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Et600 50m

Manufactured by Oxford Instruments

The ET600/50m is a high-quality lab equipment product designed for precise and reliable measurements. It features a compact and durable design, suitable for use in various laboratory settings. The core function of the ET600/50m is to provide accurate and consistent measurements to support your research and analysis needs.

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7 protocols using et600 50m

1

TIRF Microscopy Imaging Setup

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Fluorescence imaging was carried out on an inverted microscope (Nikon Instruments, Eclipse Ti) with the Perfect Focus System, applying an objective-type TIRF configuration with an oil-immersion objective (Nikon Instruments, Apo SR TIRF ×100, numerical aperture 1.49, Oil). A 561 nm (200 mW, Coherent Sapphire) laser was used for excitation. The laser beam was passed through cleanup filters (Chroma Technology, ZET561/10) and coupled into the microscope objective using a beam splitter (Chroma Technology, ZT561rdc). Fluorescence light was spectrally filtered with an emission filter (Chroma Technology, ET600/50m, and ET575lp) and imaged on a sCMOS camera (Andor, Zyla 4.2 Plus) without further magnification, resulting in an effective pixel size of 130 nm (after 2 × 2 binning).
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2

Super-Resolution Microscopy Imaging Protocol

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Imaging was carried out using an inverted
microscope (Nikon Instruments, Eclipse Ti2) and the Perfect Focus
System, by applying an objective-type total internal reflection fluorescence
(TIRF) configuration with an oil-immersion objective (Nikon Instruments,
Apo SR TIRF 100×, NA 1.49, oil). A 561 nm laser (MPB Communications
Inc., 500 mW, DPSS-system) was used for excitation and was coupled
into a single-mode fiber. The laser beam was passed through cleanup
filters (Chroma Technology, ZET561/10) and coupled into the microscope
objective using a beam splitter (Chroma Technology, ZT561rdc). Fluorescence
light was spectrally filtered with an emission filter (Chroma Technology,
ET600/50m and ET575lp) and imaged with an sCMOS camera (Andor, Zyla
4.2 Plus) without further magnification, resulting in an effective
pixel size of 130 nm after 2 × 2 binning. Camera readout sensitivity
was set to 16-bit, and readout bandwidth to 540 MHz. Imaging parameters
used in the different experiments are shown in Table S12, and NeNA values are listed in Table S13.
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3

High-resolution TIRF Microscopy Imaging

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Fluorescence imaging was carried out on an inverted microscope (Nikon Instruments, Eclipse Ti2) with the Perfect Focus System, applying an objective-type TIRF configuration equipped with an oil-immersion objective (Nikon Instruments, Apo SR TIRF 100×, NA 1.49, Oil). A 561 nm and 642 nm laser (MPB Communications Inc., 2 W, DPSS-system) were used for excitation. The laser beams were passed through cleanup filters (Chroma Technology, ZET561/10, ZET 640/10) and coupled into the microscope objective using a beam splitter (Chroma Technology, ZT561rdc, ZT640rdc). Fluorescence light was spectrally filtered with an emission filter (Chroma Technology, ET600/50m and ET700/75m) and imaged on a sCMOS camera (Andor, Zyla 4.2 Plus) without further magnification, resulting in an effective pixel size of 130 nm (after 2×2 binning). Images were acquired choosing a region of interest with the size of 512×512 pixels. More detailed imaging conditions for the respective experiments are shown in Supplementary Table 8.
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4

High-resolution DNA-PAINT Microscopy

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DNA-PAINT imaging was carried out on an inverted microscope (Nikon Instruments, Eclipse Ti2) with the Perfect Focus System, applying an objective-type total internal reflection fluorescence (TIRF) configuration equipped with an oil-immersion objective (Nikon Instruments, Apo SR TIRF 100×, NA 1.49, oil). A 488-nm (200 mW, Toptica iBeam smart) or 561-nm laser (Coherent Sapphire, 200 mW) was used for excitation and was coupled into a single-mode fiber. The laser beam was passed through cleanup filters (Chroma Technology, ZET561/10) and coupled into the microscope objective using a beam splitter (Chroma Technology, ZT561rdc). Fluorescence light was spectrally filtered with an emission filter (Chroma Technology, ET600/50 m) and imaged with a scientific complementary metal-oxide semiconductor camera (Andor, Zyla 4.2plus) without further magnification, resulting in an effective pixel size of 130 nm after 2 × 2 binning. The camera readout sensitivity was set to 16-bit, and readout bandwidth to 540 MHz. Three-dimensional imaging was performed using a cylindrical lens (Nikon Instruments, N-STORM) in the detection path.
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5

Super-Resolution Fluorescence Imaging

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Fluorescence imaging was carried out on an inverted microscope (Nikon Instruments, Eclipse Ti2) with the Perfect Focus System, applying an objective-type TIRF configuration with an oil-immersion objective (Nikon Instruments, Apo SR TIRF 100×, NA 1.49, Oil). A 561 nm and 640 nm (MPB Communications Inc, 2W, DPSS-system) laser were used for excitation. The laser beam was passed through clean-up filters (Chroma Technology, ZET561/10, ZET642/20x) and coupled into the microscope objective using a beam splitter (Chroma Technology, ZT561rdc, ZT647rdc). Fluorescence light was spectrally filtered with an emission filter (Chroma Technology, ET600/50m and ET575lp, ET705/72m and ET665lp) and imaged on a sCMOS camera (Andor, Zyla 4.2 Plus) without further magnification, resulting in an effective pixel size of 130 nm (after 2 × 2 binning).
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6

High-resolution TIRF Microscopy Imaging

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Fluorescence imaging was carried out on an inverted microscope (Nikon Instruments, Eclipse Ti2) with the Perfect Focus System, applying an objective-type TIRF configuration equipped with an oil-immersion objective (Nikon Instruments, Apo SR TIRF 100×, NA 1.49, Oil). A 561 nm and 642 nm laser (MPB Communications Inc., 2 W, DPSS-system) were used for excitation. The laser beams were passed through cleanup filters (Chroma Technology, ZET561/10, ZET 640/10) and coupled into the microscope objective using a beam splitter (Chroma Technology, ZT561rdc, ZT640rdc). Fluorescence light was spectrally filtered with an emission filter (Chroma Technology, ET600/50m and ET700/75m) and imaged on a sCMOS camera (Andor, Zyla 4.2 Plus) without further magnification, resulting in an effective pixel size of 130 nm (after 2×2 binning). Images were acquired choosing a region of interest with the size of 512×512 pixels. More detailed imaging conditions for the respective experiments are shown in Supplementary Table 8.
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7

TIRF Microscopy for Fluorescence Imaging

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Fluorescence imaging was carried out
on an inverted microscope (Nikon Instruments, Eclipse Ti2) with the
Perfect Focus System, applying an objective-type TIRF configuration
equipped with an oil-immersion objective (Nikon Instruments, Apo SR
TIRF ×100, NA 1.49, Oil). A 560 nm laser (MPB Communications,
1 W) was used for excitation. The laser beam was passed through a
cleanup filter (Chroma Technology, ZET561/10) and coupled into the
microscope objective using a beam splitter (Chroma Technology, ZT561rdc).
Fluorescence was spectrally filtered with an emission filter (Chroma
Technology, ET600/50m and ET575lp) and imaged on an sCMOS camera (Andor,
Zyla 4.2 Plus) without further magnification, resulting in an effective
pixel size of 130 nm (after 2 × 2 binning). The readout rate
was set to 540 MHz. Images were acquired by choosing a region of interest
with a size of 512 × 512 pixels. Imaging conditions for the respective
experiments are shown in Table S2.
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