000916981 001__ 916981
000916981 005__ 20230123101915.0
000916981 037__ $$aFZJ-2023-00247
000916981 1001_ $$0P:(DE-Juel1)191416$$aSchlabes, Arne$$b0$$eCorresponding author$$ufzj
000916981 1112_ $$aAPS March Meeting$$conline$$d2022-03-14 - 2022-03-18$$wusa
000916981 245__ $$aPinpointing Sweet Spots for the Kerr-Cat Qubit
000916981 260__ $$c2022
000916981 3367_ $$033$$2EndNote$$aConference Paper
000916981 3367_ $$2BibTeX$$aINPROCEEDINGS
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000916981 3367_ $$0PUB:(DE-HGF)24$$2PUB:(DE-HGF)$$aPoster$$bposter$$mposter$$s1673265706_7573$$xAfter Call
000916981 520__ $$aIntroducing a detuning and a single photon drive to the Kerr-Cat Qubit alters its eigenstates to be not coherent states. However by displacing the original coherent states the eigenstates can be approximated in such a way that only a periodic deformation is present. If the period of the X rotation caused by the detuning is a multiple of the period of the deformation we can recover the original coherent state with high fidelity.If however the deformation is maximal at the time we complete the X rotation the peak of our fidelity is cut off and only low fidelity rotations can be achieved.Thus a careful choice of parameters is required.
000916981 536__ $$0G:(DE-HGF)POF4-5224$$a5224 - Quantum Networking (POF4-522)$$cPOF4-522$$fPOF IV$$x0
000916981 909CO $$ooai:juser.fz-juelich.de:916981$$pVDB
000916981 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)191416$$aForschungszentrum Jülich$$b0$$kFZJ
000916981 9131_ $$0G:(DE-HGF)POF4-522$$1G:(DE-HGF)POF4-520$$2G:(DE-HGF)POF4-500$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$9G:(DE-HGF)POF4-5224$$aDE-HGF$$bKey Technologies$$lNatural, Artificial and Cognitive Information Processing$$vQuantum Computing$$x0
000916981 9141_ $$y2022
000916981 920__ $$lyes
000916981 9201_ $$0I:(DE-Juel1)PGI-2-20110106$$kPGI-2$$lTheoretische Nanoelektronik$$x0
000916981 980__ $$aposter
000916981 980__ $$aVDB
000916981 980__ $$aI:(DE-Juel1)PGI-2-20110106
000916981 980__ $$aUNRESTRICTED