| Literature DB >> 32967260 |
Silvia Seoni1, Paola Savoia2, Federica Veronese2, Elisa Zavattaro3, Vanessa Tarantino2, Kristen M Meiburger1.
Abstract
Background and objectives: The possible evolution of actinic keratoses (AKs) into invasive squamous cell carcinomas (SCC) makes their treatment and monitoring essential. AKs are typically monitored before and after treatment only through a visual analysis, lacking a quantitative measure to determine treatment effectiveness. Near-infrared spectroscopy (NIRS) is a non-invasive measure of the relative change of oxy-hemoglobin and deoxy-hemoglobin (O2Hb and HHb) in tissues. The aim of our study is to determine if a time and frequency analysis of the NIRS signals acquired from the skin lesion before and after a topical treatment can highlight quantitative differences between the AK skin lesion area. Materials andEntities:
Keywords: actinic keratosis; field cancerization; near-infrared spectroscopy; signal processing
Mesh:
Substances:
Year: 2020 PMID: 32967260 PMCID: PMC7560046 DOI: 10.3390/medicina56090482
Source DB: PubMed Journal: Medicina (Kaunas) ISSN: 1010-660X Impact factor: 2.430
Figure 1The position of the probes in the actinic keratosis (AK) lesions (A) and healthy skin (B).
Figure 2First row: example of AK before (A) and after the treatment (B), showing the typical AK features with erythema, telangiectasias, and slight hyperkeratotic scales (A), that were both strongly reduced after therapy (B). Second and last row: example of oxy-hemoglobin and deoxy-hemoglobin (O2Hb and HHb) signals acquired on the AK lesion before (C) and after the treatment (D). In panels (C,D), the HHb signals are blue and the O2Hb signals are red. Conc: micro moral (µMol) concentration.
Mathematical description of features.
| Feature Name | Mathematical Description |
|---|---|
| Mean |
|
| Variance |
|
| Median | Middle value of order numbers |
| Maximum | The maximum value of time series |
| Peak-to-Peak Amplitude | Difference between the maximum positive and negative amplitudes |
| Skewness |
|
| Kurtosis |
|
| Hjorth Mobility |
|
| Hjorth Complexity |
|
| Approximate Entropy |
|
| Average Rectified Value (ARV) |
|
| Root mean square RMS |
|
| Energy |
|
| Number of Zero Crossing | Number of times the signal crosses |
| Power VLF | PVLF, the spectral power between 20 and 60 mHz |
| Power LF | PLF, the spectral power between 60 and 140 mHz |
| Spectral Entropy |
|
| Mean Frequency |
|
P is power spectrum; p is normalized power spectrum; is the fraction of pattern of length ; is the criterion of similarity. Power VLF is the very low frequency spectral power (range: 20–60 mHz) and Power LF is the low frequency spectral power (range: 60–140 mHz)
Figure 3The first two canonical variables of the features of the HHb and O2Hb signals as calculated by MANOVA.
All features and their canonical variable coefficients as calculated by MANOVA. For each analyzed epoch, the MANOVA p-value is listed. The bold values are the three highest values
| Features | Coefficients | Coefficients O2Hb before | Coefficients HHb after * | Coefficients |
|---|---|---|---|---|
| Mean | 0.60 |
| 0.86 | 2.61 |
| Variance | 0.01 | 0.14 | −0.06 | 0.31 |
| Maximum Value | 0.14 | 0.28 | −0.01 | −0.29 |
| Median |
| 0.50 |
| −7.02 |
| Peak-to-Peak Amplitude | −0.04 | −0.05 | 0.01 | 0.12 |
| Kurtosis | 0.36 | 0.06 | 0.22 | −0.10 |
| Skewness | 0.39 | −0.06 | 0.79 | −0.64 |
| Spectral Entropy | 0.28 | 1.90 | −0.98 | −0.92 |
| Approximate Entropy | −3.76 | −2.68 | 1.66 |
|
| RMS | −0.54 | 0.92 | −0.93 | 0.44 |
| Average Rectified Value (ARV) | −2.33 |
| 1.36 | −0.88 |
| Hjorth Mobility |
| 0.68 |
|
|
| Hjorth Complexity |
|
|
|
|
| Number of Zero Crossing | −0.21 | −0.06 | 0.18 | −0.12 |
| Energy | 0.00 | 0.00 | 0.00 | 0.00 |
| Power VLF | 0.11 | 0.13 | −0.03 | 0.18 |
| Power LF | −0.35 | 0.61 | 0.13 | −0.03 |
| Mean Frequency | −0.23 | −0.48 | −0.13 | −1.14 |
* denotes a statistically significant difference with the Bonferroni correction.