{"title":"The second moment for counting prime geodesics","authors":"I. Kaneko","doi":"10.3792/pjaa.96.002","DOIUrl":null,"url":null,"abstract":": A brighter light has freshly been shed upon the second moment of the Prime Geodesic Theorem. We work with such moments in the two and three dimensional hyperbolic spaces. Letting E (cid:2) ð X Þ be the error term arising from counting prime geodesics associated to (cid:2) ¼ PSL 2 ð Z ½ i (cid:2)Þ , the bound E (cid:2) ð X Þ (cid:3) X 3 = 2 þ (cid:2) is proved in a square mean sense. Our second moment bound is the pure counterpart of the work of Balog et al. for (cid:2) ¼ PSL 2 ð Z Þ , and the main innovation entails the delicate analysis of sums of Kloosterman sums. We also infer pointwise bounds from the standpoint of the second moment. Finally, we announce the pointwise bound E (cid:2) ð X Þ (cid:3) X 67 = 42 þ (cid:2) for (cid:2) ¼ PSL 2 ð Z ½ i (cid:2)Þ by an application of the Weyl-type subconvexity.","PeriodicalId":0,"journal":{"name":"","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2020-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"","FirstCategoryId":"100","ListUrlMain":"https://doi.org/10.3792/pjaa.96.002","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
: A brighter light has freshly been shed upon the second moment of the Prime Geodesic Theorem. We work with such moments in the two and three dimensional hyperbolic spaces. Letting E (cid:2) ð X Þ be the error term arising from counting prime geodesics associated to (cid:2) ¼ PSL 2 ð Z ½ i (cid:2)Þ , the bound E (cid:2) ð X Þ (cid:3) X 3 = 2 þ (cid:2) is proved in a square mean sense. Our second moment bound is the pure counterpart of the work of Balog et al. for (cid:2) ¼ PSL 2 ð Z Þ , and the main innovation entails the delicate analysis of sums of Kloosterman sums. We also infer pointwise bounds from the standpoint of the second moment. Finally, we announce the pointwise bound E (cid:2) ð X Þ (cid:3) X 67 = 42 þ (cid:2) for (cid:2) ¼ PSL 2 ð Z ½ i (cid:2)Þ by an application of the Weyl-type subconvexity.