Please use this identifier to cite or link to this item: http://dspace.iitrpr.ac.in:8080/xmlui/handle/123456789/3636
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dc.contributor.authorThakur, S.-
dc.contributor.authorNanal, V.-
dc.contributor.authorSingh, P.P.-
dc.contributor.authorPillay, R.G.-
dc.contributor.authorKrishnamoorthy, H.-
dc.contributor.authorMazumdar, A.-
dc.contributor.authorReza, A.-
dc.contributor.authorRaina, P.K.-
dc.contributor.authorVatsa, V.-
dc.date.accessioned2022-07-15T11:26:24Z-
dc.date.available2022-07-15T11:26:24Z-
dc.date.issued2022-07-15-
dc.identifier.urihttp://localhost:8080/xmlui/handle/123456789/3636-
dc.description.abstractThe single β decay of 96Zr to the ground state of 96Nb is spin forbidden and poses a great experimental challenge. The β decay of 96Zr can be studied via coincident detection of de-exciting gamma rays in 96Mo, which is the end product of 96Nb β decay. Simulations are done with four high purity Ge (HPGe) detector setup (∼ 33% relative efficiency each) to optimize the source configuration. The results suggest that ∼ 70 g of 50% enriched 96Zr will yield sensitivity comparable to the reported results.en_US
dc.language.isoen_USen_US
dc.titleSimulation studies for source optimization in 96Zr β decayen_US
dc.typeArticleen_US
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