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Actinide +IV complexes with six nitrates [AnIV(NO3)6]2− (An = Th, U, Np, and Pu) have been studied by 15N and 17O NMR spectroscopy in solution and first-principles calculations. Magnetic susceptibilities were evaluated experimentally using the Evans method and are in good agreement with the ab initio values. The evolution in the series of the crystal field parameters deduced from ab initio calculations is discussed. The NMR paramagnetic shifts are analyzed based on ab initio calculations. Because the cubic symmetry of the complex quenches the dipolar contribution, they are only of Fermi contact origin. They are evaluated from first-principles based on a complete active space/density functional theory (DFT) strategy, in good accordance with the experimental one. The ligand hyperfine coupling constants are deduced from paramagnetic shifts and calculated using unrestricted DFT. The latter are decomposed in terms of the contribution of molecular orbitals. It highlights two pathways for the delocalization of the spin density from the metallic open-shell 5f orbitals to the NMR active nuclei, either through the valence 5f hybridized with 6d to the valence 2p molecular orbitals of the ligands, or by spin polarization of the metallic 6p orbitals which interact with the 2s-based molecular orbitals of the ligands.
We study the random transverse field Ising model on a finite Cayley tree. This enables us to probe key questions arising in other important disordered quantum systems, in particular the Anderson transition and the problem of dirty bosons on the Cayley tree, or the emergence of non-ergodic properties in such systems. We numerically investigate this problem building on the cavity mean-field method complemented by state-of-the art finite-size scaling analysis. Our numerics agree very well with analytical results based on an analogy with the traveling wave problem of a branching random walk in the presence of an absorbing wall. Critical properties and finite-size corrections for the zero-temperature paramagnetic-ferromagnetic transition are studied both for constant and algebraically vanishing boundary conditions. In the later case, we reveal a regime which is reminiscent of the non-ergodic delocalized phase observed in other systems, thus shedding some light on critical issues in the context of disordered quantum systems, such as Anderson transitions, the many-body localization or disordered bosons in infinite dimensions.
This work addresses a class of conjugated hydrocarbons that are expected to be singlet diradicals according to the topological Hückel Hamiltonian while possibly satisfying full on-bond electron pairing. These systems possess two degenerate singly occupied molecular orbitals (SOMOs), but aromaticity brought by properly positioned six-membered rings does prevent Jahn–Teller distortions. Density functional theory (DFT) calculations performed on two emblematic examples confirm the strong bond-length alternation in the closed-shell solutions and the clear spatial symmetry in the open-shell spin-unrestricted determinants, the latter solution always being found to have significantly lower energy. Since the SOMOs are here of different symmetry, the wave function is free from ionic valence-bond component, and spin decontamination of the unrestricted DFT solutions and wave function calculations at the CASSCF-plus-second-order-perturbation level confirm the expected pure diradical character of such molecules. In contrast to disjoint diradicals, the SOMOs of present systems have large amplitudes on neighbor atoms, and we propose to name them entangled pure diradicals, further providing some prescription rules for their design. Additional calculations point out the qualitative contrast between these molecules and the related diradicaloids.
A complete theoretical analysis using first the simple Hückel model followed by more sophisticated multi-reference calculations on a trinuclear Ni(II) complex (Tp#Ni3HHTP), bearing the non-innocent bridging ligand HHTP3−, is carried out. The three semiquinone moieties of HHTP3− couple antiferromagnetically and lead to a single unpaired electron localized on one of the moieties. The calculated exchange coupling integrals together with the zero-field parameters allow, when varied within a certain range, reproducing the experimental data. These results are generalized for two similar other trinuclear complexes containing Ni(II) and Cu(II). The electronic structure of HHTP3− turns out to be independent of both the chemical nature and the geometry of the metal ions. We also establish a direct correlation between the geometrical and the electronic structures of the non-innocent ligand that is consistent with the results of calculations. It allows experimentalists to get insight into the magnetic behavior of this type of complexes by an analysis of their X-ray structure.
In the quest of new exotic phases of matter due to the interplay of various interactions, iridates hosting a spin-orbit entangled $j_{\mathrm{eff}}=1/2$ ground state have been in the spotlight in recent years. Also in view of parallels with the low-energy physics of high-temperature superconducting cuprates, the validity of a single- or few-band picture in terms of the $j_{\mathrm{eff}}$ states is key. However, in particular for its structurally simple member Ba$_2$IrO$_4$, such a systematic construction and subsequent analysis of minimal low-energy models are still missing. Here we show by means of a combination of different ab initio techniques with dynamical mean-field theory that a three-band model in terms of Ir-$j_{\mathrm{eff}}$ states fully retains the low-energy physics of the system as compared to a full Ir-$5d$ model. Providing a detailed study of the three-band model in terms of spin-orbit coupling, Hund's coupling and Coulomb interactions, we map out a rich phase diagram and identify a region of effective one-band metal-insulator transition relevant to Ba$_2$IrO$_4$. Compared to available angle-resolved photoemission spectra, we find good agreement of salient aspects of the calculated spectral function and identify features which require the inclusion of non-local fluctuations. In a broader context, we envisage the three- and five-band models developed in this study to be relevant for the study of doped Ba$_2$IrO$_4$ and to clarify further the similarities and differences with cuprates.
Subjets
Model Hamiltonian derivation
First-order spin–orbit coupling
Model Hamiltonians
Anderson mechanism
Magnetism
Heavy fermions
Cooperative effect
Spin-orbit coupling
Déplacements chimiques paramagnétiques
MOLCAS calculations
Binuclear compounds
Electron paramagnetic resonance
Crystal-field theory and spin Hamiltonians
Electronic correlation
Bleaney's model
MECHANISM
Exchange and superexchange interactions
Magnetic anisotropy
Ionic liquid
Magnetic properties
Covalency
Heptacoordination
Manganites
Excitation energies
Crystal field parameters
Calculs ab initio relativistes et corrélés
Iridate
Density functional theory
Lanthanide
Coupled cluster calculations
Ab initio calculations
Relativistic corrections
MOLECULAR MAGNETIC-MATERIALS
Hyperfine coupling
Metal-insulator transition
Ground states
Effective Hamiltonian theory
Electron paramagnetism
DOTA ligand
Ligand-field theory
Hamiltonien modèle
Lanthanides
Bleaney's theory
Spin-orbit interactions
Dynamical mean field theory
Modeling
Basis sets
Crystal field theory
Dynamical mean-field theory
Décontamination de spin
Divalent cobalt
Finite nucleus effects
Model hamiltonian
Electron spin
Exact diagonalization
Free radicals
Magnétisme moléculaire
Correlated relativistic ab initio calculations
Complexes de métaux de transition
Anisotropy
Dzyaloshinskii-Moriya interaction
Calcul ab initio
Perturbation theory
Anisotropie magnétique
Magnetism in organic systems
Hyperfine structure
MACROCYCLIC POLYARYLMETHYL POLYRADICALS
Electronic structure
Double exchange model
Iodine
FOS Physical sciences
Actinide
NMR
Diagonalisations exactes
Iridates
Magnétisme dans les systèmes organiques
Luminescence
Magnetic Susceptibility
CLUSTERS
Actinides
Dzyaloshinskii–Moriya interaction
Isotropic and anisotropic exchange
AB-INITIO
Magneto-resistive effects
Calculs ab initio
Determinants
Ab initio calculation
Modèle de Bleaney
Effets magnéto-résistifs
Imidazolium salt
Disordered Systems and Neural Networks cond-matdis-nn
Electron g-factor
Configuration interaction
Wave functions
Magnetic susceptibility
Excited states
HIGH-SPIN
Configuration interactions
High pressure
Bleaney