Abstract

Ultrafast structural probing has greatly enhanced our understanding of the coupling of atomic motion to electronic and phononic degrees-of-freedom in quasi-bulk materials. In bi- and multilayer model systems, additionally, spatially inhomogeneous relaxation channels are accessible, often governed by pronounced interfacial couplings and local excitations in confined geometries. Here, we systematically explore the key dependencies of the low-frequency acoustic phonon spectrum in an elastically mismatched metal/semiconductor bilayer system optically excited by femtosecond laser pulses. We track the spatiotemporal strain wave propagation in the heterostructure employing a discrete numerical linear chain simulation and access acoustic wave reflections and interfacial couplings with a phonon mode description based on a continuum mechanics model. Due to the interplay of elastic properties and mass densities of the two materials, acoustic resonance frequencies of the heterostructure significantly differ from breathing modes in monolayer films. For large acoustic mismatch, the spatial localization of phonon eigenmodes is derived from analytical approximations and can be interpreted as harmonic oscillations in decoupled mechanical resonators.

Highlights

  • The complex microscopic mechanisms of pico- and femtosecond phononic processes are being uncovered by high-resolution optical spectroscopy and recently developed ultrafast methodologies

  • Ultrafast structural probing has greatly enhanced our understanding of the coupling of atomic motion to electronic and phononic degreesof-freedom in quasi-bulk materials

  • We systematically explore the key dependencies of the low-frequency acoustic phonon spectrum in an elastically mismatched metal/semiconductor bilayer system optically excited by femtosecond laser pulses

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Summary

Introduction

The complex microscopic mechanisms of pico- and femtosecond phononic processes are being uncovered by high-resolution optical spectroscopy and recently developed ultrafast methodologies. Only platinum is optically excited, it is apparent that multifrequency strain dynamics are induced in both layers due to interlayer strain coupling, in contrast to the single platinum layer exhibiting only a breathing mode with a single frequency [with additional higher order harmonic contributions, Fig. 1(b) (top)].

Results
Conclusion

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