Direct Observation of Rh and La Dopant Positions in SrTiO <sub>3</sub> Nanoparticles with Atomic-Scale Electron Microscopy

Doped SrTiO<sub>3</sub> nanoparticles constitute a leading materials platform for solar hydrogen production. One of the most ubiquitous and efficient SrTiO<sub>3</sub> materials utilizes Rh and La as dopants, designed to improve both visible-light absorption and charge separation ability. Typically, dopant positions in the SrTiO<sub>3</sub> lattice are assigned using ionic size and charge or ensemble-averaged techniques such as power X-ray diffraction or Raman spectroscopy. Direct observations of dopant locations in the SrTiO<sub>3</sub> lattice have not been previously reported. Here, we apply atomic-scale scanning transmission electron microscopy (STEM) coupled with image processing to directly elucidate dopant locations in 2% Rh-doped SrTiO<sub>3</sub> (Rh:SrTiO<sub>3</sub>) and 2% La, 2% Rh codoped SrTiO<sub>3</sub> (La,Rh:SrTiO<sub>3</sub>). Ensemble measurements were first performed to quantify aggregate properties across many particles of each type. Measurements of H<sub>2</sub> using in-line mass spectrometry suggest that the materials have different quantum yields for photocatalytic H<sub>2</sub> evolution, and Raman spectroscopy suggest that the concentration of dopants in the B-site (Ti site) differs. Simultaneous atomic-scale STEM, energy-dispersive X-ray spectroscopy (EDS), and electron energy loss spectroscopy (EELS) were performed on individual nanoparticles to directly determine dopant locations. Results indicate that in Rh:SrTiO<sub>3</sub>, Rh occupies both the A-site and the B-site, which is unexpected because ionic radii argument suggests Rh will occupy only the B-site. In La,Rh:SrTiO<sub>3</sub>, La primarily occupies the A-site and Rh primarily occupies the B-site. Precise knowledge of dopant positions is used to inform density functional theory (DFT) simulations for each doped lattice's electronic structure. These combined results suggest that La codoping can hinder photocatalytic H<sub>2</sub> evolution activity when Rh dopants exist in B-site recombination centers. The methods presented here demonstrate the effectiveness of correlating ensemble measurements, atomic-scale STEM imaging, and DFT simulations to establish structure-performance relationships for doped SrTiO<sub>3</sub> nanoparticles.

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Journal
ACS Applied Materials & Interfaces
Published
2025-11-10
DOI
https://doi.org/10.1021/acsami.5c15338
Primary Topic
Electronic and Structural Properties of Oxides
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article
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article

Direct Observation of Rh and La Dopant Positions in SrTiO 3 Nanoparticles with Atomic-Scale Electron Microscopy

Xiaoqing Pan, A. Alec Talin, Levi D. Palmer, Akihiko Kudo et al.
ACS Applied Materials & Interfaces
Electronic and Structural Properties of Oxides
article

Direct Observation of Rh and La Dopant Positions in SrTiO 3 Nanoparticles with Atomic-Scale Electron Microscopy

Xiaoqing Pan, A. Alec Talin, Levi D. Palmer, Akihiko Kudo, Joseph P. Patterson, Shane Ardo, Justin T. Mulvey, Kenta Watanabe, Zejie Chen, Scott K. Cushing, Mingjie Xu, Bradley W. Layne, Ezra Korican-Barlay, P. Prasad
article en

Abstract

Doped SrTiO<sub>3</sub> nanoparticles constitute a leading materials platform for solar hydrogen production. One of the most ubiquitous and efficient SrTiO<sub>3</sub> materials utilizes Rh and La as dopants, designed to improve both visible-light absorption and charge separation ability. Typically, dopant positions in the SrTiO<sub>3</sub> lattice are assigned using ionic size and charge or ensemble-averaged techniques such as power X-ray diffraction or Raman spectroscopy. Direct observations of dopant locations in the SrTiO<sub>3</sub> lattice have not been previously reported. Here, we apply atomic-scale scanning transmission electron microscopy (STEM) coupled with image processing to directly elucidate dopant locations in 2% Rh-doped SrTiO<sub>3</sub> (Rh:SrTiO<sub>3</sub>) and 2% La, 2% Rh codoped SrTiO<sub>3</sub> (La,Rh:SrTiO<sub>3</sub>). Ensemble measurements were first performed to quantify aggregate properties across many particles of each type. Measurements of H<sub>2</sub> using in-line mass spectrometry suggest that the materials have different quantum yields for photocatalytic H<sub>2</sub> evolution, and Raman spectroscopy suggest that the concentration of dopants in the B-site (Ti site) differs. Simultaneous atomic-scale STEM, energy-dispersive X-ray spectroscopy (EDS), and electron energy loss spectroscopy (EELS) were performed on individual nanoparticles to directly determine dopant locations. Results indicate that in Rh:SrTiO<sub>3</sub>, Rh occupies both the A-site and the B-site, which is unexpected because ionic radii argument suggests Rh will occupy only the B-site. In La,Rh:SrTiO<sub>3</sub>, La primarily occupies the A-site and Rh primarily occupies the B-site. Precise knowledge of dopant positions is used to inform density functional theory (DFT) simulations for each doped lattice's electronic structure. These combined results suggest that La codoping can hinder photocatalytic H<sub>2</sub> evolution activity when Rh dopants exist in B-site recombination centers. The methods presented here demonstrate the effectiveness of correlating ensemble measurements, atomic-scale STEM imaging, and DFT simulations to establish structure-performance relationships for doped SrTiO<sub>3</sub> nanoparticles.

ACS Applied Materials & InterfacesVol. 17(46)
California Institute of Technology (US), Tokyo University of Science (JP), Sandia National Laboratories California (US), University of California, Irvine (US), Combustion Institute (US), University of California System (US), Sandia National Laboratories (US), Division of Chemistry (US), Irvine University (US), Alstom (United States) (US), University of California, Berkeley (US)
Openalex Percentile: Top 72%
Electronic and Structural Properties of Oxides
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