Abstract

By using optical absorption and Raman spectroscopy, we have investigated the effects of pressure in the structural, electronic, and vibrational properties of ${\mathrm{Cs}}_{2}{\mathrm{CuCl}}_{4}$ in the 0--20 GPa range. Our study has provided a complete characterization of the electronic and vibrational structures of ${\mathrm{Cs}}_{2}{\mathrm{CuCl}}_{4}$ in the low-pressure Pnma phase as a function of cell volume and the Cu-Cl bond length, ${R}_{\text{Cu-Cl}}$. We have focused on the electronic structure in the Pnma phase, which is mainly related to the tetrahedral ${\mathrm{CuCl}}_{4}^{2\ensuremath{-}}$ units distorted by the Jahn-Teller effect. The strong piezochromism of ${\mathrm{Cs}}_{2}{\mathrm{CuCl}}_{4}$ is caused by the opposite shift of the charge-transfer band gap and the ${\mathrm{Cu}}^{2+}$ d-d crystal-field transitions with pressure. The high-pressure structure of ${\mathrm{Cs}}_{2}{\mathrm{CuCl}}_{4}$ above 4.9 GPa yields structural transformations that we ascribe to a change of coordination around ${\mathrm{Cu}}^{2+}$. The high-pressure phase appears largely amorphized, therefore any structural information from x-ray diffraction is ruled out. Here we use electronic and vibrational probes to get inside the structural information.

Highlights

  • Cs2CuCl4 is a wide-band-gap charge-transfer (CT) semiconductor

  • The main peaks of the second set correspond to internal Cu-Cl stretching modes of A1 and T2 in Td (A1, and E+B2, respectively, in D2d ): ν1(A1/A1)= 295 cm−1, ν3 (B2/T2)= 279 cm−1, and ν3 (E/T2)= 249 cm−1. These peaks compare well with those measured for CoCl24− (Td ) in the isostructural Cs2CoCl4 compound [3]; there is a significant difference between the Raman spectra of Cs2CoCl4 and Cs2CuCl4—that is, the splitting of some peaks in the latter compound that we associate with the lower local symmetry of CuCl24− (D2d ) due to the JT effect

  • We have demonstrated that the vibrational and electronic structures of Cs2CuCl4 can be explained to a great extent on the basis of CuCl24− with a D2d coordination symmetry, their pressure dependence being consistent with structural changes undergone by Cs2CuCl4

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Summary

INTRODUCTION

Cs2CuCl4 (orthorhombic Pnma at ambient conditions) is a wide-band-gap charge-transfer (CT) semiconductor Under pressure it exhibits a puzzling optical behavior which is associated with the Cu2+ absorption and its structural changes [1]. The relationship between dihedral Cl-Cu-Cl angle of the JT-distorted flattened tetrahedra and the Cu2+ d-orbital splitting experimentally obtained by optical absorption spectroscopy and its pressure dependence is investigated These correlations will be used to analyze the shifts experienced by the band-gap energy and d-d bands as well as the Raman peaks with pressure in the Cs2CuCl4 Pnma phase, and how they change above the structural phase transition observed 5 GPa

EXPERIMENTAL
Raman spectrum at ambient conditions
Pressure dependence
Temperature dependence of Raman spectra
CONCLUSIONS
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