Ixon3 897
The IXon3 897 is a high-performance scientific camera designed for demanding low-light imaging applications. It features an electron-multiplying CCD (EMCCD) sensor that provides high-speed, low-noise imaging capabilities. The camera is capable of capturing images with high quantum efficiency and sensitivity, making it suitable for a variety of scientific research and industrial applications.
Lab products found in correlation
31 protocols using ixon3 897
Rab37-Mediated SFRP1 Trafficking Dynamics
Super-Resolution Imaging of the DIB
Multicolor Single-Molecule Imaging Protocol
TIRF Imaging of C1-Ten Plasma Membrane Localization
Super-resolution TIRF Imaging Protocol
Super-Resolution Microscopy System Setup
Live-cell and super-resolution imaging
Super-resolution microscopy (SIM) was performed with an inverted fluorescence microscope (TI-E; Nikon) equipped with an electron-multiplying charge-coupled device camera (iXon3 897; Andor). Z-stack images were captured every 200 nm and reconstructed using NIS elements with SIM (Nikon).
Multi-channel Fluorescence Microscopy Protocol
Single-molecule BODIPY Fluorescence Imaging
an ECLIPSE Ti-E epifluoresence/TIRF microscope (NIKON, Japan) equipped
with 405, 488, 561, and 647 nm lasers (Coherent, California). All
lasers are individually shuttered and collected in a single fiber
to the sample through a 1.49 NA, ×100, apochromat TIRF oil objective
(NIKON, Japan). A dichroic mirror for the 488 nm laser (ZT491rdcxt,
CHROMA) was used. The excitation light was filtered using a laser
clean up filter (ZET 488/10x, CHROMA). The emitted light was filtered
using a band-pass filter (ET bandpass 532/50, CHROMA). Images were
recorded with an EM-CCD camera (iXon3 897, Andor). To keep the sample
in focus over time, we employed a perfect focusing system (NIKON,
Japan). Exposure time of the EM-CCD camera was set to 400 ms. We sampled
at various rates but did not observe different dynamics below a 400
ms exposure. Such an exposure time also allowed us to collect signals
of sufficient quality with the chosen laser excitation power density.
The laser power was optimized to achieve the best possible signal-to-noise
ratio and long enough bleaching time for the BODIPY fluorophore.
Confocal Imaging of Ras and PIP3 Waves
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