  A quantum many-body state built on a classical 1D Ising model with locally
entangled qubits is considered. This setup can model an infinite-player quantum
Prisoner's dilemma game with each site representing two entangled players (or
qubits). The local entanglement $\gamma$ between two qubits placed on a site in
the 1D Ising model and classical coupling between adjacent sites of the Ising
model has an apposite influence on qubits. It points to a counter-intuitive
situation wherein local entanglement at a site can exactly cancel global
correlations, signaling an artificial quantum many-body state wherein, by
locally tuning the entanglement at a particular site, one can transition from a
strongly correlated quantum state to an uncorrelated quantum state and then to
a correlated classical state. In other words, we can simulate a state similar
to a Type II superconducting state via local tuning of entanglement in a 1D
Ising chain with entangled qubits.
