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Role of Chalcogen-p States in the Optical Response of Bulk PtSe2 and PtTe2

This study reveals that the distinct optical properties of bulk PtSe2_2 and PtTe2_2, particularly the significantly stronger Drude spectral weight and mid-infrared absorption in PtTe2_2, arise from the higher energy position of chalcogen-pp states which enhances band overlap and facilitates transitions to Pt-dd bands, while the type-II Dirac points remain too deep to contribute appreciably to the interband conductivity.

Original authors: Ji Eun Lee, R. Mathew Roy, Premakumar Yanda, Chandra Shekhar, Claudia Felser, Martin Dressel

Published 2026-10-23
📖 4 min read☕ Coffee break read

Original authors: Ji Eun Lee, R. Mathew Roy, Premakumar Yanda, Chandra Shekhar, Claudia Felser, Martin Dressel

Original paper licensed under CC BY 4.0 (http://creativecommons.org/licenses/by/4.0/). ✨ This is an AI-generated explanation of the paper below. It is not written or endorsed by the authors. For technical accuracy, refer to the original paper. Read full disclaimer

In the world of materials science, researchers often look for substances that conduct electricity with unusual ease or possess electronic properties that defy standard rules. Two such materials, platinum diselenide and platinum ditelluride, belong to a family of layered crystals that have recently captured attention for hosting "Dirac fermions." These are electrons that behave as if they have no mass, moving through the crystal at incredible speeds. While these materials share the same basic atomic architecture and the same number of electrons, they behave very differently in practice. One conducts electricity far better than the other, and they react to light in distinct ways. Understanding why these two nearly identical twins act so differently is crucial for developing future technologies, such as ultra-fast sensors or devices that operate using light rather than just electricity. The key to this mystery lies not in the heavy platinum atoms that form the core of the crystal, but in the lighter atoms—selenium or tellurium—that sit on the outside.

A team of researchers set out to solve this puzzle by shining infrared light on large, high-quality crystals of both materials and measuring how they reflected and absorbed that light. They cooled the crystals down to temperatures as low as ten Kelvin, just above absolute zero, to see how their behavior changed in the cold. By comparing their measurements with detailed computer simulations of the atoms and electrons inside, they discovered that the difference in performance comes down to the energy levels of the outer atoms. In the material containing tellurium, the energy states of those outer atoms sit higher up than in the material containing selenium. This small shift in energy causes a cascade of effects that explains why one material is a much better conductor and why it absorbs light in a broad, continuous band, while the other remains relatively quiet.

The researchers found that when they measured the flow of electricity, the tellurium-based material was vastly superior. At low temperatures, the ability of its electrons to move freely was ten times greater than that of the selenium-based material. This was visible in the light experiments as a much stronger response to low-energy infrared light. The tellurium crystal also displayed a broad, continuous absorption of light across the mid-infrared range, a feature that was almost entirely absent in the selenium crystal. To understand the source of this difference, the team turned to computer models that tracked the movement of electrons between different energy bands. They found that the broad absorption in the tellurium crystal was caused by electrons jumping from a specific band dominated by tellurium atoms into a band dominated by platinum atoms. Because the tellurium energy band sits higher up, these jumps can happen with much less energy, creating a wide range of possible transitions that absorb light continuously. In the selenium crystal, this band sits lower, making these jumps much harder to trigger, which leaves a gap in the light absorption.

A significant part of the scientific conversation around these materials has focused on the presence of "Dirac points," specific locations in the crystal where the energy bands cross in a way that creates massless electrons. It was previously thought that transitions between these specific bands might be responsible for the materials' optical properties. However, this study provides a clear picture that contradicts that idea. The calculations showed that these special Dirac points lie far below the energy level where the electrons usually sit. Because the bands forming these points are completely full of electrons, no light can trigger a jump between them. Instead, the researchers found that the optical behavior is shaped entirely by other bands, specifically the interaction between the outer chalcogen atoms and the central platinum atoms. The unique properties of the tellurium material are not a result of its exotic Dirac points, but rather a consequence of how its outer atoms are positioned relative to the rest of the crystal.

The study concludes that the distinct electronic and optical personalities of these two materials are dictated by the vertical position of the outer atoms' energy levels. In the tellurium compound, the higher energy of these levels increases the overlap between different electron bands, allowing more electrons to move freely and creating the broad light absorption. In the selenium compound, the lower energy of these levels keeps the bands more separated, resulting in weaker conductivity and a lack of mid-infrared absorption. This finding clarifies that while the materials share a structure and the potential for exotic physics, their practical behavior is governed by the subtle energy shifts of their constituent atoms. The research effectively rules out the idea that the massless Dirac electrons are the primary drivers of the infrared response, pointing instead to the more conventional, yet powerful, influence of the chalcogen atoms.

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