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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.
The syntheses, structures, and photophysical properties of two new zinc(II) complexes bearing the tridentate N,N′-dimethyl-N,N′-dipyridin-2-ylpyridine-2,6-diamine (ddpd) ligand are presented. Structural investigations through single-crystal X-ray diffractometry, NMR spectroscopy, and density functional theory calculations revealed a diverse coordination behavior that depends on the counterion. Spectroscopic (UV/Vis and emission spectroscopy) and theoretical techniques (DFT and time-dependent DFT calculations) were employed to explore the photophysical properties of the complexes.
The excitation wavelength (lexc) dependence of the photoluminescence (PL) quantum yield (FPL) and decay behavior (tPL) of a series of CdSe/CdS quantum dot/Quantum rods (QDQRs), consisting of the same spherical CdSe core and rod-shaped CdS shells, with aspect ratios ranging from 2 to 20 was characterized. lexc between 400–565 nm were chosen to cover the first excitonic absorption band of the CdSe core material, the onset of absorption of the CDs shell, and the region of predominant shell absorption. A strong lexc dependence of relative and absolutely measured FPL and tPL was found particularly for the longer QDQRs with higher aspect ratios. This is attributed to combined contributions from a length-dependent shell-to-core exciton localization efficiency, an increasing number of defect states within the shell for the longest QDQRs, and probably also the presence of absorbing, yet non-emitting shell material. Although the FPL values of the QDQRs decrease at shorter wavelength, the extremely high extinction coefficients introduced by the shell outweigh this effect, leading to significantly higher brightness values at wavelengths below the absorption onset of the CdS Shell compared with direct excitation of the CdSe cores. Moreover, our results present also an interesting example for the comparability of absolutely measured FPL using an integrating sphere setup and FPL values measured relative to common FPL standards, and underline the Need for a correction for particle scattering for QDQRs with high aspect ratios.