arXiv2018
By combining the continuous matrix product state (cMPS) representation for quantum fields in the continuum with standard optimization techniques for matrix product states (MPS) on the lattice, we obtain an approximation $|Ψ\rangle$, directly in the continuum, of the ground state of non-relativistic quantum field theories. This construction works both for translation invariant systems and in the more challenging context of inhomogeneous systems, as we demonstrate for an interacting bosonic field in a periodic potential. Given the continuum Hamiltonian $H$, we consider a sequence of discretized Hamiltonians $\{H(ε_α)\}_{α=1,2,\cdots,p}$ on increasingly finer lattices with lattice spacing $ε_1 > ε_2 > \cdots > ε_p$. We first use energy minimization to optimize an MPS approximation $|Ψ(ε_1)\rangle$ for the ground state of $H(ε_1)$. Given the MPS $|Ψ(ε_α)\rangle$ optimized for the ground state of $H(ε_α)$, we use it to initialize the energy minimization for Hamiltonian $H(ε_{α+1})$, resulting in the optimized MPS $|Ψ(ε_{α+1})\rangle$. By iteration we produce an optimized MPS $|Ψ(ε_{p})\rangle$ for the ground state of $H(ε_p)$, from which we finally extract the cMPS approximation $|Ψ\rangle$ for the ground state of $H$. Two key ingredients of our proposal are: (i) a procedure to discretize $H$ into a lattice model where each site contains a two-dimensional vector space (spanned by vacuum $|0\rangle$ and one boson $|1\rangle$ states), and (ii) a procedure to map MPS representations from a coarser lattice to a finer lattice.