Using alkoxy-based side chains, PPV-derivatives such as poly [2-methoxy-5-(20-ethylhexyloxy)-p-phenylene vinylene] (MEH-PPV) [2] and later on the copolymer termed super-yellow PPV (SY-PPV, inset Figure 1d) [3] were synthesized. Amongst PPV-based PLEDs the SY-PPV LEDs reached the highest external quantum efficiencies (EQEs) of ≈4% [4,5] and a LT50 lifetime, meaning the time at which the light-output drops to half of its initial value at constant bias, of a few thousand hours at 1000 cd m −2 . Although SY-PPV PLEDs were commercialized in small displays of shavers and mobile phones by Philips, their efficiency and lifetime was too low in comparison to multilayer organic LEDs based on evaporated small molecules and the commercial application of PLEDs was discontinued. In spite of the lost industrial interest, MEH-PPV and later SY-PPV have been used as workhorse polymers by the academic community to further understand the electrical and optical characteristics of PLEDs. In the two decades after their discovery, the emphasis was mainly on understanding the charge transport and recombination processes. [6] It was found that the hole transport in PPV diodes is trap free and spacecharge limited. The charge-carrier mobility strongly depends on the amount of energetic disorder of hopping sites, which governs the electric-field and charge-carrier-density dependence of the mobility. In contrast to the hole transport, the electron transport is hindered by trapping. The resulting non-radiative recombination of trapped electrons with free holes is a significant loss process in PLEDs, especially at low voltages. For both trap-assisted and emissive bimolecular recombination, the rate coefficients are of the Langevin type, where the limiting step is the diffusion of electrons and holes toward each other under the influence of their mutual Coulombic interaction. The result is that when the electron-and hole mobility and electron trapping parameters are known, the bipolar PLED current and the voltage dependence of the efficiency can be predicted. [6] A typical example is shown in Figure 1 for a 100 nm-thick SY-PPV based PLED. The typical device architectures used for such studies are ITO/PEDOT/SY-PPV/Au for hole-only devices, Al/SY-PPV/Ba/Al for electron-only devices and ITO/PEDOT/ SY-PPV/Ba/Al for PLEDs, all on glass substrates. In Figure 1a the current density-voltage (J-V) characteristics of a SY-PPV hole-only device are plotted as a function of voltage for different temperatures (symbols). The lines are numerical simulations of a drift-diffusion model that includes a field-and density dependent mobility according to the extended GaussianThe various contributions to the external quantum efficiency (EQE) of polymer light-emitting diodes (PLEDs) are discussed. The EQE of an organic light-emitting diode is governed by a number of parameters, such as the electrical efficiency, the photoluminescence quantum yield (PLQY), the optical outcoupling efficiency and the spin statistics for singlet exciton generation. In the last decade, the e...