Resolution of Ground and Excited Electronic States within the Unitary Group Approach

Abstract

In this work ground and excited electronic states of Heisenberg cluster models, in the form of con- figuration interaction many-body wave functions, are characterized within the spin-adapted Graph- ical Unitary Group Approach framework, and relying on a novel combined unitary and symmetric group approach. Finite-size cluster models of well-defined point-group symmetry and of general local-spin Slocal ≥ 21 are presented, including J1–J2 triangular and tetrahedral clusters, which are often used to describe magnetic interactions in biological and bio-mimetic polynuclear transition metal clusters with unique catalytic activity, such as nitrogen fixation and photosynthesis. We show that a unique block-diagonal structure of the underlying Hamiltonian matrix in the spin-adapted basis emerges when an optimal lattice site ordering is chosen that reflects the internal symmetries of the model investigated. The block-diagonal structure is bound to the commutation relations between cumulative spin operators and the Hamiltonian operator, that in turn depend on the geometry of the cluster investigated. The many-body basis transformation, in the form of the orbital/site reorder- ing, exposes such commutation relations. These commutation relations represent a rigorous and formal demonstration of the block-diagonal structure in Hamiltonian matrices and the compression of the corresponding spin-adapted many-body wave functions. As a direct consequence of the block- diagonal structure of the Hamiltonian matrix it is possible to selectively optimize electronic excited states without the overhead of calculating the lower-energy states by simply relying on the initial ansatz for the targeted wave function. Additionally, more compact many-body wave functions are obtained. In extreme cases, electronic states are precisely described by a single configuration state function, despite the curse of dimensionality of the corresponding Hilbert space. These findings are crucial in the electronic structure theory framework, for they offer a conceptual route towards wave functions of reduced multi-reference character, that can be optimized more easily by approximated eigensolvers and are of more facile physical interpretation. They open the way to study larger ab initio and model Hamiltonians of increasingly larger number of correlated electrons, while keeping the computational costs at their lowest.

Thermally Stable Terbium(II) and Dysprosium(II) Bis-amidinate Complexes

“…Upon mixing all states under spin− orbit coupling (SOC), the ground pseudodoublet (which has a tunnel splitting of 0.00002 cm −1 at the CASSCF-SO level or 0.0002 cm −1 at the CASPT2-SO level, as Dy(II) is non-Kramers) is dominated by the first and second spin-free roots, meaning that it derives from the 7 H term. To interrogate the f−d coupling further, we project the total ab initio Hamiltonian onto a model space comprising of S 5d = 1/2, S 4f = 5/2, and L 4f = 5; we do so by projecting the L 4f = 5 (H) subspace from the spin-free CASSCF/CASPT2 Hamiltonians and thus removing the L 4f = 3 (F) content, 65 which is justified as the f−f interelectronic repulsion is greater than the f−d coupling here.…”