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From U(1)×U(1) symmetry breaking to Majoron cosmology: Insights from NANOGrav 15-year data

Tathagata Ghosh*, Kousik Loho†, and Sudip Manna‡

  • Regional Centre for Accelerator based Particle Physics, Harish-Chandra Research Institute, A CI of Homi Bhabha National Institute, Chhatnag Road, Jhunsi, Prayagraj 211019, India

  • *Contact author: tathagataghosh@hri.res.in
  • †Contact author: kousikloho@hri.res.in
  • ‡Contact author: sudipmanna@hri.res.in

Phys. Rev. D 113, 043036 – Published 17 February, 2026

DOI: https://doi.org/10.1103/gd2q-qdhg

Abstract

We study the cosmology of a modified Majoron model motivated by the need to protect a global U(1) symmetry from gravity-induced hard explicit breaking (by d≤4 operators) at the Planck scale. The model extends the standard model by introducing a gauged U(1)B−L and an approximate global U(1) symmetry, each spontaneously broken by a corresponding complex scalar singlet. This setup gives rise to a network of effectively global and local cosmic strings, whose stochastic gravitational wave signals can jointly account for the spectrum observed by NANOGrav collaboration, particularly for Majoron masses mχ<10−23  eV. Although the fit is not as strong as that from supermassive black hole mergers, the model still provides an alternative explanation rooted in high-energy physics. The Majoron mass induces an infrared cutoff in the gravitational wave spectrum, and we examine how this effect shapes the fit to the NANOGrav data. The model also generates light neutrino masses via the seesaw mechanism and avoids cosmological constraints from ΔNeff, cosmic microwave background (CMB) anisotropies, and isocurvature fluctuations. Although the Majoron can contribute to dark matter through thermal, coherent oscillation, and string-induced production mechanisms, its relic abundance remains subdominant in the NANOGrav-compatible region. In contrast, the measured dark matter relic density is achievable at higher mχ, though at the cost of tension with cosmological bounds. If the NANOGrav fits are viewed as constraints, given their comparatively lower Bayes factors, they yield bounds that are significantly stronger than those imposed by the CMB and other cosmological data.

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