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  The effects of electronic correlations on the electron-phonon
  (el-ph) and on the electron-spin-fluctuation (el-sp) coupling are
  studied in a two-dimensional Hubbard model as a function of doping
  and temperature.  The el-ph and el-sp vertices, which enter the
  corresponding boson mediated pairing potentials and which influence
  much-discussed issues such as the ``kinks'' in photoemission
  spectra, are extracted on the basis of a numerically exact quantum
  Monte-Carlo (QMC) technique and complimented with a diagrammatic
  analysis.  Entering, in the case of the el-ph vertex, the physically
  relevant strong-correlation regime (U ≅ 8t), we find that the
  forward scattering process (i. e. for small phonon momenta q,
  ionic el-ph coupling) stops decreasing and begins to substantially
  increase as a function of U, leading to an effective el-ph
  coupling which is peaked in the forward direction. Whereas at weak
  and intermediate Coulomb interactions, screening is the dominant
  correlation effect suppressing the el-ph coupling, at larger U
  values irreducible vertex corrections become more important and give
  rise to this increase. These vertex corrections are shown to
  crucially depend on the renormalized electronic structure of the
  strongly correlated system. Our findings deviate from a Fermi-liquid
  description and, in contrast to approximate analytical (U = ∞)
  and slave-boson results are not connected to an incipient transition
  towards a charge instability or phase separation. Implications for
  the specific role of phonon modes, for the el-ph mediated d-wave
  pairing potential and ARPES selfenergy, and for the difference
  between transport and superconducting el-ph coupling constants are
  discussed.  With a similar QMC approach, we have studied
  whether the spin-fluctuation mediated pairing is suppressed by
  vertex corrections, as has previously been suggested by
  J. R. Schrieffer in the limit of large antiferromagnetic (AF)
  correction length ξ. There remains the crucial question of how
  large must ξ be for this effect to be substantial. We find that
  both the vertex and thus also the el-sp pairing potential are
  reduced already at very short ξs (of order Cu-Cu distance),
  namely as soon as the relevant electronic states form ``spin-bag''
  quasiparticles.
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