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Projekt Nano-TG110
(2017)
Die OECD-TG110 mit dem Titel "Particle Size Distribution Fibre Length and Diameter Distribution" wurde 1981 erstellt und seither nicht überarbeitet. Nanomaterialien, wie Nanopartikel oder Nanofasern werden nicht adressiert, genausowenig wie moderne Messverfahren. Das hier vorgestellte Projekt hat zur Aufgabe, die Größenmessung von Nanopartikeln und Nanofasern in einer neuen Technical Guideline der OECD zu standardisieren. Es wird die Projekthistorie dargestellt, die Anforderungen, der aktuelle Projekt-Bearbeitungsstand wird beleuchtet und die weiteren Arbeiten werden kurz skizziert.
At the core of luminescence color and lifetime tuning of rare earth doped upconverting nanoparticles (UCNPs) is the understanding of the impact of the particle architecture for commonly used sensitizer (S) and activator (A) ions. In this respect, we present here a series of core@shell NaYF4 UCNPs doped with Yb3+ and Ho3+ ions, where the same dopant concentrations were distributed in different particle architectures following the scheme: YbHo core and YbHo@..., …@YbHo, Yb@Ho, Ho@Yb, YbHo@Yb, and Yb@YbHo core-shell NPs. As revealed by quantitative steady state and time-resolved luminescence studies, the relative spatial distribution of the A and S ions in the UCNPs and their protection from surface quenching has critical impact on their luminescent characteristics. Interestingly, although the increased amount of Yb3+ ions boosts UCNP performance by increasing the absorption, the Yb3+ ions can also dissipate the energy stored in the material through energy migration to surface, thereby reducing the overall energy transfer efficiency to the activator ions.
Immunoassays are an important field of in vitro diagnostics, as they allow for a fast and highly sensitive detection of many biologically and diagnostically relevant analytes such as proteins, hormones, and pharmaceuticals. Fluorescence immunoassays (FIA), where the antibodies and/or antigens are labeled with luminescent reporters, can be easily read out directly by measuring the intensity, decay time, or polarization of the emitted light. Moreover, FIA enable the simultaneous detection of different analytes within a single sample (multiplexing) and are particularly suited for point-of-care (POC) diagnostics and high throughput screening (HTS). The application of luminescent nanoparticles as reporters in FIA could further improve assay sensitivity, as several 100 to 1000 luminophores can be incorporated or attached to such nanoscale carriers, thereby amplifying their absorption and/or emission signals simply by increasing the number of dye molecules.
Although dye-loaded polymeric and silica nanoparticles have been increasingly used as reporters in immunoassays, achievable signal amplification factors related to the use of particle reporters are still difficult to predict and quantify, which also hampers the comparability of different nanoscale reporters. To overcome this challenge, we performed a systematic comparison of spectroscopically and analytically well characterized particle labels in a homogeneous sandwich immunoassay format for the detection of the common inflammation biomarker C-reactive protein (CRP). Hereby, we studied the influence of particle parameters like size, surface chemistry, and dye loading concentration for different dye classes, i.e. organic dyes and metal ligand complexes, varying in their signal-relevant spectroscopic properties (molar absorption coefficients, photoluminescence quantum yields, Stokes shifts, and emission decay times), for different detection schemes (direct read-out vs. dye extraction). The emitters applied were chosen to be commercially available for a reasonable price, to absorb between 400 nm and 450 nm, and to emit in the visible region, as these parameters are accessible with most established microplate readers. Based upon our findings, we highlight the advantages and limitations of nanoscale reporters with respect to the choice of suitable particles, encoding dyes, and detection strategies, and compare the achievable sensitivities and dynamic ranges for our CRP model immunoassay.
There is an increasing interest in optical reporters like semiconductor and lanthanide-based nanocrystals with emission > 800 nm and recently also > 1000 nm for bioanalysis, medical diagnostics, and safety barcodes. Mandatory for the comparison of different emitter classes and the rational design of the next generation of reporters for the short wavelength infrared (SWIR) region are reliable and quantitative photoluminescence measurements in this challenging wavelength region. This is of special relevance for nanocrystalline emitters like semiconductor quantum dots and rods as well as for upconversion and downconversion nanocrystals, where surface states and the accessibility of emissive states by quenchers largely control accomplishable quantum yields and hence, signal sizes and detection sensitivities from the reporter side. Such measurements are currently hampered by the lack of suitable methods and standards for instrument calibration and validation as well as by the lack of quantum yield standards with emission > 800 nm and especially > 1000 nm.
In this respect, we present the design of integrating sphere setups for absolute and excitation power densitydependent measurements of emission spectra and quantum yields in the wavelength region of 650 to 1650 nm
including calibration strategies and first candidates for potential fluorescence standards. Subsequently, the photoluminescence properties of different types of nanocrystals are presented and discussed including absolute photoluminescence measurements of upconversion and down conversion emission in different solvents.
Studying the interaction of nanoparticles (NPs) with cells has become a growing field of interest. Research topics are ranging from nanotoxicology to medical applications e.g. as theranostic agents. In order to evaluate nano-bio interactions, the number of NPs inside cells as well as their localisation within cellular substructures is of particular interest.
In recent years, elemental imaging of biological samples using laser ablation inductively coupled plasma mass spectrometry (LA-ICP-MS) is gaining more and more importance. Latest instrumental developments regarding spatial resolution (down to 1 µm) and detection efficiency make LA ICP-MS particularly interesting for single cell analysis.
Here, we have applied LA-ICP-MS for sub-cellular scale imaging of individual cells to study the NP pathway from uptake, via intracellular processing up to cell division. Furthermore, the local distribution of naturally occurring elements in cells like P was measured to indicate the cell morphology.
Murine fibroblast cells were incubated with different metal-containing NPs under varying experimental conditions. For LA analysis, the cells were fixed and dried. Sub-cellular resolution was achieved by careful optimisation of the laser ablation parameters. By rastering with the laser beam across the sample, a two-dimensional image of the elemental distribution can be received. Our results show that LA-ICP-MS is able to localise NP aggregates within cellular substructures. The studied NPs accumulate in the perinuclear region in the course of intracellular processing, e.g. multivesicular fusion and endosomal maturation, but do not enter the nucleus. The uptake depends on the physico-chemical properties of the nanostructures and on the incubation conditions like concentration and incubation time. Additionally, the number of NPs internalized by individual cells was determined and variations within a cell population became visible.
The findings demonstrate the potential of LA-ICP-MS providing insight into NP uptake and intracellular distribution dependent on experimental parameters.
Due to their unique physical properties, particularly their electronic and luminescent properties, graphene quantum dots (GQDs) are expected to be suitable for a wide range of applications in bioimaging, electro-optical and photonic materials or energy harvesting among others.1 Tuning the surface chemistry provides an efficient approach to modulate the fluorescence and distinct electronic properties of GQDs.2 Nevertheless, the role of surface chemistry on the electronic structure of GQDs remains poorly understood. In this presentation, we will compare systematically the electronic and chemical structures of GQDs functionalized with carboxylic and aminated groups to those of non-functionalized GQDs, combining theoretical and experimental approaches, here various photon-based spectroscopies. First, the electronic structure of GQDs was characterized by soft X-ray absorption (XA) and X-ray emission (XE) spectroscopies, probing unoccupied and occupied electronic states, respectively, at the carbon K edge for the first time. The interpretation of the XA/XE spectra was done based on theoretical calculations. Then, the chemical structure of the GQDs was characterized in situ by ATR-FTIR in water, thereby accounting for the importance of the interface between GQDs and water believed to play a central role in the chemical reactivity and the optical properties. We previously demonstrated that monitoring the OH vibrations of water molecules during exposure to humid air was a powerful method to probe H-bonding environment around carbon nanomaterials.3 For GQDs, clear surface-dependent water adsorption profiles are observed and discussed. Finally, UV/Vis absorption and photoluminescence measurements were done to characterize the optical properties of these GQDs. Our results suggest that the surface chemistry of the GQDs affects significantly their electronic structure and optical properties. These findings will contribute to an improved understanding of the structure–activity relationship of GQDs and other carbon nanomaterials with surface modifications.
There is an increasing interest in molecular and nanoscale with emission > 800 nm and recently also > 1000 nm for bioanalysis, medical diagnostics, bioimaging, and safety barcodes. Mandatory for the comparison of different emitter classes and the rational design of the next generation of reporters for the short wavelength infrared (SWIR) Region are reliable and quantitative photoluminescence measurements in this challenging wavelength region. This is of special relevance for nanocrystalline emitters like semiconductor quantum dots and rods as well as lanthanide-based upconversion and downconversion nanocrystals, where surface states and the accessibility of emissive states by quenchers largely control accomplishable photoluminescence quantum yields and hence, signal sizes and detection sensitivities from the reporter side. Such measurements are currently hampered by the lack of suitable methods and standards for instrument calibration and validation and quantum yield standards with emission > 800 nm and especially > 1000 nm.
In this respect, we present the design of integrating sphere setups for absolute and excitation power density-dependent measurements of emission spectra and photoluminescence quantum yields in the wavelength Region of 650 to 1650 nm including calibration strategies and first candidates for potential fluorescence standards.
Subsequently, the photoluminescence properties of different types of nanocrystals are presented including the upconversion and downconversion emission of differently sized and surface functionalized lanthanide-doped nanoparticles and photoluminescence quenching effects are quantified.
Functional Nanomaterials with VIS/NIR Emission-Spectroscopic Properties And Surface Group Analysis
(2017)
Optical-spectroscopic methods for the quantitative characterization of the optical properties of different types of vis/NIR-emissive nanomaterials like semiconductor quantum dots and upconversion nanocrystals will be presented and their relevance for the mechanistic understanding of nonradiative decay channels and the rational design of new nanomaterials will be underpinned. In this respect, also validation concepts for such measurements and absolute fluorometry will be introduced. In addition, the potential of optical spectroscopy for surface group and ligand analysis surface chemistry will be demonstrated exemplarily for semiconductor quantum dots.