The NANOGrav 15 yr Data Set: Chromatic Gaussian Process Noise Models for Six Pulsars

Author:

Larsen BjornORCID,Mingarelli Chiara M. F.ORCID,Hazboun Jeffrey S.ORCID,Chalumeau AurélienORCID,Good Deborah C.ORCID,Simon JosephORCID,Agazie GabriellaORCID,Anumarlapudi AkashORCID,Archibald Anne M.ORCID,Arzoumanian Zaven,Baker Paul T.ORCID,Brook Paul R.ORCID,Cromartie H. ThankfulORCID,Crowter KathrynORCID,DeCesar Megan E.ORCID,Demorest Paul B.ORCID,Dolch TimothyORCID,Ferrara Elizabeth C.ORCID,Fiore WilliamORCID,Fonseca EmmanuelORCID,Freedman Gabriel E.ORCID,Garver-Daniels NateORCID,Gentile Peter A.ORCID,Glaser JosephORCID,Jennings Ross J.ORCID,Jones Megan L.ORCID,Kaplan David L.ORCID,Kerr MatthewORCID,Lam Michael T.ORCID,Lorimer Duncan R.ORCID,Luo JingORCID,Lynch Ryan S.ORCID,McEwen AlexanderORCID,McLaughlin Maura A.ORCID,McMann NatashaORCID,Meyers Bradley W.ORCID,Ng CherryORCID,Nice David J.ORCID,Pennucci Timothy T.ORCID,Perera Benetge B. P.ORCID,Pol Nihan S.ORCID,Radovan Henri A.ORCID,Ransom Scott M.ORCID,Ray Paul S.ORCID,Schmiedekamp AnnORCID,Schmiedekamp CarlORCID,Shapiro-Albert Brent J.ORCID,Stairs Ingrid H.ORCID,Stovall KevinORCID,Susobhanan AbhimanyuORCID,Swiggum Joseph K.ORCID,Wahl Haley M.ORCID,Champion David J.ORCID,Cognard IsmaëlORCID,Guillemot LucasORCID,Hu HuanchenORCID,Keith Michael J.ORCID,Liu KuoORCID,McKee James W.ORCID,Parthasarathy AdityaORCID,Perrodin DelphineORCID,Possenti AndreaORCID,Shaifullah Golam M.ORCID,Theureau GillesORCID

Abstract

Abstract Pulsar timing arrays (PTAs) are designed to detect low-frequency gravitational waves (GWs). GWs induce achromatic signals in PTA data, meaning that the timing delays do not depend on radio frequency. However, pulse arrival times are also affected by radio-frequency-dependent “chromatic” noise from sources such as dispersion measure (DM) and scattering delay variations. Furthermore, the characterization of GW signals may be influenced by the choice of chromatic noise model for each pulsar. To better understand this effect, we assess if and how different chromatic noise models affect the achromatic noise properties in each pulsar. The models we compare include existing DM models used by the North American Nanohertz Observatory for Gravitational waves (NANOGrav) and noise models used for the European PTA Data Release 2 (EPTA DR2). We perform this comparison using a subsample of six pulsars from the NANOGrav 15 yr data set, selecting the same six pulsars as from the EPTA DR2 six-pulsar data set. We find that the choice of chromatic noise model noticeably affects the achromatic noise properties of several pulsars. This is most dramatic for PSR J1713+0747, where the amplitude of its achromatic red noise lowers from log 10 A RN = 14.1 0.1 + 0.1 to 14.7 0.5 + 0.3 , and the spectral index broadens from γ RN = 2.6 0.4 + 0.5 to γ RN = 3.5 0.9 + 1.2 . We also compare each pulsar's noise properties with those inferred from the EPTA DR2, using the same models. From the discrepancies, we identify potential areas where the noise models could be improved. These results highlight the potential for custom chromatic noise models to improve PTA sensitivity to GWs.

Funder

National Science Foundation

National Aeronautics and Space Administration

H2020 Excellent science

UKRI ∣ STFC ∣ Central Laser Facility, Science and Technology Facilities Council

UBC ∣ University of British Columbia Graduate School

Agence Nationale de la Recherche

UKRI ∣ Science and Technology Facilities Council

Publisher

American Astronomical Society

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