{"title":"The q-Onsager algebra and the quantum torus","authors":"Owen Goff","doi":"10.1016/j.jcta.2024.105939","DOIUrl":null,"url":null,"abstract":"<div><p>The <em>q</em>-Onsager algebra, denoted <span><math><msub><mrow><mi>O</mi></mrow><mrow><mi>q</mi></mrow></msub></math></span>, is defined by two generators <span><math><msub><mrow><mi>W</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>,</mo><msub><mrow><mi>W</mi></mrow><mrow><mn>1</mn></mrow></msub></math></span> and two relations called the <em>q</em>-Dolan-Grady relations. Recently, Terwilliger introduced some elements of <span><math><msub><mrow><mi>O</mi></mrow><mrow><mi>q</mi></mrow></msub></math></span>, said to be alternating. These elements are denoted<span><span><span><math><msubsup><mrow><mo>{</mo><msub><mrow><mi>W</mi></mrow><mrow><mo>−</mo><mi>k</mi></mrow></msub><mo>}</mo></mrow><mrow><mi>k</mi><mo>=</mo><mn>0</mn></mrow><mrow><mo>∞</mo></mrow></msubsup><mo>,</mo><mspace></mspace><msubsup><mrow><mo>{</mo><msub><mrow><mi>W</mi></mrow><mrow><mi>k</mi><mo>+</mo><mn>1</mn></mrow></msub><mo>}</mo></mrow><mrow><mi>k</mi><mo>=</mo><mn>0</mn></mrow><mrow><mo>∞</mo></mrow></msubsup><mo>,</mo><mspace></mspace><msubsup><mrow><mo>{</mo><msub><mrow><mi>G</mi></mrow><mrow><mi>k</mi><mo>+</mo><mn>1</mn></mrow></msub><mo>}</mo></mrow><mrow><mi>k</mi><mo>=</mo><mn>0</mn></mrow><mrow><mo>∞</mo></mrow></msubsup><mo>,</mo><mspace></mspace><msubsup><mrow><mo>{</mo><msub><mrow><mover><mrow><mi>G</mi></mrow><mrow><mo>˜</mo></mrow></mover></mrow><mrow><mi>k</mi><mo>+</mo><mn>1</mn></mrow></msub><mo>}</mo></mrow><mrow><mi>k</mi><mo>=</mo><mn>0</mn></mrow><mrow><mo>∞</mo></mrow></msubsup><mo>.</mo></math></span></span></span></p><p>The alternating elements of <span><math><msub><mrow><mi>O</mi></mrow><mrow><mi>q</mi></mrow></msub></math></span> are defined recursively. By construction, they are polynomials in <span><math><msub><mrow><mi>W</mi></mrow><mrow><mn>0</mn></mrow></msub></math></span> and <span><math><msub><mrow><mi>W</mi></mrow><mrow><mn>1</mn></mrow></msub></math></span>. It is currently unknown how to express these polynomials in closed form.</p><p>In this paper, we consider an algebra <span><math><msub><mrow><mi>T</mi></mrow><mrow><mi>q</mi></mrow></msub></math></span>, called the quantum torus. We present a basis for <span><math><msub><mrow><mi>T</mi></mrow><mrow><mi>q</mi></mrow></msub></math></span> and define an algebra homomorphism <span><math><mi>p</mi><mo>:</mo><msub><mrow><mi>O</mi></mrow><mrow><mi>q</mi></mrow></msub><mo>↦</mo><msub><mrow><mi>T</mi></mrow><mrow><mi>q</mi></mrow></msub></math></span>. In our main result, we express the <em>p</em>-images of the alternating elements of <span><math><msub><mrow><mi>O</mi></mrow><mrow><mi>q</mi></mrow></msub></math></span> in the basis for <span><math><msub><mrow><mi>T</mi></mrow><mrow><mi>q</mi></mrow></msub></math></span>. These expressions are in a closed form that we find attractive.</p></div>","PeriodicalId":0,"journal":{"name":"","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2024-08-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"","FirstCategoryId":"100","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0097316524000785","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
The q-Onsager algebra, denoted , is defined by two generators and two relations called the q-Dolan-Grady relations. Recently, Terwilliger introduced some elements of , said to be alternating. These elements are denoted
The alternating elements of are defined recursively. By construction, they are polynomials in and . It is currently unknown how to express these polynomials in closed form.
In this paper, we consider an algebra , called the quantum torus. We present a basis for and define an algebra homomorphism . In our main result, we express the p-images of the alternating elements of in the basis for . These expressions are in a closed form that we find attractive.