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 * r
4, 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 * r
4 should correspond a seriesof 60 theoretical brightnesses given by the relation
Btheor = K / r
4, as well as a series of 60 expected magnitudesgiven 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 SNeto 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) andm = 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
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:
it is assumed that the dark energy is vacuum energy (cosmological
constant).
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."