Multi-photon system has been studied by many groups. The challenge facing by most groups is the limited samples are far from enough for detecting quantum entanglement. The problem is even more serious for the quantum state tomography. Adaptive quantum state tomography is one possible way to solve the problem. We develop a distribution scheme of samples and extend it into three step to improve the performance of adaptive quantum state tomography. Mean Square Error of reconstructed density matrix is improved for several states being tested numerically. In addition, Phaselift is applied to save the storage space of measurement operator.
Multi-photon system has been studied by many groups. The challenge facing by most groups is the limited samples are far from enough for detecting quantum entanglement. The problem is even more serious for the quantum state tomography. Adaptive quantum state tomography is one possible way to solve the problem. We develop a distribution scheme of samples and extend it into three step to improve the performance of adaptive quantum state tomography. Mean Square Error of reconstructed density matrix is improved for several states being tested numerically. In addition, Phaselift is applied to save the storage space of measurement operator.
This paper introduces Adaptive Quantum State Tomography (AQST), a novel algorithm for efficiently characterizing complex quantum states. Traditional state tomography methods are computationally demanding, particularly for large and highly entangled states. AQST addresses this challenge by dynamically adjusting the sampling strategy during the tomography process, optimizing the reconstruction process and minimizing computational cost. The core mechanism relies on a superposition-based sampling technique, allowing the algorithm to effectively explore the state space and achieve accurate characterization. The paper details the algorithm's design, the rationale behind its key components, and its performance evaluation on benchmark quantum systems. We demonstrate that AQST offers a significant improvement in computational efficiency compared to existing state tomography methods, particularly for complex systems.
Adaptive measurements have recently been shown to significantly improve the performance of quantum state and process tomography. Adaptive tomography is especially useful in complicated experiments with low outcome generation rate, since it allows one to extract maximal information from a limited amount of data. However, the existing methods either cannot be simply applied to high-dimensional systems or are prohibitively computationally expensive. Here we propose and experimentally implement a tomographic protocol specially designed for the reconstruction of high-dimensional quantum states. The protocol shows qualitative improvement in infidelity scaling with the number of measurements and is fast enough to allow for complete state tomography of states with dimensionality up to 36.
The recently proposed compressed sensing (CS) method sheds light on quantum state tomography of multi-qubit systems with low rank, which greatly reduces the complexity of measurement and computation. However, the restricted isometry property requirement of CS is difficult to be promised or verified in practice, which makes this method probably assign unreasonable results. In regard to this problem, we adopt a two-step procedure and implement an adaptive strategy to update measurement operators based on the measurement results of the first step for CS, which not only serves as a way to verify the estimate but also improves the accuracy of tomography. Our numerical simulations manifest that our adaptive protocol can reduce about half of the infidelity of non-adaptive protocol and is still efficient even when the rank of the state is slightly high, which would greatly benefit multi-qubit state tomography in future experiments .
Recently, tremendous progress has been made in the field of quantum science and technologies: different platforms for quantum simulation as well as quantum computing, ranging from superconducting qubits to neutral atoms, are starting to reach unprecedentedly large systems. In order to benchmark these systems and gain physical insights, the need for efficient tools to characterize quantum states arises. The exponential growth of the Hilbert space with system size renders a full reconstruction of the quantum state prohibitively demanding in terms of the number of necessary measurements. Here we propose and implement an efficient scheme for quantum state tomography using active learning. Based on a few initial measurements, the active learning protocol proposes the next measurement basis, designed to yield the maximum information gain. We apply the active learning quantum state tomography scheme to reconstruct different multi-qubit states with varying degree of entanglement as well as to ground states of the XXZ model in 1D and a kinetically constrained spin chain. In all cases, we obtain a significantly improved reconstruction as compared to a reconstruction based on the exact same number of measurements and measurement configurations, but with randomly chosen basis configurations. Our scheme is highly relevant to gain physical insights in quantum many-body systems as well as for benchmarking and characterizing quantum devices, e.g. for quantum simulation, and paves the way for scalable adaptive protocols to probe, prepare, and manipulate quantum systems.
Quantum state tomography is a technique in quantum information science used to reconstruct the density matrix of an unknown quantum state, providing complete information about the quantum state. It is of significant importance in fields such as quantum computation, quantum communication, and quantum simulation. However, as the size of the quantum system increases, the number of measurement settings and sampling requirements for quantum state tomography grow exponentially with the number of qubits. This not only makes experimental design and implementation more complex, but also exacerbates the consumption of experimental resources. These limitations severely hinder the application of state tomography in large-scale quantum systems. To reduce measurement settings and improve sampling efficiency, this study proposes a state tomography method based on auxiliary systems. This method can be implemented through either entanglement between the quantum system to be measured and a quantum auxiliary system or through correlation between the quantum system and a probabilistic classical auxiliary system. Measurements on the entire joint system enable more efficient extraction of information about the quantum state to be measured. This method relies on standard quantum gate operations and requires only two measurement settings, with a total sampling complexity of O(d2), significantly simplifying experimental operations and measurement processes. Additionally, this study provides two schemes for measuring purity based on the proposed circuit, one of which achieves measurement precision at the Heisenberg limit. This study validates the effectiveness of the proposed method through a detailed theoretical analysis, a series of numerical simulations, and experiments.
An accurate evaluation of the performance of quantum entanglement sources-based on various physical realizations and designed for application in numerous quantum protocols-requires a thorough characterization of the ensemble of the generated output quantum states. This presents a great challenge, as numerous measurements, such as full state tomography, need to be performed on the ensemble. This incentivizes us to reduce the overall duration of the characterization procedure, so that time is saved and the effect of setup drift reduced. For many physical realizations of the quantum states, including polarization and path-encoded qubits, a traveling salesman problem of finding the optimal order of tomographic projections can be found and solved [1]. The achieved tomography speedup, found and experimentally verified [2,3] for up to six-qubit systems, is seen to increase with the size of the quantum system in question, see Fig. 1(a). For three-qubit systems already, the time spent on setting the measurement projections can be halved. A step-by-step workflow [4] is introduced to suit various tomographic scenarios.