Mirijam Lederer, Maximilian Stremel, Ian Pompermayer Machado, Tom Förster, Syed S Razi, Markus Suta, Anna M Kaczmarek
{"title":"了解LiLuF4:Tm3+,Yb3的测温行为。","authors":"Mirijam Lederer, Maximilian Stremel, Ian Pompermayer Machado, Tom Förster, Syed S Razi, Markus Suta, Anna M Kaczmarek","doi":"10.1039/d5tc01916h","DOIUrl":null,"url":null,"abstract":"<p><p>The Er<sup>3+</sup>, Yb<sup>3+</sup> upconversion couple, with its background-free green emission arising from the two thermally coupled <sup>2</sup>H<sub>11/2</sub> and <sup>4</sup>S<sub>3/2</sub> levels of Er<sup>3+</sup>, is a classic \"workhorse\" example of luminescent Boltzmann thermometry. In contrast, the Tm<sup>3+</sup>, Yb<sup>3+</sup> couple remains far less established. The Tm<sup>3+</sup>, Yb<sup>3+</sup> system offers an intense <sup>3</sup>H<sub>4</sub> → <sup>3</sup>H<sub>6</sub> electronic transition (800 nm) as a possible reference emission for UC thermometry in the NIR-I window. However, the Tm<sup>3+</sup>, Yb<sup>3+</sup> thermometry system has not yet been fully understood, limiting its potential application in medical and biological contexts, as well as in nanoelectronics, nanophotonics and in general industrial settings. In this work, we demonstrate how to exploit the temperature-dependent multiphonon relaxation from the <sup>3</sup>F<sub>3</sub> to the <sup>3</sup>H<sub>4</sub> level of Tm<sup>3+</sup>. This relaxation is fed by energy transfer from Yb<sup>3+</sup> and gives rise to two emission lines at 680 nm and 800 nm. Taking LiLuF<sub>4</sub>:1% Tm, 30% Yb as a representative example, we analyzed both micro- and nanocrystalline samples to elucidate how surface-attached ligands with higher vibrational energies than the low cutoff phonon energies (∼500 cm<sup>-1</sup>) of the fluoride matrix itself have on the Boltzmann thermometry behaviour. We show that Tm<sup>3+</sup> can only work as a wide-range Boltzmann thermometer in microcrystalline, ligand-free samples with host compounds of sufficiently low cutoff phonon energies and that its action is limited in nanocrystalline systems. A combination of experimental studies and kinetic modelling helps us to elucidate clear-cut guidelines for optimizing the performance of the Tm<sup>3+</sup>, Yb<sup>3+</sup> system as a luminescent thermometer and to compare this UC system to the well-established \"workhorse\" of the Er<sup>3+</sup>, Yb<sup>3+</sup> UC couple.</p>","PeriodicalId":84,"journal":{"name":"Journal of Materials Chemistry C","volume":" ","pages":""},"PeriodicalIF":5.1000,"publicationDate":"2025-09-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC12516696/pdf/","citationCount":"0","resultStr":"{\"title\":\"Understanding the thermometric behaviour of LiLuF<sub>4</sub>:Tm<sup>3+</sup>,Yb<sup>3</sup>.\",\"authors\":\"Mirijam Lederer, Maximilian Stremel, Ian Pompermayer Machado, Tom Förster, Syed S Razi, Markus Suta, Anna M Kaczmarek\",\"doi\":\"10.1039/d5tc01916h\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p><p>The Er<sup>3+</sup>, Yb<sup>3+</sup> upconversion couple, with its background-free green emission arising from the two thermally coupled <sup>2</sup>H<sub>11/2</sub> and <sup>4</sup>S<sub>3/2</sub> levels of Er<sup>3+</sup>, is a classic \\\"workhorse\\\" example of luminescent Boltzmann thermometry. In contrast, the Tm<sup>3+</sup>, Yb<sup>3+</sup> couple remains far less established. The Tm<sup>3+</sup>, Yb<sup>3+</sup> system offers an intense <sup>3</sup>H<sub>4</sub> → <sup>3</sup>H<sub>6</sub> electronic transition (800 nm) as a possible reference emission for UC thermometry in the NIR-I window. However, the Tm<sup>3+</sup>, Yb<sup>3+</sup> thermometry system has not yet been fully understood, limiting its potential application in medical and biological contexts, as well as in nanoelectronics, nanophotonics and in general industrial settings. In this work, we demonstrate how to exploit the temperature-dependent multiphonon relaxation from the <sup>3</sup>F<sub>3</sub> to the <sup>3</sup>H<sub>4</sub> level of Tm<sup>3+</sup>. This relaxation is fed by energy transfer from Yb<sup>3+</sup> and gives rise to two emission lines at 680 nm and 800 nm. Taking LiLuF<sub>4</sub>:1% Tm, 30% Yb as a representative example, we analyzed both micro- and nanocrystalline samples to elucidate how surface-attached ligands with higher vibrational energies than the low cutoff phonon energies (∼500 cm<sup>-1</sup>) of the fluoride matrix itself have on the Boltzmann thermometry behaviour. We show that Tm<sup>3+</sup> can only work as a wide-range Boltzmann thermometer in microcrystalline, ligand-free samples with host compounds of sufficiently low cutoff phonon energies and that its action is limited in nanocrystalline systems. 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Understanding the thermometric behaviour of LiLuF4:Tm3+,Yb3.
The Er3+, Yb3+ upconversion couple, with its background-free green emission arising from the two thermally coupled 2H11/2 and 4S3/2 levels of Er3+, is a classic "workhorse" example of luminescent Boltzmann thermometry. In contrast, the Tm3+, Yb3+ couple remains far less established. The Tm3+, Yb3+ system offers an intense 3H4 → 3H6 electronic transition (800 nm) as a possible reference emission for UC thermometry in the NIR-I window. However, the Tm3+, Yb3+ thermometry system has not yet been fully understood, limiting its potential application in medical and biological contexts, as well as in nanoelectronics, nanophotonics and in general industrial settings. In this work, we demonstrate how to exploit the temperature-dependent multiphonon relaxation from the 3F3 to the 3H4 level of Tm3+. This relaxation is fed by energy transfer from Yb3+ and gives rise to two emission lines at 680 nm and 800 nm. Taking LiLuF4:1% Tm, 30% Yb as a representative example, we analyzed both micro- and nanocrystalline samples to elucidate how surface-attached ligands with higher vibrational energies than the low cutoff phonon energies (∼500 cm-1) of the fluoride matrix itself have on the Boltzmann thermometry behaviour. We show that Tm3+ can only work as a wide-range Boltzmann thermometer in microcrystalline, ligand-free samples with host compounds of sufficiently low cutoff phonon energies and that its action is limited in nanocrystalline systems. A combination of experimental studies and kinetic modelling helps us to elucidate clear-cut guidelines for optimizing the performance of the Tm3+, Yb3+ system as a luminescent thermometer and to compare this UC system to the well-established "workhorse" of the Er3+, Yb3+ UC couple.
期刊介绍:
The Journal of Materials Chemistry is divided into three distinct sections, A, B, and C, each catering to specific applications of the materials under study:
Journal of Materials Chemistry A focuses primarily on materials intended for applications in energy and sustainability.
Journal of Materials Chemistry B specializes in materials designed for applications in biology and medicine.
Journal of Materials Chemistry C is dedicated to materials suitable for applications in optical, magnetic, and electronic devices.
Example topic areas within the scope of Journal of Materials Chemistry C are listed below. This list is neither exhaustive nor exclusive.
Bioelectronics
Conductors
Detectors
Dielectrics
Displays
Ferroelectrics
Lasers
LEDs
Lighting
Liquid crystals
Memory
Metamaterials
Multiferroics
Photonics
Photovoltaics
Semiconductors
Sensors
Single molecule conductors
Spintronics
Superconductors
Thermoelectrics
Topological insulators
Transistors