A projected entangled pair state (PEPS) with ancillas can be evolved in imaginary time to obtain thermal states of a strongly correlated quantum system on a two-dimensional lattice. Every application of a Suzuki-Trotter gate multiplies the PEPS bond dimension D by a factor k. It has to be renormalized back to the original D. In order to preserve the accuracy of the Suzuki-Trotter (ST) decomposition, the renormalization in principle has to take into account full environment made of the new tensors with the bond dimension k $\times$ D. Here, we propose a self-consistent renormalization procedure operating with the original bond dimension D, but without compromising the accuracy of the ST decomposition. The iterative procedure renormalizes the...
We propose an efficient algorithm for simulating quantum many-body systems in two spatial dimensions...
We propose a new class of tensor-network states, which we name projected entangled simplex states (P...
We speed up thermal simulations of quantum many-body systems in both one- (1D) and two-dimensional (...
A typical quantum state obeying the area law for entanglement on an infinite two-dimensional (2D) la...
A projected entangled pair state (PEPS) with ancillas is evolved in imaginary time. This tensor netw...
An infinite projected entangled pair state (iPEPS) is a tensor network ansatz to represent a quantum...
The minimally entangled typical thermal states (METTS) are an ensemble of pure states, equivalent to...
We study second-order finite-temperature phase transitions of the two-dimensional quantum Ising and ...
A Gibbs operator $e^{-\beta H}$ for a two-dimensional (2D) lattice system with a Hamiltonian H can b...
The projected entangled pair state (PEPS) ansatz can represent a thermal state in a strongly correla...
We present an algorithm to simulate two-dimensional quantum lattice systems in the thermodynamic lim...
An algorithm for imaginary time evolution of a fermionic projected entangled pair state with ancilla...
The infinite projected entangled pair states (iPEPS) algorithm [J. Jordan et al., Phys. Rev. Lett. 1...
An extension of the projected entangled-pair states (PEPS) algorithm to infinite systems, known as t...
Time evolution of an infinite 2D many body quantum lattice system can be described by the Suzuki-Tro...
We propose an efficient algorithm for simulating quantum many-body systems in two spatial dimensions...
We propose a new class of tensor-network states, which we name projected entangled simplex states (P...
We speed up thermal simulations of quantum many-body systems in both one- (1D) and two-dimensional (...
A typical quantum state obeying the area law for entanglement on an infinite two-dimensional (2D) la...
A projected entangled pair state (PEPS) with ancillas is evolved in imaginary time. This tensor netw...
An infinite projected entangled pair state (iPEPS) is a tensor network ansatz to represent a quantum...
The minimally entangled typical thermal states (METTS) are an ensemble of pure states, equivalent to...
We study second-order finite-temperature phase transitions of the two-dimensional quantum Ising and ...
A Gibbs operator $e^{-\beta H}$ for a two-dimensional (2D) lattice system with a Hamiltonian H can b...
The projected entangled pair state (PEPS) ansatz can represent a thermal state in a strongly correla...
We present an algorithm to simulate two-dimensional quantum lattice systems in the thermodynamic lim...
An algorithm for imaginary time evolution of a fermionic projected entangled pair state with ancilla...
The infinite projected entangled pair states (iPEPS) algorithm [J. Jordan et al., Phys. Rev. Lett. 1...
An extension of the projected entangled-pair states (PEPS) algorithm to infinite systems, known as t...
Time evolution of an infinite 2D many body quantum lattice system can be described by the Suzuki-Tro...
We propose an efficient algorithm for simulating quantum many-body systems in two spatial dimensions...
We propose a new class of tensor-network states, which we name projected entangled simplex states (P...
We speed up thermal simulations of quantum many-body systems in both one- (1D) and two-dimensional (...