{
  "_oai": {
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  "authors": [
    {
      "raw_name": "Pallavi Gupta", 
      "affiliations": [
        {
          "country": "India", 
          "value": "School of Physics and Materials Science, Thapar Institute of Engineering and Technology, Patiala 147004, Punjab, India"
        }
      ], 
      "surname": "Gupta", 
      "given_names": "Pallavi", 
      "full_name": "Gupta, Pallavi"
    }, 
    {
      "raw_name": "A. Upadhyay", 
      "affiliations": [
        {
          "country": "India", 
          "value": "School of Physics and Materials Science, Thapar Institute of Engineering and Technology, Patiala 147004, Punjab, India"
        }
      ], 
      "surname": "Upadhyay", 
      "given_names": "A.", 
      "full_name": "Upadhyay, A."
    }
  ], 
  "titles": [
    {
      "source": "APS", 
      "title": "Placing the newly observed state <math><mrow><msub><mrow><mi>B</mi></mrow><mrow><mi>J</mi></mrow></msub><mo>(</mo><mn>5840</mn><mo>)</mo></mrow></math> in bottom spectra along with states <math><mrow><msub><mrow><mi>B</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>(</mo><mn>5721</mn><mo>)</mo></mrow></math>, <math><msubsup><mi>B</mi><mn>2</mn><mo>*</mo></msubsup><mo>(</mo><mn>5747</mn><mo>)</mo></math>, <math><msub><mi>B</mi><mrow><mi>s</mi><mn>1</mn></mrow></msub><mo>(</mo><mn>5830</mn><mo>)</mo></math>, <math><msubsup><mi>B</mi><mrow><mn>2</mn><mi>s</mi></mrow><mo>*</mo></msubsup><mo>(</mo><mn>5840</mn><mo>)</mo></math>, and <math><msub><mi>B</mi><mi>J</mi></msub><mo>(</mo><mn>5970</mn><mo>)</mo></math>"
    }
  ], 
  "dois": [
    {
      "value": "10.1103/PhysRevD.99.094043"
    }
  ], 
  "publication_info": [
    {
      "journal_volume": "99", 
      "journal_title": "Physical Review D", 
      "material": "article", 
      "journal_issue": "9", 
      "year": 2019
    }
  ], 
  "$schema": "http://repo.scoap3.org/schemas/hep.json", 
  "acquisition_source": {
    "date": "2021-08-25T10:37:19.118669", 
    "source": "APS", 
    "method": "APS", 
    "submission_number": "810b323c058f11ecb53772fd3742099d"
  }, 
  "page_nr": [
    11
  ], 
  "license": [
    {
      "url": "https://creativecommons.org/licenses/by/4.0/", 
      "license": "CC-BY-4.0"
    }
  ], 
  "copyright": [
    {
      "statement": "Published by the American Physical Society", 
      "year": "2019"
    }
  ], 
  "control_number": "47635", 
  "record_creation_date": "2019-05-31T16:30:06.421854", 
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  "collections": [
    {
      "primary": "HEP"
    }, 
    {
      "primary": "Citeable"
    }, 
    {
      "primary": "Published"
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  ], 
  "arxiv_eprints": [
    {
      "categories": [
        "hep-ph"
      ], 
      "value": "1803.03136"
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  ], 
  "abstracts": [
    {
      "source": "APS", 
      "value": "We apply the formalism of P. Colangelo et al. [Phys. Rev. D 86, 054024 (2012)] to discuss the quantum number assignments for the recently observed <math><msub><mi>B</mi><mi>J</mi></msub><mo>(</mo><mn>5840</mn><mo>)</mo></math> state by R. Aaij et al. (LHCb Collaboration) [J. High Energy Phys. 04 (2015) 024], and we classify the six possible <math><msup><mi>J</mi><mi>P</mi></msup></math>\u2019s for this state on the basis of the theoretically available masses. By analyzing the strong decay widths and the branching ratios for all six of these cases of <math><msub><mi>B</mi><mi>J</mi></msub><mo>(</mo><mn>5840</mn><mo>)</mo></math>, we justify one of them to be the most favorable assignment. We also examine the recently observed bottom state <math><msub><mi>B</mi><mi>J</mi></msub><mo>(</mo><mn>5970</mn><mo>)</mo></math> as <math><mn>2</mn><mi>S</mi><msup><mn>1</mn><mo>\u2212</mo></msup></math> and states <math><msub><mi>B</mi><mi>J</mi></msub><mo>(</mo><mn>5721</mn><mo>)</mo></math> and <math><msubsup><mi>B</mi><mn>2</mn><mo>*</mo></msubsup><mo>(</mo><mn>5747</mn><mo>)</mo></math> with their strange partners <math><msub><mi>B</mi><mrow><mi>s</mi><mn>1</mn></mrow></msub><mo>(</mo><mn>5830</mn><mo>)</mo></math> and <math><msubsup><mi>B</mi><mrow><mn>2</mn><mi>s</mi></mrow><mo>*</mo></msubsup><mo>(</mo><mn>5840</mn><mo>)</mo></math> for their <math><msup><mi>J</mi><mi>P</mi></msup></math>\u2019s as <math><mrow><mn>1</mn><msub><mrow><mi>P</mi></mrow><mrow><mn>3</mn><mo>/</mo><mn>2</mn></mrow></msub><msup><mrow><mn>1</mn></mrow><mrow><mo>+</mo></mrow></msup></mrow></math> and <math><mn>1</mn><msub><mi>P</mi><mrow><mn>3</mn><mo>/</mo><mn>2</mn></mrow></msub><msup><mn>2</mn><mo>+</mo></msup></math>, respectively. The predicted coupling constants <math><msub><mi>g</mi><mrow><mi>X</mi><mi>H</mi></mrow></msub></math>, <math><msub><mover><mi>g</mi><mo>\u02dc</mo></mover><mrow><mi>H</mi><mi>H</mi></mrow></msub></math>, and <math><msub><mi>g</mi><mrow><mi>T</mi><mi>H</mi></mrow></msub></math> help in redeeming the strong decay width of experimentally missing bottom states <math><mrow><mi>B</mi><mo>(</mo><mn>2</mn><msub><mrow><mmultiscripts><mrow><mi>S</mi></mrow><mprescripts></mprescripts><none></none><mrow><mn>1</mn></mrow></mmultiscripts></mrow><mrow><mn>0</mn></mrow></msub><mo>)</mo></mrow></math>, <math><mrow><msub><mrow><mi>B</mi></mrow><mrow><mi>s</mi></mrow></msub><mo>(</mo><mn>2</mn><msub><mrow><mmultiscripts><mrow><mi>S</mi></mrow><mprescripts></mprescripts><none></none><mrow><mn>3</mn></mrow></mmultiscripts></mrow><mrow><mn>1</mn></mrow></msub><mo>)</mo></mrow></math>, <math><mrow><msub><mrow><mi>B</mi></mrow><mrow><mi>s</mi></mrow></msub><mo>(</mo><mn>2</mn><msub><mrow><mmultiscripts><mrow><mi>S</mi></mrow><mprescripts></mprescripts><none></none><mrow><mn>1</mn></mrow></mmultiscripts></mrow><mrow><mn>0</mn></mrow></msub><mo>)</mo></mrow></math>, <math><mrow><mi>B</mi><mo>(</mo><mn>1</mn><msub><mrow><mmultiscripts><mrow><mi>D</mi></mrow><mprescripts></mprescripts><none></none><mrow><mn>1</mn></mrow></mmultiscripts></mrow><mrow><mn>2</mn></mrow></msub><mo>)</mo></mrow></math>, <math><msub><mi>B</mi><mi>s</mi></msub><mo>(</mo><mn>1</mn><msub><mmultiscripts><mrow><mi>D</mi></mrow><mprescripts></mprescripts><none></none><mrow><mn>3</mn></mrow></mmultiscripts><mn>1</mn></msub><mo>)</mo></math>, and <math><msub><mi>B</mi><mi>s</mi></msub><mo>(</mo><mn>1</mn><msub><mmultiscripts><mrow><mi>D</mi></mrow><mprescripts></mprescripts><none></none><mrow><mn>1</mn></mrow></mmultiscripts><mn>2</mn></msub><mo>)</mo></math>. These predictions provide crucial information for upcoming experimental studies."
    }
  ], 
  "imprints": [
    {
      "date": "2019-05-31", 
      "publisher": "APS"
    }
  ]
}