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Confocal microscopy is an advanced microscopic technique. The prime advantage of the confocal microscope over other microscopy techniques is its ability to block the out-of-focus light from the illuminated samples using pinholes. It is widely used with fluorescence optics to obtain high-resolution, sharp contrast images. Unlike optical microscopes, confocal microscopes use a focused beam of light laser to scan the entire sample surface at different z-planes. These microscopes are, therefore,...
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A 72 × 60 Angle-Sensitive SPAD Imaging Array for Lens-less FLIM.

Changhyuk Lee1,2, Ben Johnson3,4, TaeSung Jung5,6

  • 1School of Electrical and Computer Engineering, Cornell University, Ithaca, NY 14853, USA. cl678@cornell.edu.

Sensors (Basel, Switzerland)
|September 7, 2016
PubMed
Summary
This summary is machine-generated.

We developed an angle-sensitive single photon avalanche diode (A-SPAD) array for lens-less 3D fluorescence lifetime imaging. This technology maps fluorescent sources in 3D space with micrometer precision using photon arrival times and incident angles.

Keywords:
3-D image sensorCMOS avalanche photodiodesSPADSPAD arraysexponential decayfill-factorfluorescence imaginghighly sensitivity photodetectorsin-vitrolab-on-chiplifetime microscopylow power imagingphoto-detectorphoton timingpoint-of-carerangefindersingle photon detectorstime-correlated measurements

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Area of Science:

  • Photonics and Imaging
  • Biomedical Optics
  • Semiconductor Device Physics

Background:

  • Lens-less imaging techniques are crucial for miniaturization and cost reduction in advanced imaging systems.
  • Fluorescence Lifetime Imaging (FLIM) provides functional information beyond intensity, but 3D FLIM is challenging.
  • Single Photon Avalanche Diodes (SPADs) offer high timing resolution for time-correlated measurements.

Purpose of the Study:

  • To introduce a novel angle-sensitive SPAD (A-SPAD) array for lens-less 3D fluorescence lifetime imaging.
  • To enable micrometer-scale 3D mapping of fluorescent sources with varying lifetimes.
  • To demonstrate a compact and efficient imaging solution without post-processing.

Main Methods:

  • Development of a 72x60 A-SPAD array integrating SPADs with diffraction gratings.
  • Utilizing time-resolved operation of SPADs to prevent saturation and precisely measure photon arrival times.
  • Incorporating pixel-level counters for reduced data rates and enhanced timing control.
  • Fabrication in standard 180 nm CMOS technology.

Main Results:

  • Successful demonstration of lens-less 3D fluorescence lifetime imaging.
  • Achieved micrometer-scale spatial resolution in 3D.
  • Validated the angle-sensitivity of the SPAD array for incident light.
  • Characterized the A-SPAD array performance without any post-processing.

Conclusions:

  • The A-SPAD array is a viable technology for high-resolution, lens-less 3D FLIM.
  • This approach simplifies imaging systems and reduces data processing requirements.
  • The integrated design offers a promising platform for advanced biomedical and materials science imaging applications.