“…Whichever method one uses the first step is to make a Hamiltonian mapping onto qubits which usually means choosing a basis to represent the operators in the system. The first step is to represent the Hamiltonian as an N ×N matrix using a discrete quantum mechanics approximation to the quantum mechanical operators which would be infinite dimensional for bosonic observables [13][14][15] [16]. In this paper we will use three different types of discrete Hamiltonians bases described below.…”