{
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  "authors": [
    {
      "raw_name": "Maria Vittoria Garzelli", 
      "affiliations": [
        {
          "country": "Hungary", 
          "value": "Institute of Physics and MTA-DE Particle Physics Research Group, University of Debrecen, H-4010 Debrecen P.O.Box 105, Hungary"
        }
      ], 
      "surname": "Garzelli", 
      "given_names": "Maria Vittoria", 
      "full_name": "Garzelli, Maria Vittoria"
    }, 
    {
      "raw_name": "Adam Kardos", 
      "affiliations": [
        {
          "country": "Hungary", 
          "value": "Institute of Physics and MTA-DE Particle Physics Research Group, University of Debrecen, H-4010 Debrecen P.O.Box 105, Hungary"
        }
      ], 
      "surname": "Kardos", 
      "given_names": "Adam", 
      "full_name": "Kardos, Adam"
    }, 
    {
      "raw_name": "Zolt\u00e1n Tr\u00f3cs\u00e1nyi", 
      "affiliations": [
        {
          "country": "Hungary", 
          "value": "Institute of Physics and MTA-DE Particle Physics Research Group, University of Debrecen, H-4010 Debrecen P.O.Box 105, Hungary"
        }
      ], 
      "surname": "Tr\u00f3cs\u00e1nyi", 
      "given_names": "Zolt\u00e1n", 
      "full_name": "Tr\u00f3cs\u00e1nyi, Zolt\u00e1n"
    }
  ], 
  "titles": [
    {
      "source": "Springer/SISSA", 
      "title": "Hadroproduction of W + W \u2212 b b \u00af $$ \\overline{\\mathrm{b}} $$ at NLO accuracy matched with shower Monte Carlo programs"
    }
  ], 
  "dois": [
    {
      "value": "10.1007/JHEP08(2014)069"
    }
  ], 
  "publication_info": [
    {
      "page_start": "069", 
      "material": "article", 
      "journal_title": "Journal of High Energy Physics", 
      "year": 2014
    }
  ], 
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  "acquisition_source": {
    "date": "2014-08-15T00:00:00", 
    "source": "Springer/SISSA", 
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    "submission_number": "6f57b39a4d2711e8b67702163e01809a"
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  "page_nr": [
    41
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  "license": [
    {
      "url": "http://creativecommons.org/licenses/by/4.0/", 
      "license": "CC-BY-4.0"
    }
  ], 
  "copyright": [
    {
      "statement": "The Author(s)"
    }
  ], 
  "control_number": "3664", 
  "record_creation_date": "2014-08-15T00:00:00", 
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  "arxiv_eprints": [
    {
      "categories": [
        "hep-ph"
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      "value": "1405.5859"
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  ], 
  "abstracts": [
    {
      "source": "Springer/SISSA", 
      "value": "We present the computation of the differential cross section for the process p p ( p \u00af $$ \\overline{p} $$ ) \u2192 (W + W \u2212 b b \u00af $$ \\overline{\\mathrm{b}} $$ \u2192) e + \u03bd e \u03bc \u2212 \u03bd \u00af $$ \\overline{\\nu} $$ \u03bc b b \u00af $$ \\overline{\\mathrm{b}} $$ + X at NLO QCD accuracy matched to Shower Monte Carlo (SMC) simulations using PowHel, on the basis of the interface between HELAC-NLO and POWHEG-BOX. We include all resonant and non-resonant contributions. This is achieved by fully taking into account the effect of off-shell t-quarks and off-shell W-bosons in the complex mass scheme. We also present a program called DECAYER that can be used to let the t-quarks present in the event files for p p ( p \u00af $$ \\overline{p} $$ ) \u2192 t t \u00af $$ \\overline{\\mathrm{t}} $$ X processes decay including both the finite width of the t-quarks and spin correlations. We present predictions for both the Tevatron and the LHC, with emphasis on differences emerging from three different W + W \u2212 b b \u00af $$ \\overline{\\mathrm{b}} $$ hadroproduction computations: (i) full implementation of the p p ( p \u00af $$ \\overline{p} $$ ) \u2192 W + W \u2212 b b \u00af $$ \\overline{\\mathrm{b}} $$ process, (ii) generating on-shell t-quarks pushed off-shell with a Breit-Wigner finite width and decayed by Decayer, and (iii) on-shell t-quark production followed by decay in the narrow width approximation, as described by the SMC."
    }
  ], 
  "imprints": [
    {
      "date": "2014-08-11", 
      "publisher": "Springer/SISSA"
    }
  ]
}