Igor Antoniazzi1,Magda Grzeszczyk2,Jakub Gawraczynski1,Tomasz Wozniak3,Jordi Ibanez4,Zahir Muhammad5,Weisheng Zhao5,Maciej Molas1,Adam Babinski1
University of Warsaw1,National University of Singapore2,Wroclaw University of Science and Technology3,Geosciences Barcelona (GEO3BCN), CSIC4,Hefei Innovation Research Institute5
Igor Antoniazzi1,Magda Grzeszczyk2,Jakub Gawraczynski1,Tomasz Wozniak3,Jordi Ibanez4,Zahir Muhammad5,Weisheng Zhao5,Maciej Molas1,Adam Babinski1
University of Warsaw1,National University of Singapore2,Wroclaw University of Science and Technology3,Geosciences Barcelona (GEO3BCN), CSIC4,Hefei Innovation Research Institute5
The effect of hydrostatic pressure on the lattice dynamics of bulk hafnium disulphide (HfS<sub>2</sub>) grown by chemical vapour transport method is investigated. The pattern of powder X-Ray diffraction of the investigated material was found to be in perfect agreement with that of the octahedral 1T phase of HfS<sub>2</sub>.<br/>The Raman scattering has been studied at room temperature in diamond anvil cells in hydrostatic pressure up to 13.7 GaP.<br/>There are four Raman modes observed at ambient pressure, which is consistent with previous studies.<br/>There is an agreement in literature on the attribution of peaks at 266 cm<sup>-1</sup> and 344 cm<sup>-1</sup> to in-plane E<sub>g</sub> and out-of-plane A<sub>1g</sub> Raman-active modes, respectively. The peak at 325 cm<sup>-1</sup> is attributed to the infrared-active E<sub>u</sub> (LO) or A<sub>2u</sub>(LO) alike mode.<br/>Not clear is also the assignment of the weak feature at 141 cm<sup>-1</sup>.Its attribution to a second-order difference processes was suggested, as such peaks can be observed in Raman scattering spectra of some transition metal dichalchogenides (TMDs) however the E<sub>u</sub> (TO) was also suggested as the signature of the mode.<br/>The Raman scattering modes blueshift with increasing hydrostatic pressure with the pressure rates from 1.6 cm<sup>-1</sup>/GPa to 4.4 cm<sup>-1</sup>/GPa, which is similar to the values reported before.<br/>The lineshape of the Raman scattering spectrum does not significantly change with increasing hydrostatic pressure up to 5.7 GPa, however a substantial enhancement of the A<sub>1g</sub> peak intensity can be noticed under the highest pressure.<br/>A change in the Raman scattering spectrum is observed in hydrostatic pressure between 6.2 GPa and 7.2 GPa.<br/>Seven vibrational modes can be observed in the spectrum above the transformation, as compared to four modes before the transformation.<br/>The frequencies of the Raman scattering modes observed change linearly with pressure coefficients up to 2.6 cm<sup>-1</sup>/GPa.<br/>A negative pressure coefficinet (-0.13 cm<sup>-1</sup>/GPa) of the Raman peak observed at the lowest enegy ( approx 95 cm<sup>-1</sup>) can also be noticed.<br/>The overall lineshape of spectrum above the transformation does not change under pressure up to 13.7 GPa during compression.<br/>Surprisingly, the seven Raman modes can be observed under hydrostatic pressure down to 1.5 GPa during decompression.<br/>The apparent hysteresis of the Raman spectrum must reflect a metastable change in the sample structure.<br/>We analyse the effect in the context of iodine (I<sub>2</sub>) molecules, which are found to be present in van der Waals gaps between the HfS<sub>2 </sub>layersin the investigated structure. Possible scenarios leading to the observed metastabilty are proposed.