COSINUS Project: A New Approach to Dark Matter Detection
COSINUS uses NaI crystals and a muon veto to investigate dark matter.
― 6 min read
Table of Contents
COSINUS is a project aimed at finding dark matter, a mysterious and invisible substance that makes up a large part of our universe. The project focuses on using special crystals called sodium iodide (NaI) that can detect energy changes caused by dark matter interactions. These crystals work like extremely sensitive detectors in a lab deep underground, where they are shielded from Background Noise like cosmic rays and other radiation.
Dark matter is a topic of great interest in science because it has been suggested to explain various astronomical observations, such as the way galaxies rotate and the gravity they exert. Despite its significance, dark matter has not been directly observed. Previous experiments have led to conflicting results regarding its presence, with one notable experiment being DAMA/LIBRA, which claimed evidence of dark matter but was challenged by other experiments producing null results.
To clarify these conflicting findings, COSINUS aims to confirm or refute the results of DAMA/LIBRA using NaI crystals. This approach benefits from a low energy threshold, meaning it can detect weak signals potentially caused by dark matter interactions.
The Challenge of Background Noise
One of the significant challenges in detecting dark matter is the presence of background noise, which can produce signals that mimic those from dark matter. In the case of COSINUS, particles created by cosmic rays, especially Muons, can produce neutrons when interacting with materials in the experiment. These muon-induced neutrons can be mistaken for dark matter signals, complicating the analysis.
To combat this interference, COSINUS uses a large tank filled with ultra-pure water as a shield. This water acts as a passive barrier against radiation and background noise. However, a more active solution is required to reduce the effects of muon-induced events. Therefore, COSINUS includes a system known as the muon veto.
The Muon Veto System
The muon veto system is designed to identify and exclude muon events from the data collected by the experiment. This system operates by placing photomultiplier tubes (PMTS) around the water tank. These tubes can detect flashes of light produced when muons or secondary particles interact in the water, generating what is known as Cherenkov Radiation.
When a muon passes through the water, it can create a shockwave of light, which the PMTs capture. By monitoring these signals, scientists can tag events that are caused by muons and exclude them from the data analyzed for dark matter searches.
A critical aspect of the design involves optimizing the number and arrangement of PMTs around the water tank to ensure maximum efficiency in detecting muon events while minimizing accidental triggers from background radiation.
Designing the Muon Veto
To create an effective muon veto, several factors must be taken into consideration:
Number of PMTs: The more PMTs used, the higher the chance of detecting Cherenkov light produced by muons. However, COSINUS has a limit on the number of PMTs due to budget and space constraints.
Arrangement of PMTs: The arrangement of the PMTs around the tank influences their ability to detect light. They need to have optimal positioning to cover as much of the tank as possible.
Trigger Conditions: To decide what counts as a muon event, the system needs to set thresholds for how many PMTs need to trigger within a certain timeframe. This is crucial for minimizing false positives caused by background radiation.
Optical Dead Layer: An optically dead region can be created around the tank to reduce the number of ambient gamma rays that trigger the PMTs unnecessarily. This dead layer acts as a buffer zone where PMTs are not placed, preventing signals from being detected in this region.
Simulations for Design Optimization
To find the best configuration for the muon veto, detailed simulations are run. These simulations help visualize how muons and gamma rays interact with the water tank and how much light is produced. By analyzing where the light is most intense when a muon passes through, scientists can decide where to place the PMTs for maximum effect.
Different scenarios are tested, including variations in PMT placement, number, reflector type, and dead layer size. The outcome of these simulations guides the decision-making process for the final design of the muon veto system.
Results from the Simulations
The simulations indicated that a configuration with a larger number of PMTs provides better detection rates for muon events. Specifically, placing the PMTs in concentric circles along the bottom of the water tank proved to be effective in capturing the maximum amount of light.
When assessing the effectiveness of different trigger conditions, the simulations showed that a balance must be struck between sensitivity (detecting true muon signals) and specificity (avoiding false triggers). The arrangement that combined a four to six PMT coincidence requirement with a reasonable dead layer size reduced the chances of unwanted signals from background radiation.
In addition, reflections of light from surfaces around the tank were considered. A highly reflective surface enhances the chances of capturing light from muon interactions, thereby increasing the veto's efficiency.
Final Configuration and Performance
After running through numerous scenarios and evaluations, the final recommended setup consists of 28 PMTs arranged in concentric circles, using a highly reflective material around the water tank. The setup will also include an optical dead layer of approximately 30-40 cm around the tank to minimize background radiation without significantly impacting the muon detection efficiency.
With this final configuration, COSINUS expects to achieve a veto efficiency of over 99% for muon events, significantly reducing the false positive rate introduced by ambient gamma rays. This level of efficiency allows the experiment to distinguish between background noise and potential dark matter signals effectively.
Future Directions and Expectation
As COSINUS moves into the next phases of construction and data collection, the focus will be on ensuring the muon veto system operates as expected. Continuous tests will be conducted to measure its performance and adjust configurations as necessary based on real data.
The collaboration among scientists from various fields will be crucial as they work together to interpret the data collected. Successful operation of the muon veto, combined with the unique detection capabilities of the NaI crystals, will hopefully lead to new insights into dark matter.
In summary, the COSINUS project presents an innovative approach in the search for dark matter using advanced technologies and robust experimental design. With the ongoing development of the muon veto system, the project aims to enhance the search and understanding of this elusive substance to potentially unlock the secrets of the universe.
Title: Water Cherenkov muon veto for the COSINUS experiment: design and simulation optimization
Abstract: COSINUS is a dark matter (DM) direct search experiment that uses sodium iodide (NaI) crystals as cryogenic calorimeters. Thanks to the low nuclear recoil energy threshold and event-by-event discrimination capability, COSINUS will address the long-standing DM claim made by the DAMA/LIBRA collaboration. The experiment is currently under construction at the Laboratori Nazionali del Gran Sasso, Italy, and employs a large cylindrical water tank as a passive shield to meet the required background rate. However, muon-induced neutrons can mimic a DM signal therefore requiring an active veto system, which is achieved by instrumenting the water tank with an array of photomultiplier tubes (PMTs). This study optimizes the number, arrangement, and trigger conditions of the PMTs as well as the size of an optically invisible region. The objective was to maximize the muon veto efficiency while minimizing the accidental trigger rate due to the ambient and instrumental background. The final configuration predicts a veto efficiency of 99.63 $\pm$ 0.16 $\%$ and 44.4 $\pm$ $5.6\%$ in the tagging of muon events and showers of secondary particles, respectively. The active veto will reduce the cosmogenic neutron background rate to 0.11 $\pm$ 0.02 cts$\cdot$kg$^{-1}$$\cdot$year$^{-1}$, corresponding to less than one background event in the region of interest for the whole COSINUS-1$\pi$ exposure of 1000 kg$\cdot$days.
Authors: G. Angloher, M. R. Bharadwaj, M. Cababie, I. Dafinei, N. Di Marco, L. Einfalt, F. Ferroni, S. Fichtinger, A. Filipponi, T. Frank, M. Friedl, Z. Ge, M. Heikinheimo, M. N. Hughes, K. Huitu, M. Kellermann, R. Maji, M. Mancuso, L. Pagnanini, F. Petricca, S. Pirro, F. Pröbst, G. Profeta, A. Puiu, F. Reindl, K. Schäffner, J. Schieck, D. Schmiedmayer, P. Schreiner, C. Schwertner, K. Shera, M. Stahlberg, A. Stendhal, M. Stukel, C. Tresca, F. Wagner, S. Yue, V. Zema, Y. Zhu
Last Update: 2024-04-25 00:00:00
Language: English
Source URL: https://arxiv.org/abs/2406.12870
Source PDF: https://arxiv.org/pdf/2406.12870
Licence: https://creativecommons.org/licenses/by/4.0/
Changes: This summary was created with assistance from AI and may have inaccuracies. For accurate information, please refer to the original source documents linked here.
Thank you to arxiv for use of its open access interoperability.