Exploring Chemistry Through the Source Function for the Electron and the Electron Spin Densities

Author(s):  
Carlo Gatti ◽  
Ahmed M. Orlando ◽  
Emanuele Monza ◽  
Leonardo Lo Presti
1981 ◽  
Vol 8 (4-6) ◽  
pp. 463-469 ◽  
Author(s):  
Toshimitsu Yamazaki
Keyword(s):  

2019 ◽  
Vol 966 ◽  
pp. 494-500
Author(s):  
Siti Nur Afifi Ahmad ◽  
Shukri Sulaiman ◽  
Lee Sin Ang ◽  
Isao Watanabe

The effects of polarization function on the spin contamination and distribution in β'-Me4P[Pd(dmit)2]2 were studied using the DFT cluster method. Two basis sets, SV and SVP were considered in the calculations, where B3LYP functional was employed in the doublet state of the one-fragment and dimer clusters. The values of <S2> before annihilation for both SV and SVP basis sets are excellent and very close to the perfect theoretical eigenvalue of 0.75. The values of the spin densities at thiolate and thione calculated using SVP were found to be smaller than the ones using SV. The difference, however, is less than eight percent. In contrast, the difference in the spin density at Pd atoms in both monomers is significantly larger for the SVP, being about 21%. The inclusion of polarization function resulted in the shifting of electron density from the sulfur atoms to the central Pd atoms. The calculated spin densities revealed the inhomogeneous distribution of the electron spin in the dimer that leads to the existence of electron-rich and electron-poor regions.


2014 ◽  
Vol 70 (a1) ◽  
pp. C281-C281 ◽  
Author(s):  
Carlo Gatti ◽  
Ahmed Orlando ◽  
Leonardo Lo Presti

The Source Function (SF) [1-3], enables one to view chemical bonding and other chemical paradigms from a new perspective and using only information from the electron density observable and its derivatives. We show how this tool may be straightforwardly applied to another important observable, the electron spin density, which analogously to the electron density may be locally interpreted in terms of a cause-effect relationship of contributions from the atoms of a molecular or crystalline system. Application of the spin density SF to molecules in vacuo and to slab or crystals, is made possible through an extension (SPINSF code) of our electron density SF code for molecules and through a progress-version of the TOPOND code, respectively. The latter has now been fully integrated in the CRYSTAL-14 code, where it provides, via the keyword TOPO of the properties section of CRYSTAL-14, a complete charge density topological analysis according to the Quantum Theory of Atoms in Molecules. Analysis of the SF for the electron spin density implies the study of its Laplacian scalar field, which may be locally positive or negative even if the two composing densities, ρα and ρβ, have both negative or positive Laplacian densities. When the latter bear the same sign, that of the spin density Laplacian depends on their relative magnitudes, that is on the relative concentration or dilution of ρα and ρβ. Hence, in general, the local source for the spin density, LSs, greatly differs from the analogous function for the density, leading to large differences in their integrated atomic SF contributions. The combined study of LSs and of the spin density neatly reveals which are the molecular or crystal regions that are "ferromagnetically" or "antiferromagnetically" coupled and the local strength of such coupling. Applications to crystals of metal-complexes where the ligands play an innocent or a non-innocent role and to crystals of iron spin-crossover complexes are discussed.


1999 ◽  
Vol 103 (1-3) ◽  
pp. 2333-2334 ◽  
Author(s):  
Goro Maruta ◽  
Sadamu Takeda ◽  
Kizashi Yamaguchi ◽  
Kazumasa Ueda ◽  
Toyonari Sugimoto

1959 ◽  
Vol 30 (3) ◽  
pp. 860-861 ◽  
Author(s):  
H. S. Gutowsky ◽  
Hazime Kusumoto ◽  
T. H. Brown ◽  
D. H. Anderson

Author(s):  
Carlo Gatti ◽  
Giovanni Macetti ◽  
Leonardo Lo Presti

The Source Function (SF) tool was applied to the analysis of thetheoreticalspin density in azido CuIIdinuclear complexes, where the azido group, acting as a coupler between the CuIIcations, is linked to the metal centres either in an end-on or in an end–end fashion. Results for only the former structural arrangement are reported in the present paper. The SF highlights to which extent the magnetic centres contribute to determine the local spin delocalization and polarization at any point in the dimetallic complex and whether an atom or group of atoms of the ligands act in favour or against a given local spin delocalization/polarization. Ball-and-stick atomic SF percentage representations allow for a visualization of the magnetic pathways and of the specific role played by each atom along these paths, at given reference points. Decomposition of SF contributions in terms of a magnetic and of a relaxation component provides further insight. Reconstruction of partial spin densities by means of the Source Function has for the first time been introduced. At variance with the standard SF percentage representations, such reconstructions offer a simultaneous view of the sources originating from specific subsets of contributing atoms, in a selected molecular plane or in the whole space, and are therefore particularly informative. The SF tool is also used to evaluate the accuracy of the analysed spin densities. It is found that those obtained at the unrestricted B3LYP DFT level, relative to those computed at the CASSCF(6,6) level, greatly overestimate spin delocalization to the ligands, but comparatively underestimate magnetic connection (spin transmission) among atoms, along the magnetic pathways. As a consequence of its excessive spin delocalization, the UB3LYP method also overestimates spin polarization mechanisms between the paramagnetic centres and the ligands. Spin delocalization measures derived from the refinement of Polarized Neutron Diffraction data seem in general superior to those obtained through the DFT UB3LYP approach and closer to the far more accurate CASSCF results. It is also shown that a visual agreement on the spin-resolved electron densities ραand ρβderived from different approaches does not warrant a corresponding agreement between their associated spin densities.


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