  The dynamics of classical hard particles in a quasi one-dimensional channel
were studied since the 1960s and used for explaining processes in chemistry,
physics and biology and in applications. Here we show that in a previously
un-described file made of anomalous, independent, particles (with jumping times
taken from, {\psi}_{\alpha} (t) t^(-1-{\alpha}), 0<{\alpha}<1), particles form
clusters. At steady state, the percentage of particles in clusters is about,
\surd(1-{\alpha}^3), only for anomalous {\alpha}, characterizing the
criticality of a phase transition. The asymptotic mean square displacement per
particle in the file is about, log^2(t). We show numerically that this exciting
phenomenon of a phase transition is very stable, and relate it with the
mysterious phenomenon of rafts in biological membranes, and with regulation of
biological channels.
