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405 nm diode laser

Manufactured by Toptica
Sourced in Germany

The 405 nm diode laser is a compact and efficient light source that emits light in the violet region of the visible spectrum. It is designed to provide a stable and reliable output power for various applications that require a 405 nm wavelength.

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3 protocols using 405 nm diode laser

1

Fluorescence Recovery After Photobleaching

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The detection system was set up on an epi-fluorescence microscope (Olympus IX81). Diode lasers (Toptica Photonics, Munich, Germany) were used for selective fluorescence excitation of GFP, YFP and Cy5/DiD at 488 nm, 514 nm and 640 nm, respectively. A 405 nm diode laser (Toptica Photonics, Munich, Germany) was used for bleaching of GFP/YFP fluorescence. Samples were illuminated in total internal reflection (TIR) configuration (CellTIRF, Olympus) using a 60 x oil immersion objective (NA  =  1.49, APON 60XO TIRF, Olympus, Munich, Germany). After appropriate filtering using standard filter sets, fluorescence was imaged onto a CCD camera (Orca-R2, Hamamatsu, Japan). Samples were mounted on an x-y-stage (CMR-STG-MHIX2-motorized table; Märzhäuser, Germany) and scanning of larger areas was supported by a laser-guided automated focus-hold system (ZDC-2; Olympus). For FRAP experiments single patterns were photobleached with a laser pulse (405 nm) applied for 100 ms. Recovery images were recorded at indicated time intervals. FRAP images were analyzed using the Multimeasure plugin of ImageJ [27] (link). Data were normalized by the pre-bleach image and curve fitting was done using Graphpad Prism. Resulting FRAP curves were plotted based on the standard error of the mean (SEM) and fitted using a bi-exponential equation. Kinetic FRAP parameters were directly obtained from curve fitting.
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2

Colocalization Analysis of Extracellular Vesicles

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Diffusion analysis
was performed by a custom written MATLAB platform (based on @msdanalyzer).52 (link) The spreadsheets with linked coordinates (output
from Trackpy tool) were used as input for @msdanalyzer. For the colocalization
analysis of internalized EVs and transferrin from human serum conjugated
with AlexaFluor647 (Invitrogen, Carlsbad, CA, USA), HeLa cells were
cultured for 48 h on glass slides coated with 1 μg/cm2 fibronectin. eGFP-CD63 EVs were diluted 1:100 in FluoroBrite medium
supplemented with 1% EV-depleted FBS and incubated with HeLa cells
for 30 min at 37 °C in 5% CO2 atmosphere. After EVs
were internalized by the cells, transferrin was added to the cells
and incubated for 10 min of incubation at 37 °C, 5% CO2. Cells were washed and fixed with 4% paraformaldehyde (PFA) in PBS.
Imaging was performed in OxEA buffer (50 mM β-mercaptoethylamine,
3% oxyrase, 100 μM DL-lactate, 30v/v% glycerine) in PBS adjusted
to pH 8.0–8.5 with NaOH. Images were acquired as previously
described. Samples were illuminated for 20 ms, and a sequence of 10 000
frames was recorded with a delay between individual images of 33 ms.
During the camera chip read-out, UV light (405 nm diode laser, Toptica
Photonics) was additionally used to activate the probes, and the laser
power was adjusted during the measurements accordingly.
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3

Resonance Raman Spectroscopy of DyP Enzymes

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RR and SERR spectra were acquired with a Raman spectrometer (Jobin Yvon U1000, Edison, NJ, USA), equipped with a 1200 lines/mm grating and a liquid-nitrogen-cooled CCD detector, which was coupled to a confocal microscope. An Olympus 20× objective was used for laser focusing onto the sample and light collection in the backscattering geometry. Spectra were measured using a 405 nm diode laser (Toptica Photonics AG, Munich, Germany).
The RR spectra of CboDyP and TfuDyP were measured as previously described [26 (link)]. ScoDyP spectra were acquired at low temperature using ca. 2 μL of the enzyme sample placed in a microscope stage (Linkham THMS 600, Tadworth, UK) cooled to the desired temperature with liquid N2.
RR experiments were performed with a 1.8 mW laser power and a 120 s accumulation time. SERR experiments were performed with a 1.3 mW laser power and 30–40 s accumulation time. Up to 16 spectra were co-added in each measurement to improve the signal-to-noise ratio (S/N). All spectra were subjected to polynomial baseline subtraction; the positions and widths of Raman bands were determined by component analysis as described previously [43 (link)].
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