Dark Clouds, Hidden Rays: Measuring the Invisible Power of Cosmic Rays

File:"Coreshine" in the L183 Dark Cloud.jpg 

 Source: https://commons.wikimedia.org/wiki/File:%22Coreshine%22_in_the_L183_Dark_Cloud.jpg

 

 Star Formation, Dark Clouds and Cosmic Rays

In space, there are very large and cold clouds of gas that are home to new stars. It's impossible to see what's happening right in the middle of these clouds because it's so dark that no light can penetrate. But cosmic rays (very fast particles traveling through space) pass through these clouds. 

The biggest problem here was that scientists did not know exactly how many cosmic rays were present in the cloud and how fast they were ionizing the gas (this is called CRIR or Cosmic Ray Ionization Rate). Until now, scientists only used to "guess" by observing other things, but they did not have any concrete proof or direct way to measure the real value of CRIR. 

This paper has found a very simple solution to this problem: the authors explain that when these cosmic rays reach the cloud, they strongly collide with the hydrogen gas (H2) molecules present there. This collision "excites" the hydrogen molecule and releases a faint infrared light. 

Scientists say that if we observe this faint light with Earth's largest telescopes, we can directly calculate the CRIR without any estimation. This will help us understand how stars are formed in the galaxy and what the "weather" of space is like.

Until now, scientists knew that cosmic rays enter these clouds, but there was no direct way to determine how much.

  1. Indirect Methods: Earlier, scientists used to estimate by observing another gas (like argon or OH+). It was like looking at a standing cycle outside someone's house and guessing how many people would be inside. This was often wrong because a lot of the chemistry changed in between.
  2. Name of the Problem (CRIR): Scientists wanted to know the Cosmic-Ray Ionization Rate (CRIR). This means how many atoms these rays are 'charging' (ionizing) in one second. Knowing this rate is important because it determines when the gas will cool and when it will form a star.

1. Search for the Brightest Light: The (1-0) O(2) Line

First, understand that when cosmic rays (CRs) collide with a hydrogen molecule (H2), the molecule doesn't emit just one kind of light, but rather emits light at different energy levels. The biggest result of this paper is that it has chosen the "winner" among all those light lines. Using physics and mathematics, the authors showed that in cold clouds, where temperatures are very low, the line called (1-0) O(2) will be the brightest.


The significance of this is that light coming from space is very faint. If we know in advance which specific line we want to find (e.g., a wavelength of 2.62 micrometers), we can focus our telescopes on it. Additionally, the paper also mentions other lines like Q(2), S(0), and O(4). All of these lines have a specific "pattern." If we see this pattern in our telescope, we can be 100% sure that the light is coming from cosmic rays, and not from any other source. 

A. Which light should you look for? (The Brightest Line)
The hydrogen molecule emits many types of light. But a telescope can't see everything. The author discovered that a particular infrared line called (1-0) O(2) would be the brightest. Why? Because in cold clouds, hydrogen exists in a special state called "para-hydrogen." When this para-hydrogen is struck by cosmic rays, it emits the most energy in this O(2) line. This is like a 'signal' for us.


2. The Real Competition: UV Radiation vs. Cosmic Rays

There are two major players in space that can shock hydrogen gas and make it emit light: the first is starlight (UV light) and the second is cosmic rays. Until now, the problem was that when we observed light through telescopes, we were confused about what produced it. 

This paper has put an end to this confusion once and for all. The authors proved that UV light cannot penetrate dense and cold clouds because the dust in the path blocks it. But cosmic rays are so powerful that they reach the deepest and darkest part of the cloud (cloud core). The result was that if we look at the "High Column Density" part of the cloud (where the gas is very dense), the light seen there is 100% due to cosmic rays. This means we no longer need to worry about UV light, and we can clearly measure the activity of cosmic rays.


3. Detection: Can We Really See It?

The authors performed calculations to see if our current telescopes are capable of detecting this faint light. The answer is: Yes!


They explained that the Very Large Telescope (VLT) in Chile, one of the largest telescopes on Earth, is perfect for this task. If we focus this telescope on a cold cloud and collect data continuously for 8 hours (integration time), we will clearly see those "H2 emission lines." This is a significant result because previously people thought that this light was so weak that it would never be visible. Now we have an "action plan" for how and for how long to observe the clouds. Furthermore, in the future, the ELT (Extremely Large Telescope) and JWST will be able to see it even more easily.

 

Milky Way | National Geographic Kids 


4. Future Benefit: The Galaxy's Climate and the Secrets of Star Formation

The biggest benefit of this method will be in the future. Cosmic rays are what determine when gas changes will shrink to form a new star. If we know how many cosmic rays (CRIR) are in different corners of the galaxy, we will be able to understand the rate of new star formation.


In addition, this method will also tell us where these cosmic rays are coming from. Do they come only from supernovae (star explosions) or do they have some other mysterious origin? After this paper, we will be able to create a "cosmic-ray map" of the entire Milky Way Galaxy. Just like we measure the temperature of every city on Earth, we will be able to measure the "heat" and "speed" of cosmic rays in every corner of space. This information will provide a new direction for understanding space science and the world of stars. 

Source: https://www.nature.com/articles/s42005-020-0293-7 

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