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

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Presentation on theme: "Numerical Simulations of Laser-Tissue Interactions Shannon M. Mandel Sophomore Intense Laser Physics Theory Unit Illinois State University Supervisor."— Presentation transcript:

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

3 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

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

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

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

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

8 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

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

10 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

11 Exact numerical simulation of Maxwell’s Equations Initial pulse satisfies :   E = 0 and   B = 0 Time evolution given by :  E ⁄  t = 1/n 2   B and  B ⁄  t = –   E First tests : Snell’s law and Fresnel coefficients

12 n1n1 Snell’s law for beams n2n2   n 1 sin    n 2 sin   Incident Reflected Refracted

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

14 Light bouncing off a random scatterers

15 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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