{"title":"弱引力透镜","authors":"D. Gruen, B. Jain, M. Troxel","doi":"10.1142/9781786348364_0012","DOIUrl":null,"url":null,"abstract":"1 • Foreground Masses Can Magnify and Distort Background Sources • Faint, High-z Galaxies Provide a “Cosmic Wallpaper” Upon Which the Lensing Mass is Projected – At even modest redshifts there are ~ 50 galaxies/arcmin2. The deepest surveys with HST reveal ~ 100/arcmin2. • Source Sizes Are Unknown but We can Compute an Average Shape for Un-lensed Field Samples and Assume Random Orientations • For Simplicity Let’s Assume Average Shape is Circular with Radius q. For a Weakly Lensed Background Source:","PeriodicalId":319407,"journal":{"name":"The Dark Energy Survey","volume":"99 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2020-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Weak Gravitational Lensing\",\"authors\":\"D. Gruen, B. Jain, M. Troxel\",\"doi\":\"10.1142/9781786348364_0012\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"1 • Foreground Masses Can Magnify and Distort Background Sources • Faint, High-z Galaxies Provide a “Cosmic Wallpaper” Upon Which the Lensing Mass is Projected – At even modest redshifts there are ~ 50 galaxies/arcmin2. The deepest surveys with HST reveal ~ 100/arcmin2. • Source Sizes Are Unknown but We can Compute an Average Shape for Un-lensed Field Samples and Assume Random Orientations • For Simplicity Let’s Assume Average Shape is Circular with Radius q. For a Weakly Lensed Background Source:\",\"PeriodicalId\":319407,\"journal\":{\"name\":\"The Dark Energy Survey\",\"volume\":\"99 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2020-09-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"The Dark Energy Survey\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1142/9781786348364_0012\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"The Dark Energy Survey","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1142/9781786348364_0012","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
1 • Foreground Masses Can Magnify and Distort Background Sources • Faint, High-z Galaxies Provide a “Cosmic Wallpaper” Upon Which the Lensing Mass is Projected – At even modest redshifts there are ~ 50 galaxies/arcmin2. The deepest surveys with HST reveal ~ 100/arcmin2. • Source Sizes Are Unknown but We can Compute an Average Shape for Un-lensed Field Samples and Assume Random Orientations • For Simplicity Let’s Assume Average Shape is Circular with Radius q. For a Weakly Lensed Background Source: