Abstract
Nowadays, transillumination imaging is more popular used in the medical field with the development of the vein finder and the non-invasive diagnosis applications. Near-infrared light with a wavelength of 700 - 1200 nm has relatively high transmission through biological tissue. Using near-infrared light, we can able to obtain a two dimensional (2D) transillumination image of the internal absorption structure such as blood vessel structure, liver ... in the body noninvasively. Even with a simple system (light-emitting diode (LED)'s array and low-cost camera), we could obtain the blood vessel transillumination image of human arm. However, the image is severely blurred due to the strong scattering in the tissue. We have devised the depth-dependent point spread function (PSF) to suppress the scattering effect in fluorescent imaging. In previous studies, we successfully applied this principle and developed a technique to reconstruct the absorbing structure in a turbid medium without using fluorescent material. The feasibility and effectiveness of the proposed technique were verified in experiments. However, this point spread function (PSF) is depth dependence, so that the depth information is required in practice. In order to make this method more practical, the new techniques for estimating the parameters of absorbing structure (depth and width) in the turbid medium by convolution and de-convolution with the point spread function (PSF) were devised. This paper presents a new technique for the estimation depth of an absorber in 2D transillumination image. This new technique was developed to estimate the depth of the absorber in turbid medium by convolution operation with the point spread function (PSF). By observing images with two-wavelength selected at which the scattering property of the medium is different. The transillumination image at one of the wavelengths is convolved with the PSF of another wavelength. Two images of alternative wavelengths are compared while changing the depth of the PSF. We can obtain the correct depth that gives a minimum difference between the two convoluted images. This technique does not require the repetition of the unstable deconvolution operation. The effectiveness of the proposed technique was verified in simulation and experiment.
Highlights
The less absorption of those main chromophores of biological tissue within the near-infrared (NIR) range (700 - 1200 nm) causes the relatively high transmission of the near-infrared light through biological tissue
By suppressing the scattering effect successfully, we could restore the clear image from the blurred image by de-convolution with the appropriated point spread function (PSF)
While changing the depth step-by-step, two convoluted images were compared after convolving the captured image at one of the wavelengths with the PSF calculated by using the absorption and scattering coefficients from another wavelength
Summary
The less absorption of those main chromophores (melanin, oxy-hemoglobin, deoxy-hemoglobin, and water) of biological tissue within the near-infrared (NIR) range (700 - 1200 nm) causes the relatively high transmission of the near-infrared light through biological tissue. We can apply the depth-dependent PSF of the light source in turbid medium calculated from Eq (3) to de-blur the observed transillumination image of the absorbing structure. This consideration was validated and verified in simulation and experiment [3,4]. Where d, ×, Ob(λi, d), Or, and PSF(λi, d), are respectively denote the depth of the absorbingstructure, the convolution operation, the observed image, the original light-absorbing structure, and the blurring PSF with medium characteristics of each wavelength. As mentioned in section Using two-wavelength perspective images, with a PSF calculated from Eq (3) at a specific depth d, we cannot restore the whole observed image of the complex light-absorbing structure. The results shown that the proposed techniques in section Using two-wavelength perspective image and section Using a single-wavelength observed image can be applied in practice with a good condition of an imaging system
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