<div class="csl-bib-body">
<div class="csl-entry">Ossiander, M., Golyari, K., Scharl, K., Lehnert, L., Siegrist, F., Bürger, J. P., Zimin, D., Gessner, J. A., Weidman, M., Floss, I., Smejkal, V., Donsa, S., Lemell, C., Libisch, F., Karpowicz, N., Burgdörfer, J., Krausz, F., & Schultze, M. (2022). The speed limit of optoelectronics. <i>Nature Communications</i>, <i>13</i>(1), Article 1620. https://doi.org/10.1038/s41467-022-29252-1</div>
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dc.identifier.issn
2041-1723
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dc.identifier.uri
http://hdl.handle.net/20.500.12708/136056
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dc.description.abstract
Light-field driven charge motion links semiconductor technology to electric fields with attosecond temporal control. Motivated by ultimate-speed electron-based signal processing, strong-field excitation has been identified viable for the ultrafast manipulation of a solid's electronic properties but found to evoke perplexing post-excitation dynamics. Here, we report on single-photon-populating the conduction band of a wide-gap dielectric within approximately one femtosecond. We control the subsequent Bloch wavepacket motion with the electric field of visible light. The resulting current allows sampling optical fields and tracking charge motion driven by optical signals. Our approach utilizes a large fraction of the conduction-band bandwidth to maximize operating speed. We identify population transfer to adjacent bands and the associated group velocity inversion as the mechanism ultimately limiting how fast electric currents can be controlled in solids. Our results imply a fundamental limit for classical signal processing and suggest the feasibility of solid-state optoelectronics up to 1 PHz frequency.