4.2. Disk evolution
The sizes of disks in the hierarchical scenario decrease significantly
with redshift
(Mao, Mo et al. 1998;
Giallongo et al. 1999;
Avila-Reese & Firmani
2001).
Interpretation of data regarding disk size and SB evolution is
controversial.
Roche et al. (1998)
using HST data concluded that since
z 1, spirals
suffered both size and luminosity evolution, while
Simard et al. (1999)
concluded that data show no size evolution.
Bouwens & Silk (2002)
show that the SB distribution of disk galaxies evolves strongly. They
re-analyzed the data of
Simard et al. introducing new corrections for SB selection bias and found
size evolution in the data. The question is open.
The SF history of disk models is driven by both the gas accretion rate
determined by the MAH, and the disk surface density determined by
(Avila-Reese & Firmani
2001).
Merging could also play a relevant role
(Kauffmann et al. 2001).
The increase of the SF rate (and B-band luminosity)
with z inferred from observations of normal spirals (e.g.,
Lilly et al. 1997;
Abraham et al. 1999)
is slightly steeper than our model predictions. The
integral colors of the models become bluer toward the past, in agreement
with observations.
The evolution of the TFR is a highly debated topic and apparently it depends
on whether the studied sample is dominated by small or normal spirals.
Model predictions show that the slope of the B-band TFR
decreases and the zero point becomes brighter at higher z's
(Fig. 3; see also
Avila-Reese & Firmani
2001).
Comparing with the observed sample of
Vogt et al. (1997)
at < z > = 0.54,
the agreement in the zero point is reasonable (for the
CDM cosmology).
On the other hand models show that the zero-point of TFR in the near
infrared band evolves in an opposite way: at z = 1 it is fainter
than at z = 0.
(see Fig. 3)
This can be understood taking into account that galaxy evolution traces
halo
evolution: the halo mass (scaling with the disk mass traced by the infrared
luminosity) decreases significantly from z = 0 to z = 1,
while Vmax
decreases only moderately. In the case of the B-band, since the
accretion
rate peaks at z ~ 1 - 2, the star formation rate, and therefore
LB, are
(slightly) higher at these reshifts. The evolution of the comoving number
density of halos is connected with the TFR; a deficit of bright (massive)
galaxies at larger redshifts translates into a dimming of the zero-point of
the infrared TFR
(Bullock et al. 2001a).
The evolution of the TFR up to high
redshifts (z ~ 3) can be a potentially powerful discriminator of
galaxy formation models
(Buchalter, Jiménez
& Kamionkowski 2001).
![]() |
Figure 3. Evolution of the model TFR in the
bands B and K. The
slopes at different redshifts were fixed to the corresponing ones at
z = 0. The zero-point becomes brighter at higher redshifts in
the band B, while in the band K the behaviour is opposite
(see text). The arrow indicates the lower limit inferred from observations
by Vogt et al. (1997);
we have passed their data to the
|