Einstein, Friedman and the cosmological constant

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In summary, Einstein initially based his considerations on the cosmological implications of general relativity on two hypotheses: the cosmological principle and a static universe. However, Friedman later showed that it was possible to preserve the cosmological principle without introducing the cosmological constant, as long as the assumption of a static universe was dropped. Friedmann's original solutions did not include the cosmological constant, but later developments have shown that it is possible to have solutions with a nonzero cosmological constant. Einstein was likely aware of these developments and may have discounted them due to his personal dislike of the cosmological constant. However, the modern viewpoint is that the cosmological constant should be included in the equations, and its actual value can only be determined empirically.
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Jaime Rudas
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In Appendix 4 of the book "Relativity, The Special and General Theory", Einstein describes the evolution of the cosmological implications of general relativity as follows:

My original considerations on the subject were based on two hypotheses:
(1)There exists an average density of matter in the whole of space which is everywhere the same and different from zero.
(2)The magnitude (“radius”) of space is independent of time.
Both these hypotheses proved to be consistent, according to the general theory of relativity, but only after a hypothetical term was added to the field equations, a term which was not required by the theory as such nor did it seem natural from a theoretical point of view (“cosmological term of the field equations”).
Hypothesis (2) appeared unavoidable to me at the time, since I thought that one would get into bottomless speculations if one departed from it.
However, already in the twenties, the Russian mathematician Friedman showed that a different hypothesis was natural from a purely theoretical point of view. He realized that it was possible to preserve hypothesis (1) without introducing the less natural cosmological term into the field equations of gravitation, if one was ready to drop hypothesis (2)."

From this, I interpret that Friedman's solutions don't include the cosmological constant, however, they do. Am I misinterpreting?
 
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Friedman's solutions can include the cosmological constant but they don't have to. It's only if you are trying to fit certain growth rate histories - such as reality or Einstein's static universe - that you need to introduce a non-zero cosmological constant.
 
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Look at what's being said:
Jaime Rudas said:
(1)There exists an average density of matter in the whole of space which is everywhere the same and different from zero.
the cosmological principle holds
Jaime Rudas said:
(2)The magnitude (“radius”) of space is independent of time.
the universe is static
Jaime Rudas said:
He realized that it was possible to preserve hypothesis (1) without introducing the less natural cosmological term into the field equations of gravitation, if one was ready to drop hypothesis (2)."
but you can very well have a universe with the cosmological principle that is not static, in which case lambda is optional.

All he's saying here is that he was too married to the idea of a static universe
 
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Jaime Rudas said:
From this, I interpret that Friedman's solutions don't include the cosmological constant
Friedmann's original solutions did not. But we now know that it is perfectly possible to have solutions which are not static but which do include the cosmological constant, and our modern version of Friedmann's equations include this possibility.
 
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  • #5
PeterDonis said:
Friedmann's original solutions did not.
A translation of the original Friedmann's 1922 paper can be seen at the following link:

https://cosmology.education/documents/friedmann_1922.pdf

Equations (12) and (13) are the Friedmann's equations that includes the cosmological constant λ.

After equation (17), Friedmann presents the non-stationary models and states:

"We most base the consideration of the nonstationary world on equations (14) and (15). The quantity λ is not determined by these equations. We shall postulate that it can have an arbitrary value."

Therefore, I consider that Friedmann's original solutions do include the cosmological constant.
 
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Jaime Rudas said:
Equations (12) and (13) are the Friedmann's equations that includes the cosmological constant λ.

After equation (17), Friedmann presents the non-stationary models and states:

"We most base the consideration of the nonstationary world on equations (14) and (15). The quantity λ is not determined by these equations. We shall postulate that it can have an arbitrary value."
Hm, interesting, I wasn't aware of that.

That could mean that Einstein, in the quote you give in your OP, was simply referring to the possibility of ##\Lambda = 0##, which is only a possibility if the static assumption is dropped. Or he might be referring to either a different paper by Friedmann, or some more informal unpublished discussion or notes. Einstein regularly communicated by letter with many other physicists, and he also was well informed about things like conference proceedings in which results that might not appear in the published literature were discussed.

It seems clear from other writings of Einstein that he was not happy with the cosmological constant (he called it "the greatest blunder of my life" after evidence for the expansion of the universe was discovered), so he might have discounted the models Friedmann proposed with a nonzero ##\Lambda## once the possibility of an expanding solution with ##\Lambda = 0## was clear to him. But of course the modern viewpoint is that the cosmological constant, on purely theoretical grounds, should be there; the question is what its actual value is, and that question we can only answer empirically, at least at our current level of knowledge.
 
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1. Who is Einstein and what is his contribution to the cosmological constant?

Einstein was a renowned physicist who proposed the theory of general relativity, which describes the relationship between gravity and the curvature of space-time. In his theory, he introduced the concept of the cosmological constant, a term that represents the energy density of empty space and can be used to explain the expansion of the universe.

2. What is the significance of Friedman's work in relation to the cosmological constant?

Alexander Friedman was a Russian mathematician who used Einstein's theory of general relativity to develop mathematical models of the universe. His work showed that the universe could either be expanding or contracting, and the value of the cosmological constant played a crucial role in determining the fate of the universe.

3. What is the current understanding of the cosmological constant?

Currently, the cosmological constant is thought to represent the energy density of the vacuum of space. It is often referred to as dark energy and is believed to be responsible for the accelerating expansion of the universe. However, the exact nature and value of the cosmological constant are still not fully understood.

4. How does the cosmological constant relate to the concept of the "Big Bang"?

The cosmological constant is closely related to the Big Bang theory, which states that the universe began as a singularity and has been expanding ever since. The value of the cosmological constant can affect the rate of expansion of the universe, which in turn can impact the age and size of the universe as predicted by the Big Bang theory.

5. Are there any ongoing research or developments related to the cosmological constant?

Yes, there is ongoing research and debate surrounding the cosmological constant, as scientists continue to try and understand its exact value and role in the universe. Some are exploring alternative theories to explain the accelerating expansion of the universe, while others are conducting experiments to measure the value of the cosmological constant more accurately.

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