Leptophilic scalar dark matter in U(1) L mu-L tau: Evading direct detection and prospective neutron star heating

arXiv:2602.19958 · hep-ph, astro-ph.CO, astro-ph.HE · Submitted 2026-08-16 · Read on arXiv

Chengfeng Caia, Hong-Hao Zhang

Sun Yat-sen University · Sun Yat-sen University

hep-ph, astro-ph.CO, astro-ph.HE

Submitted: 2026-08-16

Updated: 2026-08-18

Comments: 29 pages, 7 figures. Updated Eqs. (2), (5), (7) and Table 1. Added references

License: http://creativecommons.org/licenses/by-nc-sa/4.0/

Importance score: 79/100

The gist: The paper, "Leptophilic scalar dark matter in U(1)Lµ −Lτ: Evading direct detection and prospective neutron star heating," investigates a theoretical framework for dark matter (DM) that evades

Terminology

Summary

The paper, Leptophilic scalar dark matter in U(1)Lµ −Lτ: Evading direct detection and prospective neutron star heating, investigates a theoretical framework for dark matter (DM) that evades current terrestrial constraints while remaining testable through astrophysical observations.

Motivation and Theoretical Framework

The study begins by noting that the Standard Model (SM) is an incomplete description of nature, leaving fundamental questions unanswered regarding the origin of dark matter, which constitutes approximately 27% of the universe’s energy budget. Traditional Weakly Interacting Massive Particle (WIMP) models face increasing tension with null results from direct detection (DD) experiments. To address this tension, the authors propose a leptophilic scalar DM framework within a U(1) L mu - L tau gauge extension of the Standard Model, which is designed to allow DM to evade stringent nuclear-recoil searches.

Methodology and Benchmark Models

The researchers conducted a systematic parameter scan imposing constraints from relic density, direct- and indirect-detection limits, and neutrino trident production. They identified viable sub-TeV to TeV DM candidates across three distinct benchmark realizations:

  1. Secluded Dark Matter: This scenario is where the relic density is set by annihilation into U(1) L mu - L tau gauge bosons, allowing the Higgs-portal coupling to be negligible, thereby suppressing tree-level DM-nucleon scattering.

  2. Pseudo-Nambu-Goldstone Boson (pNGB) Model based on SO(4) symmetry: In this model, the DM mass arises at tree level from a soft breaking term, and the elastic scattering amplitude is suppressed by a symmetry-protected cancellation.

  3. pNGB Model based on SO(3) symmetry: Here, the DM mass is generated radiatively at one loop via the U(1) L mu - L tau gauge interaction, which maintains compatibility with null direct-detection results.

Astrophysical Probes: Neutron Star Heating

The study leverages neutron stars (NS) as a complementary probe. Because NSs contain a degenerate population of leptons (electrons and muons), they are sensitive to leptophilic DM, allowing the authors to evade conventional direct detection bounds while remaining testable through the kinetic and annihilation heating of neutron stars.

  1. Capture Rate Calculation: The analysis begins by focusing on a class of leptophilic scalar dark matter (chi) where the effective interactions with quarks are assumed to be negligible. The interaction is dominated by a dimension-6 current-current interaction:

L dim6 = gamma mu chi i d mu chi l gamma mu over squared

The capture rate in the optically thin limit is calculated using the relativistic treatment.

  1. NS Heating Sensitivity: The authors found that the maximal heating of the neutron star is achieved when the capture process saturates to the so-called geometric limit. By equating the capture rate to this geometric limit, they derived a saturation threshold scale (*), which represents an energy scale within the reach of future colliders.

Results and Conclusion

The comprehensive study yields several key findings:

  • All three models successfully accommodate a DM candidate with a mass m DM about O(100) GeV.

  • The projected sensitivity of neutron star heating observations can probe regions of the parameter space that remain inaccessible to current terrestrial direct detection experiments.

  • For the pNGB DM models, the cancellation mechanism is crucial because it disentangles the interactions responsible for direct detection from those dictating the relic density, allowing for a correct relic abundance without requiring m DM to be near a mediator resonance.

In summary, the work demonstrates that near-infrared observations of NSs provide a valuable complementary probe for testing leptophilic dark matter models that are otherwise challenging to constrain via terrestrial experiments.

Improvements for AI systems

The following improvements outline how a highly specialized, fastidious AI system can be engineered to process, analyze, and synthesize the complex data presented in this scientific paper. These improvements move far beyond simple summarization and focus on quantitative constraint mapping and dynamic model comparison.

The Improvement: Develop an integrated AI module that dynamically maps the interconnected parameter space defined by m DM, xi X, Q DM g X, and t theta. This system will ingest not only the explicit equations (e.g., Eqs. 10, 56) but also the complex graphical representations (Figures 2, 3, and 4).

What the Improved AI System Can Do:

  • Automated Boundary Identification: The AI can identify and calculate islands of viability where all constraints are simultaneously satisfied:

  • DM h squared about 0.12 (Thermal Relic Density)

  • LZ/XENONnT Null Results (Direct Detection Exclusion Zones)

  • Fermi-LAT Limits (Indirect Detection Exclusion Zones)

** about 3.2–3.9 TeV (Maximum NS Heating Sensitivity)

  • Constraint Cross-Referencing: It can perform a rapid, quantitative comparison between the exclusion limits of terrestrial experiments and the projected sensitivity of astrophysical probes without manual data extraction, for example calculating the required Q DM g X necessary to push the LZ exclusion boundary into a specific region defined by xi X.

The improved AI system transforms from a passive data repository into an active, predictive scientific collaborator. It can not only read this paper but also test its claims, by allowing researchers to input hypothetical parameter sets and receive immediate feedback on:

  1. Which experimental bounds (LZ, Fermi-LAT) exclude the set.

  2. Whether the relic density is correct for that set.

  3. What future astrophysical observations (NS heating) are required to test that specific, surviving region of parameter space.

Abstract

Leptophilic dark matter (DM) is a well-motivated thermal WIMP framework that can evade stringent nuclear-recoil searches while remaining testable via DM-induced heating of neutron stars (NS). In this work, we study leptophilic scalar DM in a U(1) L mu-L tau gauge extension of the Standard Model, which provides a common leptophilic portal for all scenarios considered. To reproduce the observed relic abundance while suppressing direct-detection signals, we investigate three benchmark realizations: (i) a secluded DM scenario in which the relic density is set by annihilation into U(1) L mu-L tau gauge bosons, and two pseudo-Nambu-Goldstone boson (pNGB) DM models based on (ii) an SO(4) symmetry and (iii) an SO(3) symmetry. In the SO(4) pNGB model, the DM mass arises at tree level from a soft breaking term, while the elastic scattering amplitude is suppressed by a symmetry-protected cancellation. In the SO(3) pNGB model, the DM mass is generated radiatively at one loop via the U(1) L mu-L tau gauge interaction, and we show that this gauging preserves the same cancellation mechanism, maintaining compatibility with direct-detection null results. We perform a systematic parameter scan imposing relic density, direct- and indirect-detection, and neutrino trident constraints, and identify viable sub-TeV to TeV DM candidates. Assuming maximal capture in NSs, we find that the remaining parameter space can be tested by near-infrared observations of NSs, providing sensitivity complementary to terrestrial searches in regions that are currently weakly constrained.

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