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Complementary cathodoluminescence lifetime imaging configurations in a scanning electron microscope.
Meuret, S; Solà Garcia, M; Coenen, T; Kieft, E; Zeijlemaker, H; Lätzel, M; Christiansen, S; Woo, S Y; Ra, Y H; Mi, Z; Polman, A.
Afiliação
  • Meuret S; Center for Nanophotonics, AMOLF, Science Park 104, 1098 XG Amsterdam, The Netherlands. Electronic address: s.meuret@amolf.nl.
  • Solà Garcia M; Center for Nanophotonics, AMOLF, Science Park 104, 1098 XG Amsterdam, The Netherlands.
  • Coenen T; Center for Nanophotonics, AMOLF, Science Park 104, 1098 XG Amsterdam, The Netherlands; Delmic BV, Kanaalweg 4, 2628 EB Delft, The Netherlands.
  • Kieft E; Thermo Fisher Scientific, Achtseweg Noord 5, 5651 GG Eindhoven, The Netherlands.
  • Zeijlemaker H; Center for Nanophotonics, AMOLF, Science Park 104, 1098 XG Amsterdam, The Netherlands.
  • Lätzel M; Max Planck Institute for the Science of Light, Staudtstrasse 2, 91058 Erlangen, Germany.
  • Christiansen S; Max Planck Institute for the Science of Light, Staudtstrasse 2, 91058 Erlangen, Germany.
  • Woo SY; Department of Materials Science and Engineering, Canadian Centre for Electron Microscopy, McMaster University, 1280 Main Street West, Hamilton, Ontario L8S 4M1, Canada.
  • Ra YH; Department of Electrical and Computer Engineering, McGill University, 3480 University Street, Montreal, Quebec H3A 0E9, Canada.
  • Mi Z; Department of Electrical Engineering and Computer Science, University of Michigan, Ann Arbor, MI 48109, USA.
  • Polman A; Center for Nanophotonics, AMOLF, Science Park 104, 1098 XG Amsterdam, The Netherlands.
Ultramicroscopy ; 197: 28-38, 2019 02.
Article em En | MEDLINE | ID: mdl-30476703
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.

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2019 Tipo de documento: Article

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2019 Tipo de documento: Article