Igniting New Confocal Imaging Potential
The newly developed Nikon Spatial Array Confocal (NSPARC) detector utilizes an ultra-low noise detector array to collect a two-dimensional image at each scanned point. This method of image scanning microscopy (ISM) improves signal-to-noise ratio by increasing the available signal level while simultaneously allowing imaging with lower excitation power.
Single-photon sensitivity and array detection extend the capabilities of the AX system by revealing unseen details in every image, with array detection pushes the boundaries of resolution beyond the theoretical limits.
An extremely low noise profile along with incredible sensitivity renders outstanding results even under demanding imaging conditions, including high speed resonant imaging.
As an added benefit, additional spatial information is acquired for every pixel using the detector array, which can be used to further enhance resolution and brightness.
Comparing NSPARC and GaAsP bias images (acquisition with no light to measure noise) reveal extremely low standard deviation in pixel-to-pixel intensity, significantly lower than GaAsP or PMT detectors.
Where a point scanning detector traditionally produces an intensity output only for each pixel, NSPARC comprises an array of 25 detectors that operates more like an extremely sensitive camera: two-dimensional spatial information from each scanned pixel is collected by the detector.
Optical lenses direct emission light to the detector, allowing it to be used with various objectives and magnifications, while simultaneously allowing the user to define the size of the illumination spot on the detector array. This enables oversampling of the conventional single airy unit emission from the confocal plane.
This two-dimensional information is immediately used to obtain ultra-fine structural information, which is lost in conventional detection.
With NSPARC detection, the fluorescence emission light is directed through optics to the array detector, where the projected light fills the array.
With traditional PMT or GaAsP detectors, the fluorescence emission light passes through a variable sized emission pinhole (typically set to 1 airy unit).
The combination of ultra-short dwell times with the AX R resonant scanner and NSPARC’s sensitivity allows longer, less phototoxic imaging data to be collected in live-cell assays.
With single photon detection sensitivity, the NSPARC detector’s extremely low noise profile and exceptional sensitivity make it a perfect match for AX R confocal resonant high-speed imaging, where the pixel dwell time is as short as 200 nanoseconds, enabling image acquisition at video frame rate. More details can be extracted from images for downstream analysis and computation.
NSPARC’s array detection provides spatial sampling of the confocal point spread function in every pixel. This method detects information that can be utilized to extract enhanced resolution performance both laterally and axially. Built-in variable emission optics increase flexibility to allow users to replicate the function of a pinhole. This means the ability to prioritize enhanced optical sectioning or increased overall signal collection depending upon specific experimental needs.
The variable emission optics allow Nikon to offer many compatible low and high mag objectives to match specimens. This includes silicon immersion objectives which minimize refractive index mismatches, improving overall system performance.
Coupled with the AX/AX R's ultra-large 25mm FOV, the system supports a wide selection of objectives capable of obtaining image data from large overviews down to extremely fine details, which can then be measured and analyzed.
The NSPARC detector can be integrated on its own as the only detector for the AX/AX R, or as an additional detector for a multichannel AX/AX R system with either the DUX-VB or ST detector units and an optional transmitted light detector.
Current AX users can upgrade systems to add the NSPARC detector as well.