The accurate optical characterization of highly scattering media, such as biological tissues, is of relevance in many fields, yet is faced with important challenges. We are developing novel setups to overcome some of these challenges; our current work include: time-resolved measurements and a double-integrating sphere setup for the determination of the absorption coefficient and the mean free transport path, extinction measurements using imaging, an ellipsometric setup for the measurement of the refractive index. The reliability and accuracy of all these measurement techniques are assessed via calibration studies and compared to analytical/numerical models.
Polarimetry is emerging as a promising, minimally invasive diagnostics tool.
The interaction of polarized light with matter often reveals features that are invisible to ordinary imaging techniques / diffuse optics. We have developed a versatile polarimetric microscope, that can measure with high speed cross- and auto-correlations
between arbitrarily polarized incident and backscattered light. This microscope has undegone a rigorous calibration process by performing measurements on well-characterized colloidal suspensions and comparing the results with Monte Carlo simulations.
Long term goals include differentiating tumorous from healthy tissues (in collaboration with the Neurosurgical Institute of the Inselspital Bern), diagnosing the severeness of burn injuries, as well as studying the fundamentals of polarized light propagation in random media, whereby more theoretical work is carried out.
We have built a confocal laser scanning microscope to perform fluorescence lifetime imaging to work on tissue diagnostics. The setup uses time-correlated single photon counting (TCSPC), together with a tunable picosecond pulsed excitation source.
Ongoing investigations include a collaboration with the Department of Chemistry and Biochemistry at the University of Bern, whereby the interactions of photosensitizers with their micro-environments are studied in the frame of photodynamic therapy.
Optical nerve stimulation and bone drilling are two applications that have been studied in different areas. In these applications water is the most important component. Near Infrared and infrared wavelengths have high absorption in water.
It has been observed that laser assisted bone cutting causes less damage to the tissue than mechanical drilling. We therefore investigate and optimize the use of high power infrared laser ablation for bone cutting or drilling.
In optical nerve stimulation, infrared laser light is used to stimulate peripheral nerves to generate an action potential. Optical nerve stimulation gives better spatial selectivity and has less stimulation artifacts than electrical stimulation. The technique is still new and we investigate the influence of different laser parameters on stimulation efficiency in Lumbricina.
One of our research goals is the combination of these techniques in minimally invasive cochlear implantation surgery. In this procedure drilling and stimulation could be integrated in a single optical system, where the stimulation serves as feedback to safeguard the nerves.
Tissue bonding of incisions is an important step in most surgical procedures. Conventional methods, namely sutures and staples, possess serious drawbacks, such as additional tissue injury, foreign body reactions, and difficult and tedious execution. Laser-tissue-soldering (LTS) can be faster, easier to apply, and less traumatic. In LTS, a protein solder is applied to the joined tissue edges and heated via optical absorption of laser light. Thermal alteration of the molecular structure of solder and tissue forms bonds leading to tissue fusion. We investigate a technique where the laser energy is absorbed by the chromophore indocyanine green (ICG), while the bonding strength is provided by the protein albumin. Our goal is to develop a standardized patch encapsulating both the ICG and the albumin solder, and the optimization of the temperature response.
Cilia are roughly 10_m long hair-like protrusions of the cell membrane. In the airways of higher organisms, their coordinated oscillatory beating movements causes directed motion of the mucosal fluid, cleaning the airways from adhering inhaled particles and harmful substances.
It is obvious that in order to achieve efficient directed transport, the ciliary motions must be, at least locally coordinated. Immotile cilia or lack of coordination are made responsible for different severe diseases, such as primary ciliary dyskinesia, therefore there is a demand for reliable diagnostic techniques. The key to every diagnosis is a sound knowledge of the healthy system. To achieve this goal, we focus on two complementary lines of action:
We have developed a general purpose Monte Carlo simulation package based on the concepts outlined by Rička et al. in “Optical-Thermal Response of Laser-Irradiated Tissue” (Springer, 2011) and initially intended to model light propagation in soft condensed matter such as biological tissues, but whose scope is far from being restricted to radiative transfer in tissues. The software is playfully named jaMCp3: just another Monte Carlo program for polarized photon propagation and composed of a user interface in IDL/GDL and a stand-alone photon path generation routine implemented in C++. Besides the Mie scattering model, the program includes a novel scattering model (the “polarized version of the generalized Henyey-Greenstein” scattering law) containing a structure factor parameter. The latter is particularly well-suited to describe light propagation in soft condensed matter such as biological tissue. Moreover, the simulations are conducted in a voxel space, where custom and complex geometrical structures can easily be generated. These also allow for the treatment of Fresnel reflection/refraction processes.
JaMCp3 has previously been subject to preliminary writings in its embryonic stages: “Simulating light propagation: towards realistic tissue models” (SPIE proceeding, 2011) and “Polarized Light Propagation in Biological Tissue: Towards Realistic Modeling” (Doctoral thesis, 2011). Yet, over the past years, jaMCp3 underwent rigorous testing stages (see references below). Certainly, the validation of such a MC program is a prime challenge, as quantitative comparisons, either with experiments or other simulation programs, are difficult to perform, and furthermore, the modeling of complex geometrical structures is bound to induce various numerical singularities, which might not be apparent at first glance. We are currently preparing a manuscript that details our program's main features and gives examples of its diverse possible outputs (3D fluence, 3D absorbed dose, polarimetric images...). The package, together with its user's manual, will soon be made available here for download, however, it is already possible to use it by contacting Günhan Akarçay ( hidayet.akarcay at iap.unibe.ch ).
(1) Akarçay et al., “Determining the optical properties of a gelatin‑TiO2 phantom at 780 nm,” Biomed. Opt. Exp. 3 (2012).
(2) Hiltpold, “Bestimmung optischer Gewebeparameter,” Bachelor thesis (2012).
(3) Akarçay et al., “Monte Carlo modeling of polarized light propagation: Stokes vs Jones–Part I,” Appl. Opt. (2014).
(4) Akarçay et al., “Monte Carlo modeling of polarized light propagation: Stokes vs Jones–Part II,” Appl. Opt. (2014).
ERRATUM in (4): We noticed a small error in the last column (input state |O>) of the ''Primary data'' shown in Figure 1. The images corresponding to < L+ | and < L- | analyzers should be exchanged with the images obtained with < C- | and < C+ | analyzers, respectively. This was just a small bug in the representation of the data and does not affect the other figures/results. (See entirety of figures in the .pdf file linked at the bottom of this page.)
It is remarkable that the physics of water, the substance that covers two thirds of our planet, is still not fully understood. This holds true especially also for its anomalous properties compared to other liquids.
Our research aims at the understanding of the anomalies of water, in particular those observed in the supercooled metastable state. To achieve this goal, pure water inclusions inside quartz are synthesized covering a density range of 996-916 kg m-3. Microthermometric measurements are conducted to determine the temperature at which water phase transitions occur. Single ultrashort (femtosecond) laser pulses are employed to overcome metastable phase states in high density inclusions. In pure water inclusions, the phase transition from liquid to solid is not visible from microscopic observations, thus, confocal Raman spectroscopy is used to determine ice nucleation temperatures. In addition, we use Brillouin spectroscopy to determine the speed of sound and, thus, the pressures inside the inclusions.
The experimental outcomes present valuable benchmarks to evaluate and further improve theoretical models describing the p–V–T properties of metastable water in the low-temperature region.
Spectral OA imaging exploits the wavelength-dependent optical absorption properties of specific chromophores in tissue (e.g. hemoglobin), with as goal to provide quantitative estimates of their spatially varying concentrations. A physiologically important example is the determination of local blood oxygen saturation, based on the distinct absorption spectra of oxy- and deoxyhemoglobin in the near-infrared range. This is of particular relevance for the study of oxygenation heterogeneity in tumors, the early detection and monitoring of cerebral ischemia in brain, and of other abnormalities characterized by a change in tissue oxygenation or perfusion status.
A central issue, which makes quantitative oxygenation measurements challenging, is the unknown extent of wavelength-dependent optical attenuation inside biological tissue. It engenders a spectral distortion of the recorded OA signals relative to the absorption spectrum of the chromophore's of interest. Only when this distortion is taken into account (which is referred to as "spectral correction"), a recovery of accurate quantitative information is possible.
As part of our research on quantitative deep OA imaging, we investigate techniques to correct for the spectral distortion of the recorded OA signals.
Optoacoustic (OA) Microscopy is a promising non-invasive medical imaging technique that is able to obtain 3D structural information by making use of the optoacoustic effect, i.e. the creation of ultrasonic pressure waves upon absorption of light. Combining this with the fact that the hemoglobin contained in red blood cells is the dominant absorber inside biological tissue, it provides high contrast 3D imaging of the vasculature at a spatial resolution superior to what can be achieved by MRI or micro-CT. Since blood perfusion and -oxygenation are important markers for cancer detection, OA microscopy could prove valuable in this context. Using OA microscopy, our group has studied the brain vasculature of malaria-infected mice (see Figure) and is engaged in the general development of the technique.
For clinical combined optoacoustic (OA) and ultrasound (US) imaging, maximum flexibility is provided when irradiation optics and ultrasound detector are integrated in one handheld probe. The drawback of this epi-illumination geometry is the relatively high laser intensity close to the ultrasound probe. This generates strong background signals that clutter the OA image, thus limiting imaging depth (see Figure, phantom study). We investigate various different techniques for clutter reduction, among them localized vibration tagging (LOVIT): A long pulsed ultrasound beam generates acoustic radiation force (ARF) that induces localized tissue displacement at its focus. Subtraction of OA images acquired before and after the ARF push preserves true OA signal in the displacement focus while eliminating the clutter background (see Figure). We are implementing a clinically realistic setup where the same linear array probe is used both for imaging and ARF generation.
The speed of sound (SoS) inside tissue depends on tissue composition and is therefore a promising diagnostic marker for disease progression. With the invention of computed ultrasound tomography in echo-mode (CUTE) we are now able to achieve a contrast and spatial resolution sufficient for clinical imaging. Pulse-echo ultrasound reconstructs acoustic reflectors inside the tissue based on the acoustic round-trip time of the echoes (axial resolution) and focusing (transversal resolution). CUTE is based on sensing the phase shift of local echoes when insonifying the tissue under various different angles using steered ultrasound transmissions. The echo phase shift is related to the changing round-trip time and thus to path integrals of SoS, and the spatial distribution of SoS can therefore be reconstructed by solving the inverse problem. The Figure shows a typical example of combined conventional ultrasound (left, shows the echoes) and real-time CUTE (right side) in the abdomen: The different SoS of different tissue layers are nicely resolved (s: skin, sf: subcutaneous fat, m: muscle, pf: postperitoneal fat, l: liver). In addition, we are active in further developing through transmission ultrasound tomography, which has been shown by other groups to provide high contrast images of the breast for cancer diagnosis.