Light- and Temperature-Modulated Magneto-Transport in Organic–Inorganic Lead Halide Perovskites

The optoelectronic properties and charge carrier dynamics in hybrid organic–inorganic perovskites under steady-state illumination are the key elements for understanding their high efficiency. We present temperature-dependent Hall and photoconductivity measurements down to a temperature of 4.2 K on single crystals of MAPbI₃ and MAPbBr₃ in magnetic fields up to 30 T and observed different transport regimes. For temperatures down to 25 K, charge transport is dominated by acoustic phonon scattering as inferred from the temperature dependence of both zero and high-field resistance. Below 25 K, transport is determined by thermally activated hopping of charge carriers reflected in a diverging zero-field resistance and a strong decrease in the carrier’s mobility and concentration. Our findings demonstrate the importance of performing experiments at low temperature to unravel the fundamental charge carrier dynamics and stimulate the need for a comprehensive theoretical model for perovskite-based devices

The activity of firefly luciferase in free solution or in intact 293T cells is dependent on available oxygen concentration.

<p>(<b>A</b>) Total photon flux at normoxic (21% O₂) and hypoxic (0% O₂, via addition of 1% Na₂SO₃) conditions emitted from a luciferase-dependent bioluminescence reaction in intact cells or from an equal concentration in cell lysates. Error bars, ±1 s.d. unit; <i>n</i> ≥5. (<b>B</b>, <b>C</b>) Confocal fluorescence imaging of cell mitochondria in cells exposed to (<b>B</b>) normoxic or (<b>C</b>) hypoxic oxygen concentrations. Images are maximum intensity projections of cell mitochondria stained with MitoTracker Red (red), cell nucleus stained with Hoechst (blue), and GFP signal (green) from stably transduced 293T cells. Left and right panels show the stained mitochondria with or without the other two channels, to reveal background fluorescence. Scale bar, 10 µm.</p

The available oxygen concentration induces changes in luciferase enzyme kinetics.

<p>(<b>A</b>, <b>B</b>) Dynamic time point analysis of luciferase activity with varying luciferin concentrations measured at (<b>A</b>) normoxic and (<b>B</b>) at hypoxic conditions. Measured data points were extrapolated with exponential functions to resolve the initial enzyme activity. Error bars, ±1 s.d. unit; <i>n</i> ≥3. (<b>C</b>) Lineweaver-Burk plots of initial luciferase activity show the influence of available oxygen concentration on bioluminescence kinetics-related parameters, at normoxia (<i>R²</i> = 0.74) and at hypoxia (<i>R²</i> = 0.94). Enzyme kinetics for intermediate oxygen levels (solid black lines –5, 10 and 15% O₂ from top to bottom) are determined from a square root dependent relationship with available oxygen concentration. (<b>D</b>, <b>E</b>) Average photon flux emitted from cell lysates or intact cells at different oxygen concentrations. Simulation results (dashed lines) are shown for (<b>D</b>) short and (<b>E</b>) long term analyses. Cells incubated in hypoxic conditions display a delayed bioluminescence peak activity. (<b>F</b>) Bioluminescence microscopy of intact cells imaged at saturated (21% O₂) oxygen concentrations (initial luciferin concentrations, 470 µM). Scale bar, 20 µm.</p

Validation of the bioluminescence-oxygen model for quantitative interpretation and analysis of bioluminescent light emitted from cell-seeded hydrogels.

<p>(<b>A</b>) Average photon flux measured for luciferase reporter 293T cells embedded in agarose gels that are axially confined by circular glass plates. Dynamic time point measurements were performed during 12 hour periods. (initial luciferin concentration, 47 µM) Error bars, ±1 s.d. unit; <i>n</i> ≥3 (<b>B</b>) Emission peak intensities were fitted by Gaussian functions. Time-lapse measurements of the average emitted photon flux were compared with simulation results from the bioluminescence-oxygen model in presence or absence of oxygen gradients at day 1 (<b>C</b>), day 2 (<b>D</b>), and day 3 (<b>E</b>). (<b>F</b>) Comparison of simulated peak emission intensities in presence (blue) or absence (orange) of oxygen gradients, with average viable cell densities obtained from quantitative DNA analyses (gray). Error bars, ±1 s.d. unit; <i>n</i> = 6. (<b>G</b>) 2D bioluminescence profiles of cell-seeded agarose gels imaged from top position (hydrogel diameter, 8 mm). Profiles above the dashed lines are measured with the IVIS 100, and profiles below are simulated from the bioluminescence-oxygen model. The left column shows activity at the peak position and the right column shows activity after 6 h (steady-state condition) (<b>H</b>) Bioluminescence microscopy of 293T cells embedded in agarose at the central hydrogel position and (<b>I</b>) comparison with the simulated activity in the hydrogel center.</p

Overview of the mechanisms involved in bioluminescence photon emission from luciferase reporter cells embedded in a hydrogel.

<p>These mechanisms are implemented in the mathematical bioluminescence-oxygen model to decouple intrinsic bioluminescence intensities from the cellular oxygen environment. (A) Illustrated overview of the bioluminescence reaction in intact cells. Oxygen (iv) and luciferin (iii) pass through an extracellular matrix prior to cellular uptake. Diffusion rates are obtained from Fluorescence Recovery After Photobleaching (FRAP). Luciferin is actively transported across the cell membrane (thickness, <i>λ_c</i>) and reacts with luciferase (ii) in the cell cytoplasm where this reaction is accompanied by the release of a photon (i). Oxygen availability in the cytoplasm modulates emitted light intensity and kinetics and is described by the Michaelis-Menten kinetics. (B) Setup for validation of the bioluminescence-oxygen model. Oxygen Sensing microBeads (i) and 293T cells (ii) are embedded in an agarose gel that is confined between 2 circular glass plates. Focal volume (v) imaged by combined bioluminescence and fluorescence microscopy reveals luciferase activity in single intact cells (iii) and local oxygen concentrations based on ratiometric intensities obtained from oxygen sensitive and insensitive dyes (iv). Scale bar, 1mm. Scale bar figure insets, 10 µm. (C) Radial oxygen concentration profiles in cell-seeded agarose gels measured by fluorescence intensities from embedded OSB. Colored lines indicate fitted oxygen profiles simulated by the oxygen model. Empty control gels (Contr) are imaged after 1, 2 and 3 days of incubation. Error bars, ±1 s.d. unit; <i>n</i> ≥3. (D) Polar plot of time-dependent changes in fluorescein tracer diffusion rates as measured by FRAP. R-axis of polar plot indicates tracer diffusion rate (µm²·s⁻¹). FRAP analysis showed no significant difference in average values (dashed lines) at day 1 (red, top left panel), day 2 (green, top right panel), and day 3 (blue, bottom left panel). Spatial heterogeneities in diffusion rate within the agarose gel were determined from measurements at various radial (r1 = 1 mm, red; r2 = 2 mm, green; and r3 = 3 mm, blue) and angular positions in the gel. Empty control gel (black, bottom right panel) is shown as a reference. Measurements are performed in duplicate with a small shift in spatial position, <i>n</i> ≥3.</p

Biocompatible Label-Free Detection of Carbon Black Particles by Femtosecond Pulsed Laser Microscopy

Although adverse health effects of carbon black (CB) exposure are generally accepted, a direct, label-free approach for detecting CB particles in fluids and at the cellular level is still lacking. Here, we report nonincandescence related white-light (WL) generation by dry and suspended carbon black particles under illumination with femtosecond (fs) pulsed near-infrared light as a powerful tool for the detection of these carbonaceous materials. This observation is done for four different CB species with diameters ranging from 13 to 500 nm, suggesting this WL emission under fs near-infrared illumination is a general property of CB particles. As the emitted radiation spreads over the whole visible spectrum, detection is straightforward and flexible. The unique property of the described WL emission allows optical detection and unequivocal localization of CB particles in fluids and in cellular environments while simultaneously colocalizing different cellular components using various specific fluorophores as shown here using human lung fibroblasts. The experiments are performed on a typical multiphoton laser-scanning microscopy platform, widely available in research laboratories

<i>p</i>-Xylene-Selective Metal–Organic Frameworks: A Case of Topology-Directed Selectivity

Para-disubstituted alkylaromatics such as <i>p</i>-xylene are preferentially adsorbed from an isomer mixture on three isostructural metal–organic frameworks: MIL-125(Ti) ([Ti₈O₈(OH)₄(BDC)₆]), MIL-125(Ti)-NH₂ ([Ti₈O₈(OH)₄(BDC-NH₂)₆]), and CAU-1(Al)-NH₂ ([Al₈(OH)₄(OCH₃)₈(BDC-NH₂)₆]) (BDC = 1,4-benzenedicarboxylate). Their unique structure contains octahedral cages, which can separate molecules on the basis of differences in packing and interaction with the pore walls, as well as smaller tetrahedral cages, which are capable of separating molecules by molecular sieving. These experimental data are in line with predictions by molecular simulations. Additional adsorption and microcalorimetric experiments provide insight in the complementary role of the two cage types in providing the para selectivity