{"title":"关于两粒子离散Schröodinger算子的离散谱数","authors":"Z. Muminov, Utkir Kuljanov, S. Alladustov","doi":"10.56017/2181-1318.1051","DOIUrl":null,"url":null,"abstract":"We consider a family of discrete Schrödinger operators hd(k), where k is the two-particle quasi-momentum varying in Td = (−π, π]d, associated to a system of two-particles on the d dimensional lattice Zd, d ≥ 1. The CwikelLieb-Rozenblum (CLR)-type estimates are written for hd(k) when the Fermi surface E−1 k (em(k)) of the associated dispersion relation is a one point set at em(k), the bottom of the essential spectrum. Moreover, when the Fermi surface E−1 k (em(k)) is of dimension d−1 or d−2, we obtain the necessary and su cient conditions for the existence of in nite discrete spectrum of hd(k), while in the case dimE−1 k (em(k)) ≤ d− 3, the discrete spectrum of h d(k) is nite.","PeriodicalId":127023,"journal":{"name":"Bulletin of National University of Uzbekistan: Mathematics and Natural Sciences","volume":"7 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2020-04-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":"{\"title\":\"On the number of the discrete spectrum of two-particle discrete Schröodinger operators\",\"authors\":\"Z. Muminov, Utkir Kuljanov, S. Alladustov\",\"doi\":\"10.56017/2181-1318.1051\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We consider a family of discrete Schrödinger operators hd(k), where k is the two-particle quasi-momentum varying in Td = (−π, π]d, associated to a system of two-particles on the d dimensional lattice Zd, d ≥ 1. The CwikelLieb-Rozenblum (CLR)-type estimates are written for hd(k) when the Fermi surface E−1 k (em(k)) of the associated dispersion relation is a one point set at em(k), the bottom of the essential spectrum. Moreover, when the Fermi surface E−1 k (em(k)) is of dimension d−1 or d−2, we obtain the necessary and su cient conditions for the existence of in nite discrete spectrum of hd(k), while in the case dimE−1 k (em(k)) ≤ d− 3, the discrete spectrum of h d(k) is nite.\",\"PeriodicalId\":127023,\"journal\":{\"name\":\"Bulletin of National University of Uzbekistan: Mathematics and Natural Sciences\",\"volume\":\"7 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2020-04-08\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"2\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Bulletin of National University of Uzbekistan: Mathematics and Natural Sciences\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.56017/2181-1318.1051\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Bulletin of National University of Uzbekistan: Mathematics and Natural Sciences","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.56017/2181-1318.1051","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 2
摘要
我们考虑一类离散的Schrödinger算符hd(k),其中k是在d维晶格Zd, d≥1上的两粒子系统中变化为Td =(−π, π]d的两粒子准动量。当相关色散关系的费米曲面E−1 k (em(k))是基本谱底部em(k)的一个点集时,对hd(k)写CwikelLieb-Rozenblum (CLR)型估计。此外,当费米曲面E−1 k (em(k))的维数为d−1或d−2时,我们得到了hd(k)的离散谱存在的必要和辅助条件,而当dimE−1 k (em(k))≤d−3时,hd(k)的离散谱为nite。
On the number of the discrete spectrum of two-particle discrete Schröodinger operators
We consider a family of discrete Schrödinger operators hd(k), where k is the two-particle quasi-momentum varying in Td = (−π, π]d, associated to a system of two-particles on the d dimensional lattice Zd, d ≥ 1. The CwikelLieb-Rozenblum (CLR)-type estimates are written for hd(k) when the Fermi surface E−1 k (em(k)) of the associated dispersion relation is a one point set at em(k), the bottom of the essential spectrum. Moreover, when the Fermi surface E−1 k (em(k)) is of dimension d−1 or d−2, we obtain the necessary and su cient conditions for the existence of in nite discrete spectrum of hd(k), while in the case dimE−1 k (em(k)) ≤ d− 3, the discrete spectrum of h d(k) is nite.