Abstract
As the length scales of materials decrease, the heterogeneities associated with interfaces become almost as important as the surrounding materials. This has led to extensive studies of emergent electronic and magnetic interface properties in superlattices1–9. However, the interfacial vibrations that affect the phonon-mediated properties, such as thermal conductivity10,11, are measured using macroscopic techniques that lack spatial resolution. Although it is accepted that intrinsic phonons change near boundaries12,13, the physical mechanisms and length scales through which interfacial effects influence materials remain unclear. Here we demonstrate the localized vibrational response of interfaces in strontium titanate–calcium titanate superlattices by combining advanced scanning transmission electron microscopy imaging and spectroscopy, density functional theory calculations and ultrafast optical spectroscopy. Structurally diffuse interfaces that bridge the bounding materials are observed and this local structure creates phonon modes that determine the global response of the superlattice once the spacing of the interfaces approaches the phonon spatial extent. Our results provide direct visualization of the progression of the local atomic structure and interface vibrations as they come to determine the vibrational response of an entire superlattice. Direct observation of such local atomic and vibrational phenomena demonstrates that their spatial extent needs to be quantified to understand macroscopic behaviour. Tailoring interfaces, and knowing their local vibrational response, provides a means of pursuing designer solids with emergent infrared and thermal responses.
Original language | English |
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Pages (from-to) | 556-561 |
Number of pages | 6 |
Journal | Nature |
Volume | 601 |
Issue number | 7894 |
DOIs | |
State | Published - Jan 27 2022 |
Funding
Acknowledgements E.R.H., J.A.T., S.M. and P.E.H. appreciate support from the Office of Naval Research through a MURI Program, grant number N00014-18-1-2429. J.A.T., S.M. and P.E.H. acknowledge support from Army Research Office, grant number W911NF-21-1-0119. Use of the Thermo Fisher Scientific Z-STEM and Titan instruments within UVa’s Nanoscale Materials Characterization Facility (NMCF) was fundamental to this work. Theory at Vanderbilt University was supported by the US Department of Energy, Office of Science, Basic Energy Sciences, Materials Science and Engineering Directorate grant number DE-FG02-09ER46554 and by the McMinn Endowment. Calculations were performed at the National Energy Research Scientific Computing Center (NERSC), a US Department of Energy Office of Science User Facility located at Lawrence Berkeley National Laboratory, operated under contract number DE-AC02-05CH11231. The oxide heteroepitaxy synthesis work at Berkeley and Penn State is supported by the Quantum Materials program from the DOE Office of Science, Basic Energy Sciences, under contract number DE-AC02-05CH11231, and by the MRSEC for Nanoscale Science at Penn State through grant DMR1420620. EELS experiments conducted as part of a user proposal at the Center for Nanophase Materials Sciences, which is a DOE Office of Science User Facility using instrumentation within ORNL’s Materials Characterization Core provided by UT-Battelle, LLC, under contract number DE-AC05-00OR22725 with the DOE and sponsored by the Laboratory Directed Research and Development Program of Oak Ridge National Laboratory, managed by UT-Battelle, LLC, for the US Department of Energy. R.R. also acknowledges the ARO MURI under agreement W911NF-21-2-0162. J.R. acknowledges support from the Army Research Office with award numbers W911NF-19-1-0137 and W911NF-21-1-0327. J.D.C. and J.R.M. acknowledge funding under NSF, Division of Materials Research award number 1904793. S.M. acknowledges support from the NIH Biotechnology Training Program.
Funders | Funder number |
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Materials Science and Engineering Directorate | DE-FG02-09ER46554 |
McMinn Endowment | |
National Science Foundation | |
National Institutes of Health | |
Office of Naval Research | |
U.S. Department of Energy | |
Division of Materials Research | 1904793 |
Division of Materials Research | |
Army Research Office | W911NF-21-1-0119 |
Army Research Office | |
Office of Science | |
Basic Energy Sciences | |
Oak Ridge National Laboratory | W911NF-19-1-0137, W911NF-21-1-0327 |
Oak Ridge National Laboratory | |
Lawrence Berkeley National Laboratory | DE-AC02-05CH11231 |
Lawrence Berkeley National Laboratory | |
Materials Research Science and Engineering Center, Harvard University | DE-AC05-00OR22725, DMR1420620 |
Materials Research Science and Engineering Center, Harvard University | |
Multidisciplinary University Research Initiative | N00014-18-1-2429 |
Multidisciplinary University Research Initiative |