pith. sign in

arxiv: 2605.27519 · v1 · pith:FX5JPGBHnew · submitted 2026-05-26 · ✦ hep-ph · astro-ph.CO· hep-ex· hep-th

Probing Dynamical Inverse Seesaw with Low-frequency Gravitational Waves

Pith reviewed 2026-06-29 16:39 UTC · model grok-4.3

classification ✦ hep-ph astro-ph.COhep-exhep-th
keywords inverse seesawgravitational wavesphase transitionneutrino massespulsar timing arraysheavy neutral leptonslepton number violation
0
0 comments X

The pith

Making the inverse seesaw dynamical generates a low-scale phase transition whose gravitational waves fall in the pulsar timing array band.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper examines the inverse seesaw for light neutrino masses when the lepton-number violating Majorana mass term is promoted to a dynamical scalar field. This dynamical origin places the transition scale in the sub-MeV range, producing a first-order phase transition whose stochastic gravitational wave spectrum peaks at frequencies accessible to pulsar timing arrays. The same setup remains sensitive to regions of very small active-sterile mixing that are difficult for collider or beam-dump experiments to reach, creating a potential complementarity between gravitational-wave and particle-physics searches.

Core claim

Dynamical generation of the lepton-number violating term in the inverse seesaw naturally produces a low-scale first-order phase transition whose resulting gravitational-wave background lies within the frequency window currently probed by pulsar timing arrays, while also opening sensitivity to small active-sterile mixing angles.

What carries the argument

Dynamical lepton-number violating scalar whose vacuum expectation value sets the sub-MeV Majorana mass and triggers a first-order phase transition.

If this is right

  • Detection of a nanohertz gravitational-wave background would fix the lepton-number violating scale to lie near the sub-MeV range.
  • The gravitational-wave signal remains visible even when active-sterile mixing is too small for heavy-neutral-lepton searches at colliders or fixed-target experiments.
  • The same phase transition can generate a baryon asymmetry through leptogenesis at the same low scale.
  • Complementary limits from big-bang nucleosynthesis and cosmic microwave background measurements would further restrict the allowed transition temperature.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • If the gravitational-wave signal is observed, future interferometers at higher frequencies could search for the same transition's high-frequency tail.
  • The dynamical scalar could couple to dark matter and alter the predicted relic density in ways testable by direct-detection experiments.
  • Similar dynamical mechanisms could be applied to other low-scale neutrino-mass models to predict additional gravitational-wave targets.

Load-bearing premise

The lepton-number violating scale stays below a few MeV and its dynamical realization produces a first-order phase transition whose gravitational-wave spectrum reaches the pulsar timing array frequency band.

What would settle it

A null result for a stochastic gravitational-wave background in the nanohertz to microhertz range, after subtracting known astrophysical sources, would exclude the sub-MeV dynamical inverse-seesaw parameter space that produces an observable signal.

Figures

Figures reproduced from arXiv: 2605.27519 by Debasish Borah, Indrajit Saha, Narendra Sahu, Partha Kumar Paul, Sounak Dutta.

Figure 1
Figure 1. Figure 1: FIG. 1. The effective potential as a function of the field value, [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. The gravitational wave energy density spectrum [PITH_FULL_IMAGE:figures/full_fig_p002_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Exclusion limits on active-sterile mixing strength ( [PITH_FULL_IMAGE:figures/full_fig_p003_3.png] view at source ↗
read the original abstract

We study the possibility of probing the dynamical inverse seesaw mechanism for the origin of light neutrino masses via the detection of stochastic gravitational waves (GW) in the low-frequency regime currently being probed by pulsar timing arrays. As the lepton number-violating term in inverse seesaw typically remains in the sub-MeV ballpark, its dynamical origin naturally brings the possibility of a low-scale first-order phase transition, which can be probed at low-frequency GW experiments. We also find interesting complementarity with heavy neutral lepton searches, as GW experiments remain sensitive to parameter space with small active-sterile mixing, which is out of reach for most particle physics experiments.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 0 minor

Summary. The manuscript claims that the dynamical inverse seesaw mechanism, in which the lepton-number-violating parameter μ is generated by a scalar field, naturally produces a low-scale first-order phase transition whose stochastic gravitational-wave spectrum falls in the nHz band accessible to pulsar timing arrays. It further asserts complementarity with heavy neutral lepton searches, since GW signals remain sensitive to regions of small active-sterile mixing that are out of reach for most particle-physics experiments.

Significance. If the central claim is substantiated, the work would identify a new cosmological probe of neutrino-mass generation that exploits the sub-MeV scale of μ to predict a phase transition at T ~ 100 keV. This would furnish falsifiable predictions for PTA experiments and cover parameter space complementary to direct HNL searches. No machine-checked proofs, reproducible code, or parameter-free derivations are presented.

major comments (1)
  1. [Abstract] The assertion in the abstract that the dynamical origin of μ 'naturally' yields a first-order phase transition with GW peak frequency in the PTA window is not supported by any derivation of the scalar potential, the finite-temperature effective potential, or the nucleation parameters α and β/H. Without these quantities the frequency match and first-order character remain unverified assumptions rather than demonstrated results.

Simulated Author's Rebuttal

1 responses · 1 unresolved

We thank the referee for the careful reading and the constructive comment on the abstract. We address it below.

read point-by-point responses
  1. Referee: [Abstract] The assertion in the abstract that the dynamical origin of μ 'naturally' yields a first-order phase transition with GW peak frequency in the PTA window is not supported by any derivation of the scalar potential, the finite-temperature effective potential, or the nucleation parameters α and β/H. Without these quantities the frequency match and first-order character remain unverified assumptions rather than demonstrated results.

    Authors: We agree with the referee that the current manuscript does not contain explicit derivations of the scalar potential, the finite-temperature effective potential, or the nucleation parameters α and β/H. The abstract statement relies on the sub-MeV scale of the lepton-number-violating parameter μ implying a low-scale transition, but this remains an assumption rather than a calculated result. We will revise the abstract to replace 'naturally' with 'suggests the possibility of' and will add a clarifying paragraph in the introduction or conclusions noting the assumptions and the need for dedicated follow-up calculations of the phase-transition parameters. revision: yes

standing simulated objections not resolved
  • The manuscript does not contain the requested derivations of the scalar potential, finite-temperature effective potential, or nucleation parameters.

Circularity Check

0 steps flagged

No significant circularity detected

full rationale

The paper asserts that dynamical generation of the sub-MeV LNV term in inverse seesaw 'naturally' produces a low-scale FOPT whose GW spectrum falls in the PTA band, with complementarity to HNL searches. No equations, parameter fits, or self-citations are exhibited in the provided text that reduce any claimed prediction or first-principles result to the inputs by construction (e.g., no fitted scale renamed as prediction, no uniqueness theorem imported from the same authors, no ansatz smuggled via prior work). The central claim is presented as an exploratory possibility rather than a derived quantity forced by self-reference or redefinition, rendering the derivation self-contained against the enumerated circularity patterns.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Only abstract available; no free parameters, axioms, or invented entities can be extracted or audited.

pith-pipeline@v0.9.1-grok · 5652 in / 1207 out tokens · 42046 ms · 2026-06-29T16:39:16.772277+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

128 extracted references · 95 canonical work pages · 49 internal anchors

  1. [1]

    We study the possibility of a MeV scale first-order phase transition (FOPT) driven by the singlet scalar fieldϕ

    Since we generate the lepton number violating term of inverse see- saw dynamically, a low scale realization of this seesaw naturally requires a MeV scale symmetry breaking driven by the scalar fieldϕ. We study the possibility of a MeV scale first-order phase transition (FOPT) driven by the singlet scalar fieldϕ. The scale of symmetry breaking or theµterm ...

  2. [2]

    Navaset al.(Particle Data Group), Review of particle physics, Phys

    S. Navaset al.(Particle Data Group), Review of particle physics, Phys. Rev. D110, 030001 (2024)

  3. [3]

    Minkowski,µ→eγat a Rate of One Out of 10 9 Muon Decays?, Phys

    P. Minkowski,µ→eγat a Rate of One Out of 10 9 Muon Decays?, Phys. Lett.B67, 421 (1977)

  4. [4]

    Complex Spinors and Unified Theories

    M. Gell-Mann, P. Ramond, and R. Slansky, Complex Spinors and Unified Theories,Supergravity Workshop Stony Brook, New York, September 27-28, 1979, Conf. Proc.C790927, 315 (1979), arXiv:1306.4669 [hep-th]

  5. [5]

    R. N. Mohapatra and G. Senjanovic, Neutrino Mass and Spontaneous Parity Violation, Phys. Rev. Lett.44, 912 (1980)

  6. [6]

    Sawada and A

    O. Sawada and A. Sugamoto, eds.,Proceedings: Work- shop on the Unified Theories and the Baryon Number in the Universe: Tsukuba, Japan, February 13-14, 1979 (Natl.Lab.High Energy Phys., Tsukuba, Japan, 1979)

  7. [7]

    Yanagida, Horizontal Symmetry and Masses of Neu- trinos, Prog

    T. Yanagida, Horizontal Symmetry and Masses of Neu- trinos, Prog. Theor. Phys.64, 1103 (1980)

  8. [8]

    Schechter and J

    J. Schechter and J. W. F. Valle, Neutrino Masses in SU(2) x U(1) Theories, Phys. Rev.D22, 2227 (1980)

  9. [9]

    R. N. Mohapatra and G. Senjanovic, Neutrino Masses and Mixings in Gauge Models with Spontaneous Parity Violation, Phys. Rev.D23, 165 (1981)

  10. [10]

    Schechter and J

    J. Schechter and J. W. F. Valle, Neutrino Decay and Spontaneous Violation of Lepton Number, Phys. Rev. D25, 774 (1982)

  11. [11]

    Wetterich, Neutrino Masses and the Scale of B-L Violation, Nucl

    C. Wetterich, Neutrino Masses and the Scale of B-L Violation, Nucl. Phys.B187, 343 (1981)

  12. [12]

    Lazarides, Q

    G. Lazarides, Q. Shafi, and C. Wetterich, Proton Life- time and Fermion Masses in an SO(10) Model, Nucl. Phys.B181, 287 (1981)

  13. [13]

    Unified explanation of the Solar and Atmospheric neutrino Puzzles in a minimal supersymmetric SO(10) model

    B. Brahmachari and R. N. Mohapatra, Unified expla- nation of the solar and atmospheric neutrino puzzles in 7 a minimal supersymmetric SO(10) model, Phys. Rev. D58, 015001 (1998), arXiv:hep-ph/9710371 [hep-ph]

  14. [14]

    R. Foot, H. Lew, X. G. He, and G. C. Joshi, Seesaw Neutrino Masses Induced by a Triplet of Leptons, Z. Phys.C44, 441 (1989)

  15. [15]

    A possible symmetry of the $\nu$MSM

    M. Shaposhnikov, A Possible symmetry of the nuMSM, Nucl. Phys. B763, 49 (2007), arXiv:hep-ph/0605047

  16. [16]

    Right-Handed Neutrinos at LHC and the Mechanism of Neutrino Mass Generation

    J. Kersten and A. Y. Smirnov, Right-Handed Neutri- nos at CERN LHC and the Mechanism of Neutrino Mass Generation, Phys. Rev. D76, 073005 (2007), arXiv:0705.3221 [hep-ph]

  17. [17]

    Equivalence between massless neutrinos and lepton number conservation in fermionic singlet extensions of the Standard Model

    K. Moffat, S. Pascoli, and C. Weiland, Equivalence be- tween massless neutrinos and lepton number conser- vation in fermionic singlet extensions of the Standard Model, (2017), arXiv:1712.07611 [hep-ph]

  18. [18]

    Klari´ c, M

    J. Klari´ c, M. Shaposhnikov, and I. Timiryasov, Uniting Low-Scale Leptogenesis Mechanisms, Phys. Rev. Lett. 127, 111802 (2021), arXiv:2008.13771 [hep-ph]

  19. [19]

    Drewes, Y

    M. Drewes, Y. Georis, and J. Klari´ c, Mapping the Vi- able Parameter Space for Testable Leptogenesis, Phys. Rev. Lett.128, 051801 (2022), arXiv:2106.16226 [hep- ph]

  20. [20]

    Hernandez, J

    P. Hernandez, J. Lopez-Pavon, N. Rius, and S. Sandner, Bounds on right-handed neutrino parameters from ob- servable leptogenesis, JHEP12, 012, arXiv:2207.01651 [hep-ph]

  21. [21]

    A. M. Abdullahiet al., The present and future status of heavy neutral leptons, J. Phys. G50, 020501 (2023), arXiv:2203.08039 [hep-ph]

  22. [22]

    R. N. Mohapatra, Mechanism for Understanding Small Neutrino Mass in Superstring Theories, Phys. Rev. Lett. 56, 561 (1986)

  23. [23]

    R. N. Mohapatra and J. W. F. Valle, Neutrino Mass and Baryon Number Nonconservation in Superstring Models,Sixty years of double beta decay: From nuclear physics to beyond standard model particle physics, Phys. Rev.D34, 1642 (1986), [,235(1986)]

  24. [24]

    M. C. Gonzalez-Garcia and J. W. F. Valle, Fast De- caying Neutrinos and Observable Flavor Violation in a New Class of Majoron Models, Phys. Lett. B216, 360 (1989)

  25. [25]

    Bernabeu, A

    J. Bernabeu, A. Santamaria, J. Vidal, A. Mendez, and J. W. F. Valle, Lepton Flavor Nonconservation at High- Energies in a Superstring Inspired Standard Model, Phys. Lett. B187, 303 (1987)

  26. [26]

    M. B. Gavela, T. Hambye, D. Hernandez, and P. Her- nandez, Minimal Flavour Seesaw Models, JHEP09, 038, arXiv:0906.1461 [hep-ph]

  27. [27]

    M. E. Catano, R. Martinez, and F. Ochoa, Neutrino masses in a 331 model with right-handed neutrinos with- out doubly charged Higgs bosons via inverse and dou- ble seesaw mechanisms, Phys. Rev.D86, 073015 (2012), arXiv:1206.1966 [hep-ph]

  28. [28]

    J. A. Dror, T. Hiramatsu, K. Kohri, H. Murayama, and G. White, Testing the Seesaw Mechanism and Leptoge- nesis with Gravitational Waves, Phys. Rev. Lett.124, 041804 (2020), arXiv:1908.03227 [hep-ph]

  29. [29]

    Blasi, V

    S. Blasi, V. Brdar, and K. Schmitz, Fingerprint of low-scale leptogenesis in the primordial gravitational- wave spectrum, Phys. Rev. Res.2, 043321 (2020), arXiv:2004.02889 [hep-ph]

  30. [30]

    Fornal and B

    B. Fornal and B. Shams Es Haghi, Baryon and Lep- ton Number Violation from Gravitational Waves, Phys. Rev. D102, 115037 (2020), arXiv:2008.05111 [hep-ph]

  31. [31]

    Samanta and S

    R. Samanta and S. Datta, Gravitational wave com- plementarity and impact of NANOGrav data on gravitational leptogenesis: cosmic strings, (2020), arXiv:2009.13452 [hep-ph]

  32. [32]

    Barman, D

    B. Barman, D. Borah, A. Dasgupta, and A. Ghoshal, Probing High Scale Dirac Leptogenesis via Grav- itational Waves from Domain Walls, (2022), arXiv:2205.03422 [hep-ph]

  33. [33]

    Huang and K.-P

    P. Huang and K.-P. Xie, Leptogenesis triggered by a first-order phase transition, (2022), arXiv:2206.04691 [hep-ph]

  34. [34]

    Dasgupta, P

    A. Dasgupta, P. S. B. Dev, A. Ghoshal, and A. Mazum- dar, Gravitational Wave Pathway to Testable Leptoge- nesis, (2022), arXiv:2206.07032 [hep-ph]

  35. [35]

    Probing the seesaw scale with gravitational waves

    N. Okada and O. Seto, Probing the seesaw scale with gravitational waves, Phys. Rev. D98, 063532 (2018), arXiv:1807.00336 [hep-ph]

  36. [36]

    Gravitational waves from the minimal gauged $U(1)_{B-L}$ model

    T. Hasegawa, N. Okada, and O. Seto, Gravitational waves from the minimal gaugedU(1) B−L model, Phys. Rev. D99, 095039 (2019), arXiv:1904.03020 [hep-ph]

  37. [37]

    Borah, A

    D. Borah, A. Dasgupta, and I. Saha, Leptogene- sis and dark matter through relativistic bubble walls with observable gravitational waves, JHEP11, 136, arXiv:2207.14226 [hep-ph]

  38. [38]

    Borah, S

    D. Borah, S. Jyoti Das, and R. Roshan, Probing high scale seesaw and PBH generated dark matter via gravitational waves with multiple tilts, (2022), arXiv:2208.04965 [hep-ph]

  39. [39]

    Barman, D

    B. Barman, D. Borah, S. Jyoti Das, and I. Saha, Scale of Dirac leptogenesis and left-right symmetry in the light of recent PTA results, JCAP10, 053, arXiv:2307.00656 [hep-ph]

  40. [40]

    Borah, A

    D. Borah, A. Dasgupta, and I. Saha, LIGO-VIRGO constraints on dark matter and leptogenesis triggered by a first order phase transition at high scale, (2023), arXiv:2304.08888 [hep-ph]

  41. [41]

    Gravitational waves from seesaw assisted collapsing domain walls

    D. Borah and I. Saha, Gravitational waves from seesaw assisted collapsing domain walls, (2025), arXiv:2512.22339 [hep-ph]

  42. [42]

    Borah, P

    D. Borah, P. K. Paul, and N. Sahu, Can Dirac neu- trinos destabilizeZ 2 domain wall network?, (2026), arXiv:2602.07380 [hep-ph]

  43. [43]

    A review of gravitational waves from cosmic domain walls

    K. Saikawa, A review of gravitational waves from cosmic domain walls, Universe3, 40 (2017), arXiv:1703.02576 [hep-ph]

  44. [44]

    Roshan and G

    R. Roshan and G. White, Using gravitational waves to see the first second of the Universe, (2024), arXiv:2401.04388 [hep-ph]

  45. [45]

    Bhattacharya, N

    S. Bhattacharya, N. Mondal, R. Roshan, and D. Vat- syayan, Leptogenesis, dark matter and gravitational waves from discrete symmetry breaking, JCAP06, 029, arXiv:2312.15053 [hep-ph]

  46. [46]

    Blasi, A

    S. Blasi, A. Mariotti, A. Rase, A. Sevrin, and K. Tur- bang, Friction on ALP domain walls and gravitational waves, JCAP04, 008, arXiv:2210.14246 [hep-ph]

  47. [47]

    Blasi, A

    S. Blasi, A. Mariotti, A. Rase, and A. Sevrin, Axionic domain walls at Pulsar Timing Arrays: QCD bias and particle friction, JHEP11, 169, arXiv:2306.17830 [hep- ph]

  48. [48]

    Borah, N

    D. Borah, N. Das, and R. Roshan, Observable gravi- tational waves and ∆Neff with global lepton number symmetry and dark matter, Phys. Rev. D110, 075042 (2024), arXiv:2406.04404 [hep-ph]

  49. [49]

    P. K. Paul, N. Sahu, and P. Shukla, Thermal lepto- 8 genesis, dark matter, and gravitational waves from an extended canonical seesaw scenario, Phys. Rev. D112, 015032 (2025), arXiv:2409.08828 [hep-ph]

  50. [50]

    Z. A. Borboruah, D. Borah, L. Malhotra, and U. Patel, Minimal Dirac seesaw dark matter, Phys. Rev. D112, 015022 (2025), arXiv:2412.12267 [hep-ph]

  51. [51]

    The NANOGrav 15-year Data Set: Evidence for a Gravitational-Wave Background

    G. Agazieet al.(NANOGrav), The NANOGrav 15 yr Data Set: Evidence for a Gravitational-wave Background, Astrophys. J. Lett.951, L8 (2023), arXiv:2306.16213 [astro-ph.HE]

  52. [52]

    The second data release from the European Pulsar Timing Array III. Search for gravitational wave signals

    J. Antoniadiset al.(EPTA, InPTA:), The second data release from the European Pulsar Timing Array - III. Search for gravitational wave signals, Astron. Astro- phys.678, A50 (2023), arXiv:2306.16214 [astro-ph.HE]

  53. [53]

    D. J. Reardonet al., Search for an Isotropic Gravitational-wave Background with the Parkes Pul- sar Timing Array, Astrophys. J. Lett.951, L6 (2023), arXiv:2306.16215 [astro-ph.HE]

  54. [54]

    Agazieet al.(NANOGrav), The NANOGrav 15 yr Data Set: Detector Characterization and Noise Budget, Astrophys

    G. Agazieet al.(NANOGrav), The NANOGrav 15 yr Data Set: Detector Characterization and Noise Budget, Astrophys. J. Lett.951, L10 (2023), arXiv:2306.16218 [astro-ph.HE]

  55. [55]

    Garcia-Bellido, H

    J. Garcia-Bellido, H. Murayama, and G. White, Explor- ing the Early Universe with Gaia and THEIA, (2021), arXiv:2104.04778 [hep-ph]

  56. [56]

    Unveiling the Gravitational Universe at \mu-Hz Frequencies

    A. Sesanaet al., Unveiling the gravitational universe atµ-Hz frequencies, Exper. Astron.51, 1333 (2021), arXiv:1908.11391 [astro-ph.IM]

  57. [57]

    Weltmanet al., Fundamental physics with the Square Kilometre Array, Publ

    A. Weltmanet al., Fundamental physics with the Square Kilometre Array, Publ. Astron. Soc. Austral.37, e002 (2020), arXiv:1810.02680 [astro-ph.CO]

  58. [58]

    A. M. Sirunyanet al.(CMS), Search for heavy neutral leptons in events with three charged leptons in proton- proton collisions at √s= 13 TeV, Phys. Rev. Lett.120, 221801 (2018), arXiv:1802.02965 [hep-ex]

  59. [59]

    A. M. Sirunyanet al.(CMS), Search for heavy Majo- rana neutrinos in same-sign dilepton channels in proton- proton collisions at √s= 13 TeV, JHEP01, 122, arXiv:1806.10905 [hep-ex]

  60. [60]

    G. Aadet al.(ATLAS), Search for heavy neutral leptons in decays ofWbosons produced in 13 TeVppcollisions using prompt and displaced signatures with the ATLAS detector, JHEP10, 265, arXiv:1905.09787 [hep-ex]

  61. [61]

    Search for heavy Majorana neutrinos with the ATLAS detector in pp collisions at $\sqrt{s} = 8$ TeV

    G. Aadet al.(ATLAS), Search for heavy Majorana neutrinos with the ATLAS detector in pp collisions at√s= 8 TeV, JHEP07, 162, arXiv:1506.06020 [hep-ex]

  62. [62]

    Abreuet al.(DELPHI), Search for neutral heavy lep- tons produced in Z decays, Z

    P. Abreuet al.(DELPHI), Search for neutral heavy lep- tons produced in Z decays, Z. Phys. C74, 57 (1997), [Erratum: Z.Phys.C 75, 580 (1997)]

  63. [63]

    Adrianiet al.(L3), Search for isosinglet neutral heavy leptons in Z0 decays, Phys

    O. Adrianiet al.(L3), Search for isosinglet neutral heavy leptons in Z0 decays, Phys. Lett. B295, 371 (1992)

  64. [64]

    Search for Heavy Isosinglet Neutrino in e+e- Annihilation at LEP

    P. Achardet al.(L3), Search for heavy isosinglet neu- trino ine +e− annihilation at LEP, Phys. Lett. B517, 67 (2001), arXiv:hep-ex/0107014

  65. [65]

    Search for heavy neutrinos at Belle

    D. Liventsevet al.(Belle), Search for heavy neutrinos at Belle, Phys. Rev. D87, 071102 (2013), [Erratum: Phys.Rev.D 95, 099903 (2017)], arXiv:1301.1105 [hep- ex]

  66. [66]

    Bergsmaet al.(CHARM), A Search for Decays of Heavy Neutrinos in the Mass Range 0.5-GeV to 2.8- GeV, Phys

    F. Bergsmaet al.(CHARM), A Search for Decays of Heavy Neutrinos in the Mass Range 0.5-GeV to 2.8- GeV, Phys. Lett. B166, 473 (1986)

  67. [67]

    Vilainet al.(CHARM II), Search for heavy isosinglet neutrinos, Phys

    P. Vilainet al.(CHARM II), Search for heavy isosinglet neutrinos, Phys. Lett. B343, 453 (1995)

  68. [68]

    Bernardiet al., FURTHER LIMITS ON HEAVY NEUTRINO COUPLINGS, Phys

    G. Bernardiet al., FURTHER LIMITS ON HEAVY NEUTRINO COUPLINGS, Phys. Lett. B203, 332 (1988)

  69. [69]

    Barouki, G

    R. Barouki, G. Marocco, and S. Sarkar, Blast from the past II: Constraints on heavy neutral leptons from the BEBC WA66 beam dump experiment, SciPost Phys.13, 118 (2022), arXiv:2208.00416 [hep-ph]

  70. [70]

    Badieret al.(NA3), Mass and Lifetime Limits on New Longlived Particles in 300-GeV/cπ − Interactions, Z

    J. Badieret al.(NA3), Mass and Lifetime Limits on New Longlived Particles in 300-GeV/cπ − Interactions, Z. Phys. C31, 21 (1986)

  71. [71]

    Cortina Gilet al.(NA62), Search for heavy neu- tral lepton production in K+ decays to positrons, Phys

    E. Cortina Gilet al.(NA62), Search for heavy neu- tral lepton production in K+ decays to positrons, Phys. Lett. B807, 135599 (2020), arXiv:2005.09575 [hep-ex]

  72. [72]

    Search for heavy Majorana neutrino in lepton number violating decays of D-> K pi e+ e+

    M. Ablikimet al.(BESIII), Search for heavy Majo- rana neutrino in lepton number violating decays of D→Kπe +e+, Phys. Rev. D99, 112002 (2019), arXiv:1902.02450 [hep-ex]

  73. [73]

    Non-Unitarity, sterile neutrinos, and Non-Standard neutrino Interactions

    M. Blennow, P. Coloma, E. Fernandez-Martinez, J. Hernandez-Garcia, and J. Lopez-Pavon, Non- Unitarity, sterile neutrinos, and Non-Standard neutrino Interactions, JHEP04, 153, arXiv:1609.08637 [hep-ph]

  74. [74]

    Effects of new leptons in Electroweak Precision Data

    F. del Aguila, J. de Blas, and M. Perez-Victoria, Effects of new leptons in Electroweak Precision Data, Phys. Rev.D78, 013010 (2008), arXiv:0803.4008 [hep-ph]

  75. [75]

    Electroweak limits on physics beyond the Standard Model

    J. de Blas, Electroweak limits on physics beyond the Standard Model, EPJ Web Conf.60, 19008 (2013), arXiv:1307.6173 [hep-ph]

  76. [76]

    Non-unitarity of the leptonic mixing matrix: Present bounds and future sensitivities

    S. Antusch and O. Fischer, Non-unitarity of the leptonic mixing matrix: Present bounds and future sensitivities, JHEP10, 094, arXiv:1407.6607 [hep-ph]

  77. [77]

    A. Das, P. S. B. Dev, and C. S. Kim, Constraining Ster- ile Neutrinos from Precision Higgs Data, Phys. Rev. D 95, 115013 (2017), arXiv:1704.00880 [hep-ph]

  78. [78]

    New limits on heavy sterile neutrino mixing in ${^{8}\rm{B}}$-decay obtained with the Borexino detector

    G. Belliniet al.(Borexino), New limits on heavy ster- ile neutrino mixing in B8 decay obtained with the Borexino detector, Phys. Rev. D88, 072010 (2013), arXiv:1311.5347 [hep-ex]

  79. [79]

    Hagner, M

    C. Hagner, M. Altmann, F. von Feilitzsch, L. Oberauer, Y. Declais, and E. Kajfasz, Experimental search for the neutrino decay neutrino (3) —>j-neutrino + e+ + e- and limits on neutrino mixing, Phys. Rev. D52, 1343 (1995)

  80. [80]

    A. I. Derbin, A. V. Chernyi, L. A. Popeko, V. N. Mu- ratova, G. A. Shishkina, and S. I. Bakhlanov, Experi- ment on anti-neutrino scattering by electrons at a reac- tor of the Rovno nuclear power plant, JETP Lett.57, 768 (1993)

Showing first 80 references.