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<item>
  <id>01506732</id>
  <dt>j</dt>
  <an>01506732</an>
  <augroup>
    <au>Jadach, S.</au>
    <au>Ward, B.F.L.</au>
    <au>W\c{a}s, Z.</au>
  </augroup>
  <ti>The precision Monte Carlo event generator ${\cal{KK}}$ for two-fermion final states in $e^+ e^-$ collisions.</ti>
  <so>Comput. Phys. Commun. 130, No.3, 260-325 (2000).</so>
  <py>2000</py>
  <pu>Elsevier Science B.V. (North-Holland), Amsterdam</pu>
  <lagroup>
    <la>EN</la>
  </lagroup>
  <ccgroup>
  </ccgroup>
  <utgroup>
    <ut>coherent exclusive exponentiation</ut>
    <ut>electroweak corrections</ut>
    <ut>Yennie-Frautschi-Suura exponentiation</ut>
    <ut>parton shower model</ut>
    <ut>spin polarization effects</ut>
  </utgroup>
  <cigroup>
  </cigroup>
  <ligroup>
    <li>doi:10.1016/S0010-4655(00)00048-5</li>
  </ligroup>
  <abgroup>
    <ab>Summary: We present the Monte Carlo event generator ${\cal K}{\cal K}$ version 4.13 for precision predictions of the electroweak standard model for the process $e^+ e^-\to f\overline f+ n\gamma$, $f= \mu,\tau,d,u,s,c,b$, at centre-of-mass energies from $\tau$ lepton threshold to 1 TeV, that is for LEP, SLC, future linear colliders, $b$, $c$, $\tau$-factories, etc. Effects due to photon emission from initial beams and outgoing fermions are calculated in QED up to second-order, including all interference effects, within Coherent Exclusive Exponentiation (CEEX), which is based on Yennie-Frautschi-Suura exponentiation. Electroweak corrections are included in first order, with higher-order extensions, using the DIZET 6.21 library. Final-state quarks hadronize according to the parton shower model using JETSET. Beams can be polarized longitudinally and transversely. Decay of the $\tau$ leptons is simulated using the TAUOLA library, taking into account spin polarization effects as well. In particular the complete spin correlations density matrix of the initial-state beams and final state $\tau$'s is incorporated in an exact manner. Effects due to beamstrahlung are simulated in a realistic way. The main improvements with respect to KORALZ are: (a) inclusion of the initial-final state QED interference, (b) inclusion of the exact matrix element for two photons, and (c) inclusion of the transverse spin correlations in $\tau$ decays (as in KORALB).</ab>
    <rv></rv>
  </abgroup>
</item>