scholarly journals Simulating noisy quantum circuits with matrix product density operators

2021 ◽  
Vol 3 (2) ◽  
Author(s):  
Song Cheng ◽  
Chenfeng Cao ◽  
Chao Zhang ◽  
Yongxiang Liu ◽  
Shi-Yao Hou ◽  
...  
2017 ◽  
Vol 378 ◽  
pp. 100-149 ◽  
Author(s):  
J.I. Cirac ◽  
D. Pérez-García ◽  
N. Schuch ◽  
F. Verstraete

PRX Quantum ◽  
2020 ◽  
Vol 1 (1) ◽  
Author(s):  
Jiří Guth Jarkovský ◽  
András Molnár ◽  
Norbert Schuch ◽  
J. Ignacio Cirac

2018 ◽  
Vol 91 (6) ◽  
Author(s):  
Hai-Lin Huang ◽  
Hong-Guang Cheng ◽  
Xiao Guo ◽  
Duo Zhang ◽  
Yuyin Wu ◽  
...  

2010 ◽  
Vol 2010 ◽  
pp. 1-26 ◽  
Author(s):  
Wiktor Radzki

Recurrence and explicit formulae for contractions (partial traces) of antisymmetric and symmetric products of identical trace class operators are derived. Contractions of product density operators of systems of identical fermions and bosons are proved to be asymptotically equivalent to, respectively, antisymmetric and symmetric products of density operators of a single particle, multiplied by a normalization integer. The asymptotic equivalence relation is defined in terms of the thermodynamic limit of expectation values of observables in the states represented by given density operators. For some weaker relation of asymptotic equivalence, concerning the thermodynamic limit of expectation values of product observables, normalized antisymmetric and symmetric products of density operators of a single particle are shown to be equivalent to tensor products of density operators of a single particle.


2021 ◽  
Vol 10 (2) ◽  
Author(s):  
Markus Hauru ◽  
Maarten Van Damme ◽  
Jutho Haegeman

Several tensor networks are built of isometric tensors, i.e. tensors satisfying W\dagger W = \mathbb{1}W†W=1. Prominent examples include matrix product states (MPS) in canonical form, the multiscale entanglement renormalization ansatz (MERA), and quantum circuits in general, such as those needed in state preparation and quantum variational eigensolvers. We show how gradient-based optimization methods on Riemannian manifolds can be used to optimize tensor networks of isometries to represent e.g. ground states of 1D quantum Hamiltonians. We discuss the geometry of Grassmann and Stiefel manifolds, the Riemannian manifolds of isometric tensors, and review how state-of-the-art optimization methods like nonlinear conjugate gradient and quasi-Newton algorithms can be implemented in this context. We apply these methods in the context of infinite MPS and MERA, and show benchmark results in which they outperform the best previously-known optimization methods, which are tailor-made for those specific variational classes. We also provide open-source implementations of our algorithms.


Quantum ◽  
2020 ◽  
Vol 4 ◽  
pp. 318 ◽  
Author(s):  
Kyungjoo Noh ◽  
Liang Jiang ◽  
Bill Fefferman

Understanding the computational power of noisy intermediate-scale quantum (NISQ) devices is of both fundamental and practical importance to quantum information science. Here, we address the question of whether error-uncorrected noisy quantum computers can provide computational advantage over classical computers. Specifically, we study noisy random circuit sampling in one dimension (or 1D noisy RCS) as a simple model for exploring the effects of noise on the computational power of a noisy quantum device. In particular, we simulate the real-time dynamics of 1D noisy random quantum circuits via matrix product operators (MPOs) and characterize the computational power of the 1D noisy quantum system by using a metric we call MPO entanglement entropy. The latter metric is chosen because it determines the cost of classical MPO simulation. We numerically demonstrate that for the two-qubit gate error rates we considered, there exists a characteristic system size above which adding more qubits does not bring about an exponential growth of the cost of classical MPO simulation of 1D noisy systems. Specifically, we show that above the characteristic system size, there is an optimal circuit depth, independent of the system size, where the MPO entanglement entropy is maximized. Most importantly, the maximum achievable MPO entanglement entropy is bounded by a constant that depends only on the gate error rate, not on the system size. We also provide a heuristic analysis to get the scaling of the maximum achievable MPO entanglement entropy as a function of the gate error rate. The obtained scaling suggests that although the cost of MPO simulation does not increase exponentially in the system size above a certain characteristic system size, it does increase exponentially as the gate error rate decreases, possibly making classical simulation practically not feasible even with state-of-the-art supercomputers.


Quantum ◽  
2019 ◽  
Vol 3 ◽  
pp. 203 ◽  
Author(s):  
Gemma De las Cuevas ◽  
Tom Drescher ◽  
Tim Netzer

The operator Schmidt rank is the minimum number of terms required to express a state as a sum of elementary tensor factors. Here we provide a new proof of the fact that any bipartite mixed state with operator Schmidt rank two is separable, and can be written as a sum of two positive semidefinite matrices per site. Our proof uses results from the theory of free spectrahedra and operator systems, and illustrates the use of a connection between decompositions of quantum states and decompositions of nonnegative matrices. In the multipartite case, we prove that any Hermitian Matrix Product Density Operator (MPDO) of bond dimension two is separable, and can be written as a sum of at most four positive semidefinite matrices per site. This implies that these states can only contain classical correlations, and very few of them, as measured by the entanglement of purification. In contrast, MPDOs of bond dimension three can contain an unbounded amount of classical correlations.


Entropy ◽  
2019 ◽  
Vol 21 (12) ◽  
pp. 1236 ◽  
Author(s):  
James Stokes ◽  
John Terilla

Inspired by the possibility that generative models based on quantum circuits can provide a useful inductive bias for sequence modeling tasks, we propose an efficient training algorithm for a subset of classically simulable quantum circuit models. The gradient-free algorithm, presented as a sequence of exactly solvable effective models, is a modification of the density matrix renormalization group procedure adapted for learning a probability distribution. The conclusion that circuit-based models offer a useful inductive bias for classical datasets is supported by experimental results on the parity learning problem.


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