Solid [CuI( piperazine) 0.5 ] ∞ , characterized by a structure with an infinite double chain of CuI, presents an unexpected dual luminescence. The short copper-copper distances allow the existence of both cluster-centered and 1-D delocalized electronic transitions, as emerged from theoretical calculations. Beyond the more common cluster-centered emission a higher energy band, which differs in lifetime and in temperature dependence, is observed.One of the most prominent classes of luminescent coordination compounds is that of copper(I) halides, due to their promising features for application in the field of optoelectronics. [1][2][3][4][5] They are easily synthesized 6,7 and tunable in emission color, [8][9][10] with high emission quantum yields in the solid state. 7,10,11 Copper(I) halide compounds can be considered as a valid alternative to luminescent metal complexes of precious (i.e. Ir or Os) and rare earth metals, which are expensive and environmentally problematic. 12 The luminescence properties of the copper halide clusters arise from a remarkable variety of emissive states, which have been extensively investigated in the last 30 years and can be summarized as follows: (a) a low-energy emission, attributed to a triplet cluster-centered ( 3 CC) excited state, is observed in the case of metal center interactions [13][14][15][16][17][18][19] and is independent of the nature of the ligand engaged in the complex; (b) a highenergy emission, attributed to a triplet halide-to-ligand charge transfer ( 3 XLCT) excited state, may show up in the presence of unsaturated ligands with accessible π-orbitals. 20 Moreover, recent studies have shown that several copper compounds present a thermally activated delayed fluorescence (TADF): Cu(I) halide-bridged compounds with P^N ligands are characterized by (metal + halide)-to-ligand charge transfer ((M + X) LCT) excited states where the low singlet-triplet energy gap allows emission from both the singlet and the triplet excited states, depending on the temperature. [21][22][23] The structure of [CuI( piperazine) 0.5 ] ∞ 24 is characterized by a one-dimensional copper iodide polymeric structure. The infinite double chain of CuI is described as castellated, 25 as shown in Fig. 1a, and the tetrahedral coordination of the copper(I) ions is fulfilled by the bridging piperazine to construct a 3D network (Fig. 1b and c). The inorganic chain is generated by the sequence of an inversion center and 2-fold axis symmetry elements, thus two different copper distances are present (2.771(1) Å and 2.729(1) Å). Although the presence of infinite double chain motifs has been observed in 20 struc-