My researcher life is currently getting calmer, as announced in my last post, so that I have more time for my own blog and SteemSTEM. Today, I decided to focus on science communication (in the field of particle and astroparticle physics) and discuss some recent results of the MoEDAL experiment, one of the experiments being held around the Large Hadron Collider (the LHC) at CERN.
[image credits: Luc Viatour (CC BY-SA 3.0) ] As said many times, there are good reasons to believe in the existence of new phenomena in particle physics (please see here for more information).
The MoEDAL experiment has been designed to track down two classes of exotic objects that could unravel the existence of such new phenomena: very massive stable particles and magnetic monopoles.
If these exotic objects exist, there is potentially a chance to produce them at the LHC. The MoEDAL experiment has been designed by relying on this hypothesis, and to trap these monopoles and massive stable particles for further studies using unconventional methods (ultra fast scanning microscopes, aluminium traps, detector sensitive to the faintest light).
This setup gives its name to the experiment: MoEDAL is the acronym of Monopole and Exotics Detector at the LHC.
Magnetic monopoles?
Magnetic monopoles?
In order to understand what a magnetic monopole is, it is good to go back to the concept of unit of electric charge. It serves to quantify the charge of any (macroscopic or microscopic) object.
[image credits: ESO/L. (CC BY-SA 4.0) ] For instance, a proton has an electric charge of +1, an electron of -1 and an uranium nucleus of +92. In addition, there are neutral objects with an electric charge of 0, like a neutron or matter (that is in general composed of charged constituents so that the total charge vanishes).
Magnetism is however different. There is no unit of magnetic charge. A magnet has two poles: a South and a North pole. If one cuts a magnet into two pieces, one gets two magnets with two poles again. And if we continue to reach the elementary constituents of the initial magnet, they all have two poles.
What we call a magnetic monopole is in contrast a single magnetic pole. Whilst magnetic monopoles are easy to theorize, their presence even rendering the fundamental equations of electromagnetism more elegant, they have never been observed and are thus actively searched for.
Magnetic monopoles at the LHC
Magnetic monopoles at the LHC
Monopole are predicted by many theories extending the Standard Model of particle physics. They are characterized by a (very large) mass, a spin and a fundamental magnetic charge. Their properties imply that they can be copiously pair-produced (2 is better than 1) in a very energetic environment such as at the LHC, and each produced monopole is quite energetic. But how to detect them?
[image credits: @pab.ink] Monopoles can easily ionize matter. They make use of a fraction of their energy to break neutral matter into charged components. And by easy, I really mean it. A monopole can ionize matter a few thousands times better than a proton.
Once produced at the LHC and reaching the MoEDAL detector, monopoles interact with the detector material, creating a bunch of charged particles that leave observable tracks. In the process, monopoles get less and less energetic, so that at the end of the day, they have so few energy left that they are trapped in MoEDAL. MoEDAL can then be scanned afterwards to verify whether anything is trapped inside.
The newest results
The newest results
Last March, the MoDEAL collaboration released new results. They have tried to search for monopoles of different fundamental charges, different masses and different spins. The findings are all negative. Nothing has been found after scanning every single bit of the detector.
As a consequence, limits can be set on the properties of the monopoles, like in the figure below (for the case of spin-zero monopoles).
[image credits: arXiV] In the figure, constraints are derived as a function of the monopole mass (the x-axis). I recall that a monopole of 4000 GeV means that we have a beast that weights as much as 4000 protons. For the sake of the comparison, the heaviest known element contains 118 protons. The y-axis represents the monopole production rate given for different fundamental magnetic charges (the 5 color codes, the pink being the biggest charge).
The figure then exhibits solid and dashed curves. The solid curves represent theory predictions for different fundamental magnetic charges, whilst the dashed ones are the limits derived from the non-observation of any monopole signal in MoEDAL.
Cases where predictions are larger than (or above) limits correspond to situations where one predicts so many monopoles that they could not escape detection. In other words, those scenarios are today excluded by the non-observation.
Inversely, cases where predictions are smaller than (or below) limits correspond to situations where one predicts few enough monopoles that it makes sense that we have not observed anything yet. Those scenarios are thus still allowed.
Summary
Summary
With this blog post, I am officially back to Steem with science. I discussed recent results of the MoEDAL collaboration, the scientific article being available here.
MoEDAL is actively searching for magnetic monopoles at the Large Hadron Collider. Those particles can be seen as elementary magnetic charges, i.e. a single North or South magnetic pole. However, none of them has been observed so far, so that constraints can be imposed on their existence.
The MoDEAL collaboration has investigated many theoretical setups, and its results consist in the most stringent and up-to-date bounds on monopoles. In practice, the existence of monopoles as heavy as 2000—4000 protons is forbidden. The monopole hypothesis is however not excluded, as there is nothing that prevents monopoles from being heavier than the current limits.
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