Schrodinger Cat States for Quantum Information Processing

Schrodinger Cat States for Quantum Information Processing

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1、Schr¨odingerCatStatesforQuantumInformationProcessingH.JeongandT.C.RalphDepartmentofPhysics,UniversityofQueensland,StLucia,Qld4072,Australia(Dated:August3,2011)WeextensivelydiscusshowSchr¨odingercatstates(superpositionsofwell-separatedcoherentstates)inopticalsystemscanbeusedforquantuminformatio

2、nprocessing.I.INTRODUCTIONi.e.,

3、hα

4、?αi

5、2≈0.Weidentifythetwocoherentstatesof±αasbasisstatesforalogicalqubitas

6、αi→

7、0LiIntheearlydaysofquantummechanicsmanyofitsand

8、?αi→

9、1Li,sothataqubitstateisrepresentedbyfoundersbecameveryworriedbysomeoftheparadoxi-calpredictionsthatemergedfromthoughtexperiments

10、

11、φi=A

12、0Li+B

13、1Li=A

14、αi+B

15、?αi.(2)basedonthenewtheory.Now,eightyyearson,someoftheseearlythoughtexperimentsarebeingexperimentallyThebasisstates,

16、αiand

17、?αi,canbeunambiguouslyrealized,andmorethanjustcon?rmingthefundamen-discriminatedbyasimplemeasurementschemewithatalsofthetheorytheyarealsobeingrecogn

18、izedasthe50-50beamsplitter,anauxiliarycoherent?eldofampli-basisof21stcenturytechnologies[14].Anexampleistudeαandtwophotodetectors[22].Atthebeamsplitter,theEPRparadox,proposedbyEinstein,Podolskyandthequbitstate

19、φi1ismixedwiththeauxiliarystate

20、αi2Rosenin1935[15],whichdiscussedthestrangeproper-an

21、dresultsintheoutputtiesofquantumentanglement.Today,entanglementhas√√beenobservedinoptical[1,28]andion[48]systemsand

22、φRiab=A

23、2αia

24、0ib+B

25、0ia

26、?2αib.(3)isrecognizedasaresourceformanyquantuminformationprocessingtasks[36].Thetwophotodetectoraresetformodesaandbre-AboutthesametimeastheEPRdiscussion,sp

27、ectively.IfdetectorAregistersanyphoton(s)whileSchr¨odingerproposedhisfamouscatparadox[52]thatdetectorBdoesnot,weknowthat

28、αiwasmeasured.highlightedtheunusualconsequencesofextendingtheOnthecontrary,ifAdoesnotclickwhileBdoes,theconceptofsuperpositiontomacroscopicallydistinguish-measurementoutcome

29、was

30、?αi.Eventhoughthereableobjects.Fromaquantumopticsviewpoint,theisnon-zeroprobabilityoffailureP(φ)=

31、h00

32、φi

33、2=fRR2usualparadigmistoconsidersuperpositionsofcoher-

34、A+B

35、2e?2αinwhichbothofthedetectorsdonotreg-entstateswithamplitudessu?cien

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