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We should also take into account the difference in transverse electron beam distributions, but we will not discuss these effects which should be formulated within the framework of a three dimensional analysis.
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We should also take into account the difference in transverse electron beam distributions, but we will not discuss these effects which should be formulated within the framework of a three dimensional analysis.
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We remind that the energy spread induces an increase in the saturation length proportional to f (μ̃ ε) 1+0.185 μ ε2, here the inhomogeneous broadenig effects due to the emittance are not included because negligible if we consider normalized emittances in the range of 1 mm mrad.
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