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DC Field | Value | Language |
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dc.contributor.author | Thakur, S. | - |
dc.contributor.author | Nanal, V. | - |
dc.contributor.author | Singh, P.P. | - |
dc.contributor.author | Pillay, R.G. | - |
dc.contributor.author | Krishnamoorthy, H. | - |
dc.contributor.author | Mazumdar, A. | - |
dc.contributor.author | Reza, A. | - |
dc.contributor.author | Raina, P.K. | - |
dc.contributor.author | Vatsa, V. | - |
dc.date.accessioned | 2022-07-15T11:26:24Z | - |
dc.date.available | 2022-07-15T11:26:24Z | - |
dc.date.issued | 2022-07-15 | - |
dc.identifier.uri | http://localhost:8080/xmlui/handle/123456789/3636 | - |
dc.description.abstract | The 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.iso | en_US | en_US |
dc.title | Simulation studies for source optimization in 96Zr β decay | en_US |
dc.type | Article | en_US |
Appears in Collections: | Year-2022 |
Files in This Item:
File | Description | Size | Format | |
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Full Text.pdf | 341.22 kB | Adobe PDF | View/Open Request a copy |
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