2001
DOI: 10.1007/s100520100604
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Hadronic final state predictions from CCFM: the hadron-level Monte Carlo generator Cascade

Abstract: We discuss a practical formulation of backward evolution for the CCFM small-x evolution equation and show results from its implementation in the new Monte Carlo event-generator Cascade.

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Cited by 241 publications
(363 citation statements)
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References 32 publications
(87 reference statements)
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“…In the present paper to analyze the recent H1 and ZEUS data [6][7][8][9] we use the so-called k T -factorization [11,12] (or semi-hard [13,14]) approach of QCD which has been applied earlier, in particular, in description of the charm and beauty production at HERA [15][16][17][18][19][20][21], Tevatron [22][23][24][25][26][27][28] and LEP2 [19,29,30] colliders. The k T -factorization approach is based on the Balitsky-Fadin-Kuraev-Lipatov (BFKL) [31] or Ciafaloni-Catani-Fiorani-Marchesini (CCFM) [32] gluon evolution which are valid at small x since here large logarithmic terms proportional to ln 1/x are summed up to all orders of perturbation theory (in the leading logarithmic approximation).…”
Section: Jhep08(2006)043mentioning
confidence: 99%
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“…In the present paper to analyze the recent H1 and ZEUS data [6][7][8][9] we use the so-called k T -factorization [11,12] (or semi-hard [13,14]) approach of QCD which has been applied earlier, in particular, in description of the charm and beauty production at HERA [15][16][17][18][19][20][21], Tevatron [22][23][24][25][26][27][28] and LEP2 [19,29,30] colliders. The k T -factorization approach is based on the Balitsky-Fadin-Kuraev-Lipatov (BFKL) [31] or Ciafaloni-Catani-Fiorani-Marchesini (CCFM) [32] gluon evolution which are valid at small x since here large logarithmic terms proportional to ln 1/x are summed up to all orders of perturbation theory (in the leading logarithmic approximation).…”
Section: Jhep08(2006)043mentioning
confidence: 99%
“…As it was noted already, some applications of the k T -factorization approach supplemented with the BFKL and CCFM evolution to the heavy (charm and beauty) quark production at high energies are widely discussed in the literature [15][16][17][18][19][20][21][22][23][24][25][26][27][28][29][30] (see also review [34,35]). It was shown [24][25][26][27][28] that the beauty cross section at Tevatron can be consistently described in the framework of this approach.…”
Section: Jhep08(2006)043mentioning
confidence: 99%
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