4.7 Article

Chemical bonding and Born charge in 1T-HfS2

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NATURE PORTFOLIO
DOI: 10.1038/s41699-021-00226-z

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  1. U.S. Department of Energy, Office of Basic Energy Sciences, Materials Science Division [DE-FG02-01ER45885]
  2. National Science Foundation through the University of Minnesota MRSEC [DMR-2011401]

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In this study, infrared absorption and Raman scattering spectroscopies were utilized to investigate the properties of 1T-HfS2. By analyzing the LO-TO splitting of the E-u vibrational mode and reevaluating the mode mass, unit cell volume, and dielectric constant, the Born effective charge was revealed to be ZB* = 5.3e, in agreement with first-principles calculations. Furthermore, the Born charge was decomposed into polarizability and local charge, with polar displacement-induced charge transfer from sulfur p to hafnium d being a key factor in the enhanced Born charge. The findings suggest that 1T-HfS2 is an ionic crystal with strong and dynamic covalent effects.
We combine infrared absorption and Raman scattering spectroscopies to explore the properties of the heavy transition metal dichalcogenide 1T-HfS2. We employ the LO-TO splitting of the E-u vibrational mode along with a reevaluation of mode mass, unit cell volume, and dielectric constant to reveal the Born effective charge. We find ZB* = 5.3e, in excellent agreement with complementary first-principles calculations. In addition to resolving the controversy over the nature of chemical bonding in this system, we decompose Born charge into polarizability and local charge. We find alpha = 5.07 A(3) and Z* = 5.2e, respectively. Polar displacement-induced charge transfer from sulfur p to hafnium d is responsible for the enhanced Born charge compared to the nominal 4+ in hafnium. 1T-HfS2 is thus an ionic crystal with strong and dynamic covalent effects. Taken together, our work places the vibrational properties of 1T-HfS2 on a firm foundation and opens the door to understanding the properties of tubes and sheets.

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