Electron–phonon coupling in superconducting 1T-PdTe2
Abstract We have determined the electron–phonon interaction in type II Dirac semimetallic 1T-PdTe2 by means of helium atom scattering. While 1T-PdTe2 is isostructural with 1T-PtTe2, only the former is superconductor. The difference can be traced to the substantially larger value of the electron–phon...
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doaj-e7747a9dff20420aa0967ced29a3ce6d2021-02-23T10:35:07ZengNature Publishing Groupnpj 2D Materials and Applications2397-71322021-02-01511710.1038/s41699-021-00204-5Electron–phonon coupling in superconducting 1T-PdTe2Gloria Anemone0Pablo Casado Aguilar1Manuela Garnica2Fabian Calleja3Amjad Al Taleb4Chia-Nung Kuo5Chin Shan Lue6Antonio Politano7Amadeo L. Vázquez de Parga8Giorgio Benedek9Daniel Farías10Rodolfo Miranda11Departamento de Física de la Materia Condensada, Universidad Autónoma de MadridDepartamento de Física de la Materia Condensada, Universidad Autónoma de MadridInstituto Madrileño de Estudios Avanzados en Nanociencia (IMDEA-Nanociencia)Instituto Madrileño de Estudios Avanzados en Nanociencia (IMDEA-Nanociencia)Instituto Madrileño de Estudios Avanzados en Nanociencia (IMDEA-Nanociencia)Department of Physics, National Cheng Kung UniversityDepartment of Physics, National Cheng Kung UniversityDipartimento di Scienze Fisiche e Chimiche (DSFC), Università degli Studi dell’AquilaDepartamento de Física de la Materia Condensada, Universidad Autónoma de MadridDipartimento di Scienza dei Materiali, Università di Milano-BicoccaDepartamento de Física de la Materia Condensada, Universidad Autónoma de MadridDepartamento de Física de la Materia Condensada, Universidad Autónoma de MadridAbstract We have determined the electron–phonon interaction in type II Dirac semimetallic 1T-PdTe2 by means of helium atom scattering. While 1T-PdTe2 is isostructural with 1T-PtTe2, only the former is superconductor. The difference can be traced to the substantially larger value of the electron–phonon coupling in 1T-PdTe2, λ = 0.58, obtained from the Debye-Waller attenuation of the He specular peak. With this value and the surface Debye temperature, ΘD = 106.2 K, we have figured out the superconducting critical temperature, T c = 1.83 K given by the BCS theory, which is in good agreement with T c = (1.95 ± 0.03) K obtained with low-temperature scanning tunneling microscopy. The value of the effective mass related to ΘD indicates that the large electron–phonon coupling in 1T-PdTe2 is due to coupling, not only with the zone-center optical mode O2 at 9.2 meV, as proposed in a recent theoretical study, but also with the zone-boundary acoustic mode LA. Our results suggest that the topological states of a Dirac cone play a negligible role on the onset of superconductivity.https://doi.org/10.1038/s41699-021-00204-5 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Gloria Anemone Pablo Casado Aguilar Manuela Garnica Fabian Calleja Amjad Al Taleb Chia-Nung Kuo Chin Shan Lue Antonio Politano Amadeo L. Vázquez de Parga Giorgio Benedek Daniel Farías Rodolfo Miranda |
spellingShingle |
Gloria Anemone Pablo Casado Aguilar Manuela Garnica Fabian Calleja Amjad Al Taleb Chia-Nung Kuo Chin Shan Lue Antonio Politano Amadeo L. Vázquez de Parga Giorgio Benedek Daniel Farías Rodolfo Miranda Electron–phonon coupling in superconducting 1T-PdTe2 npj 2D Materials and Applications |
author_facet |
Gloria Anemone Pablo Casado Aguilar Manuela Garnica Fabian Calleja Amjad Al Taleb Chia-Nung Kuo Chin Shan Lue Antonio Politano Amadeo L. Vázquez de Parga Giorgio Benedek Daniel Farías Rodolfo Miranda |
author_sort |
Gloria Anemone |
title |
Electron–phonon coupling in superconducting 1T-PdTe2 |
title_short |
Electron–phonon coupling in superconducting 1T-PdTe2 |
title_full |
Electron–phonon coupling in superconducting 1T-PdTe2 |
title_fullStr |
Electron–phonon coupling in superconducting 1T-PdTe2 |
title_full_unstemmed |
Electron–phonon coupling in superconducting 1T-PdTe2 |
title_sort |
electron–phonon coupling in superconducting 1t-pdte2 |
publisher |
Nature Publishing Group |
series |
npj 2D Materials and Applications |
issn |
2397-7132 |
publishDate |
2021-02-01 |
description |
Abstract We have determined the electron–phonon interaction in type II Dirac semimetallic 1T-PdTe2 by means of helium atom scattering. While 1T-PdTe2 is isostructural with 1T-PtTe2, only the former is superconductor. The difference can be traced to the substantially larger value of the electron–phonon coupling in 1T-PdTe2, λ = 0.58, obtained from the Debye-Waller attenuation of the He specular peak. With this value and the surface Debye temperature, ΘD = 106.2 K, we have figured out the superconducting critical temperature, T c = 1.83 K given by the BCS theory, which is in good agreement with T c = (1.95 ± 0.03) K obtained with low-temperature scanning tunneling microscopy. The value of the effective mass related to ΘD indicates that the large electron–phonon coupling in 1T-PdTe2 is due to coupling, not only with the zone-center optical mode O2 at 9.2 meV, as proposed in a recent theoretical study, but also with the zone-boundary acoustic mode LA. Our results suggest that the topological states of a Dirac cone play a negligible role on the onset of superconductivity. |
url |
https://doi.org/10.1038/s41699-021-00204-5 |
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