Were Population III stars powered entirely by p-p fusion?

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Discussion Overview

The discussion centers on the fusion processes powering Population III stars, particularly whether they were entirely powered by the proton-proton (p-p) fusion cycle or if other processes, such as the CNO cycle and helium fusion, played a role. Participants explore theoretical implications, simulations, and the conditions under which these stars operated, including their evolutionary timelines and the production of heavier elements.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants assert that Population III stars, being metal-free, could not initially activate the CNO cycle and were primarily powered by the p-p chain until they produced sufficient carbon through helium burning.
  • Others reference simulations indicating that for massive Population III stars, the CNO cycle becomes dominant relatively quickly after the initial formation of heavier elements.
  • There is a suggestion that helium fusion (triple-alpha process) might also occur alongside p-p fusion in these stars, raising questions about the conditions necessary for these processes to coexist.
  • Some participants discuss the implications of low-probability reactions occurring in massive stars, suggesting that these stars may have rapidly transitioned to helium burning as soon as helium was available.
  • Concerns are raised about whether p-p fusion alone could sustain the massive stars, given its slower rate compared to other fusion processes.
  • There is speculation about the characteristics of Population III red dwarf stars, including their fusion rates and lifetimes compared to modern red dwarfs, with differing opinions on whether they would burn faster or slower.

Areas of Agreement / Disagreement

Participants express differing views on the dominant fusion processes in Population III stars, with some asserting the primacy of the p-p chain and others emphasizing the role of the CNO cycle and helium fusion. The discussion remains unresolved regarding the exact mechanisms and timelines of these processes.

Contextual Notes

Participants note limitations in understanding the initial conditions and fusion processes of Population III stars, including the dependence on definitions of metallicity and the complexities of stellar evolution models.

Who May Find This Useful

Astronomers, astrophysicists, and students interested in stellar evolution, particularly in the context of early universe cosmology and the formation of the first stars.

bbbl67
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In modern stars, the more massive a star is, the more likely that it is powered by the CNO fusion cycle, where Carbon, Nitrogen, an Oxygen act as catalysts for creating helium from hydrogen. In stars over 1.3 solar masses, this is the primary fusion process. Below that that level it's a mix of the CNO and P-P cycles. P-P is supposed to be much slower than CNO, since it uses no catalysts. Since neither Carbon, Nitrogen, nor Oxygen existed during the Pop III epoch, were all of these massive stars powered simply by the P-P cycle? Well at least entirely P-P until they produced the CNO internally eventually?
 
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Yes. If a star truly has no elements heavier than helium, then it can't use the CNO cycle, at least not at first.

From Section 2.3 of Yoon, Dierks, and Langer (2012), Astronomy and Astrophysics, 542, A113:

"In metal-free massive stars, the CNO cycle cannot be activated initially. Because the energy generation due to the pp [proton-proton] chain is too weak to support a massive star with M ≥ 20 MSun for a significant fraction of the evolutionary time, the stellar core rapidly contracts until enough carbon . . . is produced by helium burning . . . . Hydrogen burning with the CNO cycle only begins thereafter."
 
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CygnusX-1 said:
"In metal-free massive stars, the CNO cycle cannot be activated initially. Because the energy generation due to the pp [proton-proton] chain is too weak to support a massive star with M ≥ 20 MSun for a significant fraction of the evolutionary time, the stellar core rapidly contracts until enough carbon . . . is produced by helium burning . . . . Hydrogen burning with the CNO cycle only begins thereafter."

So it sounds like Helium fusion (triple-alpha?) is also going on, and it's not just p-p chain?
 
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Something must be going on to get C, N, O.
 
I did some simulations of massive Population-3 stars using the stellar simulator MESA (http://mesa.sourceforge.net/). for a course I took in graduate school. For a 50 solar mass star, it only took about 1000 years to produce enough heavier elements for the CNO cycle to become dominant. Since the star lives for 10^5-10^6 years, it spends most of its time with the CNO cycle dominating.
 
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phyzguy said:
I did some simulations of massive Population-3 stars using the stellar simulator MESA (http://mesa.sourceforge.net/). for a course I took in graduate school. For a 50 solar mass star, it only took about 1000 years to produce enough heavier elements for the CNO cycle to become dominant. Since the star lives for 10^5-10^6 years, it spends most of its time with the CNO cycle dominating.
Wow, only 1000 years? I was guestimating a million years at least. So those first stars were already doing simultaneous helium fusion at the same time as hydrogen fusion in their cores?
 
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Matterwave said:
So it sounds like Helium fusion (triple-alpha?) is also going on, and it's not just p-p chain?

Is it just a matter of these two?
In high metallicity, low mass stars, protium is fused and nearly completely consumed at core temperatures of 15 million K or not much more. Triple alpha only ignites at about 100 million K, by which time protium is nearly completely gone.

But pp chain has branches.
Namely these are:
1)3He+α→7Be+γ
2)7Be+e-7Li+νe
3)7Li+p→2α
and
4)7Be+p→8B+γ
5)8B→8Be+e+e
6)8Be→2α

Note that both these branches cycle to 2α
Triple alpha process is:
7)α+α→8Be
8)8Be+α→12C

Triple alpha has very low probability because the lifetime of 8Be is just 10-16 s to process 6 which is spontaneous. Very many 8Be nuclei must form and spontaneously decay for one to turn to 12C. So triple alpha needs extremely high temperature, where 7) is a bit more frequent.
But 8B has spontaneous decay lifetime of about 1 s, and the lifetimes of 7Be and 7Li are only limited by nonspontaneous processes.
Could there be any noticeable branch processes, at high temperature:
7Be+α→?
7Li+α→?
8B+α→?
 
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-Pair instability? I suspect you would have carbon after a pair-instability pulse. I have not read anything on that.

-Gravitational collapse should heat population III stars for awhile.

-Tides, should be minor.
 
snorkack said:
Triple alpha has very low probability because the lifetime of 8Be is just 10-16 s to process 6 which is spontaneous. Very many 8Be nuclei must form and spontaneously decay for one to turn to 12C. So triple alpha needs extremely high temperature, where 7) is a bit more frequent.
But 8B has spontaneous decay lifetime of about 1 s, and the lifetimes of 7Be and 7Li are only limited by nonspontaneous processes.
Could there be any noticeable branch processes, at high temperature:
7Be+α→?
7Li+α→?
8B+α→?
2He (diproton) also has a pretty low half-life of much less than 10-9, so lots of low-probability reactions happening all at once? These stars were so massive that they brute-forced a whole bunch of low-probability reactions at once, they went straight to helium burning as soon as they got any helium to burn.

Also as a side question, they think they just discovered the first-ever Pop III red dwarf star in our galaxy. A 1st generation red dwarf would have even less CNO present inside it than today's red dwarfs, and almost no way of making their own internally, unlike the Pop III supergiants. So would this type of red dwarf be an even slower burner than modern red dwarfs? Therefore would it last even longer than most modern red dwarfs?
 
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  • #10
bbbl67 said:
These stars were so massive that they brute-forced a whole bunch of low-probability reactions at once, they went straight to helium burning as soon as they got any helium to burn.
Obviously not. They had primordial helium, yet they were not fusing it as protostars - they were too cool for that.
bbbl67 said:
Also as a side question, they think they just discovered the first-ever Pop III red dwarf star in our galaxy. A 1st generation red dwarf would have even less CNO present inside it than today's red dwarfs, and almost no way of making their own internally, unlike the Pop III supergiants. So would this type of red dwarf be an even slower burner than modern red dwarfs? Therefore would it last even longer than most modern red dwarfs?
No.
A low metallicity red dwarf should be faster burner.
The reason is that the contracting protostar reaches main sequence when heat radiating through the star´s envelope matches fusion heat produced in the core.
A low metallicity, low temperature star should lack the ion opacity possessed by high metallicity, low temperature stars, having only the free electron opacity. Therefore low metallicity, low mass star should, because of its poorer insulation, continue shrinking and reach main sequence at higher interior temperature, higher luminosity and lower lifetime than a high metallicity, low mass star.
 
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  • #11
snorkack said:
Obviously not. They had primordial helium, yet they were not fusing it as protostars - they were too cool for that.
Okay, yes they should have BB helium already inside them, I forgot about that. But does PP fusion alone produce enough power to keep such massive stars inflated, considering it's such a slow fusion process? Or would these stars have to collapse and heat up further to get enough power production?
No.
A low metallicity red dwarf should be faster burner.
The reason is that the contracting protostar reaches main sequence when heat radiating through the star´s envelope matches fusion heat produced in the core.
A low metallicity, low temperature star should lack the ion opacity possessed by high metallicity, low temperature stars, having only the free electron opacity. Therefore low metallicity, low mass star should, because of its poorer insulation, continue shrinking and reach main sequence at higher interior temperature, higher luminosity and lower lifetime than a high metallicity, low mass star.
How much of a difference to lifetimes would this make?
 
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  • #12
bbbl67 said:
Okay, yes they should have BB helium already inside them, I forgot about that. But does PP fusion alone produce enough power to keep such massive stars inflated, considering it's such a slow fusion process? Or would these stars have to collapse and heat up further to get enough power production?
...
PP fusion rate is dependent on both temperature and pressure. The rate will be enough to prevent further collapse.
 
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