Marcelo
Saito Nogueira
*ab,
Siddra
Maryam
ab,
Michael
Amissah
ab,
Shane
Killeen
c,
Micheal
O'Riordain
c and
Stefan
Andersson-Engels
ab
aTyndall National Institute, Lee Maltings, Dyke Parade, Cork, T12 R5CP, Ireland. E-mail: marcelosaitonogueira@gmail.com; marcelo.nogueira@tyndall.ie
bDepartment of Physics, University College Cork, College Road, Cork, T12 K8AF, Ireland
cDepartment of Surgery, Mercy University Hospital, Cork, T12 WE28, Ireland
First published on 5th October 2023
Colorectal cancer (CRC) is the third most common and second most deadly type of cancer worldwide, representing 11.3% of the diagnosed cancer cases and resulting in 10.2% (0.88 million) of the cancer related deaths in 2020. CRCs are typically detected at the late stage, which leads to high mortality and morbidity. Mortality and poor prognosis are partially caused by cancer recurrence and postoperative complications. Patient survival could be increased by improving precision in surgical resection using accurate surgical guidance tools based on diffuse reflectance spectroscopy (DRS). DRS enables real-time tissue identification for potential cancer margin delineation through determination of the circumferential resection margin (CRM), while also supporting non-invasive and label-free approaches for laparoscopic surgery to avoid short-term complications of open surgery as suitable. In this study, we have estimated the scattering properties and chromophore concentrations based on 2949 DRS measurements of freshly excised ex vivo specimens of 47 patients, and used this estimation to classify normal colorectal wall (CW), fat and tumor tissues. DRS measurements were performed with fiber-optic probes of 630 μm source–detector distance (SDD; probe 1) and 2500 μm SDD (probe 2) to measure tissue layers ∼0.5–1 mm and ∼0.5–2 mm deep, respectively. By using the 5-fold cross-validation of machine learning models generated with the classification and regression tree (CART) algorithm, we achieved 95.9 ± 0.7% sensitivity, 98.9 ± 0.3% specificity, 90.2 ± 0.4% accuracy, and 95.5 ± 0.3% AUC for probe 1. Similarly, we achieved 96.9 ± 0.8% sensitivity, 98.9 ± 0.2% specificity, 94.0 ± 0.4% accuracy, and 96.7 ± 0.4% AUC for probe 2.
DRS uses the diffuse reflected light travelling inside the tissue to extract tissue structural and biochemical information based on light scattering and absorption properties, respectively. Scattering properties include reduced scattering amplitude α′, Mie scattering power bMie, and the percentage contribution of Rayleigh scattering fRay to the total Mie scattering in the tissue. These scattering properties can be associated with tissue microstructures including organelles (e.g., mitochondria) and other structures (e.g., cell and organelle membranes, collagen fibers and fibrils). Similarly, absorption properties consist of volume fractions of tissue chromophores (represented by fchromophore) including β-carotene, bile (fbile), bilirubin, ceroid, collagen, deoxyhemoglobin (fHb), oxyhemoglobin (fHbO2), methemoglobin (fmetHb), water (fwater), lipid (flipid), and melanin.6,7
Previous DRS and hyperspectral imaging studies on colorectal cancer detection focused on either endoscopic8–15 or surgical16–23 applications. Feasibility DRS studies have employed surgical guidance techniques based on machine learning (ML) approaches using either spectra collected from the outer surface of tissues through surface contact probes or spectra collected from interstitial tissues through needle-shaped probes.16–23 However, previous studies have several limitations. First, these studies explored only small tissue volumes determined by small source-to-detector distances (SDDs) employed in the fiber-optic probes used. Second, the only study determining tissue chromophore concentrations and scattering properties22 used analytical models based on the diffusion equation, which is known not to describe the reflectance at small SDDs well under the conditions in which DRS spectra were collected.5,6,10,11,14,24 Third, DRS surgical guidance studies analyzed visible and near-infrared wavelengths ranging up to 1600 nm only. Finally, the number of measurements collected in DRS studies ranges from 117 to 1273 per dataset (i.e., 117–1273 DRS measurements collected under the same conditions). Machine learning models considering thousands of wavelengths directly as predictors for validation in less than thousand measurements could lead to overfitting. Our study has overcome all of the above limitations.
In this study, we quantified tissue microstructural and biochemical parameters for potential clinical decision making in open surgery, laparoscopic surgery, and robotic surgery. Our study combined ML models with reflectance spectral fitting extraction of tissue chromophore concentrations and scattering properties from 2949 locations on fresh ex vivo tissue samples of 47 patients (1386 tissue locations with a 630 μm SDD probe and 1563 locations with a 2500 μm SDD probe). This extraction relied on a reflectance lookup table (LUT) built using MC simulations of light propagation in tissues10,24 and covering a wide range of optical properties (absorption coefficient from 0.01 to 300 cm−1 and scattering coefficient varying from 0.1 to 1000 cm−1 with the anisotropy factor g = 0.9). To train these ML models, we used a classification and regression tree (CART) algorithm to estimate thresholds of scattering properties and chromophore concentrations to classify normal colorectal wall (CW), fat and tumor tissues. All DRS measurements were performed in the extended wavelength range between 350 and 1920 nm by using fiber-optic probes of 630 μm SDD (probe 1) and 2500 μm SDD (probe 2) to measure tissue layers ∼0.5–1 mm and ∼0.5–2 mm deep, respectively.8
Compared to our previous studies focusing on investigating the potential of DRS for colorectal tissue diagnostics,8–10 this study is aimed at analyzing fat and CW tissues for LS and OS guidance applications instead of malignant and healthy surrounding tissues for endoscopic applications. With that in mind, please note that our study is novel based on the analysis of a different set of tissues for a completely different clinical application from those of our previous studies. We also emphasize that the analysis of this paper cannot be used to guide endoscopic microsurgery,8–10 since tissues have been measured from outside the colon and/or rectum.
Number of patients | ||
---|---|---|
Gender | Female | 15 |
Male | 32 | |
Age (years) | Mean (± standard deviation) | 68 ± 11 |
Range | 40–89 |
We collected data from about 15 sites of freshly excised ex vivo CW tissues, 15 sites of fat tissues and 15 sites of tumor tissues on each colorectal specimen after surgical resection. To ensure sufficient representation of the tissue heterogeneity in our data collection, DRS measurements were performed over a typical area of 100 cm2. The measurement protocol consisted of first removing the colorectal specimen from the patient and transporting it to a measurement bench for DRS measurements. Next, we gently rinsed the specimen with water and cleaned it to remove any residual stool and excess of blood. Before starting DRS measurements, we placed the specimen on a measurement grid with the coordinates of the data collection locations. These locations were used to identify tissues based on demarcation by experienced surgeons and correlate tissue types with DRS spectra. On average, we took 40 minutes between specimen removal and the start of data collection, and about 1 hour after surgical resection for full data collection. We kept the tissue moist and preserved the physiological conditions to the best of our ability by putting a damp cloth on the specimen approximately every 7 measurements. Once we finished DRS data collection, we returned each specimen to the Pathology Department for processing and analysis according to standard protocols. The ground truth of our tissue types corresponding to our CRC DRS measurements was determined by histopathological analysis.
(1) |
To merge the reflectance spectra and correct for any slight reflectance mismatch between spectra collected from the two spectrometers, we used the overlapping spectral range between 1090 and 1140 nm to perform an interpolation by using the weighted sum of eqn (2):
(2) |
The resulting reflectance spectra Rexperimental(λ) were used for the estimation of chromophore concentrations and scattering parameters, as described in the next section.
(3) |
First, the spectral fitting used four types of input:
1. A measured reflectance spectrum Rexperimental(λ) to be fitted
2. The pure chromophore absorption spectra μa,chromophore(λ)
3. Wavelength-dependence of tissue scattering μ′s,tissue(λ) due to Rayleigh and Mie scattering (eqn (4))
4. A MC look-up table (LUT) of diffuse reflectance R(μa,μ′s) values generated with MC simulations
By associating the experimental reflectance of Rexperimental(λ) with a combination of (μa,tissue(λ), μ′s,tissue(λ)), we obtained Rtheoretical(λ) based on values of RMC(μa,tissue, μ′s,tissue) from the MC LUT. This association was only possible by using at least as many wavelengths as fitting parameters and allowed the extraction of fchromophore by using the equation:
(4) |
(5) |
Similarly, the scattering properties α′, bMie, and fRay were extracted by calculating the optimum μ′s,tissue(λ)
(6) |
It is worth noting that the tissue may contain traces of bilirubin found in blood at ranges between 5.8 and 40% in humans (based on bilirubin blood serum levels that vary between 10 and 50 mg dL−1 (ref. 30) and the total hemoglobin blood levels that vary between 121 and 172 mg dL−1 (ref. 29)). We did not include bilirubin as a chromophore with a significant contribution in our spectral fitting so that there is no contamination between the estimation of fbile and fbilirubin. Furthermore, we emphasize that the use of the bilirubin absorption spectrum in our reflectance spectral fitting would narrow the wavelength range of our fitting, since the bilirubin absorption spectrum was not reported over the broadband wavelength range used in our DRS measurements. Similarly, met-hemoglobin (metHb) has been taken into account not to interfere with the quantification of other chromophores due to absorption spectrum overlap and potential metHb formation in ex vivo tissues.
Finally, we removed StO2 and fmetHb predictors with variations in ex vivo settings (and thus could not be translated to an in vivo setting from our study). Therefore, we considered only THb, Rvessel, flipid, fwater, fbile, α′, fRay and bMie as input predictors for tissue classification.
Small SDD probe (probe 1) | Large SDD probe (probe 2) | |||||
---|---|---|---|---|---|---|
Biochemical/microstructural parameters | Fat | Colorectal wall (CW) | Tumor | Fat | Colorectal wall (CW) | Tumor |
THb (%) | 5.9 ± 2.0 | 6.5 ± 3.0 | 6.6 ± 3.9 | 2.3 ± 1.0 | 3.3 ± 1.3 | 4.8 ± 1.9 |
THC (μmol L−1) | 136.6 ± 46.0 | 151.8 ± 69.1 | 154 ± 90 | 52.6 ± 22.3 | 77.7 ± 30.7 | 111 ± 45 |
StO2 (%) | 99.8 ± 1.5 | 92.4 ± 13.7 | 66 ± 23 | 98.8 ± 3.7 | 73.3 ± 16.7 | 56 ± 18 |
R (μm) | 29.8 ± 29.7 | 3.8 ± 14.8 | 14 ± 11 | 20.9 ± 75.7 | 11.3 ± 6.9 | 24 ± 13 |
f lipid (%) | 64.9 ± 11.6 | 5.5 ± 14.0 | 1.4 ± 2.2 | 82.3 ± 9.5 | 10.6 ± 16.3 | 4.8 ± 3.0 |
f water (%) | 10.4 ± 10.2 | 81.9 ± 15.4 | 84.9 ± 7.2 | 12.1 ± 9.0 | 83.1 ± 16.5 | 86.7 ± 4.0 |
f bile (%) | 18.8 ± 9.2 | 6.1 ± 3.5 | 7.0 ± 4.8 | 3.3 ± 2.0 | 2.9 ± 1.5 | 3.7 ± 2.5 |
f MetHb (%) | 1.4 ± 0.8 | 0.9 ± 0.6 | 1.1 ± 0.7 | 0.4 ± 0.2 | 0.3 ± 0.2 | 0.3 ± 0.5 |
α′ (cm−1) | 14.2 ± 6.6 | 9.5 ± 3.7 | 15.9 ± 10.1 | 12.9 ± 12.2 | 5.7 ± 3.4 | 12.0 ± 5.6 |
b Mie | 0.1 ± 0.1 | 0.3 ± 0.2 | 0.5 ± 0.3 | 0.2 ± 0.4 | 0.5 ± 0.3 | 0.9 ± 0.4 |
f Ray (%) | 45.5 ± 30.2 | 32.0 ± 21.1 | 40 ± 27 | 42.5 ± 26.9 | 18.9 ± 21.3 | 36 ± 28 |
When comparing CW and tumor tissues, tumor has higher Rvessel, α′, and bMie, as well as slightly higher fwater and fbile, and slightly lower flipid. These results are valid for both probes, being more pronounced for probe 2 (2500 μm SDD probe). In particular, for probe 2, one can see that THb is slightly higher and the difference between StO2 of CW and tumor tissues is smaller compared to that in probe 1 (630 μm SDD probe). While this result may not be translated into in vivo colorectal tissues due to the study limitations described in subsequent sections,8 our results suggest that superficial tissue probed with probe 1 might be more sensitive to tissue metabolic rates once blood flow has been ceased. The higher difference in StO2 of ex vivo superficial tissues of the CW and tumor can be explained by the tumor higher metabolic rates leading to higher blood oxygen consumption, and the rates of replenishment of this oxygen through Hb exposure to atmospheric molecular oxygen forming HbO2 are significantly smaller than the blood oxygen consumption rates in tumors. On the other hand, rates of this replenishment seem to be comparable with blood oxygen consumption rates in the CW. Still, one should note that both blood oxygen consumption rates and oxygen replenishment rates change over time, as tissue cells die and Hb is converted to met-Hb which cannot bind to O2 molecules in its protein structure.
We found statistically significant differences between groups with one-way ANOVA p < 0.05 for all fitted parameters (Tables 3 and 4, column “All groups”). Pairwise comparison between groups did not show statistically significant differences (p < 0.05) between CW and tumor tissues by using the THb or THC of probe 1, between fat and tumor tissues by using R, fmetHb, α′ of probe 2, and between CW and tumor tissues by using the fmetHb of probe 2. All other parameters indicated statistically significant differences with p < 0.05 for pairwise comparisons of Tukey's HSD.
Tables 3 and 4 show the p-values corresponding to the one-way ANOVA test and post-hoc tests for all parameters listed in Table 2. These differences should be reliable for all parameters and tissue types, since all data distributions were considered normal by using the Anderson–Darling test (required for the reliability of the ANOVA test). It is worth noting that the choice of parameters for the most accurate tissue classification depends on the combination of parameters instead of the evaluation of each individual spectrally fitted parameter. With that in mind, such accuracy was evaluated by the CART analysis shown in the next section.
% of classified observations/number of observations | Predicted class | |||||||
---|---|---|---|---|---|---|---|---|
Small SDD probe (probe 1) | Large SDD probe (probe 2) | |||||||
Fat | Colorectal wall (CW) | Tumor | Fat | Colorectal wall (CW) | Tumor | |||
True class | Fat (n = 318) | 96.3 ± 0.9 | 3.7 ± 0.9 | 0.1 ± 0.3 | Fat (n = 348) | 96.3 ± 0.5 | 3.4 ± 0.5 | 0.4 ± 0.3 |
CW (n = 434) | 2.6 ± 0.5 | 86.2 ± 1.4 | 11.2 ± 1.3 | CW (n = 493) | 1.9 ± 0.6 | 92.7 ± 1.1 | 5.4 ± 1.0 | |
Tumor (n = 635) | 0.3 ± 0.2 | 9.9 ± 0.6 | 89.8 ± 0.6 | Tumor (n = 722) | 0.3 ± 0.0 | 5.9 ± 0.5 | 93.8 ± 0.5 |
A lower SNR may lead to a higher decrease in the accuracy for probe 2 measurements than that for probe 1 measurements because the amplitude of the reflected intensity is lower for probe 2. Therefore, to reproduce the results of this study, The SNR should be as high as possible to the current state-of-the-art DRS instruments and investigation should be conducted to confirm whether our results are translatable for in vivo colorectal tissues.
The SNR varies dramatically over the wide wavelength range between 350 nm and 1900 nm. For probe 1, the highest signal of a typical recorded spectrum is 1000 times stronger than the lowest signal, and the lowest signal is typically 10 times above the noise floor. Therefore, the dynamic range of the recorded spectra is 10000:1. For probe 2, the highest signal is 100 times stronger than the lowest signal, and the lowest signal is typically twice above the noise floor for water-rich tissues (such as the CW and tumor), leading to a total dynamic range of 200:1. The given dynamic range and noise of our measurements gave rise to the variations in the fitting parameters reported in Table 2. It is worth noting that the poor SNR in probe 2 occurs only between 1400 nm and 1600 nm of the fitted wavelength range, and that the spectral fitting algorithm may tend to consider fitting for the water concentration based on the wavelength range between 900 nm and 1300 nm for water-rich tissues, as the signal at the water absorption peaks is typically 50–100 times above the noise floor.
Based on our experience on studies in colorectal tissues, we recommend having a bare minimum of 10 times higher reflectance signal compared to the noise (i.e., approximately 13 dB in the power ratio) for analyzing wavelengths below 1400 nm. Further scientific evidence is needed for the calculation of minimum SNR requirements and the impact of the SNR on the performance of the spectral fitting algorithm (SFA). Such evidence requires meticulous calculation that is out of the scope of our study. The calculation of minimum SNR requirements depends on factors including the combination of (1) the spectral shape difference due to the contribution of tissue chromophores at a given fitted wavelength range, (2) the amplitude of the reflectance signal at such a range, and (3) the homogeneity of optical properties over the tissue depth probed with light at each wavelength.
Our SFA will be more accurate when the sharper and more specific chromophore spectral features are at the selected wavelength range. Accuracy is also enhanced when the more homogeneous tissue layers are in terms of optical properties at the probed depth defined by the probe geometry (e.g., source–detector distance) and light wavelength used. If tissue is sufficiently homogeneous and has spectral features that can distinguish the contribution of each chromophore via spectral shape, the SNR helps to improve accuracy by facilitating the identification of chromophore spectral features. Future studies will explore the impact of the SNR on the performance of our SFA.
Fig. 3 and 4 show the two separate branches of a decision tree with parameters leading to the most accurate classification between fat (n = 318), CW (n = 434) and tumor (n = 634) tissues by using probe 1. These parameters were THb, Rvessel, flipid, α′, and bMie. By using the 5-fold cross-validation, we achieved 95.9 ± 0.7% sensitivity, 98.9 ± 0.3% specificity, 90.2 ± 0.4% accuracy, and 95.5 ± 0.3% AUC. Also, it is important to remember that parameters appearing close to the top of the decision trees (Fig. 3–6) are the most important for tissue classification. With this in mind, the parameters appearing at the top two layers of splits for probe 1 (Fig. 3 and 4), i.e., flipid, Rvessel, and bMie can be important parameters for laparoscopic CRC detection when using the 630 μm-SDD probe.
Fig. 3 Classification decision tree of fat, colorectal wall and tumor tissues based on parameter threshold values of probe 1 (630 μm-SDD probe) for flipid < 27.25%. |
Fig. 4 Classification decision tree of fat, colorectal wall and tumor tissues based on parameter threshold values of probe 1 (600 μm-SDD probe) for flipid ≥ 27.25%. |
Fig. 5 Classification decision tree of fat, colorectal wall and tumor tissues based on parameter threshold values of probe 2 (2500 μm-SDD probe) for flipid < 33.12%. |
Fig. 6 Classification decision tree of fat, colorectal wall and tumor tissues based on parameter threshold values of probe 2 (2500 μm-SDD probe) for flipid ≥ 33.12%. |
Similar to probe 1, Fig. 5 and 6 show that the two separate branches of a decision tree with parameters leading to the most accurate classification between fat (n = 348), CW (n = 493) and tumor (n = 722) tissues by using probe 2. These parameters were THb, Rvessel, flipid, fbile, α′, and bMie. By using 5-fold cross-validation, we achieved 96.9 ± 0.8% sensitivity, 98.9 ± 0.2% specificity, 94.0 ± 0.4% accuracy, and 96.7 ± 0.4% AUC. The parameters which appear on the top two layers of splits from probe 2 (flipid, Rvessel, α′, and bMie) were similar to those from probe 1. Since THb does not appear on the two layers of splits for neither probe, THb may not be an important parameter for classification of fat, CW and tumor tissues. Still, flipid, Rvessel, and bMie appear as important parameters for both probes and may be explored in future studies for laparoscopic CRC detection. These findings need to be confirmed by in vivo tissue measurements to overcome the limitations of data collection of ex vivo tissues.
In a practical perspective, our study is the first step to overcome the limitations of prior DRS research on surgical CRC detection. By incorporating DRS into a flexible fiber-optic probe that can be either passed down a laparoscope working channel, or used with robotic surgery instruments, DRS surgical guidance can potentially increase the accuracy of surgical procedures, improve rates of complete resection and thereby decrease colorectal cancer (CRC) recurrence and mortality. If a side-firing fiber-optic probe31 can be directly integrated into the fingertip of a surgeon, open surgery could also be made more accurate.
In a research perspective, our work identified CRC categories based on the thresholds of biomarkers that may be associated with CRC recurrence and/or with patient prognosis. Prediction of treatment outcomes can potentially be achieved by future in vivo studies correlating surgical outcomes with CRC categories based on chromophore concentrations and scattering properties.
It is important to note that our approach combining spectral fitting with machine learning has a different purpose compared with approaches using only machine learning methods to identify colorectal cancer directly from reflectance spectral data. Our spectral fitting provides interpretable parameters with biological relevance while enabling tissue classification and future patient stratification based on parameters that can potentially be associated with other biochemical analysis of laboratory samples. Previous approaches using only machine learning methods used k-nearest neighbors (kNNs), support vector machines (SVMs), artificial neural networks, decision trees, and linear discriminant analysis (LDA) as methods to identify colorectal cancer in real-time without biologically/biochemically interpretable parameters.21 Future studies will include work on complementary approaches to ours including feature selection by excluding uncorrelated variables through ensembles of random forest classifiers (i.e., importance testing) and/or the maximum relevance minimum redundancy (MRMR).32
Our ex vivo measurements also could not control blood oxygenation, which could potentially be modeled by using data such as time after specimen excision, pH, and pCO2, among others in future studies. Still, in a pilot ex vivo observation of the DRS signal in 3 patients, we observed no significant variations in the average Hb and HbO2 of CRC tissues at 7 locations during the first 15 minutes of our measurements (data not shown).8–10 We are aware that, according to Baltussen et al.33fwater may decrease, and THb and StO2 may increase in ex vivo tissues compared to in vivo tissues within 1 hour after resection. Still, StO2 trends are controversial, since Salomatina et al.34 reported decreased StO2 in mouse ear tissues between 5 and 10 minutes after excision (ex vivo) of tissue and after 24 and 72 hours of storage. It is important to note that variations in THb, StO2 and fwater did not affect the results of our study because these parameters were not used to classify tissues.
We did not include non-cancer pathology in our study. Future inclusion of non-cancer pathologies such as inflammatory bowel disease, radiation-induced fibrosis, and scarring following local excision of cancers may change the classification performance of our CART model and categories of CRC to be considered on long-term follow up studies. It is worth noting that the lack of non-cancer pathology does not affect our tissue biochemical/structural parameters. Our analysis is valid and robust, considering that our dataset includes intra- and inter-patient variations (1386 + 1563 spectra of 47 patients) of both superficial and deeper tissue layers.
Also, our spectral fitting assumes homogeneous media to extract the average tissue chromophore concentrations and scattering properties. Inaccuracies may arise if the heterogeneity on the optical properties deviates significantly from the average properties estimated by assuming that tissue is homogeneous. These inaccuracies are only significant if the heterogeneity over tissue layers probed at each wavelength λ changes the spectral shape of Rexperimental(λ) at wavelength ranges pertinent to distinguish the contribution of different chromophores (e.g., heterogeneity at tissue probed between 520 nm and 560 nm when fitting primarily for Hb and HbO2). However, our results suggest that overfitting is not an issue in our study because uncertainties of fitted parameters are much smaller than uncertainties due to tissue heterogeneity.
For homogeneous medium simulating tissue optical properties, the typical coefficient of variation (COV, i.e., the ratio of the standard deviation to the mean) of each fitted parameter is about 1–10% of the true value of each parameter, except for bMie, which has typical standard deviations around 10–30% for tissue optical properties. When comparing COV in homogeneous media with COV values taken from Table 2, we can see that the average COV over all tissue types varies between 18% and 174%. The only parameters with a lower COV are StO2 (COV ranging from 2% and 35% with a mean of 18% over all tissue types) and water (COV ranging from 5% and 98% with a mean of 37% over all tissue types).
Further evidence indicating that fitted parameters may not be overfitted is that trends on lower COV values occur in the same tissue type, even when measured with different probes and using a different Monte Carlo Look-up Table for spectral fitting. We observed lower COV values only for StO2(%) in fat tissues and fwater (%) in tumor tissues, independent of the probe (or source–detector distance; SDD) used. Consistently lower COV values for independent spectral fitting procedures and probes suggest there was no overfitting even when COV values were approximately the minimum expected from the spectral fitting algorithm (SFA). Therefore, the uncertainty in the fitted parameters as evaluated by their COV should not affect our tissue classification.
In addition, StO2(%) and fwater (%) were not included in the list of the most important parameters for tissue classification and thus did not influence such a classification. This non-inclusion suggests that the tissue classification already excluded the contribution of fitted parameters with uncertainty comparable to the minimum expected from the SFA (i.e., parameters with potentially most of their uncertainties coming from the SFA instead of the tissue heterogeneity). Hence, only fitted parameters with uncertainty dictated primarily by tissue heterogeneity were considered as the most important parameters. With that in mind, our results suggest that the uncertainty on the fitted parameters did not influence our tissue classification.
Finally, previous studies have shown that reflectance measurements can accurately estimate optical properties based on the fitted parameters.35,36 A detailed study on the uncertainty on fitted parameters upon variations in reflectance is not within the scope of our study.
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