Abstract

Spin crossover in transition metal complexes can be studied in great detail with computational chemistry. Over the years, the understanding has grown that the relative stability of high-spin (HS) versus low-spin (LS) states is a subtle balance of many factors that all need to be taken into account for a reliable description. Among the different contributions, the zero-point energy (ZPE) and the entropy play key roles. These quantities are usually calculated assuming a harmonic oscillator model for the molecular vibrations. We investigated the impact of including anharmonic corrections on the ZPE and the entropy and indirectly on the critical temperature of spin crossover. As test systems, we used a set of ten Fe(II) complexes and one Fe(III) complex, covering different coordination modes (mono-, bi-, and tri-dentate ligands), decreasing coordination number upon spin crossover, coordination by second- and third-row atoms, and changes in the oxidation state. The results show that the anharmonicity has a measurable effect, but it is in general rather small, and tendencies are not easily recognized. As a conclusion, we put forward that for high precision results, one should be aware of the anharmonic effects, but as long as computational chemistry is still struggling with other larger factors like the influence of the environment and the accurate determination of the electronic energy difference between HS and LS, the anharmonicity of the vibrational modes is a minor concern.

Highlights

  • Transition metal systems in which the metal atom can display various spin states are the prototypical examples of spin crossover (SCO) materials

  • We investigated the impact of including anharmonic corrections on the zero-point energy (ZPE) and the entropy and indirectly on the critical temperature of spin crossover

  • The change in the ZPE upon the addition of the anharmonic effect was loosely related to the stiffness of the ligands coordinating the Fe ion

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Summary

Introduction

Transition metal systems in which the metal atom can display various spin states are the prototypical examples of spin crossover (SCO) materials. These systems can undergo a transition from a low-spin (LS) to a high-spin (HS) state upon a variation of temperature or pressure, or by irradiation with light, or application of magnetic fields. The discovery of spin transition controlled by light irradiation opened the possibility of exploring the use of these systems as optically-switchable devices. The so-called light-induced excited spin state trapping (LIESST) [3,4,5,6] effect allows the population at low temperatures of a metastable HS state by irradiating into the absorption bands of the LS state. In some systems, the process is reversible; irradiating the HS, the LS state is again populated

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