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ULTRASHORT LASER PULSE PROPAGATION IN HIGHLY SCATTERING MEDIA A.P. Popov
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What is the task? Pulse structure Output pulse duration τ(t i ) Photon scattering multiplicity Absorption, scattering, transmission Change of medium parameters Effect of stranger particles on skin properties 2
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Modelled setup 3 3 4 21 5 67 8 1 – Cr: forsterite laser, 2 – attenuator, 3 – “blind” mirrors, 4 – beam splitter, 5 –power meter, 6 – vessel with scattering medium, 7 – streak-camera, 8 – CCD-camera 3
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Scattering particle Detector Absorbing particle Detector Incident laser beam Scheme of the modelled experiment 4
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Forward detected photons vs registration time 5
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Behavior of scattered and unscattered parts of radiation at various sample thickness 7
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Forward detected photons vs their scattering multiplicity 8
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Maximum of scattering multiplicity vs medium thickness 10
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Radiation scattering within medium 11
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Forward detected photons vs registration time 12
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Forward detected photons vs registration time 13
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Forward detected photons vs registration time 14
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Determination of optical parameters of skin 1 – incident beam, 2, 3 – integrating spheres, dealing with reflectance and transmission respectively, 4, 5 – photodetectors, 6 – sample 1 2 3 45 6 15
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Skin structure Stratum corneum Epidermis Dermis - 1 Dermis - 2 Dermis Dermis - 3 Subcutaneous fat 16
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Parameters of epidermis with substances Skin typeμ a, mm -1 μ s, mm -1 g Diffuse reflectance R, % Transmission T, % Absorption A, % Skin0.15200.820.475.24.4 Skin + 0.25хFluo 1.00200.814.364.121.6 Skin + 1хTiO 2 0.15300.826.568.74.8 Skin + 2хTiO 2 0.15400.831.263.65.2 Skin + 0.25хFluo + 1хTiO 2 1.00300.818.657.124.3 Skin + 0.25хFluo + 2хTiO 2 1.00400.822.351.726.0 17
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Ratio of radiation components for epidermis with various substances 18
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Layer with TiO 2 Rest of stratum corneum Incident radiation Transmitted radiation Stratum corneum with particles of TiO 2 19
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Absorption in different parts of stratum corneum 20
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Pulses of various durations passed through stratum corneum with scattering substance (TiO 2 ) 21
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Summary Ballistic, snake- and diffusion components registration Scattering multiplicity, time detection of pulse maximum depends linear on μ s, L Decreasing of μ a makes detected pulses longer and increase their amplitude There exists maximum of scattered and absorbed radiation under the medium surface 22
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Summary Multiple scattering makes short pulses longer Scattering substance injection causes absorption and reflectance increase in upper skin layers, transmission decrease 23
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