Mid-infrared photonic imaging strategies
Abstract
Imaging at mid-infrared (MIR) wavelengths between from 3–12 µm can provide unique
insights and contrast mechanisms because of the low scattering of MIR light and the chemical
specificity of MIR absorption. Consequently, new light sources and spectroscopic methods
applied in the MIR offer previously unavailable capabilities for MIR hyperspectral (HS) or
depth-resolved imaging. In this thesis, I report the development of three new MIR imaging
techniques, configured in particular for applications in heritage science.
Current MIR HS imaging technologies are expensive, as they employ complex cooled
MIR detectors, or slow, in terms of acquisition rates. These factors limit widespread use
in certain applications such as pigment mapping of paintings for cultural heritage. Here, I
demonstrate two relatively inexpensive and fast HS imaging systems which utilise novel
compressive sensing strategies.
The first system is an imaging Fourier-transform spectromter (IFTS) based on recording
a set of microbolometer camera frames of a sample’s response to illumination by uniquely
spectrally structured blackbody radiation from a Michelson interferometer. The developed
non-uniform sampling strategy was, to my knowledge, the first practical implementation of
compressive sensing in Fourier-transform spectroscopy and enabled a sampling rate as low as
15% Nyquist-limited sampling with a generic prior. The instrument was used in a campaign
at the Hunterian Museum on the artwork “Uplands in Lorne” by David Young Cameron.
A second system utilised a fast digital micromirror device (DMD) to arbitrarily shape
MIR spectra, providing sample illumination by optimised spectral structures for material
identification.
OCT has seen extensive work in the visible and near-infrared (NIR) but not as much
in the MIR. This is, in part, due to the limitation of suitable MIR ultrafast sources. MIR
OCT has the advantage of greater sample penetration depth which could find applications
in the security sector. Results are presented from an MIR time-domain OCT system with
an ultrafast orientation-patterned gallium phosphide (OP-GaP) optical parametric oscillator
(OPO).