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New Signal Classification Method in XENONnT Experiment

A new model improves signal analysis for dark matter detection.

― 6 min read


Signal AnalysisSignal AnalysisBreakthroughdetection accuracy.Improved method enhances dark matter
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The XENONnT experiment is a project aimed at detecting Dark Matter, a type of matter that does not emit light and is difficult to observe. The experiment uses a special detector called a dual-phase xenon time projection chamber (TPC), which can sense the energy released when particles interact with xenon gas. This article explains how a new method was developed to analyze the Signals generated by the detector, helping scientists to differentiate between different types of interactions.

The Need for Improved Signal Analysis

In any detection experiment, figuring out what type of interaction caused a signal is crucial. In XENONnT, particles can interact with the xenon in two main ways: through Scintillation, which produces light signals known as S1, and through Ionization, which creates another type of signal called S2. Being able to accurately classify these signals helps researchers understand the nature of the particles they are studying.

Previous methods of signal classification relied heavily on manual approaches, which lacked flexibility and the ability to quantify how confident researchers were in their classifications. To improve upon this, a new model was proposed using a method called a Bayesian Network.

What is a Bayesian Network?

A Bayesian network is a statistical model that helps to evaluate the relationships between different variables. In the context of the XENONnT experiment, this model can analyze the shape of the electrical signals generated by the detector, allowing scientists to decide whether a signal originates from scintillation (S1) or ionization (S2).

By using this method, researchers have created a tool that not only classifies signals but also provides a way to measure the confidence of each classification. This is done by training the model on both simulated and real data, focusing on specific interactions that are expected to happen in the experiment.

How the Detector Works

The XENONnT detector contains 5.9 tonnes of liquid xenon. When a particle interacts with the liquid, it causes the xenon atoms to become excited or ionized. Excited atoms emit ultraviolet light, which creates the S1 signal, while ionized atoms free electrons, which eventually lead to the S2 signal. The detector collects these light signals using arrays of sensors known as photomultiplier tubes (PMTs).

For each interaction, both S1 and S2 signals are generated. The S1 signal tends to be faster and narrower, while the S2 signal is slower and broader. By analyzing the characteristics of these signals, scientists can reconstruct the energy and position of the particles that generated them.

Challenges in Signal Analysis

Detecting dark matter involves identifying very weak signals among various background noise. One significant issue is that many signals recorded may not come from genuine particle interactions within the xenon but rather from spurious signals, like those from interactions occurring in the gas above the liquid or background radiation.

This complicates the task of distinguishing between real events and noise. An efficient method for analyzing and classifying these signals is essential for ensuring that the data used in future analyses is reliable.

Developing the Bayesian Network Model

The research team set out to create a Bayesian network tailored for the signal classification needs of the XENONnT experiment. First, they constructed a model that could evaluate the likelihood of a signal being S1 or S2 based on its shape and size.

The model was trained on a combination of simulated signals and actual data collected during initial runs of the experiment. By inputting specific characteristics of the signals into the model, it learns to relate these characteristics with the types of underlying processes that generated the signals.

The training data included a range of energy levels for electronic recoil signals, which occur when electrons are kicked out of atoms by incoming particles. This allowed the model to adapt and improve its classification capabilities over time.

Classifying Detector Signals

Once the Bayesian network was established, it could be used to classify new signals. While traditional methods assessed signals based on their area and width, the Bayesian network brings a more nuanced approach. It allows classification based on a broader range of characteristics.

For each incoming signal, the Bayesian network generates a score that indicates whether the signal looks more like an S1 or S2. A higher score for S1 means the signal resembles a canonical scintillation signal, while a higher score for S2 suggests it looks like a typical ionization signal. This flexible scoring system enhances classification confidence.

Testing the Bayesian Network Model

The new Bayesian network was evaluated against prior classification methods. In tests, it significantly outperformed traditional methods by providing more accurate classifications and better handling of noise.

The researchers found that using this method increased the efficiency of selecting valid events by approximately 3%. This improvement was particularly notable in the lower energy ranges, where distinguishing between true signals and background noise is more challenging.

Analyzing Event Selection

In dark matter detection, selecting relevant events while rejecting background noise is paramount. The Bayesian network allows scientists to apply specific criteria to determine which events are likely valid.

By analyzing the S1 and S2 scores generated by the model, researchers can efficiently filter out signals that do not meet the expected characteristics of true interactions. This means that signals from errors or non-canonical shapes can be rejected, leaving behind only potential dark matter interactions.

Impact of the New Method

The introduction of the Bayesian network model marks a significant step forward for the XENONnT experiment. By offering a more reliable means of signal classification, researchers can now better understand the data they collect and enhance the search for dark matter.

As the experiment continues, the Bayesian model can be further refined. Future updates could incorporate additional variables, improve the handling of unique detector conditions, and address other challenges as they arise.

Conclusion

The development of the Bayesian network for signal classification within the XENONnT dark matter detection experiment represents a promising advancement in the field of particle physics. By allowing for better classification and event selection, this method aids in the ongoing search for dark matter by ensuring the integrity of the data used for analysis.

As new techniques are explored and the model is refined, it holds the potential to improve the sensitivity of experiments aimed at uncovering the mysteries of dark matter and the universe itself.

Original Source

Title: Detector signal characterization with a Bayesian network in XENONnT

Abstract: We developed a detector signal characterization model based on a Bayesian network trained on the waveform attributes generated by a dual-phase xenon time projection chamber. By performing inference on the model, we produced a quantitative metric of signal characterization and demonstrate that this metric can be used to determine whether a detector signal is sourced from a scintillation or an ionization process. We describe the method and its performance on electronic-recoil (ER) data taken during the first science run of the XENONnT dark matter experiment. We demonstrate the first use of a Bayesian network in a waveform-based analysis of detector signals. This method resulted in a 3% increase in ER event-selection efficiency with a simultaneously effective rejection of events outside of the region of interest. The findings of this analysis are consistent with the previous analysis from XENONnT, namely a background-only fit of the ER data.

Authors: XENON Collaboration, E. Aprile, K. Abe, S. Ahmed Maouloud, L. Althueser, B. Andrieu, E. Angelino, J. R. Angevaare, V. C. Antochi, D. Antón Martin, F. Arneodo, L. Baudis, A. L. Baxter, M. Bazyk, L. Bellagamba, R. Biondi, A. Bismark, E. J. Brookes, A. Brown, S. Bruenner, G. Bruno, R. Budnik, T. K. Bui, C. Cai, J. M. R. Cardoso, D. Cichon, A. P. Cimental Chavez, A. P. Colijn, J. Conrad, J. J. Cuenca-García, J. P. Cussonneau, V. D'Andrea, M. P. Decowski, P. Di Gangi, S. Di Pede, S. Diglio, K. Eitel, A. Elykov, S. Farrell, A. D. Ferella, C. Ferrari, H. Fischer, M. Flierman, W. Fulgione, C. Fuselli, P. Gaemers, R. Gaior, A. Gallo Rosso, M. Galloway, F. Gao, R. Glade-Beucke, L. Grandi, J. Grigat, H. Guan, M. Guida, R. Hammann, A. Higuera, C. Hils, L. Hoetzsch, N. F. Hood, J. Howlett, M. Iacovacci, Y. Itow, J. Jakob, F. Joerg, A. Joy, N. Kato, M. Kara, P. Kavrigin, S. Kazama, M. Kobayashi, G. Koltman, A. Kopec, F. Kuger, H. Landsman, R. F. Lang, L. Levinson, I. Li, S. Li, S. Liang, S. Lindemann, M. Lindner, K. Liu, J. Loizeau, F. Lombardi, J. Long, J. A. M. Lopes, Y. Ma, C. Macolino, J. Mahlstedt, A. Mancuso, L. Manenti, F. Marignetti, T. Marrodán Undagoitia, K. Martens, J. Masbou, D. Masson, E. Masson, S. Mastroianni, M. Messina, K. Miuchi, K. Mizukoshi, A. Molinario, S. Moriyama, K. Morå, Y. Mosbacher, M. Murra, J. Müller, K. Ni, U. Oberlack, B. Paetsch, J. Palacio, Q. Pellegrini, R. Peres, C. Peters, J. Pienaar, M. Pierre, V. Pizzella, G. Plante, T. R. Pollmann, J. Qi, J. Qin, D. Ramírez García, R. Singh, L. Sanchez, J. M. F. dos Santos, I. Sarnoff, G. Sartorelli, J. Schreiner, D. Schulte, P. Schulte, H. Schulze Eißing, M. Schumann, L. Scotto Lavina, M. Selvi, F. Semeria, P. Shagin, S. Shi, E. Shockley, M. Silva, H. Simgen, A. Takeda, P. -L. Tan, A. Terliuk, D. Thers, F. Toschi, G. Trinchero, C. Tunnell, F. Tönnies, K. Valerius, G. Volta, C. Weinheimer, M. Weiss, D. Wenz, C. Wittweg, T. Wolf, V. H. S. Wu, Y. Xing, D. Xu, Z. Xu, M. Yamashita, L. Yang, J. Ye, L. Yuan, G. Zavattini, M. Zhong, T. Zhu

Last Update: 2023-07-26 00:00:00

Language: English

Source URL: https://arxiv.org/abs/2304.05428

Source PDF: https://arxiv.org/pdf/2304.05428

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.

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