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The Role of Ar42 in Scientific Research

Ar42's impact on experiments analyzing dark matter and neutrinos.

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Argon is a gas that is often used in scientific experiments, particularly those that study neutrinos and dark matter. One particular form of argon, Ar42, is radioactive and can be found in the atmosphere. This gas is produced mainly through reactions involving Cosmic Rays and is important to understand because it could interfere with sensitive experiments.

What is Ar42?

Ar42 is a rare form of argon that is radioactive. It decays over time, meaning it can be a source of background noise in experiments that search for rare events, such as interactions from neutrinos or dark matter. Its main production method is through cosmic rays hitting regular argon, Ar40, in the atmosphere.

Why is Ar42 Important?

In experiments meant to detect weak signals, like those from neutrinos or dark matter, any unwanted noise can make it hard to find the desired results. Ar42, while present in low amounts, contributes to this noise. Understanding how much Ar42 is around, especially in argon taken from underground sources, helps scientists reduce this background noise.

Sources of Ar42

Ar42 is mainly created in the atmosphere when cosmic rays collide with Ar40. When energetic particles from space strike, they can produce Ar42. This reaction happens primarily in the upper atmosphere, where there's more interaction with cosmic rays. However, underground, the production rate is much lower.

Ar42 vs. Ar39

Another form of argon, Ar39, is also important. It’s more abundant than Ar42 and has a longer half-life. Due to its higher levels in atmospheric argon, it's a bigger concern in experiments. The rates of Ar39 production are several orders of magnitude greater than those of Ar42. Understanding both is crucial because they can affect the readings of experiments.

Measuring Underground Production

To estimate how much Ar42 is produced underground, scientists look at particle interactions in the crust. These include reactions caused by natural radioactivity and cosmic rays. Models and simulations help calculate the production rates based on various factors, including the rock's composition and the types of particles interacting with it.

At great depths, such as 3,000 meters underwater, the production rate of Ar42 is significantly lower compared to the atmosphere. Experiments have found that at this depth, the rates are about 7 million times lower than those of Ar39.

The Impact of Ar42 in Experiments

In liquid argon detectors, which are commonly used in physics experiments, Ar42 can produce unwanted signals. This is especially true when it decays to another isotope called K42. The decay of K42 can generate high-energy signals that confuse measurements in sensitive setups, potentially leading to false results.

For experiments like GERDA, which looks for rare types of decay, high-energy signals from K42 created from Ar42 decay posed a major challenge. This led to efforts to measure K42 levels and find ways to reduce its impact.

Argon Sources for Experiments

Scientists are looking for ways to lessen the background noise caused by argon isotopes. One method is to use argon sourced from deep underground, as it is expected to have lower levels of both Ar39 and Ar42. The idea is that the deeper the argon is taken from, the less contamination it has from cosmic rays, and therefore, the less background noise there would be.

What Happens Underground?

While there has been limited research on how Ar42 is produced underground, existing knowledge points to two main sources of particles that can create Ar42: cosmic ray muons and the decay of elements within the Earth's crust. As muons and radioactive decay particles move through the rocks, they can trigger reactions that produce Ar42.

Cosmic Rays and Their Role

Cosmic rays are high-energy particles from space that can create secondary particles when they interact with the Earth's atmosphere and crust. These secondary particles can then interact with argon isotopes, leading to the production of Ar42.

The muons created by cosmic rays can penetrate deep into the Earth, allowing them to induce reactions that produce isotopes. The amount of particles produced is dependent on the muon flux, which varies with depth and the composition of the rock.

Radiogenic Contribution

In addition to cosmic rays, radioactive decay in the Earth contributes to the production of Ar42. Natural uranium and thorium decay chains can produce neutrons and alphas that can interact with nearby isotopes, potentially creating new radioactive isotopes.

However, the contribution of radiogenic processes to Ar42 production is expected to be very low compared to cosmic processes.

Simulating the Processes

To estimate production rates, scientists use computer simulations that model how particles interact within the Earth. These simulations take into account the type of rock, the density, and other factors to provide estimates of how much Ar42 is likely to be produced underground.

Estimating Production Rates

Studies provide estimates for how much Ar42 could be produced over time in various environments. For example, at a depth of 500 meters, the production rate of Ar42 is calculated at specific values, while at deeper levels like 3,000 meters, the numbers drop significantly.

Measurements and Comparisons

By comparing measured levels of other isotopes, like Ar39, scientists can infer the levels of Ar42 present in underground argon. Looking at how much Ar39 is found in underground sources gives insights into the expected levels of Ar42.

Expected Concentration in Detectors

Estimates suggest that when argon is sourced from underground, the anticipated levels of Ar42 activity will be much lower than in atmospheric sources. This reduction means that using underground argon can help increase the sensitivity of detectors used in experiments.

Challenges of Extraction and Use

Despite the benefits of using underground argon, there are challenges in ensuring the argon remains uncontaminated. Any exposure to cosmic rays during storage or transport could lead to increased levels of Ar42, counteracting the supposed benefits of sourcing it from deep underground.

Implications for Future Experiments

Having lower levels of Ar42 has significant implications for experiments like those searching for dark matter or studying neutrinos. The need for clean backgrounds leads researchers to continuously refine their methods for extracting and using argon, ensuring that they minimize contamination.

Summary

In summary, the understanding of Ar42 and its behavior in both atmospheric and underground settings is crucial for sensitive scientific experiments. While the production of Ar42 from cosmic rays is significant, the lower levels found in underground sources could enhance the quality of data collected in future studies. As experiments continue to evolve, so too will the methods for sourcing and measuring the impact of various argon isotopes.

Original Source

Title: Subsurface cosmogenic and radiogenic production of ^{42}Ar

Abstract: Radioactive decays from ^{42}Ar and its progeny ^{42}K are potential background sources in large-scale liquid-argon-based neutrino and dark matter experiments. In the atmosphere, ^{42}Ar is produced primarily by cosmogenic activation on ^{40}Ar. The use of low radioactivity argon from cosmogenically shielded underground sources can expand the reach and sensitivity of liquid-argon-based rare event searches. We estimate ^{42}Ar production underground by nuclear reactions induced by natural radioactivity and cosmic-ray muon-induced interactions. At 3,000 mwe, ^{42}Ar production rate is 1.8E-3 atoms per ton of crust per year, 7 orders of magnitude smaller than the ^{39}Ar production rate at a similar depth in the crust. By comparing the calculated production rate of ^{42}Ar to that of ^{39}Ar for which the concentration has been measured in an underground gas sample, we estimate the activity of ^{42}Ar in gas extracted from 3,000 mwe depth to be less than 2 decays per ton of argon per year.

Authors: Sagar S. Poudel, Ben Loer, Richard Saldanha, Brianne R. Hackett, Henning O. Back

Last Update: 2023-09-28 00:00:00

Language: English

Source URL: https://arxiv.org/abs/2309.16169

Source PDF: https://arxiv.org/pdf/2309.16169

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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