{"title":"Wave packets in a semiconductor superlattice","authors":"M. Biermann, C. R. Stroud","doi":"10.1063/1.105234","DOIUrl":null,"url":null,"abstract":"When a short laser pulse excites a quantum system, a spatially localized wave packet is formed.1 In this paper, we present a theoretical study of hole wave packets in a room temperature semiconductor superlattice, the unit cell of which consists of four layers. The first and third layers are GaAs wells of width 9 and 14 monolayers, 25.4 and 39.6 A. The second and fourth are 5 monolayers, 14.1-Å thick Al0.3Ga0.7As barriers. Effectively, the material is a series of coupled quantum wells of alternating thicknesses. These parameters give an even splitting between the first three hole states. The bandgap discontinuity is split, with 43% allotted to the valence band, and the growth direction is 100. The theoretical model is a k.p. local pseudopotential method based on that of Smith and Mailhiot.2","PeriodicalId":175010,"journal":{"name":"Integrated Photonics Research","volume":"109 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1991-05-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Integrated Photonics Research","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1063/1.105234","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 2
Abstract
When a short laser pulse excites a quantum system, a spatially localized wave packet is formed.1 In this paper, we present a theoretical study of hole wave packets in a room temperature semiconductor superlattice, the unit cell of which consists of four layers. The first and third layers are GaAs wells of width 9 and 14 monolayers, 25.4 and 39.6 A. The second and fourth are 5 monolayers, 14.1-Å thick Al0.3Ga0.7As barriers. Effectively, the material is a series of coupled quantum wells of alternating thicknesses. These parameters give an even splitting between the first three hole states. The bandgap discontinuity is split, with 43% allotted to the valence band, and the growth direction is 100. The theoretical model is a k.p. local pseudopotential method based on that of Smith and Mailhiot.2