Cargando…

NIR luminescence lifetime nanothermometry based on phonon assisted Yb(3+)–Nd(3+) energy transfer

Luminescence thermometry in biomedical sciences is a highly desirable, but also highly challenging and demanding technology. Numerous artifacts have been found during steady-state spectroscopy temperature quantification, such as ratiometric spectroscopy. Oppositely, the luminescence lifetime is cons...

Descripción completa

Detalles Bibliográficos
Autores principales: Maciejewska, K., Bednarkiewicz, A., Marciniak, L.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: RSC 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9418974/
https://www.ncbi.nlm.nih.gov/pubmed/36132339
http://dx.doi.org/10.1039/d1na00285f
_version_ 1784777070745747456
author Maciejewska, K.
Bednarkiewicz, A.
Marciniak, L.
author_facet Maciejewska, K.
Bednarkiewicz, A.
Marciniak, L.
author_sort Maciejewska, K.
collection PubMed
description Luminescence thermometry in biomedical sciences is a highly desirable, but also highly challenging and demanding technology. Numerous artifacts have been found during steady-state spectroscopy temperature quantification, such as ratiometric spectroscopy. Oppositely, the luminescence lifetime is considered as the most reliable indicator of temperature thermometry because this luminescent feature is not susceptible to sample properties or luminescence reabsorption by the nanothermometers themselves. Unfortunately, this type of thermometer is much less studied and known. Here, the thermometric properties of Yb(3+) ions in Nd(0.5)RE(0.4)Yb(0.1)PO(4) luminescent temperature probes were evaluated, aiming to design and optimize luminescence lifetime based nanothermometers. Temperature dependence of the luminescence lifetimes is induced by thermally activated phonon assisted energy transfer from the (2)F(5/2) state of Yb(3+) ions to the (4)F(3/2) state of Nd(3+) ions, which in turn is responsible for the significant quenching of the Yb(3+):(2)F(5/2) lifetime. It was also found that the thermal quenching and thus the relative sensitivity of the luminescent thermometer can be intentionally altered by the RE ions used (RE = Y, Lu, La, and Gd). The highest relative sensitivity was found to be S(R) = 1.22% K(−1) at 355 K for Nd(0.5)Y(0.4)Yb(0.1)PO(4) and it remains above 1% K(−1) up to 500 K. The high sensitivity and reliable thermometric performance of Nd(0.5)La(0.4)Yb(0.1)PO(4) were confirmed by the high reproducibility of the temperature readout and the temperature uncertainty being as low as δT = 0.05 K at 383 K.
format Online
Article
Text
id pubmed-9418974
institution National Center for Biotechnology Information
language English
publishDate 2021
publisher RSC
record_format MEDLINE/PubMed
spelling pubmed-94189742022-09-20 NIR luminescence lifetime nanothermometry based on phonon assisted Yb(3+)–Nd(3+) energy transfer Maciejewska, K. Bednarkiewicz, A. Marciniak, L. Nanoscale Adv Chemistry Luminescence thermometry in biomedical sciences is a highly desirable, but also highly challenging and demanding technology. Numerous artifacts have been found during steady-state spectroscopy temperature quantification, such as ratiometric spectroscopy. Oppositely, the luminescence lifetime is considered as the most reliable indicator of temperature thermometry because this luminescent feature is not susceptible to sample properties or luminescence reabsorption by the nanothermometers themselves. Unfortunately, this type of thermometer is much less studied and known. Here, the thermometric properties of Yb(3+) ions in Nd(0.5)RE(0.4)Yb(0.1)PO(4) luminescent temperature probes were evaluated, aiming to design and optimize luminescence lifetime based nanothermometers. Temperature dependence of the luminescence lifetimes is induced by thermally activated phonon assisted energy transfer from the (2)F(5/2) state of Yb(3+) ions to the (4)F(3/2) state of Nd(3+) ions, which in turn is responsible for the significant quenching of the Yb(3+):(2)F(5/2) lifetime. It was also found that the thermal quenching and thus the relative sensitivity of the luminescent thermometer can be intentionally altered by the RE ions used (RE = Y, Lu, La, and Gd). The highest relative sensitivity was found to be S(R) = 1.22% K(−1) at 355 K for Nd(0.5)Y(0.4)Yb(0.1)PO(4) and it remains above 1% K(−1) up to 500 K. The high sensitivity and reliable thermometric performance of Nd(0.5)La(0.4)Yb(0.1)PO(4) were confirmed by the high reproducibility of the temperature readout and the temperature uncertainty being as low as δT = 0.05 K at 383 K. RSC 2021-06-14 /pmc/articles/PMC9418974/ /pubmed/36132339 http://dx.doi.org/10.1039/d1na00285f Text en This journal is © The Royal Society of Chemistry https://creativecommons.org/licenses/by/3.0/
spellingShingle Chemistry
Maciejewska, K.
Bednarkiewicz, A.
Marciniak, L.
NIR luminescence lifetime nanothermometry based on phonon assisted Yb(3+)–Nd(3+) energy transfer
title NIR luminescence lifetime nanothermometry based on phonon assisted Yb(3+)–Nd(3+) energy transfer
title_full NIR luminescence lifetime nanothermometry based on phonon assisted Yb(3+)–Nd(3+) energy transfer
title_fullStr NIR luminescence lifetime nanothermometry based on phonon assisted Yb(3+)–Nd(3+) energy transfer
title_full_unstemmed NIR luminescence lifetime nanothermometry based on phonon assisted Yb(3+)–Nd(3+) energy transfer
title_short NIR luminescence lifetime nanothermometry based on phonon assisted Yb(3+)–Nd(3+) energy transfer
title_sort nir luminescence lifetime nanothermometry based on phonon assisted yb(3+)–nd(3+) energy transfer
topic Chemistry
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9418974/
https://www.ncbi.nlm.nih.gov/pubmed/36132339
http://dx.doi.org/10.1039/d1na00285f
work_keys_str_mv AT maciejewskak nirluminescencelifetimenanothermometrybasedonphononassistedyb3nd3energytransfer
AT bednarkiewicza nirluminescencelifetimenanothermometrybasedonphononassistedyb3nd3energytransfer
AT marciniakl nirluminescencelifetimenanothermometrybasedonphononassistedyb3nd3energytransfer