MadridgeJournal of Analytical Sciences and Instrumentation Chemical shift at the X-ray K-absorption edge of Zn in some Zn compounds

It is known that the X-ray absorption edge of metal ion may change to different extent depending upon the chemical environment viz. effective charge, nature of ligands, co-ordination numbers, electronegativity of anions, covalent character of the bonds, surrounded the metal ion, even at the same oxidation state. This change in the absorption energy of the metal ion in its compound from the pure metallic state (zero oxidation state) is known as the chemical shift ΔE (eV) of the metallic ion. In the present study by means of synchrotron based X-ray absorption spectroscopy study we have calculated the chemical shift and their corresponding effective charge on the Zn atoms in different Zn compounds where the Zn is present in the 2+ oxidation state.


Introduction
The study of the chemical shift in the compounds has been carried by measuring the K absorption edge of the Zn in the Energy Scanning EXAFS beamline (BL-09) at Indus-2 Synchrotron source (2.5 GeV, 100 mA) at the Raja Ramanna Centre for Advanced Technology (RRCAT), Indore, India [1][2].

Experimental Details
The beam line operates in the photon energy range of 4-25 KeV. The beamline optics consists of an Rh/Pt coated collimating meridional cylindrical mirror used for the collimation of the beam. The collimated beam from the pre-mirror is monochromatized by a Si (111) (2d=6.2709) based double crystal monochromator (DCM). The mirror prior to the DCM is used for the higher harmonic rejection. Second sagittally bent cylindrical crystal of the DCM is used for horizontal focusing of the beam while another Rh/Pt coated bendable post mirror facing down is used for vertical focusing of the beam at the sample position. The measurements at the Zn edge have been carried out at the transmission mode using two ionization chambers of 30 cm length each. Proper gas mixture was used to have 10-20% absorption in the 1 st first ionization chamber and 70-90% absorption in the 2 nd ionization chamber. The 1 st ionization chamber measures the incident flux (I 0 ) and the 2 nd ionization chamber measures the transmitted flux (I t ). The X-ray absorption co-efficient is determined as µ = ln(I 0 /I t ). For the measurement the fine powder of the samples were palletized to 15 mm diameter and were kept in a kapton tape. Finally the experimentally obtained data was calibrated with the standard metal foil and normalized by the ATHENA subroutine of the IFEFIT software package [3].  The result shows that for all the samples there is a positive shift of the absorption edges from the pure metallic phase. This trend is attributed to the successive increase in the electronegativity of the ligands and causes a decrease in the covalent character of the bonds in the compounds [4]. Thus all the above mentioned factors involve in redistribution of the valance electrons of the constituent atoms and produce an effective nuclear charge on the metal ion which causes the shift in the absorption energy. Several empirical relations have been propped in the literature to calculate the effective charge on the metal ion in binary and ternary compounds. Among those the methods propped by Suchet [5] and Pauling [6] are mostly used methods, which have been widely used to calculate the effective charge on cations in the binary and ternary compounds [6][7][8].

Results and Discussion
According to Suchet's method [5], the effective charge on a cationic species involved in formation of a chemical bond is given by: where Z, -total number of electrons r-the ionic radius and n -oxidation number of the cation and Z'-total number of electrons in the anion and r' -the ionic radius in the anion.
Pauling [6] has alternatively represented an empirical relation of effective charge as: Where n is the valance of the absorbing cation and I be the iconicity of the metal-ligand bond which is given as: Where X l and X a are the electronegativities of the ligand and the absorbing atom, respectively, and c is the coordination number of the absorbing atom. This expression of ionicity is found to be agreeing with the experimentally obtained electric dipole moment of standard molecules.
However it has been observed that by other worker [9,10] that the above mentioned relation is not suitable to calculate the effective charge in the compound having anionic radicals like NO 3-, SO 4 2-, CO 3 2-, PO 4 3-etc. For complex samples viz., Ammonium Diuranate and Uranyl Nitrate Hexahydrate, as we have shown in earlier communication [11], the effective charges can be calculated approximately by considering the first coordination shell around the absorbing atom. We have estimated the effective charges on Zn in the studied compound by considering the first oxygen coordination shell, which is tetrahedral in case of Zn nitrate and phosphate and octahedral in case of carbonate and sulphate compounds and using Pauling's formalism described above.

Conclusion
The values of the effective charges of Zn in these compounds have also been shown in Table-1 along with the corresponding chemical shift (ΔE) values obtained from XANES data, which shows an increase in chemical shift with increase in the effective charge as expected.