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Phosphorescence Lifetime Imaging (PLIM)

A time-resolved Imaging technique based on long lived excited states in luminescent materials

Phosphorescence Lifetime Imaging (PLIM) is similar to Fluorescence Lifetime Imaging (FLIM), only that it images the phosphorescence from the sample and consequently covers time ranges up to milliseconds. Analogous to FLIM, the contrast in a PLIM image is based on the lifetime of individual fluorophores rather than their emission spectra. The phosphorescence lifetime is defined as the average time that a molecule remains in an excited state prior to returning to the ground state by emitting a photon.

PLIM, or generally the characterization of phosphorescent compounds has been of great importance in the field of materials science namely chemical sensing for many years , and has renewed its interest over the past decade with the booming development of Organic Light Emitting Diode (OLED) technology. Other typical samples include metal ions complexed with organic ligands, which can be used to, e.g., image oxygen consumption in living cells.

Scheme of general setup for a fluorescence lifetime imaging microscopeMulti-channel scaling (MCS) or Time-Correlated Single Photon Counting (TCSPC) with multi-stop capabilities is used to determine the phosphorescence lifetime. In both cases, one measures the time between sample excitation by a pulsed laser and the arrival of the emitted photon at the detector. The methods requires a defined “start”, provided by the electronics steering the laser pulse or a photodiode, and a defined “stop” signal, realized by detection with single-photon sensitive detectors (e.g. Single Photon Avalanche Diodes, SPADs or Photomultiplier Tubes, PMTs). The measurement of this time delay is repeated many times to account for the statistical nature of the fluorophores emission. The delay times are sorted into a histogram that plots the occurrence of emission over time after the excitation pulse.

In order to acquire a phosphorescence lifetime image, the photons have to be attributed to the different pixels, which is done by storing the absolute arrival times of the photons additionally to the relative arrival time in respect to the laser pulse. Line and frame marker signals from the scanner of the confocal microscope are additionally recorded in order to sort the time stream of photons into the different pixels.
In contrast to TCSPC based FLIM, PLIM can usually be performed efficiently with galvo scanners for compounds with lifetimes up to a few µs only due to their high scanning speeds that limit the dwell time per pixel. If the dwell time is shorter than the time needed for the phosphorescence to decay completely, photons will be sorted into wrong pixels, leading to distorted images. PLIM is therefore best performed with piezo scanning devices, which enable lower scanning speeds than galvo scanners. As the ideal pixel dwell time is ~50-100 times the luminescence lifetime, measurements on dyes with slow phosphorescence can take a very long time.

Consequently the essential components of a FLIM set-up are:

  • pulsed laser source - for components with lifetimes >1µs, excitation using pulse trains is recommended in order to increase the excitation efficiency
  • single photon sensitive detector
  • dichroic mirror (to separate fluorescence signal from excitation light)
  • objective (to focus the excitation light into the sample and collect fluorescence signal)
  • MCS or TCSPC unit with multi-stop capabilities to measure the time between excitation and fluorescence emission

Related technical and application notes: