In this work, three series of micro-sized heterometallic europium-containing terephthalate MOFs, (Eu1-xLnx)2bdc3·nH2O (Ln = La, Gd, Lu), are synthesized via an ultrasound-assisted method in an ...aqueous medium. La3+ and Gd3+-doped terephthalates are isostructural to Eu2bdc3·4H2O. Lu3+-doped compounds are isostructural to Eu2bdc3·4H2O with Lu contents lower than 95 at.%. The compounds that are isostructural to Lu2bdc3·2.5H2O are formed at higher Lu3+ concentrations for the (Eu1-xLux)2bdc3·nH2O series. All materials consist of micrometer-sized particles. The particle shape is determined by the crystalline phase. All the synthesized samples demonstrate an “antenna” effect: a bright-red emission corresponding to the 5D0-7FJ transitions of Eu3+ ions is observed upon 310 nm excitation into the singlet electronic excited state of terephthalate ions. The fine structure of the emission spectra is determined by the crystalline phase due to the different local symmetries of the Eu3+ ions in the different kinds of crystalline structures. The photoluminescence quantum yield and 5D0 excited state lifetime of Eu3+ are equal to 11 ± 2% and 0.44 ± 0.01 ms, respectively, for the Ln2bdc3·4H2O structures. For the (Eu1-xLux)2bdc3·2.5H2O compounds, significant increases in the photoluminescence quantum yield and 5D0 excited state lifetime of Eu3+ are observed, reaching 23% and 1.62 ms, respectively.
A new series of luminescent heterometallic europium(III)–lutetium(III) terephthalate metal–organic frameworks, namely (EuxLu1−x)2bdc3·nH2O, was synthesized using a direct reaction in a water ...solution. At the Eu3+ concentration of 1–40 at %, the MOFs were formed as a binary mixture of the (EuxLu1−x)2bdc3 and (EuxLu1−x)2bdc3·4H2O crystalline phases, where the Ln2bdc3·4H2O crystalline phase was enriched by europium(III) ions. At an Eu3+ concentration of more than 40 at %, only one crystalline phase was formed: (EuxLu1−x)2bdc3·4H2O. All MOFs containing Eu3+ exhibited sensitization of bright Eu3+-centered luminescence upon the 280 nm excitation into a 1ππ* excited state of the terephthalate ion. The fine structure of the emission spectra of Eu3+ 5D0-7FJ (J = 0–4) significantly depended on the Eu3+ concentration. The luminescence quantum yield of Eu3+ was significantly larger for Eu-Lu terephthalates containing a low concentration of Eu3+ due to the absence of Eu-Eu energy migration and the presence of the Ln2bdc3 crystalline phase with a significantly smaller nonradiative decay rate compared to the Ln2bdc3·4H2O.
Luminescent, heterometallic terbium(III)–lutetium(III) terephthalate metal-organic frameworks (MOFs) were synthesized via direct reaction between aqueous solutions of disodium terephthalate and ...nitrates of corresponding lanthanides by using two methods: synthesis from diluted and concentrated solutions. For (TbxLu1−x)2bdc3·nH2O MOFs (bdc = 1,4-benzenedicarboxylate) containing more than 30 at. % of Tb3+, only one crystalline phase was formed: Ln2bdc3·4H2O. At lower Tb3+ concentrations, MOFs crystallized as the mixture of Ln2bdc3·4H2O and Ln2bdc3·10H2O (diluted solutions) or Ln2bdc3 (concentrated solutions). All synthesized samples that contained Tb3+ ions demonstrated bright green luminescence upon excitation into the 1ππ* excited state of terephthalate ions. The photoluminescence quantum yields (PLQY) of the compounds corresponding to the Ln2bdc3 crystalline phase were significantly larger than for Ln2bdc3·4H2O and Ln2bdc3·10H2O phases due to absence of quenching from water molecules possessing high-energy O-H vibrational modes. One of the synthesized materials, namely, (Tb0.1Lu0.9)2bdc3·1.4H2O, had one of the highest PLQY among Tb-based MOFs, 95%.
The luminescent coarse-, micro- and nanocrystalline europium(III) terephthalate tetrahydrate (Eu2bdc3·4H2O) metal-organic frameworks were synthesized by the ultrasound-assisted wet-chemical method. ...Electron micrographs show that the europium(III) terephthalate microparticles are 7 μm long leaf-like plates. According to the dynamic light scattering technique, the average size of the Eu2bdc3·4H2O nanoparticles is equal to about 8 ± 2 nm. Thereby, the reported Eu2bdc3·4H2O nanoparticles are the smallest nanosized rare-earth-based MOF crystals, to the best of our knowledge. The synthesized materials demonstrate red emission due to the 5D0–7FJ transitions of Eu3+ upon 250 nm excitation into 1ππ* state of the terephthalate ion. Size reduction results in broadened emission bands, an increase in the non-radiative rate constants and a decrease in both the quantum efficiency of the 5D0 level and Eu3+ and the luminescence quantum yields. Cu2+, Cr3+, and Fe3+ ions efficiently and selectively quench the luminescence of nanocrystalline europium(III) terephthalate, which makes it a prospective material for luminescent probes to monitor these ions in waste and drinking water.
Two series of β-NaYF4:Ln3+ nanoparticles (Ln = La–Nd, Sm–Lu) containing 20 at. % and 40 at. % of Ln3+ with well-defined morphology and size were synthesized via a facile citric-acid-assisted ...hydrothermal method using rare-earth chlorides as the precursors. The materials were composed from the particles that have a shape of uniform hexagonal prisms with an approximate size of 80–1100 nm. The mean diameter of NaYF4:Ln3+ crystals non-monotonically depended on the lanthanide atomic number and the minimum size was observed for Gd3+-doped materials. At the same time, the unit cell parameters decreased from La to Lu according to XRD data analysis. The diameter-to-length ratio increased from La to Lu in both studied series. The effect of the doping lanthanide(III) ion nature on particle size and shape was explained in terms of crystal growth dynamics. This study reports the correlation between the nanoparticle morphologies and the type and content of doping lanthanide ions. The obtained results shed light on the understanding of intrinsic factors’ effect on structural features of the nanocrystalline materials.
In this work, three series of micro-sized heterometallic europium-containing terephthalate MOFs, (Eusub.1-xLnsub.x)sub.2bdcsub.3·nHsub.2O (Ln = La, Gd, Lu), are synthesized via an ultrasound-assisted ...method in an aqueous medium. Lasup.3+ and Gdsup.3+-doped terephthalates are isostructural to Eusub.2bdcsub.3·4Hsub.2O. Lusup.3+-doped compounds are isostructural to Eusub.2bdcsub.3·4Hsub.2O with Lu contents lower than 95 at.%. The compounds that are isostructural to Lusub.2bdcsub.3·2.5Hsub.2O are formed at higher Lusup.3+ concentrations for the (Eusub.1-xLusub.x)sub.2bdcsub.3·nHsub.2O series. All materials consist of micrometer-sized particles. The particle shape is determined by the crystalline phase. All the synthesized samples demonstrate an “antenna” effect: a bright-red emission corresponding to the sup.5Dsub.0-sup.7Fsub.J transitions of Eusup.3+ ions is observed upon 310 nm excitation into the singlet electronic excited state of terephthalate ions. The fine structure of the emission spectra is determined by the crystalline phase due to the different local symmetries of the Eusup.3+ ions in the different kinds of crystalline structures. The photoluminescence quantum yield and sup.5Dsub.0 excited state lifetime of Eusup.3+ are equal to 11 ± 2% and 0.44 ± 0.01 ms, respectively, for the Lnsub.2bdcsub.3·4Hsub.2O structures. For the (Eusub.1-xLusub.x)sub.2bdcsub.3·2.5Hsub.2O compounds, significant increases in the photoluminescence quantum yield and sup.5Dsub.0 excited state lifetime of Eusup.3+ are observed, reaching 23% and 1.62 ms, respectively.
Luminescent, heterometallic terbium(III)-lutetium(III) terephthalate metal-organic frameworks (MOFs) were synthesized via direct reaction between aqueous solutions of disodium terephthalate and ...nitrates of corresponding lanthanides by using two methods: synthesis from diluted and concentrated solutions. For (Tbsub.xLusub.1−x)sub.2bdcsub.3·nHsub.2O MOFs (bdc = 1,4-benzenedicarboxylate) containing more than 30 at. % of Tbsup.3+, only one crystalline phase was formed: Lnsub.2bdcsub.3·4Hsub.2O. At lower Tbsup.3+ concentrations, MOFs crystallized as the mixture of Lnsub.2bdcsub.3·4Hsub.2O and Lnsub.2bdcsub.3·10Hsub.2O (diluted solutions) or Lnsub.2bdcsub.3 (concentrated solutions). All synthesized samples that contained Tbsup.3+ ions demonstrated bright green luminescence upon excitation into the sup.1ππ* excited state of terephthalate ions. The photoluminescence quantum yields (PLQY) of the compounds corresponding to the Lnsub.2bdcsub.3 crystalline phase were significantly larger than for Lnsub.2bdcsub.3·4Hsub.2O and Lnsub.2bdcsub.3·10Hsub.2O phases due to absence of quenching from water molecules possessing high-energy O-H vibrational modes. One of the synthesized materials, namely, (Tbsub.0.1Lusub.0.9)sub.2bdcsub.3·1.4Hsub.2O, had one of the highest PLQY among Tb-based MOFs, 95%.
A new series of luminescent heterometallic europium(III)–lutetium(III) terephthalate metal–organic frameworks, namely (Eusub.x Lusub.1−x )sub.2 bdcsub.3 ·nHsub.2 O, was synthesized using a direct ...reaction in a water solution. At the Eusup.3+ concentration of 1–40 at %, the MOFs were formed as a binary mixture of the (Eusub.x Lusub.1−x )sub.2 bdcsub.3 and (Eusub.x Lusub.1−x )sub.2 bdcsub.3 ·4Hsub.2 O crystalline phases, where the Lnsub.2 bdcsub.3 ·4Hsub.2 O crystalline phase was enriched by europium(III) ions. At an Eusup.3+ concentration of more than 40 at %, only one crystalline phase was formed: (Eusub.x Lusub.1−x )sub.2 bdcsub.3 ·4Hsub.2 O. All MOFs containing Eusup.3+ exhibited sensitization of bright Eusup.3+ -centered luminescence upon the 280 nm excitation into a sup.1 ππ* excited state of the terephthalate ion. The fine structure of the emission spectra of Eusup.3+ 5 Dsub.0 -sup.7 Fsub.J (J = 0–4) significantly depended on the Eusup.3+ concentration. The luminescence quantum yield of Eusup.3+ was significantly larger for Eu-Lu terephthalates containing a low concentration of Eusup.3+ due to the absence of Eu-Eu energy migration and the presence of the Lnsub.2 bdcsub.3 crystalline phase with a significantly smaller nonradiative decay rate compared to the Lnsub.2 bdcsub.3 ·4Hsub.2 O.
In this work, three series of micro-sized heterometallic europium-containing terephthalate MOFs, (Eu
Ln
)
bdc
·nH
O (Ln = La, Gd, Lu), are synthesized via an ultrasound-assisted method in an aqueous ...medium. La
and Gd
-doped terephthalates are isostructural to Eu
bdc
·4H
O. Lu
-doped compounds are isostructural to Eu
bdc
·4H
O with Lu contents lower than 95 at.%. The compounds that are isostructural to Lu
bdc
·2.5H
O are formed at higher Lu
concentrations for the (Eu
Lu
)
bdc
·nH
O series. All materials consist of micrometer-sized particles. The particle shape is determined by the crystalline phase. All the synthesized samples demonstrate an "antenna" effect: a bright-red emission corresponding to the
D
-
F
transitions of Eu
ions is observed upon 310 nm excitation into the singlet electronic excited state of terephthalate ions. The fine structure of the emission spectra is determined by the crystalline phase due to the different local symmetries of the Eu
ions in the different kinds of crystalline structures. The photoluminescence quantum yield and
D
excited state lifetime of Eu
are equal to 11 ± 2% and 0.44 ± 0.01 ms, respectively, for the Ln
bdc
·4H
O structures. For the (Eu
Lu
)
bdc
·2.5H
O compounds, significant increases in the photoluminescence quantum yield and
D
excited state lifetime of Eu
are observed, reaching 23% and 1.62 ms, respectively.
Two series of β-NaYFsub.4:Lnsup.3+ nanoparticles (Ln = La-Nd, Sm-Lu) containing 20 at. % and 40 at. % of Lnsup.3+ with well-defined morphology and size were synthesized via a facile ...citric-acid-assisted hydrothermal method using rare-earth chlorides as the precursors. The materials were composed from the particles that have a shape of uniform hexagonal prisms with an approximate size of 80-1100 nm. The mean diameter of NaYFsub.4:Lnsup.3+ crystals non-monotonically depended on the lanthanide atomic number and the minimum size was observed for Gdsup.3+-doped materials. At the same time, the unit cell parameters decreased from La to Lu according to XRD data analysis. The diameter-to-length ratio increased from La to Lu in both studied series. The effect of the doping lanthanide(III) ion nature on particle size and shape was explained in terms of crystal growth dynamics. This study reports the correlation between the nanoparticle morphologies and the type and content of doping lanthanide ions. The obtained results shed light on the understanding of intrinsic factors' effect on structural features of the nanocrystalline materials.
PDF
