Biomedical Optics: Principles and Imaging by Lihong V. Wang PDF
By Lihong V. Wang
This entry-level textbook, overlaying the realm of tissue optics, relies at the lecture notes for a graduate direction (Bio-optical Imaging) that has been taught six instances by way of the authors at Texas A&M college. After the basics of photon shipping in organic tissues are validated, a variety of optical imaging strategies 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 elemental physics and engineering of every imaging strategy are emphasised.
A ideas guide is offered for teachers; to procure a replica please e mail the editorial division at email@example.com.Content:
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 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 procedure and Diffusion conception (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 info for Biomedical Optics: Principles and Imaging
Substituting Eq. 4) into Eq. 3), we obtain a. 6) where size parameter x is defined as x = ka. 7) NUMERICAL EXAMPLE OF RAYLEIGH THEORY Substituting Eqs. 2) into Eq. 6), we obtain os oc a6/\4. Eq. 8) The scattering efficiency depends only on x and ηκ\. If nre\ is close to unity, Eq. 9) Note that rcrei can be complex, in which case the imaginary part is responsible for absorption. 3. NUMERICAL EXAMPLE OF RAYLEIGH THEORY The Rayleigh theory can compute scattering cross section os and scattering efficiency Qs.
5. 6. 7. 00 g/cm3 Concentration of spheres in background by weight: C wt = 1 x 10~5 We compute in SI units as follows: 1. 09 x 107 m- 1 . 2. 18. 3. 209. 4. From Eq. 15 x 10~20 m2. 5. From Eq. 83 x 10~5. 6. Compute the number density of scatterers Ns. For a sphere, the mass density is Ps = ms/Vs, where ms denotes the mass and Vs denotes the volume—Vs = (4/3)πα 3 . For the background, the mass density is p^ = my, j V&, where m^ is the total mass of the background and V& is the total volume of the background.
Substituting it into Eq. 43), and then dividing the equation by / ? ( Γ ) Θ ( Θ ) Φ ( Φ ) , we obtain 1 a / 22dR\ 1 3 / . dS\ 1 32Φ f 2 Λ -Ϊ2 \r — ) + -T2 (sinG— 1 + 2 = T + * = 0. 44) Multiplying Eq. 44) by r2 sin2 Θ, we see that the third term on the left-hand side depends only on φ, whereas the other terms are independent of φ. Thus, we let 1 32Φ φ " ^ 2 constant = — m . 47) From condition Φ(0) = Φ(2π), we have m = 0, ± 1 , ±2, part from Eq. 44) is The r0-dependent l a / 27dR\ i a / .