“…In this respect, an optimal mode of implementing it is building up the antenna and the emissive center into discrete molecules. ,,− This is advantageous because chemical synthesis and design allow incorporating a large variety of organic sensitizers, tuning the distances between energy donors and acceptors, incorporating other functional properties, or tailoring the molecular properties for their processability. In this regard, probing Ln-to-Ln′ (Ln ≠ Ln′) ET within molecules is not an easy task because it requires the preparation of pure heterometallic species with the different Ln metal ions positioned selectively at specific locations of the molecular architecture. , Since the 4f valence electrons of lanthanides are strongly shielded by 5p and 5s electrons, they exhibit very similar reactivity; therefore, site-selective heterometallic Ln molecules are generally obtained via sequential methodologies that are very tedious. , These include (i) step-by-step deprotection/opening of coordination sites, (ii) covalent linkage of different preformed coordination complexes, − (iii) sequential activation and complexation of coordination sites, − or (iv) enantiomeric self-recognition and mutual binding of chiral components . Some of the valuable molecules obtained in these manners have afforded the opportunity to study for the first time interesting intramolecular Ln-to-Ln′ ET phenomena, such as Tb-to-Yb, , Tb-to-Er, or Dy-to-Tb .…”