2020
DOI: 10.48550/arxiv.2004.14256
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Efficient cavity control with SNAP gates

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Cited by 14 publications
(21 citation statements)
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“…Recently it was demonstrated that SNAP can be made first-order path-independent with respect to ancilla qubit decay [65,66]. Furthermore, a linear scaling of the circuit depth T with the state size n can be achieved for this approach [67], while many interesting experimentally achievable states can be prepared with just T ∼ 5. Inspired by this finding, we parametrize our open-loop control circuit as D † (α) SNAP(ϕ) D(α), see Fig.…”
Section: Resultsmentioning
confidence: 99%
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“…Recently it was demonstrated that SNAP can be made first-order path-independent with respect to ancilla qubit decay [65,66]. Furthermore, a linear scaling of the circuit depth T with the state size n can be achieved for this approach [67], while many interesting experimentally achievable states can be prepared with just T ∼ 5. Inspired by this finding, we parametrize our open-loop control circuit as D † (α) SNAP(ϕ) D(α), see Fig.…”
Section: Resultsmentioning
confidence: 99%
“…An automated method for selecting the circuit depth was proposed in Ref. [67], and it can be utilized here to make an educated guess of T .…”
Section: A Preparation Of Oscillator Fock Statesmentioning
confidence: 99%
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“…It should be noted that the general framework that we employed, pulse engineering via QOC, while proven powerful [27] is not the only known approach to achieve universal synthesis of unitary quantum gates defined in the Fock space for these kind of systems. For instance, the use of selective numberdependent arbitrary phase (SNAP) protocol [28,29] or echoed conditional displacement [30] are strong candidates for the universal control of a singlemode system. However, working with large photonnumber states comes with additional complications in terms of decoherence which are still theoretically not entirely understood [31,32].…”
Section: Discussion and Outlookmentioning
confidence: 99%
“…During the learning phase, the agent discovers from scratch novel strategies, in a systematic procedure which at first resembles trial and error but later begins to build on insights acquired earlier. That RL in general and deep RL in particular is a powerful approach in quantum physics has by now been demonstrated in a variety of tasks in different areas: in most works so far, these tasks did not yet require real-time feedback involving decision-making * riccardo.porotti@mpl.mpg.de based on physical measurements, but RL already proved itself to be a versatile tool even in those settings [15][16][17][18][19][20][21][22][23][24][25][26]. These publications are part of a larger drive towards the use of machine learning tools for quantum experiments (e.g.…”
Section: Introductionmentioning
confidence: 99%