[Rivet-svn] rivet: 3 new changesets

[Rivet Mercurial]

details:   https://rivet.hepforge.org/hg/rivet/rev/d5d3b4958557
branches:  release-2-5-x
changeset: 5523:d5d3b4958557
user:      Andy Buckley <andy at insectnation.org>
date:      Tue Sep 27 16:56:38 2016 +0100
description:
Add Shehu as author

details:   https://rivet.hepforge.org/hg/rivet/rev/decac6333e62
branches:  release-2-5-x
changeset: 5524:decac6333e62
user:      Andy Buckley <andy at insectnation.org>
date:      Tue Sep 27 17:19:39 2016 +0100
description:
Typos

details:   https://rivet.hepforge.org/hg/rivet/rev/dae0ce346779
branches:  release-2-5-x
changeset: 5525:dae0ce346779
user:      Andy Buckley <andy at insectnation.org>
date:      Tue Sep 27 17:20:59 2016 +0100
description:
Use static arrays where possible and change foreach to range-for

diffs (truncated from 403 to 50 lines):

--- a/data/anainfo/ATLAS_2014_I1327229.info	Sun Sep 25 09:54:10 2016 +0100
+++ b/data/anainfo/ATLAS_2014_I1327229.info	Tue Sep 27 17:20:59 2016 +0100
@@ -10,22 +10,22 @@
 References:
  - arXiv:1411.2921 [hep-ex]
 RunInfo:
-  any process producing at least 3 leptons (e.g. pair production of doubly-charged Higgs or excited leptons)
+  Any process producing at least 3 leptons (e.g. pair production of doubly-charged Higgs or excited leptons)
 Beams: [p+, p+]
 Energies: [8000]
 PtCuts: [1,5,10,10]
 NeedCrossSection: True
 Description:
   A generic search for anomalous production of events with at least three charged leptons is presented. The data sample consists of
-  $pp$ collisions at $\sqrt{s} = 8$\,TeV collected in 2012 by the ATLAS experiment at the CERN Large Hadron Collider, and corresponds 
-  to an integratedi luminosity of 20.3\,$\text{fb}^{−1}$. Events are required to have at least three selected lepton candidates, at 
-  least two of which must be electrons or muons, while the third may be a hadronically decaying tau. Selected events are categorized 
-  based on their lepton flavour content and signal regions are constructed using several kinematic variables of interest. No significant 
-  deviations from Standard Model predictions are observed. Model-independent upper limits on contributions from beyond the Standard Model 
-  phenomena are provided for each signal region, along with prescription to re-interpret the limits for any model. Constraints are also 
-  placed on models predicting doubly charged Higgs bosons and excited leptons. For doubly charged Higgs bosons decaying to $e\tau$ or 
-  $\muon\tau$, lower limits on the mass are set at 400\,GeV at 95\,\% confidence level. For excited leptons, constraints are provided as 
-  functions of both the mass of the excited state and the compositeness scale $\Lambda$, with the strongest mass constraints arising in 
+  $pp$ collisions at $\sqrt{s} = 8$\,TeV collected in 2012 by the ATLAS experiment at the CERN Large Hadron Collider, and corresponds
+  to an integratedi luminosity of 20.3\,$\text{fb}^{−1}$. Events are required to have at least three selected lepton candidates, at
+  least two of which must be electrons or muons, while the third may be a hadronically decaying tau. Selected events are categorized
+  based on their lepton flavour content and signal regions are constructed using several kinematic variables of interest. No significant
+  deviations from Standard Model predictions are observed. Model-independent upper limits on contributions from beyond the Standard Model
+  phenomena are provided for each signal region, along with prescription to re-interpret the limits for any model. Constraints are also
+  placed on models predicting doubly charged Higgs bosons and excited leptons. For doubly charged Higgs bosons decaying to $e\tau$ or
+  $\muon\tau$, lower limits on the mass are set at 400\,GeV at 95\,\% confidence level. For excited leptons, constraints are provided as
+  functions of both the mass of the excited state and the compositeness scale $\Lambda$, with the strongest mass constraints arising in
   regions where the mass equals $\Lambda$. In such scenarios, lower mass limits are set at 3.0\,TeV for excited electrons and muons,
   2.5\,TeV for excited taus, and 1.6\,TeV for every excited-neutrino flavour.
 BibKey: Aad:2014hja
--- a/data/anainfo/ATLAS_2016_I1452559.info	Sun Sep 25 09:54:10 2016 +0100
+++ b/data/anainfo/ATLAS_2016_I1452559.info	Tue Sep 27 17:20:59 2016 +0100
@@ -7,6 +7,7 @@
 Status: UNVALIDATED
 Authors:
  - Andy Buckley <andy.buckley at cern.ch>
+ - Shehu AbdusSalam <shehu at cantab.net>
 References:
  - 'Phys.Rev. D94 (2016) no.3, 032005'
  - 'DOI: 10.1103/PhysRevD.94.032005'
--- a/src/Analyses/ATLAS_2014_I1327229.cc	Sun Sep 25 09:54:10 2016 +0100
+++ b/src/Analyses/ATLAS_2014_I1327229.cc	Tue Sep 27 17:20:59 2016 +0100
@@ -27,7 +27,8 @@
       _use_fiducial_lepton_efficiency = true;