SNe Ia DATA ARE COMPATIBLE WITH A STABLE UNIVERSE

Marcel J. Luttgens

_________________________________________________________

 

ABSTRACT

________

 

Assuming a stable universe, one gets equations linking the

SNe Ia distances to their magnitudes or their brightnesses,

that fit the observational data better than general relativity

formulae based on an expanding universe.

The main reason is that the relativistic formulae don't take

specifically into account the decrease of the apparent diameter

of the supernovae in proportion to their distance.

It is imprudent to conclude –disregarding the possibility

of a mathematical artefact- that "the derived constraints for

the redshift and distance of SN 1997ff are consistent with

the early decelerating phase of a currently accelerating

Universe and thus are a valuable test of a Universe with

dark energy." (III)

 

INTRODUCTION

____________

 

According to John L. Tonry et al. (V), "supernovae provide

the only qualitative signature of the acceleration itself,

hence more supernova data, better supernova data, and supernova

data over a wider redshift range are needed to confirm cosmic

acceleration."

Certainly, more SN data are needed, especially over the

redshift range > 1, because of the great variability of the

redshift and magnitude observations.

But one should not forget that the hypothesis of a currently

accelerating Universe following a decelerating phase (see

"Excerpts from SNe Ia literature" below) rests on general

relativity formulae applying to an expanding universe.

In fact, the hypothesis of a stable universe, where the redshift

of remote objects is not due to expansion, leads to formulae

giving results that fit the observed SNe Ia data better than

the relativistic formulae at values of z greater than 1.

 

STABLE UNIVERSE

_______________

 

The used basic data are the SNe Ia redshift z and magnitudes

mBeff featured in the paper "MEASUREMENTS OF OMEGA AND LAMBDA

FROM 42 HIGH-REDSHIFT SUPERNOVAE", published by S. Perlmutter

et al. in THE ASTROPHYSICAL JOURNAL, 517: 565-586, 1999 June 1.

They relate to 42 high-redshift type Ia supernovae from the

Supernova Cosmology Project (Table 1) and 18 low-redshift

type Ia supernovae from the Calàn/Tololo Supernova Survey

(Table 2). However, 1992br (z = 0.088, Beff = 19.28) has

been discarded because of its anomalously big magnitude.

So, we are left with 59 SNe, to which we have added SN 1997ff,

with z = 1.700 , and an estimated magnitude of 25.99.

 

SN

z

mBeff

     

TABLE II

   

(1)

   

1992a1

0.014

14.47

1992bo

0.018

15.61

1992bc

0.020

15.18

1992P

0.026

16.08

1992ag

0.026

16.28

     

19900

0.030

16.26

1992bg

0.036

16.66

1992b1

0.043

17.19

1992bh

0.045

17.61

1990af

0.050

17.63

     

1993ag

0.050

17.69

19930

0.052

17.54

1992bs

0.063

18.24

1993B

0.071

18.33

1992ae

0.075

18.43

     

1992bp

0.079

18.27

1992aq

0.101

19.16

     

TABLE I

   

(1)

   

1997I

0.172

20.17

1997N

0.180

20.43

1997ac

0.320

21.86

1994F

0.354

22.38

1994am

0.372

22.26

     

1994H

0.374

21.72

1997O

0.374

23.52

1994an

0.378

22.58

1995ba

0.388

22.65

1995aw

0.400

22.36

     

1997am

0.416

22.57

1994a1

0.420

22.55

1994G

0.425

22.13

1997Q

0.430

22.57

1996cn

0.430

23.13

     

1995az

0.450

22.51

1997ai

0.450

22.83

1996cm

0.450

23.17

1995aq

0.453

23.17

1992bi

0.458

23.11

     

1995ar

0.465

23.33

1997p

0.472

23.11

1995ay

0.480

22.96

1996cg

0.490

23.10

1996ci

0.495

22.83

     

1995as

0.498

23.71

1997H

0.526

23.15

1997L

0.550

23.51

1996cf

0.570

23.27

1997af

0.579

23.48

     

1997F

0.580

23.46

1997aj

0.581

23.09

1997K

0.592

24.42

1997S

0.612

23.69

1995ax

0.615

23.19

     

1997J

0.619

23.80

1995at

0.655

23.27

1996ck

0.656

23.57

1997R

0.657

23.83

1997G

0.763

24.47

     

1996c1

0.828

24.65

1997ap

0.830

24.32

     

SN1977ff

   

(2)

   
     

1997ff

1.700

25.99

 

(1) Table 2: CALAN /TOLOLO SNE IA DATA (less SN1992br)

Table 1: SCP SNE IA DATA

(2) SN 1997ff

 

We began by calculating the brightnesses Beff of the 60 SNe Ia

with the relation Beff = 10(25.03 - mBeff)/2.5. In this relation,

25.03 corresponds to the magnitude of Vega + 25, thus Beff is

10 billion times bigger than the "true" brightness.

 

Assuming that all SNe have the same intrinsic brightness,

the product Beff * r4, where r represents the SNe distances,

should be constant.

Indeed, the brightnesses are a function, not only of the

squared distances, but also of the squared diameters of the

supernovae, because the apparent diameter of the supernovae

decreases in proportion to the square of their distance,

according to a specific law. Specific, because supernovae

don't have an intrinsic constant diameter, but nevertheless,

they cannot be treated as mere points. Around their peak

luminosity, they certainly have the form of a physical sphere,

that has of course some diameter.

 

Let's note that in a stable, i.e. non-expanding universe,

r = z / (1 + z).

 

To that constant K = Beff * r4 should correspond a series

of 60 theoretical brightnesses given by the relation

Btheor = K / r4, as well as a series of 60 expected magnitudes

given by the relation

mBexpected = 25.03 - 2.5 log(Btheor).

 

From a statistical analysis of the 60 supernovae data,

we obtained the relation

Btheor = K / (r + 0.05)4.4 , where K = 0.11.

The corresponding expected magnitudes are given by

mBexp = 25.03 – 2.5 log(K / (r + 0.05)4.4)

The high correlation coefficient between mBexp and mBeff

(0.992) is thus compatible with the hypothesis of a stable

universe.

 

EXPANDING UNIVERSE

__________________

 

Assuming a cosmic expansion, Richard Ellis and Mark Sullivan

wrote in the introduction to their paper "Verifying the use

of supernovae as probes of the cosmic expansion"

(astro- ph/ 0011369 v1 20 Nov 2000):

 

"In combination with the results of recent microwave background

measurements (de Bernardis et al. 2000; Jaffe et al. 2000)

which indicate a spatially flat infationary universe, the SNe Ia

results suggest a significant non-zero cosmological constant

(Omega = 0.28, Lambda = 0.72).

Conclusions of this importance require excellent supporting

evidence."

 

If it can be shown that a relativistic distance formula like

dL = 10 * 10(m - M)/5 pc, linking the magnitude m of the SNe

to their luminosity distance dL (for an empty universe) gives

results that are not better than those obtained with the

formula r = z / (1 + z), one could not speak of an excellent

supporting evidence.

 

Such relativistic formula can be written

dL = 10-5 * 10(m - M)/5 Mpc, where 1 Mpc = 3.2615 * 106 light-years,

and M is an absolute magnitude. For SNe Ia, M = -19.5, hence

m = 5 log(dL) + 5.5.

 

On the other hand, dL * H0 = cz(1 + z/2) Mpc,

with c = 300000 km/s and H0 = 65 km s-1 Mpc-1.

(cf. "Cosmological Results from High-z Supernovae by

John L. Tonry et al.", astro- ph/ 0305008 v1 1 May 2003).

 

From dL * H0 = cz(1 + z/2) Mpc, one gets

 

dL = (c/H0) * z(1 + z/2) Mpc = 15.05 * z(1 + z/2) Gly, thus

5 * log(dL) = 18.32 + 5 * log((z(1 + z/2)).

 

The relation m = 5 log(dL) + 5.5 becomes

 

m = 23.82 + 5 log((z * (1 + z/2))), or

(1) m = 5 log(cz) - 3.57 + 5 log(1 + z/2)

 

Till z ~ 1, the relations

mBexp = 25.03 – 2.5 log(K / (r + 0.05)4.4) and

m = 5 log(cz) - 3.57 + 5 log(1 + z/2) give more or less

similar results.

 

At z = 1.7, the obtained result is different, which is not

surprising, as the formula based on general relativity doesn't

take into account the decrease with distance of the apparent

supernovae diameter.

 

The 60 magnitudes m calculated from relation (1) are

statistically related to the 60 magnitudes mBeff by the relation

m = 0.9699 mBeff + 0.3756, with a correlation coefficient

of 0.994, which is as good as the one obtained above with

r = z / (1 + z). However, as the mean difference

(mBeff - m) = 0.2886, relation (1) becomes

 

m = 24.09 + 5 log((z * (1 + z/2)))

 

Till about z = 1, this relation gives results which are

comparable to those obtained with the non-relativistic formula

mBexp = 25.03 – 2.5 log(K / (r + 0.05)4.4)

 

At z = 1.7, which is the case of SN1977ff, the calculated

magnitude m is distinctly greater than the observed magnitude.

 

According to John L. Tonry et al. (V), "there is a tendency for

the SN Ia to be brighter at z ~ 0.9, suggesting that we are

truly seeing a change in the deceleration of the universe and

the effects of dark energy.

But such tendency is likely due to the assumed acceleration

of the universe expansion.

 

GRAPHIC COMPARISON BETWEEN m AND mBexpected

 

Let's remember that mBexpected =25.03 – 2.5 log(K / (r + 0.05)4.4),

and that m = 24.09 + 5 log(z * (1 + z/2))

 

At z = 1.7, m = 26.58, thus SN1997ff is 10(26.58 - 25.85)/2.5 = 1.96,

i.e. about twice as bright, as expected.

 

Riess and Nugent claimed not so long ago: "SN1997ff is more

than twice as bright as predicted by theories that the universe

is not accelerating, because it's closer than it would be if

it were moving away at the rate the universe is expanding now.

This means that the universe was expanding less quickly

10 billion years ago and has since accelerated."

 

In fact, such excess brightness is an artefact due to the

hypothesis of an expanding universe.

At a theoretical redshift of 5, a SN would be considered as

20.5 times too bright!

But with the non-relativistic relation, no such excess brightness

is found.

 

Marcel Luttgens, November 28, 2003

 

mluttgens@spamorange.fr

 

APPENDIX : EXCERPTS FROM SNe Ia LITERATURE

__________________________________________

 

(I) Supernovae and Cosmology (astro- ph/ 0010634 v1 31 Oct 2000)

Monique Signore, Denis Puy

From 5 Conclusions:

"After a brief review of type Ia supernovae properties (Section 2)

and of cosmological background (section 3), we presented the work

done by two separate research teams on observations of high-z SNIa

(Section 4) and their interpretation (Section 5) that the expansion

of the Universe is accelerating. If verified, this will proved

to be a remarkable discovery.

However, many questions without definitive answers remain.

What are SNIa and SNIa progenitors ?

Are they single or double degenerate stars ?

Do they fit Chandrasekhar or sub-Chandrasekhar mass models at

explosion ?

Is the mass of radioactive 56 Ni produced in the explosion really

the main parameter underlying the Phillips relation ?

If so, how important are SNIa evolutionary corrections ?

Can systematic errors be negligible and can they be converted

into statistical errors ?

Can a satellite, like SNAP, provide large homogeneous samples

of very distant SNIa and help determine several key cosmological

parameters with an accuracy exceeding that of planned CMB

observations ?

Meanwhile, cosmologists are inclined to believe the SNIa results,

because of the preexisting evidence for dark energy that led to

the prediction of accelerated expansion."

 

II. Verifying the use of supernovae as probes of the cosmic

expansion (astro- ph/ 0011369 v1 20 Nov 2000)

Richard Ellis and Mark Sullivan

From Introduction:

<..>

"In combination with the results of recent microwave background

measurements (de Bernardis et al. 2000; Jaffe et al. 2000)

which indicate a spatially flat infationary universe, the SNe Ia

results suggest a significant non-zero cosmological constant

(Omega = 0.28, Lambda = 0.72).

Conclusions of this importance require excellent supporting

evidence. In particular, it is appropriate to question the

homogeneity, environmental trends and evolutionary behaviour

of the SNe found at all redshifts.

Systematic differences between high and low redshift samples

might change the derived cosmological parameters without

destroying the small dispersion seen in the SNe Ia Hubble diagrams.

Evolutionary differences between low and high-redshift SNe Ia

might arise via the progenitor composition (Höflich 1999),

a differential dust extinction with greater amounts of dust

in high-redshift environments, either in the host galaxy

(Totani & Kobayashi 1999) or `grey' dust in the IGM (Aguirre 1999),

or a dependence of the SNe properties on host galaxy environments.

Addressing this last possibility forms the basis of this

present study."

 

III. The Farthest Known Supernova: Support for an Accelerating

Universe and a Glimpse of the Epoch of Deceleration

(astro- ph/ 0104455 v1 27 Apr 2001)

Adam G. Riess et al.

From 1. Introduction:

The unexpected faintness of Type Ia supernovae (SNe Ia) at

z ~ 0.5 provides the most direct evidence that the expansion

of the Universe is accelerating, propelled by "dark energy"

(Riess et al. 1998; Perlmutter et al. 1999).

From Abstract, p.2

"The apparent SN brightness is consistent with that expected

in the decelerating phase of the preferred cosmological model,

Omega M ~ 1/3; Omega lambda ~ 2/3.

It is inconsistent with grey dust or simple luminosity evolution,

candidate astrophysical effects which could mimic previous

evidence for an accelerating Universe from SNe Ia at z ~ 0.5.

We consider several sources of potential systematic error

including gravitational lensing, supernova misclassification,

sample selection bias, and luminosity calibration errors."

From 5. Conclusions:

"1. SN 1997ff is the highest-redshift SN Ia observed to date,

and we estimate its redshift to be ~ 1.7. <...>

2. The derived constraints for the redshift and distance of

SN 1997ff are consistent with the early decelerating phase

of a currently accelerating Universe and thus are a valuable

test of a Universe with dark energy. The results are inconsistent

with simple evolution or grey dust, the two most favored

astrophysical effects which could mimic previous evidence for

an accelerating Universe from SNe Ia at z ~ 0.5.

3. We consider several sources of potential systematic error

including gravitational lensing, supernova misclassification,

sample selection bias, and luminosity calibration errors.

Currently, none of these effects alone appears likely

to challenge our conclusions. However, observations of more

SNe Ia at z > 1 are needed to test more complex challenges

to the accelerating Universe hypothesis and to probe the

nature of dark energy."

 

IV. Do SNe Ia Provide Direct Evidence for Past Deceleration

of the Universe? (astro- ph/ 0106051 v1 4 Jun 2001)

Michael S. Turner and Adam G. Riess

From ABSTRACT:

"Observations of SN 1997ff at z ~ 1.7 favor the accelerating

Universe interpretation of the high-redshift type Ia supernova

data over simple models of intergalactic dust or SN luminosity

evolution. Taken at face-value, they provide direct lines of

evidence that the Universe was decelerating in the past,

an expected but untested feature of the current cosmological model.

We show that the strength of this conclusion depends upon

the nature of the dark energy causing the present acceleration.

Only for a cosmological constant is the SNe evidence definitive.

Using a new test which is independent of the contents of the

Universe, we show that the SN data favor recent acceleration

(z < 0.5) and past deceleration (z > 0.5)."

From Concluding remarks:

"The absence of an early, decelerating phase would be a much

bigger surprise than the discovery that the Universe is

accelerating today. It would be essentially impossible to

reconcile with the standard hot big-bang cosmology.

In addition to providing strong support for the accelerating

Universe interpretation of high-redshift SNe Ia, SN 1997ff

at z ~ 1.7 provides direct evidence for an early phase of

slowing expansion if the dark energy is a cosmological constant

(Riess et al. 2001).

However, because supernova observations do not directly measure

changes in the expansion rate, a model for H(z) or q(z)

is needed to perform a more robust test for past deceleration.

The former requires assumptions (or a deeper understanding)

about the nature of dark energy responsible for the recent

speed up while the latter requires more SNe Ia at z > 1.

<...>

In summary, we have shown that for a flat Universe the current

supernova data:

  1. provide strong, direct evidence of past deceleration if
  2. it is assumed that the dark energy is vacuum energy (cosmological

    constant).

  3. alone do not provide direct evidence of past deceleration

unless the dark-energy equation-of-state wX is close to -1.

However, using dynamical measurements of the amount of matter,

deceleration can be indirectly inferred for the redshift range

of the SN sample (if omegaM > 0.12).

3. without recourse to a specific model of the contents of

the Universe, favor deceleration at z > 0.5 with ~ 90% confidence.

An even stronger statement is that the SN data favor increasing

q(z) with increasing redshift, a sign of the assertion of

attractive gravity in the past."

 

V. Cosmological Results from High-z Supernovae

(astro- ph/ 0305008 v1 1 May 2003)

by John L. Tonry et al.

"Supernovae provide the only qualitative signature of the

acceleration itself, through the relation of luminosity distance

with redshift, and most of that effect is produced in the recent

past, from z = 1 to the present, and not at redshift 1100 where

the imprint on the CMB is formed.

This is why more supernova data, better supernova data, and

supernova data over a wider redshift range are needed to confirm

cosmic acceleration."

From p. 39:

"Evidently there is a tendency for the SN Ia to be brighter

at z > 0.9 (although the uncertainties are still large), suggesting

that we are truly seeing a change in the deceleration of the universe

and the effects of dark energy."

"Nevertheless, we are apparently starting to see SN Ia become

brighter at z ~ 0.9, rather than becoming ever dimmer because

of a systematic effect."