Within the standard 3 ν mass–mixing framework, we present an up-to-date global analysis of neutrino oscillation data (as of January 2016), including the latest available results from experiments with atmospheric neutrinos (Super-Kamiokande and IceCube DeepCore), at accelerators (first T2K ν‾ and NOνA ν runs in both appearance and disappearance modes), and at short-baseline reactors (Daya Bay and RENO far/near spectral ratios), as well as a reanalysis of older KamLAND data in the light of the “bump” feature recently observed in reactor spectra. We discuss improved constraints on the five known oscillation parameters ( δm2 , |Δm2| , sin2θ12 , sin2θ13 , sin2θ23 ), and the status of the three remaining unknown parameters: the mass hierarchy [ sign(±Δm2) ], the θ23 octant [ sign(sin2θ23−1/2) ], and the possible CP-violating phase δ . With respect to previous global fits, we find that the reanalysis of KamLAND data induces a slight decrease of both δm2 and sin2θ12 , while the latest accelerator and atmospheric data induce a slight increase of |Δm2| . Concerning the unknown parameters, we confirm the previous intriguing preference for negative values of sinδ (with best-fit values around sinδ≃−0.9 ), but we find no statistically significant indication about the θ23 octant or the mass hierarchy (normal or inverted). Assuming an alternative (so-called LEM) analysis of NOνA data, some δ ranges can be excluded at >3σ , and the normal mass hierarchy appears to be slightly favored at ∼90% C.L. We also describe in detail the covariances of selected pairs of oscillation parameters. Finally, we briefly discuss the implications of the above results on the three non-oscillation observables sensitive to the (unknown) absolute ν mass scale: the sum of ν masses Σ (in cosmology), the effective νe mass mβ (in beta decay), and the effective Majorana mass mββ (in neutrinoless double beta decay).
{ "license": [ { "url": "http://creativecommons.org/licenses/by/3.0/", "license": "CC-BY-3.0" } ], "copyright": [ { "statement": "The Authors" } ], "control_number": "14432", "_oai": { "updated": "2018-04-19T11:26:18Z", "id": "oai:repo.scoap3.org:14432", "sets": [ "NPB" ] }, "authors": [ { "surname": "Capozzi", "given_names": "F.", "raw_name": "Capozzi, F.", "affiliations": [ { "country": "Italy", "value": "Dipartimento di Fisica e Astronomia \u00e2\u0080\u009cGalileo Galilei\u00e2\u0080\u009d, Universit\u00c3 di Padova, Via F. Marzolo 8, Padova, I-35131, Italy" }, { "country": "Italy", "value": "Istituto Nazionale di Fisica Nucleare (INFN), Sezione di Padova, Via F. Marzolo 8, Padova, I-35131, Italy" } ], "full_name": "Capozzi, F.", "orcid": "0000-0001-6135-1531" }, { "raw_name": "Lisi, E.", "affiliations": [ { "country": "Italy", "value": "Istituto Nazionale di Fisica Nucleare (INFN), Sezione di Bari, Via E. Orabona 4, Bari, I-70126, Italy" } ], "surname": "Lisi", "given_names": "E.", "full_name": "Lisi, E." }, { "raw_name": "Marrone, A.", "affiliations": [ { "country": "Italy", "value": "Dipartimento Interateneo di Fisica \u00e2\u0080\u009cMichelangelo Merlin\u00e2\u0080\u009d, Universit\u00c3 di Bari, Via G. Amendola 173, Bari, I-70126, Italy" }, { "country": "Italy", "value": "Istituto Nazionale di Fisica Nucleare (INFN), Sezione di Bari, Via E. Orabona 4, Bari, I-70126, Italy" } ], "surname": "Marrone", "given_names": "A.", "full_name": "Marrone, A." }, { "raw_name": "Montanino, D.", "affiliations": [ { "country": "Italy", "value": "Dipartimento di Matematica e Fisica \u00e2\u0080\u009cEnnio de Giorgi\u00e2\u0080\u009d, Universit\u00c3 del Salento, Via Arnesano, Lecce, I-73100, Italy" }, { "country": "Italy", "value": "Istituto Nazionale di Fisica Nucleare (INFN), Sezione di Lecce, Via Arnesano, Lecce, I-73100, Italy" } ], "surname": "Montanino", "given_names": "D.", "full_name": "Montanino, D." }, { "raw_name": "Palazzo, A.", "affiliations": [ { "country": "Italy", "value": "Dipartimento Interateneo di Fisica \u00e2\u0080\u009cMichelangelo Merlin\u00e2\u0080\u009d, Universit\u00c3 di Bari, Via G. Amendola 173, Bari, I-70126, Italy" }, { "country": "Italy", "value": "Istituto Nazionale di Fisica Nucleare (INFN), Sezione di Bari, Via E. Orabona 4, Bari, I-70126, Italy" } ], "surname": "Palazzo", "given_names": "A.", "full_name": "Palazzo, A." } ], "_files": [ { "checksum": "md5:56fd03adaab90d5d1923abcbcf5edba7", "filetype": "xml", "bucket": "18034b74-3238-4009-be34-a7ed64c92901", "version_id": "0d311bbf-a021-4aa5-9375-123185aa7716", "key": "10.1016/j.nuclphysb.2016.02.016.xml", "size": 214544 }, { "checksum": "md5:2200243ef6295fb19a8c141ecf0eace1", "filetype": "pdf", "bucket": "18034b74-3238-4009-be34-a7ed64c92901", "version_id": "94b75693-754c-4605-bf78-c0cf83e2be29", "key": "10.1016/j.nuclphysb.2016.02.016.pdf", "size": 862191 }, { "checksum": "md5:adf767f733767b8d0f03c47d37af13c2", "filetype": "pdf/a", "bucket": "18034b74-3238-4009-be34-a7ed64c92901", "version_id": "5de6bfce-976e-451b-99ea-6a5e82450f3a", "key": "10.1016/j.nuclphysb.2016.02.016_a.pdf", "size": 1178832 } ], "record_creation_date": "2016-02-22T00:00:00", "titles": [ { "source": "Elsevier", "title": "Neutrino masses and mixings: Status of known and unknown 3 \u03bd parameters" } ], "dois": [ { "value": "10.1016/j.nuclphysb.2016.02.016" } ], "publication_info": [ { "journal_title": "Nuclear Physics B", "material": "article", "year": 2016 } ], "$schema": "http://repo.scoap3.org/schemas/hep.json", "abstracts": [ { "source": "Elsevier", "value": "Within the standard 3 \u03bd mass\u2013mixing framework, we present an up-to-date global analysis of neutrino oscillation data (as of January 2016), including the latest available results from experiments with atmospheric neutrinos (Super-Kamiokande and IceCube DeepCore), at accelerators (first T2K \u03bd\u203e and NO\u03bdA \u03bd runs in both appearance and disappearance modes), and at short-baseline reactors (Daya Bay and RENO far/near spectral ratios), as well as a reanalysis of older KamLAND data in the light of the \u201cbump\u201d feature recently observed in reactor spectra. We discuss improved constraints on the five known oscillation parameters ( \u03b4m2 , |\u0394m2| , sin2\u2061\u03b812 , sin2\u2061\u03b813 , sin2\u2061\u03b823 ), and the status of the three remaining unknown parameters: the mass hierarchy [ sign(\u00b1\u0394m2) ], the \u03b823 octant [ sign(sin2\u2061\u03b823\u22121/2) ], and the possible CP-violating phase \u03b4 . With respect to previous global fits, we find that the reanalysis of KamLAND data induces a slight decrease of both \u03b4m2 and sin2\u2061\u03b812 , while the latest accelerator and atmospheric data induce a slight increase of |\u0394m2| . Concerning the unknown parameters, we confirm the previous intriguing preference for negative values of sin\u2061\u03b4 (with best-fit values around sin\u2061\u03b4\u2243\u22120.9 ), but we find no statistically significant indication about the \u03b823 octant or the mass hierarchy (normal or inverted). Assuming an alternative (so-called LEM) analysis of NO\u03bdA data, some \u03b4 ranges can be excluded at >3\u03c3 , and the normal mass hierarchy appears to be slightly favored at \u223c90% C.L. We also describe in detail the covariances of selected pairs of oscillation parameters. Finally, we briefly discuss the implications of the above results on the three non-oscillation observables sensitive to the (unknown) absolute \u03bd mass scale: the sum of \u03bd masses \u03a3 (in cosmology), the effective \u03bde mass m\u03b2 (in beta decay), and the effective Majorana mass m\u03b2\u03b2 (in neutrinoless double beta decay)." } ], "imprints": [ { "date": "2016-02-23", "publisher": "Elsevier" } ], "acquisition_source": { "date": "2016-02-22T00:00:00", "source": "Elsevier", "method": "scoap3", "submission_number": "f6907c3443c211e898b102163e01809a" } }