Implications of the DLMA solution of θ12 for icecube data using different astrophysical sources

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dc.contributor.author Ghosh, Monojit
dc.contributor.author Goswami, Srubabti
dc.contributor.author Pan, Supriya
dc.contributor.author Pavlovic, Bartol
dc.coverage.spatial United States of America
dc.date.accessioned 2023-07-04T15:31:54Z
dc.date.available 2023-07-04T15:31:54Z
dc.date.issued 2023-06
dc.identifier.citation Ghosh, Monojit; Goswami, Srubabti; Pan, Supriya and Pavlovic, Bartol, "Implications of the DLMA solution of θ12 for icecube data using different astrophysical sources", arXiv, Cornell University Library, DOI: 10.48550/arXiv.2306.11653, Jun. 2023.
dc.identifier.uri https://doi.org/10.48550/arXiv.2306.11653
dc.identifier.uri https://repository.iitgn.ac.in/handle/123456789/8978
dc.description.abstract In this paper, we study the implications of the Dark Large Mixing Angle (DLMA) solutions of θ12 in the context of the IceCube data. We study the consequences in the measurement of the neutrino oscillation parameters namely θ23 and δCP in light of both Large Mixing Angle (LMA) and DLMA solutions of θ12. We find that it will be impossible for IceCube to determine the δCP and the true nature of θ12 i.e., LMA or DLMA at the same time. This is because of the existence of an intrinsic degeneracy at the Hamiltonian level between these parameters. Apart from that, we also identify a new degeneracy between θ23 and two solutions of θ12 for a fixed value of δCP. We perform a chi-square fit using three different astrophysical sources, i.e., μ source, π source, and n source to find that both μ source and π source are allowed within 1σ whereas the n source is excluded at 2σ. It is difficult to make any conclusion regarding the measurement of θ23, δCP for μ source. However, The π (n) source prefers higher (lower) octant of θ23 for both LMA and DLMA solution of θ12. The best-fit value of δCP is around 180∘ (0∘/360∘) for LMA (DLMA) solution of θ12 whereas for DLMA (LMA) solution of θ12, the best-fit value is around 0∘/360∘ (180∘) for π (n) source. If we assume the current best-fit values of θ23 and δCP to be true, then the μ and π source prefer the LMA solution of θ12 whereas the n source prefers the DLMA solution of θ12.
dc.description.statementofresponsibility by Monojit Ghosh, Srubabti Goswami, Supriya Pan and Bartol Pavlovic
dc.language.iso en_US
dc.publisher Cornell University Library
dc.subject DLMA
dc.subject LMA
dc.subject Chi-square fit
dc.subject Hamiltonian level
dc.subject IceCube
dc.title Implications of the DLMA solution of θ12 for icecube data using different astrophysical sources
dc.type Article
dc.relation.journal arXiv


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