Lanthanide metal-organic frameworks (Ln-MOFs) have received mucha ttention owing to their structural tunability and widely photofunctional applications.H owever, successful examples of Ln-MOFs with well-defined photonic performances at micro-/nanometer size are still quite limited. Herein, self-assemblies of 1,3,5-benzenetricarboxylic acid (BTC) and lanthanide ions affordi sostructural crystalline Ln-MOFs.T b-BTC,E u@Tb-BTC,a nd Eu-BTC have 1D microrod morphologies,h igh photoluminescence (PL) quantum yields,a nd different emission colors (green, orange,a nd red). Spatially PL resolved spectra confirm that Ln-MOF microrods exhibit an optical waveguide effect with loww aveguide loss coefficient (0.012 % 0.033 dB mm À1 )d uring propagation. Furthermore,t hese microrods feature both linear and chiral polarized photoemission with high anisotropy.Lanthanide metal-organic frameworks (Ln-MOFs) have attracted great attention because of their unique crystal structures, [1] fascinating photophysical properties (such as sharp emission band and high quantum yields), coupled with potential applications in biomedical imaging, [2] anti-counterfeiting tags, [3] optical fiber lasers, [4] sensors, [5] and light emitting devices. [6] Owing to the forbidden f-f transitions, trivalent lanthanide cations usually have weak light absorption, [7] and thus make the direct lanthanide excitation inefficient. This problem can be possibly overcome in Ln-MOFs with the aid of organic sensitizer through the so-called antenna effect. [8] During the ligand-to-metal energy-transfer process,i ti so fs ignificance to select suitable organic linkers with high molar absorption coefficient and appropriate energy level in the target Ln-MOFs.In general, the photonic properties of molecular materials not only depend on intra/inter-molecular excited-state (exciton) processes (such as exciton generation, migration, conversion/transfer,r ecombination and dissociation), [9] but also on the shape,size and dimension of their solid-state structures that strongly influence the optical behaviors by reflecting, refracting,a nd diffracting. [10] During the past decade,o nedimensional (1D) nano-/micro-sized systems including wires, tubes,r ods and belts have captured broad attention because of their novel physical/chemical properties,a nd wide applications in nano-and microdevices. [11] Recently,t he use of nano-to micro-sized waveguides have attracted considerable interest for their possible application as basic components in optical communication systems. [12] Up to now,r esearch on waveguides has focused on inorganic semiconductors, [13] organic chromophores, [10,14] and polymers. [15] In theory,L n-MOFs can potentially serve as idealized models to develop new optical waveguide systems due to the following reasons: 1) the design of organic chromophores and different trivalent lanthanide cations can give rise to high emission quantum yields and tunable emission colors;2 )the well-organization and ordered assembly of ligands and lanthanide cations could decrease the ...