Organisation: JGU > Faculty 08 > Institute of Physics > Group Experimental Particle & Astroparticle Physics (ETAP) > Project 8
Research: JGU > Faculty 08 > Physics > Astroparticle & Neutrino Physics > Project 8
The Project 8 collaboration aims to measure the absolute neutrino mass by combining the new technologies of Cyclotron Radiation Emission Spectroscopy and cold atomic tritium. Both molecular hydrogen and molecular tritium can be cracked into atoms by thermal dissociation. However, to trap these atoms in a magnetic field, they must first be cooled to millikelvin temperature. In Mainz, we are developing an atomic beam source that can provide atomic tritium for a next-generation neutrino mass experiment.
Despite being the most abundant particles in the universe, neutrinos are the only elements of the standard model with an unknown rest mass. Cosmological observations, in particular of the cosmic microwave background radiation and of the distribution of large-scale structures in the universe set limits on the sum of neutrino masses. In contrast, tritium endpoint spectroscopy – currently the most sensitive method to determine the neutrino mass in laboratory experiments – relies solely on energy and momentum conservation. When a tritium atom decays, an electron and an anti-electron neutrino is generated. The released energy from this decay is a combination of the electron’s maximum energy and the rest mass of the anti-electron neutrino which can be resolved through precision measurement at the endpoint of the beta decay energy spectrum.
In addition to the strict energy-resolution requirement, only about 10−13 of all tritium decays fall in the endpoint region of the spectrum. Thus, even the world leading experiment Karlsruhe Tritium Neutrino Experiment (KATRIN), which is set to finish its data taking campaign by the end of 2025, will be unable to probe neutrino masses under 200meV. New experimental techniques are needed to achieve sub-200meV sensitivities.
The Project 8 collaboration has pioneered a novel experimental technique – Cyclotron Radiation Emission Spectroscopy (CRES) – which promises a neutrino mass sensitivity of 40 meV. In the CRES approach, tritium is confined in a strong magnetic field, which forces the decay electron into a cyclotron orbit. The electron energy is determined by a precision measurement of the radio waves it emits due to its cyclotron motion. Due to relativistic effects, the radio waves’ frequency is inversely proportional to the electron energy. Even though the radiated power is as small as a femto-Watt, modern low-noise amplifier technology enable the detection of single electrons and the measurement of their energy with eV resolution. The figure on the right shows a spectrogram of such an event, where the electron is clearly identified as a high-power track above the noise, with a slope given by how fast energy is radiated away in the cyclotron motion. The intermediate jumps in frequency are caused by interactions with the rest gas. Only the frequency at the onset of the track is relevant to determine the initial electron energy.
In its molecular state, some of tritium’s decay energy will go into molecular exitations, setting a fundamental limit to the energy resolution that can be achieved. For the CRES approach, this limit can be overcome using a source of atomic tritium – which is comparatively easy to produce but difficult to retain in atomic state. We are working on building and characterizing an atomic source demonstrator that shows how atomic tritium can be produced and trapped in the quantities required to improve on the existing neutrino mass limits.
The Mainz Atomic Test Setup (MATS) should demonstrate the production of cold atomic hydrogen at rates that are needed for a next-generation neutrino mass experiment. The MATS setup uses hydrogen atoms instead of tritium since the atoms behave very similarly and the use of tritium in a University environment is restricted due to its radioactive nature. To produce large amounts of atomic hydrongen methods that are used in atomic physics are not feasible because they produce too little atom flux. In our test stand we dissociate molecular hydrogen by heating it to >2000K which cracks up the molecule into individual atoms. Our Hydrogen Atomic Beam Source (HABS) uses a hot tungstant capillary to crack the molecular hydrogen. The HABS is operated in ultra-high vaccum so that the atomic beam can propergate unattenuated. We plan on additional elements in our atomic beam line to cool down the hot atomic beam and trap it in an atomic beam trap. Many activities in Mainz are around the MATS and are described below.
While working with hydrogen, many of the devices and vacuum components can be readily upgraded or replaced. The same flexibility, however, is not possible when handling tritium, because radioactive contamination protocols are far more stringent. These constraints—together with our shared interest in atomic-tritium research—motivated the formation of the KAMATE collaboration with our colleagues at the Tritium Laboratory Karlsruhe (TLK). The main goal of this collaboration is to take the MATS design and rebuild the setup at TLK for tritium measurements. KAMATE’s milestones are as follows:
- KAMATE 0.5: Identify best atomic hydrogen source and test the need for a tilt mechanism
- KAMATE 1.0: Operate the resulting setup at TLK with Tritium
- KAMATE 2.0: Add and test the accommodator as first stage of cooling
- KAMATE 3.0: Add and test the nozzle as the second stage of cooling and beam temperature measurements.
To improve the atom producitionm, we need to measure and characterize a sources’ properties, make changes, and compare the results. Therefore, we need a varity of beam diagnostics to measure and verify the produced atom flux. We use mass spectrometer specialized on low mass-to-charge ratios and multiple analysis methods to determine the dissociation efficiency . This includes the measurement of the relative atom to molecular hydrogen flux and thus the characterization of the dissociation efficiency. The group in Mainz developed a calorimetric detector based on gold coated wires to measure the hydrogen flux, which allows to measure the spatial beam distribution. For the determination of the dissociation efficiency a measurement of the capilary temperature is needed. We are developing techniques to measure temeratures conratctles in vacuum with ~1K precision. Further we are investigating beam temperature measurements
The thermal dissociation of molecular hydrogen produces a hot (~2000K) beam of atomic hydrogen. However, to trap the atomic hydrogen it has to be cooled to mK temperatures. The cooling of the hot atomic beam happens in a (at least) two step approach. We are developing a first cooling stage for the atomic hydrogen beam based on an accomodator design which uses single or few wall collisions of the beam on a wall surface cooled to ~140K where recombination probabilities of atomic hydrogen are low. In a second step a single wall collision on a few K surface will cool the atoms further.
Once cooled to millikelvin Temperatures the atomic hydrogen beam needs to be store in an atom hydrogen trap. The atom trap is required to avoid recombination of atomic hydrogen to molecular hydrogen at the walls of the vacuum chambers. A small atom trap that uses a Ioffe-Pickard magnetic atom trap or a Halbach array of permanent magnets is currently envisioned. This trap would allow to evaluate trapping efficiency, loss rates due to various effects, etc.
The hardware work in the MATS setup is stronly supported and optimized with simulations. In particular we are simulation the process of hydrogen dissociation and recombination. Several simulation packages are in use, each with its own special purpose. Examples are thermal profiles of the heated capillary at different flow rates, the simulation of spatial beam distributions for beam lines with different skimmers, the determination of the velocity distributions within the atomic beam or simulation of wall collisions in an accomodator design for cooling purpose.
The CRES technique described above is pioniered by the Project 8 collaboration. Project 8 follows a phased approch with a series of different demonstrator experiments. In Phase II the first neutrino mass measurement using the CRES technique was performed. The group in Mainz significantly contributed to the Data Aquisition (DAQ) system for the readout of the RF frequency. The group determined the detection efficiency as function of kinetic energy by using a mono-energetic line of a meta-stable Krypton isotope and a solenoid to shift the magnetic field and thus the frequency response of the apperatus. The final data analysis using a Frequentist method was developed in Mainz and resulted in the first neutrino mass measurement with a sensitivity of 150 eV.
One major challange for the Project 8 collaboration is to scale up the CRES technique to large volumina to aquire sufficient statistics for a competitive neutrino mass measurement. Therefore the Project 8 collaboration investigated the use of radio frequency antennas to pick up the CRES signal in free space. A Free Space CRES Demonstrator (FSCD) was designed to demonstrate the detection of CRES in free space in a 1L scale active volume. However, the investigations show that the computational needs to reconstruct and detect signals from a huge array of antennas are challanging. The group in Mainz designed the magnetic bottle trap to for CRES electrons for the FSCD, developed an independent simulation tool to simulate CRES events and signals in an antenna array, developed likelihood based reconstruction technique to benchmark the best possible reconstruction resolution and investigated the neutrino mass sensitivity reach of a potential large scale experiment for neutrino mass detection based on antenna arrays in a best case scenario. While a 40meV neutrino mass sensitivity can be reached in such an experiment the computational needs in such an experiment are extremely challanging and an alternative readout scheme based on cavities is now followed.
The radiated power by a single CRES electron is on the aW – fW level depending on the magnetic field strength. To detect electrons based on this little power, the CRES electron has to be observed for a long time (µs – ms) to be detectable and reconstructable. Thus the CRES electron has to be confined in the sensitive part of the apperatus. In CRES experiments this is achived by a magnetic bottle trap, which exhibits two magnetic field bumps in axial direction of the background field. CRES electrons with little axial momentum are thus trapped. The magnetic field trap leads to additional signal features in the CRES signal and introduces additional frequency components. The CRES signal shape and reconstructability thus depends on the magnetic trap shape. For example, the mean experienced magnetic field of a CRES electron depends on its axial momentum and thus the turning points in the magnetic field trap. For high-precision determination of the CRES electron kinetic energy these effects have to be considered. In addition the design of a magnetic bottle trap has to account for technical constraints like available space and heat load on the setup. The group in Mainz is leading the design of the electron trap for several demonstrators. Currently the electron trap for the Cavity CRES apperatus (CCA) is under commissioning at the University at Washington.
Autoren: A. Esfahani et al.
arXiv:2504.15387
2025
Autoren: A. Esfahani et al.
Nuclear Inst. and Methods in Physics Research, A, Volume ,
2025
Autoren: M. Astaschov et al.
Eur. Phys. J. D, Volume 79, Page 60
2025
Autoren: A. Esfahani et al.
Phys. Rev. C, Volume 109, Page 035503
2024
Autor: L. Thorne on behalf of the Project 8 Collaboration
Proceedings of Science, TAUP2023, Volume 441, 231
2024
Autoren: A. Esfahani et al.
Phys. Rev. Lett., Volume 131, Page 102502
2023
Autor: R. Reimann on behalf of the Project 8 Collaboration
Proceedings of Science, PANIC2021, Volume 380, 283
2022
Autoren: R. Battesti et al.
Physics Reports, Volume 765-766, Pages 1-39
2018
We regularly offer
- Internships
- Bachelor Thesis
- Master Thesis
- PhD positions
- student assistant (HiWi) positions
Within our Project you can learn many different skills, e.g.
- Vacuum Technology
- Statistical Analysis Tools
- Programming in Python or C++
- Data Aquisition
- Simulations with packages like MolFlow, Kassiopeia & SPARTA
Thesis are usually available in all topics cover above. For general inquiries regarding open research positions please contact Prof. M. Fertl and Prof. S. Böser. Please be aware of the opportunities within the PRISMA+ Cluster.
To strengthen its neutrino research program, the Johannes Gutenberg University Mainz invites applications for 1 postdoctoral position (EG13 TV-L) to work on next-generation neutrino mass experiments with the Project 8 (https://www.project8.org/) and KATRIN (https://www.katrin.kit.edu/) collaborations. The position is initially term-limited to three years.
The postdoctoral scholar will coordinate the planning and implementation of the hardware and the measurement campaigns on both sites in close collaboration with the PhD students. The ideal candidate will have a strong and demonstrated experimental experience with the generation and cooling of high-flux atomic or molecular beams.
For details see the call announcement below:
To strengthen its neutrino research program, the Johannes Gutenberg University
Mainz invites applications for 1 PhD position (66% EG13 TV-L) to work on the Project 8 experiment (https://www.project8.org/).
The PhD student will investigate the interaction of hot hydrogen atoms with cryogenic
surfaces to accommodate their velocity distribution to a range that can be captured in
subsequent beamline elements. These will provide further beam cooling and trapping
of the tritium atoms. The accommodation efficiency and recombination rate on various
material will be investigated. The results provide key input parameters for the size and
performance specifications of a closed tritium re-circulation loop at TLK.
For details see the call announcement below:
We are part of the Project 8 Collaboration with partners at 17 different institutions in Belgium, Germany and the USA.
We are funded and integrated into the PRISMA + Cluster of Exellence and work together with the Detector Lab of PRISMA+.
Within the Karlsruhe Mainz Atomic Tritium Experiment (KAMATE) we are cooperating with the Tritium Laboratory Karlsruhe.