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Tumor Discovery                                                         Breast cancer optical differentiation



            2.7. Statistical analysis                          the significant differences among the various types of

            So far, the commonly used methods to calculate the   breast tissues and to select the optimum wavelength.
            scattering and absorption properties of the various   2.8. System efficiency analysis
            mediums are:
                                                               The efficiency of the presented system analysis methods is
            (i)  Monte Carlo (MC), which is a general class of   achieved by comparing the outcomes with the histological
               computational  algorithms  to  achieve  a  numerical   investigations. Regarding the results of these comparisons,
               outcome by relying on random sampling. MC in the   three numerical values (sensitivity, specificity, and accuracy)
               optical field is effective for a broad range of light µa,   could be measured to evaluate the various spectral analysis
               µs, and photon paths .                          methods, as shown in Equations XIII, XIV, and XV:
                                [57]
            (ii)  Diffuse approximation (DA), which is an alternative
               calculation method to calculate the scattering and   Sensitivity =  TP                    (XIII)
               absorption properties of turbid mediums .                     TP FN+
                                                [58]
            (iii) IAD, which is an extended method from the adding
               double (AD) method, and exploited to solve the                  TN
               radiative transport equation in the optical field sector   Specificity =  TN FP+          (XIV)
               related to the light’s interaction with the tissues in a
               slab geometry .
                           [59]
              The  radiative  transport  equation  could  be  used  to
            achieve light intensity distribution for the physical                                        (XV)
            mediums, as shown in Equation X .                    Where true positive (TP) is the cases detected by the
                                       [60]
            dI rs, ( )       s )      µ s  p ss Ir sd, (  , (  proposed system as actual masses (tumors); false negative
               ds  =−(µ  a  + µ  Ir s , ( ) +  4π  ∫  ) ′  ) ′  θ    (FN) is the cases of the system which had not been detected
                                                               and have masses; true negative (TN) is the cases detected
                                         4π
                                                        (X)    by the proposed system as normal, and they are normal
              Where I (r,s) is the measured intensity per unit length,   cases; and false positive (FP) is the cases mistakenly
            r is the target location, s is the unit direction vector,   detected by the presented system as abnormal masses, and
              (
            ps s, ′)  is the phase function, and θ is the solid angle.  they are normal cases.
              Although there is no analytical solution for Equation X,   3. Results
            it is achievable by exploiting the MC technique [61,62] .   Our primary goal of these assessments is to investigate the
            Moreover, the IAD method is used to solve the radiative   optical properties of the ex vivo breast samples (normal/
            transport equation. IAD technique and MC model have   tumor) by identifying the spectral signatures through
            offered more precise approximations of optical properties   incorporating the HS camera capabilities to provide the
            for the biological tissue (µ , µ , g) better than other methods.   essential data for diagnostic and therapeutic applications
                                a
                                  s
            Two dimensionless quantities are exploited in the whole   concerning breast cancer. We set up two diverse
            process of the IAD, that is, the albedo (a) and the optical   frameworks (reflection/transmission) methods using the
            depth ( ), which are well-defined in Equations XI and XII:  HS camera at wavelength range (400 ~ 1000 nm) and with
                    µ                                          a polychromatic light source in the VIS-NIR range for this
               a =�  s                                 (XI)
                  µ  s  +�µ  a                                 examination.
                                                                 We initially exploited the first framework (reflection
                        µ
                = ( t µ  s  + )                      (XII)    method) to measure the investigated ex vivo breast tissue
                        �
                         a
                                                               sample’s light R ; one of the investigated cases is presented
                                                                           d
              Where is the sample’s thickness (mm), the measured   in  Figure  3. The solid  red line represents the measured
            values of R , the total diffuse transmittance (T ), and the   tumor tissue’s R  spectrum, and the solid blue line identifies
                                                  d
                     d
            unscattered  collimated  transmittance  (T)  are  applied  to   the normal tissue’s R  spectrum over the VIS-NIR range.
                                                                           d
                                             c
            the IAD process to calculate the (µ , µ ).                          d
                                       a  s                    From the measured light R  for the investigated samples,
                                                                                     d
              Due to the minimum computational time and high   we could visually highlight the spectrum peaks, which
            accuracy comparable to both DA and MC methods, we   distinguish between the normal and the tumor tissues at
            exploited in our system the IAD method for breast tissue   wavelength range 600 ~ 680 nm and 750 ~ 960 nm at the
            characterization and descriptive analysis (T-test) to verify   VIS range and NIR range, respectively.
            Volume 2 Issue 1 (2023)                         7                           https://doi.org/10.36922/td.258
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