and has been studied intensively in the last decade [@bose-review; @bayat-review-book]. Very recently, experimental realization of quantum state transfer through the natural dynamics of many-body systems have been achieved in NMR [@state-transfer-NMR] and coupled optical fibers in linear optics [@kwek-perfect-transfer]. Most of the proposals so far (see [@bose-review; @bayat-review-book] and the references therein), with very few exceptions like [@bayat-densecoding], are based on attaching an extra qubit, which encodes an “unknown" quantum state, to a chain of strongly interacting particles which is usually initialized to its ground state unless for certain engineered XX chains in which local end-chain operations makes it to work for any initialization [@DiFranco-initialization]. This mode of transmission does not seek to harness the intrinsic entanglement of many-body systems and the symmetries of the Hamiltonian seems to be more important [@bayat-xxz]. Moreover, attaching and detaching a single qubit to a many-body system is practically hard and needs a very fine control over the interaction of particles which is missing in many physical systems such as cold atoms. Although at the receiver site taking the quantum state for further process ultimately may need a swap operator or equivalently controlling some local interactions, for encoding the quantum state at the 