“…Although many results have been reported regarding phonons in TiS 2 including Raman spectra at room temperature – and low temperatures (below 100 K), – infrared reflectance measurements, , neutron scattering, and theoretical works considering phonons in TiS 2 within the harmonic approximation ,,– phonon structure of this material is still poorly understood. There are two major concerns, yet unexplained, regarding typically reported Raman spectra in TiS 2 : - According to the symmetry of the pristine TiS 2 crystalthermodynamically stable in the trigonal phase ( P 3̅ m 1, CdI 2 -type structure) , often denoted as 1 T precisely two phonon modes are expected to affect the polarizability of the material and lead to Raman scattering: in-plane E g (∼235 cm –1 at the room temperature) and out-of-plane A 1g (∼335 cm –1 ). – However, the majority of reported Raman spectra also reveal the existence of an additional band at about 370–390 cm –1 , in the high-energy vicinity of the A 1g mode (Figure a)commonly called “shoulder” or “Sh” mode. , The presence of the shoulder has been reported for multiple laser wavelengths in the range of 488–633 nm (1.95–2.54 eV) with similar relative intensities of the A 1g and “Sh” features. – , To date, the most often stated hypotheses of the origin of the A 1g band’s shoulder involve phonon stiffening due to the presence of excess titanium atoms in the interlayer gaps – ,,, and the overtone (or summation) processes. ,,, None of them has yet been fully confirmed.
- The temperature evolution of the phonon frequencies evaluated within Raman experiments is intriguing. First, the measured temperature dependence of the out-of-plane A 1g and “Sh” bands’ positions significantly depends on the sample preparationleading to different slopes dω/d T in representative reports – (see...
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