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Xlpln25xsvmp2

Manufactured by Nikon

The XLPLN25XSVMP2 is a microscope objective lens manufactured by Nikon. It has a 25x magnification and a numerical aperture of 1.10, designed for use in laboratory and research applications. The lens is a Plan Apochromat type, known for its high optical performance and flat field of view.

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2 protocols using xlpln25xsvmp2

1

Laser-Scanning Microscopy Protocol

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A half-waveplate and polarizing beam splitter set the excitation power sent to the microscope following pulse gating. The beam was expanded to fill the microscope objective back aperture, which was either a 25× objective (Olympus XLPLN25XSVMP2, 1.0 NA) for in vivo imaging or a 10× objective (Nikon CFIPlan10×, 0.25 NA) for cuvette experimentation. The excitation beam was scanned using a pair of galvanometer mirrors (Thorlabs, QS7XY-AG) conjugated to the objective back aperture using a scan lens (Thorlabs, SL50-2P2, f=50  mm ) and tube lens (Thorlabs, two AC508-400-C lenses in Plössl configuration, f=200  mm ) combination. The backscattered fluorescent signal was directed to a photomultiplier tube (PMT) (Hamamatsu, H10770PB-50) with a 775 nm cutoff dichroic filter (Semrock, FF775-Di01) and was further filtered with a 609/181 bandpass filter (Semrock, FF01-609/181-25), which immediately preceded the PMT photocathode. Imaging was controlled using a custom LabVIEW software. Although it may be necessary to synchronize EOM gating with the data acquisition sampling in some situations, this was not done for this work given our low sampling rate (160 kHz) relative to the gating frequency (1 MHz).
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2

Fluorescence Imaging System Setup

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A half-waveplate and polarizing beam splitter set the excitation power sent to the microscope following pulse gating. The beam was expanded to fill the microscope objective back aperture, which was either a 25X objective (Olympus XLPLN25XSVMP2, 1.0NA) for in vivo imaging or a 10X objective (Nikon CFIPlan10X, 0.25NA) for cuvette experimentation. The excitation beam was scanned using a pair of galvanometer mirrors (Thorlabs, QS7XY-AG) conjugated the objective back aperture using a scan lens (Thorlabs, SL50-2P2) and Plössl tube lens (Thorlabs, AC508-400-C) combination. Backscattered fluorescent signal was directed to a photomultiplier tube (PMT, Hamamatsu, H10770PB-50) with a 775 nm cutoff dichroic (Semrock, FF775-Di01), and was further filtered with a 609/181 bandpass filter (Semrock, FF01-609/181-25) which immediately preceded the PMT photocathode. Imaging was controlled using a custom LabVIEW software. While it may be necessary to synchronize EOM gating with DAQ sampling in some situations, this was not done for this work given our low sampling rate (160 kHz) relative to the gating frequency (1 MHz).
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