Comparing recent PTA results on the nanohertz stochastic gravitational wave background

The Australian, Chinese, European, Indian, and North American pulsar timing array (PTA) collaborations recently reported, at varying levels, evidence for the presence of a nanohertz gravitational wave background (GWB). Given that each PTA made different choices in modeling their data, we perform a c...

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Hauptverfasser: Antoniadis, J, Anumarlapudi, A, Arzoumanian, Z, Babak, S, Bailes, M, Nielsen, A. -S. Bak, Baker, P. T, Bassa, C. G, Berthereau, A, Bhat, N. D. R, Blecha, L, Brazier, A, Brook, P. R, Burgay, M, Burnette, R, Cameron, A, Case, R, Chanlaridis, S, Charisi, M, Chatterjee, S, Chen, Z. -C, Cohen, T, Coles, W. A, Cornish, N. J, Cromartie, H. T, Crowter, K, Dai, S, Dandapat, S, DeGan, D, Dey, L, Dhanda-Batra, N, Ellis, J. A, Ferdman, R. D, Fonseca, E, Franchini, A, Gair, J. R, Garver-Daniels, N, Gentile, P. A, Goncharov, B, Gopakumar, A, Grießmeier, J. -M, Gültekin, K, Grunthal, K, Hazboun, J. S, Hisano, S, Hu, H, Izquierdo-Villalba, D, Jawor, J, Jennings, R. J, Jessner, A, Kaiser, A. R, Kapur, A, Kelley, L. Z, Kramer, M, Kulkarni, A, Lazio, T. J. W, Liu, T, Lommen, A, Main, R. A, McKee, J. W, McLaughlin, M. A, McMann, N, Meyers, B. W, Miles, M, Mitridate, A, Nathan, R. S, Ng, C, Nice, D. J, Nobleson, K, Osłowski, S, Paladi, A. K, Parthasarathy, A, Perera, B. B. P, Porayko, N. K, Ransom, S. M, Reardon, D. J, Rogers, A. F, Sardesai, S. C, Schmiedekamp, C, Sesana, A, Shaifullah, G, Speri, L, Stairs, I. H, Sun, J. P, Susarla, S. C, Taylor, J, Taylor, S. R, Turner, J. E, Unal, C, Vallisneri, M, van der Wateren, E, van Haasteren, R, Verbiest, J. P. W, Wahl, H. M, Wang, L, Wayt, K. E, Wu, Z, Young, O, Zhang, L, Zhu, X. -J
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creator Antoniadis, J
Anumarlapudi, A
Arzoumanian, Z
Babak, S
Bailes, M
Nielsen, A. -S. Bak
Baker, P. T
Bassa, C. G
Berthereau, A
Bhat, N. D. R
Blecha, L
Brazier, A
Brook, P. R
Burgay, M
Burnette, R
Cameron, A
Case, R
Chanlaridis, S
Charisi, M
Chatterjee, S
Chen, Z. -C
Cohen, T
Coles, W. A
Cornish, N. J
Cromartie, H. T
Crowter, K
Dai, S
Dandapat, S
DeGan, D
Dey, L
Dhanda-Batra, N
Ellis, J. A
Ferdman, R. D
Fonseca, E
Franchini, A
Gair, J. R
Garver-Daniels, N
Gentile, P. A
Goncharov, B
Gopakumar, A
Grießmeier, J. -M
Gültekin, K
Grunthal, K
Hazboun, J. S
Hisano, S
Hu, H
Izquierdo-Villalba, D
Jawor, J
Jennings, R. J
Jessner, A
Kaiser, A. R
Kapur, A
Kelley, L. Z
Kramer, M
Kulkarni, A
Lazio, T. J. W
Liu, T
Lommen, A
Main, R. A
McKee, J. W
McLaughlin, M. A
McMann, N
Meyers, B. W
Miles, M
Mitridate, A
Nathan, R. S
Ng, C
Nice, D. J
Nobleson, K
Osłowski, S
Paladi, A. K
Parthasarathy, A
Perera, B. B. P
Porayko, N. K
Ransom, S. M
Reardon, D. J
Rogers, A. F
Sardesai, S. C
Schmiedekamp, C
Sesana, A
Shaifullah, G
Speri, L
Stairs, I. H
Sun, J. P
Susarla, S. C
Taylor, J
Taylor, S. R
Turner, J. E
Unal, C
Vallisneri, M
van der Wateren, E
van Haasteren, R
Verbiest, J. P. W
Wahl, H. M
Wang, L
Wayt, K. E
Wu, Z
Young, O
Zhang, L
Zhu, X. -J
description The Australian, Chinese, European, Indian, and North American pulsar timing array (PTA) collaborations recently reported, at varying levels, evidence for the presence of a nanohertz gravitational wave background (GWB). Given that each PTA made different choices in modeling their data, we perform a comparison of the GWB and individual pulsar noise parameters across the results reported from the PTAs that constitute the International Pulsar Timing Array (IPTA). We show that despite making different modeling choices, there is no significant difference in the GWB parameters that are measured by the different PTAs, agreeing within $1\sigma$. The pulsar noise parameters are also consistent between different PTAs for the majority of the pulsars included in these analyses. We bridge the differences in modeling choices by adopting a standardized noise model for all pulsars and PTAs, finding that under this model there is a reduction in the tension in the pulsar noise parameters. As part of this reanalysis, we "extended" each PTA's data set by adding extra pulsars that were not timed by that PTA. Under these extensions, we find better constraints on the GWB amplitude and a higher signal-to-noise ratio for the Hellings and Downs correlations. These extensions serve as a prelude to the benefits offered by a full combination of data across all pulsars in the IPTA, i.e., the IPTA's Data Release 3, which will involve not just adding in additional pulsars, but also including data from all three PTAs where any given pulsar is timed by more than as single PTA.
doi_str_mv 10.48550/arxiv.2309.00693
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Bak ; Baker, P. T ; Bassa, C. G ; Berthereau, A ; Bhat, N. D. R ; Blecha, L ; Brazier, A ; Brook, P. R ; Burgay, M ; Burnette, R ; Cameron, A ; Case, R ; Chanlaridis, S ; Charisi, M ; Chatterjee, S ; Chen, Z. -C ; Cohen, T ; Coles, W. A ; Cornish, N. J ; Cromartie, H. T ; Crowter, K ; Dai, S ; Dandapat, S ; DeGan, D ; Dey, L ; Dhanda-Batra, N ; Ellis, J. A ; Ferdman, R. D ; Fonseca, E ; Franchini, A ; Gair, J. R ; Garver-Daniels, N ; Gentile, P. A ; Goncharov, B ; Gopakumar, A ; Grießmeier, J. -M ; Gültekin, K ; Grunthal, K ; Hazboun, J. S ; Hisano, S ; Hu, H ; Izquierdo-Villalba, D ; Jawor, J ; Jennings, R. J ; Jessner, A ; Kaiser, A. R ; Kapur, A ; Kelley, L. Z ; Kramer, M ; Kulkarni, A ; Lazio, T. J. W ; Liu, T ; Lommen, A ; Main, R. A ; McKee, J. W ; McLaughlin, M. A ; McMann, N ; Meyers, B. W ; Miles, M ; Mitridate, A ; Nathan, R. S ; Ng, C ; Nice, D. J ; Nobleson, K ; Osłowski, S ; Paladi, A. K ; Parthasarathy, A ; Perera, B. B. P ; Porayko, N. K ; Ransom, S. M ; Reardon, D. J ; Rogers, A. F ; Sardesai, S. C ; Schmiedekamp, C ; Sesana, A ; Shaifullah, G ; Speri, L ; Stairs, I. H ; Sun, J. P ; Susarla, S. C ; Taylor, J ; Taylor, S. R ; Turner, J. E ; Unal, C ; Vallisneri, M ; van der Wateren, E ; van Haasteren, R ; Verbiest, J. P. W ; Wahl, H. M ; Wang, L ; Wayt, K. E ; Wu, Z ; Young, O ; Zhang, L ; Zhu, X. -J</creator><creatorcontrib>Antoniadis, J ; Anumarlapudi, A ; Arzoumanian, Z ; Babak, S ; Bailes, M ; Nielsen, A. -S. Bak ; Baker, P. T ; Bassa, C. G ; Berthereau, A ; Bhat, N. D. R ; Blecha, L ; Brazier, A ; Brook, P. R ; Burgay, M ; Burnette, R ; Cameron, A ; Case, R ; Chanlaridis, S ; Charisi, M ; Chatterjee, S ; Chen, Z. -C ; Cohen, T ; Coles, W. A ; Cornish, N. J ; Cromartie, H. T ; Crowter, K ; Dai, S ; Dandapat, S ; DeGan, D ; Dey, L ; Dhanda-Batra, N ; Ellis, J. A ; Ferdman, R. D ; Fonseca, E ; Franchini, A ; Gair, J. R ; Garver-Daniels, N ; Gentile, P. A ; Goncharov, B ; Gopakumar, A ; Grießmeier, J. -M ; Gültekin, K ; Grunthal, K ; Hazboun, J. S ; Hisano, S ; Hu, H ; Izquierdo-Villalba, D ; Jawor, J ; Jennings, R. J ; Jessner, A ; Kaiser, A. R ; Kapur, A ; Kelley, L. Z ; Kramer, M ; Kulkarni, A ; Lazio, T. J. W ; Liu, T ; Lommen, A ; Main, R. A ; McKee, J. W ; McLaughlin, M. A ; McMann, N ; Meyers, B. W ; Miles, M ; Mitridate, A ; Nathan, R. S ; Ng, C ; Nice, D. J ; Nobleson, K ; Osłowski, S ; Paladi, A. K ; Parthasarathy, A ; Perera, B. B. P ; Porayko, N. K ; Ransom, S. M ; Reardon, D. J ; Rogers, A. F ; Sardesai, S. C ; Schmiedekamp, C ; Sesana, A ; Shaifullah, G ; Speri, L ; Stairs, I. H ; Sun, J. P ; Susarla, S. C ; Taylor, J ; Taylor, S. R ; Turner, J. E ; Unal, C ; Vallisneri, M ; van der Wateren, E ; van Haasteren, R ; Verbiest, J. P. W ; Wahl, H. M ; Wang, L ; Wayt, K. 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We bridge the differences in modeling choices by adopting a standardized noise model for all pulsars and PTAs, finding that under this model there is a reduction in the tension in the pulsar noise parameters. As part of this reanalysis, we "extended" each PTA's data set by adding extra pulsars that were not timed by that PTA. Under these extensions, we find better constraints on the GWB amplitude and a higher signal-to-noise ratio for the Hellings and Downs correlations. These extensions serve as a prelude to the benefits offered by a full combination of data across all pulsars in the IPTA, i.e., the IPTA's Data Release 3, which will involve not just adding in additional pulsars, but also including data from all three PTAs where any given pulsar is timed by more than as single PTA.</description><identifier>DOI: 10.48550/arxiv.2309.00693</identifier><language>eng</language><subject>Physics - General Relativity and Quantum Cosmology ; Physics - High Energy Astrophysical Phenomena</subject><creationdate>2023-09</creationdate><rights>http://arxiv.org/licenses/nonexclusive-distrib/1.0</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,776,881</link.rule.ids><linktorsrc>$$Uhttps://arxiv.org/abs/2309.00693$$EView_record_in_Cornell_University$$FView_record_in_$$GCornell_University$$Hfree_for_read</linktorsrc><backlink>$$Uhttps://doi.org/10.48550/arXiv.2309.00693$$DView paper in arXiv$$Hfree_for_read</backlink></links><search><creatorcontrib>Antoniadis, J</creatorcontrib><creatorcontrib>Anumarlapudi, A</creatorcontrib><creatorcontrib>Arzoumanian, Z</creatorcontrib><creatorcontrib>Babak, S</creatorcontrib><creatorcontrib>Bailes, M</creatorcontrib><creatorcontrib>Nielsen, A. -S. 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E</creatorcontrib><creatorcontrib>Unal, C</creatorcontrib><creatorcontrib>Vallisneri, M</creatorcontrib><creatorcontrib>van der Wateren, E</creatorcontrib><creatorcontrib>van Haasteren, R</creatorcontrib><creatorcontrib>Verbiest, J. P. W</creatorcontrib><creatorcontrib>Wahl, H. M</creatorcontrib><creatorcontrib>Wang, L</creatorcontrib><creatorcontrib>Wayt, K. E</creatorcontrib><creatorcontrib>Wu, Z</creatorcontrib><creatorcontrib>Young, O</creatorcontrib><creatorcontrib>Zhang, L</creatorcontrib><creatorcontrib>Zhu, X. -J</creatorcontrib><title>Comparing recent PTA results on the nanohertz stochastic gravitational wave background</title><description>The Australian, Chinese, European, Indian, and North American pulsar timing array (PTA) collaborations recently reported, at varying levels, evidence for the presence of a nanohertz gravitational wave background (GWB). Given that each PTA made different choices in modeling their data, we perform a comparison of the GWB and individual pulsar noise parameters across the results reported from the PTAs that constitute the International Pulsar Timing Array (IPTA). We show that despite making different modeling choices, there is no significant difference in the GWB parameters that are measured by the different PTAs, agreeing within $1\sigma$. The pulsar noise parameters are also consistent between different PTAs for the majority of the pulsars included in these analyses. We bridge the differences in modeling choices by adopting a standardized noise model for all pulsars and PTAs, finding that under this model there is a reduction in the tension in the pulsar noise parameters. As part of this reanalysis, we "extended" each PTA's data set by adding extra pulsars that were not timed by that PTA. Under these extensions, we find better constraints on the GWB amplitude and a higher signal-to-noise ratio for the Hellings and Downs correlations. These extensions serve as a prelude to the benefits offered by a full combination of data across all pulsars in the IPTA, i.e., the IPTA's Data Release 3, which will involve not just adding in additional pulsars, but also including data from all three PTAs where any given pulsar is timed by more than as single PTA.</description><subject>Physics - General Relativity and Quantum Cosmology</subject><subject>Physics - High Energy Astrophysical Phenomena</subject><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><sourceid>GOX</sourceid><recordid>eNotz7tOwzAYhmEvDKhwAUz4BhLs-tB4rCJOUiUYItbo9ymxmtqV44bD1QOF6XunT3oQuqGk5o0Q5A7yR1jqNSOqJkQqdone2nQ4Qg5xwNkZFwt-7bY_OZ-mMuMUcRkdjhDT6HL5wnNJZoS5BIOHDEsoUEKKMOF3WBzWYPZDTqdor9CFh2l21_-7Qt3Dfdc-VbuXx-d2u6tAblhlLOEehKUA3FnCrDTgdGPWxjJOVeOtI9JSpbVWruHeeEKNFEJ7y6TkwFbo9u_2DOuPORwgf_a_wP4MZN9eKk5M</recordid><startdate>20230901</startdate><enddate>20230901</enddate><creator>Antoniadis, J</creator><creator>Anumarlapudi, A</creator><creator>Arzoumanian, Z</creator><creator>Babak, S</creator><creator>Bailes, M</creator><creator>Nielsen, A. -S. 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E</creator><creator>Wu, Z</creator><creator>Young, O</creator><creator>Zhang, L</creator><creator>Zhu, X. -J</creator><scope>GOX</scope></search><sort><creationdate>20230901</creationdate><title>Comparing recent PTA results on the nanohertz stochastic gravitational wave background</title><author>Antoniadis, J ; Anumarlapudi, A ; Arzoumanian, Z ; Babak, S ; Bailes, M ; Nielsen, A. -S. Bak ; Baker, P. T ; Bassa, C. G ; Berthereau, A ; Bhat, N. D. R ; Blecha, L ; Brazier, A ; Brook, P. R ; Burgay, M ; Burnette, R ; Cameron, A ; Case, R ; Chanlaridis, S ; Charisi, M ; Chatterjee, S ; Chen, Z. -C ; Cohen, T ; Coles, W. A ; Cornish, N. J ; Cromartie, H. T ; Crowter, K ; Dai, S ; Dandapat, S ; DeGan, D ; Dey, L ; Dhanda-Batra, N ; Ellis, J. A ; Ferdman, R. D ; Fonseca, E ; Franchini, A ; Gair, J. R ; Garver-Daniels, N ; Gentile, P. A ; Goncharov, B ; Gopakumar, A ; Grießmeier, J. -M ; Gültekin, K ; Grunthal, K ; Hazboun, J. S ; Hisano, S ; Hu, H ; Izquierdo-Villalba, D ; Jawor, J ; Jennings, R. J ; Jessner, A ; Kaiser, A. R ; Kapur, A ; Kelley, L. Z ; Kramer, M ; Kulkarni, A ; Lazio, T. J. W ; Liu, T ; Lommen, A ; Main, R. A ; McKee, J. W ; McLaughlin, M. A ; McMann, N ; Meyers, B. W ; Miles, M ; Mitridate, A ; Nathan, R. S ; Ng, C ; Nice, D. J ; Nobleson, K ; Osłowski, S ; Paladi, A. K ; Parthasarathy, A ; Perera, B. B. P ; Porayko, N. K ; Ransom, S. M ; Reardon, D. J ; Rogers, A. F ; Sardesai, S. C ; Schmiedekamp, C ; Sesana, A ; Shaifullah, G ; Speri, L ; Stairs, I. H ; Sun, J. P ; Susarla, S. C ; Taylor, J ; Taylor, S. R ; Turner, J. E ; Unal, C ; Vallisneri, M ; van der Wateren, E ; van Haasteren, R ; Verbiest, J. P. W ; Wahl, H. M ; Wang, L ; Wayt, K. E ; Wu, Z ; Young, O ; Zhang, L ; Zhu, X. -J</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a673-cd04fa5d1aa4ed03d6caeb8c2cd34198fde06d19bbb9e84fcf01c655bfd3664a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Physics - General Relativity and Quantum Cosmology</topic><topic>Physics - High Energy Astrophysical Phenomena</topic><toplevel>online_resources</toplevel><creatorcontrib>Antoniadis, J</creatorcontrib><creatorcontrib>Anumarlapudi, A</creatorcontrib><creatorcontrib>Arzoumanian, Z</creatorcontrib><creatorcontrib>Babak, S</creatorcontrib><creatorcontrib>Bailes, M</creatorcontrib><creatorcontrib>Nielsen, A. -S. Bak</creatorcontrib><creatorcontrib>Baker, P. T</creatorcontrib><creatorcontrib>Bassa, C. G</creatorcontrib><creatorcontrib>Berthereau, A</creatorcontrib><creatorcontrib>Bhat, N. D. R</creatorcontrib><creatorcontrib>Blecha, L</creatorcontrib><creatorcontrib>Brazier, A</creatorcontrib><creatorcontrib>Brook, P. R</creatorcontrib><creatorcontrib>Burgay, M</creatorcontrib><creatorcontrib>Burnette, R</creatorcontrib><creatorcontrib>Cameron, A</creatorcontrib><creatorcontrib>Case, R</creatorcontrib><creatorcontrib>Chanlaridis, S</creatorcontrib><creatorcontrib>Charisi, M</creatorcontrib><creatorcontrib>Chatterjee, S</creatorcontrib><creatorcontrib>Chen, Z. -C</creatorcontrib><creatorcontrib>Cohen, T</creatorcontrib><creatorcontrib>Coles, W. A</creatorcontrib><creatorcontrib>Cornish, N. J</creatorcontrib><creatorcontrib>Cromartie, H. T</creatorcontrib><creatorcontrib>Crowter, K</creatorcontrib><creatorcontrib>Dai, S</creatorcontrib><creatorcontrib>Dandapat, S</creatorcontrib><creatorcontrib>DeGan, D</creatorcontrib><creatorcontrib>Dey, L</creatorcontrib><creatorcontrib>Dhanda-Batra, N</creatorcontrib><creatorcontrib>Ellis, J. A</creatorcontrib><creatorcontrib>Ferdman, R. D</creatorcontrib><creatorcontrib>Fonseca, E</creatorcontrib><creatorcontrib>Franchini, A</creatorcontrib><creatorcontrib>Gair, J. R</creatorcontrib><creatorcontrib>Garver-Daniels, N</creatorcontrib><creatorcontrib>Gentile, P. A</creatorcontrib><creatorcontrib>Goncharov, B</creatorcontrib><creatorcontrib>Gopakumar, A</creatorcontrib><creatorcontrib>Grießmeier, J. -M</creatorcontrib><creatorcontrib>Gültekin, K</creatorcontrib><creatorcontrib>Grunthal, K</creatorcontrib><creatorcontrib>Hazboun, J. S</creatorcontrib><creatorcontrib>Hisano, S</creatorcontrib><creatorcontrib>Hu, H</creatorcontrib><creatorcontrib>Izquierdo-Villalba, D</creatorcontrib><creatorcontrib>Jawor, J</creatorcontrib><creatorcontrib>Jennings, R. J</creatorcontrib><creatorcontrib>Jessner, A</creatorcontrib><creatorcontrib>Kaiser, A. R</creatorcontrib><creatorcontrib>Kapur, A</creatorcontrib><creatorcontrib>Kelley, L. Z</creatorcontrib><creatorcontrib>Kramer, M</creatorcontrib><creatorcontrib>Kulkarni, A</creatorcontrib><creatorcontrib>Lazio, T. J. W</creatorcontrib><creatorcontrib>Liu, T</creatorcontrib><creatorcontrib>Lommen, A</creatorcontrib><creatorcontrib>Main, R. A</creatorcontrib><creatorcontrib>McKee, J. W</creatorcontrib><creatorcontrib>McLaughlin, M. A</creatorcontrib><creatorcontrib>McMann, N</creatorcontrib><creatorcontrib>Meyers, B. W</creatorcontrib><creatorcontrib>Miles, M</creatorcontrib><creatorcontrib>Mitridate, A</creatorcontrib><creatorcontrib>Nathan, R. S</creatorcontrib><creatorcontrib>Ng, C</creatorcontrib><creatorcontrib>Nice, D. J</creatorcontrib><creatorcontrib>Nobleson, K</creatorcontrib><creatorcontrib>Osłowski, S</creatorcontrib><creatorcontrib>Paladi, A. K</creatorcontrib><creatorcontrib>Parthasarathy, A</creatorcontrib><creatorcontrib>Perera, B. B. P</creatorcontrib><creatorcontrib>Porayko, N. K</creatorcontrib><creatorcontrib>Ransom, S. M</creatorcontrib><creatorcontrib>Reardon, D. J</creatorcontrib><creatorcontrib>Rogers, A. F</creatorcontrib><creatorcontrib>Sardesai, S. C</creatorcontrib><creatorcontrib>Schmiedekamp, C</creatorcontrib><creatorcontrib>Sesana, A</creatorcontrib><creatorcontrib>Shaifullah, G</creatorcontrib><creatorcontrib>Speri, L</creatorcontrib><creatorcontrib>Stairs, I. H</creatorcontrib><creatorcontrib>Sun, J. P</creatorcontrib><creatorcontrib>Susarla, S. C</creatorcontrib><creatorcontrib>Taylor, J</creatorcontrib><creatorcontrib>Taylor, S. R</creatorcontrib><creatorcontrib>Turner, J. E</creatorcontrib><creatorcontrib>Unal, C</creatorcontrib><creatorcontrib>Vallisneri, M</creatorcontrib><creatorcontrib>van der Wateren, E</creatorcontrib><creatorcontrib>van Haasteren, R</creatorcontrib><creatorcontrib>Verbiest, J. P. W</creatorcontrib><creatorcontrib>Wahl, H. M</creatorcontrib><creatorcontrib>Wang, L</creatorcontrib><creatorcontrib>Wayt, K. E</creatorcontrib><creatorcontrib>Wu, Z</creatorcontrib><creatorcontrib>Young, O</creatorcontrib><creatorcontrib>Zhang, L</creatorcontrib><creatorcontrib>Zhu, X. -J</creatorcontrib><collection>arXiv.org</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Antoniadis, J</au><au>Anumarlapudi, A</au><au>Arzoumanian, Z</au><au>Babak, S</au><au>Bailes, M</au><au>Nielsen, A. -S. Bak</au><au>Baker, P. T</au><au>Bassa, C. G</au><au>Berthereau, A</au><au>Bhat, N. D. R</au><au>Blecha, L</au><au>Brazier, A</au><au>Brook, P. R</au><au>Burgay, M</au><au>Burnette, R</au><au>Cameron, A</au><au>Case, R</au><au>Chanlaridis, S</au><au>Charisi, M</au><au>Chatterjee, S</au><au>Chen, Z. -C</au><au>Cohen, T</au><au>Coles, W. A</au><au>Cornish, N. J</au><au>Cromartie, H. T</au><au>Crowter, K</au><au>Dai, S</au><au>Dandapat, S</au><au>DeGan, D</au><au>Dey, L</au><au>Dhanda-Batra, N</au><au>Ellis, J. A</au><au>Ferdman, R. D</au><au>Fonseca, E</au><au>Franchini, A</au><au>Gair, J. R</au><au>Garver-Daniels, N</au><au>Gentile, P. A</au><au>Goncharov, B</au><au>Gopakumar, A</au><au>Grießmeier, J. -M</au><au>Gültekin, K</au><au>Grunthal, K</au><au>Hazboun, J. S</au><au>Hisano, S</au><au>Hu, H</au><au>Izquierdo-Villalba, D</au><au>Jawor, J</au><au>Jennings, R. J</au><au>Jessner, A</au><au>Kaiser, A. R</au><au>Kapur, A</au><au>Kelley, L. Z</au><au>Kramer, M</au><au>Kulkarni, A</au><au>Lazio, T. J. W</au><au>Liu, T</au><au>Lommen, A</au><au>Main, R. A</au><au>McKee, J. W</au><au>McLaughlin, M. A</au><au>McMann, N</au><au>Meyers, B. W</au><au>Miles, M</au><au>Mitridate, A</au><au>Nathan, R. S</au><au>Ng, C</au><au>Nice, D. J</au><au>Nobleson, K</au><au>Osłowski, S</au><au>Paladi, A. K</au><au>Parthasarathy, A</au><au>Perera, B. B. P</au><au>Porayko, N. K</au><au>Ransom, S. M</au><au>Reardon, D. J</au><au>Rogers, A. F</au><au>Sardesai, S. C</au><au>Schmiedekamp, C</au><au>Sesana, A</au><au>Shaifullah, G</au><au>Speri, L</au><au>Stairs, I. H</au><au>Sun, J. P</au><au>Susarla, S. C</au><au>Taylor, J</au><au>Taylor, S. R</au><au>Turner, J. E</au><au>Unal, C</au><au>Vallisneri, M</au><au>van der Wateren, E</au><au>van Haasteren, R</au><au>Verbiest, J. P. W</au><au>Wahl, H. M</au><au>Wang, L</au><au>Wayt, K. E</au><au>Wu, Z</au><au>Young, O</au><au>Zhang, L</au><au>Zhu, X. -J</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Comparing recent PTA results on the nanohertz stochastic gravitational wave background</atitle><date>2023-09-01</date><risdate>2023</risdate><abstract>The Australian, Chinese, European, Indian, and North American pulsar timing array (PTA) collaborations recently reported, at varying levels, evidence for the presence of a nanohertz gravitational wave background (GWB). Given that each PTA made different choices in modeling their data, we perform a comparison of the GWB and individual pulsar noise parameters across the results reported from the PTAs that constitute the International Pulsar Timing Array (IPTA). We show that despite making different modeling choices, there is no significant difference in the GWB parameters that are measured by the different PTAs, agreeing within $1\sigma$. The pulsar noise parameters are also consistent between different PTAs for the majority of the pulsars included in these analyses. We bridge the differences in modeling choices by adopting a standardized noise model for all pulsars and PTAs, finding that under this model there is a reduction in the tension in the pulsar noise parameters. As part of this reanalysis, we "extended" each PTA's data set by adding extra pulsars that were not timed by that PTA. Under these extensions, we find better constraints on the GWB amplitude and a higher signal-to-noise ratio for the Hellings and Downs correlations. These extensions serve as a prelude to the benefits offered by a full combination of data across all pulsars in the IPTA, i.e., the IPTA's Data Release 3, which will involve not just adding in additional pulsars, but also including data from all three PTAs where any given pulsar is timed by more than as single PTA.</abstract><doi>10.48550/arxiv.2309.00693</doi><oa>free_for_read</oa></addata></record>
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subjects Physics - General Relativity and Quantum Cosmology
Physics - High Energy Astrophysical Phenomena
title Comparing recent PTA results on the nanohertz stochastic gravitational wave background
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