Neutral hydrogen and Bremsstrahlung

In summary, the conversation discusses the formation of neutral hydrogen and its relation to the emission of radiation. It is mentioned that when an electron is bound in a hydrogen atom, it follows the Rules of Quantum Mechanics and may emit photons when transitioning between energy levels. The question is raised about whether radiation plays a role in the formation of neutral hydrogen and if this process could be observed in the cosmic microwave background. One participant suggests that inverse photoionization may be the process at work, while another mentions recombination lines as a possible source of emitted radiation. Overall, the conversation highlights the complexity of this topic and the potential for further research and understanding.
  • #1
hellfire
Science Advisor
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An electron which is decelerated emits a photon (Bremsstrahlung). When neutral hydrogen is formed putting together one proton and one electron (a free electron is bound by a proton), does the electron decelerate and does it emit a photon?

Thanks.
 
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  • #2
When an electron is bound in a hydrogen atom, it is subject to the Rules of Quantum Mechanics, which, among other things, permits electron energy changes to take place in discrete (quantum) amounts (this gives rise to its spectrum). At its lowest level, it just stays at constant energy. There are a lot more details to this subject - look it up with google, or get a book on elementary quantum theory.
 
  • #3
I already took a look in google, of course, but I did not found an answer. I know that an electron bounded in an atom follows some rules, but my question is whether the electron suffers a deceleration in the time from beeing free to the time when it is bound or trapped by the proton. Let's say, it is not a question how the energetic transitions of the electron inside the atom are related to emission of absorption of radiation, but a question whether radiation plays a role between the electron beeing outside and inside of the atom. I assume that the electron will have a change in its dynamical behaviour...?

Regards.
 
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  • #4
If an electron, originally in the lowest bound state in an H atom, is 'booted out', to become a 'free' electron, then it needs to be 'given' energy - e.g. by a photon - at least equal to the "Lyman limit". If the reverse happens, do you think a photon will be emitted?

If a cloud of H atoms is between you and a distant, point source of copious photons, from gammas to radio, what will you observe in the spectrum of this bright, distant point source? The cloud of H atoms will reach some kind of equilibrium wrt the distant source of photons of many energies; what sort of equilibrium? Why don't you 'see' LyA radiation coming from the point source (caution, trick question)?
 
  • #5
I am not sure about the answer, Nereid, this is why I asked. On the other hand it is nice that you step into the thread, because my question has ultimatively to do with cosmology…

Coulds of neutral Hydrogen may absorb high energy photons and get ionzed. As far as I know, when electrons recombine with protons, then they have to step down on energy levels and an emission takes place. But I am not sure of this.

May be my question was not correctly formulated: what I want to know is whether the formation of neutral hydrogen generates radiation. Independently whether Bremsstrahlung takes place or not (it seams it does not).

The main reason what makes me doubt is that during the cosmological recombination epoch a lot of radiation should have been generated due to the formation of neutral hydrogen. I assume that this emitted radiation was not necessarily in thermal equilibrium with the rest of the photons at 3000° K.

Since this radiation was exactly at the last scattering surface it should be visible as a clear anisotropy now. I do not remember to have seen this point mentioned in the references I read about the CMB.

I apologize for the somehow chaotic way of asking this, starting this ambiguous thread. So, may be this thread should be moved to cosmology.

Regards.
 
  • #6
hellfire said:
I am not sure about the answer, Nereid, this is why I asked. On the other hand it is nice that you step into the thread, because my question has ultimatively to do with cosmology…

Coulds of neutral Hydrogen may absorb high energy photons and get ionzed. As far as I know, when electrons recombine with protons, then they have to step down on energy levels and an emission takes place. But I am not sure of this.

May be my question was not correctly formulated: what I want to know is whether the formation of neutral hydrogen generates radiation. Independently whether Bremsstrahlung takes place or not (it seams it does not).

The main reason what makes me doubt is that during the cosmological recombination epoch a lot of radiation should have been generated due to the formation of neutral hydrogen. I assume that this emitted radiation was not necessarily in thermal equilibrium with the rest of the photons at 3000° K.

Since this radiation was exactly at the last scattering surface it should be visible as a clear anisotropy now. I do not remember to have seen this point mentioned in the references I read about the CMB.

I apologize for the somehow chaotic way of asking this, starting this ambiguous thread. So, may be this thread should be moved to cosmology.

Regards.

This may not exactly answer your question, but if this process is anything similar to an inverse photoemission (IPES) process, then yes, you will get photons being emitted as the free electron (initially having some energy above the vacuum state) make a transition into one of the unoccupied bound state. In fact, one of the specific technique that is used in IPES is called the Bremsstrahlung Isochromat Spectroscopy (BIS).

This is a well-known experimental technique in condensed matter physics to study various properties of solids.

Zz.

After I posted this, I realized that I was sitting on this info - inverse photoionization, which I think it exactly what you're looking for. Try this:

http://doc.cern.ch/tmp/convert_SCAN-0004050.pdf
 
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  • #7
Thanks ZapperZ. In the meanwhile I think I have the answer now, which seams rather elemental. Recombination produces emission, since electrons have to step down energetic levels. It seams that some of this should be visible also in the CMB (it is called 'recombination lines').

Regards.
 
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  • #8
ZapperZ said:
*SNIP
After I posted this, I realized that I was sitting on this info - inverse photoionization, which I think it exactly what you're looking for. Try this:

http://doc.cern.ch/tmp/convert_SCAN-0004050.pdf
I got "Document not found" when I clicked on the link; am I too late?
 
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  • #9
hellfire said:
I am not sure about the answer, Nereid, this is why I asked. On the other hand it is nice that you step into the thread, because my question has ultimatively to do with cosmology…

Coulds of neutral Hydrogen may absorb high energy photons and get ionzed. As far as I know, when electrons recombine with protons, then they have to step down on energy levels and an emission takes place. But I am not sure of this.

May be my question was not correctly formulated: what I want to know is whether the formation of neutral hydrogen generates radiation. Independently whether Bremsstrahlung takes place or not (it seams it does not).

The main reason what makes me doubt is that during the cosmological recombination epoch a lot of radiation should have been generated due to the formation of neutral hydrogen. I assume that this emitted radiation was not necessarily in thermal equilibrium with the rest of the photons at 3000° K.

Since this radiation was exactly at the last scattering surface it should be visible as a clear anisotropy now. I do not remember to have seen this point mentioned in the references I read about the CMB.

I apologize for the somehow chaotic way of asking this, starting this ambiguous thread. So, may be this thread should be moved to cosmology.

Regards.
You seem to be OK with the answers so far to your questions, but are interested in, and maybe a little puzzled by, what we think was going on in the universe around the time of last scattering.

In particular, you seem to feel there should be some sort of anisotropy in the CMBR, in some way an imprint of photons emitted when protons and electrons combined to form neutral H atoms.

While I'm not sure I understand your question, I'd like to go back to the cloud of neutral H atoms and the intense source of photons - of all energies. Some H atoms will be ionised, so we - located on the other side of the cloud from the point source - should see a Lyman absorption spectrum of H in the light from the point source. But then, as you say, the electrons will recombine, emitting photons ... with the Lyman H spectrum! So how come there are still absorption lines? Well, the emission is isotropic, but the ionising radiation is not! (Lots of caveats, as always.)

At the time of last scattering, there wasn't an 'outside' to the universe, nor a 'point source', so the geometry which allows us to see absorption lines isn't the same.

Does this help?

BTW, no apologies needed; if you don't think about things and ask questions, how will you ever learn anything? :smile:
 
  • #10
Nereid said:
I got "Document not found" when I clicked on the link; am I too late?

You're right. Maybe it doesn't allow you to get it directly. Here, try this:

http://arc.cs.odu.edu:8080/dp9/getrecord/oai_dc/cds.cern.ch/oai:cds.cern.ch:SCAN-0004050

and click on the first url listed. That will (eventually) take you to the document.

Zz.
 
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  • #11
Nereid, I think I understand the example of the neutral Hydrogen cloud, but I am puzzled with your comment regarding CMB.

In the time between my first question till now, I found out the following:

During recombination, electrons are trapped by protons and form neutral hydrogen. The electrons step down to the lowest energy level. This produces the emission of a photon, which has enough energy to ionize a hydrogen atom again.

Recombination takes place anyway, since: (a) the emitted photons are redshifted and also (b) other energetic transitions take place which produce photons with lower energy.

Both kind of photons do not fit into the blackbody spectrum of the CMB (this is formed by the original radiation of the plasma) and must be somehow visible in a sort of anisotropy.

These references (I hope they are significative):

http://www-ra.phys.utas.edu.au/~rdodson/all_together_now/node253.html
http://arxiv.org/abs/astro-ph/0003227

explain that these photons should be redshifted now almost to the radio (or low microwave). They are called ‘recombination lines’.

Regards.
 
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  • #12
hellfire said:
During recombination, electrons are trapped by protons and form neutral hydrogen. The electrons step down to the lowest energy level. This produces the emission of a photon, which has enough energy to ionize a hydrogen atom again.

You need to be a bit careful here. What you have just described involved TWO separate transitions.

1. Free electron gets captured by proton. This involves a transition from an energy level ABOVE the vacuum state to a bound state. This can involve the emission of photons also. The bound state need not be stable, it can be a meta-stable state.

2. A second transition to the ground state - this can again involve another emission of photon. But note that the photon emitted here does NOT have enough energy to ionize another atom. A transition from one bound state to the next bound state within a H-atom is always less than 13.6 eV. So you will never have enough energy from the emitted photon to reionize another H atom.

So it appears that if there is any ionization taking place, it will have to come from photons from the first transition process. Depending on how energetic the free electron was before capture, it's energy is certainly high enough above the vacuum state to cause the emission of a photon larger than 13.6 eV if it is captured and settled to a deep-enough metastable state.

Zz.
 

Related to Neutral hydrogen and Bremsstrahlung

1. What is neutral hydrogen and how does it form?

Neutral hydrogen is a type of atom that consists of one proton and one electron. It is the most abundant element in the universe and can be found in stars, galaxies, and the space between them. It forms when an electron combines with a proton through the process of hydrogen recombination, which occurs when the universe cools down after the Big Bang.

2. How does neutral hydrogen interact with other particles?

Neutral hydrogen is a relatively stable atom and does not easily interact with other particles. However, it can absorb and emit photons of specific wavelengths, which is why it is commonly used in astronomical observations. It can also interact through collisions with other atoms or particles, such as in the process of ionization.

3. What is Bremsstrahlung and how does it relate to neutral hydrogen?

Bremsstrahlung, also known as braking radiation, is a type of electromagnetic radiation produced when a charged particle is accelerated by another particle. In astrophysics, this process is often observed in the interaction between neutral hydrogen atoms and high-energy electrons. When these electrons are deflected by the electric field of the atom's nucleus, they emit Bremsstrahlung radiation.

4. How do scientists study neutral hydrogen and Bremsstrahlung?

Scientists study neutral hydrogen and Bremsstrahlung through various techniques, including spectroscopy, which involves analyzing the wavelengths and intensities of light emitted or absorbed by these particles. They also use telescopes and detectors designed specifically to detect and measure these types of radiation, providing valuable insights into the composition and dynamics of the universe.

5. What is the significance of understanding neutral hydrogen and Bremsstrahlung?

Understanding neutral hydrogen and Bremsstrahlung is crucial in various fields of science, including astrophysics, cosmology, and plasma physics. These particles play important roles in the formation and evolution of galaxies, the structure of the universe, and the behavior of plasma in laboratory experiments. Furthermore, studying them can provide insights into the fundamental laws of physics and the origins of the universe.

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