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Plotkin, M. (1993). Tales of a Shaman s Apprentice: An Ethnobotanist Searches for New Medicines in the Amazon Rain Forest. New York: Viking Penguin. Savage, V., L. Kong, et al. (1998). The Naga Awakens: Growth and Change in Southeast Asia. Singapore: Federal Publications. Stipp, D. (2002). China s Biotech is Starting to Bloom. Fortune 146(4): 126 34. Surridge, C. (2002). The Rice Squad. Nature 416(April): 576 8. Tang, C., M. Mahmud, F. Foo, S. Chu, R. Chiu, M. Tanticharoen, L. Zhang, and T. Chang (2003). Realizing potential: the state of Asian bioentre preneurship. Bioentrepreneur. 21 April. http://www.nature.com/ cgitaf/gateway.taf g=6&file=/bioent/building/regional/042003/full/ bioent731.html. Tissue Engineering Pages. www.tissue-engineering.net. Triendl, R. (2000). Japanese support biotech start-ups. Nature 403(January): 124. Triendl, R. and R. Yoon (2001). Singapore From Microprocessor to Mi croarrays Nature Biotechnology 19(June): 521 2. Unesco. www2.unesco.org. Wade, N. (2002). The New York Times Book of Genetics. Gilford, CT: The Lyons Press. Wambugu, F. (1999). Why Africa Needs Agricultural Biotech. Nature 400(July): 15 6. WHO (2002). Genomics and World Health: Report of the Advisory Com mittee on Health Research. Geneva. World Bank Group, The. Inweb18.worldbank.org. World Factbook 2002. Washington, DC: United States Central Intelligence Agency. Yu, Q. and E. David (1999). The Implementation of China s Science and Technology Policy. Westport, CT: Quorum Books.

To establish the upper limit of elemental volume V for the definition of the phase function and the scattering coefficient, we note that if V is too large, then the definition of (7.1.6) will include the radiative transfer theory of (7.1.10) and is actually the bistatic cross section of the overall medium (rather than the elemental test volume V as used) with multiple incoherent scattering included. Thus, the upper limit of elemental volume V is that V needs to be small enough so that multiple scattering of incoherent waves can be excluded. Multiple scattering of incoherent waves will take place in the distance scale of the mean free path lmjp where

(7.1.11)

The volume V can simultaneously satisfy criteria (i) and (iii) if the mean free path is much larger than the wavelength or the wavenumber is much larger than the extinction coefficient.

>.

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To implement an interface in a class, use the Implements keyword For example, if the TimeSheetWin class implements the IMDIChild interface, it would look like this:

(7.1.12) (7.1.13)

The conditions as exhibited in (7.1.12) and (7.1.13) are actually the conditions for transport-type equations to be valid. When the condition is violated so that lmfp '::::' >. (known as the Ioffe-Regel criterion) [Sheng, 1990], strong photon localization may take place and radiative transfer-type equations are inappropriate. For real-life applications, conditions (7.1.12) and (7.1.13) are usually obeyed. However, even though (7.1.12) and (7.1.13) are obeyed, there are still cases when backscattering enhancement (weak photon localization) will take place. Backscattering enhancement is a result of cyclical scattering diagrams and is not included in the radiative transfer equations which only include ladder diagrams. We discuss backscattering enhancement in Volume III. For the case of independent scattering of the N scatterers, (IF(k s , kiW) = N(lfI 2) so that P(k s , ki) = n o (lfI 2 ), where no = N/V is the number of particles per unit volume and (111 2 ) is the averaged single-particle scattering cross section. Thus, (7.1.6) and (7.1.7) reduce to the result of conventional radiative transfer theory. In the following sections we illustrate the applications of these new definitions by using examples of two different types of random distributions of point scatterers.

Consider a distribution of N particles in a volume V (Fig. 7.2.1). Let 1/Jinc be the incident wave. The wave generally will be scattered by all the particles. Each particle will have incidence upon it, the incident wave and the multiply scattered wave from all other particles. How do we write an expression for the field 'lj; that is the final answer after multiple scattering A self-consistent result can be constructed in a manner due to Foldy [1945] and Lax [1952]. Each particle j has a single-particle scattering transition operator Tj . This is the response of the particle when it exists alone. In Volume I we have calculated single-particle scattering properties of scatterers with simple shapes. The operator T j is an exact transition operator for a single particle

/:J ~.~;~i.: .

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