We propose tissue characterization with ballistic photons, those whose direction or propagation speed is not affected by the presence of tissue. The most critical aspect of the tissue characterization problem is calibration of experimental measurements. The calibration method relates the fringe irradiance (power modulation in one interferometer arm) with the sample concentration under controlled conditions. During this step, the absorption and scattering indices β a and β sc are determined as a function of concentration for each material or tissue of interest, using a set of containers to vary travel distance D. It is assumed that linear scattering coefficient, k sc (absorption coefficient, α a ), is proportional to the number of scattering particles per unit volume, or particle concentration, c, in [ml/l]. Attenuation is proportional to concentration of scattering (absorption) centers and the sample length. The sensitivity of method is estimated at 10 -19 with uncoated plate beam-splitters and intensified photon-counting detector.
Signal broadening within tissueOptical means of tissue characterizations have become of great importance within the last 20 years, due to the availability of short pulse laser sources and detectors with nearly instantaneous response. 1-4 With the understanding of the structural changes introduced in the biological samples due to demanding sample preparation methods in electron microscopy practice, the optical techniques started to be once again considered superior in biological sample characterization.Identification of three parameters is believed to be the key to the knowledge and characterization of the biological samples under evaluation: the linear coefficient of absorption μ a [mm -1 ], the linear coefficient of scattering μ sc [mm -1 ], and an all-purpose fudge factor whose primary function is to relate linear tissue properties with their volume features. 5 Experimentally, these factors are difficult, if not impossible, to determine with a high degree of certainty because there does not exist a well-defined event in time to separate once-, twice-, and multiply-scattered photons from the ballistic photons. 6-8 We define the ballistic photons to be those that are transmitted through the sample without undergoing any scattering, not even suffering a small-angle deviation, and that are not absorbed by the sample.Previously, two partial solutions were implemented to address these shortcomings providing methodology to arrive at these two coefficients, μ a and μ sc , employing a certain amount of data fitting. Experimentally, the coherence of the illuminating laser beam was decreased to shorten the time interval during which useful signal was collected. 9 Theoretically, and within the data-processing community, increasingly sophisticated models started to be developed to determine these parameters using statistical techniques. 10 Both of these schemes led to the evaluation of parameters, even though the time-gating interval in the first does not appear to be an intrinsic consequence of ...