Biomedical Optics: Principles and Imaging by Lihong V. Wang

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By Lihong V. Wang

This entry-level textbook, masking the realm of tissue optics, relies at the lecture notes for a graduate direction (Bio-optical Imaging) that has been taught six instances through the authors at Texas A&M college. After the basics of photon shipping in organic tissues are proven, a number of optical imaging options for organic tissues are coated. The imaging modalities contain ballistic imaging, quasi-ballistic imaging (optical coherence tomography), diffusion imaging, and ultrasound-aided hybrid imaging. the fundamental physics and engineering of every imaging process are emphasised.

A strategies guide is obtainable for teachers; to procure a replica please e-mail the editorial division at
Chapter 1 advent (pages 1–15):
Chapter 2 Rayleigh conception and Mie thought for a unmarried Scatterer (pages 17–35):
Chapter three Monte Carlo Modeling of Photon delivery in organic Tissue (pages 37–65):
Chapter four Convolution for Broadbeam Responses (pages 67–82):
Chapter five Radiative move Equation and Diffusion concept (pages 83–118):
Chapter 6 Hybrid version of Monte Carlo approach and Diffusion idea (pages 119–134):
Chapter 7 Sensing of Optical houses and Spectroscopy (pages 135–151):
Chapter eight Ballistic Imaging and Microscopy (pages 153–179):
Chapter nine Optical Coherence Tomography (pages 181–218):
Chapter 10 Mueller Optical Coherence Tomography (pages 219–247):
Chapter eleven Diffuse Optical Tomography (pages 249–281):
Chapter 12 Photoacoustic Tomography (pages 283–321):
Chapter thirteen Ultrasound?Modulated Optical Tomography (pages 323–341):

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Additional resources for Biomedical Optics: Principles and Imaging

Sample text

Boundary Crossing of a Photon Packet During a step of dimensionless size s_, the photon packet may hit a boundary of the current layer. Several steps are involved in boundary crossing. Step 1. 32) where zo and z \ are the z coordinates of the upper and lower boundaries of the current layer. If μζ approaches zero, the distance approaches infinity, which is represented by constant DBL-MAX in C. Step 2. The dimensionless step size s_ and the distance db are compared as follows: db[Lt < * - , (3-33) where μ, is the extinction coefficient of the current layer.

The corresponding PDF is given by dP{s st) = exp I --Y^VtiSi 2 ^ VtiSi \1 . 20) Here, the summation is over all the segments that the photon packet has traversed before an interaction occurs; μ π is the extinction coefficient for the ith segment, Si is the length of the ith segment, and st is the total step size: st Σ*· <3·21) Equating Eq.

Double s_; /* dimensionless step size. */ long scatters; /* number of scattering events experienced. */ short layer; /* index of layer where photon packet resides. */ } PhotonStruct; PROPAGATION OF PHOTONS 43 Structure members x, y, and z represent the coordinates of a photon packet, (JC, y, z), respectively. Structure members ux, uy, and uz represent the direction cosines of the propagation direction of the photon packet, {μχ, μ>;, μ^}, respectively. Structure member w represents the weight of the photon packet, W.

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