001     916980
005     20230123101915.0
037 _ _ |a FZJ-2023-00246
041 _ _ |a English
100 1 _ |a Schlabes, Arne
|0 P:(DE-Juel1)191416
|b 0
|e Corresponding author
|u fzj
111 2 _ |a APS March Meeting
|c online
|d 2022-03-14 - 2022-03-18
|w USA
245 _ _ |a Achieving fast, high fidelity single qubit gates for the Kerr-Cat Qubit
260 _ _ |c 2022
336 7 _ |a Conference Paper
|0 33
|2 EndNote
336 7 _ |a Other
|2 DataCite
336 7 _ |a INPROCEEDINGS
|2 BibTeX
336 7 _ |a conferenceObject
|2 DRIVER
336 7 _ |a LECTURE_SPEECH
|2 ORCID
336 7 _ |a Conference Presentation
|b conf
|m conf
|0 PUB:(DE-HGF)6
|s 1673265897_20054
|2 PUB:(DE-HGF)
|x After Call
520 _ _ |a The Kerr-Cat Qubit is a biased noise qubit realised by coherent states in an oscillator. We investigated the effect of a detuning and a single photon drive on this qubit. Both of which cause the coherent states │±α〉 defined by the two photon drive and Kerr nonlinearity to be no longer eigenstates of our Hamiltonian. For a small detuning and single photon drive strength the difference to the eigenstates is small enough so that these states are a good approximation of the eigenstates. However this limits us to the regime in which X and Z rotations which are realised by a detuning and a single photon drive respectively are slow. Increasing these terms will speed up the gates but will result in considerably lower fidelities as the coherent states are deformed over time. Using coherent states that are better approximations of eigenstates than │±α〉 can result in fast, high fidelity gates. These displaced states have a semi periodic deformation in them, which needs to be considered carefully and gives rise to a discrete set of detunings and Kerr nonlinearities that produce high fidelity rotations.
536 _ _ |a 5224 - Quantum Networking (POF4-522)
|0 G:(DE-HGF)POF4-5224
|c POF4-522
|f POF IV
|x 0
909 C O |o oai:juser.fz-juelich.de:916980
|p VDB
910 1 _ |a Forschungszentrum Jülich
|0 I:(DE-588b)5008462-8
|k FZJ
|b 0
|6 P:(DE-Juel1)191416
913 1 _ |a DE-HGF
|b Key Technologies
|l Natural, Artificial and Cognitive Information Processing
|1 G:(DE-HGF)POF4-520
|0 G:(DE-HGF)POF4-522
|3 G:(DE-HGF)POF4
|2 G:(DE-HGF)POF4-500
|4 G:(DE-HGF)POF
|v Quantum Computing
|9 G:(DE-HGF)POF4-5224
|x 0
914 1 _ |y 2022
920 _ _ |l yes
920 1 _ |0 I:(DE-Juel1)PGI-2-20110106
|k PGI-2
|l Theoretische Nanoelektronik
|x 0
980 _ _ |a conf
980 _ _ |a VDB
980 _ _ |a I:(DE-Juel1)PGI-2-20110106
980 _ _ |a UNRESTRICTED


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