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Numerical Simulations of Laser-Tissue Interactions

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Presentation on theme: "Numerical Simulations of Laser-Tissue Interactions"— Presentation transcript:

1 Numerical Simulations of Laser-Tissue Interactions
Shannon M. Mandel Sophomore Intense Laser Physics Theory Unit Illinois State University Supervisor : Dr. H. Wanare

2 Examples of diffusive random media
Biological Tissue Diagnostics of cancerous tissue Radiation therapy Water and Air Atmospheric studies and oceanography Communications Remote sensing Pollution studies Earth Geological studies Propagation of pressure waves Electromagnetic & acoustic probing

3 Our Interest How does light interact with a diffusive random medium like a tissue? Tumors are hidden inside the tissue tumor

4 Properties of Random media
Index of refraction n(r) characterizes any medium Homogeneous media Inhomogeneous media Continuous n(r) Discontinuous n(r)

5 Both phenomena lead to attenuation in tissues
High Scattering versus High Absorption Both phenomena lead to attenuation in tissues

6 Why not simple X-Ray? It can damage the cells
It only creates a shadowgram CAT scan, PET are again invasive X-ray screen X-ray source

7 Existing non-invasive techniques
Magnetic resonance imaging Bulky and Expensive Photodynamic therapy Requires tumor seeking photosensitive dyes Ultrasound methods Cannot detect tumors of size < 1 cm Problem: Resolution Solution: Infrared light

8 Infrared radiation Advantages But problems in theoretical modeling ...
Noninvasive laser-tissue interaction High resolution Propagates very far in tissue Rugged and cheap sources available Reliable detectors But problems in theoretical modeling ...

9 Disadvantages of the Diffusion Approximation
No coherent effects like interference No polarization Inaccurate at low penetration depth Near-field effects are neglected need a more complete theory

10 Exact numerical simulation of Maxwell’s Equations
Initial pulse satisfies :   E = and   B = 0 Time evolution given by : E ⁄t = 1/n2   B and B ⁄t = –  E First tests : Snell’s law and Fresnel coefficients

11 Snell’s law for beams n1 n2 n1 sin a1 = n2 sin a2 a1 a2 Reflected
Incident a2 Refracted n1 sin a1 = n2 sin a2

12 Light bouncing off air-glass interface
Time-resolved treatment

13 Light bouncing off a random scatterers
Time-resolved treatment

14 Summary and Outlook Exact solution of the Maxwell’s equations
Model a tissue as a collection of spheroids of random refractive indices Systematically test the conventional diffusion approximation Understand near-field effects


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