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Fermionic Dark Matter in a Scotogenic Model with a Complex Scalar Singlet

This paper investigates the phenomenology of a complex scoto-singlet model that explains radiative neutrino masses and fermionic dark matter, identifying viable parameter spaces near Higgs resonances and coannihilation regions that are largely inaccessible to direct detection but potentially probeable via monojet searches and long-lived charged scalar signatures at colliders.

Original authors: Gustavo Ardila-Tafurth, Andrés Flórez, Victor Martín-Lozano, Avelino Vicente

Published 2026-08-05
📖 7 min read🧠 Deep dive

Original authors: Gustavo Ardila-Tafurth, Andrés Flórez, Victor Martín-Lozano, Avelino Vicente

Original paper licensed under CC BY 4.0 (http://creativecommons.org/licenses/by/4.0/). This is an AI-generated explanation of the paper below. It is not written or endorsed by the authors. For technical accuracy, refer to the original paper. Read full disclaimer

Imagine the universe as a giant, bustling party where everything we can see and touch—stars, planets, you, me—is just the VIP section. But physicists suspect there's a massive, invisible crowd in the basement called "Dark Matter." We know it's there because it pulls on the VIPs with its gravity, but we've never seen a single guest from this invisible crowd. At the same time, we've discovered that tiny particles called neutrinos, which zip through everything like ghosts, have a tiny bit of mass. In the Standard Model of physics (the rulebook for how the universe works), these neutrinos should be massless, like photons. The fact that they have mass is a glitch in the matrix, a clue that the rulebook is missing a chapter.

For decades, scientists have been trying to write a new chapter that explains both the invisible guests and the ghostly neutrinos at the same time. One popular idea is the "scotogenic model." Think of it as a secret society where the same rules that keep the party guests hidden also give the neutrinos their tiny mass. It's a clever trick: a hidden symmetry keeps the dark matter stable while allowing neutrinos to get their mass through a complex, looped process involving new, unseen particles. But what if this secret society has more members than we thought? What if there's a new, complex character joining the party? That's exactly the question a team of physicists asked in a recent study, exploring a slightly more complicated version of this hidden world to see if it fits the clues we have from the real universe.


The Complex Singlet: A New Guest at the Party

In this study, the authors took the standard "scotogenic" recipe and added a new ingredient: a "complex scalar singlet." Imagine the original model as a simple two-person dance between a fermion (a particle like an electron) and a scalar (a particle like the Higgs). The new model introduces a third dancer, a complex scalar singlet, which is a bit like a chameleon that can mix with the other dancers. This new character changes the choreography of the entire party. It doesn't change the main reason the neutrinos get their mass (the dance steps remain the same), but it adds new ways for the dark matter to interact and disappear, potentially solving some of the problems the simpler model had.

The researchers didn't just guess; they ran a massive digital simulation called a "Markov Chain Monte Carlo" scan. Think of this as a super-powered game of "Guess Who?" where they tested billions of possible combinations of particle masses and interaction strengths. They had to make sure every combination they picked passed a strict set of tests: it had to match the data we have on how neutrinos wiggle (oscillate), it couldn't break the laws of physics (like unitarity or stability), and it had to fit the observed amount of dark matter in the universe. They also checked to make sure the model didn't predict things we've already ruled out, like certain rare particle decays that experiments have never seen.

The Results: A Hidden World That's Hard to Catch

After running their simulations, the team found some fascinating, albeit tricky, results. They discovered that this new model can work. It successfully explains how dark matter could exist in the right amount to match our observations, but it does so in two very specific ways. First, there's the "Higgs funnel," a sweet spot where the dark matter particles are exactly half the mass of the Higgs boson, allowing them to annihilate each other very efficiently. Second, and more interestingly, there are "co-annihilation" zones. In these regions, the dark matter hangs out with other heavy particles that are almost the same mass. They help each other disappear, keeping the total amount of dark matter just right.

One of the coolest findings is that this model allows for lighter dark matter particles than the simpler version. The new "chameleon" particle helps the dark matter get rid of itself more easily, meaning we might be looking for particles with masses around 100 GeV (about 100 times the mass of a proton), rather than the heavier ones usually predicted.

The Catch: It's a Ghost in the Machine

Here is the big twist: while the model works on paper, it is incredibly hard to catch in the real world. The authors found that the signals for finding this dark matter are almost non-existent.

  • Direct Detection (The "Touch" Test): Usually, scientists try to catch dark matter by waiting for it to bump into an atom in a deep-underground detector. But in this model, the dark matter is so shy that it barely interacts with normal matter. The predicted "bump" is so weak that it falls below the "neutrino floor"—a fundamental limit where the background noise of neutrinos from space makes it impossible to tell if a dark matter particle hit the detector. It's like trying to hear a whisper in a hurricane; the signal is just too faint for current experiments like LUX-ZEPLIN to hear.
  • Indirect Detection (The "Smell" Test): Scientists also look for dark matter by watching for the gamma rays it might emit when two dark matter particles crash into each other and vanish. The authors found that even if this happens, the signal is billions of times weaker than what telescopes like Fermi-LAT can see. It's as if the dark matter particles are so polite they barely say "hello" before disappearing.
  • Collider Searches (The "Smash" Test): Since we can't catch them directly, the team looked at what happens if we smash particles together in the Large Hadron Collider (LHC). They found that the best chance to spot this model is in "compressed" scenarios, where the dark matter and its partners are very close in mass. In these cases, the new particles might decay into "soft" leptons (light particles like electrons or muons) that are too slow to trigger standard alarms. However, the team also found that these particles might be "long-lived," meaning they travel a noticeable distance inside the detector before decaying. This could create strange, "displaced" tracks or even particles that look like they are stuck in the detector.

The Verdict

The paper concludes that while this "complex scoto-singlet" model is a viable and elegant solution to the mysteries of neutrino mass and dark matter, it is a master of disguise. It suggests that the dark matter in this universe is likely hiding in a "compressed" mass range, perhaps around 300 GeV or lower, and is almost invisible to our current direct and indirect detection methods. The only real hope for finding it lies in the high-energy collisions of the High Luminosity LHC, specifically looking for those tricky "monojet" events (a single jet of energy recoiling against invisible particles) or for those long-lived, wandering charged particles that leave unusual tracks.

The authors are careful to note that these are simulation results. They haven't found the particle yet; they've just built a very convincing map of where it could be hiding. The path forward is clear: we need to look harder at the low-mass regions of the LHC and develop new ways to spot those long-lived, ghostly particles that refuse to play by the usual rules. Until then, the complex scoto-singlet remains a beautiful, theoretical possibility, waiting for the next generation of experiments to give it a name.

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