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Bulletin of the American Physical Society

On universal adiabatic quantum computation

Ari Mizel

Published Mar 15, 2016• 0 citations
OpenAlex

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Quantum Computation and Adiabatic Evolution

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The training of neural networks (NNs) is a computationally intensive task requiring significant time and resources. This article presents a novel approach to NN training using adiabatic quantum computing (AQC), a paradigm that leverages the principles of adiabatic evolution to solve optimization problems. We propose a universal AQC method that can be implemented on gate quantum computers, allowing for a broad range of Hamiltonians and thus enabling the training of expressive neural networks. We apply this approach to various neural networks with continuous, discrete, and binary weights. The study results indicate that AQC can very efficiently evaluate the global minimum of the loss function, offering a promising alternative to classical training methods.
Adiabatic quantum computation (AQC) is a universal model for quantum computation which seeks to transform the initial ground state of a quantum system into a final ground state encoding the answer to a computational problem. AQC initial Hamiltonians conventionally have a uniform superposition as ground state. We diverge from this practice by introducing a simple form of heuristics: the ability to start the quantum evolution with a state which is a guess to the solution of the problem. With this goal in mind, we explain the viability of this approach and the needed modifications to the conventional AQC (CAQC) algorithm. By performing a numerical study on hard-to-satisfy 6 and 7 bit random instances of the satisfiability problem (3-SAT), we show how this heuristic approach is possible and we identify that the performance of the particular algorithm proposed is largely determined by the Hamming distance of the chosen initial guess state with respect to the solution. Besides the possibility of introducing educated guesses as initial states, the new strategy allows for the possibility of restarting a failed adiabatic process from the measured excited state as opposed to restarting from the full superposition of states as in CAQC. The outcome of the measurement can be used as a more refined guess state to restart the adiabatic evolution. This concatenated restart process is another heuristic that the CAQC strategy cannot capture.
The adiabatic quantum computation (AQC) has been proved to be equivalent with the standard circuit model. To realize AQC, we have to realize the target Hamiltonian. However, usually the target Hamiltonian contains kkk-local terms where $k\ensuremath{\ge}3$ which is difficult to realize in experiment. It has been proved that a kkk-local Hamiltonian can be reduced to a two-local one. However, the reduction process needs a lot of auxiliary qubits which makes the system very complicated. Here we show that one can reduce a three-local Hamiltonian to a two-local one using only one third of the auxiliary qubits the previous approach needs and, in special cases, only three auxiliary qubits.