Soft X-ray absorption and fragmentation of tin-oxo cage photoresists

Open Access
Authors
  • J. Haitjema
  • S. Castellanos
  • O. Lugier
  • I. Bespalov
  • R. Lindblad
  • M. Timm
  • C. Bülow
  • V. Zamudio-Bayer
  • J.T. Lau
  • B. von Issendorff
  • R. Hoekstra
  • K. Witte
  • B. Watts
  • T. Schlathölter
  • A.M. Brouwer ORCID logo
Publication date 21-02-2024
Journal Physical Chemistry Chemical Physics
Volume | Issue number 26 | 7
Pages (from-to) 5986-5998
Organisations
  • Faculty of Science (FNWI) - Van 't Hoff Institute for Molecular Sciences (HIMS)
Abstract
“Tin-oxo cage” organometallic compounds are considered as photoresists for extreme ultraviolet (EUV) photolithography. To gain insight into their electronic structure and reactivity to ionizing radiation, we trapped bare gas-phase n-butyltin-oxo cage dications [(BuSn)12O14(OH)6]2+ in an ion trap and investigated their fragmentation upon soft X-ray photoabsorption by means of mass spectrometry. In complementary experiments, the tin-oxo cages with hydroxide and trifluoroacetate counter-anions were cast in thin films and studied using X-ray transmission spectroscopy. Quantum-chemical calculations were used to interpret the observed spectra. At the carbon K-edge, a distinct pre-edge absorption band can be attributed to transitions in which electrons are promoted from C1s orbitals to the lowest unoccupied molecular orbitals, which are delocalized orbitals with strong antibonding (Sn–C σ*) character. At higher energies, the most prominent resonant transitions involve C–C and C–H σ* valence states and Rydberg (3s and 3p) states. In the solid state, the onset of continuum ionization is shifted by ∼5 eV to lower energy with respect to the gas phase, due to the electrostatic effect of the counterions. The O K-edge also shows a pre-edge absorption, but it is devoid of any specific features, because there are many transitions from the different O1s orbitals to a large number of vacant orbitals. In the gas phase, formation of the parent [(BuSn)12O14(OH)6]3+ radical ion is not observed at the C K-edge nor at the O K-edge, because the loss of a butyl group from this species is very efficient. We do observe a number of triply charged photofragment ions, some of which have lost up to 5 butyl groups. Structures of these species are proposed based on quantum-chemical calculations, and pathways of formation are discussed. Our results provide insight into the electronic structure of alkyltin-oxo cages, which is a prerequisite for understanding their response to EUV photons and their performance as EUV photoresists.
Document type Article
Language English
Related dataset Data repository for: Soft X-Ray Absorption and Fragmentation of Tin-oxo Cage Photoresists
Published at https://doi.org/10.1039/d3cp05428d
Other links https://www.scopus.com/inward/record.uri?eid=2-s2.0-85183972243&doi=10.1039%2fd3cp05428d&partnerID=40&md5=d19b331eb0385a88e26558105ceafbdd
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