Nonequivalent Atomic Vibrations at Interfaces in a Polar Superlattice

Author:

Hoglund Eric R.12ORCID,Walker Harrison A.34ORCID,Hussain Kamal5,Bao De‐Liang3ORCID,Ni Haoyang67ORCID,Mamun Abdullah4ORCID,Baxter Jefferey1,Caldwell Joshua D.8ORCID,Khan Asif5,Pantelides Sokrates T.349ORCID,Hopkins Patrick E.21011ORCID,Hachtel Jordan A.1ORCID

Affiliation:

1. Center for Nanophase Materials Sciences Oak Ridge National Laboratory Oak Ridge TN 37830 USA

2. Department of Materials Science and Engineering University of Virginia Charlottesville VA 22904 USA

3. Department of Physics and Astronomy Vanderbilt University Nashville TN 37235 USA

4. Interdisciplinary Materials Science Program Vanderbilt University Nashville TN 37235 USA

5. Department of Electrical Engineering University of South Carolina Columbia SC 29208 USA

6. Department of Materials Science and Engineering University of Illinois at Urbana‐Champaign Urbana IL 61820 USA

7. Materials Research Laboratory University of Illinois at Urbana‐Champaign Urbana IL 61820 USA

8. Department of Mechanical Engineering and Electrical Engineering Vanderbilt University Nashville TN 37235 USA

9. Department of Electrical and Computer Engineering Vanderbilt University Nashville TN 37235 USA

10. Department of Mechanical and Aerospace Engineering University of Virginia Charlottesville VA 22904 USA

11. Department of Physics University of Virginia Charlottesville VA 22904 USA

Abstract

AbstractIn heterostructures made from polar materials, e.g., AlN–GaN–AlN, the nonequivalence of the two interfaces is long recognized as a critical aspect of their electronic properties; in that, they host different 2D carrier gases. Interfaces play an important role in the vibrational properties of materials, where interface states enhance thermal conductivity and can generate unique infrared‐optical activity. The nonequivalence of the corresponding interface atomic vibrations, however, is not investigated so far due to a lack of experimental techniques with both high spatial and high spectral resolution. Herein, the nonequivalence of AlN–(Al0.65Ga0.35)N and (Al0.65Ga0.35)N–AlN interface vibrations is experimentally demonstrated using monochromated electron energy‐loss spectroscopy in the scanning transmission electron microscope (STEM‐EELS) and density‐functional‐theory (DFT) calculations are employed to gain insights in the physical origins of observations. It is demonstrated that STEM‐EELS possesses sensitivity to the displacement vector of the vibrational modes as well as the frequency, which is as critical to understanding vibrations as polarization in optical spectroscopies. The combination enables direct mapping of the nonequivalent interface phonons between materials with different phonon polarizations. The results demonstrate the capacity to carefully assess the vibrational properties of complex heterostructures where interface states dominate the functional properties.

Funder

Office of Naval Research

U.S. Department of Energy

Office of Science

Basic Energy Sciences

Publisher

Wiley

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