What Lies Between the CMB and the First Stars?

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Discussion Overview

The discussion revolves around the nature of the Cosmic Microwave Background (CMB) and the conditions between the CMB and the formation of the first stars. Participants explore the implications of temperature changes in the early universe, the transition from a plasma to a gas, and the visibility of the CMB in relation to early cosmic structures.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants describe the CMB as a "bubble" or "surface of last scattering" at around 3000 K, suggesting a transition to a state of blackness before the first stars ignited.
  • Others clarify that the term "bubble" may imply a point origin, which is misleading, and emphasize that the expansion of the universe did not occur from a single point.
  • It is proposed that once the temperature of hydrogen dropped below 3000 K, it ceased to radiate detectable light, leading to a period of darkness until stellar fusion began.
  • Some participants argue that the transition from plasma to gas was not instantaneous, which affects the visibility of the CMB and suggests a blurring effect on the observed data.
  • There is a discussion about the nature of radiation from ideal black bodies versus transparent bodies, noting that the early universe closely resembles these extremes.
  • One participant mentions that the CMB power spectrum shows a tapering off of shorter wavelengths, indicating the gradual cooling process and its impact on visibility.

Areas of Agreement / Disagreement

Participants express differing views on the interpretation of the CMB and the transition from plasma to gas. While some agree on the general timeline and conditions, there is no consensus on the implications of these transitions or the terminology used to describe them.

Contextual Notes

The discussion highlights limitations in understanding the exact nature of the transition from the CMB to the first stars, including assumptions about temperature, opacity, and the characteristics of radiation in the early universe.

  • #31
phinds said:
My understanding is that it evolved over at least thousands of years.
Fair enough: the [checks dictionary] dictionary definition of "flash" just says a very non-scientific "brief". It's just a colloquialism and precisely zero time would be an impossible constraint on basically anything considered a "flash" (lightning, a camera light, bomb explosion) if one wanted to zoom in far enough on the "event" (also scientifically incorrect usage). For exactly the same reason (the same cause) it would be technically incorrect to call the CMB "homogeneous", or even to call the SLC a "surface", but I wouldn't quibble with that either if someone left off a non-scientific qualifier like "almost".

Regardless, none of this has any bearing on the question being asked and if anything applying a duration can lead him on the wrong track.
 
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  • #32
russ_watters said:
Regardless, none of this has any bearing on the question being asked and if anything applying a duration can lead him on the wrong track.
I agree, which is why I gave the longer answer explaining what is actually going on after pointing out that there was no "flash" (and I agree w/ what has been said about the actual duration not be a flash in the strictest technical meaning of that word but still an extremely brief time cosmological terms).
 
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  • #33
@Pedro Paixao I think my response could have been more courteously worded. Something like "if by 'flash' you mean one point in time, that's not quite right. The surface of last scattering evolved over thousands of years" followed by the rest of what I said.
 
  • #34
Let me try to paint a new picture:

Typically the first time a person hears about the Big Bang it's an explosion, which is where I think people get the idea of a flash that happens/is seen and then is gone. Regardless of the actual duration, it is a short event - a flash. If you are far away from an explosion, that's what you see: the light from the explosion travels outward in a sphere until it reaches you, then it is gone.

For the Big Bang and CMB, imagine you are a long-lived being who was capable of surviving in the very early universe. Early on, the universe would have looked similar to what it is like flying through a cloud in a plane; nothing but bright light in all directions, from close by.

When the universe suddenly* became transparent, it would have been like a suddenly dissipating cloud. But because this cloud is really, really big, you can watch it dissipate over time, as the last vestiges of light from further and further away reach you. A billion years after it dissipated, you see light that had to travel a billion light years to reach you at the moment of dissipation. Ten billion years after it dissipated, you see light that had to travel ten billion light years to get to you. You're seeing the cloud dissipate, from the inside, as an expanding sphere of transparency. That is why you can witness such a brief event for a long time.

*not instantly, but close enough relative to the timescale of the story.
 
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  • #35
Got it. Thank you guys!
 
  • #36
Imagine being in an infinitely large room filled uniformly with photographers. Suppose they've got the old flash bulb type cameras. Imagine they all snap your picture at the same time: what would you see? You'd see an outwardly expanding ring of light as the flashes from ever further, equidistant cameras reach you.

The photographers snapping the picture is the "last scattering" of CMB photons as the universe becomes transparent. (Yes, it's true the real CMB was not generated instantaneously like this, but it's a fine assumption for what we're talking about). The ring of light seen moment to moment is the last scattering sphere of the CMB, likewise seen moment to moment.

The key is recognizing that the CMB photons were spread uniformly throughout the cosmos prior to their release from the baryon photon plasma.
 
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  • #37
CMB photons did not decouple all at once. The oft quoted figure of 380,00 years as the age of the universe when CMB photons were last scattered represents the most likely age at which any given CMB photon was emitted. CMB photons continued to be released for another 115,000 years thereafter, and over a correspondingly similar time period prior to age 380,000 years, according to this excerpt:

'The thickness of the LSS refers to the fact that the decoupling of the photons and baryons does not happen instantaneously, but instead requires an appreciable fraction of the age of the Universe up to that era. One method to quantify exactly how long this process took uses the photon visibility function (PVF). This function is defined so that, denoting the PVF by P(t), the probability that a CMB photon last scattered between time t and t+dt is given by P(t)dt.

The maximum of the PVF (the time where it is most likely that a given CMB photon last scattered) is known quite precisely. The first-year WMAP results put the time at which P(t) is maximum as 372 +/- 14 kyr . This is often taken as the "time" at which the CMB formed. However, to figure out how long it took the photons and baryons to decouple, we need a measure of the width of the PVF. The WMAP team finds that the PVF is greater than half of its maximum value (the "full width at half maximum", of FWHM) over an interval of 115 +/- 5 kyr. By this measure, decoupling took place over roughly 115,000 years, and when it was complete, the universe was roughly 487,000 years old."

ref: http://cs.mcgill.ca/~rwest/wikispeedia/wpcd/wp/c/Cosmic_microwave_background_radiation.htm
 
  • #38
Chronos said:
The maximum of the PVF (the time where it is most likely that a given CMB photon last scattered) is known quite precisely. The first-year WMAP results put the time at which P(t) is maximum as 372 +/- 14 kyr . This is often taken as the "time" at which the CMB formed. However, to figure out how long it took the photons and baryons to decouple, we need a measure of the width of the PVF. The WMAP team finds that the PVF is greater than half of its maximum value (the "full width at half maximum", of FWHM) over an interval of 115 +/- 5 kyr. By this measure, decoupling took place over roughly 115,000 years, and when it was complete, the universe was roughly 487,000 years old."

ref: http://cs.mcgill.ca/~rwest/wikispeedia/wpcd/wp/c/Cosmic_microwave_background_radiation.htm
This looks like there's a factor of two error in the estimate. I believe that 115,000 years would be the full duration during which photons were emitted (well, at least the full duration where the emission rate was greater than half the peak: photons would have been emitted before and after at lower rates). So the approximate time where the photon emission dropped below half the peak emission rate would be somewhere near 57,500 years after the peak emission time, not 115,000 years.
 

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