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Ferroelectric triggering of carbon monoxide adsorption on lead zirco-titanate (001) surfaces
Atomically clean lead zirco-titanate PbZr(0.2)Ti(0.8)O(3) (001) layers exhibit a polarization oriented inwards P((−)), visible by a band bending of all core levels towards lower binding energies, whereas as introduced layers exhibit P((+)) polarization under air or in ultrahigh vacuum. The magnitude...
Autores principales: | , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group
2016
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5064406/ https://www.ncbi.nlm.nih.gov/pubmed/27739461 http://dx.doi.org/10.1038/srep35301 |
Sumario: | Atomically clean lead zirco-titanate PbZr(0.2)Ti(0.8)O(3) (001) layers exhibit a polarization oriented inwards P((−)), visible by a band bending of all core levels towards lower binding energies, whereas as introduced layers exhibit P((+)) polarization under air or in ultrahigh vacuum. The magnitude of the inwards polarization decreases when the temperature is increased at 700 K. CO adsorption on P((−)) polarized surfaces saturates at about one quarter of a monolayer of carbon, and occurs in both molecular (oxidized) and dissociated (reduced) states of carbon, with a large majority of reduced state. The sticking of CO on the surface in ultrahigh vacuum is found to be directly related to the P((−)) polarization state of the surface. A simple electrostatic mechanism is proposed to explain these dissociation processes and the sticking of carbon on P((−)) polarized areas. Carbon desorbs also when the surface is irradiated with soft X-rays. Carbon desorption when the polarization is lost proceeds most probably in form of CO(2). Upon carbon desorption cycles, the ferroelectric surface is depleted in oxygen and at some point reverses its polarization, owing to electrons provided by oxygen vacancies which are able to screen the depolarization field produced by positive fixed charges at the surface. |
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