2018
DOI: 10.1021/acs.inorgchem.8b02654
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Enhanced Red Emission in Er3+-Sensitized NaLuF4 Upconversion Crystals via Energy Trapping

Abstract: Luminescence efficiency of trivalent lanthanide-doped upconversion (UC) materials is significantly limited by luminescence concentration quenching. In this work, red UC emission is dramatically enhanced in Er 3+sensitized NaLuF 4 UC crystals through energy trapping under multiple excitation wavelengths. Cross-relaxation quenching and the energy migration to internal lattice defects are simultaneously suppressed by confining the excitation energy in the Er 3+ activator after introducing the Tm 3+ or Ho 3+ energ… Show more

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Cited by 29 publications
(10 citation statements)
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“…30 However, excessive doping of the Ho 3+ trapping center may increase the nonradiation loss, resulting in the decline of the emission intensity. 21 A similar result is obtained under 1532 nm NIR-II excitation (Fig. S3, ESI†).…”
Section: Resultssupporting
confidence: 78%
See 1 more Smart Citation
“…30 However, excessive doping of the Ho 3+ trapping center may increase the nonradiation loss, resulting in the decline of the emission intensity. 21 A similar result is obtained under 1532 nm NIR-II excitation (Fig. S3, ESI†).…”
Section: Resultssupporting
confidence: 78%
“…17–19 Specifically, for photodynamic therapy (PDT), chemical reactions can be induced by ultraviolet (UV)–blue emissions to kill tumor cells, 18,19 and red emission (600–700 nm) can be used for real-time imaging owing to its deep tissue penetration. 20–22 Kong's group reported a core–multishell UC nanophotoswitch, with which imaging-guided “off–on” therapy could be realized by UV–blue and red emissions under 980 and 808 nm excitations. 19 Li et al demonstrated mesoporous silica nanospheres with CaF 2 :Yb,Er UC nanocrystals entrapped in their porous structure, and they found that the coating of the thin MnO 2 layer may enhance the red-to-green ratio and red emission intensity, resulting in an efficient energy transfer to the loaded photosensitizer Chlorin e6 (Ce6), which favors the PDT.…”
Section: Introductionmentioning
confidence: 99%
“…Furthermore, we also demonstrated the possible mechanism of ET and BET processes, non-radiative transitions, and UC emissions under 808 nm excitation, as depicted in Figure 7 d. Unlike the processes under 980 nm excitation, firstly, the electrons in the ground state of Er 3+ were excited to the 4 I 9/2 state by GSA after absorbing an 808 nm photon, then reached the 4 I 11/2 state through a non-radiative transition. After that, the emitting states ( 2 H 11/2 , 4 S 3/2 and 4 F 9/2 ) could be populated by ETU, CR and BET processes, which were elaborated in Figure 5 [ 51 ]. In addition, the power dependence tendencies of the UCL in Y 2 O 3 :Er 3+ (8 mol%) and Y 2 O 3 :Er 3+ /Tm 3+ (8/1 mol%) UCNPs are given in Figure S4a,b , which indicates that all the UC emissions also exhibited a two-photon absorption process under 808 nm excitation.…”
Section: Resultsmentioning
confidence: 99%
“…The R/G ratio before the ion exchange is much larger than that after the ion exchange as the doping concentration of Tm 3+ is less than 1% (Figure e). It might due to the fact that the higher concentration of the OH – vibrations before the ion exchange can greatly depopulate the 4 I 11/2 excited state to the 4 I 13/2 excited state and further populate the 4 F 9/2 state by energy pumping with another 980 nm photon. ,, However, as the doping concentration of Tm 3+ is above 1%, the R/G ratio before the ion exchange increases quite smoothly while the R/G ratio after the ion exchange further increases sharply with the increase of Tm 3+ , and thus, the R/G ratio is obviously larger than that after the ion exchange. This is due to the fact that the OH – removal after the ion exchange effectively suppresses multiphonon nonradiative relaxation and accelerates the energy transfer between Er 3+ and Tm 3+ with the increase of Tm 3+ , which results in the enhanced R/G ratio .…”
Section: Resultsmentioning
confidence: 99%
“…Er 3+ -enriched upconversion materials usually demonstrate a high R/G ratio via the intense cross-relaxation among Er 3+ activators. In contrast to the conventional Yb 3+ -sensitized upconversion crystals, Er 3+ acts as both the sensitizer and activator. , Er 3+ -sensitized upconversion materials can be efficiently excited by multiband excitation in the near-infrared region (∼800, ∼980, and ∼1530 nm), which is essential for extending their applications . However, a high doping level of Er 3+ always causes a severe concentration quenching effect owing to fast energy migration from the sensitizers to the internal OH – defects and surface defects. An appropriate doping of Tm 3+ into the Er 3+ -enriched crystals not only favors the population of the 4 F 9/2 state and lifts the R/G ratio via the energy transfer between Er 3+ and Tm 3+ but also maximally minimizes this luminescence quenching effect as trapping excitation energies. ,, However, the main quenching pathway is still energy transfer to internal OH – defects because the internal OH – is easy to be introduced into the crystal lattice by substituting F – ions. ,, A commonly employed method for OH – removal is high-temperature annealing, but the morphology and size of the products are uncontrollable. Recently, the ion-exchange method is an attractive way to improve upconversion luminescence and preserve the crystal structure and monodispersed morphology well. A great amount of Na + and F – is essential for the ion exchange process, and the concentration of OH – defects can be greatly reduced by the replacement of F – ions.…”
Section: Introductionmentioning
confidence: 99%