What determines the performance of lanthanide-based ratiometric nanothermometers?
Luminescence intensity ratio (LIR) nanothermometers are ideally suited for noninvasive temperature detection of microelectronic devices and living cells, and the painstaking pursuit of new nanothermometers with higher absolute temperature sensitivity ( S a ) or relative temperature sensitivity ( S r...
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Published in | Nanoscale Vol. 12; no. 4; pp. 2776 - 2785 |
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Main Authors | , , , , |
Format | Journal Article |
Language | English |
Published |
Cambridge
Royal Society of Chemistry
22.10.2020
|
Subjects | |
Online Access | Get full text |
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Summary: | Luminescence intensity ratio (LIR) nanothermometers are ideally suited for noninvasive temperature detection of microelectronic devices and living cells, and the painstaking pursuit of new nanothermometers with higher absolute temperature sensitivity (
S
a
) or relative temperature sensitivity (
S
r
) has dominated recent research. However, whether higher
S
a
and
S
r
values can intrinsically improve the performance of LIR nanothermometers and what factors essentially determine their accuracy have rarely been considered; these considerations are instructive for their design and application while reducing time and costs. Here, we clarify that the accuracy of lanthanide-based LIR nanothermometers is essentially determined by
S
r
and the relative error of the luminescence intensity (
σI
/
I
) but not
S
a
based on lanthanide-doped NaYF
4
, YPO
4
, YVO
4
, CaF
2
, YF
3
, Y
2
O
3
, BaTiO
3
, LaAlO
3
and Y
3
Al
5
O
12
temperature sensors, meaning that our previous pursuit of higher
S
a
does not contribute to the accuracy of lanthanide-based LIR nanothermometers. Further research reveals that
σI
/
I
is primarily influenced by energy level splitting, which can deteriorate the temperature uncertainty. For actual temperature detection of biological tissues, in addition to the above intrinsic factors, we shed light on the effects of probe self-heating, excitation power density, emission intensity and penetration depth on temperature readouts
via
a polyethyleneimine-modified NaYF
4
:Er
3+
/Yb
3+
@NaYF
4
-PEI aqueous solution, implying that we will continue to optimize nanothermometers and calibrate readouts according to the local environment. This work unifies the metrics of lanthanide-based LIR nanothermometers, corrects the previous misunderstanding of
S
a
to mitigate invalid work, and provides careful guidance for their development.
This work unifies the metrics of lanthanide-based LIR nanothermometers, rectifies previous misunderstanding of
S
a
, and provides detailed guidance. |
---|---|
Bibliography: | a r S 10.1039/d0nr05035k and self-heating plots, TEM images, FT-IR spectra, temperature-recycle measurements and absorption spectrum. See DOI Electronic supplementary information (ESI) available: Characterization, temperature measurement parameters and fitting parameters, size distribution, power-dependent slope factors, XRD patterns, SEM micrographs, contour projection of thermal evolution spectra, fitting plots ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 |
ISSN: | 2040-3364 2040-3372 |
DOI: | 10.1039/d0nr05035k |