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Principle of the photo-acoustic microscopy. 

Principle of the photo-acoustic microscopy. 

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The manuscript concerns the optical design and the development of a non-invasive new imaging system for the early diagnosis of skin pathologies. Indeed, an early diagnosis can make the difference between malignant and benign skin lesion in order to minimize unnecessary surgical procedure.Furthermore, prognosis for the year 2015 was that more than t...

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... recently, a new medical imaging technique appeared, the photo-acoustic tomog- raphy (PAT) or photo-acoustic microscopy (PAM) for high resolution [14]. PAT/PAM is related to the photo-acoustic physical effect [15]. This effect occurs inside the sample by a thermoelastic expansion due to the absorption of a electromagnetic field (optical, radio-frequency or micro waves) and therefore, a temperature rise, typically in the millikelvin range. During the thermal relaxation process, pressure is induced leading to the generation of a mechanical wave -i.e., a high frequency acoustic wave. The time delay of the detected ultrasonic wave yields a depth information of the object position. Two or three dimensional surface scans offer a two or three dimensional lateral information about the photo-acoustic source and thus, a tomographic image [16]. Figure 9 shows the scheme of the photo-acoustic microscopy principle. The spatial resolution of PAT is related to the emitting photo-acoustic signal -i.e., higher is the frequency, better is the spatial resolution of the imaging system. For example, a high-frequency photo-acoustic signal with 50 MHz central frequency, results approx- imately in a 40 µm resolution with 3 mm imaging depth -i.e., as for high frequency ultrasound technique - [17]. PAM provides better resolution than PAT because of the focused electromagnetic wave into a small size volume through a microscope ...
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... in the plane s=0 The measurement procedure starts with the recording of through-focus slices according to the method described in the previous section. In addition, in order to retrieve low- frequency wavefront information, five derived intensity planes exponentially-spaced along the optical axis are kept [198,199]. Then, the IPR algorithm is applied and pro- cessed as in Fig. 3.9. The NA of the microlens to be tested is limited by the one of the microscope objective, as well as the sampling of the imaging system. The latter depends onto the detector pixel size ∆x, the wavelength λ, the magnification of the imaging sys-tem γ and the Nyquist sampling Q [200]. It is given by the ...

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