{
  "_oai": {
    "updated": "2022-05-19T08:07:00Z", 
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  "authors": [
    {
      "raw_name": "Nikolay Kozyrev", 
      "affiliations": [
        {
          "country": "JINR", 
          "value": "Bogoliubov Laboratory of Theoretical Physics, JINR, 141980 Dubna, Russia"
        }
      ], 
      "surname": "Kozyrev", 
      "given_names": "Nikolay", 
      "full_name": "Kozyrev, Nikolay"
    }, 
    {
      "raw_name": "Sergey Krivonos", 
      "affiliations": [
        {
          "country": "JINR", 
          "value": "Bogoliubov Laboratory of Theoretical Physics, JINR, 141980 Dubna, Russia"
        }
      ], 
      "surname": "Krivonos", 
      "given_names": "Sergey", 
      "full_name": "Krivonos, Sergey"
    }
  ], 
  "titles": [
    {
      "source": "APS", 
      "title": "<math><mi>N</mi><mo>=</mo><mn>4</mn></math> supersymmetric Schwarzian with <math><mi>D</mi><mo>(</mo><mn>1</mn><mo>,</mo><mn>2</mn><mo>;</mo><mi>\u03b1</mi><mo>)</mo></math> symmetry"
    }
  ], 
  "dois": [
    {
      "value": "10.1103/PhysRevD.105.085010"
    }
  ], 
  "publication_info": [
    {
      "journal_volume": "105", 
      "journal_title": "Physical Review D", 
      "material": "article", 
      "journal_issue": "8", 
      "year": 2022
    }
  ], 
  "$schema": "http://repo.scoap3.org/schemas/hep.json", 
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    "date": "2022-05-19T08:05:30.779094", 
    "source": "APS", 
    "method": "APS", 
    "submission_number": "6bd14ca2d74a11eca1a1661ec451a4e4"
  }, 
  "page_nr": [
    12
  ], 
  "license": [
    {
      "url": "https://creativecommons.org/licenses/by/4.0/", 
      "license": "CC-BY-4.0"
    }
  ], 
  "copyright": [
    {
      "statement": "Published by the American Physical Society", 
      "year": "2022"
    }
  ], 
  "control_number": "69263", 
  "record_creation_date": "2022-04-19T14:30:07.213500", 
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  "collections": [
    {
      "primary": "HEP"
    }, 
    {
      "primary": "Citeable"
    }, 
    {
      "primary": "Published"
    }
  ], 
  "arxiv_eprints": [
    {
      "categories": [
        "hep-th"
      ], 
      "value": "2112.14481"
    }
  ], 
  "abstracts": [
    {
      "source": "APS", 
      "value": "It was recently demonstrated that super-Schwarzian derivatives can be constructed from the Cartan forms of the superconformal supergroups <math><mrow><mi>O</mi><mi>S</mi><mi>p</mi><mo>(</mo><mn>1</mn><mo>|</mo><mn>2</mn><mo>)</mo></mrow></math>, <math><mrow><mi>S</mi><mi>U</mi><mo>(</mo><mn>1</mn><mo>,</mo><mn>1</mn><mo>|</mo><mn>1</mn><mo>)</mo></mrow></math>, <math><mrow><mi>O</mi><mi>S</mi><mi>p</mi><mo>(</mo><mn>3</mn><mo>|</mo><mn>2</mn><mo>)</mo></mrow></math>, <math><mrow><mi>S</mi><mi>U</mi><mo>(</mo><mn>1</mn><mo>,</mo><mn>1</mn><mo>|</mo><mn>2</mn><mo>)</mo></mrow></math>. Roughly speaking, the super-Schwarzian is just the component of the corresponding Cartan forms with the lowest dimension. In this paper, we apply the same approach to superalgebra <math><mi>D</mi><mo>(</mo><mn>1</mn><mo>,</mo><mn>2</mn><mo>;</mo><mi>\u03b1</mi><mo>)</mo></math>. The minimal set of constraints we used includes: (a) introducing new superspace coordinates the Cartan forms depend on, which are completely invariant with respect to the corresponding group; (b) nullifying the form for dilatation. In contrast to the <math><mi>S</mi><mi>U</mi><mo>(</mo><mn>1</mn><mo>,</mo><mn>1</mn><mo>|</mo><mn>2</mn><mo>)</mo></math> case, the new super-Schwarzian appears to be a <math><mi>d</mi><msup><mi>\u03b8</mi><mrow><mi>i</mi><mi>a</mi></mrow></msup></math> component of the form for <math><mi>s</mi><mi>u</mi><mo>(</mo><mn>2</mn><mo>)</mo></math> automorphism."
    }
  ], 
  "imprints": [
    {
      "date": "2022-04-19", 
      "publisher": "APS"
    }
  ]
}