TY - JOUR
T1 - The NANOGrav 15 yr Dataset
T2 - A Case Study for Simplified Dispersion Measure Modeling for PSR J1455−3330 and the Impact on Gravitational Wave Sensitivity
AU - Lam, Michael T.
AU - Kaplan, David L.
AU - Agazie, Gabriella
AU - Anumarlapudi, Akash
AU - Archibald, Anne M.
AU - Arzoumanian, Zaven
AU - Baker, Paul T.
AU - Brook, Paul R.
AU - Combs, Olivia A.
AU - Cromartie, H. Thankful
AU - Crowter, Kathryn
AU - DeCesar, Megan E.
AU - Demorest, Paul B.
AU - Dolch, Timothy
AU - Ferrara, Elizabeth C.
AU - Fiore, William
AU - Fonseca, Emmanuel
AU - Freedman, Gabriel E.
AU - Garver-Daniels, Nate
AU - Gentile, Peter A.
AU - Glaser, Joseph
AU - Good, Deborah C.
AU - Hazboun, Jeffrey S.
AU - Jennings, Ross J.
AU - Jones, Megan L.
AU - Kerr, Matthew
AU - Lorimer, Duncan R.
AU - Luo, Jing
AU - Lynch, Ryan S.
AU - McEwen, Alexander
AU - McLaughlin, Maura A.
AU - McMann, Natasha
AU - Meyers, Bradley W.
AU - Ng, Cherry
AU - Nice, David J.
AU - Pennucci, Timothy T.
AU - Perera, Benetge B.P.
AU - Pol, Nihan S.
AU - Radovan, Henri A.
AU - Ransom, Scott M.
AU - Ray, Paul S.
AU - Schmiedekamp, Ann
AU - Schmiedekamp, Carl
AU - Shapiro-Albert, Brent J.
AU - Simon, Joseph
AU - Stairs, Ingrid H.
AU - Stovall, Kevin
AU - Susobhanan, Abhimanyu
AU - Swiggum, Joseph K.
AU - Wahl, Haley M.
N1 - Publisher Copyright:
© 2026. The Author(s). Published by the American Astronomical Society. Original content from this work may be used under the terms of the https://creativecommons.org/licenses/by/4.0/. Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI.
PY - 2026/6/10
Y1 - 2026/6/10
N2 - Evidence for a low-frequency gravitational-wave background using pulsar timing arrays has generated recent interest in its underlying contributing sources. However, multiple investigations have seen that the significance of the evidence does not change with the choice of pulsar modeling techniques, but the resulting parameters from the gravitational wave searches do. PSR J1455−3330 is one of the longest-observed pulsars in the array monitored by the North American Nanohertz Observatory for Gravitational Waves (NANOGrav), but showed no evidence for long-timescale red noise, either intrinsic or the common signal found among many pulsars in the array. In this work, we argue that NANOGrav’s piecewise-constant function used to model variations in radio-frequency-dependent dispersive delay should not be used for this pulsar, and a much simpler physical model of a fixed solar wind density plus a linear or quadratic trend in dispersion measure is preferred. When the original model is replaced, (i) the pulsar’s timing parallax signal changes from an upper limit to a significant detection, (ii) red noise becomes significant, and (iii) the red noise is consistent with the common signal found for the other pulsars. Neither of these signals is radio-frequency dependent. While the same physical motivation will not apply to many of the pulsars currently used in pulsar timing arrays, we argue for careful, physically motivated timing and noise modeling of pulsars used in precision timing experiments.
AB - Evidence for a low-frequency gravitational-wave background using pulsar timing arrays has generated recent interest in its underlying contributing sources. However, multiple investigations have seen that the significance of the evidence does not change with the choice of pulsar modeling techniques, but the resulting parameters from the gravitational wave searches do. PSR J1455−3330 is one of the longest-observed pulsars in the array monitored by the North American Nanohertz Observatory for Gravitational Waves (NANOGrav), but showed no evidence for long-timescale red noise, either intrinsic or the common signal found among many pulsars in the array. In this work, we argue that NANOGrav’s piecewise-constant function used to model variations in radio-frequency-dependent dispersive delay should not be used for this pulsar, and a much simpler physical model of a fixed solar wind density plus a linear or quadratic trend in dispersion measure is preferred. When the original model is replaced, (i) the pulsar’s timing parallax signal changes from an upper limit to a significant detection, (ii) red noise becomes significant, and (iii) the red noise is consistent with the common signal found for the other pulsars. Neither of these signals is radio-frequency dependent. While the same physical motivation will not apply to many of the pulsars currently used in pulsar timing arrays, we argue for careful, physically motivated timing and noise modeling of pulsars used in precision timing experiments.
KW - Gravitational wave astronomy (675)
KW - Interstellar medium (847)
KW - Millisecond pulsars (1062)
UR - https://www.scopus.com/pages/publications/105041297226
U2 - 10.3847/1538-4357/ae6c1c
DO - 10.3847/1538-4357/ae6c1c
M3 - Article
AN - SCOPUS:105041297226
SN - 0004-637X
VL - 1004
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 1
M1 - 118
ER -