{"title":"大型强子对撞机重离子项目:CMS视角","authors":"E. Norbeck, Y. Onel","doi":"10.1556/APH.24.2005.1-4.48","DOIUrl":null,"url":null,"abstract":"The LHC will collide protons at √{s} = 14 TeV and lead ions at √{sNN} = 5.5 TeV. These energies are much higher than with the Fermilab Tevatron or RHIC. Huge experiments are being assembled at four interaction points along the 27 km LHC ring. Although it is a large step into the unknown, there have been extensive calculations predicting data rates for a wide variety of processes to be observed by these experiments. Here we consider primarily the results of lead collisions as will be observed by the CMS experiment.","PeriodicalId":7004,"journal":{"name":"Acta Physica Hungarica","volume":"134 6 1","pages":"353-358"},"PeriodicalIF":0.0000,"publicationDate":"2005-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"LHC Heavy-Ion Program: a CMS Perspective\",\"authors\":\"E. Norbeck, Y. Onel\",\"doi\":\"10.1556/APH.24.2005.1-4.48\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The LHC will collide protons at √{s} = 14 TeV and lead ions at √{sNN} = 5.5 TeV. These energies are much higher than with the Fermilab Tevatron or RHIC. Huge experiments are being assembled at four interaction points along the 27 km LHC ring. Although it is a large step into the unknown, there have been extensive calculations predicting data rates for a wide variety of processes to be observed by these experiments. Here we consider primarily the results of lead collisions as will be observed by the CMS experiment.\",\"PeriodicalId\":7004,\"journal\":{\"name\":\"Acta Physica Hungarica\",\"volume\":\"134 6 1\",\"pages\":\"353-358\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2005-10-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Acta Physica Hungarica\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1556/APH.24.2005.1-4.48\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Acta Physica Hungarica","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1556/APH.24.2005.1-4.48","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
The LHC will collide protons at √{s} = 14 TeV and lead ions at √{sNN} = 5.5 TeV. These energies are much higher than with the Fermilab Tevatron or RHIC. Huge experiments are being assembled at four interaction points along the 27 km LHC ring. Although it is a large step into the unknown, there have been extensive calculations predicting data rates for a wide variety of processes to be observed by these experiments. Here we consider primarily the results of lead collisions as will be observed by the CMS experiment.
京公网安备 11010802042870号
京ICP备2023020795号-1
分享
求助内容：
应助结果提醒方式：
扫码关注我们
