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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FAQ: Einstein, Friedman and the cosmological constant

Who was Albert Einstein and what is the cosmological constant?

Albert Einstein was a theoretical physicist who developed the theory of general relativity. The cosmological constant, denoted by the Greek letter Lambda (Λ), was introduced by Einstein in 1917 as a term in his equations of general relativity to allow for a static universe. It represents a constant energy density filling space homogeneously.

What is the significance of the cosmological constant in Friedman's equations?

Alexander Friedman derived solutions to Einstein's field equations in 1922, showing that the universe could be expanding or contracting, which was contrary to the then-prevailing idea of a static universe. The cosmological constant in Friedman's equations can act as a repulsive force counteracting gravity, influencing the rate of expansion of the universe.

Why did Einstein call the cosmological constant his "biggest blunder"?

Einstein referred to the cosmological constant as his "biggest blunder" after Edwin Hubble's observations in 1929 showed that the universe is expanding. This discovery rendered the need for a cosmological constant to maintain a static universe unnecessary. Einstein felt that he had missed predicting the dynamic nature of the universe.

How has the cosmological constant been reinterpreted in modern cosmology?

In modern cosmology, the cosmological constant has been reinterpreted as a form of dark energy, which is responsible for the accelerated expansion of the universe. Observations of distant supernovae in the late 1990s provided evidence for this accelerated expansion, leading to a renewed interest in the cosmological constant.

What role does the cosmological constant play in the current understanding of the universe's fate?

The cosmological constant plays a crucial role in the current Lambda Cold Dark Matter (ΛCDM) model of cosmology. It suggests that the universe's expansion will continue to accelerate due to the presence of dark energy, potentially leading to a "Big Freeze" scenario where galaxies move farther apart, and the universe becomes increasingly cold and empty.

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