{"title":"组合量子引力中的暗物质和暗能量","authors":"Carlo A. Trugenberger","doi":"arxiv-2409.09385","DOIUrl":null,"url":null,"abstract":"We point out that dark matter and dark energy arise naturally in a recently\nproposed model of combinatorial quantum gravity. Dark energy is due to the\nground-state curvature at finite coupling, dark matter arises from allotropy in\nthe discrete structure of space-time. The stable structure of the space-time\n\"crystal\" represents the curved background, the coexisting metastable\nallotropes of higher curvature and energy are natural candidates for dark\nmatter.","PeriodicalId":501339,"journal":{"name":"arXiv - PHYS - High Energy Physics - Theory","volume":"54 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Dark matter and dark energy in combinatorial quantum gravity\",\"authors\":\"Carlo A. Trugenberger\",\"doi\":\"arxiv-2409.09385\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We point out that dark matter and dark energy arise naturally in a recently\\nproposed model of combinatorial quantum gravity. Dark energy is due to the\\nground-state curvature at finite coupling, dark matter arises from allotropy in\\nthe discrete structure of space-time. The stable structure of the space-time\\n\\\"crystal\\\" represents the curved background, the coexisting metastable\\nallotropes of higher curvature and energy are natural candidates for dark\\nmatter.\",\"PeriodicalId\":501339,\"journal\":{\"name\":\"arXiv - PHYS - High Energy Physics - Theory\",\"volume\":\"54 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-14\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - High Energy Physics - Theory\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2409.09385\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - High Energy Physics - Theory","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.09385","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Dark matter and dark energy in combinatorial quantum gravity
We point out that dark matter and dark energy arise naturally in a recently
proposed model of combinatorial quantum gravity. Dark energy is due to the
ground-state curvature at finite coupling, dark matter arises from allotropy in
the discrete structure of space-time. The stable structure of the space-time
"crystal" represents the curved background, the coexisting metastable
allotropes of higher curvature and energy are natural candidates for dark
matter.