{
  "_oai": {
    "updated": "2022-04-05T09:31:06Z", 
    "id": "oai:repo.scoap3.org:62726", 
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  "authors": [
    {
      "raw_name": "Sungsik Noh", 
      "affiliations": [
        {
          "country": "South Korea", 
          "value": "Department of Physics and Institute of Physics and Applied Physics, Yonsei University, Seoul 03722, Korea"
        }
      ], 
      "surname": "Noh", 
      "given_names": "Sungsik", 
      "full_name": "Noh, Sungsik"
    }, 
    {
      "raw_name": "Woosung Park", 
      "affiliations": [
        {
          "country": "South Korea", 
          "value": "Department of Physics and Institute of Physics and Applied Physics, Yonsei University, Seoul 03722, Korea"
        }
      ], 
      "surname": "Park", 
      "given_names": "Woosung", 
      "full_name": "Park, Woosung"
    }, 
    {
      "raw_name": "Su Houng Lee", 
      "affiliations": [
        {
          "country": "South Korea", 
          "value": "Department of Physics and Institute of Physics and Applied Physics, Yonsei University, Seoul 03722, Korea"
        }
      ], 
      "surname": "Lee", 
      "given_names": "Su Houng", 
      "full_name": "Lee, Su Houng"
    }
  ], 
  "titles": [
    {
      "source": "APS", 
      "title": "Doubly heavy tetraquarks, <math><mi>q</mi><msup><mi>q</mi><mo>\u2032</mo></msup><mover><mi>Q</mi><mo>\u00af</mo></mover><mover><msup><mi>Q</mi><mo>\u2032</mo></msup><mo>\u00af</mo></mover></math>, in a nonrelativistic quark model with a complete set of harmonic oscillator bases"
    }
  ], 
  "dois": [
    {
      "value": "10.1103/PhysRevD.103.114009"
    }
  ], 
  "publication_info": [
    {
      "journal_volume": "103", 
      "journal_title": "Physical Review D", 
      "material": "article", 
      "journal_issue": "11", 
      "year": 2021
    }
  ], 
  "$schema": "http://repo.scoap3.org/schemas/hep.json", 
  "acquisition_source": {
    "date": "2022-04-05T09:18:10.770971", 
    "source": "APS", 
    "method": "APS", 
    "submission_number": "2cf5978cb4c111ec837fd6d834be26e1"
  }, 
  "page_nr": [
    21
  ], 
  "license": [
    {
      "url": "https://creativecommons.org/licenses/by/4.0/", 
      "license": "CC-BY-4.0"
    }
  ], 
  "copyright": [
    {
      "statement": "Published by the American Physical Society", 
      "year": "2021"
    }
  ], 
  "control_number": "62726", 
  "record_creation_date": "2021-06-08T18:30:21.263892", 
  "_files": [
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      "filetype": "pdf", 
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      "key": "10.1103/PhysRevD.103.114009.pdf", 
      "size": 4911460
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  ], 
  "collections": [
    {
      "primary": "HEP"
    }, 
    {
      "primary": "Citeable"
    }, 
    {
      "primary": "Published"
    }
  ], 
  "arxiv_eprints": [
    {
      "categories": [
        "hep-ph", 
        "nucl-th"
      ], 
      "value": "2102.09614"
    }
  ], 
  "abstracts": [
    {
      "source": "APS", 
      "value": "We improve our previous variational method based nonrelativistic quark model by introducing a complete set of three-dimensional harmonic oscillator bases as the spatial part of the total wave function. To assess the validity of our approach, we compare the binding energy thus calculated with the exact value for the hydrogen model. After fitting to the masses of the ground state hadrons, we apply our new method to analyzing the doubly heavy tetraquark states <math><mi>q</mi><msup><mi>q</mi><mo>\u2032</mo></msup><mover><mi>Q</mi><mo>\u00af</mo></mover><mover><msup><mi>Q</mi><mo>\u2032</mo></msup><mo>\u00af</mo></mover></math> and compare the results for the binding energies to results in other works. We also calculate the ground state masses of <math><msub><mi>T</mi><mrow><mi>s</mi><mi>c</mi></mrow></msub><mo>(</mo><mi>u</mi><mi>d</mi><mover><mi>s</mi><mo>\u00af</mo></mover><mover><mi>c</mi><mo>\u00af</mo></mover><mo>)</mo></math> and <math><msub><mi>T</mi><mrow><mi>s</mi><mi>b</mi></mrow></msub><mo>(</mo><mi>u</mi><mi>d</mi><mover><mi>s</mi><mo>\u00af</mo></mover><mover><mi>b</mi><mo>\u00af</mo></mover><mo>)</mo></math> with <math><mo>(</mo><mi>I</mi><mo>,</mo><mi>S</mi><mo>)</mo><mo>=</mo><mo>(</mo><mn>0</mn><mo>,</mo><mn>1</mn><mo>)</mo><mo>,</mo><mo>(</mo><mn>0</mn><mo>,</mo><mn>2</mn><mo>)</mo></math>. We find that <math><msub><mi>T</mi><mrow><mi>b</mi><mi>b</mi></mrow></msub><mo>(</mo><mi>u</mi><mi>d</mi><mover><mi>b</mi><mo>\u00af</mo></mover><mover><mi>b</mi><mo>\u00af</mo></mover><mo>)</mo></math> and <math><mi>u</mi><mi>s</mi><mover><mi>b</mi><mo>\u00af</mo></mover><mover><mi>b</mi><mo>\u00af</mo></mover></math>, both with <math><mo>(</mo><mi>I</mi><mo>,</mo><mi>S</mi><mo>)</mo><mo>=</mo><mo>(</mo><mn>0</mn><mo>,</mo><mn>1</mn><mo>)</mo></math>, are stable against the two lowest threshold meson states with binding energies <math><mo>\u2212</mo><mn>145</mn></math> and <math><mo>\u2212</mo><mn>42</mn><mtext> </mtext><mtext> </mtext><mi>MeV</mi></math>, respectively. We further find that <math><msub><mi>T</mi><mrow><mi>c</mi><mi>b</mi></mrow></msub><mo>(</mo><mi>u</mi><mi>d</mi><mover><mi>c</mi><mo>\u00af</mo></mover><mover><mi>b</mi><mo>\u00af</mo></mover><mo>)</mo></math> is near the lowest threshold. The spatial sizes for the tetraquarks are also discussed."
    }
  ], 
  "imprints": [
    {
      "date": "2021-06-08", 
      "publisher": "APS"
    }
  ]
}