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037 | _ | _ | |a FZJ-2023-00247 |
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 Pinpointing Sweet Spots for the Kerr-Cat Qubit |
260 | _ | _ | |c 2022 |
336 | 7 | _ | |a Conference Paper |0 33 |2 EndNote |
336 | 7 | _ | |a INPROCEEDINGS |2 BibTeX |
336 | 7 | _ | |a conferenceObject |2 DRIVER |
336 | 7 | _ | |a CONFERENCE_POSTER |2 ORCID |
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336 | 7 | _ | |a Poster |b poster |m poster |0 PUB:(DE-HGF)24 |s 1673265706_7573 |2 PUB:(DE-HGF) |x After Call |
520 | _ | _ | |a Introducing a detuning and a single photon drive to the Kerr-Cat Qubit alters its eigenstates to be not coherent states. However by displacing the original coherent states the eigenstates can be approximated in such a way that only a periodic deformation is present. If the period of the X rotation caused by the detuning is a multiple of the period of the deformation we can recover the original coherent state with high fidelity.If however the deformation is maximal at the time we complete the X rotation the peak of our fidelity is cut off and only low fidelity rotations can be achieved.Thus a careful choice of parameters is required. |
536 | _ | _ | |a 5224 - Quantum Networking (POF4-522) |0 G:(DE-HGF)POF4-5224 |c POF4-522 |f POF IV |x 0 |
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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 |
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