  The task of a telecloning protocol is to send an arbitrary qubit possessed by
a sender to multiple receivers. Instead of performing Bell measurement at the
sender's node, if one applies unsharp measurement, we show that the shared
state can be recycled for further telecloning protocol. Specifically, in case
of a single sender and two receivers, the maximal attempting number, which is
defined as the maximum number of rounds used by the channel to obtain quantum
advantage in the fidelity, turns out to be three both for optimal and
nonoptimal shared states for telecloning while the maximal number reduces to
two in case of three receivers. Although the original telecloning with quantum
advantage being possible for arbitrary numbers of receivers, we report that the
recycling of resources is not possible in telecloning involving a single sender
and more than three receivers, thereby demonstrating a no-go theorem. We also
connect the maximal achievable fidelities in each round with the bipartite
entanglement content of the reduced state between the sender and one of the
receivers as well as with the monogamy score of entanglement.
