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O2 is one of the key environmental parameters for living systems, and knowledge of the distribution of O2 and its dynamics is important for many biological studies1,2,3. The assessment of tissue oxygenation by means of phosphorescent probes4,5,6,7,8 and PLIM9,10,11,12,13 are gaining popularity in biological and medical research3,9,14,15,16,17,18,19. This is because PLIM, unlike fluorescence or phosphorescence intensity measurements, is not affected by external factors such as probe concentration, photobleaching, excitation intensity, optical alignment, scattering, and autofluorescence.
However, current O2 PLIM platforms are limited by their sensitivity, image acquisition speed, accuracy, and general usability. Time-correlated single photon counting (TCSPC), combined with a raster scanning procedure, is frequently used in PLIM and fluorescence lifetime imaging microscopy (FLIM) devices20,21,22. However, since PLIM requires a long pixel dwell time (in the millisecond range), the time of image acquisition is much longer than what is required for FLIM applications20,22,23. Other techniques, such as gated CCD/CMOS cameras, lack single photon sensitivity and have low frame rates20,24,25,26. Moreover, the existing PLIM systems are mostly used in the microscopic format, while macroscopic systems are less common27.
The TCSPC-based PLIM macro imager28 was set up to overcome many of these limitations. The design of the imager was greatly facilitated by the use of a new opto-mechanical adapter, Cricket, which has the following: i) two C-mount adapters, which provide easy coupling of the camera module on the back side and objective lens on the front side; ii) an internal housing for an image intensifier and a power socket for the latter on the outer side of the Cricket; iii) an internal space behind the front-side C-mount adapter where a standard 25 mm emission filter can be housed in front of the intensifier; and iv) a built-in light collimating optics with ring regulators, which allow optical alignment/focusing between the lens and the camera to produce crisp images on the camera chip.
In the assembled imager, the camera module is coupled to the back side of the Cricket adapter, which also houses an image intensifier consisting of a photocathode followed by a microchannel plate (MCP), an amplifier, and a fast scintillator, P47 phosphor. A 760 nm ± 50 nm emission filter is fitted inside the Cricket, and an objective lens, NMV-50M11'', is attached to the front side C-mount adapter. Finally, the lens and the camera are aligned optically with ring regulators.
The role of the intensifier is to detect incoming photons and convert them into fast bursts of light on the camera chip, which are registered and used to generate emission decays and lifetime images. The camera module comprises an advanced TCSPC-based optical sensor array (256 pixels x 256 pixels) and a new generation readout chip29,30,31,32,33, which allow the simultaneous recording of the time of arrival (TOA) and the time over threshold (TOT) of photon bursts at each pixel of the imaging chip with a time resolution of 1.6 ns and an 80 Mpixel/s readout rate.
In this configuration, the camera with the intensifier has single-photon sensitivity. It is data-driven and based on the speedy pixel detector readout (SPIDR) system34. The spatial resolution of the imager was previously characterized with planar phosphorescent O2 sensors and a resolution plate mask. The instrument response function (IRF) was measured by the imaging of a planar fluorescent sensor under the same settings as used for all the other measurements. The lifetime of the dye of around 2.6 ns was short enough for it to be used for the IRF measurement in PLIM mode. The imager can image objects of up to 18 mm x 18 mm in size with spatial and temporal resolutions of 39.4 µm and 30.6 ns (full width at half-maximum), respectively28.
The following protocols describe the assembly of the macro imager and its subsequent use for mapping the O2 concentration in biological samples stained with the previously characterized near-infrared O2 probe, NanO2-IR35. The probe is a bright, photostable, cell-permeable O2-sensing probe based on platinum (II) benzoporphyrin (PtBP) dye. It is excitable at 625 nm, emits at 760 nm, and provides a robust optical response to O2 in the physiological range (0%-21% or 0-210 µM of O2). The imager is also demonstrated to characterize different sensor materials based on Pt(II)-porphyrin dyes. Overall, the imager is compact and flexible, similar to a common photographic camera. In the current setup, the imager is appropriate for different widefield PLIM applications. Substituting the LED with a fast laser source will further improve the performance of the imager and could potentially enable nanosecond FLIM applications.