Long Exposure Imaging

Thanks to major breakthroughs in thermal noise control, the Retiga E9 CMOS has an unprecedented ultra-low dark current of <0.001 electrons per pixel per second, allowing for exposure times of over an hour.

Stretching exposure times from seconds to minutes to hours in this manner results in comfortable detection of even the weakest signals, ideal for imaging luminescence.

High Sensitivity

A combination of low read noise (1.3 e^–) and a high quantum efficiency (>90% at 550 nm) makes the Retiga E9 highly sensitive, able to image weak signals or operate at low exposure times.

If even more sensitivity is required, the Retiga E9 can be binned from 2×2 through to 16×16, maximizing sensitivity with larger pixel sizes.

Long Exposure Imaging

Thanks to major breakthroughs in thermal noise control, the Retiga E9 CMOS has an unprecedented ultra-low dark current of <0.001 electrons per pixel per second, allowing for exposure times of over an hour.

Stretching exposure times from seconds to minutes to hours in this manner results in comfortable detection of even the weakest signals, ideal for imaging luminescence.

High Sensitivity

A combination of low read noise (1.3 e^–) and a high quantum efficiency (>90% at 550 nm) makes the Retiga E9 highly sensitive, able to image weak signals or operate at low exposure times.

If even more sensitivity is required, the Retiga E9 can be binned from 2×2 through to 16×16, maximizing sensitivity with larger pixel sizes.

Long Exposure Imaging

Thanks to major breakthroughs in thermal noise control, the Retiga E9 CMOS has an unprecedented ultra-low dark current of <0.001 electrons per pixel per second, allowing for exposure times of over an hour.

Stretching exposure times from seconds to minutes to hours in this manner results in comfortable detection of even the weakest signals, ideal for imaging luminescence.

High Sensitivity

A combination of low read noise (1.3 e^–) and a high quantum efficiency (>90% at 550 nm) makes the Retiga E9 highly sensitive, able to image weak signals or operate at low exposure times.

If even more sensitivity is required, the Retiga E9 can be binned from 2×2 through to 16×16, maximizing sensitivity with larger pixel sizes.

Ultimate Flexibility

The Kinetix22 features four modes, allowing users to prioritize different camera specs, optimise imaging, and avoid compromise.

The 8 bit Speed mode offers 664 fps across the full frame, 12 bit Sensitivity mode offers low 1.2 e- read noise while operating at ~120 fps, 16 bit Dynamic range has large full well capacity for varied signal levels in the sample, and 16 bit Sub-Electron mode offers EMCCD like sensitivity with 0.7 e- read noise.

Maximizing Signal Collection

The Kinetix22 back-illuminated camera achieves a near-perfect 96% quantum efficiency.

By bringing the light in from the back of the sensor, photons land directly onto the light receiving surface, maximizing light collecting capability. This allows for the weakest signals to be displayed as high quality image, even if your sample typically only emits a handful of photons.

High Resolution

The Kinetix22 features 6.5 µm x 6.5 µm pixels, the accepted standard for most live cell applications using 40x and 60x magnification.

This pixel size provides highly detailed images across the imaging plane and is most suitable for the broadest range of microscope objectives.

7 Discrete Spectral Bands

Whatever fluorophore you intend to use, the SPECTRA X^® can bring it to life with its broad spectral range.

High Illumination Power

High maximum illumination power combined with the high-speed switching, this light engine unlocks more demanding fluorescence applications

High Speed

When synchronizing with a camera or other devices, fast turn-on and high speed switching capability is a must. The SPECTRA X^® boasts 10µs on time and 5-10 kHz switching rate, enabling high speed applications.

7 Discrete Spectral Bands

Whatever fluorophore you intend to use, the SPECTRA X^® can bring it to life with its broad spectral range.

High Illumination Power

High maximum illumination power combined with the high-speed switching, this light engine unlocks more demanding fluorescence applications

High Speed

When synchronizing with a camera or other devices, fast turn-on and high speed switching capability is a must. The SPECTRA X^® boasts 10µs on time and 5-10 kHz switching rate, enabling high speed applications.

7 Discrete Spectral Bands

Whatever fluorophore you intend to use, the SPECTRA X^® can bring it to life with its broad spectral range.

High Illumination Power

High maximum illumination power combined with the high-speed switching, this light engine unlocks more demanding fluorescence applications

High Speed

When synchronizing with a camera or other devices, fast turn-on and high speed switching capability is a must. The SPECTRA X^® boasts 10µs on time and 5-10 kHz switching rate, enabling high speed applications.

7 Discrete Spectral Bands

Whatever fluorophore you intend to use, the SPECTRA X^® can bring it to life with its broad spectral range.

High Illumination Power

High maximum illumination power combined with the high-speed switching, this light engine unlocks more demanding fluorescence applications

High Speed

When synchronizing with a camera or other devices, fast turn-on and high speed switching capability is a must. The SPECTRA X^® boasts 10µs on time and 5-10 kHz switching rate, enabling high speed applications.

7 Discrete Spectral Bands

Whatever fluorophore you intend to use, the SPECTRA X^® can bring it to life with its broad spectral range.

High Illumination Power

High maximum illumination power combined with the high-speed switching, this light engine unlocks more demanding fluorescence applications

High Speed

When synchronizing with a camera or other devices, fast turn-on and high speed switching capability is a must. The SPECTRA X^® boasts 10µs on time and 5-10 kHz switching rate, enabling high speed applications.