REDTOP: Rare Eta Decays To Observe new Physics

The experiment

REDTOP is a low-energy, fixed-target experiment in its proposal stage. It belongs to the High Intensity class of experiments, as it aims at detecting small variations from the Standard Model by studying a large sample of events produced with an intense beam. REDTOP scientists propose using a 1.8 GeV Continuous Wave (CW) proton beam impinging on a target made with 10 foils of a low-Z material (lithium or beryllium) to produce about 1013 η mesons in one year of running. The detector surrounding those targets will attempt to capture the decay products of the η mesons and, in particular, those that are either not expected or are suppressed up to the 10-11 level. Read a more detailed discussion of the physics processes of interest for REDTOP.

The beam

One of the most challenging aspects of REDTOP is related to the design of the proton beam required to produce the desired number of η/η’ mesons. The kinetic energy of that beam, in fact, needs to be high enough to generate the η mesons inside the target but, at the same time, not too high so that the background is kept at manageable levels.  Monte Carlo simulations indicate that a beam energy of 1.8 GeV is optimal for the experiment. Furthermore, the beam time structure needs to be as uniform as possible, in order to allow the detector to collect, skim and transfer the information to the data storage.

Fermilab is developing its new Muon Campus to provide beam for the Muon g-2 and Mu2e experiments. At centerstage of the complex is the Delivery Ring (DR).  For Muon g-2, 8 GeV protons will be targeted from the Main Injector/Recycler and the DR will be tuned to collect 3.1 GeV/c momentum muons.  For Mu2e, the 8 GeV protons (8.9 GeV/c) will be transferred directly from the Recycler into the DR.  The ring will have RF cavities for maintaining bunched beams as well as a slow resonant extraction system for use during Mu2e running.  Though both Muon g-2 and Mu2e will run the DR at constant field, an additional RF cavity and improvements to the power supply system of the DR would allow the DR to decelerate beam to lower energies such as those required for REDTOP.  Hence, such enhancements to the DR would open up a new realm of lower-energy, high rate experiments to augment the upcoming Muon program.  Read a more detailed discussion of the accelerator complex for REDTOP.

The detector

Of course, as it is usually the case with High Intensity beams, the rare processes that the scientists want to study are accompanied by a much larger number of background events that can potentially hide or mimic those of interest.detector_sketch

Therefore, in order to keep the background at tolerable levels, the detector must be very fast and sensitive only to those particles expected to be produced in the processes of interest, namely electrons, positrons, muons and photons. This is why the whole apparatus is based on the  detection of prompt Cerenkov light, which is promptly created while the background particles (essentially, all the hadrons) are mostly under the Cerenkov threshold. Read a more detailed discussion of REDTOP detector.

The science program

The detector being designed for the REDTOP experiment will exploit novel technologies aimed at a highly granular, nearly hermetic apparatus, with fast timing (~30 psec) and excellent particle identification. This will offer the opportunity for a broad physics program, exploiting different beam energies and beam configurations. The physics opportunities offered by an eta/eta’ factory have been recently reviewed in a recent paper and are summarized in the physics page. The planned runs are described at the following link.

However, more experiments could be envisaged with eventual small upgrades of the detector. These will encompass runs with muons or kaon beams and with different targets. The high granularity of the calorimeter could be exploited at an EDM experiment, as the inelastic events, diluting the EDM measurement, would be rejected with a larger efficiency than with a more conventional polarimeter.