Preprint
(22.09.2002)
аDate: Sun, 22 Sep 2002 23:08:18 GMT
From: redshift0@narod.ru (Alex Chepick)
Organization:а
Newsgroups: sci.physics, sci.astro,
alt.sci.physics.new-theories
Subject: Explanation of width-and stretch-factors
Key
words:
width-factor - stretch-factor
Explanation
of width- and stretch-factors
for Type Ia Supernovae
Chepick A.M., Nizhni Novgorod
22.09.2002
ааааааа Explanations of dependence on distance
are given both for the w-factor of a light curve of an absolute magnitude Type
Ia Supernovae and for s-factor not explained till now.
а 1.
Introduction
Recently found out an expansion phenomenon
(w-factor) of a light curve for absolute magnitude of Type Ia Supernovae would
be considered as the brightest proof of the universe expansion if it was not
accompanied by the not explained stretch-factor (s-factor) [Peter Nugent, Alex Kim and Saul Perlmutter, arXiv: astro-ph/0205351 v1 21 May 2002 K-corrections and Extinction Corrections for Type Ia
Supernovae; further NKP2002]
аа 2.
Light in the intergalactic environment
Speed of light practically always is less than
constant in Lorentz's transformations because of the speed depends on
environment in which light is traveling, and the "pure" vacuum is not
exist in the nature. Certainly, change of speed of light cannot be large
because of extreme low optical density of the intergalactic environment. We
shall designate cU as average speed of a photon from the
distant source. An influence of the rarefied intergalactic environment on each
photon during their movement was various, as environment is very dynamical,
first of all, because of a fast varied electromagnetic field of other photons,
including background one. We shall count therefore that distribution of photons
on speed have been defined by some average function F(v, cU),
for example, Gauss law:
dn=(2πσ2)-1/2
аN exp[-(v- cU)2/(2σ2)]
dv
where
dn is number of the photons accepted in unit of time, which speed is in limits from
v up to v+dv, N - the general number of photons radiated in unit of time and
that then will get in the receiver; σ2 - a dispersion. N
depends on time of radiation t (t=0 corresponds to the peakа radiation moment). We shall notice, that for
a source there is no distribution in the speeds - all photons have speed
"c". We shall assume, that values cU and σ2
do not depend on time and from length of a wave; and distanceа R from a source up to the receiver during
supervision is changing insignificantly (much less of R).
Let n - the general number of the photons
accepted in unit of time (depends on time of reception tТ). Let time t and t'
are defined in a system of reference of the receiver, and t' =t + R/cU
Then
n(tТ)=а ∫ N(t+ R/v - R/cU) F(v, cU) dv
The value of shift R/v - R/cU = (R/cU)(cU/v
-1) is measured in days and means an epoch concerning time t from which photons
come to the receiver at the moment of time tТ. And, the further Supernovae is
situated, the more an epoch exist photons will come from.
On the contrary, for very close Supernova the
value of shift will be practically equal 0 for any speed v, that is, simple
conformity between epoch of radiation and reception is established.
Accordingly, the further Supernovae is situated, the more an epoch exist
photons will come to from one epoch of radiation.
ааа 4.
Conclusions
All this results to that:
1.аа The
width of a light curve increases proportionally to distance both for all
spectrum, and for a separate range (w-factor);
2.ааа
The peak of accepted radiation (absolute luminosity) decreases
proportionally to distance both for all spectrum, and for a separate range
(s-factor), and the factor of proportionality depends on absolute luminosity in
this range (the formula (2) in NKP2002);
3.ааа
Color B-V at peak B-band is proportional to distance and it is a
consequence of the formula (2) as a subtractа
of luminosities (the formula (3) in NKP2002).
4.аа As
result of these reasons it is possible to estimate value cU,
assuming, that
the maximal speed v is equal "c" and that the width of a light curve
makes up 60 day for a Supernovae, that situated on distance R=3*109 l.y.:
2(R /cU)
(1ЦcU/ё) = 60 days
Whenceа
cU = ё(1-3*10-11).
5. Accordingly, the optical density of the
intergalactic environment should be equal 1+3*10-11.
6.аа We
shall take into account, that the measurement accuracy of the speed of light (in experiments with long-basic
interferometers and Cherenkov radiation) makes up some decimeters per second,
that is 10-9c. Hence, it is not possible to confirm this hypothesis
in direct laboratory experiment yet.
7.аа If
it is possible to receive reliable estimations of optical density of the
intergalactic environment, and these estimations is not coincide with that
submitted calculations there will be one more opportunity of an explanation w-
and s-factors, that is a hypothesis
about not coincidence of the light speed in vacuum and the maximal speed of a
matter interaction.
аEmail: redshift0@narod.ru
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