Consider the density contrasts of visible objects and mass,
and
, at a position
and a redshift
smoothed over a scale
[86
]. In general, the former should depend on various
other auxiliary variables
defined at different locations
and redshifts
smoothed over different
scales
in addition to the mass density contrast at the same position,
. While this relation
can be schematically expressed as
For illustrative purposes, we define the biasing factor as the ratio of the density contrasts of luminous objects and mass:
Only in very idealized situations, the above nonlocal stochastic nonlinear factor in terms ofFrom the above point of view, the local deterministic linear bias is obviously unrealistic, but is still a widely
used conventional model for biasing. In fact, the time- and scale-dependence of the linear bias
factor
was neglected in many previous studies of biased galaxy formation until very
recently. Currently, however, various models beyond the deterministic linear biasing have been
seriously considered with particular emphasis on the nonlinear and stochastic aspects of the
biasing [71, 15
, 87
, 86
].
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