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Figure 2
Radially integrated intensity as a function of distance from the centre of the direct beam. The error bars of the simulation are smaller than the linewidth. The integral of the simulated counts is directly proportional to the scattered intensity. To observe with a SANS setup the small-angle scattering of particles with a radius of 1 µm, a narrow beam and a high-resolution position-sensitive detector are needed. The maximum wavevector in this graph corresponds to 1.32 × 10−3 Å−1.

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