4.8 Article

Electronic Temperature and Two-Electron Processes in Overbias Plasmonic Emission from Tunnel Junctions

Journal

NANO LETTERS
Volume 21, Issue 16, Pages 7086-7092

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acs.nanolett.1c00951

Keywords

Scanning tunneling electroluminescence; Electronic temperature; Plasmonic nanocavities; Quasiparticle lifetime; Ag(111) surface

Funding

  1. Spanish Ministry for Economy and Competitiveness [PGC2018-098613-B-C21, PGC2018-096047-B-I00]
  2. regional government of Comunidad de Madrid [S2018/NMT-4321]
  3. IMDEA Nanoscience
  4. Severo Ochoa and Maria de Maeztu Programmes for Centres and Units of Excellence in RD (MINECO) [SEV-2016-0686, CEX2018-000805-M]
  5. regional government of Madrid
  6. Spanish Ministry of Science and Innovation [PID2019-103910GB-I00, PID2019-105488GB-I00]
  7. Projects of the Basque Government for consolidated groups of the Basque University, through the Department of Universities [IT-1246-19, IT1164-19]
  8. Universidad Autonoma de Madrid [UAM/48]

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Accurate measurement of electronic temperatures in metallic nanostructures is crucial for various technological applications. This study demonstrates that electronic temperature can be accurately determined by the shape of tunnel electroluminescence emission edge in tunnel plasmonic nanocavities, revealing a significant deviation between electronic and lattice temperatures under certain conditions. The results provide insights into the nature of overbias emission in tunnel junctions and offer a new method for determining electronic temperatures and quasiparticle dynamics.
The accurate determination of electronic temperatures in metallic nanostructures is essential for many technological applications, like plasmon-enhanced catalysis or lithographic nanofabrication procedures. In this Letter, we demonstrate that the electronic temperature can be accurately measured by the shape of the tunnel electroluminescence emission edge in tunnel plasmonic nanocavities, which follows a universal thermal distribution with the bias voltage as the chemical potential of the photon population. A significant deviation between electronic and lattice temperatures is found below 30 K for tunnel currents larger than 15 nA. This deviation is rationalized as the result of a two-electron process in which the second electron excites plasmon modes with an energy distribution that reflects the higher temperature following the first tunneling event. These results dispel a long-standing controversy on the nature of overbias emission in tunnel junctions and adds a new method for the determination of electronic temperatures and quasiparticle dynamics.

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