Unveiling the nature of the bosonic excitations that mediate the formation of Cooper pairs is a key issue for understanding unconventional superconductivity. A fundamental step toward this goal would be to identify the relative weight of the electronic and phononic contributions to the overall frequency (Ω) dependent bosonic function, Π(Ω). We perform optical spectroscopy on Bi2Sr2Ca0.92Y0.08Cu2O 8+δ crystals with simultaneous time-and frequency-resolution; this technique allows us to disentangle the electronic and phononic contributions by their different temporal evolution. The strength of the interaction (λ∼1.1) with the electronic excitations and their spectral distribution fully account for the high critical temperature of the superconducting phase transition. [7]. Inelastic neutron and X-ray scattering experiments found evidence for both QP-phonon anomalies [8] and bosonic excitations attributed to spin fluctuations [7,9] and loop currents [10]. Dip features in tunnelling experiments have been used to alternatively support the scenarios of dominant electron-phonon interactions [11] or antiferromagnetic spin fluctuations [12]. The frequency-dependent dissipation of the Drude optical conductivity, σ (ω), measured by equilibrium optical spectroscopies, has been interpreted [13][14][15] as the coupling of electrons to bosonic excitations, in which the separation of the phononic and electronic contributions is impeded by their partial coexistence on the same energy scale (<90 meV).We disentangle the electronic and phononic contributions to Π(Ω) through a non-equilibrium optical spectroscopy, in which the femtosecond time-resolution is combined with an energy-resolution smaller than 10 meV, over a wide photon energy range (0.5-2 eV). Our approach is based on the widely-used assumption [16,17] that, after the interaction between a superconductor and a short laser pulse (1.55 eV photon energy), the effective electronic temperature (T e ) relaxes toward its equilibrium value through energy exchange with the different degrees of freedom that linearly contribute to Π(Ω). In a more formal description, the total bosonic function is given by Π(Ω)=Π be (Ω)+Π SCP (Ω)+Π lat (Ω) where Π be refers to the bosonic excitations of electronic origin at the effective temperature T be , Π SCP to the small fraction of strongly-coupled phonons (SCPs) at T SCP [16] and Π lat to all other * Electronic address: s.f.p.dalconte@tue.nl † Electronic address: claudio.giannetti@unicatt.it