{"title":"The Stanley decomposition of the harmonic oscillator","authors":"L.J. Billera , R. Cushman , J.A. Sanders","doi":"10.1016/S1385-7258(88)80017-9","DOIUrl":null,"url":null,"abstract":"<div><p>This paper gives a new decomposition for the ring of polynomial functions on the variety of (<em>n</em> + 1) × (<em>n</em> + 1) complex matrices of rank less than or equal to one. This involves decomposing the monoid <span><span><span><math><mrow><msub><mo>M</mo><mi>n</mi></msub><mo>=</mo><mo>{</mo><mo>(</mo><mi>j</mi><mo>,</mo><mi>k</mi><mo>)</mo><mo>∈</mo><msup><mi>ℕ</mi><mrow><mi>n</mi><mo>+</mo><mn>1</mn></mrow></msup><mo>×</mo><msup><mi>ℕ</mi><mrow><mi>n</mi><mo>+</mo><mn>1</mn></mrow></msup><mrow><mo>|</mo><mrow><mo>|</mo><mi>j</mi><mo>|</mo><mo>=</mo><mo>|</mo><mi>k</mi><mo>|</mo></mrow></mrow><mo>}</mo></mrow></math></span></span></span> into a finite disjoint union of translates of ℕ cones based on certain 2<em>n</em> simplices in ℝ<sup>2n+2</sup>. As a consequence we have a method for writing the normal form of a perturbed <em>n</em>+1 dimensional harmonic oscillator in a unique way.</p></div>","PeriodicalId":100664,"journal":{"name":"Indagationes Mathematicae (Proceedings)","volume":"91 4","pages":"Pages 375-393"},"PeriodicalIF":0.0000,"publicationDate":"1988-12-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/S1385-7258(88)80017-9","citationCount":"36","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Indagationes Mathematicae (Proceedings)","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S1385725888800179","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 36
Abstract
This paper gives a new decomposition for the ring of polynomial functions on the variety of (n + 1) × (n + 1) complex matrices of rank less than or equal to one. This involves decomposing the monoid into a finite disjoint union of translates of ℕ cones based on certain 2n simplices in ℝ2n+2. As a consequence we have a method for writing the normal form of a perturbed n+1 dimensional harmonic oscillator in a unique way.