Considerable effort has been devoted to enabling all-optical signal processing (AOSP) for future communications systems with signifi cantly increased operational bandwidth. [ 1 ] Suitable materials for AOSP must exhibit ultrafast third-order nonlinear optical (NLO) response, as well as low linear and nonlinear optical loss, to achieve very high speed optical switching or modulation (100 Gbit/s or beyond). [ 1b ] While silicon is an attractive candidate material for AOSP due to its ease of chipscale photonic integration, its third-order NLO response is accompanied by parasitic non-linear absorption losses and longlived free carrier effects. [ 1c , 2 ] Recently, several groups have demonstrated silicon-organic hybrid (SOH) devices for AOSP with bandwidths exceeding 100 Gbit/s by integrating organic materials with silicon slot waveguides, [ 3 , 4 ] effectively combining the large non-linearities of organic materials with the extraordinary modal fi eld concentrations of silicon waveguides. Nonetheless, development of organic materials suitable for device integration which possess large non-linearities and small optical losses in the telecommunications region remains a challenge.Polymethine dyes [ 5 ] are an intriguing class of conjugated organic molecules for AOSP applications: the π -electrons along the conjugated backbone can be polarized easily, resulting in a large negative third-order molecular polarizability ( γ ) [ 6 ] and the electronic absorption bands are usually very narrow with sharp low energy band edges, which can be useful in reducing linear absorption losses at the desired operational wavelengths. Furthermore, polymethine dyes terminated with selenopyrylium end groups were recently found to exhibit large magnitudes of Re( γ ) at telecommunications wavelengths while also suppressing non-linear absorption such that excellent two-photon fi gures-of-merit (FOMs) (i.e., | Re( γ )/Im( γ ) | ) were achieved. [ 7 ] If the molecular third-order non-linearities of polymethine chromophores can be translated into macroscopic nonlinearities (e.g., χ (3) ) in high-number-density chromophoric materials, such materials could enable high-performance AOSP devices. However, there are several major challenges that need to be overcome in order to effectively translate the large γ into a large χ (3) . At high molecular number densities, the intrinsic optical properties of polymethine dyes can be deleteriously affected by intermolecular interactions resulting in, for example, aggregation [ 8 ] and ion-pairing effects, [ 9 ] both of which can lead to an increase in absorptive optical loss (linear and non-linear) at AOSP wavelengths. To mitigate the potential absorptive loss from these interactions, we have employed polymer guest-host approach to develop processable fi lms with high chromophore number density. However, with this approach, phase separation of polymethine salts in a host polymer can also lead to undesirable scattering and optical loss.Here, we report on the development of a miscible polymethine salt, polyme...