Open access peer-reviewed chapter

Small-Bang versus Big-Bang Cosmology

By Antonio Alfonso-Faus

Submitted: December 23rd 2010Reviewed: March 28th 2011Published: September 9th 2011

DOI: 10.5772/25138

Downloaded: 1099

1. Introduction

During the 1920´s the U.S. astronomer Hubble observed that the red shifts, from distant galaxies, were increasing with distance. The similarity with the well known Doppler Effect gave the way to a rapidly spreading idea: that the universe was expanding. Galaxies were thought to be receding from us at a speed proportional to their distance. Considering the universe as a “gas” of galaxies, each galaxy similar to one molecule in a gas, the expansion clearly implied that the universe was getting cooler and thinner with age. We know today that this cooling and thinning is correct: the universe is very old and its known temperature and density for today are very low: 2.7ºK (the cosmic microwave background radiation) of temperature and about 10-29 grams/cc average density.

Now, if we imagine a thought experiment and reverse the time, going backwards, we get the idea of a very hot and very dense universe at its initial stages. Going to the limit, getting closer and closer to a theoretically zero time, we have a mathematical singularity: infinite temperature and infinite density. As a result of this initial picture, we can imagine that these infinites were the result of a very big and sudden explosion: and that it expanded rapidly to a lower and lower temperature and density. Today we observe a cool temperature and a thin “gas”. The British astronomer and cosmologist Fred Hoyle ironically called this a “Big-Bang”. But if we take the imagination of a Big-Bang explosion as a fact, as many people have done, we are entitled to take as a fact too that a gas after an explosion decelerates to a lower and lower speed of expansion. Today we should observe a decelerating universe. And this is not the case.

Initial expansion (according to a hypothetical Big-Bang), and present acceleration of the universe, as observed thanks to the astrophysics of the supernovae Type Ia, are two very different things. While the expansion is very well based on observation, following the Hubble´s red shift findings, an initial explosion at a space-time point, the Big-Bang, is the result of a mathematical extrapolation, and therefore so far it is only speculation. On the other hand, the accelerated expansion of the universe is based on observation [1]. It is the result of the successful application of the scientific method, like the case of the expansion of the universe. Accelerated expansion is a very well based observation on scientific grounds, and in a direct way. This is not so for the assumed Big-Bang initial explosion.

It is very interesting to note that the cosmological model of a Big-Bang, as a frame of work, has been and still is the underpinning of the majority of the research work done in cosmology. It had, and still has, many drawbacks. One of them, a very serious one, was related to the fact that it could not explain the present size of the universe. Following the initial developments of this model the present size of the universe would be very small: may be of the order of meters. Obviously this is not the case, and one had to look for an explanation. Instead of looking for an alternative model, something that the many drawbacks of the model has demanded many times, the main stream of the scientific community in cosmology has always decided to add more and more “ad hoc” explanations to keep this frame of work alive. And it appears that this is going to go on for a long time. There is so much work, interests, beliefs, efforts, etc, behind the Big-Bang idea that the overall worldwide inertia created by this cosmological model is very big indeed.

At any rate, some of the “ad hoc” explanations to sustain the main stream ideas could be good ones. I mean good ones when one considers them isolated, independent of the reason that made them come into existence. For example: INFLATION. A very fast exponential expansion at the very early stages of the universe would bring it close to a reasonable size to avoid discrepancies. It has some predictions, flat universe, critical density, cosmic microwave background radiation properties (CMBR) etc. that have been observed. Then, it seems to be a good idea, a good scientific approach supported by the confirmation of some of its predictions.

Again, if one accepts INFLATION as a beginning of the universe, a fast exponential expansion during a very short time, one immediately imagines that after inflation a period of deceleration should follow. This is the case, but there is more to it. As mentioned above, during the last half of the age of the universe there is an observed accelerated expansion. And of course this must have a reason, a physical push to expand the universe. This physical mechanism must be of universal significance, because it has been accelerating the whole universe during the last half of its age. And during the first half it counteracted the inertial deceleration after inflation due to the gravitational universal attraction. And it reversed the deceleration giving the accelerated expansion we observe today. About half way in time the deceleration-acceleration transition implied zero acceleration. We see no need of an initial point like explosion. Inflation does the job.

History has already gone through this state of affairs. Almost one hundred years ago, when Einstein developed his cosmological equations, the general belief was to imagine the universe in a static state. Since gravitation was well known, as an attractive force, soon it was realized that a collapse was inevitable due to the pull of gravity. But no collapsing universe was observed. Then a pushing mechanism should be balancing gravitation to get a static universe. And Einstein introduced his well known cosmological constant, the lambda constant. Today we observe the universe in an accelerated expansion during the last half of its age. Then a kind of pushing mechanism is again required to explain this observation. And it could be a question of strength: the pushing force due to the Λ “constant” seems to be growing as the universe expands. On the contrary, the overall gravitational force is constant. This is enough to explain by itself the present acceleration of the expansion of the universe. And it may arrive at a disaggregation of everything in a finite time: expansion to infinity. Since the lambda constant is a very well known physical construct, the attention of most cosmologists is again in favor of such solution. The point is that such a Λ constant implies energy, and the immediate and easy way out is to imagine the existence of a kind of dark energy to explain Λ, so dark that no one has seen it yet. We do not know of any interaction between this postulated dark energy and any other well known energy we are used to observe and identify. So far, the dark energy is just a theoretical construct. But we have more choices to explain this pushing force. Aside from believing in dark energy one can believe in an equivalent mechanism to explain the push: creation of matter, as we will see [2]. Then the sequence of events to explain the dynamics of the universe would be: fast exponential inflation, and then a slow deceleration followed by a slow acceleration as of today. And our prediction is that this late acceleration is increasing and that it will disperse the whole universe to infinity in a finite time. Like a kind of second inflation at the end of the time of the universe as we know it. We may be now at about one half of the total age of our universe. The creation pressure [2] is always present, growing, and its effects are permanently present till the final stage.

Following the arguments given above, we can make now a straight forward proposal: there was no big bang at all. Instead we can say that we are the result of an initial small bang, just after inflation of an initial fluctuation, an initial quantum black hole whose inflation a little later decelerated. But this deceleration was overcome by the push of the creation pressure, the continuous creation of matter [2], [3], [4] and [5]. As we will see, most physicals properties of the universe are subject to this increase with time.

The above considerations are in agreement with the idea that the universe is a kind of black hole [6]. Black holes have a characteristic mass-size relation. Taking the gravitational constant G and the speed of light c as units, G = c = 1, the black hole mass M is equal to his size L, within a factor of 2. Then, dividing the size L by the speed of light c one gets a characteristic time t for the black hole. In these units 1 second equals 3x1010 cm, and this equals 1040 grams. We then have:

(~2) M = L = tE1

For the universe M = L = t 1056 grams 1028 cm 1010 years. For the Planck scale, a quantum black hole, one has to divide (Eq. 1) by 1061 to get the Planck´s units m = l = t 10-5 grams 10-33cms 10-44 seconds. Possibly this may be the first quantum of everything in our universe. All the basic physical properties at the Planck scale (the so called natural units) differ by the factor 10-61 from the scale of the universe.

2. Scale cosmology

It looks like the universe can be considered to be structured in different scales. Each scale is a quantum black hole, as we will see, and is in itself a universe too. A black hole has its mass M and its size L connected by the simple relation

(~2) GM/c2= LE2

On the other hand, a quantum black hole is characterized by its size L being equal to its the de Broglie wavelength (with a generalized Planck´s constant H)

=H/McE3

Now, combining (Eq. 2) and (Eq. 3) we get (for a general quantum black hole) the mass M, length L and time t as follows

= (Hc/G)1/2= (GH/c3)1/2= (GH/c5)1/2E4

If we use the natural Planck´s constant ђ in (Eq. 4) we get the Planck´s units

mp= (ђc/G)1/2    2.177 105grams lp= (Gђ/c3)1/2   1.616 1033cms tp= (Gђ/c5)1/2   5.39 1044secE5

The scale of our universe is found to be the Planck´s scale (Eq. 5) multiplied by the factor 1061or, equivalently, by using a universal Planck´s constant H ≈ 10122 ђ giving

Mu= (Hc/G)1/2   1056gramsLu= (GH/c3)1/2  1028cmstu= (GH/c5)1/2  5 1017sec E6

There is a new scale that can be defined below the Planck´s scale. The point is that the quantum of gravity [7] has a mass mg given by

mg= ђ/c2tu  2 1066gramsE7

and it defines a scale like Planck´s scale multiplied by, once again, the factor 10-61. This is equivalent to obtain this new scale by using an equivalent generalized Planck´s constant H ≈ 10-122 ђ giving the sub-Planck scale

msp= 1061(ђc/G)1/2     2 1066grams lsp= 1061 (Gђ/c3)1/2       1094cmstsp= 1061 (Gђ/c5)1/2      10104secE8

The physical meaning of the sub-Planckian scale (Eq. 8) is not yet very well known, except for the concept of the quantum of gravity mg that we have introduced [7] in the past. It may also have a meaning related to information [8]: in a parallel way it can be given a sense as the unit of information, the bit, with the physical properties in (Eq. 8). We can also give some sense for a quantum of time, defined as the minimum interval of time obtained using the mass of the universe

tsp= ђ/Muc2 10104secE9

This is a very suggestive relation: it means that the sub-Planckian scale (Eq. 8) gives us the minimum quantum of mass, length and time. The three quantum black hole scales, (Eq. 5), (Eq. 6) and (Eq. 8) are then the minimum scale (Eq. 8), sub-Planckian, the “natural” scale (Eq. 5), Planckian, and the scale of the universe (Eq. 6) where we live.

There is a new physical parallel that gives a meaning to the sub-Planckian “quantum”. It may be regarded as the unit of information, the bit [8]

3. Gravity as an emerging entropic force

Verlinde [9] has introduced the concept of the force of gravity as due to a gradient of entropy S, i.e. gravity as an emergent entropic force. Though the change in entropy S may be due to internal redistribution of masses in the system, it may also be due to a cosmological increase of mass with time, as we will see here. The basic idea can be expressed as the relation between temperature T, entropy S and energy Mc2, according to the thermodynamic relation

Δ= ΔMc2 =Δt/2E10

We have used the Machian black hole relation 2GM/c2 = ct to obtain the last term in ((10)) Dealing with a “quantum” black hole universe with H ≈ 10122 ђ, we have equations (1), and (Eq. 2), and using the Hawking [10] and Bekenstein [11] black hole relation for the entropy S

= 4π k/ђc GM2E11

we get from (Eq. 11), with G = c = ђ = k =1

Δ= 4π 2M ΔME12

And using (Eq. 10) and (Eq. 12) we have

Δ= 2π TtΔ= Δt/2E13

i.e.

4π Tt = k/h= 1E14

Then temperature varies inversely proportional to cosmological time. This is a well known relation in our universe. But here we have a surprising possibility: since the temperature T is a statistical parameter, then the time t may have this character too.

The mass of the universe must be time varying [14], so that the gradient of M in (Eq. 12) is responsible for the increase in entropy ΔS, and therefore for the force of gravity. Verlinde´s ideas [9] may be extended to a distribution of mass in the whole universe varying with cosmological time.

4. The cosmological constant versus the pressure of creation

The cosmological constant Λ has been related to the vacuum energy, and therefore to a negative pressure, to explain the accelerated expansion of the universe. Recently we have an interesting suggestion [1]: it implies that there is no cosmological constant. Its theoretical need can also be fulfilled by a creation pressure pc. At any rate, either Λ or a creation pressure implies (with c = 1), from Einstein cosmological equations:

Λ  1/t2E15

And from (Eq. 1) and (Eq. 11) we get

 t2   i.e.       Λ 1E16

The creation pressure pc [1] has been presented as equivalent to the effect of a cosmological constant Λ. A creation pressure expressed as Ωcp, a dimensionless parameter i.e.

Ωcp= (8π/3) Gpc/(c2H2)E17

as usually done in cosmology, is equivalent to the effect of a cosmological constant Λ, with omega parameter ΩΛ, if and only if the following relation holds:

 Ωcpº3ΩΛE18

This follows from the first of the cosmological equations of Einstein, i.e.

 2q + Ωp+ Ωk= 3 ΩΛE19

Here q is the deceleration parameter and Ωk the curvature. If we consider a creation pressure instead of a cosmological constant, usually taken as the dark energy constituent of the universe, we get from (Eq. 18) and (Eq. 19)

 2q + Ωk=  ΩcpE20

And using the present observations that give Ωk<< 1 we finally get for the creation pressure, instead of a cosmological constant

Ωcp= 2q  1E21

The present estimates [15] of the numerical values of the deceleration parameter q are: for very high red shift, close to the initial stages of the universe, q ≈ 0.5 which implies Ωcp ≈ 0. The initial creation pressure is very small, corresponding to a small dark energy component, if any. At this stage we should expect a small acceleration of the initial expansion that balances the gravitational attraction (may be after inflation has finished in a very short time). At the present time [15] we have the approximate value q ≈ - 0.5, which implies Ω cp≈ - 2. The present creation pressure is then pretty high. From (Eq. 18) it would correspond to a value of Ω Λ ≈ 2/3, in complete agreement with the very well known value of this parameter for today. There is no known reason for this negative increase in the creation pressure (positive increase in Λ and therefore in accelerating the expansion of the universe) to stop in the near future. We can extrapolate and consider the rather strong possibility that the universe will spread to infinity, in a finite time, due to an ever increasing accelerated expansion [8].

The creation pressure is related to the creation rate Г of the mass M [1] by the following expression

Г = ρ/ ρ + 3/= d (ln ρ R3)/dt = d (ln M)/dt =/ME22

The creation pressure pcp is defined in terms of the creation rate Г and other physical quantities [1] and is

Pcp=  ρ c2(Г/3H)E23

If we consider the universe as a black hole [6] then we have

2 GM/c2= R     i.e.  /=/= H = ГE24

where H is the Hubble parameter. The creation pressure in (Eq. 23) becomes

pcp =  (1/3) ρ c2E25

5. The cosmological constant versus the energy of the information

We can think of our universe as a kind of “quantum” black hole [6] and apply the Hawking-Bekenstein [10] and [11] formulation for its entropy S. Using the black hole relation (Eq. 2) between its mass M and its size a(t)

2GM/c2=a(t)E26

and combining (Eq. 11) and (Eq. 26) we get (with the linear relation a(t) ≈ ct)

= 4π k/ђcG(c3t/2G)2= π k/ђ (c5/G) t2E27

And in natural units G = c = ђ = k = 1 we finally get

S  t2E28

Going on using natural units, in Planck´s units of time we have then from (Eq. 28)

S  10122E29

The entropy of the universe increases with time and will arrive at a maximum at x = 2, its lifetime, and has a value of the order of 10122.

The quantum of gravity with mass mg has been presented [7] as

mg= ђ/(c2t)   1065gramsE30

Since the mass of the universe M is about 1056 grams, one has the number of gravity quanta Ng in the universe as

Ng M/mg 10122E31

The two very large numbers in (Eq. 29) and (Eq. 30), being of the same order of magnitude, give us a very strong reason to believe that the entropy S of the universe is the number of gravity quanta, as proposed 10 years ago [7], and this is the number of bits I that it contains:

 S  Ng M/mg 10122E32

Then, the unit of information, the bit, can be interpreted as having a mass mg and an energy mgc2 ≈ ђ/t, i.e.the quantum of gravitational energy ђω ≈ 10-45 ergs.

Now we can check the holographic principle, [12] and [13], for the universe: the amount of information (Eq. 31) inside the whole universe is equal to the area of the event horizon in Planck´s units (Eq. 28) and (Eq. 29).

6. The accelerated expansion of the universe

The deceleration parameter q was defined in terms of the scale factor a(t) and its derivatives as follows:

= a´´a/(a´)2E33

We see that a̦being a deceleration one has a̦< 0 and then the parameter q should be q > 0 for deceleration and q<0 for acceleration. We can take into account the definition of the Hubble parameter H

H=ḁ/aE34

So that equation (Eq. 32) transforms to

+(1+q)H2=0E35

The importance of this equation cannot be overestimated. It means that given the measured values of q [15] one can approach its time variation by the linear relationship:

q(x) =  x + ½E36

where we have defined x = t/t0 the ratio of any age of the universe t to the present age of the universe t0 ≈ 1.37 1010years. Then close to the beginning of the universe we have q ≈ ½ (i.e. x = ε << 1) and today q ≈ - ½ (x 0 ≈ 1). Rearranging equation (Eq. 34) with the change dt = t0 dx we get

H/H2=  d (1/H)/ (t0 dx) =  [ 1 + q(x) ]E37

And integrating we have

1/ Ht0=ò[ 1 + q(x) ] dx  + constant  E38

Using (Eq. 35) we get

1H/ t0= 1.5 x  0.5 x2+ constantE39

Choosing the limits of integration from 0 to x and taking into account that the present value of H is H0 ≈ 1/t0, for x = 1, the constant in (Eq. 38) has the value zero. With (Eq. 33) equation (Eq. 38) is then equivalent to

t0 a= [ 1.5 x  0.5 x2]1 = d ln a / dxE40

Integrating once more we get

ln a =ò[ 1.5 x  0.5 x2]1 dx  + ln a0E41

where a0 is the present value of the cosmological scale parameter a(t0)

a/a0= exp {ò[ 1.5 x  0.5 x2]1 dx }E42

integrating (Eq. 41) we have

a/a0= exp{(2/3) ln [2x/(3x)]} = [2x/(3x)]2/3E43

The plot of this expression is shown below in Fig. 1.

Figure 1.

In this figure 1 we have the plot of the scale factor of the universe (vertical axis), relative to its present value a0. in terms of time t (horizontal axis), relative to the present age of the universe t0. An infinite expansion appears at t = 3t0.

7. The final inflation

Having used only the relations (Eq. 32), (Eq. 33), (Eq. 34) and (Eq. 35), without using the field equations of general relativity (only the observed values of the deceleration parameter q), the predicted final “inflation” at tf = 3t0 is a result of an extrapolation towards the future. The present day observations of q cover 1/3 of this time interval and strongly support the final expansion, the finite lifetime of the universe in a surprisingly rather short time from now (only 2 aeons).

We speculate that the initial inflation may have started from the Planck´s quantum black hole, bringing the universe close to its present size. After that, an almost linear expansion goes on due to the creation pressure, thus bringing the universe to its present size. The final inflation follows at about 4x1010 years of age, giving a finite lifetime for our universe. This is clearly an unexpected result that comes from the present observations of the values of the deceleration parameter q.

8. Conclusions

The generalization of the concept of a quantum black hole (giving the sub-Planckian scale, the Planckian scale and the scale of our universe) shows that there is a numerical factor, 1061, that is equivalent to the total age of the universe in Planck´s units. It looks like this is the characteristic lifetime of a universe, in terms of the successive factors for the different scales, 10-61, 1, 1061, (or in terms of the generalized Planck´s constant, 10-122, 1, 10122. The age of a universe is intimately related to the choice of the unit of time interval. For the sub-Planckian scale we have 10-104 seconds, for the Planck scale 5 10 -44 seconds and for our universe about 5 1017 seconds.

The picture that arises for the evolution of the universe is: no big-bang, an initial inflation (an exponential expansion) of a quantum black hole, Planck´s type, a slow deceleration followed by a slow acceleration. Then we have an almost linear expansion at the present time. And a final disaggregation to infinity at about 4 1010 years of age, the lifetime of our universe.

The cosmological constant Λ can be substituted by a creation pressure. This is in line with the idea of gravitation being an emerging entropic force. For the existence of this force an increase in mass with time (a Mass-Boom, 14) is necessary, giving a positive gradient of entropy for the universe and therefore the emergent gravitation.

9. Appendix

We are going to calculate now the following important cosmological parameters, in terms of the dimensionless age, x = t/t0,and relative to the present size of the universe a0 = 1:

The speed of expansion of the universe a´(t)

The Hubble parameter a´(t)/a(t)

The acceleration of the expansion a´´(t)

The deceleration parameter q= - a´´(t) a(t)/ a´(t)2

The speed of expansion of the universe a´(t). We find the derivative of the scale factor a(t) in (Eq. 42) as

a`(t)/a(1) = 4 (2x)1/3(3x)5/3E44

Figure 2.

The speed of expansion of the universe as in (Eq. 43). There are two vertical asymptotes at x = 0 and at x = 3. They imply the initial inflation (x = 0) and the final disaggregation to infinity (x = 3) at about 4 1010 years.

The Hubble parameter H = a´(t)/a(t). If we divide the expression (Eq. 43) by the expression (Eq. 42) we get for H

= 2/x(3x)E45

The following figure 3. gives the graph of this expression:

Figure 3.

The Hubble parameter H in terms of age x. We see again the initial inflation (x=0) and the final (x=3) disaggregation given by the two vertical asymptotes.

The acceleration of the expansion a´´(t). Differentiating once more the expression (Eq. 43) we get for the acceleration of the expansion of the universe

a´´ =  8/(1/2x)4/3(1/(3x))5/3+ 20/(1/2x)1/3(1/(3x))8/3E46

Figure 4.

The acceleration of the expansion of the universe is seen here again with two vertical asymptotes. Close to the origin the negative acceleration suggests the action of gravitation balancing the inflation phase. After half of the present age of the universe we see a positive acceleration, growing, and due to the pushing force that grows with the increasing size of the universe.

The deceleration parameter

q=  a´´(t) a(t)/ a´(t)2= 0. x E47

Figure 5.

The deceleration parameter. Using the expressions (Eq. 42), (Eq. 43) and (Eq. 45) that define q gives back the original function assumed for q in (Eq. 35).

q = 0.5  x E48

Acknowledgments

I am thanking the owners of the Wolfram Mathematica Online Integrator that I have used to obtain the Fig. 1, Fig. 2, Fig. 3, Fig. 4 and Fig. 5 of this work.

© 2011 The Author(s). Licensee IntechOpen. This chapter is distributed under the terms of the Creative Commons Attribution-NonCommercial-ShareAlike-3.0 License, which permits use, distribution and reproduction for non-commercial purposes, provided the original is properly cited and derivative works building on this content are distributed under the same license.

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Antonio Alfonso-Faus (September 9th 2011). Small-Bang versus Big-Bang Cosmology, Aspects of Today's Cosmology, Antonio Alfonso-Faus, IntechOpen, DOI: 10.5772/25138. Available from:

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