Download Biomedical Optics: Principles and Imaging by Lihong V. Wang PDF

By Lihong V. Wang

This entry-level textbook, protecting the world 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 collage. After the basics of photon delivery in organic tissues are confirmed, quite a few optical imaging options for organic tissues are coated. The imaging modalities comprise ballistic imaging, quasi-ballistic imaging (optical coherence tomography), diffusion imaging, and ultrasound-aided hybrid imaging. the fundamental physics and engineering of every imaging approach 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 idea and Mie thought for a unmarried Scatterer (pages 17–35):
Chapter three Monte Carlo Modeling of Photon shipping 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 concept (pages 119–134):
Chapter 7 Sensing of Optical homes 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

Example text

19). The left-hand side of Eq. 22) is the total dimensionless step size. Note that photon paths in a clear medium do not change the dimensionless step size because the extinction coefficient is zero. 22) is used to sample the step size in MCML, where the dimensionless step size s_ is initialized to — 1η(ξ). A photon packet may travel multiple substeps of size s, in a multilayered scattering medium before reaching an interaction site. Only when the photon packet has completed — 1η(ξ) in dimensionless step size does an interaction occur.

1. Spherical polar coordinates used for light scattering, where Θ denotes the polar angle and φ denotes the azimuthal angle. where nt, denotes the refractive index of the background medium and λ denotes the wavelength in vacuum. Substituting Eq. 2) into Eq. 1), we obtain /(r, Θ) a l/λ 4 . This strong wavelength dependence explains the blue sky in broad daylight because blue light is scattered much more strongly than red light. 5) — · nb Here, ns is the refractive index of the sphere and nt, is the refractive index of the background.

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. Structure member dead represents the status of the photon packet and is initialized to zero when the photon packet is launched.

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