z-logo
open-access-imgOpen Access
Quantum dynamics simulations of the thermal and light-induced high-spin to low-spin relaxation in Fe(bpy)3 and Fe(mtz)6
Author(s) -
Marc AlíasRodríguez,
Miquel HuixRotllant,
Coen de Graaf
Publication year - 2022
Publication title -
faraday discussions
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.255
H-Index - 110
eISSN - 1364-5498
pISSN - 1359-6640
DOI - 10.1039/d2fd00027j
Subject(s) - spin crossover , population , chemistry , degenerate energy levels , spin states , atomic physics , relaxation (psychology) , fermi's golden rule , spin (aerodynamics) , condensed matter physics , thermal , molecular physics , physics , fermi gamma ray space telescope , quantum mechanics , thermodynamics , crystallography , psychology , social psychology , demography , sociology
First row transition metal complexes with d 4 o d 7 electronic configurations exhibit spin-crossover (SCO), which can be induced by external stimuli, such as temperature, pressure and light. The low-spin to high-spin transition has been widely studied, but very little is known about the reverse process. Here, we present a theoretical study of thermal and light-induced high-to-low spin crossover in prototypical Fe(II) complexes. The lifetime of the high-spin state in the thermal process is determined using Fermi's golden rule. With this methodology, we have accurately computed the transfer rate of the HS state thermal relaxation at several time scales (from sub-nanosecond to a few seconds) in two different iron complexes. The use of quasi-degenerate perturbation theory (QDPT2) in the analysis of the LS-HS spin-orbit coupling has allowed us to identify 3 T 1 as the main intermediate state coupling the LS and HS states. The light-induced process has been studied using wavepacket quantum dynamics along the main vibrational coordinates (one symmetric and two asymmetric Fe-N stretchings). The study suggests that after the initial excitation from the 5 T 2g o the 5 E g state, the population is transferred back to a vibrationally ho 5 T 2g state, from which a small amount of the population is transferred to the 1 A 1g state via he intermediate 3 T 1g . Most of the population remains trapped in the HS state at the time scale of the simulation.

The content you want is available to Zendy users.

Already have an account? Click here to sign in.
Having issues? You can contact us here
Accelerating Research

Address

John Eccles House
Robert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom