Boson creation operators constructed from linear combinations of q- deformed zero coupled nucleon pair operators acting on the nucleus (A,0), are used to derive pp-RPA equations. The solutions of these equations are the pairing vibrations in (A${\underline
theexactresultforvaluesofGnotveryclosetoGc.Fordeformedbosoncalculationthecrit-icalvalueofpairingstrengthG,forwhichtheenergyofthelowestenergystateapproacheszero,isseentogoupasthedeformationisincreased.Inotherwords,increasingthedefor-mationparametercausesthetransitiontosuperconductingphasetooccuratsuccessivelylowervaluesofG.
In g.(5b)thedeformationparameteristakentobepurelyimaginarywiththecurvesshownforτ=i0.05,i0.1andi0.15.ForagivenvalueofG,animaginarydeformationparam-eterτraisestheexcitationenergyinthebosonaswellasthequasi-bosonapproximation.Itmaybeinterpretedasananti-pairinge ect.AsthebosonapproximationenergieslielowerthantheexactenergyeigenvaluesforthesameGvalue,forasuitablechoiceofτwecanobtainadeformedbosonapproximationcurvehavingagoodoverlapwiththeexactresultsforareasonablylargerangeofGvaluesintheregionawayfromthephasetransitionregion.Deformationinthiscasesimulatesthecorrelationsnotaccountedforinthebosonapproximation.Inarealisticcase,animaginarydeformationmaybeusedasameasureofcorrelationscausedbyaresidualrepulsiveinteractionnotbeingaccountedforinthebosonorquasi-bosonapproximation.
WehaveplottedinFig.(5c)thedeformedbosonapproximationenergiesforτ=i0.104andquasi-bosonenergiesforτ=0.15thedeformationvaluesforwhichagoodagreementwiththeexactcalculationresultsisobtainedinawideregionawayfromthephasetransitionregion.
6Conclusions
Wehaveconstructedq-analoguesofbosonapproximationandquasi-bosonapproxima-tiontounderstandthephysicalmeaningofrealandimaginarydeformationinthecontextofinteractionbetweenzerocoupledpairs.Theformalismfornon-superconductingnucleihasbeenappliedtotheclassicexampleoftheDoublePairingVibrationalstate0+2inthenucleus
R=208Pb.Forarealdeformationvalueofτ=0.405,thecalculationreproducestheob-servedexcitationenergyofthe0+2state,E=4.87MeV,aswellastheratioofcrosssections,σ(0+
2)
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