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Complementary cathodoluminescence lifetime imaging configurations in a scanning electron microscope

  • S. Meuret*
  • , M. Solà Garcia
  • , T. Coenen
  • , E. Kieft
  • , H. Zeijlemaker
  • , M. Lätzel
  • , S. Christiansen
  • , S. Y. Woo
  • , Y. H. Ra
  • , Z. Mi
  • , A. Polman
  • *Corresponding author for this work
  • AMOLF
  • Delmic
  • Max Planck Institute for the Science of Light
  • McMaster University
  • McGill University
  • University of Michigan, Ann Arbor

Research output: Contribution to journalJournal articlepeer-review

Abstract

Cathodoluminescence (CL) spectroscopy provides a powerful way to characterize optical properties of materials with deep-subwavelength spatial resolution. While CL imaging to obtain optical spectra is a well-developed technology, imaging CL lifetimes with nanoscale resolution has only been explored in a few studies. In this paper we compare three different time-resolved CL techniques and compare their characteristics. Two configurations are based on the acquisition of CL decay traces using a pulsed electron beam that is generated either with an ultra-fast beam blanker, which is placed in the electron column, or by photoemission from a laser-driven electron cathode. The third configuration uses measurements of the autocorrelation function g (2) of the CL signal using either a continuous or a pulsed electron beam. The three techniques are compared in terms of complexity of implementation, spatial and temporal resolution, and measurement accuracy as a function of electron dose. A single sample of InGaN/GaN quantum wells is investigated to enable a direct comparison of lifetime measurement characteristics of the three techniques. The g (2) -based method provides decay measurements at the best spatial resolution, as it leaves the electron column configuration unaffected. The pulsed-beam methods provide better detail on the temporal excitation and decay dynamics. The ultra-fast blanker configuration delivers electron pulses as short as 30 ps at 5 keV and 250 ps at 30 keV. The repetition rate can be chosen arbitrarily up to 80 MHz and requires a conjugate plane geometry in the electron column that reduces the spatial resolution in our microscope. The photoemission configuration, pumped with 250 fs 257 nm pulses at a repetition rate from 10 kHz to 25 MHz, allows creation of electron pulses down to a few ps, with some loss in spatial resolution.

Original languageEnglish
Pages (from-to)28-38
Number of pages11
JournalUltramicroscopy
Volume197
DOIs
StatePublished - 2019.02

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