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Maybe it will be some kind of computer, maybe it will be in quantum simulations or quantum communications.
In this work, we have studied 2D ion crystals in an oblate Paul trap for use in quantum simulations.
With this system, one can trap a modest number of ions in 2D planar structures that are likely to be highly frustrated without needing a Penning trap, providing a controlled way to study the onset of frustration effects in quantum simulations.
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Quantum measurement is a crucial step in quantum simulation.
The purpose of Bristlecone, Google says, it to provide its researchers with a testbed "for research into system error rates and scalability of our qubit technology, as well as applications in quantum simulation, optimization, and machine learning".
Especially the increased isolation of the device discussed in the present work is a key prerequisite for several applications both in quantum simulation and quantum computation setups.
A new perspective in quantum simulation is to mimic fundamental interactions, such as those arising in field theories [16], and in particular, lattice gauge theories [17].
Notably, a common problem in quantum simulation is that the probability of reaching the appropriate ground state depends both on the system size and the qubit decoherence rates.
In particular we describe the use of combined quantum mechanics/molecular mechanics (QM/MM) methods in classical and quantum simulations.
In this sense, quantum simulations appear as the technique that will allow us to calculate the time evolution of interacting fermionic and bosonic theories in an optimized way [2].
In parallel, an alternate approach to quantum simulations has been developed in the last years allowing to observe in the laboratory physical phenomena beyond experimental reach, such as Zitterbewegung [6, 7] or Klein paradox [8 10].
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