{"title":"利用脉冲星定时阵列测试无滑动模型:NANOGrav 和 IPTA","authors":"Mohammadreza Davari, Alireza Allahyari, Shahram Khosravi","doi":"arxiv-2409.05956","DOIUrl":null,"url":null,"abstract":"We perform an observational study of modified gravity considering a potential\ninflationary interpretation of pulsar timing arrays (PTA). We use a motivated\nmodel known as no slip in which the gravitational wave propagation is modified.\nSpecifically, by using two different parametrizations for the model, we find\nthe approximate transfer functions for tensor perturbations. In this way, we\nobtain the spectral energy density of gravitational waves and use NANOGrav and\nIPTA second data release to constrain parameters of the model. We find that\nthere is degeneracy between the model parameters $\\xi$ and $c_M$. For $c_M$, we\nonly get an upper bound on the parameter. Thus, it is difficult to constrain\nthem with percent level accuracy with the current PTA data.","PeriodicalId":501041,"journal":{"name":"arXiv - PHYS - General Relativity and Quantum Cosmology","volume":"15 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Testing No slip model with pulsar timing arrays: NANOGrav and IPTA\",\"authors\":\"Mohammadreza Davari, Alireza Allahyari, Shahram Khosravi\",\"doi\":\"arxiv-2409.05956\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We perform an observational study of modified gravity considering a potential\\ninflationary interpretation of pulsar timing arrays (PTA). We use a motivated\\nmodel known as no slip in which the gravitational wave propagation is modified.\\nSpecifically, by using two different parametrizations for the model, we find\\nthe approximate transfer functions for tensor perturbations. In this way, we\\nobtain the spectral energy density of gravitational waves and use NANOGrav and\\nIPTA second data release to constrain parameters of the model. We find that\\nthere is degeneracy between the model parameters $\\\\xi$ and $c_M$. For $c_M$, we\\nonly get an upper bound on the parameter. Thus, it is difficult to constrain\\nthem with percent level accuracy with the current PTA data.\",\"PeriodicalId\":501041,\"journal\":{\"name\":\"arXiv - PHYS - General Relativity and Quantum Cosmology\",\"volume\":\"15 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-09\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - General Relativity and Quantum Cosmology\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2409.05956\",\"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 - General Relativity and Quantum Cosmology","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.05956","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Testing No slip model with pulsar timing arrays: NANOGrav and IPTA
We perform an observational study of modified gravity considering a potential
inflationary interpretation of pulsar timing arrays (PTA). We use a motivated
model known as no slip in which the gravitational wave propagation is modified.
Specifically, by using two different parametrizations for the model, we find
the approximate transfer functions for tensor perturbations. In this way, we
obtain the spectral energy density of gravitational waves and use NANOGrav and
IPTA second data release to constrain parameters of the model. We find that
there is degeneracy between the model parameters $\xi$ and $c_M$. For $c_M$, we
only get an upper bound on the parameter. Thus, it is difficult to constrain
them with percent level accuracy with the current PTA data.