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[CrossRef]
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[CrossRef]

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[CrossRef]

M. S. Gilmore, R. Castaño, T. Mann, R. C. Anderson, E. D. Mjolsness, R. Manduchi, and R. S. Saunders, "Strategies for autonomous rovers at Mars," J. Geophys. Res. 105, 29223-29237 (2000).

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[CrossRef]

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[CrossRef]
[PubMed]

J. Meseth, G. Müller, and R. Klein, "Reflectance field based real-time, high-quality rendering of bidirectional texture functions," Comput. Graphics 28, 105-112 (2004).

[CrossRef]

F. Drago and K. Myszkowski, "Validation proposal for global illumination and rendering techniques," Comput. Graphics 25, 511-518 (2001).

[CrossRef]

G. Macelloni, G. Nesti, P. Pampaloni, S. Sigismondi, D. Tarchi, and S. Lolli, "Experimental validation of surface scattering and emission models," IEEE Trans. Geosci. Remote Sens. 38, 459-469 (2000).

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[CrossRef]

T. Weyrich, H. Pfister, and M. Gross, "Rendering deformable surface reflectance fields," IEEE Trans. Vis. Comput. Graph. 11, 48-58 (2005).

[CrossRef]
[PubMed]

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[CrossRef]

M. Ashikhmin, S. Premoze, and P. Shirley, "A microfacet-based BRDF generator," in Proceedings of ACM SIGGRAPH 2000 (www.siggraph.org), pp. 65-74.

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[CrossRef]

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[CrossRef]
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M. S. Gilmore, R. Castaño, T. Mann, R. C. Anderson, E. D. Mjolsness, R. Manduchi, and R. S. Saunders, "Strategies for autonomous rovers at Mars," J. Geophys. Res. 105, 29223-29237 (2000).

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[CrossRef]

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[CrossRef]

M. Ashikhmin, S. Premoze, and P. Shirley, "A microfacet-based BRDF generator," in Proceedings of ACM SIGGRAPH 2000 (www.siggraph.org), pp. 65-74.

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D. D. Duncan, D. V. Hahn, and M. E. Thomas, "Physics-based polarimetric BRDF models," in Optical Diagnostic Methods for Inorganic Materials III, L.M.Hanssen, ed., Proc. SPIE 5192, 129-140 (2003).

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[CrossRef]

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W. C. Snyder, "Reciprocity of the bidirectional reflectance distribution function (BRDF) in measurements and models of structured surfaces," IEEE Trans. Geosci. Remote Sens. 36, 685-691 (1998).

[CrossRef]

F. Bernardini, I. M. Martin, and H. Rushmeier, "High-quality texture reconstruction from multiple scans," IEEE Trans. Vis. Comput. Graph. 7, 318-332 (2001).

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[CrossRef]

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It is possible to dispense with the quasi-monochromatic conditions by using the cross-spectral density W(x1,x2,nu)=∫Gamma(x1,x2,tau)exp(2pijnutau)dtau rather than the coherence function, thus proceeding in the space-frequency rather than the space-time domain. Under the quasi-monochromatic conditions these two approaches are essentially equivalent.

Some authors use the symbol µ to represent the normalized mutual intensity function. We reserve µ for the analogous correlation function in the space-frequency domain.

The meanings of the terms "high frequency" and "low frequency" in coherence theory are unfortunately essentially opposite their meanings in scattering theory. Use of these terms in this context is therefore avoided.

Derivatives of the delta function are considered in T. B. A. Senior and J. L. Volakis, Approximate Boundary Conditions in Electromagnetics (IEEE Press, 1995).

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