Tunable multicolor and white‐light upconversion luminescence in Yb3+/Tm3+/Ho3+ tri‐doped NaYF4 micro‐crystals

NaYF₄ micro‐crystals with various concentrations of Yb³⁺/Tm³⁺/Ho³⁺ were prepared successfully via a simple and reproducible hydrothermal route using EDTA as the chelating agent. Their phase structure and surface morphology were studied using powder X‐ray diffraction (XRD) and scanning electron microscopy (SEM). The XRD patterns revealed that all the samples were pure hexagonal phase NaYF₄. SEM images showed that Yb³⁺/Tm³⁺/Ho³⁺ tri‐doped NaYF₄ were hexagonal micro‐prisms. Upconversion photoluminescence spectra of Yb³⁺/Tm³⁺/Ho³⁺ tri‐doped NaYF₄ micro‐crystals with various dopant concentrations under 980 nm excitation with a 665 mW pump power were studied. Tunable multicolor (purple, purplish blue, yellowish green, green) and white light were achieved by simply adjusting the Ho³⁺ concentration in 20%Yb³⁺/1%Tm³⁺/xHo³⁺ tri‐doped NaYF₄ micro‐crystals. Furthermore, white‐light emissions could be obtained using different pump powers in 20%Yb³⁺/1%Tm³⁺/1%Ho³⁺ tri‐doped NaYF₄ micro‐crystals at 980 nm excitation. The pump power‐dependent intensity relationship was studied and relevant energy transfer processes were discussed in detail. The results suggest that Yb³⁺/Tm³⁺/Ho³⁺ tri‐doped NaYF₄ micro‐crystals have potential applications in optoelectronic devices such as photovoltaic, plasma display panel and white‐light‐emitting diodes. Copyright © 2014 John Wiley & Sons, Ltd.     

Visible‐near‐infrared luminescent lanthanide ternary complexes based on beta‐diketonate using visible‐light excitation

We used the synthesized dinaphthylmethane (Hdnm) ligand whose absorption extends to the visible‐light wavelength, to prepare a family of ternary lanthanide complexes, named as [Ln(dnm)₃phen] (Ln = Sm, Nd, Yb, Er, Tm, Pr). The properties of these complexes were investigated by Fourier transform infrared (FT‐IR) spectroscopy, diffuse reflectance (DR) spectroscopy, thermogravimetric analyses, and excitation and emission spectroscopy. Generally, excitation with visible light is much more advantageous than UV excitation. Importantly, upon excitation with visible light (401–460 nm), the complexes show characteristic visible (Sm³⁺) as well as near‐infrared (Sm³⁺, Nd³⁺, Yb³⁺, Er³⁺, Tm³⁺, Pr³⁺) luminescence of the corresponding lanthanide ions, attributed to the energy transfer from the ligands to the lanthanide ions, an antenna effect. Now, using these near‐infrared luminescent lanthanide complexes, the luminescent spectral region from 800 to 1650 nm, can be covered completely, which is of particular interest for biomedical imaging applications, laser systems, and optical amplification applications. Copyright © 2015 John Wiley & Sons, Ltd.     

Enhancement of near‐infrared up‐conversion and blue down‐conversion luminescence in LuNbO4:Yb3+,Tm3+ with Ga3+ and Ta5+ substitutions

Under a 980‐nm excitation, the up‐conversion (UC) spectra of LuNbO₄:Yb³⁺,Tm³⁺ powders exhibited predominantly near‐infrared bands (~805 nm) of Tm³⁺ through an energy transfer process from Yb³⁺ to Tm³⁺. Regarding the down‐conversion (DC) luminescence of the powders, the photoluminescence excitation spectra consisted of a broad charge transfer band (270 nm) due to [NbO₄]^3? and sharp band (360 nm) of Tm³⁺, while the corresponding emission spectra exhibited a blue emission at 458 nm. Upon substitution of Ga³⁺ and Ta⁵⁺ for Lu³⁺ and Nb⁵⁺, respectively, both UC and DC luminescence properties were significantly enhanced. For the Ga³⁺ substitution, the increased emission intensity could be explained by the crystal field asymmetry surrounding the Tm³⁺ ions induced by the large difference in ionic radius between Ga³⁺ and Lu³⁺. For the Ta⁵⁺ substitution, we believe that an M′‐LuTaO₄ substructure was formed in the host, which led to the formation of a TaO₆ octahedral coordination instead of a NbO₄ tetrahedral coordination. Consequently, the crystal symmetry of the local structure was modified, and thus the UC and DC luminescence properties were enhanced. The dual‐mode (UC and DC) luminescence demonstrates that LuNbO₄:Yb³⁺,Tm³⁺ has a great potential in the fields of temperature sensing probes, anti‐counterfeiting, and bioapplications.     

Effect of Bi3+ addition on the upconversion luminescence properties of NaYbF4:Er

In this study, Bi³⁺ incorporation in NaYbF₄:Er lattice and its influence on upconversion luminescence properties have been investigated in detail using techniques such as temperature‐dependent luminescence, Fourier transform infrared spectroscopy and X‐ray diffraction (XRD). The study was carried out to develop phosphors with improved upconversion luminescence. From photoluminescence and lifetime measurements it is inferred that luminescence intensity from NaYbF₄:Er increases with Bi³⁺ addition. The sample containing 50 at.% Bi³⁺ ions exhibited optimum upconversion luminescence. Increased distance between Yb³⁺–Yb³⁺ and Er³⁺–Er³⁺ due to Bi³⁺ incorporation into the lattice and associated decrease in the extent of dipolar interaction/self‐quenching are responsible for increase in lifetime values and luminescence intensities from Er³⁺ ions. Incorporation of Bi³⁺ into NaYbF₄:Er lattice reduced self‐quenching among Yb³⁺–Yb³⁺ions and this facilitated energy transfer from Yb³⁺ to Er³⁺. This situation also explains decrease in the extent of temperature‐assisted quenching of emission from thermally coupled ²H_11/2 and ⁴S_3/2 levels of Er³⁺. Based on Rietveld refinement of XRD patterns it was confirmed that a maximum of 10 at.% of Bi³⁺added was incorporated into the NaYbF₄:Er lattice and the remaining complex co‐exists as a BiOF phase. These results are of significant interest in the area of development of phosphors based on Yb³⁺–Er³⁺ upconversion luminescence.     

Upconverted photoluminescence in Ho3+ and Yb3+ codoped Gd2O3 nanocrystals with and without Li+ ions

The upconversion photoluminescence of Ho³⁺ ion sensitized by Yb³⁺ ion in Ho³⁺/Yb³⁺codoped Gd₂O₃ nanocrystals with and without Li⁺ is investigated in this paper. Strong fluorescence in the green (534–570 nm) and red (635–674 nm) regions of the spectrum has been observed, arising from the ⁵F₄/⁵S₂ → ⁵I₈ and ⁵F₅ → ⁵I₈ transitions of Ho³⁺ ion, respectively. Yb³⁺ ion is considered to be a better sensitizer for catching enough pumping energy and transferring considerable energy to Ho³⁺ in the Ho³⁺/Yb³⁺system. The upconversion intensity emitted by Ho³⁺ is greatly enhanced when Li⁺ is added to the Ho³⁺/Yb³⁺ codoped Gd₂O₃ nanocrystals.     

Synthesis,Structural Characterization,and Chiroptical Studies of Bidentate Salen‐Type Lanthanide (III) Complexes

The salen‐type ligand prepared with (R,R) diphenylethan‐1,2‐diamine and salicylaldehyde provides stable and inert complexes KLnL₂ upon simple reaction with lanthanide halides or pseudohalides LnX₃ (Ln = Tb³⁺‐Lu³⁺; X = Cl^? or TfO^?) of its potassium salt. All the complexes were completely characterized through nuclear magnetic resonance (NMR), electronic circular dichroism (ECD) in the UV and some (Er³⁺, Tm³⁺, Yb³⁺) also with Near‐IR ECD (NIR‐ECD) and luminescence (Tb³⁺, Tm³⁺). Careful analysis of the NMR shifts demonstrated that the complexes are isostructural in solution and afforded an accurate geometry. This was further confirmed by means of Density Functional Theory (DFT) optimization of the Lu³⁺ complex, and by comparing the ligand‐centered experimental and time‐dependent TD‐DFT computed UV‐ECD spectra. As final validation, we used the NIR‐ECD spectrum of the Yb³⁺ derivative calculated by means of Richardson's equations. The excellent match between calculated and experimental ECD spectra confirm the quality of the NMR structure.  Chirality 27:857–863, 2015. © 2015 Wiley Periodicals, Inc.     

Sensitive detection of sulfide ions in red region based on luminescence resonance energy transfer between upconversion nanoparticles and dye‐670

Many sulfides are toxic substances that easily harm the respiratory tract, therefore affecting respiratory function or damaging other organs of the body, leading to its failure. Therefore, there is a pressing need to develop methods for sensitive detection of sulfur ions (S^2?). Based on luminescence resonance energy transfer (LRET) theory, we report the construction of a near‐infrared (NIR) excitation luminescence probe using NaGdF₄:Yb³⁺,Er³⁺@NaYF₄ upconversion nanoparticles (UCNPs) as the donor and dye‐670 as the receptor for detection of S^2?. When UCNPs and dye‐670 molecules were combined using ligand exchange and electrostatic attraction, LRET occurred and UCNP luminescence was quenched. When S^2? was added to the system, sulfide ions were able to destroy the double bond of the dye, inhibiting LRET and restoring UCNP luminescence. Under optimum condition, the linear range of S^2? detection was 0.65–18.2 μM, and the detection limit was 34.2 nM. This method was applied for determination of S^2? in water with satisfactory results.     

Novel gaseous polyatomic binary and ternary lanthanide oxides

A variety of novel gaseous polyatomic binary and ternary oxides were observed at ambient temperature arising from lanthanide (Ln) nitrate Schiff base complexes, simple salts and sesquioxides, in an FAB mass spectrometer. The new binary oxides (as singly positive ions) detected are Ln₂O₃, Ln₃O₃, Ln₃O₄, Ln₄O₄, Ln₄O₅, Ln₄O₆, Ln₅O₆, Ln₅O₇, Ln₅O₈, Ln₆O₈, Ln₆O₉, Ln₇O₁₀, Ln₈O₁₁, Ln₈O₁₂ and Ln₉O₁₃; the ternary gaseous oxides are CeEuO₂, CeEu₂O₃ and Ce₂EuO₄, LaYbO₂, La₂YbO₄ and LaYb₂O₄; NdHoO₃, Nd₂HoO₄, and NdHo₂O₄; YTmO₃; Y_xTm_3−xO₄, x=1−2; Y_xTm_4−xO₆, x=1−3; Y_xTm_5−xO₇, x=1−4; Y_xTm_6−xO₉, x=1−5. Some of these oxides show the lanthanide cations in unusual oxidation states. Gadolinium-gallium ternary oxides, GdGaO₂, GdGaO₃ and Gd₂GaO₄ were also detected. The FAB MS environment is significantly reducing, yielding a homologous series Eu_nO_n where Eu²⁺ is dominant (E°(Eu³⁺/Eu²⁺)=−0.35 V) and no gallium or indium oxides (E°(M³⁺/M°=−0.34 V (In), −0.53 V (Ga)) were formed. The stoichiometry of the polylanthanide ternary oxides formed is determined largely by the chemistry of the major metallic component. The gaseous polyatomic oxides are probably formed through a reductive condensation process involving primary species Ln⁺ and LnO⁺ formed when the rare earth compounds are struck by fast Xe atoms. The demonstrated possibility of double component oxide formation broadens the number and types of gaseous lanthanide oxides which are accessible.     

Enhancement of Cerenkov Luminescence Imaging by Dual Excitation of Er3+, Yb3+-Doped Rare-Earth Microparticles

Cerenkov luminescence imaging (CLI) has been successfully utilized in various fields of preclinical studies; however, CLI is challenging due to its weak luminescent intensity and insufficient penetration capability. Here, we report the design and synthesis of a type of rare-earth microparticles (REMPs), which can be dually excited by Cerenkov luminescence (CL) resulting from the decay of radionuclides to enhance CLI in terms of intensity and penetration. Methods: Yb³⁺- and Er³⁺- codoped hexagonal NaYF₄ hollow microtubes were synthesized via a hydrothermal route. The phase, morphology, and emission spectrum were confirmed for these REMPs by power X-ray diffraction (XRD), scanning electron microscopy (SEM), and spectrophotometry, respectively. A commercial CCD camera equipped with a series of optical filters was employed to quantify the intensity and spectrum of CLI from radionuclides. The enhancement of penetration was investigated by imaging studies of nylon phantoms and nude mouse pseudotumor models. Results: the REMPs could be dually excited by CL at the wavelengths of 520 and 980 nm, and the emission peaks overlaid at 660 nm. This strategy approximately doubled the overall detectable intensity of CLI and extended its maximum penetration in nylon phantoms from 5 to 15 mm. The penetration study in living animals yielded similar results. Conclusions: this study demonstrated that CL can dually excite REMPs and that the overlaid emissions in the range of 660 nm could significantly enhance the penetration and intensity of CL. The proposed enhanced CLI strategy may have promising applications in the future.     

Magnetic nanobead-based immunoassay for the simultaneous detection of aflatoxin B1 and ochratoxin A using upconversion nanoparticles as multicolor labels

A novel and sensitive immunoassay for the simultaneous detection of aflatoxin B₁ (AFB₁) and ochratoxin A (OTA) in food samples was developed by using artificial antigen-modified magnetic nanoparticles (MNPs) as immunosensing probes and antibody functionalized upconversion nanoparticles (UCNPs) as signal probes. NaY_0.78F₄:Yb_0.2, Tm_0.02 and NaY_0.28F₄:Yb_0.7,Er_0.02 UCNPs were prepared and functionalized, respectively, with immobilized monoclonal anti-AFB₁ antibodies and anti-OTA antibodies as signal probes. Based on a competitive immunoassay format, the detection limit for both AFB₁ and OTA under optimal conditions was as low as 0.01 ng mL⁻¹, and the effective detection range was from 0.01 to 10 ng mL⁻¹. The proposed method was successfully applied to measure AFB₁ and OTA in naturally contaminated maize samples and compared to a commercially available ELISA method. The high sensitivity and selectivity of this method is due to the magnetic separation and concentration effect of the MNPs, the high sensitivity of the UCNPs, and the different emission lines of Yb/Tm and Yb/Er doped NaYF₄ UCNPs excited by 980 nm laser. Multicolor UCNPs have the potential to be used in other applications for detecting toxins in the field of food safety and other fields.     

Luminescence properties of Tm3+ ions single‐doped YF3 materials in an unconventional excitation region

According to the spectral distribution of solar radiation at the earth's surface, under the excitation region of 1150 to 1350 nm, the up‐conversion luminescence of Tm³⁺ ions was investigated. The emission bands were matched well with the spectral response region of silicon solar cells, achieved by Tm³⁺ ions single‐doped yttrium fluoride (YF₃) phosphor, which was different from the conventional Tm³⁺/Yb³⁺ ion couple co‐doped materials. Additionally, the similar emission bands of Tm³⁺ ions were achieved under excitation in the ultraviolet region. It is expected that via up‐conversion and down‐conversion routes, Tm³⁺‐sensitized materials could convert photons to the desired wavelengths in order to reduce the energy loss of silicon solar cells, thereby enhancing the photovoltaic efficiency.     

Enhanced green emissions of Er3+/Yb3+ co‐doped Gd2(MoO4)3 by co‐excited up‐conversion processes

Improving the emission from rare earth ions doped materials is of great importance to broaden their application in bio‐imaging, photovoltaics and temperature sensing. The green emissions of Gd₂(MoO₄)₃:Er³⁺/Yb³⁺ powder upon co‐excitation with 980 and 808 nm lasers were investigated in this paper. Distinct enhancement of green emissions was observed compared with single laser excitation. Based on the energy level structure of Er³⁺, the enhancement mechanism was discussed. Moreover, the result of temperature‐dependent enhancement revealed that the enhancement factor reached its maximum (2.5) as the sample heated to 120°C, which is due to the competition of two major thermal effects acting in the co‐excited up‐conversion processes. In addition, the same enhancement of green emissions was also observed in Gd₂(MoO₄)₃:Er³⁺ powder and NaYF₄:Er³⁺/Yb³⁺ powder.     

Pure red upconverted and near-infrared luminescence properties of Er3+-doped SnO2 nanocrystals for lighting applications

Tin oxide (SnO₂) nanocrystalline powders doped with erbium ion (Er³⁺) in different molar ratios (0, 3, 5, and 7 mol%) were prepared using a solid-state reaction technique. These samples were characterized by X-ray diffraction (XRD), scanning electron microscopy (SEM), ultraviolet-visible absorption, visible upconversion, and near-infrared luminescence techniques. XRD analysis revealed the tetragonal rutile structure of SnO₂ and the average crystallite size was about 32 nm. From Tauc's plots, it was confirmed that the substitution of Er³⁺ ions into the SnO₂ host lattice resulted in the narrowing its band gap. Optical absorption bands at 520 and 654 nm correspond to the 4f electron transitions of Er³⁺ further confirming visible light absorption. Infrared luminescence spectra showed a broad band centred at 1536 nm which is assigned to the ⁴I_13/2 → ⁴I_15/2 transition of Er³⁺. Visible upconverted emission spectra under 980 nm excitation exhibit a strong red luminescence with a main peak at 672 nm which is attributed to the ⁴F_9/2 → ⁴I_15/2 transition of Er³⁺. Power-dependent upconversion spectra confirmed that two photons participated in the upconversion mechanism. Enhancement in the intensities of both visible and infrared luminescence was observed when raising the concentration. The results pave the way for the potential applications of these nanocrystalline powders in energy harvesting applications such as infrared light upconverting layer in solar cells, light emitting diodes, infrared broadband sources and amplifiers, and biological labelling.     

Heterobinuclear Zn‐Ln (Ln = La,Nd, Eu,Gd, Tb,Er and Yb) complexes based on asymmetric Schiff‐base ligand: synthesis,characterization and photophysical properties

With a novel asymmetric Schiff‐base zinc complex ZnL (H₂L = N‐(3‐methoxysalicylidene)‐N′‐(5‐bromo‐3‐methoxysalicylidene)phenylene‐1,2‐diamine), obtained from phenylene‐1,2‐diamine, 3‐methoxysalicylaldehyde and 5‐bromo‐3‐methoxysalicylaldehyde, as the precursor, a series of heterobinuclear Zn‐Ln complexes [ZnLnL(NO₃)₃(CH₃CN)] (Ln = La, 1; Ln = Nd, 2; Ln = Eu, 3; Ln = Gd, 4; Ln = Tb, 5; Ln = Er, 6; Ln = Yb, 7) were synthesized by the further reaction with Ln(NO₃)₃·6H₂O, and characterized by Fourier transform‐infrared, fast atom bombardment mass spectroscopy and elemental analysis. Photophysical studies of these complexes show that the strong and characteristic near‐infrared luminescence of Nd³⁺, Yb³⁺and Er³⁺ with emissive lifetimes in the microsecond range has been sensitized from the excited state of the asymmetric Schiff‐base ligand due to effective intramolecular energy transfer; the other complexes do not show characteristic emission due to the energy gap between the chromophore and lanthanide ions. Copyright © 2012 John Wiley & Sons, Ltd.     

Intense visible multicolored luminescence from lanthanide ion‐pair codoped NaGdF4 nanocrystals

Lanthanide ion‐pair (Eu³⁺/Tb³⁺, Dy³⁺/Tb³⁺, Sm³⁺/Tb³⁺ and Eu³⁺/Dy³⁺) codoped NaGdF₄ nanocrystals using Ce³⁺ as the sensitizer were prepared via the polyol method. The nanocrystals with different codoped lanthanide ion‐pairs retain their individual optical properties and the combined spectra can be detected using single‐wavelength excitation at about 251 nm. The combined spectra intensity ratios can be adjusted through control of the doping ions molar ratios. Excited with a UV lamp at 254 nm, the as‐prepared nanocrystals in aqueous solution emit intense visible emissions of different colors. The nanocrystals were coated with SiO₂, to make them biocompatible. Copyright © 2009 John Wiley & Sons, Ltd.     

Synthesis, structure and spectroscopic properties of chloranilate-bridged 4f-4f dinuclear complexes: a comparative study of the emission properties with Cr-Ln complexes

New 4f-4f chloranilate-bridged dinuclear Ln^III complexes, [(HBpz₃)₂Ln(μ-C₆Cl₂O₄)Ln(HBpz₃)₂] (Ln(CA)Ln: Ln=Eu, Tb, Yb), were synthesized and characterized by the X-ray analysis. Their structure and spectroscopic properties were compared with those of dinuclear 3d-4f assembled molecular systems [(acac)₂Cr^III(μ-ox)Ln^III(HBpz₃)₂] (Cr(ox)Ln: acac⁻=acetylacetonate, ox²⁻=oxalate, HBpz₃ ⁻=hydrotris(pyrazol-1-yl)borate) and [(acac)₂Cr(μ-bpypz)Ln(hfac)₃] (Cr(bpypz)Ln: bpypz⁻=3,5-di(2-pyridyl)pyrazolate, hfac=hexafluoroacetylacetonate). The complex Yb(CA)Yb shows strong 4f-4f emission due to the ligand to metal energy transfer from the triplet state of the CA²⁻ to the excited 4f state of Yb^III. On the other hand, the observation of only the 4f-4f emission in the Cr(bpypz)Yb complex is in contrast to the simultaneous observation of the low temperature 3d-3d and 4f-4f emissions associated with the energy transfer from Cr^III to Yb^III in the Cr(ox)Yb complexes. This indicates that the energy transfer from Cr^III to Yb^III is faster in the Cr(bpypz)Yb as compared to that in the Cr(ox)Yb even at low temperatures leading to the stronger 4f-4f luminescence in the former complex. No observation of either Tb^IIIor Eu^III emission in the Tb(CA)Tb or Eu(CA)Eu complexes suggests the energy transfer or back-transfer from the Tb or Eu ions to the CA²⁻ moiety. Conversely, the Cr(bpypz)Eu and Cr(bpypz)Tb complexes show 3d-3d emissions as similarly to the corresponding Cr(ox)Eu and Cr(ox)Tb complexes; indicating the energy transfer from the Eu or Tb to the Cr^III moiety.     

Magnetic and luminescence characteristics of dinuclear complexes of lanthanides and a phenolic schiff base macrocyclic ligand

The magnetic and luminescence characteristics of trimorphic homodinuclear macrocyclic complexes of lanthanides and a 2:2 phenolate Schiff's base L, derived from 2,6-diformyl-p-cresol and triethylenetetramine were determined. The complexes of Pr³⁺ exhibit non-Curie-Weiss temperature dependent magnetic susceptibilities for which satisfactory fits to an axial relationship depends on crystal field splitting and a weak binuclear Pr³⁺Pr³⁺ antiferromagnetic interaction. The exchange interaction parameters are zJ′ = −2.2, −4.4 and −7.0 cm ⁻¹ for ‘off-white’ Pr₂L(NO₃)₄·2H₂O, ‘yellow’ Pr₂L(NO₃)₄, and ‘orange’ Pr₂L(NO₃)₂(OH)₂, respectively. In contrast, magnetic susceptibilities of the Ln₂L(NO₃)₃(OH) complexes (Ln = Dy, Ho) follow Curie-Weiss behavior over the entire temperature range (6 K to 300 K). The complexes of closed shell ions La³⁺, Lu³⁺, Y³⁺ and those of the half filled shell ion Gd³⁺ exhibit a strong ligand fluorescence in the 450 nm to 650 nm range with decay times at 77 K of 5–8 ns for Ln≠Gd or 2–4 ns for Ln = Gd. The complexes of Gd³⁺ also exhibit a phosphorescence at 600 nm (decay time ∼ 200 μs). The complexes containing Ce³⁺, Eu³⁺, Tb³⁺ and Er³⁺ show very weak ligand luminescence indicative of effective quenching processes. Sensitized emission from the lanthanide ion is observed only with the Eu³⁺ complexes (⁵D_o → ⁷F_j transitions). The emission lifetimes are on the order of 250 μs in the pure Eu³⁺ complexes. The emission decay curves from dilute samples of Eu³⁺ in ‘off-white’ La₂L(NO₃)_4nH₂O show a noticeable rise time as well as a biphasic decay (fast component ∼ 400 μs; slow component ∼ 2500 μs). The luminescing states of L and Eu³⁺ have a common excitation spectrum which is similar to the electronic absorption spectrum of L indicating that ligand-to-metal ion energy transfer processes are dominant. Overall the result if this study suggest that the spectral properties of the complexes are determined by the coordination mode of the lanthanide ions to the Schiff base portion of macrocyclic ligand.     

The transport kinetics of lanthanide species in a single erythrocyte probed by confocal laser scanning microscopy

 A novel method has been developed to visualize and follow the temporal course of lanthanide transport across the membrane into a single living erythrocyte. By means of confocal scanning microscopy and the optical section technique, the entry of lanthanide ions was followed by the fluorescence quenching of fluorescein isothiocyanate (FITC)-labeled membrane and cytosol. From the difference of the quenching kinetics of the whole section and the central area, the time for diffusion through the membrane and the diffusion in the extracellular and intracellular media can be deduced. To clarify the mechanism of lanthanide-induced fluorescence quenching of FITC-labeled erythrocytes and to ensure that this reaction can be used in this method, the reaction was investigated by steady-state fluorescence techniques. The results showed that the lanthanides strongly quenched the florescence emitted by FITC covalently bound to membrane proteins and cytosolic proteins. The static quenching mechanism is responsible for the fluorescence quenching of FITC-labeled proteins by Ln species. The quenching mechanism is discussed on the basis of complex formation. The dependence of fluorescence quenching on both ion size and the total orbital angular momentum L supports the complexation mechanism. The transport time across the membrane is strikingly correlated with Ln species and extracellular concentration. For a given concentration, the transport time of [Ln(cit)₂]^3– is much shorter than that of Ln³⁺, since they enter the cells via the anion channel. This is supported by the inhibition effect of 4,4′-diisothiocyanato-2,2′-stilbenendisulfonate on the transport of [Ln(cit)₂]^3–. On the other hand, the transport of free Ln³⁺ might be attributed to the enhanced permeability of erythrocytes owing to Ln³⁺ binding. These findings strongly demonstrate the existence of the non-internalization mechanism of Ln species uptake by erythrocytes. Received: 7 January 1999 / Accepted: 7 May 1999