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  • Letter

Nonperturbative determination of isotope-induced anomalous vibrational physics

Huan Wu1, Zihao Qin1, Suixuan Li1, Lucas Lindsay2, and Yongjie Hu1,*

  • 1School of Engineering and Applied Science, University of California, Los Angeles, Los Angeles, California 90095, USA
  • 2Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA

  • *yhu@seas.ucla.edu

Phys. Rev. B 108, L140302 – Published 18 October, 2023

DOI: https://doi.org/10.1103/PhysRevB.108.L140302

Abstract

In general, vibrational physics has been well described by quantum perturbation theory (QPT) to provide footprint characteristics for common crystals. However, despite weak phonon anharmonicity, the recently discovered cubic crystals (BAs and BP) have shown anomalous vibrational dynamics with elusive fundamental origin. Here, we developed a nonperturbative ab initio approach, together with spectroscopy and high-pressure experiments, to successfully determine the exact dynamic evolutions of the vibrational physics. We found that the local fluctuation and coupling isotopes significantly dictate the vibrational spectra, through the Brillouin zone folding that has previously been ignored in literature. By decomposing vibrational spectra into individual isotope eigenvectors, we observed both positive and negative contributions to Raman intensity from constitutional atoms (B10, B11, As75, or P31). Importantly, our nonperturbative theory predicts that a vibrational resonance appears at high hydrostatic pressure due to broken translational symmetry, which was indeed verified by experimental measurement under a pressure up to 31.5 GPa. In this paper, we develop fundamental understandings for the anomalous lattice physics under the failure of QPT and provide an approach in exploring transport phenomena for materials of extreme properties.

Physics Subject Headings (PhySH)

Corrections

6 November, 2023

Correction: Two terms were missing from Eq. (10) and have been inserted. The previously published Figure 3 contained an erroneous label and an incomplete curve in panel (b) and has been replaced.

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