| Literature DB >> 36226124 |
Biagio Todaro1, Filippo Begarani2,3, Federica Sartori2,3, Stefano Luin1,4.
Abstract
Diabetes has no well-established cure; thus, its management is critical for avoiding severe health complications involving multiple organs. This requires frequent glycaemia monitoring, and the gold standards for this are fingerstick tests. During the last decades, several blood-withdrawal-free platforms have been being studied to replace this test and to improve significantly the quality of life of people with diabetes (PWD). Devices estimating glycaemia level targeting blood or biofluids such as tears, saliva, breath and sweat, are gaining attention; however, most are not reliable, user-friendly and/or cheap. Given the complexity of the topic and the rise of diabetes, a careful analysis is essential to track scientific and industrial progresses in developing diabetes management systems. Here, we summarize the emerging blood glucose level (BGL) measurement methods and report some examples of devices which have been under development in the last decades, discussing the reasons for them not reaching the market or not being really non-invasive and continuous. After discussing more in depth the history of Raman spectroscopy-based researches and devices for BGL measurements, we will examine if this technique could have the potential for the development of a user-friendly, miniaturized, non-invasive and continuous blood glucose-monitoring device, which can operate reliably, without inter-patient variability, over sustained periods.Entities:
Keywords: Raman spectroscopy; blood glucose; diabetes; glycaemia monitoring devices; spectral data processing; wearable continuous non-invasive sensors
Year: 2022 PMID: 36226124 PMCID: PMC9548653 DOI: 10.3389/fchem.2022.994272
Source DB: PubMed Journal: Front Chem ISSN: 2296-2646 Impact factor: 5.545
FIGURE 1Evolution of BGL monitoring devices from invasive glucometer (A), to minimally invasive continuous glucose monitoring patch (B), and finally to non-invasive wristwatch (C). Created with BioRender.com.
FIGURE 2Example of experimental setup for infrared spectroscopy. A continuous IR source generates light over a wide range of infrared wavelengths, which irradiates the sample. The light is collected in transmission or diffuse reflectance mode, and the spectrum is measured thanks to a diffraction grating, in this example. Alternative configurations use a Fourier transform interferometer (FTIR) instead of the dispersive element, or use a monochromator or other methods for selecting the wavelength bands between IR source and sample. Created with BioRender.com.
FIGURE 3Experimental setup for a Raman spectrometer. A laser diode is focused onto the sample and the scattered light is collected by a lens (alternatively, the backscattered light could be collected). The Rayleigh scattered light is then and blocked, while the Raman scattered light can be detected and its spectrum can be analysed. Created with BioRender.com.
FIGURE 4Photoacoustic spectroscopy experimental setup. A thermal expansion of the sample (inside or in contact with the acoustic resonator) is generated by a pulsed laser source (e.g., a quantum cascade -QC- laser). The generated acoustic waves propagate through the acoustic resonator and, after amplification and possibly ADC (analogic-digital converter), is analyzed by a computer. Created with BioRender.com.
FIGURE 5A schematics of a simplified MHC device, where the detection system transforms information about temperature, humidity, blood flow rate and degree of blood oxygen saturation into estimation of glucose level. Created with BioRender.com.
Example of Raman setups.
| Raman excitation source | Beam power (mW) | Spot dimension | Spectral range | Measurement time | Sensitivity, selectivity, accuracy | Spectral data processing | References | |
|---|---|---|---|---|---|---|---|---|
| A | 830 nm diode laser | 300 | 1 mm2 (area; on human skin) | 355–1,545 cm−1 | 2 s integration time (90 times) | MAE: 5.0%, R2: 0.93 | PLS analysis, Savitsky – Golay algorithm, EGA Analysis |
|
| B | 785 nm Ti:sapphire laser | 100 | ∼1.01 mm (diameter; on rabbit retina) | 300–1,500 cm−1 | 3 s integration time (50 times) | RMSECV: 24.0mg/dl, R2: 0.99 | PLS analysis, EGA Analysis |
|
| C | 785 nm diode laser | 15 | ∼0.002 mm (diameter; on mouse skin) | 500–1800 cm−1 | 15 s integration time (25 times) | MAE: 5.7%, R2: 0.91 | PLS analysis |
|
| D | 785 nm diode laser | 400 | ∼ 8 mm (diameter; on human skin) | 541–1818 cm−1 | 10 s integration time (10 times) | R2: 0.83 | PLS analysis, EMSC, EGA Analysis |
|
| E | 830 nm continuous-wave diode laser | 300 | 0.005 mm2 (area; on human skin) | 300–1800 cm−1 | 3 min integration time (1 time) | ISUP: 1.9 MARD: 25.8%, R2: 0.69 | ISUP parameter, 15-point Savitsky-Golay 1st order algorithm, EMSC |
|
| F | 830 nm diode laser (incidence angle of 60°) | 250 | ∼1.6 mm2 (area; on swine ear skin) | 810–1,650 cm−1 | 4.75 min integration time (1 time) | Intrasubject R2: 0.94 Intersubject R2: 0.62 | Savitzky-Golay filtering, polynomial baseline subtraction, MLR analysis |
|
| G | 830 nm diode laser | 50 | 0.5 mm (diameter; on human skin) | 400–1800 cm−1 | 0.1 s integration time (6,000 times) | - | Estimation of power spectral density, Savitzky-Golay filtering |
|
PLS, partial least squares regression; EGA, clarke error grid; EMSC, extended multiplicative scatter correction; ISUP, Inter-subject unified performance; MAE, mean absolute error; MARD, mean absolute relative difference; MLR, multiple linear regression; RMSECV, root-mean-squared-error of cross validation.