Abstract

We have investigated the crystal structure of $Cs_2CuCl_4$ in the 0-20 GPa range as a function of pressure and how pressure affects its electronic properties by means of optical absorption spectroscopy. In particular, we focused on the electronic properties in the low-pressure Pnma phase, which are mainly related to the tetrahedral $CuCl_4^{2-}$ units distorted by the Jahn-Teller effect. This study provides a complete characterization of the electronic structure of $Cs_2CuCl_4$ in the Pmna phase as a function of the cell volume and the $Cu-Cl$ bond length, $R_{Cu-Cl}$. Interestingly, the opposite shift of the charge-transfer band-gap and the $Cu^{2+}$ d-d crystal-field band shift with pressure are responsible for the strong piezochromism of $Cs_2CuCl_4$. We have also explored the high-pressure structure of $Cs_2CuCl_4$ above 4.9 GPa yielding structural transformations that are probably associated with a change of coordination around $Cu^{2+}$. Since the high-pressure phase appears largely amorphized, any structural information from X-ray diffraction is ruled out. We use electronic probes to get structural information of the high-pressure phase.
 Edited by: A. Goñi, A. Cantarero, J. S. Reparaz

Highlights

  • Cs2CuCl4 is a wide-band-gap Charge-Transfer (CT) semiconductor (E g = 2.52 eV), which exhibits a puzzling optical behaviour under pressure, associated with the Cu2+ absorption and its structural changes [1]

  • We investigate the relationship between dihedral Cl-CuCl angle of the JT-distorted flattened tetrahedra and the Cu2+ d -orbital splitting experimentally observed by optical absorption and its pressure dependence

  • These correlations will be used to analyze how the band gap energy and d-d bands vary with pressure in the Cs2CuCl4 Pnma phase, and how they change after the structural phase transition above 5 GPa

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Summary

Introduction

Cs2CuCl4 (orthorhombic Pnma at ambient pressure) is a wide-band-gap Charge-Transfer (CT) semiconductor (E g = 2.52 eV), which exhibits a puzzling optical behaviour under pressure, associated with the Cu2+ absorption and its structural changes [1]. Both Cl−→Cu2+ CT and d-d absorption bands undergo unusually large pressure shifts and intensity changes showing abrupt jumps at about 5 GPa. This crystal exhibits a yellow–orange color at ambient conditions and below 5 GPa, which is mainly defined by the tail of the CT band (band gap) placed around 450 nm [2].

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