Abstract
The projection-based quantum embedding method is applied to a comprehensive set of electronic states. We embed different variants of equation-of-motion coupled-cluster singles and doubles (EOM-CCSD) theory in density functional theory and investigate electronically excited states of valence, Rydberg, and charge-transfer character, valence- and core-ionised states, as well as bound and temporary radical anions. The latter states, which are unstable towards electron loss, are treated by means of a complex-absorbing potential. Besides transition energies, we present Dyson orbitals and natural transition orbitals for embedded EOM-CCSD. We benchmark the performance of the embedded EOM-CCSD methods against full EOM-CCSD using small organic molecules microsolvated by a varying number of water molecules as test cases. Our results illustrate that embedded EOM-CCSD describes ionisation and valence excitation very well and that these transitions are quite insensitive towards technical details of the embedding procedure. On the contrary, more care is required when dealing with Rydberg excitations or electron attachment. For the latter type of transition in particular, the use of long-range corrected density functionals is mandatory and truncation of the virtual orbital space proves to be difficult.
GRAPHICAL ABSTRACT
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Acknowledgements
This article is dedicated to Professor John Stanton on the occasion of his 60th birthday. T.C.J. would like to thank him for many fruitful discussions and valuable support on different occasions. We thank Dr. Simon Bennie, Professor Basile Curchod, and Professor Fred Manby for sharing some of the raw data used for their work on embedded EOM-CCSD and Professor Anna Krylov for valuable feedback on the manuscript.
Disclosure statement
No potential conflict of interest was reported by the author(s).