Ground State and Optical Excitations in Compounds with Tetragonal CuF64- Units: Insight into KAlCuF6 and CuFAsF6.

It has been argued that AAlCuF6 (A = K, Cs) and CuFAsF6 are the only known crystals that exhibit compressed CuF64- units due to the Jahn-Teller effect. However, no grounds for this singular behavior have yet been reported. By means of first-principles calculations on such compounds and the isomorphous compounds involving Zn2+ ions instead of Cu2+, we prove that neither the ground state nor the equilibrium geometry of CuF64- complexes in KAlCuF6 and CuFAsF6 is the result of a Jahn-Teller effect. In contrast, it is shown that the internal electric field, ER(r), created by the rest of the lattice ions upon the localized electrons in the complex, plays an important role in understanding this matter as well as the d-d transitions of these two compounds. The energy of an optical transition is shown to involve two contributions: the intrinsic contribution derived for the isolated CuF64- unit at equilibrium and the extrinsic contribution coming from the ER(r) field. Aside from reproduction of the experimental d-d transitions observed for KAlCuF6, it is found that in CuFAsF6 the b1g(x2 - y2) → a1g(3z2 - r2) transition is not the lowest one due to the stronger effects from the internal field. Interestingly, the intrinsic contribution corresponding to that transition can simply be written as β(Req - Rax) where Req and Rax are the equatorial and axial Cu2+-F- distances and β = 2.7 eV/Å is the same for all systems involving tetragonal CuF64- units and an average metal-ligand distance close to 2.03 Å. This shows the existence of a common point shared by the Jahn-Teller system KZnF3:Cu2+ and other non-Jahn-Teller systems such as KAlCuF6, CuFAsF6, K2ZnF4:Cu2+, and Ba2ZnF6:Cu2+. Although most Jahn-Teller systems display an elongated geometry, there are however many Cu2+ compounds with a compressed geometry but hidden by an additional orthorhombic instability. The lack of that instability in KAlCuF6 and CuFAsF6 is also discussed.

[1]  J. A. Aramburu,et al.  Understanding the Structure and Ground State of the Prototype CuF2 Compound Not Due to the Jahn-Teller Effect. , 2019, Inorganic chemistry.

[2]  J. A. Aramburu,et al.  Insight into Compounds with Cu(H2O)62+ Units: New Ideas for Understanding Cu2+ in Tutton Salts , 2019, The Journal of Physical Chemistry C.

[3]  Jian Wang,et al.  Direct Observation of Cr3+ 3d States in Ruby: Toward Experimental Mechanistic Evidence of Metal Chemistry , 2018, The journal of physical chemistry. A.

[4]  J. A. Aramburu,et al.  Changing the Usual Interpretation of the Structure and Ground State of Cu2+-Layered Perovskites , 2018 .

[5]  J. A. Aramburu,et al.  Large Differences in the Optical Spectrum Associated with the Same Complex: The Effect of the Anisotropy of the Embedding Lattice. , 2017, Inorganic chemistry.

[6]  J. A. Aramburu,et al.  Jahn–Teller and Non-Jahn–Teller Systems Involving CuF64– Units: Role of the Internal Electric Field in Ba2ZnF6:Cu2+ and Other Insulating Systems , 2017 .

[7]  J. A. Aramburu,et al.  A Genuine Jahn-Teller System with Compressed Geometry and Quantum Effects Originating from Zero-Point Motion. , 2016, Chemphyschem : a European journal of chemical physics and physical chemistry.

[8]  J. A. Aramburu,et al.  Origin of the exotic blue color of copper-containing historical pigments. , 2015, Inorganic chemistry.

[9]  D. Khomskii Transition Metal Compounds , 2014 .

[10]  J. A. Aramburu,et al.  Electrostatic Control of Orbital Ordering in Noncubic Crystals , 2014 .

[11]  J. A. Aramburu,et al.  Origin of small barriers in Jahn-Teller systems: quantifying the role of 3d-4s hybridization in the model system NaCl:Ni+. , 2013, Inorganic chemistry.

[12]  J. A. Aramburu,et al.  Compounds Containing Tetragonal Cu2+ Complexes: Is the dx2–y2–d3z2–r2 Gap a Direct Reflection of the Distortion? , 2013 .

[13]  J. A. Aramburu,et al.  Cu2+ in layered compounds: origin of the compressed geometry in the model system K2ZnF4:Cu2+. , 2013, Inorganic chemistry.

[14]  J. A. Aramburu,et al.  Colour due to Cr3+ ions in oxides: a study of the model system MgO:Cr3+ , 2013, Journal of physics. Condensed matter : an Institute of Physics journal.

[15]  Thomas Bredow,et al.  Consistent Gaussian basis sets of triple‐zeta valence with polarization quality for solid‐state calculations , 2013, J. Comput. Chem..

[16]  Z. Mazej,et al.  Syntheses and Crystal Structures of [H3O]+/M2+ (M = Fe, Zn, Cu, Hg) Salts with [AsF6]– , 2012 .

[17]  D. Reinen The modulation of Jahn-Teller coupling by elastic and binding strain perturbations-a novel view on an old phenomenon and examples from solid-state chemistry. , 2012, Inorganic chemistry.

[18]  J. A. Aramburu,et al.  Spectrochemical series and the dependence of Racah and 10 Dq parameters on the metal-ligand distance: microscopic origin. , 2011, The journal of physical chemistry. A.

[19]  J. A. Aramburu,et al.  Jahn–Teller effect in Ag2+ doped KCl and NaCl: Is there any influence of the host lattice? , 2006 .

[20]  Z. Mazej,et al.  Compressed octahedral coordination in chain compounds containing divalent copper: structure and magnetic properties of CuFAsF6 and CsCuAlF6. , 2004, Chemistry.

[21]  F. Matthias Bickelhaupt,et al.  Chemistry with ADF , 2001, J. Comput. Chem..

[22]  A. Shengelaya,et al.  Low temperature ESR spectra of nickel — doped NaCl crystals , 1997 .

[23]  J. A. Aramburu,et al.  The dependence of 10Dq upon the metal–ligand distance, R, for transition‐metal complexes. What is its microscopic origin? , 1994 .

[24]  H. Bill,et al.  Electron paramagnetic resonance and relaxation study of copper (II) and silver (II) in CsCdF3 single crystals , 1993 .

[25]  R. Hoppe,et al.  The compressed tetragonal hexafluorocuprate(4-) (CuF64-) complex in potassium aluminum copper fluoride (KAlCuF6): an angular overlap treatment of the electronic structure and magnetic exchange coupling , 1993 .

[26]  A. Becke Density-functional thermochemistry. III. The role of exact exchange , 1993 .

[27]  K. Finnie,et al.  Spectroscopic verification of a tetragonal compression in an octahedral copper(II) compound , 1990 .

[28]  H. Gladney,et al.  Covalency and Electronic Structure of Cu2+ in ZnF2 by EPR , 1970 .

[29]  J. Sierro Paramagnetic resonance of the Ag2+ ion in irradiated alkali chlorides , 1966 .

[30]  W. Low,et al.  Jahn-teller effect of Ni1+ and Cu2+ in single crystals of calcium oxide☆ , 1963 .

[31]  S. Schweizer,et al.  Optical and magneto‐optical studies of Mn‐activated LiBaF3 , 2005 .

[32]  M. Riley Geometric and Electronic Information from the Spectroscopy of Six-Coordinate Copper(II) Compounds , 2001 .