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RESEARCH PRODUCT
Plasmon-Induced Direct Hot-Carrier Transfer at Metal-Acceptor Interfaces.
Paul ErhartMikael KuismaDaniel Marti-dafcikDaniel ReichmuthPriyank V. KumarTuomas P. RossiTuomas P. RossiDavid J. NorrisMartti J. Puskasubject
NanostructureMaterials scienceprobabilityta221General Physics and Astronomyhot holes02 engineering and technology010402 general chemistry01 natural scienceslaw.inventionMetalnanorakenteetpuolijohteetlawTransfer (computing)General Materials SciencePlasmonta114nanoelektroniikkatiheysfunktionaaliteoriaGeneral Engineeringplasmon decayTime-dependent density functional theory021001 nanoscience & nanotechnologyLaserAcceptortime-dependent density-functional theory0104 chemical sciencesdirect transferChemical physicsvisual_artFemtosecondvisual_art.visual_art_mediumtodennäköisyys0210 nano-technologyhot electronsdescription
Plasmon-induced hot-carrier transfer from a metal nanostructure to an acceptor is known to occur via two key mechanisms: (i) indirect transfer, where the hot carriers are produced in the metal nanostructure and subsequently transferred to the acceptor, and (ii) direct transfer, where the plasmons decay by directly exciting carriers from the metal to the acceptor. Unfortunately, an atomic-level understanding of the direct-transfer process, especially with regard to its quantification, remains elusive even though it is estimated to be more efficient compared to the indirect-transfer process. This is due to experimental challenges in separating direct from indirect transfer as both processes occur simultaneously at femtosecond time scales. Here, we employ time-dependent density-functional theory simulations to isolate and study the direct-transfer process at a model metal-acceptor (Ag 147 -Cd 33 Se 33 ) interface. Our simulations show that, for a 10 fs Gaussian laser pulse tuned to the plasmon frequency, the plasmon formed in the Ag 147 -Cd 33 Se 33 system decays within 10 fs and induces the direct transfer with a probability of about 40%. We decompose the direct-transfer process further and demonstrate that the direct injection of both electrons and holes into the acceptor, termed direct hot-electron transfer (DHET) and direct hot-hole transfer (DHHT), takes place with similar probabilities of about 20% each. Finally, effective strategies to control and tune the probabilities of DHET and DHHT processes are proposed. We envision our work to provide guidelines toward the design of metal-acceptor interfaces that enable more efficient plasmonic hot-carrier devices. Peer reviewed
year | journal | country | edition | language |
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2019-02-15 | ACS nano |