{
  "license": [
    {
      "url": "http://creativecommons.org/licenses/by/3.0/", 
      "license": "CC-BY-3.0"
    }
  ], 
  "copyright": [
    {
      "holder": "The Author(s)", 
      "statement": "The Author(s)", 
      "year": "2022"
    }
  ], 
  "control_number": "69498", 
  "_oai": {
    "updated": "2022-06-17T09:33:18Z", 
    "id": "oai:repo.scoap3.org:69498", 
    "sets": [
      "NPB"
    ]
  }, 
  "authors": [
    {
      "affiliations": [
        {
          "country": "India", 
          "value": "Department of Physics, Tezpur University, Assam, India"
        }, 
        {
          "country": "India", 
          "value": "Department of Physics, Indian Institute of Technology, Assam, India"
        }
      ], 
      "surname": "Das", 
      "email": "prtmdas9@gmail.com", 
      "full_name": "Das, Pritam", 
      "given_names": "Pritam"
    }, 
    {
      "surname": "Das", 
      "given_names": "Mrinal Kumar", 
      "affiliations": [
        {
          "country": "India", 
          "value": "Department of Physics, Tezpur University, Assam, India"
        }
      ], 
      "full_name": "Das, Mrinal Kumar", 
      "orcid": "0000-0001-6195-6944", 
      "email": "mkdas@tezu.ernet.in"
    }, 
    {
      "affiliations": [
        {
          "country": "India", 
          "value": "School of Physical Sciences, Indian Association for the Cultivation of Science, Kolkata, India"
        }, 
        {
          "country": "Iran", 
          "value": "School of Physics, Institute for Research in Fundamental Sciences (IPM), Tehran, Iran"
        }
      ], 
      "surname": "Khan", 
      "email": "khanphysics.123@gmail.com", 
      "full_name": "Khan, Najimuddin", 
      "given_names": "Najimuddin"
    }
  ], 
  "_files": [
    {
      "checksum": "md5:97558d05f5650dde380a0bca6788c6f0", 
      "filetype": "xml", 
      "bucket": "2153147b-9a0e-4d15-8fbf-1fd9a345f80a", 
      "version_id": "f68e4304-85bf-4226-9bc7-8348c2a80ac2", 
      "key": "10.1016/j.nuclphysb.2022.115810.xml", 
      "size": 674483
    }, 
    {
      "checksum": "md5:56b611305eacb4c7510d9e2af35f877b", 
      "filetype": "pdf", 
      "bucket": "2153147b-9a0e-4d15-8fbf-1fd9a345f80a", 
      "version_id": "ae72d931-902c-4c54-9254-94b496ddfc4d", 
      "key": "10.1016/j.nuclphysb.2022.115810.pdf", 
      "size": 1130028
    }, 
    {
      "checksum": "md5:b54edde0f5085c731a3b30a2e931b3d8", 
      "filetype": "pdf/a", 
      "bucket": "2153147b-9a0e-4d15-8fbf-1fd9a345f80a", 
      "version_id": "67bdf600-912f-4434-8e49-327ad6062448", 
      "key": "10.1016/j.nuclphysb.2022.115810_a.pdf", 
      "size": 1393107
    }
  ], 
  "record_creation_date": "2022-04-26T15:30:22.626596", 
  "titles": [
    {
      "source": "Elsevier", 
      "title": "Five-zero texture in neutrino-dark matter model within the framework of minimal extended seesaw"
    }
  ], 
  "collections": [
    {
      "primary": "Nuclear Physics B"
    }
  ], 
  "dois": [
    {
      "value": "10.1016/j.nuclphysb.2022.115810"
    }
  ], 
  "publication_info": [
    {
      "journal_volume": "980 C", 
      "journal_title": "Nuclear Physics B", 
      "material": "article", 
      "artid": "115810", 
      "year": 2022
    }
  ], 
  "$schema": "http://repo.scoap3.org/schemas/hep.json", 
  "abstracts": [
    {
      "source": "Elsevier", 
      "value": "We study a model of neutrino and dark matter within the framework of a minimal extended seesaw (MES). This model is based on <math><msub><mrow><mi>A</mi></mrow><mrow><mn>4</mn></mrow></msub></math> flavour symmetry along with the discrete <math><msub><mrow><mi>Z</mi></mrow><mrow><mn>3</mn></mrow></msub><mo>\u00d7</mo><msub><mrow><mi>Z</mi></mrow><mrow><mn>4</mn></mrow></msub></math> symmetry to stabilize the dark matter and construct desired mass matrices for neutrino mass. Five-zero textures are imposed in the final <math><mn>4</mn><mo>\u00d7</mo><mn>4</mn></math> active-sterile mass matrix, which significantly reduces the free parameter in the model. Three right-handed neutrinos were considered, two of them have degenerate masses which help us to achieve baryogenesis via resonant leptogenesis. A singlet fermion (sterile neutrino) with mass <math><mo>\u223c</mo><mi>O</mi></math>(eV) is also considered, and we are able to put bounds on active-sterile mixing parameters via neutrino oscillation data. Resonant enhancement of lepton asymmetry is studied at the TeV scale, where we discuss a few aspects of baryogenesis considering the flavour effects. The possibility of improvement in effective mass from <math><mn>0</mn><mi>\u03bd</mi><mi>\u03b2</mi><mi>\u03b2</mi></math> in the presence of a single generation of sterile neutrino flavour is also studied within the fermion sector. In the scalar sector, the imaginary component of the complex singlet scalar (\u03c7) is behaving as a potential dark matter candidate and simultaneously the real part of the complex scalar is associated with the fermion sector for sterile mass generation."
    }
  ], 
  "imprints": [
    {
      "date": "2022-06-17", 
      "publisher": "Elsevier"
    }
  ], 
  "acquisition_source": {
    "date": "2022-06-17T09:32:10.111792", 
    "source": "Elsevier", 
    "method": "Elsevier", 
    "submission_number": "0f11e08eee2011eca1a1661ec451a4e4"
  }
}