: JADE_OPAL_2000_S4300807
Year: 2000
-Summary: Jet rates in e+e- at JADE [35--44 GeV] and OPAL [91--189 GeV].
+Summary: Jet rates in $e^+e^-$ at JADE [35--44 GeV] and OPAL [91--189 GeV].
Experiment: JADE_OPAL
Collider: PETRA and LEP
SpiresID: 4300807
@@ -13,6 +13,9 @@
RunInfo:
$e^+ e^- \to$ jet jet (+ jets)
NumEvents: 1000000
+Energies: [35, 44, 91, 189]
+ToDo:
+ - Correct/complete list of valid energies in this metadata!
PtCuts: [0]
Description:
Differential and integrated jet rates for Durham and JADE jet
Modified: trunk/data/anainfo/OPAL_2004_S6132243.info
==============================================================================
--- trunk/data/anainfo/OPAL_2004_S6132243.info Tue Mar 9 15:26:46 2010 (r2321)
+++ trunk/data/anainfo/OPAL_2004_S6132243.info Tue Mar 9 17:14:32 2010 (r2322)
@@ -1,6 +1,6 @@
Name: OPAL_2004_S6132243
Year: 2004
-Summary: Event shape distributions and moments in e+ e- -> hadrons at 91-209 GeV
+Summary: Event shape distributions and moments in $e^+ e^-$ -> hadrons at 91--209 GeV
Experiment: OPAL
Collider: LEP 1 & 2
SpiresID: 6132243
Modified: trunk/data/anainfo/UA5_1982_S875503.info
==============================================================================
--- trunk/data/anainfo/UA5_1982_S875503.info Tue Mar 9 15:26:46 2010 (r2321)
+++ trunk/data/anainfo/UA5_1982_S875503.info Tue Mar 9 17:14:32 2010 (r2322)
@@ -1,11 +1,11 @@
Name: UA5_1982_S875503
SpiresID: 875503
-Summary: UA5 multiplicity and pseudorapidity distributions for pp and ppbar.
+Summary: UA5 multiplicity and pseudorapidity distributions for $pp$ and $p\bar{p}$.
Status: VALIDATED
Experiment: UA5
Collider: SPS
Year: 1982
-RunInfo: Min bias QCD events at sqrtS = 53~GeV. Run with both pp and ppbar beams.
+RunInfo: Min bias QCD events at sqrt(s) = 53~GeV. Run with both $pp$ and $p\bar{p}$ beams.
Energies: [53]
Authors:
- Andy Buckley <andy.buckley at cern.ch>
@@ -13,6 +13,6 @@
References:
- Phys.Lett.112B:183,1982
Description:
- Comparisons of multiplicity and pseudorapidity distributions for pp
- and ppbar collisions at 53 GeV, based on the UA5 53~GeV runs in 1982.
+ Comparisons of multiplicity and pseudorapidity distributions for $pp$ and
+ $p\bar{p}$ collisions at 53 GeV, based on the UA5 53~GeV runs in 1982.
Data confirms the lack of significant difference between the two beams.
Modified: trunk/data/anainfo/UA5_1986_S1583476.info
==============================================================================
--- trunk/data/anainfo/UA5_1986_S1583476.info Tue Mar 9 15:26:46 2010 (r2321)
+++ trunk/data/anainfo/UA5_1986_S1583476.info Tue Mar 9 17:14:32 2010 (r2322)
@@ -1,6 +1,6 @@
Name: UA5_1986_S1583476
Year: 1986
-Summary: Pseudorapidity distributions in ppbar (NSD, NSD+SD) events at c.m. energies of 200 and 900 GeV
+Summary: Pseudorapidity distributions in $p\bar{p}$ (NSD, NSD+SD) events at sqrt(s) = 200 and 900 GeV
Experiment: UA5
Collider: CERN SPS
SpiresID: 1583476
@@ -12,14 +12,15 @@
References:
- Eur. Phys. J. C33, 1, 1986
RunInfo:
- Elastic scattering, single and double diffractive events. ppbar collider, c.m energy 200 or 900 GeV.
- The trigger implementations for NSD events is the same as in, e.g., the UA5_1989 analysis. No
- further cuts are needed.
+ "* Single- and double-diffractive, plus non-diffractive inelastic, events.
+* $p\bar{p}$ collider, sqrt(s) = 200 or 900 GeV.
+* The trigger implementation for NSD events is the same as in, e.g., the UA5_1989
+analysis. No further cuts are needed.
NumEvents: 1000000
PtCuts: [0]
Description:
This study comprises measurements of pseudorapidity distributions measured with the UA5
detector at 200 and 900 GeV center of momentum energy. There are distributions for
- non-single diffractive (NSD) events and als for the combination of single- and double-diffractive
+ non-single diffractive (NSD) events and also for the combination of single- and double-diffractive
events. The NSD distributions are further studied for certain ranges of the events charged
multiplicity.
Modified: trunk/data/anainfo/UA5_1989_S1926373.info
==============================================================================
--- trunk/data/anainfo/UA5_1989_S1926373.info Tue Mar 9 15:26:46 2010 (r2321)
+++ trunk/data/anainfo/UA5_1989_S1926373.info Tue Mar 9 17:14:32 2010 (r2322)
@@ -19,20 +19,9 @@
NumEvents: 1000000
PtCuts: [0]
Description:
- Multiplicity distributions of charged particles produced in non
- single-diffractive collisions between protons and antiprotons at centre of
- mass energies of 200 and 900 GeV are presented. The data were recorded in the
- UA5 streamer chambers at the CERN Collider, which was operated in a pulsed
- mode between the two energies. A new method to correct for acceptance
- limitations and inefficiencies based on the principle of maximum entropy has
- been used. Multiplicity distributions in full phase space and in intervals of
- pseudorapidity are presented in tabular form. The violation of KNO scaling in
- full phase space found by the UA5 group at an energy of 546 GeV is confirmed
- also at 200 and 900 GeV. The shape of the 900 GeV distribution in full phase
- space is narrower in the peak region than at 200 GeV but exhibits a pronounced
- high multiplicity tail. The negative binomial distribution fits data at 200
- GeV in all pseudorapidity intervals and in small intervals at 900 GeV. In
- large intervals at 900 GeV, however, the negative binomial distribution. Fits
- to the partially coherent laser distribution are also presented as well as
- comparisons with predictions of the Dual Parton, the Fritiof and the Pythia
- models.
+ Multiplicity distributions of charged particles produced in non-single-diffractive
+ collisions between protons and antiprotons at centre-of-mass energies of 200 and
+ 900 GeV. The data were recorded in the UA5 streamer chambers at the CERN collider,
+ which was operated in a pulsed mode between the two energies. This analysis
+ confirms the violation of KNO scaling in full phase space found by the UA5 group
+ at an energy of 546 GeV, with similar measurements at 200 and 900 GeV.
Modified: trunk/doc/analyses.bib
==============================================================================
--- trunk/doc/analyses.bib Tue Mar 9 15:26:46 2010 (r2321)
+++ trunk/doc/analyses.bib Tue Mar 9 17:14:32 2010 (r2322)
@@ -1,17 +1,3 @@
-% Barate:1996fi
- at Article{Barate:1996fi,
- author = "Barate, R. and others",
- collaboration = "ALEPH",
- title = "{Studies of quantum chromodynamics with the ALEPH
- detector}",
- journal = "Phys. Rept.",
- volume = "294",
- year = "1998",
- pages = "1-165",
- doi = "10.1016/S0370-1573(97)00045-8",
- SLACcitation = "%%CITATION = PRPLC,294,1;%%"
-}
-
% Abe:1997eua
@Article{Abe:1997eua,
author = "Abe, F. and others",
@@ -112,23 +98,6 @@
SLACcitation = "%%CITATION = HEP-EX/0012013;%%"
}
-% Affolder:1999jh
- at Article{Affolder:1999jh,
- author = "Affolder, Anthony Allen and others",
- collaboration = "CDF",
- title = "{The transverse momentum and total cross section of $e^+e^-
- $ pairs in the $Z$ boson region from $p\bar{p}$ collisions
- at $\sqrt{s} = 1.8$ TeV}",
- journal = "Phys. Rev. Lett.",
- volume = "84",
- year = "2000",
- pages = "845-850",
- eprint = "hep-ex/0001021",
- archivePrefix = "arXiv",
- doi = "10.1103/PhysRevLett.84.845",
- SLACcitation = "%%CITATION = HEP-EX/0001021;%%"
-}
-
% Ackerstaff:1998hz
@Article{Ackerstaff:1998hz,
author = "Ackerstaff, K. and others",
@@ -320,22 +289,6 @@
SLACcitation = "%%CITATION = PHRVA,D41,2330;%%"
}
-% Acosta:2005ix
- at Article{Acosta:2005ix,
- author = "Acosta, Darin E. and others",
- collaboration = "CDF",
- title = "{Study of jet shapes in inclusive jet production in
- $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV}",
- journal = "Phys. Rev.",
- volume = "D71",
- year = "2005",
- pages = "112002",
- eprint = "hep-ex/0505013",
- archivePrefix = "arXiv",
- doi = "10.1103/PhysRevD.71.112002",
- SLACcitation = "%%CITATION = HEP-EX/0505013;%%"
-}
-
% Albajar:1989an
@Article{Albajar:1989an,
author = "Albajar, C. and others",
@@ -366,20 +319,6 @@
SLACcitation = "%%CITATION = NUCL-EX/0607033;%%"
}
-% Abt:1994ye
- at Article{Abt:1994ye,
- author = "Abt, I. and others",
- collaboration = "H1",
- title = "{Energy flow and charged particle spectrum in deep
- inelastic scattering at HERA}",
- journal = "Z. Phys.",
- volume = "C63",
- year = "1994",
- pages = "377-390",
- doi = "10.1007/BF01580319",
- SLACcitation = "%%CITATION = ZEPYA,C63,377;%%"
-}
-
% Abreu:1996na
@Article{Abreu:1996na,
author = "Abreu, P. and others",
@@ -461,6 +400,23 @@
SLACcitation = "%%CITATION = 0807.3367;%%"
}
+% Acosta:2004sn
+ at Article{Acosta:2004sn,
+ author = "Acosta, Darin E. and others",
+ collaboration = "CDF",
+ title = "{Measurement of the cross section for prompt diphoton
+ production in $p\bar{p}$ collisions at $\sqrt{s} = 1.96$
+ TeV}",
+ journal = "Phys. Rev. Lett.",
+ volume = "95",
+ year = "2005",
+ pages = "022003",
+ eprint = "hep-ex/0412050",
+ archivePrefix = "arXiv",
+ doi = "10.1103/PhysRevLett.95.022003",
+ SLACcitation = "%%CITATION = HEP-EX/0412050;%%"
+}
+
% Abazov:2010fr
@Article{Abazov:2010fr,
author = "Abazov, V. M. and others",
@@ -586,19 +542,18 @@
SLACcitation = "%%CITATION = HEP-EX/0702025;%%"
}
-% Abe:1988yu
- at Article{Abe:1988yu,
- author = "Abe, F. and others",
- collaboration = "CDF",
- title = "{Transverse momentum distributions of charged particles
- produced in $\bar{p}p$ interactions at $\sqrt{s} = 630$
- GeV and 1800 GeV}",
- journal = "Phys. Rev. Lett.",
- volume = "61",
- year = "1988",
- pages = "1819",
- doi = "10.1103/PhysRevLett.61.1819",
- SLACcitation = "%%CITATION = PRLTA,61,1819;%%"
+% Ansorge:1988kn
+ at Article{Ansorge:1988kn,
+ author = "Ansorge, R. E. and others",
+ collaboration = "UA5",
+ title = "{Charged Particle Multiplicity Distributions at 200-GeV and
+ 900-GeV Center-Of-Mass Energy}",
+ journal = "Z. Phys.",
+ volume = "C43",
+ year = "1989",
+ pages = "357",
+ doi = "10.1007/BF01506531",
+ SLACcitation = "%%CITATION = ZEPYA,C43,357;%%"
}
% :2007nt
@@ -619,18 +574,22 @@
SLACcitation = "%%CITATION = 0712.0803;%%"
}
-% Affolder:2001xt
- at Article{Affolder:2001xt,
- author = "Affolder, Anthony Allen and others",
- collaboration = "CDF",
- title = "{Charged jet evolution and the underlying event in
- $p\bar{p}$ collisions at 1.8 TeV}",
- journal = "Phys. Rev.",
- volume = "D65",
- year = "2002",
- pages = "092002",
- doi = "10.1103/PhysRevD.65.092002",
- SLACcitation = "%%CITATION = PHRVA,D65,092002;%%"
+% Abazov:2001nta
+ at Article{Abazov:2001nta,
+ author = "Abazov, V. M. and others",
+ collaboration = "D0",
+ title = "{Measurement of the ratio of differential cross sections
+ for $W$ and $Z$ boson production as a function of
+ transverse momentum in $p\bar{p}$ collisions at $\sqrt{s} =
+ 1.8$ TeV}",
+ journal = "Phys. Lett.",
+ volume = "B517",
+ year = "2001",
+ pages = "299-308",
+ eprint = "hep-ex/0107012",
+ archivePrefix = "arXiv",
+ doi = "10.1016/S0370-2693(01)01020-6",
+ SLACcitation = "%%CITATION = HEP-EX/0107012;%%"
}
% Abbiendi:2004qz
@@ -699,21 +658,32 @@
SLACcitation = "%%CITATION = HEP-EX/0409040;%%"
}
-% Acosta:2004sn
- at Article{Acosta:2004sn,
- author = "Acosta, Darin E. and others",
+% Alpgard:1982zx
+ at Article{Alpgard:1982zx,
+ author = "Alpgard, K. and others",
+ collaboration = "UA5",
+ title = "{COMPARISON OF p anti-p and p p INTERACTIONS AT s**(1/2) =
+ 53-GeV}",
+ journal = "Phys. Lett.",
+ volume = "B112",
+ year = "1982",
+ pages = "183",
+ doi = "10.1016/0370-2693(82)90325-2",
+ SLACcitation = "%%CITATION = PHLTA,B112,183;%%"
+}
+
+% Affolder:2001xt
+ at Article{Affolder:2001xt,
+ author = "Affolder, Anthony Allen and others",
collaboration = "CDF",
- title = "{Measurement of the cross section for prompt diphoton
- production in $p\bar{p}$ collisions at $\sqrt{s} = 1.96$
- TeV}",
- journal = "Phys. Rev. Lett.",
- volume = "95",
- year = "2005",
- pages = "022003",
- eprint = "hep-ex/0412050",
- archivePrefix = "arXiv",
- doi = "10.1103/PhysRevLett.95.022003",
- SLACcitation = "%%CITATION = HEP-EX/0412050;%%"
+ title = "{Charged jet evolution and the underlying event in
+ $p\bar{p}$ collisions at 1.8 TeV}",
+ journal = "Phys. Rev.",
+ volume = "D65",
+ year = "2002",
+ pages = "092002",
+ doi = "10.1103/PhysRevD.65.092002",
+ SLACcitation = "%%CITATION = PHRVA,D65,092002;%%"
}
% :2008hua
@@ -766,20 +736,16 @@
SLACcitation = "%%CITATION = HEP-EX/0608030;%%"
}
-% Abazov:2001nta
- at Article{Abazov:2001nta,
- author = "Abazov, V. M. and others",
- collaboration = "D0",
- title = "{Measurement of the ratio of differential cross sections
- for $W$ and $Z$ boson production as a function of
- transverse momentum in $p\bar{p}$ collisions at $\sqrt{s} =
- 1.8$ TeV}",
- journal = "Phys. Lett.",
- volume = "B517",
- year = "2001",
- pages = "299-308",
- eprint = "hep-ex/0107012",
- archivePrefix = "arXiv",
- doi = "10.1016/S0370-2693(01)01020-6",
- SLACcitation = "%%CITATION = HEP-EX/0107012;%%"
+% Abt:1994ye
+ at Article{Abt:1994ye,
+ author = "Abt, I. and others",
+ collaboration = "H1",
+ title = "{Energy flow and charged particle spectrum in deep
+ inelastic scattering at HERA}",
+ journal = "Z. Phys.",
+ volume = "C63",
+ year = "1994",
+ pages = "377-390",
+ doi = "10.1007/BF01580319",
+ SLACcitation = "%%CITATION = ZEPYA,C63,377;%%"
}
\ No newline at end of file
Modified: trunk/doc/analyses.tex
==============================================================================
--- trunk/doc/analyses.tex Tue Mar 9 15:26:46 2010 (r2321)
+++ trunk/doc/analyses.tex Tue Mar 9 17:14:32 2010 (r2322)
@@ -27,8 +27,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)
-\end{itemize}
+
+ \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}
\noindent 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 $20.85 \pm 0.24$, 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 production.
@@ -57,8 +57,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item $e^+e^-\to$ jets with $\pi$ and $\eta$ decays turned off.
-\end{itemize}
+
+ \item $e^+e^-\to$ jets with $\pi$ and $\eta$ decays turned off.\end{itemize}
\noindent Earlier measurements at LEP of isolated hard photons in hadronic Z decays, 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 statistical subtraction of non-prompt photons, the quark-to-photon fragmentation function, $D(z)$, is extracted directly from the measured 2-jet rate.
@@ -68,7 +68,7 @@
\clearpage
\typeout{Handling analysis ALEPH_1996_S3486095}
-\subsection[ALEPH\_1996\_S3486095]{ALEPH\_1996\_S3486095\,\cite{Barate:1996fi}}
+\subsection{ALEPH\_1996\_S3486095}
\textbf{Studies of QCD with the ALEPH detector.}\newline
\textbf{Experiment:} ALEPH (LEP 1) \newline
\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+3486095}{3486095}\newline
@@ -86,8 +86,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)
-\end{itemize}
+
+ \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}
\noindent Summary paper of QCD results as measured by ALEPH at LEP 1. The publication includes various event shape variables, multiplicities (identified particles and inclusive), and particle spectra.
@@ -115,8 +115,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)
-\end{itemize}
+
+ \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}
\noindent Measurement of the $\Xi^-$ and $\Sigma^+(1385)/\Sigma^-(1385)$ scaled momentum distributions by DELPHI at LEP 1. The paper also has the production cross-sections of these particles, but that's not implemented in Rivet.
@@ -146,8 +146,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item \ensuremath{\sqrt{s}} = 91.2 GeV, $e^+ e^- \ensuremath{\to} Z^0$ production with hadronic decays only
-\end{itemize}
+
+ \item \ensuremath{\sqrt{s}} = 91.2 GeV, $e^+ e^- \ensuremath{\to} Z^0$ production with hadronic decays only\end{itemize}
\noindent Event shape and charged particle inclusive distributions measured using 750000 decays of Z bosons to hadrons from the DELPHI detector at LEP. This data, combined with identified particle distributions from all LEP experiments, was used for tuning of shower-hadronisation event generators by the original PROFESSOR method. This is a critical analysis for MC event generator tuning of final state radiation and both flavour and kinematic aspects of hadronisation models.
@@ -174,8 +174,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)
-\end{itemize}
+
+ \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}
\noindent Measurement of the b-quark fragmentation function by DELPHI using 1994 LEP 1 data. The fragmentation function for both weakly decaying and primary b-quarks has been determined in a model independent way. Nevertheless the authors trust $f(x_B^\text{weak})$ more than $f(x_B^\text{prim})$.
@@ -186,7 +186,7 @@
\typeout{Handling analysis JADE_OPAL_2000_S4300807}
\subsection[JADE\_OPAL\_2000\_S4300807]{JADE\_OPAL\_2000\_S4300807\,\cite{Pfeifenschneider:1999rz}}
-\textbf{Jet rates in e+e- at JADE [35--44 GeV] and OPAL [91--189 GeV].}\newline
+\textbf{Jet rates in $e^+e^-$ at JADE [35--44 GeV] and OPAL [91--189 GeV].}\newline
\textbf{Experiment:} JADE_OPAL (PETRA and LEP) \newline
\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+4300807}{4300807}\newline
\textbf{Status:} VALIDATED\newline
@@ -204,8 +204,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item $e^+ e^- \to$ jet jet (+ jets)
-\end{itemize}
+
+ \item $e^+ e^- \to$ jet jet (+ jets)\end{itemize}
\noindent Differential and integrated jet rates for Durham and JADE jet algorithms.
@@ -234,8 +234,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)
-\end{itemize}
+
+ \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}
\noindent Measurement of scaled momentum distributions and total charged multiplicities in flavour tagged events at LEP 1. OPAL measured these observables in uds-, c-, and b-events separately. An inclusive measurement is also included.
@@ -246,7 +246,7 @@
\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
+\textbf{Event shape distributions and moments in $e^+ e^-$ \ensuremath{\to} hadrons at 91--209 GeV}\newline
\textbf{Experiment:} OPAL (LEP 1 \& 2) \newline
\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+6132243}{6132243}\newline
\textbf{Status:} VALIDATED\newline
@@ -264,8 +264,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item Hadronic e+ e- events at 4 representative energies (91, 133, 177, 197). Runs with \ensuremath{\sqrt{s}} above the Z mass need to have ISR suppressed, since the data has been corrected to remove radiative return to the Z.
-\end{itemize}
+
+ \item Hadronic e+ e- events at 4 representative energies (91, 133, 177, 197). Runs with \ensuremath{\sqrt{s}} above the Z mass need to have ISR suppressed, since the data has been corrected to remove radiative return to the Z.\end{itemize}
\noindent Measurement of e+ e- event shape variable distributions and their 1st to 5th moments in LEP running from the Z pole to the highest LEP 2 energy of 209 GeV.
@@ -273,7 +273,7 @@
\section{Tevatron analyses}\typeout{Handling analysis CDF_1988_S1865951}
-\subsection[CDF\_1988\_S1865951]{CDF\_1988\_S1865951\,\cite{Abe:1988yu}}
+\subsection{CDF\_1988\_S1865951}
\textbf{CDF transverse momentum distributions at 630 GeV and 1800 GeV.}\newline
\textbf{Experiment:} CDF (Tevatron Run I) \newline
\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+1865951}{1865951}\newline
@@ -293,8 +293,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item QCD min bias events at \ensuremath{\sqrt{s}} = 630 GeV and 1800 GeV, $|\eta| < 1.0$.
-\end{itemize}
+
+ \item QCD min bias events at \ensuremath{\sqrt{s}} = 630 GeV and 1800 GeV, $|\eta| < 1.0$.\end{itemize}
\noindent Transverse momentum distributions at 630 GeV and 1800 GeV based on data from the CDF experiment at the Tevatron collider.
@@ -323,8 +323,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item QCD min bias events at \ensuremath{\sqrt{s}} = 630 and 1800 GeV. Particles with $c \tau > 10$mm should be set stable.
-\end{itemize}
+
+ \item QCD min bias events at \ensuremath{\sqrt{s}} = 630 and 1800 GeV. Particles with $c \tau > 10$mm should be set stable.\end{itemize}
\noindent Pseudorapidity distributions based on the CDF 630 and 1800 GeV runs from 1987. All data is detector corrected. The data confirms the UA5 measurement of a $\d{N}/\d{\eta}$ rise with energy faster than $\ln{\sqrt{s}}$, and as such this analysis is important for constraining the energy evolution of minimum bias and underlying event characteristics in MC simulations.
@@ -353,8 +353,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item QCD events at Tevatron with $\sqrt{s}=1.8$ TeV without MPI.
-\end{itemize}
+
+ \item QCD events at Tevatron with $\sqrt{s}=1.8$ TeV without MPI.\end{itemize}
\noindent Measurement of the differential cross section $\mathrm{d}\sigma/\mathrm{d}E_\perp^j$ for the production of multijet events in $p\bar{p}$ collisions where the sum is over all jets with transverse energy $E_\perp^j > E_\perp^\mathrm{min}$.
@@ -364,7 +364,7 @@
\clearpage
\typeout{Handling analysis CDF_2000_S4155203}
-\subsection[CDF\_2000\_S4155203]{CDF\_2000\_S4155203\,\cite{Affolder:1999jh}}
+\subsection{CDF\_2000\_S4155203}
\textbf{Z \pT measurement in CDF Z \ensuremath{\to} $e^+e^-$ events}\newline
\textbf{Experiment:} CDF (Tevatron Run 1) \newline
\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+4155203}{4155203}\newline
@@ -384,11 +384,11 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item ppbar collisions at 1800 GeV. $Z/\gamma*$ Drell-Yan events with $e^+e^-$ decay mode only.
-\end{itemize}
+
+ \item $p\bar{p}$ collisions at 1800 GeV. $Z/\gamma^*$ Drell-Yan events with $e^+e^-$ decay mode only.\end{itemize}
\noindent Measurement of transverse momentum and total cross section of $e^+e^-$ pairs in the Z-boson region of $66~\text{GeV}/c^2 < m_{ee} < 116~\text{GeV}/c^2$ from pbar-p collisions at \ensuremath{\sqrt{s}} = 1.8 TeV, with the Tevatron CDF detector. The Z \pT, in a fully-factorised picture, is generated by the momentum balance against initial state radiation (ISR) and the primordial/intrinsic \pT of the Z's parent partons in the incoming hadrons. The Z \pT is important in generator tuning to fix the interplay of ISR and multi-parton interactions (MPI) ingenerating `underlying event' activity.
-This analysis is subject to ambiguities in the experimental Z \pT definition, since the Rivet implementation reconstructs the Z momentum from the dileptonpair with finite cones for photon brem summation, rather than YFS/shower unfolding or non-portable direct use of the Z in the event record.
+This analysis is subject to ambiguities in the experimental Z \pT definition, since the Rivet implementation reconstructs the Z momentum from the dilepton pair with finite cones for QED bremstrahlung summation, rather than non-portable direct use of the (sometimes absent) Z in the event record.
\clearpage
@@ -416,8 +416,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item Dijet events at Tevatron with $\sqrt{s}=1.8$ TeV
-\end{itemize}
+
+ \item Dijet events at Tevatron with $\sqrt{s}=1.8$ TeV\end{itemize}
\noindent Measurement of the cross section for production of two or more jets as a function of dijet mass in the range 180 to 1000 GeV. It is based on an integrated luminosity of $86 \mathrm{pb}^{-1}$.
@@ -447,8 +447,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item Dijet events at Tevatron with $\sqrt{s}=1.8$ TeV
-\end{itemize}
+
+ \item Dijet events at Tevatron with $\sqrt{s}=1.8$ TeV\end{itemize}
\noindent A measurement of the two-jet differential cross section, $\mathrm{d}^3\sigma/\mathrm{d}E_T \, \mathrm{d}\eta_1 \, \mathrm{d}\eta_2$, based on an integrated luminosity of $86 \mathrm{pb}^{-1}$. The differential cross section is measured as a function of the transverse energy, $E_\perp$, of a jet in the pseudorapidity region $0.1 < |\eta_1| < 0.7$ for four different pseudorapidity bins of a second jet restricted to $0.1 < |\eta_2| < 3.0$.
@@ -478,8 +478,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item Dijet events at Tevatron with $\sqrt{s}=1.8$ TeV
-\end{itemize}
+
+ \item Dijet events at Tevatron with $\sqrt{s}=1.8$ TeV\end{itemize}
\noindent Measurement of the inclusive jet cross section for jet transverse energies from 40 to 465 GeV in the pseudo-rapidity range $0.1<|\eta|<0.7$. The results are based on 87 $\mathrm{pb}^{-1}$ of data.
@@ -508,8 +508,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item ppbar QCD interactions at 1800 GeV. The leading jet is binned from 0--49 GeV, and histos can usually can be filled with a single generator run without kinematic sub-samples.
-\end{itemize}
+
+ \item ppbar QCD interactions at 1800 GeV. The leading jet is binned from 0--49 GeV, and histos can usually can be filled with a single generator run without kinematic sub-samples.\end{itemize}
\noindent The original CDF underlying event analysis, based on decomposing each event into a transverse structure with ``toward'', ``away'' and ``transverse'' regions defined relative to the azimuthal direction of the leading jet in the event. Since the toward region is by definition dominated by the hard process, as is the away region by momentum balance in the matrix element, the transverse region is most sensitive to multi-parton interactions. The transverse regions occupy $|\phi| \in [60\degree, 120\degree]$ for $|\eta| < 1$. The \pT ranges for the leading jet are divided experimentally into the `min-bias' sample from 0--20 GeV, and the `JET20' sample from 18--49 GeV.
@@ -538,8 +538,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item QCD events at \ensuremath{\sqrt{s}} = 630 and 1800 GeV.
-\end{itemize}
+
+ \item QCD events at \ensuremath{\sqrt{s}} = 630 and 1800 GeV.\end{itemize}
\noindent A study of ppbar collisions at \ensuremath{\sqrt{s}} = 1800 and 630 GeV collected 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 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.
@@ -568,8 +568,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item QCD events at \ensuremath{\sqrt{s}} = 630 \& 1800 GeV. Several \pTmin cutoffs are probably required to fill the profile histograms, e.g. 0 (min bias), 30, 90, 150 GeV at 1800 GeV, and 0 (min bias), 20, 90, 150 GeV at 630 GeV.
-\end{itemize}
+
+ \item QCD events at \ensuremath{\sqrt{s}} = 630 \& 1800 GeV. Several \pTmin cutoffs are probably required to fill the profile histograms, e.g. 0 (min bias), 30, 90, 150 GeV at 1800 GeV, and 0 (min bias), 20, 90, 150 GeV at 630 GeV.\end{itemize}
\noindent This analysis studies the underlying event via transverse cones of $R = 0.7$ at 90 degrees in \phi relative to the leading (highest E) jet, at \ensuremath{\sqrt{s}} = 630 and 1800 GeV. This is similar to the 2001 CDF UE analysis, except that cones, rather than the whole central \eta range are used. The transverse cones are categorised as TransMIN and TransMAX on an event-by-event basis, to give greater sensitivity to the UE component.
`Swiss Cheese' distributions, where cones around the leading $n$ jets are excluded from the distributions, are also included for $n = 2, 3$. This analysis is useful for constraining the energy evolution of the underlying event, since it performs the same analyses at two distinct CoM energies.
@@ -601,8 +601,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item $p \bar{p} \to \gamma \gamma$ [+ jets] at 1960 GeV. The analysis uses photons with \pT larger then 13 GeV. To allow for shifts in the shower, the ME cut on the transverse photon momentum shouldn't be too hard, e.g. 5 GeV.
-\end{itemize}
+
+ \item $p \bar{p} \to \gamma \gamma$ [+ jets] at 1960 GeV. The analysis uses photons with \pT larger then 13 GeV. To allow for shifts in the shower, the ME cut on the transverse photon momentum shouldn't be too hard, e.g. 5 GeV.\end{itemize}
\noindent Measurement of the cross section of prompt diphoton production in $p\bar{p}$ collisions at $\sqrt{s} = 1.96$ TeV using a data sample of 207~pb$^{-1}$ as a function of the diphoton mass, the transverse momentum of the diphoton system, and the azimuthal angle between the two photons.
@@ -612,7 +612,7 @@
\clearpage
\typeout{Handling analysis CDF_2005_S6217184}
-\subsection[CDF\_2005\_S6217184]{CDF\_2005\_S6217184\,\cite{Acosta:2005ix}}
+\subsection{CDF\_2005\_S6217184}
\textbf{CDF Run II jet shape analysis}\newline
\textbf{Experiment:} CDF (Tevatron Run 2) \newline
\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+6217184}{6217184}\newline
@@ -633,8 +633,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item QCD events at \ensuremath{\sqrt{s}} = 1960 GeV. Jet \pTmin in plots is 37 GeV/c --- choose generator min \pT somewhere well below this.
-\end{itemize}
+
+ \item QCD events at \ensuremath{\sqrt{s}} = 1960 GeV. Jet \pTmin in plots is 37 GeV/c --- choose generator min \pT somewhere well below this.\end{itemize}
\noindent Measurement of jet shapes in inclusive jet production in p pbar collisions at center-of-mass energy \ensuremath{\sqrt{s}} = 1.96 TeV. The data cover jet transverse momenta from 37--380 GeV and absolute jet rapidities in the range 0.1--0.7.
@@ -664,8 +664,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item ppbar \ensuremath{\to} jets at 1960 GeV
-\end{itemize}
+
+ \item ppbar \ensuremath{\to} jets at 1960 GeV\end{itemize}
\noindent Measurement of the inclusive jet cross section in ppbar interactions at $\sqrt{s}=1.96$ TeV using 385 $\mathrm{pb}^{-1}$ of data. The data cover the jet transverse momentum range from 61 to 620 GeV/c in $0.1 < |y| < 0.7$. This analysis has been updated with more data in more rapidity bins in CDF_2008_S7828950.
@@ -689,8 +689,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item ppbar QCD interactions at 1960 GeV. Particles with $c \tau > {}$10 mm should be set stable. Several $p_\perp^\text{min}$ cutoffs are probably required to fill the profile histograms. $p_\perp^\text{min} = {}$ 0 (min bias), 10, 20, 50, 100, 150 GeV. The corresponding merging points are at $p_T = $ 0, 30, 50, 80, 130, 180 GeV
-\end{itemize}
+
+ \item ppbar QCD interactions at 1960 GeV. Particles with $c \tau > {}$10 mm should be set stable. Several $p_\perp^\text{min}$ cutoffs are probably required to fill the profile histograms. $p_\perp^\text{min} = {}$ 0 (min bias), 10, 20, 50, 100, 150 GeV. The corresponding merging points are at $p_T = $ 0, 30, 50, 80, 130, 180 GeV\end{itemize}
\noindent Rick Field's measurement of the underlying event in leading jet events. If the leading jet of the event is within $|\eta| < 2$, the event is accepted and ``toward'', ``away'' and ``transverse'' regions are defined in the same way as in the original (2001) CDF underlying event analysis. The leading jet defines the $\phi$ direction of the toward region. The transverse regions are most sensitive to the underlying event.
@@ -718,8 +718,11 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item ppbar collisions at 1960 GeV. * Drell-Yan events with $Z/\gamma* \ensuremath{\to} e e$ and $Z/\gamma* \ensuremath{\to} \mu\mu$. * A mass cut $m_{ll} > 70~\text{GeV}$ can be applied on generator level. * Particles with $c \tau > 10~\text{mm}$ should be set stable.
-\end{itemize}
+
+ \item * ppbar collisions at 1960 GeV.
+ \item Drell-Yan events with $Z/\gamma* \ensuremath{\to} e e$ and $Z/\gamma* \ensuremath{\to} \mu\mu$.
+ \item A mass cut $m_{ll} > 70~\text{GeV}$ can be applied on generator level.
+ \item Particles with $c \tau > 10~\text{mm}$ should be set stable.\end{itemize}
\noindent Deepak Kar and Rick Field's measurement of the underlying event in Drell-Yan events. Z \ensuremath{\to} ee and Z \ensuremath{\to} $\mu\mu$ events are selected using a Z mass window cut between 70 and 110 GeV. ``Toward'', ``away'' and ``transverse'' regions are defined in the same way as in the original (2001) CDF underlying event analysis. The reconstructed Z defines the $\phi$ direction of the toward region. The leptons are ignored after the Z has been reconstructed. Thus the region most sensitive to the underlying event is the toward region (the recoil jet is boosted into the away region).
@@ -748,8 +751,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item $p \bar{p} \to e^+ e^-$ + jets at 1960 GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $66 < m_{ee} < 116$
-\end{itemize}
+
+ \item $p \bar{p} \to e^+ e^-$ + jets at 1960 GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $66 < m_{ee} < 116$\end{itemize}
\noindent Cross sections as a function of jet transverse momentum in 1 and 2 jet events, and jet multiplicity in ppbar collisions at \ensuremath{\sqrt{s}} = 1.96 TeV, based on an integrated luminosity of $1.7~\text{fb}^{-1}$. The measurements cover the rapidity region $|y_\text{jet}| < 2.1$ and the transverse momentum range $\pT^\text{jet} > 30~\text{GeV}/c$.
@@ -779,8 +782,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item Requires $2\rightarrow{2}$ QCD scattering processes. The minimum jet $E_\perp$ is 62 GeV, so a cut on kinematic \pTmin may be required for good statistics.
-\end{itemize}
+
+ \item Requires $2\rightarrow{2}$ QCD scattering processes. The minimum jet $E_\perp$ is 62 GeV, so a cut on kinematic \pTmin may be required for good statistics.\end{itemize}
\noindent Measurement of the inclusive jet cross section in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV as a function of jet $E_\perp$, for $E_\perp >$ 62 GeV. The data is collected by the CDF II detector and has an integrated luminosity of 1.13 fb$^{-1}$. The measurement was made using the cone-based Midpoint jet clustering algorithm in rapidity bins within $|y|<2.1$. This measurement can be used to provide increased precision in PDFs at high parton momentum fraction $x$.
@@ -808,8 +811,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item $p \bar{p} \to$ jets at 1960 GeV
-\end{itemize}
+
+ \item $p \bar{p} \to$ jets at 1960 GeV\end{itemize}
\noindent Dijet mass spectrum from 0.2 TeV to 1.4 TeV in $p \bar{p}$ collisions at $\sqrt{s} = 1.96$ TeV, based on an integrated luminosity of 1.13 fb$^{-1}$.
@@ -840,8 +843,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item ppbar QCD interactions at 1960 GeV. * Particles with $c \tau > {}$10 mm should be set stable.
-\end{itemize}
+
+ \item ppbar 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 average track \pT vs. charged multiplicity, a track \pT distribution and an inclusive $\sum E_T$ distribution.
@@ -869,8 +872,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item $p \bar{p} \to e^+ e^-$ + jets at 1960 GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $66 < m_{ee} < 116$ GeV
-\end{itemize}
+
+ \item $p \bar{p} \to e^+ e^-$ + jets at 1960 GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $66 < m_{ee} < 116$ GeV\end{itemize}
\noindent CDF measurement of the total cross section and rapidity distribution, $\mathrm{d}\sigma/\mathrm{d}y$, for $q\bar{q}\to \gamma^{*}/Z\to e^{+}e^{-}$ events in the $Z$ boson mass region ($66<M_{ee}<116$ GeV/c$^2$) produced in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV with 2.1 fb$^{-1}$ of integrated luminosity.
@@ -898,8 +901,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item $\gamma$ + jet processes in ppbar collisions at $\sqrt{s} = 1960$ GeV. Minimum \pT cut on the photon in the analysis is 30 GeV.
-\end{itemize}
+
+ \item $\gamma$ + jet processes in ppbar collisions at $\sqrt{s} = 1960$ GeV. Minimum \pT cut on the photon in the analysis is 30 GeV.\end{itemize}
\noindent A measurement of the cross section for the inclusive production of isolated photons. The measurement covers the pseudorapidity region $|\eta^\gamma|<1.0$ and the transverse energy range $E_T^\gamma>30$ GeV and is based on 2.5~fb$^{-1}$ of integrated luminosity. The cross section is measured differential in $E_\perp(\gamma)$.
@@ -929,8 +932,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item W/Z events with decays to first generation leptons, in ppbar collisions at \ensuremath{\sqrt{s}} = 1800 GeV
-\end{itemize}
+
+ \item W/Z events with decays to first generation leptons, in ppbar collisions at \ensuremath{\sqrt{s}} = 1800 GeV\end{itemize}
\noindent Measurement of differential W/Z boson cross section and ratio in p pbar collisions at center-of-mass energy \ensuremath{\sqrt{s}} = 1.8 TeV. The data cover electrons and neutrinos in a pseudo-rapidity range of -2.5 to 2.5.
@@ -959,8 +962,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item QCD events in ppbar interactions at \ensuremath{\sqrt{s}} = 1960 GeV.
-\end{itemize}
+
+ \item QCD events in ppbar interactions at \ensuremath{\sqrt{s}} = 1960 GeV.\end{itemize}
\noindent Correlations in the azimuthal angle between the two largest \pT jets have been measured using the D0 detector in ppbar collisions at 1960 GeV. The analysis is based on an inclusive dijet event sample in the central rapidity region. The correlations are determined for four different \pT intervals.
@@ -991,8 +994,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item ppbar collisions at \ensuremath{\sqrt{s}} = 1960 GeV. Requires gamma + jet (q,qbar,g) hard processes, which for Pythia 6 means MSEL=10 for with MSUB indices 14, 18, 29, 114, 115 enabled.
-\end{itemize}
+
+ \item ppbar collisions at \ensuremath{\sqrt{s}} = 1960 GeV. Requires gamma + jet (q,qbar,g) hard processes, which for Pythia 6 means MSEL=10 for with MSUB indices 14, 18, 29, 114, 115 enabled.\end{itemize}
\noindent Measurement of differential cross section for inclusive production of isolated photons in p pbar collisions at \ensuremath{\sqrt{s}} = 1.96 TeV with the D0 detector at the Fermilab Tevatron collider. The photons span transverse momenta 23--300 GeV and have pseudorapidity $|\eta| < 0.9$. Isolated direct photons are probes of pQCD via the annihilation (q qbar \ensuremath{\to} gamma g) and quark-gluon Compton scattering (q g \ensuremath{\to} gamma q) processes, the latter of which is also sensitive to the gluon PDF. The initial state radiation / resummation formalisms are sensitive to the resulting photon \pT spectrum
@@ -1023,8 +1026,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item Drell-Yan $p \bar{p} \to Z/\gamma^*$ + jets events at $\sqrt{s}$ = 1960 GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $71 < m_{ee} < 111$ GeV
-\end{itemize}
+
+ \item Drell-Yan $p \bar{p} \to Z/\gamma^*$ + jets events at $\sqrt{s}$ = 1960 GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $71 < m_{ee} < 111$ GeV\end{itemize}
\noindent Cross sections as a function of boson rapidity in $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96 TeV, based on an integrated luminosity of $0.4~\text{fb}^{-1}$.
@@ -1053,8 +1056,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item $p \bar{p} \to e^+ e^-$ + jets at 1960~GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $75 < m_{ee} < 105$ GeV.
-\end{itemize}
+
+ \item $p \bar{p} \to e^+ e^-$ + jets at 1960~GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $75 < m_{ee} < 105$ GeV.\end{itemize}
\noindent Cross sections as a function of \pT of the three leading jets and n-jet cross section ratios in ppbar collisions at $\sqrt{s}$ = 1.96 TeV, based on an integrated luminosity of $0.4~\text{fb}^{-1}$.
@@ -1083,8 +1086,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item $p \bar{p} \to e^+ e^-$ + jets at 1960~GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $40 < m_{ee} < 200$ GeV.
-\end{itemize}
+
+ \item $p \bar{p} \to e^+ e^-$ + jets at 1960~GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $40 < m_{ee} < 200$ GeV.\end{itemize}
\noindent Cross sections as a function of \pT of the vector boson inclusive and in forward region ($|y| > 2$, $\pT<30$ GeV) in $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96 TeV, based on an integrated luminosity of 0.98 fb$^{-1}$.
@@ -1115,8 +1118,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item QCD events at \ensuremath{\sqrt{s}} = 1960 GeV. A \pTmin cut is probably necessary since the lowest jet \pT bin is at 50 GeV
-\end{itemize}
+
+ \item QCD events at \ensuremath{\sqrt{s}} = 1960 GeV. A \pTmin cut is probably necessary since the lowest jet \pT bin is at 50 GeV\end{itemize}
\noindent Measurement of the inclusive jet cross section in p pbar collisions at center-of-mass energy \ensuremath{\sqrt{s}} = 1.96 TeV. The data cover jet transverse momenta from 50--600 GeV and jet rapidities in the range -2.4 to 2.4.
@@ -1147,8 +1150,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item Produce only gamma + jet (q,qbar,g) hard processes (for Pythia 6, this means MSEL=10 and MSUB indices 14, 29 \& 115 enabled). The lowest bin edge is at 30 GeV, so a kinematic \pTmin cut is probably required to fill the histograms.
-\end{itemize}
+
+ \item Produce only gamma + jet (q,qbar,g) hard processes (for Pythia 6, this means MSEL=10 and MSUB indices 14, 29 \& 115 enabled). The lowest bin edge is at 30 GeV, so a kinematic \pTmin cut is probably required to fill the histograms.\end{itemize}
\noindent The process p pbar \ensuremath{\to} photon + jet + X as studied by the D0 detector at the Fermilab Tevatron collider at center-of-mass energy \ensuremath{\sqrt{s}} = 1.96 TeV. Photons are reconstructed in the central rapidity region $|y_\gamma| < 1.0$ with transverse momenta in the range 30--400 GeV, while jets are reconstructed in either the central $|y_jet| < 0.8$ or forward $1.5 < |y_\text{jet}| < 2.5$ rapidity intervals with $\pT^\text{jet} > 15~\text{GeV}$. The differential cross section $\mathrm{d}^3 \sigma / \mathrm{d}{\pT^\gamma} \mathrm{d}{y_\gamma} \mathrm{d}{y_\text{jet}}$ is measured as a function of $\pT^\gamma$ in four regions, differing by the relative orientations of the photon and the jet. MC predictions have trouble with simultaneously describing the measured normalization and $\pT^\gamma$ dependence of the cross section in any of the four measured regions.
@@ -1179,8 +1182,10 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item Event type: W production with decay to e nu_e only * for Pythia 6: MSEL = 12, MDME(206,1) = 1 * Energy: 1.96 TeV
-\end{itemize}
+
+ \item * Event type: W production with decay to e nu_e only
+ \item for Pythia 6: MSEL = 12, MDME(206,1) = 1
+ \item Energy: 1.96 TeV\end{itemize}
\noindent 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 the incoming quarks which produce the W. Initial state radiation should also affect the \pT distribution.
@@ -1210,10 +1215,10 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item $p \bar{p} \to \mu^+ \mu^-$ + jets at 1960~GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $65 < m_{ee} < 115$ GeV.
-\end{itemize}
-\noindent Cross sections as a function of \pT and rapidity of the boson and \pT and rapidity of the leading jet in $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96 TeV, based on an integrated luminosity of 1.0 fb$^-1$.
+ \item $p \bar{p} \to \mu^+ \mu^-$ + jets at 1960~GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $65 < m_{ee} < 115$ GeV.\end{itemize}
+
+\noindent Cross sections as a function of \pT and rapidity of the boson and \pT and rapidity of the leading jet in $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96 TeV, based on an integrated luminosity of 1.0 fb$^{-1}$.
\clearpage
@@ -1239,8 +1244,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item $p \bar{p} \to e^+ e^-$ + jets at 1960~GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $65 < m_{ee} < 115$ GeV.
-\end{itemize}
+
+ \item $p \bar{p} \to e^+ e^-$ + jets at 1960~GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $65 < m_{ee} < 115$ GeV.\end{itemize}
\noindent Cross sections as a function of \pT of the three leading jets in $Z/\gamma^{*} (\to e^{+} e^{-})$ + jet + X production in $p \bar{p}$ collisions at $\sqrt{s} = 1.96$ TeV, based on an integrated luminosity of 1.0 fb$^{-1}$.
@@ -1268,8 +1273,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item $p \bar{p} \to$ jets at 1960 GeV
-\end{itemize}
+
+ \item $p \bar{p} \to$ jets at 1960 GeV\end{itemize}
\noindent Dijet angular distributions in different bins of dijet mass from 0.25 TeV to above 1.1 TeV in $p \bar{p}$ collisions at $\sqrt{s} = 1.96$ TeV, based on an integrated luminosity of 0.7 fb$^{-1}$.
@@ -1297,8 +1302,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item $p \bar{p} \to \mu^+ \mu^-$ + jets at 1960~GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $65 < m_{ee} < 115$ GeV.
-\end{itemize}
+
+ \item $p \bar{p} \to \mu^+ \mu^-$ + jets at 1960~GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $65 < m_{ee} < 115$ GeV.\end{itemize}
\noindent First measurements at a hadron collider of differential cross sections for $Z$+jet+X production in $\Delta\phi(Z, j)$, $|\Delta y(Z, j)|$ and $|y_\mathrm{boost}(Z, j)|$. Vector boson production in association with jets is an excellent probe of QCD and constitutes the main background to many small cross section processes, such as associated Higgs production. These measurements are crucial tests of the predictions of perturbative QCD and current event generators, which have varied success in describing the data. Using these measurements as inputs in tuning event generators will increase the experimental sensitivity to rare signals.
@@ -1326,14 +1331,137 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item $p \bar{p} \to$ jets at 1960 GeV. Analysis needs two hard jets above 40 GeV.
-\end{itemize}
+
+ \item $p \bar{p} \to$ jets at 1960 GeV. Analysis needs two hard jets above 40 GeV.\end{itemize}
\noindent The inclusive dijet production double differential cross section as a function of the dijet invariant mass and of the largest absolute rapidity ($|y|_\text{max}$) of the two jets with the largest transverse momentum in an event is measured using 0.7 fb$^{-1}$ of data. The measurement is performed in six rapidity regions up to $|y|_\text{max}=2.4$.
\clearpage
+\section{SPS analyses}\typeout{Handling analysis UA1_1990_S2044935}
+\subsection[UA1\_1990\_S2044935]{UA1\_1990\_S2044935\,\cite{Albajar:1989an}}
+\textbf{UA1 multiplicities, transverse momenta and transverse energy distributions.}\newline
+\textbf{Experiment:} UA1 (SPS) \newline
+\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+2044935}{2044935}\newline
+\textbf{Status:} VALIDATED\newline
+\textbf{Authors:}
+ \penalty 100
+\begin{itemize}
+ \item Andy Buckley $\langle\,$\href{mailto:andy.buckley at cern.ch}{andy.buckley at cern.ch}$\,\rangle$;
+ \item Christophe Vaillant $\langle\,$\href{mailto:c.l.j.j.vaillant at durham.ac.uk}{c.l.j.j.vaillant at durham.ac.uk}$\,\rangle$;
+\end{itemize}
+\textbf{References:}
+ \penalty 100
+\begin{itemize}
+ \item Nucl.Phys.B353:261,1990
+\end{itemize}
+\textbf{Run details:}
+ \penalty 100
+\begin{itemize}
+
+ \item QCD min bias events at sqrtS = 63, 200, 500 and 900 GeV.\end{itemize}
+
+\noindent Particle multiplicities, transverse momenta and transverse energy distributions at the UA1 experiment, at energies of 200, 500 and 900 GeV (with one plot at 63 GeV for comparison).
+
+\clearpage
+
+
+\clearpage
+
+\typeout{Handling analysis UA5_1982_S875503}
+\subsection[UA5\_1982\_S875503]{UA5\_1982\_S875503\,\cite{Alpgard:1982zx}}
+\textbf{UA5 multiplicity and pseudorapidity distributions for $pp$ and $p\bar{p}$.}\newline
+\textbf{Experiment:} UA5 (SPS) \newline
+\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+875503}{875503}\newline
+\textbf{Status:} VALIDATED\newline
+\textbf{Authors:}
+ \penalty 100
+\begin{itemize}
+ \item Andy Buckley $\langle\,$\href{mailto:andy.buckley at cern.ch}{andy.buckley at cern.ch}$\,\rangle$;
+ \item Christophe Vaillant $\langle\,$\href{mailto:c.l.j.j.vaillant at durham.ac.uk}{c.l.j.j.vaillant at durham.ac.uk}$\,\rangle$;
+\end{itemize}
+\textbf{References:}
+ \penalty 100
+\begin{itemize}
+ \item Phys.Lett.112B:183,1982
+\end{itemize}
+\textbf{Run details:}
+ \penalty 100
+\begin{itemize}
+
+ \item Min bias QCD events at \ensuremath{\sqrt{s}} = 53~GeV. Run with both $pp$ and $p\bar{p}$ beams.\end{itemize}
+
+\noindent Comparisons of multiplicity and pseudorapidity distributions for $pp$ and $p\bar{p}$ collisions at 53 GeV, based on the UA5 53~GeV runs in 1982. Data confirms the lack of significant difference between the two beams.
+
+\clearpage
+
+
+\clearpage
+
+\typeout{Handling analysis UA5_1986_S1583476}
+\subsection[UA5\_1986\_S1583476]{UA5\_1986\_S1583476\,\cite{Alner:1986xu}}
+\textbf{Pseudorapidity distributions in $p\bar{p}$ (NSD, NSD+SD) events at \ensuremath{\sqrt{s}} = 200 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+1583476}{1583476}\newline
+\textbf{Status:} VALIDATED\newline
+\textbf{Authors:}
+ \penalty 100
+\begin{itemize}
+ \item Andy Buckley $\langle\,$\href{mailto:andy.buckley at cern.ch}{andy.buckley at cern.ch}$\,\rangle$;
+ \item Holger Schulz $\langle\,$\href{mailto:holger.schulz at physik.hu-berlin.de}{holger.schulz at physik.hu-berlin.de}$\,\rangle$;
+ \item Christophe Vaillant $\langle\,$\href{mailto:c.l.j.j.vaillant at durham.ac.uk}{c.l.j.j.vaillant at durham.ac.uk}$\,\rangle$;
+\end{itemize}
+\textbf{References:}
+ \penalty 100
+\begin{itemize}
+ \item Eur. Phys. J. C33, 1, 1986
+\end{itemize}
+\textbf{Run details:}
+ \penalty 100
+\begin{itemize}
+
+ \item * Single- and double-diffractive, plus non-diffractive inelastic, events.
+ \item $par{p}$ collider, \ensuremath{\sqrt{s}} = 200 or 900 GeV.
+ \item The trigger implementation for NSD events is the same as in, e.g., the UA5_1989 analysis. No further cuts are needed. NumEvents: 1000000 PtCuts: [0] Description: This study comprises measurements of pseudorapidity distributions measured with the UA5 detector at 200 and 900 GeV center of momentum energy. There are distributions for non-single diffractive (NSD) events and also for the combination of single- and double-diffractive events. The NSD distributions are further studied for certain ranges of the events charged multiplicity. \end{itemize}
+
+\noindent
+
+\clearpage
+
+
+\clearpage
+
+\typeout{Handling analysis UA5_1989_S1926373}
+\subsection[UA5\_1989\_S1926373]{UA5\_1989\_S1926373\,\cite{Ansorge:1988kn}}
+\textbf{UA5 charged multiplicity measurements}\newline
+\textbf{Experiment:} UA5 (CERN SPS) \newline
+\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+1926373}{1926373}\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}$\,\rangle$;
+ \item Christophe L. J. Vaillant $\langle\,$\href{mailto:c.l.j.j.vaillant at durham.ac.uk}{c.l.j.j.vaillant at durham.ac.uk}$\,\rangle$;
+ \item Andy Buckley $\langle\,$\href{mailto:andy.buckley at cern.ch}{andy.buckley at cern.ch}$\,\rangle$;
+\end{itemize}
+\textbf{References:}
+ \penalty 100
+\begin{itemize}
+ \item Z. Phys. C - Particles and Fields 43, 357-374 (1989)
+ \item DOI: \href{http://dx.doi.org/10.1007/BF01506531}{10.1007/BF01506531}
+\end{itemize}
+\textbf{Run details:}
+ \penalty 100
+\begin{itemize}
+
+ \item MinBias events at \ensuremath{\sqrt{s}} = 200 and 900 GeV. Enable single and double diffractive events in addition to minimum bias and non-diffractive processes.\end{itemize}
+
+\noindent Multiplicity distributions of charged particles produced in non-single-diffractive collisions between protons and antiprotons at centre-of-mass energies of 200 and 900 GeV. The data were recorded in the UA5 streamer chambers at the CERN collider, which was operated in a pulsed mode between the two energies. This analysis confirms the violation of KNO scaling in full phase space found by the UA5 group at an energy of 546 GeV, with similar measurements at 200 and 900 GeV.
+
+\clearpage
+
+
\section{HERA analyses}\typeout{Handling analysis H1_1994_S2919893}
\subsection[H1\_1994\_S2919893]{H1\_1994\_S2919893\,\cite{Abt:1994ye}}
\textbf{H1 energy flow and charged particle spectra in DIS}\newline
@@ -1354,8 +1482,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item $e^- p$ / $e^+ p$ deep inelastic scattering, 820~GeV protons colliding with 26.7~GeV electrons
-\end{itemize}
+
+ \item $e^- p$ / $e^+ p$ deep inelastic scattering, 820~GeV protons colliding with 26.7~GeV electrons\end{itemize}
\noindent Global properties of the hadronic final state in deep inelastic scattering events at HERA are investigated. The data are corrected for detector effects. Energy flows in both the laboratory frame and the hadronic centre of mass system, and energy-energy correlations in the laboratory frame are presented. Historically, the Ariadne colour dipole model provided the only satisfactory description of this data, hence making it a useful 'target' analysis for MC shower models.
@@ -1385,8 +1513,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item $e^+ p$ deep inelastic scattering with $p$ at 820 GeV, $e^+$ at 27.5 GeV \ensuremath{\to} \ensuremath{\sqrt{s}} = 300 GeV
-\end{itemize}
+
+ \item $e^+ p$ deep inelastic scattering with $p$ at 820 GeV, $e^+$ at 27.5 GeV \ensuremath{\to} \ensuremath{\sqrt{s}} = 300 GeV\end{itemize}
\noindent Measurements of transverse energy flow for neutral current deep- inelastic scattering events produced in positron-proton collisions at HERA. The kinematic range covers squared momentum transfers $Q^2$ from 3.2 to 2200 GeV$^2$; the Bjorken scaling variable $x$ from $8 \times 10^{-5}$ to 0.11 and the hadronic mass $W$ from 66 to 233 GeV. The transverse energy flow is measured in the hadronic centre of mass frame and is studied as a function of $Q^2$, $x$, $W$ and pseudorapidity. The behaviour of the mean transverse energy in the central pseudorapidity region and an interval corresponding to the photon fragmentation region are analysed as a function of $Q^2$ and $W$. This analysis is useful for exploring the effect of photon PDFs and for tuning models of parton evolution and treatment of fragmentation and the proton remnant in DIS.
@@ -1414,8 +1542,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item pp at 200 GeV
-\end{itemize}
+
+ \item pp at 200 GeV\end{itemize}
\noindent \pT distributions of charged pions and (anti)protons in pp collisions at $\sqrt{s} = 200$ GeV, measured by the STAR experiment at RHIC in non-single-diffractive minbias events.
@@ -1444,8 +1572,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item pp at 200 GeV
-\end{itemize}
+
+ \item pp at 200 GeV\end{itemize}
\noindent \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 $\langle \pT \rangle$ vs. particle mass plot is not validated yet and might be wrong.
@@ -1474,8 +1602,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item pp at 200 GeV
-\end{itemize}
+
+ \item pp at 200 GeV\end{itemize}
\noindent Inclusive jet cross section as a function of \pT in pp collisions at $\sqrt{s} = 200$ GeV, measured by the STAR experiment at RHIC.
@@ -1495,8 +1623,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item LHC pp \ensuremath{\to} jet+jet, photon+jet, photon+photon, all with EW+QCD shower
-\end{itemize}
+
+ \item LHC pp \ensuremath{\to} jet+jet, photon+jet, photon+photon, all with EW+QCD shower\end{itemize}
\noindent Different observables related to the two photons
@@ -1505,6 +1633,29 @@
\clearpage
+\typeout{Handling analysis MC_JETS}
+\subsection{MC\_JETS}
+\textbf{Monte Carlo validation observables for jet production}\newline
+\textbf{Status:} VALIDATED\newline
+\textbf{Authors:}
+ \penalty 100
+\begin{itemize}
+ \item Frank Siegert $\langle\,$\href{mailto:frank.siegert at durham.ac.uk}{frank.siegert at durham.ac.uk}$\,\rangle$;
+\end{itemize}
+\textbf{No references listed}\\
+\textbf{Run details:}
+ \penalty 100
+\begin{itemize}
+
+ \item Pure QCD jet production events at an arbitrary collider.\end{itemize}
+
+\noindent Jets with $p_\perp>20$ GeV are constructed with a $k_\perp$ jet finder with $D=0.7$ and projected onto many different observables.
+
+\clearpage
+
+
+\clearpage
+
\typeout{Handling analysis MC_LEADINGJETS}
\subsection{MC\_LEADINGJETS}
\textbf{Underlying event in leading jet events, extended to LHC}\newline
@@ -1518,8 +1669,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item LHC pp QCD interactions at 0.9, 10 or 14 TeV. Particles with $c \tau > 10$ mm should be set stable. Several $p_\perp^\text{min}$ cutoffs are probably required to fill the profile histograms.
-\end{itemize}
+
+ \item LHC pp QCD interactions at 0.9, 10 or 14 TeV. Particles with $c \tau > 10$ mm should be set stable. Several $p_\perp^\text{min}$ cutoffs are probably required to fill the profile histograms.\end{itemize}
\noindent Rick Field's measurement of the underlying event in leading jet events, extended to the LHC. As usual, the leading jet of the defines an azimuthal toward/transverse/away decomposition, in this case the event is accepted within $|\eta| < 2$, as in the CDF 2008 version of the analysis. Since this isn't the Tevatron, I've chosen to use $k_\perp$ rather than midpoint jets.
@@ -1541,8 +1692,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item Tevatron Run II ppbar \ensuremath{\to} gamma + jets.
-\end{itemize}
+
+ \item Tevatron Run II ppbar \ensuremath{\to} gamma + jets.\end{itemize}
\noindent Different observables related to the photon and extra jets.
@@ -1564,8 +1715,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item SUSY events at any energy. \pT cutoff at 10 GeV may be advised.
-\end{itemize}
+
+ \item SUSY events at any energy. \pT cutoff at 10 GeV may be advised.\end{itemize}
\noindent Analysis of generic SUSY events at the LHC, based on Atlas Herwig++ validation analysis contents. Plotted are eta, phi and \pT observables for charged tracks, photons, isolated photons, electrons, muons, and jets, as well as various dilepton mass `edge' plots for different event selection criteria.
@@ -1587,8 +1738,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item $e \, \nu$ + jets analysis.
-\end{itemize}
+
+ \item $e \, \nu$ + jets analysis.\end{itemize}
\noindent Available observables are W mass, \pT of jets 1-4, jet multiplicity, $\Delta\eta(W, \text{jet1})$, $\Delta R(\text{jet2}, \text{jet3})$, differential jet rates 0\ensuremath{\to}1, 1\ensuremath{\to}2, 2\ensuremath{\to}3, 3\ensuremath{\to}4, integrated 0--4 jet rates.
@@ -1610,8 +1761,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item $e^+ e^-$ + jets analysis. Needs mass cut on lepton pair to avoid photon singularity, e.g. a min range of $66 < m_{ee} < 116$ GeV
-\end{itemize}
+
+ \item $e^+ e^-$ + jets analysis. Needs mass cut on lepton pair to avoid photon singularity, e.g. a min range of $66 < m_{ee} < 116$ GeV\end{itemize}
\noindent Available observables are Z mass, \pT of jets 1-4, jet multiplicity, $\Delta\eta(Z, \text{jet1})$, $\Delta R(\text{jet2}, \text{jet3})$, differential jet rates 0\ensuremath{\to}1, 1\ensuremath{\to}2, 2\ensuremath{\to}3, 3\ensuremath{\to}4, integrated 0--4 jet rates.
@@ -1631,8 +1782,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item All event types will be accepted.
-\end{itemize}
+
+ \item All event types will be accepted.\end{itemize}
\noindent This analysis is a demonstration of the Rivet analysis structure and functionality: booking histograms; the initialisation, analysis and finalisation phases; and a simple loop over event particles. It has no physical meaning, but can be used as a simple pedagogical template for writing real analyses.
@@ -1658,8 +1809,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item $e^+ e^-$ analysis on the $\Upsilon(4S)$ resonance, with CoM boost -- 8.0~GeV~($e^−$) and 3.5~GeV~($e^+$)
-\end{itemize}
+
+ \item $e^+ e^-$ analysis on the $\Upsilon(4S)$ resonance, with CoM boost -- 8.0~GeV~($e^−$) and 3.5~GeV~($e^+$)\end{itemize}
\noindent Analysis of charm quark fragmentation at 10.6 GeV, based on a data sample of 103 fb collected by the Belle detector at the KEKB accelerator. Fragmentation into charm is studied for the main charmed hadron ground states, namely $D^0$, $D^+$, $D^+_s$ and $\Lambda_c^+$, as well as the excited states $D^{*0}$ and $D^{*+}$. This analysis can be used to constrain charm fragmentation in Monte Carlo generators. Additionally, we determine the average number of these charmed hadrons produced per B decay at the $\Upsilon(4S)$ resonance and measure the distribution of their production angle in $e^+ e^-$ annihilation events and in B decays.
@@ -1687,8 +1838,8 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item Hadronic events in $e+e-$ collisions
-\end{itemize}
+
+ \item Hadronic events in $e+e-$ collisions\end{itemize}
\noindent 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. The numbers are averages from various experiments. Correlations of the systematic uncertainties were considered for the calculation of the averages.
@@ -1716,133 +1867,10 @@
\textbf{Run details:}
\penalty 100
\begin{itemize}
- \item Hadronic events in $e^+ e^-$ collisions
-\end{itemize}
-
-\noindent 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 from various experiments. Correlations of the systematic uncertainties were considered for the calculation of the averages.
-
-\clearpage
-
-
-\clearpage
-
-\typeout{Handling analysis UA1_1990_S2044935}
-\subsection[UA1\_1990\_S2044935]{UA1\_1990\_S2044935\,\cite{Albajar:1989an}}
-\textbf{UA1 multiplicities, transverse momenta and transverse energy distributions.}\newline
-\textbf{Experiment:} UA1 (SPS) \newline
-\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+2044935}{2044935}\newline
-\textbf{Status:} VALIDATED\newline
-\textbf{Authors:}
- \penalty 100
-\begin{itemize}
- \item Andy Buckley $\langle\,$\href{mailto:andy.buckley at cern.ch}{andy.buckley at cern.ch}$\,\rangle$;
- \item Christophe Vaillant $\langle\,$\href{mailto:c.l.j.j.vaillant at durham.ac.uk}{c.l.j.j.vaillant at durham.ac.uk}$\,\rangle$;
-\end{itemize}
-\textbf{References:}
- \penalty 100
-\begin{itemize}
- \item Nucl.Phys.B353:261,1990
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
- \item QCD min bias events at sqrtS = 63, 200, 500 and 900 GeV.
-\end{itemize}
-
-\noindent Particle multiplicities, transverse momenta and transverse energy distributions at the UA1 experiment, at energies of 200, 500 and 900 GeV (with one plot at 63 GeV for comparison).
-
-\clearpage
+ \item Hadronic events in $e^+ e^-$ collisions\end{itemize}
-\clearpage
-
-\typeout{Handling analysis UA5_1982_S875503}
-\subsection{UA5\_1982\_S875503}
-\textbf{UA5 multiplicity and pseudorapidity distributions for pp and ppbar.}\newline
-\textbf{Experiment:} UA5 (SPS) \newline
-\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+875503}{875503}\newline
-\textbf{Status:} VALIDATED\newline
-\textbf{Authors:}
- \penalty 100
-\begin{itemize}
- \item Andy Buckley $\langle\,$\href{mailto:andy.buckley at cern.ch}{andy.buckley at cern.ch}$\,\rangle$;
- \item Christophe Vaillant $\langle\,$\href{mailto:c.l.j.j.vaillant at durham.ac.uk}{c.l.j.j.vaillant at durham.ac.uk}$\,\rangle$;
-\end{itemize}
-\textbf{References:}
- \penalty 100
-\begin{itemize}
- \item Phys.Lett.112B:183,1982
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
- \item Min bias QCD events at sqrtS = 53~GeV. Run with both pp and ppbar beams.
-\end{itemize}
-
-\noindent Comparisons of multiplicity and pseudorapidity distributions for pp and ppbar collisions at 53 GeV, based on the UA5 53~GeV runs in 1982. Data confirms the lack of significant difference between the two beams.
-
-\clearpage
-
-
-\clearpage
-
-\typeout{Handling analysis UA5_1986_S1583476}
-\subsection[UA5\_1986\_S1583476]{UA5\_1986\_S1583476\,\cite{Alner:1986xu}}
-\textbf{Pseudorapidity distributions in ppbar (NSD, NSD+SD) events at c.m. energies of 200 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+1583476}{1583476}\newline
-\textbf{Status:} VALIDATED\newline
-\textbf{Authors:}
- \penalty 100
-\begin{itemize}
- \item Andy Buckley $\langle\,$\href{mailto:andy.buckley at cern.ch}{andy.buckley at cern.ch}$\,\rangle$;
- \item Holger Schulz $\langle\,$\href{mailto:holger.schulz at physik.hu-berlin.de}{holger.schulz at physik.hu-berlin.de}$\,\rangle$;
- \item Christophe Vaillant $\langle\,$\href{mailto:c.l.j.j.vaillant at durham.ac.uk}{c.l.j.j.vaillant at durham.ac.uk}$\,\rangle$;
-\end{itemize}
-\textbf{References:}
- \penalty 100
-\begin{itemize}
- \item Eur. Phys. J. C33, 1, 1986
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
- \item Elastic scattering, single and double diffractive events. ppbar collider, c.m energy 200 or 900 GeV. The trigger implementations for NSD events is the same as in, e.g., the UA5_1989 analysis. No further cuts are needed.
-\end{itemize}
-
-\noindent This study comprises measurements of pseudorapidity distributions measured with the UA5 detector at 200 and 900 GeV center of momentum energy. There are distributions for non-single diffractive (NSD) events and als for the combination of single- and double-diffractive events. The NSD distributions are further studied for certain ranges of the events charged multiplicity.
-
-\clearpage
-
-
-\clearpage
-
-\typeout{Handling analysis UA5_1989_S1926373}
-\subsection{UA5\_1989\_S1926373}
-\textbf{UA5 charged multiplicity measurements}\newline
-\textbf{Experiment:} UA5 (CERN SPS) \newline
-\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+1926373}{1926373}\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}$\,\rangle$;
- \item Christophe L. J. Vaillant $\langle\,$\href{mailto:c.l.j.j.vaillant at durham.ac.uk}{c.l.j.j.vaillant at durham.ac.uk}$\,\rangle$;
- \item Andy Buckley $\langle\,$\href{mailto:andy.buckley at cern.ch}{andy.buckley at cern.ch}$\,\rangle$;
-\end{itemize}
-\textbf{References:}
- \penalty 100
-\begin{itemize}
- \item Z. Phys. C - Particles and Fields 43, 357-374 (1989)
- \item DOI: \href{http://dx.doi.org/10.1007/BF01506531}{10.1007/BF01506531}
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
- \item MinBias events at \ensuremath{\sqrt{s}} = 200 and 900 GeV. Enable single and double diffractive events in addition to minimum bias and non-diffractive processes.
-\end{itemize}
-
-\noindent Multiplicity distributions of charged particles produced in non single-diffractive collisions between protons and antiprotons at centre of mass energies of 200 and 900 GeV are presented. The data were recorded in the UA5 streamer chambers at the CERN Collider, which was operated in a pulsed mode between the two energies. A new method to correct for acceptance limitations and inefficiencies based on the principle of maximum entropy has been used. Multiplicity distributions in full phase space and in intervals of pseudorapidity are presented in tabular form. The violation of KNO scaling in full phase space found by the UA5 group at an energy of 546 GeV is confirmed also at 200 and 900 GeV. The shape of the 900 GeV distribution in full phase space is narrower in the peak region than at 200 GeV but exhibits a pronounced high multiplicity tail. The negative binomial distribution fits data at 200 GeV in all pseudorapidity intervals and in small intervals at 900 GeV. In l
arge intervals at 900 GeV, however, the negative binomial distribution. Fits to the partially coherent laser distribution are also presented as well as comparisons with predictions of the Dual Parton, the Fritiof and the Pythia models.
+\noindent 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 from various experiments. Correlations of the systematic uncertainties were considered for the calculation of the averages.
\clearpage
Modified: trunk/doc/mk-analysis-latex
==============================================================================
--- trunk/doc/mk-analysis-latex Tue Mar 9 15:26:46 2010 (r2321)
+++ trunk/doc/mk-analysis-latex Tue Mar 9 17:14:32 2010 (r2322)
@@ -67,13 +67,14 @@
return t
## For BibTeX
-## TODO: use spiresbib.py as an executable to dump to a pickle-based SpiresID -> (BibKey,BibTeX) file to avoid HTTP delays in doc build
+## TODO: use spiresbib.py as an executable to dump to a pickle- or shelve-based
+## SpiresID -> (BibKey,BibTeX) file to avoid HTTP delays in doc build
import spiresbib
bib = {}
## Build analysis pages
all_analyses = rivet.AnalysisLoader.analysisNames()
-pages = { "LEP":[], "Tevatron":[], "HERA":[], "RHIC":[], "Monte Carlo":[], "Example":[], "Misc.":[] }
+pages = { "LEP":[], "Tevatron":[], "SPS":[], "HERA":[], "RHIC":[], "Monte Carlo":[], "Example":[], "Misc.":[] }
## Use list(...) ctor for 2.3 compatibility
for aname in sorted(list(all_analyses)):
print "Handling analysis '%s'" % aname
@@ -136,13 +137,11 @@
if ana.runInfo():
page += "\\textbf{Run details:}\n \\penalty 100\n"
+ infos = ana.runInfo().split(" * ")
+ print ana.runInfo(), "->", infos
page += "\\begin{itemize}\n"
- #print ana.runInfo()
- for l in ana.runInfo().split("\n*"):
- l = l.strip()
- if l.startswith("*"):
- l = l[1:].strip()
- page += " \\item %s\n" % l
+ for i in infos:
+ page += "\n \\item %s" % i
page += "\\end{itemize}\n"
else:
page += "\\textbf{No run details listed}\\\\ \n"
@@ -177,6 +176,8 @@
pages["LEP"].append(page)
elif "Tevatron" in ana.collider():
pages["Tevatron"].append(page)
+ elif "SPS" in ana.collider():
+ pages["SPS"].append(page)
elif "HERA" in ana.collider():
pages["HERA"].append(page)
elif "RHIC" in ana.collider():
@@ -212,6 +213,7 @@
body = \
groups["LEP"] + "\n\n" + \
groups["Tevatron"] + "\n\n" + \
+ groups["SPS"] + "\n\n" + \
groups["HERA"] + "\n\n" + \
groups["RHIC"] + "\n\n" + \
groups["Monte Carlo"] + "\n\n" + \
Modified: trunk/doc/rivet-manual.tex
==============================================================================
--- trunk/doc/rivet-manual.tex Tue Mar 9 15:26:46 2010 (r2321)
+++ trunk/doc/rivet-manual.tex Tue Mar 9 17:14:32 2010 (r2322)
@@ -332,8 +332,9 @@
analysis on the events in the \kbd{fifo.hepmc} data file. This analysis is the
one originally used for the \Delphi automated ``\textsc{Professor}''
generator tuning. If the first event in the data file does not have
- appropriate beams, the analysis will be disabled; since there is only one
- analysis in this case, the command will exit immediately with a warning.}
+ appropriate beam particles, the analysis will be disabled; since there is only one
+ analysis in this case, the command will exit immediately with a warning if the
+ first event is not an $\Ppositron\Pelectron$ event.}
\item \paragraph{Using all analyses:}{\kbd{rivet -n~50000 -A -} will read up to
50k events from standard input (specified by the special ``-'' input filename)
@@ -381,15 +382,15 @@
histograms in ROOT\cite{Antcheva:2009zz}. Don't worry: a few months of therapy
can work wonders. For unrepentant ROOT junkies, Rivet installs an
\kbd{aida2root} script, which converts the AIDA records to a \kbd{.root} file
-full of ROOT \kbd{TGraph}s. One word of warning: a bug in ROOT means that
-\kbd{TGraph}s do not render properly from file because the axis is not drawn by
+full of ROOT \texttt{TGraph}s. One word of warning: a bug in ROOT means that
+\texttt{TGraph}s do not render properly from file because the axis is not drawn by
default. To display the plots correctly in ROOT you will need to pass the
\kbd{"AP"} drawing option string to either the \kbd{TGraph::Draw()} method, or
in the options box in the \kbd{TBrowser} GUI interface.
\paragraph{Conversion to ``flat format''}
-Most of our histogramming is based around the YODA ``flat'' plain text format,
+Most of our histogramming is based around a ``flat'' plain text format,
which can easily be read (and written) by hand. We provide a script called
\kbd{aida2flat} to do this conversion. Run \kbd{aida2flat -h} to get usage
instructions; in particular the Gnuplot and ``split output'' options are useful
@@ -423,7 +424,7 @@
\kbd{\chophisto -b /CDF\_2001\_S4751469/d03-x01-y01:5:13 Rivet.aida}\\
%
will chop all bins with $x<5$ and $x>13$ from the histogram
-\kbd{/CDF\_2001\_S4751469/d03-x01-y01:5:13} in the file \kbd{Rivet.aida}. (In
+\kbd{/CDF\_2001\_S4751469/d03-x01-y01} in the file \kbd{Rivet.aida}. (In
this particular case, $x$ would be a leading jet \pT.)
\subsection{Normalising histograms}
Modified: trunk/doc/spiresbib.py
==============================================================================
--- trunk/doc/spiresbib.py Tue Mar 9 15:26:46 2010 (r2321)
+++ trunk/doc/spiresbib.py Tue Mar 9 17:14:32 2010 (r2322)
@@ -45,6 +45,14 @@
return key, bibtex
+def get_bibtexs_from_spires(spiresids):
+ bibdb = {}
+ for spiresid in spiresids:
+ key, bibtex = get_bibtex_from_spires(spiresid)
+ if key and bibtex:
+ bibdb[spiresid] = (key, bibtex)
+ return bibdb
+
if __name__ == '__main__':
## Parse command line options
@@ -52,7 +60,13 @@
parser = OptionParser(usage=usage)
opts, args = parser.parse_args()
- for spiresid in args:
- key, bibtex = get_bibtex_from_spires(spiresid)
- if bibtex:
- print key, "=>\n", bibtex
+ ## Build ref db
+ bibdb = get_bibtexs_from_spires(args)
+ for sid, (key, bibtex) in bibdb.iteritems():
+ print key, "=>\n", bibtex
+
+ ## Pickle ref db
+ import cPickle as pickle
+ fpkl = open("spiresbib.pkl", "w")
+ pickle.dump(bibdb)
+ fpkl.close()
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