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After passing through a spiral phase plate (SPP) with transmission function T([phi]) = exp(il[phi]) which is located just behind the GAF, the generated GSM beam becomes a GSMV beam, whose MCF is
One finds from Figure 3 that the scintillation index of a GSM or GSMV beam decreases with the decrease of [[sigma].sub.g], indicating that a partially coherent beam with low value of [[sigma].sub.g] is less affected by the turbulence as expected.