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with i being the imaginary unit and θ a real number.
Recall that and as well as.
So in the case we recover the Fermi – Dirac statistics ( minus sign ) and in the case θ = 0 ( or ) the Bose – Einstein statistics ( plus sign ).
In between we have something different.
Frank Wilczek coined the term " anyon " to describe such particles, since they can have any phase when particles are interchanged.

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