How did the CMB Lorentz frame get chosen?

  • Thread starter Thread starter Sam_Playle
  • Start date Start date
  • Tags Tags
    Cmb Frame Lorentz
AI Thread Summary
The cosmic microwave background (CMB) exhibits anisotropy, with a temperature dipole that varies by ±0.00335 K, defining a Lorentz frame that can be adjusted to make this dipole vanish. This adjustment suggests a spontaneous breaking of Lorentz symmetry, raising questions about when and how this breaking occurred—whether at the Universe's inception or during recombination. The discussion highlights that Lorentz frames are local and do not account for the curvature and expansion of spacetime, which are essential in cosmology governed by general relativity. The choice of the CMB frame is debated, with considerations of whether it reflects a local matter rest frame or a more fundamental aspect of the Universe's evolution since the Big Bang. The inquiry remains open regarding the historical and cosmological reasons for selecting this specific frame over others.
Sam_Playle
Messages
3
Reaction score
0
The cosmic microwave background is anisotropic: the temperature is distributed as a dipole with the temperature at the poles differing by ±0.00335 K from the mean.

This defines a Lorentz frame: we can boost by several hundred km/s to make the dipole vanish, on average. This new frame could be considered the rest frame of the CMB.

The laws of Physics are Lorentz invariant, so this appears to require spontaneous breaking of Lorentz symmetry by the CMB.

My question is: how and when is this breaking supposed to have occurred? Must the frame have been chosen at the start of the Universe, or is it possible for a Lorentz-invariant early Universe to break its symmetry at recombination?

Could there be topological defects that are remnants of recombination when we try to define the CMB frame globally?
 
Space news on Phys.org
A curved spacetime, or one with spatial expansion, does not have global poincaré symmetry. So from the start the U did not have the kind of symmetry you are talking about. So it did not need to be broken.

Lorentz frames do not describe things globally, they have no curvature, they do not expand.

Cosmology deals with a GR world, not an SR world. It is very different. Just by boosting you only get a LOCAL Lorentz frame that is at CMB rest--it only approximately fits reality. If you travel very far, or let substantial time elapse, you begin to realize how bad the fit is.

Maybe somebody else can take over and make this clearer, I have to do something else.
Sam_Playle said:
The cosmic microwave background is anisotropic: the temperature is distributed as a dipole with the temperature at the poles differing by ±0.00335 K from the mean.

This defines a Lorentz frame: we can boost by several hundred km/s to make the dipole vanish, on average. This new frame could be considered the rest frame of the CMB.

The laws of Physics are Lorentz invariant, so this appears to require spontaneous breaking of Lorentz symmetry by the CMB.

My question is: how and when is this breaking supposed to have occurred? Must the frame have been chosen at the start of the Universe, or is it possible for a Lorentz-invariant early Universe to break its symmetry at recombination?

Could there be topological defects that are remnants of recombination when we try to define the CMB frame globally?
 
Thanks. My question, then, is why is it this particular frame, and not another one? What is the cosmological origin? The CMB would seem to define (modulo SO(3)) a section of the frame bundle on spacetime; why is it the section that it is, instead of a different one? What is the historical fact leading to it?

marcus said:
A curved spacetime, or one with spatial expansion, does not have global poincaré symmetry. So from the start the U did not have the kind of symmetry you are talking about. So it did not need to be broken.

Lorentz frames do not describe things globally, they have no curvature, they do not expand.

Cosmology deals with a GR world, not an SR world. It is very different. Just by boosting you only get a LOCAL Lorentz frame that is at CMB rest--it only approximately fits reality. If you travel very far, or let substantial time elapse, you begin to realize how bad the fit is.

Maybe somebody else can take over and make this clearer, I have to do something else.
 
Hi Sam, I had to be out this afternoon and just got back. Isn't it true that as soon as you have matter in the picture you have picked out a section of the frame bundle? One in which the local matter, on average, isn't going anywhere?
I'm kind of surprised no one else stepped into answer your question in the past 3 hours.

I'll think a bit more about it and get back to this thead later.
 
Echoing marcus point, Lorentz invariance, like special relativity, can only be applied to local reference frames. It does not apply to the universe as a whole, which is governed by general relativity. Were this not true we would have universal laws of conservation, which is not supported by observational evidence.
 
Thanks for your replies. I am convinced that no laws are violated. However, this doesn't sate my curiosity. I want to know how this frame bundle was picked, as opposed to another one, which, a priori, would be equally permissible.

Is the local choice of frame just the rest frame of some matter in the plasma right before recombination? Or does it go back further - does the CMB section of the frame bundle define a Cauchy surface which is, in principle, the time evolution of a special Cauchy surface fixed since the big bang?
 
https://en.wikipedia.org/wiki/Recombination_(cosmology) Was a matter density right after the decoupling low enough to consider the vacuum as the actual vacuum, and not the medium through which the light propagates with the speed lower than ##({\epsilon_0\mu_0})^{-1/2}##? I'm asking this in context of the calculation of the observable universe radius, where the time integral of the inverse of the scale factor is multiplied by the constant speed of light ##c##.
The formal paper is here. The Rutgers University news has published a story about an image being closely examined at their New Brunswick campus. Here is an excerpt: Computer modeling of the gravitational lens by Keeton and Eid showed that the four visible foreground galaxies causing the gravitational bending couldn’t explain the details of the five-image pattern. Only with the addition of a large, invisible mass, in this case, a dark matter halo, could the model match the observations...
Hi, I’m pretty new to cosmology and I’m trying to get my head around the Big Bang and the potential infinite extent of the universe as a whole. There’s lots of misleading info out there but this forum and a few others have helped me and I just wanted to check I have the right idea. The Big Bang was the creation of space and time. At this instant t=0 space was infinite in size but the scale factor was zero. I’m picturing it (hopefully correctly) like an excel spreadsheet with infinite...
Back
Top