Temperature Dependence of Raman Spectra in Cu2FeSnS4 Magnetic Semiconductor Compound. Issue 10 (31st May 2019)

• Record Type: Journal Article
• Authors: Rincón, Carlos; Quintero, Eugenio; Quintero, Miguel; Moreno, Ekadink; Power, Chrystian; Morocoima, Manuel; Delgado, Gerzon E.
• Is Part Of: Physica status solidi. Volume 256:Issue 10(2019)
• Page Start: n/a
• Page End: n/a
• Publication Date: 2019-05-31
• Subjects: Cu2FeSnS4 -- quaternary compound semiconductors -- Raman spectra -- Raman shift with temperature; Solid state physics -- Periodicals; Solids -- Periodicals; Atomic structure -- Periodicals; 530.41
• DOI: 10.1002/pssb.201900076
• Languages: English
• ISSNs: 0370-1972

Abstract

Abstract : The temperature dependence of the Raman scattering by phonons performed in bulk polycrystalline Cu2 FeSnS4, that crystallizes with tetragonal symmetry in space group P 4 ¯, was measured between 10 and 300 K. The most important decay channel involves the three‐phonon process with two phonons of the same branch, including combinations of optical phonons with equal or different frequencies. Additionally, coupling of an optical mode to two phonons of different branches is observed. The strong A ‐symmetry mode at 325 cm −1 decays into two optical phonons of the same frequencies v ¯ 1 = v ¯ 2 ≈ 162 cm −1 . To explain the change of Raman shift with temperature it is necessary to take into account the contribution of thermal expansion contribution. We have observed a soft mode in the Raman spectra which accounts for the antiferromagnetic phase transition that happens in this material at a Néel temperature of about 40 K. The full width at half maximum of this A‐ symmetry mode, extrapolated to zero temperature, is of about 2.6 cm −1, when the contribution of intrinsic defect scattering, which is of about 3. cm −1, is included in the calculation. Abstract : The temperature dependence of the Raman scattering performed in Cu2 FeSnS4, which crystallizes with tetragonal symmetry, was measured between 10 and 300 K. The most important decay channel involves the three‐phonon process with two phonons of the same or different branches. To explain the Raman shift with temperature it is necessary to take into account the contribution of thermal expansion contribution.