1 simulation of the experimental data involves backscattering from a histidine group with Cu-N of 1.92

2 small shear rates (0.001 s(-1)) can increase backscattering from blooms of large phytoplankton by mor

3 tors with non-isotropic scattering caused by backscattering from boundaries and line defects.

4 es it possible to distinguish between single backscattering from epithelial-cell nuclei and multiply

5               The new Ca EXAFS clearly shows backscattering from Mn at 3.4 A, a distance that agrees

6 igh nuclear density, and the relatively weak backscattering from nuclei imposes a fundamental limit o

7                                The increased backscattering from the base of the OS is explained by a

8 crobubble contrast agents to increase signal backscattering from the blood.

9 AFS spectrum was successfully interpreted by backscattering from two His residues (Fe-N at 1.99 A), a