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[Rivet-svn] r2390 - trunk/doc
blackhole at projects.hepforge.org
blackhole at projects.hepforge.org
Mon Apr 5 20:09:23 BST 2010
Author: buckley
Date: Mon Apr 5 20:09:23 2010
New Revision: 2390
Log:
Put a newline at the end of the analyses bib file
Modified:
trunk/doc/analyses.bib
trunk/doc/analyses.tex
trunk/doc/mk-analysis-latex
Modified: trunk/doc/analyses.bib
==============================================================================
--- trunk/doc/analyses.bib Mon Apr 5 20:07:44 2010 (r2389)
+++ trunk/doc/analyses.bib Mon Apr 5 20:09:23 2010 (r2390)
@@ -1,9 +1,6 @@
% Barate:1996fi
@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;%%" }
-% Aaltonen:2008de
- at Article{Aaltonen:2008de, author = "Aaltonen, T. and others", collaboration = "CDF", title = "{Measurement of $b$-jet Shapes in Inclusive Jet Production in $p \bar{p}$ Collisions at $\sqrt{s}$ = 1.96-TeV}", journal = "Phys. Rev.", volume = "D78", year = "2008", pages = "072005", eprint = "0806.1699", archivePrefix = "arXiv", primaryClass = "hep-ex", doi = "10.1103/PhysRevD.78.072005", SLACcitation = "%%CITATION = 0806.1699;%%" }
-
% Abazov:2006gs
@Article{Abazov:2006gs, author = "Abazov, V. M. and others", collaboration = "D0", title = "{Measurement of the ratios of the Z/G* + >= n jet production cross sections to the total inclusive Z/G* cross section in ppbar collisions at sqrt(s) = 1.96 TeV}", journal = "Phys. Lett.", volume = "B658", year = "2008", pages = "112-119", eprint = "hep-ex/0608052", archivePrefix = "arXiv", doi = "10.1016/j.physletb.2007.10.046", SLACcitation = "%%CITATION = HEP-EX/0608052;%%" }
@@ -13,20 +10,14 @@
% Aaltonen:2008dn
@Article{Aaltonen:2008dn, author = "Aaltonen, T. and others", collaboration = "CDF", title = "{Search for new particles decaying into dijets in proton- antiproton collisions at sqrt(s) = 1.96 TeV}", journal = "Phys. Rev.", volume = "D79", year = "2009", pages = "112002", eprint = "0812.4036", archivePrefix = "arXiv", primaryClass = "hep-ex", doi = "10.1103/PhysRevD.79.112002", SLACcitation = "%%CITATION = 0812.4036;%%" }
-% Abachi:1996et
- at Article{Abachi:1996et, author = "Abachi, S. and others", collaboration = "D0", title = "{The Azimuthal decorrelation of jets widely separated in rapidity}", journal = "Phys. Rev. Lett.", volume = "77", year = "1996", pages = "595-600", eprint = "hep-ex/9603010", archivePrefix = "arXiv", doi = "10.1103/PhysRevLett.77.595", SLACcitation = "%%CITATION = HEP-EX/9603010;%%" }
-
-% Ansorge:1988fg
- at Article{Ansorge:1988fg, author = "Ansorge, R. E. and others", collaboration = "UA5", title = "{CHARGED PARTICLE CORRELATIONS IN ANTI-P P COLLISIONS AT C.M. ENERGIES OF 200-GEV, 546-GEV AND 900-GEV}", journal = "Z. Phys.", volume = "C37", year = "1988", pages = "191-213", doi = "10.1007/BF01579906", SLACcitation = "%%CITATION = ZEPYA,C37,191;%%" }
-
% Abazov:2009av
@Article{Abazov:2009av, author = "Abazov, V. M. and others", collaboration = "D0", title = "{Measurements of differential cross sections of $Z /\gamma^\ast$+jets+X events in proton anti-proton collisions at $\sqrt{s}$=1.96 TeV}", journal = "Phys. Lett.", volume = "B678", year = "2009", pages = "45-54", eprint = "0903.1748", archivePrefix = "arXiv", primaryClass = "hep-ex", doi = "10.1016/j.physletb.2009.05.058", SLACcitation = "%%CITATION = 0903.1748;%%" }
% Abazov:2009pp
@Article{Abazov:2009pp, author = "Abazov, Victor Mukhamedovich and others", collaboration = "D0", title = "{Measurement of $Z / \gamma^\ast +jet+X$ angular distributions in $p \bar{p}$ collisions at $\sqrt{s}=1.96$ TeV}", journal = "Phys. Lett.", volume = "B682", year = "2010", pages = "370-380", eprint = "0907.4286", archivePrefix = "arXiv", primaryClass = "hep-ex", doi = "10.1016/j.physletb.2009.11.012", SLACcitation = "%%CITATION = 0907.4286;%%" }
-% Abreu:1996na
- at Article{Abreu:1996na, author = "Abreu, P. and others", collaboration = "DELPHI", title = "{Tuning and test of fragmentation models based on identified particles and precision event shape data}", journal = "Z. Phys.", volume = "C73", year = "1996", pages = "11-60", doi = "10.1007/s002880050295", SLACcitation = "%%CITATION = ZEPYA,C73,11;%%" }
+% Pfeifenschneider:1999rz
+ at Article{Pfeifenschneider:1999rz, author = "Pfeifenschneider, P. and others", collaboration = "JADE", title = "{QCD analyses and determinations of alpha(s) in e+ e- annihilation at energies between 35-GeV and 189-GeV}", journal = "Eur. Phys. J.", volume = "C17", year = "2000", pages = "19-51", eprint = "hep-ex/0001055", archivePrefix = "arXiv", doi = "10.1007/s100520000432", SLACcitation = "%%CITATION = HEP-EX/0001055;%%" }
% Affolder:2000ew
@Article{Affolder:2000ew, author = "Affolder, Anthony Allen and others", collaboration = "CDF", title = "{Measurement of the two-jet differential cross section in $p\bar{p}$ collisions at $\sqrt{s} = 1800$ GeV}", journal = "Phys. Rev.", volume = "D64", year = "2001", pages = "012001", eprint = "hep-ex/0012013", archivePrefix = "arXiv", doi = "10.1103/PhysRevD.64.012001", SLACcitation = "%%CITATION = HEP-EX/0012013;%%" }
@@ -34,56 +25,38 @@
% Affolder:1999jh
@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;%%" }
-% 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;%%" }
-
% Ackerstaff:1998hz
@Article{Ackerstaff:1998hz, author = "Ackerstaff, K. and others", collaboration = "OPAL", title = "{Measurements of flavour dependent fragmentation functions in Z0 --> q anti-q events}", journal = "Eur. Phys. J.", volume = "C7", year = "1999", pages = "369-381", eprint = "hep-ex/9807004", archivePrefix = "arXiv", doi = "10.1007/s100529901067", SLACcitation = "%%CITATION = HEP-EX/9807004;%%" }
% Alner:1986xu
@Article{Alner:1986xu, author = "Alner, G. J. and others", collaboration = "UA5", title = "{Scaling of Pseudorapidity Distributions at c.m. Energies Up to 0.9-TeV}", journal = "Z. Phys.", volume = "C33", year = "1986", pages = "1-6", doi = "10.1007/BF01410446", SLACcitation = "%%CITATION = ZEPYA,C33,1;%%" }
-% Chekanov:2001bw
- at Article{Chekanov:2001bw, author = "Chekanov, S. and others", collaboration = "ZEUS", title = "{Dijet photoproduction at HERA and the structure of the photon}", journal = "Eur. Phys. J.", volume = "C23", year = "2002", pages = "615-631", eprint = "hep-ex/0112029", archivePrefix = "arXiv", doi = "10.1007/s100520200936", SLACcitation = "%%CITATION = HEP-EX/0112029;%%" }
-
-% Abe:1994nj
- at Article{Abe:1994nj, author = "Abe, F. and others", collaboration = "CDF", title = "{Evidence for color coherence in $p\bar{p}$ collisions at $\sqrt{s} = 1.8$ TeV}", journal = "Phys. Rev.", volume = "D50", year = "1994", pages = "5562-5579", doi = "10.1103/PhysRevD.50.5562", SLACcitation = "%%CITATION = PHRVA,D50,5562;%%" }
+% :2007cp
+ at Article{:2007cp, author = "Aaltonen, T. and others", collaboration = "CDF - Run II", title = "{Measurement of inclusive jet cross-sections in Z/gamma*(-- -> $e^{+} e^{-)}$ + jets production in $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96-TeV}", journal = "Phys. Rev. Lett.", volume = "100", year = "2008", pages = "102001", eprint = "0711.3717", archivePrefix = "arXiv", primaryClass = "hep-ex", doi = "", SLACcitation = "%%CITATION = 0711.3717;%%" }
% Aaltonen:2009pc
@Article{Aaltonen:2009pc, author = "Aaltonen, T. and others", collaboration = "CDF", title = "{Measurement of $d\sigma/dy$ of Drell-Yan $e^+e^-$ pairs in the $Z$ Mass Region from $p\bar{p}$ Collisions at $\sqrt{s}=1.96$ TeV}", year = "2009", eprint = "0908.3914", archivePrefix = "arXiv", primaryClass = "hep-ex", SLACcitation = "%%CITATION = 0908.3914;%%" }
-% Abe:1995rw
- at Article{Abe:1995rw, author = "Abe, F. and others", collaboration = "CDF", title = "{Properties of high mass multi - jet events at the Fermilab $p\bar{p}$ collider}", journal = "Phys. Rev. Lett.", volume = "75", year = "1995", pages = "608-612", doi = "10.1103/PhysRevLett.75.608", SLACcitation = "%%CITATION = PRLTA,75,608;%%" }
-
% Abe:1996mj
@Article{Abe:1996mj, author = "Abe, F. and others", collaboration = "CDF", title = "{Measurement of dijet angular distributions at CDF}", journal = "Phys. Rev. Lett.", volume = "77", year = "1996", pages = "5336-5341", eprint = "hep-ex/9609011", archivePrefix = "arXiv", doi = "10.1103/PhysRevLett.77.5336", SLACcitation = "%%CITATION = HEP-EX/9609011;%%" }
% Affolder:2001fa
@Article{Affolder:2001fa, author = "Affolder, Anthony Allen and others", collaboration = "CDF", title = "{Measurement of the inclusive jet cross section in $\bar{p}p$ collisions at $\sqrt{s} = 1.8$ TeV}", journal = "Phys. Rev.", volume = "D64", year = "2001", pages = "032001", eprint = "hep-ph/0102074", archivePrefix = "arXiv", doi = "10.1103/PhysRevD.64.032001", SLACcitation = "%%CITATION = HEP-PH/0102074;%%" }
-% Alexopoulos:1998bi
- at Article{Alexopoulos:1998bi, author = "Alexopoulos, T. and others", title = "{The role of double parton collisions in soft hadron interactions}", journal = "Phys. Lett.", volume = "B435", year = "1998", pages = "453-457", doi = "10.1016/S0370-2693(98)00921-6", SLACcitation = "%%CITATION = PHLTA,B435,453;%%" }
-
% Aad:2010rd
@Article{Aad:2010rd, author = "Aad, G. and others", collaboration = "ALTAS", title = "{Charged-particle multiplicities in pp interactions at sqrt(s) = 900 GeV measured with the ATLAS detector at the LHC}", year = "2010", eprint = "1003.3124", archivePrefix = "arXiv", primaryClass = "hep-ex", doi = "10.1016/j.physletb.2010.03.064", SLACcitation = "%%CITATION = 1003.3124;%%" }
-% Abbott:1998jy
- at Article{Abbott:1998jy, author = "Abbott, B. and others", collaboration = "D0", title = "{Measurement of the shape of the transverse momentum distribution of $W$ bosons produced in $p\bar{p}$ collisions at $\sqrt{s} = 1.8$ TeV}", journal = "Phys. Rev. Lett.", volume = "80", year = "1998", pages = "5498-5503", eprint = "hep-ex/9803003", archivePrefix = "arXiv", doi = "10.1103/PhysRevLett.80.5498", SLACcitation = "%%CITATION = HEP-EX/9803003;%%" }
-
% Abreu:1995qx
@Article{Abreu:1995qx, author = "Abreu, P. and others", collaboration = "DELPHI", title = "{Strange baryon production in Z hadronic decays}", journal = "Z. Phys.", volume = "C67", year = "1995", pages = "543-554", doi = "10.1007/BF01553980", SLACcitation = "%%CITATION = ZEPYA,C67,543;%%" }
% Abazov:2008er
@Article{Abazov:2008er, author = "Abazov, V. M. and others", collaboration = "D0", title = "{Measurement of the differential cross-section for the production of an isolated photon with associated jet in $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96-TeV}", journal = "Phys. Lett.", volume = "B666", year = "2008", pages = "435-445", eprint = "0804.1107", archivePrefix = "arXiv", primaryClass = "hep-ex", doi = "10.1016/j.physletb.2008.06.076", SLACcitation = "%%CITATION = 0804.1107;%%" }
-% 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;%%" }
-
% Abulencia:2005yg
@Article{Abulencia:2005yg, author = "Abulencia, A. and others", collaboration = "CDF", title = "{Measurement of the inclusive jet cross section in $p\bar{p}$ interactions at $\sqrt{s} =$ 1.96-TeV using a cone-based jet algorithm}", journal = "Phys. Rev.", volume = "D74", year = "2006", pages = "071103", eprint = "hep-ex/0512020", archivePrefix = "arXiv", doi = "10.1103/PhysRevD.74.071103", SLACcitation = "%%CITATION = HEP-EX/0512020;%%" }
-% Aaltonen:2007ip
- at Article{Aaltonen:2007ip, author = "Aaltonen, T. and others", collaboration = "CDF", title = "{Measurement of the cross section for $W^-$ boson production in association with jets in ppbar collisions at $\sqrt{s}$ = 1.96-TeV}", journal = "Phys. Rev.", volume = "D77", year = "2008", pages = "011108", eprint = "0711.4044", archivePrefix = "arXiv", primaryClass = "hep-ex", doi = "10.1103/PhysRevD.77.011108", SLACcitation = "%%CITATION = 0711.4044;%%" }
+% Aaltonen:2009ty
+ at Article{Aaltonen:2009ty, author = "Aaltonen, T. and others", collaboration = "CDF", title = "{Measurement of the Inclusive Isolated Prompt Photon Cross Section in ppbar Collisions at sqrt{s} = 1.96 TeV using the CDF Detector}", journal = "Phys. Rev.", volume = "D80", year = "2009", pages = "111106", eprint = "0910.3623", archivePrefix = "arXiv", primaryClass = "hep-ex", doi = "10.1103/PhysRevD.80.111106", SLACcitation = "%%CITATION = 0910.3623;%%" }
% Decamp:1991uz
@Article{Decamp:1991uz, author = "Decamp, D. and others", collaboration = "ALEPH", title = "{Measurement of the charged particle multiplicity distribution in hadronic Z decays}", journal = "Phys. Lett.", volume = "B273", year = "1991", pages = "181-192", doi = "10.1016/0370-2693(91)90575-B", SLACcitation = "%%CITATION = PHLTA,B273,181;%%" }
@@ -100,17 +73,14 @@
% Abelev:2006cs
@Article{Abelev:2006cs, author = "Abelev, B. I. and others", collaboration = "STAR", title = "{Strange particle production in p + p collisions at s**(1/2) = 200-GeV}", journal = "Phys. Rev.", volume = "C75", year = "2007", pages = "064901", eprint = "nucl-ex/0607033", archivePrefix = "arXiv", doi = "10.1103/PhysRevC.75.064901", SLACcitation = "%%CITATION = NUCL-EX/0607033;%%" }
-% Pfeifenschneider:1999rz
- at Article{Pfeifenschneider:1999rz, author = "Pfeifenschneider, P. and others", collaboration = "JADE", title = "{QCD analyses and determinations of alpha(s) in e+ e- annihilation at energies between 35-GeV and 189-GeV}", journal = "Eur. Phys. J.", volume = "C17", year = "2000", pages = "19-51", eprint = "hep-ex/0001055", archivePrefix = "arXiv", doi = "10.1007/s100520000432", SLACcitation = "%%CITATION = HEP-EX/0001055;%%" }
-
% Abt:1994ye
@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;%%" }
% Abazov:2010ah
@Article{Abazov:2010ah, author = "Abazov, V. M. and others", collaboration = "The D0", title = "{Measurement of direct photon pair production cross sections in $p \bar{p}$ collisions at $\sqrt(s)=1.96$ TeV}", year = "2010", eprint = "1002.4917", archivePrefix = "arXiv", primaryClass = "hep-ex", SLACcitation = "%%CITATION = 1002.4917;%%" }
-% Abe:1991rk
- at Article{Abe:1991rk, author = "Abe, F. and others", collaboration = "CDF", title = "{Measurement of the W P(T) distribution in $\bar{p}p$ collisions at $\sqrt{s} = 1.8$ TeV}", journal = "Phys. Rev. Lett.", volume = "66", year = "1991", pages = "2951-2955", doi = "10.1103/PhysRevLett.66.2951", SLACcitation = "%%CITATION = PRLTA,66,2951;%%" }
+% Abreu:1996na
+ at Article{Abreu:1996na, author = "Abreu, P. and others", collaboration = "DELPHI", title = "{Tuning and test of fragmentation models based on identified particles and precision event shape data}", journal = "Z. Phys.", volume = "C73", year = "1996", pages = "11-60", doi = "10.1007/s002880050295", SLACcitation = "%%CITATION = ZEPYA,C73,11;%%" }
% Acosta:2004wqa
@Article{Acosta:2004wqa, author = "Acosta, Darin E. and others", collaboration = "CDF", title = "{The underlying event in hard interactions at the Tevatron $\bar{p}p$ collider}", journal = "Phys. Rev.", volume = "D70", year = "2004", pages = "072002", eprint = "hep-ex/0404004", archivePrefix = "arXiv", doi = "10.1103/PhysRevD.70.072002", SLACcitation = "%%CITATION = HEP-EX/0404004;%%" }
@@ -118,21 +88,12 @@
% Adloff:1999ws
@Article{Adloff:1999ws, author = "Adloff, C. and others", collaboration = "H1", title = "{Measurements of transverse energy flow in deep inelastic- scattering at HERA}", journal = "Eur. Phys. J.", volume = "C12", year = "2000", pages = "595-607", eprint = "hep-ex/9907027", archivePrefix = "arXiv", doi = "10.1007/s100520000287", SLACcitation = "%%CITATION = HEP-EX/9907027;%%" }
-% Abulencia:2006ce
- at Article{Abulencia:2006ce, author = "Abulencia, A. and others", collaboration = "CDF", title = "{Measurement of the $b$ jet cross-section in events with a $Z$ boson in $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96- TeV}", journal = "Phys. Rev.", volume = "D74", year = "2006", pages = "032008", eprint = "hep-ex/0605099", archivePrefix = "arXiv", doi = "10.1103/PhysRevD.74.032008", SLACcitation = "%%CITATION = HEP-EX/0605099;%%" }
-
% Abazov:2008ez
@Article{Abazov:2008ez, author = "Abazov, V. M. and others", collaboration = "D0", title = "{Measurement of differential $Z / \gamma^{*}$ + jet + $X$ cross sections in $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96-TeV}", journal = "Phys. Lett.", volume = "B669", year = "2008", pages = "278-286", eprint = "0808.1296", archivePrefix = "arXiv", primaryClass = "hep-ex", doi = "10.1016/j.physletb.2008.09.060", SLACcitation = "%%CITATION = 0808.1296;%%" }
% Abazov:2008qv
@Article{Abazov:2008qv, author = "Abazov, V. M. and others", collaboration = "D0", title = "{Measurement of the electron charge asymmetry in $p \bar{p} \to W + X \to e \nu + X$ events at $\sqrt{s}$ = 1.96-TeV}", journal = "Phys. Rev. Lett.", volume = "101", year = "2008", pages = "211801", eprint = "0807.3367", archivePrefix = "arXiv", primaryClass = "hep-ex", doi = "10.1103/PhysRevLett.101.211801", SLACcitation = "%%CITATION = 0807.3367;%%" }
-% Nattrass:2008tw
- at Article{Nattrass:2008tw, author = "Nattrass, Christine", title = "{Energy and system dependence of high-$p_T$ triggered two- particle near-side correlations}", journal = "Eur. Phys. J.", volume = "C62", year = "2009", pages = "265-269", eprint = "0809.5261", archivePrefix = "arXiv", primaryClass = "nucl-ex", doi = "10.1140/epjc/s10052-009-1037-8", SLACcitation = "%%CITATION = 0809.5261;%%" }
-
-% Aaltonen:2009ty
- at Article{Aaltonen:2009ty, author = "Aaltonen, T. and others", collaboration = "CDF", title = "{Measurement of the Inclusive Isolated Prompt Photon Cross Section in ppbar Collisions at sqrt{s} = 1.96 TeV using the CDF Detector}", journal = "Phys. Rev.", volume = "D80", year = "2009", pages = "111106", eprint = "0910.3623", archivePrefix = "arXiv", primaryClass = "hep-ex", doi = "10.1103/PhysRevD.80.111106", SLACcitation = "%%CITATION = 0910.3623;%%" }
-
% Abazov:2010fr
@Article{Abazov:2010fr, author = "Abazov, V. M. and others", collaboration = "D0", title = "{Measurement of the dijet invariant mass cross section in $p\overline{p}$ collisions at $\sqrt{s} =$ 1.96 TeV}", year = "2010", eprint = "1002.4594", archivePrefix = "arXiv", primaryClass = "hep-ex", SLACcitation = "%%CITATION = 1002.4594;%%" }
@@ -172,17 +133,8 @@
% :2007nt
@Article{:2007nt, author = "Abazov, V. M. and others", collaboration = "D0", title = "{Measurement of the shape of the boson transverse momentum distribution in $p \bar{p} \to Z / \gamma^{*} \to e^+ e^- + X$ events produced at $\sqrt{s}$=1.96-TeV}", journal = "Phys. Rev. Lett.", volume = "100", year = "2008", pages = "102002", eprint = "0712.0803", archivePrefix = "arXiv", primaryClass = "hep-ex", doi = "10.1103/PhysRevLett.100.102002", SLACcitation = "%%CITATION = 0712.0803;%%" }
-% Aid:1995we
- at Article{Aid:1995we, author = "Aid, S. and others", collaboration = "H1", title = "{Transverse energy and forward jet production in the low x regime at HERA}", journal = "Phys. Lett.", volume = "B356", year = "1995", pages = "118-128", eprint = "hep-ex/9506012", archivePrefix = "arXiv", doi = "10.1016/0370-2693(95)00804-T", SLACcitation = "%%CITATION = HEP-EX/9506012;%%" }
-
-% Aaltonen:2008mt
- at Article{Aaltonen:2008mt, author = "Aaltonen, T. and others", collaboration = "CDF", title = "{Measurement of Cross Sections for $b$ Jet Production in Events with a $Z$ Boson in $p^-$ anti-p Collisions at $\sqrt{s}$ = 1.96-TeV}", journal = "Phys. Rev.", volume = "D79", year = "2009", pages = "052008", eprint = "0812.4458", archivePrefix = "arXiv", primaryClass = "hep-ex", doi = "10.1103/PhysRevD.79.052008", SLACcitation = "%%CITATION = 0812.4458;%%" }
-
-% Abe:1996nn
- at Article{Abe:1996nn, author = "Abe, F. and others", collaboration = "CDF", title = "{Further Properties of High-Mass Multijet Events at the Fermilab Proton-Antiproton Collider}", journal = "Phys. Rev.", volume = "D54", year = "1996", pages = "4221-4233", eprint = "hep-ex/9605004", archivePrefix = "arXiv", doi = "10.1103/PhysRevD.54.4221", SLACcitation = "%%CITATION = HEP-EX/9605004;%%" }
-
-% Breakstone:1983ns
- at Article{Breakstone:1983ns, author = "Breakstone, A. and others", collaboration = "Ames-Bologna-CERN-Dortmund-Heidelberg-Warsaw", title = "{Charged Multiplicity Distribution in p p Interactions at ISR Energies}", journal = "Phys. Rev.", volume = "D30", year = "1984", pages = "528", doi = "10.1103/PhysRevD.30.528", SLACcitation = "%%CITATION = PHRVA,D30,528;%%" }
+% 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;%%" }
% Abbiendi:2004qz
@Article{Abbiendi:2004qz, author = "Abbiendi, G. and others", collaboration = "OPAL", title = "{Measurement of event shape distributions and moments in e+ e- --> hadrons at 91-GeV - 209-GeV and a determination of alpha(s)}", journal = "Eur. Phys. J.", volume = "C40", year = "2005", pages = "287-316", eprint = "hep-ex/0503051", archivePrefix = "arXiv", doi = "10.1140/epjc/s2005-02120-6", SLACcitation = "%%CITATION = HEP-EX/0503051;%%" }
@@ -196,11 +148,8 @@
% Abazov:2004hm
@Article{Abazov:2004hm, author = "Abazov, V. M. and others", collaboration = "D0", title = "{Measurement of dijet azimuthal decorrelations at central rapidities in $p\bar{p}$ collisions at $\sqrt{s} = 1.96$ TeV}", journal = "Phys. Rev. Lett.", volume = "94", year = "2005", pages = "221801", eprint = "hep-ex/0409040", archivePrefix = "arXiv", doi = "10.1103/PhysRevLett.94.221801", SLACcitation = "%%CITATION = HEP-EX/0409040;%%" }
-% Abachi:1995zv
- at Article{Abachi:1995zv, author = "Abachi, S. and others", collaboration = "D0", title = "{Studies of Topological Distributions of the Three- and Four-Jet Events in $\bar{p}p$ Collisions at $\sqrt{s}=1800$ GeV with the D\O\\ Detector}", journal = "Phys. Rev.", volume = "D53", year = "1996", pages = "6000-6016", eprint = "hep-ex/9509005", archivePrefix = "arXiv", doi = "10.1103/PhysRevD.53.6000", SLACcitation = "%%CITATION = HEP-EX/9509005;%%" }
-
-% :2007cp
- at Article{:2007cp, author = "Aaltonen, T. and others", collaboration = "CDF - Run II", title = "{Measurement of inclusive jet cross-sections in Z/gamma*(-- -> $e^{+} e^{-)}$ + jets production in $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96-TeV}", journal = "Phys. Rev. Lett.", volume = "100", year = "2008", pages = "102001", eprint = "0711.3717", archivePrefix = "arXiv", primaryClass = "hep-ex", doi = "", SLACcitation = "%%CITATION = 0711.3717;%%" }
+% 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;%%" }
% Acosta:2004sn
@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;%%" }
@@ -214,8 +163,5 @@
% Abelev:2006uq
@Article{Abelev:2006uq, author = "Abelev, B. I. and others", collaboration = "STAR", title = "{Longitudinal double-spin asymmetry and cross section for inclusive jet production in polarized proton collisions at s**(1/2) = 200-GeV}", journal = "Phys. Rev. Lett.", volume = "97", year = "2006", pages = "252001", eprint = "hep-ex/0608030", archivePrefix = "arXiv", doi = "10.1103/PhysRevLett.97.252001", SLACcitation = "%%CITATION = HEP-EX/0608030;%%" }
-% Abe:1997yb
- at Article{Abe:1997yb, author = "Abe, F. and others", collaboration = "CDF", title = "{Properties of six-jet events with large six-jet mass at the Fermilab $p\bar{p}$ collider}", journal = "Phys. Rev.", volume = "D56", year = "1997", pages = "2532-2543", doi = "10.1103/PhysRevD.56.2532", SLACcitation = "%%CITATION = PHRVA,D56,2532;%%" }
-
% 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;%%" }
\ No newline at end of file
+ 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;%%" }
Modified: trunk/doc/analyses.tex
==============================================================================
--- trunk/doc/analyses.tex Mon Apr 5 20:07:44 2010 (r2389)
+++ trunk/doc/analyses.tex Mon Apr 5 20:09:23 2010 (r2390)
@@ -60,7 +60,7 @@
\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.
+\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.
\clearpage
@@ -215,34 +215,6 @@
\clearpage
-\typeout{Handling analysis DELPHI_2003_WUD_03_11}
-\subsection{DELPHI\_2003\_WUD\_03\_11}
-\textbf{4-jet angular distributions at LEP (note)}\newline
-\textbf{Experiment:} DELPHI (LEP 1) \newline
-\textbf{Status:} UNVALIDATED\newline
-\textbf{Authors:}
- \penalty 100
-\begin{itemize}
- \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth at cern.ch}{hendrik.hoeth at cern.ch}$\,\rangle$;
-\end{itemize}
-\textbf{References:}
- \penalty 100
-\begin{itemize}
- \item Diploma thesis WUD-03-11, University of Wuppertal
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}
-
-\noindent The 4-jet angular distributions (Bengtsson-Zerwas, K\"orner-Schierholz- Willrodt, Nachtmann-Reiter, and $\alpha_{34}$) have been measured with DELPHI at LEP 1 using Jade and Durham cluster algorithms.
-
-\clearpage
-
-
-\clearpage
-
\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
@@ -326,7 +298,7 @@
\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.
+\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.
\clearpage
@@ -392,126 +364,6 @@
\clearpage
-\typeout{Handling analysis CDF_1991_S2313472}
-\subsection[CDF\_1991\_S2313472]{CDF\_1991\_S2313472\,\cite{Abe:1991rk}}
-\textbf{W-boson \pT measurement in $p\bar{p}$ collisions at $\sqrt{s}=1.8~\TeV$}\newline
-\textbf{Experiment:} CDF (Tevatron) \newline
-\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+2313472}{2313472}\newline
-\textbf{Status:} UNVALIDATED\newline
-\textbf{Authors:}
- \penalty 100
-\begin{itemize}
- \item Holger Schulz $\langle\,$\href{mailto:hschulz at physik.hu-berlin.de}{hschulz at physik.hu-berlin.de}$\,\rangle$;
-\end{itemize}
-\textbf{References:}
- \penalty 100
-\begin{itemize}
- \item Phys.Rev.Lett.66:2951-2955,1991
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item QCD events with W+- production and electronic decays\end{itemize}
-
-\noindent This is a CDF analysis from run 1, where the distribution of the transverse momentum of W candidates that decay electronically, is measured. The electron is required to be within $\left|\eta\right| < 1.1$, to have a transverse energy of $E_\perp > 20~\GeV$ and a $p_\perp > 12~\GeV$. The neutrino is required to produce a missing energy of $E_{\perp, \text{ miss}}>20~\GeV$.
-
-\clearpage
-
-
-\clearpage
-
-\typeout{Handling analysis CDF_1994_S2952106}
-\subsection[CDF\_1994\_S2952106]{CDF\_1994\_S2952106\,\cite{Abe:1994nj}}
-\textbf{CDF Run I color coherence analysis.}\newline
-\textbf{Experiment:} CDF (Tevatron Run 1) \newline
-\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+2952106}{2952106}\newline
-\textbf{Status:} UNVALIDATED - not functional\newline
-\textbf{Authors:}
- \penalty 100
-\begin{itemize}
- \item Lars Sonnenschein $\langle\,$\href{mailto:Lars.Sonnenschein at cern.ch}{Lars.Sonnenschein at cern.ch}$\,\rangle$;
-\end{itemize}
-\textbf{References:}
- \penalty 100
-\begin{itemize}
- \item Phys.Rev.D50,5562,1994
- \item DOI: \href{http://dx.doi.org/10.1103/PhysRevD.50.5562}{10.1103/PhysRevD.50.5562}
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item QCD events at \ensuremath{\sqrt{s}} = 1800 GeV. Leading jet \pTmin = 100 GeV.\end{itemize}
-
-\noindent CDF Run I color coherence analysis. Events with $\ge 3$ jets are selected and Et distributions of the three highest-\pT jets are obtained. The plotted quantities are the $\Delta{R}$ between the 2nd and 3rd leading jets in the \pT and pseudorapidity of the 3rd jet, and $\alpha = \mathrm{d}{\eta}/\mathrm{d}{\phi}$, where $\mathrm{d}{\eta}$ is the pseudorapidity difference between the 2nd and 3rd jets and $\mathrm{d}{\phi}$ is their azimuthal angle difference. Since the data has not been detector-corrected, a bin by bin correction is applied, based on the distributions with ideal and CDF simulation as given in the publication.
-
-\clearpage
-
-
-\clearpage
-
-\typeout{Handling analysis CDF_1996_S3108457}
-\subsection[CDF\_1996\_S3108457]{CDF\_1996\_S3108457\,\cite{Abe:1995rw}}
-\textbf{Properties of High-Mass Multijet Events}\newline
-\textbf{Experiment:} CDF (Tevatron Run 1) \newline
-\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+3108457}{3108457}\newline
-\textbf{Status:} UNVALIDATED\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{References:}
- \penalty 100
-\begin{itemize}
- \item Phys.Rev.Lett.75:608-612,1995
- \item DOI: \href{http://dx.doi.org/10.1103/PhysRevLett.75.608}{10.1103/PhysRevLett.75.608}
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item Pure QCD events without underlying event.\end{itemize}
-
-\noindent Properties of two-, three-, four-, five-, and six-jet events... Multijet-mass, leading jet angle, jet \pT.
-
-\clearpage
-
-
-\clearpage
-
-\typeout{Handling analysis CDF_1996_S3349578}
-\subsection[CDF\_1996\_S3349578]{CDF\_1996\_S3349578\,\cite{Abe:1996nn}}
-\textbf{Further properties of high-mass multijet events}\newline
-\textbf{Experiment:} CDF (Tevatron Run 1) \newline
-\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+3349578}{3349578}\newline
-\textbf{Status:} UNVALIDATED\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{References:}
- \penalty 100
-\begin{itemize}
- \item Phys.Rev.D54:4221-4233,1996
- \item DOI: \href{http://dx.doi.org/10.1103/PhysRevD.54.4221}{10.1103/PhysRevD.54.4221}
- \item arXiv: \href{http://arxiv.org/abs/hep-ex/9605004}{hep-ex/9605004}
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item Pure QCD events without underlying event.\end{itemize}
-
-\noindent Multijet distributions corresponding to ($4N-4$) variables that span the $N$-body parameter space in inclusive $N = 3$-, 4-, and 5-jet events.
-
-\clearpage
-
-
-\clearpage
-
\typeout{Handling analysis CDF_1996_S3418421}
\subsection[CDF\_1996\_S3418421]{CDF\_1996\_S3418421\,\cite{Abe:1996mj}}
\textbf{Dijet angular distributions}\newline
@@ -543,37 +395,6 @@
\clearpage
-\typeout{Handling analysis CDF_1997_S3541940}
-\subsection[CDF\_1997\_S3541940]{CDF\_1997\_S3541940\,\cite{Abe:1997yb}}
-\textbf{Properties of six jet events with large six jet mass}\newline
-\textbf{Experiment:} CDF (Tevatron Run 1) \newline
-\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+3541940}{3541940}\newline
-\textbf{Status:} UNVALIDATED\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{References:}
- \penalty 100
-\begin{itemize}
- \item Phys.Rev.D56:2532-2543,1997
- \item DOI: \href{http://dx.doi.org/10.1103/PhysRevD.56.2532}{10.1103/PhysRevD.56.2532}
- \item http://lss.fnal.gov/archive/1997/pub/Pub-97-093-E.pdf
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item Pure QCD events without underlying event.\end{itemize}
-
-\noindent Multijet distributions corresponding to 20 variables that span the 6-body parameter space in inclusive 6-jet events.
-
-\clearpage
-
-
-\clearpage
-
\typeout{Handling analysis CDF_1998_S3618439}
\subsection[CDF\_1998\_S3618439]{CDF\_1998\_S3618439\,\cite{Abe:1997eua}}
\textbf{Differential cross-section for events with large total transverse energy}\newline
@@ -597,7 +418,7 @@
\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 $E_\perp^j > E_\perp^\mathrm{min}$.
+\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 $E_\perp^j > E_\perp^\mathrm{min}$.
\clearpage
@@ -628,7 +449,7 @@
\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.
+\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 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
@@ -691,7 +512,7 @@
\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 $0.1 < |\eta_2| < 3.0$.
+\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 $0.1 < |\eta_2| < 3.0$.
\clearpage
@@ -810,7 +631,7 @@
\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.
@@ -875,7 +696,7 @@
\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.
@@ -915,37 +736,6 @@
\clearpage
-\typeout{Handling analysis CDF_2006_S6653332}
-\subsection[CDF\_2006\_S6653332]{CDF\_2006\_S6653332\,\cite{Abulencia:2006ce}}
-\textbf{\pT and eta distributions of jets in Z + jet production}\newline
-\textbf{Experiment:} CDF (Tevatron Run 2) \newline
-\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+6653332}{6653332}\newline
-\textbf{Status:} UNVALIDATED - uses unphysical b quarks\newline
-\textbf{Authors:}
- \penalty 100
-\begin{itemize}
- \item Lars Sonnenschein $\langle\,$\href{mailto:Lars.Sonnenschein at cern.ch}{Lars.Sonnenschein at cern.ch}$\,\rangle$;
-\end{itemize}
-\textbf{References:}
- \penalty 100
-\begin{itemize}
- \item Phys.Rev.D.74:032008,2006
- \item DOI: \href{http://dx.doi.org/10.1103/PhysRevD.74.032008}{10.1103/PhysRevD.74.032008}
- \item arXiv: \href{http://arxiv.org/abs/hep-ex/0605099v2}{hep-ex/0605099v2}
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item Z + jets events at \ensuremath{\sqrt{s}} = 1960 GeV. Jets min \pT cut = 20~GeV, leptons min \pT cut = 10~GeV\end{itemize}
-
-\noindent Measurement of the b jet cross section in events with Z boson in p pbar collisions at center-of-mass energy \ensuremath{\sqrt{s}} = 1.96 TeV. The data cover jet transverse momenta above 20 GeV and jet pseudorapidities in the range -1.5 to 1.5. Z bosons are identified in their electron and muon decay modes in an invariant dilepton mass range between 66 and 116 GeV.
-
-\clearpage
-
-
-\clearpage
-
\typeout{Handling analysis CDF_2007_S7057202}
\subsection[CDF\_2007\_S7057202]{CDF\_2007\_S7057202\,\cite{Abulencia:2007ez}}
\textbf{CDF Run II inclusive jet cross-section using the kT algorithm}\newline
@@ -970,7 +760,7 @@
\penalty 100
\begin{itemize}
- \item p-pbar collisions at 1960~GeV. Jet \pT bins from 54~GeV to 700~GeV. Jet rapidity $< |2.1|$.\end{itemize}
+ \item p-pbar collisions at 1960~GeV. Jet \pT bins from 54~GeV to 700~GeV. Jet rapidity $< |2.1|$.\end{itemize}
\noindent CDF Run II measurement of inclusive jet cross sections at a p-pbar collision energy of 1.96~TeV. Jets are reconstructed in the central part of the detector ($|y|<2.1$) using the kT algorithm with an $R$ parameter of 0.7. The minimum jet \pT considered is 54~GeV, with a maximum around 700~GeV. The inclusive jet \pT is plotted in bins of rapidity $|y|<0.1$, $0.1<|y|<0.7$, $0.7<|y|<1.1$, $1.1<|y|<1.6$ and $1.6<|y|<2.1$.
@@ -995,7 +785,7 @@
\penalty 100
\begin{itemize}
- \item $p\bar{p}$ 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 $p\bar{p}$ 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.
@@ -1057,71 +847,9 @@
\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}
-
-\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 $\pT^\text{jet} > 30~\text{GeV}/c$.
-
-\clearpage
-
-
-\clearpage
-
-\typeout{Handling analysis CDF_2008_S7541902}
-\subsection[CDF\_2008\_S7541902]{CDF\_2008\_S7541902\,\cite{Aaltonen:2007ip}}
-\textbf{Jet \pT and multiplicity distributions in W + jets events}\newline
-\textbf{Experiment:} CDF (Tevatron Run 2) \newline
-\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+7541902}{7541902}\newline
-\textbf{Status:} UNVALIDATED\newline
-\textbf{Authors:}
- \penalty 100
-\begin{itemize}
- \item Ben Cooper $\langle\,$\href{mailto:b.d.cooper at qmul.ac.uk}{b.d.cooper at qmul.ac.uk}$\,\rangle$;
- \item Emily Nurse $\langle\,$\href{mailto:nurse at hep.ucl.ac.uk}{nurse at hep.ucl.ac.uk}$\,\rangle$;
-\end{itemize}
-\textbf{References:}
- \penalty 100
-\begin{itemize}
- \item arXiv: \href{http://arxiv.org/abs/0711.4044}{0711.4044}
- \item Phys.Rev.D77:011108,2008
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item Requires the process $p\bar{p} \rightarrow {W} \rightarrow {e}\nu$. Additional hard jets will also have to be included to get a good description. The LO process in Herwig is set with IPROC=1451.\end{itemize}
-
-\noindent Measurement of the cross section for W boson production in association with jets in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV. The analysis uses 320 pb$^{-1}$ of data collected with the CDF II detector. W bosons are identified in their $e\nu$ decay channel and jets are reconstructed using an $R < 0.4$ cone algorithm. For each $W + \geq$ n-jet sample (where n = 1--4) a measurement of d$\sigma({p}\bar{p} \rightarrow W + \geq$ n jet)/d$E_T(n^{th}$-jet) $\times$ BR($W \rightarrow{e}\nu$) is made, where d$E_T(n^{th}$-jet) is the Et of the n$^{th}$-highest Et jet above 20 GeV. A measurement of the total cross section, $\sigma(p\bar{p} \rightarrow W + \geq$ n-jet) $\times$ BR($W \rightarrow{e}\nu)$ with $E_T(n^{th}-jet) > 25$ GeV is also made. Both measurements are made for jets with $|\eta| < 2$ and for a limited region of the $W \rightarrow{e}\nu$ decay phase space; $|\eta^{e}| < 1.1$, $p_{T}^{e} > 20$ GeV, $p_{T}^{\nu} > 30$ GeV and $M_{T} > 20$ GeV. The cross secti
ons are corrected for all detector effects and can be directly compared to particle level $W$ + jet(s) predictions. These measurements can be used to test and tune QCD predictions for the number of jets in and kinematics of $W$ + jets events.
-
-\clearpage
-
-
-\clearpage
-
-\typeout{Handling analysis CDF_2008_S7782535}
-\subsection[CDF\_2008\_S7782535]{CDF\_2008\_S7782535\,\cite{Aaltonen:2008de}}
-\textbf{CDF Run II b-jet shape paper}\newline
-\textbf{Experiment:} CDF (Tevatron Run 2) \newline
-\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+7782535}{7782535}\newline
-\textbf{Status:} UNVALIDATED\newline
-\textbf{Authors:}
- \penalty 100
-\begin{itemize}
- \item Alison Lister $\langle\,$\href{mailto:alister at fnal.gov}{alister at fnal.gov}$\,\rangle$;
- \item Emily Nurse $\langle\,$\href{mailto:nurse at hep.ucl.ac.uk}{nurse at hep.ucl.ac.uk}$\,\rangle$;
-\end{itemize}
-\textbf{References:}
- \penalty 100
-\begin{itemize}
- \item arXiv: \href{http://arxiv.org/abs/0806.1699}{0806.1699}
- \item Phys.Rev.D78:072005,2008
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item Requires $2\rightarrow{2}$ QCD scattering processes. The minimum jet Et is 52 GeV, so a cut on kinematic \pTmin may be required for good statistics.\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 A measurement of the shapes of b-jets using 300 pb$^{-1}$ of data obtained with CDF II in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV. The measured quantity is the average integrated jet shape, which is computed over an ensemble of jets. This quantity is expressed as $\Psi(r/R) = \langle\frac{p_T(0 \rightarrow r)}{p_T(0 \rightarrow R)}\rangle$, where \pT (0$\rightarrow$r) is the scalar sum of the transverse momenta of all objects inside a sub-cone of radius r around the jet axis. The integrated shapes are by definition normalized such that $\Psi(r/R =1) = 1$. The measurement is done in bins of jet \pT in the range 52 to 300 GeV/c. The jets have $|\eta| < 0.7$. The b-jets are expected to be broader than inclusive jets.Moreover, b-jets containing a single b-quark are expected to be narrower than those containing a b bbar pair from gluon splitting.
+\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 $\pT^\text{jet} > 30~\text{GeV}/c$.
\clearpage
@@ -1188,35 +916,6 @@
\clearpage
-\typeout{Handling analysis CDF_2008_S8095620}
-\subsection[CDF\_2008\_S8095620]{CDF\_2008\_S8095620\,\cite{Aaltonen:2008mt}}
-\textbf{CDF Run II Z+b-jet cross section paper, 2 fb-1}\newline
-\textbf{Experiment:} CDF (Tevatron Run 2) \newline
-\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+8095620}{8095620}\newline
-\textbf{Status:} UNVALIDATED\newline
-\textbf{Authors:}
- \penalty 100
-\begin{itemize}
- \item Emily Nurse $\langle\,$\href{mailto:nurse at hep.ucl.ac.uk}{nurse at hep.ucl.ac.uk}$\,\rangle$;
-\end{itemize}
-\textbf{References:}
- \penalty 100
-\begin{itemize}
- \item arXiv: \href{http://arxiv.org/abs/0812.4458}{0812.4458}
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item Requires the process $p\bar{p} \rightarrow {Z} \rightarrow{\ell}\ell$, where $\ell$ is $e$ or $\mu$. Additional hard jets will also have to be included to get a good description.\end{itemize}
-
-\noindent Measurement of the b-jet production cross section for events containing a $Z$ boson produced in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV, using data corresponding to an integrated luminosity of 2 fb$^{-1}$ collected by the CDF II detector at the Tevatron. $Z$ bosons are selected in the electron and muon decay modes. Jets are considered with transverse energy $E_T>20$ GeV and pseudorapidity $|\eta|<1.5$. The ratio of the integrated $Z$ + b-jet cross section to the inclusive $Z$ production cross section is measured differentially in jet $E_T$, jet $\eta$, $Z$-boson transverse momentum, number of jets, and number of b-jets. The first two measurements have an entry for each b-jet in the event, the last three measurements have one entry per event.
-
-\clearpage
-
-
-\clearpage
-
\typeout{Handling analysis CDF_2009_S8233977}
\subsection[CDF\_2009\_S8233977]{CDF\_2009\_S8233977\,\cite{Aaltonen:2009ne}}
\textbf{CDF Run 2 min bias cross-section analysis}\newline
@@ -1240,7 +939,7 @@
\penalty 100
\begin{itemize}
- \item $p\bar{p}$ QCD interactions at 1960~GeV. Particles with $c \\tau > {}$10 mm should be set stable.\end{itemize}
+ \item $p\bar{p}$ QCD interactions at 1960~GeV. Particles with $c \\tau > {}$10 mm should be set stable.\end{itemize}
\noindent Niccolo Moggi's min bias analysis. Minimum bias events are used to measure the average track \pT vs. charged multiplicity, a track \pT distribution and an inclusive $\sum E_T$ distribution.
@@ -1269,7 +968,7 @@
\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.
@@ -1307,97 +1006,6 @@
\clearpage
-\typeout{Handling analysis D0_1996_S3214044}
-\subsection[D0\_1996\_S3214044]{D0\_1996\_S3214044\,\cite{Abachi:1995zv}}
-\textbf{Topological distributions of inclusive three- and four-jet events}\newline
-\textbf{Experiment:} D0 (Tevatron Run 1) \newline
-\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+3214044}{3214044}\newline
-\textbf{Status:} UNVALIDATED - currently wrong jet algorithm!\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{References:}
- \penalty 100
-\begin{itemize}
- \item Phys.Rev.D53:6000-6016,1996
- \item DOI: \href{http://dx.doi.org/10.1103/PhysRevD.53.6000}{10.1103/PhysRevD.53.6000}
- \item arXiv: \href{http://arxiv.org/abs/hep-ex/9509005}{hep-ex/9509005}
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item $p \bar{p} \to$ jets at 1800 GeV with minimum jet \pT in analysis = 20 GeV\end{itemize}
-
-\noindent The global topologies of inclusive three- and four-jet events produced in pbar p interactions are described. The three- and four-jet events are selected from data recorded by the D0 detector at the Fermilab Tevatron Collider operating at a center-of-mass energy of $\sqrt{s}$=1800 GeV. The studies also show that the topological distributions of the different subprocesses involving different numbers of quarks are very similar and reproduce the measured distributions well. The parton-shower Monte Carlo generators provide a less satisfactory description of the topologies of the three- and four-jet events.
-
-\clearpage
-
-
-\clearpage
-
-\typeout{Handling analysis D0_1996_S3324664}
-\subsection[D0\_1996\_S3324664]{D0\_1996\_S3324664\,\cite{Abachi:1996et}}
-\textbf{Azimuthal decorrelation of jets widely separated in rapidity}\newline
-\textbf{Experiment:} D0 (Tevatron Run 1) \newline
-\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+3324664}{3324664}\newline
-\textbf{Status:} UNVALIDATED - currently wrong jet algorithm!\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{References:}
- \penalty 100
-\begin{itemize}
- \item Phys.Rev.Lett.77:595-600,1996
- \item DOI: \href{http://dx.doi.org/10.1103/PhysRevLett.77.595}{10.1103/PhysRevLett.77.595}
- \item arXiv: \href{http://arxiv.org/abs/hep-ex/9603010}{hep-ex/9603010}
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item $p \bar{p} \to jets$ at 1800 GeV\end{itemize}
-
-\noindent First measurement of the azimuthal decorrelation between jets with pseudorapidity separation up to five units. The data were accumulated using the D0 detector during Tevatron Run 1 at $\sqrt{s}=1.8$ TeV.
-
-\clearpage
-
-
-\clearpage
-
-\typeout{Handling analysis D0_1998_S3711838}
-\subsection[D0\_1998\_S3711838]{D0\_1998\_S3711838\,\cite{Abbott:1998jy}}
-\textbf{W-boson \pT measurement in $p\bar{p}$ collisions at $\sqrt{s}=1.8~\TeV$}\newline
-\textbf{Experiment:} D0 (Tevatron) \newline
-\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+3711838}{3711838}\newline
-\textbf{Status:} UNVALIDATED\newline
-\textbf{Authors:}
- \penalty 100
-\begin{itemize}
- \item Holger Schulz $\langle\,$\href{mailto:hschulz at physik.hu-berlin.de}{hschulz at physik.hu-berlin.de}$\,\rangle$;
-\end{itemize}
-\textbf{References:}
- \penalty 100
-\begin{itemize}
- \item Phys. Rev. Lett. 80, 5498–5503
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item QCD events with W+- production and electronic decays\end{itemize}
-
-\noindent This is a D0 analysis from Run 1, where the distribution of the transverse momentum of W candidates that decay electronically, is measured. The electron is required to be within $\left|\eta\right| < 1.1$ and to have a transverse energy of $E_\perp > 25~\GeV$. The neutrino is required to produce a missing energy of $E_{\perp, \text{ miss}}>25~\GeV$. The analysed data sample is three times as large as the similar measurement performed at CDF in 1991.
-
-\clearpage
-
-
-\clearpage
-
\typeout{Handling analysis D0_2001_S4674421}
\subsection[D0\_2001\_S4674421]{D0\_2001\_S4674421\,\cite{Abazov:2001nta}}
\textbf{Tevatron Run I differential W/Z boson cross-section analysis}\newline
@@ -1452,7 +1060,7 @@
\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.
+\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.
\clearpage
@@ -1482,7 +1090,7 @@
\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 D\O 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 ($q \bar{q} \ensuremath{\to} \gamma g$) 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
@@ -1516,7 +1124,7 @@
\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 $0.4~\text{fb}^{-1}$.
+\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 $0.4~\text{fb}^{-1}$.
\clearpage
@@ -1607,7 +1215,7 @@
\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 $p \bar{p}$ 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.
@@ -1639,7 +1247,7 @@
\penalty 100
\begin{itemize}
- \item Produce only gamma + jet ($q,\bar{q},g$) 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 ($q,\bar{q},g$) 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 $p \bar{p}$ \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 $|y_\text{jet}| < 0.8$ 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.
@@ -1671,7 +1279,7 @@
\penalty 100
\begin{itemize}
- \item * Event type: W production with decay to $e \, \nu_e$ only
+ \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}
@@ -1856,36 +1464,6 @@
\clearpage
-\clearpage
-
-\typeout{Handling analysis E735_1998_S3905616}
-\subsection[E735\_1998\_S3905616]{E735\_1998\_S3905616\,\cite{Alexopoulos:1998bi}}
-\textbf{Charged particle multiplicity in ppbar collisions at \ensuremath{\sqrt{s}} = 1.8 TeV}\newline
-\textbf{Experiment:} E735 (Tevatron) \newline
-\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+3905616}{3905616}\newline
-\textbf{Status:} UNVALIDATED - need trigger etc.\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 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 Phys.Lett.B435:453-457,1998
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item QCD events, diffractive processes need to be switched on in order to fill the low multiplicity regions. The measurement was done in $\left|\eta\right| ~< ~3.25$ and was extrapolated to full phase space. However, the method of extrapolation remains unclear.\end{itemize}
-
-\noindent A measurement of the charged multiplicity distribution at \ensuremath{\sqrt{s}} = 1.8 TeV.
-
-\clearpage
-
-
\section{LHC analyses}\typeout{Handling analysis ATLAS_2010_S8591806}
\subsection[ATLAS\_2010\_S8591806]{ATLAS\_2010\_S8591806\,\cite{Aad:2010rd}}
\textbf{Charged particles at 900 GeV in ATLAS}\newline
@@ -1966,7 +1544,7 @@
\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.
+\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
@@ -1997,7 +1575,7 @@
\item * Single- and double-diffractive, plus non-diffractive inelastic, events.
\item $p\bar{p}$ 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.\end{itemize}
+ \item The trigger implementation 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 also for the combination of single- and double-diffractive events. The NSD distributions are further studied for certain ranges of the events charged multiplicity.
@@ -2006,35 +1584,6 @@
\clearpage
-\typeout{Handling analysis UA5_1988_S1867512}
-\subsection[UA5\_1988\_S1867512]{UA5\_1988\_S1867512\,\cite{Ansorge:1988fg}}
-\textbf{Charged particle correlations in ppbar non-single-diffractive events of the UA5 detector at \ensuremath{\sqrt{s}} = 200, 546 and 900 GeV.}\newline
-\textbf{Experiment:} UA5 (CERN SPS) \newline
-\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+1867512}{1867512}\newline
-\textbf{Status:} UNVALIDATED\newline
-\textbf{Authors:}
- \penalty 100
-\begin{itemize}
- \item Holger Schulz $\langle\,$\href{mailto:holger.schulz at physik.hu-berlin.de}{holger.schulz at physik.hu-berlin.de}$\,\rangle$;
-\end{itemize}
-\textbf{References:}
- \penalty 100
-\begin{itemize}
- \item Z.Phys.C37:191-213,1988
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item ppbar events. Non-single diffractive events need to be switched on. The trigger implementation is the same as in UA5_1989_S1926373.\end{itemize}
-
-\noindent Data on two-particle pseudorapidity and multiplicity correlations of charged particles for non single-diffractive $\bar{p}p$ collisions at c.m. energies of 200, 546 and 900 GeV. Pseudorapidity correlations interpreted in terms of a cluster model, which has been motivated by this and other experiments, require on average about two charged particles per cluster. The decay width of the clusters in pseudorapidity is approximately independent of multiplicity and of c.m. energy. The investigations of correlations in terms of pseudorapidity gaps confirm the picture of cluster production. The strength of forward-backward multiplicity correlations increases linearly with ins and depends strongly on position and size of the pseudorapidity gap separating the forward and backward interval. All our correlation studies can be understood in terms of a cluster model in which clusters contain on average about two charged particles, i.e. are of similar magnitude to earli
er estimates from the ISR.
-
-\clearpage
-
-
-\clearpage
-
\typeout{Handling analysis UA5_1989_S1926373}
\subsection[UA5\_1989\_S1926373]{UA5\_1989\_S1926373\,\cite{Ansorge:1988kn}}
\textbf{UA5 charged multiplicity measurements}\newline
@@ -2060,7 +1609,7 @@
\item Minimum bias events at \ensuremath{\sqrt{s}} = 200 and 900 GeV. Enable single and double diffractive events in addition to 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.
+\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
@@ -2095,36 +1644,6 @@
\clearpage
-\typeout{Handling analysis H1_1995_S3167097}
-\subsection[H1\_1995\_S3167097]{H1\_1995\_S3167097\,\cite{Aid:1995we}}
-\textbf{Transverse energy and forward jet production in the low-$x$ regime at H1}\newline
-\textbf{Experiment:} H1 (HERA Run I) \newline
-\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+3167097}{3167097}\newline
-\textbf{Status:} UNVALIDATED\newline
-\textbf{Authors:}
- \penalty 100
-\begin{itemize}
- \item Leif Lonnblad $\langle\,$\href{mailto:leif.lonnblad at thep.lu.se}{leif.lonnblad at thep.lu.se}$\,\rangle$;
-\end{itemize}
-\textbf{References:}
- \penalty 100
-\begin{itemize}
- \item Phys.Lett.B356:118,1995
- \item hep-ex/9506012
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item 820~GeV protons colliding with 26.7~GeV electrons. DIS events with an outgoing electron energy $> 12~\text{GeV}$. $5~\text{GeV}^2 < Q^2 < 100~\text{GeV}^2$, $10^{-4} < x < 10^{-2}$.\end{itemize}
-
-\noindent DIS events at low $x$ may be sensitive to new QCD dynamics such as BFKL or CCFM radiation. In particular, BFKL is expected to produce more radiation at high transverse energy in the rapidity span between the proton remnant and the struck quark jet. Performing a transverse energy sum in bins of $x$ and $\eta$ may distinguish between DGLAP and BFKL evolution.
-
-\clearpage
-
-
-\clearpage
-
\typeout{Handling analysis H1_2000_S4129130}
\subsection[H1\_2000\_S4129130]{H1\_2000\_S4129130\,\cite{Adloff:1999ws}}
\textbf{H1 energy flow in DIS}\newline
@@ -2147,44 +1666,13 @@
\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.
\clearpage
-\clearpage
-
-\typeout{Handling analysis ZEUS_2001_S4815815}
-\subsection[ZEUS\_2001\_S4815815]{ZEUS\_2001\_S4815815\,\cite{Chekanov:2001bw}}
-\textbf{Dijet photoproduction analysis}\newline
-\textbf{Experiment:} ZEUS (HERA Run I) \newline
-\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+4815815}{4815815}\newline
-\textbf{Status:} UNVALIDATED\newline
-\textbf{Authors:}
- \penalty 100
-\begin{itemize}
- \item Jon Butterworth $\langle\,$\href{mailto:jmb at hep.ucl.ac.uk}{jmb at hep.ucl.ac.uk}$\,\rangle$;
-\end{itemize}
-\textbf{References:}
- \penalty 100
-\begin{itemize}
- \item Eur.Phys.J.C23:615,2002
- \item DESY 01/220
- \item hep-ex/0112029
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item 820 GeV protons colliding with 27.5 GeV positrons; Direct and resolved photoproduction of dijets; Leading jet $\pT > 14$ GeV, second jet $\pT > 11$ GeV; Jet pseudorapidity $-1 < |\eta| < 2.4$\end{itemize}
-
-\noindent ZEUS photoproduction of jets from proton--positron collisions at beam energies of 820~GeV on 27.5~GeV. Photoproduction can either be direct, in which case the photon interacts directly with the parton, or resolved, in which case the photon acts as a source of quarks and gluons. A photon-proton centre of mass energy of between 134~GeV and 227~GeV is probed, with values of $x_P$, the fractional momentum of the partons inside the proton, predominantly in the region between 0.01 and 0.1. The fractional momentum of the partons from the photon, $x\gamma$, is in the region 0.1 to 1. Jets are reconstructed in the range $-1 < |\eta| < 2.4$ using the $k_\perp$ algorithm with an $R$ parameter of 1.0. The minimum \pT of the leading jet should be greater than 14~GeV, and at least one other jet must have $\pT > 11$~GeV.
-
-\clearpage
-
-
\section{RHIC analyses}\typeout{Handling analysis STAR_2006_S6500200}
\subsection[STAR\_2006\_S6500200]{STAR\_2006\_S6500200\,\cite{Adams:2006nd}}
\textbf{Identified hadron spectra in pp at 200 GeV}\newline
@@ -2209,7 +1697,7 @@
\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.
+\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.
\clearpage
@@ -2239,7 +1727,7 @@
\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.
+\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.
\clearpage
@@ -2269,93 +1757,12 @@
\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.
-
-\clearpage
-
-
-\clearpage
-
-\typeout{Handling analysis STAR_2008_S7993412}
-\subsection[STAR\_2008\_S7993412]{STAR\_2008\_S7993412\,\cite{Nattrass:2008tw}}
-\textbf{Di-hadron correlations in d-Au at 200 GeV}\newline
-\textbf{Experiment:} STAR (RHIC d-Au 200 GeV) \newline
-\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+7993412}{7993412}\newline
-\textbf{Status:} UNVALIDATED\newline
-\textbf{Authors:}
- \penalty 100
-\begin{itemize}
- \item Christine Nattrass $\langle\,$\href{mailto:christine.nattrass at yale.edu}{christine.nattrass at yale.edu}$\,\rangle$;
- \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth at cern.ch}{hendrik.hoeth at cern.ch}$\,\rangle$;
-\end{itemize}
-\textbf{References:}
- \penalty 100
-\begin{itemize}
- \item arXiv: \href{http://arxiv.org/abs/0809.5261}{0809.5261}
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item d-Au at 200 GeV (use pp Monte Carlo! See description)\end{itemize}
-
-\noindent Correlation in $\eta$ and $\phi$ between the charged hadron with the highest \pT (``trigger particle'') and the other charged hadrons in the event (``associated particles''). The data was collected in d-Au collisions at 200 GeV. Nevertheless, it is very proton-proton like and can therefore be compared to $pp$ Monte Carlo (not for tuning, but for qualitative studies.)
-
-\clearpage
-
-
-\clearpage
-
-\typeout{Handling analysis STAR_2009_UE_HELEN}
-\subsection{STAR\_2009\_UE\_HELEN}
-\textbf{UE measurement in pp at 200 GeV}\newline
-\textbf{Experiment:} STAR (RHIC pp 200 GeV) \newline
-\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+None}{None}\newline
-\textbf{Status:} VALIDATED -- but PRELIMINARY DATA!\newline
-\textbf{Authors:}
- \penalty 100
-\begin{itemize}
- \item Helen Caines $\langle\,$\href{mailto:helen.caines at yale.edu}{helen.caines at yale.edu}$\,\rangle$;
- \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth at cern.ch}{hendrik.hoeth at cern.ch}$\,\rangle$;
-\end{itemize}
-\textbf{References:}
- \penalty 100
-\begin{itemize}
- \item arXiv: \href{http://arxiv.org/abs/0910.5203}{0910.5203}
- \item arXiv: \href{http://arxiv.org/abs/0907.3460}{0907.3460}
- \item WARNING! Mark as "STAR preliminary" and contact authors when using it!
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item pp at 200 GeV\end{itemize}
-
-\noindent UE analysis similar to Rick Field's leading jet analysis. SIScone with radius/resolution parameter R=0.7 is used. Particles with $\pT > 0.2~\text{GeV}$ and $|\eta| < 1$ are included in the analysis. All particles are assumed to have zero mass. Only jets with neutral energy $< 0.7$ are included. For the transMIN and transMAX $\Delta(\phi)$ is between $\pi/3$ and $2\pi/3$, and $\Delta(\eta) < 2.0$. For the jet region the area of the jet is used for the normalization, i.e. the scaling factor is $\pi R^2$ and not $\mathrm{d}\phi\mathrm{d}\eta$ (this is different from what Rick Field does!). The tracking efficiency is $\sim 0.8$, but that is an approximation, as below $\pT \sim 0.6~\text{GeV}$ it is falling quite steeply.
-
-\clearpage
-
-
-\section{Monte Carlo analyses}\typeout{Handling analysis MC_DIJET}
-\subsection{MC\_DIJET}
-\textbf{Analysis of dijet events at the LHC.}\newline
-\textbf{Status:} UNVALIDATED\newline
-\textbf{No authors listed}\\
-\textbf{No references listed}\\
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item Generic QCD events at any energy.\end{itemize}
-
-\noindent Analysis of dijet events for the upcoming runs at the LHC, specifically studying azimuthal angle, transverse momentum distributions (including for leading jet and secondary jet), as well as charged particle multiplicities and transverse momenta.
+\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.
\clearpage
-\clearpage
-
-\typeout{Handling analysis MC_DIPHOTON}
+\section{Monte Carlo analyses}\typeout{Handling analysis MC_DIPHOTON}
\subsection{MC\_DIPHOTON}
\textbf{Monte Carlo validation observables for diphoton production at LHC}\newline
\textbf{Status:} VALIDATED\newline
@@ -2415,7 +1822,7 @@
\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.
@@ -2447,29 +1854,6 @@
\clearpage
-\typeout{Handling analysis MC_PHOTONJETUE}
-\subsection{MC\_PHOTONJETUE}
-\textbf{Study the usual underlying event observables in photon + jet events}\newline
-\textbf{Status:} UNVALIDATED\newline
-\textbf{Authors:}
- \penalty 100
-\begin{itemize}
- \item Andy Buckley $\langle\,$\href{mailto:andy.buckley at cern.ch}{andy.buckley at cern.ch}$\,\rangle$;
-\end{itemize}
-\textbf{No references listed}\\
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item Photon + jet events at any energy. \pT cutoff at 10 GeV advised.\end{itemize}
-
-\noindent Modification of the MC leading jets underlying event analysis to study the UE in hard photon+jet events. This may be of interest, because the leading QCD dipole structure is different from that in either dijet or Drell-Yan hard processes. Observables are also extended to include the variation of transverse activity as a function of jet-photon balance, and using the photon rather than the jet to define the event alignment.
-
-\clearpage
-
-
-\clearpage
-
\typeout{Handling analysis MC_SUSY}
\subsection{MC\_SUSY}
\textbf{Validate generic SUSY events, including various lepton invariant mass}\newline
@@ -2486,32 +1870,7 @@
\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.
-
-\clearpage
-
-
-\clearpage
-
-\typeout{Handling analysis MC_TTBAR}
-\subsection{MC\_TTBAR}
-\textbf{MC analysis for ttbar studies}\newline
-\textbf{Status:} UNVALIDATED\newline
-\textbf{Authors:}
- \penalty 100
-\begin{itemize}
- \item Holger Schulz $\langle\,$\href{mailto:hschulz at physik.hu-berlin.de}{hschulz at physik.hu-berlin.de}$\,\rangle$;
- \item Andy Buckley $\langle\,$\href{mailto:andy.buckley at cern.ch}{andy.buckley at cern.ch}$\,\rangle$;
-\end{itemize}
-\textbf{No references listed}\\
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item * For Pythia6, set MSEL=6.
- \item For Fortran Herwig/Jimmy select IPROC=1706.\end{itemize}
-
-\noindent This is a pure Monte Carlo study for t-tbar production.
+\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.
\clearpage
@@ -2534,7 +1893,7 @@
\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.
+\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.
\clearpage
@@ -2555,9 +1914,9 @@
\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.
+\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.
\clearpage
@@ -2605,7 +1964,7 @@
\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.
+\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.
\clearpage
@@ -2668,33 +2027,3 @@
\clearpage
-\clearpage
-
-\typeout{Handling analysis SFM_1984_S1178091}
-\subsection[SFM\_1984\_S1178091]{SFM\_1984\_S1178091\,\cite{Breakstone:1983ns}}
-\textbf{Charged multiplicity distribution in pp interactions at CERN ISR energies}\newline
-\textbf{Experiment:} SFM (CERN ISR) \newline
-\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+1178091}{1178091}\newline
-\textbf{Status:} UNVALIDATED\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 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 Phys.Rev.D30:528,1984
-\end{itemize}
-\textbf{Run details:}
- \penalty 100
-\begin{itemize}
-
- \item QCD events, double-diffractive events should be turned on as well.\end{itemize}
-
-\noindent Charged multiplicities are measured at \ensuremath{\sqrt{s}} = 30.4, 44.5, 52.2 and 62.2 GeV using a minimum-bias trigger. The data is sub-divided into inleastic as well as non-single-diffractive events. However, the implementation of the diffractive events will require some work.
-
-\clearpage
-
-
Modified: trunk/doc/mk-analysis-latex
==============================================================================
--- trunk/doc/mk-analysis-latex Mon Apr 5 20:07:44 2010 (r2389)
+++ trunk/doc/mk-analysis-latex Mon Apr 5 20:09:23 2010 (r2390)
@@ -238,5 +238,5 @@
f = open("%s.bib" % OUTNAME, "w")
#
bibentries = "\n\n".join(["%% %s\n%s" % (k,b) for k,b in bib.iteritems()])
-f.write(bibentries)
+f.write(bibentries + "\n")
f.close()
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