One-dimensional (1D) nanostructures based on molecular and polymeric materials are attracting significant research interest due to the many novel chemical, physical and electronic properties that may arise in highly anisotropic systems and the possibility for exploitation of such properties in a wide variety of applications. [1] In particular, the potential of semiconducting polymer nanowires and nanotubes has already been explored for initial demonstration of nanoelectronic and nanophotonic devices such as field effect transistors, [2] field emitters, [3] and sub-wavelength optically pumped lasers, [4] photodetectors [5] and electroluminescent diodes. [6] Successful realization of such devices will rely upon the ability to tune the opto-electronic characteristics of the constituent materials. For applications based on optical emission such as tagging, sensing, and electroluminescence, the ability to obtain pure emission colors will be essential, especially where multiplexing of optical signals, e.g., from distinct individual nanowire light sources, may be involved. However, it is difficult to achieve emission color purity in semiconducting polymers since their emission spectra have a large full-width-at-halfmaximum due to both inhomogeneous broadening and the presence of a vibronic progression. Emission color tuning in polymers has been addressed by the incorporation of luminescent chromophores such as fluorescent organic dyes, [7] phosphorescent metal complexes [8,9] and inorganic quantum dots.[10] These dopants "harvest" host matrix excitations by charge trapping and/or fluorescence resonance energy transfer processes, i.e., dipole-dipole coupling (Förster energy transfer) [11] and electron exchange (Dexter energy transfer), [12] allowing precise tuning of emission wavelength and color purity. The long-lived and near monochromatic emission of rare-earth ions, arising from weakly allowed f-f emissive transitions that are well shielded from the local environment by 5s 2 and 5p 6 electrons, has also made them attractive chromophores for such purposes.[13] While lanthanide ions are themselves insoluble in polymers, encapsulation of the ions with organic ligands as organo-lanthanide chelates allows incorporation within polymer hosts. These complexes may be designed to exploit the "antenna effect" to enhance the effective absorption cross sections of the lanthanide ions via the mechanism of ligand sensitization. [14] Ligand properties may be further tailored to ensure that a significant overlap between the host emission spectrum and the absorption spectrum of the ligands exists to permit efficient Förster energy transfer between host and dopants. [15] In this paper, we report the tuning of emission chromaticity in semiconducting polymer nanotubes by energy transfer from the host polymer to luminescent chromophore dopants. Poly(N-vinylcarbazole) (PVK), a blue emissive, hole conducting polymer was selected as the host matrix. This versatile polymeric semiconductor has been previously employed in applications ranging ...