“…[8] Such compounds are not only highly interesting from af undamental chemistry point of view,b ut their unique properties also make them valuable for industrial technologies.T hey are used, for example,incatalysis, [9] for fuel storage, [10,11] as semi-conductor materials, [12] in ferroelectrics, [13] as filtration or selection materials,i nb iomedical applications such as bioimaging and sensing, [14] biomimetic mineralisation, [15] or as drug delivery systems. [16,17] Thep otential field of application for efficient SQM methods is correspondingly large.However,universally applicable methods that are fully parameterised for transition metals are mostly limited to two method families,namely the already frequently used neglect of diatomic differential overlap (NDDO) based PMx (parametric method x)m ethods [4][5][6] and the recently introduced extended tight-binding methods GFNn-xTB, [1,2] (geometries,vibrational frequencies, and noncovalent interactions extended tight binding) from our laboratory.The robustness and quality of the GFNn-xTB methods has already been demonstrated in numerous applications with apredominant focus on organic chemistry.These applications include simulations of electron ionisation mass spectra, [18] fully automated computation of spin-spin-coupled nuclear resonance spectra, [19] including conformer-rotamer ensemble generation, atomic charge generation for the new D4 dispersion correction, [20,21] geometry optimisation of lanthanoid complexes, [22] automated determination of protonation sites, [23] pK a calculation in the SAMPL6 blind challenge, [24] metadynamics-based exploration of chemical compound conformation and reaction space, [25] and few studies on organometallic systems. [26] Thefocus here is on demonstrating the quality of GFN2-xTB and its precursor GFN1-xTB for the structure optimisation of transition-metal complexes and in particular of very large organometallic systems,w hich are to date not possible otherwise.T he recently published GFN2-xTB approach features less empiricism, improved electrostatic interactions (multipole terms up to atomic dipolequadrupole interactions), as well as adensity (atomic charge)dependent London dispersion energy correction [27,28] at even slightly ...…”