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[Rivet-svn] r2382 - in trunk: . docblackhole at projects.hepforge.org blackhole at projects.hepforge.orgMon Apr 5 13:09:06 BST 2010
Author: buckley Date: Mon Apr 5 13:09:06 2010 New Revision: 2382 Log: Oops, ChangeLog update from last commit Modified: trunk/ChangeLog trunk/doc/analyses.bib trunk/doc/analyses.tex Modified: trunk/ChangeLog ============================================================================== --- trunk/ChangeLog Mon Apr 5 13:08:36 2010 (r2381) +++ trunk/ChangeLog Mon Apr 5 13:09:06 2010 (r2382) @@ -1,3 +1,12 @@ +2010-04-05 Andy Buckley <andy at insectnation.org> + + * Updating metadata files to add Energies, Beams and PtCuts + entries to all of them. + + * Adding ToDo, NeedsCrossSection, and better treatment of Beams + and Energies entries in metadata files and in AnalysisInfo and + Analysis interfaces. + 2010-04-03 Andy Buckley <andy at insectnation.org> * Frank Siegert: Update of rivet-mkhtml to conform to improved Modified: trunk/doc/analyses.bib ============================================================================== --- trunk/doc/analyses.bib Mon Apr 5 13:08:36 2010 (r2381) +++ trunk/doc/analyses.bib Mon Apr 5 13:09:06 2010 (r2382) @@ -12,6 +12,23 @@ 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", @@ -62,6 +79,36 @@ 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", @@ -98,20 +145,18 @@ SLACcitation = "%%CITATION = 0907.4286;%%" } -% 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;%%" +% 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;%%" } % Affolder:2000ew @@ -177,22 +222,34 @@ SLACcitation = "%%CITATION = ZEPYA,C33,1;%%" } -% :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", +% 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", - primaryClass = "hep-ex", - doi = "", - SLACcitation = "%%CITATION = 0711.3717;%%" + 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;%%" } % Aaltonen:2009pc @@ -209,6 +266,20 @@ 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", @@ -240,6 +311,64 @@ 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 + at 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 + at 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", @@ -258,17 +387,18 @@ SLACcitation = "%%CITATION = 0804.1107;%%" } -% Abreu:1995qx - at 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;%%" +% 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 @@ -288,22 +418,22 @@ SLACcitation = "%%CITATION = HEP-EX/0512020;%%" } -% Aaltonen:2009ty - at Article{Aaltonen:2009ty, +% Aaltonen:2007ip + at Article{Aaltonen:2007ip, 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}", + 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 = "D80", - year = "2009", - pages = "111106", - eprint = "0910.3623", + volume = "D77", + year = "2008", + pages = "011108", + eprint = "0711.4044", archivePrefix = "arXiv", primaryClass = "hep-ex", - doi = "10.1103/PhysRevD.80.111106", - SLACcitation = "%%CITATION = 0910.3623;%%" + doi = "10.1103/PhysRevD.77.011108", + SLACcitation = "%%CITATION = 0711.4044;%%" } % Decamp:1991uz @@ -363,19 +493,6 @@ SLACcitation = "%%CITATION = NUPHA,B335,261;%%" } -% Collaboration:2010rd - at Article{Collaboration:2010rd, - author = "Collaboration, The ATLAS", - 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", - SLACcitation = "%%CITATION = 1003.3124;%%" -} - % Abelev:2006cs @Article{Abelev:2006cs, author = "Abelev, B. I. and others", @@ -392,6 +509,22 @@ 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", @@ -420,18 +553,18 @@ SLACcitation = "%%CITATION = 1002.4917;%%" } -% 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;%%" +% 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;%%" } % Acosta:2004wqa @@ -466,6 +599,23 @@ 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", @@ -501,6 +651,24 @@ SLACcitation = "%%CITATION = 0807.3367;%%" } +% 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", @@ -596,20 +764,38 @@ SLACcitation = "%%CITATION = ZEPYA,C69,365;%%" } -% Acosta:2005ix - at Article{Acosta:2005ix, - author = "Acosta, Darin E. and others", - collaboration = "CDF", - title = "{Study of jet shapes in inclusive jet production in - $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV}", +% Abulencia:2007ez + at Article{Abulencia:2007ez, + author = "Abulencia, A. and others", + collaboration = "CDF - Run II", + title = "{Measurement of the Inclusive Jet Cross Section using the + {\boldmath $k_{\rm T}$} algorithmin{\boldmath + $p\overline{p}$} Collisions at{\boldmath $\sqrt{s}$} = 1.96 + TeV with the CDF II Detector}", journal = "Phys. Rev.", - volume = "D71", - year = "2005", - pages = "112002", - eprint = "hep-ex/0505013", + volume = "D75", + year = "2007", + pages = "092006", + eprint = "hep-ex/0701051", + archivePrefix = "arXiv", + doi = "10.1103/PhysRevD.75.092006", + SLACcitation = "%%CITATION = HEP-EX/0701051;%%" +} + +% 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", - doi = "10.1103/PhysRevD.71.112002", - SLACcitation = "%%CITATION = HEP-EX/0505013;%%" + primaryClass = "nucl-ex", + doi = "10.1140/epjc/s10052-009-1037-8", + SLACcitation = "%%CITATION = 0809.5261;%%" } % Amsler:2008zzb @@ -689,18 +875,68 @@ SLACcitation = "%%CITATION = 0712.0803;%%" } -% Affolder:2001xt - at Article{Affolder:2001xt, - author = "Affolder, Anthony Allen and others", +% 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 = "{Charged jet evolution and the underlying event in - $p\bar{p}$ collisions at 1.8 TeV}", + 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 = "D65", - year = "2002", - pages = "092002", - doi = "10.1103/PhysRevD.65.092002", - SLACcitation = "%%CITATION = PHRVA,D65,092002;%%" + 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;%%" } % Abbiendi:2004qz @@ -736,22 +972,6 @@ SLACcitation = "%%CITATION = NUCL-EX/0601033;%%" } -% Affolder:1999ua - at Article{Affolder:1999ua, - author = "Affolder, Anthony Allen and others", - collaboration = "CDF", - title = "{A measurement of the differential dijet mass cross section - in $p\bar{p}$ collisions at $\sqrt{s} = 1.8$ TeV}", - journal = "Phys. Rev.", - volume = "D61", - year = "2000", - pages = "091101", - eprint = "hep-ex/9912022", - archivePrefix = "arXiv", - doi = "10.1103/PhysRevD.61.091101", - SLACcitation = "%%CITATION = HEP-EX/9912022;%%" -} - % Abazov:2004hm @Article{Abazov:2004hm, author = "Abazov, V. M. and others", @@ -769,35 +989,53 @@ SLACcitation = "%%CITATION = HEP-EX/0409040;%%" } -% 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;%%" +% 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;%%" } -% Acosta:2004sn - at Article{Acosta:2004sn, - author = "Acosta, Darin E. and others", - collaboration = "CDF", - title = "{Measurement of the cross section for prompt diphoton - production in $p\bar{p}$ collisions at $\sqrt{s} = 1.96$ - TeV}", +% :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 = "95", - year = "2005", - pages = "022003", - eprint = "hep-ex/0412050", + volume = "100", + year = "2008", + pages = "102001", + eprint = "0711.3717", archivePrefix = "arXiv", - doi = "10.1103/PhysRevLett.95.022003", - SLACcitation = "%%CITATION = HEP-EX/0412050;%%" + primaryClass = "hep-ex", + doi = "", + SLACcitation = "%%CITATION = 0711.3717;%%" +} + +% 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;%%" } % :2008hua @@ -850,6 +1088,20 @@ 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 @Article{Abazov:2001nta, author = "Abazov, V. M. and others", Modified: trunk/doc/analyses.tex ============================================================================== --- trunk/doc/analyses.tex Mon Apr 5 13:08:36 2010 (r2381) +++ trunk/doc/analyses.tex Mon Apr 5 13:09:06 2010 (r2382) @@ -13,7 +13,7 @@ \textbf{Hadronic Z decay charged multiplicity measurement}\newline \textbf{Experiment:} ALEPH (LEP 1) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+2435284}{2435284}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -42,7 +42,7 @@ \textbf{Measurement of the quark to photon fragmentation function}\newline \textbf{Experiment:} ALEPH (LEP Run 1) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+3196992}{3196992}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -72,7 +72,7 @@ \textbf{Studies of QCD with the ALEPH detector.}\newline \textbf{Experiment:} ALEPH (LEP 1) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+3486095}{3486095}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -101,7 +101,7 @@ \textbf{Jet rates and event shapes at LEP I and II}\newline \textbf{Experiment:} ALEPH (LEP Run 1 and 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+5765862}{5765862}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -132,7 +132,7 @@ \textbf{Strange baryon production in Z hadronic decays at Delphi}\newline \textbf{Experiment:} DELPHI (LEP 1) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+3137023}{3137023}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -161,7 +161,7 @@ \textbf{Delphi MC tuning on event shapes and identified particles.}\newline \textbf{Experiment:} DELPHI (LEP 1) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+3430090}{3430090}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -191,7 +191,7 @@ \subsection{DELPHI\_2002\_069\_CONF\_603} \textbf{Study of the b-quark fragmentation function at LEP 1}\newline \textbf{Experiment:} DELPHI (LEP 1) \newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -215,12 +215,40 @@ \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:} \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 \textbf{Experiment:} JADE_OPAL (PETRA and LEP) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+4300807}{4300807}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -250,7 +278,7 @@ \textbf{Measurements of flavor dependent fragmentation functions in $Z^0 \ensuremath{\to} q \bar{q}$ events}\newline \textbf{Experiment:} OPAL (LEP 1) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+3780481}{3780481}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -280,7 +308,7 @@ \textbf{Event shape distributions and moments in $e^+ e^-$ \ensuremath{\to} hadrons at 91--209 GeV}\newline \textbf{Experiment:} OPAL (LEP 1 \& 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+6132243}{6132243}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -308,7 +336,7 @@ \textbf{CDF transverse momentum distributions at 630 GeV and 1800 GeV.}\newline \textbf{Experiment:} CDF (Tevatron Run I) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+1865951}{1865951}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -339,7 +367,7 @@ \textbf{CDF pseudorapidity distributions at 630 and 1800 GeV}\newline \textbf{Experiment:} CDF (Tevatron Run 0) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+2089246}{2089246}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -364,12 +392,132 @@ \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:} \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:} \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:} \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:} \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, 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 \textbf{Experiment:} CDF (Tevatron Run 1) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+3418421}{3418421}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -395,12 +543,43 @@ \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:} \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 \textbf{Experiment:} CDF (Tevatron Run 1) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+3618439}{3618439}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -430,7 +609,7 @@ \textbf{Z \pT measurement in CDF Z \ensuremath{\to} $e^+e^-$ events}\newline \textbf{Experiment:} CDF (Tevatron Run 1) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+4155203}{4155203}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -458,11 +637,11 @@ \clearpage \typeout{Handling analysis CDF_2000_S4266730} -\subsection[CDF\_2000\_S4266730]{CDF\_2000\_S4266730\,\cite{Affolder:1999ua}} +\subsection{CDF\_2000\_S4266730} \textbf{Differential Dijet Mass Cross Section}\newline \textbf{Experiment:} CDF (Tevatron Run 1) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+4266730}{4266730}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -493,7 +672,7 @@ \textbf{Two jet triply-differential cross-section}\newline \textbf{Experiment:} CDF (Tevatron Run 1) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+4517016}{4517016}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -524,7 +703,7 @@ \textbf{Inclusive jet cross section}\newline \textbf{Experiment:} CDF (Tevatron Run 1) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+4563131}{4563131}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -555,7 +734,7 @@ \textbf{Field \& Stuart Run I underlying event analysis.}\newline \textbf{Experiment:} CDF (Tevatron Run 1) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+4751469}{4751469}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -585,7 +764,7 @@ \textbf{CDF Run 1 charged multiplicity measurement}\newline \textbf{Experiment:} CDF (Tevatron Run 1) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+4796047}{4796047}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -615,7 +794,7 @@ \textbf{Transverse cone and `Swiss cheese' underlying event studies}\newline \textbf{Experiment:} CDF (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+5839831}{5839831}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -643,11 +822,11 @@ \clearpage \typeout{Handling analysis CDF_2005_S6080774} -\subsection[CDF\_2005\_S6080774]{CDF\_2005\_S6080774\,\cite{Acosta:2004sn}} +\subsection{CDF\_2005\_S6080774} \textbf{Differential cross sections for prompt diphoton production}\newline \textbf{Experiment:} CDF (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+6080774}{6080774}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -674,11 +853,11 @@ \clearpage \typeout{Handling analysis CDF_2005_S6217184} -\subsection[CDF\_2005\_S6217184]{CDF\_2005\_S6217184\,\cite{Acosta:2005ix}} +\subsection{CDF\_2005\_S6217184} \textbf{CDF Run II jet shape analysis}\newline \textbf{Experiment:} CDF (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+6217184}{6217184}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -710,7 +889,7 @@ \textbf{Inclusive jet cross section differential in \pT}\newline \textbf{Experiment:} CDF (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+6450792}{6450792}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -736,12 +915,76 @@ \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:} \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 +\textbf{Experiment:} CDF (Tevatron Run 2) \newline +\textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+7057202}{7057202}\newline +\textbf{Status:} \newline +\textbf{Authors:} + \penalty 100 +\begin{itemize} + \item David Voong + \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.D75:092006,2007 + \item Erratum-ibid.D75:119901,2007 + \item FNAL-PUB 07/026-E + \item hep-ex/0701051 +\end{itemize} +\textbf{Run details:} + \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} + +\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 $1.6<|y|<2.1$. + +\clearpage + + +\clearpage + \typeout{Handling analysis CDF_2008_LEADINGJETS} \subsection{CDF\_2008\_LEADINGJETS} \textbf{CDF Run 2 underlying event in leading jet events}\newline \textbf{Experiment:} CDF (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+NONE}{NONE}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -766,7 +1009,7 @@ \textbf{CDF Run 2 underlying event in Drell-Yan}\newline \textbf{Experiment:} CDF (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+NONE}{NONE}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -798,7 +1041,7 @@ \textbf{Measurement of differential Z/$\gamma^*$ + jet + X cross sections}\newline \textbf{Experiment:} CDF (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+7540469}{7540469}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -823,12 +1066,74 @@ \clearpage +\typeout{Handling analysis CDF_2008_S7541902} +\subsection[CDF\_2008\_S7541902]{CDF\_2008\_S7541902\,\cite{Aaltonen:2007ip}} +\textbf{Jet \pT distributions for 4 jet multiplicity bins as well as the jet multiplicity distribution 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:} \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:} \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} + +\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. + +\clearpage + + +\clearpage + \typeout{Handling analysis CDF_2008_S7828950} \subsection[CDF\_2008\_S7828950]{CDF\_2008\_S7828950\,\cite{Aaltonen:2008eq}} \textbf{CDF Run II inclusive jet cross-section using the Midpoint algorithm}\newline \textbf{Experiment:} CDF (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+7828950}{7828950}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -859,7 +1164,7 @@ \textbf{Dijet mass spectrum}\newline \textbf{Experiment:} CDF (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+8093652}{8093652}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -883,12 +1188,41 @@ \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:} \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 \textbf{Experiment:} CDF (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+8233977}{8233977}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -920,7 +1254,7 @@ \textbf{Z rapidity measurement}\newline \textbf{Experiment:} CDF (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+8383952}{8383952}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -949,7 +1283,7 @@ \textbf{Measurement of the inclusive isolated prompt photon cross-section}\newline \textbf{Experiment:} CDF (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+8436959}{8436959}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -973,12 +1307,103 @@ \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:} \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:} \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. So far, this analysis is using the wrong jet algorithm, namely the D0 Run II Improved Legacy cone. + +\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:} \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 \textbf{Experiment:} D0 (Tevatron Run 1) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+4674421}{4674421}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -997,7 +1422,7 @@ \item W/Z events with decays to first generation leptons, in ppbar collisions at \ensuremath{\sqrt{s}} = 1800~GeV\end{itemize} -\noindent Measurement of differential W/Z boson cross section and ratio in p pbar collisions at center-of-mass energy \ensuremath{\sqrt{s}} = 1.8 TeV. The data cover electrons and neutrinos in a pseudo-rapidity range of -2.5 to 2.5. +\noindent Measurement of differential W/Z boson cross section and ratio in $p \bar{p}$ collisions at center-of-mass energy \ensuremath{\sqrt{s}} = 1.8 TeV. The data cover electrons and neutrinos in a pseudo-rapidity range of -2.5 to 2.5. \clearpage @@ -1009,7 +1434,7 @@ \textbf{Run II jet azimuthal decorrelation analysis}\newline \textbf{Experiment:} D0 (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+5992206}{5992206}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1039,7 +1464,7 @@ \textbf{Inclusive isolated photon cross-section, differential in \pT(gamma)}\newline \textbf{Experiment:} D0 (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+6438750}{6438750}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1059,7 +1484,7 @@ \item ppbar collisions at \ensuremath{\sqrt{s}} = 1960 GeV. Requires gamma + jet (q,qbar,g) hard processes, which for Pythia 6 means MSEL=10 for with MSUB indices 14, 18, 29, 114, 115 enabled.\end{itemize} -\noindent Measurement of differential cross section for inclusive production of isolated photons in p pbar collisions at \ensuremath{\sqrt{s}} = 1.96 TeV with the D0 detector at the Fermilab Tevatron collider. The photons span transverse momenta 23--300 GeV and have pseudorapidity $|\eta| < 0.9$. Isolated direct photons are probes of pQCD via the annihilation (q qbar \ensuremath{\to} gamma g) and quark-gluon Compton scattering (q g \ensuremath{\to} gamma q) processes, the latter of which is also sensitive to the gluon PDF. The initial state radiation / resummation formalisms are sensitive to the resulting photon \pT spectrum +\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 \clearpage @@ -1071,7 +1496,7 @@ \textbf{$Z/\gamma^* + X$ cross-section shape, differential in $y(Z)$}\newline \textbf{Experiment:} D0 (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+7075677}{7075677}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1103,7 +1528,7 @@ \textbf{Measurement of the ratio sigma($Z/\gamma^*$ + $n$ jets)/sigma($Z/\gamma^*$)}\newline \textbf{Experiment:} D0 (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+6879055}{6879055}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1121,7 +1546,7 @@ \item $p \bar{p} \to e^+ e^-$ + jets at 1960~GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $75 < m_{ee} < 105$ GeV.\end{itemize} -\noindent Cross sections as a function of \pT of the three leading jets and n-jet cross section ratios in ppbar collisions at $\sqrt{s}$ = 1.96 TeV, based on an integrated luminosity of $0.4~\text{fb}^{-1}$. +\noindent Cross sections as a function of \pT of the three leading jets and $n$-jet cross section ratios in $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96 TeV, based on an integrated luminosity of $0.4~\text{fb}^{-1}$. \clearpage @@ -1133,7 +1558,7 @@ \textbf{$Z/\gamma^* + X$ cross-section shape, differential in $\pT(Z)$}\newline \textbf{Experiment:} D0 (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+7554427}{7554427}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1149,10 +1574,10 @@ \penalty 100 \begin{itemize} - \item * $p \bar{p} o e^+ e^-$ + jets at 1960~GeV. + \item * $p \bar{p} \to e^+ e^-$ + jets at 1960~GeV. \item Needs mass cut on lepton pair to avoid photon singularity, looser than $40 < m_{ee} < 200$ GeV.\end{itemize} -\noindent Cross sections as a function of \pT of the vector boson inclusive and in forward region ($|y| > 2$, $\pT<30$ GeV) in $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96 TeV, based on an integrated luminosity of 0.98 fb$^{-1}$. +\noindent Cross sections as a function of \pT of the vector boson inclusive and in forward region ($|y| > 2$, $\pT<30$ GeV) in $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96 TeV, based on an integrated luminosity of 0.98~fb$^{-1}$. \clearpage @@ -1164,7 +1589,7 @@ \textbf{Measurement of D0 Run II differential jet cross sections}\newline \textbf{Experiment:} D0 (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+7662670}{7662670}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1184,7 +1609,7 @@ \item QCD events at \ensuremath{\sqrt{s}} = 1960 GeV. A \pTmin cut is probably necessary since the lowest jet \pT bin is at 50 GeV\end{itemize} -\noindent Measurement of the inclusive jet cross section in p pbar collisions at center-of-mass energy \ensuremath{\sqrt{s}} = 1.96 TeV. The data cover jet transverse momenta from 50--600 GeV and jet rapidities in the range -2.4 to 2.4. +\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. \clearpage @@ -1196,7 +1621,7 @@ \textbf{Isolated $\gamma$ + jet cross-sections, differential in \pT($\gamma$) for various $y$ bins}\newline \textbf{Experiment:} D0 (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+7719523}{7719523}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1214,9 +1639,9 @@ \penalty 100 \begin{itemize} - \item Produce only gamma + jet (q,qbar,g) hard processes (for Pythia 6, this means MSEL=10 and MSUB indices 14, 29 \& 115 enabled). The lowest bin edge is at 30 GeV, so a kinematic \pTmin cut is probably required to fill the histograms.\end{itemize} + \item Produce only gamma + jet ($q,\bar{q},g$) 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 pbar \ensuremath{\to} photon + jet + X as studied by the D0 detector at the Fermilab Tevatron collider at center-of-mass energy \ensuremath{\sqrt{s}} = 1.96 TeV. Photons are reconstructed in the central rapidity region $|y_\gamma| < 1.0$ with transverse momenta in the range 30--400 GeV, while jets are reconstructed in either the central $|y_jet| < 0.8$ or forward $1.5 < |y_\text{jet}| < 2.5$ rapidity intervals with $\pT^\text{jet} > 15~\text{GeV}$. The differential cross section $\mathrm{d}^3 \sigma / \mathrm{d}{\pT^\gamma} \mathrm{d}{y_\gamma} \mathrm{d}{y_\text{jet}}$ is measured as a function of $\pT^\gamma$ in four regions, differing by the relative orientations of the photon and the jet. MC predictions have trouble with simultaneously describing the measured normalization and $\pT^\gamma$ dependence of the cross section in any of the four measured regions. +\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. \clearpage @@ -1228,7 +1653,7 @@ \textbf{Measurement of W charge asymmetry from D0 Run II}\newline \textbf{Experiment:} D0 (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+7837160}{7837160}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1246,7 +1671,7 @@ \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} @@ -1262,7 +1687,7 @@ \textbf{Measurement of differential $Z/\gamma^*$ + jet + $X$ cross sections}\newline \textbf{Experiment:} D0 (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+7863608}{7863608}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1293,7 +1718,7 @@ \textbf{$Z/\gamma^*$ + jet + $X$ cross sections differential in \pT(jet 1,2,3)}\newline \textbf{Experiment:} D0 (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+8202443}{8202443}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1322,7 +1747,7 @@ \textbf{Dijet angular distributions}\newline \textbf{Experiment:} D0 (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+8320160}{8320160}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1351,7 +1776,7 @@ \textbf{Z+jets angular distributions}\newline \textbf{Experiment:} D0 (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+8349509}{8349509}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1380,7 +1805,7 @@ \textbf{Dijet invariant mass}\newline \textbf{Experiment:} D0 (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+8566488}{8566488}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1409,7 +1834,7 @@ \textbf{Direct photon pair production}\newline \textbf{Experiment:} CDF (Tevatron Run 2) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+8570965}{8570965}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1431,12 +1856,42 @@ \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:} \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{Collaboration:2010rd}} +\subsection[ATLAS\_2010\_S8591806]{ATLAS\_2010\_S8591806\,\cite{Aad:2010rd}} \textbf{Charged particles at 900 GeV in ATLAS}\newline \textbf{Experiment:} ATLAS (LHC 900GeV) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+8591806}{8591806}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1463,7 +1918,7 @@ \textbf{UA1 multiplicities, transverse momenta and transverse energy distributions.}\newline \textbf{Experiment:} UA1 (SPS) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+2044935}{2044935}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1493,7 +1948,7 @@ \textbf{UA5 multiplicity and pseudorapidity distributions for $pp$ and $p\bar{p}$.}\newline \textbf{Experiment:} UA5 (SPS) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+875503}{875503}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1523,7 +1978,7 @@ \textbf{Pseudorapidity distributions in $p\bar{p}$ (NSD, NSD+SD) events at \ensuremath{\sqrt{s}} = 200 and 900 GeV}\newline \textbf{Experiment:} UA5 (CERN SPS) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+1583476}{1583476}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1551,12 +2006,41 @@ \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:} \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 \textbf{Experiment:} UA5 (CERN SPS) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+1926373}{1926373}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1586,7 +2070,7 @@ \textbf{H1 energy flow and charged particle spectra in DIS}\newline \textbf{Experiment:} H1 (HERA) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+2919893}{2919893}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1611,12 +2095,42 @@ \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:} \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 \textbf{Experiment:} H1 (HERA) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+4129130}{4129130}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1640,12 +2154,43 @@ \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:} \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 xP, 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 kT algorithm with an R parameter of 1.0. The minimum \pT of the leading jet should be greater then 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 \textbf{Experiment:} STAR (RHIC pp 200 GeV) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+6500200}{6500200}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1676,7 +2221,7 @@ \textbf{Strange particle production 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+6860818}{6860818}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1706,7 +2251,7 @@ \textbf{Inclusive jet cross-section 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+6870392}{6870392}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1729,10 +2274,91 @@ \clearpage -\section{Monte Carlo analyses}\typeout{Handling analysis MC_DIPHOTON} +\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:} \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:} \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:} \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. + +\clearpage + + +\clearpage + +\typeout{Handling analysis MC_DIPHOTON} \subsection{MC\_DIPHOTON} \textbf{Monte Carlo validation observables for diphoton production at LHC}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1755,7 +2381,7 @@ \typeout{Handling analysis MC_JETS} \subsection{MC\_JETS} \textbf{Monte Carlo validation observables for jet production}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1778,7 +2404,7 @@ \typeout{Handling analysis MC_LEADINGJETS} \subsection{MC\_LEADINGJETS} \textbf{Underlying event in leading jet events, extended to LHC}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1801,7 +2427,7 @@ \typeout{Handling analysis MC_PHOTONJETS} \subsection{MC\_PHOTONJETS} \textbf{Monte Carlo validation observables for photon + jets production}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1821,10 +2447,33 @@ \clearpage +\typeout{Handling analysis MC_PHOTONJETUE} +\subsection{MC\_PHOTONJETUE} +\textbf{Study the usual underlying event observables in photon + jet events}\newline +\textbf{Status:} \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 -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1844,10 +2493,35 @@ \clearpage +\typeout{Handling analysis MC_TTBAR} +\subsection{MC\_TTBAR} +\textbf{MC analysis for ttbar studies}\newline +\textbf{Status:} \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. + +\clearpage + + +\clearpage + \typeout{Handling analysis MC_WJETS} \subsection{MC\_WJETS} \textbf{Monte Carlo validation observables for $W[e \, \nu]$ + jets production}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1870,7 +2544,7 @@ \typeout{Handling analysis MC_ZJETS} \subsection{MC\_ZJETS} \textbf{Monte Carlo validation observables for $Z[e^+ \, e^-]$ + jets production}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1891,7 +2565,7 @@ \section{Example analyses}\typeout{Handling analysis EXAMPLE} \subsection{EXAMPLE} \textbf{A demo to show aspects of writing a Rivet analysis}\newline -\textbf{Status:} EXAMPLE\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1912,7 +2586,7 @@ \section{Misc. analyses}\typeout{Handling analysis BELLE_2006_S6265367} \subsection{BELLE\_2006\_S6265367} \textbf{Charm hadrons from fragmentation and B decays on the $\Upsilon(4S)$}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1943,7 +2617,7 @@ \textbf{Hadron multiplicities in hadronic $e^+e^-$ events}\newline \textbf{Experiment:} PDG (Various) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+7857373}{7857373}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1972,7 +2646,7 @@ \textbf{Ratios (w.r.t. $\pi^+/\pi^-$) of hadron multiplicities in hadronic $e^+e^-$ events}\newline \textbf{Experiment:} PDG (Various) \newline \textbf{Spires ID:} \href{http://www.slac.stanford.edu/spires/find/hep/www?rawcmd=key+7857373}{7857373}\newline -\textbf{Status:} VALIDATED\newline +\textbf{Status:} \newline \textbf{Authors:} \penalty 100 \begin{itemize} @@ -1994,3 +2668,33 @@ \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:} \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 + +
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