000916696 001__ 916696
000916696 005__ 20230123101906.0
000916696 037__ $$aFZJ-2023-00036
000916696 1001_ $$0P:(DE-Juel1)190717$$aJiang, Zhongyi$$b0$$eCorresponding author$$ufzj
000916696 1112_ $$aJUQCA Day$$cJülich$$d2022-11-22 - 2022-11-22$$wGermany
000916696 245__ $$aSWAP Gate from Frequency Modulation
000916696 260__ $$c2022
000916696 3367_ $$033$$2EndNote$$aConference Paper
000916696 3367_ $$2DataCite$$aOther
000916696 3367_ $$2BibTeX$$aINPROCEEDINGS
000916696 3367_ $$2DRIVER$$aconferenceObject
000916696 3367_ $$2ORCID$$aLECTURE_SPEECH
000916696 3367_ $$0PUB:(DE-HGF)6$$2PUB:(DE-HGF)$$aConference Presentation$$bconf$$mconf$$s1672816545_10869$$xInvited
000916696 520__ $$aRealizing high fidelity entanglement gates is a major task for near-term quantum hardware. Withhigher fidelity gates achieved in experiments, more accurate theoretical methods are needed. Here,using non-perturbative formalism, we theoretically study an iSWAP gate activated by frequencymodulation in a transmon-transmon pair. We make a comprehensive analysis to directly solving thetime-dependency and introduce a continuous set of Fermionic Simulation gates by tuning qubit-qubitdetuning and pulse phase. Our analysis can serve as an example for studying gates beyond perturbativeregime and RWA
000916696 536__ $$0G:(DE-HGF)POF4-5224$$a5224 - Quantum Networking (POF4-522)$$cPOF4-522$$fPOF IV$$x0
000916696 7001_ $$0P:(DE-Juel1)171686$$aAnsari, Mohammad H.$$b1$$ufzj
000916696 909CO $$ooai:juser.fz-juelich.de:916696$$pVDB
000916696 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)190717$$aForschungszentrum Jülich$$b0$$kFZJ
000916696 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)171686$$aForschungszentrum Jülich$$b1$$kFZJ
000916696 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$$x0
000916696 9141_ $$y2022
000916696 920__ $$lyes
000916696 9201_ $$0I:(DE-Juel1)PGI-2-20110106$$kPGI-2$$lTheoretische Nanoelektronik$$x0
000916696 980__ $$aconf
000916696 980__ $$aVDB
000916696 980__ $$aI:(DE-Juel1)PGI-2-20110106
000916696 980__ $$aUNRESTRICTED