THE CASE AGAINST THE BIG BANG

(A critique of "The case for the relativistic hot Big Bang cosmology")

                      by  Tom Van Flandern
                          Meta Research

     [The contents  of this note are Copyright 1991 by the author
because an article based on them is in preparation for a journal.
Permission is granted to  quote freely for purposes of discussion
on this network, and to  repost  (including this notice) to other
networks.  Permission to print extensive  excrpts  in media which
are  not  in  competition with astronomy research  journals  will
probably be granted upon request.]

     The  invited  review  article  by  P.J.E.    Peebles,   D.N.
Schramm,  E.L.   Turner & R.G.  Kron with  the  cited  title  was
published in the 29 August issue of NATURE, v.  352, pp.  769-776
(1991).   Although the following rebuttal criticizes many  points
about  the Big Bang model, it should in no  way  be  taken  as  a
criticism  of  the  authors  themselves,  who  are  clearly know-
ledgeable and  sincere  authorities  writing  in  their fields of
expertise.

     In their introduction,  the  authors (henceforth abbreviated
"PSTK") cite three criteria  of  the  Big Bang which they suggest
are essential to a good  world  model:

(1) It fits and even predicts the observations well.
(2) There is no known feasible alternative model.
(3) Although there  are unsolved puzzles, nothing contradicts the
    model.

We will argue here that:

(1)  The  Big  Bang's  predictions  are  of  a  narrow,  ad  hoc,
     unconvincing variety.
(2)  Some alternative models are feasible.
(3)  There  would  be  contradictions  but  for  narrowing of the
     definition  of  the  standard  model  so as to exclude known
     contradictions.   We  also  contend  that the Big Bang model
     merely attempts to  explain  what we observe today, but does
     not  truly  explain  very  much  about  the  origin  of  the
     universe.

Section I: The standard model

     PSTK begin by defining the standard  Big  Bang  cosmology as
one  which expands according to Hubble's law.    This  is  overly
broad,  since  some  alternative  cosmologies also have expanding
universes.  By defining the Big Bang in this  way,  existing  and
potential  future contradictions to it are avoided.  For example,
if the cosmic background radiation (CBR) were found to be a local
phenomenon, PSTK would  apparently  not  count  that  as a strike
against the Big Bang  model  itself,  but  only  against  certain
variations of the basic model.

     The  PSTK  exposition  of the  standard  model  has  several
problematical  concepts.   Their primordial fireball  provides  a
reference  frame for the measurement of absolute  velocities,  in
contradiction to a premise of the theory of  relativity.    Their
expanding  universe  has  a  mass  density such that it  met  the
criteria for being a "black hole" until it had expanded  to about
1000  Mpc  in  size.    Now,  depending on the values of  certain
parameters, much  of  the  universe's matter may have escaped its
event horizon, or  will  in  the  future.    And the extrapolated
starting  conditions  imply increasing  temperatures  approaching
infinity at the origin.   This  seems  opposed  to  the  Big Bang
concept  of  a  beginning  to  time   itself,  which  implies  an
unchanging  (zero  temperature)  condition at the moment  of  the
origin of time.

     But  PSTK  avoid the most important question of  all  for  a
cosmological  model, stating that "whatever started the expansion
...   is  not  intrinsic to the standard model".  There is an old
math concept that  one  and  a  google  (a  huge number) are both
infinitely far away from  infinity.    By  taking reciprocals, it
follows that 10^17 seconds and 10^-40 seconds are both infinitely
far  away  from  being infinitesimal.   So  in  that  sense,  the
standard model still leaves us infinitely far  from understanding
the origins of the universe.  The problem is not so much that the
model doesn't deal with the question of the origin  moment, as it
is that a miracle still seems required to start such  a universe.
It  is  no coincidence that the Big Bang model has been  declared
theologically acceptable in certain  religions,  as  Hawking  has
noted.

     Another  fundamental  problem  here  is  that  the  observed
cosmological redshift is not known to  be  due to velocity.  That
interpretation  is an ad hoc assumption of  the  standard  model.
But in the standard model this assumption implies  that,  for the
universe  to have expanded from a singularity, it would  have  to
overcome gravitational  forces near the origin which indefinitely
exceed  in strength  any  known  forces  in  physics.    If  such
mega-forces were to exist,  then  how could we have confidence in
the rest of physics (e.g.  the theory of black holes)?

Section II. Cosmic background radiation

     PSTK cite the Big Bang's interpretation of this radiation as
a primordial fireball.  This interpretation is neither unique nor
compelling.  Specific problems with it are:

(1)  the smoothness of the radiation  is  in  unexpectedly  sharp
     contrast with the lumpiness in the distribution of galaxies.
(2)  The  2.8  degree  temperature of the radiation is well below
     theoretical  predictions  of  what    that  temperature  was
     expected to be in the Big Bang model (10-30 degrees).
(3)  The radiation provides a frame  of  reference  against which
     absolute velocities can be measured.
(4)  Lerner has shown that the brightness  of  radio  galaxies is
     sufficiently  attenuated  at  radio  wavelengths as compared
     with infrared wavelengths, that no microwave radiation could
     possibly  get   through  the  intergalactic  medium  without
     absorption and re-emission  many times.  So the radiation we
     observe  cannot  be  coming    to    us  directly  from  the
     "background".

Section III. Light element abundances and neutrino counting

     The abundances of heavy elements  used  to  be  an  argument
against the Big Bang.  Now  that  the standard model has accepted
that  heavy  elements  must  come  from multiple  generations  of
stellar  nucleosynthesis,  it  concentrates  only  on  the  light
elements.    Rejecting cosmic ray spallation (the explanation for
light elements  in  other  cosmologies),  the  Big  Bang  uses an
adjustable parameter (photon  to  baryon  ratio)  to  secure good
agreement among four light  elements.  But the predicted helium 4
abundance is close to the value expected from multiple generation
stellar nucleosynthesis, and is therefore not  significant.   The
deuterium  abundance  is difficult to estimate, with  the  latest
Hubble  Space Telescope values coming out smaller than  Big  Bang
predictions.

     The  implied  photon  to  baryon  ratio  requires  that  the
curvature parameter, omega, be less than 0.1 (i.e.  the  universe
is  open,  in  contradiction with certain popular versions of the
Big Bang).  And a recent determination of the Beryllium abundance
indicates that element  may  be 1000 times more abundant than the
Big Bang predicts.

     A representation that the  Big  Bang predicts the abundances
of the elements significantly better  than  any  other  model  is
presently unjustified.

Section IV. The evolution of quasars and galaxies

     PSTK  suggest  that  distant  blue  galaxies  represent  the
predicted proto- galaxies expected by the Big  Bang  model.   The
problem  is  that  the  Big  Bang  did  not    predict  that  its
proto-galaxies  would look anything like the blue galaxies, whose
true nature is still quite unknown.

     PSTK likewise assume that radio galaxies are an evolutionary
stage in  the  development  of  mature galaxies.  But this is not
consistent with the  morphologically distinct differences between
high-redshift and low-redshift radio  galaxies,  suggesting  that
they are two different classes  of object.  Similarly, if quasars
and AGN's are also evolutionary stages,  it  would  not have been
expected  that  their principal radiations would be  non-thermal.
Incorporating  all  of  these  objects  into  the standard  model
requires  ad  hoc  hypotheses,  and therefore cannot be taken  as
"evidence" for the Big Bang.

     A more serious difficulty is the time required for formation
of  superclusters  of  galaxies  --  structures so large that, at
typical galaxy relative velocities, perhaps an order of magnitude
more time than the Hubble age of the universe is required.

Section V. Quasar distances and lensing

     PSTK cite Arp's  argument that 20 quasars out of 4500 have a
magnitude 15 or brighter  galaxy  within  2  arc minutes, whereas
only  2  would be expected  by  chance.    They  then  argue  for
discovery  bias, since quasars are looked  for  more  often  near
bright galaxies.  But this argument, if  true,  implies  that the
true quasar population to be discovered away from bright galaxies
is actually at least ten times greater, even if all known quasars
were found by only while looking near bright galaxies.   I  think
the observers will be surprised to hear this.

     PSTK  argue  that high-redshift  quasars  near  low-redshift
galaxies have absorption lines, thereby implying that the quasars
are more distant than the galaxies.    But  the  absorption lines
show no metalicity, and therefore cannot be  caused  by  a galaxy
halo.  And the excessive number of absorption line systems in the
nearby,   bright  quasar  3C273  argues  against  the  idea  that
intergalactic clouds  cause  these absorption lines.  The meaning
of the absorption  lines  is  different  in different alternative
models;  but is unlikely to be as simple as the standard Big Bang
model suggests.

     PSTK  argue  that  multiple images  of  some  quasars  imply
gravitational  lensing  by  foreground  galaxies,  proving   that
quasars are much farther away than the  galaxies, as the standard
model indicates.  The difficulty is that the images are not quite
what the lensing model suggests.  The optical quasar  images fail
to  form  into  Einstein  rings  or  substantial ring arcs;   are
inconsistent in the numbers of images formed;  and generally fail
to be  distorted  or  align with the hypothetical lensing galaxy,
even when a  nearby  galaxy  can  be  seen  at all.  The observed
properties of the suggested  lensing systems are not inconsistent
with multiple images formed by  refraction as quasar light shines
through an intervening nebulosity.  It  might  even  be  fair  to
suggest that the later idea better represents  what  is  observed
than the gravitational lens hypothesis.

     PSTK state that "indications of associations between objects
with  very  different redshifts are well-worth following up", yet
they  omit  the  most  striking  of  all  such examples to  date,
Markarian 205, from  their  discussion.    The  unusual  luminous
bridge  connecting  this  quasar   to  a  galaxy  arm,  found  in
long-exposure  optical  images, has been  confirmed  in  striking
detail with computer processing of the latest CCD images.

     PSTK  agree  that,  if lensing of  quasar  images  were  not
observed, it would be a serious problem  for  the standard model.
But the cases they call "lensing" often require chance alignments
too  close  to  be  real.    For  example,  in   Q2237+0305,  the
hypothetical  lensing  galaxy  and  the background quasar must be
aligned to  within  about  0.1  arc seconds or so.  But the total
area of the  sky  is  5 x 10^11 arc seconds, which is about 10^13
times greater than the  area  containing the "lensing" galaxy and
"background" quasar.  And the  quasar  is  not even unusually far
away, at redshift 1.7.  With  fewer  than 10^4 quasars known, one
can  readily  see  the statistical problems of  an  alignment  to
within  a  part in 10^13 for this whole  interpretation  and  its
requirement of chance alignments of unassociated objects.

Section VI. The timescale problem

     PSTK  discuss  the mild inconsistency between the Hubble age
of the Big Bang universe, 10 +/- 1.3 billion years  (by),  versus
the radioactive decay age of the galaxy of 15 +/- 4  by,  and the
globular  cluster  ages  of  15  +/-  3  by.  They point out  the
unpleasant implications for simplicity  of  the standard model if
these ages stand up to further scrutiny.  They do not discuss the
minimum time required for the formation of galactic superclusters
and voids, which appears to be far larger yet.

Section VII.  Origin of galaxies

     PSTK  note  the  unexpected  smoothness  of  the  background
radiation  in  comparison with the highly structured distribution
of galaxies.  Here they cite limits on the  smoothness  which, if
violated  by  future  observations, would put the entire standard
model  "in   trouble".    Earlier  estimates  of  this  "trouble"
threshold have already been violated.

     PSTK then note  that  the  Cold Dark Matter (CDM) version of
the standard model is  apparently  already in trouble, which they
describe as a "blow to  simplicity"  for our understanding of the
universe.

Section VIII. Alternative cosmologies

     PSTK may be  less familiar with alternative cosmologies than
with the standard model,  because  this  is  the  only section in
which I would argue with  their  "facts"  instead  of  just their
interpretation.   For example, by comparing  infrared  and  radio
wavelengths, Lerner has shown that radio galaxy  luminosities  do
attenuate  with distance, contrary to what PSTK say.    And  PSTK
have  applied  their  own  equation (6), the assumption that  the
background  radiation  (CBR) is due to a cooling fireball with  a
distance-dependent temperature, to  "prove" that the CBR spectrum
is inconsistent with certain  other models.  But most alternative
cosmologies  expect  a thermalized radiation  source  of  uniform
temperature at all distances, which yields  a blackbody spectrum;
so this PSTK argument is invalid.

     PSTK  give  no  consideration to alternative cosmologies  in
which  the cosmological redshift is due to something  other  than
velocity.    This  is  certainly  a  serious limitation of  their
discussion.

Section IX. Evaluation and opportunity

     Here PSTK list possible future observations which would tend
to falsify  the  standard  model:  an important criterion for any
viable theory.  These include findings of inhomogeneity in matter
distribution  greater  than  one  part  in  10^4  over  distances
comparable with the Hubble distance;  the finding of objects with
helium 4 abundances well under 24%;    or  the  determination  of
cluster ages well in excess of the  Hubble  age.  The difficulty,
of course, is the irresistible urge to add  new hypotheses to the
model to keep it compatible with observations, no matter what may
be found in the future, as has already happened numerous times in
the history of the Big Bang model.

     As scientists,  we  understand  the necessity that models be
falsifiable;  but  as  humans,  we are loath to admit it when the
falsification criteria have been  met.    But  perhaps  we may at
least hope for a lesser goal:  if any of the arguments herein, or
any future observations, should tend to  undermine  confidence in
the  standard  model,  then  perhaps  we  could   return  to  the
scientifically more desirable status of having all viable  models
on  the  table  for  future discussion and the interpretation  of
observations,  instead  of  just one of them.  Our knowledge  and
understanding  would   surely  grow  more  rapidly  from  such  a
scientifically commendable approach.

--
Tom Van Flandern / Washington, DC / metares@well.sf.ca.us
Meta Research was founded to foster research into ideas not otherwise
supported because they conflict with mainstream theories in Astronomy.