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Longpass dichroic mirror

Manufactured by IDEX Corporation

A longpass dichroic mirror is an optical component that selectively transmits light at longer wavelengths while reflecting light at shorter wavelengths. It functions by separating light based on its wavelength, allowing certain wavelengths to pass through the mirror while reflecting others.

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2 protocols using longpass dichroic mirror

1

Multimodal Imaging Protocol for Cellular Analysis

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First, a Leica SP5 confocal laser scanning microscope (CLSM, Leica Microsystems) equipped with hybrid detectors, a 40× immersion objective lens (HCX PL APO lambda blue), a motorized stage, and a tuneable laser (470–670 nm) was used. QDs, Alexa Fluor 546, and DRAQ5 were excited at 405, 561, and 647 nm, respectively, and their individual emissions were collected at 560–580, 560–620, and 665–795 nm. Second, a custom-made two-photon laser scanning microscope (2P-LSM) equipped with a femtosecond-pulsed titanium–sapphire laser (Chameleon Ultra II; Coherent) and a Zeiss W Plan Apochromat 20× (NA 1.0) water immersion objective lens was used. For excitation of the QDs, Hoechst and Alexa 546 the laser was respectively set at 850 nm and at 830 nm. The emitted light was split by two longpass dichroic mirror (Semrock) one 560 nm, and another 405 nm, and collected by photo-multiplier tubes (Hamamatsu). For the z-stacks acquisitions no laser power depth compensation was performed. All images were processed with the FIJI (an image-processing package based on ImageJ), Imaris 8.30 (Bitplane), Graph Pad Prism 6 (Graph Pad Software, Inc.) and Matlab (version 7, MathWorks) software. For 3D imaging of microscopy z-stacks as volumes, the Java-based ImageJ 3D Viewer plugin developed by Benjamin Schmid (Biozentrum Universität Würzburg) was used.
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2

Hyperspectral Imaging of OCC-DNA Nanosensors

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A hyperspectral microscope (IMA, Photon Etc.) was used to obtain spectrally and spatially resolved OCC-DNA emission in live cells. A continuous wave 808 nm laser (2W) injected into a multimode fiber to excite the nanosensors. The excitation beam passed through a beam-shaping module to produce a top-hat intensity profile with under 10% power variation on the imaged region of the sample. The power output at the sample stage was 425.8, 370.2, and 164.8 mW for ×20, ×50, and ×100 objectives, respectively. A long pass dichroic mirror with a cut-on wavelength of 875 nm (Semrock) was aligned to reflect the laser to the sample stage of an IX-71 inverted microscope equipped with LCPLN20XIR, LCPLN50XIR, and LCPLN100XIR IR objectives (Olympus). Hyperspectral microscopy was conducted by passing the emission through a volume Bragg grating placed immediately before a thermoelectrically cooled 2D InGaAs detector (ZephIR 1.7) in the optical path.
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