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Blp01 647r 25

Manufactured by IDEX Corporation
Sourced in United States

The BLP01-647R-25 is a compact, high-performance laser diode module designed for laboratory and research applications. It emits light at a wavelength of 647 nanometers with an output power of 25 milliwatts. The module is housed in a rugged, heat-dissipating enclosure and features a collimated beam for precise targeting.

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6 protocols using blp01 647r 25

1

Super-resolution dSTORM Microscopy Setup

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Super-resolution dSTORM measurements were performed on a custom-made inverted microscope based on a Nikon Eclipse Ti-E frame (Nikon Instruments Europe BV, Amsterdam, The Netherlands). After being conditioned (through spatial filtering via fiber coupling and beam expansion), the applied laser beams were focused onto the back focal plane of the microscope objective (Nikon CFI Apo 100×, NA = 1.49), which produced a collimated beam on the sample. All dSTORM images were captured with a linearly polarized beam and EPI illumination at an excitation wavelength of 647 nm (MPB Communications Inc., Pointe-Claire, QC, Canada: 647 nm, Pmax = 300 mW). The laser intensity was controlled via an acousto-optic tunable filter (AOTF). Images were captured by an Andor iXon3 897 EMCCD camera (Andor: Belfast, UK; 512 × 512 pixels with 16 μm pixel size). Frame stacks for dSTORM super-resolution imaging were typically captured at a reduced image size (crop mode). Excitation and emission wavelengths were spectrally separated with a fluorescence filter set (Semrock, Rochester, NY, USA; LF405/488/561/635-A-000) and an additional emission filter (Semrock, BLP01-647R-25) in the detector arm. During the measurements, the perfect focus system of the microscope was used to keep the sample in focus with a precision of <30 nm.
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2

Schematic of sSMLM Experimental Setup

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Figure 1a shows the schematic of our experimental sSMLM setup. We used a 488-nm CW laser (Excelsior PC14833, Spectra-Physics) to excite the quantum dots (QDs). We focused the laser beam onto the back focal plane of the objective lens (Obj, CFI Apochromat 100×, Nikon, NA = 1.49) to uniformly illuminate the whole FOV. The resulting fluorescence emissions passed through a long-pass filter (BLP01-647R-25, Semrock) and a tube lens (TL) to form an intermediate image where we placed an adjustable slit (S) to confine the FOV. The fluorescence emission was transmitted through a diffraction grating (G) (100 grooves/mm, Star Analyser 100, Paton Hawksley Education Ltd) with a splitting ratio of 1:3 between the zeroth and first diffraction orders. The diverging beam was then collimated by a lens (L1, Nikon 50mm f/1.4 NIKKOR). We individually controlled the two detection paths corresponding to the zeroth and first diffraction orders using two pickoff mirrors (M2 and M3). Finally, a focusing lens (L2, Rokinon 85 mm f/1.4) projected the zeroth- and first-order images onto an electron-multiplying charge-coupled device (EMCCD) (ProEM 512B+, Princeton Instruments) for acquisition.
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3

Multimodal imaging of lung tissue

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Lung tissue slices were imaged on a ctASLMv2118 (link) microscope chamber controlled by navigate119 . Nuclei were imaged using the TO-PRO-3 647 via illumination with a LuxX 642 nm, 140 mW at 100% laser power and a Semrock BLP01–647R-25 filter in the detection path. Cancer cells were imaged via illumination with a LuxX 488–150, 150 mW at 100% laser power and a Semrock FF01–515/30–32 bandpass filter in the detection path. Images were acquired with a Hamamatsu ORCA-Flash 4.0 v3 with 200 ms integration time in lightsheet readout mode.
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4

Single-Molecule Imaging of Biomolecular Dynamics

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Samples were mounted in a buffer consisting of 90% glycerol and 10% 10xPBS with an overall concentration of 10mM cysteamine and 50mM sodium sulfite (J.T. Baker 3922–01). Images were recorded on a modified Nikon Ti-E inverted microscope using a 60× 1.49 N.A. oil immersion objective using an EMCCD camera (Andor IXon Ultra DU-897U-CS0-#BV). The objective was mounted on a custom mount to suppress thermal and mechanical drift and focusing was provided by a piezoelectric objective positioner (Physik Instrumente P-725.4CA). For illumination a 642nm solid-state laser (Omicron Lux, 20 kW/cm2 at the sample) was used with a dichroic (Semrock, Di02-R635-25×36) and a band-pass filter (Semrock, BLP01-647R-25) for separation of excitation and emission. Field of view were selected using metal halide lamp (Prior Lumen 200) illumination before switching to laser illumination and were then imaged for approximately 20,000 frames using an exposure time of 25 ms and an EM-multiplication setting corresponding to a gain of 35.5. Events were detected and localized (Baddeley et al., 2009 (link)) and reconstructions were rendered using jittered triangulation (Baddeley et al., 2010 (link)) (see supplemental information).
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5

Multimodal Imaging Spectroscopy Platform

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The optical setup contains an inverted optical microscope (Eclipse Ti-U with perfect-focus system, Nikon), equipped with 645-nm and 445-nm solid-state lasers with 500-mW maximum output, a high numerical aperture objective lens (100x, NA1.49, Nikon CFI apochromat TIRF) for TIRF illumination, and a home-built transmission spectrometer. The illumination power was controlled by a set of linear polarizers. The imaging filter set was consisted of a laser clean-up filter (FF01–642/10–25, Semrock), a dichroic mirror (FF649-DI01–25X36, Semrock), and a long-pass filter (BLP01–647R-25, Semrock) at the emission port to reject the reflected laser beam. The fluorescence image was then coupled into a transmission spectrometer featuring a blazed dispersive grating (150 grooves mm−1). The image further divided into a non-dispersed zero-order spatial image and a spectrally dispersed first-order spectral image and can be simultaneously collected by a high-sensitivity electron multiplying charge-coupled device (EMCCD, ProEM, Princeton Instruments).
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6

Wide-field 3D Single-Molecule Localization Microscopy

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We built a 3D SMLM imaging system with wide-field illumination on an inverted microscope body (Ti-2, Nikon). Fig. S1(A) shows the schematic for our experimental design using a cylindrical lens. Light from a continuous-wave (CW) 647-nm laser (2RU-VFL-P-1000-647-B1R, MPB Communications Inc.) first passed through a band-pass filter (FF01-642/10-25, Semrock), then was reflected by a 649-nm cutoff dichroic mirror (FF649-Di01-25 × 36, Semrock) and focused by an objective lens (OBJ, CFI SR HP Apochromat TIRF 100XC, Nikon) on the sample. The fluorescence photons passed through a 200-mm tube lens and a 647.1-nm long-pass filter (BLP01-647R-25, Semrock). The fluorescence photons passed through two lenses (L1, 100-mm focal length; L2, 100-mm focal length) and a cylindrical lens (CL, 200-mm focal length) to be focused onto an electron-multiplying charge-coupled device (EMCCD, iXon Ultra 897).
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