Non-perturbative QCD effects and the top mass at the Tevatron

We present a new, universally applicable toy model of colour reconnections in hadronic final states. The model is based on hadronising strings and has one free parameter. We next present an implementation of this model in the PYTHIA event generator and provide several parameter sets (‘tunes’), constrained by fits to Tevatron minimum-bias data. Finally, we consider the sensitivity of a simplified top mass analysis to these effects, in exclusive semi-leptonic top events at the Tevatron. A first attempt at isolating the genuine non-perturbative effects gives an estimate of order δmtop ∼ ±0.5 GeV from non-perturbative uncertainties, and a further δmtop ∼ ±1 GeV from shower effects.

[1]  L. Lönnblad Reconnecting coloured dipoles , 1996 .

[2]  Torbjörn Sjöstrand,et al.  On colour rearrangement in hadronicW+W− evemts , 1993, hep-ph/9310242.

[3]  P. Zerwas,et al.  Jet final states in WW pair production and colour screening in the QCD vacuum , 1988 .

[4]  A. Schaelicke,et al.  Matching Parton Showers and Matrix Elements , 2006, hep-ph/0602031.

[5]  T. Sjostrand,et al.  QCD radiation off heavy particles , 2001 .

[6]  T. Sjöstrand Monte Carlo generators , 2006 .

[7]  P. Z. Skands,et al.  Baryon number violation and string topologies , 2003 .

[8]  M. Hauschild,et al.  Colour reconnection studies in e+e−→W+W− at √s=183 GeV , 1999 .

[9]  R. Field Jet Physics and the Underlying Event at the Tevatron , 2006 .

[10]  J. Häkkinen,et al.  Colour interference and confinement effects in W-pair production , 1994 .

[11]  E. al.,et al.  Measurement of the top quark mass in the lepton+jets channel using the Ideogram Method , 2007, hep-ex/0702018.

[12]  Determination of the jet energy scale at the collider detector at Fermilab , 2005, hep-ex/0510047.

[13]  Measurement of the top quark mass in the lepton+jets final state with the matrix element method , 2006, hep-ex/0609053.

[14]  G. P. Yeh,et al.  Top quark mass measurement using the template method in the lepton + jets channel at CDF II , 2006 .

[15]  P. Nason,et al.  Matching NLO QCD and parton showers in heavy flavour production , 2003, hep-ph/0305252.

[16]  A. Ribon,et al.  Charged jet evolution and the underlying event in proton-antiproton collisions at 1.8 TeV , 2002, Physical Review D.

[17]  B. Söderberg,et al.  A general model for jet fragmentation , 1983 .

[18]  Colour reconnection in e+e– → W+W–at $ {\sqrt s } $=180–209 GeV , 2005, hep-ex/0508062.

[19]  T. Sjöstrand,et al.  A multiple-interaction model for the event structure in hadron collisions. , 1987, Physical review. D, Particles and fields.

[20]  G. Gustafson Dual description of a confined colour field , 1986 .

[21]  A. Sherstnev,et al.  Standard Model Handles and Candles Working Group: Tools and Jets Summary Report , 2008, 0803.0678.

[22]  X. Artru Classical string phenomenology. How strings work , 1983 .

[23]  T. Sjostrand,et al.  Colour correlations and multiplicities in top events , 1994, hep-ph/9403394.

[24]  Test of colour reconnection models using three-jet events in hadronic Z decays , 2006, hep-ex/0604042.

[25]  R. Chierici,et al.  Precision Electroweak Measurements and Constraints on the Standard Model , 2007 .

[26]  G. Ingelman,et al.  Soft Colour Interactions as the Origin of Rapidity Gaps in DIS , 1995, hep-ph/9508386.

[27]  T. Sjöstrand,et al.  Parton fragmentation and string dynamics , 1983 .

[28]  J. Rathsman A generalised area law for hadronic string reinteractions 1 Work supported by the Swedish Natural Sc , 1998, hep-ph/9812423.

[29]  M. Sandhoff,et al.  Colour annealing - a toy model of colour reconnections , 2005 .

[30]  R. Field,et al.  Pythia Tune A, Herwig, and Jimmy in Run 2 at CDF , 2005, hep-ph/0510198.

[31]  G. Gustafson,et al.  Dipole formulation of QCD cascades , 1988 .

[32]  Lep collaborations,et al.  Precision Electroweak Measurements and Constraints on the Standard Model , 2007 .

[33]  P. Z. Skands,et al.  Transverse-momentum-ordered showers and interleaved multiple interactions , 2005 .

[34]  G. P. Yeh,et al.  Measurement of the top quark mass with the dynamical likelihood method using lepton plus jets events with b-tags in pp̄ collisions at s=1.96TeV , 2006 .

[35]  T. Sjostrand,et al.  Multiple interactions and the structure of beam remnants , 2004 .

[36]  A. De Roeck,et al.  Tevatron-for-LHC Report of the QCD Working Group , 2006 .

[37]  A. Hebecker,et al.  A parton model for diffractive processes in deep inelastic scattering , 1995, hep-ph/9504374.

[38]  Quarkonium production at the Fermilab Tevatron through soft color interactions , 1997, hep-ph/9705311.

[39]  Study of leading hadrons in gluon and quark fragmentation , 2006, hep-ex/0610031.

[40]  R. Field The Underlying event in hard scattering processes , 2002, hep-ph/0201192.

[41]  L. Fanò,et al.  The Underlying Event at the LHC , 2006 .

[42]  S. Mrenna,et al.  Pythia 6.3 physics and manual , 2003, hep-ph/0308153.

[43]  M. Mangano,et al.  TOOLS FOR THE SIMULATION OF HARD HADRONIC COLLISIONS , 2005 .

[44]  Peter Richardson,et al.  A simulation of QCD radiation in top quark decays , 2007 .

[45]  J. Butterworth,et al.  Multiparton Interactions in Photoproduction at HERA , 1996 .

[46]  Soft Color Interactions and Diffractive Hard Scattering at the Fermilab Tevatron , 2001, hep-ph/0106246.

[47]  M. Mangano,et al.  Matching matrix elements and shower evolution for top-pair production in hadronic collisions , 2006, hep-ph/0611129.